diff --git a/.gitlab-ci.yml b/.gitlab-ci.yml
index 56a048c1f0..98f8c7cc93 100644
--- a/.gitlab-ci.yml
+++ b/.gitlab-ci.yml
@@ -1,4 +1,5 @@
+
 include:
     project: 'EBC/EBC_all/gitlab_ci/templates'
-    ref: AixLib
-    file: 'dymola-ci-tests/ci_templates/.gitlab-ci.yml'
+    ref: AixLibCI
+    file: 'modelica-ci-tests/scripts/.gitlab-ci.yml'
diff --git a/AixLib/.copiedFiles.txt b/AixLib/.copiedFiles.txt
deleted file mode 100644
index 8f67174064..0000000000
--- a/AixLib/.copiedFiles.txt
+++ /dev/null
@@ -1,2503 +0,0 @@
-# Do not edit this file unless you know what you are doing.
-# This file is used by the IBPSA merge script and generated by BuildingsPy.
-AixLib/Airflow/Multizone/BaseClasses/Door.mo
-AixLib/Airflow/Multizone/BaseClasses/DoorDiscretized.mo
-AixLib/Airflow/Multizone/BaseClasses/ErrorControl.mo
-AixLib/Airflow/Multizone/BaseClasses/Examples/Interpolate.mo
-AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLaw.mo
-AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLawFixedM.mo
-AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureLowRise.mo
-AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureProfile.mo
-AixLib/Airflow/Multizone/BaseClasses/Examples/package.mo
-AixLib/Airflow/Multizone/BaseClasses/Examples/package.order
-AixLib/Airflow/Multizone/BaseClasses/PartialOneWayFlowElement.mo
-AixLib/Airflow/Multizone/BaseClasses/PowerLawResistanceParameters.mo
-AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElement.mo
-AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElementBuoyancy.mo
-AixLib/Airflow/Multizone/BaseClasses/ZonalFlow.mo
-AixLib/Airflow/Multizone/BaseClasses/interpolate.mo
-AixLib/Airflow/Multizone/BaseClasses/package.mo
-AixLib/Airflow/Multizone/BaseClasses/package.order
-AixLib/Airflow/Multizone/BaseClasses/powerLaw.mo
-AixLib/Airflow/Multizone/BaseClasses/powerLawFixedM.mo
-AixLib/Airflow/Multizone/BaseClasses/windPressureLowRise.mo
-AixLib/Airflow/Multizone/BaseClasses/windPressureProfile.mo
-AixLib/Airflow/Multizone/Coefficient_V_flow.mo
-AixLib/Airflow/Multizone/Coefficient_m_flow.mo
-AixLib/Airflow/Multizone/DoorDiscretizedOpen.mo
-AixLib/Airflow/Multizone/DoorDiscretizedOperable.mo
-AixLib/Airflow/Multizone/DoorOpen.mo
-AixLib/Airflow/Multizone/DoorOperable.mo
-AixLib/Airflow/Multizone/EffectiveAirLeakageArea.mo
-AixLib/Airflow/Multizone/Examples/CO2TransportStep.mo
-AixLib/Airflow/Multizone/Examples/ChimneyShaftNoVolume.mo
-AixLib/Airflow/Multizone/Examples/ChimneyShaftWithVolume.mo
-AixLib/Airflow/Multizone/Examples/ClosedDoors.mo
-AixLib/Airflow/Multizone/Examples/NaturalVentilation.mo
-AixLib/Airflow/Multizone/Examples/OneEffectiveAirLeakageArea.mo
-AixLib/Airflow/Multizone/Examples/OneOpenDoor.mo
-AixLib/Airflow/Multizone/Examples/OneRoom.mo
-AixLib/Airflow/Multizone/Examples/Orifice.mo
-AixLib/Airflow/Multizone/Examples/PowerLaw.mo
-AixLib/Airflow/Multizone/Examples/PressurizationData.mo
-AixLib/Airflow/Multizone/Examples/ReverseBuoyancy.mo
-AixLib/Airflow/Multizone/Examples/ReverseBuoyancy3Zones.mo
-AixLib/Airflow/Multizone/Examples/TrickleVent.mo
-AixLib/Airflow/Multizone/Examples/ZonalFlow.mo
-AixLib/Airflow/Multizone/Examples/package.mo
-AixLib/Airflow/Multizone/Examples/package.order
-AixLib/Airflow/Multizone/MediumColumn.mo
-AixLib/Airflow/Multizone/MediumColumnDynamic.mo
-AixLib/Airflow/Multizone/Orifice.mo
-AixLib/Airflow/Multizone/Point_m_flow.mo
-AixLib/Airflow/Multizone/Points_m_flow.mo
-AixLib/Airflow/Multizone/Table_V_flow.mo
-AixLib/Airflow/Multizone/Table_m_flow.mo
-AixLib/Airflow/Multizone/Types/densitySelection.mo
-AixLib/Airflow/Multizone/Types/package.mo
-AixLib/Airflow/Multizone/Types/package.order
-AixLib/Airflow/Multizone/UsersGuide.mo
-AixLib/Airflow/Multizone/Validation/DoorOpenClosed.mo
-AixLib/Airflow/Multizone/Validation/OneWayFlow.mo
-AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyDynamic.mo
-AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyPressureDynamic.mo
-AixLib/Airflow/Multizone/Validation/OpenDoorPressure.mo
-AixLib/Airflow/Multizone/Validation/OpenDoorTemperature.mo
-AixLib/Airflow/Multizone/Validation/ThreeRoomsContam.mo
-AixLib/Airflow/Multizone/Validation/ThreeRoomsContamDiscretizedDoor.mo
-AixLib/Airflow/Multizone/Validation/package.mo
-AixLib/Airflow/Multizone/Validation/package.order
-AixLib/Airflow/Multizone/ZonalFlow_ACS.mo
-AixLib/Airflow/Multizone/ZonalFlow_m_flow.mo
-AixLib/Airflow/Multizone/package.mo
-AixLib/Airflow/Multizone/package.order
-AixLib/Airflow/package.mo
-AixLib/Airflow/package.order
-AixLib/BoundaryConditions/SkyTemperature/BlackBody.mo
-AixLib/BoundaryConditions/SkyTemperature/Examples/BlackBody.mo
-AixLib/BoundaryConditions/SkyTemperature/Examples/package.mo
-AixLib/BoundaryConditions/SkyTemperature/Examples/package.order
-AixLib/BoundaryConditions/SkyTemperature/package.mo
-AixLib/BoundaryConditions/SkyTemperature/package.order
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/AltitudeAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Declination.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/AltitudeAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/Declination.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/IncidenceAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarAzimuth.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarHourAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/WallSolarAzimuth.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/ZenithAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/package.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/package.order
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/IncidenceAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarAzimuth.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarHourAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/WallSolarAzimuth.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/ZenithAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/package.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/package.order
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthNoEvent.mo
-AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthWithEvent.mo
-AixLib/BoundaryConditions/SolarGeometry/Examples/IncidenceAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/Examples/ZenithAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/Examples/package.mo
-AixLib/BoundaryConditions/SolarGeometry/Examples/package.order
-AixLib/BoundaryConditions/SolarGeometry/IncidenceAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/ZenithAngle.mo
-AixLib/BoundaryConditions/SolarGeometry/package.mo
-AixLib/BoundaryConditions/SolarGeometry/package.order
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/BrighteningCoefficient.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffuseIsotropic.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffusePerez.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DirectTiltedSurface.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/BrighteningCoefficient.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/DiffuseIsotropic.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/RelativeAirMass.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyBrightness.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyClearness.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/package.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/package.order
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/PartialSolarIrradiation.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/RelativeAirMass.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyBrightness.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyClearness.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/package.mo
-AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/package.order
-AixLib/BoundaryConditions/SolarIrradiation/DiffuseIsotropic.mo
-AixLib/BoundaryConditions/SolarIrradiation/DiffusePerez.mo
-AixLib/BoundaryConditions/SolarIrradiation/DirectTiltedSurface.mo
-AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffuseIsotropic.mo
-AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffusePerez.mo
-AixLib/BoundaryConditions/SolarIrradiation/Examples/DirectTiltedSurface.mo
-AixLib/BoundaryConditions/SolarIrradiation/Examples/package.mo
-AixLib/BoundaryConditions/SolarIrradiation/Examples/package.order
-AixLib/BoundaryConditions/SolarIrradiation/package.mo
-AixLib/BoundaryConditions/SolarIrradiation/package.order
-AixLib/BoundaryConditions/Types.mo
-AixLib/BoundaryConditions/UsersGuide.mo
-AixLib/BoundaryConditions/Validation/BESTEST/WD100.mo
-AixLib/BoundaryConditions/Validation/BESTEST/WD200.mo
-AixLib/BoundaryConditions/Validation/BESTEST/WD300.mo
-AixLib/BoundaryConditions/Validation/BESTEST/WD400.mo
-AixLib/BoundaryConditions/Validation/BESTEST/WD500.mo
-AixLib/BoundaryConditions/Validation/BESTEST/WD600.mo
-AixLib/BoundaryConditions/Validation/BESTEST/package.mo
-AixLib/BoundaryConditions/Validation/BESTEST/package.order
-AixLib/BoundaryConditions/Validation/IsotropicAndPerezDiffuseRadiation.mo
-AixLib/BoundaryConditions/Validation/UsersGuide.mo
-AixLib/BoundaryConditions/Validation/package.mo
-AixLib/BoundaryConditions/Validation/package.order
-AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckBlackBodySkyTemperature.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDewPointTemperature.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDryBulbTemperature.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckPressure.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/ConvertTime.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/EquationOfTime.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckBlackBodySkyTemperature.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckPressure.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckTemperature.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTime.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimeNegativeStart.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimePositiveStart.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/EquationOfTime.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAbsolutePath.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAltitudeTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetHeaderElement.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3LongHeader.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3_NonzeroStart.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LimitMin.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LocalCivilTime.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/SolarTime.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/package.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/package.order
-AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterCeilingHeight.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterHorizontalInfraredIrradiation.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterOpaqueSkyCover.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterRelativeHumidity.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterTotalSkyCover.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindDirection.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindSpeed.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/LocalCivilTime.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiter.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiterMin.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/SolarTime.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelector.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelectorRadiation.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/getAbsolutePath.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/getAltitudeLocationTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/getHeaderElementTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/getLastHeaderElementTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/getLatitudeTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/getLongitudeTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeSpanTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeZoneTMY3.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/package.mo
-AixLib/BoundaryConditions/WeatherData/BaseClasses/package.order
-AixLib/BoundaryConditions/WeatherData/Bus.mo
-AixLib/BoundaryConditions/WeatherData/Examples/ReaderTMY3.mo
-AixLib/BoundaryConditions/WeatherData/Examples/package.mo
-AixLib/BoundaryConditions/WeatherData/Examples/package.order
-AixLib/BoundaryConditions/WeatherData/ReaderTMY3.mo
-AixLib/BoundaryConditions/WeatherData/Validation/DecemberToJanuary.mo
-AixLib/BoundaryConditions/WeatherData/Validation/OverAYear_usingOneYearData.mo
-AixLib/BoundaryConditions/WeatherData/Validation/ReaderTMY3HDirNor.mo
-AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearData.mo
-AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataNegativeStart.mo
-AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataPositiveStart.mo
-AixLib/BoundaryConditions/WeatherData/Validation/package.mo
-AixLib/BoundaryConditions/WeatherData/Validation/package.order
-AixLib/BoundaryConditions/WeatherData/package.mo
-AixLib/BoundaryConditions/WeatherData/package.order
-AixLib/BoundaryConditions/package.mo
-AixLib/BoundaryConditions/package.order
-AixLib/Controls/Continuous/Examples/LimPID.mo
-AixLib/Controls/Continuous/Examples/LimPIDWithReset.mo
-AixLib/Controls/Continuous/Examples/NumberOfRequests.mo
-AixLib/Controls/Continuous/Examples/OffTimer.mo
-AixLib/Controls/Continuous/Examples/SignalRanker.mo
-AixLib/Controls/Continuous/Examples/package.mo
-AixLib/Controls/Continuous/Examples/package.order
-AixLib/Controls/Continuous/LimPID.mo
-AixLib/Controls/Continuous/NumberOfRequests.mo
-AixLib/Controls/Continuous/OffTimer.mo
-AixLib/Controls/Continuous/SignalRanker.mo
-AixLib/Controls/Continuous/Validation/LimPIDReset.mo
-AixLib/Controls/Continuous/Validation/OffTimerNonZeroStart.mo
-AixLib/Controls/Continuous/Validation/package.mo
-AixLib/Controls/Continuous/Validation/package.order
-AixLib/Controls/Continuous/package.mo
-AixLib/Controls/Continuous/package.order
-AixLib/Controls/Discrete/BooleanDelay.mo
-AixLib/Controls/Discrete/Examples/BooleanDelay.mo
-AixLib/Controls/Discrete/Examples/package.mo
-AixLib/Controls/Discrete/Examples/package.order
-AixLib/Controls/Discrete/package.mo
-AixLib/Controls/Discrete/package.order
-AixLib/Controls/SetPoints/Examples/OccupancySchedule.mo
-AixLib/Controls/SetPoints/Examples/SupplyReturnTemperatureReset.mo
-AixLib/Controls/SetPoints/Examples/Table.mo
-AixLib/Controls/SetPoints/Examples/package.mo
-AixLib/Controls/SetPoints/Examples/package.order
-AixLib/Controls/SetPoints/OccupancySchedule.mo
-AixLib/Controls/SetPoints/SupplyReturnTemperatureReset.mo
-AixLib/Controls/SetPoints/Table.mo
-AixLib/Controls/SetPoints/Validation/OccupancyScheduleNegativeStartTime.mo
-AixLib/Controls/SetPoints/Validation/OccupancySchedulePositiveStartTime.mo
-AixLib/Controls/SetPoints/Validation/package.mo
-AixLib/Controls/SetPoints/Validation/package.order
-AixLib/Controls/SetPoints/package.mo
-AixLib/Controls/SetPoints/package.order
-AixLib/Controls/package.mo
-AixLib/Controls/package.order
-AixLib/Fluid/Actuators/BaseClasses/ActuatorSignal.mo
-AixLib/Fluid/Actuators/BaseClasses/Examples/EqualPercentageDerivativeCheck.mo
-AixLib/Fluid/Actuators/BaseClasses/Examples/package.mo
-AixLib/Fluid/Actuators/BaseClasses/Examples/package.order
-AixLib/Fluid/Actuators/BaseClasses/PartialDamperExponential.mo
-AixLib/Fluid/Actuators/BaseClasses/PartialThreeWayValve.mo
-AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValve.mo
-AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValveKv.mo
-AixLib/Fluid/Actuators/BaseClasses/ValveParameters.mo
-AixLib/Fluid/Actuators/BaseClasses/der_equalPercentage.mo
-AixLib/Fluid/Actuators/BaseClasses/equalPercentage.mo
-AixLib/Fluid/Actuators/BaseClasses/exponentialDamper.mo
-AixLib/Fluid/Actuators/BaseClasses/package.mo
-AixLib/Fluid/Actuators/BaseClasses/package.order
-AixLib/Fluid/Actuators/Dampers/Examples/Damper.mo
-AixLib/Fluid/Actuators/Dampers/Examples/MixingBox.mo
-AixLib/Fluid/Actuators/Dampers/Examples/VAVBoxExponential.mo
-AixLib/Fluid/Actuators/Dampers/Examples/package.mo
-AixLib/Fluid/Actuators/Dampers/Examples/package.order
-AixLib/Fluid/Actuators/Dampers/Exponential.mo
-AixLib/Fluid/Actuators/Dampers/MixingBox.mo
-AixLib/Fluid/Actuators/Dampers/PressureIndependent.mo
-AixLib/Fluid/Actuators/Dampers/Validation/PressureIndependent.mo
-AixLib/Fluid/Actuators/Dampers/Validation/package.mo
-AixLib/Fluid/Actuators/Dampers/Validation/package.order
-AixLib/Fluid/Actuators/Dampers/package.mo
-AixLib/Fluid/Actuators/Dampers/package.order
-AixLib/Fluid/Actuators/Motors/Examples/IdealMotor.mo
-AixLib/Fluid/Actuators/Motors/Examples/package.mo
-AixLib/Fluid/Actuators/Motors/Examples/package.order
-AixLib/Fluid/Actuators/Motors/IdealMotor.mo
-AixLib/Fluid/Actuators/Motors/package.mo
-AixLib/Fluid/Actuators/Motors/package.order
-AixLib/Fluid/Actuators/Valves/Data/Generic.mo
-AixLib/Fluid/Actuators/Valves/Data/Linear.mo
-AixLib/Fluid/Actuators/Valves/Data/package.mo
-AixLib/Fluid/Actuators/Valves/Data/package.order
-AixLib/Fluid/Actuators/Valves/Examples/ThreeWayValves.mo
-AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvePressureIndependent.mo
-AixLib/Fluid/Actuators/Valves/Examples/TwoWayValveTable.mo
-AixLib/Fluid/Actuators/Valves/Examples/TwoWayValves.mo
-AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesMotor.mo
-AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesTable.mo
-AixLib/Fluid/Actuators/Valves/Examples/package.mo
-AixLib/Fluid/Actuators/Valves/Examples/package.order
-AixLib/Fluid/Actuators/Valves/ThreeWayEqualPercentageLinear.mo
-AixLib/Fluid/Actuators/Valves/ThreeWayLinear.mo
-AixLib/Fluid/Actuators/Valves/ThreeWayTable.mo
-AixLib/Fluid/Actuators/Valves/TwoWayButterfly.mo
-AixLib/Fluid/Actuators/Valves/TwoWayEqualPercentage.mo
-AixLib/Fluid/Actuators/Valves/TwoWayLinear.mo
-AixLib/Fluid/Actuators/Valves/TwoWayPolynomial.mo
-AixLib/Fluid/Actuators/Valves/TwoWayPressureIndependent.mo
-AixLib/Fluid/Actuators/Valves/TwoWayQuickOpening.mo
-AixLib/Fluid/Actuators/Valves/TwoWayTable.mo
-AixLib/Fluid/Actuators/Valves/Validation/ThreeWayValveParameterization.mo
-AixLib/Fluid/Actuators/Valves/Validation/TwoWayValveParameterization.mo
-AixLib/Fluid/Actuators/Valves/Validation/package.mo
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-AixLib/Fluid/Actuators/Valves/package.mo
-AixLib/Fluid/Actuators/Valves/package.order
-AixLib/Fluid/Actuators/package.mo
-AixLib/Fluid/Actuators/package.order
-AixLib/Fluid/BaseClasses/ActuatorFilter.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck2.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck2.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/InverseFlowFunctions.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_dp.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_m_flow.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/package.mo
-AixLib/Fluid/BaseClasses/FlowModels/Validation/package.order
-AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp.mo
-AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der.mo
-AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der2.mo
-AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow.mo
-AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der.mo
-AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der2.mo
-AixLib/Fluid/BaseClasses/FlowModels/package.mo
-AixLib/Fluid/BaseClasses/FlowModels/package.order
-AixLib/Fluid/BaseClasses/IndexMassFraction.mo
-AixLib/Fluid/BaseClasses/MassFlowRateMultiplier.mo
-AixLib/Fluid/BaseClasses/PartialResistance.mo
-AixLib/Fluid/BaseClasses/PartialThreeWayResistance.mo
-AixLib/Fluid/BaseClasses/Validation/ActuatorFilter.mo
-AixLib/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mo
-AixLib/Fluid/BaseClasses/Validation/package.mo
-AixLib/Fluid/BaseClasses/Validation/package.order
-AixLib/Fluid/BaseClasses/package.mo
-AixLib/Fluid/BaseClasses/package.order
-AixLib/Fluid/Chillers/BaseClasses/Carnot.mo
-AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_T.mo
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-AixLib/Utilities/Math/SmoothLimit.mo
-AixLib/Utilities/Math/SmoothMax.mo
-AixLib/Utilities/Math/SmoothMin.mo
-AixLib/Utilities/Math/Splice.mo
-AixLib/Utilities/Math/TrapezoidalIntegration.mo
-AixLib/Utilities/Math/package.mo
-AixLib/Utilities/Math/package.order
-AixLib/Utilities/Psychrometrics/BaseClasses/HumidityRatioVaporPressure.mo
-AixLib/Utilities/Psychrometrics/BaseClasses/package.mo
-AixLib/Utilities/Psychrometrics/BaseClasses/package.order
-AixLib/Utilities/Psychrometrics/Constants.mo
-AixLib/Utilities/Psychrometrics/Density_pTX.mo
-AixLib/Utilities/Psychrometrics/Examples/Density_pTX.mo
-AixLib/Utilities/Psychrometrics/Examples/DewPointTemperature.mo
-AixLib/Utilities/Psychrometrics/Examples/HumidityRatioPressure.mo
-AixLib/Utilities/Psychrometrics/Examples/MassFraction_pTphi.mo
-AixLib/Utilities/Psychrometrics/Examples/Phi_pTX.mo
-AixLib/Utilities/Psychrometrics/Examples/SaturationPressure.mo
-AixLib/Utilities/Psychrometrics/Examples/SaturationPressureLiquid.mo
-AixLib/Utilities/Psychrometrics/Examples/SublimationPressureIce.mo
-AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulPhi.mo
-AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulXi.mo
-AixLib/Utilities/Psychrometrics/Examples/TotalAirDryAir.mo
-AixLib/Utilities/Psychrometrics/Examples/package.mo
-AixLib/Utilities/Psychrometrics/Examples/package.order
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck_amb.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/InverseDewPointTemperatureDerivativeCheck_amb.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/SaturationPressureDerivativeCheck.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/WaterVaporPressureDerivativeCheck.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/package.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/package.order
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_TDewPoi_pW_amb.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi_amb.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_X.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_saturationPressureLiquid.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_sublimationPressureIce.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/package.mo
-AixLib/Utilities/Psychrometrics/Functions/BaseClasses/package.order
-AixLib/Utilities/Psychrometrics/Functions/Examples/Density_pTX.mo
-AixLib/Utilities/Psychrometrics/Functions/Examples/SaturationPressure.mo
-AixLib/Utilities/Psychrometrics/Functions/Examples/X_pSatpphi.mo
-AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi.mo
-AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi_comparison.mo
-AixLib/Utilities/Psychrometrics/Functions/Examples/pW_X.mo
-AixLib/Utilities/Psychrometrics/Functions/Examples/package.mo
-AixLib/Utilities/Psychrometrics/Functions/Examples/package.order
-AixLib/Utilities/Psychrometrics/Functions/Examples/phi_pTX.mo
-AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW.mo
-AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW_amb.mo
-AixLib/Utilities/Psychrometrics/Functions/X_pSatpphi.mo
-AixLib/Utilities/Psychrometrics/Functions/X_pTphi.mo
-AixLib/Utilities/Psychrometrics/Functions/X_pW.mo
-AixLib/Utilities/Psychrometrics/Functions/density_pTX.mo
-AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi.mo
-AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi_amb.mo
-AixLib/Utilities/Psychrometrics/Functions/pW_X.mo
-AixLib/Utilities/Psychrometrics/Functions/package.mo
-AixLib/Utilities/Psychrometrics/Functions/package.order
-AixLib/Utilities/Psychrometrics/Functions/phi_pTX.mo
-AixLib/Utilities/Psychrometrics/Functions/saturationPressure.mo
-AixLib/Utilities/Psychrometrics/Functions/saturationPressureLiquid.mo
-AixLib/Utilities/Psychrometrics/Functions/sublimationPressureIce.mo
-AixLib/Utilities/Psychrometrics/Phi_pTX.mo
-AixLib/Utilities/Psychrometrics/SaturationPressure.mo
-AixLib/Utilities/Psychrometrics/SaturationPressureLiquid.mo
-AixLib/Utilities/Psychrometrics/SublimationPressureIce.mo
-AixLib/Utilities/Psychrometrics/TDewPoi_pW.mo
-AixLib/Utilities/Psychrometrics/TWetBul_TDryBulPhi.mo
-AixLib/Utilities/Psychrometrics/TWetBul_TDryBulXi.mo
-AixLib/Utilities/Psychrometrics/ToDryAir.mo
-AixLib/Utilities/Psychrometrics/ToTotalAir.mo
-AixLib/Utilities/Psychrometrics/X_pTphi.mo
-AixLib/Utilities/Psychrometrics/X_pW.mo
-AixLib/Utilities/Psychrometrics/hSat_pTSat.mo
-AixLib/Utilities/Psychrometrics/pW_TDewPoi.mo
-AixLib/Utilities/Psychrometrics/pW_X.mo
-AixLib/Utilities/Psychrometrics/package.mo
-AixLib/Utilities/Psychrometrics/package.order
-AixLib/Utilities/Time/CalendarTime.mo
-AixLib/Utilities/Time/Examples/CalendarTime.mo
-AixLib/Utilities/Time/Examples/ModelTime.mo
-AixLib/Utilities/Time/Examples/package.mo
-AixLib/Utilities/Time/Examples/package.order
-AixLib/Utilities/Time/ModelTime.mo
-AixLib/Utilities/Time/Types/ZeroTime.mo
-AixLib/Utilities/Time/Types/package.mo
-AixLib/Utilities/Time/Types/package.order
-AixLib/Utilities/Time/Validation/CalendarTimeMonths.mo
-AixLib/Utilities/Time/Validation/CalendarTimeMonthsMinus.mo
-AixLib/Utilities/Time/Validation/CalendarTimeMonthsPlus.mo
-AixLib/Utilities/Time/Validation/package.mo
-AixLib/Utilities/Time/Validation/package.order
-AixLib/Utilities/Time/package.mo
-AixLib/Utilities/Time/package.order
-AixLib/Utilities/package.mo
-AixLib/Utilities/package.order
-AixLib/package.order
diff --git a/AixLib/Airflow/Multizone/BaseClasses/Door.mo b/AixLib/Airflow/Multizone/BaseClasses/Door.mo
index c8fa35d402..c85ab3a5dc 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/Door.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/Door.mo
@@ -111,18 +111,18 @@ equation
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid)}),
     Documentation(info="<html>
- <p>
- This is a partial model for the bi-directional air flow through a door.
- </p>
- </html>",
+<p>
+This is a partial model for the bi-directional air flow through a door.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 6, 2020, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1353\">#1353</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 6, 2020, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1353\">#1353</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Door;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/DoorDiscretized.mo b/AixLib/Airflow/Multizone/BaseClasses/DoorDiscretized.mo
index 96d52116da..888602d90f 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/DoorDiscretized.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/DoorDiscretized.mo
@@ -102,72 +102,72 @@ equation
         Line(points={{-54,-58},{-36,-58}}, color={0,0,0}),
         Line(points={{-54,-32},{-36,-32}}, color={0,0,0})}),
     Documentation(info="<html>
- <p>
- This is a partial model for the bi-directional air flow through a door.
- </p>
- <p>
- To compute the bi-directional flow,
- the door is discretize along the height coordinate, and uses
- an orifice equation to compute the flow for each compartment.
- </p>
- <p>
- The compartment area <code>dA</code> is a variable, which allows
- using the model for a door that can be open or closed.
- </p>
- </html>",
+<p>
+This is a partial model for the bi-directional air flow through a door.
+</p>
+<p>
+To compute the bi-directional flow,
+the door is discretize along the height coordinate, and uses
+an orifice equation to compute the flow for each compartment.
+</p>
+<p>
+The compartment area <code>dA</code> is a variable, which allows
+using the model for a door that can be open or closed.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 8, 2019, by Michael Wetter:<br/>
- Moved parameter <code>CD</code> from
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized\">
- AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized</a>
- to
- <a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOpen\">
- AixLib.Airflow.Multizone.DoorDiscretizedOpen</a>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/971\">#971</a>.
- </li>
- <li>
- June 27, 2018, by Michael Wetter:<br/>
- Corrected old parameter annotation.
- </li>
- <li>
- June 6, 2018, by Michael Wetter:<br/>
- Removed term that assures non-zero flow rate in each path, and
- reformulated flow balance to ensure that model is symmetric.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/937\">#937</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- September 26, 2013 by Michael Wetter:<br/>
- Added missing <code>each</code> keyword.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li><i>December 6, 2011</i> by Michael Wetter:<br/>
-        Removed protected variable <code>rhoAve</code>.
- </li>
- <li><i>August 12, 2011</i> by Michael Wetter:<br/>
-        Changed model to use the new function
-        <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
-        Buildings.Airflow.Multizone.BaseClasses.powerLawFixedM</a>.
- </li>
- <li><i>July 20, 2010</i> by Michael Wetter:<br/>
-        Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li><i>February 8, 2005</i> by Michael Wetter:<br/>
-        Released first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 8, 2019, by Michael Wetter:<br/>
+Moved parameter <code>CD</code> from
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized\">
+AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized</a>
+to
+<a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOpen\">
+AixLib.Airflow.Multizone.DoorDiscretizedOpen</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/971\">#971</a>.
+</li>
+<li>
+June 27, 2018, by Michael Wetter:<br/>
+Corrected old parameter annotation.
+</li>
+<li>
+June 6, 2018, by Michael Wetter:<br/>
+Removed term that assures non-zero flow rate in each path, and
+reformulated flow balance to ensure that model is symmetric.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/937\">#937</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+September 26, 2013 by Michael Wetter:<br/>
+Added missing <code>each</code> keyword.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li><i>December 6, 2011</i> by Michael Wetter:<br/>
+       Removed protected variable <code>rhoAve</code>.
+</li>
+<li><i>August 12, 2011</i> by Michael Wetter:<br/>
+       Changed model to use the new function
+       <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
+       Buildings.Airflow.Multizone.BaseClasses.powerLawFixedM</a>.
+</li>
+<li><i>July 20, 2010</i> by Michael Wetter:<br/>
+       Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li><i>February 8, 2005</i> by Michael Wetter:<br/>
+       Released first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DoorDiscretized;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/ErrorControl.mo b/AixLib/Airflow/Multizone/BaseClasses/ErrorControl.mo
index 299b7a551c..fa0352688a 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/ErrorControl.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/ErrorControl.mo
@@ -5,41 +5,41 @@ model ErrorControl "Interface that defines parameters for error control"
     annotation(Dialog(tab="Advanced"));
 
   annotation (Documentation(info="<html>
- <p>
- This is an interface that defines parameters used for error control.
- </p>
- <p>
- Dymola does error control on state variables, such as temperature, pressure and
- species concentration.
- Flow variables such as <code>m_flow</code> are typically not checked during the error control.
- This can give large errors in flow variables, as long as the error on the volume's state variables
- that are coupled to the flow variables is small.
- Obtaining accurate flow variables can be achieved by imposing an error control
- on the exchanged mass, which can be defined as
- </p>
- <pre>
-   dm/dt = m_flow.
- </pre>
- <p>
- By setting <code>forceErrorControlOnFlow = true</code>, such an equation is imposed
- by models that extend this class.
- </p>
- </html>",
+<p>
+This is an interface that defines parameters used for error control.
+</p>
+<p>
+Dymola does error control on state variables, such as temperature, pressure and
+species concentration.
+Flow variables such as <code>m_flow</code> are typically not checked during the error control.
+This can give large errors in flow variables, as long as the error on the volume's state variables
+that are coupled to the flow variables is small.
+Obtaining accurate flow variables can be achieved by imposing an error control
+on the exchanged mass, which can be defined as
+</p>
+<pre>
+  dm/dt = m_flow.
+</pre>
+<p>
+By setting <code>forceErrorControlOnFlow = true</code>, such an equation is imposed
+by models that extend this class.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 27, 2018, by Michael Wetter:<br/>
- Moved parameter <code>forceErrorControlOnFlow</code> to the Advanced tab.
- </li>
- <li>
- July 20, 2010 by Michael Wetter:<br/>
- Integrated model into the Buildings library.
- </li>
- <li>
- November 1, 2005 by Michael Wetter:<br/>
- Released first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 27, 2018, by Michael Wetter:<br/>
+Moved parameter <code>forceErrorControlOnFlow</code> to the Advanced tab.
+</li>
+<li>
+July 20, 2010 by Michael Wetter:<br/>
+Integrated model into the Buildings library.
+</li>
+<li>
+November 1, 2005 by Michael Wetter:<br/>
+Released first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ErrorControl;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLaw.mo b/AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLaw.mo
index d6d3d644d7..cf82c37a2a 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLaw.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLaw.mo
@@ -21,19 +21,19 @@ equation
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/BaseClasses/Examples/PowerLaw.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This examples demonstrates the
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLaw\">
- Buildings.Airflow.Multizone.BaseClasses.powerLaw</a>
- function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 12, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This examples demonstrates the
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLaw\">
+Buildings.Airflow.Multizone.BaseClasses.powerLaw</a>
+function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 12, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerLaw;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLawFixedM.mo b/AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLawFixedM.mo
index 9ebb0a0ada..c452bc686b 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLawFixedM.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/Examples/PowerLawFixedM.mo
@@ -46,24 +46,24 @@ equation
 experiment(Tolerance=1e-6, StopTime=1.0),
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/BaseClasses/Examples/PowerLawFixedM.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This examples demonstrates the
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLaw\">
- Buildings.Airflow.Multizone.BaseClasses.powerLaw</a>
- and
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
- Buildings.Airflow.Multizone.BaseClasses.powerLawFixedM</a>
- functions.
- They need to return the same function value.
- This is verified by an <code>assert</code> statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 12, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This examples demonstrates the
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLaw\">
+Buildings.Airflow.Multizone.BaseClasses.powerLaw</a>
+and
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
+Buildings.Airflow.Multizone.BaseClasses.powerLawFixedM</a>
+functions.
+They need to return the same function value.
+This is verified by an <code>assert</code> statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 12, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerLawFixedM;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureLowRise.mo b/AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureLowRise.mo
index 13e4589c70..6a1fc31889 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureLowRise.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureLowRise.mo
@@ -16,19 +16,19 @@ equation
 experiment(StartTime=-2, Tolerance=1e-6, StopTime=2),
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/BaseClasses/Examples/WindPressureLowRise.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This examples demonstrates the
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise\">
- AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise</a>
- function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 27, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This examples demonstrates the
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise\">
+AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise</a>
+function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 27, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WindPressureLowRise;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureProfile.mo b/AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureProfile.mo
index 176e08ee34..0106bd6b6c 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureProfile.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/Examples/WindPressureProfile.mo
@@ -67,26 +67,26 @@ experiment(
       Tolerance=1e-06),
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/BaseClasses/Examples/WindPressureProfile.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This examples demonstrates the
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.windPressureProfile\">
- AixLib.Airflow.Multizone.BaseClasses.windPressureProfile</a>
- function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, by Klaas De Jonge:<br/>
- First implementation
- </li>
- </ul>
- </html>
- "),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This examples demonstrates the
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.windPressureProfile\">
+AixLib.Airflow.Multizone.BaseClasses.windPressureProfile</a>
+function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, by Klaas De Jonge:<br/>
+First implementation
+</li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end WindPressureProfile;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/Examples/package.order b/AixLib/Airflow/Multizone/BaseClasses/Examples/package.order
index e841c46bf2..d11030019d 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/Examples/package.order
+++ b/AixLib/Airflow/Multizone/BaseClasses/Examples/package.order
@@ -1,4 +1,3 @@
-Interpolate
 PowerLaw
 PowerLawFixedM
 WindPressureLowRise
diff --git a/AixLib/Airflow/Multizone/BaseClasses/PartialOneWayFlowElement.mo b/AixLib/Airflow/Multizone/BaseClasses/PartialOneWayFlowElement.mo
index e99337ef06..493d1f90df 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/PartialOneWayFlowElement.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/PartialOneWayFlowElement.mo
@@ -92,34 +92,34 @@ equation
 
   annotation (
     Documentation(info="<html>
- <p>
- This partial model is used to model one way flow-elements.
- It holds the conservation equations and should be extended by
- definition of <u><b>one</b></u> of the following variables:
- </p>
- <p>m_flow = mass flow rate trough the component</p>
- <p>or</p>
- <p>V_flow = volume flow rate through the component</p>
- <p>
- The flow from A-&gt;B is the positive flow.
- The resulting equation should be in the <code>extends</code> statement,
- not in the equation section since this model sets both
- <code>m_flow = V_flow*rho</code> and <code>V_flow = m_flow/rho</code>.
- </p>
- </html>",
+<p>
+This partial model is used to model one way flow-elements.
+It holds the conservation equations and should be extended by
+definition of <u><b>one</b></u> of the following variables:
+</p>
+<p>m_flow = mass flow rate trough the component</p>
+<p>or</p>
+<p>V_flow = volume flow rate through the component</p>
+<p>
+The flow from A-&gt;B is the positive flow.
+The resulting equation should be in the <code>extends</code> statement,
+not in the equation section since this model sets both
+<code>m_flow = V_flow*rho</code> and <code>V_flow = m_flow/rho</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 06, 2021, by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 06, 2021, by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialOneWayFlowElement;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/PowerLawResistanceParameters.mo b/AixLib/Airflow/Multizone/BaseClasses/PowerLawResistanceParameters.mo
index 5b30b61ad9..22625ced33 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/PowerLawResistanceParameters.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/PowerLawResistanceParameters.mo
@@ -17,17 +17,17 @@ protected
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Parameters that are required for the components that implement a power law resistance.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 26, 2021, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>
- "),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Parameters that are required for the components that implement a power law resistance.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 26, 2021, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerLawResistanceParameters;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElement.mo b/AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElement.mo
index 91c5671a0e..bb8314341a 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElement.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElement.mo
@@ -119,74 +119,74 @@ equation
           fillPattern=FillPattern.Solid,
           pattern=LinePattern.None)}),
     Documentation(info="<html>
- <p>
- This is a partial model for models that describe the bi-directional
- air flow through large openings.
- </p>
- <p>
- Models that extend this model need to compute
- <code>mAB_flow</code> and <code>mBA_flow</code>,
- or alternatively <code>VAB_flow</code> and <code>VBA_flow</code>,
- and the face area <code>area</code>.
- The face area is a variable to allow this partial model to be used
- for doors that can be open or closed as a function of an input signal.
- </p>
- </html>",
+<p>
+This is a partial model for models that describe the bi-directional
+air flow through large openings.
+</p>
+<p>
+Models that extend this model need to compute
+<code>mAB_flow</code> and <code>mBA_flow</code>,
+or alternatively <code>VAB_flow</code> and <code>VBA_flow</code>,
+and the face area <code>area</code>.
+The face area is a variable to allow this partial model to be used
+for doors that can be open or closed as a function of an input signal.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 12, 2020, by Michael Wetter:<br/>
- Changed assignment of <code>m1_flow_small</code> and
- <code>m2_flow_small</code> to <code>final</code>.
- These quantities are not used in this model and models that extend from it.
- Hence there is no need for the user to change the value.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- September 13, 2018, by Michael Wetter:<br/>
- Set <code>allowFlowReversal=true</code> as the flow can be slightly negative
- due to the regularization, in which case the <code>m_flow(min=0)</code>
- that is set in the base class
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPort\">
- AixLib.Fluid.Interfaces.PartialFourPort</a>
- is violated.<br/>
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/937\">#937</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Removed start values for inflowing density
- to simplify the parameter window, and because this can usually
- be computed from the state variables.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
- </li>
- <li>
- February 24, 2015 by Michael Wetter:<br/>
- Changed model to use
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.density_pTX\">
- Buildings.Utilities.Psychrometrics.Functions.density_pTX</a>
- for the density computation
- as
- <a href=\"modelica://AixLib.Media.Air.density\">
- Buildings.Media.Air.density</a>
- does not depend on temperature.
- </li>
- <li>June 18, 2014 by Michael Wetter:<br/>
- Added start values and <code>fixed=true</code> attribute for
- <code>mExcAB</code> and <code>mExcBA</code>.
- This avoids a warning during translation.
- </li>
- <li>July 20, 2010 by Michael Wetter:<br/>
-        Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>February 4, 2005 by Michael Wetter:<br/>
-        Released first version.
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 12, 2020, by Michael Wetter:<br/>
+Changed assignment of <code>m1_flow_small</code> and
+<code>m2_flow_small</code> to <code>final</code>.
+These quantities are not used in this model and models that extend from it.
+Hence there is no need for the user to change the value.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+September 13, 2018, by Michael Wetter:<br/>
+Set <code>allowFlowReversal=true</code> as the flow can be slightly negative
+due to the regularization, in which case the <code>m_flow(min=0)</code>
+that is set in the base class
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPort\">
+AixLib.Fluid.Interfaces.PartialFourPort</a>
+is violated.<br/>
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/937\">#937</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Removed start values for inflowing density
+to simplify the parameter window, and because this can usually
+be computed from the state variables.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
+</li>
+<li>
+February 24, 2015 by Michael Wetter:<br/>
+Changed model to use
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.density_pTX\">
+Buildings.Utilities.Psychrometrics.Functions.density_pTX</a>
+for the density computation
+as
+<a href=\"modelica://AixLib.Media.Air.density\">
+Buildings.Media.Air.density</a>
+does not depend on temperature.
+</li>
+<li>June 18, 2014 by Michael Wetter:<br/>
+Added start values and <code>fixed=true</code> attribute for
+<code>mExcAB</code> and <code>mExcBA</code>.
+This avoids a warning during translation.
+</li>
+<li>July 20, 2010 by Michael Wetter:<br/>
+       Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>February 4, 2005 by Michael Wetter:<br/>
+       Released first version.
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayFlowElement;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElementBuoyancy.mo b/AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElementBuoyancy.mo
index d33c695f50..812a07f4b5 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElementBuoyancy.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/TwoWayFlowElementBuoyancy.mo
@@ -14,33 +14,33 @@ partial model TwoWayFlowElementBuoyancy
     "Height of reference pressure zone B" annotation (Dialog(group="Geometry"));
 
   annotation (Documentation(info="<html>
- <p>
- This is a partial model for models that describe the bi-directional
- air flow through large openings.
- </p>
- <p>
- Models that extend this model need to compute
- <code>mAB_flow</code> and <code>mBA_flow</code>,
- or alternatively <code>VAB_flow</code> and <code>VBA_flow</code>,
- and the face area <code>area</code>.
- The face area is a variable to allow this partial model to be used
- for doors that can be open or closed as a function of an input signal.
- </p>
- </html>",
+<p>
+This is a partial model for models that describe the bi-directional
+air flow through large openings.
+</p>
+<p>
+Models that extend this model need to compute
+<code>mAB_flow</code> and <code>mBA_flow</code>,
+or alternatively <code>VAB_flow</code> and <code>VBA_flow</code>,
+and the face area <code>area</code>.
+The face area is a variable to allow this partial model to be used
+for doors that can be open or closed as a function of an input signal.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 27, 2018, by Michael Wetter:<br/>
- Corrected old parameter annotation.
- </li>
- <li>
- July 20, 2010 by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>
- February 4, 2005 by Michael Wetter:<br/>
- Released first version.
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 27, 2018, by Michael Wetter:<br/>
+Corrected old parameter annotation.
+</li>
+<li>
+July 20, 2010 by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>
+February 4, 2005 by Michael Wetter:<br/>
+Released first version.
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayFlowElementBuoyancy;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/ZonalFlow.mo b/AixLib/Airflow/Multizone/BaseClasses/ZonalFlow.mo
index c6ac6cd98f..2027d91aff 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/ZonalFlow.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/ZonalFlow.mo
@@ -64,39 +64,39 @@ equation
           origin={-79,-63},
           rotation=360)}),
     Documentation(info="<html>
- <p>
- This is a partial model for computing the air exchange between volumes.
- Models that extend this model need to provide an equation for
- <code>port_a1.m_flow</code> and <code>port_a2.m_flow</code>.
- </p>
- </html>",
+<p>
+This is a partial model for computing the air exchange between volumes.
+Models that extend this model need to provide an equation for
+<code>port_a1.m_flow</code> and <code>port_a2.m_flow</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 12, 2020, by Michael Wetter:<br/>
- Changed assignment of <code>m1_flow_small</code> and
- <code>m2_flow_small</code> to <code>final</code>.
- These quantities are not used in this model and models that extend from it.
- Hence there is no need for the user to change the value.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- August 18, 2014, by Michael Wetter:<br/>
- Removed parameter <code>forceErrorControlOnFlow</code> as it was not used.
- </li>
- <li>
- July 20, 2010 by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>
- January 4, 2006, by Michael Wetter:<br/>
- Implemented first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 12, 2020, by Michael Wetter:<br/>
+Changed assignment of <code>m1_flow_small</code> and
+<code>m2_flow_small</code> to <code>final</code>.
+These quantities are not used in this model and models that extend from it.
+Hence there is no need for the user to change the value.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+August 18, 2014, by Michael Wetter:<br/>
+Removed parameter <code>forceErrorControlOnFlow</code> as it was not used.
+</li>
+<li>
+July 20, 2010 by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>
+January 4, 2006, by Michael Wetter:<br/>
+Implemented first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ZonalFlow;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/package.order b/AixLib/Airflow/Multizone/BaseClasses/package.order
index 698bba52a4..ab4a1d1fef 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/package.order
+++ b/AixLib/Airflow/Multizone/BaseClasses/package.order
@@ -6,7 +6,6 @@ PowerLawResistanceParameters
 TwoWayFlowElement
 TwoWayFlowElementBuoyancy
 ZonalFlow
-interpolate
 powerLaw
 powerLawFixedM
 windPressureLowRise
diff --git a/AixLib/Airflow/Multizone/BaseClasses/powerLaw.mo b/AixLib/Airflow/Multizone/BaseClasses/powerLaw.mo
index dde6ce74a6..914b8e9983 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/powerLaw.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/powerLaw.mo
@@ -41,69 +41,69 @@ algorithm
 
   annotation (smoothOrder=2,
 Documentation(info="<html>
- <p>
- This model describes the mass flow rate and pressure difference relation
- of an orifice in the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   V&#775; = C sign(&Delta;p) |&Delta;p|<sup>m</sup>
- </p>
- <p>
- where
- <i>V&#775;</i> is the volume flow rate,
- <i>C &gt; 0</i> is a flow coefficient
- <i>&Delta; p</i> is the pressure drop and
- <i>m &isin; [0.5, 1]</i> is a flow coefficient.
- The equation is regularized for
- <i>|&Delta;p| &lt; &Delta;p<sub>t</sub></i>, where
- <i>&Delta;p<sub>t</sub></i> is a parameter.
- For turbulent flow, set <i>m=1 &frasl; 2</i> and
- for laminar flow, set <i>m=1</i>.
- </p>
- <p>
- The model is used for the interzonal air flow models.
- </p>
- <h4>Implementation</h4>
- <p>
- For <i>|&Delta;p| &lt; &Delta;p<sub>t</sub></i>, the equation is regularized
- so that it is twice continuously differentiable in <i>&Delta;p</i>, and that it
- has an infinite number of continuous derivatives in <i>m</i> and in <i>k</i>.
- </p>
- <p>
- If <i>m</i> is not a function of time, then
- <i>a</i>, <i>b</i>, <i>c</i> and <i>d</i> can be pre-computed.
- In this situation, use
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
- AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM</a>, which allows
- to compute these values outside of this function, for example as parameters
- of a model.
- </p>
- </html>",
+<p>
+This model describes the mass flow rate and pressure difference relation
+of an orifice in the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  V&#775; = C sign(&Delta;p) |&Delta;p|<sup>m</sup>
+</p>
+<p>
+where
+<i>V&#775;</i> is the volume flow rate,
+<i>C &gt; 0</i> is a flow coefficient
+<i>&Delta; p</i> is the pressure drop and
+<i>m &isin; [0.5, 1]</i> is a flow coefficient.
+The equation is regularized for
+<i>|&Delta;p| &lt; &Delta;p<sub>t</sub></i>, where
+<i>&Delta;p<sub>t</sub></i> is a parameter.
+For turbulent flow, set <i>m=1 &frasl; 2</i> and
+for laminar flow, set <i>m=1</i>.
+</p>
+<p>
+The model is used for the interzonal air flow models.
+</p>
+<h4>Implementation</h4>
+<p>
+For <i>|&Delta;p| &lt; &Delta;p<sub>t</sub></i>, the equation is regularized
+so that it is twice continuously differentiable in <i>&Delta;p</i>, and that it
+has an infinite number of continuous derivatives in <i>m</i> and in <i>k</i>.
+</p>
+<p>
+If <i>m</i> is not a function of time, then
+<i>a</i>, <i>b</i>, <i>c</i> and <i>d</i> can be pre-computed.
+In this situation, use
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
+AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM</a>, which allows
+to compute these values outside of this function, for example as parameters
+of a model.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 8, 2022, by Michael Wetter:<br/>
- Changed to use <code>C</code> for volume flow coefficient (<i>C = V_flow/dp^m</i>),
- and <code>k</code> for mass flow coefficient (<i>k = m_flow/dp^m</i>).
- This is for consistency with
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels\">AixLib.Fluid.BaseClasses.FlowModels</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- <i>August 12, 2011</i> by Michael Wetter:<br/>
- Reimplemented model so that it is continuously differentiable.
- </li>
- <li><i>July 20, 2010</i> by Michael Wetter:<br/>
-        Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li><i>February 4, 2005</i> by Michael Wetter:<br/>
-        Released first version.
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 8, 2022, by Michael Wetter:<br/>
+Changed to use <code>C</code> for volume flow coefficient (<i>C = V_flow/dp^m</i>),
+and <code>k</code> for mass flow coefficient (<i>k = m_flow/dp^m</i>).
+This is for consistency with
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels\">AixLib.Fluid.BaseClasses.FlowModels</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+<i>August 12, 2011</i> by Michael Wetter:<br/>
+Reimplemented model so that it is continuously differentiable.
+</li>
+<li><i>July 20, 2010</i> by Michael Wetter:<br/>
+       Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li><i>February 4, 2005</i> by Michael Wetter:<br/>
+       Released first version.
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end powerLaw;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/powerLawFixedM.mo b/AixLib/Airflow/Multizone/BaseClasses/powerLawFixedM.mo
index ed39f7aa36..d6a1f7106b 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/powerLawFixedM.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/powerLawFixedM.mo
@@ -33,79 +33,79 @@ algorithm
 
   annotation (smoothOrder=2,
 Documentation(info="<html>
- <p>
- This model describes the mass flow rate and pressure difference relation
- of an orifice in the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   V&#775; = C sign(&Delta;p) |&Delta;p|<sup>m</sup>
- </p>
- <p>
- where
- <i>V&#775;</i> is the volume flow rate,
- <i>C &gt; 0</i> is a flow coefficient
- <i>&Delta; p</i> is the pressure drop and
- <i>m &isin; [0.5, 1]</i> is a flow coefficient.
- The equation is regularized for
- <i>|&Delta;p| &lt; &Delta;p<sub>t</sub></i>, where
- <i>&Delta;p<sub>t</sub></i> is a parameter.
- For turbulent flow, set <i>m=1 &frasl; 2</i> and
- for laminar flow, set <i>m=1</i>.
- </p>
- <p>
- The model is used for the interzonal air flow models.
- It is identical to
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLaw\">
- AixLib.Airflow.Multizone.BaseClasses.powerLaw</a> but it
- requires the polynomial coefficients as an input.
- This allows a more efficient simulation if <i>m</i> and therefore also
- <i>a</i>, <i>b</i>, <i>c</i> and <i>d</i> are constant.
- </p>
- <h4>Implementation</h4>
- <p>
- For <i>|&Delta;p| &lt; &Delta;p<sub>t</sub></i>, the equation is regularized
- so that it is twice continuously differentiable in <i>&Delta;p</i>, and that it
- has an infinite number of continuous derivatives in <i>m</i> and in <i>k</i>.
- </p>
- <p>
- If <i>m</i>, and therefore also
- <i>a</i>, <i>b</i>, <i>c</i> and <i>d</i>, change with time, then
- it is more convenient and efficient to use
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLaw\">
- AixLib.Airflow.Multizone.BaseClasses.powerLaw</a>.
- </p>
- </html>",
+<p>
+This model describes the mass flow rate and pressure difference relation
+of an orifice in the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  V&#775; = C sign(&Delta;p) |&Delta;p|<sup>m</sup>
+</p>
+<p>
+where
+<i>V&#775;</i> is the volume flow rate,
+<i>C &gt; 0</i> is a flow coefficient
+<i>&Delta; p</i> is the pressure drop and
+<i>m &isin; [0.5, 1]</i> is a flow coefficient.
+The equation is regularized for
+<i>|&Delta;p| &lt; &Delta;p<sub>t</sub></i>, where
+<i>&Delta;p<sub>t</sub></i> is a parameter.
+For turbulent flow, set <i>m=1 &frasl; 2</i> and
+for laminar flow, set <i>m=1</i>.
+</p>
+<p>
+The model is used for the interzonal air flow models.
+It is identical to
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLaw\">
+AixLib.Airflow.Multizone.BaseClasses.powerLaw</a> but it
+requires the polynomial coefficients as an input.
+This allows a more efficient simulation if <i>m</i> and therefore also
+<i>a</i>, <i>b</i>, <i>c</i> and <i>d</i> are constant.
+</p>
+<h4>Implementation</h4>
+<p>
+For <i>|&Delta;p| &lt; &Delta;p<sub>t</sub></i>, the equation is regularized
+so that it is twice continuously differentiable in <i>&Delta;p</i>, and that it
+has an infinite number of continuous derivatives in <i>m</i> and in <i>k</i>.
+</p>
+<p>
+If <i>m</i>, and therefore also
+<i>a</i>, <i>b</i>, <i>c</i> and <i>d</i>, change with time, then
+it is more convenient and efficient to use
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLaw\">
+AixLib.Airflow.Multizone.BaseClasses.powerLaw</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 8, 2022, by Michael Wetter:<br/>
- Changed to use <code>C</code> for volume flow coefficient (<i>C = V_flow/dp^m</i>),
- and <code>k</code> for mass flow coefficient (<i>k = m_flow/dp^m</i>).
- This is for consistency with
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels\">AixLib.Fluid.BaseClasses.FlowModels</a>.
- </li>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- April 6, 2021, by Klaas De Jonge:<br/>
- Generalised the function by removing the units for flow.
- This is done because the function is used to compute both mass flow rates and volume flow rates.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- <i>August 12, 2011</i> by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 8, 2022, by Michael Wetter:<br/>
+Changed to use <code>C</code> for volume flow coefficient (<i>C = V_flow/dp^m</i>),
+and <code>k</code> for mass flow coefficient (<i>k = m_flow/dp^m</i>).
+This is for consistency with
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels\">AixLib.Fluid.BaseClasses.FlowModels</a>.
+</li>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+April 6, 2021, by Klaas De Jonge:<br/>
+Generalised the function by removing the units for flow.
+This is done because the function is used to compute both mass flow rates and volume flow rates.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+<i>August 12, 2011</i> by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end powerLawFixedM;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/windPressureLowRise.mo b/AixLib/Airflow/Multizone/BaseClasses/windPressureLowRise.mo
index 6aab5b5ebf..513433511e 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/windPressureLowRise.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/windPressureLowRise.mo
@@ -68,115 +68,115 @@ algorithm
 annotation (
 smoothOrder=1,
 Documentation(info="<html>
- <p>
- This function computes the wind pressure coefficient for
- low-rise buildings with rectangular shape.
- The correlation is the data fit from Swami and Chandra (1987),
- who fitted a function to various wind pressure coefficients from the literature.
- The same correlation is also implemented in CONTAM (Persily and Ivy, 2001).
- </p>
- <p>
- The wind pressure coefficient is computed based on the
- natural logarithm of the side ratio of the walls, which is defined as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- G = ln(x &frasl; y)
- </p>
- <p>
- where <i>x</i> is the length of the wall that will be connected to
- this model, and <i>y</i> is the length of the adjacent wall as shown
- in the figure below.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Airflow/Multizone/BaseClasses/windPressureLowRise.png\" border=\"1\" alt=\"Definition of the aspect ratio.\"/>
- </p>
- <p>
- Based on the wind incidence angle <i>&alpha;</i> and the side ratio
- of the walls, the model computes how much the wind pressure
- is attenuated compared to the reference wind pressure <code>Cp0</code>.
- The reference wind pressure <code>Cp0</code> is a user-defined parameter,
- and must be equal to the wind pressure at zero wind incidence angle, i.e.,
- <i>&alpha; = 0</i>.
- Swami and Chandra (1987) recommend <i>C<sub>p0</sub> = 0.6</i> for
- all low-rise buildings as this represents the average of
- various values reported in the literature.
- The attenuation factor is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- C<sub>p</sub> &frasl; C<sub>p0</sub> = ln(1.248 - 0.703 sin(&alpha; &frasl; 2)
-       - 1.175 sin<sup>2</sup>(&alpha;)
-       - 0.131 sin<sup>3</sup>(2 &alpha; G)
-       + 0.769 cos(&alpha; &frasl; 2)
-        +0.071 G<sup>2</sup> * sin<sup>2</sup>(&alpha; &frasl; 2)
-        + 0.717 cos<sup>2</sup>(&alpha; &frasl; 2)),
- </p>
- <p>
- where
- <i>C<sub>p</sub></i> is the wind pressure coefficient for
- the current angle of incidence.
- </p>
- <p>
- This function is used in
- <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpLowRise\">
- Buildings.Fluid.Sources.Outside_CpLowRise</a>
- which can be used directly with components of this package.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Muthusamy V. Swami and
- Subrato Chandra.
- <i>
- <a href=\"http://www.fsec.ucf.edu/en/publications/pdf/FSEC-CR-163-86.pdf\">
- Procedures for
- Calculating Natural
- Ventilation Airflow
- Rates in Buildings.</a></i>
- Florida Solar Energy Center, FSEC-CR-163-86. March, 1987.
- Cape Canaveral, Florida.
- </li>
- <li>
- Andrew K. Persily and Elizabeth M. Ivy.
- <i>
- <a href=\"http://ws680.nist.gov/publication/get_pdf.cfm?pub_id=860831\">
- Input Data for Multizone Airflow and IAQ Analysis.</a></i>
- NIST, NISTIR 6585.
- January, 2001.
- Gaithersburg, MD.
- </li>
- </ul>
- <h4>Implementation</h4>
- <p>
- Symmetry requires that the first derivative of the wind pressure coefficient
- with respect to the incidence angle is zero for incidence angles of zero and &pi;.
- However, the correlation of Swami and Chandra has non-zero derivatives at these values.
- In this implementation, the original function is therefore slightly modified for incidence angles
- between 0 and 5 degree, and between 175 and 180 degree.
- This leads to a model that is differentiable in the incidence angle,
- which generally leads to better numeric performance.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 16, 2022, by Michael Wetter:<br/>
- Changed argment name to <code>alpha</code> for consistency with figure.
- </li>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Removed <code>constant</code> keyword for <code>a180</code> as its value
- depends on the input of the function.
- </li>
- <li>
- October 27, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function computes the wind pressure coefficient for
+low-rise buildings with rectangular shape.
+The correlation is the data fit from Swami and Chandra (1987),
+who fitted a function to various wind pressure coefficients from the literature.
+The same correlation is also implemented in CONTAM (Persily and Ivy, 2001).
+</p>
+<p>
+The wind pressure coefficient is computed based on the
+natural logarithm of the side ratio of the walls, which is defined as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+G = ln(x &frasl; y)
+</p>
+<p>
+where <i>x</i> is the length of the wall that will be connected to
+this model, and <i>y</i> is the length of the adjacent wall as shown
+in the figure below.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Airflow/Multizone/BaseClasses/windPressureLowRise.png\" border=\"1\" alt=\"Definition of the aspect ratio.\"/>
+</p>
+<p>
+Based on the wind incidence angle <i>&alpha;</i> and the side ratio
+of the walls, the model computes how much the wind pressure
+is attenuated compared to the reference wind pressure <code>Cp0</code>.
+The reference wind pressure <code>Cp0</code> is a user-defined parameter,
+and must be equal to the wind pressure at zero wind incidence angle, i.e.,
+<i>&alpha; = 0</i>.
+Swami and Chandra (1987) recommend <i>C<sub>p0</sub> = 0.6</i> for
+all low-rise buildings as this represents the average of
+various values reported in the literature.
+The attenuation factor is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+C<sub>p</sub> &frasl; C<sub>p0</sub> = ln(1.248 - 0.703 sin(&alpha; &frasl; 2)
+      - 1.175 sin<sup>2</sup>(&alpha;)
+      - 0.131 sin<sup>3</sup>(2 &alpha; G)
+      + 0.769 cos(&alpha; &frasl; 2)
+       +0.071 G<sup>2</sup> * sin<sup>2</sup>(&alpha; &frasl; 2)
+       + 0.717 cos<sup>2</sup>(&alpha; &frasl; 2)),
+</p>
+<p>
+where
+<i>C<sub>p</sub></i> is the wind pressure coefficient for
+the current angle of incidence.
+</p>
+<p>
+This function is used in
+<a href=\"modelica://AixLib.Fluid.Sources.Outside_CpLowRise\">
+Buildings.Fluid.Sources.Outside_CpLowRise</a>
+which can be used directly with components of this package.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Muthusamy V. Swami and
+Subrato Chandra.
+<i>
+<a href=\"http://www.fsec.ucf.edu/en/publications/pdf/FSEC-CR-163-86.pdf\">
+Procedures for
+Calculating Natural
+Ventilation Airflow
+Rates in Buildings.</a></i>
+Florida Solar Energy Center, FSEC-CR-163-86. March, 1987.
+Cape Canaveral, Florida.
+</li>
+<li>
+Andrew K. Persily and Elizabeth M. Ivy.
+<i>
+<a href=\"http://ws680.nist.gov/publication/get_pdf.cfm?pub_id=860831\">
+Input Data for Multizone Airflow and IAQ Analysis.</a></i>
+NIST, NISTIR 6585.
+January, 2001.
+Gaithersburg, MD.
+</li>
+</ul>
+<h4>Implementation</h4>
+<p>
+Symmetry requires that the first derivative of the wind pressure coefficient
+with respect to the incidence angle is zero for incidence angles of zero and &pi;.
+However, the correlation of Swami and Chandra has non-zero derivatives at these values.
+In this implementation, the original function is therefore slightly modified for incidence angles
+between 0 and 5 degree, and between 175 and 180 degree.
+This leads to a model that is differentiable in the incidence angle,
+which generally leads to better numeric performance.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 16, 2022, by Michael Wetter:<br/>
+Changed argment name to <code>alpha</code> for consistency with figure.
+</li>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Removed <code>constant</code> keyword for <code>a180</code> as its value
+depends on the input of the function.
+</li>
+<li>
+October 27, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end windPressureLowRise;
diff --git a/AixLib/Airflow/Multizone/BaseClasses/windPressureProfile.mo b/AixLib/Airflow/Multizone/BaseClasses/windPressureProfile.mo
index 4047ee0f2d..c4221eb94e 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/windPressureProfile.mo
+++ b/AixLib/Airflow/Multizone/BaseClasses/windPressureProfile.mo
@@ -38,53 +38,53 @@ algorithm
   annotation (
 smoothOrder=1,
 Documentation(revisions="<html>
- <ul>
- <li>
- February 16, 2022, by Michael Wetter:<br/>
- Changed argment name to <code>alpha</code> for consistency with figure in
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise\">
- AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise</a>.
- </li>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- April 6, 2021, by Klaas De Jonge:<br/>
- First implementation
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+February 16, 2022, by Michael Wetter:<br/>
+Changed argment name to <code>alpha</code> for consistency with figure in
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise\">
+AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise</a>.
+</li>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+April 6, 2021, by Klaas De Jonge:<br/>
+First implementation
+</li>
+</ul>
+</html>",
 info="<html>
- <p>
- This function computes the wind pressure coefficients <i>C<sub>p</sub></i> from a user-defined table data.
- The same functionality is also implemented in CONTAM.
- </p>
- <p>
- This function is used in
- <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">
- AixLib.Fluid.Sources.Outside_CpData</a>.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- <b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
- National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
- </li>
- <li>
- <b>Andrew K. Persily and Elizabeth M. Ivy.</b>
- <i>
- <a href=\"http://ws680.nist.gov/publication/get_pdf.cfm?pub_id=860831\">
- Input Data for Multizone Airflow and IAQ Analysis.</a></i>
- NIST, NISTIR 6585.
- January, 2001.
- Gaithersburg, MD.
- </li>
- <li><b>M. W. Liddament, 1996</b>, <i>A guide to energy efficient ventilation</i>. AIVC Annex V. </li>
- </ul>
- 
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function computes the wind pressure coefficients <i>C<sub>p</sub></i> from a user-defined table data.
+The same functionality is also implemented in CONTAM.
+</p>
+<p>
+This function is used in
+<a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">
+AixLib.Fluid.Sources.Outside_CpData</a>.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+<b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
+National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
+</li>
+<li>
+<b>Andrew K. Persily and Elizabeth M. Ivy.</b>
+<i>
+<a href=\"http://ws680.nist.gov/publication/get_pdf.cfm?pub_id=860831\">
+Input Data for Multizone Airflow and IAQ Analysis.</a></i>
+NIST, NISTIR 6585.
+January, 2001.
+Gaithersburg, MD.
+</li>
+<li><b>M. W. Liddament, 1996</b>, <i>A guide to energy efficient ventilation</i>. AIVC Annex V. </li>
+</ul>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end windPressureProfile;
diff --git a/AixLib/Airflow/Multizone/Coefficient_V_flow.mo b/AixLib/Airflow/Multizone/Coefficient_V_flow.mo
index 891455a34a..f5a1fa49a4 100644
--- a/AixLib/Airflow/Multizone/Coefficient_V_flow.mo
+++ b/AixLib/Airflow/Multizone/Coefficient_V_flow.mo
@@ -58,41 +58,41 @@ model Coefficient_V_flow "Power law with coefficient for volume flow rate"
           fillPattern=FillPattern.Solid)}),
     defaultComponentName="pow",
     Documentation(info="<html>
- <p>
- This model describes the one-directional pressure driven air flow through an opening, using the equation
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- V&#775; = C &Delta;p<sup>m</sup>,
- </p>
- <p>
- where <i>V&#775;</i> is the volume flow rate in m<sup>3</sup>/s,
- <i>C</i> is a flow coefficient,
- <i>&Delta;p</i> is the pressure difference in Pa,
- and <i>m</i> is the flow exponent.
- </p>
- <p>
- A similar model is also used in the CONTAM software (Dols and Walton, 2015).
- Dols and Walton (2002) recommend to use for the flow exponent m=0.6 to m=0.7 if the flow exponent is not reported with the test results.
- </p>
- <h4>References</h4>
- <ul>
- <li><b>ASHRAE, 1997.</b> <i>ASHRAE Fundamentals</i>, American Society of Heating, Refrigeration and Air-Conditioning Engineers, 1997. </li>
- <li><b>Dols and Walton, 2002.</b> W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual, Multizone Airflow and Contaminant Transport Analysis Software</i>, Building and Fire Research Laboratory, National Institute of Standards and Technology, Tech. Report NISTIR 6921, November, 2002. </li>
- <li><b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>, National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>. </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, by Klaas De Jonge:<br/>
- First Implementation. Model expecting direct input of volume flow powerlaw coefficients.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model describes the one-directional pressure driven air flow through an opening, using the equation
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+V&#775; = C &Delta;p<sup>m</sup>,
+</p>
+<p>
+where <i>V&#775;</i> is the volume flow rate in m<sup>3</sup>/s,
+<i>C</i> is a flow coefficient,
+<i>&Delta;p</i> is the pressure difference in Pa,
+and <i>m</i> is the flow exponent.
+</p>
+<p>
+A similar model is also used in the CONTAM software (Dols and Walton, 2015).
+Dols and Walton (2002) recommend to use for the flow exponent m=0.6 to m=0.7 if the flow exponent is not reported with the test results.
+</p>
+<h4>References</h4>
+<ul>
+<li><b>ASHRAE, 1997.</b> <i>ASHRAE Fundamentals</i>, American Society of Heating, Refrigeration and Air-Conditioning Engineers, 1997. </li>
+<li><b>Dols and Walton, 2002.</b> W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual, Multizone Airflow and Contaminant Transport Analysis Software</i>, Building and Fire Research Laboratory, National Institute of Standards and Technology, Tech. Report NISTIR 6921, November, 2002. </li>
+<li><b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>, National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>. </li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, by Klaas De Jonge:<br/>
+First Implementation. Model expecting direct input of volume flow powerlaw coefficients.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Coefficient_V_flow;
diff --git a/AixLib/Airflow/Multizone/Coefficient_m_flow.mo b/AixLib/Airflow/Multizone/Coefficient_m_flow.mo
index 7aed539c8e..4e82bb7f17 100644
--- a/AixLib/Airflow/Multizone/Coefficient_m_flow.mo
+++ b/AixLib/Airflow/Multizone/Coefficient_m_flow.mo
@@ -58,40 +58,40 @@ protected
           fillPattern=FillPattern.Solid)}),
     defaultComponentName="pow",
     Documentation(info="<html>
- <p>
- This model describes the one-directional pressure driven air flow through an opening, using the equation
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- m&#775; = k &Delta;p<sup>m</sup>,
- </p>
- <p>
- where <i>m&#775;</i> is the mass flow rate in kg/s,
- <i>k</i> is a flow coefficient,
- <i>&Delta;p</i> is the pressure difference in Pa,
- and <i>m</i> is the flow exponent.
- </p>
- <p><br>A similar model is also used in the CONTAM software (Dols and Walton, 2015).
- Dols and Walton (2002) recommend to use for the flow exponent <i>m=0.6</i> to <i>m=0.7</i> if the flow exponent is not reported with the test results.
- </p>
- <h4>References</h4>
- <ul>
- <li><b>ASHRAE, 1997.</b> <i>ASHRAE Fundamentals</i>, American Society of Heating, Refrigeration and Air-Conditioning Engineers, 1997. </li>
- <li><b>Dols and Walton, 2002.</b> W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual, Multizone Airflow and Contaminant Transport Analysis Software</i>, Building and Fire Research Laboratory, National Institute of Standards and Technology, Tech. Report NISTIR 6921, November, 2002. [1]</li>
- <li><b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>, National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>. </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, by Klaas De Jonge:<br/>
- First Implementation. Model expecting direct input of mass flow powerlaw coefficients.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model describes the one-directional pressure driven air flow through an opening, using the equation
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+m&#775; = k &Delta;p<sup>m</sup>,
+</p>
+<p>
+where <i>m&#775;</i> is the mass flow rate in kg/s,
+<i>k</i> is a flow coefficient,
+<i>&Delta;p</i> is the pressure difference in Pa,
+and <i>m</i> is the flow exponent.
+</p>
+<p><br>A similar model is also used in the CONTAM software (Dols and Walton, 2015).
+Dols and Walton (2002) recommend to use for the flow exponent <i>m=0.6</i> to <i>m=0.7</i> if the flow exponent is not reported with the test results.
+</p>
+<h4>References</h4>
+<ul>
+<li><b>ASHRAE, 1997.</b> <i>ASHRAE Fundamentals</i>, American Society of Heating, Refrigeration and Air-Conditioning Engineers, 1997. </li>
+<li><b>Dols and Walton, 2002.</b> W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual, Multizone Airflow and Contaminant Transport Analysis Software</i>, Building and Fire Research Laboratory, National Institute of Standards and Technology, Tech. Report NISTIR 6921, November, 2002. [1]</li>
+<li><b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>, National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>. </li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, by Klaas De Jonge:<br/>
+First Implementation. Model expecting direct input of mass flow powerlaw coefficients.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Coefficient_m_flow;
diff --git a/AixLib/Airflow/Multizone/DoorDiscretizedOpen.mo b/AixLib/Airflow/Multizone/DoorDiscretizedOpen.mo
index a192ce09a5..24ddb1da77 100644
--- a/AixLib/Airflow/Multizone/DoorDiscretizedOpen.mo
+++ b/AixLib/Airflow/Multizone/DoorDiscretizedOpen.mo
@@ -37,58 +37,58 @@ equation
 
   annotation (defaultComponentName="doo",
 Documentation(info="<html>
- <p>
- This model describes the bi-directional air flow through an open door.
- </p>
- <p>
- To compute the bi-directional flow,
- the door is discretize along the height coordinate.
- An orifice equation is used to compute the flow for each compartment.
- </p>
- <p>
- In this model, the door is always open.
- Use the model
- <a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOperable\">
- Buildings.Airflow.Multizone.DoorDiscretizedOperable</a>
- for a door that can either be open or closed.
- </p>
- </html>",
+<p>
+This model describes the bi-directional air flow through an open door.
+</p>
+<p>
+To compute the bi-directional flow,
+the door is discretize along the height coordinate.
+An orifice equation is used to compute the flow for each compartment.
+</p>
+<p>
+In this model, the door is always open.
+Use the model
+<a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOperable\">
+Buildings.Airflow.Multizone.DoorDiscretizedOperable</a>
+for a door that can either be open or closed.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 8, 2019, by Michael Wetter:<br/>
- Moved parameter <code>CD</code> from
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized\">
- AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized</a>
- to
- <a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOpen\">
- AixLib.Airflow.Multizone.DoorDiscretizedOpen</a>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/971\">#971</a>.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>December 6, 2011 by Michael Wetter:<br/>
- Changed the computation of the discharge coefficient to use the
- nominal density instead of the actual density.
- Computing <code>sqrt(2/rho)</code> sometimes causes warnings from the solver,
- as it seems to try negative values for the density during iterative solutions.
- </li>
- <li>August 12, 2011 by Michael Wetter:<br/>
- Changed model to use the new function
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
- Buildings.Airflow.Multizone.BaseClasses.powerLawFixedM</a>.
- </li>
- <li>July 20, 2010 by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>
- February 10, 2005 by Michael Wetter:<br/>
- Released first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 8, 2019, by Michael Wetter:<br/>
+Moved parameter <code>CD</code> from
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized\">
+AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized</a>
+to
+<a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOpen\">
+AixLib.Airflow.Multizone.DoorDiscretizedOpen</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/971\">#971</a>.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>December 6, 2011 by Michael Wetter:<br/>
+Changed the computation of the discharge coefficient to use the
+nominal density instead of the actual density.
+Computing <code>sqrt(2/rho)</code> sometimes causes warnings from the solver,
+as it seems to try negative values for the density during iterative solutions.
+</li>
+<li>August 12, 2011 by Michael Wetter:<br/>
+Changed model to use the new function
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
+Buildings.Airflow.Multizone.BaseClasses.powerLawFixedM</a>.
+</li>
+<li>July 20, 2010 by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>
+February 10, 2005 by Michael Wetter:<br/>
+Released first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DoorDiscretizedOpen;
diff --git a/AixLib/Airflow/Multizone/DoorDiscretizedOperable.mo b/AixLib/Airflow/Multizone/DoorDiscretizedOperable.mo
index b2d3faf2b3..3e067b291b 100644
--- a/AixLib/Airflow/Multizone/DoorDiscretizedOperable.mo
+++ b/AixLib/Airflow/Multizone/DoorDiscretizedOperable.mo
@@ -85,68 +85,68 @@ equation
           fillPattern=FillPattern.Solid)}),
 defaultComponentName="doo",
 Documentation(info="<html>
- <p>
- This model describes the bi-directional air flow through an open door.
- </p>
- <p>
- To compute the bi-directional flow,
- the door is discretize along the height coordinate, and uses
- an orifice equation to compute the flow for each compartment.
- </p>
- <p>
- The door can be either open or closed, depending on the input signal
- <i>y</i>.
- Set <i>y=0</i> if the door is closed, and <i>y=1</i>
- if the door is open.
- Use the model
- <a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOpen\">
- AixLib.Airflow.Multizone.DoorDiscretizedOpen</a>
- for a door that is always closed.
- </p>
- </html>",
+<p>
+This model describes the bi-directional air flow through an open door.
+</p>
+<p>
+To compute the bi-directional flow,
+the door is discretize along the height coordinate, and uses
+an orifice equation to compute the flow for each compartment.
+</p>
+<p>
+The door can be either open or closed, depending on the input signal
+<i>y</i>.
+Set <i>y=0</i> if the door is closed, and <i>y=1</i>
+if the door is open.
+Use the model
+<a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOpen\">
+AixLib.Airflow.Multizone.DoorDiscretizedOpen</a>
+for a door that is always closed.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 27, 2018, by Michael Wetter:<br/>
- Corrected old parameter annotation.
- </li>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>
- December 6, 2011 by Michael Wetter:<br/>
- Changed the computation of the discharge coefficient to use the
- nominal density instead of the actual density.
- Computing <code>sqrt(2/rho)</code> sometimes causes warnings from the solver,
- as it seems to try negative values for the density during iterative solutions.
- </li>
- <li>
- August 12, 2011 by Michael Wetter:<br/>
- Changed model to use the new function
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
- Buildings.Airflow.Multizone.BaseClasses.powerLawFixedM</a>.
- </li>
- <li>
- July 20, 2010 by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>
- February 10, 2005 by Michael Wetter:<br/>
- Released first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 27, 2018, by Michael Wetter:<br/>
+Corrected old parameter annotation.
+</li>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>
+December 6, 2011 by Michael Wetter:<br/>
+Changed the computation of the discharge coefficient to use the
+nominal density instead of the actual density.
+Computing <code>sqrt(2/rho)</code> sometimes causes warnings from the solver,
+as it seems to try negative values for the density during iterative solutions.
+</li>
+<li>
+August 12, 2011 by Michael Wetter:<br/>
+Changed model to use the new function
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM\">
+Buildings.Airflow.Multizone.BaseClasses.powerLawFixedM</a>.
+</li>
+<li>
+July 20, 2010 by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>
+February 10, 2005 by Michael Wetter:<br/>
+Released first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DoorDiscretizedOperable;
diff --git a/AixLib/Airflow/Multizone/DoorOpen.mo b/AixLib/Airflow/Multizone/DoorOpen.mo
index 7552f662fe..f0338d6742 100644
--- a/AixLib/Airflow/Multizone/DoorOpen.mo
+++ b/AixLib/Airflow/Multizone/DoorOpen.mo
@@ -57,157 +57,157 @@ equation
 
   annotation (defaultComponentName="doo",
 Documentation(info="<html>
- <p>
- Model for bi-directional air flow through a large opening such as a door.
- </p>
- <p>
- In this model, the air flow is composed of two components,
- a one-directional bulk air flow
- due to static pressure difference in the adjoining two thermal zones, and
- a two-directional airflow due to temperature-induced differences in density
- of the air in the two thermal zones.
- Although turbulent air flow is a nonlinear phenomenon,
- the model is based on the simplifying assumption that these two
- air flow rates can be superposed.
- (Superposition is only exact for laminar flow.)
- This assumption is made because
- it leads to a simple model and because there is significant uncertainty
- and assumptions anyway in such simplified a model for bidirectional flow through a door.
- </p>
- <h4>Main equations</h4>
- <p>
- The air flow rate due to static pressure difference is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-     V&#775;<sub>ab,p</sub> =  C<sub>D</sub> w h (2/&rho;<sub>0</sub>)<sup>0.5</sup>  &Delta;p<sup>m</sup>,
- </p>
- <p>
- where
- <i>V&#775;</i> is the volumetric air flow rate,
- <i>C<sub>D</sub></i> is the discharge coefficient,
- <i>w</i> and <i>h</i> are the width and height of the opening,
- <i>&rho;<sub>0</sub></i> is the mass density at the medium default pressure, temperature and humidity,
- <i>m</i> is the flow exponent and
- <i>&Delta;p = p<sub>a</sub> - p<sub>b</sub></i> is the static pressure difference between
- the thermal zones.
- For this model explanation, we will assume <i>p<sub>a</sub> &gt; p<sub>b</sub></i>.
- For turbulent flow, <i>m=1/2</i> and for laminar flow <i>m=1</i>.
- </p>
- <p>
- The air flow rate due to temperature difference in the thermal zones is
- <i>V&#775;<sub>ab,t</sub></i> for flow from thermal zone <i>a</i> to <i>b</i>,
- and
- <i>V&#775;<sub>ba,t</sub></i> for air flow rate from thermal zone <i>b</i> to <i>a</i>.
- The model has two air flow paths to allow bi-directional air flow.
- The mass flow rates at these two air flow paths are
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-     m&#775;<sub>a1</sub> = &rho;<sub>0</sub> &nbsp; (+V&#775;<sub>ab,p</sub>/2 + &nbsp; V&#775;<sub>ab,t</sub>),
- </p>
- <p>
- and, similarly,
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-     V&#775;<sub>ba</sub> = &rho;<sub>0</sub> &nbsp; (-V&#775;<sub>ab,p</sub>/2 + &nbsp; V&#775;<sub>ba,t</sub>),
- </p>
- <p>
- where we simplified the calculation by using the density <i>&rho;<sub>0</sub></i>.
- To calculate <i>V&#775;<sub>ba,t</sub></i>, we again use the density <i>&rho;<sub>0</sub></i>
- and because of this simplification, we can write
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-     m&#775;<sub>ab,t</sub> =  -m&#775;<sub>ba,t</sub> = &rho;<sub>0</sub> &nbsp; V&#775;<sub>ab,t</sub>
-   =  -&rho;<sub>0</sub> &nbsp; V&#775;<sub>ba,t</sub>,
- </p>
- <p>
- from which follows that the neutral height, e.g., the height where the air flow rate due to flow
- induced by temperature difference is zero, is at <i>h/2</i>.
- Hence,
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- V&#775;<sub>ab,t</sub> = C<sub>D</sub> &int;<sub>0</sub><sup>h/2</sup> w v(z) dz,
- </p>
- <p>
- where <i>v(z)</i> is the velocity at height <i>z</i>. From the Bernoulli equation, we obtain
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- v(z) = (2 g z &Delta;&rho; &frasl; &rho;<sub>0</sub>)<sup>1/2</sup>.
- </p>
- <p>
- The density difference can be written as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &Delta;&rho; = &rho;<sub>a</sub>-&rho;<sub>b</sub>
-   &asymp; &rho;<sub>0</sub> (T<sub>b</sub> - T<sub>a</sub>) &frasl; T<sub>0</sub>,
- </p>
- <p>
- where we used
- <i>&rho;<sub>a</sub> = p<sub>0</sub> /(R T<sub>a</sub>)</i> and
- <i>T<sub>a</sub> T<sub>b</sub> &asymp; T<sub>0</sub><sup>2</sup></i>.
- Substituting this expression into the integral and integrating from <i>0</i> to <i>z</i> yields
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- V&#775;<sub>ab,t</sub> = 1&frasl;3  C<sub>D</sub> w h
- (g h &frasl; (R T<sub>0</sub> &rho;<sub>0</sub>))<sup>1/2</sup> &Delta;p<sup>1/2</sup>.
- </p>
- <p>
- The above equation is equivalent to (6) in Brown and Solvason (1962).
- <h4>Main assumptions</h4>
- <p>
- The main assumptions are as follows:
- </p>
- <ul>
- <li>
- <p>
- The air flow rates due to static pressure difference and due to temperature-difference can be superposed.
- </p>
- </li>
- <li>
- <p>
- For buoyancy-driven air flow, a constant density can be used to convert air volume flow rate to air mass flow rate.
- </p>
- </li>
- </ul>
- <p>
- From these assumptions follows that the neutral height for buoyancy-driven air flow is at half of the height
- of the opening.
- </p>
- <h4>Notes</h4>
- <p>
- For a more detailed model, use
- <a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOpen\">
- AixLib.Airflow.Multizone.DoorDiscretizedOpen</a>.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Brown, W.G. and K. R. Solvason.
- Natural Convection through rectangular openings in partitions - 1.
- <i>Int. Journal of Heat and Mass Transfer</i>.
- Vol. 5, p. 859-868. 1962.
- <a href=\"https://doi.org/10.1016/0017-9310(62)90184-9\">doi:10.1016/0017-9310(62)90184-9</a>.<br/>
- Also available at
- <a href=\"https://nrc-publications.canada.ca/eng/view/ft/?id=081c0ace-7c31-449c-9b3b-e6c14864b196\">
- https://nrc-publications.canada.ca/eng/view/ft/?id=081c0ace-7c31-449c-9b3b-e6c14864b196</a>.
- </li>
- </ul>
- </html>",
+<p>
+Model for bi-directional air flow through a large opening such as a door.
+</p>
+<p>
+In this model, the air flow is composed of two components,
+a one-directional bulk air flow
+due to static pressure difference in the adjoining two thermal zones, and
+a two-directional airflow due to temperature-induced differences in density
+of the air in the two thermal zones.
+Although turbulent air flow is a nonlinear phenomenon,
+the model is based on the simplifying assumption that these two
+air flow rates can be superposed.
+(Superposition is only exact for laminar flow.)
+This assumption is made because
+it leads to a simple model and because there is significant uncertainty
+and assumptions anyway in such simplified a model for bidirectional flow through a door.
+</p>
+<h4>Main equations</h4>
+<p>
+The air flow rate due to static pressure difference is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+    V&#775;<sub>ab,p</sub> =  C<sub>D</sub> w h (2/&rho;<sub>0</sub>)<sup>0.5</sup>  &Delta;p<sup>m</sup>,
+</p>
+<p>
+where
+<i>V&#775;</i> is the volumetric air flow rate,
+<i>C<sub>D</sub></i> is the discharge coefficient,
+<i>w</i> and <i>h</i> are the width and height of the opening,
+<i>&rho;<sub>0</sub></i> is the mass density at the medium default pressure, temperature and humidity,
+<i>m</i> is the flow exponent and
+<i>&Delta;p = p<sub>a</sub> - p<sub>b</sub></i> is the static pressure difference between
+the thermal zones.
+For this model explanation, we will assume <i>p<sub>a</sub> &gt; p<sub>b</sub></i>.
+For turbulent flow, <i>m=1/2</i> and for laminar flow <i>m=1</i>.
+</p>
+<p>
+The air flow rate due to temperature difference in the thermal zones is
+<i>V&#775;<sub>ab,t</sub></i> for flow from thermal zone <i>a</i> to <i>b</i>,
+and
+<i>V&#775;<sub>ba,t</sub></i> for air flow rate from thermal zone <i>b</i> to <i>a</i>.
+The model has two air flow paths to allow bi-directional air flow.
+The mass flow rates at these two air flow paths are
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+    m&#775;<sub>a1</sub> = &rho;<sub>0</sub> &nbsp; (+V&#775;<sub>ab,p</sub>/2 + &nbsp; V&#775;<sub>ab,t</sub>),
+</p>
+<p>
+and, similarly,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+    V&#775;<sub>ba</sub> = &rho;<sub>0</sub> &nbsp; (-V&#775;<sub>ab,p</sub>/2 + &nbsp; V&#775;<sub>ba,t</sub>),
+</p>
+<p>
+where we simplified the calculation by using the density <i>&rho;<sub>0</sub></i>.
+To calculate <i>V&#775;<sub>ba,t</sub></i>, we again use the density <i>&rho;<sub>0</sub></i>
+and because of this simplification, we can write
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+    m&#775;<sub>ab,t</sub> =  -m&#775;<sub>ba,t</sub> = &rho;<sub>0</sub> &nbsp; V&#775;<sub>ab,t</sub>
+  =  -&rho;<sub>0</sub> &nbsp; V&#775;<sub>ba,t</sub>,
+</p>
+<p>
+from which follows that the neutral height, e.g., the height where the air flow rate due to flow
+induced by temperature difference is zero, is at <i>h/2</i>.
+Hence,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+V&#775;<sub>ab,t</sub> = C<sub>D</sub> &int;<sub>0</sub><sup>h/2</sup> w v(z) dz,
+</p>
+<p>
+where <i>v(z)</i> is the velocity at height <i>z</i>. From the Bernoulli equation, we obtain
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+v(z) = (2 g z &Delta;&rho; &frasl; &rho;<sub>0</sub>)<sup>1/2</sup>.
+</p>
+<p>
+The density difference can be written as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &Delta;&rho; = &rho;<sub>a</sub>-&rho;<sub>b</sub>
+  &asymp; &rho;<sub>0</sub> (T<sub>b</sub> - T<sub>a</sub>) &frasl; T<sub>0</sub>,
+</p>
+<p>
+where we used
+<i>&rho;<sub>a</sub> = p<sub>0</sub> /(R T<sub>a</sub>)</i> and
+<i>T<sub>a</sub> T<sub>b</sub> &asymp; T<sub>0</sub><sup>2</sup></i>.
+Substituting this expression into the integral and integrating from <i>0</i> to <i>z</i> yields
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+V&#775;<sub>ab,t</sub> = 1&frasl;3  C<sub>D</sub> w h
+(g h &frasl; (R T<sub>0</sub> &rho;<sub>0</sub>))<sup>1/2</sup> &Delta;p<sup>1/2</sup>.
+</p>
+<p>
+The above equation is equivalent to (6) in Brown and Solvason (1962).
+<h4>Main assumptions</h4>
+<p>
+The main assumptions are as follows:
+</p>
+<ul>
+<li>
+<p>
+The air flow rates due to static pressure difference and due to temperature-difference can be superposed.
+</p>
+</li>
+<li>
+<p>
+For buoyancy-driven air flow, a constant density can be used to convert air volume flow rate to air mass flow rate.
+</p>
+</li>
+</ul>
+<p>
+From these assumptions follows that the neutral height for buoyancy-driven air flow is at half of the height
+of the opening.
+</p>
+<h4>Notes</h4>
+<p>
+For a more detailed model, use
+<a href=\"modelica://AixLib.Airflow.Multizone.DoorDiscretizedOpen\">
+AixLib.Airflow.Multizone.DoorDiscretizedOpen</a>.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Brown, W.G. and K. R. Solvason.
+Natural Convection through rectangular openings in partitions - 1.
+<i>Int. Journal of Heat and Mass Transfer</i>.
+Vol. 5, p. 859-868. 1962.
+<a href=\"https://doi.org/10.1016/0017-9310(62)90184-9\">doi:10.1016/0017-9310(62)90184-9</a>.<br/>
+Also available at
+<a href=\"https://nrc-publications.canada.ca/eng/view/ft/?id=081c0ace-7c31-449c-9b3b-e6c14864b196\">
+https://nrc-publications.canada.ca/eng/view/ft/?id=081c0ace-7c31-449c-9b3b-e6c14864b196</a>.
+</li>
+</ul>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 22, 2020, by Michael Wetter:<br/>
- Revised buoyancy-driven flow based on Brown and Solvason (1962).
- </li>
- <li>
- January 19, 2020, by Klaas De Jonge:<br/>
- Revised influence of stack effect.
- </li>
- <li>
- October 6, 2020, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1353\">#1353</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 22, 2020, by Michael Wetter:<br/>
+Revised buoyancy-driven flow based on Brown and Solvason (1962).
+</li>
+<li>
+January 19, 2020, by Klaas De Jonge:<br/>
+Revised influence of stack effect.
+</li>
+<li>
+October 6, 2020, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1353\">#1353</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DoorOpen;
diff --git a/AixLib/Airflow/Multizone/DoorOperable.mo b/AixLib/Airflow/Multizone/DoorOperable.mo
index e4ca01c5cb..501acf3434 100644
--- a/AixLib/Airflow/Multizone/DoorOperable.mo
+++ b/AixLib/Airflow/Multizone/DoorOperable.mo
@@ -86,108 +86,108 @@ equation
 
   annotation (defaultComponentName="doo",
 Documentation(info="<html>
- <p>
- Model for bi-directional air flow through a large opening such as a door which can be opened or closed
- based on the control input signal <i>y</i>.
- </p>
- <p>
- For the control input signal <i>y=1</i>, this model is identical to
- <a href=\"modelica://AixLib.Airflow.Multizone.DoorOpen\">
- AixLib.Airflow.Multizone.DoorOpen</a>, and for
- <i>y=0</i>, the door is assumed to be closed and the air flow rate is
- set to the air flow rate through the crack posed by the open door, <i>V&#775;<sub>clo</sub></i>.
- <p>
- The air flow rate for the closed door is computed as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-     V&#775;<sub>clo</sub> = C<sub>clo</sub> &Delta;p<sup>mClo</sup>,
- </p>
- <p>
- where
- <i>V&#775;<sub>clo</sub></i> is the volume flow rate,
- <i>C<sub>clo</sub></i> is a flow coefficient and
- <i>mClo</i> is the flow exponent.
- The flow coefficient is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- C<sub>clo</sub> = L<sub>clo</sub> C<sub>DCloRat</sub> &Delta;p<sub>Rat</sub><sup>(0.5-mClo</sup>) (2/&rho;<sub>0</sub>)<sup>0.5</sup>,
- </p>
- <p>
- where
- <i>L<sub>clo</sub></i> is the effective air leakage area,
- <i>C<sub>DCloRat</sub></i> is the discharge coefficient at the reference condition,
- <i>&Delta;p<sub>Rat</sub></i> is the pressure drop at the rating condition, and
- <i>&rho;<sub>0</sub></i> is the mass density at the medium default pressure, temperature and humidity.
- </p>
- <p>
- The effective air leakage area <i>L<sub>clo</sub></i> can be obtained, for example,
- from the ASHRAE fundamentals (ASHRAE, 1997, p. 25.18). In
- the ASHRAE fundamentals, the effective air leakage area is
- based on a reference pressure difference of <i>&Delta;p<sub>Rat</sub> = 4</i> Pa and a discharge
- coefficient of <i>C<sub>DCloRat</sub> = 1</i>.
- A similar model is also used in the CONTAM software (Dols and Walton, 2002).
- Dols and Walton (2002) recommend to use for the flow exponent
- <i>mClo=0.6</i> to <i>mClo=0.7</i> if the flow exponent is not
- reported with the test results.
- </p>
- <p>
- For the open door, the air flow rate
- <i>V&#775;<sub>ope</sub></i> is computed as described in
- <a href=\"modelica://AixLib.Airflow.Multizone.DoorOpen\">
- AixLib.Airflow.Multizone.DoorOpen</a>
- with the parameters <code>CDOpe</code> and <code>mOpe</code>.
- </p>
- <p>
- The actual air flow rate is computed as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- V&#775;<sub>clo</sub> = (y-1) V&#775;<sub>clo</sub> + y V&#775;<sub>ope</sub>,
- </p>
- <p>
- where <i>y &isin; [0, 1]</i> is the control signal.
- Note that for values of <i>y</i> that are different from <i>0</i> and
- <i>1</i>, the model simply interpolates the air flow rate between a fully open
- and a fully closed door. In practice, the air flow rate would likely increase quickly if the
- door is slightly opened, and hence we do not claim that the model is accurate for
- values other than <i>y = 0</i> and <i>y = 1</i>.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- ASHRAE.
- <i>ASHRAE Fundamentals</i>,
- American Society of Heating, Refrigeration and Air-Conditioning
- Engineers, 1997.
- </li>
- <li>
- Dols and Walton.
- W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual,
- Multizone Airflow and Contaminant Transport Analysis Software</i>,
- Building and Fire Research Laboratory,
- National Institute of Standards and Technology,
- Tech. Report NISTIR 6921,
- November, 2002.
- </li>
- </ul>
- </html>",
+<p>
+Model for bi-directional air flow through a large opening such as a door which can be opened or closed
+based on the control input signal <i>y</i>.
+</p>
+<p>
+For the control input signal <i>y=1</i>, this model is identical to
+<a href=\"modelica://AixLib.Airflow.Multizone.DoorOpen\">
+AixLib.Airflow.Multizone.DoorOpen</a>, and for
+<i>y=0</i>, the door is assumed to be closed and the air flow rate is
+set to the air flow rate through the crack posed by the open door, <i>V&#775;<sub>clo</sub></i>.
+<p>
+The air flow rate for the closed door is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+    V&#775;<sub>clo</sub> = C<sub>clo</sub> &Delta;p<sup>mClo</sup>,
+</p>
+<p>
+where
+<i>V&#775;<sub>clo</sub></i> is the volume flow rate,
+<i>C<sub>clo</sub></i> is a flow coefficient and
+<i>mClo</i> is the flow exponent.
+The flow coefficient is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+C<sub>clo</sub> = L<sub>clo</sub> C<sub>DCloRat</sub> &Delta;p<sub>Rat</sub><sup>(0.5-mClo</sup>) (2/&rho;<sub>0</sub>)<sup>0.5</sup>,
+</p>
+<p>
+where
+<i>L<sub>clo</sub></i> is the effective air leakage area,
+<i>C<sub>DCloRat</sub></i> is the discharge coefficient at the reference condition,
+<i>&Delta;p<sub>Rat</sub></i> is the pressure drop at the rating condition, and
+<i>&rho;<sub>0</sub></i> is the mass density at the medium default pressure, temperature and humidity.
+</p>
+<p>
+The effective air leakage area <i>L<sub>clo</sub></i> can be obtained, for example,
+from the ASHRAE fundamentals (ASHRAE, 1997, p. 25.18). In
+the ASHRAE fundamentals, the effective air leakage area is
+based on a reference pressure difference of <i>&Delta;p<sub>Rat</sub> = 4</i> Pa and a discharge
+coefficient of <i>C<sub>DCloRat</sub> = 1</i>.
+A similar model is also used in the CONTAM software (Dols and Walton, 2002).
+Dols and Walton (2002) recommend to use for the flow exponent
+<i>mClo=0.6</i> to <i>mClo=0.7</i> if the flow exponent is not
+reported with the test results.
+</p>
+<p>
+For the open door, the air flow rate
+<i>V&#775;<sub>ope</sub></i> is computed as described in
+<a href=\"modelica://AixLib.Airflow.Multizone.DoorOpen\">
+AixLib.Airflow.Multizone.DoorOpen</a>
+with the parameters <code>CDOpe</code> and <code>mOpe</code>.
+</p>
+<p>
+The actual air flow rate is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+V&#775;<sub>clo</sub> = (y-1) V&#775;<sub>clo</sub> + y V&#775;<sub>ope</sub>,
+</p>
+<p>
+where <i>y &isin; [0, 1]</i> is the control signal.
+Note that for values of <i>y</i> that are different from <i>0</i> and
+<i>1</i>, the model simply interpolates the air flow rate between a fully open
+and a fully closed door. In practice, the air flow rate would likely increase quickly if the
+door is slightly opened, and hence we do not claim that the model is accurate for
+values other than <i>y = 0</i> and <i>y = 1</i>.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+ASHRAE.
+<i>ASHRAE Fundamentals</i>,
+American Society of Heating, Refrigeration and Air-Conditioning
+Engineers, 1997.
+</li>
+<li>
+Dols and Walton.
+W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual,
+Multizone Airflow and Contaminant Transport Analysis Software</i>,
+Building and Fire Research Laboratory,
+National Institute of Standards and Technology,
+Tech. Report NISTIR 6921,
+November, 2002.
+</li>
+</ul>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 11, 2021, by Michael Wetter:<br/>
- Removed duplicate declaration of <code>VABp_flow</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1496\">#1496</a>.
- </li>
- <li>
- January 22, 2020, by Michael Wetter:<br/>
- Revised buoyancy-driven flow.
- </li>
- <li>
- October 6, 2020, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1353\">#1353</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 11, 2021, by Michael Wetter:<br/>
+Removed duplicate declaration of <code>VABp_flow</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1496\">#1496</a>.
+</li>
+<li>
+January 22, 2020, by Michael Wetter:<br/>
+Revised buoyancy-driven flow.
+</li>
+<li>
+October 6, 2020, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1353\">#1353</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DoorOperable;
diff --git a/AixLib/Airflow/Multizone/EffectiveAirLeakageArea.mo b/AixLib/Airflow/Multizone/EffectiveAirLeakageArea.mo
index 03fd97a625..2d1bc0ba67 100644
--- a/AixLib/Airflow/Multizone/EffectiveAirLeakageArea.mo
+++ b/AixLib/Airflow/Multizone/EffectiveAirLeakageArea.mo
@@ -72,117 +72,117 @@ model EffectiveAirLeakageArea "Effective air leakage area"
           fillPattern=FillPattern.Solid)}),
 defaultComponentName="lea",
 Documentation(info="<html>
- <p>
- This model describes the one-directional pressure driven
- air flow through a crack-like opening, using the equation
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-     V&#775; = C &Delta;p<sup>m</sup>,
- </p>
- <p>
- where
- <i>V&#775;</i> is the volume flow rate,
- <i>C</i> is a flow coefficient and
- <i>m</i> is the flow exponent.
- The flow coefficient is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- C = L C<sub>D,Rat</sub> &Delta;p<sub>Rat</sub><sup>(0.5-m)</sup> (2/&rho;<sub>0</sub>)<sup>0.5</sup>,
- </p>
- <p>
- where
- <i>L</i> is the effective air leakage area,
- <i>C<sub>D,Rat</sub></i> is the discharge coefficient at the reference condition,
- <i>&Delta;p<sub>Rat</sub></i> is the pressure drop at the rating condition, and
- <i>&rho;<sub>0</sub></i> is the mass density at the medium default pressure, temperature and humidity.
- </p>
- <p>
- The effective air leakage area <i>L</i> can be obtained, for example,
- from the ASHRAE fundamentals (ASHRAE, 1997, p. 25.18). In
- the ASHRAE fundamentals, the effective air leakage area is
- based on a reference pressure difference of <i>&Delta;p<sub>Rat</sub> = 4</i> Pa and a discharge
- coefficient of <i>C<sub>D,Rat</sub> = 1</i>.
- A similar model is also used in the CONTAM software (Dols and Walton, 2002).
- Dols and Walton (2002) recommend to use for the flow exponent
- <i>m=0.6</i> to <i>m=0.7</i> if the flow exponent is not
- reported with the test results.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- <b>ASHRAE, 1997.</b>
- <i>ASHRAE Fundamentals</i>,
- American Society of Heating, Refrigeration and Air-Conditioning
- Engineers, 1997.
- </li>
- <li>
- <b>Dols and Walton, 2002.</b>
- W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual,
- Multizone Airflow and Contaminant Transport Analysis Software</i>,
- Building and Fire Research Laboratory,
- National Institute of Standards and Technology,
- Tech. Report NISTIR 6921,
- November, 2002.
- </li>
- <li>Michael Wetter. <a href=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Wetter-airflow-2006.pdf\">Multizone Airflow Model in Modelica.</a> Proc. of the 5th International Modelica Conference, p. 431-440. Vienna, Austria, September 2006. </li>
- </ul>
- </html>",
+<p>
+This model describes the one-directional pressure driven
+air flow through a crack-like opening, using the equation
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+    V&#775; = C &Delta;p<sup>m</sup>,
+</p>
+<p>
+where
+<i>V&#775;</i> is the volume flow rate,
+<i>C</i> is a flow coefficient and
+<i>m</i> is the flow exponent.
+The flow coefficient is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+C = L C<sub>D,Rat</sub> &Delta;p<sub>Rat</sub><sup>(0.5-m)</sup> (2/&rho;<sub>0</sub>)<sup>0.5</sup>,
+</p>
+<p>
+where
+<i>L</i> is the effective air leakage area,
+<i>C<sub>D,Rat</sub></i> is the discharge coefficient at the reference condition,
+<i>&Delta;p<sub>Rat</sub></i> is the pressure drop at the rating condition, and
+<i>&rho;<sub>0</sub></i> is the mass density at the medium default pressure, temperature and humidity.
+</p>
+<p>
+The effective air leakage area <i>L</i> can be obtained, for example,
+from the ASHRAE fundamentals (ASHRAE, 1997, p. 25.18). In
+the ASHRAE fundamentals, the effective air leakage area is
+based on a reference pressure difference of <i>&Delta;p<sub>Rat</sub> = 4</i> Pa and a discharge
+coefficient of <i>C<sub>D,Rat</sub> = 1</i>.
+A similar model is also used in the CONTAM software (Dols and Walton, 2002).
+Dols and Walton (2002) recommend to use for the flow exponent
+<i>m=0.6</i> to <i>m=0.7</i> if the flow exponent is not
+reported with the test results.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+<b>ASHRAE, 1997.</b>
+<i>ASHRAE Fundamentals</i>,
+American Society of Heating, Refrigeration and Air-Conditioning
+Engineers, 1997.
+</li>
+<li>
+<b>Dols and Walton, 2002.</b>
+W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual,
+Multizone Airflow and Contaminant Transport Analysis Software</i>,
+Building and Fire Research Laboratory,
+National Institute of Standards and Technology,
+Tech. Report NISTIR 6921,
+November, 2002.
+</li>
+<li>Michael Wetter. <a href=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Wetter-airflow-2006.pdf\">Multizone Airflow Model in Modelica.</a> Proc. of the 5th International Modelica Conference, p. 431-440. Vienna, Austria, September 2006. </li>
+</ul>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, by Klaas De Jonge:<br/>
- Changes due to changes in the baseclass, velocity is now a top-level variable.
- </li>
- <li>
- June 24, 2018, by Michael Wetter:<br/>
- Removed parameter <code>lWet</code> as it is only used to compute
- the Reynolds number, and the Reynolds number is not used by this model.
- Also removed the variable <code>Re</code> for the Reynolds number.<br/>
- Changed base class to remove the parameters <code>A</code> and <code>CD</code>
- which are not used by this model.<br/>
- This change is non-backward compatible.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/932\">IBPSA, #932</a>.
- </li>
- <li>
- May 30, 2018, by Michael Wetter:<br/>
- Improved documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/546\">IBPSA, #546</a>.
- </li>
- <li>
- April 24, 2017, by Filip Jorissen:<br/>
- Corrected error in computation of <code>A</code> which was
- <code>A=CD/CDRat * L * dpRat^(0.5-m)</code> rather than
- <code>A=CDRat/CD * L * dpRat^(0.5-m)</code>.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/743\">#743</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Changed the parameter <code>useConstantDensity</code> to
- <code>useDefaultProperties</code> to use consistent names within this package.
- A conversion script can be used to update this parameter.
- </li>
- <li>
- July 20, 2010 by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>
- February 10, 2005 by Michael Wetter:<br/>
- Released first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, by Klaas De Jonge:<br/>
+Changes due to changes in the baseclass, velocity is now a top-level variable.
+</li>
+<li>
+June 24, 2018, by Michael Wetter:<br/>
+Removed parameter <code>lWet</code> as it is only used to compute
+the Reynolds number, and the Reynolds number is not used by this model.
+Also removed the variable <code>Re</code> for the Reynolds number.<br/>
+Changed base class to remove the parameters <code>A</code> and <code>CD</code>
+which are not used by this model.<br/>
+This change is non-backward compatible.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/932\">IBPSA, #932</a>.
+</li>
+<li>
+May 30, 2018, by Michael Wetter:<br/>
+Improved documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/546\">IBPSA, #546</a>.
+</li>
+<li>
+April 24, 2017, by Filip Jorissen:<br/>
+Corrected error in computation of <code>A</code> which was
+<code>A=CD/CDRat * L * dpRat^(0.5-m)</code> rather than
+<code>A=CDRat/CD * L * dpRat^(0.5-m)</code>.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/743\">#743</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Changed the parameter <code>useConstantDensity</code> to
+<code>useDefaultProperties</code> to use consistent names within this package.
+A conversion script can be used to update this parameter.
+</li>
+<li>
+July 20, 2010 by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>
+February 10, 2005 by Michael Wetter:<br/>
+Released first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EffectiveAirLeakageArea;
diff --git a/AixLib/Airflow/Multizone/Examples/CO2TransportStep.mo b/AixLib/Airflow/Multizone/Examples/CO2TransportStep.mo
index 31dd2277ba..b5b7763d41 100644
--- a/AixLib/Airflow/Multizone/Examples/CO2TransportStep.mo
+++ b/AixLib/Airflow/Multizone/Examples/CO2TransportStep.mo
@@ -5,13 +5,19 @@ model CO2TransportStep "Model with transport of CO2 through buoyancy driven flow
     volTop(nPorts=3),
     volEas(nPorts=6));
 
-  AixLib.Fluid.Sensors.TraceSubstances CO2SenTop(redeclare package Medium = Medium)
+  AixLib.Fluid.Sensors.TraceSubstances CO2SenTop(
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "CO2 sensor"
     annotation (Placement(transformation(extent={{20,120},{40,140}})));
-  AixLib.Fluid.Sensors.TraceSubstances CO2SenWes(redeclare package Medium = Medium)
+  AixLib.Fluid.Sensors.TraceSubstances CO2SenWes(
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "CO2 sensor"
     annotation (Placement(transformation(extent={{-102,10},{-82,30}})));
-  AixLib.Fluid.Sensors.TraceSubstances CO2SenEas(redeclare package Medium = Medium)
+  AixLib.Fluid.Sensors.TraceSubstances CO2SenEas(
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "CO2 sensor"
     annotation (Placement(transformation(extent={{58,10},{78,30}})));
   Modelica.Blocks.Sources.Pulse pulse(
@@ -51,32 +57,38 @@ equation
       StopTime=86400,
       Tolerance=1e-6),
     Documentation(info="<html>
- <p>
- This model is based on
- <a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
- Buildings.Airflow.Multizone.Validation.ThreeRoomsContam</a>.
- In addition, a CO<sub>2</sub> source has been added to the left room
- in the bottom floor.
- At initial time, all volumes have zero CO<sub>2</sub> concentration.
- At <i>t=3600</i> seconds, CO<sub>2</sub> is added to <code>volWes</code>.
- As time progresses, the CO<sub>2</sub> is transported to
- the other rooms, and eventually its concentration decays.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Extended model from
- <a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
- Buildings.Airflow.Multizone.Validation.ThreeRoomsContam</a>
- and added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
-end CO2TransportStep;
+<p>
+This model is based on
+<a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
+Buildings.Airflow.Multizone.Validation.ThreeRoomsContam</a>.
+In addition, a CO<sub>2</sub> source has been added to the left room
+in the bottom floor.
+At initial time, all volumes have zero CO<sub>2</sub> concentration.
+At <i>t=3600</i> seconds, CO<sub>2</sub> is added to <code>volWes</code>.
+As time progresses, the CO<sub>2</sub> is transported to
+the other rooms, and eventually its concentration decays.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2024, by Michael Wetter:<br/>
+Configured the sensor parameter to suppress the warning about being a one-port connection.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1857\">IBPSA, #1857</a>.
+</li>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Extended model from
+<a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
+Buildings.Airflow.Multizone.Validation.ThreeRoomsContam</a>
+and added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CO2TransportStep;
\ No newline at end of file
diff --git a/AixLib/Airflow/Multizone/Examples/ChimneyShaftNoVolume.mo b/AixLib/Airflow/Multizone/Examples/ChimneyShaftNoVolume.mo
index 502a1c741c..14393c566a 100644
--- a/AixLib/Airflow/Multizone/Examples/ChimneyShaftNoVolume.mo
+++ b/AixLib/Airflow/Multizone/Examples/ChimneyShaftNoVolume.mo
@@ -149,77 +149,77 @@ equation
       StopTime=3600,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This model demonstrate buoyancy-induced air flow
- through a vertical shaft.
- On the right, there are two flow paths that are connected
- to a volume, which is kept at 20&deg;C through a feedback
- controller, and to the ambient, which is at
- 0&deg;C.
- The flow path on the very right consists of an orifice
- and two models that compute the pressure difference
- <i>&Delta;p</i>
- between
- the bottom and top of the medium column using <i>&Delta;p=h &rho; g</i>,
- where
- <i>h</i> is the height of the medium column,
- <i>&rho;</i> is the density of the medium column and
- <i>g</i> is the gravity constant.
- </p>
- <p>
- The top model is parameterized to use the
- density from the ambient,
- whereas the bottom model is parameterized to use
- the density from the room volume, regardless of
- the flow direction.
- In the other flow path, the model <code>sha</code>
- is parameterized to use the density of the inflowing
- medium.
- Thus, these models can be thought of as a chimney to the left,
- and a roof with a leakage on the right. The chimney height starts
- <i>1.5</i> m below the roof, and ends <i>1.5</i> m above the roof.
- </p>
- <p>
- The flow boundary condition of the model
- <code>boundary</code> is such that at the start
- of the simulation, air flows from <code>boundary</code>
- to <code>roo</code> until <i>t=600</i> seconds. Then, the flow rate
- is set to zero until <i>t=1800</i> seconds.
- Since the shaft <code>sha</code> is filled with
- 20&deg;C air, there is a circulation in the clock-wise
- direction; up the shaft, and down the other flow path.
- Next, until <i>t=2400</i> seconds, air is extracted from
- the volume <code>roo</code>, and then the flow rate
- of <code>boundary</code> is set to zero. Since the
- shaft <code>sha</code> is now filed with air at 0&deg;C,
- there is a counter clock-wise flow; down the shaft, and
- up the other flow path.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- February 24, 2015 by Michael Wetter:<br/>
- Changed media to
- <a href=\"modelica://Modelica.Media.Air.SimpleAir\">
- Modelica.Media.Air.SimpleAir</a>
- in order to test the medium column for a media that has no moisture.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model demonstrate buoyancy-induced air flow
+through a vertical shaft.
+On the right, there are two flow paths that are connected
+to a volume, which is kept at 20&deg;C through a feedback
+controller, and to the ambient, which is at
+0&deg;C.
+The flow path on the very right consists of an orifice
+and two models that compute the pressure difference
+<i>&Delta;p</i>
+between
+the bottom and top of the medium column using <i>&Delta;p=h &rho; g</i>,
+where
+<i>h</i> is the height of the medium column,
+<i>&rho;</i> is the density of the medium column and
+<i>g</i> is the gravity constant.
+</p>
+<p>
+The top model is parameterized to use the
+density from the ambient,
+whereas the bottom model is parameterized to use
+the density from the room volume, regardless of
+the flow direction.
+In the other flow path, the model <code>sha</code>
+is parameterized to use the density of the inflowing
+medium.
+Thus, these models can be thought of as a chimney to the left,
+and a roof with a leakage on the right. The chimney height starts
+<i>1.5</i> m below the roof, and ends <i>1.5</i> m above the roof.
+</p>
+<p>
+The flow boundary condition of the model
+<code>boundary</code> is such that at the start
+of the simulation, air flows from <code>boundary</code>
+to <code>roo</code> until <i>t=600</i> seconds. Then, the flow rate
+is set to zero until <i>t=1800</i> seconds.
+Since the shaft <code>sha</code> is filled with
+20&deg;C air, there is a circulation in the clock-wise
+direction; up the shaft, and down the other flow path.
+Next, until <i>t=2400</i> seconds, air is extracted from
+the volume <code>roo</code>, and then the flow rate
+of <code>boundary</code> is set to zero. Since the
+shaft <code>sha</code> is now filed with air at 0&deg;C,
+there is a counter clock-wise flow; down the shaft, and
+up the other flow path.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+February 24, 2015 by Michael Wetter:<br/>
+Changed media to
+<a href=\"modelica://Modelica.Media.Air.SimpleAir\">
+Modelica.Media.Air.SimpleAir</a>
+in order to test the medium column for a media that has no moisture.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ChimneyShaftNoVolume;
diff --git a/AixLib/Airflow/Multizone/Examples/ChimneyShaftWithVolume.mo b/AixLib/Airflow/Multizone/Examples/ChimneyShaftWithVolume.mo
index 1120434b60..364214cbf2 100644
--- a/AixLib/Airflow/Multizone/Examples/ChimneyShaftWithVolume.mo
+++ b/AixLib/Airflow/Multizone/Examples/ChimneyShaftWithVolume.mo
@@ -151,40 +151,40 @@ equation
       StopTime=3600,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This model is identical to
- <a href=\"modelica://AixLib.Airflow.Multizone.Examples.ChimneyShaftNoVolume\">
- Buildings.Airflow.Multizone.Examples.ChimneyShaftNoVolume</a>,
- except that the chimney model is not steady-state, but rather dynamic
- as it contains an air volume. The air volume is approximated
- as being well-mixed. (Stratified volumes could be approximated by
- using multiple instances of the model <code>sha</code> that are
- connected in series.)
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- January 8, 2019, by Michael Wetter:<br/>
- Removed parameter assignment for <code>sha.m_flow_nominal</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/970\">#970</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model is identical to
+<a href=\"modelica://AixLib.Airflow.Multizone.Examples.ChimneyShaftNoVolume\">
+Buildings.Airflow.Multizone.Examples.ChimneyShaftNoVolume</a>,
+except that the chimney model is not steady-state, but rather dynamic
+as it contains an air volume. The air volume is approximated
+as being well-mixed. (Stratified volumes could be approximated by
+using multiple instances of the model <code>sha</code> that are
+connected in series.)
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+January 8, 2019, by Michael Wetter:<br/>
+Removed parameter assignment for <code>sha.m_flow_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/970\">#970</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ChimneyShaftWithVolume;
diff --git a/AixLib/Airflow/Multizone/Examples/ClosedDoors.mo b/AixLib/Airflow/Multizone/Examples/ClosedDoors.mo
index c42811fde7..5bc2eaac0a 100644
--- a/AixLib/Airflow/Multizone/Examples/ClosedDoors.mo
+++ b/AixLib/Airflow/Multizone/Examples/ClosedDoors.mo
@@ -108,40 +108,40 @@ experiment(Tolerance=1e-006, StopTime=7200),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/ClosedDoors.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model consists of three volumes that are connected among
- each other through three doors that all have the same geometry.
- All doors are closed, but they are not air-tight.
- Heat is added and removed from <code>volB</code> which induces
- a small air flow through the doors.
- </p>
- <p>
- This model uses
- <a href=\"modelica://AixLib.Media.Specialized.Air.PerfectGas\">
- Buildings.Media.Specialized.Air.PerfectGas</a>
- as the medium because
- <a href=\"modelica://AixLib.Media.Air\">
- Buildings.Media.Air</a>
- does not account for expansion if air the air is heated.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model consists of three volumes that are connected among
+each other through three doors that all have the same geometry.
+All doors are closed, but they are not air-tight.
+Heat is added and removed from <code>volB</code> which induces
+a small air flow through the doors.
+</p>
+<p>
+This model uses
+<a href=\"modelica://AixLib.Media.Specialized.Air.PerfectGas\">
+Buildings.Media.Specialized.Air.PerfectGas</a>
+as the medium because
+<a href=\"modelica://AixLib.Media.Air\">
+Buildings.Media.Air</a>
+does not account for expansion if air the air is heated.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ClosedDoors;
diff --git a/AixLib/Airflow/Multizone/Examples/NaturalVentilation.mo b/AixLib/Airflow/Multizone/Examples/NaturalVentilation.mo
index 353bcbd77f..1d0c67f139 100644
--- a/AixLib/Airflow/Multizone/Examples/NaturalVentilation.mo
+++ b/AixLib/Airflow/Multizone/Examples/NaturalVentilation.mo
@@ -87,35 +87,35 @@ experiment(Tolerance=1e-06, StopTime=7200),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/NaturalVentilation.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model illustrates buoyancy-driven natural ventilation between
- two volumes of air.
- The volume <code>volA</code> can be considered as the volume of a room,
- and the volume <code>volOut</code> is parameterized to be very large to emulate
- outside air.
- The outside air is <i>20</i>&deg;C and at initial time, the room air is
- <i>18</i>&deg;C.
- This induces an airflow in counter clock-wise direction. Since
- heat is added to the room air volume, its temperature raises above the temperature of the outside, which causes the air flow to reverse its direction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model illustrates buoyancy-driven natural ventilation between
+two volumes of air.
+The volume <code>volA</code> can be considered as the volume of a room,
+and the volume <code>volOut</code> is parameterized to be very large to emulate
+outside air.
+The outside air is <i>20</i>&deg;C and at initial time, the room air is
+<i>18</i>&deg;C.
+This induces an airflow in counter clock-wise direction. Since
+heat is added to the room air volume, its temperature raises above the temperature of the outside, which causes the air flow to reverse its direction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end NaturalVentilation;
diff --git a/AixLib/Airflow/Multizone/Examples/OneEffectiveAirLeakageArea.mo b/AixLib/Airflow/Multizone/Examples/OneEffectiveAirLeakageArea.mo
index 64ed64d43e..eff5713ace 100644
--- a/AixLib/Airflow/Multizone/Examples/OneEffectiveAirLeakageArea.mo
+++ b/AixLib/Airflow/Multizone/Examples/OneEffectiveAirLeakageArea.mo
@@ -69,30 +69,30 @@ equation
       StopTime=7200,
       Tolerance=1e-08),
     Documentation(info="<html>
- <p>
- This model consists of a model for an effective air leakage area
- that is connected to two air volumes.
- Air flows due to the addition of air to the volume <code>volA</code>
- and because heat is exchanged with <code>volB</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model consists of a model for an effective air leakage area
+that is connected to two air volumes.
+Air flows due to the addition of air to the volume <code>volA</code>
+and because heat is exchanged with <code>volB</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OneEffectiveAirLeakageArea;
diff --git a/AixLib/Airflow/Multizone/Examples/OneOpenDoor.mo b/AixLib/Airflow/Multizone/Examples/OneOpenDoor.mo
index 93b77401a0..04809a902e 100644
--- a/AixLib/Airflow/Multizone/Examples/OneOpenDoor.mo
+++ b/AixLib/Airflow/Multizone/Examples/OneOpenDoor.mo
@@ -82,38 +82,38 @@ equation
       StopTime=7200,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This model consists of two doors with the same geometry.
- For <i>t &le; 1000</i> seconds, the door <code>dooOpeClo</code>
- is closed, and afterwards it is open. The door
- <code>dooOpe</code> is always open.
- Heat is added to the volume <code>volB</code>, which causes
- a density difference between <code>volA</code> and <code>volB</code>.
- This density difference induces a bi-directional airflow through both doors.
- Both doors have exactly the same bi-directional airflow rates.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Removed parameter <code>show_V_flow</code>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model consists of two doors with the same geometry.
+For <i>t &le; 1000</i> seconds, the door <code>dooOpeClo</code>
+is closed, and afterwards it is open. The door
+<code>dooOpe</code> is always open.
+Heat is added to the volume <code>volB</code>, which causes
+a density difference between <code>volA</code> and <code>volB</code>.
+This density difference induces a bi-directional airflow through both doors.
+Both doors have exactly the same bi-directional airflow rates.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Removed parameter <code>show_V_flow</code>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OneOpenDoor;
diff --git a/AixLib/Airflow/Multizone/Examples/OneRoom.mo b/AixLib/Airflow/Multizone/Examples/OneRoom.mo
index b300fedb64..d164757c95 100644
--- a/AixLib/Airflow/Multizone/Examples/OneRoom.mo
+++ b/AixLib/Airflow/Multizone/Examples/OneRoom.mo
@@ -101,30 +101,30 @@ experiment(Tolerance=1e-06, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/OneRoom.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model has been used to validate buoyancy-driven air flow between two volumes.
- The volume <code>volEas</code> is at <i>20</i>&deg;C and the volume
- <code>volOut</code> is at <i>10</i>&deg;C.
- This initial condition induces a clock-wise airflow between the two volumes.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model has been used to validate buoyancy-driven air flow between two volumes.
+The volume <code>volEas</code> is at <i>20</i>&deg;C and the volume
+<code>volOut</code> is at <i>10</i>&deg;C.
+This initial condition induces a clock-wise airflow between the two volumes.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OneRoom;
diff --git a/AixLib/Airflow/Multizone/Examples/Orifice.mo b/AixLib/Airflow/Multizone/Examples/Orifice.mo
index 0c4239e48c..269d8da6ad 100644
--- a/AixLib/Airflow/Multizone/Examples/Orifice.mo
+++ b/AixLib/Airflow/Multizone/Examples/Orifice.mo
@@ -67,30 +67,30 @@ experiment(Tolerance=1e-06, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/Orifice.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates the use of the orifice model.
- The pressure difference across the orifice model changes
- between <i>-1</i> Pascal and <i>+1</i> Pascal, which
- causes air to flow through the orifice.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model demonstrates the use of the orifice model.
+The pressure difference across the orifice model changes
+between <i>-1</i> Pascal and <i>+1</i> Pascal, which
+causes air to flow through the orifice.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Orifice;
diff --git a/AixLib/Airflow/Multizone/Examples/PowerLaw.mo b/AixLib/Airflow/Multizone/Examples/PowerLaw.mo
index 7849759fe9..efc77545ed 100644
--- a/AixLib/Airflow/Multizone/Examples/PowerLaw.mo
+++ b/AixLib/Airflow/Multizone/Examples/PowerLaw.mo
@@ -104,23 +104,23 @@ experiment(
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/PowerLaw.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates the use of the 4 PowerLaw models present in the multizone package.
- The input data is fit so that all models have equivalent output.
- 
- The pressure difference across the models changes
- between <i>-1</i> Pascal and <i>+1</i> Pascal, which
- causes air to flow through the orifice.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 3, 2021 by Klaas De Jonge:<br/>
- Added example for the four 'Powerlaw' models in the Multizone package.
- </li>
- 
- </ul>
- </html>"),
-    Diagram(coordinateSystem(extent={{-120,-120},{120,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model demonstrates the use of the 4 PowerLaw models present in the multizone package.
+The input data is fit so that all models have equivalent output.
+
+The pressure difference across the models changes
+between <i>-1</i> Pascal and <i>+1</i> Pascal, which
+causes air to flow through the orifice.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 3, 2021 by Klaas De Jonge:<br/>
+Added example for the four 'Powerlaw' models in the Multizone package.
+</li>
+
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-120,-120},{120,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerLaw;
diff --git a/AixLib/Airflow/Multizone/Examples/PressurizationData.mo b/AixLib/Airflow/Multizone/Examples/PressurizationData.mo
index 8538067596..8e2bbf9829 100644
--- a/AixLib/Airflow/Multizone/Examples/PressurizationData.mo
+++ b/AixLib/Airflow/Multizone/Examples/PressurizationData.mo
@@ -67,40 +67,40 @@ equation
       StopTime=2592000,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This model illustrates the use of
- <a href=\"modelica://AixLib.Airflow.Multizone.Point_m_flow\">
- AixLib.Airflow.Multizone.Point_m_flow</a>
- to model
- infiltration through the building evelope for a known <i>n<sub>50</sub></i> value (also known as ACH50).
- As the <i>n<sub>50</sub></i> value and the building volume is known,
- the flow at 50 Pa is known. Dividing this flow accross the entire envelope
- (typically surface weighted) and using
- <a href=\"modelica://AixLib.Airflow.Multizone.Point_m_flow\">
- AixLib.Airflow.Multizone.Point_m_flow</a>,
- the infiltration airflow at lower pressure differences can be modelled.
- <br/>
- In this example, the two models each represent 50% of the surface where airflow occured due to the pressurization test.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 8, 2022, by Michael Wetter:<br/>
- Changed tolerance from <i>1E-8</i> to <i>1E-6</i>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1606\">IBPSA, #1606</a>.
- </li>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- May 03, 2021 by Klaas De Jonge:<br/>
- Added example for simulating infiltration airflow using the Powerlaw_1DataPoint model
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model illustrates the use of
+<a href=\"modelica://AixLib.Airflow.Multizone.Point_m_flow\">
+AixLib.Airflow.Multizone.Point_m_flow</a>
+to model
+infiltration through the building evelope for a known <i>n<sub>50</sub></i> value (also known as ACH50).
+As the <i>n<sub>50</sub></i> value and the building volume is known,
+the flow at 50 Pa is known. Dividing this flow accross the entire envelope
+(typically surface weighted) and using
+<a href=\"modelica://AixLib.Airflow.Multizone.Point_m_flow\">
+AixLib.Airflow.Multizone.Point_m_flow</a>,
+the infiltration airflow at lower pressure differences can be modelled.
+<br/>
+In this example, the two models each represent 50% of the surface where airflow occured due to the pressurization test.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 8, 2022, by Michael Wetter:<br/>
+Changed tolerance from <i>1E-8</i> to <i>1E-6</i>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1606\">IBPSA, #1606</a>.
+</li>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+May 03, 2021 by Klaas De Jonge:<br/>
+Added example for simulating infiltration airflow using the Powerlaw_1DataPoint model
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressurizationData;
diff --git a/AixLib/Airflow/Multizone/Examples/ReverseBuoyancy.mo b/AixLib/Airflow/Multizone/Examples/ReverseBuoyancy.mo
index e880841e29..742611c186 100644
--- a/AixLib/Airflow/Multizone/Examples/ReverseBuoyancy.mo
+++ b/AixLib/Airflow/Multizone/Examples/ReverseBuoyancy.mo
@@ -254,43 +254,43 @@ experiment(Tolerance=1e-06, StopTime=3600),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/ReverseBuoyancy.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model is similar than
- <a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
- AixLib.Airflow.Multizone.Validation.ThreeRoomsContam</a> but it has four
- instead of three rooms.
- The outdoor conditions are held constant at <i>10</i>&deg;C and
- atmospheric pressure.
- All four rooms are at different temperatures, with the rooms on the bottom
- floor being initially at a higher temperature than the rooms on the top floor.
- As time progresses, the temperatures of the two rooms on the respective floors
- asymptotically approach each other. The bottom floor eventually cools below
- the temperature of the top floor, because the
- bottom floor directly exchanges air with the outside.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model is similar than
+<a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
+AixLib.Airflow.Multizone.Validation.ThreeRoomsContam</a> but it has four
+instead of three rooms.
+The outdoor conditions are held constant at <i>10</i>&deg;C and
+atmospheric pressure.
+All four rooms are at different temperatures, with the rooms on the bottom
+floor being initially at a higher temperature than the rooms on the top floor.
+As time progresses, the temperatures of the two rooms on the respective floors
+asymptotically approach each other. The bottom floor eventually cools below
+the temperature of the top floor, because the
+bottom floor directly exchanges air with the outside.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReverseBuoyancy;
diff --git a/AixLib/Airflow/Multizone/Examples/ReverseBuoyancy3Zones.mo b/AixLib/Airflow/Multizone/Examples/ReverseBuoyancy3Zones.mo
index db190edb88..7e18ed018f 100644
--- a/AixLib/Airflow/Multizone/Examples/ReverseBuoyancy3Zones.mo
+++ b/AixLib/Airflow/Multizone/Examples/ReverseBuoyancy3Zones.mo
@@ -209,45 +209,45 @@ experiment(Tolerance=1e-06, StopTime=3600),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/ReverseBuoyancy3Zones.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model is similar than
- <a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
- AixLib.Airflow.Multizone.Validation.ThreeRoomsContam</a>.
- However, the initial temperatures are such that at the start of the
- simulation, the flow direction between the three rooms reverses direction.
- </p>
- <p>
- At the start of the simulation,
- the outdoor temperature is <i>15</i>&deg;C,
- and the temperatures of the volumes are
- <i>20</i>&deg;C at the top,
- <i>22</i>&deg;C at the bottom west and
- <i>25</i>&deg;C at the bottom east.
- Thus, initially there is a net flow circulation in the counter-clock
- direction.
- Because the volume on the east exchanges air with the outside,
- it cools down fast. Once it cooled down sufficiently,
- the flow direction between the three rooms reverses
- because the air in the bottom east is heaviest.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model is similar than
+<a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
+AixLib.Airflow.Multizone.Validation.ThreeRoomsContam</a>.
+However, the initial temperatures are such that at the start of the
+simulation, the flow direction between the three rooms reverses direction.
+</p>
+<p>
+At the start of the simulation,
+the outdoor temperature is <i>15</i>&deg;C,
+and the temperatures of the volumes are
+<i>20</i>&deg;C at the top,
+<i>22</i>&deg;C at the bottom west and
+<i>25</i>&deg;C at the bottom east.
+Thus, initially there is a net flow circulation in the counter-clock
+direction.
+Because the volume on the east exchanges air with the outside,
+it cools down fast. Once it cooled down sufficiently,
+the flow direction between the three rooms reverses
+because the air in the bottom east is heaviest.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReverseBuoyancy3Zones;
diff --git a/AixLib/Airflow/Multizone/Examples/TrickleVent.mo b/AixLib/Airflow/Multizone/Examples/TrickleVent.mo
index 8cc57e3429..0013e38f1e 100644
--- a/AixLib/Airflow/Multizone/Examples/TrickleVent.mo
+++ b/AixLib/Airflow/Multizone/Examples/TrickleVent.mo
@@ -103,30 +103,30 @@ equation
       Interval=600,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This model illustrates the use of the models
- <a href=\"modelica://AixLib.Airflow.Multizone.Table_V_flow\">
- AixLib.Airflow.Multizone.Table_V_flow</a>
- and
- <a href=\"modelica://AixLib.Airflow.Multizone.Table_m_flow\">
- AixLib.Airflow.Multizone.Table_m_flow</a>
- to model self regulating inlet vents.
- The models are connected to a common volume that emulates a room on one side and
- to outside conditions on the other side (east and west orientation respectively).
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- May 03, 2021 by Klaas De Jonge:<br/>
- Added example for simulating a trickle vent using the TableData models
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model illustrates the use of the models
+<a href=\"modelica://AixLib.Airflow.Multizone.Table_V_flow\">
+AixLib.Airflow.Multizone.Table_V_flow</a>
+and
+<a href=\"modelica://AixLib.Airflow.Multizone.Table_m_flow\">
+AixLib.Airflow.Multizone.Table_m_flow</a>
+to model self regulating inlet vents.
+The models are connected to a common volume that emulates a room on one side and
+to outside conditions on the other side (east and west orientation respectively).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+May 03, 2021 by Klaas De Jonge:<br/>
+Added example for simulating a trickle vent using the TableData models
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TrickleVent;
diff --git a/AixLib/Airflow/Multizone/Examples/ZonalFlow.mo b/AixLib/Airflow/Multizone/Examples/ZonalFlow.mo
index 00421bde3b..8e417336ed 100644
--- a/AixLib/Airflow/Multizone/Examples/ZonalFlow.mo
+++ b/AixLib/Airflow/Multizone/Examples/ZonalFlow.mo
@@ -66,41 +66,41 @@ experiment(Tolerance=1e-06, StopTime=3600),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/ZonalFlow.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example illustrates the use of the models that
- exchange a prescribed flow rate between the
- volumes that are attached to it.
- The block <code>ACS</code> prescribes the air exchange rate to
- 5 air changes per hour.
- The instance <code>zonFlo</code> takes as an input the air change per seconds,
- and the instance <code>floExc</code> takes as inputs the mass flow rate.
- For both instances, the air flows from
- <code>rooA</code> to <code>rooB</code>, and
- from <code>rooB</code> to <code>rooA</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- May 30, 2018, by Michael Wetter:<br/>
- Added example for instace of
- <a href=\"modelica://AixLib.Airflow.Multizone.ZonalFlow_m_flow\">AixLib.Airflow.Multizone.ZonalFlow_m_flow</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example illustrates the use of the models that
+exchange a prescribed flow rate between the
+volumes that are attached to it.
+The block <code>ACS</code> prescribes the air exchange rate to
+5 air changes per hour.
+The instance <code>zonFlo</code> takes as an input the air change per seconds,
+and the instance <code>floExc</code> takes as inputs the mass flow rate.
+For both instances, the air flows from
+<code>rooA</code> to <code>rooB</code>, and
+from <code>rooB</code> to <code>rooA</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+May 30, 2018, by Michael Wetter:<br/>
+Added example for instace of
+<a href=\"modelica://AixLib.Airflow.Multizone.ZonalFlow_m_flow\">AixLib.Airflow.Multizone.ZonalFlow_m_flow</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ZonalFlow;
diff --git a/AixLib/Airflow/Multizone/MediumColumn.mo b/AixLib/Airflow/Multizone/MediumColumn.mo
index 04d7246476..6fcfda6098 100644
--- a/AixLib/Airflow/Multizone/MediumColumn.mo
+++ b/AixLib/Airflow/Multizone/MediumColumn.mo
@@ -103,11 +103,13 @@ equation
         Text(
           extent={{24,-78},{106,-100}},
           textColor={0,0,127},
-          textString="Bottom"),
+          textString="Bottom",
+          fontSize=36),
         Text(
           extent={{32,104},{98,70}},
           textColor={0,0,127},
-          textString="Top"),
+          textString="Top",
+          fontSize=36),
         Text(
           extent={{36,26},{88,-10}},
           textColor={0,0,127},
@@ -128,8 +130,8 @@ equation
           lineColor={0,0,0}),
         Text(
           extent={{-50.5,20.5},{50.5,-20.5}},
-          lineColor={0,0,127},
-          origin={-72.5,-12.5},
+          textColor={0,0,127},
+          origin={-72.5,-0.5},
           rotation=90,
           textString="%name"),
         Rectangle(
@@ -141,7 +143,7 @@ equation
           lineColor={0,0,0}),
         Rectangle(
           visible=densitySelection == AixLib.Airflow.Multizone.Types.densitySelection.fromBottom,
-          extent={{-16,0},{16,-82}},
+          extent={{-16,0},{16,-80}},
           fillColor={85,170,255},
           fillPattern=FillPattern.Solid,
           pattern=LinePattern.None,
@@ -155,116 +157,116 @@ equation
           lineColor={0,0,0})}),
 defaultComponentName="col",
 Documentation(info="<html>
- <p>
- This model describes the pressure difference of a vertical medium
- column. It can be used to model the pressure difference caused by
- stack effect.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The model can be used with the following three configurations, which are
- controlled by the setting of the parameter <code>densitySelection</code>:
- </p>
- <ul>
- <li>
- <code>top</code>:
- Use this setting to use the density from the volume that is connected
- to <code>port_a</code>.
- </li>
- <li>
- <code>bottom</code>:
- Use this setting to use the density from the volume that is connected
- to <code>port_b</code>.
- </li>
- <li>
- <code>actual</code>:
- Use this setting to use the density based on the actual flow direction.
- </li>
- </ul>
- <p>
- The settings <code>top</code> and <code>bottom</code>
- should be used when rooms or different floors of a building are
- connected since multizone airflow models assume that each floor is completely mixed.
- For these two seetings, this model will compute the pressure between the center of the room
- and an opening that is at height <code>h</code> relative to the center of the room.
- The setting <code>actual</code> may be used to model a chimney in which
- a column of air will change its density based on the flow direction.
- </p>
- <p>
- In this model, the parameter <code>h</code> must always be positive, and the port <code>port_a</code> must be
- at the top of the column.
- </p>
- <h4>Dynamics</h4>
- <p>
- For a dynamic model, use
- <a href=\"modelica://AixLib.Airflow.Multizone.MediumColumnDynamic\">
- AixLib.Airflow.Multizone.MediumColumnDynamic</a> instead of this model.
- </p>
- </html>",
+<p>
+This model describes the pressure difference of a vertical medium
+column. It can be used to model the pressure difference caused by
+stack effect.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The model can be used with the following three configurations, which are
+controlled by the setting of the parameter <code>densitySelection</code>:
+</p>
+<ul>
+<li>
+<code>top</code>:
+Use this setting to use the density from the volume that is connected
+to <code>port_a</code>.
+</li>
+<li>
+<code>bottom</code>:
+Use this setting to use the density from the volume that is connected
+to <code>port_b</code>.
+</li>
+<li>
+<code>actual</code>:
+Use this setting to use the density based on the actual flow direction.
+</li>
+</ul>
+<p>
+The settings <code>top</code> and <code>bottom</code>
+should be used when rooms or different floors of a building are
+connected since multizone airflow models assume that each floor is completely mixed.
+For these two seetings, this model will compute the pressure between the center of the room
+and an opening that is at height <code>h</code> relative to the center of the room.
+The setting <code>actual</code> may be used to model a chimney in which
+a column of air will change its density based on the flow direction.
+</p>
+<p>
+In this model, the parameter <code>h</code> must always be positive, and the port <code>port_a</code> must be
+at the top of the column.
+</p>
+<h4>Dynamics</h4>
+<p>
+For a dynamic model, use
+<a href=\"modelica://AixLib.Airflow.Multizone.MediumColumnDynamic\">
+AixLib.Airflow.Multizone.MediumColumnDynamic</a> instead of this model.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- May 1, 2018, by Filip Jorissen:<br/>
- Removed declaration of <code>allowFlowReversal</code>
- and changed default density computation such
- that it assumes a constant pressure.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/877\">#877</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Removed start values for mass flow rate and pressure difference
- to simplify the parameter window.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- February 24, 2015 by Michael Wetter:<br/>
- Changed model to use
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.density_pTX\">
- AixLib.Utilities.Psychrometrics.Functions.density_pTX</a>
- for the density computation
- as
- <a href=\"modelica://AixLib.Media.Air.density\">
- AixLib.Media.Air.density</a>
- does not depend on temperature.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>October 4, 2014 by Michael Wetter:<br/>
- Removed assignment of <code>port_?.p.nominal</code> to avoid a warning in OpenModelica because
- alias sets have different nominal values.
- </li>
- <li>April 17, 2013 by Michael Wetter:<br/>
- Reformulated the assert statement that checks for the correct value of <code>densitySelection</code>.
- </li>
- <li>July 28, 2010 by Michael Wetter:<br/>
- Changed sign for pressure difference.
- </li>
- <li>
- July 20, 2010 by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- Reimplemented assignment of density based on flow direction or based on outflowing state.
- </li>
- <li>
- February 24, 2005 by Michael Wetter:<br/>
- Released first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+May 1, 2018, by Filip Jorissen:<br/>
+Removed declaration of <code>allowFlowReversal</code>
+and changed default density computation such
+that it assumes a constant pressure.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/877\">#877</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Removed start values for mass flow rate and pressure difference
+to simplify the parameter window.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+February 24, 2015 by Michael Wetter:<br/>
+Changed model to use
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.density_pTX\">
+AixLib.Utilities.Psychrometrics.Functions.density_pTX</a>
+for the density computation
+as
+<a href=\"modelica://AixLib.Media.Air.density\">
+AixLib.Media.Air.density</a>
+does not depend on temperature.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>October 4, 2014 by Michael Wetter:<br/>
+Removed assignment of <code>port_?.p.nominal</code> to avoid a warning in OpenModelica because
+alias sets have different nominal values.
+</li>
+<li>April 17, 2013 by Michael Wetter:<br/>
+Reformulated the assert statement that checks for the correct value of <code>densitySelection</code>.
+</li>
+<li>July 28, 2010 by Michael Wetter:<br/>
+Changed sign for pressure difference.
+</li>
+<li>
+July 20, 2010 by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+Reimplemented assignment of density based on flow direction or based on outflowing state.
+</li>
+<li>
+February 24, 2005 by Michael Wetter:<br/>
+Released first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MediumColumn;
diff --git a/AixLib/Airflow/Multizone/MediumColumnDynamic.mo b/AixLib/Airflow/Multizone/MediumColumnDynamic.mo
index 44031c441b..abd95dd94e 100644
--- a/AixLib/Airflow/Multizone/MediumColumnDynamic.mo
+++ b/AixLib/Airflow/Multizone/MediumColumnDynamic.mo
@@ -75,10 +75,10 @@ model MediumColumnDynamic
 
 equation
   connect(colBot.port_a, vol.ports[1]) annotation (Line(
-      points={{0,-40},{0,-40},{0,-2},{-10,-2}},
+      points={{0,-40},{0,-40},{0,-1},{-10,-1}},
       color={0,127,255}));
   connect(vol.ports[2], colTop.port_b) annotation (Line(
-      points={{-10,2},{0,2},{0,40},{0,40}},
+      points={{-10,1},{0,1},{0,40},{0,40}},
       color={0,127,255}));
   connect(colTop.port_a, port_a) annotation (Line(
       points={{0,60},{0,80},{0,80},{0,100}},
@@ -98,132 +98,118 @@ equation
         Text(
           extent={{24,-78},{106,-100}},
           textColor={0,0,127},
-          textString="Bottom"),
+          textString="Bottom",
+          fontSize=36),
         Text(
           extent={{32,104},{98,70}},
           textColor={0,0,127},
-          textString="Top"),
+          textString="Top",
+          fontSize=36),
         Text(
           extent={{42,26},{94,-10}},
           textColor={0,0,127},
           fillColor={255,0,0},
           fillPattern=FillPattern.Solid,
           textString="h=%h"),
-        Rectangle(
-          visible=densitySelection == AixLib.Airflow.Multizone.Types.densitySelection.fromTop,
-          extent={{-16,78},{16,-2}},
-          fillColor={85,170,255},
-          fillPattern=FillPattern.Solid,
-          pattern=LinePattern.None,
-          lineColor={0,0,0}),
         Text(
           extent={{-50.5,20.5},{50.5,-20.5}},
-          lineColor={0,0,127},
-          origin={-72.5,-12.5},
+          textColor={0,0,127},
+          origin={-72.5,-0.5},
           rotation=90,
           textString="%name"),
         Rectangle(
-          visible=densitySelection == AixLib.Airflow.Multizone.Types.densitySelection.actual,
-          extent={{-16,80},{16,54}},
-          fillColor={85,170,255},
-          fillPattern=FillPattern.Solid,
-          pattern=LinePattern.None,
-          lineColor={0,0,0}),
-        Rectangle(
-          visible=densitySelection == AixLib.Airflow.Multizone.Types.densitySelection.fromBottom,
-          extent={{-16,0},{16,-82}},
-          fillColor={85,170,255},
-          fillPattern=FillPattern.Solid,
-          pattern=LinePattern.None,
-          lineColor={0,0,0}),
-        Rectangle(
-          visible=densitySelection == AixLib.Airflow.Multizone.Types.densitySelection.actual,
-          extent={{-16,-55},{16,-80}},
+          extent={{-16,80},{16,-80}},
           fillColor={85,170,255},
           fillPattern=FillPattern.Solid,
           pattern=LinePattern.None,
           lineColor={0,0,0}),
         Ellipse(
           extent={{-40,40},{40,-40}},
-          lineColor={0,0,0},
           fillPattern=FillPattern.Sphere,
-          fillColor={0,128,255}),
+          fillColor={0,128,255},
+          pattern=LinePattern.None),
         Line(
           visible=use_HeatTransfer,
           points={{-90,0},{-40,0}},
           color={255,0,0})}),
 defaultComponentName="col",
 Documentation(info="<html>
- <p>
- This model contains a completely mixed fluid volume and
- models that take into account the pressure difference of
- a medium column that is at the same temperature as the
- fluid volume. It can be used to model the pressure difference
- caused by a stack effect.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- Set the parameter <code>use_HeatTransfer=true</code> to expose
- a <code>heatPort</code>. This <code>heatPort</code> can be used
- to add or subtract heat from the volume. This allows, for example,
- to use this model in conjunction with a model for heat transfer through
- walls to model a solar chimney that stores heat.
- </p>
- <h4>Dynamics</h4>
- <p>
- For a steady-state model, use
- <a href=\"modelica://AixLib.Airflow.Multizone.MediumColumn\">
- AixLib.Airflow.Multizone.MediumColumn</a> instead of this model.
- </p>
- <p>In this model, the parameter <code>h</code> must always be positive, and the port <code>port_a</code> must be
- at the top of the column.
- </p>
- </html>",
+<p>
+This model contains a completely mixed fluid volume and
+models that take into account the pressure difference of
+a medium column that is at the same temperature as the
+fluid volume. It can be used to model the pressure difference
+caused by a stack effect.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+Set the parameter <code>use_HeatTransfer=true</code> to expose
+a <code>heatPort</code>. This <code>heatPort</code> can be used
+to add or subtract heat from the volume. This allows, for example,
+to use this model in conjunction with a model for heat transfer through
+walls to model a solar chimney that stores heat.
+</p>
+<h4>Dynamics</h4>
+<p>
+For a steady-state model, use
+<a href=\"modelica://AixLib.Airflow.Multizone.MediumColumn\">
+AixLib.Airflow.Multizone.MediumColumn</a> instead of this model.
+</p>
+<p>In this model, the parameter <code>h</code> must always be positive, and the port <code>port_a</code> must be
+at the top of the column.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- January 8, 2019, by Michael Wetter:<br/>
- Changed public parameter <code>m_flow_nominal</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/970\">#970</a>.
- </li>
- <li>
- May 1, 2018, by Filip Jorissen:<br/>
- Removed declaration of <code>allowFlowReversal</code>
- and changed default density computation such
- that it assumes a constant pressure.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/877\">#877</a>.
- </li>
- <li>
- October 6, 2014 by Michael Wetter:<br/>
- Removed assignment of <code>port_?.p.nominal</code> to avoid a warning
- in OpenModelica because
- alias sets have different nominal values.
- </li>
- <li>
- July 31, 2011 by Michael Wetter:<br/>
- Changed model to use new base class
- <a href=\"modelica://AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
- AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
- </li>
- <li>May 25, 2011 by Michael Wetter:<br/>
- Added <code>m_flow_nominal</code>, which is used if component is configured as steady-state.
- </li>
- <li>July 28, 2010 by Michael Wetter:<br/>
- Released first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 27, 2024, by Michael Wetter:<br/>
+Removed wrong annotation that used a non-existent parameter.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1842\">#1842</a>.
+</li>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+January 8, 2019, by Michael Wetter:<br/>
+Changed public parameter <code>m_flow_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/970\">#970</a>.
+</li>
+<li>
+May 1, 2018, by Filip Jorissen:<br/>
+Removed declaration of <code>allowFlowReversal</code>
+and changed default density computation such
+that it assumes a constant pressure.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/877\">#877</a>.
+</li>
+<li>
+October 6, 2014 by Michael Wetter:<br/>
+Removed assignment of <code>port_?.p.nominal</code> to avoid a warning
+in OpenModelica because
+alias sets have different nominal values.
+</li>
+<li>
+July 31, 2011 by Michael Wetter:<br/>
+Changed model to use new base class
+<a href=\"modelica://AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
+AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
+</li>
+<li>May 25, 2011 by Michael Wetter:<br/>
+Added <code>m_flow_nominal</code>, which is used if component is configured as steady-state.
+</li>
+<li>July 28, 2010 by Michael Wetter:<br/>
+Released first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MediumColumnDynamic;
diff --git a/AixLib/Airflow/Multizone/Orifice.mo b/AixLib/Airflow/Multizone/Orifice.mo
index ed27f0261e..c0ffa74470 100644
--- a/AixLib/Airflow/Multizone/Orifice.mo
+++ b/AixLib/Airflow/Multizone/Orifice.mo
@@ -39,102 +39,102 @@ model Orifice "Orifice"
           textString="A=%A")}),
 defaultComponentName="ori",
 Documentation(info="<html>
- <p>
- This model describes the mass flow rate and pressure difference relation
- of an orifice in the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- V&#775; = C &Delta;p<sup>m</sup>,
- </p>
- <p>
- where
- <i>V&#775;</i> is the volume flow rate,
- <i>C</i> is a flow coefficient and
- <i>m</i> is the flow exponent.
- The flow coefficient is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- C = C<sub>D</sub> A (2/&rho;<sub>0</sub>)<sup>0.5</sup>,
- </p>
- <p>
- where
- <i>C<sub>D</sub></i> is the discharge coefficient,
- <i>A</i> is the cross section area and
- <i>&rho;<sub>0</sub></i> is the mass density at the medium default pressure, temperature and humidity.
- </p>
- <p>
- For turbulent flow, set <i>m=1/2</i> and
- for laminar flow, set <i>m=1</i>.
- Large openings are characterized by values close to <i>0.5</i>,
- while values near <i>0.65</i> have been found for small
- crack-like openings (Dols and Walton, 2002).
- </p>
- <h4>References</h4>
- <ul>
- <li>
- W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual,
- Multizone Airflow and Contaminant Transport Analysis Software</i>,
- Building and Fire Research Laboratory,
- National Institute of Standards and Technology,
- Tech. Report NISTIR 6921,
- November, 2002.
- </li>
- <li>Michael Wetter.
- <a href=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Wetter-airflow-2006.pdf\">Multizone Airflow Model in Modelica.</a>
- Proc. of the 5th International Modelica Conference, p. 431-440. Vienna, Austria, September 2006.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, by Klaas De Jonge:<br/>
- Changes due to changes in the baseclass, velocity is now a top-level variable.
- </li>
- <li>
- June 27, 2018, by Michael Wetter:<br/>
- Corrected old parameter annotation.
- </li>
- <li>
- June 24, 2018, by Michael Wetter:<br/>
- Removed parameter <code>lWet</code> as it is only used to compute
- the Reynolds number, and the Reynolds number is not used by this model.
- Also removed the variable <code>Re</code> for the Reynolds number.<br/>
- This change is non-backward compatible.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/932\">IBPSA, #932</a>.
- </li>
- <li>
- May 30, 2018, by Michael Wetter:<br/>
- Improved documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/546\">IBPSA, #546</a>.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Changed the parameter <code>useConstantDensity</code> to
- <code>useDefaultProperties</code> to use consistent names within this package.
- A conversion script can be used to update this parameter.
- </li>
- <li>
- December 6, 2011 by Michael Wetter:<br/>
- Replaced <code>rho</code> with <code>rho_nominal</code> because
- <code>rho</code> is computed in an <code>equation</code> section and not
- in the <code>initial equation</code> section.
- </li>
- <li>
- July 20, 2010 by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>
- February 4, 2005 by Michael Wetter:<br/>
- Released first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model describes the mass flow rate and pressure difference relation
+of an orifice in the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+V&#775; = C &Delta;p<sup>m</sup>,
+</p>
+<p>
+where
+<i>V&#775;</i> is the volume flow rate,
+<i>C</i> is a flow coefficient and
+<i>m</i> is the flow exponent.
+The flow coefficient is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+C = C<sub>D</sub> A (2/&rho;<sub>0</sub>)<sup>0.5</sup>,
+</p>
+<p>
+where
+<i>C<sub>D</sub></i> is the discharge coefficient,
+<i>A</i> is the cross section area and
+<i>&rho;<sub>0</sub></i> is the mass density at the medium default pressure, temperature and humidity.
+</p>
+<p>
+For turbulent flow, set <i>m=1/2</i> and
+for laminar flow, set <i>m=1</i>.
+Large openings are characterized by values close to <i>0.5</i>,
+while values near <i>0.65</i> have been found for small
+crack-like openings (Dols and Walton, 2002).
+</p>
+<h4>References</h4>
+<ul>
+<li>
+W. Stuart Dols and George N. Walton, <i>CONTAMW 2.0 User Manual,
+Multizone Airflow and Contaminant Transport Analysis Software</i>,
+Building and Fire Research Laboratory,
+National Institute of Standards and Technology,
+Tech. Report NISTIR 6921,
+November, 2002.
+</li>
+<li>Michael Wetter.
+<a href=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Wetter-airflow-2006.pdf\">Multizone Airflow Model in Modelica.</a>
+Proc. of the 5th International Modelica Conference, p. 431-440. Vienna, Austria, September 2006.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, by Klaas De Jonge:<br/>
+Changes due to changes in the baseclass, velocity is now a top-level variable.
+</li>
+<li>
+June 27, 2018, by Michael Wetter:<br/>
+Corrected old parameter annotation.
+</li>
+<li>
+June 24, 2018, by Michael Wetter:<br/>
+Removed parameter <code>lWet</code> as it is only used to compute
+the Reynolds number, and the Reynolds number is not used by this model.
+Also removed the variable <code>Re</code> for the Reynolds number.<br/>
+This change is non-backward compatible.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/932\">IBPSA, #932</a>.
+</li>
+<li>
+May 30, 2018, by Michael Wetter:<br/>
+Improved documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/546\">IBPSA, #546</a>.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Changed the parameter <code>useConstantDensity</code> to
+<code>useDefaultProperties</code> to use consistent names within this package.
+A conversion script can be used to update this parameter.
+</li>
+<li>
+December 6, 2011 by Michael Wetter:<br/>
+Replaced <code>rho</code> with <code>rho_nominal</code> because
+<code>rho</code> is computed in an <code>equation</code> section and not
+in the <code>initial equation</code> section.
+</li>
+<li>
+July 20, 2010 by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>
+February 4, 2005 by Michael Wetter:<br/>
+Released first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Orifice;
diff --git a/AixLib/Airflow/Multizone/Point_m_flow.mo b/AixLib/Airflow/Multizone/Point_m_flow.mo
index 07901daa92..03169cf054 100644
--- a/AixLib/Airflow/Multizone/Point_m_flow.mo
+++ b/AixLib/Airflow/Multizone/Point_m_flow.mo
@@ -50,36 +50,36 @@ annotation (
           fillPattern=FillPattern.Solid)}),
     defaultComponentName="pow",
     Documentation(info="<html>
- <p>
- Model that fits the flow coefficient of the massflow version of the
- orifice equation based on 1 datapoint of mass flow rate and pressure difference, and given flow exponent.
- </p>
- <p>
- A similar model is also used in the CONTAM software (Dols and Walton, 2015).
- </p>
- <p>
- <b>References</b>
- </p>
- <ul>
- <li>
- <b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
- National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>
- "),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that fits the flow coefficient of the massflow version of the
+orifice equation based on 1 datapoint of mass flow rate and pressure difference, and given flow exponent.
+</p>
+<p>
+A similar model is also used in the CONTAM software (Dols and Walton, 2015).
+</p>
+<p>
+<b>References</b>
+</p>
+<ul>
+<li>
+<b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
+National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Point_m_flow;
diff --git a/AixLib/Airflow/Multizone/Points_m_flow.mo b/AixLib/Airflow/Multizone/Points_m_flow.mo
index 6fea62a4c0..e68cd4d51a 100644
--- a/AixLib/Airflow/Multizone/Points_m_flow.mo
+++ b/AixLib/Airflow/Multizone/Points_m_flow.mo
@@ -54,35 +54,35 @@ protected
           fillPattern=FillPattern.Solid)}),
     defaultComponentName="pow",
     Documentation(info="<html>
- <p>
- Model that fits the flow coefficient of the massflow version of the
- orifice equation based on 2 datapoints of mass flow rate and pressure difference.
- </p>
- <p>
- A similar model is also used in the CONTAM software (Dols and Walton, 2015).
- </p>
- <p><b>References</b></p>
- <ul>
- <li>
- <b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>.
- <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
- National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>
- "),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that fits the flow coefficient of the massflow version of the
+orifice equation based on 2 datapoints of mass flow rate and pressure difference.
+</p>
+<p>
+A similar model is also used in the CONTAM software (Dols and Walton, 2015).
+</p>
+<p><b>References</b></p>
+<ul>
+<li>
+<b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>.
+<i>CONTAM User Guide and Program Documentation Version 3.2</i>,
+National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi: <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Points_m_flow;
diff --git a/AixLib/Airflow/Multizone/Table_V_flow.mo b/AixLib/Airflow/Multizone/Table_V_flow.mo
index bdd84c917b..62998dfb15 100644
--- a/AixLib/Airflow/Multizone/Table_V_flow.mo
+++ b/AixLib/Airflow/Multizone/Table_V_flow.mo
@@ -15,49 +15,49 @@ initial equation
   annotation (
     defaultComponentName="tabDat",
     Documentation(info="<html>
- <p>
- This model describes the one-directional pressure driven air flow through an
- opening based on user-provided tabular data describing the relation between volume flow rate
- and pressure difference over the component.
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- V&#775; = f(&Delta;p),
- </p>
- <p>
- where <i>V&#775;</i> is the volume flow rate and
- <i>&Delta;p</i> is the pressure difference.
- <p>
- Based on the table input, a cubic hermite spline is constructed between all points
- except for the two last pairs of points. These point are connected linearly.
- </p>
- <p>
- The constructed curve is the direct relation between <i>V&#775;</i> and <i>&Delta;p</i>.
- </p>
- <p>
- A similar model is also used in the CONTAM software (Dols and Walton, 2015).
- </p>
- <h4>References</h4>
- <ul>
- <li>
- <b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
- National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi:
- <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>
- "),Icon(graphics={
+<p>
+This model describes the one-directional pressure driven air flow through an
+opening based on user-provided tabular data describing the relation between volume flow rate
+and pressure difference over the component.
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+V&#775; = f(&Delta;p),
+</p>
+<p>
+where <i>V&#775;</i> is the volume flow rate and
+<i>&Delta;p</i> is the pressure difference.
+<p>
+Based on the table input, a cubic hermite spline is constructed between all points
+except for the two last pairs of points. These point are connected linearly.
+</p>
+<p>
+The constructed curve is the direct relation between <i>V&#775;</i> and <i>&Delta;p</i>.
+</p>
+<p>
+A similar model is also used in the CONTAM software (Dols and Walton, 2015).
+</p>
+<h4>References</h4>
+<ul>
+<li>
+<b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
+National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi:
+<a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>
+"), Icon(graphics={
         Rectangle(
           extent={{-48,80},{52,-80}},
           lineColor={0,0,255},
@@ -97,6 +97,6 @@ initial equation
           lineColor={28,108,200},
           fillColor={255,255,255},
           fillPattern=FillPattern.Forward),
-        Line(points={{2,78},{2,-78}}, color={28,108,200})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        Line(points={{2,78},{2,-78}}, color={28,108,200})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Table_V_flow;
diff --git a/AixLib/Airflow/Multizone/Table_m_flow.mo b/AixLib/Airflow/Multizone/Table_m_flow.mo
index 40ebf622c2..21268d8eb3 100644
--- a/AixLib/Airflow/Multizone/Table_m_flow.mo
+++ b/AixLib/Airflow/Multizone/Table_m_flow.mo
@@ -2,7 +2,7 @@ within AixLib.Airflow.Multizone;
 model Table_m_flow
   "Mass flow(y-axis) vs Pressure(x-axis) cubic spline fit model based from table data, with last two points linearly interpolated"
   extends AixLib.Airflow.Multizone.BaseClasses.PartialOneWayFlowElement(
-    m_flow = AixLib.Airflow.Multizone.BaseClasses.interpolate(
+    m_flow = AixLib.Utilities.Math.Functions.interpolate(
       u=dp,
       xd=dpMea_nominal,
       yd=mMea_flow_nominal,
@@ -69,48 +69,48 @@ initial equation
         Line(points={{0,78},{0,-78}}, color={28,108,200})}),
     defaultComponentName="tabDat",
     Documentation(info="<html>
- <p>
- This model describes the one-directional pressure driven air flow through an
- opening based on user-provided tabular data describing the relation between mass flow rate
- and pressure difference over the component.
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- m&#775; = f(&Delta;p),
- </p>
- <p>
- where <i>m&#775;</i> is the volume flow rate and
- <i>&Delta;p</i> is the pressure difference.
- <p>
- Based on the table input, a cubic hermite spline is constructed between all points
- except for the two last pairs of points. These point are connected linearly.
- </p>
- <p>
- The constructed curve is the direct relation between <i>m&#775;</i> and <i>&Delta;p</i>.
- </p>
- <p>
- A similar model is also used in the CONTAM software (Dols and Walton, 2015).
- </p>
- <h4>References</h4>
- <ul>
- <li>
- <b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
- National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi:
- <a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>
- "),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model describes the one-directional pressure driven air flow through an
+opening based on user-provided tabular data describing the relation between mass flow rate
+and pressure difference over the component.
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+m&#775; = f(&Delta;p),
+</p>
+<p>
+where <i>m&#775;</i> is the volume flow rate and
+<i>&Delta;p</i> is the pressure difference.
+<p>
+Based on the table input, a cubic hermite spline is constructed between all points
+except for the two last pairs of points. These point are connected linearly.
+</p>
+<p>
+The constructed curve is the direct relation between <i>m&#775;</i> and <i>&Delta;p</i>.
+</p>
+<p>
+A similar model is also used in the CONTAM software (Dols and Walton, 2015).
+</p>
+<h4>References</h4>
+<ul>
+<li>
+<b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
+National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi:
+<a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Table_m_flow;
diff --git a/AixLib/Airflow/Multizone/Types/densitySelection.mo b/AixLib/Airflow/Multizone/Types/densitySelection.mo
index 7803d0dd7d..1482d92e13 100644
--- a/AixLib/Airflow/Multizone/Types/densitySelection.mo
+++ b/AixLib/Airflow/Multizone/Types/densitySelection.mo
@@ -5,26 +5,26 @@ type densitySelection = enumeration(
     actual "Actual density based on flow direction")
   "Enumeration to select density in medium column" annotation (
     Documentation(info="<html>
- <p>
- Enumeration to define the choice of valve flow coefficient
- (to be selected via choices menu):
- </p>
- <table border=\"1\" summary=\"Explanation of the enumeration\">
- <tr><th>Enumeration</th>
-     <th>Description</th></tr>
- <tr><td>fromTop</td>
-     <td>
- Use this setting to use the density from the volume that is connected
- to the top port.
-     </td></tr>
- <tr><td>fromBottom</td>
-     <td>
- Use this setting to use the density from the volume that is connected
- to the bottom port.
- </td></tr>
- <tr><td>actual</td>
-     <td>Use this setting to use the density based on the actual flow direction.
- </td></tr>
-  </table>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Enumeration to define the choice of valve flow coefficient
+(to be selected via choices menu):
+</p>
+<table border=\"1\" summary=\"Explanation of the enumeration\">
+<tr><th>Enumeration</th>
+    <th>Description</th></tr>
+<tr><td>fromTop</td>
+    <td>
+Use this setting to use the density from the volume that is connected
+to the top port.
+    </td></tr>
+<tr><td>fromBottom</td>
+    <td>
+Use this setting to use the density from the volume that is connected
+to the bottom port.
+</td></tr>
+<tr><td>actual</td>
+    <td>Use this setting to use the density based on the actual flow direction.
+</td></tr>
+ </table>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Airflow/Multizone/Validation/DoorOpenClosed.mo b/AixLib/Airflow/Multizone/Validation/DoorOpenClosed.mo
index 021b459819..57ea135944 100644
--- a/AixLib/Airflow/Multizone/Validation/DoorOpenClosed.mo
+++ b/AixLib/Airflow/Multizone/Validation/DoorOpenClosed.mo
@@ -102,30 +102,30 @@ equation
       StopTime=1,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This model validates the door model that takes as an input a signal
- that determines whether the door is open or closed.
- In this validation, the instance <code>dooOpeClo</code> is either open or closed,
- depending on its input signal <code>y</code>.
- If the door is open, its air flow rate is identical to the air flow rate of the
- instance <code>doo</code>.
- If the door is closed, its air flow rate is identical to the air flow rate of the
- instance <code>lea</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2021 by Michael Wetter:<br/>
- Updated comments for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
- </li>
- <li>
- October 12, 2020 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model validates the door model that takes as an input a signal
+that determines whether the door is open or closed.
+In this validation, the instance <code>dooOpeClo</code> is either open or closed,
+depending on its input signal <code>y</code>.
+If the door is open, its air flow rate is identical to the air flow rate of the
+instance <code>doo</code>.
+If the door is closed, its air flow rate is identical to the air flow rate of the
+instance <code>lea</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2021 by Michael Wetter:<br/>
+Updated comments for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/515\">IBPSA, #515</a>.
+</li>
+<li>
+October 12, 2020 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(extent={{-100,-100},{100,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{80,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{80,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DoorOpenClosed;
diff --git a/AixLib/Airflow/Multizone/Validation/OneWayFlow.mo b/AixLib/Airflow/Multizone/Validation/OneWayFlow.mo
index c26bab5797..3301a2b9c2 100644
--- a/AixLib/Airflow/Multizone/Validation/OneWayFlow.mo
+++ b/AixLib/Airflow/Multizone/Validation/OneWayFlow.mo
@@ -220,19 +220,19 @@ equation
       __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Validation/OneWayFlow.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>
- "),Icon(coordinateSystem(extent={{-100,-100},{100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>
+"), Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end OneWayFlow;
diff --git a/AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyDynamic.mo b/AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyDynamic.mo
index 66d7f55444..dfbf0f8498 100644
--- a/AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyDynamic.mo
+++ b/AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyDynamic.mo
@@ -96,17 +96,17 @@ equation
       StopTime=14400,
       Tolerance=1e-08),
     Documentation(info="<html>
- <p>
- This model validates the door model for the situation where there is only buoyancy-driven air flow.
- Initially the volume is at a different temperature than the pressure source, leading to an airflow that eventually decays to zero.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 9, 2020 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates the door model for the situation where there is only buoyancy-driven air flow.
+Initially the volume is at a different temperature than the pressure source, leading to an airflow that eventually decays to zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 9, 2020 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OpenDoorBuoyancyDynamic;
diff --git a/AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyPressureDynamic.mo b/AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyPressureDynamic.mo
index 6ac2f7f534..4d1556c5ba 100644
--- a/AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyPressureDynamic.mo
+++ b/AixLib/Airflow/Multizone/Validation/OpenDoorBuoyancyPressureDynamic.mo
@@ -95,17 +95,17 @@ equation
       StopTime=14400,
       Tolerance=1e-08),
     Documentation(info="<html>
- <p>
- This model validates the door model for the situation where there is air flow due to buoyancy and static pressure difference.
- Initially the volumes are at a different temperatures and pressure, leading to an airflow that eventually decays to zero.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 9, 2020 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates the door model for the situation where there is air flow due to buoyancy and static pressure difference.
+Initially the volumes are at a different temperatures and pressure, leading to an airflow that eventually decays to zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 9, 2020 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OpenDoorBuoyancyPressureDynamic;
diff --git a/AixLib/Airflow/Multizone/Validation/OpenDoorPressure.mo b/AixLib/Airflow/Multizone/Validation/OpenDoorPressure.mo
index 1de03b4a55..15c075f228 100644
--- a/AixLib/Airflow/Multizone/Validation/OpenDoorPressure.mo
+++ b/AixLib/Airflow/Multizone/Validation/OpenDoorPressure.mo
@@ -82,16 +82,16 @@ equation
       Interval=600,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This model validates the door model for the situation where there is only pressure-driven air flow.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 9, 2020 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates the door model for the situation where there is only pressure-driven air flow.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 9, 2020 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OpenDoorPressure;
diff --git a/AixLib/Airflow/Multizone/Validation/OpenDoorTemperature.mo b/AixLib/Airflow/Multizone/Validation/OpenDoorTemperature.mo
index 947402fb15..49fcb6e5b2 100644
--- a/AixLib/Airflow/Multizone/Validation/OpenDoorTemperature.mo
+++ b/AixLib/Airflow/Multizone/Validation/OpenDoorTemperature.mo
@@ -80,16 +80,16 @@ equation
       Interval=600,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This model validates the door model for the situation where there is only temperature-driven air flow.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 9, 2020 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates the door model for the situation where there is only temperature-driven air flow.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 9, 2020 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OpenDoorTemperature;
diff --git a/AixLib/Airflow/Multizone/Validation/ThreeRoomsContam.mo b/AixLib/Airflow/Multizone/Validation/ThreeRoomsContam.mo
index 4ea3340309..fa6ba40efc 100644
--- a/AixLib/Airflow/Multizone/Validation/ThreeRoomsContam.mo
+++ b/AixLib/Airflow/Multizone/Validation/ThreeRoomsContam.mo
@@ -244,54 +244,54 @@ experiment(Tolerance=1e-06, StopTime=3600),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Validation/ThreeRoomsContam.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This is a model of three rooms that exchange air among each based
- on density difference between the air in the rooms and the outside.
- The model implements the configuration shown below.</p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Examples/3roomValidation.png\" border=\"1\" alt=\"Configuration of the three rooms.\"/>
- </p>
- <p>
- For the model that has been used for a comparative model validation between CONTAM and
- the <code>Buildings</code> library in Wetter (2006), see
- <a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContamDiscretizedDoor\">
- AixLib.Airflow.Multizone.Validation.ThreeRoomsContamDiscretizedDoor</a>.
- </p>
- <h4>References</h4>
- <p>
- Michael Wetter.
- <a href=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Wetter-airflow-2006.pdf\">
- Multizone Airflow Model in Modelica.</a>
- Proc. of the 5th International Modelica Conference, p. 431-440. Vienna, Austria, September 2006.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 9, 2020, by Michael Wetter:<br/>
- Refactored model to use the new door model.
- </li>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- June 26, 2014, by Michael Wetter:<br/>
- Set the initial conditions to be fixed to avoid a translation warning.
- This required adding a heat conductor between each volume and its prescribed
- temperature in order to avoid an overdetermined system of equations.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a model of three rooms that exchange air among each based
+on density difference between the air in the rooms and the outside.
+The model implements the configuration shown below.</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Examples/3roomValidation.png\" border=\"1\" alt=\"Configuration of the three rooms.\"/>
+</p>
+<p>
+For the model that has been used for a comparative model validation between CONTAM and
+the <code>Buildings</code> library in Wetter (2006), see
+<a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContamDiscretizedDoor\">
+AixLib.Airflow.Multizone.Validation.ThreeRoomsContamDiscretizedDoor</a>.
+</p>
+<h4>References</h4>
+<p>
+Michael Wetter.
+<a href=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Wetter-airflow-2006.pdf\">
+Multizone Airflow Model in Modelica.</a>
+Proc. of the 5th International Modelica Conference, p. 431-440. Vienna, Austria, September 2006.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 9, 2020, by Michael Wetter:<br/>
+Refactored model to use the new door model.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+June 26, 2014, by Michael Wetter:<br/>
+Set the initial conditions to be fixed to avoid a translation warning.
+This required adding a heat conductor between each volume and its prescribed
+temperature in order to avoid an overdetermined system of equations.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeRoomsContam;
diff --git a/AixLib/Airflow/Multizone/Validation/ThreeRoomsContamDiscretizedDoor.mo b/AixLib/Airflow/Multizone/Validation/ThreeRoomsContamDiscretizedDoor.mo
index db64495195..8080938646 100644
--- a/AixLib/Airflow/Multizone/Validation/ThreeRoomsContamDiscretizedDoor.mo
+++ b/AixLib/Airflow/Multizone/Validation/ThreeRoomsContamDiscretizedDoor.mo
@@ -27,54 +27,54 @@ experiment(Tolerance=1e-06, StopTime=3600),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Validation/ThreeRoomsContamDiscretizedDoor.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model is identical to
- <a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
- AixLib.Airflow.Multizone.Validation.ThreeRoomsContam</a>
- except that it uses a different door model.
- </p>
- <p>
- This model has been used for a comparative model validation between CONTAM and
- the <code>Buildings</code> library.
- See Wetter (2006) for details of the validation.
- </p>
- <h4>References</h4>
- <p>
- Michael Wetter.
- <a href=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Wetter-airflow-2006.pdf\">
- Multizone Airflow Model in Modelica.</a>
- Proc. of the 5th International Modelica Conference, p. 431-440. Vienna, Austria, September 2006.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 9, 2020, by Michael Wetter:<br/>
- Refactored model to use the base class
- <a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
- AixLib.Airflow.Multizone.Validation.ThreeRoomsContam</a>.
- </li>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- June 26, 2014, by Michael Wetter:<br/>
- Set the initial conditions to be fixed to avoid a translation warning.
- This required adding a heat conductor between each volume and its prescribed
- temperature in order to avoid an overdetermined system of equations.
- </li>
- <li>
- November 10, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model is identical to
+<a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
+AixLib.Airflow.Multizone.Validation.ThreeRoomsContam</a>
+except that it uses a different door model.
+</p>
+<p>
+This model has been used for a comparative model validation between CONTAM and
+the <code>Buildings</code> library.
+See Wetter (2006) for details of the validation.
+</p>
+<h4>References</h4>
+<p>
+Michael Wetter.
+<a href=\"modelica://AixLib/Resources/Images/Airflow/Multizone/Wetter-airflow-2006.pdf\">
+Multizone Airflow Model in Modelica.</a>
+Proc. of the 5th International Modelica Conference, p. 431-440. Vienna, Austria, September 2006.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 9, 2020, by Michael Wetter:<br/>
+Refactored model to use the base class
+<a href=\"modelica://AixLib.Airflow.Multizone.Validation.ThreeRoomsContam\">
+AixLib.Airflow.Multizone.Validation.ThreeRoomsContam</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+June 26, 2014, by Michael Wetter:<br/>
+Set the initial conditions to be fixed to avoid a translation warning.
+This required adding a heat conductor between each volume and its prescribed
+temperature in order to avoid an overdetermined system of equations.
+</li>
+<li>
+November 10, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeRoomsContamDiscretizedDoor;
diff --git a/AixLib/Airflow/Multizone/ZonalFlow_ACS.mo b/AixLib/Airflow/Multizone/ZonalFlow_ACS.mo
index 1a7ccd3a76..4490f30277 100644
--- a/AixLib/Airflow/Multizone/ZonalFlow_ACS.mo
+++ b/AixLib/Airflow/Multizone/ZonalFlow_ACS.mo
@@ -48,45 +48,45 @@ equation
                "ACS = %ACS")}),
 defaultComponentName="floExc",
 Documentation(info="<html>
- <p>
- This model computes the air exchange between volumes.
- </p>
- <p>
- Input is the air change per seconds. The volume flow rate is computed as
- </p>
- <pre>
-   V_flow = ACS * V
- </pre>
- <p>
- where <code>ACS</code> is an input and the volume <code>V</code> is a parameter.
- </p>
- </html>",
+<p>
+This model computes the air exchange between volumes.
+</p>
+<p>
+Input is the air change per seconds. The volume flow rate is computed as
+</p>
+<pre>
+  V_flow = ACS * V
+</pre>
+<p>
+where <code>ACS</code> is an input and the volume <code>V</code> is a parameter.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 18, 2014, by Michael Wetter:<br/>
- Removed parameter <code>forceErrorControlOnFlow</code> as it was not used.
- Changed message of assert statement to avoid an error in OpenModelica.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Changed the parameter <code>useConstantDensity</code> to
- <code>useDefaultProperties</code> to use consistent names within this package.
- A conversion script can be used to update this parameter.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>
- July 20, 2010 by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>
- January 4, 2006 by Michael Wetter:<br/>
- Implemented first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+August 18, 2014, by Michael Wetter:<br/>
+Removed parameter <code>forceErrorControlOnFlow</code> as it was not used.
+Changed message of assert statement to avoid an error in OpenModelica.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Changed the parameter <code>useConstantDensity</code> to
+<code>useDefaultProperties</code> to use consistent names within this package.
+A conversion script can be used to update this parameter.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>
+July 20, 2010 by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>
+January 4, 2006 by Michael Wetter:<br/>
+Implemented first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ZonalFlow_ACS;
diff --git a/AixLib/Airflow/Multizone/ZonalFlow_m_flow.mo b/AixLib/Airflow/Multizone/ZonalFlow_m_flow.mo
index 0873f82a7d..da98e72a22 100644
--- a/AixLib/Airflow/Multizone/ZonalFlow_m_flow.mo
+++ b/AixLib/Airflow/Multizone/ZonalFlow_m_flow.mo
@@ -12,30 +12,30 @@ equation
 
   annotation (defaultComponentName="floExc",
 Documentation(info="<html>
- <p>
- This model computes the air exchange between volumes.
- </p>
- <p>
- Input is the mass flow rate from
- <code>port_a1</code> to <code>port_b1</code> and from
- <code>port_a2</code> to <code>port_b2</code>.
- </p>
- </html>",
+<p>
+This model computes the air exchange between volumes.
+</p>
+<p>
+Input is the mass flow rate from
+<code>port_a1</code> to <code>port_b1</code> and from
+<code>port_a2</code> to <code>port_b2</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 18, 2014, by Michael Wetter:<br/>
- Removed parameter <code>forceErrorControlOnFlow</code> as it was not used.
- </li>
- <li>
- July 20, 2010, by Michael Wetter:<br/>
- Migrated model to Modelica 3.1 and integrated it into the Buildings library.
- </li>
- <li>
- January 17, 2006, by Michael Wetter:<br/>
- Implemented first version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+August 18, 2014, by Michael Wetter:<br/>
+Removed parameter <code>forceErrorControlOnFlow</code> as it was not used.
+</li>
+<li>
+July 20, 2010, by Michael Wetter:<br/>
+Migrated model to Modelica 3.1 and integrated it into the Buildings library.
+</li>
+<li>
+January 17, 2006, by Michael Wetter:<br/>
+Implemented first version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ZonalFlow_m_flow;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/CoeffsSunshadingInstallationVDI2078.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/CoeffsSunshadingInstallationVDI2078.mo
new file mode 100644
index 0000000000..9ea5453d6d
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/CoeffsSunshadingInstallationVDI2078.mo
@@ -0,0 +1,25 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions;
+function CoeffsSunshadingInstallationVDI2078
+  "Calculate the sunshading coefficient based on its installation defined by VDI 2078"
+  extends Modelica.Icons.Function;
+  input AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078
+    typ "Sunshading type defined in VDI 2078";
+  output Real cof "Coefficient of sunshading";
+algorithm
+  cof := if typ == AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.NoSunshading
+     then 1.0 else if typ == AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.ExternalBlindsFront
+     then 0.9 else if typ == AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.ExternalBlindsOn
+     then 0.66 else if typ == AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.Awning
+     then 1 else if typ == AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.Screen
+     then 0.33 else 0;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function finds the sunshading coefficient according to the input sunshading type. Values are defined by VDI 2078.</p>
+</html>"));
+end CoeffsSunshadingInstallationVDI2078;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/AngleToWidth.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/AngleToWidth.mo
new file mode 100644
index 0000000000..3cd1cd2e17
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/AngleToWidth.mo
@@ -0,0 +1,24 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged;
+function AngleToWidth
+  "Conversion from the hinged opening angle to hinged opening width"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.Length lenAxs(min=0)
+    "Length of the hinged axis, the axis should be parallel to a window frame";
+  input Modelica.Units.SI.Length lenAxsToFrm(min=0)
+    "Distance from the hinged axis to the frame across the opening area";
+  input Modelica.Units.SI.Angle ang(min=0, max=Modelica.Constants.pi/2)
+    "Opening angle of window sash";
+  output Modelica.Units.SI.Length width(min=0) "Opening width of window sash";
+algorithm
+  width := 2*lenAxsToFrm*sin(ang/2);
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function converts the hinged opening angle to hinged opening width.</p>
+</html>"));
+end AngleToWidth;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/CoeffOpeningAreaDIN16798.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/CoeffOpeningAreaDIN16798.mo
new file mode 100644
index 0000000000..cebcc3ae36
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/CoeffOpeningAreaDIN16798.mo
@@ -0,0 +1,26 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged;
+function CoeffOpeningAreaDIN16798
+  "Coefficient for hinged opening area according to DIN CEN/TR 16798-8 (DIN SPEC 32739-8)"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.Angle ang(min=0, max=Modelica.Constants.pi/2)
+    "Window sash opening angle";
+  output Real cof "Coefficient";
+protected
+  Modelica.Units.NonSI.Angle_deg angDeg "Window sash opening angle in deg";
+algorithm
+  angDeg := Modelica.Units.Conversions.to_deg(ang);
+  assert(angDeg <= 90,
+    "The model only applies to a maximum tilt angle of 90°",
+    AssertionLevel.error);
+  cof := 2.6e-7*(angDeg^3) - 1.19e-4*(angDeg^2) + 1.86e-2*angDeg;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function calculates the coefficient for hinged opening area according to DIN CEN/TR 16798-8 (DIN SPEC 32739-8).</p>
+</html>"));
+end CoeffOpeningAreaDIN16798;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/EffectiveOpeningArea.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/EffectiveOpeningArea.mo
new file mode 100644
index 0000000000..2b6d4a08ee
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/EffectiveOpeningArea.mo
@@ -0,0 +1,22 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged;
+function EffectiveOpeningArea
+  "Calculation of the effective opening area"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.Area AClr(min=0) "Window clear opening area";
+  input Modelica.Units.SI.Area AEqv(min=0) "Window equivalent opening area";
+  input Modelica.Units.SI.Area AEqv90(min=0)
+    "Window equivalent opening area by 90° opening";
+  output Modelica.Units.SI.Area AEff(min=0) "Effective opening area";
+algorithm
+  AEff := AEqv/AEqv90*AClr;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function calculates the effective opening area.</p>
+</html>"));
+end EffectiveOpeningArea;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/EquivalentOpeningArea.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/EquivalentOpeningArea.mo
new file mode 100644
index 0000000000..89d854e551
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/EquivalentOpeningArea.mo
@@ -0,0 +1,24 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged;
+function EquivalentOpeningArea
+  "Calculation of the equivalent opening area"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.Area AClr(min=0) "Window clear opening area";
+  input Modelica.Units.SI.Area AGeo(min=0) "Window geometric opening area";
+  output Modelica.Units.SI.Area AEqv(min=0) "Equivalent opening area";
+algorithm
+  if (AClr<Modelica.Constants.eps) or (AGeo<Modelica.Constants.eps) then
+    AEqv := 0;
+  else
+    AEqv := (AClr^(-2) + AGeo^(-2))^(-0.5);
+  end if;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function calculates the equivalent opening area.</p>
+</html>"));
+end EquivalentOpeningArea;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/GeometricOpeningArea.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/GeometricOpeningArea.mo
new file mode 100644
index 0000000000..1c82188748
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/GeometricOpeningArea.mo
@@ -0,0 +1,26 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged;
+function GeometricOpeningArea
+  "Calculation of the geometric opening area"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.PartialOpeningArea;
+protected
+  Modelica.Units.SI.Angle ang=
+    AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.WidthToAngle(
+    lenAxs, lenAxsToFrm, width) "Hinged opening angle";
+  Modelica.Units.SI.Area A1 "Opening area of oppsite side";
+  Modelica.Units.SI.Area A2 "Opening area of profile side";
+algorithm
+  A1 := width*lenAxs;
+  A2 := 0.5*width*lenAxsToFrm*cos(ang/2);
+  A := A1 + 2*A2;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function calculates the geometric opening area.</p>
+</html>"));
+end GeometricOpeningArea;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/PartialOpeningArea.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/PartialOpeningArea.mo
new file mode 100644
index 0000000000..ed3fcd2902
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/PartialOpeningArea.mo
@@ -0,0 +1,21 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged;
+partial function PartialOpeningArea
+  "Calculation of hinged-opening area by rectangular windows, unspecified types"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.Length lenAxs(min=0)
+    "Length of the hinged axis, the axis should be parallel to a window frame";
+  input Modelica.Units.SI.Length lenAxsToFrm(min=0)
+    "Distance from the hinged axis to the frame across the opening area";
+  input Modelica.Units.SI.Length width(min=0) "Opening width of window sash";
+  output Modelica.Units.SI.Area A(min=0) "Opening area";
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This partial function defines the inputs and output of the function for opening area calculation.</p>
+</html>"));
+end PartialOpeningArea;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/ProjectiveOpeningArea.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/ProjectiveOpeningArea.mo
new file mode 100644
index 0000000000..775d1b940d
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/ProjectiveOpeningArea.mo
@@ -0,0 +1,26 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged;
+function ProjectiveOpeningArea
+  "Calculation of the projective opening area"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.PartialOpeningArea;
+protected
+  Modelica.Units.SI.Angle ang=
+    AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.WidthToAngle(
+    lenAxs, lenAxsToFrm, width) "Hinged opening angle";
+  Modelica.Units.SI.Area A1 "Projective opening of oppsite side";
+  Modelica.Units.SI.Area A2 "Projectvie opening of profile side";
+algorithm
+  A1 := lenAxs*lenAxsToFrm*(1 - cos(ang));
+  A2 := 0.5*lenAxsToFrm*sin(ang)*lenAxsToFrm*cos(ang);
+  A := A1 + 2*A2;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function calculates the projective opening area.</p>
+</html>"));
+end ProjectiveOpeningArea;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/WidthToAngle.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/WidthToAngle.mo
new file mode 100644
index 0000000000..0baa06b8f4
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/WidthToAngle.mo
@@ -0,0 +1,27 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged;
+function WidthToAngle
+  "Conversion from the hinged opening width to hinged opening angle"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.Length lenAxs(min=0)
+    "Length of the hinged axis, the axis should be parallel to a window frame";
+  input Modelica.Units.SI.Length lenAxsToFrm(min=0)
+    "Distance from the hinged axis to the frame across the opening area";
+  input Modelica.Units.SI.Length width(min=0) "Opening width of window sash";
+  output Modelica.Units.SI.Angle ang(min=0, max=Modelica.Constants.pi/2)
+    "Opening angle of window sash";
+algorithm
+  assert(width <= sqrt(2)*lenAxsToFrm,
+    "The opening angle should be less or equal than 90°",
+    AssertionLevel.error);
+  ang := 2*asin(width/(2*lenAxsToFrm));
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function converts the hinged opening width to hinged opening angle.</p>
+</html>"));
+end WidthToAngle;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/package.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/package.mo
new file mode 100644
index 0000000000..e461b85665
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/package.mo
@@ -0,0 +1,4 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions;
+package OpeningAreaHinged "Calculation of different hinged-opening areas by rectangular windows"
+extends Modelica.Icons.FunctionsPackage;
+end OpeningAreaHinged;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/package.order b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/package.order
new file mode 100644
index 0000000000..81290964f0
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/package.order
@@ -0,0 +1,8 @@
+AngleToWidth
+CoeffOpeningAreaDIN16798
+EffectiveOpeningArea
+EquivalentOpeningArea
+GeometricOpeningArea
+PartialOpeningArea
+ProjectiveOpeningArea
+WidthToAngle
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/SmallestAngleDifference.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/SmallestAngleDifference.mo
new file mode 100644
index 0000000000..2de002b71e
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/SmallestAngleDifference.mo
@@ -0,0 +1,42 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Functions;
+function SmallestAngleDifference
+  "Smallest difference between two angles around a point"
+  input AixLib.Airflow.WindowVentilation.BaseClasses.Types.SmallestAngleDifferenceTypes
+    typ=AixLib.Airflow.WindowVentilation.BaseClasses.Types.SmallestAngleDifferenceTypes.Range180;
+  input Modelica.Units.SI.Angle ang1 "Input angle";
+  input Modelica.Units.SI.Angle ang2=0 "Reference angle";
+  output Modelica.Units.SI.Angle angDif "Difference between two angels";
+algorithm
+  angDif := ang1 - ang2;
+  if typ == AixLib.Airflow.WindowVentilation.BaseClasses.Types.SmallestAngleDifferenceTypes.Range180 then
+    /*Convert difference to -180°...+180°*/
+    while angDif <= -Modelica.Constants.pi loop
+      angDif := angDif + 2*Modelica.Constants.pi;
+    end while;
+    while angDif > Modelica.Constants.pi loop
+      angDif := angDif - 2*Modelica.Constants.pi;
+    end while;
+  elseif typ == AixLib.Airflow.WindowVentilation.BaseClasses.Types.SmallestAngleDifferenceTypes.Range360 then
+    /*Convert difference to 0...360°*/
+    while angDif < 0 loop
+      angDif := angDif + 2*Modelica.Constants.pi;
+    end while;
+    while angDif >= 2*Modelica.Constants.pi loop
+      angDif := angDif - 2*Modelica.Constants.pi;
+    end while;
+  else
+    /*Exceptions*/
+    angDif := 0;
+  end if;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This function finds the smallest difference between two angles around a point.</p>
+<p>The difference is calculated as input angle &apos;ang1&apos; to the reference angle &apos;ang2&apos;, positive value shows a clockwise direction from input to reference, i.e. shows a counter-clockwise by measurement.</p>
+</html>"));
+end SmallestAngleDifference;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/package.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/package.mo
new file mode 100644
index 0000000000..5c8a93a2bd
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/package.mo
@@ -0,0 +1,4 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses;
+package Functions
+extends Modelica.Icons.FunctionsPackage;
+end Functions;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/package.order b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/package.order
new file mode 100644
index 0000000000..98acfee5de
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Functions/package.order
@@ -0,0 +1,3 @@
+CoeffsSunshadingInstallationVDI2078
+SmallestAngleDifference
+OpeningAreaHinged
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlow.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlow.mo
new file mode 100644
index 0000000000..f47ba404fb
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlow.mo
@@ -0,0 +1,66 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses;
+partial model PartialEmpiricalFlow
+  "Partial model for empirical expressions of ventilation flow rate"
+  parameter Modelica.Units.SI.Length winClrWidth(min=0)
+    "Width of the window clear opening";
+  parameter Modelica.Units.SI.Height winClrHeight(min=0)
+    "Height of the window clear opening";
+  final parameter Boolean use_opnWidth_in=openingArea.use_opnWidth_in
+    "Use input port for window sash opening";
+  Modelica.Blocks.Interfaces.RealInput opnWidth_in(
+    final quantity="Length", final unit="m", min=0) if use_opnWidth_in
+    "Conditional input port for window sash opening width"
+    annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=-90,
+        origin={0,120})));
+  Modelica.Blocks.Interfaces.RealOutput V_flow(
+    final quantity="VolumeFlowRate", final unit="m3/s", min=0)
+    "Ventilation flow rate"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  replaceable model OpeningArea =
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningArea
+    constrainedby
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningArea(
+      final winClrWidth=winClrWidth,
+      final winClrHeight=winClrHeight)
+    "Model for window opening area calculation"
+    annotation(choicesAllMatching=true);
+  OpeningArea openingArea "Model instance for window opening area calculation"
+    annotation (Placement(transformation(extent={{20,60},{40,80}})));
+  //Variables and parameters for assertion check
+  Real intRes
+    "Interim result used to check the if assertion is raised in root calculation";
+  Integer errCouIntRes(start=0) "Warning counter for interim result warnings";
+  parameter String varNameIntRes "Variable name of interim result";
+initial equation
+  errCouIntRes = 0;
+equation
+  // Assertion check
+  when intRes < Modelica.Constants.eps then
+    errCouIntRes = pre(errCouIntRes) + 1;
+  end when;
+  assert(intRes > Modelica.Constants.eps or errCouIntRes > 1,
+    "In " + getInstanceName() + ": The polynomial under the square root to 
+    calculate '" + varNameIntRes + "' is equal or less than 0, '" +
+    varNameIntRes + "' will be set to 0",
+    AssertionLevel.warning);
+  // Connection(s)
+  connect(opnWidth_in, openingArea.opnWidth_in) annotation (Line(
+      points={{0,120},{0,70},{18,70}},
+      color={0,0,127},
+      pattern=DynamicSelect(LinePattern.Dash, if use_opnWidth_in then
+          LinePattern.Solid else LinePattern.Dash)));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This partial model provides a base class of models that estimate ventilation volume flow.</p>
+</html>"));
+end PartialEmpiricalFlow;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlowStack.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlowStack.mo
new file mode 100644
index 0000000000..8d6d287d64
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlowStack.mo
@@ -0,0 +1,28 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses;
+partial model PartialEmpiricalFlowStack
+  "Partial model for empirical expressions with stack effect considered"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlow;
+  Modelica.Blocks.Interfaces.RealInput TRoom(
+    final unit="K", min=273, max=313)
+    "Room temperature, ranging from 0 to 40 °C"
+    annotation (Placement(transformation(extent={{-140,60},{-100,100}})));
+  Modelica.Blocks.Interfaces.RealInput TAmb(
+    final unit="K", min=243, max=323)
+    "Ambient temperature, ranging from -30 to 50 °C"
+    annotation (Placement(transformation(extent={{-140,20},{-100,60}})));
+protected
+  Modelica.Units.SI.TemperatureDifference dTRoomAmb = TRoom - TAmb
+    "Temperature difference between room and ambient";
+  Modelica.Units.SI.Temperature TAvg = (TRoom + TAmb)/2
+    "Average temperature of room and ambient";
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This partial model provides a base class of models that estimate ventilation volume flow. The model has indoor and ambient temperature input ports to account for the thermal stack effect.</p>
+</html>"));
+end PartialEmpiricalFlowStack;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlowStackWindIncidence.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlowStackWindIncidence.mo
new file mode 100644
index 0000000000..76cdfa860d
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialEmpiricalFlowStackWindIncidence.mo
@@ -0,0 +1,27 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses;
+partial model PartialEmpiricalFlowStackWindIncidence
+  "Partial model for empirical expressions with stack effect and wind incidence angle considered"
+  extends PartialEmpiricalFlowStack;
+  parameter Modelica.Units.SI.Angle aziRef(displayUnit="deg")=0
+    "Azimuth angle of the referece surface impacted by wind";
+  Modelica.Units.SI.Angle incAng(displayUnit="deg")
+    "Incidence angle of wind on reference surface";
+  Modelica.Blocks.Interfaces.RealInput winDir(
+    final unit="rad", displayUnit="deg", min=0, max=2*Modelica.Constants.pi)
+    "Local wind direction"
+    annotation (Placement(transformation(extent={{-140,-80},{-100,-40}})));
+protected
+  Modelica.Units.NonSI.Angle_deg incAngDeg "Incidence angle in degree";
+equation
+  incAngDeg = Modelica.Units.Conversions.to_deg(incAng);
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This partial model provides a base class of models that estimate ventilation volume flow. The model has a wind direction input port to account for the wind incidence.</p>
+</html>"));
+end PartialEmpiricalFlowStackWindIncidence;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/PartialOpeningArea.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialOpeningArea.mo
new file mode 100644
index 0000000000..cd029f2513
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialOpeningArea.mo
@@ -0,0 +1,59 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses;
+partial model PartialOpeningArea
+  "Calculation of window opening area, unspecified type"
+  extends Modelica.Blocks.Icons.Block;
+  parameter Modelica.Units.SI.Length winClrWidth(min=0)
+    "Width of the window clear opening";
+  parameter Modelica.Units.SI.Height winClrHeight(min=0)
+    "Height of the window clear opening";
+  parameter Boolean use_opnWidth_in=true
+    "Use input port for window sash opening width"
+    annotation(choices(checkBox=true));
+  parameter Modelica.Units.SI.Length prescribedOpnWidth(min=0)=0
+    "Fixed value of prescribed opening width"
+    annotation(Dialog(enable = not use_opnWidth_in));
+  final parameter Modelica.Units.SI.Area AClrOpn = winClrWidth*winClrHeight
+    "Window clear opening area";
+  Modelica.Blocks.Interfaces.RealInput opnWidth_in(
+    final quantity="Length", final unit="m", min=0) if use_opnWidth_in
+    "Conditional input port for window sash opening width"
+    annotation (Placement(transformation(extent={{-140,-20},{-100,20}})));
+  Modelica.Blocks.Interfaces.RealOutput A(
+    final quantity="Area", final unit="m2", min=0)
+    "Output port for window opening area, must be defined by extended model"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  Modelica.Blocks.Interfaces.RealOutput opnWidth_internal(final unit="m", min=0)
+    "Internal port to connect to opnWidth_in or prescribedOpnWidth";
+equation
+  connect(opnWidth_in, opnWidth_internal);
+  if not use_opnWidth_in then
+    opnWidth_internal = prescribedOpnWidth;
+  end if;
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-80,100},{80,-60}},
+          lineColor={0,0,0},
+          fillColor={175,175,175},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-78,98},{78,-58}},
+          lineColor={0,0,0},
+          fillColor={215,215,215},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-72,92},{72,-52}},
+          lineColor={0,0,0},
+          fillColor={175,175,175},
+          fillPattern=FillPattern.Solid)}),                      Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This partial model provides a base class of window opening area.</p>
+</html>"));
+end PartialOpeningArea;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/PartialOpeningAreaSash.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialOpeningAreaSash.mo
new file mode 100644
index 0000000000..608a0e40de
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/PartialOpeningAreaSash.mo
@@ -0,0 +1,122 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses;
+partial model PartialOpeningAreaSash
+  "Window opening area, sash opening"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningArea;
+  parameter AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes
+    opnTyp = AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward
+    "Window opening type";
+  /*Variables to describe the opening*/
+  Modelica.Units.SI.Angle opnAng(
+    min=0, max=Modelica.Constants.pi/2, displayUnit="deg")=
+    if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward
+      or opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungOutward)
+    then
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.WidthToAngle(
+        winClrHeight, winClrWidth, opnWidth_internal)
+    else if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward
+       or opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward)
+    then
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.WidthToAngle(
+        winClrWidth, winClrHeight, opnWidth_internal)
+    else if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical)
+    then
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.WidthToAngle(
+        winClrHeight, winClrWidth/2, opnWidth_internal)
+    else if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal)
+    then
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.WidthToAngle(
+        winClrWidth, winClrHeight/2, opnWidth_internal)
+    else 0 "Window sash opening angle";
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-70,90},{70,-50}},
+          lineColor={0,0,0},
+          fillColor={102,204,255},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points=DynamicSelect({{-70,90},{70,20},{-70,-50}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward
+              then {{-70,90},{70,20},{-70,-50}} else {{-70,90}}),
+          color={0,0,0},
+          thickness=0.5),
+        Line(
+          points=DynamicSelect({{-70,90},{70,20},{-70,-50}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungOutward
+              then {{-70,90},{70,20},{-70,-50}} else {{-70,90}}),
+          color={0,0,0},
+          thickness=0.5,
+          pattern=LinePattern.Dash),
+        Line(
+          points=DynamicSelect({{-70,90},{0,-50},{70,90}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward
+              then {{-70,90},{0,-50},{70,90}} else {{-70,90}}),
+          color={0,0,0},
+          pattern=LinePattern.Dash,
+          thickness=0.5),
+        Line(
+          points=DynamicSelect({{-70,-50},{0,90},{70,-50}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward
+              then {{-70,-50},{0,90},{70,-50}} else {{-70,-50}}),
+          color={0,0,0},
+          thickness=0.5),
+        Line(
+          points=DynamicSelect({{0,90},{70,20}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical or
+              opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal
+              then {{0,90},{70,20}} else {{0,90}}),
+          color={0,0,0},
+          thickness=0.5,
+          pattern=DynamicSelect(LinePattern.Solid,
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical
+              then LinePattern.Solid else LinePattern.Dash)),
+        Line(
+          points=DynamicSelect({{70,20},{0,-50}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical or
+              opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal
+              then {{70,20},{0,-50}} else {{70,20}}),
+          color={0,0,0},
+          thickness=0.5),
+        Line(
+          points=DynamicSelect({{0,-50},{-70,20}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical or
+              opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal
+              then {{0,-50},{-70,20}} else {{0,-50}}),
+          color={0,0,0},
+          thickness=0.5,
+          pattern=DynamicSelect(LinePattern.Dash,
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical
+              then LinePattern.Dash else LinePattern.Solid)),
+        Line(
+          points=DynamicSelect({{-70,20},{0,90}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical or
+              opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal
+              then {{-70,20},{0,90}} else {{-70,20}}),
+          color={0,0,0},
+          thickness=0.5,
+          pattern=LinePattern.Dash),
+        Line(
+          points=DynamicSelect({{0,40},{0,80}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingVertical
+              then {{0,40},{0,80}} else {{0,40}}),
+          color={0,0,0},
+          thickness=0.5,
+          arrow={Arrow.None,Arrow.Filled}),
+        Line(
+          points=DynamicSelect({{20,20},{60,20}},
+            if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingHorizontal
+              then {{20,20},{60,20}} else {{20,20}}),
+          color={0,0,0},
+          thickness=0.5,
+          arrow={Arrow.None,Arrow.Filled})}),
+          Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This partial model provides a base class of window sash opening area.</p>
+</html>"));
+end PartialOpeningAreaSash;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Types/OpeningAreaTypes.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/OpeningAreaTypes.mo
new file mode 100644
index 0000000000..2dc654a66c
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/OpeningAreaTypes.mo
@@ -0,0 +1,10 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Types;
+type OpeningAreaTypes = enumeration(
+    Geometric "Geometric opening area",
+    Projective "Projective opening area",
+    Equivalent "Equivalent opening area",
+    Effective "Effective opening area")
+    "Enumeration to define window opening area types" annotation (Documentation(
+      info="<html>
+<p>This enum defines window sash opening area types, used in <a href=\"modelica://AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashCommon.mo\">AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon</a>.</p>
+</html>"));
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Types/SmallestAngleDifferenceTypes.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/SmallestAngleDifferenceTypes.mo
new file mode 100644
index 0000000000..62bef360af
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/SmallestAngleDifferenceTypes.mo
@@ -0,0 +1,8 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Types;
+type SmallestAngleDifferenceTypes = enumeration(
+    Range180 "Result in the range of -180° to +180°",
+    Range360 "Result in the range of 0 to 360°")
+    "Enumeration to define smallest angle difference types for the function"
+  annotation (Documentation(info="<html>
+<p>This enum defines types of smallest angle difference, used in <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/Functions/SmallestAngleDifference.mo\">AixLib.Airflow.WindowVentilation.BaseClasses.Functions.SmallestAngleDifference</a>.</p>
+</html>"));
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Types/SunshadingInstallationTypesVDI2078.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/SunshadingInstallationTypesVDI2078.mo
new file mode 100644
index 0000000000..8d699c4d52
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/SunshadingInstallationTypesVDI2078.mo
@@ -0,0 +1,18 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Types;
+type SunshadingInstallationTypesVDI2078 = enumeration(
+    NoSunshading "Pivot-hung window without sunshading",
+    ExternalBlindsFront "Pivot-hung window with external venetian blinds > 0.4 m in front of the window",
+    ExternalBlindsOn "Pivot-hung window with external venetian blinds on the window",
+    Awning "Pivot-hung window with an awning",
+    Screen "Pivot-hung window with a screen on the window")
+  "Common installation situations of sunshading according to VDI 2078"
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This enum defines types of sunshading coefficient, used in <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/Functions/CoeffsSunshadingInstallationVDI2078.mo\">AixLib.Airflow.WindowVentilation.BaseClasses.Functions.CoeffsSunshadingInstallationVDI2078</a>.</p>
+</html>"));
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Types/WindowOpeningTypes.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/WindowOpeningTypes.mo
new file mode 100644
index 0000000000..78c07b9b21
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/WindowOpeningTypes.mo
@@ -0,0 +1,13 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses.Types;
+type WindowOpeningTypes = enumeration(
+    SideHungInward "Side-hung opening, inward (casement)",
+    SideHungOutward "Side-hung opening, outward (casement)",
+    TopHungOutward "Top-hung opening, outward (awning)",
+    BottomHungInward "Bottom-hung opening, inward (hopper, tilt)",
+    PivotVertical "Pivot vertical opening (centre hinge vertical)",
+    PivotHorizontal "Pivot horizontal opening (centre hinge horizontal)",
+    SlidingVertical "Sliding opening vertical (single-hung or double-hung)",
+    SlidingHorizontal "Sliding opening horizontal (slider)")
+    "Enumeration to define window opening types" annotation (Documentation(info="<html>
+<p>This enum defines window sash opening types, used in <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/PartialOpeningAreaSash.mo\">AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningAreaSash</a>.</p>
+</html>"));
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Types/package.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/package.mo
new file mode 100644
index 0000000000..d7e2259733
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/package.mo
@@ -0,0 +1,4 @@
+within AixLib.Airflow.WindowVentilation.BaseClasses;
+package Types
+extends Modelica.Icons.TypesPackage;
+end Types;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/Types/package.order b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/package.order
new file mode 100644
index 0000000000..f1c84307c9
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/Types/package.order
@@ -0,0 +1,4 @@
+OpeningAreaTypes
+SmallestAngleDifferenceTypes
+SunshadingInstallationTypesVDI2078
+WindowOpeningTypes
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/package.mo b/AixLib/Airflow/WindowVentilation/BaseClasses/package.mo
new file mode 100644
index 0000000000..4d4787ad9e
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/package.mo
@@ -0,0 +1,4 @@
+within AixLib.Airflow.WindowVentilation;
+package BaseClasses
+extends Modelica.Icons.BasesPackage;
+end BaseClasses;
diff --git a/AixLib/Airflow/WindowVentilation/BaseClasses/package.order b/AixLib/Airflow/WindowVentilation/BaseClasses/package.order
new file mode 100644
index 0000000000..152c50701b
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/BaseClasses/package.order
@@ -0,0 +1,7 @@
+PartialEmpiricalFlow
+PartialEmpiricalFlowStack
+PartialEmpiricalFlowStackWindIncidence
+PartialOpeningArea
+PartialOpeningAreaSash
+Functions
+Types
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/ASHRAE.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/ASHRAE.mo
new file mode 100644
index 0000000000..edb6a8de69
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/ASHRAE.mo
@@ -0,0 +1,46 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model ASHRAE "Empirical expression according to ASHRAE handbook (2009)"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStackWindIncidence(
+      redeclare replaceable model OpeningArea =
+        AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+      final varNameIntRes = "V_flow");
+  Modelica.Blocks.Interfaces.RealInput winSpeLoc(unit="m/s", min=0)
+    "Local wind speed by window or facade"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+protected
+  Real cofDcg = 0.4 + 0.0045*abs(dTRoomAmb) "Discharge coefficient";
+  Real cofWin = 0.55 - abs(incAngDeg)/180*0.25 "Coefficient of wind speed";
+  Modelica.Units.SI.Height dHeightNPL = openingArea.winClrHeight/2
+    "Height from midpoint of lower opening to the neutral pressure level: Value
+    of 'dHeightNPL' is difficult to estimate, if one window or door represents a
+    large fraction (approximately 90%) of the total opening area in the envelope,
+    then the NPL is at the mid-height of that aperture, and dHeightNPL equals
+    one-half the height of the aperture.";
+  Modelica.Units.SI.VolumeFlowRate V_flow_th "Thermal induced volume flow";
+  Modelica.Units.SI.VolumeFlowRate V_flow_win "Wind induced volume flow";
+equation
+  V_flow_win = cofWin*openingArea.A*winSpeLoc;
+  incAng = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.SmallestAngleDifference(
+    AixLib.Airflow.WindowVentilation.BaseClasses.Types.SmallestAngleDifferenceTypes.Range180,
+    aziRef, winDir);
+  V_flow_th = cofDcg*openingArea.A*sqrt(intRes);
+  intRes = 2*Modelica.Constants.g_n*dHeightNPL*abs(dTRoomAmb)/TRoom;
+  V_flow = sqrt(V_flow_th^2 + V_flow_win^2);
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression according to ASHRAE handbook.</p>
+<p>It is also applied in EnergyPlus as the object <i>ZoneVentilation:WindandStackOpenArea</i>.</p>
+<h4>References</h4>
+<p>ASHRAE. (2009). 2009 ASHRAE handbook: Fundamentals (SI ed.). American Society of Heating, Refrigeration and Air-Conditioning Engineers.</p>
+<p>U.S. Department of Energy. (2023). EnergyPlus Version 23.1.0 Documentation: Engineering Reference [Build: 87ed9199d4]. U.S. Department of Energy. </p>
+</html>"));
+end ASHRAE;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Caciolo.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Caciolo.mo
new file mode 100644
index 0000000000..f60b6952df
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Caciolo.mo
@@ -0,0 +1,62 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model Caciolo "Empirical expression developed by Caciolo et al. (2013)"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStackWindIncidence(
+      redeclare replaceable model OpeningArea =
+        AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+      final varNameIntRes = "V_flow_th");
+    Integer errCouWinSpeLoc(start=0)
+      "Warning counter for assertion check of 'winSpeLoc'";
+  Modelica.Blocks.Interfaces.RealInput winSpeLoc(unit="m/s", min=0)
+    "Local wind speed by window or facade"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+protected
+  Real cofDcg = 0.60 "Discharge coefficient";
+  Real cofWin "Coefficient of wind";
+  Modelica.Units.SI.Velocity winSpeLim = 1.23
+    "Lower bound of wind speed in windward conditions";
+  Modelica.Units.SI.VolumeFlowRate V_flow_th "Thermal induced volume flow";
+  Modelica.Units.SI.VolumeFlowRate V_flow_win "Wind induced volume flow";
+initial equation
+  errCouWinSpeLoc = 0;
+equation
+  incAng = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.SmallestAngleDifference(
+    AixLib.Airflow.WindowVentilation.BaseClasses.Types.SmallestAngleDifferenceTypes.Range180,
+    winDir, aziRef);
+  // Assertion of wind speed
+  when (winSpeLoc < winSpeLim) and abs(incAngDeg) <= 90 then
+    errCouWinSpeLoc = pre(errCouWinSpeLoc) + 1;
+  end when;
+  assert(winSpeLoc > winSpeLim or errCouWinSpeLoc > 1,
+    "In " + getInstanceName() + ": The wind speed in the windward condition 
+    is equal or less than the limitation (" + String(winSpeLim) + " m/s), the 
+    'V_flow_win' will be set to 0",
+    AssertionLevel.warning);
+  // Calculate V_flow_win
+  if abs(incAngDeg) <= 90 then
+    /*Windward*/
+    cofWin = 1.234 - 0.490*winSpeLoc + 0.048*(winSpeLoc^2);
+    V_flow_win =if noEvent(winSpeLoc > winSpeLim) then
+      0.0357*openingArea.A*(winSpeLoc - winSpeLim) else 0;
+  else
+    /*Leeward*/
+    cofWin = 1.355 - 0.179*winSpeLoc;
+    V_flow_win = 0;
+  end if;
+  intRes = Modelica.Constants.g_n*winClrHeight*dTRoomAmb*cofWin/TAvg;
+  V_flow_th = if noEvent(intRes > Modelica.Constants.eps) then
+    1/3*openingArea.A*cofDcg*sqrt(intRes) else 0;
+  V_flow = V_flow_th + V_flow_win;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression developed by Caciolo et al..</p>
+<h4>References</h4>
+<p>Caciolo, M., Cui, S., Stabat, P., &amp; Marchio, D. (2013). Development of a new correlation for single-sided natural ventilation adapted to leeward conditions. Energy and Buildings, 60, 372&ndash;382.</p>
+</html>"));
+end Caciolo;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/DIN16798.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/DIN16798.mo
new file mode 100644
index 0000000000..c147deb1e1
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/DIN16798.mo
@@ -0,0 +1,43 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model DIN16798 "Empirical expression according to DIN EN 16798-7 (2017)"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStack(
+      redeclare replaceable model OpeningArea =
+        AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashDIN16798,
+      final varNameIntRes = "V_flow");
+  parameter Modelica.Units.SI.Height heightASL=0 "Height above sea level";
+  Modelica.Blocks.Interfaces.RealInput winSpe10(unit="m/s", min=0)
+    "Local wind speed at a height of 10 m"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+protected
+  Real cofExt = min(1, max(0, (1 - 0.1*winSpe10)*((TAmb - T0)/25 + 0.2)))
+    "Coefficient depending on external conditions";
+  Real cofTh = 0.0035 "Coefficient of thermal buoyancy";
+  Real cofWin = 0.001 "Coefficient of wind speed";
+  Modelica.Units.SI.Temperature T0 = 273.15 "Temperature at 0 °C";
+  Modelica.Units.SI.Temperature TRef = 293 "Reference temperature";
+  Modelica.Units.SI.Density rhoRefASL0 = 1.204
+    "Reference dry air density, 293 K, 0 m above see level";
+  Modelica.Units.SI.Density rhoRefASL=
+    rhoRefASL0*(1 - 0.00651*heightASL/293)^4.255
+    "Air density, 293 K, by height above sea level";
+  Modelica.Units.SI.Density rhoAmbASL = TRef/TAmb*rhoRefASL
+    "Air density, by ambient temperature, by height above sea level";
+equation
+  intRes = max(cofWin*(winSpe10^2), cofTh*winClrHeight*abs(dTRoomAmb));
+  V_flow = rhoRefASL0/rhoAmbASL*cofExt*openingArea.A/2*sqrt(intRes);
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression according to DIN CEN/TR 16798-8 (DIN SPEC 32739-8):2018-03.</p>
+<h4>References</h4>
+<p>DIN Deutsches Institut f&uuml;r Normung e. V. (2018.03). Energieeffizienz von Geb&auml;uden &ndash; L&uuml;ftung von Geb&auml;uden &ndash; Teil 8: Interpretation der Anforderungen der EN 16798-7 &ndash; Berechnungsmethoden zur Bestimmung der Luftvolumenstr&ouml;me in Geb&auml;uden einschlie&szlig;lich Infiltration (Modul M5-5): Englische Fassung CEN/TR 16798-8:2017 (DIN CEN/TR 16798-8). Beuth Verlag GmbH.</p>
+</html>"));
+end DIN16798;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/DIN4108.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/DIN4108.mo
new file mode 100644
index 0000000000..c6ab09b1c6
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/DIN4108.mo
@@ -0,0 +1,36 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model DIN4108 "Empirical expression according to DIN/TS 4108-8 (2022)"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStack(
+      redeclare replaceable model OpeningArea =
+        AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashDIN4108,
+      final varNameIntRes = "V_flow_th");
+  Modelica.Blocks.Interfaces.RealInput winSpeLoc(unit="m/s", min=0)
+    "Local wind speed by window or facade"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+protected
+  Real cofDcg = 0.61 "Discharge coefficient";
+  Real cofWin = 0.05 "Coefficient of wind speed";
+  Modelica.Units.SI.VolumeFlowRate V_flow_th "Thermal induced volume flow";
+  Modelica.Units.SI.VolumeFlowRate V_flow_win "Wind induced volume flow";
+equation
+  intRes = Modelica.Constants.g_n*winClrHeight*dTRoomAmb/TAmb;
+  V_flow_th = if noEvent(intRes > Modelica.Constants.eps) then
+    1/3*cofDcg*openingArea.A*sqrt(intRes) else 0;
+  V_flow_win = cofWin*openingArea.A*winSpeLoc;
+  V_flow = sqrt(V_flow_th^2 + V_flow_win^2);
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression according to DIN/TS 4108-8:2022-09.</p>
+<h4>References</h4>
+<p>DIN Deutsches Institut f&uuml;r Normung e. V. (2022.09). W&auml;rmeschutz und Energie-Einsparung in Geb&auml;uden &ndash; Teil 8: Vermeidung von Schimmelwachstum in Wohngeb&auml;uden: Vornorm (DIN/TS 4108-8). Beuth Verlag GmbH.</p>
+</html>"));
+end DIN4108;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/GidsPhaff.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/GidsPhaff.mo
new file mode 100644
index 0000000000..731e1140b6
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/GidsPhaff.mo
@@ -0,0 +1,31 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model GidsPhaff "Empirical expression developed by de Gids and Phaff (1982)"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStack(
+      redeclare replaceable model OpeningArea =
+        AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+      final varNameIntRes = "V_flow");
+  Modelica.Blocks.Interfaces.RealInput winSpe10(unit="m/s", min=0)
+    "Local wind speed at a height of 10 m"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+protected
+  Real cof1 = 0.001 "Coefficient 1";
+  Real cof2 = 0.0035 "Coefficient 2";
+  Real cof3 = 0.01 "Coefficient 3";
+equation
+  intRes = cof1*(winSpe10^2) + cof2*winClrHeight*abs(dTRoomAmb) + cof3;
+  V_flow = if noEvent(intRes > Modelica.Constants.eps) then
+    1/2*openingArea.A*sqrt(intRes) else 0;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression developed by de Gids and Phaff.</p>
+<h4>References</h4>
+<p>Gids, W. de, &amp; Phaff, H. (1982). Ventilation rates and energy consumption due to open windows: a brief overview of research in the Netherlands. Air Infiltration Review, 4(1), 4&ndash;5.</p>
+</html>"));
+end GidsPhaff;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Hall.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Hall.mo
new file mode 100644
index 0000000000..eedd228fe9
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Hall.mo
@@ -0,0 +1,33 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model Hall "Empirical expression developed by Hall (2004)"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStack(
+      redeclare model OpeningArea =
+        AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashHall (
+        final sWinSas=sWinSas, final widthWinGap=widthWinGap),
+      final varNameIntRes = "V_flow");
+  parameter Modelica.Units.SI.Thickness sWinSas(min=0) = 0
+    "Window sash thickness (depth)";
+  parameter Modelica.Units.SI.Length widthWinGap(min=0) = 0.01
+    "Gap width in the overlap area between the frame and the sash";
+protected
+  Real cofDcg = 0.930*(openingArea.opnWidth_internal^0.2)
+    "Discharge coefficient, case: without window reveal, without radiator";
+equation
+  intRes = 2*Modelica.Constants.g_n*winClrHeight*openingArea.corNPL*dTRoomAmb/
+    TRoom;
+  V_flow = if noEvent(intRes > Modelica.Constants.eps) then
+    cofDcg*openingArea.A*sqrt(intRes) else 0;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression developed by Hall.</p>
+<h4>References</h4>
+<p>Hall, M. (2004). Untersuchungen zum thermisch induzierten Luftwechselpotential von Kippfenstern [Dissertation]. Universit&auml;t Kassel, Kassel. </p>
+</html>"));
+end Hall;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Jiang.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Jiang.mo
new file mode 100644
index 0000000000..248e5963ed
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Jiang.mo
@@ -0,0 +1,31 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model Jiang "Empirical expression developed by Jiang et al. (2022)"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlow(
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon (
+      final opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+      final opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Effective),
+    final varNameIntRes = "V_flow");
+  Modelica.Blocks.Interfaces.RealInput dp(unit="Pa")
+    "Pressure difference between the outside and inside of the facade "
+    annotation (Placement(transformation(extent={{-140,-20},{-100,20}})));
+protected
+  Real cof1 = 0.15 "Coefficient 1";
+  Real cof2 = 0.33 "Coefficient 2";
+equation
+  intRes = cof1*dp + cof2;
+  V_flow = if noEvent(intRes > Modelica.Constants.eps) then
+    1/2*openingArea.A*sqrt(intRes) else 0;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression developed by Jiang et al..</p>
+<h4>References</h4>
+<p>Jiang, J., Yang, J., Rewitz, K., &amp; M&uuml;ller, D. (2022). Experimental Quantification of Air Volume Flow by Natural Ventilation through Window Opening. In American Society of Heating and Air-Conditioning Engineers (Chair), IAQ 2020: Indoor Environmental Quality Performance Approaches, Athens.</p>
+</html>"));
+end Jiang;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/LarsenHeiselberg.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/LarsenHeiselberg.mo
new file mode 100644
index 0000000000..60f1298499
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/LarsenHeiselberg.mo
@@ -0,0 +1,78 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model LarsenHeiselberg "Empirical expression developed by Larsen and Heiselberg (2008)"
+  extends
+    AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStackWindIncidence(
+      redeclare replaceable model OpeningArea =
+        AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+      final varNameIntRes = "V_flow");
+  parameter Modelica.Units.SI.Velocity winSpeLim(min=0.25)=1
+    "Limitation of wind speed: Due to the wind speed in the denominator, this
+    expression is not applicable to low wind speeds, output with 0 if the wind
+    speed is less than this limit.";
+  Integer errCouWinSpe10(start=0)
+    "Warning counter for assertion check of 'winSpe10'";
+  Modelica.Blocks.Interfaces.RealInput winSpe10(unit="m/s", min=0)
+    "Local wind speed at a height of 10 m"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+protected
+  Real cofWinInc
+    "Coefficient of wind incidence, equivalent to C_beta*sqrt(abs(C_p)) in the equation";
+  Real dCofWinInc
+    "Correlation of coefficient of wind incidence, equivalent to deltaC_p";
+  Real cof1, cof2, cof3 "Other coefficients";
+initial equation
+  errCouWinSpe10 = 0;
+equation
+  incAng = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.SmallestAngleDifference(
+    AixLib.Airflow.WindowVentilation.BaseClasses.Types.SmallestAngleDifferenceTypes.Range360,
+    winDir, aziRef);
+  (cofWinInc,)  = Modelica.Math.Vectors.interpolate(
+    {0, 45, 90, 135, 180, 225, 270, 315, 360},
+    {0.2, 0.53, 0.56, 0.28, 0.09, 0.28, 0.56, 0.53, 0.2},
+    incAngDeg);
+  dCofWinInc = 9.1894e-9*(incAngDeg^3) - 2.626e-6*(incAngDeg^2) - 2.354e-4*incAngDeg + 0.113;
+  if incAngDeg>=285 or incAngDeg<=75 then
+    cof1 = 0.0015;
+    cof2 = 0.0009;
+    cof3 = -0.0005;
+  elseif incAngDeg>=105 and incAngDeg<=255 then
+    cof1 = 0.0050;
+    cof2 = 0.0009;
+    cof3 = 0.0160;
+  else
+    cof1 = 0.0010;
+    cof2 = 0.0005;
+    cof3 = 0.0111;
+  end if;
+  // Assertion of wind speed check
+  when winSpe10 < winSpeLim then
+    errCouWinSpe10 = pre(errCouWinSpe10) + 1;
+  end when;
+  assert(winSpe10 > winSpeLim or errCouWinSpe10 > 1,
+    "In " + getInstanceName() + ": The wind speed is equal or less than the
+    limited value (" + String(winSpeLim) + " m/s), the term of wind correlation 
+    will be set to 0",
+    AssertionLevel.warning);
+  // Calculate intRes
+  intRes =if noEvent(winSpe10 > winSpeLim)
+    then cof1*(cofWinInc^2)*(winSpe10^2) + cof2*dTRoomAmb*winClrHeight
+      + cof3*dCofWinInc*dTRoomAmb/(winSpe10^2)
+    else cof1*(cofWinInc^2)*(winSpe10^2) + cof2*dTRoomAmb*winClrHeight + 0;
+  // Calculate volume flow
+  V_flow = if noEvent(intRes > Modelica.Constants.eps) then
+    openingArea.A*sqrt(intRes) else 0;
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression developed by Larsen and Heiselberg.</p>
+<h4>References</h4>
+<p>Larsen, T. S., &amp; Heiselberg, P. (2008). Single-sided natural ventilation driven by wind pressure and temperature difference. Energy and Buildings, 40(6), 1031&ndash;1040.</p>
+</html>"));
+end LarsenHeiselberg;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Maas.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Maas.mo
new file mode 100644
index 0000000000..e9876c8786
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Maas.mo
@@ -0,0 +1,32 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model Maas "Empirical expression developed by Maas (1995)"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStack(
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon (
+      final opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+      final opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Effective),
+    final varNameIntRes = "V_flow");
+  Modelica.Blocks.Interfaces.RealInput winSpe13(unit="m/s", min=0)
+    "Local wind speed at a height of 13 m"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+protected
+  Real cof1 = 0.0056 "Coefficient 1";
+  Real cof2 = 0.0037 "Coefficient 2";
+  Real cof3 = 0.012 "Coefficient 3";
+equation
+  intRes = cof1*(winSpe13^2) + cof2*winClrHeight*dTRoomAmb + cof3;
+  V_flow = if noEvent(intRes > Modelica.Constants.eps) then
+    1/2*openingArea.A*sqrt(intRes) else 0;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression developed by Maas.</p>
+<h4>References</h4>
+<p>Maas, A. (1995). Experimentelle Quantifizierung des Luftwechsels bei Fensterl&uuml;ftung [Dissertation]. Universit&auml;t Gesamthochschule Kassel, Kassel. </p>
+</html>"));
+end Maas;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Tang.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Tang.mo
new file mode 100644
index 0000000000..f8faa6eba5
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/Tang.mo
@@ -0,0 +1,49 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model Tang "Empirical expression developed by Tang et al. (2016)"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStack(
+    redeclare replaceable model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+    final varNameIntRes = "V_flow");
+  parameter Modelica.Units.SI.TemperatureDifference dTLim(min=0.02)=0.05
+    "Limitation of temperature difference: Due to the temperature difference in
+    the denominator, this expression is not applicable to low temperature
+    difference, output with 0 if the absolute temperature difference is less
+    than this limit.";
+  Integer errCou_dT(start=0)
+    "Warning counter for assertion check of 'dT'";
+protected
+  Real cofDcg = 0.6 "Discharge coefficient";
+  Real cof_dT = 0.02 "Coefficient of temperature difference";
+initial equation
+  errCou_dT = 0;
+equation
+  // Assertion of temperature difference check
+  when abs(dTRoomAmb) < dTLim then
+    errCou_dT = pre(errCou_dT) + 1;
+  end when;
+  assert(abs(dTRoomAmb) > dTLim or errCou_dT > 1,
+    "In " + getInstanceName() + ": The temperature difference between indoor 
+    and ambient is equal or less than the limited value (" + String(dTLim) + " 
+    K), the term of temperature difference correlation will be set to 0",
+    AssertionLevel.warning);
+  // Calculate intRes
+  intRes = if noEvent(abs(dTRoomAmb) > dTLim)
+    then Modelica.Constants.g_n*winClrHeight*abs(dTRoomAmb)/TRoom + cof_dT/
+      abs(dTRoomAmb)
+    else Modelica.Constants.g_n*winClrHeight*abs(dTRoomAmb)/TRoom + 0;
+  // Calculate volume flow
+  V_flow = if noEvent(intRes > Modelica.Constants.eps) then
+    1/3*cofDcg*openingArea.A*sqrt(intRes) else 0;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression developed by Tang et al..</p>
+<h4>References</h4>
+<p>Tang, Y., Li, X., Zhu, W., &amp; Cheng, P. L. (2016). Predicting single-sided airflow rates based on primary school experimental study. Building and Environment, 98, 71&ndash;79. </p>
+</html>"));
+end Tang;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/VDI2078.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/VDI2078.mo
new file mode 100644
index 0000000000..eec4ee4118
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/VDI2078.mo
@@ -0,0 +1,45 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model VDI2078 "Empirical expression according to VDI 2078 (2015)"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStack(
+    redeclare replaceable model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashVDI2078,
+    final varNameIntRes = "V_flow");
+  parameter Boolean use_cofSunSha_in=false
+    "Use input port for sunshading coefficient"
+    annotation(choices(checkBox=true));
+  parameter
+    AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078
+    sunShaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.NoSunshading
+    "Sunshading type"
+    annotation (Dialog(enable=not use_cofSunSha_in));
+  Modelica.Blocks.Interfaces.RealInput cofSunSha_in(min=0, max=1) if use_cofSunSha_in
+    "Conditional input port for sunshading coefficient"
+    annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={0,-120})));
+  Modelica.Blocks.Interfaces.RealOutput cofSunSha_internal(min=0, max=1)
+    "Internal port to connect to cofSunSha_in or prescribed coefficient defined by type";
+equation
+  connect(cofSunSha_in, cofSunSha_internal);
+  if not use_cofSunSha_in then
+    cofSunSha_internal =
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.CoeffsSunshadingInstallationVDI2078(
+      sunShaTyp);
+  end if;
+  intRes = Modelica.Constants.g_n*openingArea.effHeight*dTRoomAmb/(2*TAmb);
+  V_flow =if noEvent(intRes > Modelica.Constants.eps) then cofSunSha_internal*
+    openingArea.A*sqrt(intRes) else 0;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression according to VDI 2078:2015-06.</p>
+<h4>References</h4>
+<p>Verein Deutscher Ingenieure e.V. (2015.06). Berechnung der thermischen Lasten und Raumtemperaturen (Auslegung K&uuml;hllast und Jahressimulation) (VDI 2078). VDI Fachmedien GmbH &amp; Co. KG.</p>
+</html>"));
+end VDI2078;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/WarrenParkins.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/WarrenParkins.mo
new file mode 100644
index 0000000000..97ac7467ff
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/WarrenParkins.mo
@@ -0,0 +1,32 @@
+within AixLib.Airflow.WindowVentilation.EmpiricalExpressions;
+model WarrenParkins "Empirical expression developed by Warren and Parkins (1984)"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialEmpiricalFlowStack(
+    redeclare replaceable model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+    final varNameIntRes = "V_flow_th");
+  Modelica.Blocks.Interfaces.RealInput winSpe10(unit="m/s", min=0)
+    "Local wind speed at a height of 10 m"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+protected
+  Real cofDcg = 0.61 "Discharge coefficient";
+  Modelica.Units.SI.VolumeFlowRate V_flow_th "Thermal induced volume flow";
+  Modelica.Units.SI.VolumeFlowRate V_flow_win "Wind induced volume flow";
+equation
+  intRes = Modelica.Constants.g_n*winClrHeight*dTRoomAmb/TAvg;
+  V_flow_th = if noEvent(intRes > Modelica.Constants.eps) then
+    1/3*cofDcg*openingArea.A*sqrt(intRes) else 0;
+  V_flow_win = 0.025*openingArea.A*winSpe10;
+  V_flow = max(V_flow_th, V_flow_win);
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model contains the empirical expression developed by Warren and Parkins.</p>
+<h4>References</h4>
+<p>Warren, P. R., &amp; Parkins, L. M. (1984). Single-sided ventilation through open windows. In Air infiltration and Ventilation Centre (Chair), Windows in building design and maintenance, Goteborg. </p>
+</html>"));
+end WarrenParkins;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/package.mo b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/package.mo
new file mode 100644
index 0000000000..a1e71232da
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/package.mo
@@ -0,0 +1,119 @@
+within AixLib.Airflow.WindowVentilation;
+package EmpiricalExpressions "Empirical expressions for calculation of the airflow"
+  extends Modelica.Icons.VariantsPackage;
+
+annotation (Documentation(info="<html>
+<p>This package contains different empirical expressions to estimate the air flow rate by single-sided window ventilation.</p>
+<p>The table below presents the applicable use cases for each expression.</p>
+<table cellspacing=\"0\" cellpadding=\"2\" border=\"1\" width=\"100%\"><tr>
+<td><p>Model</p></td>
+<td><p>Simple opening</p></td>
+<td><p>Side-hung opening</p></td>
+<td><p>Top- and Bottom-hung opening</p></td>
+<td><p>Pivot opening</p></td>
+<td><p>Sliding opening</p></td>
+</tr>
+<tr>
+<td><p>Gids and Phaff (1982)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+</tr>
+<tr>
+<td><p>Warren and Parkins (1984)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+</tr>
+<tr>
+<td><p>Maas (1995)</p></td>
+<td><p>N</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p>N</p></td>
+<td><p>N</p></td>
+</tr>
+<tr>
+<td><p>Hall (2004)</p></td>
+<td><p>N</p></td>
+<td><p>N</p></td>
+<td><p>Only bottom-hung, inward</p></td>
+<td><p>N</p></td>
+<td><p>N</p></td>
+</tr>
+<tr>
+<td><p>Larsen and Heiselberg (2008)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+</tr>
+<tr>
+<td><p>ASHRAE (2009)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+</tr>
+<tr>
+<td><p>Caciolo et al. (2013)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+</tr>
+<tr>
+<td><p>VDI 2078 (2015)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p>N</p></td>
+<td><p>Only bottom-hung, inward</p></td>
+<td><p>N</p></td>
+<td><p>N</p></td>
+</tr>
+<tr>
+<td><p>Tang et al. (2016)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+<td><p><span style=\"color: #1c6cc8;\">?</span></p></td>
+</tr>
+<tr>
+<td><p>DIN EN 16798-7 (2017)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p>N</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p>N</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+</tr>
+<tr>
+<td><p>Jiang et al. (2022)</p></td>
+<td><p>N</p></td>
+<td><p>N</p></td>
+<td><p>Only bottom-hung, inward</p></td>
+<td><p>N</p></td>
+<td><p>N</p></td>
+</tr>
+<tr>
+<td><p>DIN/TS 4108-8 (2022)</p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+<td><p><span style=\"color: #ee2e2f;\">Y</span></p></td>
+</tr>
+</table>
+<ul>
+<li><span style=\"color: #ee2e2f;\">Y</span> = Applicable</li>
+<li><span style=\"color: #1c6cc8;\">?</span> = Applicable without validation</li>
+<li>N = Not applicable</li>
+</ul>
+</html>"));
+end EmpiricalExpressions;
diff --git a/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/package.order b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/package.order
new file mode 100644
index 0000000000..8ddae865db
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/EmpiricalExpressions/package.order
@@ -0,0 +1,12 @@
+ASHRAE
+Caciolo
+DIN16798
+DIN4108
+GidsPhaff
+Hall
+Jiang
+LarsenHeiselberg
+Maas
+Tang
+VDI2078
+WarrenParkins
diff --git a/AixLib/Airflow/WindowVentilation/Examples/OpeningArea.mo b/AixLib/Airflow/WindowVentilation/Examples/OpeningArea.mo
new file mode 100644
index 0000000000..982423257b
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Examples/OpeningArea.mo
@@ -0,0 +1,441 @@
+within AixLib.Airflow.WindowVentilation.Examples;
+model OpeningArea "Calculation of different opening areas"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Length winClrWidth = 1.0 "Window clear width";
+  parameter Modelica.Units.SI.Height winClrHeight = 1.5 "Window clear height";
+  parameter Modelica.Units.SI.Thickness sWinSas = 0.08 "Window sash thickness";
+  Modelica.Blocks.Sources.Ramp opnWidthSet(
+    height=0.5,
+    duration=50,
+    startTime=5) "Window opening width set value"
+    annotation (Placement(transformation(extent={{-160,0},{-140,20}})));
+  Modelica.Blocks.Sources.Ramp opnAngSet(
+    height=30,
+    duration=50,
+    startTime=5) "Window opening angle set value"
+    annotation (Placement(transformation(extent={{-160,-160},{-140,-140}})));
+  Modelica.Blocks.Math.UnitConversions.From_deg from_deg
+    "Convert from deg to rad"
+    annotation (Placement(transformation(extent={{-100,-160},{-80,-140}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple opnSimp(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight) "Simple opening without sash"
+    annotation (Placement(transformation(extent={{-80,120},{-60,140}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimpleVDI2078 opnSimpVDI2078(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight) "Simple opening without sash, VDI 2078"
+    annotation (Placement(transformation(extent={{-40,120},{-20,140}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasSdHunInGeo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric)
+    "Side-hung, inward, geometric opening"
+    annotation (Placement(transformation(extent={{-80,60},{-60,80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasSdHunInPrj(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Projective)
+    "Side-hung, inward, projective opening"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasSdHunInEqv(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Equivalent)
+    "Side-hung, inward, equivalent opening"
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasSdHunInEff(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Effective)
+    "Side-hung, inward, effective opening"
+    annotation (Placement(transformation(extent={{-80,-60},{-60,-40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasSdHunOutGeo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungOutward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric)
+    "Side-hung, outward, geometric opening"
+    annotation (Placement(transformation(extent={{-40,60},{-20,80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasBtmHunInGeo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric)
+    "Bottom-hung, inward, geometric opening"
+    annotation (Placement(transformation(extent={{0,60},{20,80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasBtmHunInPrj(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Projective)
+    "Bottom-hung, inward, projective opening"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasBtmHunInEqv(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Equivalent)
+    "Bottom-hung, inward, equivalent opening"
+    annotation (Placement(transformation(extent={{0,-20},{20,0}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasBtmHunInEff(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Effective)
+    "Bottom-hung, inward, effective opening"
+    annotation (Placement(transformation(extent={{0,-60},{20,-40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasTopHunOutPrj(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Projective)
+    "Top-hung, outward, projective opening"
+    annotation (Placement(transformation(extent={{-40,20},{-20,40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivVerGeo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric)
+    "Pivot, vertical, geometric opening"
+    annotation (Placement(transformation(extent={{40,60},{60,80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivVerPrj(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Projective)
+    "Pivot, vertical, projective opening"
+    annotation (Placement(transformation(extent={{40,20},{60,40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivVerEqv(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Equivalent)
+    "Pivot, vertical, equivalent opening"
+    annotation (Placement(transformation(extent={{40,-20},{60,0}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivVerEff(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Effective)
+    "Pivot, vertical, effective opening"
+    annotation (Placement(transformation(extent={{40,-60},{60,-40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivHorGeo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric)
+    "Pivot, horizontal, geometric opening"
+    annotation (Placement(transformation(extent={{80,60},{100,80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivHorPrj(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Projective)
+    "Pivot, horizontal, projective opening"
+    annotation (Placement(transformation(extent={{80,20},{100,40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivHorEqv(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Equivalent)
+    "Pivot, horizontal, equivalent opening"
+    annotation (Placement(transformation(extent={{80,-20},{100,0}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivHorEff(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Effective)
+    "Pivot, horizontal, effective opening"
+    annotation (Placement(transformation(extent={{80,-60},{100,-40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasPivHorEffPre(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    use_opnWidth_in=false,
+    prescribedOpnWidth=0.5,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Effective)
+    "Pivot, horizontal, effective opening, prescribed input"
+    annotation (Placement(transformation(extent={{120,-60},{140,-40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasSldVerGeo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingVertical,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric)
+    "Sliding, vertical, geometric opening"
+    annotation (Placement(transformation(extent={{-40,-20},{-20,0}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasSldHorGeo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingHorizontal,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric)
+    "Sliding, horizontal, geometric opening"
+    annotation (Placement(transformation(extent={{-40,-60},{-20,-40}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashDIN16798 opnSasBtmHunInDIN16798(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward)
+    "Bottom-hung, inward, DIN 16798"
+    annotation (Placement(transformation(extent={{-80,-100},{-60,-80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashDIN4108 opnSasSdHunInDIN4108(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward)
+    "Side-hung, inward, DIN 4108"
+    annotation (Placement(transformation(extent={{-40,-100},{-20,-80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashDIN4108 opnSasBtmHunInDIN4108(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward)
+    "Bottom-hung, inward, DIN 4108"
+    annotation (Placement(transformation(extent={{0,-100},{20,-80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashDIN4108 opnSasPivHorDIN4108(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal,
+    sWinSas=sWinSas) "Pivot, horizontal, DIN 4108"
+    annotation (Placement(transformation(extent={{40,-100},{60,-80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashHall opnSasBtmHunInHall(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    sWinSas=sWinSas) "Bottom-hung, inward, Hall"
+    annotation (Placement(transformation(extent={{80,-100},{100,-80}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashVDI2078 opnSasBtmHunInVDI2078(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    sWinSas=sWinSas) "Bottom-hung, inward, VDI2078"
+    annotation (Placement(transformation(extent={{120,-100},{140,-80}})));
+  AixLib.Airflow.WindowVentilation.Utilities.AngleToWidth angToWidth(lenAxs=opnSasAngBtmHunInGeo.lenAxs,
+      lenAxsToFrm=opnSasAngBtmHunInGeo.lenAxsToFrm)
+    "Convert opening angle to opening width"
+    annotation (Placement(transformation(extent={{-60,-160},{-40,-140}})));
+  AixLib.Airflow.WindowVentilation.Utilities.WidthToAngle widthToAng(lenAxs=opnSasAngBtmHunInGeo.lenAxs,
+      lenAxsToFrm=opnSasAngBtmHunInGeo.lenAxsToFrm)
+    "Convert opening width to opening angle"
+    annotation (Placement(transformation(extent={{-20,-140},{0,-120}})));
+  AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon opnSasAngBtmHunInGeo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+    opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric)
+    "Input of angle, bottom-hung, inward, geometric opening"
+    annotation (Placement(transformation(extent={{20,-160},{40,-140}})));
+
+equation
+  connect(opnWidthSet.y, opnSasSdHunInGeo.opnWidth_in) annotation (Line(points={{-139,10},
+          {-90,10},{-90,70},{-82,70}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasSdHunInPrj.opnWidth_in) annotation (Line(points={{-139,10},
+          {-90,10},{-90,30},{-82,30}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasSdHunInEqv.opnWidth_in) annotation (Line(points={{-139,10},
+          {-90,10},{-90,-10},{-82,-10}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasSdHunInEff.opnWidth_in) annotation (Line(points={{-139,10},
+          {-90,10},{-90,-50},{-82,-50}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasSdHunOutGeo.opnWidth_in) annotation (Line(points={{-139,10},
+          {-50,10},{-50,70},{-42,70}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasBtmHunInGeo.opnWidth_in) annotation (Line(points={{-139,10},
+          {-10,10},{-10,70},{-2,70}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasBtmHunInPrj.opnWidth_in) annotation (Line(points={{-139,10},
+          {-10,10},{-10,30},{-2,30}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasBtmHunInEqv.opnWidth_in) annotation (Line(points={{-139,10},
+          {-10,10},{-10,-10},{-2,-10}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasBtmHunInEff.opnWidth_in) annotation (Line(points={{-139,10},
+          {-10,10},{-10,-50},{-2,-50}},           color={0,0,127}));
+  connect(opnWidthSet.y, opnSasTopHunOutPrj.opnWidth_in) annotation (Line(
+        points={{-139,10},{-50,10},{-50,30},{-42,30}}, color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivVerGeo.opnWidth_in) annotation (Line(points={{-139,10},
+          {30,10},{30,70},{38,70}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivVerPrj.opnWidth_in) annotation (Line(points={{-139,10},
+          {30,10},{30,30},{38,30}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivVerEqv.opnWidth_in) annotation (Line(points={{-139,10},
+          {30,10},{30,-10},{38,-10}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivVerEff.opnWidth_in) annotation (Line(points={{-139,10},
+          {30,10},{30,-50},{38,-50}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivHorGeo.opnWidth_in) annotation (Line(points={{-139,10},
+          {70,10},{70,70},{78,70}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivHorPrj.opnWidth_in) annotation (Line(points={{-139,10},
+          {70,10},{70,30},{78,30}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivHorEqv.opnWidth_in) annotation (Line(points={{-139,10},
+          {70,10},{70,-10},{78,-10}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivHorEff.opnWidth_in) annotation (Line(points={{-139,10},
+          {70,10},{70,-50},{78,-50}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasSldVerGeo.opnWidth_in) annotation (Line(points={{-139,10},
+          {-50,10},{-50,-10},{-42,-10}},          color={0,0,127}));
+  connect(opnWidthSet.y, opnSasSldHorGeo.opnWidth_in) annotation (Line(points={{-139,10},
+          {-50,10},{-50,-50},{-42,-50}},          color={0,0,127}));
+  connect(opnAngSet.y, from_deg.u) annotation (Line(points={{-139,-150},{-102,-150}},
+                                color={0,0,127}));
+  connect(opnWidthSet.y, opnSasBtmHunInDIN16798.opnWidth_in) annotation (Line(
+        points={{-139,10},{-90,10},{-90,-90},{-82,-90}}, color={0,0,127}));
+  connect(opnWidthSet.y, opnSasSdHunInDIN4108.opnWidth_in) annotation (Line(
+        points={{-139,10},{-90,10},{-90,-70},{-50,-70},{-50,-90},{-42,-90}},
+        color={0,0,127}));
+  connect(opnWidthSet.y, opnSasBtmHunInDIN4108.opnWidth_in) annotation (Line(
+        points={{-139,10},{-90,10},{-90,-70},{-10,-70},{-10,-90},{-2,-90}},
+        color={0,0,127}));
+  connect(opnWidthSet.y, opnSasPivHorDIN4108.opnWidth_in) annotation (Line(
+        points={{-139,10},{-90,10},{-90,-70},{30,-70},{30,-90},{38,-90}},
+        color={0,0,127}));
+  connect(opnWidthSet.y, opnSasBtmHunInHall.opnWidth_in) annotation (Line(
+        points={{-139,10},{-90,10},{-90,-70},{70,-70},{70,-90},{78,-90}}, color=
+         {0,0,127}));
+  connect(opnWidthSet.y, opnSasBtmHunInVDI2078.opnWidth_in) annotation (Line(
+        points={{-139,10},{-90,10},{-90,-70},{110,-70},{110,-90},{118,-90}},
+                                                                          color=
+         {0,0,127}));
+  connect(from_deg.y, angToWidth.u)
+    annotation (Line(points={{-79,-150},{-62,-150}},
+                                                   color={0,0,127}));
+  connect(angToWidth.y, opnSasAngBtmHunInGeo.opnWidth_in)
+    annotation (Line(points={{-39,-150},{18,-150}},
+                                                  color={0,0,127}));
+  connect(angToWidth.y, widthToAng.u) annotation (Line(points={{-39,-150},{-30,-150},
+          {-30,-130},{-22,-130}},
+                                color={0,0,127}));
+  annotation (experiment(
+      StartTime=0,
+      StopTime=60,
+      Interval=1,
+      Tolerance=1e-06,
+      __Dymola_Algorithm="Dassl"), Diagram(coordinateSystem(extent={{-160,-160},
+            {160,160}}),                   graphics={
+        Rectangle(
+          extent={{-100,100},{-60,-60}},
+          lineColor={28,108,200},
+          fillColor={0,140,72},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-100,100},{-60,80}},
+          textColor={255,255,255},
+          textString="Side-hung
+inward"),
+        Rectangle(
+          extent={{-60,100},{-20,60}},
+          lineColor={28,108,200},
+          fillColor={28,108,200},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-60,100},{-20,80}},
+          textColor={255,255,255},
+          textString="Side-hung
+outward"),
+        Text(
+          extent={{-140,80},{-100,60}},
+          textColor={0,0,0},
+          fontSize=16,
+          textString="geo."),
+        Text(
+          extent={{-140,40},{-100,20}},
+          textColor={0,0,0},
+          fontSize=16,
+          textString="prj."),
+        Text(
+          extent={{-140,0},{-100,-20}},
+          textColor={0,0,0},
+          fontSize=16,
+          textString="eqv."),
+        Text(
+          extent={{-140,-40},{-100,-60}},
+          textColor={0,0,0},
+          textString="eff.",
+          fontSize=16),
+        Rectangle(
+          extent={{-20,100},{20,-60}},
+          lineColor={28,108,200},
+          fillColor={217,67,180},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-20,100},{20,80}},
+          textColor={255,255,255},
+          textString="Bottom-hung
+inward"),
+        Rectangle(
+          extent={{-60,60},{-20,20}},
+          lineColor={28,108,200},
+          fillColor={162,29,33},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-60,60},{-20,40}},
+          textColor={255,255,255},
+          textString="Top-hung
+outward"),
+        Rectangle(
+          extent={{20,100},{60,-60}},
+          lineColor={28,108,200},
+          fillColor={244,125,35},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{20,100},{60,80}},
+          textColor={255,255,255},
+          textString="Pivot
+vertical"),
+        Rectangle(
+          extent={{60,100},{100,-60}},
+          lineColor={28,108,200},
+          fillColor={102,44,145},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{60,100},{100,80}},
+          textColor={255,255,255},
+          textString="Pivot
+horizontal"),
+        Rectangle(
+          extent={{-60,20},{-20,-20}},
+          lineColor={28,108,200},
+          fillColor={238,46,47},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-60,20},{-20,0}},
+          textColor={255,255,255},
+          textString="Sliding
+vertical"),
+        Rectangle(
+          extent={{-60,-20},{-20,-60}},
+          lineColor={28,108,200},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-60,-20},{-20,-40}},
+          textColor={255,255,255},
+          textString="Sliding
+horizontal"),
+        Text(
+          extent={{-140,-80},{-100,-100}},
+          textColor={0,0,0},
+          fontSize=15,
+          textString="others"),
+        Text(
+          extent={{-160,160},{0,140}},
+          textColor={0,0,0},
+          fontSize=14,
+          textString="Simple opening",
+          horizontalAlignment=TextAlignment.Left),
+        Text(
+          extent={{-160,120},{0,100}},
+          textColor={0,0,0},
+          fontSize=13,
+          horizontalAlignment=TextAlignment.Left,
+          textString="Sash opening (input opening width)"),
+        Text(
+          extent={{-160,-100},{0,-120}},
+          textColor={0,0,0},
+          fontSize=12,
+          horizontalAlignment=TextAlignment.Left,
+          textString="Sash opening (input opening angle)")}),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This example simulates and checks the models in package <a href=\"modelica://AixLib/Airflow/WindowVentilation/OpeningAreas/package.mo\">OpeningAreas</a>, calculating the window opening area with variable opening width or angle.</p>
+<p>The icon of the model changes itself automatically to indicate the type of window opening that is now being set.</p>
+</html>"),
+    __Dymola_Commands(file=
+          "Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/OpeningArea.mos"
+        "Simulate and plot"));
+end OpeningArea;
diff --git a/AixLib/Airflow/WindowVentilation/Examples/VentilationFlowRateSashOpening.mo b/AixLib/Airflow/WindowVentilation/Examples/VentilationFlowRateSashOpening.mo
new file mode 100644
index 0000000000..4c9bbbbf36
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Examples/VentilationFlowRateSashOpening.mo
@@ -0,0 +1,299 @@
+within AixLib.Airflow.WindowVentilation.Examples;
+model VentilationFlowRateSashOpening
+  "Use different empirical expressions to determine the window ventilation flow rate by sash opening"
+  extends Modelica.Icons.Example;
+  /*Parameters for boundary conditions*/
+  parameter Modelica.Units.SI.Length winClrWidth(min=0)=1.0
+    "Width of the window clear opening";
+  parameter Modelica.Units.SI.Height winClrHeight(min=0)=1.8
+    "Height of the window clear opening";
+  parameter Modelica.Units.SI.Angle aziRef(displayUnit="deg")=0
+    "Azimuth angle of the referece surface impacted by wind";
+  parameter Modelica.Units.SI.Height locHeight(min=0)=4
+    "Middle local height of the ventilation zone";
+  Modelica.Blocks.Sources.Ramp TRoomSet(
+    height=15,
+    duration=120,
+    offset=15,
+    startTime=50) "Set room temperature in °C"
+    annotation (Placement(transformation(extent={{-100,80},{-80,100}})));
+  Modelica.Blocks.Math.UnitConversions.From_degC from_degC "Convert degC to K"
+    annotation (Placement(transformation(extent={{-60,80},{-40,100}})));
+  Modelica.Blocks.Sources.Ramp TAmbSet(
+    height=-40,
+    duration=160,
+    offset=40,
+    startTime=10) "Set ambient temperature in °C"
+    annotation (Placement(transformation(extent={{-100,50},{-80,70}})));
+  Modelica.Blocks.Math.UnitConversions.From_degC from_degC1 "Convert degC to K"
+    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
+  Modelica.Blocks.Sources.TimeTable winSpe10Set(table=[0,0; 20,0; 30,5; 40,0; 50,
+        10; 60,0; 70,20; 80,0; 100,0; 110,20; 120,0; 130,10; 140,0; 150,5; 160,0;
+        180,0]) "Set wind speed at the height of 10 m"
+    annotation (Placement(transformation(extent={{-100,20},{-80,40}})));
+  Modelica.Blocks.Sources.Sine winDirSet(amplitude=2*Modelica.Constants.pi, f=0.05)
+    "Set wind direction"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.WarrenParkins warrenParkins(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon (
+        opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+        opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric))
+        "Model Warren Parkins"
+    annotation (Placement(transformation(extent={{20,80},{40,100}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.GidsPhaff gidsPhaff(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon (
+        opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+        opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric))
+      "Model de Gids Phaff"
+    annotation (Placement(transformation(extent={{20,40},{40,60}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.LarsenHeiselberg larsenHeiselberg(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon (
+        opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+        opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric),
+    aziRef=aziRef) "Model Larsen Heiselberg"
+    annotation (Placement(transformation(extent={{20,0},{40,20}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.Caciolo caciolo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon (
+        opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+        opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric),
+    aziRef=aziRef) "Model Caciolo"
+    annotation (Placement(transformation(extent={{20,-40},{40,-20}})));
+  AixLib.Airflow.WindowVentilation.Utilities.WindProfilePowerLaw winSpeProLoc(
+    height=locHeight, heightRef=10)
+    "Calculate wind speed profile local"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.Tang tang(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon (
+        opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+        opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric))
+    "Model Tang"
+    annotation (Placement(transformation(extent={{20,-80},{40,-60}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.VDI2078 vdi2078_1(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashVDI2078,
+    sunShaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.NoSunshading)
+    "Model VDI 2078, without sun shading"
+    annotation (Placement(transformation(extent={{60,60},{80,80}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.VDI2078 vdi2078_2(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashVDI2078 (
+        use_opnWidth_in=false, prescribedOpnWidth=0.1),
+    sunShaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.ExternalBlindsOn)
+    "Model VDI 2078, with sun shading"
+    annotation (Placement(transformation(extent={{60,40},{80,60}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.VDI2078 vdi2078_3(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashVDI2078 (
+        use_opnWidth_in=false, prescribedOpnWidth=0.1),
+    use_cofSunSha_in=true) "Model VDI 2078, with sun shading input"
+    annotation (Placement(transformation(extent={{60,20},{80,40}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.DIN16798 din16798_1(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashDIN16798 (
+        opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward),
+    heightASL=200) "Model DIN 16798"
+    annotation (Placement(transformation(extent={{60,-20},{80,0}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.DIN4108 din4108_1(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashDIN4108 (
+        opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward))
+    "Model DIN 4108"
+    annotation (Placement(transformation(extent={{60,-60},{80,-40}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.ASHRAE ashrae(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSashCommon (
+        opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+        opnAreaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric),
+    aziRef=aziRef) "Model ASHRAE"
+    annotation (Placement(transformation(extent={{60,-100},{80,-80}})));
+  Modelica.Blocks.Sources.Pulse cofSunShaSet(
+    amplitude=0.5,
+    period=10,
+    offset=0.5) "Set sunshading coefficient"
+    annotation (Placement(transformation(extent={{50,10},{60,20}})));
+  Modelica.Blocks.Sources.SawTooth winOpnWidthSet(amplitude=0.3, period=10)
+    "Set window opening width"
+    annotation (Placement(transformation(extent={{120,80},{100,100}})));
+  Modelica.Blocks.Sources.Ramp dpSet(
+    height=20,
+    duration=160,
+    offset=-10,
+    startTime=10) "Set pressure difference"
+    annotation (Placement(transformation(extent={{-100,-100},{-80,-80}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.Maas maas(
+    winClrWidth=winClrWidth, winClrHeight=winClrHeight)
+    "Model Maas"
+    annotation (Placement(transformation(extent={{20,-120},{40,-100}})));
+  AixLib.Airflow.WindowVentilation.Utilities.WindProfilePowerLaw winSpePro13(
+    height=13, heightRef=10)
+    "Calculate wind speed profile at height of 13 m"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.Hall hall(
+    winClrWidth=winClrWidth, winClrHeight=winClrHeight)
+    "Model Hall"
+    annotation (Placement(transformation(extent={{60,-140},{80,-120}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.Jiang jiang(
+    winClrWidth=winClrWidth, winClrHeight=winClrHeight)
+    "Model Jiang"
+    annotation (Placement(transformation(extent={{-60,-100},{-40,-80}})));
+equation
+  connect(TRoomSet.y, from_degC.u)
+    annotation (Line(points={{-79,90},{-62,90}}, color={0,0,127}));
+  connect(TAmbSet.y, from_degC1.u)
+    annotation (Line(points={{-79,60},{-62,60}}, color={0,0,127}));
+  connect(winSpe10Set.y, winSpeProLoc.winSpeRef) annotation (Line(points={{-79,30},
+          {-70,30},{-70,-30},{-62,-30}}, color={0,0,127}));
+  connect(winSpe10Set.y, winSpePro13.winSpeRef) annotation (Line(points={{-79,30},
+          {-70,30},{-70,-50},{-62,-50}}, color={0,0,127}));
+  connect(cofSunShaSet.y, vdi2078_3.cofSunSha_in)
+    annotation (Line(points={{60.5,15},{70,15},{70,18}}, color={0,0,127}));
+  connect(from_degC.y, warrenParkins.TRoom) annotation (Line(points={{-39,90},{
+          10,90},{10,98},{18,98}}, color={0,0,127}));
+  connect(from_degC1.y, warrenParkins.TAmb) annotation (Line(points={{-39,60},{
+          0,60},{0,94},{18,94}}, color={0,0,127}));
+  connect(winSpe10Set.y, warrenParkins.winSpe10) annotation (Line(points={{-79,
+          30},{-10,30},{-10,88},{18,88}}, color={0,0,127}));
+  connect(from_degC.y, gidsPhaff.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,58},{18,58}}, color={0,0,127}));
+  connect(from_degC1.y, gidsPhaff.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,54},{18,54}}, color={0,0,127}));
+  connect(winSpe10Set.y, gidsPhaff.winSpe10) annotation (Line(points={{-79,30},
+          {-10,30},{-10,48},{18,48}}, color={0,0,127}));
+  connect(from_degC.y, larsenHeiselberg.TRoom) annotation (Line(points={{-39,90},
+          {10,90},{10,18},{18,18}}, color={0,0,127}));
+  connect(from_degC1.y, larsenHeiselberg.TAmb) annotation (Line(points={{-39,60},
+          {0,60},{0,14},{18,14}}, color={0,0,127}));
+  connect(winSpe10Set.y, larsenHeiselberg.winSpe10) annotation (Line(points={{
+          -79,30},{-10,30},{-10,8},{18,8}}, color={0,0,127}));
+  connect(winDirSet.y, larsenHeiselberg.winDir) annotation (Line(points={{-79,0},
+          {-20,0},{-20,4},{18,4}}, color={0,0,127}));
+  connect(from_degC.y, caciolo.TRoom) annotation (Line(points={{-39,90},{10,90},
+          {10,-22},{18,-22}}, color={0,0,127}));
+  connect(from_degC1.y, caciolo.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,-26},{18,-26}}, color={0,0,127}));
+  connect(winSpeProLoc.winSpe, caciolo.winSpeLoc) annotation (Line(points={{-39,
+          -30},{-30,-30},{-30,-32},{18,-32}}, color={0,0,127}));
+  connect(winDirSet.y, caciolo.winDir) annotation (Line(points={{-79,0},{-20,0},
+          {-20,-36},{18,-36}}, color={0,0,127}));
+  connect(from_degC.y, tang.TRoom) annotation (Line(points={{-39,90},{10,90},{
+          10,-62},{18,-62}}, color={0,0,127}));
+  connect(from_degC1.y, tang.TAmb) annotation (Line(points={{-39,60},{0,60},{0,
+          -66},{18,-66}}, color={0,0,127}));
+  connect(from_degC.y, maas.TRoom) annotation (Line(points={{-39,90},{10,90},{
+          10,-102},{18,-102}}, color={0,0,127}));
+  connect(from_degC1.y, maas.TAmb) annotation (Line(points={{-39,60},{0,60},{0,
+          -106},{18,-106}}, color={0,0,127}));
+  connect(winSpePro13.winSpe, maas.winSpe13) annotation (Line(points={{-39,-50},
+          {-34,-50},{-34,-112},{18,-112}}, color={0,0,127}));
+  connect(from_degC.y, vdi2078_1.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,78},{58,78}}, color={0,0,127}));
+  connect(from_degC1.y, vdi2078_1.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,74},{58,74}}, color={0,0,127}));
+  connect(from_degC.y, vdi2078_2.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,78},{50,78},{50,58},{58,58}}, color={0,0,127}));
+  connect(from_degC1.y, vdi2078_2.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,74},{46,74},{46,54},{58,54}}, color={0,0,127}));
+  connect(from_degC.y, vdi2078_3.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,78},{50,78},{50,38},{58,38}}, color={0,0,127}));
+  connect(from_degC1.y, vdi2078_3.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,74},{46,74},{46,34},{58,34}}, color={0,0,127}));
+  connect(from_degC.y, din16798_1.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,-2},{58,-2}}, color={0,0,127}));
+  connect(from_degC1.y, din16798_1.TAmb) annotation (Line(points={{-39,60},{0,
+          60},{0,-6},{58,-6}}, color={0,0,127}));
+  connect(winSpe10Set.y, din16798_1.winSpe10) annotation (Line(points={{-79,30},
+          {-10,30},{-10,-12},{58,-12}}, color={0,0,127}));
+  connect(from_degC.y, din4108_1.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,-42},{58,-42}}, color={0,0,127}));
+  connect(from_degC1.y, din4108_1.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,-46},{58,-46}}, color={0,0,127}));
+  connect(winSpeProLoc.winSpe, din4108_1.winSpeLoc) annotation (Line(points={{
+          -39,-30},{-30,-30},{-30,-52},{58,-52}}, color={0,0,127}));
+  connect(from_degC.y, ashrae.TRoom) annotation (Line(points={{-39,90},{10,90},
+          {10,-82},{58,-82}}, color={0,0,127}));
+  connect(from_degC1.y, ashrae.TAmb) annotation (Line(points={{-39,60},{0,60},{
+          0,-86},{58,-86}}, color={0,0,127}));
+  connect(winSpeProLoc.winSpe, ashrae.winSpeLoc) annotation (Line(points={{-39,
+          -30},{-30,-30},{-30,-92},{58,-92}}, color={0,0,127}));
+  connect(winDirSet.y, ashrae.winDir) annotation (Line(points={{-79,0},{-20,0},
+          {-20,-96},{58,-96}}, color={0,0,127}));
+  connect(from_degC.y, hall.TRoom) annotation (Line(points={{-39,90},{10,90},{
+          10,-122},{58,-122}}, color={0,0,127}));
+  connect(from_degC1.y, hall.TAmb) annotation (Line(points={{-39,60},{0,60},{0,
+          -126},{58,-126}}, color={0,0,127}));
+  connect(dpSet.y, jiang.dp)
+    annotation (Line(points={{-79,-90},{-62,-90}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, warrenParkins.opnWidth_in) annotation (Line(points=
+          {{99,90},{90,90},{90,102},{30,102}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, gidsPhaff.opnWidth_in) annotation (Line(points={{99,
+          90},{90,90},{90,62},{30,62}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, larsenHeiselberg.opnWidth_in) annotation (Line(
+        points={{99,90},{90,90},{90,22},{30,22}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, caciolo.opnWidth_in) annotation (Line(points={{99,
+          90},{90,90},{90,-18},{30,-18}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, tang.opnWidth_in) annotation (Line(points={{99,90},
+          {90,90},{90,-58},{30,-58}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, maas.opnWidth_in) annotation (Line(points={{99,90},
+          {90,90},{90,-98},{30,-98}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, vdi2078_1.opnWidth_in) annotation (Line(points={{99,
+          90},{90,90},{90,82},{70,82}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, din16798_1.opnWidth_in)
+    annotation (Line(points={{99,90},{90,90},{90,2},{70,2}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, din4108_1.opnWidth_in) annotation (Line(points={{99,
+          90},{90,90},{90,-38},{70,-38}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, ashrae.opnWidth_in) annotation (Line(points={{99,90},
+          {90,90},{90,-78},{70,-78}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, hall.opnWidth_in) annotation (Line(points={{99,90},
+          {90,90},{90,-118},{70,-118}}, color={0,0,127}));
+  connect(winOpnWidthSet.y, jiang.opnWidth_in) annotation (Line(points={{99,90},
+          {90,90},{90,-78},{-50,-78}}, color={0,0,127}));
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This example checks the models that simulate the window ventilation flow rate with the sash opening. For the sash opening type, all models are set to the bottom-hung opening.</p>
+<p>The result shows that the estimated volume flow can be quite different when using different models.</p>
+<p>Warnings are triggered when boundary conditions for an empirical expression are out of range. This could lead to inaccurate calculation results.</p>
+<p>This example is a stress test with a wide range of boundary conditions. These conditions can cause a lot of events and slow down the simulation. In practice, the warning will rarely be triggered.</p>
+</html>"), experiment(
+      StartTime=0,
+      StopTime=180,
+      Interval=0.1,
+      Tolerance=1e-06,
+      __Dymola_Algorithm="Dassl"),
+    Diagram(coordinateSystem(extent={{-100,-140},{120,100}})),
+    __Dymola_Commands(file=
+          "Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/VentilationFlowRateSashOpening.mos"
+        "Simulate and plot"));
+end VentilationFlowRateSashOpening;
diff --git a/AixLib/Airflow/WindowVentilation/Examples/VentilationFlowRateSimpleOpening.mo b/AixLib/Airflow/WindowVentilation/Examples/VentilationFlowRateSimpleOpening.mo
new file mode 100644
index 0000000000..5014466fed
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Examples/VentilationFlowRateSimpleOpening.mo
@@ -0,0 +1,219 @@
+within AixLib.Airflow.WindowVentilation.Examples;
+model VentilationFlowRateSimpleOpening
+  "Use different empirical expressions to determine the window ventilation flow rate by simple opening"
+  extends Modelica.Icons.Example;
+  /*Parameters for boundary conditions*/
+  parameter Modelica.Units.SI.Length winClrWidth(min=0)=1.0
+    "Width of the window clear opening";
+  parameter Modelica.Units.SI.Height winClrHeight(min=0)=1.8
+    "Height of the window clear opening";
+  parameter Modelica.Units.SI.Angle aziRef(displayUnit="deg")=0
+    "Azimuth angle of the referece surface impacted by wind";
+  parameter Modelica.Units.SI.Height locHeight(min=0)=4
+    "Middle local height of the ventilation zone";
+  Modelica.Blocks.Sources.Ramp TRoomSet(
+    height=15,
+    duration=120,
+    offset=15,
+    startTime=50) "Set room temperature in °C"
+    annotation (Placement(transformation(extent={{-100,80},{-80,100}})));
+  Modelica.Blocks.Math.UnitConversions.From_degC from_degC "Convert degC to K"
+    annotation (Placement(transformation(extent={{-60,80},{-40,100}})));
+  Modelica.Blocks.Sources.Ramp TAmbSet(
+    height=-40,
+    duration=160,
+    offset=40,
+    startTime=10) "Set ambient temperature in °C"
+    annotation (Placement(transformation(extent={{-100,50},{-80,70}})));
+  Modelica.Blocks.Math.UnitConversions.From_degC from_degC1 "Convert degC to K"
+    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
+  Modelica.Blocks.Sources.TimeTable winSpe10Set(table=[0,0; 20,0; 30,5; 40,0; 50,
+        10; 60,0; 70,20; 80,0; 100,0; 110,20; 120,0; 130,10; 140,0; 150,5; 160,0;
+        180,0]) "Set wind speed at the height of 10 m"
+    annotation (Placement(transformation(extent={{-100,20},{-80,40}})));
+  Modelica.Blocks.Sources.Sine winDirSet(amplitude=2*Modelica.Constants.pi, f=0.05)
+    "Set wind direction"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.WarrenParkins warrenParkins(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple)
+        "Model Warren Parkins"
+    annotation (Placement(transformation(extent={{20,80},{40,100}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.GidsPhaff gidsPhaff(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple)
+      "Model de Gids Phaff"
+    annotation (Placement(transformation(extent={{20,40},{40,60}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.LarsenHeiselberg larsenHeiselberg(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+    aziRef=aziRef) "Model Larsen Heiselberg"
+    annotation (Placement(transformation(extent={{20,0},{40,20}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.Caciolo caciolo(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+    aziRef=aziRef) "Model Caciolo"
+    annotation (Placement(transformation(extent={{20,-40},{40,-20}})));
+  AixLib.Airflow.WindowVentilation.Utilities.WindProfilePowerLaw winSpeProLoc(
+    height=locHeight, heightRef=10)
+    "Calculate wind speed profile local"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.Tang tang(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple)
+    "Model Tang"
+    annotation (Placement(transformation(extent={{20,-80},{40,-60}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.VDI2078 vdi2078_1(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimpleVDI2078,
+    sunShaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.NoSunshading)
+    "Model VDI 2078, without sun shading"
+    annotation (Placement(transformation(extent={{60,60},{80,80}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.VDI2078 vdi2078_2(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimpleVDI2078,
+    sunShaTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.SunshadingInstallationTypesVDI2078.ExternalBlindsOn)
+    "Model VDI 2078, with sun shading"
+    annotation (Placement(transformation(extent={{60,40},{80,60}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.VDI2078 vdi2078_3(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimpleVDI2078,
+    use_cofSunSha_in=true) "Model VDI 2078, with sun shading input"
+    annotation (Placement(transformation(extent={{60,20},{80,40}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.DIN16798 din16798_1(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+    heightASL=200) "Model DIN 16798"
+    annotation (Placement(transformation(extent={{60,-20},{80,0}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.DIN4108 din4108_1(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple)
+    "Model DIN 4108"
+    annotation (Placement(transformation(extent={{60,-60},{80,-40}})));
+  AixLib.Airflow.WindowVentilation.EmpiricalExpressions.ASHRAE ashrae(
+    winClrWidth=winClrWidth,
+    winClrHeight=winClrHeight,
+    redeclare model OpeningArea =
+      AixLib.Airflow.WindowVentilation.OpeningAreas.OpeningAreaSimple,
+    aziRef=aziRef) "Model ASHRAE"
+    annotation (Placement(transformation(extent={{60,-100},{80,-80}})));
+  Modelica.Blocks.Sources.Pulse cofSunShaSet(
+    amplitude=0.5,
+    period=10,
+    offset=0.5) "Set sunshading coefficient"
+    annotation (Placement(transformation(extent={{50,10},{60,20}})));
+equation
+  connect(TRoomSet.y, from_degC.u)
+    annotation (Line(points={{-79,90},{-62,90}}, color={0,0,127}));
+  connect(TAmbSet.y, from_degC1.u)
+    annotation (Line(points={{-79,60},{-62,60}}, color={0,0,127}));
+  connect(winSpe10Set.y, winSpeProLoc.winSpeRef) annotation (Line(points={{-79,30},
+          {-70,30},{-70,-30},{-62,-30}}, color={0,0,127}));
+  connect(cofSunShaSet.y, vdi2078_3.cofSunSha_in)
+    annotation (Line(points={{60.5,15},{70,15},{70,18}}, color={0,0,127}));
+  connect(from_degC.y, warrenParkins.TRoom) annotation (Line(points={{-39,90},{
+          10,90},{10,98},{18,98}}, color={0,0,127}));
+  connect(from_degC1.y, warrenParkins.TAmb) annotation (Line(points={{-39,60},{
+          0,60},{0,94},{18,94}}, color={0,0,127}));
+  connect(winSpe10Set.y, warrenParkins.winSpe10) annotation (Line(points={{-79,
+          30},{-10,30},{-10,88},{18,88}}, color={0,0,127}));
+  connect(from_degC.y, gidsPhaff.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,58},{18,58}}, color={0,0,127}));
+  connect(from_degC1.y, gidsPhaff.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,54},{18,54}}, color={0,0,127}));
+  connect(winSpe10Set.y, gidsPhaff.winSpe10) annotation (Line(points={{-79,30},
+          {-10,30},{-10,48},{18,48}}, color={0,0,127}));
+  connect(from_degC.y, larsenHeiselberg.TRoom) annotation (Line(points={{-39,90},
+          {10,90},{10,18},{18,18}}, color={0,0,127}));
+  connect(from_degC1.y, larsenHeiselberg.TAmb) annotation (Line(points={{-39,60},
+          {0,60},{0,14},{18,14}}, color={0,0,127}));
+  connect(winSpe10Set.y, larsenHeiselberg.winSpe10) annotation (Line(points={{
+          -79,30},{-10,30},{-10,8},{18,8}}, color={0,0,127}));
+  connect(winDirSet.y, larsenHeiselberg.winDir) annotation (Line(points={{-79,0},
+          {-20,0},{-20,4},{18,4}}, color={0,0,127}));
+  connect(from_degC.y, caciolo.TRoom) annotation (Line(points={{-39,90},{10,90},
+          {10,-22},{18,-22}}, color={0,0,127}));
+  connect(from_degC1.y, caciolo.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,-26},{18,-26}}, color={0,0,127}));
+  connect(winSpeProLoc.winSpe, caciolo.winSpeLoc) annotation (Line(points={{-39,
+          -30},{-30,-30},{-30,-32},{18,-32}}, color={0,0,127}));
+  connect(winDirSet.y, caciolo.winDir) annotation (Line(points={{-79,0},{-20,0},
+          {-20,-36},{18,-36}}, color={0,0,127}));
+  connect(from_degC.y, tang.TRoom) annotation (Line(points={{-39,90},{10,90},{
+          10,-62},{18,-62}}, color={0,0,127}));
+  connect(from_degC1.y, tang.TAmb) annotation (Line(points={{-39,60},{0,60},{0,
+          -66},{18,-66}}, color={0,0,127}));
+  connect(from_degC.y, vdi2078_1.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,78},{58,78}}, color={0,0,127}));
+  connect(from_degC1.y, vdi2078_1.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,74},{58,74}}, color={0,0,127}));
+  connect(from_degC.y, vdi2078_2.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,78},{50,78},{50,58},{58,58}}, color={0,0,127}));
+  connect(from_degC1.y, vdi2078_2.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,74},{46,74},{46,54},{58,54}}, color={0,0,127}));
+  connect(from_degC.y, vdi2078_3.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,78},{50,78},{50,38},{58,38}}, color={0,0,127}));
+  connect(from_degC1.y, vdi2078_3.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,74},{46,74},{46,34},{58,34}}, color={0,0,127}));
+  connect(from_degC.y, din16798_1.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,-2},{58,-2}}, color={0,0,127}));
+  connect(from_degC1.y, din16798_1.TAmb) annotation (Line(points={{-39,60},{0,
+          60},{0,-6},{58,-6}}, color={0,0,127}));
+  connect(winSpe10Set.y, din16798_1.winSpe10) annotation (Line(points={{-79,30},
+          {-10,30},{-10,-12},{58,-12}}, color={0,0,127}));
+  connect(from_degC.y, din4108_1.TRoom) annotation (Line(points={{-39,90},{10,
+          90},{10,-42},{58,-42}}, color={0,0,127}));
+  connect(from_degC1.y, din4108_1.TAmb) annotation (Line(points={{-39,60},{0,60},
+          {0,-46},{58,-46}}, color={0,0,127}));
+  connect(winSpeProLoc.winSpe, din4108_1.winSpeLoc) annotation (Line(points={{
+          -39,-30},{-30,-30},{-30,-52},{58,-52}}, color={0,0,127}));
+  connect(from_degC.y, ashrae.TRoom) annotation (Line(points={{-39,90},{10,90},
+          {10,-82},{58,-82}}, color={0,0,127}));
+  connect(from_degC1.y, ashrae.TAmb) annotation (Line(points={{-39,60},{0,60},{
+          0,-86},{58,-86}}, color={0,0,127}));
+  connect(winSpeProLoc.winSpe, ashrae.winSpeLoc) annotation (Line(points={{-39,
+          -30},{-30,-30},{-30,-92},{58,-92}}, color={0,0,127}));
+  connect(winDirSet.y, ashrae.winDir) annotation (Line(points={{-79,0},{-20,0},
+          {-20,-96},{58,-96}}, color={0,0,127}));
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This example checks the models that simulate the window ventilation flow rate with the simple opening.</p>
+<p>The result shows that the estimated volume flow can be quite different when using different models.</p>
+<p>Warnings are triggered when boundary conditions for an empirical expression are out of range. This could lead to inaccurate calculation results.</p>
+<p>This example is a stress test with a wide range of boundary conditions. These conditions can cause a lot of events and slow down the simulation. In practice, the warning will rarely be triggered.</p>
+</html>"), experiment(
+      StartTime=0,
+      StopTime=180,
+      Interval=0.1,
+      Tolerance=1e-06,
+      __Dymola_Algorithm="Dassl"),
+    __Dymola_Commands(file=
+          "Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/VentilationFlowRateSimpleOpening.mos"
+        "Simulate and plot"));
+end VentilationFlowRateSimpleOpening;
diff --git a/AixLib/Airflow/WindowVentilation/Examples/package.mo b/AixLib/Airflow/WindowVentilation/Examples/package.mo
new file mode 100644
index 0000000000..f2c83aa26c
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Examples/package.mo
@@ -0,0 +1,4 @@
+within AixLib.Airflow.WindowVentilation;
+package Examples
+extends Modelica.Icons.ExamplesPackage;
+end Examples;
diff --git a/AixLib/Airflow/WindowVentilation/Examples/package.order b/AixLib/Airflow/WindowVentilation/Examples/package.order
new file mode 100644
index 0000000000..97f8c0be12
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Examples/package.order
@@ -0,0 +1,3 @@
+OpeningArea
+VentilationFlowRateSashOpening
+VentilationFlowRateSimpleOpening
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashCommon.mo b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashCommon.mo
new file mode 100644
index 0000000000..3444f673b1
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashCommon.mo
@@ -0,0 +1,143 @@
+within AixLib.Airflow.WindowVentilation.OpeningAreas;
+model OpeningAreaSashCommon
+  "Calculate geometric, projective, equivalent, and effective window opening
+  areas, by different types of sash opening"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningAreaSash;
+  parameter AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes
+    opnAreaTyp = AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric
+    "Window opening area types to calculate";
+
+  /*Characterize lengths*/
+  final parameter Modelica.Units.SI.Length lenAxs(min=0)=
+    if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungOutward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical) then
+    winClrHeight else if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal) then
+    winClrWidth else 0
+    "Length to characterize the hung and pivot window opening:
+    length of the hinged axis";
+  final parameter Modelica.Units.SI.Length lenAxsToFrm(min=0)=
+    if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungOutward) then
+    winClrWidth else if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward) then
+    winClrHeight else if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical) then
+    winClrWidth/2 else if (opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal) then
+    winClrHeight/2 else 0
+    "Length to characterize the hung and pivot window opening:
+    distance from the hinged axis to the frame across the opening area";
+
+  /*Variables to describe the opening*/
+  Modelica.Units.SI.Area AGeoOpn(min=0) "Geometric opening area";
+  Modelica.Units.SI.Area APrjOpn(min=0) "Projective opening area";
+  Modelica.Units.SI.Area AEqvOpn(min=0) "Equivalent opening area";
+  Modelica.Units.SI.Area AEffOpn(min=0) "Effective opening area";
+protected
+  Modelica.Units.SI.Length opnWidth90(min=0)
+    "Sash opening width by 90° opening / full sliding opening";
+  Modelica.Units.SI.Area AGeoOpn90(min=0)
+    "Geometric opening area by 90° opening";
+  Modelica.Units.SI.Area AEqvOpn90(min=0)
+    "Equivalent opening area by 90° opening";
+initial equation
+  if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingVertical or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingHorizontal then
+    assert(
+      opnAreaTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric,
+      "By opening type 'Sliding', only 'geometric' opening area is valid.",
+      AssertionLevel.error);
+  end if;
+equation
+  /*Hinged opening*/
+  if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungOutward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward then
+    /*Calculate area values*/
+    AGeoOpn =
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.GeometricOpeningArea(
+      lenAxs, lenAxsToFrm, opnWidth_internal);
+    APrjOpn =
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.ProjectiveOpeningArea(
+      lenAxs, lenAxsToFrm, opnWidth_internal);
+    opnWidth90 =
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.AngleToWidth(
+      lenAxs, lenAxsToFrm, Modelica.Constants.pi/2);
+    AGeoOpn90 = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.GeometricOpeningArea(
+      lenAxs, lenAxsToFrm, opnWidth90);
+
+  /*Pivot opening*/
+  elseif opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal then
+    /*Calculate area values*/
+    AGeoOpn =
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.GeometricOpeningArea(
+      lenAxs, lenAxsToFrm, opnWidth_internal)*2;
+    APrjOpn =
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.ProjectiveOpeningArea(
+      lenAxs, lenAxsToFrm, opnWidth_internal)*2;
+    opnWidth90 =
+      AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.AngleToWidth(
+      lenAxs, lenAxsToFrm, Modelica.Constants.pi/2);
+    AGeoOpn90 = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.GeometricOpeningArea(
+      lenAxs, lenAxsToFrm, opnWidth90)*2;
+
+  /*Sliding opening*/
+  elseif opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingVertical or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingHorizontal then
+    /*Calculate area values*/
+    if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingVertical then
+      /*Vertical*/
+      AGeoOpn = winClrWidth*opnWidth_internal;
+      opnWidth90 = winClrHeight;
+      AGeoOpn90 = winClrWidth*opnWidth90;
+    else
+      /*Horizontal*/
+      AGeoOpn = winClrHeight*opnWidth_internal;
+      opnWidth90 = winClrWidth;
+      AGeoOpn90 = winClrHeight*opnWidth90;
+    end if;
+    APrjOpn = AGeoOpn;
+
+  /*Exceptions*/
+  else
+    AGeoOpn = 0;
+    APrjOpn = 0;
+    opnWidth90 = 0;
+    AGeoOpn90 = 0;
+  end if;
+
+  /*Calculate the rest area types*/
+  AEqvOpn = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.EquivalentOpeningArea(
+    AClrOpn, AGeoOpn);
+  AEqvOpn90 = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.EquivalentOpeningArea(
+    AClrOpn, AGeoOpn90);
+  AEffOpn = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.EffectiveOpeningArea(
+    AClrOpn, AEqvOpn, AEqvOpn90);
+
+  /*Export area to port based on choice*/
+  A = if opnAreaTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Geometric then
+    AGeoOpn else if opnAreaTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Projective then
+    APrjOpn else if opnAreaTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Equivalent then
+    AEqvOpn else if opnAreaTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.OpeningAreaTypes.Effective then
+    AEffOpn else 0;
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Text(
+          extent={{-100,-100},{100,-60}},
+          textColor={0,0,0},
+          textString="%opnAreaTyp")}),
+          Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This partial model provides a base class of common window sash opening area, incl. geometric, projective, equivalent, and effective opening area.</p>
+<p>Input port of this model is the opening width.</p>
+</html>"));
+end OpeningAreaSashCommon;
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashDIN16798.mo b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashDIN16798.mo
new file mode 100644
index 0000000000..0b22f752bc
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashDIN16798.mo
@@ -0,0 +1,36 @@
+within AixLib.Airflow.WindowVentilation.OpeningAreas;
+model OpeningAreaSashDIN16798
+  "Specified DIN CEN/TR 16798-8: Only valid for bottom- or top-hung opening"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningAreaSash;
+  Real cof "Coefficient depending on the kind of window";
+initial equation
+  assert(
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward,
+    "The model is only valid for top- or bottom-hung opening.",
+    AssertionLevel.error);
+  assert((winClrHeight/winClrWidth >= 1) and (winClrHeight/winClrWidth <= 2),
+    "For hinged windows, the model applies for height and width geometries of approx. 1:1 to 2:1",
+    AssertionLevel.warning);
+equation
+  cof = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.CoeffOpeningAreaDIN16798(
+    opnAng);
+  A = cof*AClrOpn;
+  annotation (Icon(graphics={
+        Text(
+          extent={{-100,-100},{100,-60}},
+          textColor={0,0,0},
+          textString="DIN CEN/TR 16798-8")}),
+                                Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model determines the window opening area according to DIN CEN/TR 16798-8 (DIN SPEC 32739-8):2018-03.</p>
+<p>Only top- or bottom-hung openings can be applied.</p>
+<p>Input port of this model is the opening width.</p>
+</html>"));
+end OpeningAreaSashDIN16798;
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashDIN4108.mo b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashDIN4108.mo
new file mode 100644
index 0000000000..36e9bdb5b1
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashDIN4108.mo
@@ -0,0 +1,65 @@
+within AixLib.Airflow.WindowVentilation.OpeningAreas;
+model OpeningAreaSashDIN4108
+  "Specified DIN/TS 4108-8: Valid for different opening types"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningAreaSash;
+  parameter Modelica.Units.SI.Thickness sWinSas(min=0) = 0
+    "Window sash thickness (depth)"
+    annotation(Dialog(enable=(
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal)));
+initial equation
+  if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward then
+    assert((winClrHeight/winClrWidth >= 1) and (winClrHeight/winClrWidth <= 2),
+      "For hinged windows, the model applies for height and width geometries of approx. 1:1 to 2:1",
+      AssertionLevel.warning);
+  end if;
+equation
+  if opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungInward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SideHungOutward then
+    A = if opnWidth_internal < Modelica.Constants.eps then 0 else sqrt(1/(
+      (winClrWidth*winClrHeight)^(-2) + (2*winClrWidth*winClrHeight*sin(opnAng/2)
+      + winClrWidth^2*sin(opnAng))^(-2)));
+
+  elseif opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.TopHungOutward or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward then
+    assert(opnAng <= Modelica.Units.Conversions.from_deg(30),
+      "The model only applies to a maximum tilt angle of 30°",
+      AssertionLevel.warning);
+    A = AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.CoeffOpeningAreaDIN16798(
+      opnAng)*winClrWidth*winClrHeight;
+
+  elseif opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotVertical or
+    opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.PivotHorizontal then
+    A = if opnWidth_internal < Modelica.Constants.eps then 0 else min(2*(
+      opnWidth_internal*(winClrWidth - 2*sWinSas) + opnWidth_internal*sqrt((
+      winClrHeight/2*opnWidth_internal/(opnWidth_internal + sWinSas))^2 - 0.25*
+      opnWidth_internal^2)), (winClrHeight - sWinSas)*winClrWidth);
+
+  elseif opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingVertical then
+    A = opnWidth_internal*winClrWidth;
+
+  elseif opnTyp == AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.SlidingHorizontal then
+    A = opnWidth_internal*winClrHeight;
+
+  else
+    A = 0;
+  end if;
+  annotation (Icon(graphics={
+        Text(
+          extent={{-100,-100},{100,-60}},
+          textColor={0,0,0},
+          textString="DIN/TS 4108-8")}),
+                                Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model determines the window opening area according to DIN/TS 4108-8:2022-09.</p>
+<p>All common <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/Types/WindowOpeningTypes.mo\">window opening types</a> can be applied.</p>
+<p>Input port of this model is the opening width.</p>
+</html>"));
+end OpeningAreaSashDIN4108;
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashHall.mo b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashHall.mo
new file mode 100644
index 0000000000..f93b36d1d5
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashHall.mo
@@ -0,0 +1,37 @@
+within AixLib.Airflow.WindowVentilation.OpeningAreas;
+model OpeningAreaSashHall
+  "Specified Hall: Only valid for bottom-hung inwards opening"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningAreaSash(
+    final opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward);
+  parameter Modelica.Units.SI.Thickness sWinSas(min=0) = 0
+    "Window sash thickness (depth)";
+  parameter Modelica.Units.SI.Length widthWinGap(min=0) = 0.01
+    "Gap width in the overlap area between the frame and the sash";
+  Real corNPL "Correction factor of the neutral pressure level";
+initial equation
+  assert(winClrHeight >= winClrWidth,
+    "The model only applies to windows whose height is not less than the width",
+    AssertionLevel.warning);
+equation
+  corNPL = sqrt((winClrWidth - opnWidth_internal)/winClrHeight);
+  A = if noEvent(opnWidth_internal > Modelica.Constants.eps) then corNPL*
+    opnWidth_internal*(winClrHeight*opnWidth_internal/(opnWidth_internal +
+    sWinSas) - winClrHeight*(1 - corNPL)) + 2*winClrHeight*sWinSas/(
+    opnWidth_internal + sWinSas)*widthWinGap else 0;
+  annotation (Icon(graphics={
+        Text(
+          extent={{-100,-100},{100,-60}},
+          textColor={0,0,0},
+          textString="Hall")}), Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model determines the window opening area according to the empirical expression developed by Hall.</p>
+<p>Only bottom-hung openings can be applied.</p>
+<p>Input port of this model is the opening width.</p>
+</html>"));
+end OpeningAreaSashHall;
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashVDI2078.mo b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashVDI2078.mo
new file mode 100644
index 0000000000..c951ef0138
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSashVDI2078.mo
@@ -0,0 +1,43 @@
+within AixLib.Airflow.WindowVentilation.OpeningAreas;
+model OpeningAreaSashVDI2078
+  "Specified VDI 2078: Only valid for bottom-hung inwards opening"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningAreaSash(
+    final opnTyp=AixLib.Airflow.WindowVentilation.BaseClasses.Types.WindowOpeningTypes.BottomHungInward);
+  parameter Modelica.Units.SI.Height heightRevToFrm = 0.1
+    "Vertical distance (height) between the reveal above the window and window top frame";
+  parameter Modelica.Units.SI.Thickness sWinSas(min=0) = 0
+    "Window sash thickness (depth)";
+  Modelica.Units.SI.Height effHeight(min=0)
+    "Effective height for the thermal updraft";
+  Modelica.Units.SI.Height ovlHeight(min=0)
+    "Height of the overlap between window frame and casement";
+  Real corRev "Correction factor of the window reveal";
+equation
+  assert(opnAng <= Modelica.Units.Conversions.from_deg(15),
+    "The model only applies to a maximum tilt angle of 15°",
+    AssertionLevel.warning);
+  effHeight = 2/3*(winClrHeight - ovlHeight);
+  ovlHeight = if sWinSas > Modelica.Constants.eps then
+    sWinSas/(opnWidth_internal + sWinSas)*winClrHeight else 0;
+  corRev = if opnWidth_internal <= heightRevToFrm then 1 else
+    1 - 0.6*(1 - heightRevToFrm/opnWidth_internal);
+  A = if noEvent(opnWidth_internal > Modelica.Constants.eps) then
+    ((winClrWidth + winClrHeight - ovlHeight)*opnWidth_internal/3)*corRev else 0;
+  annotation (Icon(graphics={
+        Text(
+          extent={{-100,-100},{100,-60}},
+          textColor={0,0,0},
+          textString="VDI 2078")}),
+                                Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model determines the window opening area according to VDI 2078:2015-06.</p>
+<p>Only bottom-hung openings can be applied.</p>
+<p>Input port of this model is the opening width.</p>
+</html>"));
+end OpeningAreaSashVDI2078;
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSimple.mo b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSimple.mo
new file mode 100644
index 0000000000..4e752e68a1
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSimple.mo
@@ -0,0 +1,27 @@
+within AixLib.Airflow.WindowVentilation.OpeningAreas;
+model OpeningAreaSimple "Common simple opening (no sash)"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningArea(
+    final use_opnWidth_in=false,
+    final prescribedOpnWidth=0);
+equation
+  A = AClrOpn;
+  annotation (Icon(graphics={
+        Rectangle(
+          extent={{-70,90},{70,-50}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-100,-100},{100,-60}},
+          textColor={0,0,0},
+          textString="Simple")}), Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model determines the window opening area by a simple opening without window sash.</p>
+</html>"));
+end OpeningAreaSimple;
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSimpleVDI2078.mo b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSimpleVDI2078.mo
new file mode 100644
index 0000000000..16e1b9b8f2
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/OpeningAreaSimpleVDI2078.mo
@@ -0,0 +1,30 @@
+within AixLib.Airflow.WindowVentilation.OpeningAreas;
+model OpeningAreaSimpleVDI2078
+  "Specified VDI 2078: Simple opening (no sash)"
+  extends AixLib.Airflow.WindowVentilation.BaseClasses.PartialOpeningArea(
+    final use_opnWidth_in=false,
+    final prescribedOpnWidth=0);
+  final parameter Modelica.Units.SI.Height effHeight(min=0) = 2/3*winClrHeight
+    "Effective height for the thermal updraft";
+equation
+  A = 1/3*AClrOpn;
+  annotation (Icon(graphics={
+        Rectangle(
+          extent={{-70,90},{70,-50}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-100,-100},{100,-60}},
+          textColor={0,0,0},
+          textString="VDI 2078")}), Documentation(revisions="<html>
+<ul>
+  <li>
+    June 14, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>This model determines the window opening area by a simple opening without window sash according to VDI 2078:2015-06.</p>
+</html>"));
+end OpeningAreaSimpleVDI2078;
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/package.mo b/AixLib/Airflow/WindowVentilation/OpeningAreas/package.mo
new file mode 100644
index 0000000000..09ea68e9b5
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/package.mo
@@ -0,0 +1,8 @@
+within AixLib.Airflow.WindowVentilation;
+package OpeningAreas "Calculation of different opening areas based on different window types"
+  extends Modelica.Icons.VariantsPackage;
+
+annotation (Documentation(info="<html>
+<p>This package contains different expressions to determine the window opening area.</p>
+</html>"));
+end OpeningAreas;
diff --git a/AixLib/Airflow/WindowVentilation/OpeningAreas/package.order b/AixLib/Airflow/WindowVentilation/OpeningAreas/package.order
new file mode 100644
index 0000000000..423d2db5aa
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/OpeningAreas/package.order
@@ -0,0 +1,7 @@
+OpeningAreaSashCommon
+OpeningAreaSashDIN16798
+OpeningAreaSashDIN4108
+OpeningAreaSashHall
+OpeningAreaSashVDI2078
+OpeningAreaSimple
+OpeningAreaSimpleVDI2078
diff --git a/AixLib/Airflow/WindowVentilation/Utilities/AngleToWidth.mo b/AixLib/Airflow/WindowVentilation/Utilities/AngleToWidth.mo
new file mode 100644
index 0000000000..95e90daedb
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Utilities/AngleToWidth.mo
@@ -0,0 +1,30 @@
+within AixLib.Airflow.WindowVentilation.Utilities;
+model AngleToWidth
+  "Convert from window opening angle to opening width"
+  extends Modelica.Blocks.Interfaces.PartialConversionBlock(
+    u(unit="rad"), y(unit="m"));
+  parameter Modelica.Units.SI.Length lenAxs(min=0)
+    "Length of the hinged axis, the axis should be parallel to a window frame";
+  parameter Modelica.Units.SI.Length lenAxsToFrm(min=0)
+    "Distance from the hinged axis to the frame across the opening area";
+equation
+  y =
+    AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.AngleToWidth(
+    lenAxs, lenAxsToFrm, u);
+  annotation (Icon(graphics={            Text(
+              extent={{-20,100},{-100,20}},
+          textColor={0,0,0},
+          textString="α"),              Text(
+              extent={{100,-20},{20,-100}},
+          textColor={0,0,0},
+          textString="s")}), Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>Convert from window opening angle to opening width.</p>
+</html>"));
+end AngleToWidth;
diff --git a/AixLib/Airflow/WindowVentilation/Utilities/WidthToAngle.mo b/AixLib/Airflow/WindowVentilation/Utilities/WidthToAngle.mo
new file mode 100644
index 0000000000..d356d56a71
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Utilities/WidthToAngle.mo
@@ -0,0 +1,30 @@
+within AixLib.Airflow.WindowVentilation.Utilities;
+model WidthToAngle
+  "Convert from window opening width to opening angle"
+  extends Modelica.Blocks.Interfaces.PartialConversionBlock(
+    u(unit="m"), y(unit="rad"));
+  parameter Modelica.Units.SI.Length lenAxs(min=0)
+    "Length of the hinged axis, the axis should be parallel to a window frame";
+  parameter Modelica.Units.SI.Length lenAxsToFrm(min=0)
+    "Distance from the hinged axis to the frame across the opening area";
+equation
+  y =
+    AixLib.Airflow.WindowVentilation.BaseClasses.Functions.OpeningAreaHinged.WidthToAngle(
+    lenAxs, lenAxsToFrm, u);
+  annotation (Icon(graphics={            Text(
+              extent={{-20,100},{-100,20}},
+          textColor={0,0,0},
+          textString="s"),               Text(
+              extent={{100,-20},{20,-100}},
+          textColor={0,0,0},
+          textString="α")}), Documentation(revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>Convert from window opening width to opening angle.</p>
+</html>"));
+end WidthToAngle;
diff --git a/AixLib/Airflow/WindowVentilation/Utilities/WindProfilePowerLaw.mo b/AixLib/Airflow/WindowVentilation/Utilities/WindProfilePowerLaw.mo
new file mode 100644
index 0000000000..ea01cac342
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Utilities/WindProfilePowerLaw.mo
@@ -0,0 +1,249 @@
+within AixLib.Airflow.WindowVentilation.Utilities;
+model WindProfilePowerLaw
+  "Wind profile power law relationship of Hellmann"
+  parameter Modelica.Units.SI.Height height(min=0)
+    "Height of the wind speed to calculate";
+  parameter Modelica.Units.SI.Height heightRef(min=0)=10
+    "Reference height of the known wind speed";
+  parameter Modelica.Units.SI.Length lenRuf(min=0)=0.6 "Roughness length";
+  final parameter Real cof = 1/log(height/lenRuf)
+    "Hellmann exponent (coefficient)";
+  Modelica.Blocks.Interfaces.RealInput winSpeRef(unit="m/s", min=0)
+    "Wind speed at the reference height"
+    annotation (Placement(transformation(extent={{-140,-20},{-100,20}})));
+  Modelica.Blocks.Interfaces.RealOutput winSpe(unit="m/s", min=0)
+    "Wind speed at height"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+initial equation
+  assert(
+    height > lenRuf,
+    "Power law not applicable by height less than the roughness length",
+    AssertionLevel.error);
+equation
+  winSpe = winSpeRef*(height/heightRef)^cof;
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html><p>
+  This model contains the wind profile power law relationship of
+  Hellmann.
+</p>
+<p>
+  The power law allows for the calculation of wind speeds at different
+  heightghts based on the reference speed and heightght.
+</p>
+<h4>
+  Roughness Classes and Lengths
+</h4>
+<table cellspacing=\"0\" cellpadding=\"2\" border=\"1\" width=\"100%\">
+  <tr>
+    <td>
+      <h4>
+        Roughness class
+      </h4>
+    </td>
+    <td>
+      <h4>
+        Roughness length / m
+      </h4>
+    </td>
+    <td>
+      <h4>
+        Land cover types
+      </h4>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        0
+      </p>
+    </td>
+    <td>
+      <p>
+        0.0002
+      </p>
+    </td>
+    <td>
+      <p>
+        Water surfaces: seas and Lakes
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <br/>
+        <br/>
+        0.5
+      </p>
+    </td>
+    <td>
+      <p>
+        0.0024
+      </p>
+    </td>
+    <td>
+      <p>
+        Open terrain with smooth surface, e.g. concrete, airport
+        runways, mown grass etc.
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <br/>
+        <br/>
+        1
+      </p>
+    </td>
+    <td>
+      <p>
+        0.03
+      </p>
+    </td>
+    <td>
+      <p>
+        Open agricultural land without fences and hedges; maybe some
+        far apart buildings and very gentle hills
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <br/>
+        <br/>
+        1.5
+      </p>
+    </td>
+    <td>
+      <p>
+        0.055
+      </p>
+    </td>
+    <td>
+      <p>
+        Agricultural land with a few buildings and 8 m high hedges
+        seperated by more than 1 km
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <br/>
+        <br/>
+        2
+      </p>
+    </td>
+    <td>
+      <p>
+        0.1
+      </p>
+    </td>
+    <td>
+      <p>
+        Agricultural land with a few buildings and 8 m high hedges
+        seperated by approx. 500 m
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <br/>
+        <br/>
+        2.5
+      </p>
+    </td>
+    <td>
+      <p>
+        0.2
+      </p>
+    </td>
+    <td>
+      <p>
+        Agricultural land with many trees, bushes and plants, or 8 m
+        high hedges seperated by approx. 250 m
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        3
+      </p>
+    </td>
+    <td>
+      <p>
+        0.4
+      </p>
+    </td>
+    <td>
+      <p>
+        Towns, villages, agricultural land with many or high hedges,
+        forests and very rough and uneven terrain
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        3.5
+      </p>
+    </td>
+    <td>
+      <p>
+        0.6
+      </p>
+    </td>
+    <td>
+      <p>
+        Large towns with high buildings
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        4
+      </p>
+    </td>
+    <td>
+      <p>
+        1.6
+      </p>
+    </td>
+    <td>
+      <p>
+        Large cities with high buildings and skyscrapers
+      </p>
+    </td>
+  </tr>
+</table>
+<p>
+  <br/>
+</p>
+<h4>
+  References
+</h4>
+<p>
+  <br/>
+  Hau, E. (2016). Windkraftanlagen: Grundlagen, Technik, Einsatz,
+  Wirtschaftlichkeit (6. Auflage). Springer Vieweg.
+</p>
+<p>
+  <br/>
+  <a href=
+  \"https://wind-data.ch/tools/profile.php\">https://wind-data.ch/tools/profile.php</a>
+</p>
+</html>", revisions="<html>
+<ul>
+  <li>
+    June 13, 2024, by Jun Jiang:<br/>
+    First implementation (see <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1492\">issue 1492</a>)
+  </li>
+</ul>
+</html>"));
+end WindProfilePowerLaw;
diff --git a/AixLib/Airflow/WindowVentilation/Utilities/package.mo b/AixLib/Airflow/WindowVentilation/Utilities/package.mo
new file mode 100644
index 0000000000..be58d4742b
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Utilities/package.mo
@@ -0,0 +1,4 @@
+within AixLib.Airflow.WindowVentilation;
+package Utilities
+extends Modelica.Icons.UtilitiesPackage;
+end Utilities;
diff --git a/AixLib/Airflow/WindowVentilation/Utilities/package.order b/AixLib/Airflow/WindowVentilation/Utilities/package.order
new file mode 100644
index 0000000000..ba3383b32b
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/Utilities/package.order
@@ -0,0 +1,3 @@
+AngleToWidth
+WidthToAngle
+WindProfilePowerLaw
diff --git a/AixLib/Airflow/WindowVentilation/package.mo b/AixLib/Airflow/WindowVentilation/package.mo
new file mode 100644
index 0000000000..64b952094f
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/package.mo
@@ -0,0 +1,61 @@
+within AixLib.Airflow;
+package WindowVentilation "Package of different window ventilation models"
+
+annotation (Documentation(info="<html>
+<h4>Overview </h4>
+<p>This package contains models of window ventilation with various types of sash openings from literature. </p>
+<p>Currently, the models are only applicable for single-sided ventilation. </p>
+<h4>Window opening types </h4>
+<p>This package considers the following types of window openings: </p>
+<ul>
+<li>Simple opening, without window sash </li>
+<li>Side-hung opening, in- or outward, for casement window </li>
+<li>Top-hung opening, outward, for awning window </li>
+<li>Bottom-hung opening, inward, for hopper window, tilt window </li>
+<li>Pivot opening, vertical or horizontal, for center hinge window </li>
+<li>Sliding opening, vertical, for single-hung or double-hung window </li>
+<li>Sliding opening, horizontal, for slider window </li>
+</ul>
+<p>These opening types are included in <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/Types/WindowOpeningTypes.mo\">WindowOpeningTypes</a>. </p>
+<p><img src=\"modelica://AixLib/Resources/Images/Airflow/WindowVentilation/WindowOpeningTypes.png\"/> </p>
+<h4>Opening area types </h4>
+<p>For hinged and pivot openings, there are five different types to define the opening area: </p>
+<ul>
+<li>Clear opening area, as shown in the figure on the left </li>
+<li>Geometric opening area, as shown in the figure in the middle, see function <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/geometricOpeningArea.mo\">geometricOpeningArea</a> </li>
+<li>Projective opening area, as shown in the figure on the right, see function <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/projectiveOpeningArea.mo\">projectiveOpeningArea</a> </li>
+<li>Equivalent opening area, derived from clear opening area and geometric opening area, see function <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/equivalentOpeningArea.mo\">equivalentOpeningArea</a> </li>
+<li>Effective opening area, derived from clear opening area and equivalent opening area, see function <a href=\"modelica://AixLib/Airflow/WindowVentilation/BaseClasses/Functions/OpeningAreaHinged/effectiveOpeningArea.mo\">effectiveOpeningArea</a> </li>
+</ul>
+<p><br><br><img src=\"modelica://AixLib/Resources/Images/Airflow/WindowVentilation/WindowOpeningAreaQu.png\"/><img src=\"modelica://AixLib/Resources/Images/Airflow/WindowVentilation/WindowOpeningAreaGeo.png\"/><img src=\"modelica://AixLib/Resources/Images/Airflow/WindowVentilation/WindowOpeningAreaProj.png\"/> </p>
+<h4>Nomenclature</h4>
+<p>Abv: Above</p>
+<p>Amb: Ambient</p>
+<p>Ang: Angle</p>
+<p>ASL: Above see level</p>
+<p>Avg: Average</p>
+<p>Axs: Axis</p>
+<p>Clr: Clear</p>
+<p>Cof: Coefficient</p>
+<p>Cor: Correlation; Correction</p>
+<p>Dcg: Discharge</p>
+<p>Dif: Difference</p>
+<p>Eff: Effective</p>
+<p>Eqv: Equivalent</p>
+<p>Ext: External</p>
+<p>Frm: Frame</p>
+<p>Geo: Geometric</p>
+<p>Inc: Incidence</p>
+<p>Int: Interim; Internal</p>
+<p>Lim: Limit</p>
+<p>Loc: Local</p>
+<p>NPL: Neutral pressure level</p>
+<p>Opn: Open; Opening</p>
+<p>Ovl: Overlap</p>
+<p>Prj: Projective</p>
+<p>Ref: Reference</p>
+<p>Rev: Reveal</p>
+<p>Ruf: Rough; Roughness</p>
+<p>Sas: Sash</p>
+</html>"));
+end WindowVentilation;
diff --git a/AixLib/Airflow/WindowVentilation/package.order b/AixLib/Airflow/WindowVentilation/package.order
new file mode 100644
index 0000000000..e081be411d
--- /dev/null
+++ b/AixLib/Airflow/WindowVentilation/package.order
@@ -0,0 +1,5 @@
+EmpiricalExpressions
+OpeningAreas
+Utilities
+Examples
+BaseClasses
diff --git a/AixLib/Airflow/package.order b/AixLib/Airflow/package.order
index ea152c453e..3374dfb70b 100644
--- a/AixLib/Airflow/package.order
+++ b/AixLib/Airflow/package.order
@@ -2,3 +2,4 @@ AirCurtain
 AirHandlingUnit
 FacadeVentilationUnit
 Multizone
+WindowVentilation
diff --git a/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/BaseClasses/PartialHumansExample.mo b/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/BaseClasses/PartialHumansExample.mo
index d22e82f1c4..635f9db950 100644
--- a/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/BaseClasses/PartialHumansExample.mo
+++ b/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/BaseClasses/PartialHumansExample.mo
@@ -20,9 +20,12 @@ equation
   connect(heatFlowSensorConv.port_b,fixedTemp. port) annotation (Line(points={{52,19},{56,19},{56,14},{60,14}}, color={191,0,0}));
   connect(fixedTemp.port,heatFlowSensorRad. port_b) annotation (Line(points={{60,14},{56,14},{56,-8},{34,-8}},
                                                                                                              color={191,0,0}));
-  connect(heatFlowSensorConv.Q_flow,sumQ_flows. u[1]) annotation (Line(points={{45,12},{46,12},{46,-50},{30,-50},{30,-61.9},{34,-61.9}}, color={0,0,127}));
-  connect(heatFlowSensorRad.Q_flow,sumQ_flows. u[2]) annotation (Line(points={{26,-16},{26,-66.1},{34,-66.1}},                          color={0,0,127}));
-  connect(sumQ_flows.y,HeatOut)  annotation (Line(points={{47.02,-64},{100,-64}},color={0,0,127}));
+  connect(heatFlowSensorConv.Q_flow,sumQ_flows. u[1]) annotation (Line(points={{45,11.3},
+          {46,11.3},{46,-50},{30,-50},{30,-65.05},{34,-65.05}},                                                                          color={0,0,127}));
+  connect(heatFlowSensorRad.Q_flow,sumQ_flows. u[2]) annotation (Line(points={{26,
+          -16.8},{26,-62.95},{34,-62.95}},                                                                                              color={0,0,127}));
+  connect(sumQ_flows.y,HeatOut)  annotation (Line(points={{47.02,-64},{24,-64},{
+          24,0},{0,0}},                                                          color={0,0,127}));
   connect(varTempRoom.port, humanIntGains.TRoom) annotation (Line(points={{-64,52},{-40,52},{-40,12.7},{-14.7,12.7}}, color={191,0,0}));
   connect(combiTimeTable.y[1], humanIntGains.uRel) annotation (Line(points={{-61,-16},{-40,-16},{-40,1},{-16,1}}, color={0,0,127}));
   connect(heatFlowSensorConv.port_a, humanIntGains.convHeat) annotation (Line(points={{38,19},{24,19},{24,8.8},{8.7,8.8}}, color={191,0,0}));
diff --git a/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/Lights.mo b/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/Lights.mo
index ae6d798372..34b0f3f72b 100644
--- a/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/Lights.mo
+++ b/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/Lights.mo
@@ -37,10 +37,8 @@ Documentation(info="<html><h4>
 <p>
   The simulation consists of the following models:
 </p>
-<table>
-  <caption>
-    \"Models\" cellspacing=\"2\" cellpadding=\"0\" border=\"0\
-  </caption>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"0\">
+  <caption>Models</caption>
   <tr>
     <td bgcolor=\"#DCDCDC\">
       <p>
@@ -62,8 +60,8 @@ Documentation(info="<html><h4>
     <td>
       <p>
         <a href=
-        \"AixLib.Building.Components.Sources.InternalGains.Lights.Lights_simple\">
-        Lights_simple</a>
+        \"AixLib.BoundaryConditions.InternalGains.Lights.LightsAreaSpecific\">
+        LightsAreaSpecific</a>
       </p>
     </td>
   </tr>
@@ -76,22 +74,8 @@ Documentation(info="<html><h4>
     <td>
       <p>
         <a href=
-        \"AixLib.Building.Components.Sources.InternalGains.Lights.Lights_relative\">
-        Lights_relative</a>
-      </p>
-    </td>
-  </tr>
-  <tr>
-    <td>
-      <p>
-        3
-      </p>
-    </td>
-    <td>
-      <p>
-        <a href=
-        \"AixLib.Building.Components.Sources.InternalGains.Lights.Lights_Avar\">
-        Lights_Avar</a>
+        \"AixLib.BoundaryConditions.InternalGains.Lights.LightsRelToMaxValue\">
+        LightsRelToMaxValue</a>
       </p>
     </td>
   </tr>
diff --git a/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/Machines.mo b/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/Machines.mo
index 448b06382b..82b521bf98 100644
--- a/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/Machines.mo
+++ b/AixLib/BoundaryConditions/InternalGains/Examples/InternalGains/Machines.mo
@@ -41,10 +41,8 @@ Documentation(info="<html><h4>
 <p>
   The simulation consists of the following models:
 </p>
-<table>
-  <caption>
-    \"Models\" cellspacing=\"2\" cellpadding=\"0\" border=\"0\
-  </caption>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"0\">
+  <caption>Models</caption>
   <tr>
     <td bgcolor=\"#DCDCDC\">
       <p>
@@ -66,8 +64,8 @@ Documentation(info="<html><h4>
     <td>
       <p>
         <a href=
-        \"AixLib.Building.Components.Sources.InternalGains.Machines.Machines_simple\">
-        Machines_simple</a>
+        \"AixLib.BoundaryConditions.InternalGains.Machines.MachinesAreaSpecific\">
+        MachinesAreaSpecific</a>
       </p>
     </td>
   </tr>
@@ -80,8 +78,8 @@ Documentation(info="<html><h4>
     <td>
       <p>
         <a href=
-        \"AixLib.Building.Components.Sources.InternalGains.Machines.Machines_DIN18599\">
-        Machines_DIN18599</a>
+        \"AixLib.BoundaryConditions.InternalGains.Machines.MachinesDIN18599\">
+        MachinesDIN18599</a>
       </p>
     </td>
   </tr>
@@ -94,8 +92,8 @@ Documentation(info="<html><h4>
     <td>
       <p>
         <a href=
-        \"AixLib.Building.Components.Sources.InternalGains.Machines.Machines_Avar\">
-        Machines_Avar</a>
+        \"AixLib.BoundaryConditions.InternalGains.Machines.MachinesRelToMaxValue\">
+        MachinesRelToMaxValue</a>
       </p>
     </td>
   </tr>
diff --git a/AixLib/BoundaryConditions/InternalGains/Machines/MachinesDIN18599.mo b/AixLib/BoundaryConditions/InternalGains/Machines/MachinesDIN18599.mo
index 8995bdf540..1e83681b03 100644
--- a/AixLib/BoundaryConditions/InternalGains/Machines/MachinesDIN18599.mo
+++ b/AixLib/BoundaryConditions/InternalGains/Machines/MachinesDIN18599.mo
@@ -6,7 +6,7 @@ model MachinesDIN18599 "Heat flow due to machines based on DIN 18599 (number of
     gain(final k=nrPeople),
     gainSurfaces(final k=areaSurfaceMachinesTotal));
 
-  parameter Integer activityType=2 "Machine activity" annotation(Dialog( compact = true, descriptionLabel = true), choices(choice=1 "low", choice = 2 "middle",  choice = 3 "high", radioButtons = true));
+  parameter AixLib.BoundaryConditions.InternalGains.Types.MachineActivity activityType=AixLib.BoundaryConditions.InternalGains.Types.MachineActivity.middle "Machine activity" annotation(Dialog( compact = true, descriptionLabel = true));
   parameter Real nrPeople=1.0 "Number of people with machines"  annotation(Dialog(descriptionLabel = true));
   parameter Modelica.Units.SI.Area areaSurfaceMachinesTotal=max(1e-4,
       surfaceMachine*nrPeople)
@@ -21,7 +21,9 @@ protected
     table=[1,50; 2,100; 3,150],
     columns={2})
     annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
-  Modelica.Blocks.Sources.Constant activity(k=activityType)
+  Modelica.Blocks.Sources.Constant activity(k=if activityType==AixLib.BoundaryConditions.InternalGains.Types.MachineActivity.low then 1
+  elseif activityType==AixLib.BoundaryConditions.InternalGains.Types.MachineActivity.middle then 2
+  else 3)
     annotation (Placement(transformation(extent={{-90,40},{-70,60}})));
 equation
   connect(activity.y, tableHeatOutput.u[1]) annotation (Line(points={{-69,50},{-62,50}}, color={0,0,127}));
@@ -276,64 +278,61 @@ equation
   The type of activity determines the load for machines in the room for
   one person according to DIN 18599-10. The following values are used:
 </p>
-<table>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"0\">
   <caption>
-    \"DIN 18599-10 activity level and produces heat output\"
-    cellspacing=\"2\" cellpadding=\"0\" border=\"0\"&gt;
-    <table>
-      <tr>
-        <td style=\"background-color: #dcdcdc\">
-          Activity Type
-        </td>
-        <td style=\"background-color: #dcdcdc\">
-          Heat Load [W]
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            1
-          </p>
-        </td>
-        <td>
-          <p>
-            50
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            2
-          </p>
-        </td>
-        <td>
-          <p>
-            100
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            3
-          </p>
-        </td>
-        <td>
-          <p>
-            150
-          </p>
-        </td>
-      </tr>
-    </table>
-    <h4>
-      <span style=\"color: #008000\">References</span>
-    </h4>
-    <p>
-      DIN 18599-10
-    </p>
+    DIN 18599-10 activity level and produces heat output
   </caption>
+  <tr>
+    <td style=\"background-color: #dcdcdc\">
+      Activity Type
+    </td>
+    <td style=\"background-color: #dcdcdc\">
+      Heat Load [W]
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        1
+      </p>
+    </td>
+    <td>
+      <p>
+        50
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        2
+      </p>
+    </td>
+    <td>
+      <p>
+        100
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        3
+      </p>
+    </td>
+    <td>
+      <p>
+        150
+      </p>
+    </td>
+  </tr>
 </table>
+<h4>
+  <span style=\"color: #008000\">References</span>
+</h4>
+<p>
+  DIN 18599-10
+</p>
 </html>",
     revisions="<html><ul>
   <li>
diff --git a/AixLib/BoundaryConditions/InternalGains/Types.mo b/AixLib/BoundaryConditions/InternalGains/Types.mo
new file mode 100644
index 0000000000..926ec806f4
--- /dev/null
+++ b/AixLib/BoundaryConditions/InternalGains/Types.mo
@@ -0,0 +1,7 @@
+within AixLib.BoundaryConditions.InternalGains;
+package Types
+  type MachineActivity = enumeration(
+      low "low",
+      middle "middle",
+      high "high") "Enumeration to define the machine activity";
+end Types;
diff --git a/AixLib/BoundaryConditions/InternalGains/package.order b/AixLib/BoundaryConditions/InternalGains/package.order
index 83e4e57d50..62677a7244 100644
--- a/AixLib/BoundaryConditions/InternalGains/package.order
+++ b/AixLib/BoundaryConditions/InternalGains/package.order
@@ -3,5 +3,6 @@ Humans
 Lights
 Machines
 Moisture
+Types
 Examples
 BaseClasses
diff --git a/AixLib/BoundaryConditions/SkyTemperature/BlackBody.mo b/AixLib/BoundaryConditions/SkyTemperature/BlackBody.mo
index e37d752200..a9a97907eb 100644
--- a/AixLib/BoundaryConditions/SkyTemperature/BlackBody.mo
+++ b/AixLib/BoundaryConditions/SkyTemperature/BlackBody.mo
@@ -50,56 +50,56 @@ equation
   annotation (
     defaultComponentName="TBlaSky",
     Documentation(info="<html>
- <p>
- This component computes the black-body sky temperature.
- </p>
- <p>
- For <code>calTSky = 0</code>, the model uses horizontal infrared irradiation.
- Otherwise, it uses dry buld temperature, dew point temperature and opaque sky cover.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 3, 2017, by Michael Wetter:<br/>
- Removed <code>import</code> statement.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/852\">#852</a>.
- </li>
- <li>
- January 6, 2016, by Moritz Lauster:<br/>
- Changed unit and comment of input <code>nOpa</code> for correct display of units
- in <code>weaBus</code> and input <code>radHorIR</code> to <code>HHorIR</code>
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">#376</a>.
- </li>
- <li>
- May 5, 2015, by Filip Jorissen:<br/>
- Converted <code>algorithm</code> section into
- <code>equation</code> section for easier differentiability.
- </li>
- <li>
- August 11, 2012, by Wangda Zuo:<br/>
- Renamed <code>radHor</code> to <code>radHorIR</code>.
- </li>
- <li>
- October 3, 2011, by Michael Wetter:<br/>
- Used enumeration to set the sky temperature computation.
- Fixed error in <code>if-then</code> statement that led to
- a selection of the wrong branch to compute the sky temperature.
- </li>
- <li>
- March 16, 2011, by Michael Wetter:<br/>
- Added types for parameters and attributes for variables.
- Removed default parameter value.
- </li>
- <li>
- March 15, 2011, by Wangda Zuo:<br/>
- Use <code>smoothMin()</code> instead of <code>min()</code>.
- </li>
- <li>
- June 1, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the black-body sky temperature.
+</p>
+<p>
+For <code>calTSky = 0</code>, the model uses horizontal infrared irradiation.
+Otherwise, it uses dry buld temperature, dew point temperature and opaque sky cover.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 3, 2017, by Michael Wetter:<br/>
+Removed <code>import</code> statement.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/852\">#852</a>.
+</li>
+<li>
+January 6, 2016, by Moritz Lauster:<br/>
+Changed unit and comment of input <code>nOpa</code> for correct display of units
+in <code>weaBus</code> and input <code>radHorIR</code> to <code>HHorIR</code>
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">#376</a>.
+</li>
+<li>
+May 5, 2015, by Filip Jorissen:<br/>
+Converted <code>algorithm</code> section into
+<code>equation</code> section for easier differentiability.
+</li>
+<li>
+August 11, 2012, by Wangda Zuo:<br/>
+Renamed <code>radHor</code> to <code>radHorIR</code>.
+</li>
+<li>
+October 3, 2011, by Michael Wetter:<br/>
+Used enumeration to set the sky temperature computation.
+Fixed error in <code>if-then</code> statement that led to
+a selection of the wrong branch to compute the sky temperature.
+</li>
+<li>
+March 16, 2011, by Michael Wetter:<br/>
+Added types for parameters and attributes for variables.
+Removed default parameter value.
+</li>
+<li>
+March 15, 2011, by Wangda Zuo:<br/>
+Use <code>smoothMin()</code> instead of <code>min()</code>.
+</li>
+<li>
+June 1, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Text(
@@ -129,6 +129,6 @@ equation
         Text(
           extent={{-88,-24},{-64,-36}},
           textColor={0,0,127},
-          textString="nOpa")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="nOpa")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BlackBody;
diff --git a/AixLib/BoundaryConditions/SkyTemperature/Examples/BlackBody.mo b/AixLib/BoundaryConditions/SkyTemperature/Examples/BlackBody.mo
index 37919a633a..0512bfe661 100644
--- a/AixLib/BoundaryConditions/SkyTemperature/Examples/BlackBody.mo
+++ b/AixLib/BoundaryConditions/SkyTemperature/Examples/BlackBody.mo
@@ -66,34 +66,34 @@ equation
       extent={{-6,3},{-6,3}}));
   annotation (
   Documentation(info="<html>
- <p>
- This example computes the black-body sky temperature
- for Chicago.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 18, 2017, by Filip Jorissen:<br/>
- Now computing both options of <code>TBlaSky</code>.
- This verifies the consistency of the two computation methods.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/648\">#648</a>.
- </li>
- <li>
- January 7, 2016, by Michael Wetter:<br/>
- Changed <code>connect</code> statement for infrared radiation due renaming of the
- variable. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">issue 376</a>.
- Added comments.
- </li>
- <li>
- June 1, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the black-body sky temperature
+for Chicago.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 18, 2017, by Filip Jorissen:<br/>
+Now computing both options of <code>TBlaSky</code>.
+This verifies the consistency of the two computation methods.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/648\">#648</a>.
+</li>
+<li>
+January 7, 2016, by Michael Wetter:<br/>
+Changed <code>connect</code> statement for infrared radiation due renaming of the
+variable. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">issue 376</a>.
+Added comments.
+</li>
+<li>
+June 1, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StartTime=0, StopTime=86400),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SkyTemperature/Examples/BlackBody.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BlackBody;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/AltitudeAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/AltitudeAngle.mo
index 05d2c2102a..b88e8f33cd 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/AltitudeAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/AltitudeAngle.mo
@@ -14,25 +14,25 @@ equation
   annotation (Icon(graphics={Bitmap(extent={{-90,-90},{90,90}}, fileName=
               "modelica://AixLib/Resources/Images/BoundaryConditions/SolarGeometry/BaseClasses/AltitudeAngle.png")}),
     defaultComponentName="altAng", Documentation(info="<html>
- <p>
- This block computes the altitude angle of the sun with respect to a horizontal surface.
- The altitude angle is the angle between the sun ray and the projection of the ray
- on a horizontal surface.
- It is the complementory angle to the zenith angle.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 5, 2015, by Michael Wetter:<br/>
- Updated comment of the output connector as this is used in the weather bus connector.
- This is for
- issue <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">376</a>.
- </li>
- <li>
- Feb 01, 2012, by Kaustubh Phalak:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This block computes the altitude angle of the sun with respect to a horizontal surface.
+The altitude angle is the angle between the sun ray and the projection of the ray
+on a horizontal surface.
+It is the complementory angle to the zenith angle.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 5, 2015, by Michael Wetter:<br/>
+Updated comment of the output connector as this is used in the weather bus connector.
+This is for
+issue <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">376</a>.
+</li>
+<li>
+Feb 01, 2012, by Kaustubh Phalak:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AltitudeAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Declination.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Declination.mo
index d76425bc07..0e400dd6ad 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Declination.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Declination.mo
@@ -1,6 +1,6 @@
 within AixLib.BoundaryConditions.SolarGeometry.BaseClasses;
 block Declination "Declination angle"
-  extends Modelica.Blocks.Icons.Block;
+  extends AixLib.BoundaryConditions.WeatherData.BaseClasses.PartialConvertTime;
   Modelica.Blocks.Interfaces.RealInput nDay(quantity="Time", unit="s")
     "Day number with units of seconds"
     annotation (Placement(transformation(extent={{-140,-20},{-100,20}})));
@@ -13,60 +13,66 @@ protected
   constant Real k1 = sin(23.45*2*Modelica.Constants.pi/360) "Constant";
   constant Real k2 = 2*Modelica.Constants.pi/365.25 "Constant";
 equation
-  decAng = Modelica.Math.asin(-k1 * Modelica.Math.cos((nDay/86400 + 10)*k2))
+  modTimAux = nDay;
+  decAng = Modelica.Math.asin(-k1 * Modelica.Math.cos((calTimAux/86400 + 10)*k2))
     "(A4.5)";
   annotation (
     defaultComponentName="decAng",
     Documentation(info="<html>
- <p>
- This component computes the solar declination, which is
- the angle between the equatorial plane and the solar beam.
- The input signal <code>nDay</code> is the one-based number of the day, but in seconds.
- Hence, during January 1, we should have <code>nDay = 86400</code> seconds.
- Since the effect of using a continuous number rather than an integer is small,
- we approximate this so that <code>nDay = 0</code> at the start of January 1,
- and <code>nDay = 86400</code> at the end of January 1.
- </p>
- <h4>Validation</h4>
- <p>
- A validation with a more detailed calculation can be found at
- <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.Declination\">
- AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.Declination</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Updated documentation and added validation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/382\">issue 382</a>.
- </li>
- <li>
- January 5, 2015, by Michael Wetter:<br/>
- Updated comment of output signal as this is used in the weather bus connector.
- This is for
- issue <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">376</a>.
- </li>
- <li>
- November 11, 2015, by Michael Wetter:<br/>
- Corrected typo in documentation.
- </li>
- <li>
- Dec 7, 2010, by Michael Wetter:<br/>
- Rewrote equation in explicit form to avoid nonlinear equations in room model.
- </li>
- <li>
- May 17, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the solar declination, which is
+the angle between the equatorial plane and the solar beam.
+The input signal <code>nDay</code> is the one-based number of the day, but in seconds.
+Hence, during January 1, we should have <code>nDay = 86400</code> seconds.
+Since the effect of using a continuous number rather than an integer is small,
+we approximate this so that <code>nDay = 0</code> at the start of January 1,
+and <code>nDay = 86400</code> at the end of January 1.
+</p>
+<h4>Validation</h4>
+<p>
+A validation with a more detailed calculation can be found at
+<a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.Declination\">
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.Declination</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 27, 2023, by Ettore Zanetti:<br/>
+Updated to use partial class for conversion from simulation time to calendar time.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1716\">IBPSA #1716</a>.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Updated documentation and added validation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/382\">issue 382</a>.
+</li>
+<li>
+January 5, 2015, by Michael Wetter:<br/>
+Updated comment of output signal as this is used in the weather bus connector.
+This is for
+issue <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">376</a>.
+</li>
+<li>
+November 11, 2015, by Michael Wetter:<br/>
+Corrected typo in documentation.
+</li>
+<li>
+Dec 7, 2010, by Michael Wetter:<br/>
+Rewrote equation in explicit form to avoid nonlinear equations in room model.
+</li>
+<li>
+May 17, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={  Bitmap(extent={{-90,-90},{90,90}}, fileName=
               "modelica://AixLib/Resources/Images/BoundaryConditions/SolarGeometry/BaseClasses/Declination.png"),
                               Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Declination;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/AltitudeAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/AltitudeAngle.mo
index fceac305bf..9de5daa92d 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/AltitudeAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/AltitudeAngle.mo
@@ -55,33 +55,33 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/BaseClasses/Examples/AltitudeAngle.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example calculates the altitude angle of the sun at a given time.
- The altitude angle is the angle between the sun ray and the projection of the ray on a horizontal surface.
- </p>
- <p>
- Components used in this model are:
- </p>
- <ul>
- <li>
- <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination\">AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination</a>
- </li>
- <li>
- <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarHourAngle\">AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarHourAngle</a>
- </li>
- <li>
- <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.ZenithAngle\">AixLib.BoundaryConditions.SolarGeometry.BaseClasses.ZenithAngle</a>
- </li>
- </ul>
- <br/>
- </html>",
+<p>
+This example calculates the altitude angle of the sun at a given time.
+The altitude angle is the angle between the sun ray and the projection of the ray on a horizontal surface.
+</p>
+<p>
+Components used in this model are:
+</p>
+<ul>
+<li>
+<a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination\">AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination</a>
+</li>
+<li>
+<a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarHourAngle\">AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarHourAngle</a>
+</li>
+<li>
+<a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.ZenithAngle\">AixLib.BoundaryConditions.SolarGeometry.BaseClasses.ZenithAngle</a>
+</li>
+</ul>
+<br/>
+</html>",
 revisions="<html>
- <ul>
- <li>
- Feb 01, 2012, by Kaustubh Phalak<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+Feb 01, 2012, by Kaustubh Phalak<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AltitudeAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/Declination.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/Declination.mo
index c1f92716fb..1599e472a7 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/Declination.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/Declination.mo
@@ -29,23 +29,23 @@ equation
       color={0,0,127}));
   annotation (
   Documentation(info="<html>
- <p>This model validates the computation of the solar declination, which is the angle between the equatorial plane and the solar beam. The time table <code><span style=\"font-family: Courier New,courier;\">solDecNOAA</span></code> outputs the solar declination according to the computation of the National Oceanic and Atmospheric Administration (NOAA), using their yearly calculator from <a href=\"http://www.esrl.noaa.gov/gmd/grad/solcalc/calcdetails.html\">http://www.esrl.noaa.gov/gmd/grad/solcalc/calcdetails.html</a>. The values differ slightly because the equation in <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination\">AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination</a> is an approximation. </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Updated documentation and added validation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/382\">issue 382</a>.
- </li>
- <li>
- May 17, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>This model validates the computation of the solar declination, which is the angle between the equatorial plane and the solar beam. The time table <code><span style=\"font-family: Courier New,courier;\">solDecNOAA</span></code> outputs the solar declination according to the computation of the National Oceanic and Atmospheric Administration (NOAA), using their yearly calculator from <a href=\"http://www.esrl.noaa.gov/gmd/grad/solcalc/calcdetails.html\">http://www.esrl.noaa.gov/gmd/grad/solcalc/calcdetails.html</a>. The values differ slightly because the equation in <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination\">AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination</a> is an approximation. </p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Updated documentation and added validation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/382\">issue 382</a>.
+</li>
+<li>
+May 17, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StopTime=3.1536e+007),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/BaseClasses/Examples/Declination.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Declination;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/IncidenceAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/IncidenceAngle.mo
index 561d8c5e53..ff31191859 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/IncidenceAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/IncidenceAngle.mo
@@ -57,29 +57,29 @@ equation
       horizontalAlignment=TextAlignment.Right));
   annotation (
   Documentation(info="<html>
- <p>
- This example computes the solar incidence angle on a tilted surface.
- This model is also part of more extensive tests that run the
- model for different orientations. These tests are at
- <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.Examples.IncidenceAngle\">
- AixLib.BoundaryConditions.SolarGeometry.Examples.IncidenceAngle</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 24, 2015, by Michael Wetter:<br/>
- Assigned azimuth and tilt using the types from
- <a href=\"modelica://AixLib.Types.Tilt\">
- AixLib.Types.Tilt</a>.
- </li>
- <li>
- May 19, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the solar incidence angle on a tilted surface.
+This model is also part of more extensive tests that run the
+model for different orientations. These tests are at
+<a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.Examples.IncidenceAngle\">
+AixLib.BoundaryConditions.SolarGeometry.Examples.IncidenceAngle</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 24, 2015, by Michael Wetter:<br/>
+Assigned azimuth and tilt using the types from
+<a href=\"modelica://AixLib.Types.Tilt\">
+AixLib.Types.Tilt</a>.
+</li>
+<li>
+May 19, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StopTime=86400),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/BaseClasses/Examples/IncidenceAngle.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end IncidenceAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarAzimuth.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarAzimuth.mo
index 3bf63b2189..26109c63af 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarAzimuth.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarAzimuth.mo
@@ -77,19 +77,19 @@ equation
     Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{150,
             100}})),
 Documentation(info="<html>
- <p>
- This example computes the solar azimuth angle.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 18, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the solar azimuth angle.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 18, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=864000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarAzimuth.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SolarAzimuth;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarHourAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarHourAngle.mo
index d1a1d926b7..117141332f 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarHourAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarHourAngle.mo
@@ -29,21 +29,21 @@ equation
       extent={{-6,3},{-6,3}}));
   annotation (experiment(Tolerance=1e-6, StopTime=86400),
 Documentation(info="<html>
- <p>
- This example computes the solar hour angle,
- which is defined as the angle between the circle
- that passes through an observer, the north pole and the south pole,
- and the circle that passes through the sun, the north and the south pole.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 17, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the solar hour angle,
+which is defined as the angle between the circle
+that passes through an observer, the north pole and the south pole,
+and the circle that passes through the sun, the north and the south pole.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/BaseClasses/Examples/SolarHourAngle.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SolarHourAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/WallSolarAzimuth.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/WallSolarAzimuth.mo
index c643425992..8b07661ba9 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/WallSolarAzimuth.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/WallSolarAzimuth.mo
@@ -47,21 +47,21 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/BaseClasses/Examples/WallSolarAzimuth.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example calculates the wall solar azimuth angle.
- </p>
- </html>",
+<p>
+This example calculates the wall solar azimuth angle.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- Feb 27, 2012, by Michael Wetter:<br/>
- Simplified example by using zenith angle from weather data bus.
- </li>
- <li>
- Feb 01, 2012, by Kaustubh Phalak<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+Feb 27, 2012, by Michael Wetter:<br/>
+Simplified example by using zenith angle from weather data bus.
+</li>
+<li>
+Feb 01, 2012, by Kaustubh Phalak<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WallSolarAzimuth;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/ZenithAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/ZenithAngle.mo
index 9baaa499e0..d1ce6557c6 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/ZenithAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/Examples/ZenithAngle.mo
@@ -55,20 +55,20 @@ equation
       horizontalAlignment=TextAlignment.Right));
   annotation (
   Documentation(info="<html>
- <p>
- This example computes the zenith angle,
- which is the angle between the earth surface normal and the sun's beam.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 17, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the zenith angle,
+which is the angle between the earth surface normal and the sun's beam.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(StartTime=100000, Tolerance=1e-6, StopTime=300000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/BaseClasses/Examples/ZenithAngle.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ZenithAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/IncidenceAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/IncidenceAngle.mo
index e898104b5a..2088fddd71 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/IncidenceAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/IncidenceAngle.mo
@@ -35,33 +35,33 @@ equation
   annotation (
     defaultComponentName="incAng",
     Documentation(info="<html>
- <p>
- This component computes the solar incidence angle on a tilted surface using the solar hour angle and the declination angle as input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- April 27, 2018, by Michael Wetter:<br/>
- Corrected <code>displayUnit</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
- </li>
- <li>
- Dec 7, 2010, by Michael Wetter:<br/>
- Rewrote equation in explicit form to avoid nonlinear equations in room model.
- </li>
- <li>
- May 19, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the solar incidence angle on a tilted surface using the solar hour angle and the declination angle as input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+April 27, 2018, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
+</li>
+<li>
+Dec 7, 2010, by Michael Wetter:<br/>
+Rewrote equation in explicit form to avoid nonlinear equations in room model.
+</li>
+<li>
+May 19, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Bitmap(extent={{-90,-90},{90,90}}, fileName=
@@ -77,6 +77,6 @@ equation
         Text(
           extent={{-98,-42},{-42,-54}},
           textColor={0,0,127},
-          textString="solHouAng")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="solHouAng")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end IncidenceAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarAzimuth.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarAzimuth.mo
index 0b760ead9b..fb67f66326 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarAzimuth.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarAzimuth.mo
@@ -48,43 +48,43 @@ equation
   annotation (
     defaultComponentName="solAzi",
     Documentation(info="<html>
- <p>
- This component computes the solar azimuth angle.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 16, 2021, by Michael Wetter:<br/>
- Removed parameter <code>lat</code> and added an input connector for this quantity.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- June 9, 2020, by David Blum:<br/>
- Reformulated to use one-line if-statements.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1373\">issue 1373</a>.
- </li>
- <li>
- October 13, 2017, by Michael Wetter:<br/>
- Reformulated to use equation rather than algorithm section.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/834\">issue 834</a>.
- </li>
- <li>
- July 5, 2012, by Michael Wetter:<br/>
- Changed model to avoid an event at solar noon.
- </li>
- <li>
- February 28, 2012, by Wangda Zuo:<br/>
- Add solar time conversion since it is removed from <code>solTim</code>.
- </li>
- <li>
- May 18, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the solar azimuth angle.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter <code>lat</code> and added an input connector for this quantity.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+June 9, 2020, by David Blum:<br/>
+Reformulated to use one-line if-statements.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1373\">issue 1373</a>.
+</li>
+<li>
+October 13, 2017, by Michael Wetter:<br/>
+Reformulated to use equation rather than algorithm section.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/834\">issue 834</a>.
+</li>
+<li>
+July 5, 2012, by Michael Wetter:<br/>
+Changed model to avoid an event at solar noon.
+</li>
+<li>
+February 28, 2012, by Wangda Zuo:<br/>
+Add solar time conversion since it is removed from <code>solTim</code>.
+</li>
+<li>
+May 18, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Bitmap(extent={{-90,-90},{90,90}}, fileName=
@@ -108,6 +108,6 @@ equation
         Text(
           extent={{-96,-86},{-54,-96}},
           textColor={0,0,127},
-          textString="lat")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="lat")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SolarAzimuth;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarHourAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarHourAngle.mo
index c2046b68b5..6578df18b5 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarHourAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/SolarHourAngle.mo
@@ -15,26 +15,26 @@ equation
   annotation (
     defaultComponentName="solHouAng",
     Documentation(info="<html>
- <p>
- This component computes the solar hour angle,
- which is defined as the angle between the circle
- that passes through an observer, the north pole and the south pole,
- and the circle that passes through the sun, the north and the south pole.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 17, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the solar hour angle,
+which is defined as the angle between the circle
+that passes through an observer, the north pole and the south pole,
+and the circle that passes through the sun, the north and the south pole.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={  Bitmap(extent={{-90,-90},{90,90}}, fileName=
               "modelica://AixLib/Resources/Images/BoundaryConditions/SolarGeometry/BaseClasses/SolarHourAngle.png"),
                               Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SolarHourAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/WallSolarAzimuth.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/WallSolarAzimuth.mo
index f8c613d026..d482e31d0b 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/WallSolarAzimuth.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/WallSolarAzimuth.mo
@@ -41,31 +41,31 @@ equation
               "modelica://AixLib/Resources/Images/BoundaryConditions/SolarGeometry/BaseClasses/WallSolarAzimuth.png")}),
 defaultComponentName="wallSolAzi",
 Documentation(info="<html>
- <p>
- This block computes the wall solar azimuth angle.
- It is the angle between the projection of the sun ray on a horizontal surface
- and the line perpendicular to the wall. The value of this angle varies from <i>0</i> to <i>180</i> degrees.
- In the northern hemisphere at solar noon, the value of the wall solar azimuth angle is zero if the wall is facing south.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 5, 2012, by Michael Wetter:<br/>
- Decreased <code>deltaX</code> from <i>1e-3</i> to <i>1e-4</i>, as
- the looser tolerance gives sharp changes in
- <a href=\"modelica://AixLib.HeatTransfer.Windows.BaseClasses.Examples.Overhang\">
- AixLib.HeatTransfer.Windows.BaseClasses.Examples.Overhang</a>.
- </li>
- <li>
- February 23, 2012, by Michael Wetter:<br/>
- Guarded against division by zero because the altitude angle can be <i>90</i> degree
- in the tropics, and hence its cosine can take on zero.
- </li>
- <li>
- Feb 01, 2012, by Kaustubh Phalak<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This block computes the wall solar azimuth angle.
+It is the angle between the projection of the sun ray on a horizontal surface
+and the line perpendicular to the wall. The value of this angle varies from <i>0</i> to <i>180</i> degrees.
+In the northern hemisphere at solar noon, the value of the wall solar azimuth angle is zero if the wall is facing south.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 5, 2012, by Michael Wetter:<br/>
+Decreased <code>deltaX</code> from <i>1e-3</i> to <i>1e-4</i>, as
+the looser tolerance gives sharp changes in
+<a href=\"modelica://AixLib.HeatTransfer.Windows.BaseClasses.Examples.Overhang\">
+AixLib.HeatTransfer.Windows.BaseClasses.Examples.Overhang</a>.
+</li>
+<li>
+February 23, 2012, by Michael Wetter:<br/>
+Guarded against division by zero because the altitude angle can be <i>90</i> degree
+in the tropics, and hence its cosine can take on zero.
+</li>
+<li>
+Feb 01, 2012, by Kaustubh Phalak<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WallSolarAzimuth;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/ZenithAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/ZenithAngle.mo
index bcb6cc42a7..71567a2576 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/ZenithAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/ZenithAngle.mo
@@ -26,34 +26,34 @@ equation
   annotation (
     defaultComponentName="zen",
     Documentation(info="<html>
- <p>
- This component computes the zenith angle, which is the angle between the earth surface normal and the sun's beam.
- Input are the solar hour angle and the declination angle.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- January 5, 2015, by Michael Wetter:<br/>
- Updated comment of the input connector as this is used in the weather bus connector.
- This is for
- issue <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">376</a>.
- </li>
- <li>
- Dec 7, 2010, by Michael Wetter:<br/>
- Rewrote equation in explicit form to avoid nonlinear equations in room model.
- </li>
- <li>
- May 17, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the zenith angle, which is the angle between the earth surface normal and the sun's beam.
+Input are the solar hour angle and the declination angle.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+January 5, 2015, by Michael Wetter:<br/>
+Updated comment of the input connector as this is used in the weather bus connector.
+This is for
+issue <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">376</a>.
+</li>
+<li>
+Dec 7, 2010, by Michael Wetter:<br/>
+Rewrote equation in explicit form to avoid nonlinear equations in room model.
+</li>
+<li>
+May 17, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Bitmap(extent={{-86,-88},{94,92}}, fileName=
@@ -69,6 +69,6 @@ equation
         Text(
           extent={{-98,-40},{-22,-58}},
           textColor={0,0,127},
-          textString="solHouAng")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="solHouAng")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ZenithAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthNoEvent.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthNoEvent.mo
index cfc7ab1a36..0c010c09a0 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthNoEvent.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthNoEvent.mo
@@ -13,21 +13,21 @@ algorithm
 
   annotation (
     Documentation(info="<html>
- <p>
- This function is used within
- <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth\">
- AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth</a> 
- to calculate solar azimuth with no events.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 9, 2020 by David Blum:<br/>
- Initial implementation.
- This is for issue
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1373\">#1373</a>. 
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function is used within
+<a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth\">
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth</a> 
+to calculate solar azimuth with no events.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2020 by David Blum:<br/>
+Initial implementation.
+This is for issue
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1373\">#1373</a>. 
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end solarAzimuthNoEvent;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthWithEvent.mo b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthWithEvent.mo
index d8007dbcf1..368ccbbd49 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthWithEvent.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/BaseClasses/solarAzimuthWithEvent.mo
@@ -12,21 +12,21 @@ algorithm
   end if;
   annotation (
     Documentation(info="<html>
- <p>
- This function is used within
- <a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth\">
- AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth</a> 
- to calculate solar azimuth with events.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 9, 2020 by David Blum:<br/>
- Initial implementation.
- This is for issue
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1373\">#1373</a>. 
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function is used within
+<a href=\"modelica://AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth\">
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth</a> 
+to calculate solar azimuth with events.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2020 by David Blum:<br/>
+Initial implementation.
+This is for issue
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1373\">#1373</a>. 
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end solarAzimuthWithEvent;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/Examples/IncidenceAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/Examples/IncidenceAngle.mo
index 0c142e7c4b..c36ec14f2e 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/Examples/IncidenceAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/Examples/IncidenceAngle.mo
@@ -48,31 +48,31 @@ equation
       thickness=0.5));
   annotation (
   Documentation(info="<html>
- <p>
- This example computes the solar incidence angle on tilted surfaces.
- There are fives surfaces, a horizontal surface and a surface
- that faces Norths, East, South and West.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 24, 2015, by Michael Wetter:<br/>
- Assigned azimuth and tilt using the types from
- <a href=\"modelica://AixLib.Types.Tilt\">
- AixLib.Types.Tilt</a>.
- </li>
- <li>
- January 16, 2015, by Michael Wetter:<br/>
- Added surfaces for each orientation.
- </li>
- <li>
- May 19, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the solar incidence angle on tilted surfaces.
+There are fives surfaces, a horizontal surface and a surface
+that faces Norths, East, South and West.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 24, 2015, by Michael Wetter:<br/>
+Assigned azimuth and tilt using the types from
+<a href=\"modelica://AixLib.Types.Tilt\">
+AixLib.Types.Tilt</a>.
+</li>
+<li>
+January 16, 2015, by Michael Wetter:<br/>
+Added surfaces for each orientation.
+</li>
+<li>
+May 19, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=86400),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/Examples/IncidenceAngle.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end IncidenceAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/Examples/ZenithAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/Examples/ZenithAngle.mo
index a7fdc7eae3..58627167b6 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/Examples/ZenithAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/Examples/ZenithAngle.mo
@@ -14,25 +14,25 @@ equation
       thickness=0.5));
   annotation (
   Documentation(info="<html>
- <p>
- This example computes the zenith angle,
- which is the angle between the earth surface normal and the sun beam.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 25, 2012, by Michael Wetter:<br/>
- Changed model to get declination angle and
- solar hour angle from weather bus.
- </li>
- <li>
- May 17, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the zenith angle,
+which is the angle between the earth surface normal and the sun beam.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 25, 2012, by Michael Wetter:<br/>
+Changed model to get declination angle and
+solar hour angle from weather bus.
+</li>
+<li>
+May 17, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(StartTime=100000, Tolerance=1e-6, StopTime=300000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarGeometry/Examples/ZenithAngle.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ZenithAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/IncidenceAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/IncidenceAngle.mo
index 2fb00e712c..721d19894e 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/IncidenceAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/IncidenceAngle.mo
@@ -59,38 +59,38 @@ equation
   annotation (
     defaultComponentName="incAng",
     Documentation(info="<html>
- <p>
- This component computes the solar incidence angle on a tilted surface.
- For a definition of the parameters, see the User's Guide
- <a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">AixLib.BoundaryConditions.UsersGuide</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- November 30, 2011, by Michael Wetter:<br/>
- Removed <code>connect(y, y)</code> statement.
- </li>
- <li>
- February 28, 2011, by Wangda Zuo:<br/>
- Use local civil time instead of clock time.
- </li>
- <li>
- May 19, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the solar incidence angle on a tilted surface.
+For a definition of the parameters, see the User's Guide
+<a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">AixLib.BoundaryConditions.UsersGuide</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+November 30, 2011, by Michael Wetter:<br/>
+Removed <code>connect(y, y)</code> statement.
+</li>
+<li>
+February 28, 2011, by Wangda Zuo:<br/>
+Use local civil time instead of clock time.
+</li>
+<li>
+May 19, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
           textString="%name",
           textColor={0,0,255}), Bitmap(extent={{-90,-90},{90,90}}, fileName=
-              "modelica://AixLib/Resources/Images/BoundaryConditions/SolarGeometry/BaseClasses/IncidenceAngle.png")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+              "modelica://AixLib/Resources/Images/BoundaryConditions/SolarGeometry/BaseClasses/IncidenceAngle.png")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end IncidenceAngle;
diff --git a/AixLib/BoundaryConditions/SolarGeometry/ZenithAngle.mo b/AixLib/BoundaryConditions/SolarGeometry/ZenithAngle.mo
index 96db1b440d..a618341190 100644
--- a/AixLib/BoundaryConditions/SolarGeometry/ZenithAngle.mo
+++ b/AixLib/BoundaryConditions/SolarGeometry/ZenithAngle.mo
@@ -35,37 +35,37 @@ equation
   annotation (
     defaultComponentName="zen",
     Documentation(info="<html>
- <p>
- This component computes the zenith angle,
- which is the angle between the earth surface normal and the sun beam.
- For a definition of the parameters, see the User's Guide
- <a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">
- AixLib.BoundaryConditions.UsersGuide</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- February 25, 2012, by Michael Wetter:<br/>
- Changed model to get declination angle and
- solar hour angle from weather bus.
- </li>
- <li>
- May 17, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the zenith angle,
+which is the angle between the earth surface normal and the sun beam.
+For a definition of the parameters, see the User's Guide
+<a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">
+AixLib.BoundaryConditions.UsersGuide</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+February 25, 2012, by Michael Wetter:<br/>
+Changed model to get declination angle and
+solar hour angle from weather bus.
+</li>
+<li>
+May 17, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
           textString="%name",
           textColor={0,0,255}), Bitmap(extent={{-90,-90},{90,90}}, fileName=
-              "modelica://AixLib/Resources/Images/BoundaryConditions/SolarGeometry/BaseClasses/ZenithAngle.png")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+              "modelica://AixLib/Resources/Images/BoundaryConditions/SolarGeometry/BaseClasses/ZenithAngle.png")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ZenithAngle;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/BrighteningCoefficient.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/BrighteningCoefficient.mo
index 8193eb49f6..f3a441e6d4 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/BrighteningCoefficient.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/BrighteningCoefficient.mo
@@ -113,29 +113,29 @@ equation
   annotation (
     defaultComponentName="briCoe",
     Documentation(info="<html>
- <p>
- This component computes the circumsolar and horizon brightening coefficients.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 27, 2018, by Michael Wetter:<br/>
- Corrected <code>displayUnit</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
- </li>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- May 25, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the circumsolar and horizon brightening coefficients.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 27, 2018, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
+</li>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+May 25, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Text(
@@ -161,6 +161,6 @@ equation
         Text(
           extent={{60,-30},{104,-52}},
           textColor={0,0,127},
-          textString="F2")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="F2")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BrighteningCoefficient;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffuseIsotropic.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffuseIsotropic.mo
index ef6f534c50..0d503ab3f5 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffuseIsotropic.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffuseIsotropic.mo
@@ -30,32 +30,32 @@ equation
   annotation (
     defaultComponentName="HDifTilIso",
     Documentation(info="<html>
- <p>
- This component computes the hemispherical diffuse irradiation on a tilted surface.
- The irradiation is composed of the diffuse horizontal solar irradiation and the irradiation
- that has been reflected by the ground. Both components are adjusted to take into account
- the tilt of the receiving surface.
- </p>
- <h4>References</h4>
- P. Ineichen, R. Perez and R. Seals (1987).
- <i>The Importance of Correct Albedo Determination for Adequately Modeling Energy Received by Tilted Surface</i>,
- Solar Energy, 39(4): 301-305.
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2012, by Wangda Zuo:<br/>
- Separated the contributions from the sky and the ground.
- </li>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the hemispherical diffuse irradiation on a tilted surface.
+The irradiation is composed of the diffuse horizontal solar irradiation and the irradiation
+that has been reflected by the ground. Both components are adjusted to take into account
+the tilt of the receiving surface.
+</p>
+<h4>References</h4>
+P. Ineichen, R. Perez and R. Seals (1987).
+<i>The Importance of Correct Albedo Determination for Adequately Modeling Energy Received by Tilted Surface</i>,
+Solar Energy, 39(4): 301-305.
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2012, by Wangda Zuo:<br/>
+Separated the contributions from the sky and the ground.
+</li>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DiffuseIsotropic;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffusePerez.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffusePerez.mo
index 72e077c9e7..4dd26dd44f 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffusePerez.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DiffusePerez.mo
@@ -56,47 +56,47 @@ equation
   annotation (
     defaultComponentName="HDifTil",
     Documentation(info="<html>
- <p>
- This component computes the hemispherical diffuse irradiation on a tilted surface by using an anisotropic model proposed by Perez.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- P. Ineichen, R. Perez and R. Seals (1987).
- <i>The Importance of Correct Albedo Determination for Adequately Modeling Energy Received by Tilted Surface</i>,
- Solar Energy, 39(4): 301-305.
- </li>
- <li>
- R. Perez, R. Seals, P. Ineichen, R. Stewart and D. Menicucci (1987).
- <i>A New Simplified Version of the Perez Diffuse Irradiance Model for Tilted Surface</i>,
- Solar Energy, 39(3): 221-231.
- </li>
- <li>
- R. Perez, P. Ineichen, R. Seals, J. Michalsky and R. Stewart (1990).
- <i>Modeling Dyalight Availability and Irradiance Componets From Direct and Global Irradiance</i>,
- Solar Energy, 44(5):271-289.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- April 27, 2018, by Michael Wetter:<br/>
- Corrected <code>displayUnit</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
- </li>
- <li>
- June 6, 2012, by Wangda Zuo:<br/>
- Separated the contribution from the sky and the ground.
- </li>
- </ul>
- <ul>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the hemispherical diffuse irradiation on a tilted surface by using an anisotropic model proposed by Perez.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+P. Ineichen, R. Perez and R. Seals (1987).
+<i>The Importance of Correct Albedo Determination for Adequately Modeling Energy Received by Tilted Surface</i>,
+Solar Energy, 39(4): 301-305.
+</li>
+<li>
+R. Perez, R. Seals, P. Ineichen, R. Stewart and D. Menicucci (1987).
+<i>A New Simplified Version of the Perez Diffuse Irradiance Model for Tilted Surface</i>,
+Solar Energy, 39(3): 221-231.
+</li>
+<li>
+R. Perez, P. Ineichen, R. Seals, J. Michalsky and R. Stewart (1990).
+<i>Modeling Dyalight Availability and Irradiance Componets From Direct and Global Irradiance</i>,
+Solar Energy, 44(5):271-289.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+April 27, 2018, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
+</li>
+<li>
+June 6, 2012, by Wangda Zuo:<br/>
+Separated the contribution from the sky and the ground.
+</li>
+</ul>
+<ul>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Text(
@@ -126,6 +126,6 @@ equation
         Text(
           extent={{-52,-76},{-104,-64}},
           textColor={0,0,127},
-          textString="incAng")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="incAng")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DiffusePerez;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DirectTiltedSurface.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DirectTiltedSurface.mo
index 7821b568d8..d62016ec6a 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DirectTiltedSurface.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/DirectTiltedSurface.mo
@@ -19,28 +19,28 @@ equation
   annotation (
     defaultComponentName="HDirTil",
     Documentation(info="<html>
- <p>
- This component computes the direct solar irradiation on a tilted surface.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 27, 2018, by Michael Wetter:<br/>
- Corrected <code>displayUnit</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
- </li>
- <li>
- May 5, 2015, by Filip Jorissen:<br/>
- Converted <code>algorithm</code> section into
- <code>equation</code> section for easier differentiability.
- </li>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the direct solar irradiation on a tilted surface.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 27, 2018, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
+</li>
+<li>
+May 5, 2015, by Filip Jorissen:<br/>
+Converted <code>algorithm</code> section into
+<code>equation</code> section for easier differentiability.
+</li>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Text(
@@ -54,6 +54,6 @@ equation
         Text(
           extent={{-54,-66},{-106,-54}},
           textColor={0,0,127},
-          textString="incAng")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="incAng")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DirectTiltedSurface;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/BrighteningCoefficient.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/BrighteningCoefficient.mo
index bb07931364..2dbcf4a529 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/BrighteningCoefficient.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/BrighteningCoefficient.mo
@@ -91,22 +91,22 @@ equation
       horizontalAlignment=TextAlignment.Right));
   annotation (
 Documentation(info="<html>
- <p>
- This example computes the circumsolar and horizon brightening coefficients.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 25, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the circumsolar and horizon brightening coefficients.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 25, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=8640000),
 __Dymola_Commands(
       file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/BrighteningCoefficient.mos"
       "Simulate and plot"),
     Diagram(coordinateSystem(extent={{-100,-100},{120,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BrighteningCoefficient;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/DiffuseIsotropic.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/DiffuseIsotropic.mo
index 6f2e06e3bf..6fb139b910 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/DiffuseIsotropic.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/DiffuseIsotropic.mo
@@ -34,19 +34,19 @@ equation
       extent={{-6,3},{-6,3}}));
   annotation (
   Documentation(info="<html>
- <p>
- This example computes the hemispherical diffuse irradiation on a tilted surface.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the hemispherical diffuse irradiation on a tilted surface.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StartTime=0, StopTime=8640000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/DiffuseIsotropic.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DiffuseIsotropic;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/RelativeAirMass.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/RelativeAirMass.mo
index 12d8b9f6e0..62b1a1e1ce 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/RelativeAirMass.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/RelativeAirMass.mo
@@ -36,19 +36,19 @@ equation
       horizontalAlignment=TextAlignment.Right));
   annotation (
 Documentation(info="<html>
- <p>
- This example computes the relative air mass for sky brightness.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 07, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the relative air mass for sky brightness.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 07, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StopTime=864000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/RelativeAirMass.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end RelativeAirMass;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyBrightness.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyBrightness.mo
index 17d4ed81a0..61d6e9ff3b 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyBrightness.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyBrightness.mo
@@ -64,25 +64,25 @@ equation
       horizontalAlignment=TextAlignment.Right));
   annotation (
 Documentation(info="<html>
- <p>
- This example computes the sky brightness.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Changed extraterrestrial radiation and added time dependent correlation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- July 07, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the sky brightness.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Changed extraterrestrial radiation and added time dependent correlation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+July 07, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=8640000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyBrightness.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SkyBrightness;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyClearness.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyClearness.mo
index 4fd4e707bb..f4f4a9ef52 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyClearness.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyClearness.mo
@@ -48,20 +48,20 @@ equation
       extent={{-6,3},{-6,3}}));
   annotation (
 Documentation(info="<html>
- <p>
- This example computes the sky clearness.
- </p>
- </html>",
+<p>
+This example computes the sky clearness.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 07, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+July 07, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(StartTime=100000, Tolerance=1e-6, StopTime=3000000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/BaseClasses/Examples/SkyClearness.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SkyClearness;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/PartialSolarIrradiation.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/PartialSolarIrradiation.mo
index 1bfd32d8ff..bd999f3616 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/PartialSolarIrradiation.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/PartialSolarIrradiation.mo
@@ -13,26 +13,26 @@ partial block PartialSolarIrradiation
 
   annotation (
     Documentation(info="<html>
- <p>
- This is a partial model that is used to implement the direct and diffuse irradiation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- Dec. 12, 2010, by Michael Wetter:<br/>
- Changed output signal to avoid ambiguity in blocks that output also other
- quantities such as the incidence angle.
- </li>
- <li>
- Sep. 4, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This is a partial model that is used to implement the direct and diffuse irradiation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Dec. 12, 2010, by Michael Wetter:<br/>
+Changed output signal to avoid ambiguity in blocks that output also other
+quantities such as the incidence angle.
+</li>
+<li>
+Sep. 4, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialSolarIrradiation;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/RelativeAirMass.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/RelativeAirMass.mo
index afe4185ba9..c750a550ed 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/RelativeAirMass.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/RelativeAirMass.mo
@@ -27,45 +27,45 @@ equation
   annotation (
     defaultComponentName="relAirMas",
     Documentation(info="<html>
- <p>
- This component computes the relative air mass for sky brightness.
- </p>
- <h4>References</h4>
- <p>
- R. Perez (1999).
- <i>Fortran Function irrpz.f</i>,
- Emailed by R. Perez to F.C. Winkelmann on May 21, 1999.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:
- Introduced altitude attenuation for relative air mass calculation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, issue 1477</a>.
- </li>
- <li>
- April 27, 2018, by Michael Wetter:<br/>
- Corrected <code>displayUnit</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
- </li>
- <li>
- July 07, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the relative air mass for sky brightness.
+</p>
+<h4>References</h4>
+<p>
+R. Perez (1999).
+<i>Fortran Function irrpz.f</i>,
+Emailed by R. Perez to F.C. Winkelmann on May 21, 1999.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:
+Introduced altitude attenuation for relative air mass calculation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, issue 1477</a>.
+</li>
+<li>
+April 27, 2018, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">IBPSA, issue 912</a>.
+</li>
+<li>
+July 07, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end RelativeAirMass;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyBrightness.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyBrightness.mo
index 208476117a..bb1c3f6fca 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyBrightness.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyBrightness.mo
@@ -26,30 +26,30 @@ equation
   annotation (
     defaultComponentName="skyBri",
     Documentation(info="<html>
- <p>
- This component computes the sky brightness.
- </p>
- <h4>References</h4>
- <p>
- R. Perez, P. Ineichen, R. Seals, J. Michalsky and R. Stewart (1990).
- <i>Modeling Dyalight Availability and Irradiance Componets From Direct and Global Irradiance</i>,
- Solar Energy, 44(5):271-289.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
- Added input connector <code>solTim</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- July 07, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the sky brightness.
+</p>
+<h4>References</h4>
+<p>
+R. Perez, P. Ineichen, R. Seals, J. Michalsky and R. Stewart (1990).
+<i>Modeling Dyalight Availability and Irradiance Componets From Direct and Global Irradiance</i>,
+Solar Energy, 44(5):271-289.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+Added input connector <code>solTim</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+July 07, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Text(
@@ -67,6 +67,6 @@ equation
         Text(
           extent={{-46,-66},{-98,-54}},
           textColor={0,0,127},
-          textString="solTim")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="solTim")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SkyBrightness;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyClearness.mo b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyClearness.mo
index acc2e6b297..d4ffeef7a1 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyClearness.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/BaseClasses/SkyClearness.mo
@@ -5,7 +5,7 @@ block SkyClearness "Sky clearness"
   Modelica.Blocks.Interfaces.RealInput zen(
     quantity="Angle",
     unit="rad",
-    displayUnit="degreeC") "Zenith angle of the sun beam"
+    displayUnit="deg") "Zenith angle of the sun beam"
     annotation (Placement(transformation(extent={{-140,-80},{-100,-40}})));
   Modelica.Blocks.Interfaces.RealInput HDifHor(quantity=
         "RadiantEnergyFluenceRate", unit="W/m2")
@@ -47,59 +47,65 @@ equation
   annotation (
     defaultComponentName="skyCle",
     Documentation(info="<html>
- <p>
- This component computes the sky clearness.
- </p>
- <h4>Implementation</h4>
- <p>
- In the <code>AixLib</code> library, <code>HGloHor</code>
- is always larger than <i>1E-4</i>,
- minus some small undershoot due to regularization. Hence,
- the implementation is not simplified for
- <code>HGloHor &lt; Modelica.Constants.small</code>.
- </p>
- <p>
- The function call
- <code>AixLib.Utilities.Math.Functions.smoothMax</code>
- is such that the regularization is usually not triggered.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
- Changed input connector <code>HGloHor</code> to <code>HDirHor</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Corrected expression for sky clearness.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">issue 1477</a>.
- </li>
- <li>
- September 23, 2016, by Michael Wetter:<br/>
- Changed <code>deltaX</code> from <code>0.1</code> to <code>0.01</code>,
- and also optimized the code.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/521\">issue 521</a>.
- </li>
- <li>
- May 5, 2015, by Michael Wetter:<br/>
- Introduced constant <code>k</code> to reduce number of operations.
- </li>
- <li>
- May 5, 2015, by Filip Jorissen:<br/>
- Converted <code>algorithm</code> section into
- <code>equation</code> section for easier differentiability.
- </li>
- <li>
- July 07, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the sky clearness.
+</p>
+<h4>Implementation</h4>
+<p>
+In the <code>AixLib</code> library, <code>HDirNor</code>
+is always larger than <i>1E-4</i>,
+minus some small undershoot due to regularization. Hence,
+the implementation is not simplified for
+<code>HDirNor &lt; Modelica.Constants.small</code>.
+</p>
+<p>
+The function call
+<code>AixLib.Utilities.Math.Functions.smoothMax</code>
+is such that the regularization is usually not triggered.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 4, 2024, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1848\">IBPSA, #1848</a>.
+</li>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+Changed input connector <code>HGloHor</code> to <code>HDirNor</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Corrected expression for sky clearness.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">issue 1477</a>.
+</li>
+<li>
+September 23, 2016, by Michael Wetter:<br/>
+Changed <code>deltaX</code> from <code>0.1</code> to <code>0.01</code>,
+and also optimized the code.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/521\">issue 521</a>.
+</li>
+<li>
+May 5, 2015, by Michael Wetter:<br/>
+Introduced constant <code>k</code> to reduce number of operations.
+</li>
+<li>
+May 5, 2015, by Filip Jorissen:<br/>
+Converted <code>algorithm</code> section into
+<code>equation</code> section for easier differentiability.
+</li>
+<li>
+July 07, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Text(
@@ -113,10 +119,10 @@ equation
         Text(
           extent={{-48,54},{-100,66}},
           textColor={0,0,127},
-          textString="HGloHor"),
+          textString="HDirNor"),
         Text(
           extent={{-48,-66},{-100,-54}},
           textColor={0,0,127},
-          textString="zen")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="zen")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SkyClearness;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/DiffuseIsotropic.mo b/AixLib/BoundaryConditions/SolarIrradiation/DiffuseIsotropic.mo
index 4f57ce29a6..cf45c909dc 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/DiffuseIsotropic.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/DiffuseIsotropic.mo
@@ -59,40 +59,40 @@ equation
   annotation (
     defaultComponentName="HDifTilIso",
     Documentation(info="<html>
- <p>
- This component computes the hemispherical diffuse irradiation
- on a tilted surface using an isotropic model.
- The irradiation is a sum composed of diffuse solar irradiation and
- radiation reflected by the ground.
- For a definition of the parameters, see the
- <a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">User's Guide</a>.
- </p>
- <h4>References</h4>
- P. Ineichen, R. Perez and R. Seals (1987).
- <i>The Importance of Correct Albedo Determination for Adequately Modeling
- Energy Received by Tilted Surface</i>,
- Solar Energy, 39(4): 301-305.
- </html>",revisions="<html>
- <ul>
- <li>
- November 14, 2015, by Michael Wetter:<br/>
- Added <code>min</code>, <code>max</code> and <code>unit</code>
- attributes for <code>rho</code>.
- </li>
- <li>
- June 6, 2012, by Wangda Zuo:<br/>
- Added contributions from sky and ground that were separated in base class.
- </li>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the hemispherical diffuse irradiation
+on a tilted surface using an isotropic model.
+The irradiation is a sum composed of diffuse solar irradiation and
+radiation reflected by the ground.
+For a definition of the parameters, see the
+<a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">User's Guide</a>.
+</p>
+<h4>References</h4>
+P. Ineichen, R. Perez and R. Seals (1987).
+<i>The Importance of Correct Albedo Determination for Adequately Modeling
+Energy Received by Tilted Surface</i>,
+Solar Energy, 39(4): 301-305.
+</html>", revisions="<html>
+<ul>
+<li>
+November 14, 2015, by Michael Wetter:<br/>
+Added <code>min</code>, <code>max</code> and <code>unit</code>
+attributes for <code>rho</code>.
+</li>
+<li>
+June 6, 2012, by Wangda Zuo:<br/>
+Added contributions from sky and ground that were separated in base class.
+</li>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DiffuseIsotropic;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/DiffusePerez.mo b/AixLib/BoundaryConditions/SolarIrradiation/DiffusePerez.mo
index 6eecae1a48..0d00221bd9 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/DiffusePerez.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/DiffusePerez.mo
@@ -154,61 +154,61 @@ equation
   annotation (
     defaultComponentName="HDifTil",
     Documentation(info="<html>
- <p>
- This component computes the hemispherical diffuse irradiation on a tilted surface using an anisotropic
- sky model proposed by Perez.
- For a definition of the parameters, see the
- <a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">User's Guide</a>.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- P. Ineichen, R. Perez and R. Seals (1987).
- <i>The Importance of Correct Albedo Determination for Adequately Modeling Energy Received by Tilted Surface</i>,
- Solar Energy, 39(4): 301-305.
- </li>
- <li>
- R. Perez, R. Seals, P. Ineichen, R. Stewart and D. Menicucci (1987).
- <i>A New Simplified Version of the Perez Diffuse Irradiance Model for Tilted Surface</i>,
- Solar Energy, 39(3): 221-231.
- </li>
- <li>
- R. Perez, P. Ineichen, R. Seals, J. Michalsky and R. Stewart (1990).
- <i>Modeling Dyalight Availability and Irradiance Componets From Direct and Global Irradiance</i>,
- Solar Energy, 44(5):271-289.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- November 14, 2015, by Michael Wetter:<br/>
- Added <code>min</code>, <code>max</code> and <code>unit</code>
- attributes for <code>rho</code>.
- </li>
- <li>
- June 6, 2012, by Wangda Zuo:<br/>
- Added contributions from sky and ground that were separated in base class.
- </li>
- <li>
- February 25, 2012, by Michael Wetter:<br/>
- Changed component to get zenith angle from weather bus.
- </li>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the hemispherical diffuse irradiation on a tilted surface using an anisotropic
+sky model proposed by Perez.
+For a definition of the parameters, see the
+<a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">User's Guide</a>.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+P. Ineichen, R. Perez and R. Seals (1987).
+<i>The Importance of Correct Albedo Determination for Adequately Modeling Energy Received by Tilted Surface</i>,
+Solar Energy, 39(4): 301-305.
+</li>
+<li>
+R. Perez, R. Seals, P. Ineichen, R. Stewart and D. Menicucci (1987).
+<i>A New Simplified Version of the Perez Diffuse Irradiance Model for Tilted Surface</i>,
+Solar Energy, 39(3): 221-231.
+</li>
+<li>
+R. Perez, P. Ineichen, R. Seals, J. Michalsky and R. Stewart (1990).
+<i>Modeling Dyalight Availability and Irradiance Componets From Direct and Global Irradiance</i>,
+Solar Energy, 44(5):271-289.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+November 14, 2015, by Michael Wetter:<br/>
+Added <code>min</code>, <code>max</code> and <code>unit</code>
+attributes for <code>rho</code>.
+</li>
+<li>
+June 6, 2012, by Wangda Zuo:<br/>
+Added contributions from sky and ground that were separated in base class.
+</li>
+<li>
+February 25, 2012, by Michael Wetter:<br/>
+Changed component to get zenith angle from weather bus.
+</li>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DiffusePerez;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/DirectTiltedSurface.mo b/AixLib/BoundaryConditions/SolarIrradiation/DirectTiltedSurface.mo
index 4ccef75467..027aace2a5 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/DirectTiltedSurface.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/DirectTiltedSurface.mo
@@ -50,40 +50,40 @@ equation
   annotation (
     defaultComponentName="HDirTil",
     Documentation(info="<html>
- <p>
- This component computes the direct solar irradiation on a tilted surface.
- For a definition of the parameters, see the
- <a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">User's Guide</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Removed duplicate instance <code>weaBus</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/461\">
- https://github.com/ibpsa/modelica-ibpsa/issues/461</a>.
- </li>
- <li>
- December 12, 2010, by Michael Wetter:<br/>
- Added incidence angle as output as this is needed for the room model.
- </li>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the direct solar irradiation on a tilted surface.
+For a definition of the parameters, see the
+<a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">User's Guide</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Removed duplicate instance <code>weaBus</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/461\">
+https://github.com/ibpsa/modelica-ibpsa/issues/461</a>.
+</li>
+<li>
+December 12, 2010, by Michael Wetter:<br/>
+Added incidence angle as output as this is needed for the room model.
+</li>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DirectTiltedSurface;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffuseIsotropic.mo b/AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffuseIsotropic.mo
index 9e3a3479a2..ce3aa664e9 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffuseIsotropic.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffuseIsotropic.mo
@@ -57,22 +57,22 @@ equation
       extent={{6,3},{6,3}}));
   annotation (
     Documentation(info="<html>
- <p>
- This example computes the hemispherical diffuse irradiation
- on a roof, wall and a floor, using an isotropic sky model.
- Since the floor only sees the ground,
- it receives the lowest amount of diffuse solar irradiation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example computes the hemispherical diffuse irradiation
+on a roof, wall and a floor, using an isotropic sky model.
+Since the floor only sees the ground,
+it receives the lowest amount of diffuse solar irradiation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(StartTime=1.82304e+07, Tolerance=1e-6, StopTime=1.83168e+07),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/Examples/DiffuseIsotropic.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DiffuseIsotropic;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffusePerez.mo b/AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffusePerez.mo
index bd71a4a49e..ad196827d0 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffusePerez.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/Examples/DiffusePerez.mo
@@ -62,22 +62,22 @@ experiment(StartTime=1.82304e+07, Tolerance=1e-6, StopTime=1.83168e+07),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/Examples/DiffusePerez.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of Perez' model for diffuse solar radiation.
- The three instances of Perez' model compute the diffuse solar
- irradiation on a roof, a wall and a floor.
- Since the floor only sees the ground but not the radiative heat flow that is
- scattered in the atmosphere, it receives the lowest amount of
- diffuse solar irradiation.
- </p>
- </html>",
+<p>
+This model tests the implementation of Perez' model for diffuse solar radiation.
+The three instances of Perez' model compute the diffuse solar
+irradiation on a roof, a wall and a floor.
+Since the floor only sees the ground but not the radiative heat flow that is
+scattered in the atmosphere, it receives the lowest amount of
+diffuse solar irradiation.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DiffusePerez;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/Examples/DirectTiltedSurface.mo b/AixLib/BoundaryConditions/SolarIrradiation/Examples/DirectTiltedSurface.mo
index 961e820e53..93cf3e8e84 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/Examples/DirectTiltedSurface.mo
+++ b/AixLib/BoundaryConditions/SolarIrradiation/Examples/DirectTiltedSurface.mo
@@ -50,19 +50,19 @@ experiment(StartTime=1.82304e+07, Tolerance=1e-6, StopTime=1.83168e+07),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/Examples/DirectTiltedSurface.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the direct solar irradiation received on a ceiling, a wall and a floor.
- The assert statement will stop the simulation if the floor receives
- any direct solar irradiation.
- </p>
- </html>",
+<p>
+This model tests the direct solar irradiation received on a ceiling, a wall and a floor.
+The assert statement will stop the simulation if the floor receives
+any direct solar irradiation.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 24, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 24, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DirectTiltedSurface;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/Examples/GlobalPerezTiltedSurface.mo b/AixLib/BoundaryConditions/SolarIrradiation/Examples/GlobalPerezTiltedSurface.mo
new file mode 100644
index 0000000000..49ef9d2104
--- /dev/null
+++ b/AixLib/BoundaryConditions/SolarIrradiation/Examples/GlobalPerezTiltedSurface.mo
@@ -0,0 +1,86 @@
+within AixLib.BoundaryConditions.SolarIrradiation.Examples;
+model GlobalPerezTiltedSurface
+  "Test model for global solar irradiation on a tilted surface with diffuse
+  irradiation calculation based on Perez"
+  extends Modelica.Icons.Example;
+
+  parameter Real rho=0.2 "Ground reflectance";
+
+  WeatherData.ReaderTMY3 weaDat(filNam=
+        Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    annotation (Placement(transformation(extent={{-40,0},{-20,20}})));
+
+  AixLib.BoundaryConditions.SolarIrradiation.GlobalPerezTiltedSurface HGloRoo(
+    til=AixLib.Types.Tilt.Ceiling,
+    azi=0.78539816339745,
+    rho=rho)
+    "Diffuse irradiation on roof"
+    annotation (Placement(transformation(extent={{40,0},{60,20}})));
+  AixLib.BoundaryConditions.SolarIrradiation.GlobalPerezTiltedSurface HGloFlo(
+    til=AixLib.Types.Tilt.Floor,
+    azi=0.78539816339745,
+    rho=rho)
+    "Diffuse irradiation on floor"
+    annotation (Placement(transformation(extent={{40,-80},{60,-60}})));
+  AixLib.BoundaryConditions.SolarIrradiation.GlobalPerezTiltedSurface HGloWal(
+    til=AixLib.Types.Tilt.Wall,
+    azi=0.78539816339745,
+    rho=rho)
+    "Diffuse irradiation on wall"
+    annotation (Placement(transformation(extent={{40,-40},{60,-20}})));
+  WeatherData.Bus weaBus
+    "Weather data bus"
+    annotation (Placement(
+        transformation(extent={{1,-1},{21,21}}), iconTransformation(extent={{20,20},
+            {21,21}})));
+equation
+  connect(weaDat.weaBus,weaBus)  annotation (Line(
+      points={{-20,10},{11,10}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(weaBus,HGloRoo. weaBus) annotation (Line(
+      points={{11,10},{40,10}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      textString="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}}));
+  connect(weaBus,HGloFlo. weaBus) annotation (Line(
+      points={{11,10},{30,10},{30,-70},{40,-70}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      textString="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}}));
+  connect(weaBus,HGloWal. weaBus) annotation (Line(
+      points={{11,10},{30,10},{30,-30},{40,-30}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      textString="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}}));
+  annotation (
+  experiment(StartTime=1.82304e+07, Tolerance=1e-6, StopTime=1.83168e+07),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/Examples/GlobalPerezTiltedSurface.mos"
+        "Simulate and plot"),
+  Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>This model tests the implementation of global irradiation computation based on Perez&apos; model for diffuse solar radiation.</p>
+<p>The three instances of the model compute the global solar irradiation on a roof, a wall and a floor.</p>
+<p>Since the floor only sees the ground but not the radiative heat flow that is scattered in the atmosphere,
+it receives the lowest amount of diffuse and global solar irradiation.</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+Nov 14, 2022, by Laura Maier:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GlobalPerezTiltedSurface;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/Examples/package.order b/AixLib/BoundaryConditions/SolarIrradiation/Examples/package.order
index f9781aef7c..4d6c798149 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/Examples/package.order
+++ b/AixLib/BoundaryConditions/SolarIrradiation/Examples/package.order
@@ -1,3 +1,4 @@
 DiffuseIsotropic
 DiffusePerez
 DirectTiltedSurface
+GlobalPerezTiltedSurface
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/GlobalPerezTiltedSurface.mo b/AixLib/BoundaryConditions/SolarIrradiation/GlobalPerezTiltedSurface.mo
new file mode 100644
index 0000000000..e2c74e082d
--- /dev/null
+++ b/AixLib/BoundaryConditions/SolarIrradiation/GlobalPerezTiltedSurface.mo
@@ -0,0 +1,71 @@
+within AixLib.BoundaryConditions.SolarIrradiation;
+block GlobalPerezTiltedSurface
+  "Global solar irradiation on a tilted surface with diffuse irradiation calculation following Perez"
+  extends
+    AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.PartialSolarIrradiation;
+  parameter Modelica.Units.SI.Angle azi "Surface azimuth";
+  parameter Real rho=0.2 "Ground reflectance";
+  parameter Boolean outSkyCon=false
+    "Output contribution of diffuse irradiation from sky";
+  parameter Boolean outGroCon=false
+    "Output contribution of diffuse irradiation from ground";
+  DiffusePerez HDifTil(
+    final til=til,
+    final rho=rho,
+    final azi=azi,
+    final outSkyCon=outSkyCon,
+    final outGroCon=outGroCon)
+    "Diffuse irradiation on tilted surface"
+    annotation (Placement(transformation(extent={{-40,20},{0,60}})));
+  DirectTiltedSurface HDirTil(
+    final til=til,
+    final azi=azi)
+    "Direct irradiation on tilted surface"
+    annotation (Placement(transformation(extent={{-40,-60},{0,-20}})));
+  Modelica.Blocks.Math.Add HGloTil(
+      final k1=1,
+      final k2=1)
+    "Global irradiation on tilted surface"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+
+equation
+  connect(weaBus, HDifTil.weaBus) annotation (Line(
+      points={{-100,0},{-100,40},{-40,40}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(weaBus, HDirTil.weaBus) annotation (Line(
+      points={{-100,0},{-100,-40},{-40,-40}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(HDifTil.H, HGloTil.u1) annotation (Line(points={{2,40},{26,40},{26,6},{38,
+          6}},            color={0,0,127}));
+  connect(HDirTil.H, HGloTil.u2) annotation (Line(points={{2,-40},{26,-40},{26,-6},
+          {38,-6}}, color={0,0,127}));
+  connect(HGloTil.y, H) annotation (Line(points={{61,0},{110,0}}, color={0,0,127}));
+  annotation (
+    defaultComponentName = "HGloTil",
+    Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+This component computes the hemispherical direct and diffuse irradiation on a tilted surface
+and outputs the global irradiation.
+</p>
+<p>
+It uses an anisotropic sky model proposed by Perez for the diffuse irradiation computation.
+</p>
+<p>
+For a definition of the parameters, see the
+<a href=\"modelica://AixLib.BoundaryConditions.UsersGuide\">
+AixLib.BoundaryConditions.UsersGuide</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Nov 14, 2022, by Laura Maier:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GlobalPerezTiltedSurface;
diff --git a/AixLib/BoundaryConditions/SolarIrradiation/package.order b/AixLib/BoundaryConditions/SolarIrradiation/package.order
index dc5b64ea25..4a22e7f5b2 100644
--- a/AixLib/BoundaryConditions/SolarIrradiation/package.order
+++ b/AixLib/BoundaryConditions/SolarIrradiation/package.order
@@ -1,5 +1,6 @@
 DiffuseIsotropic
 DiffusePerez
 DirectTiltedSurface
+GlobalPerezTiltedSurface
 Examples
 BaseClasses
diff --git a/AixLib/BoundaryConditions/Types.mo b/AixLib/BoundaryConditions/Types.mo
index 4170ad2d46..e3ef206fab 100644
--- a/AixLib/BoundaryConditions/Types.mo
+++ b/AixLib/BoundaryConditions/Types.mo
@@ -6,17 +6,17 @@ package Types "Package with type definitions"
       Parameter "Use parameter",
       Input "Use input connector") "Enumeration to define data source"
         annotation(Documentation(info="<html>
- <p>
- Enumeration to define the data source used in the weather data reader.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 20, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Enumeration to define the data source used in the weather data reader.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 20, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 
   type RadiationDataSource = enumeration(
       File "Use data from file",
@@ -28,17 +28,17 @@ package Types "Package with type definitions"
         "Direct normal and global horizontal radiation from connector")
     "Enumeration to define solar radiation data source"
         annotation(Documentation(info="<html>
- <p>
- Enumeration to define the data source used in the weather data reader.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 13, 2012, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Enumeration to define the data source used in the weather data reader.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 13, 2012, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   type SkyTemperatureCalculation = enumeration(
       HorizontalRadiation
         "Use horizontal irradiation",
@@ -46,20 +46,20 @@ package Types "Package with type definitions"
         "Use dry-bulb and dew-point temperatures and sky cover")
     "Enumeration for computation of sky temperature" annotation (Documentation(
         info =                 "<html>
- <p>
- Enumeration to define the method used to compute the sky temperature.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 3, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Enumeration to define the method used to compute the sky temperature.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 
 annotation (preferredView="info", Documentation(info="<html>
- This package contains type definitions.
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This package contains type definitions.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Types;
diff --git a/AixLib/BoundaryConditions/UsersGuide.mo b/AixLib/BoundaryConditions/UsersGuide.mo
index c5bba1dddc..a2c8a6ab8a 100644
--- a/AixLib/BoundaryConditions/UsersGuide.mo
+++ b/AixLib/BoundaryConditions/UsersGuide.mo
@@ -78,7 +78,7 @@ Note that a ceiling has a tilt of <i>0</i>
 <!-- @include_Buildings
 , and also the solar collector models
 in
-<a href=\"AixLib.Fluid.SolarCollectors\">AixLib.Fluid.SolarCollectors</a>
+<a href=\"modelica://AixLib.Fluid.SolarCollectors\">AixLib.Fluid.SolarCollectors</a>
 require a tilt of <i>0</i>
 -->
 if they are facing straight upwards.
diff --git a/AixLib/BoundaryConditions/Validation/BESTEST/WD100.mo b/AixLib/BoundaryConditions/Validation/BESTEST/WD100.mo
index 88badfa6d1..a3828c6d50 100644
--- a/AixLib/BoundaryConditions/Validation/BESTEST/WD100.mo
+++ b/AixLib/BoundaryConditions/Validation/BESTEST/WD100.mo
@@ -1,4 +1,4 @@
-within AixLib.BoundaryConditions.Validation.BESTEST;
+within AixLib.BoundaryConditions.Validation.BESTEST;
 model WD100
   "Test model for BESTEST weather data: base case"
   extends Modelica.Icons.Example;
@@ -132,62 +132,62 @@ equation
       file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/Validation/BESTEST/WD100.mos" "Simulate and plot"),
     Documentation(
       info="<html>
- <h4>WD100: Base Case</h4>
- <p>Weather data file : WD100.epw</p>
- <p><i>Table 1: Site Data for Weather file WD100.epw</i></p>
- <table summary=\"Site Data for Weather file WD100.epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
- <td><p>Latitude</p></td>
- <td><p>39.833&deg; north</p></td>
- </tr>
- <tr>
- <td><p>Longitude</p></td>
- <td><p>104.65&deg; west</p></td>
- </tr>
- <tr>
- <td><p>Altitude</p></td>
- <td><p>1650 m</p></td>
- </tr>
- <tr>
- <td><p>Time Zone</p></td>
- <td><p>-7</p></td>
- </tr>
- </table>
- <p>This model is a template for all the other test cases.
- It allows to extrapolate all the weather data from the Reader TMY3 for a specific location, incliation and azimuth.
- The model
- <a href=\"modelica://AixLib.BoundaryConditions.Validation.IsotropicAndPerezDiffuseRadiation\">AixLib.BoundaryConditions.Validation.IsotropicAndPerezDiffuseRadiation</a>
- outputs radiation data using the available Isotropic and Perez methodlogies.
- The sky temperature is calculated using both the Horizontal radiation model,
- from data reader weaBusHorRad and the dew point temperature plus sky cover model from the datareader weaBusSkyCovDewTem.</p>
- </html>",
+<h4>WD100: Base Case</h4>
+<p>Weather data file : WD100.epw</p>
+<p><i>Table 1: Site Data for Weather file WD100.epw</i></p>
+<table summary=\"Site Data for Weather file WD100.epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
+<td><p>Latitude</p></td>
+<td><p>39.833&deg; north</p></td>
+</tr>
+<tr>
+<td><p>Longitude</p></td>
+<td><p>104.65&deg; west</p></td>
+</tr>
+<tr>
+<td><p>Altitude</p></td>
+<td><p>1650 m</p></td>
+</tr>
+<tr>
+<td><p>Time Zone</p></td>
+<td><p>-7</p></td>
+</tr>
+</table>
+<p>This model is a template for all the other test cases.
+It allows to extrapolate all the weather data from the Reader TMY3 for a specific location, incliation and azimuth.
+The model
+<a href=\"modelica://AixLib.BoundaryConditions.Validation.IsotropicAndPerezDiffuseRadiation\">AixLib.BoundaryConditions.Validation.IsotropicAndPerezDiffuseRadiation</a>
+outputs radiation data using the available Isotropic and Perez methodlogies.
+The sky temperature is calculated using both the Horizontal radiation model,
+from data reader weaBusHorRad and the dew point temperature plus sky cover model from the datareader weaBusSkyCovDewTem.</p>
+</html>",
       revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- March 11, 2020, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- <li>
- April 14, 2020, by Ettore Zanetti:<br/>
- Rework after comments from pull request
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Added altitude to parameters.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+March 11, 2020, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+<li>
+April 14, 2020, by Ettore Zanetti:<br/>
+Rework after comments from pull request
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Added altitude to parameters.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WD100;
diff --git a/AixLib/BoundaryConditions/Validation/BESTEST/WD200.mo b/AixLib/BoundaryConditions/Validation/BESTEST/WD200.mo
index ed6f519f3b..e607eca1da 100644
--- a/AixLib/BoundaryConditions/Validation/BESTEST/WD200.mo
+++ b/AixLib/BoundaryConditions/Validation/BESTEST/WD200.mo
@@ -18,49 +18,49 @@ model WD200
       file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/Validation/BESTEST/WD200.mos" "Simulate and plot"),
     Documentation(
       revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- March 11, 2020, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- <li>
- April 14, 2020, by Ettore Zanetti:<br/>
- Rework after comments from pull request
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+March 11, 2020, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+<li>
+April 14, 2020, by Ettore Zanetti:<br/>
+Rework after comments from pull request
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
+</li>
+</ul>
+</html>",
       info="<html>
- <h4>WD200: Low Elevation, Hot and Humid Case.</h4>
- <p>Weather data file : WD200.epw</p>
- <p><i>Table 1: Site Data for Weather file WD200.epw</i></p>
- <table summary=\"Site Data for Weather file WD200.epw\"cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
- <td><p>Latitude</p></td>
- <td><p>33.633&deg; north</p></td>
- </tr>
- <tr>
- <td><p>Longitude</p></td>
- <td><p>84.433&deg; west</p></td>
- </tr>
- <tr>
- <td><p>Altitude</p></td>
- <td><p>308 m</p></td>
- </tr>
- <tr>
- <td><p>Time Zone</p></td>
- <td><p>-5</p></td>
- </tr>
- </table>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<h4>WD200: Low Elevation, Hot and Humid Case.</h4>
+<p>Weather data file : WD200.epw</p>
+<p><i>Table 1: Site Data for Weather file WD200.epw</i></p>
+<table summary=\"Site Data for Weather file WD200.epw\"cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
+<td><p>Latitude</p></td>
+<td><p>33.633&deg; north</p></td>
+</tr>
+<tr>
+<td><p>Longitude</p></td>
+<td><p>84.433&deg; west</p></td>
+</tr>
+<tr>
+<td><p>Altitude</p></td>
+<td><p>308 m</p></td>
+</tr>
+<tr>
+<td><p>Time Zone</p></td>
+<td><p>-5</p></td>
+</tr>
+</table>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WD200;
diff --git a/AixLib/BoundaryConditions/Validation/BESTEST/WD300.mo b/AixLib/BoundaryConditions/Validation/BESTEST/WD300.mo
index 2ab80094f7..954568eea1 100644
--- a/AixLib/BoundaryConditions/Validation/BESTEST/WD300.mo
+++ b/AixLib/BoundaryConditions/Validation/BESTEST/WD300.mo
@@ -18,49 +18,49 @@ model WD300
       file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/Validation/BESTEST/WD300.mos" "Simulate and plot"),
     Documentation(
       revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- March 11, 2020, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- <li>
- April 14, 2020, by Ettore Zanetti:<br/>
- Rework after comments from pull request
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+March 11, 2020, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+<li>
+April 14, 2020, by Ettore Zanetti:<br/>
+Rework after comments from pull request
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
+</li>
+</ul>
+</html>",
       info="<html>
- <h4>WD300: Southern Hemisphere Case</h4>
- <p>Weather data file : WD300.epw</p>
- <p><i>Table 1: Site Data for Weather file WD300.epw</i></p>
- <table summary=\"Site Data for Weather file WD300.epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
- <td><p>Latitude</p></td>
- <td><p>33.393&deg; south</p></td>
- </tr>
- <tr>
- <td><p>Longitude</p></td>
- <td><p>70.786&deg; west</p></td>
- </tr>
- <tr>
- <td><p>Altitude</p></td>
- <td><p>474 m</p></td>
- </tr>
- <tr>
- <td><p>Time Zone</p></td>
- <td><p>-4</p></td>
- </tr>
- </table>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<h4>WD300: Southern Hemisphere Case</h4>
+<p>Weather data file : WD300.epw</p>
+<p><i>Table 1: Site Data for Weather file WD300.epw</i></p>
+<table summary=\"Site Data for Weather file WD300.epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
+<td><p>Latitude</p></td>
+<td><p>33.393&deg; south</p></td>
+</tr>
+<tr>
+<td><p>Longitude</p></td>
+<td><p>70.786&deg; west</p></td>
+</tr>
+<tr>
+<td><p>Altitude</p></td>
+<td><p>474 m</p></td>
+</tr>
+<tr>
+<td><p>Time Zone</p></td>
+<td><p>-4</p></td>
+</tr>
+</table>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WD300;
diff --git a/AixLib/BoundaryConditions/Validation/BESTEST/WD400.mo b/AixLib/BoundaryConditions/Validation/BESTEST/WD400.mo
index 0a5287038b..0cc9f8f83c 100644
--- a/AixLib/BoundaryConditions/Validation/BESTEST/WD400.mo
+++ b/AixLib/BoundaryConditions/Validation/BESTEST/WD400.mo
@@ -18,49 +18,49 @@ model WD400
       file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/Validation/BESTEST/WD400.mos" "Simulate and plot"),
     Documentation(
       revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- March 11, 2020, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- <li>
- April 14, 2020, by Ettore Zanetti:<br/>
- Rework after comments from pull request
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+March 11, 2020, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+<li>
+April 14, 2020, by Ettore Zanetti:<br/>
+Rework after comments from pull request
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
+</li>
+</ul>
+</html>",
       info="<html>
- <h4>WD400: High Latitude Case</h4>
- <p>Weather data file : WD400.epw</p>
- <p><i>Table 1: Site Data for Weather file WD400.epw</i></p>
- <table summary=\"Site Data for Weather file WD400.epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
- <td><p>Latitude</p></td>
- <td><p>71.286&deg; north</p></td>
- </tr>
- <tr>
- <td><p>Longitude</p></td>
- <td><p>156.767&deg; west</p></td>
- </tr>
- <tr>
- <td><p>Altitude</p></td>
- <td><p>10 m</p></td>
- </tr>
- <tr>
- <td><p>Time Zone</p></td>
- <td><p>-9</p></td>
- </tr>
- </table>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<h4>WD400: High Latitude Case</h4>
+<p>Weather data file : WD400.epw</p>
+<p><i>Table 1: Site Data for Weather file WD400.epw</i></p>
+<table summary=\"Site Data for Weather file WD400.epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
+<td><p>Latitude</p></td>
+<td><p>71.286&deg; north</p></td>
+</tr>
+<tr>
+<td><p>Longitude</p></td>
+<td><p>156.767&deg; west</p></td>
+</tr>
+<tr>
+<td><p>Altitude</p></td>
+<td><p>10 m</p></td>
+</tr>
+<tr>
+<td><p>Time Zone</p></td>
+<td><p>-9</p></td>
+</tr>
+</table>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WD400;
diff --git a/AixLib/BoundaryConditions/Validation/BESTEST/WD500.mo b/AixLib/BoundaryConditions/Validation/BESTEST/WD500.mo
index 44e004763a..900861df55 100644
--- a/AixLib/BoundaryConditions/Validation/BESTEST/WD500.mo
+++ b/AixLib/BoundaryConditions/Validation/BESTEST/WD500.mo
@@ -18,49 +18,49 @@ model WD500
       file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/Validation/BESTEST/WD500.mos" "Simulate and plot"),
     Documentation(
       revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- March 11, 2020, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- <li>
- April 14, 2020, by Ettore Zanetti:<br/>
- Rework after comments from pull request
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+March 11, 2020, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+<li>
+April 14, 2020, by Ettore Zanetti:<br/>
+Rework after comments from pull request
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Updated weather file as explained in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1478\">#1478</a>.
+</li>
+</ul>
+</html>",
       info="<html>
- <h4>WD500: Time Zone Case</h4>
- <p>Weather data file : WD500.epw</p>
- <p><i>Table 1: Site Data for Weather file WD500epw</i></p>
- <table summary=\"Site Data for Weather file WD500epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
- <td><p>Latitude</p></td>
- <td><p>28.567&deg; north</p></td>
- </tr>
- <tr>
- <td><p>Longitude</p></td>
- <td><p>77.103&deg; east</p></td>
- </tr>
- <tr>
- <td><p>Altitude</p></td>
- <td><p>236.9 m</p></td>
- </tr>
- <tr>
- <td><p>Time Zone</p></td>
- <td><p>5.5</p></td>
- </tr>
- </table>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<h4>WD500: Time Zone Case</h4>
+<p>Weather data file : WD500.epw</p>
+<p><i>Table 1: Site Data for Weather file WD500epw</i></p>
+<table summary=\"Site Data for Weather file WD500epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
+<td><p>Latitude</p></td>
+<td><p>28.567&deg; north</p></td>
+</tr>
+<tr>
+<td><p>Longitude</p></td>
+<td><p>77.103&deg; east</p></td>
+</tr>
+<tr>
+<td><p>Altitude</p></td>
+<td><p>236.9 m</p></td>
+</tr>
+<tr>
+<td><p>Time Zone</p></td>
+<td><p>5.5</p></td>
+</tr>
+</table>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WD500;
diff --git a/AixLib/BoundaryConditions/Validation/BESTEST/WD600.mo b/AixLib/BoundaryConditions/Validation/BESTEST/WD600.mo
index f23d969b82..37ca543f4d 100644
--- a/AixLib/BoundaryConditions/Validation/BESTEST/WD600.mo
+++ b/AixLib/BoundaryConditions/Validation/BESTEST/WD600.mo
@@ -18,45 +18,45 @@ model WD600
       file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/Validation/BESTEST/WD600.mos" "Simulate and plot"),
     Documentation(
       revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- March 11, 2020, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- <li>
- April 14, 2020, by Ettore Zanetti:<br/>
- Rework after comments from pull request
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+March 11, 2020, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+<li>
+April 14, 2020, by Ettore Zanetti:<br/>
+Rework after comments from pull request
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
+</li>
+</ul>
+</html>",
       info="<html>
- <h4>WD600: Ground Reflactance</h4>
- <p>Weather data file : WD600.epw</p>
- <p><i>Table 1: Site Data for Weather file WD600.epw</i></p>
- <table summary=\"Site Data for Weather file WD600.epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
- <td><p>Latitude</p></td>
- <td><p>39.833&deg; north</p></td>
- </tr>
- <tr>
- <td><p>Longitude</p></td>
- <td><p>104.65&deg; west</p></td>
- </tr>
- <tr>
- <td><p>Altitude</p></td>
- <td><p>1650 m</p></td>
- </tr>
- <tr>
- <td><p>Time Zone</p></td>
- <td><p>-7</p></td>
- </tr>
- </table>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<h4>WD600: Ground Reflactance</h4>
+<p>Weather data file : WD600.epw</p>
+<p><i>Table 1: Site Data for Weather file WD600.epw</i></p>
+<table summary=\"Site Data for Weather file WD600.epw\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\"><tr>
+<td><p>Latitude</p></td>
+<td><p>39.833&deg; north</p></td>
+</tr>
+<tr>
+<td><p>Longitude</p></td>
+<td><p>104.65&deg; west</p></td>
+</tr>
+<tr>
+<td><p>Altitude</p></td>
+<td><p>1650 m</p></td>
+</tr>
+<tr>
+<td><p>Time Zone</p></td>
+<td><p>-7</p></td>
+</tr>
+</table>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WD600;
diff --git a/AixLib/BoundaryConditions/Validation/IsotropicAndPerezDiffuseRadiation.mo b/AixLib/BoundaryConditions/Validation/IsotropicAndPerezDiffuseRadiation.mo
index b16d907a41..938f1a5ad4 100644
--- a/AixLib/BoundaryConditions/Validation/IsotropicAndPerezDiffuseRadiation.mo
+++ b/AixLib/BoundaryConditions/Validation/IsotropicAndPerezDiffuseRadiation.mo
@@ -68,41 +68,41 @@ equation
         preserveAspectRatio=false)),
     Documentation(
       revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Added altitude to parameters.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- October 25, 2020, by Ettore Zanetti:<br/>
- Updated comments for variable descriptions
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1351\">#1351</a>.
- </li>
- <li>
- April 14, 2020, by Ettore Zanetti:<br/>
- Rework after comments from pull request
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
- </li>
- <li>
- March 11, 2020, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Removed parameter <code>lat</code> as it is now obtained from the weather data bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Added altitude to parameters.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+October 25, 2020, by Ettore Zanetti:<br/>
+Updated comments for variable descriptions
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1351\">#1351</a>.
+</li>
+<li>
+April 14, 2020, by Ettore Zanetti:<br/>
+Rework after comments from pull request
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1339\">#1339</a>.
+</li>
+<li>
+March 11, 2020, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+</ul>
+</html>",
       info="<html>
- <p>
- This model outputs the global radiation with a certain inclination and orientation
- using the isotropic sky model and the Perez sky model. The variable <code>H</code> is
- the global radiation calculated using the isotropic sky model, while <code>HPer</code> is
- the global radiation calculated using the Perez sky model.</p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the global radiation with a certain inclination and orientation
+using the isotropic sky model and the Perez sky model. The variable <code>H</code> is
+the global radiation calculated using the isotropic sky model, while <code>HPer</code> is
+the global radiation calculated using the Perez sky model.</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IsotropicAndPerezDiffuseRadiation;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckBlackBodySkyTemperature.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckBlackBodySkyTemperature.mo
index d5b9ee9368..559e9b0dbd 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckBlackBodySkyTemperature.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckBlackBodySkyTemperature.mo
@@ -29,31 +29,31 @@ equation
   annotation (
     defaultComponentName="cheSkyBlaBodTem",
     Documentation(info="<html>
- <p>
- This component checks the value of the black-body sky temperature.
- If the temperature is outside <code>TMin</code> and <code>TMax</code>,
- the simulation will stop with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Added <code>noEvent</code> and removed output connector.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1340\">#1340</a>.
- </li>
- <li>
- January 31, 2020 by Filip Jorissen:<br/>
- Improved error message.
- </li>
- <li>
- January 5, 2015 by Michael Wetter:<br/>
- First implementation, based on
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.CheckTemperature\">
- AixLib.BoundaryConditions.WeatherData.BaseClasses.CheckTemperature</a>.
- This was implemented to get the corrected documentation string in the weather bus connector.
- </li>
- </ul>
- </html>"),
+<p>
+This component checks the value of the black-body sky temperature.
+If the temperature is outside <code>TMin</code> and <code>TMax</code>,
+the simulation will stop with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Added <code>noEvent</code> and removed output connector.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1340\">#1340</a>.
+</li>
+<li>
+January 31, 2020 by Filip Jorissen:<br/>
+Improved error message.
+</li>
+<li>
+January 5, 2015 by Michael Wetter:<br/>
+First implementation, based on
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.CheckTemperature\">
+AixLib.BoundaryConditions.WeatherData.BaseClasses.CheckTemperature</a>.
+This was implemented to get the corrected documentation string in the weather bus connector.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Ellipse(
@@ -77,6 +77,6 @@ equation
           lineThickness=0.5),
         Line(
           points={{-12,40},{-12,-45}},
-          thickness=0.5)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          thickness=0.5)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckBlackBodySkyTemperature;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDewPointTemperature.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDewPointTemperature.mo
index 8ea26e1019..63eec02d22 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDewPointTemperature.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDewPointTemperature.mo
@@ -26,36 +26,36 @@ equation
   annotation (
     defaultComponentName="cheTem",
     Documentation(info="<html>
- <p>
- This component checks the value of temperature.
- If the temperature is outside <code>TMin</code> and <code>TMax</code>,
- the simulation will stop with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Added <code>noEvent</code>.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1340\">#1340</a>.
- </li>
- <li>
- January 31, 2020 by Filip Jorissen:<br/>
- Improved error message.
- </li>
- <li>
- October 27, 2011, by Wangda Zuo:<br/>
- Delete the unit conversion part and name it from ConvertTemperature to CheckTemperature.
- </li>
- <li>
- March 23, 2011, by Michael Wetter:<br/>
- Set <code>displayUnit</code> argument for temperature output signal.
- </li>
- <li>
- July 08, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component checks the value of temperature.
+If the temperature is outside <code>TMin</code> and <code>TMax</code>,
+the simulation will stop with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Added <code>noEvent</code>.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1340\">#1340</a>.
+</li>
+<li>
+January 31, 2020 by Filip Jorissen:<br/>
+Improved error message.
+</li>
+<li>
+October 27, 2011, by Wangda Zuo:<br/>
+Delete the unit conversion part and name it from ConvertTemperature to CheckTemperature.
+</li>
+<li>
+March 23, 2011, by Michael Wetter:<br/>
+Set <code>displayUnit</code> argument for temperature output signal.
+</li>
+<li>
+July 08, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Ellipse(
@@ -79,6 +79,6 @@ equation
           lineThickness=0.5),
         Line(
           points={{-14,44},{-14,-41}},
-          thickness=0.5)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          thickness=0.5)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckDewPointTemperature;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDryBulbTemperature.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDryBulbTemperature.mo
index 3eaf876b96..a97d79fc45 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDryBulbTemperature.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckDryBulbTemperature.mo
@@ -26,36 +26,36 @@ equation
   annotation (
     defaultComponentName="cheTem",
     Documentation(info="<html>
- <p>
- This component checks the value of the dry bulb temperature.
- If the temperature is outside <code>TMin</code> and <code>TMax</code>,
- the simulation will stop with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Added <code>noEvent</code>.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1340\">#1340</a>.
- </li>
- <li>
- January 31, 2020 by Filip Jorissen:<br/>
- Improved error message.
- </li>
- <li>
- October 27, 2011, by Wangda Zuo:<br/>
- Delete the unit conversion part and name it from ConvertTemperature to CheckTemperature.
- </li>
- <li>
- March 23, 2011, by Michael Wetter:<br/>
- Set <code>displayUnit</code> argument for temperature output signal.
- </li>
- <li>
- July 08, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component checks the value of the dry bulb temperature.
+If the temperature is outside <code>TMin</code> and <code>TMax</code>,
+the simulation will stop with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Added <code>noEvent</code>.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1340\">#1340</a>.
+</li>
+<li>
+January 31, 2020 by Filip Jorissen:<br/>
+Improved error message.
+</li>
+<li>
+October 27, 2011, by Wangda Zuo:<br/>
+Delete the unit conversion part and name it from ConvertTemperature to CheckTemperature.
+</li>
+<li>
+March 23, 2011, by Michael Wetter:<br/>
+Set <code>displayUnit</code> argument for temperature output signal.
+</li>
+<li>
+July 08, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Ellipse(
@@ -79,6 +79,6 @@ equation
           lineThickness=0.5),
         Line(
           points={{-10,46},{-10,-39}},
-          thickness=0.5)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          thickness=0.5)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckDryBulbTemperature;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckPressure.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckPressure.mo
index 5922cad77f..f4939b7b19 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckPressure.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/CheckPressure.mo
@@ -20,30 +20,30 @@ equation
   annotation (
     defaultComponentName="chePre",
     Documentation(info="<html>
- <p>
- This component ensures that the interpolated pressure is between <i>31,000</i> Pa and <i>120,000</i> Pa.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Added <code>noEvent</code> and removed output connector.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1340\">#1340</a>.
- </li>
- <li>
- January 31, 2020 by Filip Jorissen:<br/>
- Improved error message.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component ensures that the interpolated pressure is between <i>31,000</i> Pa and <i>120,000</i> Pa.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Added <code>noEvent</code> and removed output connector.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1340\">#1340</a>.
+</li>
+<li>
+January 31, 2020 by Filip Jorissen:<br/>
+Improved error message.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-28,42},{26,-34}},
           textColor={0,0,255},
-          textString="P")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="P")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckPressure;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/ConvertTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/ConvertTime.mo
index 6c4d9ccd35..f8ebe6521b 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/ConvertTime.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/ConvertTime.mo
@@ -1,13 +1,7 @@
 within AixLib.BoundaryConditions.WeatherData.BaseClasses;
 block ConvertTime
   "Converts the simulation time to calendar time in scale of 1 year (365 days), or a multiple of a year"
-  extends Modelica.Blocks.Icons.Block;
-
-  parameter Modelica.Units.SI.Time weaDatStaTim(displayUnit="d")
-    "Start time of weather data";
-  parameter Modelica.Units.SI.Time weaDatEndTim(displayUnit="d")
-    "End time of weather data";
-
+  extends PartialConvertTime;
   Modelica.Blocks.Interfaces.RealInput modTim(
     final quantity="Time",
     final unit="s") "Simulation time"
@@ -20,93 +14,86 @@ block ConvertTime
 protected
   constant Modelica.Units.SI.Time shiftSolarRad=1800
     "Number of seconds for the shift for solar radiation calculation";
-  parameter Modelica.Units.SI.Time lenWea=weaDatEndTim - weaDatStaTim
-    "Length of weather data";
 
-  parameter Boolean canRepeatWeatherFile = abs(mod(lenWea, 365*24*3600)) < 1E-2
-    "=true, if the weather file can be repeated, since it has the length of a year or a multiple of it";
-
-  discrete Modelica.Units.SI.Time tNext(start=0, fixed=true)
-    "Start time of next period";
 
 equation
-  when {initial(), canRepeatWeatherFile and modTim > pre(tNext)} then
-    // simulation time stamp went over the end time of the weather file
-    //(last time stamp of the weather file + average increment)
-    tNext = if canRepeatWeatherFile then integer(modTim/lenWea)*lenWea + lenWea else time;
-  end when;
-  calTim = if canRepeatWeatherFile then modTim - tNext + lenWea else modTim;
-
+  calTim = calTimAux;
+  modTimAux = modTim;
   assert(canRepeatWeatherFile or noEvent((time - weaDatEndTim) < shiftSolarRad),
     "In " + getInstanceName() + ": Insufficient weather data provided for the desired simulation period.
-     The simulation time "+ String(time) +
+    The simulation time " + String(time) +
     " exceeds the end time " + String(weaDatEndTim) + " of the weather data file.",
     AssertionLevel.error);
 
   assert(canRepeatWeatherFile or noEvent(time >= weaDatStaTim),
     "In " + getInstanceName() + ": Insufficient weather data provided for the desired simulation period.
-     The simulation time "+ String(time) +
+    The simulation time " + String(time) +
     " is less than the start time " + String(weaDatStaTim) + " of the weather data file.",
     AssertionLevel.error);
 
   annotation (
     defaultComponentName="conTim",
     Documentation(info="<html>
- <p>
- This component converts the simulation time to calendar time in a scale of 1 year (365 days),
- or a multiple of it, if this is the length of the weather file.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 15, 2020, by Michael Wetter:<br/>
- Added <code>noEvent</code> to assertion to remove zero crossing function in OPTIMICA.
- </li>
- <li>
- January 29, 2020, by Filip Jorissen:<br/>
- Revised end time assert and added assert that verifies whether the time is before the
- start time of the weather file.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1281\">#1281</a>.
- </li>
- <li>
- June 12, 2019, by Michael Wetter:<br/>
- Reformulated model to avoid having to evaluate the weather file during compilation
- (as it determined the structural parameter <code>lenWea</code>). The new formulation
- allows inclusion of the weather file in JModelica-generated FMUs, and it works with
- Dymola as well.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1147\">#1147</a>.
- </li>
- <li>
- May 21, 2019, by Michael Wetter:<br/>
- Corrected code to avoid wrong type conversion.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1142\">#1142</a>.
- </li>
- <li>
- March 4, 2019, by Michael Wetter:<br/>
- Refactored implementation to correctly account for negative start times.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">#842</a>.
- </li>
- <li>
- July 27, 2018, by Ana Constantin:<br/>
- Added shift for multiple time spans.
- </li>
- <li>
- September 27, 2011, by Wangda Zuo and Michael Wetter:<br/>
- Modify it to convert negative value of time.
- Use the when-then to allow dymola differentiating this model when
- conducting index reduction which is not allowed in previous implementation.
- </li>
- <li>
- February 27, 2011, by Wangda Zuo:<br/>
- Renamed the component.
- </li>
- <li>
- July 08, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component converts the simulation time to calendar time in a scale of 1 year (365 days),
+or a multiple of it, if this is the length of the weather file.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 27, 2023, by Ettore Zanetti:<br/>
+Updated to use partial class for conversion from simulation time to calendar time.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1716\">IBPSA #1716</a>.
+</li>
+<li>
+April 15, 2020, by Michael Wetter:<br/>
+Added <code>noEvent</code> to assertion to remove zero crossing function in OPTIMICA.
+</li>
+<li>
+January 29, 2020, by Filip Jorissen:<br/>
+Revised end time assert and added assert that verifies whether the time is before the
+start time of the weather file.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1281\">#1281</a>.
+</li>
+<li>
+June 12, 2019, by Michael Wetter:<br/>
+Reformulated model to avoid having to evaluate the weather file during compilation
+(as it determined the structural parameter <code>lenWea</code>). The new formulation
+allows inclusion of the weather file in JModelica-generated FMUs, and it works with
+Dymola as well.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1147\">#1147</a>.
+</li>
+<li>
+May 21, 2019, by Michael Wetter:<br/>
+Corrected code to avoid wrong type conversion.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1142\">#1142</a>.
+</li>
+<li>
+March 4, 2019, by Michael Wetter:<br/>
+Refactored implementation to correctly account for negative start times.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">#842</a>.
+</li>
+<li>
+July 27, 2018, by Ana Constantin:<br/>
+Added shift for multiple time spans.
+</li>
+<li>
+September 27, 2011, by Wangda Zuo and Michael Wetter:<br/>
+Modify it to convert negative value of time.
+Use the when-then to allow dymola differentiating this model when
+conducting index reduction which is not allowed in previous implementation.
+</li>
+<li>
+February 27, 2011, by Wangda Zuo:<br/>
+Renamed the component.
+</li>
+<li>
+July 08, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={
         Text(
@@ -132,6 +119,6 @@ equation
         Line(
           points={{60,-2},{-66,-2}}),
         Line(
-          points={{60,-32},{-66,-32}})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          points={{60,-32},{-66,-32}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConvertTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/EquationOfTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/EquationOfTime.mo
index 3105eeeea3..4c147e5643 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/EquationOfTime.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/EquationOfTime.mo
@@ -1,6 +1,6 @@
 within AixLib.BoundaryConditions.WeatherData.BaseClasses;
 block EquationOfTime "Equation of time"
-  extends Modelica.Blocks.Icons.Block;
+  extends PartialConvertTime;
   Modelica.Blocks.Interfaces.RealInput nDay(
     quantity="Time",
     unit="s")
@@ -14,24 +14,30 @@ block EquationOfTime "Equation of time"
 protected
   Real Bt "Intermediate variable";
 equation
-  Bt = Modelica.Constants.pi*((nDay + 86400)/86400 - 81)/182
+  modTimAux = nDay;
+  Bt = Modelica.Constants.pi*((calTimAux + 86400)/86400 - 81)/182
     "Our unit is s instead of day in (A.4.2b)";
   eqnTim = 60*(9.87*Modelica.Math.sin(2*Bt) - 7.53*Modelica.Math.cos(Bt) - 1.5*
     Modelica.Math.sin(Bt)) "Our unit is s instead of min in (A.4.2a)";
   annotation (
     defaultComponentName="eqnTim",
     Documentation(info="<html>
- <p>
- This component computes the difference between solar noon and noon of local civic time.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 13, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the difference between solar noon and noon of local civil time.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 27, 2023, by Ettore Zanetti:<br/>
+Updated to use partial class for conversion from simulation time to calendar time.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1716\">IBPSA #1716</a>.
+</li>
+<li>
+May 13, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
@@ -44,6 +50,6 @@ equation
         Text(
           extent={{-6,4},{52,-24}},
           textColor={0,0,255},
-          textString="equ")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="equ")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end EquationOfTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckBlackBodySkyTemperature.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckBlackBodySkyTemperature.mo
index 606593675a..33aa6e93d8 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckBlackBodySkyTemperature.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckBlackBodySkyTemperature.mo
@@ -15,21 +15,21 @@ equation
     annotation (Line(points={{-19,0},{18,0}}, color={0,0,127}));
   annotation (
 Documentation(info="<html>
- <p>
- This example tests the model that checks the black-body sky temperature.
- </p>
- </html>",
+<p>
+This example tests the model that checks the black-body sky temperature.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 5, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+January 5, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckBlackBodySkyTemperature.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckBlackBodySkyTemperature;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckPressure.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckPressure.mo
index eaf4ff2773..48961a4945 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckPressure.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckPressure.mo
@@ -35,25 +35,25 @@ equation
       color={0,0,127}));
   annotation (
 Documentation(info="<html>
- <p>
- This example tests the model that asserts that the pressure is within acceptable bounds.
- </p>
- </html>",
+<p>
+This example tests the model that asserts that the pressure is within acceptable bounds.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
- <code>Modelica.Utilities.Files.loadResource</code>.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
+<code>Modelica.Utilities.Files.loadResource</code>.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StartTime=0, StopTime=8640000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckPressure.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckPressure;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckTemperature.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckTemperature.mo
index f67859bd16..6121b0b7ed 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckTemperature.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckTemperature.mo
@@ -52,26 +52,26 @@ equation
       color={0,0,127}));
   annotation (
 Documentation(info="<html>
- <p>
- This example tests the model that checks the temperature.
- </p>
- </html>",
+<p>
+This example tests the model that checks the temperature.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
- <code>Modelica.Utilities.Files.loadResource</code>.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
+<code>Modelica.Utilities.Files.loadResource</code>.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StartTime=0, StopTime=8640000),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/CheckTemperature.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckTemperature;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTime.mo
index 7620fb41ef..e4da2928ca 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTime.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTime.mo
@@ -15,21 +15,21 @@ equation
       color={0,0,127}));
   annotation (
   Documentation(info="<html>
- <p>
- This example tests the model that converts time.
- </p>
- </html>",
+<p>
+This example tests the model that converts time.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StopTime=77760000),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTime.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConvertTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimeNegativeStart.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimeNegativeStart.mo
index 5f7c992423..4e7cfda878 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimeNegativeStart.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimeNegativeStart.mo
@@ -4,21 +4,21 @@ model ConvertTimeNegativeStart
   extends AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.ConvertTime;
   annotation (
   Documentation(info="<html>
- <p>
- This example tests the model that converts time for negative start time.
- </p>
- </html>",
+<p>
+This example tests the model that converts time for negative start time.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 4, 2019, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+March 4, 2019, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StartTime=-31536000, StopTime=31536000),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimeNegativeStart.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConvertTimeNegativeStart;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimePositiveStart.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimePositiveStart.mo
index f8504b8d8e..2e9f65bc16 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimePositiveStart.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimePositiveStart.mo
@@ -4,21 +4,21 @@ model ConvertTimePositiveStart
   extends AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.ConvertTime;
   annotation (
   Documentation(info="<html>
- <p>
- This example tests the model that converts time for positive start time.
- </p>
- </html>",
+<p>
+This example tests the model that converts time for positive start time.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 4, 2019, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+March 4, 2019, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StartTime=47174400, StopTime=126144000),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/ConvertTimePositiveStart.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConvertTimePositiveStart;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/EquationOfTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/EquationOfTime.mo
index 6c233fa437..00978c2ae7 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/EquationOfTime.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/EquationOfTime.mo
@@ -12,20 +12,20 @@ equation
       color={0,0,127}));
   annotation (
   Documentation(info="<html>
- <p>
- This example tests the model that computes the equation of time.
- </p>
- </html>",
+<p>
+This example tests the model that computes the equation of time.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StopTime=86400),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/EquationOfTime.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end EquationOfTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAbsolutePath.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAbsolutePath.mo
index 791c8211c6..8b64374bf7 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAbsolutePath.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAbsolutePath.mo
@@ -16,31 +16,31 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAbsolutePath.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the function that gets the absolute path of a URI.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>loadResource</code> call.
- </li>
- <li>
- November 18, 2016, by Michael Wetter:<br/>
- Removed tests that assumed that the regression test is run
- from the library root directory.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/596\">#596</a>.
- </li>
- <li>
- October 9, 2013, by Michael Wetter:<br/>
- Removed incorrect call to <code>Modelica.Utilities.Files.exist</code>.
- </li>
- <li>
- May 9, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the function that gets the absolute path of a URI.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>loadResource</code> call.
+</li>
+<li>
+November 18, 2016, by Michael Wetter:<br/>
+Removed tests that assumed that the regression test is run
+from the library root directory.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/596\">#596</a>.
+</li>
+<li>
+October 9, 2013, by Michael Wetter:<br/>
+Removed incorrect call to <code>Modelica.Utilities.Files.exist</code>.
+</li>
+<li>
+May 9, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end GetAbsolutePath;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAltitudeTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAltitudeTMY3.mo
index b34f0da4ef..652bc786d7 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAltitudeTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAltitudeTMY3.mo
@@ -9,24 +9,24 @@ model GetAltitudeTMY3 "Test model to get Altitude of TMY3"
 
   annotation (
     Documentation(info="<html>
- <p>
- This example tests getting the location altitude of a TMY3 weather data file.
- </p>
- </html>",
+<p>
+This example tests getting the location altitude of a TMY3 weather data file.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Changed <code>alt</code> from variable to parameter as it is evaluated using an impure function call.
- </li>
- <li>
- September 16, 2021, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Changed <code>alt</code> from variable to parameter as it is evaluated using an impure function call.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/GetAltitudeTMY3.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end GetAltitudeTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetHeaderElement.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetHeaderElement.mo
index 1a4dcdbca9..ca08678537 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetHeaderElement.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetHeaderElement.mo
@@ -29,31 +29,31 @@ initial equation
 
   annotation (
     Documentation(info="<html>
- <p>
- This example tests getting the header of the TMY3 weather data file.
- </p>
- </html>",
+<p>
+This example tests getting the header of the TMY3 weather data file.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Added call to
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
- AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>
- as this call has been removed from the function
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getHeaderElementTMY3\">
- AixLib.BoundaryConditions.WeatherData.BaseClasses.getHeaderElementTMY3</a>.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/506\">Buildings, #506</a>.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Added call to
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>
+as this call has been removed from the function
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getHeaderElementTMY3\">
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getHeaderElementTMY3</a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/506\">Buildings, #506</a>.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/GetHeaderElement.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end GetHeaderElement;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3.mo
index e0a6c3b619..2ae412c897 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3.mo
@@ -25,25 +25,25 @@ initial equation
 
   annotation (
     Documentation(info="<html>
- <p>
- This example tests getting the time span of a TMY3 weather data file.
- </p>
- </html>",
+<p>
+This example tests getting the time span of a TMY3 weather data file.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 16, 2019, by Michael Wetter:<br/>
- Removed call to get the absolute path of the file, corrected the <code>.mos</code>
- file name and updated the documentation
- </li>
- <li>
- April 15, 2019, by Ana Constantin:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 16, 2019, by Michael Wetter:<br/>
+Removed call to get the absolute path of the file, corrected the <code>.mos</code>
+file name and updated the documentation
+</li>
+<li>
+April 15, 2019, by Ana Constantin:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end GetTimeSpanTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3LongHeader.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3LongHeader.mo
index e025f86259..1dac92b850 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3LongHeader.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3LongHeader.mo
@@ -15,23 +15,23 @@ initial equation
   assert(abs(timeSpan[2]-14400) < 0.1, "Error in getting time span.");
   annotation (
     Documentation(info="<html>
- <p>
- This example tests getting the time span of a TMY3 weather data file with a long line in the
- header of the weather file.
- </p>
- </html>",
+<p>
+This example tests getting the time span of a TMY3 weather data file with a long line in the
+header of the weather file.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 27, 2021, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1432\">#1432</a>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+January 27, 2021, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1432\">#1432</a>.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3LongHeader.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end GetTimeSpanTMY3LongHeader;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3_NonzeroStart.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3_NonzeroStart.mo
index d23d7d1ee6..03deecf08d 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3_NonzeroStart.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3_NonzeroStart.mo
@@ -10,21 +10,21 @@ model GetTimeSpanTMY3_NonzeroStart
 
   annotation (
     Documentation(info="<html>
- <p>
- This example tests getting time span of a TMY3 weather data file that
- starts at a non-zero time.
- </p>
- </html>",
+<p>
+This example tests getting time span of a TMY3 weather data file that
+starts at a non-zero time.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 17, 2019, by Jianjun Hu:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 17, 2019, by Jianjun Hu:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/GetTimeSpanTMY3_NonzeroStart.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end GetTimeSpanTMY3_NonzeroStart;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LimitMin.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LimitMin.mo
index 8ce1b3b931..47ea666f51 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LimitMin.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LimitMin.mo
@@ -33,25 +33,25 @@ equation
       color={0,0,127}));
   annotation (
 Documentation(info="<html>
- <p>
- This example tests the model that constrains the ceiling height.
- </p>
- </html>",
+<p>
+This example tests the model that constrains the ceiling height.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
- <code>Modelica.Utilities.Files.loadResource</code>.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
+<code>Modelica.Utilities.Files.loadResource</code>.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StartTime=0, StopTime=432000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/LimitMin.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimitMin;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LocalCivilTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LocalCivilTime.mo
index 14f264da84..325ef0d65f 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LocalCivilTime.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/LocalCivilTime.mo
@@ -13,20 +13,20 @@ equation
       color={0,0,127}));
   annotation (
   Documentation(info="<html>
- <p>
- This example tests the model that computes the local civil time.
- </p>
- </html>",
+<p>
+This example tests the model that computes the local civil time.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StartTime=0, StopTime=172800),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/LocalCivilTime.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end LocalCivilTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/SolarTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/SolarTime.mo
index 5a14a91c86..dbad58d466 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/SolarTime.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/Examples/SolarTime.mo
@@ -28,19 +28,19 @@ equation
       color={0,0,127}));
   annotation (
   Documentation(info="<html>
- <p>
- This example tests the model that computes the solar time.
- </p>
- </html>",
+<p>
+This example tests the model that computes the solar time.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"), experiment(Tolerance=1e-6, StopTime=864000),
+<ul>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  experiment(Tolerance=1e-6, StopTime=864000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/BaseClasses/Examples/SolarTime.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SolarTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterCeilingHeight.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterCeilingHeight.mo
index b04d688d89..56c472c3b2 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterCeilingHeight.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterCeilingHeight.mo
@@ -9,21 +9,21 @@ block LimiterCeilingHeight "Block that limits the relative humidity"
 annotation (
 defaultComponentName="limMin",
 Documentation(info="<html>
- <p>
- Block that limits the cloud cover ceiling height to be positive.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to slightly
- negative values.
- </p>
- </html>",
+<p>
+Block that limits the cloud cover ceiling height to be positive.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to slightly
+negative values.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimiterCeilingHeight;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterHorizontalInfraredIrradiation.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterHorizontalInfraredIrradiation.mo
index fd0c795e13..d43e632305 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterHorizontalInfraredIrradiation.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterHorizontalInfraredIrradiation.mo
@@ -10,21 +10,21 @@ block LimiterHorizontalInfraredIrradiation
   annotation (
 defaultComponentName="limMin",
 Documentation(info="<html>
- <p>
- Block that limits the horizontal infrared irradiation to be positive.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to slightly
- negative values.
- </p>
- </html>",
+<p>
+Block that limits the horizontal infrared irradiation to be positive.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to slightly
+negative values.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimiterHorizontalInfraredIrradiation;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterOpaqueSkyCover.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterOpaqueSkyCover.mo
index 324234de34..90cb1f2939 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterOpaqueSkyCover.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterOpaqueSkyCover.mo
@@ -12,21 +12,21 @@ equation
   annotation (
 defaultComponentName="lim",
 Documentation(info="<html>
- <p>
- Block that limits the opaque sky cover.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to slightly
- negative values.
- </p>
- </html>",
+<p>
+Block that limits the opaque sky cover.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to slightly
+negative values.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimiterOpaqueSkyCover;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterRelativeHumidity.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterRelativeHumidity.mo
index a8330a3b93..71d5ec46ed 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterRelativeHumidity.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterRelativeHumidity.mo
@@ -12,21 +12,21 @@ equation
   annotation (
 defaultComponentName="lim",
 Documentation(info="<html>
- <p>
- Block that limits the relative humidity.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to slightly
- negative values.
- </p>
- </html>",
+<p>
+Block that limits the relative humidity.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to slightly
+negative values.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimiterRelativeHumidity;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterTotalSkyCover.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterTotalSkyCover.mo
index e415050849..832623c50a 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterTotalSkyCover.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterTotalSkyCover.mo
@@ -12,21 +12,21 @@ equation
   annotation (
 defaultComponentName="lim",
 Documentation(info="<html>
- <p>
- Block that limits the total sky cover.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to slightly
- negative values.
- </p>
- </html>",
+<p>
+Block that limits the total sky cover.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to slightly
+negative values.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimiterTotalSkyCover;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindDirection.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindDirection.mo
index 24856ade5d..25030def36 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindDirection.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindDirection.mo
@@ -13,21 +13,21 @@ equation
   annotation (
 defaultComponentName="lim",
 Documentation(info="<html>
- <p>
- Block that limits the wind direction.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to slightly
- negative values.
- </p>
- </html>",
+<p>
+Block that limits the wind direction.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to slightly
+negative values.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimiterWindDirection;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindSpeed.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindSpeed.mo
index 4ef15060da..5da8fd8afc 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindSpeed.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LimiterWindSpeed.mo
@@ -9,21 +9,21 @@ block LimiterWindSpeed "Block that limits the wind speed"
   annotation (
 defaultComponentName="limMin",
 Documentation(info="<html>
- <p>
- Block that limits the wind speed to be positive.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to slightly
- negative values.
- </p>
- </html>",
+<p>
+Block that limits the wind speed to be positive.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to slightly
+negative values.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimiterWindSpeed;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LocalCivilTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LocalCivilTime.mo
index b9a81c32b5..d0534ff8c6 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/LocalCivilTime.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/LocalCivilTime.mo
@@ -1,6 +1,6 @@
 within AixLib.BoundaryConditions.WeatherData.BaseClasses;
 block LocalCivilTime "Converts the clock time to local civil time."
-  extends Modelica.Blocks.Icons.Block;
+  extends PartialConvertTime;
   Modelica.Blocks.Interfaces.RealInput cloTim(
     final quantity="Time",
     final unit="s") "Clock time"
@@ -15,34 +15,40 @@ protected
   final parameter Modelica.Units.SI.Time diff=-timZon + lon*43200/Modelica.Constants.pi
     "Difference between local and clock time";
 equation
-  locTim = cloTim + diff;
+  modTimAux = cloTim;
+  locTim = calTimAux + diff;
 
   annotation (
     defaultComponentName="locTim",
     Documentation(info="<html>
- <p>
- This component converts the clock time to local civil time.
- The parameter <code>timZon</code> represents the time zone of the facility  (relative to Greenwich Mean Time or the 0th meridian). Time zones west of GMT (e.g. North America) are represented as negative;
- east of GMT as positive. Fraction of hours are represented in decimals (e.g. for <i>6:30</i>, use <i>6.5</i>).
- </p>
- <p>
- The formula is based on Michael Wetter's thesis (A4.1):
- </p>
- <pre>
-   locTim = greTim + (lon*180/pi)*86400/360 = cloTim - timZon + lon*43200/pi
- </pre>
- </html>",revisions="<html>
- <ul>
- <li>
- November 14, 2015, by Michael Wetter:<br/>
- Introduced <code>diff</code>.
- </li>
- <li>
- February 27, 2011, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component converts the clock time to local civil time.
+The parameter <code>timZon</code> represents the time zone of the facility  (relative to Greenwich Mean Time or the 0th meridian). Time zones west of GMT (e.g. North America) are represented as negative;
+east of GMT as positive. Fraction of hours are represented in decimals (e.g. for <i>6:30</i>, use <i>6.5</i>).
+</p>
+<p>
+The formula is based on Michael Wetter's thesis (A4.1):
+</p>
+<pre>
+  locTim = greTim + (lon*180/pi)*86400/360 = cloTim - timZon + lon*43200/pi
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+March 27, 2023, by Ettore Zanetti:<br/>
+Updated to use partial class for conversion from simulation time to calendar time.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1716\">IBPSA #1716</a>.
+</li>
+<li>
+November 14, 2015, by Michael Wetter:<br/>
+Introduced <code>diff</code>.
+</li>
+<li>
+February 27, 2011, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-98,6},{-60,-6}},
@@ -50,6 +56,6 @@ equation
           textString="cloTim"), Text(
           extent={{74,6},{98,-4}},
           textColor={0,0,127},
-          textString="calTim")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="calTim")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end LocalCivilTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialConvertTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialConvertTime.mo
new file mode 100644
index 0000000000..e22849ec6f
--- /dev/null
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialConvertTime.mo
@@ -0,0 +1,51 @@
+within AixLib.BoundaryConditions.WeatherData.BaseClasses;
+partial block PartialConvertTime
+  "Converts the simulation time to calendar time in scale of 1 year (365 days), or a multiple of a year"
+  extends Modelica.Blocks.Icons.Block;
+  parameter Modelica.Units.SI.Time weaDatStaTim(displayUnit="d") = 0
+    "Start time of weather data";
+  parameter Modelica.Units.SI.Time weaDatEndTim(displayUnit="d") = 31536000
+    "End time of weather data";
+  Modelica.Units.SI.Time modTimAux "Model time";
+  Modelica.Units.SI.Time calTimAux "Calendar time";
+
+protected
+  parameter Modelica.Units.SI.Time lenWea=weaDatEndTim - weaDatStaTim
+    "Length of weather data";
+
+  parameter Boolean canRepeatWeatherFile = abs(mod(lenWea, 365*24*3600)) < 1E-2
+    "=true, if the weather file can be repeated, since it has the length of a year or a multiple of it";
+
+  discrete Modelica.Units.SI.Time tNext(start=0, fixed=true)
+    "Start time of next period";
+
+equation
+  when {initial(), canRepeatWeatherFile and modTimAux > pre(tNext)} then
+    // simulation time stamp went over the end time of the weather file
+    //(last time stamp of the weather file + average increment)
+    tNext = if canRepeatWeatherFile then integer(modTimAux/lenWea)*lenWea + lenWea else time;
+  end when;
+  calTimAux = if canRepeatWeatherFile then modTimAux - tNext + lenWea else modTimAux;
+
+
+  annotation (
+    defaultComponentName="conTim",
+    Documentation(info="<html>
+<p>
+This component converts the simulation time to calendar time in a scale of 1 year (365 days),
+or a multiple of it, if this is the length of the weather file.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 27, 2023, by Ettore Zanetti:<br/>
+Added partial class for conversion from simulation time to calendar time, to be
+used by solar models that require calendar time for calculations.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1716\">IBPSA #1716</a>.
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
+            100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConvertTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiter.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiter.mo
index 617f43f88c..49f317bb5a 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiter.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiter.mo
@@ -12,30 +12,30 @@ partial block PartialLimiter
 annotation (
 defaultComponentName="lim",
 Documentation(info="<html>
- <p>
- Block that computes <i>y_internal=min(uMax, max(uMin, u))</i>,
- where <code>y_internal</code> is a protected connector.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to
- a slight overshoot of values. This block is extended by other blocks
- that then provide the output connector.
- Extending this block is needed for the output connector to have the correct
- comment string in the weather data bus, because the weather
- data bus displays the comment string of the output signal
- that is connected to the weather data bus.
- Without this construct, the weather data bus would simply show
- \"Connector of Real output signal\".
- </p>
- </html>",
+<p>
+Block that computes <i>y_internal=min(uMax, max(uMin, u))</i>,
+where <code>y_internal</code> is a protected connector.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to
+a slight overshoot of values. This block is extended by other blocks
+that then provide the output connector.
+Extending this block is needed for the output connector to have the correct
+comment string in the weather data bus, because the weather
+data bus displays the comment string of the output signal
+that is connected to the weather data bus.
+Without this construct, the weather data bus would simply show
+\"Connector of Real output signal\".
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
      Icon(coordinateSystem(
     preserveAspectRatio=true,
     extent={{-100,-100},{100,100}}), graphics={
@@ -58,6 +58,6 @@ revisions="<html>
           textColor={0,0,0})}),
     Diagram(coordinateSystem(
     preserveAspectRatio=true,
-    extent={{-100,-100},{100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialLimiter;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiterMin.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiterMin.mo
index 8694222738..9799dc9f46 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiterMin.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/PartialLimiterMin.mo
@@ -10,34 +10,34 @@ partial block PartialLimiterMin
 annotation (
 defaultComponentName="limMin",
 Documentation(info="<html>
- <p>
- Partial block that is used to limit a signal by a minimum value.
- </p>
- <p>
- This block is used because interpolation of weather data can lead to slightly
- negative values. This block is extended by other blocks
- that then provide the output connector.
- Extending this block is needed for the output connector to have the correct
- comment string in the weather data bus, because the weather
- data bus displays the comment string of the output signal
- that is connected to the weather data bus.
- Without this construct, the weather data bus would simply show
- \"Connector of Real output signal\".
- </p>
- </html>",
+<p>
+Partial block that is used to limit a signal by a minimum value.
+</p>
+<p>
+This block is used because interpolation of weather data can lead to slightly
+negative values. This block is extended by other blocks
+that then provide the output connector.
+Extending this block is needed for the output connector to have the correct
+comment string in the weather data bus, because the weather
+data bus displays the comment string of the output signal
+that is connected to the weather data bus.
+Without this construct, the weather data bus would simply show
+\"Connector of Real output signal\".
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(
       graphics={
         Text(
           extent={{-100,30},{98,-16}},
           textColor={0,0,0},
-          textString="0 <= u")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="0 <= u")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialLimiterMin;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/SolarTime.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/SolarTime.mo
index e57796e98a..33aea99fcb 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/SolarTime.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/SolarTime.mo
@@ -18,27 +18,27 @@ equation
   annotation (
     defaultComponentName="solTim",
     Documentation(info="<html>
- <p>
- This component computes the local solar time.
- </p>
- <p>
- <b>Note:</b> To avoid events, this block does not convert solar time to a scale of 24 hours.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- Feb. 16, 2012, by Michael Wetter:<br/>
- Removed section that limits solar time to
- <code>0 &le; solTim &le; 86400</code> as this triggers
- events, and is not needed because solar time is used in
- trigonometric functions only.
- </li>
- <li>
- May 13, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component computes the local solar time.
+</p>
+<p>
+<b>Note:</b> To avoid events, this block does not convert solar time to a scale of 24 hours.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Feb. 16, 2012, by Michael Wetter:<br/>
+Removed section that limits solar time to
+<code>0 &le; solTim &le; 86400</code> as this triggers
+events, and is not needed because solar time is used in
+trigonometric functions only.
+</li>
+<li>
+May 13, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-150,110},{150,150}},
@@ -59,6 +59,6 @@ equation
         Text(
           extent={{-96,-44},{-44,-60}},
           textColor={0,0,127},
-          textString="locTim")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="locTim")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SolarTime;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelector.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelector.mo
index 496a9b4e02..d77897bc9a 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelector.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelector.mo
@@ -24,19 +24,19 @@ equation
   annotation (
   defaultComponentName="souSel",
 Documentation(info="<html>
- <p>
- Block that produces at its output the input value <code>uCon</code>, <code>uFil</code>
- or the parameter value <code>p</code> depending on the parameter value
- <code>datSou</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block that produces at its output the input value <code>uCon</code>, <code>uFil</code>
+or the parameter value <code>p</code> depending on the parameter value
+<code>datSou</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
       Rectangle(
           extent={{-100,100},{100,-100}},
@@ -60,6 +60,6 @@ Documentation(info="<html>
         Ellipse(lineColor={0,0,255},
           pattern=LinePattern.None,
           fillPattern=FillPattern.Solid,
-          extent={{2,-8},{18,8}})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          extent={{2,-8},{18,8}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SourceSelector;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelectorRadiation.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelectorRadiation.mo
index 570665a88f..b3a5e27ed4 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelectorRadiation.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/SourceSelectorRadiation.mo
@@ -151,32 +151,32 @@ equation
   annotation (
   defaultComponentName="souSel",
 Documentation(info="<html>
- <p>
- Block that outputs the direct normal, diffuse horizontal and diffuse global
- solar irradiation.
- This block computes these output quantities based on conditionally provided
- input signals.
- </p>
- <p>
- The computations are based on Wetter (2004).
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Michael Wetter.<br/>
- <a href=\"http://simulationresearch.lbl.gov/wetter/download/mwdiss.pdf\">
- Simulation-based Building Energy Optimization</a>.<br/>
- Dissertation. University of California at Berkeley. 2004.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block that outputs the direct normal, diffuse horizontal and diffuse global
+solar irradiation.
+This block computes these output quantities based on conditionally provided
+input signals.
+</p>
+<p>
+The computations are based on Wetter (2004).
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Michael Wetter.<br/>
+<a href=\"http://simulationresearch.lbl.gov/wetter/download/mwdiss.pdf\">
+Simulation-based Building Energy Optimization</a>.<br/>
+Dissertation. University of California at Berkeley. 2004.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
       Rectangle(
           extent={{-100,100},{100,-100}},
@@ -196,6 +196,6 @@ Documentation(info="<html>
         Ellipse(lineColor={0,0,255},
           pattern=LinePattern.None,
           fillPattern=FillPattern.Solid,
-          extent={{-2,-8},{14,8}})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          extent={{-2,-8},{14,8}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SourceSelectorRadiation;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getAbsolutePath.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getAbsolutePath.mo
index 5480717575..a439076221 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getAbsolutePath.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getAbsolutePath.mo
@@ -6,53 +6,53 @@ pure function getAbsolutePath "Gets the absolute path of a URI"
 algorithm
   path := Modelica.Utilities.Files.loadResource(uri);
   annotation (Documentation(info="<html>
- <p>
- The function returns the absolute path of a
- uniform resource identifier (URI) or local file name.
- If the file is not found, then this function
- terminates with an <code>assert</code>.
- </p>
- <p>
- This function has been introduced to allow users
- to specify the name of weather data files with a path
- that is relative to the library path. This allows users
- to change the current working directory while still
- being able to read the files.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Removed assertion if file does not exist. This has been removed because it
- makes the function impure, and then the test
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetAbsolutePath\">
- AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetAbsolutePath</a>
- fails.
- </li>
- <li>
- July 07, 2016, by Thierry S. Nouidui:<br/>
- Removed the use of <code>Modelica.Utilities.Files.fullPathName</code>
- which is implicitly done in <code>Modelica.Utilities.Files.loadResource</code>. <br/>
- Removed the addition of <code>file://</code> to file names which do not start
- with <code>file://</code>, or <code>modelica://</code>.
- This is not required when using <code>Modelica.Utilities.Files.loadResource</code>.
- </li>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
- <code>Modelica.Utilities.Files.loadResource</code>.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Improved algorithm that determines the absolute path of the file.
- Now the function works from any directory as long as the <code>AixLib</code> library
- is on the <code>MODELICAPATH</code>.
- </li>
- <li>
- May 2, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+The function returns the absolute path of a
+uniform resource identifier (URI) or local file name.
+If the file is not found, then this function
+terminates with an <code>assert</code>.
+</p>
+<p>
+This function has been introduced to allow users
+to specify the name of weather data files with a path
+that is relative to the library path. This allows users
+to change the current working directory while still
+being able to read the files.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Removed assertion if file does not exist. This has been removed because it
+makes the function impure, and then the test
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetAbsolutePath\">
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetAbsolutePath</a>
+fails.
+</li>
+<li>
+July 07, 2016, by Thierry S. Nouidui:<br/>
+Removed the use of <code>Modelica.Utilities.Files.fullPathName</code>
+which is implicitly done in <code>Modelica.Utilities.Files.loadResource</code>. <br/>
+Removed the addition of <code>file://</code> to file names which do not start
+with <code>file://</code>, or <code>modelica://</code>.
+This is not required when using <code>Modelica.Utilities.Files.loadResource</code>.
+</li>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
+<code>Modelica.Utilities.Files.loadResource</code>.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Improved algorithm that determines the absolute path of the file.
+Now the function works from any directory as long as the <code>AixLib</code> library
+is on the <code>MODELICAPATH</code>.
+</li>
+<li>
+May 2, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end getAbsolutePath;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getAltitudeLocationTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getAltitudeLocationTMY3.mo
index 29e1f79902..87eb2f92df 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getAltitudeLocationTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getAltitudeLocationTMY3.mo
@@ -21,18 +21,18 @@ algorithm
     unsigned=false);
 
   annotation (Documentation(info="<html>
- This function returns the altitude of the TMY3 weather data file.
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This function returns the altitude of the TMY3 weather data file.
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end getAltitudeLocationTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getHeaderElementTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getHeaderElementTMY3.mo
index 45e8362cff..f4d5b53b7f 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getHeaderElementTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getHeaderElementTMY3.mo
@@ -61,50 +61,50 @@ algorithm
   element :=Modelica.Utilities.Strings.substring(lin, startIndex=staInd+1, endIndex=nexInd-1);
   annotation (Inline=false,
   Documentation(info="<html>
- This function scans the weather data file for a line that starts with the string <pre>
- start
- </pre>
- where <code>start</code> is a parameter.
- When this line is found, the function returns the element at the position number
- <code>position</code>, where <code>position</code> is a parameter.
- A comma is used as the delimiter of the elements.
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Removed call to
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
- AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>
- because this function calls
- <a href=\"modelica://Modelica.Utilities.Files.loadResource\">
- Modelica.Utilities.Files.loadResource</a>, which needs to be resolved at compilation
- time, which is difficult if it is inside a function.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/506\">Buildings, #506</a>.
- </li>
- <li>
- September 24, 2015, by Marcus Fuchs:<br/>
- Replace Dymola specific annotation by <code>loadSelector</code>
- for MSL compliancy as reported by @tbeu at
- <a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
- </li>
- <li>
- May 2, 2013, by Michael Wetter:<br/>
- Added function call to <code>getAbsolutePath</code>.
- </li>
- <li>
- February 25, 2012, by Michael Wetter:<br/>
- Removed default value for parameter <code>name</code>.
- </li>
- <li>
- March 5, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This function scans the weather data file for a line that starts with the string <pre>
+start
+</pre>
+where <code>start</code> is a parameter.
+When this line is found, the function returns the element at the position number
+<code>position</code>, where <code>position</code> is a parameter.
+A comma is used as the delimiter of the elements.
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Removed call to
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>
+because this function calls
+<a href=\"modelica://Modelica.Utilities.Files.loadResource\">
+Modelica.Utilities.Files.loadResource</a>, which needs to be resolved at compilation
+time, which is difficult if it is inside a function.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/506\">Buildings, #506</a>.
+</li>
+<li>
+September 24, 2015, by Marcus Fuchs:<br/>
+Replace Dymola specific annotation by <code>loadSelector</code>
+for MSL compliancy as reported by @tbeu at
+<a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
+</li>
+<li>
+May 2, 2013, by Michael Wetter:<br/>
+Added function call to <code>getAbsolutePath</code>.
+</li>
+<li>
+February 25, 2012, by Michael Wetter:<br/>
+Removed default value for parameter <code>name</code>.
+</li>
+<li>
+March 5, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end getHeaderElementTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLastHeaderElementTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLastHeaderElementTMY3.mo
index bc666a04f2..1cbb4cc08d 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLastHeaderElementTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLastHeaderElementTMY3.mo
@@ -43,50 +43,50 @@ algorithm
   element :=Modelica.Utilities.Strings.substring(lin, startIndex=staInd+1, endIndex=lasInd);
   annotation (Inline=false,
   Documentation(info="<html>
- This function scans the weather data file for a line that starts with the string <pre>
- start
- </pre>
- where <code>start</code> is a parameter.
- When this line is found, the function returns the element at the position number
- <code>position</code>, where <code>position</code> is a parameter.
- A comma is used as the delimiter of the elements.
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Removed call to
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
- AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>
- because this function calls
- <a href=\"modelica://Modelica.Utilities.Files.loadResource\">
- Modelica.Utilities.Files.loadResource</a>, which needs to be resolved at compilation
- time, which is difficult if it is inside a function.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/506\">Buildings, #506</a>.
- </li>
- <li>
- September 24, 2015, by Marcus Fuchs:<br/>
- Replace Dymola specific annotation by <code>loadSelector</code>
- for MSL compliancy as reported by @tbeu at
- <a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
- </li>
- <li>
- May 2, 2013, by Michael Wetter:<br/>
- Added function call to <code>getAbsolutePath</code>.
- </li>
- <li>
- February 25, 2012, by Michael Wetter:<br/>
- Removed default value for parameter <code>name</code>.
- </li>
- <li>
- March 5, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This function scans the weather data file for a line that starts with the string <pre>
+start
+</pre>
+where <code>start</code> is a parameter.
+When this line is found, the function returns the element at the position number
+<code>position</code>, where <code>position</code> is a parameter.
+A comma is used as the delimiter of the elements.
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Removed call to
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>
+because this function calls
+<a href=\"modelica://Modelica.Utilities.Files.loadResource\">
+Modelica.Utilities.Files.loadResource</a>, which needs to be resolved at compilation
+time, which is difficult if it is inside a function.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/506\">Buildings, #506</a>.
+</li>
+<li>
+September 24, 2015, by Marcus Fuchs:<br/>
+Replace Dymola specific annotation by <code>loadSelector</code>
+for MSL compliancy as reported by @tbeu at
+<a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
+</li>
+<li>
+May 2, 2013, by Michael Wetter:<br/>
+Added function call to <code>getAbsolutePath</code>.
+</li>
+<li>
+February 25, 2012, by Michael Wetter:<br/>
+Removed default value for parameter <code>name</code>.
+</li>
+<li>
+March 5, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end getLastHeaderElementTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLatitudeTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLatitudeTMY3.mo
index dbabd47c2c..c2a0d55fc1 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLatitudeTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLatitudeTMY3.mo
@@ -30,24 +30,24 @@ algorithm
        String(lat) + " (= " + String(lat*180/Modelica.Constants.pi) + " degrees).");
 
   annotation (Documentation(info="<html>
- This function returns the latitude of the TMY3 weather data file.
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- September 24, 2015, by Marcus Fuchs:<br/>
- Replace Dymola specific annotation by <code>loadSelector</code>
- for MSL compliancy as reported by @tbeu at
- <a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
- </li>
- <li>
- February 25, 2012, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This function returns the latitude of the TMY3 weather data file.
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+September 24, 2015, by Marcus Fuchs:<br/>
+Replace Dymola specific annotation by <code>loadSelector</code>
+for MSL compliancy as reported by @tbeu at
+<a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
+</li>
+<li>
+February 25, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end getLatitudeTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLongitudeTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLongitudeTMY3.mo
index ef7b57fe1e..846b1339b2 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLongitudeTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getLongitudeTMY3.mo
@@ -30,24 +30,24 @@ algorithm
        String(lon) + " (= " + String(lon*180/Modelica.Constants.pi) + " degrees).");
 
   annotation (Documentation(info="<html>
- This function returns the longitude of the TMY3 weather data file.
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- September 24, 2015, by Marcus Fuchs:<br/>
- Replace Dymola specific annotation by <code>loadSelector</code>
- for MSL compliancy as reported by @tbeu at
- <a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
- </li>
- <li>
- March 5, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This function returns the longitude of the TMY3 weather data file.
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+September 24, 2015, by Marcus Fuchs:<br/>
+Replace Dymola specific annotation by <code>loadSelector</code>
+for MSL compliancy as reported by @tbeu at
+<a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
+</li>
+<li>
+March 5, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end getLongitudeTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeSpanTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeSpanTMY3.mo
index a500bb8813..cdee77f3ad 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeSpanTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeSpanTMY3.mo
@@ -14,25 +14,25 @@ external "C" getTimeSpan(filNam, tabNam, timeSpan)
   IncludeDirectory="modelica://AixLib/Resources/C-Sources");
 
   annotation (Documentation(info="<html>
- <p>
- This function returns the start time (first time stamp) and end time
- (last time stamp plus average increment) of the TMY3 weather data file.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- April 16, 2019, by Jianjun Hu:<br/>
- Reimplemented to use a C function, this is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1108\">#1108</a>.
- </li>
- <li>
- November 15, 2017, by Ana Constantin:<br/>
- First implementation, as part of solution to <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">#842</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function returns the start time (first time stamp) and end time
+(last time stamp plus average increment) of the TMY3 weather data file.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+April 16, 2019, by Jianjun Hu:<br/>
+Reimplemented to use a C function, this is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1108\">#1108</a>.
+</li>
+<li>
+November 15, 2017, by Ana Constantin:<br/>
+First implementation, as part of solution to <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">#842</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end getTimeSpanTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeZoneTMY3.mo b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeZoneTMY3.mo
index 03590c5065..2b5ca8f38e 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeZoneTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/getTimeZoneTMY3.mo
@@ -29,24 +29,24 @@ algorithm
        String(timZon) + " (= " + String(timZon/3600) + " hours).");
 
   annotation (Documentation(info="<html>
- This function returns the time zone of the TMY3 weather data file.
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- September 24, 2015, by Marcus Fuchs:<br/>
- Replace Dymola specific annotation by <code>loadSelector</code>
- for MSL compliancy as reported by @tbeu at
- <a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
- </li>
- <li>
- March 5, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This function returns the time zone of the TMY3 weather data file.
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+September 24, 2015, by Marcus Fuchs:<br/>
+Replace Dymola specific annotation by <code>loadSelector</code>
+for MSL compliancy as reported by @tbeu at
+<a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
+</li>
+<li>
+March 5, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end getTimeZoneTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/BaseClasses/package.order b/AixLib/BoundaryConditions/WeatherData/BaseClasses/package.order
index ea5c1e4422..828656a40f 100644
--- a/AixLib/BoundaryConditions/WeatherData/BaseClasses/package.order
+++ b/AixLib/BoundaryConditions/WeatherData/BaseClasses/package.order
@@ -22,6 +22,7 @@ LimiterTotalSkyCover
 LimiterWindDirection
 LimiterWindSpeed
 LocalCivilTime
+PartialConvertTime
 PartialLimiter
 PartialLimiterMin
 SolarTime
diff --git a/AixLib/BoundaryConditions/WeatherData/Bus.mo b/AixLib/BoundaryConditions/WeatherData/Bus.mo
index d93b87a2d3..4120fe3175 100644
--- a/AixLib/BoundaryConditions/WeatherData/Bus.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Bus.mo
@@ -2,6 +2,40 @@ within AixLib.BoundaryConditions.WeatherData;
 expandable connector Bus "Data bus that stores weather data"
   extends Modelica.Icons.SignalBus;
 
+  Modelica.Units.SI.Temperature TDryBul(start=293.15) "Dry bulb temperature";
+  Modelica.Units.SI.Temperature TWetBul(start=293.15) "Wet bulb temperature";
+  Modelica.Units.SI.Temperature TDewPoi "Dew point temperature";
+  Modelica.Units.SI.Temperature TBlaSky "Black-body sky temperature";
+
+  Real relHum(final unit="1") "Relative humidity";
+
+  Real HDirNor(final unit="W/m2") "Direct normal solar irradiation";
+  Real HGloHor(final unit="W/m2") "Global horizontal solar irradiation";
+  Real HDifHor(final unit="W/m2") "Diffuse horizontal solar irradiation";
+
+  Real HHorIR(final unit="W/m2") "Horizontal infrared irradiation";
+
+  Modelica.Units.SI.Angle winDir "Wind direction";
+  Modelica.Units.SI.Velocity winSpe "Wind speed";
+
+  Modelica.Units.SI.Height ceiHei "Cloud cover ceiling height";
+  Real nOpa(final unit="1") "Opaque sky cover";
+  Real nTot(final unit="1") "Total sky cover";
+
+  Modelica.Units.SI.Angle lat "Latitude of the location";
+  Modelica.Units.SI.Angle lon "Longitude of the location";
+  Modelica.Units.SI.Height alt "Location altitude above sea level";
+
+  Modelica.Units.SI.AbsolutePressure pAtm "Atmospheric pressure";
+
+  Modelica.Units.SI.Angle solAlt "Solar altitude angle";
+  Modelica.Units.SI.Angle solDec "Solar declination angle";
+  Modelica.Units.SI.Angle solHouAng "Solar hour angle";
+  Modelica.Units.SI.Angle solZen "Solar zenith angle";
+
+  Modelica.Units.SI.Time solTim "Solar time";
+  Modelica.Units.SI.Time cloTim "Model time";
+
   annotation (
     defaultComponentName="weaBus",
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,
@@ -10,16 +44,27 @@ expandable connector Bus "Data bus that stores weather data"
           lineColor={255,204,51},
           lineThickness=0.5)}),
     Documentation(info="<html>
- <p>
- This component is an expandable connector that is used to implement a bus that contains the weather data.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 25, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This component is an expandable connector that is used to implement a bus that contains the weather data.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+September 22, 2023, by Michael Wetter:<br/>
+Declared the variables that are on the bus.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1798\">IBPSA, #1798</a>.
+</li>
+<li>
+June 25, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Bus;
diff --git a/AixLib/BoundaryConditions/WeatherData/Examples/ReaderTMY3.mo b/AixLib/BoundaryConditions/WeatherData/Examples/ReaderTMY3.mo
index 2e893aff49..b744b0c223 100644
--- a/AixLib/BoundaryConditions/WeatherData/Examples/ReaderTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Examples/ReaderTMY3.mo
@@ -27,20 +27,20 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/Examples/ReaderTMY3.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the TMY3 data reader.
- The instance <code>weaDat</code> obtains all weather data from the weather file,
- whereas the instance <code>weaDatInpCon</code> obtains the global horizontal and
- the diffuse horizontal solar radiation from its input connectors.
- </p>
- </html>",
+<p>
+This model tests the TMY3 data reader.
+The instance <code>weaDat</code> obtains all weather data from the weather file,
+whereas the instance <code>weaDatInpCon</code> obtains the global horizontal and
+the diffuse horizontal solar radiation from its input connectors.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 25, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 25, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReaderTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/BaseClasses/PartialRadOnTiltedSurf.mo b/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/BaseClasses/PartialRadOnTiltedSurf.mo
index 5bc36fc8f9..846505b76c 100644
--- a/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/BaseClasses/PartialRadOnTiltedSurf.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/BaseClasses/PartialRadOnTiltedSurf.mo
@@ -1,7 +1,7 @@
 within AixLib.BoundaryConditions.WeatherData.Old.WeatherTRY.RadiationOnTiltedSurface.BaseClasses;
 partial model PartialRadOnTiltedSurf
-  parameter Integer WeatherFormat = 1 "Format weather file" annotation (Dialog(group=
-        "Properties of Weather Data",                                                                              compact = true, descriptionLabel = true), choices(choice = 1 "TRY", choice= 2 "TMY", radioButtons = true));
+  parameter Boolean WeatherFormat = false "Format weather file: If checked TMY, else TRY" annotation (Dialog(group=
+        "Properties of Weather Data",                                                                              descriptionLabel = true), choices(checkBox = true));
   parameter Modelica.Units.NonSI.Angle_deg Latitude=49.5 "latitude of location"
     annotation (Dialog(group="Location Properties"));
   parameter Real GroundReflection=0.2 "ground reflection coefficient"
diff --git a/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/RadOnTiltedSurf_Liu.mo b/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/RadOnTiltedSurf_Liu.mo
index 52d5a86bba..f11fc2787c 100644
--- a/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/RadOnTiltedSurf_Liu.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/RadOnTiltedSurf_Liu.mo
@@ -48,10 +48,10 @@ equation
   R = R_help;
 
   // conversion of direct and diffuse horizontal radiation
-  if WeatherFormat == 1 then // TRY
+  if not WeatherFormat then // TRY
     InBeamRadHor = solarInput1;
     InDiffRadHor = solarInput2;
-  else  // WeatherFormat == 2 , TMY then
+  else  // WeatherFormat == true , TMY then
     InBeamRadHor = solarInput1 * cos_theta_z;
     InDiffRadHor = max(solarInput2-InBeamRadHor, 0);
   end if;
diff --git a/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/RadOnTiltedSurf_Perez.mo b/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/RadOnTiltedSurf_Perez.mo
index 82616f4158..8cfd077cdf 100644
--- a/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/RadOnTiltedSurf_Perez.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/RadiationOnTiltedSurface/RadOnTiltedSurf_Perez.mo
@@ -192,10 +192,10 @@ equation
       R = a / b;
 
   // conversion of direct and diffuse horizontal radiation
-  if WeatherFormat == 1 then // TRY
+  if not WeatherFormat then // TRY
     InBeamRadHor = solarInput1;
     InDiffRadHor = solarInput2;
-  else  // WeatherFormat == 2 , TMY then
+  else  // WeatherFormat == true , TMY then
     InBeamRadHor = solarInput1 * cos_theta_z;
     InDiffRadHor = max(solarInput2-InBeamRadHor, 0);
   end if;
diff --git a/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/Weather.mo b/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/Weather.mo
index 9e0f6a52a6..eb3acfeef5 100644
--- a/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/Weather.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Old/WeatherTRY/Weather.mo
@@ -25,16 +25,15 @@ model Weather "Complex weather model"
 
   replaceable model RadOnTiltedSurface =
       AixLib.BoundaryConditions.WeatherData.Old.WeatherTRY.RadiationOnTiltedSurface.RadOnTiltedSurf_Liu
-    constrainedby AixLib.BoundaryConditions.WeatherData.Old.WeatherTRY.RadiationOnTiltedSurface.BaseClasses.PartialRadOnTiltedSurf
+    constrainedby
+    AixLib.BoundaryConditions.WeatherData.Old.WeatherTRY.RadiationOnTiltedSurface.BaseClasses.PartialRadOnTiltedSurf
     "Model for calculating radiation on tilted surfaces"                                                                            annotation(Dialog(group="Solar radiation on oriented surfaces", descriptionLabel = true), choicesAllMatching= true);
 
   parameter
     DataBase.Weather.SurfaceOrientation.SurfaceOrientationBaseDataDefinition         SOD = DataBase.Weather.SurfaceOrientation.SurfaceOrientationData_N_E_S_W_Hor()
     "Surface orientation data"                                                                                                     annotation(Dialog(group = "Solar radiation on oriented surfaces", descriptionLabel = true), choicesAllMatching = true);
   Utilities.Interfaces.SolarRad_out SolarRadiation_OrientedSurfaces[SOD.nSurfaces] annotation(Placement(transformation(extent = {{-10, -10}, {10, 10}}, rotation = 90, origin={50,96}),    iconTransformation(extent = {{-10, -10}, {10, 10}}, rotation = 270, origin = {-78, -110})));
-  parameter Integer Outopt = 2 "Output options" annotation(Dialog(tab = "Optional output vector", compact = true, descriptionLabel = true), choices(choice = 1
-        "one vector",                                                                                                    choice = 2
-        "individual vectors",                                                                                                    radioButtons = true));
+  parameter Boolean outOpt = true "Output individual vectors instead of one vector [-]" annotation(Dialog(tab = "Optional output vector", descriptionLabel = true), choices(checkBox = true));
   parameter Boolean Cloud_cover = false "Cloud cover [-] (TRY col 7)" annotation(Dialog(tab = "Optional output vector", descriptionLabel = true), choices(checkBox = true));
   parameter Boolean Wind_dir = false "Wind direction [deg] (TRY col 8)" annotation(Dialog(tab = "Optional output vector", descriptionLabel = true), choices(checkBox = true));
   parameter Boolean Wind_speed = false "Wind speed [m/s]  (TRY col 9)" annotation(Dialog(tab = "Optional output vector", descriptionLabel = true), choices(checkBox = true));
@@ -52,24 +51,24 @@ model Weather "Complex weather model"
     Latitude=Latitude,
     DiffWeatherDataTime=DiffWeatherDataTime) annotation (Placement(
         transformation(extent={{-62,18},{-38,42}})));
-  RadOnTiltedSurface RadOnTiltedSurf[SOD.nSurfaces](each Latitude = Latitude, each GroundReflection = GroundReflection, Azimut = SOD.Azimut, Tilt = SOD.Tilt, each WeatherFormat=1) annotation(Placement(transformation(extent = {{-2, 18}, {22, 42}})));
+  RadOnTiltedSurface RadOnTiltedSurf[SOD.nSurfaces](each Latitude = Latitude, each GroundReflection = GroundReflection, Azimut = SOD.Azimut, Tilt = SOD.Tilt, each WeatherFormat=false) annotation(Placement(transformation(extent = {{-2, 18}, {22, 42}})));
   Modelica.Blocks.Sources.CombiTimeTable WeatherData(fileName = Modelica.Utilities.Files.loadResource(fileName), columns = columns, offset = offset, table = [0, 0; 1, 1], startTime = scalar(startTime), tableName = tableName, tableOnFile = tableName <> "NoName", smoothness = smoothness, extrapolation = extrapolation) annotation(Placement(transformation(extent = {{-60, -70}, {-40, -50}})));
   Modelica.Blocks.Routing.DeMultiplex3 deMultiplex(n3 = 9) annotation(Placement(transformation(extent = {{-26, -70}, {-6, -50}})));
-  Modelica.Blocks.Interfaces.RealOutput WeatherDataVector[m] if Outopt == 1 and (Cloud_cover or Wind_dir or Wind_speed or Air_temp or Air_press or Mass_frac or Rel_hum or Sky_rad or Ter_rad) annotation(Placement(transformation(origin = {-1, -110}, extent = {{-10, -10}, {10, 10}}, rotation = 270)));
-  Modelica.Blocks.Interfaces.RealOutput CloudCover if Cloud_cover and Outopt == 2 "[0..8]" annotation(Placement(transformation(extent = {{114, 74}, {134, 94}}), iconTransformation(extent = {{150, 110}, {170, 130}})));
-  Modelica.Blocks.Interfaces.RealOutput WindDirection(unit = "deg") if Wind_dir and Outopt == 2
+  Modelica.Blocks.Interfaces.RealOutput WeatherDataVector[m] if outOpt == false and (Cloud_cover or Wind_dir or Wind_speed or Air_temp or Air_press or Mass_frac or Rel_hum or Sky_rad or Ter_rad) annotation(Placement(transformation(origin = {-1, -110}, extent = {{-10, -10}, {10, 10}}, rotation = 270)));
+  Modelica.Blocks.Interfaces.RealOutput CloudCover if Cloud_cover and outOpt "[0..8]" annotation(Placement(transformation(extent = {{114, 74}, {134, 94}}), iconTransformation(extent = {{150, 110}, {170, 130}})));
+  Modelica.Blocks.Interfaces.RealOutput WindDirection(unit = "deg") if Wind_dir and outOpt
     "in deg [0...360]"                                                                                             annotation(Placement(transformation(extent = {{126, 52}, {146, 72}}), iconTransformation(extent = {{150, 80}, {170, 100}})));
-  Modelica.Blocks.Interfaces.RealOutput WindSpeed(unit = "m/s") if Wind_speed and Outopt == 2 "in m/s" annotation(Placement(transformation(extent = {{126, 32}, {146, 52}}), iconTransformation(extent = {{150, 50}, {170, 70}})));
-  Modelica.Blocks.Interfaces.RealOutput AirTemp(unit = "K") if Air_temp and Outopt == 2
+  Modelica.Blocks.Interfaces.RealOutput WindSpeed(unit = "m/s") if Wind_speed and outOpt "in m/s" annotation(Placement(transformation(extent = {{126, 32}, {146, 52}}), iconTransformation(extent = {{150, 50}, {170, 70}})));
+  Modelica.Blocks.Interfaces.RealOutput AirTemp(unit = "K") if Air_temp and outOpt
     "in Kelvin"                                                                                     annotation(Placement(transformation(extent = {{126, 14}, {146, 34}}), iconTransformation(extent = {{150, 20}, {170, 40}})));
-  Modelica.Blocks.Interfaces.RealOutput AirPressure(unit = "Pa") if Air_press and Outopt == 2 "in Pa" annotation(Placement(transformation(extent = {{126, -8}, {146, 12}}), iconTransformation(extent = {{150, -10}, {170, 10}})));
-  Modelica.Blocks.Interfaces.RealOutput WaterInAir if Mass_frac and Outopt == 2
+  Modelica.Blocks.Interfaces.RealOutput AirPressure(unit = "Pa") if Air_press and outOpt "in Pa" annotation(Placement(transformation(extent = {{126, -8}, {146, 12}}), iconTransformation(extent = {{150, -10}, {170, 10}})));
+  Modelica.Blocks.Interfaces.RealOutput WaterInAir if Mass_frac and outOpt
     "in kg/kg"                                                                             annotation(Placement(transformation(extent = {{126, -24}, {146, -4}}), iconTransformation(extent = {{150, -40}, {170, -20}})));
-  Modelica.Blocks.Interfaces.RealOutput RelHumidity if Rel_hum and Outopt == 2
+  Modelica.Blocks.Interfaces.RealOutput RelHumidity if Rel_hum and outOpt
     "in percent"                                                                            annotation(Placement(transformation(extent = {{126, -42}, {146, -22}}), iconTransformation(extent = {{150, -70}, {170, -50}})));
-  Modelica.Blocks.Interfaces.RealOutput SkyRadiation(unit = "W/m2") if Sky_rad and Outopt == 2 "in W/m2"
-                                                                                                        annotation(Placement(transformation(extent = {{126, -62}, {146, -42}}), iconTransformation(extent = {{150, -100}, {170, -80}})));
-  Modelica.Blocks.Interfaces.RealOutput TerrestrialRadiation(unit = "W/m2") if Ter_rad and Outopt == 2 "in W/m2"
+  Modelica.Blocks.Interfaces.RealOutput SkyRadiation(unit = "W/m2") if Sky_rad and outOpt "in W/m2"
+                                                                                                   annotation(Placement(transformation(extent = {{126, -62}, {146, -42}}), iconTransformation(extent = {{150, -100}, {170, -80}})));
+  Modelica.Blocks.Interfaces.RealOutput TerrestrialRadiation(unit = "W/m2") if Ter_rad and outOpt "in W/m2"
                                                                                                         annotation(Placement(transformation(extent = {{126, -78}, {146, -58}}), iconTransformation(extent = {{150, -130}, {170, -110}})));
   Modelica.Blocks.Math.Gain hPa_to_Pa(k = 100) if Air_press annotation(Placement(transformation(extent = {{26, -60}, {36, -50}})));
   Modelica.Blocks.Math.Gain percent_to_unit(k = 0.01) if Rel_hum annotation(Placement(transformation(extent = {{26, -78}, {36, -68}})));
@@ -93,7 +92,7 @@ initial equation
 equation
   // cloud cover
   if Cloud_cover then
-    if Outopt == 1 then
+    if outOpt == false then
       connect(WeatherDataVector[PosWV[1]], deMultiplex.y3[1]);
     else
       connect(CloudCover, deMultiplex.y3[1]);
@@ -101,7 +100,7 @@ equation
   end if;
   // wind direction
   if Wind_dir then
-    if Outopt == 1 then
+    if not outOpt then
       connect(WeatherDataVector[PosWV[2]], deMultiplex.y3[2]);
     else
       connect(WindDirection, deMultiplex.y3[2]);
@@ -109,7 +108,7 @@ equation
   end if;
   // wind speed
   if Wind_speed then
-    if Outopt == 1 then
+    if not outOpt then
       connect(WeatherDataVector[PosWV[3]], deMultiplex.y3[3]);
     else
       connect(WindSpeed, deMultiplex.y3[3]);
@@ -117,7 +116,7 @@ equation
   end if;
   // air temperature
   if Air_temp then
-    if Outopt == 1 then
+    if not outOpt then
       connect(deMultiplex.y3[4], from_degC.u);
       connect(WeatherDataVector[PosWV[4]], from_degC.y);
     else
@@ -127,7 +126,7 @@ equation
   end if;
   // air pressure, conversion from hPa to Pa
   if Air_press then
-    if Outopt == 1 then
+    if not outOpt then
       connect(deMultiplex.y3[5], hPa_to_Pa.u);
       connect(WeatherDataVector[PosWV[5]], hPa_to_Pa.y);
     else
@@ -137,7 +136,7 @@ equation
   end if;
   // mass fraction water in dry air, conversion from g/kg to kg/kg
   if Mass_frac then
-    if Outopt == 1 then
+    if not outOpt then
       connect(deMultiplex.y3[6], g_to_kg.u);
       connect(WeatherDataVector[PosWV[6]], g_to_kg.y);
     else
@@ -147,7 +146,7 @@ equation
   end if;
   // rel. humidity, conversion from % to 0..1
   if Rel_hum then
-    if Outopt == 1 then
+    if not outOpt then
       connect(deMultiplex.y3[7], percent_to_unit.u);
       connect(WeatherDataVector[PosWV[7]], percent_to_unit.y);
     else
@@ -157,7 +156,7 @@ equation
   end if;
   // longwave sky radiation
   if Sky_rad then
-    if Outopt == 1 then
+    if not outOpt then
       connect(WeatherDataVector[PosWV[8]], deMultiplex.y3[8]);
     else
       connect(SkyRadiation, deMultiplex.y3[8]);
@@ -165,7 +164,7 @@ equation
   end if;
   // longwave terrestric radiation
   if Ter_rad then
-    if Outopt == 1 then
+    if not outOpt then
       connect(WeatherDataVector[PosWV[9]], deMultiplex.y3[9]);
     else
       connect(TerrestrialRadiation, deMultiplex.y3[9]);
diff --git a/AixLib/BoundaryConditions/WeatherData/ReaderTMY3.mo b/AixLib/BoundaryConditions/WeatherData/ReaderTMY3.mo
index 224fc7409e..09820cef66 100644
--- a/AixLib/BoundaryConditions/WeatherData/ReaderTMY3.mo
+++ b/AixLib/BoundaryConditions/WeatherData/ReaderTMY3.mo
@@ -222,16 +222,16 @@ block ReaderTMY3 "Reader for TMY3 weather data"
     Evaluate=true,
     Dialog(tab="Advanced", group="Sky temperature"));
 
-  final parameter Modelica.Units.SI.Angle lon(displayUnit="deg")=
+  final parameter Modelica.Units.SI.Angle lon(displayUnit="deg") =
     AixLib.BoundaryConditions.WeatherData.BaseClasses.getLongitudeTMY3(filNam)
     "Longitude";
-  final parameter Modelica.Units.SI.Angle lat(displayUnit="deg")=
+  final parameter Modelica.Units.SI.Angle lat(displayUnit="deg") =
     AixLib.BoundaryConditions.WeatherData.BaseClasses.getLatitudeTMY3(filNam)
     "Latitude";
-  final parameter Modelica.Units.SI.Time timZon(displayUnit="h")=
+  final parameter Modelica.Units.SI.Time timZon(displayUnit="h") =
     AixLib.BoundaryConditions.WeatherData.BaseClasses.getTimeZoneTMY3(filNam)
     "Time zone";
-  final parameter Modelica.Units.SI.Length alt(displayUnit="m")=
+  final parameter Modelica.Units.SI.Length alt(displayUnit="m") =
     AixLib.BoundaryConditions.WeatherData.BaseClasses.getAltitudeLocationTMY3(
     filNam) "Location altitude above sea level";
 
@@ -450,28 +450,28 @@ protected
           textColor={0,0,0},
             textString="Latitude")}),
     Documentation(info="<html>
- <p>
- Block to output the latitude of the location.
- This block is added so that the latitude is displayed
- with a comment in the GUI of the weather bus connector.
- </p>
- <h4>Implementation</h4>
- <p>
- If
- <a href=\"modelica://Modelica.Blocks.Sources.Constant\">
- Modelica.Blocks.Sources.Constant</a> where used, then
- the comment for the latitude would be \"Connector of Real output signal\".
- As this documentation string cannot be overwritten, a new block
- was implemented.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 4, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Block to output the latitude of the location.
+This block is added so that the latitude is displayed
+with a comment in the GUI of the weather bus connector.
+</p>
+<h4>Implementation</h4>
+<p>
+If
+<a href=\"modelica://Modelica.Blocks.Sources.Constant\">
+Modelica.Blocks.Sources.Constant</a> where used, then
+the comment for the latitude would be \"Connector of Real output signal\".
+As this documentation string cannot be overwritten, a new block
+was implemented.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 4, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end Latitude;
 
   block Longitude "Generate constant signal of type Real"
@@ -494,28 +494,28 @@ protected
           textColor={0,0,0},
             textString="Longitude")}),
     Documentation(info="<html>
- <p>
- Block to output the longitude of the location.
- This block is added so that the longitude is displayed
- with a comment in the GUI of the weather bus connector.
- </p>
- <h4>Implementation</h4>
- <p>
- If
- <a href=\"modelica://Modelica.Blocks.Sources.Constant\">
- Modelica.Blocks.Sources.Constant</a> where used, then
- the comment for the longitude would be \"Connector of Real output signal\".
- As this documentation string cannot be overwritten, a new block
- was implemented.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 4, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Block to output the longitude of the location.
+This block is added so that the longitude is displayed
+with a comment in the GUI of the weather bus connector.
+</p>
+<h4>Implementation</h4>
+<p>
+If
+<a href=\"modelica://Modelica.Blocks.Sources.Constant\">
+Modelica.Blocks.Sources.Constant</a> where used, then
+the comment for the longitude would be \"Connector of Real output signal\".
+As this documentation string cannot be overwritten, a new block
+was implemented.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 4, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end Longitude;
 
   block Altitude "Generate constant signal of type Real"
@@ -538,28 +538,28 @@ protected
           textColor={0,0,0},
             textString="Altitude")}),
     Documentation(info="<html>
- <p>
- Block to output the altitude of the location.
- This block is added so that the altitude is displayed
- with a comment in the GUI of the weather bus connector.
- </p>
- <h4>Implementation</h4>
- <p>
- If
- <a href=\"modelica://Modelica.Blocks.Sources.Constant\">
- Modelica.Blocks.Sources.Constant</a> where used, then
- the comment for the Altitude would be \"Connector of Real output signal\".
- As this documentation string cannot be overwritten, a new block
- was implemented.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Block to output the altitude of the location.
+This block is added so that the altitude is displayed
+with a comment in the GUI of the weather bus connector.
+</p>
+<h4>Implementation</h4>
+<p>
+If
+<a href=\"modelica://Modelica.Blocks.Sources.Constant\">
+Modelica.Blocks.Sources.Constant</a> where used, then
+the comment for the Altitude would be \"Connector of Real output signal\".
+As this documentation string cannot be overwritten, a new block
+was implemented.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end Altitude;
 
 equation
@@ -946,891 +946,891 @@ equation
           textColor={255,255,255},
           textString=DynamicSelect("", String(weaBus.TDryBul-273.15, format=".1f")))}),
     Documentation(info="<html>
- <p>
- This component reads TMY3 weather data (Wilcox and Marion, 2008) or user specified weather data.
- The Modelica built-in variable <code>time</code> determines what row
- of the weather file is read.
- The value of <code>time</code> is the number of seconds
- that have passed since January 1st at midnight (00:00) in the local time zone.
- The local time zone value, longitude and latitute are also read from the weather data,
- such that the solar position computations are consistent with the weather data.
- </p>
- <p>
- The weather data format is the Typical Meteorological Year (TMY3)
- as obtained from the EnergyPlus web site at
- <a href=\"http://energyplus.net/weather\">
- http://energyplus.net/weather</a>. These
- data, which are in the EnergyPlus format, need to be converted as described
- below.
- </p>
- <!-- ============================================== -->
- <h4>Output to weaBus</h4>
- <p>
- The following variables serve as output and are accessible via <code>weaBus</code>:
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <!-- ============================================== -->
- <tr>
-   <th>Name
-   </th>
-   <th>Unit
-   </th>
-   <th>Description
-   </th>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>HDifHor</code>
-   </td>
-   <td>
-     W/m2
-   </td>
-   <td>
-     Horizontal diffuse solar radiation.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>HDifNor</code>
-   </td>
-   <td>
-     W/m2
-   </td>
-   <td>
-     Direct normal radiation.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>HGloHor</code>
-   </td>
-   <td>
-     W/m2
-   </td>
-   <td>
-     Horizontal global radiation.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>HHorIR</code>
-   </td>
-   <td>
-     W/m2
-   </td>
-   <td>
-     Horizontal infrared irradiation.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>TBlaSky</code>
-   </td>
-   <td>
-     K
-   </td>
-   <td>
-     Output temperature.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>TDewPoi</code>
-   </td>
-   <td>
-     K
-   </td>
-   <td>
-     Dew point temperature.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>TDryBul</code>
-   </td>
-   <td>
-     K
-   </td>
-   <td>
-     Dry bulb temperature at ground level.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>TWetBul</code>
-   </td>
-   <td>
-     K
-   </td>
-   <td>
-     Wet bulb temperature.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>celHei</code>
-   </td>
-   <td>
-     m
-   </td>
-   <td>
-     Ceiling height.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>cloTim</code>
-   </td>
-   <td>
-     s
-   </td>
-   <td>
-     One-based day number in seconds.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>lat</code>
-   </td>
-   <td>
-     rad
-   </td>
-   <td>
-   Latitude of the location.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>lon</code>
-   </td>
-   <td>
-     rad
-   </td>
-   <td>
-   Longitude of the location.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>nOpa</code>
-   </td>
-   <td>
-     1
-   </td>
-   <td>
-   Opaque sky cover [0, 1].
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>nTot</code>
-   </td>
-   <td>
-     1
-   </td>
-   <td>
-    Total sky Cover [0, 1].
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>pAtm</code>
-   </td>
-   <td>
-     Pa
-   </td>
-   <td>
-     Atmospheric pressure.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>relHum</code>
-   </td>
-   <td>
-     1
-   </td>
-   <td>
-     Relative humidity.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>solAlt</code>
-   </td>
-   <td>
-     rad
-   </td>
-   <td>
-     Altitude angle.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>solDec</code>
-   </td>
-   <td>
-     rad
-   </td>
-   <td>
-     Declination angle.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>solHouAng</code>
-   </td>
-   <td>
-     rad
-   </td>
-   <td>
-     Solar hour angle.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>solTim</code>
-   </td>
-   <td>
-     s
-   </td>
-   <td>
-     Solar time.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>solZen</code>
-   </td>
-   <td>
-     rad
-   </td>
-   <td>
-     Zenith angle.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>winDir</code>
-   </td>
-   <td>
-     rad
-   </td>
-   <td>
-     Wind direction.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     <code>winSpe</code>
-   </td>
-   <td>
-     m/s
-   </td>
-   <td>
-     Wind speed.
-   </td>
- </tr>
- </table>
- <!-- ============================================== -->
- <h4>Adding new weather data</h4>
- <p>
- To add new weather data, proceed as follows:
- </p>
- <ol>
- <li>
- Download the weather data file with the <code>epw</code> extension from
- <a href=\"http://energyplus.net/weather\">
- http://energyplus.net/weather</a>.
- </li>
- <li>
- Add the file to <code>AixLib/Resources/weatherdata</code> (or to any directory
- for which you have write permission).
- </li>
- <li>
- On a console window, type<pre>
-   cd AixLib/Resources/weatherdata
-   java -jar ../bin/ConvertWeatherData.jar inputFile.epw
- </pre>
-   if inputFile contains space in the name:
- <pre>
-   java -jar ../bin/ConvertWeatherData.jar \"inputFile .epw\"
- </pre>
- This will generate the weather data file <code>inputFile.mos</code>, which can be read
- by the model
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
- AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>.
- </li>
- </ol>
- <!-- ============================================== -->
- <h4>Location data that are read automatically from the weather data file</h4>
- <p>
- The following location data are automatically read from the weather file:
- </p>
- <ul>
- <li>
- The latitude of the weather station, <code>lat</code>,
- </li>
- <li>
- the longitude of the weather station, <code>lon</code>, and
- </li>
- <li>
- the time zone relative to Greenwich Mean Time, <code>timZone</code>.
- </li>
- </ul>
- <!-- ============================================== -->
- <h4>Wet bulb temperature</h4>
- <p>
- By default, the data bus contains the wet bulb temperature.
- This introduces a nonlinear equation.
- However, we have not observed an increase in computing time because
- of this equation.
- To disable the computation of the wet bulb temperature, set
- <code>computeWetBulbTemperature=false</code>.
- </p>
- <!-- ============================================== -->
- <h4>Using constant or user-defined input signals for weather data</h4>
- <p>
- This model has the option of using a constant value, using the data from the weather file,
- or using data from an input connector for the following variables:
- </p>
- <ul>
- <li>
- The atmospheric pressure,
- </li>
- <li>
- the ceiling height,
- </li>
- <li>
- the total sky cover,
- </li>
- <li>
- the opaque sky cover,
- </li>
- <li>
- the dry bulb temperature,
- </li>
- <li>
- the dew point temperature,
- </li>
- <li>
- the sky black body temperature,
- </li>
- <li>
- the relative humidity,
- </li>
- <li>
- the wind direction,
- </li>
- <li>
- the wind speed,
- </li>
- <li>
- the global horizontal radiation, direct normal and diffuse horizontal radiation,
- and
- </li>
- <li>
- the infrared horizontal radiation.
- </li>
- </ul>
- <p>
- By default, all data are obtained from the weather data file,
- except for the atmospheric pressure, which is set to the
- parameter <code>pAtm=101325</code> Pascals.
- </p>
- <p>
- The parameter <code>*Sou</code> configures the source of the data.
- For the atmospheric pressure, temperatures, relative humidity, wind speed and wind direction,
- the enumeration
- <a href=\"modelica://AixLib.BoundaryConditions.Types.DataSource\">
- AixLib.BoundaryConditions.Types.DataSource</a>
- is used as follows:
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <!-- ============================================== -->
- <tr>
-   <th>Parameter <code>*Sou</code>
-   </th>
-   <th>Data used to compute weather data.
-   </th>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     File
-   </td>
-   <td>
-     Use data from file.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     Parameter
-   </td>
-   <td>
-     Use value specified by the parameter.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     Input
-   </td>
-   <td>
-     Use value from the input connector.
-   </td>
- </tr>
- </table>
- <p>
- Because global, diffuse and direct radiation are related to each other, the parameter
- <code>HSou</code> is treated differently.
- It is set to a value of the enumeration
- <a href=\"modelica://AixLib.BoundaryConditions.Types.RadiationDataSource\">
- AixLib.BoundaryConditions.Types.RadiationDataSource</a>,
- and allows the following configurations:
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <!-- ============================================== -->
- <tr>
-   <th>Parameter <code>HSou</code>
-   </th>
-   <th>Data used to compute weather data.
-   </th>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     File
-   </td>
-   <td>
-     Use data from file.
-   </td>
- </tr>
- <!-- ============================================== -->
- <tr>
-   <td>
-     Input_HGloHor_HDifHor
-   </td>
-   <td>
-     Use global horizontal and diffuse horizontal radiation from input connector.
-   </td>
- </tr>
- <tr>
-   <td>
-     Input_HDirNor_HDifHor
-   </td>
-   <td>
-     Use direct normal and diffuse horizontal radiation from input connector.
-   </td>
- </tr>
- <tr>
-   <td>
-     Input_HDirNor_HGloHor
-   </td>
-   <td>
-     Use direct normal and global horizontal radiation from input connector.
-   </td>
- </tr>
- </table>
- <!-- ============================================== -->
- <h4>Length of weather data and simulation period</h4>
- <p>
- If weather data span a year, which is the default for TMY3 data, or multiple years,
- then this model can be used for simulations that span multiple years. The simulation
- start time needs to be set to the clock time of the respective start time. For example,
- to start at January 2 at 10am, set start time to <code>t=(24+10)*3600</code> seconds.
- For this computation, the used date and time (here January 2, 10 am) must be expressed in the same time zone
- as the one that is used to define the TMY3 file. This is usually the local (winter) time zone.
- The parameter `timZon` represents the TMY3 file time zone, expressed in seconds compared to UTC.
- </p>
- <p>
- Moreover, weather data need not span a whole year, or it can span across New Year.
- In this case, the simulation cannot exceed the time of the weather data file. Otherwise,
- the simulation stops with an error.
- </p>
- <p>
- As weather data have one entry at the start of the time interval, the end time of the weather
- data file is computed as the last time entry plus the average time increment of the file.
- For example, an hourly weather data file has 8760 entries, starting on January 1 at 0:00.
- The last entry in the file will be for December 31 at 23:00. As the time increment is 1 hour,
- the model assumes the weather file to end at December 31 at 23:00 plus 1 hour, e.g., at January 1 at 0:00.
- </p>
- <!-- ============================================== -->
- <h4>Notes</h4>
- <ol>
- <li>
- <p>
- In HVAC systems, when the fan is off, changes in atmospheric pressure can cause small air flow rates
- in the duct system due to change in pressure and hence in the mass of air that is stored
- in air volumes (such as in fluid junctions or in the room model).
- This may increase computing time. Therefore, the default value for the atmospheric pressure is set to a constant.
- Furthermore, if the initial pressure of air volumes are different
- from the atmospheric pressure, then fast pressure transients can happen in the first few seconds of the simulation.
- This can cause numerical problems for the solver. To avoid this problem, set the atmospheric pressure to the
- same value as the medium default pressure, which is typically set to the parameter <code>Medium.p_default</code>.
- For medium models for moist air and dry air, the default is
- <code>Medium.p_default=101325</code> Pascals.
- </p>
- </li>
- <li>
- <p>
- Different units apply depending on whether data are obtained from a file, or
- from a parameter or an input connector:
- </p>
- <ul>
- <li>
- When using TMY3 data from a file (e.g. <code>USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos</code>), the units must be the same as the original TMY3 file used by EnergyPlus (e.g.
- <code>USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.epw</code>).
- The TMY3 data used by EnergyPlus are in both SI units and non-SI units.
- If <code>Resources/bin/ConvertWeatherData.jar</code> is used to convert the <code>.epw</code> file to an <code>.mos</code> file, the units of the TMY3 data are preserved and the file can be directly
- used by this data reader.
- The data reader will automatically convert units to the SI units used by Modelica.
- For example, the dry bulb temperature <code>TDryBul</code> in TMY3 is in degree Celsius.
- The data reader will automatically convert the data to Kelvin.
- The wind direction <code>winDir</code> in TMY3 is degrees and will be automatically converted to radians.
- </li>
- <li>
- When using data from a parameter or from an input connector,
- the data must be in the SI units used by Modelica.
- For instance, the unit must be
- <code>Pa</code> for pressure,
- <code>K</code> for temperature,
- <code>W/m2</code> for solar radiations and
- <code>rad</code> for wind direction.
- </li>
- </ul>
- </li>
- <li>
- <p>
- Hourly and subhourly timestamp are handled in a different way in <code>.epw</code> files.
- From the EnergyPlus Auxiliary Programs Document (v9.3.0, p. 63):
- In hourly data the minute field can be <code>00</code> or <code>60</code>. In this case as mentioned in the previous section, the weather data
- is reported at the hourly value and the minute field has to be ignored, writing <code>1, 60</code> or <code>1, 00</code> is equivalent.
- If the minute field is between <code>00</code> and <code>60</code>, the file becomes subhourly, in this case the timestamp corresponds to the
- minute field in the considered hour. For example: <code>1, 30</code> is equivalent to <i>00:30</i> and <code>3, 45</code> is equivalent to <i>02:45</i>.<br/>
- (Note the offset in the hour digit.)
- </p>
- </li>
- <li>
- The ReaderTMY3 should only be used with TMY3 data. It contains a time shift for solar radiation data
- that is explained below. This time shift needs to be removed if the user may want to
- use the ReaderTMY3 for other weather data types.
- </li>
- </ol>
- <h4>Implementation</h4>
- <h5>Start and end data for annual weather data files</h5>
- <p>
- The TMY3 weather data, as well as the EnergyPlus weather data, start at 1:00 AM
- on January 1, and provide hourly data until midnight on December 31.
- Thus, the first entry for temperatures, humidity, wind speed etc. are values
- at 1:00 AM and not at midnight. Furthermore, the TMY3 weather data files can have
- values at midnight of December 31 that may be significantly different from the values
- at 1:00 AM on January 1.
- Since annual simulations require weather data that start at 0:00 on January 1,
- data need to be provided for this hour. Due to the possibly large change in
- weatherdata between 1:00 AM on January 1 and midnight at December 31,
- the weather data files in the AixLib library do not use the data entry from
- midnight at December 31 as the value for <i>t=0</i>. Rather, the
- value from 1:00 AM on January 1 is duplicated and used for 0:00 on January 1.
- To maintain a data record with <i>8760</i> hours, the weather data record from
- midnight at December 31 is deleted.
- These changes in the weather data file are done in the Java program
- <code>AixLib/Resources/bin/ConvertWeatherData.jar</code> that converts
- EnergyPlus weather data file to Modelica weather data files, and which is described
- above.
- The length of the weather data is calculated as the
- end time stamp minus start time stamp plus average increment, where the
- average increment is equal to the end time stamp minus start time stamp divided
- by the number of rows minus 1.
- This only works correctly for weather files with equidistant time stamps.
- </p>
- <h5>Time shift for solar radiation data</h5>
- <p>
- To read weather data from the TMY3 weather data file, there are
- two data readers in this model. One data reader obtains all data
- except solar radiation, and the other data reader reads only the
- solar radiation data, shifted by <i>30</i> minutes.
- The reason for this time shift is as follows:
- The TMY3 weather data file contains for solar radiation the
- \"...radiation received
- on a horizontal surface during
- the 60-minute period ending at
- the timestamp.\"
- 
- Thus, as the figure below shows, a more accurate interpolation is obtained if
- time is shifted by <i>30</i> minutes prior to reading the weather data.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/BoundaryConditions/WeatherData/RadiationTimeShift.png\"
- border=\"1\" />
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Wilcox S. and W. Marion. <i>Users Manual for TMY3 Data Sets</i>.
- Technical Report, NREL/TP-581-43156, revised May 2008.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed alt and lat to real inputs.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- May 2, 2021, by Ettore Zanetti:<br/>
- Added altitude to parameters.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- October 4, 2020, by Ettore Zanetti:<br/>
- Updated documentation for Java weather file generator.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1396\">#1396</a>.
- </li>
- <li>
- August 20, 2019, by Filip Jorissen:<br/>
- Better clarified the meaning of <code>time</code> in the documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1192\">#1192</a>.
- </li>
- <li>
- March 5, 2019, by Michael Wetter:<br/>
- Updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">#842</a>.
- </li>
- <li>
- September 20, 2018, by Michael Wetter:<br/>
- Corrected documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1022\">#1022</a>.
- </li>
- <li>
- December 4, 2017, by Michael Wetter:<br/>
- Removed function call to <code>getAbsolutePath</code>, as this causes in Dymola 2018FD01
- the error
- \"A call of loadResource with a non-literal string remains in the generated code; it will not work for an URI.\"
- when exporting <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone</a>
- as an FMU. Instead, if the weather file is specified as a Modelica, URI, syntax such as
- <code>Modelica.Utilities.Files.loadResource(\"modelica://AixLib/Resources/weatherdata/USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos\")</code>
- should be used.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/867\">#867</a>.
- </li>
- <li>
- February 18, 2017, by Filip Jorissen:<br/>
- Infrared radiation on horizontal surface is now delayed by 30 minutes
- such that the results in
- <a href=\"modelica://AixLib.BoundaryConditions.SkyTemperature.Examples.BlackBody\">TBlaSky</a>
- are consistent.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/648\">#648</a>.
- </li>
- <li>
- December 06, 2016, by Thierry S. Nouidui:<br/>
- Constrained the direct normal radiation to not be bigger than the solar constant when using
- global and diffuse solar radiation data provided via the inputs connectors.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/608\">#608</a>.
- </li>
- <li>
- April 21, 2016, by Michael Wetter:<br/>
- Introduced <code>absFilNam</code> to avoid multiple calls to
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
- AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/506\">Buildings, #506</a>.
- </li>
- <li>
- January 6, 2016, by Moritz Lauster:<br/>
- Changed output <code>radHorIR</code> to <code>HHorIR</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">#376</a>.
- </li>
- <li>
- January 4, 2016, by Moritz Lauster:<br/>
- Added a table in documentation with output variables accessible via <code>weaBus</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">#376</a>.
- </li>
- <li>
- December 15, 2015, by Michael Wetter:<br/>
- Added the block <code>cheTemBlaSky</code>. This also allows to graphically
- connect the black body sky temperature to the weather bus, which is required
- in Dymola 2016 for the variable <code>weaBus.TBlaSky</code> to appear
- in the graphical editor.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/377\">#377</a>.
- </li>
- <li>
- September 24, 2015, by Marcus Fuchs:<br/>
- Replace Dymola specific annotation by <code>loadSelector</code>
- for MSL compliancy as reported by @tbeu at
- <a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
- </li>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Removed redundant but consistent
- <code>connect(TBlaSkyCom.TBlaSky, weaBus.TBlaSky)</code>
- statement.
- This avoids a warning if
- <a href=\"modelica://AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.SkyClearness\">
- AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.SkyClearness</a>
- is translated in pedantic mode in Dymola 2016.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- March 26, 2015, by Michael Wetter:<br/>
- Added option to obtain the black body sky temperature
- from a parameter or an input signal.
- </li>
- <li>
- October 17, 2014, by Michael Wetter:<br/>
- Corrected error that led the total and opaque sky cover to be ten times
- too low if its value was obtained from the parameter or the input connector.
- For the standard configuration in which the sky cover is obtained from
- the weather data file, the model was correct. This error only affected
- the other two possible configurations.
- </li>
- <li>
- September 12, 2014, by Michael Wetter:<br/>
- Removed redundant connection <code>connect(conHorRad.HOut, cheHorRad.HIn);</code>.
- </li>
- <li>
- May 30, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- May 5, 2013, by Thierry S. Nouidui:<br/>
- Added the option to use a constant, an input signal or the weather file as the source
- for the ceiling height, the total sky cover, the opaque sky cover, the dew point temperature,
- and the infrared horizontal radiation <code>HInfHor</code>.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Improved the algorithm that determines the absolute path of the file.
- Now weather files are searched in the path specified, and if not found, the urls
- <code>file://</code>, <code>modelica://</code> and <code>modelica://AixLib</code>
- are added in this order to search for the weather file.
- This allows using the data reader without having to specify an absolute path,
- as long as the <code>AixLib</code> library
- is on the <code>MODELICAPATH</code>.
- This change was implemented in
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
- AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>
- and improves this weather data reader.
- </li>
- <li>
- May 2, 2013, by Michael Wetter:<br/>
- Added function call to <code>getAbsolutePath</code>.
- </li>
- <li>
- October 16, 2012, by Michael Wetter:<br/>
- Added computation of the wet bulb temperature.
- Computing the wet bulb temperature introduces a nonlinear
- equation. As we have not observed an increase in computing time
- because of computing the wet bulb temperature, it is computed
- by default. By setting the parameter
- <code>computeWetBulbTemperature=false</code>, the computation of the
- wet bulb temperature can be removed.
- Revised documentation.
- </li>
- <li>
- August 11, 2012, by Wangda Zuo:<br/>
- Renamed <code>radHor</code> to <code>radHorIR</code> and
- improved the optional inputs for radiation data.
- </li>
- <li>
- July 24, 2012, by Wangda Zuo:<br/>
- Corrected the notes of SI unit requirements for input files.
- </li>
- <li>
- July 13, 2012, by Michael Wetter:<br/>
- Removed assignment of <code>HGloHor_in</code> in its declaration,
- because this gives an overdetermined system if the input connector
- is used.
- Removed non-required assignments of attribute <code>displayUnit</code>.
- </li>
- <li>
- February 25, 2012, by Michael Wetter:<br/>
- Added subbus for solar position, which is needed by irradition and
- shading model.
- </li>
- <li>
- November 29, 2011, by Michael Wetter:<br/>
- Fixed wrong display unit for <code>pAtm_in_internal</code> and
- made propagation of parameter final.
- </li>
- <li>
- October 27, 2011, by Wangda Zuo:<br/>
- <ol>
- <li>
- Added optional connectors for dry bulb temperature, relative humidity, wind speed, wind direction, global horizontal radiation, diffuse horizontal radiation.<br/>
- </li>
- <li>
- Separate the unit conversion for TMY3 data and data validity check.
- </li>
- </ol>
- </li>
- <li>
- October 3, 2011, by Michael Wetter:<br/>
- Propagated value for sky temperature calculation to make it accessible as a parameter.
- </li>
- <li>
- July 20, 2011, by Michael Wetter:<br/>
- Added the option to use a constant, an input signal or the weather file as the source
- for the atmospheric pressure.
- </li><li>
- March 15, 2011, by Wangda Zuo:<br/>
- Delete the wet bulb temperature since it may cause numerical problem.
- </li>
- <li>
- March 7, 2011, by Wangda Zuo:<br/>
- Added wet bulb temperature. Changed reader to read only needed columns.
- Added explanation for 30 minutes shift for radiation data.
- </li>
- <li>
- March 5, 2011, by Michael Wetter:<br/>
- Changed implementation to obtain longitude and time zone directly
- from weather file.
- </li>
- <li>
- June 25, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component reads TMY3 weather data (Wilcox and Marion, 2008) or user specified weather data.
+The Modelica built-in variable <code>time</code> determines what row
+of the weather file is read.
+The value of <code>time</code> is the number of seconds
+that have passed since January 1st at midnight (00:00) in the local time zone.
+The local time zone value, longitude and latitute are also read from the weather data,
+such that the solar position computations are consistent with the weather data.
+</p>
+<p>
+The weather data format is the Typical Meteorological Year (TMY3)
+as obtained from the EnergyPlus web site at
+<a href=\"http://energyplus.net/weather\">
+http://energyplus.net/weather</a>. These
+data, which are in the EnergyPlus format, need to be converted as described
+below.
+</p>
+<!-- ============================================== -->
+<h4>Output to weaBus</h4>
+<p>
+The following variables serve as output and are accessible via <code>weaBus</code>:
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<!-- ============================================== -->
+<tr>
+  <th>Name
+  </th>
+  <th>Unit
+  </th>
+  <th>Description
+  </th>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>HDifHor</code>
+  </td>
+  <td>
+    W/m2
+  </td>
+  <td>
+    Horizontal diffuse solar radiation.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>HDifNor</code>
+  </td>
+  <td>
+    W/m2
+  </td>
+  <td>
+    Direct normal radiation.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>HGloHor</code>
+  </td>
+  <td>
+    W/m2
+  </td>
+  <td>
+    Horizontal global radiation.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>HHorIR</code>
+  </td>
+  <td>
+    W/m2
+  </td>
+  <td>
+    Horizontal infrared irradiation.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>TBlaSky</code>
+  </td>
+  <td>
+    K
+  </td>
+  <td>
+    Output temperature.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>TDewPoi</code>
+  </td>
+  <td>
+    K
+  </td>
+  <td>
+    Dew point temperature.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>TDryBul</code>
+  </td>
+  <td>
+    K
+  </td>
+  <td>
+    Dry bulb temperature at ground level.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>TWetBul</code>
+  </td>
+  <td>
+    K
+  </td>
+  <td>
+    Wet bulb temperature.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>celHei</code>
+  </td>
+  <td>
+    m
+  </td>
+  <td>
+    Ceiling height.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>cloTim</code>
+  </td>
+  <td>
+    s
+  </td>
+  <td>
+    One-based day number in seconds.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>lat</code>
+  </td>
+  <td>
+    rad
+  </td>
+  <td>
+  Latitude of the location.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>lon</code>
+  </td>
+  <td>
+    rad
+  </td>
+  <td>
+  Longitude of the location.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>nOpa</code>
+  </td>
+  <td>
+    1
+  </td>
+  <td>
+  Opaque sky cover [0, 1].
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>nTot</code>
+  </td>
+  <td>
+    1
+  </td>
+  <td>
+   Total sky Cover [0, 1].
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>pAtm</code>
+  </td>
+  <td>
+    Pa
+  </td>
+  <td>
+    Atmospheric pressure.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>relHum</code>
+  </td>
+  <td>
+    1
+  </td>
+  <td>
+    Relative humidity.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>solAlt</code>
+  </td>
+  <td>
+    rad
+  </td>
+  <td>
+    Altitude angle.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>solDec</code>
+  </td>
+  <td>
+    rad
+  </td>
+  <td>
+    Declination angle.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>solHouAng</code>
+  </td>
+  <td>
+    rad
+  </td>
+  <td>
+    Solar hour angle.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>solTim</code>
+  </td>
+  <td>
+    s
+  </td>
+  <td>
+    Solar time.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>solZen</code>
+  </td>
+  <td>
+    rad
+  </td>
+  <td>
+    Zenith angle.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>winDir</code>
+  </td>
+  <td>
+    rad
+  </td>
+  <td>
+    Wind direction.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    <code>winSpe</code>
+  </td>
+  <td>
+    m/s
+  </td>
+  <td>
+    Wind speed.
+  </td>
+</tr>
+</table>
+<!-- ============================================== -->
+<h4>Adding new weather data</h4>
+<p>
+To add new weather data, proceed as follows:
+</p>
+<ol>
+<li>
+Download the weather data file with the <code>epw</code> extension from
+<a href=\"http://energyplus.net/weather\">
+http://energyplus.net/weather</a>.
+</li>
+<li>
+Add the file to <code>AixLib/Resources/weatherdata</code> (or to any directory
+for which you have write permission).
+</li>
+<li>
+On a console window, type<pre>
+  cd AixLib/Resources/weatherdata
+  java -jar ../bin/ConvertWeatherData.jar inputFile.epw
+</pre>
+  if inputFile contains space in the name:
+<pre>
+  java -jar ../bin/ConvertWeatherData.jar \"inputFile .epw\"
+</pre>
+This will generate the weather data file <code>inputFile.mos</code>, which can be read
+by the model
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>.
+</li>
+</ol>
+<!-- ============================================== -->
+<h4>Location data that are read automatically from the weather data file</h4>
+<p>
+The following location data are automatically read from the weather file:
+</p>
+<ul>
+<li>
+The latitude of the weather station, <code>lat</code>,
+</li>
+<li>
+the longitude of the weather station, <code>lon</code>, and
+</li>
+<li>
+the time zone relative to Greenwich Mean Time, <code>timZone</code>.
+</li>
+</ul>
+<!-- ============================================== -->
+<h4>Wet bulb temperature</h4>
+<p>
+By default, the data bus contains the wet bulb temperature.
+This introduces a nonlinear equation.
+However, we have not observed an increase in computing time because
+of this equation.
+To disable the computation of the wet bulb temperature, set
+<code>computeWetBulbTemperature=false</code>.
+</p>
+<!-- ============================================== -->
+<h4>Using constant or user-defined input signals for weather data</h4>
+<p>
+This model has the option of using a constant value, using the data from the weather file,
+or using data from an input connector for the following variables:
+</p>
+<ul>
+<li>
+The atmospheric pressure,
+</li>
+<li>
+the ceiling height,
+</li>
+<li>
+the total sky cover,
+</li>
+<li>
+the opaque sky cover,
+</li>
+<li>
+the dry bulb temperature,
+</li>
+<li>
+the dew point temperature,
+</li>
+<li>
+the sky black body temperature,
+</li>
+<li>
+the relative humidity,
+</li>
+<li>
+the wind direction,
+</li>
+<li>
+the wind speed,
+</li>
+<li>
+the global horizontal radiation, direct normal and diffuse horizontal radiation,
+and
+</li>
+<li>
+the infrared horizontal radiation.
+</li>
+</ul>
+<p>
+By default, all data are obtained from the weather data file,
+except for the atmospheric pressure, which is set to the
+parameter <code>pAtm=101325</code> Pascals.
+</p>
+<p>
+The parameter <code>*Sou</code> configures the source of the data.
+For the atmospheric pressure, temperatures, relative humidity, wind speed and wind direction,
+the enumeration
+<a href=\"modelica://AixLib.BoundaryConditions.Types.DataSource\">
+AixLib.BoundaryConditions.Types.DataSource</a>
+is used as follows:
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<!-- ============================================== -->
+<tr>
+  <th>Parameter <code>*Sou</code>
+  </th>
+  <th>Data used to compute weather data.
+  </th>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    File
+  </td>
+  <td>
+    Use data from file.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    Parameter
+  </td>
+  <td>
+    Use value specified by the parameter.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    Input
+  </td>
+  <td>
+    Use value from the input connector.
+  </td>
+</tr>
+</table>
+<p>
+Because global, diffuse and direct radiation are related to each other, the parameter
+<code>HSou</code> is treated differently.
+It is set to a value of the enumeration
+<a href=\"modelica://AixLib.BoundaryConditions.Types.RadiationDataSource\">
+AixLib.BoundaryConditions.Types.RadiationDataSource</a>,
+and allows the following configurations:
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<!-- ============================================== -->
+<tr>
+  <th>Parameter <code>HSou</code>
+  </th>
+  <th>Data used to compute weather data.
+  </th>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    File
+  </td>
+  <td>
+    Use data from file.
+  </td>
+</tr>
+<!-- ============================================== -->
+<tr>
+  <td>
+    Input_HGloHor_HDifHor
+  </td>
+  <td>
+    Use global horizontal and diffuse horizontal radiation from input connector.
+  </td>
+</tr>
+<tr>
+  <td>
+    Input_HDirNor_HDifHor
+  </td>
+  <td>
+    Use direct normal and diffuse horizontal radiation from input connector.
+  </td>
+</tr>
+<tr>
+  <td>
+    Input_HDirNor_HGloHor
+  </td>
+  <td>
+    Use direct normal and global horizontal radiation from input connector.
+  </td>
+</tr>
+</table>
+<!-- ============================================== -->
+<h4>Length of weather data and simulation period</h4>
+<p>
+If weather data span a year, which is the default for TMY3 data, or multiple years,
+then this model can be used for simulations that span multiple years. The simulation
+start time needs to be set to the clock time of the respective start time. For example,
+to start at January 2 at 10am, set start time to <code>t=(24+10)*3600</code> seconds.
+For this computation, the used date and time (here January 2, 10 am) must be expressed in the same time zone
+as the one that is used to define the TMY3 file. This is usually the local (winter) time zone.
+The parameter `timZon` represents the TMY3 file time zone, expressed in seconds compared to UTC.
+</p>
+<p>
+Moreover, weather data need not span a whole year, or it can span across New Year.
+In this case, the simulation cannot exceed the time of the weather data file. Otherwise,
+the simulation stops with an error.
+</p>
+<p>
+As weather data have one entry at the start of the time interval, the end time of the weather
+data file is computed as the last time entry plus the average time increment of the file.
+For example, an hourly weather data file has 8760 entries, starting on January 1 at 0:00.
+The last entry in the file will be for December 31 at 23:00. As the time increment is 1 hour,
+the model assumes the weather file to end at December 31 at 23:00 plus 1 hour, e.g., at January 1 at 0:00.
+</p>
+<!-- ============================================== -->
+<h4>Notes</h4>
+<ol>
+<li>
+<p>
+In HVAC systems, when the fan is off, changes in atmospheric pressure can cause small air flow rates
+in the duct system due to change in pressure and hence in the mass of air that is stored
+in air volumes (such as in fluid junctions or in the room model).
+This may increase computing time. Therefore, the default value for the atmospheric pressure is set to a constant.
+Furthermore, if the initial pressure of air volumes are different
+from the atmospheric pressure, then fast pressure transients can happen in the first few seconds of the simulation.
+This can cause numerical problems for the solver. To avoid this problem, set the atmospheric pressure to the
+same value as the medium default pressure, which is typically set to the parameter <code>Medium.p_default</code>.
+For medium models for moist air and dry air, the default is
+<code>Medium.p_default=101325</code> Pascals.
+</p>
+</li>
+<li>
+<p>
+Different units apply depending on whether data are obtained from a file, or
+from a parameter or an input connector:
+</p>
+<ul>
+<li>
+When using TMY3 data from a file (e.g. <code>USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos</code>), the units must be the same as the original TMY3 file used by EnergyPlus (e.g.
+<code>USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.epw</code>).
+The TMY3 data used by EnergyPlus are in both SI units and non-SI units.
+If <code>Resources/bin/ConvertWeatherData.jar</code> is used to convert the <code>.epw</code> file to an <code>.mos</code> file, the units of the TMY3 data are preserved and the file can be directly
+used by this data reader.
+The data reader will automatically convert units to the SI units used by Modelica.
+For example, the dry bulb temperature <code>TDryBul</code> in TMY3 is in degree Celsius.
+The data reader will automatically convert the data to Kelvin.
+The wind direction <code>winDir</code> in TMY3 is degrees and will be automatically converted to radians.
+</li>
+<li>
+When using data from a parameter or from an input connector,
+the data must be in the SI units used by Modelica.
+For instance, the unit must be
+<code>Pa</code> for pressure,
+<code>K</code> for temperature,
+<code>W/m2</code> for solar radiations and
+<code>rad</code> for wind direction.
+</li>
+</ul>
+</li>
+<li>
+<p>
+Hourly and subhourly timestamp are handled in a different way in <code>.epw</code> files.
+From the EnergyPlus Auxiliary Programs Document (v9.3.0, p. 63):
+In hourly data the minute field can be <code>00</code> or <code>60</code>. In this case as mentioned in the previous section, the weather data
+is reported at the hourly value and the minute field has to be ignored, writing <code>1, 60</code> or <code>1, 00</code> is equivalent.
+If the minute field is between <code>00</code> and <code>60</code>, the file becomes subhourly, in this case the timestamp corresponds to the
+minute field in the considered hour. For example: <code>1, 30</code> is equivalent to <i>00:30</i> and <code>3, 45</code> is equivalent to <i>02:45</i>.<br/>
+(Note the offset in the hour digit.)
+</p>
+</li>
+<li>
+The ReaderTMY3 should only be used with TMY3 data. It contains a time shift for solar radiation data
+that is explained below. This time shift needs to be removed if the user may want to
+use the ReaderTMY3 for other weather data types.
+</li>
+</ol>
+<h4>Implementation</h4>
+<h5>Start and end data for annual weather data files</h5>
+<p>
+The TMY3 weather data, as well as the EnergyPlus weather data, start at 1:00 AM
+on January 1, and provide hourly data until midnight on December 31.
+Thus, the first entry for temperatures, humidity, wind speed etc. are values
+at 1:00 AM and not at midnight. Furthermore, the TMY3 weather data files can have
+values at midnight of December 31 that may be significantly different from the values
+at 1:00 AM on January 1.
+Since annual simulations require weather data that start at 0:00 on January 1,
+data need to be provided for this hour. Due to the possibly large change in
+weatherdata between 1:00 AM on January 1 and midnight at December 31,
+the weather data files in the AixLib library do not use the data entry from
+midnight at December 31 as the value for <i>t=0</i>. Rather, the
+value from 1:00 AM on January 1 is duplicated and used for 0:00 on January 1.
+To maintain a data record with <i>8760</i> hours, the weather data record from
+midnight at December 31 is deleted.
+These changes in the weather data file are done in the Java program
+<code>AixLib/Resources/bin/ConvertWeatherData.jar</code> that converts
+EnergyPlus weather data file to Modelica weather data files, and which is described
+above.
+The length of the weather data is calculated as the
+end time stamp minus start time stamp plus average increment, where the
+average increment is equal to the end time stamp minus start time stamp divided
+by the number of rows minus 1.
+This only works correctly for weather files with equidistant time stamps.
+</p>
+<h5>Time shift for solar radiation data</h5>
+<p>
+To read weather data from the TMY3 weather data file, there are
+two data readers in this model. One data reader obtains all data
+except solar radiation, and the other data reader reads only the
+solar radiation data, shifted by <i>30</i> minutes.
+The reason for this time shift is as follows:
+The TMY3 weather data file contains for solar radiation the
+\"...radiation received
+on a horizontal surface during
+the 60-minute period ending at
+the timestamp.\"
+
+Thus, as the figure below shows, a more accurate interpolation is obtained if
+time is shifted by <i>30</i> minutes prior to reading the weather data.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/BoundaryConditions/WeatherData/RadiationTimeShift.png\"
+border=\"1\" />
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Wilcox S. and W. Marion. <i>Users Manual for TMY3 Data Sets</i>.
+Technical Report, NREL/TP-581-43156, revised May 2008.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed alt and lat to real inputs.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+May 2, 2021, by Ettore Zanetti:<br/>
+Added altitude to parameters.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+October 4, 2020, by Ettore Zanetti:<br/>
+Updated documentation for Java weather file generator.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1396\">#1396</a>.
+</li>
+<li>
+August 20, 2019, by Filip Jorissen:<br/>
+Better clarified the meaning of <code>time</code> in the documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1192\">#1192</a>.
+</li>
+<li>
+March 5, 2019, by Michael Wetter:<br/>
+Updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">#842</a>.
+</li>
+<li>
+September 20, 2018, by Michael Wetter:<br/>
+Corrected documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1022\">#1022</a>.
+</li>
+<li>
+December 4, 2017, by Michael Wetter:<br/>
+Removed function call to <code>getAbsolutePath</code>, as this causes in Dymola 2018FD01
+the error
+\"A call of loadResource with a non-literal string remains in the generated code; it will not work for an URI.\"
+when exporting <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone</a>
+as an FMU. Instead, if the weather file is specified as a Modelica, URI, syntax such as
+<code>Modelica.Utilities.Files.loadResource(\"modelica://AixLib/Resources/weatherdata/USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos\")</code>
+should be used.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/867\">#867</a>.
+</li>
+<li>
+February 18, 2017, by Filip Jorissen:<br/>
+Infrared radiation on horizontal surface is now delayed by 30 minutes
+such that the results in
+<a href=\"modelica://AixLib.BoundaryConditions.SkyTemperature.Examples.BlackBody\">TBlaSky</a>
+are consistent.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/648\">#648</a>.
+</li>
+<li>
+December 06, 2016, by Thierry S. Nouidui:<br/>
+Constrained the direct normal radiation to not be bigger than the solar constant when using
+global and diffuse solar radiation data provided via the inputs connectors.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/608\">#608</a>.
+</li>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Introduced <code>absFilNam</code> to avoid multiple calls to
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/506\">Buildings, #506</a>.
+</li>
+<li>
+January 6, 2016, by Moritz Lauster:<br/>
+Changed output <code>radHorIR</code> to <code>HHorIR</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">#376</a>.
+</li>
+<li>
+January 4, 2016, by Moritz Lauster:<br/>
+Added a table in documentation with output variables accessible via <code>weaBus</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/376\">#376</a>.
+</li>
+<li>
+December 15, 2015, by Michael Wetter:<br/>
+Added the block <code>cheTemBlaSky</code>. This also allows to graphically
+connect the black body sky temperature to the weather bus, which is required
+in Dymola 2016 for the variable <code>weaBus.TBlaSky</code> to appear
+in the graphical editor.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/377\">#377</a>.
+</li>
+<li>
+September 24, 2015, by Marcus Fuchs:<br/>
+Replace Dymola specific annotation by <code>loadSelector</code>
+for MSL compliancy as reported by @tbeu at
+<a href=\"https://github.com/RWTH-EBC/AixLib/pull/107\">RWTH-EBC/AixLib#107</a>
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Removed redundant but consistent
+<code>connect(TBlaSkyCom.TBlaSky, weaBus.TBlaSky)</code>
+statement.
+This avoids a warning if
+<a href=\"modelica://AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.SkyClearness\">
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.SkyClearness</a>
+is translated in pedantic mode in Dymola 2016.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+March 26, 2015, by Michael Wetter:<br/>
+Added option to obtain the black body sky temperature
+from a parameter or an input signal.
+</li>
+<li>
+October 17, 2014, by Michael Wetter:<br/>
+Corrected error that led the total and opaque sky cover to be ten times
+too low if its value was obtained from the parameter or the input connector.
+For the standard configuration in which the sky cover is obtained from
+the weather data file, the model was correct. This error only affected
+the other two possible configurations.
+</li>
+<li>
+September 12, 2014, by Michael Wetter:<br/>
+Removed redundant connection <code>connect(conHorRad.HOut, cheHorRad.HIn);</code>.
+</li>
+<li>
+May 30, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+May 5, 2013, by Thierry S. Nouidui:<br/>
+Added the option to use a constant, an input signal or the weather file as the source
+for the ceiling height, the total sky cover, the opaque sky cover, the dew point temperature,
+and the infrared horizontal radiation <code>HInfHor</code>.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Improved the algorithm that determines the absolute path of the file.
+Now weather files are searched in the path specified, and if not found, the urls
+<code>file://</code>, <code>modelica://</code> and <code>modelica://AixLib</code>
+are added in this order to search for the weather file.
+This allows using the data reader without having to specify an absolute path,
+as long as the <code>AixLib</code> library
+is on the <code>MODELICAPATH</code>.
+This change was implemented in
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath\">
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath</a>
+and improves this weather data reader.
+</li>
+<li>
+May 2, 2013, by Michael Wetter:<br/>
+Added function call to <code>getAbsolutePath</code>.
+</li>
+<li>
+October 16, 2012, by Michael Wetter:<br/>
+Added computation of the wet bulb temperature.
+Computing the wet bulb temperature introduces a nonlinear
+equation. As we have not observed an increase in computing time
+because of computing the wet bulb temperature, it is computed
+by default. By setting the parameter
+<code>computeWetBulbTemperature=false</code>, the computation of the
+wet bulb temperature can be removed.
+Revised documentation.
+</li>
+<li>
+August 11, 2012, by Wangda Zuo:<br/>
+Renamed <code>radHor</code> to <code>radHorIR</code> and
+improved the optional inputs for radiation data.
+</li>
+<li>
+July 24, 2012, by Wangda Zuo:<br/>
+Corrected the notes of SI unit requirements for input files.
+</li>
+<li>
+July 13, 2012, by Michael Wetter:<br/>
+Removed assignment of <code>HGloHor_in</code> in its declaration,
+because this gives an overdetermined system if the input connector
+is used.
+Removed non-required assignments of attribute <code>displayUnit</code>.
+</li>
+<li>
+February 25, 2012, by Michael Wetter:<br/>
+Added subbus for solar position, which is needed by irradition and
+shading model.
+</li>
+<li>
+November 29, 2011, by Michael Wetter:<br/>
+Fixed wrong display unit for <code>pAtm_in_internal</code> and
+made propagation of parameter final.
+</li>
+<li>
+October 27, 2011, by Wangda Zuo:<br/>
+<ol>
+<li>
+Added optional connectors for dry bulb temperature, relative humidity, wind speed, wind direction, global horizontal radiation, diffuse horizontal radiation.<br/>
+</li>
+<li>
+Separate the unit conversion for TMY3 data and data validity check.
+</li>
+</ol>
+</li>
+<li>
+October 3, 2011, by Michael Wetter:<br/>
+Propagated value for sky temperature calculation to make it accessible as a parameter.
+</li>
+<li>
+July 20, 2011, by Michael Wetter:<br/>
+Added the option to use a constant, an input signal or the weather file as the source
+for the atmospheric pressure.
+</li><li>
+March 15, 2011, by Wangda Zuo:<br/>
+Delete the wet bulb temperature since it may cause numerical problem.
+</li>
+<li>
+March 7, 2011, by Wangda Zuo:<br/>
+Added wet bulb temperature. Changed reader to read only needed columns.
+Added explanation for 30 minutes shift for radiation data.
+</li>
+<li>
+March 5, 2011, by Michael Wetter:<br/>
+Changed implementation to obtain longitude and time zone directly
+from weather file.
+</li>
+<li>
+June 25, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=false,
-     extent={{-200,-300},{300,300}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+     extent={{-200,-300},{300,300}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReaderTMY3;
diff --git a/AixLib/BoundaryConditions/WeatherData/Validation/DecemberToJanuary.mo b/AixLib/BoundaryConditions/WeatherData/Validation/DecemberToJanuary.mo
index 58fd54c00b..15a5faff4a 100644
--- a/AixLib/BoundaryConditions/WeatherData/Validation/DecemberToJanuary.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Validation/DecemberToJanuary.mo
@@ -21,18 +21,18 @@ model DecemberToJanuary
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/Validation/DecemberToJanuary.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This is a validation case for a data file that has a few incomplete days in December and goes into
- a few days into January. The data does not start and does not end at midnight.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 26, 2017, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a validation case for a data file that has a few incomplete days in December and goes into
+a few days into January. The data does not start and does not end at midnight.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 26, 2017, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DecemberToJanuary;
diff --git a/AixLib/BoundaryConditions/WeatherData/Validation/OverAYear_usingOneYearData.mo b/AixLib/BoundaryConditions/WeatherData/Validation/OverAYear_usingOneYearData.mo
index 38c8941b04..71f26079dc 100644
--- a/AixLib/BoundaryConditions/WeatherData/Validation/OverAYear_usingOneYearData.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Validation/OverAYear_usingOneYearData.mo
@@ -19,19 +19,19 @@ model OverAYear_usingOneYearData
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/Validation/OverAYear_usingOneYearData.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This is a validation case for a simulation extending with two months over one year,
- but using data for only one year.
- </p>
- <p>
- The test script plots the dry bulb temperature for the days 0-10 and 365-375 for comparison.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>September 3, 2018 by Ana Constantin:<br/>
- First implementation for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a validation case for a simulation extending with two months over one year,
+but using data for only one year.
+</p>
+<p>
+The test script plots the dry bulb temperature for the days 0-10 and 365-375 for comparison.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>September 3, 2018 by Ana Constantin:<br/>
+First implementation for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OverAYear_usingOneYearData;
diff --git a/AixLib/BoundaryConditions/WeatherData/Validation/ReaderTMY3HDirNor.mo b/AixLib/BoundaryConditions/WeatherData/Validation/ReaderTMY3HDirNor.mo
index 6ea7ed67cb..beddf4a63d 100644
--- a/AixLib/BoundaryConditions/WeatherData/Validation/ReaderTMY3HDirNor.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Validation/ReaderTMY3HDirNor.mo
@@ -41,19 +41,19 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/Validation/ReaderTMY3HDirNor.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the calculation of the direct normal radiation.
- The instance <code>weaDatInpCon</code> obtains the global horizontal and
- the diffuse horizontal solar radiation from its inputs connectors.
- </p>
- </html>",
+<p>
+This model tests the calculation of the direct normal radiation.
+The instance <code>weaDatInpCon</code> obtains the global horizontal and
+the diffuse horizontal solar radiation from its inputs connectors.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 06, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 06, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReaderTMY3HDirNor;
diff --git a/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearData.mo b/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearData.mo
index 13bde4896d..2b129ebc78 100644
--- a/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearData.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearData.mo
@@ -19,16 +19,16 @@ model ThreeYears_usingTwoYearData
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearData.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This is a validation case for a simulation extending over three years,
- but using only two years of data with equidistant monthly values.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>September 3, 2018 by Ana Constantin:<br/>
- First implementation for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a validation case for a simulation extending over three years,
+but using only two years of data with equidistant monthly values.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>September 3, 2018 by Ana Constantin:<br/>
+First implementation for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeYears_usingTwoYearData;
diff --git a/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataNegativeStart.mo b/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataNegativeStart.mo
index a8374ad0c2..e32fd7f3e5 100644
--- a/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataNegativeStart.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataNegativeStart.mo
@@ -11,17 +11,17 @@ model ThreeYears_usingTwoYearDataNegativeStart
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataNegativeStart.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This is a validation case for a simulation extending over six years
- starting at a negative start date,
- but using only two years of data with equidistant monthly values.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>March 5, 2019 by Michael Wetter:<br/>
- First implementation for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a validation case for a simulation extending over six years
+starting at a negative start date,
+but using only two years of data with equidistant monthly values.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>March 5, 2019 by Michael Wetter:<br/>
+First implementation for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeYears_usingTwoYearDataNegativeStart;
diff --git a/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataPositiveStart.mo b/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataPositiveStart.mo
index ae42e1d370..7a066d71fb 100644
--- a/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataPositiveStart.mo
+++ b/AixLib/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataPositiveStart.mo
@@ -11,17 +11,17 @@ model ThreeYears_usingTwoYearDataPositiveStart
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/BoundaryConditions/WeatherData/Validation/ThreeYears_usingTwoYearDataPositiveStart.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This is a validation case for a simulation extending over six years
- starting at a positive start date,
- but using only two years of data with equidistant monthly values.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>March 5, 2019 by Michael Wetter:<br/>
- First implementation for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a validation case for a simulation extending over six years
+starting at a positive start date,
+but using only two years of data with equidistant monthly values.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>March 5, 2019 by Michael Wetter:<br/>
+First implementation for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/842\">issue 842</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeYears_usingTwoYearDataPositiveStart;
diff --git a/AixLib/Controls/Continuous/Examples/LimPID.mo b/AixLib/Controls/Continuous/Examples/LimPID.mo
index 7ff52cfc7d..06b8dbf4ea 100644
--- a/AixLib/Controls/Continuous/Examples/LimPID.mo
+++ b/AixLib/Controls/Continuous/Examples/LimPID.mo
@@ -80,35 +80,35 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/Continuous/Examples/LimPID.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- April 26, 2016, by Michael Wetter:<br/>
- Relaxed tolerance of assertions from <i>1E-10</i>
- to <i>1E-3</i> as the default relative tolerance in JModelica
- is <i>1E-4</i>.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">
- Buildings, issue 510</a>.
- </li>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model tests the implementation of the
- PID controller with optional reverse action.
- The model <code>limPIDOri</code> is the original
- implementation of the controller from the Modelica
- Standard Library. The models <code>limPID</code>
- and <code>limPIDRev</code> are the implementations
- from the AixLib library. The model
- <code>limPIDRev</code> is parameterized to have
- reverse action.
- The assertion blocks test whether the results
- of all three controllers are identical.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 26, 2016, by Michael Wetter:<br/>
+Relaxed tolerance of assertions from <i>1E-10</i>
+to <i>1E-3</i> as the default relative tolerance in JModelica
+is <i>1E-4</i>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">
+Buildings, issue 510</a>.
+</li>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model tests the implementation of the
+PID controller with optional reverse action.
+The model <code>limPIDOri</code> is the original
+implementation of the controller from the Modelica
+Standard Library. The models <code>limPID</code>
+and <code>limPIDRev</code> are the implementations
+from the AixLib library. The model
+<code>limPIDRev</code> is parameterized to have
+reverse action.
+The assertion blocks test whether the results
+of all three controllers are identical.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimPID;
diff --git a/AixLib/Controls/Continuous/Examples/LimPIDWithReset.mo b/AixLib/Controls/Continuous/Examples/LimPIDWithReset.mo
index 0ca80f4385..9d01897de7 100644
--- a/AixLib/Controls/Continuous/Examples/LimPIDWithReset.mo
+++ b/AixLib/Controls/Continuous/Examples/LimPIDWithReset.mo
@@ -80,26 +80,26 @@ protected
     connect(preHea.port, cap.port)
       annotation (Line(points={{-58,0},{-28,0}}, color={191,0,0}));
     annotation (Documentation(info="<html>
- <p>
- Plant model for
- <a href=\"modelica://AixLib.Controls.Continuous.Examples.LimPIDWithReset\">
- AixLib.Controls.Continuous.Examples.LimPIDWithReset</a>.
- consisting of a simple heat transfer model.
- </p>
- <h4>Implementation</h4>
- <p>
- To compare the effect of the controller output reset, the plant and control
- models have been implemented in separate blocks so they can be instantiated
- twice in the system model with the appropriate control settings.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- October 3, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Plant model for
+<a href=\"modelica://AixLib.Controls.Continuous.Examples.LimPIDWithReset\">
+AixLib.Controls.Continuous.Examples.LimPIDWithReset</a>.
+consisting of a simple heat transfer model.
+</p>
+<h4>Implementation</h4>
+<p>
+To compare the effect of the controller output reset, the plant and control
+models have been implemented in separate blocks so they can be instantiated
+twice in the system model with the appropriate control settings.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+October 3, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end Plant;
 
   model Controller "PID controller with optional output reset"
@@ -155,34 +155,34 @@ protected
     connect(gain.y, y)
       annotation (Line(points={{51,0},{100,0},{110,0}}, color={0,0,127}));
     annotation (Documentation(info="<html>
- <p>
- Controller model for
- <a href=\"modelica://AixLib.Controls.Continuous.Examples.LimPIDWithReset\">
- AixLib.Controls.Continuous.Examples.LimPIDWithReset</a>.
- </p>
- <p>
- The controller is reset whenever the input signal becomes bigger than
- <i>30</i>&deg;C.
- </p>
- <h4>Implementation</h4>
- <p>
- To compare the effect of the controller output reset, the plant and control
- models have been implemented in separate blocks so they can be instantiated
- twice in the system model with the appropriate control settings.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- October 10, 2016, by Michael Wetter:<br/>
- Added full path in the type declaration.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/540\">issue 540</a>.
- </li>
- <li>
- October 3, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Controller model for
+<a href=\"modelica://AixLib.Controls.Continuous.Examples.LimPIDWithReset\">
+AixLib.Controls.Continuous.Examples.LimPIDWithReset</a>.
+</p>
+<p>
+The controller is reset whenever the input signal becomes bigger than
+<i>30</i>&deg;C.
+</p>
+<h4>Implementation</h4>
+<p>
+To compare the effect of the controller output reset, the plant and control
+models have been implemented in separate blocks so they can be instantiated
+twice in the system model with the appropriate control settings.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+October 10, 2016, by Michael Wetter:<br/>
+Added full path in the type declaration.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/540\">issue 540</a>.
+</li>
+<li>
+October 3, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end Controller;
 
 equation
@@ -205,23 +205,23 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/Cont
         "Simulate and plot"),
     Documentation(
 info="<html>
- <p>
- Example that demonstrates the effect
- of the integrator reset.
- The top model has the reset of the controller output enabled.
- By plotting the controller error, one sees that the integrator reset
- improves the closed loop performance slightly.
- Note, however, that both controllers have an integrator anti-windup
- and hence the integrator reset has limited benefits.
- </p>
- </html>",
+<p>
+Example that demonstrates the effect
+of the integrator reset.
+The top model has the reset of the controller output enabled.
+By plotting the controller error, one sees that the integrator reset
+improves the closed loop performance slightly.
+Note, however, that both controllers have an integrator anti-windup
+and hence the integrator reset has limited benefits.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 29, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 29, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimPIDWithReset;
diff --git a/AixLib/Controls/Continuous/Examples/NumberOfRequests.mo b/AixLib/Controls/Continuous/Examples/NumberOfRequests.mo
index 7b1e20f322..73369e7ef2 100644
--- a/AixLib/Controls/Continuous/Examples/NumberOfRequests.mo
+++ b/AixLib/Controls/Continuous/Examples/NumberOfRequests.mo
@@ -8,7 +8,10 @@ model NumberOfRequests
     kind=0) annotation (Placement(transformation(extent={{0,20},{20,40}})));
   Modelica.Blocks.Sources.Sine sine(f=2)
     annotation (Placement(transformation(extent={{-60,-20},{-40,0}})));
-  Modelica.Blocks.Sources.Pulse pulse(period=0.35)
+  Modelica.Blocks.Sources.Pulse pulse(
+    amplitude=1-pulse.offset,
+    period=0.35,
+    offset=-0.01)
     annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
 equation
   connect(sine.y, numReq.u[1]) annotation (Line(points={{-39,-10},{-19.5,-10},{
@@ -19,30 +22,36 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/Continuous/Examples/NumberOfRequests.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- January 12, 2017, by Thierry S. Nouidui:<br/>
- Modified example to prevent simultaneous events
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/646\">#646</a>.
- </li>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example that demonstrates the use of the block
- <a href=\"modelica://AixLib.Controls.Continuous.NumberOfRequests\">
- AixLib.Controls.Continuous.NumberOfRequests</a>.
- The parameters of the block are such that the output is incremented
- for each input signal that is strictly larger than <i>0</i>.
- The figure below shows the inputs and the output of the block.
- </p>
- <p align=\"center\">
- <img alt=\"Simulation results\" src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/NumberOfRequests.png\" border=\"1\" />
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 16, 2024, by Hongxiang Fu:<br/>
+Changed pulse input from 0 to 1 to 0.01 to 1.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1897\">#1897</a>.
+</li>
+<li>
+January 12, 2017, by Thierry S. Nouidui:<br/>
+Modified example to prevent simultaneous events
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/646\">#646</a>.
+</li>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example that demonstrates the use of the block
+<a href=\"modelica://AixLib.Controls.Continuous.NumberOfRequests\">
+AixLib.Controls.Continuous.NumberOfRequests</a>.
+The parameters of the block are such that the output is incremented
+for each input signal that is strictly larger than <i>0</i>.
+The figure below shows the inputs and the output of the block.
+</p>
+<p align=\"center\">
+<img alt=\"Simulation results\" src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/NumberOfRequests.png\" border=\"1\" />
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end NumberOfRequests;
diff --git a/AixLib/Controls/Continuous/Examples/OffTimer.mo b/AixLib/Controls/Continuous/Examples/OffTimer.mo
index 87df209fd6..4428c98a2c 100644
--- a/AixLib/Controls/Continuous/Examples/OffTimer.mo
+++ b/AixLib/Controls/Continuous/Examples/OffTimer.mo
@@ -26,26 +26,26 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/Cont
         "Simulate and plot"),
     Documentation(
 info="<html>
- <p>
- Example that demonstrates the use of the model
- <a href=\"modelica://AixLib.Controls.Continuous.OffTimer\">
- AixLib.Controls.Continuous.OffTimer</a>.
- The input to the two timers are alternating boolean values.
- Whenever the input becomes <code>false(=0)</code>, the timer is reset.
- The figures below show the input and output of the blocks.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/OffTimer1.png\" border=\"1\" alt=\"Input and output of the OffTimer offTim1.\"/><br/>
- <img src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/OffTimer2.png\" border=\"1\" alt=\"Input and output of the OffTimer offTim1.\"/>
- </p>
- </html>",
+<p>
+Example that demonstrates the use of the model
+<a href=\"modelica://AixLib.Controls.Continuous.OffTimer\">
+AixLib.Controls.Continuous.OffTimer</a>.
+The input to the two timers are alternating boolean values.
+Whenever the input becomes <code>false(=0)</code>, the timer is reset.
+The figures below show the input and output of the blocks.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/OffTimer1.png\" border=\"1\" alt=\"Input and output of the OffTimer offTim1.\"/><br/>
+<img src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/OffTimer2.png\" border=\"1\" alt=\"Input and output of the OffTimer offTim1.\"/>
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OffTimer;
diff --git a/AixLib/Controls/Continuous/Examples/SignalRanker.mo b/AixLib/Controls/Continuous/Examples/SignalRanker.mo
index a3fc432561..7ca6060c92 100644
--- a/AixLib/Controls/Continuous/Examples/SignalRanker.mo
+++ b/AixLib/Controls/Continuous/Examples/SignalRanker.mo
@@ -24,29 +24,29 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/Continuous/Examples/SignalRanker.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example that demonstrates the use of the signal ranker model.
- The figure below shows the input and output signals of the block.
- Note that
- <code>sigRan.y[1] &ge; sigRan.y[2] &ge; sigRan.y[3]</code>.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/SignalRankerU.png\" border=\"1\" alt=\"Input to signal ranker.\"/><br/>
- <img src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/SignalRankerY.png\" border=\"1\" alt=\"Output of signal ranker.\"/>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 15, 2021, by Michael Wetter:<br/>
- Moved start time of sine input signal to avoid simultaneous state event and time event.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1534\">IBPSA, #1534</a>.
- </li>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example that demonstrates the use of the signal ranker model.
+The figure below shows the input and output signals of the block.
+Note that
+<code>sigRan.y[1] &ge; sigRan.y[2] &ge; sigRan.y[3]</code>.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/SignalRankerU.png\" border=\"1\" alt=\"Input to signal ranker.\"/><br/>
+<img src=\"modelica://AixLib/Resources/Images/Controls/Continuous/Examples/SignalRankerY.png\" border=\"1\" alt=\"Output of signal ranker.\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 15, 2021, by Michael Wetter:<br/>
+Moved start time of sine input signal to avoid simultaneous state event and time event.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1534\">IBPSA, #1534</a>.
+</li>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SignalRanker;
diff --git a/AixLib/Controls/Continuous/LimPID.mo b/AixLib/Controls/Continuous/LimPID.mo
index 0c112fd3f2..291f8a7ee9 100644
--- a/AixLib/Controls/Continuous/LimPID.mo
+++ b/AixLib/Controls/Continuous/LimPID.mo
@@ -89,6 +89,7 @@ block LimPID
     annotation (Placement(transformation(extent={{-40,40},{-20,60}})));
   Utilities.Math.IntegratorWithReset I(
     final reset=if reset == AixLib.Types.Reset.Disabled then reset else AixLib.Types.Reset.Input,
+
     final y_reset=y_reset,
     final k=unitTime/Ti,
     final y_start=xi_start,
@@ -344,148 +345,148 @@ equation
    annotation (
 defaultComponentName="conPID",
 Documentation(info="<html>
- <p>
- PID controller in the standard form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- y = k &nbsp; ( e(t) + 1 &frasl; T<sub>i</sub> &nbsp; &int; e(s) ds + T<sub>d</sub> de(t)&frasl;dt ),
- </p>
- <p>
- where
- <i>y</i> is the control signal,
- <i>e(t) = u<sub>s</sub> - u<sub>m</sub></i> is the control error,
- with <i>u<sub>s</sub></i> being the set point and <i>u<sub>m</sub></i> being
- the measured quantity,
- <i>k</i> is the gain,
- <i>T<sub>i</sub></i> is the time constant of the integral term and
- <i>T<sub>d</sub></i> is the time constant of the derivative term.
- </p>
- <p>
- Note that the units of <i>k</i> are the inverse of the units of the control error,
- while the units of <i>T<sub>i</sub></i> and <i>T<sub>d</sub></i> are seconds.
- </p>
- <p>
- For detailed treatment of integrator anti-windup, set-point weights and output limitation, see
- <a href=\"modelica://Modelica.Blocks.Continuous.LimPID\">Modelica.Blocks.Continuous.LimPID</a>.
- </p>
- <h4>Options</h4>
- This controller can be configured as follows.
- <h5>P, PI, PD, or PID action</h5>
- <p>
- Through the parameter <code>controllerType</code>, the controller can be configured
- as P, PI, PD or PID controller. The default configuration is PI.
- </p>
- <h5>Direct or reverse acting</h5>
- <p>
- Through the parameter <code>reverseActing</code>, the controller can be configured to
- be reverse or direct acting.
- The above standard form is reverse acting, which is the default configuration.
- For a reverse acting controller, for a constant set point,
- an increase in measurement signal <code>u_m</code> decreases the control output signal <code>y</code>
- (Montgomery and McDowall, 2008).
- Thus,
- </p>
- <ul>
-   <li>
-   for a heating coil with a two-way valve, leave <code>reverseActing = true</code>, but
-   </li>
-   <li>
-   for a cooling coil with a two-way valve, set <code>reverseActing = false</code>.
-   </li>
- </ul>
- <h5>Reset of the controller output</h5>
- <p>
- The controller can be configured to enable an input port that allows resetting the controller
- output. The controller output can be reset as follows:
- </p>
- <ul>
-   <li>
-   If <code>reset = AixLib.Types.Reset.Disabled</code>, which is the default,
-   then the controller output is never reset.
-   </li>
-   <li>
-   If <code>reset = AixLib.Types.Reset.Parameter</code>, then a boolean
-   input signal <code>trigger</code> is enabled. Whenever the value of
-   this input changes from <code>false</code> to <code>true</code>,
-   the controller output is reset by setting <code>y</code>
-   to the value of the parameter <code>y_reset</code>.
-   </li>
-   <li>
-   If <code>reset = AixLib.Types.Reset.Input</code>, then a boolean
-   input signal <code>trigger</code> and a real input signal <code>y_reset_in</code>
-   are enabled. Whenever the value of
-   <code>trigger</code> changes from <code>false</code> to <code>true</code>,
-   the controller output is reset by setting the value of <code>y</code>
-   to <code>y_reset_in</code>.
-   </li>
- </ul>
- <p>
- Note that this controller implements an integrator anti-windup. Therefore,
- for most applications, keeping the default setting of
- <code>reset = AixLib.Types.Reset.Disabled</code> is sufficient.
- However, if the controller is used in conjuction with equipment that is being
- switched on, better control performance may be achieved by resetting the controller
- output when the equipment is switched on.
- This is in particular the case in situations
- where the equipment control input should continuously increase as the equipment is
- switched on, such as a light dimmer that may slowly increase the luminance, or
- a variable speed drive of a motor that should continuously increase the speed.
- </p>
- <h4>References</h4>
- <p>
- R. Montgomery and R. McDowall (2008).
- \"Fundamentals of HVAC Control Systems.\"
- American Society of Heating Refrigerating and Air-Conditioning Engineers Inc. Atlanta, GA.
- </p>
- 
- </html>",
+<p>
+PID controller in the standard form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+y = k &nbsp; ( e(t) + 1 &frasl; T<sub>i</sub> &nbsp; &int; e(s) ds + T<sub>d</sub> de(t)&frasl;dt ),
+</p>
+<p>
+where
+<i>y</i> is the control signal,
+<i>e(t) = u<sub>s</sub> - u<sub>m</sub></i> is the control error,
+with <i>u<sub>s</sub></i> being the set point and <i>u<sub>m</sub></i> being
+the measured quantity,
+<i>k</i> is the gain,
+<i>T<sub>i</sub></i> is the time constant of the integral term and
+<i>T<sub>d</sub></i> is the time constant of the derivative term.
+</p>
+<p>
+Note that the units of <i>k</i> are the inverse of the units of the control error,
+while the units of <i>T<sub>i</sub></i> and <i>T<sub>d</sub></i> are seconds.
+</p>
+<p>
+For detailed treatment of integrator anti-windup, set-point weights and output limitation, see
+<a href=\"modelica://Modelica.Blocks.Continuous.LimPID\">Modelica.Blocks.Continuous.LimPID</a>.
+</p>
+<h4>Options</h4>
+This controller can be configured as follows.
+<h5>P, PI, PD, or PID action</h5>
+<p>
+Through the parameter <code>controllerType</code>, the controller can be configured
+as P, PI, PD or PID controller. The default configuration is PI.
+</p>
+<h5>Direct or reverse acting</h5>
+<p>
+Through the parameter <code>reverseActing</code>, the controller can be configured to
+be reverse or direct acting.
+The above standard form is reverse acting, which is the default configuration.
+For a reverse acting controller, for a constant set point,
+an increase in measurement signal <code>u_m</code> decreases the control output signal <code>y</code>
+(Montgomery and McDowall, 2008).
+Thus,
+</p>
+<ul>
+  <li>
+  for a heating coil with a two-way valve, leave <code>reverseActing = true</code>, but
+  </li>
+  <li>
+  for a cooling coil with a two-way valve, set <code>reverseActing = false</code>.
+  </li>
+</ul>
+<h5>Reset of the controller output</h5>
+<p>
+The controller can be configured to enable an input port that allows resetting the controller
+output. The controller output can be reset as follows:
+</p>
+<ul>
+  <li>
+  If <code>reset = AixLib.Types.Reset.Disabled</code>, which is the default,
+  then the controller output is never reset.
+  </li>
+  <li>
+  If <code>reset = AixLib.Types.Reset.Parameter</code>, then a boolean
+  input signal <code>trigger</code> is enabled. Whenever the value of
+  this input changes from <code>false</code> to <code>true</code>,
+  the controller output is reset by setting <code>y</code>
+  to the value of the parameter <code>y_reset</code>.
+  </li>
+  <li>
+  If <code>reset = AixLib.Types.Reset.Input</code>, then a boolean
+  input signal <code>trigger</code> and a real input signal <code>y_reset_in</code>
+  are enabled. Whenever the value of
+  <code>trigger</code> changes from <code>false</code> to <code>true</code>,
+  the controller output is reset by setting the value of <code>y</code>
+  to <code>y_reset_in</code>.
+  </li>
+</ul>
+<p>
+Note that this controller implements an integrator anti-windup. Therefore,
+for most applications, keeping the default setting of
+<code>reset = AixLib.Types.Reset.Disabled</code> is sufficient.
+However, if the controller is used in conjuction with equipment that is being
+switched on, better control performance may be achieved by resetting the controller
+output when the equipment is switched on.
+This is in particular the case in situations
+where the equipment control input should continuously increase as the equipment is
+switched on, such as a light dimmer that may slowly increase the luminance, or
+a variable speed drive of a motor that should continuously increase the speed.
+</p>
+<h4>References</h4>
+<p>
+R. Montgomery and R. McDowall (2008).
+\"Fundamentals of HVAC Control Systems.\"
+American Society of Heating Refrigerating and Air-Conditioning Engineers Inc. Atlanta, GA.
+</p>
+
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 1, 2020, by Michael Wetter:<br/>
- Corrected wrong convention of reverse and direct action.<br/>
- Changed default configuration from PID to PI.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1365\">issue 1365</a>.
- </li>
- <li>
- March 9, 2020, by Michael Wetter:<br/>
- Corrected wrong unit declaration for parameter <code>k</code>.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1316\">issue 1316</a>.
- </li>
- <li>
- October 19, 2019, by Filip Jorissen:<br/>
- Disabled homotopy to ensure bounded outputs
- by copying the implementation from MSL 3.2.3 and by
- hardcoding the implementation for <code>homotopyType=NoHomotopy</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1221\">issue 1221</a>.
- </li>
- <li>
- September 29, 2016, by Michael Wetter:<br/>
- Refactored model.
- </li>
- <li>
- August 25, 2016, by Michael Wetter:<br/>
- Removed parameter <code>limitsAtInit</code> because it was only propagated to
- the instance <code>limiter</code>, but this block no longer makes use of this parameter.
- This is a non-backward compatible change.<br/>
- Revised implemenentation, added comments, made some parameter in the instances final.
- </li>
- <li>July 18, 2016, by Philipp Mehrfeld:<br/>
- Added integrator reset.
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/494\">issue 494</a>.
- </li>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Changed the default value to <code>strict=true</code> in order to avoid events
- when the controller saturates.
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/433\">issue 433</a>.
- </li>
- <li>
- February 24, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<ul>
+<li>
+June 1, 2020, by Michael Wetter:<br/>
+Corrected wrong convention of reverse and direct action.<br/>
+Changed default configuration from PID to PI.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1365\">issue 1365</a>.
+</li>
+<li>
+March 9, 2020, by Michael Wetter:<br/>
+Corrected wrong unit declaration for parameter <code>k</code>.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1316\">issue 1316</a>.
+</li>
+<li>
+October 19, 2019, by Filip Jorissen:<br/>
+Disabled homotopy to ensure bounded outputs
+by copying the implementation from MSL 3.2.3 and by
+hardcoding the implementation for <code>homotopyType=NoHomotopy</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1221\">issue 1221</a>.
+</li>
+<li>
+September 29, 2016, by Michael Wetter:<br/>
+Refactored model.
+</li>
+<li>
+August 25, 2016, by Michael Wetter:<br/>
+Removed parameter <code>limitsAtInit</code> because it was only propagated to
+the instance <code>limiter</code>, but this block no longer makes use of this parameter.
+This is a non-backward compatible change.<br/>
+Revised implemenentation, added comments, made some parameter in the instances final.
+</li>
+<li>July 18, 2016, by Philipp Mehrfeld:<br/>
+Added integrator reset.
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/494\">issue 494</a>.
+</li>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Changed the default value to <code>strict=true</code> in order to avoid events
+when the controller saturates.
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/433\">issue 433</a>.
+</li>
+<li>
+February 24, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Rectangle(
           extent={{-6,-20},{66,-66}},
           lineColor={255,255,255},
@@ -536,6 +537,6 @@ revisions="<html>
           visible=strict,
           points={{30,60},{81,60}},
           color={255,0,0},
-          smooth=Smooth.None)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          smooth=Smooth.None)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimPID;
diff --git a/AixLib/Controls/Continuous/NumberOfRequests.mo b/AixLib/Controls/Continuous/NumberOfRequests.mo
index 141eb9b7c2..07481d0fe9 100644
--- a/AixLib/Controls/Continuous/NumberOfRequests.mo
+++ b/AixLib/Controls/Continuous/NumberOfRequests.mo
@@ -39,50 +39,50 @@ algorithm
   annotation (
 defaultComponentName="numReq",
 Documentation(info="<html>
- <p>
- Block that outputs the number of inputs that exceed a threshold.
- The parameter <code>kind</code> is used to determine the kind of the
- inequality. The table below shows the allowed settings.
- </p>
- <table border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\" summary=\"Allowed parameter settings.\">
- <tr>
- <th>Value of parameter <code>kind</code></th>
- <th>Output signal incremented by 1 for each <i>i &isin; {1, ..., nin}</i> if</th>
- </tr>
- <tr>
- <td>0</td>
- <td><code>u[i] &gt; threShold</code></td>
- </tr>
- <tr>
- <td>1</td>
- <td><code>u[i] &ge; threShold</code></td>
- </tr>
- <tr>
- <td>2</td>
- <td><code>u[i] &le; threShold</code></td>
- </tr>
- <tr>
- <td>3</td>
- <td><code>u[i] &lt; threShold</code></td>
- </tr>
- </table>
- <p>
- This model may be used to check how many rooms
- exceed a temperature threshold.
- </p>
- </html>",
+<p>
+Block that outputs the number of inputs that exceed a threshold.
+The parameter <code>kind</code> is used to determine the kind of the
+inequality. The table below shows the allowed settings.
+</p>
+<table border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\" summary=\"Allowed parameter settings.\">
+<tr>
+<th>Value of parameter <code>kind</code></th>
+<th>Output signal incremented by 1 for each <i>i &isin; {1, ..., nin}</i> if</th>
+</tr>
+<tr>
+<td>0</td>
+<td><code>u[i] &gt; threShold</code></td>
+</tr>
+<tr>
+<td>1</td>
+<td><code>u[i] &ge; threShold</code></td>
+</tr>
+<tr>
+<td>2</td>
+<td><code>u[i] &le; threShold</code></td>
+</tr>
+<tr>
+<td>3</td>
+<td><code>u[i] &lt; threShold</code></td>
+</tr>
+</table>
+<p>
+This model may be used to check how many rooms
+exceed a temperature threshold.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Improved documentation.
- </li>
- <li>
- November 25, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<ul>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Improved documentation.
+</li>
+<li>
+November 25, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Text(
           extent={{-128,88},{-6,28}},
           textColor={0,0,255},
@@ -96,6 +96,6 @@ revisions="<html>
         Line(points={{-18,24},{66,54}}, color={255,0,0}),
         Line(points={{-78,-50},{78,-50}}),
         Line(points={{70,-46},{78,-50}}),
-        Line(points={{70,-54},{78,-50}})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        Line(points={{70,-54},{78,-50}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end NumberOfRequests;
diff --git a/AixLib/Controls/Continuous/OffTimer.mo b/AixLib/Controls/Continuous/OffTimer.mo
index aa76a97ad6..ff12661637 100644
--- a/AixLib/Controls/Continuous/OffTimer.mo
+++ b/AixLib/Controls/Continuous/OffTimer.mo
@@ -37,33 +37,33 @@ equation
               {40,-78},{68,-78}}, color={255,0,255})}),
 defaultComponentName="offTim",
     Documentation(info="<html>
- <p>
- Timer that starts at the initial time with a value of <i>0</i>,
- and gets reset each time the input signal switches to <code>false</code>.
- </p>
- <p>
- For example, if the simulation starts at <i>t = 10</i> and at <i>t=11</i>,
- the input becomes <code>false</code>, then the timer outputs
- <i>y=t-10</i> for <i>t &lt; 11</i>, and <i>y=t-11</i> afterwards, unless
- the input becomes false again.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 12, 2017, by Michael Wetter:<br/>
- Corrected implementation for non-zero start time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/780\">issue 780</a>.
- </li>
- <li>
- January 4, 2011, by Wangda Zuo and Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- February 12, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Timer that starts at the initial time with a value of <i>0</i>,
+and gets reset each time the input signal switches to <code>false</code>.
+</p>
+<p>
+For example, if the simulation starts at <i>t = 10</i> and at <i>t=11</i>,
+the input becomes <code>false</code>, then the timer outputs
+<i>y=t-10</i> for <i>t &lt; 11</i>, and <i>y=t-11</i> afterwards, unless
+the input becomes false again.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 12, 2017, by Michael Wetter:<br/>
+Corrected implementation for non-zero start time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/780\">issue 780</a>.
+</li>
+<li>
+January 4, 2011, by Wangda Zuo and Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+February 12, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OffTimer;
diff --git a/AixLib/Controls/Continuous/SignalRanker.mo b/AixLib/Controls/Continuous/SignalRanker.mo
index 1628399877..ce0523b9be 100644
--- a/AixLib/Controls/Continuous/SignalRanker.mo
+++ b/AixLib/Controls/Continuous/SignalRanker.mo
@@ -6,36 +6,36 @@ equation
   annotation (
 defaultComponentName="sigRan",
 Documentation(info="<html>
- <p>
- Block that sorts the input signal <code>u[:]</code> such that the output
- signal satisfies <code>y[i] &gt;= y[i+1]</code> for all <code>i=1, ..., nin-1</code>.
- </p>
- <p>
- This block may for example be used in a variable air volume flow
- controller to access the position of the dampers that are most open.
- </p>
- </html>",
+<p>
+Block that sorts the input signal <code>u[:]</code> such that the output
+signal satisfies <code>y[i] &gt;= y[i+1]</code> for all <code>i=1, ..., nin-1</code>.
+</p>
+<p>
+This block may for example be used in a variable air volume flow
+controller to access the position of the dampers that are most open.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 15, 2021, by Michael Wetter:<br/>
- Changed implementation to use sort function from Modelica Standard Library.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1534\">IBPSA, #1534</a>.
- </li>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Removed <code>assert</code> statement.
- </li>
- <li>
- November 25, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+October 15, 2021, by Michael Wetter:<br/>
+Changed implementation to use sort function from Modelica Standard Library.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1534\">IBPSA, #1534</a>.
+</li>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Removed <code>assert</code> statement.
+</li>
+<li>
+November 25, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 Icon(graphics={Text(
           extent={{-94,34},{96,-164}},
           textColor={0,0,255},
-          textString="y[i] >= y[i+1]")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="y[i] >= y[i+1]")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SignalRanker;
diff --git a/AixLib/Controls/Continuous/Validation/LimPIDReset.mo b/AixLib/Controls/Continuous/Validation/LimPIDReset.mo
index 97407eb96f..f7fd056fa3 100644
--- a/AixLib/Controls/Continuous/Validation/LimPIDReset.mo
+++ b/AixLib/Controls/Continuous/Validation/LimPIDReset.mo
@@ -94,32 +94,32 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/Continuous/Validation/LimPIDReset.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- September 29, 2016, by Michael Wetter:<br/>
- Revised example to increase code coverage.
- </li>
- <li>
- August 25, 2016, by Michael Wetter:<br/>
- Revised documentation and added script for regression test.
- </li>
- <li>
- August 02, 2016, by Philipp Mehrfeld:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>This model tests the implementation the
- <a href=\"Modelica://AixLib.Controls.Continuous.LimPID\">AixLib.Controls.Continuous.LimPID</a>
- with integrator reset.
- </p>
- <p>
- The instance <code>limPIOri</code> is the original implementation of the controller
- from the Modelica Standard Library.
- The instance <code>limPIWithReset</code> is the implementation from this library
- with integrator reset enabled. Whenever the boolean pulse input becomes true,
- the integrator is reset to <code>y_reset</code>.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 29, 2016, by Michael Wetter:<br/>
+Revised example to increase code coverage.
+</li>
+<li>
+August 25, 2016, by Michael Wetter:<br/>
+Revised documentation and added script for regression test.
+</li>
+<li>
+August 02, 2016, by Philipp Mehrfeld:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>This model tests the implementation the
+<a href=\"Modelica://AixLib.Controls.Continuous.LimPID\">AixLib.Controls.Continuous.LimPID</a>
+with integrator reset.
+</p>
+<p>
+The instance <code>limPIOri</code> is the original implementation of the controller
+from the Modelica Standard Library.
+The instance <code>limPIWithReset</code> is the implementation from this library
+with integrator reset enabled. Whenever the boolean pulse input becomes true,
+the integrator is reset to <code>y_reset</code>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LimPIDReset;
diff --git a/AixLib/Controls/Continuous/Validation/OffTimerNonZeroStart.mo b/AixLib/Controls/Continuous/Validation/OffTimerNonZeroStart.mo
index a5fe0f1723..7fc4bd1e8c 100644
--- a/AixLib/Controls/Continuous/Validation/OffTimerNonZeroStart.mo
+++ b/AixLib/Controls/Continuous/Validation/OffTimerNonZeroStart.mo
@@ -8,17 +8,17 @@ model OffTimerNonZeroStart
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/Continuous/Validation/OffTimerNonZeroStart.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- May 12, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>This model tests the implementation the
- <a href=\"Modelica://AixLib.Controls.Continuous.OffTimer\">AixLib.Controls.Continuous.OffTimer</a>
- for negative start time.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 12, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>This model tests the implementation the
+<a href=\"Modelica://AixLib.Controls.Continuous.OffTimer\">AixLib.Controls.Continuous.OffTimer</a>
+for negative start time.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OffTimerNonZeroStart;
diff --git a/AixLib/Controls/Discrete/BooleanDelay.mo b/AixLib/Controls/Discrete/BooleanDelay.mo
index 5366c80321..b6bada8dc5 100644
--- a/AixLib/Controls/Discrete/BooleanDelay.mo
+++ b/AixLib/Controls/Discrete/BooleanDelay.mo
@@ -21,40 +21,40 @@ algorithm
 defaultComponentName="del",
 Documentation(
 info="<html>
- <p>
- Block that delays the boolean input signal by
- one sampling interval.
- For example,
- if <i>u</i> denotes the input,
- <i>y</i> denotes the output, and
- <i>t<sub>i</sub></i> and <i>t<sub>i+1</sub></i>
- denote subsequent sampling
- instants, then the model outputs
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- y(t<sub>i+1</sub>) = u(t<sub>i</sub>).
- </p>
- </html>",
+<p>
+Block that delays the boolean input signal by
+one sampling interval.
+For example,
+if <i>u</i> denotes the input,
+<i>y</i> denotes the output, and
+<i>t<sub>i</sub></i> and <i>t<sub>i+1</sub></i>
+denote subsequent sampling
+instants, then the model outputs
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+y(t<sub>i+1</sub>) = u(t<sub>i</sub>).
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Set start value and <code>fixed</code> attribute
- for <code>firstTrigger</code>
- to avoid a translation warning in pedantic mode
- in Dymola 2016.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Improved documentation.
- </li>
- <li>
- November 26, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Set start value and <code>fixed</code> attribute
+for <code>firstTrigger</code>
+to avoid a translation warning in pedantic mode
+in Dymola 2016.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Improved documentation.
+</li>
+<li>
+November 26, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BooleanDelay;
diff --git a/AixLib/Controls/Discrete/Examples/BooleanDelay.mo b/AixLib/Controls/Discrete/Examples/BooleanDelay.mo
index 696c068a80..5c1a863873 100644
--- a/AixLib/Controls/Discrete/Examples/BooleanDelay.mo
+++ b/AixLib/Controls/Discrete/Examples/BooleanDelay.mo
@@ -17,23 +17,23 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/Discrete/Examples/BooleanDelay.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example that demonstrates the use of the boolean delay block.
- The output signal of the block is delayed by one sampling interval.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 3, 2017, by Michael Wetter:<br/>
- Changed sampling interval to avoid simultaneous events.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/641\">#641</a>.
- </li>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example that demonstrates the use of the boolean delay block.
+The output signal of the block is delayed by one sampling interval.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 3, 2017, by Michael Wetter:<br/>
+Changed sampling interval to avoid simultaneous events.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/641\">#641</a>.
+</li>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BooleanDelay;
diff --git a/AixLib/Controls/HVACAgentBasedControl/Examples/BuildingHeatingSystems/BuildingHeating.mo b/AixLib/Controls/HVACAgentBasedControl/Examples/BuildingHeatingSystems/BuildingHeating.mo
index dc9516b6ed..7bac400f4b 100644
--- a/AixLib/Controls/HVACAgentBasedControl/Examples/BuildingHeatingSystems/BuildingHeating.mo
+++ b/AixLib/Controls/HVACAgentBasedControl/Examples/BuildingHeatingSystems/BuildingHeating.mo
@@ -4,15 +4,14 @@ model BuildingHeating
   parameter AixLib.DataBase.Weather.TRYWeatherBaseDataDefinition weatherDataDay = AixLib.DataBase.Weather.TRYWinterDay();
 
   ThermalZones.ReducedOrder.ThermalZone.ThermalZone
-              thermalZone(zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler(),
-                                                                 redeclare
-      package Medium = Modelica.Media.Air.SimpleAir)                                                annotation(Placement(transformation(extent={{-60,58},
+    thermalZone(
+      redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam,
+      redeclare package Medium = Modelica.Media.Air.SimpleAir)                                                annotation(Placement(transformation(extent={{-60,58},
             {-34,84}})));
   ThermalZones.ReducedOrder.ThermalZone.ThermalZone
               thermalZone1(redeclare package Medium =
-        Modelica.Media.Air.SimpleAir, zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler())                      annotation(Placement(transformation(extent={{22,58},
+        Modelica.Media.Air.SimpleAir, 
+    redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam)                      annotation(Placement(transformation(extent={{22,58},
             {48,84}})));
   AixLib.Fluid.Movers.FlowControlled_m_flow fan(redeclare package Medium =
         Modelica.Media.Water.ConstantPropertyLiquidWater, m_flow_nominal=2)
diff --git a/AixLib/Controls/HVACAgentBasedControl/Examples/BuildingHeatingSystems/BuildingWithPV.mo b/AixLib/Controls/HVACAgentBasedControl/Examples/BuildingHeatingSystems/BuildingWithPV.mo
index 3f8609d4f1..d01ed9a4a8 100644
--- a/AixLib/Controls/HVACAgentBasedControl/Examples/BuildingHeatingSystems/BuildingWithPV.mo
+++ b/AixLib/Controls/HVACAgentBasedControl/Examples/BuildingHeatingSystems/BuildingWithPV.mo
@@ -169,13 +169,14 @@ model BuildingWithPV
     annotation (Placement(transformation(extent={{-60,118},{-40,138}})));
   ThermalZones.ReducedOrder.ThermalZone.ThermalZone
               thermalZone(redeclare package Medium =
-        Modelica.Media.Air.SimpleAir, zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler())                      annotation(Placement(transformation(extent={{-18,70},
+        Modelica.Media.Air.SimpleAir, 
+    redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam)
+    annotation(Placement(transformation(extent={{-18,70},
             {8,96}})));
   ThermalZones.ReducedOrder.ThermalZone.ThermalZone
               thermalZone1(redeclare package Medium =
-        Modelica.Media.Air.SimpleAir, zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler())                      annotation(Placement(transformation(extent={{64,70},
+        Modelica.Media.Air.SimpleAir, 
+        redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam)                      annotation(Placement(transformation(extent={{64,70},
             {90,96}})));
   BoundaryConditions.WeatherData.Bus        weaBus
     "Weather data bus"
diff --git a/AixLib/Controls/SetPoints/Examples/OccupancySchedule.mo b/AixLib/Controls/SetPoints/Examples/OccupancySchedule.mo
index 81b0fcb9f0..5b48de8da3 100644
--- a/AixLib/Controls/SetPoints/Examples/OccupancySchedule.mo
+++ b/AixLib/Controls/SetPoints/Examples/OccupancySchedule.mo
@@ -10,22 +10,22 @@ model OccupancySchedule "Test model for occupancy schedule with look-ahead"
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/SetPoints/Examples/OccupancySchedule.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example that demonstrates the use of the occupancy schedule.
- The figure below shows how the time until the next occupancy starts or ends
- is decreased. The red line hits zero when the schedule indicates an occupied time,
- and the blue line hits zero when the schedule indicates a non-occupied time.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Controls/SetPoints/Examples/OccupancySchedule.png\" border=\"1\" alt=\"Time until next occupancy.\"/>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example that demonstrates the use of the occupancy schedule.
+The figure below shows how the time until the next occupancy starts or ends
+is decreased. The red line hits zero when the schedule indicates an occupied time,
+and the blue line hits zero when the schedule indicates a non-occupied time.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Controls/SetPoints/Examples/OccupancySchedule.png\" border=\"1\" alt=\"Time until next occupancy.\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OccupancySchedule;
diff --git a/AixLib/Controls/SetPoints/Examples/SupplyReturnTemperatureReset.mo b/AixLib/Controls/SetPoints/Examples/SupplyReturnTemperatureReset.mo
index 5425057512..2c2cf9a4f2 100644
--- a/AixLib/Controls/SetPoints/Examples/SupplyReturnTemperatureReset.mo
+++ b/AixLib/Controls/SetPoints/Examples/SupplyReturnTemperatureReset.mo
@@ -45,30 +45,30 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/SetPoints/Examples/SupplyReturnTemperatureReset.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example that demonstrates the use of the hot water temperature reset
- for a heating system.
- The parameters of the block <code>heaCur</code>
- are for a heating system with
- <i>60</i>&deg;C supply water temperature and
- <i>40</i>&deg;C return water temperature at
- an outside temperature of
- <i>-10</i>&deg;C and a room temperature of
- <i>20</i>&deg;C. The offset for the temperature reset is
- <i>8</i> Kelvin, i.e., above
- <i>12</i>&deg;C outside temperature, there is no heating load.
- The figure below shows the computed supply and return water temperatures.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Controls/SetPoints/Examples/SupplyReturnTemperatureReset.png\" border=\"1\" alt=\"Supply and return water temperatures.\"/>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example that demonstrates the use of the hot water temperature reset
+for a heating system.
+The parameters of the block <code>heaCur</code>
+are for a heating system with
+<i>60</i>&deg;C supply water temperature and
+<i>40</i>&deg;C return water temperature at
+an outside temperature of
+<i>-10</i>&deg;C and a room temperature of
+<i>20</i>&deg;C. The offset for the temperature reset is
+<i>8</i> Kelvin, i.e., above
+<i>12</i>&deg;C outside temperature, there is no heating load.
+The figure below shows the computed supply and return water temperatures.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Controls/SetPoints/Examples/SupplyReturnTemperatureReset.png\" border=\"1\" alt=\"Supply and return water temperatures.\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SupplyReturnTemperatureReset;
diff --git a/AixLib/Controls/SetPoints/Examples/Table.mo b/AixLib/Controls/SetPoints/Examples/Table.mo
index 5672083d0b..cc81b99b42 100644
--- a/AixLib/Controls/SetPoints/Examples/Table.mo
+++ b/AixLib/Controls/SetPoints/Examples/Table.mo
@@ -23,18 +23,18 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/SetPoints/Examples/Table.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example that demonstrates the use of the block
- <a href=\"modelica://AixLib.Controls.SetPoints.Table\">
- AixLib.Controls.SetPoints.Table</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example that demonstrates the use of the block
+<a href=\"modelica://AixLib.Controls.SetPoints.Table\">
+AixLib.Controls.SetPoints.Table</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Table;
diff --git a/AixLib/Controls/SetPoints/OccupancySchedule.mo b/AixLib/Controls/SetPoints/OccupancySchedule.mo
index bbd53c9ecb..055b0d5c14 100644
--- a/AixLib/Controls/SetPoints/OccupancySchedule.mo
+++ b/AixLib/Controls/SetPoints/OccupancySchedule.mo
@@ -175,68 +175,68 @@ equation
           textString="occupied")}),
 defaultComponentName="occSch",
 Documentation(info="<html>
- <p>
- This model outputs whether the building is currently occupied,
- and how long it will take until the next time when the building
- will be occupied or non-occupied.
- The latter may be used, for example, to start a ventilation system
- half an hour before occupancy starts in order to ventilate the room.
- </p>
- <p>
- The occupancy is defined by a time schedule of the form
- </p>
- <pre>
-   occupancy = 3600*{7, 12, 14, 19}
- </pre>
- <p>
- This indicates that the occupancy is from <i>7:00</i> until <i>12:00</i>
- and from <i>14:00</i> to <i>19:00</i>. This will be repeated periodically.
- The parameter <code>periodicity</code> defines the periodicity.
- The period always starts at <i>t=0</i> seconds.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 25, 2021, by Michael Wetter:<br/>
- Integrated changes from Buildings for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1454\">IBPSA, #1454</a>.
- </li>
- <li>
- February 26, 2021, by Michael Wetter:<br/>
- Refactored implementation to use a function to compute the next time events.<br/>
- This is a work-around for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2369\">Buildings, issue 2369</a>.
- </li>
- <li>
- October 30, 2017, by Michael Wetter:<br/>
- Rewrote using <code>equation</code> rather than <code>algorithm</code>
- and removed assertion.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/844\">issue 844</a>.
- </li>
- <li>
- September 11, 2012, by Michael Wetter:<br/>
- Added <code>pre</code> operator in <code>when</code> clause and relaxed
- tolerance in <code>assert</code> statement.
- </li>
- <li>
- July 26, 2012, by Michael Wetter:<br/>
- Fixed a bug that caused an error in the schedule if the simulation start time was negative or equal to the first entry in the schedule.
- </li>
- <li>
- February 16, 2012, by Michael Wetter:<br/>
- Removed parameter <code>startTime</code>. It was removed because <code>startTime=0</code>
- would imply that the schedule should not start for one day if the simulation were
- to be started at <i>t=-8760</i> seconds.
- Fixed bug that prevented schedule to start when the simulation was started at a time that
- is higher than <code>endTime</code>.
- Renamed parameter <code>endTime</code> to <code>period</code>.
- </li>
- <li>
- April 2, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs whether the building is currently occupied,
+and how long it will take until the next time when the building
+will be occupied or non-occupied.
+The latter may be used, for example, to start a ventilation system
+half an hour before occupancy starts in order to ventilate the room.
+</p>
+<p>
+The occupancy is defined by a time schedule of the form
+</p>
+<pre>
+  occupancy = 3600*{7, 12, 14, 19}
+</pre>
+<p>
+This indicates that the occupancy is from <i>7:00</i> until <i>12:00</i>
+and from <i>14:00</i> to <i>19:00</i>. This will be repeated periodically.
+The parameter <code>periodicity</code> defines the periodicity.
+The period always starts at <i>t=0</i> seconds.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 25, 2021, by Michael Wetter:<br/>
+Integrated changes from Buildings for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1454\">IBPSA, #1454</a>.
+</li>
+<li>
+February 26, 2021, by Michael Wetter:<br/>
+Refactored implementation to use a function to compute the next time events.<br/>
+This is a work-around for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2369\">Buildings, issue 2369</a>.
+</li>
+<li>
+October 30, 2017, by Michael Wetter:<br/>
+Rewrote using <code>equation</code> rather than <code>algorithm</code>
+and removed assertion.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/844\">issue 844</a>.
+</li>
+<li>
+September 11, 2012, by Michael Wetter:<br/>
+Added <code>pre</code> operator in <code>when</code> clause and relaxed
+tolerance in <code>assert</code> statement.
+</li>
+<li>
+July 26, 2012, by Michael Wetter:<br/>
+Fixed a bug that caused an error in the schedule if the simulation start time was negative or equal to the first entry in the schedule.
+</li>
+<li>
+February 16, 2012, by Michael Wetter:<br/>
+Removed parameter <code>startTime</code>. It was removed because <code>startTime=0</code>
+would imply that the schedule should not start for one day if the simulation were
+to be started at <i>t=-8760</i> seconds.
+Fixed bug that prevented schedule to start when the simulation was started at a time that
+is higher than <code>endTime</code>.
+Renamed parameter <code>endTime</code> to <code>period</code>.
+</li>
+<li>
+April 2, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OccupancySchedule;
diff --git a/AixLib/Controls/SetPoints/SupplyReturnTemperatureReset.mo b/AixLib/Controls/SetPoints/SupplyReturnTemperatureReset.mo
index 91444cbd06..996283a4f0 100644
--- a/AixLib/Controls/SetPoints/SupplyReturnTemperatureReset.mo
+++ b/AixLib/Controls/SetPoints/SupplyReturnTemperatureReset.mo
@@ -15,12 +15,12 @@ block SupplyReturnTemperatureReset
 
   parameter Boolean use_TRoo_in = false
     "Get the room temperature set point from the input connector"
-    annotation(Evaluate=true, HideResult=true);
+    annotation(Evaluate=true);
   parameter Modelica.Units.SI.Temperature TRoo=293.15
     "Fixed value of room temperature set point"
     annotation (Dialog(enable=not use_TRoo_in));
-  parameter Modelica.Units.SI.TemperatureDifference dTOutHeaBal(displayUnit="K")=
-       8 "Offset for heating curve";
+  parameter Modelica.Units.SI.TemperatureDifference dTOutHeaBal(displayUnit="K")
+     = 8 "Offset for heating curve";
   Modelica.Blocks.Interfaces.RealInput TRoo_in(final quantity="ThermodynamicTemperature",
                                                final unit = "K", displayUnit = "degC", min=0)
        if use_TRoo_in "Room air temperature set point"
@@ -65,53 +65,59 @@ equation
   annotation (
 defaultComponentName="watRes",
 Documentation(info="<html>
- <p>
- This block computes the set point temperatures for the
- supply and return water temperature.
- The set point for the room air temperature can either be specified
- by a parameter, or it can be an input to the model. The latter allows
- to use this model with systems that have night set back.
- </p>
- <p>
- If used to reset the temperature in a heating system,
- the parameter <code>dTOutHeaBal</code> can be used to shift the heating curve
- to take into account that heat gains from solar, equipment and people
- make up for some of the transmission losses.
- For example, in energy efficient houses, the heating may not be switched on if
- the outside air temperature is greater than
- <i>12</i>&deg;C, even if a room temperature of <i>20</i>&deg;C is required.
- In such a situation, set <code>dTOutHeaBal=20-12=8</code> Kelvin to
- shift the heating curve.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 03, 2020, by Jianjun Hu:<br/>
- Changed name from <code>HotWaterTemperatureReset</code> to 
- <code>SupplyReturnTemperatureReset</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1273\">#1273</a>.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- February 13, 2013, by Michael Wetter:<br/>
- Corrected error that led to wrong results if the room air temperature is
- different from its nominal value <code>TRoo_nominal</code>.
- See ticket <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/74\">#74</a>.
- </li>
- <li>
- November 21, 2011, by Michael Wetter:<br/>
- Improved documentation.
- </li>
- <li>
- February 5, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<p>
+This block computes the set point temperatures for the
+supply and return water temperature.
+The set point for the room air temperature can either be specified
+by a parameter, or it can be an input to the model. The latter allows
+to use this model with systems that have night set back.
+</p>
+<p>
+If used to reset the temperature in a heating system,
+the parameter <code>dTOutHeaBal</code> can be used to shift the heating curve
+to take into account that heat gains from solar, equipment and people
+make up for some of the transmission losses.
+For example, in energy efficient houses, the heating may not be switched on if
+the outside air temperature is greater than
+<i>12</i>&deg;C, even if a room temperature of <i>20</i>&deg;C is required.
+In such a situation, set <code>dTOutHeaBal=20-12=8</code> Kelvin to
+shift the heating curve.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+January 03, 2020, by Jianjun Hu:<br/>
+Changed name from <code>HotWaterTemperatureReset</code> to
+<code>SupplyReturnTemperatureReset</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1273\">#1273</a>.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+February 13, 2013, by Michael Wetter:<br/>
+Corrected error that led to wrong results if the room air temperature is
+different from its nominal value <code>TRoo_nominal</code>.
+See ticket <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/74\">#74</a>.
+</li>
+<li>
+November 21, 2011, by Michael Wetter:<br/>
+Improved documentation.
+</li>
+<li>
+February 5, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Polygon(
           points={{90,-82},{68,-74},{68,-90},{90,-82}},
           lineColor={192,192,192},
@@ -148,6 +154,6 @@ Documentation(info="<html>
         Text(
           extent={{42,-30},{92,-80}},
           textColor={0,0,127},
-          textString="TRet")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="TRet")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SupplyReturnTemperatureReset;
diff --git a/AixLib/Controls/SetPoints/Table.mo b/AixLib/Controls/SetPoints/Table.mo
index 055c7bc170..67484c3ab2 100644
--- a/AixLib/Controls/SetPoints/Table.mo
+++ b/AixLib/Controls/SetPoints/Table.mo
@@ -36,57 +36,57 @@ equation
   annotation (
 defaultComponentName="tab",
 Documentation(info="<html>
- <p>
- This block can be used to schedule a set-point by using piecewise linear functions.
- For example, the instances
- </p>
- <pre>
- AixLib.Controls.SetPoints.Table tabLinExt(constantExtrapolation=false,
-                                              table=[20, 0.0;
-                                                     22, 0.5;
-                                                     25, 0.5;
-                                                     26, 1.0]);
- AixLib.Controls.SetPoints.Table tabConExt(constantExtrapolation=true,
-                                              table=[20, 0.0;
-                                                     22, 0.5;
-                                                     25, 0.5;
-                                                     26, 1.0]);
- </pre>
- <p>
- will cause the following output:
- </p>
- <p>
- <img src=\"modelica://AixLib/Resources/Images/Controls/SetPoints/Table.png\" border=\"1\" alt=\"Table output.\"/>
- </p>
- <p>
- For the default setting <code>constantExtrapolation=true</code>, the
- block outputs
- <code>y=y1+offset</code> for <code>u &le; u1</code>, and
- <code>y=yMax+offset</code> for <code>u &ge; uMax</code>.
- Otherwise, the table is linearly extrapolated with a constant derivative.
- </p>
- <p>
- Note that the first column must be strictly increasing.
- </p>
- </html>",
+<p>
+This block can be used to schedule a set-point by using piecewise linear functions.
+For example, the instances
+</p>
+<pre>
+AixLib.Controls.SetPoints.Table tabLinExt(constantExtrapolation=false,
+                                             table=[20, 0.0;
+                                                    22, 0.5;
+                                                    25, 0.5;
+                                                    26, 1.0]);
+AixLib.Controls.SetPoints.Table tabConExt(constantExtrapolation=true,
+                                             table=[20, 0.0;
+                                                    22, 0.5;
+                                                    25, 0.5;
+                                                    26, 1.0]);
+</pre>
+<p>
+will cause the following output:
+</p>
+<p>
+<img src=\"modelica://AixLib/Resources/Images/Controls/SetPoints/Table.png\" border=\"1\" alt=\"Table output.\"/>
+</p>
+<p>
+For the default setting <code>constantExtrapolation=true</code>, the
+block outputs
+<code>y=y1+offset</code> for <code>u &le; u1</code>, and
+<code>y=yMax+offset</code> for <code>u &ge; uMax</code>.
+Otherwise, the table is linearly extrapolated with a constant derivative.
+</p>
+<p>
+Note that the first column must be strictly increasing.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 30, 2016, by Michael Wetter:<br/>
- Changed protected final parameter <code>nCol</code> to <code>nRow</code>.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/555\">issue 555</a>.
- </li>
- <li>
- April 5, 2011, by Michael Wetter:<br/>
- Fixed wrong table declaration.
- </li>
- <li>
- July 13, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+August 30, 2016, by Michael Wetter:<br/>
+Changed protected final parameter <code>nCol</code> to <code>nRow</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/555\">issue 555</a>.
+</li>
+<li>
+April 5, 2011, by Michael Wetter:<br/>
+Fixed wrong table declaration.
+</li>
+<li>
+July 13, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
     Text(
       extent={{-78,-45},{-40,-56}},
@@ -134,6 +134,6 @@ revisions="<html>
     Line(
       points={{26,24},{77,24}},
       color={0,0,255},
-      thickness=0.5)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+      thickness=0.5)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Table;
diff --git a/AixLib/Controls/SetPoints/Validation/OccupancyScheduleNegativeStartTime.mo b/AixLib/Controls/SetPoints/Validation/OccupancyScheduleNegativeStartTime.mo
index 25b8016f2c..6fefe9cfc5 100644
--- a/AixLib/Controls/SetPoints/Validation/OccupancyScheduleNegativeStartTime.mo
+++ b/AixLib/Controls/SetPoints/Validation/OccupancyScheduleNegativeStartTime.mo
@@ -18,17 +18,17 @@ model OccupancyScheduleNegativeStartTime
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/SetPoints/Validation/OccupancyScheduleNegativeStartTime.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example that validates the occupancy schedule
- for a negative start time.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 30, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example that validates the occupancy schedule
+for a negative start time.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 30, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OccupancyScheduleNegativeStartTime;
diff --git a/AixLib/Controls/SetPoints/Validation/OccupancySchedulePositiveStartTime.mo b/AixLib/Controls/SetPoints/Validation/OccupancySchedulePositiveStartTime.mo
index b0423ba34a..cb02ce8a85 100644
--- a/AixLib/Controls/SetPoints/Validation/OccupancySchedulePositiveStartTime.mo
+++ b/AixLib/Controls/SetPoints/Validation/OccupancySchedulePositiveStartTime.mo
@@ -9,17 +9,17 @@ model OccupancySchedulePositiveStartTime
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Controls/SetPoints/Validation/OccupancySchedulePositiveStartTime.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example that validates the occupancy schedule
- for a positive start time.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 30, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example that validates the occupancy schedule
+for a positive start time.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 30, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OccupancySchedulePositiveStartTime;
diff --git a/AixLib/DataBase/CHP/CHPDataSimple/CHP_Cleanergy_C9G.mo b/AixLib/DataBase/CHP/CHPDataSimple/CHP_Cleanergy_C9G.mo
index f07ca7e765..59695e39d2 100644
--- a/AixLib/DataBase/CHP/CHPDataSimple/CHP_Cleanergy_C9G.mo
+++ b/AixLib/DataBase/CHP/CHPDataSimple/CHP_Cleanergy_C9G.mo
@@ -53,10 +53,7 @@ record CHP_Cleanergy_C9G
 <h4>
   <span style=\"color:#008000\">Data Sheet (English, German)</span>
 </h4>
-<table>
-  <caption>
-    \"Data Sheet\" cellspacing=\"0\" cellpadding=\"0\" border=\"0\
-  </caption>
+<table cellspacing=\"0\" cellpadding=\"0\" border=\"1\">
   <tr>
     <td valign=\"top\">
       <p>
diff --git a/AixLib/DataBase/CHP/CHPDataSimple/CHP_XRGI_9kWel.mo b/AixLib/DataBase/CHP/CHPDataSimple/CHP_XRGI_9kWel.mo
index c72d42af43..241ffa8576 100644
--- a/AixLib/DataBase/CHP/CHPDataSimple/CHP_XRGI_9kWel.mo
+++ b/AixLib/DataBase/CHP/CHPDataSimple/CHP_XRGI_9kWel.mo
@@ -42,10 +42,7 @@ record CHP_XRGI_9kWel "Eco Power: mini BHKW XRGI 9 (12-20 kW thermal)"
 <h4>
   <span style=\"color:#008000\">Data Sheet (English, German)</span>
 </h4>
-<table>
-  <caption>
-    \"Data Sheet\" cellspacing=\"0\" cellpadding=\"0\" border=\"0\
-  </caption>
+<table cellspacing=\"0\" cellpadding=\"0\" border=\"1\">
   <tr>
     <td valign=\"top\">
       <p>
@@ -255,9 +252,10 @@ record CHP_XRGI_9kWel "Eco Power: mini BHKW XRGI 9 (12-20 kW thermal)"
     </td>
   </tr>
 </table>
-<table>
+<br>
+<table cellspacing=\"0\" cellpadding=\"0\" border=\"1\">
   <caption>
-    \"Emmisions\" cellspacing=\"0\" cellpadding=\"0\" border=\"0\
+    Emissions
   </caption>
   <tr>
     <td valign=\"top\">
diff --git a/AixLib/DataBase/Pools/ChildrensPool.mo b/AixLib/DataBase/Pools/ChildrensPool.mo
new file mode 100644
index 0000000000..a36f63b80f
--- /dev/null
+++ b/AixLib/DataBase/Pools/ChildrensPool.mo
@@ -0,0 +1,40 @@
+within AixLib.DataBase.Pools;
+record ChildrensPool "Pool which is mainly used by children"
+  extends AixLib.DataBase.Pools.IndoorSwimmingPoolBaseDataDefinition(
+    TPool=303.15,
+    VPool=126.8,
+    APool=125.0,
+    depthPool=0.9303008070432868,
+    VSto=69.333925940005700,
+    V_flow_nominal=0.028045267489711933,
+    V_flow_par=0.0125,
+    use_parLoa=true,
+    dpHeaExcPool=0,
+    use_ideHeaExc=true,
+    KHeat=1000,
+    timeHea=1,
+    QMaxHeat=1000000,
+    QMinHeat=0,
+    betaInUse=0.011111111111111112,
+    use_poolCov=false,
+    use_watRec=false,
+    x_rec=0.0,
+    m_flow_out=0.055645372003397,
+    use_HRS=true,
+    etaHRS=0.8,
+    use_wavPool=false,
+    heiWav=0,
+    widWav=0,
+    perWavPul=1800,
+    timeWavPul_start=0,
+    widWavPul=0,
+    AWalInt=0.001,
+    AWalExt=156.5,
+    AFloInt=0.001,
+    AFloExt=156.5,
+    hConWatHor=50.0,
+    hConWatVer=5200.0);
+annotation (Documentation(info="<html>
+<p>The swimming pool &quot;ChildrensPool&quot; describes a typical indoor swimming pool, which is mainly used by children and to teach children swimming. </p>
+</html>"));
+end ChildrensPool;
diff --git a/AixLib/DataBase/Pools/IndoorSwimmingPoolBaseDataDefinition.mo b/AixLib/DataBase/Pools/IndoorSwimmingPoolBaseDataDefinition.mo
new file mode 100644
index 0000000000..e797fc5905
--- /dev/null
+++ b/AixLib/DataBase/Pools/IndoorSwimmingPoolBaseDataDefinition.mo
@@ -0,0 +1,74 @@
+within AixLib.DataBase.Pools;
+record IndoorSwimmingPoolBaseDataDefinition
+  extends Modelica.Icons.Record;
+
+  parameter Modelica.Units.SI.Temperature TPool
+    "Set water temperature of swimming pool";
+  parameter Modelica.Units.SI.Volume VPool "Volume of pool water";
+  parameter Modelica.Units.SI.Area APool(min=0)
+    "Area of water surface of swimming pool";
+  parameter Modelica.Units.SI.Length depthPool(min=0)
+    "Average depth of swimming pool";
+  parameter Modelica.Units.SI.Volume VSto
+    "Usable Volume of water storage, DIN 19643-1";
+
+  // parameter for pool water circulation
+  parameter Modelica.Units.SI.VolumeFlowRate V_flow_nominal(min=0.001)
+    "Circulation volume flow rate";
+  parameter Modelica.Units.SI.VolumeFlowRate V_flow_par(min=0)
+    "In the case of partial load: circulation volume flow rate during non-opening hours, DIN 19643-1";
+  parameter Boolean use_parLoa=false  "Partial load operation implemented for non opening hours?";
+  parameter Modelica.Units.SI.PressureDifference dpHeaExcPool
+    "Pressure drop of heat exchanger, should be zero for an indeal heated pool";
+  parameter Boolean use_ideHeaExc=true "Include an ideal heat exchanger into the circulation system";
+  parameter Real KHeat "Gain of controller for ideal heater";
+  parameter Modelica.Units.SI.Time timeHea "Time constant of Integrator block for ideal heater";
+  parameter Real QMaxHeat "Upper limit of output for ideal heater";
+  parameter Real QMinHeat "Lower limit of output for ideal heater";
+
+  // parameter for evaporation
+  parameter Real betaInUse(unit="m/s") "Water transfer coefficient during opening hours if pool is used, VDI 2089";
+  parameter Boolean use_poolCov=false "Pool covered during non opening hours";
+
+  // parameter for fresh water
+  parameter Boolean use_watRec= false "Recycled water used for refilling pool water?";
+  parameter Real x_rec(min=0) "Percentage of refilling water provided by recycled  pool water, DIN 19643-1: <= 0,8";
+  parameter Modelica.Units.SI.MassFlowRate m_flow_out(min=0.0001)
+    "Waterexchange due to people in the pool, DIN 19643-1";
+  parameter Boolean use_HRS=false "Is a heat recovery system physically integrated?";
+  parameter Modelica.Units.SI.Efficiency etaHRS
+    "Effieciency of heat recovery system";
+
+ // Wave mode
+  parameter Boolean use_wavPool=false "Is there a wave machine installed?";
+  parameter Modelica.Units.SI.Length heiWav "Height of generated wave";
+  parameter Modelica.Units.SI.Length widWav
+    "Width of generated wave/ width of wave machineoutlet";
+  parameter Modelica.Units.SI.Time timeWavPul_start
+    "Start time of first wave cycle";
+  parameter Modelica.Units.SI.Time perWavPul "Time of cycling period";
+  parameter Real widWavPul "Fraction of time of wave generation within cycling period";
+
+ // Pool Walls
+  parameter Modelica.Units.SI.Area AWalInt "Area of pool walls which is connected to inner rooms (inner pool walls)";
+  parameter Modelica.Units.SI.Area AWalExt "Area of pool walls which is connected to the ground (pool wall with earth contact)";
+  parameter Modelica.Units.SI.Area AFloInt "Area of pool floors which is connected to inner rooms (inner pool floor)";
+  parameter Modelica.Units.SI.Area AFloExt "Area of pool floors which is connected to teh ground (pool floor with earth contact)";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConWatHor "Mean value for the heat transfer coefficient of free convection on horizontal pool floors";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConWatVer "Mean value for the heat transfer coefficient of free convection on vertical pool walls";
+
+  annotation (Documentation(info="<html>
+
+  This is the base definition of indoor swimming pool records used in <a href=
+  \"AixLib.Fluid.Pools.IndoorSwimmingPool\">AixLib.Fluid.Pools.IndoorSwimmingPool</a>.
+  It aggregates all parameters at one record to enhance usability,
+  exchanging entire datasets and automatic generation of these
+  datasets.
+<h4>References </h4>
+<ul>
+<li>German Association of Engineers: Guideline VDI 2089-1, January 2010: Building Services in swimming baths - Indoor Pools</li>
+<li>German Institute for Standardization DIN 19643-1, November 2012: Treatment of water of swimming pools and baths - Part 1 General Requirements</li>
+<li>Chroistoph Saunus, 2005: Schwimmb&auml;der Planung - Ausf&uuml;hrung - Betrieb</li>
+</ul>
+</html>"));
+end IndoorSwimmingPoolBaseDataDefinition;
diff --git a/AixLib/DataBase/Pools/IndoorSwimmingPoolDummy.mo b/AixLib/DataBase/Pools/IndoorSwimmingPoolDummy.mo
new file mode 100644
index 0000000000..9f22bfe50c
--- /dev/null
+++ b/AixLib/DataBase/Pools/IndoorSwimmingPoolDummy.mo
@@ -0,0 +1,41 @@
+within AixLib.DataBase.Pools;
+record IndoorSwimmingPoolDummy
+  "This is a dummy record with non-physical parameter values."
+  extends AixLib.DataBase.Pools.IndoorSwimmingPoolBaseDataDefinition(
+    TPool=Modelica.Constants.eps,
+    VPool=Modelica.Constants.inf,
+    APool=Modelica.Constants.inf,
+    depthPool=Modelica.Constants.inf,
+    VSto=Modelica.Constants.inf,
+    V_flow_nominal=Modelica.Constants.inf,
+    V_flow_par=Modelica.Constants.inf,
+    use_parLoa=false,
+    dpHeaExcPool=Modelica.Constants.inf,
+    use_ideHeaExc=true,
+    KHeat=Modelica.Constants.inf,
+    timeHea=Modelica.Constants.inf,
+    QMaxHeat=Modelica.Constants.inf,
+    QMinHeat=Modelica.Constants.inf,
+    betaInUse=Modelica.Constants.inf,
+    use_poolCov=false,
+    use_watRec=false,
+    x_rec=Modelica.Constants.inf,
+    m_flow_out=Modelica.Constants.inf,
+    use_HRS=false,
+    etaHRS=Modelica.Constants.eps,
+    use_wavPool=false,
+    heiWav=Modelica.Constants.inf,
+    widWav=Modelica.Constants.inf,
+    perWavPul=Modelica.Constants.eps,
+    timeWavPul_start=Modelica.Constants.eps,
+    widWavPul=Modelica.Constants.eps,
+    AWalInt=Modelica.Constants.inf,
+    AWalExt=Modelica.Constants.inf,
+    AFloExt=Modelica.Constants.inf,
+    AFloInt=Modelica.Constants.inf,
+    hConWatHor=Modelica.Constants.inf,
+    hConWatVer=Modelica.Constants.inf);
+  annotation (Documentation(info="<html>
+<p>This record is a place holder for zones without swimming pools to avoid error messages.</p>
+</html>"));
+end IndoorSwimmingPoolDummy;
diff --git a/AixLib/DataBase/Pools/SportPool.mo b/AixLib/DataBase/Pools/SportPool.mo
new file mode 100644
index 0000000000..a9e9e3e29f
--- /dev/null
+++ b/AixLib/DataBase/Pools/SportPool.mo
@@ -0,0 +1,40 @@
+within AixLib.DataBase.Pools;
+record SportPool "Pool which is mainly used by sport swimmers"
+  extends AixLib.DataBase.Pools.IndoorSwimmingPoolBaseDataDefinition(
+    TPool=301.15,
+    VPool=942.956,
+    APool=416.5,
+    depthPool=2.2640000000000002,
+    VSto=69.333925940005700,
+    V_flow_nominal=0.0856995884773662,
+    V_flow_par=0.023144444444444443,
+    use_parLoa=true,
+    dpHeaExcPool=0,
+    use_ideHeaExc=true,
+    KHeat=1000,
+    timeHea=1,
+    QMaxHeat=1000000,
+    QMinHeat=0,
+    betaInUse=0.011111111111111112,
+    use_poolCov=false,
+    use_watRec=false,
+    x_rec=0.0,
+    m_flow_out=0.170038866026520,
+    use_HRS=true,
+    etaHRS=0.8,
+    use_wavPool=false,
+    heiWav=0,
+    widWav=0,
+    perWavPul=1800,
+    timeWavPul_start=0,
+    widWavPul=10/30*100,
+    AWalInt=21.658,
+    AWalExt=143.32,
+    AFloInt=0.001,
+    AFloExt=559.82,
+    hConWatHor=50.0,
+    hConWatVer=5200.0);
+  annotation (Documentation(info="<html>
+<p>The swimming pool &quot;SportPool&quot; describes a typical indoor swimming pool, which is mainly used for sport swimming. </p>
+</html>"));
+end SportPool;
diff --git a/AixLib/DataBase/Pools/SwimmingPoolWalls/ConcreteInsulationConstruction.mo b/AixLib/DataBase/Pools/SwimmingPoolWalls/ConcreteInsulationConstruction.mo
new file mode 100644
index 0000000000..1ff635dbef
--- /dev/null
+++ b/AixLib/DataBase/Pools/SwimmingPoolWalls/ConcreteInsulationConstruction.mo
@@ -0,0 +1,13 @@
+within AixLib.DataBase.Pools.SwimmingPoolWalls;
+record ConcreteInsulationConstruction
+  "Concrete pool construction with insulation"
+  extends AixLib.DataBase.Walls.WallBaseDataDefinition(
+    n(min=1) = 3 "Number of wall layers",
+    d={0.05,0.2,0.1} "Thickness of wall layers",
+    rho={1940,2330,30} "Density of wall layers",
+    lambda={1.4,2.1,0.035} "Thermal conductivity of wall layers",
+    c={0.0001,0.001,0.00138} "Specific heat capacity of wall layers",
+    eps=0.9 "Emissivity of inner wall surface");
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end ConcreteInsulationConstruction;
diff --git a/AixLib/DataBase/Pools/SwimmingPoolWalls/StainlessSteelConstruction.mo b/AixLib/DataBase/Pools/SwimmingPoolWalls/StainlessSteelConstruction.mo
new file mode 100644
index 0000000000..0f6a93fff7
--- /dev/null
+++ b/AixLib/DataBase/Pools/SwimmingPoolWalls/StainlessSteelConstruction.mo
@@ -0,0 +1,13 @@
+within AixLib.DataBase.Pools.SwimmingPoolWalls;
+record StainlessSteelConstruction
+  "Stainless steel pool construction without insulation"
+  extends AixLib.DataBase.Walls.WallBaseDataDefinition(
+    n(min=1) = 1 "Number of wall layers",
+    d={0.05} "Thickness of wall layers",
+    rho={7900} "Density of wall layers",
+    lambda={15} "Thermal conductivity of wall layers",
+    c={500} "Specific heat capacity of wall layers",
+    eps=0.9 "Emissivity of inner wall surface");
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end StainlessSteelConstruction;
diff --git a/AixLib/DataBase/Pools/SwimmingPoolWalls/WallDummy.mo b/AixLib/DataBase/Pools/SwimmingPoolWalls/WallDummy.mo
new file mode 100644
index 0000000000..b774b05586
--- /dev/null
+++ b/AixLib/DataBase/Pools/SwimmingPoolWalls/WallDummy.mo
@@ -0,0 +1,12 @@
+within AixLib.DataBase.Pools.SwimmingPoolWalls;
+record WallDummy
+  extends AixLib.DataBase.Walls.WallBaseDataDefinition(
+    n(min=1) = 1 "Number of wall layers",
+    d={1} "Thickness of wall layers",
+    rho={1} "Density of wall layers",
+    lambda={1} "Thermal conductivity of wall layers",
+    c={1} "Specific heat capacity of wall layers",
+    eps=1 "Emissivity of inner wall surface");
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end WallDummy;
diff --git a/AixLib/DataBase/Pools/SwimmingPoolWalls/package.mo b/AixLib/DataBase/Pools/SwimmingPoolWalls/package.mo
new file mode 100644
index 0000000000..f30a5470d1
--- /dev/null
+++ b/AixLib/DataBase/Pools/SwimmingPoolWalls/package.mo
@@ -0,0 +1,3 @@
+within AixLib.DataBase.Pools;
+package SwimmingPoolWalls
+end SwimmingPoolWalls;
diff --git a/AixLib/DataBase/Pools/SwimmingPoolWalls/package.order b/AixLib/DataBase/Pools/SwimmingPoolWalls/package.order
new file mode 100644
index 0000000000..00e3e0df3f
--- /dev/null
+++ b/AixLib/DataBase/Pools/SwimmingPoolWalls/package.order
@@ -0,0 +1,3 @@
+ConcreteInsulationConstruction
+StainlessSteelConstruction
+WallDummy
diff --git a/AixLib/DataBase/Pools/package.mo b/AixLib/DataBase/Pools/package.mo
new file mode 100644
index 0000000000..a508758aed
--- /dev/null
+++ b/AixLib/DataBase/Pools/package.mo
@@ -0,0 +1,3 @@
+within AixLib.DataBase;
+package Pools
+end Pools;
diff --git a/AixLib/DataBase/Pools/package.order b/AixLib/DataBase/Pools/package.order
new file mode 100644
index 0000000000..5acacb2f4f
--- /dev/null
+++ b/AixLib/DataBase/Pools/package.order
@@ -0,0 +1,5 @@
+ChildrensPool
+IndoorSwimmingPoolBaseDataDefinition
+IndoorSwimmingPoolDummy
+SportPool
+SwimmingPoolWalls
diff --git a/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN25_H05_12.mo b/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN25_H05_12.mo
new file mode 100644
index 0000000000..a0e698b631
--- /dev/null
+++ b/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN25_H05_12.mo
@@ -0,0 +1,138 @@
+within AixLib.DataBase.Pumps.PumpPolynomialBased;
+record Pump_DN25_H05_12 "Pump with head 0.5 to 12,4m and 12,4m^3/h volume flow (25/0.5-12 PN)"
+   extends PumpBaseRecord(
+     maxMinHeight=[
+           0.00, 12.30,  0.367;
+           0.40, 12.37,  0.335;
+           0.79, 12.44,  0.303;
+           1.19, 12.40,  0.287;
+           1.59, 12.23,  0.288;
+           1.98, 12.07,  0.290;
+           2.38, 11.84,  0.000;
+           2.78, 11.61,  0.000;
+           3.17, 11.35,  0.000;
+           3.57, 11.07,  0.000;
+           3.97, 10.79,  0.000;
+           4.36, 10.48,  0.000;
+           4.76, 10.17,  0.000;
+           5.16,  9.83,  0.000;
+           5.55,  9.47,  0.000;
+           5.95,  9.11,  0.000;
+           6.34,  8.78,  0.000;
+           6.74,  8.47,  0.000;
+           7.14,  8.15,  0.000;
+           7.53,  7.82,  0.000;
+           7.93,  7.49,  0.000;
+           8.33,  7.14,  0.000;
+           8.72,  6.80,  0.000;
+           9.12,  6.45,  0.000;
+           9.52,  6.10,  0.000;
+           9.91,  5.75,  0.000;
+          10.31,  5.34,  0.000;
+          10.71,  4.91,  0.000;
+          11.10,  4.48,  0.000;
+          11.50,  4.05,  0.000]
+      "maximum and minimum boundaries of pump (Q,Hmax,Hmin)",
+    maxMinSpeedCurves = [
+           0.00, 4333,  739;
+           0.40, 4334,  740;
+           0.79, 4335,  741;
+           1.19, 4320,  753;
+           1.59, 4286,  777;
+           1.98, 4253,  801;
+           2.38, 4208,  802;
+           2.78, 4163,  802;
+           3.17, 4128,  802;
+           3.57, 4106,  802;
+           3.97, 4084,  802;
+           4.36, 4030,  802;
+           4.76, 3974,  802;
+           5.16, 3917,  802;
+           5.55, 3861,  802;
+           5.95, 3804,  802;
+           6.34, 3768,  802;
+           6.74, 3734,  802;
+           7.14, 3705,  802;
+           7.53, 3683,  802;
+           7.93, 3661,  802;
+           8.33, 3639,  802;
+           8.72, 3617,  802;
+           9.12, 3595,  802;
+           9.52, 3573,  802;
+           9.91, 3551,  802;
+          10.31, 3517,  802;
+          10.71, 3479,  802;
+          11.10, 3442,  802;
+          11.50, 3405,  802]
+      "maximum and minimum boundaries of pump speed (Q,nMax,nMin)",
+    nMin=750,
+    nMax=4350,
+    cHQN=[ 0.00000e+00,  0.00000e+00,  6.52362e-07;
+           0.00000e+00,  6.12540e-05,  0.00000e+00;
+          -4.34488e-02,  0.00000e+00,  0.00000e+00]
+       "coefficients for H = f(Q,N)",
+    cPQN=[1.17764e+00,  2.85662e-03, -2.38557e-06,  3.01986e-09, -2.01864e-13;
+           0.00000e+00,  0.00000e+00,  1.75607e-06,  0.00000e+00,  0.00000e+00;
+           0.00000e+00,  2.57857e-04,  0.00000e+00,  0.00000e+00,  0.00000e+00;
+          -8.92872e-02,  0.00000e+00,  0.00000e+00,  0.00000e+00,  0.00000e+00]
+       "coefficients for P = f(Q,N)");
+
+  annotation(preferredView="text", Documentation(revisions="<html><ul>
+
+  <li>2023-10-19 by Sarah Leidolf:<br/>
+    Generated
+  </li>
+</ul>
+
+</html>", info="<html><h4>
+  Measurement and Regression Data
+</h4>
+<p>
+  Impure curves at high pump speed because of inaccurate data of upper
+  and lower limit of pump speed.
+</p>
+<p>
+  <img src=
+  \"modelica://AixLib/Resources/Images/DataBase/Pumps/PumpsPolynomialBased/Pump_DN25_H05_12.png\"
+  alt=\"1\">
+
+</p>
+<p>
+  cHQN:
+</p>
+<p>
+
+  <span style=\"font-family: Courier New;\">0.00000e+00, 0.00000e+00,
+  6.52362e-07;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 6.12540e-05,
+  0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-4.34488e-02, 0.00000e+00,
+  0.00000e+00</span>
+
+</p>
+<p>
+  cPQN:
+</p>
+<p>
+
+  <span style=\"font-family: Courier New;\">1.17764e+00, 2.85662e-03,
+  -2.38557e-06, 3.01986e-09, -2.01864e-13;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 0.00000e+00,
+  1.75607e-06, 0.00000e+00, 0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 2.57857e-04,
+  0.00000e+00, 0.00000e+00, 0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-8.92872e-02, 0.00000e+00,
+  0.00000e+00, 0.00000e+00, 0.00000e+00</span>
+</p>
+</html>"));
+end Pump_DN25_H05_12;
diff --git a/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN30_H1_12.mo b/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN30_H1_12.mo
new file mode 100644
index 0000000000..6718cfe7dc
--- /dev/null
+++ b/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN30_H1_12.mo
@@ -0,0 +1,144 @@
+within AixLib.DataBase.Pumps.PumpPolynomialBased;
+record Pump_DN30_H1_12 "Pump with head 1 to 11m and 10,7m^3/h volume flow (Wilo Stratos 30/1-12)"
+ extends PumpBaseRecord(
+    maxMinHeight=[
+           0.00, 11.53,  0.800;
+           0.41, 11.62,  0.832;
+           0.83, 11.71,  0.865;
+           1.24, 11.79,  0.897;
+           1.66, 11.88,  0.929;
+           2.07, 11.97,  0.944;
+           2.49, 12.05,  0.825;
+           2.90, 12.14,  0.706;
+           3.32, 12.18,  0.587;
+           3.73, 11.66,  0.467;
+           4.15, 11.14,  0.000;
+           4.56, 10.62,  0.000;
+           4.98, 10.09,  0.000;
+           5.39,  9.64,  0.000;
+           5.81,  9.21,  0.000;
+           6.22,  8.78,  0.000;
+           6.63,  8.35,  0.000;
+           7.05,  7.92,  0.000;
+           7.46,  7.50,  0.000;
+           7.88,  7.09,  0.000;
+           8.29,  6.67,  0.000;
+           8.71,  6.25,  0.000;
+           9.12,  5.82,  0.000;
+           9.54,  5.34,  0.000;
+           9.95,  4.86,  0.000;
+          10.37,  4.39,  0.000;
+          10.78,  3.90,  0.000;
+          11.20,  3.32,  0.000;
+          11.61,  2.73,  0.000;
+          12.03,  2.15,  0.000]
+      "maximum and minimum boundaries of pump (Q,Hmax,Hmin)",
+    maxMinSpeedCurves = [
+            0.00, 4800, 1400;
+           0.41, 4800, 1400;
+           0.83, 4800, 1400;
+           1.24, 4800, 1400;
+           1.66, 4800, 1400;
+           2.07, 4800, 1400;
+           2.49, 4800, 1400;
+           2.90, 4800, 1400;
+           3.32, 4798, 1400;
+           3.73, 4773, 1400;
+           4.15, 4747, 1400;
+           4.56, 4722, 1400;
+           4.98, 4696, 1400;
+           5.39, 4662, 1400;
+           5.81, 4625, 1400;
+           6.22, 4588, 1400;
+           6.63, 4550, 1400;
+           7.05, 4514, 1400;
+           7.46, 4480, 1400;
+           7.88, 4447, 1400;
+           8.29, 4413, 1400;
+           8.71, 4379, 1400;
+           9.12, 4345, 1400;
+           9.54, 4309, 1400;
+           9.95, 4274, 1400;
+          10.37, 4238, 1400;
+          10.78, 4202, 1400;
+          11.20, 4168, 1400;
+          11.61, 4134, 1400;
+          12.03, 4100, 1400]
+      "maximum and minimum boundaries of pump speed (Q,nMax,nMin)",
+    nMin=1400,
+    nMax=4800,
+    cHQN=[0.00000e+00,  0.00000e+00,  5.07080e-07;
+           0.00000e+00,  6.15992e-05,  0.00000e+00;
+          -6.58190e-02,  0.00000e+00,  0.00000e+00]
+       "coefficients for H = f(Q,N)",
+    cPQN=[4.06360e-05,  2.77185e-02, -2.02099e-05,  8.49238e-09, -8.67775e-13;
+           0.00000e+00,  0.00000e+00,  1.21688e-06,  0.00000e+00,  0.00000e+00;
+           0.00000e+00,  6.87022e-06,  0.00000e+00,  0.00000e+00,  0.00000e+00;
+          -3.71130e-02,  0.00000e+00,  0.00000e+00,  0.00000e+00,  0.00000e+00]
+       "coefficients for P = f(Q,N)");
+
+  annotation(preferredView="text", Documentation(revisions="<html><ul>
+  <li>2023-10-19 by Sarah Leidolf:<br/>
+    Generated
+  </li>
+</ul>
+
+</html>", info="<html><h4>
+  Measurement and Regression Data
+</h4>
+<p>
+  Dimension estimate, but inaccuracies occur due to lack of information
+  in the data sheets.
+</p>
+<p>
+  Espacially because of missing information of upper and lower limit of
+  pump speed.
+</p>
+<p>
+  <br/>
+  <img src=
+  \"modelica://AixLib/Resources/Images/DataBase/Pumps/PumpsPolynomialBased/Pump_DN30_H1_12.png\"
+  alt=\"1\">
+
+</p>
+<p>
+  cHQN:
+</p>
+<p>
+
+  <span style=\"font-family: Courier New;\">0.00000e+00, 0.00000e+00,
+  5.07080e-07;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 6.15992e-05,
+  0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-6.58190e-02, 0.00000e+00,
+  0.00000e+00</span>
+
+</p>
+<p>
+  cPQN:
+</p>
+<p>
+
+  <span style=\"font-family: Courier New;\">4.06360e-05, 2.77185e-02,
+  -2.02099e-05, 8.49238e-09, -8.67775e-13;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 0.00000e+00,
+  1.21688e-06, 0.00000e+00, 0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 6.87022e-06,
+  0.00000e+00, 0.00000e+00, 0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-3.71130e-02, 0.00000e+00,
+  0.00000e+00, 0.00000e+00, 0.00000e+00</span>
+
+</p>
+</html>"));
+
+end Pump_DN30_H1_12;
diff --git a/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN50_H05_16.mo b/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN50_H05_16.mo
new file mode 100644
index 0000000000..b0b2fa1ba2
--- /dev/null
+++ b/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN50_H05_16.mo
@@ -0,0 +1,140 @@
+within AixLib.DataBase.Pumps.PumpPolynomialBased;
+record Pump_DN50_H05_16 "Pump with head 0.5 to 15,8m and 54m^3/h volume flow (Wilo Stratos Maxo 50/0.5-16 PN6/10)"
+   extends PumpBaseRecord(
+    maxMinHeight=[
+           0.00, 15.73,  0.427;
+           1.82, 15.83,  0.451;
+           3.64, 15.93,  0.475;
+           5.45, 15.95,  0.422;
+           7.27, 15.95,  0.349;
+           9.09, 15.89,  0.246;
+          10.91, 15.79,  0.123;
+          12.73, 15.59,  0.000;
+          14.54, 15.22,  0.000;
+          16.36, 14.81,  0.000;
+          18.18, 14.18,  0.000;
+          20.00, 13.55,  0.000;
+          21.82, 12.99,  0.000;
+          23.63, 12.43,  0.000;
+          25.45, 11.89,  0.000;
+          27.27, 11.36,  0.000;
+          29.09, 10.84,  0.000;
+          30.91, 10.33,  0.000;
+          32.72,  9.82,  0.000;
+          34.54,  9.31,  0.000;
+          36.36,  8.80,  0.000;
+          38.18,  8.24,  0.000;
+          40.00,  7.68,  0.000;
+          41.81,  7.03,  0.000;
+          43.63,  6.37,  0.000;
+          45.45,  5.72,  0.000;
+          47.27,  5.06,  0.000;
+          49.09,  4.44,  0.000;
+          50.90,  3.83,  0.000;
+          52.72,  3.09,  0.000]
+      "maximum and minimum boundaries of pump (Q,Hmax,Hmin)",
+    maxMinSpeedCurves = [
+           0.00, 3226,  534;
+           1.82, 3186,  542;
+           3.64, 3146,  551;
+           5.45, 3121,  551;
+           7.27, 3100,  549;
+           9.09, 3085,  536;
+          10.91, 3073,  515;
+          12.73, 3047,  549;
+          14.54, 2996,  549;
+          16.36, 2946,  549;
+          18.18, 2896,  549;
+          20.00, 2846,  549;
+          21.82, 2806,  549;
+          23.63, 2765,  549;
+          25.45, 2725,  549;
+          27.27, 2685,  549;
+          29.09, 2656,  549;
+          30.91, 2635,  549;
+          32.72, 2610,  549;
+          34.54, 2579,  549;
+          36.36, 2550,  549;
+          38.18, 2530,  549;
+          40.00, 2509,  549;
+          41.81, 2488,  549;
+          43.63, 2467,  549;
+          45.45, 2461,  549;
+          47.27, 2460,  549;
+          49.09, 2446,  549;
+          50.90, 2425,  549;
+          52.72, 2391,  549]
+      "maximum and minimum boundaries of pump speed (Q,nMax,nMin)",
+    nMin=500,
+    nMax=3200,
+    cHQN=[ 0.00000e+00,  0.00000e+00,  1.52394e-06;
+           0.00000e+00,  5.07893e-05,  0.00000e+00;
+          -4.42148e-03,  0.00000e+00,  0.00000e+00]
+       "coefficients for H = f(Q,N)",
+    cPQN=[ 8.61711e+01, -3.19500e-01,  3.36762e-04, -1.12746e-07,  1.59435e-11;
+           0.00000e+00,  0.00000e+00,  4.33938e-06,  0.00000e+00,  0.00000e+00;
+           0.00000e+00,  5.09522e-05,  0.00000e+00,  0.00000e+00,  0.00000e+00;
+          -4.54214e-03,  0.00000e+00,  0.00000e+00,  0.00000e+00,  0.00000e+00]
+       "coefficients for P = f(Q,N)");
+
+      annotation(preferredView="text", Documentation(revisions="<html><ul>
+
+  <li>2023-10-19 by Sarah Leidolf:<br/>
+    Generated
+  </li>
+</ul>
+
+</html>", info="<html><h4>
+  Measurement and Regression Data
+</h4>
+<p>
+  Impure curves at high pump speed because of inaccurate data of upper
+  and lower limit of pump speed.
+</p>
+<p>
+  <img src=
+  \"modelica://AixLib/Resources/Images/DataBase/Pumps/PumpsPolynomialBased/Pump_DN50_H05_16.png\"
+  alt=\"1\">
+
+</p>
+<p>
+  cHQN:
+</p>
+<p>
+
+  <span style=\"font-family: Courier New;\">0.00000e+00, 0.00000e+00,
+  1.52394e-06;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 5.07893e-05,
+  0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-4.42148e-03, 0.00000e+00,
+  0.00000e+000</span>
+
+</p>
+<p>
+  cPQN:
+</p>
+<p>
+
+  <span style=\"font-family: Courier New;\">8.61711e+01, -3.19500e-01,
+  3.36762e-04, -1.12746e-07, 1.59435e-11;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 0.00000e+00,
+  4.33938e-06, 0.00000e+00, 0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 5.09522e-05,
+  0.00000e+00, 0.00000e+00, 0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-4.54214e-03, 0.00000e+00,
+  0.00000e+00, 0.00000e+00, 0.00000e+00</span>
+
+</p>
+</html>"));
+
+end Pump_DN50_H05_16;
diff --git a/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN50_H1_10.mo b/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN50_H1_10.mo
new file mode 100644
index 0000000000..e832a4cbc5
--- /dev/null
+++ b/AixLib/DataBase/Pumps/PumpPolynomialBased/Pump_DN50_H1_10.mo
@@ -0,0 +1,141 @@
+within AixLib.DataBase.Pumps.PumpPolynomialBased;
+record Pump_DN50_H1_10 "Pump with head 1 to 10.8m and 11.5m^3/h volume flow (Wilo Stratos 50/1-10)"
+ extends PumpBaseRecord(
+     maxMinHeight=[
+           0.00, 10.26,  0.900;
+           0.38, 10.32,  0.909;
+           0.76, 10.37,  0.918;
+           1.14, 10.43,  0.928;
+           1.52, 10.49,  0.937;
+           1.90, 10.55,  0.946;
+           2.28, 10.60,  0.850;
+           2.66, 10.64,  0.712;
+           3.03, 10.68,  0.574;
+           3.41, 10.44,  0.435;
+           3.79,  9.96,  0.297;
+           4.17,  9.46,  0.000;
+           4.55,  8.95,  0.000;
+           4.93,  8.44,  0.000;
+           5.31,  7.94,  0.000;
+           5.69,  7.47,  0.000;
+           6.07,  7.01,  0.000;
+           6.45,  6.58,  0.000;
+           6.83,  6.15,  0.000;
+           7.21,  5.74,  0.000;
+           7.59,  5.34,  0.000;
+           7.97,  4.94,  0.000;
+           8.34,  4.48,  0.000;
+           8.72,  4.00,  0.000;
+           9.10,  3.54,  0.000;
+           9.48,  3.08,  0.000;
+           9.86,  2.63,  0.000;
+          10.24,  2.11,  0.000;
+          10.62,  1.55,  0.000;
+          11.00,  1.00,  0.000]
+      "maximum and minimum boundaries of pump (Q,Hmax,Hmin)",
+    maxMinSpeedCurves = [
+          0.00, 4450, 1400;
+           0.40, 4450, 1400;
+           0.79, 4450, 1400;
+           1.19, 4450, 1400;
+           1.59, 4450, 1400;
+           1.98, 4450, 1400;
+           2.38, 4450, 1400;
+           2.78, 4450, 1400;
+           3.17, 4450, 1400;
+           3.57, 4431, 1400;
+           3.97, 4411, 1400;
+           4.36, 4381, 1400;
+           4.76, 4349, 1400;
+           5.16, 4318, 1400;
+           5.55, 4286, 1400;
+           5.95, 4254, 1400;
+           6.34, 4224, 1400;
+           6.74, 4195, 1400;
+           7.14, 4164, 1400;
+           7.53, 4131, 1400;
+           7.93, 4098, 1400;
+           8.33, 4065, 1400;
+           8.72, 4033, 1400;
+           9.12, 4001, 1400;
+           9.52, 3969, 1400;
+           9.91, 3937, 1400;
+          10.31, 3905, 1400;
+          10.71, 3873, 1400;
+          11.10, 3846, 1400;
+          11.50, 3830, 1400]
+      "maximum and minimum boundaries of pump speed (Q,nMax,nMin)",
+    nMin=1400,
+    nMax=4450,
+    cHQN=[0.00000e+00,  0.00000e+00,  5.29109e-07;
+           0.00000e+00,  1.41007e-04, -2.69160e-08;
+          -6.78540e-02,  0.00000e+00,  0.00000e+00]
+       "coefficients for H = f(Q,N)",
+    cPQN=[1.27173e+00,  2.83414e-02, -3.32976e-05,  1.37583e-08, -1.49621e-12;
+           3.36126e+01, -2.82618e-02,  6.76678e-06,  0.00000e+00,  0.00000e+00;
+          -7.91039e+00,  8.00678e-03, -1.65276e-06,  0.00000e+00,  0.00000e+00;
+          -4.10723e-01,  0.00000e+00,  2.94088e-08,  0.00000e+00,  0.00000e+00]
+       "coefficients for P = f(Q,N)");
+
+      annotation(preferredView="text", Documentation(revisions="<html><ul>
+
+  <li>2023-10-19 by Sarah Leidolf:<br/>
+    Generated
+  </li>
+</ul>
+
+</html>", info="<html><h4>
+  Measurement and Regression Data
+</h4>
+<p>
+  Dimension estimate, but inaccuracies occur due to lack of information
+  in the data sheets.
+</p>
+<p>
+  Espacially because of missing information of upper and lower limit of
+  pump speed.
+</p>
+<p>
+  <img src=
+  \"modelica://AixLib/Resources/Images/DataBase/Pumps/PumpsPolynomialBased/Pump_DN50_H1_10.png\"
+  alt=\"1\">
+</p>
+<p>
+  cHQN:
+</p>
+<p>
+
+  <span style=\"font-family: Courier New;\">0.00000e+00, 0.00000e+00,
+  5.29109e-07;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">0.00000e+00, 1.41007e-04,
+  -2.69160e-08;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-6.78540e-02, 0.00000e+00,
+  0.00000e+00</span>
+
+</p>
+<p>
+  cPQN:
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">1.27173e+00, 2.83414e-02,
+  -3.32976e-05, 1.37583e-08, -1.49621e-12;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">3.36126e+01, -2.82618e-02,
+  6.76678e-06, 0.00000e+00, 0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-7.91039e+00, 8.00678e-03,
+  -1.65276e-06, 0.00000e+00, 0.00000e+00;</span>
+</p>
+<p>
+  <span style=\"font-family: Courier New;\">-4.10723e-01, 0.00000e+00,
+  2.94088e-08, 0.00000e+00, 0.00000e+00</span>
+
+</p>
+</html>"));
+end Pump_DN50_H1_10;
diff --git a/AixLib/DataBase/Pumps/PumpPolynomialBased/package.order b/AixLib/DataBase/Pumps/PumpPolynomialBased/package.order
index ccd0aca633..74b86c5975 100644
--- a/AixLib/DataBase/Pumps/PumpPolynomialBased/package.order
+++ b/AixLib/DataBase/Pumps/PumpPolynomialBased/package.order
@@ -2,11 +2,13 @@ PumpBaseRecord
 Pump_DN100
 Pump_DN100_H1_17
 Pump_DN200
+Pump_DN25_H05_12
 Pump_DN25_H1_4_V3
 Pump_DN25_H1_6_V4
 Pump_DN25_H1_6_V8
 Pump_DN25_H1_8_V5
 Pump_DN25_H1_8_V9
+Pump_DN30_H1_12
 Pump_DN30_H1_12_V13
 Pump_DN32
 Pump_DN40
@@ -16,7 +18,9 @@ Pump_DN40_H1_16_V29
 Pump_DN40_H1_45
 Pump_DN40_H1_8_V17
 Pump_DN50
+Pump_DN50_H05_16
 Pump_DN50_H10
+Pump_DN50_H1_10
 Pump_DN50_H1_38
 Pump_DN50_H1_9_V29
 Pump_DN65
diff --git a/AixLib/DataBase/SolarElectric/PVBaseDataDefinition.mo b/AixLib/DataBase/SolarElectric/PVBaseDataDefinition.mo
new file mode 100644
index 0000000000..df4f7b8170
--- /dev/null
+++ b/AixLib/DataBase/SolarElectric/PVBaseDataDefinition.mo
@@ -0,0 +1,57 @@
+within AixLib.DataBase.SolarElectric;
+record PVBaseDataDefinition "Basic record of a PV module"
+   extends Modelica.Icons.Record;
+
+  parameter Modelica.Units.SI.Efficiency eta_0
+    "Efficiency under standard conditions. If not found in data sheet, use eta_0 = ((V_mp0*I_mp0)/(1000*A_cel*n_ser))"
+    annotation (Dialog(group="General"));
+   parameter Real n_ser
+      "Number of cells connected in series on the PV panel"
+      annotation(Dialog(group="General"));
+   parameter Real n_par
+      "Number of parallel cell circuits on the PV panel"
+      annotation(Dialog(group="General"));
+  parameter Modelica.Units.SI.Area A_cel
+    "Area of a single cell. If not found in data sheet, use A_cel = ((V_mp0*I_mp0)/(1000*eta_0))/n_ser"
+    annotation (Dialog(group="Cell specific: Geometrical data"));
+  parameter Modelica.Units.SI.Area A_pan=A_cel*n_ser*n_par
+    "Area of one Panel, must not be confused with area of the whole module"
+    annotation (Dialog(group="Cell specific: Geometrical data"));
+  parameter Modelica.Units.SI.Area A_mod "Area of one module (housing)"
+    annotation (Dialog(group="Cell specific: Geometrical data"));
+  parameter Modelica.Units.SI.Voltage V_oc0
+    "Open circuit voltage under standard conditions"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+  parameter Modelica.Units.SI.ElectricCurrent I_sc0
+    "Short circuit current under standard conditions"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+  parameter Modelica.Units.SI.Voltage V_mp0
+    "MPP voltage under standard conditions"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+  parameter Modelica.Units.SI.ElectricCurrent I_mp0
+    "MPP current under standard conditions"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+  parameter Modelica.Units.SI.Power P_mp0
+    "MPP power of one PV module under standard conditions"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+   parameter Real TCoeff_Isc(unit = "A/K")
+      "Temperature coefficient for short circuit current, >0. If not found in data sheet, use TCoeff_Isc=alpha_Isc*I_sc0 and type in alpha_Isc manually"
+      annotation(Dialog(group="Cell specific: Electrical characteristics"));
+   parameter Real TCoeff_Voc(unit = "V/K")
+      "Temperature coefficient for open circuit voltage, <0. If not found in data sheet, use TCoeff_Voc=beta_Voc*V_oc0 and type in beta_Voc manually"
+      annotation(Dialog(group="Cell specific: Electrical characteristics"));
+  parameter Modelica.Units.SI.LinearTemperatureCoefficient alpha_Isc=TCoeff_Isc
+      /I_sc0 "Normalized temperature coefficient for short circuit current, >0"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+  parameter Modelica.Units.SI.LinearTemperatureCoefficient beta_Voc=TCoeff_Voc/
+      V_oc0 "Normalized temperature coefficient for open circuit voltage, <0"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+  parameter Modelica.Units.SI.LinearTemperatureCoefficient gamma_Pmp
+    "Normalized temperature coefficient for power at MPP"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+  parameter Modelica.Units.SI.Temperature T_NOCT
+    "Cell temperature under NOCT conditions"
+    annotation (Dialog(group="Cell specific: Electrical characteristics"));
+    annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(coordinateSystem(
+            preserveAspectRatio=false)));
+end PVBaseDataDefinition;
\ No newline at end of file
diff --git a/AixLib/DataBase/SolarElectric/QPlusBFRG41285.mo b/AixLib/DataBase/SolarElectric/QPlusBFRG41285.mo
new file mode 100644
index 0000000000..a69c4bfeca
--- /dev/null
+++ b/AixLib/DataBase/SolarElectric/QPlusBFRG41285.mo
@@ -0,0 +1,33 @@
+within AixLib.DataBase.SolarElectric;
+record QPlusBFRG41285 "Q.Plus BFR-G4.1 285"
+   extends AixLib.DataBase.SolarElectric.PVBaseDataDefinition(
+     n_ser=60,
+     n_par=1,
+     A_cel=((V_mp0*I_mp0)/(1000*eta_0))/n_ser,
+     A_mod=1.000*1.670,
+     eta_0=0.171,
+     V_oc0=39.22,
+     I_sc0=9.46,
+     V_mp0=31.99,
+     I_mp0=8.91,
+     P_mp0=285,
+     TCoeff_Isc=0.0004*I_sc0,
+     TCoeff_Voc=-0.0029*V_oc0,
+     gamma_Pmp=-0.004,
+     T_NOCT=45+273.15);
+    annotation (Documentation(info="<html><h4>
+  <span style=\"color: #008000\">References</span>
+</h4>
+<p>
+  Record for record used with AixLib.Fluid.Solar.Electric.PVsystem
+</p>
+</html>",
+        revisions="<html><ul>
+  <li>
+    <i>May 6, 2021</i> by Laura Maier:<br/>
+    Adapted record which is also used in research project FUBIC
+    suppored by the BMWi (promotional reference: 03ET1619)
+  </li>
+</ul>
+</html>"));
+end QPlusBFRG41285;
diff --git a/AixLib/DataBase/SolarElectric/package.mo b/AixLib/DataBase/SolarElectric/package.mo
index 9e9efa6a13..d25a925831 100644
--- a/AixLib/DataBase/SolarElectric/package.mo
+++ b/AixLib/DataBase/SolarElectric/package.mo
@@ -1,92 +1,4 @@
 within AixLib.DataBase;
 package SolarElectric
-  record PVBaseDataDefinition "Basic record of a PV module"
-   extends Modelica.Icons.Record;
-
-  parameter Modelica.Units.SI.Efficiency eta_0
-    "Efficiency under standard conditions. If not found in data sheet, use eta_0 = ((V_mp0*I_mp0)/(1000*A_cel*n_ser))"
-    annotation (Dialog(group="General"));
-   parameter Real n_ser
-      "Number of cells connected in series on the PV panel"
-      annotation(Dialog(group="General"));
-   parameter Real n_par
-      "Number of parallel cell circuits on the PV panel"
-      annotation(Dialog(group="General"));
-  parameter Modelica.Units.SI.Area A_cel
-    "Area of a single cell. If not found in data sheet, use A_cel = ((V_mp0*I_mp0)/(1000*eta_0))/n_ser"
-    annotation (Dialog(group="Cell specific: Geometrical data"));
-  parameter Modelica.Units.SI.Area A_pan=A_cel*n_ser*n_par
-    "Area of one Panel, must not be confused with area of the whole module"
-    annotation (Dialog(group="Cell specific: Geometrical data"));
-  parameter Modelica.Units.SI.Area A_mod "Area of one module (housing)"
-    annotation (Dialog(group="Cell specific: Geometrical data"));
-  parameter Modelica.Units.SI.Voltage V_oc0
-    "Open circuit voltage under standard conditions"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-  parameter Modelica.Units.SI.ElectricCurrent I_sc0
-    "Short circuit current under standard conditions"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-  parameter Modelica.Units.SI.Voltage V_mp0
-    "MPP voltage under standard conditions"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-  parameter Modelica.Units.SI.ElectricCurrent I_mp0
-    "MPP current under standard conditions"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-  parameter Modelica.Units.SI.Power P_mp0
-    "MPP power of one PV module under standard conditions"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-   parameter Real TCoeff_Isc(unit = "A/K")
-      "Temperature coefficient for short circuit current, >0. If not found in data sheet, use TCoeff_Isc=alpha_Isc*I_sc0 and type in alpha_Isc manually"
-      annotation(Dialog(group="Cell specific: Electrical characteristics"));
-   parameter Real TCoeff_Voc(unit = "V/K")
-      "Temperature coefficient for open circuit voltage, <0. If not found in data sheet, use TCoeff_Voc=beta_Voc*V_oc0 and type in beta_Voc manually"
-      annotation(Dialog(group="Cell specific: Electrical characteristics"));
-  parameter Modelica.Units.SI.LinearTemperatureCoefficient alpha_Isc=TCoeff_Isc
-      /I_sc0 "Normalized temperature coefficient for short circuit current, >0"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-  parameter Modelica.Units.SI.LinearTemperatureCoefficient beta_Voc=TCoeff_Voc/
-      V_oc0 "Normalized temperature coefficient for open circuit voltage, <0"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-  parameter Modelica.Units.SI.LinearTemperatureCoefficient gamma_Pmp
-    "Normalized temperature coefficient for power at MPP"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-  parameter Modelica.Units.SI.Temperature T_NOCT
-    "Cell temperature under NOCT conditions"
-    annotation (Dialog(group="Cell specific: Electrical characteristics"));
-    annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(coordinateSystem(
-            preserveAspectRatio=false)));
-  end PVBaseDataDefinition;
-
-  record QPlusBFRG41285 "Q.Plus BFR-G4.1 285"
-   extends AixLib.DataBase.SolarElectric.PVBaseDataDefinition(
-     n_ser=60,
-     n_par=1,
-     A_cel=((V_mp0*I_mp0)/(1000*eta_0))/n_ser,
-     A_mod=1.000*1.670,
-     eta_0=0.171,
-     V_oc0=39.22,
-     I_sc0=9.46,
-     V_mp0=31.99,
-     I_mp0=8.91,
-     P_mp0=285,
-     TCoeff_Isc=0.0004*I_sc0,
-     TCoeff_Voc=-0.0029*V_oc0,
-     gamma_Pmp=-0.004,
-     T_NOCT=45+273.15);
-    annotation (Documentation(info="<html><h4>
-  <span style=\"color: #008000\">References</span>
-</h4>
-<p>
-  Record for record used with AixLib.Fluid.Solar.Electric.PVsystem
-</p>
-</html>",
-        revisions="<html><ul>
-  <li>
-    <i>May 6, 2021</i> by Laura Maier:<br/>
-    Adapted record which is also used in research project FUBIC
-    suppored by the BMWi (promotional reference: 03ET1619)
-  </li>
-</ul>
-</html>"));
-  end QPlusBFRG41285;
+  
 end SolarElectric;
diff --git a/AixLib/DataBase/SolarElectric/package.order b/AixLib/DataBase/SolarElectric/package.order
index c2dea74488..e73f8bcf0b 100644
--- a/AixLib/DataBase/SolarElectric/package.order
+++ b/AixLib/DataBase/SolarElectric/package.order
@@ -1,7 +1,7 @@
 AleoS24185
 CanadianSolarCS6P250P
+PVBaseDataDefinition
+QPlusBFRG41285
 SchuecoSPV170SME1
 SharpNUU235F2
 ShellSP70
-PVBaseDataDefinition
-QPlusBFRG41285
diff --git a/AixLib/DataBase/Storage/Generic_New_2000l.mo b/AixLib/DataBase/Storage/Generic_New_2000l.mo
index d6164365a7..7b463457b3 100644
--- a/AixLib/DataBase/Storage/Generic_New_2000l.mo
+++ b/AixLib/DataBase/Storage/Generic_New_2000l.mo
@@ -1,6 +1,6 @@
 within AixLib.DataBase.Storage;
 record Generic_New_2000l "Pseudo storage with 2000 l (standing)"
-  extends BufferStorageBaseDataDefinition(
+  extends StorageDetailedBaseDataDefinition(
     hTank=2.145,
     hLowerPortDemand=0.1,
     hUpperPortDemand=2.1,
diff --git a/AixLib/DataBase/Storage/BufferStorageBaseDataDefinition.mo b/AixLib/DataBase/Storage/StorageDetailedBaseDataDefinition.mo
similarity index 51%
rename from AixLib/DataBase/Storage/BufferStorageBaseDataDefinition.mo
rename to AixLib/DataBase/Storage/StorageDetailedBaseDataDefinition.mo
index 3497fd1ccf..41f765953c 100644
--- a/AixLib/DataBase/Storage/BufferStorageBaseDataDefinition.mo
+++ b/AixLib/DataBase/Storage/StorageDetailedBaseDataDefinition.mo
@@ -1,35 +1,34 @@
 within AixLib.DataBase.Storage;
-record BufferStorageBaseDataDefinition
+record StorageDetailedBaseDataDefinition
   "Base data definition for Buffer storage records"
   extends Modelica.Icons.Record;
 ///////////input parameters////////////
-  import      Modelica.Units.SI;
-  parameter SI.Height hTank "Height of storage";
-  parameter SI.Height hLowerPortDemand "Height of lower demand port";
-  parameter SI.Height hUpperPortDemand "Height of upper demand port";
-  parameter SI.Height hLowerPortSupply "Height of lower supply port";
-  parameter SI.Height hUpperPortSupply "Height of upper supply port";
-  parameter SI.Height hHC1Up "Height of heating Coil";
-  parameter SI.Height hHC1Low "Height of heating Coil";
-  parameter SI.Height hHC2Up "Height of heating Coil";
-  parameter SI.Height hHC2Low "Height of heating Coil";
-  parameter SI.Height hHR "Height of heating Rod";
-  parameter SI.Diameter dTank "Inner diameter of storage";
-  parameter SI.Length sWall "Thickness of storage Wall";
-  parameter SI.Length sIns "Thickness of storage insulation";
+  parameter Modelica.Units.SI.Height hTank "Height of storage";
+  parameter Modelica.Units.SI.Height hLowerPortDemand "Height of lower demand port";
+  parameter Modelica.Units.SI.Height hUpperPortDemand "Height of upper demand port";
+  parameter Modelica.Units.SI.Height hLowerPortSupply "Height of lower supply port";
+  parameter Modelica.Units.SI.Height hUpperPortSupply "Height of upper supply port";
+  parameter Modelica.Units.SI.Height hHC1Up "Height of heating Coil";
+  parameter Modelica.Units.SI.Height hHC1Low "Height of heating Coil";
+  parameter Modelica.Units.SI.Height hHC2Up "Height of heating Coil";
+  parameter Modelica.Units.SI.Height hHC2Low "Height of heating Coil";
+  parameter Modelica.Units.SI.Height hHR "Height of heating Rod";
+  parameter Modelica.Units.SI.Diameter dTank "Inner diameter of storage";
+  parameter Modelica.Units.SI.Length sWall "Thickness of storage Wall";
+  parameter Modelica.Units.SI.Length sIns "Thickness of storage insulation";
   parameter Modelica.Units.SI.ThermalConductivity lambdaWall
     "thermal conductivity of storage wall";
   parameter Modelica.Units.SI.ThermalConductivity lambdaIns
     "thermal conductivity of storage insulation";
   //parameter SI.CoefficientOfHeatTransfer alpha
     //"Coefficient of heat transfer air <-> insulation of tank";
-  parameter SI.Length hTS1 "Height of lower temperature sensor";
-  parameter SI.Length hTS2 "Height of upper temperature sensor";
-  parameter SI.Density rhoIns "Density of insulation";
-  parameter SI.SpecificHeatCapacity cIns "Heat capacity of insulation";
-  parameter SI.Density rhoWall "Density of wall";
-  parameter SI.SpecificHeatCapacity cWall "Heat capacity of wall";
-  parameter SI.Length roughness "Inner roughness of storage wall";
+  parameter Modelica.Units.SI.Length hTS1 "Height of lower temperature sensor";
+  parameter Modelica.Units.SI.Length hTS2 "Height of upper temperature sensor";
+  parameter Modelica.Units.SI.Density rhoIns "Density of insulation";
+  parameter Modelica.Units.SI.SpecificHeatCapacity cIns "Heat capacity of insulation";
+  parameter Modelica.Units.SI.Density rhoWall "Density of wall";
+  parameter Modelica.Units.SI.SpecificHeatCapacity cWall "Heat capacity of wall";
+  parameter Modelica.Units.SI.Length roughness "Inner roughness of storage wall";
 
   // Heat exchanger Pipes
 
@@ -72,4 +71,4 @@ record BufferStorageBaseDataDefinition
   </li>
 </ul>
 </html>"));
-end BufferStorageBaseDataDefinition;
+end StorageDetailedBaseDataDefinition;
diff --git a/AixLib/DataBase/Storage/package.order b/AixLib/DataBase/Storage/package.order
index 39c4070da7..77109571c1 100644
--- a/AixLib/DataBase/Storage/package.order
+++ b/AixLib/DataBase/Storage/package.order
@@ -1,2 +1,2 @@
-BufferStorageBaseDataDefinition
 Generic_New_2000l
+StorageDetailedBaseDataDefinition
diff --git a/AixLib/DataBase/ThermalZones/SwimmingFacility/Changing.mo b/AixLib/DataBase/ThermalZones/SwimmingFacility/Changing.mo
new file mode 100644
index 0000000000..2b198bb15f
--- /dev/null
+++ b/AixLib/DataBase/ThermalZones/SwimmingFacility/Changing.mo
@@ -0,0 +1,95 @@
+within AixLib.DataBase.ThermalZones.SwimmingFacility;
+record Changing "Swimming facility - Changing rooms"
+  extends AixLib.DataBase.ThermalZones.ZoneBaseRecord(
+    T_start = 299.15,
+    withAirCap = true,
+    VAir = 963.9,
+    AZone = 267.75,
+    hRad = 5.0,
+    lat = 0.88645272708792,
+    nOrientations = 4,
+    AWin = {0.001, 0.001, 0.001, 15.819999999999999},
+    ATransparent = {0.001, 0.001, 0.001, 15.819999999999999},
+    hConWin = 2.6999999999999997,
+    RWin = 0.06832339512615061,
+    gWin = 0.67,
+    UWin= 0.7993916878977316,
+    ratioWinConRad = 0.029999999999999995,
+    AExt = {0.001, 0.001, 27.625, 102.375},
+    hConExt = 2.6999999999999997,
+    nExt = 1,
+    RExt = {0.00032814117663926046},
+    RExtRem = 0.031521067523942944,
+    CExt = {52866706.08494557},
+    AInt = 78.8125,
+    hConInt = 2.7,
+    nInt = 1,
+    RInt = {0.002527733856125566},
+    CInt = {10121920.163930776},
+    AFloor = 267.75,
+    hConFloor = 1.7000000000000002,
+    nFloor = 1,
+    RFloor = {0.0002447814807941062},
+    RFloorRem =  0.009559540982521146,
+    CFloor = {138546109.20531926},
+    ARoof = 267.75,
+    hConRoof = 1.7000000000000002,
+    nRoof = 1,
+   RRoof = {0.0001075568636157786},
+    RRoofRem = 0.02396280906053166,
+    CRoof = {8024305.002921475},
+    nOrientationsRoof = 1,
+    tiltRoof = {0.0},
+    aziRoof = {0.0},
+    wfRoof = {1.0},
+    aRoof = 0.5,
+    aExt = 0.5,
+    TSoil = 286.15,
+    hConWallOut = 20.0,
+    hRadWall = 5.0,
+    hConWinOut = 19.999999999999996,
+    hConRoofOut = 20.000000000000004,
+    hRadRoof = 5.0,
+    tiltExtWalls = {1.5707963267948966, 1.5707963267948966, 1.5707963267948966, 1.5707963267948966},
+    aziExtWalls = {0.0, 1.5707963267948966, -1.5707963267948966, 3.141592653589793},
+    wfWall = {7.692189350933062e-06, 7.692189350933062e-06, 0.2124967308195258, 0.7874878848017722},
+    wfWin = {6.319914049168934e-05, 6.319914049168934e-05, 6.319914049168934e-05, 0.9998104025785252},
+    wfGro = 0.0,
+    specificPeople = 0.07142857142857142,
+    internalGainsMoistureNoPeople = 0.5,
+    fixedHeatFlowRatePersons = 70,
+    activityDegree = 1.2,
+    ratioConvectiveHeatPeople = 0.5,
+    internalGainsMachinesSpecific = 7.0,
+    ratioConvectiveHeatMachines = 0.75,
+    lightingPowerSpecific = 12.5,
+    ratioConvectiveHeatLighting = 0.9,
+    useConstantACHrate = true,
+    baseACH = 0.5,
+    maxUserACH = 1.0,
+    maxOverheatingACH = {3.0, 2.0},
+    maxSummerACH = {1.0, 283.15, 290.15},
+    winterReduction = {0.2, 273.15, 283.15},
+    maxIrr = {100.0, 100.0, 100.0, 100.0},
+    shadingFactor = {1.0, 1.0, 1.0, 1.0},
+    withAHU = true,
+    minAHU = 0.0,
+    maxAHU = 2.6,
+    hHeat = 100000.0,
+    lHeat = 0,
+    KRHeat = 10000,
+    TNHeat = 300,
+    HeaterOn = false,
+    hCool = 0,
+    lCool = -100000.0,
+    KRCool = 10000,
+    TNCool = 1,
+    heaLoadFacOut=0,
+    heaLoadFacGrd=0,
+    CoolerOn = false,
+    withIdealThresholds = false,
+    TThresholdHeater = 288.15,
+    TThresholdCooler = 295.15);
+   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end Changing;
diff --git a/AixLib/DataBase/ThermalZones/SwimmingFacility/Entrance.mo b/AixLib/DataBase/ThermalZones/SwimmingFacility/Entrance.mo
new file mode 100644
index 0000000000..4f2370237a
--- /dev/null
+++ b/AixLib/DataBase/ThermalZones/SwimmingFacility/Entrance.mo
@@ -0,0 +1,95 @@
+within AixLib.DataBase.ThermalZones.SwimmingFacility;
+record Entrance "Swimming facility - Entrance hall"
+   extends AixLib.DataBase.ThermalZones.ZoneBaseRecord(
+    T_start = 294.15,
+    withAirCap = true,
+    VAir = 1528.3,
+    AZone = 246.5,
+    hRad = 5.0,
+    lat = 0.88645272708792,
+    nOrientations = 4,
+    AWin = {0.001, 0.001, 172.25, 0.001},
+    ATransparent = {0.001, 0.001, 172.25, 0.001},
+    hConWin = 2.6999999999999997,
+    RWin = 0.006276123382937199,
+    gWin = 0.67,
+    UWin= 0.7993916878977319,
+    ratioWinConRad = 0.029999999999999992,
+    AExt = {0.001, 0.001, 188.5, 0.001},
+    hConExt = 2.7,
+    nExt = 1,
+    RExt = {0.00022630413969781447},
+    RExtRem = 0.021738655725625746,
+    CExt = {76656764.48924243},
+    AInt = 135.25300000000001,
+    hConInt = 2.7,
+    nInt = 1,
+    RInt = {0.0014729212996081136},
+    CInt = {17370595.62800481},
+    AFloor = 246.5,
+    hConFloor = 1.7000000000000002,
+    nFloor = 1,
+    RFloor = {0.0002658833325867016},
+    RFloorRem =  0.010383639343083312,
+    CFloor = {127550386.25251614},
+    ARoof = 246.5,
+    hConRoof = 1.7000000000000002,
+    nRoof = 1,
+    RRoof = {0.00011682900703093194},
+    RRoofRem = 0.026028568462301633,
+    CRoof = {7387455.399515009},
+    nOrientationsRoof = 1,
+    tiltRoof = {0.0},
+    aziRoof = {0.0},
+    wfRoof = {1.0},
+    aRoof = 0.5,
+    aExt = 0.5,
+    TSoil = 286.15,
+    hConWallOut = 20.0,
+    hRadWall = 5.0,
+    hConWinOut = 19.999999999999996,
+    hConRoofOut = 20.000000000000007,
+    hRadRoof = 5.0,
+    tiltExtWalls = {1.5707963267948966, 1.5707963267948966, 1.5707963267948966, 1.5707963267948966},
+    aziExtWalls = {0.0, 1.5707963267948966, -1.5707963267948966, 3.141592653589793},
+    wfWall = {5.304955358800656e-06, 5.304955358800656e-06, 0.9999840851339238, 5.304955358800656e-06},
+    wfWin = {5.805414129216908e-06, 5.805414129216908e-06, 0.9999825837576122, 5.805414129216908e-06},
+    wfGro = 0.0,
+    specificPeople = 0.08333333333333333,
+    internalGainsMoistureNoPeople = 0.5,
+    fixedHeatFlowRatePersons = 70,
+    activityDegree = 1.2,
+    ratioConvectiveHeatPeople = 0.5,
+    internalGainsMachinesSpecific = 0.0,
+    ratioConvectiveHeatMachines = 0.75,
+    lightingPowerSpecific = 4.4,
+    ratioConvectiveHeatLighting = 0.9,
+    useConstantACHrate = false,
+    baseACH = 0.5,
+    maxUserACH = 1.0,
+    maxOverheatingACH = {3.0, 2.0},
+    maxSummerACH = {1.0, 283.15, 290.15},
+    winterReduction = {0.2, 273.15, 283.15},
+    maxIrr = {100.0, 100.0, 100.0, 100.0},
+    shadingFactor = {1.0, 1.0, 1.0, 1.0},
+    withAHU = true,
+    minAHU = 0.0,
+    maxAHU = 0.0,
+    hHeat = 100000.0,
+    lHeat = 0,
+    KRHeat = 10000,
+    TNHeat = 300,
+    HeaterOn = false,
+    hCool = 0,
+    lCool = -100000.0,
+    KRCool = 10000,
+    TNCool = 1,
+    heaLoadFacOut=0,
+    heaLoadFacGrd=0,
+    CoolerOn = false,
+    withIdealThresholds = false,
+    TThresholdHeater = 288.15,
+    TThresholdCooler = 295.15);
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end Entrance;
diff --git a/AixLib/DataBase/ThermalZones/SwimmingFacility/Showers.mo b/AixLib/DataBase/ThermalZones/SwimmingFacility/Showers.mo
new file mode 100644
index 0000000000..0ff35e007b
--- /dev/null
+++ b/AixLib/DataBase/ThermalZones/SwimmingFacility/Showers.mo
@@ -0,0 +1,95 @@
+within AixLib.DataBase.ThermalZones.SwimmingFacility;
+record Showers "Swimming facility - Showers and other sanitary areas"
+   extends AixLib.DataBase.ThermalZones.ZoneBaseRecord(
+    T_start = 301.15,
+    withAirCap = true,
+    VAir = 819.0,
+    AZone = 252.0,
+    hRad = 5.0,
+    lat = 0.88645272708792,
+    nOrientations = 4,
+    AWin = {0.001, 0.001, 0.001, 0.001},
+    ATransparent = {0.001, 0.001, 0.001, 0.001},
+    hConWin = 2.7,
+    RWin = 270.27027027027026,
+    gWin = 0.67,
+    UWin= 0.7993916878977319,
+    ratioWinConRad = 0.03,
+    AExt = {0.001, 0.001, 0.001, 0.001},
+    hConExt = 2.7,
+    nExt = 1,
+    RExt = {10.664752311364285},
+    RExtRem = 1024.4504550619076,
+    CExt = {1626.642854262106},
+    AInt = 388.375,
+    hConInt = 2.7,
+    nInt = 1,
+    RInt = {0.0005129501758246443},
+    CInt = {49879152.97277226},
+    AFloor = 252.0,
+    hConFloor = 1.7000000000000002,
+    nFloor = 1,
+    RFloor = {0.00026008032334373784},
+    RFloorRem =  0.010157012293928715,
+    CFloor = {130396338.07559462},
+    ARoof = 252.0,
+    hConRoof = 1.7000000000000002,
+    nRoof = 1,
+   RRoof = {0.00011427916759176477},
+    RRoofRem = 0.025460484626814887,
+    CRoof = {7552287.061573154},
+    nOrientationsRoof = 1,
+    tiltRoof = {0.0},
+    aziRoof = {0.0},
+    wfRoof = {1.0},
+    aRoof = 0.5,
+    aExt = 0.5,
+    TSoil = 286.15,
+    hConWallOut = 20.0,
+    hRadWall = 5.0,
+    hConWinOut = 20.0,
+    hConRoofOut = 20.000000000000007,
+    hRadRoof = 5.0,
+    tiltExtWalls = {1.5707963267948966, 1.5707963267948966, 1.5707963267948966, 1.5707963267948966},
+    aziExtWalls = {0.0, 1.5707963267948966, -1.5707963267948966, 3.141592653589793},
+    wfWall = {0.25, 0.25, 0.25, 0.25},
+    wfWin = {0.25, 0.25, 0.25, 0.25},
+    wfGro = 0.0,
+    specificPeople = 0.0,
+    internalGainsMoistureNoPeople = 10,
+    fixedHeatFlowRatePersons = 70,
+    activityDegree = 1.2,
+    ratioConvectiveHeatPeople = 0.5,
+    internalGainsMachinesSpecific = 0.0,
+    ratioConvectiveHeatMachines = 0.75,
+    lightingPowerSpecific = 11.1,
+    ratioConvectiveHeatLighting = 0.9,
+    useConstantACHrate = true,
+    baseACH = 0.5,
+    maxUserACH = 1.0,
+    maxOverheatingACH = {3.0, 2.0},
+    maxSummerACH = {1.0, 283.15, 290.15},
+    winterReduction = {0.2, 273.15, 283.15},
+    maxIrr = {100.0, 100.0, 100.0, 100.0},
+    shadingFactor = {1.0, 1.0, 1.0, 1.0},
+    withAHU = true,
+    minAHU = 0.0,
+    maxAHU = 8.0,
+    hHeat = 100000.0,
+    lHeat = 0,
+    KRHeat = 10000,
+    TNHeat = 300,
+    HeaterOn = false,
+    hCool = 0,
+    lCool = -100000.0,
+    KRCool = 10000,
+    TNCool = 1,
+    heaLoadFacOut=0,
+    heaLoadFacGrd=0,
+    CoolerOn = false,
+    withIdealThresholds = false,
+    TThresholdHeater = 288.15,
+    TThresholdCooler = 295.15);
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end Showers;
diff --git a/AixLib/DataBase/ThermalZones/SwimmingFacility/Supervisory.mo b/AixLib/DataBase/ThermalZones/SwimmingFacility/Supervisory.mo
new file mode 100644
index 0000000000..047572c39a
--- /dev/null
+++ b/AixLib/DataBase/ThermalZones/SwimmingFacility/Supervisory.mo
@@ -0,0 +1,95 @@
+within AixLib.DataBase.ThermalZones.SwimmingFacility;
+record Supervisory "Swimming facility - Supervisory and control rooms"
+    extends AixLib.DataBase.ThermalZones.ZoneBaseRecord(
+    T_start = 297.15,
+    withAirCap = true,
+    VAir = 68.89999999999999,
+    AZone = 21.2,
+    hRad = 4.999999999999999,
+    lat = 0.88645272708792,
+    nOrientations = 4,
+    AWin = {0.001, 0.001, 0.001, 0.001},
+    ATransparent = {0.001, 0.001, 0.001, 0.001},
+    hConWin = 2.7,
+    RWin = 270.27027027027026,
+    gWin = 0.67,
+    UWin= 0.7993916878977319,
+    ratioWinConRad = 0.03,
+    AExt = {0.001, 0.001, 0.001, 0.001},
+    hConExt = 2.7,
+    nExt = 1,
+    RExt = {10.664752311364285},
+    RExtRem = 1024.4504550619076,
+    CExt = {1626.642854262106},
+    AInt = 137.79999999999998,
+    hConInt = 2.7,
+    nInt = 1,
+    RInt = {0.0014456968398831363},
+    CInt = {17697707.833017103},
+    AFloor = 0.001,
+    hConFloor = 1.7000000000000002,
+    nFloor = 1,
+    RFloor = {65.54024148262194},
+    RFloorRem =  2559.567098070036,
+    CFloor = {517.4457860142643},
+    ARoof = 0.001,
+    hConRoof = 1.7000000000000002,
+    nRoof = 1,
+    RRoof = {28.798350233124722},
+    RRoofRem = 6416.042125957352,
+    CRoof = {29.96939310148077},
+    nOrientationsRoof = 1,
+    tiltRoof = {0.0},
+    aziRoof = {0.0},
+    wfRoof = {1.0},
+    aRoof = 0.5,
+    aExt = 0.5,
+    TSoil = 286.15,
+    hConWallOut = 20.0,
+    hRadWall = 5.0,
+    hConWinOut = 20.0,
+    hConRoofOut = 20.000000000000007,
+    hRadRoof = 5.0,
+    tiltExtWalls = {1.5707963267948966, 1.5707963267948966, 1.5707963267948966, 1.5707963267948966},
+    aziExtWalls = {0.0, 1.5707963267948966, -1.5707963267948966, 3.141592653589793},
+    wfWall = {0.25, 0.25, 0.25, 0.25},
+    wfWin = {0.25, 0.25, 0.25, 0.25},
+    wfGro = 0.0,
+    specificPeople = 0.3333333333333333,
+    internalGainsMoistureNoPeople = 0.5,
+    fixedHeatFlowRatePersons = 70,
+    activityDegree = 1.2,
+    ratioConvectiveHeatPeople = 0.5,
+    internalGainsMachinesSpecific = 2.0,
+    ratioConvectiveHeatMachines = 0.75,
+    lightingPowerSpecific = 15.9,
+    ratioConvectiveHeatLighting = 0.9,
+    useConstantACHrate = false,
+    baseACH = 0.5,
+    maxUserACH = 1.0,
+    maxOverheatingACH = {3.0, 2.0},
+    maxSummerACH = {1.0, 283.15, 290.15},
+    winterReduction = {0.2, 273.15, 283.15},
+    maxIrr = {100.0, 100.0, 100.0, 100.0},
+    shadingFactor = {1.0, 1.0, 1.0, 1.0},
+    withAHU = true,
+    minAHU = 0.0,
+    maxAHU = 12.0,
+    hHeat = 100000.0,
+    lHeat = 0,
+    KRHeat = 10000,
+    TNHeat = 300,
+    HeaterOn = false,
+    hCool = 0,
+    lCool = -100000.0,
+    KRCool = 10000,
+    TNCool = 1,
+    heaLoadFacOut=0,
+    heaLoadFacGrd=0,
+    CoolerOn = false,
+    withIdealThresholds = false,
+    TThresholdHeater = 288.15,
+    TThresholdCooler = 295.15);
+                                                                       annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end Supervisory;
diff --git a/AixLib/DataBase/ThermalZones/SwimmingFacility/SwimmingHall.mo b/AixLib/DataBase/ThermalZones/SwimmingFacility/SwimmingHall.mo
new file mode 100644
index 0000000000..db860f73f7
--- /dev/null
+++ b/AixLib/DataBase/ThermalZones/SwimmingFacility/SwimmingHall.mo
@@ -0,0 +1,115 @@
+within AixLib.DataBase.ThermalZones.SwimmingFacility;
+record SwimmingHall "Swimming facility - Swimming hall"
+  extends AixLib.DataBase.ThermalZones.ZoneBaseRecord(
+    T_start = 305.15,
+    withAirCap = true,
+    VAir = 8215.0,
+    AZone = 1325.0,
+    hRad = 4.999999999999999,
+    lat = 0.88645272708792,
+    nOrientations = 4,
+    AWin = {234.8, 154.256, 0.001, 18.6},
+    ATransparent = {234.8, 154.256, 0.001, 18.6},
+    hConWin = 2.7000000000000006,
+    RWin = 0.002651937979922045,
+    gWin = 0.67,
+    UWin= 0.7993916878977316,
+    ratioWinConRad = 0.03,
+    AExt = {267.8, 154.256, 0.001, 62.0},
+    hConExt = 2.6999999999999997,
+    nExt = 1,
+    RExt = {8.812807013524674e-05},
+    RExtRem = 0.008465535712214946,
+    CExt = {196846965.02638808},
+    AInt = 297.6,
+    hConInt = 2.7,
+    nInt = 1,
+    RInt = {0.000669412044811479},
+    CInt = {38220884.26056525},
+    AFloor = 552.0,
+    hConFloor = 1.7000000000000002,
+    nFloor = 1,
+    RFloor = {0.000118732321526489},
+    RFloorRem =  0.004636896916793544,
+    CFloor = {285630073.87987393},
+    ARoof = 1325.0,
+    hConRoof = 1.7000000000000002,
+    nRoof = 1,
+       RRoof = {2.173460394952809e-05},
+    RRoofRem = 0.004842295944118755,
+    CRoof = {39709445.85946224},
+    nOrientationsRoof = 1,
+    tiltRoof = {0.0},
+    aziRoof = {0.0},
+    wfRoof = {1.0},
+    aRoof = 0.5,
+    aExt = 0.5,
+    TSoil = 286.15,
+    hConWallOut = 20.0,
+    hRadWall = 5.0,
+    hConWinOut = 20.0,
+    hConRoofOut = 20.000000000000007,
+    hRadRoof = 5.0,
+    tiltExtWalls = {1.5707963267948966, 1.5707963267948966, 1.5707963267948966, 1.5707963267948966},
+    aziExtWalls = {0.0, 1.5707963267948966, -1.5707963267948966, 3.141592653589793},
+    wfWall = {0.5532406307521635, 0.3186732141049505, 2.0658724075883626e-06, 0.12808408927047849},
+    wfWin = {0.575974409859269, 0.37839654415354085, 2.4530426314278916e-06, 0.045626592944558786},
+    wfGro = 0.0,
+    specificPeople = 0.05,
+    internalGainsMoistureNoPeople = 0.0,
+    fixedHeatFlowRatePersons = 120,
+    activityDegree = 3.0,
+    ratioConvectiveHeatPeople = 0.5,
+    internalGainsMachinesSpecific = 0.0,
+    ratioConvectiveHeatMachines = 0.75,
+    lightingPowerSpecific = 10.5,
+    ratioConvectiveHeatLighting = 0.9,
+    useConstantACHrate = true,
+    baseACH = 0.4,
+    maxUserACH = 0.0,
+    maxOverheatingACH = {3.0, 2.0},
+    maxSummerACH = {1.0, 283.15, 290.15},
+    winterReduction = {0.2, 273.15, 283.15},
+    maxIrr = {100.0, 100.0, 100.0, 100.0},
+    shadingFactor = {1.0, 1.0, 1.0, 1.0},
+    withAHU = true,
+    minAHU = 0.0,
+    maxAHU = 174.3,
+    hHeat = 2000000.0,
+    lHeat = 0,
+    KRHeat = 10000,
+    TNHeat = 300,
+    HeaterOn = false,
+    hCool = 0,
+    lCool = -2000000.0,
+    KRCool = 10000,
+    TNCool = 1,
+    heaLoadFacOut=0,
+    heaLoadFacGrd=0,
+    CoolerOn = false,
+    withIdealThresholds = false,
+    TThresholdHeater = 303.15,
+    TThresholdCooler = 308.15);
+  annotation (Documentation(revisions="<html><ul>
+  <li>November 27, 2019, by David Jansen:<br/>
+    Integrate threshold for heater and cooler.
+  </li>
+  <li>February 28, 2019, by Niklas Huelsenbeck, dja, mre:<br/>
+    Adapting nrPeople and nrPeopleMachines to area specific approach
+  </li>
+  <li>September 27, 2016, by Moritz Lauster:<br/>
+    Reimplementation.
+  </li>
+  <li>June, 2015, by Moritz Lauster:<br/>
+    Implemented.
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  <span style=\"font-family: MS Shell Dlg 2;\">Zone \"Office\" of an
+  example building according to an office building with passive house
+  standard. The building is divided in six zones, this is a typical
+  zoning for an office building.</span>
+</p>
+</html>"));
+end SwimmingHall;
diff --git a/AixLib/DataBase/ThermalZones/SwimmingFacility/Technichal.mo b/AixLib/DataBase/ThermalZones/SwimmingFacility/Technichal.mo
new file mode 100644
index 0000000000..7a97cab465
--- /dev/null
+++ b/AixLib/DataBase/ThermalZones/SwimmingFacility/Technichal.mo
@@ -0,0 +1,95 @@
+within AixLib.DataBase.ThermalZones.SwimmingFacility;
+record Technichal "Swimming facility - Technical rooms"
+  extends AixLib.DataBase.ThermalZones.ZoneBaseRecord(
+    T_start = 298.15,
+    withAirCap = true,
+    VAir = 1251.545,
+    AZone = 369.1,
+    hRad = 4.999999999999999,
+    lat = 0.88645272708792,
+    nOrientations = 4,
+    AWin = {0.001, 8.64, 0.001, 6.04},
+    ATransparent = {0.001, 8.64, 0.001, 6.04},
+    hConWin = 2.7,
+    RWin = 0.07363309365761349,
+    gWin = 0.67,
+    UWin= 0.7993916878977316,
+    ratioWinConRad = 0.029999999999999992,
+    AExt = {0.001, 41.0, 0.001, 62.5},
+    hConExt = 2.7,
+    nExt = 1,
+    RExt = {0.0004121563761613994},
+    RExtRem = 0.0395915230647488,
+    CExt = {42090197.17545912},
+    AInt = 244.6741,
+    hConInt = 2.6999999999999997,
+    nInt = 1,
+    RInt = {0.0008142137828887332},
+    CInt = {31423590.247506615},
+    AFloor = 466.1496,
+    hConFloor = 1.7000000000000002,
+    nFloor = 1,
+    RFloor = {0.0001405991584732067},
+    RFloorRem =  0.00549087052326128,
+    CFloor = {241207146.17223492},
+    ARoof = 137.6,
+    hConRoof = 1.7000000000000006,
+    nRoof = 1,
+    RRoof = {0.0002092903359965459},
+    RRoofRem = 0.04662821312469006,
+    CRoof = {4123788.490763755},
+    nOrientationsRoof = 1,
+    tiltRoof = {0.0},
+    aziRoof = {0.0},
+    wfRoof = {1.0},
+    aRoof = 0.5,
+    aExt = 0.5,
+    TSoil = 286.15,
+    hConWallOut = 20.0,
+    hRadWall = 5.0,
+    hConWinOut = 19.999999999999996,
+    hConRoofOut = 20.000000000000004,
+    hRadRoof = 5.0,
+    tiltExtWalls = {1.5707963267948966, 1.5707963267948966, 1.5707963267948966, 1.5707963267948966},
+    aziExtWalls = {0.0, 1.5707963267948966, -1.5707963267948966, 3.141592653589793},
+    wfWall = {9.661649050259899e-06, 0.39612761106065586, 9.661649050259899e-06, 0.6038530656412436},
+    wfWin = {6.811061163329247e-05, 0.588475684511647, 6.811061163329247e-05, 0.41138809426508643},
+    wfGro = 0.0,
+    specificPeople = 0.025,
+    internalGainsMoistureNoPeople = 0.0,
+    fixedHeatFlowRatePersons = 90,
+    activityDegree = 2.0,
+    ratioConvectiveHeatPeople = 0.5,
+    internalGainsMachinesSpecific = 0.0,
+    ratioConvectiveHeatMachines = 0.75,
+    lightingPowerSpecific = 11.3,
+    ratioConvectiveHeatLighting = 0.9,
+    useConstantACHrate = true,
+    baseACH = 0.5,
+    maxUserACH = 1.0,
+    maxOverheatingACH = {3.0, 2.0},
+    maxSummerACH = {1.0, 283.15, 290.15},
+    winterReduction = {0.2, 273.15, 283.15},
+    maxIrr = {100.0, 100.0, 100.0, 100.0},
+    shadingFactor = {1.0, 1.0, 1.0, 1.0},
+    withAHU = true,
+    minAHU = 0.0,
+    maxAHU = 0.5,
+    hHeat = 100000.0,
+    lHeat = 0,
+    KRHeat = 10000,
+    TNHeat = 300,
+    HeaterOn = false,
+    hCool = 0,
+    lCool = -100000.0,
+    KRCool = 10000,
+    TNCool = 1,
+    heaLoadFacOut=0,
+    heaLoadFacGrd=0,
+    CoolerOn = false,
+    withIdealThresholds = false,
+    TThresholdHeater = 288.15,
+    TThresholdCooler = 295.15);
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end Technichal;
diff --git a/AixLib/DataBase/ThermalZones/SwimmingFacility/package.mo b/AixLib/DataBase/ThermalZones/SwimmingFacility/package.mo
new file mode 100644
index 0000000000..e1fe9654ab
--- /dev/null
+++ b/AixLib/DataBase/ThermalZones/SwimmingFacility/package.mo
@@ -0,0 +1,4 @@
+within AixLib.DataBase.ThermalZones;
+package SwimmingFacility
+  extends Modelica.Icons.MaterialPropertiesPackage;
+end SwimmingFacility;
diff --git a/AixLib/DataBase/ThermalZones/SwimmingFacility/package.order b/AixLib/DataBase/ThermalZones/SwimmingFacility/package.order
new file mode 100644
index 0000000000..8f551ffc8a
--- /dev/null
+++ b/AixLib/DataBase/ThermalZones/SwimmingFacility/package.order
@@ -0,0 +1,6 @@
+Changing
+Entrance
+Showers
+Supervisory
+SwimmingHall
+Technichal
diff --git a/AixLib/DataBase/ThermalZones/package.order b/AixLib/DataBase/ThermalZones/package.order
index feed1fc10e..b9eb9cb2b9 100644
--- a/AixLib/DataBase/ThermalZones/package.order
+++ b/AixLib/DataBase/ThermalZones/package.order
@@ -1,4 +1,5 @@
+Office_1995_1000
 ZoneBaseRecord
 ZoneRecordDummy
 OfficePassiveHouse
-Office_1995_1000
+SwimmingFacility
diff --git a/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_NE_SE_SW_NW_Hor.mo b/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_NE_SE_SW_NW_Hor.mo
index 4e8f930763..9e7f337d28 100644
--- a/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_NE_SE_SW_NW_Hor.mo
+++ b/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_NE_SE_SW_NW_Hor.mo
@@ -14,10 +14,10 @@ record SurfaceOrientationData_NE_SE_SW_NW_Hor
 <p>
   Data in this set:
 </p>
-<table>
   <caption>
-    \"Data\" cellspacing=\"2\" cellpadding=\"0\" border=\"0\
+    Data
   </caption>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"0\">
   <tr>
     <td style=\"background-color: #dcdcdc\">
       <p>
diff --git a/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_N_E_S_W_Hor.mo b/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_N_E_S_W_Hor.mo
index 2bac867734..3a9325711b 100644
--- a/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_N_E_S_W_Hor.mo
+++ b/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_N_E_S_W_Hor.mo
@@ -14,10 +14,10 @@ record SurfaceOrientationData_N_E_S_W_Hor
 <p>
   Data in this set:
 </p>
-<table>
   <caption>
-    \"Data\" cellspacing=\"2\" cellpadding=\"0\" border=\"0\
+    Data
   </caption>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"0\">
   <tr>
     <td style=\"background-color: #dcdcdc\">
       <p>
diff --git a/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_N_E_S_W_RoofN_Roof_S.mo b/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_N_E_S_W_RoofN_Roof_S.mo
index 2602ff4cec..b46840a61f 100644
--- a/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_N_E_S_W_RoofN_Roof_S.mo
+++ b/AixLib/DataBase/Weather/SurfaceOrientation/SurfaceOrientationData_N_E_S_W_RoofN_Roof_S.mo
@@ -15,9 +15,9 @@ record SurfaceOrientationData_N_E_S_W_RoofN_Roof_S
 <p>
   Data in this set:
 </p>
-<table>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"0\">
   <caption>
-    \"Data\" cellspacing=\"2\" cellpadding=\"0\" border=\"0\
+    Data
   </caption>
   <tr>
     <td style=\"background-color: #dcdcdc\">
diff --git a/AixLib/DataBase/package.order b/AixLib/DataBase/package.order
index 6fb02d10f1..95961bb866 100644
--- a/AixLib/DataBase/package.order
+++ b/AixLib/DataBase/package.order
@@ -5,6 +5,7 @@ Chiller
 HeatPump
 Media
 Pipes
+Pools
 Profiles
 Pumps
 Radiators
diff --git a/AixLib/Electrical/AC/Interfaces/PowerOutput.mo b/AixLib/Electrical/AC/Interfaces/PowerOutput.mo
new file mode 100644
index 0000000000..f4a92adf7e
--- /dev/null
+++ b/AixLib/Electrical/AC/Interfaces/PowerOutput.mo
@@ -0,0 +1,34 @@
+within AixLib.Electrical.AC.Interfaces;
+connector PowerOutput
+  "Connector with real power, reactive power and power factor"
+  output Modelica.Units.SI.Power real "Real power";
+  output Modelica.Units.SI.ReactivePower apparent "Apparent power";
+  output Modelica.Units.SI.Angle phi "Phase shift";
+  output Real cosPhi "Power factor";
+
+  annotation (Icon(graphics={ Polygon(
+          points={{-100,100},{100,0},{-100,-100},{-100,100}},
+          lineColor={0,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Diagram(graphics={
+                               Polygon(
+          points={{-100,50},{0,0},{-100,-50},{-100,50}},
+          lineColor={0,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid), Text(
+          extent={{30,110},{30,60}},
+          textColor={0,0,127},
+          textString="%name")}),
+    Documentation(info="<html>
+This connector contains multiple quantities that can be used to monitor
+the power consumption of a generic AC systems.
+</html>", revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PowerOutput;
diff --git a/AixLib/Electrical/AC/Interfaces/package.mo b/AixLib/Electrical/AC/Interfaces/package.mo
new file mode 100644
index 0000000000..2609934925
--- /dev/null
+++ b/AixLib/Electrical/AC/Interfaces/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Electrical.AC;
+package Interfaces "Package that contains some useful interfaces"
+extends Modelica.Icons.InterfacesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains interfaces that are used by the models in the
+<a href=\"modelica://AixLib.Electrical.AC\">AixLib.Electrical.AC</a> package.
+</p>
+</html>"));
+end Interfaces;
diff --git a/AixLib/Electrical/AC/Interfaces/package.order b/AixLib/Electrical/AC/Interfaces/package.order
new file mode 100644
index 0000000000..29b1329317
--- /dev/null
+++ b/AixLib/Electrical/AC/Interfaces/package.order
@@ -0,0 +1 @@
+PowerOutput
diff --git a/AixLib/Electrical/AC/OnePhase/Basics/Ground.mo b/AixLib/Electrical/AC/OnePhase/Basics/Ground.mo
new file mode 100644
index 0000000000..ef825b1014
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Basics/Ground.mo
@@ -0,0 +1,38 @@
+within AixLib.Electrical.AC.OnePhase.Basics;
+model Ground "Ground connection"
+  extends AixLib.Electrical.Interfaces.Ground(
+    redeclare package PhaseSystem = PhaseSystems.OnePhase,
+    redeclare Interfaces.Terminal_n terminal);
+  annotation (
+    defaultComponentName="gnd",
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Line(
+          points={{0,90},{0,0}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Line(
+          points={{-80,0},{80,0}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,-20},{60,-20}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Line(
+          points={{-40,-40},{40,-40}},
+          color={0,120,120},
+          smooth=Smooth.None)}), Documentation(info="<html>
+<p>
+This model represents a connection to the ground.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 4, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Ground;
diff --git a/AixLib/Electrical/AC/OnePhase/Basics/package.mo b/AixLib/Electrical/AC/OnePhase/Basics/package.mo
new file mode 100644
index 0000000000..8316551a65
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Basics/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.AC.OnePhase;
+package Basics "Package with basic models"
+extends Modelica.Icons.BasesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains simple models used in AC single phase networks.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 4, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end Basics;
diff --git a/AixLib/Electrical/AC/OnePhase/Basics/package.order b/AixLib/Electrical/AC/OnePhase/Basics/package.order
new file mode 100644
index 0000000000..4c72fd81ec
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Basics/package.order
@@ -0,0 +1 @@
+Ground
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/ACACConverter.mo b/AixLib/Electrical/AC/OnePhase/Conversion/ACACConverter.mo
new file mode 100644
index 0000000000..cc41f80f5c
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/ACACConverter.mo
@@ -0,0 +1,158 @@
+within AixLib.Electrical.AC.OnePhase.Conversion;
+model ACACConverter "AC AC converter single phase systems"
+  extends AixLib.Electrical.Icons.RefAngleConversion;
+  extends AixLib.Electrical.Interfaces.PartialConversion(
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n
+      constrainedby Interfaces.Terminal_n(
+      i(start = zeros(PhaseSystem_n.n),
+      each stateSelect = StateSelect.prefer)),
+    redeclare replaceable Interfaces.Terminal_p terminal_p
+      constrainedby Interfaces.Terminal_p(
+      i(start = zeros(PhaseSystem_p.n),
+      each stateSelect = StateSelect.prefer)));
+  parameter Real conversionFactor(min = Modelica.Constants.eps)
+    "Ratio of QS rms voltage on side 2 / QS rms voltage on side 1";
+  parameter Real eta(min=0, max=1)
+    "Converter efficiency, pLoss = (1-eta) * Ptr";
+  parameter Boolean ground_1 = false
+    "If true, connect side 1 of converter to ground"
+     annotation(Evaluate=true,Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true
+    "If true, connect side 2 of converter to ground"
+    annotation(Evaluate=true, Dialog(tab = "Ground", group="side 2"));
+  Modelica.Units.SI.Power LossPower[2] "Loss power";
+protected
+  Modelica.Units.SI.Power P_p[2]=PhaseSystem_p.phasePowers_vi(terminal_p.v,
+      terminal_p.i) "Power transmitted at pin p";
+  Modelica.Units.SI.Power P_n[2]=PhaseSystem_n.phasePowers_vi(terminal_n.v,
+      terminal_n.i) "Power transmitted at pin n";
+equation
+
+  // Ideal transformation
+  terminal_p.v = conversionFactor*terminal_n.v;
+
+  // Power loss term
+  terminal_p.i[1] = terminal_n.i[1]/conversionFactor*
+    AixLib.Utilities.Math.Functions.spliceFunction(eta-2, 1/(eta-2), P_p[1], deltax=0.1);
+  terminal_p.i[2] = terminal_n.i[2]/conversionFactor*
+    AixLib.Utilities.Math.Functions.spliceFunction(eta-2, 1/(eta-2), P_p[1], deltax=0.1);
+  LossPower = P_p + P_n;
+
+  // The two sides have the same reference angle
+  terminal_p.theta = terminal_n.theta;
+
+  if ground_1 then
+    Connections.potentialRoot(terminal_n.theta);
+  end if;
+  if ground_2 then
+    Connections.root(terminal_p.theta);
+  end if;
+
+  annotation (
+  defaultComponentName="conACAC",
+ Icon(coordinateSystem(preserveAspectRatio=false,
+          extent={{-100,-100},{100,100}}),
+                                      graphics={
+        Line(
+          points={{2,60},{2,60},{82,60},{2,60},{82,-60},{2,-60},{2,60},{2,-60}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Line(
+          points={{-2,60},{-2,60},{-82,60},{-2,60},{-82,-60},{-2,-60},{-2,60},{
+              -2,-60}},
+          color={11,193,87},
+          smooth=Smooth.None),
+        Text(
+          extent={{-100,92},{100,60}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%conversionFactor"),
+        Text(
+          extent={{-100,-100},{100,-132}},
+          textColor={0,120,120},
+          textString="%eta"),
+        Text(
+          extent={{-132,78},{-72,38}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-88,52},{-28,12}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{32,52},{92,12}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,78},{130,38}},
+          textColor={0,120,120},
+          textString="2")}),
+    Documentation(info="<html>
+<p>
+This is an AC/AC converter, based on a power balance between both circuit sides.
+The parameter <i>conversionFactor</i> defines the ratio between the RMS voltages
+as
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+V<sub>2</sub> = conversionFactor  V<sub>1</sub>
+</p>
+
+<p>
+where <i>V<sub>1</sub></i> and <i>V<sub>2</sub></i> are the RMS voltages
+at the primary and secondary sides of the transformer, i.e., the
+connector N and P, respectively.
+</p>
+
+<p>
+The loss of the converter is proportional to the power transmitted.
+The parameter <code>eta</code> is the efficiency of the transfer.
+The loss is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+P<sub>loss</sub> = (1-&eta;) P<sub>tr</sub>,
+</p>
+<p>
+where <i>P<sub>tr</sub></i> is the power transmitted. The model is bi-directional
+and the power can flow from the primary to the secondary side and vice-versa.
+Furthermore, reactive power on both side are set to zero.
+</p>
+<h4>Note:</h4>
+<p>
+This model is derived from
+<a href=\"modelica://Modelica.Electrical.QuasiStatic.SinglePhase.Utilities.IdealACDCConverter\">
+Modelica.Electrical.QuasiStatic.SinglePhase.Utilities.IdealACDCConverter</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 30, 2019, by Michael Wetter:<br/>
+Added missing <code>replaceable</code> for the terminal.
+</li>
+<li>
+September 4, 2014, by Michael Wetter:<br/>
+Revised model.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 9, 2014, by Marco Bonvini:<br/>
+Revised implementation and added <code>stateSelect</code> statement to use
+the current <code>i[:]</code> on the connectors as iteration variable for the
+initialization problem.
+</li>
+<li>
+January 29, 2012, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACConverter;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/ACACTransformer.mo b/AixLib/Electrical/AC/OnePhase/Conversion/ACACTransformer.mo
new file mode 100644
index 0000000000..6326425138
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/ACACTransformer.mo
@@ -0,0 +1,295 @@
+within AixLib.Electrical.AC.OnePhase.Conversion;
+model ACACTransformer "AC AC transformer simplified equivalent circuit"
+  extends AixLib.Electrical.Icons.RefAngleConversion;
+  extends AixLib.Electrical.Interfaces.PartialConversion(
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n
+      constrainedby Interfaces.Terminal_n(
+      i(start = zeros(PhaseSystem_n.n),
+      each stateSelect = StateSelect.prefer)),
+    redeclare replaceable Interfaces.Terminal_p terminal_p
+      constrainedby Interfaces.Terminal_p(
+      i(start = zeros(PhaseSystem_p.n),
+      each stateSelect = StateSelect.prefer)));
+  parameter Modelica.Units.SI.Voltage VHigh
+    "Rms voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "Rms voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Real XoverR
+    "Ratio between the complex and real components of the impedance (XL/R)";
+  parameter Real Zperc "Short circuit impedance";
+  parameter Boolean ground_1 = false
+    "If true, connect side 1 of converter to ground"
+    annotation(Evaluate=true,Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true
+    "If true, connect side 2 of converter to ground"
+    annotation(Evaluate=true, Dialog(tab = "Ground", group="side 2"));
+  parameter Modelica.Units.SI.Angle phi_1=0
+    "Angle of the voltage side 1 at initialization"
+    annotation (Evaluate=true, Dialog(tab="Initialization"));
+  parameter Modelica.Units.SI.Angle phi_2=phi_1
+    "Angle of the voltage side 2 at initialization"
+    annotation (Evaluate=true, Dialog(tab="Initialization"));
+  Modelica.Units.SI.Efficiency eta "Efficiency";
+  Modelica.Units.SI.Power PLoss[2] "Loss power";
+
+  Modelica.Units.SI.Voltage V1[2](start=PhaseSystem_n.phaseVoltages(VHigh,
+        phi_1)) "Voltage at the winding - primary side";
+  Modelica.Units.SI.Voltage V2[2](start=PhaseSystem_p.phaseVoltages(VLow, phi_2))
+    "Voltage at the winding - secondary side";
+protected
+  Real N = VHigh/VLow "Winding ratio";
+  Modelica.Units.SI.Current IHigh=VABase/VHigh
+    "Nominal current on primary side";
+  Modelica.Units.SI.Current ILow=VABase/VLow
+    "Nominal current on secondary side";
+  Modelica.Units.SI.Current IscHigh=IHigh/Zperc
+    "Short circuit current on primary side";
+  Modelica.Units.SI.Current IscLow=ILow/Zperc
+    "Short circuit current on secondary side";
+  Modelica.Units.SI.Impedance Zp=VHigh/IscHigh
+    "Impedance of the primary side (module)";
+  Modelica.Units.SI.Impedance Z1[2]={Zp*cos(atan(XoverR)),Zp*sin(atan(XoverR))}
+    "Impedance of the primary side of the transformer";
+  Modelica.Units.SI.Impedance Zs=VLow/IscLow
+    "Impedance of the secondary side (module)";
+  Modelica.Units.SI.Impedance Z2[2]={Zs*cos(atan(XoverR)),Zs*sin(atan(XoverR))}
+    "Impedance of the secondary side of the transformer";
+  Modelica.Units.SI.Power P_p[2]=PhaseSystem_p.phasePowers_vi(terminal_p.v,
+      terminal_p.i) "Power transmitted at pin p (secondary)";
+  Modelica.Units.SI.Power P_n[2]=PhaseSystem_n.phasePowers_vi(terminal_n.v,
+      terminal_n.i) "Power transmitted at pin n (primary)";
+  Modelica.Units.SI.Power S_p=Modelica.Fluid.Utilities.regRoot(P_p[1]^2 + P_p[2]
+      ^2, delta=0.1) "Apparent power at terminal p";
+  Modelica.Units.SI.Power S_n=Modelica.Fluid.Utilities.regRoot(P_n[1]^2 + P_n[2]
+      ^2, delta=0.1) "Apparent power at terminal n";
+
+equation
+  // Efficiency
+  eta = AixLib.Utilities.Math.Functions.smoothMin(
+        x1=
+        Modelica.Fluid.Utilities.regRoot(P_p[1]^2 + P_p[2]^2, delta=0.01)/
+        Modelica.Fluid.Utilities.regRoot(P_n[1]^2 + P_n[2]^2 + 1e-6, delta=0.01),
+        x2=
+        Modelica.Fluid.Utilities.regRoot(P_n[1]^2 + P_n[2]^2, delta=0.01)/
+        Modelica.Fluid.Utilities.regRoot(P_p[1]^2 + P_p[2]^2 + 1e-6, delta=0.01),
+        deltaX = 0.01);
+
+  // Ideal transformation
+  V2 = V1/N;
+  terminal_p.i[1] + terminal_n.i[1]*N = 0;
+  terminal_p.i[2] + terminal_n.i[2]*N = 0;
+
+  // Losses due to the impedance
+  terminal_n.v = V1 + AixLib.Electrical.PhaseSystems.OnePhase.product(
+    terminal_n.i, Z1);
+  V2 = terminal_p.v;
+
+  // Loss of power
+  PLoss = P_p + P_n;
+
+  // The two sides have the same reference angle
+  terminal_p.theta = terminal_n.theta;
+
+  if ground_1 then
+    Connections.potentialRoot(terminal_n.theta);
+  end if;
+  if ground_2 then
+    Connections.root(terminal_p.theta);
+  end if;
+
+  annotation (
+  defaultComponentName="traACAC",
+ Icon(coordinateSystem(preserveAspectRatio=false,
+          extent={{-100,-100},{100,100}}),
+                                      graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-130,60},{-70,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,60},{130,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-72,40},{-66,40},{-64,44},{-60,36},{-56,44},{-52,36},{-48,44},
+              {-44,36},{-42,40},{-38,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-60,-7.34764e-15}},
+          color={0,127,127},
+          origin={-40,40},
+          rotation=180),
+        Ellipse(
+          extent={{-30,46},{-18,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-18,46},{-6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,46},{6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-30,40},{6,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,40},{20,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{14,20},{26,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,8},{26,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,-4},{26,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{10,20},{20,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,-16},{20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{20,-40},{-70,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{34,40},{34,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{40,20},{28,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,8},{28,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,-4},{28,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{44,20},{34,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{34,-16},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,-40},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,40},{34,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-64,60},{-48,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-20,60},{-4,48}},
+          textColor={0,120,120},
+          textString="L")}),
+    Documentation(info="<html>
+<p>
+This is a simplified equivalent transformer model.
+The model accounts for winding Joule losses and leakage reactances
+that are represented by a series of a resistance <i>R</i> and an
+inductance <i>L</i>. The resistance and the inductance represent both the
+effects of the secondary and primary side of the transformer.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>VHigh</code> - RMS voltage at primary side,</li>
+<li><code>VLow</code> - RMS voltage at secondary side,</li>
+<li><code>VABase</code> - apparent nominal power of the transformer,</li>
+<li><code>XoverR</code> - ratio between reactance and resistance, and</li>
+<li><code>Zperc</code> - the short circuit impedance.</li>
+</ul>
+<p>
+Given the nominal conditions,the model computes the values of the resistance and the inductance.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 30, 2019, by Michael Wetter:<br/>
+Added missing <code>replaceable</code> for the terminal.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Made voltage public to allow setting a start value in
+<a href=\"modelica://Buildings.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.DY\">
+Buildings.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.DY</a>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+September 4, 2014, by Michael Wetter:<br/>
+Revised model.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>June 17, 2014, by Marco Bonvini:<br/>
+Adde parameter <code>phi_1</code> and <code>phi_2</code> that are
+used during initialization to specify the angle of the voltage phasor.
+</li>
+<li>
+June 9, 2014, by Marco Bonvini:<br/>
+Revised implementation and added <code>stateSelect</code> statement to use
+the current <code>i[:]</code> on the connectors as iteration variable for the
+initialization problem.
+</li>
+<li>
+January 29, 2012, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformer;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/ACACTransformerFull.mo b/AixLib/Electrical/AC/OnePhase/Conversion/ACACTransformerFull.mo
new file mode 100644
index 0000000000..62afc4e5d8
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/ACACTransformerFull.mo
@@ -0,0 +1,425 @@
+within AixLib.Electrical.AC.OnePhase.Conversion;
+model ACACTransformerFull "AC AC transformer with detailed equivalent circuit"
+  extends AixLib.Electrical.Icons.RefAngleConversion;
+  extends AixLib.Electrical.Interfaces.PartialConversion(
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n
+      constrainedby Interfaces.Terminal_n(
+      i(start = zeros(PhaseSystem_n.n),
+      each stateSelect = StateSelect.prefer)),
+    redeclare replaceable Interfaces.Terminal_p terminal_p
+      constrainedby Interfaces.Terminal_p(
+      i(start = zeros(PhaseSystem_p.n),
+      each stateSelect = StateSelect.prefer)));
+  parameter Modelica.Units.SI.Voltage VHigh
+    "RMS voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "RMS voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Modelica.Units.SI.Frequency f(start=60) "Nominal frequency";
+  parameter AixLib.Electrical.Types.PerUnit R1(min=0)
+    "Resistance on side 1 of the transformer (pu)";
+  parameter AixLib.Electrical.Types.PerUnit L1(min=0)
+    "Inductance on side 1 of the transformer (pu)";
+  parameter AixLib.Electrical.Types.PerUnit R2(min=0)
+    "Resistance on side 2 of the transformer (pu)";
+  parameter AixLib.Electrical.Types.PerUnit L2(min=0)
+    "Inductance on side 2 of the transformer (pu)";
+  parameter Boolean magEffects = false
+    "If true, introduce magnetization effects"
+    annotation(Evaluate=true, Dialog(group="Magnetization"));
+  parameter AixLib.Electrical.Types.PerUnit Rm(min=0)
+    "Magnetization resistance (pu)"
+    annotation(Evaluate=true, Dialog(group="Magnetization", enable = magEffects));
+  parameter AixLib.Electrical.Types.PerUnit Lm(min=0)
+    "Magnetization inductance (pu)"
+    annotation(Evaluate=true, Dialog(group="Magnetization", enable = magEffects));
+  parameter Boolean ground_1 = false "Connect side 1 of converter to ground"
+   annotation(Evaluate=true,Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of converter to ground"
+   annotation(Evaluate=true, Dialog(tab = "Ground", group="side 2"));
+  parameter Modelica.Units.SI.Angle phi_1=0
+    "Angle of the voltage side 1 at initialization"
+    annotation (Evaluate=true, Dialog(tab="Initialization"));
+  parameter Modelica.Units.SI.Angle phi_2=phi_1
+    "Angle of the voltage side 2 at initialization"
+    annotation (Evaluate=true, Dialog(tab="Initialization"));
+  Modelica.Units.SI.Efficiency eta "Efficiency";
+  Modelica.Units.SI.Power PLoss[2] "Loss power";
+
+  Modelica.Units.SI.Voltage V1[2](start=PhaseSystem_n.phaseVoltages(VHigh,
+        phi_1)) "Voltage at the winding - primary side";
+  Modelica.Units.SI.Voltage V2[2](start=PhaseSystem_n.phaseVoltages(VLow, phi_2))
+    "Voltage at the winding - secondary side";
+protected
+  parameter Modelica.Units.SI.AngularVelocity omega_n=2*Modelica.Constants.pi*f;
+  parameter Real N = VHigh/VLow "Winding ratio";
+  parameter Modelica.Units.SI.Resistance RBaseHigh=VHigh^2/VABase
+    "Base impedance of the primary side";
+  parameter Modelica.Units.SI.Resistance RBaseLow=VLow^2/VABase
+    "Base impedance of the secondary side";
+  Modelica.Units.SI.Impedance Z1[2]={RBaseHigh*R1,omega*L1*RBaseHigh/omega_n}
+    "Impedance of the primary side of the transformer";
+  Modelica.Units.SI.Impedance Z2[2]={RBaseLow*R2,omega*L2*RBaseLow/omega_n}
+    "Impedance of the secondary side of the transformer";
+  Modelica.Units.SI.Impedance Zrm[2]={RBaseHigh*Rm,0}
+    "Magnetization impedance - resistance";
+  Modelica.Units.SI.Impedance Zlm[2]={0,omega*Lm*RBaseHigh/omega_n}
+    "Magnetization impedance - impedence";
+  Modelica.Units.SI.Power P_p[2]=PhaseSystem_p.phasePowers_vi(terminal_p.v,
+      terminal_p.i) "Power transmitted at pin p (secondary)";
+  Modelica.Units.SI.Power P_n[2]=PhaseSystem_n.phasePowers_vi(terminal_n.v,
+      terminal_n.i) "Power transmitted at pin n (primary)";
+  Modelica.Units.SI.Power S_p=Modelica.Fluid.Utilities.regRoot(P_p[1]^2 + P_p[2]
+      ^2, delta=0.1) "Apparent power at terminal p";
+  Modelica.Units.SI.Power S_n=Modelica.Fluid.Utilities.regRoot(P_n[1]^2 + P_n[2]
+      ^2, delta=0.1) "Apparent power at terminal n";
+  Modelica.Units.SI.AngularVelocity omega "Angular velocity";
+  Modelica.Units.SI.Current Im[2] "Magnetization current";
+  Modelica.Units.SI.Angle theRef "Absolute angle of rotating reference system";
+equation
+  assert(sqrt(P_p[1]^2 + P_p[2]^2) <= VABase*1.01,
+    "The load power of the transformer is higher than VABase");
+
+  // Angular velocity
+  theRef = PhaseSystem_p.thetaRef(terminal_p.theta);
+  omega = der(theRef);
+
+  // Efficiency
+  eta = AixLib.Utilities.Math.Functions.smoothMin(
+        x1=
+        Modelica.Fluid.Utilities.regRoot(P_p[1]^2 + P_p[2]^2, delta=0.01)/
+        Modelica.Fluid.Utilities.regRoot(P_n[1]^2 + P_n[2]^2 + 1e-6, delta=0.01),
+        x2=
+        Modelica.Fluid.Utilities.regRoot(P_n[1]^2 + P_n[2]^2, delta=0.01)/
+        Modelica.Fluid.Utilities.regRoot(P_p[1]^2 + P_p[2]^2 + 1e-6, delta=0.01),
+        deltaX = 0.01);
+
+  // Ideal transformation
+  V2 = V1/N;
+  terminal_p.i[1] + (terminal_n.i[1] - Im[1])*N = 0;
+  terminal_p.i[2] + (terminal_n.i[2] - Im[2])*N = 0;
+
+  // Magnetization current
+  if magEffects then
+    Im = AixLib.Electrical.PhaseSystems.OnePhase.divide(V1, Zrm) +
+         AixLib.Electrical.PhaseSystems.OnePhase.divide(V1, Zlm);
+  else
+    Im = zeros(2);
+  end if;
+
+  // Losses due to the impedance - primary side
+  terminal_n.v = V1 + AixLib.Electrical.PhaseSystems.OnePhase.product(
+    terminal_n.i, Z1);
+
+  // Losses due to the impedance - secondary side
+  terminal_p.v = V2 + AixLib.Electrical.PhaseSystems.OnePhase.product(
+    terminal_p.i, Z2);
+
+  // Loss of power
+  PLoss = P_p + P_n;
+
+  // The two sides have the same reference angle
+  terminal_p.theta = terminal_n.theta;
+
+  if ground_1 then
+    Connections.potentialRoot(terminal_n.theta);
+  end if;
+  if ground_2 then
+    Connections.root(terminal_p.theta);
+  end if;
+
+  annotation (
+defaultComponentName="traACAC",
+ Icon(coordinateSystem(preserveAspectRatio=false,
+          extent={{-100,-100},{100,100}}),
+                                      graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-140,60},{-80,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{80,60},{140,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-100,40},{-94,40},{-92,44},{-88,36},{-84,44},{-80,36},{-76,44},
+              {-72,36},{-70,40},{-64,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-64,46},{-52,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-52,46},{-40,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-40,46},{-28,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-64,40},{-26,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{0,40},{0,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-6,20},{6,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,8},{6,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,-4},{6,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-10,20},{0,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{0,-16},{0,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{0,-40},{-90,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{14,40},{14,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{20,20},{8,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{20,8},{8,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{20,-4},{8,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{24,20},{14,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{14,-16},{14,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{100,-40},{14,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-80,60},{-64,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-54,60},{-38,48}},
+          textColor={0,120,120},
+          textString="L"),
+        Line(
+          points={{66,40},{72,40},{74,44},{78,36},{82,44},{86,36},{90,44},{94,36},
+              {96,40},{100,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-54,-6.61288e-15}},
+          color={0,127,127},
+          origin={14,40},
+          rotation=180),
+        Ellipse(
+          extent={{26,46},{38,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{38,46},{50,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{50,46},{62,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{26,40},{62,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Text(
+          extent={{76,60},{92,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{36,60},{52,48}},
+          textColor={0,120,120},
+          textString="L"),
+        Line(
+          points={{-26,-1},{-10,-1},{-9,4},{-5,-4},{-1,4},{3,-4},{7,4},{10,-5},{
+              12,-1},{22,-1}},
+          color={0,127,127},
+          smooth=Smooth.None,
+          origin={-45,2},
+          rotation=90),
+        Ellipse(
+          extent={{-36,18},{-24,6}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-36,6},{-24,-6}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-36,-6},{-24,-18}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-40,18},{-30,-18}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-28,-2.09669e-15}},
+          color={0,127,127},
+          origin={-28,40},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-1.53415e-16,-6}},
+          color={0,127,127},
+          origin={-30,18},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-1.53415e-16,-6}},
+          color={0,127,127},
+          origin={-30,-24},
+          rotation=180),
+        Line(
+          points={{-44,24},{-20,24},{-20,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{-44,-24},{-20,-24},{-20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-70,22},{-54,10}},
+          textColor={0,120,120},
+          textString="Rm"),
+        Text(
+          extent={{-70,-8},{-54,-20}},
+          textColor={0,120,120},
+          textString="Lm")}),
+    Documentation(info="<html>
+<p>
+This is a detailed transformer model that takes into account the winding Joule losses
+and the leakage reactances on both primary and secondary side. The model also describes
+the core or iron losses and the losses due to magnetization effects.
+</p>
+<p>
+The losses are represented by a series of resistances <i>R<sub>1</sub></i>, <i>R<sub>2</sub></i>,
+<i>R<sub>m</sub></i> and inductances <i>L<sub>1</sub></i>, <i>L<sub>2</sub></i>, and
+<i>L<sub>m</sub></i>.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>VHigh</code> - RMS voltage at primary side,</li>
+<li><code>VLow</code> - RMS voltage at secondary side,</li>
+<li><code>VABase</code> - apparent nominal power of the transformer,</li>
+<li><code>f</code> - frequency,</li>
+<li><code>R_1, L_1</code> - resistance and inductance at primary side (per unit),</li>
+<li><code>R_2, L_2</code> - resistance and inductance at secondary side (per unit), and</li>
+<li><code>R_m, L_m</code> - resistance and inductance for magnetization effects (per unit).</li>
+</ul>
+<p>
+Given the nominal conditions, the model computes the values of the nominal impedances
+at both primary and secondary side. Given these values, the per unit values are transformed into
+the actual values of the resistances and inductances.
+</p>
+<p>
+The magnetization losses can be enabled or disabled using the boolean flag <code>magEffects</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 30, 2019, by Michael Wetter:<br/>
+Added missing <code>replaceable</code> for the terminal.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Made voltage public to allow setting a start value.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+May 26, 2016, by Michael Wetter:<br/>
+Moved function call to <code>PhaseSystem.thetaRef</code> out of
+derivative operator as this is not yet supported by JModelica.
+</li>
+<li>
+September 4, 2014, by Michael Wetter:<br/>
+Revised model.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>June 17, 2014, by Marco Bonvini:<br/>
+Adde parameter <code>phi_1</code> and <code>phi_2</code> that are
+used during initialization to specify the angle of the voltage phasor.
+</li>
+<li>
+June 9, 2014, by Marco Bonvini:<br/>
+Revised implementation and added <code>stateSelect</code> statement to use
+the current <code>i[:]</code> on the connectors as iteration variable for the
+initialization problem.
+</li>
+<li>
+January 29, 2012, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerFull;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/ACDCConverter.mo b/AixLib/Electrical/AC/OnePhase/Conversion/ACDCConverter.mo
new file mode 100644
index 0000000000..4c407249c9
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/ACDCConverter.mo
@@ -0,0 +1,181 @@
+within AixLib.Electrical.AC.OnePhase.Conversion;
+model ACDCConverter "AC DC converter"
+  extends AixLib.Electrical.Interfaces.PartialConversion(
+    redeclare package PhaseSystem_p = PhaseSystems.TwoConductor,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n
+      constrainedby Interfaces.Terminal_n(
+        i(start = zeros(PhaseSystem_n.n),
+        each stateSelect = StateSelect.prefer)),
+    redeclare DC.Interfaces.Terminal_p terminal_p(
+        i(start = zeros(PhaseSystem_p.n),
+        each stateSelect = StateSelect.prefer)));
+  parameter Real conversionFactor(min = Modelica.Constants.eps)
+    "Ratio of DC voltage / AC RMS voltage";
+  parameter Real eta(min=0, max=1)
+    "Converter efficiency, pLoss = (1-eta) * Ptr";
+  Modelica.Units.SI.Power PLoss "Loss power";
+  parameter Boolean ground_AC = false "Connect AC side of converter to ground" annotation(Evaluate=true, Dialog(tab = "Ground", group="AC side"));
+  parameter Boolean ground_DC = true "Connect DC side of converter to ground" annotation(Evaluate=true, Dialog(tab = "Ground", group="DC side"));
+protected
+  PhaseSystem_p.Current i_dc "DC current";
+  PhaseSystem_p.Voltage v_dc "DC voltage";
+  Modelica.Units.SI.Power P_p[2]=PhaseSystem_p.phasePowers_vi(terminal_p.v,
+      terminal_p.i) "Power transmitted at pin p (secondary)";
+  Modelica.Units.SI.Power P_n[2](each start=0) = PhaseSystem_n.phasePowers_vi(
+    terminal_n.v, terminal_n.i) "Power transmitted at pin n (primary)";
+equation
+  //voltage relation
+  v_p = v_n*conversionFactor;
+
+  // Power losses
+  PLoss = (1-eta)*
+    AixLib.Utilities.Math.Functions.spliceFunction(P_p[1], P_n[1], i_p, deltax=0.1);
+  P_n + P_p = {PLoss, 0};
+
+  if ground_AC then
+    Connections.potentialRoot(terminal_n.theta);
+  end if;
+
+  if ground_DC then
+    v_dc = 0;
+    Connections.root(terminal_p.theta);
+  else
+    i_dc = 0;
+    Connections.potentialRoot(terminal_p.theta);
+  end if;
+
+  v_dc = terminal_p.v[2];
+  sum(terminal_p.i) + i_dc = 0;
+
+  annotation (
+defaultComponentName="conACDC",
+ Icon(coordinateSystem(preserveAspectRatio=false,
+          extent={{-100,-100},{100,100}}),
+                                      graphics={
+        Line(
+          points={{2,60},{2,60},{82,60},{2,60},{82,-60},{2,-60},{2,60},{2,-60}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Text(
+          extent={{36,54},{96,14}},
+          textColor={0,0,255},
+          textString="DC"),
+        Line(
+          points={{-2,60},{-2,60},{-82,60},{-2,60},{-82,-60},{-2,-60},{-2,60},{
+              -2,-60}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Text(
+          extent={{-100,52},{-40,12}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{-100,92},{100,60}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%conversionFactor"),
+        Text(
+          extent={{-100,-100},{100,-132}},
+          textColor={0,0,0},
+          textString="%eta"),
+        Line(visible = ground_DC == true,
+          points={{100,-100},{100,-12}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = ground_DC == true,
+          points={{80,-100},{120,-100}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = ground_DC == true,
+          points={{88,-106},{112,-106}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = ground_DC == true,
+          points={{94,-112},{108,-112}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = ground_AC == true,
+          points={{-80,-40},{-120,-40}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = ground_AC == true,
+          points={{-80,-40},{-106,-14}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = ground_AC == true,
+          points={{-102,-16},{-114,-24},{-118,-42}},
+          color={0,120,120},
+          smooth=Smooth.Bezier)}),
+    Documentation(info="<html>
+<p>
+This is an AC/DC converter, based on a power balance between both circuit sides.
+The parameter <code>conversionFactor</code> defines the ratio between the RMS voltages
+as
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+V<sub>DC</sub> = conversionFactor V<sub>AC</sub>,
+</p>
+
+<p>
+where <i>V<sub>DC</sub></i> is the voltage of the DC circuit and <i>V<sub>AC</sub></i>
+is the RMS voltage at the primary side of the transformer.
+</p>
+
+<p>
+The loss of the converter is proportional to the power transmitted.
+The parameter <code>eta</code> is the efficiency of the transfer.
+The loss is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+P<sub>loss</sub> = (1-&eta;) P<sub>tr</sub>
+</p>
+<p>
+where <i>P<sub>tr</sub></i> is the power transmitted. The model is bi-directional
+and the power can flow from both the primary to the secondary side and vice-versa.
+Furthermore, reactive power on both side are set to <i>0</i>.
+</p>
+<h4>Note:</h4>
+<p>
+This model is derived from
+<a href=\"modelica://Modelica.Electrical.QuasiStatic.SinglePhase.Utilities.IdealACDCConverter\">
+Modelica.Electrical.QuasiStatic.SinglePhase.Utilities.IdealACDCConverter</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 30, 2019, by Michael Wetter:<br/>
+Added missing <code>replaceable</code> for the terminal.
+</li>
+<li>
+March 30, 2015, by Michael Wetter:<br/>
+Added missing <code>each</code>.
+</li>
+<li>
+September 4, 2014, by Michael Wetter:<br/>
+Revised model.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 9, 2014, by Marco Bonvini:<br/>
+Revised implementation and added <code>stateSelect</code> statement to use
+the current <code>i[:]</code> on the connectors as iteration variable for the
+initialization problem.
+</li>
+<li>
+January 4, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACDCConverter;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACConverter.mo b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACConverter.mo
new file mode 100644
index 0000000000..1b01e8a7ef
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACConverter.mo
@@ -0,0 +1,69 @@
+within AixLib.Electrical.AC.OnePhase.Conversion.Examples;
+model ACACConverter
+  "This example illustrates how to use the AC/AC converter model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter
+    conACAC(eta=0.9, conversionFactor=60/120) "ACAC transformer"
+    annotation (Placement(transformation(extent={{-10,0},{10,20}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage                 sou(
+    definiteReference=true,
+    f=60,
+    V=120) "Voltage source"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-60,10})));
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive load(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=60) "Load model"
+    annotation (Placement(transformation(extent={{24,0},{44,20}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=0.5,
+    startTime=0.3,
+    height=2000,
+    offset=-1000) "Power consumed by the model"
+    annotation (Placement(transformation(extent={{80,0},{60,20}})));
+equation
+  connect(sou.terminal, conACAC.terminal_n) annotation (Line(
+      points={{-50,10},{-10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(conACAC.terminal_p, load.terminal)     annotation (Line(
+      points={{10,10},{24,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow) annotation (Line(
+      points={{59,10},{44,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This example illustrates the use of a model that converts AC voltage to AC voltage.
+The transformer model assumes a linear loss when transmitting the power.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Removed binding of <code>P_nominal</code> as
+this parameter is disabled and assigned a value
+in the <code>initial equation</code> section.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACConverter.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACConverter;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformer.mo b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformer.mo
new file mode 100644
index 0000000000..9202ec13e6
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformer.mo
@@ -0,0 +1,116 @@
+within AixLib.Electrical.AC.OnePhase.Conversion.Examples;
+model ACACTransformer
+  "This example illustrates how to use the AC/AC simplified transformer model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer tra_load(
+    Zperc=0.03,
+    VABase=4000,
+    XoverR=8,
+    VHigh=120,
+    VLow=60) "Transformer with load"
+    annotation (Placement(transformation(extent={{-18,40},{2,60}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage sou(
+    definiteReference=true,
+    f=60,
+    V=120) "Voltage source"
+      annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,50})));
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive load(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    pf=0.8,
+    V_nominal=60) "Load model"
+    annotation (Placement(transformation(extent={{10,40},{30,60}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=0.5,
+    startTime=0.3,
+    offset=0,
+    height=-4000*0.8) "Load power consumption profile"
+    annotation (Placement(transformation(extent={{70,40},{50,60}})));
+  AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer tra_cc(
+    XoverR=8,
+    Zperc=0.03,
+    VABase=4000,
+    VHigh=120,
+    VLow=60) "Transformer with short circuit"
+    annotation (Placement(transformation(extent={{-16,0},{4,20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance shortCircuit(R=1e-8)
+    "Short circuit"
+    annotation (Placement(transformation(extent={{10,0},{30,20}})));
+  AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer tra_void(
+    XoverR=8,
+    Zperc=0.03,
+    VABase=4000,
+    VHigh=120,
+    VLow=60) "Transformer with secondary not connected"
+    annotation (Placement(transformation(extent={{-16,-30},{4,-10}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage sou1(
+    definiteReference=true,
+    f=60,
+    V=120) "Voltage source for open and short circuit tests"
+                          annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,10})));
+equation
+  connect(sou.terminal, tra_load.terminal_n)
+                                            annotation (Line(
+      points={{-60,50},{-18,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(tra_load.terminal_p, load.terminal)    annotation (Line(
+      points={{2,50},{10,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow) annotation (Line(
+      points={{49,50},{30,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(tra_cc.terminal_p, shortCircuit.terminal) annotation (Line(
+      points={{4,10},{10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou1.terminal, tra_cc.terminal_n) annotation (Line(
+      points={{-60,10},{-16,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou1.terminal, tra_void.terminal_n) annotation (Line(
+      points={{-60,10},{-38,10},{-38,-20},{-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This example illustrates the use of a the AC/AC transformer model.
+The example shows three different configurations:
+</p>
+<ul>
+<li>With a load connected,</li>
+<li>without a load connected, and</li>
+<li>with a short circuit connection.</li>
+</ul>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Removed binding of <code>P_nominal</code> as
+this parameter is disabled and assigned a value
+in the <code>initial equation</code> section.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformer.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformer;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformerFull.mo b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformerFull.mo
new file mode 100644
index 0000000000..62f44c2f36
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformerFull.mo
@@ -0,0 +1,137 @@
+within AixLib.Electrical.AC.OnePhase.Conversion.Examples;
+model ACACTransformerFull
+  "This example illustrates how to use the AC/AC transformer model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull tra_load(
+    R1=0.0001,
+    L1=0.0001,
+    R2=0.0001,
+    L2=0.0001,
+    VABase=4000,
+    magEffects=true,
+    Rm=10,
+    Lm=10,
+    VHigh=120,
+    VLow=60,
+    f=60) "Transformer with load"
+    annotation (Placement(transformation(extent={{-18,40},{2,60}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage sou(
+    definiteReference=true,
+    f=60,
+    V=120) "Voltage source"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,50})));
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive load(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    pf=0.8,
+    V_nominal=60) "Load model"
+            annotation (Placement(transformation(extent={{10,40},{30,60}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=0.5,
+    startTime=0.3,
+    offset=0,
+    height=-4000*0.8) "Load power consumption profile"
+    annotation (Placement(transformation(extent={{70,40},{50,60}})));
+  AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull
+                                                              tra_cc(
+    VABase=4000,
+    R1=0.01,
+    L1=0.01,
+    R2=0.01,
+    L2=0.01,
+    magEffects=false,
+    Rm=100,
+    Lm=100,
+    VHigh=120,
+    VLow=60,
+    f=60) "Transformer with short circuit connection"
+    annotation (Placement(transformation(extent={{-16,0},{4,20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance shortCircuit(R=1e-8)
+    "Short circuit"
+    annotation (Placement(transformation(extent={{10,0},{30,20}})));
+  AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull tra_void(
+    VABase=4000,
+    R1=0.01,
+    L1=0.01,
+    R2=0.01,
+    L2=0.01,
+    magEffects=false,
+    Rm=100,
+    Lm=100,
+    VHigh=120,
+    VLow=60,
+    f=60) "Transformer with open connection"
+    annotation (Placement(transformation(extent={{-16,-30},{4,-10}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage sou1(
+    definiteReference=true,
+    f=60,
+    V=120) "Voltage source for short circuit and open tests "
+                          annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,10})));
+equation
+  connect(sou.terminal, tra_load.terminal_n)
+                                            annotation (Line(
+      points={{-60,50},{-18,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(tra_load.terminal_p, load.terminal)    annotation (Line(
+      points={{2,50},{10,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow) annotation (Line(
+      points={{49,50},{30,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(tra_cc.terminal_p, shortCircuit.terminal) annotation (Line(
+      points={{4,10},{10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou1.terminal, tra_cc.terminal_n) annotation (Line(
+      points={{-60,10},{-16,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou1.terminal, tra_void.terminal_n) annotation (Line(
+      points={{-60,10},{-38,10},{-38,-20},{-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This example illustrates the use of the AC/AC transformer model
+that includes losses at the primary and secondary side and magnetization
+effects.
+The example shows three different configurations:
+</p>
+<ul>
+<li>With a load connected,</li>
+<li>without a load connected, and</li>
+<li>with a short circuit connection.</li>
+</ul>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Removed binding of <code>P_nominal</code> as
+this parameter is disabled and assigned a value
+in the <code>initial equation</code> section.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformerFull.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerFull;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACDCConverter.mo b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACDCConverter.mo
new file mode 100644
index 0000000000..43b6c81b4a
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/ACDCConverter.mo
@@ -0,0 +1,85 @@
+within AixLib.Electrical.AC.OnePhase.Conversion.Examples;
+model ACDCConverter
+  "This example illustrates how to use the AC/DC converter model"
+  extends Modelica.Icons.Example;
+
+  AixLib.Electrical.DC.Loads.Resistor res(R=1, V_nominal=60)
+    "Resistive load" annotation (Placement(
+        transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={50,10})));
+  AixLib.Electrical.AC.OnePhase.Conversion.ACDCConverter conversion(
+    eta=0.9,
+    ground_AC=false,
+    ground_DC=true,
+    conversionFactor=60/120) "AC/DC transformer"
+    annotation (Placement(transformation(extent={{-10,0},{10,20}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage sou(
+    definiteReference=true,
+    f=60,
+    V=120) "Voltage source"                  annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-62,10})));
+  AixLib.Electrical.DC.Loads.Conductor load(mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=60) "Variable resistive load"
+    annotation (Placement(
+        transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={50,-10})));
+  Modelica.Blocks.Sources.Ramp pow(
+    duration=0.5,
+    startTime=0.2,
+    offset=-200,
+    height=5200) "Variable load profile"
+    annotation (Placement(transformation(extent={{90,-20},{70,0}})));
+equation
+  connect(sou.terminal, conversion.terminal_n) annotation (Line(
+      points={{-52,10},{-10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(conversion.terminal_p, res.terminal) annotation (Line(
+      points={{10,10},{40,10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(conversion.terminal_p, load.terminal) annotation (Line(
+      points={{10,10},{30,10},{30,-10},{40,-10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(pow.y, load.Pow) annotation (Line(
+      points={{69,-10},{60,-10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This example illustrates the use of a model that converts AC voltage to DC voltage.
+The transformer model assumes a linear loss when transmitting the power.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Removed binding of <code>P_nominal</code> as
+this parameter is disabled and assigned a value
+in the <code>initial equation</code> section.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACDCConverter.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACDCConverter;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/Examples/package.mo b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/package.mo
new file mode 100644
index 0000000000..5d19c56ade
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.OnePhase.Conversion;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion\">
+AixLib.Electrical.AC.OnePhase.Conversion</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/Examples/package.order b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/package.order
new file mode 100644
index 0000000000..4e2ad8d42f
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/Examples/package.order
@@ -0,0 +1,4 @@
+ACACConverter
+ACACTransformer
+ACACTransformerFull
+ACDCConverter
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/package.mo b/AixLib/Electrical/AC/OnePhase/Conversion/package.mo
new file mode 100644
index 0000000000..31477ab5b2
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.AC.OnePhase;
+package Conversion "Package with models for AC/AC and AC/DC conversion"
+  extends Modelica.Icons.Package;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models for AC/AC and AC/DC conversion.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Conversion;
diff --git a/AixLib/Electrical/AC/OnePhase/Conversion/package.order b/AixLib/Electrical/AC/OnePhase/Conversion/package.order
new file mode 100644
index 0000000000..6e342d1531
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Conversion/package.order
@@ -0,0 +1,5 @@
+ACACConverter
+ACACTransformer
+ACACTransformerFull
+ACDCConverter
+Examples
diff --git a/AixLib/Electrical/AC/OnePhase/Examples/GeneratorLoadGrid.mo b/AixLib/Electrical/AC/OnePhase/Examples/GeneratorLoadGrid.mo
new file mode 100644
index 0000000000..e768224222
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Examples/GeneratorLoadGrid.mo
@@ -0,0 +1,64 @@
+within AixLib.Electrical.AC.OnePhase.Examples;
+model GeneratorLoadGrid "Generator with a load and grid connection"
+  extends Modelica.Icons.Example;
+
+  Sources.Grid grid(
+    f=60,
+    V=120,
+    phiSou=0.5235987755983) "Electrical grid"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  Sources.Generator sou(f=60, phiGen(displayUnit="rad")) "Gas turbine"
+                    annotation (Placement(transformation(
+        extent={{-10,10},{10,-10}},
+        origin={-30,-10})));
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive res(
+    mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    P_nominal=-5e3,
+    V_nominal=120,
+    pf=1) "Inductive load"      annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={30,-10})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    height=1e4,
+    duration=0.6,
+    startTime=0.1,
+    offset=0)
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+equation
+  connect(ramp.y, sou.P) annotation (Line(
+      points={{-59,-10},{-40,-10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou.terminal, grid.terminal) annotation (Line(
+      points={{-20,-10},{10,-10},{10,40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(res.terminal, grid.terminal) annotation (Line(
+      points={{20,-10},{10,-10},{10,40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(
+      StopTime=1.0,
+      Tolerance=1e-6),
+      __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Examples/GeneratorLoadGrid.mos"
+        "Simulate and plot"),
+        Documentation(info="<html>
+<p>
+This model illustrates a generator, an inductive load and a grid connection.
+The power output of the generator is equal to its input signal, which is
+a ramp function.
+The output <code>grid.P</code> shows
+the actual and apparent power, the power factor and
+the phase angle.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 10, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneratorLoadGrid;
diff --git a/AixLib/Electrical/AC/OnePhase/Examples/GridDCLoad.mo b/AixLib/Electrical/AC/OnePhase/Examples/GridDCLoad.mo
new file mode 100644
index 0000000000..a3d3a7cef8
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Examples/GridDCLoad.mo
@@ -0,0 +1,54 @@
+within AixLib.Electrical.AC.OnePhase.Examples;
+model GridDCLoad "Model of a DC load connected to the grid"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sources.Grid
+               grid(
+    f=60,
+    phiSou=0,
+    V=120)
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+  AixLib.Electrical.AC.OnePhase.Conversion.ACDCConverter
+                                                   idealACDCConverter1(
+                               eta=0.9,
+    ground_AC=false,
+    conversionFactor=12/120)
+    annotation (Placement(transformation(extent={{-50,-40},{-30,-20}})));
+  AixLib.Electrical.DC.Loads.Resistor    resistor(R=1, V_nominal=12)
+                                                          annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        origin={10,-30})));
+equation
+  connect(grid.terminal, idealACDCConverter1.terminal_n) annotation (Line(
+      points={{-70,-20},{-70,-30},{-50,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(idealACDCConverter1.terminal_p, resistor.terminal) annotation (Line(
+      points={{-30,-30},{0,-30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation (experiment(
+      StopTime=1.0,
+      Tolerance=1e-6),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Examples/GridDCLoad.mos"
+        "Simulate and plot"),
+Documentation(info="<html>
+<p>
+This model illustrates the use of a model for inductive load. The circuit on the left hand side
+uses an inductive load, whereas the circuit on the right hand side uses a resistor and inductance in
+series.
+The parameters of the inductor and resistor are such that the real power and the phase angle are
+identical (up to the numerical precision of the parameters) for the two systems.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+January 2, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GridDCLoad;
diff --git a/AixLib/Electrical/AC/OnePhase/Examples/package.mo b/AixLib/Electrical/AC/OnePhase/Examples/package.mo
new file mode 100644
index 0000000000..835417a40c
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Examples/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Electrical.AC.OnePhase;
+package Examples "Package with example models"
+extends Modelica.Icons.ExamplesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase\">
+AixLib.Electrical.AC.OnePhase</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/OnePhase/Examples/package.order b/AixLib/Electrical/AC/OnePhase/Examples/package.order
new file mode 100644
index 0000000000..b4069ef5bf
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Examples/package.order
@@ -0,0 +1,2 @@
+GeneratorLoadGrid
+GridDCLoad
diff --git a/AixLib/Electrical/AC/OnePhase/Interfaces/Terminal_n.mo b/AixLib/Electrical/AC/OnePhase/Interfaces/Terminal_n.mo
new file mode 100644
index 0000000000..f8ac6d5746
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Interfaces/Terminal_n.mo
@@ -0,0 +1,40 @@
+within AixLib.Electrical.AC.OnePhase.Interfaces;
+connector Terminal_n "Terminal n for AC one phase systems"
+  extends AixLib.Electrical.Interfaces.Terminal(
+    redeclare replaceable package PhaseSystem =
+        AixLib.Electrical.PhaseSystems.OnePhase);
+  annotation (defaultComponentName = "term_p",
+  Documentation(info="<html>
+<p>Electric connector for AC one phase systems.</p>
+</html>"),
+  Icon(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={           Text(
+          extent={{-60,60},{60,-60}},
+          textColor={255,255,255},
+          pattern=LinePattern.None,
+          textString=""),                    Polygon(
+          points={{0,100},{-100,0},{0,-100},{100,0},{0,100}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}),
+  Diagram(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+        Text(
+          extent={{-120,120},{100,60}},
+          textColor={0,120,120},
+          textString="%name"),
+        Text(
+          extent={{14,16},{114,-84}},
+          textColor={255,255,255},
+          pattern=LinePattern.None,
+          textString=""),                    Polygon(
+          points={{-50,50},{-100,0},{-50,-50},{0,0},{-50,50}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal_n;
diff --git a/AixLib/Electrical/AC/OnePhase/Interfaces/Terminal_p.mo b/AixLib/Electrical/AC/OnePhase/Interfaces/Terminal_p.mo
new file mode 100644
index 0000000000..59afc1b495
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Interfaces/Terminal_p.mo
@@ -0,0 +1,40 @@
+within AixLib.Electrical.AC.OnePhase.Interfaces;
+connector Terminal_p "Terminal p for AC one phase systems"
+  extends AixLib.Electrical.Interfaces.Terminal(
+    redeclare replaceable package PhaseSystem =
+        AixLib.Electrical.PhaseSystems.OnePhase);
+  annotation (defaultComponentName = "term_p",
+  Documentation(info="<html>
+<p>Electric connector for AC one phase systems.</p>
+</html>"),
+  Icon(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={           Text(
+          extent={{-60,60},{60,-60}},
+          textColor={255,255,255},
+          pattern=LinePattern.None,
+          textString=""),                    Polygon(
+          points={{0,100},{-100,0},{0,-100},{100,0},{0,100}},
+          lineColor={0,120,120},
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid)}),
+  Diagram(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+        Text(
+          extent={{-120,120},{100,60}},
+          textColor={0,120,120},
+          textString="%name"),
+        Text(
+          extent={{14,16},{114,-84}},
+          textColor={255,255,255},
+          pattern=LinePattern.None,
+          textString=""),                    Polygon(
+          points={{50,50},{0,0},{50,-50},{100,0},{50,50}},
+          lineColor={0,120,120},
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal_p;
diff --git a/AixLib/Electrical/AC/OnePhase/Interfaces/package.mo b/AixLib/Electrical/AC/OnePhase/Interfaces/package.mo
new file mode 100644
index 0000000000..fa7f9764da
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Interfaces/package.mo
@@ -0,0 +1,22 @@
+within AixLib.Electrical.AC.OnePhase;
+package Interfaces "Package with interfaces for one phase AC systems"
+  extends Modelica.Icons.InterfacesPackage;
+
+
+  annotation (Documentation(info="<html>
+<p>
+This package contains connectors that are used by the models in the
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase\">AixLib.Electrical.AC.OnePhase</a> package.
+The connectors extend the basic connectors
+<a href=\"modelica://AixLib.Electrical.Interfaces.Terminal\">AixLib.Electrical.Interfaces.Terminal</a>
+and define a new graphical icon in order to be distinguished by connectors of other electrical systems (e.g. DC systems).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Interfaces;
diff --git a/AixLib/Electrical/AC/OnePhase/Interfaces/package.order b/AixLib/Electrical/AC/OnePhase/Interfaces/package.order
new file mode 100644
index 0000000000..d23ecfc486
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Interfaces/package.order
@@ -0,0 +1,2 @@
+Terminal_n
+Terminal_p
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine.mo b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine.mo
new file mode 100644
index 0000000000..286e0efbf7
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine.mo
@@ -0,0 +1,135 @@
+within AixLib.Electrical.AC.OnePhase.Lines.Examples;
+model ACLine
+  "Test model for a single phase line that uses commercial cable information"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage E(      definiteReference=true,
+    f=60,
+    V=120) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  Line line_1(
+    P_nominal=5000,
+    l=2000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    V_nominal=120) "Resistive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+  Line line_2a(
+    P_nominal=5000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    l=1000,
+    V_nominal=120) "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  Loads.Impedance R2(
+    R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Line line_2b(
+    P_nominal=5000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    l=1000,
+    V_nominal=120) "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-32,-30},{-12,-10}})));
+  Line line_3a(
+    P_nominal=5000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    l=4000,
+    V_nominal=120) "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  Line line_3b(
+    P_nominal=5000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    l=4000,
+    V_nominal=120) "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-70},{-40,-50}})));
+  Loads.Impedance R3(
+    R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-60},{20,-40}})));
+  Line line_sc(
+    P_nominal=5000,
+    l=2000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    V_nominal=120) "Line that connects the source and the short circuit"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Loads.Impedance load_sc(R=0) "Short circuit"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+equation
+  connect(line_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-40,0},{-24,0},{-24,6.66134e-16},{-4.44089e-16,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_1.terminal_n) annotation (Line(
+      points={{-80,4.44089e-16},{-60,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_2a.terminal_n) annotation (Line(
+      points={{-80,4.44089e-16},{-70,4.44089e-16},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_2a.terminal_p, line_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-32,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-12,-20},{0,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-40},{-20,-40},{-20,-50},{0,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-60},{-20,-60},{-20,-50},{-5.55112e-16,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-40},{-60,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-60},{-60,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_sc.terminal_p, load_sc.terminal) annotation (Line(
+      points={{-40,30},{-4.44089e-16,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a line model to connect
+a source to a load that uses commercial cable information.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the impedance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations,
+however the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draws the same current.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_L.mo b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_L.mo
new file mode 100644
index 0000000000..32daece346
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_L.mo
@@ -0,0 +1,107 @@
+within AixLib.Electrical.AC.OnePhase.Lines.Examples;
+model ACLine_L "Test model for a single phase inductive line"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Inductance Lbase=10/2/Modelica.Constants.pi/60
+    "Base value for the line inductances";
+  Sources.FixedVoltage E(      definiteReference=true,
+    f=60,
+    V=120) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Loads.Impedance R2(
+    R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Loads.Impedance R3(
+    R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-62},{20,-42}})));
+  Loads.Impedance load_sc(R=0) "Short circuit"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  TwoPortInductance Lline_sc(L=Lbase)
+    "Inductive line connected to the short circuit"
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+  TwoPortInductance Lline_1(L=Lbase) "Inductive line connected to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  TwoPortInductance Lline_2a(L=0.5*Lbase) "Inductive line connected to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  TwoPortInductance Lline_2b(L=0.5*Lbase) "Inductive line connected to load 2"
+    annotation (Placement(transformation(extent={{-36,-30},{-16,-10}})));
+  TwoPortInductance Lline_3(L=2*Lbase) "Inductive line connected to load 3"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  TwoPortInductance Lline_3b(L=2*Lbase) "Inductive line connected to load 3"
+    annotation (Placement(transformation(extent={{-60,-70},{-40,-50}})));
+equation
+  connect(E.terminal, Lline_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_sc.terminal_p, load_sc.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Lline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Lline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_2a.terminal_p, Lline_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-36,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-16,-20},{-4.44089e-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Lline_3.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-40},{-60,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Lline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-60},{-60,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_3.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-40},{-20,-40},{-20,-52},{0,-52}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-60},{-20,-60},{-20,-52},{0,-52}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-06),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_L.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a purely inductive line model to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the inductance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations,
+however the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draw the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_L;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_R.mo b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_R.mo
new file mode 100644
index 0000000000..2d7fc116c6
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_R.mo
@@ -0,0 +1,105 @@
+within AixLib.Electrical.AC.OnePhase.Lines.Examples;
+model ACLine_R "Test model for a single phase resistive line"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage E(definiteReference=true,
+    f=60,
+    V=120) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Loads.Impedance R2(
+    R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Loads.Impedance R3(
+    R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-70},{20,-50}})));
+  Loads.Impedance sc_load(R=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  TwoPortResistance Rline_sc(R=10, useHeatPort=false)
+    "Resistive line that connects to the short circuit"
+    annotation (Placement(transformation(extent={{-60,60},{-40,40}})));
+  TwoPortResistance Rline_1(R=10) "Resistive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  TwoPortResistance Rline_2a(R=5) "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  TwoPortResistance Rline_2b(R=5) "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-36,-30},{-16,-10}})));
+  TwoPortResistance Rline_3a(R=20) "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  TwoPortResistance Rline_3b(R=20) "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+equation
+  connect(E.terminal, Rline_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_sc.terminal_p, sc_load.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2a.terminal_p, Rline_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-36,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-16,-20},{-4.44089e-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-70},{-60,-70}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-70},{-20,-70},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_R.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a resistive line model to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the resistance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations,
+however the equivalent resistance between each load and the source is the same.
+Since the equivalent resistances are the same, each load draw the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_R;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_RL.mo b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_RL.mo
new file mode 100644
index 0000000000..d386e877f4
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACLine_RL.mo
@@ -0,0 +1,93 @@
+within AixLib.Electrical.AC.OnePhase.Lines.Examples;
+model ACLine_RL "Test model for a single phase inductive-resistive line"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Resistance Rbase=10
+    "Base value for the line resistance";
+  parameter Modelica.Units.SI.Inductance Lbase=Rbase/2/Modelica.Constants.pi/60
+    "Base value for the line inductance";
+  Sources.FixedVoltage E(      definiteReference=true,
+    f=60,
+    V=120) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance load_sc_1(R=0) "Short circuit 1"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  Loads.Impedance load_sc_2(R=0) "Short circuit 2"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  TwoPortRL RL_2(R=Rbase, L=Lbase)
+    "Resistive-Inductive line connected to short circuit 2"
+    annotation (Placement(transformation(extent={{-48,-10},{-28,10}})));
+  TwoPortResistance R_1(R=Rbase) "Resistance line connected to short circuit 1"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  TwoPortInductance L_1(L=Lbase) "Inductance line connected to short circuit 1"
+    annotation (Placement(transformation(extent={{-30,20},{-10,40}})));
+  TwoPortRL RL_3(
+    R=Rbase,
+    L=Lbase,
+    mode=AixLib.Electrical.Types.Load.FixedZ_dynamic,
+    i_start={0,0})
+    "Dynamic resistive-inductive line connected to short circuit 3"
+    annotation (Placement(transformation(extent={{-48,-40},{-28,-20}})));
+  Loads.Impedance load_sc_3(R=0) "Short circuit 3"
+    annotation (Placement(transformation(extent={{0,-40},{20,-20}})));
+equation
+  connect(E.terminal, R_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(R_1.terminal_p, L_1.terminal_n) annotation (Line(
+      points={{-40,30},{-30,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(L_1.terminal_p, load_sc_1.terminal) annotation (Line(
+      points={{-10,30},{0,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RL_2.terminal_n) annotation (Line(
+      points={{-80,0},{-48,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RL_2.terminal_p, load_sc_2.terminal) annotation (Line(
+      points={{-28,0},{0,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RL_3.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-30},{-48,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RL_3.terminal_p, load_sc_3.terminal) annotation (Line(
+      points={{-28,-30},{0,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-06),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_RL.mos"
+        "Simulate and plot"),
+  Documentation(revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a resistive-inductive line model to connect
+a source to a load.
+</p>
+<p>
+The model has three loads <code>load_sc_1</code>, <code>load_sc_2</code>,
+and <code>load_sc_3</code> representing short circuits <i>R=0</i>.
+The current that flows through the load depends on the impedance of the line.
+</p>
+<p>
+Each load is connected to the source with different configurations,
+however the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draw the same current.
+</p>
+<p>
+<b>Note:</b>
+The line model <code>RL_3</code> is the same as <code>RL_2</code> but it uses
+dynamic phasors.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_RL;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACSimpleGrid.mo b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACSimpleGrid.mo
new file mode 100644
index 0000000000..36adca2404
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Examples/ACSimpleGrid.mo
@@ -0,0 +1,82 @@
+within AixLib.Electrical.AC.OnePhase.Lines.Examples;
+model ACSimpleGrid "Test model for a network model"
+  extends Modelica.Icons.Example;
+  Network network(
+    redeclare AixLib.Electrical.Transmission.Grids.TestGrid2Nodes grid,
+    V_nominal=120)
+    "Network model that represents the connection between the source and the load"
+    annotation (Placement(transformation(extent={{20,-10},{0,10}})));
+  Loads.Inductive load(
+    mode=Types.Load.VariableZ_P_input,
+    V_nominal=120) "Load connected to the network"
+    annotation (Placement(transformation(extent={{-28,10},{-48,30}})));
+  Sources.FixedVoltage E(f=60, V=120) "Voltage source"
+                                          annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={-70,0})));
+  Modelica.Blocks.Sources.Ramp load_inputs(
+    height=5000,
+    duration=2,
+    offset=-2000,
+    startTime=0.5) "Input signal for the power consumption of the loads"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+equation
+  connect(load.terminal, network.terminal[2]) annotation (Line(
+      points={{-28,20},{-20,20},{-20,4.44089e-16},{-4.44089e-16,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, network.terminal[1]) annotation (Line(
+      points={{-60,-8.88178e-16},{-56,-8.88178e-16},{-56,4.44089e-16},{-4.44089e-16,
+          4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load_inputs.y, load.Pow) annotation (Line(
+      points={{-59,30},{-54,30},{-54,20},{-48,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACSimpleGrid.mos"
+        "Simulate and plot"),
+Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Removed binding of <code>P_nominal</code> as
+this parameter is disabled and assigned a value
+in the <code>initial equation</code> section.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a network model to connect
+a source to a load. In this simple case the network has two nodes
+that are connected by a commercial line cable.
+</p>
+<p>
+At the beginning of the simulation the load consumes power while at the
+and it produces power. The voltage at the load at the beginning is lower
+than the nominal RMS voltage (120 V) while at the end of the simulation it is higher.
+The voltage drop and increase are due to the presence of the cable between
+the source and the load.
+</p>
+<p>
+The network uses cables of the type <code>LowVoltageCable.Cu35</code> with
+a length of <i>200</i> m.
+</p>
+<p>
+The picture below describes the grid topology.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/testGrid2Nodes.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACSimpleGrid;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Examples/package.mo b/AixLib/Electrical/AC/OnePhase/Lines/Examples/package.mo
new file mode 100644
index 0000000000..aac5a0a1c7
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.OnePhase.Lines;
+package Examples "Package with example models"
+extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Lines\">
+AixLib.Electrical.AC.OnePhase.Lines</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Examples/package.order b/AixLib/Electrical/AC/OnePhase/Lines/Examples/package.order
new file mode 100644
index 0000000000..cc13c92dd1
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Examples/package.order
@@ -0,0 +1,5 @@
+ACLine
+ACLine_L
+ACLine_R
+ACLine_RL
+ACSimpleGrid
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Line.mo b/AixLib/Electrical/AC/OnePhase/Lines/Line.mo
new file mode 100644
index 0000000000..b60c47b75d
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Line.mo
@@ -0,0 +1,109 @@
+within AixLib.Electrical.AC.OnePhase.Lines;
+model Line "Model of an electrical line"
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialLine(
+    V_nominal(start = 110),
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n,
+    redeclare replaceable Interfaces.Terminal_p terminal_p,
+    commercialCable = AixLib.Electrical.Transmission.Functions.selectCable_low(P_nominal, V_nominal));
+protected
+  replaceable TwoPortRL line(
+    R=R/3,
+    L=L/3,
+    mode=modelMode) constrainedby
+    AixLib.Electrical.Transmission.BaseClasses.PartialTwoPortRLC(
+      useHeatPort=true,
+      M=M,
+      T_ref=T_ref) "Model of the line"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+
+equation
+  connect(cableTemp.port, line.heatPort)       annotation (Line(
+      points={{-40,22},{-28,22},{-28,-10},{4.44089e-16,-10}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(line.terminal_n, terminal_n)       annotation (Line(
+      points={{-10,4.44089e-16},{-48,4.44089e-16},{-48,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_p, line.terminal_p)       annotation (Line(
+      points={{100,0},{56,0},{56,4.44089e-16},{10,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  annotation (
+defaultComponentName="line",
+ Icon(graphics={
+        Ellipse(
+          extent={{-70,10},{-50,-10}},
+          lineColor={0,0,0},
+          fillColor={0,94,94},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-60,10},{60,-10}},
+          fillColor={0,94,94},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{50,10},{70,-10}},
+          lineColor={0,0,0},
+          fillColor={255,128,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-70,0},{-90,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,10},{60,10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,-10},{60,-10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{96,0},{60,0}},
+          color={0,0,0},
+          smooth=Smooth.None)}),
+    Documentation(
+info="<html>
+<p>
+This model represents an AC single phase cable. The model is based on
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Lines.TwoPortRLC\">
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortRLC</a>
+and provides functionalities to parametrize the values of <i>R</i>, <i>L</i> and <i>C</i>,
+either using commercial cables or using default values.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Added <code>replaceable</code> to terminal redeclaration as they are redeclared by
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Line\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Line</a>.
+</li>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Corrected wrong assignment of parameter <code>mode</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/571\">#571</a>.
+</li>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Moved here the default declaration of the parameter <code>commercialCable</code>.<br/>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px;\">
+<span style=\" font-family:'Courier New,courier';\">commercialCable = </span>
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\"> AixLib.Electrical.Transmission.Functions.selectCable_low</span>
+<span style=\" font-family:'Courier New,courier';\">(P_nominal, V_nominal)</span>
+</p>
+</li>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Line;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/Network.mo b/AixLib/Electrical/AC/OnePhase/Lines/Network.mo
new file mode 100644
index 0000000000..c42c28ffb9
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/Network.mo
@@ -0,0 +1,59 @@
+within AixLib.Electrical.AC.OnePhase.Lines;
+model Network "Single phase AC network"
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialNetwork(
+    V_nominal(start = 110),
+    redeclare Interfaces.Terminal_p terminal,
+    redeclare replaceable Transmission.Grids.TestGrid2Nodes grid,
+    redeclare Line lines(
+      commercialCable=grid.cables,
+      each use_C=use_C,
+      each modelMode=modelMode));
+  parameter Boolean use_C = false "If true, model the cable capacity"
+    annotation(Dialog(tab="Model", group="Assumptions"));
+  parameter AixLib.Electrical.Types.Load modelMode=Types.Load.FixedZ_steady_state
+    "Select between steady state and dynamic model" annotation (Dialog(
+      tab="Model",
+      group="Assumptions",
+      enable=use_C), choices(choice=AixLib.Electrical.Types.Load.FixedZ_steady_state
+        "Steady state", choice=AixLib.Electrical.Types.Load.FixedZ_dynamic "Dynamic"));
+  Modelica.Units.SI.Voltage VAbs[grid.nNodes] "RMS voltage of the grid nodes";
+equation
+  for i in 1:grid.nLinks loop
+    connect(lines[i].terminal_p, terminal[grid.fromTo[i,1]]);
+    connect(lines[i].terminal_n, terminal[grid.fromTo[i,2]]);
+  end for;
+
+  for i in 1:grid.nNodes loop
+    VAbs[i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal[i].v);
+  end for;
+
+  annotation (
+    defaultComponentName="net",
+Icon(graphics={             Line(
+          points={{-92,-60},{-72,-20},{-52,-60},{-32,-100},{-12,-60}},
+          color={0,0,0},
+          smooth=Smooth.Bezier)}), Documentation(info="<html>
+<p>
+This model represents a generalized electrical AC single phase network.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.BaseClasses.PartialNetwork\">
+AixLib.Electrical.Transmission.BaseClasses.PartialNetwork</a>
+for information about the network model.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.Grids.PartialGrid\">
+AixLib.Electrical.Transmission.Grids.PartialGrid</a>
+for more information about the topology of the network, such as
+the number of nodes, how they are connected, and the length of each connection.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Network;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/TwoPortInductance.mo b/AixLib/Electrical/AC/OnePhase/Lines/TwoPortInductance.mo
new file mode 100644
index 0000000000..c07dbd5943
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/TwoPortInductance.mo
@@ -0,0 +1,75 @@
+within AixLib.Electrical.AC.OnePhase.Lines;
+model TwoPortInductance
+  "Model of an inductive element with two electrical ports"
+  extends
+    AixLib.Electrical.Transmission.BaseClasses.PartialTwoPortInductance(
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n,
+    redeclare replaceable Interfaces.Terminal_p terminal_p);
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.VariableZ_y_input)=
+    AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Type of model (e.g., steady state, dynamic, prescribed power consumption, etc.)"
+    annotation (Evaluate=true, Dialog(group="Modeling assumption"));
+protected
+  Modelica.Units.SI.AngularVelocity omega
+    "Frequency of the quasi-stationary sine waves";
+  Modelica.Units.SI.Angle theRef "Absolute angle of rotating reference system";
+
+equation
+  theRef = PhaseSystem_p.thetaRef(terminal_p.theta);
+  omega = der(theRef);
+
+  if mode==AixLib.Electrical.Types.Load.FixedZ_dynamic then
+    // Dynamics of the system
+    der(L*terminal_p.i) + L*omega*PhaseSystem_p.j(terminal_p.i) = terminal_p.v - terminal_n.v;
+
+  else
+    // Steady state relationship
+    L*omega*PhaseSystem_p.j(terminal_p.i) = terminal_p.v - terminal_n.v;
+
+  end if;
+
+  annotation (
+    defaultComponentName="lineL",
+  Diagram(graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,0}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,0}),
+          Line(points={{70,0},{90,0}}, color={0,0,0})}),     Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+        graphics={
+          Text(
+            extent={{-140,80},{140,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+This model represents an inductance that connects two AC one phase interfaces.
+This model can be used to represent a single phase cable in a AC grid.
+</p>
+<p>
+The model represents the lumped inductance as shown in the figure below.
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/OnePhase/Lines/twoPortL.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2019, by Michael Wetter:<br/>
+Added <code>replaceable</code> for terminal.
+</li>
+<li>
+May 26, 2016, by Michael Wetter:<br/>
+Moved function call to <code>PhaseSystem.thetaRef</code> out of
+derivative operator as this is not yet supported by JModelica.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortInductance;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/TwoPortRL.mo b/AixLib/Electrical/AC/OnePhase/Lines/TwoPortRL.mo
new file mode 100644
index 0000000000..c2271aa9f8
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/TwoPortRL.mo
@@ -0,0 +1,104 @@
+within AixLib.Electrical.AC.OnePhase.Lines;
+model TwoPortRL
+  "Model of a resistive-inductive element with two electrical ports"
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialTwoPortRLC(
+    final V_nominal=0,
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n,
+    redeclare replaceable Interfaces.Terminal_p terminal_p,
+    final C=0);
+  parameter Modelica.Units.SI.Current i_start[PhaseSystem_p.n]=zeros(
+      PhaseSystem_p.n)
+    "Initial current phasor of the line (positive if entering from terminal p)"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.FixedZ_dynamic)=
+    AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Type of model (e.g., steady state, dynamic, prescribed power consumption, etc.)"
+    annotation (Evaluate=true, Dialog(group="Modeling assumption"));
+protected
+  Modelica.Units.SI.Current i_p[2](start=i_start, each stateSelect=StateSelect.prefer)
+    "Current phasor at terminal p";
+  Modelica.Units.SI.AngularVelocity omega
+    "Frequency of the quasi-stationary sine waves";
+  Modelica.Units.SI.Angle theRef "Absolute angle of rotating reference system";
+
+initial equation
+  if mode==AixLib.Electrical.Types.Load.FixedZ_dynamic then
+    i_p = i_start;
+  end if;
+equation
+  theRef = PhaseSystem_p.thetaRef(terminal_p.theta);
+  omega = der(theRef);
+
+  terminal_p.i = - terminal_n.i;
+  i_p = terminal_p.i;
+
+  if mode==AixLib.Electrical.Types.Load.FixedZ_dynamic then
+    // Dynamics of the system
+    der(L*i_p) + L*omega*PhaseSystem_p.j(i_p) +
+      i_p*diagonal(ones(PhaseSystem_p.n)*R_actual)
+       = terminal_p.v - terminal_n.v;
+
+  else
+    // steady state relationship
+    L*omega*PhaseSystem_p.j(i_p) +
+      i_p*diagonal(ones(PhaseSystem_p.n)*R_actual)
+      = terminal_p.v - terminal_n.v;
+  end if;
+
+  // Joule losses
+  LossPower = R_actual*(i_p[1]^2 + i_p[2]^2);
+
+  annotation (
+defaultComponentName="lineRL",
+Diagram(graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,0}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,0}),
+          Line(points={{70,0},{90,0}}, color={0,0,0})}),     Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                                                  graphics={
+          Text(
+            extent={{-140,80},{140,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+This model represents a resistance and an inductance connected in series with
+two AC one phase interfaces. This model can be used
+to represent a single phase cable in a AC grid.
+</p>
+<p>
+The model represents the lumped RL cable as shown in the figure below.
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/OnePhase/Lines/twoPortRL.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2019, by Michael Wetter:<br/>
+Added <code>replaceable</code> for terminal.
+</li>
+<li>
+May 26, 2016, by Michael Wetter:<br/>
+Moved function call to <code>PhaseSystem.thetaRef</code> out of
+derivative operator as this is not yet supported by JModelica.
+</li>
+<li>
+March 9, 2015, by Marco Bonvini:<br/>
+Added parameter for start value of the current.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added equation that represents Joule losses
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRL;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/TwoPortRLC.mo b/AixLib/Electrical/AC/OnePhase/Lines/TwoPortRLC.mo
new file mode 100644
index 0000000000..74831c1250
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/TwoPortRLC.mo
@@ -0,0 +1,118 @@
+within AixLib.Electrical.AC.OnePhase.Lines;
+model TwoPortRLC "Model of an RLC element with two electrical ports"
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialTwoPortRLC(
+    V_nominal(start = 110),
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n(
+      redeclare package PhaseSystem = PhaseSystem_n),
+    redeclare replaceable Interfaces.Terminal_p terminal_p(
+      redeclare package PhaseSystem = PhaseSystem_p));
+  parameter Modelica.Units.SI.Voltage Vc_start[2]={V_nominal,0}
+    "Initial voltage phasor of the capacitance located in the middle of the line"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.FixedZ_dynamic)=
+    AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Type of model (e.g., steady state, dynamic, prescribed power consumption, etc.)"
+    annotation (Evaluate=true, Dialog(group="Modeling assumption"));
+protected
+  Modelica.Units.SI.Voltage Vc[2](start=Vc_start, each stateSelect=StateSelect.prefer)
+    "Voltage of the Capacitance located in the middle of the line";
+  Modelica.Units.SI.Current Ic[2]
+    "Currenbt of the capacitance located in the middle of the line";
+  Modelica.Units.SI.AngularVelocity omega
+    "Frequency of the quasi-stationary sine waves";
+  Modelica.Units.SI.Angle theRef "Absolute angle of rotating reference system";
+
+initial equation
+  if C > 0 and mode == AixLib.Electrical.Types.Load.FixedZ_dynamic then
+    Vc = Vc_start;
+  end if;
+equation
+  theRef = PhaseSystem_p.thetaRef(terminal_p.theta);
+  omega = der(theRef);
+
+  terminal_p.i + terminal_n.i = Ic;
+
+  L/2*omega*AixLib.Electrical.PhaseSystems.OnePhase.j(terminal_p.i) +
+    terminal_p.i*diagonal(ones(PhaseSystem_p.n)*R_actual/2) = terminal_p.v - Vc;
+  L/2*omega*AixLib.Electrical.PhaseSystems.OnePhase.j(terminal_n.i) +
+    terminal_n.i*diagonal(ones(PhaseSystem_n.n)*R_actual/2) = terminal_n.v - Vc;
+
+  if C > 0 then
+    if mode == AixLib.Electrical.Types.Load.FixedZ_dynamic then
+      // Dynamics of the system
+      C*der(Vc) + omega*C*AixLib.Electrical.PhaseSystems.OnePhase.j(Vc) = Ic;
+    else
+      // steady state relationship
+      omega*C*AixLib.Electrical.PhaseSystems.OnePhase.j(Vc) = Ic;
+    end if;
+  else
+    // No capacitive effect, the voltage in the middle of the line is the linear
+    // interpolation of the two phasors
+    Vc = (terminal_p.v + terminal_n.v)/2;
+  end if;
+
+  // Joule losses
+  LossPower = R_actual/2*(terminal_p.i[1]^2 + terminal_p.i[2]^2) +
+              R_actual/2*(terminal_n.i[1]^2 + terminal_n.i[2]^2);
+
+  annotation (
+  defaultComponentName="lineRLC",
+Diagram(graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,0}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,0}),
+          Line(points={{70,0},{90,0}}, color={0,0,0})}),     Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                                                  graphics={
+          Text(
+            extent={{-140,80},{140,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+This model represents a series of two resistive-inductive impedances and a capacitance
+that connects two AC single phase interfaces.
+This model can be used to represent a cable in a AC grid.
+</p>
+<p>
+The model represents the lumped resistances and capacity, as a T-model, as shown in the figure below.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/OnePhase/Lines/twoPortRLC.png\"/>
+</p>
+<p>
+As can be seen in the figure, the resistance <i>R</i> and the inductance <i>L</i> are split in two halves
+and the capacitance is located in the center.
+The capacitance in the center is optional. If it is not present, set the
+parameter <code>C=0</code>.
+The model is either dynamic or static depending on the
+presence of the capacitive effect.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Added <code>replaceable</code> to terminal redeclaration as they are redeclared by
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortRLC\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortRLC</a>.
+</li>
+<li>
+May 26, 2016, by Michael Wetter:<br/>
+Moved function call to <code>PhaseSystem.thetaRef</code> out of
+derivative operator as this is not yet supported by JModelica.
+</li>
+<li>
+March 9, 2015, by Marco Bonvini:<br/>
+Added parameter for start value of the voltage.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRLC;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/TwoPortResistance.mo b/AixLib/Electrical/AC/OnePhase/Lines/TwoPortResistance.mo
new file mode 100644
index 0000000000..6726649953
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/TwoPortResistance.mo
@@ -0,0 +1,57 @@
+within AixLib.Electrical.AC.OnePhase.Lines;
+model TwoPortResistance "Model of a resistance with two electrical ports"
+  extends
+    AixLib.Electrical.Transmission.BaseClasses.PartialTwoPortResistance(
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal_n,
+    redeclare replaceable Interfaces.Terminal_p terminal_p);
+equation
+  terminal_p.v - terminal_n.v = terminal_p.i*diagonal(ones(PhaseSystem_p.n)*R_actual);
+
+  // Joule losses
+  LossPower = R_actual*(terminal_p.i[1]^2 + terminal_p.i[2]^2);
+  annotation (
+    defaultComponentName="lineR",
+    Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+            -100},{100,100}}),
+                      graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,0}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,0}),
+          Line(points={{70,0},{90,0}}, color={0,0,0})}),     Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                                                  graphics={
+          Text(
+            extent={{-140,80},{140,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(
+info="<html>
+<p>
+This model represents a resistance that connects two AC one phase interfaces.
+This model can be used to represent a single phase cable in a AC grid.
+</p>
+<p>
+The model represents the lumped resistance as shown in the figure below.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/OnePhase/Lines/twoPortR.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2019, by Michael Wetter:<br/>
+Added <code>replaceable</code> for terminal.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added equation that represents Joule losses
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortResistance;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/package.mo b/AixLib/Electrical/AC/OnePhase/Lines/package.mo
new file mode 100644
index 0000000000..dfb40c57c2
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/package.mo
@@ -0,0 +1,35 @@
+within AixLib.Electrical.AC.OnePhase;
+package Lines "Package with models for AC electrical lines"
+  extends Modelica.Icons.Package;
+
+
+annotation (Icon(graphics={
+      Ellipse(
+        extent={{40,8},{16,-28}},
+        lineColor={0,0,0},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),
+      Line(
+        points={{28,8},{-54,8},{-64,8},{-72,-10},{-64,-28},{-52,-28},{28,-28}},
+        color={0,0,0},
+        smooth=Smooth.Bezier),
+      Line(
+        points={{-70,-10},{-88,-10}},
+        color={0,0,0},
+        smooth=Smooth.None),
+      Line(
+        points={{54,-10},{28,-10}},
+        color={0,0,0},
+        smooth=Smooth.None)}), Documentation(info="<html>
+<p>
+This package contains models for transmission lines and electrical networks.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Lines;
diff --git a/AixLib/Electrical/AC/OnePhase/Lines/package.order b/AixLib/Electrical/AC/OnePhase/Lines/package.order
new file mode 100644
index 0000000000..c13075e17a
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Lines/package.order
@@ -0,0 +1,7 @@
+Line
+Network
+TwoPortInductance
+TwoPortRL
+TwoPortRLC
+TwoPortResistance
+Examples
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Capacitive.mo b/AixLib/Electrical/AC/OnePhase/Loads/Capacitive.mo
new file mode 100644
index 0000000000..ee2be357b2
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Capacitive.mo
@@ -0,0 +1,230 @@
+within AixLib.Electrical.AC.OnePhase.Loads;
+model Capacitive "Model of a capacitive and resistive load"
+  extends AixLib.Electrical.Interfaces.CapacitiveLoad(
+    redeclare package PhaseSystem = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal,
+    V_nominal(start = 110));
+
+protected
+  Modelica.Units.SI.Angle theRef "Absolute angle of rotating reference system";
+
+initial equation
+  if mode == AixLib.Electrical.Types.Load.FixedZ_dynamic then
+    // q = Y[2]*{V_nominal, 0}/omega;
+    // Steady state initialization
+    der(q) = zeros(PhaseSystem.n);
+  end if;
+equation
+  theRef = PhaseSystem.thetaRef(terminal.theta);
+  omega = der(theRef);
+
+  if mode == AixLib.Electrical.Types.Load.FixedZ_dynamic then
+
+    // Use the dynamic phasorial representation
+    Y[1] = -(P_nominal/pf)*pf/V_nominal^2;
+    Y[2] = -(P_nominal/pf)*Modelica.Fluid.Utilities.regRoot(1 - pf^2, delta=0.001)/V_nominal^2;
+
+    // Electric charge
+    q = Y[2]*{v[1], v[2]}/omega;
+
+    // Dynamics of the system
+    der(q) + omega*j(q) + Y[1]*v = i;
+
+  else
+
+    // Use the power specified by the parameter or inputs
+    if linearized then
+      i[1] = -homotopy(actual= (v[2]*Q + v[1]*P)/(V_nominal^2), simplified= v[1]*Modelica.Constants.eps*1e3);
+      i[2] = -homotopy(actual= (v[2]*P - v[1]*Q)/(V_nominal^2), simplified= v[2]*Modelica.Constants.eps*1e3);
+    else
+      if initMode == AixLib.Electrical.Types.InitMode.zero_current then
+        i[1] = -homotopy(actual=(v[2]*Q + v[1]*P)/(v[1]^2 + v[2]^2), simplified=0.0);
+        i[2] = -homotopy(actual=(v[2]*P - v[1]*Q)/(v[1]^2 + v[2]^2), simplified=0.0);
+      else
+        i[1] = -homotopy(actual=(v[2]*Q + v[1]*P)/(v[1]^2 + v[2]^2), simplified=(v[2]*Q + v[1]*P)/(V_nominal^2));
+        i[2] = -homotopy(actual=(v[2]*P - v[1]*Q)/(v[1]^2 + v[2]^2), simplified=(v[2]*P - v[1]*Q)/(V_nominal^2));
+      end if;
+
+    end if;
+
+    Y = {0, 0};
+    q = {0, 0};
+
+  end if;
+
+  annotation (
+    defaultComponentName="loa",
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+            -100},{100,100}}),      graphics={
+        Rectangle(
+          extent={{-80,40},{80,-40}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{0,28},{0,-28}},
+          color={0,0,0},
+          origin={48,0},
+          rotation=180),
+        Line(
+          points={{0,28},{0,-28}},
+          color={0,0,0},
+          origin={40,0},
+          rotation=180),
+          Line(points={{-42,-5.14335e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-2,0},
+          rotation=180),
+          Line(points={{-26,-3.18398e-15},{0,0}},
+                                         color={0,0,0},
+          origin={48,0},
+          rotation=180),
+          Line(points={{-10,-1.22461e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-42,1},
+          rotation=90),
+        Text(
+          extent={{-120,80},{120,40}},
+          textColor={0,0,0},
+          textString="%name")}), Documentation(info="<html>
+
+<p>
+Model of an capacitive load. It may be used to model a bank of capacitors.
+</p>
+<p>
+The model computes the complex power vector as
+<p align=\"center\" style=\"font-style:italic;\">
+S = P + jQ = V &sdot; i<sup>*</sup>
+</p>
+<p>
+where <i>V</i> is the voltage phasor and <i>i<sup>*</sup></i> is the complex
+conjugate of the current phasor. The voltage and current phasors are shifted
+by an angle <i>&phi;</i>.
+</p>
+
+<p>
+The load model takes as input the power consumed by the inductive load and
+the power factor <i>pf=cos(&phi;)</i>. The power
+can be either fixed using the parameter <code>P_nominal</code>, or
+it is possible to specify a variable power using the inputs <code>y</code> or
+<code>Pow</code>.
+
+The power factor can be either specified by the parameter <code>pf</code>
+or using the input variable <code>pf_in</code>.
+
+The different modes can be selected with the parameter
+<code>mode</code> and <code>use_pf_in</code>, see <a href=\"modelica://AixLib.Electrical.Interfaces.Load\">
+AixLib.Electrical.Interfaces.Load</a> and
+<a href=\"modelica://AixLib.Electrical.Interfaces.CapacitiveLoad\">
+AixLib.Electrical.Interfaces.CapacitiveLoad</a> for more information.
+</p>
+
+<p>
+Given the active power <i>P</i> and the power factor <i>pf</i> the complex
+power <i>Q</i> is computed as
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+Q = - P  tan(arccos(pf)).
+</p>
+
+<p>
+The equations of the model can be rewritten as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>1</sub> = (P V<sub>1</sub> + Q V<sub>2</sub>)/(V<sub>1</sub><sup>2</sup> + V<sub>2</sub><sup>2</sup>),
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>2</sub> = (P V<sub>2</sub> - Q V<sub>1</sub>)/(V<sub>1</sub><sup>2</sup> + V<sub>2</sub><sup>2</sup>),
+</p>
+
+<p>
+where <i>i<sub>1</sub></i>, <i>i<sub>2</sub></i>, <i>V<sub>1</sub></i>, and <i>V<sub>2</sub></i>
+are the real and imaginary parts of the current and voltage phasors.
+</p>
+<p>
+The nonlinearity of the model is due to the fact that the load consumes the power specified by the variables <i>P</i>
+and <i>Q</i> irrespectively of the voltage of the load.
+</p>
+<p>
+When multiple loads are connected in a grid through cables that cause voltage drops,
+the dimension of the system of nonlinear equations increases linearly with the number of loads.
+This nonlinear system of equations introduces challenges during the initialization,
+as Newton solvers may diverge if initialized far from a solution, as well during the simulation.
+In this situation, the model can be parameterized to use a linear approximation
+as discussed in the next section.
+</p>
+
+<h4>Linearized model</h4>
+<p>
+Given the constraints and the two-dimensional nature of the problem, it is difficult to
+find a linearized version of the AC load model. A solution could be to divide the voltage
+domain into sectors, and for each sector compute the best linear approximation.
+However the selection of the proper approximation depending on the value of the
+voltage can generate events that increase the simulation time. For these reasons, the
+linearized model assumes a voltage that is equal to the nominal value
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>1</sub> = (P V<sub>1</sub> + Q V<sub>2</sub>)/V<sub>RMS</sub><sup>2</sup>,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>2</sub> = (P V<sub>2</sub> - Q V<sub>1</sub>)/V<sub>RMS</sub><sup>2</sup>,
+</p>
+<p>
+where <i>V<sub>RMS</sub></i> is the Root Mean Square voltage os the AC system.
+Even though this linearized version of the load model introduces an approximation
+error in the current, it satisfies the constraints related to the ratio of the
+active and reactive powers.
+</p>
+
+<h4>Initialization</h4>
+<p>
+The initialization problem can be simplified using the homotopy operator. The homotopy operator
+uses two different types of equations to compute the value of a variable: the actual one
+and a simplified one. The actual equation is the one used during the normal operation.
+During initialization, the simplified equation is first solved and then slowly replaced
+with the actual equation to compute the initial values for the nonlinear systems of
+equations. The load model uses the homotopy operator, with the linearized model being used
+as the simplified equation. This numerical expedient has proven useful when simulating models
+with more than ten connected loads.
+</p>
+<p>
+The load model has a parameter <code>initMode</code> that can be used to select
+the assumption to use during the initialization phase by the homotopy operator.
+The choices are between a null current or the linearized model.
+</p>
+
+
+</html>",
+      revisions="<html>
+<ul>
+<li>
+January 29, 2019, by Michael Wetter:<br/>
+Added <code>replaceable</code> for terminal.
+</li>
+<li>
+May 26, 2016, by Michael Wetter:<br/>
+Moved function call to <code>PhaseSystem.thetaRef</code> out of
+derivative operator as this is not yet supported by JModelica.
+</li>
+<li>September 4, 2014, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Capacitive;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Examples/DynamicLoads.mo b/AixLib/Electrical/AC/OnePhase/Loads/Examples/DynamicLoads.mo
new file mode 100644
index 0000000000..bfc03bfb91
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Examples/DynamicLoads.mo
@@ -0,0 +1,69 @@
+within AixLib.Electrical.AC.OnePhase.Loads.Examples;
+model DynamicLoads "Example that illustrates the use of dynamic loads"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage source(
+    f=60,
+    V=120) "Voltage source" annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,10})));
+  AixLib.Electrical.AC.OnePhase.Loads.Capacitive dynRC(
+    pf=0.8,
+    mode=AixLib.Electrical.Types.Load.FixedZ_dynamic,
+    P_nominal=-1200,
+    V_nominal=120) "Dynamic RC load"
+    annotation (Placement(transformation(extent={{0,-20},{20,0}})));
+  AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance line(R=0.1)
+    "Line resistance"
+    annotation (Placement(transformation(extent={{-40,0},{-20,20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive dynRL(
+    pf=0.8,
+    mode=AixLib.Electrical.Types.Load.FixedZ_dynamic,
+    P_nominal=-1200,
+    V_nominal=120) "Dynamic RL load"
+    annotation (Placement(transformation(extent={{0,10},{20,30}})));
+equation
+  connect(source.terminal, line.terminal_n) annotation (Line(
+      points={{-60,10},{-40,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line.terminal_p, dynRC.terminal) annotation (Line(
+      points={{-20,10},{-10,10},{-10,-10},{-4.44089e-16,-10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(dynRL.terminal, line.terminal_p) annotation (Line(
+      points={{-4.44089e-16,20},{-10,20},{-10,10},{-20,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+    Documentation(info="<html>
+<p>
+This model compares two dynamic load models that use the dynamic
+phasors.
+</p>
+<p>
+The loads at nominal conditions should consume an active power equal
+to <i>1.2</i> kW. Because of the line resistance the voltage at the load is
+attenuated and they consume less power.
+</p>
+<p>
+As expected the real part of the current vector drawn by the loads are
+the same while the complex parts have opposite signs.
+</p>
+</html>",
+    revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 3, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/DynamicLoads.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end DynamicLoads;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Examples/ParallelLoads.mo b/AixLib/Electrical/AC/OnePhase/Loads/Examples/ParallelLoads.mo
new file mode 100644
index 0000000000..302f6ad2f6
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Examples/ParallelLoads.mo
@@ -0,0 +1,121 @@
+within AixLib.Electrical.AC.OnePhase.Loads.Examples;
+model ParallelLoads
+  "Example that illustrates the use of the load models at constant voltage"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive varRL(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    linearized=false,
+    V_nominal=120) "Variable inductor and resistor"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        origin={10,50})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage source(f=60, V=120)
+    "Voltage source"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,10})));
+  Modelica.Blocks.Sources.Ramp load_y(duration=0.5, startTime=0.2)
+    "Input signal for RC load"
+    annotation (Placement(transformation(extent={{60,0},{40,20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive RL(
+    P_nominal=-1e3,
+    linearized=false,
+    V_nominal=120) "Constant inductor and resistor"
+                                     annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={10,30})));
+  AixLib.Electrical.AC.OnePhase.Loads.Capacitive varRC(mode=AixLib.Electrical.Types.Load.VariableZ_y_input,
+      P_nominal=-1e3,
+    linearized=false,
+    V_nominal=120) "Variable conductor and resistor"        annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        origin={10,10})));
+  AixLib.Electrical.AC.OnePhase.Loads.Capacitive RC(mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+      P_nominal=-1e3,
+    linearized=false,
+    V_nominal=120) "Constant conductor and resistor"        annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        origin={10,-10})));
+  AixLib.Electrical.AC.OnePhase.Loads.Resistive R(
+    P_nominal=-1e3,
+    mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    linearized=false,
+    V_nominal=120) "Resistive load"
+                     annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={10,-30})));
+  Modelica.Blocks.Sources.Ramp load_P(
+    startTime=0.2,
+    duration=0.5,
+    height=-2000,
+    offset=1000) "Power signal for load varRL"
+    annotation (Placement(transformation(extent={{60,40},{40,60}})));
+equation
+  connect(source.terminal, varRL.terminal)  annotation (Line(
+      points={{-60,10},{-30,10},{-30,50},{0,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(source.terminal, RL.terminal)  annotation (Line(
+      points={{-60,10},{-30,10},{-30,30},{0,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(source.terminal, varRC.terminal)  annotation (Line(
+      points={{-60,10},{0,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(source.terminal, R.terminal)
+                                      annotation (Line(
+      points={{-60,10},{-30,10},{-30,-30},{0,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RC.terminal, R.terminal) annotation (Line(
+      points={{0,-10},{-30,-10},{-30,-30},{-5.55112e-16,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load_y.y, varRC.y)
+                           annotation (Line(
+      points={{39,10},{20,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load_P.y, varRL.Pow)
+                              annotation (Line(
+      points={{39,50},{20,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (
+    experiment(StopTime=1.0, Tolerance=1e-6),
+    Documentation(info="<html>
+<p>
+This model illustrates the use of the load models.
+The first two lines are inductive loads, followed by two capacitive loads and a resistive load.
+
+The inductive load <code>varRL</code> and the capacitive load <code>varRC</code>
+have a variable load specified by the inputs <code>Pow</code> and <code>y</code>
+respectively.
+
+All the loads have a nominal power of 1kW, and <code>varRL</code> is the only one
+that at <i>t=0</i> produces power 1kW and as the time increases it start to
+consume up to 1kW.
+
+</p>
+</html>",
+    revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 3, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ParallelLoads.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ParallelLoads;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Examples/ParallelResistors.mo b/AixLib/Electrical/AC/OnePhase/Loads/Examples/ParallelResistors.mo
new file mode 100644
index 0000000000..9bb80db0ea
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Examples/ParallelResistors.mo
@@ -0,0 +1,75 @@
+within AixLib.Electrical.AC.OnePhase.Loads.Examples;
+model ParallelResistors
+  "Example that illustrates the use of the load models at constant voltage"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage
+    source(f=60, V=120) "Voltage source"
+                            annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,10})));
+  Modelica.Blocks.Sources.Ramp load(duration=0.5, startTime=0.2,
+    height=2400,
+    offset=-1200) "Power signal for load R"
+    annotation (Placement(transformation(extent={{40,0},{20,20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Resistive R(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=120) "Variable resistive load"
+                                     annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-22,10})));
+  AixLib.Electrical.AC.OnePhase.Loads.Resistive R1(
+    mode=AixLib.Electrical.Types.Load.FixedZ_steady_state, P_nominal=-1.2e3,
+    V_nominal=120) "Fixed resistive load"
+                                     annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-22,-10})));
+equation
+  connect(source.terminal, R.terminal) annotation (Line(
+      points={{-60,10},{-32,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load.y, R.Pow) annotation (Line(
+      points={{19,10},{-12,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(source.terminal, R1.terminal) annotation (Line(
+      points={{-60,10},{-46,10},{-46,-10},{-32,-10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+    experiment(StopTime=1.0, Tolerance=1e-6),
+    Documentation(info="<html>
+<p>
+This model compares two resistive loads. Model <code>R</code> consumes or produces
+a variable amount of power, while model <code>R1</code> consumes a fixed power.
+</p>
+<p>
+At time <i>t=0</i> <code>R</code> and <code>R1</code> consumes the same amount of power
+while at <i>t=1</i> <code>R</code> produces the same power consumed by <code>R1</code>.
+</p>
+</html>",
+    revisions="<html>
+<ul>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Removed binding of <code>P_nominal</code> as
+this parameter is disabled and assigned a value
+in the <code>initial equation</code> section.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 3, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ParallelResistors.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ParallelResistors;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Examples/TestImpedance.mo b/AixLib/Electrical/AC/OnePhase/Loads/Examples/TestImpedance.mo
new file mode 100644
index 0000000000..01ea3724f1
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Examples/TestImpedance.mo
@@ -0,0 +1,70 @@
+within AixLib.Electrical.AC.OnePhase.Loads.Examples;
+model TestImpedance "Example that illustrates the use of the impedances"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage V(f=60, V=120)
+           annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Z1(R=0,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60)) "Inductive impedance"
+    annotation (Placement(transformation(extent={{-20,20},{0,40}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Z2(R=0,
+    inductive=false,
+    C=1/(2*Modelica.Constants.pi*60)) "Capacitive impedance"
+    annotation (Placement(transformation(extent={{-20,0},{0,20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Z3(R=1)
+    "Resistive impedance"
+    annotation (Placement(transformation(extent={{-20,-20},{0,0}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Z4(
+    R=1,
+    L=1/(2*Modelica.Constants.pi*60)) "Inductive-resistive impedance"
+    annotation (Placement(transformation(extent={{-20,-40},{0,-20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Z5(
+    R=1,
+    inductive=false,
+    C=1/(2*Modelica.Constants.pi*60)) "Capacitive-resistive impedance"
+    annotation (Placement(transformation(extent={{-20,-60},{0,-40}})));
+equation
+  connect(V.terminal, Z1.terminal)  annotation (Line(
+      points={{-60,30},{-20,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(V.terminal, Z2.terminal) annotation (Line(
+      points={{-60,30},{-40,30},{-40,10},{-20,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(V.terminal, Z3.terminal) annotation (Line(
+      points={{-60,30},{-40,30},{-40,-10},{-20,-10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(V.terminal, Z4.terminal) annotation (Line(
+      points={{-60,30},{-40,30},{-40,-30},{-20,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(V.terminal, Z5.terminal) annotation (Line(
+      points={{-60,30},{-40,30},{-40,-50},{-20,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-06),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/TestImpedance.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This model shows how to use the impedance model in different configurations:
+</p>
+<ul>
+<li>Resistive (model <code>Z3</code>)</li>
+<li>Inductive (model <code>Z1</code>)</li>
+<li>Capacitive (model <code>Z2</code>)</li>
+<li>Resistive-Inductive (model <code>Z4</code>)</li>
+<li>Resistive-Capacitive (model <code>Z5</code>)</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TestImpedance;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Examples/ThreePhases.mo b/AixLib/Electrical/AC/OnePhase/Loads/Examples/ThreePhases.mo
new file mode 100644
index 0000000000..9038bfdfb4
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Examples/ThreePhases.mo
@@ -0,0 +1,67 @@
+within AixLib.Electrical.AC.OnePhase.Loads.Examples;
+model ThreePhases
+  "Examples that illustrates how to replicate a three-phase balanced system"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage Va(
+    definiteReference=true,
+    f=60,
+    V=120) "Source phase A"
+           annotation (Placement(transformation(extent={{-40,40},{-20,60}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Za(
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60),
+    R=12) "Impedance phase A"
+    annotation (Placement(transformation(extent={{20,40},{40,60}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage Vb(
+    definiteReference=true, phiSou=-2.0943951023932,
+    f=60,
+    V=120) "Source phase B"
+           annotation (Placement(transformation(extent={{-40,0},{-20,20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Zb(
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60),
+    R=12) "Impedance phase B"
+    annotation (Placement(transformation(extent={{20,0},{40,20}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage Vc(
+    definiteReference=true, phiSou=2.0943951023932,
+    f=60,
+    V=120) "Source phase C"
+           annotation (Placement(transformation(extent={{-40,-40},{-20,
+            -20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Zc(
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60),
+    R=12) "Impedance phase C"
+    annotation (Placement(transformation(extent={{20,-40},{40,-20}})));
+equation
+  connect(Va.terminal, Za.terminal) annotation (Line(
+      points={{-20,50},{20,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Vb.terminal, Zb.terminal) annotation (Line(
+      points={{-20,10},{20,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Vc.terminal, Zc.terminal) annotation (Line(
+      points={{-20,-30},{20,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-06),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ThreePhases.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This model shows how a balanced three phase system can be represented with three
+independent single phase circuits.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ThreePhases;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Examples/VariableImpedance.mo b/AixLib/Electrical/AC/OnePhase/Loads/Examples/VariableImpedance.mo
new file mode 100644
index 0000000000..64393e0bbe
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Examples/VariableImpedance.mo
@@ -0,0 +1,81 @@
+within AixLib.Electrical.AC.OnePhase.Loads.Examples;
+model VariableImpedance
+  "Example that illustrates how using variable impedances"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage V(f=60, V=120)
+    "Voltage source"
+           annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Z_L(
+    R=0,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60),
+    use_L_in=true,
+    LMin=1/(2*Modelica.Constants.pi*60),
+    LMax=2/(2*Modelica.Constants.pi*60)) "Impedance with variable L"
+    annotation (Placement(transformation(extent={{-20,-60},{0,-40}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Z_C(
+    R=0,
+    inductive=false,
+    C=1/(2*Modelica.Constants.pi*60),
+    use_C_in=true,
+    CMin=1/(2*Modelica.Constants.pi*60),
+    CMax=2/(2*Modelica.Constants.pi*60)) "Impedance with variable C"
+    annotation (Placement(transformation(extent={{-20,-10},{0,10}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Impedance Z_R(
+    R=1,
+    RMin=1,
+    RMax=2,
+    use_R_in=true,
+    L=0) "Impedance with variable R"
+    annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+  Modelica.Blocks.Sources.Ramp load(duration=0.5, startTime=0.2,
+    height=1,
+    offset=0) "Input signal for the loads"
+    annotation (Placement(transformation(extent={{60,-10},{40,10}})));
+equation
+  connect(V.terminal, Z_L.terminal) annotation (Line(
+      points={{-60,6.66134e-16},{-40,6.66134e-16},{-40,-50},{-20,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(V.terminal, Z_C.terminal)
+                                   annotation (Line(
+      points={{-60,6.66134e-16},{-20,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(V.terminal, Z_R.terminal)
+                                   annotation (Line(
+      points={{-60,6.66134e-16},{-40,6.66134e-16},{-40,50},{-20,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load.y, Z_R.y_R) annotation (Line(
+      points={{39,0},{30,0},{30,80},{-14,80},{-14,60}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, Z_C.y_C) annotation (Line(
+      points={{39,4.44089e-16},{30,4.44089e-16},{30,20},{-10,20},{-10,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, Z_L.y_L) annotation (Line(
+      points={{39,6.66134e-16},{34,6.66134e-16},{34,0},{30,0},{30,-20},{-6,-20},
+          {-6,-40}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-06),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/VariableImpedance.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This model shows how to vary the resistance,
+capacitance or inductance of an impedance model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end VariableImpedance;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Examples/package.mo b/AixLib/Electrical/AC/OnePhase/Loads/Examples/package.mo
new file mode 100644
index 0000000000..bc91a42a7d
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Electrical.AC.OnePhase.Loads;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads\">
+AixLib.Electrical.AC.OnePhase.Loads</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Examples/package.order b/AixLib/Electrical/AC/OnePhase/Loads/Examples/package.order
new file mode 100644
index 0000000000..9b5e430313
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Examples/package.order
@@ -0,0 +1,6 @@
+DynamicLoads
+ParallelLoads
+ParallelResistors
+TestImpedance
+ThreePhases
+VariableImpedance
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Impedance.mo b/AixLib/Electrical/AC/OnePhase/Loads/Impedance.mo
new file mode 100644
index 0000000000..c8b4873745
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Impedance.mo
@@ -0,0 +1,92 @@
+within AixLib.Electrical.AC.OnePhase.Loads;
+model Impedance "Model of a generic impedance"
+  extends AixLib.Electrical.Interfaces.Impedance(
+    redeclare replaceable package PhaseSystem = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal);
+
+protected
+  Modelica.Units.SI.Angle theRef "Absolute angle of rotating reference system";
+  Modelica.Units.SI.AngularVelocity omega
+    "Frequency of the quasi-stationary sine waves";
+  Modelica.Units.SI.Reactance X(start=1) "Complex component of the impedance";
+equation
+  theRef = PhaseSystem.thetaRef(terminal.theta);
+  omega = der(theRef);
+
+  if inductive then
+    X = omega*L_internal;
+  else
+    X = -1/(omega*C_internal);
+  end if;
+
+  terminal.v = {{R_internal,-X}*terminal.i, {X,R_internal}*terminal.i};
+  annotation (
+    defaultComponentName="imp",
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+          Rectangle(
+            extent={{-80,40},{80,-40}},
+            lineColor={0,0,0},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+          origin={0,3.55271e-15},
+          rotation=180),
+          Line(points={{0,0},{12,0}},  color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+        Text(
+          extent={{-120,-40},{120,-80}},
+          textColor={0,0,0},
+          textString="%name")}),
+          Documentation(info="<html>
+<p>
+Model of an impedance. This model can be used to represent any type
+of resistive, inductive or capacitive load.
+</p>
+<p>
+Note that the power consumed by the impedance model will drecrease if its voltage
+decreases.
+</p>
+<p>
+The model of the impedance is
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+V = Z i,
+</p>
+
+<p>
+where <i>Z = R + j X</i> is the impedance. The value of the resistance <i>R</i> and the
+reactance <i>X</i> depend on the type of impedance. Different types of impedances
+can be selected using the boolean parameters <code>inductive</code>, <code>use_R_in</code>,
+<code>use_L_in</code>, and <code>use_C_in</code>. See
+<a href=\"modelica://AixLib.Electrical.Interfaces.Impedance\">
+AixLib.Electrical.Interfaces.Impedance</a> for more details.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 26, 2016, by Michael Wetter:<br/>
+Moved function call to <code>PhaseSystem.thetaRef</code> out of
+derivative operator as this is not yet supported by JModelica.
+</li>
+<li>
+March 30, 2015, by Michael Wetter:<br/>
+Made <code>PhaseSystem</code> and <code>terminal</code> replaceable. This was detected
+by the OpenModelica regression tests.
+</li>
+<li>September 4, 2014, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedance;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Inductive.mo b/AixLib/Electrical/AC/OnePhase/Loads/Inductive.mo
new file mode 100644
index 0000000000..31f9f09a9a
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Inductive.mo
@@ -0,0 +1,235 @@
+within AixLib.Electrical.AC.OnePhase.Loads;
+model Inductive "Model of an inductive and resistive load"
+  extends AixLib.Electrical.Interfaces.InductiveLoad(
+    redeclare package PhaseSystem = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal,
+    V_nominal(start = 110));
+
+protected
+  Modelica.Units.SI.Angle theRef "Absolute angle of rotating reference system";
+
+initial equation
+  if mode == AixLib.Electrical.Types.Load.FixedZ_dynamic then
+    // psi = Z[2]*{P_nominal/V_nominal, 0}/omega;
+    // Steady state initialization
+    der(psi) = zeros(PhaseSystem.n);
+  end if;
+equation
+  theRef = PhaseSystem.thetaRef(terminal.theta);
+  omega = der(theRef);
+
+  if mode == AixLib.Electrical.Types.Load.FixedZ_dynamic then
+
+    // Use the dynamic phasorial representation
+    Z[1] = -pf*(V_nominal^2)/(P_nominal/pf);
+    Z[2] = -Modelica.Fluid.Utilities.regRoot(1-pf^2, delta=0.001)*(V_nominal^2)/(P_nominal/pf);
+
+    // Dynamics of the system
+    der(psi) + omega*j(psi) + Z[1]*i = v;
+
+    // Magnetic flux
+    psi = Z[2]*{i[1], i[2]}/omega;
+
+  else
+
+    // Use the power specified by the parameter or inputs
+    if linearized then
+      i[1] = -homotopy(actual= (v[2]*Q + v[1]*P)/(V_nominal^2), simplified= v[1]*Modelica.Constants.eps*1e3);
+      i[2] = -homotopy(actual= (v[2]*P - v[1]*Q)/(V_nominal^2), simplified= v[2]*Modelica.Constants.eps*1e3);
+    else
+      //PhaseSystem.phasePowers_vi(terminal.v, terminal.i) = PhaseSystem.phasePowers(P, Q);
+      if initMode == AixLib.Electrical.Types.InitMode.zero_current then
+        i[1] = -homotopy(actual = (v[2]*Q + v[1]*P)/(v[1]^2 + v[2]^2), simplified= 0.0);
+        i[2] = -homotopy(actual = (v[2]*P - v[1]*Q)/(v[1]^2 + v[2]^2), simplified= 0.0);
+      else
+        i[1] = -homotopy(actual = (v[2]*Q + v[1]*P)/(v[1]^2 + v[2]^2), simplified= (v[2]*Q + v[1]*P)/(V_nominal^2));
+        i[2] = -homotopy(actual = (v[2]*P - v[1]*Q)/(v[1]^2 + v[2]^2), simplified= (v[2]*P - v[1]*Q)/(V_nominal^2));
+      end if;
+    end if;
+
+    Z = {0,0};
+    psi = {0,0};
+
+  end if;
+  annotation (
+    defaultComponentName="loa",
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Rectangle(
+          extent={{-80,40},{80,-40}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+                                   Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+        Ellipse(extent={{-10,-10},{10,10}},
+          origin={10,0},
+          rotation=360),
+        Ellipse(extent={{40,-10},{60,10}}),
+        Ellipse(extent={{20,-10},{40,10}}),
+        Rectangle(
+          extent={{0,0},{60,-12}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,0}},    color={0,0,0},
+          rotation=180),
+          Line(points={{0,0},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={70,0},
+          rotation=180),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-42,1},
+          rotation=90),
+          Line(points={{-10,-1.22461e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Text(
+          extent={{-120,80},{120,40}},
+          textColor={0,0,0},
+          textString="%name")}),    Documentation(info="<html>
+
+<p>
+Model of an inductive load. It may be used to model an inductive motor.
+</p>
+<p>
+The model computes the complex power vector as
+<p align=\"center\" style=\"font-style:italic;\">
+S = P + jQ = V &sdot; i<sup>*</sup>,
+</p>
+<p>
+where <i>V</i> is the voltage phasor and <i>i<sup>*</sup></i> is the complex
+conjugate of the current phasor. The voltage and current phasors are shifted
+by an angle <i>&phi;</i>.
+</p>
+
+<p>
+The load model takes as input the power consumed by the inductive load and
+the power factor <i>pf=cos(&phi;)</i>. The power
+can be either fixed using the parameter <code>P_nominal</code>, or
+it is possible to specify a variable power using the inputs <code>y</code> or
+<code>Pow</code>.
+
+The power factor can be either specified by the parameter <code>pf</code>
+or using the input connector <code>pf_in</code>.
+
+The different modes can be selected with the parameter
+<code>mode</code> and <code>use_pf_in</code>, see <a href=\"modelica://AixLib.Electrical.Interfaces.Load\">
+AixLib.Electrical.Interfaces.Load</a> and
+<a href=\"modelica://AixLib.Electrical.Interfaces.InductiveLoad\">
+AixLib.Electrical.Interfaces.InductiveLoad</a> for more information.
+</p>
+
+<p>
+Given the active power <i>P</i> and the power factor <i>pf</i>, the complex
+power <i>Q</i> is computed as
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+Q = P  tan(arccos(pf)).
+</p>
+
+<p>
+The equations of the model can be rewritten as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>1</sub> = (P V<sub>1</sub> + Q V<sub>2</sub>)/(V<sub>1</sub><sup>2</sup> + V<sub>2</sub><sup>2</sup>),
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>2</sub> = (P V<sub>2</sub> - Q V<sub>1</sub>)/(V<sub>1</sub><sup>2</sup> + V<sub>2</sub><sup>2</sup>),
+</p>
+
+<p>
+where <i>i<sub>1</sub></i>, <i>i<sub>2</sub></i>, <i>V<sub>1</sub></i>, and <i>V<sub>2</sub></i>
+are the real and imaginary parts of the current and voltage phasors.
+</p>
+<p>
+The nonlinearity of the model is due to the fact that the load consumes the power specified by the variables <i>P</i>
+and <i>Q</i>, irrespectively of the voltage of the load.
+</p>
+<p>
+When multiple loads are connected in a grid through cables that cause voltage drops,
+the dimension of the system of nonlinear equations increases linearly with the number of loads.
+This nonlinear system of equations introduces challenges during the initialization,
+as Newton solvers may diverge if initialized far from a solution, as well during the simulation.
+In this situation, the model can be parameterized to use a linear approximation
+as discussed in the next section.
+</p>
+
+<h4>Linearized model</h4>
+<p>
+Given the constraints and the two-dimensional nature of the problem, it is difficult to
+find a linearized version of the AC load model. A solution could be to divide the voltage
+domain into sectors, and for each sector compute the best linear approximation.
+However the selection of the proper approximation depending on the value of the
+voltage can generate events that increase the simulation time. For these reasons, the
+linearized model assumes a voltage that is equal to the nominal value
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>1</sub> = (P V<sub>1</sub> + Q V<sub>2</sub>)/V<sub>RMS</sub><sup>2</sup>,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>2</sub> = (P V<sub>2</sub> - Q V<sub>1</sub>)/V<sub>RMS</sub><sup>2</sup>,
+</p>
+<p>
+where <i>V<sub>RMS</sub></i> is the Root Mean Square voltage of the AC system.
+Even though this linearized version of the load model introduces an approximation
+error in the current, it satisfies the constraints related to the ratio of the
+active and reactive powers.
+</p>
+
+<h4>Initialization</h4>
+<p>
+The initialization problem can be simplified using the homotopy operator. The homotopy operator
+uses two different types of equations to compute the value of a variable: the actual one
+and a simplified one. The actual equation is the one used during the normal operation.
+During initialization, the simplified equation is first solved and then slowly replaced
+with the actual equation to compute the initial values for the nonlinear systems of
+equations. The load model uses the homotopy operator, with the linearized model being used
+as the simplified equation. This numerical expedient has proven useful when simulating models
+with more than ten connected loads.
+</p>
+<p>
+The load model has a parameter <code>initMode</code> that can be used to select
+the assumption to use during the initialization phase by the homotopy operator.
+The choices are between a null current or the linearized model.
+</p>
+
+
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Added <code>replaceable</code> to terminal redeclaration as they are redeclared by
+<a href=\"modelica://Buildings.Electrical.AC.ThreePhasesBalanced.Loads.Inductive\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Inductive</a>.
+</li>
+<li>
+May 26, 2016, by Michael Wetter:<br/>
+Moved function call to <code>PhaseSystem.thetaRef</code> out of
+derivative operator as this is not yet supported by JModelica.
+</li>
+<li>September 4, 2014, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>June 17, 2014, by Marco Bonvini:<br/>
+Adde parameter <code>initMode</code> that can be used to
+select the assumption to be used during initialization phase
+by the homotopy operator.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Inductive;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/Resistive.mo b/AixLib/Electrical/AC/OnePhase/Loads/Resistive.mo
new file mode 100644
index 0000000000..90ffbe1aea
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/Resistive.mo
@@ -0,0 +1,189 @@
+within AixLib.Electrical.AC.OnePhase.Loads;
+model Resistive "Model of a resistive load"
+  extends AixLib.Electrical.Interfaces.ResistiveLoad(
+    redeclare package PhaseSystem = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_n terminal,
+    V_nominal(start = 110));
+equation
+
+  if linearized then
+    i[1] = -homotopy(actual = v[1]*P/V_nominal^2, simplified = v[1]*Modelica.Constants.eps*1e3);
+    i[2] = -homotopy(actual = v[2]*P/V_nominal^2, simplified = v[2]*Modelica.Constants.eps*1e3);
+  else
+    if initMode == AixLib.Electrical.Types.InitMode.zero_current then
+      i[1] = -homotopy(actual= v[1]*P/(v[1]^2 + v[2]^2),  simplified= 0.0);
+      i[2] = -homotopy(actual= v[2]*P/(v[1]^2 + v[2]^2),  simplified= 0.0);
+    else
+      i[1] = -homotopy(actual= v[1]*P/(v[1]^2 + v[2]^2),
+                       simplified= v[1]*P/V_nominal^2);
+      i[2] = -homotopy(actual= v[2]*P/(v[1]^2 + v[2]^2),
+                       simplified= v[2]*P/V_nominal^2);
+    end if;
+  end if;
+  annotation (
+    defaultComponentName="loa",
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+          Rectangle(
+            extent={{-80,40},{80,-40}},
+            lineColor={0,0,0},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+          origin={0,3.55271e-15},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{12,1.46953e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+        Text(
+          extent={{-120,80},{120,40}},
+          textColor={0,0,0},
+          textString="%name")}),
+          Documentation(info="<html>
+<p>
+Model of a resistive load. It may be used to model a load that has
+a power factor of one.
+</p>
+<p>
+The model computes the complex power vector as
+<p align=\"center\" style=\"font-style:italic;\">
+S = P + jQ = V &sdot; i<sup>*</sup>
+</p>
+<p>
+where <i>V</i> is the voltage phasor and <i>i<sup>*</sup></i> is the complex
+conjugate of the current phasor.
+</p>
+
+<p>
+The load model takes as input the power consumed by the inductive load and
+the power factor <i>pf=cos(&phi;)</i>. The power
+can be either fixed using the parameter <code>P_nominal</code>, or
+it is possible to specify a variable power using the inputs <code>y</code> or
+<code>Pow</code>. The different modes can be selected with the parameter
+<code>mode</code>, see <a href=\"modelica://AixLib.Electrical.Interfaces.Load\">
+AixLib.Electrical.Interfaces.Load</a> for more information.
+</p>
+
+<p>
+The equations of the model can be rewritten as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>1</sub> = (P V<sub>1</sub> + Q V<sub>2</sub>)/(V<sub>1</sub><sup>2</sup> + V<sub>2</sub><sup>2</sup>),
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>2</sub> = (P V<sub>2</sub> - Q V<sub>1</sub>)/(V<sub>1</sub><sup>2</sup> + V<sub>2</sub><sup>2</sup>),
+</p>
+
+<p>
+where <i>i<sub>1</sub></i>, <i>i<sub>2</sub></i>, <i>V<sub>1</sub></i>, and <i>V<sub>2</sub></i>
+are the real and imaginary parts of the current and voltage phasors.
+</p>
+
+<p>
+Since the model represents a load with a power factor of one, the complex
+power is <i>Q = 0</i>. This leads to the following equations where
+there are nonlinear equations that relate the current to the voltage
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>1</sub> = P V<sub>1</sub>/(V<sub>1</sub><sup>2</sup> + V<sub>2</sub><sup>2</sup>)
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>2</sub> = P V<sub>2</sub>/(V<sub>1</sub><sup>2</sup> + V<sub>2</sub><sup>2</sup>)
+</p>
+
+<p>
+The non-linearity is due to the fact that the load consumes the power specified by the variable <i>P</i>,
+irrespectively of the voltage of the load. The figure below shows the relationship
+between the real part of the current phasor and the real and imaginary voltages of the load.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/OnePhase/Loads/NonlinearLoad_labels.png\"/>
+</p>
+
+<p>
+When multiple loads are connected in a grid through cables that cause voltage drops,
+the dimension of the system of nonlinear equations increases linearly with the number of loads.
+This nonlinear system of equations introduces challenges during the initialization,
+as Newton solvers may diverge if initialized far from a solution, as well during the simulation.
+In this situation, the model can be parameterized to use a linear approximation
+as discussed in the next section.
+</p>
+
+<h4>Linearized model</h4>
+<p>
+Given the constraints and the two-dimensional nature of the problem, it is difficult to
+find a linearized version of the AC load model. A solution could be to divide the voltage
+domain into sectors, and for each sector compute the best linear approximation.
+However, the selection of the proper approximation depending on the value of the
+voltage can generate events that increase the simulation time. For these reasons, the
+linearized model assumes a voltage that is equal to the nominal value
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>1</sub> = P V<sub>1</sub>/V<sub>RMS</sub><sup>2</sup>
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+i<sub>2</sub> = P V<sub>2</sub>/V<sub>RMS</sub><sup>2</sup>
+</p>
+<p>
+where <i>V<sub>RMS</sub></i> is the Root Mean Square voltage of the AC system.
+Even though this linearized version of the load model introduces an approximation
+error in the current, it satisfies the constraints related to the ratio of the
+active and reactive powers.
+</p>
+<p>
+The image below show the linearized function
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/OnePhase/Loads/LinearLoad_labels.png\"/>
+</p>
+
+<h4>Initialization</h4>
+<p>
+The initialization problem can be simplified using the homotopy operator. The homotopy operator
+uses two different types of equations to compute the value of a variable: the actual one
+ and a simplified one. The actual equation is the one used during the normal operation.
+During initialization, the simplified equation is first solved and then slowly replaced
+with the actual equation to compute the initial values for the nonlinear system of
+equations. The load model uses the homotopy operator, with the linearized model being used
+as the simplified equation. This numerical expedient has proven useful when simulating models
+with more than ten connected loads.
+</p>
+<p>
+The load model has a parameter <code>initMode</code> that can be used to select
+the assumption to use during the initialization phase by the homotopy operator.
+The choices are between a null current or the linearized model.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2019, by Michael Wetter:<br/>
+Added <code>replaceable</code> for terminal.
+</li>
+<li>May 14, 2015, by Marco Bonvini:<br/>
+Changed parent class to <a href=\"modelica://Buildings.Electrical.Interfaces.ResistiveLoad\">
+AixLib.Electrical.Interfaces.ResistiveLoad</a> in order
+to help openmodelica parsing the model. This fixes issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/415\">#415</a>.
+</li>
+<li>September 4, 2014, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>June 17, 2014, by Marco Bonvini:<br/>
+Added parameter <code>initMode</code> that can be used to
+select the assumption to be used during initialization phase
+by the homotopy operator.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Resistive;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/package.mo b/AixLib/Electrical/AC/OnePhase/Loads/package.mo
new file mode 100644
index 0000000000..588c872015
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/package.mo
@@ -0,0 +1,22 @@
+within AixLib.Electrical.AC.OnePhase;
+package Loads "Package with load models for one phase AC systems"
+  extends Modelica.Icons.VariantsPackage;
+
+
+
+
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models that represent different types of AC single phase loads.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 4, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end Loads;
diff --git a/AixLib/Electrical/AC/OnePhase/Loads/package.order b/AixLib/Electrical/AC/OnePhase/Loads/package.order
new file mode 100644
index 0000000000..865b97b429
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Loads/package.order
@@ -0,0 +1,5 @@
+Capacitive
+Impedance
+Inductive
+Resistive
+Examples
diff --git a/AixLib/Electrical/AC/OnePhase/Sensors/Examples/GeneralizedSensor.mo b/AixLib/Electrical/AC/OnePhase/Sensors/Examples/GeneralizedSensor.mo
new file mode 100644
index 0000000000..2bcf01c9fa
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sensors/Examples/GeneralizedSensor.mo
@@ -0,0 +1,53 @@
+within AixLib.Electrical.AC.OnePhase.Sensors.Examples;
+model GeneralizedSensor
+  "This example illustrates how to use the generalized sensor model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sensors.GeneralizedSensor sen
+    "Sensor that measures V, I, and S"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Capacitive loa(
+    mode=AixLib.Electrical.Types.Load.FixedZ_dynamic,
+    P_nominal=-100,
+    V_nominal=120) "Constant load"
+    annotation (Placement(transformation(extent={{40,0},{60,20}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage sou(f=60, V=120)
+    "Voltage source"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance res(R=0.05)
+    "Line resistance"
+    annotation (Placement(transformation(extent={{-32,0},{-12,20}})));
+equation
+  connect(sen.terminal_p, loa.terminal)
+    annotation (Line(points={{20,10},{40,10}},          smooth=Smooth.None));
+  connect(sou.terminal, res.terminal_n) annotation (Line(
+      points={{-40,10},{-32,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(res.terminal_p, sen.terminal_n) annotation (Line(
+      points={{-12,10},{-4.44089e-16,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  Documentation(
+  info="<html>
+<p>
+This example illustrates the use of the generalized sensor.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+July 24, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sensors/Examples/GeneralizedSensor.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor;
diff --git a/AixLib/Electrical/AC/OnePhase/Sensors/Examples/Probe.mo b/AixLib/Electrical/AC/OnePhase/Sensors/Examples/Probe.mo
new file mode 100644
index 0000000000..49373a2e39
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sensors/Examples/Probe.mo
@@ -0,0 +1,83 @@
+within AixLib.Electrical.AC.OnePhase.Sensors.Examples;
+model Probe "This example illustrates how to use the probe model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Loads.Capacitive loaRC(
+    mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    P_nominal=-10000,
+    V_nominal=120) "Constant load"
+    annotation (Placement(transformation(extent={{10,0},{30,20}})));
+  AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage sou(f=60, V=120)
+    "Voltage source"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance res1(R=0.1)
+    "First line resistance"
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+  AixLib.Electrical.AC.OnePhase.Sensors.Probe probe_source(V_nominal=120)
+    "Probe that measures at the voltage source"
+    annotation (Placement(transformation(extent={{-50,30},{-30,50}})));
+  AixLib.Electrical.AC.OnePhase.Sensors.Probe probe_loadRC(V_nominal=120)
+    "Probe that measures at the RC load"
+    annotation (Placement(transformation(extent={{-10,30},{10,50}})));
+  AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance res2(R=0.1)
+    "Second line resistance"
+    annotation (Placement(transformation(extent={{-26,-70},{-6,-50}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive loaRL(
+    mode=AixLib.Electrical.Types.Load.FixedZ_steady_state, P_nominal=-10000,
+    V_nominal=120) "Constant load"
+    annotation (Placement(transformation(extent={{10,-70},{30,-50}})));
+  AixLib.Electrical.AC.OnePhase.Sensors.Probe probe_loadRL(V_nominal=120)
+    "Probe that measures at the RL load"
+    annotation (Placement(transformation(extent={{-10,-28},{10,-8}})));
+equation
+  connect(sou.terminal, res1.terminal_n) annotation (Line(
+      points={{-40,-20},{-40,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(res1.terminal_p, loaRC.terminal) annotation (Line(
+      points={{-6,10},{10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, probe_source.term) annotation (Line(
+      points={{-40,-20},{-40,31}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(loaRC.terminal, probe_loadRC.term) annotation (Line(
+      points={{10,10},{6.66134e-16,10},{6.66134e-16,31}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, res2.terminal_n) annotation (Line(
+      points={{-40,-20},{-40,-60},{-26,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(res2.terminal_p, loaRL.terminal) annotation (Line(
+      points={{-6,-60},{10,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(loaRL.terminal, probe_loadRL.term) annotation (Line(
+      points={{10,-60},{6.66134e-16,-60},{6.66134e-16,-27}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  Documentation(
+  info="<html>
+<p>
+This example illustrates the use of the probe model.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sensors/Examples/Probe.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Probe;
diff --git a/AixLib/Electrical/AC/OnePhase/Sensors/Examples/package.mo b/AixLib/Electrical/AC/OnePhase/Sensors/Examples/package.mo
new file mode 100644
index 0000000000..1ed5d3b4fd
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sensors/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.OnePhase.Sensors;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Sensors\">
+AixLib.Electrical.AC.OnePhase.Sensors</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/OnePhase/Sensors/Examples/package.order b/AixLib/Electrical/AC/OnePhase/Sensors/Examples/package.order
new file mode 100644
index 0000000000..e4597e24c3
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sensors/Examples/package.order
@@ -0,0 +1,2 @@
+GeneralizedSensor
+Probe
diff --git a/AixLib/Electrical/AC/OnePhase/Sensors/GeneralizedSensor.mo b/AixLib/Electrical/AC/OnePhase/Sensors/GeneralizedSensor.mo
new file mode 100644
index 0000000000..6504653a2d
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sensors/GeneralizedSensor.mo
@@ -0,0 +1,86 @@
+within AixLib.Electrical.AC.OnePhase.Sensors;
+model GeneralizedSensor "Sensor for power, voltage and current"
+  extends AixLib.Electrical.Icons.GeneralizedSensor;
+  extends AixLib.Electrical.Interfaces.PartialTwoPort(
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  Modelica.Blocks.Interfaces.RealOutput V(final quantity="ElectricPotential",
+                                          final unit="V")=
+      AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal_n.v)
+    "Voltage"
+      annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-50}),   iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-90})));
+  Modelica.Blocks.Interfaces.RealOutput I(final quantity="ElectricCurrent",
+                                          final unit="A")=
+    AixLib.Electrical.PhaseSystems.OnePhase.systemCurrent(terminal_n.i)
+    "Current"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-50}), iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-90})));
+  Modelica.Blocks.Interfaces.RealOutput S[PhaseSystems.OnePhase.n](
+                                          each final quantity="Power",
+                                          each final unit="W")=
+     AixLib.Electrical.PhaseSystems.OnePhase.phasePowers_vi(v=terminal_n.v, i=terminal_n.i)
+    "Phase powers"
+     annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-60,-50}),iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-60,-90})));
+equation
+  connect(terminal_n, terminal_p) annotation (Line(
+      points={{-100,0},{2,0},{2,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (defaultComponentName="sen",
+  Documentation(info="<html>
+<p>
+Ideal sensor that measures power, voltage and current.
+The two components of the power <i>S</i> are the active and reactive power.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Fixed bug. The model was referencing the wrong PhaseSystem.
+</li>
+<li>September 4, 2014, by Michael Wetter:<br/>
+Revised model, changed <code>equation</code> section to
+avoid mixing graphical and textual modeling.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+July 24, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Icon(graphics={
+        Text(
+          extent={{-120,-42},{0,-82}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="S")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor;
diff --git a/AixLib/Electrical/AC/OnePhase/Sensors/Probe.mo b/AixLib/Electrical/AC/OnePhase/Sensors/Probe.mo
new file mode 100644
index 0000000000..84c919aea2
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sensors/Probe.mo
@@ -0,0 +1,73 @@
+within AixLib.Electrical.AC.OnePhase.Sensors;
+model Probe "Model of a probe that measures RMS voltage and angle"
+  extends Icons.GeneralizedProbe;
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=110)
+    "Nominal voltage (V_nominal >= 0)";
+  parameter Boolean perUnit = true "If true, display voltage in p.u.";
+  replaceable Interfaces.Terminal_n term "Electrical connector" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,-90})));
+  Modelica.Blocks.Interfaces.RealOutput V(unit=if perUnit then "1" else "V")
+    "Voltage phasor magnitude"                                                                          annotation (Placement(
+        transformation(extent={{60,20},{80,40}}), iconTransformation(extent={{60,
+            20},{80,40}})));
+  Modelica.Blocks.Interfaces.RealOutput theta(unit="rad", displayUnit="deg")
+    "Voltage phasor angle"
+                         annotation (Placement(
+        transformation(extent={{60,-40},{80,-20}}), iconTransformation(extent={{60,
+            -40},{80,-20}})));
+equation
+  theta = AixLib.Electrical.PhaseSystems.OnePhase.phase(term.v);
+  if perUnit then
+    V = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(term.v)/V_nominal;
+  else
+    V = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(term.v);
+  end if;
+  term.i = zeros(AixLib.Electrical.PhaseSystems.OnePhase.n);
+  annotation (
+  defaultComponentName="sen",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={Text(
+          extent={{40,60},{100,40}},
+          textColor={0,0,0},
+          pattern=LinePattern.Dash,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid,
+          textString="V"), Text(
+          extent={{18,-40},{140,-60}},
+          textColor={0,0,0},
+          pattern=LinePattern.Dash,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid,
+          textString="theta")}),    Documentation(info="<html>
+<p>
+This model represents a probe that measures the RMS voltage and the angle
+of the voltage phasor at a given point.
+</p>
+<p>
+Optionally, given a reference voltage, the model can compute the voltage in per unit.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 30, 2015, by Michael Wetter:<br/>
+Made <code>term</code> replaceable. This was detected
+by the OpenModelica regression tests.
+</li>
+<li>September 4, 2014, by Michael Wetter:<br/>
+Revised model.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Probe;
diff --git a/AixLib/Electrical/AC/OnePhase/Sensors/package.mo b/AixLib/Electrical/AC/OnePhase/Sensors/package.mo
new file mode 100644
index 0000000000..14ea97335a
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sensors/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.AC.OnePhase;
+package Sensors "Package with sensors for AC electrical systems"
+extends Modelica.Icons.SensorsPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models for voltage, current and power sensors.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Sensors;
diff --git a/AixLib/Electrical/AC/OnePhase/Sensors/package.order b/AixLib/Electrical/AC/OnePhase/Sensors/package.order
new file mode 100644
index 0000000000..0fb45c82b3
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sensors/package.order
@@ -0,0 +1,3 @@
+GeneralizedSensor
+Probe
+Examples
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/Examples/FixedVoltageSource.mo b/AixLib/Electrical/AC/OnePhase/Sources/Examples/FixedVoltageSource.mo
new file mode 100644
index 0000000000..f38d2ac5b1
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/Examples/FixedVoltageSource.mo
@@ -0,0 +1,44 @@
+within AixLib.Electrical.AC.OnePhase.Sources.Examples;
+model FixedVoltageSource
+  "This example illustrates how using a fixed voltage source"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive RL(
+      P_nominal=-300, mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    V_nominal=120) "Load model"
+    annotation (Placement(transformation(extent={{20,-10},{40,10}})));
+  FixedVoltage grid(
+    f=60,
+    V=120,
+    phiSou=0.34906585039887) "AC one phase electrical grid"
+           annotation (Placement(transformation(extent={{-40,-10},{-20,10}})));
+  Sensors.Probe sen(V_nominal=120)
+    "Probe that measures the voltage at the load"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+equation
+  connect(grid.terminal, RL.terminal)
+                                     annotation (Line(
+      points={{-20,4.44089e-16},{-20,0},{20,0},{20,5.55112e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(grid.terminal, sen.term) annotation (Line(
+      points={{-20,6.66134e-16},{0,6.66134e-16},{0,21},{4.44089e-16,21}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (    experiment(StopTime=1.0, Tolerance=1e-6),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/FixedVoltageSource.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example shows how to use a fixed voltage generator model.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FixedVoltageSource;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/Examples/VariablePowerSource.mo b/AixLib/Electrical/AC/OnePhase/Sources/Examples/VariablePowerSource.mo
new file mode 100644
index 0000000000..79500078aa
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/Examples/VariablePowerSource.mo
@@ -0,0 +1,68 @@
+within AixLib.Electrical.AC.OnePhase.Sources.Examples;
+model VariablePowerSource
+  "This example illustrates how using a variable power source"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sources.Generator generator(phiGen(displayUnit="deg") = 0.26179938779915, f=60)
+    "AC generator model"
+    annotation (Placement(transformation(extent={{-50,-10},{-30,10}})));
+  Modelica.Blocks.Sources.Sine generation(
+    offset=200,
+    startTime=1,
+    amplitude=100,
+    f=0.05) "Generated power"
+    annotation (Placement(transformation(extent={{-92,-10},{-72,10}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Inductive RL(mode=Types.Load.VariableZ_y_input,
+      P_nominal=-300,
+    V_nominal=120) "Load model"
+    annotation (Placement(transformation(extent={{20,-10},{40,10}})));
+  AixLib.Electrical.AC.OnePhase.Sources.Grid grid(f=60, V=120)
+    "AC one phase electrical grid"
+           annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+  Modelica.Blocks.Sources.Trapezoid load(
+    rising=2,
+    width=3,
+    falling=3,
+    period=10,
+    startTime=1,
+    amplitude=0.8,
+    offset=0.2) "Power consumption profile"
+    annotation (Placement(transformation(extent={{80,-10},{60,10}})));
+equation
+  connect(generation.y, generator.P) annotation (Line(
+      points={{-71,0},{-50,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(generator.terminal, RL.terminal)
+                                          annotation (Line(
+      points={{-30,0},{20,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(grid.terminal, RL.terminal)
+                                     annotation (Line(
+      points={{-10,40},{-10,0},{20,0},{20,5.55112e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load.y, RL.y)
+                       annotation (Line(
+      points={{59,0},{40,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (    experiment(StopTime=1.0, Tolerance=1e-6),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/VariablePowerSource.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example shows how to use a variable generator model. The model has to be used
+together with a voltage source generator.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end VariablePowerSource;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/Examples/WindTurbine.mo b/AixLib/Electrical/AC/OnePhase/Sources/Examples/WindTurbine.mo
new file mode 100644
index 0000000000..d20a275e8e
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/Examples/WindTurbine.mo
@@ -0,0 +1,85 @@
+within AixLib.Electrical.AC.OnePhase.Sources.Examples;
+model WindTurbine "Example for the WindTurbine AC model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.OnePhase.Sources.WindTurbine  tur(
+    table=[3.5, 0;
+           5.5,   100;
+           12, 900;
+           14, 1000;
+           25, 1000], h=10,
+    scale=10,
+    V_nominal=120) "Wind turbine"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={60,0})));
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
+      computeWetBulbTemperature=false, filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data"
+    annotation (Placement(transformation(extent={{-52,36},{-32,56}})));
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather bus"
+    annotation (Placement(transformation(extent={{16,36},{36,56}})));
+  AixLib.Electrical.AC.OnePhase.Loads.Resistive
+                                            res(P_nominal=-500, V_nominal=120)
+    "Resistive line"
+    annotation (Placement(transformation(extent={{-22,-30},{-2,-10}})));
+  AixLib.Electrical.AC.OnePhase.Sources.Grid sou(f=60, V=120)
+    "Voltage source"
+    annotation (Placement(transformation(extent={{-80,10},{-60,30}})));
+  AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance
+                                                  lin(R=0.1)
+    "Transmission line"
+    annotation (Placement(transformation(extent={{-22,-10},{-2,10}})));
+  AixLib.Electrical.AC.OnePhase.Sensors.GeneralizedSensor
+                                                    sen "Generalized sensor"
+    annotation (Placement(transformation(extent={{8,-10},{28,10}})));
+equation
+  connect(weaDat.weaBus,weaBus)  annotation (Line(
+      points={{-32,46},{26,46}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(weaBus.winSpe,tur. vWin) annotation (Line(
+      points={{26,46},{60,46},{60,12}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(sou.terminal, lin.terminal_n) annotation (Line(
+      points={{-70,10},{-70,0},{-22,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, res.terminal) annotation (Line(
+      points={{-70,10},{-70,-20},{-22,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(lin.terminal_p, sen.terminal_n) annotation (Line(
+      points={{-2,0},{8,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, tur.terminal) annotation (Line(
+      points={{28,0},{50,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (    experiment(StopTime=172800, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This model illustrates the use of the wind turbine model which is connected to a AC voltage source and a resistance.
+This voltage source can represent the grid to which the
+circuit is connected.
+Wind data for San Francisco, CA, are used.
+The turbine cut-in wind speed is <i>3.5</i> m/s,
+and hence it is off in the first day when the wind speed is low.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/WindTurbine.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end WindTurbine;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/Examples/package.mo b/AixLib/Electrical/AC/OnePhase/Sources/Examples/package.mo
new file mode 100644
index 0000000000..a6b7734c4f
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Electrical.AC.OnePhase.Sources;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Sources\">
+AixLib.Electrical.AC.OnePhase.Sources</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/Examples/package.order b/AixLib/Electrical/AC/OnePhase/Sources/Examples/package.order
new file mode 100644
index 0000000000..b61d6f70a5
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/Examples/package.order
@@ -0,0 +1,3 @@
+FixedVoltageSource
+VariablePowerSource
+WindTurbine
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/FixedVoltage.mo b/AixLib/Electrical/AC/OnePhase/Sources/FixedVoltage.mo
new file mode 100644
index 0000000000..40008484c8
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/FixedVoltage.mo
@@ -0,0 +1,83 @@
+within AixLib.Electrical.AC.OnePhase.Sources;
+model FixedVoltage "Fixed single phase AC voltage source"
+  extends AixLib.Electrical.Interfaces.Source(
+    redeclare package PhaseSystem = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_p terminal);
+  parameter Modelica.Units.SI.Frequency f(start=60) "Frequency of the source";
+  parameter Modelica.Units.SI.Voltage V(start=110) "RMS voltage of the source";
+  parameter Modelica.Units.SI.Angle phiSou=0 "Phase shift of the source";
+protected
+  Modelica.Units.SI.Angle thetaRel
+    "Absolute angle of rotating system as offset to thetaRef";
+equation
+  if Connections.isRoot(terminal.theta) then
+    PhaseSystem.thetaRef(terminal.theta) =  2*Modelica.Constants.pi*f*time;
+  end if;
+  thetaRel = PhaseSystem.thetaRel(terminal.theta);
+  terminal.v = PhaseSystem.phaseVoltages(V, thetaRel + phiSou);
+
+  annotation (
+    defaultComponentName="fixVol",
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+            -100},{100,100}}),
+                   graphics={
+        Ellipse(
+          extent={{-60,60},{60,-60}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid), Line(
+          points={{-44,0},{-24,40},{-4,0},{16,-40},{36,0}},
+          color={0,0,0},
+          smooth=Smooth.Bezier),
+        Text(
+          extent={{-120,100},{120,60}},
+          textColor={0,0,0},
+          textString="%name"),
+        Line(
+          points={{60,0},{90,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(visible = definiteReference == true,
+          points={{80,-46},{120,-46}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = definiteReference == true,
+          points={{80,-46},{106,-20}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = definiteReference == true,
+          points={{102,-22},{114,-30},{118,-48}},
+          color={0,120,120},
+          smooth=Smooth.Bezier),
+        Text(
+          extent={{-118,-60},{122,-100}},
+          textColor={0,0,0},
+          textString="V = %V")}),
+      Documentation(info="<html>
+<p>
+This is a constant voltage source. The complex voltage is specified by the RMS voltage
+and the phase shift.
+</p>
+</html>",
+ revisions="<html>
+<ul>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Added <code>replaceable</code> to terminal redeclaration as they are redeclared by
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage</a>.
+</li>
+<li>
+September 4, 2014, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FixedVoltage;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/Generator.mo b/AixLib/Electrical/AC/OnePhase/Sources/Generator.mo
new file mode 100644
index 0000000000..3a587bd4e5
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/Generator.mo
@@ -0,0 +1,109 @@
+within AixLib.Electrical.AC.OnePhase.Sources;
+model Generator "Model of a generator"
+  extends AixLib.Electrical.Interfaces.Source(
+    redeclare package PhaseSystem = PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_p terminal);
+  parameter Modelica.Units.SI.Frequency f(start=60) "Frequency of the source";
+  parameter Modelica.Units.SI.Angle phiGen(displayUnit="deg") = 0
+    "Phase shift of the source";
+  Modelica.Units.SI.Current I "value of current";
+  Modelica.Blocks.Interfaces.RealInput P
+    "Variable power generated by the source"
+     annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        origin={-100,0}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        origin={-100,0})));
+protected
+  Modelica.Units.SI.Angle thetaRel
+    "Absolute angle of rotating system as offset to thetaRef";
+equation
+  if Connections.isRoot(terminal.theta) then
+      PhaseSystem.thetaRef(terminal.theta) =  2*Modelica.Constants.pi*f*time;
+  end if;
+
+  thetaRel = PhaseSystem.thetaRel(terminal.theta);
+
+  terminal.i = PhaseSystem.phaseCurrents(I, thetaRel+phiGen);
+  0 = PhaseSystem.activePower(terminal.v, terminal.i) + P;
+
+  annotation (
+      defaultComponentName="gen",
+      Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+            -100},{100,100}}),
+                         graphics={Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Polygon(
+          points={{-52,48},{-52,-52},{60,-16},{60,12},{-52,48}},
+          lineColor={0,0,0},
+          smooth=Smooth.None,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-120,130},{120,100}},
+          textColor={0,0,0},
+          textString="%name"),
+        Line(visible = definiteReference == true,
+          points={{-20,-128},{20,-128}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = definiteReference == true,
+          points={{-20,-128},{6,-102}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = definiteReference == true,
+          points={{2,-104},{14,-112},{18,-130}},
+          color={0,120,120},
+          smooth=Smooth.Bezier)}),
+    Documentation(info="<html>
+<p>
+Model of a generator that produces real power
+<code>P</code> with a given phase shift <code>phiGen</code>.
+</p>
+<p>
+This model must be used with
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Sources.Grid\">
+AixLib.Electrical.AC.OnePhase.Sources.Grid</a>
+or with a voltage source from the package
+<a href=\"modelica://Modelica.Electrical.QuasiStatic.SinglePhase.Sources\">
+Modelica.Electrical.QuasiStatic.SinglePhase.Sources</a>.
+Otherwise, there will be no equation that defines the phase
+angle of the voltage.
+</p>
+<p>
+The boolean flags <code>potentialReference</code> and
+<code>definiteReference</code> allows to select the phase angle of the
+generator as reference for the models connected to it. More info about
+these flags are available in
+<a href=\"modelica://AixLib.Electrical.AC.UsersGuide\">
+AixLib.Electrical.AC.UsersGuide</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2019, by Michael Wetter:<br/>
+Added <code>replaceable</code> for terminal.
+</li>
+<li>
+September 4, 2014, by Michael Wetter:<br/>
+Revised model.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 4, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generator;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/Grid.mo b/AixLib/Electrical/AC/OnePhase/Sources/Grid.mo
new file mode 100644
index 0000000000..67a6659068
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/Grid.mo
@@ -0,0 +1,159 @@
+within AixLib.Electrical.AC.OnePhase.Sources;
+model Grid "Electrical grid"
+
+  replaceable AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_p terminal
+    annotation (Placement(transformation(extent={{-10,
+            -110},{10,-90}}), iconTransformation(extent={{-10,-110},{10,-90}})));
+  parameter Modelica.Units.SI.Frequency f(start=60) "Frequency of the source";
+  parameter Modelica.Units.SI.Voltage V(start=110) "RMS voltage of the source";
+  parameter Modelica.Units.SI.Angle phiSou=0 "Phase shift angle of the source";
+  AixLib.Electrical.AC.Interfaces.PowerOutput P
+    "Power consumed from grid if positive, or fed to grid if negative"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  replaceable AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage sou(
+    potentialReference=true,
+    definiteReference=true,
+    final f=f,
+    final V=V,
+    final phiSou=phiSou) "Voltage source"
+     annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        origin={10,0})));
+equation
+  P.real = -sou.S[1];
+  P.apparent = Modelica.Fluid.Utilities.regRoot(sou.S[2]^2 + sou.S[1]^2, delta = 0.01);
+  P.phi = sou.phi;
+  P.cosPhi = cos(sou.phi);
+  connect(sou.terminal, terminal) annotation (Line(
+      points={{-4.44089e-16,6.66134e-16},{-4.44089e-16,-100},{4.44089e-16,-100}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="gri",
+    Documentation(info="<html>
+<p>
+Model that can be used to represent the electrical grid supply.
+</p>
+<p>
+The model has an output connector named <code>P</code> that
+contains information about the power supplied by the grid to the network.
+The convention is that <code>P.real</code> is positive if real power is
+consumed from the grid, and negative if it is fed into the grid.
+</p>
+<p>
+The parameter <code>V</code> is the root means square of the voltage.
+In US households, this is <i>120</i> Volts at <i>60</i> Hz,
+in Europe it is <i>230</i> Volts at <i>50</i> Hz.
+</p>
+</html>",
+ revisions="<html>
+<ul>
+<li>
+August 31, 2016, by Michael Wetter:<br/>
+Corrected sign error in documentation string of variable <code>P</code>.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-120,130},{120,100}},
+          textColor={0,0,0},
+          textString="%name"),
+        Line(
+          points={{-60,-32},{-60,-72}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-74,-32},{-44,-32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-72,-38},{-48,-28},{-28,-16},{-16,-2},{-12,14}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-46,-38},{-22,-28},{-2,-16},{10,-2},{14,14}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-72,-32},{-72,-38}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-46,-32},{-46,-38}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-14,20},{16,20}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{0,20},{0,-20}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-12,20},{-12,14}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{14,20},{14,14}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{14,14},{38,24},{58,36},{70,50},{74,66}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-12,14},{12,24},{32,36},{44,50},{48,66}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{60,72},{60,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{46,72},{76,72}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{48,72},{48,66}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{74,72},{74,66}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-100,-76},{-96,-74},{-88,-68},{-76,-54},{-72,-38}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-100,-88},{-82,-80},{-62,-68},{-50,-54},{-46,-38}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{48,68},{72,78},{92,90},{98,94},{100,96}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{74,68},{84,72},{100,82}},
+          color={175,175,175},
+          smooth=Smooth.Bezier)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Grid;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/WindTurbine.mo b/AixLib/Electrical/AC/OnePhase/Sources/WindTurbine.mo
new file mode 100644
index 0000000000..b68f13b257
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/WindTurbine.mo
@@ -0,0 +1,93 @@
+within AixLib.Electrical.AC.OnePhase.Sources;
+model WindTurbine "Simple wind turbine model"
+  extends AixLib.Electrical.BaseClasses.WindTurbine.PartialWindTurbine(
+    redeclare package PhaseSystem = AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare replaceable Interfaces.Terminal_p terminal,
+    V_nominal(start = 110));
+
+  parameter Real pf(min=0, max=1) = 0.9 "Power factor"
+    annotation (Dialog(group="AC-Conversion"));
+  parameter Real eta_DCAC(min=0, max=1) = 0.9 "Efficiency of DC/AC conversion"
+    annotation (Dialog(group="AC-Conversion"));
+  replaceable AixLib.Electrical.AC.OnePhase.Loads.Capacitive load(
+    final mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    final pf=pf,
+    final P_nominal=0,
+    final V_nominal=V_nominal) "Load model"
+    annotation (Placement(transformation(extent={{12,-10},{32,10}})));
+protected
+  Modelica.Blocks.Math.Gain gain_DCAC(final k=eta_DCAC) annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=180,
+        origin={52,0})));
+equation
+  connect(load.terminal, terminal) annotation (Line(
+      points={{12,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(gain_DCAC.y, load.Pow) annotation (Line(
+      points={{41,0},{32,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(gain.y, gain_DCAC.u) annotation (Line(
+      points={{23,30},{80,30},{80,0},{64,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (
+defaultComponentName="winTur",
+ Documentation(info="<html>
+<p>
+Model of a wind turbine whose power is computed as a function of wind-speed as defined in a table.
+</p>
+<p>
+Input to the model is the local wind speed.
+The model requires the specification of a table that maps wind speed in meters per second to generated
+power <i>P<sub>t</sub></i> in Watts.
+The model has a parameter called <code>scale</code> with a default value of one
+that can be used to scale the power generated by the wind turbine.
+The generated active electrical power is
+<p align=\"center\" style=\"font-style:italic;\">
+P = P<sub>t</sub> scale &eta;<sub>DCAC</sub>
+</p>
+<p>
+where <i>&eta;<sub>DCAC</sub></i> is the efficiency of the conversion of the DC electrical power to AC.
+For example, the following specification (with default <code>scale=1</code>) of a wind turbine
+</p>
+<pre>
+  WindTurbine_Table tur(
+    table=[3.5, 0;
+           5.5,   100;
+           12, 900;
+           14, 1000;
+           25, 1000]) \"Wind turbine\";
+</pre>
+<p>
+yields the performance shown below. In this example, the cut-in wind speed is <i>3.5</i> meters per second,
+and the cut-out wind speed is <i>25</i> meters per second,
+as entered by the first and last entry of the wind speed column.
+Below and above these wind speeds, the generated power is zero.
+</p>
+<p align=\"center\">
+<img alt=\"alt-image\" src=\"modelica://AixLib/Resources/Images/Electrical/DC/Sources/WindTurbine_Table.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2019, by Michael Wetter:<br/>
+Added <code>replaceable</code> for terminal.
+</li>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+In load, set <code>P_nominal = 0</code> as it is not used.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WindTurbine;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/package.mo b/AixLib/Electrical/AC/OnePhase/Sources/package.mo
new file mode 100644
index 0000000000..acbd1d018c
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.AC.OnePhase;
+package Sources "Package with sources models for one phase AC systems"
+  extends Modelica.Icons.SourcesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models of AC sources.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Sources;
diff --git a/AixLib/Electrical/AC/OnePhase/Sources/package.order b/AixLib/Electrical/AC/OnePhase/Sources/package.order
new file mode 100644
index 0000000000..6e0d521abb
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/Sources/package.order
@@ -0,0 +1,5 @@
+FixedVoltage
+Generator
+Grid
+WindTurbine
+Examples
diff --git a/AixLib/Electrical/AC/OnePhase/package.mo b/AixLib/Electrical/AC/OnePhase/package.mo
new file mode 100644
index 0000000000..84598abba5
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/package.mo
@@ -0,0 +1,21 @@
+within AixLib.Electrical.AC;
+package OnePhase "One phase AC systems"
+extends Modelica.Icons.VariantsPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+Package with models for alternate current (AC) single phase systems.<br/>
+The models contained in this package use the phase system
+<a href=\"modelica://AixLib.Electrical.PhaseSystems.OnePhase\">
+AixLib.Electrical.PhaseSystems.OnePhase</a> and they assume 120 V as nominal RMS voltage.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 4, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end OnePhase;
diff --git a/AixLib/Electrical/AC/OnePhase/package.order b/AixLib/Electrical/AC/OnePhase/package.order
new file mode 100644
index 0000000000..0e47a34334
--- /dev/null
+++ b/AixLib/Electrical/AC/OnePhase/package.order
@@ -0,0 +1,8 @@
+Basics
+Conversion
+Lines
+Loads
+Sensors
+Sources
+Examples
+Interfaces
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACConverter.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACConverter.mo
new file mode 100644
index 0000000000..d6ecaebab7
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACConverter.mo
@@ -0,0 +1,33 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion;
+model ACACConverter "AC AC converter three phase balanced systems"
+  extends AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter(
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  annotation (
+  defaultComponentName="conACAC",
+  Documentation(info="<html>
+<p>
+This model represents a simplified conversion between two AC
+three-phase balanced systems. The conversion losses are represented by a
+constant efficiency <i>&eta;</i>.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter</a> for more
+information.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 29, 2012, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACConverter;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACTransformer.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACTransformer.mo
new file mode 100644
index 0000000000..1d613ddfa8
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACTransformer.mo
@@ -0,0 +1,33 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion;
+model ACACTransformer "AC AC transformer three phase balanced systems"
+  extends AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer(
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  annotation (
+  defaultComponentName="traACAC",
+  Documentation(info="<html>
+<p>
+Simple transformer model for three-phase
+balanced AC systems. The model does not include core and
+magnetic losses.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer</a> for more
+information.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 29, 2012, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformer;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACTransformerFull.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACTransformerFull.mo
new file mode 100644
index 0000000000..e80bdddb2a
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACACTransformerFull.mo
@@ -0,0 +1,33 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion;
+model ACACTransformerFull
+  "AC AC transformer full model for three phase balanced systems"
+  extends AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull(
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  annotation (
+defaultComponentName="traACAC",
+Documentation(info="<html>
+<p>
+Model of a transformer for three-phase
+balanced AC systems. The model includes core and magnetic losses.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull</a> for more
+information.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 29, 2012, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerFull;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACDCConverter.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACDCConverter.mo
new file mode 100644
index 0000000000..97d06079e0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/ACDCConverter.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion;
+model ACDCConverter "AC DC converter"
+  extends AixLib.Electrical.AC.OnePhase.Conversion.ACDCConverter(
+    redeclare Interfaces.Terminal_n terminal_n);
+
+  annotation (
+defaultComponentName="conACDC",
+Documentation(info="<html>
+<p>
+This model represents a simplified conversion between a three-phase
+balanced AC system and a DC systems.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACDCConverter\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACDCConverter</a> for more
+information.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+July 24, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACDCConverter;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACConverter.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACConverter.mo
new file mode 100644
index 0000000000..cba34c6c78
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACConverter.mo
@@ -0,0 +1,67 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples;
+model ACACConverter
+  "This example illustrates how to use the AC/AC converter model"
+  extends Modelica.Icons.Example;
+
+  AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACConverter
+    conACAC(eta=0.9, conversionFactor=120/480) "ACAC transformer"
+    annotation (Placement(transformation(extent={{-10,0},{10,20}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage sou(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-60,10})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Inductive load(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=120) "Load model"
+    annotation (Placement(transformation(extent={{24,0},{44,20}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=0.5,
+    startTime=0.3,
+    height=2000,
+    offset=-1000) "Power consumed by the model"
+    annotation (Placement(transformation(extent={{80,0},{60,20}})));
+equation
+  connect(sou.terminal, conACAC.terminal_n) annotation (Line(
+      points={{-50,10},{-10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(conACAC.terminal_p, load.terminal)     annotation (Line(
+      points={{10,10},{24,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow) annotation (Line(
+      points={{59,10},{44,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This example illustrates the use of a model that converts AC voltage to AC voltage.
+The transformer model assumes a linear loss when transmitting the power.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+October 1, 2015, by Michael Wetter:<br/>
+Removed assignment of <code>load.P_nominal</code> as it is
+not required and leads to dublicate assignments.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACConverter.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACConverter;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformer.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformer.mo
new file mode 100644
index 0000000000..7f2dc5f237
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformer.mo
@@ -0,0 +1,112 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples;
+model ACACTransformer
+  "This example illustrates how to use the AC/AC simplified transformer model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACTransformer tra_load(
+    Zperc=0.03,
+    VABase=4000,
+    XoverR=8,
+    VHigh=480,
+    VLow=120) "Transformer with load"
+    annotation (Placement(transformation(extent={{-18,40},{2,60}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage sou(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+      annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,50})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Inductive load(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    pf=0.8,
+    V_nominal=120) "Load model"
+    annotation (Placement(transformation(extent={{10,40},{30,60}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=0.5,
+    startTime=0.3,
+    offset=0,
+    height=-4000*0.8) "Load power consumption profile"
+    annotation (Placement(transformation(extent={{70,40},{50,60}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACTransformer tra_cc(
+    XoverR=8,
+    Zperc=0.03,
+    VABase=4000,
+    VHigh=480,
+    VLow=120) "Transformer with short circuit"
+    annotation (Placement(transformation(extent={{-16,0},{4,20}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Impedance shortCircuit(R=1e-8)
+    "Short circuit"
+    annotation (Placement(transformation(extent={{10,0},{30,20}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACTransformer tra_void(
+    XoverR=8,
+    Zperc=0.03,
+    VABase=4000,
+    VHigh=480,
+    VLow=120) "Transformer with secondary not connected"
+    annotation (Placement(transformation(extent={{-16,-30},{4,-10}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage sou1(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source for open and short circuit tests"
+                          annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,10})));
+equation
+  connect(sou.terminal, tra_load.terminal_n)
+                                            annotation (Line(
+      points={{-60,50},{-18,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(tra_load.terminal_p, load.terminal)    annotation (Line(
+      points={{2,50},{10,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow) annotation (Line(
+      points={{49,50},{30,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(tra_cc.terminal_p, shortCircuit.terminal) annotation (Line(
+      points={{4,10},{10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou1.terminal, tra_cc.terminal_n) annotation (Line(
+      points={{-60,10},{-16,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou1.terminal, tra_void.terminal_n) annotation (Line(
+      points={{-60,10},{-38,10},{-38,-20},{-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This example illustrates the use of the AC/AC transformer model.
+The example shows three different configurations:
+</p>
+<ul>
+<li>With a load connected,</li>
+<li>without a load connected, and</li>
+<li>with a short circuit connection.</li>
+</ul>
+</html>",    revisions="<html>
+<ul>
+<li>
+October 1, 2015, by Michael Wetter:<br/>
+Removed assignment of <code>load.P_nominal</code> as it is
+not required and leads to dublicate assignments.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformer.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformer;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformerFull.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformerFull.mo
new file mode 100644
index 0000000000..fd5c792b43
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformerFull.mo
@@ -0,0 +1,133 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples;
+model ACACTransformerFull
+  "This example illustrates how to use the AC/AC transformer model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACTransformerFull tra_load(
+    R1=0.0001,
+    L1=0.0001,
+    R2=0.0001,
+    L2=0.0001,
+    VABase=4000,
+    magEffects=true,
+    Rm=10,
+    Lm=10,
+    VHigh=480,
+    VLow=120,
+    f=60) "Transformer with load"
+    annotation (Placement(transformation(extent={{-18,40},{2,60}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage sou(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,50})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Inductive load(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    pf=0.8,
+    V_nominal=120) "Load"
+    annotation (Placement(transformation(extent={{10,40},{30,60}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=0.5,
+    startTime=0.3,
+    offset=0,
+    height=-4000*0.8) "Load power consumption profile"
+    annotation (Placement(transformation(extent={{70,40},{50,60}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACTransformerFull tra_cc(
+    VABase=4000,
+    R1=0.01,
+    L1=0.01,
+    R2=0.01,
+    L2=0.01,
+    magEffects=false,
+    Rm=100,
+    Lm=100,
+    VHigh=480,
+    VLow=120,
+    f=60) "Transformer with short circuit connection"
+    annotation (Placement(transformation(extent={{-16,0},{4,20}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Impedance shortCircuit(R=1e-8)
+    "Short circuit"
+    annotation (Placement(transformation(extent={{10,0},{30,20}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACTransformerFull tra_void(
+    VABase=4000,
+    R1=0.01,
+    L1=0.01,
+    R2=0.01,
+    L2=0.01,
+    magEffects=false,
+    Rm=100,
+    Lm=100,
+    VHigh=480,
+    VLow=120,
+    f=60) "Transformer with open connection"
+    annotation (Placement(transformation(extent={{-16,-30},{4,-10}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage sou1(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source for short circuit and open tests"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-70,10})));
+equation
+  connect(sou.terminal, tra_load.terminal_n)
+    annotation (Line(
+      points={{-60,50},{-18,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(tra_load.terminal_p, load.terminal)    annotation (Line(
+      points={{2,50},{10,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow) annotation (Line(
+      points={{49,50},{30,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(tra_cc.terminal_p, shortCircuit.terminal) annotation (Line(
+      points={{4,10},{10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou1.terminal, tra_cc.terminal_n) annotation (Line(
+      points={{-60,10},{-16,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou1.terminal, tra_void.terminal_n) annotation (Line(
+      points={{-60,10},{-38,10},{-38,-20},{-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This example illustrates the use of the AC/AC transformer model
+that includes losses at the primary and secondary side and magnetization
+effects.
+The example shows three different configurations:
+</p>
+<ul>
+<li>With a load connected,</li>
+<li>without a load connected, and</li>
+<li>with a short circuit connection.</li>
+</ul>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+October 1, 2015, by Michael Wetter:<br/>
+Removed assignment of <code>load.P_nominal</code> as it is
+not required and leads to dublicate assignments.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformerFull.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerFull;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACDCConverter.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACDCConverter.mo
new file mode 100644
index 0000000000..b4e71178d2
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACDCConverter.mo
@@ -0,0 +1,86 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples;
+model ACDCConverter
+  "This example illustrates how to use the AC/DC converter model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.DC.Loads.Resistor res(
+    R=1,
+    V_nominal=120,
+    i(each start=0))
+    "Resistive load" annotation (Placement(
+        transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={50,10})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACDCConverter conversion(
+    eta=0.9,
+    ground_AC=false,
+    ground_DC=true,
+    conversionFactor=120/480) "AC/DC transformer"
+    annotation (Placement(transformation(extent={{-10,0},{10,20}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage sou(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-62,10})));
+  AixLib.Electrical.DC.Loads.Conductor load(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=120) "Variable resistive load"
+    annotation (Placement(
+        transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={50,-10})));
+  Modelica.Blocks.Sources.Ramp pow(
+    duration=0.5,
+    startTime=0.2,
+    offset=-200,
+    height=5200) "Variable load profile"
+    annotation (Placement(transformation(extent={{90,-20},{70,0}})));
+equation
+  connect(sou.terminal, conversion.terminal_n) annotation (Line(
+      points={{-52,10},{-10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(conversion.terminal_p, res.terminal) annotation (Line(
+      points={{10,10},{40,10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(conversion.terminal_p, load.terminal) annotation (Line(
+      points={{10,10},{30,10},{30,-10},{40,-10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(pow.y, load.Pow) annotation (Line(
+      points={{69,-10},{60,-10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This example illustrates the use of a model that converts AC voltage to DC voltage.
+The transformer model assumes a linear loss when transmitting the power.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+October 1, 2015, by Michael Wetter:<br/>
+Removed assignment of <code>load.P_nominal</code> as it is
+not required and leads to dublicate assignments.
+</li>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACDCConverter.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACDCConverter;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/package.mo
new file mode 100644
index 0000000000..9951ec19b9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Conversion;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Conversion\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/package.order
new file mode 100644
index 0000000000..4e2ad8d42f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/package.order
@@ -0,0 +1,4 @@
+ACACConverter
+ACACTransformer
+ACACTransformerFull
+ACDCConverter
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/package.mo
new file mode 100644
index 0000000000..fea18417b0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced;
+package Conversion "Package with transformers and converter models for three-phase balanced AC systems"
+  extends Modelica.Icons.Package;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models for three-phase balanced AC/AC
+transformers and AC/DC converters.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Conversion;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/package.order
new file mode 100644
index 0000000000..6e342d1531
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Conversion/package.order
@@ -0,0 +1,5 @@
+ACACConverter
+ACACTransformer
+ACACTransformerFull
+ACDCConverter
+Examples
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/Terminal_n.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/Terminal_n.mo
new file mode 100644
index 0000000000..0356f1a5e9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/Terminal_n.mo
@@ -0,0 +1,39 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Interfaces;
+connector Terminal_n "AC three-phase balanced terminal ('negative')"
+  extends AixLib.Electrical.Interfaces.Terminal(
+    redeclare replaceable package PhaseSystem = PhaseSystems.OnePhase);
+  annotation (defaultComponentName = "term_p",
+  Documentation(info="<html>
+<p>Electric connector with a vector of negative pins.</p>
+</html>"),
+  Icon(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={           Text(
+          extent={{-60,60},{60,-60}},
+          textColor={255,255,255},
+          pattern=LinePattern.None,
+          textString=""),                    Polygon(
+          points={{-100,100},{-100,-100},{100,-100},{100,100},{-100,100}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}),
+  Diagram(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+        Text(
+          extent={{-120,120},{100,60}},
+          textColor={0,120,120},
+          textString="%name"),
+        Text(
+          extent={{14,16},{114,-84}},
+          textColor={255,255,255},
+          pattern=LinePattern.None,
+          textString=""),                    Polygon(
+          points={{-100,50},{-100,-50},{0,-50},{0,50},{-100,50}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal_n;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/Terminal_p.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/Terminal_p.mo
new file mode 100644
index 0000000000..7ae77e9826
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/Terminal_p.mo
@@ -0,0 +1,39 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Interfaces;
+connector Terminal_p "AC three-phase balanced terminal ('positive')"
+  extends AixLib.Electrical.Interfaces.Terminal(
+    redeclare replaceable package PhaseSystem = PhaseSystems.OnePhase);
+  annotation (defaultComponentName = "term_p",
+  Documentation(info="<html>
+<p>Electric connector with a vector of positive pins.</p>
+</html>"),
+  Icon(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={           Text(
+          extent={{-60,60},{60,-60}},
+          textColor={255,255,255},
+          pattern=LinePattern.None,
+          textString=""),                    Polygon(
+              points={{-100,100},{-100,-100},{100,-100},{100,100},{-100,100}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid)}),
+  Diagram(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+        Text(
+          extent={{-120,120},{100,60}},
+          textColor={0,120,120},
+          textString="%name"),
+        Text(
+          extent={{14,16},{114,-84}},
+          textColor={255,255,255},
+          pattern=LinePattern.None,
+          textString=""),                    Polygon(
+          points={{0,50},{0,-50},{100,-50},{100,50},{0,50}},
+          lineColor={0,120,120},
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal_p;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/package.mo
new file mode 100644
index 0000000000..87368ea927
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/package.mo
@@ -0,0 +1,22 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced;
+package Interfaces "Package interfaces for three-phase balanced AC systems"
+  extends Modelica.Icons.InterfacesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains connectors that are used by the models in the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced\">AixLib.Electrical.AC.ThreePhasesBalanced</a> package.
+The connectors extends the basic connectors
+<a href=\"modelica://AixLib.Electrical.Interfaces.Terminal\">AixLib.Electrical.Interfaces.Terminal</a>
+and define a new graphical icon in order to be distinguishable from connectors of other electrical systems (e.g. DC systems).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Interfaces;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/package.order
new file mode 100644
index 0000000000..d23ecfc486
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Interfaces/package.order
@@ -0,0 +1,2 @@
+Terminal_n
+Terminal_p
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine.mo
new file mode 100644
index 0000000000..60b771cb7f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine.mo
@@ -0,0 +1,132 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples;
+model ACLine "Test model for single phase lines that use commercial cables"
+  extends Modelica.Icons.Example;
+  ThreePhasesBalanced.Sources.FixedVoltage E(definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  ThreePhasesBalanced.Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  ThreePhasesBalanced.Lines.Line line_1(
+    P_nominal=5000,
+    l=2000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    V_nominal=480) "Resistive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+  ThreePhasesBalanced.Lines.Line line_2a(
+    P_nominal=5000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    l=1000,
+    V_nominal=480) "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  ThreePhasesBalanced.Loads.Impedance R2(R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  ThreePhasesBalanced.Lines.Line line_2b(
+    P_nominal=5000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    l=1000,
+    V_nominal=480) "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-32,-30},{-12,-10}})));
+  ThreePhasesBalanced.Lines.Line line_3a(
+    P_nominal=5000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    l=4000,
+    V_nominal=480) "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  ThreePhasesBalanced.Lines.Line line_3b(
+    P_nominal=5000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    l=4000,
+    V_nominal=480) "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-70},{-40,-50}})));
+  ThreePhasesBalanced.Loads.Impedance R3(R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-60},{20,-40}})));
+  ThreePhasesBalanced.Lines.Line line_sc(
+    P_nominal=5000,
+    l=2000,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.Cu50(),
+    V_nominal=480) "Line that connects the source and the short circuit"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  ThreePhasesBalanced.Loads.Impedance load_sc(R=0) "Short circuit"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+equation
+  connect(line_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-40,0},{-24,0},{-24,6.66134e-16},{-4.44089e-16,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_1.terminal_n) annotation (Line(
+      points={{-80,4.44089e-16},{-60,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_2a.terminal_n) annotation (Line(
+      points={{-80,4.44089e-16},{-70,4.44089e-16},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_2a.terminal_p, line_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-32,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-12,-20},{0,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-40},{-20,-40},{-20,-50},{0,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-60},{-20,-60},{-20,-50},{-5.55112e-16,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-40},{-60,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-60},{-60,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_sc.terminal_p, load_sc.terminal) annotation (Line(
+      points={{-40,30},{-4.44089e-16,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a line model to connect
+a source to a load that uses commercial cables.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the impedance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations.
+However, the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draws the same current.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLineMedium.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLineMedium.mo
new file mode 100644
index 0000000000..73e19d644b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLineMedium.mo
@@ -0,0 +1,166 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples;
+model ACLineMedium
+  "Test model for a single phase line that uses medium voltage commercial cable information "
+  extends Modelica.Icons.Example;
+  ThreePhasesBalanced.Sources.FixedVoltage E(definiteReference=true, V=15000,
+    f=60) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  ThreePhasesBalanced.Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  ThreePhasesBalanced.Lines.Line line_1(
+    P_nominal=5000,
+    l=2000,
+    redeclare AixLib.Electrical.Transmission.MediumVoltageCables.Generic
+          commercialCable = AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_10(),
+    V_nominal=15000) "Resistive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-58,-10},{-38,10}})));
+  ThreePhasesBalanced.Lines.Line line_2a(
+    P_nominal=5000,
+    l=1000,
+    redeclare AixLib.Electrical.Transmission.MediumVoltageCables.Generic
+          commercialCable = AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_10(),
+    V_nominal=15000) "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  ThreePhasesBalanced.Loads.Impedance R2(R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  ThreePhasesBalanced.Lines.Line line_2b(
+    P_nominal=5000,
+    l=1000,
+    redeclare AixLib.Electrical.Transmission.MediumVoltageCables.Generic
+          commercialCable = AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_10(),
+    V_nominal=15000) "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-32,-30},{-12,-10}})));
+  ThreePhasesBalanced.Lines.Line line_3a(
+    P_nominal=5000,
+    l=4000,
+    redeclare AixLib.Electrical.Transmission.MediumVoltageCables.Generic
+          commercialCable = AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_10(),
+    V_nominal=15000) "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  ThreePhasesBalanced.Lines.Line line_3b(
+    P_nominal=5000,
+    l=4000,
+    redeclare AixLib.Electrical.Transmission.MediumVoltageCables.Generic
+          commercialCable = AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_10(),
+    V_nominal=15000) "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-70},{-40,-50}})));
+  ThreePhasesBalanced.Loads.Impedance R3(R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-60},{20,-40}})));
+  ThreePhasesBalanced.Lines.Line line_sc(
+    P_nominal=5000,
+    l=2000,
+    redeclare AixLib.Electrical.Transmission.MediumVoltageCables.Generic
+          commercialCable = AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_10(),
+    V_nominal=15000) "Line that connects the source and the short circuit"
+    annotation (Placement(transformation(extent={{-58,20},{-38,40}})));
+  ThreePhasesBalanced.Loads.Impedance load_sc(R=0) "Short circuit"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+equation
+  connect(line_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-38,0},{-24,0},{-24,6.66134e-16},{-4.44089e-16,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_1.terminal_n) annotation (Line(
+      points={{-80,4.44089e-16},{-58,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_2a.terminal_n) annotation (Line(
+      points={{-80,4.44089e-16},{-70,4.44089e-16},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_2a.terminal_p, line_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-32,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-12,-20},{0,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-40},{-20,-40},{-20,-50},{0,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-60},{-20,-60},{-20,-50},{-5.55112e-16,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-40},{-60,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-60},{-60,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_sc.terminal_p, load_sc.terminal) annotation (Line(
+      points={{-38,30},{-4.44089e-16,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-58,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLineMedium.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Documentation and example added.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a line model to connect
+a source to a load that uses medium voltage commercial cable information.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the impedance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations,
+however the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draws the same current.
+</p>
+
+<h4>Note:</h4>
+
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px;\">
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">ThreePhasesBalanced.Lines.Line</span>
+<span style=\" font-family:'Courier New,courier';\"> line_1(</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier';\">    V_nominal=220,</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier';\">    P_nominal=5000,</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier';\">    l=2000,</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">redeclare </span>
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">AixLib.Electrical.Transmission.MediumVoltageCables.Generic</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier';\">          commercialCable =</span>
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\"> AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_10</span>
+<span style=\" font-family:'Courier New,courier';\">()) </span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#006400;\">    &quot;Resistive line that connects to load 1&quot;</span>
+</p>
+
+<p>
+The code snippet shows how a line model <code>line_1</code> redeclared its
+record type in order to be <code>AixLib.Electrical.Transmission.MediumVoltageCables.Generic</code>.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLineMedium;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_L.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_L.mo
new file mode 100644
index 0000000000..08b3739cf5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_L.mo
@@ -0,0 +1,110 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples;
+model ACLine_L "Test model for single phase inductive lines"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Inductance Lbase=10/2/Modelica.Constants.pi/60
+    "Base value for the line inductances";
+  ThreePhasesBalanced.Sources.FixedVoltage E(definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  ThreePhasesBalanced.Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  ThreePhasesBalanced.Loads.Impedance R2(R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  ThreePhasesBalanced.Loads.Impedance R3(R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-62},{20,-42}})));
+  ThreePhasesBalanced.Loads.Impedance load_sc(R=0) "Short circuit"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  ThreePhasesBalanced.Lines.TwoPortInductance Lline_sc(L=Lbase)
+    "Inductive line connected to the short circuit"
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+  ThreePhasesBalanced.Lines.TwoPortInductance Lline_1(L=Lbase)
+    "Inductive line connected to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  ThreePhasesBalanced.Lines.TwoPortInductance Lline_2a(L=0.5*Lbase)
+    "Inductive line connected to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  ThreePhasesBalanced.Lines.TwoPortInductance Lline_2b(L=0.5*Lbase)
+    "Inductive line connected to load 2"
+    annotation (Placement(transformation(extent={{-36,-30},{-16,-10}})));
+  ThreePhasesBalanced.Lines.TwoPortInductance Lline_3(L=2*Lbase)
+    "Inductive line connected to load 3"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  ThreePhasesBalanced.Lines.TwoPortInductance Lline_3b(L=2*Lbase)
+    "Inductive line connected to load 3"
+    annotation (Placement(transformation(extent={{-60,-70},{-40,-50}})));
+equation
+  connect(E.terminal, Lline_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_sc.terminal_p, load_sc.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Lline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Lline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_2a.terminal_p, Lline_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-36,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-16,-20},{-4.44089e-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Lline_3.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-40},{-60,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Lline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-60},{-60,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_3.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-40},{-20,-40},{-20,-52},{0,-52}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-60},{-20,-60},{-20,-52},{0,-52}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-06),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_L.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a purely inductive line model to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the inductance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations.
+However, the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draws the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_L;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_R.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_R.mo
new file mode 100644
index 0000000000..1b87cf846e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_R.mo
@@ -0,0 +1,108 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples;
+model ACLine_R "Test model for single phase resistive lines"
+  extends Modelica.Icons.Example;
+  ThreePhasesBalanced.Sources.FixedVoltage E(definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  ThreePhasesBalanced.Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  ThreePhasesBalanced.Loads.Impedance R2(R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  ThreePhasesBalanced.Loads.Impedance R3(R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-70},{20,-50}})));
+  ThreePhasesBalanced.Loads.Impedance sc_load(R=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  ThreePhasesBalanced.Lines.TwoPortResistance Rline_sc(R=10, useHeatPort=false)
+    "Resistive line that connects to the short circuit"
+    annotation (Placement(transformation(extent={{-60,60},{-40,40}})));
+  ThreePhasesBalanced.Lines.TwoPortResistance Rline_1(R=10)
+    "Resistive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  ThreePhasesBalanced.Lines.TwoPortResistance Rline_2a(R=5)
+    "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  ThreePhasesBalanced.Lines.TwoPortResistance Rline_2b(R=5)
+    "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-36,-30},{-16,-10}})));
+  ThreePhasesBalanced.Lines.TwoPortResistance Rline_3a(R=20)
+    "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  ThreePhasesBalanced.Lines.TwoPortResistance Rline_3b(R=20)
+    "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+equation
+  connect(E.terminal, Rline_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_sc.terminal_p, sc_load.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2a.terminal_p, Rline_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-36,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-16,-20},{-4.44089e-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-70},{-60,-70}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-70},{-20,-70},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_R.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a resistive line model to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the resistance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations.
+However, the equivalent resistance between each load and the source is the same.
+Since the equivalent resistances are the same, each load draws the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_R;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_RL.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_RL.mo
new file mode 100644
index 0000000000..73d899f77e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_RL.mo
@@ -0,0 +1,94 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples;
+model ACLine_RL "Test model for single phase inductive-resistive lines"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Resistance Rbase=10
+    "Base value for the line resistance";
+  parameter Modelica.Units.SI.Inductance Lbase=Rbase/2/Modelica.Constants.pi/60
+    "Base value for the line inductance";
+  ThreePhasesBalanced.Sources.FixedVoltage E(definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  ThreePhasesBalanced.Loads.Impedance load_sc_1(R=0) "Short circuit 1"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  ThreePhasesBalanced.Loads.Impedance load_sc_2(R=0) "Short circuit 2"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  ThreePhasesBalanced.Lines.TwoPortRL RL_2(R=Rbase, L=Lbase)
+    "Resistive-Inductive line connected to short circuit 2"
+    annotation (Placement(transformation(extent={{-48,-10},{-28,10}})));
+  ThreePhasesBalanced.Lines.TwoPortResistance R_1(R=Rbase)
+    "Resistance line connected to short circuit 1"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  ThreePhasesBalanced.Lines.TwoPortInductance L_1(L=Lbase)
+    "Inductance line connected to short circuit 1"
+    annotation (Placement(transformation(extent={{-30,20},{-10,40}})));
+  ThreePhasesBalanced.Lines.TwoPortRL RL_3(
+    R=Rbase,
+    L=Lbase,
+    mode=AixLib.Electrical.Types.Load.FixedZ_dynamic)
+    "Dynamic resistive-inductive line connected to short circuit 3"
+    annotation (Placement(transformation(extent={{-48,-40},{-28,-20}})));
+  ThreePhasesBalanced.Loads.Impedance load_sc_3(R=0) "Short circuit 3"
+    annotation (Placement(transformation(extent={{0,-40},{20,-20}})));
+equation
+  connect(E.terminal, R_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(R_1.terminal_p, L_1.terminal_n) annotation (Line(
+      points={{-40,30},{-30,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(L_1.terminal_p, load_sc_1.terminal) annotation (Line(
+      points={{-10,30},{0,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RL_2.terminal_n) annotation (Line(
+      points={{-80,0},{-48,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RL_2.terminal_p, load_sc_2.terminal) annotation (Line(
+      points={{-28,0},{0,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RL_3.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-30},{-48,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RL_3.terminal_p, load_sc_3.terminal) annotation (Line(
+      points={{-28,-30},{0,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (  experiment(StopTime=1.0,Tolerance=1e-6),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_RL.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a resistive-inductive line model to connect
+a source to a load.
+</p>
+<p>
+The model has three loads <code>load_sc_1</code>, <code>load_sc_2</code>,
+and <code>load_sc_3</code> representing short circuits <i>R=0</i>.
+The current that flows through the load depends on the impedance of the line.
+</p>
+<p>
+Each load is connected to the source with different configurations.
+However, the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draws the same current.
+</p>
+<p>
+<b>Note:</b>
+The line model <code>RL_3</code> is the same as <code>RL_2</code> but it uses
+dynamic phasors.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_RL;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGrid.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGrid.mo
new file mode 100644
index 0000000000..3ad19f5b47
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGrid.mo
@@ -0,0 +1,76 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples;
+model ACSimpleGrid "Test model for a network model"
+  extends Modelica.Icons.Example;
+  ThreePhasesBalanced.Lines.Network network(
+    redeclare AixLib.Electrical.Transmission.Grids.TestGrid2Nodes grid,
+      V_nominal=480)
+    "Network model that represents the connection between the source and the load"
+    annotation (Placement(transformation(extent={{20,-10},{0,10}})));
+  ThreePhasesBalanced.Loads.Inductive load(
+    P_nominal=2500,
+    mode=Types.Load.VariableZ_P_input,
+    V_nominal=480) "Load connected to the network"
+    annotation (Placement(transformation(extent={{-28,10},{-48,30}})));
+  ThreePhasesBalanced.Sources.FixedVoltage E(f=60, V=480) "Voltage source"
+   annotation (Placement(
+        transformation(
+        extent={{10,10},{-10,-10}},
+        rotation=180,
+        origin={-70,0})));
+  Modelica.Blocks.Sources.Ramp load_inputs(
+    height=5000,
+    duration=2,
+    offset=-2000,
+    startTime=0.5) "Input signal for the power consumption of the loads"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+equation
+  connect(load.terminal, network.terminal[2]) annotation (Line(
+      points={{-28,20},{-20,20},{-20,4.44089e-16},{-4.44089e-16,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, network.terminal[1]) annotation (Line(
+      points={{-60,-1.33227e-15},{-56,-1.33227e-15},{-56,4.44089e-16},{
+          -4.44089e-16,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load_inputs.y, load.Pow) annotation (Line(
+      points={{-59,30},{-54,30},{-54,20},{-48,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGrid.mos"
+        "Simulate and plot"),
+Documentation(revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a network model to connect
+a source to a load. In this simple case the network has two nodes
+that are connected by a commercial line cable.
+</p>
+<p>
+At the beginning of the simulation the load consumes power while at the
+and it produces power. The voltage at the load at the beginning is lower
+than the nominal RMS voltage (480 V) while at the end of the simulation it is higher.
+The voltage drop and increase are due to the presence of the cable between
+the source and the load.
+</p>
+<p>
+The network uses cables of the type <code>LowVoltageCable.Cu35</code> with
+a length of <i>200</i> m.
+</p>
+<p>
+The picture below describes the grid topology.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/testGrid2Nodes.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACSimpleGrid;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGridMedium.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGridMedium.mo
new file mode 100644
index 0000000000..cdb1ba5963
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGridMedium.mo
@@ -0,0 +1,117 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples;
+model ACSimpleGridMedium "Test model for a network model with medium voltage"
+  extends Modelica.Icons.Example;
+  ThreePhasesBalanced.Lines.Network network(
+      redeclare AixLib.Electrical.Transmission.Grids.TestGrid2NodesMedium grid,
+      lines(redeclare
+        AixLib.Electrical.Transmission.MediumVoltageCables.Generic
+        commercialCable = network.grid.cables,
+        each V_nominal = network.V_nominal),
+    V_nominal=15000)
+    "Network model that represents the connection between the source and the load"
+    annotation (Placement(transformation(extent={{20,-10},{0,10}})));
+  ThreePhasesBalanced.Loads.Inductive load(mode=Types.Load.VariableZ_P_input,
+    P_nominal=250000,
+    V_nominal=15000) "Load connected to the network"
+    annotation (Placement(transformation(extent={{-28,10},{-48,30}})));
+  ThreePhasesBalanced.Sources.FixedVoltage E(V=15000, f=60) "Voltage source"
+                                                              annotation (Placement(
+        transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={-70,0})));
+  Modelica.Blocks.Sources.Ramp load_inputs(
+    height=5000,
+    duration=2,
+    offset=-2000,
+    startTime=0.5) "Input signal for the power consumption of the loads"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+equation
+  connect(load.terminal, network.terminal[2]) annotation (Line(
+      points={{-28,20},{-20,20},{-20,4.44089e-16},{-4.44089e-16,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, network.terminal[1]) annotation (Line(
+      points={{-60,-8.88178e-16},{-56,-8.88178e-16},{-56,4.44089e-16},{-4.44089e-16,
+          4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load_inputs.y, load.Pow) annotation (Line(
+      points={{-59,30},{-54,30},{-54,20},{-48,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGridMedium.mos"
+        "Simulate and plot"),
+Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Documentation and example added.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a network model to connect
+a source to a load (using a medium voltage cable). In this simple case the network has two nodes
+that are connected by a commercial line cable.
+</p>
+<p>
+At the beginning of the simulation the load consumes power while at the
+end it produces power. The voltage at the load at the beginning is lower
+than the nominal RMS voltage (15 kV) while at the end of the simulation it is higher.
+The voltage drop and increase are due to the presence of the cable between
+the source and the load.
+</p>
+<p>
+The network uses cables of the type <code>MediumVoltageCables.Annealed_Al_30</code> with
+a length of <i>200</i> m.
+</p>
+<p>
+The picture below describes the grid topology.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/testGrid2Nodes.png\"/>
+</p>
+<h4>Note:</h4>
+<p>
+The cables are usually defined using the <code>LowVoltageCable.Generic</code> type. In order to use a
+medium voltage cable it is necessary to redeclare the type of the record <code>commercialCable</code>.
+</p>
+
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px;\">
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">ThreePhasesBalanced.Lines.Network</span>
+<span style=\" font-family:'Courier New,courier';\"> network(</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">redeclare </span>
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">AixLib.Electrical.Transmission.Grids.TestGrid2NodesMedium</span>
+<span style=\" font-family:'Courier New,courier';\"> grid,</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier';\">      lines(</span>
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">redeclare </span>
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">AixLib.Electrical.Transmission.MediumVoltageCables.Generic</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier';\">        commercialCable = network.grid.cables,</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">each </span>
+<span style=\" font-family:'Courier New,courier';\">V_nominal = network.V_nominal),</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier';\">    V_nominal=15000) </span>
+</p>
+
+<p>
+The code snippet shows how each line that is part of the vector <code>lines</code> is
+redeclared in order to have as type the record
+<code>AixLib.Electrical.Transmission.MediumVoltageCables.Generic</code>. The lines are initialized
+using the cables of the grid <code>network.grid.cables</code>. All the lines have the same
+nominal voltage <code>each V_nominal = network.V_nominal</code>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACSimpleGridMedium;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/package.mo
new file mode 100644
index 0000000000..285fcf1cb6
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Lines\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/package.order
new file mode 100644
index 0000000000..acaf01147b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Examples/package.order
@@ -0,0 +1,7 @@
+ACLine
+ACLineMedium
+ACLine_L
+ACLine_R
+ACLine_RL
+ACSimpleGrid
+ACSimpleGridMedium
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Line.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Line.mo
new file mode 100644
index 0000000000..8cc045dbe0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Line.mo
@@ -0,0 +1,71 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines;
+model Line "Model of an electrical line"
+  extends AixLib.Electrical.AC.OnePhase.Lines.Line(
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p,
+    V_nominal(start=480),
+    redeclare TwoPortRLC line(
+     R=R,
+     L=L,
+     C=C,
+     V_nominal=V_nominal));
+
+  annotation (
+    defaultComponentName="line",
+ Icon(graphics={
+        Ellipse(
+          extent={{-70,10},{-50,-10}},
+          lineColor={0,0,0},
+          fillColor={11,193,87},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-60,10},{60,-10}},
+          fillColor={11,193,87},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{50,10},{70,-10}},
+          lineColor={0,0,0},
+          fillColor={255,128,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-70,0},{-90,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,10},{60,10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,-10},{60,-10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{96,0},{60,0}},
+          color={0,0,0},
+          smooth=Smooth.None)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a cable for three-phase balanced AC systems. The model is based on
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortRLC\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortRLC</a>
+and provides functionalities to parametrize the values of <i>R</i>, <i>L</i> and <i>C</i> either
+using commercial cables or using default values.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Lines.Line\">
+AixLib.Electrical.AC.OnePhase.Lines.Line</a> for more
+information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Line;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Network.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Network.mo
new file mode 100644
index 0000000000..698ff6465b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/Network.mo
@@ -0,0 +1,66 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines;
+model Network "Three phases balanced AC network"
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialNetwork(
+    V_nominal(start = 480),
+    redeclare Interfaces.Terminal_p terminal,
+    redeclare replaceable Transmission.Grids.TestGrid2Nodes grid,
+    redeclare Lines.Line lines(
+    redeclare replaceable
+        AixLib.Electrical.Transmission.LowVoltageCables.Generic commercialCable=grid.cables));
+  Modelica.Units.SI.Voltage VAbs[grid.nNodes] "RMS voltage of the grid nodes";
+equation
+  for i in 1:grid.nLinks loop
+    connect(lines[i].terminal_p, terminal[grid.fromTo[i,1]]);
+    connect(lines[i].terminal_n, terminal[grid.fromTo[i,2]]);
+  end for;
+
+  for i in 1:grid.nNodes loop
+    VAbs[i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal[i].v);
+  end for;
+
+  annotation (
+    defaultComponentName="net",
+    Icon(graphics={             Line(
+          points={{-98,-60},{-78,-20},{-58,-60},{-38,-100},{-18,-60}},
+          color={0,0,0},
+          smooth=Smooth.Bezier),          Line(
+          points={{-88,-60},{-68,-20},{-48,-60},{-28,-100},{-8,-60}},
+          color={120,120,120},
+          smooth=Smooth.Bezier),          Line(
+          points={{-78,-60},{-58,-20},{-38,-60},{-18,-100},{2,-60}},
+          color={215,215,215},
+          smooth=Smooth.Bezier)}), Documentation(revisions="<html>
+<ul>
+<li>
+March 30, 2015, by Michael Wetter:<br/>
+Made <code>grid</code> replaceable. This error was caught by
+the regression tests of OpenModelica.
+</li>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Maintained replaceable the parameter <code>commercialCable</code> when redeclaring
+the type of line.
+</li>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a generalized electrical AC three-phase balanced network.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.BaseClasses.PartialNetwork\">
+AixLib.Electrical.Transmission.BaseClasses.PartialNetwork</a>
+for information about the network model.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.Grids.PartialGrid\">
+AixLib.Electrical.Transmission.Grids.PartialGrid</a>
+for more information about the topology of the network, such as
+the number of nodes, how they are connected, and the length of each connection.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Network;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortInductance.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortInductance.mo
new file mode 100644
index 0000000000..1507d6f7b7
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortInductance.mo
@@ -0,0 +1,29 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines;
+model TwoPortInductance "Model of an inductance with two electrical ports"
+  extends AixLib.Electrical.AC.OnePhase.Lines.TwoPortInductance(
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  annotation (
+    defaultComponentName="lineL",
+    Documentation(revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Inductance that connects two AC three-phase
+balanced interfaces. This model can be used to represent a
+cable in a three-phase balanced AC system.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Lines.TwoPortInductance\">
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortInductance</a> for more
+information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortInductance;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortRL.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortRL.mo
new file mode 100644
index 0000000000..b9f8803d32
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortRL.mo
@@ -0,0 +1,30 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines;
+model TwoPortRL
+  "Model of a resistive-inductive element with two electrical ports"
+  extends AixLib.Electrical.AC.OnePhase.Lines.TwoPortRL(
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  annotation (
+    defaultComponentName="lineRL",
+    Documentation(revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Resistive-inductive impedance that connects two AC three-phase
+balanced interfaces. This model can be used to represent a
+cable in a three-phase balanced AC system.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Lines.TwoPortRL\">
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortRL</a> for more
+information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRL;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortRLC.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortRLC.mo
new file mode 100644
index 0000000000..2e7ab06f31
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortRLC.mo
@@ -0,0 +1,29 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines;
+model TwoPortRLC "Model of a RLC element with two electrical ports"
+  extends AixLib.Electrical.AC.OnePhase.Lines.TwoPortRLC(
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  annotation (
+    defaultComponentName="lineRLC",
+    Documentation(revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+RLC impedance that connects two AC three-phase
+balanced interfaces. This model can be used to represent a
+cable in a three-phase balanced AC system.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Lines.TwoPortRLC\">
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortRLC</a> for more
+information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRLC;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortResistance.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortResistance.mo
new file mode 100644
index 0000000000..7fe9d21d69
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/TwoPortResistance.mo
@@ -0,0 +1,29 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Lines;
+model TwoPortResistance "Model of a resistance with two electrical ports"
+  extends AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance(
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  annotation (
+    defaultComponentName="lineR",
+    Documentation(revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Resistance that connects two AC three-phase
+balanced interfaces. This model can be used to represent a
+cable in a three-phase balanced AC system.
+</p>
+<p>
+See model
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance\">
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance</a> for more
+information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortResistance;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/package.mo
new file mode 100644
index 0000000000..e2ca932690
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/package.mo
@@ -0,0 +1,35 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced;
+package Lines "Package with line models for three-phase balanced AC systems"
+  extends Modelica.Icons.Package;
+
+
+  annotation (Icon(graphics={
+      Ellipse(
+        extent={{44,6},{20,-30}},
+        lineColor={0,0,0},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),
+      Line(
+        points={{32,6},{-50,6},{-60,6},{-68,-12},{-60,-30},{-48,-30},{32,-30}},
+        color={0,0,0},
+        smooth=Smooth.Bezier),
+      Line(
+        points={{-66,-12},{-84,-12}},
+        color={0,0,0},
+        smooth=Smooth.None),
+      Line(
+        points={{58,-12},{32,-12}},
+        color={0,0,0},
+        smooth=Smooth.None)}), Documentation(info="<html>
+<p>
+This package contains models for transmission lines and electrical networks.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Lines;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/package.order
new file mode 100644
index 0000000000..c13075e17a
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Lines/package.order
@@ -0,0 +1,7 @@
+Line
+Network
+TwoPortInductance
+TwoPortRL
+TwoPortRLC
+TwoPortResistance
+Examples
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Capacitive.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Capacitive.mo
new file mode 100644
index 0000000000..3db7fec377
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Capacitive.mo
@@ -0,0 +1,130 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Loads;
+model Capacitive "Model of a capacitive and resistive load"
+  extends AixLib.Electrical.AC.OnePhase.Loads.Capacitive(
+    redeclare Interfaces.Terminal_n terminal,
+    V_nominal(start=480));
+  annotation (
+  defaultComponentName="loa",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+            -100},{100,100}}),      graphics={
+        Rectangle(
+          extent={{-80,80},{80,-80}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Line(points={{-2,-2.44921e-16},{10,0}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Text(
+          extent={{-120,120},{120,80}},
+          textColor={0,0,0},
+          textString="%name"),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,1},
+          rotation=90),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{44,5.38825e-15}},
+                                         color={0,0,0},
+          origin={60,50},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,51},
+          rotation=90),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,-51},
+          rotation=90),
+        Line(
+          points={{60,50},{76,0},{60,-52}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,-52},
+          rotation=180),
+        Line(
+          points={{10,68},{10,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{16,68},{16,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{60,7.34764e-15}},
+                                         color={0,0,0},
+          origin={76,0},
+          rotation=180),
+        Line(
+          points={{16,18},{16,-18}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{10,18},{10,-18}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{44,5.38825e-15}},
+                                         color={0,0,0},
+          origin={60,-52},
+          rotation=180),
+        Line(
+          points={{16,-34},{16,-70}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{10,-34},{10,-70}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,-52},
+          rotation=180)}),       Documentation(info="<html>
+<p>
+Model of a capacitive load. See
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Capacitive\">
+AixLib.Electrical.AC.OnePhase.Loads.Capacitive</a> for more information.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Capacitive;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/Impedances.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/Impedances.mo
new file mode 100644
index 0000000000..fd909331b8
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/Impedances.mo
@@ -0,0 +1,69 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Examples;
+model Impedances "Example that illustrates the use of the impedance models"
+   extends Modelica.Icons.Example;
+  Sources.FixedVoltage sou(f=60, V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+  Impedance Z1(R=0,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60),
+    star=true) "Impedance purely inductive"
+    annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+  Impedance Z2(R=1, star=true) "Impedance purely resistive"
+    annotation (Placement(transformation(extent={{-20,10},{0,30}})));
+  Impedance Z3(R=0,
+    inductive=false,
+    C=1/(2*Modelica.Constants.pi*60),
+    star=true) "Impedance purely capacitive"
+    annotation (Placement(transformation(extent={{-20,-20},{0,0}})));
+  Impedance Z4(
+    inductive=false,
+    R=1,
+    C=1/(2*Modelica.Constants.pi*60),
+    star=true) "Impedance capacitive"
+    annotation (Placement(transformation(extent={{-20,-50},{0,-30}})));
+  Impedance Z5(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60),
+    star=true) "Impedance inductive"
+    annotation (Placement(transformation(extent={{-20,-78},{0,-58}})));
+equation
+  connect(sou.terminal, Z1.terminal) annotation (Line(
+      points={{-60,-10},{-40,-10},{-40,50},{-20,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, Z2.terminal) annotation (Line(
+      points={{-60,-10},{-40,-10},{-40,20},{-20,20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, Z3.terminal) annotation (Line(
+      points={{-60,-10},{-20,-10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, Z4.terminal) annotation (Line(
+      points={{-60,-10},{-40,-10},{-40,-40},{-20,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, Z5.terminal) annotation (Line(
+      points={{-60,-10},{-40,-10},{-40,-68},{-20,-68}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+September 22, 2014 by Marco Bonvini:<br/>
+Added documentation and revised the example.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model illustrates the use of the impedance models.
+The impedances have unitary values such that the RMS value of the voltage and of the current are the same.
+</p>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=1.0),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/Impedances.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedances;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ParallelLoads.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ParallelLoads.mo
new file mode 100644
index 0000000000..762d42fbdf
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ParallelLoads.mo
@@ -0,0 +1,99 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Examples;
+model ParallelLoads "Example that illustrates the use of the load models"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage E(f=60, V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+  Resistive R(P_nominal=-2000, V_nominal=480) "Resistive load"
+    annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+  Inductive RL_pf(
+    pf=0.8,
+    P_nominal=-2000,
+    use_pf_in=true,
+    V_nominal=480) "Inductive load with variable power factor"
+    annotation (Placement(transformation(extent={{-20,-10},{0,10}})));
+  Modelica.Blocks.Sources.Ramp load(              startTime=0.2, duration=0.3)
+    "Power signal profile"
+    annotation (Placement(transformation(extent={{60,-50},{40,-30}})));
+  Inductive varRL_y(                                   P_nominal=-2000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.Load.VariableZ_y_input)
+    "Inductive load with y as input"
+    annotation (Placement(transformation(extent={{-20,-36},{0,-16}})));
+  Capacitive varRC_y(                                   P_nominal=-2000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.Load.VariableZ_y_input)
+    "Capacitive load with y as input"
+    annotation (Placement(transformation(extent={{-20,-60},{0,-40}})));
+  Inductive varRL_P(pf=0.8,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input)
+    "Inductive load with P as input"
+    annotation (Placement(transformation(extent={{-20,14},{0,34}})));
+  Modelica.Blocks.Sources.Ramp pow(
+    startTime=0.2,
+    duration=0.3,
+    height=4000,
+    offset=-2000) "Power consumption profile"
+    annotation (Placement(transformation(extent={{60,14},{40,34}})));
+  Modelica.Blocks.Sources.Ramp pf(
+    height=0.2,
+    duration=0.2,
+    offset=0.8,
+    startTime=0.7) "Power factor profile"
+    annotation (Placement(transformation(extent={{60,-20},{40,0}})));
+equation
+  connect(E.terminal, R.terminal) annotation (Line(
+      points={{-60,4.44089e-16},{-40,4.44089e-16},{-40,50},{-20,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RL_pf.terminal) annotation (Line(
+      points={{-60,4.44089e-16},{-40,4.44089e-16},{-40,0},{-20,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, varRL_y.terminal) annotation (Line(
+      points={{-60,4.44089e-16},{-40,4.44089e-16},{-40,-26},{-20,-26}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, varRC_y.terminal) annotation (Line(
+      points={{-60,4.44089e-16},{-40,4.44089e-16},{-40,-50},{-20,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load.y, varRL_y.y) annotation (Line(
+      points={{39,-40},{20,-40},{20,-26},{4.44089e-16,-26}},
+      color={0,0,127},
+      smooth=Smooth.None));
+
+  connect(load.y, varRC_y.y) annotation (Line(
+      points={{39,-40},{20,-40},{20,-50},{4.44089e-16,-50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, varRL_P.terminal) annotation (Line(
+      points={{-60,4.44089e-16},{-40,4.44089e-16},{-40,24},{-20,24}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(pow.y, varRL_P.Pow) annotation (Line(
+      points={{39,24},{4.44089e-16,24}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf.y, RL_pf.pf_in) annotation (Line(
+      points={{39,-10},{30,-10},{30,6},{4.44089e-16,6}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (    Documentation(revisions="<html>
+<ul>
+<li>
+September 22, 2014 by Marco Bonvini:<br/>
+Added documentation and revised the example.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model illustrates the use of the three-phase unbalanced load models.
+</p>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=1.0),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ParallelLoads.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ParallelLoads;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ThreePhases.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ThreePhases.mo
new file mode 100644
index 0000000000..53ad6af3d2
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ThreePhases.mo
@@ -0,0 +1,209 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Examples;
+model ThreePhases
+  "Example that provides a comparison between AC one phase and three-phase balanced"
+  extends Modelica.Icons.Example;
+  Modelica.Units.SI.Power errorY=sqrt((sen_Y.S[1] - (sen_a.S[1] + sen_b.S[1] +
+      sen_c.S[1]))^2 + (sen_Y.S[2] - (sen_a.S[2] + sen_b.S[2] + sen_c.S[2]))^2)
+    "Difference of the power consumption in the star (Y) connection";
+  Modelica.Units.SI.Power errorD=sqrt((sen_D.S[1] - (sen_ab.S[1] + sen_bc.S[1]
+       + sen_ca.S[1]))^2 + (sen_D.S[2] - (sen_ab.S[2] + sen_bc.S[2] + sen_ca.S[
+      2]))^2)
+    "Difference of the power consumption in the triangle (D) connection";
+  Sources.FixedVoltage sou(definiteReference=true,
+    f=60,
+    V=480) "Three phases balanced voltage source"
+    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
+  Impedance RL_star(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60)) "Impedance with Y connection"
+    annotation (Placement(transformation(extent={{40,50},{60,70}})));
+  OnePhase.Sources.FixedVoltage sou_a(V=480/sqrt(3), definiteReference=true,
+    f=60) "Voltage source phase a"
+    annotation (Placement(transformation(extent={{-90,-30},{-70,-10}})));
+  OnePhase.Sources.FixedVoltage sou_b(
+    V=480/sqrt(3),
+    definiteReference=true,
+    phiSou=2.0943951023932,
+    f=60) "Voltage source phase b"
+    annotation (Placement(transformation(extent={{-90,-60},{-70,-40}})));
+  OnePhase.Sources.FixedVoltage sou_c(
+    V=480/sqrt(3),
+    definiteReference=true,
+    phiSou=-2.0943951023932,
+    f=60) "Voltage source phase c"
+    annotation (Placement(transformation(extent={{-90,-90},{-70,-70}})));
+  OnePhase.Loads.Impedance RL_a(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60)) "Impedance on phase A"
+    annotation (Placement(transformation(extent={{-40,-30},{-20,-10}})));
+  OnePhase.Loads.Impedance RL_b(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60)) "Impedance on phase B"
+    annotation (Placement(transformation(extent={{-40,-60},{-20,-40}})));
+  OnePhase.Loads.Impedance RL_c(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60)) "Impedance on phase C"
+    annotation (Placement(transformation(extent={{-40,-90},{-20,-70}})));
+  Impedance RL_tri(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60),
+    star=false) "Impedance with D connection"
+    annotation (Placement(transformation(extent={{40,20},{60,40}})));
+  OnePhase.Sources.FixedVoltage sou_ab(
+    V=480,
+    phiSou=-0.5235987755983,
+    definiteReference=true,
+    f=60) "Voltage source line ab"
+    annotation (Placement(transformation(extent={{10,-30},{30,-10}})));
+  OnePhase.Sources.FixedVoltage sou_bc(
+    phiSou=1.5707963267949,
+    V=480,
+    definiteReference=true,
+    f=60) "Voltage source line bc"
+    annotation (Placement(transformation(extent={{10,-60},{30,-40}})));
+  OnePhase.Sources.FixedVoltage sou_ca(
+    phiSou=-3.6651914291881,
+    V=480,
+    definiteReference=true,
+    f=60) "Voltage source line ca"
+    annotation (Placement(transformation(extent={{10,-90},{30,-70}})));
+  OnePhase.Loads.Impedance RL_ab(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60)) "Impedance on line AB"
+    annotation (Placement(transformation(extent={{60,-30},{80,-10}})));
+  OnePhase.Loads.Impedance RL_bc(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60)) "Impedance on line BC"
+    annotation (Placement(transformation(extent={{60,-60},{80,-40}})));
+  OnePhase.Loads.Impedance RL_c1(
+    R=1,
+    inductive=true,
+    L=1/(2*Modelica.Constants.pi*60)) "Impedance on linease CA"
+    annotation (Placement(transformation(extent={{60,-90},{80,-70}})));
+  OnePhase.Sensors.GeneralizedSensor sen_a
+    "Sensor located on phase A (Y connection)"
+    annotation (Placement(transformation(extent={{-66,-30},{-46,-10}})));
+  OnePhase.Sensors.GeneralizedSensor sen_ab
+    "Sensor located on line AB (D connection)"
+    annotation (Placement(transformation(extent={{34,-30},{54,-10}})));
+  Sensors.GeneralizedSensor sen_Y "Sensor for Y connection (balanced case)"
+    annotation (Placement(transformation(extent={{12,50},{32,70}})));
+  Sensors.GeneralizedSensor sen_D "Sensor for D connection (balanced case)"
+    annotation (Placement(transformation(extent={{12,20},{32,40}})));
+  OnePhase.Sensors.GeneralizedSensor sen_b
+    "Sensor located on phase B (Y connection)"
+    annotation (Placement(transformation(extent={{-66,-60},{-46,-40}})));
+  OnePhase.Sensors.GeneralizedSensor sen_c
+    "Sensor located on phase C (Y connection)"
+    annotation (Placement(transformation(extent={{-66,-90},{-46,-70}})));
+  OnePhase.Sensors.GeneralizedSensor sen_bc
+    "Sensor located on line BC (D connection)"
+    annotation (Placement(transformation(extent={{34,-60},{54,-40}})));
+  OnePhase.Sensors.GeneralizedSensor sen_ca
+    "Sensor located on line CA (D connection)"
+    annotation (Placement(transformation(extent={{34,-90},{54,-70}})));
+equation
+  connect(sou_a.terminal, sen_a.terminal_n) annotation (Line(
+      points={{-70,-20},{-66,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen_a.terminal_p, RL_a.terminal) annotation (Line(
+      points={{-46,-20},{-40,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou_ab.terminal, sen_ab.terminal_n) annotation (Line(
+      points={{30,-20},{34,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen_ab.terminal_p, RL_ab.terminal) annotation (Line(
+      points={{54,-20},{60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, sen_Y.terminal_n) annotation (Line(
+      points={{-40,60},{12,60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen_Y.terminal_p, RL_star.terminal) annotation (Line(
+      points={{32,60},{40,60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, sen_D.terminal_n) annotation (Line(
+      points={{-40,60},{0,60},{0,30},{12,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen_D.terminal_p, RL_tri.terminal) annotation (Line(
+      points={{32,30},{40,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou_b.terminal, sen_b.terminal_n) annotation (Line(
+      points={{-70,-50},{-66,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen_b.terminal_p, RL_b.terminal) annotation (Line(
+      points={{-46,-50},{-40,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou_c.terminal, sen_c.terminal_n) annotation (Line(
+      points={{-70,-80},{-66,-80}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen_c.terminal_p, RL_c.terminal) annotation (Line(
+      points={{-46,-80},{-40,-80}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou_bc.terminal, sen_bc.terminal_n) annotation (Line(
+      points={{30,-50},{34,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen_bc.terminal_p, RL_bc.terminal) annotation (Line(
+      points={{54,-50},{60,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou_ca.terminal, sen_ca.terminal_n) annotation (Line(
+      points={{30,-80},{34,-80}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen_ca.terminal_p, RL_c1.terminal) annotation (Line(
+      points={{54,-80},{60,-80}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+            -100},{100,100}}),        graphics={
+        Text(
+          extent={{-60,100},{60,80}},
+          textColor={0,0,0},
+          textString="Three phases, balanced (Y and D connection) "),
+        Text(
+          extent={{-100,10},{-4,-10}},
+          textColor={0,0,0},
+          textString="Three phases, balanced (Y connection) "),
+        Text(
+          extent={{4,10},{100,-10}},
+          textColor={0,0,0},
+          textString="Three phases, balanced (D connection) ")}), Documentation(
+        revisions="<html>
+<ul>
+<li>
+September 22, 2014 by Marco Bonvini:<br/>
+Added documentation and revised the example.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model illustrates the use of the impedance models and how the three-phase balanced model
+can reproduce the same results obtained using three separate one phase circuits.
+</p>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=1.0),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ThreePhases.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ThreePhases;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/package.mo
new file mode 100644
index 0000000000..881a942329
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Loads;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Loads\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Loads</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/package.order
new file mode 100644
index 0000000000..3d9b976ee0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Examples/package.order
@@ -0,0 +1,3 @@
+Impedances
+ParallelLoads
+ThreePhases
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Impedance.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Impedance.mo
new file mode 100644
index 0000000000..077be5ac5f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Impedance.mo
@@ -0,0 +1,162 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Loads;
+model Impedance "Model of a resistive load"
+  extends AixLib.Electrical.Interfaces.Impedance(
+    redeclare package PhaseSystem = PhaseSystems.OnePhase,
+    redeclare Interfaces.Terminal_n terminal);
+
+  parameter Boolean star = true
+    "Type of load connection: true = star, false = triangle" annotation(Evaluate=true, choices(
+      choice=true "Star",
+      choice=false "Triangle",
+      __Dymola_radioButtons=true));
+
+protected
+  Modelica.Units.SI.Angle theRef "Absolute angle of rotating reference system";
+  Modelica.Units.SI.AngularVelocity omega
+    "Frequency of the quasi-stationary sine waves";
+  Modelica.Units.SI.Reactance X(start=1) "Complex component of the impedance";
+
+equation
+  theRef = PhaseSystem.thetaRef(terminal.theta);
+  omega = der(theRef);
+
+  // Inductance of each line
+  if inductive then
+    X = omega*L_internal;
+  else
+    X = -1/(omega*C_internal);
+  end if;
+
+  // Ohm's law
+  if star then
+    terminal.v = {{R_internal,-X}*terminal.i, {X,R_internal}*terminal.i};
+  else
+    terminal.v = {{R_internal/3,-X/3}*terminal.i, {X/3,R_internal/3}*terminal.i};
+  end if;
+  annotation (
+  defaultComponentName="loa",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+          Rectangle(
+            extent={{-80,80},{80,-80}},
+            lineColor={0,0,0},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+          origin={7.10543e-15,7.10543e-15},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{12,1.46953e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+        Text(
+          extent={{-120,-80},{120,-120}},
+          textColor={0,0,0},
+          textString="%name"),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={2,49},
+          rotation=90),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={2,1},
+          rotation=90),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={2,-49},
+          rotation=90),
+        Line(
+          visible=star == true,
+          points={{52,50},{68,0},{52,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(visible = star == true,
+          points={{68,0},{52,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-68,50},{-28,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-68,0},{-28,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-68,-50},{-28,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{32,50},{52,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{32,0},{52,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{32,-50},{52,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(visible = star == false,
+          points={{52,50},{52,36},{-50,14},{-50,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(visible = star == false,
+          points={{52,0},{52,-14},{-50,-36},{-50,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(visible = star == false,
+          points={{52,-50},{72,-50},{72,68},{-50,68},{-50,50}},
+          color={0,0,0},
+          smooth=Smooth.None)}),
+          Documentation(info="<html>
+<p>
+Model of a three-phase balanced impedance.
+</p>
+<p>
+If <code>inductive=true</code>, then the
+inductance is a parameter, otherwise
+the capacitance is a parameter.
+</p>
+<p>
+The boolean parameter <code>star</code> is used to
+select whether the star (Y) or triangle (D)
+configuration is used to connect the impedance.
+By default, the impedance is assumed to be connected
+with a star configuration.
+</p>
+<p>
+When the connection type changes from
+<code>star</code> to <code>triangle</code>, the value of the impedance
+is recomputed in such a way that the nominal power consumed by the impedance
+does not change.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 26, 2016, by Michael Wetter:<br/>
+Moved function call to <code>PhaseSystem.thetaRef</code> out of
+derivative operator as this is not yet supported by JModelica.
+</li>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedance;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Inductive.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Inductive.mo
new file mode 100644
index 0000000000..793465558e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Inductive.mo
@@ -0,0 +1,134 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Loads;
+model Inductive "Model of an inductive and resistive load"
+  extends AixLib.Electrical.AC.OnePhase.Loads.Inductive(
+    redeclare Interfaces.Terminal_n terminal,
+    V_nominal(start=480));
+  annotation (
+  defaultComponentName="loa",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+            -100},{100,100}}),
+                         graphics={
+        Rectangle(
+          extent={{-80,80},{80,-80}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+                                   Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+        Ellipse(extent={{-10,-10},{10,10}},
+          rotation=360),
+        Ellipse(extent={{30,-10},{50,10}}),
+        Ellipse(extent={{10,-10},{30,10}}),
+        Rectangle(
+          extent={{-10,0},{50,-12}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{26,3.18398e-15}},
+                                         color={0,0,0},
+          origin={76,0},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,1},
+          rotation=90),
+          Line(points={{-2,-2.44921e-16},{10,0}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Text(
+          extent={{-120,120},{120,80}},
+          textColor={0,0,0},
+          textString="%name"),
+        Ellipse(extent={{-10,-10},{10,10}},
+          origin={0,50},
+          rotation=360),
+        Ellipse(extent={{30,40},{50,60}}),
+        Ellipse(extent={{10,40},{30,60}}),
+        Rectangle(
+          extent={{-10,50},{50,38}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={60,50},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,51},
+          rotation=90),
+        Ellipse(extent={{-10,-10},{10,10}},
+          origin={0,-52},
+          rotation=360),
+        Ellipse(extent={{30,-62},{50,-42}}),
+        Ellipse(extent={{10,-62},{30,-42}}),
+        Rectangle(
+          extent={{-10,-52},{50,-64}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,-52},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={60,-52},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,-51},
+          rotation=90),
+        Line(
+          points={{60,50},{76,0},{60,-52}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,-52},
+          rotation=180)}),    Documentation(info="<html>
+<p>
+Model of an inductive load. See
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Inductive\">
+AixLib.Electrical.AC.OnePhase.Loads.Inductive</a> for more information.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Inductive;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Resistive.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Resistive.mo
new file mode 100644
index 0000000000..2014ec2abe
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/Resistive.mo
@@ -0,0 +1,94 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Loads;
+model Resistive "Model of a resistive load"
+  extends AixLib.Electrical.AC.OnePhase.Loads.Resistive(
+    redeclare Interfaces.Terminal_n terminal,
+    V_nominal(start=480));
+  annotation (
+  defaultComponentName="loa",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+          Rectangle(
+            extent={{-80,80},{80,-80}},
+            lineColor={0,0,0},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+          origin={7.10543e-15,7.10543e-15},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{12,1.46953e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+        Text(
+          extent={{-120,120},{120,80}},
+          textColor={0,0,0},
+          textString="%name"),
+        Line(
+          points={{-66,50},{-26,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,49},
+          rotation=90),
+        Line(
+          points={{34,50},{54,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{54,50},{70,0},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{34,0},{70,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,1},
+          rotation=90),
+        Line(
+          points={{-66,0},{-26,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-66,-50},{-26,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,-49},
+          rotation=90),
+        Line(
+          points={{34,-50},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None)}),
+          Documentation(info="<html>
+<p>
+Model of a resistive load. See
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Resistive\">
+AixLib.Electrical.AC.OnePhase.Loads.Resistive</a> for more information.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Resistive;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/package.mo
new file mode 100644
index 0000000000..ee07b6be0b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced;
+package Loads "Package with load models for three-phase balanced AC systems"
+  extends Modelica.Icons.VariantsPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models that represent different types of three
+phases balanced AC loads.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Loads;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/package.order
new file mode 100644
index 0000000000..865b97b429
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Loads/package.order
@@ -0,0 +1,5 @@
+Capacitive
+Impedance
+Inductive
+Resistive
+Examples
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/GeneralizedSensor.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/GeneralizedSensor.mo
new file mode 100644
index 0000000000..8dc0d19868
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/GeneralizedSensor.mo
@@ -0,0 +1,37 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sensors.Examples;
+model GeneralizedSensor "Example model for generalized sensor"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sensors.GeneralizedSensor
+    sen "Sensor model"
+    annotation (Placement(transformation(extent={{-20,2},{0,22}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Capacitive loa(
+                   V_nominal=480, P_nominal=-100) "Constant load"
+    annotation (Placement(transformation(extent={{40,2},{60,22}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage
+    sou(f=60, V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-60,2},{-40,22}})));
+equation
+  connect(sen.terminal_p, loa.terminal)
+    annotation (Line(points={{5.55112e-16,12},{40,12}}, smooth=Smooth.None));
+  connect(sen.terminal_n, sou.terminal)
+    annotation (Line(points={{-20,12},{-40,12}}, smooth=Smooth.None));
+  annotation (Documentation(
+  info="<html>
+<p>
+This example illustrates the use of the generalized sensor.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+July 24, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/GeneralizedSensor.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/Probe.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/Probe.mo
new file mode 100644
index 0000000000..295c9ba7fe
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/Probe.mo
@@ -0,0 +1,84 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sensors.Examples;
+model Probe "This example illustrates how to use the probe model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Capacitive loaRC(
+    mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    P_nominal=-10000,
+    V_nominal=480) "Constant load"
+    annotation (Placement(transformation(extent={{10,0},{30,20}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage sou(f=60, V=
+        480) "Voltage source"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortResistance res1(R=0.1)
+    "First line resistance"
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sensors.Probe probe_source(V_nominal=
+       480) "Probe that measures at the voltage source"
+    annotation (Placement(transformation(extent={{-50,30},{-30,50}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sensors.Probe probe_loadRC(V_nominal=
+       480) "Probe that measures at the RC load"
+    annotation (Placement(transformation(extent={{-10,30},{10,50}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortResistance res2(R=0.1)
+    "Second line resistance"
+    annotation (Placement(transformation(extent={{-26,-70},{-6,-50}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Inductive loaRL(
+    mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    P_nominal=-10000,
+    V_nominal=480) "Constant load"
+    annotation (Placement(transformation(extent={{10,-70},{30,-50}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sensors.Probe probe_loadRL(V_nominal=
+       480) "Probe that measures at the RL load"
+    annotation (Placement(transformation(extent={{-10,-28},{10,-8}})));
+equation
+  connect(sou.terminal, res1.terminal_n) annotation (Line(
+      points={{-40,-20},{-40,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(res1.terminal_p, loaRC.terminal) annotation (Line(
+      points={{-6,10},{10,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, probe_source.term) annotation (Line(
+      points={{-40,-20},{-40,31}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(loaRC.terminal, probe_loadRC.term) annotation (Line(
+      points={{10,10},{6.66134e-16,10},{6.66134e-16,31}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, res2.terminal_n) annotation (Line(
+      points={{-40,-20},{-40,-60},{-26,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(res2.terminal_p, loaRL.terminal) annotation (Line(
+      points={{-6,-60},{10,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(loaRL.terminal, probe_loadRL.term) annotation (Line(
+      points={{10,-60},{6.66134e-16,-60},{6.66134e-16,-27}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  Documentation(
+  info="<html>
+<p>
+This example illustrates the use of the probe model.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+August 5, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/Probe.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Probe;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/package.mo
new file mode 100644
index 0000000000..6522b91ca2
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sensors;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Sensors\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Sensors</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/package.order
new file mode 100644
index 0000000000..e4597e24c3
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/package.order
@@ -0,0 +1,2 @@
+GeneralizedSensor
+Probe
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/GeneralizedSensor.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/GeneralizedSensor.mo
new file mode 100644
index 0000000000..811d557599
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/GeneralizedSensor.mo
@@ -0,0 +1,92 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sensors;
+model GeneralizedSensor "Sensor for power, voltage and current"
+  extends AixLib.Electrical.Icons.GeneralizedSensor;
+  extends AixLib.Electrical.Interfaces.PartialTwoPort(
+    redeclare package PhaseSystem_p = PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n = PhaseSystems.OnePhase,
+    redeclare Interfaces.Terminal_n terminal_n(redeclare package PhaseSystem =
+          PhaseSystem_n),
+    redeclare Interfaces.Terminal_p terminal_p(redeclare package PhaseSystem =
+          PhaseSystem_p));
+  Modelica.Blocks.Interfaces.RealOutput V(
+    final quantity="ElectricPotential",
+    final unit="V")=
+      AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal_n.v)
+    "Voltage"
+      annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-50}),   iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-90})));
+  Modelica.Blocks.Interfaces.RealOutput I(
+    final quantity="ElectricCurrent",
+    final unit="A")=
+      AixLib.Electrical.PhaseSystems.OnePhase.systemCurrent(terminal_n.i)
+    "Current"
+      annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-50}), iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-90})));
+  Modelica.Blocks.Interfaces.RealOutput S[PhaseSystems.OnePhase.n](
+    each final quantity="Power",
+    each final unit="W")=
+      AixLib.Electrical.PhaseSystems.OnePhase.phasePowers_vi(v=terminal_n.v, i=terminal_n.i)
+    "Phase powers"
+      annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-60,-50}),iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-60,-90})));
+equation
+  connect(terminal_n, terminal_p) annotation (Line(
+      points={{-100,0},{2,0},{2,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (defaultComponentName="sen",
+  Documentation(info="<html>
+<p>
+Ideal sensor that measures power, voltage and current.
+The two components of the power <i>S</i> are the active and reactive power.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Michael Wetter:<br/>
+Moved assignments outside of equation section to avoid mixing
+textual and graphical modeling.
+</li>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Fixed bug. The model was referencing the wrong PhaseSystem.
+</li>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+July 24, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
+            100}}), graphics={
+        Text(
+          extent={{-120,-42},{0,-82}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="S")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Probe.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Probe.mo
new file mode 100644
index 0000000000..dfeae421ac
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/Probe.mo
@@ -0,0 +1,22 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sensors;
+model Probe "Model of a probe that measures RMS voltage and angle"
+  extends OnePhase.Sensors.Probe(
+  redeclare AixLib.Electrical.AC.ThreePhasesBalanced.Interfaces.Terminal_n term,
+  V_nominal(start=480));
+  annotation (
+  defaultComponentName="sen",
+  Documentation(info="<html>
+<p>
+This model represents a probe that measures the RMS voltage and the angle
+of the voltage phasor at a given point.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Probe;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/package.mo
new file mode 100644
index 0000000000..5de861e6cb
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced;
+package Sensors "Package with sensors models for three-phase balanced AC systems"
+extends Modelica.Icons.SensorsPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models for voltage, current and power sensors.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Sensors;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/package.order
new file mode 100644
index 0000000000..0fb45c82b3
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sensors/package.order
@@ -0,0 +1,3 @@
+GeneralizedSensor
+Probe
+Examples
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/FixedVoltageSource.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/FixedVoltageSource.mo
new file mode 100644
index 0000000000..c688331127
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/FixedVoltageSource.mo
@@ -0,0 +1,44 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sources.Examples;
+model FixedVoltageSource
+  "This example illustrates how using a fixed voltage source"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Inductive RL(
+      P_nominal=-300, mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    V_nominal=480) "Load model"
+    annotation (Placement(transformation(extent={{20,-10},{40,10}})));
+  ThreePhasesBalanced.Sources.FixedVoltage grid(
+    f=60,
+    V=480,
+    phiSou=0.34906585039887) "AC one phase electrical grid"
+    annotation (Placement(transformation(extent={{-40,-10},{-20,10}})));
+  ThreePhasesBalanced.Sensors.Probe sen(V_nominal=480)
+    "Probe that measures the voltage at the load"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+equation
+  connect(grid.terminal, RL.terminal)
+                                     annotation (Line(
+      points={{-20,4.44089e-16},{-20,0},{20,0},{20,5.55112e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(grid.terminal, sen.term) annotation (Line(
+      points={{-20,6.66134e-16},{0,6.66134e-16},{0,21},{4.44089e-16,21}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sources/Examples/FixedVoltageSource.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example shows how to use a fixed voltage generator model.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FixedVoltageSource;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/VariablePowerSource.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/VariablePowerSource.mo
new file mode 100644
index 0000000000..37469c0c6b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/VariablePowerSource.mo
@@ -0,0 +1,69 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sources.Examples;
+model VariablePowerSource
+  "This example illustrates how using a variable power source"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.Generator generator(f=60,
+      phiGen=0.26179938779915) "AC generator model"
+    annotation (Placement(transformation(extent={{-50,-10},{-30,10}})));
+  Modelica.Blocks.Sources.Sine generation(
+    offset=200,
+    startTime=1,
+    amplitude=100,
+    f=0.05) "Generated power"
+    annotation (Placement(transformation(extent={{-92,-10},{-72,10}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Inductive RL(mode=Types.Load.VariableZ_y_input,
+      P_nominal=-300,
+    V_nominal=480) "Load model"
+    annotation (Placement(transformation(extent={{20,-10},{40,10}})));
+  AixLib.Electrical.AC.ThreePhasesBalanced.Sources.Grid grid(f=60, V=480)
+    "AC one phase electrical grid"
+           annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+  Modelica.Blocks.Sources.Trapezoid load(
+    rising=2,
+    width=3,
+    falling=3,
+    period=10,
+    startTime=1,
+    amplitude=0.8,
+    offset=0.2) "Power consumption profile"
+    annotation (Placement(transformation(extent={{80,-10},{60,10}})));
+equation
+  connect(generation.y, generator.P) annotation (Line(
+      points={{-71,0},{-50,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(generator.terminal, RL.terminal)
+                                          annotation (Line(
+      points={{-30,0},{20,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(grid.terminal, RL.terminal)
+                                     annotation (Line(
+      points={{-10,40},{-10,0},{20,0},{20,5.55112e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load.y, RL.y)
+                       annotation (Line(
+      points={{59,0},{40,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (    experiment(StopTime=1.0, Tolerance=1e-6),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sources/Examples/VariablePowerSource.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 22, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example shows how to use a variable generator model. The generator model has to be used
+together with a voltage source generator, which is in this example the
+grid model.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end VariablePowerSource;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/package.mo
new file mode 100644
index 0000000000..1cd11799d7
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sources;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Sources\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Sources</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/package.order
new file mode 100644
index 0000000000..0da5691906
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Examples/package.order
@@ -0,0 +1,2 @@
+FixedVoltageSource
+VariablePowerSource
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/FixedVoltage.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/FixedVoltage.mo
new file mode 100644
index 0000000000..bba3b7f5f4
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/FixedVoltage.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sources;
+model FixedVoltage "Fixed three-phase balanced AC voltage source"
+  extends AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage(
+    redeclare Interfaces.Terminal_p terminal,
+    f(start=60),
+    V(start=480));
+  annotation (
+    defaultComponentName="fixVol",
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}),
+                   graphics={             Line(
+          points={{-34,0},{-14,40},{6,0},{26,-40},{46,0}},
+          color={120,120,120},
+          smooth=Smooth.Bezier),          Line(
+          points={{-24,0},{-4,40},{16,0},{36,-40},{56,0}},
+          color={215,215,215},
+          smooth=Smooth.Bezier)}),
+      Documentation(info="<html>
+<p>
+This is a constant voltage source, specifying the complex voltage
+by the RMS voltage and the phase shift.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FixedVoltage;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Generator.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Generator.mo
new file mode 100644
index 0000000000..4a865630ad
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Generator.mo
@@ -0,0 +1,30 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sources;
+model Generator "Model of a generator"
+  extends AixLib.Electrical.AC.OnePhase.Sources.Generator(
+    redeclare Interfaces.Terminal_p terminal,
+    f(start=60));
+  annotation (
+    defaultComponentName="gen",
+    Documentation(info="<html>
+<p>
+Model of an inductive generator.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.AC.OnePhase.Sources.Generator\">
+AixLib.Electrical.AC.OnePhase.Sources.Generator</a> for
+more information.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 4, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generator;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Grid.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Grid.mo
new file mode 100644
index 0000000000..78c0b16955
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/Grid.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced.Sources;
+model Grid "Electrical grid"
+  extends AixLib.Electrical.AC.OnePhase.Sources.Grid(
+    redeclare Interfaces.Terminal_p terminal,
+    f(start=60),
+    V(start=480),
+    redeclare AixLib.Electrical.AC.ThreePhasesBalanced.Sources.FixedVoltage sou);
+
+  annotation (
+  defaultComponentName="gri",
+    Documentation(info="<html>
+<p>
+Model that can be used to represent the electrical grid supply.
+See <a href=\"modelica://AixLib.Electrical.AC.OnePhase.Sources.Grid\">
+AixLib.Electrical.AC.OnePhase.Sources.Grid</a> for
+more information.
+</p>
+</html>",
+ revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+January 2, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Grid;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/package.mo
new file mode 100644
index 0000000000..daf22f53f9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.AC.ThreePhasesBalanced;
+package Sources "Package with source models for three-phase balanced AC systems"
+  extends Modelica.Icons.SourcesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models for three-phase balanced AC sources.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Revised User's guide.
+</li>
+</ul>
+</html>"));
+end Sources;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/package.order
new file mode 100644
index 0000000000..7398239cc6
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/Sources/package.order
@@ -0,0 +1,4 @@
+FixedVoltage
+Generator
+Grid
+Examples
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/package.mo b/AixLib/Electrical/AC/ThreePhasesBalanced/package.mo
new file mode 100644
index 0000000000..671a43560b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/package.mo
@@ -0,0 +1,26 @@
+within AixLib.Electrical.AC;
+package ThreePhasesBalanced "Three phases balanced AC systems"
+  extends Modelica.Icons.VariantsPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+Package with models for alternate current (AC) three phase balanced systems.<br/>
+Because the phases are balanced, the models in this
+package extend the models of the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase\">
+AixLib.Electrical.AC.OnePhase</a>.
+</p>
+<p>
+The models that are part of this package assume by default 480 V as nominal RMS phase
+to phase voltage. This default value can be changed.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end ThreePhasesBalanced;
diff --git a/AixLib/Electrical/AC/ThreePhasesBalanced/package.order b/AixLib/Electrical/AC/ThreePhasesBalanced/package.order
new file mode 100644
index 0000000000..1c45c7275c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesBalanced/package.order
@@ -0,0 +1,6 @@
+Conversion
+Lines
+Loads
+Sensors
+Sources
+Interfaces
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACConverter.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACConverter.mo
new file mode 100644
index 0000000000..6293f3bc30
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACConverter.mo
@@ -0,0 +1,126 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+model ACACConverter "AC AC converter single phase systems (YY)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY(
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter conv1(
+      conversionFactor=conversionFactor,
+      eta=eta,
+      ground_1=ground_1,
+      ground_2=ground_2),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter conv2(
+      conversionFactor=conversionFactor,
+      eta=eta,
+      ground_1=ground_1,
+      ground_2=ground_2),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter conv3(
+      conversionFactor=conversionFactor,
+      eta=eta,
+      ground_1=ground_1,
+      ground_2=ground_2));
+  parameter Real conversionFactor
+    "Ratio of QS rms voltage on side 2 / QS rms voltage on side 1";
+  parameter Modelica.Units.SI.Efficiency eta(max=1)
+    "Converter efficiency, pLoss = (1-eta) * Ptr";
+  parameter Boolean ground_1 = false "Connect side 1 of converter to ground" annotation(Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of converter to ground" annotation(Dialog(tab = "Ground", group="side 2"));
+
+  annotation (
+  defaultComponentName="conv",
+ Icon(graphics={
+        Line(
+          points={{2,60},{2,60},{82,60},{2,60},{82,-60},{2,-60},{2,60},{2,-60}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Line(
+          points={{-2,60},{-2,60},{-82,60},{-2,60},{-82,-60},{-2,-60},{-2,60},{
+              -2,-60}},
+          color={11,193,87},
+          smooth=Smooth.None),
+        Text(
+          extent={{-100,92},{100,60}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%conversionFactor"),
+        Text(
+          extent={{-132,78},{-72,38}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-88,52},{-28,12}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{32,52},{92,12}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,78},{130,38}},
+          textColor={0,120,120},
+          textString="2")}),
+    Documentation(info="<html>
+<p>
+This is an AC AC converter, based on a power balance between both circuit sides.
+The parameter <i>conversionFactor</i> defines the ratio between the RMS voltages
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+V<sub>2</sub> = conversionFactor * V<sub>1</sub>
+</p>
+
+<p>
+where <i>V<sub>1</sub></i> and <i>V<sub>2</sub></i> are the RMS voltages
+at the primary and secondary sides of the transformer (connector N and P
+respectively).
+</p>
+
+<p>
+The loss of the converter is proportional to the power transmitted.
+The parameter <code>eta</code> is the efficiency of the transfer.
+The loss is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+P<sub>loss</sub> = (1-&eta;) P<sub>tr</sub>
+</p>
+<p>
+where <i>P<sub>tr</sub></i> is the power transmitted. The model is bi-directional
+and the power can flow from both the primary to the secondary and vice-versa.
+Furthermore, reactive power on both side are set to 0.
+</p>
+
+<h4>Configuration:</h4>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/YY.png\"/>
+</p>
+
+<h4>Note:</h4>
+<p>
+This model reuses models from
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY</a> for
+details on the connections.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACConverter;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformer.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformer.mo
new file mode 100644
index 0000000000..28ad29b6c5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformer.mo
@@ -0,0 +1,227 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+model ACACTransformer "AC AC transformer simplified equivalent circuit (YY)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY(
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv1(
+      VHigh=VHigh/sqrt(3),
+      VLow=VLow/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      phi_1=0),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv2(
+      VHigh=VHigh/sqrt(3),
+      VLow=VLow/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      phi_1=-2.0943951023932),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv3(
+      VHigh=VHigh/sqrt(3),
+      VLow=VLow/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      phi_1=2.0943951023932));
+  parameter Modelica.Units.SI.Voltage VHigh
+    "Rms voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "Rms voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Real XoverR
+    "Ratio between the complex and real components of the impedance (XL/R)";
+  parameter Real Zperc "Short circuit impedance";
+  parameter Boolean ground_1 = false "Connect side 1 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 2"));
+equation
+
+  annotation (
+  defaultComponentName="tra",
+ Icon(graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-130,60},{-70,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,60},{130,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-72,40},{-66,40},{-64,44},{-60,36},{-56,44},{-52,36},{-48,44},
+              {-44,36},{-42,40},{-38,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-60,-7.34764e-15}},
+          color={0,127,127},
+          origin={-40,40},
+          rotation=180),
+        Ellipse(
+          extent={{-30,46},{-18,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-18,46},{-6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,46},{6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-30,40},{6,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,40},{20,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{14,20},{26,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,8},{26,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,-4},{26,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{10,20},{20,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,-16},{20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{20,-40},{-70,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{34,40},{34,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{40,20},{28,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,8},{28,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,-4},{28,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{44,20},{34,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{34,-16},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,-40},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,40},{34,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-64,60},{-48,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-20,60},{-4,48}},
+          textColor={0,120,120},
+          textString="L")}),
+    Documentation(info="<html>
+<p>
+This is a simplified equivalent transformer model.
+The model accounts for winding Joule losses and leakage reactances
+that are represented by a series of a resistance <i>R</i> and an
+inductance <i>L</i>. The resistance and the inductance represent both the
+effects of the secondary and primary side of the transformer.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>Vhigh</code> - RMS voltage at primary side,</li>
+<li><code>Vlow</code> - RMS voltage at secondary side,</li>
+<li><code>VAbase</code> - apparent nominal power of the transformer,</li>
+<li><code>XoverR</code> - ratio between reactance and resistance, and</li>
+<li><code>Zperc</code> - the short circuit impedance.</li>
+</ul>
+<p>
+Given the nominal conditions, the model computes the values of the resistance and inductance.
+</p>
+<h4>Configuration:</h4>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/YY.png\"/>
+</p>
+<h4>Note:</h4>
+<p>
+This model reuses models from
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY</a> for
+details on the connections.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformer;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerDD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerDD.mo
new file mode 100644
index 0000000000..733234a75d
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerDD.mo
@@ -0,0 +1,237 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+model ACACTransformerDD "AC AC transformer simplified equivalent circuit (DD)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterDD(
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv1(
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VHigh=VHigh,
+      VLow=VLow,
+      phi_1=0.5235987755983),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv2(
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VHigh=VHigh,
+      VLow=VLow,
+      phi_1=-1.5707963267949),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv3(
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VHigh=VHigh,
+      VLow=VLow,
+      phi_1=2.6179938779915));
+  parameter Modelica.Units.SI.Voltage VHigh
+    "Rms voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "Rms voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Real XoverR
+    "Ratio between the complex and real components of the impedance (XL/R)";
+  parameter Real Zperc "Short circuit impedance";
+  parameter Boolean ground_1 = false "Connect side 1 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 2"));
+equation
+
+  annotation (
+  defaultComponentName="tra",
+ Icon(graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-130,60},{-70,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,60},{130,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-72,40},{-66,40},{-64,44},{-60,36},{-56,44},{-52,36},{-48,44},
+              {-44,36},{-42,40},{-38,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-60,-7.34764e-15}},
+          color={0,127,127},
+          origin={-40,40},
+          rotation=180),
+        Ellipse(
+          extent={{-30,46},{-18,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-18,46},{-6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,46},{6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-30,40},{6,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,40},{20,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{14,20},{26,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,8},{26,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,-4},{26,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{10,20},{20,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,-16},{20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{20,-40},{-70,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{34,40},{34,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{40,20},{28,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,8},{28,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,-4},{28,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{44,20},{34,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{34,-16},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,-40},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,40},{34,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-64,60},{-48,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-20,60},{-4,48}},
+          textColor={0,120,120},
+          textString="L"),
+        Line(
+          points={{-50,-8},{-30,22},{-10,-8},{-50,-8}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{40,-8},{60,22},{80,-8},{40,-8}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5)}),
+    Documentation(info="<html>
+<p>
+This is a simplified equivalent transformer model with Delta-Delta connection.
+The model accounts for winding Joule losses and leakage reactances
+that are represented by a series of a resistance <i>R</i> and an
+inductance <i>L</i>. The resistance and the inductance represent the
+effects of the secondary and primary side of the transformer.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>Vhigh</code> - RMS voltage at primary side,</li>
+<li><code>Vlow</code> - RMS voltage at secondary side,</li>
+<li><code>VAbase</code> - apparent nominal power of the transformer,</li>
+<li><code>XoverR</code> - ratio between reactance and resistance, and</li>
+<li><code>Zperc</code> - the short circuit impedance.</li>
+</ul>
+<p>
+Given the nominal conditions, the model computes the values of the resistance and inductance.
+</p>
+<h4>Configuration:</h4>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/DD.png\"/>
+</p>
+<h4>Note:</h4>
+<p>
+This model reuses models from
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterDD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterDD</a> for
+details on the connections.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerDD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerFull.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerFull.mo
new file mode 100644
index 0000000000..2d2de67418
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerFull.mo
@@ -0,0 +1,253 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+model ACACTransformerFull "AC AC transformer detailed equivalent circuit (YY)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY(
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull conv1(
+      VHigh=VHigh/sqrt(3),
+      VLow=VLow/sqrt(3),
+      f = f,
+      VABase=VABase,
+      R1=R1,L1=L1,R2=R2,L2=L2,
+      magEffects=magEffects,
+      Rm=Rm,Lm=Lm,
+      ground_1=ground_1,
+      ground_2=ground_2),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull conv2(
+      VHigh=VHigh/sqrt(3),
+      VLow=VLow/sqrt(3),
+      f = f,
+      VABase=VABase,
+      R1=R1,L1=L1,R2=R2,L2=L2,
+      magEffects=magEffects,
+      Rm=Rm,Lm=Lm,
+      ground_1=ground_1,
+      ground_2=ground_2),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull conv3(
+      VHigh=VHigh/sqrt(3),
+      VLow=VLow/sqrt(3),
+      f = f,
+      VABase=VABase,
+      R1=R1,L1=L1,R2=R2,L2=L2,
+      magEffects=magEffects,
+      Rm=Rm,Lm=Lm,
+      ground_1=ground_1,
+      ground_2=ground_2));
+
+  parameter Modelica.Units.SI.Voltage VHigh
+    "Rms voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "Rms voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Modelica.Units.SI.Frequency f(start=60) "Nominal frequency";
+  parameter AixLib.Electrical.Types.PerUnit R1(min=0)
+    "Resistance on side 1 of the transformer (pu)";
+  parameter AixLib.Electrical.Types.PerUnit L1(min=0)
+    "Inductance on side 1 of the transformer (pu)";
+  parameter AixLib.Electrical.Types.PerUnit R2(min=0)
+    "Resistance on side 2 of the transformer (pu)";
+  parameter AixLib.Electrical.Types.PerUnit L2(min=0)
+    "Inductance on side 2 of the transformer (pu)";
+  parameter Boolean magEffects = false
+    "If =true introduce magnetization effects"
+    annotation(Dialog(group="Magnetization"));
+  parameter AixLib.Electrical.Types.PerUnit Rm(min=0,start=0)
+    "Magnetization resistance (pu)" annotation(Dialog(group="Magnetization", enable = magEffects));
+  parameter AixLib.Electrical.Types.PerUnit Lm(min=0,start=0)
+    "Magnetization inductance (pu)" annotation(Dialog(group="Magnetization", enable = magEffects));
+  parameter Boolean ground_1 = false "Connect side 1 of converter to ground" annotation(Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of converter to ground" annotation(Dialog(tab = "Ground", group="side 2"));
+
+  annotation (
+  defaultComponentName="tra",
+ Icon(graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-130,60},{-70,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,60},{130,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-72,40},{-66,40},{-64,44},{-60,36},{-56,44},{-52,36},{-48,44},
+              {-44,36},{-42,40},{-38,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-60,-7.34764e-15}},
+          color={0,127,127},
+          origin={-40,40},
+          rotation=180),
+        Ellipse(
+          extent={{-30,46},{-18,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-18,46},{-6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,46},{6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-30,40},{6,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,40},{20,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{14,20},{26,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,8},{26,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,-4},{26,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{10,20},{20,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,-16},{20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{20,-40},{-70,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{34,40},{34,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{40,20},{28,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,8},{28,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,-4},{28,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{44,20},{34,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{34,-16},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,-40},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,40},{34,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-64,60},{-48,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-20,60},{-4,48}},
+          textColor={0,120,120},
+          textString="L")}),
+    Documentation(info="<html>
+<p>
+This is a detailed transformer model that takes into accounts the winding Joule losses,
+and the leakage reactances on the primary and secondary side. The model also takes into account
+the core or iron losses and the losses due to magnetization effects.
+</p>
+<p>
+The losses are represented by a series of resistances <i>R<sub>1</sub></i>, <i>R<sub>2</sub></i>,
+<i>R<sub>m</sub></i> and inductances <i>L<sub>1</sub></i>, <i>L<sub>2</sub></i>, and
+<i>L<sub>m</sub></i>.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>Vhigh</code> - RMS voltage at primary side,</li>
+<li><code>Vlow</code> - RMS voltage at secondary side,</li>
+<li><code>VAbase</code> - apparent nominal power of the transformer,</li>
+<li><code>f</code> - frequency,</li>
+<li><code>R_1, L_1</code> - resistance and inductance at primary side (per unit),</li>
+<li><code>R_2, L_2</code> - resistance and inductance at secondary side (per unit), and</li>
+<li><code>R_m, L_m</code> - resistance and inductance for magnetization effects (per unit).</li>
+</ul>
+<p>
+Given the nominal conditions, the model computes the values of the nominal impedances
+at the primary and secondary side. Given these values, the per unit values are transformed into
+the actual values of the resistances and inductancs.
+</p>
+<p>
+The magnetization losses can be enabled or disabled using the boolean flag <code>magEffects</code>.
+</p>
+<h4>Configuration:</h4>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/YY.png\"/>
+</p>
+<h4>Note:</h4>
+<p>
+This model reuses models from
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterYY</a> for
+details on the connections.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerFull;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepDownDY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepDownDY.mo
new file mode 100644
index 0000000000..8ed7a47765
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepDownDY.mo
@@ -0,0 +1,260 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+model ACACTransformerStepDownDY
+  "AC AC transformer simplified equivalent circuit (DY step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepDownDY(
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv1(
+      VHigh=VHigh,
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=-VLow/sqrt(3),
+      phi_1=2.6179938779915),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv2(
+      VHigh=VHigh,
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=-VLow/sqrt(3),
+      phi_1=0.5235987755983),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv3(
+      VHigh=VHigh,
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=-VLow/sqrt(3),
+      phi_1=-1.5707963267949));
+  parameter Modelica.Units.SI.Voltage VHigh
+    "Rms voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "Rms voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Real XoverR
+    "Ratio between the complex and real components of the impedance (XL/R)";
+  parameter Real Zperc "Short circuit impedance";
+  parameter Boolean ground_1 = false "Connect side 1 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 2"));
+equation
+
+  annotation (
+  defaultComponentName="tra",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-130,60},{-70,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,60},{130,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-72,40},{-66,40},{-64,44},{-60,36},{-56,44},{-52,36},{-48,44},
+              {-44,36},{-42,40},{-38,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-60,-7.34764e-15}},
+          color={0,127,127},
+          origin={-40,40},
+          rotation=180),
+        Ellipse(
+          extent={{-30,46},{-18,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-18,46},{-6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,46},{6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-30,40},{6,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,40},{20,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{14,20},{26,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,8},{26,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,-4},{26,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{10,20},{20,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,-16},{20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{20,-40},{-70,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{34,40},{34,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{40,20},{28,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,8},{28,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,-4},{28,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{44,20},{34,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{34,-16},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,-40},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,40},{34,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-64,60},{-48,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-20,60},{-4,48}},
+          textColor={0,120,120},
+          textString="L"),
+        Line(
+          points={{60,26},{60,6},{46,-8}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{60,6},{74,-8}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{-52,-6},{-32,24},{-12,-6},{-52,-6}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{0,100},{32,68}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Polygon(
+          points={{0,-6},{6,6},{-6,0},{0,-6}},
+          lineColor={0,120,120},
+          smooth=Smooth.None,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid,
+          origin={34,66},
+          rotation=-90)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a simplified equivalent transformer model with Y-Delta connection
+(voltage step down).
+The model accounts for winding Joule losses and leakage reactances
+that are represented by a series of a resistance <i>R</i> and an
+inductance <i>L</i>. The resistance and the inductance represent the
+effects of the secondary and primary side of the transformer.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>Vhigh</code> - RMS voltage at primary side,</li>
+<li><code>Vlow</code> - RMS voltage at secondary side,</li>
+<li><code>VAbase</code> - apparent nominal power of the transformer,</li>
+<li><code>XoverR</code> - ratio between reactance and resistance, and</li>
+<li><code>Zperc</code> - the short circuit impedance.</li>
+</ul>
+<p>
+Given the nominal conditions, the model computes the values of the resistance and inductance.
+</p>
+
+<h4>Configuration:</h4>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/DY_a.png\"/>
+</p>
+
+<h4>Note:</h4>
+<p>
+This model reuses models from
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepDownDY\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepDownDY</a> for
+details on the connections.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerStepDownDY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepDownYD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepDownYD.mo
new file mode 100644
index 0000000000..1cc798531f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepDownYD.mo
@@ -0,0 +1,258 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+model ACACTransformerStepDownYD
+  "AC AC transformer simplified equivalent circuit (YD step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepDownYD(
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv1(
+      VHigh=VHigh/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=VLow,
+      phi_1=0),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv2(
+      VHigh=VHigh/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=VLow,
+      phi_1=-2.0943951023932),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv3(
+      VHigh=VHigh/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=VLow,
+      phi_1=2.0943951023932));
+  parameter Modelica.Units.SI.Voltage VHigh
+    "Rms voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "Rms voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Real XoverR
+    "Ratio between the complex and real components of the impedance (XL/R)";
+  parameter Real Zperc "Short circuit impedance";
+  parameter Boolean ground_1 = false "Connect side 1 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 2"));
+equation
+
+  annotation (
+  defaultComponentName="tra",
+ Icon(graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-130,60},{-70,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,60},{130,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-72,40},{-66,40},{-64,44},{-60,36},{-56,44},{-52,36},{-48,44},
+              {-44,36},{-42,40},{-38,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-60,-7.34764e-15}},
+          color={0,127,127},
+          origin={-40,40},
+          rotation=180),
+        Ellipse(
+          extent={{-30,46},{-18,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-18,46},{-6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,46},{6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-30,40},{6,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,40},{20,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{14,20},{26,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,8},{26,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,-4},{26,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{10,20},{20,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,-16},{20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{20,-40},{-70,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{34,40},{34,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{40,20},{28,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,8},{28,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,-4},{28,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{44,20},{34,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{34,-16},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,-40},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,40},{34,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-64,60},{-48,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-20,60},{-4,48}},
+          textColor={0,120,120},
+          textString="L"),
+        Line(
+          points={{-40,20},{-40,0},{-54,-14}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{-40,0},{-26,-14}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{40,-10},{60,20},{80,-10},{40,-10}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{0,100},{32,68}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Polygon(
+          points={{0,-6},{6,6},{-6,0},{0,-6}},
+          lineColor={0,120,120},
+          smooth=Smooth.None,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid,
+          origin={34,66},
+          rotation=-90)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a simplified equivalent transformer model with Y-Delta connection
+(voltage step down).
+The model accounts for winding Joule losses and leakage reactances
+that are represented by a series of a resistance <i>R</i> and an
+inductance <i>L</i>. The resistance and the inductance represent the
+effects of the secondary and primary side of the transformer.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>Vhigh</code> - RMS voltage at primary side,</li>
+<li><code>Vlow</code> - RMS voltage at secondary side,</li>
+<li><code>VAbase</code> - apparent nominal power of the transformer,</li>
+<li><code>XoverR</code> - ratio between reactance and resistance, and</li>
+<li><code>Zperc</code> - the short circuit impedance.</li>
+</ul>
+<p>
+Given the nominal conditions, the model computes the values of the resistance and inductance.
+</p>
+
+<h4>Configuration:</h4>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/YD_a.png\"/>
+</p>
+
+<h4>Note:</h4>
+<p>
+This model reuses models from
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepDownYD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepDownYD</a> for
+details on the connections.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerStepDownYD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepUpDY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepUpDY.mo
new file mode 100644
index 0000000000..de02e6f259
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepUpDY.mo
@@ -0,0 +1,256 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+model ACACTransformerStepUpDY
+  "AC AC transformer simplified equivalent circuit (DY step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepUpDY(
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv1(
+      VHigh=VHigh,
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=VLow/sqrt(3),
+      phi_1=0.5235987755983),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv2(
+      VHigh=VHigh,
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=VLow/sqrt(3),
+      phi_1=-1.5707963267949),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv3(
+      VHigh=VHigh,
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=VLow/sqrt(3),
+      phi_1=2.6179938779915));
+  parameter Modelica.Units.SI.Voltage VHigh
+    "Rms voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "Rms voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Real XoverR
+    "Ratio between the complex and real components of the impedance (XL/R)";
+  parameter Real Zperc "Short circuit impedance";
+  parameter Boolean ground_1 = false "Connect side 1 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 2"));
+equation
+
+  annotation (
+  defaultComponentName="tra",
+ Icon(graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-130,60},{-70,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,60},{130,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-72,40},{-66,40},{-64,44},{-60,36},{-56,44},{-52,36},{-48,44},
+              {-44,36},{-42,40},{-38,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-60,-7.34764e-15}},
+          color={0,127,127},
+          origin={-40,40},
+          rotation=180),
+        Ellipse(
+          extent={{-30,46},{-18,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-18,46},{-6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,46},{6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-30,40},{6,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,40},{20,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{14,20},{26,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,8},{26,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,-4},{26,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{10,20},{20,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,-16},{20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{20,-40},{-70,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{34,40},{34,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{40,20},{28,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,8},{28,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,-4},{28,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{44,20},{34,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{34,-16},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,-40},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,40},{34,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-64,60},{-48,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-20,60},{-4,48}},
+          textColor={0,120,120},
+          textString="L"),
+        Line(
+          points={{60,26},{60,6},{46,-8}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{60,6},{74,-8}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{-52,-6},{-32,24},{-12,-6},{-52,-6}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{0,60},{32,92}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Polygon(
+          points={{34,88},{40,100},{28,94},{34,88}},
+          lineColor={0,120,120},
+          smooth=Smooth.None,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a simplified equivalent transformer model with Delta-Y connection
+(voltage step up).
+The model accounts for winding Joule losses and leakage reactances
+that are represented by a series of a resistance <i>R</i> and an
+inductance <i>L</i>. The resistance and the inductance represent the
+effects of the secondary and primary side of the transformer.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>Vhigh</code> - RMS voltage at primary side,</li>
+<li><code>Vlow</code> - RMS voltage at secondary side,</li>
+<li><code>VAbase</code> - apparent nominal power of the transformer,</li>
+<li><code>XoverR</code> - ratio between reactance and resistance, and</li>
+<li><code>Zperc</code> - the short circuit impedance.</li>
+</ul>
+<p>
+Given the nominal conditions, the model computes the values of the resistance and inductance.
+</p>
+
+<h4>Configuration:</h4>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/DY_b.png\"/>
+</p>
+
+<h4>Note:</h4>
+<p>
+This model reuses models from
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepUpDY\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepUpDY</a> for
+details on the connections.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerStepUpDY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepUpYD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepUpYD.mo
new file mode 100644
index 0000000000..2cb82448d5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/ACACTransformerStepUpYD.mo
@@ -0,0 +1,256 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+model ACACTransformerStepUpYD
+  "AC AC transformer simplified equivalent circuit (YD step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepUpYD(
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv1(
+      VHigh=VHigh/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=-VLow,
+      phi_1=0),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv2(
+      VHigh=VHigh/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=-VLow,
+      phi_1=-2.0943951023932),
+    redeclare AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer conv3(
+      VHigh=VHigh/sqrt(3),
+      XoverR=XoverR,
+      Zperc=Zperc,
+      ground_1=ground_1,
+      ground_2=ground_2,
+      VABase=VABase/3,
+      VLow=-VLow,
+      phi_1=2.0943951023932));
+  parameter Modelica.Units.SI.Voltage VHigh
+    "Rms voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "Rms voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.ApparentPower VABase
+    "Nominal power of the transformer";
+  parameter Real XoverR
+    "Ratio between the complex and real components of the impedance (XL/R)";
+  parameter Real Zperc "Short circuit impedance";
+  parameter Boolean ground_1 = false "Connect side 1 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of transformer to ground" annotation(Dialog(tab = "Ground", group="side 2"));
+equation
+
+  annotation (
+  defaultComponentName="tra",
+ Icon(graphics={
+        Text(
+          extent={{-100,-60},{100,-92}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-130,60},{-70,20}},
+          textColor={11,193,87},
+          textString="1"),
+        Text(
+          extent={{-130,100},{-70,60}},
+          textColor={11,193,87},
+          textString="AC"),
+        Text(
+          extent={{70,100},{130,60}},
+          textColor={0,120,120},
+          textString="AC"),
+        Text(
+          extent={{70,60},{130,20}},
+          textColor={0,120,120},
+          textString="2"),
+        Line(
+          points={{-72,40},{-66,40},{-64,44},{-60,36},{-56,44},{-52,36},{-48,44},
+              {-44,36},{-42,40},{-38,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-60,-7.34764e-15}},
+          color={0,127,127},
+          origin={-40,40},
+          rotation=180),
+        Ellipse(
+          extent={{-30,46},{-18,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-18,46},{-6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,46},{6,34}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-30,40},{6,28}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,40},{20,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{14,20},{26,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,8},{26,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,-4},{26,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{10,20},{20,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{20,-16},{20,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{20,-40},{-70,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{34,40},{34,20}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{40,20},{28,8}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,8},{28,-4}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{40,-4},{28,-16}},
+          lineColor={0,127,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{44,20},{34,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Line(
+          points={{34,-16},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,-40},{34,-40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Line(
+          points={{70,40},{34,40}},
+          color={0,127,127},
+          smooth=Smooth.None),
+        Text(
+          extent={{-64,60},{-48,48}},
+          textColor={0,120,120},
+          textString="R"),
+        Text(
+          extent={{-20,60},{-4,48}},
+          textColor={0,120,120},
+          textString="L"),
+        Line(
+          points={{-40,20},{-40,0},{-54,-14}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{-40,0},{-26,-14}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{40,-10},{60,20},{80,-10},{40,-10}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{0,60},{32,92}},
+          color={0,120,120},
+          smooth=Smooth.None),
+        Polygon(
+          points={{34,88},{40,100},{28,94},{34,88}},
+          lineColor={0,120,120},
+          smooth=Smooth.None,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a simplified equivalent transformer model with Y-Delta connection
+(voltage step up).
+The model accounts for winding Joule losses and leakage reactances
+that are represented by a series of a resistance <i>R</i> and an
+inductance <i>L</i>. The resistance and the inductance represent the
+effects of the secondary and primary side of the transformer.
+</p>
+<p>
+The model is parameterized using the following parameters
+</p>
+<ul>
+<li><code>Vhigh</code> - RMS voltage at primary side,</li>
+<li><code>Vlow</code> - RMS voltage at secondary side,</li>
+<li><code>VAbase</code> - apparent nominal power of the transformer,</li>
+<li><code>XoverR</code> - ratio between reactance and resistance, and</li>
+<li><code>Zperc</code> - the short circuit impedance.</li>
+</ul>
+<p>
+Given the nominal conditions, the model computes the values of the resistance and inductance.
+</p>
+
+<h4>Configuration:</h4>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/YD_b.png\"/>
+</p>
+
+<h4>Note:</h4>
+<p>
+This model reuses models from
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer\">
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepUpYD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverterStepUpYD</a> for
+details on the connections.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACACTransformerStepUpYD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverter.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverter.mo
new file mode 100644
index 0000000000..c2dbb105ef
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverter.mo
@@ -0,0 +1,52 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses;
+partial model PartialConverter "Partial model of a transformer"
+  extends AixLib.Electrical.Icons.RefAngleConversion;
+  replaceable AixLib.Electrical.Interfaces.PartialConversion
+    conv1 constrainedby AixLib.Electrical.Interfaces.PartialConversion(
+    redeclare package PhaseSystem_p =
+        AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n =
+        AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare Electrical.AC.OnePhase.Interfaces.Terminal_n terminal_n,
+    redeclare Electrical.AC.OnePhase.Interfaces.Terminal_p terminal_p)
+    "Transformer phase 1"
+    annotation (Placement(transformation(extent={{-10,42},{10,62}})));
+  replaceable AixLib.Electrical.Interfaces.PartialConversion
+    conv2 constrainedby AixLib.Electrical.Interfaces.PartialConversion(
+    redeclare package PhaseSystem_p =
+        AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n =
+        AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare Electrical.AC.OnePhase.Interfaces.Terminal_n terminal_n,
+    redeclare Electrical.AC.OnePhase.Interfaces.Terminal_p terminal_p)
+    "Transformer phase 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  replaceable AixLib.Electrical.Interfaces.PartialConversion
+    conv3 constrainedby AixLib.Electrical.Interfaces.PartialConversion(
+    redeclare package PhaseSystem_p =
+        AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare package PhaseSystem_n =
+        AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare Electrical.AC.OnePhase.Interfaces.Terminal_n terminal_n,
+    redeclare Electrical.AC.OnePhase.Interfaces.Terminal_p terminal_p)
+    "Transformer phase 3"
+    annotation (Placement(transformation(extent={{-10,-70},{10,-50}})));
+  Interfaces.Terminal_n terminal_n "Electrical connector side N"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+  Interfaces.Terminal_p terminal_p "Electrical connector side P"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}})));
+  annotation (    Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model that represents a three-phase unbalanced
+transformer without neutral cable connection.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConverter;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterDD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterDD.mo
new file mode 100644
index 0000000000..923abb3f92
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterDD.mo
@@ -0,0 +1,75 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses;
+partial model PartialConverterDD "Model of a transformer with D connection primary side and D
+  connection secondary side"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverter;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToDelta wye_to_delta
+    "Delta to wye connection"
+    annotation (Placement(transformation(extent={{78,-10},{58,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToDelta delta_to_wye
+    "Delta to wye connection"
+    annotation (Placement(transformation(extent={{-76,-10},{-56,10}})));
+protected
+  Interfaces.Adapter3to3 ada_n "Adapter"
+    annotation (Placement(transformation(extent={{-30,-10},{-50,10}})));
+  Interfaces.Adapter3to3 ada_p "Adapter"
+    annotation (Placement(transformation(extent={{30,-10},{50,10}})));
+equation
+
+  connect(delta_to_wye.wye, terminal_n) annotation (Line(
+      points={{-76,4.44089e-16},{-80,4.44089e-16},{-80,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(wye_to_delta.wye, terminal_p) annotation (Line(
+      points={{78,6.66134e-16},{82,6.66134e-16},{82,0},{92,0},{92,4.44089e-16},{100,
+          4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(delta_to_wye.delta, ada_n.terminal)
+    annotation (Line(points={{-56,0},{-50,0}}, color={0,120,120}));
+  connect(wye_to_delta.delta, ada_p.terminal)
+    annotation (Line(points={{58,0},{50,0}}, color={0,120,120}));
+  connect(conv1.terminal_n, ada_n.terminals[1]) annotation (Line(points={{-10,
+          52},{-20,52},{-20,0.533333},{-30.2,0.533333}}, color={0,0,0}));
+  connect(conv2.terminal_n, ada_n.terminals[2]) annotation (Line(points={{-10,0},
+          {-20,0},{-20,0},{-30.2,0}}, color={0,0,0}));
+  connect(conv3.terminal_n, ada_n.terminals[3]) annotation (Line(points={{-10,
+          -60},{-20,-60},{-20,-14},{-20,-0.533333},{-30.2,-0.533333}}, color={0,
+          0,0}));
+  connect(conv1.terminal_p, ada_p.terminals[1]) annotation (Line(points={{10,52},
+          {20,52},{20,0.533333},{30.2,0.533333}}, color={0,0,0}));
+  connect(conv2.terminal_p, ada_p.terminals[2])
+    annotation (Line(points={{10,0},{20,0},{20,0},{30.2,0}}, color={0,0,0}));
+  connect(conv3.terminal_p, ada_p.terminals[3]) annotation (Line(points={{10,
+          -60},{20,-60},{20,-26},{20,-0.533333},{30.2,-0.533333}}, color={0,0,0}));
+  annotation(Documentation(revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapter for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model that represents a three-phase unbalanced
+transformer with delta connection on both primary and secondary side.
+</p>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/DD.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConverterDD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepDownDY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepDownDY.mo
new file mode 100644
index 0000000000..2df5060f02
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepDownDY.mo
@@ -0,0 +1,75 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses;
+partial model PartialConverterStepDownDY "Model of a transformer with D connection primary side and
+  Y connection secondary side (Voltage step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverter;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToWyeGround wye_to_wyeg
+    "Wye to wye grounded connection"
+    annotation (Placement(transformation(extent={{78,-10},{58,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToDelta delta_to_wye
+    "Delta to wye connection"
+    annotation (Placement(transformation(extent={{-76,-10},{-56,10}})));
+protected
+  Interfaces.Adapter3to3 ada3to3_n "Adapter for connections"
+    annotation (Placement(transformation(extent={{-30,-10},{-50,10}})));
+  Interfaces.Adapter3to3 ada3to3_p "Adapter for connections"
+    annotation (Placement(transformation(extent={{30,-10},{50,10}})));
+equation
+
+  connect(delta_to_wye.wye, terminal_n) annotation (Line(
+      points={{-76,4.44089e-16},{-80,4.44089e-16},{-80,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(wye_to_wyeg.wye, terminal_p) annotation (Line(
+      points={{78,6.66134e-16},{82,6.66134e-16},{82,0},{92,0},{92,4.44089e-16},{100,
+          4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(conv1.terminal_n, ada3to3_n.terminals[3]) annotation (Line(points={{-10,52},
+          {-20,52},{-20,0.533333},{-30,0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_n, ada3to3_n.terminals[1])
+    annotation (Line(points={{-10,0},{-30,0},{-30,-0.533333}}, color={0,0,0}));
+  connect(conv3.terminal_n, ada3to3_n.terminals[2]) annotation (Line(points={{-10,
+          -60},{-20,-60},{-20,0},{-30,0}}, color={0,0,0}));
+  connect(delta_to_wye.delta, ada3to3_n.terminal)
+    annotation (Line(points={{-56,0},{-53,0},{-50,0}}, color={0,120,120}));
+  connect(conv1.terminal_p, ada3to3_p.terminals[1]) annotation (Line(points={{10,52},
+          {20,52},{20,-0.533333},{30,-0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_p, ada3to3_p.terminals[2])
+    annotation (Line(points={{10,0},{20,0},{30,0}}, color={0,0,0}));
+  connect(conv3.terminal_p, ada3to3_p.terminals[3]) annotation (Line(points={{10,-60},
+          {20,-60},{20,0.533333},{30,0.533333}},      color={0,0,0}));
+  connect(ada3to3_p.terminal, wye_to_wyeg.wyeg)
+    annotation (Line(points={{50,0},{54,0},{58,0}}, color={0,120,120}));
+  annotation (    Documentation(revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapter for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model that represents a three-phase unbalanced
+transformer with delta connection on the primary and Y connection on
+the secondary side. The configuration is for voltage step down.
+</p>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/DY_a.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConverterStepDownDY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepDownYD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepDownYD.mo
new file mode 100644
index 0000000000..f76fec63af
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepDownYD.mo
@@ -0,0 +1,75 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses;
+partial model PartialConverterStepDownYD "Model of a transformer with Y connection primary side and D
+connection secondary side (Voltage step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverter;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToWyeGround wye_to_wyeg
+    "Wye to wye grounded connection"
+    annotation (Placement(transformation(extent={{-82,-10},{-62,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToDelta delta_to_wye
+    "Delta to wye connection "
+    annotation (Placement(transformation(extent={{80,-10},{60,10}})));
+protected
+  Interfaces.Adapter3to3 ada3to3_n "Adapter for connections"
+    annotation (Placement(transformation(extent={{-30,-10},{-50,10}})));
+  Interfaces.Adapter3to3 ada3to3_p "Adapter for connections"
+    annotation (Placement(transformation(extent={{30,-10},{50,10}})));
+equation
+
+  connect(delta_to_wye.wye, terminal_p) annotation (Line(
+      points={{80,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(wye_to_wyeg.wye, terminal_n) annotation (Line(
+      points={{-82,6.66134e-16},{-84,6.66134e-16},{-84,0},{-86,0},{-86,4.44089e-16},
+          {-100,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(conv1.terminal_n, ada3to3_n.terminals[1]) annotation (Line(points={{-10,52},
+          {-20,52},{-20,-0.533333},{-30,-0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_n, ada3to3_n.terminals[2])
+    annotation (Line(points={{-10,0},{-30,0},{-30,0}}, color={0,0,0}));
+  connect(conv3.terminal_n, ada3to3_n.terminals[3]) annotation (Line(points={{-10,-60},
+          {-20,-60},{-20,0.533333},{-30,0.533333}},      color={0,0,0}));
+  connect(conv1.terminal_p, ada3to3_p.terminals[1]) annotation (Line(points={{10,52},
+          {20,52},{20,-0.533333},{30,-0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_p, ada3to3_p.terminals[2])
+    annotation (Line(points={{10,0},{20,0},{30,0}}, color={0,0,0}));
+  connect(conv3.terminal_p, ada3to3_p.terminals[3]) annotation (Line(points={{10,-60},
+          {20,-60},{20,0.533333},{30,0.533333}},      color={0,0,0}));
+  connect(ada3to3_p.terminal, delta_to_wye.delta)
+    annotation (Line(points={{50,0},{55,0},{60,0}}, color={0,120,120}));
+  connect(wye_to_wyeg.wyeg, ada3to3_n.terminal)
+    annotation (Line(points={{-62,0},{-56,0},{-50,0}}, color={0,120,120}));
+  annotation (    Documentation(revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapter for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model that represents a three-phase unbalanced
+transformer with Y connection on primary and delta connection on
+the secondary one. The configuration is for voltage step down.
+</p>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/YD_a.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConverterStepDownYD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepUpDY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepUpDY.mo
new file mode 100644
index 0000000000..233b2732f1
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepUpDY.mo
@@ -0,0 +1,75 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses;
+partial model PartialConverterStepUpDY "Model of a transformer with D connection primary side and Y connection
+  secondary side (Voltage step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverter;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToWyeGround wye_to_wyeg
+    "Wye to wye grounded connection"
+    annotation (Placement(transformation(extent={{78,-10},{58,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToDelta delta_to_wye
+    "Delta to wye connection"
+    annotation (Placement(transformation(extent={{-76,-10},{-56,10}})));
+protected
+  Interfaces.Adapter3to3 ada3to3_n "Adapter for connections"
+    annotation (Placement(transformation(extent={{-30,-10},{-50,10}})));
+  Interfaces.Adapter3to3 ada3to3_p "Adapter for connections"
+    annotation (Placement(transformation(extent={{30,-10},{50,10}})));
+equation
+
+  connect(delta_to_wye.wye, terminal_n) annotation (Line(
+      points={{-76,4.44089e-16},{-80,4.44089e-16},{-80,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(wye_to_wyeg.wye, terminal_p) annotation (Line(
+      points={{78,6.66134e-16},{82,6.66134e-16},{82,0},{92,0},{92,4.44089e-16},{100,
+          4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(conv1.terminal_n,ada3to3_n. terminals[1]) annotation (Line(points={{-10,52},
+          {-20,52},{-20,-0.533333},{-30,-0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_n,ada3to3_n. terminals[2])
+    annotation (Line(points={{-10,0},{-30,0}},         color={0,0,0}));
+  connect(conv3.terminal_n,ada3to3_n. terminals[3]) annotation (Line(points={{-10,-60},
+          {-20,-60},{-20,0.533333},{-30,0.533333}},      color={0,0,0}));
+  connect(conv1.terminal_p,ada3to3_p. terminals[1]) annotation (Line(points={{10,52},
+          {20,52},{20,-0.533333},{30,-0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_p,ada3to3_p. terminals[2])
+    annotation (Line(points={{10,0},{10,0},{30,0}}, color={0,0,0}));
+  connect(conv3.terminal_p,ada3to3_p. terminals[3]) annotation (Line(points={{10,-60},
+          {20,-60},{20,0.533333},{30,0.533333}},      color={0,0,0}));
+  connect(ada3to3_p.terminal, wye_to_wyeg.wyeg)
+    annotation (Line(points={{50,0},{54,0},{58,0}}, color={0,120,120}));
+  connect(delta_to_wye.delta, ada3to3_n.terminal)
+    annotation (Line(points={{-56,0},{-50,0}}, color={0,120,120}));
+  annotation (    Documentation(revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapter for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model that represents a three-phase unbalanced
+transformer with delta connection on the primary and Y connection on
+the secondary side. The configuration is for voltage step up.
+</p>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/DY_b.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConverterStepUpDY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepUpYD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepUpYD.mo
new file mode 100644
index 0000000000..84ed898320
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterStepUpYD.mo
@@ -0,0 +1,76 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses;
+partial model PartialConverterStepUpYD "Model of a transformer with Y connection primary side and D connection
+  secondary side (Voltage step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverter;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToWyeGround wye_to_wyeg
+    "Wye to wye grounded connection"
+    annotation (Placement(transformation(extent={{-82,-10},{-62,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToDelta delta_to_wye
+    "Delta to wye connection"
+    annotation (Placement(transformation(extent={{80,-10},{60,10}})));
+protected
+  Interfaces.Adapter3to3 ada3to3_n "Adapter for connections"
+    annotation (Placement(transformation(extent={{-30,-10},{-50,10}})));
+  Interfaces.Adapter3to3 ada3to3_p "Adapter for connections"
+    annotation (Placement(transformation(extent={{26,-10},{46,10}})));
+equation
+
+  connect(delta_to_wye.wye, terminal_p) annotation (Line(
+      points={{80,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(wye_to_wyeg.wye, terminal_n) annotation (Line(
+      points={{-82,6.66134e-16},{-84,6.66134e-16},{-84,0},{-86,0},{-86,4.44089e-16},
+          {-100,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(conv1.terminal_n,ada3to3_n. terminals[1]) annotation (Line(points={{-10,52},
+          {-20,52},{-20,-0.533333},{-30,-0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_n,ada3to3_n. terminals[2])
+    annotation (Line(points={{-10,0},{-26,0},{-30,0}}, color={0,0,0}));
+  connect(conv3.terminal_n,ada3to3_n. terminals[3]) annotation (Line(points={{-10,-60},
+          {-20,-60},{-20,0.533333},{-30,0.533333}},      color={0,0,0}));
+  connect(wye_to_wyeg.wyeg, ada3to3_n.terminal)
+    annotation (Line(points={{-62,0},{-56,0},{-50,0}}, color={0,120,120}));
+  connect(conv1.terminal_p, ada3to3_p.terminals[3]) annotation (Line(points={{10,52},
+          {20,52},{20,0.533333},{26,0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_p, ada3to3_p.terminals[1]) annotation (Line(points={{10,0},{
+          28,0},{28,-0.533333},{26,-0.533333}},     color={0,0,0}));
+  connect(conv3.terminal_p, ada3to3_p.terminals[2]) annotation (Line(points={{10,
+          -60},{10,-60},{16,-60},{16,-60},{20,-60},{20,0},{26,0},{26,0}}, color=
+         {0,0,0}));
+  connect(ada3to3_p.terminal, delta_to_wye.delta)
+    annotation (Line(points={{46,0},{53,0},{60,0}}, color={0,120,120}));
+  annotation (    Documentation(revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapter for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model that represents a three-phase unbalanced
+transformer with Y connection on the primary and delta connection on
+the secondary side. The configuration is for voltage step up.
+</p>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/YD_b.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConverterStepUpYD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterYY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterYY.mo
new file mode 100644
index 0000000000..1332f9315b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/PartialConverterYY.mo
@@ -0,0 +1,77 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses;
+partial model PartialConverterYY "Model of a transformer with Y connection primary side and Y
+  connection secondary side"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverter;
+  Interfaces.Connection3to3Ground_n connection3to4_n
+    "Conversion between 3 to 4 connectors"
+    annotation (Placement(transformation(extent={{-60,-10},{-80,10}})));
+  Interfaces.Connection3to3Ground_p connection3to4_p
+    "Conversion between 3 to 4 connectors"
+    annotation (Placement(transformation(extent={{60,-10},{80,10}})));
+  OnePhase.Basics.Ground ground_n "Ground reference"
+    annotation (Placement(transformation(extent={{-70,-90},{-50,-70}})));
+  OnePhase.Basics.Ground ground_p "Ground reference"
+    annotation (Placement(transformation(extent={{50,-90},{70,-70}})));
+protected
+  Interfaces.Adapter3to3 ada3to3_n "Adapter for connections"
+    annotation (Placement(transformation(extent={{-30,-10},{-50,10}})));
+  Interfaces.Adapter3to3 ada3to3_p "Adapter for connections"
+    annotation (Placement(transformation(extent={{30,-10},{50,10}})));
+equation
+
+  connect(terminal_p, connection3to4_p.terminal3) annotation (Line(
+      points={{100,0},{80,0},{80,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n, connection3to4_n.terminal3) annotation (Line(
+      points={{-100,4.44089e-16},{-80,4.44089e-16},{-80,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(connection3to4_p.ground4, ground_p.terminal)
+    annotation (Line(points={{59.6,-6},{60,-6},{60,-70}}, color={0,120,120}));
+  connect(ground_n.terminal, connection3to4_n.ground4) annotation (Line(points={
+          {-60,-70},{-60,-6},{-60.1,-6}}, color={0,120,120}));
+  connect(connection3to4_n.terminal4, ada3to3_n.terminal)
+    annotation (Line(points={{-60,0},{-55,0},{-50,0}}, color={0,120,120}));
+  connect(ada3to3_n.terminals[1], conv1.terminal_n) annotation (Line(points={{-30,
+          -0.533333},{-26,-0.533333},{-20,-0.533333},{-20,52},{-10,52}}, color={
+          0,0,0}));
+  connect(ada3to3_n.terminals[2], conv2.terminal_n)
+    annotation (Line(points={{-30,0},{-20,0},{-10,0}}, color={0,0,0}));
+  connect(ada3to3_n.terminals[3], conv3.terminal_n) annotation (Line(points={{-30,
+          0.533333},{-20,0.533333},{-20,-60},{-10,-60}}, color={0,0,0}));
+  connect(conv1.terminal_p, ada3to3_p.terminals[1]) annotation (Line(points={{10,52},
+          {20,52},{20,-0.533333},{30,-0.533333}},     color={0,0,0}));
+  connect(conv2.terminal_p, ada3to3_p.terminals[2])
+    annotation (Line(points={{10,0},{20,0},{30,0}}, color={0,0,0}));
+  connect(conv3.terminal_p, ada3to3_p.terminals[3]) annotation (Line(points={{10,-60},
+          {20,-60},{20,0.533333},{30,0.533333}},      color={0,0,0}));
+  connect(ada3to3_p.terminal, connection3to4_p.terminal4)
+    annotation (Line(points={{50,0},{55,0},{60,0}}, color={0,120,120}));
+  annotation (    Documentation(revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapters for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model that represents a three-phase unbalanced
+transformer with Y connection on both primary and secondary side.
+</p>
+<p>
+The image below describes the connection of the windings.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/YY.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConverterYY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/package.mo
new file mode 100644
index 0000000000..17f1639c13
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+package BaseClasses "Package with base class models"
+extends Modelica.Icons.BasesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains base classes used by the models that are part of the package
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/package.order
new file mode 100644
index 0000000000..ea6d2d73c9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/BaseClasses/package.order
@@ -0,0 +1,7 @@
+PartialConverter
+PartialConverterDD
+PartialConverterStepDownDY
+PartialConverterStepDownYD
+PartialConverterStepUpDY
+PartialConverterStepUpYD
+PartialConverterYY
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/TransformerExample.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/TransformerExample.mo
new file mode 100644
index 0000000000..116d6522ba
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/TransformerExample.mo
@@ -0,0 +1,77 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.BaseClasses;
+model TransformerExample
+  "This example represents the basic test for a transformer model"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Voltage V_primary=12470
+    "RMS Voltage on the primary side of the transformer";
+  parameter Modelica.Units.SI.Voltage V_secondary=4160
+    "RMS Voltage on the secondary side of the transformer";
+  Sources.FixedVoltage sou(
+    f=60,
+    V=V_primary) "Voltage source"
+    annotation (Placement(transformation(extent={{-70,-10},{-50,10}})));
+  replaceable
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.BaseClasses.PartialConverter
+    tra "Transformer model"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  Loads.Resistive load(
+    loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_wyeg,
+    P_nominal=-1800e3,
+    V_nominal=V_secondary,
+    linearized=true)       "Load model"
+    annotation (Placement(transformation(extent={{50,-10},{70,10}})));
+  Sensors.ProbeWye probe_Y_1(perUnit=false, V_nominal = V_primary)
+    "Probe that measures the voltage in Y configuration, primary side"
+    annotation (Placement(transformation(extent={{-40,30},{-20,50}})));
+  Sensors.ProbeDelta probe_D_1(perUnit=false, V_nominal = V_primary)
+    "Probe that measures the voltage in D configuration, primary side"
+    annotation (Placement(transformation(extent={{-40,-30},{-20,-50}})));
+  replaceable Sensors.BaseClasses.GeneralizedProbe probe_2 constrainedby
+    Sensors.BaseClasses.GeneralizedProbe(perUnit=false,
+    V_nominal=V_secondary)
+    "Probe that measures the voltage at the secondary side"
+    annotation (Placement(transformation(extent={{20,30},{40,50}})));
+
+equation
+  connect(sou.terminal, tra.terminal_n) annotation (Line(
+      points={{-50,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(probe_Y_1.term, tra.terminal_n) annotation (Line(
+      points={{-30,31},{-30,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(probe_D_1.term, tra.terminal_n) annotation (Line(
+      points={{-30,-31},{-30,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(tra.terminal_p, load.terminal) annotation (Line(
+      points={{10,0},{50,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Linearized load to avoid large nonlinear system of equations.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/568\">issue 568</a>.
+</li>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model is the base classes used by the examples that are part of the package
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples</a>.
+</p>
+<p>
+The model has a voltage source, a transformer and a load. The transformer
+model is replaceable so that different types of transformers can easily be tested.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TransformerExample;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/package.mo
new file mode 100644
index 0000000000..ca964dd1ba
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+package BaseClasses "This package contains base classes inherited by the examples"
+extends Modelica.Icons.BasesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+This package contains base classes used by the examples that are part of the package
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/package.order
new file mode 100644
index 0000000000..a13655a958
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/BaseClasses/package.order
@@ -0,0 +1 @@
+TransformerExample
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Converter.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Converter.mo
new file mode 100644
index 0000000000..95625c5ac5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Converter.mo
@@ -0,0 +1,35 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+model Converter "Test for the AC/AC converter model"
+  extends BaseClasses.TransformerExample(
+  V_primary = 480,
+  V_secondary = 240,
+  redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye probe_2,
+  redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACConverter
+  tra(conversionFactor=0.5,eta=0.9));
+
+equation
+  connect(probe_2.term, tra.terminal_p) annotation (Line(
+      points={{30,31},{30,4.44089e-16},{10,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example model tests the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACConverter\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACConverter</a> model.
+</p>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Converter.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Converter;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Transformer.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Transformer.mo
new file mode 100644
index 0000000000..365b1d7d79
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Transformer.mo
@@ -0,0 +1,37 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+model Transformer "Test for the AC/AC transformer model"
+  extends BaseClasses.TransformerExample(
+  redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye probe_2,
+  redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformer
+  tra(VHigh=V_primary,
+      VLow=V_secondary,
+      XoverR=6,
+      Zperc=sqrt(0.01^2 + 0.06^2),
+      VABase=6000000));
+
+equation
+  connect(probe_2.term, load.terminal) annotation (Line(
+      points={{30,31},{30,0},{50,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example model tests the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformer\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformer</a> model.
+</p>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Transformer.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Transformer;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerDD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerDD.mo
new file mode 100644
index 0000000000..db75db82f7
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerDD.mo
@@ -0,0 +1,44 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+model TransformerDD
+  "Test for the AC/AC transformer model with Delta-Delta configuration"
+  extends BaseClasses.TransformerExample(
+  redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta probe_2,
+  redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerDD
+  tra(VHigh=V_primary,
+      VLow=V_secondary,
+      XoverR=6,
+      Zperc=sqrt(0.01^2 + 0.06^2),
+      VABase=6000000));
+
+equation
+  connect(probe_2.term, load.terminal) annotation (Line(
+      points={{30,31},{30,0},{50,0},{50,5.55112e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example model tests the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerDD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerDD</a> model.
+</p>
+<h4>Note:</h4>
+<p>
+When the secondary side of the transformer is in the Delta (D) configuration,
+measuring the voltage with a Wye (Y) is not possible because the voltage vectors
+in the connector do not have a neutral reference.
+</p>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerDD.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end TransformerDD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerFull.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerFull.mo
new file mode 100644
index 0000000000..042e7089fc
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerFull.mo
@@ -0,0 +1,44 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+model TransformerFull "Test for the AC/AC transformer full model"
+  extends BaseClasses.TransformerExample(
+  redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye probe_2,
+  redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerFull
+  tra(VHigh=V_primary,
+      VLow=V_secondary,
+      VABase=6000000,
+      f=60,
+      R1=0.005,
+      L1=0.005*6,
+      R2=0.005,
+      L2=0.005*6,
+      magEffects=true,
+      Rm=10,
+      Lm=10),
+      load(initMode=AixLib.Electrical.Types.InitMode.linearized));
+
+equation
+  connect(probe_2.term, load.terminal) annotation (Line(
+      points={{30,31},{30,0},{50,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example model tests the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerFull\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerFull</a> model.
+</p>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerFull.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end TransformerFull;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownDY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownDY.mo
new file mode 100644
index 0000000000..4012c1af6e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownDY.mo
@@ -0,0 +1,38 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+model TransformerStepDownDY
+  "Test for the AC/AC transformer model with Delta-Wye configuration (step-down voltage)"
+  extends BaseClasses.TransformerExample(
+  redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye probe_2,
+  redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownDY
+  tra(VHigh=V_primary,
+      VLow=V_secondary,
+      XoverR=6,
+      Zperc=sqrt(0.01^2 + 0.06^2),
+      VABase=6000000));
+
+equation
+  connect(probe_2.term, load.terminal) annotation (Line(
+      points={{30,31},{30,0},{50,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example model tests the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownDY\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownDY</a> model.
+</p>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownDY.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end TransformerStepDownDY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownYD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownYD.mo
new file mode 100644
index 0000000000..a5b1fde931
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownYD.mo
@@ -0,0 +1,44 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+model TransformerStepDownYD
+  "Test for the AC/AC transformer model with Wye-Delta configuration (step-down voltage)"
+  extends BaseClasses.TransformerExample(
+  redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta probe_2,
+  redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownYD
+  tra(VHigh=V_primary,
+      VLow=V_secondary,
+      XoverR=6,
+      Zperc=sqrt(0.01^2 + 0.06^2),
+      VABase=6000000));
+
+equation
+  connect(probe_2.term, load.terminal) annotation (Line(
+      points={{30,31},{30,0},{50,0},{50,5.55112e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example model tests the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownYD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownYD</a> model.
+</p>
+<h4>Note:</h4>
+<p>
+When the secondary side of the transformer is in the Delta (D) configuration,
+measuring the voltage with a Wye (Y) is not possible because the voltage vectors
+in the connector do not have a neutral reference.
+</p>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownYD.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end TransformerStepDownYD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpDY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpDY.mo
new file mode 100644
index 0000000000..5020428a0b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpDY.mo
@@ -0,0 +1,40 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+model TransformerStepUpDY
+  "Test for the AC/AC transformer model with Delta-Wye configuration (step-up voltage)"
+  extends BaseClasses.TransformerExample(
+  V_primary = 4160,
+  V_secondary = 12470,
+  redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye probe_2,
+  redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpDY
+  tra(VHigh=V_primary,
+      VLow=V_secondary,
+      XoverR=6,
+      Zperc=sqrt(0.01^2 + 0.06^2),
+      VABase=6000000));
+
+equation
+  connect(probe_2.term, load.terminal) annotation (Line(
+      points={{30,31},{30,0},{50,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example model tests the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpDY\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpDY</a> model.
+</p>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpDY.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end TransformerStepUpDY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpYD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpYD.mo
new file mode 100644
index 0000000000..94bf1efe5c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpYD.mo
@@ -0,0 +1,46 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples;
+model TransformerStepUpYD
+  "Test for the AC/AC transformer model with Wye-Delta configuration (step-up voltage)"
+  extends BaseClasses.TransformerExample(
+  V_primary = 4160,
+  V_secondary = 12470,
+  redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta probe_2,
+  redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpYD
+  tra(VHigh=V_primary,
+      VLow=V_secondary,
+      XoverR=6,
+      Zperc=sqrt(0.01^2 + 0.06^2),
+      VABase=6000000));
+
+equation
+  connect(probe_2.term, load.terminal) annotation (Line(
+      points={{30,31},{30,0},{50,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example model tests the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpYD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpYD</a> model.
+</p>
+<h4>Note:</h4>
+<p>
+When the secondary side of the transformer is in the Delta (D) configuration,
+measuring the voltage with a Wye (Y) is not possible because the voltage vectors
+in the connector do not have a neutral reference.
+</p>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpYD.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end TransformerStepUpYD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/package.mo
new file mode 100644
index 0000000000..29ef8222c6
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/package.mo
@@ -0,0 +1,21 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+
+  annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/package.order
new file mode 100644
index 0000000000..ad3a368e02
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/package.order
@@ -0,0 +1,9 @@
+Converter
+Transformer
+TransformerDD
+TransformerFull
+TransformerStepDownDY
+TransformerStepDownYD
+TransformerStepUpDY
+TransformerStepUpYD
+BaseClasses
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/package.mo
new file mode 100644
index 0000000000..6dc13bd698
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced;
+package Conversion "Package with converter and transformer models for three-phase
+  unbalanced AC systems"
+  extends Modelica.Icons.Package;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains models that represent different types of three
+phases unbalanced AC/AC transformers and AC/DC converters.
+</p>
+</html>"));
+end Conversion;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/package.order
new file mode 100644
index 0000000000..03efaf099a
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Conversion/package.order
@@ -0,0 +1,10 @@
+ACACConverter
+ACACTransformer
+ACACTransformerDD
+ACACTransformerFull
+ACACTransformerStepDownDY
+ACACTransformerStepDownYD
+ACACTransformerStepUpDY
+ACACTransformerStepUpYD
+Examples
+BaseClasses
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Adapter3to3.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Adapter3to3.mo
new file mode 100644
index 0000000000..157f1655cc
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Adapter3to3.mo
@@ -0,0 +1,40 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+model Adapter3to3
+  "Adapter from 3 single phase connectors to a connector with 3 phases"
+  extends Modelica.Blocks.Icons.Block;
+
+  AixLib.Electrical.Interfaces.Terminal terminals[3](
+    redeclare final package PhaseSystem = PhaseSystems.OnePhase)
+    "Generalized terminal"
+    annotation (Placement(transformation(extent={{-92,-6},{-108,10}}),
+        iconTransformation(extent={{-106,8},{-90,-8}})));
+
+  Interfaces.Terminal_p terminal "Connector with 3 lines"
+   annotation (Placement(transformation(extent={{90,-10},{110,10}}),
+                          iconTransformation(extent={{90,-10},{110,10}})));
+equation
+  for i in 1:3 loop
+    terminal.phase[i].v     = terminals[i].v;
+    terminal.phase[i].i     = -terminals[i].i;
+    Connections.branch(terminal.phase[i].theta, terminals[i].theta);
+    terminal.phase[i].theta = terminals[i].theta;
+  end for;
+
+  annotation (
+  defaultComponentName="ada",
+  Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Line(points={{-64,0},{66,0}}, color={28,108,200})}),    Documentation(info="<html>
+<p>
+Adapter that connect 3 single phase connectors with a connector that has 3 phases.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 25, 2016, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Adapter3to3;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to3Ground_n.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to3Ground_n.mo
new file mode 100644
index 0000000000..a4ef7800b7
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to3Ground_n.mo
@@ -0,0 +1,87 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+model Connection3to3Ground_n
+  "Adapter between Terminal4 (3 phases and ground) and Terminal3 N"
+
+  Terminal_n terminal4 "Connector for side with neutral" annotation (Placement(transformation(extent={{-110,-10},
+            {-90,10}}), iconTransformation(extent={{-110,-10},{-90,10}})));
+  AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n ground4
+    "Connector for neutral"
+    annotation (Placement(transformation(extent={{-109,-70},{-89,-50}}),
+                        iconTransformation(extent={{-109,-70},{-89,-50}})));
+  Terminal_n terminal3 "Connector without neutral" annotation (Placement(transformation(extent={{90,-10},{110,
+            10}}), iconTransformation(extent={{90,-10},{110,10}})));
+equation
+
+  // Connection branches required to propagate the reference angle
+  Connections.branch(terminal4.phase[1].theta, ground4.theta);
+  terminal4.phase[1].theta = ground4.theta;
+  for i in 1:3 loop
+    Connections.branch(terminal3.phase[i].theta, terminal4.phase[i].theta);
+    terminal3.phase[i].theta = terminal4.phase[i].theta;
+  end for;
+
+  // KVL and KCL
+  terminal3.phase[1].v[:] = terminal4.phase[1].v[:] - ground4.v[:];
+  terminal3.phase[2].v[:] = terminal4.phase[2].v[:] - ground4.v[:];
+  terminal3.phase[3].v[:] = terminal4.phase[3].v[:] - ground4.v[:];
+
+  terminal4.phase[1].i[:] + terminal4.phase[2].i[:] = -terminal4.phase[3].i[:] - ground4.i[:];
+  terminal4.phase[1].i[:] = - terminal3.phase[1].i[:];
+  terminal4.phase[2].i[:] = - terminal3.phase[2].i[:];
+  terminal4.phase[3].i[:] = - terminal3.phase[3].i[:];
+
+  annotation ( Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+                                             Polygon(
+          points={{-80,110},{-80,70},{0,70},{0,110},{-80,110}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,50},{-80,10},{0,10},{0,50},{-80,50}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,-10},{-80,-50},{0,-50},{0,-10},{-80,-10}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,-70},{-80,-110},{0,-110},{0,-70},{-80,-70}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{0,-40},{0,-80},{80,-80},{80,-40},{0,-40}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{0,20},{0,-20},{80,-20},{80,20},{0,20}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{0,80},{0,40},{80,40},{80,80},{0,80}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+February 25, 2016, by Michael Wetter:<br/>
+First implementation based on previous
+<code>AixLib.Electrical.AC.ThreePhasesUnbalanced.InterfacesConnection3to4_p</code>
+which did not conform to the Modelica Language Definition.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Adapter between electric connectors type n for AC three-phase unbalanced systems.
+This adapter connects a connector without neutral cable to a connector without
+neutral cable.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Connection3to3Ground_n;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to3Ground_p.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to3Ground_p.mo
new file mode 100644
index 0000000000..e832523990
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to3Ground_p.mo
@@ -0,0 +1,85 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+model Connection3to3Ground_p
+  "Adapter between Terminal4 (3 phases and ground) and Terminal3 P"
+
+  Terminal_p terminal4 "Connector with neutral" annotation (Placement(transformation(extent={{-110,-10},
+            {-90,10}}), iconTransformation(extent={{-110,-10},{-90,10}})));
+  AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_p ground4
+    "Connector for neutral"
+    annotation (Placement(transformation(extent={{-114,-70},{-94,-50}}),
+                        iconTransformation(extent={{-114,-70},{-94,-50}})));
+  Terminal_p terminal3 "Connector without neutral" annotation (Placement(transformation(extent={{90,-10},{110,
+            10}}), iconTransformation(extent={{90,-10},{110,10}})));
+equation
+
+  // Connection branches required to propagate the reference angle
+  Connections.branch(terminal4.phase[1].theta, ground4.theta);
+  terminal4.phase[1].theta = ground4.theta;
+  for i in 1:3 loop
+    Connections.branch(terminal3.phase[i].theta, terminal4.phase[i].theta);
+    terminal3.phase[i].theta = terminal4.phase[i].theta;
+  end for;
+
+  // KVL and KCL
+  terminal3.phase[1].v[:] = terminal4.phase[1].v[:] - ground4.v[:];
+  terminal3.phase[2].v[:] = terminal4.phase[2].v[:] - ground4.v[:];
+  terminal3.phase[3].v[:] = terminal4.phase[3].v[:] - ground4.v[:];
+
+  terminal4.phase[1].i[:] + terminal4.phase[2].i[:] = -terminal4.phase[3].i[:] - ground4.i[:];
+  terminal4.phase[1].i[:] = - terminal3.phase[1].i[:];
+  terminal4.phase[2].i[:] = - terminal3.phase[2].i[:];
+  terminal4.phase[3].i[:] = - terminal3.phase[3].i[:];
+
+  annotation ( Icon(graphics={               Polygon(
+          points={{-80,110},{-80,70},{0,70},{0,110},{-80,110}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,50},{-80,10},{0,10},{0,50},{-80,50}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,-10},{-80,-50},{0,-50},{0,-10},{-80,-10}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,-70},{-80,-110},{0,-110},{0,-70},{-80,-70}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+              points={{0,80},{0,40},{80,40},{80,80},{0,80}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid),Polygon(
+              points={{0,20},{0,-20},{80,-20},{80,20},{0,20}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid),Polygon(
+              points={{0,-40},{0,-80},{80,-80},{80,-40},{0,-40}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+February 25, 2016, by Michael Wetter:<br/>
+First implementation based on previous
+<code>AixLib.Electrical.AC.ThreePhasesUnbalanced.InterfacesConnection3to4_p</code>
+which did not conform to the Modelica Language Definition.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Adapter between electric connectors type p for AC three-phase unbalanced systems.
+This adapter connects a connector without neutral cable to a connector without
+neutral cable.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Connection3to3Ground_p;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to4_n.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to4_n.mo
new file mode 100644
index 0000000000..ea5f510c41
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to4_n.mo
@@ -0,0 +1,73 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+model Connection3to4_n "Adapter between Terminal4 and Terminal3 N"
+
+  Terminal4_n terminal4 "Connector with neutral" annotation (Placement(transformation(extent={{-110,-10},
+            {-90,10}}), iconTransformation(extent={{-110,-10},{-90,10}})));
+  Terminal_n terminal3 "Connector without neutral" annotation (Placement(transformation(extent={{90,-10},{110,
+            10}}), iconTransformation(extent={{90,-10},{110,10}})));
+equation
+
+  // Connection branches required to propagate the reference angle
+  Connections.branch(terminal4.phase[1].theta, terminal4.phase[4].theta);
+  terminal4.phase[1].theta = terminal4.phase[4].theta;
+  for i in 1:3 loop
+    Connections.branch(terminal3.phase[i].theta, terminal4.phase[i].theta);
+    terminal3.phase[i].theta = terminal4.phase[i].theta;
+  end for;
+
+  // KVL and KCL
+  terminal3.phase[1].v[:] = terminal4.phase[1].v[:] - terminal4.phase[4].v[:];
+  terminal3.phase[2].v[:] = terminal4.phase[2].v[:] - terminal4.phase[4].v[:];
+  terminal3.phase[3].v[:] = terminal4.phase[3].v[:] - terminal4.phase[4].v[:];
+
+  terminal4.phase[1].i[:] + terminal4.phase[2].i[:] = -terminal4.phase[3].i[:] - terminal4.phase[4].i[:];
+  terminal4.phase[1].i[:] = - terminal3.phase[1].i[:];
+  terminal4.phase[2].i[:] = - terminal3.phase[2].i[:];
+  terminal4.phase[3].i[:] = - terminal3.phase[3].i[:];
+
+  annotation ( Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+                                             Polygon(
+          points={{-80,110},{-80,70},{0,70},{0,110},{-80,110}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,50},{-80,10},{0,10},{0,50},{-80,50}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,-10},{-80,-50},{0,-50},{0,-10},{-80,-10}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,-70},{-80,-110},{0,-110},{0,-70},{-80,-70}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{0,-40},{0,-80},{80,-80},{80,-40},{0,-40}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{0,20},{0,-20},{80,-20},{80,20},{0,20}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{0,80},{0,40},{80,40},{80,80},{0,80}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Adapter between electric connectors type n for AC three-phase unbalanced systems.
+This adapter connects a connector without neutral cable with a one that has it
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Connection3to4_n;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to4_p.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to4_p.mo
new file mode 100644
index 0000000000..a52b8ca3c3
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Connection3to4_p.mo
@@ -0,0 +1,71 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+model Connection3to4_p "Adapter between Terminal4 and Terminal3 P"
+
+  Terminal4_p terminal4 "Connector with neutral" annotation (Placement(transformation(extent={{-110,-10},
+            {-90,10}}), iconTransformation(extent={{-110,-10},{-90,10}})));
+  Terminal_p terminal3 "Connector without neutral" annotation (Placement(transformation(extent={{90,-10},{110,
+            10}}), iconTransformation(extent={{90,-10},{110,10}})));
+equation
+
+  // Connection branches required to propagate the reference angle
+  Connections.branch(terminal4.phase[1].theta, terminal4.phase[4].theta);
+  terminal4.phase[1].theta = terminal4.phase[4].theta;
+  for i in 1:3 loop
+    Connections.branch(terminal3.phase[i].theta, terminal4.phase[i].theta);
+    terminal3.phase[i].theta = terminal4.phase[i].theta;
+  end for;
+
+  // KVL and KCL
+  terminal3.phase[1].v[:] = terminal4.phase[1].v[:] - terminal4.phase[4].v[:];
+  terminal3.phase[2].v[:] = terminal4.phase[2].v[:] - terminal4.phase[4].v[:];
+  terminal3.phase[3].v[:] = terminal4.phase[3].v[:] - terminal4.phase[4].v[:];
+
+  terminal4.phase[1].i[:] + terminal4.phase[2].i[:] = -terminal4.phase[3].i[:] - terminal4.phase[4].i[:];
+  terminal4.phase[1].i[:] = - terminal3.phase[1].i[:];
+  terminal4.phase[2].i[:] = - terminal3.phase[2].i[:];
+  terminal4.phase[3].i[:] = - terminal3.phase[3].i[:];
+
+  annotation ( Icon(graphics={               Polygon(
+          points={{-80,110},{-80,70},{0,70},{0,110},{-80,110}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,50},{-80,10},{0,10},{0,50},{-80,50}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,-10},{-80,-50},{0,-50},{0,-10},{-80,-10}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-80,-70},{-80,-110},{0,-110},{0,-70},{-80,-70}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+              points={{0,80},{0,40},{80,40},{80,80},{0,80}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid),Polygon(
+              points={{0,20},{0,-20},{80,-20},{80,20},{0,20}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid),Polygon(
+              points={{0,-40},{0,-80},{80,-80},{80,-40},{0,-40}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Adapter between electric connectors type p for AC three-phase unbalanced systems.
+This adapter connects two connectors without and without a neutral cable.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Connection3to4_p;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/WyeToDelta.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/WyeToDelta.mo
new file mode 100644
index 0000000000..130dc739ad
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/WyeToDelta.mo
@@ -0,0 +1,62 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Examples;
+model WyeToDelta "Test for Y to D connection"
+  extends Modelica.Icons.Example;
+
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToDelta wyeToDelta
+    "Conversion of the voltages from Y to D"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.FixedVoltage V1(f=60, V=
+        480) "Voltage source"
+           annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye probe_Y(perUnit=
+       false, V_nominal=480)
+    "Probe that measures the voltage and the angles on each phase"
+    annotation (Placement(transformation(extent={{-30,10},{-10,30}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye probeD(perUnit=
+        false, V_nominal=480)
+    "Probe that measures the voltage and the angles on each phase"
+    annotation (Placement(transformation(extent={{10,10},{30,30}})));
+equation
+  connect(V1.terminal, wyeToDelta.wye) annotation (Line(
+      points={{-40,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(probe_Y.term, wyeToDelta.wye) annotation (Line(
+      points={{-20,11},{-20,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(probeD.term, wyeToDelta.delta) annotation (Line(
+      points={{20,11},{20,0},{10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/WyeToDelta.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised example and documentation.
+</li>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Added info section.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This simple example shows how to use a Y to D adapter.
+</p>
+<p>
+The probe <code>probe_Y</code> mesaures the phase voltages before they
+are converted into D. Their RMS value is equal to <i>480/sqrt(3)</i> V.
+</p>
+<p>
+The probe <code>probe_D</code> measures the phase
+voltages after the conversion to D. Their RMS value is equal to <i>480</i> V,
+the line voltage provided by the voltage source.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WyeToDelta;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/package.mo
new file mode 100644
index 0000000000..b1136be7a0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+package Examples "Package with example models"
+extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/package.order
new file mode 100644
index 0000000000..867feeeb98
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/package.order
@@ -0,0 +1 @@
+WyeToDelta
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal4_n.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal4_n.mo
new file mode 100644
index 0000000000..6face14b04
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal4_n.mo
@@ -0,0 +1,33 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+connector Terminal4_n
+  "Terminal N for AC three-phase unbalanced systems (neutral cable)"
+  AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n phase[4];
+  annotation (Icon(graphics={                Polygon(
+          points={{-100,110},{-100,70},{100,70},{100,110},{-100,110}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-100,-10},{-100,-50},{100,-50},{100,-10},{-100,-10}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-100,50},{-100,10},{100,10},{100,50},{-100,50}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-100,-70},{-100,-110},{100,-110},{100,-70},{-100,-70}},
+          lineColor={127,0,127},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>Electric connector type n for AC three-phase unbalanced systems
+with neutral cable connection.</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal4_n;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal4_p.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal4_p.mo
new file mode 100644
index 0000000000..16e8d68b00
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal4_p.mo
@@ -0,0 +1,34 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+connector Terminal4_p
+  "Terminal P for AC three-phase unbalanced systems (neutral cable)"
+  AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_p phase[4]
+    "Terminal with 3 phases and neutral cable";
+  annotation (Icon(graphics={                Polygon(
+          points={{-100,110},{-100,70},{100,70},{100,110},{-100,110}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-100,50},{-100,10},{100,10},{100,50},{-100,50}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-100,-10},{-100,-50},{100,-50},{100,-10},{-100,-10}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-100,-70},{-100,-110},{100,-110},{100,-70},{-100,-70}},
+          lineColor={127,0,127},
+          fillColor={127,0,127},
+          fillPattern=FillPattern.Solid)}), Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>Electric connector type p for AC three-phase unbalanced systems
+with neutral cable connection.</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal4_p;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal_n.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal_n.mo
new file mode 100644
index 0000000000..40b5f9531c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal_n.mo
@@ -0,0 +1,28 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+connector Terminal_n
+  "Terminal N for AC three-phase unbalanced systems (no neutral cable)"
+  AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n phase[3];
+  annotation (Icon(graphics={                Polygon(
+          points={{-100,100},{-100,60},{100,60},{100,100},{-100,100}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-100,-60},{-100,-100},{100,-100},{100,-60},{-100,-60}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),    Polygon(
+          points={{-100,20},{-100,-20},{100,-20},{100,20},{-100,20}},
+          lineColor={0,120,120},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>Electric connector type n for AC three-phase unbalanced systems.</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal_n;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal_p.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal_p.mo
new file mode 100644
index 0000000000..cc66ae65f4
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Terminal_p.mo
@@ -0,0 +1,28 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+connector Terminal_p
+  "Terminal P for AC three-phase unbalanced systems (no neutral cable)"
+  AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_p phase[3];
+  annotation (Icon(graphics={                Polygon(
+          points={{-100,100},{-100,60},{100,60},{100,100},{-100,100}},
+          lineColor={0,120,120},
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid),    Polygon(
+              points={{-100,-100},{100,-100},{100,-60},{-100,-60},{-100,-100}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid),Polygon(
+              points={{-100,-20},{100,-20},{100,20},{-100,20},{-100,-20}},
+              lineColor={0,120,120},
+              fillColor={0,120,120},
+              fillPattern=FillPattern.Solid)}), Documentation(info="<html>
+<p>Electric connector type p for AC three-phase unbalanced systems.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal_p;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/TwoPort.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/TwoPort.mo
new file mode 100644
index 0000000000..969c509a7d
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/TwoPort.mo
@@ -0,0 +1,28 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+partial model TwoPort
+  "Partial model interface for a two port component without neutral cable"
+
+  Terminal_p terminal_p "Electric terminal side p"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}}),
+        iconTransformation(extent={{90,-10},{110,10}})));
+  Terminal_n terminal_n "Electric terminal side n"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Added model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Interface model for an AC three-phase unbalanced component with two ports
+and without neutral cable.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPort;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/TwoPort_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/TwoPort_N.mo
new file mode 100644
index 0000000000..d05740ca7c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/TwoPort_N.mo
@@ -0,0 +1,28 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+partial model TwoPort_N
+  "Partial model interface for a two port component with neutral cable"
+
+  Terminal4_p terminal_p "Electric terminal side p"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}}),
+        iconTransformation(extent={{90,-10},{110,10}})));
+  Terminal4_n terminal_n "Electric terminal side n"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Added model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Interface model for an AC three-phase unbalanced component with two ports
+and with neutral cable.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPort_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/WyeToDelta.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/WyeToDelta.mo
new file mode 100644
index 0000000000..0b5a68650c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/WyeToDelta.mo
@@ -0,0 +1,60 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+model WyeToDelta "This model represent a connection between wye to delta"
+
+  Terminal_n wye "Terminal Y" annotation (Placement(transformation(extent={{-110,-10},{-90,10}}),
+        iconTransformation(extent={{-110,-10},{-90,10}})));
+  Terminal_n delta "Terminal D" annotation (Placement(transformation(extent={{90,-10},{110,10}}),
+        iconTransformation(extent={{90,-10},{110,10}})));
+equation
+
+  for i in 1:3 loop
+    Connections.branch(wye.phase[i].theta, delta.phase[i].theta);
+    wye.phase[i].theta = delta.phase[i].theta;
+  end for;
+
+  delta.phase[1].v[:] = wye.phase[1].v[:] - wye.phase[2].v[:];
+  delta.phase[2].v[:] = wye.phase[2].v[:] - wye.phase[3].v[:];
+  delta.phase[3].v[:] = wye.phase[3].v[:] - wye.phase[1].v[:];
+
+  -wye.phase[1].i[:] + delta.phase[3].i[:] = delta.phase[1].i[:];
+  -wye.phase[2].i[:] + delta.phase[1].i[:] = delta.phase[2].i[:];
+  -wye.phase[3].i[:] + delta.phase[2].i[:] = delta.phase[3].i[:];
+
+  annotation (
+  defaultComponentName="y2d",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+        Line(
+          points={{-40,-26},{0,34},{40,-26},{-40,-26}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 5, 2014, by Marco Bonvini:<br/>
+Added model.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Adapter from Wye (Y) to Delta (D) connector.
+A three-phase unbalanced connector has three AC single phase
+connectors. Each AC single phase connector contains the phase voltage,
+which is measured between the phase and the neutral.
+This model converts the phase voltage to the line voltage, measured between
+the phases.
+</p>
+<p>
+The image below show how the phasors are computed when converting from Y to D.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Interfaces/YtoD.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WyeToDelta;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/WyeToWyeGround.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/WyeToWyeGround.mo
new file mode 100644
index 0000000000..d80df9f241
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/WyeToWyeGround.mo
@@ -0,0 +1,83 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces;
+model WyeToWyeGround
+  "This model represent a connection between wye to wye grounded"
+
+  Terminal_n wye "Terminal Y" annotation (Placement(transformation(extent={{-110,-10},{-90,10}}),
+        iconTransformation(extent={{-110,-10},{-90,10}})));
+  Terminal_n wyeg "Terminal Y with ground connection" annotation (Placement(transformation(extent={{90,-10},{110,10}}),
+        iconTransformation(extent={{90,-10},{110,10}})));
+  Connection3to3Ground_n connection3to4
+    "Adapter between Termina3 and Terminal4"
+    annotation (Placement(transformation(extent={{-40,-10},{-60,10}})));
+  AixLib.Electrical.AC.OnePhase.Basics.Ground ground "Ground reference"
+    annotation (Placement(transformation(extent={{-30,-40},{-10,-20}})));
+equation
+  connect(wye, connection3to4.terminal3)
+    annotation (Line(points={{-100,0},{-60,0}},         color={0,120,120}));
+  connect(connection3to4.terminal4, wyeg) annotation (Line(points={{-40,0},{28,0},
+          {100,0}},           color={0,120,120}));
+  connect(connection3to4.ground4, ground.terminal) annotation (Line(points={{-40.6,
+          -6},{-20,-6},{-20,-20}}, color={0,120,120}));
+  annotation (
+  defaultComponentName="y2yg",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+        Line(
+          points={{0,40},{0,0},{-30,-30}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{0,0},{30,-30}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{0,0},{0,-40}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.25),
+        Line(
+          points={{-8,-40},{8,-40}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.25),
+        Line(
+          points={{-6,-42},{6,-42}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.25),
+        Line(
+          points={{-4,-44},{4,-44}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.25)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Replaced <code>connection3to4</code> with new model.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 5, 2014, by Marco Bonvini:<br/>
+Added model.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Adapter from wye (Y) to wye grounded (Yg) connector.
+A three-phase unbalanced connector has three AC single phase
+connectors. Each AC single phase connector contains a the phase voltage,
+which is measured
+between the phase and the neutral. This model assures that the voltage of the neutral
+cable is equal to zero.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WyeToWyeGround;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/package.mo
new file mode 100644
index 0000000000..358e8aec0b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/package.mo
@@ -0,0 +1,22 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced;
+package Interfaces "Package with interfaces for three-phase unbalanced AC models"
+  extends Modelica.Icons.InterfacesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains connectors that are used by the models in the
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced\">AixLib.Electrical.AC.ThreePhasesUnbalanced</a> package.
+The connectors extends the basic connectors
+<a href=\"modelica://AixLib.Electrical.Interfaces.Terminal\">AixLib.Electrical.Interfaces.Terminal</a>
+and define a new graphical icon in order to be distinguished by connectors of other electrical systems (e.g. DC systems).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end Interfaces;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/package.order
new file mode 100644
index 0000000000..bc33a34500
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Interfaces/package.order
@@ -0,0 +1,14 @@
+Adapter3to3
+Connection3to3Ground_n
+Connection3to3Ground_p
+Connection3to4_n
+Connection3to4_p
+Terminal4_n
+Terminal4_p
+Terminal_n
+Terminal_p
+TwoPort
+TwoPort_N
+WyeToDelta
+WyeToWyeGround
+Examples
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine.mo
new file mode 100644
index 0000000000..e8f27e6429
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine.mo
@@ -0,0 +1,117 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine
+  "Test model for a three-phase unbalanced commercial cable without neutral"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage E(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+  Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{22,20},{42,40}})));
+  Loads.Impedance R2(R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{22,-10},{42,10}})));
+  Loads.Impedance R3(R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{22,-50},{42,-30}})));
+  Line line_1(
+    l=1000,
+    P_nominal=2000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 1"
+    annotation (Placement(transformation(extent={{-38,20},{-18,40}})));
+  Line line_2a(
+    l=500,
+    P_nominal=2000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 2"
+    annotation (Placement(transformation(extent={{-38,-10},{-18,10}})));
+  Line line_2b(
+    l=500,
+    P_nominal=2000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 2"
+    annotation (Placement(transformation(extent={{-14,-10},{6,10}})));
+  Line line_3a(
+    l=2000,
+    P_nominal=1000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 3"
+    annotation (Placement(transformation(extent={{-38,-40},{-18,-20}})));
+  Line line_3b(
+    l=2000,
+    P_nominal=1000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 3"
+    annotation (Placement(transformation(extent={{-38,-60},{-18,-40}})));
+equation
+  connect(E.terminal, line_1.terminal_n) annotation (Line(
+      points={{-60,0},{-50,0},{-50,30},{-38,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-18,30},{22,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_2a.terminal_n) annotation (Line(
+      points={{-60,0},{-50,0},{-50,6.66134e-16},{-38,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_2a.terminal_p, line_2b.terminal_n) annotation (Line(
+      points={{-18,0},{-14,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{6,0},{22,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3a.terminal_n) annotation (Line(
+      points={{-60,0},{-50,0},{-50,-30},{-38,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3b.terminal_n) annotation (Line(
+      points={{-60,0},{-50,0},{-50,-50},{-38,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-18,-30},{2,-30},{2,-40},{22,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-18,-50},{2,-50},{2,-40},{22,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine.mos"
+        "Simulate and plot"),
+ Documentation(info="<html>
+<p>
+This example demonstrates how to use a cable model without neutral line
+to connect a source to a load.
+</p>
+<p>
+The model has three resistive loads <code>R1</code>, <code>R2</code>, and <code>R3</code>.
+Each load is connected to the source with different configurations,
+but the equivalent resistance between each load and the source is the same.
+Since the equivalent resistances are the same, each load draws the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL.mo
new file mode 100644
index 0000000000..0eb2bba4d3
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL.mo
@@ -0,0 +1,120 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLineMatrix_RL
+  "Test model for a three-phase unbalanced inductive-resistive line specified by a Z matrix"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage E(
+    definiteReference=true,
+    f=60,
+    V=100*sqrt(3)) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance sc_load1(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  Loads.Impedance sc_load2(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  Loads.Impedance sc_load3(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,-50},{20,-30}})));
+  Lines.TwoPortMatrixRL Rline_1(
+    Z11={10,10},
+    Z12={0,0},
+    Z13={0,0},
+    Z22={10,10},
+    Z23={0,0},
+    Z33={10,10},
+    V_nominal=100*sqrt(3)) "RL line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Lines.TwoPortMatrixRL Rline_2a(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    Z11=0.5*{10,10},
+    Z22=0.5*{10,10},
+    Z33=0.5*{10,10},
+    V_nominal=100*sqrt(3)) "RL line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+  Lines.TwoPortMatrixRL Rline_2b(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    Z11=0.5*{10,10},
+    Z22=0.5*{10,10},
+    Z33=0.5*{10,10},
+    V_nominal=100*sqrt(3)) "RL line that connects to load 2"
+    annotation (Placement(transformation(extent={{-36,-10},{-16,10}})));
+  Lines.TwoPortMatrixRL Rline_3a(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    Z11=2*{10,10},
+    Z22=2*{10,10},
+    Z33=2*{10,10},
+    V_nominal=100*sqrt(3)) "RL line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+  Lines.TwoPortMatrixRL Rline_3b(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    Z11=2*{10,10},
+    Z22=2*{10,10},
+    Z33=2*{10,10},
+    V_nominal=100*sqrt(3)) "RL line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+equation
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, sc_load1.terminal) annotation (Line(
+      points={{-40,30},{0,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,6.66134e-16},{-60,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2a.terminal_p, Rline_2b.terminal_n) annotation (Line(
+      points={{-40,0},{-36,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2b.terminal_p, sc_load2.terminal) annotation (Line(
+      points={{-16,0},{-4.44089e-16,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-30},{-60,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3a.terminal_p, sc_load3.terminal) annotation (Line(
+      points={{-40,-30},{-20,-30},{-20,-40},{0,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3b.terminal_p, sc_load3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-40},{0,-40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use an inductive resistive line model to connect
+a source to a load. The model is parameterized using the impedance matrix <i>Z</i>.
+</p>
+<p>
+The model has three loads. The loads represent a short circuit <i>R=0</i>.
+The current that flows through the load depends on the resistance of the line.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLineMatrix_RL;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC.mo
new file mode 100644
index 0000000000..50c516e464
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC.mo
@@ -0,0 +1,79 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLineMatrix_RLC
+  "Test model for a three-phase unbalanced RLC line specified by Z and B matrices"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage E(
+    definiteReference=true,
+    f=60,
+    V=100*sqrt(3)) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance sc_load1(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  Lines.TwoPortMatrixRLC Rline_1(
+    Z11={10,10},
+    Z12={0,0},
+    Z13={0,0},
+    Z22={10,10},
+    Z23={0,0},
+    Z33={10,10},
+    V_nominal=100*sqrt(3),
+    B12=0,
+    B13=0,
+    B23=0,
+    B11=10,
+    B22=10,
+    B33=10) "RL line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Lines.TwoPortMatrixRLC Rline_2(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    V_nominal=100*sqrt(3),
+    B12=0,
+    B13=0,
+    B23=0,
+    Z11={0,0},
+    Z22={0,0},
+    Z33={0,0},
+    B11=0.1,
+    B22=0.1,
+    B33=0.1) "RL line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+equation
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, sc_load1.terminal) annotation (Line(
+      points={{-40,30},{0,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,6.66134e-16},{-60,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a RLC line model to connect
+a source to a load. The model is parameterized using the impedance matrix Z
+and the admittance matrix B.
+</p>
+<p>
+The example shows two configurations to test a zero and non-zero matrix <i>B</i>.
+In the second case the impedance matrix <i>Z</i> has been set to zero.
+Therefore, the line model does not have a load connected to it.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLineMatrix_RLC;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC_N.mo
new file mode 100644
index 0000000000..15a9efe470
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC_N.mo
@@ -0,0 +1,95 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLineMatrix_RLC_N
+  "Test model for a three-phase unbalanced RLC line with neutral cable specified by Z and B matrices"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage_N E(
+    definiteReference=true,
+    f=60,
+    V=100*sqrt(3)) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance_N sc_load1(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  Lines.TwoPortMatrixRLC_N Rline_1(
+    Z11={10,10},
+    Z12={0,0},
+    Z13={0,0},
+    Z22={10,10},
+    Z23={0,0},
+    Z33={10,10},
+    V_nominal=100*sqrt(3),
+    B12=0,
+    B13=0,
+    B23=0,
+    B11=10,
+    B22=10,
+    B33=10,
+    Z14={0,0},
+    Z24={0,0},
+    Z34={0,0},
+    Z44={10,10},
+    B14=0,
+    B24=0,
+    B34=0,
+    B44=10) "RL line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Lines.TwoPortMatrixRLC_N Rline_2(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    V_nominal=100*sqrt(3),
+    B12=0,
+    B13=0,
+    B23=0,
+    Z11={0,0},
+    Z22={0,0},
+    Z33={0,0},
+    B11=0.1,
+    B22=0.1,
+    B33=0.1,
+    Z14={0,0},
+    Z24={0,0},
+    B14=0,
+    B24=0,
+    B34=0,
+    B44=0.1,
+    Z34={0,0},
+    Z44={0,0}) "RL line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+equation
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2.terminal_n) annotation (Line(
+      points={{-80,0},{-60,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, sc_load1.terminal) annotation (Line(
+      points={{-40,30},{0,30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC_N.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a RLC line model with neutral line to connect
+a source to a load. The model is parameterized using the impedance matrix Z
+and the admittance matrix B.
+</p>
+<p>
+The example shows two configurations to test a zero and non-zero matrix <i>B</i>.
+In the second case the impedance matrix <i>Z</i> has been set to zero.
+Therefore, the line model does not have a load connected to it.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLineMatrix_RLC_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL_N.mo
new file mode 100644
index 0000000000..5bf773731f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL_N.mo
@@ -0,0 +1,140 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLineMatrix_RL_N
+  "Test model for a three-phase unbalanced inductive-resistive line with neutral cable specified by a Z matrix"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage_N E(
+    definiteReference=true,
+    f=60,
+    V=100*sqrt(3)) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance_N sc_load1(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  Loads.Impedance_N sc_load2(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  Loads.Impedance_N sc_load3(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,-50},{20,-30}})));
+  Lines.TwoPortMatrixRL_N Rline_1(
+    Z11={10,10},
+    Z12={0,0},
+    Z13={0,0},
+    Z22={10,10},
+    Z23={0,0},
+    Z33={10,10},
+    V_nominal=100*sqrt(3),
+    Z14={0,0},
+    Z24={0,0},
+    Z34={0,0},
+    Z44={10,10}) "RL line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Lines.TwoPortMatrixRL_N Rline_2a(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    Z11=0.5*{10,10},
+    Z22=0.5*{10,10},
+    Z33=0.5*{10,10},
+    V_nominal=100*sqrt(3),
+    Z14={0,0},
+    Z24={0,0},
+    Z34={0,0},
+    Z44=0.5*{10,10}) "RL line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+  Lines.TwoPortMatrixRL_N Rline_2b(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    Z11=0.5*{10,10},
+    Z22=0.5*{10,10},
+    Z33=0.5*{10,10},
+    V_nominal=100*sqrt(3),
+    Z14={0,0},
+    Z24={0,0},
+    Z34={0,0},
+    Z44=0.5*{10,10}) "RL line that connects to load 2"
+    annotation (Placement(transformation(extent={{-32,-10},{-12,10}})));
+  Lines.TwoPortMatrixRL_N Rline_3a(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    Z11=2*{10,10},
+    Z22=2*{10,10},
+    Z33=2*{10,10},
+    V_nominal=100*sqrt(3),
+    Z14={0,0},
+    Z24={0,0},
+    Z34={0,0},
+    Z44=2*{10,10}) "RL line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+  Lines.TwoPortMatrixRL_N Rline_3b(
+    Z12={0,0},
+    Z13={0,0},
+    Z23={0,0},
+    Z11=2*{10,10},
+    Z22=2*{10,10},
+    Z33=2*{10,10},
+    V_nominal=100*sqrt(3),
+    Z14={0,0},
+    Z24={0,0},
+    Z34={0,0},
+    Z44=2*{10,10}) "RL line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+equation
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-60,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-30},{-60,-30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_3b.terminal_p, sc_load3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-40},{0,-40}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_3a.terminal_p, sc_load3.terminal) annotation (Line(
+      points={{-40,-30},{-20,-30},{-20,-40},{0,-40}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_2b.terminal_p, sc_load2.terminal) annotation (Line(
+      points={{-12,0},{0,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, sc_load1.terminal) annotation (Line(
+      points={{-40,30},{0,30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_2a.terminal_p, Rline_2b.terminal_n) annotation (Line(
+      points={{-40,0},{-32,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL_N.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use an inductive resistive line model with neutral line to connect
+a source to a load. The model is parameterized using the impedance matrix <i>Z</i>.
+</p>
+<p>
+The model has three loads. The loads represent a short circuit <i>R=0</i>.
+The current that flows through the load depends on the resistance of the line.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLineMatrix_RL_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L.mo
new file mode 100644
index 0000000000..566250d5ce
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L.mo
@@ -0,0 +1,111 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_L "Test model for a three-phase unbalanced inductive line"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Inductance Lbase=10/2/Modelica.Constants.pi/60
+    "Base value for the line inductances";
+  Sources.FixedVoltage E(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance L1(R=0, L=Lbase) "Inductive load 1"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Loads.Impedance L2(R=0, L=Lbase) "Inductive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Loads.Impedance L3(R=0, L=Lbase) "Inductive load 3"
+    annotation (Placement(transformation(extent={{0,-70},{20,-50}})));
+  Loads.Impedance sc_load(R=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  Lines.TwoPortInductance Lline_sc(L=6*Lbase)
+    "Inductive line that connects to the short circuit"
+    annotation (Placement(transformation(extent={{-60,60},{-40,40}})));
+  Lines.TwoPortInductance Rline_1(L=3*Lbase)
+    "Inductive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  Lines.TwoPortInductance Rline_2a(L=3*Lbase/2)
+    "Inductive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  Lines.TwoPortInductance Rline_2b(L=3*Lbase/2)
+    "Inductive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-36,-30},{-16,-10}})));
+  Lines.TwoPortInductance Rline_3a(L=6*Lbase)
+    "Inductive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  Lines.TwoPortInductance Rline_3b(L=6*Lbase)
+    "Inductive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+equation
+  connect(E.terminal,Lline_sc. terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Lline_sc.terminal_p, sc_load.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p,L1. terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2a.terminal_p, Rline_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-36,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2b.terminal_p,L2. terminal) annotation (Line(
+      points={{-16,-20},{-4.44089e-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-70},{-60,-70}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3a.terminal_p,L3. terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3b.terminal_p,L3. terminal) annotation (Line(
+      points={{-40,-70},{-20,-70},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a purely inductive line model to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the resistance of the line.
+</p>
+<p>
+The remaining three loads <code>L1</code>, <code>L2</code>, and <code>L3</code>
+are inductive loads. Each load is connected to the source with different configurations,
+but the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draws the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_L;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L_N.mo
new file mode 100644
index 0000000000..7c24d62a53
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L_N.mo
@@ -0,0 +1,112 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_L_N
+  "Test model for a three-phase unbalanced inductive line with neutral cable"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Inductance Lbase=10/2/Modelica.Constants.pi/60
+    "Base value for the line inductances";
+  Sources.FixedVoltage_N E(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance_N L1(R=0, L=Lbase) "Inductive load 1"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Loads.Impedance_N L2(R=0, L=Lbase) "Inductive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Loads.Impedance_N L3(R=0, L=Lbase) "Inductive load 3"
+    annotation (Placement(transformation(extent={{0,-70},{20,-50}})));
+  Loads.Impedance_N sc_load(R=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  Lines.TwoPortInductance_N Lline_sc(L=6*Lbase, Ln=Lbase)
+    "Inductive line that connects to the short circuit"
+    annotation (Placement(transformation(extent={{-60,60},{-40,40}})));
+  Lines.TwoPortInductance_N Rline_1(L=3*Lbase, Ln=0.5*Lbase)
+    "Inductive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  Lines.TwoPortInductance_N Rline_2a(L=3*Lbase/2, Ln=0.5*Lbase/2)
+    "Inductive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  Lines.TwoPortInductance_N Rline_2b(L=3*Lbase/2, Ln=0.5*Lbase/2)
+    "Inductive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-32,-30},{-12,-10}})));
+  Lines.TwoPortInductance_N Rline_3a(L=6*Lbase, Ln=Lbase)
+    "Inductive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  Lines.TwoPortInductance_N Rline_3b(L=6*Lbase, Ln=Lbase)
+    "Inductive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+equation
+  connect(E.terminal, Lline_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-70},{-60,-70}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_3b.terminal_p, L3.terminal) annotation (Line(
+      points={{-40,-70},{-20,-70},{-20,-60},{0,-60}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_3a.terminal_p, L3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-60},{0,-60}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_2b.terminal_p, L2.terminal) annotation (Line(
+      points={{-12,-20},{0,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_2a.terminal_p, Rline_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-32,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, L1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Lline_sc.terminal_p, sc_load.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L_N.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a purely inductive line model with neutral cable to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the resistance of the line.
+</p>
+<p>
+The remaining three loads <code>L1</code>, <code>L2</code>, and <code>L3</code>
+are inductive loads. Each load is connected to the source with different configurations,
+but the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draws the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_L_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_N.mo
new file mode 100644
index 0000000000..7c868f36f4
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_N.mo
@@ -0,0 +1,117 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_N
+  "Test model for a three-phase unbalanced commercial cable with neutral"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage_N E(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+  Loads.Impedance_N R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{22,20},{42,40}})));
+  Loads.Impedance_N R2(R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{22,-10},{42,10}})));
+  Loads.Impedance_N R3(R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{22,-50},{42,-30}})));
+  Line_N line_1(
+    l=1000,
+    P_nominal=2000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 1"
+    annotation (Placement(transformation(extent={{-38,20},{-18,40}})));
+  Line_N line_2a(
+    l=500,
+    P_nominal=2000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 2"
+    annotation (Placement(transformation(extent={{-44,-10},{-24,10}})));
+  Line_N line_2b(
+    l=500,
+    P_nominal=2000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 2"
+    annotation (Placement(transformation(extent={{-14,-10},{6,10}})));
+  Line_N line_3a(
+    l=2000,
+    P_nominal=1000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 3"
+    annotation (Placement(transformation(extent={{-38,-40},{-18,-20}})));
+  Line_N line_3b(
+    l=2000,
+    P_nominal=1000,
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu35
+      commercialCable) "Cable that connects to load 3"
+    annotation (Placement(transformation(extent={{-38,-60},{-18,-40}})));
+equation
+  connect(E.terminal, line_2a.terminal_n) annotation (Line(
+      points={{-60,0},{-44,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, line_1.terminal_n) annotation (Line(
+      points={{-60,0},{-50,0},{-50,30},{-38,30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(line_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-18,30},{22,30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3a.terminal_n) annotation (Line(
+      points={{-60,0},{-50,0},{-50,-30},{-38,-30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, line_3b.terminal_n) annotation (Line(
+      points={{-60,4.44089e-16},{-50,4.44089e-16},{-50,-50},{-38,-50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(line_2a.terminal_p, line_2b.terminal_n) annotation (Line(
+      points={{-24,0},{-14,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(line_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-18,-30},{2,-30},{2,-40},{22,-40}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(line_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-18,-50},{2,-50},{2,-40},{22,-40}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(line_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{6,0},{22,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_N.mos"
+        "Simulate and plot"),
+ Documentation(info="<html>
+<p>
+This example demonstrates how to use a cable line model with
+neutral to connect a source to a load.
+</p>
+<p>
+The model has three resistive loads <code>R1</code>, <code>R2</code>, and <code>R3</code>.
+Each load is connected to the source with different configurations,
+but the equivalent resistance between each load and the source is the same.
+Since the equivalent resistances are the same, each load draws the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R.mo
new file mode 100644
index 0000000000..6ce2af0ce2
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R.mo
@@ -0,0 +1,109 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_R "Test model for a three-phase unbalanced resistive line"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage E(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Loads.Impedance R2(R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Loads.Impedance R3(R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-70},{20,-50}})));
+  Loads.Impedance sc_load(R=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  Lines.TwoPortResistance Rline_sc(      useHeatPort=false, R=60)
+    "Resistive line that connects to the short circuit"
+    annotation (Placement(transformation(extent={{-60,60},{-40,40}})));
+  Lines.TwoPortResistance Rline_1(R=30)
+    "Resistive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  Lines.TwoPortResistance Rline_2a(R=15)
+    "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  Lines.TwoPortResistance Rline_2b(R=15)
+    "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-36,-30},{-16,-10}})));
+  Lines.TwoPortResistance Rline_3a(R=60)
+    "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  Lines.TwoPortResistance Rline_3b(R=60)
+    "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+equation
+  connect(E.terminal, Rline_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_sc.terminal_p, sc_load.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2a.terminal_p, Rline_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-36,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-16,-20},{-4.44089e-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-70},{-60,-70}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(Rline_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-70},{-20,-70},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a resistive line model to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the resistance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations,
+but the equivalent resistance between each load and the source is the same.
+Since the equivalent resistances are the same, each load draws the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_R;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL.mo
new file mode 100644
index 0000000000..58ad8cb6fb
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL.mo
@@ -0,0 +1,98 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_RL
+  "Test model for a three-phase unbalanced inductive-resistive line"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Resistance Rbase=3*10
+    "Base value for the line resistance";
+  parameter Modelica.Units.SI.Inductance Lbase=Rbase/2/Modelica.Constants.pi/60
+    "Base value for the line inductance";
+  Sources.FixedVoltage E(
+    definiteReference=true,
+    f=60,
+    V=100*sqrt(3)) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance load_sc_1(R=0) "Short circuit 1"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  Loads.Impedance load_sc_2(R=0) "Short circuit 2"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  Lines.TwoPortRL RL_2(
+    R=Rbase,
+    L=Lbase) "Resistive-Inductive line connected to short circuit 2"
+    annotation (Placement(transformation(extent={{-48,-10},{-28,10}})));
+  Lines.TwoPortResistance R_1(R=Rbase)
+    "Resistance line connected to short circuit 1"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Lines.TwoPortInductance L_1(L=Lbase)
+    "Inductance line connected to short circuit 1"
+    annotation (Placement(transformation(extent={{-30,20},{-10,40}})));
+  Lines.TwoPortRL RL_3(
+    R=Rbase,
+    L=Lbase,
+    mode=AixLib.Electrical.Types.Load.FixedZ_dynamic)
+    "Dynamic resistive-inductive line connected to short circuit 3"
+    annotation (Placement(transformation(extent={{-48,-40},{-28,-20}})));
+  Loads.Impedance load_sc_3(R=0) "Short circuit 3"
+    annotation (Placement(transformation(extent={{0,-40},{20,-20}})));
+equation
+  connect(E.terminal, R_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(R_1.terminal_p, L_1.terminal_n) annotation (Line(
+      points={{-40,30},{-30,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(L_1.terminal_p, load_sc_1.terminal) annotation (Line(
+      points={{-10,30},{0,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RL_2.terminal_n) annotation (Line(
+      points={{-80,0},{-48,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RL_2.terminal_p, load_sc_2.terminal) annotation (Line(
+      points={{-28,0},{0,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RL_3.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-30},{-48,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RL_3.terminal_p, load_sc_3.terminal) annotation (Line(
+      points={{-28,-30},{0,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (  experiment(StopTime=1.0,Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+August 24, 2014, by Marco Bonvini:<br/>
+Documentation and example revised.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a resistive-inductive line model to connect
+a source to a load.
+</p>
+<p>
+The model has three loads <code>load_sc_1</code>, <code>load_sc_2</code>,
+and <code>load_sc_3</code> representing short circuits <i>R=0</i>.
+The current that flows through the load depends on the impedance of the line.
+</p>
+<p>
+Each load is connected to the source with different configurations,
+but the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draw the same current.
+</p>
+<p>
+<b>Note:</b>
+The line model <code>RL_3</code> is the same as <code>RL_2</code> but it uses
+dynamic phasors.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_RL;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC.mo
new file mode 100644
index 0000000000..696084a02d
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC.mo
@@ -0,0 +1,171 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_RLC "Test model for a three-phase unbalanced RLC line"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Resistance RBase=3*10
+    "Base value for the line resistance";
+  parameter Modelica.Units.SI.Inductance LBase=RBase/(2*Modelica.Constants.pi*
+      60) "Base value for the line inductances";
+  parameter Modelica.Units.SI.Capacitance CBase=3*0.1/(2*Modelica.Constants.pi*
+      60) "Base value for the line inductances";
+  Sources.FixedVoltage E(
+    definiteReference=true,
+    f=60,
+    V=100*sqrt(3)) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance sc_load1(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Loads.Impedance sc_load2(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Loads.Impedance sc_load3(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,-70},{20,-50}})));
+  Loads.Impedance sc_load(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  Lines.TwoPortRLC RLCLine_sc(
+    R=RBase,
+    C=CBase,
+    L=LBase,
+    mode=AixLib.Electrical.Types.Load.FixedZ_dynamic,
+    V_nominal=480) "RLC line that connects to the short circuit"
+    annotation (Placement(transformation(extent={{-60,60},{-40,40}})));
+  Lines.TwoPortRLC RLCLine_1(
+    R=RBase,
+    C=CBase,
+    L=LBase,
+    V_nominal=480) "RLC line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  Lines.TwoPortRLC RLCLine_2a(
+    V_nominal=480,
+    R=RBase/2,
+    L=LBase/2,
+    C=CBase/2) "RLC line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  Lines.TwoPortRLC RLCLine_2b(
+    V_nominal=480,
+    R=RBase/2,
+    L=LBase/2,
+    C=CBase/2) "RLC line that connects to load 2"
+    annotation (Placement(transformation(extent={{-30,-30},{-10,-10}})));
+  Lines.TwoPortRLC RLCLine_3a(
+    R=2*RBase,
+    L=2*LBase,
+    V_nominal=480,
+    C=CBase/2) "RLC line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  Lines.TwoPortRLC RLCLine_3b(
+    R=2*RBase,
+    L=2*LBase,
+    V_nominal=480,
+    C=CBase/2) "RLC line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+equation
+  connect(E.terminal, RLCLine_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RLCLine_sc.terminal_p, sc_load.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RLCLine_1.terminal_p, sc_load1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RLCLine_2a.terminal_p, RLCLine_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-30,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RLCLine_2b.terminal_p, sc_load2.terminal) annotation (Line(
+      points={{-10,-20},{-4.44089e-16,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-70},{-60,-70}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RLCLine_3a.terminal_p, sc_load3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(RLCLine_3b.terminal_p, sc_load3.terminal) annotation (Line(
+      points={{-40,-70},{-20,-70},{-20,-60},{0,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (  experiment(StopTime=1.0,Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use an RLC line model to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The loads <code>sc_load</code>,
+<code>sc_load1</code>, <code>sc_load2</code>, <code>sc_load3</code> represent
+short circuits <i>R=0</i>. The current that flows through the load depends
+on the resistance, inductance and capacitance of the line.
+</p>
+<p>
+The parameter <i>R</i>, <i>L</i> and <i>C</i> are such that at the nominal
+frequency <i>f<sub>nom</sub> = 60 Hz</i> the respective resistance and
+reactances are all equal to 10 &Omega;.
+</p>
+<p>
+The lines used in this example have a T model (see
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortRLC\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortRLC</a>).
+The equivalent impedance of the line on each phase is equal to
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Z<sub>EQ</sub> = R/2 +jX<sub>L</sub>/2 + (R/2 +jX<sub>L</sub>/2)(-jX<sub>C</sub>)/
+(R/2 +jX<sub>L</sub>/2 -jX<sub>C</sub>)
+</p>
+<p>
+that in this case is equal to <i>Z<sub>EQ</sub> = 15 + j5 </i> &Omega;.
+</p>
+<p>
+Given the equivalent impedance of each phase, and a voltage
+with an RMS value of 100 V produces a current equal to
+<i>I = 6 - j2 </i> A flowing through phase 1.
+</p>
+<h4>Notes</h4>
+<p>
+<b>(1) Note:</b>
+The line model <code>RLCLine_sc</code> is the same as <code>RLCLine_1</code> but it uses
+dynamic phasors.
+</p>
+
+<p>
+<b>(2) Note:</b>
+The line model <code>RLCLine_2a</code> has a current that is different
+from the one passing in <code>RLCLine_1</code> because the series of two T
+line models is different from the sum of the two separate line models.
+</p>
+
+<p>
+<b>(3) Note:</b>
+The line models <code>RLCLine_3a</code> and <code>RLCLine_3b</code> have currents that are
+50% of the other lines because they are in parallel.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_RLC;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC_N.mo
new file mode 100644
index 0000000000..4636734eb8
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC_N.mo
@@ -0,0 +1,190 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_RLC_N
+  "Test model for a three-phase unbalanced RLC line with neutral cable"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Resistance RBase=3*10
+    "Base value for the line resistance";
+  parameter Modelica.Units.SI.Inductance LBase=RBase/(2*Modelica.Constants.pi*
+      60) "Base value for the line inductances";
+  parameter Modelica.Units.SI.Capacitance CBase=3*0.1/(2*Modelica.Constants.pi*
+      60) "Base value for the line inductances";
+  Sources.FixedVoltage_N E(
+    definiteReference=true,
+    f=60,
+    V=100*sqrt(3)) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance_N sc_load1(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Loads.Impedance_N sc_load2(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Loads.Impedance_N sc_load3(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,-70},{20,-50}})));
+  Loads.Impedance_N sc_load(R=0, L=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  Lines.TwoPortRLC_N RLCLine_sc(
+    R=RBase,
+    C=CBase,
+    L=LBase,
+    mode=AixLib.Electrical.Types.Load.FixedZ_dynamic,
+    V_nominal=480,
+    Rn=RBase,
+    Cn=CBase,
+    Ln=LBase) "RLC line that connects to the short circuit"
+    annotation (Placement(transformation(extent={{-60,60},{-40,40}})));
+  Lines.TwoPortRLC_N RLCLine_1(
+    R=RBase,
+    C=CBase,
+    L=LBase,
+    V_nominal=480,
+    Rn=RBase,
+    Cn=CBase,
+    Ln=LBase) "RLC line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  Lines.TwoPortRLC_N RLCLine_2a(
+    V_nominal=480,
+    R=RBase/2,
+    L=LBase/2,
+    C=CBase/2,
+    Rn=RBase/2,
+    Cn=CBase/2,
+    Ln=LBase/2) "RLC line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  Lines.TwoPortRLC_N RLCLine_2b(
+    V_nominal=480,
+    R=RBase/2,
+    L=LBase/2,
+    C=CBase/2,
+    Rn=RBase/2,
+    Cn=CBase/2,
+    Ln=LBase/2) "RLC line that connects to load 2"
+    annotation (Placement(transformation(extent={{-30,-30},{-10,-10}})));
+  Lines.TwoPortRLC_N RLCLine_3a(
+    R=2*RBase,
+    L=2*LBase,
+    V_nominal=480,
+    C=CBase/2,
+    Rn=2*RBase,
+    Cn=CBase/2,
+    Ln=2*LBase) "RLC line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  Lines.TwoPortRLC_N RLCLine_3b(
+    R=2*RBase,
+    L=2*LBase,
+    V_nominal=480,
+    C=CBase/2,
+    Rn=2*RBase,
+    Cn=CBase/2,
+    Ln=2*LBase) "RLC line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+equation
+  connect(RLCLine_2a.terminal_p, RLCLine_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-30,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(RLCLine_2b.terminal_p, sc_load2.terminal) annotation (Line(
+      points={{-10,-20},{0,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(RLCLine_3a.terminal_p, sc_load3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-60},{0,-60}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(RLCLine_3b.terminal_p, sc_load3.terminal) annotation (Line(
+      points={{-40,-70},{-20,-70},{-20,-60},{0,-60}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(RLCLine_1.terminal_p, sc_load1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(RLCLine_sc.terminal_p, sc_load.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, RLCLine_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-70},{-60,-70}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (  experiment(StopTime=1.0,Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC_N.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use an RLC line model with neutral cable to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The loads <code>sc_load</code>,
+<code>sc_load1</code>, <code>sc_load2</code>, <code>sc_load3</code> represent
+short circuits <i>R=0</i>. The current that flows through the load depends
+on the resistance, inductance and capacitance of the line.
+</p>
+<p>
+The parameter <i>R</i>, <i>L</i> and <i>C</i> are such that at the nominal
+frequency <i>f<sub>nom</sub> = 60 Hz</i> the respective resistance and
+reactances are all equal to 10 &Omega;.
+</p>
+<p>
+The lines used in this example have a T model (see
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortRLC\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortRLC</a>).
+The equivalent impedance of the line on each phase is equal to
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Z<sub>EQ</sub> = R/2 +jX<sub>L</sub>/2 + (R/2 +jX<sub>L</sub>/2)(-jX<sub>C</sub>)/
+(R/2 +jX<sub>L</sub>/2 -jX<sub>C</sub>)
+</p>
+<p>
+that in this case is equal to <i>Z<sub>EQ</sub> = 15 + j5 </i> &Omega;.
+</p>
+<p>
+Given the equivalent impedance of each phase, and a voltage
+with an RMS value of 100 V produces a current equal to
+<i>I = 6 - j2 </i> A flowing through phase 1.
+</p>
+<h4>Notes</h4>
+<p>
+<b>(1) Note:</b>
+The line model <code>RLCLine_sc</code> is the same as <code>RLCLine_1</code> but it uses
+dynamic phasors.
+</p>
+
+<p>
+<b>(2) Note:</b>
+The line model <code>RLCLine_2a</code> has a current that is different
+from the one passing in <code>RLCLine_1</code> because the series of two T
+line models is different from the sum of the two separate line models.
+</p>
+
+<p>
+<b>(3) Note:</b>
+The line models <code>RLCLine_3a</code> and <code>RLCLine_3b</code> have currents that are
+50% of the other lines because they are in parallel.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_RLC_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL_N.mo
new file mode 100644
index 0000000000..dc8fdf0eb0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL_N.mo
@@ -0,0 +1,88 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_RL_N
+  "Test model for a three-phase unbalanced inductive-resistive line with neutral cable"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Resistance Rbase=3*10
+    "Base value for the line resistance";
+  parameter Modelica.Units.SI.Inductance Lbase=Rbase/2/Modelica.Constants.pi/60
+    "Base value for the line inductance";
+  Sources.FixedVoltage_N E(
+    definiteReference=true,
+    f=60,
+    V=100*sqrt(3)) "Voltage source"
+    annotation (Placement(transformation(extent={{-96,-10},{-76,10}})));
+  Loads.Impedance_N load_sc_1(R=0) "Short circuit 1"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  Loads.Impedance_N load_sc_2(R=0) "Short circuit 2"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  Lines.TwoPortRL_N RL_2(
+    R=Rbase,
+    L=Lbase,
+    Rn=0.5*Rbase,
+    Ln=0.5*Lbase) "Resistive-Inductive line connected to short circuit 2"
+    annotation (Placement(transformation(extent={{-48,-10},{-28,10}})));
+  Lines.TwoPortResistance_N R_1(R=Rbase, Rn=0.5*Rbase)
+    "Resistance line connected to short circuit 1"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Lines.TwoPortInductance_N L_1(L=Lbase, Ln=0.5*Lbase)
+    "Inductance line connected to short circuit 1"
+    annotation (Placement(transformation(extent={{-30,20},{-10,40}})));
+equation
+  connect(RL_2.terminal_p, load_sc_2.terminal) annotation (Line(
+      points={{-28,0},{0,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(L_1.terminal_p, load_sc_1.terminal) annotation (Line(
+      points={{-10,30},{0,30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(L_1.terminal_n, R_1.terminal_p) annotation (Line(
+      points={{-30,30},{-40,30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(R_1.terminal_n, E.terminal) annotation (Line(
+      points={{-60,30},{-70,30},{-70,0},{-76,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, RL_2.terminal_n) annotation (Line(
+      points={{-76,0},{-48,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (  experiment(StopTime=1.0,Tolerance=1e-06),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL_N.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+March 20, 2015, by Michael Wetter:<br/>
+Removed dynamic load model as this caused divergence.
+(Dassault SR00259003.)
+</li>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added initial conditions for the dynamic load model.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a resistive-inductive line model with neutral cable to connect
+a source to a load.
+</p>
+<p>
+The model has two loads <code>load_sc_1</code> and <code>load_sc_2</code>
+representing short circuits <i>R=0</i>.
+The current that flows through the load depends on the impedance of the line.
+</p>
+<p>
+Each load is connected to the source with different configurations,
+but the equivalent impedance between each load and the source is the same.
+Since the equivalent impedances are the same, each load draw the same current.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_RL_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R_N.mo
new file mode 100644
index 0000000000..bd819e28e6
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R_N.mo
@@ -0,0 +1,110 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACLine_R_N
+  "Test model for a three-phase unbalanced resistive line with neutral cable"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage_N E(
+    definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Loads.Impedance_N R1(R=10) "Resistive load 1"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Loads.Impedance_N R2(R=10) "Resistive load 2"
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Loads.Impedance_N R3(R=10) "Resistive load 3"
+    annotation (Placement(transformation(extent={{0,-70},{20,-50}})));
+  Loads.Impedance_N sc_load(R=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  Lines.TwoPortResistance_N Rline_sc(      useHeatPort=false, R=60,
+    Rn=20) "Resistive line that connects to the short circuit"
+    annotation (Placement(transformation(extent={{-60,60},{-40,40}})));
+  Lines.TwoPortResistance_N Rline_1(R=30, Rn=10)
+    "Resistive line that connects to load 1"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  Lines.TwoPortResistance_N Rline_2a(R=15, Rn=5)
+    "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  Lines.TwoPortResistance_N Rline_2b(R=15, Rn=5)
+    "Resistive line that connects to load 2"
+    annotation (Placement(transformation(extent={{-32,-30},{-12,-10}})));
+  Lines.TwoPortResistance_N Rline_3a(R=60, Rn=20)
+    "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+  Lines.TwoPortResistance_N Rline_3b(R=60, Rn=20)
+    "Resistive line that connects to load 3"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+equation
+  connect(Rline_sc.terminal_p, sc_load.terminal) annotation (Line(
+      points={{-40,50},{0,50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_1.terminal_p, R1.terminal) annotation (Line(
+      points={{-40,10},{0,10}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_2b.terminal_p, R2.terminal) annotation (Line(
+      points={{-12,-20},{0,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_2a.terminal_p, Rline_2b.terminal_n) annotation (Line(
+      points={{-40,-20},{-32,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_3b.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-70},{-20,-70},{-20,-60},{0,-60}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(Rline_3a.terminal_p, R3.terminal) annotation (Line(
+      points={{-40,-50},{-20,-50},{-20,-60},{0,-60}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_sc.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,50},{-60,50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_1.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,10},{-60,10}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_2a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-20},{-60,-20}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3a.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-50},{-60,-50}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(E.terminal, Rline_3b.terminal_n) annotation (Line(
+      points={{-80,0},{-70,0},{-70,-70},{-60,-70}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R_N.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates how to use a resistive line model with neutral cable to connect
+a source to a load.
+</p>
+<p>
+The model has four different loads. The load <code>sc_load</code> represents
+a short circuit <i>R=0</i>. The current that flows through the load depends
+on the resistance of the line.
+</p>
+<p>
+The remaining three loads <code>R1</code>, <code>R2</code>, and <code>R3</code>
+are resistive loads. Each load is connected to the source with different configurations,
+but the equivalent resistance between each load and the source is the same.
+Since the equivalent resistances are the same, each load draws the same current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACLine_R_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid.mo
new file mode 100644
index 0000000000..d18a1f116f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid.mo
@@ -0,0 +1,80 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACSimpleGrid
+  "Test model for a network model for three-phase unbalanced systems without neutral cable"
+  extends Modelica.Icons.Example;
+  Network network(
+    redeclare AixLib.Electrical.Transmission.Grids.TestGrid2Nodes grid,
+    V_nominal=480)
+    "Network model that represents the connection between the source and the load"
+    annotation (Placement(transformation(extent={{20,-10},{0,10}})));
+  Loads.Inductive load(
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    plugPhase3=false) "Load connected to the network"
+    annotation (Placement(transformation(extent={{-34,10},{-54,30}})));
+  Sources.FixedVoltage E(f=60, V=480,
+    definiteReference=true) "Voltage source"           annotation (
+      Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={-50,-20})));
+  Modelica.Blocks.Sources.Ramp load_inputs(
+    height=5000,
+    offset=-2000,
+    duration=0.5,
+    startTime=0.25) "Input signal for the power consumption of the loads"
+    annotation (Placement(transformation(extent={{-90,10},{-70,30}})));
+equation
+  connect(E.terminal, network.terminal[1]) annotation (Line(
+      points={{-40,-20},{-20,-20},{-20,0},{0,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load.terminal, network.terminal[2]) annotation (Line(
+      points={{-34,20},{-20,20},{-20,0},{0,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load_inputs.y, load.Pow1) annotation (Line(
+      points={{-69,20},{-62,20},{-62,28},{-56,28}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load_inputs.y, load.Pow2) annotation (Line(
+      points={{-69,20},{-56,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid.mos"
+        "Simulate and plot"),
+Documentation(revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a network model to connect
+a source to a load. In this simple case the network has two nodes
+that are connected by a commercial cable without a neutral line.
+</p>
+<p>
+At the beginning of the simulation, the load consumes power while at the
+and it produces power. The voltage at the load at the beginning is lower
+than the nominal RMS voltage (480 V), while at the end of the simulation it is higher.
+The voltage drop and increase are due to the presence of the cable between
+the source and the load.
+</p>
+<p>
+The network uses cables of the type <code>LowVoltageCable.Cu35</code> with
+a length of <i>200</i> m.
+</p>
+<p>
+The picture below describes the grid topology.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/testGrid2Nodes.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACSimpleGrid;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid_N.mo
new file mode 100644
index 0000000000..d5d15333a0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid_N.mo
@@ -0,0 +1,83 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples;
+model ACSimpleGrid_N
+  "Test model for a network model for three-phase unbalanced systems with neutral cable"
+  extends Modelica.Icons.Example;
+  Network_N network(
+    redeclare AixLib.Electrical.Transmission.Grids.TestGrid2Nodes grid,
+    V_nominal=480)
+    "Network model that represents the connection between the source and the load"
+    annotation (Placement(transformation(extent={{20,-10},{0,10}})));
+  Loads.Inductive_N load(
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    plugPhase3=false) "Load connected to the network"
+    annotation (Placement(transformation(extent={{-34,10},{-54,30}})));
+  Sources.FixedVoltage_N E(
+    f=60,
+    V=480,
+    definiteReference=true) "Voltage source"
+    annotation (
+      Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={-50,-20})));
+  Modelica.Blocks.Sources.Ramp load_inputs(
+    height=5000,
+    offset=-2000,
+    duration=0.5,
+    startTime=0.25) "Input signal for the power consumption of the loads"
+    annotation (Placement(transformation(extent={{-90,10},{-70,30}})));
+equation
+  connect(E.terminal, network.terminal[1]) annotation (Line(
+      points={{-40,-20},{-20,-20},{-20,0},{0,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load.terminal, network.terminal[2]) annotation (Line(
+      points={{-34,20},{-20,20},{-20,0},{0,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load_inputs.y, load.Pow1) annotation (Line(
+      points={{-69,20},{-62,20},{-62,28},{-56,28}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load_inputs.y, load.Pow2) annotation (Line(
+      points={{-69,20},{-56,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid_N.mos"
+        "Simulate and plot"),
+Documentation(revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates how to use a network model to connect
+a source to a load. In this simple case the network has two nodes
+that are connected by a commercial cable with neutral line.
+</p>
+<p>
+At the beginning of the simulation the load consumes power while at the
+and it produces power. The voltage at the load at the beginning is lower
+than the nominal RMS voltage (480 V) while at the end of the simulation it is higher.
+The voltage drop and increase are due to the presence of the cable between
+the source and the load.
+</p>
+<p>
+The network uses cables of the type <code>LowVoltageCable.Cu35</code> with
+a length of <i>200</i> m.
+</p>
+<p>
+The picture below describes the grid topology.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/testGrid2Nodes.png\"/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ACSimpleGrid_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/package.mo
new file mode 100644
index 0000000000..9584307139
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+  annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/package.order
new file mode 100644
index 0000000000..a489517a6f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/package.order
@@ -0,0 +1,16 @@
+ACLine
+ACLineMatrix_RL
+ACLineMatrix_RLC
+ACLineMatrix_RLC_N
+ACLineMatrix_RL_N
+ACLine_L
+ACLine_L_N
+ACLine_N
+ACLine_R
+ACLine_RL
+ACLine_RLC
+ACLine_RLC_N
+ACLine_RL_N
+ACLine_R_N
+ACSimpleGrid
+ACSimpleGrid_N
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Line.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Line.mo
new file mode 100644
index 0000000000..4ee8316afd
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Line.mo
@@ -0,0 +1,128 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model Line "Model of an electrical line without neutral cable"
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort(
+    terminal_p(phase(v(each nominal = V_nominal))),
+    terminal_n(phase(v(each nominal = V_nominal))));
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine(
+  V_nominal(start = 480),
+  commercialCable = AixLib.Electrical.Transmission.Functions.selectCable_low(P_nominal, V_nominal));
+  OnePhase.Lines.TwoPortRL phase1(
+    final useHeatPort=true,
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=modelMode) "Impedance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortRL phase2(
+    final useHeatPort=true,
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=modelMode) "Impedance line 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortRL phase3(
+    final useHeatPort=true,
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=modelMode) "Impedance line 3"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+equation
+
+  connect(cableTemp.port, phase1.heatPort) annotation (Line(
+      points={{-40,22},{-26,22},{-26,10},{6.66134e-16,10},{6.66134e-16,20}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(cableTemp.port, phase2.heatPort) annotation (Line(
+      points={{-40,22},{-26,22},{-26,-20},{0,-20},{0,-10},{4.44089e-16,-10}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(cableTemp.port, phase3.heatPort) annotation (Line(
+      points={{-40,22},{-26,22},{-26,-50},{0,-50},{0,-40}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,4.44089e-16},{100,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,4.44089e-16},{100,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(graphics={
+        Ellipse(
+          extent={{-70,10},{-50,-10}},
+          lineColor={0,0,0},
+          fillColor={11,193,87},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-60,10},{60,-10}},
+          fillColor={11,193,87},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{50,10},{70,-10}},
+          lineColor={0,0,0},
+          fillColor={255,128,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-70,0},{-90,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,10},{60,10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,-10},{60,-10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{96,0},{60,0}},
+          color={0,0,0},
+          smooth=Smooth.None)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+April 5, 2023, by Michael Wetter:<br/>
+Set nominal attribute for voltage at terminal.
+</li>
+<li>
+October 6, 2014, by Marco Bonvini:<br/>
+Revised documentation and model.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents an AC three-phase unbalanced cable without
+neutral connection. The model is based on
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortRLC\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortRLC</a>
+and provides functionalities to parametrize the values of <i>R</i>, <i>L</i> and <i>C</i>
+using either commercial cables or default values.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Line;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Line_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Line_N.mo
new file mode 100644
index 0000000000..5df5396f95
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Line_N.mo
@@ -0,0 +1,150 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model Line_N "Model of an electrical line with neutral cable"
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort_N(
+    terminal_p(phase(v(each nominal = V_nominal))),
+    terminal_n(phase(v(each nominal = V_nominal))));
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine(
+  V_nominal(start = 480),
+  commercialCable = AixLib.Electrical.Transmission.Functions.selectCable_low(P_nominal, V_nominal));
+  OnePhase.Lines.TwoPortRL phase1(
+    final useHeatPort=true,
+    final T_ref=T_ref,
+    final M=M,
+    final mode=modelMode,
+    final R=R/3,
+    final L=L/3) "Impedance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortRL phase2(
+    final useHeatPort=true,
+    final T_ref=T_ref,
+    final M=M,
+    final mode=modelMode,
+    final R=R/3,
+    final L=L/3) "Impedance line 1"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortRL phase3(
+    final useHeatPort=true,
+    final T_ref=T_ref,
+    final M=M,
+    final mode=modelMode,
+    final R=R/3,
+    final L=L/3) "Impedance line 1"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  OnePhase.Lines.TwoPortRL neutral(
+    final useHeatPort=true,
+    final T_ref=T_ref,
+    final M=M,
+    final mode=modelMode,
+    final R=R/3,
+    final L=L/3) "Impedance of the neutral cable"
+    annotation (Placement(transformation(extent={{-10,-70},{10,-50}})));
+equation
+
+  connect(cableTemp.port, phase1.heatPort) annotation (Line(
+      points={{-40,22},{-26,22},{-26,10},{6.66134e-16,10},{6.66134e-16,20}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(cableTemp.port, phase2.heatPort) annotation (Line(
+      points={{-40,22},{-26,22},{-26,-20},{0,-20},{0,-10},{4.44089e-16,-10}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(cableTemp.port, phase3.heatPort) annotation (Line(
+      points={{-40,22},{-26,22},{-26,-50},{0,-50},{0,-40}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,4.44089e-16},{100,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,4.44089e-16},{100,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(cableTemp.port, neutral.heatPort) annotation (Line(
+      points={{-40,22},{-26,22},{-26,-74},{6.66134e-16,-74},{6.66134e-16,-70}},
+      color={191,0,0},
+      smooth=Smooth.None));
+
+  // Neutral cable connection
+  connect(terminal_n.phase[4], neutral.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-60},{-10,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_p.phase[4], neutral.terminal_p) annotation (Line(
+      points={{100,4.44089e-16},{20,4.44089e-16},{20,-60},{10,-60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(graphics={
+        Ellipse(
+          extent={{-70,10},{-50,-10}},
+          lineColor={0,0,0},
+          fillColor={11,193,87},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-60,10},{60,-10}},
+          fillColor={11,193,87},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{50,10},{70,-10}},
+          lineColor={0,0,0},
+          fillColor={255,128,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-70,0},{-90,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,10},{60,10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,-10},{60,-10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{96,0},{60,0}},
+          color={0,0,0},
+          smooth=Smooth.None)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+April 5, 2023, by Michael Wetter:<br/>
+Set nominal attribute for voltage at terminal.
+</li>
+<li>
+October 6, 2014, by Marco Bonvini:<br/>
+Revised documentation and model.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents an AC three-phase unbalanced cable with
+neutral connection. The model is based on
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortRLC\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortRLC</a>
+and provides functionalities to parametrize the values of <i>R</i>, <i>L</i> and <i>C</i>
+using either commercial cables or default values.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Line_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Network.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Network.mo
new file mode 100644
index 0000000000..e8e73b58e5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Network.mo
@@ -0,0 +1,52 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model Network "Three phases unbalanced AC network without neutral cable"
+  extends Transmission.BaseClasses.PartialNetwork(
+    redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal_p terminal,
+    redeclare replaceable Transmission.Grids.TestGrid2Nodes grid,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Line lines(commercialCable=grid.cables));
+  Modelica.Units.SI.Voltage VAbs[3,grid.nNodes] "RMS voltage of the grid nodes";
+equation
+  for i in 1:grid.nLinks loop
+    connect(lines[i].terminal_p, terminal[grid.fromTo[i,1]]);
+    connect(lines[i].terminal_n, terminal[grid.fromTo[i,2]]);
+  end for;
+
+  for i in 1:grid.nNodes loop
+    VAbs[1,i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal[i].phase[1].v);
+    VAbs[2,i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal[i].phase[2].v);
+    VAbs[3,i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal[i].phase[3].v);
+  end for;
+  annotation (
+  defaultComponentName="net",
+ Documentation(revisions="<html>
+ <ul>
+ <li>
+March 30, 2015, by Michael Wetter:<br/>
+Made <code>network</code> replaceable. This was detected
+by the OpenModelica regression tests.
+</li>
+<li>
+October 6, 2014, by Marco Bonvini:<br/>
+Revised documentation and model.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a generalized electrical AC three-phase unbalanced network
+without neutral cable.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.BaseClasses.PartialNetwork\">
+AixLib.Electrical.Transmission.BaseClasses.PartialNetwork</a>
+for information about the network model.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.Grids.PartialGrid\">
+AixLib.Electrical.Transmission.Grids.PartialGrid</a>
+for more information about the topology of the network, such as
+the number of nodes, how they are connected, and the length of each connection.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Network;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Network_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Network_N.mo
new file mode 100644
index 0000000000..763d1b4bfa
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/Network_N.mo
@@ -0,0 +1,53 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model Network_N "Three phases unbalanced AC network with neutral cable"
+  extends Transmission.BaseClasses.PartialNetwork(
+    redeclare
+      AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal4_p terminal,
+    redeclare replaceable Transmission.Grids.TestGrid2Nodes grid,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Line_N lines(
+        commercialCable=grid.cables));
+  Modelica.Units.SI.Voltage VAbs[3,grid.nNodes] "RMS voltage of the grid nodes";
+equation
+  for i in 1:grid.nLinks loop
+    connect(lines[i].terminal_p, terminal[grid.fromTo[i,1]]);
+    connect(lines[i].terminal_n, terminal[grid.fromTo[i,2]]);
+  end for;
+
+  for i in 1:grid.nNodes loop
+    VAbs[1,i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal[i].phase[1].v - terminal[i].phase[4].v);
+    VAbs[2,i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal[i].phase[2].v - terminal[i].phase[4].v);
+    VAbs[3,i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal[i].phase[3].v - terminal[i].phase[4].v);
+  end for;
+  annotation (
+  defaultComponentName="net",
+ Documentation(revisions="<html>
+<ul>
+<li>
+March 30, 2015, by Michael Wetter:<br/>
+Made <code>term</code> replaceable. This was detected
+by the OpenModelica regression tests.
+</li>
+<li>
+October 6, 2014, by Marco Bonvini:<br/>
+Revised documentation and model.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a generalized electrical AC three-phase unbalanced network
+with neutral cable.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.BaseClasses.PartialNetwork\">
+AixLib.Electrical.Transmission.BaseClasses.PartialNetwork</a>
+for information about the network model.
+</p>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.Grids.PartialGrid\">
+AixLib.Electrical.Transmission.Grids.PartialGrid</a>
+for more information about the topology of the network, such as
+the number of nodes, how they are connected, and the length of each connection.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Network_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortInductance.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortInductance.mo
new file mode 100644
index 0000000000..10c8beecab
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortInductance.mo
@@ -0,0 +1,116 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortInductance "Model of an inductance with two electrical ports"
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort;
+  parameter Modelica.Units.SI.Inductance L "Inductance";
+  OnePhase.Lines.TwoPortInductance  phase1(
+    final L=L/3) "Inductance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortInductance phase2(
+    final L=L/3) "Inductance line 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortInductance phase3(
+    final L=L/3) "Inductance line 3"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+equation
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+        Rectangle(
+          extent={{-72,32},{68,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,14},{42,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Text(
+            extent={{-140,-28},{140,-60}},
+            textColor={0,0,0},
+          textString="L=%L"),
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+          Text(
+            extent={{-142,80},{138,40}},
+            textColor={0,0,0},
+          textString="%name"),
+          Line(
+          points={{0,0},{12,1.46953e-15}},
+          color={0,0,0},
+          origin={-42,0},
+          rotation=180),
+        Ellipse(
+          extent={{-42,14},{-14,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-14,14},{14,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-42,0},{48,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+          color={0,0,0},
+          origin={52,0},
+          rotation=180)}),
+    Documentation(info="<html>
+<p>
+Inductive model that connects two AC three-phase
+unbalanced interfaces. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortL.png\"/>
+</p>
+
+<p>
+The model represents the lumped inductances as shown in the figure above.
+Assuming that the inductance <i>L</i> is the overall inductance of the cable,
+each line has an inductance equal to <i>L/3</i>.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Added model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortInductance;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortInductance_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortInductance_N.mo
new file mode 100644
index 0000000000..46e5daf6cc
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortInductance_N.mo
@@ -0,0 +1,132 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortInductance_N
+  "Model of an inductance with two electrical ports and neutral line cable"
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort_N;
+  parameter Modelica.Units.SI.Inductance L "Inductance";
+  parameter Modelica.Units.SI.Inductance Ln "Inductance of neutral cable";
+  OnePhase.Lines.TwoPortInductance  phase1(
+    final L=L/3) "Inductance line 1"
+    annotation (Placement(transformation(extent={{-10,32},{10,52}})));
+  OnePhase.Lines.TwoPortInductance phase2(
+    final L=L/3) "Inductance line 2"
+    annotation (Placement(transformation(extent={{-10,2},{10,22}})));
+  OnePhase.Lines.TwoPortInductance phase3(
+    final L=L/3) "Inductance line 3"
+    annotation (Placement(transformation(extent={{-10,-28},{10,-8}})));
+  OnePhase.Lines.TwoPortInductance phase4(
+    final L=L/3) "Inductance line 3"
+    annotation (Placement(transformation(extent={{-10,-58},{10,-38}})));
+equation
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,42},{-10,42}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,12},{-10,12}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-18},{-10,-18}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,42},{20,42},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,12},{20,12},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-18},{20,-18},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(phase4.terminal_p, terminal_p.phase[4]) annotation (Line(
+      points={{10,-48},{20,-48},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase4.terminal_n, terminal_n.phase[4]) annotation (Line(
+      points={{-10,-48},{-20,-48},{-20,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+        Rectangle(
+          extent={{-72,32},{68,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,14},{42,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Text(
+            extent={{-140,-28},{140,-60}},
+            textColor={0,0,0},
+          textString="L=%L"),
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+          Text(
+            extent={{-142,80},{138,40}},
+            textColor={0,0,0},
+          textString="%name"),
+          Line(
+          points={{0,0},{12,1.46953e-15}},
+          color={0,0,0},
+          origin={-42,0},
+          rotation=180),
+        Ellipse(
+          extent={{-42,14},{-14,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-14,14},{14,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-42,0},{48,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+          color={0,0,0},
+          origin={52,0},
+          rotation=180)}),
+    Documentation(info="<html>
+<p>
+Inductive model that connects two AC three-phase
+unbalanced interfaces with neutral line. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortL_N.png\"/>
+</p>
+
+<p>
+The model represents the lumped inductances as shown in the figure above.
+Assuming that the inductance <i>L</i> is the overall inductance of the cable,
+each line has an inductance equal to <i>L/3</i>.
+</p>
+<p>
+The inductance of the neutral cable is defined separately using the parameter
+<code>Ln</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added model and user guide
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortInductance_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRL.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRL.mo
new file mode 100644
index 0000000000..2f6314e297
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRL.mo
@@ -0,0 +1,169 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortMatrixRL
+  "Model of an RL line parameterized with impedance matrices"
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort(
+    terminal_p(phase(v(each nominal = V_nominal))),
+    terminal_n(phase(v(each nominal = V_nominal))));
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=480)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Evaluate=true, Dialog(group="Nominal conditions"));
+  parameter Modelica.Units.SI.Impedance Z11[2]
+    "Element [1,1] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z12[2]
+    "Element [1,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z13[2]
+    "Element [1,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z22[2]
+    "Element [2,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z23[2]
+    "Element [2,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z33[2]
+    "Element [3,3] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z21=Z12
+    "Element [2,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z31=Z13
+    "Element [3,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z32=Z23
+    "Element [3,1] of impedance matrix";
+
+  Modelica.Units.SI.Current i1[2](each stateSelect=StateSelect.prefer)=
+    terminal_n.phase[1].i "Current in line 1";
+  Modelica.Units.SI.Current i2[2](each stateSelect=StateSelect.prefer)=
+    terminal_n.phase[2].i "Current in line 2";
+  Modelica.Units.SI.Current i3[2](each stateSelect=StateSelect.prefer)=
+    terminal_n.phase[3].i "Current in line 3";
+  Modelica.Units.SI.Voltage v1_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=0),
+    each stateSelect=StateSelect.never) = terminal_n.phase[1].v
+    "Voltage in line 1 at connector N";
+  Modelica.Units.SI.Voltage v2_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=-2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_n.phase[2].v
+    "Voltage in line 2 at connector N";
+  Modelica.Units.SI.Voltage v3_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_n.phase[3].v
+    "Voltage in line 3 at connector N";
+  Modelica.Units.SI.Voltage v1_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=0),
+    each stateSelect=StateSelect.never) = terminal_p.phase[1].v
+    "Voltage in line 1 at connector P";
+  Modelica.Units.SI.Voltage v2_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=-2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_p.phase[2].v
+    "Voltage in line 2 at connector P";
+  Modelica.Units.SI.Voltage v3_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_p.phase[3].v
+    "Voltage in line 3 at connector P";
+
+protected
+  function productAC1p = AixLib.Electrical.PhaseSystems.OnePhase.product
+    "Product between complex quantities";
+equation
+
+  // Link the connectors to propagate the overdetermined variable
+  for i in 1:3 loop
+      Connections.branch(terminal_p.phase[i].theta, terminal_n.phase[i].theta);
+      terminal_p.phase[i].theta = terminal_n.phase[i].theta;
+
+      // No current losses, they are preserved in each line
+      terminal_p.phase[i].i = - terminal_n.phase[i].i;
+  end for;
+
+  // Voltage drop caused by the impedance matrix
+  v1_n - v1_p = productAC1p(Z11, i1) + productAC1p(Z12, i2) + productAC1p(Z13, i3);
+  v2_n - v2_p = productAC1p(Z21, i1) + productAC1p(Z22, i2) + productAC1p(Z23, i3);
+  v3_n - v3_p = productAC1p(Z31, i1) + productAC1p(Z32, i2) + productAC1p(Z33, i3);
+
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,40},{70,-40}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-26,16},{10,4}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Text(
+            extent={{-140,100},{140,60}},
+            textColor={0,0,0},
+          textString="%name"),
+          Text(
+            extent={{-70,10},{70,-10}},
+            textColor={0,0,0},
+          textString="R+jX 3x3")}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+April 5, 2022, by Michael Wetter:<br/>
+Set nominal attribute for voltage at terminals.
+This is required for
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.DD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.DD</a>
+to converge with Dymola 2023 beta3.
+Inspecting the homotopy trajectory showed that this variable diverged to an unreasonable value.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Removed zero start value for currents <code>i1</code>, <code>i2</code> and
+<code>i3</code>.
+Setting a zero start value led Dymola 2017 on Linux to find a different solution
+for
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.YD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.YD</a>.
+Also, the current is typically non-zero and zero is anyway the default start value, hence there is no need to set it.<br/>
+Made current and voltage public to allow setting start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 6, 2014, by Marco Bonvini:<br/>
+Revised documentation and model.
+</li>
+<li>
+June 5, 2014, by Marco Bonvini:<br/>
+Added model.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Resistive-inductive model that connects two AC three-phase
+unbalanced interfaces. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+The voltage between the ports is
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix.png\"/>
+</p>
+
+<p>
+where <i>V<sub>i</sub><sup>{p,n}</sup></i> is the voltage phasor at the connector <code>p</code> or
+<code>n</code> of the <i>i</i>-th phase, while <i>I<sub>i</sub><sup>p</sup></i>
+the current phasor entering from the connector <code>p</code> of the <i>i</i>-th phase.
+</p>
+
+<p>
+The model is parameterized with an impedance matrix <i>Z</i>.
+The matrix is symmetric thus just the upper triangular
+part of it has to be defined.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortMatrixRL;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRLC.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRLC.mo
new file mode 100644
index 0000000000..f55a32ccc5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRLC.mo
@@ -0,0 +1,212 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortMatrixRLC
+  "PI model of a line parameterized with impedance and admittance matrices"
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort(
+    terminal_p(phase(v(each nominal = V_nominal))),
+    terminal_n(phase(v(each nominal = V_nominal))));
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=480)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Evaluate=true, Dialog(group="Nominal conditions"));
+  parameter Modelica.Units.SI.Impedance Z11[2]
+    "Element [1,1] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z12[2]
+    "Element [1,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z13[2]
+    "Element [1,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z22[2]
+    "Element [2,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z23[2]
+    "Element [2,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z33[2]
+    "Element [3,3] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z21=Z12
+    "Element [2,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z31=Z13
+    "Element [3,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z32=Z23
+    "Element [3,1] of impedance matrix";
+
+  parameter Modelica.Units.SI.Admittance B11
+    "Element [1,1] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B12
+    "Element [1,2] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B13
+    "Element [1,3] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B22
+    "Element [2,2] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B23
+    "Element [2,3] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B33
+    "Element [3,3] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B21=B12
+    "Element [2,1] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B31=B13
+    "Element [3,1] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B32=B23
+    "Element [3,2] of admittance matrix";
+
+  Modelica.Units.SI.Voltage v1_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=0),
+    each stateSelect=StateSelect.never) = terminal_n.phase[1].v
+    "Voltage in line 1 at connector N";
+  Modelica.Units.SI.Voltage v2_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=-2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_n.phase[2].v
+    "Voltage in line 2 at connector N";
+  Modelica.Units.SI.Voltage v3_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_n.phase[3].v
+    "Voltage in line 3 at connector N";
+  Modelica.Units.SI.Voltage v1_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=0),
+    each stateSelect=StateSelect.never) = terminal_p.phase[1].v
+    "Voltage in line 1 at connector P";
+  Modelica.Units.SI.Voltage v2_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=-2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_p.phase[2].v
+    "Voltage in line 2 at connector P";
+  Modelica.Units.SI.Voltage v3_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_p.phase[3].v
+    "Voltage in line 3 at connector P";
+
+protected
+  function productAC1p = AixLib.Electrical.PhaseSystems.OnePhase.product
+    "Product between complex quantities";
+  Modelica.Units.SI.Current Isr[3,2](start=zeros(3, AixLib.Electrical.PhaseSystems.OnePhase.n),
+      each stateSelect=StateSelect.prefer)
+    "Currents that pass through the lines";
+  Modelica.Units.SI.Current Ish_p[3,2](start=zeros(3, AixLib.Electrical.PhaseSystems.OnePhase.n),
+      each stateSelect=StateSelect.prefer) "Shunt current on side p";
+  Modelica.Units.SI.Current Ish_n[3,2](start=zeros(3, AixLib.Electrical.PhaseSystems.OnePhase.n),
+      each stateSelect=StateSelect.prefer) "Shunt current on side n";
+
+equation
+
+  // Link the connectors to propagate the overdetermined variable
+  for i in 1:3 loop
+      Connections.branch(terminal_p.phase[i].theta, terminal_n.phase[i].theta);
+      terminal_p.phase[i].theta = terminal_n.phase[i].theta;
+  end for;
+
+  // Kirkoff current law for the terminal n (left side)
+  Isr[1,:] = terminal_n.phase[1].i - Ish_n[1,:];
+  Isr[2,:] = terminal_n.phase[2].i - Ish_n[2,:];
+  Isr[3,:] = terminal_n.phase[3].i - Ish_n[3,:];
+
+  // Kirkoff current law for the terminal p (right side)
+  Isr[1,:] + terminal_p.phase[1].i = Ish_p[1,:];
+  Isr[2,:] + terminal_p.phase[2].i = Ish_p[2,:];
+  Isr[3,:] + terminal_p.phase[3].i = Ish_p[3,:];
+
+  // Voltage drop caused by the impedance matrix
+  terminal_n.phase[1].v - terminal_p.phase[1].v = productAC1p(Z11, terminal_n.phase[1].i)
+                                                + productAC1p(Z12, terminal_n.phase[2].i)
+                                                + productAC1p(Z13, terminal_n.phase[3].i);
+  terminal_n.phase[2].v - terminal_p.phase[2].v = productAC1p(Z21, terminal_n.phase[1].i)
+                                                + productAC1p(Z22, terminal_n.phase[2].i)
+                                                + productAC1p(Z23, terminal_n.phase[3].i);
+  terminal_n.phase[3].v - terminal_p.phase[3].v = productAC1p(Z31, terminal_n.phase[1].i)
+                                                + productAC1p(Z32, terminal_n.phase[2].i)
+                                                + productAC1p(Z33, terminal_n.phase[3].i);
+
+  // Current loss at the terminal n
+  Ish_n[1,:] = productAC1p({0, B11/2}, v1_n)
+             + productAC1p({0, B12/2}, v2_n)
+             + productAC1p({0, B13/2}, v3_n);
+  Ish_n[2,:] = productAC1p({0, B21/2}, v1_n)
+             + productAC1p({0, B22/2}, v2_n)
+             + productAC1p({0, B23/2}, v3_n);
+  Ish_n[3,:] = productAC1p({0, B31/2}, v1_n)
+             + productAC1p({0, B32/2}, v2_n)
+             + productAC1p({0, B33/2}, v3_n);
+
+  // Current loss at the terminal n
+  Ish_p[1,:] = productAC1p({0, B11/2}, v1_p)
+             + productAC1p({0, B12/2}, v2_p)
+             + productAC1p({0, B13/2}, v3_p);
+  Ish_p[2,:] = productAC1p({0, B21/2}, v1_p)
+             + productAC1p({0, B22/2}, v2_p)
+             + productAC1p({0, B23/2}, v3_p);
+  Ish_p[3,:] = productAC1p({0, B31/2}, v1_p)
+             + productAC1p({0, B32/2}, v2_p)
+             + productAC1p({0, B33/2}, v3_p);
+
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,40},{70,-40}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Text(
+            extent={{-140,100},{140,60}},
+            textColor={0,0,0},
+          textString="%name"),
+          Text(
+            extent={{-72,30},{70,10}},
+            textColor={0,0,0},
+          textString="R+jX 3x3"),
+          Text(
+            extent={{-72,-10},{70,-30}},
+            textColor={0,0,0},
+          textString="C 3x3")}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+April 5, 2023, by Michael Wetter:<br/>
+Set nominal attribute for voltage at terminal.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Made current and voltage public to allow setting start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 6, 2014, by Marco Bonvini:<br/>
+Revised documentation and model.
+</li>
+<li>
+June 5, 2014, by Marco Bonvini:<br/>
+Added model.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+RLC line model (&pi;-model) that connects two AC three-phase
+unbalanced interfaces. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLCMatrix.png\"/>
+</p>
+
+<p>
+The model is parameterized with an impedance matrix <i>Z</i> and
+an admittance matrix <i>B</i>.
+The impedance matrix is symmetric, and therefore only the upper triangular
+part of the matrix needs to be defined.
+</p>
+
+<p>
+This model is a more detailed version of the model <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortMatrixRL\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortMatrixRL</a> that includes
+the capacitive effects of the lines.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortMatrixRLC;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRLC_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRLC_N.mo
new file mode 100644
index 0000000000..3ef00d36e8
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRLC_N.mo
@@ -0,0 +1,284 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortMatrixRLC_N
+  "PI model of a line parameterized with impedance and admittance matrices and neutral line"
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort_N(
+    terminal_p(phase(v(each nominal = V_nominal))),
+    terminal_n(phase(v(each nominal = V_nominal))));
+
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=480)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Evaluate=true, Dialog(group="Nominal conditions"));
+  parameter Modelica.Units.SI.Impedance Z11[2]
+    "Element [1,1] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z12[2]
+    "Element [1,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z13[2]
+    "Element [1,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z14[2]
+    "Element [1,4] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z22[2]
+    "Element [2,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z23[2]
+    "Element [2,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z24[2]
+    "Element [2,4] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z33[2]
+    "Element [3,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z34[2]
+    "Element [3,4] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z44[2]
+    "Element [4,4] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z21=Z12
+    "Element [2,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z31=Z13
+    "Element [3,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z32=Z23
+    "Element [3,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z41=Z14
+    "Element [4,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z42=Z24
+    "Element [4,2] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z43=Z34
+    "Element [4,3] of impedance matrix";
+
+  parameter Modelica.Units.SI.Admittance B11
+    "Element [1,1] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B12
+    "Element [1,2] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B13
+    "Element [1,3] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B14
+    "Element [1,4] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B22
+    "Element [2,2] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B23
+    "Element [2,3] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B24
+    "Element [2,4] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B33
+    "Element [3,3] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B34
+    "Element [3,4] of admittance matrix";
+  parameter Modelica.Units.SI.Admittance B44
+    "Element [4,4] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B21=B12
+    "Element [2,1] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B31=B13
+    "Element [3,1] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B32=B23
+    "Element [3,2] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B41=B14
+    "Element [4,1] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B42=B24
+    "Element [4,2] of admittance matrix";
+  final parameter Modelica.Units.SI.Admittance B43=B34
+    "Element [4,3] of admittance matrix";
+
+  Modelica.Units.SI.Voltage v1_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=0),
+    each stateSelect=StateSelect.never) = terminal_n.phase[1].v
+    "Voltage in line 1 at connector N";
+  Modelica.Units.SI.Voltage v2_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=-2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_n.phase[2].v
+    "Voltage in line 2 at connector N";
+  Modelica.Units.SI.Voltage v3_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_n.phase[3].v
+    "Voltage in line 3 at connector N";
+  Modelica.Units.SI.Voltage v4_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(0),
+    each stateSelect=StateSelect.never) = terminal_n.phase[4].v
+    "Voltage in line 4 (neutral) at connector N";
+  Modelica.Units.SI.Voltage v1_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=0),
+    each stateSelect=StateSelect.never) = terminal_p.phase[1].v
+    "Voltage in line 1 at connector P";
+  Modelica.Units.SI.Voltage v2_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=-2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_p.phase[2].v
+    "Voltage in line 2 at connector P";
+  Modelica.Units.SI.Voltage v3_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_p.phase[3].v
+    "Voltage in line 3 at connector P";
+  Modelica.Units.SI.Voltage v4_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(0),
+    each stateSelect=StateSelect.never) = terminal_p.phase[4].v
+    "Voltage in line 4 (neutral) at connector P";
+
+protected
+  function productAC1p = AixLib.Electrical.PhaseSystems.OnePhase.product
+    "Product between complex quantities";
+  Modelica.Units.SI.Current Isr[4,2](each stateSelect=StateSelect.prefer)
+    "Currents that pass through the lines";
+  Modelica.Units.SI.Current Ish_p[4,2](each stateSelect=StateSelect.prefer)
+    "Shunt current on side p";
+  Modelica.Units.SI.Current Ish_n[4,2](each stateSelect=StateSelect.prefer)
+    "Shunt current on side n";
+
+equation
+
+  // Link the connectors to propagate the overdetermined variable
+  for i in 1:4 loop
+      Connections.branch(terminal_p.phase[i].theta, terminal_n.phase[i].theta);
+      terminal_p.phase[i].theta = terminal_n.phase[i].theta;
+  end for;
+
+  // Kirkoff current law for the terminal n (left side)
+  Isr[1,:] = terminal_n.phase[1].i - Ish_n[1,:];
+  Isr[2,:] = terminal_n.phase[2].i - Ish_n[2,:];
+  Isr[3,:] = terminal_n.phase[3].i - Ish_n[3,:];
+  Isr[4,:] = terminal_n.phase[4].i - Ish_n[4,:];
+
+  // Kirkoff current law for the terminal p (right side)
+  Isr[1,:] + terminal_p.phase[1].i = Ish_p[1,:];
+  Isr[2,:] + terminal_p.phase[2].i = Ish_p[2,:];
+  Isr[3,:] + terminal_p.phase[3].i = Ish_p[3,:];
+  Isr[4,:] + terminal_p.phase[4].i = Ish_p[4,:];
+
+  // Voltage drop caused by the impedance matrix
+  terminal_n.phase[1].v - terminal_p.phase[1].v = productAC1p(Z11, terminal_n.phase[1].i)
+                                                + productAC1p(Z12, terminal_n.phase[2].i)
+                                                + productAC1p(Z13, terminal_n.phase[3].i)
+                                                + productAC1p(Z14, terminal_n.phase[4].i);
+  terminal_n.phase[2].v - terminal_p.phase[2].v = productAC1p(Z21, terminal_n.phase[1].i)
+                                                + productAC1p(Z22, terminal_n.phase[2].i)
+                                                + productAC1p(Z23, terminal_n.phase[3].i)
+                                                + productAC1p(Z24, terminal_n.phase[4].i);
+  terminal_n.phase[3].v - terminal_p.phase[3].v = productAC1p(Z31, terminal_n.phase[1].i)
+                                                + productAC1p(Z32, terminal_n.phase[2].i)
+                                                + productAC1p(Z33, terminal_n.phase[3].i)
+                                                + productAC1p(Z34, terminal_n.phase[4].i);
+  terminal_n.phase[4].v - terminal_p.phase[4].v = productAC1p(Z41, terminal_n.phase[1].i)
+                                                + productAC1p(Z42, terminal_n.phase[2].i)
+                                                + productAC1p(Z43, terminal_n.phase[3].i)
+                                                + productAC1p(Z44, terminal_n.phase[4].i);
+
+  // Current loss at the terminal n
+  Ish_n[1,:] = productAC1p({0, B11/2}, v1_n)
+             + productAC1p({0, B12/2}, v2_n)
+             + productAC1p({0, B13/2}, v3_n)
+             + productAC1p({0, B14/2}, v4_n);
+  Ish_n[2,:] = productAC1p({0, B21/2}, v1_n)
+             + productAC1p({0, B22/2}, v2_n)
+             + productAC1p({0, B23/2}, v3_n)
+             + productAC1p({0, B24/2}, v4_n);
+  Ish_n[3,:] = productAC1p({0, B31/2}, v1_n)
+             + productAC1p({0, B32/2}, v2_n)
+             + productAC1p({0, B33/2}, v3_n)
+             + productAC1p({0, B34/2}, v4_n);
+  Ish_n[4,:] = productAC1p({0, B41/2}, v1_n)
+             + productAC1p({0, B42/2}, v2_n)
+             + productAC1p({0, B43/2}, v3_n)
+             + productAC1p({0, B44/2}, v4_n);
+
+  // Current loss at the terminal n
+  Ish_p[1,:] = productAC1p({0, B11/2}, v1_p)
+             + productAC1p({0, B12/2}, v2_p)
+             + productAC1p({0, B13/2}, v3_p)
+             + productAC1p({0, B14/2}, v4_p);
+  Ish_p[2,:] = productAC1p({0, B21/2}, v1_p)
+             + productAC1p({0, B22/2}, v2_p)
+             + productAC1p({0, B23/2}, v3_p)
+             + productAC1p({0, B24/2}, v4_p);
+  Ish_p[3,:] = productAC1p({0, B31/2}, v1_p)
+             + productAC1p({0, B32/2}, v2_p)
+             + productAC1p({0, B33/2}, v3_p)
+             + productAC1p({0, B34/2}, v4_p);
+  Ish_p[4,:] = productAC1p({0, B41/2}, v1_p)
+             + productAC1p({0, B42/2}, v2_p)
+             + productAC1p({0, B43/2}, v3_p)
+             + productAC1p({0, B44/2}, v4_p);
+
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,40},{70,-40}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Text(
+            extent={{-140,100},{140,60}},
+            textColor={0,0,0},
+          textString="%name"),
+          Text(
+            extent={{-72,30},{70,10}},
+            textColor={0,0,0},
+          textString="R+jX 4x4"),
+          Text(
+            extent={{-72,-10},{70,-30}},
+            textColor={0,0,0},
+          textString="C 4x4")}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+April 5, 2023, by Michael Wetter:<br/>
+Set nominal attribute for voltage at terminal.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Made current and voltage public to allow setting start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Removed zero start value for currents <code>i1</code>, <code>i2</code> and
+<code>i3</code>.
+Setting a zero start value led Dymola 2017 on Linux to find a different solution
+for
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.YD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.YD</a>.
+Also, the current is typically non-zero and zero is anyway the default start value, hence there is no need to set it.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+RLC line model (&pi;-model) that connects two AC three-phase
+unbalanced interfaces and neutral line. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLCMatrix_N.png\"/>
+</p>
+
+<p>
+The model is parameterized with an impedance matrix <i>Z</i> and
+an admittance matrix <i>B</i>.
+The impedance matrix is symmetric, and therefore only the upper triangular
+part of the matrix needs to be defined.
+</p>
+
+<p>
+This model is a more detailed version of the model <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortMatrixRL_N\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortMatrixRL_N</a> that includes
+the capacitive effects of the lines.
+</p>
+
+<h4>Note</h4>
+<p>
+The fourth line is the neutral one.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortMatrixRLC_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRL_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRL_N.mo
new file mode 100644
index 0000000000..f845784dab
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortMatrixRL_N.mo
@@ -0,0 +1,196 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortMatrixRL_N
+  "Model of an RL line parameterized with impedance matrices and neutral line"
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort_N(
+    terminal_p(phase(v(each nominal = V_nominal))),
+    terminal_n(phase(v(each nominal = V_nominal))));
+
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=480)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Evaluate=true, Dialog(group="Nominal conditions"));
+  parameter Modelica.Units.SI.Impedance Z11[2]
+    "Element [1,1] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z12[2]
+    "Element [1,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z13[2]
+    "Element [1,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z14[2]
+    "Element [1,4] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z22[2]
+    "Element [2,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z23[2]
+    "Element [2,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z24[2]
+    "Element [2,4] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z33[2]
+    "Element [3,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z34[2]
+    "Element [3,4] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z44[2]
+    "Element [4,4] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z21=Z12
+    "Element [2,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z31=Z13
+    "Element [3,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z32=Z23
+    "Element [3,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z41=Z14
+    "Element [4,1] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z42=Z24
+    "Element [4,2] of impedance matrix";
+  final parameter Modelica.Units.SI.Impedance[2] Z43=Z34
+    "Element [4,3] of impedance matrix";
+
+  Modelica.Units.SI.Current i1[2](each stateSelect=StateSelect.prefer)=
+    terminal_n.phase[1].i "Current in line 1";
+  Modelica.Units.SI.Current i2[2](each stateSelect=StateSelect.prefer)=
+    terminal_n.phase[2].i "Current in line 2";
+  Modelica.Units.SI.Current i3[2](each stateSelect=StateSelect.prefer)=
+    terminal_n.phase[3].i "Current in line 3";
+  Modelica.Units.SI.Current i4[2](each stateSelect=StateSelect.prefer)=
+    terminal_n.phase[4].i "Current in line 4 (neutral)";
+  Modelica.Units.SI.Voltage v1_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=0),
+    each stateSelect=StateSelect.never) = terminal_n.phase[1].v
+    "Voltage in line 1 at connector N";
+  Modelica.Units.SI.Voltage v2_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=-2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_n.phase[2].v
+    "Voltage in line 2 at connector N";
+  Modelica.Units.SI.Voltage v3_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_n.phase[3].v
+    "Voltage in line 3 at connector N";
+  Modelica.Units.SI.Voltage v4_n[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(0),
+    each stateSelect=StateSelect.never) = terminal_n.phase[4].v
+    "Voltage in line 4 (neutral) at connector N";
+  Modelica.Units.SI.Voltage v1_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=0),
+    each stateSelect=StateSelect.never) = terminal_p.phase[1].v
+    "Voltage in line 1 at connector P";
+  Modelica.Units.SI.Voltage v2_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=-2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_p.phase[2].v
+    "Voltage in line 2 at connector P";
+  Modelica.Units.SI.Voltage v3_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(V_nominal/
+        sqrt(3), phi=2*Modelica.Constants.pi/3),
+    each stateSelect=StateSelect.never) = terminal_p.phase[3].v
+    "Voltage in line 3 at connector P";
+  Modelica.Units.SI.Voltage v4_p[2](
+    start=AixLib.Electrical.PhaseSystems.OnePhase.phaseVoltages(0),
+    each stateSelect=StateSelect.never) = terminal_p.phase[4].v
+    "Voltage in line 4 (neutral) at connector P";
+
+protected
+  function productAC1p = AixLib.Electrical.PhaseSystems.OnePhase.product
+    "Product between complex quantities";
+equation
+
+  // Link the connectors to propagate the overdetermined variable
+  for i in 1:4 loop
+      Connections.branch(terminal_p.phase[i].theta, terminal_n.phase[i].theta);
+      terminal_p.phase[i].theta = terminal_n.phase[i].theta;
+
+      // No current losses, they are preserved in each line
+      terminal_p.phase[i].i = - terminal_n.phase[i].i;
+  end for;
+
+  // Voltage drop caused by the impedance matrix
+  v1_n - v1_p = productAC1p(Z11, i1) + productAC1p(Z12, i2) + productAC1p(Z13, i3)+ productAC1p(Z14, i4);
+  v2_n - v2_p = productAC1p(Z21, i1) + productAC1p(Z22, i2) + productAC1p(Z23, i3)+ productAC1p(Z24, i4);
+  v3_n - v3_p = productAC1p(Z31, i1) + productAC1p(Z32, i2) + productAC1p(Z33, i3)+ productAC1p(Z34, i4);
+  v4_n - v4_p = productAC1p(Z41, i1) + productAC1p(Z42, i2) + productAC1p(Z43, i3)+ productAC1p(Z44, i4);
+
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,40},{70,-40}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-26,16},{10,4}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Text(
+            extent={{-140,100},{140,60}},
+            textColor={0,0,0},
+          textString="%name"),
+          Text(
+            extent={{-70,10},{70,-10}},
+            textColor={0,0,0},
+          textString="R+jX 4x4")}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+April 5, 2023, by Michael Wetter:<br/>
+Set nominal attribute for voltage at terminal.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Made current and voltage public to allow setting start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Removed zero start value for currents <code>i1</code>, <code>i2</code> and
+<code>i3</code>.
+Setting a zero start value led Dymola 2017 on Linux to find a different solution
+for
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.YD\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.YD</a>.
+Also, the current is typically non-zero and zero is anyway the default start value, hence there is no need to set it.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Created model and documantation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Resistive-inductive model that connects two AC three-phase
+unbalanced interfaces with neutral line. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+The voltage between the ports is
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix_N.png\"/>
+</p>
+
+<p>
+where <i>V<sub>i</sub><sup>{p,n}</sup></i> is the voltage phasor at the connector <code>p</code> or
+<code>n</code> of the <i>i</i>-th phase, while <i>I<sub>i</sub><sup>p</sup></i>
+the current phasor entering from the connector <code>p</code> of the <i>i</i>-th phase.
+</p>
+
+<p>
+The model is parameterized with an impedance matrix <i>Z</i>.
+The matrix is symmetric thus just the upper triangular
+part of it has to be defined.
+</p>
+
+<h4>Note</h4>
+<p>
+The fourth line is the neutral one.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortMatrixRL_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRL.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRL.mo
new file mode 100644
index 0000000000..3a95a351ec
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRL.mo
@@ -0,0 +1,182 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortRL
+  "Model of a resistive-inductive element with two electrical ports"
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort;
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort;
+  parameter Modelica.Units.SI.Resistance R "Resistance at temperature T_ref"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Temperature T_ref=298.15 "Reference temperature"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Temperature M=507.65
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Inductance L "Inductance";
+  parameter Modelica.Units.SI.Current i1_start[2]={0,0}
+    "Initial current phasor of phase 1 (positive if entering from terminal p)"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter Modelica.Units.SI.Current i2_start[2]={0,0}
+    "Initial current phasor of phase 2 (positive if entering from terminal p)"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter Modelica.Units.SI.Current i3_start[2]={0,0}
+    "Initial current phasor of phase 3 (positive if entering from terminal p)"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.FixedZ_dynamic) = AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Type of model (e.g., steady state, dynamic, prescribed power consumption, etc.)"
+    annotation (Evaluate=true, Dialog(group="Modeling assumption"));
+  OnePhase.Lines.TwoPortRL phase1(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=mode,
+    final useHeatPort=useHeatPort,
+    i_start=i1_start) "Impedance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortRL phase2(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=mode,
+    final useHeatPort=useHeatPort,
+    i_start=i2_start) "Impedance line 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortRL phase3(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=mode,
+    final useHeatPort=useHeatPort,
+    i_start=i3_start) "Impedance line 3"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+equation
+  // Joule Losses
+  LossPower = phase1.LossPower + phase2.LossPower + phase3.LossPower;
+
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-99.95,0.05},{-20,0.05},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-99.95,0.05},{-54,0.05},{-54,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-99.95,0.05},{-20,0.05},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,0.05},{100.05,0.05}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{56,0},{56,0.05},{100.05,0.05}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,0.05},{100.05,0.05}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(phase1.heatPort, heatPort) annotation (Line(
+      points={{0,20},{0,14},{-32,14},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase3.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-40},{0,-40},{0,-100},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase2.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-10},{4.44089e-16,-16},{-32,-16},{-32,-72},{
+          4.44089e-16,-72},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Text(
+            extent={{-150,-28},{136,-60}},
+            textColor={0,0,0},
+          textString="R=%R, L=%L"),
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,32},{68,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{66,8.0824e-15}},
+          color={0,0,0},
+          origin={52,0},
+          rotation=180),
+        Line(
+          points={{-48,0},{-42,0},{-40,4},{-36,-4},{-32,4},{-28,-4},{-24,4},{-20,
+              -4},{-18,0},{-14,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-6,6},{6,-6}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{6,6},{18,-6}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{18,6},{30,-6}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-6,0},{30,-12}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Text(
+            extent={{-142,80},{138,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+Resistive-inductive model that connects two AC three-phase
+unbalanced interfaces. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRL.png\"/>
+</p>
+
+<p>
+The model represents the lumped impedances as shown in the figure above.
+Assuming that the overall cable has a resistance <i>R</i> and an inductance
+<i>L</i>, each line has an inductance equal to <i>L/3</i> and a resistance
+equal to <i>R/3</i>.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2015, by Marco Bonvini:<br/>
+Added parameter for start value of the current.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added equation that represents Joule losses
+</li>
+<li>
+October 6, 2014, by Marco Bonvini:<br/>
+Revised documentation and model.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRL;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRLC.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRLC.mo
new file mode 100644
index 0000000000..55798cde7d
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRLC.mo
@@ -0,0 +1,231 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortRLC "Model of an RLC element with two electrical ports"
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort;
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort(
+    terminal_p(phase(v(each nominal = V_nominal))),
+    terminal_n(phase(v(each nominal = V_nominal))));
+
+  parameter Modelica.Units.SI.Resistance R "Resistance at temperature T_ref";
+  parameter Modelica.Units.SI.Capacitance C "Capacity";
+  parameter Modelica.Units.SI.Inductance L "Inductance";
+  parameter Modelica.Units.SI.Temperature T_ref=298.15 "Reference temperature"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Temperature M=507.65
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Voltage Vc1_start[2]=V_nominal/sqrt(3)*{1,0}
+    "Initial voltage phasor of the capacitance located in the middle of phase 1"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter Modelica.Units.SI.Voltage Vc2_start[2]=V_nominal/sqrt(3)*{-1/2,-
+      sqrt(3)/2}
+    "Initial voltage phasor of the capacitance located in the middle of phase 1"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter Modelica.Units.SI.Voltage Vc3_start[2]=V_nominal/sqrt(3)*{-1/2,+
+      sqrt(3)/2}
+    "Initial voltage phasor of the capacitance located in the middle of phase 1"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.FixedZ_dynamic)=
+    AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Type of model (e.g., steady state, dynamic, prescribed power consumption, etc.)"
+    annotation (Evaluate=true, Dialog(group="Modeling assumption"));
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=480)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Evaluate=true, Dialog(group="Nominal conditions"));
+  OnePhase.Lines.TwoPortRLC phase1(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final C=C/3,
+    final mode=mode,
+    final V_nominal = V_nominal/sqrt(3),
+    final useHeatPort=useHeatPort,
+    Vc_start=Vc1_start) "Impedance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortRLC phase2(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final C=C/3,
+    final mode=mode,
+    final V_nominal = V_nominal/sqrt(3),
+    final useHeatPort=useHeatPort,
+    Vc_start=Vc2_start) "Impedance line 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortRLC phase3(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final C=C/3,
+    final mode=mode,
+    final V_nominal = V_nominal/sqrt(3),
+    final useHeatPort=useHeatPort,
+    Vc_start=Vc3_start) "Impedance line 3"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+equation
+  // Joule Losses
+  LossPower = phase1.LossPower + phase2.LossPower + phase3.LossPower;
+
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(phase1.heatPort, heatPort) annotation (Line(
+      points={{0,20},{0,14},{-32,14},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase3.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-40},{0,-40},{0,-100},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase2.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-10},{4.44089e-16,-16},{-32,-16},{-32,-72},{
+          4.44089e-16,-72},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Text(
+            extent={{-150,-28},{136,-60}},
+            textColor={0,0,0},
+          textString="R=%R, L=%L"),
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,32},{68,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{96,1.22003e-14}},
+          color={0,0,0},
+          origin={62,16},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-4.17982e-15,16}},
+          color={0,0,0},
+          origin={20,16},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{16,1.95937e-15}},
+          color={0,0,0},
+          origin={28,0},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{16,1.95937e-15}},
+          color={0,0,0},
+          origin={28,-4},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-2.40346e-15,16}},
+          color={0,0,0},
+          origin={20,-4},
+          rotation=180),
+        Line(
+          points={{-68,16},{-62,16},{-60,20},{-56,12},{-52,20},{-48,12},{-44,20},
+              {-40,12},{-38,16},{-34,16}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-26,22},{-14,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-14,22},{-2,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-2,22},{10,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-26,16},{10,4}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Text(
+            extent={{-144,-56},{142,-88}},
+            textColor={0,0,0},
+          textString="C=%C"),
+          Text(
+            extent={{-142,80},{138,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+RLC line model (T-model) that connects two AC three-phase
+unbalanced interfaces. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLC.png\"/>
+</p>
+
+<p>
+The model represents the lumped impedances as shown in the figure above.
+Assuming that the overall cable has a resistance <i>R</i>, an inductance
+<i>L</i>, and a capacitance <i>C</i>, each line has an inductance equal
+to <i>L/3</i>, a resistance equal to <i>R/3</i> and a capacity equal to
+<i>C/3</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 5, 2023, by Michael Wetter:<br/>
+Set nominal attribute for voltage at terminal.
+</li>
+<li>
+September 17, 2016, by Michael Wetter:<br/>
+Corrected wrong annotation to avoid an error in the pedantic model check
+in Dymola 2017 FD01 beta2.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/557\">issue 557</a>.
+</li>
+<li>
+March 9, 2015, by Marco Bonvini:<br/>
+Added parameter for start value of the voltage.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added equation that represents Joule losses
+</li>
+<li>
+October 6, 2014, by Marco Bonvini:<br/>
+Revised documentation and model.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRLC;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRLC_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRLC_N.mo
new file mode 100644
index 0000000000..1d6b1e7e11
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRLC_N.mo
@@ -0,0 +1,259 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortRLC_N
+  "Model of an RLC element with two electrical ports and neutral line cable"
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort;
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort_N(
+    terminal_p(phase(v(each nominal = V_nominal))),
+    terminal_n(phase(v(each nominal = V_nominal))));
+
+  parameter Modelica.Units.SI.Resistance R "Resistance at temperature T_ref";
+  parameter Modelica.Units.SI.Resistance Rn
+    "Resistance of neutral cable at temperature T_ref";
+  parameter Modelica.Units.SI.Capacitance C "Capacity";
+  parameter Modelica.Units.SI.Capacitance Cn "Capacityof neutral cable";
+  parameter Modelica.Units.SI.Inductance L "Inductance";
+  parameter Modelica.Units.SI.Inductance Ln "Inductance of neutral cable";
+  parameter Modelica.Units.SI.Temperature T_ref=298.15 "Reference temperature"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Temperature M=507.65
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Voltage Vc1_start[2]=V_nominal/sqrt(3)*{1,0}
+    "Initial voltage phasor of the capacitance located in the middle of phase 1"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter Modelica.Units.SI.Voltage Vc2_start[2]=V_nominal/sqrt(3)*{-1/2,-
+      sqrt(3)/2}
+    "Initial voltage phasor of the capacitance located in the middle of phase 1"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter Modelica.Units.SI.Voltage Vc3_start[2]=V_nominal/sqrt(3)*{-1/2,+
+      sqrt(3)/2}
+    "Initial voltage phasor of the capacitance located in the middle of phase 1"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.FixedZ_dynamic)=
+    AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Type of model (e.g., steady state, dynamic, prescribed power consumption, etc.)"
+    annotation (Evaluate=true, Dialog(group="Modeling assumption"));
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=480)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Evaluate=true, Dialog(group="Nominal conditions"));
+  OnePhase.Lines.TwoPortRLC phase1(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final C=C/3,
+    final mode=mode,
+    final V_nominal = V_nominal/sqrt(3),
+    final useHeatPort=useHeatPort,
+    Vc_start=Vc1_start) "Impedance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortRLC phase2(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final C=C/3,
+    final mode=mode,
+    final V_nominal = V_nominal/sqrt(3),
+    final useHeatPort=useHeatPort,
+    Vc_start=Vc2_start) "Impedance line 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortRLC phase3(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final C=C/3,
+    final mode=mode,
+    final V_nominal = V_nominal/sqrt(3),
+    final useHeatPort=useHeatPort,
+    Vc_start=Vc3_start) "Impedance line 3"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  OnePhase.Lines.TwoPortRLC neutral(
+    final T_ref=T_ref,
+    final M=M,
+    final mode=mode,
+    final V_nominal=V_nominal/sqrt(3),
+    final useHeatPort=useHeatPort,
+    final R=Rn,
+    final C=Cn,
+    final L=Ln,
+    Vc_start=-Vc1_start - Vc2_start - Vc3_start) "Neutral line RLC model"
+    annotation (Placement(transformation(extent={{-10,-64},{10,-44}})));
+equation
+  // Joule Losses
+  LossPower = phase1.LossPower + phase2.LossPower + phase3.LossPower + neutral.LossPower;
+
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(phase1.heatPort, heatPort) annotation (Line(
+      points={{0,20},{0,14},{-32,14},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase3.heatPort, heatPort) annotation (Line(
+      points={{0,-40},{-32,-40},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase2.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-10},{4.44089e-16,-16},{-32,-16},{-32,-72},{
+          4.44089e-16,-72},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(neutral.terminal_p, terminal_p.phase[4]) annotation (Line(
+      points={{10,-54},{20,-54},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(neutral.terminal_n, terminal_n.phase[4]) annotation (Line(
+      points={{-10,-54},{-20,-54},{-20,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(neutral.heatPort, heatPort) annotation (Line(
+      points={{0,-64},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Text(
+            extent={{-150,-28},{136,-60}},
+            textColor={0,0,0},
+          textString="R=%R, L=%L"),
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,32},{68,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{96,1.22003e-14}},
+          color={0,0,0},
+          origin={62,16},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-4.17982e-15,16}},
+          color={0,0,0},
+          origin={20,16},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{16,1.95937e-15}},
+          color={0,0,0},
+          origin={28,0},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{16,1.95937e-15}},
+          color={0,0,0},
+          origin={28,-4},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{-2.40346e-15,16}},
+          color={0,0,0},
+          origin={20,-4},
+          rotation=180),
+        Line(
+          points={{-68,16},{-62,16},{-60,20},{-56,12},{-52,20},{-48,12},{-44,20},
+              {-40,12},{-38,16},{-34,16}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-26,22},{-14,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-14,22},{-2,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-2,22},{10,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-26,16},{10,4}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Text(
+            extent={{-144,-56},{142,-88}},
+            textColor={0,0,0},
+          textString="C=%C"),
+          Text(
+            extent={{-142,80},{138,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+RLC line model (T-model) that connects two AC three-phase
+unbalanced interfaces with neutral line. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLC_N.png\"/>
+</p>
+
+<p>
+The model represents the lumped impedances as shown in the figure above.
+Assuming that the overall cable has a resistance <i>R</i>, an inductance
+<i>L</i>, and a capacitance <i>C</i>, each line has an inductance equal
+to <i>L/3</i>, a resistance equal to <i>R/3</i> and a capacity equal to
+<i>C/3</i>.
+</p>
+<p>
+The resistance, capacitance and inductance of the neutral cable are defined separately using the parameters
+<code>Rn</code> <code>Cn</code>, and <code>Ln</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 5, 2023, by Michael Wetter:<br/>
+Set nominal attribute for voltage at terminal.
+</li>
+<li>
+September 17, 2016, by Michael Wetter:<br/>
+Corrected wrong annotation to avoid an error in the pedantic model check
+in Dymola 2017 FD01 beta2.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/557\">issue 557</a>.
+</li>
+<li>
+March 9, 2015, by Marco Bonvini:<br/>
+Added parameter for start value of the voltage.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added model and user guide
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRLC_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRL_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRL_N.mo
new file mode 100644
index 0000000000..b62df319f0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortRL_N.mo
@@ -0,0 +1,204 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortRL_N
+  "Model of a resistive-inductive element with two electrical ports and neutral line cable"
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort;
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort_N;
+  parameter Modelica.Units.SI.Resistance R "Resistance at temperature T_ref";
+  parameter Modelica.Units.SI.Resistance Rn
+    "Resistance of neutral cable at temperature T_ref";
+  parameter Modelica.Units.SI.Temperature T_ref=298.15 "Reference temperature"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Temperature M=507.65
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Inductance L "Inductance";
+  parameter Modelica.Units.SI.Inductance Ln "Inductance of neutral cable";
+  parameter Modelica.Units.SI.Current i1_start[2]={0,0}
+    "Initial current phasor of phase 1 (positive if entering from terminal p)"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter Modelica.Units.SI.Current i2_start[2]={0,0}
+    "Initial current phasor of phase 2 (positive if entering from terminal p)"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter Modelica.Units.SI.Current i3_start[2]={0,0}
+    "Initial current phasor of phase 3 (positive if entering from terminal p)"
+    annotation (Dialog(enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic)));
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.FixedZ_dynamic) = AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Type of model (e.g., steady state, dynamic, prescribed power consumption, etc.)"
+    annotation (Evaluate=true, Dialog(group="Modeling assumption"));
+  OnePhase.Lines.TwoPortRL  phase1(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=mode,
+    final useHeatPort=useHeatPort,
+    i_start=i1_start) "Impedance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortRL phase2(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=mode,
+    final useHeatPort=useHeatPort,
+    i_start=i2_start) "Impedance line 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortRL phase3(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final L=L/3,
+    final mode=mode,
+    final useHeatPort=useHeatPort,
+    i_start=i3_start) "Impedance line 3"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  OnePhase.Lines.TwoPortRL neutral(
+    final T_ref=T_ref,
+    final M=M,
+    final mode=mode,
+    final useHeatPort=useHeatPort,
+    final R=Rn,
+    final L=Ln,
+    i_start=-i1_start - i2_start - i3_start) "neutral cable RL model"
+    annotation (Placement(transformation(extent={{-10,-66},{10,-46}})));
+equation
+  // Joule Losses
+  LossPower = phase1.LossPower + phase2.LossPower + phase3.LossPower + neutral.LossPower;
+
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(phase1.heatPort, heatPort) annotation (Line(
+      points={{0,20},{0,14},{-32,14},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase3.heatPort, heatPort) annotation (Line(
+      points={{0,-40},{0,-44},{-32,-44},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase2.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-10},{4.44089e-16,-16},{-32,-16},{-32,-72},{
+          4.44089e-16,-72},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(neutral.heatPort, heatPort) annotation (Line(
+      points={{0,-66},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(neutral.terminal_p, terminal_p.phase[4]) annotation (Line(
+      points={{10,-56},{20,-56},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(neutral.terminal_n, terminal_n.phase[4]) annotation (Line(
+      points={{-10,-56},{-20,-56},{-20,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Text(
+            extent={{-150,-28},{136,-60}},
+            textColor={0,0,0},
+          textString="R=%R, L=%L"),
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,32},{68,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{66,8.0824e-15}},
+          color={0,0,0},
+          origin={52,0},
+          rotation=180),
+        Line(
+          points={{-48,0},{-42,0},{-40,4},{-36,-4},{-32,4},{-28,-4},{-24,4},{-20,
+              -4},{-18,0},{-14,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-6,6},{6,-6}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{6,6},{18,-6}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{18,6},{30,-6}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-6,0},{30,-12}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Text(
+            extent={{-142,80},{138,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+Resistive-inductive model that connects two AC three-phase
+unbalanced interfaces with neutral line. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRL_N.png\"/>
+</p>
+
+<p>
+The model represents the lumped impedances as shown in the figure above.
+Assuming that the overall cable has a resistance <i>R</i> and an inductance
+<i>L</i>, each line has an inductance equal to <i>L/3</i> and a resistance
+equal to <i>R/3</i>.
+</p>
+<p>
+The resistance and the inductance of the neutral cable are defined separately using the parameters
+<code>Rn</code> and <code>Ln</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2015, by Marco Bonvini:<br/>
+Added parameter for start value of the current.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added model and user guide
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRL_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortResistance.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortResistance.mo
new file mode 100644
index 0000000000..65d2b05f83
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortResistance.mo
@@ -0,0 +1,120 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortResistance "Model of a resistance with two electrical ports"
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort;
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort;
+  parameter Modelica.Units.SI.Temperature T_ref=298.15 "Reference temperature"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Temperature M=507.65
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Resistance R "Resistance at temperature T_ref";
+  OnePhase.Lines.TwoPortResistance  phase1(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final useHeatPort=useHeatPort) "Resistance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortResistance phase2(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final useHeatPort=useHeatPort) "Resistance line 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortResistance phase3(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final useHeatPort=useHeatPort) "Resistance line 3"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+equation
+  // Joule Losses
+  LossPower = phase1.LossPower + phase2.LossPower + phase3.LossPower;
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(phase1.heatPort, heatPort) annotation (Line(
+      points={{0,20},{0,14},{-32,14},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase3.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-40},{0,-40},{0,-100},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase2.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-10},{4.44089e-16,-16},{-32,-16},{-32,-72},{
+          4.44089e-16,-72},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Text(
+            extent={{-140,-28},{138,-60}},
+            textColor={0,0,0},
+          textString="R=%R"),
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,32},{68,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Text(
+            extent={{-142,80},{138,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+Resistive model that connects two AC three-phase
+unbalanced interfaces. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortR.png\"/>
+</p>
+
+<p>
+The model represents the lumped resistance as shown in the figure above.
+Assuming that the resistance <i>R</i> is the overall resistance of the cable,
+each line has a resistance equal to <i>R/3</i>.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added equation that represents Joule losses
+</li>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Added model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortResistance;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortResistance_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortResistance_N.mo
new file mode 100644
index 0000000000..4518b012bd
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/TwoPortResistance_N.mo
@@ -0,0 +1,140 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines;
+model TwoPortResistance_N
+  "Model of a resistance with two electrical ports and neutral cable"
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort;
+  extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.TwoPort_N;
+  parameter Modelica.Units.SI.Temperature T_ref=298.15 "Reference temperature"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Temperature M=507.65
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Resistance R "Resistance at temperature T_ref";
+  parameter Modelica.Units.SI.Resistance Rn
+    "Resistance of neutral cable at temperature T_ref";
+  OnePhase.Lines.TwoPortResistance  phase1(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final useHeatPort=useHeatPort) "Resistance line 1"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  OnePhase.Lines.TwoPortResistance phase2(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final useHeatPort=useHeatPort) "Resistance line 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  OnePhase.Lines.TwoPortResistance phase3(
+    final T_ref=T_ref,
+    final M=M,
+    final R=R/3,
+    final useHeatPort=useHeatPort) "Resistance line 3"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  OnePhase.Lines.TwoPortResistance neutral(
+    final T_ref=T_ref,
+    final M=M,
+    final useHeatPort=useHeatPort,
+    final R=Rn) "Resistance neutral cable"
+    annotation (Placement(transformation(extent={{-10,-64},{10,-44}})));
+equation
+  // Joule Losses
+  LossPower = phase1.LossPower + phase2.LossPower + phase3.LossPower + neutral.LossPower;
+  connect(terminal_n.phase[1], phase1.terminal_n) annotation (Line(
+      points={{-100,0},{-20,0},{-20,30},{-10,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[2], phase2.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal_n.phase[3], phase3.terminal_n) annotation (Line(
+      points={{-100,4.44089e-16},{-20,4.44089e-16},{-20,-30},{-10,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase1.terminal_p, terminal_p.phase[1]) annotation (Line(
+      points={{10,30},{20,30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase2.terminal_p, terminal_p.phase[2]) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(phase3.terminal_p, terminal_p.phase[3]) annotation (Line(
+      points={{10,-30},{20,-30},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(phase1.heatPort, heatPort) annotation (Line(
+      points={{0,20},{0,14},{-32,14},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase3.heatPort, heatPort) annotation (Line(
+      points={{0,-40},{-32,-40},{-32,-72},{0,-72},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(phase2.heatPort, heatPort) annotation (Line(
+      points={{4.44089e-16,-10},{4.44089e-16,-16},{-32,-16},{-32,-72},{
+          4.44089e-16,-72},{4.44089e-16,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(neutral.heatPort, heatPort) annotation (Line(
+      points={{0,-64},{0,-100}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(neutral.terminal_p, terminal_p.phase[4]) annotation (Line(
+      points={{10,-54},{20,-54},{20,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(neutral.terminal_n, terminal_n.phase[4]) annotation (Line(
+      points={{-10,-54},{-20,-54},{-20,0},{-100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="line",
+ Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                               graphics={
+          Text(
+            extent={{-140,-28},{138,-60}},
+            textColor={0,0,0},
+          textString="R=%R"),
+          Line(points={{-92,0},{-72,0}}, color={0,0,0}),
+          Line(points={{68,0},{88,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-72,32},{68,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Text(
+            extent={{-142,80},{138,40}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+Resistive model that connects two AC three-phase
+unbalanced interfaces with neutral line. This model can be used to represent a
+cable in a three-phase unbalanced AC system.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortR_N.png\"/>
+</p>
+
+<p>
+The model represents the lumped resistance as shown in the figure above.
+Assuming that the resistance <i>R</i> is the overall resistance of the cable,
+each line has a resistance equal to <i>R/3</i>.
+</p>
+<p>
+The resistance of the neutral cable is defined separately using the parameter
+<code>Rn</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added model and user guide
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortResistance_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/package.mo
new file mode 100644
index 0000000000..9cd633f419
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/package.mo
@@ -0,0 +1,40 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced;
+package Lines "Package with transmission line models for three-phase unbalanced AC systems"
+  extends Modelica.Icons.Package;
+
+
+annotation (Icon(graphics={
+      Ellipse(
+        extent={{42,6},{18,-30}},
+        lineColor={0,0,0},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),
+      Line(
+        points={{30,6},{-52,6},{-62,6},{-70,-12},{-62,-30},{-50,-30},{30,-30}},
+        color={0,0,0},
+        smooth=Smooth.Bezier),
+      Line(
+        points={{-68,-12},{-86,-12}},
+        color={0,0,0},
+        smooth=Smooth.None),
+      Line(
+        points={{56,-12},{30,-12}},
+        color={0,0,0},
+        smooth=Smooth.None)}), Documentation(revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Revised package: added examples, checked results and added unit tests.
+</li>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains models for transmission lines and electrical networks
+of AC three-phase unbalanced systems.
+</p>
+</html>"));
+end Lines;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/package.order
new file mode 100644
index 0000000000..7a0a209c23
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Lines/package.order
@@ -0,0 +1,17 @@
+Line
+Line_N
+Network
+Network_N
+TwoPortInductance
+TwoPortInductance_N
+TwoPortMatrixRL
+TwoPortMatrixRLC
+TwoPortMatrixRLC_N
+TwoPortMatrixRL_N
+TwoPortRL
+TwoPortRLC
+TwoPortRLC_N
+TwoPortRL_N
+TwoPortResistance
+TwoPortResistance_N
+Examples
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/BaseImpedance.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/BaseImpedance.mo
new file mode 100644
index 0000000000..0ea626023c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/BaseImpedance.mo
@@ -0,0 +1,302 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses;
+partial model BaseImpedance
+  "Partial model of a three-phase unbalanced impedance"
+  extends AixLib.Electrical.Interfaces.PartialPluggableUnbalanced;
+  replaceable AixLib.Electrical.AC.OnePhase.Loads.Impedance
+    load1(
+    inductive=inductive,
+    R=R,
+    L=L,
+    C=C,
+    use_R_in=use_R_in,
+    RMin=RMin,
+    RMax=RMax,
+    use_C_in=use_C_in,
+    CMin=CMin,
+    CMax=CMax,
+    use_L_in=use_L_in,
+    LMin=LMin,
+    LMax=LMax)
+    if plugPhase1 "Load 1"
+    annotation (Placement(transformation(extent={{-10,30},{10,50}})));
+  replaceable AixLib.Electrical.AC.OnePhase.Loads.Impedance
+    load2(
+    inductive=inductive,
+    R=R,
+    L=L,
+    C=C,
+    use_R_in=use_R_in,
+    RMin=RMin,
+    RMax=RMax,
+    use_C_in=use_C_in,
+    CMin=CMin,
+    CMax=CMax,
+    use_L_in=use_L_in,
+    LMin=LMin,
+    LMax=LMax)
+    if plugPhase2 "Load 2"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  replaceable AixLib.Electrical.AC.OnePhase.Loads.Impedance
+    load3(
+    inductive=inductive,
+    R=R,
+    L=L,
+    C=C,
+    use_R_in=use_R_in,
+    RMin=RMin,
+    RMax=RMax,
+    use_C_in=use_C_in,
+    CMin=CMin,
+    CMax=CMax,
+    use_L_in=use_L_in,
+    LMin=LMin,
+    LMax=LMax)
+    if plugPhase3 "Load 3"
+    annotation (Placement(transformation(extent={{-10,-50},{10,-30}})));
+  parameter AixLib.Electrical.Types.LoadConnection loadConn=
+    AixLib.Electrical.Types.LoadConnection.wye_to_wyeg
+    "Type of load connection (Yg or D)";
+  parameter Boolean inductive=true
+    "If =true the load is inductive, otherwise it is capacitive"
+    annotation (Evaluate=true, choices(
+      choice=true "Inductive",
+      choice=false "Capacitive",
+      __Dymola_radioButtons=true));
+  parameter Modelica.Units.SI.Resistance R(
+    start=1,
+    min=0) = 1 "Resistance" annotation (Dialog(enable=not use_R_in));
+  parameter Modelica.Units.SI.Inductance L(
+    start=0,
+    min=0) = 0 "Inductance"
+    annotation (Dialog(enable=inductive and (not use_L_in)));
+  parameter Modelica.Units.SI.Capacitance C(
+    start=0,
+    min=0) = 0 "Capacitance"
+    annotation (Dialog(enable=(not inductive) and (not use_C_in)));
+  parameter Boolean use_R_in = false "if true, R is specified by an input"
+     annotation(Evaluate=true, Dialog(tab = "Variable load", group="Resistance"));
+  parameter Modelica.Units.SI.Resistance RMin(
+    start=R,
+    min=Modelica.Constants.eps) = 1e-4 "Minimum value of the resistance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_R_in,
+      tab="Variable load",
+      group="Resistance"));
+  parameter Modelica.Units.SI.Resistance RMax(
+    start=R,
+    min=Modelica.Constants.eps) = 1e2 "Maximum value of the resistance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_R_in,
+      tab="Variable load",
+      group="Resistance"));
+  parameter Boolean use_C_in = false "if true, C is specified by an input"
+    annotation(Evaluate=true, Dialog(tab = "Variable load", group="Capacitance"));
+  parameter Modelica.Units.SI.Capacitance CMin(
+    start=C,
+    min=Modelica.Constants.eps) = 1e-4 "Minimum value of the capacitance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_C_in,
+      tab="Variable load",
+      group="Capacitance"));
+  parameter Modelica.Units.SI.Capacitance CMax(
+    start=C,
+    min=Modelica.Constants.eps) = 1e2 "Maximum value of the capacitance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_C_in,
+      tab="Variable load",
+      group="Capacitance"));
+  parameter Boolean use_L_in = false "if true, L is specified by an input"
+     annotation(Evaluate=true, Dialog(tab = "Variable load", group="Inductance"));
+  parameter Modelica.Units.SI.Inductance LMin(
+    start=L,
+    min=Modelica.Constants.eps) = 1e-4 "Minimum value of the inductance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_L_in,
+      tab="Variable load",
+      group="Inductance"));
+  parameter Modelica.Units.SI.Inductance LMax(
+    start=L,
+    min=Modelica.Constants.eps) = 1e2 "Maximum value of the inductance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_L_in,
+      tab="Variable load",
+      group="Inductance"));
+  Modelica.Blocks.Interfaces.RealInput y_R(min=0, max=1) if use_R_in
+    "Input that sepecifies variable R"
+    annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=270,
+        origin={-40,100})));
+  Modelica.Blocks.Interfaces.RealInput y_C(min=0, max=1) if use_C_in
+    "Input that sepecifies variable C"
+    annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=270,
+        origin={0,100})));
+  Modelica.Blocks.Interfaces.RealInput y_L(min=0, max=1) if use_L_in
+    "Input that sepecifies variable L"
+    annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=270,
+        origin={40,100})));
+
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToDelta
+    wyeToDelta if (loadConn == AixLib.Electrical.Types.LoadConnection.wye_to_delta)
+    "Wye to delta load connection"
+    annotation (Placement(transformation(extent={{-64,0},{-44,20}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.WyeToWyeGround
+    wyeToWyeGround if (loadConn == AixLib.Electrical.Types.LoadConnection.wye_to_wyeg)
+    "Wye to grounded wye connection"
+    annotation (Placement(transformation(extent={{-64,-20},{-44,0}})));
+protected
+  Interfaces.Adapter3to3 adaDel
+    if (loadConn == AixLib.Electrical.Types.LoadConnection.wye_to_delta)
+    "Adapter"
+    annotation (Placement(transformation(extent={{-40,-50},{-60,-30}})));
+  Interfaces.Adapter3to3 adaWye
+    if (loadConn == AixLib.Electrical.Types.LoadConnection.wye_to_wyeg)
+    "Adapter"
+    annotation (Placement(transformation(extent={{-40,-80},{-60,-60}})));
+equation
+
+  // Conditional connections to load 1
+  if plugPhase1 then
+    if use_R_in then
+      connect(y_R, load1.y_R) annotation (Line(
+      points={{-40,100},{-40,60},{-4,60},{-4,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if use_C_in then
+      connect(y_C, load1.y_C) annotation (Line(
+      points={{8.88178e-16,100},{8.88178e-16,75},{0,75},{0,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if use_L_in then
+      connect(y_L, load1.y_L) annotation (Line(
+      points={{40,100},{40,60},{4,60},{4,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+  end if;
+  // Conditional connections to load 2
+  if plugPhase2 then
+    if use_R_in then
+      connect(y_R, load2.y_R) annotation (Line(
+      points={{-40,100},{-40,20},{-4,20},{-4,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if use_L_in then
+      connect(y_L, load2.y_L) annotation (Line(
+      points={{40,100},{40,10},{4,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if use_C_in then
+      connect(y_C, load2.y_C) annotation (Line(
+        points={{0,100},{0,70},{-20,70},{-20,24},{0,24},{0,10}},
+        color={0,0,127},
+        smooth=Smooth.None));
+    end if;
+  end if;
+
+  // Conditional connections to load 3
+  if plugPhase3 then
+    if use_R_in then
+      connect(y_R, load3.y_R) annotation (Line(
+      points={{-40,100},{-40,-20},{-4,-20},{-4,-30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if use_C_in then
+      connect(y_C, load3.y_C) annotation (Line(
+        points={{0,100},{0,70},{-20,70},{-20,-16},{0,-16},{0,-30}},
+        color={0,0,127},
+        smooth=Smooth.None));
+    end if;
+    if use_L_in then
+      connect(y_L, load3.y_L) annotation (Line(
+        points={{40,100},{40,-20},{4,-20},{4,-30}},
+        color={0,0,127},
+        smooth=Smooth.None));
+    end if;
+  end if;
+
+  // Connection of the single loads to the 3phases connector
+  if plugPhase1 then
+    connect(load1.terminal, adaDel.terminals[1]) annotation (Line(points={{-10,40},
+            {-26,40},{-26,-40.5333},{-40,-40.5333}},
+                                                   color={0,120,120}));
+    connect(load1.terminal, adaWye.terminals[1]) annotation (Line(points={{-10,40},
+            {-26,40},{-26,-70.5333},{-40,-70.5333}},
+                                                   color={0,120,120}));
+  end if;
+
+  if plugPhase2 then
+    connect(load2.terminal, adaDel.terminals[2]) annotation (Line(points={{-10,0},
+            {-22,0},{-22,-40},{-40,-40}}, color={0,120,120}));
+    connect(load2.terminal, adaWye.terminals[2]) annotation (Line(points={{-10,0},
+            {-22,0},{-22,-70},{-40,-70}}, color={0,120,120}));
+  end if;
+  if plugPhase3 then
+    connect(load3.terminal, adaDel.terminals[3]) annotation (Line(points={{-10,-40},
+            {-20,-40},{-20,-40},{-30,-40},{-30,-39.4667},{-40,-39.4667}},
+                                                              color={0,120,120}));
+    connect(load3.terminal, adaWye.terminals[3]) annotation (Line(points={{-10,-40},
+            {-20,-40},{-20,-69.4667},{-40,-69.4667}},
+                                                    color={0,120,120}));
+  end if;
+
+  connect(adaDel.terminal, wyeToDelta.delta) annotation (Line(points={{-60,-40},
+          {-64,-40},{-64,-20},{-28,-20},{-28,10},{-44,10}}, color={0,120,120}));
+  connect(adaWye.terminal, wyeToWyeGround.wyeg) annotation (Line(points={{-60,-70},
+          {-66,-70},{-66,-18},{-30,-18},{-30,-10},{-44,-10}}, color={0,120,120}));
+
+  annotation (    Documentation(info="<html>
+<p>
+This model represents a partial interface for a three-phase AC
+unbalanced impedance.
+</p>
+<p>
+The model can be configured in order to represent different type of
+impedances as well as configurations.
+</p>
+<p>
+The loads can be connected either in wye (Y) or delta (D) configuration.
+The parameter <code>loadConn</code> can be used for such a purpose.
+</p>
+<p>
+The model has three impedances that can be either connected in Y or
+D configuration. The parameter <code>loadConn</code> can be used for
+such a purpose. The Boolean parameter <code>inductive</code> can be selected
+to specify the type of impedance.
+</p>
+<p>
+The impedances on each phase can be removed using the boolean flags
+<code>plugPhase1</code>, <code>plugPhase2</code>, and <code>plugPhase3</code>.
+These parameters can be used to generate unbalanced loads.
+</p>
+<p>
+The values of the impedances are computed starting from the parameters <code>R</code>,
+<code>L</code>, and <code>C</code>. Depending on the values of the boolean flag
+<code>inductive</code> some of these parameters may be disabled. There are additional
+flags <code>use_R_in</code>, <code>use_L_in</code>, and <code>use_C_in</code> that can
+be used to specify time varying impedances.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapters for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Created model from previus version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BaseImpedance;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/BaseLoadCtrl.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/BaseLoadCtrl.mo
new file mode 100644
index 0000000000..f16e69e324
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/BaseLoadCtrl.mo
@@ -0,0 +1,394 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses;
+partial model BaseLoadCtrl
+  "Partial model of a three-phase unbalanced load with voltage controllers"
+  extends AixLib.Electrical.Interfaces.PartialPluggableUnbalanced;
+  parameter AixLib.Electrical.Types.LoadConnection loadConn=
+    AixLib.Electrical.Types.LoadConnection.wye_to_wyeg
+    "Type of load connection (Yg or D)";
+  parameter Boolean linearized = false
+    "If =true introduce a linearization in the load" annotation(Dialog(group="Modeling assumption"));
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.VariableZ_y_input)=
+    AixLib.Electrical.Types.Load.FixedZ_steady_state "Parameters that specifies the mode of the load (e.g., steady state,
+    dynamic, prescribed power consumption, etc.)" annotation(Dialog(group="Modeling assumption"));
+
+  parameter Modelica.Units.SI.Power P_nominal=0
+    "Nominal power (negative if consumed, positive if generated)" annotation (
+      Dialog(group="Nominal conditions", enable=mode <> AixLib.Electrical.Types.Load.VariableZ_P_input));
+
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=480)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Dialog(group="Nominal conditions"));
+  parameter Boolean voltageCtrl = false "This flag enables the voltage control"
+                                            annotation(Evaluate=true, Dialog(group="Voltage CTRL"));
+  parameter Real vThresh(min=0.0, max=1.0) = 0.1
+    "Threshold that activates voltage ctrl (ratio of nominal voltage)" annotation(Dialog(group="Voltage CTRL",
+        enable = voltageCtrl));
+  parameter Modelica.Units.SI.Time tDelay=300
+    "Time to wait before plugging the load again after disconnection"
+    annotation (Dialog(group="Voltage CTRL", enable=voltageCtrl));
+  parameter Types.InitMode initMode=AixLib.Electrical.Types.InitMode.zero_current
+    "Initialization mode for homotopy operator"
+    annotation (Dialog(tab="Initialization"));
+  replaceable AixLib.Electrical.Interfaces.Load load1(
+    redeclare package PhaseSystem = AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n terminal,
+    final linearized=linearized,
+    final mode=mode,
+    final P_nominal = P_nominal,
+    final V_nominal=V_nominal/sqrt(3),
+    final initMode=initMode)
+    if plugPhase1 "Load 1"
+    annotation (Placement(transformation(extent={{-10,40},{10,60}})));
+  replaceable AixLib.Electrical.Interfaces.Load load2(
+    redeclare package PhaseSystem = AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n terminal,
+    final linearized=linearized,
+    final mode=mode,
+    final P_nominal = P_nominal,
+    final V_nominal=V_nominal/sqrt(3),
+    final initMode=initMode)
+    if plugPhase2 "Load 2"
+    annotation (Placement(transformation(extent={{-10,-30},{10,-10}})));
+  replaceable AixLib.Electrical.Interfaces.Load load3(
+    redeclare package PhaseSystem = AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n terminal,
+    final linearized=linearized,
+    final mode=mode,
+    final P_nominal = P_nominal,
+    final V_nominal=V_nominal/sqrt(3),
+    final initMode=initMode)
+    if plugPhase3 "Load 3"
+    annotation (Placement(transformation(extent={{-10,-98},{10,-78}})));
+  Modelica.Blocks.Interfaces.RealInput y1  if plugPhase1 and
+    mode == AixLib.Electrical.Types.Load.VariableZ_y_input
+    "Fraction of the nominal power consumed"                       annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,80}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,80})));
+  Modelica.Blocks.Interfaces.RealInput Pow1(unit="W") if plugPhase1 and
+    mode == AixLib.Electrical.Types.Load.VariableZ_P_input "Power consumed"
+                                           annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,80}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,80})));
+  Modelica.Blocks.Interfaces.RealInput y2 if plugPhase2 and
+    mode == AixLib.Electrical.Types.Load.VariableZ_y_input
+    "Fraction of the nominal power consumed"                       annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,0}), iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,0})));
+  Modelica.Blocks.Interfaces.RealInput Pow2(unit="W") if plugPhase2 and
+    mode == AixLib.Electrical.Types.Load.VariableZ_P_input "Power consumed"
+                                           annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,0}), iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,0})));
+  Modelica.Blocks.Interfaces.RealInput y3 if plugPhase3 and
+    mode == AixLib.Electrical.Types.Load.VariableZ_y_input
+    "Fraction of the nominal power consumed"                       annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,-80}),
+                         iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,-80})));
+  Modelica.Blocks.Interfaces.RealInput Pow3(unit="W") if plugPhase3 and
+    mode == AixLib.Electrical.Types.Load.VariableZ_P_input "Power consumed"
+                                           annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,-80}),
+                         iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={120,-80})));
+  AixLib.Electrical.Utilities.VoltageControl vCTRL_1(
+    redeclare package PhaseSystem = AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n terminal,
+    vThresh=vThresh,
+    tDelay=tDelay,
+    V_nominal=V_nominal/sqrt(3))
+    if plugPhase1 and voltageCtrl "Voltage controller for load 1"
+    annotation (Placement(transformation(extent={{10,80},{30,100}})));
+  Modelica.Blocks.Math.Product cmd1 if plugPhase1 and voltageCtrl
+    "Block that impose voltage ctrl"
+    annotation (Placement(transformation(extent={{56,56},{36,76}})));
+  AixLib.Electrical.Utilities.VoltageControl vCTRL_2(
+    redeclare package PhaseSystem = AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n terminal,
+    vThresh=vThresh,
+    tDelay=tDelay,
+    V_nominal=V_nominal/sqrt(3))
+    if plugPhase2 and voltageCtrl "Voltage controller for load 2"
+    annotation (Placement(transformation(extent={{10,10},{30,30}})));
+  Modelica.Blocks.Math.Product cmd2 if plugPhase2 and voltageCtrl
+    "Block that impose voltage ctrl"
+    annotation (Placement(transformation(extent={{56,-16},{36,4}})));
+  AixLib.Electrical.Utilities.VoltageControl vCTRL_3(
+    redeclare package PhaseSystem = AixLib.Electrical.PhaseSystems.OnePhase,
+    redeclare AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n terminal,
+    vThresh=vThresh,
+    tDelay=tDelay,
+    V_nominal=V_nominal/sqrt(3))
+    if plugPhase3 and voltageCtrl "Voltage controller for load 3"
+    annotation (Placement(transformation(extent={{10,-60},{30,-40}})));
+  Modelica.Blocks.Math.Product cmd3 if plugPhase3 and voltageCtrl
+    "Block that impose voltage ctrl"
+    annotation (Placement(transformation(extent={{56,-80},{36,-60}})));
+  Interfaces.WyeToDelta
+    wyeToDelta if (loadConn == AixLib.Electrical.Types.LoadConnection.wye_to_delta)
+    "Wye to delta load connection"
+    annotation (Placement(transformation(extent={{-54,0},{-34,20}})));
+  Interfaces.WyeToWyeGround
+    wyeToWyeGround if (loadConn == AixLib.Electrical.Types.LoadConnection.wye_to_wyeg)
+    "Wye to wye grounded connection"
+    annotation (Placement(transformation(extent={{-54,-20},{-34,0}})));
+protected
+  Interfaces.Adapter3to3 adaDel
+    if (loadConn == AixLib.Electrical.Types.LoadConnection.wye_to_delta)
+    "Adapter"
+    annotation (Placement(transformation(extent={{-40,-50},{-60,-30}})));
+  Interfaces.Adapter3to3 adaWye
+    if (loadConn == AixLib.Electrical.Types.LoadConnection.wye_to_wyeg)
+    "Adapter"
+    annotation (Placement(transformation(extent={{-40,-80},{-60,-60}})));
+equation
+  // Connections enabled when the input provided is y (between 0 and 1)
+  if mode==AixLib.Electrical.Types.Load.VariableZ_y_input then
+    if plugPhase1 and voltageCtrl then
+      connect(cmd1.y, load1.y) annotation (Line(
+        points={{35,66},{20,66},{20,50},{10,50}},
+        color={0,0,127},
+        smooth=Smooth.None));
+      connect(cmd1.u2, y1) annotation (Line(
+        points={{58,60},{90,60},{90,80},{120,80}},
+        color={0,0,127},
+        smooth=Smooth.None));
+    end if;
+    if plugPhase1 and not voltageCtrl then
+      connect(y1, load1.y) annotation (Line(
+        points={{120,80},{66,80},{66,50},{10,50}},
+        color={0,0,127},
+        smooth=Smooth.None));
+    end if;
+
+    if plugPhase2 and voltageCtrl then
+      connect(cmd2.y, load2.y) annotation (Line(
+      points={{35,-6},{23,-6},{23,-20},{10,-20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+      connect(cmd2.u2, y2) annotation (Line(
+      points={{58,-12},{72,-12},{72,0},{120,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if plugPhase2 and not voltageCtrl then
+      connect(y2, load2.y) annotation (Line(
+      points={{120,0},{66,0},{66,-20},{10,-20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+
+    if plugPhase3 and voltageCtrl then
+      connect(cmd3.y, load3.y) annotation (Line(
+      points={{35,-70},{24,-70},{24,-88},{10,-88}},
+      color={0,0,127},
+      smooth=Smooth.None));
+      connect(cmd3.u2, y3) annotation (Line(
+      points={{58,-76},{72,-76},{72,-80},{120,-80}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if plugPhase3 and not voltageCtrl then
+      connect(y3, load3.y) annotation (Line(
+      points={{120,-80},{72,-80},{72,-88},{10,-88}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+  end if;
+
+  // Connections enabled when the input provided is the power
+  if mode==AixLib.Electrical.Types.Load.VariableZ_P_input then
+    if plugPhase1 and voltageCtrl then
+      connect(cmd1.y, load1.Pow) annotation (Line(
+        points={{35,66},{20,66},{20,50},{10,50}},
+        color={0,0,127},
+        smooth=Smooth.None));
+      connect(cmd1.u2, Pow1) annotation (Line(
+        points={{58,60},{82,60},{82,80},{120,80}},
+        color={0,0,127},
+        smooth=Smooth.None));
+    end if;
+    if plugPhase1 and not voltageCtrl then
+      connect(Pow1, load1.Pow) annotation (Line(
+        points={{120,80},{70,80},{70,50},{10,50}},
+        color={0,0,127},
+        smooth=Smooth.None));
+    end if;
+
+    if plugPhase2 and voltageCtrl then
+      connect(cmd2.y, load2.Pow) annotation (Line(
+      points={{35,-6},{23,-6},{23,-20},{10,-20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+      connect(cmd2.u2, Pow2) annotation (Line(
+      points={{58,-12},{72,-12},{72,0},{120,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if plugPhase2 and not voltageCtrl then
+      connect(Pow2, load2.Pow) annotation (Line(
+      points={{120,0},{72,0},{72,-20},{10,-20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+
+    if plugPhase3 and voltageCtrl then
+      connect(cmd3.y, load3.Pow) annotation (Line(
+      points={{35,-70},{24,-70},{24,-88},{10,-88}},
+      color={0,0,127},
+      smooth=Smooth.None));
+      connect(cmd3.u2, Pow3) annotation (Line(
+      points={{58,-76},{72,-76},{72,-80},{120,-80}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+    if plugPhase3 and not voltageCtrl then
+      connect(Pow3, load3.Pow) annotation (Line(
+      points={{120,-80},{72,-80},{72,-88},{10,-88}},
+      color={0,0,127},
+      smooth=Smooth.None));
+    end if;
+  end if;
+
+  // Connections enabled when phase 1 is plugged and voltage ctrl activated
+  if plugPhase1 and voltageCtrl then
+    connect(load1.terminal, vCTRL_1.terminal)        annotation (Line(
+      points={{-10,50},{-20,50},{-20,90},{10,90}},
+      color={0,120,120},
+      smooth=Smooth.None));
+    connect(vCTRL_1.y, cmd1.u1)        annotation (Line(
+        points={{30.6,90},{70,90},{70,72},{58,72}},
+        color={0,0,127},
+        smooth=Smooth.None));
+  end if;
+
+  if plugPhase2 and voltageCtrl then
+    connect(load2.terminal, vCTRL_2.terminal) annotation (Line(
+      points={{-10,-20},{-20,-20},{-20,20},{10,20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+    connect(vCTRL_2.y, cmd2.u1) annotation (Line(
+        points={{30.6,20},{66,20},{66,0},{58,0}},
+        color={0,0,127},
+        smooth=Smooth.None));
+  end if;
+
+  if plugPhase3 and voltageCtrl then
+    connect(load3.terminal, vCTRL_3.terminal) annotation (Line(
+      points={{-10,-88},{-20,-88},{-20,-50},{10,-50}},
+      color={0,120,120},
+      smooth=Smooth.None));
+    connect(vCTRL_3.y, cmd3.u1) annotation (Line(
+        points={{30.6,-50},{66,-50},{66,-64},{58,-64}},
+        color={0,0,127},
+        smooth=Smooth.None));
+  end if;
+
+  // Connection of the single loads to the 3phases connector
+  if plugPhase1 then
+    connect(load1.terminal, adaDel.terminals[1]) annotation (Line(points={{-10,50},
+            {-26,50},{-26,-39.4667},{-40.2,-39.4667}},
+                                                   color={0,120,120}));
+    connect(load1.terminal, adaWye.terminals[1]) annotation (Line(points={{-10,50},
+            {-26,50},{-26,-69.4667},{-40.2,-69.4667}},
+                                                   color={0,120,120}));
+  end if;
+
+  if plugPhase2 then
+    connect(load2.terminal, adaDel.terminals[2]) annotation (Line(points={{-10,-20},
+            {-22,-20},{-22,-40},{-40.2,-40}},
+                                          color={0,120,120}));
+    connect(load2.terminal, adaWye.terminals[2]) annotation (Line(points={{-10,-20},
+            {-22,-20},{-22,-70},{-40.2,-70}},
+                                          color={0,120,120}));
+  end if;
+  if plugPhase3 then
+    connect(load3.terminal, adaDel.terminals[3]) annotation (Line(points={{-10,-88},
+            {-16,-88},{-20,-88},{-20,-40.5333},{-40.2,-40.5333}},
+                                                              color={0,120,120}));
+    connect(load3.terminal, adaWye.terminals[3]) annotation (Line(points={{-10,-88},
+            {-20,-88},{-20,-70.5333},{-40.2,-70.5333}},
+                                                    color={0,120,120}));
+  end if;
+
+  connect(adaDel.terminal, wyeToDelta.delta) annotation (Line(points={{-60,-40},
+          {-64,-40},{-64,-20},{-28,-20},{-28,10},{-34,10}}, color={0,120,120}));
+  connect(adaWye.terminal, wyeToWyeGround.wyeg) annotation (Line(points={{-60,-70},
+          {-66,-70},{-66,-18},{-30,-18},{-30,-10},{-34,-10}}, color={0,120,120}));
+    annotation (    Documentation(info="<html>
+<p>
+This model represents a partial interface for a three-phase AC unbalanced
+load.
+</p>
+<p>
+The loads on each phase can be removed using the boolean flags
+<code>plugPhase1</code>, <code>plugPhase2</code>, and <code>plugPhase3</code>.
+These parameters can be used to generate unbalanced loads.
+</p>
+<p>
+The loads can be connected either in wye (Y) or delta (D) configuration.
+The parameter <code>loadConn</code> can be used for such a purpose.
+</p>
+<p>
+Each load model has the option to be controlled by a voltage controller.
+When enabled, the voltage controller unplugs the load for a certain amount of
+time if the voltage exceeds a given threshold. Mode information about the
+voltage controller can be found
+<a href=\"modelica://AixLib.Electrical.Utilities.VoltageControl\">here</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 17, 2016, by Michael Wetter:<br/>
+Corrected wrong annotation to avoid an error in the pedantic model check
+in Dymola 2017 FD01 beta2.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/557\">issue 557</a>.
+</li>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapters for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Provided value for <code>P_nominal</code> if
+<code>mode &lt;&gt; AixLib.Electrical.Types.Load.VariableZ_P_input</code>.
+This avoids a warning during translation of
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Inductive\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Inductive</a>.
+</li>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BaseLoadCtrl;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/Impedance.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/Impedance.mo
new file mode 100644
index 0000000000..6369a0bbc9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/Impedance.mo
@@ -0,0 +1,59 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses;
+partial model Impedance
+  "Partial model of a three-phase unbalanced impedance without neutral cable"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.BaseImpedance;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal_n terminal
+    "Electrical connector"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+
+equation
+  connect(terminal, wyeToDelta.wye) annotation (Line(
+      points={{-100,0},{-80,0},{-80,10},{-64,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal, wyeToWyeGround.wye) annotation (Line(
+      points={{-100,0},{-80,0},{-80,-10},{-64,-10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (    Documentation(info="<html>
+<p>
+This model represents a partial interface for a three-phase AC
+unbalanced impedance without neutral cable.
+</p>
+<p>
+The model can be configured in order to represent different type of
+impedances as well as configurations.
+</p>
+<p>
+The loads can be connected either in wye (Y) or delta (D) configuration.
+The parameter <code>loadConn</code> can be used for such a purpose.
+</p>
+<p>
+The model has three impedances that can be either connected in Y or
+Delta configuration. The parameter <code>loadConn</code> can be used for
+such a purpose. The Boolean parameter <code>inductive</code> can be selected
+to specify the type of impedance.
+</p>
+<p>
+The impedances on each phase can be removed using the boolean flags
+<code>plugPhase1</code>, <code>plugPhase2</code>, and <code>plugPhase3</code>.
+These parameters can be used to generate unbalanced loads.
+</p>
+<p>
+The values of the impedances are computed starting from the parameters <code>R</code>,
+<code>L</code>, and <code>C</code>. Depending on the values of the boolean flag
+<code>inductive</code> some of these parameters may be disabled. There are additional
+flags <code>use_R_in</code>, <code>use_L_in</code>, and <code>use_C_in</code> that can
+be used to specify time varying impedances.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Created model from previus version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedance;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/Impedance_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/Impedance_N.mo
new file mode 100644
index 0000000000..373823f3cb
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/Impedance_N.mo
@@ -0,0 +1,65 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses;
+partial model Impedance_N
+  "Partial model of a three-phase unbalanced impedance with neutral cable"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.BaseImpedance;
+  Interfaces.Terminal4_n terminal "Electrical connector"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+  Interfaces.Connection3to4_n connection3to4
+    "Connection from three-phase and neutral to three-phase" annotation (Placement(transformation(extent={{-88,-10},{-68,10}})));
+equation
+
+  connect(connection3to4.terminal3, wyeToDelta.wye) annotation (Line(
+      points={{-68,6.66134e-16},{-68,10},{-64,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(connection3to4.terminal3, wyeToWyeGround.wye) annotation (Line(
+      points={{-68,4.44089e-16},{-68,-10},{-64,-10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(connection3to4.terminal4, terminal) annotation (Line(
+      points={{-88,0},{-100,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (    Documentation(info="<html>
+<p>
+This model represents a partial interface for a three-phase AC
+unbalanced impedance with a neutral cable. The current in the neutral
+cable is computed as the algebraic sum of the currents in the loads.
+</p>
+<p>
+The model can be configured in order to represent different type of
+impedances as well as configurations.
+</p>
+<p>
+The loads can be connected either in wye (Y) or delta (D) configuration.
+The parameter <code>loadConn</code> can be used for such a purpose.
+</p>
+<p>
+The model has three impedances that can be either connected in Y or
+Delta configuration. The parameter <code>loadConn</code> can be used for
+such a purpose. The Boolean parameter <code>inductive</code> can be selected
+to specify the type of impedance.
+</p>
+<p>
+The impedances on each phase can be removed using the boolean flags
+<code>plugPhase1</code>, <code>plugPhase2</code>, and <code>plugPhase3</code>.
+These parameters can be used to generate unbalanced loads.
+</p>
+<p>
+The values of the impedances are computed starting from the parameters <code>R</code>,
+<code>L</code>, and <code>C</code>. Depending on the values of the boolean flag
+<code>inductive</code> some of these parameters may be disabled. There are additional
+flags <code>use_R_in</code>, <code>use_L_in</code>, and <code>use_C_in</code> that can
+be used to specify time varying impedances.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Created model from previus version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedance_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/LoadCtrl.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/LoadCtrl.mo
new file mode 100644
index 0000000000..b73af9b37c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/LoadCtrl.mo
@@ -0,0 +1,55 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses;
+partial model LoadCtrl
+  "Partial model of a three-phase load with voltage controller without neutral cable"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.BaseLoadCtrl;
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal_n terminal
+    "Connector for three-phase unbalanced systems without neutral cable"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+equation
+
+  connect(terminal, wyeToDelta.wye) annotation (Line(
+      points={{-100,0},{-78,0},{-78,10},{-54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(terminal, wyeToWyeGround.wye) annotation (Line(
+      points={{-100,0},{-78,0},{-78,-10},{-54,-10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (    Documentation(info="<html>
+<p>
+This model represents a partial interface for a three-phase AC unbalanced
+load without neutral cable.
+</p>
+<p>
+The loads on each phase can be removed using the boolean flags
+<code>plugPhase1</code>, <code>plugPhase2</code>, and <code>plugPhase3</code>.
+These parameters can be used to generate unbalanced loads.
+</p>
+<p>
+The loads can be connected either in wye (Y) or delta (D) configuration.
+The parameter <code>loadConn</code> can be used for such a purpose.
+</p>
+<p>
+Each load model has the option to be controlled by a voltage controller.
+When enabled, the voltage controller unplugs the load for a certain amount of
+time if the voltage exceeds a given threshold. Mode information about the
+voltage controller can be found
+<a href=\"modelica://AixLib.Electrical.Utilities.VoltageControl\">here</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised model, it now extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.PartialLoadCtrl\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.PartialLoadCtrl</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end LoadCtrl;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/LoadCtrl_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/LoadCtrl_N.mo
new file mode 100644
index 0000000000..4f35805102
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/LoadCtrl_N.mo
@@ -0,0 +1,63 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses;
+partial model LoadCtrl_N
+  "Partial model of a three-phase unbalanced load with voltage controller and neutral cable"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.BaseLoadCtrl;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal4_n terminal
+    "Connector for three-phase unbalanced systems with neutral cable"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Connection3to4_n
+    connection3to4 "Connection from three-phase and neutral to three-phase"
+    annotation (Placement(transformation(extent={{-84,-10},{-64,10}})));
+equation
+
+  connect(connection3to4.terminal3, wyeToDelta.wye) annotation (Line(
+      points={{-64,0},{-58,0},{-58,10},{-54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(connection3to4.terminal3, wyeToWyeGround.wye) annotation (Line(
+      points={{-64,0},{-58,0},{-58,-10},{-54,-10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(connection3to4.terminal4, terminal) annotation (Line(
+      points={{-84,0},{-100,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+    annotation (    Documentation(info="<html>
+<p>
+This model represents a partial interface for a three-phase AC unbalanced
+load with neutral cable. The current in the neutral cable is computed as the
+algebraic sum of the currents in the loads.
+</p>
+<p>
+The loads on each phase can be removed using the boolean flags
+<code>plugPhase1</code>, <code>plugPhase2</code>, and <code>plugPhase3</code>.
+These parameters can be used to generate unbalanced loads.
+</p>
+<p>
+The loads can be connected either in wye (Y) or delta (D) configuration.
+The parameter <code>loadConn</code> can be used for such a purpose.
+</p>
+<p>
+Each load model has the option to be controlled by a voltage controller.
+When enabled, the voltage controller unplugs the load for a certain amount of
+time if the voltage exceeds a given threshold. Mode information about the
+voltage controller can be found
+<a href=\"modelica://AixLib.Electrical.Utilities.VoltageControl\">here</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised model, it now extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.PartialLoadCtrl\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.PartialLoadCtrl</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end LoadCtrl_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/package.mo
new file mode 100644
index 0000000000..bc58d4deae
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+package BaseClasses "Package with base class models"
+extends Modelica.Icons.BasesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains base classes used by the models that are part of the package
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/package.order
new file mode 100644
index 0000000000..8803d072ba
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/BaseClasses/package.order
@@ -0,0 +1,6 @@
+BaseImpedance
+BaseLoadCtrl
+Impedance
+Impedance_N
+LoadCtrl
+LoadCtrl_N
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Capacitive.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Capacitive.mo
new file mode 100644
index 0000000000..b1fbcbea38
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Capacitive.mo
@@ -0,0 +1,212 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+model Capacitive
+  "Model of a three-phase unbalanced capacitive load without neutral cable"
+  extends BaseClasses.LoadCtrl(
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Capacitive load1(pf=pf,
+        use_pf_in=use_pf_in),
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Capacitive load2(pf=pf,
+        use_pf_in=use_pf_in),
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Capacitive load3(pf=pf,
+        use_pf_in=use_pf_in));
+  parameter Boolean use_pf_in = false
+    "If true, the power factor is defined by an input"
+    annotation(Dialog(group="Modeling assumption"));
+  parameter Real pf(min=0, max=1) = 0.8 "Power factor"
+  annotation(Dialog(group="Nominal conditions"));
+  Modelica.Blocks.Interfaces.RealInput pf_in_1(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase1) "Power factor of load on phase 1" annotation (Placement(
+        transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-60,-120}),
+                          iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-60,-100})));
+  Modelica.Blocks.Interfaces.RealInput pf_in_2(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase2) "Power factor of load on phase 2" annotation (Placement(
+        transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={30,-120}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={0,-100})));
+  Modelica.Blocks.Interfaces.RealInput pf_in_3(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase3) "Power factor of load on phase 3" annotation (Placement(
+        transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={80,-120}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={60,-100})));
+equation
+  connect(pf_in_1, load1.pf_in) annotation (Line(
+      points={{-60,-120},{-60,56},{10,56}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  connect(pf_in_2, load2.pf_in) annotation (Line(
+      points={{30,-120},{30,-14},{10,-14}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  connect(pf_in_3, load3.pf_in) annotation (Line(
+      points={{80,-120},{80,-82},{10,-82}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  annotation (
+  defaultComponentName="loa",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+       graphics={
+        Rectangle(
+          extent={{-80,80},{80,-80}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Line(points={{-42,-5.14335e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-2,0},
+          rotation=180),
+          Line(points={{-26,-3.18398e-15},{6.85214e-44,8.39117e-60}},
+                                         color={0,0,0},
+          origin={48,0},
+          rotation=180),
+          Line(points={{-10,-1.22461e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+          Line(points={{-2,-2.44921e-16},{16,1.95937e-15}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Text(
+          extent={{-120,120},{120,80}},
+          textColor={0,0,0},
+          textString="%name"),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,1},
+          rotation=90),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{44,5.38825e-15}},
+                                         color={0,0,0},
+          origin={60,50},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,51},
+          rotation=90),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,-51},
+          rotation=90),
+        Line(
+          points={{60,50},{76,0},{60,-52}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,-52},
+          rotation=180),
+        Line(
+          points={{10,68},{10,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{16,68},{16,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{60,7.34764e-15}},
+                                         color={0,0,0},
+          origin={76,0},
+          rotation=180),
+        Line(
+          points={{16,18},{16,-18}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{10,18},{10,-18}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{44,5.38825e-15}},
+                                         color={0,0,0},
+          origin={60,-52},
+          rotation=180),
+        Line(
+          points={{16,-34},{16,-70}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{10,-34},{10,-70}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,-52},
+          rotation=180)}),    Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a three-phase unbalanced capacitive load.
+The model extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl</a>
+and uses the load model from the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads\">
+AixLib.Electrical.AC.OnePhase.Loads</a>.
+The model computes the voltages, currents and powers on each phase.
+</p>
+<p>
+For more information, see <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl</a> and
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Capacitive\">
+AixLib.Electrical.AC.OnePhase.Loads.Capacitive</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Capacitive;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Capacitive_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Capacitive_N.mo
new file mode 100644
index 0000000000..5026b2f992
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Capacitive_N.mo
@@ -0,0 +1,216 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+model Capacitive_N
+  "Model of a three-phase unbalanced capacitive load with neutral cable"
+  extends BaseClasses.LoadCtrl_N(
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Capacitive load1(pf=pf,
+        use_pf_in=use_pf_in),
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Capacitive load2(pf=pf,
+        use_pf_in=use_pf_in),
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Capacitive load3(pf=pf,
+        use_pf_in=use_pf_in));
+  parameter Boolean use_pf_in = false
+    "If true, the power factor is defined by an input"
+    annotation(Dialog(group="Modeling assumption"));
+  parameter Real pf(min=0, max=1) = 0.8 "Power factor"
+  annotation(Dialog(group="Nominal conditions"));
+  Modelica.Blocks.Interfaces.RealInput pf_in_1(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase1) "Power factor of load on phase 1" annotation (Placement(
+        transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-60,-120}),
+                          iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-60,-100})));
+  Modelica.Blocks.Interfaces.RealInput pf_in_2(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase2) "Power factor of load on phase 2" annotation (Placement(
+        transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={30,-120}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={0,-100})));
+  Modelica.Blocks.Interfaces.RealInput pf_in_3(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase3) "Power factor of load on phase 3" annotation (Placement(
+        transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={80,-120}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={60,-100})));
+equation
+  connect(pf_in_1, load1.pf_in) annotation (Line(
+      points={{-60,-120},{-60,56},{10,56}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  connect(pf_in_2, load2.pf_in) annotation (Line(
+      points={{30,-120},{30,-14},{10,-14}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  connect(pf_in_3, load3.pf_in) annotation (Line(
+      points={{80,-120},{80,-82},{10,-82}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  annotation (
+  defaultComponentName="loa",
+  Icon(graphics={
+        Rectangle(
+          extent={{-80,80},{80,-80}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Line(points={{-42,-5.14335e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-2,0},
+          rotation=180),
+          Line(points={{-26,-3.18398e-15},{6.85214e-44,8.39117e-60}},
+                                         color={0,0,0},
+          origin={48,0},
+          rotation=180),
+          Line(points={{-10,-1.22461e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+          Line(points={{-2,-2.44921e-16},{16,1.95937e-15}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Text(
+          extent={{-120,120},{120,80}},
+          textColor={0,0,0},
+          textString="%name"),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,1},
+          rotation=90),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{44,5.38825e-15}},
+                                         color={0,0,0},
+          origin={60,50},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,51},
+          rotation=90),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,-51},
+          rotation=90),
+        Line(
+          points={{60,50},{76,0},{60,-52}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,-52},
+          rotation=180),
+        Line(
+          points={{10,68},{10,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{16,68},{16,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{60,7.34764e-15}},
+                                         color={0,0,0},
+          origin={76,0},
+          rotation=180),
+        Line(
+          points={{16,18},{16,-18}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{10,18},{10,-18}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{44,5.38825e-15}},
+                                         color={0,0,0},
+          origin={60,-52},
+          rotation=180),
+        Line(
+          points={{16,-34},{16,-70}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{10,-34},{10,-70}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(
+          points={{0,0},{32,3.91873e-15}},
+          color={0,0,0},
+          origin={10,-52},
+          rotation=180)}), Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a three-phase unbalanced capacitive load.
+The model extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N</a>
+and uses the load model from the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads\">
+AixLib.Electrical.AC.OnePhase.Loads</a>.
+The model computes the voltages, currents and powers on each phase.
+</p>
+<p>
+This model has a connector with four cables and it represents the neutral cable.
+The current in the neutral cable is computed as the algebraic sum of the currents
+of the loads.
+</p>
+<p>
+For more information, see <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N</a> and
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Capacitive\">
+AixLib.Electrical.AC.OnePhase.Loads.Capacitive</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Capacitive_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Impedances.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Impedances.mo
new file mode 100644
index 0000000000..f8058d0970
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Impedances.mo
@@ -0,0 +1,113 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Examples;
+model Impedances
+  "This model tests three-phase unbalanced impedances with and without neutral cable"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage_N sou_N(definiteReference=true,
+    f=60,
+    V=480) "Voltage source with neutral cable"
+    annotation (Placement(transformation(extent={{-94,-50},{-74,-30}})));
+  Sensors.GeneralizedSensor_N sen_N "Power sensor with neutral cable"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  Impedance_N imp_N(
+    plugPhase2=false,
+    use_R_in=true,
+    RMin=1,
+    RMax=10,
+    use_L_in=true,
+    LMin=0.1,
+    LMax=1) "Impedance with neutral cable"
+    annotation (Placement(transformation(extent={{0,-50},{20,-30}})));
+  Sources.FixedVoltage sou(definiteReference=true,
+    f=60,
+    V=480) "Voltage source without neutral cable"
+    annotation (Placement(transformation(extent={{-94,30},{-74,50}})));
+  Sensors.GeneralizedSensor sen "Power sensor without neutral cable"
+    annotation (Placement(transformation(extent={{-60,30},{-40,50}})));
+  Impedance imp(
+    plugPhase2=false,
+    use_R_in=true,
+    RMin=1,
+    RMax=10,
+    use_L_in=true,
+    LMin=0.1,
+    LMax=1) "Impedance without neutral cable"
+    annotation (Placement(transformation(extent={{0,30},{20,50}})));
+  Modelica.Blocks.Sources.Ramp var_RL(
+    duration=0.5,
+    startTime=0.25,
+    height=1,
+    offset=0) "Power signal for loads on phase 1"
+    annotation (Placement(transformation(extent={{60,-10},{40,10}})));
+equation
+
+  connect(sou.terminal, sen.terminal_n) annotation (Line(
+      points={{-74,40},{-60,40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, imp.terminal) annotation (Line(
+      points={{-40,40},{0,40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(var_RL.y, imp.y_R) annotation (Line(
+      points={{39,0},{36,0},{36,70},{6,70},{6,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(var_RL.y, imp.y_L) annotation (Line(
+      points={{39,6.66134e-16},{26,6.66134e-16},{26,62},{14,62},{14,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(var_RL.y, imp_N.y_R) annotation (Line(
+      points={{39,0},{6,0},{6,-30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(var_RL.y, imp_N.y_L) annotation (Line(
+      points={{39,0},{14,0},{14,-30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou_N.terminal, sen_N.terminal_n) annotation (Line(
+      points={{-74,-40},{-60,-40}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(sen_N.terminal_p, imp_N.terminal) annotation (Line(
+      points={{-40,-40},{0,-40}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+            -100},{100,100}}),      graphics={Text(
+          extent={{-80,80},{0,74}},
+          textColor={0,0,0},
+          pattern=LinePattern.Dash,
+          textString="Without neutral"), Text(
+          extent={{-80,-10},{0,-16}},
+          textColor={0,0,0},
+          pattern=LinePattern.Dash,
+          textString="With neutral")}),        Documentation(info="<html>
+<p>
+This example model shows how to use three-phase unbalanced impedances with and without neutral cable.
+</p>
+<p>
+This model contains two identical inductive impedances with and without neutral cable.
+The impedances have inputs that allow to change the value of their resistances and inductances
+externally. The values start to change from their minimum to their maximum values at time
+<i>t = 0.25 s</i>.
+</p>
+<p>
+The unbalanced impedance that has the neutral cable
+<code>sen_N.I[4]</code> is able to measure the current in the neutral. that is
+the current necessary to satisfy the Kirchoff Current Law (KCL)
+such that the algebraic sum of the phase current in each impedance is equal to zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Created model from previus version and added documentation.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=1.0),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Impedances.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedances;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/LoadCtrl.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/LoadCtrl.mo
new file mode 100644
index 0000000000..484f9ce5f9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/LoadCtrl.mo
@@ -0,0 +1,102 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Examples;
+model LoadCtrl
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage_N sou(f=60, V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+  Modelica.Blocks.Sources.Sine pow_1(
+    f=0.1,
+    amplitude=4500,
+    offset=6000) "Power on phase 1"
+    annotation (Placement(transformation(extent={{60,10},{40,30}})));
+  Resistive_N load_ctrl(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    vThresh=0.05,
+    tDelay=2,
+    voltageCtrl=true,
+    plugPhase2=false,
+    plugPhase3=false,
+    V_nominal=480) "Voltage controlled load"
+              annotation (Placement(transformation(extent={{-8,-10},{12,10}})));
+  Lines.Line_N line1(
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu10
+      commercialCable,
+    l=400,
+    P_nominal=10000,
+    V_nominal=480) "Transmission line to voltage controlled load"
+    annotation (Placement(transformation(extent={{-46,-10},{-26,10}})));
+  Resistive_N load(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    plugPhase2=false,
+    plugPhase3=false,
+    V_nominal=480) "Load"
+    annotation (Placement(transformation(extent={{-8,-40},{12,-20}})));
+  Lines.Line_N line(
+    mode=AixLib.Electrical.Types.CableMode.commercial,
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Cu10
+      commercialCable,
+    l=400,
+    P_nominal=10000,
+    V_nominal=480)
+    annotation (Placement(transformation(extent={{-46,-40},{-26,-20}})));
+equation
+  connect(pow_1.y, load_ctrl.Pow1) annotation (Line(
+      points={{39,20},{30,20},{30,8},{14,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pow_1.y, load.Pow1) annotation (Line(
+      points={{39,20},{30,20},{30,-22},{14,-22}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou.terminal, line1.terminal_n) annotation (Line(
+      points={{-60,0},{-46,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(sou.terminal, line.terminal_n) annotation (Line(
+      points={{-60,0},{-54,0},{-54,-30},{-46,-30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(line.terminal_p, load.terminal) annotation (Line(
+      points={{-26,-30},{-8,-30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, load_ctrl.terminal) annotation (Line(
+      points={{-26,0},{-8,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (    experiment(Tolerance=1e-6, StopTime=10.0),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/LoadCtrl.mos"
+        "Simulate and plot"),
+Documentation(info="<html>
+<p>
+This example model shows how the voltage controller can act on a three-phase unbalanced load.
+</p>
+<p>
+This model contains two loads: one with voltage control and one without.
+The loads produce power only on the first phase that is connected through a transmission line to a voltage
+source. When the power production increases, the losses on the line cause an increase of the voltage
+at the load. The load with voltage controller detects when the overvoltage happens
+and unplugs the load for 2 seconds. After 2 seconds the load is plugged again and if this causes an other
+overvoltage it will be unplugged again.
+</p>
+<p>
+The model contains both a controlled and a not controlled load so the user can
+compare the difference in the voltages and powers when the load is unplugged.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2015, by Michael Wetter:<br/>
+Removed assignment of <code>P_nominal</code> to avoid the warning
+\"The following parameters with fixed = false also have a binding\"
+in Dymola 2016.
+</li>
+<li>
+March 10, 2015, by Marco Bonvini:<br/>
+Revised documentation of the example.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end LoadCtrl;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads.mo
new file mode 100644
index 0000000000..589b3c0eb9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads.mo
@@ -0,0 +1,169 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Examples;
+model Loads "This model tests the load models without neutral cable connection"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage sou(definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-94,-10},{-74,10}})));
+  Modelica.Blocks.Sources.Sine ph_1(
+    amplitude=2000,
+    f=10,
+    offset=-2500) "Power signal for loads on phase 1"
+    annotation (Placement(transformation(extent={{80,30},{60,50}})));
+  Modelica.Blocks.Sources.Constant ph_23(k=0)
+    "Power signal for loads on phase 2 and 3"
+    annotation (Placement(transformation(extent={{100,-10},{80,10}})));
+  Resistive loaR(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=480) "Resistive load"
+    annotation (Placement(transformation(extent={{-8,-10},{12,10}})));
+  Inductive loaRL(mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=480) "Inductive load"
+    annotation (Placement(transformation(extent={{-8,-40},{12,-20}})));
+  Capacitive loaRC(mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=480) "Capacitive load"
+    annotation (Placement(transformation(extent={{-8,-80},{12,-60}})));
+  Sensors.GeneralizedSensor sen "Power sensor"
+    annotation (Placement(transformation(extent={{-64,-10},{-44,10}})));
+  Sensors.GeneralizedSensor senSingleConn "Power sensor"
+    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
+  Capacitive loaRC1(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    plugPhase2=false,
+    plugPhase3=false,
+    V_nominal=480) "Capacitive load"
+    annotation (Placement(transformation(extent={{10,30},{30,50}})));
+  Inductive loaRL1(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    plugPhase2=false,
+    plugPhase3=false,
+    V_nominal=480) "Inductive load"
+    annotation (Placement(transformation(extent={{-10,50},{10,70}})));
+  Resistive loaR1(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    plugPhase2=false,
+    plugPhase3=false,
+    V_nominal=480) "Resistive load"
+    annotation (Placement(transformation(extent={{-30,70},{-10,90}})));
+equation
+  connect(ph_1.y, loaR.Pow1) annotation (Line(
+      points={{59,40},{54,40},{54,8},{14,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaR.Pow3) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-8},{14,-8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaR.Pow2) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,6.66134e-16},{14,6.66134e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_1.y, loaRL.Pow1) annotation (Line(
+      points={{59,40},{54,40},{54,-22},{14,-22}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_1.y, loaRC.Pow1) annotation (Line(
+      points={{59,40},{54,40},{54,-62},{14,-62}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaRL.Pow2) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-30},{14,-30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaRL.Pow3) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-38},{14,-38}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaRC.Pow2) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-70},{14,-70}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaRC.Pow3) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-78},{14,-78}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou.terminal, sen.terminal_n) annotation (Line(
+      points={{-74,5.55112e-16},{-66,5.55112e-16},{-66,4.44089e-16},{-64,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+
+  connect(sen.terminal_p, loaR.terminal) annotation (Line(
+      points={{-44,0},{-8,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, loaRL.terminal) annotation (Line(
+      points={{-44,0},{-26,0},{-26,-30},{-8,-30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, loaRC.terminal) annotation (Line(
+      points={{-44,0},{-26,0},{-26,-70},{-8,-70}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(senSingleConn.terminal_p, loaR1.terminal) annotation (Line(
+      points={{-40,60},{-36,60},{-36,80},{-30,80}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(senSingleConn.terminal_p, loaRL1.terminal) annotation (Line(
+      points={{-40,60},{-10,60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(senSingleConn.terminal_p, loaRC1.terminal) annotation (Line(
+      points={{-40,60},{-16,60},{-16,40},{10,40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ph_1.y, loaRC1.Pow1) annotation (Line(
+      points={{59,40},{46,40},{46,48},{32,48}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_1.y, loaRL1.Pow1) annotation (Line(
+      points={{59,40},{46,40},{46,68},{12,68}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_1.y, loaR1.Pow1) annotation (Line(
+      points={{59,40},{46,40},{46,88},{-8,88}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou.terminal, senSingleConn.terminal_n) annotation (Line(
+      points={{-74,0},{-68,0},{-68,60},{-60,60}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation ( Documentation(info="<html>
+<p>
+This example model shows how three-phase unbalanced loads can be used.
+</p>
+<p>
+This model contains two set of loads (one for each type: resistive, inductive and capacitive)
+that consume power just on the first phase. The example shows how it's possible to model
+this situation in two different ways. It's possible to not connect the loads on the phases
+setting the parameters <code>plugLoad*=false</code>.
+The alternative is to impose the load on a specific phase equal to zero.
+</p>
+<p>
+The power measured by the sensors on each phase show that the results are equal.
+</p>
+<h4>Note:</h4>
+<p>
+Whenever possible it is preferred to disable the load on a specific phase using the parameter <code>plugLoad*</code>
+because the equations relative to the load are conditionally removed, reducing the size
+of the system of equations.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2015, by Michael Wetter:<br/>
+Removed assignment of <code>P_nominal</code> to avoid the warning
+\"The following parameters with fixed = false also have a binding\"
+in Dymola 2016.
+</li>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Created model from previus version and added documentation.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=1.0),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Loads;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads_N.mo
new file mode 100644
index 0000000000..1ac6abfdeb
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads_N.mo
@@ -0,0 +1,124 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Examples;
+model Loads_N
+  "This model tests unbalanced load models with neutral cable connection"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage_N
+                       sou(definiteReference=true,
+    f=60,
+    V=480) "Voltage source"
+    annotation (Placement(transformation(extent={{-94,-10},{-74,10}})));
+  Modelica.Blocks.Sources.Ramp ph_1(
+    offset=-1000,
+    duration=0.5,
+    startTime=0.25,
+    height=-500) "Power signal for loads on phase 1"
+               annotation (Placement(transformation(extent={{80,30},{60,50}})));
+  Modelica.Blocks.Sources.Constant ph_23(k=-1000)
+    "Power signal for loads on phase 2 and 3"
+    annotation (Placement(transformation(extent={{100,-10},{80,10}})));
+  Resistive_N loaR_N(mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=480) "Resistive load with neutral cable"
+    annotation (Placement(transformation(extent={{-8,-10},{12,10}})));
+  Inductive_N loaRL_N(mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+      pf=0.9,
+    V_nominal=480) "Inductive load with neutral cable"
+    annotation (Placement(transformation(extent={{-8,-40},{12,-20}})));
+  Capacitive_N loaRC_N(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    pf=0.7,
+    V_nominal=480) "Capacitive load with neutral cable"
+    annotation (Placement(transformation(extent={{-8,-80},{12,-60}})));
+  Sensors.GeneralizedSensor_N
+                            sen "Power sensor with neutral cable"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+equation
+  connect(ph_1.y, loaR_N.Pow1) annotation (Line(
+      points={{59,40},{54,40},{54,8},{14,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaR_N.Pow3) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-8},{14,-8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaR_N.Pow2) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,6.66134e-16},{14,6.66134e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+
+  connect(ph_1.y, loaRL_N.Pow1) annotation (Line(
+      points={{59,40},{54,40},{54,-22},{14,-22}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_1.y, loaRC_N.Pow1) annotation (Line(
+      points={{59,40},{54,40},{54,-62},{14,-62}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaRL_N.Pow2) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-30},{14,-30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaRL_N.Pow3) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-38},{14,-38}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaRC_N.Pow2) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-70},{14,-70}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ph_23.y, loaRC_N.Pow3) annotation (Line(
+      points={{79,4.44089e-16},{68,4.44089e-16},{68,-78},{14,-78}},
+      color={0,0,127},
+      smooth=Smooth.None));
+
+  connect(sou.terminal, sen.terminal_n) annotation (Line(
+      points={{-74,0},{-60,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, loaR_N.terminal) annotation (Line(
+      points={{-40,0},{-8,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, loaRL_N.terminal) annotation (Line(
+      points={{-40,0},{-26,0},{-26,-30},{-8,-30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, loaRC_N.terminal) annotation (Line(
+      points={{-40,0},{-26,0},{-26,-70},{-8,-70}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation ( Documentation(info="<html>
+<p>
+This example model shows how three-phase unbalanced loads with the neutral cable can be used.
+</p>
+<p>
+This model contains three different loads of different type. They start in a balanced configuration
+and at time <i>t = 0.25 s</i> the loads on the first phase start to increase their power consumption.
+</p>
+<p>
+When the loads start to be unbalanced the sensors starts to measure a current in the neutral cable
+<code>sen.I[4]</code>. This is the current necessary to satisfy the Kirchoff Current Law (KCL)
+such that the algebraic sum of the phase current in each load is equal to zero.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/unbalancedLoads.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2015, by Michael Wetter:<br/>
+Removed assignment of <code>P_nominal</code> to avoid the warning
+\"The following parameters with fixed = false also have a binding\"
+in Dymola 2016.
+</li>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Created model from previus version and added documentation.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=1.0),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads_N.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Loads_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/package.mo
new file mode 100644
index 0000000000..4d4ccd758e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/package.order
new file mode 100644
index 0000000000..1ae3c2a8a5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/package.order
@@ -0,0 +1,4 @@
+Impedances
+LoadCtrl
+Loads
+Loads_N
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Impedance.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Impedance.mo
new file mode 100644
index 0000000000..af5d053950
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Impedance.mo
@@ -0,0 +1,101 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+model Impedance
+  "Model of a three-phase unbalanced impedance without neutral cable"
+  extends BaseClasses.Impedance(
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Impedance load1,
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Impedance load2,
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Impedance load3);
+equation
+
+  annotation (
+  defaultComponentName="imp",
+  Icon(graphics={      Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+          Rectangle(
+            extent={{-80,80},{80,-80}},
+            lineColor={0,0,0},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+          origin={7.10543e-15,7.10543e-15},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{12,1.46953e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{18,2.20429e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+        Text(
+          extent={{-120,-80},{120,-120}},
+          textColor={0,0,0},
+          textString="%name"),
+        Line(
+          points={{-66,50},{-26,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,49},
+          rotation=90),
+        Line(
+          points={{34,50},{54,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{54,50},{70,0},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{34,0},{70,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,1},
+          rotation=90),
+        Line(
+          points={{-66,0},{-26,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-66,-50},{-26,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,-49},
+          rotation=90),
+        Line(
+          points={{34,-50},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None)}), Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a three-phase unbalanced impedance without neutral cable.
+The model extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.Impedance\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.Impedance</a>
+and uses the load model from the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Impedance\">
+AixLib.Electrical.AC.OnePhase.Loads.Impedance</a>.
+The model computes the voltages, currents and powers on each phase.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedance;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Impedance_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Impedance_N.mo
new file mode 100644
index 0000000000..7195d9c06a
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Impedance_N.mo
@@ -0,0 +1,103 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+model Impedance_N
+  "Model of a three-phase unbalanced impedance with neutral cable"
+  extends BaseClasses.Impedance_N(
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Impedance load1,
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Impedance load2,
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Impedance load3);
+equation
+
+  annotation (
+  defaultComponentName="imp",
+  Icon(graphics={      Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+          Rectangle(
+            extent={{-80,80},{80,-80}},
+            lineColor={0,0,0},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+          origin={7.10543e-15,7.10543e-15},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{12,1.46953e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{18,2.20429e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+        Text(
+          extent={{-120,-80},{120,-120}},
+          textColor={0,0,0},
+          textString="%name"),
+        Line(
+          points={{-66,50},{-26,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,49},
+          rotation=90),
+        Line(
+          points={{34,50},{54,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{54,50},{70,0},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{34,0},{70,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,1},
+          rotation=90),
+        Line(
+          points={{-66,0},{-26,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-66,-50},{-26,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,-49},
+          rotation=90),
+        Line(
+          points={{34,-50},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None)}), Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a three-phase unbalanced impedance with neutral cable.
+The current in the neutral cable is computed as the algebraic sum of the currents
+of the loads.
+The model extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.Impedance_N\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.Impedance_N</a>
+and uses the load model from the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Impedance\">
+AixLib.Electrical.AC.OnePhase.Loads.Impedance</a>.
+The model computes the voltages, currents and powers on each phase.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedance_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Inductive.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Inductive.mo
new file mode 100644
index 0000000000..700574959d
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Inductive.mo
@@ -0,0 +1,222 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+model Inductive
+  "Model of a three-phase unbalanced inductive load without neutral cable"
+  extends BaseClasses.LoadCtrl(
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Inductive load1(
+      pf=pf,
+      use_pf_in=use_pf_in),
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Inductive load2(
+      pf=pf,
+      use_pf_in=use_pf_in),
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Inductive load3(
+      pf=pf,
+      use_pf_in=use_pf_in));
+  parameter Boolean use_pf_in = false
+    "If true, the power factor is defined by an input"
+    annotation(Dialog(group="Modeling assumption"));
+  parameter Real pf(min=0, max=1) = 0.8 "Power factor"
+  annotation(Dialog(group="Nominal conditions"));
+  Modelica.Blocks.Interfaces.RealInput pf_in_1(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase1) "Power factor of load on phase 1" annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-60,-120}),
+                          iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-60,-100})));
+  Modelica.Blocks.Interfaces.RealInput pf_in_2(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase2) "Power factor of load on phase 2" annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={50,-120}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={0,-100})));
+  Modelica.Blocks.Interfaces.RealInput pf_in_3(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase3) "Power factor of load on phase 3" annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={20,-120}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={62,-100})));
+
+equation
+  connect(pf_in_1, load1.pf_in) annotation (Line(
+      points={{-60,-120},{-60,56},{10,56}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  connect(pf_in_2, load2.pf_in) annotation (Line(
+      points={{50,-120},{50,-14},{10,-14}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  connect(pf_in_3, load3.pf_in) annotation (Line(
+      points={{20,-120},{20,-82},{10,-82}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  annotation (
+  defaultComponentName="loa",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}),
+                   graphics={
+        Rectangle(
+          extent={{-80,80},{80,-80}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+                                   Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+        Rectangle(
+          extent={{0,0},{60,-12}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={70,0},
+          rotation=180),
+          Line(points={{-10,-1.22461e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Ellipse(extent={{-10,-10},{10,10}},
+          rotation=360),
+        Ellipse(extent={{30,-10},{50,10}}),
+        Ellipse(extent={{10,-10},{30,10}}),
+        Rectangle(
+          extent={{-10,0},{50,-12}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{26,3.18398e-15}},
+                                         color={0,0,0},
+          origin={76,0},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,1},
+          rotation=90),
+          Line(points={{-2,-2.44921e-16},{18,2.20429e-15}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Text(
+          extent={{-120,120},{120,80}},
+          textColor={0,0,0},
+          textString="%name"),
+        Ellipse(extent={{-10,-10},{10,10}},
+          origin={0,50},
+          rotation=360),
+        Ellipse(extent={{30,40},{50,60}}),
+        Ellipse(extent={{10,40},{30,60}}),
+        Rectangle(
+          extent={{-10,50},{50,38}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={60,50},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,51},
+          rotation=90),
+        Ellipse(extent={{-10,-10},{10,10}},
+          origin={0,-52},
+          rotation=360),
+        Ellipse(extent={{30,-62},{50,-42}}),
+        Ellipse(extent={{10,-62},{30,-42}}),
+        Rectangle(
+          extent={{-10,-52},{50,-64}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,-52},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={60,-52},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,-51},
+          rotation=90),
+        Line(
+          points={{60,50},{76,0},{60,-52}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,-52},
+          rotation=180)}),    Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a three-phase unbalanced inductive load.
+The model extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl</a>
+and uses the load model from the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads\">
+AixLib.Electrical.AC.OnePhase.Loads</a>.
+The model computes the voltages, currents and powers on each phase.
+</p>
+<p>
+For more information, see <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl</a> and
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Inductive\">
+AixLib.Electrical.AC.OnePhase.Loads.Inductive</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Inductive;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Inductive_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Inductive_N.mo
new file mode 100644
index 0000000000..558d0719b9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Inductive_N.mo
@@ -0,0 +1,220 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+model Inductive_N
+  "Model of a three-phase unbalanced inductive load with neutral cable"
+  extends BaseClasses.LoadCtrl_N(
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Inductive load1(pf=pf,
+        use_pf_in=use_pf_in),
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Inductive load2(pf=pf,
+        use_pf_in=use_pf_in),
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Inductive load3(pf=pf,
+        use_pf_in=use_pf_in));
+  parameter Boolean use_pf_in = false
+    "If true, the power factor is defined by an input"
+    annotation(Dialog(group="Modeling assumption"));
+  parameter Real pf(min=0, max=1) = 0.8 "Power factor"  annotation(Dialog(group="Nominal conditions"));
+  Modelica.Blocks.Interfaces.RealInput pf_in_1(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase1) "Power factor of load on phase 1" annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={80,-120}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-60,-100})));
+  Modelica.Blocks.Interfaces.RealInput pf_in_2(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase2) "Power factor of load on phase 2" annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={40,-120}),iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={0,-100})));
+  Modelica.Blocks.Interfaces.RealInput pf_in_3(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in and plugPhase3) "Power factor of load on phase 3" annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-60,-120}),
+                          iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={62,-100})));
+equation
+  connect(pf_in_1, load1.pf_in) annotation (Line(
+      points={{80,-120},{80,56},{10,56}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  connect(pf_in_2, load2.pf_in) annotation (Line(
+      points={{40,-120},{40,-14},{10,-14}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  connect(pf_in_3, load3.pf_in) annotation (Line(
+      points={{-60,-120},{-60,-82},{10,-82}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  annotation (
+  defaultComponentName="loa",
+  Icon(graphics={
+        Rectangle(
+          extent={{-80,80},{80,-80}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+                                   Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+        Rectangle(
+          extent={{0,0},{60,-12}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={70,0},
+          rotation=180),
+          Line(points={{-10,-1.22461e-15},{10,0}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Ellipse(extent={{-10,-10},{10,10}},
+          rotation=360),
+        Ellipse(extent={{30,-10},{50,10}}),
+        Ellipse(extent={{10,-10},{30,10}}),
+        Rectangle(
+          extent={{-10,0},{50,-12}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{26,3.18398e-15}},
+                                         color={0,0,0},
+          origin={76,0},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,1},
+          rotation=90),
+          Line(points={{-2,-2.44921e-16},{18,2.20429e-15}},
+                                         color={0,0,0},
+          origin={-82,0},
+          rotation=180),
+        Text(
+          extent={{-120,120},{120,80}},
+          textColor={0,0,0},
+          textString="%name"),
+        Ellipse(extent={{-10,-10},{10,10}},
+          origin={0,50},
+          rotation=360),
+        Ellipse(extent={{30,40},{50,60}}),
+        Ellipse(extent={{10,40},{30,60}}),
+        Rectangle(
+          extent={{-10,50},{50,38}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={60,50},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,51},
+          rotation=90),
+        Ellipse(extent={{-10,-10},{10,10}},
+          origin={0,-52},
+          rotation=360),
+        Ellipse(extent={{30,-62},{50,-42}}),
+        Ellipse(extent={{10,-62},{30,-42}}),
+        Rectangle(
+          extent={{-10,-52},{50,-64}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(points={{0,0},{12,1.46953e-15}},
+                                         color={0,0,0},
+          origin={-10,-52},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={60,-52},
+          rotation=180),
+        Rectangle(
+          extent={{-11,22},{11,-22}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={-44,-51},
+          rotation=90),
+        Line(
+          points={{60,50},{76,0},{60,-52}},
+          color={0,0,0},
+          smooth=Smooth.None),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,50},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+                                         color={0,0,0},
+          origin={-66,-52},
+          rotation=180)}), Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a three-phase unbalanced inductive load.
+The model extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N</a>
+and uses the load model from the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads\">
+AixLib.Electrical.AC.OnePhase.Loads</a>.
+The model computes the voltages, currents and powers on each phase.
+</p>
+<p>
+This model has a connector with four cables and it represents the neutral cable.
+The current in the neutral cable is computed as the algebraic sum of the currents
+of the loads.
+</p>
+<p>
+For more information, see <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N</a> and
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Inductive\">
+AixLib.Electrical.AC.OnePhase.Loads.Inductive</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Inductive_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Resistive.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Resistive.mo
new file mode 100644
index 0000000000..dbbba381b3
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Resistive.mo
@@ -0,0 +1,112 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+model Resistive
+  "Model of a three-phase unbalanced resistive load without neutral cable"
+  extends BaseClasses.LoadCtrl(
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Resistive load1,
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Resistive load2,
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Resistive load3);
+equation
+
+  annotation (
+  defaultComponentName="loa",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+       graphics={      Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+          Rectangle(
+            extent={{-80,80},{80,-80}},
+            lineColor={0,0,0},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+          origin={7.10543e-15,7.10543e-15},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{12,1.46953e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{18,2.20429e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+        Text(
+          extent={{-120,120},{120,80}},
+          textColor={0,0,0},
+          textString="%name"),
+        Line(
+          points={{-66,50},{-26,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,49},
+          rotation=90),
+        Line(
+          points={{34,50},{54,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{54,50},{70,0},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{34,0},{70,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,1},
+          rotation=90),
+        Line(
+          points={{-66,0},{-26,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-66,-50},{-26,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,-49},
+          rotation=90),
+        Line(
+          points={{34,-50},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None)}), Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a three-phase unbalanced resistive load.
+The model extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl</a>
+and uses the load model from the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads\">
+AixLib.Electrical.AC.OnePhase.Loads</a>.
+The model computes the voltages, currents and powers on each phase.
+</p>
+<p>
+For more information, see <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl</a> and
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Resistive\">
+AixLib.Electrical.AC.OnePhase.Loads.Resistive</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Resistive;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Resistive_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Resistive_N.mo
new file mode 100644
index 0000000000..70e8533935
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/Resistive_N.mo
@@ -0,0 +1,116 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads;
+model Resistive_N
+  "Model of a three-phase unbalanced resistive load with neutral cable"
+  extends BaseClasses.LoadCtrl_N(
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Resistive load1,
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Resistive load2,
+    redeclare AixLib.Electrical.AC.OnePhase.Loads.Resistive load3);
+equation
+
+  annotation (
+  defaultComponentName="loa",
+  Icon(graphics={      Rectangle(extent={{-100,100},{100,-100}},
+            lineColor={255,255,255}),
+          Rectangle(
+            extent={{-80,80},{80,-80}},
+            lineColor={0,0,0},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+          origin={7.10543e-15,7.10543e-15},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{12,1.46953e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+          Line(points={{-6.85214e-44,-8.39117e-60},{18,2.20429e-15}},
+                                       color={0,0,0},
+          origin={-80,0},
+          rotation=180),
+        Text(
+          extent={{-114,116},{126,76}},
+          textColor={0,0,0},
+          textString="%name"),
+        Line(
+          points={{-66,50},{-26,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,49},
+          rotation=90),
+        Line(
+          points={{34,50},{54,50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{54,50},{70,0},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{34,0},{70,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,1},
+          rotation=90),
+        Line(
+          points={{-66,0},{-26,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-66,-50},{-26,-50}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Rectangle(
+          extent={{-11,30},{11,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={4,-49},
+          rotation=90),
+        Line(
+          points={{34,-50},{54,-50}},
+          color={0,0,0},
+          smooth=Smooth.None)}), Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a three-phase unbalanced resistive load.
+The model extends from
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N</a>
+and uses the load model from the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads\">
+AixLib.Electrical.AC.OnePhase.Loads</a>.
+The model computes the voltages, currents and powers on each phase.
+</p>
+<p>
+This model has a connector with four cables and it represents the neutral cable.
+The current in the neutral cable is computed as the algebraic sum of the currents
+of the loads.
+</p>
+<p>
+For more information, see <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.BaseClasses.LoadCtrl_N</a> and
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Resistive\">
+AixLib.Electrical.AC.OnePhase.Loads.Resistive</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Resistive_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/package.mo
new file mode 100644
index 0000000000..ff1d9ec887
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/package.mo
@@ -0,0 +1,24 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced;
+package Loads "Package with load models for three-phase unbalanced AC systems"
+  extends Modelica.Icons.VariantsPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised load models, now they all have the optional voltage controller and the
+ability to select the type of connection: Wye (Y) or Delta (D).
+</li>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains models that represent different types of three
+phases unbalanced AC loads.
+</p>
+</html>"));
+end Loads;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/package.order
new file mode 100644
index 0000000000..6e70aae27a
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Loads/package.order
@@ -0,0 +1,10 @@
+Capacitive
+Capacitive_N
+Impedance
+Impedance_N
+Inductive
+Inductive_N
+Resistive
+Resistive_N
+Examples
+BaseClasses
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/GeneralizedProbe.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/GeneralizedProbe.mo
new file mode 100644
index 0000000000..4259c0c37b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/GeneralizedProbe.mo
@@ -0,0 +1,49 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.BaseClasses;
+partial model GeneralizedProbe
+  "Partial model of a generalized three-phase probe"
+  extends Icons.GeneralizedProbe;
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=480)
+    "RMS Nominal voltage (V_nominal >= 0)";
+  parameter Boolean perUnit = true "This flag display voltage in p.u.";
+  Modelica.Blocks.Interfaces.RealOutput V[3](each unit="1")
+    "Voltage in per unit"                                                         annotation (Placement(
+        transformation(extent={{60,20},{80,40}}), iconTransformation(extent={{60,
+            20},{80,40}})));
+  Modelica.Blocks.Interfaces.RealOutput theta[3](each unit="rad", each displayUnit="deg") "Angle" annotation (Placement(
+        transformation(extent={{60,-40},{80,-20}}), iconTransformation(extent={{60,
+            -40},{80,-20}})));
+  annotation (Icon(graphics={      Text(
+          extent={{40,60},{100,40}},
+          textColor={0,0,0},
+          pattern=LinePattern.Dash,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid,
+          textString="V"), Text(
+          extent={{18,-40},{140,-60}},
+          textColor={0,0,0},
+          pattern=LinePattern.Dash,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid,
+          textString="theta")}), Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model contains the parameters and connectors that are used by
+probe models such as <a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye</a> and
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta</a>.
+The output connectors are for the RMS voltage and the angle of the voltage phasors.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedProbe;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/package.mo
new file mode 100644
index 0000000000..2b21be9b7b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors;
+package BaseClasses "Package that contains base classes"
+extends Modelica.Icons.BasesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains base classes used by the models that are part of the package
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/package.order
new file mode 100644
index 0000000000..80ee31c9d0
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/BaseClasses/package.order
@@ -0,0 +1 @@
+GeneralizedProbe
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/Sensors.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/Sensors.mo
new file mode 100644
index 0000000000..34f8e17eba
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/Sensors.mo
@@ -0,0 +1,134 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.Examples;
+model Sensors "Test models for sensors and probes"
+  extends Modelica.Icons.Example;
+  Sources.FixedVoltage source(
+    f=60,
+    V=480)
+    "Voltage source without neutral cable"
+           annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  Loads.Resistive load(
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input)
+    "Load model"
+    annotation (Placement(transformation(extent={{20,20},{40,40}})));
+  ProbeWye probeWye(V_nominal=480) "Probe that measures the phase voltages"
+    annotation (Placement(transformation(extent={{-46,48},{-26,68}})));
+  ProbeDelta probeDelta(V_nominal=480) "Probe that measures the line voltages"
+    annotation (Placement(transformation(extent={{-20,48},{0,68}})));
+  Sources.FixedVoltage_N source_N(
+    f=60,
+    V=480)
+    "Voltage source with neutral cable"
+    annotation (Placement(transformation(extent={{-80,-40},{-60,-20}})));
+  Loads.Resistive_N load_N(
+    V_nominal=480,
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input)
+    "Load model"
+    annotation (Placement(transformation(extent={{20,-40},{40,-20}})));
+  ProbeWye_N probeWye_N(V_nominal=480)
+    annotation (Placement(transformation(extent={{-30,-12},{-10,8}})));
+  GeneralizedSensor sen "Generalized sensor withour neutral cable"
+    annotation (Placement(transformation(extent={{-4,20},{16,40}})));
+  GeneralizedSensor_N sen_N "Generalized sensor with neutral cable"
+    annotation (Placement(transformation(extent={{-8,-40},{12,-20}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    height=2e4,
+    duration=0.5,
+    offset=-1e4,
+    startTime=0.25)
+    annotation (Placement(transformation(extent={{80,-10},{60,10}})));
+equation
+  connect(probeWye.term, source.terminal) annotation (Line(
+      points={{-36,49},{-36,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(probeDelta.term, source.terminal) annotation (Line(
+      points={{-10,49},{-10,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(source_N.terminal, probeWye_N.term) annotation (Line(
+      points={{-60,-30},{-20,-30},{-20,-11}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(source_N.terminal, sen_N.terminal_n) annotation (Line(
+      points={{-60,-30},{-8,-30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(sen_N.terminal_p, load_N.terminal) annotation (Line(
+      points={{12,-30},{20,-30}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, load.terminal) annotation (Line(
+      points={{16,30},{20,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen.terminal_n, source.terminal) annotation (Line(
+      points={{-4,30},{-60,30}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow1) annotation (Line(
+      points={{59,0},{50,0},{50,38},{42,38}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow2) annotation (Line(
+      points={{59,0},{50,0},{50,30},{42,30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ramp.y, load.Pow3) annotation (Line(
+      points={{59,0},{50,0},{50,22},{42,22}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ramp.y, load_N.Pow1) annotation (Line(
+      points={{59,0},{50,0},{50,-22},{42,-22}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ramp.y, load_N.Pow2) annotation (Line(
+      points={{59,0},{50,0},{50,-30},{42,-30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ramp.y, load_N.Pow3) annotation (Line(
+      points={{59,0},{50,0},{50,-38},{42,-38}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation ( Documentation(
+revisions="<html>
+<ul>
+<li>
+February 27, 2016 by Michael Wetter:<br/>
+Stored example in a single file rather than a file with multiple examples.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/488\">#488</a>.
+</li>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Removed unused parameter assignment for <code>P_nominal</code>.
+</li>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>",
+info="<html>
+<p>
+This example shows how different types of sensors and probes can be used
+to measure the voltages, currents and powers in a three-phase
+unbalanced system.
+</p>
+<p>
+In this example all the loads are directly connected to the sources,
+avoiding voltage losses. The loads are all resistive and they start
+by consuming <i>10</i> kW for each phase, while at the end of the simulation
+they all produce <i>10</i> kW.
+</p>
+</html>"),
+experiment(StopTime=1.0, Tolerance=1e-6),
+__Dymola_Commands(file=
+ "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/Sensors.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Sensors;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/package.mo
new file mode 100644
index 0000000000..c556f29152
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+  annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/package.order
new file mode 100644
index 0000000000..c57005d181
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/package.order
@@ -0,0 +1 @@
+Sensors
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/GeneralizedSensor.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/GeneralizedSensor.mo
new file mode 100644
index 0000000000..21562ab9be
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/GeneralizedSensor.mo
@@ -0,0 +1,131 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors;
+model GeneralizedSensor
+  "Sensor for power, voltage and current (3 wire system, no neutral cable)"
+
+  Interfaces.Terminal_n terminal_n "Electrical connector side N"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+  Interfaces.Terminal_p terminal_p "Electrical connector side P"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}})));
+  Modelica.Blocks.Interfaces.RealOutput V[3](each final quantity="ElectricPotential",
+                                          each final unit="V") "Voltage"           annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={10,-40}),  iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-90})));
+  Modelica.Blocks.Interfaces.RealOutput I[3](each final quantity="ElectricCurrent",
+                                          each final unit="A") "Current"           annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={70,-40}), iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-90})));
+  Modelica.Blocks.Interfaces.RealOutput S[3, AixLib.Electrical.PhaseSystems.OnePhase.n](
+                                          each final quantity="Power",
+                                          each final unit="W") "Phase powers"             annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-50,-40}),iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-60,-90})));
+equation
+
+  for i in 1:3 loop
+    V[i]   = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal_n.phase[i].v);
+    I[i]   = AixLib.Electrical.PhaseSystems.OnePhase.systemCurrent(terminal_n.phase[i].i);
+    S[i,:] = AixLib.Electrical.PhaseSystems.OnePhase.phasePowers_vi(v=terminal_n.phase[i].v, i=terminal_n.phase[i].i);
+  end for;
+
+  connect(terminal_n, terminal_p) annotation (Line(
+      points={{-100,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (defaultComponentName="sen",
+ Icon(graphics={
+        Rectangle(
+          extent={{-70,28},{70,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-60,60},{60,-60}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-92,0},{-70,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Text(
+          extent={{-120,-42},{0,-82}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="S"),
+        Polygon(
+          points={{-0.48,33.6},{18,28},{18,59.2},{-0.48,33.6}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(points={{-37.6,15.7},{-54,22}},     color={0,0,0}),
+        Line(points={{-22.9,34.8},{-32,50}},     color={0,0,0}),
+        Line(points={{0,60},{0,42}}, color={0,0,0}),
+        Line(points={{22.9,34.8},{32,50}},     color={0,0,0}),
+        Line(points={{37.6,15.7},{54,24}},     color={0,0,0}),
+        Line(points={{0,2},{9.02,30.6}}, color={0,0,0}),
+        Ellipse(
+          extent={{-5,7},{5,-3}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{70,0},{92,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Text(
+          extent={{-60,-42},{60,-82}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="V"),
+        Text(
+          extent={{0,-40},{120,-80}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="I"),
+        Text(
+          extent={{-120,100},{120,60}},
+          textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+Ideal sensor that measures power, voltage and current in a three-phase unbalanced system
+without a neutral cable.
+The two components of the power <i>S</i> are the active and reactive power for each phase.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Corrected wrong access to phase system.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/570\">#570</a>.
+</li>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/GeneralizedSensor_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/GeneralizedSensor_N.mo
new file mode 100644
index 0000000000..e83f4a53a7
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/GeneralizedSensor_N.mo
@@ -0,0 +1,134 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors;
+model GeneralizedSensor_N
+  "Sensor for power, voltage and current (4 wire system, with neutral cable)"
+
+  Interfaces.Terminal4_n terminal_n "Electrical connector side N"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+  Interfaces.Terminal4_p terminal_p "Electrical connector side P"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}})));
+  Modelica.Blocks.Interfaces.RealOutput V[4](each final quantity="ElectricPotential",
+                                          each final unit="V") "Voltage"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={10,-40}),  iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-90})));
+  Modelica.Blocks.Interfaces.RealOutput I[4](each final quantity="ElectricCurrent",
+                                          each final unit="A") "Current"
+   annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={70,-40}), iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-90})));
+  Modelica.Blocks.Interfaces.RealOutput S[4, AixLib.Electrical.PhaseSystems.OnePhase.n](
+                                          each final quantity="Power",
+                                          each final unit="W") "Phase powers"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-50,-40}),iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-60,-90})));
+equation
+
+  for i in 1:4 loop
+    V[i]   = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(terminal_n.phase[i].v);
+    I[i]   = AixLib.Electrical.PhaseSystems.OnePhase.systemCurrent(terminal_n.phase[i].i);
+    S[i,:] = AixLib.Electrical.PhaseSystems.OnePhase.phasePowers_vi(v=terminal_n.phase[i].v, i=terminal_n.phase[i].i);
+  end for;
+
+  connect(terminal_n, terminal_p) annotation (Line(
+      points={{-100,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (defaultComponentName="sen",
+ Icon(graphics={
+        Rectangle(
+          extent={{-70,28},{70,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-60,60},{60,-60}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-92,0},{-70,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Text(
+          extent={{-120,-42},{0,-82}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="S"),
+        Polygon(
+          points={{-0.48,33.6},{18,28},{18,59.2},{-0.48,33.6}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(points={{-37.6,15.7},{-54,22}},     color={0,0,0}),
+        Line(points={{-22.9,34.8},{-32,50}},     color={0,0,0}),
+        Line(points={{0,60},{0,42}}, color={0,0,0}),
+        Line(points={{22.9,34.8},{32,50}},     color={0,0,0}),
+        Line(points={{37.6,15.7},{54,24}},     color={0,0,0}),
+        Line(points={{0,2},{9.02,30.6}}, color={0,0,0}),
+        Ellipse(
+          extent={{-5,7},{5,-3}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{70,0},{92,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Text(
+          extent={{-60,-42},{60,-82}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="V"),
+        Text(
+          extent={{0,-40},{120,-80}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="I"),
+        Text(
+          extent={{-120,100},{120,60}},
+          textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+Ideal sensor that measures power, voltage and current in a three-phase unbalanced system
+with neutral cable.
+The two components of the power <i>S</i> are the active and reactive power for each phase.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Corrected wrong access to phase system.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/570\">#570</a>.
+</li>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeDelta.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeDelta.mo
new file mode 100644
index 0000000000..83fbe08746
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeDelta.mo
@@ -0,0 +1,63 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors;
+model ProbeDelta
+  "Model of a probe that measures voltage magnitude and angle (Delta configuration)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.BaseClasses.GeneralizedProbe;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal_n
+  term "Electrical connector" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,-90})));
+  Interfaces.WyeToDelta wyeToDelta "Y to D transformation"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
+        origin={20,0})));
+equation
+  for i in 1:3 loop
+      theta[i] = AixLib.Electrical.PhaseSystems.OnePhase.phase(wyeToDelta.delta.phase[i].v);
+      if perUnit then
+        V[i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(wyeToDelta.delta.phase[i].v)/V_nominal;
+      else
+        V[i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(wyeToDelta.delta.phase[i].v);
+      end if;
+  end for;
+
+  connect(term, wyeToDelta.wye) annotation (Line(
+      points={{0,-90},{0,4.44089e-16},{10,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (defaultComponentName="sen",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={Text(
+          extent={{40,60},{100,40}},
+          textColor={0,120,120},
+          pattern=LinePattern.Dash,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid,
+          textString="V"), Text(
+          extent={{18,-40},{140,-60}},
+          textColor={0,120,120},
+          pattern=LinePattern.Dash,
+          fillColor={0,120,120},
+          fillPattern=FillPattern.Solid,
+          textString="theta"),
+        Line(
+          points={{-20,-44},{0,-14},{20,-44},{-20,-44}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5)}),         Documentation(info="<html>
+<p>
+This model represents a probe that measures the RMS voltage and the angle
+of the voltage phasors at a given point. The probes are connected
+in the Wye (Y) grounded configuration.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ProbeDelta;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeWye.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeWye.mo
new file mode 100644
index 0000000000..62f49ea39e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeWye.mo
@@ -0,0 +1,57 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors;
+model ProbeWye
+  "Model of a probe that measures voltage magnitude and angle (Wye configuration)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.BaseClasses.GeneralizedProbe;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal_n
+    term "Electrical connector" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,-90})));
+  Interfaces.WyeToWyeGround wyeToWyeGround "Y to Y grounded transformation"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
+        origin={20,0})));
+equation
+  for i in 1:3 loop
+      theta[i] = AixLib.Electrical.PhaseSystems.OnePhase.phase(wyeToWyeGround.wyeg.phase[i].v);
+      if perUnit then
+        V[i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(wyeToWyeGround.wyeg.phase[i].v)/(V_nominal/sqrt(3));
+      else
+        V[i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(wyeToWyeGround.wyeg.phase[i].v);
+      end if;
+  end for;
+
+  connect(term, wyeToWyeGround.wye) annotation (Line(
+      points={{0,-90},{0,4.44089e-16},{10,4.44089e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (defaultComponentName="sen",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Line(
+          points={{0,-10},{0,-30},{-14,-44}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{0,-30},{14,-44}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5)}),
+Documentation(info="<html>
+<p>
+This model represents a probe that measures the RMS voltage and the angle
+of the voltage phasors at a given point. The probes are connected
+in the Wye (Y) grounded configuration.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ProbeWye;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeWye_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeWye_N.mo
new file mode 100644
index 0000000000..ef6e00d912
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/ProbeWye_N.mo
@@ -0,0 +1,54 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors;
+model ProbeWye_N
+  "Model of a probe that measures voltage magnitude and angle (Wye configuration) witn neutral cable connection"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.BaseClasses.GeneralizedProbe;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal4_n
+    term "Electrical connector" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,-90})));
+equation
+
+  for i in 1:4 loop
+    term.phase[i].i = zeros(AixLib.Electrical.PhaseSystems.OnePhase.n);
+  end for;
+
+  for i in 1:3 loop
+      theta[i] = AixLib.Electrical.PhaseSystems.OnePhase.phase(term.phase[i].v - term.phase[4].v);
+      if perUnit then
+        V[i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(term.phase[i].v - term.phase[4].v)/(V_nominal/sqrt(3));
+      else
+        V[i] = AixLib.Electrical.PhaseSystems.OnePhase.systemVoltage(term.phase[i].v - term.phase[4].v);
+      end if;
+  end for;
+  annotation (defaultComponentName="sen",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Line(
+          points={{0,-10},{0,-30},{-14,-44}},
+          color={127,0,127},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(
+          points={{0,-30},{14,-44}},
+          color={127,0,127},
+          smooth=Smooth.None,
+          thickness=0.5)}),
+Documentation(info="<html>
+<p>
+This model represents a probe that measures the RMS voltage and the angle
+of the voltage phasors at a given point. The probes are connected
+in the Wye (Y) grounded configuration.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ProbeWye_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/package.mo
new file mode 100644
index 0000000000..65e28db372
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced;
+package Sensors "Package with sensor models for three-phase unbalanced AC systems"
+  extends Modelica.Icons.SensorsPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains models that represent different types of three
+phases unbalanced AC/AC sensors.
+</p>
+</html>"));
+end Sensors;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/package.order
new file mode 100644
index 0000000000..9d932a9926
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sensors/package.order
@@ -0,0 +1,7 @@
+GeneralizedSensor
+GeneralizedSensor_N
+ProbeDelta
+ProbeWye
+ProbeWye_N
+Examples
+BaseClasses
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/BaseUnbalancedWindTurbine.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/BaseUnbalancedWindTurbine.mo
new file mode 100644
index 0000000000..ae0818ebc2
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/BaseUnbalancedWindTurbine.mo
@@ -0,0 +1,205 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses;
+partial model BaseUnbalancedWindTurbine
+  "Partial model for an unbalanced wind power source"
+  extends AixLib.Electrical.Interfaces.PartialPluggableUnbalanced;
+  extends AixLib.Electrical.Interfaces.PartialAcDcParameters;
+  extends AixLib.Electrical.BaseClasses.WindTurbine.PartialWindTurbineBase(
+    V_nominal(start = 480));
+  parameter Real scaleFraction[3](each min=0, each max=1.0) = ones(3)/3
+    "Fraction of power allocated to the wind turbines of each phase";
+  replaceable OnePhase.Sources.WindTurbine wt_phase2(
+    pf=pf,
+    eta_DCAC=eta_DCAC,
+    scale=scale*scaleFraction[2],
+    h=h,
+    hRef=hRef,
+    nWin=nWin,
+    tableOnFile=tableOnFile,
+    table=table,
+    tableName=tableName,
+    fileName=fileName,
+    V_nominal=V_nominal/sqrt(3))
+      if plugPhase2 "Wind turbine phase 2"
+    annotation (Placement(transformation(extent={{-20,-10},{-40,10}})));
+
+  replaceable OnePhase.Sources.WindTurbine wt_phase3(
+    pf=pf,
+    eta_DCAC=eta_DCAC,
+    scale=scale*scaleFraction[3],
+    h=h,
+    hRef=hRef,
+    nWin=nWin,
+    tableOnFile=tableOnFile,
+    table=table,
+    tableName=tableName,
+    fileName=fileName,
+    V_nominal=V_nominal/sqrt(3))
+      if plugPhase3 "Wind turbine phase 3"
+    annotation (Placement(transformation(extent={{-20,-60},{-40,-40}})));
+
+  replaceable OnePhase.Sources.WindTurbine wt_phase1(
+    pf=pf,
+    eta_DCAC=eta_DCAC,
+    scale=scale*scaleFraction[1],
+    h=h,
+    hRef=hRef,
+    nWin=nWin,
+    tableOnFile=tableOnFile,
+    table=table,
+    tableName=tableName,
+    fileName=fileName,
+    V_nominal=V_nominal/sqrt(3))
+      if plugPhase1 "Wind turbine phase 1"
+    annotation (Placement(transformation(extent={{-18,40},{-38,60}})));
+  Modelica.Blocks.Math.Add3 sumBlock "Sum of th epower generated on each phase"
+    annotation (Placement(transformation(extent={{32,50},{52,70}})));
+equation
+
+  assert(abs(sum(scaleFraction)-1) < Modelica.Constants.eps,
+  "Model that extends AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses.BaseUnbalancedWindTurbine,
+  has an invalid value for the vector scaleFraction[:]. The sum of the
+  elements has to be equal to 1.0.",
+  level=AssertionLevel.error);
+
+  if plugPhase1 then
+    connect(wt_phase1.P, sumBlock.u1) annotation (Line(
+      points={{-39,56},{-60,56},{-60,82},{20,82},{20,68},{30,68}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  else
+    sumBlock.u1 = 0;
+  end if;
+
+  if plugPhase2 then
+    connect(wt_phase2.P, sumBlock.u2) annotation (Line(
+      points={{-41,6},{-64,6},{-64,86},{12,86},{12,60},{30,60}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  else
+    sumBlock.u2 = 0;
+  end if;
+
+  if plugPhase3 then
+    connect(wt_phase3.P, sumBlock.u3) annotation (Line(
+      points={{-41,-44},{-68,-44},{-68,90},{4,90},{4,52},{30,52}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+  else
+    sumBlock.u3 = 0;
+  end if;
+
+  connect(sumBlock.y, P) annotation (Line(
+      points={{53,60},{110,60}},
+      color={0,0,127},
+      smooth=Smooth.None,
+      pattern=LinePattern.Dash));
+
+  connect(vWin, wt_phase1.vWin) annotation (Line(
+      points={{0,120},{0,72},{-28,72},{-28,62}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(vWin, wt_phase2.vWin) annotation (Line(
+      points={{0,120},{0,72},{-52,72},{-52,20},{-30,20},{-30,12}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(vWin, wt_phase3.vWin) annotation (Line(
+      points={{0,120},{0,72},{-52,72},{-52,-26},{-30,-26},{-30,-38}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation ( Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          pattern=LinePattern.None,
+          fillColor={202,230,255},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{42,44},{46,-54}},
+          fillColor={233,233,233},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{-42,12},{-38,-86}},
+          fillColor={233,233,233},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-44,10},{-26,-42},{-38,14},{-44,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-38,10},{8,44},{-42,16},{-38,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-42,10},{-90,38},{-38,16},{-42,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{40,42},{100,38},{42,48},{40,42}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-21,-17},{27,17},{-25,-11},{-21,-17}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          origin={29,67},
+          rotation=90,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{24,-14},{-20,22},{26,-8},{24,-14}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          origin={32,18},
+          rotation=90,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{-46,18},{-34,6}},
+          lineColor={0,0,0},
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{38,50},{50,38}},
+          lineColor={0,0,0},
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(info="<html>
+<p>
+This model is a partial class extended by three-phase unbalanced
+wind turbine power sources.
+</p>
+<p>
+The model has boolean parameters <code>plugPhase1</code>, <code>plugPhase2</code>,
+and <code>plugPhase3</code> that can be used to connect the wind turbines in an
+unbalanced configuration.
+</p>
+<p>
+The model has an array <code>scaleFraction[3]</code> that is used to determine how
+to partition the power of the wind turbines on the three-phase. By default it is assumed
+a uniform partition <code>scaleFraction[3] = {1/3, 1/3, 1/3}</code>.
+</p>
+</html>",
+        revisions="<html>
+<ul>
+<li>
+September 25, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BaseUnbalancedWindTurbine;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/PartialSource.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/PartialSource.mo
new file mode 100644
index 0000000000..723f0b2fa8
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/PartialSource.mo
@@ -0,0 +1,37 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses;
+partial model PartialSource
+  "Partial model for a three-phase AC unbalanced voltage source without neutral cable"
+
+  Interfaces.Connection3to3Ground_p connection3to4
+    "Connection between three to four AC connectors with ground connection"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+  OnePhase.Basics.Ground ground "Ground reference"
+    annotation (Placement(transformation(extent={{10,-60},{30,-40}})));
+  Interfaces.Terminal_p terminal "Connector for three-phase unbalanced systems"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}})));
+equation
+
+  connect(connection3to4.terminal3,terminal)  annotation (Line(
+      points={{60,0},{100,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(ground.terminal, connection3to4.ground4) annotation (Line(
+      points={{20,-40},{20,-6},{39.6,-6}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation ( Documentation(info="<html>
+<p>
+This model is a partial class extended by three-phase unbalanced
+voltage sources without neutral cable connection.
+</p>
+</html>",
+        revisions="<html>
+<ul>
+<li>
+September 25, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialSource;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/PartialSource_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/PartialSource_N.mo
new file mode 100644
index 0000000000..fc15b9818f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/PartialSource_N.mo
@@ -0,0 +1,38 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses;
+partial model PartialSource_N "Partial model for a three-phase AC unbalanced voltage source
+  with neutral cable"
+
+  OnePhase.Basics.Ground ground "Ground reference"
+    annotation (Placement(transformation(extent={{10,-60},{30,-40}})));
+  Interfaces.Terminal4_p terminal
+    "Connector for three-phase unbalanced systems with neutral cable"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}})));
+equation
+
+  connect(ground.terminal, terminal.phase[4]) annotation (Line(
+      points={{20,-40},{20,0},{100,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation ( Documentation(info="<html>
+<p>
+This model is a partial class extended by three-phase unbalanced
+voltage sources that have a neutral cable.
+</p>
+<p>
+The neutral cable is connected to the ground reference.
+</p>
+</html>",
+        revisions="<html>
+<ul>
+<li>
+September 25, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialSource_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/UnbalancedWindTurbine.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/UnbalancedWindTurbine.mo
new file mode 100644
index 0000000000..466153bce5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/UnbalancedWindTurbine.mo
@@ -0,0 +1,121 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses;
+model UnbalancedWindTurbine
+  "Base model for an unbalanced wind power source without neutral cable"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses.BaseUnbalancedWindTurbine;
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses.PartialSource;
+protected
+  Interfaces.Adapter3to3 ada "Adapter"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+equation
+  if plugPhase1 then
+    connect(wt_phase1.terminal, ada.terminals[1]) annotation (Line(points={{-18,50},
+            {-12,50},{-12,-0.533333},{-10,-0.533333}},
+                                                     color={0,120,120}));  end if;
+
+  if plugPhase2 then
+    connect(wt_phase2.terminal, ada.terminals[2])
+    annotation (Line(points={{-20,0},{-15,0},{-10,0}}, color={0,120,120}));
+   end if;
+
+  if plugPhase3 then
+   connect(wt_phase3.terminal, ada.terminals[3]) annotation (Line(points={{-20,-50},
+            {-14,-50},{-14,-30},{-14,0.533333},{-10,0.533333}},
+                                                              color={0,120,120}));
+  end if;
+  connect(ada.terminal, connection3to4.terminal4)
+    annotation (Line(points={{10,0},{26,0},{40,0}}, color={0,120,120}));
+  annotation ( Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          pattern=LinePattern.None,
+          fillColor={202,230,255},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{42,44},{46,-54}},
+          fillColor={233,233,233},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{-42,12},{-38,-86}},
+          fillColor={233,233,233},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-44,10},{-26,-42},{-38,14},{-44,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-38,10},{8,44},{-42,16},{-38,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-42,10},{-90,38},{-38,16},{-42,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{40,42},{100,38},{42,48},{40,42}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-21,-17},{27,17},{-25,-11},{-21,-17}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          origin={29,67},
+          rotation=90,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{24,-14},{-20,22},{26,-8},{24,-14}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          origin={32,18},
+          rotation=90,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{-46,18},{-34,6}},
+          lineColor={0,0,0},
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{38,50},{50,38}},
+          lineColor={0,0,0},
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(info="<html>
+<p>
+This model is a class extended by three-phase unbalanced
+wind turbine power sources without neutral cable.
+</p>
+</html>",
+        revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapter for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+September 25, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end UnbalancedWindTurbine;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/UnbalancedWindTurbine_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/UnbalancedWindTurbine_N.mo
new file mode 100644
index 0000000000..fc93e08b83
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/UnbalancedWindTurbine_N.mo
@@ -0,0 +1,136 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses;
+model UnbalancedWindTurbine_N
+  "Base model for an unbalanced wind power source with neutral cable"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses.BaseUnbalancedWindTurbine;
+  Interfaces.Terminal4_p terminal
+    "Connector for three-phase unbalanced systems with neutral cable"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}})));
+  Interfaces.Connection3to4_p conn3to4 "Connection between 3 to 4 wire"
+    annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        origin={40,0})));
+protected
+  Interfaces.Adapter3to3 ada "Adapter"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+equation
+
+  if plugPhase1 then
+    connect(wt_phase1.terminal, ada.terminals[1]) annotation (Line(points={{-18,50},
+            {-10,50},{-10,-0.533333},{0,-0.533333}},
+                                                   color={0,120,120}));
+  end if;
+
+  if plugPhase2 then
+    connect(wt_phase2.terminal, ada.terminals[2])
+    annotation (Line(points={{-20,0},{-10,0},{0,0}}, color={0,120,120}));
+  end if;
+
+  if plugPhase3 then
+    connect(wt_phase3.terminal, ada.terminals[3]) annotation (Line(points={{-20,-50},
+            {-10,-50},{-10,0.533333},{0,0.533333}},
+                                                  color={0,120,120}));
+  end if;
+
+  connect(conn3to4.terminal4, terminal) annotation (Line(
+      points={{50,0},{100,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(ada.terminal, conn3to4.terminal3)
+    annotation (Line(points={{20,0},{25,0},{30,0}}, color={0,120,120}));
+  annotation ( Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          pattern=LinePattern.None,
+          fillColor={202,230,255},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{42,44},{46,-54}},
+          fillColor={233,233,233},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{-42,12},{-38,-86}},
+          fillColor={233,233,233},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-44,10},{-26,-42},{-38,14},{-44,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-38,10},{8,44},{-42,16},{-38,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-42,10},{-90,38},{-38,16},{-42,10}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{40,42},{100,38},{42,48},{40,42}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-21,-17},{27,17},{-25,-11},{-21,-17}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          origin={29,67},
+          rotation=90,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{24,-14},{-20,22},{26,-8},{24,-14}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          origin={32,18},
+          rotation=90,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{-46,18},{-34,6}},
+          lineColor={0,0,0},
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{38,50},{50,38}},
+          lineColor={0,0,0},
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(info="<html>
+<p>
+This model is a class extended by three-phase unbalanced
+wind turbine power sources with neutral cable connection.
+</p>
+<p>
+The neutral cable is connected to the ground reference.
+</p>
+</html>",
+        revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapter for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+September 25, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end UnbalancedWindTurbine_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/package.mo
new file mode 100644
index 0000000000..299e603557
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/package.mo
@@ -0,0 +1,26 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources;
+package BaseClasses "Package with base class models"
+  extends Modelica.Icons.BasesPackage;
+
+
+
+
+
+
+
+
+  annotation (Documentation(info="<html>
+<p>
+This package contains base classes used by the models that are part of the package
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/package.order
new file mode 100644
index 0000000000..d34825613e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/BaseClasses/package.order
@@ -0,0 +1,5 @@
+BaseUnbalancedWindTurbine
+PartialSource
+PartialSource_N
+UnbalancedWindTurbine
+UnbalancedWindTurbine_N
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/FixedVoltageSource.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/FixedVoltageSource.mo
new file mode 100644
index 0000000000..39253d913e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/FixedVoltageSource.mo
@@ -0,0 +1,61 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.Examples;
+model FixedVoltageSource
+  "This example illustrates how using a fixed voltage source"
+  extends Modelica.Icons.Example;
+  FixedVoltage                             grid(
+    f=60,
+    V=480,
+    definiteReference=true,
+    phiSou=0.17453292519943) "AC one phase electrical grid"
+    annotation (Placement(transformation(extent={{-40,30},{-20,50}})));
+  Sensors.ProbeWye                  sen(V_nominal=480)
+    "Probe that measures the voltage at the load"
+    annotation (Placement(transformation(extent={{-10,60},{10,80}})));
+  Loads.Inductive loa(P_nominal=-2000, V_nominal=480) "Inductive load"
+    annotation (Placement(transformation(extent={{20,30},{40,50}})));
+  FixedVoltage_N grid_N(
+    f=60,
+    V=480,
+    definiteReference=true,
+    phiSou=0.17453292519943) "AC one phase electrical grid"
+    annotation (Placement(transformation(extent={{-40,-70},{-20,-50}})));
+  Sensors.ProbeWye_N sen_N(V_nominal=480)
+    "Probe that measures the voltage at the load"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  Loads.Inductive_N loa_N(P_nominal=-2000, V_nominal=480) "Inductive load"
+    annotation (Placement(transformation(extent={{20,-70},{40,-50}})));
+equation
+  connect(grid.terminal, loa.terminal) annotation (Line(
+      points={{-20,40},{20,40}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(grid.terminal, sen.term) annotation (Line(
+      points={{-20,40},{0,40},{0,61}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(grid_N.terminal, loa_N.terminal) annotation (Line(
+      points={{-20,-60},{20,-60}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(grid_N.terminal, sen_N.term) annotation (Line(
+      points={{-20,-60},{0,-60},{0,-39}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (    experiment(StopTime=1.0, Tolerance=1e-6),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/FixedVoltageSource.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 25, 2014, by Marco Bonvini:<br/>
+Created model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example shows how to use a fixed voltage generator model.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FixedVoltageSource;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine.mo
new file mode 100644
index 0000000000..9f291918ee
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine.mo
@@ -0,0 +1,93 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.Examples;
+model WindTurbine "Example for the WindTurbine AC model"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.WindTurbine tur(
+    table=[3.5, 0;
+           5.5,   100;
+           12, 900;
+           14, 1000;
+           25, 1000], h=10,
+    scale=10,
+    V_nominal=480,
+    scaleFraction={0.5,0.25,0.25}) "Wind turbine"
+    annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        origin={60,0})));
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
+      computeWetBulbTemperature=false,
+      filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data"
+    annotation (Placement(transformation(extent={{-52,36},{-32,56}})));
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather bus";
+  Loads.Resistive                           res(P_nominal=-500, V_nominal=480)
+    "Resistive line"
+    annotation (Placement(transformation(extent={{-22,-30},{-2,-10}})));
+  Grid                                                     sou(f=60, V=480)
+    "Voltage source"
+    annotation (Placement(transformation(extent={{-80,10},{-60,30}})));
+  Sensors.GeneralizedSensor                         sen "Generalized sensor"
+    annotation (Placement(transformation(extent={{8,-10},{28,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Line line(
+    l=200,
+    P_nominal=5000,
+    V_nominal=480)
+    annotation (Placement(transformation(extent={{-40,-10},{-20,10}})));
+equation
+  connect(weaDat.weaBus,weaBus)  annotation (Line(
+      points={{-32,46},{26,46}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(weaBus.winSpe,tur. vWin) annotation (Line(
+      points={{26,46},{60,46},{60,12}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(sou.terminal, res.terminal) annotation (Line(
+      points={{-70,10},{-70,-20},{-22,-20}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, tur.terminal) annotation (Line(
+      points={{28,0},{50,0}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(sou.terminal, line.terminal_n) annotation (Line(
+      points={{-70,10},{-70,0},{-40,5.55112e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line.terminal_p, sen.terminal_n) annotation (Line(
+      points={{-20,5.55112e-16},{8,0},{8,6.66134e-16}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (    experiment(StopTime=172800, Tolerance=1e-6),
+    Documentation(info="<html>
+<p>
+This model illustrates the use of the wind turbine model,
+which is connected to a AC voltage source and a resistive load.
+This voltage source can represent the grid to which the
+circuit is connected.
+Wind data for San Francisco, CA, are used.
+The turbine cut-in wind speed is <i>3.5</i> m/s,
+and hence it is off in the first day when the wind speed is low.
+</p>
+<p>
+The wind turbines produce different amounts of power on each phase according to the fractions
+specified by the vector <code>scaleFraction={0.5,0.25,0.25}</code>. In this example, 50%
+of the power generation is on phase 1, 30% on phase 2 and 20% on phase 3.
+As expected the phase with the higher power production has the higher voltage deviation
+from the nominal condition.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+September 25, 2014, by Marco Bonvini:<br/>
+Created model and documentation
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end WindTurbine;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine_N.mo
new file mode 100644
index 0000000000..408a42c293
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine_N.mo
@@ -0,0 +1,94 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.Examples;
+model WindTurbine_N "Example for the WindTurbine AC model with neutral cable"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.WindTurbine_N tur(
+    table=[3.5, 0;
+           5.5,   100;
+           12, 900;
+           14, 1000;
+           25, 1000], h=10,
+    scale=10,
+    V_nominal=480,
+    plugPhase2=false,
+    scaleFraction={0.4,0.0,0.6}) "Wind turbine"
+    annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        origin={60,0})));
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
+      computeWetBulbTemperature=false,
+      filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data"
+    annotation (Placement(transformation(extent={{-52,36},{-32,56}})));
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather bus";
+  Loads.Resistive_N                          res(P_nominal=-500, V_nominal=480)
+    "Resistive line"
+    annotation (Placement(transformation(extent={{-22,-30},{-2,-10}})));
+  Grid_N                                                     sou(f=60, V=480)
+    "Voltage source"
+    annotation (Placement(transformation(extent={{-80,10},{-60,30}})));
+  Sensors.GeneralizedSensor_N                         sen "Generalized sensor"
+    annotation (Placement(transformation(extent={{8,-10},{28,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Line_N line(
+    l=200,
+    P_nominal=5000,
+    V_nominal=480)
+    annotation (Placement(transformation(extent={{-40,-10},{-20,10}})));
+equation
+  connect(weaDat.weaBus,weaBus)  annotation (Line(
+      points={{-32,46},{26,46}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(weaBus.winSpe,tur. vWin) annotation (Line(
+      points={{26,46},{60,46},{60,12}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(tur.terminal, sen.terminal_p) annotation (Line(
+      points={{50,0},{28,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(sen.terminal_n, line.terminal_p) annotation (Line(
+      points={{8,0},{-20,0}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(line.terminal_n, sou.terminal) annotation (Line(
+      points={{-40,0},{-70,0},{-70,10}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  connect(res.terminal, sou.terminal) annotation (Line(
+      points={{-22,-20},{-70,-20},{-70,10}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (    experiment(StopTime=172800, Tolerance=1e-6),
+    Documentation(info="<html>
+<p>
+This model illustrates the use of the wind turbine model with neutral cable,
+which is connected to a AC voltage source and a resistive load.
+This voltage source can represent the grid to which the
+circuit is connected.
+Wind data for San Francisco, CA, are used.
+The turbine cut-in wind speed is <i>3.5</i> m/s,
+and hence it is off in the first day when the wind speed is low.
+</p>
+<p>
+The wind turbines produce different amounts of power on each phase according to the fractions
+specified by the vector <code>scaleFraction={0.4,0.0,0.6}</code>. In this example, 40%
+of the power generation is on phase 1, 0% on phase 2 (disconnected) and 60% on phase 3.
+As expected the phase with the higher power production has the higher voltage deviation
+from the nominal condition.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+January 10, 2014, by Marco Bonvini:<br/>
+Created model and documentation
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine_N.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end WindTurbine_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/package.mo
new file mode 100644
index 0000000000..688afe299d
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+  annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/package.order
new file mode 100644
index 0000000000..0a5a5c8383
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/package.order
@@ -0,0 +1,3 @@
+FixedVoltageSource
+WindTurbine
+WindTurbine_N
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/FixedVoltage.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/FixedVoltage.mo
new file mode 100644
index 0000000000..8e01b4e19b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/FixedVoltage.mo
@@ -0,0 +1,102 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources;
+model FixedVoltage "Fixed voltage source"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses.PartialSource;
+  parameter Modelica.Units.SI.Frequency f(start=60) "Frequency of the source";
+  parameter Modelica.Units.SI.Voltage V(start=480) "RMS voltage of the source";
+  parameter Modelica.Units.SI.Angle phiSou=0 "Phase shift of the source";
+  parameter Boolean potentialReference = true
+    "Serve as potential root for the reference angle theta"
+     annotation (Evaluate=true, Dialog(group="Reference Parameters"));
+  parameter Boolean definiteReference = false
+    "Serve as definite root for the reference angle theta"
+     annotation (Evaluate=true, Dialog(group="Reference Parameters"));
+  constant Modelica.Units.SI.Angle angle120=2*Modelica.Constants.pi/3
+    "Phase shift between the phase voltages";
+  OnePhase.Sources.FixedVoltage vPhase[3](
+    each f=f,
+    potentialReference={potentialReference, potentialReference, potentialReference},
+    definiteReference={definiteReference, false, false},
+    phiSou={phiSou,phiSou - angle120,phiSou + angle120},
+    each V=V/sqrt(3)) "Voltage sources on the three-phase"
+             annotation (Placement(transformation(extent={{-50,-10},{-30,10}})));
+protected
+  Interfaces.Adapter3to3 ada "Adapter between the different connectors"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+equation
+
+  connect(vPhase.terminal, ada.terminals)
+    annotation (Line(points={{-30,0},{-9.8,0},{-9.8,0}},
+                                                       color={0,120,120}));
+  connect(ada.terminal, connection3to4.terminal4)
+    annotation (Line(points={{10,0},{25,0},{40,0}}, color={0,120,120}));
+  annotation (
+  defaultComponentName="sou",
+ Icon(graphics={
+        Ellipse(
+          extent={{-60,60},{60,-60}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid), Line(
+          points={{-34,0},{-14,40},{6,0},{26,-40},{46,0}},
+          color={120,120,120},
+          smooth=Smooth.Bezier),          Line(
+          points={{-44,0},{-24,40},{-4,0},{16,-40},{36,0}},
+          color={0,0,0},
+          smooth=Smooth.Bezier),          Line(
+          points={{-24,0},{-4,40},{16,0},{36,-40},{56,0}},
+          color={215,215,215},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{60,0},{90,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Text(
+          extent={{-120,100},{120,60}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-120,-60},{120,-100}},
+          textColor={0,0,0},
+          textString="V = %V")}),
+    Documentation(info="<html>
+<p>
+This is a constant voltage source, specifying the complex voltage
+by the RMS voltage and the phase shift.
+</p>
+<p>
+The parameters <code>potentialReference</code> and <code>definiteReference</code>
+are used to define if the source model should be selected as source for
+the reference angles <code>theta</code> or not.
+More information about overdetermined connectors can be found
+in <a href=\"#Olsson2008\">Olsson Et Al. (2008)</a>.
+</p>
+
+<h4>References</h4>
+<p>
+<a name=\"Olsson2008\"/>
+Hans Olsson, Martin Otter, Sven Erik Mattson and Hilding Elmqvist.<br/>
+<a href=\"http://elib-v3.dlr.de/55892/1/otter2008-modelica-balanced-models.pdf\">
+Balanced Models in Modelica 3.0 for Increased Model Quality</a>.<br/>
+Proc. of the 7th Modelica Conference, Bielefeld, Germany, March 2008.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Updated documentation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/427\">issue 427</a>.
+</li>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Added adapter model for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">issue 426</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FixedVoltage;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/FixedVoltage_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/FixedVoltage_N.mo
new file mode 100644
index 0000000000..c1d9a46252
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/FixedVoltage_N.mo
@@ -0,0 +1,102 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources;
+model FixedVoltage_N "Fixed voltage source with neutral cable"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.BaseClasses.PartialSource_N;
+  parameter Modelica.Units.SI.Frequency f(start=60) "Frequency of the source";
+  parameter Modelica.Units.SI.Voltage V(start=480) "RMS voltage of the source";
+  parameter Modelica.Units.SI.Angle phiSou=0 "Phase shift of the source";
+  parameter Boolean potentialReference = true
+    "Serve as potential root for the reference angle theta"
+     annotation (Evaluate=true, Dialog(group="Reference Parameters"));
+  parameter Boolean definiteReference = false
+    "Serve as definite root for the reference angle theta"
+     annotation (Evaluate=true, Dialog(group="Reference Parameters"));
+  constant Modelica.Units.SI.Angle angle120=2*Modelica.Constants.pi/3
+    "Phase shift between the phase voltages";
+  OnePhase.Sources.FixedVoltage vPhase[3](
+    each f=f,
+    phiSou={phiSou, phiSou + angle120, phiSou + 2*angle120},
+    potentialReference={potentialReference, potentialReference, potentialReference},
+    definiteReference={definiteReference, false, false},
+    each V=V/sqrt(3)) "Voltage sources on the three-phase"
+             annotation (Placement(transformation(extent={{-30,-10},{-10,10}})));
+equation
+
+  connect(vPhase[1].terminal, terminal.phase[1]) annotation (Line(
+      points={{-10,0},{20,0},{20,0.05},{100.05,0.05}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(vPhase[2].terminal, terminal.phase[2]) annotation (Line(
+      points={{-10,0},{10,0},{10,0.05},{100.05,0.05}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(vPhase[3].terminal, terminal.phase[3]) annotation (Line(
+      points={{-10,0},{45,0},{45,0.05},{100.05,0.05}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="sou",
+ Icon(graphics={
+        Ellipse(
+          extent={{-60,60},{60,-60}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid), Line(
+          points={{-34,0},{-14,40},{6,0},{26,-40},{46,0}},
+          color={120,120,120},
+          smooth=Smooth.Bezier),          Line(
+          points={{-44,0},{-24,40},{-4,0},{16,-40},{36,0}},
+          color={0,0,0},
+          smooth=Smooth.Bezier),          Line(
+          points={{-24,0},{-4,40},{16,0},{36,-40},{56,0}},
+          color={215,215,215},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{60,0},{90,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Text(
+          extent={{-120,100},{120,60}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-120,-60},{120,-100}},
+          textColor={0,0,0},
+          textString="V = %V")}),
+    Documentation(info="<html>
+<p>
+This is a constant voltage source, specifying the complex
+voltage by the RMS voltage and the phase shift. The model has also
+the neutral cable, connected to a ground reference by default.
+</p>
+<p>
+The parameters <code>potentialReference</code> and <code>definiteReference</code>
+are used to define if the source model should be selected as source for
+the reference angles <code>theta</code> or not.
+More information about overdetermined connectors can be found
+in <a href=\"#Olsson2008\">Olsson Et Al. (2008)</a>.
+</p>
+
+<h4>References</h4>
+<p>
+<a name=\"Olsson2008\"/>
+Hans Olsson, Martin Otter, Sven Erik Mattson and Hilding Elmqvist.<br/>
+<a href=\"http://elib-v3.dlr.de/55892/1/otter2008-modelica-balanced-models.pdf\">
+Balanced Models in Modelica 3.0 for Increased Model Quality</a>.<br/>
+Proc. of the 7th Modelica Conference, Bielefeld, Germany, March 2008.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Updated documentation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/427\">issue 427</a>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FixedVoltage_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Grid.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Grid.mo
new file mode 100644
index 0000000000..9f326119c8
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Grid.mo
@@ -0,0 +1,160 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources;
+model Grid "Electrical grid"
+  parameter Modelica.Units.SI.Frequency f(start=60) "Frequency of the source";
+  parameter Modelica.Units.SI.Voltage V(start=480) "RMS voltage of the source";
+  parameter Modelica.Units.SI.Angle phiSou=0 "Phase shift of the source";
+  AixLib.Electrical.AC.Interfaces.PowerOutput P[3]
+    "Power consumed from grid if positive, or fed to grid if negative"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal_p terminal
+    "Connector for three-phase unbalanced systems"            annotation (Placement(transformation(extent={{-10,
+            -110},{10,-90}}), iconTransformation(extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,-100})));
+
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.FixedVoltage sou(
+    potentialReference=true,
+    definiteReference=true,
+    f=f,
+    V=V,
+    phiSou=phiSou) "Voltage source"
+     annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        origin={10,0})));
+equation
+  for i in 1:3 loop
+    P[i].real = -sou.vPhase[i].S[1];
+    P[i].apparent = sqrt(sou.vPhase[i].S[2]^2 + sou.vPhase[i].S[1]^2);
+    P[i].phi = sou.vPhase[i].phi;
+    P[i].cosPhi = cos(sou.vPhase[i].phi);
+  end for;
+  connect(sou.terminal, terminal) annotation (Line(
+      points={{-4.44089e-16,6.66134e-16},{-4.44089e-16,-100},{4.44089e-16,-100}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="gri",
+    Documentation(info="<html>
+<p>
+Model that can be used to represent the electrical grid supply.
+</p>
+<p>
+The model has an output connector named <code>P[n]</code> with <code>n = 3</code> that
+contains information about the power supplied by the grid to the network.
+The convention is that <code>P[i].real</code> is positive if real power is
+consumed from the grid, and negative if it is fed into the grid.
+The connector has size equal to three because each element
+of the vector refers to a single phase.
+</p>
+<p>
+The parameter <code>V</code> is the root means square of the voltage.
+In US, a typical value <i>480</i> Volts.
+</p>
+</html>",
+ revisions="<html>
+<ul>
+<li>
+August 31, 2016, by Michael Wetter:<br/>
+Corrected sign error in documentation string of variable <code>P</code>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-120,130},{120,100}},
+          textColor={0,120,120},
+          textString="%name"),
+        Line(
+          points={{-60,-32},{-60,-72}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-74,-32},{-44,-32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-72,-38},{-48,-28},{-28,-16},{-16,-2},{-12,14}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-46,-38},{-22,-28},{-2,-16},{10,-2},{14,14}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-72,-32},{-72,-38}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-46,-32},{-46,-38}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-14,20},{16,20}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{0,20},{0,-20}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-12,20},{-12,14}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{14,20},{14,14}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{14,14},{38,24},{58,36},{70,50},{74,66}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-12,14},{12,24},{32,36},{44,50},{48,66}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{60,72},{60,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{46,72},{76,72}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{48,72},{48,66}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{74,72},{74,66}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-100,-76},{-96,-74},{-88,-68},{-76,-54},{-72,-38}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-100,-88},{-82,-80},{-62,-68},{-50,-54},{-46,-38}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{48,68},{72,78},{92,90},{98,94},{100,96}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{74,68},{84,72},{100,82}},
+          color={175,175,175},
+          smooth=Smooth.Bezier)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Grid;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Grid_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Grid_N.mo
new file mode 100644
index 0000000000..bb48230dd5
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/Grid_N.mo
@@ -0,0 +1,161 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources;
+model Grid_N "Electrical grid with neutral cable"
+  parameter Modelica.Units.SI.Frequency f(start=60) "Frequency of the source";
+  parameter Modelica.Units.SI.Voltage V(start=480) "RMS voltage of the source";
+  parameter Modelica.Units.SI.Angle phiSou=0 "Phase shift of the source";
+  AixLib.Electrical.AC.Interfaces.PowerOutput P[3]
+    "Power consumed from grid if positive, or fed to grid if negative"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Terminal4_p terminal
+    "Connector for three-phase unbalanced systems"
+                                                  annotation (Placement(transformation(extent={{-10,
+            -110},{10,-90}}), iconTransformation(extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,-100})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.FixedVoltage_N sou(
+    potentialReference=true,
+    definiteReference=true,
+    f=f,
+    V=V,
+    phiSou=phiSou) "Voltage source"
+     annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        origin={10,0})));
+equation
+  for i in 1:3 loop
+    P[i].real = -sou.vPhase[i].S[1];
+    P[i].apparent = sqrt(sou.vPhase[i].S[2]^2 + sou.vPhase[i].S[1]^2);
+    P[i].phi = sou.vPhase[i].phi;
+    P[i].cosPhi = cos(sou.vPhase[i].phi);
+  end for;
+  connect(sou.terminal, terminal) annotation (Line(
+      points={{-4.44089e-16,6.66134e-16},{-4.44089e-16,-100},{4.44089e-16,-100}},
+      color={127,0,127},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="gri",
+    Documentation(info="<html>
+<p>
+Model that can be used to represent the electrical grid supply with a neutral cable connection.
+The neutral cable is connected to the ground.
+</p>
+<p>
+The model has an output connector named <code>P[n]</code> with <code>n = 3</code> that
+contains information about the power supplied by the grid to the network.
+The convention is that <code>P[i].real</code> is positive if real power is
+consumed from the grid, and negative if it is fed into the grid.
+The connector has size equal to three because each element
+of the vector refers to a single phase.
+</p>
+<p>
+The parameter <code>V</code> is the root means square of the voltage.
+In US, a typical value <i>480</i> Volts.
+</p>
+</html>",
+ revisions="<html>
+<ul>
+<li>
+August 31, 2016, by Michael Wetter:<br/>
+Corrected sign error in documentation string of variable <code>P</code>.
+</li>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-120,130},{120,100}},
+          textColor={0,120,120},
+          textString="%name"),
+        Line(
+          points={{-60,-32},{-60,-72}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-74,-32},{-44,-32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-72,-38},{-48,-28},{-28,-16},{-16,-2},{-12,14}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-46,-38},{-22,-28},{-2,-16},{10,-2},{14,14}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-72,-32},{-72,-38}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-46,-32},{-46,-38}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-14,20},{16,20}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{0,20},{0,-20}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-12,20},{-12,14}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{14,20},{14,14}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{14,14},{38,24},{58,36},{70,50},{74,66}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-12,14},{12,24},{32,36},{44,50},{48,66}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{60,72},{60,32}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{46,72},{76,72}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{48,72},{48,66}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{74,72},{74,66}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-100,-76},{-96,-74},{-88,-68},{-76,-54},{-72,-38}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-100,-88},{-82,-80},{-62,-68},{-50,-54},{-46,-38}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{48,68},{72,78},{92,90},{98,94},{100,96}},
+          color={175,175,175},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{74,68},{84,72},{100,82}},
+          color={175,175,175},
+          smooth=Smooth.Bezier)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Grid_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/WindTurbine.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/WindTurbine.mo
new file mode 100644
index 0000000000..ac1e8c8372
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/WindTurbine.mo
@@ -0,0 +1,28 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources;
+model WindTurbine "Simple wind turbine source without neutral cable"
+  extends BaseClasses.UnbalancedWindTurbine(
+  redeclare AixLib.Electrical.AC.OnePhase.Sources.WindTurbine wt_phase1,
+  redeclare AixLib.Electrical.AC.OnePhase.Sources.WindTurbine wt_phase2,
+  redeclare AixLib.Electrical.AC.OnePhase.Sources.WindTurbine wt_phase3);
+  annotation (
+  defaultComponentName="winTur",
+ Documentation(revisions="<html>
+<ul>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Simple wind turbine model for three-phase unbalanced systems
+without neutral cable connection.
+</p>
+<p>
+For more information, see
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Sources.WindTurbine\">
+AixLib.Electrical.AC.OnePhase.Sources.WindTurbine</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WindTurbine;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/WindTurbine_N.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/WindTurbine_N.mo
new file mode 100644
index 0000000000..93cf44ef8a
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/WindTurbine_N.mo
@@ -0,0 +1,28 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources;
+model WindTurbine_N "Simple wind turbine source with neutral cable"
+  extends BaseClasses.UnbalancedWindTurbine_N(
+  redeclare AixLib.Electrical.AC.OnePhase.Sources.WindTurbine wt_phase1,
+  redeclare AixLib.Electrical.AC.OnePhase.Sources.WindTurbine wt_phase2,
+  redeclare AixLib.Electrical.AC.OnePhase.Sources.WindTurbine wt_phase3);
+  annotation (
+  defaultComponentName="winTur",
+ Documentation(revisions="<html>
+<ul>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Simple wind turbine model for three-phase unbalanced systems
+with neutral cable connection.
+</p>
+<p>
+For more information, see
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Sources.WindTurbine\">
+AixLib.Electrical.AC.OnePhase.Sources.WindTurbine</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WindTurbine_N;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/package.mo
new file mode 100644
index 0000000000..2478d12244
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced;
+package Sources "Package with sources model for three-phase unbalanced AC systems"
+  extends Modelica.Icons.SourcesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains models that represent different types of three
+phases unbalanced AC sources.
+</p>
+</html>"));
+end Sources;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/package.order
new file mode 100644
index 0000000000..abf070be7a
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Sources/package.order
@@ -0,0 +1,8 @@
+FixedVoltage
+FixedVoltage_N
+Grid
+Grid_N
+WindTurbine
+WindTurbine_N
+Examples
+BaseClasses
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DD.mo
new file mode 100644
index 0000000000..fcb931653f
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DD.mo
@@ -0,0 +1,108 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown;
+model DD
+  "IEEE 4 node test feeder model with balanced load and D - D connection (step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=false,
+    final line2_use_Z_y=false,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=4.16e3,
+    final VARbase=6000e3,
+    final V2_ref={12339,12349,12321},
+    final V3_ref={3911,3914,3905},
+    final V4_ref={3442,3497,3384},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{29.7,-90.4,149.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{26.5,-93.6,146.4},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{22.3,-99.4,140.7},
+    loadRL(use_pf_in=false, loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_delta));
+  Modelica.Blocks.Sources.Constant load(k=-1800e3)
+    annotation (Placement(transformation(extent={{54,62},{74,82}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerDD
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+equation
+  connect(load.y, loadRL.Pow1) annotation (Line(
+      points={{75,72},{90,72},{90,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow2) annotation (Line(
+      points={{75,72},{90,72},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow3) annotation (Line(
+      points={{75,72},{90,72},{90,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DD.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html><ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on each phase <i>P<sub>1,2,3</sub> = 1800 kW</i></li>
+  <li>power factor on each phase <i>cos&phi;<sub>1,2,3</sub> = 0.9</i></li>
+  </ul>
+</li>
+<li>voltage step-down transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 4.16kV</i>),</li>
+<li>D-D transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DY.mo
new file mode 100644
index 0000000000..5d1ee87bb8
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DY.mo
@@ -0,0 +1,117 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown;
+model DY
+  "IEEE 4 node test feeder model with balanced load and D - Y connection (step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=false,
+    final line2_use_Z_y=true,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=4.16e3,
+    final VARbase=6000e3,
+    final V2_ref={12340,12349,12318},
+    final V3_ref={2249,2263,2259},
+    final V4_ref={1920,2054,1986},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{29.7,-90.4,149.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{-33.7,-153.4,86.4},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{-39.1,-158.3,80.9},
+    loadRL(use_pf_in=false,
+    load1(v(start={1500, 1200}))));
+  Modelica.Blocks.Sources.Constant load(k=-1800e3)
+    annotation (Placement(transformation(extent={{54,62},{74,82}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownDY
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+equation
+  connect(load.y, loadRL.Pow1) annotation (Line(
+      points={{75,72},{90,72},{90,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow2) annotation (Line(
+      points={{75,72},{90,72},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow3) annotation (Line(
+      points={{75,72},{90,72},{90,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DY.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html><ul>
+<li>
+April 7, 2021, by Michael Wetter:<br/>
+Set start values
+<code>loadRL(load1(v(start = {1500, 1200})))</code>
+as the model seems to have more than one solution.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2432\">#2432</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on each phase <i>P<sub>1,2,3</sub> = 1800 kW</i></li>
+  <li>power factor on each phase <i>cos&phi;<sub>1,2,3</sub> = 0.9</i></li>
+  </ul>
+</li>
+<li>voltage step-down transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 4.16kV</i>),</li>
+<li>D-Y transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YD.mo
new file mode 100644
index 0000000000..6cd4a45766
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YD.mo
@@ -0,0 +1,116 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown;
+model YD
+  "IEEE 4 node test feeder model with balanced load and Y - D connection (step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=true,
+    final line2_use_Z_y=false,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=4.16e3,
+    final VARbase=6000e3,
+    final V2_ref={7113,7132,7123},
+    final V3_ref={3906,3915,3909},
+    final V4_ref={3437,3497,3388},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{-0.3,-120.3,119.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{-3.5,-123.6,116.3},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{-7.8,-129.3,110.6},
+    loadRL(use_pf_in=false, loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_delta));
+  Modelica.Blocks.Sources.Constant load(k=-1800e3)
+    annotation (Placement(transformation(extent={{54,62},{74,82}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownYD
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase,
+    conv1(
+      terminal_p(i(start={-477, 327})),
+      V1(start={7000, -400})))
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+equation
+  connect(load.y, loadRL.Pow1) annotation (Line(
+      points={{75,72},{90,72},{90,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow2) annotation (Line(
+      points={{75,72},{90,72},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow3) annotation (Line(
+      points={{75,72},{90,72},{90,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-40,10},{-40,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YD.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+December 22, 2016, by Michael Wetter:<br/>
+Set start values for Dymola 2017FD01.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on each phase <i>P<sub>1,2,3</sub> = 1800 kW</i></li>
+  <li>power factor on each phase <i>cos&phi;<sub>1,2,3</sub> = 0.9</i></li>
+  </ul>
+</li>
+<li>voltage step-down transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 4.16kV</i>),</li>
+<li>Y-D transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end YD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YY.mo
new file mode 100644
index 0000000000..13b3518ade
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YY.mo
@@ -0,0 +1,109 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown;
+model YY
+  "IEEE 4 node test feeder model with balanced load and Y - Y connection (step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=true,
+    final line2_use_Z_y=true,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=4.16e3,
+    final VARbase=6000e3,
+    final V2_ref={7107,7140,7121},
+    final V3_ref={2247,2269,2256},
+    final V4_ref={1918,2061,1981},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{-0.3,-120.3,119.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{-3.7,-123.5,116.4},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{-9.1,-128.3,110.9},
+    loadRL(use_pf_in=false));
+
+  Modelica.Blocks.Sources.Constant load(k=-1800e3)
+    annotation (Placement(transformation(extent={{54,62},{74,82}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformer
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-28,0},{-8,20}})));
+equation
+  connect(load.y, loadRL.Pow1) annotation (Line(
+      points={{75,72},{90,72},{90,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow2) annotation (Line(
+      points={{75,72},{90,72},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow3) annotation (Line(
+      points={{75,72},{90,72},{90,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-28,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-8,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-28,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YY.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html><ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on each phase <i>P<sub>1,2,3</sub> = 1800 kW</i></li>
+  <li>power factor on each phase <i>cos&phi;<sub>1,2,3</sub> = 0.9</i></li>
+  </ul>
+</li>
+<li>voltage step-down transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 4.16kV</i>),</li>
+<li>Y-Y transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end YY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/package.mo
new file mode 100644
index 0000000000..206123abb3
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder;
+package BalancedStepDown "Package that contains the examples for balanced loads and step down transformer"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the IEEE 4 nodes test validation
+whith balanced load and step down in the voltage of the transformers.
+</p>
+</html>"));
+end BalancedStepDown;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/package.order
new file mode 100644
index 0000000000..99b37afbd9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/package.order
@@ -0,0 +1,4 @@
+DD
+DY
+YD
+YY
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DD.mo
new file mode 100644
index 0000000000..18451362bb
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DD.mo
@@ -0,0 +1,108 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepUp;
+model DD
+  "IEEE 4 node test feeder model with balanced load and D - D connection (step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=false,
+    final line2_use_Z_y=false,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=24.9e3,
+    final VARbase=6000e3,
+    final V2_ref={12361,12372,12348},
+    final V3_ref={23723,23746,23698},
+    final V4_ref={23657,23688,23625},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{29.7,-90.4,149.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{26.7,-93.4,146.6},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{26.6,-93.6,146.5},
+    loadRL(use_pf_in=false, loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_delta));
+  Modelica.Blocks.Sources.Constant load(k=-1800e3)
+    annotation (Placement(transformation(extent={{54,62},{74,82}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerDD
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+equation
+  connect(load.y, loadRL.Pow1) annotation (Line(
+      points={{75,72},{90,72},{90,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow2) annotation (Line(
+      points={{75,72},{90,72},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow3) annotation (Line(
+      points={{75,72},{90,72},{90,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DD.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html><ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on each phase <i>P<sub>1,2,3</sub> = 1800 kW</i></li>
+  <li>power factor on each phase <i>cos&phi;<sub>1,2,3</sub> = 0.9</i></li>
+  </ul>
+</li>
+<li>voltage step-up transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 24.9kV</i>),</li>
+<li>D-D transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DY.mo
new file mode 100644
index 0000000000..206ec3644c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DY.mo
@@ -0,0 +1,117 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepUp;
+model DY
+  "IEEE 4 node test feeder model with balanced load and D - Y connection (step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=false,
+    final line2_use_Z_y=true,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=24.9e3,
+    final VARbase=6000e3,
+    final V2_ref={12361,12372,12348},
+    final V3_ref={13697,13710,13681},
+    final V4_ref={13653,13678,13644},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{29.7,-90.4,149.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{26.7,-93.4,146.6},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{26.6,-93.5,146.5},
+    loadRL(use_pf_in=false));
+  Modelica.Blocks.Sources.Constant load(k=-1800e3)
+    annotation (Placement(transformation(extent={{54,62},{74,82}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpDY
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase,
+    conv1(V1(start={11E3, 6E3})),
+    conv2(V1(start={-700, -11E3})))
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+equation
+  connect(load.y, loadRL.Pow1) annotation (Line(
+      points={{75,72},{90,72},{90,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow2) annotation (Line(
+      points={{75,72},{90,72},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow3) annotation (Line(
+      points={{75,72},{90,72},{90,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DY.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Set start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 9, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on each phase <i>P<sub>1,2,3</sub> = 1800 kW</i></li>
+  <li>power factor on each phase <i>cos&phi;<sub>1,2,3</sub> = 0.9</i></li>
+  </ul>
+</li>
+<li>voltage step-up transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 24.9kV</i>),</li>
+<li>D-Y transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YD.mo
new file mode 100644
index 0000000000..21802fbe2e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YD.mo
@@ -0,0 +1,127 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepUp;
+model YD
+  "IEEE 4 node test feeder model with balanced load and Y - D connection (step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=true,
+    final line2_use_Z_y=false,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=24.9e3,
+    final VARbase=6000e3,
+    final V2_ref={7128,7145,7137},
+    final V3_ref={23746,23722,23698},
+    final V4_ref={23680,23663,23625},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{-0.3,-120.3,119.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{56.7,-63.4,176.7},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{56.6,-63.6,176.5},
+    loadRL(use_pf_in=false,
+           loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_delta,
+           load1(v(start = {13000, 20000}))));
+  Modelica.Blocks.Sources.Constant load(k=-1800e3)
+    annotation (Placement(transformation(extent={{54,62},{74,82}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpYD
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+equation
+  connect(load.y, loadRL.Pow1) annotation (Line(
+      points={{75,72},{90,72},{90,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow2) annotation (Line(
+      points={{75,72},{90,72},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow3) annotation (Line(
+      points={{75,72},{90,72},{90,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YD.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+April 7, 2021, by Michael Wetter:<br/>
+Set better start values
+<code>loadRL(load1(v(start = {13000, 20000})))</code>
+because for one component, the start value is far from a solution
+and if specified, Dymola 2022 beta3 fails to initialize the model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2432\">#2432</a>.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Set start value for <code>loadRL(load1(v(each start = 15000)))</code> which
+is needed for Dymola 2017 to find the correct solution.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on each phase <i>P<sub>1,2,3</sub> = 1800 kW</i></li>
+  <li>power factor on each phase <i>cos&phi;<sub>1,2,3</sub> = 0.9</i></li>
+  </ul>
+</li>
+<li>voltage step-up transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 24.9kV</i>),</li>
+<li>Y-D transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end YD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YY.mo
new file mode 100644
index 0000000000..6535496eb3
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YY.mo
@@ -0,0 +1,108 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepUp;
+model YY
+  "IEEE 4 node test feeder model with balanced load and Y - Y connection (step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=true,
+    final line2_use_Z_y=true,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=24.9e3,
+    final VARbase=6000e3,
+    final V2_ref={7126,7145,7137},
+    final V3_ref={13675,13715,13698},
+    final V4_ref={13631,13682,13661},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{-0.3,-120.4,119.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{-3.3,-123.4,116.6},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{-3.5,-123.5,116.5},
+    loadRL(use_pf_in=false));
+  Modelica.Blocks.Sources.Constant load(k=-1800e3)
+    annotation (Placement(transformation(extent={{54,62},{74,82}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformer
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+equation
+  connect(load.y, loadRL.Pow1) annotation (Line(
+      points={{75,72},{90,72},{90,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow2) annotation (Line(
+      points={{75,72},{90,72},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load.y, loadRL.Pow3) annotation (Line(
+      points={{75,72},{90,72},{90,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, source.terminal) annotation (Line(
+      points={{-74,29},{-74,30},{-74,30},{-74,10},{-74,10},{-78,10},{-78,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YY.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html><ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on each phase <i>P<sub>1,2,3</sub> = 1800 kW</i></li>
+  <li>power factor on each phase <i>cos&phi;<sub>1,2,3</sub> = 0.9</i></li>
+  </ul>
+</li>
+<li>voltage step-up transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 24.9kV</i>),</li>
+<li>Y-Y transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end YY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/package.mo
new file mode 100644
index 0000000000..1b63a1ac5e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder;
+package BalancedStepUp "Package that contains the examples for balanced loads and step up transformer"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the IEEE 4 nodes test validation
+whith balanced load and step up in the voltage of the transformers.
+</p>
+</html>"));
+end BalancedStepUp;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/package.order
new file mode 100644
index 0000000000..99b37afbd9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/package.order
@@ -0,0 +1,4 @@
+DD
+DY
+YD
+YY
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/IEEE4.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/IEEE4.mo
new file mode 100644
index 0000000000..6407ac7d93
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/IEEE4.mo
@@ -0,0 +1,257 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses;
+partial model IEEE4 "Base model of the IEEE 4 nodes test feeder"
+  extends Modelica.Icons.Example;
+  parameter Modelica.Units.SI.Voltage VLL_side1=12.47e3
+    "Voltage line to line side 1";
+  parameter Modelica.Units.SI.Voltage VLL_side2=4.16e3
+    "Voltage line to line side 2";
+
+  parameter Modelica.Units.SI.ApparentPower VARbase=6000e3
+    "Base VA power of the transformer";
+
+  parameter Boolean line1_use_Z_y = true
+    "Choose between Zy or Zd impedance matrix for line 1";
+  parameter Boolean line2_use_Z_y = true
+    "Choose between Zy or Zd impedance matrix for line 2";
+
+  parameter Modelica.Units.SI.Voltage V2_ref[3]={7107,7140,7121}
+    "Reference RMS voltage node 2 - IEEE results";
+  parameter Modelica.Units.SI.Voltage V3_ref[3]={2247,2269,2256}
+    "Reference RMS voltage node 3 - IEEE results";
+  parameter Modelica.Units.SI.Voltage V4_ref[3]={1918,2061,1981}
+    "Reference RMS voltage node 4 - IEEE results";
+  parameter Modelica.Units.SI.Angle Theta2_ref[3](each displayUnit="deg") = {-0.3,
+    -120.3,119.6} "Reference voltage phase angle node 2 - IEEE results";
+  parameter Modelica.Units.SI.Angle Theta3_ref[3](each displayUnit="deg") = {-3.7,
+    -123.5,116.4} "Reference voltage phase angle node 3 - IEEE results";
+  parameter Modelica.Units.SI.Angle Theta4_ref[3](each displayUnit="deg") = {-9.1,
+    -128.3,110.9} "Reference voltage phase angle node 4 - IEEE results";
+  Modelica.Units.SI.Voltage err_V2[3]=node2.V - V2_ref
+    "Error on voltage at node 2";
+  Modelica.Units.SI.Voltage err_V3[3]=node3.V - V3_ref
+    "Error on voltage at node 3";
+  Modelica.Units.SI.Voltage err_V4[3]=node4.V - V4_ref
+    "Error on voltage at node 4";
+  Modelica.Units.SI.Angle err_Theta2[3](each displayUnit="deg") = node2.theta
+     - Theta2_ref "Error on voltage at node 2";
+  Modelica.Units.SI.Angle err_Theta3[3](each displayUnit="deg") = node3.theta
+     - Theta3_ref "Error on voltage at node 3";
+  Modelica.Units.SI.Angle err_Theta4[3](each displayUnit="deg") = node4.theta
+     - Theta4_ref "Error on voltage at node 4";
+  Real err_V2_percent[3] = 100*{err_V2[i]/V2_ref[i] for i in 1:3}
+    "Error in RMS voltage at node 2 -- percent";
+  Real err_V3_percent[3] = 100*{err_V3[i]/V3_ref[i] for i in 1:3}
+    "Error in RMS voltage at node 3 -- percent";
+  Real err_V4_percent[3] = 100*{err_V4[i]/V4_ref[i] for i in 1:3}
+    "Error in RMS voltage at node 4 -- percent";
+  Real err_Theta2_percent[3] = 100*{err_Theta2[i]/Theta2_ref[i] for i in 1:3}
+    "Error in voltage phase angle at node 2 -- percent";
+  Real err_Theta3_percent[3] = 100*{err_Theta3[i]/Theta3_ref[i] for i in 1:3}
+    "Error in voltage phase angle at node 3 -- percent";
+  Real err_Theta4_percent[3] = 100*{err_Theta4[i]/Theta4_ref[i] for i in 1:3}
+    "Error in voltage phase angle at node 4 -- percent";
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.FixedVoltage source(
+    f=60,
+    V=VLL_side1) "Voltage source" annotation (Placement(transformation(extent={{-98,0},{-78,20}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortMatrixRL line1(
+    Z11=L1*(if line1_use_Z_y then Z11_y else Z11_d),
+    Z12=L1*(if line1_use_Z_y then Z12_y else Z12_d),
+    Z13=L1*(if line1_use_Z_y then Z13_y else Z13_d),
+    Z22=L1*(if line1_use_Z_y then Z22_y else Z22_d),
+    Z23=L1*(if line1_use_Z_y then Z23_y else Z23_d),
+    Z33=L1*(if line1_use_Z_y then Z33_y else Z33_d),
+    V_nominal=VLL_side1) "Line at primary side"
+    annotation (Placement(transformation(extent={{-68,0},{-48,20}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.TwoPortMatrixRL line2(
+    Z11=L2*(if line2_use_Z_y then Z11_y else Z11_d),
+    Z12=L2*(if line2_use_Z_y then Z12_y else Z12_d),
+    Z13=L2*(if line2_use_Z_y then Z13_y else Z13_d),
+    Z22=L2*(if line2_use_Z_y then Z22_y else Z22_d),
+    Z23=L2*(if line2_use_Z_y then Z23_y else Z23_d),
+    Z33=L2*(if line2_use_Z_y then Z33_y else Z33_d),
+    V_nominal=VLL_side2) "Line at secondary side"
+    annotation (Placement(transformation(extent={{12,0},{32,20}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Inductive loadRL(
+    pf=0.9,
+    V_nominal=VLL_side2,
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    use_pf_in=true) "Load"
+    annotation (Placement(transformation(extent={{54,0},{74,20}})));
+  replaceable
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.BaseClasses.GeneralizedProbe
+    node1(perUnit=false, V_nominal=VLL_side1) "Probe at source"
+    annotation (Placement(transformation(extent={{-84,28},{-64,48}})));
+  replaceable
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.BaseClasses.GeneralizedProbe
+    node2(perUnit=false, V_nominal=VLL_side1)
+    "Probe at the primary side of the transformer"
+    annotation (Placement(transformation(extent={{-52,28},{-32,48}})));
+  replaceable
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.BaseClasses.GeneralizedProbe
+    node3(perUnit=false, V_nominal=VLL_side2)
+    "Probe at the secondary side of the transformer"
+              annotation (Placement(transformation(extent={{-4,28},{16,48}})));
+  replaceable
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.BaseClasses.GeneralizedProbe
+    node4(perUnit=false, V_nominal=VLL_side2) "Probe at the load"
+              annotation (Placement(transformation(extent={{28,28},{48,48}})));
+
+protected
+  parameter Real L1 = 2000*(1.0/5280.0) "Length line 1 in miles";
+  parameter Real L2 = 2500*(1.0/5280.0) "Length line 2 in miles";
+
+  parameter Modelica.Units.SI.Impedance Z11_d[2]={0.4013,1.4133}
+    "Element [1,1] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z12_d[2]={0.0953,0.8515}
+    "Element [1,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z13_d[2]={0.0953,0.7266}
+    "Element [1,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z22_d[2]={0.4013,1.4133}
+    "Element [2,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z23_d[2]={0.0953,0.7802}
+    "Element [2,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z33_d[2]={0.4013,1.4133}
+    "Element [3,3] of impedance matrix";
+
+  parameter Modelica.Units.SI.Impedance Z11_y[2]={0.4576,1.078}
+    "Element [1,1] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z12_y[2]={0.1559,0.5017}
+    "Element [1,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z13_y[2]={0.1535,0.3849}
+    "Element [1,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z22_y[2]={0.4666,1.0482}
+    "Element [2,2] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z23_y[2]={0.158,0.4236}
+    "Element [2,3] of impedance matrix";
+  parameter Modelica.Units.SI.Impedance Z33_y[2]={0.4615,1.0651}
+    "Element [3,3] of impedance matrix";
+equation
+  connect(source.terminal, line1.terminal_n) annotation (Line(
+      points={{-78,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(line2.terminal_p, loadRL.terminal) annotation (Line(
+      points={{32,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation ( Documentation(revisions="<html>
+<ul>
+<li>
+October 1, 2015, by Michael Wetter:<br/>
+Removed <code>loadRL.P_nominal</code> as the power is an input and
+<code>P_nominal</code> is disabled in this configuration.
+</li>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a partial model that is extended by all the other validation test cases.
+This model defined replaceable probes and transformer so they can be
+easily changed when implementing the different tests.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4nodesFeeder/IEEE_4nodes_schema.png\"/>
+</p>
+
+<p>
+More information can be found in each model that extends this
+one.
+</p>
+
+<h4>Reference results</h4>
+<p>
+The reference results for the tests are saved as parameter of the model and compared to
+the simulated ones. The error between the results (herein called <i>X<sub>model</sub></i>)
+ and the references (herein called  <i>X<sub>ref</sub></i>) are computed in both
+absolute and relative way. Note that  <i>X<sub>model</sub></i> and  <i>X<sub>ref</sub></i>
+can be either voltage amplitudes or phase angles.
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Err<sub>abs</sub> = X<sub>model</sub> - X<sub>ref</sub>
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Err<sub>%</sub> = Err<sub>abs</sub> / X<sub>ref</sub>
+</p>
+
+<p>The variables that store the results of the comparison are listed in the
+table below</p>
+
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+  <th>Variable</th>
+  <th>Description</th>
+  <th>Unit</th>
+</tr>
+<tr>
+  <td><code>err_V2[3]</code></td>
+  <td>Error between simulated voltage at node 2 and reference results</td>
+  <td>[V]</td>
+</tr>
+<tr>
+  <td><code>err_V3[3]</code></td>
+  <td>Error between simulated voltage at node 3 and reference results</td>
+  <td>[V]</td>
+</tr>
+<tr>
+  <td><code>err_V4[3]</code></td>
+  <td>Error between simulated voltage at node 4 and reference results</td>
+  <td>[V]</td>
+</tr>
+<tr>
+  <td><code>err_Theta2[3]</code></td>
+  <td>Error between simulated phase angle at node 2 and reference phase angle</td>
+  <td>[rad], displayed as [deg]</td>
+</tr>
+<tr>
+  <td><code>err_Theta3[3]</code></td>
+  <td>Error between simulated phase angle at node 2 and reference phase angle</td>
+  <td>[rad], displayed as [deg]</td>
+</tr>
+<tr>
+  <td><code>err_Theta4[3]</code></td>
+  <td>Error between simulated phase angle at node 2 and reference phase angle</td>
+  <td>[rad], displayed as [deg]</td>
+</tr>
+<tr>
+  <td><code>err_V2_percent[3]</code></td>
+  <td>Relative error between simulated voltage at node 2 and reference results</td>
+  <td>[%]</td>
+</tr>
+<tr>
+  <td><code>err_V3_percent[3]</code></td>
+  <td>Relative error between simulated voltage at node 3 and reference results</td>
+  <td>[%]</td>
+</tr>
+<tr>
+  <td><code>err_V4_percent[3]</code></td>
+  <td>Relative error between simulated voltage at node 4 and reference results</td>
+  <td>[%]</td>
+</tr>
+<tr>
+  <td><code>err_Theta2_percent[3]</code></td>
+  <td>Relative error between simulated phase angle at node 2 and reference phase angle</td>
+  <td>[%]</td>
+</tr>
+<tr>
+  <td><code>err_Theta3_percent[3]</code></td>
+  <td>Relative error between simulated phase angle at node 2 and reference phase angle</td>
+  <td>[%]</td>
+</tr>
+<tr>
+  <td><code>err_Theta4_percent[3]</code></td>
+  <td>Relative error between simulated phase angle at node 2 and reference phase angle</td>
+  <td>[%]</td>
+</tr>
+</table>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end IEEE4;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/package.mo
new file mode 100644
index 0000000000..2b82992992
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder;
+package BaseClasses "This package contains the base classes used by the IEEE 4 nodes test feeder"
+extends Modelica.Icons.BasesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains base classes used by the models that are part of the package
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/package.order
new file mode 100644
index 0000000000..39abb5aee9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BaseClasses/package.order
@@ -0,0 +1 @@
+IEEE4
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DD.mo
new file mode 100644
index 0000000000..71a85b345d
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DD.mo
@@ -0,0 +1,133 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepDown;
+model DD
+  "IEEE 4 node test feeder model with unbalanced load and D - D connection (step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=false,
+    final line2_use_Z_y=false,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=4.16e3,
+    final VARbase=6000e3,
+    final V2_ref={12341,12370,12302},
+    final V3_ref={3902,3972,3871},
+    final V4_ref={3431,3647,3294},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{29.8,-90.5,149.5},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{27.2,-93.9,145.7},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{24.3,-100.4,138.6},
+    loadRL(loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_delta,
+        use_pf_in=true));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerDD
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+  Modelica.Blocks.Sources.Constant load3(k=-2375e3)
+    annotation (Placement(transformation(extent={{8,76},{28,96}})));
+  Modelica.Blocks.Sources.Constant load2(k=-1800e3)
+    annotation (Placement(transformation(extent={{34,58},{54,78}})));
+  Modelica.Blocks.Sources.Constant load1(k=-1275e3)
+    annotation (Placement(transformation(extent={{54,30},{74,50}})));
+  Modelica.Blocks.Sources.Constant pf1(k=0.85)
+    annotation (Placement(transformation(extent={{-6,-30},{14,-10}})));
+  Modelica.Blocks.Sources.Constant pf2(k=0.9)
+    annotation (Placement(transformation(extent={{16,-50},{36,-30}})));
+  Modelica.Blocks.Sources.Constant pf3(k=0.95)
+    annotation (Placement(transformation(extent={{38,-70},{58,-50}})));
+equation
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load1.y, loadRL.Pow1) annotation (Line(
+      points={{75,40},{80,40},{80,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load2.y, loadRL.Pow2) annotation (Line(
+      points={{55,68},{84,68},{84,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load3.y, loadRL.Pow3) annotation (Line(
+      points={{29,86},{88,86},{88,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf1.y, loadRL.pf_in_1) annotation (Line(
+      points={{15,-20},{58,-20},{58,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf2.y, loadRL.pf_in_2) annotation (Line(
+      points={{37,-40},{64,-40},{64,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf3.y, loadRL.pf_in_3) annotation (Line(
+      points={{59,-60},{70.2,-60},{70.2,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DD.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html><ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on phases <i>P<sub>1</sub> = 2375 kW</i>,
+  <i>P<sub>2</sub> = 1800 kW</i>, and <i>P<sub>3</sub> = 1275 kW</i></li>
+  <li>power factor on phases <i>cos&phi;<sub>1</sub> = 0.85</i>,
+  <i>cos&phi;<sub>2</sub> = 0.9</i>, and <i>cos&phi;<sub>3</sub> = 0.95</i></li>
+  </ul>
+</li>
+<li>voltage step-down transformer (<i>V<sub>Pri</sub>=12.47 kV</i>
+<i>V<sub>Sec</sub> = 4.16kV</i>),</li>
+<li>D-D transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DY.mo
new file mode 100644
index 0000000000..3f97e551d4
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DY.mo
@@ -0,0 +1,144 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepDown;
+model DY
+  "IEEE 4 node test feeder model with unbalanced load and D - Y connection (step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=false,
+    final line2_use_Z_y=true,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=4.16e3,
+    final VARbase=6000e3,
+    final V2_ref={12350,12314,12333},
+    final V3_ref={2290,2261,2214},
+    final V4_ref={2157,1936,1849},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{29.6,-90.4,149.8},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{-32.4,-153.8,85.2},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{-34.2,-157.0,73.4},
+    loadRL(use_pf_in=true),
+    line2(terminal_p(phase(v(each start=-1)))));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownDY
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+  Modelica.Blocks.Sources.Constant load3(k=-2375e3)
+    annotation (Placement(transformation(extent={{14,76},{34,96}})));
+  Modelica.Blocks.Sources.Constant load2(k=-1800e3)
+    annotation (Placement(transformation(extent={{40,58},{60,78}})));
+  Modelica.Blocks.Sources.Constant pf1(k=0.85)
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Modelica.Blocks.Sources.Constant pf2(k=0.9)
+    annotation (Placement(transformation(extent={{22,-50},{42,-30}})));
+  Modelica.Blocks.Sources.Constant pf3(k=0.95)
+    annotation (Placement(transformation(extent={{44,-70},{64,-50}})));
+  Modelica.Blocks.Sources.Constant load1(k=-1275e3)
+    annotation (Placement(transformation(extent={{60,30},{80,50}})));
+equation
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(pf1.y, loadRL.pf_in_1) annotation (Line(
+      points={{21,-20},{58,-20},{58,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf2.y, loadRL.pf_in_2) annotation (Line(
+      points={{43,-40},{64,-40},{64,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf3.y, loadRL.pf_in_3) annotation (Line(
+      points={{65,-60},{70.2,-60},{70.2,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load2.y, loadRL.Pow2) annotation (Line(
+      points={{61,68},{90,68},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load3.y, loadRL.Pow3) annotation (Line(
+      points={{35,86},{94,86},{94,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load1.y, loadRL.Pow1) annotation (Line(
+      points={{81,40},{86,40},{86,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DY.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+January 12, 2019, by Michael Wetter:<br/>
+Corrected wrong use of <code>each</code>.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Set start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on phases <i>P<sub>1</sub> = 2375 kW</i>,
+  <i>P<sub>2</sub> = 1800 kW</i>, and <i>P<sub>3</sub> = 1275 kW</i></li>
+  <li>power factor on phases <i>cos&phi;<sub>1</sub> = 0.85</i>,
+  <i>cos&phi;<sub>2</sub> = 0.9</i>, and <i>cos&phi;<sub>3</sub> = 0.95</i></li>
+  </ul>
+</li>
+<li>voltage step-down transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 4.16kV</i>),</li>
+<li>D-Y transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YD.mo
new file mode 100644
index 0000000000..2c69f4a35b
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YD.mo
@@ -0,0 +1,142 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepDown;
+model YD
+  "IEEE 4 node test feeder model with unbalanced load and Y - D connection (step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=true,
+    final line2_use_Z_y=false,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=4.16e3,
+    final VARbase=6000e3,
+    final V2_ref={7113,7144,7111},
+    final V3_ref={3896,3972,3875},
+    final V4_ref={3425,3646,3298},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{-0.2,-120.4,119.5},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{-2.8,-123.8,115.7},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{-5.8,-130.3,108.6},
+    loadRL(loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_delta,
+           use_pf_in=true,
+           load1(v(each start = 3000))),
+    line1(i1(each start=200)));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepDownYD
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+  Modelica.Blocks.Sources.Constant load3(k=-2375e3)
+    annotation (Placement(transformation(extent={{14,74},{34,94}})));
+  Modelica.Blocks.Sources.Constant load2(k=-1800e3)
+    annotation (Placement(transformation(extent={{40,56},{60,76}})));
+  Modelica.Blocks.Sources.Constant load1(k=-1275e3)
+    annotation (Placement(transformation(extent={{60,28},{80,48}})));
+  Modelica.Blocks.Sources.Constant pf1(k=0.85)
+    annotation (Placement(transformation(extent={{0,-32},{20,-12}})));
+  Modelica.Blocks.Sources.Constant pf2(k=0.9)
+    annotation (Placement(transformation(extent={{22,-52},{42,-32}})));
+  Modelica.Blocks.Sources.Constant pf3(k=0.95)
+    annotation (Placement(transformation(extent={{44,-72},{64,-52}})));
+equation
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load2.y, loadRL.Pow2) annotation (Line(
+      points={{61,66},{90,66},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load3.y, loadRL.Pow3) annotation (Line(
+      points={{35,84},{94,84},{94,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load1.y, loadRL.Pow1) annotation (Line(
+      points={{81,38},{86,38},{86,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf1.y, loadRL.pf_in_1) annotation (Line(
+      points={{21,-22},{58,-22},{58,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf2.y, loadRL.pf_in_2) annotation (Line(
+      points={{43,-42},{64,-42},{64,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf3.y, loadRL.pf_in_3) annotation (Line(
+      points={{65,-62},{70.2,-62},{70.2,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YD.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Set start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on phases <i>P<sub>1</sub> = 2375 kW</i>,
+  <i>P<sub>2</sub> = 1800 kW</i>, and <i>P<sub>3</sub> = 1275 kW</i></li>
+  <li>power factor on phases <i>cos&phi;<sub>1</sub> = 0.85</i>,
+  <i>cos&phi;<sub>2</sub> = 0.9</i>, and <i>cos&phi;<sub>3</sub> = 0.95</i></li>
+  </ul>
+</li>
+<li>voltage step-down transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 4.16kV</i>),</li>
+<li>Y-D transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end YD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YY.mo
new file mode 100644
index 0000000000..9ab941dfbf
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YY.mo
@@ -0,0 +1,145 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepDown;
+model YY
+  "IEEE 4 node test feeder model with unbalanced load and Y - Y connection (step down)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=true,
+    final line2_use_Z_y=true,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=4.16e3,
+    final VARbase=6000e3,
+    final V2_ref={7164,7110,7082},
+    final V3_ref={2305,2255,2203},
+    final V4_ref={2175,1930,1833},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{-0.1,-120.2,119.3},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{-2.3,-123.6,114.8},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{-4.1,-126.8,102.8},
+    loadRL(use_pf_in=true),
+    line1(i1(start={180, -130}),
+          i2(start={-300, -160}),
+          i3(start={40, 450})),
+    line2(i2(start={-900, -480}),
+          i3(start={130, 1400})));
+
+  Modelica.Blocks.Sources.Constant load1(k=-1275e3)
+    annotation (Placement(transformation(extent={{54,30},{74,50}})));
+  Modelica.Blocks.Sources.Constant load2(k=-1800e3)
+    annotation (Placement(transformation(extent={{28,58},{48,78}})));
+  Modelica.Blocks.Sources.Constant load3(k=-2375e3)
+    annotation (Placement(transformation(extent={{2,74},{22,94}})));
+  Modelica.Blocks.Sources.Constant pf1(k=0.85)
+    annotation (Placement(transformation(extent={{-16,-38},{4,-18}})));
+  Modelica.Blocks.Sources.Constant pf2(k=0.9)
+    annotation (Placement(transformation(extent={{2,-64},{22,-44}})));
+  Modelica.Blocks.Sources.Constant pf3(k=0.95)
+    annotation (Placement(transformation(extent={{24,-88},{44,-68}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformer
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-28,0},{-8,20}})));
+equation
+  connect(load1.y, loadRL.Pow1) annotation (Line(
+      points={{75,40},{82,40},{82,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load2.y, loadRL.Pow2) annotation (Line(
+      points={{49,68},{84,68},{84,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load3.y, loadRL.Pow3) annotation (Line(
+      points={{23,84},{86,84},{86,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf1.y, loadRL.pf_in_1) annotation (Line(
+      points={{5,-28},{58,-28},{58,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf2.y, loadRL.pf_in_2) annotation (Line(
+      points={{23,-54},{64,-54},{64,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf3.y, loadRL.pf_in_3) annotation (Line(
+      points={{45,-78},{70.2,-78},{70.2,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-28,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-8,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-28,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YY.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Set start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on phases <i>P<sub>1</sub> = 2375 kW</i>,
+  <i>P<sub>2</sub> = 1800 kW</i>, and <i>P<sub>3</sub> = 1275 kW</i></li>
+  <li>power factor on phases <i>cos&phi;<sub>1</sub> = 0.85</i>,
+  <i>cos&phi;<sub>2</sub> = 0.9</i>, and <i>cos&phi;<sub>3</sub> = 0.95</i></li>
+  </ul>
+</li>
+<li>voltage step-down transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 4.16kV</i>),</li>
+<li>Y-Y transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end YY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/package.mo
new file mode 100644
index 0000000000..e1a7b14e5e
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder;
+package UnbalancedStepDown "Package that contains the examples for unbalanced loads and step down transformer"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the IEEE 4 nodes test validation
+whith unbalanced load and step down in the voltage of the transformers.
+</p>
+</html>"));
+end UnbalancedStepDown;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/package.order
new file mode 100644
index 0000000000..99b37afbd9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/package.order
@@ -0,0 +1,4 @@
+DD
+DY
+YD
+YY
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DD.mo
new file mode 100644
index 0000000000..d26a41c9ae
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DD.mo
@@ -0,0 +1,133 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp;
+model DD
+  "IEEE 4 node test feeder model with unbalanced load and D - D connection (step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=false,
+    final line2_use_Z_y=false,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=24.9e3,
+    final VARbase=6000e3,
+    final V2_ref={12362,12392,12334},
+    final V3_ref={23675,24060,23573},
+    final V4_ref={23610,24015,23492},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{29.8,-90.4,149.5},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{27.2,-93.6,146.0},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{27.2,-93.7,145.9},
+    loadRL(loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_delta,
+        use_pf_in=true));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerDD
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+  Modelica.Blocks.Sources.Constant load3(k=-2375e3)
+    annotation (Placement(transformation(extent={{8,76},{28,96}})));
+  Modelica.Blocks.Sources.Constant load2(k=-1800e3)
+    annotation (Placement(transformation(extent={{34,58},{54,78}})));
+  Modelica.Blocks.Sources.Constant load1(k=-1275e3)
+    annotation (Placement(transformation(extent={{54,30},{74,50}})));
+  Modelica.Blocks.Sources.Constant pf1(k=0.85)
+    annotation (Placement(transformation(extent={{-6,-30},{14,-10}})));
+  Modelica.Blocks.Sources.Constant pf2(k=0.9)
+    annotation (Placement(transformation(extent={{16,-50},{36,-30}})));
+  Modelica.Blocks.Sources.Constant pf3(k=0.95)
+    annotation (Placement(transformation(extent={{38,-70},{58,-50}})));
+equation
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load1.y, loadRL.Pow1) annotation (Line(
+      points={{75,40},{80,40},{80,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load2.y, loadRL.Pow2) annotation (Line(
+      points={{55,68},{84,68},{84,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load3.y, loadRL.Pow3) annotation (Line(
+      points={{29,86},{88,86},{88,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf1.y, loadRL.pf_in_1) annotation (Line(
+      points={{15,-20},{58,-20},{58,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf2.y, loadRL.pf_in_2) annotation (Line(
+      points={{37,-40},{64,-40},{64,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf3.y, loadRL.pf_in_3) annotation (Line(
+      points={{59,-60},{70.2,-60},{70.2,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(node1.term, source.terminal) annotation (Line(
+      points={{-74,29},{-74,30},{-74,30},{-74,10},{-74,10},{-78,10},{-78,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DD.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html><ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on phases <i>P<sub>1</sub> = 2375 kW</i>,
+  <i>P<sub>2</sub> = 1800 kW</i>, and <i>P<sub>3</sub> = 1275 kW</i></li>
+  <li>power factor on phases <i>cos&phi;<sub>1</sub> = 0.85</i>,
+  <i>cos&phi;<sub>2</sub> = 0.9</i>, and <i>cos&phi;<sub>3</sub> = 0.95</i></li>
+  </ul>
+</li>
+<li>voltage step-up transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 24.9kV</i>),</li>
+<li>D-D transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DY.mo
new file mode 100644
index 0000000000..8f9642b49c
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DY.mo
@@ -0,0 +1,140 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp;
+model DY
+  "IEEE 4 node test feeder model with unbalanced load and D - Y connection (step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=false,
+    final line2_use_Z_y=true,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=24.9e3,
+    final VARbase=6000e3,
+    final V2_ref={12364,12391,12333},
+    final V3_ref={13792,13733,13641},
+    final V4_ref={13768,13684,13600},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{29.8,-90.5,149.6},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{27.7,-93.5,145.4},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{27.7,-93.6,145.2},
+    loadRL(use_pf_in=true));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpDY
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase,
+    conv1(V1(start={10E3, 5.5E3})))
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+  Modelica.Blocks.Sources.Constant load3(k=-2375e3)
+    annotation (Placement(transformation(extent={{14,76},{34,96}})));
+  Modelica.Blocks.Sources.Constant load2(k=-1800e3)
+    annotation (Placement(transformation(extent={{40,58},{60,78}})));
+  Modelica.Blocks.Sources.Constant pf1(k=0.85)
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Modelica.Blocks.Sources.Constant pf2(k=0.9)
+    annotation (Placement(transformation(extent={{22,-50},{42,-30}})));
+  Modelica.Blocks.Sources.Constant pf3(k=0.95)
+    annotation (Placement(transformation(extent={{44,-70},{64,-50}})));
+  Modelica.Blocks.Sources.Constant load1(k=-1275e3)
+    annotation (Placement(transformation(extent={{60,30},{80,50}})));
+equation
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(pf1.y, loadRL.pf_in_1) annotation (Line(
+      points={{21,-20},{58,-20},{58,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf2.y, loadRL.pf_in_2) annotation (Line(
+      points={{43,-40},{64,-40},{64,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf3.y, loadRL.pf_in_3) annotation (Line(
+      points={{65,-60},{70.2,-60},{70.2,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load2.y, loadRL.Pow2) annotation (Line(
+      points={{61,68},{90,68},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load3.y, loadRL.Pow3) annotation (Line(
+      points={{35,86},{94,86},{94,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load1.y, loadRL.Pow1) annotation (Line(
+      points={{81,40},{86,40},{86,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DY.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Set start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 9, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on phases <i>P<sub>1</sub> = 2375 kW</i>,
+  <i>P<sub>2</sub> = 1800 kW</i>, and <i>P<sub>3</sub> = 1275 kW</i></li>
+  <li>power factor on phases <i>cos&phi;<sub>1</sub> = 0.85</i>,
+  <i>cos&phi;<sub>2</sub> = 0.9</i>, and <i>cos&phi;<sub>3</sub> = 0.95</i></li>
+  </ul>
+</li>
+<li>voltage step-up transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 24.9kV</i>),</li>
+<li>D-Y transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YD.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YD.mo
new file mode 100644
index 0000000000..b8adc01aa1
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YD.mo
@@ -0,0 +1,133 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp;
+model YD
+  "IEEE 4 node test feeder model with unbalanced load and Y - D connection (step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=true,
+    final line2_use_Z_y=false,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeDelta
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=24.9e3,
+    final VARbase=6000e3,
+    final V2_ref={7121,7147,7150},
+    final V3_ref={23703,24040,23576},
+    final V4_ref={23637,23995,23496},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{-0.4,-120.3,119.5},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{57.2,-63.6,176.1},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{57.1,-63.8,175.9},
+    loadRL(loadConn=AixLib.Electrical.Types.LoadConnection.wye_to_delta,
+        use_pf_in=true));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformerStepUpYD
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase)
+    annotation (Placement(transformation(extent={{-26,0},{-6,20}})));
+  Modelica.Blocks.Sources.Constant load3(k=-2375e3)
+    annotation (Placement(transformation(extent={{14,76},{34,96}})));
+  Modelica.Blocks.Sources.Constant load2(k=-1800e3)
+    annotation (Placement(transformation(extent={{40,58},{60,78}})));
+  Modelica.Blocks.Sources.Constant load1(k=-1275e3)
+    annotation (Placement(transformation(extent={{60,30},{80,50}})));
+  Modelica.Blocks.Sources.Constant pf1(k=0.85)
+    annotation (Placement(transformation(extent={{0,-30},{20,-10}})));
+  Modelica.Blocks.Sources.Constant pf2(k=0.9)
+    annotation (Placement(transformation(extent={{22,-50},{42,-30}})));
+  Modelica.Blocks.Sources.Constant pf3(k=0.95)
+    annotation (Placement(transformation(extent={{44,-70},{64,-50}})));
+equation
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(load2.y, loadRL.Pow2) annotation (Line(
+      points={{61,68},{90,68},{90,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load3.y, loadRL.Pow3) annotation (Line(
+      points={{35,86},{94,86},{94,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load1.y, loadRL.Pow1) annotation (Line(
+      points={{81,40},{86,40},{86,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf1.y, loadRL.pf_in_1) annotation (Line(
+      points={{21,-20},{58,-20},{58,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf2.y, loadRL.pf_in_2) annotation (Line(
+      points={{43,-40},{64,-40},{64,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf3.y, loadRL.pf_in_3) annotation (Line(
+      points={{65,-60},{70.2,-60},{70.2,-4.44089e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-26,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YD.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html><ul>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on phases <i>P<sub>1</sub> = 2375 kW</i>,
+  <i>P<sub>2</sub> = 1800 kW</i>, and <i>P<sub>3</sub> = 1275 kW</i></li>
+  <li>power factor on phases <i>cos&phi;<sub>1</sub> = 0.85</i>,
+  <i>cos&phi;<sub>2</sub> = 0.9</i>, and <i>cos&phi;<sub>3</sub> = 0.95</i></li>
+  </ul>
+</li>
+<li>voltage step-up transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 24.9kV</i>),</li>
+<li>Y-D transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end YD;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YY.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YY.mo
new file mode 100644
index 0000000000..ece65280ec
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YY.mo
@@ -0,0 +1,141 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp;
+model YY
+  "IEEE 4 node test feeder model with unbalanced load and Y - Y connection (step up)"
+  extends
+    AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BaseClasses.IEEE4(
+    final line1_use_Z_y=true,
+    final line2_use_Z_y=true,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node1,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node2,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node3,
+    redeclare AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.ProbeWye
+      node4,
+    final VLL_side1=12.47e3,
+    final VLL_side2=24.9e3,
+    final VARbase=6000e3,
+    final V2_ref={7161,7120,7128},
+    final V3_ref={13839,13663,13655},
+    final V4_ref={13815,13614,13615},
+    final Theta2_ref=Modelica.Constants.pi/180.0*{-0.1,-120.3,119.3},
+    final Theta3_ref=Modelica.Constants.pi/180.0*{-2.1,-123.3,115.1},
+    final Theta4_ref=Modelica.Constants.pi/180.0*{-2.2,-123.4,114.9},
+    loadRL(use_pf_in=true));
+  Modelica.Blocks.Sources.Constant load2(k=-1800e3)
+    annotation (Placement(transformation(extent={{30,58},{50,78}})));
+  Modelica.Blocks.Sources.Constant load3(k=-2375e3)
+    annotation (Placement(transformation(extent={{4,74},{24,94}})));
+  Modelica.Blocks.Sources.Constant load1(k=-1275e3)
+    annotation (Placement(transformation(extent={{56,30},{76,50}})));
+  Modelica.Blocks.Sources.Constant pf1(k=0.85)
+    annotation (Placement(transformation(extent={{-6,-28},{14,-8}})));
+  Modelica.Blocks.Sources.Constant pf2(k=0.9)
+    annotation (Placement(transformation(extent={{12,-54},{32,-34}})));
+  Modelica.Blocks.Sources.Constant pf3(k=0.95)
+    annotation (Placement(transformation(extent={{34,-78},{54,-58}})));
+  AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.ACACTransformer
+    transformer(
+    VHigh=VLL_side1,
+    VLow=VLL_side2,
+    XoverR=6,
+    Zperc=sqrt(0.01^2 + 0.06^2),
+    VABase=VARbase,
+    conv1(V1(start={6.9E3, -250})),
+    conv2(V1(start={-3.8E3, -5.7E3})))
+    annotation (Placement(transformation(extent={{-28,0},{-8,20}})));
+equation
+  connect(load2.y, loadRL.Pow2) annotation (Line(
+      points={{51,68},{86,68},{86,10},{76,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load3.y, loadRL.Pow3) annotation (Line(
+      points={{25,84},{88,84},{88,2},{76,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(load1.y, loadRL.Pow1) annotation (Line(
+      points={{77,40},{84,40},{84,18},{76,18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf1.y, loadRL.pf_in_1) annotation (Line(
+      points={{15,-18},{58,-18},{58,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf2.y, loadRL.pf_in_2) annotation (Line(
+      points={{33,-44},{64,-44},{64,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pf3.y, loadRL.pf_in_3) annotation (Line(
+      points={{55,-68},{70.2,-68},{70.2,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, transformer.terminal_n) annotation (Line(
+      points={{-48,10},{-28,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(transformer.terminal_p, line2.terminal_n) annotation (Line(
+      points={{-8,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node1.term, line1.terminal_n) annotation (Line(
+      points={{-74,29},{-74,10},{-68,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node2.term, transformer.terminal_n) annotation (Line(
+      points={{-42,29},{-42,10},{-28,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node3.term, line2.terminal_n) annotation (Line(
+      points={{6,29},{6,10},{12,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  connect(node4.term, loadRL.terminal) annotation (Line(
+      points={{38,29},{38,10},{54,10}},
+      color={0,120,120},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0, Tolerance=1e-6),
+  __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YY.mos"
+        "Simulate and plot"),
+ Documentation(revisions="<html>
+<ul>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Set start values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+October 9, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Moved to Examples IEEE package AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.YY
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+IEEE 4 nodes validation test case with the following characteristics
+</p>
+<ul>
+<li>balanced load,
+  <ul>
+  <li>power consumption on phases <i>P<sub>1</sub> = 2375 kW</i>,
+  <i>P<sub>2</sub> = 1800 kW</i>, and <i>P<sub>3</sub> = 1275 kW</i></li>
+  <li>power factor on phases <i>cos&phi;<sub>1</sub> = 0.85</i>,
+  <i>cos&phi;<sub>2</sub> = 0.9</i>, and <i>cos&phi;<sub>3</sub> = 0.95</i></li>
+  </ul>
+</li>
+<li>voltage step-up transformer (<i>V<sub>Pri</sub>=12.47 kV</i>,
+<i>V<sub>Sec</sub> = 24.9kV</i>),</li>
+<li>Y-Y transformer</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end YY;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/package.mo
new file mode 100644
index 0000000000..6484092df9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder;
+package UnbalancedStepUp "Package that contains the examples for unbalanced loads and step up transformer"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the IEEE 4 nodes test validation
+whith unbalanced load and step up in the voltage of the transformers.
+</p>
+</html>"));
+end UnbalancedStepUp;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/package.order
new file mode 100644
index 0000000000..99b37afbd9
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/package.order
@@ -0,0 +1,4 @@
+DD
+DY
+YD
+YY
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/package.mo
new file mode 100644
index 0000000000..4950d3feeb
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/package.mo
@@ -0,0 +1,115 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests;
+package Test4NodesFeeder "This package contains models for the IEEE 4 nodes test feeder"
+extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples that shows the validation of the models
+against the IEEE four-nodes test feeder validation procedure <a href=\"#\"></a>.
+The tests that are part of the validation certify the capability to represent
+transformers of various configurations, full three-phase lines, and unbalanced loads.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4nodesFeeder/IEEE_4nodes_schema.png\"/>
+</p>
+<p>
+The figure shows the structure of the four-nodes network. The voltage
+source is connected to the load through two lines and a transformer. The validation procedure
+consists of mutliple tests in which the type of the load and the type of the transformer vary.
+The test cases that have been successfully implemented using the models of the
+<a href=\"modelica://AixLib.Electrical\">AixLib.Electrical</a>
+package.
+</p>
+<p>
+Each example in this package is part of the validation tests.
+The examples have been grouped into sub-packages depending on the characteristics
+of the validation test. The table below summarizes the examples that are part of this
+package.
+</p>
+
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+  <th>Transformer</th>
+  <th>Load</th>
+</tr>
+<tr>
+  <td>Gr Y - Gr Y Step Up</td>
+  <td>Balanced</td>
+</tr>
+<tr>
+  <td>Gr Y - D Step Up</td>
+  <td>Balanced</td>
+</tr>
+<tr>
+  <td>D - D Step Up</td>
+  <td>Balanced</td>
+</tr>
+<tr>
+  <td>Gr Y - Gr Y Step Down</td>
+  <td>Balanced</td>
+</tr>
+<tr>
+  <td>Gr Y - D Step Down</td>
+  <td>Balanced</td>
+</tr>
+<tr>
+  <td>D - D Step Down</td>
+  <td>Balanced</td>
+</tr>
+<tr>
+  <td>Gr Y - Gr Y Step Up</td>
+  <td>Unbalanced</td>
+</tr>
+<tr>
+  <td>Gr Y - D Step Up</td>
+  <td>Unbalanced</td>
+</tr>
+<tr>
+  <td>D - D Step Up</td>
+  <td>Unbalanced</td>
+</tr>
+<tr>
+  <td>Gr Y - Gr Y Step Down</td>
+  <td>Unbalanced</td>
+</tr>
+<tr>
+  <td>Gr Y - D Step Down</td>
+  <td>Unbalanced</td>
+</tr>
+<tr>
+  <td>D - D Step Down</td>
+  <td>Unbalanced</td>
+</tr>
+</table>
+
+<p>
+For example Gr Y - D Step Up indicates that the transformer has a grounded Y connection at the primary
+side, and a D connection at the secondary side. Step up indicates that the voltage at the secondary
+side is higher than the primary side.
+Each test listed in the table produces results that differ from the reference IEEE values by
+less than 0.05%, which is the threshold defined by IEEE to determine whether results should be accepted or not.
+</p>
+
+<h4>References</h4>
+<p>
+<a name=\"kersting2001radial\"/>
+Kersting, William H.<br/>
+<a href=\"http://ewh.ieee.org/soc/pes/dsacom/testfeeders/\">
+Radial distribution test feeders</a><br/>
+<i>Power Engineering Society Winter Meeting (2) p. 908-912, 2001. IEEE</i><br/>
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+October 8, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end Test4NodesFeeder;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/package.order
new file mode 100644
index 0000000000..9893808af1
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/package.order
@@ -0,0 +1,5 @@
+BalancedStepDown
+BalancedStepUp
+UnbalancedStepDown
+UnbalancedStepUp
+BaseClasses
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/package.mo
new file mode 100644
index 0000000000..c5b24c1889
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation;
+package IEEETests "This package contains models of the IEEE tests for feeders"
+extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples based on IEEE tests.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end IEEETests;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/package.order
new file mode 100644
index 0000000000..74bf159f20
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/package.order
@@ -0,0 +1 @@
+Test4NodesFeeder
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/package.mo
new file mode 100644
index 0000000000..3f0df44e92
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.AC.ThreePhasesUnbalanced;
+package Validation "Package with validation examples and tests for the AC three-phase unbalanced models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the validation of models that can be found in
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesUnbalanced\">
+AixLib.Electrical.AC.ThreePhasesUnbalanced</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end Validation;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/package.order
new file mode 100644
index 0000000000..6d88d1a6cc
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/Validation/package.order
@@ -0,0 +1 @@
+IEEETests
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/package.mo b/AixLib/Electrical/AC/ThreePhasesUnbalanced/package.mo
new file mode 100644
index 0000000000..7d1086e403
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/package.mo
@@ -0,0 +1,45 @@
+within AixLib.Electrical.AC;
+package ThreePhasesUnbalanced "Three phases unbalanced AC systems"
+  extends Modelica.Icons.VariantsPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+Package with models for alternate current (AC) three phase unbalanced systems.<br/>
+The models in this package use the models of the package
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase\">
+AixLib.Electrical.AC.OnePhase</a> to fully describe the three-phase.
+</p>
+<p>
+The models that are part of this package assume by default <i>480</i> V
+as the nominal RMS phase to phase voltage. This default can be changed.
+</p>
+
+<h4>Conventions</h4>
+
+<p>
+In this package the voltage phasors are measured using the convention shown below.
+The phase to phase RMS voltages are by default <i>480</i> V,
+which is equal to <code>sqrt(3)</code> times the
+phase to neutral voltage <i>V</i>, which is <i>277.13</i> V.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/PhaseConvention.png\"/>
+</p>
+
+<p>
+In this package the voltage phasors are measured using the convention shown above.
+The phase to phase RMS voltage equal to 480 V, is equal to <code>sqrt(3)</code> times the
+phase to neutral voltage <i>V</i> that is equal to 277.13 V.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"));
+end ThreePhasesUnbalanced;
diff --git a/AixLib/Electrical/AC/ThreePhasesUnbalanced/package.order b/AixLib/Electrical/AC/ThreePhasesUnbalanced/package.order
new file mode 100644
index 0000000000..43372ff740
--- /dev/null
+++ b/AixLib/Electrical/AC/ThreePhasesUnbalanced/package.order
@@ -0,0 +1,7 @@
+Conversion
+Lines
+Loads
+Sensors
+Sources
+Validation
+Interfaces
diff --git a/AixLib/Electrical/AC/package.mo b/AixLib/Electrical/AC/package.mo
new file mode 100644
index 0000000000..2b5ee683e2
--- /dev/null
+++ b/AixLib/Electrical/AC/package.mo
@@ -0,0 +1,149 @@
+within AixLib.Electrical;
+package AC "Package for electrical systems in which the frequency is modeled as quasi-stationary"
+  extends Modelica.Icons.Package;
+
+package UsersGuide "User's Guide"
+  extends Modelica.Icons.Information;
+
+    annotation (preferredView="info",
+Documentation(info="<html>
+<p>
+The package
+<a href=\"modelica://AixLib.Electrical.AC\">AixLib.Electrical.AC</a>
+models alternate current electrical systems.
+</p>
+
+<h4>Modeling assumptions</h4>
+<p>
+The package <a href=\"modelica://AixLib.Electrical.AC\">AixLib.Electrical.AC</a> contains
+component models for AC systems. The mathematics that describes AC systems is contained in the package
+<a href=\"modelica://AixLib.Electrical.PhaseSystems.OnePhase\">AixLib.Electrical.PhaseSystems.OnePhase</a>,
+in which <code>n = 2</code> and <code>m = 1</code>. The AC models that are part of the library can use two different assumptions.
+</p>
+<p>
+The first assumption is that the frequency is modeled as quasi-stationary, assuming a perfect sine
+wave with no higher harmonics. Voltages and currents are considered as sine waves and just their
+amplitudes and phase shifts are taken into account during the analysis.
+With such an assumption, electric quantities can be represented with a phasor, i.e., a vector
+in the complex plane.
+</p>
+<p>
+The second assumption is the so-called dynamic phasorial representation. The basic idea of the
+dynamic phasorial representation is to account for dynamic variations of the amplitude and
+the angle of the phasors. With such an approach, it is possible to analyze faster dynamics
+without directly representing all the electromagnetic effects and high-order harmonics
+(for more details, see <a href=\"#Stankovic1999\">Stankovic Et Al. 1999</a>, and
+<a href=\"#Stankovic2000\">Stankovic A.M. and Aydin T.</a>).
+</p>
+
+<h4>Phasorial representation</h4>
+<p>
+Both the quasi-stationary and the dynamic phasors represent electric
+quantities such as voltages and currents using phasors.
+The phasors are described by complex numbers that internally are represented as a vector
+with two components. The vectors can be represented in the so called Argand plane where on the x-axis
+are represented Real numbers while on the y-axis imaginary numbers.
+</p>
+<p>
+With such a representation the complex voltages, currents, and powers are represented as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+<span style=\"text-decoration: overline;\">V</span> = V<sub>Re</sub> + j V<sub>Im</sub>,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+<span style=\"text-decoration: overline;\">I</span> = I<sub>Re</sub> + j I<sub>Im</sub>,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+<span style=\"text-decoration: overline;\">S</span> = P + j Q,
+</p>
+
+<p>
+The images below shows how the complex power vector <i><span style=\"text-decoration: overline;\">S</span></i>
+changes depending on the type of load.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/AC/OnePhase/ComplexPower.png\"/>
+</p>
+
+<p>
+where the subscripts indicates a
+</p>
+
+<ul>
+<li><i>R</i> - purely resistive load</li>
+<li><i>L</i> - purely inductive load</li>
+<li><i>C</i> - purely capacitive load</li>
+<li><i>RL</i> - resistive inductive load</li>
+<li><i>RC</i> - resistive capacitive load</li>
+</ul>
+
+<h4>Reference angle for AC systems</h4>
+<p>
+The AC connector has an additional vector that represents the
+reference angle <code>theta[PhaseSystem.m]</code>. The reference angle is used, for example in the
+AC single phase systems to describe the phase angle of the reference voltage.
+This extra information in the connector makes it overdetermined
+because the number of effort variables is higher than the number of flow variables.
+The over-determined connectors are defined and used in such a way that a Modelica tool is able
+to remove the superfluous but consistent equations, arriving at a balanced set of equations based on a
+graph analysis of the connection structure. The models in the library uses constructs specified
+by the Modelica language to handle this situation, as described by <a href=\"#Olsson2008\">Olsson et al. (2008)</a>.
+</p>
+<p>
+The reference angles are usually defined by the sources (e.g., voltage sources or generators) and
+their values need to be propagated to all the components connected to them.
+If more than one generator are connected to the same network, the Modelica tool is able to remove the superfluous equations,
+arriving at a balanced set of equations based on a graph analysis of the connection structure.
+The flags <code>potentialReference</code> and <code>definiteReference</code> are used to help the
+Modelica tool during the selection of the reference angle. If <code>definiteReference = true</code>,
+then the reference angle of the source has to be used as reference, while if
+<code>potentialReference = true</code>, the reference angle is used only if there are no
+definite sources defined.
+</p>
+<p>
+When a model is set as definite source an icon representing a phase angle is placed close to its
+electrical terminal.
+</p>
+
+
+<h4>References</h4>
+<p>
+<a name=\"Stankovic1999\"/>
+A.M. Stankovic, B.C. Lesieutre, T. Aydin; Modeling and analysis of single-pahse
+induction machines with dynamic phasors<br/>
+<a href=\"http://www.ece.neu.edu/faculty/stankovic/Jour_papers/pwrs299im.pdf\">
+<i>IEEE Transactions on Power Systems</i>, 14(1), Feb. 1999, pp. 9-14.</a><br/>
+<a name=\"Stankovic2000\"/>
+A.M. Stankovic, T. Aydin; Analysis of asymmetrical faults in power systems using
+dynamic phasors<br/>
+<a href=\"http://www.ece.neu.edu/faculty/stankovic/Jour_papers/pwrs299im.pdf\">
+<i>IEEE Transactions on Power Systems</i>, 15(3), 2000, pp. 1062-1068 .</a><br/>
+<a name=\"Olsson2008\"/>
+Hans Olsson, Martin Otter, Sven Erik Mattson and Hilding Elmqvist.<br/>
+<a href=\"http://elib-v3.dlr.de/55892/1/otter2008-modelica-balanced-models.pdf\">
+Balanced Models in Modelica 3.0 for Increased Model Quality</a>.<br/>
+Proc. of the 7th Modelica Conference, Bielefeld, Germany, March 2008.<br/>
+</p>
+
+</html>"));
+end UsersGuide;
+
+  annotation (Icon(graphics={ Line(points={{-92,-10},{-80.7,24.2},{-73.5,43.1},{
+              -67.1,56.4},{-61.4,64.6},{-55.8,69.1},{-50.2,69.8},{-44.6,66.6},{-38.9,
+              59.7},{-33.3,49.4},{-26.9,34.1},{-18.83,11.2},{-1.9,-40.8},{5.3,-60.2},
+              {11.7,-74.2},{17.3,-83.1},{23,-88.4},{28.6,-90},{34.2,-87.6},{39.9,
+              -81.5},{45.5,-71.9},{51.9,-57.2},{60,-34.8},{68,-10}}, color={0,0,
+              0})}), Documentation(info="<html>
+<p>
+Package with models for alternating current (AC) systems.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 27, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"));
+end AC;
\ No newline at end of file
diff --git a/AixLib/Electrical/AC/package.order b/AixLib/Electrical/AC/package.order
new file mode 100644
index 0000000000..d9dd383f4c
--- /dev/null
+++ b/AixLib/Electrical/AC/package.order
@@ -0,0 +1,5 @@
+UsersGuide
+OnePhase
+ThreePhasesBalanced
+ThreePhasesUnbalanced
+Interfaces
diff --git a/AixLib/Electrical/BaseClasses/WindTurbine/PartialWindTurbine.mo b/AixLib/Electrical/BaseClasses/WindTurbine/PartialWindTurbine.mo
new file mode 100644
index 0000000000..92c3cd33b7
--- /dev/null
+++ b/AixLib/Electrical/BaseClasses/WindTurbine/PartialWindTurbine.mo
@@ -0,0 +1,189 @@
+within AixLib.Electrical.BaseClasses.WindTurbine;
+model PartialWindTurbine
+  "Partial model of a wind turbine with power output based on table as a function of wind speed"
+  extends AixLib.Electrical.BaseClasses.WindTurbine.PartialWindTurbineBase;
+  replaceable package PhaseSystem =
+      AixLib.Electrical.PhaseSystems.PartialPhaseSystem
+       constrainedby AixLib.Electrical.PhaseSystems.PartialPhaseSystem
+    "Phase system"
+    annotation (choicesAllMatching=true);
+
+  replaceable AixLib.Electrical.Interfaces.Terminal terminal(
+    redeclare package PhaseSystem = PhaseSystem) "Generalized terminal"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+protected
+  Modelica.Blocks.Tables.CombiTable1Ds per(
+    final tableOnFile=tableOnFile,
+    final table=cat(1, cat(1, [0, 0], table),
+                    [vOut+10*Modelica.Constants.eps, 0;
+                     vOut+20*Modelica.Constants.eps, 0]),
+    final tableName=tableName,
+    final fileName=fileName,
+    final columns=2:2,
+    final smoothness=Modelica.Blocks.Types.Smoothness.LinearSegments)
+    "Performance table that maps wind speed to electrical power output"
+    annotation (Placement(transformation(extent={{-30,20},{-10,40}})));
+  Modelica.Blocks.Math.Gain gain(final k=scale)
+    "Gain, used to allow a user to easily scale the power"
+    annotation (Placement(transformation(extent={{2,20},{22,40}})));
+  DC.Sources.BaseClasses.WindCorrection                      cor(
+    final h=h,
+    final hRef=hRef,
+    final n=nWin) "Correction for wind"
+  annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-50,30})));
+initial equation
+  assert(abs(table[1,2]) < Modelica.Constants.eps,
+  "First data point of performance table must be at cut-in wind speed,
+   and be equal to 0 Watts.
+   Received + " + String(table[1,1]) + " m/s with " + String(table[1,2]) + " Watts");
+equation
+  assert(gain.y>=0, "Wind power must be positive");
+  connect(per.y[1],gain. u) annotation (Line(
+      points={{-9,30},{0,30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(vWin,cor. vRef) annotation (Line(
+      points={{1.77636e-15,120},{1.77636e-15,90},{-70,90},{-70,30},{-62.2,30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(cor.vLoc,per. u) annotation (Line(
+      points={{-39,30},{-32,30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(gain.y, P) annotation (Line(
+      points={{23,30},{60,30},{60,60},{110,60}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+        graphics={
+        Rectangle(
+          extent={{-100,102},{100,-98}},
+          pattern=LinePattern.None,
+          fillColor={202,230,255},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{42,46},{46,-52}},
+          fillColor={233,233,233},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{-42,14},{-38,-84}},
+          fillColor={233,233,233},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-44,12},{-26,-40},{-38,16},{-44,12}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-38,12},{8,46},{-42,18},{-38,12}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-42,12},{-90,40},{-38,18},{-42,12}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{40,44},{100,40},{42,50},{40,44}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{-21,-17},{27,17},{-25,-11},{-21,-17}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          origin={29,69},
+          rotation=90,
+          lineColor={0,0,0}),
+        Polygon(
+          points={{24,-14},{-20,22},{26,-8},{24,-14}},
+          smooth=Smooth.None,
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid,
+          origin={32,20},
+          rotation=90,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{-46,20},{-34,8}},
+          lineColor={0,0,0},
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{38,52},{50,40}},
+          lineColor={0,0,0},
+          fillColor={222,222,222},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-42,134},{-20,108}},
+          textColor={0,0,127},
+          textString="v"),
+        Text(
+          extent={{100,100},{122,74}},
+          textColor={0,0,127},
+          textString="P")}),
+    Documentation(info="<html>
+<p>
+Model of a wind turbine whose power is computed as a function of wind-speed as defined in a table.
+</p>
+<p>
+Input to the model is the local wind speed.
+The model requires the specification of a table that maps wind speed in meters per second to generated
+power <i>P<sub>t</sub></i> in Watts.
+The model has a parameter called <code>scale</code> with a default value of one
+that can be used to scale the power generated by the wind turbine.
+The generated electrical power is
+<p align=\"center\" style=\"font-style:italic;\">
+P = P<sub>t</sub> scale
+</p>
+<p>
+For example, the following specification (with default <code>scale=1</code>) of a wind turbine
+</p>
+<pre>
+  WindTurbine_Table tur(
+    table=[3.5, 0;
+           5.5,   100;
+           12, 900;
+           14, 1000;
+           25, 1000]) \"Wind turbine\";
+</pre>
+<p>
+yields the performance shown below. In this example, the cut-in wind speed is
+<i>3.5</i> meters per second,
+and the cut-out wind speed is <i>25</i> meters per second,
+as entered by the first and last entry of the wind speed column.
+Below and above these wind speeds, the generated power is zero.
+</p>
+<p align=\"center\">
+<img alt=\"alt-image\" src=\"modelica://AixLib/Resources/Images/Electrical/DC/Sources/WindTurbine_Table.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 1, 2016, by Michael Wetter:<br/>
+Removed test for equality of <code>Real</code> variables.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-AixLib/issues/493\">issue 493</a>.
+</li>
+<li>
+January 10, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+Models included in the AixLib library. Modified the information section.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialWindTurbine;
diff --git a/AixLib/Electrical/BaseClasses/WindTurbine/PartialWindTurbineBase.mo b/AixLib/Electrical/BaseClasses/WindTurbine/PartialWindTurbineBase.mo
new file mode 100644
index 0000000000..f238642062
--- /dev/null
+++ b/AixLib/Electrical/BaseClasses/WindTurbine/PartialWindTurbineBase.mo
@@ -0,0 +1,60 @@
+within AixLib.Electrical.BaseClasses.WindTurbine;
+partial model PartialWindTurbineBase
+  "Base class for turbine model that contains basic parameters"
+  final parameter Modelica.Units.SI.Velocity vIn=table[1, 1]
+    "Cut-in steady wind speed";
+  final parameter Modelica.Units.SI.Velocity vOut=table[size(table, 1), 1]
+    "Cut-out steady wind speed";
+  parameter Real scale(min=0)=1
+    "Scaling factor, used to allow adjusting the power output without changing the table";
+
+  parameter Real h "Height over ground"
+    annotation (Dialog(group="Wind correction"));
+  parameter Modelica.Units.SI.Height hRef=10
+    "Reference height for wind measurement"
+    annotation (Dialog(group="Wind correction"));
+ parameter Real nWin(min=0) = 0.4
+    "Height exponent for wind profile calculation"
+   annotation (Dialog(group="Wind correction"));
+
+  parameter Boolean tableOnFile=false
+    "true, if table is defined on file or in function usertab";
+  parameter Real table[:,2]=
+          [3.5, 0;
+           5.5, 0.1;
+           12, 0.9;
+           14, 1;
+           25, 1]
+    "Table of generated power (first column is wind speed, second column is power)";
+  parameter String tableName="NoName"
+    "Table name on file or in function usertab (see documentation)";
+  parameter String fileName="NoName" "File where matrix is stored";
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=110)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Evaluate=true, Dialog(group="Nominal conditions"));
+  Modelica.Blocks.Interfaces.RealInput vWin(unit="m/s") "Steady wind speed"
+     annotation (Placement(transformation(
+        origin={0,120},
+        extent={{-20,-20},{20,20}},
+        rotation=270), iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=270,
+        origin={0,120})));
+  Modelica.Blocks.Interfaces.RealOutput P(unit="W") "Generated power"
+    annotation (Placement(transformation(extent={{100,50},{120,70}})));
+  annotation (Documentation(info="<html>
+<p>
+This partial model contains the minimum set of parameters necessary to describe
+a wind turbine.
+The model defines also an output <code>P</code> for the power generated by the wind turbine.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 10, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialWindTurbineBase;
diff --git a/AixLib/Electrical/BaseClasses/WindTurbine/package.mo b/AixLib/Electrical/BaseClasses/WindTurbine/package.mo
new file mode 100644
index 0000000000..26e85e6219
--- /dev/null
+++ b/AixLib/Electrical/BaseClasses/WindTurbine/package.mo
@@ -0,0 +1,16 @@
+within AixLib.Electrical.BaseClasses;
+package WindTurbine
+  annotation(preferredView="info",Documentation(info="<html>
+  <p>
+This package contains base classes that are used model the WindTurbine models.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+June 9, 2023, by Laura Maier:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"));
+end WindTurbine;
diff --git a/AixLib/Electrical/BaseClasses/WindTurbine/package.order b/AixLib/Electrical/BaseClasses/WindTurbine/package.order
new file mode 100644
index 0000000000..0f87db0aa9
--- /dev/null
+++ b/AixLib/Electrical/BaseClasses/WindTurbine/package.order
@@ -0,0 +1,2 @@
+PartialWindTurbine
+PartialWindTurbineBase
diff --git a/AixLib/Electrical/BaseClasses/package.mo b/AixLib/Electrical/BaseClasses/package.mo
new file mode 100644
index 0000000000..84a065128f
--- /dev/null
+++ b/AixLib/Electrical/BaseClasses/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Electrical;
+package BaseClasses "Package with base classes for AixLib.Electrical"
+  extends Modelica.Icons.BasesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains base classes that are used to construct the models in
+<a href=\"modelica://AixLib.Electrical\">AixLib.Electrical</a>.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/BaseClasses/package.order b/AixLib/Electrical/BaseClasses/package.order
new file mode 100644
index 0000000000..cf1431701e
--- /dev/null
+++ b/AixLib/Electrical/BaseClasses/package.order
@@ -0,0 +1 @@
+WindTurbine
diff --git a/AixLib/Electrical/DC/Conversion/DCDCConverter.mo b/AixLib/Electrical/DC/Conversion/DCDCConverter.mo
new file mode 100644
index 0000000000..ff7cafcd21
--- /dev/null
+++ b/AixLib/Electrical/DC/Conversion/DCDCConverter.mo
@@ -0,0 +1,177 @@
+within AixLib.Electrical.DC.Conversion;
+model DCDCConverter "DC DC converter"
+  extends AixLib.Electrical.Interfaces.PartialConversion(
+    redeclare package PhaseSystem_p = PhaseSystems.TwoConductor,
+    redeclare package PhaseSystem_n = PhaseSystems.TwoConductor,
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  parameter Modelica.Units.SI.Voltage VHigh
+    "DC voltage on side 1 of the transformer (primary side)";
+  parameter Modelica.Units.SI.Voltage VLow
+    "DC voltage on side 2 of the transformer (secondary side)";
+  parameter Modelica.Units.SI.Efficiency eta(max=1) "Converter efficiency";
+  parameter Boolean ground_1 = true "Connect side 1 of converter to ground" annotation(Evaluate=true, Dialog(tab = "Ground", group="side 1"));
+  parameter Boolean ground_2 = true "Connect side 2 of converter to ground" annotation(Evaluate=true, Dialog(tab = "Ground", group="side 2"));
+  Modelica.Units.SI.Power LossPower "Loss power";
+protected
+  parameter Real conversionFactor = VLow/VHigh
+    "Ratio of high versus low voltage";
+  Modelica.Units.SI.Current i1;
+  Modelica.Units.SI.Current i2;
+  Modelica.Units.SI.Voltage v1;
+  Modelica.Units.SI.Voltage v2;
+  Modelica.Units.SI.Power P_p "Power at terminal p";
+  Modelica.Units.SI.Power P_n "Power at terminal n";
+equation
+  Connections.potentialRoot(terminal_n.theta);
+  Connections.potentialRoot(terminal_p.theta);
+
+  if not ground_1 then
+    i1 = 0;
+  else
+    v1 = 0;
+  end if;
+  if not ground_2 then
+    i2 = 0;
+  else
+    v2 = 0;
+  end if;
+
+  P_p = PhaseSystem_p.activePower(terminal_p.v, terminal_p.i);
+  P_n = PhaseSystem_n.activePower(terminal_n.v, terminal_n.i);
+
+  v1 = terminal_n.v[2];
+  v2 = terminal_p.v[2];
+  sum(terminal_n.i) + i1 = 0;
+  sum(terminal_p.i) + i2 = 0;
+
+  // Voltage relation
+  v_p = v_n*conversionFactor;
+
+  // OLD equations that take into account the power at the secondary
+  // power balance
+  // LossPower = (1-eta) * abs(P_p);
+  // P_n + P_p - LossPower = 0;
+
+  // Symmetric and linear version
+  LossPower = P_p + P_n;
+  if i_n >=0 then
+    i_p = i_n/conversionFactor/(eta - 2);
+  else
+    i_n = conversionFactor*i_p/(eta - 2);
+  end if;
+
+  annotation ( Icon(coordinateSystem(preserveAspectRatio=false,
+          extent={{-100,-100},{100,100}}),
+                                      graphics={
+        Line(
+          points={{2,100},{2,60},{82,60},{2,60},{82,-60},{2,-60},{2,60},{2,-100}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Text(
+          extent={{30,54},{90,14}},
+          textColor={0,0,255},
+          textString="DC"),
+        Line(
+          points={{-2,100},{-2,60},{-82,60},{-2,60},{-82,-60},{-2,-60},{-2,60},
+              {-2,-100}},
+          color={85,170,255},
+          smooth=Smooth.None),
+        Text(
+          extent={{-88,54},{-28,14}},
+          textColor={85,170,255},
+          textString="DC"),
+        Text(
+          extent={{-100,92},{100,60}},
+          textColor={0,0,0},
+          textString="%name"),
+        Text(
+          extent={{-120,-60},{-2,-90}},
+          textColor={0,0,0},
+          textString="%VHigh"),
+        Text(
+          extent={{-100,-100},{100,-132}},
+          textColor={0,0,255},
+          textString="%eta"),
+        Text(
+          extent={{-132,80},{-72,40}},
+          textColor={85,170,255},
+          textString="1"),
+        Text(
+          extent={{70,80},{130,40}},
+          textColor={0,0,255},
+          textString="2"),
+        Line(visible = (ground_1 == true),
+          points={{-120,-100},{-80,-100}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = (ground_1 == true),
+          points={{-112,-106},{-88,-106}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = (ground_1 == true),
+          points={{-106,-112},{-92,-112}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = (ground_1 == true),
+          points={{-100,-100},{-100,-12}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = (ground_2 == true),
+          points={{100,-100},{100,-12}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = (ground_2 == true),
+          points={{80,-100},{120,-100}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = (ground_2 == true),
+          points={{88,-106},{112,-106}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Line(visible = (ground_2 == true),
+          points={{94,-112},{108,-112}},
+          color={0,0,255},
+          smooth=Smooth.None),
+        Text(
+          extent={{2,-60},{120,-90}},
+          textColor={0,0,0},
+          textString="%VLow")}),
+    Documentation(info="<html>
+<p>
+This is a DC/DC converter, based on a power balance between the two DC sides.
+The parameter <i>conversionFactor</i> defines the ratio between the two averaged DC voltages.
+The loss of the converter is proportional to the power transmitted at the second DC side.
+The parameter <code>eta</code> is the efficiency of the transfer.
+The loss is computed as
+<p align=\"center\" style=\"font-style:italic;\">
+P<sub>loss</sub> = (1-&eta;) P<sub>DC</sub>,
+</p>
+<p>
+where <i>P<sub>DC</sub></i> is the power transmitted. This model is symmetric and the power
+can be transmitted in both directions. The loss is computed depending on the direction
+of the power flow.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Michael Wetter:<br/>
+Removed redeclaration of phase system in <code>Terminal_n</code> and
+<code>Terminal_p</code> as it is already declared to the be the same
+phase system, and it is not declared to be replaceable.
+This avoids a translation error in OpenModelica.
+</li>
+<li>
+June 2, 2014, by Marco Bonvini:<br/>
+Revised model and documentation. Changed parameter sof the model,
+now the user specify <code>VHigh</code> and <code>VLow</code>
+instead of <code>conversionFactor</code>.
+</li>
+<li>
+January 28, 2012, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DCDCConverter;
diff --git a/AixLib/Electrical/DC/Conversion/Examples/DCDCConverter.mo b/AixLib/Electrical/DC/Conversion/Examples/DCDCConverter.mo
new file mode 100644
index 0000000000..0ce32bf823
--- /dev/null
+++ b/AixLib/Electrical/DC/Conversion/Examples/DCDCConverter.mo
@@ -0,0 +1,78 @@
+within AixLib.Electrical.DC.Conversion.Examples;
+model DCDCConverter "Test model DC to DC converter"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.DC.Loads.Conductor resistor(
+    mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    P_nominal=-2000,
+    V_nominal=60) "Resistive load"
+    annotation (Placement(transformation(extent={{38,30},{58,50}})));
+  AixLib.Electrical.DC.Sources.ConstantVoltage sou(V=120)
+    "Voltage source"
+    annotation (Placement(transformation(extent={{-90,-10},{-70,10}})));
+  AixLib.Electrical.DC.Conversion.DCDCConverter conDCDC(
+    VHigh=120,
+    VLow=60,
+    eta=0.9,
+    i_n(start=0)) "DC/DC transformer"
+    annotation (Placement(transformation(extent={{-20,-10},{0,10}})));
+  AixLib.Electrical.DC.Loads.Conductor conductor(mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+      V_nominal=60,
+    P_nominal=10e3) "Variable resistive load"
+    annotation (Placement(transformation(extent={{38,-30},{58,-10}})));
+  Modelica.Blocks.Sources.Ramp varLoad_P(
+    duration=0.5,
+    startTime=0.3,
+    offset=-1000,
+    height=10000)
+    annotation (Placement(transformation(extent={{90,-30},{70,-10}})));
+  AixLib.Electrical.DC.Sensors.GeneralizedSensor sen "Power sensor"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+equation
+  connect(varLoad_P.y, conductor.Pow) annotation (Line(
+      points={{69,-20},{58,-20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(conDCDC.terminal_p, resistor.terminal) annotation (Line(
+      points={{4.44089e-16,0},{10,0},{10,40},{38,40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(conDCDC.terminal_p, conductor.terminal) annotation (Line(
+      points={{4.44089e-16,0},{10,0},{10,-20},{38,-20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sou.terminal, sen.terminal_n) annotation (Line(
+      points={{-70,0},{-60,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, conDCDC.terminal_n) annotation (Line(
+      points={{-40,0},{-20,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0,Tolerance=1e-06),
+    Documentation(info="<html>
+<p>
+This model illustrates the use of a model that converts between DC voltages.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+January 30, 2019, by Michael Wetter:<br/>
+Added start value.
+</li>
+<li>
+June 2, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+January 29, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Conversion/Examples/DCDCConverter.mos"
+        "Simulate and plot"),
+    Icon(coordinateSystem(extent={{-140,-100},{100,140}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end DCDCConverter;
diff --git a/AixLib/Electrical/DC/Conversion/Examples/package.mo b/AixLib/Electrical/DC/Conversion/Examples/package.mo
new file mode 100644
index 0000000000..5ad4e4b819
--- /dev/null
+++ b/AixLib/Electrical/DC/Conversion/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Electrical.DC.Conversion;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.DC.Conversion\">
+AixLib.Electrical.DC.Conversion</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/DC/Conversion/Examples/package.order b/AixLib/Electrical/DC/Conversion/Examples/package.order
new file mode 100644
index 0000000000..427cd314cc
--- /dev/null
+++ b/AixLib/Electrical/DC/Conversion/Examples/package.order
@@ -0,0 +1 @@
+DCDCConverter
diff --git a/AixLib/Electrical/DC/Conversion/package.mo b/AixLib/Electrical/DC/Conversion/package.mo
new file mode 100644
index 0000000000..076b888de9
--- /dev/null
+++ b/AixLib/Electrical/DC/Conversion/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Electrical.DC;
+package Conversion "Package with models for DC/DC conversion"
+  extends Modelica.Icons.Package;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models for DC/DC conversion.
+AC/DC converters can be found in the respective AC package.
+</p>
+</html>"));
+end Conversion;
diff --git a/AixLib/Electrical/DC/Conversion/package.order b/AixLib/Electrical/DC/Conversion/package.order
new file mode 100644
index 0000000000..18c912e5fd
--- /dev/null
+++ b/AixLib/Electrical/DC/Conversion/package.order
@@ -0,0 +1,2 @@
+DCDCConverter
+Examples
diff --git a/AixLib/Electrical/DC/Interfaces/Terminal_n.mo b/AixLib/Electrical/DC/Interfaces/Terminal_n.mo
new file mode 100644
index 0000000000..12c3b01193
--- /dev/null
+++ b/AixLib/Electrical/DC/Interfaces/Terminal_n.mo
@@ -0,0 +1,14 @@
+within AixLib.Electrical.DC.Interfaces;
+connector Terminal_n "Terminal n for DC electrical systems"
+  extends AixLib.Electrical.Interfaces.Terminal(
+    redeclare package PhaseSystem =
+        AixLib.Electrical.PhaseSystems.TwoConductor);
+  annotation (Icon(graphics={  Polygon(
+          points={{-120,0},{0,-120},{120,0},{0,120},{-120,0}},
+          lineColor={0,0,255},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Documentation(info="<html>
+<p>Electric connector for DC electrical systems.</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal_n;
diff --git a/AixLib/Electrical/DC/Interfaces/Terminal_p.mo b/AixLib/Electrical/DC/Interfaces/Terminal_p.mo
new file mode 100644
index 0000000000..71019dd6e5
--- /dev/null
+++ b/AixLib/Electrical/DC/Interfaces/Terminal_p.mo
@@ -0,0 +1,14 @@
+within AixLib.Electrical.DC.Interfaces;
+connector Terminal_p "Terminal p for DC electrical systems"
+  extends AixLib.Electrical.Interfaces.Terminal(
+    redeclare package PhaseSystem =
+        AixLib.Electrical.PhaseSystems.TwoConductor);
+  annotation (Icon(graphics={  Polygon(
+          points={{-120,0},{0,-120},{120,0},{0,120},{-120,0}},
+          lineColor={0,0,255},
+          fillColor={0,0,255},
+          fillPattern=FillPattern.Solid)}), Documentation(info="<html>
+<p>Electric connector for DC electrical systems.</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal_p;
diff --git a/AixLib/Electrical/DC/Interfaces/package.mo b/AixLib/Electrical/DC/Interfaces/package.mo
new file mode 100644
index 0000000000..167b8a759b
--- /dev/null
+++ b/AixLib/Electrical/DC/Interfaces/package.mo
@@ -0,0 +1,15 @@
+within AixLib.Electrical.DC;
+package Interfaces "Package with interfaces for DC electrical systems"
+  extends Modelica.Icons.InterfacesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains connectors that are used by the models in the
+<a href=\"modelica://AixLib.Electrical.DC\">AixLib.Electrical.DC</a> package.
+The connectors extends the basic connectors
+<a href=\"modelica://AixLib.Electrical.Interfaces.Terminal\">AixLib.Electrical.Interfaces.Terminal</a>
+and define a new graphical icon in order to be distinguished by connectors of other electrical systems (e.g. AC systems).
+</p>
+</html>"));
+end Interfaces;
diff --git a/AixLib/Electrical/DC/Interfaces/package.order b/AixLib/Electrical/DC/Interfaces/package.order
new file mode 100644
index 0000000000..d23ecfc486
--- /dev/null
+++ b/AixLib/Electrical/DC/Interfaces/package.order
@@ -0,0 +1,2 @@
+Terminal_n
+Terminal_p
diff --git a/AixLib/Electrical/DC/Lines/Examples/DCLine.mo b/AixLib/Electrical/DC/Lines/Examples/DCLine.mo
new file mode 100644
index 0000000000..f772d36c4f
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/Examples/DCLine.mo
@@ -0,0 +1,93 @@
+within AixLib.Electrical.DC.Lines.Examples;
+model DCLine "Example model to test the DC lines"
+  extends Modelica.Icons.Example;
+  Line line(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=100) "Transmission line"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Sources.ConstantVoltage E(V=50) "Voltage source"
+    annotation (Placement(transformation(extent={{-80,0},{-60,20}})));
+  Line line1(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=100) "Transmission line"
+    annotation (Placement(transformation(extent={{0,-20},{20,0}})));
+  Line line2(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=100) "Transmission line"
+    annotation (Placement(transformation(extent={{0,-40},{20,-20}})));
+  Modelica.Electrical.Analog.Basic.Ground ground
+    annotation (Placement(transformation(extent={{-90,-20},{-70,0}})));
+  Loads.Conductor load1(mode=Types.Load.VariableZ_y_input,
+    V_nominal=50,
+    linearized=false,
+    P_nominal=-50) "Variable load"
+    annotation (Placement(transformation(extent={{40,0},{60,20}})));
+  Loads.Conductor load2(
+    V_nominal=50,
+    linearized=false,
+    P_nominal=-150) "Load"
+    annotation (Placement(transformation(extent={{40,-20},{60,0}})));
+  Loads.Conductor load3(
+    V_nominal=50,
+    linearized=false,
+    P_nominal=-200) "Load"
+    annotation (Placement(transformation(extent={{40,-40},{60,-20}})));
+  Modelica.Blocks.Sources.Ramp varLoad(
+    height=0.8,
+    duration=0.5,
+    offset=0.2,
+    startTime=0.3) "Load consumption profile"
+    annotation (Placement(transformation(extent={{96,0},{76,20}})));
+equation
+  connect(E.terminal, line.terminal_n) annotation (Line(
+      points={{-60,10},{-4.44089e-16,10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(E.terminal, line1.terminal_n) annotation (Line(
+      points={{-60,10},{-30,10},{-30,-10},{0,-10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(E.terminal, line2.terminal_n) annotation (Line(
+      points={{-60,10},{-30,10},{-30,-30},{0,-30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(load1.terminal, line.terminal_p) annotation (Line(
+      points={{40,10},{20,10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, load2.terminal) annotation (Line(
+      points={{20,-10},{40,-10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line2.terminal_p, load3.terminal) annotation (Line(
+      points={{20,-30},{40,-30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(varLoad.y, load1.y) annotation (Line(
+      points={{75,10},{60,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(E.n, ground.p) annotation (Line(
+      points={{-80,10},{-80,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=1.0,Tolerance=1e-06),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLine.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This model is a simple test case that show how to use a line model
+and parametrize it using a commercial cable.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DCLine;
diff --git a/AixLib/Electrical/DC/Lines/Examples/DCLines.mo b/AixLib/Electrical/DC/Lines/Examples/DCLines.mo
new file mode 100644
index 0000000000..e0f8301c98
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/Examples/DCLines.mo
@@ -0,0 +1,428 @@
+within AixLib.Electrical.DC.Lines.Examples;
+model DCLines
+  "Example model to test the possible combinations between line and load models"
+  extends Modelica.Icons.Example;
+  parameter Boolean linearLoads = false
+    "Flag that selects between linearized or nonlinear load models";
+  parameter Real L = 10 "Length of each cable";
+  Modelica.Units.SI.Power Sloads=load1.S[1] + load2.S[1] + load3.S[1] + load4.S[
+      1] + load5.S[1] + load6.S[1] + load7.S[1] + load8.S[1] + load9.S[1] +
+      load10.S[1] "Sum of the power consumed by the loads";
+  Line line(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L,
+    terminal_n(v(each start=0))) "Transmission line"
+    annotation (Placement(transformation(extent={{-2,70},{18,90}})));
+  Sources.ConstantVoltage E(V=50) "Voltage source"
+    annotation (Placement(transformation(extent={{-90,70},{-70,90}})));
+  Line line1(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{-32,70},{-12,90}})));
+
+  Line line2(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{-34,30},{-14,50}})));
+
+  Modelica.Electrical.Analog.Basic.Ground ground
+    annotation (Placement(transformation(extent={{-100,50},{-80,70}})));
+  Loads.Conductor load1(mode=Types.Load.VariableZ_y_input,
+    V_nominal=50,
+    linearized=linearLoads,
+    P_nominal=-150) "Load"
+    annotation (Placement(transformation(extent={{30,70},{50,90}})));
+  Loads.Conductor load2(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-120) "Load"
+    annotation (Placement(transformation(extent={{30,50},{50,70}})));
+  Loads.Conductor load3(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-200) "Load"
+    annotation (Placement(transformation(extent={{30,30},{50,50}})));
+  Modelica.Blocks.Sources.Trapezoid
+                               varLoad1(
+    offset=0.4,
+    amplitude=0.6,
+    rising=600,
+    width=1000,
+    falling=800,
+    period=3600,
+    startTime=1800) "Power consumption profile"
+    annotation (Placement(transformation(extent={{86,30},{66,50}})));
+  Loads.Conductor load4(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-120) "Load"
+    annotation (Placement(transformation(extent={{30,12},{50,32}})));
+  Line line3(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{2,30},{22,50}})));
+
+  Line line4(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{0,50},{20,70}})));
+
+  Line line5(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{2,12},{22,32}})));
+
+  Line line0(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{-64,70},{-44,90}})));
+
+  Modelica.Blocks.Sources.Trapezoid
+                               varLoad2(
+    startTime=1800,
+    amplitude=0.8,
+    rising=400,
+    width=1300,
+    falling=900,
+    period=4000,
+    offset=0.1) "Power consumption profile"
+    annotation (Placement(transformation(extent={{86,70},{66,90}})));
+  Line line6(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{-34,-10},{-14,10}})));
+
+  Loads.Conductor load5(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-200) "Load"
+    annotation (Placement(transformation(extent={{30,-10},{50,10}})));
+  Modelica.Blocks.Sources.Trapezoid
+                               varLoad3(
+    amplitude=0.7,
+    rising=660,
+    width=900,
+    falling=300,
+    period=3700,
+    offset=0.3,
+    startTime=200) "Power consumption profile"
+    annotation (Placement(transformation(extent={{86,-10},{66,10}})));
+  Loads.Conductor load6(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-120) "Load"
+    annotation (Placement(transformation(extent={{30,-28},{50,-8}})));
+  Line line7(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{2,-10},{22,10}})));
+
+  Line line8(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{2,-28},{22,-8}})));
+
+  Line line9(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{-34,-50},{-14,-30}})));
+
+  Loads.Conductor load7(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-200) "Load"
+    annotation (Placement(transformation(extent={{30,-50},{50,-30}})));
+  Modelica.Blocks.Sources.Trapezoid
+                               varLoad4(
+    rising=600,
+    width=1000,
+    falling=800,
+    period=3600,
+    amplitude=0.1,
+    offset=0.8,
+    startTime=3300) "Power consumption profile"
+    annotation (Placement(transformation(extent={{86,-50},{66,-30}})));
+  Loads.Conductor load8(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-120) "Load"
+    annotation (Placement(transformation(extent={{30,-68},{50,-48}})));
+  Line line10(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{2,-50},{22,-30}})));
+
+  Line line11(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{2,-68},{22,-48}})));
+
+  Line line12(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{-34,-90},{-14,-70}})));
+
+  Loads.Conductor load9(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-200) "Load"
+    annotation (Placement(transformation(extent={{30,-90},{50,-70}})));
+  Modelica.Blocks.Sources.Trapezoid
+                               varLoad5(
+    falling=800,
+    amplitude=0.5,
+    rising=800,
+    width=800,
+    period=3000,
+    offset=0.5,
+    startTime=0) "Power consumption profile"
+    annotation (Placement(transformation(extent={{86,-90},{66,-70}})));
+  Loads.Conductor load10(
+    V_nominal=50,
+    mode=Types.Load.VariableZ_y_input,
+    linearized=linearLoads,
+    P_nominal=-120) "Load"
+    annotation (Placement(transformation(extent={{30,-108},{50,-88}})));
+  Line line13(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=L) "Transmission line"
+    annotation (Placement(transformation(extent={{2,-90},{22,-70}})));
+
+  Line line14(
+    P_nominal=500,
+    V_nominal=50,
+    mode=Types.CableMode.commercial,
+    commercialCable=Transmission.LowVoltageCables.PvcAl16(),
+    l=100) "Transmission line"
+    annotation (Placement(transformation(extent={{2,-108},{22,-88}})));
+
+equation
+  connect(load1.terminal, line.terminal_p) annotation (Line(
+      points={{30,80},{18,80}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, line.terminal_n) annotation (Line(
+      points={{-12,80},{-2,80}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line2.terminal_p, line3.terminal_n) annotation (Line(
+      points={{-14,40},{2,40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line3.terminal_p, load3.terminal) annotation (Line(
+      points={{22,40},{30,40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line1.terminal_p, line4.terminal_n) annotation (Line(
+      points={{-12,80},{-6,80},{-6,60},{0,60}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line4.terminal_p, load2.terminal) annotation (Line(
+      points={{20,60},{30,60}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(load4.terminal, line5.terminal_p) annotation (Line(
+      points={{30,22},{22,22}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line5.terminal_n, line3.terminal_n) annotation (Line(
+      points={{2,22},{-8,22},{-8,40},{2,40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(E.terminal, line0.terminal_n) annotation (Line(
+      points={{-70,80},{-64,80}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line0.terminal_p, line1.terminal_n) annotation (Line(
+      points={{-44,80},{-32,80}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(varLoad1.y, load3.y) annotation (Line(
+      points={{65,40},{50,40}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(varLoad1.y, load4.y) annotation (Line(
+      points={{65,40},{58,40},{58,22},{50,22}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(varLoad2.y, load1.y) annotation (Line(
+      points={{65,80},{50,80}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(varLoad2.y, load2.y) annotation (Line(
+      points={{65,80},{58,80},{58,60},{50,60}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line6.terminal_p,line7. terminal_n) annotation (Line(
+      points={{-14,0},{2,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line7.terminal_p,load5. terminal) annotation (Line(
+      points={{22,0},{30,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(load6.terminal,line8. terminal_p) annotation (Line(
+      points={{30,-18},{22,-18}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line8.terminal_n,line7. terminal_n) annotation (Line(
+      points={{2,-18},{-8,-18},{-8,0},{2,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(varLoad3.y,load5. y) annotation (Line(
+      points={{65,0},{50,0}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(varLoad3.y,load6. y) annotation (Line(
+      points={{65,0},{58,0},{58,-18},{50,-18}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line9.terminal_p, line10.terminal_n)
+                                              annotation (Line(
+      points={{-14,-40},{2,-40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line10.terminal_p, load7.terminal)
+                                            annotation (Line(
+      points={{22,-40},{30,-40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(load8.terminal, line11.terminal_p)
+                                            annotation (Line(
+      points={{30,-58},{22,-58}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line11.terminal_n, line10.terminal_n)
+                                              annotation (Line(
+      points={{2,-58},{-8,-58},{-8,-40},{2,-40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(varLoad4.y,load7. y) annotation (Line(
+      points={{65,-40},{50,-40}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(varLoad4.y,load8. y) annotation (Line(
+      points={{65,-40},{58,-40},{58,-58},{50,-58}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line12.terminal_p, line13.terminal_n)
+                                              annotation (Line(
+      points={{-14,-80},{2,-80}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line13.terminal_p, load9.terminal)
+                                            annotation (Line(
+      points={{22,-80},{30,-80}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(load10.terminal, line14.terminal_p)
+                                            annotation (Line(
+      points={{30,-98},{22,-98}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line14.terminal_n, line13.terminal_n)
+                                              annotation (Line(
+      points={{2,-98},{-8,-98},{-8,-80},{2,-80}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(varLoad5.y,load9. y) annotation (Line(
+      points={{65,-80},{50,-80}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(varLoad5.y, load10.y)
+                               annotation (Line(
+      points={{65,-80},{58,-80},{58,-98},{50,-98}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(line2.terminal_n, line4.terminal_n) annotation (Line(
+      points={{-34,40},{-34,60},{0,60}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line6.terminal_n, line3.terminal_n) annotation (Line(
+      points={{-34,0},{-34,22},{-8,22},{-8,40},{2,40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line9.terminal_n, line7.terminal_n) annotation (Line(
+      points={{-34,-40},{-34,-18},{-8,-18},{-8,0},{2,0},{2,5.55112e-16}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(line12.terminal_n, line10.terminal_n) annotation (Line(
+      points={{-34,-80},{-34,-58},{-8,-58},{-8,-40},{2,-40}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(E.n, ground.p) annotation (Line(
+      points={{-90,80},{-90,70}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation (experiment(StopTime=4000,Tolerance=1e-06),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLines.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This model shows a DC grid with 10 loads and 16 cables.
+Each cable is of length <i>l = 10</i> meters, a parameter that can be modified.
+Each load can be either be a full nonlinear model, or be replaced by the
+linearized version. The parameter <code>linearLoads = false</code>
+can be used to switch between linear and nonlinear implementation.
+</p>
+<p>
+This model can be used to test how the linearized loads are affected by the voltage drop
+caused by the lines. The longer the distance between the load and the source,
+the bigger is the voltage drop and thus the error introduced by the linearization.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DCLines;
diff --git a/AixLib/Electrical/DC/Lines/Examples/DCLinesLinearized.mo b/AixLib/Electrical/DC/Lines/Examples/DCLinesLinearized.mo
new file mode 100644
index 0000000000..f07d90c1e0
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/Examples/DCLinesLinearized.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.DC.Lines.Examples;
+model DCLinesLinearized
+  "Example model to test the possible combinations between line and load models"
+  extends AixLib.Electrical.DC.Lines.Examples.DCLines(linearLoads = true);
+
+  annotation (Documentation(info="<html>
+<p>
+This model is the linearized version of the model
+<a href=\"modelica://AixLib.Electrical.DC.Lines.Examples.DCLines\">
+AixLib.Electrical.DC.Lines.Examples.DCLines</a> and
+can be used to test how the linearized loads are affected by the voltage drop
+caused by the lines. The longer the distance between the load and the source,
+the bigger is the voltage drop and thus the error introduced by the linearization.
+</p>
+</html>"),
+experiment(Tolerance=1e-06, StopTime=4000),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLinesLinearized.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end DCLinesLinearized;
diff --git a/AixLib/Electrical/DC/Lines/Examples/RCModel.mo b/AixLib/Electrical/DC/Lines/Examples/RCModel.mo
new file mode 100644
index 0000000000..f3667ef9bd
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/Examples/RCModel.mo
@@ -0,0 +1,96 @@
+within AixLib.Electrical.DC.Lines.Examples;
+model RCModel "Example model to test for the DC RC two port model"
+  extends Modelica.Icons.Example;
+
+  TwoPortRCLine RC_ss(
+    C=1,
+    V_nominal=50,
+    R=8) "Line resistance"
+         annotation (Placement(transformation(extent={{-30,10},{-10,30}})));
+  Sources.ConstantVoltage constantVoltage(V=50) "Voltage source"
+    annotation (Placement(transformation(extent={{-60,10},{-40,30}})));
+  Modelica.Electrical.Analog.Basic.Ground ground
+    annotation (Placement(transformation(extent={{-72,-16},{-52,4}})));
+  Loads.Resistor sc_ss(V_nominal=50, R=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{30,10},{50,30}})));
+  Sensors.GeneralizedSensor sen_ss "Sensor"
+    annotation (Placement(transformation(extent={{0,10},{20,30}})));
+  TwoPortRCLine RC_dyn(
+    C=1,
+    V_nominal=50,
+    use_C=true,
+    R=8) "Line resistance"
+         annotation (Placement(transformation(extent={{-28,-20},{-8,0}})));
+  Loads.Resistor sc_dyn(V_nominal=50, R=0) "Load"
+    annotation (Placement(transformation(extent={{32,-20},{52,0}})));
+  Sensors.GeneralizedSensor sen_dyn "Sensor"
+    annotation (Placement(transformation(extent={{2,-20},{22,0}})));
+equation
+  connect(ground.p, constantVoltage.n) annotation (Line(
+      points={{-62,4},{-62,20},{-60,20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(constantVoltage.terminal, RC_ss.terminal_n) annotation (Line(
+      points={{-40,20},{-30,20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(RC_ss.terminal_p, sen_ss.terminal_n) annotation (Line(
+      points={{-10,20},{0,20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen_ss.terminal_p, sc_ss.terminal) annotation (Line(
+      points={{20,20},{30,20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(RC_dyn.terminal_p, sen_dyn.terminal_n) annotation (Line(
+      points={{-8,-10},{2,-10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen_dyn.terminal_p, sc_dyn.terminal) annotation (Line(
+      points={{22,-10},{32,-10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(constantVoltage.terminal, RC_dyn.terminal_n) annotation (Line(
+      points={{-40,20},{-34,20},{-34,-10},{-28,-10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation (
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/RCModel.mos"
+        "Simulate and plot"),
+        experiment(StopTime=15.0,Tolerance=1e-06),
+    Documentation(info="<html>
+<p>
+This model shows how to use a two port resistance-capacitance model.
+The example also shows a comparison between the dynamic and steady state version model
+that can be selected by changing the boolean flag <code>use_C</code>.
+</p>
+<p>
+In this example the RC connects an ideal constant voltage source with
+a short circuit. The steady state current value passing through the RC
+model depends just on the value of <i>R</i>.
+</p>
+<p>
+The RC model implement a T-model to represent the electric connection between the
+two connectors (see <a href=\"modelica://AixLib.Electrical.DC.Lines.TwoPortRCLine\">
+AixLib.Electrical.DC.Lines.TwoPortRCLine</a> for more details).
+</p>
+<p>
+The capacitance <i>C</i> see an equivalent Thevenin's resistance that is equal to
+<i>R<sub>EQ</sub> = 0.5 R</i> and thus the time constant associated to the capacitance is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&tau; = R<sub>EQ</sub> C = 0.5 R C = 2 seconds,
+</p>
+<p>
+thus the duration of transient period is about 10 seconds.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 4, 2014, by Marco Bonvini:<br/>
+Added model, documentation and results for regression test.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end RCModel;
diff --git a/AixLib/Electrical/DC/Lines/Examples/Resistance.mo b/AixLib/Electrical/DC/Lines/Examples/Resistance.mo
new file mode 100644
index 0000000000..4e18dd0553
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/Examples/Resistance.mo
@@ -0,0 +1,51 @@
+within AixLib.Electrical.DC.Lines.Examples;
+model Resistance "Example model to test for the DC resistance two port model"
+  extends Modelica.Icons.Example;
+
+  TwoPortResistance lineR(R=10) "Line resistance"
+    annotation (Placement(transformation(extent={{-30,10},{-10,30}})));
+  Sources.ConstantVoltage constantVoltage(V=50) "Voltage source"
+    annotation (Placement(transformation(extent={{-60,10},{-40,30}})));
+  Modelica.Electrical.Analog.Basic.Ground ground
+    annotation (Placement(transformation(extent={{-72,-16},{-52,4}})));
+  Loads.Resistor short_circuit(V_nominal=50, R=0) "Short circuit load"
+    annotation (Placement(transformation(extent={{30,10},{50,30}})));
+  Sensors.GeneralizedSensor sen "Power sensor"
+    annotation (Placement(transformation(extent={{0,10},{20,30}})));
+equation
+  connect(ground.p, constantVoltage.n) annotation (Line(
+      points={{-62,4},{-62,20},{-60,20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(constantVoltage.terminal, lineR.terminal_n) annotation (Line(
+      points={{-40,20},{-30,20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(lineR.terminal_p, sen.terminal_n) annotation (Line(
+      points={{-10,20},{0,20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, short_circuit.terminal) annotation (Line(
+      points={{20,20},{30,20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation ( Documentation(info="<html>
+<p>
+This model shows how to use a two port resistance.
+In this example the resistance connects an ideal constant voltage source with
+a short circuit. The current flowing through the circuit depends just
+on the value of the two port resistance.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 4, 2014, by Marco Bonvini:<br/>
+Added model, documentation and results for regression test.
+</li>
+</ul>
+</html>"),
+experiment(Tolerance=1e-06, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/Resistance.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Resistance;
diff --git a/AixLib/Electrical/DC/Lines/Examples/package.mo b/AixLib/Electrical/DC/Lines/Examples/package.mo
new file mode 100644
index 0000000000..07e4071e38
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Electrical.DC.Lines;
+package Examples "Package with example models"
+extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.DC.Lines\">
+AixLib.Electrical.DC.Lines</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/DC/Lines/Examples/package.order b/AixLib/Electrical/DC/Lines/Examples/package.order
new file mode 100644
index 0000000000..0af379de9f
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/Examples/package.order
@@ -0,0 +1,5 @@
+DCLine
+DCLines
+DCLinesLinearized
+RCModel
+Resistance
diff --git a/AixLib/Electrical/DC/Lines/Line.mo b/AixLib/Electrical/DC/Lines/Line.mo
new file mode 100644
index 0000000000..d99a381f40
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/Line.mo
@@ -0,0 +1,94 @@
+within AixLib.Electrical.DC.Lines;
+model Line "Model of a DC electrical line"
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialLine(
+    redeclare package PhaseSystem_p = PhaseSystems.TwoConductor,
+    redeclare package PhaseSystem_n = PhaseSystems.TwoConductor,
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p,
+    final modelMode=Types.Load.FixedZ_steady_state,
+    commercialCable = AixLib.Electrical.Transmission.Functions.selectCable_low(P_nominal, V_nominal));
+
+  TwoPortRCLine lineRC(
+    final useHeatPort=true,
+    final R=R,
+    final V_nominal=V_nominal,
+    final T_ref=T_ref,
+    final M=M,
+    final C=C,
+    final use_C=use_C)
+    annotation (Placement(transformation(extent={{-10,10},{10,-10}})));
+equation
+  connect(terminal_n, lineRC.terminal_n) annotation (Line(
+      points={{-100,0},{-10,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(lineRC.terminal_p, terminal_p) annotation (Line(
+      points={{10,0},{100,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(cableTemp.port, lineRC.heatPort) annotation (Line(
+      points={{-40,22},{0,22},{0,10}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  annotation ( Icon(graphics={
+        Ellipse(
+          extent={{-70,10},{-50,-10}},
+          lineColor={0,0,0},
+          fillColor={96,107,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-60,10},{60,-10}},
+          fillColor={96,107,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{50,10},{70,-10}},
+          lineColor={0,0,0},
+          fillColor={255,128,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-70,0},{-90,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,10},{60,10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,-10},{60,-10}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{96,0},{60,0}},
+          color={0,0,0},
+          smooth=Smooth.None)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Michael Wetter:<br/>
+Removed redeclaration of phase system in <code>Terminal_n</code> and
+<code>Terminal_p</code> as it is already declared to the be the same
+phase system, and it is not declared to be replaceable.
+This avoids a translation error in OpenModelica.
+</li>
+<li>
+June 2, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a DC cable. The model is based on
+<a href=\"modelica://AixLib.Electrical.DC.Lines.TwoPortRCLine\">
+AixLib.Electrical.DC.Lines.TwoPortRCLine</a>
+and provides functionalities to parametrize the values of <i>R</i> and <i>C</i> either
+using commercial cables or using default values.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Line;
diff --git a/AixLib/Electrical/DC/Lines/TwoPortRCLine.mo b/AixLib/Electrical/DC/Lines/TwoPortRCLine.mo
new file mode 100644
index 0000000000..382bcff8b3
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/TwoPortRCLine.mo
@@ -0,0 +1,99 @@
+within AixLib.Electrical.DC.Lines;
+model TwoPortRCLine "Model of a two port DC resistance and capacity (T-model)"
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialTwoPortRLC(
+    redeclare package PhaseSystem_p = PhaseSystems.TwoConductor,
+    redeclare package PhaseSystem_n = PhaseSystems.TwoConductor,
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p,
+    final L=0);
+  parameter Boolean use_C = false
+    "Set to true to add a capacitance in the center of the line"
+    annotation(Dialog(tab="Model", group="Assumptions"));
+  parameter Modelica.Units.SI.Voltage Vc_start=V_nominal
+    "Initial value of the voltage of the capacitance in the middle of the line";
+  Modelica.Units.SI.Voltage Vc(start=Vc_start, stateSelect=StateSelect.prefer)
+    "Voltage of the capacitor";
+initial equation
+  if C>0 and use_C then
+    Vc = Vc_start;
+  end if;
+equation
+  terminal_p.v[1] - (Vc+terminal_p.v[2]) = terminal_p.i[1]*R_actual/2;
+  terminal_n.v[1] - (Vc+terminal_p.v[2]) = terminal_n.i[1]*R_actual/2;
+
+  if C>0 and use_C then
+    C*der(Vc) = terminal_p.i[1] + terminal_n.i[1];
+  else
+    Vc = 0.5*(terminal_p.v[1] - terminal_p.v[2] + terminal_n.v[1] - terminal_n.v[2]);
+  end if;
+
+  terminal_p.v[2] = terminal_n.v[2];
+  terminal_p.i[2] + terminal_n.i[2] = 0;
+
+  // Joule losses
+  LossPower = R_actual/2*terminal_p.i[1]^2 + R_actual/2*terminal_n.i[1]^2;
+
+  annotation (Diagram(graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,255}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Line(points={{70,0},{90,0}},   color={0,0,255})}), Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                                                  graphics={
+          Text(
+            extent={{-144,97},{156,57}},
+            textColor={0,0,0},
+          textString="%name"),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Line(points={{70,0},{90,0}},   color={0,0,255}),
+        Rectangle(
+          extent={{-70,32},{70,-28}},
+          lineColor={0,0,255},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(info="<html>
+<p>
+This model represents a series of two resistances and a capacitance that connect two DC interfaces.
+This model can be used to represent a cable in a DC grid.
+</p>
+<p>
+The model represents the lumped resistances and capacity (T-model) as shown in the figure below.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/DC/Lines/twoPortRC.png\"/>
+</p>
+<p>
+As can be seen in the figure, the resistance <i>R</i> is split in two halves
+and the capacitance is located in the center.
+The capacitance in the center is optional and can be selected using the
+boolean flag <code>use_C = true</code>. The model is either dynamic or static depending on the
+presence of the capacitive effect.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Michael Wetter:<br/>
+Removed redeclaration of phase system in <code>Terminal_n</code> and
+<code>Terminal_p</code> as it is already declared to the be the same
+phase system, and it is not declared to be replaceable.
+This avoids a translation error in OpenModelica.
+</li>
+<li>
+March 10, 2015, by Marco Bonvini:<br/>
+Added initial equation and parameter <code>Vc_start</code>.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added equation that represents Joule losses
+</li>
+<li>
+June 2, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortRCLine;
diff --git a/AixLib/Electrical/DC/Lines/TwoPortResistance.mo b/AixLib/Electrical/DC/Lines/TwoPortResistance.mo
new file mode 100644
index 0000000000..93f8919f70
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/TwoPortResistance.mo
@@ -0,0 +1,74 @@
+within AixLib.Electrical.DC.Lines;
+model TwoPortResistance "Model of a two port DC resistance"
+  extends
+    AixLib.Electrical.Transmission.BaseClasses.PartialTwoPortResistance(
+    redeclare package PhaseSystem_p = PhaseSystems.TwoConductor,
+    redeclare package PhaseSystem_n = PhaseSystems.TwoConductor,
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+equation
+  // Voltage drop on the resistance lumped on connection between terminals
+  // p.v[1] and n.v[1]
+  terminal_p.v[1] - terminal_n.v[1] = terminal_p.i[1]*R_actual;
+  terminal_p.v[2] = terminal_n.v[2];
+
+  // Joule losses
+  LossPower = R_actual*terminal_p.i[1]^2;
+
+  annotation (Diagram(graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,255}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Line(points={{70,0},{90,0}},   color={0,0,255})}), Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                                                  graphics={
+          Text(
+            extent={{-144,97},{156,57}},
+            textColor={0,0,0},
+          textString="%name"),
+          Text(
+            extent={{-142,-30},{144,-62}},
+            textColor={0,0,0},
+          textString="R=%R"),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Line(points={{70,0},{90,0}},   color={0,0,255}),
+        Rectangle(
+          extent={{-70,30},{70,-30}},
+          lineColor={0,0,255},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(info="<html>
+<p>
+This model represents a resistance that connect two DC interfaces. This model can be used
+to represent a cable in a DC grid.
+</p>
+<p>
+The model represents the lumped resistance as shown in the figure below.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/DC/Lines/twoPortR.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Michael Wetter:<br/>
+Removed redeclaration of phase system in <code>Terminal_n</code> and
+<code>Terminal_p</code> as it is already declared to the be the same
+phase system, and it is not declared to be replaceable.
+This avoids a translation error in OpenModelica.
+</li>
+<li>
+January 14, 2015, by Marco Bonvini:<br/>
+Added equation that represents Joule losses
+</li>
+<li>
+June 2, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoPortResistance;
diff --git a/AixLib/Electrical/DC/Lines/package.mo b/AixLib/Electrical/DC/Lines/package.mo
new file mode 100644
index 0000000000..8b487e4e5a
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/package.mo
@@ -0,0 +1,28 @@
+within AixLib.Electrical.DC;
+package Lines "Package with models for DC electrical lines"
+  extends Modelica.Icons.Package;
+
+
+annotation (Icon(graphics={
+      Ellipse(
+        extent={{40,8},{16,-28}},
+        lineColor={0,0,0},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),
+      Line(
+        points={{28,8},{-54,8},{-64,8},{-72,-10},{-64,-28},{-52,-28},{28,-28}},
+        color={0,0,0},
+        smooth=Smooth.Bezier),
+      Line(
+        points={{-70,-10},{-88,-10}},
+        color={0,0,0},
+        smooth=Smooth.None),
+      Line(
+        points={{54,-10},{28,-10}},
+        color={0,0,0},
+        smooth=Smooth.None)}), Documentation(info="<html>
+<p>
+This package contains models for lines for DC circuits.
+</p>
+</html>"));
+end Lines;
diff --git a/AixLib/Electrical/DC/Lines/package.order b/AixLib/Electrical/DC/Lines/package.order
new file mode 100644
index 0000000000..7f10e753a9
--- /dev/null
+++ b/AixLib/Electrical/DC/Lines/package.order
@@ -0,0 +1,4 @@
+Line
+TwoPortRCLine
+TwoPortResistance
+Examples
diff --git a/AixLib/Electrical/DC/Loads/Conductor.mo b/AixLib/Electrical/DC/Loads/Conductor.mo
new file mode 100644
index 0000000000..6e6ea8a941
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/Conductor.mo
@@ -0,0 +1,185 @@
+within AixLib.Electrical.DC.Loads;
+model Conductor "Model of a generic DC load"
+    extends AixLib.Electrical.Interfaces.ResistiveLoad(
+     redeclare package PhaseSystem = PhaseSystems.TwoConductor,
+     redeclare Interfaces.Terminal_n terminal);
+protected
+  Modelica.Units.SI.Voltage absDV
+    "Absolute value of the voltage difference between the two conductors (used by the linearized model)";
+equation
+
+  absDV = abs(terminal.v[1]-terminal.v[2]);
+
+  if linearized then
+
+    // Linearized version of the model
+    if absDV <= (8/9)*V_nominal then
+      terminal.i[1] + P*(2/(0.8*V_nominal) - (terminal.v[1]-terminal.v[2])/(0.8*V_nominal)^2) = 0;
+    elseif absDV >= (12/11)*V_nominal then
+      terminal.i[1] + P*(2/(1.2*V_nominal) - (terminal.v[1]-terminal.v[2])/(1.2*V_nominal)^2) = 0;
+    else
+      terminal.i[1] + P*(2/V_nominal - (terminal.v[1]-terminal.v[2])/V_nominal^2) = 0;
+    end if;
+
+  else
+    // Full nonlinear version of the model
+    // PhaseSystem.activePower(terminal.v, terminal.i) + P = 0;
+    if initMode == AixLib.Electrical.Types.InitMode.zero_current then
+      i[1] = - homotopy(actual= P/(v[1] - v[2]),  simplified= 0);
+    else
+      i[1] = - homotopy(actual= P/(v[1] - v[2]),  simplified= P*(2/V_nominal - (v[1]-v[2])/V_nominal^2));
+    end if;
+
+  end if;
+
+  // Since the connector is a two conductor, the sum of the currents at the terminal
+  // is null
+  sum(i) = 0;
+  annotation (
+    Documentation(info="<html>
+<p>
+Model of a generic DC load. The load can be either constant or variable depending on the value of the
+parameter <code>mode</code>.
+See the model <a href=\"modelica://AixLib.Electrical.Interfaces.Load\">AixLib.Electrical.Interfaces.Load</a>
+for more information.
+</p>
+
+<p>
+The model computes the current drawn from the load as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+P = V i,
+</p>
+<p>
+where <i>P</i> is the power, <i>V</i> is the voltage and <i>i</i> is the current.<br/>
+If the component consumes power, then <i>P &lt; 0</i>.
+If it feeds power into the electrical grid, then <i>P &gt; 0</i>.
+</p>
+
+<h4>Linearization</h4>
+<p>
+Consider the simple DC circuit shown in the figure below
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/DC/Loads/simpleLoad.png\"/>
+</p>
+<p>
+where <i>V<sub>S</sub></i> is a constant voltage source, and <i>R</i> is the line resistance.
+The load has a voltage <i>V</i> across its electrical pins and a current <i>i</i> is flowing through it.
+If the power consumption drawn by the load is prescribed by the variable <i>P<sub>LOAD</sub></i>,
+ the equation that describes the circuit is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+V<sub>S</sub> - R i - P<sub>LOAD</sub>/i = 0
+</p>
+<p>
+The unknown variable <i>i</i> appears in a nonlinear equation. This means that in order to compute the current
+that is drawn by the load, a nonlinear equation has to be solved. If the number of loads increases (as typically
+happens in real case examples) the number of nonlinear equations to be solved increases too, and the resulting system
+of nonlinear equations can slow down the simulation. It is possible to avoid such a problem by introducing a linearized
+model.
+</p>
+
+<p>
+The first step to linearize the load model is to define its nominal voltage conditions <i>V<sub>nom</sub></i>,
+around which the equations will be linearized.<br/>
+The constitutive equation of the load can be linearized around the nominal voltage condition <i>V<sub>nom</sub></i> as
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+i = P<sub>LOAD</sub>/V = P<sub>LOAD</sub>/V<sub>nom</sub> +
+(V - V<sub>nom</sub>)[&part; (P<sub>LOAD</sub>/V)/ &part;V ]<sub>V = V<sub>nom</sub></sub>
++ &#8338;((V - V<sub>nom</sub>)<sup>2</sup>),
+</p>
+
+<p>
+which leads to the linearized formulation
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+i &#8771; P<sub>LOAD</sub> (2/V<sub>nom</sub> - V/V<sub>nom</sub><sup>2</sup>).
+</p>
+
+<p>
+The linearized formulation approximates the load power consumption (or production),
+with the approximation error being proportional to <i>(V - V<sub>nom</sub>)<sup>2</sup></i>.
+A further approximation has been introduced to improve the
+approximation of the linearized model even if the voltage is far from the nominal condition.
+This piecewise linearized approximation instead of approximating the model just in the neighborhood of the nominal
+voltage <i>V<sub>nom</sub></i> introduces two new points where the model is approximated.
+The points are at <i>0.8 V<sub>nom</sub></i> and <i>1.2 V<sub>nom</sub></i>.
+</p>
+
+<table summary=\"equations\" border = \"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collape;\">
+<tr><th>Equation</th><th>Condition</th></tr>
+<tr>
+<td>i &#8771; P<sub>LOAD</sub> (2/(0.8 V<sub>nom</sub>) - V/(0.8 V<sub>nom</sub><sup>2</sup>))</td>
+<td>V &lt; 8/9&sdot; V<sub>nom</sub></td>
+</tr>
+
+<tr>
+<td>i &#8771; P<sub>LOAD</sub> (2/(1.2  V<sub>nom</sub>) - V/(1.2 V<sub>nom</sub><sup>2</sup>))</td>
+<td>V &ge; 12/11&sdot; V<sub>nom</sub></td>
+</tr>
+
+<tr>
+<td>i &#8771; P<sub>LOAD</sub> (2/V<sub>nom</sub> - V/V<sub>nom</sub><sup>2</sup>)</td>
+<td>Otherwise</td>
+</tr>
+</table>
+
+</html>", revisions="<html>
+<ul>
+<li>May 14, 2015, by Marco Bonvini:<br/>
+Changed parent class to <a href=\"modelica://Buildings.Electrical.Interfaces.ResistiveLoad\">
+AixLib.Electrical.Interfaces.ResistiveLoad</a> in order
+to help openmodelica parsing the model. This fixes issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/415\">#415</a>.
+</li>
+<li>June 17, 2014, by Marco Bonvini:<br/>
+Adde parameter <code>initMode</code> that can be used to
+select the assumption to be used during initialization phase
+by the homotopy operator.
+</li>
+<li>
+February 1, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+<li>
+January 2014, by Marco Bonvini:<br/>
+Added linearized version of the model.
+</li>
+<li>
+May 28, 2014, by Marco Bonvini:<br/>
+Added and revised documentation.
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(
+        preserveAspectRatio=true,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+          Rectangle(
+            extent={{-70,30},{70,-30}},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid,
+            lineColor={0,0,255}),
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,255}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Text(
+            extent={{-152,87},{148,47}},
+            textColor={0,0,0},
+          textString="%name"),
+          Text(
+            extent={{-144,-38},{142,-70}},
+            textColor={0,0,0},
+            textString="G=%G")}),
+    Diagram(coordinateSystem(
+        preserveAspectRatio=false,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+          Line(points={{-96,0},{-70,0}}, color={0,0,255}),
+          Line(points={{70,0},{96,0}}, color={0,0,255}),
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Conductor;
diff --git a/AixLib/Electrical/DC/Loads/Examples/LinearizedLoad.mo b/AixLib/Electrical/DC/Loads/Examples/LinearizedLoad.mo
new file mode 100644
index 0000000000..fd007e45f4
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/Examples/LinearizedLoad.mo
@@ -0,0 +1,105 @@
+within AixLib.Electrical.DC.Loads.Examples;
+model LinearizedLoad "Example model to check the linearized load model"
+  extends Modelica.Icons.Example;
+  Real error = (sen_nlin.P - sen_lin.P)*100/sen_nlin.P
+    "Percentage of error between the linearized and actual power consumption";
+  Real deltaV = LinearLoad.V_nominal - sen_lin.V
+    "Voltage distance between nominal condition and actual voltage";
+  AixLib.Electrical.DC.Loads.Conductor NonlinearLoad(
+    linearized=false,
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=100,
+    P_nominal=0) "Nonlinear load model"
+    annotation (Placement(transformation(extent={{30,-40},{50,-20}})));
+  Sources.ConstantVoltage sou(V=100) "Voltage source"
+    annotation (Placement(transformation(extent={{-90,-10},{-70,10}})));
+  Modelica.Electrical.Analog.Basic.Ground gro "Ground"
+    annotation (Placement(transformation(extent={{-100,-32},{-80,-12}})));
+  Lines.TwoPortResistance Rline1(R=2) "Line resistance"
+    annotation (Placement(transformation(extent={{-50,-40},{-30,-20}})));
+  Sensors.GeneralizedSensor sen_nlin "Sensor"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  AixLib.Electrical.DC.Loads.Conductor LinearLoad(
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input,
+    V_nominal=100,
+    linearized=true,
+    P_nominal=0) "Linearized load model"
+    annotation (Placement(transformation(extent={{30,20},{50,40}})));
+  Sensors.GeneralizedSensor sen_lin "Sensor"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  Lines.TwoPortResistance Rline2(R=2) "Line resistance"
+    annotation (Placement(transformation(extent={{-50,20},{-30,40}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=0.5,
+    startTime=0.2,
+    offset=-50,
+    height=-950) "Power consumption"
+    annotation (Placement(transformation(extent={{90,-10},{70,10}})));
+equation
+  connect(sou.terminal, Rline1.terminal_n)
+                                      annotation (Line(
+      points={{-70,0},{-60,0},{-60,-30},{-50,-30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(Rline1.terminal_p, sen_nlin.terminal_n)
+                                          annotation (Line(
+      points={{-30,-30},{-10,-30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen_nlin.terminal_p, NonlinearLoad.terminal)
+                                         annotation (Line(
+      points={{10,-30},{30,-30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(LinearLoad.terminal, sen_lin.terminal_p)
+                                          annotation (Line(
+      points={{30,30},{10,30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sou.n, gro.p) annotation (Line(
+      points={{-90,0},{-90,-12}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sou.terminal, Rline2.terminal_n) annotation (Line(
+      points={{-70,0},{-60,0},{-60,30},{-50,30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(Rline2.terminal_p, sen_lin.terminal_n)
+                                              annotation (Line(
+      points={{-30,30},{-10,30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(LinearLoad.Pow, ramp.y) annotation (Line(
+      points={{50,30},{60,30},{60,6.66134e-16},{69,6.66134e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(NonlinearLoad.Pow, ramp.y) annotation (Line(
+      points={{50,-30},{60,-30},{60,6.66134e-16},{69,6.66134e-16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (            experiment(StopTime=1.0, Tolerance=1e-06),
+            __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/LinearizedLoad.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>This example demonstrates the use of a linealized load model <a href=\"modelica://AixLib.Electrical.DC.Loads.Conductor\">AixLib.Electrical.DC.Loads.Conductor</a>. </p>
+<p>Both loads are connected to the same DC voltage source through a resistive element that represents a line. The loads consume the same amount of power that is specified by the input ramp signal. </p>
+<p>The nonlinear conductor model <code>NonlinearLoad</code> consumes exactly the amount of power specified by the input <code>NonlinearLoad.Pow</code>. </p>
+<p>The linearized conductor model <code>LinearizedLoad</code> does not consumes the amount of power specified by the input <code>LinearizedLoad.Pow</code>. The voltage at the load deviates from the nominal value when the power consumption increases. Since the model is approximated in a neighbor of the nominal voltage, moving from that point introduces approximation errors. The plot below shows the error introduced with such an approximation. </p>
+<p align=\"center\"><img src=\"modelica://AixLib/Resources/Images/Electrical/DC/Loads/Examples/DCload_approx.png\" alt=\"image\"/> </p>
+<p>The linearized load is tested over a voltage variation of about 30 % of the nominal voltage and within this range
+the maximum error is 1.23457 % that occurs when the voltage deviation is 11.11 %.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 2, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+August 16, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end LinearizedLoad;
diff --git a/AixLib/Electrical/DC/Loads/Examples/Resistor.mo b/AixLib/Electrical/DC/Loads/Examples/Resistor.mo
new file mode 100644
index 0000000000..62e254b83e
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/Examples/Resistor.mo
@@ -0,0 +1,61 @@
+within AixLib.Electrical.DC.Loads.Examples;
+model Resistor "Example model for resistor"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.DC.Loads.Resistor res2(R=2, V_nominal=12) "Resistor"
+    annotation (Placement(transformation(extent={{40,20},{60,40}})));
+  Sources.ConstantVoltage sou(V=12) "Voltage source"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  Modelica.Electrical.Analog.Basic.Ground gro "Ground"
+    annotation (Placement(transformation(extent={{-90,-2},{-70,18}})));
+  Lines.TwoPortResistance res(R=2) "Line resistance"
+    annotation (Placement(transformation(extent={{-40,20},{-20,40}})));
+  Sensors.GeneralizedSensor sen "Sensor"
+    annotation (Placement(transformation(extent={{0,20},{20,40}})));
+  AixLib.Electrical.DC.Loads.Resistor res1(R=2, V_nominal=12) "Resistor"
+    annotation (Placement(transformation(extent={{40,50},{60,70}})));
+  Sensors.GeneralizedSensor sen1 "Sensor"
+    annotation (Placement(transformation(extent={{0,50},{20,70}})));
+equation
+  connect(sou.terminal, res.terminal_n)
+                                      annotation (Line(
+      points={{-60,30},{-40,30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(res.terminal_p, sen.terminal_n) annotation (Line(
+      points={{-20,30},{0,30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen.terminal_p,res2. terminal) annotation (Line(
+      points={{20,30},{40,30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(res1.terminal, sen1.terminal_p) annotation (Line(
+      points={{40,60},{20,60}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen1.terminal_n, res.terminal_n) annotation (Line(
+      points={{0,60},{-40,60},{-40,30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sou.n, gro.p) annotation (Line(
+      points={{-80,30},{-80,18}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation (            experiment(StopTime=1.0, Tolerance=1e-06),
+            __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/Resistor.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example demonstrates the use of the resistor model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 16, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Resistor;
diff --git a/AixLib/Electrical/DC/Loads/Examples/VariableLoad.mo b/AixLib/Electrical/DC/Loads/Examples/VariableLoad.mo
new file mode 100644
index 0000000000..25fb47a505
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/Examples/VariableLoad.mo
@@ -0,0 +1,101 @@
+within AixLib.Electrical.DC.Loads.Examples;
+model VariableLoad "Example using variable loads models"
+  extends Modelica.Icons.Example;
+  Conductor loa1(
+    V_nominal=12,
+    linearized=false,
+    P_nominal=-50) "Load"
+    annotation (Placement(transformation(extent={{40,40},{60,60}})));
+  Sources.ConstantVoltage sou(V=12) "Voltage source"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  Modelica.Electrical.Analog.Basic.Ground gro "Ground"
+    annotation (Placement(transformation(extent={{-90,-2},{-70,18}})));
+  Conductor loa2(              mode=Types.Load.VariableZ_y_input,
+    V_nominal=12,
+    P_nominal=-50) "Load"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Modelica.Blocks.Sources.Ramp varLoad_y(
+    height=0.8,
+    duration=0.5,
+    startTime=0.3,
+    offset=0) "Power signal"
+    annotation (Placement(transformation(extent={{60,0},{40,20}})));
+  Conductor loa3(
+    V_nominal=12,
+    P_nominal=0,
+    mode=AixLib.Electrical.Types.Load.VariableZ_P_input) "Load"
+    annotation (Placement(transformation(extent={{0,-40},{20,-20}})));
+  Modelica.Blocks.Sources.Ramp varLoad_P(
+    duration=0.5,
+    startTime=0.3,
+    height=120,
+    offset=-20) "Power signal"
+    annotation (Placement(transformation(extent={{60,-40},{40,-20}})));
+  Lines.TwoPortResistance res(R=0.1) "Line resistance"
+    annotation (Placement(transformation(extent={{-32,40},{-12,60}})));
+  Sensors.GeneralizedSensor sen "Sensor"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+equation
+  connect(sou.terminal, loa2.terminal)
+                                      annotation (Line(
+      points={{-60,30},{-40,30},{-40,10},{-4.44089e-16,10}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(varLoad_y.y, loa2.y)  annotation (Line(
+      points={{39,10},{20,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou.terminal, loa3.terminal)
+                                      annotation (Line(
+      points={{-60,30},{-40,30},{-40,-30},{-4.44089e-16,-30}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(varLoad_P.y, loa3.Pow)  annotation (Line(
+      points={{39,-30},{20,-30}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou.terminal, res.terminal_n)
+                                      annotation (Line(
+      points={{-60,30},{-40,30},{-40,50},{-32,50}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(res.terminal_p, sen.terminal_n) annotation (Line(
+      points={{-12,50},{0,50}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, loa1.terminal) annotation (Line(
+      points={{20,50},{40,50}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sou.n, gro.p) annotation (Line(
+      points={{-80,30},{-80,18}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation (            experiment(StopTime=1.0, Tolerance=1e-06),
+            __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/VariableLoad.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example shows how to use three different types of load models.
+Each load is of type <a href=\"modelica://AixLib.Electrical.DC.Loads.Conductor\">
+AixLib.Electrical.DC.Loads.Conductor</a>.
+</p>
+<p>
+The first load <code>loa1</code>consumes a constant amount of power.
+The second and the third loads (<code>loa2</code> and <code>loa3</code>) consume a variable amount of power.
+The load <code>loa2</code> has a variable input <code>y</code> between 0 and 1 that specifies the portion of
+nominal power that is consumed.
+The load <code>loa3</code> has a variable input <code>Pow</code> that represents the actual power consumed
+(or produced) by the load.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 2, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end VariableLoad;
diff --git a/AixLib/Electrical/DC/Loads/Examples/package.mo b/AixLib/Electrical/DC/Loads/Examples/package.mo
new file mode 100644
index 0000000000..8187653357
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Electrical.DC.Loads;
+package Examples "Package with example models"
+extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.DC.Loads\">
+AixLib.Electrical.DC.Loads</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/DC/Loads/Examples/package.order b/AixLib/Electrical/DC/Loads/Examples/package.order
new file mode 100644
index 0000000000..815b57469d
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/Examples/package.order
@@ -0,0 +1,3 @@
+LinearizedLoad
+Resistor
+VariableLoad
diff --git a/AixLib/Electrical/DC/Loads/Resistor.mo b/AixLib/Electrical/DC/Loads/Resistor.mo
new file mode 100644
index 0000000000..48f3cd7ef3
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/Resistor.mo
@@ -0,0 +1,98 @@
+within AixLib.Electrical.DC.Loads;
+model Resistor "Ideal linear electrical resistor"
+  extends AixLib.Electrical.Interfaces.ResistiveLoad(
+    redeclare package PhaseSystem = PhaseSystems.TwoConductor,
+    redeclare Interfaces.Terminal_n terminal,
+    final mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    final P_nominal=V_nominal^2/max(R, Modelica.Constants.small));
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort(T = T_ref);
+  parameter Modelica.Units.SI.Resistance R(start=1)
+    "Resistance at temperature T_ref";
+  parameter Modelica.Units.SI.Temperature T_ref=300.15 "Reference temperature";
+  parameter Modelica.Units.SI.LinearTemperatureCoefficient alpha=0
+    "Temperature coefficient of resistance (R_actual = R*(1 + alpha*(T_heatPort - T_ref))";
+  Modelica.Units.SI.Resistance R_actual
+    "Actual resistance = R*(1 + alpha*(T_heatPort - T_ref))";
+equation
+  assert((1 + alpha*(T_heatPort - T_ref)) >= Modelica.Constants.eps, "Temperature outside of scope of model");
+  R_actual = R*(1 + alpha*(T_heatPort - T_ref));
+  PhaseSystem.systemVoltage(v) = R_actual*PhaseSystem.systemCurrent(i);
+  LossPower = PhaseSystem.activePower(v,i);
+  sum(i) = 0;
+  annotation (
+    Documentation(info="<html>
+<p>
+Model of a linear DC resistor that can vary with respect to temperature.
+</p>
+<p>
+The model implements the Ohm's law
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+V = R(T) i.
+</p>
+<p>
+The resistance <i>R(T)</i> varies depending on the temperature <i>T</i> as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+R(T) = R (1 + &alpha; (T - T<sub>ref</sub>)),
+</p>
+<p>
+where the resistance <i>R</i> is the reference value of the resistance, <i>&alpha;</i> is the
+linear temperature coefficient, and <i>T<sub>ref</sub></i> is the reference temperature.
+The temperature <i>T</i> is the temperature of the heat port if <code>useHeatPort = true</code>.
+</p>
+</html>",
+ revisions="<html>
+<ul>
+<li>November 3, 2015, by Michael Wetter:<br/>
+Set default value for <code>P_nominal</code> to avoid an error when translating
+the model in Dymola's pedantic mode.
+</li>
+<li>May 14, 2015, by Marco Bonvini:<br/>
+Changed parent class to <a href=\"modelica://Buildings.Electrical.Interfaces.ResistiveLoad\">
+AixLib.Electrical.Interfaces.ResistiveLoad</a> in order
+to help openmodelica parsing the model. This fixes issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/415\">#415</a>.
+</li>
+<li>
+February 1, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+<li>
+May 28, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(
+        preserveAspectRatio=true,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+          Rectangle(
+            extent={{-70,30},{70,-30}},
+            lineColor={0,0,255},
+            fillColor={255,255,255},
+            fillPattern=FillPattern.Solid),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Text(
+            extent={{-144,-40},{142,-72}},
+            textColor={0,0,0},
+          textString="R=%R"),
+          Line(
+            visible=useHeatPort,
+            points={{0,-100},{0,-30}},
+            color={127,0,0},
+            smooth=Smooth.None,
+            pattern=LinePattern.Dot),
+          Text(
+            extent={{-152,87},{148,47}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Diagram(coordinateSystem(
+        preserveAspectRatio=true,
+        extent={{-100,-100},{100,100}},
+        grid={2,2}), graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,255}),
+          Line(points={{-96,0},{-70,0}}, color={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Resistor;
diff --git a/AixLib/Electrical/DC/Loads/package.mo b/AixLib/Electrical/DC/Loads/package.mo
new file mode 100644
index 0000000000..d9a11b1c64
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Electrical.DC;
+package Loads "Package with models for DC electrical loads"
+  extends Modelica.Icons.VariantsPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models that represent different types of DC loads.
+</p>
+</html>"));
+end Loads;
diff --git a/AixLib/Electrical/DC/Loads/package.order b/AixLib/Electrical/DC/Loads/package.order
new file mode 100644
index 0000000000..7e5a266009
--- /dev/null
+++ b/AixLib/Electrical/DC/Loads/package.order
@@ -0,0 +1,3 @@
+Conductor
+Resistor
+Examples
diff --git a/AixLib/Electrical/DC/Sensors/Examples/GeneralizedSensor.mo b/AixLib/Electrical/DC/Sensors/Examples/GeneralizedSensor.mo
new file mode 100644
index 0000000000..19f0bbda71
--- /dev/null
+++ b/AixLib/Electrical/DC/Sensors/Examples/GeneralizedSensor.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.DC.Sensors.Examples;
+model GeneralizedSensor "Example model for generalized sensor"
+  extends Modelica.Icons.Example;
+  AixLib.Electrical.DC.Sensors.GeneralizedSensor sen "Power sensor"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  AixLib.Electrical.DC.Loads.Conductor loa(V_nominal=120, P_nominal=120)
+    "Constant load"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+  AixLib.Electrical.DC.Sources.ConstantVoltage sou(V=120) "Voltage source"
+    annotation (Placement(transformation(extent={{-50,-10},{-30,10}})));
+  Modelica.Electrical.Analog.Basic.Ground ground
+    annotation (Placement(transformation(extent={{-60,-32},{-40,-12}})));
+equation
+  connect(sen.terminal_p, loa.terminal)
+    annotation (Line(points={{10,0},{40,0}},            smooth=Smooth.None));
+  connect(sen.terminal_n, sou.terminal)
+    annotation (Line(points={{-10,0},{-30,0}},   smooth=Smooth.None));
+  connect(sou.n, ground.p) annotation (Line(
+      points={{-50,0},{-50,-12}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  annotation ( experiment(StopTime=1.0,Tolerance=1e-06),
+  Documentation(
+  info="<html>
+<p>
+This example illustrates the use of the generalized sensor.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+July 24, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+__Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Sensors/Examples/GeneralizedSensor.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor;
diff --git a/AixLib/Electrical/DC/Sensors/Examples/package.mo b/AixLib/Electrical/DC/Sensors/Examples/package.mo
new file mode 100644
index 0000000000..d3cef743d2
--- /dev/null
+++ b/AixLib/Electrical/DC/Sensors/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Electrical.DC.Sensors;
+package Examples "Collection of models that illustrate model use and test models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.DC.Sensors\">
+AixLib.Electrical.DC.Sensors</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/DC/Sensors/Examples/package.order b/AixLib/Electrical/DC/Sensors/Examples/package.order
new file mode 100644
index 0000000000..b638efa963
--- /dev/null
+++ b/AixLib/Electrical/DC/Sensors/Examples/package.order
@@ -0,0 +1 @@
+GeneralizedSensor
diff --git a/AixLib/Electrical/DC/Sensors/GeneralizedSensor.mo b/AixLib/Electrical/DC/Sensors/GeneralizedSensor.mo
new file mode 100644
index 0000000000..4a551f91f2
--- /dev/null
+++ b/AixLib/Electrical/DC/Sensors/GeneralizedSensor.mo
@@ -0,0 +1,86 @@
+within AixLib.Electrical.DC.Sensors;
+model GeneralizedSensor "Sensor for power, voltage and current"
+  extends AixLib.Electrical.Icons.GeneralizedSensor;
+  extends AixLib.Electrical.Interfaces.PartialTwoPort(
+    redeclare package PhaseSystem_p = PhaseSystems.TwoConductor,
+    redeclare package PhaseSystem_n = PhaseSystems.TwoConductor,
+    redeclare Interfaces.Terminal_n terminal_n,
+    redeclare Interfaces.Terminal_p terminal_p);
+  Modelica.Blocks.Interfaces.RealOutput V(final quantity="ElectricPotential",
+                                          final unit="V") "Voltage"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-50}),   iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-90})));
+  Modelica.Blocks.Interfaces.RealOutput I(final quantity="ElectricCurrent",
+                                          final unit="A") "Current"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-50}), iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-90})));
+  Modelica.Blocks.Interfaces.RealOutput P(
+    final quantity="Power",
+    final unit="W") "Power" annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-60,-50}), iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-60,-90})));
+equation
+  Connections.branch(terminal_p.theta, terminal_n.theta);
+  terminal_p.theta = terminal_n.theta;
+
+  V = AixLib.Electrical.PhaseSystems.TwoConductor.systemVoltage(terminal_n.v);
+  I = AixLib.Electrical.PhaseSystems.TwoConductor.systemCurrent(terminal_n.i);
+  P = AixLib.Electrical.PhaseSystems.TwoConductor.activePower(v=terminal_n.v, i=terminal_n.i);
+
+  connect(terminal_n, terminal_p) annotation (Line(
+      points={{-100,0},{100,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+
+  annotation (defaultComponentName="sen",
+  Documentation(info="<html>
+<p>
+Ideal sensor that measures power, voltage and current.
+The two components of the power <i>S</i> are the active and reactive power.
+As this sensor is configured to measure DC power, the reactive power is always zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 12, 2019, by Michael Wetter:<br/>
+Removed wrong use of <code>each</code>.
+</li>
+<li>
+March 19, 2015, by Michael Wetter:<br/>
+Removed redeclaration of phase system in <code>Terminal_n</code> and
+<code>Terminal_p</code> as it is already declared to the be the same
+phase system, and it is not declared to be replaceable.
+This avoids a translation error in OpenModelica.
+</li>
+<li>
+July 24, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Icon(graphics={
+        Text(
+          extent={{-120,-42},{0,-82}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="P")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor;
diff --git a/AixLib/Electrical/DC/Sensors/package.mo b/AixLib/Electrical/DC/Sensors/package.mo
new file mode 100644
index 0000000000..d6385104ae
--- /dev/null
+++ b/AixLib/Electrical/DC/Sensors/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Electrical.DC;
+package Sensors "Package with sensors for DC electrical systems"
+extends Modelica.Icons.SensorsPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models for sensors for DC circuits.
+</p>
+</html>"));
+end Sensors;
diff --git a/AixLib/Electrical/DC/Sensors/package.order b/AixLib/Electrical/DC/Sensors/package.order
new file mode 100644
index 0000000000..2923d15c82
--- /dev/null
+++ b/AixLib/Electrical/DC/Sensors/package.order
@@ -0,0 +1,2 @@
+GeneralizedSensor
+Examples
diff --git a/AixLib/Electrical/DC/Sources/BaseClasses/WindCorrection.mo b/AixLib/Electrical/DC/Sources/BaseClasses/WindCorrection.mo
new file mode 100644
index 0000000000..1d030f83ac
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/BaseClasses/WindCorrection.mo
@@ -0,0 +1,76 @@
+within AixLib.Electrical.DC.Sources.BaseClasses;
+block WindCorrection "Block for wind correction"
+  extends Modelica.Blocks.Icons.Block;
+  parameter Modelica.Units.SI.Height h "Height over ground";
+  parameter Modelica.Units.SI.Height hRef
+    "Reference height for wind measurement";
+  parameter Real n(min=0) = 0.4 "Height exponent for wind profile calculation";
+  Modelica.Blocks.Interfaces.RealOutput vLoc( unit="m/s")
+    "Wind velocity at the location"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  Modelica.Blocks.Interfaces.RealInput vRef(unit="m/s")
+    "Wind velocity at the reference height"
+    annotation (Placement(transformation(extent={{-120,-10},{-100,10}}),
+        iconTransformation(extent={{-142,-20},{-102,20}})));
+equation
+  vLoc=vRef * (h / hRef)^n;
+  annotation (
+  defaultComponentName = "cor",
+  Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+       graphics={
+        Text(
+          extent={{-92,48},{-32,-50}},
+          textColor={0,128,255},
+          fillColor={85,170,255},
+          fillPattern=FillPattern.Solid,
+          textString="vRef"),
+        Polygon(
+          points={{26,0},{6,20},{6,10},{-24,10},{-24,-10},{6,-10},{6,-20},{26,0}},
+          lineColor={0,128,255},
+          fillColor={85,170,255},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{30,50},{90,-48}},
+          textColor={0,128,0},
+          fillColor={85,170,255},
+          fillPattern=FillPattern.Solid,
+          textString="vLoc")}),Documentation(info="<html>
+<p>
+This model calculates the wind velocity at the location as a function of the height over ground.
+The equation is based on Gash (1991).
+
+The model computes the wind velocity <i>vLoc</i> as
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+vLoc = vRef * (h / hRef)<sup>n</sup>
+</p>
+
+<p>
+where <i>vRef</i> is the wind velocity at the reference height, <i>h</i> is the height over ground, <i>hRef</i>
+is the reference height, and <i>n</i> is the height exponent for wind calculation.
+</p>
+<h4>Reference</h4>
+<p>
+Gasch, R. 1991. Windkraftanlagen. Grundlagen und Entwurf (German). Teubner, Stuttgart.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+June 2, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+<li>
+February 7, 2013, by Michael Wetter:<br/>
+Removed <code>final</code> keyword for parameters to allow users to adjust them,
+and removed default value for <code>h</code>.
+</li>
+<li>
+February 1, 2013, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WindCorrection;
diff --git a/AixLib/Electrical/DC/Sources/BaseClasses/package.mo b/AixLib/Electrical/DC/Sources/BaseClasses/package.mo
new file mode 100644
index 0000000000..ffa1b88a7f
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/BaseClasses/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Electrical.DC.Sources;
+package BaseClasses "Package with base classes for DC sources"
+  extends Modelica.Icons.BasesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains base classes that are used to construct the models in
+<a href=\"modelica://AixLib.Electrical.DC.Sources\">AixLib.Electrical.DC.Sources</a>.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/DC/Sources/BaseClasses/package.order b/AixLib/Electrical/DC/Sources/BaseClasses/package.order
new file mode 100644
index 0000000000..b7efbc807b
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/BaseClasses/package.order
@@ -0,0 +1 @@
+WindCorrection
diff --git a/AixLib/Electrical/DC/Sources/ConstantVoltage.mo b/AixLib/Electrical/DC/Sources/ConstantVoltage.mo
new file mode 100644
index 0000000000..7a10edc4c9
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/ConstantVoltage.mo
@@ -0,0 +1,60 @@
+within AixLib.Electrical.DC.Sources;
+model ConstantVoltage "Model of a constant DC voltage source"
+  extends AixLib.Electrical.Interfaces.Source(
+    redeclare package PhaseSystem = PhaseSystems.TwoConductor,
+    redeclare Interfaces.Terminal_p terminal,
+    final potentialReference=true,
+    final definiteReference=false);
+  parameter Modelica.Units.SI.Voltage V(start=1) "Value of constant voltage";
+  Modelica.Electrical.Analog.Interfaces.NegativePin n "Negative pin"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+equation
+  terminal.v[1] = V;
+  terminal.v[2] = n.v;
+  sum(terminal.i) + n.i = 0;
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Line(points={{-40,0},{40,0}},  color={0,0,0},
+          origin={10,0},
+          rotation=90),
+        Line(points={{0,26},{0,-54}},     color={0,0,0},
+          origin={36,0},
+          rotation=90),
+        Line(points={{0,46},{0,-34}}, color={0,0,0},
+          origin={-44,0},
+          rotation=90),
+        Line(points={{-20,0},{20,0}},
+                                    color={0,0,0},
+          origin={-10,0},
+          rotation=90),
+        Text(
+          extent={{50,70},{150,20}},
+          textColor={0,0,0},
+          textString="+"),
+        Text(
+          extent={{50,-12},{150,-62}},
+          textColor={0,0,0},
+          textString="-"),
+        Text(
+          extent={{-150,60},{150,100}},
+          textColor={0,0,0},
+          textString="V=%V")}),    Documentation(info="<html>
+<p>
+This model represents a simple DC voltage source with constant voltage.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Michael Wetter:<br/>
+Set <code>final potentialReference=true</code> and
+<code>final definiteReference=false</code> as this
+model is for a DC voltage.
+</li>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+Revised documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ConstantVoltage;
diff --git a/AixLib/Electrical/DC/Sources/Examples/VoltageSource.mo b/AixLib/Electrical/DC/Sources/Examples/VoltageSource.mo
new file mode 100644
index 0000000000..ff4c89657c
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/Examples/VoltageSource.mo
@@ -0,0 +1,64 @@
+within AixLib.Electrical.DC.Sources.Examples;
+model VoltageSource "Example for the variable voltage source model"
+  extends Modelica.Icons.Example;
+  Modelica.Electrical.Analog.Basic.Ground ground
+    annotation (Placement(transformation(extent={{-92,-40},{-72,-20}})));
+  AixLib.Electrical.DC.Loads.Resistor res(R=0.5, V_nominal=12)
+    "Resistance"
+    annotation (Placement(transformation(extent={{26,-10},{46,10}})));
+  AixLib.Electrical.DC.Sources.VoltageSource sou "Voltage source"
+    annotation (Placement(transformation(extent={{-82,-10},{-62,10}})));
+  AixLib.Electrical.DC.Lines.TwoPortResistance lin(R=0.5)
+    "Transmission line"
+    annotation (Placement(transformation(extent={{-52,-10},{-32,10}})));
+  AixLib.Electrical.DC.Sensors.GeneralizedSensor sen "Sensor"
+    annotation (Placement(transformation(extent={{-14,-10},{6,10}})));
+  Modelica.Blocks.Sources.Sine cosine(
+    phase=0,
+    f=1,
+    offset=12,
+    amplitude=3) "Variable voltage signal"
+    annotation (Placement(transformation(extent={{-120,-4},{-100,16}})));
+equation
+  connect(lin.terminal_p, sen.terminal_n) annotation (Line(
+      points={{-32,0},{-14,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sou.n, ground.p) annotation (Line(
+      points={{-82,0},{-82,-20}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sen.terminal_p, res.terminal) annotation (Line(
+      points={{6,0},{26,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(sou.terminal, lin.terminal_n) annotation (Line(
+      points={{-62,0},{-52,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(cosine.y, sou.V_in) annotation (Line(
+      points={{-99,6},{-82,6}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-140,
+            -100},{100,140}}),      graphics),
+    experiment(StopTime=1, Tolerance=1e-6),
+Documentation(info="<html>
+<p>
+This model illustrates the use of the variable voltage source model.
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+October 14, 2012, by Marco Bonvini:<br/>
+Added model and documentation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/DC/Sources/Examples/VoltageSource.mos"
+        "Simulate and plot"),
+    Icon(coordinateSystem(extent={{-140,-100},{100,140}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end VoltageSource;
diff --git a/AixLib/Electrical/DC/Sources/Examples/package.mo b/AixLib/Electrical/DC/Sources/Examples/package.mo
new file mode 100644
index 0000000000..3e6c45e395
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Electrical.DC.Sources;
+package Examples "Package with example models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.DC.Sources\">
+AixLib.Electrical.DC.Sources</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/DC/Sources/Examples/package.order b/AixLib/Electrical/DC/Sources/Examples/package.order
new file mode 100644
index 0000000000..800d45b3d3
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/Examples/package.order
@@ -0,0 +1 @@
+VoltageSource
diff --git a/AixLib/Electrical/DC/Sources/VoltageSource.mo b/AixLib/Electrical/DC/Sources/VoltageSource.mo
new file mode 100644
index 0000000000..602f2b50e2
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/VoltageSource.mo
@@ -0,0 +1,54 @@
+within AixLib.Electrical.DC.Sources;
+model VoltageSource "Model of a generoic DC voltage source"
+  extends AixLib.Electrical.Interfaces.VariableVoltageSource(
+    V(start = 1),
+    redeclare package PhaseSystem = PhaseSystems.TwoConductor,
+    redeclare Interfaces.Terminal_p terminal,
+    final potentialReference=true,
+    final definiteReference=false);
+  Modelica.Electrical.Analog.Interfaces.NegativePin n "Negative pin"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+equation
+  terminal.v[1] = V_in_internal;
+  terminal.v[2] = n.v;
+  sum(terminal.i) + n.i = 0;
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Line(points={{-40,0},{40,0}},  color={0,0,0},
+          origin={10,0},
+          rotation=90),
+        Line(points={{0,26},{0,-54}},     color={0,0,0},
+          origin={36,0},
+          rotation=90),
+        Line(points={{0,46},{0,-34}}, color={0,0,0},
+          origin={-44,0},
+          rotation=90),
+        Line(points={{-20,0},{20,0}},
+                                    color={0,0,0},
+          origin={-10,0},
+          rotation=90),
+        Text(
+          extent={{50,70},{150,20}},
+          textColor={0,0,0},
+          textString="+"),
+        Text(
+          extent={{50,-12},{150,-62}},
+          textColor={0,0,0},
+          textString="-"),
+        Text(visible = not use_V_in,
+          extent={{-150,60},{150,100}},
+          textColor={0,0,0},
+          textString="V=%V")}),    Documentation(info="<html>
+<p>
+This model represents a simple DC voltage source with variable voltage.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 14, 2014, by Marco Bonvini:<br/>
+Added model and documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end VoltageSource;
diff --git a/AixLib/Electrical/DC/Sources/package.mo b/AixLib/Electrical/DC/Sources/package.mo
new file mode 100644
index 0000000000..ad00e3bf3b
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Electrical.DC;
+package Sources "Package with models for DC sources"
+  extends Modelica.Icons.SourcesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models that represent different types of DC sources.
+</p>
+</html>"));
+end Sources;
diff --git a/AixLib/Electrical/DC/Sources/package.order b/AixLib/Electrical/DC/Sources/package.order
new file mode 100644
index 0000000000..44097be245
--- /dev/null
+++ b/AixLib/Electrical/DC/Sources/package.order
@@ -0,0 +1,4 @@
+ConstantVoltage
+VoltageSource
+Examples
+BaseClasses
diff --git a/AixLib/Electrical/DC/package.mo b/AixLib/Electrical/DC/package.mo
new file mode 100644
index 0000000000..386873b3a4
--- /dev/null
+++ b/AixLib/Electrical/DC/package.mo
@@ -0,0 +1,36 @@
+within AixLib.Electrical;
+package DC "Package for analog direct current (DC) electrical circuits"
+  extends Modelica.Icons.Package;
+
+
+  annotation (Documentation(info="<html>
+<p>
+Package with models for direct current (DC) systems.<br/>
+The models contained in this package use the phase system <a href=\"modelica://AixLib.Electrical.PhaseSystems.TwoConductor\">AixLib.Electrical.PhaseSystems.TwoConductor</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 28, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"), Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+          {100,100}}), graphics={
+      Line(
+        points={{-82,20},{58,20}},
+        color={0,0,0},
+        smooth=Smooth.None),
+      Line(
+        points={{-82,-18},{-52,-18},{-42,-18}},
+        color={0,0,0},
+        smooth=Smooth.None),
+      Line(
+        points={{-22,-18},{-2,-18},{-2,-18}},
+        color={0,0,0},
+        smooth=Smooth.None),
+      Line(
+        points={{18,-18},{48,-18},{58,-18}},
+        color={0,0,0},
+        smooth=Smooth.None)}));
+end DC;
diff --git a/AixLib/Electrical/DC/package.order b/AixLib/Electrical/DC/package.order
new file mode 100644
index 0000000000..1c45c7275c
--- /dev/null
+++ b/AixLib/Electrical/DC/package.order
@@ -0,0 +1,6 @@
+Conversion
+Lines
+Loads
+Sensors
+Sources
+Interfaces
diff --git a/AixLib/Electrical/Icons/GeneralizedProbe.mo b/AixLib/Electrical/Icons/GeneralizedProbe.mo
new file mode 100644
index 0000000000..82dd126ed4
--- /dev/null
+++ b/AixLib/Electrical/Icons/GeneralizedProbe.mo
@@ -0,0 +1,50 @@
+within AixLib.Electrical.Icons;
+partial class GeneralizedProbe
+  "Icon representing a generalized probe that measures voltage, and phase angle"
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Rectangle(
+          extent={{-40,30},{40,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          origin={1.77636e-15,-40},
+          rotation=90),
+        Ellipse(
+          extent={{-60,60},{60,-60}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Polygon(
+          points={{-0.48,33.6},{18,28},{18,59.2},{-0.48,33.6}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(points={{-37.6,15.7},{-54,22}},     color={0,0,0}),
+        Line(points={{-22.9,34.8},{-32,50}},     color={0,0,0}),
+        Line(points={{0,60},{0,42}}, color={0,0,0}),
+        Line(points={{22.9,34.8},{32,50}},     color={0,0,0}),
+        Line(points={{37.6,15.7},{54,24}},     color={0,0,0}),
+        Line(points={{0,2},{9.02,30.6}}, color={0,0,0}),
+        Ellipse(
+          extent={{-5,7},{5,-3}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+                              Text(
+          extent={{-140,110},{140,70}},
+          textColor={0,0,0},
+          textString="%name")}),    Documentation(info="<html>
+<p>
+This is the icon for a probe that measure voltage magnitude and phase.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedProbe;
diff --git a/AixLib/Electrical/Icons/GeneralizedSensor.mo b/AixLib/Electrical/Icons/GeneralizedSensor.mo
new file mode 100644
index 0000000000..8303bf516c
--- /dev/null
+++ b/AixLib/Electrical/Icons/GeneralizedSensor.mo
@@ -0,0 +1,69 @@
+within AixLib.Electrical.Icons;
+partial class GeneralizedSensor
+  "Icon representing a generalized sensor that measures voltage, current and power"
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Rectangle(
+          extent={{-70,28},{70,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-60,60},{60,-60}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-92,0},{-70,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Polygon(
+          points={{-0.48,33.6},{18,28},{18,59.2},{-0.48,33.6}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(points={{-37.6,15.7},{-54,22}},     color={0,0,0}),
+        Line(points={{-22.9,34.8},{-32,50}},     color={0,0,0}),
+        Line(points={{0,60},{0,42}}, color={0,0,0}),
+        Line(points={{22.9,34.8},{32,50}},     color={0,0,0}),
+        Line(points={{37.6,15.7},{54,24}},     color={0,0,0}),
+        Line(points={{0,2},{9.02,30.6}}, color={0,0,0}),
+        Ellipse(
+          extent={{-5,7},{5,-3}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{70,0},{92,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Text(
+          extent={{-60,-42},{60,-82}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="V"),
+        Text(
+          extent={{0,-40},{120,-80}},
+          textColor={0,0,0},
+          lineThickness=1,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="I"),    Text(
+          extent={{-140,110},{140,70}},
+          textColor={0,0,0},
+          textString="%name")}),    Documentation(info="<html>
+<p>
+This is the icon for ideal sensors that measure power, voltage and current.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 24, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GeneralizedSensor;
diff --git a/AixLib/Electrical/Icons/RefAngleConversion.mo b/AixLib/Electrical/Icons/RefAngleConversion.mo
new file mode 100644
index 0000000000..4d79a40a77
--- /dev/null
+++ b/AixLib/Electrical/Icons/RefAngleConversion.mo
@@ -0,0 +1,46 @@
+within AixLib.Electrical.Icons;
+partial model RefAngleConversion
+  "Icon that represents if the angle symble should be displayed or not"
+  annotation (Icon(graphics={
+        Line(visible = ground_2 == true,
+          points={{80,-40},{120,-40}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = ground_2 == true,
+          points={{80,-40},{106,-14}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = ground_2 == true,
+          points={{102,-16},{114,-24},{118,-42}},
+          color={0,120,120},
+          smooth=Smooth.Bezier),
+        Line(visible = ground_1 == true,
+          points={{-102,-16},{-114,-24},{-118,-42}},
+          color={0,120,120},
+          smooth=Smooth.Bezier),
+        Line(visible = ground_1 == true,
+          points={{-80,-40},{-106,-14}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5),
+        Line(visible = ground_1 == true,
+          points={{-80,-40},{-120,-40}},
+          color={0,120,120},
+          smooth=Smooth.None,
+          thickness=0.5)}), Documentation(info="<html>
+<p>
+This is the icon that conditionally draws the angle symbol for a
+conversion model (e.g., a transformer).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end RefAngleConversion;
diff --git a/AixLib/Electrical/Icons/package.mo b/AixLib/Electrical/Icons/package.mo
new file mode 100644
index 0000000000..ef5ed6f272
--- /dev/null
+++ b/AixLib/Electrical/Icons/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical;
+package Icons "This package contains icons used by the electric models"
+  extends Modelica.Icons.IconsPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+Aug 28, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Package that contains icons.
+</p>
+</html>"));
+end Icons;
diff --git a/AixLib/Electrical/Icons/package.order b/AixLib/Electrical/Icons/package.order
new file mode 100644
index 0000000000..b8b8852717
--- /dev/null
+++ b/AixLib/Electrical/Icons/package.order
@@ -0,0 +1,3 @@
+GeneralizedProbe
+GeneralizedSensor
+RefAngleConversion
diff --git a/AixLib/Electrical/Interfaces/BaseTerminal.mo b/AixLib/Electrical/Interfaces/BaseTerminal.mo
new file mode 100644
index 0000000000..796cf8bfe1
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/BaseTerminal.mo
@@ -0,0 +1,16 @@
+within AixLib.Electrical.Interfaces;
+connector BaseTerminal "Empty connector used by partial models"
+
+  annotation (Documentation(info="<html>
+This empty connector represents the base class extended by every electric connector of type
+<a href=\"modelica://AixLib.Electrical.Interfaces.Terminal\">AixLib.Electrical.Interfaces.Terminal</a>.
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BaseTerminal;
diff --git a/AixLib/Electrical/Interfaces/CapacitiveLoad.mo b/AixLib/Electrical/Interfaces/CapacitiveLoad.mo
new file mode 100644
index 0000000000..d92c3df5a3
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/CapacitiveLoad.mo
@@ -0,0 +1,68 @@
+within AixLib.Electrical.Interfaces;
+partial model CapacitiveLoad "Partial model of a capacitive load"
+  extends Load;
+  parameter Boolean use_pf_in = false "If true, the power factor is defined by an input"
+    annotation(Dialog(group="Modeling assumption"));
+  parameter Real pf(min=0, max=1) = 0.8 "Power factor"
+  annotation(Dialog(group="Nominal conditions"));
+  Modelica.Blocks.Interfaces.RealInput pf_in(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in) "Power factor"
+                   annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={100,60}),  iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={100,60})));
+protected
+  function j = PhaseSystem.j "J operator that rotates of 90 degrees";
+  Modelica.Blocks.Interfaces.RealInput pf_internal
+    "Hidden value of the input load for the conditional connector";
+  Modelica.Units.SI.ElectricCharge q[2](each stateSelect=StateSelect.prefer)
+    "Electric charge";
+  Modelica.Units.SI.Admittance[2] Y "Admittance";
+  Modelica.Units.SI.AngularVelocity omega "Angular velocity";
+  Modelica.Units.SI.Power Q=P*tan(-acos(pf_internal))
+    "Reactive power (negative because capacitive load)";
+equation
+  connect(pf_in, pf_internal);
+
+  if not use_pf_in then
+    pf_internal = pf;
+  end if;
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+June 06, 2014, by Marco Bonvini:<br/>
+Added power factor input <code>pf_in</code> and updated documentation.
+</li>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+Model included into the AixLib library.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a model of a generic capacitive load. This model is an extension of the base load model
+<a href=\"modelica://AixLib.Electrical.Interfaces.Load\">AixLib.Electrical.Interfaces.Load</a>.
+</p>
+<p>
+This model assumes a fixed power factor <code>pf</code> when the flag <code>use_pf_in = false</code>
+otherwise it uses the power factor specified by the input <code>pf_in</code>.
+</p>
+<p>The power factor (either the input or the parameter) is used to compute the reactive power
+<code>Q</code> given the active power <code>P</code>
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q = - P * tan(arccos(pf))
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CapacitiveLoad;
diff --git a/AixLib/Electrical/Interfaces/Ground.mo b/AixLib/Electrical/Interfaces/Ground.mo
new file mode 100644
index 0000000000..3fe206f7fb
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/Ground.mo
@@ -0,0 +1,36 @@
+within AixLib.Electrical.Interfaces;
+model Ground "Generalized model of a ground connection."
+  replaceable package PhaseSystem =
+      AixLib.Electrical.PhaseSystems.PartialPhaseSystem constrainedby
+    AixLib.Electrical.PhaseSystems.PartialPhaseSystem "Phase system"
+    annotation (choicesAllMatching=true);
+
+  replaceable AixLib.Electrical.Interfaces.Terminal terminal(
+    redeclare package PhaseSystem = PhaseSystem) "Generalized terminal"
+    annotation (Placement(transformation(extent={{-8,92},{8,108}}),
+        iconTransformation(extent={{-8,92},{8,108}})));
+equation
+  terminal.v = zeros(PhaseSystem.n);
+  annotation (Documentation(info="<html>
+<p>
+Given a generic electric connector
+<a href=\"modelica://AixLib.Electrical.Interfaces.Terminal\">
+AixLib.Electrical.Interfaces.Terminal</a> this
+model imposes the following condition on the voltage <code>V[PhaseSystem.n]</code>
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+<b>V</b> = <span style=\"text-decoration: overline;\">0</span>,
+</p>
+<p>
+where <span style=\"text-decoration: overline;\">0</span> is a null vector of length <code>PhaseSystem.n</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Ground;
diff --git a/AixLib/Electrical/Interfaces/Impedance.mo b/AixLib/Electrical/Interfaces/Impedance.mo
new file mode 100644
index 0000000000..2654f10286
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/Impedance.mo
@@ -0,0 +1,197 @@
+within AixLib.Electrical.Interfaces;
+model Impedance "Partial model representing a generalized impedance"
+  extends AixLib.Electrical.Interfaces.Load(
+    final linearized = false,
+    final mode=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    final P_nominal(fixed = true)=0,
+    final V_nominal(fixed = true)=1);
+  parameter Boolean inductive=true
+    "If true, the load is inductive, otherwise it is capacitive"
+    annotation (Evaluate=true, choices(
+      choice=true "Inductive",
+      choice=false "Capacitive",
+      __Dymola_radioButtons=true));
+  parameter Modelica.Units.SI.Resistance R(
+    start=1,
+    min=0) = 1 "Resistance" annotation (Dialog(enable=not use_R_in));
+  parameter Modelica.Units.SI.Inductance L(
+    start=0,
+    min=0) = 0 "Inductance"
+    annotation (Dialog(enable=inductive and (not use_L_in)));
+  parameter Modelica.Units.SI.Capacitance C(
+    start=0,
+    min=0) = 0 "Capacitance"
+    annotation (Dialog(enable=(not inductive) and (not use_C_in)));
+  parameter Boolean use_R_in = false "If true, R is specified by an input"
+     annotation(Evaluate=true, Dialog(tab = "Variable load", group="Resistance"));
+  parameter Modelica.Units.SI.Resistance RMin(
+    start=R,
+    min=Modelica.Constants.eps) = 1e-4 "Minimum value of the resistance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_R_in,
+      tab="Variable load",
+      group="Resistance"));
+  parameter Modelica.Units.SI.Resistance RMax(
+    start=R,
+    min=Modelica.Constants.eps) = 1e2 "Maximum value of the resistance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_R_in,
+      tab="Variable load",
+      group="Resistance"));
+  parameter Boolean use_C_in = false "If true, C is specified by an input"
+    annotation(Evaluate=true, Dialog(tab = "Variable load", group="Capacitance"));
+  parameter Modelica.Units.SI.Capacitance CMin(
+    start=C,
+    min=Modelica.Constants.eps) = 1e-4 "Minimum value of the capacitance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_C_in,
+      tab="Variable load",
+      group="Capacitance"));
+  parameter Modelica.Units.SI.Capacitance CMax(
+    start=C,
+    min=Modelica.Constants.eps) = 1e2 "Maximum value of the capacitance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_C_in,
+      tab="Variable load",
+      group="Capacitance"));
+  parameter Boolean use_L_in = false "If true, L is specified by an input"
+     annotation(Evaluate=true, Dialog(tab = "Variable load", group="Inductance"));
+  parameter Modelica.Units.SI.Inductance LMin(
+    start=L,
+    min=Modelica.Constants.eps) = 1e-4 "Minimum value of the inductance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_L_in,
+      tab="Variable load",
+      group="Inductance"));
+  parameter Modelica.Units.SI.Inductance LMax(
+    start=L,
+    min=Modelica.Constants.eps) = 1e2 "Maximum value of the inductance"
+    annotation (Evaluate=true, Dialog(
+      enable=use_L_in,
+      tab="Variable load",
+      group="Inductance"));
+  Modelica.Blocks.Interfaces.RealInput y_R(min=0, max=1) if use_R_in
+    "Input that sepecify variable R"
+    annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=270,
+        origin={-40,100})));
+  Modelica.Blocks.Interfaces.RealInput y_C(min=0, max=1) if use_C_in
+    "Input that sepecify variable C"
+    annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=270,
+        origin={0,100})));
+  Modelica.Blocks.Interfaces.RealInput y_L(min=0, max=1) if use_L_in
+    "Input that sepecify variable L"
+    annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=270,
+        origin={40,100})));
+protected
+  Modelica.Blocks.Interfaces.RealOutput y_R_internal
+    "Internal signal used to compute the variable R_internal";
+  Modelica.Blocks.Interfaces.RealOutput y_C_internal
+    "Internal signal used to compute the variable C_internal";
+  Modelica.Blocks.Interfaces.RealOutput y_L_internal
+    "Internal signal used to compute the variable L_internal";
+  Modelica.Units.SI.Resistance R_internal
+    "Actual resistance used to compute the impedance";
+  Modelica.Units.SI.Inductance L_internal
+    "Actual inductance used to compute the impedance";
+  Modelica.Units.SI.Capacitance C_internal
+    "Actual capacitance used to compute the impedance";
+equation
+  // These assertions ensures that if the variable R, L or C is computed using the inputs
+  // the parameters min and max are sorted
+  assert((not use_R_in) or RMin < RMax, "The value of RMin has to be lower than RMax");
+  assert((not use_L_in) or LMin < LMax, "The value of Lmin has to be lower than Lmax");
+  assert((not use_C_in) or CMin < CMax, "The value of Cmin has to be lower than Cmax");
+
+  // Connections to internal connectors
+  connect(y_R, y_R_internal);
+  connect(y_C, y_C_internal);
+  connect(y_L, y_L_internal);
+
+  // Default assignment when connectors are conditionally removed
+  if not use_R_in then
+    y_R_internal = 0;
+  end if;
+
+  if not use_C_in then
+    y_C_internal = 0;
+  end if;
+
+  if not use_L_in then
+    y_L_internal = 0;
+  end if;
+
+  // Retrieve the value of the R,L,C either if fixed or
+  // varying
+  if not use_R_in then
+    R_internal = R;
+  else
+    R_internal = RMin + y_R_internal*(RMax - RMin);
+  end if;
+
+  if not use_C_in then
+    C_internal = C;
+  else
+    C_internal = CMin + y_C_internal*(CMax - CMin);
+  end if;
+
+  if not use_L_in then
+    L_internal = L;
+  else
+    L_internal = LMin + y_L_internal*(LMax - LMin);
+  end if;
+
+  annotation ( Documentation(info="<html>
+<p>
+This model represents a generalized interface for an impedance.
+</p>
+<p>
+The model has a single generalized electric terminal of type
+<a href=\"modelica://AixLib.Electrical.Interfaces.Terminal\">
+AixLib.Electrical.Interfaces.Terminal</a>
+that can be redeclared.
+The impedance can be of different types:
+</p>
+<ol>
+<li>resistive,</li>
+<li>inductive,</li>
+<li>resistive and inductive,</li>
+<li>capacitive, and</li>
+<li>resistive and capacitive.</li>
+</ol>
+<p>
+The values of the resistance <code>R</code>, capacitance <code>C</code> and
+inductance <code>L</code> can be
+specified as parameters of the model.
+</p>
+<p>
+The values of the resistance <code>R</code>, capacitance <code>C</code>
+and inductance <code>L</code> can also be
+specified by using the input variables <code>y_R</code>, <code>y_C</code>,
+and <code>y_L</code> that are Real values between <i>[0,1]</i>.<br/>
+These input values are enabled by the boolean flags <code>use_R_in</code>,
+<code>use_L_in</code>, and
+<code>use_C_in</code>.
+</p>
+<h5>Example</h5>
+<p>
+If the flag <code>use_R_in = true</code>, the value of <code>R</code> is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+R = R<sub>min</sub> + y<sub>R</sub> (R<sub>max</sub> - R<sub>min</sub>)
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Impedance;
diff --git a/AixLib/Electrical/Interfaces/InductiveLoad.mo b/AixLib/Electrical/Interfaces/InductiveLoad.mo
new file mode 100644
index 0000000000..3bc344825f
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/InductiveLoad.mo
@@ -0,0 +1,80 @@
+within AixLib.Electrical.Interfaces;
+partial model InductiveLoad "Partial model of an inductive load"
+  extends Load;
+  parameter Boolean use_pf_in = false "If true, the power factor is defined by an input"
+    annotation(Dialog(group="Modeling assumption"));
+  parameter Real pf(min=0, max=1) = 0.8 "Power factor"
+  annotation(Dialog(group="Nominal conditions"));
+  Modelica.Blocks.Interfaces.RealInput pf_in(
+    min=0,
+    max=1,
+    unit="1") if (use_pf_in) "Power factor"
+                   annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={100,60}),  iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={100,60})));
+protected
+  function j = PhaseSystem.j "J operator that rotates of 90 degrees";
+  Modelica.Blocks.Interfaces.RealInput pf_internal
+    "Hidden value of the input load for the conditional connector";
+  Modelica.Units.SI.MagneticFlux psi[2](each stateSelect=StateSelect.prefer)
+    "Magnetic flux";
+  Modelica.Units.SI.Impedance Z[2] "Impedance of the load";
+  Modelica.Units.SI.AngularVelocity omega "Angular frequency";
+  Modelica.Units.SI.Power Q=P*tan(acos(
+    AixLib.Utilities.Math.Functions.smoothMin(
+      x1=pf_internal,
+      x2=0.99999,
+      deltaX=0.0000025)))
+    "Reactive power (positive because inductive load)";
+equation
+  connect(pf_in, pf_internal);
+
+  if not use_pf_in then
+    pf_internal = pf;
+  end if;
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+April 4, 2024, by Michael Wetter:<br/>
+Reformulated calculation of reactive power to bound argument of tangent away from &pi;,
+which avoids an infinite function value.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3776\">Buildings, #3776</a>.
+</li>
+<li>
+June 06, 2014, by Marco Bonvini:<br/>
+Added power factor input <code>pf_in</code> and updated documentation.
+</li>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+Model included into the Buildings library.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a model of a generic inductive load. This model is an extension of the base load model
+<a href=\"modelica://AixLib.Electrical.Interfaces.Load\">
+AixLib.Electrical.Interfaces.Load</a>.
+</p>
+<p>
+This model assumes a fixed power factor <code>pf</code> when the flag <code>use_pf_in = false</code>
+otherwise it uses the power factor specified by the input <code>pf_in</code>.
+</p>
+<p>The power factor (either the input or the parameter) is used to compute the reactive power
+<code>Q</code> given the active power <code>P</code>
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q = P  tan(arccos(pf))
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end InductiveLoad;
diff --git a/AixLib/Electrical/Interfaces/Load.mo b/AixLib/Electrical/Interfaces/Load.mo
new file mode 100644
index 0000000000..0fe0fa6248
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/Load.mo
@@ -0,0 +1,257 @@
+within AixLib.Electrical.Interfaces;
+model Load "Partial model for a generic load"
+  replaceable package PhaseSystem =
+      AixLib.Electrical.PhaseSystems.PartialPhaseSystem constrainedby
+    AixLib.Electrical.PhaseSystems.PartialPhaseSystem "Phase system"
+    annotation (choicesAllMatching=true);
+  parameter Boolean linearized = false "If true, the load model is linearized"
+    annotation(Evaluate=true,Dialog(group="Modeling assumption"));
+  parameter AixLib.Electrical.Types.Load mode(
+    min=AixLib.Electrical.Types.Load.FixedZ_steady_state,
+    max=AixLib.Electrical.Types.Load.VariableZ_y_input) = AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Type of load model (e.g., steady state, dynamic, prescribed power consumption, etc.)"
+    annotation (Evaluate=true, Dialog(group="Modeling assumption"));
+
+  parameter Modelica.Units.SI.Power P_nominal=0
+    "Nominal power (negative if consumed, positive if generated). Used if mode <> AixLib.Electrical.Types.Load.VariableZ_P_input"
+    annotation (Dialog(group="Nominal conditions", enable=mode <> AixLib.Electrical.Types.Load.VariableZ_P_input));
+
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=110)
+    "Nominal voltage (V_nominal >= 0)" annotation (Evaluate=true, Dialog(group=
+          "Nominal conditions", enable=(mode == AixLib.Electrical.Types.Load.FixedZ_dynamic
+           or linearized)));
+  parameter AixLib.Electrical.Types.InitMode initMode(
+  min=AixLib.Electrical.Types.InitMode.zero_current,
+  max=AixLib.Electrical.Types.InitMode.linearized) = AixLib.Electrical.Types.InitMode.zero_current
+    "Initialization mode for homotopy operator"  annotation(Dialog(tab = "Initialization"));
+
+  Modelica.Units.SI.Voltage v[:](start=PhaseSystem.phaseVoltages(V_nominal)) =
+    terminal.v "Voltage vector";
+  Modelica.Units.SI.Current i[:](each start=0) = terminal.i "Current vector";
+  Modelica.Units.SI.Power S[PhaseSystem.n]=PhaseSystem.phasePowers_vi(v, -i)
+    "Phase powers";
+  Modelica.Units.SI.Power P(start=0)
+    "Power of the load (negative if consumed, positive if fed into the electrical grid)";
+
+  Modelica.Blocks.Interfaces.RealInput y(min=0, max=1, unit="1")
+    if (mode == AixLib.Electrical.Types.Load.VariableZ_y_input)
+    "Fraction of the nominal power consumed" annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={100,0}), iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={100,0})));
+  Modelica.Blocks.Interfaces.RealInput Pow(unit="W")
+    if (mode == AixLib.Electrical.Types.Load.VariableZ_P_input)
+    "Power consumed" annotation (Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={100,0}), iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=180,
+        origin={100,0})));
+  replaceable AixLib.Electrical.Interfaces.Terminal terminal(
+    redeclare replaceable package PhaseSystem = PhaseSystem)
+    "Generalized electric terminal"
+    annotation (Placement(transformation(extent={{-108,-8},{-92,8}}),
+        iconTransformation(extent={{-108,-8},{-92,8}})));
+
+protected
+  Modelica.Blocks.Interfaces.RealInput y_internal
+    "Hidden value of the input load for the conditional connector";
+  Modelica.Blocks.Interfaces.RealInput P_internal
+    "Hidden value of the input power for the conditional connector";
+  Real load(min=eps, max=1)
+    "Internal representation of control signal, used to avoid singularity";
+  constant Real eps = 1E-10
+    "Small number used to avoid a singularity if the power is zero";
+  constant Real oneEps = 1-eps
+    "Small number used to avoid a singularity if the power is zero";
+
+initial equation
+  if mode == AixLib.Electrical.Types.Load.VariableZ_P_input then
+    assert(abs(P_nominal) < 1E-10, "*** Warning: P_nominal = " + String(P_nominal) + ", but this value will be ignored.",
+           AssertionLevel.warning);
+  end if;
+
+equation
+  assert(y_internal>=0 and y_internal<=1+eps, "The power load fraction P (input of the model) must be within [0,1]");
+
+  // Connection between the conditional and inner connector
+  connect(y,y_internal);
+  connect(Pow,P_internal);
+
+  // If the power is fixed, inner connector value is equal to 1
+  if mode==AixLib.Electrical.Types.Load.FixedZ_steady_state or
+     mode==AixLib.Electrical.Types.Load.FixedZ_dynamic then
+    y_internal   = 1;
+    P_internal = 0;
+  elseif mode==AixLib.Electrical.Types.Load.VariableZ_y_input then
+    P_internal = 0;
+  elseif mode==AixLib.Electrical.Types.Load.VariableZ_P_input then
+    y_internal = 1;
+  end if;
+
+  // Value of the load, depending on the type: fixed or variable
+  if mode==AixLib.Electrical.Types.Load.VariableZ_y_input then
+    load = eps + oneEps*y_internal;
+  else
+    load = 1;
+  end if;
+
+  // Power consumption
+  if mode==AixLib.Electrical.Types.Load.FixedZ_steady_state or
+     mode==AixLib.Electrical.Types.Load.FixedZ_dynamic then
+    P = P_nominal;
+  elseif mode==AixLib.Electrical.Types.Load.VariableZ_P_input then
+    P = P_internal;
+  else
+    P = P_nominal*load;
+  end if;
+
+  annotation ( Documentation(revisions="<html>
+<ul>
+<li>
+January 30, 2019, by Michael Wetter:<br/>
+Set start value for <code>P</code>.
+</li>
+<li>
+November 28, 2016, by Michael Wetter:<br/>
+Removed zero start value for current.
+The current is typically non-zero and zero is anyway the default start value, hence there is no need to set it.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/584\">#584</a>.
+</li>
+<li>
+September 17, 2016, by Michael Wetter:<br/>
+Corrected wrong annotation to avoid an error in the pedantic model check
+in Dymola 2017 FD01 beta2.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/557\">issue 557</a>.
+</li>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Set default value for <code>P_nominal</code>
+and removed assertion warning.
+This is required for pedantic model check in Dymola.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
+</li>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Provided value for <code>P_nominal</code> if
+<code>mode &lt;&gt; AixLib.Electrical.Types.Load.VariableZ_P_input</code>.
+This avoids a warning during translation of
+<a href=\"modelica://AixLib.Examples.ChillerPlant.DataCenterRenewables\">
+AixLib.Examples.ChillerPlant.DataCenterRenewables</a>.
+</li>
+<li>
+September 4, 2014, by Michael Wetter:<br/>
+Changed the parameter from <code>linear</code> to <code>linearized</code>
+because <code>AixLib.Fluid</code> also uses <code>linearized</code>.
+This change has been done to use a consistent naming across the library.
+</li>
+<li>June 17, 2014, by Marco Bonvini:<br/>
+Adde parameter <code>initMode</code> that can be used to
+select the assumption to be used during initialization phase
+by the homotopy operator.
+</li>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation and revised model.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+Model included in the Buildings library.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a generic load that can be extended to represent
+either a DC or an AC load.
+</p>
+<p>
+The model has a single generalized electric terminal of type
+<a href=\"modelica://AixLib.Electrical.Interfaces.Terminal\">
+AixLib.Electrical.Interfaces.Terminal</a>
+that can be redeclared.
+The generalized load is modeled as an impedance whose value can change. The value of the impedance
+can change depending on the value of the parameter <code>mode</code>, which is of type
+<a href=\"modelica://AixLib.Electrical.Types.Load\">AixLib.Electrical.Types.Load</a>:
+</p>
+
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<th>Mode</th>
+<th>Description</th>
+<th>Explanation</th>
+</tr>
+<!-- ************ -->
+<tr>
+<td>AixLib.Electrical.Types.Load.FixedZ_steady_state</td>
+<td>fixed Z steady state</td>
+<td>The load consumes exactly the power
+specified by the parameter <code>P_nominal</code>.
+</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>AixLib.Electrical.Types.Load.FixedZ_dynamic</td>
+<td>fixed Z dynamic</td>
+<td>
+The load consumes exactly the power
+specified by the parameter <code>P_nominal</code> at steady state.
+Depending on the type
+of load (e.g., inductive or capacitive)
+different dynamics are represented.
+</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>AixLib.Electrical.Types.Load.VariableZ_P_input</td>
+<td>variable Z P input</td>
+<td>
+The load consumes exactly the power specified
+by the input variable <code>Pow</code>.
+</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>AixLib.Electrical.Types.Load.VariableZ_y_input</td>
+<td>variable Z y input</td>
+<td>
+The load consumes exactly the a fraction of the nominal power
+<code>P_nominal</code> specified by the input variable <code>y</code>.
+</td>
+</tr>
+<!-- ************ -->
+</table>
+
+
+<h4>Conventions</h4>
+<p>
+It is assumed that the power <code>P</code> of the load is positive when produced
+(e.g., the load acts like a source) and negative when consumed (e.g., the
+source acts like a utilizer).
+</p>
+
+<h4>Linearized models</h4>
+<p>
+The model has a Boolean parameter <code>linearized</code> that by default is equal to <code>false</code>.
+When the power consumption of the load is imposed, this introduces
+a nonlinear equation between the voltage and the current of the load. This flag is used to
+select between a linearized version
+of the equations or the original nonlinear ones.<br/>
+When the linearized version of the model is used, the parameter <code>V_nominal</code> has to
+be specified. The nominal voltage is needed to linearize the nonlinear equations.<br/>
+</p>
+<p>
+<b>Note:</b>
+A linearized model will not consume the nominal power if the voltage
+at the terminal differs from the nominal voltage.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Load;
diff --git a/AixLib/Electrical/Interfaces/PartialAcDcParameters.mo b/AixLib/Electrical/Interfaces/PartialAcDcParameters.mo
new file mode 100644
index 0000000000..31db4d73cb
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/PartialAcDcParameters.mo
@@ -0,0 +1,22 @@
+within AixLib.Electrical.Interfaces;
+record PartialAcDcParameters
+  "Partial model that contains basic parameters for a DC/AC conversion system"
+  parameter Real pf(min=0, max=1) = 0.9 "Power factor"
+    annotation (Dialog(group="AC-Conversion"));
+  parameter Real eta_DCAC(min=0, max=1) = 0.9 "Efficiency of DC/AC conversion"
+    annotation (Dialog(group="AC-Conversion"));
+  annotation (Documentation(info="<html>
+<p>
+This model contains the minimum set of parameters necessary to describe
+an AC/DC converter.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2014, by Marco Bonvini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialAcDcParameters;
diff --git a/AixLib/Electrical/Interfaces/PartialBaseTwoPort.mo b/AixLib/Electrical/Interfaces/PartialBaseTwoPort.mo
new file mode 100644
index 0000000000..7156bc9222
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/PartialBaseTwoPort.mo
@@ -0,0 +1,24 @@
+within AixLib.Electrical.Interfaces;
+model PartialBaseTwoPort "Model of a generic two port component"
+
+  replaceable AixLib.Electrical.Interfaces.BaseTerminal terminal_n
+    "Electric terminal side p"
+    annotation (Placement(transformation(extent={{-108,-8},{-92,8}})));
+  replaceable AixLib.Electrical.Interfaces.BaseTerminal terminal_p
+    "Electric terminal side n"
+    annotation (Placement(transformation(extent={{92,-8},{108,8}})));
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model declares connectors for electrical components with two terminals.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialBaseTwoPort;
diff --git a/AixLib/Electrical/Interfaces/PartialConversion.mo b/AixLib/Electrical/Interfaces/PartialConversion.mo
new file mode 100644
index 0000000000..56f7e38955
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/PartialConversion.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Interfaces;
+model PartialConversion
+  "Model representing a generic two port system for conversion"
+  extends AixLib.Electrical.Interfaces.PartialTwoPort;
+  Modelica.Units.SI.Voltage v_p "Voltage drop between the two positive pins";
+  Modelica.Units.SI.Voltage v_n "Voltage drop between the two negative pins";
+  Modelica.Units.SI.Current i_p "Current flowing through the positive pins";
+  Modelica.Units.SI.Current i_n "Current flowing through the negative pins";
+equation
+  i_p = PhaseSystem_p.systemCurrent(terminal_p.i);
+  i_n = PhaseSystem_n.systemCurrent(terminal_n.i);
+
+  v_p = PhaseSystem_p.systemVoltage(terminal_p.v);
+  v_n = PhaseSystem_n.systemVoltage(terminal_n.v);
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+Model included in the AixLib library.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model extends the base class
+<a href=\"modelica://AixLib.Electrical.Interfaces.PartialTwoPort\">
+AixLib.Electrical.Interfaces.PartialTwoPort</a>
+model and declares the variables
+<code>v_p</code> and <code>i_p</code> that represents the voltage and the
+current at the <code>terminal_p</code>, and the variables
+<code>v_n</code> and <code>i_n</code> that represents the voltage and the
+current at the <code>terminal_n</code>.
+These variables are used in conversion models such as transformers and AC/DC converters.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialConversion;
diff --git a/AixLib/Electrical/Interfaces/PartialPluggableUnbalanced.mo b/AixLib/Electrical/Interfaces/PartialPluggableUnbalanced.mo
new file mode 100644
index 0000000000..5a3d62da3d
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/PartialPluggableUnbalanced.mo
@@ -0,0 +1,25 @@
+within AixLib.Electrical.Interfaces;
+record PartialPluggableUnbalanced "Partial interface for unbalanced loads"
+  parameter Boolean plugPhase1 = true "If true, phase 1 is connected";
+  parameter Boolean plugPhase2 = true "If true, phase 2 is connected";
+  parameter Boolean plugPhase3 = true "If true, phase 3 is connected";
+  annotation (Documentation(info="<html>
+<p>
+This record contains a set of parameters that are used when
+modeling three-phase unbalanced systems. The record contains three boolean flags
+that are used to determine which of the three-phase are connected to the network.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Changed <code>PlugPhase*</code> to <code>plugPhase*</code>.
+</li>
+<li>
+June 4, 2014, by Marco Bonvini:<br/>
+Added the information section.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialPluggableUnbalanced;
diff --git a/AixLib/Electrical/Interfaces/PartialTwoPort.mo b/AixLib/Electrical/Interfaces/PartialTwoPort.mo
new file mode 100644
index 0000000000..c7e9b4bf5b
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/PartialTwoPort.mo
@@ -0,0 +1,42 @@
+within AixLib.Electrical.Interfaces;
+model PartialTwoPort "Model of a generic two port component with phase systems"
+
+  replaceable package PhaseSystem_p =
+      AixLib.Electrical.PhaseSystems.PartialPhaseSystem constrainedby
+    AixLib.Electrical.PhaseSystems.PartialPhaseSystem
+    "Phase system of terminal p"
+    annotation (choicesAllMatching=true);
+
+  replaceable package PhaseSystem_n =
+      AixLib.Electrical.PhaseSystems.PartialPhaseSystem constrainedby
+    AixLib.Electrical.PhaseSystems.PartialPhaseSystem
+    "Phase system of terminal n"
+    annotation (choicesAllMatching=true);
+
+  extends AixLib.Electrical.Interfaces.PartialBaseTwoPort(
+    redeclare replaceable AixLib.Electrical.Interfaces.Terminal terminal_n
+      constrainedby AixLib.Electrical.Interfaces.Terminal(
+        redeclare replaceable package PhaseSystem = PhaseSystem_n),
+    redeclare replaceable AixLib.Electrical.Interfaces.Terminal terminal_p
+      constrainedby AixLib.Electrical.Interfaces.Terminal(
+        redeclare replaceable package PhaseSystem=PhaseSystem_p));
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+Model included into the AixLib library.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a model of a component with two electric terminals.
+It represents a common interface that is extended by other models.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialTwoPort;
diff --git a/AixLib/Electrical/Interfaces/ResistiveLoad.mo b/AixLib/Electrical/Interfaces/ResistiveLoad.mo
new file mode 100644
index 0000000000..b4749c7de6
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/ResistiveLoad.mo
@@ -0,0 +1,36 @@
+within AixLib.Electrical.Interfaces;
+partial model ResistiveLoad "Partial model of a resistive load"
+  extends Load;
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+May 14, 2015, by Marco Bonvini:<br/>
+Created model to solve problems related to OpenModelica as described
+in issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/415\">#415</a>.<br/>
+OpenModelica cannot determine the value
+<code>PhaseSystem.n</code> when models like
+<a href=\"modelica://Buildings.Electrical.AC.OnePhase.Loads.Resistive\">
+Buildings.Electrical.AC.OnePhase.Loads.Resistive</a>
+inherit directly from
+<a href=\"modelica://Buildings.Electrical.Interfaces.LoadAixLib.Electrical.Interfaces.Load\">
+Buildings.Electrical.Interfaces.LoadAixLib.Electrical.Interfaces.Load</a>.<br/>
+The same problem does not happen with models like
+<a href=\"modelica://Buildings.Electrical.AC.OnePhase.Loads.Capacitive\">
+Buildings.Electrical.AC.OnePhase.Loads.Capacitive</a> or
+<a href=\"modelica://Buildings.Electrical.AC.OnePhase.Loads.Inductive\">
+Buildings.Electrical.AC.OnePhase.Loads.Inductive</a> since they inherit
+from a different model.<br/>
+For such a reason this interface for resistive load model has been
+added to the library.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a model of a generic resistive load. This model is an extension of the base load model
+<a href=\"modelica://AixLib.Electrical.Interfaces.Load\">
+AixLib.Electrical.Interfaces.Load</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ResistiveLoad;
diff --git a/AixLib/Electrical/Interfaces/Source.mo b/AixLib/Electrical/Interfaces/Source.mo
new file mode 100644
index 0000000000..9c5d7e645e
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/Source.mo
@@ -0,0 +1,72 @@
+within AixLib.Electrical.Interfaces;
+model Source "Partial model of a generic source."
+  replaceable package PhaseSystem =
+      AixLib.Electrical.PhaseSystems.OnePhase constrainedby
+    AixLib.Electrical.PhaseSystems.PartialPhaseSystem "Phase system"
+    annotation (choicesAllMatching=true);
+  parameter Boolean potentialReference = true
+    "Serve as potential root for the reference angle theta"
+     annotation (Evaluate=true, Dialog(group="Reference Parameters"));
+  parameter Boolean definiteReference = false
+    "Serve as definite root for the reference angle theta"
+     annotation (Evaluate=true, Dialog(group="Reference Parameters"));
+  Modelica.Units.SI.Power S[PhaseSystem.n]=PhaseSystem.phasePowers_vi(terminal.v,
+      terminal.i) "Complex power S[1] = P, S[2]= Q";
+  Modelica.Units.SI.Angle phi=PhaseSystem.phase(terminal.v) - PhaseSystem.phase(
+      -terminal.i) "Phase shift with respect to reference angle";
+  replaceable AixLib.Electrical.Interfaces.Terminal terminal(
+    redeclare final replaceable package PhaseSystem = PhaseSystem)
+    "Generalized terminal"
+    annotation (Placement(transformation(extent={{92,-8},{108,8}})));
+protected
+  function j = PhaseSystem.j;
+equation
+  if potentialReference then
+      if definiteReference then
+        Connections.root(terminal.theta);
+      else
+        Connections.potentialRoot(terminal.theta);
+      end if;
+  end if;
+  annotation ( Documentation(revisions="<html>
+<ul>
+<li>
+February 26, 2016, by Michael Wetter:<br/>
+Updated documentation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/427\">issue 427</a>.
+</li>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+Model included into the AixLib library.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a generic source.
+</p>
+<p>
+In case the phase system has <code>PhaseSystem.m &gt; 0</code> and
+thus the connectors are over determined,
+the source can be selected to serve as reference point.
+The parameters <code>potentialReference</code> and <code>definiteReference</code>
+are used to define if the source model should be selected as source for
+the reference angles <code>theta</code> or not.
+More information about overdetermined connectors can be found
+in <a href=\"#Olsson2008\">Olsson Et Al. (2008)</a>.
+</p>
+
+<h4>References</h4>
+<p>
+<a name=\"Olsson2008\"/>
+Hans Olsson, Martin Otter, Sven Erik Mattson and Hilding Elmqvist.<br/>
+<a href=\"http://elib-v3.dlr.de/55892/1/otter2008-modelica-balanced-models.pdf\">
+Balanced Models in Modelica 3.0 for Increased Model Quality</a>.<br/>
+Proc. of the 7th Modelica Conference, Bielefeld, Germany, March 2008.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Source;
diff --git a/AixLib/Electrical/Interfaces/Terminal.mo b/AixLib/Electrical/Interfaces/Terminal.mo
new file mode 100644
index 0000000000..9ac5411635
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/Terminal.mo
@@ -0,0 +1,80 @@
+within AixLib.Electrical.Interfaces;
+connector Terminal "Generalized electric terminal"
+  extends AixLib.Electrical.Interfaces.BaseTerminal;
+replaceable package PhaseSystem = PhaseSystems.PartialPhaseSystem
+    "Phase system"
+  annotation (choicesAllMatching=true);
+PhaseSystem.Voltage v[PhaseSystem.n] "Voltage vector";
+flow PhaseSystem.Current i[PhaseSystem.n](each start=0) "Current vector";
+PhaseSystem.ReferenceAngle theta[PhaseSystem.m]
+    "Optional vector of phase angles";
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+<li>
+October 31, 2013, by Marco Bonvini:<br/>
+Model included into the AixLib library.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This connector represents a generalized electric terminal. The generalization is made possible by the
+replaceable package <a href=\"modelica://AixLib.Electrical.Interfaces.Terminal.PhaseSystem\">
+AixLib.Electrical.Interfaces.Terminal.PhaseSystem</a>.
+The package <code>PhaseSystem</code> can be one of the packages contained in
+<a href=\"modelica://AixLib.Electrical.PhaseSystems\">
+AixLib.Electrical.PhaseSystems</a>.
+Using this approach allows to represent DC, single phase AC and
+multi phases balanced and unbalanced AC systems with the same connector.
+</p>
+<p>
+This connector is compatible with the following Modelica libraries:
+</p>
+<ul>
+<li><a href=\"http://www.modelon.com/products/modelica-libraries/electric-power-library\">
+Electric Power Library</a>
+developed by Modelon, and
+</li>
+<li>
+<a href=\"https://github.com/modelica/PowerSystems\">Power Systems Library</a>
+developed by <a href=\"mailto:Ruediger.Franke@de.abb.com\">Ruediger Franke</a> (ABB).
+</li>
+</ul>
+<p>
+The connector is overdetermined since the number of effort variables
+is higher than the number of flow variables.
+This happens when the phase system has a number of reference angles
+<code>PhaseSystem.m &gt; 0</code>.
+The over-determined connectors are defined and used in such a way
+that a Modelica tool is able
+to remove the superfluous but consistent equations arriving
+at a balanced set of equations, based on a
+graph analysis of the connection structure.
+The models have to use ad-hoc constructs specified by the Modelica language to handle this situation.
+More information can be found in <a href=\"#Olsson2008\">Olsson Et Al. (2008)</a>.
+</p>
+<p>
+More details about the generalized electrical terminal
+can be found in <a href=\"#RuedigerEtAl2014\">Franke and Wiesmann (2014)</a>.
+</p>
+<h4>References</h4>
+<p>
+<a name=\"Olsson2008\"/>
+Hans Olsson, Martin Otter, Sven Erik Mattson and Hilding Elmqvist.<br/>
+<a href=\"http://elib-v3.dlr.de/55892/1/otter2008-modelica-balanced-models.pdf\">
+Balanced Models in Modelica 3.0 for Increased Model Quality</a>.<br/>
+Proc. of the 7th Modelica Conference, Bielefeld, Germany, March 2008.<br/>
+</p>
+<p>
+<a name=\"RuedigerEtAl2014\"/>
+Ruediger Franke and Hansjurg Wiesmann.<br/>
+<a href=\"https://www.modelica.org/events/modelica2014/proceedings/html/submissions/ECP14096515_FrankeWiesmann.pdf\">
+Flexible modeling of electrical power systems - the Modelica PowerSystems library</a>.<br/>
+Proc. of the 10th Modelica Conference, Lund, Sweden, March 2014.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Terminal;
diff --git a/AixLib/Electrical/Interfaces/VariableVoltageSource.mo b/AixLib/Electrical/Interfaces/VariableVoltageSource.mo
new file mode 100644
index 0000000000..ee1e9cdaab
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/VariableVoltageSource.mo
@@ -0,0 +1,64 @@
+within AixLib.Electrical.Interfaces;
+model VariableVoltageSource
+  "Partial model of a generic variable voltage source."
+  extends AixLib.Electrical.Interfaces.Source;
+  parameter Boolean use_V_in = true "If true, the voltage is an input";
+  parameter Modelica.Units.SI.Voltage V=1 "Value of constant voltage"
+    annotation (Dialog(enable=not use_V_in));
+  Modelica.Blocks.Interfaces.RealInput V_in(unit="V", min=0, start = 1)
+    if use_V_in "Input voltage"
+                    annotation (Placement(transformation(
+        extent={{20,-20},{-20,20}},
+        rotation=180,
+        origin={-100,60}),
+                         iconTransformation(
+        extent={{20,-20},{-20,20}},
+        rotation=180,
+        origin={-100,60})));
+protected
+  Modelica.Blocks.Interfaces.RealInput  V_in_internal(unit="V")
+    "Hidden value of the input voltage for the conditional connector";
+equation
+
+  // Connection between the conditional and inner connector
+  connect(V_in,V_in_internal);
+
+  // If the voltage is fixed, inner connector value is equal to parameter V
+  if use_V_in == false then
+    V_in_internal = V;
+  end if;
+  annotation ( Documentation(revisions="<html>
+<ul>
+<li>
+October 14, 2014, by Marco Bonvini:<br/>
+Model included into the AixLib library, added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model represents a generic variable voltage source. The model has a boolean
+flag <code>use_V_in</code>, when this flag is equal to <code>true</code>
+the voltage of the source is imposed by the input variable <code>V_in</code>.
+When the flag is equal to <code>false</code> the voltage source is equal to the parameter <code>V</code>.
+</p>
+<p>
+In case the phase system adopted has <code>PhaseSystem.m &gt; 0</code> and
+thus the connectors are over determined,
+the source can be selected to serve as reference point.
+The parameters <code>potentialReference</code> and <code>definiteReference</code> are used to define if the
+source model should be selected as source for the reference angles or not.
+More information about overdetermined connectors can be found
+in <a href=\"#Olsson2008\">Olsson Et Al. (2008)</a>.
+</p>
+
+<h4>References</h4>
+<p>
+<a name=\"Olsson2008\"/>
+Hans Olsson, Martin Otter, Sven Erik Mattson and Hilding Elmqvist.<br/>
+<a href=\"http://elib-v3.dlr.de/55892/1/otter2008-modelica-balanced-models.pdf\">
+Balanced Models in Modelica 3.0 for Increased Model Quality</a>.<br/>
+Proc. of the 7th Modelica Conference, Bielefeld, Germany, March 2008.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end VariableVoltageSource;
diff --git a/AixLib/Electrical/Interfaces/package.mo b/AixLib/Electrical/Interfaces/package.mo
new file mode 100644
index 0000000000..3860971cf8
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/package.mo
@@ -0,0 +1,22 @@
+within AixLib.Electrical;
+package Interfaces "This package contains interfaces and partial models that are inherited by other components"
+  extends Modelica.Icons.InterfacesPackage;
+
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains basic classes that are used to build
+component models for electrical systems.
+The classes are not directly usable, but can
+be extended when building a new model.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end Interfaces;
diff --git a/AixLib/Electrical/Interfaces/package.order b/AixLib/Electrical/Interfaces/package.order
new file mode 100644
index 0000000000..51dea4d83d
--- /dev/null
+++ b/AixLib/Electrical/Interfaces/package.order
@@ -0,0 +1,15 @@
+BaseTerminal
+CapacitiveLoad
+Ground
+Impedance
+InductiveLoad
+Load
+PartialBaseTwoPort
+PartialConversion
+PartialTwoPort
+ResistiveLoad
+Source
+Terminal
+VariableVoltageSource
+PartialAcDcParameters
+PartialPluggableUnbalanced
diff --git a/AixLib/Electrical/Machines/PVInverterRMS.mo b/AixLib/Electrical/Machines/PVInverterRMS.mo
index 43f4d4743a..960d1319e5 100644
--- a/AixLib/Electrical/Machines/PVInverterRMS.mo
+++ b/AixLib/Electrical/Machines/PVInverterRMS.mo
@@ -1,7 +1,7 @@
 within AixLib.Electrical.Machines;
 model PVInverterRMS "Inverter model including system management"
 
-  parameter Modelica.Units.SI.Power uMax2
+  parameter Modelica.Units.SI.Power uMax2=3800
     "Upper limits of input signals (MaxOutputPower)";
  Modelica.Blocks.Interfaces.RealOutput PVPowerRmsW(
   final quantity="Power",
@@ -66,9 +66,6 @@ equation
      Line(
       points={{-48,-34},{55,-34}},
       color={0,0,0})}),
-   experiment(
-    StopTime=1,
-    StartTime=0),
      Documentation(revisions="<html><ul>
   <li>
     <i>October 11, 2016</i> by Tobias Blacha:<br/>
diff --git a/AixLib/Electrical/PVSystem/BaseClasses/PVRadiationHorizontal.mo b/AixLib/Electrical/PVSystem/BaseClasses/PVRadiationHorizontal.mo
index d096159ef9..456901ecef 100644
--- a/AixLib/Electrical/PVSystem/BaseClasses/PVRadiationHorizontal.mo
+++ b/AixLib/Electrical/PVSystem/BaseClasses/PVRadiationHorizontal.mo
@@ -143,7 +143,7 @@ model PVRadiationHorizontal "PV radiation and absorptance model - input: total i
   AixLib.BoundaryConditions.SolarGeometry.BaseClasses.ZenithAngle zenAng(
    lat=lat) "Zenith angle";
 
-  Utilities.Time.ModelTime modTim "Block that outputs simulation time";
+  AixLib.Utilities.Time.ModelTime modTim "Block that outputs simulation time";
 
 
   Modelica.Blocks.Interfaces.RealOutput radTil(final quantity="Irradiance",
diff --git a/AixLib/Electrical/PVSystem/BaseClasses/package.order b/AixLib/Electrical/PVSystem/BaseClasses/package.order
index 67066ffeb1..309d1d5092 100644
--- a/AixLib/Electrical/PVSystem/BaseClasses/package.order
+++ b/AixLib/Electrical/PVSystem/BaseClasses/package.order
@@ -5,4 +5,3 @@ IVCharacteristics5pAnalytical
 PVRadiationHorizontal
 PartialCellTemperature
 Wsimple
-PartialIVCharacteristics
diff --git a/AixLib/Electrical/PhaseSystems/DirectCurrent.mo b/AixLib/Electrical/PhaseSystems/DirectCurrent.mo
new file mode 100644
index 0000000000..40ac30bea9
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/DirectCurrent.mo
@@ -0,0 +1,108 @@
+within AixLib.Electrical.PhaseSystems;
+package DirectCurrent "DC system"
+  extends PartialPhaseSystem(phaseSystemName="DirectCurrent", n=1, m=0);
+
+
+  redeclare function extends j "Direct current has no complex component"
+  algorithm
+    y := zeros(n);
+    annotation(Inline=true);
+  end j;
+
+
+ redeclare function extends rotate
+  "Rotate a vector of an angle theta (anti-counterclock)"
+ algorithm
+    y[n] := x[n];
+    annotation(Inline=true);
+ end rotate;
+
+
+ redeclare function extends thetaRel
+  "Return absolute angle of rotating system as offset to thetaRef"
+ algorithm
+    thetaRel := 0;
+    annotation(Inline=true);
+ end thetaRel;
+
+
+ redeclare function extends thetaRef
+  "Return absolute angle of rotating reference system"
+ algorithm
+    thetaRef := 0;
+    annotation(Inline=true);
+ end thetaRef;
+
+
+ redeclare function extends phase "Return phase"
+ algorithm
+    phase := 0;
+    annotation(Inline=true);
+ end phase;
+
+
+  redeclare replaceable function extends phaseVoltages
+  "Return phase to neutral voltages"
+  algorithm
+    v := {V};
+    annotation(Inline=true);
+  end phaseVoltages;
+
+
+  redeclare function extends phaseCurrents "Return phase currents"
+  algorithm
+    i := {I};
+    annotation(Inline=true);
+  end phaseCurrents;
+
+
+  redeclare function extends phasePowers "Return phase powers"
+  algorithm
+    p := {P};
+    annotation(Inline=true);
+  end phasePowers;
+
+
+  redeclare function extends phasePowers_vi "Return phase powers"
+  algorithm
+    p := {v*i};
+    annotation(Inline=true);
+  end phasePowers_vi;
+
+
+  redeclare replaceable function extends systemVoltage
+  "Return system voltage as function of phase voltages"
+  algorithm
+    V := v[1];
+    annotation(Inline=true);
+  end systemVoltage;
+
+
+  redeclare function extends systemCurrent
+  "Return system current as function of phase currents"
+  algorithm
+    I := i[1];
+    annotation(Inline=true);
+  end systemCurrent;
+
+
+  redeclare function extends activePower
+  "Return total power as function of phase powers"
+  algorithm
+    P := v*i;
+    annotation(Inline=true);
+  end activePower;
+
+
+  annotation (Icon(graphics={Line(
+          points={{-70,-10},{50,-10}},
+          color={95,95,95},
+          smooth=Smooth.None)}),
+Documentation(info="<html>
+<p>
+This package declares the functions that are used to implement
+the DC models.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end DirectCurrent;
diff --git a/AixLib/Electrical/PhaseSystems/OnePhase.mo b/AixLib/Electrical/PhaseSystems/OnePhase.mo
new file mode 100644
index 0000000000..96eb709fa9
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/OnePhase.mo
@@ -0,0 +1,126 @@
+within AixLib.Electrical.PhaseSystems;
+package OnePhase "Single phase two connectors AC system"
+  extends PartialPhaseSystem(phaseSystemName="OnePhase", n=2, m=1);
+
+
+  redeclare function extends j "Return vector rotated by 90 degrees"
+  algorithm
+    y := {-x[2], x[1]};
+    annotation(Inline=true);
+  end j;
+
+
+  redeclare function extends rotate
+  "Rotate a vector of an angle theta (anti-counterclock)"
+  algorithm
+    y[1] := cos(theta)*x[1] - sin(theta)*x[2];
+    y[2] := sin(theta)*x[1] + cos(theta)*x[2];
+    annotation(Inline=true);
+  end rotate;
+
+
+  redeclare function extends product
+  "Multiply two complex numbers represented by vectors x[2] and y[2]"
+  algorithm
+    z := {x[1]*y[1] - x[2]*y[2], x[1]*y[2] + x[2]*y[1]};
+    annotation(Inline=true);
+  end product;
+
+
+  redeclare function extends divide
+  "Divide two complex numbers represented by vectors x[2] and y[2]"
+  algorithm
+    z := {x[1]*y[1] + x[2]*y[2], x[2]*y[1] - x[1]*y[2]}/(y[1]^2 + y[2]^2);
+    annotation(Inline=true);
+  end divide;
+
+
+  redeclare function extends thetaRel
+  "Return absolute angle of rotating system as offset to thetaRef"
+  algorithm
+    thetaRel := 0;
+    annotation(Inline=true);
+  end thetaRel;
+
+
+  redeclare function extends thetaRef
+  "Return absolute angle of rotating reference system"
+  algorithm
+    thetaRef := theta[1];
+    annotation(Inline=true);
+  end thetaRef;
+
+
+  redeclare function extends phase "Return phase"
+  algorithm
+    phase := atan2(x[2], x[1]);
+    annotation(Inline=true);
+  end phase;
+
+
+  redeclare function extends phaseVoltages "Return phase to neutral voltages"
+  algorithm
+    v := {V*cos(phi), V*sin(phi)};
+    annotation(Inline=true);
+  end phaseVoltages;
+
+
+  redeclare function extends phaseCurrents "Return phase currents"
+  algorithm
+    i := {I*cos(phi), I*sin(phi)};
+    annotation(Inline=true);
+  end phaseCurrents;
+
+
+  redeclare function extends phasePowers "Return phase powers"
+  algorithm
+    p := {P, P*tan(phi)};
+    annotation(Inline=true);
+  end phasePowers;
+
+
+  redeclare function extends phasePowers_vi "Return phase powers"
+  algorithm
+    p := {v[1]*i[1] + v[2]*i[2], v[2]*i[1] - v[1]*i[2]};
+    annotation(Inline=true);
+  end phasePowers_vi;
+
+
+  redeclare function extends systemVoltage
+  "Return system voltage as function of phase voltages"
+  algorithm
+    V := Modelica.Fluid.Utilities.regRoot(v*v, delta = 1e-5);
+    annotation(Inline=true);
+  end systemVoltage;
+
+
+  redeclare function extends systemCurrent
+  "Return system current as function of phase currents"
+  algorithm
+    I := Modelica.Fluid.Utilities.regRoot(i*i, delta = 1e-5);
+    annotation(Inline=true);
+  end systemCurrent;
+
+
+  redeclare function extends activePower
+  "Return total power as function of phase powers"
+  algorithm
+    // P = v[1]*i[1] + v[2]*i[2]
+    P := v*i;
+    annotation(Inline=true);
+  end activePower;
+
+
+  annotation (Icon(graphics={
+        Line(
+          points={{-70,-10},{-58,10},{-38,30},{-22,10},{-10,-10},{2,-30},{22,-50},
+              {40,-30},{50,-10}},
+          color={95,95,95},
+          smooth=Smooth.Bezier)}), Documentation(info="<html>
+<p>
+This package declares the functions that are used to implement
+the AC single phase models.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end OnePhase;
diff --git a/AixLib/Electrical/PhaseSystems/PartialPhaseSystem.mo b/AixLib/Electrical/PhaseSystems/PartialPhaseSystem.mo
new file mode 100644
index 0000000000..8d99d64bf2
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/PartialPhaseSystem.mo
@@ -0,0 +1,161 @@
+within AixLib.Electrical.PhaseSystems;
+package PartialPhaseSystem "Base package of all phase systems"
+  extends Modelica.Icons.Package;
+  constant String phaseSystemName = "UnspecifiedPhaseSystem"
+    "Name of the phase system represented by the package";
+  constant Integer n "Number of independent voltage and current components";
+  constant Integer m "Number of reference angles";
+
+  type Current = Real(unit = "A", quantity = "Current." + phaseSystemName)
+    "Current for connector" annotation (Documentation(info="<html>
+This type defines the current for a specific connector that extends
+<a href=\"modelica://AixLib.Electrical.PhaseSystems.PartialPhaseSystem\">
+AixLib.Electrical.PhaseSystems.PartialPhaseSystem</a>.
+</html>"));
+
+  type Voltage = Real(unit = "V", quantity = "Voltage." + phaseSystemName)
+    "Voltage for connector" annotation (Documentation(info="<html>
+This type defines the voltage for a specific connector that extends
+<a href=\"modelica://AixLib.Electrical.PhaseSystems.PartialPhaseSystem\">
+AixLib.Electrical.PhaseSystems.PartialPhaseSystem</a>.
+</html>"));
+
+  type ReferenceAngle "Reference angle for connector"
+    extends Modelica.Units.SI.Angle;
+
+    function equalityConstraint "Assert that angles are equal"
+      extends Modelica.Icons.Function;
+      input ReferenceAngle theta1[:];
+      input ReferenceAngle theta2[:];
+      output Real residue[0];
+    algorithm
+      for i in 1:size(theta1, 1) loop
+        assert(abs(theta1[i] - theta2[i]) < Modelica.Constants.eps,
+          "Angles theta1 and theta2 are not equal over the connection.");
+      end for;
+    end equalityConstraint;
+    annotation (Documentation(info="<html>
+This type defines the voltage angle (used by the phasorial approach) for a specific connector that extends
+<a href=\"modelica://AixLib.Electrical.PhaseSystems.PartialPhaseSystem\">
+AixLib.Electrical.PhaseSystems.PartialPhaseSystem</a>.
+</html>"));
+  end ReferenceAngle;
+
+  replaceable partial function j "Return vector rotated by 90 degrees"
+    extends Modelica.Icons.Function;
+    input Real x[n];
+    output Real y[n];
+  end j;
+
+  replaceable partial function jj "Vectorized version of j"
+    extends Modelica.Icons.Function;
+    input Real[:,:] xx "array of voltage or current vectors";
+    output Real[size(xx,1),size(xx,2)] yy "array of rotated vectors";
+  algorithm
+    //yy := {j(xx[:,k]) for k in 1:size(xx,2)};
+    // Note: Dymola 2013 fails to expand
+    for k in 1:size(xx,2) loop
+      yy[:,k] := j(xx[:,k]);
+    end for;
+  end jj;
+
+  replaceable partial function rotate
+    "Rotate a vector of an angle theta (anti-counterclock)"
+    extends Modelica.Icons.Function;
+    input Real x[n];
+    input Modelica.Units.SI.Angle theta;
+    output Real y[n];
+  end rotate;
+
+  replaceable partial function product "Multiply two vectors"
+      extends Modelica.Icons.Function;
+      input Real x[n];
+      input Real y[n];
+      output Real z[n];
+  end product;
+
+  replaceable partial function divide "Divide two vectors"
+      extends Modelica.Icons.Function;
+      input Real x[n];
+      input Real y[n];
+      output Real z[n];
+  end divide;
+
+  replaceable partial function thetaRel
+    "Return absolute angle of rotating system as offset to thetaRef"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Angle theta[m];
+    output Modelica.Units.SI.Angle thetaRel;
+  end thetaRel;
+
+  replaceable partial function thetaRef
+    "Return absolute angle of rotating reference system"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Angle theta[m];
+    output Modelica.Units.SI.Angle thetaRef;
+  end thetaRef;
+
+  replaceable partial function phase "Return phase"
+    extends Modelica.Icons.Function;
+    input Real x[n];
+    output Modelica.Units.SI.Angle phase;
+  end phase;
+
+  replaceable partial function phaseVoltages "Return phase to neutral voltages"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Voltage V "system voltage";
+    input Modelica.Units.SI.Angle phi=0 "phase angle";
+    output Modelica.Units.SI.Voltage v[n] "phase to neutral voltages";
+  end phaseVoltages;
+
+  replaceable partial function phaseCurrents "Return phase currents"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Current I "system current";
+    input Modelica.Units.SI.Angle phi=0 "phase angle";
+    output Modelica.Units.SI.Current i[n] "phase currents";
+  end phaseCurrents;
+
+  replaceable partial function phasePowers "Return phase powers"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.ActivePower P "active system power";
+    input Modelica.Units.SI.Angle phi=0 "phase angle";
+    output Modelica.Units.SI.Power p[n] "phase powers";
+  end phasePowers;
+
+  replaceable partial function phasePowers_vi "Return phase powers"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Voltage v[n] "phase voltages";
+    input Modelica.Units.SI.Current i[n] "phase currents";
+    output Modelica.Units.SI.Power p[n] "phase powers";
+  end phasePowers_vi;
+
+  replaceable partial function systemVoltage
+    "Return system voltage as function of phase voltages"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Voltage v[n];
+    output Modelica.Units.SI.Voltage V;
+  end systemVoltage;
+
+  replaceable partial function systemCurrent
+    "Return system current as function of phase currents"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Current i[n];
+    output Modelica.Units.SI.Current I;
+  end systemCurrent;
+
+  replaceable partial function activePower
+    "Return total power as function of phase powers"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Voltage v[n] "phase voltages";
+    input Modelica.Units.SI.Current i[n] "phase currents";
+    output Modelica.Units.SI.ActivePower P "active system power";
+  end activePower;
+
+annotation (Documentation(info="<html>
+<p>
+This package declares the functions that are used to implement
+the different phase systems.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialPhaseSystem;
diff --git a/AixLib/Electrical/PhaseSystems/ThreePhase_d.mo b/AixLib/Electrical/PhaseSystems/ThreePhase_d.mo
new file mode 100644
index 0000000000..c42c252569
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/ThreePhase_d.mo
@@ -0,0 +1,38 @@
+within AixLib.Electrical.PhaseSystems;
+package ThreePhase_d "AC system covering only resistive loads with three symmetric phases"
+  extends DirectCurrent(phaseSystemName="ThreePhase_d");
+
+
+  redeclare function phaseVoltages "Return phase to neutral voltages"
+    extends Modelica.Icons.Function;
+    input SI.Voltage V "system voltage";
+    input SI.Angle phi = 0 "phase angle";
+    output SI.Voltage v[n] "phase to neutral voltages";
+  algorithm
+    v := {V}/sqrt(3);
+  end phaseVoltages;
+
+
+  redeclare function systemVoltage
+  "Return system voltage as function of phase voltages"
+    extends Modelica.Icons.Function;
+    input SI.Voltage v[n];
+    output SI.Voltage V;
+  algorithm
+    V := sqrt(3)*v[1];
+  end systemVoltage;
+
+
+  annotation (Icon(graphics={
+        Line(
+          points={{-70,-10},{-58,10},{-38,30},{-22,10},{-10,-10},{2,-30},{22,
+              -50},{40,-30},{50,-10}},
+          color={95,95,95},
+          smooth=Smooth.Bezier)}), Documentation(info="<html>
+<p>
+This package declares the functions that are used to implement
+the AC three-phase balanced and purely resistive models.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ThreePhase_d;
diff --git a/AixLib/Electrical/PhaseSystems/ThreePhase_dq.mo b/AixLib/Electrical/PhaseSystems/ThreePhase_dq.mo
new file mode 100644
index 0000000000..00260444c1
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/ThreePhase_dq.mo
@@ -0,0 +1,108 @@
+within AixLib.Electrical.PhaseSystems;
+package ThreePhase_dq "AC system, symmetrically loaded three-phase"
+  extends PartialPhaseSystem(phaseSystemName="ThreePhase_dq", n=2, m=1);
+
+
+  redeclare function extends j "Return vector rotated by 90 degrees"
+  algorithm
+    y := {-x[2], x[1]};
+    annotation(Inline=true);
+  end j;
+
+
+  redeclare function extends thetaRel
+  "Return absolute angle of rotating system as offset to thetaRef"
+  algorithm
+    thetaRel := 0;
+    annotation(Inline=true);
+  end thetaRel;
+
+
+  redeclare function extends thetaRef
+  "Return absolute angle of rotating reference system"
+  algorithm
+    thetaRef := theta[1];
+    annotation(Inline=true);
+  end thetaRef;
+
+
+  redeclare function extends phase "Return phase"
+  algorithm
+    phase := atan2(x[2], x[1]);
+    annotation(Inline=true);
+  end phase;
+
+
+  redeclare function extends phaseVoltages "Return phase to neutral voltages"
+  algorithm
+    v := {V*cos(phi), V*sin(phi)}/sqrt(3);
+    annotation(Inline=true);
+  end phaseVoltages;
+
+
+  redeclare function extends phaseCurrents "Return phase currents"
+  algorithm
+    i := {I*cos(phi), I*sin(phi)};
+    annotation(Inline=true);
+  end phaseCurrents;
+
+
+  redeclare function extends phasePowers "Return phase powers"
+  algorithm
+    p := {P, P*tan(phi)};
+    annotation(Inline=true);
+  end phasePowers;
+
+
+  redeclare function extends phasePowers_vi "Return phase powers"
+  algorithm
+    p := {v*i, -j(v)*i};
+    annotation(Inline=true);
+  end phasePowers_vi;
+
+
+  redeclare function extends systemVoltage
+  "Return system voltage as function of phase voltages"
+  algorithm
+    V := Modelica.Fluid.Utilities.regRoot(3*v*v, delta = 1e-5);
+    annotation(Inline=true);
+  end systemVoltage;
+
+
+  redeclare function extends systemCurrent
+  "Return system current as function of phase currents"
+  algorithm
+    I := Modelica.Fluid.Utilities.regRoot(i*i, delta = 1e-5);
+    annotation(Inline=true);
+  end systemCurrent;
+
+
+  redeclare function extends activePower
+  "Return total power as function of phase powers"
+  algorithm
+    P := v[1]*i[1];
+    annotation(Inline=true);
+  end activePower;
+
+
+  annotation (Icon(graphics={
+        Line(
+          points={{-70,12},{-58,32},{-38,52},{-22,32},{-10,12},{2,-8},{22,-28},
+              {40,-8},{50,12}},
+          color={95,95,95},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-70,-70},{50,-70}},
+          color={95,95,95},
+          smooth=Smooth.None),
+        Line(
+          points={{-70,-46},{50,-46}},
+          color={95,95,95},
+          smooth=Smooth.None)}), Documentation(info="<html>
+<p>
+This package declares the functions that are used to implement
+the AC three-phase balanced models using the DQ representation.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ThreePhase_dq;
diff --git a/AixLib/Electrical/PhaseSystems/ThreePhase_dq0.mo b/AixLib/Electrical/PhaseSystems/ThreePhase_dq0.mo
new file mode 100644
index 0000000000..8bf95aa833
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/ThreePhase_dq0.mo
@@ -0,0 +1,135 @@
+within AixLib.Electrical.PhaseSystems;
+package ThreePhase_dq0 "AC system in dqo representation"
+  extends PartialPhaseSystem(phaseSystemName="ThreePhase_dqo", n=3, m=2);
+
+
+  redeclare function extends j
+  "Rotation(pi/2) of vector around {0,0,1} and projection on North plane"
+  algorithm
+    y := cat(1, {-x[2], x[1]}, zeros(size(x,1)-2));
+    annotation(Inline=true);
+  end j;
+
+
+  redeclare function extends rotate
+  "Rotate a vector of an angle theta (anti-counterclock)"
+  algorithm
+    y[1] := cos(theta)*x[1] - sin(theta)*x[2];
+    y[2] := sin(theta)*x[1] + cos(theta)*x[2];
+    y[3] := x[3];
+    annotation(Inline=true);
+  end rotate;
+
+
+  redeclare function jj "Vectorized version of j"
+  extends Modelica.Icons.Function;
+    input Real[:,:] xx "array of voltage or current vectors";
+    output Real[size(xx,1),size(xx,2)] yy "array of rotated vectors";
+  algorithm
+    yy := cat(1, {-xx[2,:], xx[1,:]}, zeros(size(xx,1)-2, size(xx,2)));
+    annotation(Inline=true);
+  end jj;
+
+
+  redeclare function extends thetaRel
+  "Return absolute angle of rotating system as offset to thetaRef"
+  algorithm
+    thetaRel := theta[1];
+    annotation(Inline=true);
+  end thetaRel;
+
+
+  redeclare function extends thetaRef
+  "Return absolute angle of rotating reference system"
+  algorithm
+    thetaRef := theta[2];
+    annotation(Inline=true);
+  end thetaRef;
+
+
+  redeclare function extends phase "Return phase"
+  algorithm
+    phase := atan2(x[2], x[1]);
+    annotation(Inline=true);
+  end phase;
+
+
+  redeclare function extends phaseVoltages "Return phase to neutral voltages"
+  protected
+    Voltage neutral_v = 0;
+  algorithm
+    v := {V*cos(phi), V*sin(phi), sqrt(3)*neutral_v}/sqrt(3);
+    annotation(Inline=true);
+  end phaseVoltages;
+
+
+  redeclare function extends phaseCurrents "Return phase currents"
+  algorithm
+    i := {I*cos(phi), I*sin(phi), 0};
+    annotation(Inline=true);
+  end phaseCurrents;
+
+
+  redeclare function extends phasePowers "Return phase powers"
+  algorithm
+    p := {P, P*tan(phi), 0};
+    annotation(Inline=true);
+  end phasePowers;
+
+
+  redeclare function extends phasePowers_vi "Return phase powers"
+  algorithm
+    p := {v[1:2]*i[1:2], -j(v[1:2])*i[1:2], v[3]*i[3]};
+    annotation(Inline=true);
+  end phasePowers_vi;
+
+
+  redeclare function extends systemVoltage
+  "Return system voltage as function of phase voltages"
+  algorithm
+    V := Modelica.Fluid.Utilities.regRoot(v*v, delta = 1e-5);
+    annotation(Inline=true);
+  end systemVoltage;
+
+
+  redeclare function extends systemCurrent
+  "Return system current as function of phase currents"
+  algorithm
+    I := Modelica.Fluid.Utilities.regRoot(i*i, delta = 1e-5);
+    annotation(Inline=true);
+  end systemCurrent;
+
+
+  redeclare function extends activePower
+  "Return total power as function of phase powers"
+  algorithm
+    P := v[1]*i[1];
+    annotation(Inline=true);
+  end activePower;
+
+
+  annotation (Icon(graphics={
+        Line(
+          points={{-70,28},{-58,48},{-38,68},{-22,48},{-10,28},{2,8},{22,-12},
+              {40,8},{50,28}},
+          color={95,95,95},
+          smooth=Smooth.Bezier),
+        Line(
+          points={{-70,-54},{50,-54}},
+          color={95,95,95},
+          smooth=Smooth.None),
+        Line(
+          points={{-70,-78},{50,-78}},
+          color={95,95,95},
+          smooth=Smooth.None),
+        Line(
+          points={{-70,-28},{50,-28}},
+          color={95,95,95},
+          smooth=Smooth.None)}), Documentation(info="<html>
+<p>
+This package declares the functions that are used to implement
+the AC three-phase balanced models using the DQ0 representation.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ThreePhase_dq0;
diff --git a/AixLib/Electrical/PhaseSystems/TwoConductor.mo b/AixLib/Electrical/PhaseSystems/TwoConductor.mo
new file mode 100644
index 0000000000..ab9e3fedd6
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/TwoConductor.mo
@@ -0,0 +1,111 @@
+within AixLib.Electrical.PhaseSystems;
+package TwoConductor "Two conductors for DC components"
+  extends PartialPhaseSystem(phaseSystemName="TwoConductor", n=2, m=0);
+
+
+  redeclare function extends j "Direct current has no complex component"
+  algorithm
+    y := zeros(n);
+    annotation(Inline=true);
+  end j;
+
+
+  redeclare function extends rotate
+  "Rotate a vector of an angle theta (anti-counterclock)"
+  algorithm
+    y[n] := x[n];
+    annotation(Inline=true);
+  end rotate;
+
+
+  redeclare function extends thetaRel
+  "Return absolute angle of rotating system as offset to thetaRef"
+  algorithm
+    thetaRel := 0;
+    annotation(Inline=true);
+  end thetaRel;
+
+
+  redeclare function extends thetaRef
+  "Return absolute angle of rotating reference system"
+  algorithm
+    thetaRef := 0;
+    annotation(Inline=true);
+  end thetaRef;
+
+
+  redeclare function extends phase "Return phase"
+  algorithm
+    phase := 0;
+    annotation(Inline=true);
+  end phase;
+
+
+  redeclare replaceable function extends phaseVoltages
+  "Return phase to neutral voltages"
+  algorithm
+    v := 0.5*{V, -V};
+    annotation(Inline=true);
+  end phaseVoltages;
+
+
+  redeclare function extends phaseCurrents "Return phase currents"
+  algorithm
+    i := {I, -I};
+    annotation(Inline=true);
+  end phaseCurrents;
+
+
+  redeclare function extends phasePowers "Return phase powers"
+  algorithm
+    p := {P, 0};
+    annotation(Inline=true);
+  end phasePowers;
+
+
+  redeclare function extends phasePowers_vi "Return phase powers"
+  algorithm
+    p := v.*i;
+    annotation(Inline=true);
+  end phasePowers_vi;
+
+
+  redeclare replaceable function extends systemVoltage
+  "Return system voltage as function of phase voltages"
+  algorithm
+    V := v[1] - v[2];
+    annotation(Inline=true);
+  end systemVoltage;
+
+
+  redeclare function extends systemCurrent
+  "Return system current as function of phase currents"
+  algorithm
+    I := (i[1] - i[2])/2;
+    annotation(Inline=true);
+  end systemCurrent;
+
+
+  redeclare function extends activePower
+  "Return total power as function of phase powers"
+  algorithm
+    P := v*i;
+    annotation(Inline=true);
+  end activePower;
+
+
+  annotation (Icon(graphics={Line(
+          points={{-70,-28},{50,-28}},
+          color={95,95,95},
+          smooth=Smooth.None),
+                             Line(
+          points={{-70,6},{50,6}},
+          color={95,95,95},
+          smooth=Smooth.None)}), Documentation(info="<html>
+<p>
+This package declares the functions that are used to implement
+the DC models with double conductors.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TwoConductor;
diff --git a/AixLib/Electrical/PhaseSystems/package.mo b/AixLib/Electrical/PhaseSystems/package.mo
new file mode 100644
index 0000000000..d95958ac09
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/package.mo
@@ -0,0 +1,72 @@
+within AixLib.Electrical;
+package PhaseSystems "Phase systems used in power connectors"
+  extends Modelica.Icons.Package;
+  import      Modelica.Units.SI;
+  import Modelica.Constants.pi;
+
+
+  annotation (Icon(graphics={Line(
+          points={{-70,-52},{50,-52}},
+          color={95,95,95},
+          smooth=Smooth.None), Line(
+          points={{-70,8},{-58,28},{-38,48},{-22,28},{-10,8},{2,-12},{22,-32},{
+              40,-12},{50,8}},
+          color={95,95,95},
+          smooth=Smooth.Bezier)}),
+preferredView="info",
+Documentation(info="<html>
+<p>
+This package contains a list of packages that represent different type of electric systems.
+Each package inherits from <a href=\"modelica://AixLib.Electrical.PhaseSystems.PartialPhaseSystem\">
+AixLib.Electrical.PhaseSystems.PartialPhaseSystem</a>.
+</p>
+<p>
+The packages represent various types of electrical systems. The basic idea behind this
+approach is to use the same connector for different electrical domains.
+Each connector has a replaceable package that inherits from
+<a href=\"modelica://AixLib.Electrical.PhaseSystems.PartialPhaseSystem\">
+AixLib.Electrical.PhaseSystems.PartialPhaseSystem</a>
+depending on the type of electrical system.
+The electrical systems represented are:
+</p>
+
+<ul>
+<li>DC systems,</li>
+<li>DC systems with two conductors,</li>
+<li>one-phase AC systems,</li>
+<li>three-phase resistive balanced AC systems,</li>
+<li>three-phase balanced AC systems,</li>
+<li>three-phase unbalanced AC systems (dq0 representation).</li>
+</ul>
+
+<p>
+This approach has been used by the following Modelica libraries:
+</p>
+
+<ul>
+<li><a href=\"http://www.modelon.com/products/modelica-libraries/electric-power-library\">Electric Power Library</a>,
+developed by Modelon,</li>
+<li><a href=\"https://github.com/modelica/PowerSystems\">Power Systems Library</a>, and
+developed by <a href=\"mailto:Ruediger.Franke@de.abb.com\">Rudiger Franke</a> (ABB).</li>
+</ul>
+
+<p>
+More details about the phase system packages can be found in <a href=\"#RuedigerEtAl2014\">Franke and Wiesmann (2014)</a>.
+</p>
+<h4>References</h4>
+<p>
+<a name=\"RuedigerEtAl2014\"/>
+Ruediger Franke and Hansjurg Wiesmann.<br/>
+<a href=\"https://www.modelica.org/events/modelica2014/proceedings/html/submissions/ECP14096515_FrankeWiesmann.pdf\">
+Flexible modeling of electrical power systems - the Modelica PowerSystems library</a>.<br/>
+Proc. of the 10th Modelica Conference, Lund, Sweden, March 2014.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 27, 2014, by Marco Bonvini:<br/>
+Created documentation.
+</li>
+</ul>
+</html>"));
+end PhaseSystems;
diff --git a/AixLib/Electrical/PhaseSystems/package.order b/AixLib/Electrical/PhaseSystems/package.order
new file mode 100644
index 0000000000..d1d8938c49
--- /dev/null
+++ b/AixLib/Electrical/PhaseSystems/package.order
@@ -0,0 +1,7 @@
+DirectCurrent
+OnePhase
+PartialPhaseSystem
+ThreePhase_d
+ThreePhase_dq
+ThreePhase_dq0
+TwoConductor
diff --git a/AixLib/Electrical/Transmission/BaseClasses/BaseCable.mo b/AixLib/Electrical/Transmission/BaseClasses/BaseCable.mo
new file mode 100644
index 0000000000..b3013b97c2
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/BaseCable.mo
@@ -0,0 +1,102 @@
+within AixLib.Electrical.Transmission.BaseClasses;
+record BaseCable "Record that contains the properties of a generic cable"
+  parameter AixLib.Electrical.Transmission.Types.Material material = AixLib.Electrical.Transmission.Types.Material.Al
+    "Material of the cable";
+  parameter Modelica.Units.SI.Current Amp(start=0.0) = 0.0
+    "Ampacitance of the cable";
+  parameter Modelica.Units.SI.Temperature T_ref=298.15
+    "Reference cable temperature";
+  parameter Modelica.Units.SI.Temperature M=228.1 + 273.15
+    "Temperature constant of the material";
+
+  replaceable partial function lineResistance
+    "Function that computes the resistance of a cable"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Length l "Length of the cable";
+    input Modelica.Units.SI.Frequency f=50
+      "Frequency considered in the definition of cables properties";
+    output Modelica.Units.SI.Resistance R "Resistance of the cable";
+  protected
+    parameter Modelica.Units.SI.AngularVelocity omega=2*Modelica.Constants.pi*f;
+    annotation (Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>"));
+  end lineResistance;
+
+  replaceable partial function lineInductance
+    "Function that computes the inductance of a cable"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Length l "Length of the cable";
+    input Modelica.Units.SI.Frequency f=50
+      "Frequency considered in the definition of cables properties";
+    output Modelica.Units.SI.Inductance L "Inductance of the cable";
+  protected
+    parameter Modelica.Units.SI.AngularVelocity omega=2*Modelica.Constants.pi*f;
+    annotation (Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>"));
+  end lineInductance;
+
+  replaceable partial function lineCapacitance
+    "Function that computes the capacitance of a cable"
+    extends Modelica.Icons.Function;
+    input Modelica.Units.SI.Length l "Length of the cable";
+    input Modelica.Units.SI.Frequency f=50
+      "Frequency considered in the definition of cables properties";
+    output Modelica.Units.SI.Capacitance C "Capacitance of the cable";
+  protected
+    parameter Modelica.Units.SI.AngularVelocity omega=2*Modelica.Constants.pi*f;
+    annotation (Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>"));
+  end lineCapacitance;
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, not it contains just the minimum amount of
+information needed to describe a cable.<br/>
+It also contains partial function that compute the properties of the cable.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This record contains the basic properties to describe a commercial
+cable.
+</p>
+<p>
+The low voltage and medium voltage cables extends this base records and add
+other specific parameters like the geometrical properties.
+</p>
+<p>
+The record contains four partial replaceable functions used to compute
+the properties of the cable such its resistance, inductance or capacitance.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BaseCable;
diff --git a/AixLib/Electrical/Transmission/BaseClasses/PartialBaseLine.mo b/AixLib/Electrical/Transmission/BaseClasses/PartialBaseLine.mo
new file mode 100644
index 0000000000..577f277c77
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/PartialBaseLine.mo
@@ -0,0 +1,172 @@
+within AixLib.Electrical.Transmission.BaseClasses;
+partial model PartialBaseLine "Partial cable line dispersion model"
+  parameter Modelica.Units.SI.Length l(min=0) "Length of the line";
+  parameter Modelica.Units.SI.Power P_nominal(min=0)
+    "Nominal power of the line";
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=220)
+    "Nominal voltage of the line";
+  final parameter Modelica.Units.SI.Frequency f_n=50
+    "Frequency considered in the definition of cables properties";
+
+  parameter Boolean use_C = false
+    "Set to true to add a capacitance in the center of the line"
+    annotation(Evaluate=true, Dialog(tab="Model", group="Assumptions"));
+  parameter AixLib.Electrical.Types.Load modelMode=AixLib.Electrical.Types.Load.FixedZ_steady_state
+    "Select between steady state and dynamic model"
+    annotation(Evaluate=true, Dialog(tab="Model", group="Assumptions", enable = use_C), choices(choice=AixLib.Electrical.Types.Load.FixedZ_steady_state
+        "Steady state", choice=AixLib.Electrical.Types.Load.FixedZ_dynamic "Dynamic"));
+  parameter Boolean use_T = false
+    "If true, enables the input for the temperature of the cable" annotation(Evaluate = true, Dialog(tab="Model", group="Thermal"));
+  parameter Modelica.Units.SI.Temperature TCable=T_ref
+    "Fixed temperature of the cable" annotation (Dialog(
+      tab="Model",
+      group="Thermal",
+      enable=not use_T));
+
+  parameter AixLib.Electrical.Types.CableMode mode=AixLib.Electrical.Types.CableMode.automatic
+    "Select if choosing the cable automatically or between a list of commercial options"
+    annotation(Evaluate=true, Dialog(tab="Tech. specification", group="Auto/Manual mode"), choicesAllMatching=true);
+
+  replaceable parameter
+    AixLib.Electrical.Transmission.LowVoltageCables.Generic
+     commercialCable constrainedby
+    AixLib.Electrical.Transmission.BaseClasses.BaseCable
+    "Commercial cables options"
+    annotation(Evaluate=true, Dialog(tab="Tech. specification", group="Manual mode",
+    enable = mode == AixLib.Electrical.Types.CableMode.commercial),
+               choicesAllMatching = true);
+
+  final parameter Modelica.Units.SI.Temperature T_ref=commercialCable.T_ref
+    "Reference temperature of the line" annotation (Evaluate=True);
+  final parameter Modelica.Units.SI.Temperature M=commercialCable.M
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))";
+  final parameter Modelica.Units.SI.Resistance R=commercialCable.lineResistance(
+      l,
+      f_n,
+      commercialCable) "Resistance of the cable" annotation (Evaluate=True);
+  final parameter Modelica.Units.SI.Inductance L=commercialCable.lineInductance(
+      l,
+      f_n,
+      commercialCable)
+    "Inductance of the cable due to mutual and self inductance"
+    annotation (Evaluate=True);
+  final parameter Modelica.Units.SI.Capacitance C=
+      commercialCable.lineCapacitance(
+      l,
+      f_n,
+      commercialCable) "Capacitance of the cable" annotation (Evaluate=True);
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature cableTemp
+    "Temperature of the cable"
+    annotation (Placement(transformation(extent={{-60,12},{-40,32}})));
+  Modelica.Blocks.Interfaces.RealInput T if use_T "Temperature of the cable"
+   annotation (
+     Placement(transformation(extent={{-42,28},{-2,68}}), iconTransformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,30})));
+  Modelica.Blocks.Sources.RealExpression cableTemperature(y=T_in)
+    "Temperature of the cable"
+    annotation (Placement(transformation(extent={{-92,12},{-72,32}})));
+protected
+  Modelica.Blocks.Interfaces.RealInput T_in
+    "Internal variable for conditional temperature";
+equation
+  assert(L>=0 and R>=0 and C>=0, "The parameters R,L,C must be positive. Check cable properties and size.");
+  connect(T_in, T);
+
+  if not use_T then
+    T_in = TCable;
+  end if;
+
+  connect(cableTemperature.y, cableTemp.T) annotation (Line(
+      points={{-71,22},{-62,22}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation ( Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+          Text(
+            extent={{-150,-19},{150,-59}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(info="<html>
+<p>
+This partial model contains parameters and variables needed to parametrize a
+generic cable. The resistance, inductance and capacitance
+are computed by the functions associated to the type of cable selected.
+The type of cable is specified using a record that inherits from
+<a href=\"modelica://AixLib.Electrical.Transmission.BaseClasses.BaseCable\">
+AixLib.Electrical.Transmission.BaseClasses.BaseCable</a> such as (
+<a href=\"modelica://AixLib.Electrical.Transmission.LowVoltageCables.Generic\">
+AixLib.Electrical.Transmission.LowVoltageCables.Generic</a> or
+<a href=\"modelica://AixLib.Electrical.Transmission.MediumVoltageCables.Generic\">
+AixLib.Electrical.Transmission.MediumVoltageCables.Generic</a>).
+The record contains functions that depending on the properties of cable compute its
+resistance, inductance or capacitance.
+</p>
+<p>
+The model has two parameters <code>use_C</code> and <code>modelMode</code> that
+change the behaviour of the model. It is possible to include the effects
+of a capacity or select the model to be dynamic or steady state. More information
+are available in the line models that extends this partial model.
+</p>
+
+<h4>Commercial cable mode</h4>
+<p>
+If <code>mode = commercial</code>, the user can select the type of cable from a list
+of commercial cables. The cables are divided in three different categories:
+</p>
+<ul>
+<li>Low voltage,</li>
+<li>Medium voltage, and</li>
+<li>High voltage.</li>
+</ul>
+<p>
+The details and type of cables can be found in
+<a href=\"modelica://AixLib.Electrical.Transmission.LowVoltageCables\">
+AixLib.Electrical.Transmission.LowVoltageCables</a> and
+<a href=\"modelica://AixLib.Electrical.Transmission.MediumVoltageCables\">
+AixLib.Electrical.Transmission.MediumVoltageCables</a>.
+</p>
+
+<h4>Automatic cable mode</h4>
+<p>
+If <code>mode = automatic</code>, the type of cable is automatically selected
+depending on the value of the parameters <code>V_nominal</code> and
+<code>P_nominal</code>.
+</p>
+
+<h4>Note:</h4>
+<p>
+More details about the functions that compute the type of cable and its
+properties can be found in <a href=\"modelica://AixLib.Electrical.Transmission.Functions\">
+AixLib.Electrical.Transmission.Functions</a>.
+</p>
+<p>
+The parameter <code>commercialCable</code> is assumed to be
+<a href=\"modelica://AixLib.Electrical.Transmission.LowVoltageCables.Generic\">
+AixLib.Electrical.Transmission.LowVoltageCables.Generic</a>.
+The parameter is replaceable so it can be redeclared using a different type, for example
+<a href=\"modelica://AixLib.Electrical.Transmission.MediumVoltageCables.Generic\">
+AixLib.Electrical.Transmission.MediumVoltageCables.Generic</a>.<br/>
+The example models
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLineMedium\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLineMedium</a> and
+<a href=\"modelica://AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACSimpleGridMedium\">
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACSimpleGridMedium</a>
+show how this can be done.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Revised model and documentation according to change in the structure of the cable record.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialBaseLine;
diff --git a/AixLib/Electrical/Transmission/BaseClasses/PartialLine.mo b/AixLib/Electrical/Transmission/BaseClasses/PartialLine.mo
new file mode 100644
index 0000000000..5d0492fce4
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/PartialLine.mo
@@ -0,0 +1,43 @@
+within AixLib.Electrical.Transmission.BaseClasses;
+partial model PartialLine "Partial cable line dispersion model"
+  extends AixLib.Electrical.Interfaces.PartialTwoPort;
+  extends AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine;
+  Real VoltageLosses(unit = "1") = abs(PhaseSystem_p.systemVoltage(terminal_p.v) -
+    PhaseSystem_n.systemVoltage(terminal_n.v))/
+    AixLib.Utilities.Math.Functions.smoothMax(
+      PhaseSystem_p.systemVoltage(terminal_p.v),
+      PhaseSystem_n.systemVoltage(terminal_n.v),
+      1.0) "Percentage of voltage losses across the line";
+protected
+  parameter Integer n_ = size(terminal_n.i,1) "Number of cables";
+  parameter Real nominal_i_ = P_nominal / V_nominal
+    "Nominal current flowing through the line";
+  parameter Real nominal_v_ = V_nominal "Nominal voltage of the line";
+
+  annotation ( Icon(coordinateSystem(
+          preserveAspectRatio=false, extent={{-100,-100},{100,100}}), graphics={
+          Text(
+            extent={{-150,-19},{150,-59}},
+            textColor={0,0,0},
+          textString="%name")}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This partial model extends the model <a href=\"modelica://AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine\">
+AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine</a>.
+It adds two generalized electric connectors.
+</p>
+<h4>Note:</h4>
+<p>
+See <a href=\"modelica://AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine\">
+AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine</a> for more information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialLine;
diff --git a/AixLib/Electrical/Transmission/BaseClasses/PartialNetwork.mo b/AixLib/Electrical/Transmission/BaseClasses/PartialNetwork.mo
new file mode 100644
index 0000000000..80cd8476c9
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/PartialNetwork.mo
@@ -0,0 +1,132 @@
+within AixLib.Electrical.Transmission.BaseClasses;
+partial model PartialNetwork "Partial model that represent an electric network"
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=110)
+    "Nominal voltage of the lines in the network";
+  replaceable parameter AixLib.Electrical.Transmission.Grids.PartialGrid grid
+    "Record that describe the grid with the number of nodes, links, connections, etc."
+    annotation (choicesAllMatching=true,
+                Placement(transformation(extent={{40,60},{60,80}})));
+  replaceable AixLib.Electrical.Interfaces.BaseTerminal terminal[grid.nNodes]
+    "Electric terminals for each node of the network"
+    annotation (Placement(transformation(extent={{90,-10},{110,10}})));
+  replaceable AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine lines[grid.nLinks](
+    each mode=AixLib.Electrical.Types.CableMode.commercial,
+    l={grid.l[i, 1] for i in 1:grid.nLinks},
+    each P_nominal=1000,
+    each V_nominal=V_nominal)
+    "Array of line models, each line connecting two nodes of the grid";
+
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillPattern=FillPattern.Solid,
+          fillColor={255,255,255}),
+        Ellipse(
+          extent={{-6,86},{6,74}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-86,46},{-74,34}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-36,-24},{-24,-36}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{74,46},{86,34}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{74,-54},{86,-66}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-6,-74},{6,-86}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-66,6},{-54,-6}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{54,6},{66,-6}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-80,40},{0,80}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-60,0},{0,80}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{0,-80},{60,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{-32,-28},{-60,0}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{80,40},{0,80}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{0,-80},{0,80}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Line(
+          points={{80,-62},{80,40}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Text(
+          extent={{-140,140},{140,100}},
+          textColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          textString="%name")}), Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This partial model represents a generalized electrical network.
+</p>
+<p>
+The model has three main components. The parameter <code>grid</code> declares the type
+<a href=\"modelica://AixLib.Electrical.Transmission.Grids.PartialGrid\">
+AixLib.Electrical.Transmission.Grids.PartialGrid</a>
+that contains the information about the topology of the network, such as
+the number of nodes,
+how they are connected, and the length of each connection.
+The parameter <code>terminal[...]</code> declares
+an array of generalized electric connectors that are associated to each node of the grid.
+The parameter <code>lines[...]</code> is an array of type
+<a href=\"modelica://AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine\">
+AixLib.Electrical.Transmission.BaseClasses.PartialBaseLine</a> that represent the cables
+in the grid.
+</p>
+<h4>Note:</h4>
+<p>
+This is a partial model that once extended can represent either DC or AC networks.
+This model is based on the assumption that the topology of the network does not depend on
+the type of cables that connect the nodes.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialNetwork;
diff --git a/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortInductance.mo b/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortInductance.mo
new file mode 100644
index 0000000000..81c281066a
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortInductance.mo
@@ -0,0 +1,73 @@
+within AixLib.Electrical.Transmission.BaseClasses;
+partial model PartialTwoPortInductance
+  "Partial model of an inductive element that links two electrical connectors"
+  extends Interfaces.PartialTwoPort;
+  parameter Modelica.Units.SI.Inductance L "Inductance"
+    annotation (Evaluate=true);
+equation
+  Connections.branch(terminal_p.theta, terminal_n.theta);
+  terminal_p.theta = terminal_n.theta;
+
+  terminal_p.i = - terminal_n.i;
+
+  annotation (Diagram(graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,255}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Line(points={{70,0},{90,0}},   color={0,0,255})}), Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                                                  graphics={
+          Text(
+            extent={{-142,-30},{144,-62}},
+            textColor={0,0,0},
+          textString="L=%L"),
+          Line(points={{-90,0},{-70,0}}, color={0,0,0}),
+          Line(points={{70,0},{90,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-70,30},{70,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-42,14},{-14,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-14,14},{14,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,14},{42,-14}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-44,0},{44,-16}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Line(
+          points={{0,0},{12,1.46953e-15}},
+          color={0,0,0},
+          origin={-42,0},
+          rotation=180),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{10,1.22461e-15}},
+          color={0,0,0},
+          origin={52,0},
+          rotation=180)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model of an inductance that links two generalized electrical connectors.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialTwoPortInductance;
diff --git a/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortRLC.mo b/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortRLC.mo
new file mode 100644
index 0000000000..e34e959da4
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortRLC.mo
@@ -0,0 +1,132 @@
+within AixLib.Electrical.Transmission.BaseClasses;
+partial model PartialTwoPortRLC
+  "Partial model of an RLC element that links two electrical connectors"
+  extends AixLib.Electrical.Interfaces.PartialTwoPort;
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort(T = T_ref);
+  parameter Modelica.Units.SI.Resistance R "Resistance at temperature T_ref"
+    annotation (Evaluate=true);
+  parameter Modelica.Units.SI.Temperature T_ref=298.15 "Reference temperature";
+  parameter Modelica.Units.SI.Temperature M=507.65
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))";
+  parameter Modelica.Units.SI.Capacitance C "Capacity";
+  parameter Modelica.Units.SI.Inductance L "Inductance";
+  parameter Modelica.Units.SI.Voltage V_nominal(min=0, start=110)
+    "Nominal voltage (V_nominal >= 0)"
+    annotation (Dialog(group="Nominal conditions"));
+  Modelica.Units.SI.Resistance R_actual
+    "Actual resistance = R*(M + T_heatPort)/(M + T_ref) ";
+equation
+  Connections.branch(terminal_p.theta, terminal_n.theta);
+  terminal_p.theta = terminal_n.theta;
+
+  assert(R_actual>=0,
+   "The value of R_actual must be positive, check reference and actual temperatures");
+
+  R_actual =R*(M + Modelica.Units.Conversions.to_degC(T_heatPort))/(M +
+    Modelica.Units.Conversions.to_degC(T_ref));
+
+  annotation (Diagram(graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,255}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Line(points={{70,0},{90,0}},   color={0,0,255})}), Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                                                  graphics={
+          Text(
+            extent={{-148,-28},{138,-60}},
+            textColor={0,0,0},
+          textString="R=%R, L=%L"),
+          Line(points={{-90,0},{-70,0}}, color={0,0,0}),
+          Line(points={{70,0},{90,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-70,32},{70,-28}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+          Line(
+          points={{-6.85214e-44,-8.39117e-60},{96,1.22003e-14}},
+          color={0,0,0},
+          origin={64,16},
+          rotation=180),
+          Line(
+          visible = C > 0,
+          points={{-6.85214e-44,-8.39117e-60},{-4.17982e-15,16}},
+          color={0,0,0},
+          origin={22,16},
+          rotation=180),
+          Line(
+          visible = C > 0,
+          points={{-6.85214e-44,-8.39117e-60},{16,1.95937e-15}},
+          color={0,0,0},
+          origin={30,0},
+          rotation=180),
+          Line(
+          visible = C > 0,
+          points={{-6.85214e-44,-8.39117e-60},{16,1.95937e-15}},
+          color={0,0,0},
+          origin={30,-4},
+          rotation=180),
+          Line(
+          visible = C > 0,
+          points={{-6.85214e-44,-8.39117e-60},{-2.40346e-15,16}},
+          color={0,0,0},
+          origin={22,-4},
+          rotation=180),
+        Line(
+          points={{-66,16},{-60,16},{-58,20},{-54,12},{-50,20},{-46,12},{-42,20},
+              {-38,12},{-36,16},{-32,16}},
+          color={0,0,0},
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-24,22},{-12,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-12,22},{0,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{0,22},{12,10}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-24,16},{12,4}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Text(
+            extent={{-142,-56},{144,-88}},
+            textColor={0,0,0},
+          textString="C=%C")}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model of a resistance that links two generalized electrical connectors.
+</p>
+<p>
+The model computes a resistance <i>R(T)</i> that varies depending on the temperature <i>T</i> as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+R(T) = R<sub>ref</sub> (M + T)/(M + T<sub>ref</sub>),
+</p>
+<p>
+where the resistance <i>R<sub>ref</sub></i> is the reference value of the resistance,
+<i>M</i> is the temperature coefficient of the cable material, and
+<i>T<sub>ref</sub></i> is the reference temperature.
+The temperature <i>T</i> is the temperature of the heat port if <code>useHeatPort = true</code>.
+</p>
+<p>
+The impedance <i>L</i> and the capacity <i>C</i> do not vary with respect to the temperature
+and are specified by the user.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialTwoPortRLC;
diff --git a/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortResistance.mo b/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortResistance.mo
new file mode 100644
index 0000000000..88d9c0943c
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/PartialTwoPortResistance.mo
@@ -0,0 +1,67 @@
+within AixLib.Electrical.Transmission.BaseClasses;
+partial model PartialTwoPortResistance
+  "Partial model of a resistive element that links two electrical connectors"
+  extends Interfaces.PartialTwoPort;
+  extends Modelica.Electrical.Analog.Interfaces.ConditionalHeatPort(T = T_ref);
+  parameter Modelica.Units.SI.Resistance R "Resistance at temperature T_ref";
+  parameter Modelica.Units.SI.Temperature T_ref=298.15 "Reference temperature";
+  parameter Modelica.Units.SI.Temperature M=507.65
+    "Temperature constant (R_actual = R*(M + T_heatPort)/(M + T_ref))";
+  Modelica.Units.SI.Resistance R_actual
+    "Actual resistance = R*(M + T_heatPort)/(M + T_ref) ";
+equation
+  Connections.branch(terminal_p.theta, terminal_n.theta);
+  terminal_p.theta = terminal_n.theta;
+
+  assert(R_actual>=0,
+   "The value of R_actual must be positive, check reference and actual temperatures.");
+
+  R_actual =R*(M + Modelica.Units.Conversions.to_degC(T_heatPort))/(M +
+    Modelica.Units.Conversions.to_degC(T_ref));
+
+  terminal_p.i = - terminal_n.i;
+
+  annotation (Diagram(graphics={
+          Rectangle(extent={{-70,30},{70,-30}}, lineColor={0,0,255}),
+          Line(points={{-90,0},{-70,0}}, color={0,0,255}),
+          Line(points={{70,0},{90,0}},   color={0,0,255})}), Icon(
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+                                                                  graphics={
+          Text(
+            extent={{-142,-30},{144,-62}},
+            textColor={0,0,0},
+          textString="R=%R"),
+          Line(points={{-90,0},{-70,0}}, color={0,0,0}),
+          Line(points={{70,0},{90,0}}, color={0,0,0}),
+        Rectangle(
+          extent={{-70,30},{70,-30}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}),
+    Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model of a resistance that links two generalized electrical connectors.
+</p>
+<p>
+The model computes a resistance <i>R(T)</i> that varies depending on the temperature <i>T</i> as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+R(T) = R<sub>ref</sub> (M + T)/(M + T<sub>ref</sub>),
+</p>
+<p>
+where the resistance <i>R<sub>ref</sub></i> is the reference value of the resistance,
+<i>M</i> is the temperature coefficient of the cable material,
+and <i>T<sub>ref</sub></i> is the reference temperature.
+The temperature <i>T</i> is the temperature of the heat port
+if <code>useHeatPort = true</code>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialTwoPortResistance;
diff --git a/AixLib/Electrical/Transmission/BaseClasses/package.mo b/AixLib/Electrical/Transmission/BaseClasses/package.mo
new file mode 100644
index 0000000000..3fec32338f
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.Transmission;
+package BaseClasses "Package that contains partial models for lines and cables"
+  extends Modelica.Icons.BasesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains partial models that describe electric
+lines and cables.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Electrical/Transmission/BaseClasses/package.order b/AixLib/Electrical/Transmission/BaseClasses/package.order
new file mode 100644
index 0000000000..70fcbed17b
--- /dev/null
+++ b/AixLib/Electrical/Transmission/BaseClasses/package.order
@@ -0,0 +1,7 @@
+PartialBaseLine
+PartialLine
+PartialNetwork
+PartialTwoPortInductance
+PartialTwoPortRLC
+PartialTwoPortResistance
+BaseCable
diff --git a/AixLib/Electrical/Transmission/Functions/R_AC_correction.mo b/AixLib/Electrical/Transmission/Functions/R_AC_correction.mo
new file mode 100644
index 0000000000..966975319c
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/R_AC_correction.mo
@@ -0,0 +1,294 @@
+within AixLib.Electrical.Transmission.Functions;
+function R_AC_correction
+  "This function computes the correction factor of the DC resistance for AC systems at 60 Hz"
+  input String size "Size of the commercial cable (AWG or kcmil)";
+  input AixLib.Electrical.Transmission.Types.Material material
+    "Material of the cable";
+  output Real correction "Correction factor";
+algorithm
+  if material == AixLib.Electrical.Transmission.Types.Material.Al then
+    if size == "1/0" then
+      correction := 1.0;
+    elseif size == "2/0" then
+      correction := 1.001;
+    elseif size == "3/0" then
+      correction := 1.001;
+    elseif size == "4/0" then
+      correction := 1.001;
+    elseif size == "250" then
+      correction := 1.002;
+    elseif size == "300" then
+      correction := 1.003;
+    elseif size == "350" then
+      correction := 1.004;
+    elseif size == "400" then
+      correction := 1.005;
+    elseif size == "500" then
+      correction := 1.007;
+    elseif size == "600" then
+      correction := 1.01;
+    elseif size == "700" then
+      correction := 1.013;
+    elseif size == "750" then
+      correction := 1.015;
+    elseif size == "800" then
+      correction := 1.017;
+    elseif size == "1000" then
+      correction := 1.026;
+    elseif size == "1250" then
+      correction := 1.04;
+    elseif size == "1500" then
+      correction := 1.058;
+    elseif size == "1750" then
+      correction := 1.079;
+    elseif size == "2000" then
+      correction := 1.1;
+    elseif size == "2500" then
+      correction := 1.142;
+    else
+      correction := 1.0;
+    end if;
+
+  elseif material == AixLib.Electrical.Transmission.Types.Material.Cu then
+    if size == "1/0" then
+      correction := 1.0;
+    elseif size == "2/0" then
+      correction := 1.001;
+    elseif size == "3/0" then
+      correction := 1.002;
+    elseif size == "4/0" then
+      correction := 1.004;
+    elseif size == "250" then
+      correction := 1.005;
+    elseif size == "300" then
+      correction := 1.006;
+    elseif size == "350" then
+      correction := 1.009;
+    elseif size == "400" then
+      correction := 1.011;
+    elseif size == "500" then
+      correction := 1.018;
+    elseif size == "600" then
+      correction := 1.025;
+    elseif size == "700" then
+      correction := 1.034;
+    elseif size == "750" then
+      correction := 1.039;
+    elseif size == "800" then
+      correction := 1.044;
+    elseif size == "1000" then
+      correction := 1.067;
+    elseif size == "1250" then
+      correction := 1.102;
+    elseif size == "1500" then
+      correction := 1.142;
+    elseif size == "1750" then
+      correction := 1.185;
+    elseif size == "2000" then
+      correction := 1.233;
+    elseif size == "2500" then
+      correction := 1.326;
+    else
+      correction := 1.0;
+    end if;
+  else
+    assert(material <> AixLib.Electrical.Transmission.Types.Material.Al and
+           material <> AixLib.Electrical.Transmission.Types.Material.Cu,
+    "In function AixLib.Electrical.Transmission.Functions.R_AC_Correction,
+    does not support material " + String(material) + ".
+    The selected cable has the R_AC_Correction of the Copper.",
+    level = AssertionLevel.warning);
+
+    correction := 1.0;
+  end if;
+annotation(Inline = true, Documentation(revisions="<html>
+<ul>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added warning instead of print.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes a correction factor for adapting the DC resistance
+when working with AC voltages. The correction factor assumes <i>f = 60 Hz</i>.
+</p>
+<p>
+The correction is based on the type of cabel (AWG or kcmil) and the material.
+</p>
+
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<th>Type (AWG or kcmil)</th>
+<th>Material</th>
+<th>Correction factor</th>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1/0</td><td>Aluminium</td><td>1.0</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>2/0</td><td>Aluminium</td><td>1.001</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>3/0</td><td>Aluminium</td><td>1.001</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>4/0</td><td>Aluminium</td><td>1.001</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>250</td><td>Aluminium</td><td>1.002</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>300</td><td>Aluminium</td><td>1.003</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>350</td><td>Aluminium</td><td>1.004</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>400</td><td>Aluminium</td><td>1.005</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>500</td><td>Aluminium</td><td>1.007</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>600</td><td>Aluminium</td><td>1.010</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>700</td><td>Aluminium</td><td>1.013</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>750</td><td>Aluminium</td><td>1.015</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>800</td><td>Aluminium</td><td>1.017</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1000</td><td>Aluminium</td><td>1.026</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1250</td><td>Aluminium</td><td>1.040</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1500</td><td>Aluminium</td><td>1.058</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1750</td><td>Aluminium</td><td>1.079</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>2000</td><td>Aluminium</td><td>1.100</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>2500</td><td>Aluminium</td><td>1.142</td>
+</tr>
+</table>
+
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<th>Type (AWG or kcmil)</th>
+<th>Material</th>
+<th>Correction factor</th>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1/0</td><td>Copper</td><td>1.0</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>2/0</td><td>Copper</td><td>1.001</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>3/0</td><td>Copper</td><td>1.002</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>4/0</td><td>Copper</td><td>1.004</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>250</td><td>Copper</td><td>1.005</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>300</td><td>Copper</td><td>1.006</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>350</td><td>Copper</td><td>1.009</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>400</td><td>Copper</td><td>1.011</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>500</td><td>Copper</td><td>1.018</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>600</td><td>Copper</td><td>1.025</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>700</td><td>Copper</td><td>1.034</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>750</td><td>Copper</td><td>1.039</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>800</td><td>Copper</td><td>1.044</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1000</td><td>Copper</td><td>1.067</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1250</td><td>Copper</td><td>1.102</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1500</td><td>Copper</td><td>1.142</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>1750</td><td>Copper</td><td>1.185</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>2000</td><td>Copper</td><td>1.233</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>2500</td><td>Copper</td><td>1.326</td>
+</tr>
+</table>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end R_AC_correction;
diff --git a/AixLib/Electrical/Transmission/Functions/Validation/SelectCable_low.mo b/AixLib/Electrical/Transmission/Functions/Validation/SelectCable_low.mo
new file mode 100644
index 0000000000..03aec75237
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/Validation/SelectCable_low.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.Functions.Validation;
+model SelectCable_low
+  "Validation model for the function that selects the cable"
+  extends Modelica.Icons.Example;
+
+  parameter Modelica.Units.SI.Voltage V_nominal=480 "Rated voltage";
+
+  parameter Modelica.Units.SI.Power[:] P_nominal=I_nominal*V_nominal/
+      safety_factor "Rated power";
+  parameter Modelica.Units.SI.Current[:] I_nominal={65,95,110,130,170,220,230}
+       .- 10 "Nominal current";
+
+  parameter Real safety_factor = 1.2 "Safety factor";
+
+  parameter AixLib.Electrical.Transmission.LowVoltageCables.Generic[:] cab = AixLib.Electrical.Transmission.Functions.selectCable_low(
+    P_nominal = P_nominal,
+    V_nominal = V_nominal)
+    "Selected cable";
+
+annotation (
+experiment(Tolerance=1e-6, StopTime=1.0),
+  __Dymola_Commands(
+file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/Transmission/Functions/Validation/SelectCable_low.mos"
+"Simulate and plot"),
+Documentation(info="<html>
+<p>
+This model validates
+<a href=\"modelica://AixLib.Electrical.Transmission.Functions.selectCable_low\">
+AixLib.Electrical.Transmission.Functions.selectCable_low</a>
+for a different range of currents.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end SelectCable_low;
diff --git a/AixLib/Electrical/Transmission/Functions/Validation/SelectCable_med.mo b/AixLib/Electrical/Transmission/Functions/Validation/SelectCable_med.mo
new file mode 100644
index 0000000000..636d0ba868
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/Validation/SelectCable_med.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.Functions.Validation;
+model SelectCable_med
+  "Validation model for the function that selects the cable"
+  extends Modelica.Icons.Example;
+
+  parameter Modelica.Units.SI.Voltage V_nominal=25e3 "Rated voltage";
+
+  parameter Modelica.Units.SI.Power[:] P_nominal=I_nominal*V_nominal/
+      safety_factor "Rated power";
+  parameter Modelica.Units.SI.Current[:] I_nominal={195,250,285,375,450,640,800}
+       .- 10 "Nominal current";
+
+  parameter Real safety_factor = 1.2 "Safety factor";
+
+  parameter AixLib.Electrical.Transmission.MediumVoltageCables.Generic[:] cab = AixLib.Electrical.Transmission.Functions.selectCable_med(
+    P_nominal = P_nominal,
+    V_nominal = V_nominal)
+    "Selected cable";
+
+annotation (
+experiment(Tolerance=1e-6, StopTime=1.0),
+  __Dymola_Commands(
+file="modelica://AixLib/Resources/Scripts/Dymola/Electrical/Transmission/Functions/Validation/SelectCable_med.mos"
+"Simulate and plot"),
+Documentation(info="<html>
+<p>
+This model validates
+<a href=\"modelica://AixLib.Electrical.Transmission.Functions.selectCable_med\">
+AixLib.Electrical.Transmission.Functions.selectCable_med</a>
+for a different range of currents.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 25, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end SelectCable_med;
diff --git a/AixLib/Electrical/Transmission/Functions/Validation/package.mo b/AixLib/Electrical/Transmission/Functions/Validation/package.mo
new file mode 100644
index 0000000000..eb9831ea10
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/Validation/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.Transmission.Functions;
+package Validation
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+This package contains validation models for the classes in
+<a href=\"modelica://AixLib.Electrical.Transmission.Functions\">
+AixLib.Electrical.Transmission.Functions</a>.
+</p>
+<p>
+Note that most validation models contain simple input data which may not be realistic,
+but for which the correct output can be obtained through an analytic solution.
+The examples plot various outputs, which have been verified against these solutions.
+These model outputs are stored as reference data and used for continuous validation
+whenever models in the library change.
+</html>"));
+end Validation;
diff --git a/AixLib/Electrical/Transmission/Functions/Validation/package.order b/AixLib/Electrical/Transmission/Functions/Validation/package.order
new file mode 100644
index 0000000000..17fc38e447
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/Validation/package.order
@@ -0,0 +1,2 @@
+SelectCable_low
+SelectCable_med
diff --git a/AixLib/Electrical/Transmission/Functions/computeGMD.mo b/AixLib/Electrical/Transmission/Functions/computeGMD.mo
new file mode 100644
index 0000000000..d6c705c04a
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/computeGMD.mo
@@ -0,0 +1,33 @@
+within AixLib.Electrical.Transmission.Functions;
+function computeGMD
+  "This function computes the geometric mean distance of a three-phase transmission line"
+  input Modelica.Units.SI.Length d1 "Distance between conductors";
+  input Modelica.Units.SI.Length d2=d1 "Distance between conductors";
+  input Modelica.Units.SI.Length d3=2*d1 "Distance between conductors";
+  output Modelica.Units.SI.Length GMD "Geometric Mean Distance";
+algorithm
+  GMD := (d1*d2*d3)^(1.0/3.0);
+annotation(Inline = true, Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the Geometric Mean Distance of a cable.
+</p>
+<p>
+The GMD is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+GMD = (d<sub>1</sub> d<sub>2</sub> d<sub>3</sub>)<sup>1/3</sup>,
+</p>
+<p>
+where <i>d<sub>1</sub></i>, <i>d<sub>2</sub></i>, and <i>d<sub>3</sub></i> are
+ the distances between the conductors.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end computeGMD;
diff --git a/AixLib/Electrical/Transmission/Functions/computeGMR.mo b/AixLib/Electrical/Transmission/Functions/computeGMR.mo
new file mode 100644
index 0000000000..062944c23f
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/computeGMR.mo
@@ -0,0 +1,61 @@
+within AixLib.Electrical.Transmission.Functions;
+function computeGMR
+  "This function computes the geometric mean radius of a cable with 1 to 4 conductors"
+  input Modelica.Units.SI.Length d "Diameter of the conductor";
+  input Integer N = 1 "Number of conductors";
+  output Modelica.Units.SI.Length GMR "Geometric Mean Radius";
+algorithm
+  assert(N > 0 and N < 5,
+    "The number of conductors N must be between 1 and 4, received N=" + String(N) + ".");
+  if N==1 then
+    GMR := 0.5*d*0.7788;
+  elseif N==2 then
+    GMR := sqrt(d);
+  elseif N==3 then
+    GMR := (d^2)^(1/3);
+  else // N == 4
+    GMR := 1.09*(d^3)^(1/4);
+  end if;
+annotation(Inline = true, Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the Geometric Mean Radius (GMR) of a cable.
+</p>
+<p>
+The GMR is computed as follow, depending on the number of conductors <i>N</i>
+that are part of the cable, and the diamater of the conductor <i>d</i>.
+</p>
+
+<table summary=\"equations\" border = \"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collape;\">
+<tr><th>Equation</th><th>Condition</th></tr>
+<tr>
+<td>0.7788 (d/2) </td>
+<td>N = 1</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>d<sup>1/2</sup></td>
+<td>N = 2</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>d<sup>2/3</sup></td>
+<td>N = 3</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td>d<sup>2/3</sup></td>
+<td>N = 4</td>
+</tr>
+<!-- ************ -->
+</table>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end computeGMR;
diff --git a/AixLib/Electrical/Transmission/Functions/package.mo b/AixLib/Electrical/Transmission/Functions/package.mo
new file mode 100644
index 0000000000..78c5d2a268
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.Transmission;
+package Functions "Package that contains functions to compute cable properties"
+  extends Modelica.Icons.Package;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains various functions that are used to compute
+cable properties and select the default cable during
+automatic parametrization.
+</p>
+</html>"));
+end Functions;
diff --git a/AixLib/Electrical/Transmission/Functions/package.order b/AixLib/Electrical/Transmission/Functions/package.order
new file mode 100644
index 0000000000..d62457d0b8
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/package.order
@@ -0,0 +1,7 @@
+R_AC_correction
+computeGMD
+computeGMR
+selectCable_low
+selectCable_med
+selectVoltageLevel
+Validation
diff --git a/AixLib/Electrical/Transmission/Functions/selectCable_low.mo b/AixLib/Electrical/Transmission/Functions/selectCable_low.mo
new file mode 100644
index 0000000000..aaa94f68c5
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/selectCable_low.mo
@@ -0,0 +1,91 @@
+within AixLib.Electrical.Transmission.Functions;
+function selectCable_low "This function is used to automatically select the
+    type of cable for low voltages"
+  input Modelica.Units.SI.Power P_nominal=0 "Rated power";
+  input Modelica.Units.SI.Voltage V_nominal=0 "Rated voltage";
+  output AixLib.Electrical.Transmission.LowVoltageCables.Generic cable "Cable";
+protected
+  parameter Real safety_factor = 1.2;
+  Modelica.Units.SI.Current I_nominal
+    "Nominal current flowing through the line";
+  AixLib.Electrical.Transmission.LowVoltageCables.Cu10 cu10;
+  AixLib.Electrical.Transmission.LowVoltageCables.Cu20 cu20;
+  AixLib.Electrical.Transmission.LowVoltageCables.Cu25 cu25;
+  AixLib.Electrical.Transmission.LowVoltageCables.Cu35 cu35;
+  AixLib.Electrical.Transmission.LowVoltageCables.Cu50 cu50;
+  AixLib.Electrical.Transmission.LowVoltageCables.Cu95 cu95;
+  AixLib.Electrical.Transmission.LowVoltageCables.Cu100 cu100;
+algorithm
+
+  assert(Transmission.Functions.selectVoltageLevel(V_nominal) == AixLib.Electrical.Types.VoltageLevel.Low,
+  "In function AixLib.Electrical.Transmission.Functions.selectCable_low,
+  cable autosizing has a nominal Voltage " + String(V_nominal) + " [V].
+  The low voltage cables do not support such a voltage level.",
+  level=AssertionLevel.error);
+
+  // Check if it's possible to compute the current
+  if V_nominal > 0 then
+    I_nominal :=safety_factor*P_nominal/V_nominal;
+  else
+    I_nominal :=0;
+  end if;
+
+  // Assumed the material is Copper
+  if I_nominal < cu10.Amp then
+        cable := cu10;
+  elseif I_nominal >= cu10.Amp and I_nominal < cu20.Amp then
+        cable := cu20;
+  elseif I_nominal >= cu20.Amp and I_nominal < cu25.Amp then
+        cable := cu25;
+  elseif I_nominal >= cu25.Amp and I_nominal < cu35.Amp then
+        cable := cu35;
+  elseif I_nominal >= cu35.Amp and I_nominal < cu50.Amp then
+        cable := cu50;
+  elseif I_nominal >= cu50.Amp and I_nominal < cu95.Amp then
+        cable := cu95;
+  elseif I_nominal >= cu95.Amp and I_nominal < cu100.Amp then
+        cable := cu100;
+  else
+    assert(I_nominal < cu100.Amp,
+"In function AixLib.Electrical.Transmission.Functions.selectCable_low,
+  cable autosizing does not support a current of " + String(I_nominal) + " [A].
+  The selected cable will be undersized.",
+  level=AssertionLevel.warning);
+        cable := cu100;
+  end if;
+annotation(Inline = true, Documentation(revisions="<html>
+<ul>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added warning instead of print.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function selects the default cable for a low voltage
+transmission line.
+</p>
+<p>
+The function takes as inputs the nominal voltage <i>V<sub>nominal</sub></i> and the
+nominal power <i>P<sub>nominal</sub></i>. It computes the maximum current current that
+can flow through the cable as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+I<sub>MAX</sub> = S<sub>F</sub> P<sub>nominal</sub> / V<sub>nominal</sub>,
+</p>
+<p>
+where <i>S<sub>F</sub></i> is the safety factor. By default the safety factor is equal to <i>1.2</i>.
+</p>
+<p>
+Using <i>I<sub>MAX</sub></i>, the function selects the smallest cable that has an ampacity
+higher than I<sub>MAX</sub>. The cables are selected from
+<a href=\"modelica://AixLib.Electrical.Transmission.LowVoltageCables\">
+AixLib.Electrical.Transmission.LowVoltageCables</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end selectCable_low;
diff --git a/AixLib/Electrical/Transmission/Functions/selectCable_med.mo b/AixLib/Electrical/Transmission/Functions/selectCable_med.mo
new file mode 100644
index 0000000000..ff9c9e4aa1
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/selectCable_med.mo
@@ -0,0 +1,92 @@
+within AixLib.Electrical.Transmission.Functions;
+function selectCable_med "This function is used to automatically select the
+    type of cable for medium voltages"
+  input Modelica.Units.SI.Power P_nominal=0 "Rated power";
+  input Modelica.Units.SI.Voltage V_nominal=0 "Rated voltage";
+  output AixLib.Electrical.Transmission.MediumVoltageCables.Generic cable "Cable";
+protected
+  parameter Real safety_factor = 1.2;
+  Modelica.Units.SI.Current I_nominal
+    "Nominal current flowing through the line";
+  AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_10 Al10;
+  AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_30 Al30;
+  AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_40 Al40;
+  AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_350 Al350;
+  AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_500 Al500;
+  AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_1000 Al1000;
+  AixLib.Electrical.Transmission.MediumVoltageCables.Annealed_Al_1500 Al1500;
+algorithm
+
+  assert(Transmission.Functions.selectVoltageLevel(V_nominal) == AixLib.Electrical.Types.VoltageLevel.Medium,
+  "In function AixLib.Electrical.Transmission.Functions.selectCable_med,
+  cable autosizing has a nominal Voltage " + String(V_nominal) + " [V].
+  The medium voltage cables do not support such a voltage level.",
+  level=AssertionLevel.error);
+
+  // Check if it's possible to compute the current
+  if V_nominal > 0 then
+    I_nominal :=safety_factor*P_nominal/V_nominal;
+  else
+    I_nominal :=0;
+  end if;
+
+  // Assumed the material is Copper
+  if I_nominal < Al10.Amp then
+        cable := Al10;
+  elseif I_nominal >= Al10.Amp and I_nominal < Al30.Amp then
+        cable := Al30;
+  elseif I_nominal >= Al30.Amp and I_nominal < Al40.Amp then
+        cable := Al40;
+  elseif I_nominal >= Al40.Amp and I_nominal < Al350.Amp then
+        cable := Al350;
+  elseif I_nominal >= Al350.Amp and I_nominal < Al500.Amp then
+        cable := Al500;
+  elseif I_nominal >= Al500.Amp and I_nominal < Al1000.Amp then
+        cable := Al1000;
+  elseif I_nominal >= Al1000.Amp and I_nominal < Al1500.Amp then
+        cable := Al1500;
+  else
+    assert(I_nominal < Al1500.Amp,
+"Warning: In function AixLib.Electrical.Transmission.Functions.selectCable_med,
+  cable autosizing does not support a current of " + String(I_nominal) + " [A].
+  The selected cable will be undersized.",
+  level=AssertionLevel.warning);
+
+        cable := Al10;
+  end if;
+annotation(Inline = true, Documentation(revisions="<html>
+<ul>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added warning instead of print.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function selects the default cable for a medium voltage
+transmission line.
+</p>
+<p>
+The function takes as inputs the nominal voltage <i>V<sub>nominal</sub></i> and the
+nominal power <i>P<sub>nominal</sub></i>. It computes the maximum current current that
+can flow through the cable as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+I<sub>MAX</sub> = S<sub>F</sub> P<sub>nominal</sub> / V<sub>nominal</sub>,
+</p>
+<p>
+where <i>S<sub>F</sub></i> is the safety factor. By default the safety factor is equal to <i>1.2</i>.
+</p>
+<p>
+Using <i>I<sub>MAX</sub></i>, the function selects the smallest cable that has an ampacity
+higher than I<sub>MAX</sub>. The cables are selected from
+<a href=\"modelica://AixLib.Electrical.Transmission.MediumVoltageCables\">
+AixLib.Electrical.Transmission.MediumVoltageCables</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end selectCable_med;
diff --git a/AixLib/Electrical/Transmission/Functions/selectVoltageLevel.mo b/AixLib/Electrical/Transmission/Functions/selectVoltageLevel.mo
new file mode 100644
index 0000000000..5c02108889
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Functions/selectVoltageLevel.mo
@@ -0,0 +1,62 @@
+within AixLib.Electrical.Transmission.Functions;
+function selectVoltageLevel
+  "This function computes the voltage level (low, medium or high) given the nominal voltage"
+  input Modelica.Units.SI.Voltage V "Nominal voltage";
+  output AixLib.Electrical.Types.VoltageLevel level "Type of voltage level";
+algorithm
+  if V <= 0 then
+    assert(V > 0,
+     "In function AixLib.Electrical.Transmission.Functions.selectVoltageLevel,
+      does not support a voltage of " + String(V) + " [V].
+      The selected voltage level will be assumed to be low.",
+      level = AssertionLevel.warning);
+    level := AixLib.Electrical.Types.VoltageLevel.Low;
+  elseif V <= 1000 then
+    level := AixLib.Electrical.Types.VoltageLevel.Low;
+  elseif V > 1000 and V <= 50000 then
+    level := AixLib.Electrical.Types.VoltageLevel.Medium;
+  else
+    level := AixLib.Electrical.Types.VoltageLevel.High;
+  end if;
+annotation(Inline = true, Documentation(revisions="<html>
+<ul>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added warning instead of print.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the voltage level for a given voltage.
+The computation is as follows:
+</p>
+
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<th>Condition</th>
+<th>Voltage Level</th>
+</tr>
+<!-- ************ -->
+<tr>
+<td><i>0 &le; V &lt; 1 kV</i></td>
+<td>Low voltage</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td><i>1 kV &le; V &lt; 50 kV</i></td>
+<td>Medium voltage</td>
+</tr>
+<!-- ************ -->
+<tr>
+<td><i> V &ge; 50 kV</i></td>
+<td>HIgh voltage</td>
+</tr>
+</table>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end selectVoltageLevel;
diff --git a/AixLib/Electrical/Transmission/Grids/IEEE_34_AL120.mo b/AixLib/Electrical/Transmission/Grids/IEEE_34_AL120.mo
new file mode 100644
index 0000000000..69ae6b64d7
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Grids/IEEE_34_AL120.mo
@@ -0,0 +1,73 @@
+within AixLib.Electrical.Transmission.Grids;
+record IEEE_34_AL120 "Grid model inspired to the IEEE 34 Node test feeder"
+  extends AixLib.Electrical.Transmission.Grids.PartialGrid(
+    nNodes=34,
+    nLinks=33,
+    l=[48;16;16;40;32;16;16;16;16;16;16;32;32;16;32;32;32;48;48;32;32;16;16;16;
+        16;16;32;32;16;32;16;16;16],
+    fromTo=[[1,2]; [2,3]; [3,4]; [4,5]; [4,6]; [6,7]; [7,8]; [9,26]; [10,26]; [
+        11,9]; [12,11]; [13,10]; [14,10]; [15,14]; [16,15]; [17,27]; [18,27]; [
+        19,31]; [20,31]; [21,32]; [22,32]; [23,20]; [24,23]; [25,24]; [26,8]; [
+        27,29]; [28,16]; [29,16]; [30,17]; [31,17]; [32,19]; [33,22]; [34,18]],
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Generic cables=
+       {LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl120(),
+        LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl120(),
+        LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl120(),
+        LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl120(),
+        LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl120(),
+        LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl120(),
+        LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl120(),
+        LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl70(),
+        LowVoltageCables.PvcAl70(),LowVoltageCables.PvcAl35(),
+        LowVoltageCables.PvcAl35(),LowVoltageCables.PvcAl35(),
+        LowVoltageCables.PvcAl35(),LowVoltageCables.PvcAl35(),
+        LowVoltageCables.PvcAl35(),LowVoltageCables.PvcAl35(),
+        LowVoltageCables.PvcAl120(),LowVoltageCables.PvcAl70(),
+        LowVoltageCables.PvcAl70(),LowVoltageCables.PvcAl70(),
+        LowVoltageCables.PvcAl70(),LowVoltageCables.PvcAl70(),
+        LowVoltageCables.PvcAl35(),LowVoltageCables.PvcAl35(),
+        LowVoltageCables.PvcAl70()});
+
+   /*
+   LEFT HERE TO CHECK CONSISTENCY
+
+   LenVec={
+   0,48,16,16,40,
+   32,16,16,16,16,
+   16,16,32,32,16,
+   32,32,32,48,48,
+   32,32,16,16,16,
+   16,16,32,32,16,
+   32,16,16,16},
+
+    CabTyp={
+               ,.PvcAl120(),.PvcAl120(),.PvcAl120(),.PvcAl120(),
+    .PvcAl120(),.PvcAl120(),.PvcAl120(),.PvcAl120(),.PvcAl120(),
+    .PvcAl120(),.PvcAl120(),.PvcAl120(),.PvcAl120(),.PvcAl120(),
+    .PvcAl120(),.PvcAl70(),.PvcAl70(),.PvcAl35(),.PvcAl35(),
+    .PvcAl35(),.PvcAl35(),.PvcAl35(),.PvcAl35(),.PvcAl35(),
+    .PvcAl120(),.PvcAl70(),.PvcAl70(),.PvcAl70(),.PvcAl70(),
+    .PvcAl70(),.PvcAl35(),.PvcAl35(),.PvcAl70()});
+
+   */
+  annotation (Documentation(info="<html>
+<p> This model represents a grid inspired by the IEEE 34 node test feeder.
+In this example, the cable types and lengths have been modified in order to
+represent a typical distribution feeder.</p>
+<p>The following three type of cables are in the grid: AL120, AL70, and Al35.
+</p>
+<p><img alt=\"alt-image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/IEEE_34.png\"/></p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added redeclare statement needed to specify the type of cables used in the array.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end IEEE_34_AL120;
diff --git a/AixLib/Electrical/Transmission/Grids/PartialGrid.mo b/AixLib/Electrical/Transmission/Grids/PartialGrid.mo
new file mode 100644
index 0000000000..be45c2a26c
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Grids/PartialGrid.mo
@@ -0,0 +1,48 @@
+within AixLib.Electrical.Transmission.Grids;
+record PartialGrid "Partial model that represents a generalized grid"
+  extends Modelica.Icons.MaterialProperty;
+  parameter Integer nNodes "Number of nodes of the grid";
+  parameter Integer nLinks "Number of links connecting the nodes";
+  parameter Integer fromTo[nLinks,2]
+    "Indexes [i,1]->[i,2] of the nodes connected by link i";
+  parameter Modelica.Units.SI.Length l[nLinks,1](each min=0)
+    "Length of the cable";
+  replaceable AixLib.Electrical.Transmission.BaseClasses.BaseCable cables[nLinks]
+    "Array that contains the characteristics of each cable";
+  annotation (Documentation(info="<html>
+<p>
+This abstract grid model specifies the topology of the network by
+</p>
+<ul>
+<li>the number of nodes,</li>
+<li>the number of links,</li>
+<li>the length of links, and</li>
+<li>the connection between links and nodes.</li>
+</ul>
+<p>
+The picture below describes the meaning of the
+values contained in the matrices.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/partialGrid.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Revised model structure. Now the type of the cable is replaceable
+so it's possible to use either low voltage or medium voltage cable.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"), Icon(graphics={
+        Text(
+          textColor={0,0,255},
+          extent={{-154,104},{146,144}},
+          textString="%name")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialGrid;
diff --git a/AixLib/Electrical/Transmission/Grids/TestGrid2Nodes.mo b/AixLib/Electrical/Transmission/Grids/TestGrid2Nodes.mo
new file mode 100644
index 0000000000..73c0a068d1
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Grids/TestGrid2Nodes.mo
@@ -0,0 +1,33 @@
+within AixLib.Electrical.Transmission.Grids;
+record TestGrid2Nodes "Simple model of a grid with 2 nodes and 1 link"
+  extends AixLib.Electrical.Transmission.Grids.PartialGrid(
+    nNodes=2,
+    nLinks=1,
+    fromTo=[[1,2]],
+    l=[200],
+    redeclare AixLib.Electrical.Transmission.LowVoltageCables.Generic
+    cables = {LowVoltageCables.Cu35()});
+  annotation (Documentation(info="<html>
+<p>
+This model represents a simple grid with two nodes and a single link between them.
+</p>
+<p>
+The picture below describes the grid topology.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/testGrid2Nodes.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added redeclare statement needed to specify the type of cables used in the array.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TestGrid2Nodes;
diff --git a/AixLib/Electrical/Transmission/Grids/TestGrid2NodesMedium.mo b/AixLib/Electrical/Transmission/Grids/TestGrid2NodesMedium.mo
new file mode 100644
index 0000000000..5fd863bd0c
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Grids/TestGrid2NodesMedium.mo
@@ -0,0 +1,38 @@
+within AixLib.Electrical.Transmission.Grids;
+record TestGrid2NodesMedium
+  "Simple model of a grid with 2 nodes and 1 link for medium voltage"
+  extends AixLib.Electrical.Transmission.Grids.PartialGrid(
+    nNodes=2,
+    nLinks=1,
+    fromTo=[[1,2]],
+    l=[200],
+    redeclare AixLib.Electrical.Transmission.MediumVoltageCables.Generic
+    cables = {MediumVoltageCables.Annealed_Al_30()});
+  annotation (Documentation(info="<html>
+<p>
+This model represents a simple grid with two nodes and a single link between them.
+This model differs from
+<a href=\"modelica://AixLib.Electrical.Transmission.Grids.TestGrid2Nodes\">
+AixLib.Electrical.Transmission.Grids.TestGrid2Nodes</a> because it defines a medium voltage
+cable instead of a low voltage cable.
+</p>
+<p>
+The picture below describes the grid topology.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Transmission/Grids/testGrid2Nodes.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added redeclare statement needed to specify the type of cables used in the array.
+</li>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TestGrid2NodesMedium;
diff --git a/AixLib/Electrical/Transmission/Grids/package.mo b/AixLib/Electrical/Transmission/Grids/package.mo
new file mode 100644
index 0000000000..ff25c3dc05
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Grids/package.mo
@@ -0,0 +1,25 @@
+within AixLib.Electrical.Transmission;
+package Grids "Package that contains different types of grids"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains different types of grids that can be used to represent
+electrical networks. The topology of the network is specified by
+</p>
+<ul>
+<li>the number of nodes,</li>
+<li>the number of links,</li>
+<li>the length of links, and</li>
+<li>the connection between links and nodes.</li>
+</ul>
+</html>"));
+end Grids;
diff --git a/AixLib/Electrical/Transmission/Grids/package.order b/AixLib/Electrical/Transmission/Grids/package.order
new file mode 100644
index 0000000000..ea44995adc
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Grids/package.order
@@ -0,0 +1,4 @@
+IEEE_34_AL120
+PartialGrid
+TestGrid2Nodes
+TestGrid2NodesMedium
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/Cu10.mo b/AixLib/Electrical/Transmission/LowVoltageCables/Cu10.mo
new file mode 100644
index 0000000000..6f6af505e2
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/Cu10.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record Cu10 "Cu cable 10 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Cu,
+    M = 234.5 + 273.15,
+    Amp=65,
+    RCha=1.81e-003,
+    XCha=0.076e-003);
+  annotation (Documentation(info="<html>
+<p>
+Copper cable with a cross-sectional area of 10mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 1.810-003 // Characteristic resistance [Ohm/m]
+XCha = 0.076e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Cu10;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/Cu100.mo b/AixLib/Electrical/Transmission/LowVoltageCables/Cu100.mo
new file mode 100644
index 0000000000..6283c03d18
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/Cu100.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record Cu100 "Cu cable 100 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Cu,
+    M = 234.5 + 273.15,
+    Amp = 230,
+    RCha=0.181e-003,
+    XCha=0.072e-003);
+  annotation (Documentation(info="<html>
+<p>
+Copper cable with a cross-sectional area of 100mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.181e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.072e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Cu100;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/Cu20.mo b/AixLib/Electrical/Transmission/LowVoltageCables/Cu20.mo
new file mode 100644
index 0000000000..c0f26aa96a
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/Cu20.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record Cu20 "Cu cable 20 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Cu,
+    M = 234.5 + 273.15,
+    Amp=95,
+    RCha=0.905e-003,
+    XCha=0.075e-003);
+  annotation (Documentation(info="<html>
+<p>
+Copper cable with a cross-sectional area of 20mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.905e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.075e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Cu20;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/Cu25.mo b/AixLib/Electrical/Transmission/LowVoltageCables/Cu25.mo
new file mode 100644
index 0000000000..4723ab8d78
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/Cu25.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record Cu25 "Cu cable 25 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Cu,
+    M = 234.5 + 273.15,
+    Amp=110,
+    RCha=0.727e-003,
+    XCha=0.075e-003);
+  annotation (Documentation(info="<html>
+<p>
+Copper cable with a cross-sectional area of 25mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.727e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.075e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Cu25;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/Cu35.mo b/AixLib/Electrical/Transmission/LowVoltageCables/Cu35.mo
new file mode 100644
index 0000000000..031369fb8c
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/Cu35.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record Cu35 "Cu cable 35 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Cu,
+    M = 234.5 + 273.15,
+    Amp=130,
+    RCha=0.517e-003,
+    XCha=0.074e-003);
+  annotation (Documentation(info="<html>
+<p>
+Copper cable with a cross-sectional area of 35mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.517e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.074e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Cu35;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/Cu50.mo b/AixLib/Electrical/Transmission/LowVoltageCables/Cu50.mo
new file mode 100644
index 0000000000..ef09cad44a
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/Cu50.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record Cu50 "Cu cable 50 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Cu,
+    M = 234.5 + 273.15,
+    Amp=170,
+    RCha=0.362e-003,
+    XCha=0.073e-003);
+  annotation (Documentation(info="<html>
+<p>
+Copper cable with a cross-sectional area of 50mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.362e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.073e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Cu50;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/Cu95.mo b/AixLib/Electrical/Transmission/LowVoltageCables/Cu95.mo
new file mode 100644
index 0000000000..a3cbe2426a
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/Cu95.mo
@@ -0,0 +1,32 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record Cu95 "Cu cable 95 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Cu,
+    M = 234.5 + 273.15,
+    Amp=220,
+    RCha=0.191e-003,
+    XCha=0.072e-003);
+  annotation (Documentation(info="<html>
+<p>
+Copper cable with a cross-sectional area of 95mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.191e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.072e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Cu95;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/Generic.mo b/AixLib/Electrical/Transmission/LowVoltageCables/Generic.mo
new file mode 100644
index 0000000000..3879f688f6
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/Generic.mo
@@ -0,0 +1,125 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record Generic "Data record for a generic low voltage cable"
+  extends Modelica.Icons.MaterialProperty;
+  extends AixLib.Electrical.Transmission.BaseClasses.BaseCable;
+  parameter AixLib.Electrical.Types.CharacteristicResistance RCha(start=0)
+    "Characteristic resistance of the cable";
+  parameter AixLib.Electrical.Types.CharacteristicReactance XCha(start=0)
+    "Characteristic reactance of the cable";
+
+  redeclare function extends lineResistance
+    "Function that computes the resistance of a cable"
+   input AixLib.Electrical.Transmission.LowVoltageCables.Generic cable
+      "Record that contains cable properties";
+  algorithm
+      R :=cable.RCha*l;
+      annotation(Inline=true, Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the overall resistance of a cable.
+</p>
+
+<p>
+The low voltage cable is described by a characteristic resistance per unit
+length, given this value the overall resistance is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+R = R<sub>CHA</sub> l<sub>CABLE</sub>,
+</p>
+<p>
+where <i>R<sub>CHA</sub></i> is the characteristic resistance per unit length, and
+<i>l<sub>CABLE</sub></i> is the length of the cable.
+</p>
+</html>"));
+  end lineResistance;
+
+  redeclare function extends lineInductance
+    "Function that computes the resistance of a cable"
+   input AixLib.Electrical.Transmission.LowVoltageCables.Generic cable
+      "Record that contains cable properties";
+  algorithm
+      L := l*(cable.XCha/omega);
+      annotation(Inline=true, Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the overall inductance of a cable.
+</p>
+<p>
+When the voltage level is low, the cables have a characteristic reactance per unit
+length, which is specified at <i>f = 50 Hz</i>.
+The overall inductance is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+L = (X<sub>CHA</sub>/&omega;) l<sub>CABLE</sub>,
+</p>
+<p>
+where <i>X<sub>CHA</sub></i> is the characteristic reactance per unit length,
+<i>&omega; = 2 &pi; f</i> is the angular velocity, and <i>l<sub>CABLE</sub></i> is
+the length of the cable.
+</p>
+</html>"));
+  end lineInductance;
+
+  redeclare function extends lineCapacitance
+    "Function that computes the capacitance of a cable"
+   input AixLib.Electrical.Transmission.LowVoltageCables.Generic cable
+      "Record that contains cable properties";
+  algorithm
+      C := 0.0;
+      annotation(Inline=true, Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the overall capacity of a cable.
+</p>
+<p>
+When the voltage level is low, the cables do not consider the capacitive effect. Hence,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+C = 0.
+</p>
+</html>"));
+  end lineCapacitance;
+
+  annotation (Documentation(info="<html>
+<p>
+This is a base record for specifying physical properties for low
+voltage commercial cables. New cables can be added by extending the
+it.
+</p>
+<p>
+For low voltage cables, only the characteristic resistance and reactance are
+specified.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, not it extends the base records
+and add details for the low voltage cables.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generic;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl120.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl120.mo
new file mode 100644
index 0000000000..5e4b1b421a
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl120.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl120 "Aluminum cable 120mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.269e-003,
+    XCha=0.071e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 120mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.269e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.071e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl120;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl120_ECM.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl120_ECM.mo
new file mode 100644
index 0000000000..6f7e0b33ec
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl120_ECM.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl120_ECM "Aluminum cable 120mm^2"
+    extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.278e-003,
+    XCha=0.071e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 120mm^2, ECM type.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.278e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.071e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl120_ECM;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl150.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl150.mo
new file mode 100644
index 0000000000..8fe751ba03
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl150.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl150 "Aluminum cable 150mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.206e-003,
+    XCha=0.070e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 150mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.206e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.070e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl150;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl16.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl16.mo
new file mode 100644
index 0000000000..9dc9c535ff
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl16.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl16 "Aluminum cable 16 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=2.105e-003,
+    XCha=0.076e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 16mm^2, ECM type.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 2.105e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.076e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl16;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl16_ECM.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl16_ECM.mo
new file mode 100644
index 0000000000..772d96de63
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl16_ECM.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl16_ECM "Aluminum cable 16 mm^2"
+    extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=2.105e-003,
+    XCha=0.076e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 16mm^2, ECM type.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 2.105e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.076e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl16_ECM;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl25.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl25.mo
new file mode 100644
index 0000000000..9b5f21db14
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl25.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl25 "Aluminum cable 25 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=1.292e-003,
+    XCha=0.075e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 25mm^2, ECM type.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 1.292e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.075e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl25;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl25_ECM.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl25_ECM.mo
new file mode 100644
index 0000000000..715438bd3d
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl25_ECM.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl25_ECM "Aluminum cable 25 mm^2"
+    extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=1.32e-003,
+    XCha=0.075e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 25mm^2, ECM type.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 1.320e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.075e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl25_ECM;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl35.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl35.mo
new file mode 100644
index 0000000000..3aa63de9c2
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl35.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl35 "Aluminum cable 35 mm^2"
+extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.923e-003,
+    XCha=0.074e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 35mm^2, ECM type.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.923e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.074e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl35;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl35_ECM.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl35_ECM.mo
new file mode 100644
index 0000000000..e5d919ba9d
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl35_ECM.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl35_ECM "Aluminum cable 35 mm^2"
+    extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.956e-003,
+    XCha=0.074e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 35mm^2, ECM type.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.956e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.074e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl35_ECM;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl50.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl50.mo
new file mode 100644
index 0000000000..0cbc7335e4
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl50.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl50 "Aluminum cable 50 mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.641e-003,
+    XCha=0.073e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 50mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.641e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.073e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl50;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl70.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl70.mo
new file mode 100644
index 0000000000..a46cf6e888
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl70.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl70 "Aluminum cable 70mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.5071e-003,
+    XCha=0.072e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 70mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.5071e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.072e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl70;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl70_ECM.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl70_ECM.mo
new file mode 100644
index 0000000000..1f96f3564d
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl70_ECM.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl70_ECM "Aluminum cable 70mm^2"
+    extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.488e-003,
+    XCha=0.072e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 70mm^2, ECM type.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.488e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.072e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl70_ECM;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl75.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl75.mo
new file mode 100644
index 0000000000..52ba6be108
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl75.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl75 "Aluminum cable 75mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.431e-003,
+    XCha=0.072e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 75mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.431e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.072e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl75;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl95.mo b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl95.mo
new file mode 100644
index 0000000000..6a32341ca8
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/PvcAl95.mo
@@ -0,0 +1,31 @@
+within AixLib.Electrical.Transmission.LowVoltageCables;
+record PvcAl95 "Aluminum cable 95mm^2"
+  extends AixLib.Electrical.Transmission.LowVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    RCha=0.320e-003,
+    XCha=0.072e-003);
+  annotation (Documentation(info="<html>
+<p>
+Aluminium cable with a cross-sectional area of 95mm^2.
+This type of cable has the following properties
+</p>
+<pre>
+RCha = 0.320e-003 // Characteristic resistance [Ohm/m]
+XCha = 0.072e-003 // Characteristic reactance [Ohm/m]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PvcAl95;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/package.mo b/AixLib/Electrical/Transmission/LowVoltageCables/package.mo
new file mode 100644
index 0000000000..d8f5023fb3
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/package.mo
@@ -0,0 +1,27 @@
+within AixLib.Electrical.Transmission;
+package LowVoltageCables "Package of low voltage electricity cables used in distribution grid"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+This package contains records of physical properties for low
+voltage commercial cables. New cables can be added by extending the
+base record
+<a href=\"modelia://AixLib.Electrical.Transmission.LowVoltageCables.Generic\">
+AixLib.Electrical.Transmission.LowVoltageCables.Generic</a>.
+</p>
+<p>
+For low voltage cables, only the characteristic resistance and reactance are
+specified. See <a href=\"modelia://AixLib.Electrical.Transmission.Base.BaseCable\">
+AixLib.Electrical.Transmission.Base.BaseCable</a> for a comprehensive list of
+parameters that can be specified for a cable.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end LowVoltageCables;
diff --git a/AixLib/Electrical/Transmission/LowVoltageCables/package.order b/AixLib/Electrical/Transmission/LowVoltageCables/package.order
new file mode 100644
index 0000000000..945d5c3614
--- /dev/null
+++ b/AixLib/Electrical/Transmission/LowVoltageCables/package.order
@@ -0,0 +1,22 @@
+Cu10
+Cu100
+Cu20
+Cu25
+Cu35
+Cu50
+Cu95
+Generic
+PvcAl120
+PvcAl120_ECM
+PvcAl150
+PvcAl16
+PvcAl16_ECM
+PvcAl25
+PvcAl25_ECM
+PvcAl35
+PvcAl35_ECM
+PvcAl50
+PvcAl70
+PvcAl70_ECM
+PvcAl75
+PvcAl95
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_10.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_10.mo
new file mode 100644
index 0000000000..f791c5d950
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_10.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.MediumVoltageCables;
+record Annealed_Al_10 "Annealed Al cable - AWG 1/0"
+  extends AixLib.Electrical.Transmission.MediumVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    size="1/0",
+    Rdc=0.551181e-3,
+    T_ref=298.15,
+    d=9.195e-3,
+    D=26.543e-3,
+    GMR=AixLib.Electrical.Transmission.Functions.computeGMR(d),
+    GMD=AixLib.Electrical.Transmission.Functions.computeGMD(0.1905),
+    Amp=195);
+  annotation (Documentation(info="<html>
+<p>
+Annealed aluminium cable with a cross-sectional AWG 1/0
+(American Wire Gauge).
+This type of cable has the following properties
+</p>
+<pre>
+Rdc  = 0.551181e-3 // Characteristic DC resistance at T = T_ref[Ohm/m]
+T_ref= 298.15      // Reference temperature of the material [K]
+d    = 9.195e-3    // Inner diameter [m]
+D    = 26.543e-3   // Outer diameter [m]
+Amp  = 195         // Ampacity [A]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Annealed_Al_10;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_1000.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_1000.mo
new file mode 100644
index 0000000000..1682ef15bf
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_1000.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.MediumVoltageCables;
+record Annealed_Al_1000 "Annealed Al cable - AWG 1000"
+  extends AixLib.Electrical.Transmission.MediumVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    size="1000",
+    Rdc=5.80709e-5,
+    T_ref=298.15,
+    d=28.372e-3,
+    D=46.101e-3,
+    GMR=AixLib.Electrical.Transmission.Functions.computeGMR(d),
+    GMD=AixLib.Electrical.Transmission.Functions.computeGMD(0.1905),
+    Amp=640);
+  annotation (Documentation(info="<html>
+<p>
+Annealed aluminium cable with a cross-sectional kcmil 1000
+(thousand of Circular Mils).
+This type of cable has the following properties
+</p>
+<pre>
+Rdc  = 5.80709e-5  // Characteristic DC resistance at T = T_ref[Ohm/m]
+T_ref= 298.15      // Reference temperature of the material [K]
+d    = 28.372e-3   // Inner diameter [m]
+D    = 46.101e-3   // Outer diameter [m]
+Amp  = 640         // Ampacity [A]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Annealed_Al_1000;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_1500.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_1500.mo
new file mode 100644
index 0000000000..f67d4c8dc3
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_1500.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.MediumVoltageCables;
+record Annealed_Al_1500 "Annealed Al cable - AWG 1500"
+  extends AixLib.Electrical.Transmission.MediumVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    size="1500",
+    Rdc=3.87139e-5,
+    T_ref=298.15,
+    d=34.798e-3,
+    D=53.34e-3,
+    GMR=AixLib.Electrical.Transmission.Functions.computeGMR(d),
+    GMD=AixLib.Electrical.Transmission.Functions.computeGMD(0.1905),
+    Amp=800);
+  annotation (Documentation(info="<html>
+<p>
+Annealed aluminium cable with a cross-sectional kcmil 1500
+(thousand of Circular Mils).
+This type of cable has the following properties
+</p>
+<pre>
+Rdc  = 3.87139e-5 // Characteristic DC resistance at T = T_ref[Ohm/m]
+T_ref= 298.15      // Reference temperature of the material [K]
+d    = 34.798e-3   // Inner diameter [m]
+D    = 53.34e-3   // Outer diameter [m]
+Amp  = 800         // Ampacity [A]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Annealed_Al_1500;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_30.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_30.mo
new file mode 100644
index 0000000000..0609c4efd2
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_30.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.MediumVoltageCables;
+record Annealed_Al_30 "Annealed Al cable - AWG 3/0"
+  extends AixLib.Electrical.Transmission.MediumVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    size="3/0",
+    Rdc=0.344488e-3,
+    T_ref=298.15,
+    d=11.582e-3,
+    D=28.956e-3,
+    GMR=AixLib.Electrical.Transmission.Functions.computeGMR(d),
+    GMD=AixLib.Electrical.Transmission.Functions.computeGMD(0.1905),
+    Amp=250);
+  annotation (Documentation(info="<html>
+<p>
+Annealed aluminium cable with a cross-sectional AWG 2/0
+(American Wire Gauge).
+This type of cable has the following properties
+</p>
+<pre>
+Rdc  = 0.344488e-3 // Characteristic DC resistance at T = T_ref[Ohm/m]
+T_ref= 298.15      // Reference temperature of the material [K]
+d    = 11.582e-3   // Inner diameter [m]
+D    = 28.956e-3   // Outer diameter [m]
+Amp  = 250         // Ampacity [A]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Annealed_Al_30;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_350.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_350.mo
new file mode 100644
index 0000000000..85588bced9
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_350.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.MediumVoltageCables;
+record Annealed_Al_350 "Annealed Al cable - kcmil 350"
+  extends AixLib.Electrical.Transmission.MediumVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    size="350",
+    Rdc=0.165682e-3,
+    T_ref=298.15,
+    d=16.789e-3,
+    D=34.417e-3,
+    GMR=AixLib.Electrical.Transmission.Functions.computeGMR(d),
+    GMD=AixLib.Electrical.Transmission.Functions.computeGMD(0.1905),
+    Amp=375);
+  annotation (Documentation(info="<html>
+<p>
+Annealed aluminium cable with a cross-sectional kcmil 350
+(thousand of Circular Mils).
+This type of cable has the following properties
+</p>
+<pre>
+Rdc  = 0.165682e-3 // Characteristic DC resistance at T = T_ref[Ohm/m]
+T_ref= 298.15      // Reference temperature of the material [K]
+d    = 16.789e-3   // Inner diameter [m]
+D    = 34.417e-3   // Outer diameter [m]
+Amp  = 375         // Ampacity [A]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Annealed_Al_350;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_40.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_40.mo
new file mode 100644
index 0000000000..9a1c0e5d14
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_40.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.MediumVoltageCables;
+record Annealed_Al_40 "Annealed Al cable - AWG 4/0"
+  extends AixLib.Electrical.Transmission.MediumVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    size="4/0",
+    Rdc=0.274278e-3,
+    T_ref=298.15,
+    d=13.005e-3,
+    D=30.353e-3,
+    GMR=AixLib.Electrical.Transmission.Functions.computeGMR(d),
+    GMD=AixLib.Electrical.Transmission.Functions.computeGMD(0.1905),
+    Amp=285);
+  annotation (Documentation(info="<html>
+<p>
+Annealed aluminium cable with a cross-sectional AWG 4/0
+(American Wire Gauge).
+This type of cable has the following properties
+</p>
+<pre>
+Rdc  = 0.274278e-3 // Characteristic DC resistance at T = T_ref[Ohm/m]
+T_ref= 298.15      // Reference temperature of the material [K]
+d    = 13.005e-3   // Inner diameter [m]
+D    = 30.353e-3   // Outer diameter [m]
+Amp  = 285         // Ampacity [A]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Annealed_Al_40;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_500.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_500.mo
new file mode 100644
index 0000000000..321abd0b1d
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/Annealed_Al_500.mo
@@ -0,0 +1,41 @@
+within AixLib.Electrical.Transmission.MediumVoltageCables;
+record Annealed_Al_500 "Annealed Al cable - AWG 500"
+  extends AixLib.Electrical.Transmission.MediumVoltageCables.Generic(
+    material=Types.Material.Al,
+    M = 228.1 + 273.15,
+    size="500",
+    Rdc=0.116142e-3,
+    T_ref=298.15,
+    d=20.066e-3,
+    D=37.592e-3,
+    GMR=AixLib.Electrical.Transmission.Functions.computeGMR(d),
+    GMD=AixLib.Electrical.Transmission.Functions.computeGMD(0.1905),
+    Amp=450);
+  annotation (Documentation(info="<html>
+<p>
+Annealed aluminium cable with a cross-sectional kcmil 500
+(thousand of Circular Mils).
+This type of cable has the following properties
+</p>
+<pre>
+Rdc  = 0.116142e-3 // Characteristic DC resistance at T = T_ref[Ohm/m]
+T_ref= 298.15      // Reference temperature of the material [K]
+d    = 20.066e-3   // Inner diameter [m]
+D    = 37.592e-3   // Outer diameter [m]
+Amp  = 450         // Ampacity [A]
+</pre>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, now the temperature constant <code>M</code>
+is directly specified in the record.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Annealed_Al_500;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/Generic.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/Generic.mo
new file mode 100644
index 0000000000..c7bb5f3c51
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/Generic.mo
@@ -0,0 +1,157 @@
+within AixLib.Electrical.Transmission.MediumVoltageCables;
+record Generic "Data record for a generic medium voltage cable"
+  extends Modelica.Icons.MaterialProperty;
+  extends AixLib.Electrical.Transmission.BaseClasses.BaseCable;
+  parameter String size(start="")
+    "AWG or kcmil code representing the conductor size";
+  parameter AixLib.Electrical.Types.CharacteristicResistance Rdc(start=0)
+    "Characteristic DC resistance of the cable @ T_ref";
+  parameter Modelica.Units.SI.Length d "Inner diameter";
+  parameter Modelica.Units.SI.Length D "Outer diameter";
+  parameter Modelica.Units.SI.Length GMR "Geometrical Mean Radius of the cable";
+  parameter Modelica.Units.SI.Length GMD
+    "Geometrical Mean Diameter of the cable";
+
+  redeclare function extends lineResistance
+    "Function that computes the resistance of a cable"
+      input AixLib.Electrical.Transmission.MediumVoltageCables.Generic cable
+      "Record that contains cable properties";
+  algorithm
+    R := l*cable.Rdc*AixLib.Electrical.Transmission.Functions.R_AC_correction(
+    cable.size, cable.material);
+      annotation(Inline=true, Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the overall resistance of a cable.
+</p>
+<p>
+When the voltage level is medium or high, the cables have a DC resistance that needs
+to be corrected to account for the effects cause by the AC voltage.
+The correction is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+R = l<sub>CABLE</sub> R<sub>DC</sub> f<sub>CORR</sub>(s, m),
+</p>
+<p>
+where <i>R<sub>DC</sub> </i> is the characteristic DC resistance per unit length,
+<i>l<sub>CABLE</sub></i> is the length of the cable, and
+<i>f<sub>CORR</sub>(s, m)</i> is a function that corrects the DC value and depends on the
+size of the cable <i>s</i> and its material <i>m</i>. See
+<a href=\"modelica://AixLib.Electrical.Transmission.Functions.R_AC_correction\">
+AixLib.Electrical.Transmission.Functions.R_AC_correction</a> for more details.
+</p>
+
+</html>"));
+  end lineResistance;
+
+  redeclare function extends lineInductance
+    "Function that computes the resistance of a cable"
+    input AixLib.Electrical.Transmission.MediumVoltageCables.Generic cable
+      "Record that contains cable properties";
+  algorithm
+    L := l*2e-7*log(cable.GMD/cable.GMR);
+      annotation(Inline=true, Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the overall inductance of a cable.
+</p>
+<p>
+When the voltage level is medium or high, the cables have geometric parameters that can
+be used to compute the inductance as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+R = l<sub>CABLE</sub> 2 10<sup>-7</sup> log(GMD/GMR),
+</p>
+<p>
+where <i>l<sub>CABLE</sub></i> is the length of the cable, and
+<i>GMD</i> and <i>GMR</i> are the geometric mean distance and the geometric mean radius
+of the cable.
+</p>
+</html>"));
+  end lineInductance;
+
+  redeclare function extends lineCapacitance
+    "Function that computes the capacitance of a cable"
+    input AixLib.Electrical.Transmission.MediumVoltageCables.Generic cable
+      "Record that contains cable properties";
+  protected
+    Modelica.Units.SI.Length r "Radius";
+  algorithm
+    r := cable.d/2.0;
+    C := l*2*Modelica.Constants.pi*Modelica.Constants.epsilon_0/log(cable.GMD/r);
+      annotation(Inline=true, Documentation(revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Added function and documentation
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This function computes the overall capacity of a cable.
+</p>
+<p>
+When the voltage level is medium or high, the cables have geometric parameters that can
+be used to compute the capacity as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+C = l<sub>CABLE</sub> 2 &pi; &epsilon;<sub>0</sub>/log(GMD/r),
+</p>
+<p>
+where <i>l<sub>CABLE</sub></i> is the length of the cable,
+<i>&epsilon;<sub>0</sub></i> is the dielectric constant of the air, <i>GMD</i>
+is the geometric mean distance, and <i>r = d/2</i> where <i>d</i> is the inner
+diameter of the cable.
+</p>
+</html>"));
+  end lineCapacitance;
+
+  annotation (Documentation(info="<html>
+<p>
+This is a base record for specifying physical properties for medium
+voltage commercial cables. New cables can be added by extending
+it.
+</p>
+<p>
+For medium voltage cables, the geometric properties of the cable and the material are
+specified. For example some of the properties that are specified are:
+</p>
+<pre>
+Rdc   : Characteristic DC resistance at T = T_ref[Ohm/m]
+T_ref : Reference temperature of the material [K]
+d     : Inner diameter [m]
+D     : Outer diameter [m]
+Amp   : Ampacity [A]
+</pre>
+<p>
+other properties such as the geometric mean diameter GMD and the
+geometric mean radius GMR are by default computed using functions,
+but this can be overriden.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 23, 2014, by Marco Bonvini:<br/>
+Revised structure of the record, not it extends the base records
+and add details for the medium voltage cables.
+</li>
+<li>
+Sept 19, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generic;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/package.mo b/AixLib/Electrical/Transmission/MediumVoltageCables/package.mo
new file mode 100644
index 0000000000..b858cc197d
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/package.mo
@@ -0,0 +1,22 @@
+within AixLib.Electrical.Transmission;
+package MediumVoltageCables "Package of medium voltage electricity cables used in distribution grid"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+
+annotation (Documentation(info="<html>
+<p>
+This package contains records of physical properties of medium
+voltage commercial cables. New cables can be added by extending the
+base record
+<a href=\"modelia://AixLib.Electrical.Transmission.MediumVoltageCables.Generic\">
+AixLib.Electrical.Transmission.MediumVoltageCables.Generic</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end MediumVoltageCables;
diff --git a/AixLib/Electrical/Transmission/MediumVoltageCables/package.order b/AixLib/Electrical/Transmission/MediumVoltageCables/package.order
new file mode 100644
index 0000000000..bbbc0da18c
--- /dev/null
+++ b/AixLib/Electrical/Transmission/MediumVoltageCables/package.order
@@ -0,0 +1,8 @@
+Annealed_Al_10
+Annealed_Al_1000
+Annealed_Al_1500
+Annealed_Al_30
+Annealed_Al_350
+Annealed_Al_40
+Annealed_Al_500
+Generic
diff --git a/AixLib/Electrical/Transmission/Types/Material.mo b/AixLib/Electrical/Transmission/Types/Material.mo
new file mode 100644
index 0000000000..9bc8305450
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Types/Material.mo
@@ -0,0 +1,17 @@
+within AixLib.Electrical.Transmission.Types;
+type Material = enumeration(
+    Cu "Copper",
+    Al "Aluminium") "Material of the cable" annotation (Documentation(revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Enumeration for materials that can be used
+for cables.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Transmission/Types/package.mo b/AixLib/Electrical/Transmission/Types/package.mo
new file mode 100644
index 0000000000..b2a1367a06
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Types/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.Transmission;
+package Types "Package that contains cables materials"
+  extends Modelica.Icons.TypesPackage;
+
+
+annotation (preferredView="info",
+Documentation(info="<html>
+<p>
+This package contains an enumeration for materials.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end Types;
diff --git a/AixLib/Electrical/Transmission/Types/package.order b/AixLib/Electrical/Transmission/Types/package.order
new file mode 100644
index 0000000000..f4c8dcd2bc
--- /dev/null
+++ b/AixLib/Electrical/Transmission/Types/package.order
@@ -0,0 +1 @@
+Material
diff --git a/AixLib/Electrical/Transmission/package.mo b/AixLib/Electrical/Transmission/package.mo
new file mode 100644
index 0000000000..dd6d932018
--- /dev/null
+++ b/AixLib/Electrical/Transmission/package.mo
@@ -0,0 +1,74 @@
+within AixLib.Electrical;
+package Transmission "Package with models for transmission lines"
+  extends Modelica.Icons.Package;
+
+annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+          {100,100}}), graphics={
+      Ellipse(
+        extent={{40,8},{16,-28}},
+        lineColor={0,0,0},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),
+      Line(
+        points={{28,8},{-54,8},{-64,8},{-72,-10},{-64,-28},{-52,-28},{28,-28}},
+        color={0,0,0},
+        smooth=Smooth.Bezier),
+      Line(
+        points={{-70,-10},{-88,-10}},
+        color={0,0,0},
+        smooth=Smooth.None),
+      Line(
+        points={{54,-10},{28,-10}},
+        color={0,0,0},
+        smooth=Smooth.None)}), Documentation(info="<html>
+<p>
+This package contains cables that can be used
+to represent a line in a electric grid. The package contains
+several functions and records to parametrize cables either using
+default values or values from commercial cables.
+</p>
+<p>
+The package
+<a href=\"modelica://AixLib.Electrical.Transmission.Grids\">
+AixLib.Electrical.Transmission.Grids</a>
+contains models of
+electrical networks.
+</p>
+<h4>Commercial cables</h4>
+<p>
+The package contains several low voltage and medium voltage cable with
+pre-defined physical and geometrical properties like characteristic resistances and
+diameters. There are different conventions to measure the cables.
+</p>
+
+<h5>Cross-sectional area</h5>
+<p>
+A measure of cross-sectional area in square mm. E.g. 50 mm<sup>2</sup>
+wire has a nominal circula area of 50 mm<sup>2</sup> and a diameter of
+7.98 mm.
+</p>
+
+<h5>AWG (American Wire Gauge)</h5>
+<p>
+A measure of wire thickness (which also dictates cross-sectional area, and
+for a given material, ampacity). E.g. 24 AWG wire has a nominal diameter of
+0.0201 in or 0.511 mm.
+</p>
+
+<h5>kcmil (thousand of Circular Mils)</h5>
+<p>
+kcmil is an abbreviation for thousands of circular mils, an old measurement of
+wire gauge. 1 kcmil = 0.5067 square millimeters. A mil is 1/1000 inch.
+A wire 200 mils in diameter is 40 kcmil. kcmil is generally used for very
+large-diameter wire. Most wires use AWG.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+June 3, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end Transmission;
diff --git a/AixLib/Electrical/Transmission/package.order b/AixLib/Electrical/Transmission/package.order
new file mode 100644
index 0000000000..8954d8b84a
--- /dev/null
+++ b/AixLib/Electrical/Transmission/package.order
@@ -0,0 +1,6 @@
+Functions
+Grids
+LowVoltageCables
+MediumVoltageCables
+Types
+BaseClasses
diff --git a/AixLib/Electrical/Types/CableMode.mo b/AixLib/Electrical/Types/CableMode.mo
new file mode 100644
index 0000000000..fedbd4beaa
--- /dev/null
+++ b/AixLib/Electrical/Types/CableMode.mo
@@ -0,0 +1,19 @@
+within AixLib.Electrical.Types;
+type CableMode = enumeration(
+    automatic "Select automatically the size of the cable",
+    commercial "Select the cable from a list of commercial options")
+  "Enumeration that defines how a cable can be parameterized" annotation (
+    Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+This type is used to indicate in which mode the cable model works.
+In automatic mode the cable is automatically sized using basic information like
+nominal voltage and power, in commercial mode the user can select among a list of
+commercially available cables.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Types/CharacteristicReactance.mo b/AixLib/Electrical/Types/CharacteristicReactance.mo
new file mode 100644
index 0000000000..242a7b117f
--- /dev/null
+++ b/AixLib/Electrical/Types/CharacteristicReactance.mo
@@ -0,0 +1,14 @@
+within AixLib.Electrical.Types;
+type CharacteristicReactance =  Real (final quantity="Reactance per meter",  final unit="Ohm/m")
+  "Reactance per unit length" annotation (Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+This type defines the reactance per unit length. It is typically used
+to describe physical properties of line cables.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Types/CharacteristicResistance.mo b/AixLib/Electrical/Types/CharacteristicResistance.mo
new file mode 100644
index 0000000000..3dc3bacaab
--- /dev/null
+++ b/AixLib/Electrical/Types/CharacteristicResistance.mo
@@ -0,0 +1,14 @@
+within AixLib.Electrical.Types;
+type CharacteristicResistance = Real (final quantity="Resistance per meter", final unit="Ohm/m")
+  "Resistance per unit length" annotation (Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+This type defines the resistance per unit length and it typically used
+to describe physical properties of the line cables.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Types/InitMode.mo b/AixLib/Electrical/Types/InitMode.mo
new file mode 100644
index 0000000000..a25d87da41
--- /dev/null
+++ b/AixLib/Electrical/Types/InitMode.mo
@@ -0,0 +1,17 @@
+within AixLib.Electrical.Types;
+type InitMode = enumeration(
+    zero_current "Assume i=0 during homotopy initialization",
+    linearized "Uses linear model during homotopy initialization")
+  "Enumeration that defines the type of initialization assumption can be used for a load model"
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+This type is used to indicate how a model
+should be initialized.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Types/Load.mo b/AixLib/Electrical/Types/Load.mo
new file mode 100644
index 0000000000..11de2a6c0d
--- /dev/null
+++ b/AixLib/Electrical/Types/Load.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.Types;
+type Load = enumeration(
+    FixedZ_steady_state "Fixed Z, steady-state",
+    FixedZ_dynamic "Fixed Z, dynamic",
+    VariableZ_P_input "Variable Z, P input",
+    VariableZ_y_input "Variable Z, y input")
+  "Enumeration that defines the modeling assumption of the load." annotation (
+    Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+This type indicates in which mode the load model operates.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Types/LoadConnection.mo b/AixLib/Electrical/Types/LoadConnection.mo
new file mode 100644
index 0000000000..120002189a
--- /dev/null
+++ b/AixLib/Electrical/Types/LoadConnection.mo
@@ -0,0 +1,17 @@
+within AixLib.Electrical.Types;
+type LoadConnection = enumeration(
+    wye_to_wyeg "Wye to wye grounded",
+    wye_to_delta "Wye to delta")
+  "Enumeration that defines the type of connection can be used for three-phase unbalanced systems"
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+This type is used to describe different types of connections that can be used in
+unbalanced three phase systems.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Types/PerUnit.mo b/AixLib/Electrical/Types/PerUnit.mo
new file mode 100644
index 0000000000..dbe0eeed3e
--- /dev/null
+++ b/AixLib/Electrical/Types/PerUnit.mo
@@ -0,0 +1,16 @@
+within AixLib.Electrical.Types;
+type PerUnit = Real (final quantity="Per unit", final unit="1", min=0)
+  "Used to represent electric quantities with respect to reference value"
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+This type is used to declare whether an electric quantity such as voltage
+is expressed in SI units or in per units (i.e., the value divided by its nominal
+value).
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Types/VoltageLevel.mo b/AixLib/Electrical/Types/VoltageLevel.mo
new file mode 100644
index 0000000000..542437b4c0
--- /dev/null
+++ b/AixLib/Electrical/Types/VoltageLevel.mo
@@ -0,0 +1,17 @@
+within AixLib.Electrical.Types;
+type VoltageLevel = enumeration(
+    Low "Low voltage",
+    Medium "Medium voltage",
+    High "High voltage") "Enumeration that defines the type of voltage level"
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+March 19, 2015, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+This type is used to define which type of voltage level is used.
+This is typically used for computing or selecting the line cables.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Electrical/Types/package.mo b/AixLib/Electrical/Types/package.mo
new file mode 100644
index 0000000000..26fe2befd8
--- /dev/null
+++ b/AixLib/Electrical/Types/package.mo
@@ -0,0 +1,28 @@
+within AixLib.Electrical;
+package Types "This package contains new types used within the Electrical package"
+  extends Modelica.Icons.TypesPackage;
+
+annotation (preferredView="info",
+Documentation(
+info="<html>
+This package contains type definitions.
+</html>",
+revisions="<html>
+<ul>
+<li>
+June 17, 2014, by Marco Bonvini:<br/>
+Added new type <code>InitMode</code> to represent different types
+of initialization assumptions for the load model.
+</li>
+<li>
+June 5, 2014, by Marco Bonvini:<br/>
+Added new type <code>LoadConnection</code> to represent different types
+of unbalanced connection.
+</li>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Added User's guide.
+</li>
+</ul>
+</html>"));
+end Types;
diff --git a/AixLib/Electrical/Types/package.order b/AixLib/Electrical/Types/package.order
new file mode 100644
index 0000000000..e17893b71e
--- /dev/null
+++ b/AixLib/Electrical/Types/package.order
@@ -0,0 +1,8 @@
+CableMode
+CharacteristicReactance
+CharacteristicResistance
+InitMode
+Load
+LoadConnection
+PerUnit
+VoltageLevel
diff --git a/AixLib/Electrical/UsersGuide.mo b/AixLib/Electrical/UsersGuide.mo
new file mode 100644
index 0000000000..99bf9dba52
--- /dev/null
+++ b/AixLib/Electrical/UsersGuide.mo
@@ -0,0 +1,275 @@
+within AixLib.Electrical;
+package UsersGuide "Electrical package user's guide"
+  extends Modelica.Icons.Information;
+  annotation (preferredView="info",
+Documentation(info="<html>
+
+<h4>Overview</h4>
+<p>
+The <a href=\"modelica://AixLib.Electrical\">AixLib.Electrical</a> package extends the
+capabilities of the AixLib library with models for electrical systems, allowing
+to study building-to-grid integration such as the effect of large scale PV on the
+voltage of the electrical distribution grid.
+The package contains models for different types of sources, loads, storage equipment,
+and transmission lines for electric power. The package contains models that can be used to
+represent DC, AC one-phase, and AC three-phase balanced and unbalanced systems.
+The models can be used to scale from the building level up to the distribution level.
+The models have been successfully validated against the IEEE four nodes test feeder.
+</p>
+
+<h4>Connectors</h4>
+<p>
+The <a href=\"modelica://AixLib.Electrical\">AixLib.Electrical</a> package uses a
+new type of generalized connector that has been introduced by <a href=\"#RuedigerEtAl2014\">R. Franke and Wiesman (2014)</a>
+and is used by the <a href=\"https://github.com/modelica/PowerSystems\">Power Systems Library</a>
+and the <a href=\"http://www.modelon.com/products/modelica-libraries/electric-power-library\">
+Electric Power Library</a>.
+</p>
+<p>
+The Modelica Standard Library (MSL) version 3.2.1 has different connectors depending on the
+type of electric system being modeled. For example, DC and AC continuous time systems have
+a connector (<a href=\"modelica://Modelica.Electrical.Analog.Interfaces.Pin\">Modelica.Electrical.Analog.Interfaces.Pin</a>)
+that differs from the one used by AC models, which use the
+quasi-stationary assumption (<a href=\"modelica://Modelica.Electrical.QuasiStatic.SinglePhase.Interfaces.Pin\">
+Modelica.Electrical.QuasiStatic.SinglePhase.Interfaces.Pin</a>).
+</p>
+<p>
+The generalized electrical connector overcomes this limitation. It uses a paradigm
+that is similar to the one used by the <code>Modelica.Fluid</code> connectors.
+The generalized connector is as follows:
+</p>
+
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px;\">
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">connector</span>
+<span style=\" font-family:'Courier New,courier';\"> Terminal </span>
+<span style=\" font-family:'Courier New,courier'; color:#006400;\">&quot;Generalized electric terminal&quot;</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">extends </span>
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">AixLib.Electrical.Interfaces.BaseTerminal</span>
+<span style=\" font-family:'Courier New,courier';\">;</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">replaceable package</span>
+<span style=\" font-family:'Courier New,courier';\"> PhaseSystem = </span>
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">AixLib.Electrical.PhaseSystems.PartialPhaseSystem </span>
+<span style=\" font-family:'Courier New,courier'; color:#006400;\">&quot;Phase system&quot;</span>
+<span style=\" font-family:'Courier New,courier';\">;</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">PhaseSystem.Voltage</span>
+<span style=\" font-family:'Courier New,courier';\"> v[PhaseSystem.n] </span>
+<span style=\" font-family:'Courier New,courier'; color:#006400;\">&quot;Voltage vector&quot;</span>
+<span style=\" font-family:'Courier New,courier';\">;</span
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">flow </span>
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">PhaseSystem.Current</span>
+<span style=\" font-family:'Courier New,courier';\"> i[PhaseSystem.n] </span>
+<span style=\" font-family:'Courier New,courier'; color:#006400;\">&quot;Current vector&quot;</span>
+<span style=\" font-family:'Courier New,courier';\">;</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#ff0000;\">PhaseSystem.ReferenceAngle</span>
+<span style=\" font-family:'Courier New,courier';\"> theta[PhaseSystem.m] </span>
+<span style=\" font-family:'Courier New,courier'; color:#006400;\">&quot;Optional vector of phase angles&quot;</span>
+<span style=\" font-family:'Courier New,courier';\">;</span>
+</p>
+<p style=\" margin-top:0px; margin-bottom:0px; margin-left:0px; margin-right:0px; -qt-block-indent:0; text-indent:0px; -qt-user-state:8;\">
+<span style=\" font-family:'Courier New,courier'; color:#0000ff;\">end </span>
+<span style=\" font-family:'Courier New,courier';\">Terminal;</span>
+</p>
+
+<p>
+The connector has a package called <code>PhaseSystem</code> that contains constants, functions,
+and equations of the specific electric domain. This allows to represent different electrical domains using the
+same connector, reusing the same standardized interfaces.
+</p>
+
+<p>
+As the electrical connectors of the Modelica Standard Library, the <code>Terminal</code> has a vector of voltages as effort variables and
+a vector of currents as flow variables. The connector has an additional vector that represents the
+reference angle <code>theta[PhaseSystem.m]</code>. If <code>PhaseSystem.m &gt; 0</code> the connector is overdetermined
+because the number of effort variables is higher than the number of flow variables.
+The over-determined connectors are defined and used in such a way that a Modelica tool is able
+to remove the superfluous but consistent equations, arriving at a balanced set of equations based on a
+graph analysis of the connection structure. The models in the library uses constructs specified
+by the Modelica language to handle this situation <a href=\"#Olsson2008\">Olsson Et Al. (2008)</a>.
+</p>
+
+<h4>PhaseSystem</h4>
+
+<p>
+The connector has a package called <code>PhaseSystem</code> that allows to represent different
+electrical domains using the same connector, reusing the same standardized interfaces.
+The available <code>PhaseSystems</code> are contained in the package
+<a href=\"modelica://AixLib.Electrical.PhaseSystems\">
+AixLib.Electrical.PhaseSystems</a>.
+</p>
+<p>
+Each of the available packages represent a different type of electrical systems.
+The electrical systems represented are:
+</p>
+<ul>
+<li>DC systems,</li>
+<li>DC systems with two conductors,</li>
+<li>one-phase AC systems,</li>
+<li>three-phase resistive balanced AC systems,</li>
+<li>three-phase balanced AC systems,</li>
+<li>three-phase unbalanced AC systems (dq0 representation).</li>
+</ul>
+
+<h4>Linearized models and homotopy initialization</h4>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/DC/Loads/simpleLoad.png\"/>
+</p>
+<p>
+Consider the simple DC circuit shown above, where <i>V<sub>S</sub></i> is a
+constant voltage source and <i>R</i> is a line resistance. The load has a voltage <i>V</i> across
+its electrical pins and a current <i>i</i>. If the power consumed
+by the load is <i>P<sub>LOAD</sub></i>, the equation that describes the circuit is nonlinear.
+</p>
+
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/UsersGuide/nonlinearEq.png\"/>
+</p>
+
+<p>
+If the number of loads increases, as typically happens in grid simulations, the size of the system of
+nonlinear equations to be solved increases too, causing the numerical solver to slow the simulation.
+A linearized load model can solve such a problem. All the load models in the
+<a href=\"modelica://AixLib.Electrical\">AixLib.Electrical</a> package have a linearized version.
+The linearized version of the model can be selected by setting the boolean flag <code>linearized = true</code>.
+Details about the implementation of the linearized models can be found in
+<a href=\"modelica://AixLib.Electrical.DC.Loads.Conductor\">AixLib.Electrical.DC.Loads.Conductor</a>
+or
+<a href=\"modelica://AixLib.Electrical.AC.OnePhase.Loads.Resistive\">AixLib.Electrical.AC.OnePhase.Loads.Resistive</a>.
+</p>
+
+<p>
+When multiple loads are connected in a grid through cables that cause voltage drops,
+the dimension of the system of nonlinear equations increases linearly with the number of loads.
+This nonlinear system of equations introduces challenges during the initialization, as Newton solvers
+may diverge if initialized far from a solution.
+The initialization problem can be simplified using the homotopy
+operator. The homotopy operator uses two different types of equations to compute the value of a
+variable: the actual one and a simplified one. The actual equation is the one used during the normal
+operation. During initialization, the simplified equation is first solved and then slowly replaced with the
+actual equation to compute the initial values for the nonlinear systems of equations.
+The load model uses the homotopy operator, with the linearized model being used
+as the simplified equation. This numerical expedient has proven useful
+when simulating models with more than ten connected loads.
+All the load models of the <a href=\"modelica://AixLib.Electrical\">AixLib.Electrical</a> package use the
+the homotopy operator during the initialization. The parameter <code>initMode</code> is used to select which
+simplified equation should be used by the homotopy operator:
+</p>
+<ul>
+<li><code>AixLib.Electrical.Types.InitMode.zeroCurrent</code></li>
+<li><code>AixLib.Electrical.Types.InitMode.linearized</code></li>
+</ul>
+
+<h4>Nominal values</h4>
+<p>
+Most components have a parameters for the nominal operating conditions.
+These parameters have names that end in <code>_nominal</code> and
+they should be set to the values that the component typically
+have if they are run at design conditions. Depending on the model, these
+parameters are used differently, and the respective model documentation or code
+should be consulted for details. However, the table below shows the typical use of
+the parameters in various models to help the user understand how they are used.
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<th>Parameter</th>
+<th>Model</th>
+<th>Functionality</th>
+</tr>
+<tr>
+  <td>V_nominal<br/>
+      P_nominal</td>
+  <td>Load models</td>
+  <td>
+  <code>V_nominal</code> is the RMS (Root Mean Square) voltage at which the load consumes the
+  nominal real power (measured in [W]) <code>P_nominal</code>.
+  When the load model are linearized, the linearization is done for <code>V = V_nominal</code>.
+  </td>
+</tr>
+<tr>
+  <td>V_nominal<br/>
+      P_nominal</td>
+  <td>Transmission line models
+  </td>
+  <td>
+  <code>V_nominal</code> is the RMS (Root Mean Square) voltage at which the line operates
+  while <code>P_nominal</code> is the power flowing through it. These values are used in some
+  cases to automatically select the right cable properties.
+  </td>
+</tr>
+<tr>
+  <td>V_nominal</td>
+  <td>Storage<br/>
+      PVs<br/>
+      Wind turbine
+  </td>
+  <td>
+  <code>V_nominal</code> is the RMS (Root Mean Square) voltage at which these components
+  typically operate. Since these model contain load models, <code>V_nominal</code> can be used
+  for linearization purposes.
+  </td>
+</tr>
+<tr>
+  <td>V_nominal</td>
+  <td>Sensors</td>
+  <td>
+  <code>V_nominal</code> is the RMS (Root Mean Square) voltage of the system
+  that is currently measured, it can be used to measure quantities in per unit [pu].
+  </td>
+</tr>
+</table>
+
+<h4>Other information</h4>
+<p>
+Other information about the models and the packages can be found in the
+info section of each model or sub-packages.
+</p>
+
+<h4>Awards</h4>
+<p>
+The paper titled <a href=\"modelica://AixLib/Resources/Images/Electrical/UsersGuide/2014-BauSim-BonviniWetterNouidui.pdf\">
+A Modelica package for building-to-electrical grid integration</a> won the best paper
+award at the BauSIM 2014 conference.
+</p>
+
+<h4>References</h4>
+<p>
+<a name=\"BonviniEtAl2014\"/>
+Marco Bonvini, Michael Wetter, and Thierry Stephane Nouidui.<br/>
+<a href=\"modelica://AixLib/Resources/Images/Electrical/UsersGuide/2014-BauSim-BonviniWetterNouidui.pdf\">
+A Modelica package for building-to-electrical grid integration</a><br/>
+<i>BauSIM 2014 Conference</i>, Aachen, Germany, September 2014.<br/>
+</p>
+
+<p>
+<a name=\"RuedigerEtAl2014\"/>
+Rudiger Franke and Hansjorg Wiesmann.<br/>
+<a href=\"https://www.modelica.org/events/modelica2014/proceedings/html/submissions/ECP14096515_FrankeWiesmann.pdf\">
+Flexible modeling of electrical power systems - the Modelica PowerSystems library</a>.<br/>
+Proc. of the 10th Modelica Conference, Lund, Sweden, March 2014.<br/>
+</p>
+
+<p>
+<a name=\"Olsson2008\"/>
+Hans Olsson, Martin Otter, Sven Erik Mattson and Hilding Elmqvist.<br/>
+<a href=\"http://elib-v3.dlr.de/55892/1/otter2008-modelica-balanced-models.pdf\">
+Balanced Models in Modelica 3.0 for Increased Model Quality</a>.<br/>
+Proc. of the 7th Modelica Conference, Bielefeld, Germany, March 2008.<br/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2014, by Marco Bonvini:<br/>
+Created User's guide.
+</li>
+</ul>
+</html>"));
+end UsersGuide;
diff --git a/AixLib/Electrical/Utilities/Controllers/StateMachineVoltCtrl.mo b/AixLib/Electrical/Utilities/Controllers/StateMachineVoltCtrl.mo
new file mode 100644
index 0000000000..cfd1a49a7c
--- /dev/null
+++ b/AixLib/Electrical/Utilities/Controllers/StateMachineVoltCtrl.mo
@@ -0,0 +1,65 @@
+within AixLib.Electrical.Utilities.Controllers;
+model StateMachineVoltCtrl "This model represents a simple voltage controller that unplug a load when
+  there is a voltage fluctuation higher that a given threshold."
+  Modelica.Blocks.Interfaces.RealInput V "Voltage of the node to be controlled";
+  parameter Modelica.Units.SI.Voltage V_nominal
+    "Nominal voltage of the node to be controlled";
+  parameter Real vThresh(min=0.0, max=1.0) = 0.1
+    "Threshold that activates voltage ctrl (ratio of nominal voltage)";
+  parameter Modelica.Units.SI.Time tDelay=300
+    "Time to wait before plugging the load back";
+  output Real y
+    "Output signal that represents whether the load should be connected to the grid or not";
+protected
+  discrete Boolean connected
+    "Boolean variable that indicates when the load is connected";
+  discrete Real tSwitch "Time instant when the last event occurred";
+initial algorithm
+  // Initialize with load connected and last event at t = 0
+  connected := true;
+  tSwitch := 0;
+equation
+
+  // Output for every state, connected or not
+  if connected then
+    y = 1.0;
+  else
+    y = 0.0;
+  end if;
+
+algorithm
+
+  // Detect an overshoot in the voltage
+  when
+      (connected and (V > V_nominal*(1+vThresh))) then
+    tSwitch := time;
+    connected := false;
+  end when;
+
+  // Transition between not connected and connected again after the delay time has been elapsed
+  when
+      (not connected and time >= tSwitch + tDelay) then
+    connected := true;
+  end when;
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+Aug 28, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Function that implements a state machine that detects voltage
+deviations. If the voltage input <code>V</code> exceeds the
+nominal value <code>V_nominal</code> by more than <i>1+V<sub>tr</sub></i>
+then the control signal <code>y</code> becones zero for
+a period equal to <code>tDelay</code>.
+</p>
+<p>
+A signal <code>y = 0</code> can be used to turn off a load.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end StateMachineVoltCtrl;
diff --git a/AixLib/Electrical/Utilities/Controllers/package.mo b/AixLib/Electrical/Utilities/Controllers/package.mo
new file mode 100644
index 0000000000..1555b9bd9a
--- /dev/null
+++ b/AixLib/Electrical/Utilities/Controllers/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Electrical.Utilities;
+package Controllers "Package that contains state machines and control models used by the utilities"
+extends Modelica.Icons.BasesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+Aug 28, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains state machines and controller models used by the utilities.
+</p>
+</html>"));
+end Controllers;
diff --git a/AixLib/Electrical/Utilities/Controllers/package.order b/AixLib/Electrical/Utilities/Controllers/package.order
new file mode 100644
index 0000000000..f8716a28cc
--- /dev/null
+++ b/AixLib/Electrical/Utilities/Controllers/package.order
@@ -0,0 +1 @@
+StateMachineVoltCtrl
diff --git a/AixLib/Electrical/Utilities/Examples/TestVoltageCTRL.mo b/AixLib/Electrical/Utilities/Examples/TestVoltageCTRL.mo
new file mode 100644
index 0000000000..6ba09c10ed
--- /dev/null
+++ b/AixLib/Electrical/Utilities/Examples/TestVoltageCTRL.mo
@@ -0,0 +1,91 @@
+within AixLib.Electrical.Utilities.Examples;
+model TestVoltageCTRL
+  "This test check the correctness of the voltage controller model"
+  extends Modelica.Icons.Example;
+  VoltageControl voltageControl(
+  redeclare AixLib.Electrical.DC.Interfaces.Terminal_p terminal,
+    redeclare package PhaseSystem =
+        AixLib.Electrical.PhaseSystems.TwoConductor,
+    V_nominal=120,
+    tDelay=2) "Voltage controller"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  DC.Sources.VoltageSource sou "Varriable voltage source"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+  Modelica.Electrical.Analog.Basic.Ground ground
+    annotation (Placement(transformation(extent={{-70,-36},{-50,-16}})));
+  Modelica.Blocks.Sources.Sine cosine(
+    amplitude=20,
+    f=0.1,
+    phase=0,
+    offset=120) "Variable voltage signal"
+    annotation (Placement(transformation(extent={{-94,-4},{-74,16}})));
+  Modelica.Blocks.Sources.Constant Vtr_high(k=120*(1 + 0.1))
+    "Voltage threshold high"
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+equation
+  connect(sou.terminal, voltageControl.terminal) annotation (Line(
+      points={{-40,0},{-10,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(ground.p, sou.n) annotation (Line(
+      points={{-60,-16},{-60,0}},
+      color={0,0,255},
+      smooth=Smooth.None));
+  connect(cosine.y, sou.V_in) annotation (Line(
+      points={{-73,6},{-60,6}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+March 10, 2015, by Marco Bonvini:<br/>
+Revised image of the example after modification to the voltage controller
+(added first order dynamics in the switch).
+</li>
+<li>
+Oct 14, 2014, by Marco Bonvini:<br/>
+Added model and documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example shows the use of the voltage controller.
+</p>
+<p>
+The voltage controller is connected to a variable voltage source
+that oscillates between <i>140</i> and <i>100</i> V. The nominal voltage is
+<i>V<sub>nom</sub> = 120 </i> V. The controller has the following settings:
+</p>
+<ul>
+<li>Nominal voltage <i>V<sub>nom</sub> = 120 </i> V,</li>
+<li>Threshold <i>V<sub>tr</sub> = 0.1 (10%)</i>,</li>
+<li>tdelay <i>T<sub>delay</sub> = 2 </i> s.</li>
+</ul>
+<p>
+Therefore, when the voltage controller measures a voltage that
+is 10% higher that 120 V (that is 132 V), it sets its output signal <code>y</code> to zero.
+The output signal stays at zero for <i>T<sub>delay</sub></i>,
+after which it expires.
+Then, the controllers check again if the voltage is within the
+accepted thresholds.
+</p>
+<p>
+The image below shows how the signal becomes equal to zero when the measured
+voltage exceeds the threshold.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Electrical/Utilities/Examples/VoltCTRL.png\"/>
+</p>
+<p>
+The figure shows that the signal <code>y</code> becomes zero around <i>t = 1</i> s. After
+<i>T<sub>delay</sub></i> the voltage is still higher that 123 V and thus the controller waits until
+<i>t = 5</i> s to change the signal to one.
+</p>
+</html>"),    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Electrical/Utilities/Examples/TestVoltageCTRL.mos"
+        "Simulate and plot"),
+    experiment(
+      StopTime=10,
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end TestVoltageCTRL;
diff --git a/AixLib/Electrical/Utilities/Examples/package.mo b/AixLib/Electrical/Utilities/Examples/package.mo
new file mode 100644
index 0000000000..6c77fdab1d
--- /dev/null
+++ b/AixLib/Electrical/Utilities/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Electrical.Utilities;
+package Examples "This package contais tests for check the correctness of the models"
+extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (Documentation(revisions="<html>
+<ul>
+<li>
+Aug 28, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Electrical.Utilities\">
+AixLib.Electrical.Utilities</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Electrical/Utilities/Examples/package.order b/AixLib/Electrical/Utilities/Examples/package.order
new file mode 100644
index 0000000000..b7048b5bb5
--- /dev/null
+++ b/AixLib/Electrical/Utilities/Examples/package.order
@@ -0,0 +1 @@
+TestVoltageCTRL
diff --git a/AixLib/Electrical/Utilities/VoltageControl.mo b/AixLib/Electrical/Utilities/VoltageControl.mo
new file mode 100644
index 0000000000..27888823b8
--- /dev/null
+++ b/AixLib/Electrical/Utilities/VoltageControl.mo
@@ -0,0 +1,99 @@
+within AixLib.Electrical.Utilities;
+model VoltageControl "Voltage controller"
+  replaceable package PhaseSystem =
+      AixLib.Electrical.PhaseSystems.PartialPhaseSystem constrainedby
+    AixLib.Electrical.PhaseSystems.PartialPhaseSystem "Phase system"
+    annotation (choicesAllMatching=true);
+  parameter Modelica.Units.SI.Voltage V_nominal
+    "Nominal voltage of the node to be controlled";
+  parameter Real vThresh(min=0.0, max=1.0) = 0.1
+    "Threshold that activates voltage ctrl (ratio of nominal voltage)";
+  parameter Modelica.Units.SI.Time tDelay=300
+    "Time to wait before plugging the load back";
+  parameter Modelica.Units.SI.Time T=0.01
+    "Time constant representing the switching time";
+  parameter Real y_start = 1.0 "Initial value of the control output signal";
+  final parameter Modelica.Units.SI.Voltage Vmin=V_nominal*(1 - vThresh)
+    "Low threshold";
+  final parameter Modelica.Units.SI.Voltage Vmax=V_nominal*(1 + vThresh)
+    "High threshold";
+  Modelica.Blocks.Interfaces.RealOutput y(start = y_start, stateSelect = StateSelect.prefer)
+    "Control signal"
+    annotation (Placement(transformation(extent={{96,-10},{116,10}})));
+  replaceable AixLib.Electrical.Interfaces.Terminal terminal(
+    redeclare replaceable package PhaseSystem = PhaseSystem)
+    "Generalized terminal"
+    annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
+  AixLib.Electrical.Utilities.Controllers.StateMachineVoltCtrl ctrl(
+    V_nominal=V_nominal,
+    vThresh=vThresh,
+    tDelay=tDelay)
+    "Model that implements the state machines voltage controller";
+initial equation
+  y = y_start;
+equation
+
+  // Output of the control block
+  y + T*der(y) = ctrl.y;
+
+  // Voltage measurements
+  ctrl.V = terminal.PhaseSystem.systemVoltage(terminal.v);
+
+  // The controller does not consume current
+  terminal.i = zeros(PhaseSystem.n);
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+            {100,100}}), graphics={Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          lineThickness=0.5,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid), Text(
+          extent={{-100,-40},{100,-80}},
+          textColor={0,0,0},
+          lineThickness=0.5,
+          fillColor={0,0,255},
+          fillPattern=FillPattern.Solid,
+          textString="Voltage
+CTRL"),                                   Text(
+          extent={{-100,72},{100,40}},
+          textColor={0,0,0},
+          lineThickness=0.5,
+          fillColor={0,0,255},
+          fillPattern=FillPattern.Solid,
+          textString="%name")}), Documentation(revisions="<html>
+<ul>
+<li>
+March 10, 2014, by Marco Bonvini:<br/>
+Added time constant <code>T</code> and first order filer to avoid
+differentiation of the outputs of the finite state machine.
+</li>
+<li>
+Oct 14, 2014, by Marco Bonvini:<br/>
+Revised model and documentation.
+</li>
+<li>
+Aug 28, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Model representing a voltage controller that unplugs a load when
+its voltage is outside of the accepted thresholds.
+</p>
+<p>
+The model contains a finite state machine controller that detects voltage
+deviations. If the voltage input <code>V</code> exceeds the
+nominal value <code>V_nominal</code> by more than <i>1+V<sub>tr</sub></i>
+then the control signal <code>y</code> becomes zero for
+a period <code>t = tDelay</code>. If after this period the voltage is still
+higher than the thresholds the output remains equal to zero.
+The model has a parameter <code>T</code> that represents the time constant
+associated to the electrical switch. This time constant is used to parametrize
+a first order filter that represents such a dynamic effect. The presence of the first order
+filter avoids that the output of the finite state machine controller
+are differentiated (causing runtime errors).
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end VoltageControl;
diff --git a/AixLib/Electrical/Utilities/package.mo b/AixLib/Electrical/Utilities/package.mo
new file mode 100644
index 0000000000..fbeeccf583
--- /dev/null
+++ b/AixLib/Electrical/Utilities/package.mo
@@ -0,0 +1,33 @@
+within AixLib.Electrical;
+package Utilities "Package with models and functions that are used by other models"
+  extends Modelica.Icons.Package;
+
+
+annotation (
+preferredView="info", Documentation(info="<html>
+<p>
+This package contains utility models and functions.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Aug 28, 2014, by Marco Bonvini:<br/>
+Added documentation.
+</li>
+</ul>
+</html>"),
+Icon(coordinateSystem(extent={{-100.0,-100.0},{100.0,100.0}}), graphics={
+    Polygon(
+      origin={1.3835,-4.1418},
+      rotation=45.0,
+      fillColor={64,64,64},
+      pattern=LinePattern.None,
+      fillPattern=FillPattern.Solid,
+      points={{-15.0,93.333},{-15.0,68.333},{0.0,58.333},{15.0,68.333},{15.0,93.333},{20.0,93.333},{25.0,83.333},{25.0,58.333},{10.0,43.333},{10.0,-41.667},{25.0,-56.667},{25.0,-76.667},{10.0,-91.667},{0.0,-91.667},{0.0,-81.667},{5.0,-81.667},{15.0,-71.667},{15.0,-61.667},{5.0,-51.667},{-5.0,-51.667},{-15.0,-61.667},{-15.0,-71.667},{-5.0,-81.667},{0.0,-81.667},{0.0,-91.667},{-10.0,-91.667},{-25.0,-76.667},{-25.0,-56.667},{-10.0,-41.667},{-10.0,43.333},{-25.0,58.333},{-25.0,83.333},{-20.0,93.333}}),
+    Polygon(
+      origin={10.1018,5.218},
+      rotation=-45.0,
+      fillColor={255,255,255},
+      fillPattern=FillPattern.Solid,
+      points={{-15.0,87.273},{15.0,87.273},{20.0,82.273},{20.0,27.273},{10.0,17.273},{10.0,7.273},{20.0,2.273},{20.0,-2.727},{5.0,-2.727},{5.0,-77.727},{10.0,-87.727},{5.0,-112.727},{-5.0,-112.727},{-10.0,-87.727},{-5.0,-77.727},{-5.0,-2.727},{-20.0,-2.727},{-20.0,2.273},{-10.0,7.273},{-10.0,17.273},{-20.0,27.273},{-20.0,82.273}})}));
+end Utilities;
diff --git a/AixLib/Electrical/Utilities/package.order b/AixLib/Electrical/Utilities/package.order
new file mode 100644
index 0000000000..63f77692bc
--- /dev/null
+++ b/AixLib/Electrical/Utilities/package.order
@@ -0,0 +1,3 @@
+VoltageControl
+Controllers
+Examples
diff --git a/AixLib/Electrical/package.mo b/AixLib/Electrical/package.mo
index 83834775d1..7ff1eae2ca 100644
--- a/AixLib/Electrical/package.mo
+++ b/AixLib/Electrical/package.mo
@@ -1,38 +1,20 @@
 within AixLib;
-package Electrical "This package contains models for electric components such as Photovoltaics or Batteries"
+package Electrical "Package with models for electrical systems"
   extends Modelica.Icons.Package;
 
-  annotation (
-  Documentation(info="<html><p>
-  This library contains electrical components to build up analog and
-  digital circuits, as well as machines to model electrical motors and
-  generators, especially three phase induction machines such as an
-  asynchronous motor.
+
+annotation (Documentation(info="<html>
+<p>
+This package contains models for both DC and AC electrical systems.
 </p>
-</html>"),
-  Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100.0,-100.0},{100.0,100.0}}), graphics={
-    Rectangle(
-      origin={20.3125,82.8571},
-      extent={{-45.3125,-57.8571},{4.6875,-27.8571}}),
-    Line(
-      origin={8.0,48.0},
-      points={{32.0,-58.0},{72.0,-58.0}}),
-    Line(
-      origin={9.0,54.0},
-      points={{31.0,-49.0},{71.0,-49.0}}),
-    Line(
-      origin={-2.0,55.0},
-      points={{-83.0,-50.0},{-33.0,-50.0}}),
-    Line(
-      origin={-3.0,45.0},
-      points={{-72.0,-55.0},{-42.0,-55.0}}),
-    Line(
-      origin={1.0,50.0},
-      points={{-61.0,-45.0},{-61.0,-10.0},{-26.0,-10.0}}),
-    Line(
-      origin={7.0,50.0},
-      points={{18.0,-10.0},{53.0,-10.0},{53.0,-45.0}}),
-    Line(
-      origin={6.2593,48.0},
-      points={{53.7407,-58.0},{53.7407,-93.0},{-66.2593,-93.0},{-66.2593,-58.0}})}));
+</html>"), Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+          {100,100}}), graphics={Line(
+        points={{32,80},{-36,12},{24,12},{-58,-74},{-58,-74}},
+        color={0,0,0},
+        smooth=Smooth.None), Polygon(
+        points={{-58,-74},{-42,-24},{-8,-56},{-58,-74}},
+        lineColor={0,0,0},
+        smooth=Smooth.None,
+        fillPattern=FillPattern.Solid,
+        fillColor={0,0,0})}));
 end Electrical;
diff --git a/AixLib/Electrical/package.order b/AixLib/Electrical/package.order
index 20674fd4b8..ce123540ca 100644
--- a/AixLib/Electrical/package.order
+++ b/AixLib/Electrical/package.order
@@ -1,2 +1,12 @@
+UsersGuide
+AC
+DC
+Icons
 Machines
 PVSystem
+PhaseSystems
+Transmission
+Utilities
+Types
+Interfaces
+BaseClasses
diff --git a/AixLib/Examples/SimpleHouse.mo b/AixLib/Examples/SimpleHouse.mo
new file mode 100644
index 0000000000..8379db2ce5
--- /dev/null
+++ b/AixLib/Examples/SimpleHouse.mo
@@ -0,0 +1,380 @@
+within AixLib.Examples;
+model SimpleHouse
+  "Illustrative example of a simple heating, ventilation and room model"
+  extends Modelica.Icons.Example;
+
+  package MediumAir = AixLib.Media.Air;
+  package MediumWater = AixLib.Media.Water;
+
+  parameter Modelica.Units.SI.Area AWall=100 "Wall area";
+  parameter Modelica.Units.SI.Area AWin=5 "Window area";
+  parameter Real gWin(min=0, max=1, unit="1") = 0.3 "Solar heat gain coefficient of window";
+  parameter Modelica.Units.SI.Volume VZone=AWall*3 "Wall area";
+  parameter Modelica.Units.SI.HeatFlowRate QHea_flow_nominal=700
+    "Nominal capacity of heating system";
+  parameter Modelica.Units.SI.MassFlowRate mWat_flow_nominal=QHea_flow_nominal/
+      10/4200 "Nominal mass flow rate for water loop";
+  parameter Modelica.Units.SI.MassFlowRate mAir_flow_nominal=VZone*2*1.2/3600
+    "Nominal mass flow rate for air loop";
+
+  parameter Modelica.Units.SI.PressureDifference dpAir_nominal=200
+    "Pressure drop at nominal mass flow rate for air loop";
+  parameter Boolean allowFlowReversal=false
+    "= false because flow will not reverse in these circuits";
+
+  Modelica.Thermal.HeatTransfer.Components.HeatCapacitor walCap(
+    T(fixed=true),
+    C=10*AWall*0.05*1000*1000)
+    "Thermal mass of walls"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={170,0})));
+  Fluid.MixingVolumes.MixingVolume zon(
+    redeclare package Medium = MediumAir,
+    V=VZone,
+    nPorts=2,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    m_flow_nominal=mAir_flow_nominal,
+    massDynamics=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial)
+    "Very based zone air model"
+    annotation (Placement(transformation(extent={{160,50},{180,30}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalResistor conRes(R=1/2/AWall)
+    "Thermal resistance for convective heat transfer with h=2" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={110,20})));
+  Fluid.HeatExchangers.Radiators.RadiatorEN442_2 rad(
+    redeclare package Medium = MediumWater,
+    T_a_nominal=273.15 + 50,
+    T_b_nominal=273.15 + 40,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    allowFlowReversal=allowFlowReversal,
+    Q_flow_nominal=QHea_flow_nominal)
+                                 "Radiator"
+    annotation (Placement(transformation(extent={{120,-140},{140,-120}})));
+
+  Fluid.Sources.Boundary_pT bouAir(
+    redeclare package Medium = MediumAir,
+    nPorts=2,
+    use_T_in=true) "Air boundary with constant temperature" annotation (
+      Placement(transformation(extent={{-10,-10},{10,10}}, origin={-110,140})));
+  Fluid.Sources.Boundary_pT bouWat(redeclare package Medium = MediumWater,
+      nPorts=1) "Pressure bound for water circuit" annotation (Placement(
+        transformation(extent={{-10,-10},{10,10}}, origin={20,-180})));
+  BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
+    filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos"))
+    "Weather data reader"
+    annotation (Placement(transformation(extent={{-180,-10},{-160,10}})));
+  BoundaryConditions.WeatherData.Bus weaBus "Weather data bus"
+    annotation (Placement(transformation(extent={{-140,-10},{-120,10}}),
+        iconTransformation(extent={{-160,-10},{-140,10}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalResistor walRes(R=0.25/AWall/
+        0.04) "Thermal resistor for wall: 25 cm of rockwool"
+    annotation (Placement(transformation(extent={{60,-10},{80,10}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature TOut
+    "Exterior temperature boundary condition"
+    annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+  Fluid.HeatExchangers.HeaterCooler_u heaWat(
+    redeclare package Medium = MediumWater,
+    m_flow_nominal=mWat_flow_nominal,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    allowFlowReversal=allowFlowReversal,
+    dp_nominal=5000,
+    Q_flow_nominal=QHea_flow_nominal)
+                                 "Heater for water circuit"
+    annotation (Placement(transformation(extent={{60,-140},{80,-120}})));
+
+  Fluid.Movers.FlowControlled_m_flow pum(
+    redeclare package Medium = MediumWater,
+    use_inputFilter=false,
+    m_flow_nominal=mWat_flow_nominal,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    allowFlowReversal=allowFlowReversal,
+    nominalValuesDefineDefaultPressureCurve=true,
+    inputType=AixLib.Fluid.Types.InputType.Stages,
+    massFlowRates=mWat_flow_nominal*{1}) "Pump"
+    annotation (Placement(transformation(extent={{140,-190},{120,-170}})));
+  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor senTemZonAir
+    "Zone air temperature sensor"
+    annotation (Placement(transformation(extent={{120,170},{100,190}})));
+  Fluid.Actuators.Dampers.Exponential vavDam(
+    redeclare package Medium = MediumAir,
+    from_dp=true,
+    m_flow_nominal=mAir_flow_nominal,
+    dpDamper_nominal=10,
+    dpFixed_nominal=dpAir_nominal - 10) "Damper" annotation (Placement(
+        transformation(extent={{-10,10},{10,-10}}, origin={110,130})));
+
+  Fluid.Movers.FlowControlled_dp fan(
+    redeclare package Medium = MediumAir,
+    dp_nominal=dpAir_nominal,
+    use_inputFilter=false,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    nominalValuesDefineDefaultPressureCurve=true,
+    m_flow_nominal=mAir_flow_nominal,
+    show_T=true) "Constant head fan" annotation (Placement(transformation(
+          extent={{-10,10},{10,-10}}, origin={-10,130})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow win
+    "Very simple window model"
+    annotation (Placement(transformation(extent={{60,-50},{80,-30}})));
+  Fluid.HeatExchangers.ConstantEffectiveness hexRec(
+    redeclare package Medium1 = MediumAir,
+    redeclare package Medium2 = MediumAir,
+    dp1_nominal=0,
+    dp2_nominal=0,
+    m1_flow_nominal=mAir_flow_nominal,
+    m2_flow_nominal=mAir_flow_nominal,
+    eps=0.85) "Heat exchanger for heat recuperation"
+    annotation (Placement(transformation(extent={{-45,124},{-75,156}})));
+  Modelica.Blocks.Logical.Hysteresis hysRad(uLow=273.15 + 20, uHigh=273.15 + 22)
+    "Hysteresis controller for radiator"
+    annotation (Placement(transformation(extent={{-80,-120},{-60,-100}})));
+  Modelica.Blocks.Logical.Not not1
+    "negation for enabling heating when temperatur is low"
+    annotation (Placement(transformation(extent={{-40,-120},{-20,-100}})));
+  Modelica.Blocks.Math.BooleanToReal booToRea "Boolean to real"
+    annotation (Placement(transformation(extent={{0,-120},{20,-100}})));
+  Modelica.Blocks.Sources.Constant con_dp(k=dpAir_nominal) "Pressure head"
+    annotation (Placement(transformation(extent={{-50,90},{-30,110}})));
+
+  Modelica.Blocks.Math.Gain gaiWin(k=AWin*gWin)
+    "Gain for window solar transmittance and area as HGloHor is in W/m2"
+    annotation (Placement(transformation(extent={{20,-50},{40,-30}})));
+  Modelica.Blocks.Math.BooleanToInteger booToInt "Boolean to integer"
+    annotation (Placement(transformation(extent={{0,-160},{20,-140}})));
+  Controls.Continuous.LimPID conDam(
+      controllerType=Modelica.Blocks.Types.SimpleController.P,
+      yMin=0.25) "Controller for damper"
+    annotation (Placement(transformation(extent={{80,90},{100,110}})));
+  Modelica.Blocks.Sources.Constant TSetRoo(k=273.15 + 24)
+    "Room temperature set point for air system"
+    annotation (Placement(transformation(extent={{40,90},{60,110}})));
+  Fluid.HeatExchangers.SensibleCooler_T cooAir(
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    allowFlowReversal=allowFlowReversal,
+    m_flow_nominal=mAir_flow_nominal,
+    dp_nominal=0,
+    redeclare package Medium = MediumAir) "Cooling for supply air"
+    annotation (Placement(transformation(extent={{30,140},{50,120}})));
+  Modelica.Blocks.Sources.Constant TSupAirCoo(k=273.15 + 20)
+    "Cooling setpoint for supply air"
+    annotation (Placement(transformation(extent={{0,90},{20,110}})));
+equation
+  connect(conRes.port_a, zon.heatPort)
+    annotation (Line(points={{110,30},{110,40},{160,40}},   color={191,0,0}));
+  connect(weaDat.weaBus, weaBus) annotation (Line(
+      points={{-160,0},{-130,0}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(walRes.port_b, walCap.port) annotation (Line(points={{80,0},{122,0},{122,
+          1.77636e-15},{160,1.77636e-15}},
+                         color={191,0,0}));
+  connect(TOut.T, weaBus.TDryBul)
+    annotation (Line(points={{-82,0},{-130,0}},           color={0,0,127}));
+  connect(TOut.port, walRes.port_a)
+    annotation (Line(points={{-60,0},{60,0}},     color={191,0,0}));
+  connect(heaWat.port_b, rad.port_a) annotation (Line(points={{80,-130},{120,-130}},
+                       color={0,127,255}));
+  connect(bouWat.ports[1], heaWat.port_a) annotation (Line(points={{30,-180},{42,
+          -180},{42,-130},{60,-130}}, color={0,127,255}));
+  connect(rad.port_b, pum.port_a) annotation (Line(points={{140,-130},{150,-130},
+          {150,-180},{140,-180}},color={0,127,255}));
+  connect(senTemZonAir.port, zon.heatPort) annotation (Line(points={{120,180},{160,
+          180},{160,40}},                      color={191,0,0}));
+  connect(bouAir.ports[1], hexRec.port_b1) annotation (Line(points={{-100,139},{
+          -100,149.6},{-75,149.6}},
+                              color={0,127,255}));
+  connect(rad.heatPortCon, zon.heatPort) annotation (Line(points={{128,-122.8},{
+          128,40},{160,40}},                    color={191,0,0}));
+  connect(not1.y, booToRea.u) annotation (Line(points={{-19,-110},{-2,-110}},
+                  color={255,0,255}));
+  connect(not1.u, hysRad.y) annotation (Line(points={{-42,-110},{-59,-110}},
+                  color={255,0,255}));
+  connect(booToRea.y, heaWat.u) annotation (Line(points={{21,-110},{40,-110},{40,
+          -124},{58,-124}}, color={0,0,127}));
+  connect(heaWat.port_a, pum.port_b) annotation (Line(points={{60,-130},{42,-130},
+          {42,-180},{120,-180}},          color={0,127,255}));
+  connect(con_dp.y, fan.dp_in) annotation (Line(points={{-29,100},{-10,100},{-10,
+          118}},           color={0,0,127}));
+  connect(gaiWin.y, win.Q_flow) annotation (Line(points={{41,-40},{60,-40}},
+                           color={0,0,127}));
+  connect(gaiWin.u, weaBus.HGloHor) annotation (Line(points={{18,-40},{-130,-40},
+          {-130,0}},             color={0,0,127}));
+  connect(booToInt.u, not1.y) annotation (Line(points={{-2,-150},{-11,-150},{-11,
+          -110},{-19,-110}}, color={255,0,255}));
+  connect(booToInt.y, pum.stage) annotation (Line(points={{21,-150},{130,-150},{
+          130,-168}},       color={255,127,0}));
+  connect(hexRec.port_b2, fan.port_a) annotation (Line(points={{-45,130.4},{-30,
+          130.4},{-30,130},{-20,130}}, color={0,127,255}));
+  connect(vavDam.port_b, zon.ports[1])
+    annotation (Line(points={{120,130},{140,130},{140,50},{169,50}},
+                                                          color={0,127,255}));
+  connect(senTemZonAir.T, hysRad.u) annotation (Line(points={{99,180},{-209.25,180},
+          {-209.25,-110},{-82,-110}},         color={0,0,127}));
+  connect(senTemZonAir.T,conDam. u_s) annotation (Line(points={{99,180},{74,180},
+          {74,100},{78,100}},             color={0,0,127}));
+  connect(conDam.y, vavDam.y) annotation (Line(points={{101,100},{110,100},{110,
+          118}},color={0,0,127}));
+  connect(TSetRoo.y,conDam. u_m) annotation (Line(points={{61,100},{70,100},{70,
+          82},{90,82},{90,88}},
+                         color={0,0,127}));
+  connect(fan.port_b, cooAir.port_a)
+    annotation (Line(points={{0,130},{30,130}},   color={0,127,255}));
+  connect(cooAir.port_b, vavDam.port_a)
+    annotation (Line(points={{50,130},{100,130}},         color={0,127,255}));
+  connect(TSupAirCoo.y, cooAir.TSet) annotation (Line(points={{21,100},{24,100},
+          {24,122},{28,122}},color={0,0,127}));
+  connect(bouAir.T_in, weaBus.TDryBul) annotation (Line(points={{-122,144},{
+          -130,144},{-130,0}},  color={0,0,127}));
+  connect(bouAir.ports[2], hexRec.port_a2) annotation (Line(points={{-100,141},{
+          -100,130.4},{-75,130.4}}, color={0,127,255}));
+  connect(hexRec.port_a1, zon.ports[2]) annotation (Line(points={{-45,149.6},{171,
+          149.6},{171,50}}, color={0,127,255}));
+  connect(conRes.port_b, walCap.port) annotation (Line(points={{110,10},{110,0},
+          {122,0},{122,1.77636e-15},{160,1.77636e-15}}, color={191,0,0}));
+  connect(win.port, walCap.port) annotation (Line(points={{80,-40},{110,-40},{110,
+          0},{132,0},{132,1.77636e-15},{160,1.77636e-15}}, color={191,0,0}));
+  connect(rad.heatPortRad, walCap.port) annotation (Line(points={{132,-122.8},{132,
+          1.77636e-15},{160,1.77636e-15}}, color={191,0,0}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-220,
+            -220},{220,220}}), graphics={
+        Rectangle(
+          extent={{-200,200},{200,80}},
+          fillColor={238,238,238},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Rectangle(
+          extent={{-200,-80.25},{200,-199.75}},
+          fillColor={238,238,238},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Rectangle(
+          extent={{-199.75,60},{-20.25,-60}},
+          fillColor={238,238,238},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Text(
+          extent={{-63,182},{-197,198}},
+          textColor={0,0,127},
+          fillColor={255,213,170},
+          fillPattern=FillPattern.Solid,
+          textString="Cooling and ventilation"),
+        Rectangle(
+          extent={{0,60},{200,-60}},
+          fillColor={238,238,238},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Text(
+          extent={{64.5,40.5},{-4.5,59.5}},
+          textColor={0,0,127},
+          fillColor={255,213,170},
+          fillPattern=FillPattern.Solid,
+          textString="Building"),
+        Text(
+          extent={{-137,-99},{-203,-81}},
+          textColor={0,0,127},
+          fillColor={255,213,170},
+          fillPattern=FillPattern.Solid,
+          textString="Heating"),
+        Text(
+          extent={{-141,41},{-199,59}},
+          textColor={0,0,127},
+          fillColor={255,213,170},
+          fillPattern=FillPattern.Solid,
+          textString="Weather")}),
+    experiment(Tolerance=1e-06, StopTime=3.1536e+07),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 15, 2023, by Jelger Jansen:<br/>
+Move the example model to <a href=\"modelica://AixLib.Examples\">AixLib.Examples</a>, 
+update the information section, and revise lay-out.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1791\">IBPSA, #1791</a>.
+</li>
+<li>
+June 15, 2022, by Hongxiang Fu:<br/>
+Changed <code>conDam.yMin</code> from 0.1 to 0.25.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1624\">IBPSA, #1624</a>.
+</li>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">IBPSA, #763</a>.
+</li>
+<li>
+November 10, 2016, by Michael Wetter:<br/>
+Connected supply air temperature to outdoor air temperature,
+added cooling to supply air,
+changed capacity of heating system, switched heating pump off when heater is off,
+and added proportional controller for the air damper.<br/>
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/584\">IBPSA, #584</a>.
+</li>
+<li>
+September 9, 2016, by Michael Wetter:<br/>
+Corrected error in window model, as the solar heat gain was
+not multiplied with the window area. Dymola 2017 reported this
+error due to mismatching units of <code>W/m2</code> and <code>W</code>.
+</li>
+<li>
+June 23, 2016, by Michael Wetter:<br/>
+Changed graphical annotation.
+</li>
+<li>
+March 11, 2016, by Michael Wetter:<br/>
+Corrected wrong limits for <code>hysAir</code> so that
+<code>uLow &lt; uHigh</code>.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/429\">IBPSA, #429</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">IBPSA, #404</a>.
+</li>
+<li>
+September 19, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model contains a simple model of a house
+with a heating system, ventilation, and weather boundary conditions.
+It serves as a demonstration case of how the <code>AixLib</code> library can be used.
+</p>
+<p>
+A step-by-step tutorial on how to build up this model can be found in
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse\">
+AixLib.Examples.Tutorial.SimpleHouse</a>.
+There are however some minor differences between this model and the models in the tutorial:
+</p>
+<ul>
+<li>
+Different numerical values are used for almost all model parameters.
+</li>
+<li>
+The solar irradiation (in <i>W/m<sup>2</sup></i>) is calculated as
+the global horizontal irradiation multiplied with a solar heat gain coefficient
+instead of the direct normal irradiation.
+</li>
+<li>
+The ventilation system is equiped with a cooler that sets the temperature
+of the air flow entering the zone equal to a constant value of <i>20°C</i>.
+</li>
+<li>
+The damper in the ventilation system is operated by
+a proportional-controller instead of a hysteresis controller.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Examples/SimpleHouse.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleHouse;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse0.mo b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse0.mo
new file mode 100644
index 0000000000..9bd028c2bb
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse0.mo
@@ -0,0 +1,103 @@
+within AixLib.Examples.Tutorial.SimpleHouse;
+model SimpleHouse0
+  "Start file for simple house example"
+  extends Modelica.Icons.Example;
+  package MediumAir = AixLib.Media.Air "Medium model for air";
+  package MediumWater = AixLib.Media.Water "Medium model for water";
+  parameter Modelica.Units.SI.Area AWall = 100 "Wall area";
+  parameter Modelica.Units.SI.Length dWall = 0.25 "Wall thickness";
+  parameter Modelica.Units.SI.ThermalConductivity kWall = 0.04 "Wall thermal conductivity";
+  parameter Modelica.Units.SI.Density rhoWall = 2000 "Wall density";
+  parameter Modelica.Units.SI.SpecificHeatCapacity cpWall = 1000 "Wall specific heat capacity";
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+        Modelica.Utilities.Files.loadResource(
+        "modelica://AixLib/Resources/weatherdata/USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos"))
+    "Weather data reader"
+    annotation (Placement(transformation(extent={{-180,-10},{-160,10}})));
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather data bus"
+    annotation (Placement(transformation(extent={{-140,-10},{-120,10}}),
+        iconTransformation(extent={{-152,-10},{-132,10}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature TOut
+    "Exterior temperature boundary condition"
+    annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+equation
+  connect(weaDat.weaBus, weaBus) annotation (Line(
+      points={{-160,0},{-130,0}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(TOut.T, weaBus.TDryBul)
+    annotation (Line(points={{-82,0},{-130,0}},           color={0,0,127}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-220,
+            -220},{220,220}}), graphics={
+        Rectangle(
+          extent={{-200,60},{-20,-60}},
+          fillColor={238,238,238},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Rectangle(
+          extent={{-200,-80},{200,-200}},
+          fillColor={238,238,238},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Rectangle(
+          extent={{-200,200},{200,80}},
+          fillColor={238,238,238},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Rectangle(
+          extent={{0,60},{200,-60}},
+          fillColor={238,238,238},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Text(
+          extent={{57.25,40.25},{2.75,59.75}},
+          textColor={0,0,127},
+          fillColor={255,213,170},
+          fillPattern=FillPattern.Solid,
+          textString="Building"),
+        Text(
+          extent={{-137,-99},{-203,-81}},
+          textColor={0,0,127},
+          fillColor={255,213,170},
+          fillPattern=FillPattern.Solid,
+          textString="Heating"),
+        Text(
+          extent={{-102,39},{-198,61}},
+          textColor={0,0,127},
+          fillColor={255,213,170},
+          fillPattern=FillPattern.Solid,
+          textString="Weather inputs"),
+        Text(
+          extent={{-61,179},{-199,201}},
+          textColor={0,0,127},
+          fillColor={255,213,170},
+          fillPattern=FillPattern.Solid,
+          textString="Cooling and ventilation")}),
+    experiment(Tolerance=1E-6, StopTime=1e+06),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 4, 2023, by Jelger Jansen:<br/>
+Replace IDEAS by AixLib models and general revision/update of the model.
+</li>
+<li>
+October 11, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model is used as the starting point for the
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse\">AixLib.Examples.Tutorial.SimpleHouse</a>
+tutorial.
+It contains a weather data reader and a <code>PrescribedTemperature</code> component
+that allows the user to connect thermal components to the dry bulb temperature.
+It was based on from the Modelica crash course organised by KU Leuven
+(<a href=\"https://github.com/open-ideas/__CrashCourse__\">https://github.com/open-ideas/__CrashCourse__</a>).
+</p>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse0.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleHouse0;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse1.mo b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse1.mo
new file mode 100644
index 0000000000..a742bdc161
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse1.mo
@@ -0,0 +1,91 @@
+within AixLib.Examples.Tutorial.SimpleHouse;
+model SimpleHouse1 "Building wall model"
+  extends SimpleHouse0;
+
+  Modelica.Thermal.HeatTransfer.Components.HeatCapacitor walCap(
+    C=AWall*dWall*cpWall*rhoWall,
+    T(fixed=true))
+    "Thermal mass of wall"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={170,0})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalResistor walRes(
+    R=dWall/AWall/kWall) "Thermal resistor for wall: 25 cm of rockwool"
+    annotation (Placement(transformation(extent={{60,-10},{80,10}})));
+equation
+  connect(walRes.port_b, walCap.port) annotation (Line(points={{80,0},{100,0},{100,
+          1.77636e-15},{160,1.77636e-15}},      color={191,0,0}));
+  connect(TOut.port, walRes.port_a)
+    annotation (Line(points={{-60,0},{60,0}}, color={191,0,0}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-220,
+            -220},{220,220}})),
+    experiment(Tolerance=1e-6, StopTime=1e+06),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 4, 2023, by Jelger Jansen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+A very simple building envelope model will be constructed manually using thermal resistors and heat capacitors.
+The house consists of a wall represented by a single heat capacitor and a thermal resistor.
+The boundary temperature are already included in
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse0\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse0</a>.
+The wall has a surface area of <i>A<sub>wall</sub>=100 m<sup>2</sup></i>,
+a thickness of <i>d<sub>wall</sub>=25 cm</i>,
+a thermal conductivity of <i>k<sub>wall</sub>=0.04 W/(m K)</i>,
+a density of <i>&rho;<sub>wall</sub>=2000 kg/m<sup>3</sup></i>,
+and a specific heat capacity of <i>c<sub>p,wall</sub>= 1000 J/(kg K)</i>
+</p>
+<p>
+These parameters are already declared in the equation section of
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse0\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse0</a>.
+You can use this way of declaring parameters in the remainder of this exercise, but this is not required.
+</p>
+<p>
+The conductive thermal resistance value of a wall may be computed as <i>R=d/(A*k)</i>.
+The heat capacity value of a wall may be computed as <i>C=A*d*c<sub>p</sub>*&rho;</i>
+</p>
+<h4>Required models</h4>
+<ul>
+<li>
+<a href=\"modelica://Modelica.Thermal.HeatTransfer.Components.HeatCapacitor\">
+Modelica.Thermal.HeatTransfer.Components.HeatCapacitor</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Thermal.HeatTransfer.Components.ThermalResistor\">
+Modelica.Thermal.HeatTransfer.Components.ThermalResistor</a>
+</li>
+</ul>
+<h4>Connection instructions</h4>
+<p>
+Connect one side of the thermal resistor to the output of <code>PrescribedTemperature</code>
+and the other side of the thermal resistor to the heat capacitor.
+</p>
+<h4>Reference result</h4>
+<p>
+If you correctly added the model of the heat capacitor,
+connected it to the resistor and added the parameter values for <i>C</i>,
+then you should be able to simulate the model.
+To do this, press the <i>Simulation Setup</i> and set the model <i>Stop time</i> to 1e6 seconds.
+You can now simulate the model by pressing the <i>Simulate</i> button.
+</p>
+<p>
+You can plot individual variables values by clicking on their name in the variable browser on the left.
+Now plot the wall capacitor temperature value <i>T</i>.
+It should look like the figure below (1 Ms is around 12 days).
+</p>
+<p align=\"center\">
+<img alt=\"Wall temperature as function of time.\"
+src=\"modelica://AixLib/Resources/Images/Examples/Tutorial/SimpleHouse/result1.png\" width=\"1000\"/>
+</p>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse1.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleHouse1;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse2.mo b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse2.mo
new file mode 100644
index 0000000000..04158f57e1
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse2.mo
@@ -0,0 +1,80 @@
+within AixLib.Examples.Tutorial.SimpleHouse;
+model SimpleHouse2 "Building window model"
+  extends SimpleHouse1;
+
+  parameter Modelica.Units.SI.Area AWin=2 "Window area";
+
+  Modelica.Blocks.Math.Gain gaiWin(k=AWin)
+    "Gain for solar irradiance through the window"
+    annotation (Placement(transformation(extent={{20,-50},{40,-30}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow win
+    "Very simple window model"
+    annotation (Placement(transformation(extent={{60,-50},{80,-30}})));
+equation
+  connect(gaiWin.y, win.Q_flow)
+    annotation (Line(points={{41,-40},{60,-40}},   color={0,0,127}));
+  connect(gaiWin.u, weaBus.HDirNor) annotation (Line(points={{18,-40},{-130,-40},
+          {-130,0}},   color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(win.port, walCap.port) annotation (Line(points={{80,-40},{110,-40},{110,
+          1.77636e-15},{160,1.77636e-15}}, color={191,0,0}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-220,
+            -220},{220,220}})),
+    experiment(Tolerance=1e-6, StopTime=1e+06),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 4, 2023, by Jelger Jansen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+The window has a surface area of <i>2 m<sup>2</sup></i>.
+In this simple model we will therefore assume that
+two times the outdoor solar irradiance is injected as heat onto the inside of the wall.
+</p>
+<h4>Required models</h4>
+<ul>
+<li>
+<a href=\"modelica://Modelica.Blocks.Math.Gain\">
+Modelica.Blocks.Math.Gain</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow\">
+Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow</a>
+</li>
+</ul>
+<h4>Connection instructions</h4>
+<p>
+To be able to use the value of the outdoor solar irradiance
+you will need to access the weather data reader.
+To do this, make a connection to the <code>weaBus</code>.
+In the dialog box, select <code>HDirNor</code>,
+which is the direct solar irradiance on a surface of <i>1 m<sup>2</sup></i>,
+perpendicular to the sun rays.
+Set the gain factor <code>k</code> to 2,
+in order to get the solar irradiance through the window of <i>2 m<sup>2</sup></i>.
+</p>
+<p>
+Make a connection with the <code>PrescribedHeatFlow</code> as well.
+This block makes the connection between the heat flow from the gain, represented as a real value,
+and a heat port that is compatible with the connectors of the thermal capacitance and resistance.
+</p>
+<h4>Reference result</h4>
+<p>
+The result with and without the window model is plotted in the figure below.
+</p>
+<p align=\"center\">
+<img alt=\"Wall temperature as function of time, with (blue) and without (red) window.\"
+src=\"modelica://AixLib/Resources/Images/Examples/Tutorial/SimpleHouse/result2.png\" width=\"1000\"/>
+</p>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse2.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleHouse2;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse3.mo b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse3.mo
new file mode 100644
index 0000000000..1991c2ba0a
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse3.mo
@@ -0,0 +1,88 @@
+within AixLib.Examples.Tutorial.SimpleHouse;
+model SimpleHouse3 "Air model"
+  extends SimpleHouse2;
+
+  parameter Modelica.Units.SI.Volume VZone=8*8*3 "Zone volume";
+  parameter Modelica.Units.SI.MassFlowRate mAir_flow_nominal=1
+    "Nominal mass flow rate for air loop";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hWall=2
+    "Convective heat transfer coefficient at the wall";
+
+  Modelica.Thermal.HeatTransfer.Components.ThermalResistor conRes(R=1/hWall/
+        AWall) "Thermal resistance for convective heat transfer" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={110,20})));
+  AixLib.Fluid.MixingVolumes.MixingVolume zon(
+    redeclare package Medium = MediumAir,
+    V=VZone,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    m_flow_nominal=mAir_flow_nominal) "Very simple zone air model"
+    annotation (Placement(transformation(extent={{160,50},{180,30}})));
+equation
+  connect(zon.heatPort, conRes.port_a)
+    annotation (Line(points={{160,40},{110,40},{110,30}},   color={191,0,0}));
+  connect(conRes.port_b, walCap.port) annotation (Line(points={{110,10},{110,1.77636e-15},
+          {160,1.77636e-15}}, color={191,0,0}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-220,
+            -220},{220,220}})),
+    experiment(Tolerance=1e-6, StopTime=1e+06),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 4, 2023, by Jelger Jansen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+To increase the model detail we now add an air model assuming the zone is <i>8m</i> x <i>8m</i> x <i>3m</i> in size.
+The air will exchange heat with the wall.
+This may be modelled using a thermal resistance representing
+the convective heat resistance which is equal to <i>R<sub>conv</sub>=1/(h*A)</i>,
+where <i>A</i> is the heat exchange surface area and <i>h=2 W/(m<sup>2</sup>*K)</i> is the convective heat transfer coefficient.
+</p>
+<h4>Required models</h4>
+<ul>
+<li>
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
+AixLib.Fluid.MixingVolumes.MixingVolume</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Thermal.HeatTransfer.Components.ThermalResistor\">
+Modelica.Thermal.HeatTransfer.Components.ThermalResistor</a>
+</li>
+</ul>
+<h4>Connection instructions</h4>
+<p>
+The <code>MixingVolume</code> <code>Medium</code> parameter contains information about
+the type of fluid and its properties that should be modelled by the <code>MixingVolume</code>.
+Set its value to <code>MediumAir</code>, which is declared in the template,
+by typing <code>redeclare package Medium = MediumAir</code>.
+For the nominal mass flow rate you may assume a value of <i>1 kg/s</i> for now.
+You will have to change this value once you add a ventilation system to the model (see
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse6\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse6</a>).
+Finally, set the <code>energyDynamics</code> of the <code>MixingVolume</code>,
+which can be found in the <code>Dynamics</code> tab of the model parameter window, to <code>FixedInitial</code>.
+</p>
+<p>
+Make a connection with the <code>PrescribedHeatFlow</code> as well.
+This block makes the connection between the heat flow from the gain, represented as a real value,
+and a heat port that is compatible with the connectors of the thermal capacitance and resistance.
+</p>
+<h4>Reference result</h4>
+<p>
+The result with and without the air model is plotted in the figure below.
+</p>
+<p align=\"center\">
+<img alt=\"Wall temperature as function of time, with (green) and without (blue) air model.\"
+src=\"modelica://AixLib/Resources/Images/Examples/Tutorial/SimpleHouse/result3.png\" width=\"1000\"/>
+</p>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse3.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleHouse3;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse4.mo b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse4.mo
new file mode 100644
index 0000000000..08038c74f1
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse4.mo
@@ -0,0 +1,153 @@
+within AixLib.Examples.Tutorial.SimpleHouse;
+model SimpleHouse4 "Heating model"
+  extends SimpleHouse3;
+
+  constant Boolean use_constantHeater=true
+    "To enable/disable the connection between the constant source and heater and circulation pump";
+
+  parameter Modelica.Units.SI.HeatFlowRate QHea_flow_nominal=3000
+    "Nominal capacity of heating system";
+  parameter Modelica.Units.SI.MassFlowRate mWat_flow_nominal=0.1
+    "Nominal mass flow rate for water loop";
+
+
+  AixLib.Fluid.HeatExchangers.Radiators.RadiatorEN442_2 rad(
+    redeclare package Medium = MediumWater,
+    T_a_nominal=333.15,
+    T_b_nominal=313.15,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    allowFlowReversal=false,
+    Q_flow_nominal=QHea_flow_nominal) "Radiator"
+    annotation (Placement(transformation(extent={{140,-140},{160,-120}})));
+
+  AixLib.Fluid.HeatExchangers.HeaterCooler_u heaWat(
+    redeclare package Medium = MediumWater,
+    m_flow_nominal=mWat_flow_nominal,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    allowFlowReversal=false,
+    dp_nominal=5000,
+    Q_flow_nominal=QHea_flow_nominal) "Heater for water circuit"
+    annotation (Placement(transformation(extent={{60,-140},{80,-120}})));
+
+  Fluid.Movers.Preconfigured.FlowControlled_m_flow pum(
+    redeclare package Medium = MediumWater,
+    use_inputFilter=false,
+    m_flow_nominal=mWat_flow_nominal,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    allowFlowReversal=false) "Pump"
+    annotation (Placement(transformation(extent={{110,-190},{90,-170}})));
+
+  AixLib.Fluid.Sources.Boundary_pT bouWat(
+    redeclare package Medium = MediumWater,
+    nPorts=1)
+    "Pressure bound for water circuit"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={20,-180})));
+  Modelica.Blocks.Sources.Constant conHea(k=1)
+    if use_constantHeater "Gain for heater"
+    annotation (Placement(transformation(extent={{80,-110},{60,-90}})));
+  Modelica.Blocks.Sources.Constant conPum(k=mWat_flow_nominal)
+    if use_constantHeater "Gain for pump"
+    annotation (Placement(transformation(extent={{130,-160},{110,-140}})));
+equation
+  connect(heaWat.port_b,rad. port_a) annotation (Line(points={{80,-130},{140,-130}},
+                       color={0,127,255}));
+  connect(rad.port_b, pum.port_a) annotation (Line(points={{160,-130},{175,-130},
+          {175,-180},{110,-180}}, color={0,127,255}));
+  connect(heaWat.port_a, pum.port_b) annotation (Line(points={{60,-130},{39.75,-130},
+          {39.75,-180},{90,-180}},       color={0,127,255}));
+  connect(rad.heatPortCon, zon.heatPort) annotation (Line(points={{148,-122.8},{
+          148,40},{160,40}},   color={191,0,0}));
+  connect(rad.heatPortRad, walCap.port) annotation (Line(points={{152,-122.8},{152,
+          1.77636e-15},{160,1.77636e-15}},                     color={191,0,0}));
+  connect(conPum.y, pum.m_flow_in) annotation (Line(points={{109,-150},{100,-150},
+          {100,-168}}, color={0,0,127}));
+  connect(conHea.y, heaWat.u) annotation (Line(points={{59,-100},{40,-100},{40,-124},
+          {58,-124}}, color={0,0,127}));
+  connect(bouWat.ports[1], pum.port_b)
+    annotation (Line(points={{30,-180},{90,-180}}, color={0,127,255}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-220,
+            -220},{220,220}})),
+    experiment(Tolerance=1e-6, StopTime=1e+06),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 4, 2023, by Jelger Jansen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+The wall temperature (and therefore the room temperature) is quite low.
+In this step a heating system is added to resolve this. It consists of a radiator, a pump and a heater.
+The radiator has a nominal power of <i>3 kW</i> for an inlet and outlet temperature of the radiator of <i>60°C</i>
+and <i>40°C</i>, and a room air and radiative temperature of <i>20°C</i>.
+The pump has a (nominal) mass flow rate of <i>0.1 kg/s</i>.
+Since the heating system uses water as a heat carrier fluid,
+the media for the models in the heating circuit should be set to <i>MediumWater</i>.
+</p>
+<h4>Required models</h4>
+<ul>
+<li>
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
+AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>
+</li>
+<li>
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Radiators.RadiatorEN442_2\">
+AixLib.Fluid.HeatExchangers.Radiators.RadiatorEN442_2</a>
+</li>
+<li>
+<a href=\"modelica://AixLib.Fluid.Movers.Preconfigured.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.Preconfigured.FlowControlled_m_flow</a>
+</li>
+<li>
+<a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Blocks.Sources.Constant\">
+Modelica.Blocks.Sources.Constant</a>
+</li>
+</ul>
+<h4>Connection instructions</h4>
+<p>
+The radiator contains one port for convective heat transfer and one for radiative heat transfer.
+Connect both in a reasonable way. Since the heating system uses water as a heat carrier fluid,
+the media for the models should be set to <code>MediumWater</code>.
+</p>
+<p>
+The <code>Boundary_pT</code> model needs to be used to set an absolute pressure somewhere in the system.
+Otherwise the absolute pressure in the system is undefined.
+Pressure difference modelling may be disregarded in the heating circuit
+since the chosen pump sets a fixed mass flow rate regardless of the pressure drop.
+</p>
+<p>
+Set the heater input to <i>1</i>, meaning that it will produce <i>1</i> times its nominal power.
+</p>
+<h4>Implementation</h4>
+<p>
+The pump and the heater need a control input, which we set here to a constant
+of <i>1</i>.
+However, in the next version of this model, we want to connect an actual controller to these models.
+We can therefore introduce a <code>Boolean constant</code> (or a <code>Boolean parameter</code>
+would also work), and use this to conditionally remove the Modelica block
+that outputs the control signal. When Modelica removes such a block, then all
+connections to it will also be removed.
+</p>
+<h4>Reference result</h4>
+<p>
+The result of the air temperature is plotted in the figure below.
+The temperature rises very steeply since the wall is relatively well insulated (<i>k=0.04 W/(m*K)</i>)
+and the heater is not disabled when it becomes too warm.
+</p>
+<p align=\"center\">
+<img alt=\"Air temperature as function of time.\"
+src=\"modelica://AixLib/Resources/Images/Examples/Tutorial/SimpleHouse/result4.png\" width=\"1000\"/>
+</p>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse4.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleHouse4;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse5.mo b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse5.mo
new file mode 100644
index 0000000000..908a856dcf
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse5.mo
@@ -0,0 +1,87 @@
+within AixLib.Examples.Tutorial.SimpleHouse;
+model SimpleHouse5 "Heating controller model"
+  extends SimpleHouse4(final use_constantHeater=false);
+
+  Modelica.Blocks.Math.BooleanToReal booRea1(realTrue=mWat_flow_nominal)
+    "Boolean to integer"
+    annotation (Placement(transformation(extent={{0,-160},{20,-140}})));
+  Modelica.Blocks.Math.BooleanToReal booRea "Boolean to real"
+    annotation (Placement(transformation(extent={{0,-120},{20,-100}})));
+  Modelica.Blocks.Logical.Hysteresis hysRad(uLow=273.15 + 21, uHigh=273.15 + 23)
+    "Hysteresis controller for radiator"
+    annotation (Placement(transformation(extent={{-80,-120},{-60,-100}})));
+  Modelica.Blocks.Logical.Not not1
+    "Negation for enabling heating when temperature is low"
+    annotation (Placement(transformation(extent={{-40,-120},{-20,-100}})));
+  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor senTemZonAir
+    "Zone air temperature sensor"
+    annotation (Placement(transformation(extent={{90,160},{70,180}})));
+equation
+  connect(booRea1.u, not1.y) annotation (Line(points={{-2,-150},{-11.5,-150},{-11.5,
+          -110},{-19,-110}}, color={255,0,255}));
+  connect(not1.u,hysRad. y) annotation (Line(points={{-42,-110},{-59,-110}},
+                  color={255,0,255}));
+  connect(senTemZonAir.T,hysRad. u) annotation (Line(points={{69,170},{-210,170},
+          {-210,-110},{-82,-110}},            color={0,0,127}));
+  connect(senTemZonAir.port, zon.heatPort)
+    annotation (Line(points={{90,170},{160,170},{160,40}},  color={191,0,0}));
+  connect(not1.y, booRea.u)
+    annotation (Line(points={{-19,-110},{-2,-110}}, color={255,0,255}));
+  connect(booRea.y, heaWat.u) annotation (Line(points={{21,-110},{40,-110},{40,-124},
+          {58,-124}}, color={0,0,127}));
+  connect(booRea1.y, pum.m_flow_in) annotation (Line(points={{21,-150},{100,-150},
+          {100,-168}}, color={0,0,127}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-220,
+            -220},{220,220}})),
+    experiment(Tolerance=1e-6, StopTime=1e+06),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 4, 2023, by Jelger Jansen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Since the zone becomes too warm, a controller is required that disables the heater when a setpoint is reached.
+We will implement a hysteresis controller with a setpoint of <i>295.15 +/- 1K</i> (<i>21-23°C</i>).
+A temperature sensor will measure the zone air temperature.
+</p>
+<h4>Required models</h4>
+<ul>
+<li>
+<a href=\"modelica://Modelica.Blocks.Logical.Hysteresis\">
+Modelica.Blocks.Logical.Hysteresis</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Blocks.Logical.Not\">
+Modelica.Blocks.Logical.Not</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Blocks.Math.BooleanToReal\">
+Modelica.Blocks.Math.BooleanToReal</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor\">
+Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor</a>
+</li>
+</ul>
+<h4>Connection instructions</h4>
+<p>
+The heater modulation level should be set to <i>1</i> when the heater is on and to <i>0</i> otherwise.
+Furthermore, the pump should only circulate water when the heater is on.
+</p>
+<h4>Reference result</h4>
+<p>
+The figure below shows the air temperature after the controller is added.
+</p>
+<p align=\"center\">
+<img alt=\"Air temperature as function of time.\"
+src=\"modelica://AixLib/Resources/Images/Examples/Tutorial/SimpleHouse/result5.png\" width=\"1000\"/>
+</p>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse5.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleHouse5;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse6.mo b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse6.mo
new file mode 100644
index 0000000000..fa5500fbac
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/SimpleHouse6.mo
@@ -0,0 +1,162 @@
+within AixLib.Examples.Tutorial.SimpleHouse;
+model SimpleHouse6 "Free cooling model"
+  extends SimpleHouse5(
+    zon(nPorts=2),
+    mAir_flow_nominal=0.1,
+    AWin=6);
+
+  parameter Modelica.Units.SI.PressureDifference dpAir_nominal=200
+    "Pressure drop at nominal mass flow rate for air loop";
+
+  AixLib.Fluid.Actuators.Dampers.Exponential vavDam(
+    redeclare package Medium = MediumAir,
+    from_dp=true,
+    m_flow_nominal=mAir_flow_nominal,
+    dpDamper_nominal=dpAir_nominal)
+    "Damper" annotation (Placement(transformation(extent={{-10,10},{10,
+            -10}}, origin={110,130})));
+  Fluid.Movers.Preconfigured.FlowControlled_dp fan(
+    redeclare package Medium = MediumAir,
+    show_T=true,
+    dp_nominal=dpAir_nominal,
+    use_inputFilter=false,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    m_flow_nominal=mAir_flow_nominal)
+    "Constant head fan" annotation (Placement(transformation(
+        extent={{-10,10},{10,-10}},
+        origin={0,130})));
+
+  AixLib.Fluid.HeatExchangers.ConstantEffectiveness hexRec(
+    redeclare package Medium1 = MediumAir,
+    redeclare package Medium2 = MediumAir,
+    dp1_nominal=10,
+    dp2_nominal=10,
+    m1_flow_nominal=mAir_flow_nominal,
+    m2_flow_nominal=mAir_flow_nominal,
+    eps=0.85) "Heat exchanger for heat recuperation"
+    annotation (Placement(transformation(extent={{-55,124},{-85,156}})));
+  AixLib.Fluid.Sources.Boundary_pT bouAir(
+    redeclare package Medium = MediumAir,
+    use_T_in=true,
+    nPorts=2) "Air boundary with constant temperature"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-110,140})));
+  Modelica.Blocks.Logical.Hysteresis hysAir(uLow=273.15 + 23, uHigh=273.15 + 25)
+    "Hysteresis controller for damper"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={50,110})));
+  Modelica.Blocks.Math.BooleanToReal booRea2 "Boolean to real"
+    annotation (Placement(transformation(extent={{80,80},{100,100}})));
+  Modelica.Blocks.Math.BooleanToReal booRea3(realTrue=dpAir_nominal)
+    "Boolean to real"
+    annotation (Placement(transformation(extent={{30,80},{10,100}})));
+equation
+  connect(hexRec.port_a1, zon.ports[1]) annotation (Line(points={{-55,149.6},{169,
+          149.6},{169,50},{170,50}},     color={0,127,255}));
+  connect(bouAir.T_in, weaBus.TDryBul) annotation (Line(points={{-122,144},{-130,
+          144},{-130,0}},       color={0,0,127}));
+  connect(vavDam.port_b, zon.ports[2]) annotation (Line(points={{120,130},{142,130},
+          {142,50},{170,50}},
+                           color={0,127,255}));
+  connect(booRea2.y, vavDam.y)
+    annotation (Line(points={{101,90},{110,90},{110,118}}, color={0,0,127}));
+  connect(hysAir.y, booRea2.u)
+    annotation (Line(points={{50,99},{50,90},{78,90}}, color={255,0,255}));
+  connect(vavDam.port_a, fan.port_b)
+    annotation (Line(points={{100,130},{10,130}}, color={0,127,255}));
+  connect(bouAir.ports[1], hexRec.port_a2) annotation (Line(points={{-100,139},{
+          -100,130.4},{-85,130.4}},   color={0,127,255}));
+  connect(fan.port_a, hexRec.port_b2) annotation (Line(points={{-10,130},{-32,130},
+          {-32,130.4},{-55,130.4}}, color={0,127,255}));
+  connect(hexRec.port_b1, bouAir.ports[2]) annotation (Line(points={{-85,149.6},
+          {-100,149.6},{-100,141}}, color={0,127,255}));
+  connect(booRea1.y, pum.m_flow_in) annotation (Line(points={{21,-150},{100,
+          -150},{100,-168}}, color={0,0,127}));
+  connect(hysAir.u, hysRad.u) annotation (Line(points={{50,122},{50,170},{-210,
+          170},{-210,-110},{-82,-110}}, color={0,0,127}));
+  connect(booRea3.y, fan.dp_in)
+    annotation (Line(points={{9,90},{0,90},{0,118}}, color={0,0,127}));
+  connect(booRea3.u, hysAir.y)
+    annotation (Line(points={{32,90},{50,90},{50,99}}, color={255,0,255}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-220,
+            -220},{220,220}})),
+    experiment(Tolerance=1e-6, StopTime=1e+06),
+    Documentation(revisions="<html>
+<ul>
+<li>
+September 4, 2023, by Jelger Jansen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+For this last exercise, we first increase the <b>window size</b>
+from <i>2 m<sup>2</sup></i> <b>to <i>6 m<sup>2</sup></i></b>.
+</p>
+<p>
+We will add a ventilation model that allows to perform free cooling
+using outside air when solar irradiation heats up the room too much.
+The system consists of a fan, a damper, a controller with an air temperature setpoint
+between <i>23°C</i> and <i>25°C</i>,
+and a heat recovery unit with a constant effectiveness of <i>85%</i>.
+The damper and fan have a nominal pressure drop/raise of <i>200 Pa</i>.
+The heat recovery unit has a nominal pressure drop of <i>10 Pa</i> at both sides.
+The nominal mass flow rate of the ventilation system is <i>0.1 kg/s</i>.
+</p>
+<h4>Required models</h4>
+<ul>
+<li>
+<a href=\"modelica://AixLib.Fluid.Actuators.Dampers.Exponential\">
+AixLib.Fluid.Actuators.Dampers.Exponential</a>
+</li>
+<li>
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ConstantEffectiveness\">
+AixLib.Fluid.HeatExchangers.ConstantEffectiveness</a>
+</li>
+<li>
+<a href=\"modelica://AixLib.Fluid.Movers.Preconfigured.FlowControlled_dp\">
+AixLib.Fluid.Movers.Preconfigured.FlowControlled_dp</a>
+</li>
+<li>
+<a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Blocks.Logical.Hysteresis\">
+Modelica.Blocks.Logical.Hysteresis</a>
+</li>
+<li>
+<a href=\"modelica://Modelica.Blocks.Math.BooleanToReal\">
+Modelica.Blocks.Math.BooleanToReal</a>
+</li>
+</ul>
+<h4>Connection instructions</h4>
+<p>
+Connect the components such that they exchange mass (and therefore also energy)
+with the <code>MixingVolume</code> representing the zone air.
+Add a <code>boundary_pT</code> to draw air from the environment.
+Enable its temperature input and connect it to the <code>TDryBul</code> variable in the weather data reader.
+Also reconsider the nominal mass flow rate parameter value in the <code>MixingVolume</code>
+given the flow rate information of the ventilation system.
+Finally, make sure that the fan is only active when the damper is open.
+</p>
+<h4>Reference result</h4>
+<p>
+The figures below show the results.
+</p>
+<p align=\"center\">
+<img alt=\"Air temperature as function of time.\"
+src=\"modelica://AixLib/Resources/Images/Examples/Tutorial/SimpleHouse/result6.png\" width=\"1000\"/>
+</p>
+<p align=\"center\">
+<img alt=\"Ventilation control signal as function of time.\"
+src=\"modelica://AixLib/Resources/Images/Examples/Tutorial/SimpleHouse/result7.png\" width=\"1000\"/>
+</p>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse6.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleHouse6;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/package.mo b/AixLib/Examples/Tutorial/SimpleHouse/package.mo
new file mode 100644
index 0000000000..73a6c3a197
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/package.mo
@@ -0,0 +1,88 @@
+within AixLib.Examples.Tutorial;
+package SimpleHouse "Package with example for how to build a simple building envelope with a radiator heating system and ventilation system"
+extends Modelica.Icons.ExamplesPackage;
+
+  annotation (Documentation(info="<html>
+<p>
+This package contains examples with step-by-step instructions for how to build a system model
+for a simple house with a heating system, ventilation, and weather boundary conditions.
+It serves as a demonstration case of how the <code>AixLib</code> library can be used.
+</p>
+<p>
+The goal of this exercise is to become familiar with Modelica and the AixLib library.
+Since the AixLib library components are typically used by combining several components graphically,
+the use of equations falls outside of the scope of this exercise.
+</p>
+<p>
+For this exercise you will create a model of a simple house,
+consisting of a heating system, one building zone, and a ventilation model.
+The exercise starts from a template file that should not produce any errors.
+This file will be extended in several steps, adding complexity.
+In between each step the user should be able to simulate the model,
+i.e., no errors should be produced and simulation results may be compared.
+</p>
+<p>
+The model has been created in the following stages:
+</p>
+<ol>
+<li>
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse0\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse0</a>
+contains a weather data reader which connects the data of the dry bulb temperature
+to a <code>PrescribedTemperature</code> component
+and serves as a starting model to implement the entire <code>SimpleHouse</code> model.
+</li>
+<li>
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse1\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse1</a>
+implements the building wall by adding a thermal capacity.
+</li>
+<li>
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse2\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse2</a>
+adds a window to the building wall.
+It is assumed that the total injected heat through the window equals the window surface area
+multiplied by the direct horizontal solar irradiance.
+</li>
+<li>
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse3\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse3</a>
+adds an air model which represents the room in the building.
+</li>
+<li>
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse4\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse4</a>
+adds heating circuit consisting of a boiler, a radiator, 
+and an on/off circulation pump with a constant mass flow rate.
+No controller is implemented yet, i.e. the pump and heater are always on.
+</li>
+<li>
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse5\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse5</a>
+adds a hysteresis controller for the heating circuit that uses the room temperature as an input.
+</li>
+<li>
+<a href=\"modelica://AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse6\">
+AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse6</a>
+adds a ventilation system consisting of a fan, a damper, a heat recovery unit,
+and a hysteresis controller, that allows to perform free cooling using outside air.
+</li>
+</ol>
+<p>
+For each stage, firstly the model part is qualitatively explained.
+Next, the names of the required Modelica models (from the Modelica Standard Library and/or AixLib library) are listed.
+Finally, we provide high-level instructions of how to set up the model.
+If these instructions are not clear immediately, have a look at the model documentation and at the type of connectors the model has,
+try out some things, make an educated guess, etc.
+Finally, we provide reference results that allow you to check if your implementation is correct.
+Depending on the parameter values that you choose, results may differ.
+</p>
+<p>
+The graphical representation of the final model is given below.
+</p>
+<p align=\"center\">
+<img alt=\"Graphical representation of the final simple house model.\"
+src=\"modelica://AixLib/Resources/Images/Examples/Tutorial/SimpleHouse/simpleHouse.png\"/>
+</p>
+</html>"));
+end SimpleHouse;
diff --git a/AixLib/Examples/Tutorial/SimpleHouse/package.order b/AixLib/Examples/Tutorial/SimpleHouse/package.order
new file mode 100644
index 0000000000..e975e02c46
--- /dev/null
+++ b/AixLib/Examples/Tutorial/SimpleHouse/package.order
@@ -0,0 +1,7 @@
+SimpleHouse0
+SimpleHouse1
+SimpleHouse2
+SimpleHouse3
+SimpleHouse4
+SimpleHouse5
+SimpleHouse6
diff --git a/AixLib/Examples/Tutorial/package.mo b/AixLib/Examples/Tutorial/package.mo
new file mode 100644
index 0000000000..d2937e2a21
--- /dev/null
+++ b/AixLib/Examples/Tutorial/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Examples;
+package Tutorial "Tutorial with step by step instructions for how to build system models"
+  extends Modelica.Icons.Information;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains examples of system models with step by step
+instructions for how to build such models.
+The examples are meant to instruct new users on how to build
+large system models.
+</p>
+</html>"));
+end Tutorial;
diff --git a/AixLib/Examples/Tutorial/package.order b/AixLib/Examples/Tutorial/package.order
new file mode 100644
index 0000000000..6e0ff92568
--- /dev/null
+++ b/AixLib/Examples/Tutorial/package.order
@@ -0,0 +1 @@
+SimpleHouse
diff --git a/AixLib/Examples/package.mo b/AixLib/Examples/package.mo
new file mode 100644
index 0000000000..9be3d3d03d
--- /dev/null
+++ b/AixLib/Examples/package.mo
@@ -0,0 +1,22 @@
+within AixLib;
+package Examples "Collection of models that illustrate model use and test models"
+  extends Modelica.Icons.ExamplesPackage;
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains examples and tutorials with step-by-step instructions
+for how to build system models.
+</p>
+<p>
+The examples illustrate
+the scope of the library. Smaller examples that typically only
+use models from a few packages can be found in the individual packages.
+For example, see
+<a href=\"modelica://Buildings.Airflow.Multizone.Examples\">
+Buildings.Airflow.Multizone.Examples</a> for examples of
+multizone airflow and contaminant transport models, or
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples\">
+AixLib.Fluid.HeatExchangers.Examples</a> for
+examples of heat exchanger models.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Examples/package.order b/AixLib/Examples/package.order
new file mode 100644
index 0000000000..cea794e60c
--- /dev/null
+++ b/AixLib/Examples/package.order
@@ -0,0 +1,2 @@
+Tutorial
+SimpleHouse
diff --git a/AixLib/Fluid/Actuators/BaseClasses/ActuatorSignal.mo b/AixLib/Fluid/Actuators/BaseClasses/ActuatorSignal.mo
index 429679d5a1..5766efb102 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/ActuatorSignal.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/ActuatorSignal.mo
@@ -103,69 +103,69 @@ equation
           textColor={0,0,0},
           textString=DynamicSelect("", String(y, format=".2f")))}),
 Documentation(info="<html>
- <p>
- This model implements the filter that is used to approximate the travel
- time of the actuator.
- Models that extend this model use the signal
- <code>y_actual</code> to obtain the
- current position of the actuator.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>
- for a description of the filter.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- April 6, 2020, by Antoine Gautier:<br/>
- Add the boolean parameter <code>casePreInd</code>.<br/>
- This is needed for the computation of the damper opening in
- <a href=\"modelica://AixLib.Fluid.Actuators.Dampers.PressureIndependent\">
- AixLib.Fluid.Actuators.Dampers.PressureIndependent</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- November 14, 2019, by Michael Wetter:<br/>
- Set <code>start</code> attribute for <code>filter.x</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1252\">#1252</a>.
- </li>
- <li>
- October 25, 2019, by Jianjun Hu:<br/>
- Improved icon graphics annotation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
- </li>
- <li>
- February 16, 2018, by Filip Jorissen:<br/>
- Propagated parameter <code>order</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/891\">#891</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- February 14, 2012 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model implements the filter that is used to approximate the travel
+time of the actuator.
+Models that extend this model use the signal
+<code>y_actual</code> to obtain the
+current position of the actuator.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>
+for a description of the filter.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+April 6, 2020, by Antoine Gautier:<br/>
+Add the boolean parameter <code>casePreInd</code>.<br/>
+This is needed for the computation of the damper opening in
+<a href=\"modelica://AixLib.Fluid.Actuators.Dampers.PressureIndependent\">
+AixLib.Fluid.Actuators.Dampers.PressureIndependent</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+November 14, 2019, by Michael Wetter:<br/>
+Set <code>start</code> attribute for <code>filter.x</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1252\">#1252</a>.
+</li>
+<li>
+October 25, 2019, by Jianjun Hu:<br/>
+Improved icon graphics annotation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
+</li>
+<li>
+February 16, 2018, by Filip Jorissen:<br/>
+Propagated parameter <code>order</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/891\">#891</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+February 14, 2012 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ActuatorSignal;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/Examples/EqualPercentageDerivativeCheck.mo b/AixLib/Fluid/Actuators/BaseClasses/Examples/EqualPercentageDerivativeCheck.mo
index 88f94f869a..6b2818cdd9 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/Examples/EqualPercentageDerivativeCheck.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/Examples/EqualPercentageDerivativeCheck.mo
@@ -17,18 +17,18 @@ equation
  annotation(experiment(Tolerance=1e-6, StartTime=0, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/BaseClasses/Examples/EqualPercentageDerivativeCheck.mos" "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EqualPercentageDerivativeCheck;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/PartialDamperExponential.mo b/AixLib/Fluid/Actuators/BaseClasses/PartialDamperExponential.mo
index 2e10d2959e..cc44828079 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/PartialDamperExponential.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/PartialDamperExponential.mo
@@ -121,164 +121,164 @@ equation
     yU=yU);
   k = if dpFixed_nominal > Modelica.Constants.eps then sqrt(1/(1/kFixed^2 + 1/kDam^2)) else kDam;
 annotation(Documentation(info="<html>
- <p>
- Partial model for air dampers with exponential opening characteristics.
- This is the base model for air dampers.
- The model implements the functions that relate the opening signal and the
- flow coefficient.
- The model also defines parameters that are used by different air damper
- models.
- </p>
- <p>
- The model is as in ASHRAE 825-RP except that a control signal of
- <code>y=0</code> means the damper is closed, and <code>y=1</code> means
- the damper is open.
- This is opposite of the implementation of ASHRAE 825-RP, but used here
- for consistency within this library.
- </p>
- <p>
- For <code>yL &lt; y &lt; yU</code>, the damper characteristics is:
- </p>
- <p style=\"font-style:italic;\">
-   k<sub>d</sub>(y) = exp(a+b (1-y))
- </p>
- <p>
- where <i>kd</i> is the loss coefficient (total pressure drop divided
- by dynamic pressure) and <i>y</i> is the fractional opening.
- </p>
- <p>
- Outside this range, the damper characteristics is defined by a quadratic polynomial that
- matches the damper resistance at <code>y=0</code> and <code>y=yL</code> or
- <code>y=yU</code> and <code>y=1</code>, respectively.
- In addition, the polynomials are such that <i>k<sub>d</sub>(y)</i> is differentiable in
- <i>y</i> and the derivative is continuous.
- </p>
- <p>
- The damper characteristics is then used to compute the flow coefficient <i>k(y)</i> as:
- </p>
- <p style=\"font-style:italic;\">
- k(y) = (2 &rho; &frasl; k<sub>d</sub>(y))<sup>1/2</sup> A
- </p>
- <p>
- where <i>A</i> is the face area, which is computed using the nominal
- mass flow rate <code>m_flow_nominal</code>, the nominal velocity
- <code>v_nominal</code> and the density of the medium.
- </p>
- <p>
- ASHRAE 825-RP lists the following parameter values as typical (note that the
- default values in the model correspond to opposed blades).
- <br/>
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\"
- style=\"border-collapse:collapse;\">
- <tr>
- <td></td><th>opposed blades</th><th>single blades</th>
- </tr>
- <tr>
- <td>yL</td><td>15/90</td><td>15/90</td>
- </tr>
- <tr>
- <td>yU</td><td>55/90</td><td>65/90</td>
- </tr>
- <tr>
- <td>k1</td><td>0.2 to 0.5</td><td>0.2 to 0.5</td>
- </tr>
- <tr>
- <td>a</td><td>-1.51</td><td>-1.51</td>
- </tr>
- <tr>
- <td>b</td><td>0.105*90</td><td>0.0842*90</td>
- </tr>
- </table>
- <p>
- (The loss coefficient in fully closed position <code>k0</code> is computed based on the leakage coefficient
- and the coefficient in fully open position.)
- </p>
- <h4>References</h4>
- <p>
- P. Haves, L. K. Norford, M. DeSimone and L. Mei,
- <i>A Standard Simulation Testbed for the Evaluation of Control Algorithms &amp; Strategies</i>,
- ASHRAE Final Report 825-RP, Atlanta, GA.
- </p>
- </html>",
+<p>
+Partial model for air dampers with exponential opening characteristics.
+This is the base model for air dampers.
+The model implements the functions that relate the opening signal and the
+flow coefficient.
+The model also defines parameters that are used by different air damper
+models.
+</p>
+<p>
+The model is as in ASHRAE 825-RP except that a control signal of
+<code>y=0</code> means the damper is closed, and <code>y=1</code> means
+the damper is open.
+This is opposite of the implementation of ASHRAE 825-RP, but used here
+for consistency within this library.
+</p>
+<p>
+For <code>yL &lt; y &lt; yU</code>, the damper characteristics is:
+</p>
+<p style=\"font-style:italic;\">
+  k<sub>d</sub>(y) = exp(a+b (1-y))
+</p>
+<p>
+where <i>kd</i> is the loss coefficient (total pressure drop divided
+by dynamic pressure) and <i>y</i> is the fractional opening.
+</p>
+<p>
+Outside this range, the damper characteristics is defined by a quadratic polynomial that
+matches the damper resistance at <code>y=0</code> and <code>y=yL</code> or
+<code>y=yU</code> and <code>y=1</code>, respectively.
+In addition, the polynomials are such that <i>k<sub>d</sub>(y)</i> is differentiable in
+<i>y</i> and the derivative is continuous.
+</p>
+<p>
+The damper characteristics is then used to compute the flow coefficient <i>k(y)</i> as:
+</p>
+<p style=\"font-style:italic;\">
+k(y) = (2 &rho; &frasl; k<sub>d</sub>(y))<sup>1/2</sup> A
+</p>
+<p>
+where <i>A</i> is the face area, which is computed using the nominal
+mass flow rate <code>m_flow_nominal</code>, the nominal velocity
+<code>v_nominal</code> and the density of the medium.
+</p>
+<p>
+ASHRAE 825-RP lists the following parameter values as typical (note that the
+default values in the model correspond to opposed blades).
+<br/>
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\"
+style=\"border-collapse:collapse;\">
+<tr>
+<td></td><th>opposed blades</th><th>single blades</th>
+</tr>
+<tr>
+<td>yL</td><td>15/90</td><td>15/90</td>
+</tr>
+<tr>
+<td>yU</td><td>55/90</td><td>65/90</td>
+</tr>
+<tr>
+<td>k1</td><td>0.2 to 0.5</td><td>0.2 to 0.5</td>
+</tr>
+<tr>
+<td>a</td><td>-1.51</td><td>-1.51</td>
+</tr>
+<tr>
+<td>b</td><td>0.105*90</td><td>0.0842*90</td>
+</tr>
+</table>
+<p>
+(The loss coefficient in fully closed position <code>k0</code> is computed based on the leakage coefficient
+and the coefficient in fully open position.)
+</p>
+<h4>References</h4>
+<p>
+P. Haves, L. K. Norford, M. DeSimone and L. Mei,
+<i>A Standard Simulation Testbed for the Evaluation of Control Algorithms &amp; Strategies</i>,
+ASHRAE Final Report 825-RP, Atlanta, GA.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 21, 2021, by Michael Wetter:<br/>
- Corrected typo in comments.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1525\">#1525</a>.
- </li>
- <li>
- December 23, 2019, by Antoine Gautier:<br/>
- Removed the equations involving <code>m_flow</code> and <code>dp</code> that now need
- to be added in each derived damper model.<br/>
- Added the declaration of <code>dpDamper_nominal</code> and <code>dpFixed_nominal</code>.<br/>
- Replaced <code>k0</code> by leakage coefficient.<br/>
- Modified the limiting values for <code>k0</code> and <code>k1</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1188\">#1188</a>.
- </li>
- <li>
- March 22, 2017, by Michael Wetter:<br/>
- Added back <code>v_nominal</code>, but set the assignment of <code>A</code>
- to be final. This allows scaling the model with <code>m_flow_nominal</code>,
- which is generally known in the flow leg,
- and <code>v_nominal</code>, for which a default value can be specified.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/544\">#544</a>.
- </li>
- <li>
- October 12, 2016 by David Blum:<br/>
- Removed parameter <code>v_nominal</code> and variable <code>area</code>,
- to simplify parameterization of the model.
- Also added assertion statements upon initialization
- for parameters <code>k0</code> and <code>k1</code> so that they fall within
- suggested ranges found in ASHRAE 825-RP. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/544\">#544</a>.
- </li>
- <li>
- January 27, 2015 by Michael Wetter:<br/>
- Set <code>Evaluate=true</code> for <code>use_constant_density</code>.
- This is a structural parameter. Adding this annotation leads to fewer
- numerical Jacobians for
- <code>Buildings.Examples.VAVReheat.ClosedLoop</code>
- with
- <code>Buildings.Media.PerfectGases.MoistAirUnsaturated</code>.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>
- January 16, 2012 by Michael Wetter:<br/>
- To simplify object inheritance tree, revised base classes
- <code>AixLib.Fluid.BaseClasses.PartialResistance</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialActuator</code>
- and model
- <code>AixLib.Fluid.FixedResistances.PressureDrop</code>.
- </li>
- <li>
- August 5, 2011, by Michael Wetter:<br/>
- Moved linearized pressure drop equation from the function body to the equation
- section. With the previous implementation,
- the symbolic processor may not rearrange the equations, which can lead
- to coupled equations instead of an explicit solution.
- </li>
- <li>
- June 22, 2008 by Michael Wetter:<br/>
- Extended range of control signal from 0 to 1 by implementing the function
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.exponentialDamper\">
- exponentialDamper</a>.
- </li>
- <li>
- June 10, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+September 21, 2021, by Michael Wetter:<br/>
+Corrected typo in comments.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1525\">#1525</a>.
+</li>
+<li>
+December 23, 2019, by Antoine Gautier:<br/>
+Removed the equations involving <code>m_flow</code> and <code>dp</code> that now need
+to be added in each derived damper model.<br/>
+Added the declaration of <code>dpDamper_nominal</code> and <code>dpFixed_nominal</code>.<br/>
+Replaced <code>k0</code> by leakage coefficient.<br/>
+Modified the limiting values for <code>k0</code> and <code>k1</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1188\">#1188</a>.
+</li>
+<li>
+March 22, 2017, by Michael Wetter:<br/>
+Added back <code>v_nominal</code>, but set the assignment of <code>A</code>
+to be final. This allows scaling the model with <code>m_flow_nominal</code>,
+which is generally known in the flow leg,
+and <code>v_nominal</code>, for which a default value can be specified.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/544\">#544</a>.
+</li>
+<li>
+October 12, 2016 by David Blum:<br/>
+Removed parameter <code>v_nominal</code> and variable <code>area</code>,
+to simplify parameterization of the model.
+Also added assertion statements upon initialization
+for parameters <code>k0</code> and <code>k1</code> so that they fall within
+suggested ranges found in ASHRAE 825-RP. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/544\">#544</a>.
+</li>
+<li>
+January 27, 2015 by Michael Wetter:<br/>
+Set <code>Evaluate=true</code> for <code>use_constant_density</code>.
+This is a structural parameter. Adding this annotation leads to fewer
+numerical Jacobians for
+<code>Buildings.Examples.VAVReheat.ClosedLoop</code>
+with
+<code>Buildings.Media.PerfectGases.MoistAirUnsaturated</code>.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>
+January 16, 2012 by Michael Wetter:<br/>
+To simplify object inheritance tree, revised base classes
+<code>AixLib.Fluid.BaseClasses.PartialResistance</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialActuator</code>
+and model
+<code>AixLib.Fluid.FixedResistances.PressureDrop</code>.
+</li>
+<li>
+August 5, 2011, by Michael Wetter:<br/>
+Moved linearized pressure drop equation from the function body to the equation
+section. With the previous implementation,
+the symbolic processor may not rearrange the equations, which can lead
+to coupled equations instead of an explicit solution.
+</li>
+<li>
+June 22, 2008 by Michael Wetter:<br/>
+Extended range of control signal from 0 to 1 by implementing the function
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.exponentialDamper\">
+exponentialDamper</a>.
+</li>
+<li>
+June 10, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
    Icon(graphics={Line(
          points={{0,100},{0,-24}}),
         Rectangle(
@@ -290,6 +290,6 @@ revisions="<html>
           extent={{-100,22},{100,-24}},
           lineColor={0,0,0},
           fillPattern=FillPattern.HorizontalCylinder,
-          fillColor={0,127,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={0,127,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialDamperExponential;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/PartialThreeWayValve.mo b/AixLib/Fluid/Actuators/BaseClasses/PartialThreeWayValve.mo
index d7f108618b..e091c33de5 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/PartialThreeWayValve.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/PartialThreeWayValve.mo
@@ -7,7 +7,6 @@ partial model PartialThreeWayValve "Partial three way valve"
       AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve res1
         constrainedby AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve(
           deltaM=deltaM,
-          dp(start=dpValve_nominal/2),
           from_dp=from_dp,
           final linearized=linearized[1],
           final homotopyInitialization=homotopyInitialization,
@@ -15,14 +14,14 @@ partial model PartialThreeWayValve "Partial three way valve"
           final m_flow_nominal=m_flow_nominal,
           final dpValve_nominal=dpValve_nominal,
           final dpFixed_nominal=dpFixed_nominal[1],
-          final use_inputFilter=false),
+          final use_inputFilter=false,
+          final riseTime=riseTime),
       redeclare FixedResistances.LosslessPipe res2(
         m_flow_nominal=m_flow_nominal),
       redeclare replaceable
       AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve res3
         constrainedby AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve(
           deltaM=deltaM,
-          dp(start=dpValve_nominal/2),
           from_dp=from_dp,
           final linearized=linearized[2],
           final homotopyInitialization=homotopyInitialization,
@@ -30,7 +29,8 @@ partial model PartialThreeWayValve "Partial three way valve"
           final m_flow_nominal=m_flow_nominal,
           final dpValve_nominal=dpValve_nominal/fraK^2,
           final dpFixed_nominal=dpFixed_nominal[2],
-          final use_inputFilter=false));
+          final use_inputFilter=false,
+          final riseTime=riseTime));
     extends AixLib.Fluid.Actuators.BaseClasses.ActuatorSignal;
     extends AixLib.Fluid.Actuators.BaseClasses.ValveParameters(
       rhoStd=Medium.density_pTX(101325, 273.15+4, Medium.X_default));
@@ -123,111 +123,123 @@ equation
       visible=not use_inputFilter,
       points={{0,100},{0,40}})}),
     Documentation(info="<html>
- <p>
- Partial model of a three way valve. This is the base model for valves
- with different opening characteristics, such as linear, equal percentage
- or quick opening. The three way valve model consists of a mixer where
- valves are placed in two of the flow legs. The third flow leg
- has no friction.
- The flow coefficient <code>Kv</code> for flow from <code>port_1 &rarr; port_2</code> is
- a parameter.
- The flow coefficient for the bypass flow from <code>port_3 &rarr; port_2</code>
- is computed as
- </p>
- <pre>
-          Kv(port_3 &rarr; port_2)
-   fraK = ----------------------
-          Kv(port_1 &rarr; port_2)
- </pre>
- <p>
- where <code>0 &lt; fraK &le; 1</code> is a parameter with a default value
- of <code>fraK=0.7</code>.
- </p>
- <p>
- Since this model uses two way valves to construct a three way valve, see
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>
- for details regarding the valve implementation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- November 5, 2019, by Michael Wetter:<br/>
- Moved assignment of leakage from <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
- to the parent classes.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1227\">#1227</a>.
- </li>
- <li>
- October 25, 2019, by Jianjun Hu:<br/>
- Improved icon graphics annotation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- December 17, 2015, by Michael Wetter:<br/>
- Removed assignment <code>redeclare final package Medium=Medium</code>
- as this is now done in the base class.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/475\">
- https://github.com/lbl-srg/modelica-buildings/issues/475</a>.
- </li>
- <li>
- November 23, 2015 by Filip Jorissen:<br/>
- Corrected valve leakage value to avoid warnings.
- </li>
- <li>
- February 28, 2013, by Michael Wetter:<br/>
- Reformulated assignment of parameters.
- Removed default value for <code>dpValve_nominal</code>, as this
- parameter has the attribute <code>fixed=false</code> for some values
- of <code>CvData</code>. In this case, assigning a value is not allowed.
- Corrected wrong documentation of parameter <code>fraK(min=0, max=1) = 0.7</code>.
- The documenation was
- <i>Fraction Kv(port_1&rarr;port_2)/Kv(port_3&rarr;port_2)</i> instead of
- <i>Fraction Kv(port_3&rarr;port_2)/Kv(port_1&rarr;port_2)</i>.
- Because the parameter set correctly its attributes <code>min=0</code> and <code>max=1</code>,
- instances of this model used the correct value.
- </li>
- <li>
- April 12, 2012 by Michael Wetter:<br/>
- Removed duplicate declaration of <code>m_flow_nominal</code>.
- </li>
- <li>
- February 20, 2012 by Michael Wetter:<br/>
- Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
- and added new parameter <code>dpFixed_nominal=0</code>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>.
- </li>
- <li>
- March 25, 2011, by Michael Wetter:<br/>
- Added homotopy method.
- </li>
- <li>
- June 3, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model of a three way valve. This is the base model for valves
+with different opening characteristics, such as linear, equal percentage
+or quick opening. The three way valve model consists of a mixer where
+valves are placed in two of the flow legs. The third flow leg
+has no friction.
+The flow coefficient <code>Kv</code> for flow from <code>port_1 &rarr; port_2</code> is
+a parameter.
+The flow coefficient for the bypass flow from <code>port_3 &rarr; port_2</code>
+is computed as
+</p>
+<pre>
+         Kv(port_3 &rarr; port_2)
+  fraK = ----------------------
+         Kv(port_1 &rarr; port_2)
+</pre>
+<p>
+where <code>0 &lt; fraK &le; 1</code> is a parameter with a default value
+of <code>fraK=0.7</code>.
+</p>
+<p>
+Since this model uses two way valves to construct a three way valve, see
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>
+for details regarding the valve implementation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 3, 2023, by Michael Wetter:<br/>
+Removed start value for <code>dp</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3231\">Buildings, #3231</a>.
+</li>
+<li>
+November 16, 2022, by Michael Wetter:<br/>
+Propagated parameter <code>riseTime</code> to valves. The value is not used as the filter is disabled,
+but it will show in the result file. Having a consistent value for all these parameters in the result filter
+helps during debugging.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+November 5, 2019, by Michael Wetter:<br/>
+Moved assignment of leakage from <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
+to the parent classes.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1227\">#1227</a>.
+</li>
+<li>
+October 25, 2019, by Jianjun Hu:<br/>
+Improved icon graphics annotation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+December 17, 2015, by Michael Wetter:<br/>
+Removed assignment <code>redeclare final package Medium=Medium</code>
+as this is now done in the base class.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/475\">
+https://github.com/lbl-srg/modelica-buildings/issues/475</a>.
+</li>
+<li>
+November 23, 2015 by Filip Jorissen:<br/>
+Corrected valve leakage value to avoid warnings.
+</li>
+<li>
+February 28, 2013, by Michael Wetter:<br/>
+Reformulated assignment of parameters.
+Removed default value for <code>dpValve_nominal</code>, as this
+parameter has the attribute <code>fixed=false</code> for some values
+of <code>CvData</code>. In this case, assigning a value is not allowed.
+Corrected wrong documentation of parameter <code>fraK(min=0, max=1) = 0.7</code>.
+The documenation was
+<i>Fraction Kv(port_1&rarr;port_2)/Kv(port_3&rarr;port_2)</i> instead of
+<i>Fraction Kv(port_3&rarr;port_2)/Kv(port_1&rarr;port_2)</i>.
+Because the parameter set correctly its attributes <code>min=0</code> and <code>max=1</code>,
+instances of this model used the correct value.
+</li>
+<li>
+April 12, 2012 by Michael Wetter:<br/>
+Removed duplicate declaration of <code>m_flow_nominal</code>.
+</li>
+<li>
+February 20, 2012 by Michael Wetter:<br/>
+Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
+and added new parameter <code>dpFixed_nominal=0</code>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>.
+</li>
+<li>
+March 25, 2011, by Michael Wetter:<br/>
+Added homotopy method.
+</li>
+<li>
+June 3, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialThreeWayValve;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValve.mo b/AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValve.mo
index e89a8dafd0..1b8769a022 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValve.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValve.mo
@@ -55,197 +55,197 @@ initial equation
       visible=not use_inputFilter,
       points={{0,100},{0,40}})}),
 Documentation(info="<html>
- <p>
- Partial model for a two way valve. This is the base model for valves
- with different opening characteristics, such as linear, equal percentage,
- quick opening or pressure-independent.
- </p>
- <p>
- To prevent the derivative <code>d/dP (m_flow)</code> to be infinite near
- the origin, this model linearizes the pressure drop versus flow relation
- ship. The region in which it is linearized is parameterized by
- </p>
- <pre>
-   m_turbulent_flow = deltaM * m_flow_nominal
- </pre>
- <p>
- Because the parameterization contains <code>Kv_SI</code>, the values for
- <code>deltaM</code> and <code>dp_nominal</code> need not be changed if the valve size
- changes.
- </p>
- <p>
- In contrast to the model in <a href=\"modelica://Modelica.Fluid\">
- Modelica.Fluid</a>, this model uses the parameter <code>Kv_SI</code>,
- which is the flow coefficient in SI units, i.e.,
- it is the ratio between mass flow rate in <code>kg/s</code> and square root
- of pressure drop in <code>Pa</code>.
- </p>
- <h4>Options</h4>
- <p>
- This model allows different parameterization of the flow resistance.
- The different parameterizations are described in
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.ValveParameters\">
- AixLib.Fluid.Actuators.BaseClasses.ValveParameters</a>.
- </p>
- <h4>Implementation</h4>
- <p>
- The two way valve models are implemented using this partial model, as opposed to using
- different functions for the valve opening characteristics, because
- each valve opening characteristics has different parameters.
- </p>
- </html>",
+<p>
+Partial model for a two way valve. This is the base model for valves
+with different opening characteristics, such as linear, equal percentage,
+quick opening or pressure-independent.
+</p>
+<p>
+To prevent the derivative <code>d/dP (m_flow)</code> to be infinite near
+the origin, this model linearizes the pressure drop versus flow relation
+ship. The region in which it is linearized is parameterized by
+</p>
+<pre>
+  m_turbulent_flow = deltaM * m_flow_nominal
+</pre>
+<p>
+Because the parameterization contains <code>Kv_SI</code>, the values for
+<code>deltaM</code> and <code>dp_nominal</code> need not be changed if the valve size
+changes.
+</p>
+<p>
+In contrast to the model in <a href=\"modelica://Modelica.Fluid\">
+Modelica.Fluid</a>, this model uses the parameter <code>Kv_SI</code>,
+which is the flow coefficient in SI units, i.e.,
+it is the ratio between mass flow rate in <code>kg/s</code> and square root
+of pressure drop in <code>Pa</code>.
+</p>
+<h4>Options</h4>
+<p>
+This model allows different parameterization of the flow resistance.
+The different parameterizations are described in
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.ValveParameters\">
+AixLib.Fluid.Actuators.BaseClasses.ValveParameters</a>.
+</p>
+<h4>Implementation</h4>
+<p>
+The two way valve models are implemented using this partial model, as opposed to using
+different functions for the valve opening characteristics, because
+each valve opening characteristics has different parameters.
+</p>
+</html>",
 revisions="<html>
- <ul>
- 
- <li>
- April 2, 2020, by Filip Jorissen:<br/>
- Added model name in assert message.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1334\">#1334</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating stage.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- November 9, 2019, by Filip Jorissen:<br/>
- Removed assert for <code>phi>-0.2</code>
- since the valve control input is now lower limited
- to zero.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
- issue 1223</a>.
- </li>
- <li>
- October 25, 2019, by Jianjun Hu:<br/>
- Improved icon graphics annotation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- November 16, 2017, by Michael Wetter:<br/>
- Relaxed assertion on <code>phi</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/592\">#592</a>.
- </li>
- <li>
- October 27, 2016, by Filip Jorissen:<br/>
- Added assert for <code>phi &gt; 0</code>.
- This fixes a bug that caused valves to behave
- like pumps for negative control signals.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/558\">#558</a>.
- </li>
- <li>
- April 23, 2016, by Michael Wetter:<br/>
- Changed test in assertion from <code>dpFixed_nominal > -Modelica.Constants.small</code>
- to
- <code>dpFixed_nominal > -Modelica.Constants.eps</code>.
- Otherwise, JModelica evaluates it as <code>true</code> in
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.Examples.TwoWayValves\">
- AixLib.Fluid.Actuators.Valves.Examples.TwoWayValves</a>.
- See also
- <a href=\"https://trac.jmodelica.org/ticket/4932\">https://trac.jmodelica.org/ticket/4932</a>.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- January 29, 2015, by Filip Jorissen:<br/>
- Moved the governing equations to
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValveKv\">
- PartialTwoWayValveKv</a>
- in order to be able to extend from this partial in
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayPressureIndependent\">
- TwoWayPressureIndependent</a>
- </li>
- <li>
- August 8, 2014, by Michael Wetter:<br/>
- Reformulated the computation of <code>k</code> to make the model
- work in OpenModelica.
- </li>
- <li>
- April 4, 2014, by Michael Wetter:<br/>
- Added keyword <code>input</code> to variable <code>phi</code>
- to require models that extend this model to provide a binding equation.
- This is done to use the same modeling concept as is used for example in
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
- AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>.
- </li>
- <li>
- March 27, 2014 by Michael Wetter:<br/>
- Revised model for implementation of new valve model that computes the flow function
- based on a table.
- </li>
- <li>
- March 20, 2013, by Michael Wetter:<br/>
- Set <code>dp(nominal=6000)</code> as the previous formulation gives an error during model check
- in Dymola 2014. The reason is that the previous formulation used <code>dpValve_nominal</code>, which
- is not known at translation time.
- </li>
- <li>
- February 28, 2013, by Michael Wetter:<br/>
- Reformulated assignment of parameters.
- Removed default value for <code>dpValve_nominal</code>, as this
- parameter has the attribute <code>fixed=false</code> for some values
- of <code>CvData</code>. In this case, assigning a value is not allowed.
- Changed assignment of nominal attribute of <code>dp</code> to avoid assigning
- a non-literal value.
- </li>
- <li>
- February 20, 2012 by Michael Wetter:<br/>
- Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
- and added new parameter <code>dpFixed_nominal</code>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>.
- </li>
- <li>
- January 16, 2012 by Michael Wetter:<br/>
- To simplify object inheritance tree, revised base classes
- <code>AixLib.Fluid.BaseClasses.PartialResistance</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialActuator</code>
- and model
- <code>AixLib.Fluid.FixedResistances.PressureDrop</code>.
- </li>
- <li>
- August 12, 2011 by Michael Wetter:<br/>
- Added <code>assert</code> statement to prevent <code>l=0</code> due to the
- implementation of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>.
- </li>
- <li>
- April 4, 2011 by Michael Wetter:<br/>
- Revised implementation to use new base class for actuators.
- </li>
- <li>
- February 18, 2009 by Michael Wetter:<br/>
- Implemented parameterization of flow coefficient as in
- <code>Modelica.Fluid</code>.
- </li>
- <li>
- August 15, 2008 by Michael Wetter:<br/>
- Set valve leakage to nonzero value.
- </li>
- <li>
- June 3, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+
+<li>
+April 2, 2020, by Filip Jorissen:<br/>
+Added model name in assert message.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1334\">#1334</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating stage.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+November 9, 2019, by Filip Jorissen:<br/>
+Removed assert for <code>phi>-0.2</code>
+since the valve control input is now lower limited
+to zero.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
+issue 1223</a>.
+</li>
+<li>
+October 25, 2019, by Jianjun Hu:<br/>
+Improved icon graphics annotation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+November 16, 2017, by Michael Wetter:<br/>
+Relaxed assertion on <code>phi</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/592\">#592</a>.
+</li>
+<li>
+October 27, 2016, by Filip Jorissen:<br/>
+Added assert for <code>phi &gt; 0</code>.
+This fixes a bug that caused valves to behave
+like pumps for negative control signals.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/558\">#558</a>.
+</li>
+<li>
+April 23, 2016, by Michael Wetter:<br/>
+Changed test in assertion from <code>dpFixed_nominal > -Modelica.Constants.small</code>
+to
+<code>dpFixed_nominal > -Modelica.Constants.eps</code>.
+Otherwise, JModelica evaluates it as <code>true</code> in
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.Examples.TwoWayValves\">
+AixLib.Fluid.Actuators.Valves.Examples.TwoWayValves</a>.
+See also
+<a href=\"https://trac.jmodelica.org/ticket/4932\">https://trac.jmodelica.org/ticket/4932</a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+January 29, 2015, by Filip Jorissen:<br/>
+Moved the governing equations to
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValveKv\">
+PartialTwoWayValveKv</a>
+in order to be able to extend from this partial in
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayPressureIndependent\">
+TwoWayPressureIndependent</a>
+</li>
+<li>
+August 8, 2014, by Michael Wetter:<br/>
+Reformulated the computation of <code>k</code> to make the model
+work in OpenModelica.
+</li>
+<li>
+April 4, 2014, by Michael Wetter:<br/>
+Added keyword <code>input</code> to variable <code>phi</code>
+to require models that extend this model to provide a binding equation.
+This is done to use the same modeling concept as is used for example in
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
+AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>.
+</li>
+<li>
+March 27, 2014 by Michael Wetter:<br/>
+Revised model for implementation of new valve model that computes the flow function
+based on a table.
+</li>
+<li>
+March 20, 2013, by Michael Wetter:<br/>
+Set <code>dp(nominal=6000)</code> as the previous formulation gives an error during model check
+in Dymola 2014. The reason is that the previous formulation used <code>dpValve_nominal</code>, which
+is not known at translation time.
+</li>
+<li>
+February 28, 2013, by Michael Wetter:<br/>
+Reformulated assignment of parameters.
+Removed default value for <code>dpValve_nominal</code>, as this
+parameter has the attribute <code>fixed=false</code> for some values
+of <code>CvData</code>. In this case, assigning a value is not allowed.
+Changed assignment of nominal attribute of <code>dp</code> to avoid assigning
+a non-literal value.
+</li>
+<li>
+February 20, 2012 by Michael Wetter:<br/>
+Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
+and added new parameter <code>dpFixed_nominal</code>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>.
+</li>
+<li>
+January 16, 2012 by Michael Wetter:<br/>
+To simplify object inheritance tree, revised base classes
+<code>AixLib.Fluid.BaseClasses.PartialResistance</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialActuator</code>
+and model
+<code>AixLib.Fluid.FixedResistances.PressureDrop</code>.
+</li>
+<li>
+August 12, 2011 by Michael Wetter:<br/>
+Added <code>assert</code> statement to prevent <code>l=0</code> due to the
+implementation of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>.
+</li>
+<li>
+April 4, 2011 by Michael Wetter:<br/>
+Revised implementation to use new base class for actuators.
+</li>
+<li>
+February 18, 2009 by Michael Wetter:<br/>
+Implemented parameterization of flow coefficient as in
+<code>Modelica.Fluid</code>.
+</li>
+<li>
+August 15, 2008 by Michael Wetter:<br/>
+Set valve leakage to nonzero value.
+</li>
+<li>
+June 3, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialTwoWayValve;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValveKv.mo b/AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValveKv.mo
index 4cd0973818..1121208042 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValveKv.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/PartialTwoWayValveKv.mo
@@ -38,40 +38,40 @@ equation
  end if; // linearized
   annotation (
 Documentation(info="<html>
- <p>
- Partial model for valves with different opening characteristics,
- such as linear, equal percentage or quick opening. This partial extends from
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>
- and also contains the governing equations for these three two way valve models.
- </p>
- <h4>Implementation</h4>
- <p>
- Models that extend this model need to provide a binding equation
- for the flow function <code>phi</code>.
- An example of such a code can be found in
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayLinear\">
- AixLib.Fluid.Actuators.Valves.TwoWayLinear</a>.
- </p>
- </html>",
+<p>
+Partial model for valves with different opening characteristics,
+such as linear, equal percentage or quick opening. This partial extends from
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>
+and also contains the governing equations for these three two way valve models.
+</p>
+<h4>Implementation</h4>
+<p>
+Models that extend this model need to provide a binding equation
+for the flow function <code>phi</code>.
+An example of such a code can be found in
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayLinear\">
+AixLib.Fluid.Actuators.Valves.TwoWayLinear</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 25, 2019, by Jianjun Hu:<br/>
- Removed icon graphics annotation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- January 29, 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 25, 2019, by Jianjun Hu:<br/>
+Removed icon graphics annotation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+January 29, 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialTwoWayValveKv;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/ValveParameters.mo b/AixLib/Fluid/Actuators/BaseClasses/ValveParameters.mo
index 2ee3fc59fa..a3d9570b97 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/ValveParameters.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/ValveParameters.mo
@@ -61,7 +61,7 @@ initial equation
     dpValve_nominal =  (m_flow_nominal/Kv_SI)^2;
   else
     assert(CvData == AixLib.Fluid.Types.CvTypes.Av, "Invalid value for CvData.
- Obtained CvData = "+ String(CvData) + ".");
+Obtained CvData = " + String(CvData) + ".");
     Kv_SI =           Av*sqrt(rhoStd);
     Kv    =           Kv_SI/(rhoStd/3600/sqrt(1E5));
     Cv    =           Kv_SI/(rhoStd*0.0631/1000/sqrt(6895));
@@ -69,89 +69,89 @@ initial equation
   end if;
 
   annotation (Documentation(info="<html>
- <p>
- Model that computes the flow coefficients of valves. This base class allows the following modeling options,
- which have been adapted from the valve implementation
- in <a href=\"modelica://Modelica.Fluid\">
- Modelica.Fluid</a>
- to specify the valve flow coefficient in fully open conditions:
- </p>
- <ul>
- <li><code>CvData = AixLib.Fluid.Types.CvTypes.Av</code>: the flow coefficient is given by the metric <code>Av</code> coefficient (m^2).</li>
- <li><code>CvData = AixLib.Fluid.Types.CvTypes.Kv</code>: the flow coefficient is given by the metric <code>Kv</code> coefficient (m^3/h).</li>
- <li><code>CvData = AixLib.Fluid.Types.CvTypes.Cv</code>: the flow coefficient is given by the US <code>Cv</code> coefficient (USG/min).</li>
- <li><code>CvData = AixLib.Fluid.Types.CvTypes.OpPoint</code>: the flow is computed from the nominal operating point specified by <code>dp_nominal</code> and <code>m_flow_nominal</code>.</li>
- </ul>
- <p>
- The treatment of parameters <code>Kv</code> and <code>Cv</code> is
- explained in detail in the
- <a href=\"modelica://Modelica.Fluid.UsersGuide.ComponentDefinition.ValveCharacteristics\">Users Guide</a>.
- </p>
- <p>
- In contrast to the model in <a href=\"modelica://Modelica.Fluid\">
- Modelica.Fluid</a>, this model uses the protected parameter <code>Kv_SI</code>,
- which is the flow coefficient in SI units, i.e.,
- it is the ratio between mass flow rate in <code>kg/s</code> and square root
- of pressure drop in <code>Pa</code>.
- The value of <code>Kv_SI</code> is computed based on the parameters
- <code>Av</code>,
- <code>Kv</code>,
- <code>Cv</code>, or, if
- <code>CvData = AixLib.Fluid.Types.CvTypes.OpPoint</code>, based on
- <code>m_flow_nominal</code> and <code>dpValve_nominal</code>.
- Conversely, if
- <code>CvData &lt;&gt; AixLib.Fluid.Types.CvTypes.OpPoint</code>, then
- <code>dpValve_nominal</code> is computed based on
- <code>Av</code>,
- <code>Kv</code>, or
- <code>Cv</code>, and the nominal mass flow rate <code>m_flow_nominal</code>.
- Therefore, if
- <code>CvData &lt;&gt; AixLib.Fluid.Types.CvTypes.OpPoint</code>,
- then specifying a value for <code>dpValve_nominal</code> is a syntax error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- August 12, 2014, by Michael Wetter:<br/>
- Changed attribute <code>min</code> of <code>dpValve_nominal</code>
- to <code>0</code>.
- This is needed as for example in
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable\">
- AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable</a>,
- <code>dpValve_nominal=0</code>.
- </li>
- <li>
- August 8, 2014, by Michael Wetter:<br/>
- Changed the <code>initial algorithm</code> to an <code>initial equation</code>
- section. Otherwise, OpenModelica attempts to solve for the parameter
- values using numerical iteration, and fails in doing so.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- March 25, 2013, by Michael Wetter:<br/>
- Removed stray backslash in write statement.
- </li>
- <li>
- February 28, 2013, by Michael Wetter:<br/>
- Reformulated assignment of parameters, and removed <code>Kv_SI</code> as
- a public parameter because it is always computed based on other parameters.
- This change avoids a translation error in Dymola 2014 beta1 in
- the pedantic mode, and a translation warning otherwise.
- </li>
- <li>
- February 18, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that computes the flow coefficients of valves. This base class allows the following modeling options,
+which have been adapted from the valve implementation
+in <a href=\"modelica://Modelica.Fluid\">
+Modelica.Fluid</a>
+to specify the valve flow coefficient in fully open conditions:
+</p>
+<ul>
+<li><code>CvData = AixLib.Fluid.Types.CvTypes.Av</code>: the flow coefficient is given by the metric <code>Av</code> coefficient (m^2).</li>
+<li><code>CvData = AixLib.Fluid.Types.CvTypes.Kv</code>: the flow coefficient is given by the metric <code>Kv</code> coefficient (m^3/h).</li>
+<li><code>CvData = AixLib.Fluid.Types.CvTypes.Cv</code>: the flow coefficient is given by the US <code>Cv</code> coefficient (USG/min).</li>
+<li><code>CvData = AixLib.Fluid.Types.CvTypes.OpPoint</code>: the flow is computed from the nominal operating point specified by <code>dp_nominal</code> and <code>m_flow_nominal</code>.</li>
+</ul>
+<p>
+The treatment of parameters <code>Kv</code> and <code>Cv</code> is
+explained in detail in the
+<a href=\"modelica://Modelica.Fluid.UsersGuide.ComponentDefinition.ValveCharacteristics\">Users Guide</a>.
+</p>
+<p>
+In contrast to the model in <a href=\"modelica://Modelica.Fluid\">
+Modelica.Fluid</a>, this model uses the protected parameter <code>Kv_SI</code>,
+which is the flow coefficient in SI units, i.e.,
+it is the ratio between mass flow rate in <code>kg/s</code> and square root
+of pressure drop in <code>Pa</code>.
+The value of <code>Kv_SI</code> is computed based on the parameters
+<code>Av</code>,
+<code>Kv</code>,
+<code>Cv</code>, or, if
+<code>CvData = AixLib.Fluid.Types.CvTypes.OpPoint</code>, based on
+<code>m_flow_nominal</code> and <code>dpValve_nominal</code>.
+Conversely, if
+<code>CvData &lt;&gt; AixLib.Fluid.Types.CvTypes.OpPoint</code>, then
+<code>dpValve_nominal</code> is computed based on
+<code>Av</code>,
+<code>Kv</code>, or
+<code>Cv</code>, and the nominal mass flow rate <code>m_flow_nominal</code>.
+Therefore, if
+<code>CvData &lt;&gt; AixLib.Fluid.Types.CvTypes.OpPoint</code>,
+then specifying a value for <code>dpValve_nominal</code> is a syntax error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+August 12, 2014, by Michael Wetter:<br/>
+Changed attribute <code>min</code> of <code>dpValve_nominal</code>
+to <code>0</code>.
+This is needed as for example in
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable\">
+AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable</a>,
+<code>dpValve_nominal=0</code>.
+</li>
+<li>
+August 8, 2014, by Michael Wetter:<br/>
+Changed the <code>initial algorithm</code> to an <code>initial equation</code>
+section. Otherwise, OpenModelica attempts to solve for the parameter
+values using numerical iteration, and fails in doing so.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+March 25, 2013, by Michael Wetter:<br/>
+Removed stray backslash in write statement.
+</li>
+<li>
+February 28, 2013, by Michael Wetter:<br/>
+Reformulated assignment of parameters, and removed <code>Kv_SI</code> as
+a public parameter because it is always computed based on other parameters.
+This change avoids a translation error in Dymola 2014 beta1 in
+the pedantic mode, and a translation warning otherwise.
+</li>
+<li>
+February 18, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ValveParameters;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/der_equalPercentage.mo b/AixLib/Fluid/Actuators/BaseClasses/der_equalPercentage.mo
index af7085f180..14c34a8d3b 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/der_equalPercentage.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/der_equalPercentage.mo
@@ -37,30 +37,30 @@ algorithm
   end if;
 annotation (
 Documentation(info="<html>
- <p>
- This function computes the derivative of the opening characteristics of an equal percentage valve.
- </p><p>
- The function is the derivative of
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.equalPercentage\">
- AixLib.Fluid.Actuators.BaseClasses.equalPercentage</a>.
- </p>
- </html>",
+<p>
+This function computes the derivative of the opening characteristics of an equal percentage valve.
+</p><p>
+The function is the derivative of
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.equalPercentage\">
+AixLib.Fluid.Actuators.BaseClasses.equalPercentage</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 30, 2011 by Michael Wetter:<br/>
- Removed inputs for which no derivative is implemented from the argument list, and added
- <code>zeroDerivative</code> keyword in function that calls this function.
- </li>
- <li>
- February 4, 2010 by Michael Wetter:<br/>
- Fixed implementation of derivative function.
- </li>
- <li>
- June 6, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 30, 2011 by Michael Wetter:<br/>
+Removed inputs for which no derivative is implemented from the argument list, and added
+<code>zeroDerivative</code> keyword in function that calls this function.
+</li>
+<li>
+February 4, 2010 by Michael Wetter:<br/>
+Fixed implementation of derivative function.
+</li>
+<li>
+June 6, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_equalPercentage;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/equalPercentage.mo b/AixLib/Fluid/Actuators/BaseClasses/equalPercentage.mo
index afeabc60a1..f144626b15 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/equalPercentage.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/equalPercentage.mo
@@ -37,36 +37,36 @@ algorithm
   end if;
 annotation (
 Documentation(info="<html>
- <p>
- This function computes the opening characteristics of an equal percentage valve.
- </p><p>
- The function is used by the model
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayEqualPercentage\">
- AixLib.Fluid.Actuators.Valves.TwoWayEqualPercentage</a>.
- </p><p>
- For <code>y &lt; delta/2</code>, the valve characteristics is linear. For <code> y &gt; 3*delta/2</code>
- the valve characteristics is equal percentage. In between, a cubic spline is used to ensure
- that the valve characteristics is once continuously differentiable with respect to <code>y</code>.
- </p>
- </html>",
+<p>
+This function computes the opening characteristics of an equal percentage valve.
+</p><p>
+The function is used by the model
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayEqualPercentage\">
+AixLib.Fluid.Actuators.Valves.TwoWayEqualPercentage</a>.
+</p><p>
+For <code>y &lt; delta/2</code>, the valve characteristics is linear. For <code> y &gt; 3*delta/2</code>
+the valve characteristics is equal percentage. In between, a cubic spline is used to ensure
+that the valve characteristics is once continuously differentiable with respect to <code>y</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- March 30, 2011 by Michael Wetter:<br/>
- Added <code>zeroDerivative</code> keyword.
- </li>
- <li>
- June 5, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+March 30, 2011 by Michael Wetter:<br/>
+Added <code>zeroDerivative</code> keyword.
+</li>
+<li>
+June 5, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 smoothOrder=1,
-derivative(zeroDerivative=R, zeroDerivative=l, zeroDerivative=delta)=der_equalPercentage,
-  __Dymola_LockedEditing="Model from IBPSA");
+derivative(zeroDerivative=R, zeroDerivative=l, zeroDerivative=delta)=der_equalPercentage, 
+   __Dymola_LockedEditing="Model from IBPSA");
 end equalPercentage;
diff --git a/AixLib/Fluid/Actuators/BaseClasses/exponentialDamper.mo b/AixLib/Fluid/Actuators/BaseClasses/exponentialDamper.mo
index f857735445..c26ede92c1 100644
--- a/AixLib/Fluid/Actuators/BaseClasses/exponentialDamper.mo
+++ b/AixLib/Fluid/Actuators/BaseClasses/exponentialDamper.mo
@@ -29,52 +29,52 @@ algorithm
   end if;
 annotation (
 Documentation(info="<html>
- <p>
- This function computes the opening characteristics of an exponential damper.
- </p><p>
- The function is used by the model
- <a href=\"modelica://AixLib.Fluid.Actuators.Dampers.Exponential\">
- AixLib.Fluid.Actuators.Dampers.Exponential</a>.
- </p><p>
- For <code>yL &lt; y &lt; yU</code>, the damper characteristics is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   k<sub>d</sub>(y) = exp(a+b (1-y)).
- </p>
- <p>
- Outside this range, the damper characteristic is defined by a quadratic polynomial.
- </p>
- <p>
- Note that this implementation returns <i>sqrt(k<sub>d</sub>(y))</i> instead of <i>k<sub>d</sub>(y)</i>.
- This is done for numerical reason since otherwise <i>k<sub>d</sub>(y)</i> may be an iteration
- variable, which may cause a lot of warnings and slower convergence if the solver
- attempts <i>k<sub>d</sub>(y) &lt; 0</i> during the iterative solution procedure.
- </p>
- </html>",
+<p>
+This function computes the opening characteristics of an exponential damper.
+</p><p>
+The function is used by the model
+<a href=\"modelica://AixLib.Fluid.Actuators.Dampers.Exponential\">
+AixLib.Fluid.Actuators.Dampers.Exponential</a>.
+</p><p>
+For <code>yL &lt; y &lt; yU</code>, the damper characteristics is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  k<sub>d</sub>(y) = exp(a+b (1-y)).
+</p>
+<p>
+Outside this range, the damper characteristic is defined by a quadratic polynomial.
+</p>
+<p>
+Note that this implementation returns <i>sqrt(k<sub>d</sub>(y))</i> instead of <i>k<sub>d</sub>(y)</i>.
+This is done for numerical reason since otherwise <i>k<sub>d</sub>(y)</i> may be an iteration
+variable, which may cause a lot of warnings and slower convergence if the solver
+attempts <i>k<sub>d</sub>(y) &lt; 0</i> during the iterative solution procedure.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2014 by Michael Wetter:<br/>
- Improved documentation.
- </li>
- <li>
- July 1, 2011 by Michael Wetter:<br/>
- Added constraint to control input to avoid using a number outside
- <code>0</code> and <code>1</code> in case that the control input
- has a numerical integration error.
- </li>
- <li>
- April 4, 2010 by Michael Wetter:<br/>
- Reformulated implementation. The new implementation computes
- <code>sqrt(kTheta)</code>. This avoid having <code>kTheta</code> in
- the iteration variables, which caused warnings when the solver attempted
- <code>kTheta &lt; 0</code>.
- </li>
- <li>
- June 22, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),  smoothOrder=1,
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 14, 2014 by Michael Wetter:<br/>
+Improved documentation.
+</li>
+<li>
+July 1, 2011 by Michael Wetter:<br/>
+Added constraint to control input to avoid using a number outside
+<code>0</code> and <code>1</code> in case that the control input
+has a numerical integration error.
+</li>
+<li>
+April 4, 2010 by Michael Wetter:<br/>
+Reformulated implementation. The new implementation computes
+<code>sqrt(kTheta)</code>. This avoid having <code>kTheta</code> in
+the iteration variables, which caused warnings when the solver attempted
+<code>kTheta &lt; 0</code>.
+</li>
+<li>
+June 22, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),   smoothOrder=1, 
+   __Dymola_LockedEditing="Model from IBPSA");
 end exponentialDamper;
diff --git a/AixLib/Fluid/Actuators/Dampers/Examples/Damper.mo b/AixLib/Fluid/Actuators/Dampers/Examples/Damper.mo
index ac91902523..63ec13938a 100644
--- a/AixLib/Fluid/Actuators/Dampers/Examples/Damper.mo
+++ b/AixLib/Fluid/Actuators/Dampers/Examples/Damper.mo
@@ -92,22 +92,22 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Dampers/Examples/Damper.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- Test model for exponential and linear air dampers.
- The air dampers are connected to models for constant inlet and outlet
- pressures. The control signal of the dampers is a ramp.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 21, 2017 by David Blum:<br/>
- Added Linear damper models <code>lin</code>, <code>preIndFrom_dp</code>, and <code>preInd</code>.
- </li>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for exponential and linear air dampers.
+The air dampers are connected to models for constant inlet and outlet
+pressures. The control signal of the dampers is a ramp.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2017 by David Blum:<br/>
+Added Linear damper models <code>lin</code>, <code>preIndFrom_dp</code>, and <code>preInd</code>.
+</li>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Damper;
diff --git a/AixLib/Fluid/Actuators/Dampers/Examples/MixingBox.mo b/AixLib/Fluid/Actuators/Dampers/Examples/MixingBox.mo
index c07a8cc117..e82812380c 100644
--- a/AixLib/Fluid/Actuators/Dampers/Examples/MixingBox.mo
+++ b/AixLib/Fluid/Actuators/Dampers/Examples/MixingBox.mo
@@ -81,18 +81,18 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=240),
 Documentation(info="<html>
- <p>
- Test model for the economizer mixing box.
- The economizer mixing box is exposed to time varying pressure boundary
- conditions and input signals.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 23, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for the economizer mixing box.
+The economizer mixing box is exposed to time varying pressure boundary
+conditions and input signals.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 23, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingBox;
diff --git a/AixLib/Fluid/Actuators/Dampers/Examples/VAVBoxExponential.mo b/AixLib/Fluid/Actuators/Dampers/Examples/VAVBoxExponential.mo
index 789330a99a..6d1dba8bc8 100644
--- a/AixLib/Fluid/Actuators/Dampers/Examples/VAVBoxExponential.mo
+++ b/AixLib/Fluid/Actuators/Dampers/Examples/VAVBoxExponential.mo
@@ -74,25 +74,25 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=240),
 Documentation(info="<html>
- <p>
- Test model for the variable air volume flow box.
- The model has two flow legs, both are connected to models for constant inlet and outlet
- pressures.
- The top flow leg has a flow resistance and an air damper, and
- the bottom flow leg combines both of these resistances into one model.
- Both flow legs have identical mass flow rates, except at very small
- flow rates. The reason for this difference is that the equations
- are regularized for numerical reasons, and combining the two components
- within one component leads to a slightly different equation for the
- regularization.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for the variable air volume flow box.
+The model has two flow legs, both are connected to models for constant inlet and outlet
+pressures.
+The top flow leg has a flow resistance and an air damper, and
+the bottom flow leg combines both of these resistances into one model.
+Both flow legs have identical mass flow rates, except at very small
+flow rates. The reason for this difference is that the equations
+are regularized for numerical reasons, and combining the two components
+within one component leads to a slightly different equation for the
+regularization.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VAVBoxExponential;
diff --git a/AixLib/Fluid/Actuators/Dampers/Exponential.mo b/AixLib/Fluid/Actuators/Dampers/Exponential.mo
index 9c72bef5ea..da355edf32 100644
--- a/AixLib/Fluid/Actuators/Dampers/Exponential.mo
+++ b/AixLib/Fluid/Actuators/Dampers/Exponential.mo
@@ -34,100 +34,100 @@ equation
 annotation (
 defaultComponentName="damExp",
 Documentation(info="<html>
- <p>
- Model of two flow resistances in series:
- </p>
- <ul>
- <li>
- one resistance has a fixed flow coefficient;
- </li>
- <li>
- the other resistance represents a damper whose flow coefficient is an
- exponential function of the opening angle.
- </li>
- </ul>
- <p>
- The lumped flow coefficient <i>k(y)</i> (function of the fractional opening
- <i>y</i>) is used to compute the mass flow rate versus pressure drop relation as:
- </p>
- <p style=\"font-style:italic;\">
-   m&#775; = sign(&Delta;p) k(y)  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
- </p>
- <p>
- with regularization near the origin.
- <p>
- For a description of the damper opening characteristics and typical
- parameter values, see the partial model
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential\">
- AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- April 12, 2021, by Michael Wetter:<br/>
- Guarded against division by zero if the pressure equation is removed.
- This then leads to a more meaningful error message.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1243\">IBPSA, #1243</a>.
- </li>
- <li>
- December 23, 2019, by Antoine Gautier:<br/>
- Added the pressure drop calculation as it is no longer in the base class.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1188\">IBPSA, #1188</a>.
- </li>
- <li>
- March 22, 2017, by Michael Wetter:<br/>
- Updated documentation.
- </li>
- <li>
- April 14, 2014 by Michael Wetter:<br/>
- Improved documentation.
- </li>
- <li>
- September 26, 2013 by Michael Wetter:<br/>
- Moved assignment of <code>kDam_default</code> and <code>kThetaSqRt_default</code>
- from <code>initial algorithm</code> to the variable declaration, to avoid a division
- by zero in OpenModelica.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>
- June 22, 2008 by Michael Wetter:<br/>
- Extended range of control signal from 0 to 1 by implementing the function
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.exponentialDamper\">
- AixLib.Fluid.Actuators.BaseClasses.exponentialDamper</a>.
- </li>
- <li>
- June 10, 2008 by Michael Wetter:<br/>
- Introduced new partial base class,
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential\">
- PartialDamperExponential</a>.
- </li>
- <li>
- June 30, 2007 by Michael Wetter:<br/>
- Introduced new partial base class,
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialActuator\">PartialActuator</a>.
- </li>
- <li>
- July 27, 2007 by Michael Wetter:<br/>
- Introduced partial base class.
- </li>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},
+<p>
+Model of two flow resistances in series:
+</p>
+<ul>
+<li>
+one resistance has a fixed flow coefficient;
+</li>
+<li>
+the other resistance represents a damper whose flow coefficient is an
+exponential function of the opening angle.
+</li>
+</ul>
+<p>
+The lumped flow coefficient <i>k(y)</i> (function of the fractional opening
+<i>y</i>) is used to compute the mass flow rate versus pressure drop relation as:
+</p>
+<p style=\"font-style:italic;\">
+  m&#775; = sign(&Delta;p) k(y)  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
+</p>
+<p>
+with regularization near the origin.
+<p>
+For a description of the damper opening characteristics and typical
+parameter values, see the partial model
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential\">
+AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+April 12, 2021, by Michael Wetter:<br/>
+Guarded against division by zero if the pressure equation is removed.
+This then leads to a more meaningful error message.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1243\">IBPSA, #1243</a>.
+</li>
+<li>
+December 23, 2019, by Antoine Gautier:<br/>
+Added the pressure drop calculation as it is no longer in the base class.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1188\">IBPSA, #1188</a>.
+</li>
+<li>
+March 22, 2017, by Michael Wetter:<br/>
+Updated documentation.
+</li>
+<li>
+April 14, 2014 by Michael Wetter:<br/>
+Improved documentation.
+</li>
+<li>
+September 26, 2013 by Michael Wetter:<br/>
+Moved assignment of <code>kDam_default</code> and <code>kThetaSqRt_default</code>
+from <code>initial algorithm</code> to the variable declaration, to avoid a division
+by zero in OpenModelica.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>
+June 22, 2008 by Michael Wetter:<br/>
+Extended range of control signal from 0 to 1 by implementing the function
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.exponentialDamper\">
+AixLib.Fluid.Actuators.BaseClasses.exponentialDamper</a>.
+</li>
+<li>
+June 10, 2008 by Michael Wetter:<br/>
+Introduced new partial base class,
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential\">
+PartialDamperExponential</a>.
+</li>
+<li>
+June 30, 2007 by Michael Wetter:<br/>
+Introduced new partial base class,
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialActuator\">PartialActuator</a>.
+</li>
+<li>
+July 27, 2007 by Michael Wetter:<br/>
+Introduced partial base class.
+</li>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},
             {100,100}}), graphics={
         Rectangle(
           extent={{-100,22},{100,-24}},
@@ -139,6 +139,6 @@ Documentation(info="<html>
           fillPattern=FillPattern.Solid), Polygon(
           points={{-22,-32},{26,10},{26,-2},{-22,-44},{-22,-32}},
           lineColor={0,0,0},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Exponential;
diff --git a/AixLib/Fluid/Actuators/Dampers/MixingBox.mo b/AixLib/Fluid/Actuators/Dampers/MixingBox.mo
index 985e4e5d82..b7b2982361 100644
--- a/AixLib/Fluid/Actuators/Dampers/MixingBox.mo
+++ b/AixLib/Fluid/Actuators/Dampers/MixingBox.mo
@@ -296,82 +296,82 @@ equation
                "%name")}),
 defaultComponentName="eco",
 Documentation(revisions="<html>
- <ul>
- <li>
- September 21, 2021, by Michael Wetter:<br/>
- Corrected typo in comments.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1525\">#1525</a>.
- </li>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- December 23, 2019, by Antoine Gautier:<br/>
- Updated parameter bindings consistently with refactoring of
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential\">
- AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</a>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1188\">#1188</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- March 22, 2017, by Michael Wetter:<br/>
- Removed the assignments of <code>AOut</code>, <code>AExh</code> and <code>ARec</code> as these are done in the damper instance using
- a final assignment of the parameter.
- This allows scaling the model with <code>m_flow_nominal</code>,
- which is generally known in the flow leg,
- and <code>v_nominal</code>, for which a default value can be specified.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/544\">#544</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>
- February 14, 2012 by Michael Wetter:<br/>
- Added filter to approximate the travel time of the actuator.
- </li>
- <li>
- February 3, 2012, by Michael Wetter:<br/>
- Removed assignment of <code>m_flow_small</code> as it is no
- longer used in its base class.
- </li>
- <li>
- February 23, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Model of an outside air mixing box with exponential dampers.
- Set <code>y=0</code> to close the outside air and exhaust air dampers.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.Dampers.Exponential\">
- AixLib.Fluid.Actuators.Dampers.Exponential</a>
- for the description of the exponential damper model.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 21, 2021, by Michael Wetter:<br/>
+Corrected typo in comments.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1525\">#1525</a>.
+</li>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+December 23, 2019, by Antoine Gautier:<br/>
+Updated parameter bindings consistently with refactoring of
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential\">
+AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1188\">#1188</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+March 22, 2017, by Michael Wetter:<br/>
+Removed the assignments of <code>AOut</code>, <code>AExh</code> and <code>ARec</code> as these are done in the damper instance using
+a final assignment of the parameter.
+This allows scaling the model with <code>m_flow_nominal</code>,
+which is generally known in the flow leg,
+and <code>v_nominal</code>, for which a default value can be specified.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/544\">#544</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>
+February 14, 2012 by Michael Wetter:<br/>
+Added filter to approximate the travel time of the actuator.
+</li>
+<li>
+February 3, 2012, by Michael Wetter:<br/>
+Removed assignment of <code>m_flow_small</code> as it is no
+longer used in its base class.
+</li>
+<li>
+February 23, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Model of an outside air mixing box with exponential dampers.
+Set <code>y=0</code> to close the outside air and exhaust air dampers.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.Dampers.Exponential\">
+AixLib.Fluid.Actuators.Dampers.Exponential</a>
+for the description of the exponential damper model.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingBox;
diff --git a/AixLib/Fluid/Actuators/Dampers/PressureIndependent.mo b/AixLib/Fluid/Actuators/Dampers/PressureIndependent.mo
index a4456819d0..7bb819588c 100644
--- a/AixLib/Fluid/Actuators/Dampers/PressureIndependent.mo
+++ b/AixLib/Fluid/Actuators/Dampers/PressureIndependent.mo
@@ -274,94 +274,94 @@ equation
 annotation (
   defaultComponentName="damPreInd",
   Documentation(info="<html>
- <p>
- Model for an air damper whose airflow is proportional to the input signal, assuming
- that at <code>y = 1</code>, <code>m_flow = m_flow_nominal</code>. This is unless the pressure difference
- <code>dp</code> is too low,
- in which case a <code>kDam = m_flow_nominal/sqrt(dp_nominal)</code> characteristic is used.
- </p>
- <p>
- The model is similar to
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayPressureIndependent\">
- AixLib.Fluid.Actuators.Valves.TwoWayPressureIndependent</a>,
- except for adaptations for damper parameters.
- Please see that documentation for more information.
- </p>
- <h4>Computation of the damper opening</h4>
- <p>
- The fractional opening of the damper is computed by
- </p>
- <ul>
- <li>
- inverting the quadratic flow function to compute the flow coefficient
- from the flow rate and the pressure drop values (under the assumption
- of a turbulent flow regime);
- </li>
- <li>
- inverting the exponential characteristics to compute the fractional opening
- from the loss coefficient value (directly derived from the flow coefficient).
- </li>
- </ul>
- <p>
- The quadratic interpolation used outside the exponential domain in the function
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.exponentialDamper\">
- AixLib.Fluid.Actuators.BaseClasses.exponentialDamper</a>
- yields a local extremum.
- Therefore, the formal inversion of the function is not possible.
- A cubic spline is used instead to fit the inverse of the damper characteristics.
- The central domain of the characteritics having a monotonous exponential profile, its
- inverse can be properly approximated with three equidistant support points.
- However, the quadratic functions used outside of the exponential domain can have
- various profiles depending on the damper coefficients.
- Therefore, five linearly distributed support points are used on each side domain to
- ensure a good fit of the inverse.
- </p>
- <p>
- Note that below a threshold value of the input control signal (fixed at 0.02),
- the fractional opening is forced to zero and no more related to the actual
- flow coefficient of the damper.
- This avoids steep transients of the computed opening while transitioning from reverse flow.
- This is to be considered as a modeling workaround (avoiding the introduction of
- an additional state variable) to prevent control chattering during
- shut off operation where the pressure difference at the damper boundaries
- can vary between slightly positive and negative values due to outdoor pressure
- variations.
- </p>
- </html>",
+<p>
+Model for an air damper whose airflow is proportional to the input signal, assuming
+that at <code>y = 1</code>, <code>m_flow = m_flow_nominal</code>. This is unless the pressure difference
+<code>dp</code> is too low,
+in which case a <code>kDam = m_flow_nominal/sqrt(dp_nominal)</code> characteristic is used.
+</p>
+<p>
+The model is similar to
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayPressureIndependent\">
+AixLib.Fluid.Actuators.Valves.TwoWayPressureIndependent</a>,
+except for adaptations for damper parameters.
+Please see that documentation for more information.
+</p>
+<h4>Computation of the damper opening</h4>
+<p>
+The fractional opening of the damper is computed by
+</p>
+<ul>
+<li>
+inverting the quadratic flow function to compute the flow coefficient
+from the flow rate and the pressure drop values (under the assumption
+of a turbulent flow regime);
+</li>
+<li>
+inverting the exponential characteristics to compute the fractional opening
+from the loss coefficient value (directly derived from the flow coefficient).
+</li>
+</ul>
+<p>
+The quadratic interpolation used outside the exponential domain in the function
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.exponentialDamper\">
+AixLib.Fluid.Actuators.BaseClasses.exponentialDamper</a>
+yields a local extremum.
+Therefore, the formal inversion of the function is not possible.
+A cubic spline is used instead to fit the inverse of the damper characteristics.
+The central domain of the characteritics having a monotonous exponential profile, its
+inverse can be properly approximated with three equidistant support points.
+However, the quadratic functions used outside of the exponential domain can have
+various profiles depending on the damper coefficients.
+Therefore, five linearly distributed support points are used on each side domain to
+ensure a good fit of the inverse.
+</p>
+<p>
+Note that below a threshold value of the input control signal (fixed at 0.02),
+the fractional opening is forced to zero and no more related to the actual
+flow coefficient of the damper.
+This avoids steep transients of the computed opening while transitioning from reverse flow.
+This is to be considered as a modeling workaround (avoiding the introduction of
+an additional state variable) to prevent control chattering during
+shut off operation where the pressure difference at the damper boundaries
+can vary between slightly positive and negative values due to outdoor pressure
+variations.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 11, 2021, by Michael Wetter:<br/>
- Reformulated initial equation section to avoid warning in OPTIMICA about
- variable array index.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1513\">IBPSA #1513</a>.
- </li>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">IBPSA #1498</a>.
- </li>
- <li>
- April 6, 2020, by Antoine Gautier:<br/>
- Added the computation of the damper opening.
- </li>
- <li>
- December 23, 2019 by Antoine Gautier:<br/>
- Refactored as the model can now extend directly
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential\">
- AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</a>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1188\">IBPSA #1188</a>.
- </li>
- <li>
- March 21, 2017 by David Blum:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+August 11, 2021, by Michael Wetter:<br/>
+Reformulated initial equation section to avoid warning in OPTIMICA about
+variable array index.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1513\">IBPSA #1513</a>.
+</li>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">IBPSA #1498</a>.
+</li>
+<li>
+April 6, 2020, by Antoine Gautier:<br/>
+Added the computation of the damper opening.
+</li>
+<li>
+December 23, 2019 by Antoine Gautier:<br/>
+Refactored as the model can now extend directly
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential\">
+AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1188\">IBPSA #1188</a>.
+</li>
+<li>
+March 21, 2017 by David Blum:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
    Icon(graphics={Line(
          points={{0,100},{0,-24}}),
         Rectangle(
@@ -373,6 +373,6 @@ revisions="<html>
           extent={{-100,22},{100,-24}},
           lineColor={0,0,0},
           fillPattern=FillPattern.HorizontalCylinder,
-          fillColor={0,127,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={0,127,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureIndependent;
diff --git a/AixLib/Fluid/Actuators/Dampers/Validation/PressureIndependent.mo b/AixLib/Fluid/Actuators/Dampers/Validation/PressureIndependent.mo
index 795237427e..fcb54c2555 100644
--- a/AixLib/Fluid/Actuators/Dampers/Validation/PressureIndependent.mo
+++ b/AixLib/Fluid/Actuators/Dampers/Validation/PressureIndependent.mo
@@ -4,8 +4,8 @@ model PressureIndependent
   extends Modelica.Icons.Example;
 
   package Medium = AixLib.Media.Air "Medium model for air";
-  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")=
-       10 "Damper nominal pressure drop";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+     = 10 "Damper nominal pressure drop";
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=1
     "Damper nominal mass flow rate";
   AixLib.Fluid.Actuators.Dampers.Exponential damExp(
@@ -123,53 +123,53 @@ __Dymola_Commands(
 file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Dampers/Validation/PressureIndependent.mos"
 "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model validates
- <a href=\"modelica://AixLib.Fluid.Actuators.Dampers.PressureIndependent\">
- AixLib.Fluid.Actuators.Dampers.PressureIndependent</a>
- by comparing it with
- </p>
- <ul>
- <li>
- an exponential damper model which opening is the one computed by the
- pressure independent model, see <code>damExp</code>,
- </li>
- <li>
- an exponential damper model which opening is computed by a PI controller
- tracking the same discharge mass flow rate, see <code>damExpPI</code>.
- </li>
- </ul>
- <p>
- The simulation consists in exposing these three models to
- <ol>
- <li>
- a first increase in the pressure drop at the damper boundaries, from negative
- to positive values, with a zero input control signal,
- </li>
- <li>
- a consecutive increase of input control signal, from zero to one, with a
- constant pressure drop at the damper boundaries,
- </li>
- <li>
- an eventual decrease in the pressure drop, from positive to negative values,
- with an input control signal equal to one.
- </li>
- </ol>
- <p>
- One can notice a small variation of the computed damper opening in the last
- transient around flow reversal.
- This is because the expression of the flow coefficient as a function of the
- mass flow rate and pressure drop is ill-defined near zero flow rate and
- the damper opening value results from the regularization process.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 5, 2020 by Antoine Gautier:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    Diagram(coordinateSystem(extent={{-120,-120},{120,120}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates
+<a href=\"modelica://AixLib.Fluid.Actuators.Dampers.PressureIndependent\">
+AixLib.Fluid.Actuators.Dampers.PressureIndependent</a>
+by comparing it with
+</p>
+<ul>
+<li>
+an exponential damper model which opening is the one computed by the
+pressure independent model, see <code>damExp</code>,
+</li>
+<li>
+an exponential damper model which opening is computed by a PI controller
+tracking the same discharge mass flow rate, see <code>damExpPI</code>.
+</li>
+</ul>
+<p>
+The simulation consists in exposing these three models to
+<ol>
+<li>
+a first increase in the pressure drop at the damper boundaries, from negative
+to positive values, with a zero input control signal,
+</li>
+<li>
+a consecutive increase of input control signal, from zero to one, with a
+constant pressure drop at the damper boundaries,
+</li>
+<li>
+an eventual decrease in the pressure drop, from positive to negative values,
+with an input control signal equal to one.
+</li>
+</ol>
+<p>
+One can notice a small variation of the computed damper opening in the last
+transient around flow reversal.
+This is because the expression of the flow coefficient as a function of the
+mass flow rate and pressure drop is ill-defined near zero flow rate and
+the damper opening value results from the regularization process.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 5, 2020 by Antoine Gautier:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-120,-120},{120,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureIndependent;
diff --git a/AixLib/Fluid/Actuators/Motors/Examples/IdealMotor.mo b/AixLib/Fluid/Actuators/Motors/Examples/IdealMotor.mo
index 2f31584ee7..8dbacac344 100644
--- a/AixLib/Fluid/Actuators/Motors/Examples/IdealMotor.mo
+++ b/AixLib/Fluid/Actuators/Motors/Examples/IdealMotor.mo
@@ -15,19 +15,19 @@ experiment(Tolerance=1e-6, StopTime=600),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Motors/Examples/IdealMotor.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- Test model for the ideal motor with hysteresis model.
- The motor receives at its control input a time-varying signal.
- It adjusts its position whenever the input signal differs
- from the current position by more than the hysteresis.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 8, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for the ideal motor with hysteresis model.
+The motor receives at its control input a time-varying signal.
+It adjusts its position whenever the input signal differs
+from the current position by more than the hysteresis.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 8, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IdealMotor;
diff --git a/AixLib/Fluid/Actuators/Motors/IdealMotor.mo b/AixLib/Fluid/Actuators/Motors/IdealMotor.mo
index fd82cd0783..851258f2e2 100644
--- a/AixLib/Fluid/Actuators/Motors/IdealMotor.mo
+++ b/AixLib/Fluid/Actuators/Motors/IdealMotor.mo
@@ -73,45 +73,45 @@ equation
    annotation (
 defaultComponentName="mot",
 Documentation(info="<html>
- <p>
- Ideal actuator motor model with hysteresis and finite actuation speed.
- If the current actuator position <code>y</code> is below (or above) the
- input signal <code>u</code> by an amount bigger than the hysteresis
- <code>delta</code>, then the position <code>y</code> is increased (decreased)
- until it reaches <code>u</code>.
- The output <code>y</code> is bounded between <code>0</code> and <code>1</code>.
- </p>
- <p>
- <b>Note:</b> This model can introduce state events which increase the computation time.
- For a more efficient implementation that approximates a motor, set in
- the valve or damper model the parameter <code>use_inputFilter=true</code>
- instead of using this motor model.
- See also
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- September 8, 2008 by Michael Wetter:<br/>
- Added to instance <code>int</code> the attribute
- <code>y(stateSelect=StateSelect.always)</code>. Without this attribute,
- the model <a href=\"modelica://AixLib.Fluid.Examples.TwoWayValves\">
- AixLib.Fluid.Examples.TwoWayValves</a> sets <code>y=3</code>
- which is consistent with this model.
- </li>
- <li>
- September 8, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<p>
+Ideal actuator motor model with hysteresis and finite actuation speed.
+If the current actuator position <code>y</code> is below (or above) the
+input signal <code>u</code> by an amount bigger than the hysteresis
+<code>delta</code>, then the position <code>y</code> is increased (decreased)
+until it reaches <code>u</code>.
+The output <code>y</code> is bounded between <code>0</code> and <code>1</code>.
+</p>
+<p>
+<b>Note:</b> This model can introduce state events which increase the computation time.
+For a more efficient implementation that approximates a motor, set in
+the valve or damper model the parameter <code>use_inputFilter=true</code>
+instead of using this motor model.
+See also
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+September 8, 2008 by Michael Wetter:<br/>
+Added to instance <code>int</code> the attribute
+<code>y(stateSelect=StateSelect.always)</code>. Without this attribute,
+the model <a href=\"modelica://AixLib.Fluid.Examples.TwoWayValves\">
+AixLib.Fluid.Examples.TwoWayValves</a> sets <code>y=3</code>
+which is consistent with this model.
+</li>
+<li>
+September 8, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Line(points={{-8,-86},{-8,68}}, color={192,192,192}),
         Polygon(
           points={{-7,85},{-15,63},{1,63},{-7,85}},
@@ -183,6 +183,6 @@ Documentation(info="<html>
           thickness=0.5),
         Line(
           points={{6,-13},{16,-18},{6,-23}},
-          thickness=0.5)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          thickness=0.5)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end IdealMotor;
diff --git a/AixLib/Fluid/Actuators/Valves/Data/Generic.mo b/AixLib/Fluid/Actuators/Valves/Data/Generic.mo
index f83ca5fc32..07d1a279ce 100644
--- a/AixLib/Fluid/Actuators/Valves/Data/Generic.mo
+++ b/AixLib/Fluid/Actuators/Valves/Data/Generic.mo
@@ -9,28 +9,28 @@ record Generic "Generic record for valve parameters"
 defaultComponentName="datVal",
 defaultComponentPrefixes="parameter",
 Documentation(info="<html>
- <p>
- This is a generic record for the normalized volume flow
- rates for different valve opening positions.
- See the documentation of
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.Data\">
- AixLib.Fluid.Actuators.Valves.Data</a>
- for how to use this record.
- </p>
- </html>",
+<p>
+This is a generic record for the normalized volume flow
+rates for different valve opening positions.
+See the documentation of
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.Data\">
+AixLib.Fluid.Actuators.Valves.Data</a>
+for how to use this record.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added annotation <code>defaultComponentPrefixes=\"parameter\"</code>
- so that the <code>parameter</code> keyword is added when dragging
- the record into a model.
- </li>
- <li>
- March 27, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added annotation <code>defaultComponentPrefixes=\"parameter\"</code>
+so that the <code>parameter</code> keyword is added when dragging
+the record into a model.
+</li>
+<li>
+March 27, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Generic;
diff --git a/AixLib/Fluid/Actuators/Valves/Data/Linear.mo b/AixLib/Fluid/Actuators/Valves/Data/Linear.mo
index 797ea5acac..4952b20e3e 100644
--- a/AixLib/Fluid/Actuators/Valves/Data/Linear.mo
+++ b/AixLib/Fluid/Actuators/Valves/Data/Linear.mo
@@ -6,29 +6,29 @@ record Linear = Generic (
 defaultComponentName="datValLin",
 defaultComponentPrefixes="parameter",
 Documentation(info="<html>
- <p>
- Linear valve opening characteristics with
- a normalized leakage flow rate of <i>0.0001</i>.
- </p>
- <p>
- <b>Note</b>: This record is only for demonstration,
- as the implementation in
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayLinear\">
- AixLib.Fluid.Actuators.Valves.TwoWayLinear</a>
- is more efficient.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added annotation <code>defaultComponentPrefixes=\"parameter\"</code>
- so that the <code>parameter</code> keyword is added when dragging
- the record into a model.
- </li>
- <li>
- March 27, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Linear valve opening characteristics with
+a normalized leakage flow rate of <i>0.0001</i>.
+</p>
+<p>
+<b>Note</b>: This record is only for demonstration,
+as the implementation in
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayLinear\">
+AixLib.Fluid.Actuators.Valves.TwoWayLinear</a>
+is more efficient.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added annotation <code>defaultComponentPrefixes=\"parameter\"</code>
+so that the <code>parameter</code> keyword is added when dragging
+the record into a model.
+</li>
+<li>
+March 27, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/Actuators/Valves/Examples/ThreeWayValves.mo b/AixLib/Fluid/Actuators/Valves/Examples/ThreeWayValves.mo
index 5729015cbe..c48c07c5ea 100644
--- a/AixLib/Fluid/Actuators/Valves/Examples/ThreeWayValves.mo
+++ b/AixLib/Fluid/Actuators/Valves/Examples/ThreeWayValves.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.Actuators.Valves.Examples;
+within AixLib.Fluid.Actuators.Valves.Examples;
 model ThreeWayValves "Three way valves with different opening characteristics"
   extends Modelica.Icons.Example;
 
@@ -107,29 +107,29 @@ equation
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Valves/Examples/ThreeWayValves.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Test model for three way valves. Note that the
- leakage flow rate has been set to a large value
- and the rangeability to a small value
- for better visualization of the valve characteristics.
- To use common values, use the default values.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 17, 2019, by Alexander Kümpel:<br/>
- Added <a href=\"modelica://AixLib.Fluid.Actuators.Valves.ThreeWayTable\">AixLib.Fluid.Actuators.Valves.ThreeWayTable</a>
- to example.
- </li>
- <li>
- February 28, 2013, by Michael Wetter:<br/>
- Added default value for <code>dpValve_nominal</code>.
- </li>
- <li>
- June 16, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for three way valves. Note that the
+leakage flow rate has been set to a large value
+and the rangeability to a small value
+for better visualization of the valve characteristics.
+To use common values, use the default values.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 17, 2019, by Alexander Kümpel:<br/>
+Added <a href=\"modelica://AixLib.Fluid.Actuators.Valves.ThreeWayTable\">AixLib.Fluid.Actuators.Valves.ThreeWayTable</a>
+to example.
+</li>
+<li>
+February 28, 2013, by Michael Wetter:<br/>
+Added default value for <code>dpValve_nominal</code>.
+</li>
+<li>
+June 16, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeWayValves;
diff --git a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvePressureIndependent.mo b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvePressureIndependent.mo
index 80b4cb10ed..25791cb95c 100644
--- a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvePressureIndependent.mo
+++ b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvePressureIndependent.mo
@@ -98,15 +98,15 @@ __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Valves/Examples/TwoWayValvePressureIndependent.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>Test model for pressure independent valves. Note that the leakage at full mass flow rate (<code>l2</code>) has been set to a large value for better visualization of the valve characteristics. To use common values, use the default values. </p>
- <p>The parameter <code>filterOpening</code> is set to <code>false</code>, as this model is used to plot the flow at different opening signals without taking into account the travel time of the actuator. </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 29, 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>Test model for pressure independent valves. Note that the leakage at full mass flow rate (<code>l2</code>) has been set to a large value for better visualization of the valve characteristics. To use common values, use the default values. </p>
+<p>The parameter <code>filterOpening</code> is set to <code>false</code>, as this model is used to plot the flow at different opening signals without taking into account the travel time of the actuator. </p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayValvePressureIndependent;
diff --git a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValveTable.mo b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValveTable.mo
index e09f5984b7..aa322e28c2 100644
--- a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValveTable.mo
+++ b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValveTable.mo
@@ -91,50 +91,50 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Valves/Examples/TwoWayValveTable.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Test model for a two way valve in which a table is used to specify the
- opening characteristics.
- The valve has the following opening characteristics, which is taken from a test case
- of the IEA EBC Annex 60 project.
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <tr><td><i>y</i></td>
-   <td>0</td>  <td>0.1667</td>  <td>0.3333</td>  <td>0.5</td>  <td>0.6667</td>  <td>1</td>
- </tr>
- <tr><td><i>K<sub>v</sub></i></td>
-   <td>0</td>  <td>0.19</td>  <td>0.35</td>  <td>0.45</td>  <td>0.5</td>  <td>0.65</td>       </tr>
- </table>
- <p>
- The <i>K<sub>v</sub></i> value is the volume flow rate in m<sup>3</sup>/h at a pressure difference
- of 1 bar.
- Hence, the <i>K<sub>v</sub></i> value of the fully open valve is <i>K<sub>v</sub>=0.65</i>.
- </p>
- <p>
- Plotting the variables <code>kv.y</code> versus <code>y.y</code> shows that the valve
- reproduces the <i>K<sub>v</sub></i> values shown in the above table.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Actuators/Valves/Examples/TwoWayValveTable_kv.png\"/>
- </p>
- <p>
- The parameter <code>filterOpening</code> is set to <code>false</code>,
- as this model is used to plot the flow at different opening signals
- without taking into account the travel time of the actuator.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 12, 2014 by Michael Wetter:<br/>
- Added <code>parameter</code> keyword to <code>datVal</code>,
- as this is needed to asssign <code>datVal</code> to a parameter
- in the instance <code>valTab</code>.
- This also avoids an error in OpenModelica.
- </li>
- <li>
- April 2, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for a two way valve in which a table is used to specify the
+opening characteristics.
+The valve has the following opening characteristics, which is taken from a test case
+of the IEA EBC Annex 60 project.
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr><td><i>y</i></td>
+  <td>0</td>  <td>0.1667</td>  <td>0.3333</td>  <td>0.5</td>  <td>0.6667</td>  <td>1</td>
+</tr>
+<tr><td><i>K<sub>v</sub></i></td>
+  <td>0</td>  <td>0.19</td>  <td>0.35</td>  <td>0.45</td>  <td>0.5</td>  <td>0.65</td>       </tr>
+</table>
+<p>
+The <i>K<sub>v</sub></i> value is the volume flow rate in m<sup>3</sup>/h at a pressure difference
+of 1 bar.
+Hence, the <i>K<sub>v</sub></i> value of the fully open valve is <i>K<sub>v</sub>=0.65</i>.
+</p>
+<p>
+Plotting the variables <code>kv.y</code> versus <code>y.y</code> shows that the valve
+reproduces the <i>K<sub>v</sub></i> values shown in the above table.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Actuators/Valves/Examples/TwoWayValveTable_kv.png\"/>
+</p>
+<p>
+The parameter <code>filterOpening</code> is set to <code>false</code>,
+as this model is used to plot the flow at different opening signals
+without taking into account the travel time of the actuator.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 12, 2014 by Michael Wetter:<br/>
+Added <code>parameter</code> keyword to <code>datVal</code>,
+as this is needed to asssign <code>datVal</code> to a parameter
+in the instance <code>valTab</code>.
+This also avoids an error in OpenModelica.
+</li>
+<li>
+April 2, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayValveTable;
diff --git a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValves.mo b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValves.mo
index 449186423f..99fc2cd0eb 100644
--- a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValves.mo
+++ b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValves.mo
@@ -124,40 +124,40 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Valves/Examples/TwoWayValves.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Test model for two way valves. Note that the
- leakage flow rate has been set to a large value
- and the rangeability to a small value
- for better visualization of the valve characteristics.
- To use common values, use the default values.
- </p>
- <p>
- The parameter <code>filterOpening</code> is set to <code>false</code>,
- as this model is used to plot the flow at different opening signals
- without taking into account the travel time of the actuator.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 8, 2018, by Filip Jorissen:<br/>
- Added butterfly valve
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/975\">#975</a>.
- </li>
- <li>
- January 29, 2015, by Filip Jorissen:<br/>
- Added pressure-independent valve.
- </li>
- <li>
- February 28, 2013, by Michael Wetter:<br/>
- Added default value for <code>dpValve_nominal</code>.
- </li>
- <li>
- June 16, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Test model for two way valves. Note that the
+leakage flow rate has been set to a large value
+and the rangeability to a small value
+for better visualization of the valve characteristics.
+To use common values, use the default values.
+</p>
+<p>
+The parameter <code>filterOpening</code> is set to <code>false</code>,
+as this model is used to plot the flow at different opening signals
+without taking into account the travel time of the actuator.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 8, 2018, by Filip Jorissen:<br/>
+Added butterfly valve
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/975\">#975</a>.
+</li>
+<li>
+January 29, 2015, by Filip Jorissen:<br/>
+Added pressure-independent valve.
+</li>
+<li>
+February 28, 2013, by Michael Wetter:<br/>
+Added default value for <code>dpValve_nominal</code>.
+</li>
+<li>
+June 16, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(extent={{-100,-140},{100,120}})),
-    Icon(coordinateSystem(extent={{-100,-140},{100,120}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-140},{100,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayValves;
diff --git a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesMotor.mo b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesMotor.mo
index 48223810bc..2b06b58a73 100644
--- a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesMotor.mo
+++ b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesMotor.mo
@@ -106,35 +106,35 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Valves/Examples/TwoWayValvesMotor.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Test model for two way valves. Note that the
- leakage flow rate has been set to a large value
- and the rangeability to a small value
- for better visualization of the valve characteristics.
- To use common values, use the default values.
- </p>
- <p>
- All valves are connected to a model of a motor with
- hysteresis. A more efficient implementation that approximates
- a motor but lacks hysteresis would be to
- set the valve parameter <code>use_inputFilter=true</code> instead
- of using the motor model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 29, 2015, by Filip Jorissen:<br/>
- Added pressure-independent valve.
- </li>
- <li>
- February 28, 2013, by Michael Wetter:<br/>
- Added default value for <code>dpValve_nominal</code>.
- </li>
- <li>
- June 16, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for two way valves. Note that the
+leakage flow rate has been set to a large value
+and the rangeability to a small value
+for better visualization of the valve characteristics.
+To use common values, use the default values.
+</p>
+<p>
+All valves are connected to a model of a motor with
+hysteresis. A more efficient implementation that approximates
+a motor but lacks hysteresis would be to
+set the valve parameter <code>use_inputFilter=true</code> instead
+of using the motor model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 29, 2015, by Filip Jorissen:<br/>
+Added pressure-independent valve.
+</li>
+<li>
+February 28, 2013, by Michael Wetter:<br/>
+Added default value for <code>dpValve_nominal</code>.
+</li>
+<li>
+June 16, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayValvesMotor;
diff --git a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesTable.mo b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesTable.mo
index a019f0ba5a..3f7cf2518e 100644
--- a/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesTable.mo
+++ b/AixLib/Fluid/Actuators/Valves/Examples/TwoWayValvesTable.mo
@@ -63,32 +63,32 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Valves/Examples/TwoWayValvesTable.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Test model for two way valves.
- The instance <code>valTab</code> has a linear opening characteristics
- based on a table, while <code>valLin</code> also has a linear opening
- characteristics that is directly implemented in the model.
- For practical applications in which valves with linear opening characteristics
- are used, one should use <code>valLin</code> rather
- than <code>valTab</code> as <code>valLin</code> is a more efficient
- implementation.
- </p>
- <p>
- This test demonstrates that both valves have, as expected, the same
- mass flow rate for the whole range of the opening signal.
- </p>
- <p>
- The parameter <code>filterOpening</code> is set to <code>false</code>,
- as this model is used to plot the flow at different opening signals
- without taking into account the travel time of the actuator.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 26, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for two way valves.
+The instance <code>valTab</code> has a linear opening characteristics
+based on a table, while <code>valLin</code> also has a linear opening
+characteristics that is directly implemented in the model.
+For practical applications in which valves with linear opening characteristics
+are used, one should use <code>valLin</code> rather
+than <code>valTab</code> as <code>valLin</code> is a more efficient
+implementation.
+</p>
+<p>
+This test demonstrates that both valves have, as expected, the same
+mass flow rate for the whole range of the opening signal.
+</p>
+<p>
+The parameter <code>filterOpening</code> is set to <code>false</code>,
+as this model is used to plot the flow at different opening signals
+without taking into account the travel time of the actuator.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayValvesTable;
diff --git a/AixLib/Fluid/Actuators/Valves/ThreeWayEqualPercentageLinear.mo b/AixLib/Fluid/Actuators/Valves/ThreeWayEqualPercentageLinear.mo
index 68cd548c12..2c222b5023 100644
--- a/AixLib/Fluid/Actuators/Valves/ThreeWayEqualPercentageLinear.mo
+++ b/AixLib/Fluid/Actuators/Valves/ThreeWayEqualPercentageLinear.mo
@@ -13,14 +13,13 @@ model ThreeWayEqualPercentageLinear
     "Range of significant deviation from equal percentage law";
 
 equation
-  connect(inv.y, res3.y) annotation (Line(points={{-62.6,46},{20,46},{20,46},{
-          20,-50},{12,-50}},
+  connect(inv.y, res3.y) annotation (Line(points={{-62.6,46},{30,46},{30,-50},{
+          12,-50}},      color={0,0,127}));
+  connect(y_actual, inv.u2) annotation (Line(points={{50,70},{88,70},{88,34},{
+          -68,34},{-68,41.2}},
                          color={0,0,127}));
-  connect(y_actual, inv.u2) annotation (Line(points={{50,70},{84,70},{84,32},{-68,
-          32},{-68,41.2}},
-                         color={0,0,127}));
-  connect(y_actual, res1.y) annotation (Line(points={{50,70},{84,70},{84,32},{
-          -50,32},{-50,12}},
+  connect(y_actual, res1.y) annotation (Line(points={{50,70},{88,70},{88,34},{
+          -50,34},{-50,12}},
         color={0,0,127}));
   annotation (                       Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,
             -100},{100,100}}), graphics={Text(
@@ -30,78 +29,78 @@ equation
           textString="%%")}),
 defaultComponentName="val",
 Documentation(info="<html>
- <p>
- Three way valve with equal percentage characteristics
- between <code>port_1</code> and <code>port_2</code>
- and linear opening characteristic between <code>port_3</code> and <code>port_2</code>.
- Such opening characteristics were typical for valves from Landis &amp; Gyr (now
- Siemens).
- </p><p>
- This model is based on the partial valve models
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a> and
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
- for the implementation of the three way valve
- and see
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>
- for the implementation of the regularization near the origin.
- </p>
- </html>",
+<p>
+Three way valve with equal percentage characteristics
+between <code>port_1</code> and <code>port_2</code>
+and linear opening characteristic between <code>port_3</code> and <code>port_2</code>.
+Such opening characteristics were typical for valves from Landis &amp; Gyr (now
+Siemens).
+</p><p>
+This model is based on the partial valve models
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a> and
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
+for the implementation of the three way valve
+and see
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>
+for the implementation of the regularization near the origin.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating stage.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- November 5, 2019, by Michael Wetter:<br/>
- Moved assignment of leakage from <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
- to the parent classes.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1227\">#1227</a>.
- </li>
- <li>
- February 20, 2012 by Michael Wetter:<br/>
- Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
- and added new parameter <code>dpFixed_nominal</code>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>.
- </li>
- <li>
- February 14, 2012 by Michael Wetter:<br/>
- Added filter to approximate the travel time of the actuator.
- </li>
- <li>
- March 25, 2011, by Michael Wetter:<br/>
- Added homotopy method.
- </li>
- <li>
- June 16, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating stage.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+November 5, 2019, by Michael Wetter:<br/>
+Moved assignment of leakage from <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
+to the parent classes.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1227\">#1227</a>.
+</li>
+<li>
+February 20, 2012 by Michael Wetter:<br/>
+Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
+and added new parameter <code>dpFixed_nominal</code>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>.
+</li>
+<li>
+February 14, 2012 by Michael Wetter:<br/>
+Added filter to approximate the travel time of the actuator.
+</li>
+<li>
+March 25, 2011, by Michael Wetter:<br/>
+Added homotopy method.
+</li>
+<li>
+June 16, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeWayEqualPercentageLinear;
diff --git a/AixLib/Fluid/Actuators/Valves/ThreeWayLinear.mo b/AixLib/Fluid/Actuators/Valves/ThreeWayLinear.mo
index 6d6a01432e..e3f424b7bc 100644
--- a/AixLib/Fluid/Actuators/Valves/ThreeWayLinear.mo
+++ b/AixLib/Fluid/Actuators/Valves/ThreeWayLinear.mo
@@ -7,7 +7,7 @@ model ThreeWayLinear "Three way valve with linear characteristics"
         final l=l[2]));
 
 equation
-  connect(inv.y, res3.y) annotation (Line(points={{-62.6,46},{20,46},{20,-50},{
+  connect(inv.y, res3.y) annotation (Line(points={{-62.6,46},{30,46},{30,-50},{
           12,-50}},      color={0,0,127}));
   connect(y_actual, inv.u2) annotation (Line(points={{50,70},{88,70},{88,34},{
           -68,34},{-68,41.2}},
@@ -17,68 +17,68 @@ equation
         color={0,0,127}));
   annotation (defaultComponentName="val",
 Documentation(info="<html>
- <p>
- Three way valve with linear opening characteristic.
- </p><p>
- This model is based on the partial valve models
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a> and
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
- for the implementation of the three way valve
- and see
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>
- for the implementation of the regularization near the origin.
- </p>
- </html>",
+<p>
+Three way valve with linear opening characteristic.
+</p><p>
+This model is based on the partial valve models
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a> and
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
+for the implementation of the three way valve
+and see
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>
+for the implementation of the regularization near the origin.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- November 5, 2019, by Michael Wetter:<br/>
- Moved assignment of leakage from <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
- to the parent classes.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1227\">#1227</a>.
- </li>
- <li>
- February 20, 2012 by Michael Wetter:<br/>
- Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
- and added new parameter <code>dpFixed_nominal</code>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>.
- </li>
- <li>
- February 14, 2012 by Michael Wetter:<br/>
- Added filter to approximate the travel time of the actuator.
- </li>
- <li>
- March 25, 2011, by Michael Wetter:<br/>
- Added homotopy method.
- </li>
- <li>
- June 16, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+November 5, 2019, by Michael Wetter:<br/>
+Moved assignment of leakage from <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>
+to the parent classes.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1227\">#1227</a>.
+</li>
+<li>
+February 20, 2012 by Michael Wetter:<br/>
+Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
+and added new parameter <code>dpFixed_nominal</code>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>.
+</li>
+<li>
+February 14, 2012 by Michael Wetter:<br/>
+Added filter to approximate the travel time of the actuator.
+</li>
+<li>
+March 25, 2011, by Michael Wetter:<br/>
+Added homotopy method.
+</li>
+<li>
+June 16, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeWayLinear;
diff --git a/AixLib/Fluid/Actuators/Valves/ThreeWayTable.mo b/AixLib/Fluid/Actuators/Valves/ThreeWayTable.mo
index efe9ed1b17..8891887f93 100644
--- a/AixLib/Fluid/Actuators/Valves/ThreeWayTable.mo
+++ b/AixLib/Fluid/Actuators/Valves/ThreeWayTable.mo
@@ -15,127 +15,127 @@ model ThreeWayTable
             {-30,100}})));
 equation
   connect(inv.y, res3.y)
-  annotation (Line(points={{-62.6,46},{20,46},{20,-50},{12,-50}}, color={0,0,127}));
+  annotation (Line(points={{-62.6,46},{30,46},{30,-50},{12,-50}}, color={0,0,127}));
   connect(y_actual, inv.u2)
   annotation (Line(points={{50,70},{88,70},{88,34},{-68,34},{-68,41.2}}, color={0,0,127}));
   connect(y_actual, res1.y)
   annotation (Line(points={{50,70},{88,70},{88,34},{-50,34},{-50,12}}, color={0,0,127}));
   annotation (defaultComponentName="val",
 Documentation(info="<html>
- <p>
- Three way valve with table-specified opening characteristics.
- A separate characteristic for each flow path is used.
- </p>
- <p>
- Each flow path uses an instance of the model
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayTable\">
- AixLib.Fluid.Actuators.Valves.TwoWayTable</a>.
- Therefore, this model needs to be parameterized the same way as
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayTable\">
- AixLib.Fluid.Actuators.Valves.TwoWayTable</a>.
- Specifically,
- the mass flow rate for the fully open valve is determined based
- on the value of the parameter <code>CvData</code>.
- For the different valve positions <i>y &isin; [0, 1]</i>, this nominal flow rate is
- scaled by the values of the parameter
- <code>flowCharacteristics1</code> and <code>flowCharacteristics3</code>, respectively.
- These parameters declare a table of the form
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <tr>
- <td><i>y</i></td>  <td>0</td>  <td>...</td>  <td>1</td>
- </tr>
- <tr>
- <td><i>&phi;</i></td>  <td><i>l</i></td>  <td>...</td>  <td>1</td>
- </tr>
- </table>
- <p>
- where <i>l = K<sub>v</sub>(y=0)/K<sub>v</sub>(y=1) &gt; 0</i> is the valve leakage.
- The first row is the valve opening, and the second row is the
- mass flow rate, relative to the mass flow rate of the fully open
- valve, under the assumption of a constant pressure difference across the
- valve.
- A suggested value for the valve leakage is <i>l=0.0001</i>.
- If <i>l = 0</i>, then this model will replace it with
- <i>l = 10<sup>-8</sup></i> for numerical reasons.
- For example, if a valve has <i>K<sub>v</sub>=0.5</i> [m<sup>3</sup>/h/bar<sup>1/2</sup>] and
- a linear opening characteristics and
- a valve leakage of <i>l=0.0001</i>, then one would set
- </p>
- <pre>
-  CvData=AixLib.Fluid.Types.CvTypes.Kv
-  Kv = 0.5
-  flowCharacteristics1(y={0,1}, phi={0.0001,1})
-  flowCharacteristics3(y={0,1}, phi={0.0001,1})
- </pre>
- <p>
- Note, however, that
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.ThreeWayLinear\">
- AixLib.Fluid.Actuators.Valves.ThreeWayLinear</a> provides a more
- efficient implementation for this simple case.
- </p>
- <p>
- The parameters <code>flowCharacteristics1</code> and <code>flowCharacteristics3</code> must meet the following
- requirements, otherwise the model stops with an error:
- </p>
- <ul>
- <li>
- Their arrays
- <code>y</code> and <code>phi</code>
- must be strictly monotonic increasing.
- </li>
- <li>
- The first value must satisfy
- <code>y[1]=0</code>, and
- <code>phi[1]</code> must be equal to the
- leakage flow rate, which must be bigger than zero.
- Otherwise, a default value of <code>1E-8</code> is used.
- </li>
- <li>
- The last values must satisfy
- <code>y[end]=1</code> and
- <code>phi[end]=1</code>.
- </li>
- </ul>
- <p>
- This model is based on the partial valve model
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
- Check this model for more information, such
- as the regularization near the origin.
- </p>
- <p>
- For an example that specifies an opening characteristics, see
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable\">
- AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable</a>.
- </p>
- 
- </html>",
+<p>
+Three way valve with table-specified opening characteristics.
+A separate characteristic for each flow path is used.
+</p>
+<p>
+Each flow path uses an instance of the model
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayTable\">
+AixLib.Fluid.Actuators.Valves.TwoWayTable</a>.
+Therefore, this model needs to be parameterized the same way as
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayTable\">
+AixLib.Fluid.Actuators.Valves.TwoWayTable</a>.
+Specifically,
+the mass flow rate for the fully open valve is determined based
+on the value of the parameter <code>CvData</code>.
+For the different valve positions <i>y &isin; [0, 1]</i>, this nominal flow rate is
+scaled by the values of the parameter
+<code>flowCharacteristics1</code> and <code>flowCharacteristics3</code>, respectively.
+These parameters declare a table of the form
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<td><i>y</i></td>  <td>0</td>  <td>...</td>  <td>1</td>
+</tr>
+<tr>
+<td><i>&phi;</i></td>  <td><i>l</i></td>  <td>...</td>  <td>1</td>
+</tr>
+</table>
+<p>
+where <i>l = K<sub>v</sub>(y=0)/K<sub>v</sub>(y=1) &gt; 0</i> is the valve leakage.
+The first row is the valve opening, and the second row is the
+mass flow rate, relative to the mass flow rate of the fully open
+valve, under the assumption of a constant pressure difference across the
+valve.
+A suggested value for the valve leakage is <i>l=0.0001</i>.
+If <i>l = 0</i>, then this model will replace it with
+<i>l = 10<sup>-8</sup></i> for numerical reasons.
+For example, if a valve has <i>K<sub>v</sub>=0.5</i> [m<sup>3</sup>/h/bar<sup>1/2</sup>] and
+a linear opening characteristics and
+a valve leakage of <i>l=0.0001</i>, then one would set
+</p>
+<pre>
+ CvData=AixLib.Fluid.Types.CvTypes.Kv
+ Kv = 0.5
+ flowCharacteristics1(y={0,1}, phi={0.0001,1})
+ flowCharacteristics3(y={0,1}, phi={0.0001,1})
+</pre>
+<p>
+Note, however, that
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.ThreeWayLinear\">
+AixLib.Fluid.Actuators.Valves.ThreeWayLinear</a> provides a more
+efficient implementation for this simple case.
+</p>
+<p>
+The parameters <code>flowCharacteristics1</code> and <code>flowCharacteristics3</code> must meet the following
+requirements, otherwise the model stops with an error:
+</p>
+<ul>
+<li>
+Their arrays
+<code>y</code> and <code>phi</code>
+must be strictly monotonic increasing.
+</li>
+<li>
+The first value must satisfy
+<code>y[1]=0</code>, and
+<code>phi[1]</code> must be equal to the
+leakage flow rate, which must be bigger than zero.
+Otherwise, a default value of <code>1E-8</code> is used.
+</li>
+<li>
+The last values must satisfy
+<code>y[end]=1</code> and
+<code>phi[end]=1</code>.
+</li>
+</ul>
+<p>
+This model is based on the partial valve model
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
+Check this model for more information, such
+as the regularization near the origin.
+</p>
+<p>
+For an example that specifies an opening characteristics, see
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable\">
+AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable</a>.
+</p>
+
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- November 28, 2019, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- November 15, 2019, by Alexander K&uuml;mpel:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+November 28, 2019, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+November 15, 2019, by Alexander K&uuml;mpel:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Rectangle(
           origin={-80,-79},
@@ -149,6 +149,6 @@ revisions="<html>
         Line(
           points={{-92,-76},{-68,-76}}),
         Line(
-          points={{-92,-84},{-68,-84}})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          points={{-92,-84},{-68,-84}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeWayTable;
diff --git a/AixLib/Fluid/Actuators/Valves/TwoWayButterfly.mo b/AixLib/Fluid/Actuators/Valves/TwoWayButterfly.mo
index 48c20c03c3..23a25dac73 100644
--- a/AixLib/Fluid/Actuators/Valves/TwoWayButterfly.mo
+++ b/AixLib/Fluid/Actuators/Valves/TwoWayButterfly.mo
@@ -45,49 +45,49 @@ model TwoWayButterfly
 annotation (
 defaultComponentName="valBut",
 Documentation(info="<html>
- <p>
- Two way valve with the flow characteristic of a typical butterfly valve as listed below.
- </p>
- <p>
- <img src=\"modelica://AixLib/Resources/Images/Fluid/Actuators/Valves/Examples/TwoWayButterfly.png\" alt=\"Butterfly valve characteristic\"/>
- </p>
- <h4>Implementation</h4>
- <p>
- The model assigns a <code>Kv</code> based on the table at
- <a href=\"http://www.mydatabook.org/fluid-mechanics/flow-coefficient-opening-and-closure-curves-of-butterfly-valves/\">mydatabook.org</a>.
- The <code>Kv</code> values listed in the parameter <code>Kvs</code> are reasonable assumptions,
- but the actual value can depend much on the design of the specific valve.
- Moreover, the <code>Kv</code> values for DN value smaller than DN 150 are a quadratic extrapolation
- from the value at DN 150.
- </p>
- </html>",
+<p>
+Two way valve with the flow characteristic of a typical butterfly valve as listed below.
+</p>
+<p>
+<img src=\"modelica://AixLib/Resources/Images/Fluid/Actuators/Valves/Examples/TwoWayButterfly.png\" alt=\"Butterfly valve characteristic\"/>
+</p>
+<h4>Implementation</h4>
+<p>
+The model assigns a <code>Kv</code> based on the table at
+<a href=\"http://www.mydatabook.org/fluid-mechanics/flow-coefficient-opening-and-closure-curves-of-butterfly-valves/\">mydatabook.org</a>.
+The <code>Kv</code> values listed in the parameter <code>Kvs</code> are reasonable assumptions,
+but the actual value can depend much on the design of the specific valve.
+Moreover, the <code>Kv</code> values for DN value smaller than DN 150 are a quadratic extrapolation
+from the value at DN 150.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- December 22, 2020 by Michael Wetter:<br/>
- Add parameter <code>Kvs</code>.
- </li>
- <li>
- December 20, 2020 by Filip Jorissen:<br/>
- Revised implementation with default <code>Kv</code> computation.
- </li>
- <li>
- July 8, 2018 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+December 22, 2020 by Michael Wetter:<br/>
+Add parameter <code>Kvs</code>.
+</li>
+<li>
+December 20, 2020 by Filip Jorissen:<br/>
+Revised implementation with default <code>Kv</code> computation.
+</li>
+<li>
+July 8, 2018 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={Ellipse(
           extent={{-16,18},{16,-14}},
           lineColor={0,0,0},
           fillColor={0,0,0},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayButterfly;
diff --git a/AixLib/Fluid/Actuators/Valves/TwoWayEqualPercentage.mo b/AixLib/Fluid/Actuators/Valves/TwoWayEqualPercentage.mo
index 2621ee976b..1951742113 100644
--- a/AixLib/Fluid/Actuators/Valves/TwoWayEqualPercentage.mo
+++ b/AixLib/Fluid/Actuators/Valves/TwoWayEqualPercentage.mo
@@ -28,84 +28,84 @@ initial equation
   annotation (
     defaultComponentName="val",
     Documentation(info="<html>
- <p>
- Two way valve with an equal percentage valve opening characteristic.
- </p><p>
- This model is based on the partial valve model
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
- Check this model for more information, such
- as the regularization near the origin.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- August 7, 2020, by Ettore Zanetti:<br/>
- changed the computation of <code>phi</code> using
- <code>max(0.1*l, . )</code> to avoid
- phi=0.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
- issue 1376</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- November 9, 2019, by Filip Jorissen:<br/>
- Guarded the computation of <code>phi</code> using
- <code>max(0, . )</code> to avoid
- negative phi.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
- issue 1223</a>.
- </li>
- <li>
- April 4, 2014, by Michael Wetter:<br/>
- Moved the assignment of the flow function <code>phi</code>
- to the model instantiation because in its base class,
- the keyword <code>input</code>
- has been added to the variable <code>phi</code>.
- </li>
- <li>
- March 27, 2014 by Michael Wetter:<br/>
- Revised model for implementation of new valve model that computes the flow function
- based on a table.
- </li>
- <li>
- February 20, 2012 by Michael Wetter:<br/>
- Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
- and added new parameter <code>dpFixed_nominal</code>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>.
- </li>
- <li>
- February 14, 2012 by Michael Wetter:<br/>
- Added filter to approximate the travel time of the actuator.
- </li>
- <li>
- March 25, 2011, by Michael Wetter:<br/>
- Added homotopy method.
- </li>
- <li>
- June 5, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+<p>
+Two way valve with an equal percentage valve opening characteristic.
+</p><p>
+This model is based on the partial valve model
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
+Check this model for more information, such
+as the regularization near the origin.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+August 7, 2020, by Ettore Zanetti:<br/>
+changed the computation of <code>phi</code> using
+<code>max(0.1*l, . )</code> to avoid
+phi=0.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
+issue 1376</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+November 9, 2019, by Filip Jorissen:<br/>
+Guarded the computation of <code>phi</code> using
+<code>max(0, . )</code> to avoid
+negative phi.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
+issue 1223</a>.
+</li>
+<li>
+April 4, 2014, by Michael Wetter:<br/>
+Moved the assignment of the flow function <code>phi</code>
+to the model instantiation because in its base class,
+the keyword <code>input</code>
+has been added to the variable <code>phi</code>.
+</li>
+<li>
+March 27, 2014 by Michael Wetter:<br/>
+Revised model for implementation of new valve model that computes the flow function
+based on a table.
+</li>
+<li>
+February 20, 2012 by Michael Wetter:<br/>
+Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
+and added new parameter <code>dpFixed_nominal</code>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>.
+</li>
+<li>
+February 14, 2012 by Michael Wetter:<br/>
+Added filter to approximate the travel time of the actuator.
+</li>
+<li>
+March 25, 2011, by Michael Wetter:<br/>
+Added homotopy method.
+</li>
+<li>
+June 5, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
             {100,100}}), graphics={Text(
           extent={{-74,20},{-36,-24}},
           textColor=DynamicSelect({255,255,255}, (1-y)*{255,255,255}),
           fillPattern=FillPattern.Solid,
-          textString="%%")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="%%")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayEqualPercentage;
diff --git a/AixLib/Fluid/Actuators/Valves/TwoWayLinear.mo b/AixLib/Fluid/Actuators/Valves/TwoWayLinear.mo
index f7f4ece5af..8f6d29a09b 100644
--- a/AixLib/Fluid/Actuators/Valves/TwoWayLinear.mo
+++ b/AixLib/Fluid/Actuators/Valves/TwoWayLinear.mo
@@ -9,66 +9,66 @@ initial equation
 annotation (
 defaultComponentName="val",
 Documentation(info="<html>
- <p>
- Two way valve with linear opening characteristic.
- </p><p>
- This model is based on the partial valve model
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
- Check this model for more information, such
- as the regularization near the origin.
- </p>
- </html>",
+<p>
+Two way valve with linear opening characteristic.
+</p><p>
+This model is based on the partial valve model
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
+Check this model for more information, such
+as the regularization near the origin.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- August 7, 2020, by Ettore Zanetti:<br/>
- changed the computation of <code>phi</code> using
- <code>max(0.1*l, . )</code> to avoid
- phi=0.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
- issue 1376</a>.
- </li>
- <li>
- November 9, 2019, by Filip Jorissen:<br/>
- Guarded the computation of <code>phi</code> using
- <code>max(0, . )</code> to avoid
- negative phi.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
- issue 1223</a>.
- </li>
- <li>
- April 4, 2014, by Michael Wetter:<br/>
- Moved the assignment of the flow function <code>phi</code>
- to the model instantiation because in its base class,
- the keyword <code>input</code>
- has been added to the variable <code>phi</code>.
- </li>
- <li>
- March 27, 2014 by Michael Wetter:<br/>
- Revised model for implementation of new valve model that computes the flow function
- based on a table.
- </li>
- <li>
- February 20, 2012 by Michael Wetter:<br/>
- Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
- and added new parameter <code>dpFixed_nominal=0</code>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>.
- </li>
- <li>
- June 3, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+August 7, 2020, by Ettore Zanetti:<br/>
+changed the computation of <code>phi</code> using
+<code>max(0.1*l, . )</code> to avoid
+phi=0.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
+issue 1376</a>.
+</li>
+<li>
+November 9, 2019, by Filip Jorissen:<br/>
+Guarded the computation of <code>phi</code> using
+<code>max(0, . )</code> to avoid
+negative phi.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
+issue 1223</a>.
+</li>
+<li>
+April 4, 2014, by Michael Wetter:<br/>
+Moved the assignment of the flow function <code>phi</code>
+to the model instantiation because in its base class,
+the keyword <code>input</code>
+has been added to the variable <code>phi</code>.
+</li>
+<li>
+March 27, 2014 by Michael Wetter:<br/>
+Revised model for implementation of new valve model that computes the flow function
+based on a table.
+</li>
+<li>
+February 20, 2012 by Michael Wetter:<br/>
+Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
+and added new parameter <code>dpFixed_nominal=0</code>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>.
+</li>
+<li>
+June 3, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayLinear;
diff --git a/AixLib/Fluid/Actuators/Valves/TwoWayPolynomial.mo b/AixLib/Fluid/Actuators/Valves/TwoWayPolynomial.mo
index 5e1adcd85b..987db67156 100644
--- a/AixLib/Fluid/Actuators/Valves/TwoWayPolynomial.mo
+++ b/AixLib/Fluid/Actuators/Valves/TwoWayPolynomial.mo
@@ -20,64 +20,64 @@ initial equation
     for i in 0:nP/2 loop
       assert(sum({c[j+1]*j*(i/nP)^(j-1) for j in 1:size(c, 1) - 1})>=0,
       "The provided valve polynomial coefficients 
-       do not lead to a strictly increasing characteristic for y="+ String(i/nP)+ ". This is not allowed.");
+      do not lead to a strictly increasing characteristic for y=" + String(i/nP)+ ". This is not allowed.");
     end for;
   end if;
   assert(c[1]>=0, "The provided valve polynomial coefficients do not lead to 
-   a valve opening that is larger than or equal to zero for a control signal of zero.");
+  a valve opening that is larger than or equal to zero for a control signal of zero.");
   assert(sum(c)<=1.1, "The provided valve polynomial coefficients do not lead to 
-   a valve opening that is smaller than or equal to one for a control signal of one.");
+  a valve opening that is smaller than or equal to one for a control signal of one.");
 
 annotation (
 defaultComponentName="val",
 Documentation(info="<html>
- <p>
- Two way valve with polynomial opening characteristic.
- The polynomial coefficients are defined using parameter <code>c</code>.
- The elements of <code>c</code> are coefficients for increasing powers of <code>y</code>,
- starting with the power <code>0</code>, which corresponds to a fixed offset.
- This valve model can be used to implement valves with a custom
- opening characteristic, such as a combination
- of a linear and an equal percentage characteristic.
- </p>
- <p>
- This model is based on the partial valve model
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
- Check this model for more information, such
- as the regularization near the origin.
- </p>
- </html>",
+<p>
+Two way valve with polynomial opening characteristic.
+The polynomial coefficients are defined using parameter <code>c</code>.
+The elements of <code>c</code> are coefficients for increasing powers of <code>y</code>,
+starting with the power <code>0</code>, which corresponds to a fixed offset.
+This valve model can be used to implement valves with a custom
+opening characteristic, such as a combination
+of a linear and an equal percentage characteristic.
+</p>
+<p>
+This model is based on the partial valve model
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
+Check this model for more information, such
+as the regularization near the origin.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- August 7, 2020, by Ettore Zanetti:<br/>
- changed the computation of <code>phi</code> using
- <code>max(0.1*l, . )</code> to avoid
- phi=0.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
- issue 1376</a>.
- </li>
- <li>
- November 9, 2019, by Filip Jorissen:<br/>
- Guarded the computation of <code>phi</code> using
- <code>max(0, . )</code> to avoid
- negative phi.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
- issue 1223</a>.
- </li>
- <li>
- September 30, 2017 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+August 7, 2020, by Ettore Zanetti:<br/>
+changed the computation of <code>phi</code> using
+<code>max(0.1*l, . )</code> to avoid
+phi=0.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
+issue 1376</a>.
+</li>
+<li>
+November 9, 2019, by Filip Jorissen:<br/>
+Guarded the computation of <code>phi</code> using
+<code>max(0, . )</code> to avoid
+negative phi.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
+issue 1223</a>.
+</li>
+<li>
+September 30, 2017 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayPolynomial;
diff --git a/AixLib/Fluid/Actuators/Valves/TwoWayPressureIndependent.mo b/AixLib/Fluid/Actuators/Valves/TwoWayPressureIndependent.mo
index da26bfe7f4..3baab70b89 100644
--- a/AixLib/Fluid/Actuators/Valves/TwoWayPressureIndependent.mo
+++ b/AixLib/Fluid/Actuators/Valves/TwoWayPressureIndependent.mo
@@ -158,132 +158,132 @@ equation
   end if;
   annotation (defaultComponentName="val",
 Documentation(info="<html>
- <p>
- Two way valve with a pressure-independent valve opening characteristic.
- The mass flow rate is controlled such that it is nearly equal to its
- set point <code>y*m_flow_nominal</code>, unless the pressure
- <code>dp</code> is too low, in which case a regular <code>Kv</code>
- characteristic is used.
- </p>
- <h4>Main equations</h4>
- <p>
- First the minimum pressure head <code>dp_min</code>
- required for delivering the requested mass flow rate
- <code>y*m_flow_nominal</code> is computed. If
- <code>dp &gt; dp_min</code> then the requested mass flow
- rate is supplied. If <code>dp &lt; dp_min</code> then
- <code>m_flow = Kv/sqrt(dp)</code>. Transition between
- these two flow regimes happens in a smooth way.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- This model is configured by setting <code>m_flow_nominal</code>
- to the mass flow rate that the valve should supply when it is
- completely open, i.e., <code>y = 1</code>. The pressure drop corresponding
- to this working point can be set using <code>dpValve_nominal</code>,
- or using a <code>Kv</code>, <code>Cv</code> or <code>Av</code>
- value. The parameter <code>dpValve_fixed</code> can be used to add
- additional pressure drops, although in this valve it is equivalent to
- add these to <code>dpValve_nominal</code>.
- </p>
- <p>
- The parameter <code>l2</code> represents the non-ideal
- leakage behaviour of this valve for high pressures.
- It is assumed that the mass flow rate will rise beyond
- the requested mass flow rate <code>y*m_flow_nominal</code>
- if <code>dp &gt; dpValve_nominal+dpFixed_nominal</code>.
- The parameter <code>l2</code> represents the slope
- of this rise:
- <code>d(m_flow)/d(dp) = l2* m_flow_nominal/dp_nominal</code>.
- In the ideal case <code>l2=0</code>, but
- this may introduce singularities, for instance when
- connecting this component with a fixed mass flow source.
- </p>
- <h4>Options</h4>
- <p>
- Parameter <code>deltax</code> sets the duration of
- the transition region between the two flow regimes
- as a fraction of <code>dp_nominal</code> or <code>m_flow_nominal</code>,
- depending on the value of <code>from_dp</code>.
- </p>
- <h4>Implementation</h4>
- <p>
- Note that the result in the transition region when
- using <code>from_dp = true</code> is not identical to
- the result when using <code>from_dp = false</code>.
- </p>
- <p>
- Variables <code>*_y1</code> and <code>*_y2</code>
- serve a dual use.
- They are used to
- 1) compute the support points at <code>*_x1</code> and <code>*_x2</code>,
- which should not depend on <code>m_flow</code> or <code>dp</code> and
- 2) to compute the flow functions when outside of this regime,
- which does depend on <code>m_flow</code> or <code>dp</code>.
- Min and max functions are therefore used such that one equation
- can serve both puroposes.
- </p>
- </html>",
+<p>
+Two way valve with a pressure-independent valve opening characteristic.
+The mass flow rate is controlled such that it is nearly equal to its
+set point <code>y*m_flow_nominal</code>, unless the pressure
+<code>dp</code> is too low, in which case a regular <code>Kv</code>
+characteristic is used.
+</p>
+<h4>Main equations</h4>
+<p>
+First the minimum pressure head <code>dp_min</code>
+required for delivering the requested mass flow rate
+<code>y*m_flow_nominal</code> is computed. If
+<code>dp &gt; dp_min</code> then the requested mass flow
+rate is supplied. If <code>dp &lt; dp_min</code> then
+<code>m_flow = Kv/sqrt(dp)</code>. Transition between
+these two flow regimes happens in a smooth way.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+This model is configured by setting <code>m_flow_nominal</code>
+to the mass flow rate that the valve should supply when it is
+completely open, i.e., <code>y = 1</code>. The pressure drop corresponding
+to this working point can be set using <code>dpValve_nominal</code>,
+or using a <code>Kv</code>, <code>Cv</code> or <code>Av</code>
+value. The parameter <code>dpValve_fixed</code> can be used to add
+additional pressure drops, although in this valve it is equivalent to
+add these to <code>dpValve_nominal</code>.
+</p>
+<p>
+The parameter <code>l2</code> represents the non-ideal
+leakage behaviour of this valve for high pressures.
+It is assumed that the mass flow rate will rise beyond
+the requested mass flow rate <code>y*m_flow_nominal</code>
+if <code>dp &gt; dpValve_nominal+dpFixed_nominal</code>.
+The parameter <code>l2</code> represents the slope
+of this rise:
+<code>d(m_flow)/d(dp) = l2* m_flow_nominal/dp_nominal</code>.
+In the ideal case <code>l2=0</code>, but
+this may introduce singularities, for instance when
+connecting this component with a fixed mass flow source.
+</p>
+<h4>Options</h4>
+<p>
+Parameter <code>deltax</code> sets the duration of
+the transition region between the two flow regimes
+as a fraction of <code>dp_nominal</code> or <code>m_flow_nominal</code>,
+depending on the value of <code>from_dp</code>.
+</p>
+<h4>Implementation</h4>
+<p>
+Note that the result in the transition region when
+using <code>from_dp = true</code> is not identical to
+the result when using <code>from_dp = false</code>.
+</p>
+<p>
+Variables <code>*_y1</code> and <code>*_y2</code>
+serve a dual use.
+They are used to
+1) compute the support points at <code>*_x1</code> and <code>*_x2</code>,
+which should not depend on <code>m_flow</code> or <code>dp</code> and
+2) to compute the flow functions when outside of this regime,
+which does depend on <code>m_flow</code> or <code>dp</code>.
+Min and max functions are therefore used such that one equation
+can serve both puroposes.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- August 7, 2020, by Ettore Zanetti:<br/>
- changed the computation of <code>phi</code> using
- <code>max(0.1*l, . )</code> to avoid
- phi=0.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
- issue 1376</a>.
- </li>
- <li>
- November 9, 2019, by Filip Jorissen:<br/>
- Guarded the computation of <code>phi</code> using
- <code>max(0, . )</code> to avoid
- negative phi.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
- issue 1223</a>.
- </li>
- <li>
- October 25, 2019, by Jianjun Hu:<br/>
- Removed icon graphics annotation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
- </li>
- <li>
- April 14, 2017, by Filip Jorissen:<br/>
- Revised implementation using <code>cubicHermite</code>
- such that it does not have a local maximum
- and such that it is C2-continuous.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/156\">#156</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- January 29, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+August 7, 2020, by Ettore Zanetti:<br/>
+changed the computation of <code>phi</code> using
+<code>max(0.1*l, . )</code> to avoid
+phi=0.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
+issue 1376</a>.
+</li>
+<li>
+November 9, 2019, by Filip Jorissen:<br/>
+Guarded the computation of <code>phi</code> using
+<code>max(0, . )</code> to avoid
+negative phi.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
+issue 1223</a>.
+</li>
+<li>
+October 25, 2019, by Jianjun Hu:<br/>
+Removed icon graphics annotation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
+</li>
+<li>
+April 14, 2017, by Filip Jorissen:<br/>
+Revised implementation using <code>cubicHermite</code>
+such that it does not have a local maximum
+and such that it is C2-continuous.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/156\">#156</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredInput</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+January 29, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayPressureIndependent;
diff --git a/AixLib/Fluid/Actuators/Valves/TwoWayQuickOpening.mo b/AixLib/Fluid/Actuators/Valves/TwoWayQuickOpening.mo
index 77e5a72a15..befd2918ea 100644
--- a/AixLib/Fluid/Actuators/Valves/TwoWayQuickOpening.mo
+++ b/AixLib/Fluid/Actuators/Valves/TwoWayQuickOpening.mo
@@ -25,71 +25,71 @@ initial equation
 annotation (
 defaultComponentName="val",
 Documentation(info="<html>
- <p>
- Two way valve with a power function for the valve opening characteristic.
- Valves that need to open quickly typically have such a valve characteristics.
- </p><p>
- This model is based on the partial valve model
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
- Check this model for more information, such
- as the regularization near the origin.
- </p>
- </html>",
+<p>
+Two way valve with a power function for the valve opening characteristic.
+Valves that need to open quickly typically have such a valve characteristics.
+</p><p>
+This model is based on the partial valve model
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
+Check this model for more information, such
+as the regularization near the origin.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- August 7, 2020, by Ettore Zanetti:<br/>
- changed the computation of <code>phi</code> using
- <code>max(0.1*l, . )</code> to avoid
- phi=0.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
- issue 1376</a>.
- </li>
- <li>
- November 9, 2019, by Filip Jorissen:<br/>
- Guarded the computation of <code>phi</code> using
- <code>max(0, . )</code> to avoid
- negative phi.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
- issue 1223</a>.
- </li>
- <li>
- April 4, 2014, by Michael Wetter:<br/>
- Moved the assignment of the flow function <code>phi</code>
- to the model instantiation because in its base class,
- the keyword <code>input</code>
- has been added to the variable <code>phi</code>.
- </li>
- <li>
- March 27, 2014 by Michael Wetter:<br/>
- Revised model for implementation of new valve model that computes the flow function
- based on a table.
- </li>
- <li>
- February 20, 2012 by Michael Wetter:<br/>
- Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
- and added new parameter <code>dpFixed_nominal=0</code>.
- See
- <a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
- AixLib.Fluid.Actuators.UsersGuide</a>.
- </li>
- <li>
- March 25, 2011, by Michael Wetter:<br/>
- Added homotopy method.
- </li>
- <li>
- June 3, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+August 7, 2020, by Ettore Zanetti:<br/>
+changed the computation of <code>phi</code> using
+<code>max(0.1*l, . )</code> to avoid
+phi=0.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
+issue 1376</a>.
+</li>
+<li>
+November 9, 2019, by Filip Jorissen:<br/>
+Guarded the computation of <code>phi</code> using
+<code>max(0, . )</code> to avoid
+negative phi.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
+issue 1223</a>.
+</li>
+<li>
+April 4, 2014, by Michael Wetter:<br/>
+Moved the assignment of the flow function <code>phi</code>
+to the model instantiation because in its base class,
+the keyword <code>input</code>
+has been added to the variable <code>phi</code>.
+</li>
+<li>
+March 27, 2014 by Michael Wetter:<br/>
+Revised model for implementation of new valve model that computes the flow function
+based on a table.
+</li>
+<li>
+February 20, 2012 by Michael Wetter:<br/>
+Renamed parameter <code>dp_nominal</code> to <code>dpValve_nominal</code>,
+and added new parameter <code>dpFixed_nominal=0</code>.
+See
+<a href=\"modelica://AixLib.Fluid.Actuators.UsersGuide\">
+AixLib.Fluid.Actuators.UsersGuide</a>.
+</li>
+<li>
+March 25, 2011, by Michael Wetter:<br/>
+Added homotopy method.
+</li>
+<li>
+June 3, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayQuickOpening;
diff --git a/AixLib/Fluid/Actuators/Valves/TwoWayTable.mo b/AixLib/Fluid/Actuators/Valves/TwoWayTable.mo
index 5796879999..319ca65b70 100644
--- a/AixLib/Fluid/Actuators/Valves/TwoWayTable.mo
+++ b/AixLib/Fluid/Actuators/Valves/TwoWayTable.mo
@@ -17,6 +17,7 @@ protected
         1,
         {max(flowCharacteristics.phi[1], 1E-8)},
         {flowCharacteristics.phi[i] for i in 2:size(flowCharacteristics.phi, 1)})],
+
     final columns=2:2,
     final smoothness=Modelica.Blocks.Types.Smoothness.ContinuousDerivative)
     "Normalized mass flow rate for the given valve position under the assumption of a constant pressure"
@@ -32,15 +33,15 @@ initial equation
     Modelica.Constants.eps,
     "flowCharateristics.phi[end] must be 1.");
 
-  // Assert that the sequences are strictly monotonic increasing
+  // Assert that the sequences are strictly increasing
   assert(AixLib.Utilities.Math.Functions.isMonotonic(
            x=flowCharacteristics.y,
            strict=true),
-         "The values for y in flowCharacteristics must be strictly monotone increasing.");
+         "The values for y in flowCharacteristics must be strictly increasing.");
   assert(AixLib.Utilities.Math.Functions.isMonotonic(
            x=flowCharacteristics.phi,
            strict=true),
-         "The values for phi in flowCharacteristics must be strictly monotone increasing.");
+         "The values for phi in flowCharacteristics must be strictly increasing.");
 
 equation
   connect(phiLooUp.u[1], y_actual) annotation (Line(
@@ -49,133 +50,133 @@ equation
   annotation (
     defaultComponentName="val",
     Documentation(info="<html>
- <p>
- Two way valve with opening characteristic that is configured through
- a table.
- </p>
- <p>
- The mass flow rate for the fully open valve is determined based
- on the value of the parameter <code>CvData</code>.
- For the different valve positions <i>y &isin; [0, 1]</i>, this nominal flow rate is
- scaled by the values of the parameter
- <code>flowCharacteristics</code>.
- The parameter <code>flowCharacteristics</code> declares a table of the form
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <tr>
- <td><i>y</i></td>  <td>0</td>  <td>...</td>  <td>1</td>
- </tr>
- <tr>
- <td><i>&phi;</i></td>  <td><i>l</i></td>  <td>...</td>  <td>1</td>
- </tr>
- </table>
- <p>
- where <i>l = K<sub>v</sub>(y=0)/K<sub>v</sub>(y=1) &gt; 0</i> is the valve leakage.
- The first row is the valve opening, and the second row is the
- mass flow rate, relative to the mass flow rate of the fully open
- valve, under the assumption of a constant pressure difference across the
- valve.
- A suggested value for the valve leakage is <i>l=0.0001</i>.
- If <i>l = 0</i>, then this model will replace it with
- <i>l = 10<sup>-8</sup></i> for numerical reasons.
- For example, if a valve has <i>K<sub>v</sub>=0.5</i> [m<sup>3</sup>/h/bar<sup>1/2</sup>] and
- a linear opening characteristics and
- a valve leakage of <i>l=0.0001</i>, then one would set
- </p>
- <pre>
-  CvData=AixLib.Fluid.Types.CvTypes.Kv
-  Kv = 0.5
-  flowCharacteristics(y={0,1}, phi={0.0001,1})
-  </pre>
- <p>
- Note, however, that
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayLinear\">
- AixLib.Fluid.Actuators.Valves.TwoWayLinear</a> provides a more
- efficient implementation for this simple case.
- </p>
- <p>
- The parameter <code>flowCharacteristics</code> must meet the following
- requirements, otherwise the model stops with an error:
- </p>
- <ul>
- <li>
- Their arrays
- <code>y</code> and <code>phi</code>
- must be strictly monotonic increasing.
- </li>
- <li>
- The first value must satisfy
- <code>y[1]=0</code>, and
- <code>phi[1]</code> must be equal to the
- leakage flow rate, which must be bigger than zero.
- Otherwise, a default value of <code>1E-8</code> is used.
- </li>
- <li>
- The last values must satisfy
- <code>y[end]=1</code> and
- <code>phi[end]=1</code>.
- </li>
- </ul>
- <p>
- This model is based on the partial valve model
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
- Check this model for more information, such
- as the regularization near the origin.
- </p>
- <p>
- For an example that specifies an opening characteristics, see
- <a href=\"modelica://AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable\">
- AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 10, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter and changed the parameter <code>order</code> to a constant
- as most users need not change this value.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- August 7, 2020, by Ettore Zanetti:<br/>
- changed the computation of <code>phi</code> using
- <code>max(0.1*l, . )</code> to avoid
- phi=0.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
- issue 1376</a>.
- </li>
- <li>
- November 9, 2019, by Filip Jorissen:<br/>
- Guarded the computation of <code>phi</code> using
- <code>max(0, . )</code> to avoid
- negative phi.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
- issue 1223</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Removed equality comparison for <code>Real</code> in the
- <code>assert</code> statements as this is not allowed in Modelica.
- </li>
- <li>
- August 12, 2014, by Michael Wetter:<br/>
- Removed the <code>end</code> keyword when accessing array elements,
- as this language construct caused an error in OpenModelica.
- </li>
- <li>
- April 4, 2014, by Michael Wetter:<br/>
- Moved the assignment of the flow function <code>phi</code>
- to the model instantiation because in its base class,
- the keyword <code>input</code>
- has been added to the variable <code>phi</code>.
- </li>
- <li>
- March 26, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Two way valve with opening characteristic that is configured through
+a table.
+</p>
+<p>
+The mass flow rate for the fully open valve is determined based
+on the value of the parameter <code>CvData</code>.
+For the different valve positions <i>y &isin; [0, 1]</i>, this nominal flow rate is
+scaled by the values of the parameter
+<code>flowCharacteristics</code>.
+The parameter <code>flowCharacteristics</code> declares a table of the form
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<td><i>y</i></td>  <td>0</td>  <td>...</td>  <td>1</td>
+</tr>
+<tr>
+<td><i>&phi;</i></td>  <td><i>l</i></td>  <td>...</td>  <td>1</td>
+</tr>
+</table>
+<p>
+where <i>l = K<sub>v</sub>(y=0)/K<sub>v</sub>(y=1) &gt; 0</i> is the valve leakage.
+The first row is the valve opening, and the second row is the
+mass flow rate, relative to the mass flow rate of the fully open
+valve, under the assumption of a constant pressure difference across the
+valve.
+A suggested value for the valve leakage is <i>l=0.0001</i>.
+If <i>l = 0</i>, then this model will replace it with
+<i>l = 10<sup>-8</sup></i> for numerical reasons.
+For example, if a valve has <i>K<sub>v</sub>=0.5</i> [m<sup>3</sup>/h/bar<sup>1/2</sup>] and
+a linear opening characteristics and
+a valve leakage of <i>l=0.0001</i>, then one would set
+</p>
+<pre>
+ CvData=AixLib.Fluid.Types.CvTypes.Kv
+ Kv = 0.5
+ flowCharacteristics(y={0,1}, phi={0.0001,1})
+ </pre>
+<p>
+Note, however, that
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.TwoWayLinear\">
+AixLib.Fluid.Actuators.Valves.TwoWayLinear</a> provides a more
+efficient implementation for this simple case.
+</p>
+<p>
+The parameter <code>flowCharacteristics</code> must meet the following
+requirements, otherwise the model stops with an error:
+</p>
+<ul>
+<li>
+Their arrays
+<code>y</code> and <code>phi</code>
+must be strictly increasing.
+</li>
+<li>
+The first value must satisfy
+<code>y[1]=0</code>, and
+<code>phi[1]</code> must be equal to the
+leakage flow rate, which must be bigger than zero.
+Otherwise, a default value of <code>1E-8</code> is used.
+</li>
+<li>
+The last values must satisfy
+<code>y[end]=1</code> and
+<code>phi[end]=1</code>.
+</li>
+</ul>
+<p>
+This model is based on the partial valve model
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</a>.
+Check this model for more information, such
+as the regularization near the origin.
+</p>
+<p>
+For an example that specifies an opening characteristics, see
+<a href=\"modelica://AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable\">
+AixLib.Fluid.Actuators.Valves.Examples.TwoWayValveTable</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 10, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter and changed the parameter <code>order</code> to a constant
+as most users need not change this value.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+August 7, 2020, by Ettore Zanetti:<br/>
+changed the computation of <code>phi</code> using
+<code>max(0.1*l, . )</code> to avoid
+phi=0.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1376\">
+issue 1376</a>.
+</li>
+<li>
+November 9, 2019, by Filip Jorissen:<br/>
+Guarded the computation of <code>phi</code> using
+<code>max(0, . )</code> to avoid
+negative phi.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1223\">
+issue 1223</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Removed equality comparison for <code>Real</code> in the
+<code>assert</code> statements as this is not allowed in Modelica.
+</li>
+<li>
+August 12, 2014, by Michael Wetter:<br/>
+Removed the <code>end</code> keyword when accessing array elements,
+as this language construct caused an error in OpenModelica.
+</li>
+<li>
+April 4, 2014, by Michael Wetter:<br/>
+Moved the assignment of the flow function <code>phi</code>
+to the model instantiation because in its base class,
+the keyword <code>input</code>
+has been added to the variable <code>phi</code>.
+</li>
+<li>
+March 26, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={
         Rectangle(
@@ -190,6 +191,6 @@ equation
         Line(
           points={{-56,-74},{-56,-96}}),
         Line(
-          points={{-68,-82},{-44,-82}})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          points={{-68,-82},{-44,-82}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayTable;
diff --git a/AixLib/Fluid/Actuators/Valves/Validation/ThreeWayValveParameterization.mo b/AixLib/Fluid/Actuators/Valves/Validation/ThreeWayValveParameterization.mo
index 29e698baed..06fabc83c0 100644
--- a/AixLib/Fluid/Actuators/Valves/Validation/ThreeWayValveParameterization.mo
+++ b/AixLib/Fluid/Actuators/Valves/Validation/ThreeWayValveParameterization.mo
@@ -154,18 +154,18 @@ equation
         "Simulate and plot"),
     Diagram(coordinateSystem(extent={{-100,-140},{140,140}})),
     Documentation(info="<html>
- <p>
- This model test the parameterization of three-way valves.
- All valves are sized equally, but use different configuration options.
- Therefore, the valves have all the same mass flow rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model test the parameterization of three-way valves.
+All valves are sized equally, but use different configuration options.
+Therefore, the valves have all the same mass flow rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeWayValveParameterization;
diff --git a/AixLib/Fluid/Actuators/Valves/Validation/TwoWayValveParameterization.mo b/AixLib/Fluid/Actuators/Valves/Validation/TwoWayValveParameterization.mo
index 22c4390228..653bd7c5f3 100644
--- a/AixLib/Fluid/Actuators/Valves/Validation/TwoWayValveParameterization.mo
+++ b/AixLib/Fluid/Actuators/Valves/Validation/TwoWayValveParameterization.mo
@@ -136,34 +136,34 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Actuators/Valves/Validation/TwoWayValveParameterization.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Test model for two way valves. This model tests the
- different parameterization of the valve model.
- All valves have the same mass flow rates.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2017, by Michael Wetter:<br/>
- Removed assertion blocks, exposed common parameters,
- and added a valve that uses <code>Av</code> as the parameter.
- </li>
- <li>
- April 1, 2013, by Michael Wetter:<br/>
- Removed the valve from <code>Modelica.Fluid</code> to allow a successful check
- of the model in the pedantic mode in Dymola 2014.
- </li>
- <li>
- March 1, 2013, by Michael Wetter:<br/>
- Removed assignment of <code>dpValve_nominal</code> if
- <code>CvData &lt;&gt; AixLib.Fluid.Types.CvTypes.OpPoint</code>,
- as in this case, it is computed by the model.
- </li>
- <li>
- February 18, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for two way valves. This model tests the
+different parameterization of the valve model.
+All valves have the same mass flow rates.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2017, by Michael Wetter:<br/>
+Removed assertion blocks, exposed common parameters,
+and added a valve that uses <code>Av</code> as the parameter.
+</li>
+<li>
+April 1, 2013, by Michael Wetter:<br/>
+Removed the valve from <code>Modelica.Fluid</code> to allow a successful check
+of the model in the pedantic mode in Dymola 2014.
+</li>
+<li>
+March 1, 2013, by Michael Wetter:<br/>
+Removed assignment of <code>dpValve_nominal</code> if
+<code>CvData &lt;&gt; AixLib.Fluid.Types.CvTypes.OpPoint</code>,
+as in this case, it is computed by the model.
+</li>
+<li>
+February 18, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoWayValveParameterization;
diff --git a/AixLib/Fluid/BaseClasses/ActuatorFilter.mo b/AixLib/Fluid/BaseClasses/ActuatorFilter.mo
index 9038be7785..e35b7918b1 100644
--- a/AixLib/Fluid/BaseClasses/ActuatorFilter.mo
+++ b/AixLib/Fluid/BaseClasses/ActuatorFilter.mo
@@ -83,28 +83,28 @@ equation
     Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{
             100,100}})),
     Documentation(info="<html>
- <p>
- This block implements a filter that is used to approximate the actuators
- of valves, dampers and fans.
- </p>
- <h4>Implementation</h4>
- <p>
- The implementation is based on
- <a href=\"modelica://Modelica.Blocks.Continuous.CriticalDamping\">
- Modelica.Blocks.Continuous.CriticalDamping</a>.
- It differs from that model in that the internal state of the filter <code>s</code>
- is transformed using <code>x = u_nominal*s</code>.
- It turns out that this transformation leads to smaller system of nonlinear equations if <code>u_nominal &ne; 0</code>, see
- <a href=\"https://https://github.com/ibpsa/modelica-ibpsa/issues/1498#issuecomment-885020611\">IBPSA, #1498</a>
- for a discussion.
- </html>",revisions="<html>
- <ul>
- <li>
- July 22, 2021, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://https://github.com/ibpsa/modelica-ibpsa/issues/1498\">IBPSA, #1498</a>
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This block implements a filter that is used to approximate the actuators
+of valves, dampers and fans.
+</p>
+<h4>Implementation</h4>
+<p>
+The implementation is based on
+<a href=\"modelica://Modelica.Blocks.Continuous.CriticalDamping\">
+Modelica.Blocks.Continuous.CriticalDamping</a>.
+It differs from that model in that the internal state of the filter <code>s</code>
+is transformed using <code>x = u_nominal*s</code>.
+It turns out that this transformation leads to smaller system of nonlinear equations if <code>u_nominal &ne; 0</code>, see
+<a href=\"https://https://github.com/ibpsa/modelica-ibpsa/issues/1498#issuecomment-885020611\">IBPSA, #1498</a>
+for a discussion.
+</html>", revisions="<html>
+<ul>
+<li>
+July 22, 2021, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://https://github.com/ibpsa/modelica-ibpsa/issues/1498\">IBPSA, #1498</a>
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ActuatorFilter;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck.mo b/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck.mo
index 54eeb1809c..cfcaf4d96b 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck.mo
@@ -31,29 +31,29 @@ experiment(
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model validates the implementation of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
- and its first order derivative
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der</a>.
- If the derivative implementation is wrong, the simulation will stop with an error.
- </p>
- </html>",
+<p>
+This model validates the implementation of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
+and its first order derivative
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der</a>.
+If the derivative implementation is wrong, the simulation will stop with an error.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 29, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 29, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BasicFlowFunction_dp_DerivativeCheck;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck2.mo b/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck2.mo
index cc59dc8ccc..f0eaf53236 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck2.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck2.mo
@@ -47,38 +47,38 @@ experiment(
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_dp_DerivativeCheck2.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model validates the implementation of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
- and its second order derivative
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2</a>.
- If the derivative implementation is wrong, the simulation will stop with an error.
- </p>
- <h4>Implementation</h4>
- <p>
- The pressure drop <code>dp</code> is increased non-linearly in order
- for the first and second derivatives in
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2</a>
- to be non-zero during part of the simulation. This will ensure
- full code coverage of this function.
- </p>
- </html>",
+<p>
+This model validates the implementation of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
+and its second order derivative
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2</a>.
+If the derivative implementation is wrong, the simulation will stop with an error.
+</p>
+<h4>Implementation</h4>
+<p>
+The pressure drop <code>dp</code> is increased non-linearly in order
+for the first and second derivatives in
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2</a>
+to be non-zero during part of the simulation. This will ensure
+full code coverage of this function.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 29, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 29, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BasicFlowFunction_dp_DerivativeCheck2;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck.mo b/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck.mo
index bcd615f015..764f93d60e 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck.mo
@@ -30,29 +30,29 @@ experiment(StartTime=-2,
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model validates the implementation of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
- and its first order derivative
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der</a>.
- If the derivative implementation is wrong, the simulation will stop with an error.
- </p>
- </html>",
+<p>
+This model validates the implementation of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
+and its first order derivative
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der</a>.
+If the derivative implementation is wrong, the simulation will stop with an error.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 29, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 29, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BasicFlowFunction_m_flow_DerivativeCheck;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck2.mo b/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck2.mo
index 140edc23f7..58bc66e3aa 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck2.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck2.mo
@@ -57,32 +57,32 @@ experiment(
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/FlowModels/Validation/BasicFlowFunction_m_flow_DerivativeCheck2.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model validates the implementation of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
- and its second order derivative
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2</a>.
- If the derivative implementation is wrong, the simulation will stop with an error.
- </p>
- <h4>Implementation</h4>
- <p>
- The mass flow rate <code>m_flow</code> is increased non-linearly in order
- for the first and second derivatives in
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2</a>
- to be non-zero during part of the simulation. This will ensure
- full code coverage of this function.
- </p>
- </html>",
+<p>
+This model validates the implementation of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
+and its second order derivative
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2</a>.
+If the derivative implementation is wrong, the simulation will stop with an error.
+</p>
+<h4>Implementation</h4>
+<p>
+The mass flow rate <code>m_flow</code> is increased non-linearly in order
+for the first and second derivatives in
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2</a>
+to be non-zero during part of the simulation. This will ensure
+full code coverage of this function.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 29, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 29, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BasicFlowFunction_m_flow_DerivativeCheck2;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/Validation/InverseFlowFunctions.mo b/AixLib/Fluid/BaseClasses/FlowModels/Validation/InverseFlowFunctions.mo
index 473356713a..ad02cb0668 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/Validation/InverseFlowFunctions.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/Validation/InverseFlowFunctions.mo
@@ -21,35 +21,35 @@ experiment(Tolerance=1e-06, StopTime=1),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/FlowModels/Validation/InverseFlowFunctions.mos"
         "Simulate and plot"),
               Documentation(info="<html>
- <p>
- This model tests the inverse formulation of the flow functions.
- The pressure difference <code>dp</code> and <code>dpCalc</code> need to
- be equal up to the solver tolerance, except for a small neighborhood
- around the origin. In this neighborhood around the origin, the functions
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
- and
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
- are not invertible.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- August 8, 2012, by Michael Wetter:<br/>
- Updated documentation.
- </li>
- <li>
- July 12, 2012, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the inverse formulation of the flow functions.
+The pressure difference <code>dp</code> and <code>dpCalc</code> need to
+be equal up to the solver tolerance, except for a small neighborhood
+around the origin. In this neighborhood around the origin, the functions
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
+and
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
+are not invertible.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+August 8, 2012, by Michael Wetter:<br/>
+Updated documentation.
+</li>
+<li>
+July 12, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InverseFlowFunctions;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_dp.mo b/AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_dp.mo
index c24743dfab..8e7146d5c9 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_dp.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_dp.mo
@@ -19,35 +19,35 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_dp.mos"
         "Simulate and plot"),
               Documentation(info="<html>
- <p>
- This model tests whether the Modelica translator substitutes the
- inverse function for
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>.
- Specifically, this function declares in its <code>annotation</code> section
- that its inverse is provided by
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>.
- Translating this model should therefore give no nonlinear equations
- after the symbolic manipulation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 25, 2019, by Michael Wetter:<br/>
- Added start value to avoid warning in JModelica.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- August 5, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the Modelica translator substitutes the
+inverse function for
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>.
+Specifically, this function declares in its <code>annotation</code> section
+that its inverse is provided by
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>.
+Translating this model should therefore give no nonlinear equations
+after the symbolic manipulation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 25, 2019, by Michael Wetter:<br/>
+Added start value to avoid warning in JModelica.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+August 5, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InvertingBasicFlowFunction_dp;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_m_flow.mo b/AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_m_flow.mo
index cf694edc28..5d0d17404d 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_m_flow.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_m_flow.mo
@@ -19,35 +19,35 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/FlowModels/Validation/InvertingBasicFlowFunction_m_flow.mos"
         "Simulate and plot"),
               Documentation(info="<html>
- <p>
- This model tests whether the Modelica translator substitutes the
- inverse function for
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>.
- Specifically, this function declares in its <code>annotation</code> section
- that its inverse is provided by
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>.
- Translating this model should therefore give no nonlinear equations
- after the symbolic manipulation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 25, 2019, by Michael Wetter:<br/>
- Added start value to avoid warning in JModelica.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- August 5, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the Modelica translator substitutes the
+inverse function for
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>.
+Specifically, this function declares in its <code>annotation</code> section
+that its inverse is provided by
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>.
+Translating this model should therefore give no nonlinear equations
+after the symbolic manipulation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 25, 2019, by Michael Wetter:<br/>
+Added start value to avoid warning in JModelica.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+August 5, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InvertingBasicFlowFunction_m_flow;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp.mo b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp.mo
index efb6779b42..e3d7eb98f5 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp.mo
@@ -38,97 +38,97 @@ algorithm
           fillColor={232,0,0},
           textString="%name")}),
 Documentation(info="<html>
- <p>
- Function that computes the pressure drop of flow elements as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   m = sign(&Delta;p) k  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
- </p>
- <p>
- with regularization near the origin.
- Therefore, the flow coefficient is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   k = m &frasl; &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
- </p>
- <p>
- The input <code>m_flow_turbulent</code> determines the location of the regularization.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 9, 2019, by Filip Jorissen:<br/>
- Added <code>smooth(2, . )</code> for avoiding
- a warning in the check valve model.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1240\">#1240</a>.
- </li>
- <li>
- January 4, 2019, by Michael Wetter:<br/>
- Set `Inline=false`.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
- </li>
- <li>
- May 1, 2017, by Filip Jorissen:<br/>
- Revised implementation such that
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">basicFlowFunction_dp</a>
- is C2 continuous.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
- </li>
- <li>
- March 19, 2016, by Michael Wetter:<br/>
- Added <code>abs</code> function for
- <code>AixLib.Fluid.FixedResistances.Validation.PressureDropsExplicit</code>
- to work in OpenModelica.
- See <a href=\"https://trac.openmodelica.org/OpenModelica/ticket/3778\">
- OpenModelica ticket 3778</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 28, 2015, by Michael Wetter:<br/>
- Removed double declaration of <code>smooth(..)</code> and <code>smoothOrder</code>
- and changed <code>Inline=true</code> to <code>LateInline=true</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/301\">issue 301</a>.
- </li>
- <li>
- July 15, 2015, by Filip Jorissen:<br/>
- New, more efficient implementation based on regularisation using simple polynomial.
- Expanded common subexpressions for function inlining to be possible.
- Set <code>Inline=true</code> for inlining to occur.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/279\">#279</a>.
- </li>
- <li>
- January 9, 2014, by Michael Wetter:<br/>
- Correct revision section, of which there were two.
- </li>
- <li>
- August 10, 2011, by Michael Wetter:<br/>
- Removed <code>if-then</code> optimization that set <code>m_flow=0</code> if <code>dp=0</code>,
- as this causes the derivative to be discontinuous at <code>dp=0</code>.
- </li>
- <li>
- August 4, 2011, by Michael Wetter:<br/>
- Removed option to use a linear function. The linear implementation is now done
- in models that call this function. With the previous implementation,
- the symbolic processor may not rearrange the equations, which can lead
- to coupled equations instead of an explicit solution.
- </li>
- <li>
- March 29, 2010 by Michael Wetter:<br/>
- Changed implementation to allow <code>k=0</code>, which is
- the case for a closed valve with no leakage
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that computes the pressure drop of flow elements as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  m&#775; = sign(&Delta;p) k  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
+</p>
+<p>
+with regularization near the origin.
+Therefore, the flow coefficient is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  k = m&#775; &frasl; &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
+</p>
+<p>
+The input <code>m_flow_turbulent</code> determines the location of the regularization.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 9, 2019, by Filip Jorissen:<br/>
+Added <code>smooth(2, . )</code> for avoiding
+a warning in the check valve model.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1240\">#1240</a>.
+</li>
+<li>
+January 4, 2019, by Michael Wetter:<br/>
+Set `Inline=false`.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
+</li>
+<li>
+May 1, 2017, by Filip Jorissen:<br/>
+Revised implementation such that
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">basicFlowFunction_dp</a>
+is C2 continuous.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
+</li>
+<li>
+March 19, 2016, by Michael Wetter:<br/>
+Added <code>abs</code> function for
+<code>AixLib.Fluid.FixedResistances.Validation.PressureDropsExplicit</code>
+to work in OpenModelica.
+See <a href=\"https://trac.openmodelica.org/OpenModelica/ticket/3778\">
+OpenModelica ticket 3778</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 28, 2015, by Michael Wetter:<br/>
+Removed double declaration of <code>smooth(..)</code> and <code>smoothOrder</code>
+and changed <code>Inline=true</code> to <code>LateInline=true</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/301\">issue 301</a>.
+</li>
+<li>
+July 15, 2015, by Filip Jorissen:<br/>
+New, more efficient implementation based on regularisation using simple polynomial.
+Expanded common subexpressions for function inlining to be possible.
+Set <code>Inline=true</code> for inlining to occur.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/279\">#279</a>.
+</li>
+<li>
+January 9, 2014, by Michael Wetter:<br/>
+Correct revision section, of which there were two.
+</li>
+<li>
+August 10, 2011, by Michael Wetter:<br/>
+Removed <code>if-then</code> optimization that set <code>m_flow=0</code> if <code>dp=0</code>,
+as this causes the derivative to be discontinuous at <code>dp=0</code>.
+</li>
+<li>
+August 4, 2011, by Michael Wetter:<br/>
+Removed option to use a linear function. The linear implementation is now done
+in models that call this function. With the previous implementation,
+the symbolic processor may not rearrange the equations, which can lead
+to coupled equations instead of an explicit solution.
+</li>
+<li>
+March 29, 2010 by Michael Wetter:<br/>
+Changed implementation to allow <code>k=0</code>, which is
+the case for a closed valve with no leakage
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end basicFlowFunction_dp;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der.mo b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der.mo
index c807a7ce5b..82f49de967 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der.mo
@@ -27,47 +27,47 @@ algorithm
              derivative(order=2, zeroDerivative=k, zeroDerivative=m_flow_turbulent)=
                AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp_der2,
 Documentation(info="<html>
- <p>
- Function that implements the first order derivative of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
- with respect to the mass flow rate.
- </p>
- </html>",
+<p>
+Function that implements the first order derivative of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
+with respect to the mass flow rate.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 4, 2019, by Michael Wetter:<br/>
- Set `Inline=false`.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
- </li>
- <li>
- May 1, 2017, by Filip Jorissen:<br/>
- Revised implementation such that
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
- is C2 continuous.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
- </li>
- <li>
- April 14, 2017, by Filip Jorissen:<br/>
- Changed implementation such that it cannot lead to square roots
- of negative numbers and reduced the number of required operations.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/723\">#723</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 29, 2015, by Michael Wetter:<br/>
- First implementation to avoid in Dymola 2016 the warning
- \"Differentiating ... under the assumption that it is continuous at switching\".
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 4, 2019, by Michael Wetter:<br/>
+Set `Inline=false`.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
+</li>
+<li>
+May 1, 2017, by Filip Jorissen:<br/>
+Revised implementation such that
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
+is C2 continuous.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
+</li>
+<li>
+April 14, 2017, by Filip Jorissen:<br/>
+Changed implementation such that it cannot lead to square roots
+of negative numbers and reduced the number of required operations.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/723\">#723</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 29, 2015, by Michael Wetter:<br/>
+First implementation to avoid in Dymola 2016 the warning
+\"Differentiating ... under the assumption that it is continuous at switching\".
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end basicFlowFunction_dp_der;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der2.mo b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der2.mo
index d645bc9db9..f91f59d4ee 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der2.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_dp_der2.mo
@@ -32,40 +32,40 @@ algorithm
  annotation (smoothOrder=0,
  Inline=false,
 Documentation(info="<html>
- <p>
- Function that implements the second order derivative of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
- with respect to the mass flow rate.
- </p>
- </html>",
+<p>
+Function that implements the second order derivative of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
+with respect to the mass flow rate.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 4, 2019, by Michael Wetter:<br/>
- Set `Inline=false`.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
- </li>
- <li>
- May 1, 2017, by Filip Jorissen:<br/>
- Revised implementation such that
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
- is C2 continuous.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 29, 2015, by Michael Wetter:<br/>
- First implementation to avoid in Dymola 2016 the warning
- \"Differentiating ... under the assumption that it is continuous at switching\".
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 4, 2019, by Michael Wetter:<br/>
+Set `Inline=false`.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
+</li>
+<li>
+May 1, 2017, by Filip Jorissen:<br/>
+Revised implementation such that
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
+is C2 continuous.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 29, 2015, by Michael Wetter:<br/>
+First implementation to avoid in Dymola 2016 the warning
+\"Differentiating ... under the assumption that it is continuous at switching\".
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end basicFlowFunction_dp_der2;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow.mo b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow.mo
index 92e626ae66..d1d072b436 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow.mo
@@ -40,83 +40,83 @@ algorithm
           fillColor={232,0,0},
           textString="%name")}),
 Documentation(info="<html>
- <p>
- Function that computes the pressure drop of flow elements as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &Delta;p = sign(m) (m &frasl; k)<sup>2</sup>
- </p>
- <p>
- with regularization near the origin.
- Therefore, the flow coefficient is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   k = m &frasl; &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
- </p>
- <p>
- The input <code>m_flow_turbulent</code> determines the location of the regularization.
- </p>
- </html>",
+<p>
+Function that computes the pressure drop of flow elements as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &Delta;p = sign(m&#775;) (m&#775; &frasl; k)<sup>2</sup>
+</p>
+<p>
+with regularization near the origin.
+Therefore, the flow coefficient is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  k = m&#775; &frasl; &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
+</p>
+<p>
+The input <code>m_flow_turbulent</code> determines the location of the regularization.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 9, 2019, by Michael Wetter:<br/>
- Added <code>smooth(2, . )</code>, similar to
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1240\">#1240</a>.
- </li>
- <li>
- January 4, 2019, by Michael Wetter:<br/>
- Set `Inline=false`.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
- </li>
- <li>
- May 1, 2017, by Filip Jorissen:<br/>
- Revised implementation such that
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
- is C2 continuous.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 28, 2015, by Michael Wetter:<br/>
- Removed double declaration of <code>smooth(..)</code> and <code>smoothOrder</code>
- and changed <code>Inline=true</code> to <code>LateInline=true</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/301\">issue 301</a>.
- </li>
- <li>
- July 15, 2015, by Filip Jorissen:<br/>
- New, more efficient implementation based on regularisation using simple polynomial.
- Expanded common subexpressions for function inlining to be possible.
- Set <code>Inline=true</code> for inlining to occur.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/279\">#279</a>.
- </li>
- <li>
- August 10, 2011, by Michael Wetter:<br/>
- Removed <code>if-then</code> optimization that set <code>dp=0</code> if <code>m_flow=0</code>,
- as this causes the derivative to be discontinuous at <code>m_flow=0</code>.
- </li>
- <li>
- August 4, 2011, by Michael Wetter:<br/>
- Removed option to use a linear function. The linear implementation is now done
- in models that call this function. With the previous implementation,
- the symbolic processor may not rearrange the equations, which can lead
- to coupled equations instead of an explicit solution.
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 9, 2019, by Michael Wetter:<br/>
+Added <code>smooth(2, . )</code>, similar to
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1240\">#1240</a>.
+</li>
+<li>
+January 4, 2019, by Michael Wetter:<br/>
+Set `Inline=false`.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
+</li>
+<li>
+May 1, 2017, by Filip Jorissen:<br/>
+Revised implementation such that
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
+is C2 continuous.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 28, 2015, by Michael Wetter:<br/>
+Removed double declaration of <code>smooth(..)</code> and <code>smoothOrder</code>
+and changed <code>Inline=true</code> to <code>LateInline=true</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/301\">issue 301</a>.
+</li>
+<li>
+July 15, 2015, by Filip Jorissen:<br/>
+New, more efficient implementation based on regularisation using simple polynomial.
+Expanded common subexpressions for function inlining to be possible.
+Set <code>Inline=true</code> for inlining to occur.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/279\">#279</a>.
+</li>
+<li>
+August 10, 2011, by Michael Wetter:<br/>
+Removed <code>if-then</code> optimization that set <code>dp=0</code> if <code>m_flow=0</code>,
+as this causes the derivative to be discontinuous at <code>m_flow=0</code>.
+</li>
+<li>
+August 4, 2011, by Michael Wetter:<br/>
+Removed option to use a linear function. The linear implementation is now done
+in models that call this function. With the previous implementation,
+the symbolic processor may not rearrange the equations, which can lead
+to coupled equations instead of an explicit solution.
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end basicFlowFunction_m_flow;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der.mo b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der.mo
index 25a49c2fd1..adfc37926a 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der.mo
@@ -28,34 +28,34 @@ algorithm
              derivative(order=2, zeroDerivative=k, zeroDerivative=m_flow_turbulent)=
              AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow_der2,
 Documentation(info="<html>
- <p>
- Function that implements the first order derivative of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
- with respect to the mass flow rate.
- </p>
- </html>",
+<p>
+Function that implements the first order derivative of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
+with respect to the mass flow rate.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 4, 2019, by Michael Wetter:<br/>
- Set `Inline=false`.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
- </li>
- <li>
- May 1, 2017, by Filip Jorissen:<br/>
- Revised implementation such that
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
- is C2 continuous.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
- </li>
- <li>
- July 29, 2015, by Michael Wetter:<br/>
- First implementation to avoid in Dymola 2016 the warning
- \"Differentiating ... under the assumption that it is continuous at switching\".
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 4, 2019, by Michael Wetter:<br/>
+Set `Inline=false`.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
+</li>
+<li>
+May 1, 2017, by Filip Jorissen:<br/>
+Revised implementation such that
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
+is C2 continuous.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
+</li>
+<li>
+July 29, 2015, by Michael Wetter:<br/>
+First implementation to avoid in Dymola 2016 the warning
+\"Differentiating ... under the assumption that it is continuous at switching\".
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end basicFlowFunction_m_flow_der;
diff --git a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der2.mo b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der2.mo
index ed90259e91..99e9802d07 100644
--- a/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der2.mo
+++ b/AixLib/Fluid/BaseClasses/FlowModels/basicFlowFunction_m_flow_der2.mo
@@ -32,39 +32,39 @@ algorithm
  annotation (smoothOrder=0,
  Inline=false,
 Documentation(info="<html>
- <p>
- Function that implements the second order derivative of
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
- with respect to the mass flow rate.
- </p>
- </html>",
+<p>
+Function that implements the second order derivative of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_m_flow</a>
+with respect to the mass flow rate.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 4, 2019, by Michael Wetter:<br/>
- Set `Inline=false`.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
- </li>
- <li>
- May 1, 2017, by Filip Jorissen:<br/>
- Revised implementation such that
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
- AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
- is C2 continuous.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 29, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 4, 2019, by Michael Wetter:<br/>
+Set `Inline=false`.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1070\">#1070</a>.
+</li>
+<li>
+May 1, 2017, by Filip Jorissen:<br/>
+Revised implementation such that
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp\">
+AixLib.Fluid.BaseClasses.FlowModels.basicFlowFunction_dp</a>
+is C2 continuous.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/725\">#725</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 29, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end basicFlowFunction_m_flow_der2;
diff --git a/AixLib/Fluid/BaseClasses/IndexMassFraction.mo b/AixLib/Fluid/BaseClasses/IndexMassFraction.mo
index 058ff8440c..8450f2a8f2 100644
--- a/AixLib/Fluid/BaseClasses/IndexMassFraction.mo
+++ b/AixLib/Fluid/BaseClasses/IndexMassFraction.mo
@@ -20,37 +20,37 @@ initial equation
                   + "Change medium model to one that has '" + substanceName + "' as a substance.");
 
   annotation (Documentation(info="<html>
- <p>
- This block computes the index that the subtance with name
- <code>substanceName</code> has in the mass fraction vector <code>X</code>.
- If the medium model has no component called <code>substanceName</code>,
- then the block writes an error message and terminates the simulation.
- </p>
- <p>
- This block is used for example to obtain the index of the subtance 'water'
- to obtain the water vapor concentration, or to measure any other mass fraction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 14, 2019, by Michael Wetter:<br/>
- Rewrote assignment of <code>i_x</code> to avoid a variable array index.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1250\">#1250</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Revised the model and added the parameter <code>substanceName</code>.
- </li>
- <li>
- December 18, 2012, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This block computes the index that the subtance with name
+<code>substanceName</code> has in the mass fraction vector <code>X</code>.
+If the medium model has no component called <code>substanceName</code>,
+then the block writes an error message and terminates the simulation.
+</p>
+<p>
+This block is used for example to obtain the index of the subtance 'water'
+to obtain the water vapor concentration, or to measure any other mass fraction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 14, 2019, by Michael Wetter:<br/>
+Rewrote assignment of <code>i_x</code> to avoid a variable array index.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1250\">#1250</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Revised the model and added the parameter <code>substanceName</code>.
+</li>
+<li>
+December 18, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IndexMassFraction;
diff --git a/AixLib/Fluid/BaseClasses/MassFlowRateMultiplier.mo b/AixLib/Fluid/BaseClasses/MassFlowRateMultiplier.mo
index bd61a66549..f090cc7ec8 100644
--- a/AixLib/Fluid/BaseClasses/MassFlowRateMultiplier.mo
+++ b/AixLib/Fluid/BaseClasses/MassFlowRateMultiplier.mo
@@ -2,17 +2,55 @@ within AixLib.Fluid.BaseClasses;
 model MassFlowRateMultiplier "Model that multiplies the mass flow rate"
   extends AixLib.Fluid.Interfaces.PartialTwoPort;
 
-  parameter Real k "Gain for mass flow rate";
+  parameter Boolean use_input=false
+    "Set to true for multiplier factor provided as an input instead of a parameter"
+    annotation(Evaluate=true);
+  parameter Real k=1
+    "Gain for mass flow rate"
+    annotation(Dialog(enable=not use_input));
+
+  Modelica.Blocks.Interfaces.RealInput u(
+    final unit="1",
+    final min=Modelica.Constants.small) if use_input
+    "Multiplier factor"
+    annotation (Placement(transformation(extent={{-140,40},{-100,80}}),
+        iconTransformation(extent={{-140,40},{-100,80}})));
+  Modelica.Blocks.Interfaces.RealOutput uInv if use_input
+    "Inverse of the multiplier factor"
+    annotation (Placement(transformation(
+          extent={{100,50},{120,70}}), iconTransformation(extent={{100,50},{120,
+            70}})));
+protected
+  Modelica.Blocks.Interfaces.RealInput u_internal
+    "Connector for multiplier factor for internal use only"
+    annotation (Placement(
+    transformation(extent={{-60,20},{-20,60}}),iconTransformation(extent={{100,40},
+    {140,80}})));
+
+  Modelica.Blocks.Sources.Constant cst(
+    final k=k) if not use_input
+    "Constant gain value"
+    annotation (Placement(transformation(extent={{-90,30},{-70,50}})));
+  Modelica.Blocks.Math.Division div1 if use_input
+    "Compute the inverse"
+    annotation (Placement(transformation(extent={{20,50},{40,70}})));
+  Modelica.Blocks.Sources.Constant one(
+    final k=1) if use_input
+    "Constant 1"
+    annotation (Placement(transformation(extent={{-40,70},{-20,90}})));
 
 initial equation
-  assert(k > Modelica.Constants.small or -k < -Modelica.Constants.small,
-    "Gain must not be zero. Received k = " + String(k));
+  assert(k > Modelica.Constants.small,
+    "Gain must be strictly positive. Received k = " + String(k));
 equation
-    // Pressure drop in design flow direction
+  assert(u_internal > Modelica.Constants.small,
+    "Gain must be strictly positive. Received u = " + String(u_internal));
+
+  // Pressure drop in design flow direction
   port_a.p = port_b.p;
 
   // Mass balance (mass is not conserved by this model!)
-  port_b.m_flow = -k*port_a.m_flow;
+  port_b.m_flow = -u_internal * port_a.m_flow;
 
   // Specific enthalpy flow rate
   port_a.h_outflow = inStream(port_b.h_outflow);
@@ -24,34 +62,56 @@ equation
   port_a.C_outflow = inStream(port_b.C_outflow);
   port_b.C_outflow = inStream(port_a.C_outflow);
 
+  connect(cst.y, u_internal)
+    annotation (Line(points={{-69,40},{-40,40}},color={0,0,127}));
+  connect(u_internal, div1.u2)
+    annotation (Line(points={{-40,40},{0,40},{0,54},{18,54}}, color={0,0,127}));
+  connect(one.y, div1.u1)
+    annotation (Line(points={{-19,80},{0,80},{0,66},{18,66}}, color={0,0,127}));
+  connect(div1.y, uInv)
+    annotation (Line(points={{41,60},{110,60}}, color={0,0,127}));
+  connect(u, u_internal) annotation (Line(points={{-120,60},{-60,60},{-60,40},{-40,
+          40}}, color={0,0,127}));
+
   annotation (Documentation(info="<html>
- <p>
- This model multiplies the mass flow rate so that
- <code>0 = port_b.m_flow + k * port_a.m_flow</code>.
- </p>
- <p>
- The specific enthalpy, the species concentration and the trace substance concentration
- remain unchanged.
- Therefore, this model does not conserve mass or energy.
- It is used in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.PartialBorefield\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.PartialBorefield</a>
- and also in the Buildings library
- to avoid having to instantiate circuits in parallel, with each
- having the same mass flow rate and temperatures.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 27, 2013, by Michael Wetter:<br/>
- Changed implementation to extend from <code>Modelica.Fluid</code>.
- </li>
- <li>
- June 27, 2012, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<p>
+This model multiplies the mass flow rate so that
+<code>0 = port_b.m_flow + gain * port_a.m_flow</code>
+where <code>gain &gt; 0</code> is either equal to
+the input variable <code>u</code> if <code>use_input</code>
+is set to <code>true</code>, or equal to
+the parameter <code>k</code> if <code>use_input</code>
+is set to <code>false</code>.
+</p>
+<p>
+The specific enthalpy, the species concentration and the trace substance concentration
+remain unchanged.
+Therefore, this model does not conserve mass or energy.
+It is used in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.PartialBorefield\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.PartialBorefield</a>
+and also in the Buildings library
+to avoid having to instantiate circuits in parallel, with each
+having the same mass flow rate and temperatures.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 11, 2023, by Antoine Gautier:<br/>
+Added option to use input connector as multiplier factor.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1684\">#1684</a>.
+</li>
+<li>
+March 27, 2013, by Michael Wetter:<br/>
+Changed implementation to extend from <code>Modelica.Fluid</code>.
+</li>
+<li>
+June 27, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Rectangle(
           extent={{-100,100},{100,-100}},
           fillColor={255,237,228},
@@ -63,6 +123,6 @@ equation
           lineColor={0,0,255},
           smooth=Smooth.None,
           fillColor={0,0,255},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFlowRateMultiplier;
diff --git a/AixLib/Fluid/BaseClasses/PartialResistance.mo b/AixLib/Fluid/BaseClasses/PartialResistance.mo
index b85be0e099..6ac12b519c 100644
--- a/AixLib/Fluid/BaseClasses/PartialResistance.mo
+++ b/AixLib/Fluid/BaseClasses/PartialResistance.mo
@@ -92,150 +92,150 @@ equation
           pattern=LinePattern.None)}),
           defaultComponentName="res",
 Documentation(info="<html>
- <p>
- Partial model for a flow resistance, possible with variable flow coefficient.
- Models that extend this class need to implement an equation that relates
- <code>m_flow</code> and <code>dp</code>, and they need to assign the parameter
- <code>m_flow_turbulent</code>.
- </p>
- <p>
- See for example
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
- AixLib.Fluid.FixedResistances.PressureDrop</a> for a model that extends
- this base class.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- February 26, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- October 25, 2019, by Jianjun Hu:<br/>
- Improved icon graphics annotation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Removed start value for pressure difference
- to simplify the parameter window.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Avoided assignment of <code>dp(nominal=0)</code> if <code>dp_nominal_pos = 0</code>
- and of <code>m_flow(nominal=0)</code> if <code>m_flow_nominal_pos = 0</code>
- as nominal values are not allowed to be zero.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- August 15, 2015, by Filip Jorissen:<br/>
- Implemented more efficient computation of <code>port_a.Xi_outflow</code>,
- <code>port_a.h_outflow</code>
- and <code>port_a.C_outflow</code> when <code>allowFlowReversal=false</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/281\">#281</a>.
- </li>
- <li>
- January 13, 2015, by Marcus Fuchs:<br/>
- Revised revisions section (there were two revisions statements)
- </li>
- <li>
- November 20, 2014 by Michael Wetter:<br/>
- Removed <code>start</code> attribute for <code>m_flow</code>
- as this is already set in its base class.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Removed propagation of <code>show_V_flow</code>
- to base class as it has no longer this parameter.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>
- February 12, 2012, by Michael Wetter:<br/>
- Removed duplicate declaration of <code>m_flow_nominal</code>.
- </li>
- <li>
- February 3, 2012, by Michael Wetter:<br/>
- Made assignment of <code>m_flow_small</code> <code>final</code> as it is no
- longer used in the base class.
- </li>
- <li>
- January 16, 2012, by Michael Wetter:<br/>
- To simplify object inheritance tree, revised base classes
- <code>AixLib.Fluid.BaseClasses.PartialResistance</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialActuator</code>
- and model
- <code>AixLib.Fluid.FixedResistances.PressureDrop</code>.
- </li>
- <li>
- August 5, 2011, by Michael Wetter:<br/>
- Moved linearized pressure drop equation from the function body to the equation
- section. With the previous implementation,
- the symbolic processor may not rearrange the equations, which can lead
- to coupled equations instead of an explicit solution.
- </li>
- <li>
- June 20, 2011, by Michael Wetter:<br/>
- Set start values for <code>m_flow</code> and <code>dp</code> to zero, since
- most HVAC systems start at zero flow. With this change, the start values
- appear in the GUI and can be set by the user.
- </li>
- <li>
- April 2, 2011 by Michael Wetter:<br/>
- Added <code>m_flow_nominal_pos</code> and <code>dp_nominal_pos</code> to allow
- providing negative nominal values which will be used, for example, to set start
- values of flow splitters which may have negative flow rates and pressure drop
- at the initial condition.
- </li>
- <li>
- March 27, 2011, by Michael Wetter:<br/>
- Added <code>homotopy</code> operator.
- </li>
- <li>
- March 23, 2011 by Michael Wetter:<br/>
- Added homotopy operator.
- </li>
- <li>
- March 30, 2010 by Michael Wetter:<br/>
- Changed base classes to allow easier initialization.
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- Extracted pressure drop computation and implemented it in the
- new model
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.BasicFlowModel\">
- AixLib.Fluid.BaseClasses.FlowModels.BasicFlowModel</a>.
- </li>
- <li>
- September 18, 2008, by Michael Wetter:<br/>
- Added equations for the mass balance of extra species flow,
- i.e., <code>C</code> and <code>mC_flow</code>.
- </li>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model for a flow resistance, possible with variable flow coefficient.
+Models that extend this class need to implement an equation that relates
+<code>m_flow</code> and <code>dp</code>, and they need to assign the parameter
+<code>m_flow_turbulent</code>.
+</p>
+<p>
+See for example
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
+AixLib.Fluid.FixedResistances.PressureDrop</a> for a model that extends
+this base class.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+February 26, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+October 25, 2019, by Jianjun Hu:<br/>
+Improved icon graphics annotation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Removed start value for pressure difference
+to simplify the parameter window.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Avoided assignment of <code>dp(nominal=0)</code> if <code>dp_nominal_pos = 0</code>
+and of <code>m_flow(nominal=0)</code> if <code>m_flow_nominal_pos = 0</code>
+as nominal values are not allowed to be zero.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+August 15, 2015, by Filip Jorissen:<br/>
+Implemented more efficient computation of <code>port_a.Xi_outflow</code>,
+<code>port_a.h_outflow</code>
+and <code>port_a.C_outflow</code> when <code>allowFlowReversal=false</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/281\">#281</a>.
+</li>
+<li>
+January 13, 2015, by Marcus Fuchs:<br/>
+Revised revisions section (there were two revisions statements)
+</li>
+<li>
+November 20, 2014 by Michael Wetter:<br/>
+Removed <code>start</code> attribute for <code>m_flow</code>
+as this is already set in its base class.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Removed propagation of <code>show_V_flow</code>
+to base class as it has no longer this parameter.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>
+February 12, 2012, by Michael Wetter:<br/>
+Removed duplicate declaration of <code>m_flow_nominal</code>.
+</li>
+<li>
+February 3, 2012, by Michael Wetter:<br/>
+Made assignment of <code>m_flow_small</code> <code>final</code> as it is no
+longer used in the base class.
+</li>
+<li>
+January 16, 2012, by Michael Wetter:<br/>
+To simplify object inheritance tree, revised base classes
+<code>AixLib.Fluid.BaseClasses.PartialResistance</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialActuator</code>
+and model
+<code>AixLib.Fluid.FixedResistances.PressureDrop</code>.
+</li>
+<li>
+August 5, 2011, by Michael Wetter:<br/>
+Moved linearized pressure drop equation from the function body to the equation
+section. With the previous implementation,
+the symbolic processor may not rearrange the equations, which can lead
+to coupled equations instead of an explicit solution.
+</li>
+<li>
+June 20, 2011, by Michael Wetter:<br/>
+Set start values for <code>m_flow</code> and <code>dp</code> to zero, since
+most HVAC systems start at zero flow. With this change, the start values
+appear in the GUI and can be set by the user.
+</li>
+<li>
+April 2, 2011 by Michael Wetter:<br/>
+Added <code>m_flow_nominal_pos</code> and <code>dp_nominal_pos</code> to allow
+providing negative nominal values which will be used, for example, to set start
+values of flow splitters which may have negative flow rates and pressure drop
+at the initial condition.
+</li>
+<li>
+March 27, 2011, by Michael Wetter:<br/>
+Added <code>homotopy</code> operator.
+</li>
+<li>
+March 23, 2011 by Michael Wetter:<br/>
+Added homotopy operator.
+</li>
+<li>
+March 30, 2010 by Michael Wetter:<br/>
+Changed base classes to allow easier initialization.
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+Extracted pressure drop computation and implemented it in the
+new model
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels.BasicFlowModel\">
+AixLib.Fluid.BaseClasses.FlowModels.BasicFlowModel</a>.
+</li>
+<li>
+September 18, 2008, by Michael Wetter:<br/>
+Added equations for the mass balance of extra species flow,
+i.e., <code>C</code> and <code>mC_flow</code>.
+</li>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialResistance;
diff --git a/AixLib/Fluid/BaseClasses/PartialReversibleVapourCompressionMachine.mo b/AixLib/Fluid/BaseClasses/PartialReversibleVapourCompressionMachine.mo
index 4cf93d15c0..4da9d823ff 100644
--- a/AixLib/Fluid/BaseClasses/PartialReversibleVapourCompressionMachine.mo
+++ b/AixLib/Fluid/BaseClasses/PartialReversibleVapourCompressionMachine.mo
@@ -30,7 +30,7 @@ partial model PartialReversibleVapourCompressionMachine
   parameter Boolean use_autoCalc=false
     "Enable automatic estimation of volumes and mass flows?"
     annotation(choices(checkBox=true), Dialog(descriptionLabel=true));
-  parameter Modelica.Units.SI.Power Q_useNominal(start=0)
+  parameter Modelica.Units.SI.Power Q_useNominal=0
     "Nominal usable heat flow of the vapour compression machine (HP: Heating; Chiller: Cooling)"
     annotation (Dialog(enable=use_autoCalc));
   parameter Real scalingFactor=1 "Scaling-factor of vapour compression machine";
@@ -76,13 +76,13 @@ partial model PartialReversibleVapourCompressionMachine
       group="Heat Losses",
       tab="Condenser",
       enable=use_conCap));
-  parameter Modelica.Units.SI.ThermalConductance GConOut
+  parameter Modelica.Units.SI.ThermalConductance GConOut=0
     "Constant parameter for heat transfer to the ambient. Represents a sum of thermal resistances such as conductance, insulation and natural convection. If you want to simulate a condenser with additional dry mass but without external heat losses, set the value to zero"
     annotation (Evaluate=true, Dialog(
       group="Heat Losses",
       tab="Condenser",
       enable=use_conCap));
-  parameter Modelica.Units.SI.ThermalConductance GConIns
+  parameter Modelica.Units.SI.ThermalConductance GConIns=0
     "Constant parameter for heat transfer to heat exchangers capacity. Represents a sum of thermal resistances such as forced convection and conduction inside of the capacity"
     annotation (Evaluate=true, Dialog(
       group="Heat Losses",
@@ -117,13 +117,13 @@ partial model PartialReversibleVapourCompressionMachine
       group="Heat Losses",
       tab="Evaporator",
       enable=use_evaCap));
-  parameter Modelica.Units.SI.ThermalConductance GEvaOut
+  parameter Modelica.Units.SI.ThermalConductance GEvaOut=0
     "Constant parameter for heat transfer to the ambient. Represents a sum of thermal resistances such as conductance, insulation and natural convection. If you want to simulate a evaporator with additional dry mass but without external heat losses, set the value to zero"
     annotation (Evaluate=true, Dialog(
       group="Heat Losses",
       tab="Evaporator",
       enable=use_evaCap));
-  parameter Modelica.Units.SI.ThermalConductance GEvaIns
+  parameter Modelica.Units.SI.ThermalConductance GEvaIns=0
     "Constant parameter for heat transfer to heat exchangers capacity. Represents a sum of thermal resistances such as forced convection and conduction inside of the capacity"
     annotation (Evaluate=true, Dialog(
       group="Heat Losses",
@@ -788,7 +788,7 @@ equation
 <ol>
   <li>
     <a href=
-    \"AixLib.Fluid.HeatPumps.BaseClasses.InnerCycle\">InnerCycle</a>
+    \"AixLib.Fluid.HeatPumps.BaseClasses.InnerCycle_HeatPump\">InnerCycle</a>
     (Black Box): Here, the user can use between several input models or
     just easily create his own, modular black box model. Please look at
     the model description for more info.
diff --git a/AixLib/Fluid/BaseClasses/PartialThreeWayResistance.mo b/AixLib/Fluid/BaseClasses/PartialThreeWayResistance.mo
index a644948ec3..29e005dcdd 100644
--- a/AixLib/Fluid/BaseClasses/PartialThreeWayResistance.mo
+++ b/AixLib/Fluid/BaseClasses/PartialThreeWayResistance.mo
@@ -109,49 +109,49 @@ initial equation
          portFlowDirection_2<>Modelica.Fluid.Types.PortFlowDirection.Leaving or
          portFlowDirection_3<>Modelica.Fluid.Types.PortFlowDirection.Leaving,
          "In " + getInstanceName() + ": All ports are configured to
-          Modelica.Fluid.Types.PortFlowDirection.Leaving, which is non-physical.");
+         Modelica.Fluid.Types.PortFlowDirection.Leaving, which is non-physical.");
   assert(portFlowDirection_1<>Modelica.Fluid.Types.PortFlowDirection.Entering or
          portFlowDirection_2<>Modelica.Fluid.Types.PortFlowDirection.Entering or
          portFlowDirection_3<>Modelica.Fluid.Types.PortFlowDirection.Entering,
          "In " + getInstanceName() + ": All ports are configured to
-          Modelica.Fluid.Types.PortFlowDirection.Entering, which is non-physical.");
+         Modelica.Fluid.Types.PortFlowDirection.Entering, which is non-physical.");
 
 equation
   if verifyFlowReversal then
     if portFlowDirection_1==Modelica.Fluid.Types.PortFlowDirection.Entering then
       assert(port_1.m_flow> -m_flow_small,
       "In " + getInstanceName() + ":
-       Flow is leaving port_1 despite portFlowDirection_1=PortFlowDirection.Entering, since m_flow="+
+      Flow is leaving port_1 despite portFlowDirection_1=PortFlowDirection.Entering, since m_flow=" +
       String(port_1.m_flow) + "<-"+String(m_flow_small));
     end if;
     if portFlowDirection_1==Modelica.Fluid.Types.PortFlowDirection.Leaving then
       assert(port_1.m_flow< m_flow_small,
       "In " + getInstanceName() + ":
-       Flow is entering port_1 despite portFlowDirection_1=PortFlowDirection.Leaving, since m_flow="+
+      Flow is entering port_1 despite portFlowDirection_1=PortFlowDirection.Leaving, since m_flow=" +
       String(port_1.m_flow) + ">"+String(m_flow_small));
     end if;
     if portFlowDirection_2==Modelica.Fluid.Types.PortFlowDirection.Entering then
       assert(port_2.m_flow> -m_flow_small,
       "In " + getInstanceName() + ":
-       Flow is leaving port_2 despite portFlowDirection_2=PortFlowDirection.Entering, since m_flow="+
+      Flow is leaving port_2 despite portFlowDirection_2=PortFlowDirection.Entering, since m_flow=" +
       String(port_2.m_flow) + "<-"+String(m_flow_small));
     end if;
     if portFlowDirection_2==Modelica.Fluid.Types.PortFlowDirection.Leaving then
       assert(port_2.m_flow< m_flow_small,
       "In " + getInstanceName() + ":
-       Flow is entering port_2 despite portFlowDirection_2=PortFlowDirection.Leaving, since m_flow="+
+      Flow is entering port_2 despite portFlowDirection_2=PortFlowDirection.Leaving, since m_flow=" +
       String(port_2.m_flow) + ">"+String(m_flow_small));
     end if;
     if portFlowDirection_3==Modelica.Fluid.Types.PortFlowDirection.Entering then
       assert(port_3.m_flow> -m_flow_small,
       "In " + getInstanceName() + ":
-       Flow is leaving port_3 despite portFlowDirection_3=PortFlowDirection.Entering, since m_flow="+
+      Flow is leaving port_3 despite portFlowDirection_3=PortFlowDirection.Entering, since m_flow=" +
       String(port_3.m_flow) + "<-"+String(m_flow_small));
     end if;
     if portFlowDirection_3==Modelica.Fluid.Types.PortFlowDirection.Leaving then
       assert(port_3.m_flow< m_flow_small,
       "In " + getInstanceName() + ":
-       Flow is entering port_3 despite portFlowDirection_3=PortFlowDirection.Leaving, since m_flow="+
+      Flow is entering port_3 despite portFlowDirection_3=PortFlowDirection.Leaving, since m_flow=" +
       String(port_3.m_flow) + ">"+String(m_flow_small));
     end if;
   end if;
@@ -230,91 +230,91 @@ equation
   end if;
    annotation (
     Documentation(info="<html>
- <p>
- Partial model for flow resistances with three ports such as a
- flow mixer/splitter or a three way valve.
- </p>
- <p>
- If <code>energyDynamics &ne; Modelica.Fluid.Types.Dynamics.SteadyState</code>,
- then at the junction of the three flows,
- a mixing volume will be present. This will introduce a dynamic energy and momentum
- balance, which often breaks algebraic loops.
- The time constant of the mixing volume is determined by the parameter <code>tau</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- March 22, 2020, by Filip Jorissen:<br/>
- Corrected error message of asserts that verify whether flow reversal occurs when
- <code>verifyFlowReversal=true</code> and <code>portFlowDirection&lt;&gt;Bidirectional</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1327\">#1327</a>.
- </li>
- <li>
- July 7, 2018, by Filip Jorissen:<br/>
- Added asserts that verify whether flow reversal occurs when
- <code>verifyFlowReversal=true</code> and <code>portFlowDirection&lt;&gt;Bidirectional</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/963\">#963</a>.
- </li>
- <li>
- July 8, 2018, by Filip Jorissen:<br/>
- Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
- </li>
- <li>
- March 30, 2018, by Filip Jorissen:<br/>
- Added graphical illustrations for the values of <code>portFlowDirection</code>.
- Added asserts that verify the consistency of
- the values of <code>portFlowDirection</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/902\">#902</a>.
- </li>
- <li>
- February 22, 2016, by Michael Wetter:<br/>
- Conditionally removed control volume <code>vol</code>, and added the conditional connnector
- <code>port_internal</code>.
- This was already done when the parameter <code>dynamicBalance</code> was present, but
- was updated wrong when this parameter was removed.
- Without these conditional components, the regression test for
- <code>AixLib.Fluid.Examples.ResistanceVolumeFlowReversal</code> fails to simulate.
- </li>
- <li>
- December 17, 2015, by Michael Wetter:<br/>
- Added assignment <code>redeclare final package Medium=Medium</code>
- as this is required for OpenModelica.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/475\">
- https://github.com/lbl-srg/modelica-buildings/issues/475</a>.
- </li>
- <li>
- February 20, 2016, by Ruben Baetens:<br/>
- Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
- </li>
- <li>
- April 13 2015, by Filip Jorissen:<br/>
- Exposed options for flow reversal to users and added corresponding implementation.
- </li>
- <li>
- March 23 2010, by Michael Wetter:<br/>
- Changed start values from <code>system.p_start</code> or (code <code>T_start</code>)
- to <code>Medium.p_default</code>.
- </li>
- <li>
- September 18, 2008 by Michael Wetter:<br/>
- Replaced splitter model with a fluid port since the
- splitter model in Modelica.Fluid 1.0 beta does not transport
- <code>mC_flow</code>.
- </li>
- <li>
- June 11, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<p>
+Partial model for flow resistances with three ports such as a
+flow mixer/splitter or a three way valve.
+</p>
+<p>
+If <code>energyDynamics &ne; Modelica.Fluid.Types.Dynamics.SteadyState</code>,
+then at the junction of the three flows,
+a mixing volume will be present. This will introduce a dynamic energy and momentum
+balance, which often breaks algebraic loops.
+The time constant of the mixing volume is determined by the parameter <code>tau</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+March 22, 2020, by Filip Jorissen:<br/>
+Corrected error message of asserts that verify whether flow reversal occurs when
+<code>verifyFlowReversal=true</code> and <code>portFlowDirection&lt;&gt;Bidirectional</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1327\">#1327</a>.
+</li>
+<li>
+July 7, 2018, by Filip Jorissen:<br/>
+Added asserts that verify whether flow reversal occurs when
+<code>verifyFlowReversal=true</code> and <code>portFlowDirection&lt;&gt;Bidirectional</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/963\">#963</a>.
+</li>
+<li>
+July 8, 2018, by Filip Jorissen:<br/>
+Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
+</li>
+<li>
+March 30, 2018, by Filip Jorissen:<br/>
+Added graphical illustrations for the values of <code>portFlowDirection</code>.
+Added asserts that verify the consistency of
+the values of <code>portFlowDirection</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/902\">#902</a>.
+</li>
+<li>
+February 22, 2016, by Michael Wetter:<br/>
+Conditionally removed control volume <code>vol</code>, and added the conditional connnector
+<code>port_internal</code>.
+This was already done when the parameter <code>dynamicBalance</code> was present, but
+was updated wrong when this parameter was removed.
+Without these conditional components, the regression test for
+<code>AixLib.Fluid.Examples.ResistanceVolumeFlowReversal</code> fails to simulate.
+</li>
+<li>
+December 17, 2015, by Michael Wetter:<br/>
+Added assignment <code>redeclare final package Medium=Medium</code>
+as this is required for OpenModelica.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/475\">
+https://github.com/lbl-srg/modelica-buildings/issues/475</a>.
+</li>
+<li>
+February 20, 2016, by Ruben Baetens:<br/>
+Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
+</li>
+<li>
+April 13 2015, by Filip Jorissen:<br/>
+Exposed options for flow reversal to users and added corresponding implementation.
+</li>
+<li>
+March 23 2010, by Michael Wetter:<br/>
+Changed start values from <code>system.p_start</code> or (code <code>T_start</code>)
+to <code>Medium.p_default</code>.
+</li>
+<li>
+September 18, 2008 by Michael Wetter:<br/>
+Replaced splitter model with a fluid port since the
+splitter model in Modelica.Fluid 1.0 beta does not transport
+<code>mC_flow</code>.
+</li>
+<li>
+June 11, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Polygon(
           points={{104,28},{124,20},{104,12},{104,28}},
           lineColor={0,128,255},
@@ -354,6 +354,6 @@ equation
           fillPattern=FillPattern.Solid,
           visible=portFlowDirection_3==Modelica.Fluid.Types.PortFlowDirection.Leaving,
           origin={26,-125},
-          rotation=90)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          rotation=90)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialThreeWayResistance;
diff --git a/AixLib/Fluid/BaseClasses/Validation/ActuatorFilter.mo b/AixLib/Fluid/BaseClasses/Validation/ActuatorFilter.mo
index 4d9508f1e3..2016bc73a4 100644
--- a/AixLib/Fluid/BaseClasses/Validation/ActuatorFilter.mo
+++ b/AixLib/Fluid/BaseClasses/Validation/ActuatorFilter.mo
@@ -46,21 +46,21 @@ equation
       StopTime=20,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- This example validates
- <a href=\"modelica://AixLib.Fluid.BaseClasses.ActuatorFilter\">
- AixLib.Fluid.BaseClasses.ActuatorFilter</a>.
- The validation is done for different settings of <code>u_nominal</code> and for
- different start values of the filter output.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 22, 2021, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://https://github.com/ibpsa/modelica-ibpsa/issues/1498\">IBPSA, #1498</a>
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates
+<a href=\"modelica://AixLib.Fluid.BaseClasses.ActuatorFilter\">
+AixLib.Fluid.BaseClasses.ActuatorFilter</a>.
+The validation is done for different settings of <code>u_nominal</code> and for
+different start values of the filter output.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 22, 2021, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://https://github.com/ibpsa/modelica-ibpsa/issues/1498\">IBPSA, #1498</a>
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ActuatorFilter;
diff --git a/AixLib/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mo b/AixLib/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mo
index 12ba555d2e..15c3fad485 100644
--- a/AixLib/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mo
+++ b/AixLib/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mo
@@ -21,36 +21,64 @@ model MassFlowRateMultiplier "Example use of MassFlowRateMultiplier"
     annotation (Placement(transformation(extent={{-40,-10},{-20,10}})));
   AixLib.Fluid.Sources.Boundary_pT sin(
     redeclare package Medium = Medium,
-    nPorts=1)
+    nPorts=2)
     "Mass flow sink"
     annotation (Placement(transformation(extent={{-10,-10},{10,10}},
         rotation=180,
         origin={70,0})));
+  AixLib.Fluid.BaseClasses.MassFlowRateMultiplier
+    massFlowRateMultiplier1(
+    redeclare package Medium = Medium,
+    use_input=true,
+    k=5)
+      "Mass flow rate multiplier"
+    annotation (Placement(transformation(extent={{10,-70},{30,-50}})));
+  Modelica.Blocks.Sources.Ramp gaiMasFlo(
+    height=4.9,
+    duration=10,
+    offset=0.1) "Mass flow rate multiplier factor"
+    annotation (Placement(transformation(extent={{-80,-50},{-60,-30}})));
+  AixLib.Fluid.Sources.MassFlowSource_T sou1(
+    redeclare package Medium = Medium,
+    use_m_flow_in=true,
+    nPorts=1) "Mass flow source"
+    annotation (Placement(transformation(extent={{-40,-70},{-20,-50}})));
 equation
   connect(ram_m_flow.y, sou.m_flow_in)
     annotation (Line(points={{-59,8},{-42,8}}, color={0,0,127}));
   connect(sou.ports[1], massFlowRateMultiplier.port_a)
     annotation (Line(points={{-20,0},{10,0}},          color={0,127,255}));
   connect(massFlowRateMultiplier.port_b, sin.ports[1])
-    annotation (Line(points={{30,0},{60,0}},        color={0,127,255}));
+    annotation (Line(points={{30,0},{60,0},{60,1}}, color={0,127,255}));
+  connect(sou1.ports[1], massFlowRateMultiplier1.port_a)
+    annotation (Line(points={{-20,-60},{10,-60}}, color={0,127,255}));
+  connect(massFlowRateMultiplier1.port_b, sin.ports[2])
+    annotation (Line(points={{30,-60},{60,-60},{60,-1}}, color={0,127,255}));
+  connect(gaiMasFlo.y, massFlowRateMultiplier1.u) annotation (Line(points={{-59,
+          -40},{0,-40},{0,-54},{8,-54}}, color={0,0,127}));
+  connect(ram_m_flow.y, sou1.m_flow_in) annotation (Line(points={{-59,8},{-50,8},
+          {-50,-52},{-42,-52}}, color={0,0,127}));
   annotation (
     __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mos"
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StartTime=0.0, StopTime=10.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of 
- <a href=\"modelica://AixLib.Fluid.BaseClasses.MassFlowRateMultiplier\">
- AixLib.Fluid.BaseClasses.MassFlowRateMultiplier</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 19, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of
+<a href=\"modelica://AixLib.Fluid.BaseClasses.MassFlowRateMultiplier\">
+AixLib.Fluid.BaseClasses.MassFlowRateMultiplier</a>,
+using either a parameter to specify the multiplier factor
+(see the instance <code>massFlowRateMultiplier</code>) or
+an input signal (see the instance <code>massFlowRateMultiplier1</code>).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 19, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFlowRateMultiplier;
diff --git a/AixLib/Fluid/BoilerCHP/Examples/CHPSystem.mo b/AixLib/Fluid/BoilerCHP/Examples/CHPSystem.mo
index 4eef49ec61..78f42bc240 100644
--- a/AixLib/Fluid/BoilerCHP/Examples/CHPSystem.mo
+++ b/AixLib/Fluid/BoilerCHP/Examples/CHPSystem.mo
@@ -2,21 +2,26 @@ within AixLib.Fluid.BoilerCHP.Examples;
 model CHPSystem "Example that illustrates use of CHP model"
   extends Modelica.Icons.Example;
 
-  CHP combinedHeatPower(
+  AixLib.Fluid.BoilerCHP.CHP combinedHeatPower(
     redeclare package Medium =
         Media.Specialized.Water.TemperatureDependentDensity,
     m_flow_nominal=0.02,
     TSetIn=true,
     minCapacity=20,
     delayTime=300,
-    param=DataBase.CHP.CHPDataSimple.CHP_FMB_65_GSK()) "CHP"
+    param=DataBase.CHP.CHPDataSimple.CHP_FMB_65_GSK(),
+    vol(energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial),
+    Kc=0.02,
+    Tc=100,
+    elControl(initType=Modelica.Blocks.Types.Init.InitialOutput))
+                                                       "CHP"
     annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
   Modelica.Fluid.Sources.MassFlowSource_T source(
     redeclare package Medium =
         Media.Specialized.Water.TemperatureDependentDensity,
     use_T_in=true,
     nPorts=1,
-    m_flow=0.5)
+    m_flow=0.1)
     "Source"
     annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
   Modelica.Fluid.Sources.Boundary_pT sink(
@@ -38,7 +43,7 @@ model CHPSystem "Example that illustrates use of CHP model"
   Modelica.Blocks.Sources.BooleanConstant on
     "CHP is always on"
     annotation (Placement(transformation(extent={{-40,-40},{-20,-20}})));
-  Modelica.Blocks.Sources.Constant TSet(k=80 + 273.15)
+  Modelica.Blocks.Sources.Constant TSet(k=80 + 273.15, y(unit="K"))
     "Set temperature"
     annotation (Placement(transformation(extent={{-40,20},{-20,40}})));
 
@@ -82,5 +87,7 @@ equation
   </li>
 </ul>
 </html>"),
-experiment(StopTime=35000, Interval=60));
+experiment(Tolerance=1e-6, StopTime=1200, Interval=60), __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/BoilerCHP/Examples/CHPSystem.mos"
+        "Simulate and Plot"));
 end CHPSystem;
diff --git a/AixLib/Fluid/BoilerCHP/Examples/CHPSystemNoControl.mo b/AixLib/Fluid/BoilerCHP/Examples/CHPSystemNoControl.mo
index 5d0db3567c..4dae0cdfdf 100644
--- a/AixLib/Fluid/BoilerCHP/Examples/CHPSystemNoControl.mo
+++ b/AixLib/Fluid/BoilerCHP/Examples/CHPSystemNoControl.mo
@@ -3,8 +3,7 @@ model CHPSystemNoControl "Example that illustrates use of CHPNoControl model"
   extends Modelica.Icons.Example;
   package Medium = AixLib.Media.Water
     annotation (choicesAllMatching=true);
-  CHPNoControl
-      combinedHeatPower(
+  AixLib.Fluid.BoilerCHP.CHPNoControl combinedHeatPower(
     redeclare package Medium = Medium,
     m_flow_nominal=0.02,
     param=DataBase.CHP.CHPDataSimple.CHP_FMB_65_GSK()) "CHP"
@@ -62,6 +61,6 @@ equation
 </html>"),
 experiment(Tolerance=1e-6, StopTime=300, Interval=60),
     __Dymola_Commands(file=
-          "Resources/Scripts/Dymola/Fluid/BoilerCHP/Examples/CHPSystemNoControl.mos"
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/BoilerCHP/Examples/CHPSystemNoControl.mos"
         "Simulate and Plot"));
 end CHPSystemNoControl;
diff --git a/AixLib/Fluid/Chillers/BaseClasses/Carnot.mo b/AixLib/Fluid/Chillers/BaseClasses/Carnot.mo
index 5aa4e30516..1526322e1c 100644
--- a/AixLib/Fluid/Chillers/BaseClasses/Carnot.mo
+++ b/AixLib/Fluid/Chillers/BaseClasses/Carnot.mo
@@ -13,25 +13,24 @@ partial model Carnot
   parameter Modelica.Units.SI.HeatFlowRate QCon_flow_nominal(min=0)
     "Nominal heating flow rate" annotation (Dialog(group="Nominal condition"));
 
-  parameter Modelica.Units.SI.TemperatureDifference dTEva_nominal(final max=0)=
-       -10 "Temperature difference evaporator outlet-inlet"
+  parameter Modelica.Units.SI.TemperatureDifference dTEva_nominal(final max=0)
+     = -10 "Temperature difference evaporator outlet-inlet"
     annotation (Dialog(group="Nominal condition"));
-  parameter Modelica.Units.SI.TemperatureDifference dTCon_nominal(final min=0)=
-       10 "Temperature difference condenser outlet-inlet"
+  parameter Modelica.Units.SI.TemperatureDifference dTCon_nominal(final min=0)
+     = 10 "Temperature difference condenser outlet-inlet"
     annotation (Dialog(group="Nominal condition"));
 
   // Efficiency
   parameter Boolean use_eta_Carnot_nominal = true
     "Set to true to use Carnot effectiveness etaCarnot_nominal rather than COP_nominal"
     annotation(Dialog(group="Efficiency"));
-  parameter Real etaCarnot_nominal(unit="1") = COP_nominal/
-    (TUseAct_nominal/(TCon_nominal+TAppCon_nominal - (TEva_nominal-TAppEva_nominal)))
-    "Carnot effectiveness (=COP/COP_Carnot) used if use_eta_Carnot_nominal = true"
+  parameter Real etaCarnot_nominal(unit="1") = 0.3
+    "Carnot effectiveness (=COP/COP_Carnot) used during simulation if use_eta_Carnot_nominal = true"
     annotation (Dialog(group="Efficiency", enable=use_eta_Carnot_nominal));
 
   parameter Real COP_nominal(unit="1") = etaCarnot_nominal*TUseAct_nominal/
     (TCon_nominal+TAppCon_nominal - (TEva_nominal-TAppEva_nominal))
-    "Coefficient of performance at TEva_nominal and TCon_nominal, used if use_eta_Carnot_nominal = false"
+    "Coefficient of performance at TEva_nominal and TCon_nominal, used during simulation if use_eta_Carnot_nominal = false"
     annotation (Dialog(group="Efficiency", enable=not use_eta_Carnot_nominal));
 
   parameter Modelica.Units.SI.Temperature TCon_nominal=303.15
@@ -52,12 +51,12 @@ partial model Carnot
     "Pressure difference over evaporator"
     annotation (Dialog(group="Nominal condition"));
 
-  parameter Modelica.Units.SI.TemperatureDifference TAppCon_nominal(min=0)=
+  parameter Modelica.Units.SI.TemperatureDifference TAppCon_nominal(min=0) =
     if cp1_default < 1500 then 5 else 2
     "Temperature difference between refrigerant and working fluid outlet in condenser"
     annotation (Dialog(group="Efficiency"));
 
-  parameter Modelica.Units.SI.TemperatureDifference TAppEva_nominal(min=0)=
+  parameter Modelica.Units.SI.TemperatureDifference TAppEva_nominal(min=0) =
     if cp2_default < 1500 then 5 else 2
     "Temperature difference between refrigerant and working fluid outlet in evaporator"
     annotation (Dialog(group="Efficiency"));
@@ -137,12 +136,12 @@ partial model Carnot
     x2=TConAct - TEvaAct,
     deltaX=0.25) "Carnot efficiency";
 
-  Modelica.Units.SI.Temperature TConAct(start=TCon_nominal + TAppCon_nominal)=
-       Medium1.temperature(staB1) + QCon_flow/QCon_flow_nominal*TAppCon_nominal
+  Modelica.Units.SI.Temperature TConAct(start=TCon_nominal + TAppCon_nominal)
+     = Medium1.temperature(staB1) + QCon_flow/QCon_flow_nominal*TAppCon_nominal
     "Condenser temperature used to compute efficiency, taking into account pinch temperature between fluid and refrigerant";
 
-  Modelica.Units.SI.Temperature TEvaAct(start=TEva_nominal - TAppEva_nominal)=
-       Medium2.temperature(staB2) - QEva_flow/QEva_flow_nominal*TAppEva_nominal
+  Modelica.Units.SI.Temperature TEvaAct(start=TEva_nominal - TAppEva_nominal)
+     = Medium2.temperature(staB2) - QEva_flow/QEva_flow_nominal*TAppEva_nominal
     "Evaporator temperature used to compute efficiency, taking into account pinch temperature between fluid and refrigerant";
 
 protected
@@ -330,101 +329,117 @@ equation
         Line(points={{0,-70},{0,-90},{100,-90}}, color={0,0,255}),
         Line(points={{62,0},{100,0}},                 color={0,0,255})}),
       Documentation(info="<html>
- <p>
- This is the base class for the Carnot chiller and the Carnot heat pump
- whose coefficient of performance COP changes
- with temperatures in the same way as the Carnot efficiency changes.
- </p>
- <p>
- The model allows to either specify the Carnot effectivness
- <i>&eta;<sub>Carnot,0</sub></i>, or
- a <i>COP<sub>0</sub></i>
- at the nominal conditions, together with
- the evaporator temperature <i>T<sub>eva,0</sub></i> and
- the condenser temperature <i>T<sub>con,0</sub></i>, in which
- case the model computes the Carnot effectivness as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &eta;<sub>Carnot,0</sub> =
-   COP<sub>0</sub>
- &frasl;  (T<sub>use,0</sub> &frasl; (T<sub>con,0</sub>-T<sub>eva,0</sub>)),
- </p>
- <p>
- where
- <i>T<sub>use</sub></i> is the temperature of the the useful heat,
- e.g., the evaporator temperature for a chiller or the condenser temperature
- for a heat pump.
- </p>
- <p>
- The COP is computed as the product
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
- </p>
- <p>
- where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
- <i>&eta;<sub>PL</sub></i> is the part load efficiency, expressed using
- a polynomial.
- This polynomial has the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y + a<sub>3</sub> y<sup>2</sup> + ...
- </p>
- <p>
- where <i>y &isin; [0, 1]</i> is
- either the part load for cooling in case of a chiller, or the part load of heating in
- case of a heat pump, and the coefficients <i>a<sub>i</sub></i>
- are declared by the parameter <code>a</code>.
- </p>
- <h4>Implementation</h4>
- <p>
- To make this base class applicable to chiller or heat pumps, it uses
- the boolean constant <code>COP_is_for_cooling</code>.
- Depending on its value, the equations for the coefficient of performance
- and the part load ratio are set up.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- September 12, 2019, by Michael Wetter:<br/>
- Corrected value of <code>evaluate_etaPL</code> and how it is used.
- This correction only affects protected variables and does not affect the results.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1200\">
- #1200</a>.
- </li>
- <li>
- June 16, 2017, by Michael Wetter:<br/>
- Added temperature difference between fluids in condenser and evaporator
- for computation of nominal COP and effectiveness.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/698\">
- #698</a>.
- </li>
- <li>
- March 28, 2017, by Felix Buenning:<br/>
- Added temperature difference between fluids in condenser and evaporator.
- The difference is based on discussions with Emerson Climate Technologies.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/698\">
- #698</a>.
- </li>
- <li>
- January 2, 2017, by Filip Jorissen:<br/>
- Removed option for choosing what temperature
- should be used to compute the Carnot efficiency.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- issue 497</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- First implementation of this base class.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is the base class for the Carnot chiller and the Carnot heat pump
+whose coefficient of performance COP changes
+with temperatures in the same way as the Carnot efficiency changes.
+</p>
+<p>
+Set <code>use_eta_Carnot_nominal=true</code> to specify directly
+the Carnot effectiveness <i>&eta;<sub>Carnot,0</sub></i>,
+in which case the value of the parameter <code>COP_nominal</code>
+will not affect the simulation.
+If <code>use_eta_Carnot_nominal=false</code>, the model will use
+the value of the parameter <code>COP_nominal</code>
+together with the specified nominal temperatures
+to compute the Carnot effectiveness as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&eta;<sub>Carnot,0</sub> =
+  COP<sub>0</sub>
+&frasl;  (T<sub>use,0</sub> &frasl; (T<sub>con,0</sub> + T<sub>app,con,0</sub> - (T<sub>eva,0</sub>-T<sub>app,eva,0</sub>))),
+</p>
+<p>
+where
+<i>T<sub>eva,0</sub></i> is the evaporator temperature,
+<i>T<sub>con,0</sub></i> is the condenser temperature,
+<i>T<sub>app,eva,0</sub></i> is the evaporator approach temperature,
+<i>T<sub>app,con,0</sub></i> is the condenser approach temperature, and
+<i>T<sub>use,0</sub></i> is the temperature of the the useful heat.
+If <code>COP_is_for_cooling=true</code>,
+then <i>T<sub>use,0</sub></i> is the condenser temperature of a heat pump plus the approach temperature,
+otherwise it is the evaporator temperature minus the approach temperature of a chiller.
+</p>
+<p>
+The COP is computed as the product
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
+</p>
+<p>
+where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
+<i>&eta;<sub>PL</sub></i> is the part load efficiency, expressed using
+a polynomial.
+This polynomial has the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y + a<sub>3</sub> y<sup>2</sup> + ...,
+</p>
+<p>
+where <i>y &isin; [0, 1]</i> is
+either the part load for cooling in case of a chiller, or the part load of heating in
+case of a heat pump, and the coefficients <i>a<sub>i</sub></i>
+are declared by the parameter <code>a</code>.
+</p>
+<h4>Implementation</h4>
+<p>
+To make this base class applicable to chiller or heat pumps, it uses
+the boolean constant <code>COP_is_for_cooling</code>.
+Depending on its value, the equations for the coefficient of performance
+and the part load ratio are set up.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 3, 2023, by Michael Wetter:<br/>
+Changed parameter binding
+<code>etaCarnot_nominal(unit=\"1\") = COP_nominal/(TUseAct_nominal/(TCon_nominal+TAppCon_nominal - (TEva_nominal-TAppEva_nominal)))</code>
+to
+<code>etaCarnot_nominal(unit=\"1\") = 0.3</code> to avoid a circular assignment.<br/>
+Improved documentation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3226\">Buildings, #3226</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+September 12, 2019, by Michael Wetter:<br/>
+Corrected value of <code>evaluate_etaPL</code> and how it is used.
+This correction only affects protected variables and does not affect the results.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1200\">
+#1200</a>.
+</li>
+<li>
+June 16, 2017, by Michael Wetter:<br/>
+Added temperature difference between fluids in condenser and evaporator
+for computation of nominal COP and effectiveness.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/698\">
+#698</a>.
+</li>
+<li>
+March 28, 2017, by Felix Buenning:<br/>
+Added temperature difference between fluids in condenser and evaporator.
+The difference is based on discussions with Emerson Climate Technologies.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/698\">
+#698</a>.
+</li>
+<li>
+January 2, 2017, by Filip Jorissen:<br/>
+Removed option for choosing what temperature
+should be used to compute the Carnot efficiency.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+issue 497</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+First implementation of this base class.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot;
diff --git a/AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_T.mo b/AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_T.mo
index abf4e75fcb..7d149723c7 100644
--- a/AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_T.mo
+++ b/AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_T.mo
@@ -12,20 +12,20 @@ equation
     annotation (Line(points={{61,0},{110,0},{110,0}}, color={0,0,127}));
   annotation (
 Documentation(info="<html>
- <p>
- This is a partial model of a chiller whose coefficient of performance (COP) changes
- with temperatures in the same way as the Carnot efficiency changes.
- This base class is used for the Carnot chiller and Carnot heat pump
- that uses the compressor part load ratio as the control signal.
- </p>
- </html>",
+<p>
+This is a partial model of a chiller whose coefficient of performance (COP) changes
+with temperatures in the same way as the Carnot efficiency changes.
+This base class is used for the Carnot chiller and Carnot heat pump
+that uses the compressor part load ratio as the control signal.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- First implementation of this base class.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+First implementation of this base class.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialCarnot_T;
diff --git a/AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_y.mo b/AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_y.mo
index 835994d8f1..973fa89555 100644
--- a/AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_y.mo
+++ b/AixLib/Fluid/Chillers/BaseClasses/PartialCarnot_y.mo
@@ -36,9 +36,9 @@ partial model PartialCarnot_y
     annotation (Placement(transformation(extent={{-140,70},{-100,110}})));
 
 protected
-  Modelica.Units.SI.HeatFlowRate QCon_flow_internal(start=QCon_flow_nominal)=
+  Modelica.Units.SI.HeatFlowRate QCon_flow_internal(start=QCon_flow_nominal) =
     P - QEva_flow_internal "Condenser heat input";
-  Modelica.Units.SI.HeatFlowRate QEva_flow_internal(start=QEva_flow_nominal)=
+  Modelica.Units.SI.HeatFlowRate QEva_flow_internal(start=QEva_flow_nominal) =
     if COP_is_for_cooling then -COP*P else (1 - COP)*P "Evaporator heat input";
 
   Modelica.Blocks.Sources.RealExpression yEva_flow_in(
@@ -154,79 +154,79 @@ equation
         Line(points={{62,0},{100,0}},                 color={0,0,255})}),
 defaultComponentName="chi",
 Documentation(info="<html>
- <p>
- This is a partial model of a chiller whose coefficient of performance (COP) changes
- with temperatures in the same way as the Carnot efficiency changes.
- This base class is used for the Carnot chiller and Carnot heat pump
- that uses the leaving fluid temperature as the control signal.
- </p>
- </html>",
+<p>
+This is a partial model of a chiller whose coefficient of performance (COP) changes
+with temperatures in the same way as the Carnot efficiency changes.
+This base class is used for the Carnot chiller and Carnot heat pump
+that uses the leaving fluid temperature as the control signal.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 15, 2017, by Michael Wetter:<br/>
- Added <code>min</code> attribute to parameter <code>P_nominal</code>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Implemented in the Annex 60 library the models
- <a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">AixLib.Fluid.Chillers.Carnot_y</a>
- and
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">AixLib.Fluid.HeatPumps.Carnot_y</a>
- and refactored these models to use the same base class.<br/>
- Implemented the removal of the flow direction dependency of
- <code>staA1</code>, <code>staB1</code>, <code>staA2</code> and <code>staB2</code> as the
- efficiency of the Carnot machine should only be computed in the design flow direction,
- as corrected by Damien Picard.
- </li>
- <li>
- December 18, 2015, by Michael Wetter:<br/>
- Corrected wrong computation of <code>staB1</code> and <code>staB2</code>
- which mistakenly used the <code>inStream</code> operator
- for the configuration without flow reversal.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/476\">
- issue 476</a>.
- </li>
- <li>
- November 25, 2015 by Michael Wetter:<br/>
- Changed sign convention for <code>dTEva_nominal</code> to be consistent with
- other models.
- The model will still work with the old values for <code>dTEva_nominal</code>,
- but it will write a warning so that users can transition their models.
- <br/>
- Corrected <code>assert</code> statement for the efficiency curve.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/468\">
- issue 468</a>.
- </li>
- <li>
- September 3, 2015 by Michael Wetter:<br/>
- Expanded documentation.
- </li>
- <li>
- May 6, 2015 by Michael Wetter:<br/>
- Added <code>prescribedHeatFlowRate=true</code> for <code>vol2</code>.
- </li>
- <li>
- October 9, 2013 by Michael Wetter:<br/>
- Reimplemented the computation of the port states to avoid using
- the conditionally removed variables <code>sta_a1</code>,
- <code>sta_a2</code>, <code>sta_b1</code> and <code>sta_b2</code>.
- </li>
- <li>
- May 10, 2013 by Michael Wetter:<br/>
- Added electric power <code>P</code> as an output signal.
- </li>
- <li>
- October 11, 2010 by Michael Wetter:<br/>
- Fixed bug in energy balance.
- </li>
- <li>
- March 3, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 15, 2017, by Michael Wetter:<br/>
+Added <code>min</code> attribute to parameter <code>P_nominal</code>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Implemented in the Annex 60 library the models
+<a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">AixLib.Fluid.Chillers.Carnot_y</a>
+and
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">AixLib.Fluid.HeatPumps.Carnot_y</a>
+and refactored these models to use the same base class.<br/>
+Implemented the removal of the flow direction dependency of
+<code>staA1</code>, <code>staB1</code>, <code>staA2</code> and <code>staB2</code> as the
+efficiency of the Carnot machine should only be computed in the design flow direction,
+as corrected by Damien Picard.
+</li>
+<li>
+December 18, 2015, by Michael Wetter:<br/>
+Corrected wrong computation of <code>staB1</code> and <code>staB2</code>
+which mistakenly used the <code>inStream</code> operator
+for the configuration without flow reversal.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/476\">
+issue 476</a>.
+</li>
+<li>
+November 25, 2015 by Michael Wetter:<br/>
+Changed sign convention for <code>dTEva_nominal</code> to be consistent with
+other models.
+The model will still work with the old values for <code>dTEva_nominal</code>,
+but it will write a warning so that users can transition their models.
+<br/>
+Corrected <code>assert</code> statement for the efficiency curve.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/468\">
+issue 468</a>.
+</li>
+<li>
+September 3, 2015 by Michael Wetter:<br/>
+Expanded documentation.
+</li>
+<li>
+May 6, 2015 by Michael Wetter:<br/>
+Added <code>prescribedHeatFlowRate=true</code> for <code>vol2</code>.
+</li>
+<li>
+October 9, 2013 by Michael Wetter:<br/>
+Reimplemented the computation of the port states to avoid using
+the conditionally removed variables <code>sta_a1</code>,
+<code>sta_a2</code>, <code>sta_b1</code> and <code>sta_b2</code>.
+</li>
+<li>
+May 10, 2013 by Michael Wetter:<br/>
+Added electric power <code>P</code> as an output signal.
+</li>
+<li>
+October 11, 2010 by Michael Wetter:<br/>
+Fixed bug in energy balance.
+</li>
+<li>
+March 3, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialCarnot_y;
diff --git a/AixLib/Fluid/Chillers/Carnot_TEva.mo b/AixLib/Fluid/Chillers/Carnot_TEva.mo
index f4442513cc..51b6c328e6 100644
--- a/AixLib/Fluid/Chillers/Carnot_TEva.mo
+++ b/AixLib/Fluid/Chillers/Carnot_TEva.mo
@@ -69,119 +69,133 @@ equation
         Line(points={{-100,90},{-80,90},{-80,-56}}, color={0,0,255})}),
 defaultComponentName="chi",
 Documentation(info="<html>
- <p>
- This is a model of a chiller whose coefficient of performance COP changes
- with temperatures in the same way as the Carnot efficiency changes.
- The control input is the setpoint of the evaporator leaving temperature, which
- is met exactly at steady state if the chiller has sufficient capacity.
- </p>
- <p>
- The model allows to either specify the Carnot effectivness
- <i>&eta;<sub>Carnot,0</sub></i>, or
- a <i>COP<sub>0</sub></i>
- at the nominal conditions, together with
- the evaporator temperature <i>T<sub>eva,0</sub></i> and
- the condenser temperature <i>T<sub>con,0</sub></i>, in which
- case the model computes the Carnot effectivness as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &eta;<sub>Carnot,0</sub> =
-   COP<sub>0</sub>
- &frasl;  (T<sub>eva,0</sub> &frasl; (T<sub>con,0</sub>-T<sub>eva,0</sub>)).
- </p>
- <p>
- On the <code>Advanced</code> tab, a user can specify the temperatures that
- will be used as the evaporator and condenser temperature.
- </p>
- <p>
- During the simulation, the chiller COP is computed as the product
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
- </p>
- <p>
- where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
- <i>&eta;<sub>PL</sub></i> is a polynomial in the cooling part load ratio <i>y<sub>PL</sub></i>
- that can be used to take into account a change in <i>COP</i> at part load
- conditions.
- This polynomial has the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y<sub>PL</sub> + a<sub>3</sub> y<sub>PL</sub><sup>2</sup> + ...
- </p>
- <p>
- where the coefficients <i>a<sub>i</sub></i>
- are declared by the parameter <code>a</code>.
- </p>
- <p>
- On the <code>Dynamics</code> tag, the model can be parametrized to compute a transient
- or steady-state response.
- The transient response of the model is computed using a first
- order differential equation for the evaporator and condenser fluid volumes.
- The chiller outlet temperatures are equal to the temperatures of these lumped volumes.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- When using this component, make sure that the condenser has sufficient mass flow rate.
- Based on the evaporator mass flow rate, temperature difference and the efficiencies,
- the model computes how much heat will be added to the condenser.
- If the mass flow rate is too small, very high outlet temperatures can result.
- </p>
- <p>
- The evaporator heat flow rate <code>QEva_flow_nominal</code> is used to assign
- the default value for the mass flow rates, which are used for the pressure drop
- calculations.
- It is also used to compute the part load efficiency.
- Hence, make sure that <code>QEva_flow_nominal</code> is set to a reasonable value.
- </p>
- <p>
- The maximum cooling capacity is set by the parameter <code>QEva_flow_min</code>,
- which is by default set to negative infinity.
- </p>
- <p>
- The coefficient of performance depends on the
- evaporator and condenser leaving temperature
- since otherwise the second law of thermodynamics may be violated.
- </p>
- <h4>Notes</h4>
- <p>
- For a similar model that can be used as a heat pump, see
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_TCon\">
- AixLib.Fluid.HeatPumps.Examples.Carnot_TCon</a>.
- </p>
- </html>",
+<p>
+This is a model of a chiller whose coefficient of performance COP changes
+with temperatures in the same way as the Carnot efficiency changes.
+The control input is the setpoint of the evaporator leaving temperature, which
+is met exactly at steady state if the chiller has sufficient capacity.
+</p>
+<p>
+Set <code>use_eta_Carnot_nominal=true</code> to specify directly
+the Carnot effectiveness <i>&eta;<sub>Carnot,0</sub></i>,
+in which case the value of the parameter <code>COP_nominal</code>
+will not affect the simulation.
+If <code>use_eta_Carnot_nominal=false</code>, the model will use
+the value of the parameter <code>COP_nominal</code>
+together with the specified nominal temperatures
+to compute the Carnot effectiveness as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&eta;<sub>Carnot,0</sub> =
+  COP<sub>0</sub>
+&frasl;  (T<sub>eva,0</sub> &frasl; (T<sub>con,0</sub> + T<sub>app,con,0</sub> - (T<sub>eva,0</sub>-T<sub>app,eva,0</sub>))),
+</p>
+<p>
+where
+<i>T<sub>eva,0</sub></i> is the evaporator temperature,
+<i>T<sub>con,0</sub></i> is the condenser temperature,
+<i>T<sub>app,eva,0</sub></i> is the evaporator approach temperature and
+<i>T<sub>app,con,0</sub></i> is the condenser approach temperature.
+</p>
+<p>
+The COP is computed as the product
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
+</p>
+<p>
+where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
+<i>&eta;<sub>PL</sub></i> is the part load efficiency, expressed using
+a polynomial.
+This polynomial has the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y + a<sub>3</sub> y<sup>2</sup> + ...,
+</p>
+<p>
+where <i>y &isin; [0, 1]</i> is
+the part load for cooling and the coefficients <i>a<sub>i</sub></i>
+are declared by the parameter <code>a</code>.
+</p>
+<p>
+On the <code>Dynamics</code> tag, the model can be parametrized to compute a transient
+or steady-state response.
+The transient response of the model is computed using a first
+order differential equation for the evaporator and condenser fluid volumes.
+The chiller outlet temperatures are equal to the temperatures of these lumped volumes.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+When using this component, make sure that the condenser has sufficient mass flow rate.
+Based on the evaporator mass flow rate, temperature difference and the efficiencies,
+the model computes how much heat will be added to the condenser.
+If the mass flow rate is too small, very high outlet temperatures can result.
+</p>
+<p>
+The evaporator heat flow rate <code>QEva_flow_nominal</code> is used to assign
+the default value for the mass flow rates, which are used for the pressure drop
+calculations.
+It is also used to compute the part load efficiency.
+Hence, make sure that <code>QEva_flow_nominal</code> is set to a reasonable value.
+</p>
+<p>
+The maximum cooling capacity is set by the parameter <code>QEva_flow_min</code>,
+which is by default set to negative infinity.
+</p>
+<p>
+The coefficient of performance depends on the
+evaporator and condenser leaving temperature
+since otherwise the second law of thermodynamics may be violated.
+</p>
+<h4>Notes</h4>
+<p>
+For a similar model that can be used as a heat pump, see
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_TCon\">
+AixLib.Fluid.HeatPumps.Examples.Carnot_TCon</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Replaced model that interfaces with fluid stream.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- January 2, 2017, by Filip Jorissen:<br/>
- Removed parameters
- <code>effInpEva</code> and <code>effInpCon</code>
- and updated documentation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- issue 497</a>.
- </li>
- <li>
- August 8, 2016, by Michael Wetter:<br/>
- Changed default temperature to compute COP to be the leaving temperature as
- use of the entering temperature can violate the 2nd law if the temperature
- lift is small.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- Annex 60, issue 497</a>.
- </li>
- <li>
- November 25, 2015 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 3, 2023, by Michael Wetter:<br/>
+Changed in base class the parameter binding
+<code>etaCarnot_nominal(unit=\"1\") = COP_nominal/(TUseAct_nominal/(TCon_nominal+TAppCon_nominal - (TEva_nominal-TAppEva_nominal)))</code>
+to
+<code>etaCarnot_nominal(unit=\"1\") = 0.3</code> to avoid a circular assignment.<br/>
+Improved documentation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3226\">Buildings, #3226</a>.
+</li>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Replaced model that interfaces with fluid stream.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+January 2, 2017, by Filip Jorissen:<br/>
+Removed parameters
+<code>effInpEva</code> and <code>effInpCon</code>
+and updated documentation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+issue 497</a>.
+</li>
+<li>
+August 8, 2016, by Michael Wetter:<br/>
+Changed default temperature to compute COP to be the leaving temperature as
+use of the entering temperature can violate the 2nd law if the temperature
+lift is small.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+Annex 60, issue 497</a>.
+</li>
+<li>
+November 25, 2015 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TEva;
diff --git a/AixLib/Fluid/Chillers/Carnot_y.mo b/AixLib/Fluid/Chillers/Carnot_y.mo
index 2df9e6f33f..e0e6701c66 100644
--- a/AixLib/Fluid/Chillers/Carnot_y.mo
+++ b/AixLib/Fluid/Chillers/Carnot_y.mo
@@ -7,161 +7,179 @@ model Carnot_y
   annotation (
 defaultComponentName="chi",
 Documentation(info="<html>
- <p>
- This is model of a chiller whose coefficient of performance COP changes
- with temperatures in the same way as the Carnot efficiency changes.
- The input signal <i>y</i> is the control signal for the compressor.
- </p>
- <p>
- The model allows to either specify the Carnot effectivness
- <i>&eta;<sub>Carnot,0</sub></i>, or
- a <i>COP<sub>0</sub></i>
- at the nominal conditions, together with
- the evaporator temperature <i>T<sub>eva,0</sub></i> and
- the condenser temperature <i>T<sub>con,0</sub></i>, in which
- case the model computes the Carnot effectivness as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &eta;<sub>Carnot,0</sub> =
-   COP<sub>0</sub>
- &frasl;  (T<sub>eva,0</sub> &frasl; (T<sub>con,0</sub>-T<sub>eva,0</sub>)).
- </p>
- <p>
- The chiller COP is computed as the product
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
- </p>
- <p>
- where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
- <i>&eta;<sub>PL</sub></i> is a polynomial in the cooling part load ratio <i>y<sub>PL</sub></i>
- that can be used to take into account a change in <i>COP</i> at part load
- conditions.
- This polynomial has the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y<sub>PL</sub> + a<sub>3</sub> y<sub>PL</sub><sup>2</sup> + ...
- </p>
- <p>
- where the coefficients <i>a<sub>i</sub></i>
- are declared by the parameter <code>a</code>.
- </p>
- <p>
- On the <code>Dynamics</code> tag, the model can be parametrized to compute a transient
- or steady-state response.
- The transient response of the model is computed using a first
- order differential equation for the evaporator and condenser fluid volumes.
- The chiller outlet temperatures are equal to the temperatures of these lumped volumes.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- When using this component, make sure that the evaporator and the condenser have sufficient mass flow rate.
- Based on the mass flow rates, the compressor power, temperature difference and the efficiencies,
- the model computes how much heat will be added to the condenser and removed at the evaporator.
- If the mass flow rates are too small, very high temperature differences can result.
- </p>
- <p>
- The evaporator heat flow rate <code>QEva_flow_nominal</code> is used to assign
- the default value for the mass flow rates, which are used for the pressure drop
- calculations.
- It is also used to compute the part load efficiency.
- Hence, make sure that <code>QEva_flow_nominal</code> is set to a reasonable value.
- </p>
- <p>
- The maximum cooling capacity is set by the parameter <code>QEva_flow_min</code>,
- which is by default set to negative infinity.
- </p>
- <p>
- The coefficient of performance depends on the
- evaporator and condenser leaving temperature
- since otherwise the second law of thermodynamics may be violated.
- </p>
- <h4>Notes</h4>
- <p>
- For a similar model that can be used as a heat pump, see
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">AixLib.Fluid.HeatPumps.Carnot_y</a>.
- </p>
- </html>",
+<p>
+This is a model of a chiller whose coefficient of performance COP changes
+with temperatures in the same way as the Carnot efficiency changes.
+The input signal <i>y</i> is the control signal for the compressor.
+</p>
+<p>
+Set <code>use_eta_Carnot_nominal=true</code> to specify directly
+the Carnot effectiveness <i>&eta;<sub>Carnot,0</sub></i>,
+in which case the value of the parameter <code>COP_nominal</code>
+will not affect the simulation.
+If <code>use_eta_Carnot_nominal=false</code>, the model will use
+the value of the parameter <code>COP_nominal</code>
+together with the specified nominal temperatures
+to compute the Carnot effectiveness as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&eta;<sub>Carnot,0</sub> =
+  COP<sub>0</sub>
+&frasl;  (T<sub>eva,0</sub> &frasl; (T<sub>con,0</sub> + T<sub>app,con,0</sub> - (T<sub>eva,0</sub>-T<sub>app,eva,0</sub>))),
+</p>
+<p>
+where
+<i>T<sub>eva,0</sub></i> is the evaporator temperature,
+<i>T<sub>con,0</sub></i> is the condenser temperature,
+<i>T<sub>app,eva,0</sub></i> is the evaporator approach temperature and
+<i>T<sub>app,con,0</sub></i> is the condenser approach temperature.
+</p>
+<p>
+The COP is computed as the product
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
+</p>
+<p>
+where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
+<i>&eta;<sub>PL</sub></i> is the part load efficiency, expressed using
+a polynomial.
+This polynomial has the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y + a<sub>3</sub> y<sup>2</sup> + ...,
+</p>
+<p>
+where <i>y &isin; [0, 1]</i> is
+the part load for cooling and the coefficients <i>a<sub>i</sub></i>
+are declared by the parameter <code>a</code>.
+</p>
+<p>
+On the <code>Dynamics</code> tag, the model can be parametrized to compute a transient
+or steady-state response.
+The transient response of the model is computed using a first
+order differential equation for the evaporator and condenser fluid volumes.
+The chiller outlet temperatures are equal to the temperatures of these lumped volumes.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+When using this component, make sure that the evaporator and the condenser have sufficient mass flow rate.
+Based on the mass flow rates, the compressor power, temperature difference and the efficiencies,
+the model computes how much heat will be added to the condenser and removed at the evaporator.
+If the mass flow rates are too small, very high temperature differences can result.
+</p>
+<p>
+The evaporator heat flow rate <code>QEva_flow_nominal</code> is used to assign
+the default value for the mass flow rates, which are used for the pressure drop
+calculations.
+It is also used to compute the part load efficiency.
+Hence, make sure that <code>QEva_flow_nominal</code> is set to a reasonable value.
+</p>
+<p>
+The maximum cooling capacity is set by the parameter <code>QEva_flow_min</code>,
+which is by default set to negative infinity.
+</p>
+<p>
+The coefficient of performance depends on the
+evaporator and condenser leaving temperature
+since otherwise the second law of thermodynamics may be violated.
+</p>
+<h4>Notes</h4>
+<p>
+For a similar model that can be used as a heat pump, see
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">AixLib.Fluid.HeatPumps.Carnot_y</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 2, 2017, by Filip Jorissen:<br/>
- Removed parameters
- <code>effInpEva</code> and <code>effInpCon</code>
- and updated documentation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- issue 497</a>.
- </li>
- <li>
- August 8, 2016, by Michael Wetter:<br/>
- Changed default temperature to compute COP to be the leaving temperature as
- use of the entering temperature can violate the 2nd law if the temperature
- lift is small.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- Annex 60, issue 497</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Refactored model to use the same base class as
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">AixLib.Fluid.HeatPumps.Carnot_y</a>.
- <br/>
- Changed part load efficiency to depend on cooling part load ratio rather than on the compressor
- part load ratio.<br/>
- Changed sign convention of <code>dTEva_nominal</code> to be negative rather than positive.
- For positive values, the simulation will stop with an assertion.
- </li>
- <li>
- December 18, 2015, by Michael Wetter:<br/>
- Corrected wrong computation of <code>staB1</code> and <code>staB2</code>
- which mistakenly used the <code>inStream</code> operator
- for the configuration without flow reversal.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/476\">
- issue 476</a>.
- </li>
- <li>
- November 25, 2015 by Michael Wetter:<br/>
- Changed sign convention for <code>dTEva_nominal</code> to be consistent with
- other models.
- The model will still work with the old values for <code>dTEva_nominal</code>,
- but it will write a warning so that users can transition their models.
- <br/>
- Corrected <code>assert</code> statement for the efficiency curve.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/468\">
- issue 468</a>.
- </li>
- <li>
- September 3, 2015 by Michael Wetter:<br/>
- Expanded documentation.
- </li>
- <li>
- May 6, 2015 by Michael Wetter:<br/>
- Added <code>prescribedHeatFlowRate=true</code> for <code>vol2</code>.
- </li>
- <li>
- October 9, 2013 by Michael Wetter:<br/>
- Reimplemented the computation of the port states to avoid using
- the conditionally removed variables <code>sta_a1</code>,
- <code>sta_a2</code>, <code>sta_b1</code> and <code>sta_b2</code>.
- </li>
- <li>
- May 10, 2013 by Michael Wetter:<br/>
- Added electric power <code>P</code> as an output signal.
- </li>
- <li>
- October 11, 2010 by Michael Wetter:<br/>
- Fixed bug in energy balance.
- </li>
- <li>
- March 3, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+February 3, 2023, by Michael Wetter:<br/>
+Changed in base class the parameter binding
+<code>etaCarnot_nominal(unit=\"1\") = COP_nominal/(TUseAct_nominal/(TCon_nominal+TAppCon_nominal - (TEva_nominal-TAppEva_nominal)))</code>
+to
+<code>etaCarnot_nominal(unit=\"1\") = 0.3</code> to avoid a circular assignment.<br/>
+Improved documentation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3226\">Buildings, #3226</a>.
+</li>
+<li>
+January 2, 2017, by Filip Jorissen:<br/>
+Removed parameters
+<code>effInpEva</code> and <code>effInpCon</code>
+and updated documentation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+issue 497</a>.
+</li>
+<li>
+August 8, 2016, by Michael Wetter:<br/>
+Changed default temperature to compute COP to be the leaving temperature as
+use of the entering temperature can violate the 2nd law if the temperature
+lift is small.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+Annex 60, issue 497</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Refactored model to use the same base class as
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">AixLib.Fluid.HeatPumps.Carnot_y</a>.
+<br/>
+Changed part load efficiency to depend on cooling part load ratio rather than on the compressor
+part load ratio.<br/>
+Changed sign convention of <code>dTEva_nominal</code> to be negative rather than positive.
+For positive values, the simulation will stop with an assertion.
+</li>
+<li>
+December 18, 2015, by Michael Wetter:<br/>
+Corrected wrong computation of <code>staB1</code> and <code>staB2</code>
+which mistakenly used the <code>inStream</code> operator
+for the configuration without flow reversal.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/476\">
+issue 476</a>.
+</li>
+<li>
+November 25, 2015 by Michael Wetter:<br/>
+Changed sign convention for <code>dTEva_nominal</code> to be consistent with
+other models.
+The model will still work with the old values for <code>dTEva_nominal</code>,
+but it will write a warning so that users can transition their models.
+<br/>
+Corrected <code>assert</code> statement for the efficiency curve.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/468\">
+issue 468</a>.
+</li>
+<li>
+September 3, 2015 by Michael Wetter:<br/>
+Expanded documentation.
+</li>
+<li>
+May 6, 2015 by Michael Wetter:<br/>
+Added <code>prescribedHeatFlowRate=true</code> for <code>vol2</code>.
+</li>
+<li>
+October 9, 2013 by Michael Wetter:<br/>
+Reimplemented the computation of the port states to avoid using
+the conditionally removed variables <code>sta_a1</code>,
+<code>sta_a2</code>, <code>sta_b1</code> and <code>sta_b2</code>.
+</li>
+<li>
+May 10, 2013 by Michael Wetter:<br/>
+Added electric power <code>P</code> as an output signal.
+</li>
+<li>
+October 11, 2010 by Michael Wetter:<br/>
+Fixed bug in energy balance.
+</li>
+<li>
+March 3, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
-        Line(points={{0,-70},{0,-90},{100,-90}}, color={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        Line(points={{0,-70},{0,-90},{100,-90}}, color={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_y;
diff --git a/AixLib/Fluid/Chillers/Examples/Carnot_TEva.mo b/AixLib/Fluid/Chillers/Examples/Carnot_TEva.mo
index 18f6240ff2..c27e369f67 100644
--- a/AixLib/Fluid/Chillers/Examples/Carnot_TEva.mo
+++ b/AixLib/Fluid/Chillers/Examples/Carnot_TEva.mo
@@ -26,7 +26,6 @@ model Carnot_TEva
     allowFlowReversal1=false,
     allowFlowReversal2=false,
     use_eta_Carnot_nominal=true,
-    etaCarnot_nominal=0.3,
     dp1_nominal=6000,
     dp2_nominal=6000) "Chiller model"
     annotation (Placement(transformation(extent={{10,-10},{30,10}})));
@@ -104,26 +103,32 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chiller
         "Simulate and plot"),
     Documentation(
 info="<html>
- <p>
- Example that simulates a chiller whose efficiency is scaled based on the
- Carnot cycle.
- The chiller takes as an input the evaporator leaving water temperature.
- The condenser mass flow rate is computed in such a way that it has
- a temperature difference equal to <code>dTEva_nominal</code>.
- </p>
- </html>",
+<p>
+Example that simulates a chiller whose efficiency is scaled based on the
+Carnot cycle.
+The chiller takes as an input the evaporator leaving water temperature.
+The condenser mass flow rate is computed in such a way that it has
+a temperature difference equal to <code>dTEva_nominal</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 25, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 10, 2023, by Michael Wetter:<br/>
+Removed binding of parameter with same value as the default.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1692\">#1692</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 25, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TEva;
diff --git a/AixLib/Fluid/Chillers/Examples/Carnot_y.mo b/AixLib/Fluid/Chillers/Examples/Carnot_y.mo
index 2df2de4dd8..ab9d96ec69 100644
--- a/AixLib/Fluid/Chillers/Examples/Carnot_y.mo
+++ b/AixLib/Fluid/Chillers/Examples/Carnot_y.mo
@@ -26,7 +26,6 @@ model Carnot_y "Test model for chiller based on Carnot_y efficiency"
     dTEva_nominal=dTEva_nominal,
     dTCon_nominal=dTCon_nominal,
     use_eta_Carnot_nominal=true,
-    etaCarnot_nominal=0.3,
     dp1_nominal=6000,
     dp2_nominal=6000,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
@@ -111,37 +110,43 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/Examples/Carnot_y.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 25, 2015 by Michael Wetter:<br/>
- Changed sign of <code>dTEva_nominal</code> to be consistent.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- March 26, 2013 by Michael Wetter:<br/>
- Removed assignment of parameter that had attribute <code>fixed=false</code>.
- </li>
- <li>
- March 3, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example that simulates a chiller whose efficiency is scaled based on the
- Carnot cycle.
- The chiller control signal is the compressor speed.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 10, 2023, by Michael Wetter:<br/>
+Removed binding of parameter with same value as the default.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1692\">#1692</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 25, 2015 by Michael Wetter:<br/>
+Changed sign of <code>dTEva_nominal</code> to be consistent.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+March 26, 2013 by Michael Wetter:<br/>
+Removed assignment of parameter that had attribute <code>fixed=false</code>.
+</li>
+<li>
+March 3, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example that simulates a chiller whose efficiency is scaled based on the
+Carnot cycle.
+The chiller control signal is the compressor speed.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_y;
diff --git a/AixLib/Fluid/Chillers/Examples/Chiller.mo b/AixLib/Fluid/Chillers/Examples/Chiller.mo
index 0c55920aa2..95d58a9c7a 100644
--- a/AixLib/Fluid/Chillers/Examples/Chiller.mo
+++ b/AixLib/Fluid/Chillers/Examples/Chiller.mo
@@ -84,8 +84,7 @@ model Chiller "Example for the reversible chiller model."
     offset=500,
     phase=3.1415926535898)
     annotation (Placement(transformation(extent={{76,56},{84,64}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm
-                                    pumSou(
+  Movers.SpeedControlled_y                                   pumSou(
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     redeclare final AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to8 per,
     final allowFlowReversal=true,
@@ -109,7 +108,8 @@ model Chiller "Example for the reversible chiller model."
         rotation=270,
         origin={86,2})));
 
-  Modelica.Blocks.Sources.Constant nIn(k=100) annotation (Placement(
+  Modelica.Blocks.Sources.Constant nIn(k=100/3040)
+                                              annotation (Placement(
         transformation(
         extent={{4,-4},{-4,4}},
         rotation=90,
@@ -164,20 +164,18 @@ model Chiller "Example for the reversible chiller model."
     annotation (Placement(transformation(extent={{10,-78},{0,-88}})));
 equation
 
-  connect(nIn.y, pumSou.Nrpm)
-    annotation (Line(points={{50,51.6},{50,46}}, color={0,0,127}));
   connect(Room.heatPort,heatFlowRateEva. port)
     annotation (Line(points={{86,12},{96,12},{96,18}},color={191,0,0}));
   connect(sine.y, gain.u) annotation (Line(points={{84.4,60},{92,60},{92,56.8},
           {96,56.8}}, color={0,0,127}));
   connect(heatFlowRateEva.Q_flow, gain.y) annotation (Line(points={{96,34},{96,
           47.6}},                   color={0,0,127}));
-  connect(Room.ports[1], pumSou.port_a) annotation (Line(points={{76,4},{76,26},
-          {60,26},{60,34}},color={0,127,255}));
+  connect(Room.ports[1], pumSou.port_a) annotation (Line(points={{76,3},{76,34},
+          {60,34}},        color={0,127,255}));
   connect(senTAct.port_b, sourceSideFixedBoundary.ports[1]) annotation (Line(
         points={{64,-38},{78,-38}},                   color={0,127,255}));
-  connect(senTAct.port_b, Room.ports[2]) annotation (Line(points={{64,-38},{66,-38},
-          {66,0},{76,0}},          color={0,127,255}));
+  connect(senTAct.port_b, Room.ports[2]) annotation (Line(points={{64,-38},{66,
+          -38},{66,1},{76,1}},     color={0,127,255}));
   connect(chiller.nSet, booleanToReal.y) annotation (Line(points={{-2.83333,
           -26.84},{-3,-26.84},{-3,-45.3}}, color={0,0,127}));
           connect(sinkSideMassFlowSource.ports[1], chiller.port_a1) annotation (Line(
@@ -208,6 +206,8 @@ equation
           -92},{16,-87},{11,-87}}, color={255,0,255}));
   connect(booleanStep.y, logicalSwitch.u2) annotation (Line(points={{23.2,-54},{
           14,-54},{14,-83},{11,-83}}, color={255,0,255}));
+  connect(nIn.y, pumSou.y)
+    annotation (Line(points={{50,51.6},{50,46}}, color={0,0,127}));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
             -100},{100,100}})),
     experiment(Tolerance=1e-6, StopTime=3600),
diff --git a/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/RefrigerantCycle.mo b/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/RefrigerantCycle.mo
new file mode 100644
index 0000000000..cd6b85477b
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/RefrigerantCycle.mo
@@ -0,0 +1,185 @@
+within AixLib.Fluid.Chillers.ModularReversible.BaseClasses;
+model RefrigerantCycle "Refrigerant cycle model of a chiller"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialModularRefrigerantCycle;
+
+  parameter Boolean allowDifferentDeviceIdentifiers=false
+    "if use_rev=true, device data for cooling and heating need to entered. Set allowDifferentDeviceIdentifiers=true to allow different device identifiers devIde"
+    annotation(Dialog(enable=use_rev));
+
+  replaceable model RefrigerantCycleChillerCooling =
+      AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.NoCooling(
+        useInChi=true)
+    constrainedby
+      AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle
+    "Replaceable model for refrigerant cycle of a chiller in main operation mode"
+    annotation (choicesAllMatching=true);
+
+  replaceable model RefrigerantCycleChillerHeating =
+      AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.NoHeating(
+        useInHeaPum=true)
+    constrainedby
+      AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle
+    "Replaceable model for refrigerant cycle of a chiller in reversed operation mode"
+    annotation (Dialog(enable=use_rev),choicesAllMatching=true);
+
+  RefrigerantCycleChillerCooling refCycChiCoo
+    "Refrigerant cycle instance for cooling"
+    annotation (Placement(transformation(extent={{21,40},{60,80}}, rotation=0)));
+  RefrigerantCycleChillerHeating refCycChiHea
+    "Refrigerant cycle instance for heating"
+    annotation (Placement(transformation(extent={{-60,38},{-19,80}}, rotation=0)));
+
+protected
+  parameter String devIde =
+    if use_rev then refCycChiHea.devIde else refCycChiCoo.devIde
+    "Data source for refrigerant cycle";
+
+initial algorithm
+  if not allowDifferentDeviceIdentifiers then
+    assert(
+      devIde == refCycChiCoo.devIde,
+      "In " + getInstanceName() + ": Device identifiers devIde for reversible operation are not equal.
+      Cooling device identifier is '" + refCycChiCoo.devIde + "' but heating is '"
+      + devIde + "'. To allow this, set 'allowDifferentDeviceIdentifiers=true'.",
+      AssertionLevel.error);
+  end if;
+equation
+  connect(pasTrhModSet.u, sigBus.coo);
+
+  connect(sigBus,refCycChiHea.sigBus)  annotation (Line(
+      points={{0,100},{0,92},{-39.3292,92},{-39.3292,80}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(sigBus,refCycChiCoo.sigBus)  annotation (Line(
+      points={{0,100},{0,92},{40.6625,92},{40.6625,80}},
+      color={255,204,51},
+      thickness=0.5));
+
+  connect(swiPEle.u2, sigBus.coo) annotation (Line(points={{2.22045e-15,-58},{
+          2.22045e-15,-2},{0,-2},{0,100}},
+                               color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(swiQEva.u2, sigBus.coo) annotation (Line(points={{-58,0},{0,0},{0,100}},
+        color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(swiQCon.u2, sigBus.coo) annotation (Line(points={{58,0},{0,0},{0,100}},
+        color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(refCycChiCoo.QEva_flow, swiQEva.u1) annotation (Line(points={{53.5,
+          38.3333},{53.5,24},{-10,24},{-10,8},{-58,8}}, color={0,0,127}));
+  connect(refCycChiCoo.QCon_flow, swiQCon.u1)
+    annotation (Line(points={{27.5,38.3333},{27.5,8},{58,8}}, color={0,0,127}));
+  connect(refCycChiCoo.PEle, swiPEle.u1) annotation (Line(points={{40.5,38.3333},
+          {40.5,-48},{8,-48},{8,-58}}, color={0,0,127}));
+  connect(refCycChiHea.PEle, swiPEle.u3) annotation (Line(points={{-39.5,36.25},{
+          -39.5,-48},{-8,-48},{-8,-58}}, color={0,0,127}));
+  connect(refCycChiHea.QCon_flow, swiQEva.u3) annotation (Line(points={{-53.1667,
+          36.25},{-53.1667,-8},{-58,-8}}, color={0,0,127}));
+  connect(refCycChiHea.QEva_flow, swiQCon.u3) annotation (Line(points={{-25.8333,
+          36.25},{-25.8333,-8},{58,-8}}, color={0,0,127}));
+
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={238,46,47},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-24,88},{22,44}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{-16,82},{20,74}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-18,52},{20,58}},
+          color={28,108,200},
+          thickness=0.5),
+        Rectangle(
+          extent={{-98,40},{-60,-28}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{-20,-60},{-20,-70},{-20,-80},{20,-60},{20,-80},{-20,-60}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-122,34},{-66,34},{-82,10},{-66,-22},{-120,-22}},
+          color={28,108,200},
+          thickness=0.5),
+        Rectangle(
+          extent={{60,40},{98,-28}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{120,34},{64,34},{80,10},{64,-22},{118,-22}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-80,40},{-80,68},{-24,68}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{22,66},{80,66},{80,40}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{78,-28},{78,-70}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{78,-70},{62,-70},{20,-70}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-80,-26},{-80,-68},{-20,-68}},
+          color={28,108,200},
+          thickness=0.5),
+        Text(
+          extent={{-151,147},{149,107}},
+          textColor={0,0,255},
+          fillPattern=FillPattern.HorizontalCylinder,
+          fillColor={0,127,255},
+          textString="%name")}), Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+  <ul>
+  <li>
+  May 2, 2024, by Michael Wetter:<br/>
+  Refactored check for device identifiers.<br/>
+  This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">IBPSA, #1576</a>.
+  </li>
+  <li>
+    <i>May 22, 2019,</i> by Julian Matthes:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/715\">AixLib #715</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Modular refrigerant cycle model for chiller applications used in
+  the model <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.Modular\">
+  AixLib.Fluid.Chillers.ModularReversible.Modular</a> and extending models
+  of the modular approach.
+</p>
+<p>
+  This model adds the replaceable model approaches for cooling and heating data
+  to the partial refrigerant cylce.
+</p>
+<p>
+  Further, an asseration warning is raised if the model approaches or
+  sources for performance data differ. This indicates that they are not
+  for the same device.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end RefrigerantCycle;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/package.mo b/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/package.mo
new file mode 100644
index 0000000000..abedfbfc94
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+package BaseClasses "Package with base classes for AixLib.Fluid.Chillers.ModularReversible"
+  extends Modelica.Icons.BasesPackage;
+
+  annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains base classes that are used to construct the models in
+<a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible\">AixLib.Fluid.Chillers.ModularReversible</a>.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/package.order b/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/package.order
new file mode 100644
index 0000000000..6d3b42a60a
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/BaseClasses/package.order
@@ -0,0 +1 @@
+RefrigerantCycle
diff --git a/AixLib/Fluid/Chillers/ModularReversible/CarnotWithLosses.mo b/AixLib/Fluid/Chillers/ModularReversible/CarnotWithLosses.mo
new file mode 100644
index 0000000000..cf59236d97
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/CarnotWithLosses.mo
@@ -0,0 +1,93 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+model CarnotWithLosses
+  "Reversible chiller using Carnot approach with losses (frost, heat, inertia)"
+  extends AixLib.Fluid.Chillers.ModularReversible.Modular(
+    QHea_flow_nominal=PEle_nominal*refCyc.refCycChiHea.COP_nominal,
+    redeclare model RefrigerantCycleChillerHeating =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness
+        (
+        PEle_nominal=PEle_nominal,
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+          iceFacCal,
+        etaCarnot_nominal=etaCarnot_nominal,
+        use_constAppTem=true,
+        TAppCon_nominal=TAppCon_nominal,
+        TAppEva_nominal=TAppEva_nominal),
+    redeclare model RefrigerantCycleChillerCooling =
+        AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness
+        (
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.FunctionalIcingFactor
+          iceFacCal(redeclare function icingFactor =
+              AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.Functions.wetterAfjei1997),
+        TAppCon_nominal=TAppCon_nominal,
+        TAppEva_nominal=TAppEva_nominal,
+        etaCarnot_nominal=etaCarnot_nominal),
+    final allowDifferentDeviceIdentifiers=false,
+    redeclare model RefrigerantCycleInertia =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.VariableOrder
+        (
+        final refIneFreConst=1/refIneTimCon,
+        final nthOrd=1,
+        initType=Modelica.Blocks.Types.Init.InitialOutput));
+
+  parameter Real etaCarnot_nominal=0.3 "Constant Carnot effectiveness";
+  parameter Modelica.Units.SI.TemperatureDifference TAppCon_nominal=if
+      cpCon < 1500 then 5 else 2
+    "Temperature difference between refrigerant and working fluid outlet in condenser"
+    annotation(Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.TemperatureDifference TAppEva_nominal=if
+      cpEva < 1500 then 5 else 2
+    "Temperature difference between refrigerant and working fluid outlet in evaporator"
+    annotation(Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.Time refIneTimCon = 300
+    "Refrigerant cycle inertia time constant for first order delay"
+    annotation(Dialog(group="Refrigerant cycle inertia"));
+  parameter Integer nthOrd=1 "Order of refrigerant cycle interia"
+    annotation(Dialog(group="Refrigerant cycle inertia"));
+
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>", info="<html>
+<p>
+  Model of a reversible chiller.
+</p>
+<p>
+  This model extends
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.Modular\">
+  AixLib.Fluid.Chillers.ModularReversible.Modular</a> and selects the
+  constant Carnot effectiveness module for chillers
+  (<a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness\">
+  AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness</a>)
+  and heat pumps
+  (<a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness</a>)
+  to model a reversible chiller.
+  For the heating operation, the nominal approach temperatures are used
+  as a constant to avoid nonlinear system of equations.
+</p>
+<p>
+  Furthermore, losses are enabled to model
+  the chiller with a more realistic behaviour:
+</p>
+<ul>
+<li>Heat losses to the ambient (can be disabled)</li>
+<li>Refrigerant inertia using a first order delay</li>
+<li>Evaporator frosting assuming an air-sink chiller</li>
+</ul>
+<p>
+For more information, see
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CarnotWithLosses;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/OperationalEnvelope.mo b/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/OperationalEnvelope.mo
new file mode 100644
index 0000000000..15fdbe35f4
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/OperationalEnvelope.mo
@@ -0,0 +1,79 @@
+within AixLib.Fluid.Chillers.ModularReversible.Controls.Safety;
+model OperationalEnvelope
+  "Indicates if the chiller operation is within a defined envelope"
+  extends
+    HeatPumps.ModularReversible.Controls.Safety.BaseClasses.PartialOperationalEnvelope;
+  Modelica.Blocks.Logical.Not notCoo "=true for heating" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-50,0})));
+equation
+    if use_TEvaOutHea then
+    connect(bouMapHea.TUseSid, sigBus.TEvaOutMea) annotation (Line(points={{-84.2,
+            82},{-104,82},{-104,-61},{-119,-61}},                       color={0,
+            0,127}));
+  else
+    connect(bouMapHea.TUseSid, sigBus.TEvaInMea) annotation (Line(points={{-84.2,
+            82},{-104,82},{-104,-61},{-119,-61}},                       color={0,
+            0,127}));
+  end if;
+  if use_TConOutCoo then
+    connect(bouMapCoo.TAmbSid, sigBus.TConOutMea) annotation (Line(points={{-84.8,
+            -62},{-104,-62},{-104,-61},{-119,-61}},
+                                                color={0,0,127}));
+  else
+    connect(bouMapCoo.TAmbSid, sigBus.TConInMea) annotation (Line(points={{-84.8,
+            -62},{-104,-62},{-104,-61},{-119,-61}},
+                                                color={0,0,127}));
+  end if;
+  if use_TConOutHea then
+    connect(bouMapHea.TAmbSid, sigBus.TConOutMea) annotation (Line(points={{-84.8,
+            58},{-104,58},{-104,-60},{-106,-60},{-106,-61},{-119,-61}},
+                                                color={0,0,127}));
+  else
+    connect(bouMapHea.TAmbSid, sigBus.TConInMea) annotation (Line(points={{-84.8,
+            58},{-104,58},{-104,-60},{-112,-60},{-112,-61},{-119,-61}},
+                                                color={0,0,127}));
+  end if;
+  if use_TEvaOutCoo then
+    connect(bouMapCoo.TUseSid, sigBus.TEvaOutMea) annotation (Line(points={{-84.2,
+            -38},{-104,-38},{-104,-60},{-112,-60},{-112,-61},{-119,-61}},
+                                                      color={0,0,127}));
+  else
+    connect(bouMapCoo.TUseSid, sigBus.TEvaInMea) annotation (Line(points={{-84.2,
+            -38},{-104,-38},{-104,-60},{-112,-60},{-112,-61},{-119,-61}},
+                                                      color={0,0,127}));
+  end if;
+  connect(notCoo.y, swiHeaCoo.u2)
+    annotation (Line(points={{-39,0},{-6,0}}, color={255,0,255}));
+  connect(notCoo.u, sigBus.coo) annotation (Line(points={{-62,0},{-70,0},{-70,
+          -8},{-104,-8},{-104,-60},{-112,-60},{-112,-61},{-119,-61}},
+                       color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  annotation (Diagram(coordinateSystem(extent={{-120,-120},{120,120}})),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Model to check if the operating conditions of a chiller are inside
+  the given boundaries. If not, the heat pump or chiller will switch off.
+</p>
+<p>
+  Read the documentation of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.PartialOperationalEnvelope\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.PartialOperationalEnvelope</a>
+  for more information.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end OperationalEnvelope;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/package.mo b/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/package.mo
new file mode 100644
index 0000000000..7c04449299
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/package.mo
@@ -0,0 +1,36 @@
+within AixLib.Fluid.Chillers.ModularReversible.Controls;
+package Safety "Contains typical safety controllers for chillers"
+  extends Modelica.Icons.Package;
+
+  annotation (Icon(graphics={
+        Ellipse(
+          extent={{-48,-12},{48,80}},
+          lineColor={0,0,0},
+          fillColor={91,91,91},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-36,0},{36,68}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-60,34},{60,-66}},
+          lineColor={0,0,0},
+          fillColor={91,91,91},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-10,-16},{10,-56}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-14,-26},{16,2}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Documentation(info="<html>
+<p>
+  Package with safety controls typically
+  applied in chiller devices.
+</p>
+</html>"));
+end Safety;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/package.order b/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/package.order
new file mode 100644
index 0000000000..85f0324561
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Controls/Safety/package.order
@@ -0,0 +1 @@
+OperationalEnvelope
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Controls/package.mo b/AixLib/Fluid/Chillers/ModularReversible/Controls/package.mo
new file mode 100644
index 0000000000..00f191fcad
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Controls/package.mo
@@ -0,0 +1,38 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+package Controls "Package of control sequences"
+  extends Modelica.Icons.Package;
+
+  annotation (
+    preferredView="info",
+    Documentation(
+      info="<html>
+<p>
+This package contains control logic for the chiller internal controls.
+</p>
+</html>"),
+Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100.0,-100.0},{100.0,100.0}}), graphics={
+      Rectangle(
+        origin={0.0,35.1488},
+        fillColor={255,255,255},
+        extent={{-30.0,-20.1488},{30.0,20.1488}}),
+      Rectangle(
+        origin={0.0,-34.8512},
+        fillColor={255,255,255},
+        extent={{-30.0,-20.1488},{30.0,20.1488}}),
+      Line(
+        origin={-51.25,0.0},
+        points={{21.25,-35.0},{-13.75,-35.0},{-13.75,35.0},{6.25,35.0}}),
+      Polygon(
+        origin={-40.0,35.0},
+        pattern=LinePattern.None,
+        fillPattern=FillPattern.Solid,
+        points={{10.0,0.0},{-5.0,5.0},{-5.0,-5.0}}),
+      Line(
+        origin={51.25,0.0},
+        points={{-21.25,35.0},{13.75,35.0},{13.75,-35.0},{-6.25,-35.0}}),
+      Polygon(
+        origin={40.0,-35.0},
+        pattern=LinePattern.None,
+        fillPattern=FillPattern.Solid,
+        points={{-10.0,0.0},{5.0,5.0},{5.0,-5.0}})}));
+end Controls;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Controls/package.order b/AixLib/Fluid/Chillers/ModularReversible/Controls/package.order
new file mode 100644
index 0000000000..64ee735bc3
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Controls/package.order
@@ -0,0 +1 @@
+Safety
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/Carrier30XWP1012_1MW.mo b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/Carrier30XWP1012_1MW.mo
new file mode 100644
index 0000000000..dcc57ab894
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/Carrier30XWP1012_1MW.mo
@@ -0,0 +1,50 @@
+within AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.EN14511;
+record Carrier30XWP1012_1MW
+  "Carrier 30XW-P 1012 with roughly 1 MW cooling output"
+  extends AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic(
+    tabQEva_flow=[0,298.15,303.15,308.15,313.15,318.15; 278.15,-1003000,-968000,
+        -932000,-894000,-854000; 280.15,-1054000,-1035000,-995000,-954000,-911000; 283.15,
+        -1102000,-1120000,-1096000,-1050000,-1002000; 288.15,-1181000,-1199000,-1226000,
+        -1227000,-1170000; 291.15,-1227000,-1244000,-1275000,-1311000,-1278000],
+    tabPEle=[0,298.15,303.15,308.15,313.15,318.15; 278.15,158954,181955,208036,
+        237766,271111; 280.15,159215,182218,208159,237905,271131; 283.15,159479,
+        182708,208762,238095,271545; 288.15,160462,183333,209573,239648,272727;
+        291.15,161024,183752,210396,240550,274249],
+    mCon_flow_nominal=49.85,
+    mEva_flow_nominal=49.85,
+    dpCon_nominal=32000,
+    dpEva_nominal=44000,
+    tabLowBou=[293.15,276.15; 323.15,276.15],
+    devIde="Carrier30XWP1012",
+    use_TConOutForOpeEnv=true,
+    use_TEvaOutForOpeEnv=true,
+    use_TConOutForTab=false,
+    use_TEvaOutForTab=true);
+
+  annotation (
+    Icon(coordinateSystem(preserveAspectRatio=false)),
+    Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+  Performance data for Daikin FTXM20R_RXM20R for the cooling mode.
+</p>
+<p>
+  Boundaries are for dry-bulb temperature.
+</p>
+<h4>References</h4>
+<p>
+Carrier, Water-Cooled Liquid Chillers Pro-Dialog plus, 30XW- 30XWHDaikin
+<a href=\"http://www.carrier.com.kw/pdf/pdf/Chilled%20Water%20Products/30XW.pdf\">
+http://www.carrier.com.kw/pdf/pdf/Chilled%20Water%20Products/30XW.pdf</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Carrier30XWP1012_1MW;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/SingleSplitRXM20R.mo b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/SingleSplitRXM20R.mo
new file mode 100644
index 0000000000..e89c85b247
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/SingleSplitRXM20R.mo
@@ -0,0 +1,51 @@
+within AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.EN14511;
+record SingleSplitRXM20R "Daikin_FTXM20R_RXM20R cooling mode"
+  extends AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic(
+    dpEva_nominal=0,
+    dpCon_nominal=0,
+    tabPEle=[0,298.15,303.15,308.15,313.15; 293.15,340,370,400,410,430,470;
+        295.15,340,370,400,420,430,470; 298.15,340,370,400,420,440,470; 300.15,
+        340,370,410,420,440,470; 303.15,340,380,410,420,440,470; 305.15,350,380,
+        410,420,440,470],
+    tabQEva_flow=[0,298.15,303.15,308.15,313.15; 293.15,-2050,-1960,-1860,-1830,-1770,
+        -1680; 295.15,-2140,-2050,-1950,-1920,-1860,-1770; 298.15,-2230,-2140,-2050,-2010,
+        -1950,-1860; 300.15,-2280,-2190,-2090,-2060,-2000,1910; 303.15,-2420,-2320,-2230,
+        -2190,-2140,-2050; 305.15,-2510,-2420,-2320,-2290,-2230,-2140],
+    mCon_flow_nominal=36*1.2/60,
+    mEva_flow_nominal=(9.642*1.2)/60,
+    tabLowBou=[263.15,291.15; 323.15,291.15],
+    devIde="DaikinRXM20R",
+    use_TConOutForOpeEnv=false,
+    use_TEvaOutForOpeEnv=false,
+    use_TConOutForTab=false,
+    use_TEvaOutForTab=false);
+
+  annotation (
+    Icon(coordinateSystem(preserveAspectRatio=false)),
+    Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+  Performance data for Daikin FTXM20R_RXM20R for the cooling mode.
+</p>
+<p>
+  Boundaries are for dry-bulb temperature. Pressure drops are not provided
+  in the datasheet.
+</p>
+<h4>References</h4>
+<p>
+Daikin, Technical data book RXM-R
+<a href=\"https://www.heizman24.de/media/pdf/fa/50/2c/Daikin-RXM-R-Produktdatenbuch.pdf\">
+https://www.heizman24.de/media/pdf/fa/50/2c/Daikin-RXM-R-Produktdatenbuch.pdf</a>
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end SingleSplitRXM20R;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/Vitocal251A08.mo b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/Vitocal251A08.mo
new file mode 100644
index 0000000000..bdf8457e99
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/Vitocal251A08.mo
@@ -0,0 +1,47 @@
+within AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.EN14511;
+record Vitocal251A08 "A2W Vitocal 251 by Viessmann"
+  extends AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic(
+    tabLowBou=[283.15,280.15; 318.15,280.15],
+    dpEva_nominal=0,
+    dpCon_nominal=0,
+    use_TConOutForOpeEnv=false,
+    use_TEvaOutForOpeEnv=true,
+    tabQEva_flow=[
+      0, 293.15, 298.15, 300.15, 303.15, 308.15, 313.15, 318.15;
+      280.15, -8500, -7800, -7000, -6000, -4500, -3100, -1900;
+      291.15, -10300, -9900, -9700, -9300, -6900, -3400, -2800],
+    tabPEle=[
+      0, 293.15, 298.15, 300.15, 303.15, 308.15, 313.15, 318.15;
+      280.15, 1735, 1902, 1842, 1765, 1607, 1348, 1056;
+      291.15, 1493, 1707, 1764, 1860, 1725, 1259, 1037],
+    mEva_flow_nominal=5600/5/4184,
+    mCon_flow_nominal=2125/3600/1.204,
+    use_TConOutForTab=false,
+    use_TEvaOutForTab=true,
+    devIde="Vitocal251A08");
+  annotation (Documentation(info="<html>
+<p>
+  Data from the planning book (Planungshandbuch) from Viessmann.
+</p>
+<p>
+  While the product exists in different sizes,
+  this record contains the data for the subtype 251-A08.
+  If you want to model the pressure losses of the device,
+  check out the data sheet and the installed pumps.
+  The pressure loss depends mostly on the hydraulic system
+  according to the datasheet.
+</p>
+<p>
+  The nominal mass flow rate is calculated for the nominal point A7/W35,
+  with a temperature spread of 5 K.
+</p>
+<h4>References</h4>
+<p>
+Viessmann, Planungshandbuch.
+<a href=\"https://www.haustechnik-handrich.de/media/pdf/54/c4/14/vie-pa-z022164.pdf\">
+https://www.haustechnik-handrich.de/media/pdf/54/c4/14/vie-pa-z022164.pdf</a>.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Vitocal251A08;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/package.mo b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/package.mo
new file mode 100644
index 0000000000..bfa2d1ca42
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/package.mo
@@ -0,0 +1,23 @@
+within AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D;
+package EN14511 "Package for EN15411 data records"
+
+annotation (preferredView="info",
+Documentation(revisions="<html><ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  Adapted based on AixLib implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+<li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This package contains data records for chiller
+  data according to European Norm 14511.
+</p>
+</html>"));
+end EN14511;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/package.order b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/package.order
new file mode 100644
index 0000000000..d2dbb701ac
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/EN14511/package.order
@@ -0,0 +1,3 @@
+Carrier30XWP1012_1MW
+SingleSplitRXM20R
+Vitocal251A08
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/Generic.mo b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/Generic.mo
new file mode 100644
index 0000000000..be03ffecc1
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/Generic.mo
@@ -0,0 +1,38 @@
+within AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D;
+record Generic "Basic chiller data"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.Generic;
+
+  parameter Real tabQEva_flow[:,:]
+    "Cooling power consumption table, T in K, Q_flow in W";
+  parameter Real tabLowBou[:,2]
+    "Points to define lower boundary for source temperature";
+  parameter Boolean use_TEvaOutForOpeEnv=false
+    "=true to use evaporator outlet temperature for operational envelope, false for inlet";
+  parameter Boolean use_TConOutForOpeEnv=false
+    "=true to use condenser outlet temperature for operational envelope, false for inlet";
+  annotation (Documentation(info="<html>
+
+  <h4>Overview</h4>
+<p>
+  Base data definition used in the chiller model.
+</p>
+<p>
+  It extends <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.Generic\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2DData.RefrigerantCycle2DBaseDataDefinition</a>
+  to restrict to intended selections.</p>
+<p>
+  It adds the table data for lower temperature limits
+  which serves as the operational envelope of the compressor.
+</p>
+</html>",
+        revisions="<html><ul>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>"),
+   Icon, 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generic;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/package.mo b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/package.mo
new file mode 100644
index 0000000000..c9dce3c6b7
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.Chillers.ModularReversible.Data;
+package TableData2D "Package with two-dimensional data"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+  annotation (preferredView="info",
+  Documentation(info="<html>
+<p>
+  This package contains data records for chiller
+  data with two-dimensional tables.
+</p>
+</html>"));
+end TableData2D;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/package.order b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/package.order
new file mode 100644
index 0000000000..95701f8e32
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/TableData2D/package.order
@@ -0,0 +1,2 @@
+Generic
+EN14511
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/package.mo b/AixLib/Fluid/Chillers/ModularReversible/Data/package.mo
new file mode 100644
index 0000000000..e7e61e60d8
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/package.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+package Data "Package for data records"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains data records for chillers.
+</p>
+</html>"));
+end Data;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Data/package.order b/AixLib/Fluid/Chillers/ModularReversible/Data/package.order
new file mode 100644
index 0000000000..45578af2cf
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Data/package.order
@@ -0,0 +1 @@
+TableData2D
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Examples/CarnotWithLosses.mo b/AixLib/Fluid/Chillers/ModularReversible/Examples/CarnotWithLosses.mo
new file mode 100644
index 0000000000..d1bb7dfc7d
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Examples/CarnotWithLosses.mo
@@ -0,0 +1,135 @@
+within AixLib.Fluid.Chillers.ModularReversible.Examples;
+model CarnotWithLosses
+  "Example for reversible Carnot chiller model"
+  extends Modelica.Icons.Example;
+  package MediumCon = AixLib.Media.Water "Medium model for condenser";
+  package MediumEva = AixLib.Media.Water "Medium model for evaporator";
+
+  AixLib.Fluid.Chillers.ModularReversible.CarnotWithLosses chi(
+    redeclare package MediumCon = MediumCon,
+    redeclare package MediumEva = MediumEva,
+    QCoo_flow_nominal=-30000,
+    redeclare
+      AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021
+      safCtrPar(
+      minOffTime=100,
+      use_maxCycRat=false,
+      tabUppHea=[263.15,313.15; 333.15,313.15],
+      tabLowCoo=[263.15,283.15; 333.15,283.15],
+      use_TEvaOutCoo=true),
+    TConCoo_nominal=313.15,
+    dpCon_nominal(displayUnit="Pa") = 6000,
+    use_conCap=false,
+    CCon=0,
+    GConOut=0,
+    GConIns=0,
+    TEvaCoo_nominal=278.15,
+    dTEva_nominal(displayUnit="K") = 10,
+    dTCon_nominal(displayUnit="K") = 5,
+    dpEva_nominal(displayUnit="Pa") = 6000,
+    use_evaCap=false,
+    CEva=0,
+    GEvaOut=0,
+    GEvaIns=0,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    show_T=true,
+    QHea_flow_nominal=40000,
+    TConHea_nominal=293.15,
+    TEvaHea_nominal=303.15)
+                 "Chiller instance with reversbile Carnot approach"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  AixLib.Fluid.Sources.MassFlowSource_T souCon(
+    nPorts=1,
+    redeclare package Medium = MediumCon,
+    use_T_in=true,
+    m_flow=chi.mCon_flow_nominal,
+    T=298.15) "Condenser source"
+    annotation (Placement(transformation(extent={{-60,6},{-40,26}})));
+  AixLib.Fluid.Sources.MassFlowSource_T souEva(
+    nPorts=1,
+    redeclare package Medium = MediumEva,
+    use_T_in=true,
+    m_flow=chi.mEva_flow_nominal,
+    T=291.15) "Evaporator source"
+    annotation (Placement(transformation(extent={{60,-6},{40,14}})));
+  AixLib.Fluid.Sources.Boundary_pT sinCon(nPorts=1, redeclare package Medium =
+        MediumCon) "Condenser sink" annotation (Placement(transformation(extent={{
+            10,-10},{-10,10}}, origin={70,40})));
+  AixLib.Fluid.Sources.Boundary_pT sinEva(nPorts=1, redeclare package Medium =
+        MediumEva) "Evaporator sink" annotation (Placement(transformation(extent={
+            {-10,-10},{10,10}}, origin={-50,-20})));
+  Modelica.Blocks.Sources.SawTooth ySet(
+    amplitude=-1,
+    period=500,
+    offset=1,
+    startTime=500)  "Compressor control signal"
+    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
+  Modelica.Blocks.Sources.Ramp TConIn(
+    height=10,
+    duration=60,
+    offset=273.15 + 30,
+    startTime=60) "Condenser inlet temperature"
+    annotation (Placement(transformation(extent={{-90,10},{-70,30}})));
+  Modelica.Blocks.Sources.Ramp TEvaIn(
+    height=10,
+    duration=60,
+    startTime=900,
+    offset=273.15 + 15) "Evaporator inlet temperature"
+    annotation (Placement(transformation(extent={{52,-40},{72,-20}})));
+equation
+  connect(souCon.ports[1], chi.port_a1) annotation (Line(
+      points={{-40,16},{-20,16},{-20,16},{-5.55112e-16,16}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(souEva.ports[1], chi.port_a2) annotation (Line(
+      points={{40,4},{30,4},{30,4},{20,4}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(chi.port_b1, sinCon.ports[1]) annotation (Line(
+      points={{20,16},{30,16},{30,40},{60,40}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(sinEva.ports[1], chi.port_b2) annotation (Line(
+      points={{-40,-20},{-10,-20},{-10,4},{-5.55112e-16,4}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TConIn.y, souCon.T_in) annotation (Line(
+      points={{-69,20},{-62,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(TEvaIn.y, souEva.T_in) annotation (Line(
+      points={{73,-30},{80,-30},{80,8},{62,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ySet.y, chi.ySet) annotation (Line(points={{-39,60},{-16,60},{-16,
+          11.9},{-1.1,11.9}},            color={0,0,127}));
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/CarnotWithLosses.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>", info="<html>
+<p>
+  Example that simulates a chiller based on the modular reversible approach
+  using the
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.CarnotWithLosses\">
+  AixLib.Fluid.Chillers.ModularReversible.CarnotWithLosses</a>.
+  model directly.
+  The chiller control signal is the compressor speed
+  <code>ySet</code> and the mode <code>coo</code>.
+</p>
+<p>
+  As the model contains internal safety controls, the
+  compressor set speed <code>ySet</code> and actually applied
+  speed <code>yMea</code> are plotted to show the influence of
+  the safety control.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CarnotWithLosses;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Examples/LargeScaleWaterToWater.mo b/AixLib/Fluid/Chillers/ModularReversible/Examples/LargeScaleWaterToWater.mo
new file mode 100644
index 0000000000..c80b243e03
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Examples/LargeScaleWaterToWater.mo
@@ -0,0 +1,119 @@
+within AixLib.Fluid.Chillers.ModularReversible.Examples;
+model LargeScaleWaterToWater
+  "Example for large scale water to water chiller"
+  extends Modelica.Icons.Example;
+  package MediumCon = AixLib.Media.Water "Medium model for condenser";
+  package MediumEva = AixLib.Media.Water "Medium model for evaporator";
+
+  AixLib.Fluid.Chillers.ModularReversible.LargeScaleWaterToWater chi(
+    redeclare
+      AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.EN14511.Carrier30XWP1012_1MW
+      datTab,
+    redeclare AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021
+      safCtrPar,
+    redeclare package MediumCon = MediumCon,
+    redeclare package MediumEva = MediumEva,
+    QCoo_flow_nominal=-1000000,
+    TConCoo_nominal=313.15,
+    dpCon_nominal(displayUnit="Pa") = 6000,
+    TEvaCoo_nominal=278.15,
+    dpEva_nominal(displayUnit="Pa") = 6000,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial)
+    "Large scale water to water chiller"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  AixLib.Fluid.Sources.MassFlowSource_T souCon(
+    nPorts=1,
+    redeclare package Medium = MediumCon,
+    use_T_in=true,
+    m_flow=chi.mCon_flow_nominal,
+    T=298.15) "Condenser source"
+    annotation (Placement(transformation(extent={{-60,6},{-40,26}})));
+  AixLib.Fluid.Sources.MassFlowSource_T souEva(
+    nPorts=1,
+    redeclare package Medium = MediumEva,
+    use_T_in=true,
+    m_flow=chi.mEva_flow_nominal,
+    T=291.15) "Evaporator source"
+    annotation (Placement(transformation(extent={{60,-6},{40,14}})));
+  AixLib.Fluid.Sources.Boundary_pT sinCon(nPorts=1, redeclare package Medium =
+        MediumCon) "Condenser sink" annotation (Placement(transformation(extent={{
+            10,-10},{-10,10}}, origin={70,40})));
+  AixLib.Fluid.Sources.Boundary_pT sinEva(nPorts=1, redeclare package Medium =
+        MediumEva) "Evaporator sink" annotation (Placement(transformation(extent={
+            {-10,-10},{10,10}}, origin={-50,-20})));
+  Modelica.Blocks.Sources.Ramp ySet(
+    height=-1,
+    duration=900,
+    offset=1,
+    startTime=1800) "Compressor control signal"
+    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
+  Modelica.Blocks.Sources.Ramp TConIn(
+    height=10,
+    duration=60,
+    offset=273.15 + 30,
+    startTime=60) "Condenser inlet temperature"
+    annotation (Placement(transformation(extent={{-90,10},{-70,30}})));
+  Modelica.Blocks.Sources.Ramp TEvaIn(
+    height=10,
+    duration=60,
+    startTime=900,
+    offset=273.15 + 15) "Evaporator inlet temperature"
+    annotation (Placement(transformation(extent={{52,-40},{72,-20}})));
+equation
+  connect(souCon.ports[1], chi.port_a1) annotation (Line(
+      points={{-40,16},{-20,16},{-20,16},{-5.55112e-16,16}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(souEva.ports[1], chi.port_a2) annotation (Line(
+      points={{40,4},{30,4},{30,4},{20,4}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(chi.port_b1, sinCon.ports[1]) annotation (Line(
+      points={{20,16},{30,16},{30,40},{60,40}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(sinEva.ports[1], chi.port_b2) annotation (Line(
+      points={{-40,-20},{-10,-20},{-10,4},{-5.55112e-16,4}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TConIn.y, souCon.T_in) annotation (Line(
+      points={{-69,20},{-62,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(TEvaIn.y, souEva.T_in) annotation (Line(
+      points={{73,-30},{80,-30},{80,8},{62,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ySet.y, chi.ySet) annotation (Line(points={{-39,60},{-16,60},{-16,12},{-1.2,
+          12}},                              color={0,0,127}));
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/LargeScaleWaterToWater.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>", info="<html>
+<p>
+  Example that simulates a chiller based on the modular reversible approach
+  using the
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.LargeScaleWaterToWater\">
+  AixLib.Fluid.Chillers.ModularReversible.LargeScaleWaterToWater</a>.
+  model directly.
+  The chiller control signal is the compressor speed
+  <code>ySet</code> and the mode <code>coo</code>.
+</p>
+<p>
+  As the model contains internal safety controls, the
+  compressor set speed <code>ySet</code> and actually applied
+  speed <code>yMea</code> are plotted to show the influence of
+  the safety control.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end LargeScaleWaterToWater;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Examples/Modular.mo b/AixLib/Fluid/Chillers/ModularReversible/Examples/Modular.mo
new file mode 100644
index 0000000000..bdbf293385
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Examples/Modular.mo
@@ -0,0 +1,154 @@
+within AixLib.Fluid.Chillers.ModularReversible.Examples;
+model Modular
+  "Example for modular reversible chiller"
+  extends Modelica.Icons.Example;
+  package MediumCon = AixLib.Media.Air "Medium model for condenser";
+  package MediumEva = AixLib.Media.Water "Medium model for evaporator";
+
+  AixLib.Fluid.Chillers.ModularReversible.Modular chi(
+    redeclare package MediumCon = MediumCon,
+    redeclare package MediumEva = MediumEva,
+    use_rev=true,
+    allowDifferentDeviceIdentifiers=true,
+    QCoo_flow_nominal=-30000,
+    redeclare model RefrigerantCycleInertia =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.VariableOrder
+        (
+        refIneFreConst=1/300,
+        nthOrd=1,
+        initType=Modelica.Blocks.Types.Init.InitialState),
+    redeclare
+      AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021
+      safCtrPar(minOffTime=100, use_opeEnv=false),
+    TConCoo_nominal=313.15,
+    dpCon_nominal(displayUnit="Pa") = 6000,
+    use_conCap=false,
+    CCon=0,
+    GConOut=0,
+    GConIns=0,
+    TEvaCoo_nominal=278.15,
+    dTEva_nominal=5,
+    dTCon_nominal=5,
+    dpEva_nominal(displayUnit="Pa") = 6000,
+    use_evaCap=false,
+    CEva=0,
+    GEvaOut=0,
+    GEvaIns=0,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    show_T=true,
+    QHea_flow_nominal=30000,
+    redeclare model RefrigerantCycleChillerCooling =
+        AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness
+        (etaCarnot_nominal=0.35),
+    redeclare model RefrigerantCycleChillerHeating =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D (
+          redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+          iceFacCal, datTab=
+            AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.EN14511.Vitocal251A08()),
+    TEvaHea_nominal=303.15,
+    TConHea_nominal=298.15)
+                 "Modular reversible chiller instance"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  AixLib.Fluid.Sources.MassFlowSource_T souCon(
+    nPorts=1,
+    redeclare package Medium = MediumCon,
+    use_T_in=true,
+    m_flow=chi.mCon_flow_nominal,
+    T=298.15) "Condenser source"
+    annotation (Placement(transformation(extent={{-60,6},{-40,26}})));
+  AixLib.Fluid.Sources.MassFlowSource_T souEva(
+    nPorts=1,
+    redeclare package Medium = MediumEva,
+    use_T_in=true,
+    m_flow=chi.mEva_flow_nominal,
+    T=291.15) "Evaporator source"
+    annotation (Placement(transformation(extent={{60,-6},{40,14}})));
+  AixLib.Fluid.Sources.Boundary_pT sinCon(nPorts=1, redeclare package Medium =
+        MediumCon) "Condenser sink" annotation (Placement(transformation(extent={{
+            10,-10},{-10,10}}, origin={70,40})));
+  AixLib.Fluid.Sources.Boundary_pT sinEva(nPorts=1, redeclare package Medium =
+        MediumEva) "Evaporator sink" annotation (Placement(transformation(extent={
+            {-10,-10},{10,10}}, origin={-50,-20})));
+  Modelica.Blocks.Sources.SawTooth ySet(
+    amplitude=-1,
+    period=500,
+    offset=1,
+    startTime=500)  "Compressor control signal"
+    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
+  Modelica.Blocks.Sources.Ramp TConIn(
+    height=10,
+    duration=60,
+    offset=273.15 + 30,
+    startTime=60) "Condenser inlet temperature"
+    annotation (Placement(transformation(extent={{-90,10},{-70,30}})));
+  Modelica.Blocks.Sources.Ramp TEvaIn(
+    height=10,
+    duration=60,
+    startTime=900,
+    offset=273.15 + 15) "Evaporator inlet temperature"
+    annotation (Placement(transformation(extent={{54,-40},{74,-20}})));
+  Modelica.Blocks.Sources.BooleanStep chiCoo(startTime=2100, startValue=true)
+    "Chilling mode on"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+equation
+  connect(souCon.ports[1], chi.port_a1) annotation (Line(
+      points={{-40,16},{0,16}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(souEva.ports[1], chi.port_a2) annotation (Line(
+      points={{40,4},{20,4}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(chi.port_b1, sinCon.ports[1]) annotation (Line(
+      points={{20,16},{30,16},{30,40},{60,40}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(sinEva.ports[1], chi.port_b2) annotation (Line(
+      points={{-40,-20},{-10,-20},{-10,4},{0,4}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TConIn.y, souCon.T_in) annotation (Line(
+      points={{-69,20},{-62,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(TEvaIn.y, souEva.T_in) annotation (Line(
+      points={{75,-30},{80,-30},{80,8},{62,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(ySet.y, chi.ySet) annotation (Line(points={{-39,60},{-16,60},{-16,12},{
+          -1.2,12}},                color={0,0,127}));
+  connect(chiCoo.y, chi.coo) annotation (Line(points={{-39,-50},{-22,-50},{-22,
+          7.9},{-1.1,7.9}}, color={255,0,255}));
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/Modular.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>", info="<html>
+<p>
+  Example that simulates a chiller based on the modular reversible approach.
+  The chiller control signal is the compressor speed
+  <code>ySet</code> and the mode <code>coo</code>.
+</p>
+<p>
+  As the model contains internal safety controls, the
+  compressor set speed <code>ySet</code> and actually applied
+  speed <code>yMea</code> are plotted to show the influence of
+  the safety control.
+</p>
+<p>
+  The example further demonstrates how to redeclare the replaceable options
+  in the model approach
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.Modular\">
+  AixLib.Fluid.Chillers.ModularReversible.Modular</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Modular;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Examples/package.mo b/AixLib/Fluid/Chillers/ModularReversible/Examples/package.mo
new file mode 100644
index 0000000000..21b7b4693a
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Examples/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+package Examples "Collection of models that illustrate model use and test models"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible\">
+AixLib.Fluid.Chillers.ModularReversible</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Examples/package.order b/AixLib/Fluid/Chillers/ModularReversible/Examples/package.order
new file mode 100644
index 0000000000..1b66df68b2
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Examples/package.order
@@ -0,0 +1,3 @@
+CarnotWithLosses
+LargeScaleWaterToWater
+Modular
diff --git a/AixLib/Fluid/Chillers/ModularReversible/LargeScaleWaterToWater.mo b/AixLib/Fluid/Chillers/ModularReversible/LargeScaleWaterToWater.mo
new file mode 100644
index 0000000000..7c609e24a2
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/LargeScaleWaterToWater.mo
@@ -0,0 +1,102 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+model LargeScaleWaterToWater "Large scale water to water chiller"
+  extends Modular(
+    dpEva_nominal=datTab.dpEva_nominal*scaFac^2,
+    dpCon_nominal=datTab.dpCon_nominal*scaFac^2,
+    final dTEva_nominal=-QCoo_flow_nominal/cpEva/mEva_flow_nominal,
+    final dTCon_nominal=(PEle_nominal - QCoo_flow_nominal)/cpCon/mCon_flow_nominal,
+    redeclare replaceable package MediumCon = AixLib.Media.Water,
+    redeclare replaceable package MediumEva = AixLib.Media.Water,
+    final GEvaIns=0,
+    final GEvaOut=0,
+    final CEva=0,
+    final use_evaCap=false,
+    final GConIns=0,
+    final GConOut=0,
+    final CCon=0,
+    final TConHea_nominal=0,
+    final TEvaHea_nominal=0,
+    final use_conCap=false,
+        redeclare replaceable
+    AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021 safCtrPar
+      constrainedby
+      AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Generic(
+      final tabUppHea=datTab.tabLowBou,
+      final tabLowCoo=datTab.tabLowBou,
+      final use_TEvaOutCoo=datTab.use_TEvaOutForOpeEnv,
+      final use_TConOutCoo=datTab.use_TConOutForOpeEnv),
+    redeclare model RefrigerantCycleInertia =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.NoInertia,
+    redeclare model RefrigerantCycleChillerHeating =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.NoHeating,
+    redeclare model RefrigerantCycleChillerCooling =
+        AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D (
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+          iceFacCal, datTab=datTab),
+    final use_rev=false,
+    final QHea_flow_nominal=0,
+    final mCon_flow_nominal=autCalMasCon_flow,
+    final mEva_flow_nominal=autCalMasEva_flow,
+    final tauCon=autCalVCon*rhoCon/autCalMasCon_flow,
+    final tauEva=autCalVEva*rhoEva/autCalMasEva_flow);
+  final parameter Real scaFac=refCyc.refCycChiCoo.scaFac "Scaling factor of chiller";
+
+  extends AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.LargeScaleWaterToWaterDeclarations(
+    final autCalMasCon_flow=max(5E-5*abs(QCoo_flow_nominal) + 0.3161, autCalMMin_flow),
+    final autCalMasEva_flow=max(5E-5*abs(QCoo_flow_nominal) - 0.5662, autCalMMin_flow),
+    final autCalVCon=max(2E-7*abs(QCoo_flow_nominal) - 84E-4, autCalVMin),
+    final autCalVEva=max(1E-7*abs(QCoo_flow_nominal) - 66E-4, autCalVMin));
+  replaceable parameter
+    AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic
+    datTab constrainedby Data.TableData2D.Generic "Data Table of Chiller"
+    annotation (choicesAllMatching=true,
+    Placement(transformation(extent={{42,12},{58,28}})));
+
+  annotation (Documentation(info="<html>
+<p>
+  Large scale water-to-water chiller,
+  using the
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.Modular\">
+  AixLib.Fluid.Chillers.ModularReversible.Modular</a> approach.
+</p>
+<p>
+  Contrary to the standard sizing approach for the <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.Modular\">
+  AixLib.Fluid.Chillers.ModularReversible.Modular</a> models,
+  the parameters are based on an automatic estimation as described in
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.LargeScaleWaterToWaterDeclarations\">
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.LargeScaleWaterToWaterDeclarations</a>.
+</p>
+<p>
+  For more information on the approach, see
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  UsersGuide</a>.
+</p>
+<p>
+  The documentation of the model for cooling is at
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D\">
+  AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D</a>.
+</p>
+<h4>Assumptions</h4>
+<ul>
+<li>
+  As heat losses are implicitly included in measured
+  data in manufacturer dataseheets, heat losses are disabled.
+</li>
+<li>
+  Pressure losses are not provided in datasheets. As typical
+  values are unknown, the pressure loss is set to <i>0</i> to enable
+  easier usage. However, the parameter is not final and should be
+  replaced if pump electrical power consumption is of interest for your simulation aim.
+</li>
+</ul>
+</html>", revisions="<html><ul>
+  <li>
+    <i>Novemeber 11, 2022</i> by Fabian Wuellhorst:<br/>
+    Implemented <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end LargeScaleWaterToWater;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Modular.mo b/AixLib/Fluid/Chillers/ModularReversible/Modular.mo
new file mode 100644
index 0000000000..20095e3140
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Modular.mo
@@ -0,0 +1,142 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+model Modular
+  "Grey-box model for reversible and non-reversible chillers"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialReversibleRefrigerantMachine(
+    final use_COP=use_rev,
+    final use_EER=true,
+    con(preDro(m_flow(nominal=-QCoo_flow_nominal/1000/10))),
+    eva(preDro(m_flow(nominal=-QCoo_flow_nominal/1000/10))),
+    safCtr(redeclare
+        AixLib.Fluid.Chillers.ModularReversible.Controls.Safety.OperationalEnvelope
+        opeEnv),
+    final PEle_nominal=refCyc.refCycChiCoo.PEle_nominal,
+    mEva_flow_nominal=-QCoo_flow_nominal/(dTEva_nominal*cpEva),
+    mCon_flow_nominal=(PEle_nominal - QCoo_flow_nominal)/(dTCon_nominal*cpCon),
+    use_rev=false,
+    redeclare final AixLib.Fluid.Chillers.ModularReversible.BaseClasses.RefrigerantCycle refCyc(
+      redeclare model RefrigerantCycleChillerCooling = RefrigerantCycleChillerCooling,
+      redeclare model RefrigerantCycleChillerHeating = RefrigerantCycleChillerHeating,
+      final allowDifferentDeviceIdentifiers=allowDifferentDeviceIdentifiers));
+  parameter Modelica.Units.SI.HeatFlowRate QCoo_flow_nominal(max=0)
+    "Nominal cooling capcaity"
+      annotation(Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.HeatFlowRate QHea_flow_nominal=0
+    "Nominal heating capacity"
+      annotation(Dialog(group="Nominal condition - Heating", enable=use_rev));
+
+  replaceable model RefrigerantCycleChillerCooling =
+      AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle
+      (PEle_nominal=0)
+    constrainedby
+    AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle(
+       final useInChi=true,
+       final TCon_nominal=TConCoo_nominal,
+       final TEva_nominal=TEvaCoo_nominal,
+       final QCoo_flow_nominal=QCoo_flow_nominal,
+       final cpCon=cpCon,
+       final cpEva=cpEva)
+  "Refrigerant cycle module for the cooling mode"
+    annotation (choicesAllMatching=true);
+
+  replaceable model RefrigerantCycleChillerHeating =
+      AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.NoHeating
+      (PEle_nominal=PEle_nominal)
+       constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle(
+       final useInHeaPum=false,
+       final TCon_nominal=TEvaHea_nominal,
+       final TEva_nominal=TConHea_nominal,
+       final QHea_flow_nominal=QHea_flow_nominal,
+       final cpCon=cpCon,
+       final cpEva=cpEva)
+  "Refrigerant cycle module for the heating mode"
+    annotation (Dialog(enable=use_rev),choicesAllMatching=true);
+  parameter Modelica.Units.SI.Temperature TEvaCoo_nominal
+    "Nominal temperature of the cooled fluid"
+    annotation(Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.Temperature TConCoo_nominal
+    "Nominal temperature of the heated fluid"
+    annotation(Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.Temperature TEvaHea_nominal
+    "Nominal temperature of the heated fluid"
+    annotation (Dialog(enable=use_rev, group="Nominal condition - Heating"));
+  parameter Modelica.Units.SI.Temperature TConHea_nominal
+    "Nominal temperature of the cooled fluid"
+    annotation (Dialog(enable=use_rev, group="Nominal condition - Heating"));
+
+
+  Modelica.Blocks.Interfaces.BooleanInput coo if not use_busConOnl and use_rev
+    "=true for cooling, =false for heating"
+    annotation (Placement(transformation(extent={{-172,-86},{-140,-54}}),
+        iconTransformation(extent={{-120,-30},{-102,-12}})));
+  Modelica.Blocks.Sources.BooleanConstant conCoo(final k=true)
+    if not use_busConOnl and not use_rev
+    "Locks the device in cooling mode if designated to be not reversible" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-110,-130})));
+  Modelica.Blocks.Logical.Not notCoo "Not cooling is heating" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={70,50})));
+equation
+  connect(conCoo.y, sigBus.coo)
+    annotation (Line(points={{-99,-130},{-76,-130},{-76,-40},{-138,-40},{-138,-42},
+          {-140,-42},{-140,-41},{-141,-41}},
+                                color={255,0,255}));
+  connect(coo, sigBus.coo)
+    annotation (Line(points={{-156,-70},{-128,-70},{-128,-40},{-134,-40},{-134,
+          -41},{-141,-41}},
+                       color={255,0,255}));
+  connect(eff.QUse_flow, refCycIneEva.y) annotation (Line(points={{98,37},{48,37},
+          {48,0},{26,0},{26,-68},{0,-68},{0,-61}}, color={0,0,127}));
+  connect(eff.hea, notCoo.y) annotation (Line(points={{98,30},{90,30},{90,50},{81,
+          50}}, color={255,0,255}));
+  connect(notCoo.u, sigBus.coo) annotation (Line(points={{58,50},{48,50},{48,0},{
+          26,0},{26,-30},{-20,-30},{-20,-41},{-141,-41}}, color={255,0,255}),
+      Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  annotation (Icon(coordinateSystem(extent={{-100,-100},{100,100}})),
+    Diagram(coordinateSystem(extent={{-140,-160},{140,160}})),
+    Documentation(revisions="<html>
+  <ul>
+  <li>
+  May 2, 2024, by Michael Wetter:<br/>
+  Refactored check for device identifiers.<br/>
+  This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">IBPSA, #1576</a>.
+  </li>
+  <li>
+    <i>May 22, 2019,</i> by Julian Matthes:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/715\">AixLib #715</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Model of a reversible, modular chiller.
+  This models allows combining any of the available modules
+  for refrigerant heating or cooling cycles, inertias,
+  heat losses, and safety controls.
+  All features are optional.
+</p>
+<p>
+  Adding to the partial model (
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialReversibleRefrigerantMachine\">
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialReversibleRefrigerantMachine</a>),
+  this model has the <code>coo</code> signal to choose
+  the operation mode of the chiller.
+</p>
+<p>
+  For more information, see
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Modular;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/NoCooling.mo b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/NoCooling.mo
new file mode 100644
index 0000000000..0df85c0b59
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/NoCooling.mo
@@ -0,0 +1,40 @@
+within AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses;
+model NoCooling
+  "Placeholder to disable cooling"
+  extends PartialChillerCycle(
+    TEva_nominal=273.15,
+    TCon_nominal=273.15,
+    cpEva=4184,
+    cpCon=4184,
+    PEle_nominal=0,
+    redeclare final
+      AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+      iceFacCal,
+    devIde="NoCooling",
+    QCoo_flow_nominal=0);
+
+  Modelica.Blocks.Sources.Constant const(final k=0) "Zero energy flows"
+    annotation (Placement(transformation(extent={{-88,16},{-68,36}})));
+equation
+  connect(const.y, redQCon.u2) annotation (Line(points={{-67,26},{64,26},{64,-78}},
+                               color={0,0,127}));
+  connect(const.y, PEle)
+    annotation (Line(points={{-67,26},{0,26},{0,-130}}, color={0,0,127}));
+  connect(const.y, proRedQEva.u2)
+    annotation (Line(points={{-67,26},{-24,26},{-24,-78}}, color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  Using this model, the chiller will always be off.
+  This option is mainly used to avoid warnings about
+  partial model which must be replaced.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end NoCooling;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/PartialChillerCycle.mo b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/PartialChillerCycle.mo
new file mode 100644
index 0000000000..29824ddf09
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/PartialChillerCycle.mo
@@ -0,0 +1,41 @@
+within AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses;
+partial model PartialChillerCycle
+  "Partial model of refrigerant cycle used for chiller applications"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle;
+  parameter Modelica.Units.SI.HeatFlowRate QCoo_flow_nominal
+    "Nominal cooling capacity"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Boolean useInChi
+    "=false to indicate that this model is used as a heat pump";
+equation
+  connect(iceFacCal.iceFac, sigBus.iceFacChiMea) annotation (Line(points={{-81.2,-50},
+          {-72,-50},{-72,-30},{-110,-30},{-110,120},{1,120}},      color={0,0,
+          127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  annotation (Documentation(
+  info="<html>
+<p>
+  Partial refrigerant cycle model for chillers.
+  It adds the specification for frosting calculation
+  and restricts to the intended choices under
+  <code>choicesAllMatching</code>.</p>
+</html>", revisions="<html>
+<ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adapted based on AixLib implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialChillerCycle;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/package.mo b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/package.mo
new file mode 100644
index 0000000000..6af0669ed8
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/package.mo
@@ -0,0 +1,37 @@
+within AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle;
+package BaseClasses "Package with partial classes of performance Data"
+annotation (Icon(graphics={
+        Rectangle(
+          lineColor={200,200,200},
+          fillColor={248,248,248},
+          fillPattern=FillPattern.HorizontalCylinder,
+          extent={{-100.0,-100.0},{100.0,100.0}},
+          radius=25.0),
+        Rectangle(
+          lineColor={128,128,128},
+          extent={{-100.0,-100.0},{100.0,100.0}},
+          radius=25.0),
+        Ellipse(
+          extent={{-30.0,-30.0},{30.0,30.0}},
+          lineColor={128,128,128},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Documentation(revisions="<html><ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  Adapted based on AixLib implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+<li>
+  <i>May 22, 2019,</i> by Julian Matthes:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/RWTH-EBC/AixLib/issues/715\">AixLib #715</a>)
+</li>
+</ul>
+</html>", info="<html>
+<p>
+  This package contains base classes for the package <a href=
+  \"AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle\">
+  AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle</a>.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/package.order b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/package.order
new file mode 100644
index 0000000000..6206835469
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/BaseClasses/package.order
@@ -0,0 +1,2 @@
+NoCooling
+PartialChillerCycle
diff --git a/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/ConstantCarnotEffectiveness.mo b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/ConstantCarnotEffectiveness.mo
new file mode 100644
index 0000000000..fcd1ea10d5
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/ConstantCarnotEffectiveness.mo
@@ -0,0 +1,132 @@
+within AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle;
+model ConstantCarnotEffectiveness "Carnot EER with a constant Carnot effectiveness"
+  extends
+    AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle(
+      useInChi=true,
+      PEle_nominal=-QCoo_flow_nominal/EER_nominal,
+      devIde="ConstantCarnotEffectiveness");
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialCarnot(
+     TAppCon_nominal=if cpCon < 1500 then 5 else 2,
+     TAppEva_nominal=if cpEva < 1500 then 5 else 2,
+     final useForChi=true,
+     final QEva_flow_nominal=QCoo_flow_nominal,
+     final QCon_flow_nominal=PEle_nominal-QCoo_flow_nominal,
+     constPEle(final k=PEle_nominal),
+    proQUse_flow(nu=4));
+  parameter Real EER_nominal(
+    min=0,
+    final unit="1") = etaCarnot_nominal*(TEva_nominal - TAppEva_nominal)/(
+    TCon_nominal + TAppCon_nominal - (TEva_nominal - TAppEva_nominal))
+    "Nominal EER";
+
+  Modelica.Blocks.Sources.Constant constNegOne(final k=-1)
+    "Negative one to negative evaporator heat flow rate" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-90,30})));
+equation
+  connect(swiQUse.u2, sigBus.onOffMea) annotation (Line(points={{-50,22},{-50,30},
+          {0,30},{0,120},{1,120}},      color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(swiPEle.y, redQCon.u2) annotation (Line(points={{50,-1},{50,-36},{64,
+          -36},{64,-78}}, color={0,0,127}));
+  connect(swiPEle.y, PEle) annotation (Line(points={{50,-1},{50,-8},{0,-8},{0,
+          -130}},
+        color={0,0,127}));
+  connect(swiPEle.u2, sigBus.onOffMea) annotation (Line(points={{50,22},{50,30},{
+          0,30},{0,120},{1,120}},
+                           color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(pasThrYMea.u, sigBus.yMea) annotation (Line(points={{18,70},{1,70},{1,
+          120}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  if useInChi then
+    connect(pasThrTCon.u, sigBus.TConOutMea) annotation (Line(points={{-30,102},{
+            -30,120},{1,120}},
+                           color={0,0,127}));
+    connect(pasThrTEva.u, sigBus.TEvaOutMea) annotation (Line(points={{-70,102},{
+            -70,120},{1,120}},
+                           color={0,0,127}));
+  else
+    connect(pasThrTCon.u, sigBus.TEvaOutMea) annotation (Line(points={{-30,102},{
+            -30,120},{1,120}},
+                           color={0,0,127}));
+    connect(pasThrTEva.u, sigBus.TConOutMea) annotation (Line(points={{-70,102},{
+            -70,120},{1,120}},
+                           color={0,0,127}));
+  end if;
+  connect(swiQUse.y, proRedQEva.u2) annotation (Line(points={{-50,-1},{-50,-30},{
+          -24,-30},{-24,-78}},  color={0,0,127}));
+  connect(constNegOne.y, proQUse_flow.u[4]) annotation (Line(points={{-79,30},{
+          -68,30},{-68,70},{-50,70},{-50,60}}, color={0,0,127}));
+  annotation (Documentation(revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This model uses a constant Carnot effectiveness approach
+  to compute the efficiency of the chiller.
+</p>
+<p>
+  <code>PEle_nominal</code> is computed from the provided
+  <code>QCoo_flow_nominal</code> and other nominal conditions.
+  <code>PEle_nominal</code> stays constant over all boundary conditions
+  and is used to calculate <code>PEle</code> by multiplying it with the
+  relative compressor speed.
+  <code>QEva_flow</code> is computed using the Carnot approach:
+</p>
+<p>
+  <code>
+    QEva_flow = PEle_nominal * etaCarnot_nominal * yMea *
+    (TEvaOut - TAppEva) /
+    (TConOut + TAppCon - (TEvaOut - TAppEva))
+  </code>
+</p>
+<p>
+  <code>
+    PEle = PEle_nominal * yMea 
+  </code>
+</p>
+<p>
+  These equations follow the same methods used in
+  <a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">
+  AixLib.Fluid.Chillers.Carnot_y</a>
+  Similarly, the variables <code>TAppCon</code> and
+  <code>TAppEva</code> define the approach (pinch) temperature differences.
+</p>
+<p>
+  The approach temperatures
+  are calculated using the following equation:
+</p>
+<p>
+  <code>
+  TApp = TApp_nominal * Q_flow / Q_flow_nominal
+  </code>
+</p>
+<p>
+  This introduces nonlinear equations to the model, which
+  can lead to solver issues for reversible operation.
+  You can use the nominal values as a constant by
+  enabling <code>use_constAppTem</code>
+</p>
+</html>"), Icon(graphics={Text(
+          extent={{-78,68},{74,-78}},
+          textColor={0,0,127},
+          textString="Carnot")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ConstantCarnotEffectiveness;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/TableData2D.mo b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/TableData2D.mo
new file mode 100644
index 0000000000..9a77772f59
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/TableData2D.mo
@@ -0,0 +1,210 @@
+within AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle;
+model TableData2D
+  "Performance data based on condenser outlet and evaporator inlet temperature"
+  extends
+    AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle(
+    final devIde=datTab.devIde,
+    PEle_nominal=Modelica.Blocks.Tables.Internal.getTable2DValueNoDer2(
+        tabIdePEle,
+        TEva_nominal,
+        TCon_nominal) * scaFac);
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialTableData2D(
+    final useInRevDev=not useInChi,
+    final use_TConOutForTab=datTab.use_TConOutForTab,
+    final use_TEvaOutForTab=datTab.use_TEvaOutForTab,
+    tabQUse_flow(final table=datTab.tabQEva_flow),
+    tabPEle(final table=datTab.tabPEle),
+    scaFac=QCoo_flow_nominal/QCooNoSca_flow_nominal,
+    mEva_flow_nominal=datTab.mEva_flow_nominal*scaFac,
+    mCon_flow_nominal=datTab.mCon_flow_nominal*scaFac,
+    final valTabQEva_flow = {{-tabQUse_flow.table[j, i] for i in 2:numCol} for j in 2:numRow},
+    final valTabQCon_flow = valTabQEva_flow .+ valTabPEle,
+    final mCon_flow_max=max(valTabQCon_flow) * scaFac / cpCon / dTMin,
+    final mCon_flow_min=min(valTabQCon_flow) * scaFac / cpCon / dTMax,
+    final mEva_flow_min=min(valTabQEva_flow) * scaFac / cpEva / dTMax,
+    final mEva_flow_max=max(valTabQEva_flow) * scaFac / cpEva / dTMin);
+  parameter Modelica.Units.SI.HeatFlowRate QCooNoSca_flow_nominal=
+        Modelica.Blocks.Tables.Internal.getTable2DValueNoDer2(
+        tabIdeQUse_flow,
+        TEva_nominal,
+        TCon_nominal)
+    "Unscaled nominal cooling capacity "
+    annotation (Dialog(group="Nominal condition"));
+  replaceable parameter AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic datTab
+    "Data Table of Chiller" annotation (choicesAllMatching=true);
+
+equation
+
+  connect(scaFacTimPel.y, PEle) annotation (Line(points={{-40,-9},{-40,-26},{-30,
+          -26},{-30,-94},{0,-94},{0,-130}}, color={0,0,127}));
+  connect(scaFacTimPel.y, redQCon.u2) annotation (Line(points={{-40,-9},{-40,-26},
+          {-30,-26},{-30,-48},{64,-48},{64,-78}}, color={0,0,127}));
+  connect(scaFacTimQUse_flow.y, proRedQEva.u2) annotation (Line(points={{40,-9},{
+          40,-40},{-24,-40},{-24,-78}},  color={0,0,127}));
+  connect(yMeaTimScaFac.u1, sigBus.yMea) annotation (Line(points={{-54,62},{-54,
+          72},{-70,72},{-70,120},{1,120}},   color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(reaPasThrTEvaOut.u, sigBus.TEvaOutMea) annotation (Line(points={{-10,102},
+          {-10,120},{1,120}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(reaPasThrTEvaIn.u, sigBus.TEvaInMea) annotation (Line(points={{-50,102},
+          {-50,120},{1,120}},                 color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(reaPasThrTConIn.u, sigBus.TConInMea) annotation (Line(points={{50,102},
+          {50,120},{1,120}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(reaPasThrTConOut.u, sigBus.TConOutMea) annotation (Line(points={{90,102},
+          {90,120},{1,120}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+
+  if useInChi then
+    connect(reaPasThrTConOut.y, tabPEle.u2)
+      annotation (Line(points={{90,79},{90,70},{84,70},{84,62}}, color={0,0,127}));
+    connect(reaPasThrTConIn.y, tabPEle.u2)
+      annotation (Line(points={{50,79},{50,70},{84,70},{84,62}}, color={0,0,127}));
+    connect(reaPasThrTConIn.y, tabQUse_flow.u2)
+      annotation (Line(points={{50,79},{50,70},{44,70},{44,62}}, color={0,0,127}));
+    connect(reaPasThrTConOut.y, tabQUse_flow.u2)
+      annotation (Line(points={{90,79},{90,70},{44,70},{44,62}}, color={0,0,127}));
+    connect(reaPasThrTEvaOut.y, tabQUse_flow.u1) annotation (Line(points={{-10,79},
+            {-10,70},{56,70},{56,62}},color={0,0,127}));
+    connect(reaPasThrTEvaIn.y, tabQUse_flow.u1) annotation (Line(points={{-50,79},
+            {-50,70},{56,70},{56,62}},
+                                  color={0,0,127}));
+    connect(reaPasThrTEvaOut.y, tabPEle.u1) annotation (Line(points={{-10,79},{
+            -10,70},{96,70},{96,62}},
+                              color={0,0,127}));
+    connect(reaPasThrTEvaIn.y, tabPEle.u1) annotation (Line(points={{-50,79},{-50,
+            70},{96,70},{96,62}},
+                                color={0,0,127}));
+  else
+    connect(reaPasThrTConOut.y, tabPEle.u1)
+      annotation (Line(points={{90,79},{90,70},{96,70},{96,62}}, color={0,0,127}));
+    connect(reaPasThrTConOut.y, tabQUse_flow.u1)
+      annotation (Line(points={{90,79},{90,70},{56,70},{56,62}}, color={0,0,127}));
+    connect(reaPasThrTConIn.y, tabQUse_flow.u1)
+      annotation (Line(points={{50,79},{50,70},{56,70},{56,62}}, color={0,0,127}));
+    connect(reaPasThrTConIn.y, tabPEle.u1)
+      annotation (Line(points={{50,79},{50,70},{96,70},{96,62}}, color={0,0,127}));
+    connect(reaPasThrTEvaOut.y, tabPEle.u2) annotation (Line(points={{-10,79},{
+            -10,70},{84,70},{84,62}},         color={0,0,127}));
+    connect(reaPasThrTEvaOut.y, tabQUse_flow.u2) annotation (Line(points={{-10,79},
+            {-10,70},{44,70},{44,62}},                color={0,0,127}));
+    connect(reaPasThrTEvaIn.y, tabQUse_flow.u2) annotation (Line(points={{-50,79},
+            {-50,70},{44,70},{44,62}},            color={0,0,127}));
+    connect(reaPasThrTEvaIn.y, tabPEle.u2) annotation (Line(points={{-50,79},{-50,
+            70},{84,70},{84,62}},             color={0,0,127}));
+  end if;
+  annotation (Icon(graphics={
+    Line(points={{-60.0,40.0},{-60.0,-40.0},{60.0,-40.0},{60.0,40.0},
+      {30.0,40.0},{30.0,-40.0},{-30.0,-40.0},{-30.0,40.0},{-60.0,40.0},
+      {-60.0,20.0},{60.0,20.0},{60.0,0.0},{-60.0,0.0},{-60.0,-20.0},
+      {60.0,-20.0},{60.0,-40.0},{-60.0,-40.0},{-60.0,40.0},{60.0,40.0},
+      {60.0,-40.0}}),
+    Line(points={{0.0,40.0},{0.0,-40.0}}),
+    Rectangle(fillColor={255,215,136},
+      fillPattern=FillPattern.Solid,
+      extent={{-60.0,20.0},{-30.0,40.0}}),
+    Rectangle(fillColor={255,215,136},
+      fillPattern=FillPattern.Solid,
+      extent={{-60.0,0.0},{-30.0,20.0}}),
+    Rectangle(fillColor={255,215,136},
+      fillPattern=FillPattern.Solid,
+      extent={{-60.0,-20.0},{-30.0,0.0}}),
+    Rectangle(fillColor={255,215,136},
+      fillPattern=FillPattern.Solid,
+      extent={{-60.0,-40.0},{-30.0,-20.0}})}), Documentation(revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on the discussion in this issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>May 22, 2019,</i> by Julian Matthes:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/715\">AixLib #715</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This model uses two-dimensional table data typically given
+  by manufacturers as required by e.g. European Norm 14511
+  or ASHRAE 205 to calculate
+  <code>QEva_flow</code> and <code>PEle</code>.
+</p>
+<p>
+  For different condenser outlet and evaporator inlet temperatures,
+  the tables must provide two of the three following values:
+  electrical power consumption, evaporator heat flow rate, and COP.
+</p>
+<p>
+  Note that losses are often implicitly included in measured data.
+  In this case, the frosting modules should be disabled.
+</p>
+
+<h4>Scaling factor</h4>
+<p>
+For the scaling factor, the table data for evaporator heat flow rate (<code>QEvaTabDat_flow</code>)
+is evaluated at nominal conditions. Hence, the scaling factor is</p>
+<pre>
+scaFac = QEva_flow_nominal/QEvaTabDat_flow(TEva_nominal, TCon_nominal).
+
+</pre>
+<p>
+Using <code>scaFac</code>, the table data is scaled linearly.
+This implies a constant COP over different design sizes:
+</p>
+<p><code>QEva_flow = scaFac * tabQEva_flow.y</code> </p>
+<p><code>PEle = scaFac * tabPel.y</code></p>
+
+
+<h4>Known Limitations </h4>
+<ul>
+<li>
+  Manufacturers are not required to provide the compressor speed at which
+  the data are measured. Thus, nominal values may be obtained at different
+  compressor speeds and, thus, efficiencies.
+  To accurately model the available thermal output,
+  please check that you use tables of the maximal thermal output,
+  which is often provided in the data sheets from the manufacturers.
+  This limitation only holds for inverter driven chillers.
+</li>
+<li>
+  We assume that the efficiency is contant over the whole
+  compressor speed range. Typically, efficiencies will drop at minimal
+  and maximal compressor speeds.
+  To model an inverter controlled chiller, the relative
+  compressor speed <code>yMea</code> is used to scale
+  the ouput of the tables linearly.
+  For models including the compressor speed, check the SDF-Library
+  dependent refrigerant cycle models in the
+  <a href=\"https://github.com/RWTH-EBC/AixLib\">AixLib</a> Library.
+</li>
+</ul>
+<h4>References</h4>
+<p>
+EN 14511-2018: Air conditioners, liquid chilling packages and heat pumps for space
+heating and cooling and process chillers, with electrically driven compressors
+<a href=\"https://www.beuth.de/de/norm/din-en-14511-1/298537524\">
+https://www.beuth.de/de/norm/din-en-14511-1/298537524</a>
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TableData2D;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/package.mo b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/package.mo
new file mode 100644
index 0000000000..6b8d331f14
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/package.mo
@@ -0,0 +1,21 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+package RefrigerantCycle "Package for chiller refrigerant cycle modules"
+   extends Modelica.Icons.MaterialPropertiesPackage;
+
+
+
+annotation (Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This package contains models and data to for
+  dynamic refrigerant cycles with stationary data points,
+  evaporator frosting, and cycle inertia.
+</p>
+</html>"));
+end RefrigerantCycle;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/package.order b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/package.order
new file mode 100644
index 0000000000..5ffb6c022f
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/RefrigerantCycle/package.order
@@ -0,0 +1,3 @@
+ConstantCarnotEffectiveness
+TableData2D
+BaseClasses
diff --git a/AixLib/Fluid/Chillers/ModularReversible/UsersGuide.mo b/AixLib/Fluid/Chillers/ModularReversible/UsersGuide.mo
new file mode 100644
index 0000000000..2725307431
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/UsersGuide.mo
@@ -0,0 +1,14 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+package UsersGuide
+  "User's Guide for modular reversible heat pump and chiller models"
+  extends Modelica.Icons.Information;
+  annotation (preferredView="info",
+  Documentation(info="<html>
+<p>
+This package contains the chiller models as part of the implementation of the
+modular reversible approach. For information of both chiller and heat pump
+models, see
+<a href=\"Modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>.
+</html>"));
+end UsersGuide;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/PartialModularComparison.mo b/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/PartialModularComparison.mo
new file mode 100644
index 0000000000..d59414b6b8
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/PartialModularComparison.mo
@@ -0,0 +1,71 @@
+within AixLib.Fluid.Chillers.ModularReversible.Validation.BaseClasses;
+partial model PartialModularComparison
+  "Partial model for comparison to the Carnot model"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative.BaseClasses.PartialComparison(
+    m1_flow_nominal=chi.mCon_flow_nominal,
+    m2_flow_nominal=chi.mEva_flow_nominal,
+    sou1(nPorts=1),
+    sin2(nPorts=1),
+    sou2(nPorts=1),
+    sin1(nPorts=1));
+
+  Modular chi(
+    redeclare final package MediumCon = Medium1,
+    redeclare final package MediumEva = Medium2,
+    QCoo_flow_nominal=-QUse_flow_nominal,
+    redeclare final model RefrigerantCycleInertia =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.NoInertia,
+    final use_rev=false,
+    final use_intSafCtr=false,
+    final tauCon=tau1,
+    final TConCoo_nominal=TCon_nominal,
+    final dTCon_nominal=dTCon_nominal,
+    final dpCon_nominal=dp1_nominal,
+    final use_conCap=false,
+    final CCon=0,
+    final GConOut=0,
+    final TEvaHea_nominal=0,
+    final TConHea_nominal=0,
+    final GConIns=0,
+    final tauEva=tau2,
+    final TEvaCoo_nominal=TEva_nominal,
+    final dTEva_nominal=dTEva_nominal,
+    final dpEva_nominal=dp2_nominal,
+    final use_evaCap=false,
+    final CEva=0,
+    final GEvaOut=0,
+    final GEvaIns=0,
+    final TCon_start=T1_start,
+    final TEva_start=T2_start,
+    final energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial)
+    "Modular chiller model"
+    annotation (Placement(transformation(extent={{-8,-10},{12,10}})));
+
+equation
+  connect(chi.port_a1, sou1.ports[1])
+    annotation (Line(points={{-8,6},{-40,6}},  color={0,127,255}));
+  connect(chi.port_b2, sin2.ports[1]) annotation (Line(points={{-8,-6},{-32,-6},{
+          -32,-30},{-40,-30}}, color={0,127,255}));
+  connect(chi.port_a2, sou2.ports[1])
+    annotation (Line(points={{12,-6},{40,-6}}, color={0,127,255}));
+  connect(chi.port_b1, sin1.ports[1])
+    annotation (Line(points={{12,6},{36,6},{36,30},{60,30}}, color={0,127,255}));
+  connect(chi.ySet, uCom.y) annotation (Line(points={{-9.2,2},{-34,2},{-34,50},{
+          -39,50}},          color={0,0,127}));
+
+  annotation (
+    Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model to have consistent parameterization of the
+modular reversible model approaches.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialModularComparison;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/package.mo b/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/package.mo
new file mode 100644
index 0000000000..e4642b2bbb
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/package.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.Chillers.ModularReversible.Validation;
+package BaseClasses "Package with partial validation models"
+extends Modelica.Icons.BasesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains partial models for comparative validation.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/package.order b/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/package.order
new file mode 100644
index 0000000000..1d1cd0e020
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Validation/BaseClasses/package.order
@@ -0,0 +1 @@
+PartialModularComparison
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Validation/Carnot_y.mo b/AixLib/Fluid/Chillers/ModularReversible/Validation/Carnot_y.mo
new file mode 100644
index 0000000000..defd59697e
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Validation/Carnot_y.mo
@@ -0,0 +1,63 @@
+within AixLib.Fluid.Chillers.ModularReversible.Validation;
+model Carnot_y "Example using the Carnot model approach"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative.BaseClasses.PartialComparison(
+    m1_flow_nominal=chi.m1_flow_nominal,
+    m2_flow_nominal=chi.m2_flow_nominal,
+    sin2(nPorts=1),
+    sou2(nPorts=1),
+    sin1(nPorts=1),
+    sou1(nPorts=1));
+  extends Modelica.Icons.Example;
+  AixLib.Fluid.Chillers.Carnot_y chi(
+    redeclare package Medium1 = Medium1,
+    redeclare package Medium2 = Medium2,
+    etaCarnot_nominal=etaCarnot_nominal,
+    TCon_nominal=TCon_nominal,
+    TEva_nominal=TEva_nominal,
+    tau1=tau1,
+    tau2=tau2,
+    P_nominal=QUse_flow_nominal/chi.COP_nominal,
+    dTEva_nominal=-dTEva_nominal,
+    dTCon_nominal=dTCon_nominal,
+    use_eta_Carnot_nominal=false,
+    dp1_nominal=dp1_nominal,
+    dp2_nominal=dp2_nominal,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    show_T=true,
+    T1_start=T1_start,
+    T2_start=T2_start)
+                     "Chiller model"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+
+equation
+  connect(sin2.ports[1], chi.port_b2) annotation (Line(points={{-40,-30},{-16,-30},
+          {-16,-6},{-10,-6}}, color={0,127,255}));
+  connect(chi.port_a2, sou2.ports[1])
+    annotation (Line(points={{10,-6},{40,-6}}, color={0,127,255}));
+  connect(chi.port_b1, sin1.ports[1])
+    annotation (Line(points={{10,6},{36,6},{36,30},{60,30}}, color={0,127,255}));
+  connect(chi.port_a1, sou1.ports[1]) annotation (Line(points={{-10,6},{-40,6}},
+                       color={0,127,255}));
+  connect(chi.y, uCom.y)
+    annotation (Line(points={{-12,9},{-12,50},{-39,50}}, color={0,0,127}));
+
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/Carnot_y.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Validation case for <a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">
+AixLib.Fluid.Chillers.Carnot_y</a>, duplicate of the example
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_y\">
+AixLib.Fluid.Chillers.Examples.Carnot_y</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Carnot_y;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Validation/ConstantCarnotEffectiveness.mo b/AixLib/Fluid/Chillers/ModularReversible/Validation/ConstantCarnotEffectiveness.mo
new file mode 100644
index 0000000000..11243b510f
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Validation/ConstantCarnotEffectiveness.mo
@@ -0,0 +1,27 @@
+within AixLib.Fluid.Chillers.ModularReversible.Validation;
+model ConstantCarnotEffectiveness
+  "Validation case for modular Carnot approach"
+  extends BaseClasses.PartialModularComparison(chi(redeclare model
+        RefrigerantCycleChillerCooling =
+          AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness
+          (etaCarnot_nominal=etaCarnot_nominal)));
+  extends Modelica.Icons.Example;
+
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/ConstantCarnotEffectiveness.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Validation case for <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness\">
+AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ConstantCarnotEffectiveness;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Validation/TableData2D.mo b/AixLib/Fluid/Chillers/ModularReversible/Validation/TableData2D.mo
new file mode 100644
index 0000000000..74117f0d00
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Validation/TableData2D.mo
@@ -0,0 +1,41 @@
+within AixLib.Fluid.Chillers.ModularReversible.Validation;
+model TableData2D "Validation case for table data approach"
+  extends BaseClasses.PartialModularComparison(
+    TEva_nominal=TEvaIn_nominal,
+    TCon_nominal=TConIn_nominal,
+    chi(redeclare model RefrigerantCycleChillerCooling =
+          AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D (
+            datTab(
+            tabPEle=[0,293.15,303.15; 288.15,14122.8,14122.8; 298.15,14122.8,14122.8],
+            mCon_flow_nominal=m1_flow_nominal,
+            mEva_flow_nominal=m2_flow_nominal,
+            dpCon_nominal=0,
+            dpEva_nominal=0,
+            devIde="CarnotTableData",
+            use_TEvaOutForTab=false,
+            use_TConOutForTab=false,
+            tabQEva_flow=[0,293.15,303.15; 288.15,-35499.7,-30000; 298.15,0,-36220.8],
+            tabLowBou=[273.15,273.15; 273.15,273.15],
+            use_TEvaOutForOpeEnv=false,
+            use_TConOutForOpeEnv=false))));
+
+  extends Modelica.Icons.Example;
+
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/TableData2D.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Validation case for <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D\">
+AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TableData2D;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Validation/package.mo b/AixLib/Fluid/Chillers/ModularReversible/Validation/package.mo
new file mode 100644
index 0000000000..30a693b7b7
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Validation/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Fluid.Chillers.ModularReversible;
+package Validation "Package for model validation"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains models that validate the modular reversible chiller models
+using comparative validation against the Carnot model:
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_y\">
+AixLib.Fluid.Chillers.Examples.Carnot_y</a>
+</p>
+</html>"));
+end Validation;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/Validation/package.order b/AixLib/Fluid/Chillers/ModularReversible/Validation/package.order
new file mode 100644
index 0000000000..bc40b5cefa
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/Validation/package.order
@@ -0,0 +1,4 @@
+Carnot_y
+ConstantCarnotEffectiveness
+TableData2D
+BaseClasses
diff --git a/AixLib/Fluid/Chillers/ModularReversible/package.mo b/AixLib/Fluid/Chillers/ModularReversible/package.mo
new file mode 100644
index 0000000000..bcadf5d435
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/package.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.Chillers;
+package ModularReversible "Package for reversible and non-reversible chillers using a modular model approach"
+extends Modelica.Icons.VariantsPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+Package with models and packages for the modular reversible chiller approach.
+See the <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>
+for more information.
+</html>"));
+end ModularReversible;
diff --git a/AixLib/Fluid/Chillers/ModularReversible/package.order b/AixLib/Fluid/Chillers/ModularReversible/package.order
new file mode 100644
index 0000000000..d92b0a0660
--- /dev/null
+++ b/AixLib/Fluid/Chillers/ModularReversible/package.order
@@ -0,0 +1,10 @@
+UsersGuide
+CarnotWithLosses
+LargeScaleWaterToWater
+Modular
+Controls
+RefrigerantCycle
+Data
+Examples
+Validation
+BaseClasses
diff --git a/AixLib/Fluid/Chillers/Validation/CarnotVerifyCOP.mo b/AixLib/Fluid/Chillers/Validation/CarnotVerifyCOP.mo
index 248594836d..e364cadd6b 100644
--- a/AixLib/Fluid/Chillers/Validation/CarnotVerifyCOP.mo
+++ b/AixLib/Fluid/Chillers/Validation/CarnotVerifyCOP.mo
@@ -8,7 +8,7 @@ model CarnotVerifyCOP
   parameter Real COP_nominal = 3 "Coefficient of performance";
 
   parameter Modelica.Units.SI.Temperature TCon_nominal=273.15 + 30
-    "Nominal condensor temperature";
+    "Nominal condenser temperature";
   parameter Modelica.Units.SI.Temperature TEva_nominal=273.15 + 5
     "Nominal evaporator temperature";
 
@@ -62,7 +62,7 @@ model CarnotVerifyCOP
     redeclare package Medium = Medium,
     m_flow=mCon_flow_nominal,
     T=TCon_nominal - QCon_flow_nominal/cp_default/mCon_flow_nominal)
-    "Boundary condition for condener"
+    "Boundary condition for condenser"
     annotation (Placement(transformation(extent={{-80,46},{-60,66}})));
   Sources.MassFlowSource_T bouEva(
     redeclare package Medium = Medium,
@@ -155,19 +155,19 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/Validation/CarnotVerifyCOP.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example verifies that the coefficient of performance is identical
- to the one specified for the nominal operating point if the current
- operating conditions are the same as the nominal conditions.
- It thus verifies the correct deviation of the nominal parameters.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 15, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example verifies that the coefficient of performance is identical
+to the one specified for the nominal operating point if the current
+operating conditions are the same as the nominal conditions.
+It thus verifies the correct deviation of the nominal parameters.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 15, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CarnotVerifyCOP;
diff --git a/AixLib/Fluid/Chillers/Validation/CarnotVerifyEtaCarnot.mo b/AixLib/Fluid/Chillers/Validation/CarnotVerifyEtaCarnot.mo
index 62237dcfb6..0665bfa41f 100644
--- a/AixLib/Fluid/Chillers/Validation/CarnotVerifyEtaCarnot.mo
+++ b/AixLib/Fluid/Chillers/Validation/CarnotVerifyEtaCarnot.mo
@@ -18,7 +18,7 @@ model CarnotVerifyEtaCarnot
     (TCon_nominal + TAppCon_nominal - (TEva_nominal-TAppEva_nominal))  "Coefficient of performance";
 
   parameter Modelica.Units.SI.Temperature TCon_nominal=273.15 + 30
-    "Nominal condensor temperature";
+    "Nominal condenser temperature";
 
   parameter Modelica.Units.SI.Temperature TEva_nominal=273.15 + 5
     "Nominal evaporator temperature";
@@ -169,20 +169,20 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/Validation/CarnotVerifyEtaCarnot.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example verifies that the coefficient of performance is identical
- to the one specified for the nominal operating point if the current
- operating conditions are the same as the nominal conditions.
- It thus verifies the correct deviation of the nominal parameters
- for the situation where the Carnot effectiveness is specified as a parameter.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 15, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example verifies that the coefficient of performance is identical
+to the one specified for the nominal operating point if the current
+operating conditions are the same as the nominal conditions.
+It thus verifies the correct deviation of the nominal parameters
+for the situation where the Carnot effectiveness is specified as a parameter.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 15, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CarnotVerifyEtaCarnot;
diff --git a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_2ndLaw.mo b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_2ndLaw.mo
index 95ad7f5b1e..a8697e8e4b 100644
--- a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_2ndLaw.mo
+++ b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_2ndLaw.mo
@@ -18,7 +18,7 @@ model Carnot_TEva_2ndLaw
 
   final parameter Modelica.Units.SI.MassFlowRate m1_flow_nominal=-
       m2_flow_nominal/dTCon_nominal*dTEva_nominal
-    "Nominal mass flow rate at condeser water side";
+    "Nominal mass flow rate at condenser water side";
 
   Modelica.Blocks.Sources.Constant TEvaIn(k=273.15 + 20)
     "Evaporator inlet temperature"
@@ -63,7 +63,7 @@ protected
     parameter Modelica.Units.SI.HeatFlowRate QEva_flow_nominal
       "Evaporator heat flow rate";
     parameter Modelica.Units.SI.MassFlowRate m1_flow_nominal
-      "Nominal mass flow rate at condeser water side";
+      "Nominal mass flow rate at condenser water side";
     parameter Modelica.Units.SI.MassFlowRate m2_flow_nominal
       "Nominal mass flow rate at chilled water side";
 
@@ -88,7 +88,6 @@ protected
       QEva_flow_nominal=QEva_flow_nominal,
       allowFlowReversal1=false,
       allowFlowReversal2=false,
-      etaCarnot_nominal=0.3,
       dp1_nominal=0,
       dp2_nominal=0,
       energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
@@ -150,8 +149,8 @@ protected
           origin={152,-46})));
   equation
     assert(SGen_flow > 0, "Entropy generated is zero or negative, which violates the 2nd law.
-   This is because the model is configured to use the inlet temperatures
-   to compute the Carnot efficiency, which can lead to non-physical results.",
+  This is because the model is configured to use the inlet temperatures
+  to compute the Carnot efficiency, which can lead to non-physical results.",
     level = AssertionLevel.warning);
     connect(SIn_flow.y, dS_flow.u1)
       annotation (Line(points={{81,50},{88,50},{88,46},{98,46}},
@@ -219,31 +218,37 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/Validation/Carnot_TEva_2ndLaw.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example verifies that the 2nd law of thermodynamics is not violated
- despite of a very small temperature lift.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- January 9, 2017, by Michael Wetter:<br/>
- Renamed internal protected class <code>Chiller</code> to be upper-case.
- </li>
- <li>
- January 3, 2017, by Michael Wetter:<br/>
- Updated model because the option to use the inlet temperatures to compute the COP
- has been removed.
- </li>
- <li>
- November 18, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example verifies that the 2nd law of thermodynamics is not violated
+despite of a very small temperature lift.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 10, 2023, by Michael Wetter:<br/>
+Removed binding of parameter with same value as the default.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1692\">#1692</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+January 9, 2017, by Michael Wetter:<br/>
+Renamed internal protected class <code>Chiller</code> to be upper-case.
+</li>
+<li>
+January 3, 2017, by Michael Wetter:<br/>
+Updated model because the option to use the inlet temperatures to compute the COP
+has been removed.
+</li>
+<li>
+November 18, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TEva_2ndLaw;
diff --git a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_HighTemperature.mo b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_HighTemperature.mo
index 4ce628943f..7b90138ceb 100644
--- a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_HighTemperature.mo
+++ b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_HighTemperature.mo
@@ -15,24 +15,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/Validation/Carnot_TEva_HighTemperature.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_TEva\">
- AixLib.Fluid.Chillers.Examples.Carnot_TEva</a>
- but increases the set point for the leaving evaporator temperature
- to be above its inlet temperature, in which case the model provides no cooling.
- Towards the end of the simulation, the inlet temperature of the evaporator is increased
- to be above the condenser temperature. In this domain, the model requires cooling
- again. While this is not a meaningful operating point for the model, the example
- verifies that it robustly simulates this regime.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 10, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_TEva\">
+AixLib.Fluid.Chillers.Examples.Carnot_TEva</a>
+but increases the set point for the leaving evaporator temperature
+to be above its inlet temperature, in which case the model provides no cooling.
+Towards the end of the simulation, the inlet temperature of the evaporator is increased
+to be above the condenser temperature. In this domain, the model requires cooling
+again. While this is not a meaningful operating point for the model, the example
+verifies that it robustly simulates this regime.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 10, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TEva_HighTemperature;
diff --git a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_LimitedCapacity.mo b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_LimitedCapacity.mo
index f0f033e417..2ce0b5217e 100644
--- a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_LimitedCapacity.mo
+++ b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_LimitedCapacity.mo
@@ -7,19 +7,19 @@ model Carnot_TEva_LimitedCapacity
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/Validation/Carnot_TEva_LimitedCapacity.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_TEva\">
- AixLib.Fluid.Chillers.Examples.Carnot_TEva</a>
- but limits the cooling capacity.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 10, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_TEva\">
+AixLib.Fluid.Chillers.Examples.Carnot_TEva</a>
+but limits the cooling capacity.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 10, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TEva_LimitedCapacity;
diff --git a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_etaPL.mo b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_etaPL.mo
index 918befc50c..36ffa9bc9e 100644
--- a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_etaPL.mo
+++ b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_etaPL.mo
@@ -8,19 +8,19 @@ model Carnot_TEva_etaPL
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/Validation/Carnot_TEva_etaPL.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_TEva\">
- AixLib.Fluid.Chillers.Examples.Carnot_TEva</a>
- but has a part load efficiency that varies with the load.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 10, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_TEva\">
+AixLib.Fluid.Chillers.Examples.Carnot_TEva</a>
+but has a part load efficiency that varies with the load.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 10, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TEva_etaPL;
diff --git a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_reverseFlow.mo b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_reverseFlow.mo
index 4189468279..cfcac7a694 100644
--- a/AixLib/Fluid/Chillers/Validation/Carnot_TEva_reverseFlow.mo
+++ b/AixLib/Fluid/Chillers/Validation/Carnot_TEva_reverseFlow.mo
@@ -24,7 +24,6 @@ model Carnot_TEva_reverseFlow
     dTEva_nominal=dTEva_nominal,
     dTCon_nominal=dTCon_nominal,
     use_eta_Carnot_nominal=true,
-    etaCarnot_nominal=0.3,
     m1_flow_nominal=m1_flow_nominal,
     m2_flow_nominal=m2_flow_nominal,
     show_T=true,
@@ -80,7 +79,7 @@ model Carnot_TEva_reverseFlow
     duration=60,
     startTime=1800,
     height=-2*m2_flow_nominal,
-    offset=m2_flow_nominal) "Mass flow rate for evaporater"
+    offset=m2_flow_nominal) "Mass flow rate for evaporator"
     annotation (Placement(transformation(extent={{92,-8},{72,12}})));
 equation
   connect(sou1.ports[1], chi.port_a1)    annotation (Line(
@@ -117,29 +116,35 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chiller
         "Simulate and plot"),
     Documentation(
 info="<html>
- <p>
- Example that simulates a chiller whose efficiency is scaled based on the
- Carnot cycle.
- The chiller takes as an input the evaporator leaving water temperature.
- The condenser mass flow rate is computed in such a way that it has
- a temperature difference equal to <code>dTEva_nominal</code>.
- </p>
- <p>
- This example checks the correct behavior if a mass flow rate attains zero.
- </p>
- </html>",
+<p>
+Example that simulates a chiller whose efficiency is scaled based on the
+Carnot cycle.
+The chiller takes as an input the evaporator leaving water temperature.
+The condenser mass flow rate is computed in such a way that it has
+a temperature difference equal to <code>dTEva_nominal</code>.
+</p>
+<p>
+This example checks the correct behavior if a mass flow rate attains zero.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 25, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 10, 2023, by Michael Wetter:<br/>
+Removed binding of parameter with same value as the default.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1692\">#1692</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 25, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TEva_reverseFlow;
diff --git a/AixLib/Fluid/Chillers/Validation/Carnot_y_etaPL.mo b/AixLib/Fluid/Chillers/Validation/Carnot_y_etaPL.mo
index 647f562278..1745b40347 100644
--- a/AixLib/Fluid/Chillers/Validation/Carnot_y_etaPL.mo
+++ b/AixLib/Fluid/Chillers/Validation/Carnot_y_etaPL.mo
@@ -7,19 +7,19 @@ model Carnot_y_etaPL
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Chillers/Validation/Carnot_y_etaPL.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_y\">
- AixLib.Fluid.Chillers.Examples.Carnot_y</a>
- but uses a part load efficiency curve that is different from <i>1</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 10, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_y\">
+AixLib.Fluid.Chillers.Examples.Carnot_y</a>
+but uses a part load efficiency curve that is different from <i>1</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 10, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_y_etaPL;
diff --git a/AixLib/Fluid/Chillers/package.order b/AixLib/Fluid/Chillers/package.order
index 481c5ed6f4..0e5718dd71 100644
--- a/AixLib/Fluid/Chillers/package.order
+++ b/AixLib/Fluid/Chillers/package.order
@@ -1,6 +1,7 @@
 Carnot_TEva
 Carnot_y
 Chiller
+ModularReversible
 Examples
 Validation
 BaseClasses
diff --git a/AixLib/Fluid/Delays/DelayFirstOrder.mo b/AixLib/Fluid/Delays/DelayFirstOrder.mo
index 8f50fbfbcc..019f831610 100644
--- a/AixLib/Fluid/Delays/DelayFirstOrder.mo
+++ b/AixLib/Fluid/Delays/DelayFirstOrder.mo
@@ -7,7 +7,7 @@ model DelayFirstOrder
     final mSenFac=1);
 
   parameter Modelica.Units.SI.Time tau=60 "Time constant at nominal flow"
-    annotation (Dialog(tab="Dynamics", group="Nominal condition"));
+    annotation (Dialog(group="Delay time"));
 
 protected
   parameter Modelica.Units.SI.Volume V_nominal=m_flow_nominal*tau/rho_default
@@ -19,47 +19,53 @@ protected
           textString="tau=%tau")}),
 defaultComponentName="del",
     Documentation(info="<html>
- <p>
- This model approximates a transport delay using a first order differential equations.
- </p>
- <p>
- The model consists of a mixing volume with two ports. The size of the
- mixing volume is such that at the nominal mass flow rate
- <code>m_flow_nominal</code>,
- the time constant of the volume is equal to the parameter <code>tau</code>.
- </p>
- <p>
- The heat flux connector is optional, it need not be connnected.
- </p>
- </html>",
+<p>
+This model approximates a transport delay using first order differential equations.
+</p>
+<p>
+The model consists of a mixing volume with two ports. The size of the
+mixing volume is such that at the nominal mass flow rate
+<code>m_flow_nominal</code>,
+the time constant of the volume is equal to the parameter <code>tau</code>.
+</p>
+<p>
+The heat flux connector is optional and need not be connnected.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- September 14, 2013, by Michael Wetter:<br/>
- Renamed <code>V0</code> to <code>V_nominal</code> to use consistent notation.
- </li>
- <li>
- September 24, 2008, by Michael Wetter:<br/>
- Changed base class from <code>Modelica.Fluid</code> to <code>AixLib</code> library.
- This was done to track the auxiliary species flow <code>mC_flow</code>.
- </li>
- <li>
- September 4, 2008, by Michael Wetter:<br/>
- Fixed bug in assignment of parameter <code>sta0</code>.
- The earlier implementation
- required temperature to be a state, which is not always the case.
- </li>
- <li>
- March 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 12, 2024, by Michael Wetter:<br/>
+Moved parameter <code>tau</code> to the main parameter tab.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1906\">#1906</a>.
+</li>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+September 14, 2013, by Michael Wetter:<br/>
+Renamed <code>V0</code> to <code>V_nominal</code> to use consistent notation.
+</li>
+<li>
+September 24, 2008, by Michael Wetter:<br/>
+Changed base class from <code>Modelica.Fluid</code> to <code>AixLib</code> library.
+This was done to track the auxiliary species flow <code>mC_flow</code>.
+</li>
+<li>
+September 4, 2008, by Michael Wetter:<br/>
+Fixed bug in assignment of parameter <code>sta0</code>.
+The earlier implementation
+required temperature to be a state, which is not always the case.
+</li>
+<li>
+March 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DelayFirstOrder;
diff --git a/AixLib/Fluid/Delays/Examples/Delay.mo b/AixLib/Fluid/Delays/Examples/Delay.mo
index 4df2cdb28c..44b54cda5a 100644
--- a/AixLib/Fluid/Delays/Examples/Delay.mo
+++ b/AixLib/Fluid/Delays/Examples/Delay.mo
@@ -61,6 +61,6 @@ equation
       color={0,127,255}));
     annotation (experiment(Tolerance=1e-6, StopTime=300),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Delays/Examples/Delay.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Delay;
diff --git a/AixLib/Fluid/Examples/FlowSystem/Basic.mo b/AixLib/Fluid/Examples/FlowSystem/Basic.mo
index e007c4665b..968511ab58 100644
--- a/AixLib/Fluid/Examples/FlowSystem/Basic.mo
+++ b/AixLib/Fluid/Examples/FlowSystem/Basic.mo
@@ -481,57 +481,57 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Example model demonstrating the use of the <code>AixLib</code> components in a larger system.
- This model is extended in
- <a href=\"modelica://AixLib.Fluid.Examples.FlowSystem.Simplified1\">
- AixLib.Fluid.Examples.FlowSystem.Simplified1</a>,
- <a href=\"modelica://AixLib.Fluid.Examples.FlowSystem.Simplified2\">
- AixLib.Fluid.Examples.FlowSystem.Simplified2</a>,
- <a href=\"modelica://AixLib.Fluid.Examples.FlowSystem.Simplified3\">
- AixLib.Fluid.Examples.FlowSystem.Simplified3</a>.
- In these examples, the flow network is simplified in three steps, which reduces the size of algebraic loops.
- </p>
- <p>
- The system model is for a hydronic system with a hot and cold water production device,
- each having its own circulation pump.
- The warm and cold supply water temperatures are selected by switching the bottom two-way valves.
- The building consists of a west and east wing.
- Each wing has multiple zones that are heated or cooled using the hydronic system.
- Each wing has a north and south section with a different supply temperature,
- which is controlled using two main three way valves.
- In total there are therefore four supply pipes,
- which are each connected to four or eight emission devices in the zones.
- The flow through the emission devices is controlled using two way valves.
- The emission device itself also generates a pressure drop,
- represented by components <code>tabsX</code>.
- Note that the emission devices are in the real building
- cooling and heating concrete slabs, but this simplified example
- only models their flow resistance.
- The control model consists of dummy inputs.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 11, 2019 by Michael Wetter:<br/>
- Removed <code>each</code> statements.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1079\">#1079</a>.
- </li>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- October 7, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Example model demonstrating the use of the <code>AixLib</code> components in a larger system.
+This model is extended in
+<a href=\"modelica://AixLib.Fluid.Examples.FlowSystem.Simplified1\">
+AixLib.Fluid.Examples.FlowSystem.Simplified1</a>,
+<a href=\"modelica://AixLib.Fluid.Examples.FlowSystem.Simplified2\">
+AixLib.Fluid.Examples.FlowSystem.Simplified2</a>,
+<a href=\"modelica://AixLib.Fluid.Examples.FlowSystem.Simplified3\">
+AixLib.Fluid.Examples.FlowSystem.Simplified3</a>.
+In these examples, the flow network is simplified in three steps, which reduces the size of algebraic loops.
+</p>
+<p>
+The system model is for a hydronic system with a hot and cold water production device,
+each having its own circulation pump.
+The warm and cold supply water temperatures are selected by switching the bottom two-way valves.
+The building consists of a west and east wing.
+Each wing has multiple zones that are heated or cooled using the hydronic system.
+Each wing has a north and south section with a different supply temperature,
+which is controlled using two main three way valves.
+In total there are therefore four supply pipes,
+which are each connected to four or eight emission devices in the zones.
+The flow through the emission devices is controlled using two way valves.
+The emission device itself also generates a pressure drop,
+represented by components <code>tabsX</code>.
+Note that the emission devices are in the real building
+cooling and heating concrete slabs, but this simplified example
+only models their flow resistance.
+The control model consists of dummy inputs.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 11, 2019 by Michael Wetter:<br/>
+Removed <code>each</code> statements.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1079\">#1079</a>.
+</li>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+October 7, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/FlowSystem/Basic.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Basic;
diff --git a/AixLib/Fluid/Examples/FlowSystem/Simplified1.mo b/AixLib/Fluid/Examples/FlowSystem/Simplified1.mo
index 3903784066..c761e6be38 100644
--- a/AixLib/Fluid/Examples/FlowSystem/Simplified1.mo
+++ b/AixLib/Fluid/Examples/FlowSystem/Simplified1.mo
@@ -10,25 +10,25 @@ model Simplified1 "Aggregated pressure drops"
     valNorth1(each dpFixed_nominal=50000),
     valNorth2(each dpFixed_nominal=50000));
   annotation (Documentation(info="<html>
- <p>
- The model is simplified: series pressure drop components are aggregated into the valve model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 22, 2017, by Filip Jorissen:<br/>
- Revised simulation duration since otherwise
- the model only operates in the laminar region.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/825\">#825</a>.
- </li>
- <li>
- October 7, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+The model is simplified: series pressure drop components are aggregated into the valve model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2017, by Filip Jorissen:<br/>
+Revised simulation duration since otherwise
+the model only operates in the laminar region.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/825\">#825</a>.
+</li>
+<li>
+October 7, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(StopTime=1000, Tolerance=1e-06),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/FlowSystem/Simplified1.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Simplified1;
diff --git a/AixLib/Fluid/Examples/FlowSystem/Simplified2.mo b/AixLib/Fluid/Examples/FlowSystem/Simplified2.mo
index 3b7d6b915f..a9398afcea 100644
--- a/AixLib/Fluid/Examples/FlowSystem/Simplified2.mo
+++ b/AixLib/Fluid/Examples/FlowSystem/Simplified2.mo
@@ -6,23 +6,23 @@ model Simplified2 "Using from_dp"
     valNorth1(each from_dp=true),
     valNorth2(each from_dp=true));
   annotation (Documentation(info="<html>
- <p>
- The model is simplified: using <code>from_dp</code> to find more efficient tearing variables.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 14, 2016, by Michael Wetter:<br/>
- Added missing <code>each</code> keyword.
- </li>
- <li>
- October 7, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+The model is simplified: using <code>from_dp</code> to find more efficient tearing variables.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 14, 2016, by Michael Wetter:<br/>
+Added missing <code>each</code> keyword.
+</li>
+<li>
+October 7, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/FlowSystem/Simplified2.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Simplified2;
diff --git a/AixLib/Fluid/Examples/FlowSystem/Simplified3.mo b/AixLib/Fluid/Examples/FlowSystem/Simplified3.mo
index 4ccb025684..355ba2b43a 100644
--- a/AixLib/Fluid/Examples/FlowSystem/Simplified3.mo
+++ b/AixLib/Fluid/Examples/FlowSystem/Simplified3.mo
@@ -6,20 +6,20 @@ model Simplified3 "Neglecting pressure drop in splitters"
     spl3(dp_nominal={0,0,0}),
     spl2(dp_nominal={1000,0,0}));
   annotation (Documentation(info="<html>
- <p>
- The model is further simplified by removing some small pressure drops in the bypass.
- This allows the solver to identify sub-circuits.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 7, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+The model is further simplified by removing some small pressure drops in the bypass.
+This allows the solver to identify sub-circuits.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 7, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/FlowSystem/Simplified3.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Simplified3;
diff --git a/AixLib/Fluid/Examples/FlowSystem/Simplified4.mo b/AixLib/Fluid/Examples/FlowSystem/Simplified4.mo
index 3c688f6955..0b8c09fee0 100644
--- a/AixLib/Fluid/Examples/FlowSystem/Simplified4.mo
+++ b/AixLib/Fluid/Examples/FlowSystem/Simplified4.mo
@@ -18,29 +18,29 @@ model Simplified4 "Removed valve dynamics"
     valCoo(use_inputFilter=false),
     valHea(use_inputFilter=false));
   annotation (Documentation(info="<html>
- <p>
- The model is further simplified by removing the valve and pump control dynamics.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 12, 2019 by Michael Wetter:<br/>
- Removed <code>each</code> statements.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1079\">#1079</a>.
- </li>
- <li>
- December 14, 2016, by Michael Wetter:<br/>
- Added missing <code>each</code> keywords.
- </li>
- <li>
- October 7, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+The model is further simplified by removing the valve and pump control dynamics.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 12, 2019 by Michael Wetter:<br/>
+Removed <code>each</code> statements.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1079\">#1079</a>.
+</li>
+<li>
+December 14, 2016, by Michael Wetter:<br/>
+Added missing <code>each</code> keywords.
+</li>
+<li>
+October 7, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/FlowSystem/Simplified4.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Simplified4;
diff --git a/AixLib/Fluid/Examples/FlowSystem/Simplified5.mo b/AixLib/Fluid/Examples/FlowSystem/Simplified5.mo
index 5e21a69f19..c0453d87f3 100644
--- a/AixLib/Fluid/Examples/FlowSystem/Simplified5.mo
+++ b/AixLib/Fluid/Examples/FlowSystem/Simplified5.mo
@@ -9,26 +9,26 @@ model Simplified5 "Removed most mass/energy dynamics"
     pumpHea(energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState),
     heater(energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial));
   annotation (Documentation(info="<html>
- <p>
- The model is further simplified by setting the mass dynamics and energy dynamics
- of most models to be steady state.
- Note that by default, the mass dynamics is set to the same configuration
- as the energy dynamics.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 14, 2016, by Michael Wetter:<br/>
- Removed superfluous assignment of mass dynamics.
- </li>
- <li>
- October 7, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+The model is further simplified by setting the mass dynamics and energy dynamics
+of most models to be steady state.
+Note that by default, the mass dynamics is set to the same configuration
+as the energy dynamics.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 14, 2016, by Michael Wetter:<br/>
+Removed superfluous assignment of mass dynamics.
+</li>
+<li>
+October 7, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/FlowSystem/Simplified5.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Simplified5;
diff --git a/AixLib/Fluid/Examples/FlowSystem/Simplified6.mo b/AixLib/Fluid/Examples/FlowSystem/Simplified6.mo
index ce19bb9c44..a6b8d5c614 100644
--- a/AixLib/Fluid/Examples/FlowSystem/Simplified6.mo
+++ b/AixLib/Fluid/Examples/FlowSystem/Simplified6.mo
@@ -21,23 +21,23 @@ model Simplified6 "Set allowFlowReversal=false"
     valCoo(allowFlowReversal=false),
     valHea(allowFlowReversal=false));
   annotation (Documentation(info="<html>
- <p>
- The model is further simplified by setting <code>allowFlowReversal=false</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 14, 2016, by Michael Wetter:<br/>
- Added missing <code>each</code> keywords.
- </li>
- <li>
- October 7, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+The model is further simplified by setting <code>allowFlowReversal=false</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 14, 2016, by Michael Wetter:<br/>
+Added missing <code>each</code> keywords.
+</li>
+<li>
+October 7, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1000),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/FlowSystem/Simplified6.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Simplified6;
diff --git a/AixLib/Fluid/Examples/GeothermalHeatPump/BaseClasses/GeothermalHeatPumpBase.mo b/AixLib/Fluid/Examples/GeothermalHeatPump/BaseClasses/GeothermalHeatPumpBase.mo
index f104829a76..f20ec93d99 100644
--- a/AixLib/Fluid/Examples/GeothermalHeatPump/BaseClasses/GeothermalHeatPumpBase.mo
+++ b/AixLib/Fluid/Examples/GeothermalHeatPump/BaseClasses/GeothermalHeatPumpBase.mo
@@ -11,12 +11,15 @@ partial model GeothermalHeatPumpBase
   parameter Modelica.Units.SI.Temperature T_start_hot=300
     "Initial temperature of warm components";
 
-    replaceable AixLib.Fluid.Interfaces.PartialTwoPortTransport PeakLoadDevice(
-      redeclare package Medium = Medium)                                       constrainedby
-    AixLib.Fluid.Interfaces.PartialTwoPort
+  replaceable model PeakLoadDeviceModel =
+      AixLib.Fluid.Interfaces.PartialTwoPortTransport constrainedby
+    AixLib.Fluid.Interfaces.PartialTwoPortTransport(redeclare package Medium=Medium)
+    annotation(choicesAllMatching=true);
+
+    PeakLoadDeviceModel peaLoaDev
     annotation (Placement(transformation(extent={{108,-56},{120,-44}})));
 
-  Storage.BufferStorage
+  Storage.StorageDetailed
                   coldStorage(
     redeclare package Medium = Medium,
     redeclare package MediumHC1 = Medium,
@@ -38,7 +41,8 @@ partial model GeothermalHeatPumpBase
     n=5,
     hConIn=100,
     hConOut=10,
-    hConHC1=500)
+    hConHC1=500,
+    upToDownHC1=false)
          "Storage tank for buffering cold demand" annotation (Placement(transformation(extent={{24,-14},
             {52,20}})));
   FixedResistances.PressureDrop                     resistanceColdStorage(
@@ -86,7 +90,7 @@ partial model GeothermalHeatPumpBase
         extent={{-6,-7},{6,7}},
         rotation=90,
         origin={-60,1})));
-  Storage.BufferStorage
+  Storage.StorageDetailed
                   heatStorage(
     redeclare package Medium = Medium,
     redeclare package MediumHC1 = Medium,
@@ -256,7 +260,7 @@ equation
     annotation (Line(points={{-82,-54},{-79,-54},{-76,-54}}, color={0,127,255}));
   connect(pumpGeothermalSource.port_a, geothFieldSource.ports[1])
     annotation (Line(points={{-96,-54},{-146,-54}}, color={0,127,255}));
-  connect(resistanceHeatConsumerFlow.port_b, PeakLoadDevice.port_a) annotation (
+  connect(resistanceHeatConsumerFlow.port_b, peaLoaDev.port_a) annotation (
      Line(points={{94,-50},{102,-50},{108,-50}}, color={0,127,255}));
   connect(heatPump.port_b1, geothField_sink1.ports[1]) annotation (Line(points={{-16.5,
           20},{-16,20},{-16,28},{-146,28},{-146,27.2}},        color={0,127,255}));
@@ -283,11 +287,6 @@ equation
       Line(points={{33.275,-14.34},{33.275,-20},{58,-20}}, color={0,127,255}));
   connect(coldStorage.fluidportTop1, resistanceColdConsumerReturn.port_b)
     annotation (Line(points={{33.1,20.17},{33.1,32},{80,32}}, color={0,127,255}));
-  connect(heatPump.port_b2, coldStorage.portHC1Out) annotation (Line(points={{
-          -33.5,-8.00002},{-33.5,-22},{16,-22},{16,7.42},{23.825,7.42}}, color=
-          {0,127,255}));
-  connect(pumpEvaporator.port_a, coldStorage.portHC1In) annotation (Line(points=
-         {{14,36},{18,36},{18,12.69},{23.65,12.69}}, color={0,127,255}));
   connect(pumpCondenser.port_a, heatStorage.portHC1Out) annotation (Line(points=
          {{6,-98},{16,-98},{16,-74.58},{23.825,-74.58}}, color={0,127,255}));
   connect(heatPump.port_b1, heatStorage.portHC1In) annotation (Line(points={{
@@ -297,6 +296,11 @@ equation
   connect(resistanceHeatConsumerReturn.port_b, heatStorage.fluidportBottom2)
     annotation (Line(points={{80,-106},{42.025,-106},{42.025,-96.17}}, color={0,
           127,255}));
+  connect(pumpEvaporator.port_a, coldStorage.portHC1Out) annotation (Line(
+        points={{14,36},{16,36},{16,7.42},{23.825,7.42}}, color={0,127,255}));
+  connect(heatPump.port_b2, coldStorage.portHC1In) annotation (Line(points={{
+          -33.5,-8.00002},{-33.5,-16},{14,-16},{14,12.69},{23.65,12.69}}, color
+        ={0,127,255}));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-160,
           -120},{160,80}})),              Icon(coordinateSystem(
           preserveAspectRatio=false, extent={{-160,-120},{160,80}})),
diff --git a/AixLib/Fluid/Examples/GeothermalHeatPump/GeothermalHeatPump.mo b/AixLib/Fluid/Examples/GeothermalHeatPump/GeothermalHeatPump.mo
index 48be7fd6ae..94b155f3c3 100644
--- a/AixLib/Fluid/Examples/GeothermalHeatPump/GeothermalHeatPump.mo
+++ b/AixLib/Fluid/Examples/GeothermalHeatPump/GeothermalHeatPump.mo
@@ -1,11 +1,12 @@
-within AixLib.Fluid.Examples.GeothermalHeatPump;
+within AixLib.Fluid.Examples.GeothermalHeatPump;
 model GeothermalHeatPump "Example of a geothermal heat pump system"
 
   extends Modelica.Icons.Example;
 
   extends AixLib.Fluid.Examples.GeothermalHeatPump.BaseClasses.GeothermalHeatPumpControlledBase(
-  redeclare AixLib.Fluid.Examples.GeothermalHeatPump.Components.BoilerStandAlone PeakLoadDevice(redeclare
-        package                                                                                                   Medium =
+  redeclare model PeakLoadDeviceModel=
+        AixLib.Fluid.Examples.GeothermalHeatPump.Components.BoilerStandAlone (                             redeclare
+          package                                                                                                 Medium =
                          Medium, energyDynamics=energyDynamics),
                                   heatPump(
       redeclare package Medium_con = Medium,
@@ -36,6 +37,7 @@ model GeothermalHeatPump "Example of a geothermal heat pump system"
               AixLib.DataBase.HeatPump.EN255.Vitocal350BWH110()),
       redeclare model PerDataRevHP =
           DataBase.Chiller.PerformanceData.LookUpTable2D),
+    heatPumpControlBus.iceFacMea = 1,
     heatStorage(energyDynamics=energyDynamics),
     coldStorage(energyDynamics=energyDynamics),
     pumpCondenser(energyDynamics=energyDynamics),
@@ -113,7 +115,7 @@ equation
   connect(pumpGeothermalSource.dp_in,pressureDifference. y) annotation (Line(
         points={{-89,-45.6},{-89,-36},{56,-36},{56,6},{147.4,6}},      color={0,
           0,127}));
-  connect(PeakLoadDevice.port_b,heatConsumerFlow. ports[1]) annotation (Line(
+  connect(peaLoaDev.port_b,heatConsumerFlow. ports[1]) annotation (Line(
         points={{120,-50},{120,-50},{148,-50}}, color={0,127,255}));
   connect(hPControllerOnOff.heatPumpControlBus, heatPumpControlBus) annotation (
      Line(
@@ -123,7 +125,7 @@ equation
       string="%second",
       index=1,
       extent={{6,3},{6,3}}));
-  connect(PeakLoadDevice.chemicalEnergyFlowRate, chemicalEnergyFlowRate)
+  connect(peaLoaDev.chemicalEnergyFlowRate, chemicalEnergyFlowRate)
     annotation (Line(points={{112.77,-56.54},{112.77,-118},{-26,-118},{-26,-100},
           {-71.5,-100},{-71.5,-119.5}}, color={0,0,127}));
   connect(getTStorageLower.y,geothermalFieldControllerCold. temperature)
@@ -151,7 +153,7 @@ equation
           -147.4,6},{-130,6},{-130,76},{-78,76}}, color={0,0,127}));
   connect(getTStorageUpper.y, hPControllerOnOff.TMea)
     annotation (Line(points={{-139,68},{-78,68}}, color={0,0,127}));
-  annotation (experiment(Tolerance=1e-6, StartTime=0, StopTime=86400), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/GeothermalHeatPump.mos"
+  annotation (experiment(Tolerance=1e-6, StartTime=0, Interval=500, StopTime=86400, __Dymola_Algorithm="Dassl"), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/GeothermalHeatPump.mos"
         "Simulate and plot"), Documentation(revisions="<html><ul>
   <li>
     <i>May 5, 2021</i> by Fabian Wüllhorst:<br/>
diff --git a/AixLib/Fluid/Examples/Performance/BaseClasses/Example1.mo b/AixLib/Fluid/Examples/Performance/BaseClasses/Example1.mo
index 9af2f8b2a4..420ebb80f7 100644
--- a/AixLib/Fluid/Examples/Performance/BaseClasses/Example1.mo
+++ b/AixLib/Fluid/Examples/Performance/BaseClasses/Example1.mo
@@ -97,38 +97,38 @@ equation
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-20},{100,
             100}}), graphics),
     Documentation(info="<html>
- <p>
- This partial model is extended by
- <a href=\"modelica://AixLib.Fluid.Examples.Performance.Example1v1\">
- AixLib.Fluid.Examples.Performance.Example1v1</a>
- and
- <a href=\"modelica://AixLib.Fluid.Examples.Performance.Example1v2\">
- AixLib.Fluid.Examples.Performance.Example1v2</a>
- and is created to avoid errors in the implementation of the two depending examples.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- February 22, 2016, by Michael Wetter:<br/>
- Removed parameter <code>dynamicBalance</code> for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/411\">issue 411</a>.
- </li>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This partial model is extended by
+<a href=\"modelica://AixLib.Fluid.Examples.Performance.Example1v1\">
+AixLib.Fluid.Examples.Performance.Example1v1</a>
+and
+<a href=\"modelica://AixLib.Fluid.Examples.Performance.Example1v2\">
+AixLib.Fluid.Examples.Performance.Example1v2</a>
+and is created to avoid errors in the implementation of the two depending examples.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+February 22, 2016, by Michael Wetter:<br/>
+Removed parameter <code>dynamicBalance</code> for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/411\">issue 411</a>.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example1;
diff --git a/AixLib/Fluid/Examples/Performance/Example1v1.mo b/AixLib/Fluid/Examples/Performance/Example1v1.mo
index ccbe17576b..e50c300ad8 100644
--- a/AixLib/Fluid/Examples/Performance/Example1v1.mo
+++ b/AixLib/Fluid/Examples/Performance/Example1v1.mo
@@ -18,96 +18,96 @@ equation
           fillPattern=FillPattern.Solid,
           fillColor={0,0,255})}),
     Documentation(info="<html>
- <p>
- This model demonstrates the impact of the <code>allowFlowReversal</code>
- and <code>from_dp</code> parameters on the sizes of nonlinear algebraic loops.
- The user can change the parameter value in the respective
- <code>BooleanConstant</code> blocks and rerun the simulation to compare the performance.
- The results are also demonstrated below for <code>nRes.k = 20</code>,
- the number of parallel branches, which contain one pressure drop element each.
- </p>
- <p>
- These results were generated using Dymola 2015FD01 64 bit on Ubuntu 14.04.
- </p>
- <h4>Default case:</h4>
- <p>
- <code>AllowFlowReversal = true</code> and <code>from_dp = false</code>
- </p>
- <p>
- Sizes of nonlinear systems of equations: {6, 21, <b>46</b>}
- </p>
- <p>
- Sizes after manipulation of the nonlinear systems: {1, 19, <b>22</b>}
- </p>
- <h4>Change 1: </h4>
- <p>
- <code>AllowFlowReversal = false</code> and <code>from_dp = false</code>
- </p>
- <p>
- Sizes of nonlinear systems of equations: {6, 21}
- </p>
- <p>
- Sizes after manipulation of the nonlinear systems: {1, 19}
- </p>
- <h4>Change 2: </h4>
- <p>
- <code>AllowFlowReversal = false</code> and <code>from_dp = true</code>
- </p>
- <p>
- Sizes of nonlinear systems of equations: {6, 21}
- </p>
- <p>
- Sizes after manipulation of the nonlinear systems: {1, <b>1</b>}
- </p>
- <p>
- These changes also have a significant impact on the computational speed.
- </p>
- <p>
- Following script can be used in Dymola to compare the CPU times.
- For this script to work, make sure that Dymola stores at least 4 results.
- </p>
- <p>
- <code>
- cpuOld=OutputCPUtime;<br/>
- evaluateOld=Evaluate;<br/>
- OutputCPUtime:=true;<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example1v1(allowFlowReversal.k=true, from_dp.k=false)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example1v1\");<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example1v2(from_dp.k=true, allowFlowReversal.k=true)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example1v2\");<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example1v1(allowFlowReversal.k=false, from_dp.k=false)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example1v1\");<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example1v1(allowFlowReversal.k=false, from_dp.k=true)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example1v1\");<br/>
- createPlot(id=1, position={15, 10, 592, 421}, range={0.0, 10000.0, -0.01, 0.35}, autoscale=false, grid=true);<br/>
- plotExpression(apply(Example1v1[end-2].CPUtime), false, \"Default case\", 1);<br/>
- plotExpression(apply(Example1v2[end].CPUtime), false, \"Adding dummy states\", 1);<br/>
- plotExpression(apply(Example1v1[end-1].CPUtime), false, \"allowFlowReversal=false\", 1);<br/>
- plotExpression(apply(Example1v1[end].CPUtime), false, \"allowFlowReversal=false, from_dp=true\", 1);<br/>
- OutputCPUtime=cpuOld;<br/>
- Evaluate=evaluateOld;</code>
- </p>
- <p>
- See Jorissen et al. (2015) for a discussion.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
- Simulation speed analysis and improvements of Modelica
- models for building energy simulation.<br/>
- Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the impact of the <code>allowFlowReversal</code>
+and <code>from_dp</code> parameters on the sizes of nonlinear algebraic loops.
+The user can change the parameter value in the respective
+<code>BooleanConstant</code> blocks and rerun the simulation to compare the performance.
+The results are also demonstrated below for <code>nRes.k = 20</code>,
+the number of parallel branches, which contain one pressure drop element each.
+</p>
+<p>
+These results were generated using Dymola 2015FD01 64 bit on Ubuntu 14.04.
+</p>
+<h4>Default case:</h4>
+<p>
+<code>AllowFlowReversal = true</code> and <code>from_dp = false</code>
+</p>
+<p>
+Sizes of nonlinear systems of equations: {6, 21, <b>46</b>}
+</p>
+<p>
+Sizes after manipulation of the nonlinear systems: {1, 19, <b>22</b>}
+</p>
+<h4>Change 1: </h4>
+<p>
+<code>AllowFlowReversal = false</code> and <code>from_dp = false</code>
+</p>
+<p>
+Sizes of nonlinear systems of equations: {6, 21}
+</p>
+<p>
+Sizes after manipulation of the nonlinear systems: {1, 19}
+</p>
+<h4>Change 2: </h4>
+<p>
+<code>AllowFlowReversal = false</code> and <code>from_dp = true</code>
+</p>
+<p>
+Sizes of nonlinear systems of equations: {6, 21}
+</p>
+<p>
+Sizes after manipulation of the nonlinear systems: {1, <b>1</b>}
+</p>
+<p>
+These changes also have a significant impact on the computational speed.
+</p>
+<p>
+Following script can be used in Dymola to compare the CPU times.
+For this script to work, make sure that Dymola stores at least 4 results.
+</p>
+<p>
+<code>
+cpuOld=OutputCPUtime;<br/>
+evaluateOld=Evaluate;<br/>
+OutputCPUtime:=true;<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example1v1(allowFlowReversal.k=true, from_dp.k=false)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example1v1\");<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example1v2(from_dp.k=true, allowFlowReversal.k=true)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example1v2\");<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example1v1(allowFlowReversal.k=false, from_dp.k=false)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example1v1\");<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example1v1(allowFlowReversal.k=false, from_dp.k=true)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example1v1\");<br/>
+createPlot(id=1, position={15, 10, 592, 421}, range={0.0, 10000.0, -0.01, 0.35}, autoscale=false, grid=true);<br/>
+plotExpression(apply(Example1v1[end-2].CPUtime), false, \"Default case\", 1);<br/>
+plotExpression(apply(Example1v2[end].CPUtime), false, \"Adding dummy states\", 1);<br/>
+plotExpression(apply(Example1v1[end-1].CPUtime), false, \"allowFlowReversal=false\", 1);<br/>
+plotExpression(apply(Example1v1[end].CPUtime), false, \"allowFlowReversal=false, from_dp=true\", 1);<br/>
+OutputCPUtime=cpuOld;<br/>
+Evaluate=evaluateOld;</code>
+</p>
+<p>
+See Jorissen et al. (2015) for a discussion.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
+Simulation speed analysis and improvements of Modelica
+models for building energy simulation.<br/>
+Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example1v1.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example1v1;
diff --git a/AixLib/Fluid/Examples/Performance/Example1v2.mo b/AixLib/Fluid/Examples/Performance/Example1v2.mo
index 7181f3d3d3..8e6b07ed1e 100644
--- a/AixLib/Fluid/Examples/Performance/Example1v2.mo
+++ b/AixLib/Fluid/Examples/Performance/Example1v2.mo
@@ -28,57 +28,57 @@ equation
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-20},{100,
             100}}), graphics),
     Documentation(info="<html>
- <p>
- This example is an extension of
- <a href=\"modelica://AixLib.Fluid.Examples.Performance.Example1v1\">
- AixLib.Fluid.Examples.Performance.Example1v1</a>
- and demonstrates the use of
- mixing volumes for decoupling the algebraic loop that solves for the enthalpy of the system.
- </p>
- <h4>Example1v1:</h4>
- <p>
- Sizes of nonlinear systems of equations: {6, 21, <b>46</b>}
- </p>
- <p>
- Sizes after manipulation of the nonlinear systems: {1, 19, <b>22</b>}
- </p>
- <h4>Example1v2 using mixing volumes: </h4>
- <p>
- Sizes of nonlinear systems of equations: {6, 21, <b>4</b>}
- </p>
- <p>
- Sizes after manipulation of the nonlinear systems: {1, 19, <b>1</b>}
- </p>
- <p>
- See Jorissen et al. (2015) for a discussion.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
- Simulation speed analysis and improvements of Modelica
- models for building energy simulation.<br/>
- Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- August 31, 2015, by Michael Wetter:<br/>
- Added missing <code>each</code> in declaration of the energy balance
- for the volume.
- </li>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example is an extension of
+<a href=\"modelica://AixLib.Fluid.Examples.Performance.Example1v1\">
+AixLib.Fluid.Examples.Performance.Example1v1</a>
+and demonstrates the use of
+mixing volumes for decoupling the algebraic loop that solves for the enthalpy of the system.
+</p>
+<h4>Example1v1:</h4>
+<p>
+Sizes of nonlinear systems of equations: {6, 21, <b>46</b>}
+</p>
+<p>
+Sizes after manipulation of the nonlinear systems: {1, 19, <b>22</b>}
+</p>
+<h4>Example1v2 using mixing volumes: </h4>
+<p>
+Sizes of nonlinear systems of equations: {6, 21, <b>4</b>}
+</p>
+<p>
+Sizes after manipulation of the nonlinear systems: {1, 19, <b>1</b>}
+</p>
+<p>
+See Jorissen et al. (2015) for a discussion.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
+Simulation speed analysis and improvements of Modelica
+models for building energy simulation.<br/>
+Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+August 31, 2015, by Michael Wetter:<br/>
+Added missing <code>each</code> in declaration of the energy balance
+for the volume.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example1v2.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example1v2;
diff --git a/AixLib/Fluid/Examples/Performance/Example2.mo b/AixLib/Fluid/Examples/Performance/Example2.mo
index 920cb5ff18..aed7daa8f4 100644
--- a/AixLib/Fluid/Examples/Performance/Example2.mo
+++ b/AixLib/Fluid/Examples/Performance/Example2.mo
@@ -59,72 +59,72 @@ equation
             -40},{40,60}}),    graphics),
     experiment(Tolerance=1e-6, StopTime=20),
     Documentation(info="<html>
- <p>
- This example demonstrates that the use of the parameter <code>from_dp</code>
- can be important for reducing the size of algebraic loops in hydraulic
- circuits with many pressure drop components connected in series and
- a pump setting the pressure head.
- </p>
- <p>
- If <code>from_dp=true</code>, we obtain: <br/>
- 
- Sizes of nonlinear systems of equations: {7}<br/>
- Sizes after manipulation of the nonlinear systems: {<b>5</b>}<br/>
- If <code>from_dp=false</code>, we obtain: <br/>
- Sizes of nonlinear systems of equations: {7}<br/>
- Sizes after manipulation of the nonlinear systems: {<b>1</b>}<br/>
- </p>
- <p>
- This can have a large impact on computational speed.
- </p>
- <p>
- Following script can be used in Dymola to compare the CPU times.
- </p>
- <p>
- <code>
- cpuOld=OutputCPUtime;<br/>
- evaluateOld=Evaluate;<br/>
- OutputCPUtime:=true;<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example2(from_dp.k=false)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example2\");<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example2(from_dp.k=true)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example2\");<br/>
- createPlot(id=1, position={15, 10, 592, 421}, range={0.0, 10000.0, -0.01, 25}, autoscale=false, grid=true);<br/>
- plotExpression(apply(Example2[end-1].CPUtime), false, \"from_dp=false\", 1);<br/>
- plotExpression(apply(Example2[end].CPUtime), false, \"from_dp=true\", 1);<br/>
- OutputCPUtime=cpuOld;<br/>
- Evaluate=evaluateOld;<br/>
- </code>
- </p>
- <p>
- See Jorissen et al. (2015) for a discussion.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
- Simulation speed analysis and improvements of Modelica
- models for building energy simulation.<br/>
- Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- May 20, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates that the use of the parameter <code>from_dp</code>
+can be important for reducing the size of algebraic loops in hydraulic
+circuits with many pressure drop components connected in series and
+a pump setting the pressure head.
+</p>
+<p>
+If <code>from_dp=true</code>, we obtain: <br/>
+
+Sizes of nonlinear systems of equations: {7}<br/>
+Sizes after manipulation of the nonlinear systems: {<b>5</b>}<br/>
+If <code>from_dp=false</code>, we obtain: <br/>
+Sizes of nonlinear systems of equations: {7}<br/>
+Sizes after manipulation of the nonlinear systems: {<b>1</b>}<br/>
+</p>
+<p>
+This can have a large impact on computational speed.
+</p>
+<p>
+Following script can be used in Dymola to compare the CPU times.
+</p>
+<p>
+<code>
+cpuOld=OutputCPUtime;<br/>
+evaluateOld=Evaluate;<br/>
+OutputCPUtime:=true;<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example2(from_dp.k=false)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example2\");<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example2(from_dp.k=true)\", stopTime=10000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example2\");<br/>
+createPlot(id=1, position={15, 10, 592, 421}, range={0.0, 10000.0, -0.01, 25}, autoscale=false, grid=true);<br/>
+plotExpression(apply(Example2[end-1].CPUtime), false, \"from_dp=false\", 1);<br/>
+plotExpression(apply(Example2[end].CPUtime), false, \"from_dp=true\", 1);<br/>
+OutputCPUtime=cpuOld;<br/>
+Evaluate=evaluateOld;<br/>
+</code>
+</p>
+<p>
+See Jorissen et al. (2015) for a discussion.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
+Simulation speed analysis and improvements of Modelica
+models for building energy simulation.<br/>
+Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+May 20, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example2.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example2;
diff --git a/AixLib/Fluid/Examples/Performance/Example3.mo b/AixLib/Fluid/Examples/Performance/Example3.mo
index ee1af3018b..e0a7e164e3 100644
--- a/AixLib/Fluid/Examples/Performance/Example3.mo
+++ b/AixLib/Fluid/Examples/Performance/Example3.mo
@@ -74,66 +74,66 @@ equation
             -60},{60,40}}),    graphics),
     experiment(Tolerance=1e-6, StopTime=20),
     Documentation(revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This example demonstrates the importance of merging
- pressure drop components that are connected in series,
- into one pressure drop component.
- Parameter <code>mergeDp.k</code> can be used to merge two components
- that are connected in series.
- Parameter <code>from_dp</code> also has an influence of the computational speed.
- </p>
- <p>
- Following script can be used in Dymola to compare the CPU times.
- For this script to work, make sure that Dymola stores at least 4 results.
- </p>
- <p>
- <code>
- cpuOld=OutputCPUtime;<br/>
- evaluateOld=Evaluate;<br/>
- OutputCPUtime:=true;<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example3(from_dp.k=false, mergeDp.k=false, nRes.k=10)\", stopTime=1000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example3\");<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example3(from_dp.k=false, mergeDp.k=true, nRes.k=10)\", stopTime=1000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example3\");<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example3(from_dp.k=true, mergeDp.k=false, nRes.k=10)\", stopTime=1000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example3\");<br/>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example3(from_dp.k=true, mergeDp.k=true, nRes.k=10)\", stopTime=1000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example3\");<br/>
- createPlot(id=1, position={15, 10, 592, 421}, range={0.0, 1000.0, -0.01, 8}, autoscale=false, grid=true);<br/>
- plotExpression(apply(Example3[end-3].CPUtime), false, \"from_dp=false, mergeDp=false\", 1);<br/>
- plotExpression(apply(Example3[end-2].CPUtime), false, \"from_dp=false, mergeDp=true\", 1);<br/>
- plotExpression(apply(Example3[end-1].CPUtime), false, \"from_dp=true, mergeDp=false\", 1);<br/>
- plotExpression(apply(Example3[end].CPUtime), false, \"from_dp=true, mergeDp=true\", 1);<br/>
- OutputCPUtime=cpuOld;<br/>
- Evaluate=evaluateOld;</code>
- </p>
- <p>
- See Jorissen et al. (2015) for a discussion.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
- Simulation speed analysis and improvements of Modelica
- models for building energy simulation.<br/>
- Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example demonstrates the importance of merging
+pressure drop components that are connected in series,
+into one pressure drop component.
+Parameter <code>mergeDp.k</code> can be used to merge two components
+that are connected in series.
+Parameter <code>from_dp</code> also has an influence of the computational speed.
+</p>
+<p>
+Following script can be used in Dymola to compare the CPU times.
+For this script to work, make sure that Dymola stores at least 4 results.
+</p>
+<p>
+<code>
+cpuOld=OutputCPUtime;<br/>
+evaluateOld=Evaluate;<br/>
+OutputCPUtime:=true;<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example3(from_dp.k=false, mergeDp.k=false, nRes.k=10)\", stopTime=1000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example3\");<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example3(from_dp.k=false, mergeDp.k=true, nRes.k=10)\", stopTime=1000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example3\");<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example3(from_dp.k=true, mergeDp.k=false, nRes.k=10)\", stopTime=1000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example3\");<br/>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example3(from_dp.k=true, mergeDp.k=true, nRes.k=10)\", stopTime=1000, numberOfIntervals=10, method=\"dassl\", resultFile=\"Example3\");<br/>
+createPlot(id=1, position={15, 10, 592, 421}, range={0.0, 1000.0, -0.01, 8}, autoscale=false, grid=true);<br/>
+plotExpression(apply(Example3[end-3].CPUtime), false, \"from_dp=false, mergeDp=false\", 1);<br/>
+plotExpression(apply(Example3[end-2].CPUtime), false, \"from_dp=false, mergeDp=true\", 1);<br/>
+plotExpression(apply(Example3[end-1].CPUtime), false, \"from_dp=true, mergeDp=false\", 1);<br/>
+plotExpression(apply(Example3[end].CPUtime), false, \"from_dp=true, mergeDp=true\", 1);<br/>
+OutputCPUtime=cpuOld;<br/>
+Evaluate=evaluateOld;</code>
+</p>
+<p>
+See Jorissen et al. (2015) for a discussion.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
+Simulation speed analysis and improvements of Modelica
+models for building energy simulation.<br/>
+Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example3.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example3;
diff --git a/AixLib/Fluid/Examples/Performance/Example4.mo b/AixLib/Fluid/Examples/Performance/Example4.mo
index bc71c643a7..6c35bc0c39 100644
--- a/AixLib/Fluid/Examples/Performance/Example4.mo
+++ b/AixLib/Fluid/Examples/Performance/Example4.mo
@@ -106,60 +106,60 @@ equation
       color={0,127,255}));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-80,-20},
             {80,60}}),         graphics),    Documentation(revisions="<html>
- <ul>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed connection that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- July 28, 2015, by Michael Wetter:<br/>
- Moved assignment of <code>m_condens</code> from equation section to
- declaration to avoid graphical and textual equations.
- </li>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This example generates a non-linear algebraic loop
- that consists of <i>12</i> equations before manipulation.
- This loop can be decoupled and removed by changing the equation
- </p>
- <pre>
- port_a.m_flow + port_b.m_flow = -mWat_flow;
- </pre>
- <p>
- in
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- to
- </p>
- <pre>
- port_a.m_flow + port_b.m_flow = 0;
- </pre>
- <p>
- See Jorissen et al. (2015) for a discussion.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
- Simulation speed analysis and improvements of Modelica
- models for building energy simulation.<br/>
- Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed connection that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+July 28, 2015, by Michael Wetter:<br/>
+Moved assignment of <code>m_condens</code> from equation section to
+declaration to avoid graphical and textual equations.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example generates a non-linear algebraic loop
+that consists of <i>12</i> equations before manipulation.
+This loop can be decoupled and removed by changing the equation
+</p>
+<pre>
+port_a.m_flow + port_b.m_flow = -mWat_flow;
+</pre>
+<p>
+in
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+to
+</p>
+<pre>
+port_a.m_flow + port_b.m_flow = 0;
+</pre>
+<p>
+See Jorissen et al. (2015) for a discussion.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
+Simulation speed analysis and improvements of Modelica
+models for building energy simulation.<br/>
+Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=20),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example4.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example4;
diff --git a/AixLib/Fluid/Examples/Performance/Example5.mo b/AixLib/Fluid/Examples/Performance/Example5.mo
index 6b9a6c0ab0..d1e7f55ffc 100644
--- a/AixLib/Fluid/Examples/Performance/Example5.mo
+++ b/AixLib/Fluid/Examples/Performance/Example5.mo
@@ -9,11 +9,14 @@ model Example5
   parameter Real b=sum(a);
 
   Real c;
+protected
+  constant Real k(final unit="1/s") = 1
+    "Unit conversion to satisfy unit check";
 initial equation
   c=0;
 
 equation
-  der(c) = sin(time)*(if efficient then b else sum(a));
+  der(c) = sin(k*time)*(if efficient then b else sum(a));
 
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,
             -40},{40,60}}),    graphics={Text(
@@ -22,60 +25,66 @@ equation
           textString="See code")}),
     experiment(Tolerance=1e-6, StopTime=20),
     Documentation(revisions="<html>
- <ul>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This example illustrates the impact of
- Modelica code formulations on the C-code.
- </p>
- <p>
- Compare the C-code in dsmodel.c when setting the parameter
- <code>efficient</code> to <code>true</code> or <code>false</code>
- and when adding <code>annotation(Evaluate=true)</code> to the parameter <code>efficient</code>.
- </p>
- <p>
- This produces:
- </p>
- <h4>Efficient = false and Evaluate = false</h4>
- <pre>
- helpvar[0] = sin(Time);
- F_[0] = helpvar[0]*(IF DP_[0] THEN W_[0] ELSE DP_[1]+DP_[2]+DP_[3]);
- </pre>
- <h4>Efficient = false and Evaluate = true</h4>
- <pre>
- helpvar[0] = sin(Time);
- F_[0] = helpvar[0]*(DP_[0]+DP_[1]+DP_[2]);
- </pre>
- <h4>Efficient = true and Evaluate = true</h4>
- <pre>
- helpvar[0] = sin(Time);
- F_[0] = helpvar[0]*W_[1];
- </pre>
- <p>
- The last option requires much less operations to be performed and is therefore more efficient.
- </p>
- <p>
- See Jorissen et al. (2015) for a discussion.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
- Simulation speed analysis and improvements of Modelica
- models for building energy simulation.<br/>
- Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
- </li>
- </ul>
- </html>"),__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example5.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 6, 2023, by Michael Wetter:<br/>
+Added a constant in order for unit check to pass.<br/>
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1711\">#1711</a>
+for a discussion.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example illustrates the impact of
+Modelica code formulations on the C-code.
+</p>
+<p>
+Compare the C-code in dsmodel.c when setting the parameter
+<code>efficient</code> to <code>true</code> or <code>false</code>
+and when adding <code>annotation(Evaluate=true)</code> to the parameter <code>efficient</code>.
+</p>
+<p>
+This produces:
+</p>
+<h4>Efficient = false and Evaluate = false</h4>
+<pre>
+helpvar[0] = sin(Time);
+F_[0] = helpvar[0]*(IF DP_[0] THEN W_[0] ELSE DP_[1]+DP_[2]+DP_[3]);
+</pre>
+<h4>Efficient = false and Evaluate = true</h4>
+<pre>
+helpvar[0] = sin(Time);
+F_[0] = helpvar[0]*(DP_[0]+DP_[1]+DP_[2]);
+</pre>
+<h4>Efficient = true and Evaluate = true</h4>
+<pre>
+helpvar[0] = sin(Time);
+F_[0] = helpvar[0]*W_[1];
+</pre>
+<p>
+The last option requires much less operations to be performed and is therefore more efficient.
+</p>
+<p>
+See Jorissen et al. (2015) for a discussion.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
+Simulation speed analysis and improvements of Modelica
+models for building energy simulation.<br/>
+Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
+</li>
+</ul>
+</html>"), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example5.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example5;
diff --git a/AixLib/Fluid/Examples/Performance/Example6.mo b/AixLib/Fluid/Examples/Performance/Example6.mo
index b423c8c67c..d255b982eb 100644
--- a/AixLib/Fluid/Examples/Performance/Example6.mo
+++ b/AixLib/Fluid/Examples/Performance/Example6.mo
@@ -10,10 +10,14 @@ model Example6
 
   Real[nCapacitors] T;
   Real[nCapacitors+1] Q_flow;
+
+protected
+  constant Real k(final unit="1/s") = 1
+    "Unit conversion to satisfy unit check";
 initial equation
   T = fill(273.15,nCapacitors);
 equation
-  Q_flow[1]=((273.15+sin(time))-T[1])/R;
+  Q_flow[1]=((273.15+sin(k*time))-T[1])/R;
   der(T[1])=(Q_flow[1]-Q_flow[2])/C;
   for i in 2:nCapacitors loop
     Q_flow[i] = (T[i-1] - T[i])/R;
@@ -29,75 +33,81 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=100),
     Documentation(revisions="<html>
- <ul>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>This example, together with
- <a href=\"modelica://AixLib.Fluid.Examples.Performance.Example7\">
- AixLib.Fluid.Examples.Performance.Example7</a>,
- illustrates the overhead
- generated by divisions by parameters. See Jorissen et al. (2015) for a complementary discussion.
- </p>
- <p>
- Running the following commands allows comparing the CPU times of the two models,
- disregarding as much as possible the influence of the integrator:
- </p>
- <pre>
- simulateModel(\"AixLib.Fluid.Examples.PerformanceExamples.Example6\", stopTime=100, numberOfIntervals=1, method=\"Rkfix4\", fixedstepsize=0.001, resultFile=\"Example6\");
- simulateModel(\"AixLib.Fluid.Examples.PerformanceExamples.Example7\", stopTime=100, numberOfIntervals=1, method=\"Rkfix4\", fixedstepsize=0.001, resultFile=\"Example7\");
- </pre>
- <p>
- Comparing the CPU times indicates a speed improvement of <i>56%</i>.
- This difference almost disappears when adding <code>annotation(Evaluate=true)</code>
- to <code>R</code> and <code>C</code>.
- </p>
- <p>
- In <code>dsmodel.c</code> we find:
- </p>
- <pre>
- DynamicsSection
- W_[2] = divmacro(X_[0]-X_[1],\"T[1]-T[2]\",DP_[0],\"R\");
- F_[0] = divmacro(W_[1]-W_[2],\"Q_flow[1]-Q_flow[2]\",DP_[1],\"C\");
- </pre>
- <p>
- This suggests that the parameter division needs to be handled during
- each function evaluation, probably causing the increased overhead.
- </p>
- <p>
- The following command allows comparing the CPU times objectively.
- </p>
- <p>
- <code>
- simulateModel(\"AixLib.Fluid.Examples.Performance.Example6\", stopTime=100, numberOfIntervals=1, method=\"Euler\", fixedstepsize=0.001, resultFile=\"Example6\");
- </code>
- </p>
- <p>
- See Jorissen et al. (2015) for a discussion.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
- Simulation speed analysis and improvements of Modelica
- models for building energy simulation.<br/>
- Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+March 6, 2023, by Michael Wetter:<br/>
+Added a constant in order for unit check to pass.<br/>
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1711\">#1711</a>
+for a discussion.
+</li>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>This example, together with
+<a href=\"modelica://AixLib.Fluid.Examples.Performance.Example7\">
+AixLib.Fluid.Examples.Performance.Example7</a>,
+illustrates the overhead
+generated by divisions by parameters. See Jorissen et al. (2015) for a complementary discussion.
+</p>
+<p>
+Running the following commands allows comparing the CPU times of the two models,
+disregarding as much as possible the influence of the integrator:
+</p>
+<pre>
+simulateModel(\"AixLib.Fluid.Examples.PerformanceExamples.Example6\", stopTime=100, numberOfIntervals=1, method=\"Rkfix4\", fixedstepsize=0.001, resultFile=\"Example6\");
+simulateModel(\"AixLib.Fluid.Examples.PerformanceExamples.Example7\", stopTime=100, numberOfIntervals=1, method=\"Rkfix4\", fixedstepsize=0.001, resultFile=\"Example7\");
+</pre>
+<p>
+Comparing the CPU times indicates a speed improvement of <i>56%</i>.
+This difference almost disappears when adding <code>annotation(Evaluate=true)</code>
+to <code>R</code> and <code>C</code>.
+</p>
+<p>
+In <code>dsmodel.c</code> we find:
+</p>
+<pre>
+DynamicsSection
+W_[2] = divmacro(X_[0]-X_[1],\"T[1]-T[2]\",DP_[0],\"R\");
+F_[0] = divmacro(W_[1]-W_[2],\"Q_flow[1]-Q_flow[2]\",DP_[1],\"C\");
+</pre>
+<p>
+This suggests that the parameter division needs to be handled during
+each function evaluation, probably causing the increased overhead.
+</p>
+<p>
+The following command allows comparing the CPU times objectively.
+</p>
+<p>
+<code>
+simulateModel(\"AixLib.Fluid.Examples.Performance.Example6\", stopTime=100, numberOfIntervals=1, method=\"Euler\", fixedstepsize=0.001, resultFile=\"Example6\");
+</code>
+</p>
+<p>
+See Jorissen et al. (2015) for a discussion.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Filip Jorissen, Michael Wetter and Lieve Helsen.<br/>
+Simulation speed analysis and improvements of Modelica
+models for building energy simulation.<br/>
+Submitted: 11th Modelica Conference. Paris, France. Sep. 2015.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example6.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example6;
diff --git a/AixLib/Fluid/Examples/Performance/Example7.mo b/AixLib/Fluid/Examples/Performance/Example7.mo
index 90dd478a50..1423c65fca 100644
--- a/AixLib/Fluid/Examples/Performance/Example7.mo
+++ b/AixLib/Fluid/Examples/Performance/Example7.mo
@@ -8,10 +8,15 @@ model Example7
   parameter Real tauInv = 1/(R*C);
 
   Real[nTem] T;
+
+protected
+  constant Real k(final unit="1/s") = 1
+    "Unit conversion to satisfy unit check";
+
 initial equation
   T = fill(273.15, nTem);
 equation
-  der(T[1])= ((273.15+sin(time))-2*T[1] + T[2])*tauInv;
+  der(T[1])= ((273.15+sin(k*time))-2*T[1] + T[2])*tauInv;
   for i in 2:nTem-1 loop
     der(T[i])=(T[i+1]+T[i-1]-2*T[i])*tauInv;
   end for;
@@ -25,29 +30,35 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=100),
     Documentation(revisions="<html>
- <ul>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.Examples.Performance.Example6\">
- AixLib.Fluid.Examples.Performance.Example6</a> for the documentation.
- </p>
- </html>"),
+<ul>
+<li>
+March 6, 2023, by Michael Wetter:<br/>
+Added a constant in order for unit check to pass.<br/>
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1711\">#1711</a>
+for a discussion.
+</li>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.Examples.Performance.Example6\">
+AixLib.Fluid.Examples.Performance.Example6</a> for the documentation.
+</p>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example7.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example7;
diff --git a/AixLib/Fluid/Examples/Performance/Example8.mo b/AixLib/Fluid/Examples/Performance/Example8.mo
index e8ab71e005..db0a69c1cb 100644
--- a/AixLib/Fluid/Examples/Performance/Example8.mo
+++ b/AixLib/Fluid/Examples/Performance/Example8.mo
@@ -1,8 +1,13 @@
 within AixLib.Fluid.Examples.Performance;
 model Example8 "Common subexpression elimination example"
   extends Modelica.Icons.Example;
-  Real a = sin(time+1);
-  Real b = sin(time+1);
+
+  Real a = sin(k*time+1);
+  Real b = sin(k*time+1);
+
+protected
+  constant Real k(final unit="1/s") = 1
+    "Unit conversion to satisfy unit check";
 
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,
             -40},{40,60}}),    graphics={Text(
@@ -12,30 +17,36 @@ model Example8 "Common subexpression elimination example"
     experiment(
       Tolerance=1e-6, StopTime=50),
     Documentation(revisions="<html>
- <ul>
- <li>
- July 14, 2015, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- June 18, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This is a very simple example demonstrating common subexpression elimination.
- The Dymola generated <code>C-code</code> of this model is:
- </p>
- <pre>
- W_[0] = sin(Time+1);
- W_[1] = W_[0];
- </pre>
- <p>
- Hence, the sine and addition are evaluated once only, which is more efficient.
- </p>
- </html>"),
+<ul>
+<li>
+March 6, 2023, by Michael Wetter:<br/>
+Added a constant in order for unit check to pass.<br/>
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1711\">#1711</a>
+for a discussion.
+</li>
+<li>
+July 14, 2015, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+June 18, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This is a very simple example demonstrating common subexpression elimination.
+The Dymola generated <code>C-code</code> of this model is:
+</p>
+<pre>
+W_[0] = sin(Time+1);
+W_[1] = W_[0];
+</pre>
+<p>
+Hence, the sine and addition are evaluated once only, which is more efficient.
+</p>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/Example8.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example8;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelDp.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelDp.mo
index 2a6ca0cf8a..2199159567 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelDp.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelDp.mo
@@ -47,22 +47,22 @@ equation
     annotation (Line(points={{-10,0},{-20,0},{-40,0}}, color={0,127,255}));
 
    annotation (    Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"),
     experiment(Tolerance=1e-6, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/ParallelDp.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ParallelDp;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelDpOptimised.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelDpOptimised.mo
index c1bc61b87e..5dbb40dd69 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelDpOptimised.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelDpOptimised.mo
@@ -3,21 +3,21 @@ model ParallelDpOptimised
   "Parallel connection with prescribed pressure difference and optimised parameters"
   extends ParallelDp(resParallel(each from_dp=true));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),experiment(Tolerance=1e-6, StopTime=1),
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"), experiment(Tolerance=1e-6, StopTime=1),
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/ParallelDpOptimised.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ParallelDpOptimised;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelFlow.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelFlow.mo
index 5c4bf86728..38fb393746 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelFlow.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelFlow.mo
@@ -46,22 +46,22 @@ equation
   connect(pulse_m_flow.y, sou.m_flow_in)
     annotation (Line(points={{-79,8},{-62,8}},           color={0,0,127}));
    annotation (    Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"),
     experiment(Tolerance=1e-6, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/ParallelFlow.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ParallelFlow;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelFlowOptimised.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelFlowOptimised.mo
index 2b51775d60..dad7c99d50 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelFlowOptimised.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/ParallelFlowOptimised.mo
@@ -4,20 +4,20 @@ model ParallelFlowOptimised
   extends ParallelFlow(
     resParallel(each from_dp=true));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/ParallelFlowOptimised.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"), experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/ParallelFlowOptimised.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ParallelFlowOptimised;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesDp.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesDp.mo
index d314afceb8..a91657a1f6 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesDp.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesDp.mo
@@ -45,22 +45,22 @@ equation
     annotation (Line(points={{-10,0},{-20,0},{-40,0}}, color={0,127,255}));
 
    annotation (    Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"),
     experiment(Tolerance=1e-6, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesDp.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SeriesDp;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesDpOptimised.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesDpOptimised.mo
index bcb15aed11..933094f5fe 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesDpOptimised.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesDpOptimised.mo
@@ -4,20 +4,20 @@ model SeriesDpOptimised
   extends SeriesDp(
     resSeries(each from_dp=false));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesDpOptimised.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"), experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesDpOptimised.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SeriesDpOptimised;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesFlow.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesFlow.mo
index 41649c28e4..e1175c200f 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesFlow.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesFlow.mo
@@ -44,22 +44,22 @@ equation
   connect(sou.m_flow_in, pulse_p.y) annotation (Line(points={{-62,8},{-62,8},{
           -79,8}},           color={0,0,127}));
    annotation (    Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"),
     experiment(Tolerance=1e-06, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesFlow.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SeriesFlow;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesFlowOptimised.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesFlowOptimised.mo
index 5cfdc7dde4..0d6b208c66 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesFlowOptimised.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesFlowOptimised.mo
@@ -3,20 +3,20 @@ model SeriesFlowOptimised
   "Series connection with prescribed flow and optimised parameters"
   extends SeriesFlow(resSeries(each from_dp=false));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesFlowOptimised.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"), experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesFlowOptimised.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SeriesFlowOptimised;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelDp.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelDp.mo
index 382902c4bf..7352c47974 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelDp.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelDp.mo
@@ -56,22 +56,22 @@ equation
   connect(pulse_m_flow.y, sou.p_in)
     annotation (Line(points={{-79,8},{-62,8}},           color={0,0,127}));
    annotation (    Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"),
     experiment(Tolerance=1e-6, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesParallelDp.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SeriesParallelDp;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelDpOptimised.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelDpOptimised.mo
index d66cfda66d..5584fd859d 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelDpOptimised.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelDpOptimised.mo
@@ -5,20 +5,20 @@ model SeriesParallelDpOptimised
     res2(from_dp=true),
     resParallel(each from_dp=true));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesParallelDpOptimised.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"), experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesParallelDpOptimised.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SeriesParallelDpOptimised;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlow.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlow.mo
index 97e8499206..387506769c 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlow.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlow.mo
@@ -54,22 +54,22 @@ equation
   connect(res2.port_b, sin.ports[1])
     annotation (Line(points={{50,0},{65,0},{80,0}}, color={0,127,255}));
    annotation (    Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"),
     experiment(Tolerance=1e-6, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlow.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SeriesParallelFlow;
diff --git a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlowOptimised.mo b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlowOptimised.mo
index ae351c0cc5..411819fa32 100644
--- a/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlowOptimised.mo
+++ b/AixLib/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlowOptimised.mo
@@ -5,20 +5,20 @@ model SeriesParallelFlowOptimised
     res2(from_dp=false),
     resParallel(each from_dp=true));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- May 26, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model that demonstrates how translation statistics
- depend on the type of boundary conditions,
- the parallel or series configuration of the components
- and the value of parameter <code>from_dp</code>.
- </p>
- </html>"),experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlowOptimised.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 26, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model that demonstrates how translation statistics
+depend on the type of boundary conditions,
+the parallel or series configuration of the components
+and the value of parameter <code>from_dp</code>.
+</p>
+</html>"), experiment(Tolerance=1e-6, StopTime=1), __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/Performance/PressureDrop/SeriesParallelFlowOptimised.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SeriesParallelFlowOptimised;
diff --git a/AixLib/Fluid/Examples/ResistanceVolumeFlowReversal.mo b/AixLib/Fluid/Examples/ResistanceVolumeFlowReversal.mo
index cc7319c8fd..dc4d96dbca 100644
--- a/AixLib/Fluid/Examples/ResistanceVolumeFlowReversal.mo
+++ b/AixLib/Fluid/Examples/ResistanceVolumeFlowReversal.mo
@@ -100,87 +100,87 @@ equation
        __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/ResistanceVolumeFlowReversal.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates the impact of the <code>allowFlowReversal</code> parameter on the size
- of nonlinear systems of equations. The user can change the parameter value in the <code>allowFlowReversal</code>
- block and rerun the simulation. The results are also demonstrated below for <code>nRes.k = 10</code>,
- which is the number of parallel branches containing one pressure drop element and one mixing volume each.
- </p>
- <p>
- This model was created to demonstrate the influence of a new implementation of
- <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.ConservationEquation</a>.
- The old implementation used the <code>actualStream()</code> function
- whereas the new implementation uses the <code>semiLinear()</code>
- function. This change allows Dymola to exploit knowledge about the <code>min</code> and <code>max</code> attributes
- of <code>m_flow</code>.
- When Dymola knows in which way the medium will flow, nonlinear systems can be simplified or completely removed.
- This is illustrated by the results below.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/216\">issue 216</a> for a discussion.
- </p>
- <p>
- Note that Dymola 2015FD01 can only reliable solve the last case. For the other
- two cases the Newton solver of the nonlinear system does not converge.
- </p>
- <p>
- These results were generated using Dymola 2015FD01 64 bit on Ubuntu 14.04
- and with <code>Evaluate=false</code>.
- </p>
- <h4>
- ResistanceVolumeFlowReversal = true
- </h4>
- <p>
- Sizes of nonlinear systems of equations: {6, 11, <b>56</b>}<br/>
- Sizes after manipulation of the nonlinear systems: {1, 9, <b>12</b>}
- </p>
- <h4>
- ResistanceVolumeFlowReversal = false
- </h4>
- <p>
- <b>Old implementation</b>
- </p>
- <p>
- Sizes of nonlinear systems of equations: {6, 11, <b>44</b>}<br/>
- Sizes after manipulation of the nonlinear systems: {1, 9, <b>11</b>}
- </p>
- <p>
- <b>New implementation</b>
- </p>
- <p>
- Sizes of nonlinear systems of equations: {6, 11, <b>4</b>}<br/>
- Sizes after manipulation of the nonlinear systems: {1, 9, <b>1</b>}
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2017, by Michael Wetter:<br/>
- Corrected parameterization to be independent of <code>k</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/825\">
- AixLib, #825</a>.
- </li>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- February 22, 2016, by Michael Wetter:<br/>
- Removed parameter <code>dynamicBalance</code> for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/411\">issue 411</a>.
- </li>
- <li>
- April 17, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model demonstrates the impact of the <code>allowFlowReversal</code> parameter on the size
+of nonlinear systems of equations. The user can change the parameter value in the <code>allowFlowReversal</code>
+block and rerun the simulation. The results are also demonstrated below for <code>nRes.k = 10</code>,
+which is the number of parallel branches containing one pressure drop element and one mixing volume each.
+</p>
+<p>
+This model was created to demonstrate the influence of a new implementation of
+<a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.ConservationEquation</a>.
+The old implementation used the <code>actualStream()</code> function
+whereas the new implementation uses the <code>semiLinear()</code>
+function. This change allows Dymola to exploit knowledge about the <code>min</code> and <code>max</code> attributes
+of <code>m_flow</code>.
+When Dymola knows in which way the medium will flow, nonlinear systems can be simplified or completely removed.
+This is illustrated by the results below.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/216\">issue 216</a> for a discussion.
+</p>
+<p>
+Note that Dymola 2015FD01 can only reliably solve the last case. For the other
+two cases the Newton solver of the nonlinear system does not converge.
+</p>
+<p>
+These results were generated using Dymola 2015FD01 64 bit on Ubuntu 14.04
+and with <code>Evaluate=false</code>.
+</p>
+<h4>
+ResistanceVolumeFlowReversal = true
+</h4>
+<p>
+Sizes of nonlinear systems of equations: {6, 11, <b>56</b>}<br/>
+Sizes after manipulation of the nonlinear systems: {1, 9, <b>12</b>}
+</p>
+<h4>
+ResistanceVolumeFlowReversal = false
+</h4>
+<p>
+<b>Old implementation</b>
+</p>
+<p>
+Sizes of nonlinear systems of equations: {6, 11, <b>44</b>}<br/>
+Sizes after manipulation of the nonlinear systems: {1, 9, <b>11</b>}
+</p>
+<p>
+<b>New implementation</b>
+</p>
+<p>
+Sizes of nonlinear systems of equations: {6, 11, <b>4</b>}<br/>
+Sizes after manipulation of the nonlinear systems: {1, 9, <b>1</b>}
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2017, by Michael Wetter:<br/>
+Corrected parameterization to be independent of <code>k</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/825\">
+AixLib, #825</a>.
+</li>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+February 22, 2016, by Michael Wetter:<br/>
+Removed parameter <code>dynamicBalance</code> for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/411\">issue 411</a>.
+</li>
+<li>
+April 17, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ResistanceVolumeFlowReversal;
diff --git a/AixLib/Fluid/Examples/SimpleHouse.mo b/AixLib/Fluid/Examples/SimpleHouse.mo
deleted file mode 100644
index dc4dfa01a0..0000000000
--- a/AixLib/Fluid/Examples/SimpleHouse.mo
+++ /dev/null
@@ -1,345 +0,0 @@
-within AixLib.Fluid.Examples;
-model SimpleHouse
-  "Illustrative example of a simple heating, ventilation and room model"
-  extends Modelica.Icons.Example;
-
-  package MediumAir = AixLib.Media.Air;
-  package MediumWater = AixLib.Media.Water;
-
-  parameter Modelica.Units.SI.Area A_wall=100 "Wall area";
-  parameter Modelica.Units.SI.Area A_win=5 "Window area";
-  parameter Real g_win(min=0, max=1, unit="1") = 0.3 "Solar heat gain coefficient of window";
-  parameter Modelica.Units.SI.Volume V_zone=A_wall*3 "Wall area";
-  parameter Modelica.Units.SI.HeatFlowRate QHea_nominal=700
-    "Nominal capacity of heating system";
-  parameter Modelica.Units.SI.MassFlowRate mWat_flow_nominal=QHea_nominal/10/
-      4200 "Nominal mass flow rate for water loop";
-  parameter Modelica.Units.SI.MassFlowRate mAir_flow_nominal=V_zone*2*1.2/3600
-    "Nominal mass flow rate for air loop";
-
-  parameter Modelica.Units.SI.PressureDifference dpAir_nominal=200
-    "Pressure drop at nominal mass flow rate for air loop";
-  parameter Boolean allowFlowReversal=false
-    "= false because flow will not reverse in these circuits";
-
-  Modelica.Thermal.HeatTransfer.Components.HeatCapacitor walCap(
-    T(fixed=true),
-    C=10*A_wall*0.05*1000*1000)
-    "Thermal mass of walls"
-    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
-        rotation=270,
-        origin={142,-8})));
-  MixingVolumes.MixingVolume zone(
-    redeclare package Medium = MediumAir,
-    V=V_zone,
-    nPorts=2,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
-    m_flow_nominal=mAir_flow_nominal,
-    massDynamics=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial)
-    "Very based zone air model"
-    annotation (Placement(transformation(extent={{102,140},{82,160}})));
-  Modelica.Thermal.HeatTransfer.Components.ThermalResistor convRes(R=1/2/A_wall)
-    "Thermal resistance for convective heat transfer with h=2"
-    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
-        rotation=270,
-        origin={132,22})));
-  HeatExchangers.Radiators.RadiatorEN442_2 rad(
-    redeclare package Medium = MediumWater,
-    T_a_nominal=273.15 + 50,
-    T_b_nominal=273.15 + 40,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
-    allowFlowReversal=allowFlowReversal,
-    Q_flow_nominal=QHea_nominal)                  "Radiator"
-    annotation (Placement(transformation(extent={{104,-116},{124,-96}})));
-
-  Sources.Boundary_pT bouAir(redeclare package Medium = MediumAir, nPorts=2,
-    use_T_in=true) "Air boundary with constant temperature"
-    annotation (Placement(transformation(
-        extent={{-10,-10},{10,10}},
-        origin={-112,140})));
-  Sources.Boundary_pT bouWat(redeclare package Medium = MediumWater, nPorts=1)
-    "Pressure bound for water circuit" annotation (Placement(transformation(
-        extent={{-10,-10},{10,10}},
-        origin={-8,-170})));
-  BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
-    filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos"))
-    "Weather data reader"
-    annotation (Placement(transformation(extent={{-200,-18},{-180,2}})));
-  BoundaryConditions.WeatherData.Bus weaBus "Weather data bus"
-    annotation (Placement(transformation(extent={{-162,-18},{-142,2}})));
-  Modelica.Thermal.HeatTransfer.Components.ThermalResistor wallRes(R=0.25/
-        A_wall/0.04) "Thermal resistor for wall: 25 cm of rockwool"
-    annotation (Placement(transformation(extent={{66,-10},{86,10}})));
-  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature Tout
-    "Exterior temperature boundary condition"
-    annotation (Placement(transformation(extent={{-20,-10},{0,10}})));
-  HeatExchangers.HeaterCooler_u heaWat(
-    redeclare package Medium = MediumWater,
-    m_flow_nominal=mWat_flow_nominal,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
-    allowFlowReversal=allowFlowReversal,
-    dp_nominal=5000,
-    Q_flow_nominal=QHea_nominal) "Heater for water circuit"
-    annotation (Placement(transformation(extent={{44,-116},{64,-96}})));
-
-  Movers.FlowControlled_m_flow pump(
-    redeclare package Medium = MediumWater,
-    use_inputFilter=false,
-    m_flow_nominal=mWat_flow_nominal,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
-    allowFlowReversal=allowFlowReversal,
-    nominalValuesDefineDefaultPressureCurve=true,
-    inputType=AixLib.Fluid.Types.InputType.Stages,
-    massFlowRates=mWat_flow_nominal*{1}) "Pump"
-    annotation (Placement(transformation(extent={{80,-180},{60,-160}})));
-  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor senTemZonAir
-    "Zone air temperature sensor"
-    annotation (Placement(transformation(extent={{80,170},{60,190}})));
-  Actuators.Dampers.Exponential vavDam(
-    redeclare package Medium = MediumAir,
-    from_dp=true,
-    m_flow_nominal=mAir_flow_nominal,
-    dpDamper_nominal=10,
-    dpFixed_nominal=dpAir_nominal - 10)
-    "Damper" annotation (Placement(transformation(extent={{-10,10},{10,
-            -10}}, origin={72,120})));
-
-  Movers.FlowControlled_dp fan(
-    redeclare package Medium = MediumAir,
-    dp_nominal=dpAir_nominal,
-    use_inputFilter=false,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
-    nominalValuesDefineDefaultPressureCurve=true,
-    m_flow_nominal=mAir_flow_nominal,
-    show_T=true) "Constant head fan" annotation (Placement(transformation(
-        extent={{-10,-10},{10,10}},
-        origin={-22,120})));
-  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow window
-    "Very simple window model"
-    annotation (Placement(transformation(extent={{-20,-36},{0,-16}})));
-  HeatExchangers.ConstantEffectiveness hexRec(
-    redeclare package Medium1 = MediumAir,
-    redeclare package Medium2 = MediumAir,
-    dp1_nominal=0,
-    dp2_nominal=0,
-    m1_flow_nominal=mAir_flow_nominal,
-    m2_flow_nominal=mAir_flow_nominal,
-    eps=0.85)      "Heat exchanger for heat recuperation"
-    annotation (Placement(transformation(extent={{-54,114},{-84,146}})));
-  Modelica.Blocks.Logical.Hysteresis hysRad(uLow=273.15 + 20, uHigh=273.15 + 22)
-    "Hysteresis controller for radiator"
-    annotation (Placement(transformation(extent={{-74,-110},{-54,-90}})));
-  Modelica.Blocks.Math.BooleanToReal booleanToReal1 "Boolean to real"
-    annotation (Placement(transformation(extent={{-16,-110},{4,-90}})));
-  Modelica.Blocks.Logical.Not not1
-    "negation for enabling heating when temperatur is low"
-    annotation (Placement(transformation(extent={{-46,-110},{-26,-90}})));
-  Modelica.Blocks.Sources.Constant const_dp(k=dpAir_nominal) "Pressure head"
-    annotation (Placement(transformation(extent={{-52,150},{-32,170}})));
-
-  Modelica.Blocks.Math.Gain gaiWin(k=A_win*g_win)
-    "Gain for window solar transmittance and area as HGloHor is in W/m2"
-    annotation (Placement(transformation(extent={{-60,-36},{-40,-16}})));
-  Modelica.Blocks.Math.BooleanToInteger booleanToInt "Boolean to integer"
-    annotation (Placement(transformation(extent={{-16,-144},{4,-124}})));
-  Controls.Continuous.LimPID conDam(
-      controllerType=Modelica.Blocks.Types.SimpleController.P,
-      yMin=0.1) "Controller for damper"
-    annotation (Placement(transformation(extent={{-20,80},{0,100}})));
-  Modelica.Blocks.Sources.Constant TSetRoo(k=273.15 + 24)
-    "Room temperature set point for air system"
-    annotation (Placement(transformation(extent={{-60,60},{-40,80}})));
-  HeatExchangers.SensibleCooler_T cooAir(
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
-    allowFlowReversal=allowFlowReversal,
-    m_flow_nominal=mAir_flow_nominal,
-    dp_nominal=0,
-    redeclare package Medium = MediumAir) "Cooling for supply air"
-    annotation (Placement(transformation(extent={{30,110},{50,130}})));
-  Modelica.Blocks.Sources.Constant TSupAirCoo(k=273.15 + 20)
-    "Cooling setpoint for supply air"
-    annotation (Placement(transformation(extent={{-12,150},{8,170}})));
-equation
-  connect(convRes.port_b, walCap.port)
-    annotation (Line(points={{132,12},{132,12},{132,-8}},    color={191,0,0}));
-  connect(convRes.port_a, zone.heatPort) annotation (Line(points={{132,32},{132,
-          150},{102,150}},           color={191,0,0}));
-  connect(weaDat.weaBus, weaBus) annotation (Line(
-      points={{-180,-8},{-180,-8},{-152,-8}},
-      color={255,204,51},
-      thickness=0.5));
-  connect(wallRes.port_b, walCap.port) annotation (Line(points={{86,0},{132,0},{
-          132,-6},{132,-8}},    color={191,0,0}));
-  connect(Tout.T, weaBus.TDryBul)
-    annotation (Line(points={{-22,0},{-152,0},{-152,-8}}, color={0,0,127}));
-  connect(Tout.port, wallRes.port_a)
-    annotation (Line(points={{0,0},{0,0},{66,0}},    color={191,0,0}));
-  connect(heaWat.port_b, rad.port_a) annotation (Line(points={{64,-106},{84,-106},
-          {104,-106}}, color={0,127,255}));
-  connect(bouWat.ports[1], heaWat.port_a) annotation (Line(points={{2,-170},{40,
-          -170},{40,-106},{44,-106}}, color={0,127,255}));
-  connect(rad.port_b, pump.port_a) annotation (Line(points={{124,-106},{130,-106},
-          {130,-170},{80,-170}}, color={0,127,255}));
-  connect(senTemZonAir.port, zone.heatPort) annotation (Line(points={{80,180},{80,
-          180},{112,180},{112,150},{102,150}},
-                                     color={191,0,0}));
-  connect(window.port, walCap.port) annotation (Line(points={{0,-26},{132,-26},{
-          132,-12},{132,-8}},
-                         color={191,0,0}));
-  connect(bouAir.ports[1], hexRec.port_b1) annotation (Line(points={{-102,142},{
-          -102,139.6},{-84,139.6}},
-                              color={0,127,255}));
-  connect(hexRec.port_a1, zone.ports[1]) annotation (Line(points={{-54,139.6},{85,
-          139.6},{85,140},{94,140}},      color={0,127,255}));
-  connect(rad.heatPortCon, zone.heatPort) annotation (Line(points={{112,-98.8},{
-          112,-98.8},{112,48},{112,150},{102,150}},   color={191,0,0}));
-  connect(rad.heatPortRad, walCap.port) annotation (Line(points={{116,-98.8},{116,
-          -98.8},{116,-70},{116,-26},{132,-26},{132,-8}},
-                                                   color={191,0,0}));
-  connect(not1.y, booleanToReal1.u) annotation (Line(points={{-25,-100},{-22,-100},
-          {-18,-100}}, color={255,0,255}));
-  connect(not1.u, hysRad.y) annotation (Line(points={{-48,-100},{-52,-100},{-53,
-          -100}}, color={255,0,255}));
-  connect(booleanToReal1.y, heaWat.u) annotation (Line(points={{5,-100},{16,-100},
-          {26,-100},{42,-100}}, color={0,0,127}));
-  connect(heaWat.port_a, pump.port_b) annotation (Line(points={{44,-106},{40,-106},
-          {40,-112},{40,-170},{60,-170}}, color={0,127,255}));
-  connect(const_dp.y, fan.dp_in) annotation (Line(points={{-31,160},{-22,160},{
-          -22,132},{-22,132}},                       color={0,0,127}));
-  connect(gaiWin.y, window.Q_flow) annotation (Line(points={{-39,-26},{-34,-26},
-          {-30,-26},{-20,-26}}, color={0,0,127}));
-  connect(gaiWin.u, weaBus.HGloHor) annotation (Line(points={{-62,-26},{-90,-26},
-          {-152,-26},{-152,-8}}, color={0,0,127}));
-  connect(booleanToInt.u, not1.y) annotation (Line(points={{-18,-134},{-22,-134},
-          {-22,-100},{-25,-100}}, color={255,0,255}));
-  connect(booleanToInt.y, pump.stage) annotation (Line(points={{5,-134},{32,-134},
-          {70,-134},{70,-158}}, color={255,127,0}));
-  connect(bouAir.ports[2], hexRec.port_a2) annotation (Line(points={{-102,138},{
-          -102,142},{-90,142},{-90,120.4},{-84,120.4}}, color={0,127,255}));
-  connect(hexRec.port_b2, fan.port_a) annotation (Line(points={{-54,120.4},{-44,
-          120.4},{-44,120},{-32,120}}, color={0,127,255}));
-  connect(vavDam.port_b, zone.ports[2])
-    annotation (Line(points={{82,120},{90,120},{90,140}}, color={0,127,255}));
-  connect(senTemZonAir.T, hysRad.u) annotation (Line(points={{60,180},{60,180},{
-          -132,180},{-132,-100},{-76,-100}},  color={0,0,127}));
-  connect(senTemZonAir.T,conDam. u_s) annotation (Line(points={{60,180},{60,180},
-          {-132,180},{-132,90},{-62,90},{-22,90}},
-                                          color={0,0,127}));
-  connect(conDam.y, vavDam.y) annotation (Line(points={{1,90},{26,90},{72,90},{72,
-          108}},color={0,0,127}));
-  connect(TSetRoo.y,conDam. u_m) annotation (Line(points={{-39,70},{-40,70},{-36,
-          70},{-40,70},{-10,70},{-10,78}},
-                         color={0,0,127}));
-  connect(fan.port_b, cooAir.port_a)
-    annotation (Line(points={{-12,120},{30,120}}, color={0,127,255}));
-  connect(cooAir.port_b, vavDam.port_a)
-    annotation (Line(points={{50,120},{50,120},{62,120}}, color={0,127,255}));
-  connect(TSupAirCoo.y, cooAir.TSet) annotation (Line(points={{9,160},{20,160},{
-          20,128},{28,128}}, color={0,0,127}));
-  connect(bouAir.T_in, weaBus.TDryBul) annotation (Line(points={{-124,144},{
-          -152,144},{-152,-8}}, color={0,0,127}));
-  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-240,
-            -220},{200,220}}), graphics={
-        Rectangle(
-          extent={{-222,200},{180,50}},
-          fillColor={238,238,238},
-          fillPattern=FillPattern.Solid,
-          pattern=LinePattern.None),
-        Rectangle(
-          extent={{-220,-60},{180,-200}},
-          fillColor={238,238,238},
-          fillPattern=FillPattern.Solid,
-          pattern=LinePattern.None),
-        Rectangle(
-          extent={{-220,40},{20,-48}},
-          fillColor={238,238,238},
-          fillPattern=FillPattern.Solid,
-          pattern=LinePattern.None),
-        Text(
-          extent={{-78,182},{-212,198}},
-          textColor={0,0,127},
-          fillColor={255,213,170},
-          fillPattern=FillPattern.Solid,
-          textString="Cooling and ventilation"),
-        Rectangle(
-          extent={{40,40},{180,-46}},
-          fillColor={238,238,238},
-          fillPattern=FillPattern.Solid,
-          pattern=LinePattern.None),
-        Text(
-          extent={{98,20},{32,38}},
-          textColor={0,0,127},
-          fillColor={255,213,170},
-          fillPattern=FillPattern.Solid,
-          textString="Wall"),
-        Text(
-          extent={{-148,-86},{-214,-68}},
-          textColor={0,0,127},
-          fillColor={255,213,170},
-          fillPattern=FillPattern.Solid,
-          textString="Heating"),
-        Text(
-          extent={{-154,20},{-212,38}},
-          textColor={0,0,127},
-          fillColor={255,213,170},
-          fillPattern=FillPattern.Solid,
-          textString="Weather")}),
-    experiment(Tolerance=1e-06, StopTime=3.1536e+07),
-    Documentation(revisions="<html>
- <ul>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- November 10, 2016, by Michael Wetter:<br/>
- Connected supply air temperature to outdoor air temperature,
- added cooling to supply air,
- changed capacity of heating system, switched heating pump off when heater is off,
- and added proportional controller for the air damper.<br/>
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/584\">#584</a>.
- </li>
- <li>
- September 9, 2016, by Michael Wetter:<br/>
- Corrected error in window model, as the solar heat gain was
- not multiplied with the window area. Dymola 2017 reported this
- error due to mismatching units of <code>W/m2</code> and <code>W</code>.
- </li>
- <li>
- June 23, 2016, by Michael Wetter:<br/>
- Changed graphical annotation.
- </li>
- <li>
- March 11, 2016, by Michael Wetter:<br/>
- Corrected wrong limits for <code>hysAir</code> so that
- <code>uLow &lt; uHigh</code>.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/429\">#429</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- September 19, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model contains a simple model of a house
- with a heating system, ventilation and weather boundary conditions.
- It servers as a demonstration case of how the <code>AixLib</code> library can be used.
- </p>
- </html>"),
-    __Dymola_Commands(file=
-          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Examples/SimpleHouse.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
-end SimpleHouse;
diff --git a/AixLib/Fluid/Examples/package.order b/AixLib/Fluid/Examples/package.order
index 31d406bbbf..f77cd1ae1f 100644
--- a/AixLib/Fluid/Examples/package.order
+++ b/AixLib/Fluid/Examples/package.order
@@ -1,5 +1,4 @@
 ResistanceVolumeFlowReversal
-SimpleHouse
 FlowSystem
 GeothermalHeatPump
 Performance
diff --git a/AixLib/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACNoExhaust.mo b/AixLib/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACNoExhaust.mo
index a2aab06a14..122dfd7e3d 100644
--- a/AixLib/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACNoExhaust.mo
+++ b/AixLib/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACNoExhaust.mo
@@ -148,66 +148,66 @@ equation
         Text(
           extent={{-190,124},{-152,100}},
           pattern=LinePattern.None,
-          lineColor={0,0,127},
+          textColor={0,0,127},
           horizontalAlignment=TextAlignment.Left,
           textString="Simplified model of
- an HVAC system
- in Modelica that could
- be exposed as an FMU"),
+an HVAC system
+in Modelica that could
+be exposed as an FMU"),
         Text(
           extent={{90,118},{128,94}},
           pattern=LinePattern.None,
-          lineColor={0,0,127},
+          textColor={0,0,127},
           horizontalAlignment=TextAlignment.Left,
           textString="Simplified model of
- a thermal zone that
- may be in an FMU
- (but is here for simplicity
- also implemented in Modelica)")}),
+a thermal zone that
+may be in an FMU
+(but is here for simplicity
+also implemented in Modelica)")}),
     Documentation(info="<html>
- <p>
- This example demonstrates how to
- use the adaptors
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.HVAC\">
- AixLib.Fluid.FMI.Adaptors.HVAC</a>
- and
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.ThermalZone\">
- AixLib.Fluid.FMI.Adaptors.ThermalZone</a>
- </p>
- <p>
- On the left hand side is an HVAC system with supply and return air stream.
- These are all connected to the adaptor.
- On the right of the adaptor is a simple room model, approximated by a volume with
- first order dynamics and heat loss to the ambient.
- </p>
- <p>
- Note that the there is zero net air flow into and out of the volume <code>vol</code>
- because the adaptor <code>hvacAda</code> conserves mass. Hence, any infiltration or
- exfiltration needs to be
- connected to the adaptor <code>hvacAda</code>, rather than the volume <code>vol</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 11, 2020, by Michael Wetter:<br/>
- Removed <code>fontSize</code> in annotation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1318\">#1318</a>.
- </li>
- <li>
- November 29, 2016, by Michael Wetter:<br/>
- Added separate signal for outdoor temperature used by HVAC system. This is
- to improve clarity regarding what signals are exchanged, see also
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/598\">#598</a>.
- </li>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to
+use the adaptors
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.HVAC\">
+AixLib.Fluid.FMI.Adaptors.HVAC</a>
+and
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.ThermalZone\">
+AixLib.Fluid.FMI.Adaptors.ThermalZone</a>
+</p>
+<p>
+On the left hand side is an HVAC system with supply and return air stream.
+These are all connected to the adaptor.
+On the right of the adaptor is a simple room model, approximated by a volume with
+first order dynamics and heat loss to the ambient.
+</p>
+<p>
+Note that the there is zero net air flow into and out of the volume <code>vol</code>
+because the adaptor <code>hvacAda</code> conserves mass. Hence, any infiltration or
+exfiltration needs to be
+connected to the adaptor <code>hvacAda</code>, rather than the volume <code>vol</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 11, 2020, by Michael Wetter:<br/>
+Removed <code>fontSize</code> in annotation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1318\">#1318</a>.
+</li>
+<li>
+November 29, 2016, by Michael Wetter:<br/>
+Added separate signal for outdoor temperature used by HVAC system. This is
+to improve clarity regarding what signals are exchanged, see also
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/598\">#598</a>.
+</li>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACNoExhaust.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=172800),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=172800), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZoneHVACNoExhaust;
diff --git a/AixLib/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACWithExhaust.mo b/AixLib/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACWithExhaust.mo
index 3a35958b8c..920147dc29 100644
--- a/AixLib/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACWithExhaust.mo
+++ b/AixLib/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACWithExhaust.mo
@@ -28,31 +28,31 @@ equation
 
  annotation (
     Documentation(info="<html>
- <p>
- This example demonstrates how to
- use the adaptors
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.HVAC\">
- AixLib.Fluid.FMI.Adaptors.HVAC</a>
- and
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.ThermalZone\">
- AixLib.Fluid.FMI.Adaptors.ThermalZone</a>
- </p>
- <p>
- It is identical to
- <a href=\"AixLib.Fluid.FMI.Adaptors.Examples.ThermalZoneHVACNoExhaust\">
- AixLib.Fluid.FMI.Adaptors.Examples.ThermalZoneHVACNoExhaust</a>
- except that it adds a forced exhaust air stream.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to
+use the adaptors
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.HVAC\">
+AixLib.Fluid.FMI.Adaptors.HVAC</a>
+and
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.ThermalZone\">
+AixLib.Fluid.FMI.Adaptors.ThermalZone</a>
+</p>
+<p>
+It is identical to
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Examples.ThermalZoneHVACNoExhaust\">
+AixLib.Fluid.FMI.Adaptors.Examples.ThermalZoneHVACNoExhaust</a>
+except that it adds a forced exhaust air stream.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Adaptors/Examples/ThermalZoneHVACWithExhaust.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=172800),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=172800), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZoneHVACWithExhaust;
diff --git a/AixLib/Fluid/FMI/Adaptors/HVAC.mo b/AixLib/Fluid/FMI/Adaptors/HVAC.mo
index a44c68aff9..7422d8b8e9 100644
--- a/AixLib/Fluid/FMI/Adaptors/HVAC.mo
+++ b/AixLib/Fluid/FMI/Adaptors/HVAC.mo
@@ -134,12 +134,12 @@ protected
           extent={{-150,90},{140,50}},
           textString="%name",
           textColor={0,0,255})}), Documentation(info="<html>
- <p>
- The (time varying) vector <code>Real</code> output signal of this block can be defined in its
- parameter menu via variable <code>y</code>. The purpose is to support the
- easy definition of vector-valued Real expressions in a block diagram.
- </p>
- </html>"));
+<p>
+The (time varying) vector <code>Real</code> output signal of this block can be defined in its
+parameter menu via variable <code>y</code>. The purpose is to support the
+easy definition of vector-valued Real expressions in a block diagram.
+</p>
+</html>"));
 
   end RealVectorExpression;
 
@@ -249,109 +249,109 @@ equation
             Bitmap(extent={{-96,52},{-24,108}},fileName=
             "modelica://AixLib/Resources/Images/Fluid/FMI/modelica_icon.png")}),
     Documentation(info="<html>
- <p>
- Adaptor that can be used to connect an HVAC system (with acausal ports)
- to input/output signals, which then can be exposed in an FMI interface.
- </p>
- <p>
- The adaptor has a vector of fluid ports called <code>ports</code>.
- The supply and return air ducts need to be connected to these ports.
- Also, if a thermal zone has interzonal air exchange or air infiltration,
- these flow paths also need be connected to <code>ports</code>.
- </p>
- <p>
- This model outputs at the port <code>fluPor</code> the mass flow rate for
- each flow that is connected to <code>ports</code>, together with its
- temperature, water vapor mass fraction per total mass of the air (not per kg dry
- air), and trace substances. These quantities are always as if the flow
- enters the room, even if the flow is zero or negative.
- If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
- if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
- the output signal for these properties are removed.
- These quantities are always as if the flow
- enters the room, even if the flow is zero or negative.
- Thus, a thermal zone model that uses these signals to compute the
- heat added by the HVAC system need to implement an equation such as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
- </p>
- <p>
- where
- <i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
- <i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
- the port <code>fluPor</code> (which is negative if it is an exhaust),
- <i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
- <i>T<sub>sup</sub></i> is the supply air temperature and
- <i>T<sub>air,zon</sub></i> is the zone air temperature.
- Note that without the <i>max(&middot;, &middot;)</i> function, the energy
- balance would be wrong.
- </p>
- <p>
- The output signals of this model are the zone air temperature,
- the water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>)
- and trace substances (unless <code>Medium.nC=0</code>).
- These output connectors can be used to connect to a controller.
- These values are obtained from the fluid stream(s) that flow into this component
- at the port <code>fluPor</code>, e.g., from the connector
- <code>fluPor.backward</code>.
- Note that there are <code>nPorts</code> of these signals.
- For a completely mixed room, they will all have the same value, but
- for a room with non-uniform temperatures, they can have different values.
- </p>
- <h4>Assumption and limitations</h4>
- <p>
- The mass flow rates at <code>ports</code> sum to zero, hence this
- model conserves mass.
- </p>
- <p>
- This model does not impose any pressure, other than setting the pressure
- of all fluid connections to <code>ports</code> to be equal.
- The reason is that setting a pressure can lead to non-physical system models,
- for example if a mass flow rate is imposed and the HVAC system is connected
- to a model that sets a pressure boundary condition such as
- <a href=\"modelica://AixLib.Fluid.Sources.Outside\">
- AixLib.Fluid.Sources.Outside</a>.
- Also, setting a pressure would make it impossible to use multiple instances
- of this model (one for each thermal zone) and build in Modelica an airflow network
- model with pressure driven mass flow rates.
- </p>
- <p>
- The model has no pressure drop. Hence, the pressure drop
- of an air diffuser or of an exhaust grill need to be modelled
- in models that are connected to <code>ports</code>.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
- for a model that uses this model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- September 13, 2017, by Michael Wetter:<br/>
- Removed erroneous <code>each</code>.
- </li>
- <li>
- October 4, 2016, by Michael Wetter:<br/>
- Corrected assignment of <code>quantity</code> in <code>CZon</code>.
- </li>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- April 14, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Adaptor that can be used to connect an HVAC system (with acausal ports)
+to input/output signals, which then can be exposed in an FMI interface.
+</p>
+<p>
+The adaptor has a vector of fluid ports called <code>ports</code>.
+The supply and return air ducts need to be connected to these ports.
+Also, if a thermal zone has interzonal air exchange or air infiltration,
+these flow paths also need be connected to <code>ports</code>.
+</p>
+<p>
+This model outputs at the port <code>fluPor</code> the mass flow rate for
+each flow that is connected to <code>ports</code>, together with its
+temperature, water vapor mass fraction per total mass of the air (not per kg dry
+air), and trace substances. These quantities are always as if the flow
+enters the room, even if the flow is zero or negative.
+If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
+if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
+the output signal for these properties are removed.
+These quantities are always as if the flow
+enters the room, even if the flow is zero or negative.
+Thus, a thermal zone model that uses these signals to compute the
+heat added by the HVAC system need to implement an equation such as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
+</p>
+<p>
+where
+<i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
+<i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
+the port <code>fluPor</code> (which is negative if it is an exhaust),
+<i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
+<i>T<sub>sup</sub></i> is the supply air temperature and
+<i>T<sub>air,zon</sub></i> is the zone air temperature.
+Note that without the <i>max(&middot;, &middot;)</i> function, the energy
+balance would be wrong.
+</p>
+<p>
+The output signals of this model are the zone air temperature,
+the water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>)
+and trace substances (unless <code>Medium.nC=0</code>).
+These output connectors can be used to connect to a controller.
+These values are obtained from the fluid stream(s) that flow into this component
+at the port <code>fluPor</code>, e.g., from the connector
+<code>fluPor.backward</code>.
+Note that there are <code>nPorts</code> of these signals.
+For a completely mixed room, they will all have the same value, but
+for a room with non-uniform temperatures, they can have different values.
+</p>
+<h4>Assumption and limitations</h4>
+<p>
+The mass flow rates at <code>ports</code> sum to zero, hence this
+model conserves mass.
+</p>
+<p>
+This model does not impose any pressure, other than setting the pressure
+of all fluid connections to <code>ports</code> to be equal.
+The reason is that setting a pressure can lead to non-physical system models,
+for example if a mass flow rate is imposed and the HVAC system is connected
+to a model that sets a pressure boundary condition such as
+<a href=\"modelica://AixLib.Fluid.Sources.Outside\">
+AixLib.Fluid.Sources.Outside</a>.
+Also, setting a pressure would make it impossible to use multiple instances
+of this model (one for each thermal zone) and build in Modelica an airflow network
+model with pressure driven mass flow rates.
+</p>
+<p>
+The model has no pressure drop. Hence, the pressure drop
+of an air diffuser or of an exhaust grill need to be modelled
+in models that are connected to <code>ports</code>.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
+for a model that uses this model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+September 13, 2017, by Michael Wetter:<br/>
+Removed erroneous <code>each</code>.
+</li>
+<li>
+October 4, 2016, by Michael Wetter:<br/>
+Corrected assignment of <code>quantity</code> in <code>CZon</code>.
+</li>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+April 14, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVAC;
diff --git a/AixLib/Fluid/FMI/Adaptors/Inlet.mo b/AixLib/Fluid/FMI/Adaptors/Inlet.mo
index 39469b8c88..1151ca8d22 100644
--- a/AixLib/Fluid/FMI/Adaptors/Inlet.mo
+++ b/AixLib/Fluid/FMI/Adaptors/Inlet.mo
@@ -35,14 +35,14 @@ model Inlet "Adaptor for connecting a fluid inlet to the FMI interface"
         rotation=270,
         origin={0,-110})));
 protected
-  AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
+  input AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
     redeclare final package Medium = Medium)
     "Internal connector for fluid properties for back flow";
   AixLib.Fluid.FMI.Interfaces.PressureOutput p_in_internal
     "Internal connector for pressure";
-  AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_in_internal
+  output AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_in_internal
     "Internal connector for mass fraction of forward flow properties";
-  AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_out_internal
+  output AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_out_internal
     "Internal connector for mass fraction of backward flow properties";
 initial equation
    assert(Medium.nXi < 2,
@@ -150,54 +150,59 @@ equation
           visible=use_p_in,
           textString="p")}),
     Documentation(info="<html>
- <p>
- Model that is used to connect an input signal to a fluid port.
- The model needs to be used in conjunction with an instance of
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Outlet\">
- AixLib.Fluid.FMI.Adaptors.Outlet</a> in order for
- fluid mass flow rate and pressure to be properly assigned to
- the acausal fluid models.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.PartialTwoPort\">
- AixLib.Fluid.FMI.ExportContainers.PartialTwoPort</a>
- or
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume</a>
- for how to use this model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air and water.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- November 8, 2016, by Michael Wetter:<br/>
- Corrected wrong argument type in function call of <code>Medium.temperature_phX</code> and
- <code>Medium.specificEnthalpy_pTX</code>.
- </li>
- <li>
- October 23, 2016, by Michael Wetter:<br/>
- Changed type of pressure output connector.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Redesigned to conditionally remove the pressure connector
- if <code>use_p_in=false</code>.
- </li>
- <li>
- April 15, 2015 by Michael Wetter:<br/>
- Changed connector variable to be temperature instead of
- specific enthalpy.
- </li>
- <li>
- January 21, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that is used to connect an input signal to a fluid port.
+The model needs to be used in conjunction with an instance of
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Outlet\">
+AixLib.Fluid.FMI.Adaptors.Outlet</a> in order for
+fluid mass flow rate and pressure to be properly assigned to
+the acausal fluid models.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.PartialTwoPort\">
+AixLib.Fluid.FMI.ExportContainers.PartialTwoPort</a>
+or
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume</a>
+for how to use this model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 18, 2024, by Michael Wetter:<br/>
+Added causality.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1853\">IBPSA, #1853</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air and water.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Corrected wrong argument type in function call of <code>Medium.temperature_phX</code> and
+<code>Medium.specificEnthalpy_pTX</code>.
+</li>
+<li>
+October 23, 2016, by Michael Wetter:<br/>
+Changed type of pressure output connector.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Redesigned to conditionally remove the pressure connector
+if <code>use_p_in=false</code>.
+</li>
+<li>
+April 15, 2015 by Michael Wetter:<br/>
+Changed connector variable to be temperature instead of
+specific enthalpy.
+</li>
+<li>
+January 21, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Inlet;
diff --git a/AixLib/Fluid/FMI/Adaptors/Outlet.mo b/AixLib/Fluid/FMI/Adaptors/Outlet.mo
index fe1524d535..a90a4ebb42 100644
--- a/AixLib/Fluid/FMI/Adaptors/Outlet.mo
+++ b/AixLib/Fluid/FMI/Adaptors/Outlet.mo
@@ -36,15 +36,15 @@ model Outlet "Adaptor for connecting a fluid outlet to the FMI interface"
         rotation=90,
         origin={0,-120})));
 protected
-  AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
+  output AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
     redeclare final package Medium = Medium)
     "Internal connector for fluid properties for back flow";
   AixLib.Fluid.FMI.Interfaces.PressureOutput p_in_internal
     "Internal connector for pressure";
 
-  AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_in_internal
+  input AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_in_internal
     "Internal connector for mass fraction of forward flow properties";
-  AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_out_internal
+  output AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_out_internal
     "Internal connector for mass fraction of backward flow properties";
 initial equation
    assert(Medium.nXi < 2,
@@ -85,7 +85,7 @@ equation
   bacPro_internal.T  = Medium.temperature_phX(
     p = p_in_internal,
     h = port_a.h_outflow,
-    X = port_a.Xi_outflow);
+    X = cat(1, port_a.Xi_outflow, {1-sum(port_a.Xi_outflow)}));
   bacPro_internal.C  = port_a.C_outflow;
 
   // Conditional connectors for pressure
@@ -133,49 +133,59 @@ equation
           textString="p",
           visible=use_p_in)}),
     Documentation(info="<html>
- <p>
- Model that is used to connect a fluid port with an output signal.
- The model needs to be used in conjunction with an instance of
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Inlet\">
- AixLib.Fluid.FMI.Adaptors.Inlet</a> in order for
- fluid mass flow rate and pressure to be properly assigned to
- the acausal fluid models.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.PartialTwoPort\">
- AixLib.Fluid.FMI.ExportContainers.PartialTwoPort</a>
- or
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume</a>
- for how to use this model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air and water.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- November 8, 2016, by Michael Wetter:<br/>
- Corrected wrong argument type in function call of <code>Medium.temperature_phX</code>.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Redesigned to conditionally remove the pressure connector
- if <code>use_p_in=false</code>.
- </li>
- <li>
- April 15, 2015 by Michael Wetter:<br/>
- Changed connector variable to be temperature instead of
- specific enthalpy.
- </li>
- <li>
- January 21, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that is used to connect a fluid port with an output signal.
+The model needs to be used in conjunction with an instance of
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Inlet\">
+AixLib.Fluid.FMI.Adaptors.Inlet</a> in order for
+fluid mass flow rate and pressure to be properly assigned to
+the acausal fluid models.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.PartialTwoPort\">
+AixLib.Fluid.FMI.ExportContainers.PartialTwoPort</a>
+or
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume</a>
+for how to use this model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 18, 2024, by Michael Wetter:<br/>
+Added causality.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1853\">IBPSA, #1853</a>.
+</li>
+<li>
+June 29, 2023, by Michael Wetter:<br/>
+Corrected dimension of <code>X</code> in function call.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1768\">#1768</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air and water.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Corrected wrong argument type in function call of <code>Medium.temperature_phX</code>.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Redesigned to conditionally remove the pressure connector
+if <code>use_p_in=false</code>.
+</li>
+<li>
+April 15, 2015 by Michael Wetter:<br/>
+Changed connector variable to be temperature instead of
+specific enthalpy.
+</li>
+<li>
+January 21, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outlet;
diff --git a/AixLib/Fluid/FMI/Adaptors/ThermalZone.mo b/AixLib/Fluid/FMI/Adaptors/ThermalZone.mo
index c43e39750f..8e15e9dda6 100644
--- a/AixLib/Fluid/FMI/Adaptors/ThermalZone.mo
+++ b/AixLib/Fluid/FMI/Adaptors/ThermalZone.mo
@@ -114,19 +114,19 @@ protected
           extent={{-150,90},{140,50}},
           textString="%name",
           textColor={0,0,255})}), Documentation(info="<html>
- <p>
- The (time varying) vector <code>Real</code> output signal of this block can be defined in its
- parameter menu via variable <code>y</code>. The purpose is to support the
- easy definition of vector-valued Real expressions in a block diagram.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 27, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+The (time varying) vector <code>Real</code> output signal of this block can be defined in its
+parameter menu via variable <code>y</code>. The purpose is to support the
+easy definition of vector-valued Real expressions in a block diagram.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 27, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end RealVectorExpression;
 
   block x_i_toX_w "Conversion from Xi to X"
@@ -163,32 +163,32 @@ protected
   X_w_internal = sum(Xi_internal);
   connect( X_w, X_w_internal)
   annotation (Documentation(revisions="<html>
-   <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- November 8, 2016, by Michael Wetter:<br/>
- Removed wrong usage of <code>each</code> keyword.
- </li>
- <li>
- April 27, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Block that converts a vector input for the water mass fraction <code>Xi</code>
- to a scalar output <code>X</code>.
- This is needed for models in which a scalar input signal <code>Xi</code> that
- may be conditionally removed is to be connected to a model with a vector
- input <code>X</code>, because the conversion from scalar to vector
- needs to access the conditional connector, but conditional connectors
- can only be used in <code>connect</code> statements.
- </p>
- </html>"));
+  <ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Removed wrong usage of <code>each</code> keyword.
+</li>
+<li>
+April 27, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Block that converts a vector input for the water mass fraction <code>Xi</code>
+to a scalar output <code>X</code>.
+This is needed for models in which a scalar input signal <code>Xi</code> that
+may be conditionally removed is to be connected to a model with a vector
+input <code>X</code>, because the conversion from scalar to vector
+needs to access the conditional connector, but conditional connectors
+can only be used in <code>connect</code> statements.
+</p>
+</html>"));
   end x_i_toX_w;
 
 initial equation
@@ -333,70 +333,70 @@ equation
           horizontalAlignment=TextAlignment.Right,
           textString="[%nPorts]")}),
     Documentation(info="<html>
- <p>
- Adaptor that can be used to connect a model of a thermal zone (with acausal ports)
- to input/output signals, which can be exposed in an FMI interface.
- </p>
- <p>
- This model has a vector <code>fluPor</code> with dimension <code>nPorts</code>
- which can be exposed at the FMI interface for the connecting the HVAC system.
- These connectors contain for each fluid inlet the mass flow rate, the temperature,
- the water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>),
- and the trace substances (unless <code>Medium.nC=0</code>).
- </p>
- 
- <p>
- The connector <code>ports</code> can be used to connect the model with a thermal zone.
- The number of connections to <code>ports</code> must
- be equal to <code>nPorts</code>.
- </p>
- 
- <h4>Assumption and limitations</h4>
- <p>
- The mass flow rates at <code>ports</code> sum to zero, hence this
- model conserves mass. If the mass flow rates at <code>fluPor</code>
- do not sum to zero, then this model stops with an error.
- </p>
- <p>
- This model does not impose any pressure, other than setting the pressure
- of all fluid connections to <code>ports</code> to be equal.
- The reason is that setting a pressure can lead to non-physical system models,
- for example if a mass flow rate is imposed and the HVAC system is connected
- to a model that sets a pressure boundary condition such as
- <a href=\"modelica://AixLib.Fluid.Sources.Outside\">
- AixLib.Fluid.Sources.Outside</a>.
- Also, setting a pressure would make it impossible to use multiple instances
- of this model (one for each thermal zone) and build in Modelica an airflow network
- model with pressure driven mass flow rates.
- </p>
- <p>
- The model has no pressure drop.
- </p>
- 
- <h4>Typical use</h4>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZone
- </a>
- for a model that uses this model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- Revised implementation and documentation.
- </li>
- <li>
- April 27, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Adaptor that can be used to connect a model of a thermal zone (with acausal ports)
+to input/output signals, which can be exposed in an FMI interface.
+</p>
+<p>
+This model has a vector <code>fluPor</code> with dimension <code>nPorts</code>
+which can be exposed at the FMI interface for the connecting the HVAC system.
+These connectors contain for each fluid inlet the mass flow rate, the temperature,
+the water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>),
+and the trace substances (unless <code>Medium.nC=0</code>).
+</p>
+
+<p>
+The connector <code>ports</code> can be used to connect the model with a thermal zone.
+The number of connections to <code>ports</code> must
+be equal to <code>nPorts</code>.
+</p>
+
+<h4>Assumption and limitations</h4>
+<p>
+The mass flow rates at <code>ports</code> sum to zero, hence this
+model conserves mass. If the mass flow rates at <code>fluPor</code>
+do not sum to zero, then this model stops with an error.
+</p>
+<p>
+This model does not impose any pressure, other than setting the pressure
+of all fluid connections to <code>ports</code> to be equal.
+The reason is that setting a pressure can lead to non-physical system models,
+for example if a mass flow rate is imposed and the HVAC system is connected
+to a model that sets a pressure boundary condition such as
+<a href=\"modelica://AixLib.Fluid.Sources.Outside\">
+AixLib.Fluid.Sources.Outside</a>.
+Also, setting a pressure would make it impossible to use multiple instances
+of this model (one for each thermal zone) and build in Modelica an airflow network
+model with pressure driven mass flow rates.
+</p>
+<p>
+The model has no pressure drop.
+</p>
+
+<h4>Typical use</h4>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZone
+</a>
+for a model that uses this model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+Revised implementation and documentation.
+</li>
+<li>
+April 27, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZone;
diff --git a/AixLib/Fluid/FMI/BaseClasses/X_w_toX.mo b/AixLib/Fluid/FMI/BaseClasses/X_w_toX.mo
index bebd398102..a0ac426d11 100644
--- a/AixLib/Fluid/FMI/BaseClasses/X_w_toX.mo
+++ b/AixLib/Fluid/FMI/BaseClasses/X_w_toX.mo
@@ -25,33 +25,33 @@ equation
   // Assign vector to output connector
  X = if Medium.nX == 1 then ones(Medium.nX) else cat(1, {X_w_internal}, {1-X_w_internal});
   annotation (Documentation(revisions="<html>
-   <ul>
-   <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- March 17, 2017, by Michael Wetter:<br/>
- Changed assignment of <code>X</code>.<br/>
- This is for
- <a href=\"https://github.com/iea-annex60/modelica-annex60/issues/675\">Annex 60, #675</a>.
- </li>
- <li>
- April 15, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Block that converts a scalar input for the water mass fraction <code>Xi</code>
- to a vector output <code>X</code>.
- This is needed for models in which a scalar input signal <code>Xi</code> that
- may be conditionally removed is to be connected to a model with a vector
- input <code>X</code>, because the conversion from scalar to vector
- needs to access the conditional connector, but conditional connectors
- can only be used in <code>connect</code> statements.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <ul>
+  <li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+March 17, 2017, by Michael Wetter:<br/>
+Changed assignment of <code>X</code>.<br/>
+This is for
+<a href=\"https://github.com/iea-annex60/modelica-annex60/issues/675\">Annex 60, #675</a>.
+</li>
+<li>
+April 15, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Block that converts a scalar input for the water mass fraction <code>Xi</code>
+to a vector output <code>X</code>.
+This is needed for models in which a scalar input signal <code>Xi</code> that
+may be conditionally removed is to be connected to a model with a vector
+input <code>X</code>, because the conversion from scalar to vector
+needs to access the conditional connector, but conditional connectors
+can only be used in <code>connect</code> statements.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end X_w_toX;
diff --git a/AixLib/Fluid/FMI/BaseClasses/hOut_toT.mo b/AixLib/Fluid/FMI/BaseClasses/hOut_toT.mo
index 3a25ece8c1..8306d78f8d 100644
--- a/AixLib/Fluid/FMI/BaseClasses/hOut_toT.mo
+++ b/AixLib/Fluid/FMI/BaseClasses/hOut_toT.mo
@@ -34,21 +34,21 @@ equation
       X=Xi_internal);
 
 annotation (Documentation(revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- April 28, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Block that converts enthalpy to temperature.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+April 28, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Block that converts enthalpy to temperature.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end hOut_toT;
diff --git a/AixLib/Fluid/FMI/Conversion/AirToOutlet.mo b/AixLib/Fluid/FMI/Conversion/AirToOutlet.mo
index beb9ae7f34..d4e68c4860 100644
--- a/AixLib/Fluid/FMI/Conversion/AirToOutlet.mo
+++ b/AixLib/Fluid/FMI/Conversion/AirToOutlet.mo
@@ -48,7 +48,7 @@ block AirToOutlet
     if allowFlowReversal
     "Temperature of the backward flowing medium in the connector outlet"
     annotation (Placement(
-        visible=allowFloWReserval,
+        visible=allowFlowReversal,
         transformation(extent={{20,20},{-20,-20}},
         rotation=90,
         origin={-60,-120}),
@@ -61,7 +61,7 @@ block AirToOutlet
     if Medium.nXi > 0 and allowFlowReversal
     "Water mass fraction per total air mass of the backward flowing medium in the connector outlet"
     annotation (Placement(
-        visible=allowFloWReserval,
+        visible=allowFlowReversal,
         transformation(extent={{20,20},{-20,-20}},
         rotation=90,
         origin={0,-120}),
@@ -74,7 +74,7 @@ block AirToOutlet
     if allowFlowReversal
     "Trace substances of the backward flowing medium in the connector outlet"
     annotation (Placement(
-        visible=allowFloWReserval,
+        visible=allowFlowReversal,
         transformation(extent={{20,20},{-20,-20}},
         rotation=90,
         origin={60,-120}),
@@ -93,7 +93,7 @@ protected
     "Internal connector for water vapor concentration in kg/kg total air";
 
    // Conditional connectors for the backward flowing medium
-  AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
+  output AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
     redeclare final package Medium = Medium)
     "Internal connector for fluid properties for back flow";
 
@@ -159,35 +159,40 @@ equation
   connect(outlet.backward, bacPro_internal);
   annotation (defaultComponentName = "con",
     Documentation(info="<html>
- <p>
- Block that takes real inputs for properties of an air-based HVAC
- system and converts them to an outlet connector of type
- <a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Outlet\">
- AixLib.Fluid.FMI.Interfaces.Outlet</a>.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.HVAC\">
- AixLib.Fluid.FMI.Adaptors.HVAC</a>
- for its usage.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- November 8, 2016, by Michael Wetter:<br/>
- Corrected wrong argument type in function call of <code>Medium.temperature_phX</code>.
- </li>
- <li>
- April 20, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block that takes real inputs for properties of an air-based HVAC
+system and converts them to an outlet connector of type
+<a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Outlet\">
+AixLib.Fluid.FMI.Interfaces.Outlet</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.HVAC\">
+AixLib.Fluid.FMI.Adaptors.HVAC</a>
+for its usage.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 1, 2024, by Michael Wetter:<br/>
+Added causality.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1829\">#1829</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+November 8, 2016, by Michael Wetter:<br/>
+Corrected wrong argument type in function call of <code>Medium.temperature_phX</code>.
+</li>
+<li>
+April 20, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Text(
           extent={{-98,52},{-66,26}},
@@ -227,6 +232,6 @@ equation
           fillColor={0,0,255},
           fillPattern=FillPattern.Solid,
           origin={-4,-58},
-          rotation=270)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          rotation=270)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirToOutlet;
diff --git a/AixLib/Fluid/FMI/Conversion/InletToAir.mo b/AixLib/Fluid/FMI/Conversion/InletToAir.mo
index 80e2ebf6b5..feccd90e7a 100644
--- a/AixLib/Fluid/FMI/Conversion/InletToAir.mo
+++ b/AixLib/Fluid/FMI/Conversion/InletToAir.mo
@@ -24,7 +24,7 @@ block InletToAir
     if allowFlowReversal
     "Zone air temperature"
     annotation (Placement(
-        visible=allowFloWReserval,
+        visible=allowFlowReversal,
         transformation(extent={{-20,-20},{20,20}},
         rotation=90,
         origin={-60,-120}),
@@ -37,7 +37,7 @@ block InletToAir
     if Medium.nXi > 0 and allowFlowReversal
     "Zone air water mass fraction per total air mass"
     annotation (Placement(
-        visible=allowFloWReserval,
+        visible=allowFlowReversal,
         transformation(extent={{-20,-20},{20,20}},
         rotation=90,
         origin={0,-120}),
@@ -50,7 +50,7 @@ block InletToAir
     if allowFlowReversal
     "Zone air trace substances"
     annotation (Placement(
-        visible=allowFloWReserval,
+        visible=allowFlowReversal,
         transformation(extent={{-20,-20},{20,20}},
         rotation=90,
         origin={60,-120}),
@@ -77,7 +77,7 @@ block InletToAir
     annotation (Placement(transformation(extent={{100,-100},{140,-60}})));
 
 protected
-  AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
+  input AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
     redeclare final package Medium = Medium)
     "Internal connector for fluid properties for back flow";
 
@@ -131,63 +131,68 @@ equation
 
   annotation (defaultComponentName = "con",
     Documentation(info="<html>
- <p>
- Block that takes an inlet connector of type
- <a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Inlet\">
- AixLib.Fluid.FMI.Interfaces.Inlet
- </a>
- and converts
- it to real outputs for properties of an air-based
- HVAC system.
- </p>
- <p>
- The output signal <code>m_flow</code> is equal to
- <code>inlet.m_flow</code>, whereas the output signals
- <code>T</code>, <code>X_w</code> and <code>C</code>
- are set the the properties
- <code>inlet.forward</code>.
- Similarly, the properties of
- <code>inlet.backward</code> are set the the values
- of the input signals
- <code>TAirZon</code>, <code>X_wZon</code> and <code>CZon</code>.
- </p>
- <p>
- If <code>allowFlowReversal = true</code>,
- input signal connectors are enabled that are used
- to set the fluid properties for backflow in the connector
- <code>inlet.backward</code>.
- This can be used if this block is used to connect an HVAC
- system to a thermal zone, in which case the supply air
- properties are in the connector
- <code>inlet.forward</code>,
- and the return air properties are in the connector
- <code>inlet.backward</code>.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.ThermalZone\">
- AixLib.Fluid.FMI.Adaptors.ThermalZone</a>
- for its usage.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- June 28, 2016, by Michael Wetter:<br/>
- Revised implementation to allow flow out of the
- thermal zone, for example to model the return
- air flow.
- </li>
- <li>
- April 27, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block that takes an inlet connector of type
+<a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Inlet\">
+AixLib.Fluid.FMI.Interfaces.Inlet
+</a>
+and converts
+it to real outputs for properties of an air-based
+HVAC system.
+</p>
+<p>
+The output signal <code>m_flow</code> is equal to
+<code>inlet.m_flow</code>, whereas the output signals
+<code>T</code>, <code>X_w</code> and <code>C</code>
+are set the the properties
+<code>inlet.forward</code>.
+Similarly, the properties of
+<code>inlet.backward</code> are set the the values
+of the input signals
+<code>TAirZon</code>, <code>X_wZon</code> and <code>CZon</code>.
+</p>
+<p>
+If <code>allowFlowReversal = true</code>,
+input signal connectors are enabled that are used
+to set the fluid properties for backflow in the connector
+<code>inlet.backward</code>.
+This can be used if this block is used to connect an HVAC
+system to a thermal zone, in which case the supply air
+properties are in the connector
+<code>inlet.forward</code>,
+and the return air properties are in the connector
+<code>inlet.backward</code>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.ThermalZone\">
+AixLib.Fluid.FMI.Adaptors.ThermalZone</a>
+for its usage.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 1, 2024, by Michael Wetter:<br/>
+Added causality.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1829\">#1829</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+June 28, 2016, by Michael Wetter:<br/>
+Revised implementation to allow flow out of the
+thermal zone, for example to model the return
+air flow.
+</li>
+<li>
+April 27, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Text(
           extent={{58,60},{90,34}},
@@ -219,7 +224,7 @@ equation
         Text(
           visible=allowFlowReversal and Medium.nXi > 0,
           extent={{-28,-68},{36,-94}},
-          lineColor={0,0,127},
+          textColor={0,0,127},
           textString="X_w"),
         Polygon(
           visible=allowFlowReversal,
@@ -233,6 +238,6 @@ equation
           visible=allowFlowReversal,
           points={{-76,-16},{-34,-36},{-8,-66}},
           color={0,0,255},
-          smooth=Smooth.Bezier)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          smooth=Smooth.Bezier)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InletToAir;
diff --git a/AixLib/Fluid/FMI/Conversion/Validation/AirToOutlet.mo b/AixLib/Fluid/FMI/Conversion/Validation/AirToOutlet.mo
index f739a89f63..57832fa714 100644
--- a/AixLib/Fluid/FMI/Conversion/Validation/AirToOutlet.mo
+++ b/AixLib/Fluid/FMI/Conversion/Validation/AirToOutlet.mo
@@ -63,27 +63,27 @@ equation
           -14,-78},{-2,-78}}, color={0,0,127}));
 annotation (
     Documentation(info="<html>
- <p>
- This example validates the conversion model
- <a href=\"modelica://AixLib.Fluid.FMI.Conversion.AirToOutlet\">
- AixLib.Fluid.FMI.Conversion.AirToOutlet</a>
- for the situation without reverse flow.
- </p>
- <p>
- The conversion elements all have either a dry or
- moist air medium, with our without trace substances,
- in order to test all combinations of air.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 20, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates the conversion model
+<a href=\"modelica://AixLib.Fluid.FMI.Conversion.AirToOutlet\">
+AixLib.Fluid.FMI.Conversion.AirToOutlet</a>
+for the situation without reverse flow.
+</p>
+<p>
+The conversion elements all have either a dry or
+moist air medium, with our without trace substances,
+in order to test all combinations of air.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 20, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Conversion/Validation/AirToOutlet.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirToOutlet;
diff --git a/AixLib/Fluid/FMI/Conversion/Validation/AirToOutletFlowReversal.mo b/AixLib/Fluid/FMI/Conversion/Validation/AirToOutletFlowReversal.mo
index e976e89680..4eda2cbfd5 100644
--- a/AixLib/Fluid/FMI/Conversion/Validation/AirToOutletFlowReversal.mo
+++ b/AixLib/Fluid/FMI/Conversion/Validation/AirToOutletFlowReversal.mo
@@ -78,27 +78,27 @@ equation
   connect(bouDryAirWithC.inlet, conDryAirWithC.outlet)
     annotation (Line(points={{39,-70},{21,-70}},          color={0,0,255}));
   annotation (Documentation(info="<html>
- <p>
- This example is identical to
- <a href=\"modelica://AixLib.Fluid.FMI.Conversion.Validation.AirToOutlet\">
- AixLib.Fluid.FMI.Conversion.Validation.AirToOutlet</a>,
- except that it has reverse flow.
- This tests whether the fluid properties from
- the upstream media are correctly converted to
- the output signals of
- <a href=\"modelica://AixLib.Fluid.FMI.Conversion.AirToOutlet\">
- AixLib.Fluid.FMI.Conversion.AirToOutlet</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 29, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example is identical to
+<a href=\"modelica://AixLib.Fluid.FMI.Conversion.Validation.AirToOutlet\">
+AixLib.Fluid.FMI.Conversion.Validation.AirToOutlet</a>,
+except that it has reverse flow.
+This tests whether the fluid properties from
+the upstream media are correctly converted to
+the output signals of
+<a href=\"modelica://AixLib.Fluid.FMI.Conversion.AirToOutlet\">
+AixLib.Fluid.FMI.Conversion.AirToOutlet</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 29, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Conversion/Validation/AirToOutletFlowReversal.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirToOutletFlowReversal;
diff --git a/AixLib/Fluid/FMI/Conversion/Validation/InletToAirDryAir.mo b/AixLib/Fluid/FMI/Conversion/Validation/InletToAirDryAir.mo
index 67c37a2dda..d5d80a2c1d 100644
--- a/AixLib/Fluid/FMI/Conversion/Validation/InletToAirDryAir.mo
+++ b/AixLib/Fluid/FMI/Conversion/Validation/InletToAirDryAir.mo
@@ -4,23 +4,23 @@ model InletToAirDryAir
   extends AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir(
     redeclare replaceable package Medium = Modelica.Media.Air.SimpleAir);
   annotation (Documentation(info="<html>
- <p>
- This validation test is identical to
- <a href=\"modelica://AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir\">
- AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir</a>
- except that it uses a medium model without moisture.
- Hence, it tests whether the water vapor connectors are correctly removed.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This validation test is identical to
+<a href=\"modelica://AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir\">
+AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir</a>
+except that it uses a medium model without moisture.
+Hence, it tests whether the water vapor connectors are correctly removed.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Conversion/Validation/InletToAirDryAir.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InletToAirDryAir;
diff --git a/AixLib/Fluid/FMI/Conversion/Validation/InletToAirDryAirCO2.mo b/AixLib/Fluid/FMI/Conversion/Validation/InletToAirDryAirCO2.mo
index b2a99b28fe..e3121c5c31 100644
--- a/AixLib/Fluid/FMI/Conversion/Validation/InletToAirDryAirCO2.mo
+++ b/AixLib/Fluid/FMI/Conversion/Validation/InletToAirDryAirCO2.mo
@@ -4,23 +4,23 @@ model InletToAirDryAirCO2
   extends AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAirCO2(
     redeclare replaceable package Medium = Modelica.Media.Air.SimpleAir(extraPropertiesNames={"CO2"}));
   annotation (Documentation(info="<html>
- <p>
- This validation test is identical to
- <a href=\"modelica://AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAirCO2\">
- AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAirCO2</a>
- except that it uses a medium model without moisture.
- Hence, it tests whether the water vapor connectors are correctly removed.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This validation test is identical to
+<a href=\"modelica://AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAirCO2\">
+AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAirCO2</a>
+except that it uses a medium model without moisture.
+Hence, it tests whether the water vapor connectors are correctly removed.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Conversion/Validation/InletToAirDryAirCO2.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InletToAirDryAirCO2;
diff --git a/AixLib/Fluid/FMI/Conversion/Validation/InletToAirMoistAir.mo b/AixLib/Fluid/FMI/Conversion/Validation/InletToAirMoistAir.mo
index 3dcb12b2f5..17124eee85 100644
--- a/AixLib/Fluid/FMI/Conversion/Validation/InletToAirMoistAir.mo
+++ b/AixLib/Fluid/FMI/Conversion/Validation/InletToAirMoistAir.mo
@@ -81,33 +81,33 @@ equation
           {64,-52},{30,-52},{30,-42}}, color={0,0,127}));
 annotation (
     Documentation(info="<html>
- <p>
- This example validates the conversion model
- <a href=\"modelica://AixLib.Fluid.FMI.Conversion.InletToAir\">
- AixLib.Fluid.FMI.Conversion.InletToAir
- </a>.
- The medium used is
- <a href=\"modelica://AixLib.Media.Air\">
- AixLib.Media.Air
- </a>
- without trace substances.
- The top model has no reverse flow, whereas the
- bottom model has reverse flow.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- Added validation test for reverse flow.
- </li>
- <li>
- April 28, 2016 by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates the conversion model
+<a href=\"modelica://AixLib.Fluid.FMI.Conversion.InletToAir\">
+AixLib.Fluid.FMI.Conversion.InletToAir
+</a>.
+The medium used is
+<a href=\"modelica://AixLib.Media.Air\">
+AixLib.Media.Air
+</a>
+without trace substances.
+The top model has no reverse flow, whereas the
+bottom model has reverse flow.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+Added validation test for reverse flow.
+</li>
+<li>
+April 28, 2016 by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Conversion/Validation/InletToAirMoistAir.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InletToAirMoistAir;
diff --git a/AixLib/Fluid/FMI/Conversion/Validation/InletToAirMoistAirCO2.mo b/AixLib/Fluid/FMI/Conversion/Validation/InletToAirMoistAirCO2.mo
index c1073f8589..5be668bf41 100644
--- a/AixLib/Fluid/FMI/Conversion/Validation/InletToAirMoistAirCO2.mo
+++ b/AixLib/Fluid/FMI/Conversion/Validation/InletToAirMoistAirCO2.mo
@@ -11,31 +11,31 @@ equation
           {36,-70},{36,-42}}, color={0,0,127}));
   annotation (
     Documentation(info="<html>
- <p>
- This example validates the conversion model
- <a href=\"modelica://AixLib.Fluid.FMI.Conversion.InletToAir\">
- AixLib.Fluid.FMI.Conversion.InletToAir
- </a>.
- It is identical to
- <a href=\"modelica://AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir\">
- AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir</a>
- except that
- the medium has <code>C02</code> trace substances.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- Added validation test for reverse flow.
- </li>
- <li>
- April 28, 2016 by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates the conversion model
+<a href=\"modelica://AixLib.Fluid.FMI.Conversion.InletToAir\">
+AixLib.Fluid.FMI.Conversion.InletToAir
+</a>.
+It is identical to
+<a href=\"modelica://AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir\">
+AixLib.Fluid.FMI.Conversion.Validation.InletToAirMoistAir</a>
+except that
+the medium has <code>C02</code> trace substances.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+Added validation test for reverse flow.
+</li>
+<li>
+April 28, 2016 by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Conversion/Validation/InletToAirMoistAirCO2.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InletToAirMoistAirCO2;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Fan.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Fan.mo
index 9c72cb9d09..a5914de2e2 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Fan.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Fan.mo
@@ -3,6 +3,7 @@ block Fan "Declaration of an FMU that exports a fan"
    extends AixLib.Fluid.FMI.ExportContainers.ReplaceableTwoPort(
      redeclare replaceable package Medium =  AixLib.Media.Air,
      redeclare final Movers.FlowControlled_dp com(
+      nominalValuesDefineDefaultPressureCurve=true,
       final m_flow_nominal=m_flow_nominal,
       final use_inputFilter=
                           false,
@@ -10,8 +11,8 @@ block Fan "Declaration of an FMU that exports a fan"
 
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=0.01
     "Nominal mass flow rate";
-  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")=
-       500 "Pressure drop at nominal mass flow rate";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+     = 500 "Pressure drop at nominal mass flow rate";
 
   Modelica.Blocks.Interfaces.RealInput dp_in(min=0, final unit="Pa")
     "Prescribed pressure rise"
@@ -28,33 +29,40 @@ equation
       smooth=Smooth.None));
   annotation (
   Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU with a fluid flow component.
- The FMU has an instance of
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
- AixLib.Fluid.Movers.FlowControlled_dp</a>.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">
- AixLib.Fluid.FMI.UsersGuide</a> for why there is no model that exports
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
- AixLib.Fluid.Movers.FlowControlled_m_flow</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 3, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU with a fluid flow component.
+The FMU has an instance of
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
+AixLib.Fluid.Movers.FlowControlled_dp</a>.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">
+AixLib.Fluid.FMI.UsersGuide</a> for why there is no model that exports
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.FlowControlled_m_flow</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 9, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 3, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/Fan.mos"
         "Export FMU"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
@@ -74,6 +82,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
           lineColor={0,0,0},
           pattern=LinePattern.None,
           fillPattern=FillPattern.HorizontalCylinder,
-          fillColor={255,255,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={255,255,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Fan;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/FlowSplitter_u.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/FlowSplitter_u.mo
index 5722b1deb6..2954700ae9 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/FlowSplitter_u.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/FlowSplitter_u.mo
@@ -7,21 +7,21 @@ block FlowSplitter_u "Declaration of an FMU that exports a flow splitter"
         allowFlowReversal(start=false));
 
   annotation (  Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU with a fluid flow component.
- The FMU is an instance of
- <a href=\"modelica://AixLib.Fluid.FMI.FlowSplitter_u\">
- AixLib.Fluid.FMI.FlowSplitter_u</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 20, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU with a fluid flow component.
+The FMU is an instance of
+<a href=\"modelica://AixLib.Fluid.FMI.FlowSplitter_u\">
+AixLib.Fluid.FMI.FlowSplitter_u</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 20, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/FlowSplitter_u.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowSplitter_u;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZone.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZone.mo
index 1b2527bba8..96b2c38390 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZone.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZone.mo
@@ -253,62 +253,62 @@ equation
           textString="TOut")}),                                  Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-160,-160},{160,160}})),
     Documentation(info="<html>
- <p>
- This example demonstrates how to export a model of an HVAC system
- that only provides convective cooling to a single thermal zone.
- <!-- @include_Buildings
- The HVAC system is adapted from
- <a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
- AixLib.Examples.Tutorial.SpaceCooling.System3</a>,
- but flow resistances have been added to have the same configuration as
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones</a>.
- -->
- <!-- @include_Buildings
- Having the same configuration is needed for the validation test
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
- AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>.
- -->
- </p>
- <p>
- The example extends from
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone
- </a>
- which provides the input and output signals that are needed to interface
- the acausal HVAC system model with causal connectors of FMI.
- The instance <code>hvacAda</code> is the HVAC adapter
- that contains on the left a fluid port, and on the right signal ports
- which are then used to connect at the top-level of the model to signal
- ports which are exposed at the FMU interface.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2021 by David Blum:<br/>
- Correct supply and return water parameterization.<br/>
- Use explicit calculation of sensible and latent load to determine design load
- on cooling coil.<br/>
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2624\">#2624</a>.
- </li>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 11, 2016, by Michael Wetter:<br/>
- Made the cooling coil replaceable because the Buildings library
- uses the model for validation with a cooling coil model that is not
- in the Annex 60 library.
- </li>
- <li>
- April 16, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export a model of an HVAC system
+that only provides convective cooling to a single thermal zone.
+<!-- @include_Buildings
+The HVAC system is adapted from
+<a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
+AixLib.Examples.Tutorial.SpaceCooling.System3</a>,
+but flow resistances have been added to have the same configuration as
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones</a>.
+-->
+<!-- @include_Buildings
+Having the same configuration is needed for the validation test
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
+AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>.
+-->
+</p>
+<p>
+The example extends from
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone
+</a>
+which provides the input and output signals that are needed to interface
+the acausal HVAC system model with causal connectors of FMI.
+The instance <code>hvacAda</code> is the HVAC adapter
+that contains on the left a fluid port, and on the right signal ports
+which are then used to connect at the top-level of the model to signal
+ports which are exposed at the FMU interface.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2021 by David Blum:<br/>
+Correct supply and return water parameterization.<br/>
+Use explicit calculation of sensible and latent load to determine design load
+on cooling coil.<br/>
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2624\">#2624</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 11, 2016, by Michael Wetter:<br/>
+Made the cooling coil replaceable because the Buildings library
+uses the model for validation with a cooling coil model that is not
+in the Annex 60 library.
+</li>
+<li>
+April 16, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZone.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACZone;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZones.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZones.mo
index 20242cbffa..8f61678c87 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZones.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZones.mo
@@ -64,6 +64,7 @@ block HVACZones
     annotation (Placement(transformation(extent={{100,-100},{120,-80}})));
   Movers.FlowControlled_m_flow fan(
     redeclare package Medium = MediumA,
+    nominalValuesDefineDefaultPressureCurve=true,
     m_flow_nominal=mA_flow_nominal,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     allowFlowReversal=allowFlowReversal) "Supply air fan"
@@ -162,6 +163,7 @@ block HVACZones
     redeclare package Medium = MediumA,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     allowFlowReversal=allowFlowReversal,
+    nominalValuesDefineDefaultPressureCurve=true,
     m_flow_nominal=mA_flow_nominal/10,
     inputType=AixLib.Fluid.Types.InputType.Constant)
     "Supply air fan that extracts a constant amount of outside air"
@@ -306,57 +308,64 @@ equation
           textString="TOut")}),                                  Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-160,-160},{160,180}})),
     Documentation(info="<html>
- <p>
- This example demonstrates how to export a model of an HVAC system
- that only provides convective cooling to two thermal zones.
- The example is similar to
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone</a>
- except that is serves two thermal zones rather than one.
- </p>
- <p>
- The example extends from
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZones\">
- AixLib.Fluid.FMI.ExportContainers.HVACZones
- </a>
- which provides the input and output signals that are needed to interface
- the acausal HVAC system model with causal connectors of FMI.
- The instance <code>hvacAda</code> is the HVAC adapter
- that contains on the left a fluid port, and on the right signal ports
- which are then used to connect at the top-level of the model to signal
- ports which are exposed at the FMU interface.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2021 by David Blum:<br/>
- Correct supply and return water parameterization.<br/>
- Use explicit calculation of sensible and latent load to determine design load
- on cooling coil.<br/>
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2624\">#2624</a>.
- </li>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- April 4, 2017, by Michael Wetter:<br/>
- Removed import statement.
- </li>
- <li>
- November 11, 2016, by Michael Wetter:<br/>
- Made the cooling coil replaceable because the Buildings library
- uses the model for validation with a cooling coil model that is not
- in the Annex 60 library.
- </li>
- <li>
- April 16, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export a model of an HVAC system
+that only provides convective cooling to two thermal zones.
+The example is similar to
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone</a>
+except that is serves two thermal zones rather than one.
+</p>
+<p>
+The example extends from
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZones\">
+AixLib.Fluid.FMI.ExportContainers.HVACZones
+</a>
+which provides the input and output signals that are needed to interface
+the acausal HVAC system model with causal connectors of FMI.
+The instance <code>hvacAda</code> is the HVAC adapter
+that contains on the left a fluid port, and on the right signal ports
+which are then used to connect at the top-level of the model to signal
+ports which are exposed at the FMU interface.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 9, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+September 21, 2021 by David Blum:<br/>
+Correct supply and return water parameterization.<br/>
+Use explicit calculation of sensible and latent load to determine design load
+on cooling coil.<br/>
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2624\">#2624</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+April 4, 2017, by Michael Wetter:<br/>
+Removed import statement.
+</li>
+<li>
+November 11, 2016, by Michael Wetter:<br/>
+Made the cooling coil replaceable because the Buildings library
+uses the model for validation with a cooling coil model that is not
+in the Annex 60 library.
+</li>
+<li>
+April 16, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/HVACZones.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACZones;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HeaterCooler_u.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HeaterCooler_u.mo
index 483beff164..f6361d3c29 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HeaterCooler_u.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/HeaterCooler_u.mo
@@ -25,40 +25,40 @@ equation
       smooth=Smooth.None));
 
   annotation (  Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU with a heater
- that takes as an input signal the normalized heat flow rate.
- The FMU has an instance of
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
- AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>.
- </p>
- <p>
- The mass dynamics has been set to
- <code>massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState</code>.
- See the
- <a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">user's guide</a>
- for the rationale.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 3, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU with a heater
+that takes as an input signal the normalized heat flow rate.
+The FMU has an instance of
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
+AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>.
+</p>
+<p>
+The mass dynamics has been set to
+<code>massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState</code>.
+See the
+<a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">user's guide</a>
+for the rationale.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 3, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/HeaterCooler_u.mos"
         "Export FMU"),
     Icon(graphics={
@@ -106,6 +106,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
         Text(
           extent={{-104,94},{-60,66}},
           textColor={0,0,255},
-          textString="u")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="u")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeaterCooler_u;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Heater_T.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Heater_T.mo
index bc5f6312a8..684abf5450 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Heater_T.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Heater_T.mo
@@ -15,8 +15,8 @@ block Heater_T
     "Maximum heat flow rate for cooling (negative)";
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=0.01
     "Nominal mass flow rate";
-  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")=
-       0 "Pressure";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+     = 0 "Pressure";
 
   Modelica.Blocks.Interfaces.RealInput TSet(unit="K", displayUnit="degC")
     "Set point temperature of the fluid that leaves port_b"
@@ -36,34 +36,34 @@ equation
       color={0,0,127},
       smooth=Smooth.None));
   annotation (  Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU with a heater
- that takes as an input signal the leaving fluid temperature.
- The FMU has an instance of
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.PrescribedOutlet\">
- AixLib.Fluid.HeatExchangers.PrescribedOutlet</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 20, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU with a heater
+that takes as an input signal the leaving fluid temperature.
+The FMU has an instance of
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.PrescribedOutlet\">
+AixLib.Fluid.HeatExchangers.PrescribedOutlet</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 20, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/Heater_T.mos"
         "Export FMU"),
     Icon(graphics={
@@ -125,6 +125,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
                    Text(
           extent={{26,-28},{70,-74}},
           textColor={255,255,255},
-          textString="+")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="+")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Heater_T;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Humidifier_u.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Humidifier_u.mo
index 9468334513..59444358db 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Humidifier_u.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/Humidifier_u.mo
@@ -12,8 +12,8 @@ block Humidifier_u
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=0.01
     "Nominal mass flow rate";
 
-  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")=
-       0 "Pressure";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+     = 0 "Pressure";
 
   parameter Modelica.Units.SI.MassFlowRate mWat_flow_nominal=0.01*0.005
     "Water mass flow rate at u=1, positive for humidification";
@@ -28,41 +28,41 @@ equation
       smooth=Smooth.None));
 
   annotation (  Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU with a humidifier
- that takes as an input signal the normalized mass flow rate of water that
- will be added to the medium.
- The FMU has an instance of
- <a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
- AixLib.Fluid.Humidifiers.Humidifier_u</a>.
- </p>
- <p>
- The mass dynamics has been set to
- <code>massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState</code>.
- See the
- <a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">user's guide</a>
- for the rationale.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed temperature that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- April 29, 2015 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU with a humidifier
+that takes as an input signal the normalized mass flow rate of water that
+will be added to the medium.
+The FMU has an instance of
+<a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
+AixLib.Fluid.Humidifiers.Humidifier_u</a>.
+</p>
+<p>
+The mass dynamics has been set to
+<code>massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState</code>.
+See the
+<a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">user's guide</a>
+for the rationale.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed temperature that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+April 29, 2015 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/Humidifier_u.mos"
         "Export FMU"),
     Icon(graphics={
@@ -110,6 +110,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
         Text(
           extent={{-104,94},{-60,66}},
           textColor={0,0,255},
-          textString="u")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="u")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Humidifier_u;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/IdealSource_m_flow.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/IdealSource_m_flow.mo
index c17fddfda8..9eeed9d10c 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/IdealSource_m_flow.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/IdealSource_m_flow.mo
@@ -12,7 +12,7 @@ block IdealSource_m_flow "Declaration of an FMU that exports a mass flow source
 equation
   assert(abs(inlet.m_flow-outlet.m_flow) < 1E-2,
   "The mass flow rate of port_a and port_b is not conserved.
-   This indicates a wrong configuration of your system model.");
+  This indicates a wrong configuration of your system model.");
   outlet.m_flow = m_flow_in;
 
   // We use connect statements
@@ -27,22 +27,22 @@ equation
 
   annotation (
   Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU that sets the mass flow rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 24, 2015 by Michael Wetter:<br/>
- Changed assignment of pressure to a <code>connect</code> statement
- because the pressure can be conditionally removed.
- </li>
- <li>
- November 3, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU that sets the mass flow rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Changed assignment of pressure to a <code>connect</code> statement
+because the pressure can be conditionally removed.
+</li>
+<li>
+November 3, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/IdealSource_m_flow.mos"
         "Export FMU"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
@@ -66,6 +66,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
           lineColor={0,0,0},
           pattern=LinePattern.None,
           fillPattern=FillPattern.HorizontalCylinder,
-          fillColor={255,255,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={255,255,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end IdealSource_m_flow;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/MixingVolume.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/MixingVolume.mo
index 86c88dbc31..7bf5a4e2ca 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/MixingVolume.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/MixingVolume.mo
@@ -50,28 +50,28 @@ equation
   annotation (
   defaultComponentName="vol",
 Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU with a
- control volume.
- The FMU has an instance of
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
- AixLib.Fluid.MixingVolumes.MixingVolume</a>.
- </p>
- <p>
- The mass dynamics has been set to
- <code>massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState</code>.
- See the
- <a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">user's guide</a>
- for the rationale.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 21, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU with a
+control volume.
+The FMU has an instance of
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
+AixLib.Fluid.MixingVolumes.MixingVolume</a>.
+</p>
+<p>
+The mass dynamics has been set to
+<code>massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState</code>.
+See the
+<a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">user's guide</a>
+for the rationale.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 21, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/MixingVolume.mos"
         "Export FMU"),
     Icon(graphics={
@@ -84,6 +84,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
           extent={{-26,30},{40,-36}},
           lineColor={0,0,0},
           fillPattern=FillPattern.Sphere,
-          fillColor={170,213,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={170,213,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolume;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/PressureDrop.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/PressureDrop.mo
index ff7e80bae1..254348d4f3 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/PressureDrop.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/PressureDrop.mo
@@ -8,30 +8,30 @@ block PressureDrop
 
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=0.01
     "Nominal mass flow rate";
-  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")=
-       100 "Pressure drop at nominal mass flow rate";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+     = 100 "Pressure drop at nominal mass flow rate";
   annotation (
   Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU with a fluid flow component.
- The FMU has an instance of
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
- AixLib.Fluid.FixedResistances.PressureDrop</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 3, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU with a fluid flow component.
+The FMU has an instance of
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
+AixLib.Fluid.FixedResistances.PressureDrop</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 3, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/PressureDrop.mos"
         "Export FMU"),
     Icon(graphics={
@@ -44,6 +44,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
           extent={{-100,14},{100,-16}},
           lineColor={0,0,0},
           fillColor={0,127,255},
-          fillPattern=FillPattern.HorizontalCylinder)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.HorizontalCylinder)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureDrop;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ResistanceVolume.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ResistanceVolume.mo
index ff436b7fde..074fbda113 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ResistanceVolume.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ResistanceVolume.mo
@@ -79,36 +79,36 @@ equation
       color={0,127,255},
       smooth=Smooth.None));
   annotation (Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU with a
- flow resistance and a control volume.
- The FMU has an instance of
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
- AixLib.Fluid.FixedResistances.PressureDrop</a> and
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
- AixLib.Fluid.MixingVolumes.MixingVolume</a>.
- </p>
- <p>
- The mass dynamics has been set to
- <code>massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState</code>.
- See the
- <a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">user's guide</a>
- for the rationale.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 8, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU with a
+flow resistance and a control volume.
+The FMU has an instance of
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
+AixLib.Fluid.FixedResistances.PressureDrop</a> and
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
+AixLib.Fluid.MixingVolumes.MixingVolume</a>.
+</p>
+<p>
+The mass dynamics has been set to
+<code>massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState</code>.
+See the
+<a href=\"modelica://AixLib.Fluid.FMI.UsersGuide\">user's guide</a>
+for the rationale.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 8, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/ResistanceVolume.mos"
         "Export FMU"),
     Icon(graphics={
@@ -126,6 +126,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
           extent={{18,32},{84,-34}},
           lineColor={0,0,0},
           fillPattern=FillPattern.Sphere,
-          fillColor={170,213,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={170,213,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ResistanceVolume;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZone.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZone.mo
index f9459ec2f5..fa4245ac44 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZone.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZone.mo
@@ -127,71 +127,71 @@ equation
         Text(
           extent={{76,134},{114,110}},
           pattern=LinePattern.None,
-          lineColor={0,0,127},
+          textColor={0,0,127},
           horizontalAlignment=TextAlignment.Left,
           textString="Simplified model of
- a thermal zone.")}),
+a thermal zone.")}),
     Documentation(info="<html>
- <p>
- This example demonstrates how to export a model
- that contains one thermal zone with convective heat input from the
- HVAC system only. The thermal zone is connected to an adaptor so that
- it can be coupled
- to an air-based HVAC system.
- <!-- @include_Buildings
- The thermal zone is
- taken from
- <a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
- AixLib.Examples.Tutorial.SpaceCooling.System3</a>.
- -->
- </p>
- <p>
- The example extends from
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZone
- </a>
- which provides
- the input and output signals that are needed to interface
- the acausal thermal zone model with causal connectors of FMI.
- The instance <code>theZonAda</code> is the thermal zone adaptor
- that contains on the right a fluid port, and on
- the left signal ports which are then used to connect at
- the top-level of the model to signal ports which are
- exposed at the FMU interface.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 11, 2020, by Michael Wetter:<br/>
- Removed <code>fontSize</code> in annotation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1318\">#1318</a>.
- </li>
- <li>
- December 4, 2017, by Michael Wetter:<br/>
- Added call to <code>Modelica.Utilities.Files.loadResource</code>
- for weather data file.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/867\">#867</a>.
- </li>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed temperature that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- September 20, 2016, by Thierry S. Nouidui:<br/>
- Revised implementation and added mass flow rate sensors
- to connect the thermal zone adaptor to the thermal zone.
- </li>
- <li>
- April 28, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export a model
+that contains one thermal zone with convective heat input from the
+HVAC system only. The thermal zone is connected to an adaptor so that
+it can be coupled
+to an air-based HVAC system.
+<!-- @include_Buildings
+The thermal zone is
+taken from
+<a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
+AixLib.Examples.Tutorial.SpaceCooling.System3</a>.
+-->
+</p>
+<p>
+The example extends from
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZone
+</a>
+which provides
+the input and output signals that are needed to interface
+the acausal thermal zone model with causal connectors of FMI.
+The instance <code>theZonAda</code> is the thermal zone adaptor
+that contains on the right a fluid port, and on
+the left signal ports which are then used to connect at
+the top-level of the model to signal ports which are
+exposed at the FMU interface.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 11, 2020, by Michael Wetter:<br/>
+Removed <code>fontSize</code> in annotation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1318\">#1318</a>.
+</li>
+<li>
+December 4, 2017, by Michael Wetter:<br/>
+Added call to <code>Modelica.Utilities.Files.loadResource</code>
+for weather data file.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/867\">#867</a>.
+</li>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed temperature that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+September 20, 2016, by Thierry S. Nouidui:<br/>
+Revised implementation and added mass flow rate sensors
+to connect the thermal zone adaptor to the thermal zone.
+</li>
+<li>
+April 28, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZone.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZone;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZones.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZones.mo
index 6191af2275..415251c786 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZones.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZones.mo
@@ -164,11 +164,11 @@ equation
         Text(
           extent={{68,132},{106,108}},
           pattern=LinePattern.None,
-          lineColor={0,0,127},
+          textColor={0,0,127},
           horizontalAlignment=TextAlignment.Left,
           textString="Very simplified
- model of
- a thermal zone."),
+model of
+a thermal zone."),
         Rectangle(
           extent={{20,0},{112,-126}},
           fillColor={215,215,215},
@@ -177,60 +177,60 @@ equation
         Text(
           extent={{68,-4},{106,-28}},
           pattern=LinePattern.None,
-          lineColor={0,0,127},
+          textColor={0,0,127},
           horizontalAlignment=TextAlignment.Left,
           textString="Very simplified
- model of
- a thermal zone.")}),
+model of
+a thermal zone.")}),
     Documentation(info="<html>
- <p>
- This example demonstrates how to export a model
- that contains two thermal zones with convective heat input from the
- HVAC system only. The thermal zones are connected to an adaptor so that
- they can be coupled
- to an air-based HVAC system.
- <!-- @include_Buildings
- The thermal zone is
- taken from
- <a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
- AixLib.Examples.Tutorial.SpaceCooling.System3</a>.
- -->
- </p>
- <p>
- The example extends from
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZones\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZones</a>
- which provides
- the input and output signals that are needed to interface
- the acausal thermal zone models with causal connectors of FMI.
- The instance <code>theZonAda</code> is the thermal zone adaptor
- that contains on the right a fluid port, and on
- the left signal ports which are then used to connect at
- the top-level of the model to signal ports which are
- exposed at the FMU interface.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 11, 2020, by Michael Wetter:<br/>
- Removed <code>fontSize</code> in annotation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1318\">#1318</a>.
- </li>
- <li>
- December 4, 2017, by Michael Wetter:<br/>
- Added call to <code>Modelica.Utilities.Files.loadResource</code>
- for weather data file.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/867\">#867</a>.
- </li>
- <li>
- September 14, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export a model
+that contains two thermal zones with convective heat input from the
+HVAC system only. The thermal zones are connected to an adaptor so that
+they can be coupled
+to an air-based HVAC system.
+<!-- @include_Buildings
+The thermal zone is
+taken from
+<a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
+AixLib.Examples.Tutorial.SpaceCooling.System3</a>.
+-->
+</p>
+<p>
+The example extends from
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZones\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZones</a>
+which provides
+the input and output signals that are needed to interface
+the acausal thermal zone models with causal connectors of FMI.
+The instance <code>theZonAda</code> is the thermal zone adaptor
+that contains on the right a fluid port, and on
+the left signal ports which are then used to connect at
+the top-level of the model to signal ports which are
+exposed at the FMU interface.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 11, 2020, by Michael Wetter:<br/>
+Removed <code>fontSize</code> in annotation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1318\">#1318</a>.
+</li>
+<li>
+December 4, 2017, by Michael Wetter:<br/>
+Added call to <code>Modelica.Utilities.Files.loadResource</code>
+for weather data file.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/867\">#867</a>.
+</li>
+<li>
+September 14, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/ThermalZones.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZones;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/TwoPortPassThrough.mo b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/TwoPortPassThrough.mo
index bf94a489c9..d36956709f 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/TwoPortPassThrough.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Examples/FMUs/TwoPortPassThrough.mo
@@ -11,20 +11,20 @@ equation
       smooth=Smooth.None));
   annotation (
   Documentation(info="<html>
- <p>
- This example demonstrates how to export an FMU
- that simply passes all its inputs to its outputs.
- Such an FMU could for example be used in a block diagram as a place-holder
- for another FMU that provides an actual implementation of a component.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 16, 2015 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to export an FMU
+that simply passes all its inputs to its outputs.
+Such an FMU could for example be used in a block diagram as a place-holder
+for another FMU that provides an actual implementation of a component.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 16, 2015 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Examples/FMUs/TwoPortPassThrough.mos"
         "Export FMU"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
@@ -35,6 +35,6 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Exp
           smooth=Smooth.None), Line(
           points={{-100,0},{100,0}},
           color={0,0,255},
-          smooth=Smooth.None)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          smooth=Smooth.None)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoPortPassThrough;
diff --git a/AixLib/Fluid/FMI/ExportContainers/HVACZone.mo b/AixLib/Fluid/FMI/ExportContainers/HVACZone.mo
index d82d546d77..dd678547db 100644
--- a/AixLib/Fluid/FMI/ExportContainers/HVACZone.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/HVACZone.mo
@@ -109,128 +109,128 @@ equation
         Line(points={{-88,66},{-124,-56}}, color={0,0,0})}),     Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-160,-160},{160,160}})),
     Documentation(info="<html>
- <p>
- Model that is used as a container for an HVAC system that is
- to be exported as an FMU and that serves a single zone.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- To use this model as a container for an FMU, extend
- from this model, rather than instantiate it,
- and add your HVAC system. By extending from this model, the top-level
- signal connectors on the right stay at the top-level, and hence
- will be visible at the FMI interface.
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone</a>
- shows how a simple HVAC system can be implemented and exported as
- an FMU.
- <!-- @include_Buildings
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
- AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
- shows how such an FMU can be connected
- to a room model that has signal flow.
- -->
- </p>
- <p>
- The conversion between the fluid ports and signal ports is done
- in the HVAC adapter <code>hvacAda</code>.
- This adapter has a vector of fluid ports called <code>ports</code>.
- The supply and return air ducts, including any resistance model for the inlet
- diffusor or exhaust grill, need to be connected to these ports.
- Also, if a thermal zone has interzonal air exchange or air infiltration,
- these flows need to be connected to <code>ports</code>.
- This model outputs at the port <code>fluPor</code> the mass flow rate for
- each flow that is connected to <code>ports</code>, together with its
- temperature, water vapor mass fraction per total mass of the air (not per kg dry
- air), and trace substances. These quantities are always as if the flow
- enters the room, even if the flow is zero or negative.
- If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
- if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
- the output signal for these properties are removed.
- These quantities are always as if the flow
- enters the room, even if the flow is zero or negative.
- Thus, a thermal zone model that uses these signals to compute the
- heat added by the HVAC system needs to implement an equation such as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
- </p>
- <p>
- where
- <i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
- <i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
- the port <code>fluPor</code> (which is negative if it is an exhaust),
- <i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
- <i>T<sub>sup</sub></i> is the supply air temperature and
- <i>T<sub>air,zon</sub></i> is the zone air temperature.
- Note that without the <i>max(&middot;, &middot;)</i>, the energy
- balance would be wrong.
- </p>
- <p>
- The input signals of this model are the zone radiative temperature.
- The the zone air temperature,
- the water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>)
- and trace substances (unless <code>Medium.nC=0</code>) are obtained from the connector
- <code>fluPor.backward</code>.
- The outflowing fluid stream(s) at the port <code>ports</code> will be at the
- states obtained from <code>fluPor.backward</code>.
- All fluid streams at port <code>ports</code> are at the same
- pressure.
- For convenience, the instance <code>hvacAda</code> also outputs the
- properties obtained from <code>fluPor.backward</code>. These can be used
- to connect a controller. The properties are available for each flow path in
- <code>fluPor.backward</code>. For a thermal zone with mixed air, these are
- all equal, while for a stratified room model, they can be different.
- </p>
- 
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone</a>
- for a model that uses this model.
- </p>
- <p>
- For models that multiple thermal zones connected to the HVAC system,
- use the model
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZones\">
- AixLib.Fluid.FMI.ExportContainers.HVACZones</a>.
- </p>
- <h4>Assumption and limitations</h4>
- <p>
- The mass flow rates at <code>ports</code> sum to zero, hence this
- model conserves mass.
- </p>
- <p>
- This model does not impose any pressure, other than setting the pressure
- of all fluid connections to <code>ports</code> to be equal.
- The reason is that setting a pressure can lead to non-physical system models,
- for example if a mass flow rate is imposed and the HVAC system is connected
- to a model that sets a pressure boundary condition such as
- <a href=\"modelica://AixLib.Fluid.Sources.Outside\">
- AixLib.Fluid.Sources.Outside</a>.
- Also, setting a pressure would make it impossible to use multiple instances
- of this model (one for each thermal zone) and build in Modelica an airflow network
- model with pressure driven mass flow rates.
- </p>
- <p>
- The model has no pressure drop. Hence, the pressure drop
- of an air diffuser or of an exhaust grill needs to be modelled
- in models that are connected to <code>ports</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- April 15, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that is used as a container for an HVAC system that is
+to be exported as an FMU and that serves a single zone.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+To use this model as a container for an FMU, extend
+from this model, rather than instantiate it,
+and add your HVAC system. By extending from this model, the top-level
+signal connectors on the right stay at the top-level, and hence
+will be visible at the FMI interface.
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone</a>
+shows how a simple HVAC system can be implemented and exported as
+an FMU.
+<!-- @include_Buildings
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
+AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
+shows how such an FMU can be connected
+to a room model that has signal flow.
+-->
+</p>
+<p>
+The conversion between the fluid ports and signal ports is done
+in the HVAC adapter <code>hvacAda</code>.
+This adapter has a vector of fluid ports called <code>ports</code>.
+The supply and return air ducts, including any resistance model for the inlet
+diffusor or exhaust grill, need to be connected to these ports.
+Also, if a thermal zone has interzonal air exchange or air infiltration,
+these flows need to be connected to <code>ports</code>.
+This model outputs at the port <code>fluPor</code> the mass flow rate for
+each flow that is connected to <code>ports</code>, together with its
+temperature, water vapor mass fraction per total mass of the air (not per kg dry
+air), and trace substances. These quantities are always as if the flow
+enters the room, even if the flow is zero or negative.
+If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
+if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
+the output signal for these properties are removed.
+These quantities are always as if the flow
+enters the room, even if the flow is zero or negative.
+Thus, a thermal zone model that uses these signals to compute the
+heat added by the HVAC system needs to implement an equation such as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
+</p>
+<p>
+where
+<i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
+<i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
+the port <code>fluPor</code> (which is negative if it is an exhaust),
+<i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
+<i>T<sub>sup</sub></i> is the supply air temperature and
+<i>T<sub>air,zon</sub></i> is the zone air temperature.
+Note that without the <i>max(&middot;, &middot;)</i>, the energy
+balance would be wrong.
+</p>
+<p>
+The input signals of this model are the zone radiative temperature.
+The the zone air temperature,
+the water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>)
+and trace substances (unless <code>Medium.nC=0</code>) are obtained from the connector
+<code>fluPor.backward</code>.
+The outflowing fluid stream(s) at the port <code>ports</code> will be at the
+states obtained from <code>fluPor.backward</code>.
+All fluid streams at port <code>ports</code> are at the same
+pressure.
+For convenience, the instance <code>hvacAda</code> also outputs the
+properties obtained from <code>fluPor.backward</code>. These can be used
+to connect a controller. The properties are available for each flow path in
+<code>fluPor.backward</code>. For a thermal zone with mixed air, these are
+all equal, while for a stratified room model, they can be different.
+</p>
+
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZone</a>
+for a model that uses this model.
+</p>
+<p>
+For models that multiple thermal zones connected to the HVAC system,
+use the model
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZones\">
+AixLib.Fluid.FMI.ExportContainers.HVACZones</a>.
+</p>
+<h4>Assumption and limitations</h4>
+<p>
+The mass flow rates at <code>ports</code> sum to zero, hence this
+model conserves mass.
+</p>
+<p>
+This model does not impose any pressure, other than setting the pressure
+of all fluid connections to <code>ports</code> to be equal.
+The reason is that setting a pressure can lead to non-physical system models,
+for example if a mass flow rate is imposed and the HVAC system is connected
+to a model that sets a pressure boundary condition such as
+<a href=\"modelica://AixLib.Fluid.Sources.Outside\">
+AixLib.Fluid.Sources.Outside</a>.
+Also, setting a pressure would make it impossible to use multiple instances
+of this model (one for each thermal zone) and build in Modelica an airflow network
+model with pressure driven mass flow rates.
+</p>
+<p>
+The model has no pressure drop. Hence, the pressure drop
+of an air diffuser or of an exhaust grill needs to be modelled
+in models that are connected to <code>ports</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+April 15, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACZone;
diff --git a/AixLib/Fluid/FMI/ExportContainers/HVACZones.mo b/AixLib/Fluid/FMI/ExportContainers/HVACZones.mo
index 04dde52ec4..0a7a244dd0 100644
--- a/AixLib/Fluid/FMI/ExportContainers/HVACZones.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/HVACZones.mo
@@ -156,146 +156,146 @@ equation
           textColor={0,0,127},
           textString="[%nZon, %nPorts]")}),
     Documentation(info="<html>
- <p>
- Model that is used as a container for an HVAC system that is
- to be exported as an FMU and that serves multiple zones.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- To use this model as a container for an FMU, simply extend
- from this model, rather than instantiate it,
- and add your HVAC system. By extending from this model, the top-level
- signal connectors on the right stay at the top-level, and hence
- will be visible at the FMI interface.
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones</a>
- shows how a simple HVAC system that serves two rooms can be implemented and exported as
- an FMU.
- <!-- @include_Buildings
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
- AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
- shows how such an FMU can be connected
- to a room model that has signal flow.
- -->
- </p>
- <p>
- The following two parameters need to be assigned by the user:
- Set <code>nZon</code> to the number of thermal zones to which the
- FMU will be connected.
- Set <code>nPorts</code> to the largest number of fluid ports
- that the thermal zones has. For example,
- if <code>nZon=2</code> and zone <i>1</i> has one inlet and one outlet
- (hence it has 2 ports),
- and zone <i>2</i> has one inlets and two outlets
- (hence it has 3 ports), then
- set <code>nPorts=3</code>. This will add more fluid ports than are needed
- for zone <i>1</i>, but this causes no overhead if they are not connected.
- </p>
- <p>
- The conversion between the fluid ports and signal ports is done
- in the HVAC adapter <code>hvacAda</code>.
- This adapter has a vector of fluid ports called <code>ports</code>.
- The supply and return air ducts, including any resistance model for the inlet
- diffusor or exhaust grill, need to be connected to these ports.
- Also, if a thermal zone has interzonal air exchange or air infiltration,
- these flows need to be connected to <code>ports</code>.
- This model outputs at the port <code>fluPor</code> the mass flow rate for
- each flow that is connected to <code>ports</code>, together with its
- temperature, water vapor mass fraction per total mass of the air (not per kg dry
- air), and trace substances. These quantities are always as if the flow
- enters the room, even if the flow is zero or negative.
- If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
- if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
- the output signal for these properties are removed.
- These quantities are always as if the flow
- enters the room, even if the flow is zero or negative.
- Thus, a thermal zone model that uses these signals to compute the
- heat added by the HVAC system need to implement an equation such as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
- </p>
- <p>
- where
- <i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
- <i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
- the port <code>fluPor</code> (which is negative if it is an exhaust),
- <i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
- <i>T<sub>sup</sub></i> is the supply air temperature and
- <i>T<sub>air,zon</sub></i> is the zone air temperature.
- Note that without the <i>max(&middot;, &middot;)</i>, the energy
- balance would be wrong.
- </p>
- 
- <p>
- The input signals of this model are the radiative temperature of each zone.
- The the zone air temperatures,
- the water vapor mass fractions per total mass of the air (unless <code>Medium.nXi=0</code>)
- and trace substances (unless <code>Medium.nC=0</code>) are obtained from the connector
- <code>fluPor.backward</code>.
- The outflowing fluid stream(s) at the port <code>ports</code> will be at the
- states obtained from <code>fluPor.backward</code>.
- For any given <i>i<sub>zon</sub> &isin; {1, ..., n<sub>zon</sub>}</i>,
- for each <i>i<sub>ports</sub> &isin; {1, ..., n<sub>ports</sub>}</i>
- all fluid streams at port <code>ports[i<sub>zon</sub>, i<sub>ports</sub>]</code> are at the same
- pressure.
- For convenience, the instance <code>hvacAda</code> also outputs the
- properties obtained from <code>fluPor.backward</code>. These can be used
- to connect a controller. The properties are available for each flow path in
- <code>fluPor.backward</code>. For a thermal zone with mixed air, these are
- all equal, while for a stratified room model, they can be different.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones</a>
- for a model that uses this model.
- </p>
- <p>
- For models that only have one thermal zone connected to the HVAC system,
- use the simpler model
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone</a>.
- </p>
- <h4>Assumption and limitations</h4>
- <p>
- The mass flow rates at <code>ports</code> sum to zero, hence this
- model conserves mass for each thermal zone.
- </p>
- <p>
- This model does not impose any pressure, other than,
- for any given <i>i<sub>zon</sub> &isin; {1, ..., n<sub>zon</sub>}</i> and
- for each <i>j,k &isin; {1, ..., n<sub>ports</sub>}</i>,
- setting the pressure of <code>ports[i<sub>zon</sub>, j].p = ports[i<sub>zon</sub>, k].p</code>
- to be the same.
- The reason is that setting a pressure can lead to non-physical system models,
- for example if a mass flow rate is imposed and the HVAC system is connected
- to a model that sets a pressure boundary condition such as
- <a href=\"modelica://AixLib.Fluid.Sources.Outside\">
- AixLib.Fluid.Sources.Outside</a>.
- Also, setting a pressure would make it impossible to use multiple instances
- of this model (one for each thermal zone) and build in Modelica an airflow network
- model with pressure driven mass flow rates.
- </p>
- <p>
- The model has no pressure drop. Hence, the pressure drop
- of an air diffuser or of an exhaust grill needs to be modelled
- in models that are connected to <code>ports</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- May 25, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that is used as a container for an HVAC system that is
+to be exported as an FMU and that serves multiple zones.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+To use this model as a container for an FMU, simply extend
+from this model, rather than instantiate it,
+and add your HVAC system. By extending from this model, the top-level
+signal connectors on the right stay at the top-level, and hence
+will be visible at the FMI interface.
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones</a>
+shows how a simple HVAC system that serves two rooms can be implemented and exported as
+an FMU.
+<!-- @include_Buildings
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
+AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
+shows how such an FMU can be connected
+to a room model that has signal flow.
+-->
+</p>
+<p>
+The following two parameters need to be assigned by the user:
+Set <code>nZon</code> to the number of thermal zones to which the
+FMU will be connected.
+Set <code>nPorts</code> to the largest number of fluid ports
+that the thermal zones has. For example,
+if <code>nZon=2</code> and zone <i>1</i> has one inlet and one outlet
+(hence it has 2 ports),
+and zone <i>2</i> has one inlets and two outlets
+(hence it has 3 ports), then
+set <code>nPorts=3</code>. This will add more fluid ports than are needed
+for zone <i>1</i>, but this causes no overhead if they are not connected.
+</p>
+<p>
+The conversion between the fluid ports and signal ports is done
+in the HVAC adapter <code>hvacAda</code>.
+This adapter has a vector of fluid ports called <code>ports</code>.
+The supply and return air ducts, including any resistance model for the inlet
+diffusor or exhaust grill, need to be connected to these ports.
+Also, if a thermal zone has interzonal air exchange or air infiltration,
+these flows need to be connected to <code>ports</code>.
+This model outputs at the port <code>fluPor</code> the mass flow rate for
+each flow that is connected to <code>ports</code>, together with its
+temperature, water vapor mass fraction per total mass of the air (not per kg dry
+air), and trace substances. These quantities are always as if the flow
+enters the room, even if the flow is zero or negative.
+If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
+if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
+the output signal for these properties are removed.
+These quantities are always as if the flow
+enters the room, even if the flow is zero or negative.
+Thus, a thermal zone model that uses these signals to compute the
+heat added by the HVAC system need to implement an equation such as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
+</p>
+<p>
+where
+<i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
+<i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
+the port <code>fluPor</code> (which is negative if it is an exhaust),
+<i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
+<i>T<sub>sup</sub></i> is the supply air temperature and
+<i>T<sub>air,zon</sub></i> is the zone air temperature.
+Note that without the <i>max(&middot;, &middot;)</i>, the energy
+balance would be wrong.
+</p>
+
+<p>
+The input signals of this model are the radiative temperature of each zone.
+The the zone air temperatures,
+the water vapor mass fractions per total mass of the air (unless <code>Medium.nXi=0</code>)
+and trace substances (unless <code>Medium.nC=0</code>) are obtained from the connector
+<code>fluPor.backward</code>.
+The outflowing fluid stream(s) at the port <code>ports</code> will be at the
+states obtained from <code>fluPor.backward</code>.
+For any given <i>i<sub>zon</sub> &isin; {1, ..., n<sub>zon</sub>}</i>,
+for each <i>i<sub>ports</sub> &isin; {1, ..., n<sub>ports</sub>}</i>
+all fluid streams at port <code>ports[i<sub>zon</sub>, i<sub>ports</sub>]</code> are at the same
+pressure.
+For convenience, the instance <code>hvacAda</code> also outputs the
+properties obtained from <code>fluPor.backward</code>. These can be used
+to connect a controller. The properties are available for each flow path in
+<code>fluPor.backward</code>. For a thermal zone with mixed air, these are
+all equal, while for a stratified room model, they can be different.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HVACZones</a>
+for a model that uses this model.
+</p>
+<p>
+For models that only have one thermal zone connected to the HVAC system,
+use the simpler model
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone</a>.
+</p>
+<h4>Assumption and limitations</h4>
+<p>
+The mass flow rates at <code>ports</code> sum to zero, hence this
+model conserves mass for each thermal zone.
+</p>
+<p>
+This model does not impose any pressure, other than,
+for any given <i>i<sub>zon</sub> &isin; {1, ..., n<sub>zon</sub>}</i> and
+for each <i>j,k &isin; {1, ..., n<sub>ports</sub>}</i>,
+setting the pressure of <code>ports[i<sub>zon</sub>, j].p = ports[i<sub>zon</sub>, k].p</code>
+to be the same.
+The reason is that setting a pressure can lead to non-physical system models,
+for example if a mass flow rate is imposed and the HVAC system is connected
+to a model that sets a pressure boundary condition such as
+<a href=\"modelica://AixLib.Fluid.Sources.Outside\">
+AixLib.Fluid.Sources.Outside</a>.
+Also, setting a pressure would make it impossible to use multiple instances
+of this model (one for each thermal zone) and build in Modelica an airflow network
+model with pressure driven mass flow rates.
+</p>
+<p>
+The model has no pressure drop. Hence, the pressure drop
+of an air diffuser or of an exhaust grill needs to be modelled
+in models that are connected to <code>ports</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+May 25, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACZones;
diff --git a/AixLib/Fluid/FMI/ExportContainers/PartialTwoPort.mo b/AixLib/Fluid/FMI/ExportContainers/PartialTwoPort.mo
index 03d037a44b..6dfe4e1905 100644
--- a/AixLib/Fluid/FMI/ExportContainers/PartialTwoPort.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/PartialTwoPort.mo
@@ -44,34 +44,34 @@ partial block PartialTwoPort
           fillPattern=FillPattern.HorizontalCylinder,
           fillColor={0,127,255},
           textString="%name")}),    Documentation(info="<html>
- <p>
- Partial model that can be used to export thermofluid flow models as an FMU.
- This model only declares the inlet and outlet ports, the medium and
- whether flow reversal is allowed.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume</a>
- for a block that extends this partial block.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Redesigned to conditionally remove the pressure connector
- if <code>use_p_in=false</code>.
- </li>
- <li>
- November 8, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model that can be used to export thermofluid flow models as an FMU.
+This model only declares the inlet and outlet ports, the medium and
+whether flow reversal is allowed.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume</a>
+for a block that extends this partial block.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Redesigned to conditionally remove the pressure connector
+if <code>use_p_in=false</code>.
+</li>
+<li>
+November 8, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialTwoPort;
diff --git a/AixLib/Fluid/FMI/ExportContainers/ReplaceableTwoPort.mo b/AixLib/Fluid/FMI/ExportContainers/ReplaceableTwoPort.mo
index 66eb5827fe..ad01fd5822 100644
--- a/AixLib/Fluid/FMI/ExportContainers/ReplaceableTwoPort.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/ReplaceableTwoPort.mo
@@ -59,46 +59,46 @@ equation
       color={0,0,127},
       smooth=Smooth.None));
   annotation ( Documentation(info="<html>
- <p>
- Block that serves as a container to export a thermofluid flow component.
- This block contains a replaceable model <code>com</code> that needs to
- be redeclared to export any model that has as its base class
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPort\">
- AixLib.Fluid.Interfaces.PartialTwoPort</a>.
- This allows exporting a large variety of thermofluid flow models
- with a simple redeclare.
- </p>
- <p>
- See for example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.PressureDrop\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.PressureDrop</a>
- or
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HeaterCooler_u\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HeaterCooler_u</a>
- for how to use this block.
- </p>
- <p>
- Note that this block must not be used if the instance <code>com</code>
- sets a constant pressure. In such a situation, use
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.PartialTwoPort\">
- AixLib.Fluid.FMI.ExportContainers.PartialTwoPort</a>
- together with
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Inlet\">
- AixLib.Fluid.FMI.Adaptors.Inlet</a>
- and
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Outlet\">
- AixLib.Fluid.FMI.Adaptors.Outlet</a>
- and set the pressure to be equal to the port <code>p</code> of
- <a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Outlet\">
- AixLib.Fluid.FMI.Adaptors.Outlet</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 8, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Block that serves as a container to export a thermofluid flow component.
+This block contains a replaceable model <code>com</code> that needs to
+be redeclared to export any model that has as its base class
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPort\">
+AixLib.Fluid.Interfaces.PartialTwoPort</a>.
+This allows exporting a large variety of thermofluid flow models
+with a simple redeclare.
+</p>
+<p>
+See for example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.PressureDrop\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.PressureDrop</a>
+or
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HeaterCooler_u\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HeaterCooler_u</a>
+for how to use this block.
+</p>
+<p>
+Note that this block must not be used if the instance <code>com</code>
+sets a constant pressure. In such a situation, use
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.PartialTwoPort\">
+AixLib.Fluid.FMI.ExportContainers.PartialTwoPort</a>
+together with
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Inlet\">
+AixLib.Fluid.FMI.Adaptors.Inlet</a>
+and
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Outlet\">
+AixLib.Fluid.FMI.Adaptors.Outlet</a>
+and set the pressure to be equal to the port <code>p</code> of
+<a href=\"modelica://AixLib.Fluid.FMI.Adaptors.Outlet\">
+AixLib.Fluid.FMI.Adaptors.Outlet</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReplaceableTwoPort;
diff --git a/AixLib/Fluid/FMI/ExportContainers/ThermalZone.mo b/AixLib/Fluid/FMI/ExportContainers/ThermalZone.mo
index 3070507f69..879e59b6ec 100644
--- a/AixLib/Fluid/FMI/ExportContainers/ThermalZone.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/ThermalZone.mo
@@ -57,150 +57,150 @@ equation
           fillPattern=FillPattern.Solid)}),                      Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-160,-140},{160,180}})),
     Documentation(info="<html>
- <p>
- Model that is used as a container for a single thermal zone
- that is to be exported as an FMU.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- To use this model as a container for an FMU, extend
- from this model, rather than instantiate it,
- add your thermal zone and a vector of mass flow rate sensors.
- By extending from this model, the top-level
- signal connectors on the left stay at the top-level, and hence
- will be visible at the FMI interface.
- </p>
- 
- Note that
- <ul>
- <li>
- The vector of mass flow rate sensors is used to connect
- the thermal zone adapter and your thermal zone.
- </li>
- <li>
- The vector of mass flow rate sensors must have the size <code>nPorts</code>.
- </li>
- <li>
- All fluid ports of the mass flow rate sensor must be connected.
- </li>
- <li>
- If the vector of mass flow rate sensors is not used, and your themal zone
- has fluid ports which are autosized, then a direct connection between
- the thermal zone adpater <code>theZonAda</code> and your thermal
- zone will be rejected. The reason is because autosized fluid ports
- can only be connected to vector of ports whose sizes are literal.
- </li>
- </ul>
- 
- <p>
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone</a>
- shows how a simple thermal zone can be implemented and exported as
- an FMU.
- <!-- @include_Buildings
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
- AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
- shows how such an FMU can be connected
- to an HVAC system that has signal flow.
- -->
- </p>
- 
- <p>
- The conversion between the fluid ports and signal ports is done
- in the thermal zone adapter <code>theZonAda</code>.
- This adapter has a vector of fluid ports called <code>ports[nPorts]</code>
- which needs to be connected to the air volume of the thermal zone.
- At this port, air exchanged between the thermal zone, the HVAC system
- and any infiltration flow paths.
- </p>
- <p>
- This model has input signals <code>fluPor[nPorts]</code>, which carry
- the mass flow rate for each flow that is connected to <code>ports</code>, together with its
- temperature, water vapor mass fraction per total mass of the air (not per kg dry
- air), and trace substances. These quantities are always as if the flow
- enters the room, even if the flow is zero or negative.
- If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
- if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
- the output signal for these properties are removed.
- Thus, a thermal zone model that uses these signals to compute the
- heat added by the HVAC system need to implement an equation such as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
- </p>
- <p>
- where
- <i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
- <i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
- the port <code>fluPor</code> (which is negative if it is an exhaust),
- <i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
- <i>T<sub>sup</sub></i> is the supply air temperature and
- <i>T<sub>air,zon</sub></i> is the zone air temperature.
- Note that without the <i>max(&middot;, &middot;)</i>, the energy
- balance would be wrong.
- For example,
- <!-- @include_Buildings
- models in the package
- <a href=\"modelica://AixLib.ThermalZones.Detailed\">
- AixLib.ThermalZones.Detailed</a> as well as
- -->
- the control volumes in
- <a href=\"modelica://AixLib.Fluid.MixingVolumes\">
- AixLib.Fluid.MixingVolumes</a>
- implement such a <i>max(&middot;, &middot;)</i> function.
- </p>
- <p>
- The zone air temperature,
- the water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>)
- and trace substances (unless <code>Medium.nC=0</code>)
- can be obtained from the outupt connector
- <code>fluPor.backward</code>.
- These signals are the same as the inflowing fluid stream(s)
- at the port <code>theAdaZon.ports[1:nPorts]</code>.
- The fluid connector <code>ports[nPorts]</code> has a prescribed mass flow rate, but
- it does not set any pressure.
- </p>
- <p>
- This model has a user-defined parameter <code>nPorts</code>
- which sets the number of fluid ports, which in turn is used
- for the ports <code>fluPor</code> and <code>ports</code>.
- All <code>nPorts</code>
- <code>ports[1:nPorts]</code> need to be connected as demonstrated in the example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone</a>.
- </p>
- <p>
- <!-- @include_Buildings
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
- AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
- shows conceptually how such an FMU can then be connected to a HVAC system
- that has signal flow.
- -->
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- September 20, 2016, by Thierry S. Nouidui:<br/>
- Revised documentation to explain the rationale
- of needing mass flow rate sensors.
- </li>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- Revised implementation and documentation.
- </li>
- <li>
- April 27, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that is used as a container for a single thermal zone
+that is to be exported as an FMU.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+To use this model as a container for an FMU, extend
+from this model, rather than instantiate it,
+add your thermal zone and a vector of mass flow rate sensors.
+By extending from this model, the top-level
+signal connectors on the left stay at the top-level, and hence
+will be visible at the FMI interface.
+</p>
+
+Note that
+<ul>
+<li>
+The vector of mass flow rate sensors is used to connect
+the thermal zone adapter and your thermal zone.
+</li>
+<li>
+The vector of mass flow rate sensors must have the size <code>nPorts</code>.
+</li>
+<li>
+All fluid ports of the mass flow rate sensor must be connected.
+</li>
+<li>
+If the vector of mass flow rate sensors is not used, and your themal zone
+has fluid ports which are autosized, then a direct connection between
+the thermal zone adpater <code>theZonAda</code> and your thermal
+zone will be rejected. The reason is because autosized fluid ports
+can only be connected to vector of ports whose sizes are literal.
+</li>
+</ul>
+
+<p>
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone</a>
+shows how a simple thermal zone can be implemented and exported as
+an FMU.
+<!-- @include_Buildings
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
+AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
+shows how such an FMU can be connected
+to an HVAC system that has signal flow.
+-->
+</p>
+
+<p>
+The conversion between the fluid ports and signal ports is done
+in the thermal zone adapter <code>theZonAda</code>.
+This adapter has a vector of fluid ports called <code>ports[nPorts]</code>
+which needs to be connected to the air volume of the thermal zone.
+At this port, air exchanged between the thermal zone, the HVAC system
+and any infiltration flow paths.
+</p>
+<p>
+This model has input signals <code>fluPor[nPorts]</code>, which carry
+the mass flow rate for each flow that is connected to <code>ports</code>, together with its
+temperature, water vapor mass fraction per total mass of the air (not per kg dry
+air), and trace substances. These quantities are always as if the flow
+enters the room, even if the flow is zero or negative.
+If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
+if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
+the output signal for these properties are removed.
+Thus, a thermal zone model that uses these signals to compute the
+heat added by the HVAC system need to implement an equation such as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
+</p>
+<p>
+where
+<i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
+<i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
+the port <code>fluPor</code> (which is negative if it is an exhaust),
+<i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
+<i>T<sub>sup</sub></i> is the supply air temperature and
+<i>T<sub>air,zon</sub></i> is the zone air temperature.
+Note that without the <i>max(&middot;, &middot;)</i>, the energy
+balance would be wrong.
+For example,
+<!-- @include_Buildings
+models in the package
+<a href=\"modelica://AixLib.ThermalZones.Detailed\">
+AixLib.ThermalZones.Detailed</a> as well as
+-->
+the control volumes in
+<a href=\"modelica://AixLib.Fluid.MixingVolumes\">
+AixLib.Fluid.MixingVolumes</a>
+implement such a <i>max(&middot;, &middot;)</i> function.
+</p>
+<p>
+The zone air temperature,
+the water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>)
+and trace substances (unless <code>Medium.nC=0</code>)
+can be obtained from the outupt connector
+<code>fluPor.backward</code>.
+These signals are the same as the inflowing fluid stream(s)
+at the port <code>theAdaZon.ports[1:nPorts]</code>.
+The fluid connector <code>ports[nPorts]</code> has a prescribed mass flow rate, but
+it does not set any pressure.
+</p>
+<p>
+This model has a user-defined parameter <code>nPorts</code>
+which sets the number of fluid ports, which in turn is used
+for the ports <code>fluPor</code> and <code>ports</code>.
+All <code>nPorts</code>
+<code>ports[1:nPorts]</code> need to be connected as demonstrated in the example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZone</a>.
+</p>
+<p>
+<!-- @include_Buildings
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
+AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
+shows conceptually how such an FMU can then be connected to a HVAC system
+that has signal flow.
+-->
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+September 20, 2016, by Thierry S. Nouidui:<br/>
+Revised documentation to explain the rationale
+of needing mass flow rate sensors.
+</li>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+Revised implementation and documentation.
+</li>
+<li>
+April 27, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZone;
diff --git a/AixLib/Fluid/FMI/ExportContainers/ThermalZones.mo b/AixLib/Fluid/FMI/ExportContainers/ThermalZones.mo
index d0457a7f55..b7cc3a7002 100644
--- a/AixLib/Fluid/FMI/ExportContainers/ThermalZones.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/ThermalZones.mo
@@ -91,157 +91,157 @@ equation
           textColor={0,0,127},
           textString="[%nZon, %nPorts]")}),
     Documentation(info="<html>
-     <p>
- Model that is used as a container for a multiple thermal zones
- that are to be exported as an FMU.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- To use this model as a container for an FMU, extend
- from this model, rather than instantiate it,
- add your thermal zones. For each thermal zone,
- add a vector of mass flow rate sensors.
- By extending from this model, the top-level
- signal connectors on the left stay at the top-level, and hence
- will be visible at the FMI interface.
- </p>
- 
- Note that
- <ul>
- <li>
- A vector of mass flow rate sensors is used to connect
- one element of the thermal zone adapter with one thermal zone.
- </li>
- <li>
- The size of the thermal zone adapter must be the same as the number
- of vectors of mass flow rate sensors.
- </li>
- <li>
- The vector of mass flow rate sensors must have the size <code>nPorts</code>.
- </li>
- <li>
- All fluid ports of the mass flow rate sensor must be connected.
- </li>
- <li>
- If mass flow rate sensors are not used, and your themal zone
- has fluid ports which are autosized, then a direct connection between
- an element of the thermal zone adpater <code>theZonAda</code> and your thermal
- zone will be rejected. The reason is because autosized fluid ports
- can only be connected to vector of ports whose sizes are literal.
- </li>
- </ul>
- 
- <p>
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZones\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZones</a>
- shows how multiple simple thermal zones can be implemented and exported as
- an FMU.
- <!-- @include_Buildings
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
- AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
- shows how such an FMU can be connected
- to an HVAC system that has signal flow.
- -->
- </p>
- 
- <p>
- The conversion between the fluid ports and signal ports is done
- in the thermal zone adapter <code>theZonAda[nZon]</code>.
- This adapter has a vector of fluid ports called <code>ports[nPorts]</code>
- which needs to be connected to the air volume of the thermal zones.
- At this port, air exchanged between the thermal zones, the HVAC system
- and any infiltration flow paths.
- </p>
- <p>
- This model has input signals <code>fluPor[nZon, nPorts]</code> which carry
- the mass flow rate for each flow that is connected to <code>ports[1:nPorts]</code>
- for the respective zone, together with its
- temperature, water vapor mass fraction per total mass of the air (not per kg dry
- air), and trace substances. These quantities are always as if the flow
- enters the respective room, even if the flow is zero or negative.
- If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
- if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
- the output signal for these properties are removed.
- Thus, a thermal zone model that uses these signals to compute the
- heat added by the HVAC system need to implement an equation such as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
- </p>
- <p>
- where
- <i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
- <i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
- the port <code>fluPor</code> (which is negative if it is an exhaust),
- <i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
- <i>T<sub>sup</sub></i> is the supply air temperature and
- <i>T<sub>air,zon</sub></i> is the zone air temperature.
- Note that without the <i>max(&middot;, &middot;)</i>, the energy
- balance would be wrong.
- For example,
- <!-- @include_Buildings
- models in the package
- <a href=\"modelica://AixLib.ThermalZones.Detailed\">
- AixLib.ThermalZones.Detailed</a> as well as
- -->
- the control volumes in
- <a href=\"modelica://AixLib.Fluid.MixingVolumes\">
- AixLib.Fluid.MixingVolumes</a>
- implement such a <i>max(&middot;, &middot;)</i> function.
- </p>
- <p>
- For each zone, its air temperature,
- water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>)
- and trace substances (unless <code>Medium.nC=0</code>)
- can be obtained from the outupt connector
- <code>fluPor[1:nZon].backward</code>.
- These signals are the same as the inflowing fluid stream(s)
- at the port <code>theAdaZon[1:nZon].ports[1:nPorts]</code>.
- The fluid connector <code>ports[nPorts]</code> has a prescribed mass flow rate, but
- it does not set any pressure.
- </p>
- <p>
- This model has a user-defined parameter <code>nPorts</code>
- which sets the number of fluid ports, which in turn is used
- for the ports <code>fluPor</code> and <code>ports</code>.
- All zones must have the same number of fluid ports <code>nPorts</code>.
- All <code>nPorts</code>
- <code>ports[1:nPorts]</code> need to be connected as demonstrated in the example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZones\">
- AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZones</a>.
- </p>
- <p>
- <!-- @include_Buildings
- The example
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
- AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
- shows conceptually how such an FMU can then be connected to a HVAC system
- that has signal flow.
- -->
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- September 20, 2016, by Thierry S. Nouidui:<br/>
- Revised documentation to explain the rationale
- of needing mass flow rate sensors.
- </li>
- <li>
- June 29, 2016, by Michael Wetter:<br/>
- Revised implementation and documentation.
- </li>
- <li>
- April 27, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+    <p>
+Model that is used as a container for a multiple thermal zones
+that are to be exported as an FMU.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+To use this model as a container for an FMU, extend
+from this model, rather than instantiate it,
+add your thermal zones. For each thermal zone,
+add a vector of mass flow rate sensors.
+By extending from this model, the top-level
+signal connectors on the left stay at the top-level, and hence
+will be visible at the FMI interface.
+</p>
+
+Note that
+<ul>
+<li>
+A vector of mass flow rate sensors is used to connect
+one element of the thermal zone adapter with one thermal zone.
+</li>
+<li>
+The size of the thermal zone adapter must be the same as the number
+of vectors of mass flow rate sensors.
+</li>
+<li>
+The vector of mass flow rate sensors must have the size <code>nPorts</code>.
+</li>
+<li>
+All fluid ports of the mass flow rate sensor must be connected.
+</li>
+<li>
+If mass flow rate sensors are not used, and your themal zone
+has fluid ports which are autosized, then a direct connection between
+an element of the thermal zone adpater <code>theZonAda</code> and your thermal
+zone will be rejected. The reason is because autosized fluid ports
+can only be connected to vector of ports whose sizes are literal.
+</li>
+</ul>
+
+<p>
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZones\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZones</a>
+shows how multiple simple thermal zones can be implemented and exported as
+an FMU.
+<!-- @include_Buildings
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
+AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
+shows how such an FMU can be connected
+to an HVAC system that has signal flow.
+-->
+</p>
+
+<p>
+The conversion between the fluid ports and signal ports is done
+in the thermal zone adapter <code>theZonAda[nZon]</code>.
+This adapter has a vector of fluid ports called <code>ports[nPorts]</code>
+which needs to be connected to the air volume of the thermal zones.
+At this port, air exchanged between the thermal zones, the HVAC system
+and any infiltration flow paths.
+</p>
+<p>
+This model has input signals <code>fluPor[nZon, nPorts]</code> which carry
+the mass flow rate for each flow that is connected to <code>ports[1:nPorts]</code>
+for the respective zone, together with its
+temperature, water vapor mass fraction per total mass of the air (not per kg dry
+air), and trace substances. These quantities are always as if the flow
+enters the respective room, even if the flow is zero or negative.
+If a medium has no moisture, e.g., if <code>Medium.nXi=0</code>, or
+if it has no trace substances, e.g., if <code>Medium.nC=0</code>, then
+the output signal for these properties are removed.
+Thus, a thermal zone model that uses these signals to compute the
+heat added by the HVAC system need to implement an equation such as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>sen</sub> = max(0, &#7745;<sub>sup</sub>) &nbsp; c<sub>p</sub> &nbsp; (T<sub>sup</sub> - T<sub>air,zon</sub>),
+</p>
+<p>
+where
+<i>Q<sub>sen</sub></i> is the sensible heat flow rate added to the thermal zone,
+<i>&#7745;<sub>sup</sub></i> is the supply air mass flow rate from
+the port <code>fluPor</code> (which is negative if it is an exhaust),
+<i>c<sub>p</sub></i> is the specific heat capacity at constant pressure,
+<i>T<sub>sup</sub></i> is the supply air temperature and
+<i>T<sub>air,zon</sub></i> is the zone air temperature.
+Note that without the <i>max(&middot;, &middot;)</i>, the energy
+balance would be wrong.
+For example,
+<!-- @include_Buildings
+models in the package
+<a href=\"modelica://AixLib.ThermalZones.Detailed\">
+AixLib.ThermalZones.Detailed</a> as well as
+-->
+the control volumes in
+<a href=\"modelica://AixLib.Fluid.MixingVolumes\">
+AixLib.Fluid.MixingVolumes</a>
+implement such a <i>max(&middot;, &middot;)</i> function.
+</p>
+<p>
+For each zone, its air temperature,
+water vapor mass fraction per total mass of the air (unless <code>Medium.nXi=0</code>)
+and trace substances (unless <code>Medium.nC=0</code>)
+can be obtained from the outupt connector
+<code>fluPor[1:nZon].backward</code>.
+These signals are the same as the inflowing fluid stream(s)
+at the port <code>theAdaZon[1:nZon].ports[1:nPorts]</code>.
+The fluid connector <code>ports[nPorts]</code> has a prescribed mass flow rate, but
+it does not set any pressure.
+</p>
+<p>
+This model has a user-defined parameter <code>nPorts</code>
+which sets the number of fluid ports, which in turn is used
+for the ports <code>fluPor</code> and <code>ports</code>.
+All zones must have the same number of fluid ports <code>nPorts</code>.
+All <code>nPorts</code>
+<code>ports[1:nPorts]</code> need to be connected as demonstrated in the example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZones\">
+AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ThermalZones</a>.
+</p>
+<p>
+<!-- @include_Buildings
+The example
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC\">
+AixLib.Fluid.FMI.ExportContainers.Validation.RoomHVAC</a>
+shows conceptually how such an FMU can then be connected to a HVAC system
+that has signal flow.
+-->
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+September 20, 2016, by Thierry S. Nouidui:<br/>
+Revised documentation to explain the rationale
+of needing mass flow rate sensors.
+</li>
+<li>
+June 29, 2016, by Michael Wetter:<br/>
+Revised implementation and documentation.
+</li>
+<li>
+April 27, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZones;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir1.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir1.mo
index edde246825..55bafb6066 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir1.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir1.mo
@@ -48,21 +48,21 @@ equation
     annotation (Line(points={{40,140},{50,140},{60,140}}, color={0,127,255}));
 annotation (
     Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir1.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACThermalZoneAir1;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir2.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir2.mo
index ef4dff3ad6..cfdbaf17cc 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir2.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir2.mo
@@ -4,21 +4,21 @@ block HVACThermalZoneAir2 "Validation model for the convective HVAC system"
     redeclare package Medium = AixLib.Media.Air(extraPropertiesNames={"CO2"}));
 annotation (
     Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir2.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACThermalZoneAir2;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir3.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir3.mo
index 15c67cbc5e..b3d0ff2f8a 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir3.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir3.mo
@@ -4,21 +4,21 @@ block HVACThermalZoneAir3 "Validation model for the convective HVAC system"
     redeclare package Medium = AixLib.Media.Air(extraPropertiesNames={"CO2", "VOC", "CH2O"}));
 annotation (
     Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneAir3.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACThermalZoneAir3;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir1.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir1.mo
index 0a2b67dba5..5ba84bf70d 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir1.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir1.mo
@@ -5,21 +5,21 @@ block HVACThermalZoneSimpleAir1
     redeclare package Medium = Modelica.Media.Air.SimpleAir);
 annotation (
     Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir1.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACThermalZoneSimpleAir1;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir2.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir2.mo
index 76a04c3d3f..44e848e654 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir2.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir2.mo
@@ -5,21 +5,21 @@ block HVACThermalZoneSimpleAir2
     redeclare package Medium = Modelica.Media.Air.SimpleAir(extraPropertiesNames={"CO2"}));
 annotation (
     Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir2.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACThermalZoneSimpleAir2;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir3.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir3.mo
index 14e68f334e..556fd8ad42 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir3.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir3.mo
@@ -5,21 +5,21 @@ block HVACThermalZoneSimpleAir3
     redeclare package Medium = Modelica.Media.Air.SimpleAir(extraPropertiesNames={"CO2", "VOC", "CH2O"}));
 annotation (
     Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
- AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2016 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.HVACZone\">
+AixLib.Fluid.FMI.ExportContainers.HVACZone</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2016 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/HVACThermalZoneSimpleAir3.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HVACThermalZoneSimpleAir3;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir1.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir1.mo
index e6e9fa61fb..bf38d065e2 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir1.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir1.mo
@@ -107,27 +107,27 @@ equation
           textString="TOut")}),                                  Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-160,-140},{160,180}})),
     Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZone
- </a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 20, 2016, by Thierry S. Nouidui:<br/>
- Revised implementation and added mass flow rate sensors
- to connect the thermal zone adaptor to the thermal zone.
- </li>
- <li>
- April 28, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZone
+</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 20, 2016, by Thierry S. Nouidui:<br/>
+Revised implementation and added mass flow rate sensors
+to connect the thermal zone adaptor to the thermal zone.
+</li>
+<li>
+April 28, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir1.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZoneAir1;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir2.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir2.mo
index c2cfc2ed2c..373c5a530a 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir2.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir2.mo
@@ -3,22 +3,22 @@ block ThermalZoneAir2 "Validation of simple thermal zone"
   extends AixLib.Fluid.FMI.ExportContainers.Validation.FMUs.ThermalZoneAir1(
     redeclare package Medium = AixLib.Media.Air(extraPropertiesNames={"CO2"}));
   annotation (Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZone
- </a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 03, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZone
+</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 03, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir2.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZoneAir2;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir3.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir3.mo
index de973f2163..0b2b95b04f 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir3.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir3.mo
@@ -3,22 +3,22 @@ block ThermalZoneAir3 "Validation of simple thermal zone"
   extends AixLib.Fluid.FMI.ExportContainers.Validation.FMUs.ThermalZoneAir1(
     redeclare package Medium = AixLib.Media.Air(extraPropertiesNames={"CO2", "VOC", "CH2O"}));
   annotation (Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZone
- </a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 03, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZone
+</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 03, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneAir3.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZoneAir3;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir1.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir1.mo
index f5ee900d82..a750d9227a 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir1.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir1.mo
@@ -3,22 +3,22 @@ block ThermalZoneSimpleAir1 "Validation of simple thermal zone"
   extends AixLib.Fluid.FMI.ExportContainers.Validation.FMUs.ThermalZoneAir1(
     redeclare package Medium = Modelica.Media.Air.SimpleAir);
   annotation (Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZone
- </a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 03, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZone
+</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 03, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir1.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZoneSimpleAir1;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir2.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir2.mo
index cba9f6deab..029cd4de44 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir2.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir2.mo
@@ -3,22 +3,22 @@ block ThermalZoneSimpleAir2 "Validation of simple thermal zone"
   extends AixLib.Fluid.FMI.ExportContainers.Validation.FMUs.ThermalZoneAir1(
     redeclare package Medium = Modelica.Media.Air.SimpleAir(extraPropertiesNames={"CO2"}));
   annotation (Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZone
- </a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 03, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZone
+</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 03, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir2.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZoneSimpleAir2;
diff --git a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir3.mo b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir3.mo
index ee47f57ce3..1e274478ee 100644
--- a/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir3.mo
+++ b/AixLib/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir3.mo
@@ -3,22 +3,22 @@ block ThermalZoneSimpleAir3 "Validation of simple thermal zone"
   extends AixLib.Fluid.FMI.ExportContainers.Validation.FMUs.ThermalZoneAir1(
     redeclare package Medium = Modelica.Media.Air.SimpleAir(extraPropertiesNames={"CO2", "VOC", "CH2O"}));
   annotation (Documentation(info="<html>
- <p>
- This example validates that
- <a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
- AixLib.Fluid.FMI.ExportContainers.ThermalZone
- </a>
- exports correctly as an FMU.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 03, 2016, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example validates that
+<a href=\"modelica://AixLib.Fluid.FMI.ExportContainers.ThermalZone\">
+AixLib.Fluid.FMI.ExportContainers.ThermalZone
+</a>
+exports correctly as an FMU.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 03, 2016, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/ExportContainers/Validation/FMUs/ThermalZoneSimpleAir3.mos"
-        "Export FMU"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Export FMU"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermalZoneSimpleAir3;
diff --git a/AixLib/Fluid/FMI/FlowSplitter_u.mo b/AixLib/Fluid/FMI/FlowSplitter_u.mo
index 35e7a2f8a2..8b77b552d1 100644
--- a/AixLib/Fluid/FMI/FlowSplitter_u.mo
+++ b/AixLib/Fluid/FMI/FlowSplitter_u.mo
@@ -44,10 +44,10 @@ protected
   final parameter Modelica.Units.SI.MassFlowRate mAve_flow_nominal=sum(
       m_flow_nominal)/nout "Average nominal mass flow rate";
 protected
-  AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
+  input AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
     redeclare final package Medium = Medium)
     "Internal connector for fluid properties for back flow";
-  AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_out_internal = 0
+  output AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_out_internal = 0
     "Internal connector for mass fraction of backward flow properties";
 
 initial equation
@@ -127,60 +127,65 @@ Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
           fillPattern=FillPattern.HorizontalCylinder)}),
     Documentation(
 info="<html>
- <p>
- Block that takes as an input the inflowing fluid at the port <code>inlet</code>
- and a vector of control signals for the mass flow rates <code>u</code>.
- The mass flow of all outlet ports <code>i</code>
- is set to the value of <code>u[i] m_flow_nominal[i]</code>.
- If the inflowing mass flow rate at the port <code>inlet</code> is not equal
- to the sum of <code>u[i] m_flow_in[i]</code>, the simulation stops with an assert.
- </p>
- <h4>Assumptions and limitations</h4>
- <p>
- The mass flow rates at all outlet ports must be non-negative.
- Reverse flow is not yet implemented.
- If either of these limitations are violated, then
- the model stops with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- June 9, 2016, by Thierry S. Nouidui:<br/>
- Removed <code>assert()</code> statement which was triggered
- when the model was exported as an FMU
- depending on the execution sequence of the master algorithm.
- </li>
- <li>
- May 27, 2016, by Michael Wetter:<br/>
- Replaced <code>outlet[i].forward = inlet.forward;</code>
- with a <code>connect</code> statement as
- accesses to composite components other than records are not allowed.
- This was done for JModelica compliance.
- </li>
- <li>
- July 28, 2015, by Thierry S. Nouidui:<br/>
- Corrected wrong <code>assert</code> statement.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Redesigned to conditionally remove the pressure connector
- if <code>use_p_in=false</code>.
- </li>
- <li>
- April 15, 2015 by Michael Wetter:<br/>
- Changed connector variable to be temperature instead of
- specific enthalpy.
- </li>
- <li>
- November 20, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Block that takes as an input the inflowing fluid at the port <code>inlet</code>
+and a vector of control signals for the mass flow rates <code>u</code>.
+The mass flow of all outlet ports <code>i</code>
+is set to the value of <code>u[i] m_flow_nominal[i]</code>.
+If the inflowing mass flow rate at the port <code>inlet</code> is not equal
+to the sum of <code>u[i] m_flow_in[i]</code>, the simulation stops with an assert.
+</p>
+<h4>Assumptions and limitations</h4>
+<p>
+The mass flow rates at all outlet ports must be non-negative.
+Reverse flow is not yet implemented.
+If either of these limitations are violated, then
+the model stops with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 18, 2024, by Michael Wetter:<br/>
+Added causality.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1853\">IBPSA, #1853</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+June 9, 2016, by Thierry S. Nouidui:<br/>
+Removed <code>assert()</code> statement which was triggered
+when the model was exported as an FMU
+depending on the execution sequence of the master algorithm.
+</li>
+<li>
+May 27, 2016, by Michael Wetter:<br/>
+Replaced <code>outlet[i].forward = inlet.forward;</code>
+with a <code>connect</code> statement as
+accesses to composite components other than records are not allowed.
+This was done for JModelica compliance.
+</li>
+<li>
+July 28, 2015, by Thierry S. Nouidui:<br/>
+Corrected wrong <code>assert</code> statement.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Redesigned to conditionally remove the pressure connector
+if <code>use_p_in=false</code>.
+</li>
+<li>
+April 15, 2015 by Michael Wetter:<br/>
+Changed connector variable to be temperature instead of
+specific enthalpy.
+</li>
+<li>
+November 20, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowSplitter_u;
diff --git a/AixLib/Fluid/FMI/Interfaces/FluidProperties.mo b/AixLib/Fluid/FMI/Interfaces/FluidProperties.mo
index a4e24acff3..ff64bec95c 100644
--- a/AixLib/Fluid/FMI/Interfaces/FluidProperties.mo
+++ b/AixLib/Fluid/FMI/Interfaces/FluidProperties.mo
@@ -18,56 +18,56 @@ connector FluidProperties "Type definition for fluid properties"
   Medium.ExtraProperty C[Medium.nC] "Properties c_i/m";
 
   annotation (Documentation(info="<html>
- <p>
- This is a connector that declares the following fluid properties:
- </p>
- <ul>
- <li>
- The temperature <code>T</code>.
- </li>
- <li>
- The mass fraction of water vapor <code>X_w</code> per kg of total air,
- unless <code>Medium.nXi=0</code>.
- Note that the mass fraction is not per kg of dry air, but rather
- per kg of total air as is customary in Modelica.
- </li>
- <li>
- The trace substances
- <code>C</code>,
- unless <code>Medium.nC=0</code>.
- </li>
- </ul>
- <p>
- These quantities are used in the connectors
- <a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Inlet\">
- AixLib.Fluid.FMI.Interfaces.Inlet</a>
- and
- <a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Outlet\">
- AixLib.Fluid.FMI.Interfaces.Outlet</a>.
- </p>
- <p>
- Note that none of these quantities is declared to be an
- <code>input</code> or <code>output</code>, because the role
- is reversed whether the properties are in inlet or
- outlet connector.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- April 15, 2015 by Michael Wetter:<br/>
- Changed connector variable to be temperature instead of
- specific enthalpy.
- </li>
- <li>
- November 8, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a connector that declares the following fluid properties:
+</p>
+<ul>
+<li>
+The temperature <code>T</code>.
+</li>
+<li>
+The mass fraction of water vapor <code>X_w</code> per kg of total air,
+unless <code>Medium.nXi=0</code>.
+Note that the mass fraction is not per kg of dry air, but rather
+per kg of total air as is customary in Modelica.
+</li>
+<li>
+The trace substances
+<code>C</code>,
+unless <code>Medium.nC=0</code>.
+</li>
+</ul>
+<p>
+These quantities are used in the connectors
+<a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Inlet\">
+AixLib.Fluid.FMI.Interfaces.Inlet</a>
+and
+<a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Outlet\">
+AixLib.Fluid.FMI.Interfaces.Outlet</a>.
+</p>
+<p>
+Note that none of these quantities is declared to be an
+<code>input</code> or <code>output</code>, because the role
+is reversed whether the properties are in inlet or
+outlet connector.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+April 15, 2015 by Michael Wetter:<br/>
+Changed connector variable to be temperature instead of
+specific enthalpy.
+</li>
+<li>
+November 8, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FluidProperties;
diff --git a/AixLib/Fluid/FMI/Interfaces/Inlet.mo b/AixLib/Fluid/FMI/Interfaces/Inlet.mo
index a0c587a5bd..568123539a 100644
--- a/AixLib/Fluid/FMI/Interfaces/Inlet.mo
+++ b/AixLib/Fluid/FMI/Interfaces/Inlet.mo
@@ -43,81 +43,81 @@ annotation (defaultComponentName="inlet",
           textColor={0,0,255},
           textString="%name")}),
     Documentation(info="<html>
- <p>
- This is a connector for a fluid inlet.
- The connector takes as an input the
- following quantities:
- </p>
- <ul>
- <li>
- The mass flow rate <code>m_flow</code>.
- </li>
- <li>
- The pressure <code>p</code>,
- unless <code>use_p_in=false</code>.
- </li>
- <li>
- The temperature of the inflowing fluid
- <code>forward.T</code>,
- e.g., the temperature of the fluid that streams out of the component if <code>m_flow &gt; 0</code>.
- </li>
- <li>
- The mass fraction of the inflowing fluid
- <code>forward.Xi</code>,
- unless <code>Medium.nXi=0</code>.
- </li>
- <li>
- The trace substances of the inflowing fluid
- <code>forward.C</code>,
- unless <code>Medium.nC=0</code>.
- </li>
- </ul>
- <p>
- If <code>allowFlowReversal = true</code>,
- the connector also outputs the following quantities.
- </p>
- <ul>
- <li>
- The temperature of the outflowing fluid
- <code>backward.T</code>,
- e.g., if <code>m_flow &le; 0</code>.
- </li>
- <li>
- The mass fraction of the outflowing fluid
- <code>backward.Xi</code>,
- unless <code>Medium.nXi=0</code>.
- </li>
- <li>
- The trace substances of the outflowing fluid
- <code>backward.C</code>,
- unless <code>Medium.nC=0</code>.
- </li>
- </ul>
- <p>
- If <code>allowFlowReversal = false</code>, then these outputs are not present.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Redesigned to conditionally remove the pressure connector
- if <code>use_p_in=false</code>.
- </li>
- <li>
- April 15, 2015 by Michael Wetter:<br/>
- Changed connector variable to be temperature instead of
- specific enthalpy.
- </li>
- <li>
- November 8, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a connector for a fluid inlet.
+The connector takes as an input the
+following quantities:
+</p>
+<ul>
+<li>
+The mass flow rate <code>m_flow</code>.
+</li>
+<li>
+The pressure <code>p</code>,
+unless <code>use_p_in=false</code>.
+</li>
+<li>
+The temperature of the inflowing fluid
+<code>forward.T</code>,
+e.g., the temperature of the fluid that streams out of the component if <code>m_flow &gt; 0</code>.
+</li>
+<li>
+The mass fraction of the inflowing fluid
+<code>forward.Xi</code>,
+unless <code>Medium.nXi=0</code>.
+</li>
+<li>
+The trace substances of the inflowing fluid
+<code>forward.C</code>,
+unless <code>Medium.nC=0</code>.
+</li>
+</ul>
+<p>
+If <code>allowFlowReversal = true</code>,
+the connector also outputs the following quantities.
+</p>
+<ul>
+<li>
+The temperature of the outflowing fluid
+<code>backward.T</code>,
+e.g., if <code>m_flow &le; 0</code>.
+</li>
+<li>
+The mass fraction of the outflowing fluid
+<code>backward.Xi</code>,
+unless <code>Medium.nXi=0</code>.
+</li>
+<li>
+The trace substances of the outflowing fluid
+<code>backward.C</code>,
+unless <code>Medium.nC=0</code>.
+</li>
+</ul>
+<p>
+If <code>allowFlowReversal = false</code>, then these outputs are not present.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Redesigned to conditionally remove the pressure connector
+if <code>use_p_in=false</code>.
+</li>
+<li>
+April 15, 2015 by Michael Wetter:<br/>
+Changed connector variable to be temperature instead of
+specific enthalpy.
+</li>
+<li>
+November 8, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Inlet;
diff --git a/AixLib/Fluid/FMI/Interfaces/MassFractionConnector.mo b/AixLib/Fluid/FMI/Interfaces/MassFractionConnector.mo
index 3d6c1e1070..d8c22e9d8c 100644
--- a/AixLib/Fluid/FMI/Interfaces/MassFractionConnector.mo
+++ b/AixLib/Fluid/FMI/Interfaces/MassFractionConnector.mo
@@ -18,25 +18,25 @@ connector MassFractionConnector =
       extent={{-10.0,60.0},{-10.0,85.0}},
       textString="%name")}),
   Documentation(info="<html>
- <p>
- Connector with variable of type <code>Modelica.Units.SI.MassFraction</code>.
- Note that the mass fraction is in kg water vapor per total mass
- of air, rathern than per kg of dry air.
- </p>
- <p>
- This connector has been implemented to conditionally remove
- the mass fraction if the medium has only one species.
- While this could have been done using a vector of mass fractions
- with zero length, as is used in fluid connectors,
- this implemantation uses a scalar to avoid vectorized inputs
- and outputs of FMUs.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 29,2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Connector with variable of type <code>Modelica.Units.SI.MassFraction</code>.
+Note that the mass fraction is in kg water vapor per total mass
+of air, rathern than per kg of dry air.
+</p>
+<p>
+This connector has been implemented to conditionally remove
+the mass fraction if the medium has only one species.
+While this could have been done using a vector of mass fractions
+with zero length, as is used in fluid connectors,
+this implemantation uses a scalar to avoid vectorized inputs
+and outputs of FMUs.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 29,2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/FMI/Interfaces/Outlet.mo b/AixLib/Fluid/FMI/Interfaces/Outlet.mo
index f8650f7ec0..8b661bf7f7 100644
--- a/AixLib/Fluid/FMI/Interfaces/Outlet.mo
+++ b/AixLib/Fluid/FMI/Interfaces/Outlet.mo
@@ -44,82 +44,82 @@ connector Outlet "Connector for fluid outlet"
           textColor={0,0,255},
           textString="%name")}),
     Documentation(info="<html>
- <p>
- This is a connector for a fluid outlet.
- The connector produces as an output the
- following quantities:
- </p>
- <ul>
- <li>
- The mass flow rate <code>m_flow</code>.
- </li>
- <li>
- The pressure <code>p</code>,
- unless <code>use_p_in=false</code>.
- </li>
- <li>
- The temperature of the inflowing fluid
- <code>forward.T</code>,
- e.g., the temperature of the fluid that streams out of the component if <code>m_flow &gt; 0</code>.
- </li>
- <li>
- The mass fraction of the inflowing fluid
- <code>forward.Xi</code>,
- unless <code>Medium.nXi=0</code>.
- </li>
- <li>
- The trace substances of the inflowing fluid
- <code>forward.C</code>,
- unless <code>Medium.nC=0</code>.
- </li>
- </ul>
- <p>
- If <code>allowFlowReversal = true</code>,
- the connector requires as input the following quantities.
- </p>
- <ul>
- <li>
- The temperature of the outflowing fluid
- <code>backward.T</code>,
- e.g., if <code>m_flow &le; 0</code>.
- </li>
- <li>
- The mass fraction of the outflowing fluid
- <code>backward.Xi</code>,
- unless <code>Medium.nXi=0</code>.
- </li>
- <li>
- The trace substances of the outflowing fluid
- <code>backward.C</code>,
- unless <code>Medium.nC=0</code>.
- </li>
- </ul>
- <p>
- If <code>allowFlowReversal = false</code>, then these inputs are not present
- and hence not required to be provided.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Redesigned to conditionally remove the pressure connector
- if <code>use_p_in=false</code>.
- </li>
- <li>
- April 15, 2015 by Michael Wetter:<br/>
- Changed connector variable to be temperature instead of
- specific enthalpy.
- </li>
- <li>
- November 8, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a connector for a fluid outlet.
+The connector produces as an output the
+following quantities:
+</p>
+<ul>
+<li>
+The mass flow rate <code>m_flow</code>.
+</li>
+<li>
+The pressure <code>p</code>,
+unless <code>use_p_in=false</code>.
+</li>
+<li>
+The temperature of the inflowing fluid
+<code>forward.T</code>,
+e.g., the temperature of the fluid that streams out of the component if <code>m_flow &gt; 0</code>.
+</li>
+<li>
+The mass fraction of the inflowing fluid
+<code>forward.Xi</code>,
+unless <code>Medium.nXi=0</code>.
+</li>
+<li>
+The trace substances of the inflowing fluid
+<code>forward.C</code>,
+unless <code>Medium.nC=0</code>.
+</li>
+</ul>
+<p>
+If <code>allowFlowReversal = true</code>,
+the connector requires as input the following quantities.
+</p>
+<ul>
+<li>
+The temperature of the outflowing fluid
+<code>backward.T</code>,
+e.g., if <code>m_flow &le; 0</code>.
+</li>
+<li>
+The mass fraction of the outflowing fluid
+<code>backward.Xi</code>,
+unless <code>Medium.nXi=0</code>.
+</li>
+<li>
+The trace substances of the outflowing fluid
+<code>backward.C</code>,
+unless <code>Medium.nC=0</code>.
+</li>
+</ul>
+<p>
+If <code>allowFlowReversal = false</code>, then these inputs are not present
+and hence not required to be provided.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Redesigned to conditionally remove the pressure connector
+if <code>use_p_in=false</code>.
+</li>
+<li>
+April 15, 2015 by Michael Wetter:<br/>
+Changed connector variable to be temperature instead of
+specific enthalpy.
+</li>
+<li>
+November 8, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outlet;
diff --git a/AixLib/Fluid/FMI/Interfaces/PressureInput.mo b/AixLib/Fluid/FMI/Interfaces/PressureInput.mo
index 6a066c901f..23c9a5963a 100644
--- a/AixLib/Fluid/FMI/Interfaces/PressureInput.mo
+++ b/AixLib/Fluid/FMI/Interfaces/PressureInput.mo
@@ -29,17 +29,17 @@ connector PressureInput =
       extent={{-10.0,60.0},{-10.0,85.0}},
       textString="%name")}),
   Documentation(info="<html>
- <p>
- Connector with one input signal of type <code>Modelica.Units.SI.AbsolutePressure</code>.
- This connector has been implemented to conditionally remove
- the pressure if no pressure drop calculation is requested.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 29,2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Connector with one input signal of type <code>Modelica.Units.SI.AbsolutePressure</code>.
+This connector has been implemented to conditionally remove
+the pressure if no pressure drop calculation is requested.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 29,2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/FMI/Interfaces/PressureOutput.mo b/AixLib/Fluid/FMI/Interfaces/PressureOutput.mo
index bd44b56015..43e969be74 100644
--- a/AixLib/Fluid/FMI/Interfaces/PressureOutput.mo
+++ b/AixLib/Fluid/FMI/Interfaces/PressureOutput.mo
@@ -28,17 +28,17 @@ connector PressureOutput =
       extent={{30.0,60.0},{30.0,110.0}},
       textString="%name")}),
   Documentation(info="<html>
- <p>
- Connector with one output signal of type <code>Modelica.Units.SI.AbsolutePressure</code>.
- This connector has been implemented to conditionally remove
- the pressure if no pressure drop calculation is requested.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 29,2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Connector with one output signal of type <code>Modelica.Units.SI.AbsolutePressure</code>.
+This connector has been implemented to conditionally remove
+the pressure if no pressure drop calculation is requested.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 29,2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/FMI/Sink_T.mo b/AixLib/Fluid/FMI/Sink_T.mo
index 105874e65b..b74c1d96a3 100644
--- a/AixLib/Fluid/FMI/Sink_T.mo
+++ b/AixLib/Fluid/FMI/Sink_T.mo
@@ -46,7 +46,7 @@ model Sink_T
         rotation=180,
         origin={-120,-80})));
 protected
-  AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
+  input AixLib.Fluid.FMI.Interfaces.FluidProperties bacPro_internal(
     redeclare final package Medium = Medium)
     "Internal connector for fluid properties for back flow";
   AixLib.Fluid.FMI.Interfaces.PressureOutput p_in_internal
@@ -93,51 +93,56 @@ equation
           textString="P",
           visible=use_p_in)}),
     Documentation(info="<html>
- <p>
- Model of a sink that takes as an input the medium properties
- temperature, mass fractions (if <code>Medium.nXi &gt; 0</code>)
- and trace substances (if <code>Medium.nC &gt; 0</code>).
- These properties are used during reverse flow.
- </p>
- <p>
- For a system of components with the connectors of the
- <a href=\"modelica://AixLib.Fluid.FMI\">
- AixLib.Fluid.FMI</a>
- package, this component is required to set the medium properties
- for the reverse flow.
- </p>
- <p>
- If the parameter <code>use_p_in</code> is set to <code>true</code>,
- then the model has an output connector <code>p</code>.
- This can be used to obtain the pressure of the sink, which
- may be needed to iteratively solve for the mass flow rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air and water.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Redesigned to conditionally remove the pressure connector
- if <code>use_p_in=false</code>.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Added pressure output signal which is needed to solve for algebraic loops.
- </li>
- <li>
- April 15, 2015 by Michael Wetter:<br/>
- Changed connector variable to be temperature instead of
- specific enthalpy.
- </li>
- <li>
- November 8, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model of a sink that takes as an input the medium properties
+temperature, mass fractions (if <code>Medium.nXi &gt; 0</code>)
+and trace substances (if <code>Medium.nC &gt; 0</code>).
+These properties are used during reverse flow.
+</p>
+<p>
+For a system of components with the connectors of the
+<a href=\"modelica://AixLib.Fluid.FMI\">
+AixLib.Fluid.FMI</a>
+package, this component is required to set the medium properties
+for the reverse flow.
+</p>
+<p>
+If the parameter <code>use_p_in</code> is set to <code>true</code>,
+then the model has an output connector <code>p</code>.
+This can be used to obtain the pressure of the sink, which
+may be needed to iteratively solve for the mass flow rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 18, 2024, by Michael Wetter:<br/>
+Added causality.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1853\">IBPSA, #1853</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air and water.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Redesigned to conditionally remove the pressure connector
+if <code>use_p_in=false</code>.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Added pressure output signal which is needed to solve for algebraic loops.
+</li>
+<li>
+April 15, 2015 by Michael Wetter:<br/>
+Changed connector variable to be temperature instead of
+specific enthalpy.
+</li>
+<li>
+November 8, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Sink_T;
diff --git a/AixLib/Fluid/FMI/Source_T.mo b/AixLib/Fluid/FMI/Source_T.mo
index b6f5f5fb37..dd4e86052b 100644
--- a/AixLib/Fluid/FMI/Source_T.mo
+++ b/AixLib/Fluid/FMI/Source_T.mo
@@ -47,7 +47,7 @@ model Source_T
 protected
   AixLib.Fluid.FMI.Interfaces.PressureOutput p_in_internal
     "Internal connector for pressure";
-  AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_in_internal
+  input AixLib.Fluid.FMI.Interfaces.MassFractionConnector X_w_in_internal
     "Internal connector for mass fraction of forward flow properties";
 initial equation
    assert(Medium.nXi < 2,
@@ -84,47 +84,52 @@ equation
           extent={{-94,60},{94,-58}},
           textColor={0,0,255},
           textString="m_flow
- p")}),
+p")}),
     Documentation(info="<html>
- <p>
- Model of a source that takes as an input the mass flow rate,
- pressure and the medium properties
- temperature, mass fractions (if <code>Medium.nXi &gt; 0</code>)
- and trace substances (if <code>Medium.nC &gt; 0</code>).
- </p>
- <p>
- For a system of components with the connectors of the
- <a href=\"modelica://AixLib.Fluid.FMI\">
- AixLib.Fluid.FMI</a>
- package, this component is required to set the pressure
- and the mass flow rate of the system.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to moist air only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- October 15, 2016, by Michael Wetter:<br/>
- Removed redundant connection.
- </li>
- <li>
- April 29, 2015, by Michael Wetter:<br/>
- Redesigned to conditionally remove the pressure connector
- if <code>use_p_in=false</code>.
- </li>
- <li>
- April 15, 2015 by Michael Wetter:<br/>
- Changed connector variable to be temperature instead of
- specific enthalpy.
- </li>
- <li>
- November 8, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model of a source that takes as an input the mass flow rate,
+pressure and the medium properties
+temperature, mass fractions (if <code>Medium.nXi &gt; 0</code>)
+and trace substances (if <code>Medium.nC &gt; 0</code>).
+</p>
+<p>
+For a system of components with the connectors of the
+<a href=\"modelica://AixLib.Fluid.FMI\">
+AixLib.Fluid.FMI</a>
+package, this component is required to set the pressure
+and the mass flow rate of the system.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 18, 2024, by Michael Wetter:<br/>
+Added causality.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1853\">IBPSA, #1853</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to moist air only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+October 15, 2016, by Michael Wetter:<br/>
+Removed redundant connection.
+</li>
+<li>
+April 29, 2015, by Michael Wetter:<br/>
+Redesigned to conditionally remove the pressure connector
+if <code>use_p_in=false</code>.
+</li>
+<li>
+April 15, 2015 by Michael Wetter:<br/>
+Changed connector variable to be temperature instead of
+specific enthalpy.
+</li>
+<li>
+November 8, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Source_T;
diff --git a/AixLib/Fluid/FMI/UsersGuide.mo b/AixLib/Fluid/FMI/UsersGuide.mo
index cf2287abf2..e719150540 100644
--- a/AixLib/Fluid/FMI/UsersGuide.mo
+++ b/AixLib/Fluid/FMI/UsersGuide.mo
@@ -249,7 +249,7 @@ The model
 <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
 AixLib.Fluid.Movers.FlowControlled_m_flow</a>
 cannot be exported as an FMU.
-This is because it assignes the mass flow rate.
+This is because it assigns the mass flow rate.
 However, the input connector
 <a href=\"modelica://AixLib.Fluid.FMI.Interfaces.Inlet\">
 AixLib.Fluid.FMI.Interfaces.Inlet</a>
diff --git a/AixLib/Fluid/FMI/Validation/FlowSplitter_u.mo b/AixLib/Fluid/FMI/Validation/FlowSplitter_u.mo
index 7d49e2bfb2..b3f0267dd4 100644
--- a/AixLib/Fluid/FMI/Validation/FlowSplitter_u.mo
+++ b/AixLib/Fluid/FMI/Validation/FlowSplitter_u.mo
@@ -78,23 +78,23 @@ equation
       smooth=Smooth.None));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,
             -100},{140,100}}), graphics), Documentation(info="<html>
- <p>
- This example demonstrates how to configure a model with a flow splitter.
- </p>
- <p>
- For this example, the model is not exported as an FMU. However, the
- thermofluid flow models are wrapped using input/output blocks.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 28, 2015, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to configure a model with a flow splitter.
+</p>
+<p>
+For this example, the model is not exported as an FMU. However, the
+thermofluid flow models are wrapped using input/output blocks.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 28, 2015, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Validation/FlowSplitter_u.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowSplitter_u;
diff --git a/AixLib/Fluid/FMI/Validation/HeaterFan.mo b/AixLib/Fluid/FMI/Validation/HeaterFan.mo
index 58f200f75f..7decd761bf 100644
--- a/AixLib/Fluid/FMI/Validation/HeaterFan.mo
+++ b/AixLib/Fluid/FMI/Validation/HeaterFan.mo
@@ -6,8 +6,8 @@ model HeaterFan
 
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=Q_flow_nominal/1000/
       10 "Nominal mass flow rate";
-  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")=
-       2000 "Pressure";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+     = 2000 "Pressure";
   parameter Modelica.Units.SI.HeatFlowRate Q_flow_nominal=1000
     "Heat flow rate at u=1, positive for heating";
 
@@ -126,40 +126,40 @@ equation
       smooth=Smooth.None));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,
             -100},{140,100}}), graphics), Documentation(info="<html>
- <p>
- This example demonstrates how to configure a model with a heater
- and a fan that causes a pressure rise in the air stream.
- Note that the mass flow rate and the absolute pressure are
- set by the component <code>sou</code>.
- Therefore, the fan simply increases the pressure of the medium,
- and it also computes how much power is needed for this pressure rise,
- which is an input to the fan model.
- </p>
- <p>
- For a model with that computes the mass flow rate based on the pressure drop, see
- <a href=\"modelica://AixLib.Fluid.FMI.Validation.HeaterFanPressureDriven\">
- AixLib.Fluid.FMI.Validation.HeaterFanPressureDriven</a>.
- </p>
- <p>
- For this example, the models are not exported as FMUs. However, the
- thermofluid flow models are wrapped using input/output blocks.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 8, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to configure a model with a heater
+and a fan that causes a pressure rise in the air stream.
+Note that the mass flow rate and the absolute pressure are
+set by the component <code>sou</code>.
+Therefore, the fan simply increases the pressure of the medium,
+and it also computes how much power is needed for this pressure rise,
+which is an input to the fan model.
+</p>
+<p>
+For a model with that computes the mass flow rate based on the pressure drop, see
+<a href=\"modelica://AixLib.Fluid.FMI.Validation.HeaterFanPressureDriven\">
+AixLib.Fluid.FMI.Validation.HeaterFanPressureDriven</a>.
+</p>
+<p>
+For this example, the models are not exported as FMUs. However, the
+thermofluid flow models are wrapped using input/output blocks.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 8, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Validation/HeaterFan.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeaterFan;
diff --git a/AixLib/Fluid/FMI/Validation/HeaterFanPressureDriven.mo b/AixLib/Fluid/FMI/Validation/HeaterFanPressureDriven.mo
index ba2c12e7c6..11963d2436 100644
--- a/AixLib/Fluid/FMI/Validation/HeaterFanPressureDriven.mo
+++ b/AixLib/Fluid/FMI/Validation/HeaterFanPressureDriven.mo
@@ -6,8 +6,8 @@ model HeaterFanPressureDriven
 
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=Q_flow_nominal/1000/
       10 "Nominal mass flow rate";
-  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")=
-       2000 "Pressure";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+     = 2000 "Pressure";
   parameter Modelica.Units.SI.HeatFlowRate Q_flow_nominal=1000
     "Heat flow rate at u=1, positive for heating";
 
@@ -135,42 +135,42 @@ equation
       smooth=Smooth.None));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,
             -100},{140,100}}), graphics), Documentation(info="<html>
- <p>
- This example demonstrates how to configure a model with a heater
- and a fan that causes a pressure rise in the air stream.
- The fan increases the pressure of the medium,
- and it also computes how much power is needed for this pressure rise,
- which is an input to the fan model.
- </p>
- <p>
- The component <code>invBloCon</code> at the bottom of the model sets up
- an equality constraint on the pressure between the sink and the source.
- It also outputs a signal for the mass flow rate. Hence, this component is
- used to declare how to break the algebraic loop in this signal flow diagram.
- For a model with prescribed mass flow rate, see
- <a href=\"modelica://AixLib.Fluid.FMI.Validation.HeaterFan\">
- AixLib.Fluid.FMI.Validation.HeaterFan</a>.
- </p>
- <p>
- For this example, the models are not exported as FMUs. However, the
- thermofluid flow models are wrapped using input/output blocks.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 8, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to configure a model with a heater
+and a fan that causes a pressure rise in the air stream.
+The fan increases the pressure of the medium,
+and it also computes how much power is needed for this pressure rise,
+which is an input to the fan model.
+</p>
+<p>
+The component <code>invBloCon</code> at the bottom of the model sets up
+an equality constraint on the pressure between the sink and the source.
+It also outputs a signal for the mass flow rate. Hence, this component is
+used to declare how to break the algebraic loop in this signal flow diagram.
+For a model with prescribed mass flow rate, see
+<a href=\"modelica://AixLib.Fluid.FMI.Validation.HeaterFan\">
+AixLib.Fluid.FMI.Validation.HeaterFan</a>.
+</p>
+<p>
+For this example, the models are not exported as FMUs. However, the
+thermofluid flow models are wrapped using input/output blocks.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 8, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Validation/HeaterFanPressureDriven.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeaterFanPressureDriven;
diff --git a/AixLib/Fluid/FMI/Validation/HeaterFan_noReverseFlow.mo b/AixLib/Fluid/FMI/Validation/HeaterFan_noReverseFlow.mo
index 2862545807..60feb00390 100644
--- a/AixLib/Fluid/FMI/Validation/HeaterFan_noReverseFlow.mo
+++ b/AixLib/Fluid/FMI/Validation/HeaterFan_noReverseFlow.mo
@@ -13,8 +13,8 @@ model HeaterFan_noReverseFlow
 
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=Q_flow_nominal/1000/
       10 "Nominal mass flow rate";
-  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")=
-       2000 "Pressure";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+     = 2000 "Pressure";
   parameter Modelica.Units.SI.HeatFlowRate Q_flow_nominal=1000
     "Heat flow rate at u=1, positive for heating";
 
@@ -100,36 +100,36 @@ equation
       color={0,0,127},
       smooth=Smooth.None));
     annotation(Documentation(info="<html>
- <p>
- This example demonstrates how to configure a model with a heater
- and a fan that causes a pressure rise in the air stream.
- The model is identical with
- <a href=\"modelica://AixLib.Fluid.FMI.Validation.HeaterFan\">
- AixLib.Fluid.FMI.Validation.HeaterFan</a>
- except that reverse flow is not allowed due to the parameter
- <code>allowFlowReversal=false</code>.
- Consequently, the connectors for the fluid properties for the reverse flow
- are removed, and the blocks on the right hand side of the model
- <a href=\"modelica://AixLib.Fluid.FMI.Validation.HeaterFan\">
- AixLib.Fluid.FMI.Validation.HeaterFan</a>
- have been deleted.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 8, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates how to configure a model with a heater
+and a fan that causes a pressure rise in the air stream.
+The model is identical with
+<a href=\"modelica://AixLib.Fluid.FMI.Validation.HeaterFan\">
+AixLib.Fluid.FMI.Validation.HeaterFan</a>
+except that reverse flow is not allowed due to the parameter
+<code>allowFlowReversal=false</code>.
+Consequently, the connectors for the fluid properties for the reverse flow
+are removed, and the blocks on the right hand side of the model
+<a href=\"modelica://AixLib.Fluid.FMI.Validation.HeaterFan\">
+AixLib.Fluid.FMI.Validation.HeaterFan</a>
+have been deleted.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 8, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FMI/Validation/HeaterFan_noReverseFlow.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=1.0),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=1.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeaterFan_noReverseFlow;
diff --git a/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlow.mo b/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlow.mo
index ec2e71f525..3b59ace963 100644
--- a/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlow.mo
+++ b/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlow.mo
@@ -125,55 +125,55 @@ equation
           fillPattern=FillPattern.HorizontalCylinder,
           fillColor={175,175,175})}),
     Documentation(revisions="<html>
- <ul>
- <li>
- October 20, 2017, by Michael Wetter:<br/>
- Deleted various parameters and variables that were not used.
- <br/>
- Revised documentation to follow the guidelines.
- </li>
- <li>
- May 19, 2016 by Marcus Fuchs:<br/>
- Remove condition on <code>show_V_flow</code> for calculation of
- <code>V_flow</code> to conform with pedantic checking.
- </li>
- <li>
- October 10, 2015 by Marcus Fuchs:<br/>
- Copy Icon from KUL implementation and rename model.
- </li>
- <li>
- June 23, 2015 by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Model that computes the temperature propagation of
- a fluid flow through a pipe, idealized as a plug flow.
- </p>
- <h4>Main equation</h4>
- <p>
- The transport delay is computed using the one-dimensional wave equation
- without source or sink terms,
- <p align=\"center\" style=\"font-style:italic;\">
- &part;z(x,t)/&part;t + v(t) &part;z(x,t)/&part;x = 0,
- </p>
- <p>where <i>z(x,t)</i> is the spatial distribution as a function of time of any
- property <i>z</i> of the fluid.
- For the temperature propagation, <i>z </i>will be replaced by <i>T</i>.
- </p>
- <h4>Assumptions</h4>
- <p>
- This model is based on the following assumptions:
- </p>
- <ul>
- <li>
- Axial diffusion in water is assumed to be negligibe.
- </li>
- <li>
- The water temperature is assumed uniform in a cross section.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 20, 2017, by Michael Wetter:<br/>
+Deleted various parameters and variables that were not used.
+<br/>
+Revised documentation to follow the guidelines.
+</li>
+<li>
+May 19, 2016 by Marcus Fuchs:<br/>
+Remove condition on <code>show_V_flow</code> for calculation of
+<code>V_flow</code> to conform with pedantic checking.
+</li>
+<li>
+October 10, 2015 by Marcus Fuchs:<br/>
+Copy Icon from KUL implementation and rename model.
+</li>
+<li>
+June 23, 2015 by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Model that computes the temperature propagation of
+a fluid flow through a pipe, idealized as a plug flow.
+</p>
+<h4>Main equation</h4>
+<p>
+The transport delay is computed using the one-dimensional wave equation
+without source or sink terms,
+<p align=\"center\" style=\"font-style:italic;\">
+&part;z(x,t)/&part;t + v(t) &part;z(x,t)/&part;x = 0,
+</p>
+<p>where <i>z(x,t)</i> is the spatial distribution as a function of time of any
+property <i>z</i> of the fluid.
+For the temperature propagation, <i>z </i>will be replaced by <i>T</i>.
+</p>
+<h4>Assumptions</h4>
+<p>
+This model is based on the following assumptions:
+</p>
+<ul>
+<li>
+Axial diffusion in water is assumed to be negligibe.
+</li>
+<li>
+The water temperature is assumed uniform in a cross section.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlow;
diff --git a/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowHeatLoss.mo b/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowHeatLoss.mo
index 08170a2f09..7ab65d577d 100644
--- a/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowHeatLoss.mo
+++ b/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowHeatLoss.mo
@@ -87,78 +87,78 @@ equation
           fillColor={238,46,47},
           fillPattern=FillPattern.Solid)}),
     Documentation(info="<html>
- <p>
- Component that calculates the heat losses at the end of a plug flow pipe
- when the flow goes in the design direction.
- </p>
- <h4>Main equations</h4>
- <p>
- The governing equations are
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- T<sub>out</sub> = T<sub>b</sub> + (T<sub>in</sub> - T<sub>b</sub>)
- exp((t<sub>out</sub> - t<sub>in</sub>)/tau<sub>char</sub>)
- </p>
- <p>
- with
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- tau<sub>char</sub> = R C
- </p>
- <h4>Assumptions and limitations</h4>
- <p>
- This model is based on the following assumptions:
- </p>
- <ul>
- <li>The water temperature is uniform in the cross section.</li>
- <li>There is no axial heat transfer in the water or surrounding.</li>
- <li>The boundary temperature along the pipe is uniform.</li>
- <li>Heat losses are steady-state.</li>
- </ul>
- <h4>Implementation</h4>
- <p>
- Heat losses are only considered in design flow direction.
- For heat loss consideration in both directions, use one of these models at
- both ends of a
- <a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow\">
- AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow</a> model.
- The outlet temperature is calculated as in the equation above,
- using the inlet temperature at <code>port_a</code> and the instantaneous
- time delay and boundary temperature.
- The boundary temperature can be either the air temperature
- or the undisturbed ground temperature, depending on the definition of the
- thermal resistance <i>R</i>.
- </p>
- <p>
- This component requires the delay time and the instantaneous ambient temperature
- as an input.
- This component is to be used in single pipes or in more advanced configurations
- where no influence from other pipes is considered.</p>
- </html>",
+<p>
+Component that calculates the heat losses at the end of a plug flow pipe
+when the flow goes in the design direction.
+</p>
+<h4>Main equations</h4>
+<p>
+The governing equations are
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+T<sub>out</sub> = T<sub>b</sub> + (T<sub>in</sub> - T<sub>b</sub>)
+exp((t<sub>out</sub> - t<sub>in</sub>)/tau<sub>char</sub>)
+</p>
+<p>
+with
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+tau<sub>char</sub> = R C
+</p>
+<h4>Assumptions and limitations</h4>
+<p>
+This model is based on the following assumptions:
+</p>
+<ul>
+<li>The water temperature is uniform in the cross section.</li>
+<li>There is no axial heat transfer in the water or surrounding.</li>
+<li>The boundary temperature along the pipe is uniform.</li>
+<li>Heat losses are steady-state.</li>
+</ul>
+<h4>Implementation</h4>
+<p>
+Heat losses are only considered in design flow direction.
+For heat loss consideration in both directions, use one of these models at
+both ends of a
+<a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow\">
+AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow</a> model.
+The outlet temperature is calculated as in the equation above,
+using the inlet temperature at <code>port_a</code> and the instantaneous
+time delay and boundary temperature.
+The boundary temperature can be either the air temperature
+or the undisturbed ground temperature, depending on the definition of the
+thermal resistance <i>R</i>.
+</p>
+<p>
+This component requires the delay time and the instantaneous ambient temperature
+as an input.
+This component is to be used in single pipes or in more advanced configurations
+where no influence from other pipes is considered.</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 6, 2017, by Michael Wetter:<br/>
- Reformulated call to medium function.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/869\">
- issue 869</a>.
- </li>
- <li>
- October 20, 2017, by Michael Wetter:<br/>
- Revised implementation to avoid graphical and textual modeling.
- Revised variable names and documentation to follow guidelines.
- </li>
- <li>
- November 6, 2015 by Bram van der Heijde:<br/>
- Make time delay input instead of calculation inside this model.
- </li>
- <li>
- September, 2015 by Marcus Fuchs:<br/>
- First implementation.</li>
- </ul>
- </html>"),
+<ul>
+<li>
+December 6, 2017, by Michael Wetter:<br/>
+Reformulated call to medium function.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/869\">
+issue 869</a>.
+</li>
+<li>
+October 20, 2017, by Michael Wetter:<br/>
+Revised implementation to avoid graphical and textual modeling.
+Revised variable names and documentation to follow guidelines.
+</li>
+<li>
+November 6, 2015 by Bram van der Heijde:<br/>
+Make time delay input instead of calculation inside this model.
+</li>
+<li>
+September, 2015 by Marcus Fuchs:<br/>
+First implementation.</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
-            100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowHeatLoss;
diff --git a/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowPipe.mo b/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowPipe.mo
index 00892a32a2..56ebeb2475 100644
--- a/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowPipe.mo
+++ b/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowPipe.mo
@@ -13,11 +13,11 @@ model PlugFlowPipe
 
   parameter Boolean have_pipCap=true
     "= true, a mixing volume is added that corresponds
-     to the heat capacity of the pipe wall"
+    to the heat capacity of the pipe wall"
     annotation (Dialog(tab="Advanced"));
   parameter Boolean have_symmetry=true
     "= false, the mixing volume is only on port_b,
-     which improve performances, but reduces dynamic accuracy."
+    which improve performances, but reduces dynamic accuracy."
     annotation (Dialog(tab="Advanced", enable=have_pipCap));
 
   parameter Modelica.Units.SI.Length dh=sqrt(4*m_flow_nominal/rho_default/
@@ -58,11 +58,11 @@ model PlugFlowPipe
   parameter Modelica.Units.SI.Length thickness=0.0035 "Pipe wall thickness"
     annotation (Dialog(group="Material"));
 
-  parameter Modelica.Units.SI.Temperature T_start_in(start=Medium.T_default)=
+  parameter Modelica.Units.SI.Temperature T_start_in(start=Medium.T_default) =
     Medium.T_default "Initialization temperature at pipe inlet"
     annotation (Dialog(tab="Initialization"));
-  parameter Modelica.Units.SI.Temperature T_start_out(start=Medium.T_default)=
-       T_start_in "Initialization temperature at pipe outlet"
+  parameter Modelica.Units.SI.Temperature T_start_out(start=Medium.T_default)
+     = T_start_in "Initialization temperature at pipe outlet"
     annotation (Dialog(tab="Initialization"));
   parameter Boolean initDelay = false
     "Initialize delay for a constant mass flow rate if true, otherwise start from 0"
@@ -78,7 +78,7 @@ model PlugFlowPipe
 
   parameter Real fac=1
     "Factor to take into account flow resistance of bends etc.,
-     fac=dp_nominal/dpStraightPipe_nominal";
+    fac=dp_nominal/dpStraightPipe_nominal";
 
   parameter Boolean linearized = false
     "= true, use linear relation between m_flow and dp for any flow rate"
@@ -206,7 +206,7 @@ protected
     final energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     final mSenFac=if rho_default > 500 then 1 else 10) if have_pipCap
     "Control volume connected to port_b.
-     Represents equivalent pipe wall thermal capacity."
+    Represents equivalent pipe wall thermal capacity."
     annotation (Placement(transformation(extent={{70,20},{90,40}})));
   LosslessPipe noMixPip_b(
     redeclare final package Medium = Medium,
@@ -225,7 +225,7 @@ protected
     final energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     final mSenFac=if rho_default > 500 then 1 else 10) if have_pipCap_a
     "Control volume connected to port_a.
-     Represents equivalent pipe wall thermal capacity."
+    Represents equivalent pipe wall thermal capacity."
     annotation (Placement(transformation(extent={{-90,20},{-70,40}})));
   LosslessPipe noMixPip_a(
     redeclare final package Medium = Medium,
@@ -233,13 +233,13 @@ protected
     final m_flow_small=m_flow_small,
     final allowFlowReversal=allowFlowReversal) if not have_pipCap_a
     "Lossless pipe for connecting the outlet port when have_pipCap=false
-     or have_symmetry=false"
+    or have_symmetry=false"
     annotation (Placement(transformation(extent={{-90,-30},{-70,-10}})));
 
 initial equation
   assert(homotopyInitialization, "In " + getInstanceName() +
     ": The constant homotopyInitialization has been modified from its default
-     value. This constant will be removed in future releases.",
+    value. This constant will be removed in future releases.",
     level = AssertionLevel.warning);
 
 equation
@@ -338,158 +338,158 @@ equation
           textColor={0,0,0},
           textString="L = %length")}),
     Documentation(revisions="<html>
- <ul>
- <li>
- October 15, 2021, by Michael Wetter:<br/>
- Moved model to <code>BaseClasses</code>. This allows
- <a href=\"AixLib.Fluid.FixedResistances.PlugFlowPipe\">AixLib.Fluid.FixedResistances.PlugFlowPipe</a>
- to redeclare the resistance as final, thereby avoiding that a GUI presents this instance
- to users as a replaceable class.
- </li>
- <li>
- October 05, 2021, by Baptiste Ravache:<br/>
- Made model symmetrical and extends from
- <a href=\"AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
- AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>.
- </li>
- <li>
- September 14, 2021, by Michael Wetter:<br/>
- Made most instances protected and exposed main variables of interest.
- </li>
- <li>
- July 9, 2021, by Baptiste Ravache:<br/>
- Replaced the vectorized outlet port <code>ports_b</code> with
- a single outlet port <code>port_b</code>.<br/>
- Expanded the core pipe model that was previously a component.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1494\">IBPSA, #1494</a>.<br/>
- This change is not backward compatible.<br/>
- The previous classes definitions were moved to
- <a href=\"modelica://AixLib.Obsolete.Fluid.FixedResistances.PlugFlowPipe\">
- AixLib.Obsolete.Fluid.FixedResistances.PlugFlowPipe</a>.
- <a href=\"modelica://AixLib.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore\">
- AixLib.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore</a>.
- </li>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- March 6, 2020, by Jelger Jansen:<br/>
- Revised calculation of thermal resistance <code>R</code>
- by using correct radiuses.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1310\">#1310</a>.
- </li>
- <li>
- October 23, 2017, by Michael Wetter:<br/>
- Revised variable names and documentation to follow guidelines.
- Corrected malformed hyperlinks.
- </li>
- <li>
- July 4, 2016 by Bram van der Heijde:<br/>
- Introduce <code>pipVol</code>.
- </li>
- <li>
- October 10, 2015 by Marcus Fuchs:<br/>
- Copy Icon from KUL implementation and rename model.
- Replace resistance and temperature delay by an adiabatic pipe.
- </li>
- <li>September, 2015 by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Pipe with heat loss using the time delay based heat losses and transport
- of the fluid using a plug flow model, applicable for simulation of long
- pipes such as in district heating and cooling systems.</p>
- <p>
- This model takes into account transport delay along the pipe length idealized
- as a plug flow.
- The model also includes thermal inertia of the pipe wall.
- </p>
- <h4>Implementation</h4>
- <p>
- The
- <code>spatialDistribution</code> operator is used for the temperature wave propagation
- through the length of the pipe. This operator is contained in
- <a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow\">
- AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow</a>.
- </p>
- <p>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlowHeatLoss\">
- AixLib.Fluid.FixedResistances.BaseClasses.PlugFlowHeatLoss</a>
- implements a heat loss in design direction, but leaves the enthalpy unchanged
- in opposite flow direction. Therefore it is used in front of and behind the time delay.
- </p>
- <p>
- The pressure drop is implemented using
- <a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
- AixLib.Fluid.FixedResistances.HydraulicDiameter</a>.
- This instance is replaceable to allow
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipeDiscretized\">
- AixLib.Fluid.FixedResistances.PlugFlowPipeDiscretized</a>
- to compute the pressure drop only once rather than for each segment.
- </p>
- <p>
- The thermal capacity of the pipe wall is implemented as a mixing volume
- of the fluid in the pipe, of which the thermal capacity is equal to that
- of the pipe wall material.
- In addition, this mixing volume allows the hydraulic separation of subsequent pipes.
- <br/>
- The mixing volume is either split between the inlet and outlet ports
- (port_a and port_b) or lumped in at the outlet (port_b)
- if <code>have_symmetry</code> is set to false.
- This mixing volume can be removed from this model with the Boolean parameter
- <code>have_pipCap</code>, in cases where the pipe wall heat capacity
- is negligible and a state is not needed at the pipe outlet
- (see the note below about numerical Jacobians).
- </p>
- <p>
- Note that in order to model a branched network it is recommended to use
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Junction\">
- AixLib.Fluid.FixedResistances.Junction</a> at each junction and to configure
- that junction model with a state
- (<code>energyDynamics &lt;&gt; Modelica.Fluid.Types.Dynamics.SteadyState</code>),
- see for instance
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>.
- This will avoid the numerical Jacobian that is otherwise created when
- the inlet ports of two instances of the plug flow model are connected together.
- </p>
- <h4>Assumptions</h4>
- <ul>
- <li>
- Heat losses are for steady-state operation.
- </li>
- <li>
- The axial heat diffusion in the fluid, the pipe wall and the ground are neglected.
- </li>
- <li>
- The boundary temperature is uniform.
- </li>
- <li>
- The thermal inertia of the pipe wall material is lumped on the side of the pipe
- that is connected to <code>port_b</code>.
- </li>
- </ul>
- <h4>References</h4>
- <p>
- Full details on the model implementation and experimental validation can be found
- in:
- </p>
- <p>
- van der Heijde, B., Fuchs, M., Ribas Tugores, C., Schweiger, G., Sartor, K.,
- Basciotti, D., M&uuml;ller, D., Nytsch-Geusen, C., Wetter, M. and Helsen, L.
- (2017).<br/>
- Dynamic equation-based thermo-hydraulic pipe model for district heating and
- cooling systems.<br/>
- <i>Energy Conversion and Management</i>, vol. 151, p. 158-169.
- <a href=\"https://doi.org/10.1016/j.enconman.2017.08.072\">doi:
- 10.1016/j.enconman.2017.08.072</a>.</p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 15, 2021, by Michael Wetter:<br/>
+Moved model to <code>BaseClasses</code>. This allows
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">AixLib.Fluid.FixedResistances.PlugFlowPipe</a>
+to redeclare the resistance as final, thereby avoiding that a GUI presents this instance
+to users as a replaceable class.
+</li>
+<li>
+October 05, 2021, by Baptiste Ravache:<br/>
+Made model symmetrical and extends from
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>.
+</li>
+<li>
+September 14, 2021, by Michael Wetter:<br/>
+Made most instances protected and exposed main variables of interest.
+</li>
+<li>
+July 9, 2021, by Baptiste Ravache:<br/>
+Replaced the vectorized outlet port <code>ports_b</code> with
+a single outlet port <code>port_b</code>.<br/>
+Expanded the core pipe model that was previously a component.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1494\">IBPSA, #1494</a>.<br/>
+This change is not backward compatible.<br/>
+The previous classes definitions were moved to
+<a href=\"modelica://AixLib.Obsolete.Fluid.FixedResistances.PlugFlowPipe\">
+AixLib.Obsolete.Fluid.FixedResistances.PlugFlowPipe</a>.
+<a href=\"modelica://AixLib.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore\">
+AixLib.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+March 6, 2020, by Jelger Jansen:<br/>
+Revised calculation of thermal resistance <code>R</code>
+by using correct radiuses.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1310\">#1310</a>.
+</li>
+<li>
+October 23, 2017, by Michael Wetter:<br/>
+Revised variable names and documentation to follow guidelines.
+Corrected malformed hyperlinks.
+</li>
+<li>
+July 4, 2016 by Bram van der Heijde:<br/>
+Introduce <code>pipVol</code>.
+</li>
+<li>
+October 10, 2015 by Marcus Fuchs:<br/>
+Copy Icon from KUL implementation and rename model.
+Replace resistance and temperature delay by an adiabatic pipe.
+</li>
+<li>September, 2015 by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Pipe with heat loss using the time delay based heat losses and transport
+of the fluid using a plug flow model, applicable for simulation of long
+pipes such as in district heating and cooling systems.</p>
+<p>
+This model takes into account transport delay along the pipe length idealized
+as a plug flow.
+The model also includes thermal inertia of the pipe wall.
+</p>
+<h4>Implementation</h4>
+<p>
+The
+<code>spatialDistribution</code> operator is used for the temperature wave propagation
+through the length of the pipe. This operator is contained in
+<a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow\">
+AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow</a>.
+</p>
+<p>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlowHeatLoss\">
+AixLib.Fluid.FixedResistances.BaseClasses.PlugFlowHeatLoss</a>
+implements a heat loss in design direction, but leaves the enthalpy unchanged
+in opposite flow direction. Therefore it is used in front of and behind the time delay.
+</p>
+<p>
+The pressure drop is implemented using
+<a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
+AixLib.Fluid.FixedResistances.HydraulicDiameter</a>.
+This instance is replaceable to allow
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipeDiscretized\">
+AixLib.Fluid.FixedResistances.PlugFlowPipeDiscretized</a>
+to compute the pressure drop only once rather than for each segment.
+</p>
+<p>
+The thermal capacity of the pipe wall is implemented as a mixing volume
+of the fluid in the pipe, of which the thermal capacity is equal to that
+of the pipe wall material.
+In addition, this mixing volume allows the hydraulic separation of subsequent pipes.
+<br/>
+The mixing volume is either split between the inlet and outlet ports
+(port_a and port_b) or lumped in at the outlet (port_b)
+if <code>have_symmetry</code> is set to false.
+This mixing volume can be removed from this model with the Boolean parameter
+<code>have_pipCap</code>, in cases where the pipe wall heat capacity
+is negligible and a state is not needed at the pipe outlet
+(see the note below about numerical Jacobians).
+</p>
+<p>
+Note that in order to model a branched network it is recommended to use
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Junction\">
+AixLib.Fluid.FixedResistances.Junction</a> at each junction and to configure
+that junction model with a state
+(<code>energyDynamics &lt;&gt; Modelica.Fluid.Types.Dynamics.SteadyState</code>),
+see for instance
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>.
+This will avoid the numerical Jacobian that is otherwise created when
+the inlet ports of two instances of the plug flow model are connected together.
+</p>
+<h4>Assumptions</h4>
+<ul>
+<li>
+Heat losses are for steady-state operation.
+</li>
+<li>
+The axial heat diffusion in the fluid, the pipe wall and the ground are neglected.
+</li>
+<li>
+The boundary temperature is uniform.
+</li>
+<li>
+The thermal inertia of the pipe wall material is lumped on the side of the pipe
+that is connected to <code>port_b</code>.
+</li>
+</ul>
+<h4>References</h4>
+<p>
+Full details on the model implementation and experimental validation can be found
+in:
+</p>
+<p>
+van der Heijde, B., Fuchs, M., Ribas Tugores, C., Schweiger, G., Sartor, K.,
+Basciotti, D., M&uuml;ller, D., Nytsch-Geusen, C., Wetter, M. and Helsen, L.
+(2017).<br/>
+Dynamic equation-based thermo-hydraulic pipe model for district heating and
+cooling systems.<br/>
+<i>Energy Conversion and Management</i>, vol. 151, p. 158-169.
+<a href=\"https://doi.org/10.1016/j.enconman.2017.08.072\">doi:
+10.1016/j.enconman.2017.08.072</a>.</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowPipe;
diff --git a/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowTransportDelay.mo b/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowTransportDelay.mo
index 65aca26a40..e9bafff392 100644
--- a/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowTransportDelay.mo
+++ b/AixLib/Fluid/FixedResistances/BaseClasses/PlugFlowTransportDelay.mo
@@ -99,74 +99,74 @@ equation
           textColor={0,0,255},
           textString="%name")}),
     Documentation(info="<html>
- <p>
- Calculates time delay at both sides of the pipe as the difference between the
- current simulation time and the inlet time of the fluid at both ends of the pipe.
- </p>
- <h4>Main equation</h4>
- <p align=\"center\">
- <i>&part;z(x,t)/&part;t + v(t) &part;z(x,t)/&part;x = 0,</i>
- </p>
- <p>
- where <i>z(x,t)</i> is the spatial distribution as a function of time of any
- property <i>z</i> of the fluid. For the inlet time propagation, <i>z</i> will
- be replaced by the inlet time of the fluid <i>t<sub>in</sub></i>.
- </p>
- <h4>Implementation</h4>
- <p>
- The inlet time is approached as a fluid property and its propagation follows
- the one-dimensional wave equation, implemented using the spatialDistribution
- function. This components requires the mass flow through the pipe and the pipe
- dimensions in order to derive information about the fluid propagation.
- </p>
- <p>
- The component calculates the delay time at the inlet and the outlet port of the pipe.
- For the forward flow, the time delay is exposed at the output <code>tau</code>,
- and for the backward flow, the time delay is exposed at the output <code>tauRev</code>.
- </p>
- <h4>Assumption</h4>
- <p>
- No axial mixing takes place in the pipe.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 2, 2020, by Philipp Mehrfeld:<br/>
- Corrected calculation of <code>tau</code> and <code>tauRev</code> to be be 
- only positive.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1427\">#1427</a>.
- </li>
- <li>
- December 14, 2018, by Michael Wetter:<br/>
- Corrected argument of <code>spatialDistribution</code> operator to be a parameter
- expression.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1055\">#1055</a>.
- </li>
- <li>
- September 9, 2016 by Bram van der Heijde:<br/>
- Rename from PDETime_massFlowMod to PlugFlowTransportDelayMod
- </li>
- <li>
- December 2015 by Carles Ribas Tugores:<br/>
- Modification in delay calculation to fix issues.
- </li>
- <li>
- November 6, 2015 by Bram van der Heijde:<br/>
- Adapted flow parameter to mass flow rate instead of velocity.
- This change should also fix the reverse and zero flow issues.
- </li>
- <li>
- October 13, 2015 by Marcus Fuchs:<br/>
- Use <code>abs()</code> of normalized velocity input in order to avoid negative
- delay times.
- </li>
- <li>
- July 2015 by Arnout Aertgeerts:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calculates time delay at both sides of the pipe as the difference between the
+current simulation time and the inlet time of the fluid at both ends of the pipe.
+</p>
+<h4>Main equation</h4>
+<p align=\"center\">
+<i>&part;z(x,t)/&part;t + v(t) &part;z(x,t)/&part;x = 0,</i>
+</p>
+<p>
+where <i>z(x,t)</i> is the spatial distribution as a function of time of any
+property <i>z</i> of the fluid. For the inlet time propagation, <i>z</i> will
+be replaced by the inlet time of the fluid <i>t<sub>in</sub></i>.
+</p>
+<h4>Implementation</h4>
+<p>
+The inlet time is approached as a fluid property and its propagation follows
+the one-dimensional wave equation, implemented using the spatialDistribution
+function. This components requires the mass flow through the pipe and the pipe
+dimensions in order to derive information about the fluid propagation.
+</p>
+<p>
+The component calculates the delay time at the inlet and the outlet port of the pipe.
+For the forward flow, the time delay is exposed at the output <code>tau</code>,
+and for the backward flow, the time delay is exposed at the output <code>tauRev</code>.
+</p>
+<h4>Assumption</h4>
+<p>
+No axial mixing takes place in the pipe.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 2, 2020, by Philipp Mehrfeld:<br/>
+Corrected calculation of <code>tau</code> and <code>tauRev</code> to be be 
+only positive.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1427\">#1427</a>.
+</li>
+<li>
+December 14, 2018, by Michael Wetter:<br/>
+Corrected argument of <code>spatialDistribution</code> operator to be a parameter
+expression.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1055\">#1055</a>.
+</li>
+<li>
+September 9, 2016 by Bram van der Heijde:<br/>
+Rename from PDETime_massFlowMod to PlugFlowTransportDelayMod
+</li>
+<li>
+December 2015 by Carles Ribas Tugores:<br/>
+Modification in delay calculation to fix issues.
+</li>
+<li>
+November 6, 2015 by Bram van der Heijde:<br/>
+Adapted flow parameter to mass flow rate instead of velocity.
+This change should also fix the reverse and zero flow issues.
+</li>
+<li>
+October 13, 2015 by Marcus Fuchs:<br/>
+Use <code>abs()</code> of normalized velocity input in order to avoid negative
+delay times.
+</li>
+<li>
+July 2015 by Arnout Aertgeerts:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowTransportDelay;
diff --git a/AixLib/Fluid/FixedResistances/BaseClasses/package.order b/AixLib/Fluid/FixedResistances/BaseClasses/package.order
index 06493b07b5..ad57712609 100644
--- a/AixLib/Fluid/FixedResistances/BaseClasses/package.order
+++ b/AixLib/Fluid/FixedResistances/BaseClasses/package.order
@@ -1,5 +1,5 @@
 PlugFlow
+PlugFlowCore
 PlugFlowHeatLoss
 PlugFlowPipe
 PlugFlowTransportDelay
-PlugFlowCore
diff --git a/AixLib/Fluid/FixedResistances/CheckValve.mo b/AixLib/Fluid/FixedResistances/CheckValve.mo
index ad0e3489a7..0ce73a4f04 100644
--- a/AixLib/Fluid/FixedResistances/CheckValve.mo
+++ b/AixLib/Fluid/FixedResistances/CheckValve.mo
@@ -25,12 +25,12 @@ model CheckValve "Check valve that avoids flow reversal"
     if dpFixed_nominal > Modelica.Constants.eps then
       m_flow_nominal/sqrt(dpFixed_nominal)
     else 0
-    "Flow coefficient of fixed resistance that may be in series with valve, 
-     k=m_flow/sqrt(dp), with unit=(kg.m)^(1/2).";
+    "Flow coefficient of fixed resistance that may be in series with valve,
+    k=m_flow/sqrt(dp), with unit=(kg.m)^(1/2).";
 
   Real k(min=Modelica.Constants.small)
-    "Flow coefficient of valve and pipe in series in allowed/forward direction, 
-     k=m_flow/sqrt(dp), with unit=(kg.m)^(1/2).";
+    "Flow coefficient of valve and pipe in series in allowed/forward direction,
+    k=m_flow/sqrt(dp), with unit=(kg.m)^(1/2).";
 
 protected
   Real a
@@ -42,8 +42,8 @@ protected
 
 initial equation
   assert(dpFixed_nominal > -Modelica.Constants.eps,
-    "In " + getInstanceName() + ": We require dpFixed_nominal >= 0. 
-     Received dpFixed_nominal = "+ String(dpFixed_nominal) + " Pa.");
+    "In " + getInstanceName() + ": We require dpFixed_nominal >= 0.
+    Received dpFixed_nominal = " + String(dpFixed_nominal) + " Pa.");
   assert(l > -Modelica.Constants.eps,
     "In " + getInstanceName() + ": We require l >= 0. Received l = " + String(l));
 equation
@@ -80,15 +80,15 @@ equation
         Line(
           points={{-100,0},{-70,0}},
           color={0,128,255},
-          lineThickness=0.5),
+          thickness=0.5),
         Line(
           points={{0,70},{-70,0}},
           color={0,128,255},
-          lineThickness=0.5),
+          thickness=0.5),
         Line(
           points={{0,-70},{-70,0}},
           color={0,128,255},
-          lineThickness=0.5),
+          thickness=0.5),
         Ellipse(
           extent={{-40,-55},{70,55}},
           lineColor={0,128,255},
@@ -98,69 +98,73 @@ equation
         Line(
           points={{70,0},{100,0}},
           color={0,128,255},
-          lineThickness=0.5)}),
+          thickness=0.5)}),
 defaultComponentName="cheVal",
 Documentation(info="<html>
- <p>
- Implementation of a hydraulic check valve.
- Note that the small reverse flows can still occur with this model.
- </p>
- <h4>Main equations</h4>
- <p>
- The basic flow function
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   m = sign(&Delta;p) k  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>,
- </p>
- <p>
- with regularization near the origin, is used to compute the pressure drop.
- The flow coefficient
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   k = m &frasl; &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
- </p>
- <p>
- is increased from <code>l*KV_Si</code> to <code>KV_Si</code>,
- where <code>KV_Si</code> is equal to <code>Kv</code> but in SI units.
- Therefore, the flow coefficient <code>k</code> is set to a value close to zero for negative pressure differences, thereby
- restricting reverse flow to a small value.
- The flow coefficient <code>k</code> saturates to its maximum value at the pressure <code>dpValve_closing</code>.
- For larger pressure drops, the pressure drop is a quadratic function of the flow rate.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The parameters <code>m_flow_nominal</code> and <code>dpValve_nominal</code> 
- determine the flow coefficient of the check valve when it is fully opened. 
- A typical value for a nominal flow rate of <i>1</i> m/s is
- <code>dpValve_nominal = 3400 Pa</code>.
- The leakage ratio <code>l</code> determines the minimum flow coefficient, 
- for negative pressure differences.
- The parameter <code>dpFixed_nominal</code> allows to include a series
- pressure drop with a fixed flow coefficient into the model.
- The parameter <code>dpValve_closing</code> determines when the
- flow coefficient starts to increase,
- which is typically in the order of <code>dpValve_nominal</code>.
- </p>
- <h4>Implementation</h4>
- <p>
- The check valve implementation approximates the physics
- where a forward pressure difference opens the valve such that
- the valve opening increases, causing a growing orifice area
- and thus increasing the flow coefficient.
- Near <code>dp=dpValve_closing</code>, the valve is fully open and the flow coefficient saturates
- to the flow coefficient value determined by <code>dpValve_nominal</code> and <code>m_flow_nominal</code>.
- For typical valve diameters, the check valve is only fully open
- near nominal mass flow rate. Therefore, the model sets <code>dpValve_closing=dpValve_nominal/2</code>
- by default.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 16, 2019, by Kristoff Six and Filip Jorissen:<br/>
- Implementation of a hydraulic check valve. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1198\">issue 1198</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Implementation of a hydraulic check valve.
+Note that the small reverse flows can still occur with this model.
+</p>
+<h4>Main equations</h4>
+<p>
+The basic flow function
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  m&#775; = sign(&Delta;p) k  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>,
+</p>
+<p>
+with regularization near the origin, is used to compute the pressure drop.
+The flow coefficient
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  k = m&#775; &frasl; &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
+</p>
+<p>
+is increased from <code>l*KV_Si</code> to <code>KV_Si</code>,
+where <code>KV_Si</code> is equal to <code>Kv</code> but in SI units.
+Therefore, the flow coefficient <code>k</code> is set to a value close to zero for negative pressure differences, thereby
+restricting reverse flow to a small value.
+The flow coefficient <code>k</code> saturates to its maximum value at the pressure <code>dpValve_closing</code>.
+For larger pressure drops, the pressure drop is a quadratic function of the flow rate.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The parameters <code>m_flow_nominal</code> and <code>dpValve_nominal</code>
+determine the flow coefficient of the check valve when it is fully opened.
+A typical value for a nominal flow rate of <i>1</i> m/s is
+<code>dpValve_nominal = 3400 Pa</code>.
+The leakage ratio <code>l</code> determines the minimum flow coefficient,
+for negative pressure differences.
+The parameter <code>dpFixed_nominal</code> allows to include a series
+pressure drop with a fixed flow coefficient into the model.
+The parameter <code>dpValve_closing</code> determines when the
+flow coefficient starts to increase,
+which is typically in the order of <code>dpValve_nominal</code>.
+</p>
+<h4>Implementation</h4>
+<p>
+The check valve implementation approximates the physics
+where a forward pressure difference opens the valve such that
+the valve opening increases, causing a growing orifice area
+and thus increasing the flow coefficient.
+Near <code>dp=dpValve_closing</code>, the valve is fully open and the flow coefficient saturates
+to the flow coefficient value determined by <code>dpValve_nominal</code> and <code>m_flow_nominal</code>.
+For typical valve diameters, the check valve is only fully open
+near nominal mass flow rate. Therefore, the model sets <code>dpValve_closing=dpValve_nominal/2</code>
+by default.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 3, 2023, by Michael Wetter:<br/>
+Corrected grahpical annotation.
+</li>
+<li>
+September 16, 2019, by Kristoff Six and Filip Jorissen:<br/>
+Implementation of a hydraulic check valve. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1198\">issue 1198</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckValve;
diff --git a/AixLib/Fluid/FixedResistances/Examples/CheckValve.mo b/AixLib/Fluid/FixedResistances/Examples/CheckValve.mo
index c063178277..23a40d4559 100644
--- a/AixLib/Fluid/FixedResistances/Examples/CheckValve.mo
+++ b/AixLib/Fluid/FixedResistances/Examples/CheckValve.mo
@@ -81,17 +81,17 @@ equation
       __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Examples/CheckValve.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- September 16, 2019, by Kristoff Six and Filip Jorissen:<br/>
- Implementation of a hydraulic check valve. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1198\">issue 1198</a>.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example model for the use of a hydraulic check valve.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 16, 2019, by Kristoff Six and Filip Jorissen:<br/>
+Implementation of a hydraulic check valve. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1198\">issue 1198</a>.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example model for the use of a hydraulic check valve.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckValve;
diff --git a/AixLib/Fluid/FixedResistances/Examples/FlowJunction.mo b/AixLib/Fluid/FixedResistances/Examples/FlowJunction.mo
index 0c72f9a9fe..6826d0ab53 100644
--- a/AixLib/Fluid/FixedResistances/Examples/FlowJunction.mo
+++ b/AixLib/Fluid/FixedResistances/Examples/FlowJunction.mo
@@ -95,29 +95,29 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Examples/FlowJunction.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model demonstrates the use of the flow junction model
- for different flow directions.
- The example is configured such that the flow changes its direction in
- each flow leg between <i>t = 0</i> seconds to <i>t = 100</i> seconds.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 2, 2017, by Michael Wetter:<br/>
- Removed import statement.
- </li>
- <li>
- October 14, 2017 by Michael Wetter:<br/>
- Updated documentation and added to Annex 60 library.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
- </li>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model demonstrates the use of the flow junction model
+for different flow directions.
+The example is configured such that the flow changes its direction in
+each flow leg between <i>t = 0</i> seconds to <i>t = 100</i> seconds.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 2, 2017, by Michael Wetter:<br/>
+Removed import statement.
+</li>
+<li>
+October 14, 2017 by Michael Wetter:<br/>
+Updated documentation and added to Annex 60 library.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
+</li>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowJunction;
diff --git a/AixLib/Fluid/FixedResistances/Examples/HydraulicDiameter.mo b/AixLib/Fluid/FixedResistances/Examples/HydraulicDiameter.mo
index 8ed1c7c80e..d086e8c8da 100644
--- a/AixLib/Fluid/FixedResistances/Examples/HydraulicDiameter.mo
+++ b/AixLib/Fluid/FixedResistances/Examples/HydraulicDiameter.mo
@@ -62,23 +62,23 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Examples/HydraulicDiameter.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example model for a fixed resistance that takes as a parameter the hydraulic diameter.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2018, by Michael Wetter:<br/>
- Updated example to add a large diameter pipe, and to use water.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1026\">#1026</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example model for a fixed resistance that takes as a parameter the hydraulic diameter.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2018, by Michael Wetter:<br/>
+Updated example to add a large diameter pipe, and to use water.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1026\">#1026</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HydraulicDiameter;
diff --git a/AixLib/Fluid/FixedResistances/Examples/PlugFlowPipe.mo b/AixLib/Fluid/FixedResistances/Examples/PlugFlowPipe.mo
index aa4bdac249..38a4da24f4 100644
--- a/AixLib/Fluid/FixedResistances/Examples/PlugFlowPipe.mo
+++ b/AixLib/Fluid/FixedResistances/Examples/PlugFlowPipe.mo
@@ -126,20 +126,20 @@ equation
         "Simulate and Plot"),
     experiment(StopTime=1000, Tolerance=1e-006),
     Documentation(info="<html>
- <p>Basic test of model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
- AixLib.Fluid.FixedResistances.PlugFlowPipe</a> with and without outlet mixing volume.
- This test includes an inlet temperature step under a constant mass flow rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>July 27, 2021 by Baptiste Ravache<br/>Add case without mixing volume</li>
- </ul>
- <ul>
- <li>September 8, 2017 by Bram van der Heijde<br/>First implementation</li>
- </ul>
- </html>"),
+<p>Basic test of model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
+AixLib.Fluid.FixedResistances.PlugFlowPipe</a> with and without outlet mixing volume.
+This test includes an inlet temperature step under a constant mass flow rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>July 27, 2021 by Baptiste Ravache<br/>Add case without mixing volume</li>
+</ul>
+<ul>
+<li>September 8, 2017 by Bram van der Heijde<br/>First implementation</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(extent={{-120,-100},{120,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowPipe;
diff --git a/AixLib/Fluid/FixedResistances/Examples/PlugFlowPipeDiscretized.mo b/AixLib/Fluid/FixedResistances/Examples/PlugFlowPipeDiscretized.mo
index 40f75969da..e9bcfe5b3c 100644
--- a/AixLib/Fluid/FixedResistances/Examples/PlugFlowPipeDiscretized.mo
+++ b/AixLib/Fluid/FixedResistances/Examples/PlugFlowPipeDiscretized.mo
@@ -70,18 +70,18 @@ equation
         "Simulate and Plot"),
     experiment(StopTime=1000, Tolerance=1e-006),
     Documentation(info="<html>
- <p>Basic test of model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipeDiscretized\">
- AixLib.Fluid.FixedResistances.PlugFlowPipeDiscretized</a>.
- This test includes an inlet temperature step under a constant mass flow rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 9, 2021, by Baptiste Ravache:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>Basic test of model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipeDiscretized\">
+AixLib.Fluid.FixedResistances.PlugFlowPipeDiscretized</a>.
+This test includes an inlet temperature step under a constant mass flow rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 9, 2021, by Baptiste Ravache:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowPipeDiscretized;
diff --git a/AixLib/Fluid/FixedResistances/Examples/PressureDrop.mo b/AixLib/Fluid/FixedResistances/Examples/PressureDrop.mo
index 3a2dfc66ed..42b661f99b 100644
--- a/AixLib/Fluid/FixedResistances/Examples/PressureDrop.mo
+++ b/AixLib/Fluid/FixedResistances/Examples/PressureDrop.mo
@@ -48,18 +48,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Examples/PressureDrop.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Example model for a fixed resistance that takes as a parameter the
- pressure drop at nominal condition.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example model for a fixed resistance that takes as a parameter the
+pressure drop at nominal condition.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureDrop;
diff --git a/AixLib/Fluid/FixedResistances/HydraulicDiameter.mo b/AixLib/Fluid/FixedResistances/HydraulicDiameter.mo
index 8e2f0513d0..f7838829cf 100644
--- a/AixLib/Fluid/FixedResistances/HydraulicDiameter.mo
+++ b/AixLib/Fluid/FixedResistances/HydraulicDiameter.mo
@@ -25,7 +25,7 @@ model HydraulicDiameter "Fixed flow resistance with hydraulic diameter and m_flo
     "Factor to take into account resistance of bends etc., fac=dp_nominal/dpStraightPipe_nominal";
 
   final parameter Modelica.Units.SI.PressureDifference dpStraightPipe_nominal(
-      displayUnit="Pa")=
+      displayUnit="Pa") =
     Modelica.Fluid.Pipes.BaseClasses.WallFriction.Detailed.pressureLoss_m_flow(
     m_flow=m_flow_nominal,
     rho_a=rho_default,
@@ -60,138 +60,138 @@ protected
 
 annotation (defaultComponentName="res",
 Documentation(info="<html>
- <p>
- This is a model of a flow resistance with a fixed flow coefficient.
- The mass flow rate is computed as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- m&#775; = k
- &radic;<span style=\"text-decoration:overline;\">&Delta;P</span>,
- </p>
- <p>
- where
- <i>k</i> is a constant and
- <i>&Delta;P</i> is the pressure drop.
- The constant <i>k</i> is equal to
- <code>k=m_flow_nominal/sqrt(dp_nominal)</code>,
- where <code>m_flow_nominal</code> is a parameter.
- </p>
- <h4>Assumptions</h4>
- <p>
- In the region
- <code>abs(m_flow) &lt; m_flow_turbulent</code>,
- the square root is replaced by a differentiable function
- with finite slope.
- The value of <code>m_flow_turbulent</code> is
- computed as
- <code>m_flow_turbulent = eta_nominal*dh/4*&pi;*ReC</code>,
- where
- <code>eta_nominal</code> is the dynamic viscosity, obtained from
- the medium model. The parameter
- <code>dh</code> is the hydraulic diameter and
- <code>ReC=4000</code> is the critical Reynolds number, which both
- can be set by the user.
- </p>
- <h4>Important parameters</h4>
- <p>
- By default, the pressure drop at nominal flow rate is computed as
- </p>
- <pre>
- dp_nominal = fac * dpStraightPipe_nominal,
- </pre>
- <p>
- where <code>dpStraightPipe_nominal</code> is a parameter that is automatically computed
- based on the
- nominal mass flow rate, hydraulic diameter, pipe roughness and medium properties.
- The hydraulic diameter <code>dh</code> is by default
- computed based on the flow velocity <code>v_nominal</code> and the nominal
- mass flow rate <code>m_flow_nominal</code>. Hence, users should change the
- default values of <code>dh</code> or <code>v_nominal</code>
- if they are not applicable for their model.
- </p>
- <p>
- The factor <code>fac</code> takes into account additional resistances such as
- for bends. The default value of <code>2</code> can be changed by the user.
- </p>
- <p>
- The parameter <code>from_dp</code> is used to determine
- whether the mass flow rate is computed as a function of the
- pressure drop (if <code>from_dp=true</code>), or vice versa.
- This setting can affect the size of the nonlinear system of equations.
- </p>
- <p>
- If the parameter <code>linearized</code> is set to <code>true</code>,
- then the pressure drop is computed as a linear function of the
- mass flow rate.
- </p>
- <p>
- Setting <code>allowFlowReversal=false</code> can lead to simpler
- equations. However, this should only be set to <code>false</code>
- if one can guarantee that the flow never reverses its direction.
- This can be difficult to guarantee, as pressure imbalance after
- the initialization, or due to medium expansion and contraction,
- can lead to reverse flow.
- </p>
- <p>
- If the parameter
- <code>show_T</code> is set to <code>true</code>,
- then the model will compute the
- temperature at its ports. Note that this can lead to state events
- when the mass flow rate approaches zero,
- which can increase computing time.
- </p>
- <h4>Notes</h4>
- <p>
- For more detailed models that compute the actual flow friction,
- models from the package
- <a href=\"modelica://Modelica.Fluid\">
- Modelica.Fluid</a>
- can be used and combined with models from the
- <code>AixLib</code> library.
- </p>
- <p>
- For a model that uses <code>dp_nominal</code> as a parameter rather than
- geoemetric data, use
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
- AixLib.Fluid.FixedResistances.PressureDrop</a>.
- </p>
- <h4>Implementation</h4>
- <p>
- The pressure drop is computed by calling a function in the package
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels\">
- AixLib.Fluid.BaseClasses.FlowModels</a>,
- This package contains regularized implementations of the equation
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   m = sign(&Delta;p) k  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
- </p>
- <p>
- and its inverse function.
- </p>
- <p>
- To decouple the energy equation from the mass equations,
- the pressure drop is a function of the mass flow rate,
- and not the volume flow rate.
- This leads to simpler equations.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2021, by Michael Wetter:<br/>
- Corrected typo in comments.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1525\">#1525</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- </ul>
- </html>"),
+<p>
+This is a model of a flow resistance with a fixed flow coefficient.
+The mass flow rate is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+m&#775; = k
+&radic;<span style=\"text-decoration:overline;\">&Delta;p</span>,
+</p>
+<p>
+where
+<i>k</i> is a constant and
+<i>&Delta;p</i> is the pressure drop.
+The constant <i>k</i> is equal to
+<code>k=m_flow_nominal/sqrt(dp_nominal)</code>,
+where <code>m_flow_nominal</code> is a parameter.
+</p>
+<h4>Assumptions</h4>
+<p>
+In the region
+<code>abs(m_flow) &lt; m_flow_turbulent</code>,
+the square root is replaced by a differentiable function
+with finite slope.
+The value of <code>m_flow_turbulent</code> is
+computed as
+<code>m_flow_turbulent = eta_nominal*dh/4*&pi;*ReC</code>,
+where
+<code>eta_nominal</code> is the dynamic viscosity, obtained from
+the medium model. The parameter
+<code>dh</code> is the hydraulic diameter and
+<code>ReC=4000</code> is the critical Reynolds number, which both
+can be set by the user.
+</p>
+<h4>Important parameters</h4>
+<p>
+By default, the pressure drop at nominal flow rate is computed as
+</p>
+<pre>
+dp_nominal = fac * dpStraightPipe_nominal,
+</pre>
+<p>
+where <code>dpStraightPipe_nominal</code> is a parameter that is automatically computed
+based on the
+nominal mass flow rate, hydraulic diameter, pipe roughness and medium properties.
+The hydraulic diameter <code>dh</code> is by default
+computed based on the flow velocity <code>v_nominal</code> and the nominal
+mass flow rate <code>m_flow_nominal</code>. Hence, users should change the
+default values of <code>dh</code> or <code>v_nominal</code>
+if they are not applicable for their model.
+</p>
+<p>
+The factor <code>fac</code> takes into account additional resistances such as
+for bends. The default value of <code>2</code> can be changed by the user.
+</p>
+<p>
+The parameter <code>from_dp</code> is used to determine
+whether the mass flow rate is computed as a function of the
+pressure drop (if <code>from_dp=true</code>), or vice versa.
+This setting can affect the size of the nonlinear system of equations.
+</p>
+<p>
+If the parameter <code>linearized</code> is set to <code>true</code>,
+then the pressure drop is computed as a linear function of the
+mass flow rate.
+</p>
+<p>
+Setting <code>allowFlowReversal=false</code> can lead to simpler
+equations. However, this should only be set to <code>false</code>
+if one can guarantee that the flow never reverses its direction.
+This can be difficult to guarantee, as pressure imbalance after
+the initialization, or due to medium expansion and contraction,
+can lead to reverse flow.
+</p>
+<p>
+If the parameter
+<code>show_T</code> is set to <code>true</code>,
+then the model will compute the
+temperature at its ports. Note that this can lead to state events
+when the mass flow rate approaches zero,
+which can increase computing time.
+</p>
+<h4>Notes</h4>
+<p>
+For more detailed models that compute the actual flow friction,
+models from the package
+<a href=\"modelica://Modelica.Fluid\">
+Modelica.Fluid</a>
+can be used and combined with models from the
+<code>AixLib</code> library.
+</p>
+<p>
+For a model that uses <code>dp_nominal</code> as a parameter rather than
+geoemetric data, use
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
+AixLib.Fluid.FixedResistances.PressureDrop</a>.
+</p>
+<h4>Implementation</h4>
+<p>
+The pressure drop is computed by calling a function in the package
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels\">
+AixLib.Fluid.BaseClasses.FlowModels</a>,
+This package contains regularized implementations of the equation
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  m&#775; = sign(&Delta;p) k  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
+</p>
+<p>
+and its inverse function.
+</p>
+<p>
+To decouple the energy equation from the mass equations,
+the pressure drop is a function of the mass flow rate,
+and not the volume flow rate.
+This leads to simpler equations.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2021, by Michael Wetter:<br/>
+Corrected typo in comments.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1525\">#1525</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+</ul>
+</html>"),
   Icon(graphics={Text(
           extent={{-40,18},{38,-20}},
           textColor={255,255,255},
-          textString="dh")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="dh")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HydraulicDiameter;
diff --git a/AixLib/Fluid/FixedResistances/Junction.mo b/AixLib/Fluid/FixedResistances/Junction.mo
index a6d4663f67..4a33e37427 100644
--- a/AixLib/Fluid/FixedResistances/Junction.mo
+++ b/AixLib/Fluid/FixedResistances/Junction.mo
@@ -112,114 +112,114 @@ initial equation
           fillPattern=FillPattern.Solid)}),
 defaultComponentName="jun",
     Documentation(info="<html>
- <p>
- Model of a flow junction with an optional fixed resistance in each flow leg
- and an optional mixing volume at the junction.
- </p>
- <p>
- The pressure drop is implemented using the model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
- AixLib.Fluid.FixedResistances.PressureDrop</a>.
- If its nominal pressure drop is set to zero, then the pressure drop
- model will be removed.
- For example, the pressure drop declaration
- </p>
- <pre>
-   m_flow_nominal={ 0.1, 0.1,  -0.2},
-   dp_nominal =   {500,    0, -6000}
- </pre>
- <p>
- would model a flow mixer that has the nominal flow rates and associated pressure drops
- as shown in the figure below. Note that <code>port_3</code> is set to negative values.
- The negative values indicate that at the nominal conditions, fluid is leaving the component.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Junction.png\"/>
- </p>
- <p>
- If
- <code>energyDynamics &lt;&gt; Modelica.Fluid.Types.Dynamics.SteadyState</code>,
- then at the flow junction, a fluid volume is modeled.
- The fluid volume is implemented using the model
- <a href=\"modelica://AixLib.Fluid.Delays.DelayFirstOrder\">
- AixLib.Fluid.Delays.DelayFirstOrder</a>.
- The fluid volume has the size
- </p>
- <pre>
-   V = sum(abs(m_flow_nominal[:])/3)*tau/rho_nominal
- </pre>
- <p>
- where <code>tau</code> is a parameter and <code>rho_nominal</code> is the density
- of the medium in the volume at nominal condition.
- Setting <code>energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial</code>
- can help reducing the size of the nonlinear
- system of equations.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- February 26, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- March 26, 2018 by Filip Jorissen:<br/>
- Removed <code>final allowFlowReversal=true</code> from all resistances
- since this overrides the default simplification when the flow
- is not bidirectional.
- This change can lead to smaller algebraic loops.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/898\">issue 898</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- Renamed model from <code>SplitterFixedResistanceDpM</code> to
- <code>FlowJunction</code> and removed the parameters
- <code>use_dh</code>, <code>dh</code> and <code>ReC</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
- </li>
- <li>
- October 14, 2016 by Michael Wetter:<br/>
- Added to Annex 60 library.<br/>
- Updated comment for parameter <code>use_dh</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
- </li>
- <li>
- Removed parameter <code>dynamicBalance</code> that overwrote the setting
- of <code>energyDynamics</code> and <code>massDynamics</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/411\">
- Annex 60, issue 411</a>.
- </li>
- <li>
- February 1, 2012 by Michael Wetter:<br/>
- Expanded documentation.
- </li>
- <li>
- August 4, 2011 by Michael Wetter:<br/>
- Added <code>final allowFlowReversal=true</code> to all resistances since it is impractical
- to avoid flow reversal in large flow networks where such a setting may be useful.
- </li>
- <li>
- June 11, 2008 by Michael Wetter:<br/>
- Based class on
- <a href=\"modelica://AixLib.Fluid.BaseClasses.PartialThreeWayFixedResistance\">
- AixLib.Fluid.BaseClasses.PartialThreeWayFixedResistance</a>.
- </li>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model of a flow junction with an optional fixed resistance in each flow leg
+and an optional mixing volume at the junction.
+</p>
+<p>
+The pressure drop is implemented using the model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PressureDrop\">
+AixLib.Fluid.FixedResistances.PressureDrop</a>.
+If its nominal pressure drop is set to zero, then the pressure drop
+model will be removed.
+For example, the pressure drop declaration
+</p>
+<pre>
+  m_flow_nominal={ 0.1, 0.1,  -0.2},
+  dp_nominal =   {500,    0, -6000}
+</pre>
+<p>
+would model a flow mixer that has the nominal flow rates and associated pressure drops
+as shown in the figure below. Note that <code>port_3</code> is set to negative values.
+The negative values indicate that at the nominal conditions, fluid is leaving the component.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Junction.png\"/>
+</p>
+<p>
+If
+<code>energyDynamics &lt;&gt; Modelica.Fluid.Types.Dynamics.SteadyState</code>,
+then at the flow junction, a fluid volume is modeled.
+The fluid volume is implemented using the model
+<a href=\"modelica://AixLib.Fluid.Delays.DelayFirstOrder\">
+AixLib.Fluid.Delays.DelayFirstOrder</a>.
+The fluid volume has the size
+</p>
+<pre>
+  V = sum(abs(m_flow_nominal[:])/3)*tau/rho_nominal
+</pre>
+<p>
+where <code>tau</code> is a parameter and <code>rho_nominal</code> is the density
+of the medium in the volume at nominal condition.
+Setting <code>energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial</code>
+can help reducing the size of the nonlinear
+system of equations.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+February 26, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+March 26, 2018 by Filip Jorissen:<br/>
+Removed <code>final allowFlowReversal=true</code> from all resistances
+since this overrides the default simplification when the flow
+is not bidirectional.
+This change can lead to smaller algebraic loops.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/898\">issue 898</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+Renamed model from <code>SplitterFixedResistanceDpM</code> to
+<code>FlowJunction</code> and removed the parameters
+<code>use_dh</code>, <code>dh</code> and <code>ReC</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
+</li>
+<li>
+October 14, 2016 by Michael Wetter:<br/>
+Added to Annex 60 library.<br/>
+Updated comment for parameter <code>use_dh</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
+</li>
+<li>
+Removed parameter <code>dynamicBalance</code> that overwrote the setting
+of <code>energyDynamics</code> and <code>massDynamics</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/411\">
+Annex 60, issue 411</a>.
+</li>
+<li>
+February 1, 2012 by Michael Wetter:<br/>
+Expanded documentation.
+</li>
+<li>
+August 4, 2011 by Michael Wetter:<br/>
+Added <code>final allowFlowReversal=true</code> to all resistances since it is impractical
+to avoid flow reversal in large flow networks where such a setting may be useful.
+</li>
+<li>
+June 11, 2008 by Michael Wetter:<br/>
+Based class on
+<a href=\"modelica://AixLib.Fluid.BaseClasses.PartialThreeWayFixedResistance\">
+AixLib.Fluid.BaseClasses.PartialThreeWayFixedResistance</a>.
+</li>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Junction;
diff --git a/AixLib/Fluid/FixedResistances/LosslessPipe.mo b/AixLib/Fluid/FixedResistances/LosslessPipe.mo
index 3d11ebe74c..a729d2a82b 100644
--- a/AixLib/Fluid/FixedResistances/LosslessPipe.mo
+++ b/AixLib/Fluid/FixedResistances/LosslessPipe.mo
@@ -31,32 +31,32 @@ equation
           fillColor={217,236,255})}),
 defaultComponentName="pip",
     Documentation(info="<html>
- <p>
- Model of a pipe with no flow resistance, no heat loss and no transport delay.
- This model can be used to replace a <code>replaceable</code> pipe model
- in flow legs in which no friction should be modeled.
- This is for example done in the outlet port of the
- base class for three way valves,
- <a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
- AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>.
- </p>
- </html>",
+<p>
+Model of a pipe with no flow resistance, no heat loss and no transport delay.
+This model can be used to replace a <code>replaceable</code> pipe model
+in flow legs in which no friction should be modeled.
+This is for example done in the outlet port of the
+base class for three way valves,
+<a href=\"modelica://AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve\">
+AixLib.Fluid.Actuators.BaseClasses.PartialThreeWayValve</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 23, 2018, by Filip Jorissen:<br/>
- Implementation is now more efficient for <code>allowFlowReversal=false</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/949\">#949</a>.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Removed parameter <code>show_V_flow</code>.
- </li>
- <li>
- June 13, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 23, 2018, by Filip Jorissen:<br/>
+Implementation is now more efficient for <code>allowFlowReversal=false</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/949\">#949</a>.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Removed parameter <code>show_V_flow</code>.
+</li>
+<li>
+June 13, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LosslessPipe;
diff --git a/AixLib/Fluid/FixedResistances/PlugFlowPipe.mo b/AixLib/Fluid/FixedResistances/PlugFlowPipe.mo
index a391701fa2..745a003249 100644
--- a/AixLib/Fluid/FixedResistances/PlugFlowPipe.mo
+++ b/AixLib/Fluid/FixedResistances/PlugFlowPipe.mo
@@ -60,118 +60,118 @@ model PlugFlowPipe
           textColor={0,0,0},
           textString="L = %length")}),
     Documentation(revisions="<html>
- <ul>
- <li>
- October 05, 2021, by Baptiste Ravache:<br/>
- Made model symmetrical and extends from
- <a href=\"AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
- AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>.
- </li>
- <li>
- September 14, 2021, by Michael Wetter:<br/>
- Made most instances protected and exposed main variables of interest.
- </li>
- <li>
- July 9, 2021, by Baptiste Ravache:<br/>
- Replaced the vectorized outlet port <code>ports_b</code> with
- a single outlet port <code>port_b</code>.<br/>
- Expanded the core pipe model that was previously a component.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1494\">IBPSA, #1494</a>.<br/>
- This change is not backward compatible.<br/>
- The previous classes definitions were moved to
- <a href=\"modelica://AixLib.Obsolete.Fluid.FixedResistances.PlugFlowPipe\">
- AixLib.Obsolete.Fluid.FixedResistances.PlugFlowPipe</a>.
- <a href=\"modelica://AixLib.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore\">
- AixLib.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore</a>.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Pipe with heat loss using the time delay based heat losses and transport
- of the fluid using a plug flow model, applicable for simulation of long
- pipes such as in district heating and cooling systems.</p>
- <p>
- This model takes into account transport delay along the pipe length idealized
- as a plug flow.
- The model also includes thermal inertia of the pipe wall.
- </p>
- <h4>Implementation</h4>
- <p>
- The
- <code>spatialDistribution</code> operator is used for the temperature wave propagation
- through the length of the pipe. This operator is contained in
- <a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow\">
- AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow</a>.
- </p>
- <p>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlowHeatLoss\">
- AixLib.Fluid.FixedResistances.BaseClasses.PlugFlowHeatLoss</a>
- implements a heat loss in design direction, but leaves the enthalpy unchanged
- in opposite flow direction. Therefore it is used in front of and behind the time delay.
- </p>
- <p>
- The pressure drop is implemented using
- <a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
- AixLib.Fluid.FixedResistances.HydraulicDiameter</a>.
- </p>
- <p>
- The thermal capacity of the pipe wall is implemented as a mixing volume
- of the fluid in the pipe, of which the thermal capacity is equal to that
- of the pipe wall material.
- In addition, this mixing volume allows the hydraulic separation of subsequent pipes.
- <br/>
- The mixing volume is either split between the inlet and outlet ports
- (port_a and port_b) or lumped in at the outlet (port_b)
- if <code>have_symmetry</code> is set to false.
- This mixing volume can be removed from this model with the Boolean parameter
- <code>have_pipCap</code>, in cases where the pipe wall heat capacity
- is negligible and a state is not needed at the pipe outlet
- (see the note below about numerical Jacobians).
- </p>
- <p>
- Note that in order to model a branched network it is recommended to use
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Junction\">
- AixLib.Fluid.FixedResistances.Junction</a> at each junction and to configure
- that junction model with a state
- (<code>energyDynamics &lt;&gt; Modelica.Fluid.Types.Dynamics.SteadyState</code>),
- see for instance
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>.
- This will avoid the numerical Jacobian that is otherwise created when
- the inlet ports of two instances of the plug flow model are connected together.
- </p>
- <h4>Assumptions</h4>
- <ul>
- <li>
- Heat losses are for steady-state operation.
- </li>
- <li>
- The axial heat diffusion in the fluid, the pipe wall and the ground are neglected.
- </li>
- <li>
- The boundary temperature is uniform.
- </li>
- <li>
- The thermal inertia of the pipe wall material is lumped on the side of the pipe
- that is connected to <code>port_b</code>.
- </li>
- </ul>
- <h4>References</h4>
- <p>
- Full details on the model implementation and experimental validation can be found
- in:
- </p>
- <p>
- van der Heijde, B., Fuchs, M., Ribas Tugores, C., Schweiger, G., Sartor, K.,
- Basciotti, D., M&uuml;ller, D., Nytsch-Geusen, C., Wetter, M. and Helsen, L.
- (2017).<br/>
- Dynamic equation-based thermo-hydraulic pipe model for district heating and
- cooling systems.<br/>
- <i>Energy Conversion and Management</i>, vol. 151, p. 158-169.
- <a href=\"https://doi.org/10.1016/j.enconman.2017.08.072\">doi:
- 10.1016/j.enconman.2017.08.072</a>.</p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 05, 2021, by Baptiste Ravache:<br/>
+Made model symmetrical and extends from
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>.
+</li>
+<li>
+September 14, 2021, by Michael Wetter:<br/>
+Made most instances protected and exposed main variables of interest.
+</li>
+<li>
+July 9, 2021, by Baptiste Ravache:<br/>
+Replaced the vectorized outlet port <code>ports_b</code> with
+a single outlet port <code>port_b</code>.<br/>
+Expanded the core pipe model that was previously a component.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1494\">IBPSA, #1494</a>.<br/>
+This change is not backward compatible.<br/>
+The previous classes definitions were moved to
+<a href=\"modelica://AixLib.Obsolete.Fluid.FixedResistances.PlugFlowPipe\">
+AixLib.Obsolete.Fluid.FixedResistances.PlugFlowPipe</a>.
+<a href=\"modelica://AixLib.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore\">
+AixLib.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore</a>.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Pipe with heat loss using the time delay based heat losses and transport
+of the fluid using a plug flow model, applicable for simulation of long
+pipes such as in district heating and cooling systems.</p>
+<p>
+This model takes into account transport delay along the pipe length idealized
+as a plug flow.
+The model also includes thermal inertia of the pipe wall.
+</p>
+<h4>Implementation</h4>
+<p>
+The
+<code>spatialDistribution</code> operator is used for the temperature wave propagation
+through the length of the pipe. This operator is contained in
+<a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow\">
+AixLib.Fluid.FixedResistances.BaseClasses.PlugFlow</a>.
+</p>
+<p>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.BaseClasses.PlugFlowHeatLoss\">
+AixLib.Fluid.FixedResistances.BaseClasses.PlugFlowHeatLoss</a>
+implements a heat loss in design direction, but leaves the enthalpy unchanged
+in opposite flow direction. Therefore it is used in front of and behind the time delay.
+</p>
+<p>
+The pressure drop is implemented using
+<a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
+AixLib.Fluid.FixedResistances.HydraulicDiameter</a>.
+</p>
+<p>
+The thermal capacity of the pipe wall is implemented as a mixing volume
+of the fluid in the pipe, of which the thermal capacity is equal to that
+of the pipe wall material.
+In addition, this mixing volume allows the hydraulic separation of subsequent pipes.
+<br/>
+The mixing volume is either split between the inlet and outlet ports
+(port_a and port_b) or lumped in at the outlet (port_b)
+if <code>have_symmetry</code> is set to false.
+This mixing volume can be removed from this model with the Boolean parameter
+<code>have_pipCap</code>, in cases where the pipe wall heat capacity
+is negligible and a state is not needed at the pipe outlet
+(see the note below about numerical Jacobians).
+</p>
+<p>
+Note that in order to model a branched network it is recommended to use
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Junction\">
+AixLib.Fluid.FixedResistances.Junction</a> at each junction and to configure
+that junction model with a state
+(<code>energyDynamics &lt;&gt; Modelica.Fluid.Types.Dynamics.SteadyState</code>),
+see for instance
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>.
+This will avoid the numerical Jacobian that is otherwise created when
+the inlet ports of two instances of the plug flow model are connected together.
+</p>
+<h4>Assumptions</h4>
+<ul>
+<li>
+Heat losses are for steady-state operation.
+</li>
+<li>
+The axial heat diffusion in the fluid, the pipe wall and the ground are neglected.
+</li>
+<li>
+The boundary temperature is uniform.
+</li>
+<li>
+The thermal inertia of the pipe wall material is lumped on the side of the pipe
+that is connected to <code>port_b</code>.
+</li>
+</ul>
+<h4>References</h4>
+<p>
+Full details on the model implementation and experimental validation can be found
+in:
+</p>
+<p>
+van der Heijde, B., Fuchs, M., Ribas Tugores, C., Schweiger, G., Sartor, K.,
+Basciotti, D., M&uuml;ller, D., Nytsch-Geusen, C., Wetter, M. and Helsen, L.
+(2017).<br/>
+Dynamic equation-based thermo-hydraulic pipe model for district heating and
+cooling systems.<br/>
+<i>Energy Conversion and Management</i>, vol. 151, p. 158-169.
+<a href=\"https://doi.org/10.1016/j.enconman.2017.08.072\">doi:
+10.1016/j.enconman.2017.08.072</a>.</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowPipe;
diff --git a/AixLib/Fluid/FixedResistances/PlugFlowPipeDiscretized.mo b/AixLib/Fluid/FixedResistances/PlugFlowPipeDiscretized.mo
index ce2870ad61..bbb715cfc4 100644
--- a/AixLib/Fluid/FixedResistances/PlugFlowPipeDiscretized.mo
+++ b/AixLib/Fluid/FixedResistances/PlugFlowPipeDiscretized.mo
@@ -14,11 +14,11 @@ model PlugFlowPipeDiscretized
 
   parameter Boolean have_pipCap=true
     "= true, a mixing volume is added to each segment that corresponds 
-     to the heat capacity of the pipe segment wall"
+    to the heat capacity of the pipe segment wall"
     annotation (Dialog(tab="Advanced"));
   parameter Boolean have_symmetry=true
     "= false, the mixing volume is only on port_b of each segment,
-     which improve performances, but reduces dynamic accuracy"
+    which improve performances, but reduces dynamic accuracy"
     annotation (Dialog(tab="Advanced", enable=have_pipCap));
 
   parameter Modelica.Units.SI.Length dh "Hydraulic diameter"
@@ -249,30 +249,30 @@ equation
           color={162,29,33},
           thickness=0.5)}),
     Documentation(revisions="<html>
- <ul>
- <li>
- May 17, 2021, by Baptiste Ravache:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Wrapper around <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
- AixLib.Fluid.FixedResistances.PlugFlowPipe</a> which allows to specify <code>nSeg</code>
- successive segments of pipes (connected in series).
- </p>
- <p>
- This wrapper simplifies use-cases where different segments of the same
- pipe might have different boundary conditions. This would be the case,
- for instance, for sufficiently long stretches of buried pipes.
- </p>
- <p>
- To reduce coupled nonlinear equations, the pipe flow resistance
- is aggregated to a single instance of
- <a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
- AixLib.Fluid.FixedResistances.HydraulicDiameter</a> rather than being
- instantiated separately for each segment.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 17, 2021, by Baptiste Ravache:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Wrapper around <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
+AixLib.Fluid.FixedResistances.PlugFlowPipe</a> which allows to specify <code>nSeg</code>
+successive segments of pipes (connected in series).
+</p>
+<p>
+This wrapper simplifies use-cases where different segments of the same
+pipe might have different boundary conditions. This would be the case,
+for instance, for sufficiently long stretches of buried pipes.
+</p>
+<p>
+To reduce coupled nonlinear equations, the pipe flow resistance
+is aggregated to a single instance of
+<a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
+AixLib.Fluid.FixedResistances.HydraulicDiameter</a> rather than being
+instantiated separately for each segment.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowPipeDiscretized;
diff --git a/AixLib/Fluid/FixedResistances/PressureDrop.mo b/AixLib/Fluid/FixedResistances/PressureDrop.mo
index 40b0b1b34b..53fd7e1ccb 100644
--- a/AixLib/Fluid/FixedResistances/PressureDrop.mo
+++ b/AixLib/Fluid/FixedResistances/PressureDrop.mo
@@ -74,185 +74,185 @@ equation
 
   annotation (defaultComponentName="res",
 Documentation(info="<html>
- <p>
- Model of a flow resistance with a fixed flow coefficient.
- The mass flow rate is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- m&#775; = k
- &radic;<span style=\"text-decoration:overline;\">&Delta;P</span>,
- </p>
- <p>
- where
- <i>k</i> is a constant and
- <i>&Delta;P</i> is the pressure drop.
- The constant <i>k</i> is equal to
- <code>k=m_flow_nominal/sqrt(dp_nominal)</code>,
- where <code>m_flow_nominal</code> and <code>dp_nominal</code>
- are parameters.
- </p>
- <h4>Assumptions</h4>
- <p>
- In the region
- <code>abs(m_flow) &lt; m_flow_turbulent</code>,
- the square root is replaced by a differentiable function
- with finite slope.
- The value of <code>m_flow_turbulent</code> is
- computed as
- <code>m_flow_turbulent = deltaM * abs(m_flow_nominal)</code>,
- where <code>deltaM=0.3</code> and
- <code>m_flow_nominal</code> are parameters that can be set by the user.
- </p>
- <p>
- The figure below shows the pressure drop for the parameters
- <code>m_flow_nominal=5</code> kg/s,
- <code>dp_nominal=10</code> Pa and
- <code>deltaM=0.3</code>.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/PressureDrop.png\"/>
- </p>
- <h4>Important parameters</h4>
- <p>
- The parameter <code>from_dp</code> is used to determine
- whether the mass flow rate is computed as a function of the
- pressure drop (if <code>from_dp=true</code>), or vice versa.
- This setting can affect the size of the nonlinear system of equations.
- </p>
- <p>
- If the parameter <code>linearized</code> is set to <code>true</code>,
- then the pressure drop is computed as a linear function of the
- mass flow rate.
- </p>
- <p>
- Setting <code>allowFlowReversal=false</code> can lead to simpler
- equations. However, this should only be set to <code>false</code>
- if one can guarantee that the flow never reverses its direction.
- This can be difficult to guarantee, as pressure imbalance after
- the initialization, or due to medium expansion and contraction,
- can lead to reverse flow.
- </p>
- <p>
- If the parameter
- <code>show_T</code> is set to <code>true</code>,
- then the model will compute the
- temperature at its ports. Note that this can lead to state events
- when the mass flow rate approaches zero,
- which can increase computing time.
- </p>
- <h4>Notes</h4>
- <p>
- For more detailed models that compute the actual flow friction,
- models from the package
- <a href=\"modelica://Modelica.Fluid\">
- Modelica.Fluid</a>
- can be used and combined with models from the
- <code>AixLib</code> library.
- </p>
- <p>
- For a model that uses the hydraulic parameter and flow velocity at nominal conditions
- as a parameter, use
- <a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
- AixLib.Fluid.FixedResistances.HydraulicDiameter</a>.
- </p>
- <h4>Implementation</h4>
- <p>
- The pressure drop is computed by calling a function in the package
- <a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels\">
- AixLib.Fluid.BaseClasses.FlowModels</a>,
- This package contains regularized implementations of the equation
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   m = sign(&Delta;p) k  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
- </p>
- <p>
- and its inverse function.
- </p>
- <p>
- To decouple the energy equation from the mass equations,
- the pressure drop is a function of the mass flow rate,
- and not the volume flow rate.
- This leads to simpler equations.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2018, by Michael Wetter:<br/>
- Decrease value of <code>deltaM(min=...)</code> attribute.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1026\">#1026</a>.
- </li>
- <li>
- February 3, 2018, by Filip Jorissen:<br/>
- Revised implementation of pressure drop equation
- such that it depends on <code>from_dp</code>
- when <code>linearized=true</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/884\">#884</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- Simplified model by removing the geometry dependent parameters into the new
- model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
- AixLib.Fluid.FixedResistances.HydraulicDiameter</a>.
- </li>
- <li>
- November 23, 2016, by Filip Jorissen:<br/>
- Removed <code>dp_nominal</code> and
- <code>m_flow_nominal</code> labels from icon.
- </li>
- <li>
- October 14, 2016, by Michael Wetter:<br/>
- Updated comment for parameter <code>use_dh</code>.
- </li>
- <li>
- November 26, 2014, by Michael Wetter:<br/>
- Added the required <code>annotation(Evaluate=true)</code> so
- that the system of nonlinear equations in
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PressureDropsExplicit\">
- AixLib.Fluid.FixedResistances.Validation.PressureDropsExplicit</a>
- remains the same.
- </li>
- <li>
- November 20, 2014, by Michael Wetter:<br/>
- Rewrote the warning message using an <code>assert</code> with
- <code>AssertionLevel.warning</code>
- as this is the proper way to write warnings in Modelica.
- </li>
- <li>
- August 5, 2014, by Michael Wetter:<br/>
- Corrected error in documentation of computation of <code>k</code>.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Removed parameter <code>show_V_flow</code>.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>
- January 16, 2012 by Michael Wetter:<br/>
- To simplify object inheritance tree, revised base classes
- <code>AixLib.Fluid.BaseClasses.PartialResistance</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</code>,
- <code>AixLib.Fluid.Actuators.BaseClasses.PartialActuator</code>
- and model
- <code>AixLib.Fluid.FixedResistances.PressureDrop</code>.
- </li>
- <li>
- May 30, 2008 by Michael Wetter:<br/>
- Added parameters <code>use_dh</code> and <code>deltaM</code> for easier parameterization.
- </li>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model of a flow resistance with a fixed flow coefficient.
+The mass flow rate is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+m&#775; = k
+&radic;<span style=\"text-decoration:overline;\">&Delta;p</span>,
+</p>
+<p>
+where
+<i>k</i> is a constant and
+<i>&Delta;p</i> is the pressure drop.
+The constant <i>k</i> is equal to
+<code>k=m_flow_nominal/sqrt(dp_nominal)</code>,
+where <code>m_flow_nominal</code> and <code>dp_nominal</code>
+are parameters.
+</p>
+<h4>Assumptions</h4>
+<p>
+In the region
+<code>abs(m_flow) &lt; m_flow_turbulent</code>,
+the square root is replaced by a differentiable function
+with finite slope.
+The value of <code>m_flow_turbulent</code> is
+computed as
+<code>m_flow_turbulent = deltaM * abs(m_flow_nominal)</code>,
+where <code>deltaM=0.3</code> and
+<code>m_flow_nominal</code> are parameters that can be set by the user.
+</p>
+<p>
+The figure below shows the pressure drop for the parameters
+<code>m_flow_nominal=5</code> kg/s,
+<code>dp_nominal=10</code> Pa and
+<code>deltaM=0.3</code>.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/PressureDrop.png\"/>
+</p>
+<h4>Important parameters</h4>
+<p>
+The parameter <code>from_dp</code> is used to determine
+whether the mass flow rate is computed as a function of the
+pressure drop (if <code>from_dp=true</code>), or vice versa.
+This setting can affect the size of the nonlinear system of equations.
+</p>
+<p>
+If the parameter <code>linearized</code> is set to <code>true</code>,
+then the pressure drop is computed as a linear function of the
+mass flow rate.
+</p>
+<p>
+Setting <code>allowFlowReversal=false</code> can lead to simpler
+equations. However, this should only be set to <code>false</code>
+if one can guarantee that the flow never reverses its direction.
+This can be difficult to guarantee, as pressure imbalance after
+the initialization, or due to medium expansion and contraction,
+can lead to reverse flow.
+</p>
+<p>
+If the parameter
+<code>show_T</code> is set to <code>true</code>,
+then the model will compute the
+temperature at its ports. Note that this can lead to state events
+when the mass flow rate approaches zero,
+which can increase computing time.
+</p>
+<h4>Notes</h4>
+<p>
+For more detailed models that compute the actual flow friction,
+models from the package
+<a href=\"modelica://Modelica.Fluid\">
+Modelica.Fluid</a>
+can be used and combined with models from the
+<code>AixLib</code> library.
+</p>
+<p>
+For a model that uses the hydraulic parameter and flow velocity at nominal conditions
+as a parameter, use
+<a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
+AixLib.Fluid.FixedResistances.HydraulicDiameter</a>.
+</p>
+<h4>Implementation</h4>
+<p>
+The pressure drop is computed by calling a function in the package
+<a href=\"modelica://AixLib.Fluid.BaseClasses.FlowModels\">
+AixLib.Fluid.BaseClasses.FlowModels</a>,
+This package contains regularized implementations of the equation
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  m&#775; = sign(&Delta;p) k  &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
+</p>
+<p>
+and its inverse function.
+</p>
+<p>
+To decouple the energy equation from the mass equations,
+the pressure drop is a function of the mass flow rate,
+and not the volume flow rate.
+This leads to simpler equations.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2018, by Michael Wetter:<br/>
+Decrease value of <code>deltaM(min=...)</code> attribute.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1026\">#1026</a>.
+</li>
+<li>
+February 3, 2018, by Filip Jorissen:<br/>
+Revised implementation of pressure drop equation
+such that it depends on <code>from_dp</code>
+when <code>linearized=true</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/884\">#884</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+Simplified model by removing the geometry dependent parameters into the new
+model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.HydraulicDiameter\">
+AixLib.Fluid.FixedResistances.HydraulicDiameter</a>.
+</li>
+<li>
+November 23, 2016, by Filip Jorissen:<br/>
+Removed <code>dp_nominal</code> and
+<code>m_flow_nominal</code> labels from icon.
+</li>
+<li>
+October 14, 2016, by Michael Wetter:<br/>
+Updated comment for parameter <code>use_dh</code>.
+</li>
+<li>
+November 26, 2014, by Michael Wetter:<br/>
+Added the required <code>annotation(Evaluate=true)</code> so
+that the system of nonlinear equations in
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PressureDropsExplicit\">
+AixLib.Fluid.FixedResistances.Validation.PressureDropsExplicit</a>
+remains the same.
+</li>
+<li>
+November 20, 2014, by Michael Wetter:<br/>
+Rewrote the warning message using an <code>assert</code> with
+<code>AssertionLevel.warning</code>
+as this is the proper way to write warnings in Modelica.
+</li>
+<li>
+August 5, 2014, by Michael Wetter:<br/>
+Corrected error in documentation of computation of <code>k</code>.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Removed parameter <code>show_V_flow</code>.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>
+January 16, 2012 by Michael Wetter:<br/>
+To simplify object inheritance tree, revised base classes
+<code>AixLib.Fluid.BaseClasses.PartialResistance</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialTwoWayValve</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialDamperExponential</code>,
+<code>AixLib.Fluid.Actuators.BaseClasses.PartialActuator</code>
+and model
+<code>AixLib.Fluid.FixedResistances.PressureDrop</code>.
+</li>
+<li>
+May 30, 2008 by Michael Wetter:<br/>
+Added parameters <code>use_dh</code> and <code>deltaM</code> for easier parameterization.
+</li>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureDrop;
diff --git a/AixLib/Fluid/FixedResistances/Validation/FlowJunctionSteadyState.mo b/AixLib/Fluid/FixedResistances/Validation/FlowJunctionSteadyState.mo
index bef098fe32..071ed4f66a 100644
--- a/AixLib/Fluid/FixedResistances/Validation/FlowJunctionSteadyState.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/FlowJunctionSteadyState.mo
@@ -92,28 +92,28 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/FlowJunctionSteadyState.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model validates the use of the splitter and mixer model
- for different flow directions.
- The example is configured such that the flow changes its direction in
- each flow leg between <i>t = 0</i> seconds to <i>t = 100</i> seconds.
- The splitter model has been configured as a steady-state model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2017, by Michael Wetter:<br/>
- Changed <code>spl.m_flow_nominal</code>, boundary condition and enabled sensor dynamics.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/657\">issue 657</a>.
- </li>
- <li>
- October 14, 2016, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates the use of the splitter and mixer model
+for different flow directions.
+The example is configured such that the flow changes its direction in
+each flow leg between <i>t = 0</i> seconds to <i>t = 100</i> seconds.
+The splitter model has been configured as a steady-state model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2017, by Michael Wetter:<br/>
+Changed <code>spl.m_flow_nominal</code>, boundary condition and enabled sensor dynamics.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/657\">issue 657</a>.
+</li>
+<li>
+October 14, 2016, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowJunctionSteadyState;
diff --git a/AixLib/Fluid/FixedResistances/Validation/FlowJunctionSteadyStateNoPressureDrop.mo b/AixLib/Fluid/FixedResistances/Validation/FlowJunctionSteadyStateNoPressureDrop.mo
index b8fc10378d..9320ab866e 100644
--- a/AixLib/Fluid/FixedResistances/Validation/FlowJunctionSteadyStateNoPressureDrop.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/FlowJunctionSteadyStateNoPressureDrop.mo
@@ -88,29 +88,29 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/FlowJunctionSteadyStateNoPressureDrop.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model validates the use of the splitter and mixer model
- for different flow directions.
- The example is configured such that the flow changes its direction in
- each flow leg between <i>t = 0</i> seconds to <i>t = 100</i> seconds.
- The splitter model has been configured as a steady-state model,
- with no flow resistance.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2017, by Michael Wetter:<br/>
- Changed <code>spl.m_flow_nominal</code>, boundary condition and enabled sensor dynamics.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/657\">issue 657</a>.
- </li>
- <li>
- October 14, 2016, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates the use of the splitter and mixer model
+for different flow directions.
+The example is configured such that the flow changes its direction in
+each flow leg between <i>t = 0</i> seconds to <i>t = 100</i> seconds.
+The splitter model has been configured as a steady-state model,
+with no flow resistance.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2017, by Michael Wetter:<br/>
+Changed <code>spl.m_flow_nominal</code>, boundary condition and enabled sensor dynamics.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/657\">issue 657</a>.
+</li>
+<li>
+October 14, 2016, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/451\">issue 451</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowJunctionSteadyStateNoPressureDrop;
diff --git a/AixLib/Fluid/FixedResistances/Validation/LosslessPipe.mo b/AixLib/Fluid/FixedResistances/Validation/LosslessPipe.mo
index 3a0c0b3f4d..2aa07629b9 100644
--- a/AixLib/Fluid/FixedResistances/Validation/LosslessPipe.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/LosslessPipe.mo
@@ -46,17 +46,17 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/LosslessPipe.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Validation model for a the pipe model with no friction and no heat loss.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Validation model for a the pipe model with no friction and no heat loss.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LosslessPipe;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/BaseClasses/PipeDataBaseDefinition.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/BaseClasses/PipeDataBaseDefinition.mo
index 2a28eaaeac..6e88b03c2b 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/BaseClasses/PipeDataBaseDefinition.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/BaseClasses/PipeDataBaseDefinition.mo
@@ -6,38 +6,38 @@ partial record PipeDataBaseDefinition
       parameter String filNam
       "Name of data file";
       annotation(Documentation(info="<html>
- <p>
- Defines basic record of experimental data with <code>n</code> measured points.
- The first column corresponds to <code>time</code>, further columns to measured data.
- </p>
- </html>",
+<p>
+Defines basic record of experimental data with <code>n</code> measured points.
+The first column corresponds to <code>time</code>, further columns to measured data.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- Januar 19, 2016 by Carles Ribas:<br/>
- Move experiment documentation to the <a href=\"modelica://AixLib.Experimental.Pipe.Data.PipeDatauLg150801\">
- specific model</a>. Add parameter <code>n</code> to facilitate use of extends clause.
- </li>
- <li>
- October 14, 2015 by Kevin Sartor:<br/>
- Add documentation about the test bench and how is conducted the experiment
- </li>
- <li>
- October 12, 2015 by Marcus Fuchs:<br/>
- Add rudimentary documentation and integrate into experimental pipe package
- </li>
- <li>
- October 7, 2015 by Kevin Sartor:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+Januar 19, 2016 by Carles Ribas:<br/>
+Move experiment documentation to the <a href=\"modelica://AixLib.Experimental.Pipe.Data.PipeDatauLg150801\">
+specific model</a>. Add parameter <code>n</code> to facilitate use of extends clause.
+</li>
+<li>
+October 14, 2015 by Kevin Sartor:<br/>
+Add documentation about the test bench and how is conducted the experiment
+</li>
+<li>
+October 12, 2015 by Marcus Fuchs:<br/>
+Add rudimentary documentation and integrate into experimental pipe package
+</li>
+<li>
+October 7, 2015 by Kevin Sartor:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataBaseDefinition;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/BaseClasses/PipeDataULg.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/BaseClasses/PipeDataULg.mo
index 84552757ba..f44613026e 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/BaseClasses/PipeDataULg.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/BaseClasses/PipeDataULg.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses;
 partial record PipeDataULg "Base class for ULg experimental data"
   extends PipeDataBaseDefinition;
   parameter Modelica.Units.NonSI.Temperature_degC T_start_in=20
@@ -8,68 +8,68 @@ partial record PipeDataULg "Base class for ULg experimental data"
   parameter Modelica.Units.SI.MassFlowRate m_flowIni=0
     "Mass flow initialization";
   annotation (Documentation(info="<html>
- <p>
- This record contains information of an aproximately 15 minutes long test bench
- carried out at the University of Liège.
- </p>
- 
- <h4>Data structure</h4>
- <p>Column 1: Time in s </p>
- <p>Column 2: Mass flow rate in kg/s</p>
- <p>Column 3: Outlet pipe temperature in °C  </p>
- <p>Column 4: Outlet water temperature in °C </p>
- <p>Column 5: Inlet pipe temperature in °C  </p>
- <p>Column 6: Inlet water temperature in °C  </p>
- 
- <h4>Test procedure</h4>
- <p>
- Before to perform a test, the water city network is pushed inside
- the approximately 39 meter long studied pipe during about 10 minutes
- to be sure that it is at the same temperature.
- During this time period, valves V3 and V1 are opened, the boiler is off and
- the valve V2 is closed.
- </p>
- <p>
- Then, the valve V1 is closed and the valve V2 and V3 are opened.
- The boiler is started to reach the setpoint hot water temperature.
- When the temperature setpoint is achieved, data starts to be recorded,
- the valve V1 is opened and the valve V2 is closed at the same time
- to supply the studied pipe in hot water.
- After the outlet pipe temperature is stabilized, the boiler is shut off.
- </p>
- <p>
- During the test, the ambient temperature is equal to <i>18</i>&deg;C and
- the mass flow rate is set to <i>1.245</i> kg/s.</p>
- 
- <h4>Test bench schematic</h4>
- <p><img alt=\"Schematic of test rig at ULg\"
- src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/ULgTestBench.png\" border=\"1\"/></p>
- <p>Notice: length are approximate</p>
- 
- <h4>Pipe characteristics</h4>
- 
- <ul>
- <li>Metal density about 7800 kg/m<sup>3</sup></li>
- <li>Specific heat capacity about 480 J/kg/K</li>
- <li>Thickness 3.91 mm (Outer diameter 0.0603 m)</li>
- <li>Inner diameter: 0.05248 m</li>
- <li>Roughness is currently neglected</li>
- <li>Initial temperature of the pipe is considered equal
- to the initial temperature of the water (cooling before test)
- </li>
- <li>Heat transfer coefficient between the pipe and the ambient is assumed
- at 5 W/m<sup>2</sup>K (from internal model) due to insulation.
- The pipe is insulated by Tubolit 60/13 (13mm of thickness) whose
- nominal thermal coefficient is inferior 0.04.
- Notice the insulation is quite aged therefore
- the nominal thermal coefficient could be higher
- </li>
- <li>
- Heat transfer coefficient between water and pipe is a function of
- the fluid temperature (determined by EES software).
- </li>
- </ul>
- 
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This record contains information of an aproximately 15 minutes long test bench
+carried out at the University of Liège.
+</p>
+
+<h4>Data structure</h4>
+<p>Column 1: Time in s </p>
+<p>Column 2: Mass flow rate in kg/s</p>
+<p>Column 3: Outlet pipe temperature in °C  </p>
+<p>Column 4: Outlet water temperature in °C </p>
+<p>Column 5: Inlet pipe temperature in °C  </p>
+<p>Column 6: Inlet water temperature in °C  </p>
+
+<h4>Test procedure</h4>
+<p>
+Before to perform a test, the water city network is pushed inside
+the approximately 39 meter long studied pipe during about 10 minutes
+to be sure that it is at the same temperature.
+During this time period, valves V3 and V1 are opened, the boiler is off and
+the valve V2 is closed.
+</p>
+<p>
+Then, the valve V1 is closed and the valve V2 and V3 are opened.
+The boiler is started to reach the setpoint hot water temperature.
+When the temperature setpoint is achieved, data starts to be recorded,
+the valve V1 is opened and the valve V2 is closed at the same time
+to supply the studied pipe in hot water.
+After the outlet pipe temperature is stabilized, the boiler is shut off.
+</p>
+<p>
+During the test, the ambient temperature is equal to <i>18</i>&deg;C and
+the mass flow rate is set to <i>1.245</i> kg/s.</p>
+
+<h4>Test bench schematic</h4>
+<p><img alt=\"Schematic of test rig at ULg\"
+src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/ULgTestBench.png\" border=\"1\"/></p>
+<p>Notice: length are approximate</p>
+
+<h4>Pipe characteristics</h4>
+
+<ul>
+<li>Metal density about 7800 kg/m<sup>3</sup></li>
+<li>Specific heat capacity about 480 J/kg/K</li>
+<li>Thickness 3.91 mm (Outer diameter 0.0603 m)</li>
+<li>Inner diameter: 0.05248 m</li>
+<li>Roughness is currently neglected</li>
+<li>Initial temperature of the pipe is considered equal
+to the initial temperature of the water (cooling before test)
+</li>
+<li>Heat transfer coefficient between the pipe and the ambient is assumed
+at 5 W/m<sup>2</sup>K (from internal model) due to insulation.
+The pipe is insulated by Tubolit 60/13 (13mm of thickness) whose
+nominal thermal coefficient is inferior 0.04.
+Notice the insulation is quite aged therefore
+the nominal thermal coefficient could be higher
+</li>
+<li>
+Heat transfer coefficient between water and pipe is a function of
+the fluid temperature (determined by EES software).
+</li>
+</ul>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataULg;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataAIT151218.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataAIT151218.mo
index 8120018c35..9b97ec6ea4 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataAIT151218.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataAIT151218.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
 record PipeDataAIT151218
   "Experimental data from AIT monitoring data December 18, 2015"
     extends BaseClasses.PipeDataBaseDefinition(
@@ -6,58 +6,58 @@ record PipeDataAIT151218
       final filNam = Modelica.Utilities.Files.loadResource(
   "modelica://AixLib/Resources/Data/Fluid/FixedResistances/Validation/PlugFlowPipes/PipeDataAIT151218.mos"));
      annotation (Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- December 18, 2015 by Daniele Basciotti:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p><b><span style=\"color: #008000;\">Overview</span></b> </p>
- <p>This record contains data of a real disitrict heating network for week-long period (23-29 Januar 2009) monitored by the Austrian Institut for Technology.</p>
- <p> Pipes are layed underground
- 
- <p><b><span style=\"color: #008000;\">Data structure</span></b> </p>
- <p>Column 1: Time in s </p>
- <p>Column 2: Temperature in point 1 in K</p>
- <p>Column 3: Temperature in point 2 in K</p>
- <p>Column 4: Temperature in point 3 in K</p>
- <p>Column 5: Temperature in point 4 in K</p>
- <p>Column 6: Mass flow rate in point 1 in kg/s</p>
- <p>Column 7: Mass flow rate in point 2 in kg/s</p>
- <p>Column 8: Mass flow rate in point 3 in kg/s</p>
- <p>Column 9: Mass flow rate in point 4 in kg/s</p>
- <p>Column 10: Outdoor temperature in K</p>
- 
- <p><b><span style=\"color: #008000;\">Test procedure</span></b> </p>
- Information at several points of the district heating network is recorded during a week.
- 
- <p><b><span style=\"color: #008000;\">Test bench schematic</span></b> </p>
- <p><img alt=\"Schematic of test district heating network in Pongau\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/AITTestBench.png\" border=\"1\"/>
- </p>
- 
- <p>
- Notice that length are approximated
- </p>
- 
- <p><b><span style=\"color: #008000;\">Pipe characteristics</span></b> </p>
- <ul>
- <li>Inner diameter: 0.0825 m (DN080)</li>
- <li>Outer diameter: 0.0889 m (stell wall thickness 3.2 mm)</li>
- <li>Casing diameter: 0.18 m </li>
- <li>Insulation material: Polyurethane </li>
- <li>Heat conductivity of insulation material: 0.024 W/(m K) (average value at 50 °C) </li>
- <li>Length specific pipe's heat loss coefficient: 0.208 W/(m K) </li>
- <li>Wall roughness coefficient: 0.1 mm </li>
- </ul>
- 
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+December 18, 2015 by Daniele Basciotti:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p><b><span style=\"color: #008000;\">Overview</span></b> </p>
+<p>This record contains data of a real disitrict heating network for week-long period (23-29 Januar 2009) monitored by the Austrian Institut for Technology.</p>
+<p> Pipes are layed underground
+
+<p><b><span style=\"color: #008000;\">Data structure</span></b> </p>
+<p>Column 1: Time in s </p>
+<p>Column 2: Temperature in point 1 in K</p>
+<p>Column 3: Temperature in point 2 in K</p>
+<p>Column 4: Temperature in point 3 in K</p>
+<p>Column 5: Temperature in point 4 in K</p>
+<p>Column 6: Mass flow rate in point 1 in kg/s</p>
+<p>Column 7: Mass flow rate in point 2 in kg/s</p>
+<p>Column 8: Mass flow rate in point 3 in kg/s</p>
+<p>Column 9: Mass flow rate in point 4 in kg/s</p>
+<p>Column 10: Outdoor temperature in K</p>
+
+<p><b><span style=\"color: #008000;\">Test procedure</span></b> </p>
+Information at several points of the district heating network is recorded during a week.
+
+<p><b><span style=\"color: #008000;\">Test bench schematic</span></b> </p>
+<p><img alt=\"Schematic of test district heating network in Pongau\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/AITTestBench.png\" border=\"1\"/>
+</p>
+
+<p>
+Notice that length are approximated
+</p>
+
+<p><b><span style=\"color: #008000;\">Pipe characteristics</span></b> </p>
+<ul>
+<li>Inner diameter: 0.0825 m (DN080)</li>
+<li>Outer diameter: 0.0889 m (stell wall thickness 3.2 mm)</li>
+<li>Casing diameter: 0.18 m </li>
+<li>Insulation material: Polyurethane </li>
+<li>Heat conductivity of insulation material: 0.024 W/(m K) (average value at 50 °C) </li>
+<li>Length specific pipe's heat loss coefficient: 0.208 W/(m K) </li>
+<li>Wall roughness coefficient: 0.1 mm </li>
+</ul>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataAIT151218;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg150801.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg150801.mo
index 648d5c6a50..c82a16ca5b 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg150801.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg150801.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
 record PipeDataULg150801
   "Experimental data from ULg's pipe test bench from August 1"
   extends AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg(
@@ -9,35 +9,35 @@ record PipeDataULg150801
     final filNam = Modelica.Utilities.Files.loadResource(
   "modelica://AixLib/Resources/Data/Fluid/FixedResistances/Validation/PlugFlowPipes/PipeDataULg150801.mos"));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- October 14, 2015 by Kevin Sartor:<br/>
- Add some information about the test.
- </li>
- <li>
- October 12, 2015 by Marcus Fuchs:<br/>
- Add rudimentary documentation and integrate into experimental pipe package
- </li>
- <li>
- October 7, 2015 by Kevin Sartor:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This data record contains the experimental data from the
- long test bench carried out at the University of Liège.
- See <a href=\"AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
- for more information.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+October 14, 2015 by Kevin Sartor:<br/>
+Add some information about the test.
+</li>
+<li>
+October 12, 2015 by Marcus Fuchs:<br/>
+Add rudimentary documentation and integrate into experimental pipe package
+</li>
+<li>
+October 7, 2015 by Kevin Sartor:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This data record contains the experimental data from the
+long test bench carried out at the University of Liège.
+See <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
+for more information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataULg150801;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151202.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151202.mo
index fd07dc72b2..71e8246bd7 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151202.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151202.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
 record PipeDataULg151202
   "Experimental data from ULg's pipe test bench from December 2, 2015"
   extends AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg(
@@ -9,35 +9,35 @@ record PipeDataULg151202
     final filNam = Modelica.Utilities.Files.loadResource(
   "modelica://AixLib/Resources/Data/Fluid/FixedResistances/Validation/PlugFlowPipes/PipeDataULg151202.mos"));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- October 14, 2015 by Kevin Sartor:<br/>
- Add some information about the test.
- </li>
- <li>
- October 12, 2015 by Marcus Fuchs:<br/>
- Add rudimentary documentation and integrate into experimental pipe package
- </li>
- <li>
- October 7, 2015 by Kevin Sartor:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This data record contains the experimental data from the
- long test bench carried out at the University of Liège.
- See <a href=\"AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
- for more information.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+October 14, 2015 by Kevin Sartor:<br/>
+Add some information about the test.
+</li>
+<li>
+October 12, 2015 by Marcus Fuchs:<br/>
+Add rudimentary documentation and integrate into experimental pipe package
+</li>
+<li>
+October 7, 2015 by Kevin Sartor:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This data record contains the experimental data from the
+long test bench carried out at the University of Liège.
+See <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
+for more information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataULg151202;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_1.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_1.mo
index 5617bf1b2e..135ebc400e 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_1.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_1.mo
@@ -1,7 +1,7 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
 record PipeDataULg151204_1
   "Experimental data from ULg's pipe test bench from December 4, 2015 (1);
-   increase followed by a decrease in temperature"
+  increase followed by a decrease in temperature"
   extends AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg(
     T_start_out=14.0,
     T_start_in=14.0,
@@ -10,35 +10,35 @@ record PipeDataULg151204_1
     final filNam = Modelica.Utilities.Files.loadResource(
   "modelica://AixLib/Resources/Data/Fluid/FixedResistances/Validation/PlugFlowPipes/PipeDataULg151204_1.mos"));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- October 14, 2015 by Kevin Sartor:<br/>
- Add some information about the test.
- </li>
- <li>
- October 12, 2015 by Marcus Fuchs:<br/>
- Add rudimentary documentation and integrate into experimental pipe package
- </li>
- <li>
- October 7, 2015 by Kevin Sartor:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This data record contains the experimental data from the
- long test bench carried out at the University of Liège.
- See <a href=\"AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
- for more information.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+October 14, 2015 by Kevin Sartor:<br/>
+Add some information about the test.
+</li>
+<li>
+October 12, 2015 by Marcus Fuchs:<br/>
+Add rudimentary documentation and integrate into experimental pipe package
+</li>
+<li>
+October 7, 2015 by Kevin Sartor:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This data record contains the experimental data from the
+long test bench carried out at the University of Liège.
+See <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
+for more information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataULg151204_1;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_2.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_2.mo
index bfa7ae280d..530e2edfbc 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_2.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_2.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
 record PipeDataULg151204_2
   "Experimental data from ULg's pipe test bench from December 4, 2015 (2)"
   extends AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg(
@@ -9,35 +9,35 @@ record PipeDataULg151204_2
     final filNam = Modelica.Utilities.Files.loadResource(
   "modelica://AixLib/Resources/Data/Fluid/FixedResistances/Validation/PlugFlowPipes/PipeDataULg151204_2.mos"));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- October 14, 2015 by Kevin Sartor:<br/>
- Add some information about the test.
- </li>
- <li>
- October 12, 2015 by Marcus Fuchs:<br/>
- Add rudimentary documentation and integrate into experimental pipe package
- </li>
- <li>
- October 7, 2015 by Kevin Sartor:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This data record contains the experimental data from the
- long test bench carried out at the University of Liège.
- See <a href=\"AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
- for more information.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+October 14, 2015 by Kevin Sartor:<br/>
+Add some information about the test.
+</li>
+<li>
+October 12, 2015 by Marcus Fuchs:<br/>
+Add rudimentary documentation and integrate into experimental pipe package
+</li>
+<li>
+October 7, 2015 by Kevin Sartor:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This data record contains the experimental data from the
+long test bench carried out at the University of Liège.
+See <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
+for more information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataULg151204_2;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_4.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_4.mo
index 788fac8974..173ff5fa57 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_4.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg151204_4.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
 record PipeDataULg151204_4
   "Experimental data from ULg's pipe test bench from December 4, 2015 (4); an increase followed by a decrease temperature"
   extends AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg(
@@ -9,35 +9,35 @@ record PipeDataULg151204_4
     final filNam = Modelica.Utilities.Files.loadResource(
   "modelica://AixLib/Resources/Data/Fluid/FixedResistances/Validation/PlugFlowPipes/PipeDataULg151204_4.mos"));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- October 14, 2015 by Kevin Sartor:<br/>
- Add some information about the test.
- </li>
- <li>
- October 12, 2015 by Marcus Fuchs:<br/>
- Add rudimentary documentation and integrate into experimental pipe package
- </li>
- <li>
- October 7, 2015 by Kevin Sartor:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This data record contains the experimental data from the
- long test bench carried out at the University of Liège.
- See <a href=\"AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
- for more information.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+October 14, 2015 by Kevin Sartor:<br/>
+Add some information about the test.
+</li>
+<li>
+October 12, 2015 by Marcus Fuchs:<br/>
+Add rudimentary documentation and integrate into experimental pipe package
+</li>
+<li>
+October 7, 2015 by Kevin Sartor:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This data record contains the experimental data from the
+long test bench carried out at the University of Liège.
+See <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
+for more information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataULg151204_4;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg160104_2.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg160104_2.mo
index 1dbc22637b..aebe808933 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg160104_2.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg160104_2.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
 record PipeDataULg160104_2 "Experimental data from ULg's pipe test bench from 4 January 2016. Low mass flow"
   extends AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg(
     T_start_out=15.0,
@@ -8,35 +8,35 @@ record PipeDataULg160104_2 "Experimental data from ULg's pipe test bench from 4
     final filNam = Modelica.Utilities.Files.loadResource(
   "modelica://AixLib/Resources/Data/Fluid/FixedResistances/Validation/PlugFlowPipes/PipeDataULg160104_2.mos"));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- October 14, 2015 by Kevin Sartor:<br/>
- Add some information about the test.
- </li>
- <li>
- October 12, 2015 by Marcus Fuchs:<br/>
- Add rudimentary documentation and integrate into experimental pipe package
- </li>
- <li>
- October 7, 2015 by Kevin Sartor:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This data record contains the experimental data from the
- long test bench carried out at the University of Liège.
- See <a href=\"AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
- for more information.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+October 14, 2015 by Kevin Sartor:<br/>
+Add some information about the test.
+</li>
+<li>
+October 12, 2015 by Marcus Fuchs:<br/>
+Add rudimentary documentation and integrate into experimental pipe package
+</li>
+<li>
+October 7, 2015 by Kevin Sartor:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This data record contains the experimental data from the
+long test bench carried out at the University of Liège.
+See <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
+for more information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataULg160104_2;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg160118_1.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg160118_1.mo
index 36c93404dc..c6b7286f2c 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg160118_1.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/PipeDataULg160118_1.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data;
 record PipeDataULg160118_1
   "Experimental data from ULg's pipe test bench from January 18, 2016"
   extends AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg(
@@ -9,35 +9,35 @@ record PipeDataULg160118_1
     final filNam = Modelica.Utilities.Files.loadResource(
   "modelica://AixLib/Resources/Data/Fluid/FixedResistances/Validation/PlugFlowPipes/PipeDataULg160118_1.mos"));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- October 14, 2015 by Kevin Sartor:<br/>
- Add some information about the test.
- </li>
- <li>
- October 12, 2015 by Marcus Fuchs:<br/>
- Add rudimentary documentation and integrate into experimental pipe package
- </li>
- <li>
- October 7, 2015 by Kevin Sartor:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This data record contains the experimental data from the
- long test bench carried out at the University of Liège.
- See <a href=\"AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
- for more information.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+October 14, 2015 by Kevin Sartor:<br/>
+Add some information about the test.
+</li>
+<li>
+October 12, 2015 by Marcus Fuchs:<br/>
+Add rudimentary documentation and integrate into experimental pipe package
+</li>
+<li>
+October 7, 2015 by Kevin Sartor:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This data record contains the experimental data from the
+long test bench carried out at the University of Liège.
+See <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.BaseClasses.PipeDataULg</a>
+for more information.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PipeDataULg160118_1;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/TestData.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/TestData.mo
index ed558d2da8..70f85b3309 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/TestData.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/TestData.mo
@@ -15,27 +15,26 @@ equation
       annotation (experiment(StopTime=603900, Interval=900, Tolerance=1e-6),
       Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-40,-40},{60,40}})),
       Documentation(info="<html>
-     <p>Model used to visualize and check data of district heating networks</p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- January 19, 2016 by Carles Ribas:<br/>
- Use replaceable data and addition of <code>.mos</code> file.
- </li>
- <li>
- December 18, 2015 by Daniele Basciotti:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-          __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/TestData.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+    <p>Model used to visualize and check data of district heating networks</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+January 19, 2016 by Carles Ribas:<br/>
+Use replaceable data and addition of <code>.mos</code> file.
+</li>
+<li>
+December 18, 2015 by Daniele Basciotti:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/TestData.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestData;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/package.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/package.mo
index 6309474c3f..7c0651b686 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/package.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/Data/package.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes;
 package Data "Experimental data for verification of pipe models"
 
 
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/FlowReversal.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/FlowReversal.mo
index cacd4cf640..b0614cf9ba 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/FlowReversal.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/FlowReversal.mo
@@ -66,21 +66,21 @@ equation
         "Simulate and Plot"),
     experiment(StopTime=150, Tolerance=1e-006),
     Documentation(info="<html>
- <p>
- Validation model in which water flows into the pipe and then the flow is reversed.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 12, 2021, by Baptiste Ravache:<br/>
- Changed outlet boundary pressure to avoid negative
- pressure at the inlet when flow is reversed.
- </li>
- <li>
- October 25, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Validation model in which water flows into the pipe and then the flow is reversed.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 12, 2021, by Baptiste Ravache:<br/>
+Changed outlet boundary pressure to avoid negative
+pressure at the inlet when flow is reversed.
+</li>
+<li>
+October 25, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowReversal;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT.mo
index d110a8e9cb..b632109586 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT.mo
@@ -444,90 +444,90 @@ equation
        __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- The example contains
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.PipeDataAIT151218\">
- experimental data</a> from a real district heating network.
- This data is used to validate this library's
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
- AixLib.Fluid.FixedResistances.PlugFlowPipe</a> in
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>.
- This model compares its performance with the original Modelica Standard Library
- pipes, using one discretization element per unit length of pipe.
- For a coarser discretization, please refer to
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes\">
- MSLAIT2Nodes</a>.
- </p>
- <p>
- Note that these three models are identical, except for the pipe model that is used:
- </p>
- <ul>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT</a>
- uses the pipe model from the Modelica Standard Library, with a fine discretization.
- See the parameter <code>nNodes</code>.
- </li>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes</a>
- uses the same model as above, but sets <code>nNodes=2</code>.
- </li>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>
- uses the plug flow model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
- AixLib.Fluid.FixedResistances.PlugFlowPipe</a>.
- </li>
- </ul>
- <p>
- This comparison between different discretization levels and pipe models is made
- to check the influence of the discretization and pipe model on computation time
- and simulation accuracy.
- </p>
- <p>The pipes' temperatures are not initialized, thus results of outflow
- temperature before approximately the first 10000 seconds should not be considered.
- </p>
- <h4>Test bench schematic</h4>
- <p><img alt=\"Schematic of test district heating network\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/AITTestBench.png\"/> </p>
- <h4>Calibration</h4>
- <p>To calculate the length specific thermal resistance <code>R</code> of the
- pipe, the thermal resistance of the surrounding ground is added. </p>
- <p align=\"center\"style=\"font-style:italic;\">
- R=1/(0.208)+1/(2 &nbsp; lambda_g &nbsp; Modelica.Constants.pi) &nbsp; log(1/0.18)</p>
- <p>
- Where the thermal conductivity of the ground <code>lambda_g</code> = 2.4 W/(m K).
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>November 28, 2016 by Bram van der Heijde:<br/>Remove <code>pipVol.</code>
- </li>
- <li>August 24, 2016 by Bram van der Heijde:<br/>
- Implement validation with MSL pipes for comparison, based on AIT validation.
- </li>
- <li>
- July 4, 2016 by Bram van der Heijde:<br/>Added parameters to test the
- influence of allowFlowReversal and the presence of explicit volumes in the pipe.
- </li>
- <li>January 26, 2016 by Carles Ribas:<br/>First implementation. </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+The example contains
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.PipeDataAIT151218\">
+experimental data</a> from a real district heating network.
+This data is used to validate this library's
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
+AixLib.Fluid.FixedResistances.PlugFlowPipe</a> in
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>.
+This model compares its performance with the original Modelica Standard Library
+pipes, using one discretization element per unit length of pipe.
+For a coarser discretization, please refer to
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes\">
+MSLAIT2Nodes</a>.
+</p>
+<p>
+Note that these three models are identical, except for the pipe model that is used:
+</p>
+<ul>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT</a>
+uses the pipe model from the Modelica Standard Library, with a fine discretization.
+See the parameter <code>nNodes</code>.
+</li>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes</a>
+uses the same model as above, but sets <code>nNodes=2</code>.
+</li>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>
+uses the plug flow model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
+AixLib.Fluid.FixedResistances.PlugFlowPipe</a>.
+</li>
+</ul>
+<p>
+This comparison between different discretization levels and pipe models is made
+to check the influence of the discretization and pipe model on computation time
+and simulation accuracy.
+</p>
+<p>The pipes' temperatures are not initialized, thus results of outflow
+temperature before approximately the first 10000 seconds should not be considered.
+</p>
+<h4>Test bench schematic</h4>
+<p><img alt=\"Schematic of test district heating network\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/AITTestBench.png\"/> </p>
+<h4>Calibration</h4>
+<p>To calculate the length specific thermal resistance <code>R</code> of the
+pipe, the thermal resistance of the surrounding ground is added. </p>
+<p align=\"center\"style=\"font-style:italic;\">
+R=1/(0.208)+1/(2 &nbsp; lambda_g &nbsp; Modelica.Constants.pi) &nbsp; log(1/0.18)</p>
+<p>
+Where the thermal conductivity of the ground <code>lambda_g</code> = 2.4 W/(m K).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>November 28, 2016 by Bram van der Heijde:<br/>Remove <code>pipVol.</code>
+</li>
+<li>August 24, 2016 by Bram van der Heijde:<br/>
+Implement validation with MSL pipes for comparison, based on AIT validation.
+</li>
+<li>
+July 4, 2016 by Bram van der Heijde:<br/>Added parameters to test the
+influence of allowFlowReversal and the presence of explicit volumes in the pipe.
+</li>
+<li>January 26, 2016 by Carles Ribas:<br/>First implementation. </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MSLAIT;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT2Nodes.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT2Nodes.mo
index 0118b74f3b..adc291be40 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT2Nodes.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT2Nodes.mo
@@ -437,87 +437,87 @@ equation
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PlugFlowPipes/MSLAIT2Nodes.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>The example contains
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.PipeDataAIT151218\">
- experimental data</a> from a real district heating network.
- This data is used to validate this library's
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">plug flow pipe model</a>
- in <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>.
- </p>
- <p>
- Note that these three models are identical, except for the pipe model that is used:
- </p>
- <ul>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT</a>
- uses the pipe model from the Modelica Standard Library, with a fine discretization.
- See the parameter <code>nNodes</code>.
- </li>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes</a>
- uses the same model as above, but sets <code>nNodes=2</code>.
- </li>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>
- uses the plug flow model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
- AixLib.Fluid.FixedResistances.PlugFlowPipe</a>.
- </li>
- </ul>
- <p>
- This comparison between different discretization levels and pipe models is made
- to check the influence of the discretization and pipe model on computation time
- and simulation accuracy.
- </p>
- <p>The pipes' temperatures are not initialized, thus results of outflow temperature
- before approximately the first 10000 seconds should not be considered.
- </p>
- <h4>Test bench schematic</h4>
- <p><img alt=\"Schematic of test district heating network\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/AITTestBench.png\"/> </p>
- <h4>Calibration</h4>
- <p>
- To calculate the length specific thermal resistance <code>R</code> of the pipe,
- the thermal resistance of the surrounding ground is added.
- </p>
- <p align=\"center\"style=\"font-style:italic;\">
- R=1/(0.208)+1/(2 &nbsp; lambda<sub>g</sub> Modelica.Constants.pi) &nbsp; log(1/0.18)
- </p>
- <p>
- Where the thermal conductivity of the ground <code>lambda_g</code> = 2.4 W/(m K).
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>November 28, 2016 by Bram van der Heijde:<br/>Remove <code>pipVol.</code>
- </li>
- <li>
- August 24, 2016 by Bram van der Heijde:<br/>
- Implement validation with MSL pipes for comparison, based on AIT validation.
- </li>
- <li>
- July 4, 2016 by Bram van der Heijde:<br/>Added parameters to test the
- influence of allowFlowReversal and the presence of explicit volumes in the pipe.
- </li>
- <li>January 26, 2016 by Carles Ribas:<br/>First implementation. </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>The example contains
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.PipeDataAIT151218\">
+experimental data</a> from a real district heating network.
+This data is used to validate this library's
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">plug flow pipe model</a>
+in <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>.
+</p>
+<p>
+Note that these three models are identical, except for the pipe model that is used:
+</p>
+<ul>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT</a>
+uses the pipe model from the Modelica Standard Library, with a fine discretization.
+See the parameter <code>nNodes</code>.
+</li>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes</a>
+uses the same model as above, but sets <code>nNodes=2</code>.
+</li>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>
+uses the plug flow model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
+AixLib.Fluid.FixedResistances.PlugFlowPipe</a>.
+</li>
+</ul>
+<p>
+This comparison between different discretization levels and pipe models is made
+to check the influence of the discretization and pipe model on computation time
+and simulation accuracy.
+</p>
+<p>The pipes' temperatures are not initialized, thus results of outflow temperature
+before approximately the first 10000 seconds should not be considered.
+</p>
+<h4>Test bench schematic</h4>
+<p><img alt=\"Schematic of test district heating network\" src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/AITTestBench.png\"/> </p>
+<h4>Calibration</h4>
+<p>
+To calculate the length specific thermal resistance <code>R</code> of the pipe,
+the thermal resistance of the surrounding ground is added.
+</p>
+<p align=\"center\"style=\"font-style:italic;\">
+R=1/(0.208)+1/(2 &nbsp; lambda<sub>g</sub> Modelica.Constants.pi) &nbsp; log(1/0.18)
+</p>
+<p>
+Where the thermal conductivity of the ground <code>lambda_g</code> = 2.4 W/(m K).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>November 28, 2016 by Bram van der Heijde:<br/>Remove <code>pipVol.</code>
+</li>
+<li>
+August 24, 2016 by Bram van der Heijde:<br/>
+Implement validation with MSL pipes for comparison, based on AIT validation.
+</li>
+<li>
+July 4, 2016 by Bram van der Heijde:<br/>Added parameters to test the
+influence of allowFlowReversal and the presence of explicit volumes in the pipe.
+</li>
+<li>January 26, 2016 by Carles Ribas:<br/>First implementation. </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MSLAIT2Nodes;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowAIT.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowAIT.mo
index ab785406f9..5c4053aeac 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowAIT.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowAIT.mo
@@ -375,81 +375,81 @@ equation
   annotation (
     experiment(
       StopTime=603900,
-      Interval=900,
+      Interval=120,
       Tolerance=1e-006),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowAIT.mos"
         "Simulate and plot"),
     Diagram(coordinateSystem(extent={{-120,-160},{160,160}})),
     Documentation(info="<html>
- <p>
- The example contains
- experimental data from a real district heating network.
- </p>
- <p>The pipes' temperatures are not initialized. Therefore, results of
- outflow temperature before approximately the first 10000 seconds should not be
- considered.
- </p>
- <p>
- Note that these three models are identical, except for the pipe model that is used:
- </p>
- <ul>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT</a>
- uses the pipe model from the Modelica Standard Library, with a fine discretization.
- See the parameter <code>nNodes</code>.
- </li>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes</a>
- uses the same model as above, but sets <code>nNodes=2</code>.
- </li>
- <li>
- The model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
- AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>
- uses the plug flow model
- <a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
- AixLib.Fluid.FixedResistances.PlugFlowPipe</a>.
- </li>
- </ul>
- <p>
- This comparison between different discretization levels and pipe models is made
- to check the influence of the discretization and pipe model on computation time
- and simulation accuracy.
- </p>
- <h4>Test bench schematic</h4>
- <p><img alt=\"Schematic of test district heating network\"
- src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/AITTestBench.png\"/>
- </p>
- <h4>Calibration</h4>
- <p>To calculate the length specific thermal resistance <code>R</code> of the pipe,
- the thermal resistance of the surrounding ground is added, which yields</p>
- <p align=\"center\"style=\"font-style:italic;\">
- R=1/(0.208)+1/(2 &nbsp; lambda_g &nbsp; Modelica.Constants.pi) &nbsp; log(1/0.18),</p>
- <p>where the thermal conductivity of the ground <code>lambda_g</code> = 2.4 W/(m K).
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>July 4, 2016 by Bram van der Heijde:<br/>Added parameters to test the
- influence of allowFlowReversal and the presence of explicit volumes in the pipe.
- </li>
- <li>January 26, 2016 by Carles Ribas:<br/>First implementation. </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+The example contains
+experimental data from a real district heating network.
+</p>
+<p>The pipes' temperatures are not initialized. Therefore, results of
+outflow temperature before approximately the first 10000 seconds should not be
+considered.
+</p>
+<p>
+Note that these three models are identical, except for the pipe model that is used:
+</p>
+<ul>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT</a>
+uses the pipe model from the Modelica Standard Library, with a fine discretization.
+See the parameter <code>nNodes</code>.
+</li>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.MSLAIT2Nodes</a>
+uses the same model as above, but sets <code>nNodes=2</code>.
+</li>
+<li>
+The model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT\">
+AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.PlugFlowAIT</a>
+uses the plug flow model
+<a href=\"modelica://AixLib.Fluid.FixedResistances.PlugFlowPipe\">
+AixLib.Fluid.FixedResistances.PlugFlowPipe</a>.
+</li>
+</ul>
+<p>
+This comparison between different discretization levels and pipe models is made
+to check the influence of the discretization and pipe model on computation time
+and simulation accuracy.
+</p>
+<h4>Test bench schematic</h4>
+<p><img alt=\"Schematic of test district heating network\"
+src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/AITTestBench.png\"/>
+</p>
+<h4>Calibration</h4>
+<p>To calculate the length specific thermal resistance <code>R</code> of the pipe,
+the thermal resistance of the surrounding ground is added, which yields</p>
+<p align=\"center\"style=\"font-style:italic;\">
+R=1/(0.208)+1/(2 &nbsp; lambda_g &nbsp; Modelica.Constants.pi) &nbsp; log(1/0.18),</p>
+<p>where the thermal conductivity of the ground <code>lambda_g</code> = 2.4 W/(m K).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>July 4, 2016 by Bram van der Heijde:<br/>Added parameters to test the
+influence of allowFlowReversal and the presence of explicit volumes in the pipe.
+</li>
+<li>January 26, 2016 by Carles Ribas:<br/>First implementation. </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowAIT;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowULg.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowULg.mo
index a19312bac0..d20cc3dfb5 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowULg.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowULg.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes;
+within AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes;
 model PlugFlowULg "Validation against data from Université de Liège"
   extends Modelica.Icons.Example;
   package Medium = AixLib.Media.Water;
@@ -179,55 +179,55 @@ equation
     annotation (Line(points={{78,66},{-130,66},{-130,11}}, color={0,0,127}));
   annotation (
     Documentation(info="<html>
- <p>
- The example contains
- experimental data from a real district heating network.
- </p>
- <p>
- This model compares the results with the original Modelica Standard Library pipes.
- </p>
- <p>The pipes' temperatures are not initialized. Therefore, results of
- outflow temperature before approximately the first 10000 seconds should not be
- considered.
- </p>
- <h4>Test bench schematic</h4>
- <p><img alt=\"Schematic of test rig at ULg\"
- src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/ULgTestBench.png\"/> </p>
- <h4>Calibration</h4>
- <p>
- There are some uncertainties about the heat loss coefficient between pipe and
- surrounding air as well as regarding the heat conductivity of the insulation
- material.
- With the <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.PipeDataULg150801\">
- given data</a>, the length specific thermal resistance is <code>R = 2.164
- </code>((m K)/W), calculated as follows:
- </p>
- <p align=\"center\"style=\"font-style:italic;\">
- R=((1/(2*pipe.kIns)*log((0.0603+2*pipe.dIns)/(0.0603)))+1/(5*(0.0603+2*pipe.dIns)))/Modelica.Constants.pi</p>
- <p align=\"center\"style=\"font-style:italic;\">
- U = 1/R = 0.462 W/(m K)</p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2020, by Michael Wetter:<br/>
- Replaced measured data from specification in Modelica file to external table,
- as this reduces the computing time.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
- </li>
- <li>
- November 24, 2016 by Bram van der Heijde:<br/>Add pipe thickness for wall
- capacity calculation and expand documentation section.</li>
- <li>April 2, 2016 by Bram van der Heijde:<br/>Change thermal conductivity and
- put boundary condition in K.
- </li>
- <li>Januar 26, 2016 by Carles Ribas:<br/>First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+The example contains
+experimental data from a real district heating network.
+</p>
+<p>
+This model compares the results with the original Modelica Standard Library pipes.
+</p>
+<p>The pipes' temperatures are not initialized. Therefore, results of
+outflow temperature before approximately the first 10000 seconds should not be
+considered.
+</p>
+<h4>Test bench schematic</h4>
+<p><img alt=\"Schematic of test rig at ULg\"
+src=\"modelica://AixLib/Resources/Images/Fluid/FixedResistances/Validation/PlugFlowPipes/ULgTestBench.png\"/> </p>
+<h4>Calibration</h4>
+<p>
+There are some uncertainties about the heat loss coefficient between pipe and
+surrounding air as well as regarding the heat conductivity of the insulation
+material.
+With the <a href=\"modelica://AixLib.Fluid.FixedResistances.Validation.PlugFlowPipes.Data.PipeDataULg150801\">
+given data</a>, the length specific thermal resistance is <code>R = 2.164
+</code>((m K)/W), calculated as follows:
+</p>
+<p align=\"center\"style=\"font-style:italic;\">
+R=((1/(2*pipe.kIns)*log((0.0603+2*pipe.dIns)/(0.0603)))+1/(5*(0.0603+2*pipe.dIns)))/Modelica.Constants.pi</p>
+<p align=\"center\"style=\"font-style:italic;\">
+U = 1/R = 0.462 W/(m K)</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2020, by Michael Wetter:<br/>
+Replaced measured data from specification in Modelica file to external table,
+as this reduces the computing time.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1289\"> #1289</a>.
+</li>
+<li>
+November 24, 2016 by Bram van der Heijde:<br/>Add pipe thickness for wall
+capacity calculation and expand documentation section.</li>
+<li>April 2, 2016 by Bram van der Heijde:<br/>Change thermal conductivity and
+put boundary condition in K.
+</li>
+<li>Januar 26, 2016 by Carles Ribas:<br/>First implementation.
+</li>
+</ul>
+</html>"),
     experiment(StopTime=875, Tolerance=1e-006),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PlugFlowPipes/PlugFlowULg.mos"
         "Simulate and plot"),
-    Diagram(coordinateSystem(extent={{-260,-120},{260,120}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Diagram(coordinateSystem(extent={{-260,-120},{260,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PlugFlowULg;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/TransportWaterAir.mo b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/TransportWaterAir.mo
index f02181629f..07ef204dfa 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/TransportWaterAir.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PlugFlowPipes/TransportWaterAir.mo
@@ -140,18 +140,18 @@ equation
         "Simulate and Plot"),
     experiment(StopTime=1000, Tolerance=1e-006),
     Documentation(info="<html>
- <p>
- Validation model in which a step input is applied to
- the transport of air and water with a species concentration.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 25, 2017 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    Diagram(coordinateSystem(extent={{-100,-140},{100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Validation model in which a step input is applied to
+the transport of air and water with a species concentration.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 25, 2017 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-100,-140},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TransportWaterAir;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PressureDropsExplicit.mo b/AixLib/Fluid/FixedResistances/Validation/PressureDropsExplicit.mo
index f9c201c88e..cd45101bae 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PressureDropsExplicit.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PressureDropsExplicit.mo
@@ -230,16 +230,16 @@ experiment(StartTime=-1, Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PressureDropsExplicit.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests multiple flow resistances in series.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests multiple flow resistances in series.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureDropsExplicit;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PressureDropsExplicitLinearized.mo b/AixLib/Fluid/FixedResistances/Validation/PressureDropsExplicitLinearized.mo
index 6f0b35523a..a3e038ffc8 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PressureDropsExplicitLinearized.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PressureDropsExplicitLinearized.mo
@@ -15,16 +15,16 @@ experiment(StartTime=-1, Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PressureDropsExplicitLinearized.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests multiple linearized flow resistances in series.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests multiple linearized flow resistances in series.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureDropsExplicitLinearized;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PressureDropsParallel.mo b/AixLib/Fluid/FixedResistances/Validation/PressureDropsParallel.mo
index 0c5ff4c4cd..e5ab2138b7 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PressureDropsParallel.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PressureDropsParallel.mo
@@ -88,16 +88,16 @@ equation
 annotation (experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PressureDropsParallel.mos" "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests two resistances in parallel.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests two resistances in parallel.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureDropsParallel;
diff --git a/AixLib/Fluid/FixedResistances/Validation/PressureDropsSeries.mo b/AixLib/Fluid/FixedResistances/Validation/PressureDropsSeries.mo
index 477f8ca0b7..5ad437d0e6 100644
--- a/AixLib/Fluid/FixedResistances/Validation/PressureDropsSeries.mo
+++ b/AixLib/Fluid/FixedResistances/Validation/PressureDropsSeries.mo
@@ -54,16 +54,16 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Validation/PressureDropsSeries.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model tests multiple resistances in series.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 20, 2007 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests multiple resistances in series.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 20, 2007 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PressureDropsSeries;
diff --git a/AixLib/Fluid/FixedResistances/package.mo b/AixLib/Fluid/FixedResistances/package.mo
index 894f1c9827..1392c92654 100644
--- a/AixLib/Fluid/FixedResistances/package.mo
+++ b/AixLib/Fluid/FixedResistances/package.mo
@@ -10,7 +10,7 @@ flow coefficient
 </p>
 <p align=\"center\" style=\"font-style:italic;\">
 k = m &frasl;
-&radic;<span style=\"text-decoration:overline;\">&Delta;P</span>.
+&radic;<span style=\"text-decoration:overline;\">&Delta;p</span>.
 </p>
 <p>
 For models of valves and air dampers, see
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Data/Rock.mo b/AixLib/Fluid/Geothermal/Aquifer/Data/Rock.mo
new file mode 100644
index 0000000000..2985d6f18e
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Data/Rock.mo
@@ -0,0 +1,27 @@
+within AixLib.Fluid.Geothermal.Aquifer.Data;
+record Rock "Soil data record of rock heat transfer properties"
+  extends AixLib.Fluid.Geothermal.Aquifer.Data.Template(
+    kSoi=2.8,
+    dSoi=2680,
+    cSoi=833,
+    phi=0.2,
+    K=1E-5);
+  annotation (
+  defaultComponentPrefixes="parameter",
+  defaultComponentName="aquDat",
+Documentation(
+info="<html>
+<p>
+This data record contains the heat transfer properties of rock.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+May 2023, Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Rock;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Data/Template.mo b/AixLib/Fluid/Geothermal/Aquifer/Data/Template.mo
new file mode 100644
index 0000000000..c74dec2776
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Data/Template.mo
@@ -0,0 +1,42 @@
+within AixLib.Fluid.Geothermal.Aquifer.Data;
+record Template
+  "Template for soil data records"
+  extends Modelica.Icons.Record;
+  parameter Modelica.Units.SI.ThermalConductivity kSoi
+    "Thermal conductivity of the soil material";
+  parameter Modelica.Units.SI.SpecificHeatCapacity cSoi
+    "Specific heat capacity of the soil material";
+  parameter Modelica.Units.SI.Density dSoi(displayUnit="kg/m3")
+    "Density of the soil material";
+  parameter Real phi(final unit="1")
+    "Reservoir porosity";
+  parameter Modelica.Units.SI.Velocity K
+    "Hydraulic conductivity";
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+  defaultComponentPrefixes="parameter",
+  defaultComponentName="aquDat",
+  Documentation(
+info="<html>
+<p>
+This record is a template for the records in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Aquifer.MultiWell\">
+AixLib.Fluid.Geothermal.Aquifer.MultiWell</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+March 25, 2024, by Michael Wetter:<br/>
+Corrected broken link.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1855\">IBPSA, issue 1855</a>.
+</li>
+<li>
+May 2023, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Template;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Data/package.mo b/AixLib/Fluid/Geothermal/Aquifer/Data/package.mo
new file mode 100644
index 0000000000..911258672e
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Data/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.Geothermal.Aquifer;
+package Data "Collection of data records for aquifer thermal energy storage"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains data records for heat properties of aquifers
+<a href=\"modelica://AixLib.Fluid.Geothermal.Aquifer\">
+AixLib.Fluid.Geothermal.Aquifer</a>.
+</p>
+</html>"));
+end Data;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Data/package.order b/AixLib/Fluid/Geothermal/Aquifer/Data/package.order
new file mode 100644
index 0000000000..a4b770a71b
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Data/package.order
@@ -0,0 +1,2 @@
+Rock
+Template
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Examples/CoolingOffice.mo b/AixLib/Fluid/Geothermal/Aquifer/Examples/CoolingOffice.mo
new file mode 100644
index 0000000000..57f1f7618b
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Examples/CoolingOffice.mo
@@ -0,0 +1,84 @@
+within AixLib.Fluid.Geothermal.Aquifer.Examples;
+model CoolingOffice
+  extends Modelica.Icons.Example;
+  package Medium = AixLib.Media.Water "Medium model";
+
+  parameter Modelica.Units.SI.HeatFlowRate QCoo_flow_nominal=30000
+    "Cooling power";
+  parameter Modelica.Units.SI.TemperatureDifference deltaT=4 "Temperature difference at heat exchanger";
+  parameter Modelica.Units.SI.SpecificHeatCapacity cpWat=4186 "Heat capacity of water";
+  parameter Modelica.Units.SI.MassFlowRate mWat_flow_nominal=
+    QCoo_flow_nominal/(deltaT*cpWat) "Nominal water mass flow rate";
+
+  HeatExchangers.HeaterCooler_u hea(
+    redeclare package Medium = Medium,
+    m_flow_nominal=mWat_flow_nominal,
+    dp_nominal=100,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    Q_flow_nominal=QCoo_flow_nominal) "Heat exchanger"
+    annotation (Placement(transformation(extent={{-10,54},{10,74}})));
+  Modelica.Blocks.Sources.Constant uPum(k=1) "Pump control signal"
+    annotation (Placement(transformation(extent={{-60,-20},{-40,0}})));
+  Modelica.Blocks.Sources.Constant uHea(k=1) "Heat load control signal"
+    annotation (Placement(transformation(extent={{-60,60},{-40,80}})));
+  MultiWell aquWel(
+    redeclare package Medium = Medium,
+    nVol=80,
+    h=20,
+    d=1000,
+    length=40,
+    TCol_start=285.15,
+    THot_start=285.15,
+    aquDat=AixLib.Fluid.Geothermal.Aquifer.Data.Rock(),
+    m_flow_nominal=mWat_flow_nominal,
+    dpExt_nominal=5000)
+                       "Acquifer well"
+    annotation (Placement(transformation(extent={{-10,-20},{10,0}})));
+  Sources.Boundary_pT bou(
+    redeclare package Medium = Medium,
+    nPorts=1) "Pressure boundary condition" annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+equation
+  connect(uHea.y, hea.u)
+    annotation (Line(points={{-39,70},{-12,70}}, color={0,0,127}));
+  connect(aquWel.port_Hot, hea.port_b) annotation (Line(points={{6,0},{6,30},{20,
+          30},{20,64},{10,64}},    color={0,127,255}));
+  connect(aquWel.port_Col, hea.port_a) annotation (Line(points={{-6,0},{-6,0},{-6,
+          30},{-20,30},{-20,64},{-10,64}},    color={0,127,255}));
+  connect(bou.ports[1], hea.port_a) annotation (Line(points={{-60,30},{-20,30},
+          {-20,64},{-10,64}},                  color={0,127,255}));
+  connect(uPum.y, aquWel.u)
+    annotation (Line(points={{-39,-10},{-26,-10},{-26,-10},{-12,-10}},
+                                                 color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    experiment(StopTime=7776000,Tolerance=1e-6),
+    __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Examples/CoolingOffice.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This example shows the application of the model
+<a href=\"modelica://AixLib.Fluid.Geothermal.Aquifer.MultiWell\">AixLib.Fluid.Geothermal.Aquifer.MultiWell</a>.
+</p>
+<p>
+The system consists of two wells, a warm well and a cold well. Water is extracted from the cold well at 12&deg;C and
+after passing through a heat exchanger it is injected in the warm well at 16&deg;C. This may represent the operation of an
+aquifer thermal energy storage system that cools an office building with a constant load of 30 kW.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+March 25, 2024, by Michael Wetter:<br/>
+Corrected broken link and revised documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1855\">IBPSA, issue 1855</a>.
+</li>
+<li>
+May 2023, by Alessandro Maccarini:<br/>
+First Implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CoolingOffice;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Examples/package.mo b/AixLib/Fluid/Geothermal/Aquifer/Examples/package.mo
new file mode 100644
index 0000000000..ea48e7dc09
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Examples/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.Geothermal.Aquifer;
+package Examples "Example models for AixLib.Fluid.Geothermal.Aquifer"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains example models for the classes in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Aquifer\">
+AixLib.Fluid.Geothermal.Aquifer</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Examples/package.order b/AixLib/Fluid/Geothermal/Aquifer/Examples/package.order
new file mode 100644
index 0000000000..36b8a6c3c7
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Examples/package.order
@@ -0,0 +1 @@
+CoolingOffice
diff --git a/AixLib/Fluid/Geothermal/Aquifer/MultiWell.mo b/AixLib/Fluid/Geothermal/Aquifer/MultiWell.mo
new file mode 100644
index 0000000000..5479917ff5
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/MultiWell.mo
@@ -0,0 +1,541 @@
+within AixLib.Fluid.Geothermal.Aquifer;
+model MultiWell "Model of a single well for aquifer thermal energy storage"
+ replaceable package Medium = Modelica.Media.Interfaces.PartialMedium "Medium in the component" annotation (choices(
+        choice(redeclare package Medium = AixLib.Media.Water "Water")));
+  parameter Integer nVol(min=1)=10 "Number of control volumes used in discretization" annotation (
+      Dialog(group="Subsurface"));
+  parameter Modelica.Units.SI.Height h "Aquifer thickness";
+  parameter Modelica.Units.SI.Length d "Distance between wells";
+  parameter Modelica.Units.SI.Height length
+    "Length of one well, used to compute pressure drop";
+  parameter Real nPai=1 "Number of paired wells";
+  parameter Modelica.Units.SI.Radius rWB=0.1 "Wellbore radius" annotation (
+      Dialog(group="Subsurface"));
+  parameter Modelica.Units.SI.Radius rMax=d/2 "Domain radius" annotation (
+      Dialog(group="Subsurface"));
+  parameter Real griFac(min=1) = 1.15 "Grid factor for spacing" annotation (
+      Dialog(group="Subsurface"));
+  parameter Modelica.Units.SI.Temperature TCol_start=283.15
+     "Initial temperature of cold well" annotation (
+      Dialog(group="Subsurface"));
+  parameter Modelica.Units.SI.Temperature THot_start=TCol_start
+     "Initial temperature of warm well" annotation (
+      Dialog(group="Subsurface"));
+  parameter Modelica.Units.SI.Temperature TGroCol=285.15
+     "Undisturbed ground temperature (cold well)" annotation (
+      Dialog(group="Properties of ground"));
+  parameter Modelica.Units.SI.Temperature TGroHot=TGroCol
+     "Undisturbed ground temperature (warm well)" annotation (
+      Dialog(group="Properties of ground"));
+  parameter AixLib.Fluid.Geothermal.Aquifer.Data.Template aquDat
+     "Aquifer thermal properties" annotation (choicesAllMatching=true);
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal "Nominal mass flow rate" annotation (
+      Dialog(group="Hydraulic circuit"));
+  parameter Modelica.Units.SI.PressureDifference dpAquifer_nominal(displayUnit= "Pa")=
+    m_flow_nominal/nPai*Modelica.Constants.g_n/2/Modelica.Constants.pi/h/aquDat.K*log(d/rWB)
+     "Pressure drop at nominal mass flow rate in the aquifer"  annotation (
+      Dialog(group="Hydraulic circuit"));
+  final parameter Modelica.Units.SI.PressureDifference dpWell_nominal(
+      displayUnit="Pa") = 2*resWelCol.dp_nominal
+    "Pressure drop at nominal mass flow rate in the well"
+    annotation (Dialog(group="Hydraulic circuit"));
+  parameter Modelica.Units.SI.PressureDifference dpExt_nominal(displayUnit="Pa")
+    "Pressure drop at nominal mass flow rate in the above-surface system (used to size the head of the well pump)" annotation (
+      Dialog(group="Hydraulic circuit"));
+
+  final parameter Modelica.Units.SI.Radius rVol[nVol](
+    each final fixed=false)
+    "Radius to the center of the i-th domain";
+
+  Modelica.Blocks.Interfaces.RealInput u(
+      final min=-1,
+      final max=1,
+      final unit="1")
+      "Pump control input (-1: extract from hot well, +1: extract from cold well, 0: off)"
+    annotation (Placement(transformation(extent={{-220,-20},{-180,20}}),
+        iconTransformation(extent={{-140,-20},{-100,20}})));
+  Modelica.Blocks.Interfaces.RealOutput PTot(
+    final unit="W")
+  "Total power consumed by all circulation pumps in the wells"
+    annotation (Placement(transformation(extent={{180,30},{200,50}}),
+        iconTransformation(extent={{100,40},{120,60}})));
+
+  Modelica.Fluid.Interfaces.FluidPort_a port_Col(
+    redeclare final package Medium = Medium) "Fluid connector" annotation (Placement(transformation(extent={{-130,
+            130},{-110,150}}),    iconTransformation(extent={{-70,90},{-50,110}})));
+
+  Modelica.Fluid.Interfaces.FluidPort_a port_Hot(
+    redeclare final package Medium = Medium) "Fluid connector" annotation (Placement(transformation(extent={{110,130},
+            {130,150}}),        iconTransformation(extent={{50,90},{70,110}})));
+
+  Modelica.Units.SI.Temperature TAquHot[nVol] = heaCapHot.T
+    "Temperatures of the hot aquifer";
+  Modelica.Units.SI.Temperature TAquCol[nVol] = heaCapCol.T
+    "Temperatures of the cold aquifer";
+
+  Movers.Preconfigured.SpeedControlled_y pumCol(
+    redeclare final package Medium = Medium,
+    final m_flow_nominal=m_flow_nominal/nPai,
+    final dp_nominal=resAqu.dpMea_nominal + 2* resWelCol.dp_nominal + dpExt_nominal)
+       "Pump to extract from cold well" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-120,0})));
+  Movers.Preconfigured.SpeedControlled_y pumHot(
+    redeclare final package Medium = Medium,
+    final m_flow_nominal=pumCol.m_flow_nominal,
+    final dp_nominal=pumCol.dp_nominal) "Pump to extract from hot well"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={120,0})));
+
+  FixedResistances.PressureDrop resWelCol(
+    redeclare final package Medium = Medium,
+    m_flow_nominal=m_flow_nominal/nPai,
+    final from_dp=false,
+    dp_nominal=
+        Modelica.Fluid.Pipes.BaseClasses.WallFriction.Detailed.pressureLoss_m_flow(
+        m_flow=m_flow_nominal/nPai,
+        rho_a=rhoWat,
+        rho_b=rhoWat,
+        mu_a=mu,
+        mu_b=mu,
+        length=length,
+        diameter=rWB,
+        roughness=2.5e-5)) "Pressure drop in the cold well" annotation (
+      Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=-90,
+        origin={-120,70})));
+
+  // The resistances on the hot side are set to be the negative of the cold
+  // side, as they have the same geometry and flow rate.
+  // This reduces the size of the nonlinear system of equations,
+  // and leads to fewer equations in the model.
+  Movers.BaseClasses.IdealSource resWelHot(
+    redeclare final package Medium = Medium,
+    final allowFlowReversal=true,
+    final control_m_flow=false,
+    final control_dp=true,
+    final m_flow_small=1E-4*abs(m_flow_nominal))
+    "Pressure drop in the warm well" annotation (Placement(
+        transformation(
+        extent={{10,10},{-10,-10}},
+        rotation=-90,
+        origin={120,70})));
+
+  BaseClasses.MassFlowRateMultiplier mulCol(
+    redeclare final package Medium = Medium,
+    k=nPai)
+    "Mass flow multiplier for the cold well"
+    annotation (Placement(transformation(
+        extent={{-10,10},{10,-10}},
+        rotation=90,
+        origin={-120,110})));
+  BaseClasses.MassFlowRateMultiplier mulHot(
+    redeclare final package Medium = Medium,
+    k=nPai)
+    "Mass flow multiplier for the warm well"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={120,110})));
+
+  Modelica.Blocks.Math.Add addPum(
+    final k1=1,
+    final k2=1)
+    "Sum of pump electrical power"
+    annotation (Placement(transformation(extent={{40,30},{60,50}})));
+
+  Sensors.RelativePressure dpWelCol(
+    redeclare package Medium = Medium)
+    "Pressure drop of cold well" annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=90,
+        origin={-100,70})));
+
+  Airflow.Multizone.Point_m_flow resAqu(
+    redeclare final package Medium = Medium,
+    m=1,
+    final dpMea_nominal=dpAquifer_nominal,
+    final mMea_flow_nominal=m_flow_nominal/nPai)
+    "Pressure drop in the cold and warm side of the aquifer" annotation (
+      Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=0,
+        origin={0,-70})));
+protected
+  parameter Modelica.Units.SI.Radius r[nVol + 1](each fixed=false)
+    "Radius to the boundary of the i-th domain";
+  parameter Modelica.Units.SI.HeatCapacity C[nVol](each fixed=false)
+    "Heat capacity of segment";
+  parameter Modelica.Units.SI.Volume VWat[nVol](each fixed=false)
+    "Volumes of water";
+  parameter Modelica.Units.SI.ThermalResistance R[nVol](each fixed=false)
+    "Thermal resistances between nodes";
+  parameter Real cAqu(fixed=false)
+    "Heat capacity normalized with volume for aquifer";
+  parameter Real kVol(fixed=false)
+    "Heat conductivity normalized with volume";
+  parameter Modelica.Units.SI.DynamicViscosity mu=Medium.dynamicViscosity(Medium.setState_pTX(
+    Medium.p_default,
+    Medium.T_default,
+    Medium.X_default)) "Water dynamic viscosity";
+  parameter Modelica.Units.SI.SpecificHeatCapacity cpWat=Medium.specificHeatCapacityCp(Medium.setState_pTX(
+    Medium.p_default,
+    Medium.T_default,
+    Medium.X_default)) "Water specific heat capacity";
+  parameter Modelica.Units.SI.Density rhoWat=Medium.density(Medium.setState_pTX(
+    Medium.p_default,
+    Medium.T_default,
+    Medium.X_default)) "Water density";
+  parameter Modelica.Units.SI.ThermalConductivity kWat=Medium.thermalConductivity(Medium.setState_pTX(
+    Medium.p_default,
+    Medium.T_default,
+    Medium.X_default)) "Water thermal conductivity";
+
+  AixLib.Fluid.MixingVolumes.MixingVolume volCol[nVol](
+    redeclare final package Medium = Medium,
+    each final T_start=TCol_start,
+    each final m_flow_nominal=m_flow_nominal,
+    final V=VWat,
+    each nPorts=2)
+    "Array of fluid volumes representing the fluid flow in the cold side of the aquifer"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-100}})));
+
+  Modelica.Thermal.HeatTransfer.Components.HeatCapacitor heaCapCol[nVol](C=C,
+      each T(start=TCol_start, fixed=true))
+    "Array of thermal capacitor in the cold side of the aquifer"
+    annotation (Placement(transformation(extent={{-60,-128},{-40,-108}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalResistor theResCol[nVol](R=R)
+    "Array of thermal resistances in the cold side of the aquifer"
+    annotation (Placement(transformation(extent={{-80,-140},{-100,-120}})));
+
+  MixingVolumes.MixingVolume volHot[nVol](
+    redeclare final package Medium = Medium,
+    each T_start=THot_start,
+    each m_flow_nominal=m_flow_nominal,
+    V=VWat,
+    each nPorts=2)
+    "Array of fluid volumes representing the fluid flow in the warm side of the aquifer"
+    annotation (Placement(transformation(extent={{50,-80},{30,-100}})));
+  Modelica.Thermal.HeatTransfer.Components.HeatCapacitor heaCapHot[nVol](C=C,
+    each T(start=THot_start, fixed=true))
+    "Array of thermal capacitor in the warm side of the aquifer"
+    annotation (Placement(transformation(extent={{50,-128},{30,-108}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalResistor theResHot[nVol](R=R)
+    "Array of thermal resistances in the warm side of the aquifer"
+    annotation (Placement(transformation(extent={{80,-140},{100,-120}})));
+
+  Modelica.Thermal.HeatTransfer.Sources.FixedTemperature groTemCol(
+    final T=TGroCol)
+    "Boundary condition ground temperature in the cold side of the aquifer"
+    annotation (Placement(transformation(extent={{-140,-140},{-120,-120}})));
+  Modelica.Thermal.HeatTransfer.Sources.FixedTemperature groTemHot(
+    final T=TGroHot)
+    "Boundary condition ground temperature in the warm side of the aquifer"
+    annotation (Placement(transformation(extent={{140,-140},{120,-120}})));
+
+  Modelica.Blocks.Nonlinear.Limiter limCol(final uMax=1, final uMin=0) "Limiter for pump signal"
+    annotation (Placement(transformation(extent={{-160,-10},{-140,10}})));
+  Modelica.Blocks.Math.Gain gaiCon(final k=-1) "Inversion of control signal"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+  Modelica.Blocks.Nonlinear.Limiter limHot(final uMax=1, final uMin=0) "Limiter for pump signal"
+    annotation (Placement(transformation(extent={{80,-10},{100,10}})));
+
+  Modelica.Blocks.Math.Gain gaiPum(final k=nPai) "Gain used to scale the pump electrical power"
+    annotation (Placement(transformation(extent={{80,30},{100,50}})));
+initial equation
+  assert(rWB < rMax, "In " + getInstanceName() + ": Require rWB < rMax");
+  assert(0 < rWB, "In " + getInstanceName() + ": Require 0 < rWB");
+  assert(rMax <= d/2, "In " + getInstanceName() + ": Require rMax <= d/2");
+
+  cAqu=aquDat.dSoi*aquDat.cSoi*(1-aquDat.phi);
+  kVol=kWat*aquDat.phi+aquDat.kSoi*(1-aquDat.phi);
+
+  r[1] = rWB;
+  for i in 2:nVol+1 loop
+    r[i]= r[i-1] + (rMax - rWB)  * (1-griFac)/(1-griFac^(nVol)) * griFac^(i-2);
+  end for;
+  for i in 1:nVol loop
+    rVol[i] = (r[i]+r[i+1])/2;
+  end for;
+  for i in 1:nVol loop
+    C[i] = cAqu*h*3.14*(r[i+1]^2-r[i]^2);
+  end for;
+  for i in 1:nVol loop
+    VWat[i] = aquDat.phi*h*3.14*(r[i+1]^2-r[i]^2);
+  end for;
+
+  R[nVol]=Modelica.Math.log(rMax/rVol[nVol])/(2*Modelica.Constants.pi*kVol*h);
+  for i in 1:nVol-1 loop
+    R[i] = Modelica.Math.log(rVol[i+1]/rVol[i])/(2*Modelica.Constants.pi*kVol*h);
+  end for;
+
+equation
+  if nVol > 1 then
+    for i in 1:(nVol - 1) loop
+      connect(volCol[i].ports[2], volCol[i + 1].ports[1]);
+    end for;
+  end if;
+  connect(resAqu.port_b, volCol[nVol].ports[2]) annotation (Line(points={{-10,-70},
+          {-49,-70},{-49,-80}}, color={0,127,255}));
+  connect(resAqu.port_a, volHot[nVol].ports[2])
+    annotation (Line(points={{10,-70},{39,-70},{39,-80}},color={0,127,255}));
+  connect(pumCol.port_a, volCol[1].ports[1]) annotation (Line(points={{-120,-10},
+          {-120,-70},{-51,-70},{-51,-80}}, color={0,127,255}));
+  connect(pumHot.port_a, volHot[1].ports[1]) annotation (Line(points={{120,-10},
+          {120,-70},{41,-70},{41,-80}}, color={0,127,255}));
+
+  if nVol > 1 then
+    for i in 1:(nVol - 1) loop
+      connect(volHot[i].ports[2], volHot[i + 1].ports[1]);
+    end for;
+  end if;
+
+  if nVol > 1 then
+    for i in 1:(nVol - 1) loop
+      connect(heaCapCol[i + 1].port, theResCol[i].port_b);
+    end for;
+  end if;
+
+  if nVol > 1 then
+    for i in 1:(nVol - 1) loop
+      connect(heaCapHot[i + 1].port, theResHot[i].port_b);
+    end for;
+  end if;
+
+  connect(groTemCol.port, theResCol[nVol].port_b)
+    annotation (Line(points={{-120,-130},{-100,-130}},
+                                                   color={191,0,0}));
+
+  connect(volCol.heatPort, heaCapCol.port) annotation (Line(points={{-60,-90},{-70,
+          -90},{-70,-130},{-50,-130},{-50,-128}},
+                                    color={191,0,0}));
+  connect(theResCol.port_a, volCol.heatPort) annotation (Line(points={{-80,-130},
+          {-70,-130},{-70,-90},{-60,-90}},
+                                        color={191,0,0}));
+  connect(groTemHot.port, theResHot[nVol].port_b)
+    annotation (Line(points={{120,-130},{100,-130}},
+                                                 color={191,0,0}));
+  connect(volHot.heatPort, heaCapHot.port) annotation (Line(points={{50,-90},{60,
+          -90},{60,-130},{40,-130},{40,-128}},
+                                  color={191,0,0}));
+  connect(theResHot.port_a, volHot.heatPort) annotation (Line(points={{80,-130},
+          {60,-130},{60,-90},{50,-90}},
+                                    color={191,0,0}));
+  connect(pumCol.port_b, resWelCol.port_a)
+    annotation (Line(points={{-120,10},{-120,60}},
+                                                 color={0,127,255}));
+  connect(resWelHot.port_a, pumHot.port_b)
+    annotation (Line(points={{120,60},{120,10}},
+                                               color={0,127,255}));
+  connect(limCol.y, pumCol.y) annotation (Line(points={{-139,0},{-138,0},{-138,6.66134e-16},
+          {-132,6.66134e-16}},                                                             color={0,0,127}));
+  connect(gaiCon.y, limHot.u) annotation (Line(points={{61,0},{78,0}},   color={0,0,127}));
+  connect(limHot.y, pumHot.y) annotation (Line(points={{101,0},{100,0},{100,6.66134e-16},
+          {108,6.66134e-16}},                                                          color={0,0,127}));
+  connect(gaiCon.u, u) annotation (Line(points={{38,0},{0,0},{0,20},{-170,20},{-170,
+          0},{-200,0}},                                                                color={0,0,127}));
+  connect(limCol.u, u) annotation (Line(points={{-162,0},{-200,0}},                    color={0,0,127}));
+  connect(resWelCol.port_b, mulCol.port_a)
+    annotation (Line(points={{-120,80},{-120,100}},
+                                                 color={0,127,255}));
+  connect(mulCol.port_b, port_Col) annotation (Line(points={{-120,120},{-120,140}},                color={0,127,255}));
+  connect(mulHot.port_b, port_Hot) annotation (Line(points={{120,120},{120,140}},              color={0,127,255}));
+  connect(resWelHot.port_b, mulHot.port_a)
+    annotation (Line(points={{120,80},{120,100}},
+                                               color={0,127,255}));
+  connect(pumCol.P, addPum.u1)
+    annotation (Line(points={{-129,11},{-129,46},{38,46}},                  color={0,0,127}));
+  connect(addPum.y, gaiPum.u) annotation (Line(points={{61,40},{78,40}},  color={0,0,127}));
+  connect(pumHot.P, addPum.u2) annotation (Line(points={{111,11},{111,20},{20,20},
+          {20,34},{38,34}}, color={0,0,127}));
+  connect(gaiPum.y, PTot) annotation (Line(points={{101,40},{190,40}}, color={0,0,127}));
+  connect(dpWelCol.port_a, resWelCol.port_b) annotation (Line(points={{-100,80},
+          {-100,90},{-120,90},{-120,80}},
+                                      color={0,127,255}));
+  connect(dpWelCol.port_b, resWelCol.port_a) annotation (Line(points={{-100,60},
+          {-100,52},{-120,52},{-120,60}},
+                                      color={0,127,255}));
+  connect(dpWelCol.p_rel, resWelHot.dp_in) annotation (Line(points={{-91,70},{
+          100,70},{100,76},{112,76}}, color={0,0,127}));
+
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false,
+    extent={{-100,-100},
+            {100,100}}),
+    graphics={
+        Rectangle(
+          extent={{-20,100},{20,-2}},
+          fillColor={175,175,175},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{20,2},{-20,-6}},
+          lineColor={0,0,0},
+          fillColor={175,175,175},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={211,168,137},
+          fillPattern=FillPattern.Forward),
+        Rectangle(
+          extent={{-100,20},{100,-48}},
+          fillColor={241,241,0},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Rectangle(
+          extent={{-100,100},{100,82}},
+          lineColor={0,0,0},
+          fillColor={0,140,72},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-84,100},{-36,-14}},
+          fillColor={85,170,255},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{-36,-6},{-84,-22}},
+          lineColor={0,0,0},
+          fillColor={28,108,200},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-147,-108},{153,-148}},
+          textColor={0,0,255},
+          textString="%name"),
+        Rectangle(
+          extent={{36,100},{84,-14}},
+          fillColor={238,22,26},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{84,-6},{36,-22}},
+          lineColor={0,0,0},
+          fillColor={182,12,18},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-140,46},{-110,22}},
+          textColor={0,0,127},
+          textString="uPum"),
+        Text(
+          extent={{106,84},{136,60}},
+          textColor={0,0,127},
+          textString="PTot"),
+        Text(
+         extent={{-52,144},{-172,94}},
+          textColor={0,0,100},
+          textString=DynamicSelect("", String(pumCol.heatPort.T-273.15, format=".1f"))),
+        Text(
+         extent={{170,144},{50,94}},
+          textColor={0,0,100},
+          textString=DynamicSelect("", String(pumHot.heatPort.T-273.15, format=".1f")))}),
+        Diagram(
+        coordinateSystem(preserveAspectRatio=false, extent={{-180,-160},{180,140}})),
+        defaultComponentName="aquWel",
+        Documentation(info="<html>
+<p>
+This model simulates aquifer thermal energy storage, using one or multiple pairs of cold and hot wells.
+</p>
+<p>
+To calculate aquifer temperature at different locations over time, the model applies
+physical principles of water flow and heat transfer phenomena. The model is based on
+the partial differential equation (PDE) for 1D conductive-convective transient
+radial heat transport in porous media
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&rho; c (&part; T(r,t) &frasl; &part;t) =
+k (&part;&sup2; T(r,t) &frasl; &part;r&sup2;) - &rho;<sub>w</sub> c<sub>w</sub> u(&part; T(r,t) &frasl; &part;t),
+</p>
+<p>
+where
+<i>&rho;</i>
+is the mass density,
+<i>c</i>
+is the specific heat capacity per unit mass,
+<i>T</i>
+is the temperature at location <i>r</i> and time <i>t</i>,
+<i>u</i> is water velocity and
+<i>k</i> is the heat conductivity. The subscript <i>w</i> indicates water.
+The first term on the right hand side of the equation describes the effect of conduction, while
+the second term describes the fluid flow.
+</p>
+<p>
+The pressure losses in the aquifer are calculated using the Darcy's law
+<p align=\"center\" style=\"font-style:italic;\">
+&#916;p = &#7745; g &frasl; (2 &#960; K h ln(rMax &frasl; rWB)),
+</p>
+<p>
+where <i>&#7745;</i> is the water mass flow rate, <i>g</i> is the gravitational acceleration,
+<i>K</i> is the hydraulic conductivity, <i>h</i> is the thickness of the aquifer, 
+<i>rMax</i> is the domain radius and <i>rWB</i> is the well radius.
+The pressure losses in the wells are calculated using
+<a href=\"modelica://Modelica.Fluid.Pipes.BaseClasses.WallFriction.Detailed.pressureLoss_m_flow\">
+Modelica.Fluid.Pipes.BaseClasses.WallFriction.Detailed.pressureLoss_m_flow</a>.
+</p>
+<h4>Spatial discretization</h4>
+<p>
+To discretize the conductive-convective equation, the domain is divided into a series
+of thermal capacitances and thermal resistances along the radial direction. The
+implementation uses an array of
+<a href=\"modelica://Modelica.Thermal.HeatTransfer.Components.HeatCapacitor\">
+Modelica.Thermal.HeatTransfer.Components.HeatCapacitor</a>
+and <a href=\"modelica://Modelica.Thermal.HeatTransfer.Components.ThermalResistor\">
+Modelica.Thermal.HeatTransfer.Components.ThermalResistor</a>.
+Fluid flow was modelled by adding a series of fluid volumes, which are connected
+to the thermal capacitances via heat ports. The fluid stream was developed using
+the model <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">AixLib.Fluid.MixingVolumes.MixingVolume</a>.
+The geometric representation of the model is illustrated in the figure below.
+</p>
+<p align=\"center\">
+<img  alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Aquifer/Geometry.png\">
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+By default, the component consists of a single pair of wells: one cold well and one warm well.
+The number of paired wells can be increased by modifing the parameters <code>nPai</code>.
+The effect is a proportional increase of thermal capacity, and the mass flow rate at <code>port_a</code>
+and <code>port_b</code> is equally distributed to the pairs of well, thus
+all pairs have the same mass flow rates and temperatures, and the quantities
+at the fluid ports is for all well combined, as is the electricity consumption <code>PTot</code>
+for the well pumps.
+</p>
+<p>
+To ensure conservation of energy, the wells are connected via fluid ports.
+To avoid thermal interferences, make sure that the aquifer domain radius
+<code>rMax</code> is large enough for your specific use case.
+</p>
+<p>
+Circulation pumps are included in the model and they can be controlled by acting on the input connector.
+The input must vary between <i>[1, -1]</i>.
+A positive value will circulate water
+clockwise (from <code>port_Hot</code> to <code>port_Col</code>, thus 
+extraction from the cold well and injection into the warm well).
+A negative value will circulate water anticlockwise.
+</p>
+<p>
+The temperature values in the warm and cold aquifers can be accessed using
+<code>TAquHot</code> and <code>TAquCol</code>.
+These temperatures correspond to the temperatures of each thermal capacitance
+in the discretized domain. The location of the thermal capacitance is expressed by <code>rVol</code>.
+</p>
+<h4>Implementation</h4>
+<p>
+The model computes the flow resistance of the cold well and the cold acquifer.
+Because of symmetry, the warm side has the same flow resistances.
+To reduce the number of equations in the model, the flow resistance of the warm
+side is set to the same flow resistance as on the cold side, but with the
+sign reversed.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22 2023, by Alessandro Maccarini and Michael Wetter:<br/>
+First Implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end MultiWell;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Validation/NumberWells.mo b/AixLib/Fluid/Geothermal/Aquifer/Validation/NumberWells.mo
new file mode 100644
index 0000000000..a2ae884d80
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Validation/NumberWells.mo
@@ -0,0 +1,86 @@
+within AixLib.Fluid.Geothermal.Aquifer.Validation;
+model NumberWells
+  "Test model for aquifer thermal energy storage with multiple wells"
+  extends Modelica.Icons.Example;
+
+  package Medium = AixLib.Media.Water "Medium model";
+
+  model MyWell = MultiWell (
+    redeclare package Medium = AixLib.Media.Water,
+    nVol=50,
+    h=10,
+    d=4800,
+    length=200,
+    THot_start=303.15,
+    TGroCol=273.15,
+    TGroHot=303.15,
+    aquDat=AixLib.Fluid.Geothermal.Aquifer.Data.Rock(),
+    m_flow_nominal=0.1,
+    dpExt_nominal=0) "Well model";
+
+  MyWell aquWel1(d=4800)
+  "ATES with one pair of wells"
+    annotation (Placement(transformation(extent={{-20,20},{0,40}})));
+
+  MyWell aquWel2(
+    d=4800,
+     nPai=2,
+     m_flow_nominal=0.2)
+    "ATES with two pairs of wells"
+    annotation (Placement(transformation(extent={{-20,-60},{0,-40}})));
+  Modelica.Blocks.Sources.Constant uPum(k=1) "Pump control signal"
+    annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+  Sources.Boundary_pT bou(
+    redeclare package Medium = Medium,
+    nPorts=2) "Sink"
+           annotation (Placement(transformation(extent={{60,-10},{40,10}})));
+  Modelica.Blocks.Sources.RealExpression temWel1(
+    y=aquWel1.TAquHot[10])
+    "Temperature output from aquifer model with one pair of wells"
+    annotation (Placement(transformation(extent={{20,72},{40,92}})));
+  Modelica.Blocks.Sources.RealExpression temWel2(
+    y=aquWel2.TAquHot[10])
+    "Temperature output from aquifer model with two pairs of wells"
+    annotation (Placement(transformation(extent={{20,40},{40,60}})));
+  AixLib.Utilities.Diagnostics.CheckEquality cheEqu
+    "Assertion that checks for equality of results"
+    annotation (Placement(transformation(extent={{60,60},{80,80}})));
+equation
+  connect(uPum.y, aquWel1.u) annotation (Line(points={{-59,0},{-40,0},{-40,30},
+          {-22,30}}, color={0,0,127}));
+  connect(aquWel2.u,uPum. y) annotation (Line(points={{-22,-50},{-40,-50},{-40,
+          0},{-59,0}}, color={0,0,127}));
+  connect(aquWel2.port_Col, aquWel2.port_Hot) annotation (Line(points={{-16,-40},
+          {-16,-20},{-4,-20},{-4,-40}}, color={0,127,255}));
+  connect(aquWel1.port_Col, aquWel1.port_Hot) annotation (Line(points={{-16,40},
+          {-16,60},{-4,60},{-4,40}}, color={0,127,255}));
+  connect(bou.ports[1], aquWel1.port_Hot) annotation (Line(points={{40,-1},{6,-1},
+          {6,60},{-4,60},{-4,40}},     color={0,127,255}));
+  connect(bou.ports[2], aquWel2.port_Hot) annotation (Line(points={{40,1},{26,1},
+          {26,0},{6,0},{6,-20},{-4,-20},{-4,-40}}, color={0,127,255}));
+  connect(cheEqu.u1, temWel1.y) annotation (Line(points={{58,76},{46,76},{46,82},
+          {41,82}}, color={0,0,127}));
+  connect(cheEqu.u2, temWel2.y) annotation (Line(points={{58,64},{46,64},{46,50},
+          {41,50}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    experiment(StopTime=31536000, Tolerance=1e-6),
+    __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Validation/NumberWells.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+Example that verifies the scalability of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Aquifer.MultiWell\">AixLib.Fluid.Geothermal.Aquifer.MultiWell</a>
+when multiple wells are used.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 2023, by Alessandro Maccarini:<br/>
+First Implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end NumberWells;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Validation/SimulationTest.mo b/AixLib/Fluid/Geothermal/Aquifer/Validation/SimulationTest.mo
new file mode 100644
index 0000000000..67536b7556
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Validation/SimulationTest.mo
@@ -0,0 +1,90 @@
+within AixLib.Fluid.Geothermal.Aquifer.Validation;
+model SimulationTest
+  "Test model for aquifer thermal energy storage in comparison with other geothermal simulators"
+  extends Modelica.Icons.Example;
+
+  package Medium = AixLib.Media.Water "Medium model";
+
+  MultiWell aquWel(
+    redeclare package Medium = Medium,
+    nVol=232,
+    h=200,
+    d=4800,
+    length=40,
+    griFac=1.1,
+    TCol_start=307.15,
+    THot_start=393.15,
+    TGroCol=307.15,
+    TGroHot=393.15,
+    aquDat=AixLib.Fluid.Geothermal.Aquifer.Data.Rock(),
+    m_flow_nominal=1,
+    dpExt_nominal=0) "Aquifer wells"
+    annotation (Placement(transformation(extent={{-20,20},{0,40}})));
+  Sources.Boundary_pT bou(
+    redeclare package Medium = Medium,
+    nPorts=1) "Boundary condition for pressure"
+           annotation (Placement(transformation(extent={{60,50},{40,70}})));
+  Modelica.Blocks.Sources.CombiTimeTable uPum(table=[0.0,-1; 86400*120,-1; 86400
+        *120,0; 86400*180,0; 86400*180,1; 86400*300,1; 86400*300,0])
+    "Pump control signal"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+equation
+  connect(aquWel.port_Col, aquWel.port_Hot) annotation (Line(points={{-16,40},{
+          -16,60},{-4,60},{-4,40}}, color={0,127,255}));
+  connect(bou.ports[1], aquWel.port_Hot)
+    annotation (Line(points={{40,60},{-4,60},{-4,40}}, color={0,127,255}));
+  connect(uPum.y[1], aquWel.u)
+    annotation (Line(points={{-59,30},{-22,30}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    experiment(StopTime=31536000, Tolerance=1e-6),
+    __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Validation/SimulationTest.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This validation case simulates an idealized operation of an aquifer thermal storage system. Results
+are compared with simulations from a test suite developed by Mindel et al. (2021).
+This test suite comprises a set of cases to assess the thermo-hydraulic modelling capabilities of various geothermal simulators.
+</p>
+<p>
+The comparison was carried out with respect to the test case called TC2 - well-test comparison.
+The main goal of TC2 is to compare aquifer temperatures under a typical operation of an ATES system
+consisting of injection, falloff, drawdown, and build-up. The injection phase represents the charging period,
+while the drawdown phase represents the discharge period.
+Intermediate phases of falloff and build-up represent periods of storage or inactivity.
+The overall operational period is one year, and the sequence of the different phases is the following:
+</p>
+<ul>
+<li>Injection: Water is pumped at Q = 0.001 m<sup>3</sup> s<sup>-1</sup> and T<sub>inj</sub> = 120C for 120 days.</li>
+<li>Falloff: Well is shut-in, Q = 0 m<sup>3</sup> s<sup>-1</sup> for 60 days.</li>
+<li>Drawdown: Water is pumped at Q = -0.001 m<sup>3</sup> s<sup>-1</sup> for 120 days.</li>
+<li>Build-up phase: Well is shut-in, at Q = 0 m<sup>3</sup> s<sup>-1</sup> for 65.25.</li>
+</ul>
+The figure below shows the temperature vs. time comparison for a virtual sensor located at r = 1 m and r= 10 m from the well.
+<p align=\"center\">
+<img  alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Aquifer/results.png\" width=\"600\">
+</p>
+<h4>References</h4>
+<p>
+Julian E. Mindel, Peter Alt-Epping, Antoine Armandine Les Landes, Stijn Beernink, Daniel T. Birdsell,
+Martin Bloemendal, Virginie Hamm, Simon Lopez, Charles Maragna, Carsten M. Nielsen, Sebastia Olivella,
+Marc Perreaux, Maarten W. Saaltink, Martin O. Saar, Daniela Van den Heuvel, Ruben Vidal, Thomas Driesner,
+<i>Benchmark study of simulators for thermo-hydraulic modelling of low enthalpy geothermal processes</i>,
+Geothermics,
+Volume 96,
+2021,
+102130,
+ISSN 0375-6505,
+https://doi.org/10.1016/j.geothermics.2021.102130.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 2023, by Alessandro Maccarini:<br/>
+First Implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimulationTest;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Validation/package.mo b/AixLib/Fluid/Geothermal/Aquifer/Validation/package.mo
new file mode 100644
index 0000000000..6a0e115e02
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Validation/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.Geothermal.Aquifer;
+package Validation "Validation models for aquifer thermal energy storage"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains validation models for the classes in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Aquifer\">
+AixLib.Fluid.Geothermal.Aquifer</a>.
+</p>
+</html>"));
+end Validation;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/Validation/package.order b/AixLib/Fluid/Geothermal/Aquifer/Validation/package.order
new file mode 100644
index 0000000000..7413e308d5
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/Validation/package.order
@@ -0,0 +1,2 @@
+NumberWells
+SimulationTest
diff --git a/AixLib/Fluid/Geothermal/Aquifer/package.mo b/AixLib/Fluid/Geothermal/Aquifer/package.mo
new file mode 100644
index 0000000000..abe29ff733
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/package.mo
@@ -0,0 +1,33 @@
+within AixLib.Fluid.Geothermal;
+package Aquifer "Package with aquifer thermal energy storage models"
+  extends Modelica.Icons.Package;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+Package with models for aquifer thermal energy storage.
+</p>
+</html>"),
+    Icon(graphics={
+        Rectangle(
+          extent={{-54,66},{-40,-16}},
+          fillColor={95,95,95},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0},
+          pattern=LinePattern.None),
+        Ellipse(
+          extent={{-86,-14},{-4,-58}},
+          fillColor={95,95,95},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Ellipse(
+          extent={{4,-14},{86,-58}},
+          fillColor={95,95,95},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Rectangle(
+          extent={{36,66},{50,-16}},
+          fillColor={95,95,95},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0},
+          pattern=LinePattern.None)}));
+end Aquifer;
diff --git a/AixLib/Fluid/Geothermal/Aquifer/package.order b/AixLib/Fluid/Geothermal/Aquifer/package.order
new file mode 100644
index 0000000000..810a212652
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Aquifer/package.order
@@ -0,0 +1,4 @@
+MultiWell
+Data
+Examples
+Validation
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXOneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXOneUTube.mo
index 1b6f307ecd..271cda4436 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXOneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXOneUTube.mo
@@ -88,19 +88,19 @@ equation
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXOneUTube.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This example simulates the interior thermal behavior of a single U-tube borehole segment.
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source FixedBoundary with Boundary_pT. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- June 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This example simulates the interior thermal behavior of a single U-tube borehole segment.
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source FixedBoundary with Boundary_pT. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+June 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalHEXOneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXTwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXTwoUTube.mo
index 9f94dcd369..494072ad22 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXTwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXTwoUTube.mo
@@ -18,7 +18,6 @@ model InternalHEXTwoUTube
     dp2_nominal=10,
     dp3_nominal=10,
     dp4_nominal=10,
-    dynFil=true,
     borFieDat=borFieDat,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     TGro_start(displayUnit="K") = 285.15,
@@ -116,19 +115,25 @@ equation
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalHEXTwoUTube.mos"
         "Simulate and plot"),
             Documentation(info="<html>
- This example simulates the interior thermal behavior of a double U-tube borehole segment.
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source FixedBoundary with Boundary_pT. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- June 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This example simulates the interior thermal behavior of a double U-tube borehole segment.
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source FixedBoundary with Boundary_pT. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+June 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalHEXTwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesOneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesOneUTube.mo
index cb539317c2..5597e15d4a 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesOneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesOneUTube.mo
@@ -62,17 +62,17 @@ equation
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesOneUTube.mos"
         "Simulate and plot"),
   Documentation(info="<html>
-   This example tests the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesOneUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesOneUTube</a>
- for the dynamic behavior of the filling material in a single U-tube borehole.
- </html>",revisions="<html>
- <ul>
- <li>
- July 19, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  This example tests the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesOneUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesOneUTube</a>
+for the dynamic behavior of the filling material in a single U-tube borehole.
+</html>", revisions="<html>
+<ul>
+<li>
+July 19, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalResistancesOneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesTwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesTwoUTube.mo
index 439e4a2cc4..04d887d3bd 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesTwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesTwoUTube.mo
@@ -76,17 +76,17 @@ equation
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Examples/InternalResistancesTwoUTube.mos"
         "Simulate and plot"),
   Documentation(info="<html>
- This example tests the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesTwoUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesTwoUTube</a>
- for the dynamic behavior of the filling material in a double U-tube borehole.
- </html>",revisions="<html>
- <ul>
- <li>
- July 19, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This example tests the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesTwoUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesTwoUTube</a>
+for the dynamic behavior of the filling material in a double U-tube borehole.
+</html>", revisions="<html>
+<ul>
+<li>
+July 19, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalResistancesTwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/ConvectionResistanceCircularPipe.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/ConvectionResistanceCircularPipe.mo
index 68f941e72e..277cea4924 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/ConvectionResistanceCircularPipe.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/ConvectionResistanceCircularPipe.mo
@@ -41,23 +41,23 @@ equation
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/ConvectionResistanceCircularPipe.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example validates the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.convectionResistanceCircularPipe\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.convectionResistanceCircularPipe</a>
- for the evaluation of the convection thermal resistance in circular pipes.
- </p>
- <p>
- In this validation case, the fluid mass flow rate increases with time so that
- <i>Re = t</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 21, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.convectionResistanceCircularPipe\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.convectionResistanceCircularPipe</a>
+for the evaluation of the convection thermal resistance in circular pipes.
+</p>
+<p>
+In this validation case, the fluid mass flow rate increases with time so that
+<i>Re = t</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 21, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConvectionResistanceCircularPipe;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesOneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesOneUTube.mo
index da6053348d..65a1561703 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesOneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesOneUTube.mo
@@ -57,7 +57,8 @@ initial equation
       kMed=kMed,
       muMed=muMed,
       cpMed=cpMed,
-      m_flow_nominal=m_flow_nominal);
+      m_flow_nominal=m_flow_nominal,
+      instanceName=getInstanceName());
 
   annotation (
     __Dymola_Commands(file=
@@ -65,20 +66,27 @@ initial equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=1.0),
     Documentation(info="<html>
- <p>
- This example validates the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube</a>
- for the evaluation of the internal thermal resistances of a single U-tube
- borehole.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 21, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube</a>
+for the evaluation of the internal thermal resistances of a single U-tube
+borehole.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+June 21, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalResistancesOneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesOneUTubeNegative.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesOneUTubeNegative.mo
index 216adb374f..2db4d8c0d1 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesOneUTubeNegative.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesOneUTubeNegative.mo
@@ -56,7 +56,8 @@ initial equation
       kMed=kMed,
       muMed=muMed,
       cpMed=cpMed,
-      m_flow_nominal=m_flow_nominal);
+      m_flow_nominal=m_flow_nominal,
+      instanceName=getInstanceName());
 
   annotation (
     __Dymola_Commands(file=
@@ -64,25 +65,32 @@ initial equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=1.0),
     Documentation(info="<html>
- <p>
- This example validates the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube</a>
- for the evaluation of the internal thermal resistances of a single U-tube
- borehole.
- </p>
- <p>
- In this case, the shank spacing is defined such that the pipes are close to the
- borehole wall, rendering the short-circuit thermal resistances negative. The
- capacity location <code>x</code> is then automatically set to zero.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 21, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube</a>
+for the evaluation of the internal thermal resistances of a single U-tube
+borehole.
+</p>
+<p>
+In this case, the shank spacing is defined such that the pipes are close to the
+borehole wall, rendering the short-circuit thermal resistances negative. The
+capacity location <code>x</code> is then automatically set to zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+June 21, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalResistancesOneUTubeNegative;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesTwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesTwoUTube.mo
index 06d6456981..f00adcb852 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesTwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesTwoUTube.mo
@@ -58,7 +58,8 @@ initial equation
       kMed=kMed,
       muMed=muMed,
       cpMed=cpMed,
-      m_flow_nominal=m_flow_nominal);
+      m_flow_nominal=m_flow_nominal,
+      instanceName=getInstanceName());
 
   annotation (
     __Dymola_Commands(file=
@@ -66,20 +67,27 @@ initial equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=1.0),
     Documentation(info="<html>
- <p>
- This example validates the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube</a>
- for the evaluation of the internal thermal resistances of a double U-tube
- borehole.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 21, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube</a>
+for the evaluation of the internal thermal resistances of a double U-tube
+borehole.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+June 21, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalResistancesTwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesTwoUTubeNegative.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesTwoUTubeNegative.mo
index 1e3728ea1f..089597e556 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesTwoUTubeNegative.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/InternalResistancesTwoUTubeNegative.mo
@@ -58,7 +58,8 @@ initial equation
       kMed=kMed,
       muMed=muMed,
       cpMed=cpMed,
-      m_flow_nominal=m_flow_nominal);
+      m_flow_nominal=m_flow_nominal,
+      instanceName=getInstanceName());
 
   annotation (
     __Dymola_Commands(file=
@@ -66,25 +67,32 @@ initial equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=1.0),
     Documentation(info="<html>
- <p>
- This example validates the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube</a>
- for the evaluation of the internal thermal resistances of a double U-tube
- borehole.
- </p>
- <p>
- In this case, the shank spacing is defined such that the pipes are close to the
- borehole wall, rendering the short-circuit thermal resistances negative. The
- capacity location <code>x</code> is then automatically set to zero.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 21, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube</a>
+for the evaluation of the internal thermal resistances of a double U-tube
+borehole.
+</p>
+<p>
+In this case, the shank spacing is defined such that the pipes are close to the
+borehole wall, rendering the short-circuit thermal resistances negative. The
+capacity location <code>x</code> is then automatically set to zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+June 21, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalResistancesTwoUTubeNegative;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/MultipoleThermalResistances_OneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/MultipoleThermalResistances_OneUTube.mo
index aab3a8d335..023b0c0fce 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/MultipoleThermalResistances_OneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/MultipoleThermalResistances_OneUTube.mo
@@ -44,30 +44,30 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=1.0),
     Documentation(info="<html>
- <p>
- This example validates the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.multipoleThermalResistances\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.multipoleThermalResistances</a>
- for the evaluation of the borehole thermal resistances.
- </p>
- <p>
- The multipole method is used to evaluate thermal resistances for a single U-tube
- borehole with asymmetrically positionned pipes. Results are compared to
- reference values given in Claesson and Hellstr&ouml;m (2011).
- </p>
- <h4>References</h4>
- <p>
- Claesson, J., &amp; Hellstr&ouml;m, G. (2011). Multipole method to calculate
- borehole thermal resistances in a borehole heat exchanger. <i>HVAC&amp;R
- Research, 17</i>(6), 895-911.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 21, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.multipoleThermalResistances\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.multipoleThermalResistances</a>
+for the evaluation of the borehole thermal resistances.
+</p>
+<p>
+The multipole method is used to evaluate thermal resistances for a single U-tube
+borehole with asymmetrically positionned pipes. Results are compared to
+reference values given in Claesson and Hellstr&ouml;m (2011).
+</p>
+<h4>References</h4>
+<p>
+Claesson, J., &amp; Hellstr&ouml;m, G. (2011). Multipole method to calculate
+borehole thermal resistances in a borehole heat exchanger. <i>HVAC&amp;R
+Research, 17</i>(6), 895-911.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 21, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MultipoleThermalResistances_OneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/MultipoleThermalResistances_TwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/MultipoleThermalResistances_TwoUTube.mo
index 591f9f5f3f..b593cfb94c 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/MultipoleThermalResistances_TwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/Validation/MultipoleThermalResistances_TwoUTube.mo
@@ -50,30 +50,30 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=1.0),
     Documentation(info="<html>
- <p>
- This example validates the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.multipoleThermalResistances\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.multipoleThermalResistances</a>
- for the evaluation of the borehole thermal resistances.
- </p>
- <p>
- The multipole method is used to evaluate thermal resistances for a double U-tube
- borehole with symmetrically positionned pipes. Results are compared to
- reference values given in Claesson (2012).
- </p>
- <h4>References</h4>
- <p>
- Claesson, J. (2012). Multipole method to calculate borehole thermal resistances.
- Mathematical report. Department of Building Physics, Lund University, Box 118,
- SE-221 00 Lund, Sweden. 128 pages.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 21, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.multipoleThermalResistances\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.multipoleThermalResistances</a>
+for the evaluation of the borehole thermal resistances.
+</p>
+<p>
+The multipole method is used to evaluate thermal resistances for a double U-tube
+borehole with symmetrically positionned pipes. Results are compared to
+reference values given in Claesson (2012).
+</p>
+<h4>References</h4>
+<p>
+Claesson, J. (2012). Multipole method to calculate borehole thermal resistances.
+Mathematical report. Department of Building Physics, Lund University, Box 118,
+SE-221 00 Lund, Sweden. 128 pages.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 21, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MultipoleThermalResistances_TwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/convectionResistanceCircularPipe.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/convectionResistanceCircularPipe.mo
index f3066daec5..2a6ae4ee44 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/convectionResistanceCircularPipe.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/convectionResistanceCircularPipe.mo
@@ -22,7 +22,7 @@ function convectionResistanceCircularPipe
     "Convection resistance (or conduction in fluid if no mass flow)";
 
 protected
-  parameter Modelica.Units.SI.Radius rTub_in=rTub - eTub "Pipe inner radius";
+  Modelica.Units.SI.Radius rTub_in=rTub - eTub "Pipe inner radius";
   Modelica.Units.SI.CoefficientOfHeatTransfer h
     "Convective heat transfer coefficient of the fluid";
 
@@ -64,56 +64,61 @@ algorithm
 
   RFluPip := 1/(2*Modelica.Constants.pi*rTub_in*hSeg*h);
 
-  annotation (Diagram(graphics), Documentation(info="<html>
- <p>
- This model computes the convection resistance in the pipes of a borehole segment 
- with heigth <i>h<sub>Seg</sub></i> using correlations suggested by Bergman et al. (2011).
- </p>
- <p>
- If the flow is laminar (<i>Re &le; 2300</i>, with <i>Re</i> being the Reynolds number of the flow),
- the Nusselt number of the flow is assumed to be constant at 3.66. If the flow is turbulent (<i>Re &gt; 2300</i>),
- the correlation of Dittus-Boelter is used to find the convection heat transfer coefficient as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   Nu = 0.023 &nbsp; Re<sup>0.8</sup> &nbsp; Pr<sup>n</sup>,
- </p>
- <p>
- where <i>Nu</i> is the Nusselt number and 
- <i>Pr</i> is the Prandlt number.
- A value of <i>n=0.35</i> is used, as the reference uses <i>n=0.4</i> for heating and 
- <i>n=0.3</i> for cooling. To ensure that the function is continuously differentiable,
- a smooth transition between the laminar and turbulent values is created for the
- range <i>2300 &lt; Re &lt; 2400</i>.
- </p>
- <h4>References</h4>
- <p>
- Bergman, T. L., Incropera, F. P., DeWitt, D. P., &amp; Lavine, A. S. (2011). <i>Fundamentals of heat and mass
- transfer</i> (7th ed.). New York: John Wiley &amp; Sons.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 10, 2018, by Alex Laferri&egrave;re:<br/>
- Added laminar flow and smooth laminar-turbulent transition.
- Revised documentation.
- </li>
- <li>
- February 14, 2014, by Michael Wetter:<br/>
- Removed unused input <code>rBor</code>.
- Revised documentation.
- </li>
- <li>
- January 24, 2014, by Michael Wetter:<br/>
- Revised implementation. 
- Changed <code>cpFluid</code> to <code>cpMed</code> to use consistent notation.
- Added regularization for computation of convective heat transfer coefficient to
- avoid an event and a non-differentiability.
- </li>
- <li>
- January 23, 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  annotation (Documentation(info="<html>
+<p>
+This model computes the convection resistance in the pipes of a borehole segment
+with heigth <i>h<sub>Seg</sub></i> using correlations suggested by Bergman et al. (2011).
+</p>
+<p>
+If the flow is laminar (<i>Re &le; 2300</i>, with <i>Re</i> being the Reynolds number of the flow),
+the Nusselt number of the flow is assumed to be constant at 3.66. If the flow is turbulent (<i>Re &gt; 2300</i>),
+the correlation of Dittus-Boelter is used to find the convection heat transfer coefficient as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  Nu = 0.023 &nbsp; Re<sup>0.8</sup> &nbsp; Pr<sup>n</sup>,
+</p>
+<p>
+where <i>Nu</i> is the Nusselt number and
+<i>Pr</i> is the Prandlt number.
+A value of <i>n=0.35</i> is used, as the reference uses <i>n=0.4</i> for heating and
+<i>n=0.3</i> for cooling. To ensure that the function is continuously differentiable,
+a smooth transition between the laminar and turbulent values is created for the
+range <i>2300 &lt; Re &lt; 2400</i>.
+</p>
+<h4>References</h4>
+<p>
+Bergman, T. L., Incropera, F. P., DeWitt, D. P., &amp; Lavine, A. S. (2011). <i>Fundamentals of heat and mass
+transfer</i> (7th ed.). New York: John Wiley &amp; Sons.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 4, 2023, by Michael Wetter:<br/>
+Corrected variability.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1762\">IBPSA, #1762</a>.
+</li>
+<li>
+July 10, 2018, by Alex Laferri&egrave;re:<br/>
+Added laminar flow and smooth laminar-turbulent transition.
+Revised documentation.
+</li>
+<li>
+February 14, 2014, by Michael Wetter:<br/>
+Removed unused input <code>rBor</code>.
+Revised documentation.
+</li>
+<li>
+January 24, 2014, by Michael Wetter:<br/>
+Revised implementation.
+Changed <code>cpFluid</code> to <code>cpMed</code> to use consistent notation.
+Added regularization for computation of convective heat transfer coefficient to
+avoid an event and a non-differentiability.
+</li>
+<li>
+January 23, 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end convectionResistanceCircularPipe;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/internalResistancesOneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/internalResistancesOneUTube.mo
index 06382879a1..cb4876d3b1 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/internalResistancesOneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/internalResistancesOneUTube.mo
@@ -81,76 +81,83 @@ algorithm
       i := i + 1;
     end while;
   end if;
-  assert(test, "In " + getInstanceName() + ":\n" +
+  assert(test, "In " + instanceName + ":\n" +
   "Maximum number of iterations exceeded. Check the borehole geometry.
-   The tubes may be too close to the borehole wall.
-   Input to the function
-   AixLib.Fluid.HeatExchangers.Boreholes.BaseClasses.singleUTubeResistances
-   is
-            hSeg = "+ String(hSeg) + " m
-            rBor = "+ String(rBor) + " m
-            rTub = "+ String(rTub) + " m
-            eTub = "+ String(eTub) + " m
-            kSoi = "+ String(kSoi) + " W/m/K
-            kFil = "+ String(kFil) + " W/m/K
-            kTub = "+ String(kTub) + " W/m/K
-            i = " + String(i) + "
-   Computed x    = "+ String(x) + " K/W
-            Rgb  = "+ String(Rgb) + " K/W
-            Rgg  = "+ String(Rgg) + " K/W");
+  The tubes may be too close to the borehole wall.
+  Input to the function
+  AixLib.Fluid.HeatExchangers.Boreholes.BaseClasses.singleUTubeResistances
+  is
+           hSeg = " + String(hSeg) + " m
+           rBor = " + String(rBor) + " m
+           rTub = " + String(rTub) + " m
+           eTub = " + String(eTub) + " m
+           kSoi = " + String(kSoi) + " W/m/K
+           kFil = " + String(kFil) + " W/m/K
+           kTub = " + String(kTub) + " W/m/K
+           i = "  + String(i) + "
+  Computed x    = " + String(x) + " K/W
+           Rgb  = " + String(Rgb) + " K/W
+           Rgg  = " + String(Rgg) + " K/W");
 
 annotation (
   Documentation(info="<html>
- <p>
- This model computes the different thermal resistances present in a single-U-tube borehole
- using the method of Bauer et al. (2011).
- It also computes the fluid-to-ground thermal resistance <i>R<sub>b</sub></i>
- and the grout-to-grout thermal resistance <i>R<sub>a</sub></i>
- as defined by Claesson and Hellstrom (2011) using the multipole method.
- </p>
- 
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom.
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- <p>D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
- <i>Thermal resistance and capacity models for borehole heat exchangers</i>.
- International Journal of Energy Research, 35:312&ndash;320, 2011.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 7, 2022, by Michael Wetter:<br/>
- Changed function to be <code>pure</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
- </li>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- July 18, 2018 by Massimo Cimmino:<br/>
- Implemented multipole method.
- </li>
- <li>
- February 14, 2014 by Michael Wetter:<br/>
- Added an assert statement to test for non-physical values.
- </li>
- <li>
- February 12, 2014, by Damien Picard:<br/>
- Remove the flow dependency of the resistances, as this function calculates the conduction resistances only.
- </li>
- <li>
- January 24, 2014, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- January 23, 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model computes the different thermal resistances present in a single-U-tube borehole
+using the method of Bauer et al. (2011).
+It also computes the fluid-to-ground thermal resistance <i>R<sub>b</sub></i>
+and the grout-to-grout thermal resistance <i>R<sub>a</sub></i>
+as defined by Claesson and Hellstrom (2011) using the multipole method.
+</p>
+
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom.
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+<p>D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
+<i>Thermal resistance and capacity models for borehole heat exchangers</i>.
+International Journal of Energy Research, 35:312&ndash;320, 2011.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+February 7, 2022, by Michael Wetter:<br/>
+Changed function to be <code>pure</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
+</li>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+July 18, 2018 by Massimo Cimmino:<br/>
+Implemented multipole method.
+</li>
+<li>
+February 14, 2014 by Michael Wetter:<br/>
+Added an assert statement to test for non-physical values.
+</li>
+<li>
+February 12, 2014, by Damien Picard:<br/>
+Remove the flow dependency of the resistances, as this function calculates the conduction resistances only.
+</li>
+<li>
+January 24, 2014, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+January 23, 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end internalResistancesOneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/internalResistancesTwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/internalResistancesTwoUTube.mo
index 100f41eece..7c1216d73e 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/internalResistancesTwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/internalResistancesTwoUTube.mo
@@ -88,77 +88,84 @@ algorithm
       i := i + 1;
     end while;
   end if;
-  assert(test, "In " + getInstanceName() + ":\n" +
+  assert(test, "In " + instanceName + ":\n" +
   "Maximum number of iterations exceeded. Check the borehole geometry.
-   The tubes may be too close to the borehole wall.
-   Input to the function
-   AixLib.Fluid.HeatExchangers.Boreholes.BaseClasses.doubleUTubeResistances
-   is
-             hSeg = "+ String(hSeg) + " m
-             rBor = "+ String(rBor) + " m
-             rTub = "+ String(rTub) + " m
-             eTub = "+ String(eTub) + " m
-             sha = "+ String(sha) + " m
-             kSoi = "+ String(kSoi) + " W/m/K
-             kFil = "+ String(kFil) + " W/m/K
-             kTub = "+ String(kTub) + " W/m/K
-   Computed x    = "+ String(x) + " m
-             Rgb  = "+ String(Rgb) + " K/W
-             Rgg1  = "+ String(Rgg1) + " K/W
-             Rgg2  = "+ String(Rgg2) + " K/W");
+  The tubes may be too close to the borehole wall.
+  Input to the function
+  AixLib.Fluid.HeatExchangers.Boreholes.BaseClasses.doubleUTubeResistances
+  is
+            hSeg = " + String(hSeg) + " m
+            rBor = " + String(rBor) + " m
+            rTub = " + String(rTub) + " m
+            eTub = " + String(eTub) + " m
+            sha = " + String(sha) + " m
+            kSoi = " + String(kSoi) + " W/m/K
+            kFil = " + String(kFil) + " W/m/K
+            kTub = " + String(kTub) + " W/m/K
+  Computed x    = " + String(x) + " m
+            Rgb  = " + String(Rgb) + " K/W
+            Rgg1  = " + String(Rgg1) + " K/W
+            Rgg2  = " + String(Rgg2) + " K/W");
 
 annotation (
   Documentation(info="<html>
- <p>
- This model computes the different thermal resistances present in a double U-tube
- borehole using the method of Bauer et al. (2011).
- It also computes the fluid-to-ground thermal resistance <i>R<sub>b</sub></i>
- and the grout-to-grout thermal resistance <i>R<sub>a</sub></i>
- as defined by Claesson and Hellstrom (2011) using the multipole method.
- </p>
- 
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom.
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- <p>D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
- <i>Thermal resistance and capacity models for borehole heat exchangers</i>.
- International Journal of Energy Research, 35:312&ndash;320, 2011.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 7, 2022, by Michael Wetter:<br/>
- Changed function to be <code>pure</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
- </li>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- July 18, 2018 by Massimo Cimmino:<br/>
- Implemented multipole method.
- </li>
- <li>
- February 14, 2014 by Michael Wetter:<br/>
- Added an assert statement to test for non-physical values.
- </li>
- <li>
- February 12, 2014, by Damien Picard:<br/>
- Remove the flow dependency of the resistances, as this function calculates the conduction resistances only.
- </li>
- <li>
- January 24, 2014, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- January 23, 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model computes the different thermal resistances present in a double U-tube
+borehole using the method of Bauer et al. (2011).
+It also computes the fluid-to-ground thermal resistance <i>R<sub>b</sub></i>
+and the grout-to-grout thermal resistance <i>R<sub>a</sub></i>
+as defined by Claesson and Hellstrom (2011) using the multipole method.
+</p>
+
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom.
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+<p>D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
+<i>Thermal resistance and capacity models for borehole heat exchangers</i>.
+International Journal of Energy Research, 35:312&ndash;320, 2011.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+February 7, 2022, by Michael Wetter:<br/>
+Changed function to be <code>pure</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
+</li>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+July 18, 2018 by Massimo Cimmino:<br/>
+Implemented multipole method.
+</li>
+<li>
+February 14, 2014 by Michael Wetter:<br/>
+Added an assert statement to test for non-physical values.
+</li>
+<li>
+February 12, 2014, by Damien Picard:<br/>
+Remove the flow dependency of the resistances, as this function calculates the conduction resistances only.
+</li>
+<li>
+January 24, 2014, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+January 23, 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end internalResistancesTwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleFluidTemperature.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleFluidTemperature.mo
index d056b54d47..0232838c26 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleFluidTemperature.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleFluidTemperature.mo
@@ -144,21 +144,21 @@ algorithm
   end if;
 
   annotation (Documentation(info="<html>
- <p> This model evaluates the fluid temperatures using the multipole method of Claesson and Hellstrom (2011).
- </p>
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom. 
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. 
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 12, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p> This model evaluates the fluid temperatures using the multipole method of Claesson and Hellstrom (2011).
+</p>
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom. 
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. 
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 12, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end multipoleFluidTemperature;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleFmk.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleFmk.mo
index bbc0581b94..8d5e3fb115 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleFmk.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleFmk.mo
@@ -68,21 +68,21 @@ algorithm
   end for;
 
   annotation (Documentation(info="<html>
- <p>This model evaluates the complex coefficient matrix F_mk from Claesson and Hellstrom (2011).
- </p>
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom. 
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. 
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 12, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>This model evaluates the complex coefficient matrix F_mk from Claesson and Hellstrom (2011).
+</p>
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom. 
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. 
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 12, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end multipoleFmk;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleThermalResistances.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleThermalResistances.mo
index 0cd559d745..11b8ee300b 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleThermalResistances.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/multipoleThermalResistances.mo
@@ -67,21 +67,21 @@ algorithm
   end for;
 
   annotation (Documentation(info="<html>
- <p>This model evaluates the delta-circuit borehole thermal resistances using the multipole method of Claesson and Hellstrom (2011).
- </p>
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom. 
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. 
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 12, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>This model evaluates the delta-circuit borehole thermal resistances using the multipole method of Claesson and Hellstrom (2011).
+</p>
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom. 
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. 
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 12, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end multipoleThermalResistances;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/partialInternalResistances.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/partialInternalResistances.mo
index 9adc1296e0..078742bf2f 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/partialInternalResistances.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/Functions/partialInternalResistances.mo
@@ -29,6 +29,8 @@ partial function partialInternalResistances
   input Modelica.Units.SI.SpecificHeatCapacity cpMed
     "Specific heat capacity of the fluid";
   input Modelica.Units.SI.MassFlowRate m_flow_nominal "Nominal mass flow rate";
+  input String instanceName="undeclared caller"
+    "Instance name of the model or block that calls this function";
 
   // Outputs
   output Real x "Capacity location";
@@ -36,7 +38,7 @@ partial function partialInternalResistances
 protected
   parameter Real pi = 3.141592653589793 "pi";
 
-  parameter Real rTub_in = rTub-eTub "Inner radius of tube";
+  Real rTub_in = rTub-eTub "Inner radius of tube";
 
   Real RConv(unit="(m.K)/W")=
     AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.convectionResistanceCircularPipe(
@@ -64,39 +66,51 @@ protected
 
 annotation (
   Documentation(info="<html>
- <p>
- This partial function defines the common inputs to functions that calculate
- the borehole internal resistances.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 28, 2022, by Massimo Cimmino:<br/>
- Changed function to be <code>pure</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
- </li>
- <li>
- July 18, 2018 by Massimo Cimmino:<br/>
- Implemented multipole method.
- </li>
- <li>
- February 14, 2014 by Michael Wetter:<br/>
- Added an assert statement to test for non-physical values.
- </li>
- <li>
- February 12, 2014, by Damien Picard:<br/>
- Remove the flow dependency of the resistances, as this function calculates the conduction resistances only.
- </li>
- <li>
- January 24, 2014, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- January 23, 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This partial function defines the common inputs to functions that calculate
+the borehole internal resistances.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+June 4, 2023, by Michael Wetter:<br/>
+Corrected variability.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1762\">IBPSA, #1762</a>.
+</li>
+<li>
+February 28, 2022, by Massimo Cimmino:<br/>
+Changed function to be <code>pure</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
+</li>
+<li>
+July 18, 2018 by Massimo Cimmino:<br/>
+Implemented multipole method.
+</li>
+<li>
+February 14, 2014 by Michael Wetter:<br/>
+Added an assert statement to test for non-physical values.
+</li>
+<li>
+February 12, 2014, by Damien Picard:<br/>
+Remove the flow dependency of the resistances, as this function calculates the conduction resistances only.
+</li>
+<li>
+January 24, 2014, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+January 23, 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end partialInternalResistances;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalHEXOneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalHEXOneUTube.mo
index 59d5ba509c..b7bba24451 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalHEXOneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalHEXOneUTube.mo
@@ -56,7 +56,6 @@ public
 
   AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.InternalResistancesOneUTube
     intResUTub(
-      dynFil=dynFil,
       hSeg=hSeg,
       energyDynamics=energyDynamics,
       Rgb_val=Rgb_val,
@@ -92,12 +91,13 @@ initial equation
       kMed=kMed,
       muMed=muMed,
       cpMed=cpMed,
-      m_flow_nominal=m1_flow_nominal);
+      m_flow_nominal=m1_flow_nominal,
+      instanceName=getInstanceName());
 
 equation
     assert(borFieDat.conDat.borCon == AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.SingleUTube,
   "This model should be used for single U-type borefield, not double U-type.
-   Check that the conDat record has been correctly parametrized");
+  Check that the conDat record has been correctly parametrized");
   connect(RVol2.y, RConv2.Rc) annotation (Line(points={{-79,-8},{-60,-8},{-40,
           -8},{-40,-28},{-12,-28}},
                                 color={0,0,127}));
@@ -127,78 +127,91 @@ equation
           fillColor={0,0,255},
           fillPattern=FillPattern.Solid)}),
     Documentation(info="<html>
- <p>
- Model for the heat transfer between the fluid and within the borehole filling
- for a single borehole segment.
- This model computes the dynamic response of the fluid in the tubes,
- the heat transfer between the fluid and the borehole filling,
- and the heat storage within the fluid and the borehole filling.
- </p>
- <p>
- This model computes the different thermal resistances present
- in a single-U-tube borehole using the method of Bauer et al. (2011)
- and computing explicitely the fluid-to-ground thermal resistance
- <i>R<sub>b</sub></i> and the
- grout-to-grout resistance
- <i>R<sub>a</sub></i> as defined by Claesson and Hellstrom (2011)
- using the multipole method.
- </p>
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom.
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- <p>
- D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
- <i>
- Thermal resistance and capacity models for borehole heat exchangers
- </i>.
- International Journal Of Energy Research, 35:312-320, 2011.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- February 28, 2022, by Massimo Cimmino:<br/>
- Removed <code>printDebug</code> parameter from call to
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube</a>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
- </li>
- <li>
- July 10, 2018, by Alex Laferri&egrave;re:<br/>
- Updated documentation following major changes to the AixLib.Fluid.HeatExchangers.Ground package.
- Additionally, implemented a partial InternalHex model.
- </li>
- <li>
- June 18, 2014, by Michael Wetter:<br/>
- Added initialization for temperatures and derivatives of <code>capFil1</code>
- and <code>capFil2</code> to avoid a warning during translation.
- </li>
- <li>
- February 14, 2014, by Michael Wetter:<br/>
- Removed unused parameters <code>B0</code> and <code>B1</code>.
- </li>
- <li>
- January 24, 2014, by Michael Wetter:<br/>
- Revised implementation, added comments, replaced
- <code>HeatTransfer.Windows.BaseClasses.ThermalConductor</code>
- with resistance models from the Modelica Standard Library.
- </li>
- <li>
- January 23, 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model for the heat transfer between the fluid and within the borehole filling
+for a single borehole segment.
+This model computes the dynamic response of the fluid in the tubes,
+the heat transfer between the fluid and the borehole filling,
+and the heat storage within the fluid and the borehole filling.
+</p>
+<p>
+This model computes the different thermal resistances present
+in a single-U-tube borehole using the method of Bauer et al. (2011)
+and computing explicitely the fluid-to-ground thermal resistance
+<i>R<sub>b</sub></i> and the
+grout-to-grout resistance
+<i>R<sub>a</sub></i> as defined by Claesson and Hellstrom (2011)
+using the multipole method.
+</p>
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom.
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+<p>
+D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
+<i>
+Thermal resistance and capacity models for borehole heat exchangers
+</i>.
+International Journal Of Energy Research, 35:312-320, 2011.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+February 28, 2022, by Massimo Cimmino:<br/>
+Removed <code>printDebug</code> parameter from call to
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesOneUTube</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
+</li>
+<li>
+July 10, 2018, by Alex Laferri&egrave;re:<br/>
+Updated documentation following major changes to the AixLib.Fluid.HeatExchangers.Ground package.
+Additionally, implemented a partial InternalHex model.
+</li>
+<li>
+June 18, 2014, by Michael Wetter:<br/>
+Added initialization for temperatures and derivatives of <code>capFil1</code>
+and <code>capFil2</code> to avoid a warning during translation.
+</li>
+<li>
+February 14, 2014, by Michael Wetter:<br/>
+Removed unused parameters <code>B0</code> and <code>B1</code>.
+</li>
+<li>
+January 24, 2014, by Michael Wetter:<br/>
+Revised implementation, added comments, replaced
+<code>HeatTransfer.Windows.BaseClasses.ThermalConductor</code>
+with resistance models from the Modelica Standard Library.
+</li>
+<li>
+January 23, 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=false, initialScale=0.1),
-    graphics),
-  __Dymola_LockedEditing="Model from IBPSA");
+    graphics), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalHEXOneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalHEXTwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalHEXTwoUTube.mo
index 9c5a4ce83c..7c3ccc0973 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalHEXTwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalHEXTwoUTube.mo
@@ -104,7 +104,6 @@ model InternalHEXTwoUTube
     Rgg1_val=Rgg1_val,
     Rgg2_val=Rgg2_val,
     RCondGro_val=RCondGro_val,
-    dynFil=dynFil,
     energyDynamics=energyDynamics,
     T_start=TGro_start)
                    "Internal resistances for a double U-tube configuration"
@@ -153,13 +152,14 @@ initial equation
       kMed=kMed,
       muMed=muMed,
       cpMed=cpMed,
-      m_flow_nominal=m1_flow_nominal);
+      m_flow_nominal=m1_flow_nominal,
+      instanceName=getInstanceName());
 
 equation
   assert(borFieDat.conDat.borCon == AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.DoubleUTubeParallel
      or borFieDat.conDat.borCon == AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.DoubleUTubeSeries,
     "This model should be used for double U-type borefield, not single U-type.
-   Check that the conDat record has been correctly parametrized");
+  Check that the conDat record has been correctly parametrized");
   connect(RVol1.y, RConv1.Rc) annotation (Line(
       points={{-30.7,64},{-34,64},{-34,46},{-8,46}},
       color={0,0,127},
@@ -222,77 +222,90 @@ equation
           fillColor={0,0,255},
           fillPattern=FillPattern.Solid)}),
     Documentation(info="<html>
- <p>
- Model for the heat transfer between the fluid and within the borehole filling.
- This model computes the dynamic response of the fluid in the tubes,
- the heat transfer between the fluid and the borehole filling,
- and the heat storage within the fluid and the borehole filling.
- </p>
- <p>
- This model computes the different thermal resistances present
- in a single-U-tube borehole using the method of Bauer et al. (2011)
- and computing explicitely the fluid-to-ground thermal resistance
- <i>R<sub>b</sub></i> and the
- grout-to-grout resistance
- <i>R<sub>a</sub></i> as defined by Claesson and Hellstrom (2011)
- using the multipole method.
- </p>
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom.
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- <p>
- D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
- <i>
- Thermal resistance and capacity models for borehole heat exchangers
- </i>.
- International Journal Of Energy Research, 35:312-320, 2011.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- February 28, 2022, by Massimo Cimmino:<br/>
- Removed <code>printDebug</code> parameter from call to
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube</a>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
- </li>
- <li>
- July 10, 2018, by Alex Laferri&egrave;re:<br/>
- Updated documentation following major changes to the AixLib.Fluid.HeatExchangers.Ground package.
- Additionally, implemented a partial InternalHex model.
- </li>
- <li>
- June 18, 2014, by Michael Wetter:<br/>
- Added initialization for temperatures and derivatives of <code>capFil1</code>
- and <code>capFil2</code> to avoid a warning during translation.
- </li>
- <li>
- February 14, 2014, by Michael Wetter:<br/>
- Removed unused parameters <code>B0</code> and <code>B1</code>.
- </li>
- <li>
- January 24, 2014, by Michael Wetter:<br/>
- Revised implementation, added comments, replaced
- <code>HeatTransfer.Windows.BaseClasses.ThermalConductor</code>
- with resistance models from the Modelica Standard Library.
- </li>
- <li>
- January 23, 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model for the heat transfer between the fluid and within the borehole filling.
+This model computes the dynamic response of the fluid in the tubes,
+the heat transfer between the fluid and the borehole filling,
+and the heat storage within the fluid and the borehole filling.
+</p>
+<p>
+This model computes the different thermal resistances present
+in a single-U-tube borehole using the method of Bauer et al. (2011)
+and computing explicitely the fluid-to-ground thermal resistance
+<i>R<sub>b</sub></i> and the
+grout-to-grout resistance
+<i>R<sub>a</sub></i> as defined by Claesson and Hellstrom (2011)
+using the multipole method.
+</p>
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom.
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+<p>
+D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
+<i>
+Thermal resistance and capacity models for borehole heat exchangers
+</i>.
+International Journal Of Energy Research, 35:312-320, 2011.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+November 22, 2023, by Michael Wetter:<br/>
+Corrected use of <code>getInstanceName()</code> which was called inside a function which
+is not allowed.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1814\">IBPSA, #1814</a>.
+</li>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+February 28, 2022, by Massimo Cimmino:<br/>
+Removed <code>printDebug</code> parameter from call to
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.BaseClasses.Functions.internalResistancesTwoUTube</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1582\">IBPSA, #1582</a>.
+</li>
+<li>
+July 10, 2018, by Alex Laferri&egrave;re:<br/>
+Updated documentation following major changes to the AixLib.Fluid.HeatExchangers.Ground package.
+Additionally, implemented a partial InternalHex model.
+</li>
+<li>
+June 18, 2014, by Michael Wetter:<br/>
+Added initialization for temperatures and derivatives of <code>capFil1</code>
+and <code>capFil2</code> to avoid a warning during translation.
+</li>
+<li>
+February 14, 2014, by Michael Wetter:<br/>
+Removed unused parameters <code>B0</code> and <code>B1</code>.
+</li>
+<li>
+January 24, 2014, by Michael Wetter:<br/>
+Revised implementation, added comments, replaced
+<code>HeatTransfer.Windows.BaseClasses.ThermalConductor</code>
+with resistance models from the Modelica Standard Library.
+</li>
+<li>
+January 23, 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
-            100}}), graphics),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100}}), graphics), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalHEXTwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalResistancesOneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalResistancesOneUTube.mo
index b570003f0a..b817787cfe 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalResistancesOneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalResistancesOneUTube.mo
@@ -25,7 +25,7 @@ model InternalResistancesOneUTube
     C=Co_fil/2,
     T(start=T_start, fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial)),
     der_T(fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyStateInitial)))
-    if dynFil
+    if not borFieDat.filDat.steadyState
     "Heat capacity of the filling material" annotation (Placement(
         transformation(
         extent={{-10,-10},{10,10}},
@@ -35,7 +35,7 @@ model InternalResistancesOneUTube
     C=Co_fil/2,
     T(start=T_start, fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial)),
     der_T(fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyStateInitial)))
-    if dynFil
+    if not borFieDat.filDat.steadyState
     "Heat capacity of the filling material" annotation (Placement(
         transformation(
         extent={{-10,10},{10,-10}},
@@ -81,40 +81,46 @@ equation
 
     annotation (
     Documentation(info="<html>
- <p>
- This model simulates the internal thermal resistance network of a borehole segment in
- the case of a single U-tube borehole using the method of Bauer et al. (2011) 
- and computing explicitely the fluid-to-ground thermal resistance 
- <i>R<sub>b</sub></i> and the 
- grout-to-grout resistance
- <i>R<sub>a</sub></i> as defined by Claesson and Hellstrom (2011)
- using the multipole method. 
- </p>
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom. 
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. 
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- <p>
- D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
- <i>
- Thermal resistance and capacity models for borehole heat exchangers
- </i>.
- International Journal Of Energy Research, 35:312-320, 2011.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 5, 2018, by Alex Laferri&egrave;re:<br/>
- Extended the model from a partial class.
- </li>
- <li>
- June, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<p>
+This model simulates the internal thermal resistance network of a borehole segment in
+the case of a single U-tube borehole using the method of Bauer et al. (2011)
+and computing explicitely the fluid-to-ground thermal resistance
+<i>R<sub>b</sub></i> and the
+grout-to-grout resistance
+<i>R<sub>a</sub></i> as defined by Claesson and Hellstrom (2011)
+using the multipole method.
+</p>
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom.
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+<p>
+D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
+<i>
+Thermal resistance and capacity models for borehole heat exchangers
+</i>.
+International Journal Of Energy Research, 35:312-320, 2011.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+July 5, 2018, by Alex Laferri&egrave;re:<br/>
+Extended the model from a partial class.
+</li>
+<li>
+June, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Line(
           points={{-2,100}},
           color={0,0,0},
@@ -123,6 +129,6 @@ equation
           textColor={0,0,255},
           fillPattern=FillPattern.HorizontalCylinder,
           fillColor={0,127,255},
-          textString="%name")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="%name")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalResistancesOneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalResistancesTwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalResistancesTwoUTube.mo
index 2b1695b91f..6e4a4c7cea 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalResistancesTwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/InternalResistancesTwoUTube.mo
@@ -8,9 +8,10 @@ model InternalResistancesTwoUTube
     "Thermal resistance between two neightbouring grout capacities, as defined by Bauer et al (2010)";
   parameter Modelica.Units.SI.ThermalResistance Rgg2_val
     "Thermal resistance between two  grout capacities opposite to each other, as defined by Bauer et al (2010)";
-  parameter Modelica.Units.SI.HeatCapacity Co_fil=borFieDat.filDat.dFil*
-      borFieDat.filDat.cFil*hSeg*Modelica.Constants.pi*(borFieDat.conDat.rBor^2
-       - 4*borFieDat.conDat.rTub^2)
+  parameter Modelica.Units.SI.HeatCapacity Co_fil=
+     if borFieDat.filDat.steadyState then 0
+     else borFieDat.filDat.dFil*borFieDat.filDat.cFil*hSeg*Modelica.Constants.pi*
+          (borFieDat.conDat.rBor^2 - 4*borFieDat.conDat.rTub^2)
     "Heat capacity of the whole filling material";
 
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a port_3
@@ -92,7 +93,7 @@ model InternalResistancesTwoUTube
   Modelica.Thermal.HeatTransfer.Components.HeatCapacitor capFil1(T(start=
           T_start, fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial)),
       der_T(fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyStateInitial)),
-    C=Co_fil/4)  if dynFil "Heat capacity of the filling material"
+    C=Co_fil/4)  if not borFieDat.filDat.steadyState "Heat capacity of the filling material"
                                             annotation (Placement(transformation(extent={{-8,-8},
             {8,8}},
         rotation=90,
@@ -100,13 +101,13 @@ model InternalResistancesTwoUTube
   Modelica.Thermal.HeatTransfer.Components.HeatCapacitor capFil2(T(start=
           T_start, fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial)),
       der_T(fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyStateInitial)),
-    C=Co_fil/4)  if dynFil "Heat capacity of the filling material"
+    C=Co_fil/4)  if not borFieDat.filDat.steadyState "Heat capacity of the filling material"
                                             annotation (Placement(transformation(extent={{58,8},{
             74,24}})));
   Modelica.Thermal.HeatTransfer.Components.HeatCapacitor capFil3(T(start=
           T_start, fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial)),
       der_T(fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyStateInitial)),
-    C=Co_fil/4)  if dynFil "Heat capacity of the filling material"
+    C=Co_fil/4)  if not borFieDat.filDat.steadyState "Heat capacity of the filling material"
                                             annotation (Placement(transformation(extent={{-8,-8},
             {8,8}},
         rotation=90,
@@ -114,7 +115,7 @@ model InternalResistancesTwoUTube
   Modelica.Thermal.HeatTransfer.Components.HeatCapacitor capFil4(T(start=
           T_start, fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial)),
       der_T(fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyStateInitial)),
-    C=Co_fil/4)  if dynFil "Heat capacity of the filling material"
+    C=Co_fil/4)  if not borFieDat.filDat.steadyState "Heat capacity of the filling material"
                                             annotation (Placement(transformation(extent={{-82,20},
             {-66,36}})));
 equation
@@ -218,39 +219,45 @@ equation
           textString="%name")}),                                 Diagram(
         coordinateSystem(preserveAspectRatio=false)),
         Documentation(info="<html>
- <p>
- This model simulates the internal thermal resistance network of a borehole segment in
- the case of a double U-tube borehole using the method of Bauer et al. (2011) 
- and computing explicitely the fluid-to-ground thermal resistance 
- <i>R<sub>b</sub></i> and the 
- grout-to-grout resistance
- <i>R<sub>a</sub></i> as defined by Claesson and Hellstrom (2011)
- using the multipole method. 
- </p>
- <h4>References</h4>
- <p>J. Claesson and G. Hellstrom. 
- <i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger. 
- </i>
- HVAC&amp;R Research,
- 17(6): 895-911, 2011.</p>
- <p>
- D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
- <i>
- Thermal resistance and capacity models for borehole heat exchangers
- </i>.
- International Journal Of Energy Research, 35:312-320, 2011.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 5, 2018, by Alex Laferri&egrave;re:<br/>
- Extended the model from a partial class.
- </li>
- <li>
- June, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model simulates the internal thermal resistance network of a borehole segment in
+the case of a double U-tube borehole using the method of Bauer et al. (2011)
+and computing explicitely the fluid-to-ground thermal resistance
+<i>R<sub>b</sub></i> and the
+grout-to-grout resistance
+<i>R<sub>a</sub></i> as defined by Claesson and Hellstrom (2011)
+using the multipole method.
+</p>
+<h4>References</h4>
+<p>J. Claesson and G. Hellstrom.
+<i>Multipole method to calculate borehole thermal resistances in a borehole heat exchanger.
+</i>
+HVAC&amp;R Research,
+17(6): 895-911, 2011.</p>
+<p>
+D. Bauer, W. Heidemann, H. M&uuml;ller-Steinhagen, and H.-J. G. Diersch.
+<i>
+Thermal resistance and capacity models for borehole heat exchangers
+</i>.
+International Journal Of Energy Research, 35:312-320, 2011.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+July 5, 2018, by Alex Laferri&egrave;re:<br/>
+Extended the model from a partial class.
+</li>
+<li>
+June, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InternalResistancesTwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialBorehole.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialBorehole.mo
index eec84d53c1..33b3d01229 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialBorehole.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialBorehole.mo
@@ -37,9 +37,6 @@ partial model PartialBorehole
     "Start value of pressure"
     annotation(Dialog(tab = "Initialization"));
 
-  parameter Boolean dynFil=true
-      "Set to false to remove the dynamics of the filling material"
-      annotation (Dialog(tab="Dynamics"));
   parameter Data.Borefield.Template borFieDat "Borefield parameters"
     annotation (Placement(transformation(extent={{-80,-80},{-60,-60}})));
 
@@ -48,26 +45,32 @@ partial model PartialBorehole
     annotation (Placement(transformation(extent={{-10,90},{10,110}})));
 
     annotation(Documentation(info="<html>
- <p>
- Partial model to implement models simulating geothermal U-tube boreholes modeled
- as several borehole segments, with a uniform borehole wall boundary condition.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to water and glycolWater.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- July 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation of partial model.
- </li>
- <li>
- July 2014, by Damien Picard:<br/>
- First implementation.
- </ul>
- </html>"),
+<p>
+Partial model to implement models simulating geothermal U-tube boreholes modeled
+as several borehole segments, with a uniform borehole wall boundary condition.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to water and glycolWater.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+July 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation of partial model.
+</li>
+<li>
+July 2014, by Damien Picard:<br/>
+First implementation.
+</ul>
+</html>"),
 Icon(coordinateSystem(
         preserveAspectRatio=true,
         extent={{-100,-100},{100,100}},
@@ -106,6 +109,6 @@ Icon(coordinateSystem(
           extent={{64,76},{74,-84}},
           lineColor={0,0,0},
           fillColor={192,192,192},
-          fillPattern=FillPattern.Backward)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Backward)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialBorehole;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialInternalHEX.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialInternalHEX.mo
index 5aa9c01e29..35ef3475e5 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialInternalHEX.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialInternalHEX.mo
@@ -15,9 +15,7 @@ partial model PartialInternalHEX
               "Propylene glycol water, 40% mass fraction")));
   constant Real mSenFac=1
     "Factor for scaling the sensible thermal mass of the volume";
-  parameter Boolean dynFil=true
-    "Set to false to remove the dynamics of the filling material"
-    annotation (Dialog(tab="Dynamics"));
+
   parameter Modelica.Units.SI.Length hSeg
     "Length of the internal heat exchanger";
   parameter Modelica.Units.SI.Volume VTubSeg=hSeg*Modelica.Constants.pi*(
@@ -55,8 +53,8 @@ initial equation
   assert(borFieDat.conDat.rBor > borFieDat.conDat.xC + borFieDat.conDat.rTub and
          0 < borFieDat.conDat.xC - borFieDat.conDat.rTub,
          "The borehole geometry is not physical. Check the borefield data record
-          to ensure that the shank spacing is larger than the outer tube radius
-          and that the borehole radius is sufficiently large.");
+         to ensure that the shank spacing is larger than the outer tube radius
+         and that the borehole radius is sufficiently large.");
   annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
         Rectangle(
           extent={{-70,80},{70,-80}},
@@ -66,58 +64,64 @@ initial equation
           fillPattern=FillPattern.Solid)}),                      Diagram(
         coordinateSystem(preserveAspectRatio=false)),
   Documentation(info="<html>
- <p>
- Partial model to implement models simulating the thermal and fluid behaviour of a borehole segment.
- </p>
- <p>
- The thermodynamic properties of the fluid circulating in the borehole are calculated
- as protected parameters in this partial model: <i>c<sub>p</sub></i> (<code>cpMed</code>),
- <i>k</i> (<code>kMed</code>) and <i>&mu;</i> (<code>muMed</code>). Additionally, the
- following parameters are already declared as protected parameters and thus do not
- need to be declared in models which extend this partial model:
- </p>
- <ul>
- <li>
- <code>Rgb_val</code> (Thermal resistance between grout zone and borehole wall)
- </li>
- <li>
- <code>RCondGro_val</code> (Thermal resistance between pipe wall and capacity in grout)
- </li>
- <li>
- <code>x</code> (Grout capacity location)
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to water and glycolWater.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- July 10, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation of partial model.
- </li>
- <li>
- June 18, 2014, by Michael Wetter:<br/>
- Added initialization for temperatures and derivatives of <code>capFil1</code>
- and <code>capFil2</code> to avoid a warning during translation.
- </li>
- <li>
- February 14, 2014, by Michael Wetter:<br/>
- Removed unused parameters <code>B0</code> and <code>B1</code>.
- </li>
- <li>
- January 24, 2014, by Michael Wetter:<br/>
- Revised implementation, added comments, replaced
- <code>HeatTransfer.Windows.BaseClasses.ThermalConductor</code>
- with resistance models from the Modelica Standard Library.
- </li>
- <li>
- January 23, 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model to implement models simulating the thermal and fluid behaviour of a borehole segment.
+</p>
+<p>
+The thermodynamic properties of the fluid circulating in the borehole are calculated
+as protected parameters in this partial model: <i>c<sub>p</sub></i> (<code>cpMed</code>),
+<i>k</i> (<code>kMed</code>) and <i>&mu;</i> (<code>muMed</code>). Additionally, the
+following parameters are already declared as protected parameters and thus do not
+need to be declared in models which extend this partial model:
+</p>
+<ul>
+<li>
+<code>Rgb_val</code> (Thermal resistance between grout zone and borehole wall)
+</li>
+<li>
+<code>RCondGro_val</code> (Thermal resistance between pipe wall and capacity in grout)
+</li>
+<li>
+<code>x</code> (Grout capacity location)
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to water and glycolWater.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+July 10, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation of partial model.
+</li>
+<li>
+June 18, 2014, by Michael Wetter:<br/>
+Added initialization for temperatures and derivatives of <code>capFil1</code>
+and <code>capFil2</code> to avoid a warning during translation.
+</li>
+<li>
+February 14, 2014, by Michael Wetter:<br/>
+Removed unused parameters <code>B0</code> and <code>B1</code>.
+</li>
+<li>
+January 24, 2014, by Michael Wetter:<br/>
+Revised implementation, added comments, replaced
+<code>HeatTransfer.Windows.BaseClasses.ThermalConductor</code>
+with resistance models from the Modelica Standard Library.
+</li>
+<li>
+January 23, 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialInternalHEX;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialInternalResistances.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialInternalResistances.mo
index f9660da905..6b09a7f58f 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialInternalResistances.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/BaseClasses/PartialInternalResistances.mo
@@ -14,9 +14,6 @@ partial model PartialInternalResistances
   parameter Modelica.Fluid.Types.Dynamics energyDynamics=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial
     "Type of energy balance: dynamic (3 initialization options) or steady state"
     annotation(Evaluate=true, Dialog(tab = "Dynamics", group="Conservation equations"));
-  parameter Boolean dynFil=true
-      "Set to false to remove the dynamics of the filling material."
-      annotation (Dialog(tab="Dynamics"));
 
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a port_1
     "Thermal connection for pipe 1"
@@ -27,6 +24,7 @@ partial model PartialInternalResistances
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a port_2
     "Thermal connection for borehole wall"
     annotation (Placement(transformation(extent={{90,-10},{110,10}})));
+
   annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
         Rectangle(
           extent={{-100,100},{100,-100}},
@@ -53,25 +51,31 @@ partial model PartialInternalResistances
           thickness=0.5)}),                                      Diagram(
         coordinateSystem(preserveAspectRatio=false)),
         Documentation(info="<html>
- <p>
- Partial model to implement the inner resistance network of a borehole segment.
- </p>
- <p>
- The partial model uses a thermal port representing a uniform borehole wall for
- that segment, and at least two other thermal ports (one for each tube going through the borehole
- segment).
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation of partial class.
- </li>
- <li>
- June, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model to implement the inner resistance network of a borehole segment.
+</p>
+<p>
+The partial model uses a thermal port representing a uniform borehole wall for
+that segment, and at least two other thermal ports (one for each tube going through the borehole
+segment).
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+July 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation of partial class.
+</li>
+<li>
+June, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialInternalResistances;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BaseClasses/PartialBorehole.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BaseClasses/PartialBorehole.mo
index eebb05be42..50050676ec 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BaseClasses/PartialBorehole.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BaseClasses/PartialBorehole.mo
@@ -70,18 +70,18 @@ equation
   connect(borHol.port_wall, preTem.port) annotation (Line(points={{1.77636e-15,14},
           {0,14},{0,70},{-40,70}}, color={191,0,0}));
   annotation(Documentation(info="<html>
- <p>
- This partial model is used for examples using boreholes models which extend
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.Examples.BaseClasses.PartialBorehole\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.Examples.BaseClasses.PartialBorehole</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 9, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This partial model is used for examples using boreholes models which extend
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.Examples.BaseClasses.PartialBorehole\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.Examples.BaseClasses.PartialBorehole</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 9, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialBorehole;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeDynamics.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeDynamics.mo
index 1950b6d7db..8a0f054c79 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeDynamics.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeDynamics.mo
@@ -14,7 +14,6 @@ model BoreholeDynamics "Example model for different borehole models and dynamics
     borFieDat=borFieUTubDat,
     m_flow_nominal=borFieUTubDat.conDat.mBor_flow_nominal,
     dp_nominal=borFieUTubDat.conDat.dp_nominal,
-    dynFil=true,
     nSeg=nSeg,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     TGro_start = {T_start for i in 1:nSeg},
@@ -43,7 +42,7 @@ model BoreholeDynamics "Example model for different borehole models and dynamics
   parameter
     AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Example
     borFieUTubDat "Borefield parameters with UTube borehole configuration"
-    annotation (Placement(transformation(extent={{80,20},{100,40}})));
+    annotation (Placement(transformation(extent={{90,40},{110,60}})));
   AixLib.Fluid.Sensors.TemperatureTwoPort TBorIn(m_flow_nominal=borFieUTubDat.conDat.mBor_flow_nominal,
     redeclare package Medium = Medium,
     tau=0)
@@ -68,10 +67,9 @@ model BoreholeDynamics "Example model for different borehole models and dynamics
         origin={-98,90})));
   AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.OneUTube borHolOneUTubSteSta(
     redeclare package Medium = Medium,
-    borFieDat=borFieUTubDat,
-    m_flow_nominal=borFieUTubDat.conDat.mBor_flow_nominal,
-    dp_nominal=borFieUTubDat.conDat.dp_nominal,
-    dynFil=false,
+    borFieDat=borFieUTubDatSteSta,
+    m_flow_nominal=borFieUTubDatSteSta.conDat.mBor_flow_nominal,
+    dp_nominal=borFieUTubDatSteSta.conDat.dp_nominal,
     nSeg=nSeg,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     TGro_start = {T_start for i in 1:nSeg},
@@ -117,7 +115,6 @@ model BoreholeDynamics "Example model for different borehole models and dynamics
   AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.TwoUTube borHol2UTubDyn(
     redeclare package Medium = Medium,
     dp_nominal=borFie2UTubDat.conDat.dp_nominal,
-    dynFil=true,
     m_flow_nominal=borFie2UTubDat.conDat.mBor_flow_nominal,
     borFieDat=borFie2UTubDat,
     nSeg=nSeg,
@@ -145,13 +142,11 @@ model BoreholeDynamics "Example model for different borehole models and dynamics
     p=101330,
     T=283.15) "Sink" annotation (Placement(transformation(extent={{80,-70},{60,-50}},
                   rotation=0)));
-  parameter
-    AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Example
-    borFie2UTubDat(conDat=
-        AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Example(
-         borCon=AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.DoubleUTubeParallel))
+  parameter AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Example borFie2UTubDat(
+    conDat=AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Example(
+      borCon=AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.DoubleUTubeParallel))
     "Borefield parameters with UTube borehole configuration"
-    annotation (Placement(transformation(extent={{80,-100},{100,-80}})));
+    annotation (Placement(transformation(extent={{90,-80},{110,-60}})));
   AixLib.Fluid.Sensors.TemperatureTwoPort TBorIn2(redeclare package Medium =
         Medium, m_flow_nominal=borFie2UTubDat.conDat.mBor_flow_nominal,
     tau=0)
@@ -171,10 +166,9 @@ model BoreholeDynamics "Example model for different borehole models and dynamics
 
   AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.TwoUTube borHol2UTubSteSta(
     redeclare package Medium = Medium,
-    dp_nominal=borFie2UTubDat.conDat.dp_nominal,
-    dynFil=false,
-    m_flow_nominal=borFie2UTubDat.conDat.mBor_flow_nominal,
-    borFieDat=borFie2UTubDat,
+    dp_nominal=borFie2UTubDatSteSta.conDat.dp_nominal,
+    m_flow_nominal=borFie2UTubDatSteSta.conDat.mBor_flow_nominal,
+    borFieDat=borFie2UTubDatSteSta,
     nSeg=nSeg,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     TGro_start = {T_start for i in 1:nSeg},
@@ -230,6 +224,18 @@ model BoreholeDynamics "Example model for different borehole models and dynamics
   Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature
     prescribedTemperature3
     annotation (Placement(transformation(extent={{-70,-100},{-50,-80}})));
+  parameter AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Example borFieUTubDatSteSta(filDat=
+        AixLib.Fluid.Geothermal.Borefields.Data.Filling.Bentonite(
+        steadyState=true))
+    "Borefield parameters with UTube borehole configuration and steady-state filling"
+    annotation (Placement(transformation(extent={{90,0},{110,20}})));
+  parameter AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Example borFie2UTubDatSteSta(
+    filDat=AixLib.Fluid.Geothermal.Borefields.Data.Filling.Bentonite(
+        steadyState=true),
+    conDat=AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Example(
+        borCon=AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.DoubleUTubeParallel))
+    "Borefield parameters with UTube borehole configuration and steady-state filling"
+    annotation (Placement(transformation(extent={{90,-120},{110,-100}})));
 equation
   connect(sou.ports[1],TBorIn. port_a)
     annotation (Line(points={{-48,60},{-40,60}},
@@ -294,21 +300,27 @@ equation
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeDynamics.mos"
         "Simulate and Plot"),
         Documentation(info="<html>
- <p>
- This example illustrates different borehole models using different mass
- and energy dynamics.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 10, 2018, by Alex Laferri&egrave;re:<br/>
- Removed ground heat transfer models so the example focuses on the boreholes.
- </li>
- <li>
- February, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example illustrates different borehole models using different mass
+and energy dynamics.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+July 10, 2018, by Alex Laferri&egrave;re:<br/>
+Removed ground heat transfer models so the example focuses on the boreholes.
+</li>
+<li>
+February, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BoreholeDynamics;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeOneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeOneUTube.mo
index 71c5f4d948..a1378e4c20 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeOneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeOneUTube.mo
@@ -14,26 +14,26 @@ model BoreholeOneUTube "Test for the single U-tube borehole model"
     Diagram(coordinateSystem(preserveAspectRatio=false,extent={{-100,-100},{100,
             100}})),
     Documentation(info="<html>
- <p>
- This example illustrates the use of the
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.OneUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.OneUTubes</a>
- model. It simulates the behavior of a borehole with a prescribed
- borehole wall temperature boundary condition.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 10, 2018, by Alex Laferri&egrave;re:<br/>
- Adjusted the example following major changes to the AixLib.Fluid.HeatExchangers.Ground package.
- Additionally, implemented a partial example model.
- </li>
- <li>
- August 30, 2011, by Pierre Vigouroux:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    experiment(Tolerance=1e-6, StopTime=360000),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example illustrates the use of the
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.OneUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.OneUTubes</a>
+model. It simulates the behavior of a borehole with a prescribed
+borehole wall temperature boundary condition.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 10, 2018, by Alex Laferri&egrave;re:<br/>
+Adjusted the example following major changes to the AixLib.Fluid.HeatExchangers.Ground package.
+Additionally, implemented a partial example model.
+</li>
+<li>
+August 30, 2011, by Pierre Vigouroux:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=360000), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BoreholeOneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeTwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeTwoUTube.mo
index 2c7ae07d0a..fcd6b798e6 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeTwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeTwoUTube.mo
@@ -12,25 +12,25 @@ model BoreholeTwoUTube "Test for the double U-tube borehole model"
         __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/Examples/BoreholeTwoUTube.mos"
         "Simulate and Plot"),
         Documentation(info="<html>
- <p>
- This example illustrates the use of the
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.TwoUTube\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.TwoUTube</a>
- model. It simulates the behavior of a borehole with a prescribed
- borehole wall boundary condition.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 10, 2018, by Alex Laferri&egrave;re:<br/>
- Adjusted the example following major changes to the AixLib.Fluid.HeatExchangers.Ground package.
- Additionally, implemented a partial example model.
- </li>
- <li>
- August 30, 2011, by Pierre Vigouroux:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example illustrates the use of the
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.TwoUTube\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.TwoUTube</a>
+model. It simulates the behavior of a borehole with a prescribed
+borehole wall boundary condition.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 10, 2018, by Alex Laferri&egrave;re:<br/>
+Adjusted the example following major changes to the AixLib.Fluid.HeatExchangers.Ground package.
+Additionally, implemented a partial example model.
+</li>
+<li>
+August 30, 2011, by Pierre Vigouroux:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BoreholeTwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/OneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/OneUTube.mo
index 137b378393..d0c8e4c04c 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/OneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/OneUTube.mo
@@ -13,7 +13,6 @@ model OneUTube "Single U-tube borehole heat exchanger"
     each final deltaM1=deltaM,
     each final deltaM2=deltaM,
     each final energyDynamics=energyDynamics,
-    each final dynFil=dynFil,
     each final mSenFac=mSenFac,
     final dp1_nominal={if i == 1 then dp_nominal else 0 for i in 1:nSeg},
     each final dp2_nominal=0,
@@ -90,35 +89,41 @@ equation
           textColor={0,0,255},
           textString="")}),
     Documentation(info="<html>
- <p>
- Model of a single U-tube borehole heat exchanger. 
- The borehole heat exchanger is vertically discretized into
- <i>n<sub>seg</sub></i> elements of height
- <i>h=h<sub>Bor</sub>&frasl;n<sub>seg</sub></i>.
- Each segment contains a model for the heat transfer in the borehole, 
- with a uniform borehole wall boundary temperature given by the
- <code>port_wall</code> port.
- </p>
- <p>
- The heat transfer in the borehole is computed using a convective heat transfer
- coefficient that depends on the fluid velocity, a heat resistance between the
- two pipes, and a heat resistance between the pipes and the borehole wall.
- The heat capacity of the fluid and the heat capacity of the grout are taken
- into account. The vertical heat flow is assumed to be zero.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 2018, by Alex Laferri&egrave;re:<br/>
- Following major changes to the structure of the AixLib.Fluid.HeatExchangers.Ground package,
- the documentation has been changed to reflect the new role of this model.
- Additionally, this model now extends a partial borehole model.
- </li>
- <li>
- July 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model of a single U-tube borehole heat exchanger.
+The borehole heat exchanger is vertically discretized into
+<i>n<sub>seg</sub></i> elements of height
+<i>h=h<sub>Bor</sub>&frasl;n<sub>seg</sub></i>.
+Each segment contains a model for the heat transfer in the borehole,
+with a uniform borehole wall boundary temperature given by the
+<code>port_wall</code> port.
+</p>
+<p>
+The heat transfer in the borehole is computed using a convective heat transfer
+coefficient that depends on the fluid velocity, a heat resistance between the
+two pipes, and a heat resistance between the pipes and the borehole wall.
+The heat capacity of the fluid and the heat capacity of the grout are taken
+into account. The vertical heat flow is assumed to be zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+July 2018, by Alex Laferri&egrave;re:<br/>
+Following major changes to the structure of the AixLib.Fluid.HeatExchangers.Ground package,
+the documentation has been changed to reflect the new role of this model.
+Additionally, this model now extends a partial borehole model.
+</li>
+<li>
+July 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/TwoUTube.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/TwoUTube.mo
index 230df77905..d6b36674e8 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/TwoUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/Boreholes/TwoUTube.mo
@@ -33,7 +33,6 @@ model TwoUTube "Double U-tube borehole heat exchanger"
          then borFieDat.conDat.mBor_flow_small/2 else borFieDat.conDat.mBor_flow_small,
     each final m4_flow_small=if borFieDat.conDat.borCon == AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.DoubleUTubeParallel
          then borFieDat.conDat.mBor_flow_small/2 else borFieDat.conDat.mBor_flow_small,
-    each final dynFil=dynFil,
     each final mSenFac=mSenFac,
     each final allowFlowReversal1=allowFlowReversal,
     each final allowFlowReversal2=allowFlowReversal,
@@ -173,35 +172,41 @@ equation
           textColor={0,0,255},
           textString="")}),
     Documentation(info="<html>
- <p>
- Model of a double U-tube borehole heat exchanger. 
- The borehole heat exchanger is vertically discretized into
- <i>n<sub>seg</sub></i> elements of height
- <i>h=h<sub>Bor</sub>&frasl;n<sub>seg</sub></i>.
- Each segment contains a model for the heat transfer in the borehole, 
- with a uniform borehole wall boundary temperature given by the
- <code>port_wall</code> port.
- </p>
- <p>
- The heat transfer in the borehole is computed using a convective heat transfer
- coefficient that depends on the fluid velocity, a heat resistance between each
- pair of pipes, and a heat resistance between the pipes and the borehole wall.
- The heat capacity of the fluid and the heat capacity of the grout are taken
- into account. The vertical heat flow is assumed to be zero. 
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 2018, by Alex Laferri&egrave;re:<br/>
- Following major changes to the structure of the AixLib.Fluid.HeatExchangers.Ground package,
- the documentation has been changed to reflect the new role of this model.
- Additionally, this model now extends a partial borehole model.
- </li>
- <li>
- July 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model of a double U-tube borehole heat exchanger.
+The borehole heat exchanger is vertically discretized into
+<i>n<sub>seg</sub></i> elements of height
+<i>h=h<sub>Bor</sub>&frasl;n<sub>seg</sub></i>.
+Each segment contains a model for the heat transfer in the borehole,
+with a uniform borehole wall boundary temperature given by the
+<code>port_wall</code> port.
+</p>
+<p>
+The heat transfer in the borehole is computed using a convective heat transfer
+coefficient that depends on the fluid velocity, a heat resistance between each
+pair of pipes, and a heat resistance between the pipes and the borehole wall.
+The heat capacity of the fluid and the heat capacity of the grout are taken
+into account. The vertical heat flow is assumed to be zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+July 2018, by Alex Laferri&egrave;re:<br/>
+Following major changes to the structure of the AixLib.Fluid.HeatExchangers.Ground package,
+the documentation has been changed to reflect the new role of this model.
+Additionally, this model now extends a partial borehole model.
+</li>
+<li>
+July 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Cylindrical.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Cylindrical.mo
index 7143615790..a2c026f1be 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Cylindrical.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Cylindrical.mo
@@ -199,71 +199,71 @@ equation
           textString="%name")}),
     defaultComponentName="lay",
     Documentation(info="<html>
- <p>
- Model for radial heat transfer in a hollow cylinder.
- </p>
- <p>
- If the heat capacity of the material is non-zero, then this model computes transient heat conduction, i.e., it
- computes a numerical approximation to the solution of the heat equation
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-    &rho; c ( &part; T(r,t) &frasl; &part;t ) = 
-     k ( &part;&sup2; T(r,t) &frasl; &part;r&sup2; + 1 &frasl; r &nbsp;  &part; T(r,t) &frasl; &part;r ),
- </p>
- <p>
- where 
- <i>&rho;</i>
- is the mass density,
- <i>c</i>
- is the specific heat capacity per unit mass,
- <i>T</i>
- is the temperature at location <i>r</i> and time <i>t</i> and
- <i>k</i> is the heat conductivity. 
- At the locations <i>r=r<sub>a</sub></i> and <i>r=r<sub>b</sub></i>, 
- the temperature and heat flow rate are equal to the 
- temperature and heat flow rate of the heat ports.
- </p>
- <p>
- If the heat capacity of the material is set to zero, then steady-state heat flow is computed using
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-    Q = 2 &pi; k (T<sub>a</sub>-T<sub>b</sub>)&frasl; ln(r<sub>a</sub> &frasl; r<sub>b</sub>),
- </p>
- <p>
- where
- <i>r<sub>a</sub></i> is the internal radius,
- <i>r<sub>b</sub></i> is the external radius,
- <i>T<sub>a</sub></i> is the temperature at port a and
- <i>T<sub>b</sub></i> is the temperature at port b.
- </p>
- <h4>Implementation</h4>
- <p>
- To spatially discretize the heat equation, the construction is 
- divided into compartments with <code>nSta &ge; 1</code> state variables. 
- The state variables are connected to each other through thermal conductors. 
- There is also a thermal conductor
- between the surfaces and the outermost state variables. Thus, to obtain
- the surface temperature, use <code>port_a.T</code> (or <code>port_b.T</code>)
- and not the variable <code>T[1]</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January, 2014, by Damien Picard:<br/>
- Modify the discretization of the cilindrical layer so that the first three layers have an equal thickness the following an exponentionally growing thickness.
- This follows the guidelines of Eskilson (P. Eskilson. Thermal analysis of heat extraction
- boreholes. PhD thesis, Dep. of Mathematical
- Physics, University of Lund, Sweden, 1987).
- </li>
- <li>
- March 9, 2012, by Michael Wetter:<br/>
- Removed protected variable <code>der_T</code> as it is not required.
- </li>
- <li>
- April 14 2011, by Pierre Vigouroux:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model for radial heat transfer in a hollow cylinder.
+</p>
+<p>
+If the heat capacity of the material is non-zero, then this model computes transient heat conduction, i.e., it
+computes a numerical approximation to the solution of the heat equation
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+   &rho; c ( &part; T(r,t) &frasl; &part;t ) = 
+    k ( &part;&sup2; T(r,t) &frasl; &part;r&sup2; + 1 &frasl; r &nbsp;  &part; T(r,t) &frasl; &part;r ),
+</p>
+<p>
+where 
+<i>&rho;</i>
+is the mass density,
+<i>c</i>
+is the specific heat capacity per unit mass,
+<i>T</i>
+is the temperature at location <i>r</i> and time <i>t</i> and
+<i>k</i> is the heat conductivity. 
+At the locations <i>r=r<sub>a</sub></i> and <i>r=r<sub>b</sub></i>, 
+the temperature and heat flow rate are equal to the 
+temperature and heat flow rate of the heat ports.
+</p>
+<p>
+If the heat capacity of the material is set to zero, then steady-state heat flow is computed using
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+   Q = 2 &pi; k (T<sub>a</sub>-T<sub>b</sub>)&frasl; ln(r<sub>a</sub> &frasl; r<sub>b</sub>),
+</p>
+<p>
+where
+<i>r<sub>a</sub></i> is the internal radius,
+<i>r<sub>b</sub></i> is the external radius,
+<i>T<sub>a</sub></i> is the temperature at port a and
+<i>T<sub>b</sub></i> is the temperature at port b.
+</p>
+<h4>Implementation</h4>
+<p>
+To spatially discretize the heat equation, the construction is 
+divided into compartments with <code>nSta &ge; 1</code> state variables. 
+The state variables are connected to each other through thermal conductors. 
+There is also a thermal conductor
+between the surfaces and the outermost state variables. Thus, to obtain
+the surface temperature, use <code>port_a.T</code> (or <code>port_b.T</code>)
+and not the variable <code>T[1]</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January, 2014, by Damien Picard:<br/>
+Modify the discretization of the cilindrical layer so that the first three layers have an equal thickness the following an exponentionally growing thickness.
+This follows the guidelines of Eskilson (P. Eskilson. Thermal analysis of heat extraction
+boreholes. PhD thesis, Dep. of Mathematical
+Physics, University of Lund, Sweden, 1987).
+</li>
+<li>
+March 9, 2012, by Michael Wetter:<br/>
+Removed protected variable <code>der_T</code> as it is not required.
+</li>
+<li>
+April 14 2011, by Pierre Vigouroux:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Cylindrical;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/GroundTemperatureResponse.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/GroundTemperatureResponse.mo
index c73ab51b30..82fc495534 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/GroundTemperatureResponse.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/GroundTemperatureResponse.mo
@@ -3,6 +3,9 @@ model GroundTemperatureResponse "Model calculating discrete load aggregation"
   parameter Modelica.Units.SI.Time tLoaAgg(final min=Modelica.Constants.eps)=
     3600 "Time resolution of load aggregation";
   parameter Integer nCel(min=1)=5 "Number of cells per aggregation level";
+  parameter Integer nSeg=12
+    "Number of segments per borehole for g-function calculation";
+  parameter Integer nClu=5 "Number of clusters for g-function calculation";
   parameter Boolean forceGFunCalc = false
     "Set to true to force the thermal response to be calculated at the start instead of checking whether it has been pre-computed";
   parameter AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Template borFieDat
@@ -19,9 +22,6 @@ model GroundTemperatureResponse "Model calculating discrete load aggregation"
         iconTransformation(extent={{-120,-10},{-100,10}})));
 
 protected
-  constant Integer nSegMax = 1500 "Max total number of segments in g-function calculation";
-  final parameter Integer nSeg = integer(if 12*borFieDat.conDat.nBor<nSegMax then 12 else floor(nSegMax/borFieDat.conDat.nBor))
-    "Number of segments per borehole for g-function calculation";
   constant Integer nTimSho = 26 "Number of time steps in short time region";
   constant Integer nTimLon = 50 "Number of time steps in long time region";
   constant Real ttsMax = exp(5) "Maximum non-dimensional time for g-function calculation";
@@ -38,6 +38,7 @@ protected
       rBor=borFieDat.conDat.rBor,
       aSoi=borFieDat.soiDat.aSoi,
       nSeg=nSeg,
+      nClu=nClu,
       nTimSho=nTimSho,
       nTimLon=nTimLon,
       ttsMax=ttsMax) "String with encrypted g-function arguments";
@@ -114,6 +115,7 @@ initial equation
       aSoi=borFieDat.soiDat.aSoi,
       kSoi=borFieDat.soiDat.kSoi,
       nSeg=nSeg,
+      nClu=nClu,
       nTimSho=nTimSho,
       nTimLon=nTimLon,
       nTimTot=nTimTot,
@@ -185,164 +187,176 @@ equation
   Diagram(
         coordinateSystem(preserveAspectRatio=false)),
         Documentation(info="<html>
- <p>
- This model calculates the ground temperature response to obtain the temperature
- at the borehole wall in a geothermal system where heat is being injected into or
- extracted from the ground.
- </p>
- <p>
- A load-aggregation scheme based on that developed by Claesson and Javed (2012) is
- used to calculate the borehole wall temperature response with the temporal superposition
- of ground thermal loads. In its base form, the
- load-aggregation scheme uses fixed-length aggregation cells to agglomerate
- thermal load history together, with more distant cells (denoted with a higher cell and vector index)
- representing more distant thermal history. The more distant the thermal load, the
- less impactful it is on the borehole wall temperature change at the current time step.
- Each cell has an <em>aggregation time</em> associated to it denoted by <code>nu</code>,
- which corresponds to the simulation time (since the beginning of heat injection or
- extraction) at which the cell will begin shifting its thermal load to more distant
- cells. To determine <code>nu</code>, cells have a temporal size <i>r<sub>cel</sub></i>
- (<code>rcel</code> in this model)
- which follows the exponential growth
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_02.png\" />
- </p>
- <p>
- where <i>n<sub>Cel</sub></i> is the number of consecutive cells which can have the same size.
- Decreasing <i>r<sub>cel</sub></i> will generally decrease calculation times, at the cost of
- precision in the temporal superposition. <code>rcel</code> is expressed in multiples
- of the aggregation time resolution (via the parameter <code>tLoaAgg</code>).
- Then, <code>nu</code> may be expressed as the sum of all <code>rcel</code> values
- (multiplied by the aggregation time resolution) up to and including that cell in question.
- </p>
- <p>
- To determine the weighting factors, the borefield's temperature
- step response at the borefield wall is determined as
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_03.png\" />
- </p>
- <p>
- where <i>g(&middot;)</i> is the borefield's thermal response factor known as the <em>g-function</em>,
- <i>H</i> is the total length of all boreholes and <i>k<sub>s</sub></i> is the thermal
- conductivity of the soil. The weighting factors <code>kappa</code> (<i>&kappa;</i> in the equation below)
- for a given cell <i>i</i> are then expressed as follows.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_04.png\" />
- </p>
- <p>
- where <i>&nu;</i> refers to the vector <code>nu</code> in this model and
- <i>T<sub>step</sub>(&nu;<sub>0</sub>)</i>=0.
- </p>
- <p>
- At every aggregation time step, a time event is generated to perform the load aggregation steps.
- First, the thermal load is shifted. When shifting between cells of different size, total
- energy is conserved. This operation is illustred in the figure below by Cimmino (2014).
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_01.png\" />
- </p>
- <p>
- After the cell-shifting operation is performed, the first aggregation cell has its
- value set to the average thermal load since the last aggregation step.
- Temporal superposition is then applied by means
- of a scalar product between the aggregated thermal loads <code>QAgg_flow</code> and the
- weighting factors <i>&kappa;</i>.
- </p>
- <p>
- Due to Modelica's variable time steps, the load aggregation scheme is modified by separating
- the thermal response between the current aggregation time step and everything preceding it.
- This is done according to
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_05.png\" />
- <br/>
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_06.png\" />
- </p>
- <p>
- where <i>T<sub>b</sub></i> is the borehole wall temperature,
- <i>T<sub>g</sub></i>
- is the undisturbed ground temperature,
- <i>Q</i> is the ground thermal load per borehole length and <i>h = g/(2 &pi; k<sub>s</sub>)</i>
- is a temperature response factor based on the g-function. <i>t<sub>k</sub></i>
- is the last discrete aggregation time step, meaning that the current time <i>t</i>
- satisfies <i>t<sub>k</sub>&le;t&le;t<sub>k+1</sub></i>.
- <i>&Delta;t<sub>agg</sub>(=t<sub>k+1</sub>-t<sub>k</sub>)</i> is the
- parameter <code>tLoaAgg</code> in the present model.
- </p>
- <p>
- Thus,
- <i>&Delta;T<sub>b</sub>*(t)</i>
- is the borehole wall temperature change due to the thermal history prior to the current
- aggregation step. At every aggregation time step, load aggregation and temporal superposition
- are used to calculate its discrete value. Assuming no heat injection or extraction until
- <i>t<sub>k+1</sub></i>, this term is assumed to have a linear
- time derivative, which is given by the difference between <i>&Delta;T<sub>b</sub>*(t<sub>k+1</sub>)</i>
- (the temperature change from load history at the next discrete aggregation time step, which
- is constant over the duration of the ongoing aggregation time step) and the total
- temperature change at the last aggregation time step, <i>&Delta;T<sub>b</sub>(t)</i>.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_09.png\" />
- </p>
- <p>
- The second term <i>&Delta;T<sub>b,q</sub>(t)</i> concerns the ongoing aggregation time step.
- To obtain the time derivative of this term, the thermal response factor <i>h</i> is assumed
- to vary linearly over the course of an aggregation time step. Therefore, because
- the ongoing aggregation time step always concerns the first aggregation cell, its derivative (denoted
- by the parameter <code>dTStepdt</code> in this model) can be calculated as
- <code>kappa[1]</code>, the first value in the <code>kappa</code> vector,
- divided by the aggregation time step <i>&Delta;t</i>.
- The derivative of the temperature change at the borehole wall is then expressed
- as the multiplication of <code>dTStepdt</code> (which only needs to be
- calculated once at the start of the simulation) and the heat flow <i>Q</i> at
- the borehole wall.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_10.png\" />
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_11.png\" />
- </p>
- <p>
- With the two terms in the expression of <i>&Delta;T<sub>b</sub>(t)</i> expressed
- as time derivatives, <i>&Delta;T<sub>b</sub>(t)</i> can itself also be
- expressed as its time derivative and implemented as such directly in the Modelica
- equations block with the <code>der()</code> operator.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_07.png\" />
- <br/>
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_08.png\" />
- </p>
- <p>
- This load aggregation scheme is validated in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Validation.Analytic_20Years\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Validation.Analytic_20Years</a>.
- </p>
- <h4>References</h4>
- <p>
- Cimmino, M. 2014. <i>D&eacute;veloppement et validation exp&eacute;rimentale de facteurs de r&eacute;ponse
- thermique pour champs de puits g&eacute;othermiques</i>,
- Ph.D. Thesis, &Eacute;cole Polytechnique de Montr&eacute;al.
- </p>
- <p>
- Claesson, J. and Javed, S. 2012. <i>A load-aggregation method to calculate extraction temperatures of borehole heat exchangers</i>. ASHRAE Transactions 118(1): 530-539.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 30, 2018, by Michael Wetter:<br/>
- Refactored model to compute the temperature difference relative to the initial temperature,
- because the model is independent of the initial temperature.
- </li>
- <li>
- April 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model calculates the ground temperature response to obtain the temperature
+at the borehole wall in a geothermal system where heat is being injected into or
+extracted from the ground.
+</p>
+<p>
+A load-aggregation scheme based on that developed by Claesson and Javed (2012) is
+used to calculate the borehole wall temperature response with the temporal superposition
+of ground thermal loads. In its base form, the
+load-aggregation scheme uses fixed-length aggregation cells to agglomerate
+thermal load history together, with more distant cells (denoted with a higher cell and vector index)
+representing more distant thermal history. The more distant the thermal load, the
+less impactful it is on the borehole wall temperature change at the current time step.
+Each cell has an <em>aggregation time</em> associated to it denoted by <code>nu</code>,
+which corresponds to the simulation time (since the beginning of heat injection or
+extraction) at which the cell will begin shifting its thermal load to more distant
+cells. To determine <code>nu</code>, cells have a temporal size <i>r<sub>cel</sub></i>
+(<code>rcel</code> in this model)
+which follows the exponential growth
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_02.png\" />
+</p>
+<p>
+where <i>n<sub>Cel</sub></i> is the number of consecutive cells which can have the same size.
+Decreasing <i>r<sub>cel</sub></i> will generally decrease calculation times, at the cost of
+precision in the temporal superposition. <code>rcel</code> is expressed in multiples
+of the aggregation time resolution (via the parameter <code>tLoaAgg</code>).
+Then, <code>nu</code> may be expressed as the sum of all <code>rcel</code> values
+(multiplied by the aggregation time resolution) up to and including that cell in question.
+</p>
+<p>
+To determine the weighting factors, the borefield's temperature
+step response at the borefield wall is determined as
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_03.png\" />
+</p>
+<p>
+where <i>g(&middot;)</i> is the borefield's thermal response factor known as the <em>g-function</em>,
+<i>H</i> is the total length of all boreholes and <i>k<sub>s</sub></i> is the thermal
+conductivity of the soil. The weighting factors <code>kappa</code> (<i>&kappa;</i> in the equation below)
+for a given cell <i>i</i> are then expressed as follows.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_04.png\" />
+</p>
+<p>
+where <i>&nu;</i> refers to the vector <code>nu</code> in this model and
+<i>T<sub>step</sub>(&nu;<sub>0</sub>)</i>=0.
+</p>
+<p>
+At every aggregation time step, a time event is generated to perform the load aggregation steps.
+First, the thermal load is shifted. When shifting between cells of different size, total
+energy is conserved. This operation is illustred in the figure below by Cimmino (2014).
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_01.png\" />
+</p>
+<p>
+After the cell-shifting operation is performed, the first aggregation cell has its
+value set to the average thermal load since the last aggregation step.
+Temporal superposition is then applied by means
+of a scalar product between the aggregated thermal loads <code>QAgg_flow</code> and the
+weighting factors <i>&kappa;</i>.
+</p>
+<p>
+Due to Modelica's variable time steps, the load aggregation scheme is modified by separating
+the thermal response between the current aggregation time step and everything preceding it.
+This is done according to
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_05.png\" />
+<br/>
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_06.png\" />
+</p>
+<p>
+where <i>T<sub>b</sub></i> is the borehole wall temperature,
+<i>T<sub>g</sub></i>
+is the undisturbed ground temperature,
+<i>Q</i> is the ground thermal load per borehole length and <i>h = g/(2 &pi; k<sub>s</sub>)</i>
+is a temperature response factor based on the g-function. <i>t<sub>k</sub></i>
+is the last discrete aggregation time step, meaning that the current time <i>t</i>
+satisfies <i>t<sub>k</sub>&le;t&le;t<sub>k+1</sub></i>.
+<i>&Delta;t<sub>agg</sub>(=t<sub>k+1</sub>-t<sub>k</sub>)</i> is the
+parameter <code>tLoaAgg</code> in the present model.
+</p>
+<p>
+Thus,
+<i>&Delta;T<sub>b</sub>*(t)</i>
+is the borehole wall temperature change due to the thermal history prior to the current
+aggregation step. At every aggregation time step, load aggregation and temporal superposition
+are used to calculate its discrete value. Assuming no heat injection or extraction until
+<i>t<sub>k+1</sub></i>, this term is assumed to have a linear
+time derivative, which is given by the difference between <i>&Delta;T<sub>b</sub>*(t<sub>k+1</sub>)</i>
+(the temperature change from load history at the next discrete aggregation time step, which
+is constant over the duration of the ongoing aggregation time step) and the total
+temperature change at the last aggregation time step, <i>&Delta;T<sub>b</sub>(t)</i>.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_09.png\" />
+</p>
+<p>
+The second term <i>&Delta;T<sub>b,q</sub>(t)</i> concerns the ongoing aggregation time step.
+To obtain the time derivative of this term, the thermal response factor <i>h</i> is assumed
+to vary linearly over the course of an aggregation time step. Therefore, because
+the ongoing aggregation time step always concerns the first aggregation cell, its derivative (denoted
+by the parameter <code>dTStepdt</code> in this model) can be calculated as
+<code>kappa[1]</code>, the first value in the <code>kappa</code> vector,
+divided by the aggregation time step <i>&Delta;t</i>.
+The derivative of the temperature change at the borehole wall is then expressed
+as the multiplication of <code>dTStepdt</code> (which only needs to be
+calculated once at the start of the simulation) and the heat flow <i>Q</i> at
+the borehole wall.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_10.png\" />
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_11.png\" />
+</p>
+<p>
+With the two terms in the expression of <i>&Delta;T<sub>b</sub>(t)</i> expressed
+as time derivatives, <i>&Delta;T<sub>b</sub>(t)</i> can itself also be
+expressed as its time derivative and implemented as such directly in the Modelica
+equations block with the <code>der()</code> operator.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_07.png\" />
+<br/>
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_08.png\" />
+</p>
+<p>
+This load aggregation scheme is validated in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Validation.Analytic_20Years\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Validation.Analytic_20Years</a>.
+</p>
+<h4>References</h4>
+<p>
+Cimmino, M. 2014. <i>D&eacute;veloppement et validation exp&eacute;rimentale de facteurs de r&eacute;ponse
+thermique pour champs de puits g&eacute;othermiques</i>,
+Ph.D. Thesis, &Eacute;cole Polytechnique de Montr&eacute;al.
+</p>
+<p>
+Claesson, J. and Javed, S. 2012. <i>A load-aggregation method to calculate extraction temperatures of borehole heat exchangers</i>. ASHRAE Transactions 118(1): 530-539.
+</p>
+<p>
+Prieto, C. and Cimmino, M. 2021. <i>Thermal interactions in large irregular
+fields of geothermal boreholes: the method of equivalent boreholes</i>. Journal
+of Building Performance Simulation 14(4): 446-460.
+<a href=\"https://doi.org/10.1080/19401493.2021.1968953\">
+doi:10.1080/19401493.2021.1968953</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022 by Massimo Cimmino:<br/>
+Updated the function to use the more efficient method of Prieto and Cimmino
+(2021).
+</li>
+<li>
+August 30, 2018, by Michael Wetter:<br/>
+Refactored model to compute the temperature difference relative to the initial temperature,
+because the model is independent of the initial temperature.
+</li>
+<li>
+April 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end GroundTemperatureResponse;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationCellTimes.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationCellTimes.mo
index d50ea58af0..d6653e2bdb 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationCellTimes.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationCellTimes.mo
@@ -30,19 +30,19 @@ annotation (experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationCellTimes.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This validation case builds the aggregation vectors (<code>rCel</code> and <code>nu</code>)
- for a fictional case with 6 cells, built in 3 layers of 2 cells which double in size
- each level. The <code>timFin</code> input to the function called is lower than the aggregation
- time of the 6th cell, and the 6th cell must therefore be truncated from a size of 4 to a size of 2.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case builds the aggregation vectors (<code>rCel</code> and <code>nu</code>)
+for a fictional case with 6 cells, built in 3 layers of 2 cells which double in size
+each level. The <code>timFin</code> input to the function called is lower than the aggregation
+time of the 6th cell, and the 6th cell must therefore be truncated from a size of 4 to a size of 2.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 18, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AggregationCellTimes;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationWeightingFactors.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationWeightingFactors.mo
index 3fc2746d44..452dbe2fec 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationWeightingFactors.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationWeightingFactors.mo
@@ -25,21 +25,21 @@ annotation (experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/AggregationWeightingFactors.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This validation case uses the first few values of a borehole temperature reponse
- time series to construct the weighting factors <code>kappa</code>. The aggregation
- cells are chosen such that there is a change in levels (and therefore a doubling
- in the size of the cells) from cell 5 to 6. Therefore, <code>kappa[5]</code> is lower than
- <code>kappa[4]</code> and <code>kappa[7]</code> is lower than <code>kappa[6]</code>, but
- <code>kappa[6]</code> is higher than <code>kappa[5]</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case uses the first few values of a borehole temperature reponse
+time series to construct the weighting factors <code>kappa</code>. The aggregation
+cells are chosen such that there is a change in levels (and therefore a doubling
+in the size of the cells) from cell 5 to 6. Therefore, <code>kappa[5]</code> is lower than
+<code>kappa[4]</code> and <code>kappa[7]</code> is lower than <code>kappa[6]</code>, but
+<code>kappa[6]</code> is higher than <code>kappa[5]</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 18, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AggregationWeightingFactors;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/CountAggregationCells.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/CountAggregationCells.mo
index f0ddacb453..b05973f928 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/CountAggregationCells.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/CountAggregationCells.mo
@@ -15,19 +15,19 @@ annotation (experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/CountAggregationCells.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This validation case counts the required length of the aggregation vectors for the
- same fictional case as in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.LoadAggregation.Validation.AggregationCellTimes\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.LoadAggregation.Validation.AggregationCellTimes</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case counts the required length of the aggregation vectors for the
+same fictional case as in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.LoadAggregation.Validation.AggregationCellTimes\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.LoadAggregation.Validation.AggregationCellTimes</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 18, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CountAggregationCells;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/ShiftAggregationCells.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/ShiftAggregationCells.mo
index ece9de0f7f..737c1328fe 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/ShiftAggregationCells.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/ShiftAggregationCells.mo
@@ -24,25 +24,25 @@ annotation (experiment(StartTime=3.5,StopTime=5.5,Tolerance=1e-6),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/ShiftAggregationCells.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This validation case replicates the load-shifting procedure illustred in the figure below by Cimmino (2014).
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_01.png\" />
- </p>
- <h4>References</h4>
- <p>
- Cimmino, M. 2014. <i>D&eacute;veloppement et validation exp&eacute;rimentale de facteurs de r&eacute;ponse
- thermique pour champs de puits g&eacute;othermiques</i>,
- Ph.D. Thesis, &Eacute;cole Polytechnique de Montr&eacute;al.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case replicates the load-shifting procedure illustred in the figure below by Cimmino (2014).
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/LoadAggregation_01.png\" />
+</p>
+<h4>References</h4>
+<p>
+Cimmino, M. 2014. <i>D&eacute;veloppement et validation exp&eacute;rimentale de facteurs de r&eacute;ponse
+thermique pour champs de puits g&eacute;othermiques</i>,
+Ph.D. Thesis, &Eacute;cole Polytechnique de Montr&eacute;al.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 18, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ShiftAggregationCells;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemperatureResponseMatrix.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemperatureResponseMatrix.mo
index 4b7103d44e..f81a175fe0 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemperatureResponseMatrix.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemperatureResponseMatrix.mo
@@ -13,6 +13,7 @@ model TemperatureResponseMatrix
       aSoi=1e-6,
       kSoi=3,
       nSeg=12,
+      nClu=1,
       nTimSho=26,
       nTimLon=50,
       nTimTot=26 + 50,
@@ -28,19 +29,19 @@ annotation (experiment(StopTime=31536000,Tolerance=1e-6),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemperatureResponseMatrix.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This validation case calculates the g-function for a defined single borehole, turns it
- into a temperature step response, saves it as &#34;TemperatureResponseMatrix_validationTStep.mat&#34;,
- reads this .mat file and shows the evolution of the temperature step reponse over
- the course of the first year.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case calculates the g-function for a defined single borehole, turns it
+into a temperature step response, saves it as &#34;TemperatureResponseMatrix_validationTStep.mat&#34;,
+reads this .mat file and shows the evolution of the temperature step reponse over
+the course of the first year.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 18, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureResponseMatrix;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemporalSuperposition.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemporalSuperposition.mo
index 4bee95222f..7e5e8f11bc 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemporalSuperposition.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemporalSuperposition.mo
@@ -17,19 +17,19 @@ annotation (experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/Validation/TemporalSuperposition.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This validation case uses a fictional load profile and weighting factors to ensure
- that the temporal superposition is correctly done. The <code>curCel</code> input to
- the function called truncates the vectors involved in the scalar product such that
- the large load in the <code>QAgg_flow</code> vector mustn't affect the final result.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case uses a fictional load profile and weighting factors to ensure
+that the temporal superposition is correctly done. The <code>curCel</code> input to
+the function called truncates the vectors involved in the scalar product such that
+the large load in the <code>QAgg_flow</code> vector mustn't affect the final result.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 18, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemporalSuperposition;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/aggregationCellTimes.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/aggregationCellTimes.mo
index c5dc471d08..85ad1fba6c 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/aggregationCellTimes.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/aggregationCellTimes.mo
@@ -32,23 +32,23 @@ algorithm
   end if;
 
   annotation (Documentation(info="<html>
- <p>Simultaneously constructs both the <code>nu</code> vector, which is the
- aggregation time of each cell, and the <code>rCel</code> vector, which
- is the temporal size of each cell normalized with the time resolution of load
- aggregation <code>tLoaAgg</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Added <code>min=Modelica.Constants.small</code> to <code>tLoaAgg</code>
- so that a tool can infer that this quantity is non-zero.
- </li>
- <li>
- March 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>Simultaneously constructs both the <code>nu</code> vector, which is the
+aggregation time of each cell, and the <code>rCel</code> vector, which
+is the temporal size of each cell normalized with the time resolution of load
+aggregation <code>tLoaAgg</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Added <code>min=Modelica.Constants.small</code> to <code>tLoaAgg</code>
+so that a tool can infer that this quantity is non-zero.
+</li>
+<li>
+March 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end aggregationCellTimes;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/aggregationWeightingFactors.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/aggregationWeightingFactors.mo
index d8c83146c9..741fb077b7 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/aggregationWeightingFactors.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/aggregationWeightingFactors.mo
@@ -67,19 +67,19 @@ algorithm
   end for;
 
   annotation (Documentation(info="<html>
- <p>
- This function uses spline interpolation to construct the weighting factors
- vector <code>kappa</code> using the aggregation times <code>nu</code> and the
- temperature step reponse (a time-series in the form of a matrix) of the
- borefield as an input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function uses spline interpolation to construct the weighting factors
+vector <code>kappa</code> using the aggregation times <code>nu</code> and the
+temperature step reponse (a time-series in the form of a matrix) of the
+borefield as an input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end aggregationWeightingFactors;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/countAggregationCells.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/countAggregationCells.mo
index 8824d4600f..5b7cdda627 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/countAggregationCells.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/countAggregationCells.mo
@@ -27,23 +27,23 @@ algorithm
   end while;
 
 annotation (Documentation(info="<html>
- <p>
- Function that counts the required length of the aggregation time vector
- <code>nu</code> and of the weighting factor vectors <code>kappa</code> based on
- the maximum time for calculations related to the ground temperature response.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Added <code>min=1</code> to <code>nCel</code>
- so that a tool can infer that this quantity is non-zero.
- </li>
- <li>
- March 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that counts the required length of the aggregation time vector
+<code>nu</code> and of the weighting factor vectors <code>kappa</code> based on
+the maximum time for calculations related to the ground temperature response.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Added <code>min=1</code> to <code>nCel</code>
+so that a tool can infer that this quantity is non-zero.
+</li>
+<li>
+March 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end countAggregationCells;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/shiftAggregationCells.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/shiftAggregationCells.mo
index 76bb0ef8cf..4351b175d9 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/shiftAggregationCells.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/shiftAggregationCells.mo
@@ -33,24 +33,24 @@ algorithm
   QAggShi_flow[1] := 0;
 
   annotation (Documentation(info="<html>
- <p>
- Performs the shifting operation which propagates the thermal load history
- towards the more distant aggregation cells, and then sets the current cell's
- value at <i>0</i>. Additionally, this function also outputs the last filled load
- aggregation cell.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Added <code>min=Modelica.Constants.small</code> to <code>rCel</code>
- so that a tool can infer that this quantity is non-zero.
- </li>
- <li>
- March 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Performs the shifting operation which propagates the thermal load history
+towards the more distant aggregation cells, and then sets the current cell's
+value at <i>0</i>. Additionally, this function also outputs the last filled load
+aggregation cell.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Added <code>min=Modelica.Constants.small</code> to <code>rCel</code>
+so that a tool can infer that this quantity is non-zero.
+</li>
+<li>
+March 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end shiftAggregationCells;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/temperatureResponseMatrix.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/temperatureResponseMatrix.mo
index f84a2f22c9..9eb3d4d551 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/temperatureResponseMatrix.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/temperatureResponseMatrix.mo
@@ -12,6 +12,7 @@ impure function temperatureResponseMatrix
   input Modelica.Units.SI.ThermalConductivity kSoi
     "Thermal conductivity of soil";
   input Integer nSeg "Number of line source segments per borehole";
+  input Integer nClu "Number of clusters for g-function calculation";
   input Integer nTimSho "Number of time steps in short time region";
   input Integer nTimLon "Number of time steps in long time region";
   input Integer nTimTot "Number of g-function points";
@@ -28,11 +29,22 @@ protected
   Modelica.Units.SI.Time[nTimTot] tGFun "g-function evaluation times";
   Real[nTimTot] gFun "g-function vector";
   Boolean writegFun = false "True if g-function was succesfully written to file";
+  Integer labels[nBor](each fixed=false) "Cluster label associated with each data point";
+  Integer cluSiz[nClu](each fixed=false) "Size of the clusters";
+  Integer nCluUni "Number of unique borehole clusters";
 
 algorithm
   pathSave := "tmp/temperatureResponseMatrix/" + sha + "TStep.mat";
 
   if forceGFunCalc or not Modelica.Utilities.Files.exist(pathSave) then
+    (labels, cluSiz, nCluUni) :=
+      AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.clusterBoreholes(
+      nBor=nBor,
+      cooBor=cooBor,
+      hBor=hBor,
+      dBor=dBor,
+      rBor=rBor,
+      nClu=nClu);
     (tGFun,gFun) :=
       AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.gFunction(
       nBor=nBor,
@@ -42,9 +54,12 @@ algorithm
       rBor=rBor,
       aSoi=aSoi,
       nSeg=nSeg,
+      nClu=nCluUni,
       nTimSho=nTimSho,
       nTimLon=nTimLon,
-      ttsMax=ttsMax);
+      ttsMax=ttsMax,
+      labels = labels,
+      cluSiz = cluSiz[1:nCluUni]);
 
     for i in 1:nTimTot loop
       TStep[i,1] := tGFun[i];
@@ -69,43 +84,43 @@ algorithm
     ncol=2);
 
   annotation (Documentation(info="<html>
- <p>
- This function uses the parameters required to calculate the borefield's thermal
- response to build a SHA1-encrypted string unique to the borefield in question.
- Then, if the <code>forceGFunCalc</code> input is <code>true</code> or if
- there is no <code>.mat</code> file with the SHA1 hash as its filename in the
- <code>tmp/temperatureResponseMatrix</code> folder,
- the thermal response will be calculated and written as a
- <code>.mat</code> file. Otherwise, the
- thermal response will simply be read from the
- <code>.mat</code> file. In the <code>.mat</code> file, the data
- is saved in a matrix with the name <code>TStep</code>, where the first column is
- the time (in seconds) and the second column is the temperature step response,
- which is the g-function divided by <i>2 &pi; H k<sub>soi</sub></i>, with
- <code>H</code> being the borehole length and <i>k<sub>soi</sub></i> being the thermal
- conductivity of the soil.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>impure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- August 27, 2018, by Michael Wetter:<br/>
- Changed name of temporary directory so that it is clear for users
- that this is a temporary directory.
- </li>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Changed implementation to use matrix read and write from
- the Modelica Standard Library.
- </li>
- <li>
- March 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function uses the parameters required to calculate the borefield's thermal
+response to build a SHA1-encrypted string unique to the borefield in question.
+Then, if the <code>forceGFunCalc</code> input is <code>true</code> or if
+there is no <code>.mat</code> file with the SHA1 hash as its filename in the
+<code>tmp/temperatureResponseMatrix</code> folder,
+the thermal response will be calculated and written as a
+<code>.mat</code> file. Otherwise, the
+thermal response will simply be read from the
+<code>.mat</code> file. In the <code>.mat</code> file, the data
+is saved in a matrix with the name <code>TStep</code>, where the first column is
+the time (in seconds) and the second column is the temperature step response,
+which is the g-function divided by <i>2 &pi; H k<sub>soi</sub></i>, with
+<code>H</code> being the borehole length and <i>k<sub>soi</sub></i> being the thermal
+conductivity of the soil.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>impure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+August 27, 2018, by Michael Wetter:<br/>
+Changed name of temporary directory so that it is clear for users
+that this is a temporary directory.
+</li>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Changed implementation to use matrix read and write from
+the Modelica Standard Library.
+</li>
+<li>
+March 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end temperatureResponseMatrix;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/temporalSuperposition.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/temporalSuperposition.mo
index 0b54259d08..e9a21e1634 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/temporalSuperposition.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/LoadAggregation/temporalSuperposition.mo
@@ -18,20 +18,20 @@ algorithm
   annotation (
 Inline=true,
 Documentation(info="<html>
- <p>
- Performs the temporal superposition operation to obtain the temperature change
- at the borehole wall at the current time step, which is the scalar product of
- the aggregated load vector and the <code>kappa</code> step response vector. To
- avoid unnecessary calculations, the current aggregation cell in the simulation
- is used to truncate the values from the vectors that are not required.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Performs the temporal superposition operation to obtain the temperature change
+at the borehole wall at the current time step, which is the scalar product of
+the aggregated load vector and the <code>kappa</code> step response vector. To
+avoid unnecessary calculations, the current aggregation cell in the simulation
+is used to truncate the values from the vectors that are not required.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end temporalSuperposition;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ClusterBoreholes_100boreholes.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ClusterBoreholes_100boreholes.mo
new file mode 100644
index 0000000000..9309cc548b
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ClusterBoreholes_100boreholes.mo
@@ -0,0 +1,51 @@
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation;
+model ClusterBoreholes_100boreholes
+  "Clustering of a field of 100 boreholes"
+  extends Modelica.Icons.Example;
+
+  parameter Integer nBor = 100 "Number of boreholes";
+  parameter Modelica.Units.SI.Position cooBor[nBor, 2] = {{7.5*mod(i-1,10), 7.5*floor((i-1)/10)} for i in 1:nBor}
+    "Coordinates of boreholes";
+  parameter Modelica.Units.SI.Height hBor=150 "Borehole length";
+  parameter Modelica.Units.SI.Height dBor=4 "Borehole buried depth";
+  parameter Modelica.Units.SI.Radius rBor=0.075 "Borehole radius";
+  parameter Integer k=4 "Number of clusters to be generated";
+
+  parameter Integer labels[nBor](each fixed=false) "Cluster label associated with each data point";
+  parameter Integer cluSiz[k](each fixed=false) "Size of the clusters";
+
+  parameter Integer labelsExp[nBor]=
+    {3, 3, 3, 4, 4, 4, 4, 3, 3, 3, 3, 4, 4, 2, 2, 2, 2, 4, 4, 3, 3, 4, 2, 2, 1,
+     1, 2, 2, 4, 3, 4, 2, 2, 1, 1, 1, 1, 2, 2, 4, 4, 2, 1, 1, 1, 1, 1, 1, 2, 4,
+     4, 2, 1, 1, 1, 1, 1, 1, 2, 4, 4, 2, 2, 1, 1, 1, 1, 2, 2, 4, 3, 4, 2, 2, 1,
+     1, 2, 2, 4, 3, 3, 4, 4, 2, 2, 2, 2, 4, 4, 3, 3, 3, 3, 4, 4, 4, 4, 3, 3, 3}
+    "Expected cluster labels";
+
+  // Comparison result
+  Boolean cmp "Comparison result";
+
+initial equation
+  (labels, cluSiz) = AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.clusterBoreholes(nBor,cooBor,hBor,dBor,rBor,k);
+
+equation
+  cmp = Modelica.Math.Vectors.isEqual(labels, labelsExp);
+
+annotation (experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ClusterBoreholes_100boreholes.mos"
+        "Simulate and plot"),
+      Documentation(info="<html>
+<p>
+This example uses a rectangular field of 10 by 10 boreholes to test the
+identification borehole clusters.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+June 9, 2022 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ClusterBoreholes_100boreholes;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/CylindricalHeatSource.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/CylindricalHeatSource.mo
index 1ab4f54bfb..7188e08a40 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/CylindricalHeatSource.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/CylindricalHeatSource.mo
@@ -26,17 +26,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=15.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for the evaluation of the
- cylindrical heat source solution.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 11, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for the evaluation of the
+cylindrical heat source solution.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 11, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CylindricalHeatSource;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/CylindricalHeatSource_Integrand.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/CylindricalHeatSource_Integrand.mo
index 9a13ca163d..770ecb5eea 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/CylindricalHeatSource_Integrand.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/CylindricalHeatSource_Integrand.mo
@@ -23,17 +23,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StartTime=0.01, StopTime=15.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the evaluation of the
- cylindrical heat source integrand function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the evaluation of the
+cylindrical heat source integrand function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CylindricalHeatSource_Integrand;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource.mo
index da7f7ad1a0..fcec40d1d2 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource.mo
@@ -59,18 +59,18 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=20.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for the evaluation of the
- finite line source solution. The solution is evaluated at different positions
- and averaged over different lengths around line heat sources.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 12, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for the evaluation of the
+finite line source solution. The solution is evaluated at different positions
+and averaged over different lengths around line heat sources.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 12, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FiniteLineSource;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Equivalent.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Equivalent.mo
new file mode 100644
index 0000000000..0b97705733
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Equivalent.mo
@@ -0,0 +1,89 @@
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation;
+model FiniteLineSource_Equivalent
+  "Test case for finite line source for equivalent boreholes"
+  extends Modelica.Icons.Example;
+
+  parameter Modelica.Units.SI.ThermalDiffusivity aSoi=1.0e-6
+    "Ground thermal diffusivity";
+  parameter Modelica.Units.SI.Distance[2] dis={7.0, 7.0*sqrt(2)}
+    "Radial distance between borehole axes";
+  parameter Integer[2] wDis={4, 2}
+    "Number of occurences of each distance";
+  parameter Modelica.Units.SI.Height len1=150.0 "Length of emitting sources";
+  parameter Modelica.Units.SI.Height burDep1=4.0
+    "Buried depth of emitting sources";
+  parameter Modelica.Units.SI.Height len2=150.0 "Length of receiving lines";
+  parameter Modelica.Units.SI.Height burDep2=4.0
+    "Buried depth of receiving lines";
+  parameter Integer nBor2=3 "Number of receiving lines";
+  parameter Integer n_dis=2 "Number of unique distances";
+
+  Modelica.Units.SI.Time t "Time";
+  Real hRea "Finite line source solution (Real part)";
+  Real hMir "Finite line source solution (Mirror part)";
+  Real h "Finite line source solution";
+
+equation
+
+  t = exp(time) - 1.0;
+  hRea =
+    AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Equivalent(
+    t=t,
+    aSoi=aSoi,
+    dis=dis,
+    wDis=wDis,
+    n_dis=n_dis,
+    len1=len1,
+    burDep1=burDep1,
+    len2=len2,
+    burDep2=burDep2,
+    nBor2=nBor2,
+    includeMirrorSource=false);
+  hMir =
+    AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Equivalent(
+    t=t,
+    aSoi=aSoi,
+    dis=dis,
+    wDis=wDis,
+    n_dis=n_dis,
+    len1=len1,
+    burDep1=burDep1,
+    len2=len2,
+    burDep2=burDep2,
+    nBor2=nBor2,
+    includeRealSource=false);
+  h =
+    AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Equivalent(
+    t=t,
+    aSoi=aSoi,
+    dis=dis,
+    wDis=wDis,
+    n_dis=n_dis,
+    len1=len1,
+    burDep1=burDep1,
+    len2=len2,
+    burDep2=burDep2,
+    nBor2=nBor2);
+
+  annotation (
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Equivalent.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=20.0),
+    Documentation(info="<html>
+<p>
+This example demonstrates the use of the function for the evaluation of the
+finite line source solution for equivalent boreholes. The solution is evaluated
+for the interactions between 3 interacting boreholes on a right triangle pattern
+with coordinates (x,y) = {(0,0), (0,7), (7,0)}.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FiniteLineSource_Equivalent;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Erfint.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Erfint.mo
index bc3f279e0d..fbf53fc731 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Erfint.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Erfint.mo
@@ -23,17 +23,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StartTime=0.0, StopTime=15.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the evaluation of the
- integral of the error function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the evaluation of the
+integral of the error function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FiniteLineSource_Erfint;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand.mo
index 1fab6f92cf..7e49fce12f 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand.mo
@@ -30,17 +30,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StartTime=0.01, StopTime=15.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the evaluation of the
- finite line source integrand function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the evaluation of the
+finite line source integrand function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FiniteLineSource_Integrand;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Equivalent.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Equivalent.mo
new file mode 100644
index 0000000000..db47313b4b
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Equivalent.mo
@@ -0,0 +1,85 @@
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation;
+model FiniteLineSource_Integrand_Equivalent
+  "Test case for finite line source integrand function for equivalent boreholes"
+  extends Modelica.Icons.Example;
+
+  parameter Modelica.Units.SI.ThermalDiffusivity aSoi=1.0e-6
+    "Ground thermal diffusivity";
+  parameter Modelica.Units.SI.Distance[2] dis={7.0, 7.0*sqrt(2)}
+    "Radial distance between borehole axes";
+  parameter Integer[2] wDis={4, 2}
+    "Number of occurences of each distance";
+  parameter Modelica.Units.SI.Height len1=150.0 "Length of emitting sources";
+  parameter Modelica.Units.SI.Height burDep1=4.0
+    "Buried depth of emitting sources";
+  parameter Modelica.Units.SI.Height len2=150.0 "Length of receiving lines";
+  parameter Modelica.Units.SI.Height burDep2=4.0
+    "Buried depth of receiving lines";
+  parameter Integer nBor2=3 "Number of receiving lines";
+  parameter Integer n_dis=2 "Number of unique distances";
+
+  Real u "Integration variable";
+  Real yRea "Finite line source integrand (Real part)";
+  Real yMir "Finite line source integrand (Mirror part)";
+  Real y "Finite line source integrand";
+
+equation
+  u = time;
+  yRea =
+    AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand_Equivalent(
+    u=u,
+    dis=dis,
+    wDis=wDis,
+    len1=len1,
+    burDep1=burDep1,
+    len2=len2,
+    burDep2=burDep2,
+    nBor2=nBor2,
+    n_dis=n_dis,
+    includeMirrorSource=false);
+  yMir =
+    AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand_Equivalent(
+    u=u,
+    dis=dis,
+    wDis=wDis,
+    len1=len1,
+    burDep1=burDep1,
+    len2=len2,
+    burDep2=burDep2,
+    nBor2=nBor2,
+    n_dis=n_dis,
+    includeRealSource=false);
+  y =
+    AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand_Equivalent(
+    u=u,
+    dis=dis,
+    wDis=wDis,
+    len1=len1,
+    burDep1=burDep1,
+    len2=len2,
+    burDep2=burDep2,
+    nBor2=nBor2,
+    n_dis=n_dis);
+
+  annotation (
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Equivalent.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StartTime=0.01, StopTime=1.0),
+    Documentation(info="<html>
+<p>
+This example demonstrates the use of the function for the evaluation of the
+finite line source integrand for equivalent boreholes. The solution is evaluated
+for the interactions between 3 interacting boreholes on a right triangle pattern
+with coordinates (x,y) = {(0,0), (0,7), (7,0)}.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FiniteLineSource_Integrand_Equivalent;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Length.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Length.mo
index 77696bb3df..1d5960f737 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Length.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Length.mo
@@ -67,17 +67,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StartTime=0.01, StopTime=500.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the evaluation of the
- finite line source integrand function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 15, 2019, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the evaluation of the
+finite line source integrand function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 15, 2019, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FiniteLineSource_Integrand_Length;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_SteadyState.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_SteadyState.mo
new file mode 100644
index 0000000000..82a363f2db
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_SteadyState.mo
@@ -0,0 +1,66 @@
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation;
+model FiniteLineSource_SteadyState
+  "Test case for steady-state solution of the finite line source"
+  extends Modelica.Icons.Example;
+
+  parameter Modelica.Units.SI.Height len1=150.0 "Length of emitting source";
+  parameter Modelica.Units.SI.Height burDep1=4.0
+    "Buried depth of emitting source";
+  parameter Modelica.Units.SI.Height len2=125.0
+    "Length of receiving line";
+  parameter Modelica.Units.SI.Height burDep2=3.5
+    "Buried depth of receiving line";
+
+  Modelica.Units.SI.Distance dis "Radial distance";
+  Real hRea "Finite line source solution (Real part)";
+  Real hMir "Finite line source solution (Mirror part)";
+  Real h "Finite line source solution";
+
+protected
+  constant Real uniCon(unit="m/s") = 1 "Constant to satisify unit check";
+equation
+
+  dis = 0.075 + uniCon*time;
+
+  hRea = AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_SteadyState(
+    dis = dis,
+    len1 = len1,
+    burDep1 = burDep1,
+    len2 = len2,
+    burDep2 = burDep2,
+    includeMirrorSource=false);
+  hMir = AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_SteadyState(
+    dis = dis,
+    len1 = len1,
+    burDep1 = burDep1,
+    len2 = len2,
+    burDep2 = burDep2,
+    includeRealSource=false);
+  h = AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_SteadyState(
+    dis = dis,
+    len1 = len1,
+    burDep1 = burDep1,
+    len2 = len2,
+    burDep2 = burDep2);
+
+  annotation (
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_SteadyState.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=50.0),
+    Documentation(info="<html>
+<p>
+This example demonstrates the use of the function for the evaluation of the
+steady-state finite line source solution. The solution is evaluated at different
+distances between the emitting and receiving boreholes.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FiniteLineSource_SteadyState;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_100boreholes.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_100boreholes.mo
index 67a97aecf3..fc2d9263e6 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_100boreholes.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_100boreholes.mo
@@ -22,6 +22,10 @@ model GFunction_100boreholes
   final parameter Modelica.Units.SI.Time[nTimTot] tGFun(each fixed=false);
   final parameter Real[nTimTot] dspline(each fixed=false);
 
+  parameter Integer nClu=5 "Number of clusters to be generated";
+  parameter Integer labels[nBor](each fixed=false) "Cluster label associated with each data point";
+  parameter Integer cluSiz[nClu](each fixed=false) "Size of the clusters";
+
   Real gFun_int "Interpolated value of g-function";
   Real lntts_int "Non-dimensional logarithmic time for interpolation";
 
@@ -35,6 +39,13 @@ model GFunction_100boreholes
 
 initial equation
   // Evaluate g-function for the specified bore field configuration
+  (labels, cluSiz) = AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.clusterBoreholes(
+    nBor = nBor,
+    cooBor = cooBor,
+    hBor = hBor,
+    dBor = dBor,
+    rBor = rBor,
+    nClu = nClu);
   (tGFun,gFun) =
     AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.gFunction(
       nBor = nBor,
@@ -46,7 +57,10 @@ initial equation
       nSeg = nSeg,
       nTimSho = nTimSho,
       nTimLon = nTimLon,
-      ttsMax = ttsMax);
+      ttsMax = ttsMax,
+      nClu = nClu,
+      labels = labels,
+      cluSiz = cluSiz);
   lntts = log(tGFun/ts .+ Modelica.Constants.small);
   // Initialize parameters for interpolation
   dspline = AixLib.Utilities.Math.Functions.splineDerivatives(
@@ -83,18 +97,23 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_100boreholes.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks the implementation of functions that evaluate the
- g-function of a borefield of 100 boreholes in a 10 by 10 configuration.
- </p>
- </html>",
+<p>
+This example checks the implementation of functions that evaluate the
+g-function of a borefield of 100 boreholes in a 10 by 10 configuration.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 20, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 9, 2022, by Massimo Cimmino:<br/>
+Added parameters to define the number of clusters for the method of Prieto and
+Cimmino (2021).
+</li>
+<li>
+March 20, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end GFunction_100boreholes;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_1borehole_5meters.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_1borehole_5meters.mo
index 6af34e42e4..b6a1026ff0 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_1borehole_5meters.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_1borehole_5meters.mo
@@ -22,6 +22,10 @@ model GFunction_1borehole_5meters
   final parameter Modelica.Units.SI.Time[nTimTot] tGFun(each fixed=false);
   final parameter Real[nTimTot] dspline(each fixed=false);
 
+  parameter Integer nClu=1 "Number of clusters to be generated";
+  parameter Integer labels[nBor](each fixed=false) "Cluster label associated with each data point";
+  parameter Integer cluSiz[nClu](each fixed=false) "Size of the clusters";
+
   Real gFun_int "Interpolated value of g-function";
   Real lntts_int "Non-dimensional logarithmic time for interpolation";
 
@@ -35,6 +39,13 @@ model GFunction_1borehole_5meters
 
 initial equation
   // Evaluate g-function for the specified bore field configuration
+  (labels, cluSiz) = AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.clusterBoreholes(
+    nBor = nBor,
+    cooBor = cooBor,
+    hBor = hBor,
+    dBor = dBor,
+    rBor = rBor,
+    nClu = nClu);
   (tGFun,gFun) =
     AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.gFunction(
       nBor = nBor,
@@ -46,7 +57,10 @@ initial equation
       nSeg = nSeg,
       nTimSho = nTimSho,
       nTimLon = nTimLon,
-      ttsMax = ttsMax);
+      ttsMax = ttsMax,
+      nClu = nClu,
+      labels = labels,
+      cluSiz = cluSiz);
   lntts = log(tGFun/ts .+ Modelica.Constants.small);
   // Initialize parameters for interpolation
   dspline = AixLib.Utilities.Math.Functions.splineDerivatives(
@@ -83,18 +97,23 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_1borehole_5meters.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks the implementation of functions that evaluate the
- g-function of a borefield of <i>100</i> boreholes in a <i>1</i> configuration.
- </p>
- </html>",
+<p>
+This example checks the implementation of functions that evaluate the
+g-function of a borefield of <i>100</i> boreholes in a <i>1</i> configuration.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 15, 2019, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 9, 2022, by Massimo Cimmino:<br/>
+Added parameters to define the number of clusters for the method of Prieto and
+Cimmino (2021).
+</li>
+<li>
+March 15, 2019, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end GFunction_1borehole_5meters;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_SmallScaleValidation.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_SmallScaleValidation.mo
index f6c6e36614..7b2b9db446 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_SmallScaleValidation.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_SmallScaleValidation.mo
@@ -31,6 +31,10 @@ model GFunction_SmallScaleValidation
   Real gFun_int "Interpolated value of g-function";
   Real lntts_int "Non-dimensional logarithmic time for interpolation";
 
+  parameter Integer nClu=1 "Number of clusters to be generated";
+  parameter Integer labels[nBor](each fixed=false) "Cluster label associated with each data point";
+  parameter Integer cluSiz[nClu](each fixed=false) "Size of the clusters";
+
   discrete Integer k "Current interpolation interval";
   discrete Modelica.Units.SI.Time t1 "Previous value of time for interpolation";
   discrete Modelica.Units.SI.Time t2 "Next value of time for interpolation";
@@ -41,6 +45,13 @@ model GFunction_SmallScaleValidation
 
 initial equation
   // Evaluate g-function for the specified bore field configuration
+  (labels, cluSiz) = AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.clusterBoreholes(
+    nBor = nBor,
+    cooBor = cooBor,
+    hBor = hBor,
+    dBor = dBor,
+    rBor = rBor,
+    nClu = nClu);
   (tGFun,gFun) =
     AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.gFunction(
       nBor = nBor,
@@ -52,7 +63,10 @@ initial equation
       nSeg = nSeg,
       nTimSho = nTimSho,
       nTimLon = nTimLon,
-      ttsMax = ttsMax);
+      ttsMax = ttsMax,
+      nClu = nClu,
+      labels = labels,
+      cluSiz = cluSiz);
   lntts = log(tGFun/ts .+ Modelica.Constants.small);
   // Initialize parameters for interpolation
   dspline = AixLib.Utilities.Math.Functions.splineDerivatives(
@@ -89,24 +103,29 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/GFunction_SmallScaleValidation.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks the implementation of functions that evaluate the
- g-function of the borehole used in the small-scale experiment of Cimmino and
- Bernier (2015).
- </p>
- <h4>References</h4>
- <p>
- Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
- g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
- </p>
- </html>",
+<p>
+This example checks the implementation of functions that evaluate the
+g-function of the borehole used in the small-scale experiment of Cimmino and
+Bernier (2015).
+</p>
+<h4>References</h4>
+<p>
+Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
+g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 9, 2022, by Massimo Cimmino:<br/>
+Added parameters to define the number of clusters for the method of Prieto and
+Cimmino (2021).
+</li>
+<li>
+July 18, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end GFunction_SmallScaleValidation;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/InfiniteLineSource.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/InfiniteLineSource.mo
index 1b28f71099..b0f5b98cf5 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/InfiniteLineSource.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/InfiniteLineSource.mo
@@ -24,17 +24,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=15.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for the evaluation of the
- infinite line source solution.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 12, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for the evaluation of the
+infinite line source solution.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 12, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InfiniteLineSource;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ShaGFunction.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ShaGFunction.mo
index fffc9902ac..91cbc8a4dd 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ShaGFunction.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ShaGFunction.mo
@@ -13,13 +13,14 @@ model ShaGFunction
     0.075,
     1e-6,
     12,
+    1,
     26,
     50,
     exp(5)) "SHA1-encrypted g-function inputs";
 
-  //Expected output (SHA1-encryption of (1,{{0,0}},150,4,0.075,1e-6,12,26,50,exp(5)))
+  //Expected output (SHA1-encryption of (1,{{0,0}},150,4,0.075,1e-6,12,1,26,50,exp(5)))
   parameter String strEx=
-    "f1213b0067741511110ed55c9689cd740f9d42ae"
+    "6dc3c2b9dfa5807ce25f7d34dc9e718a1119ce9f"
     "Expected string output";
 
   //Comparison result
@@ -32,17 +33,21 @@ annotation (experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ShaGFunction.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example uses a typical single borehole to test the SHA1-encryption of the
- arguments required to determine the borehole's thermal response factor.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example uses a typical single borehole to test the SHA1-encryption of the
+arguments required to determine the borehole's thermal response factor.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022, by Massimo Cimmino:<br/>
+Added number of clusters to the function call.
+</li>
+<li>
+July 18, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ShaGFunction;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/TimeGeometric.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/TimeGeometric.mo
index f2c1af07b0..7b95f64135 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/TimeGeometric.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/TimeGeometric.mo
@@ -22,17 +22,17 @@ initial equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=1.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the construction of vector of geometrically expanding
- time values.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the construction of vector of geometrically expanding
+time values.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TimeGeometric;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/package.order b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/package.order
index f9152733c5..3b389ae2f5 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/package.order
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/package.order
@@ -1,9 +1,13 @@
+ClusterBoreholes_100boreholes
 CylindricalHeatSource
 CylindricalHeatSource_Integrand
 FiniteLineSource
+FiniteLineSource_Equivalent
 FiniteLineSource_Erfint
 FiniteLineSource_Integrand
+FiniteLineSource_Integrand_Equivalent
 FiniteLineSource_Integrand_Length
+FiniteLineSource_SteadyState
 GFunction_100boreholes
 GFunction_1borehole_5meters
 GFunction_SmallScaleValidation
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/clusterBoreholes.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/clusterBoreholes.mo
new file mode 100644
index 0000000000..ec13adc49c
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/clusterBoreholes.mo
@@ -0,0 +1,118 @@
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors;
+impure function clusterBoreholes
+  "Identify clusters of boreholes with similar heat interactions"
+  extends Modelica.Icons.Function;
+
+  input Integer nBor "Number of boreholes";
+  input Modelica.Units.SI.Position cooBor[nBor, 2] "Coordinates of boreholes";
+  input Modelica.Units.SI.Height hBor "Borehole length";
+  input Modelica.Units.SI.Height dBor "Borehole buried depth";
+  input Modelica.Units.SI.Radius rBor "Borehole radius";
+  input Integer nClu "Number of clusters to be generated";
+  input Modelica.Units.SI.TemperatureDifference TTol = 0.001
+    "Absolute tolerance on the borehole wall temperature for the identification of clusters";
+
+  output Integer labels[nBor] "Cluster label associated with each data point";
+  output Integer cluSiz[nClu] "Size of the clusters";
+  output Integer N "Number of unique clusters";
+
+protected
+  Modelica.Units.SI.Temperature TBor[nBor,1] "Steady-state borehole wall temperatures";
+  Modelica.Units.SI.Temperature TBor_Unique[nBor] "Unique borehole wall temperatures under tolerance";
+  Modelica.Units.SI.Length dis "Distance between boreholes";
+
+algorithm
+  // ---- Evaluate borehole wall temperatures
+  for i in 1:nBor loop
+    TBor[i,1] := 0;
+    for j in 1:nBor loop
+      if i <> j then
+        dis := sqrt((cooBor[i,1]-cooBor[j,1])^2 + (cooBor[i,2]-cooBor[j,2])^2);
+      else
+        dis := rBor;
+      end if;
+      TBor[i,1] := TBor[i,1] + AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_SteadyState(dis, hBor, dBor, hBor, dBor);
+    end for;
+  end for;
+
+  // ---- Find all unique borehole wall temperatures under tolerance
+  // The number of clusters is min(N, nClu)
+  N := 1;
+  TBor_Unique[1] := TBor[1,1];
+  if nClu > 1 and nBor > 1 then
+    for i in 2:nBor loop
+      for j in 1:N loop
+        if abs(TBor[i,1] - TBor_Unique[j]) < TTol then
+          break;
+        elseif j == N then
+          TBor_Unique[N+1] := TBor[i,1];
+          N := N + 1;
+        end if;
+      end for;
+    end for;
+  end if;
+  N := min(N, nClu);
+
+  // ---- Identify borehole clusters
+  // This function is impure
+  (,labels,cluSiz) := AixLib.Utilities.Clustering.KMeans(
+    TBor,
+    N,
+    nBor,
+    1,
+    n_cluster_size=nClu);
+
+annotation (
+Inline=true,
+Documentation(info="<html>
+<p>
+This function identifies groups of similarly behaving boreholes using a
+<i>k</i>-means clustering algorithm. Boreholes are clustered based on their
+steady-state dimensionless borehole wall temperatures obtained from the spatial
+superposition of the steady-state finite line source solution (see
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_SteadyState\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_SteadyState</a>).
+</p>
+<h4>Implementation</h4>
+<p>
+The implemented method differs from the method presented by Prieto and Cimmino
+(2021). They used a hierarchical agglomerative clustering method with complete
+linkage to identify the borehole clusters. The <i>optimal</i> number of clusters
+was identified by cutting the dendrogram generated during the clustering
+process.
+</p>
+<p>
+Here, a <i>k</i>-means algorithm is used instead, using the euclidian distance
+between steady-state borehole wall temperatures. The number of clusters is a
+parameter in this approach. However, as observed by Prieto and Cimmino (2021),
+<code>nClu=5</code> clusters should provide acceptable accuracy in most
+practical cases. This number can be increased without significant change in the
+computational cost.
+</p>
+<h4>References</h4>
+<p>
+Prieto, C. and Cimmino, M. 2021. <i>Thermal interactions in large irregular
+fields of geothermal boreholes: the method of equivalent boreholes</i>. Journal
+of Building Performance Simulation 14(4): 446-460.
+<a href=\"https://doi.org/10.1080/19401493.2021.1968953\">
+doi:10.1080/19401493.2021.1968953</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 1, 2023, by Michael Wetter:<br/>
+Added <code>impure</code> declaration which is needed for compliance with the Modelica Language Specification,
+and is required by Optimica.
+</li>
+<li>
+February 1, 2023, by Michael Wetter:<br/>
+Added units.
+</li>
+<li>
+June 9, 2022 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end clusterBoreholes;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/cylindricalHeatSource.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/cylindricalHeatSource.mo
index 328f5b2752..e6416e852f 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/cylindricalHeatSource.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/cylindricalHeatSource.mo
@@ -26,42 +26,42 @@ algorithm
 annotation (
 Inline=true,
 Documentation(info="<html>
- <p>
- This function evaluates the cylindrical heat source solution. This solution
- gives the relation between the constant heat transfer rate (per unit length)
- injected by a cylindrical heat source of infinite length and the temperature
- raise in the medium. The cylindrical heat source solution is defined by
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/CylindricalHeatSource_01.png\" />
- </p>
- <p>
- where <i>&Delta;T(t,r)</i> is the temperature raise after a time <i>t</i> of
- constant heat injection and at a distance <i>r</i> from the cylindrical source,
- <i>Q'</i> is the heat injection rate per unit length, <i>k<sub>s</sub></i> is
- the soil thermal conductivity, <i>Fo</i> is the Fourier number,
- <i>aSoi<sub>s</sub></i> is the ground thermal diffusivity,
- <i>r<sub>b</sub></i> is the radius of the cylindrical source and <i>G</i>
- is the cylindrical heat source solution.
- </p>
- <p>
- The cylindrical heat source solution is given by:
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/CylindricalHeatSource_02.png\" />
- </p>
- <p>
- The integral is solved numerically, with the integrand defined in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource_Integrand\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource_Integrand</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 22, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function evaluates the cylindrical heat source solution. This solution
+gives the relation between the constant heat transfer rate (per unit length)
+injected by a cylindrical heat source of infinite length and the temperature
+raise in the medium. The cylindrical heat source solution is defined by
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/CylindricalHeatSource_01.png\" />
+</p>
+<p>
+where <i>&Delta;T(t,r)</i> is the temperature raise after a time <i>t</i> of
+constant heat injection and at a distance <i>r</i> from the cylindrical source,
+<i>Q'</i> is the heat injection rate per unit length, <i>k<sub>s</sub></i> is
+the soil thermal conductivity, <i>Fo</i> is the Fourier number,
+<i>aSoi<sub>s</sub></i> is the ground thermal diffusivity,
+<i>r<sub>b</sub></i> is the radius of the cylindrical source and <i>G</i>
+is the cylindrical heat source solution.
+</p>
+<p>
+The cylindrical heat source solution is given by:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/CylindricalHeatSource_02.png\" />
+</p>
+<p>
+The integral is solved numerically, with the integrand defined in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource_Integrand\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource_Integrand</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 22, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end cylindricalHeatSource;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/cylindricalHeatSource_Integrand.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/cylindricalHeatSource_Integrand.mo
index a58e4a8d82..7eebccb441 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/cylindricalHeatSource_Integrand.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/cylindricalHeatSource_Integrand.mo
@@ -18,18 +18,18 @@ algorithm
 annotation (
 Inline=true,
 Documentation(info="<html>
- <p>
- Integrand of the cylindrical heat source solution for use in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 22, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Integrand of the cylindrical heat source solution for use in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 22, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end cylindricalHeatSource_Integrand;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource.mo
index b7114fadaf..252c7bbd42 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource.mo
@@ -82,53 +82,53 @@ algorithm
 
 annotation (
 Documentation(info="<html>
- <p>
- This function evaluates the finite line source solution. This solution
- gives the relation between the constant heat transfer rate (per unit length)
- injected by a line source of finite length <i>H<sub>1</sub></i> buried at a
- distance <i>D<sub>1</sub></i> from a constant temperature surface
- (<i>T=0</i>) and the average temperature raise over a line of finite length
- <i>H<sub>2</sub></i> buried at a distance <i>D<sub>2</sub></i> from the constant
- temperature surface.
- The finite line source solution is defined by:
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_01.png\" />
- </p>
- <p>
- where <i>&Delta;T<sub>1-2</sub>(t,r,H<sub>1</sub>,D<sub>1</sub>,H<sub>2</sub>,D<sub>2</sub>)</i>
- is the temperature raise after a time <i>t</i> of constant heat injection and at
- a distance <i>r</i> from the line heat source, <i>Q'</i> is the heat injection
- rate per unit length, <i>k<sub>s</sub></i> is the soil thermal conductivity and
- <i>h<sub>FLS</sub></i> is the finite line source solution.
- </p>
- <p>
- The finite line source solution is given by:
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_02.png\" />
- </p>
- <p>
- where <i>&alpha;<sub>s</sub></i> is the ground thermal diffusivity and
- <i>erfint</i> is the integral of the error function, defined in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint\">AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_erfint</a>.
- The integral is solved numerically, with the integrand defined in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand\">AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 17, 2019, by Massimo Cimmino:<br/>
- Modified the upper bound of integration to avoid underestimating the value of
- the integral.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1107\">IBPSA, issue 1107</a>.
- </li>
- <li>
- March 22, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function evaluates the finite line source solution. This solution
+gives the relation between the constant heat transfer rate (per unit length)
+injected by a line source of finite length <i>H<sub>1</sub></i> buried at a
+distance <i>D<sub>1</sub></i> from a constant temperature surface
+(<i>T=0</i>) and the average temperature raise over a line of finite length
+<i>H<sub>2</sub></i> buried at a distance <i>D<sub>2</sub></i> from the constant
+temperature surface.
+The finite line source solution is defined by:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_01.png\" />
+</p>
+<p>
+where <i>&Delta;T<sub>1-2</sub>(t,r,H<sub>1</sub>,D<sub>1</sub>,H<sub>2</sub>,D<sub>2</sub>)</i>
+is the temperature raise after a time <i>t</i> of constant heat injection and at
+a distance <i>r</i> from the line heat source, <i>Q'</i> is the heat injection
+rate per unit length, <i>k<sub>s</sub></i> is the soil thermal conductivity and
+<i>h<sub>FLS</sub></i> is the finite line source solution.
+</p>
+<p>
+The finite line source solution is given by:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_02.png\" />
+</p>
+<p>
+where <i>&alpha;<sub>s</sub></i> is the ground thermal diffusivity and
+<i>erfint</i> is the integral of the error function, defined in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint\">AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_erfint</a>.
+The integral is solved numerically, with the integrand defined in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand\">AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 17, 2019, by Massimo Cimmino:<br/>
+Modified the upper bound of integration to avoid underestimating the value of
+the integral.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1107\">IBPSA, issue 1107</a>.
+</li>
+<li>
+March 22, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end finiteLineSource;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Equivalent.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Equivalent.mo
new file mode 100644
index 0000000000..08989a8797
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Equivalent.mo
@@ -0,0 +1,138 @@
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors;
+function finiteLineSource_Equivalent
+  "Finite line source solution of Prieto and Cimmino"
+  extends Modelica.Icons.Function;
+
+  input Modelica.Units.SI.Time t "Time";
+  input Modelica.Units.SI.ThermalDiffusivity aSoi "Ground thermal diffusivity";
+  input Modelica.Units.SI.Distance dis[n_dis] "Radial distance between borehole axes";
+  input Integer wDis[n_dis] "Number of occurences of each distance";
+  input Modelica.Units.SI.Height len1 "Length of emitting boreholes";
+  input Modelica.Units.SI.Height burDep1 "Buried depth of emitting boreholes";
+  input Modelica.Units.SI.Height len2 "Length of receiving boreholes";
+  input Modelica.Units.SI.Height burDep2 "Buried depth of receiving boreholes";
+  input Integer nBor2 "Number of receiving boreholes";
+  input Integer n_dis "Number of unique distances";
+  input Boolean includeRealSource = true "True if contribution of real source is included";
+  input Boolean includeMirrorSource = true "True if contribution of mirror source is included";
+
+  output Real h_21 "Thermal response factor of borehole 1 on borehole 2";
+
+protected
+  Real lowBou(unit="m-1") "Lower bound of integration";
+  // Upper bound is infinite
+  Real uppBou(unit="m-1") = max(100.0, 10.0/min(dis)) "Upper bound of integration";
+  Modelica.Units.SI.Distance disMin
+    "Minimum distance between sources and receiving line";
+  Modelica.Units.SI.Time timTre "Time treshold for evaluation of the solution";
+
+algorithm
+
+  h_21 := 0;
+  if t > 0 and (includeRealSource or includeMirrorSource) then
+    // Find the minimum distance between the line source and the line where the
+    // finite line source solution is evaluated.
+    if includeRealSource then
+      if (burDep2 + len2) < burDep1 then
+        disMin := sqrt(min(dis)^2 + (burDep1 - burDep2 - len2)^2);
+      elseif burDep2 > (burDep1 + len1) then
+        disMin := sqrt(min(dis)^2 + (burDep1 - burDep2 + len1)^2);
+      else
+        disMin := min(dis);
+      end if;
+    else
+      disMin := sqrt(min(dis)^2 + (burDep1 + burDep2)^2);
+    end if;
+    // The traveled distance of the temperature front is assumed to be:
+    // d = 5*sqrt(aSoi*t).
+    // The solution is only evaluated at times when the traveled distance is
+    // greater than the minimum distance.
+    timTre := disMin^2/(25*aSoi);
+
+    if t >= timTre then
+      lowBou := 1.0/sqrt(4*aSoi*t);
+      h_21 :=Modelica.Math.Nonlinear.quadratureLobatto(
+        function
+          AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand_Equivalent(
+          dis=dis,
+          wDis=wDis,
+          len1=len1,
+          burDep1=burDep1,
+          len2=len2,
+          burDep2=burDep2,
+          nBor2=nBor2,
+          n_dis=n_dis,
+          includeRealSource=includeRealSource,
+          includeMirrorSource=includeMirrorSource),
+        lowBou,
+        uppBou,
+        1.0e-6);
+    else
+      // Linearize the solution at times below the time treshold.
+      lowBou := 1.0/sqrt(4*aSoi*timTre);
+      h_21 :=t/timTre*Modelica.Math.Nonlinear.quadratureLobatto(
+        function
+          AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand_Equivalent(
+          dis=dis,
+          wDis=wDis,
+          len1=len1,
+          burDep1=burDep1,
+          len2=len2,
+          burDep2=burDep2,
+          nBor2=nBor2,
+          n_dis=n_dis,
+          includeRealSource=includeRealSource,
+          includeMirrorSource=includeMirrorSource),
+        lowBou,
+        uppBou,
+        1.0e-6);
+    end if;
+  end if;
+
+annotation (
+Documentation(info="<html>
+<p>
+This function evaluates the finite line source solution. This solution
+gives the relation between the constant heat transfer rate (per unit length)
+injected by a group of line sources of finite length <i>H<sub>1</sub></i> buried
+at a distance <i>D<sub>1</sub></i> from a constant temperature surface
+(<i>T=0</i>) and the average temperature raise over a group of
+<i>N<sub>2</sub></i> lines of finite length <i>H<sub>2</sub></i> buried at a
+distance <i>D<sub>2</sub></i> from the constant temperature surface.
+The finite line source solution is defined by:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_EquivalentBoreholes_01.png\" />
+</p>
+<p>
+where <i>&Delta;T<sub>1-2</sub>(t,r<sub>1->2</sub>,H<sub>1</sub>,D<sub>1</sub>,H<sub>2</sub>,D<sub>2</sub>,N<sub>2</sub>)</i>
+is the temperature raise over lines in group <i>2</i> after a time <i>t</i> of
+constant heat injection, <i>r<sub>1->2</sub></i> is the list of distance between
+all pairs of lines in groups <i>1</i> and <i>2</i>, <i>N<sub>1->2</sub></i> is
+the number of distances, <i>Q'</i> is the heat injection
+rate per unit length, <i>k<sub>s</sub></i> is the soil thermal conductivity and
+<i>h<sub>FLS</sub></i> is the finite line source solution.
+</p>
+<p>
+The finite line source solution is given by:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_EquivalentBoreholes_02.png\" />
+</p>
+<p>
+where <i>&alpha;<sub>s</sub></i> is the ground thermal diffusivity and
+<i>erfint</i> is the integral of the error function, defined in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint\">AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_erfint</a>.
+The integral is solved numerically, with the integrand defined in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand_Equivalent\">AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Integrand_Equivalent</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end finiteLineSource_Equivalent;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Erfint.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Erfint.mo
index 81ef68b7cb..1bd09d11a4 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Erfint.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Erfint.mo
@@ -8,19 +8,19 @@ algorithm
 annotation (
 Inline=true,
 Documentation(info="<html>
- <p>
- This function evaluates the integral of the error function, given by:
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/ErrorFunctionIntegral_01.png\" />
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 22, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function evaluates the integral of the error function, given by:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/ErrorFunctionIntegral_01.png\" />
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 22, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end finiteLineSource_Erfint;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Integrand.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Integrand.mo
index a063968d0f..25fe3af924 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Integrand.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Integrand.mo
@@ -46,22 +46,22 @@ algorithm
 
 annotation (
 Documentation(info="<html>
- <p>
- Integrand of the cylindrical heat source solution for use in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 23, 2018 by Michael Wetter:<br/>
- Reformulated function to use <code>sum</code>.
- </li>
- <li>
- March 22, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Integrand of the finite line source solution for use in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 23, 2018 by Michael Wetter:<br/>
+Reformulated function to use <code>sum</code>.
+</li>
+<li>
+March 22, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end finiteLineSource_Integrand;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Integrand_Equivalent.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Integrand_Equivalent.mo
new file mode 100644
index 0000000000..01b43c601e
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_Integrand_Equivalent.mo
@@ -0,0 +1,66 @@
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors;
+function finiteLineSource_Integrand_Equivalent
+  "Integrand function for finite line source evaluation"
+  extends Modelica.Icons.Function;
+
+  input Real u(unit="1/m") "Integration variable";
+  input Modelica.Units.SI.Distance dis[n_dis] "Radial distance between borehole axes";
+  input Integer wDis[n_dis];
+  input Modelica.Units.SI.Height len1 "Length of emitting boreholes";
+  input Modelica.Units.SI.Height burDep1 "Buried depth of emitting boreholes";
+  input Modelica.Units.SI.Height len2 "Length of receiving boreholes";
+  input Modelica.Units.SI.Height burDep2 "Buried depth of receiving boreholes";
+  input Integer nBor2 "Number of receiving boreholes over which the response is averaged";
+  input Integer n_dis "Number of unique distances between emitting and receiving boreholes";
+  input Boolean includeRealSource = true "true if contribution of real source is included";
+  input Boolean includeMirrorSource = true "true if contribution of mirror source is included";
+
+  output Real y(unit="m") "Value of integrand";
+
+protected
+  Real f "Intermediate variable";
+algorithm
+  if includeRealSource then
+    f := sum({
+      +AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint(
+       (burDep2 - burDep1 + len2)*u),
+      -AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint(
+       (burDep2 - burDep1)*u),
+      +AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint(
+       (burDep2 - burDep1 - len1)*u),
+      -AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint(
+       (burDep2 - burDep1 + len2 - len1)*u)});
+  else
+    f := 0;
+  end if;
+  if includeMirrorSource then
+    f := f + sum({
+      +AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint(
+      (burDep2 + burDep1 + len2)*u),
+      -AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint(
+      (burDep2 + burDep1)*u),
+      +AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint(
+      (burDep2 + burDep1 + len1)*u),
+      -AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Erfint(
+      (burDep2 + burDep1 + len2 + len1)*u)});
+  end if;
+
+  y := 0.5/(nBor2*len2*u^2)*f* (wDis*exp(-dis.*dis*u^2));
+
+annotation (
+Documentation(info="<html>
+<p>
+Integrand of the finite line source solution for use in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Equivalent\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Equivalent</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end finiteLineSource_Integrand_Equivalent;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_SteadyState.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_SteadyState.mo
new file mode 100644
index 0000000000..048a4e82a3
--- /dev/null
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/finiteLineSource_SteadyState.mo
@@ -0,0 +1,79 @@
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors;
+function finiteLineSource_SteadyState
+  "Steady-state finite line source solution"
+  extends Modelica.Icons.Function;
+
+  input Modelica.Units.SI.Distance dis "Radial distance between borehole axes";
+  input Modelica.Units.SI.Height len1 "Length of emitting borehole";
+  input Modelica.Units.SI.Height burDep1 "Buried depth of emitting borehole";
+  input Modelica.Units.SI.Height len2 "Length of receiving borehole";
+  input Modelica.Units.SI.Height burDep2 "Buried depth of receiving borehole";
+  input Boolean includeRealSource = true "True if contribution of real source is included";
+  input Boolean includeMirrorSource = true "True if contribution of mirror source is included";
+
+  output Real h_21 "Thermal response factor of borehole 1 on borehole 2";
+
+protected
+  Real f "Intermediate variable for FLS solution";
+  Real p[4] =  {1., -1., 1., -1.} "Intermediate variable for sum coefficients";
+  Real q[4] "Intermediate variable for axial distances";
+algorithm
+  if includeRealSource then
+    q := {burDep2 - burDep1 + len2,
+          burDep2 - burDep1,
+          burDep2 - burDep1 - len1,
+          burDep2 - burDep1 + len2 - len1};
+    f := p * (q .* log((q + sqrt(q.*q + ones(4)*dis^2)) / dis) - sqrt(q.*q + ones(4)*dis^2));
+  else
+    f := 0;
+  end if;
+  if includeMirrorSource then
+    q := {burDep2 + burDep1 + len2,
+          burDep2 + burDep1,
+          burDep2 + burDep1 + len1,
+          burDep2 + burDep1 + len2 + len1};
+    f := f + p * (q .* log((q + sqrt(q.*q + ones(4)*dis^2)) / dis) - sqrt(q.*q + ones(4)*dis^2));
+  end if;
+  h_21 := 0.5 * f / len2;
+
+annotation (
+Documentation(info="<html>
+<p>
+This function evaluates the steady-state value of finite line source solution.
+This solution gives the relation between the constant heat transfer rate (per
+unit length) injected by a line source of finite length <i>H<sub>1</sub></i>
+buried at a distance <i>D<sub>1</sub></i> from a constant temperature surface
+(<i>T=0</i>) and the average temperature raise over a line of finite length
+<i>H<sub>2</sub></i> buried at a distance <i>D<sub>2</sub></i> from the constant
+temperature surface.
+The finite line source solution is defined by:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_01.png\" />
+</p>
+<p>
+where <i>&Delta;T<sub>1-2</sub>(t,r,H<sub>1</sub>,D<sub>1</sub>,H<sub>2</sub>,D<sub>2</sub>)</i>
+is the temperature raise after a time <i>t</i> of constant heat injection and at
+a distance <i>r</i> from the line heat source, <i>Q'</i> is the heat injection
+rate per unit length, <i>k<sub>s</sub></i> is the soil thermal conductivity and
+<i>h<sub>FLS</sub></i> is the finite line source solution.
+</p>
+<p>
+The steady-state finite line source solution is given by:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_SteadyState_01.png\" />
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/FiniteLineSource_SteadyState_02.png\" />
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end finiteLineSource_SteadyState;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/gFunction.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/gFunction.mo
index 2a7bb3d0c1..68bc8f32b9 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/gFunction.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/gFunction.mo
@@ -1,5 +1,6 @@
 within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors;
-function gFunction "Evaluate the g-function of a bore field"
+function gFunction
+  "Evaluate the g-function of a bore field"
   extends Modelica.Icons.Function;
 
   input Integer nBor "Number of boreholes";
@@ -13,6 +14,9 @@ function gFunction "Evaluate the g-function of a bore field"
   input Integer nTimSho "Number of time steps in short time region";
   input Integer nTimLon "Number of time steps in long time region";
   input Real ttsMax "Maximum adimensional time for gfunc calculation";
+  input Integer nClu "Number of clusters";
+  input Integer labels[nBor] "Cluster label associated with each data point";
+  input Integer cluSiz[nClu] "Size of the clusters";
   input Real relTol = 0.02 "Relative tolerance on distance between boreholes";
 
   output Modelica.Units.SI.Time tGFun[nTimSho + nTimLon]
@@ -31,22 +35,60 @@ protected
   Modelica.Units.SI.Time tSho[nTimSho]
     "Time vector for short time calculations";
   Modelica.Units.SI.Time tLon[nTimLon] "Time vector for long time calculations";
-  Modelica.Units.SI.Distance dis "Separation distance between boreholes";
-  Modelica.Units.SI.Distance dis_mn "Separation distance for comparison";
+  Integer n_max = max(cluSiz.*cluSiz);
+  Modelica.Units.SI.Distance dis[nClu,nClu,n_max] "Separation distance between boreholes";
+  Modelica.Units.SI.Distance dis_ij "Separation distance between boreholes";
+  Integer wDis[nClu,nClu,n_max] "Number of occurence of separation distances";
+  Integer n_dis[nClu,nClu];
   Modelica.Units.SI.Radius rLin=0.0005*hBor
     "Radius for evaluation of same-borehole line source solutions";
   Real hSegRea[nSeg] "Real part of the FLS solution";
   Real hSegMir[2*nSeg-1] "Mirror part of the FLS solution";
   Modelica.Units.SI.Height dSeg "Buried depth of borehole segment";
-  Integer Done[nBor, nBor] "Matrix for tracking of FLS evaluations";
-  Real A[nSeg*nBor+1, nSeg*nBor+1] "Coefficient matrix for system of equations";
-  Real B[nSeg*nBor+1] "Coefficient vector for system of equations";
-  Real X[nSeg*nBor+1] "Solution vector for system of equations";
+  Real A[nSeg*nClu+1, nSeg*nClu+1] "Coefficient matrix for system of equations";
+  Real B[nSeg*nClu+1] "Coefficient vector for system of equations";
+  Real X[nSeg*nClu+1] "Solution vector for system of equations";
   Real FLS "Finite line source solution";
   Real ILS "Infinite line source solution";
   Real CHS "Cylindrical heat source solution";
+  Boolean found "Flag, true if a cluster has been found";
 
 algorithm
+  // Distances between borehole clusters
+  n_dis := zeros(nClu,nClu);
+  wDis := zeros(nClu,nClu,n_max);
+  for i in 1:nBor loop
+    for j in i:nBor loop
+      // Distance between boreholes
+      if i <> j then
+        dis_ij := sqrt((cooBor[i,1] - cooBor[j,1])^2 + (cooBor[i,2] - cooBor[j,2])^2);
+      else
+        dis_ij := rLin;
+      end if;
+      found := false;
+      for n in 1:n_dis[labels[i],labels[j]] loop
+        if abs(dis_ij - dis[labels[i],labels[j],n]) / dis[labels[i],labels[j],n] < relTol then
+          wDis[labels[i],labels[j],n] := wDis[labels[i],labels[j],n] + 1;
+          found := true;
+          if i <> j then
+            wDis[labels[j],labels[i],n] := wDis[labels[j],labels[i],n] + 1;
+          end if;
+          break;
+        end if;
+      end for;
+      if not found then
+        n_dis[labels[i],labels[j]] := n_dis[labels[i],labels[j]] + 1;
+        wDis[labels[i],labels[j],n_dis[labels[i],labels[j]]] := wDis[labels[i],labels[j],n_dis[labels[i],labels[j]]] + 1;
+        dis[labels[i],labels[j],n_dis[labels[i],labels[j]]] := dis_ij;
+        if i <> j then
+          n_dis[labels[j],labels[i]] := n_dis[labels[j],labels[i]] + 1;
+          wDis[labels[j],labels[i],n_dis[labels[j],labels[i]]] := wDis[labels[j],labels[i],n_dis[labels[j],labels[i]]] + 1;
+          dis[labels[j],labels[i],n_dis[labels[j],labels[i]]] := dis_ij;
+        end if;
+      end if;
+    end for;
+  end for;
+
   // Generate geometrically expanding time vectors
   tSho :=
     AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.timeGeometric(
@@ -93,87 +135,68 @@ algorithm
   // Long time calculations
   // ----------------------
   // Initialize coefficient matrix A
-  for m in 1:nBor loop
+  for m in 1:nClu loop
     for u in 1:nSeg loop
       // Tb coefficient in spatial superposition equations
-      A[(m-1)*nSeg+u,nBor*nSeg+1] := -1;
+      A[(m-1)*nSeg+u,nClu*nSeg+1] := -1;
       // Q coefficient in heat balance equation
-      A[nBor*nSeg+1,(m-1)*nSeg+u] := 1;
+      A[nClu*nSeg+1,(m-1)*nSeg+u] := cluSiz[m];
     end for;
   end for;
   // Initialize coefficient vector B
   // The total heat extraction rate is constant
-  B[nBor*nSeg+1] := nBor*nSeg;
+  B[nClu*nSeg+1] := nBor*nSeg;
 
   // Evaluate thermal response matrix at all times
   for k in 1:nTimLon-1 loop
-    for i in 1:nBor loop
-      for j in i:nBor loop
-        // Distance between boreholes
-        if i == j then
-          // If same borehole, distance is the radius
-          dis := rLin;
-        else
-          dis := sqrt((cooBor[i,1] - cooBor[j,1])^2 + (cooBor[i,2] - cooBor[j,2])^2);
-        end if;
-        // Only evaluate the thermal response factors if not already evaluated
-        if Done[i,j] < k then
-          // Evaluate Real and Mirror parts of FLS solution
-          // Real part
-          for m in 1:nSeg loop
-            hSegRea[m] :=
-              AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource(
+    for i in 1:nClu loop
+      for j in i:nClu loop
+        // Evaluate Real and Mirror parts of FLS solution
+        // Real part
+        for m in 1:nSeg loop
+          hSegRea[m] :=
+            AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Equivalent(
               tLon[k + 1],
               aSoi,
-              dis,
+              dis[i,j,1:n_dis[i,j]],
+              wDis[i,j,1:n_dis[i,j]],
               hBor/nSeg,
               dBor,
               hBor/nSeg,
               dBor + (m - 1)*hBor/nSeg,
+              cluSiz[i],
+              n_dis[i,j],
               includeMirrorSource=false);
-          end for;
+        end for;
         // Mirror part
-          for m in 1:(2*nSeg-1) loop
-            hSegMir[m] :=
-              AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource(
+        for m in 1:(2*nSeg-1) loop
+          hSegMir[m] :=
+            AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource_Equivalent(
               tLon[k + 1],
               aSoi,
-              dis,
+              dis[i,j,1:n_dis[i,j]],
+              wDis[i,j,1:n_dis[i,j]],
               hBor/nSeg,
               dBor,
               hBor/nSeg,
               dBor + (m - 1)*hBor/nSeg,
+              cluSiz[i],
+              n_dis[i,j],
               includeRealSource=false);
+        end for;
+        // Add thermal response factor to coefficient matrix A
+        for u in 1:nSeg loop
+          for v in 1:nSeg loop
+            A[(i-1)*nSeg+u,(j-1)*nSeg+v] := hSegRea[abs(u-v)+1] + hSegMir[u+v-1];
+            A[(j-1)*nSeg+v,(i-1)*nSeg+u] := (hSegRea[abs(u-v)+1] + hSegMir[u+v-1]) * cluSiz[i] / cluSiz[j];
           end for;
-        // Apply to all pairs that have the same separation distance
-          for m in 1:nBor loop
-            for n in m:nBor loop
-              if m == n then
-                dis_mn := rLin;
-              else
-                dis_mn := sqrt((cooBor[m,1] - cooBor[n,1])^2 + (cooBor[m,2] - cooBor[n,2])^2);
-              end if;
-              if abs(dis_mn - dis) < relTol*dis then
-                // Add thermal response factor to coefficient matrix A
-                for u in 1:nSeg loop
-                  for v in 1:nSeg loop
-                    A[(m-1)*nSeg+u,(n-1)*nSeg+v] := hSegRea[abs(u-v)+1] + hSegMir[u+v-1];
-                    A[(n-1)*nSeg+v,(m-1)*nSeg+u] := hSegRea[abs(u-v)+1] + hSegMir[u+v-1];
-                  end for;
-                end for;
-                // Mark current pair as evaluated
-                Done[m,n] := k;
-                Done[n,m] := k;
-              end if;
-            end for;
-          end for;
-        end if;
+        end for;
       end for;
     end for;
     // Solve the system of equations
     X := Modelica.Math.Matrices.solve(A,B);
     // The g-function is equal to the borehole wall temperature
-    g[nTimSho+k+1] := X[nBor*nSeg+1];
+    g[nTimSho+k+1] := X[nClu*nSeg+1];
   end for;
   // Correct finite line source solution for cylindrical geometry
   for k in 2:nTimLon loop
@@ -195,95 +218,116 @@ algorithm
 
 annotation (
 Documentation(info="<html>
- <p>
- This function implements the <i>g</i>-function evaluation method introduced by
- Cimmino and Bernier (see: Cimmino and Bernier (2014), and Cimmino (2018)) based
- on the <i>g</i>-function function concept first introduced by Eskilson (1987).
- The <i>g</i>-function gives the relation between the variation of the borehole
- wall temperature at a time <i>t</i> and the heat extraction and injection rates
- at all times preceding time <i>t</i> as
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/GFunction_01.png\" />
- </p>
- <p>
- where <i>T<sub>b</sub></i> is the borehole wall temperature,
- <i>T<sub>g</sub></i> is the undisturbed ground temperature, <i>Q</i> is the
- heat injection rate into the ground through the borehole wall per unit borehole
- length, <i>k<sub>s</sub></i> is the soil thermal conductivity and <i>g</i> is
- the <i>g</i>-function.
- </p>
- <p>
- The <i>g</i>-function is constructed from the combination of the combination of
- the finite line source (FLS) solution (see
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource</a>),
- the cylindrical heat source (CHS) solution (see
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource</a>),
- and the infinite line source (ILS) solution (see
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.infiniteLineSource\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.infiniteLineSource</a>).
- To obtain the <i>g</i>-function of a bore field, each borehole is divided into a
- series of <code>nSeg</code> segments of equal length, each modeled as a line
- source of finite length. The finite line source solution is superimposed in
- space to obtain a system of equations that gives the relation between the heat
- injection rate at each of the segments and the borehole wall temperature at each
- of the segments. The system is solved to obtain the uniform borehole wall
- temperature required at any time to maintain a constant total heat injection
- rate (<i>Q<sub>tot</sub> = 2&pi;k<sub>s</sub>H<sub>tot</sub>)</i> into the bore
- field. The uniform borehole wall temperature is then equal to the finite line
- source based <i>g</i>-function.
- </p>
- <p>
- Since this <i>g</i>-function is based on line sources of heat, rather than
- cylinders, the <i>g</i>-function is corrected to consider the cylindrical
- geometry. The correction factor is then the difference between the cylindrical
- heat source solution and the infinite line source solution, as proposed by
- Li et al. (2014) as
- </p>
- <p align=\"center\">
- <i>g(t) = g<sub>FLS</sub> + (g<sub>CHS</sub> - g<sub>ILS</sub>)</i>
- </p>
- <h4>Implementation</h4>
- <p>
- The calculation of the <i>g</i>-function is separated into two regions: the
- short-time region and the long-time region. In the short-time region,
- corresponding to times <i>t</i> &lt; 1 hour, heat interaction between boreholes
- and axial variations of heat injection rate are not considered. The
- <i>g</i>-function is calculated using only one borehole and one segment. In the
- long-time region, corresponding to times <i>t</i> &gt; 1 hour, all boreholes
- are represented as series of <code>nSeg</code> line segments and the
- <i>g</i>-function is evaluated as described above.
- </p>
- <h4>References</h4>
- <p>
- Cimmino, M. and Bernier, M. 2014. <i>A semi-analytical method to generate
- g-functions for geothermal bore fields</i>. International Journal of Heat and
- Mass Transfer 70: 641-650.
- </p>
- <p>
- Cimmino, M. 2018. <i>Fast calculation of the g-functions of geothermal borehole
- fields using similarities in the evaluation of the finite line source
- solution</i>. Journal of Building Performance Simulation. DOI:
- 10.1080/19401493.2017.1423390.
- </p>
- <p>
- Eskilson, P. 1987. <i>Thermal analysis of heat extraction boreholes</i>. Ph.D.
- Thesis. Department of Mathematical Physics. University of Lund. Sweden.
- </p>
- <p>
- Li, M., Li, P., Chan, V. and Lai, A.C.K. 2014. <i>Full-scale temperature
- response function (G-function) for heat transfer by borehole heat exchangers
- (GHEs) from sub-hour to decades</i>. Applied Energy 136: 197-205.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 22, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function implements the <i>g</i>-function evaluation method introduced by
+Cimmino and Bernier (see: Cimmino and Bernier (2014), Cimmino (2018), and Prieto
+and Cimmino (2021)) based on the <i>g</i>-function function concept first
+introduced by Eskilson (1987).
+The <i>g</i>-function gives the relation between the variation of the borehole
+wall temperature at a time <i>t</i> and the heat extraction and injection rates
+at all times preceding time <i>t</i> as
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/GFunction_01.png\" />
+</p>
+<p>
+where <i>T<sub>b</sub></i> is the borehole wall temperature,
+<i>T<sub>g</sub></i> is the undisturbed ground temperature, <i>Q</i> is the
+heat injection rate into the ground through the borehole wall per unit borehole
+length, <i>k<sub>s</sub></i> is the soil thermal conductivity and <i>g</i> is
+the <i>g</i>-function.
+</p>
+<p>
+The <i>g</i>-function is constructed from the combination of the combination of
+the finite line source (FLS) solution (see
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.finiteLineSource</a>),
+the cylindrical heat source (CHS) solution (see
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.cylindricalHeatSource</a>),
+and the infinite line source (ILS) solution (see
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.infiniteLineSource\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.infiniteLineSource</a>).
+To obtain the <i>g</i>-function of a bore field, the bore field is first divided
+into <code>nClu</code> groups of similarly behaving boreholes. Each group
+is represented by a single <i>equivalent</i> borehole. Each equivalent borehole
+is then divided into a series of <code>nSeg</code> segments of equal length,
+each modeled as a line source of finite length. The finite line source solution
+is superimposed in space to obtain a system of equations that gives the relation
+between the heat injection rate at each of the segments and the borehole wall
+temperature at each of the segments. The system is solved to obtain the uniform
+borehole wall temperature required at any time to maintain a constant total heat
+injection rate (<i>Q<sub>tot</sub> = 2&pi;k<sub>s</sub>H<sub>tot</sub>)</i> into
+the bore field. The uniform borehole wall temperature is then equal to the
+finite line source based <i>g</i>-function.
+</p>
+<p>
+Since this <i>g</i>-function is based on line sources of heat, rather than
+cylinders, the <i>g</i>-function is corrected to consider the cylindrical
+geometry. The correction factor is then the difference between the cylindrical
+heat source solution and the infinite line source solution, as proposed by
+Li et al. (2014) as
+</p>
+<p align=\"center\">
+<i>g(t) = g<sub>FLS</sub> + (g<sub>CHS</sub> - g<sub>ILS</sub>)</i>
+</p>
+<h4>Implementation</h4>
+<p>
+The calculation of the <i>g</i>-function is separated into two regions: the
+short-time region and the long-time region. In the short-time region,
+corresponding to times <i>t</i> &lt; 1 hour, heat interaction between boreholes
+and axial variations of heat injection rate are not considered. The
+<i>g</i>-function is calculated using only one borehole and one segment. In the
+long-time region, corresponding to times <i>t</i> &gt; 1 hour, all boreholes
+are represented as series of <code>nSeg</code> line segments and the
+<i>g</i>-function is evaluated as described above.
+</p>
+<h4>References</h4>
+<p>
+Cimmino, M. and Bernier, M. 2014. <i>A semi-analytical method to generate
+g-functions for geothermal bore fields</i>. International Journal of Heat and
+Mass Transfer 70: 641-650.
+</p>
+<p>
+Cimmino, M. 2018. <i>Fast calculation of the g-functions of geothermal borehole
+fields using similarities in the evaluation of the finite line source
+solution</i>. Journal of Building Performance Simulation 11(6): 655-668.
+</p>
+<p>
+Eskilson, P. 1987. <i>Thermal analysis of heat extraction boreholes</i>. Ph.D.
+Thesis. Department of Mathematical Physics. University of Lund. Sweden.
+</p>
+<p>
+Li, M., Li, P., Chan, V. and Lai, A.C.K. 2014. <i>Full-scale temperature
+response function (G-function) for heat transfer by borehole heat exchangers
+(GHEs) from sub-hour to decades</i>. Applied Energy 136: 197-205.
+</p>
+<p>
+Prieto, C. and Cimmino, M. 2021. <i>Thermal interactions in large irregular
+fields of geothermal boreholes: the method of equivalent boreholes</i>. Journal
+of Building Performance Simulation 14(4): 446-460.
+<a href=\"https://doi.org/10.1080/19401493.2021.1968953\">
+doi:10.1080/19401493.2021.1968953</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022 by Massimo Cimmino:<br/>
+Updated the function to use the more efficient method of Prieto and Cimmino
+(2021).
+</li>
+<li>
+November 16, 2022, by Michael Wetter:<br/>
+Initialized variable <code>Done</code>.<br/>
+See
+<a href=\"https://github.com/OpenModelica/OpenModelica/issues/9707#issuecomment-1317631281\">
+OpenModelica, #9707</a>.
+</li>
+<li>
+March 22, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end gFunction;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/infiniteLineSource.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/infiniteLineSource.mo
index e711e6c261..157fe82880 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/infiniteLineSource.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/infiniteLineSource.mo
@@ -17,40 +17,40 @@ algorithm
 annotation (
 Inline=true,
 Documentation(info="<html>
- <p>
- This function evaluates the infinite line source solution. This solution gives
- the relation between the constant heat transfer rate (per unit length) injected
- by a line heat source of infinite length and the temperature raise in the
- medium. The infinite line source solution is defined by
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/InfiniteLineSource_01.png\" />
- </p>
- <p>
- where <i>&Delta;T(t,r)</i> is the temperature raise after a time <i>t</i> of
- constant heat injection and at a distance <i>r</i> from the line source,
- <i>Q'</i> is the heat injection rate per unit length, <i>k<sub>s</sub></i> is
- the soil thermal conductivity and <i>h<sub>ILS</sub></i> is the infinite line
- source solution.
- </p>
- <p>
- The infinite line source solution is given by the exponential integral
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/InfiniteLineSource_02.png\" />
- </p>
- <p>
- where <i>&alpha;<sub>s</sub></i> is the ground thermal diffusivity. The
- exponential integral is implemented in
- <a href=\"modelica://AixLib.Utilities.Math.Functions.exponentialIntegralE1\">AixLib.Utilities.Math.Functions.exponentialIntegralE1</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 22, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function evaluates the infinite line source solution. This solution gives
+the relation between the constant heat transfer rate (per unit length) injected
+by a line heat source of infinite length and the temperature raise in the
+medium. The infinite line source solution is defined by
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/InfiniteLineSource_01.png\" />
+</p>
+<p>
+where <i>&Delta;T(t,r)</i> is the temperature raise after a time <i>t</i> of
+constant heat injection and at a distance <i>r</i> from the line source,
+<i>Q'</i> is the heat injection rate per unit length, <i>k<sub>s</sub></i> is
+the soil thermal conductivity and <i>h<sub>ILS</sub></i> is the infinite line
+source solution.
+</p>
+<p>
+The infinite line source solution is given by the exponential integral
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Geothermal/Borefields/InfiniteLineSource_02.png\" />
+</p>
+<p>
+where <i>&alpha;<sub>s</sub></i> is the ground thermal diffusivity. The
+exponential integral is implemented in
+<a href=\"modelica://AixLib.Utilities.Math.Functions.exponentialIntegralE1\">AixLib.Utilities.Math.Functions.exponentialIntegralE1</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 22, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end infiniteLineSource;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/package.order b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/package.order
index b60af0e8a5..5d99433ff2 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/package.order
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/package.order
@@ -1,8 +1,12 @@
+clusterBoreholes
 cylindricalHeatSource
 cylindricalHeatSource_Integrand
 finiteLineSource
+finiteLineSource_Equivalent
 finiteLineSource_Erfint
 finiteLineSource_Integrand
+finiteLineSource_Integrand_Equivalent
+finiteLineSource_SteadyState
 gFunction
 infiniteLineSource
 shaGFunction
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/shaGFunction.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/shaGFunction.mo
index 7c9934fe82..4c115da05c 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/shaGFunction.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/shaGFunction.mo
@@ -10,6 +10,7 @@ function shaGFunction
   input Modelica.Units.SI.ThermalDiffusivity aSoi
     "Ground thermal diffusivity used in g-function evaluation";
   input Integer nSeg "Number of line source segments per borehole";
+  input Integer nClu "Number of clusters for g-function calculation";
   input Integer nTimSho "Number of time steps in short time region";
   input Integer nTimLon "Number of time steps in long time region";
   input Real ttsMax "Maximum adimensional time for gfunc calculation";
@@ -27,6 +28,7 @@ algorithm
   sha := AixLib.Utilities.Cryptographics.sha(sha + String(rBor, format=formatStrGen));
   sha := AixLib.Utilities.Cryptographics.sha(sha + String(aSoi, format=formatStrGen));
   sha := AixLib.Utilities.Cryptographics.sha(sha + String(nSeg, format=formatStrGen));
+  sha := AixLib.Utilities.Cryptographics.sha(sha + String(nClu, format=formatStrGen));
   sha := AixLib.Utilities.Cryptographics.sha(sha + String(nTimSho, format=formatStrGen));
   sha := AixLib.Utilities.Cryptographics.sha(sha + String(nTimLon, format=formatStrGen));
   sha := AixLib.Utilities.Cryptographics.sha(sha + String(ttsMax, format=formatStrGen));
@@ -38,43 +40,47 @@ algorithm
 annotation (
 Inline=false,
 Documentation(info="<html>
- <p>
- This function returns the SHA1 encryption of its arguments.
- </p>
- <h4>Implementation</h4>
- <p>
- Each argument is formatted in exponential notation
- with four significant digits, for example <code>1.234e+001</code>, with no spaces or
- other separating characters between each argument value.
- To prevent too long strings that can cause buffer overflows,
- the sha encoding of each argument is computed and added to the next string that
- is parsed.
- </p>
- <p>
- The SHA1 encryption is computed using
- <a href=\"modelica://AixLib.Utilities.Cryptographics.sha\">AixLib.Utilities.Cryptographics.sha</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 1, 2019 by Michael Wetter:<br/>
- Declared string as a constant due to JModelica's tigther type checking.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1230\">#1230</a>.
- </li>
- <li>
- September 11, 2018, by Michael Wetter:<br/>
- Refactored implementation to avoid buffer overflow.
- </li>
- <li>
- September 11, 2018 by Damien Picard:<br/>
- Split long strings into small strings to avoid buffer overflow.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1018\">#1018</a>.
- </li>
- <li>
- June 22, 2018 by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function returns the SHA1 encryption of its arguments.
+</p>
+<h4>Implementation</h4>
+<p>
+Each argument is formatted in exponential notation
+with four significant digits, for example <code>1.234e+001</code>, with no spaces or
+other separating characters between each argument value.
+To prevent too long strings that can cause buffer overflows,
+the sha encoding of each argument is computed and added to the next string that
+is parsed.
+</p>
+<p>
+The SHA1 encryption is computed using
+<a href=\"modelica://AixLib.Utilities.Cryptographics.sha\">AixLib.Utilities.Cryptographics.sha</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 9, 2022, by Massimo Cimmino:<br/>
+Added the number of clusters to the encryption.
+</li>
+<li>
+November 1, 2019 by Michael Wetter:<br/>
+Declared string as a constant due to JModelica's tigther type checking.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1230\">#1230</a>.
+</li>
+<li>
+September 11, 2018, by Michael Wetter:<br/>
+Refactored implementation to avoid buffer overflow.
+</li>
+<li>
+September 11, 2018 by Damien Picard:<br/>
+Split long strings into small strings to avoid buffer overflow.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1018\">#1018</a>.
+</li>
+<li>
+June 22, 2018 by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end shaGFunction;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/timeGeometric.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/timeGeometric.mo
index 5ac408e6d6..19dbea9261 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/timeGeometric.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/timeGeometric.mo
@@ -37,32 +37,32 @@ algorithm
   end if;
 annotation (
 Documentation(info="<html>
- <p>
- This function attemps to build a vector of length <code>nTim</code> with a geometric
- expansion of the time variable between <code>dt</code> and <code>t_max</code>.
- </p>
- <p>
- If <code>t_max &gt; nTim*dt</code>, then a geometrically expanding vector is built as
- </p>
- <p align=\"center\">
- <i>t = [dt, dt*(1-r<sup>2</sup>)/(1-r), ... , dt*(1-r<sup>n</sup>)/(1-r), ... , t<sub>max</sub>],</i>
- </p>
- <p>
- where <i>r</i> is the geometric expansion factor.
- </p>
- <p>
- If <code>t_max &lt; nTim*dt</code>, then a linearly expanding vector is built as
- </p>
- <p align=\"center\">
- <i>t = [dt, 2*dt, ... , n*dt, ... , <code>nTim</code>*dt]</i>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 28, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function attemps to build a vector of length <code>nTim</code> with a geometric
+expansion of the time variable between <code>dt</code> and <code>t_max</code>.
+</p>
+<p>
+If <code>t_max &gt; nTim*dt</code>, then a geometrically expanding vector is built as
+</p>
+<p align=\"center\">
+<i>t = [dt, dt*(1-r<sup>2</sup>)/(1-r), ... , dt*(1-r<sup>n</sup>)/(1-r), ... , t<sub>max</sub>],</i>
+</p>
+<p>
+where <i>r</i> is the geometric expansion factor.
+</p>
+<p>
+If <code>t_max &lt; nTim*dt</code>, then a linearly expanding vector is built as
+</p>
+<p align=\"center\">
+<i>t = [dt, 2*dt, ... , n*dt, ... , <code>nTim</code>*dt]</i>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 28, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end timeGeometric;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Analytic_20Years.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Analytic_20Years.mo
index 3b0f8965c2..31d9d270eb 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Analytic_20Years.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Analytic_20Years.mo
@@ -1,4 +1,4 @@
-within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Validation;
+within AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Validation;
 model Analytic_20Years
   "Long term validation of ground temperature response model"
   extends Modelica.Icons.Example;
@@ -32,6 +32,7 @@ model Analytic_20Years
   AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse groTemRes(
     tLoaAgg=3600,
     nCel=5,
+    nSeg=12,
     borFieDat=borFieDat,
     forceGFunCalc=true) "Ground temperature response of borehole"
     annotation (Placement(transformation(extent={{-40,40},{-20,60}})));
@@ -91,30 +92,30 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Analytic_20Years.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This validation case applies the asymetrical synthetic load profile developed
- by Pinel (2003) over a 20 year period by directly injecting the heat at the
- borehole wall in the ground temperature response model. The difference between
- the resulting borehole wall temperature and the same temperature precalculated
- by using a fast Fourier transform is calculated with the <code>add</code>
- component. The fast Fourier transform calculation was done using the same
- g-function as was calculated by
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.gFunction\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.gFunction</a>.
- </p>
- <h4>References</h4>
- <p>
- Pinel, P. 2003. <i>Am&eacute;lioration, validation et implantation d’un algorithme de calcul
- pour &eacute;valuer le transfert thermique dans les puits verticaux de syst&egrave;mes de pompes &agrave; chaleur g&eacute;othermiques</i>,
- M.A.Sc. Thesis, &Eacute;cole Polytechnique de Montréal.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 5, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case applies the asymetrical synthetic load profile developed
+by Pinel (2003) over a 20 year period by directly injecting the heat at the
+borehole wall in the ground temperature response model. The difference between
+the resulting borehole wall temperature and the same temperature precalculated
+by using a fast Fourier transform is calculated with the <code>add</code>
+component. The fast Fourier transform calculation was done using the same
+g-function as was calculated by
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.gFunction\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.gFunction</a>.
+</p>
+<h4>References</h4>
+<p>
+Pinel, P. 2003. <i>Am&eacute;lioration, validation et implantation d&#8217;un algorithme de calcul
+pour &eacute;valuer le transfert thermique dans les puits verticaux de syst&egrave;mes de pompes &agrave; chaleur g&eacute;othermiques</i>,
+M.A.Sc. Thesis, &Eacute;cole Polytechnique de Montr&eacute;al.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 5, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Analytic_20Years;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Borefield.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Borefield.mo
index 52c8d70f07..e3e5e9a18d 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Borefield.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Borefield.mo
@@ -12,28 +12,28 @@ record SmallScale_Borefield
   defaultComponentName="borFieDat",
 Documentation(
 info="<html>
- <p>
- This record contains the borefield data of the Cimmino and
- Bernier (2015) experiment.
- </p>
- <h4>References</h4>
- <p>
- Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
- g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
- </p>
- </html>",
+<p>
+This record contains the borefield data of the Cimmino and
+Bernier (2015) experiment.
+</p>
+<h4>References</h4>
+<p>
+Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
+g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmallScale_Borefield;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Configuration.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Configuration.mo
index 3df2ff9f0d..5bc935fcdf 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Configuration.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Configuration.mo
@@ -21,30 +21,30 @@ defaultComponentPrefixes="parameter",
 defaultComponentName="conDat",
 Documentation(
 info="<html>
- <p>
- This record contains the configuration data of the Cimmino and
- Bernier (2015) experiment. Since the model is not adapted to the simulation of
- small scale boreholes, the borehole dimensions are multiplied by a factor 375
- to obtain a scaled-up 150.0 m long borehole.
- </p>
- <h4>References</h4>
- <p>
- Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
- g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
- </p>
- </html>",
+<p>
+This record contains the configuration data of the Cimmino and
+Bernier (2015) experiment. Since the model is not adapted to the simulation of
+small scale boreholes, the borehole dimensions are multiplied by a factor 375
+to obtain a scaled-up 150.0 m long borehole.
+</p>
+<h4>References</h4>
+<p>
+Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
+g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmallScale_Configuration;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Filling.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Filling.mo
index ad641756fa..4965cbf27a 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Filling.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Filling.mo
@@ -11,26 +11,26 @@ record SmallScale_Filling
   defaultComponentName="filDat",
 Documentation(
 info="<html>
- <p>This record contains the filling data of the Cimmino and
- Bernier (2015) experiment.</p>
- <h4>References</h4>
- <p>
- Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
- g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
- </p>
- </html>",
+<p>This record contains the filling data of the Cimmino and
+Bernier (2015) experiment.</p>
+<h4>References</h4>
+<p>
+Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
+g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmallScale_Filling;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Soil.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Soil.mo
index d6b69b8163..0b933ba4a0 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Soil.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/BaseClasses/SmallScale_Soil.mo
@@ -11,27 +11,27 @@ record SmallScale_Soil
   defaultComponentName="soiDat",
 Documentation(
 info="<html>
- <p>
- This record contains the soil data of the Cimmino and Bernier (2015) experiment.
- </p>
- <h4>References</h4>
- <p>
- Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
- g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
- </p>
- </html>",
+<p>
+This record contains the soil data of the Cimmino and Bernier (2015) experiment.
+</p>
+<h4>References</h4>
+<p>
+Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
+g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmallScale_Soil;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Cylindrical.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Cylindrical.mo
index bbe27d752f..b536d31e61 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Cylindrical.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Cylindrical.mo
@@ -49,23 +49,23 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=360000.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Cylindrical\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Cylindrical</a>.
- </p>
- <p>
- After a short delay, a constant heat flow rate is applied to the inner surface
- of a cylindrical ground layer while the outer surface is kept at a constant
- temperature.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 13, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Cylindrical\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Cylindrical</a>.
+</p>
+<p>
+After a short delay, a constant heat flow rate is applied to the inner surface
+of a cylindrical ground layer while the outer surface is kept at a constant
+temperature.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 13, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Cylindrical;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/FiniteDifference_1Week.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/FiniteDifference_1Week.mo
index ef91ded6cf..917e957534 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/FiniteDifference_1Week.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/FiniteDifference_1Week.mo
@@ -52,6 +52,7 @@ model FiniteDifference_1Week
     amplitude=1e8) "Heat flow signal"
     annotation (Placement(transformation(extent={{-92,-10},{-72,10}})));
   AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse groTemRes(
+    nSeg=12,
     borFieDat=borFieDat,
     nCel=5,
     tLoaAgg=30) "Heat conduction in the soil"
@@ -90,7 +91,7 @@ equation
     annotation (Line(points={{50,60},{60,60},{60,88},{-66,88},{-66,-36},{-73,
           -36}},                                             color={0,0,127}));
   connect(temSenDis.T, deltaT.u1)
-    annotation (Line(points={{10,20},{20,20},{20,6},{28,6}}, color={0,0,127}));
+    annotation (Line(points={{11,20},{20,20},{20,6},{28,6}}, color={0,0,127}));
   connect(soi.port_a, temSenDis.port) annotation (Line(points={{-12,60},{-20,60},
           {-20,20},{-10,20}}, color={191,0,0}));
 
@@ -108,28 +109,28 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=604800.0),
     Documentation(info="<html>
- <p>
- This example validates the implementation of
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse</a>
- for the evaluation of the borehole wall temperature at a short time scale.
- </p>
- <p>
- After a short delay, a sinusoidal heat flow rate is applied to borehole heat
- exchanger. The temperature at the borehole wall evaluated with
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse</a>
- is compared to the temperature obtained with
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Cylindrical\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Cylindrical</a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 13, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example validates the implementation of
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse</a>
+for the evaluation of the borehole wall temperature at a short time scale.
+</p>
+<p>
+After a short delay, a sinusoidal heat flow rate is applied to borehole heat
+exchanger. The temperature at the borehole wall evaluated with
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse</a>
+is compared to the temperature obtained with
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Cylindrical\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.Cylindrical</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 13, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FiniteDifference_1Week;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Measured_SmallScale.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Measured_SmallScale.mo
index 4722a3b9f6..d1a4cead5a 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Measured_SmallScale.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Measured_SmallScale.mo
@@ -10,6 +10,7 @@ model Measured_SmallScale
 
   AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse groTemRes(
     nCel=5,
+    nSeg=12,
     borFieDat=borFieDat,
     forceGFunCalc=true,
     tLoaAgg=360000) "Ground temperature response of borehole"
@@ -56,42 +57,42 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/Validation/Measured_SmallScale.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This validation case simulates the experiment of Cimmino and Bernier (2015).
- The experiment consists in the injection of heat at an average rate of 8.67 W
- in a 0.40 m long borehole over a period of 168 h. Borehole wall tempratures
- were measured by a series of 22 thermocouples welded to the stainless steel
- pipe that contains the borehole and acts as the borehole wall.
- </p>
- <p>
- Since the model is not adapted to the simulation of small scale boreholes, the
- borehole dimensions are multiplied by a factor 375 to obtain a scaled-up 150.0 m
- long borehole. The time values of the experimental data are then multiplied by a
- factor 375<sup>2</sup>. The predicted borehole wall temperature is compared to
- the experimental data.
- </p>
- <p>
- A sharp increase in the rate of change of the borehole wall temperature is
- observed at <i>t=500 years</i>. This is caused by a sudden change in the rate
- of heat injected to the fluid at the same moment. The simulated borehole wall
- temperature is more affected the measured borehole wall temperature since the
- validation model does not consider the dynamics of the borehole and the fluid,
- and that heat is directly injected at the borehole wall. In the experiment, the
- sudden change in heat injection rate was dampened by the circulating fluid, the
- borehole filling material, and the measurement apparatus.
- </p>
- <h4>References</h4>
- <p>
- Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
- g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case simulates the experiment of Cimmino and Bernier (2015).
+The experiment consists in the injection of heat at an average rate of 8.67 W
+in a 0.40 m long borehole over a period of 168 h. Borehole wall tempratures
+were measured by a series of 22 thermocouples welded to the stainless steel
+pipe that contains the borehole and acts as the borehole wall.
+</p>
+<p>
+Since the model is not adapted to the simulation of small scale boreholes, the
+borehole dimensions are multiplied by a factor 375 to obtain a scaled-up 150.0 m
+long borehole. The time values of the experimental data are then multiplied by a
+factor 375<sup>2</sup>. The predicted borehole wall temperature is compared to
+the experimental data.
+</p>
+<p>
+A sharp increase in the rate of change of the borehole wall temperature is
+observed at <i>t=500 years</i>. This is caused by a sudden change in the rate
+of heat injected to the fluid at the same moment. The simulated borehole wall
+temperature is more affected the measured borehole wall temperature since the
+validation model does not consider the dynamics of the borehole and the fluid,
+and that heat is directly injected at the borehole wall. In the experiment, the
+sudden change in heat injection rate was dampened by the circulating fluid, the
+borehole filling material, and the measurement apparatus.
+</p>
+<h4>References</h4>
+<p>
+Cimmino, M. and Bernier, M. 2015. <i>Experimental determination of the
+g-functions of a small-scale geothermal borehole</i>. Geothermics 56: 60-71.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 18, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Measured_SmallScale;
diff --git a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/PartialBorefield.mo b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/PartialBorefield.mo
index 2e39e593d6..c97dc39e94 100644
--- a/AixLib/Fluid/Geothermal/Borefields/BaseClasses/PartialBorefield.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/BaseClasses/PartialBorefield.mo
@@ -39,7 +39,12 @@ partial model PartialBorefield
     "Number of segments to use in vertical discretization of the boreholes";
   parameter Boolean forceGFunCalc = false
     "Set to true to force the thermal response to be calculated at the start instead of checking whether this has been pre-computed"
-    annotation (Dialog(tab="Advanced"));
+    annotation (Dialog(tab="Advanced", group="g-function"));
+  parameter Integer nSegGFun(min=1)=12 "Number of segments to use in the calculation of the g-function"
+    annotation (Dialog(tab="Advanced", group="g-function"));
+  parameter Integer nClu(min=1)=5
+    "Number of borehole clusters to use in the calculation of the g-function"
+    annotation (Dialog(tab="Advanced", group="g-function"));
 
   // General parameters of borefield
   parameter AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Template borFieDat "Borefield data"
@@ -68,11 +73,6 @@ partial model PartialBorefield
     "Vertical temperature gradient of the undisturbed soil for h below z0"
     annotation (Dialog(tab="Initialization", group="Temperature profile"));
 
-  // Dynamics of filling material
-  parameter Boolean dynFil=true
-    "Set to false to remove the dynamics of the filling material."
-    annotation (Dialog(tab="Dynamics"));
-
   Modelica.Blocks.Interfaces.RealOutput TBorAve(final quantity="ThermodynamicTemperature",
                                                 final unit="K",
                                                 displayUnit = "degC",
@@ -83,6 +83,8 @@ partial model PartialBorefield
   AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse groTemRes(
     final tLoaAgg=tLoaAgg,
     final nCel=nCel,
+    final nSeg=nSegGFun,
+    final nClu=nClu,
     final borFieDat=borFieDat,
     final forceGFunCalc=forceGFunCalc)
     "Ground temperature response"
@@ -105,7 +107,6 @@ partial model PartialBorefield
     final energyDynamics=energyDynamics,
     final p_start=p_start,
     final mSenFac=mSenFac,
-    final dynFil=dynFil,
     final TFlu_start=TFlu_start,
     final TGro_start=TGro_start) "Borehole"
     annotation (Placement(transformation(extent={{-10,-50},{10,-30}})));
@@ -117,14 +118,16 @@ protected
 
   AixLib.Fluid.BaseClasses.MassFlowRateMultiplier masFloDiv(
     redeclare final package Medium = Medium,
-    allowFlowReversal=allowFlowReversal,
+    final allowFlowReversal=allowFlowReversal,
+    final use_input=false,
     final k=1/borFieDat.conDat.nBor)
                                    "Division of flow rate"
     annotation (Placement(transformation(extent={{-80,-50},{-60,-30}})));
 
   AixLib.Fluid.BaseClasses.MassFlowRateMultiplier masFloMul(
     redeclare final package Medium = Medium,
-    allowFlowReversal=allowFlowReversal,
+    final allowFlowReversal=allowFlowReversal,
+    final use_input=false,
     final k=borFieDat.conDat.nBor) "Mass flow multiplier"
     annotation (Placement(transformation(extent={{60,-50},{80,-30}})));
 
@@ -181,7 +184,7 @@ equation
     annotation (Line(points={{-4.44089e-16,-20},{0,-20},{0,-30}},
                                                         color={191,0,0}));
   connect(QBorHol.Q_flow, QTotSeg_flow.u)
-    annotation (Line(points={{-10,-10},{-86,-10},{-86,80},{-62,80}},
+    annotation (Line(points={{-11,-10},{-86,-10},{-86,80},{-62,80}},
                                                           color={0,0,127}));
   connect(groTemRes.delTBor, repDelTBor.u)
     annotation (Line(points={{41,80},{58,80}}, color={0,0,127}));
@@ -273,73 +276,73 @@ equation
           fillPattern=FillPattern.Forward)}),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}})),Documentation(info="<html>
- <p>
- This model simulates a borefield containing one or multiple boreholes
- using the parameters in the <code>borFieDat</code> record.
- </p>
- <p>
- Heat transfer to the soil is modeled using only one borehole heat exchanger
- (To be added in an extended model). The
- fluid mass flow rate into the borehole is divided to reflect the per-borehole
- fluid mass flow rate. The borehole model calculates the dynamics within the
- borehole itself using an axial discretization and a resistance-capacitance
- network for the internal thermal resistances between the individual pipes and
- between each pipe and the borehole wall.
- </p>
- <p>
- The thermal interaction between the borehole wall and the surrounding soil
- is modeled using
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse</a>,
- which uses a cell-shifting load aggregation technique to calculate the borehole wall
- temperature after calculating and/or read (from a previous calculation) the borefield's thermal response factor.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 9, 2021, by Michael Wetter:<br/>
- Corrected placement of <code>each</code> keyword.<br/>
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/2440\">Buildings, PR #2440</a>.
- </li>
- <li>
- August 25, 2020, by Filip Jorissen:<br/>
- Switched port connections for <code>masFloDiv</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/41\">#41</a>.
- </li>
- <li>
- March 24, 2020, by Damien Picard:<br/>
- Propagated flowReversal into <code>masFloDiv</code> and <code>masFloMul</code>.
- </li>
- <li>
- June 7, 2019, by Massimo Cimmino:<br/>
- Converted instances that are not of interest to user to be <code>protected</code>.
- </li>
- <li>
- June 4, 2019, by Massimo Cimmino:<br/>
- Added an output for the average borehole wall temperature.
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1107\">#1107</a>.
- </li>
- <li>
- April 11, 2019, by Filip Jorissen:<br/>
- Added <code>choicesAllMatching</code> for <code>borFieDat</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1117\">#1117</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice to water and glycolWater.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- July 2018, by Alex Laferri&egrave;re:<br/>
- Changed into a partial model and changed documentation to reflect the new approach
- used by the borefield models.
- </li>
- <li>
- July 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model simulates a borefield containing one or multiple boreholes
+using the parameters in the <code>borFieDat</code> record.
+</p>
+<p>
+Heat transfer to the soil is modeled using only one borehole heat exchanger
+(To be added in an extended model). The
+fluid mass flow rate into the borehole is divided to reflect the per-borehole
+fluid mass flow rate. The borehole model calculates the dynamics within the
+borehole itself using an axial discretization and a resistance-capacitance
+network for the internal thermal resistances between the individual pipes and
+between each pipe and the borehole wall.
+</p>
+<p>
+The thermal interaction between the borehole wall and the surrounding soil
+is modeled using
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureResponse</a>,
+which uses a cell-shifting load aggregation technique to calculate the borehole wall
+temperature after calculating and/or read (from a previous calculation) the borefield's thermal response factor.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 9, 2021, by Michael Wetter:<br/>
+Corrected placement of <code>each</code> keyword.<br/>
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/2440\">Buildings, PR #2440</a>.
+</li>
+<li>
+August 25, 2020, by Filip Jorissen:<br/>
+Switched port connections for <code>masFloDiv</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/41\">#41</a>.
+</li>
+<li>
+March 24, 2020, by Damien Picard:<br/>
+Propagated flowReversal into <code>masFloDiv</code> and <code>masFloMul</code>.
+</li>
+<li>
+June 7, 2019, by Massimo Cimmino:<br/>
+Converted instances that are not of interest to user to be <code>protected</code>.
+</li>
+<li>
+June 4, 2019, by Massimo Cimmino:<br/>
+Added an output for the average borehole wall temperature.
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1107\">#1107</a>.
+</li>
+<li>
+April 11, 2019, by Filip Jorissen:<br/>
+Added <code>choicesAllMatching</code> for <code>borFieDat</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1117\">#1117</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice to water and glycolWater.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+July 2018, by Alex Laferri&egrave;re:<br/>
+Changed into a partial model and changed documentation to reflect the new approach
+used by the borefield models.
+</li>
+<li>
+July 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialBorefield;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Data/Borefield/Example.mo b/AixLib/Fluid/Geothermal/Borefields/Data/Borefield/Example.mo
index 407d35fa54..4d456d9100 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Data/Borefield/Example.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Data/Borefield/Example.mo
@@ -11,23 +11,23 @@ defaultComponentPrefixes="parameter",
 defaultComponentName="borFieDat",
 Documentation(
 info="<html>
- <p>This record presents an example on how to define borefield records
- using the template in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Template\">
- AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Template</a>.</p>
- </html>",
+<p>This record presents an example on how to define borefield records
+using the template in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Template\">
+AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Template</a>.</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Data/Borefield/Template.mo b/AixLib/Fluid/Geothermal/Borefields/Data/Borefield/Template.mo
index 063b19c50d..51f6eecde2 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Data/Borefield/Template.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Data/Borefield/Template.mo
@@ -14,24 +14,24 @@ record Template
   defaultComponentName="borFieDat",
 Documentation(
 info="<html>
- <p>
- This record is a template for the records in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Borefield\">
- AixLib.Fluid.Geothermal.Borefields.Data.Borefield</a>.
- </p>
- </html>",
+<p>
+This record is a template for the records in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Borefield\">
+AixLib.Fluid.Geothermal.Borefields.Data.Borefield</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Template;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Data/Configuration/Example.mo b/AixLib/Fluid/Geothermal/Borefields/Data/Configuration/Example.mo
index 4d9c34bacd..e6ea2e63dc 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Data/Configuration/Example.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Data/Configuration/Example.mo
@@ -19,25 +19,25 @@ record Example
   defaultComponentName="conDat",
     Documentation(
 info="<html>
- <p>
- This record presents an example for how to define configuration data records
- using the template in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Template\">
- AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Template</a>.
- </p>
- </html>",
+<p>
+This record presents an example for how to define configuration data records
+using the template in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Template\">
+AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Template</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Example;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Data/Configuration/Template.mo b/AixLib/Fluid/Geothermal/Borefields/Data/Configuration/Template.mo
index 1eaf4ef577..64e09f8772 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Data/Configuration/Template.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Data/Configuration/Template.mo
@@ -60,24 +60,24 @@ record Template
   defaultComponentName="conDat",
     Documentation(
 info="<html>
- <p>
- This record is a template for the records in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Configuration\">
- AixLib.Fluid.Geothermal.Borefields.Data.Configuration</a>.
- </p>
- </html>",
+<p>
+This record is a template for the records in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Configuration\">
+AixLib.Fluid.Geothermal.Borefields.Data.Configuration</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Template;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Data/Filling/Bentonite.mo b/AixLib/Fluid/Geothermal/Borefields/Data/Filling/Bentonite.mo
index 339624ffdf..7f5021017d 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Data/Filling/Bentonite.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Data/Filling/Bentonite.mo
@@ -11,22 +11,22 @@ record Bentonite
   defaultComponentName="filDat",
 Documentation(
 info="<html>
- <p>
- This filling data record contains the heat transfer properties of bentonite.
- </p>
- </html>",
+<p>
+This filling data record contains the heat transfer properties of bentonite.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Bentonite;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Data/Filling/Template.mo b/AixLib/Fluid/Geothermal/Borefields/Data/Filling/Template.mo
index 998fdcae0b..d932f08030 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Data/Filling/Template.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Data/Filling/Template.mo
@@ -18,23 +18,23 @@ record Template
   defaultComponentName="filDat",
 Documentation(
 info="<html>
- <p>This record is a template for the records in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Filling\">
- AixLib.Fluid.Geothermal.Borefields.Data.Filling</a>.</p>
- </html>",
+<p>This record is a template for the records in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Filling\">
+AixLib.Fluid.Geothermal.Borefields.Data.Filling</a>.</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- Corrected check of real variable against zero which is not allowed in Modelica.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+Corrected check of real variable against zero which is not allowed in Modelica.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Template;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Data/Soil/SandStone.mo b/AixLib/Fluid/Geothermal/Borefields/Data/Soil/SandStone.mo
index c3f29228df..a297e18e97 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Data/Soil/SandStone.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Data/Soil/SandStone.mo
@@ -11,30 +11,30 @@ record SandStone
   defaultComponentName="soiDat",
 Documentation(
 info="<html>
- <p>
- This soil data record contains the heat transfer properties of sandstone.
- </p>
- </html>",
+<p>
+This soil data record contains the heat transfer properties of sandstone.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 21, 2018, by Jianjun Hu:<br/>
- Changed the default properties based on Table 4 in the
- <a href=\"http://www.15000inc.com/wp/wp-content/uploads/Geothermal-Heat-Pump-Design-Manual.pdf\">
- McQuay geothermal heat pump design manual</a>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1062\">#1062</a>.
- </li>
- 
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 21, 2018, by Jianjun Hu:<br/>
+Changed the default properties based on Table 4 in the
+<a href=\"http://www.15000inc.com/wp/wp-content/uploads/Geothermal-Heat-Pump-Design-Manual.pdf\">
+McQuay geothermal heat pump design manual</a>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1062\">#1062</a>.
+</li>
+
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SandStone;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Data/Soil/Template.mo b/AixLib/Fluid/Geothermal/Borefields/Data/Soil/Template.mo
index 782d091f1e..bfbce0a2b6 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Data/Soil/Template.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Data/Soil/Template.mo
@@ -18,25 +18,25 @@ record Template
   defaultComponentName="soiDat",
 Documentation(
 info="<html>
- <p>
- This record is a template for the records in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Soil\">
- AixLib.Fluid.Geothermal.Borefields.Data.Soil</a>.
- </p>
- </html>",
+<p>
+This record is a template for the records in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.Data.Soil\">
+AixLib.Fluid.Geothermal.Borefields.Data.Soil</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- Corrected check of real variable against zero which is not allowed in Modelica.
- </li>
- <li>
- June28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+Corrected check of real variable against zero which is not allowed in Modelica.
+</li>
+<li>
+June28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Template;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Examples/Borefields.mo b/AixLib/Fluid/Geothermal/Borefields/Examples/Borefields.mo
index ae55aaf354..fd62fea53a 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Examples/Borefields.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Examples/Borefields.mo
@@ -13,7 +13,6 @@ model Borefields
     redeclare package Medium = Medium,
     borFieDat=borFie2UTubParDat,
     tLoaAgg=tLoaAgg,
-    dynFil=false,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     TExt0_start=TGro)
     "Borefield with a 2-U-tube connected in parallel borehole configuration"
@@ -46,6 +45,8 @@ model Borefields
     "Outlet temperature of the borefield with 2-UTube in parallel configuration"
     annotation (Placement(transformation(extent={{40,-10},{60,10}})));
   parameter AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Example borFieUTubDat(
+    filDat=AixLib.Fluid.Geothermal.Borefields.Data.Filling.Bentonite(
+    steadyState=true),
     conDat=AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Example(
     borCon=AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.SingleUTube))
     annotation (Placement(transformation(extent={{70,-100},{90,-80}})));
@@ -54,7 +55,6 @@ model Borefields
     redeclare package Medium = Medium,
     borFieDat=borFie2UTubSerDat,
     tLoaAgg=tLoaAgg,
-    dynFil=false,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     TExt0_start=TGro)
     "Borefield with a 2-U-tube connected in serie borehole configuration"
@@ -88,6 +88,8 @@ model Borefields
     "Outlet temperature of the borefield with 2-UTube in serie configuration"
     annotation (Placement(transformation(extent={{42,50},{62,70}})));
   parameter AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Example borFie2UTubParDat(
+    filDat=AixLib.Fluid.Geothermal.Borefields.Data.Filling.Bentonite(
+    steadyState=true),
     conDat=AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Example(
     borCon=AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.DoubleUTubeParallel))
     "Data from the borefield with 2-UTube in parallel borehole configuration"
@@ -96,7 +98,6 @@ model Borefields
     redeclare package Medium = Medium,
     borFieDat=borFieUTubDat,
     tLoaAgg=tLoaAgg,
-    dynFil=false,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     TExt0_start=TGro)
     "Borefield with a U-tube borehole configuration"
@@ -129,6 +130,8 @@ model Borefields
     "Inlet temperature of the borefield with UTube configuration"
     annotation (Placement(transformation(extent={{40,-70},{60,-50}})));
   parameter AixLib.Fluid.Geothermal.Borefields.Data.Borefield.Example borFie2UTubSerDat(
+      filDat=AixLib.Fluid.Geothermal.Borefields.Data.Filling.Bentonite(
+        steadyState=true),
     conDat=AixLib.Fluid.Geothermal.Borefields.Data.Configuration.Example(
     borCon=AixLib.Fluid.Geothermal.Borefields.Types.BoreholeConfiguration.DoubleUTubeSeries))
     "Data from the borefield with 2-UTube in serie borehole configuration"
@@ -162,26 +165,32 @@ equation
   annotation (__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/Examples/Borefields.mos"
         "Simulate and plot"),
   Documentation(info="<html>
- <p>
- This example shows three different borefields, each with a different configuration
- (single U-tube, double U-tube in parallel, and double U-tube in series) and compares
- the thermal behaviour of the circulating fluid in each case.
- </p>
- </html>",
+<p>
+This example shows three different borefields, each with a different configuration
+(single U-tube, double U-tube in parallel, and double U-tube in series) and compares
+the thermal behaviour of the circulating fluid in each case.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 8, 2021, by Michael Wetter:<br/>
- Added missing <code>parameter</code> keyword.<br/>
- For <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1464\">IBPSA, issue 1464</a>.
- </li>
- <li>
- June 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+May 17, 2024, by Michael Wetter:<br/>
+Updated model due to removal of parameter <code>dynFil</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1885\">IBPSA, #1885</a>.
+</li>
+<li>
+April 8, 2021, by Michael Wetter:<br/>
+Added missing <code>parameter</code> keyword.<br/>
+For <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1464\">IBPSA, issue 1464</a>.
+</li>
+<li>
+June 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
-      StopTime=36000,Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      StopTime=36000,Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Borefields;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Examples/RectangularBorefield.mo b/AixLib/Fluid/Geothermal/Borefields/Examples/RectangularBorefield.mo
index 8ba3cbcdf1..6644c8c033 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Examples/RectangularBorefield.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Examples/RectangularBorefield.mo
@@ -73,6 +73,7 @@ model RectangularBorefield "Example model of a rectangular borefield"
   AixLib.Fluid.Movers.FlowControlled_m_flow pum(
     redeclare package Medium = Medium,
     addPowerToMedium=false,
+    nominalValuesDefineDefaultPressureCurve=true,
     use_inputFilter=false,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     inputType=AixLib.Fluid.Types.InputType.Constant,
@@ -104,30 +105,37 @@ equation
   connect(pum.port_a, bou.ports[1])
     annotation (Line(points={{0,0},{0,-60},{-40,-60}}, color={0,127,255}));
   annotation (Documentation(info="<html>
- <p>
- This example model illustrates how to configure the layout
- of the boreholes for a rectangular borefield.
- The configuration is
- </p>
- <pre>
- cooBor = {{dBorHol*mod((i-1),nXBorHol), dBorHol*floor((i-1)/nXBorHol)} for i in 1:nBorHol}
- </pre>
- <p>
- where <code>dBorHol</code> is the distance between the boreholes,
- <code>nXBorHol</code> is the number of boreholes in the x-direction, and
- <code>nBorHol</code> is the total number of boreholes.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 10, 2018, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example model illustrates how to configure the layout
+of the boreholes for a rectangular borefield.
+The configuration is
+</p>
+<pre>
+cooBor = {{dBorHol*mod((i-1),nXBorHol), dBorHol*floor((i-1)/nXBorHol)} for i in 1:nBorHol}
+</pre>
+<p>
+where <code>dBorHol</code> is the distance between the boreholes,
+<code>nXBorHol</code> is the number of boreholes in the x-direction, and
+<code>nBorHol</code> is the total number of boreholes.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 9, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+September 10, 2018, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/Examples/RectangularBorefield.mos"
         "Simulate and plot"),
   experiment(
-      StopTime=2678400,Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      StopTime=2678400,Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end RectangularBorefield;
diff --git a/AixLib/Fluid/Geothermal/Borefields/OneUTube.mo b/AixLib/Fluid/Geothermal/Borefields/OneUTube.mo
index 674eb6e7c2..b13fc541e3 100644
--- a/AixLib/Fluid/Geothermal/Borefields/OneUTube.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/OneUTube.mo
@@ -7,30 +7,30 @@ model OneUTube
   annotation (
   defaultComponentName="borFie",
   Documentation(info="<html>
- <p>
- This model simulates a borefield containing one or many single U-tube boreholes
- using the parameters in the <code>borFieDat</code> record.
- </p>
- <p>
- Heat transfer to the soil is modeled using only one borehole heat exchanger. The
- fluid mass flow rate into the borehole is divided to reflect the per-borehole
- fluid mass flow rate. The borehole model calculates the dynamics within the
- borehole itself using an axial discretization and a resistance-capacitance
- network for the internal thermal resistances between the individual pipes and
- between each pipe and the borehole wall.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 2018, by Alex Laferri&egrave;re:<br/>
- Extended partial model and changed documentation to reflect the new approach
- used by the borefield models.
- </li>
- <li>
- July 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model simulates a borefield containing one or many single U-tube boreholes
+using the parameters in the <code>borFieDat</code> record.
+</p>
+<p>
+Heat transfer to the soil is modeled using only one borehole heat exchanger. The
+fluid mass flow rate into the borehole is divided to reflect the per-borehole
+fluid mass flow rate. The borehole model calculates the dynamics within the
+borehole itself using an axial discretization and a resistance-capacitance
+network for the internal thermal resistances between the individual pipes and
+between each pipe and the borehole wall.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 2018, by Alex Laferri&egrave;re:<br/>
+Extended partial model and changed documentation to reflect the new approach
+used by the borefield models.
+</li>
+<li>
+July 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OneUTube;
diff --git a/AixLib/Fluid/Geothermal/Borefields/TwoUTubes.mo b/AixLib/Fluid/Geothermal/Borefields/TwoUTubes.mo
index 941f6ff92e..f1f1506f41 100644
--- a/AixLib/Fluid/Geothermal/Borefields/TwoUTubes.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/TwoUTubes.mo
@@ -6,30 +6,30 @@ model TwoUTubes
   annotation (
   defaultComponentName="borFie",
   Documentation(info="<html>
- <p>
- This model simulates a borefield containing one or many double U-tube boreholes
- using the parameters in the <code>borFieDat</code> record.
- </p>
- <p>
- Heat transfer to the soil is modeled using only one borehole heat exchanger. The
- fluid mass flow rate into the borehole is divided to reflect the per-borehole
- fluid mass flow rate. The borehole model calculates the dynamics within the
- borehole itself using an axial discretization and a resistance-capacitance
- network for the internal thermal resistances between the individual pipes and
- between each pipe and the borehole wall.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 2018, by Alex Laferri&egrave;re:<br/>
- Extended partial model and changed documentation to reflect the new approach
- used by the borefield models.
- </li>
- <li>
- July 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model simulates a borefield containing one or many double U-tube boreholes
+using the parameters in the <code>borFieDat</code> record.
+</p>
+<p>
+Heat transfer to the soil is modeled using only one borehole heat exchanger. The
+fluid mass flow rate into the borehole is divided to reflect the per-borehole
+fluid mass flow rate. The borehole model calculates the dynamics within the
+borehole itself using an axial discretization and a resistance-capacitance
+network for the internal thermal resistances between the individual pipes and
+between each pipe and the borehole wall.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 2018, by Alex Laferri&egrave;re:<br/>
+Extended partial model and changed documentation to reflect the new approach
+used by the borefield models.
+</li>
+<li>
+July 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoUTubes;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Types.mo b/AixLib/Fluid/Geothermal/Borefields/Types.mo
index 48e1084eba..600ffca658 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Types.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Types.mo
@@ -11,32 +11,32 @@ package Types "Package with type definitions"
     "Double U-tube configuration with pipes connected in series")
   "Enumaration to define the borehole configurations"
   annotation (Documentation(info="<html>
- <p>
- Enumeration that defines the pipe configuration in the borehole.
- </p>
- <p>
- The following pipe configurations are available in this enumeration:
- </p>
- <table summary=\"summary\" border=\"1\">
- <tr><th>Enumeration</th><th>Description</th></tr>
- <tr><td>SingleUTube</td><td>Single U-tube configuration</td></tr>
- 
- <tr><td>DoubleUTubeParallel</td><td>Double U-tube configuration with pipes connected in parallel</td></tr>
- <tr><td>DoubleUTubeSeries</td><td>Double U-tube configuration with pipes connected in series</td></tr>
- </table>
- </html>",
+<p>
+Enumeration that defines the pipe configuration in the borehole.
+</p>
+<p>
+The following pipe configurations are available in this enumeration:
+</p>
+<table summary=\"summary\" border=\"1\">
+<tr><th>Enumeration</th><th>Description</th></tr>
+<tr><td>SingleUTube</td><td>Single U-tube configuration</td></tr>
+
+<tr><td>DoubleUTubeParallel</td><td>Double U-tube configuration with pipes connected in parallel</td></tr>
+<tr><td>DoubleUTubeSeries</td><td>Double U-tube configuration with pipes connected in series</td></tr>
+</table>
+</html>",
   revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   annotation (preferredView="info", Documentation(info="<html>
-  <p>
-  This package contains type definitions.
-  </p>
-  </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+ <p>
+ This package contains type definitions.
+ </p>
+ </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Types;
diff --git a/AixLib/Fluid/Geothermal/Borefields/UsersGuide.mo b/AixLib/Fluid/Geothermal/Borefields/UsersGuide.mo
index 7edd9b3e7e..25a9d03232 100644
--- a/AixLib/Fluid/Geothermal/Borefields/UsersGuide.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/UsersGuide.mo
@@ -17,7 +17,7 @@ AixLib.Fluid.Geothermal.Borefields.Validation</a>,
 respectively.
 </p>
 <p>
-The major features and configurations currently supported are:
+The following major features and configurations are supported:
 <ul>
 <li> User-defined borefield characteristics and geometry (borehole radius, pipe radius, shank spacing, etc.),
 including single U-tube, double U-tube in parallel and double U-tube in series configurations.
@@ -131,7 +131,8 @@ AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.GroundTemperatureRes
 Other parameters which can be modified include the dynamics, initial conditions,
 and further information regarding the fluid flow, for example whether the flow is reversible.
 It is worth noting that regardless of the <code>energyDynamics</code> chosen,
-the <code>dynFil</code> parameter can be set to <code>false</code>
+the <code>steadyState</code> parameter can be set to <code>true</code>
+in the data record for the filling material
 to remove the effect of the thermal capacitance
 of the filling material in the borehole(s).
 The <code>nSeg</code> parameter specifies the number of segments for the vertical discretization of the borehole(s).
@@ -178,7 +179,8 @@ short-term thermal effects in the borehole. The borehole segments do not take in
 thus only radial (horizontal) effects are considered within the borehole(s). The thermal
 behavior between the pipes and borehole wall are modeled as a resistance-capacitance network, with
 the grout capacitance being split in the number of pipes present in a borehole section.
-The capacitance is only present if the <code>dynFil</code> parameter is set to <code>true</code>.
+The capacitance is only present if the parameter <code>steadyState</code> of the filling
+material data record is <code>false</code>, which is the default setting.
 The figure below shows an example for a borehole section within a single U-tube configuration.
 </p>
 <p align=\"center\">
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Borefield.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Borefield.mo
index b80e559329..e11a25e3a6 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Borefield.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Borefield.mo
@@ -10,17 +10,17 @@ defaultComponentPrefixes="parameter",
 defaultComponentName="borFieDat",
 Documentation(
 info="<html>
- <p>
- This record contains the borefield data of a field of <i>100</i> boreholes.
- </p>
- </html>",
+<p>
+This record contains the borefield data of a field of <i>100</i> boreholes.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 27, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 27, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantHeatInjection_100Boreholes_Borefield;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Configuration.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Configuration.mo
index 23b31b1b23..16b9f3ce4e 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Configuration.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Configuration.mo
@@ -18,17 +18,17 @@ record ConstantHeatInjection_100Boreholes_Configuration
   defaultComponentName="conDat",
     Documentation(
 info="<html>
- <p>
- This record contains the configuration data of a field of <i>100</i> boreholes.
- </p>
- </html>",
+<p>
+This record contains the configuration data of a field of <i>100</i> boreholes.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 27, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 27, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantHeatInjection_100Boreholes_Configuration;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Filling.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Filling.mo
index fcf6452a0d..5a01ad0fb5 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Filling.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Filling.mo
@@ -10,17 +10,17 @@ record ConstantHeatInjection_100Boreholes_Filling
   defaultComponentName="filDat",
 Documentation(
 info="<html>
- <p>
- This record contains the filling data of a field of <i>100</i> boreholes.
- </p>
- </html>",
+<p>
+This record contains the filling data of a field of <i>100</i> boreholes.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 27, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 27, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantHeatInjection_100Boreholes_Filling;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Soil.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Soil.mo
index 82ada7607b..97a949c245 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Soil.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/ConstantHeatInjection_100Boreholes_Soil.mo
@@ -10,17 +10,17 @@ record ConstantHeatInjection_100Boreholes_Soil
   defaultComponentName="soiDat",
 Documentation(
 info="<html>
- <p>
- This record contains the soil data of a field of <i>100</i> boreholes.
- </p>
- </html>",
+<p>
+This record contains the soil data of a field of <i>100</i> boreholes.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 27, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 27, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantHeatInjection_100Boreholes_Soil;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Borefield.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Borefield.mo
index a2961a9a0b..f8a4d14bf5 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Borefield.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Borefield.mo
@@ -12,28 +12,28 @@ record SandBox_Borefield
   defaultComponentName="borFieDat",
     Documentation(
 info="<html>
- <p>
- This record contains the borefield data of the Beier et al. (2011) experiment.
- </p>
- <h4>References</h4>
- <p>
- Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
- vertical borehole ground heat exchanger models and thermal response test
- analysis</i>. Geothermics 40: 79-85.
- </p>
- </html>",
+<p>
+This record contains the borefield data of the Beier et al. (2011) experiment.
+</p>
+<h4>References</h4>
+<p>
+Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
+vertical borehole ground heat exchanger models and thermal response test
+analysis</i>. Geothermics 40: 79-85.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SandBox_Borefield;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Configuration.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Configuration.mo
index 970d3c12d7..eb287bd466 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Configuration.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Configuration.mo
@@ -22,28 +22,28 @@ record SandBox_Configuration
   defaultComponentName="conDat",
 Documentation(
 info="<html>
- <p>
- This record contains the configuration data of the Beier et al. (2011) experiment.
- </p>
- <h4>References</h4>
- <p>
- Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
- vertical borehole ground heat exchanger models and thermal response test
- analysis</i>. Geothermics 40: 79-85.
- </p>
- </html>",
+<p>
+This record contains the configuration data of the Beier et al. (2011) experiment.
+</p>
+<h4>References</h4>
+<p>
+Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
+vertical borehole ground heat exchanger models and thermal response test
+analysis</i>. Geothermics 40: 79-85.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SandBox_Configuration;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Filling.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Filling.mo
index d4278a22b6..9227320242 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Filling.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Filling.mo
@@ -11,28 +11,28 @@ record SandBox_Filling
   defaultComponentName="filDat",
 Documentation(
 info="<html>
- <p>
- This record contains the filling data of the Beier et al. (2011) experiment.
- </p>
- <h4>References</h4>
- <p>
- Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
- vertical borehole ground heat exchanger models and thermal response test
- analysis</i>. Geothermics 40: 79-85.
- </p>
- </html>",
+<p>
+This record contains the filling data of the Beier et al. (2011) experiment.
+</p>
+<h4>References</h4>
+<p>
+Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
+vertical borehole ground heat exchanger models and thermal response test
+analysis</i>. Geothermics 40: 79-85.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SandBox_Filling;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Soil.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Soil.mo
index 53956299c3..4568ef64c6 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Soil.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/BaseClasses/SandBox_Soil.mo
@@ -11,28 +11,28 @@ record SandBox_Soil
   defaultComponentName="soiDat",
 Documentation(
 info="<html>
- <p>
- This record contains the soil data of the Beier et al. (2011) experiment.
- </p>
- <h4>References</h4>
- <p>
- Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
- vertical borehole ground heat exchanger models and thermal response test
- analysis</i>. Geothermics 40: 79-85.
- </p>
- </html>",
+<p>
+This record contains the soil data of the Beier et al. (2011) experiment.
+</p>
+<h4>References</h4>
+<p>
+Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
+vertical borehole ground heat exchanger models and thermal response test
+analysis</i>. Geothermics 40: 79-85.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 15, 2018, by Michael Wetter:<br/>
- Revised implementation, added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code>.
- </li>
- <li>
- June 28, 2018, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+July 15, 2018, by Michael Wetter:<br/>
+Revised implementation, added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code>.
+</li>
+<li>
+June 28, 2018, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SandBox_Soil;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/ConstantHeatInjection_100Boreholes.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/ConstantHeatInjection_100Boreholes.mo
index 87cfeaa7b2..e896680b7d 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/ConstantHeatInjection_100Boreholes.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/ConstantHeatInjection_100Boreholes.mo
@@ -24,7 +24,8 @@ model ConstantHeatInjection_100Boreholes
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     m_flow_nominal=borFieDat.conDat.mBorFie_flow_nominal,
     nominalValuesDefineDefaultPressureCurve=true,
-    inputType=AixLib.Fluid.Types.InputType.Constant)
+    inputType=AixLib.Fluid.Types.InputType.Constant,
+    dp_nominal=60E3) "Circulation pump"
     annotation (Placement(transformation(extent={{-20,-10},{0,-30}})));
   AixLib.Fluid.Sensors.TemperatureTwoPort TBorFieIn(
     redeclare package Medium = Medium,
@@ -83,36 +84,42 @@ equation
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/Validation/ConstantHeatInjection_100Boreholes.mos"
         "Simulate and Plot"),
 Documentation(info="<html>
- <p>
- This validation case simulates a borefield of 100 boreholes on a square 10 by 10
- grid.
- </p>
- <p>
- The heat injection rate in the borefield is constant and equal to
- <code>2*pi*kSoi*hBor*nBor</code>. In this case, the borehole wall temperature
- variation corresponds to the g-function of the borefield, as evaluated in
- <a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation.GFunction_100boreholes\">
- AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation.GFunction_100boreholes</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 8, 2021, by Michael Wetter:<br/>
- Added missing <code>parameter</code> keyword.<br/>
- For <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1464\">IBPSA, issue 1464</a>.
- </li>
- <li>
- June 24, 2019, by Michael Wetter:<br/>
- Changed <code>StopTime</code> from integer to floating point.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1163\">issue 1163</a>.
- </li>
- <li>
- May 27, 2019, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    Diagram(coordinateSystem(extent={{-120,-120},{120,120}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case simulates a borefield of 100 boreholes on a square 10 by 10
+grid.
+</p>
+<p>
+The heat injection rate in the borefield is constant and equal to
+<code>2*pi*kSoi*hBor*nBor</code>. In this case, the borehole wall temperature
+variation corresponds to the g-function of the borefield, as evaluated in
+<a href=\"modelica://AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation.GFunction_100boreholes\">
+AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation.GFunction_100boreholes</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 15, 2022, by Michael Wetter:<br/>
+Set proper head for pump.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1659\">IBPSA, issue 1659</a>.
+</li>
+<li>
+April 8, 2021, by Michael Wetter:<br/>
+Added missing <code>parameter</code> keyword.<br/>
+For <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1464\">IBPSA, issue 1464</a>.
+</li>
+<li>
+June 24, 2019, by Michael Wetter:<br/>
+Changed <code>StopTime</code> from integer to floating point.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1163\">issue 1163</a>.
+</li>
+<li>
+May 27, 2019, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-120,-120},{120,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantHeatInjection_100Boreholes;
diff --git a/AixLib/Fluid/Geothermal/Borefields/Validation/Sandbox.mo b/AixLib/Fluid/Geothermal/Borefields/Validation/Sandbox.mo
index c6018b7616..db0c68de6b 100644
--- a/AixLib/Fluid/Geothermal/Borefields/Validation/Sandbox.mo
+++ b/AixLib/Fluid/Geothermal/Borefields/Validation/Sandbox.mo
@@ -33,7 +33,8 @@ model Sandbox "Validation of BorefieldOneUTube based on the experiment of Beier
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     m_flow_nominal=borFieDat.conDat.mBorFie_flow_nominal,
     nominalValuesDefineDefaultPressureCurve=true,
-    inputType=AixLib.Fluid.Types.InputType.Constant)
+    inputType=AixLib.Fluid.Types.InputType.Constant,
+    dp_nominal=60E3) "Circulation pump"
     annotation (Placement(transformation(extent={{-20,-10},{0,-30}})));
   AixLib.Fluid.Sensors.TemperatureTwoPort TBorFieIn(
     redeclare package Medium = Medium,
@@ -95,49 +96,55 @@ equation
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/Validation/Sandbox.mos"
         "Simulate and Plot"),
 Documentation(info="<html>
- <p>
- This validation case simulates the experiment of Beier et al. (2011). Measured
- experimental data is taken from the reference.
- </p>
- <p>
- The experiment consists in the injection of heat at an average rate of 1142 W
- in a 18 m long borehole over a period 52 h. Dimensions and thermal properties
- reported by Beier et al. (2011) are used in the model. The authors conducted
- multiple independent measurements of soil thermal conductivity. The average of
- reported values (2.88 W/m-K) is used here. Finally, the filling material thermal
- capacity and density was not reported. Values were chosen from the estimated
- volumetric heat capacity used by Pasquier and Marcotte (2014).
- </p>
- <p>
- The construction of the borehole is non-conventional: the borehole is
- contained within an aluminum pipe that acts as the borehole wall. As this
- modifies the thermal resistances inside the borehole, the values evaluated by
- the multipole method are modified to obtain the effective borehole thermal
- resistance reported by Beier et al. (2011).
- <h4>References</h4>
- <p>
- Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
- vertical borehole ground heat exchanger models and thermal response test
- analysis</i>. Geothermics 40: 79-85.
- </p>
- <p>
- Pasquier, P., and Marcotte, D. 2014. <i>Joint use of quasi-3D response model and
- spectral method to simulate borehole heat exchanger</i>. Geothermics 51:
- 281-299.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 8, 2021, by Michael Wetter:<br/>
- Added missing <code>parameter</code> keyword.<br/>
- For <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1464\">IBPSA, issue 1464</a>.
- </li>
- <li>
- July 18, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    Diagram(coordinateSystem(extent={{-120,-120},{120,120}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation case simulates the experiment of Beier et al. (2011). Measured
+experimental data is taken from the reference.
+</p>
+<p>
+The experiment consists in the injection of heat at an average rate of 1142 W
+in a 18 m long borehole over a period 52 h. Dimensions and thermal properties
+reported by Beier et al. (2011) are used in the model. The authors conducted
+multiple independent measurements of soil thermal conductivity. The average of
+reported values (2.88 W/m-K) is used here. Finally, the filling material thermal
+capacity and density was not reported. Values were chosen from the estimated
+volumetric heat capacity used by Pasquier and Marcotte (2014).
+</p>
+<p>
+The construction of the borehole is non-conventional: the borehole is
+contained within an aluminum pipe that acts as the borehole wall. As this
+modifies the thermal resistances inside the borehole, the values evaluated by
+the multipole method are modified to obtain the effective borehole thermal
+resistance reported by Beier et al. (2011).
+<h4>References</h4>
+<p>
+Beier, R.A., Smith, M.D. and Spitler, J.D. 2011. <i>Reference data sets for
+vertical borehole ground heat exchanger models and thermal response test
+analysis</i>. Geothermics 40: 79-85.
+</p>
+<p>
+Pasquier, P., and Marcotte, D. 2014. <i>Joint use of quasi-3D response model and
+spectral method to simulate borehole heat exchanger</i>. Geothermics 51:
+281-299.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 15, 2022, by Michael Wetter:<br/>
+Set proper head for pump.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1659\">IBPSA, issue 1659</a>.
+</li>
+<li>
+April 8, 2021, by Michael Wetter:<br/>
+Added missing <code>parameter</code> keyword.<br/>
+For <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1464\">IBPSA, issue 1464</a>.
+</li>
+<li>
+July 18, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-120,-120},{120,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Sandbox;
diff --git a/AixLib/Fluid/Geothermal/package.order b/AixLib/Fluid/Geothermal/package.order
index b4d445b8a6..5a2a2839b5 100644
--- a/AixLib/Fluid/Geothermal/package.order
+++ b/AixLib/Fluid/Geothermal/package.order
@@ -1 +1,2 @@
+Aquifer
 Borefields
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Convector.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Convector.mo
index 9ae1d7e03b..31d9e614d4 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Convector.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Convector.mo
@@ -138,42 +138,42 @@ equation
           fillPattern=FillPattern.VerticalCylinder,
           fillColor={95,95,95})}), defaultComponentName="con",
            Documentation(info="<html>
- <p>
- In cooling mode, this model adds heat to the water stream. The heat added is equal to:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q<sub>Beam</sub> = Q<sub>rated</sub> f<sub><code>&#916;</code>T</sub> f<sub>SA</sub> f<sub>W</sub>
- </p>
- <p>
- In heating mode, the heat is removed from the water stream.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 3, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
- </li>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Made assignment of <code>senTem.y</code> final.
- </li>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+In cooling mode, this model adds heat to the water stream. The heat added is equal to:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>Beam</sub> = Q<sub>rated</sub> f<sub><code>&#916;</code>T</sub> f<sub>SA</sub> f<sub>W</sub>
+</p>
+<p>
+In heating mode, the heat is removed from the water stream.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 3, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Made assignment of <code>senTem.y</code> final.
+</li>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Convector;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/DerivativesCubicSpline.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/DerivativesCubicSpline.mo
index 36c92234b2..9346b1e8ab 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/DerivativesCubicSpline.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/DerivativesCubicSpline.mo
@@ -41,28 +41,28 @@ algorithm
 annotation (
   defaultComponentName="cubSpl",
   Documentation(info="<html>
- <p>
- This model calculates the output based on the cubic hermite interpolation
- and linear extrapolation of predefined values. The predefined values must create a monotone curve.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 15, 2016, by Michael Wetter:<br/>
- Removed wrong annotations.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/629\">#629</a>.
- </li>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model calculates the output based on the cubic hermite interpolation
+and linear extrapolation of predefined values. The predefined values must create a monotone curve.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 15, 2016, by Michael Wetter:<br/>
+Removed wrong annotations.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/629\">#629</a>.
+</li>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
     Line(points={{46,-76},{46,58}},
                                   color={192,192,192}),
@@ -79,6 +79,6 @@ annotation (
           points={{-82,-72},{-40,-72},{-18,-56},{-6,-32},{0,-8},{14,26},{32,46},
               {46,50},{80,50}},
           color={0,0,0},
-          smooth=Smooth.Bezier)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          smooth=Smooth.Bezier)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DerivativesCubicSpline;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/Convector.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/Convector.mo
index 6ac1d0a66d..45c923588d 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/Convector.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/Convector.mo
@@ -49,28 +49,28 @@ equation
   annotation (experiment(Tolerance=1e-6, StopTime=10),__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/Convector.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- The example tests the implementation of
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.Convector\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.Convector</a>.
- The room air temperature and the water mass flow rate are constant while the air flow rate varys with a ramp.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+The example tests the implementation of
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.Convector\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.Convector</a>.
+The room air temperature and the water mass flow rate are constant while the air flow rate varys with a ramp.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Convector;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/DerivateCubicSpline.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/DerivateCubicSpline.mo
index d80055bdd7..628e87e181 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/DerivateCubicSpline.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/DerivateCubicSpline.mo
@@ -13,24 +13,24 @@ equation
   annotation (experiment(Tolerance=1e-6, StopTime=1.0),__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/DerivateCubicSpline.mos"
         "Simulate and plot"),
         Documentation(info="<html>
- <p>
- The example tests the implementation of
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.DerivativesCubicSpline\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.DerivativesCubicSpline</a>.
- Default vectors are: <i>x=[0,0.5,1]</i> and <i>y=[0,0.75,1]</i>.
- Input to the model is the simulation time.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+The example tests the implementation of
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.DerivativesCubicSpline\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.DerivativesCubicSpline</a>.
+Default vectors are: <i>x=[0,0.5,1]</i> and <i>y=[0,0.75,1]</i>.
+Input to the model is the simulation time.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DerivateCubicSpline;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/ModificationFactor.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/ModificationFactor.mo
index bad97853f6..41f85babc8 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/ModificationFactor.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/ModificationFactor.mo
@@ -38,22 +38,22 @@ equation
             __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/ActiveBeams/BaseClasses/Examples/ModificationFactor.mos"
         "Simulate and plot"),
         Documentation(info="<html>
- <p>
- This example tests the implementation of
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.ModificationFactor\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.ModificationFactor</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the implementation of
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.ModificationFactor\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.BaseClasses.ModificationFactor</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ModificationFactor;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/ModificationFactor.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/ModificationFactor.mo
index 45ef406346..59b622db9a 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/ModificationFactor.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/BaseClasses/ModificationFactor.mo
@@ -105,31 +105,31 @@ equation
           {60,-40},{60,-2.8},{64,-2.8}}, color={0,0,127}));
   annotation ( defaultComponentName="mod",
             Documentation(info="<html>
- <p>
- This model determines the three modification factors described in
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.UsersGuide\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.UsersGuide</a>
- by comparing the actual values of air mass flow rate,
- water mass flow rate and room-water temperature difference with the nominal values.
- The three modification factors are then multiplied.
- Input to this model are the total mass flow rates of all parallel beams combined.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model determines the three modification factors described in
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.UsersGuide\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.UsersGuide</a>
+by comparing the actual values of air mass flow rate,
+water mass flow rate and room-water temperature difference with the nominal values.
+The three modification factors are then multiplied.
+Input to this model are the total mass flow rates of all parallel beams combined.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{100,100},{-100,-100}},
           textColor={0,0,0},
-          textString="f")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="f")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ModificationFactor;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Cooling.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Cooling.mo
index c262a3bd36..c273ecada9 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Cooling.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Cooling.mo
@@ -268,75 +268,75 @@ defaultComponentName="actBea",
 Diagram(coordinateSystem(
           preserveAspectRatio=false, extent={{-140,-120},{140,120}})),
 Documentation(info="<html>
- <p>
- Model of an active beam, based on the EnergyPlus beam model  <code>AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam</code>.
- </p>
- <p>
- This model operates only in cooling mode. For a model that operates in both heating and cooling mode,
- use <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating</a>.
- </p>
- <p>
- For a description of the equations, see the
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.UsersGuide\">
- User's Guide</a>.
- </p>
- <p>
- Performance data are available from
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Data\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.Data</a>.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- DOE(2015) EnergyPlus documentation v8.4.0 - Engineering Reference.
- </li>
- </ul>
- </html>",revisions="<html>
- <ul>
- <li>
- March 3, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
- </li>
- <li>
- March 30, 2021, by Michael Wetter:<br/>
- Added annotation <code>HideResult=true</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
- </li>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Set <code>final alpha=0</code> for prescribed heat flow rate.
- </li>
- <li>
- September 17, 2016, by Michael Wetter:<br/>
- Corrected wrong annotation to avoid an error in the pedantic model check
- in Dymola 2017 FD01 beta2.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/557\">issue 557</a>.
- </li>
- <li>
- June 14, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model of an active beam, based on the EnergyPlus beam model  <code>AirTerminal:SingleDuct:ConstantVolume:FourPipeBeam</code>.
+</p>
+<p>
+This model operates only in cooling mode. For a model that operates in both heating and cooling mode,
+use <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating</a>.
+</p>
+<p>
+For a description of the equations, see the
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.UsersGuide\">
+User's Guide</a>.
+</p>
+<p>
+Performance data are available from
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Data\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.Data</a>.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+DOE(2015) EnergyPlus documentation v8.4.0 - Engineering Reference.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+March 3, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
+</li>
+<li>
+March 30, 2021, by Michael Wetter:<br/>
+Added annotation <code>HideResult=true</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Set <code>final alpha=0</code> for prescribed heat flow rate.
+</li>
+<li>
+September 17, 2016, by Michael Wetter:<br/>
+Corrected wrong annotation to avoid an error in the pedantic model check
+in Dymola 2017 FD01 beta2.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/557\">issue 557</a>.
+</li>
+<li>
+June 14, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Cooling;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/CoolingAndHeating.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/CoolingAndHeating.mo
index a292356800..0212360f02 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/CoolingAndHeating.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/CoolingAndHeating.mo
@@ -110,34 +110,34 @@ equation
         Line(points={{-112,0},{-66,0},{-82,10}}, color={255,0,0}),
         Line(points={{-66,0},{-82,-8}}, color={255,0,0})}),
           Documentation(info="<html>
- <p>
- This model is identical to
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Cooling\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.Cooling</a>,
- except that an additional water stream and convector is added to allow for heating
- in addition to cooling.
- </p>
- <p>
- For a description of the equations, see the
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.UsersGuide\">
- User's Guide</a>.
- </p>
- <p>
- Performance data are available from
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Data\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.Data</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 14, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model is identical to
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Cooling\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.Cooling</a>,
+except that an additional water stream and convector is added to allow for heating
+in addition to cooling.
+</p>
+<p>
+For a description of the equations, see the
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.UsersGuide\">
+User's Guide</a>.
+</p>
+<p>
+Performance data are available from
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Data\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.Data</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 14, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoolingAndHeating;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/AirFlow.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/AirFlow.mo
index 5603d3f188..a5657eba6a 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/AirFlow.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/AirFlow.mo
@@ -7,28 +7,28 @@ record AirFlow "Record for primary air parameters"
     "Normalized performance factor at these flow rates";
 
   annotation (Documentation(info="<html>
- <p>
- Data record for performance data that describe the air volume flow rate versus
- the change in the rate of heating or cooling.
- </p>
- <p>
- The normamlized volume flow rate <i>r<sub>V</sub></i> must be strictly increasing, i.e.,
- <i>r<sub>V</sub><sup>i</sup> &lt; r<sub>V</sub><sup>i+1</sup></i>.
- Both vectors, <i>r<sub>V</sub></i> and <i>f</i>
- must have the same size.
- </p>
- </html>",
+<p>
+Data record for performance data that describe the air volume flow rate versus
+the change in the rate of heating or cooling.
+</p>
+<p>
+The normamlized volume flow rate <i>r<sub>V</sub></i> must be strictly increasing, i.e.,
+<i>r<sub>V</sub><sup>i</sup> &lt; r<sub>V</sub><sup>i+1</sup></i>.
+Both vectors, <i>r<sub>V</sub></i> and <i>f</i>
+must have the same size.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirFlow;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/TemperatureDifference.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/TemperatureDifference.mo
index 4b276b0858..e2c9a68a9d 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/TemperatureDifference.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/TemperatureDifference.mo
@@ -3,50 +3,50 @@ record TemperatureDifference "Record for temperature difference"
   extends Modelica.Icons.Record;
   parameter Real r_dT[:](each min=0, each final unit="1")
    "Normalized temperature difference, e.g., temperature difference at
-  user-selected operating points divided by nominal temperature difference.
-  Must be positive.";
+ user-selected operating points divided by nominal temperature difference.
+ Must be positive.";
   parameter Real f[size(r_dT, 1)](each min=0, each final unit="1")
     "Normalized performance factor at these normalized temperature differences";
 
   annotation (Documentation(info="<html>
- <p>
- Data record for performance data that describe the normalized
- temperature difference
- versus the change in the rate of heating or cooling.
- The normalized temperature difference is defined as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- r<sub>&#916;T</sub><sup>i</sup>=
- &#916;T<sup>i</sup> &frasl; &#916;T<sub>nominal</sub>
- =
- (T<sub>w</sub><sup>i</sup>-T<sub>z</sub>)
- &frasl;
- (T<sub>w,nominal</sub>-T<sub>z</sub>),
- </p>
- <p>
- where
- <i>T<sub>w</sub><sup>i</sup></i> is the water inlet temperature,
- <i>T<sub>z</sub></i> is the zone air temperature and
- <i>T<sub>w,nominal</sub></i> is the nominal water inlet temperature.
- </p>
- <p>
- The normalized temperature difference <i>r<sub>&#916;T</sub></i> must be strictly increasing, i.e.,
- <i>r<sub>&#916;T</sub><sup>i</sup> &lt; r<sub>&#916;T</sub><sup>i+1</sup></i>.
- Both vectors, <i>r<sub>&#916;T</sub></i> and <i>f</i>
- must have the same size.
- </p>
- </html>",
+<p>
+Data record for performance data that describe the normalized
+temperature difference
+versus the change in the rate of heating or cooling.
+The normalized temperature difference is defined as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+r<sub>&#916;T</sub><sup>i</sup>=
+&#916;T<sup>i</sup> &frasl; &#916;T<sub>nominal</sub>
+=
+(T<sub>w</sub><sup>i</sup>-T<sub>z</sub>)
+&frasl;
+(T<sub>w,nominal</sub>-T<sub>z</sub>),
+</p>
+<p>
+where
+<i>T<sub>w</sub><sup>i</sup></i> is the water inlet temperature,
+<i>T<sub>z</sub></i> is the zone air temperature and
+<i>T<sub>w,nominal</sub></i> is the nominal water inlet temperature.
+</p>
+<p>
+The normalized temperature difference <i>r<sub>&#916;T</sub></i> must be strictly increasing, i.e.,
+<i>r<sub>&#916;T</sub><sup>i</sup> &lt; r<sub>&#916;T</sub><sup>i+1</sup></i>.
+Both vectors, <i>r<sub>&#916;T</sub></i> and <i>f</i>
+must have the same size.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureDifference;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/WaterFlow.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/WaterFlow.mo
index 5cfbf4c57b..57af5446d9 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/WaterFlow.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/BaseClasses/WaterFlow.mo
@@ -7,28 +7,28 @@ record WaterFlow "Record for water parameters"
     "Normalized performance factor at these flow rates";
 
   annotation (Documentation(info="<html>
- <p>
- Data record for performance data that describe the water volume flow rate versus
- the change in the rate of heating or cooling.
- </p>
- <p>
- The normamlized volume flow rate <i>r<sub>V</sub></i> must be strictly increasing, i.e.,
- <i>r<sub>V</sub><sup>i</sup> &lt; r<sub>V</sub><sup>i+1</sup></i>.
- Both vectors, <i>r<sub>V</sub></i> and <i>f</i>
- must have the same size.
- </p>
- </html>",
+<p>
+Data record for performance data that describe the water volume flow rate versus
+the change in the rate of heating or cooling.
+</p>
+<p>
+The normamlized volume flow rate <i>r<sub>V</sub></i> must be strictly increasing, i.e.,
+<i>r<sub>V</sub><sup>i</sup> &lt; r<sub>V</sub><sup>i+1</sup></i>.
+Both vectors, <i>r<sub>V</sub></i> and <i>f</i>
+must have the same size.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterFlow;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/Generic.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/Generic.mo
index e86a8bf560..bd021cef16 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/Generic.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/Generic.mo
@@ -38,20 +38,20 @@ record Generic "Generic data record for active beam"
 
   annotation (defaultComponentName="per",
 Documentation(revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Performance data for a generic active beam.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Performance data for a generic active beam.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Generic;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/Trox.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/Trox.mo
index 061a026c10..36c1d115c1 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/Trox.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Data/Trox.mo
@@ -21,21 +21,21 @@ package Trox "Performance data for Trox"
   "Performance data for Trox DID 632A for cooling mode"
        annotation (
     Documentation(revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Performance data for Trox active beam for cooling mode.
- </p>
- </html>"));
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Performance data for Trox active beam for cooling mode.
+</p>
+</html>"));
 
 
   record DID632A_nozzleH_length6ft_heating =
@@ -59,27 +59,27 @@ package Trox "Performance data for Trox"
   "Performance data for Trox DID 632A for heating mode"
       annotation (
     Documentation(revisions="<html>
- <ul>
- <li>
- June 13, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Performance data for Trox active beam for heating mode.
- </p>
- </html>"));
+<ul>
+<li>
+June 13, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Performance data for Trox active beam for heating mode.
+</p>
+</html>"));
 
 
 annotation (Documentation(revisions="", info="<html>
- <p>
- Package with performance data for active beams from Trox.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Package with performance data for active beams from Trox.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Trox;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/CoolingAndHeating.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/CoolingAndHeating.mo
index 3b50e9ef53..f67e94ab41 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/CoolingAndHeating.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/CoolingAndHeating.mo
@@ -141,37 +141,37 @@ equation
         "Simulate and plot"),
     Icon(coordinateSystem(extent={{-120,-120},{120,120}})),
      Documentation(info="<html>
- <p>
- This example tests the implementation of
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating</a>
- for both heating and cooling mode. An air volume is maintained at a temperature between <i>22&deg;</i>C and
- <i>25&deg;</i>C by two controllers that regulate the water flow rate in the active beam.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- June 25, 2016, by Michael Wetter:<br/>
- Changed medium start temperature to avoid conflicting
- start values of the same precedence in Dymola 2016.
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/485\">
- issue 485</a>.
- </li>
- <li>
- June 14, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the implementation of
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating</a>
+for both heating and cooling mode. An air volume is maintained at a temperature between <i>22&deg;</i>C and
+<i>25&deg;</i>C by two controllers that regulate the water flow rate in the active beam.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+June 25, 2016, by Michael Wetter:<br/>
+Changed medium start temperature to avoid conflicting
+start values of the same precedence in Dymola 2016.
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/485\">
+issue 485</a>.
+</li>
+<li>
+June 14, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoolingAndHeating;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/CoolingOnly.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/CoolingOnly.mo
index a29b199e37..e7ad1b04e5 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/CoolingOnly.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/CoolingOnly.mo
@@ -108,28 +108,28 @@ equation
         "Simulate and plot"),
     Icon(coordinateSystem(extent={{-120,-120},{120,120}})),
      Documentation(info="<html>
- <p>
- This example tests the implementation of <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Cooling\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.Cooling</a>.
- An air volume is maintained at a temperature below <i>25&deg;</i>C by a controller
- that regulates the water flow rate in the active beam.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- June 14, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the implementation of <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Cooling\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.Cooling</a>.
+An air volume is maintained at a temperature below <i>25&deg;</i>C by a controller
+that regulates the water flow rate in the active beam.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+June 14, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoolingOnly;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/HeatingOnly.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/HeatingOnly.mo
index 7f4519e107..0e5496814a 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/HeatingOnly.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Examples/HeatingOnly.mo
@@ -121,28 +121,28 @@ equation
         "Simulate and plot"),
     Icon(coordinateSystem(extent={{-120,-120},{120,120}})),
      Documentation(info="<html>
- <p>
- This example tests the implementation of <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating</a>, but operates it only in heating mode.
- An air volume is maintained at a temperature above <i>22&deg;</i>C by a controller
- that regulates the water flow rate in the active beam.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- June 14, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the implementation of <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating</a>, but operates it only in heating mode.
+An air volume is maintained at a temperature above <i>22&deg;</i>C by a controller
+that regulates the water flow rate in the active beam.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+June 14, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeatingOnly;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeams.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeams.mo
index f88be3a703..169c8dff1e 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeams.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeams.mo
@@ -184,34 +184,34 @@ equation
    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeams.mos"
         "Simulate and plot"),
      Documentation(info="<html>
- <p>
- This model validates the scaling of the heat tranfer and pressure drop for
- <code>nBeams &gt; 1</code>.
- </p>
- <p>
- It uses two instances of
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating</a>,
- one with
- <code>nBeams = 1</code> and one with
- <code>nBeams = 10</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- June 14, 2016, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- May 20, 2016, by Alessandro Maccarini:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates the scaling of the heat tranfer and pressure drop for
+<code>nBeams &gt; 1</code>.
+</p>
+<p>
+It uses two instances of
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.CoolingAndHeating</a>,
+one with
+<code>nBeams = 1</code> and one with
+<code>nBeams = 10</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+June 14, 2016, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+May 20, 2016, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end NumberOfBeams;
diff --git a/AixLib/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeamsDynamics.mo b/AixLib/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeamsDynamics.mo
index efb1601ae8..1067360cac 100644
--- a/AixLib/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeamsDynamics.mo
+++ b/AixLib/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeamsDynamics.mo
@@ -24,21 +24,21 @@ experiment(Tolerance=1e-6, StopTime=500),
    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/ActiveBeams/Validation/NumberOfBeamsDynamics.mos"
         "Simulate and plot"),
   Documentation(info="<html>
- <p>
- This model validates whether the transient response is indeed
- independent of the number of beams.
- The model is similar to
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Validation.NumberOfBeams\">
- AixLib.Fluid.HeatExchangers.ActiveBeams.Validation.NumberOfBeams</a>,
- except that it is configured with a dynamic balance and non-default initial conditions.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 24, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates whether the transient response is indeed
+independent of the number of beams.
+The model is similar to
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ActiveBeams.Validation.NumberOfBeams\">
+AixLib.Fluid.HeatExchangers.ActiveBeams.Validation.NumberOfBeams</a>,
+except that it is configured with a dynamic balance and non-default initial conditions.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 24, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end NumberOfBeamsDynamics;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HACoilInside.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HACoilInside.mo
index 2a789af8cd..c4580871d1 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HACoilInside.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HACoilInside.mo
@@ -31,17 +31,17 @@ equation
         "Simulate and plot"),
         experiment(Tolerance=1e-6, StopTime=15),
         Documentation(info="<html>
-         <p>
-         Test model for <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.HACoilInside\">
-         AixLib.Fluid.HeatExchanger.BaseClassess.HACoilInside</a>.
-         </p>
-         </html>",revisions="<html>
- <ul>
- <li>
- May 11, 2013, by Michael Wetter:<br/>
- First version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        <p>
+        Test model for <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.HACoilInside\">
+        AixLib.Fluid.HeatExchanger.BaseClassess.HACoilInside</a>.
+        </p>
+        </html>", revisions="<html>
+<ul>
+<li>
+May 11, 2013, by Michael Wetter:<br/>
+First version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HACoilInside;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HADryCoil.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HADryCoil.mo
index 1924e54b39..ca26ce1154 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HADryCoil.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HADryCoil.mo
@@ -77,17 +77,17 @@ equation
   experiment(StopTime=80.0,
              Tolerance=1E-6),
   Documentation(info="<html>
- <p>
- Test model for <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.HADryCoil\">
- AixLib.Fluid.HeatExchangers.BaseClasses.HADryCoil</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 9, 2017, by Michael Wetter:<br/>
- First version.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Test model for <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.HADryCoil\">
+AixLib.Fluid.HeatExchangers.BaseClasses.HADryCoil</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 9, 2017, by Michael Wetter:<br/>
+First version.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HADryCoil;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HANaturalCylinder.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HANaturalCylinder.mo
index ad9a15044f..3e54d49fc4 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HANaturalCylinder.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/Examples/HANaturalCylinder.mo
@@ -34,10 +34,10 @@ equation
         "Simulate and plot"),
         experiment(Tolerance=1e-6, StopTime=250),
         Documentation(info="<html>
-         <p>
-         Test model for <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.HANaturalCylinder\">
-         AixLib.Fluid.HeatExchangers.BaseClasses.HANaturalCylinder</a>.
-         </p>
-         </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        <p>
+        Test model for <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.HANaturalCylinder\">
+        AixLib.Fluid.HeatExchangers.BaseClasses.HANaturalCylinder</a>.
+        </p>
+        </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HANaturalCylinder;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/HACoilInside.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/HACoilInside.mo
index 90bd9ad99d..918d2edc2a 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/HACoilInside.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/HACoilInside.mo
@@ -55,24 +55,24 @@ equation
 
 annotation (                    defaultComponentName="HASin",
 Documentation(info="<html>
- <p>
- Model for convective heat transfer coefficients inside a coil.
- Optionally, the convective heat transfer coefficient can
- be computed as a function of temperature and mass flow rate.
- </p>
- </html>",
+<p>
+Model for convective heat transfer coefficients inside a coil.
+Optionally, the convective heat transfer coefficient can
+be computed as a function of temperature and mass flow rate.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 10, 2013, by Michael Wetter:<br/>
- Revised and simplified the implementation.
- </li>
- <li>
- February 26, 2013, by Peter Grant:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+May 10, 2013, by Michael Wetter:<br/>
+Revised and simplified the implementation.
+</li>
+<li>
+February 26, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={            Text(
           extent={{-66,88},{60,-2}},
@@ -91,6 +91,6 @@ revisions="<html>
           fillColor={255,255,255},
           fillPattern=FillPattern.Solid),
         Line(points={{-52,-40},{56,-40},{44,-32}}, color={175,175,175}),
-        Line(points={{56,-40},{44,-48}}, color={175,175,175})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        Line(points={{56,-40},{44,-48}}, color={175,175,175})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HACoilInside;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/HADryCoil.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/HADryCoil.mo
index 2df74d6d92..542e984f4c 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/HADryCoil.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/HADryCoil.mo
@@ -33,11 +33,11 @@ model HADryCoil
   parameter Real r_nominal(min=0)=0.5
     "Ratio between air-side and water-side convective heat transfer coefficient"
           annotation(Dialog(tab="General", group="Nominal condition"));
-  parameter Modelica.Units.SI.ThermalConductance hA_nominal_w(min=0)=
+  parameter Modelica.Units.SI.ThermalConductance hA_nominal_w(min=0) =
     UA_nominal*(r_nominal + 1)/r_nominal
     "Water side convective heat transfer coefficient"
     annotation (Dialog(tab="General", group="Nominal condition"));
-  parameter Modelica.Units.SI.ThermalConductance hA_nominal_a(min=0)=
+  parameter Modelica.Units.SI.ThermalConductance hA_nominal_a(min=0) =
     r_nominal*hA_nominal_w
     "Air side convective heat transfer coefficient, including fin resistance"
     annotation (Dialog(tab="General", group="Nominal condition"));
@@ -100,58 +100,58 @@ equation
     hA_2 = x_a * hA_nominal_a;
   end if;
 annotation (Documentation(info="<html>
- <p>
- Model for sensible convective heat transfer coefficients for an air to water coil.
- </p>
- <p>
- This model computes the convective heat transfer coefficient
- for an air to water coil.
- The parameters allow a user to enable or disable, individually
- for each medium, the mass flow and/or the temperature dependence
- of the convective heat transfer coefficients.
- For a detailed explanation of the equation, see
- the references below.
- </p>
- <h4>References</h4>
- <ul>
- <li>
- Wetter Michael,
- <a href=\"http://www.osti.gov/energycitations/product.biblio.jsp?osti_id=7353\">
- Simulation model finned water-air-coil without condensation</a>,
- LBNL-42355,
- Lawrence Berkeley National Laboratory,
- Berkeley, CA, 1999.
- </li>
- <li>
- Wetter Michael,
- <a href=\"http://www.osti.gov/energycitations/product.biblio.jsp?osti_id=7352\">
- Simulation model air-to-air plate heat exchanger</a>,
- LBNL-42354,
- Lawrence Berkeley National Laboratory,
- Berkeley, CA, 1999.
- </li>
- </ul>
- </html>",
+<p>
+Model for sensible convective heat transfer coefficients for an air to water coil.
+</p>
+<p>
+This model computes the convective heat transfer coefficient
+for an air to water coil.
+The parameters allow a user to enable or disable, individually
+for each medium, the mass flow and/or the temperature dependence
+of the convective heat transfer coefficients.
+For a detailed explanation of the equation, see
+the references below.
+</p>
+<h4>References</h4>
+<ul>
+<li>
+Wetter Michael,
+<a href=\"http://www.osti.gov/energycitations/product.biblio.jsp?osti_id=7353\">
+Simulation model finned water-air-coil without condensation</a>,
+LBNL-42355,
+Lawrence Berkeley National Laboratory,
+Berkeley, CA, 1999.
+</li>
+<li>
+Wetter Michael,
+<a href=\"http://www.osti.gov/energycitations/product.biblio.jsp?osti_id=7352\">
+Simulation model air-to-air plate heat exchanger</a>,
+LBNL-42354,
+Lawrence Berkeley National Laboratory,
+Berkeley, CA, 1999.
+</li>
+</ul>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 9, 2017, by Michael Wetter:<br/>
- Corrected coefficient in Taylor expansion of <code>x_a</code>.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/698\">#698</a>.
- </li>
- <li>
- June 8, 2010, by Michael Wetter:<br/>
- Fixed bug in computation of <code>s_w</code>.
- The old implementation used the current inlet water temperature instead
- of the design condition that corresponds to <code>UA_nominal</code>.
- </li>
- <li>
- April 16, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 9, 2017, by Michael Wetter:<br/>
+Corrected coefficient in Taylor expansion of <code>x_a</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/698\">#698</a>.
+</li>
+<li>
+June 8, 2010, by Michael Wetter:<br/>
+Fixed bug in computation of <code>s_w</code>.
+The old implementation used the current inlet water temperature instead
+of the design condition that corresponds to <code>UA_nominal</code>.
+</li>
+<li>
+April 16, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={            Text(
           extent={{-60,90},{66,0}},
@@ -218,6 +218,6 @@ revisions="<html>
           extent={{30,-66},{50,-88}},
           lineColor={0,0,0},
           fillColor={0,0,0},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HADryCoil;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/HANaturalCylinder.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/HANaturalCylinder.mo
index df6903e431..83c9e5105d 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/HANaturalCylinder.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/HANaturalCylinder.mo
@@ -134,59 +134,59 @@ equation
   hA = h*A;
   annotation (            defaultComponentName="hNat",
             Documentation(info="<html>
-             <p>
-             This model calculates the convection coefficient <i>h</i> for natural convection
-             from a cylinder submerged in fluid. <i>h</i> is calcualted using Eq 9.34 from
-             Incropera and DeWitt (1996).
-             Output of the block is the <i>hA</i> value.
-             </p>
-             <p>
-             The Nusselt number is computed as
-             </p>
-             <p align=\"center\" style=\"font-style:italic;\">
-             Nu<sub>D</sub> = (0.6 + (0.387 Ra<sub>D</sub><sup>(1/6)</sup>)/(1+(0.559 Pr)<sup>
-             (9/16)</sup>)<sup>(8/27)</sup>)<sup>2</sup>);
-             </p>
-             <p>
-             where <i>Nu<sub>D</sub></i> is the Nusselt number, <i>Ra<sub>D</sub></i> is the
-             Rayleigh number and
-             <i>Pr</i> is the Prandtl number.<br/>
-             This correclation is accurate for <i>Ra<sub>D</sub></i> less than 10<sup>12</sup>.
-             </p>
-             <p>
-             <i>h</i> is then calculated from the Nusselt number. The equation is
-             </p>
-             <p align=\"center\" style=\"font-style:italic;\">
-             h = Nu<sub>D</sub> k/D
-             </p>
-             <p>
-             where <i>k</i> is the thermal conductivity of the fluid and <i>D</i> is the diameter
-             of the submerged cylinder.
-             </p>
-             <h4>References</h4>
-             <p>
-             Fundamentals of Heat and Mass Transfer (Fourth Edition), Frank Incropera and David
-             DeWitt, John Wiley and Sons, 1996
-             </p>
-             </html>",revisions="<html>
-             <ul>
- <li>
- August 29, 2014 by Michael Wetter:<br/>
- Refactored function calls for medium properties.
- </li>
- <li>
- May 10, 2013 by Michael Wetter:<br/>
- Revised implementation to use <code>hA_nominal</code> as a parameter, and compute the
- associated surface area <code>A</code>. This revision was required to have a consistent
- computation of the <code>hA</code> values inside and outside of the coil in the
- heat exchanger model of the water tank.
- </li>
- <li>
- February 26, 2013 by Peter Grant:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+            <p>
+            This model calculates the convection coefficient <i>h</i> for natural convection
+            from a cylinder submerged in fluid. <i>h</i> is calcualted using Eq 9.34 from
+            Incropera and DeWitt (1996).
+            Output of the block is the <i>hA</i> value.
+            </p>
+            <p>
+            The Nusselt number is computed as
+            </p>
+            <p align=\"center\" style=\"font-style:italic;\">
+            Nu<sub>D</sub> = (0.6 + (0.387 Ra<sub>D</sub><sup>(1/6)</sup>)/(1+(0.559 Pr)<sup>
+            (9/16)</sup>)<sup>(8/27)</sup>)<sup>2</sup>);
+            </p>
+            <p>
+            where <i>Nu<sub>D</sub></i> is the Nusselt number, <i>Ra<sub>D</sub></i> is the
+            Rayleigh number and
+            <i>Pr</i> is the Prandtl number.<br/>
+            This correclation is accurate for <i>Ra<sub>D</sub></i> less than 10<sup>12</sup>.
+            </p>
+            <p>
+            <i>h</i> is then calculated from the Nusselt number. The equation is
+            </p>
+            <p align=\"center\" style=\"font-style:italic;\">
+            h = Nu<sub>D</sub> k/D
+            </p>
+            <p>
+            where <i>k</i> is the thermal conductivity of the fluid and <i>D</i> is the diameter
+            of the submerged cylinder.
+            </p>
+            <h4>References</h4>
+            <p>
+            Fundamentals of Heat and Mass Transfer (Fourth Edition), Frank Incropera and David
+            DeWitt, John Wiley and Sons, 1996
+            </p>
+            </html>", revisions="<html>
+            <ul>
+<li>
+August 29, 2014 by Michael Wetter:<br/>
+Refactored function calls for medium properties.
+</li>
+<li>
+May 10, 2013 by Michael Wetter:<br/>
+Revised implementation to use <code>hA_nominal</code> as a parameter, and compute the
+associated surface area <code>A</code>. This revision was required to have a consistent
+computation of the <code>hA</code> values inside and outside of the coil in the
+heat exchanger model of the water tank.
+</li>
+<li>
+February 26, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={                       Text(
           extent={{-66,88},{60,-2}},
           textColor={0,0,0},
@@ -243,6 +243,6 @@ equation
         Line(
           points={{42,-18},{46,-38},{36,-52},{48,-72},{40,-86}},
           color={175,175,175},
-          smooth=Smooth.Bezier)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          smooth=Smooth.Bezier)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HANaturalCylinder;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/PartialEffectiveness.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/PartialEffectiveness.mo
index 3cb9fb5342..29b290b467 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/PartialEffectiveness.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/PartialEffectiveness.mo
@@ -14,12 +14,16 @@ partial model PartialEffectiveness
     fra_a2 * Medium2.temperature(state_a2_inflow) + fra_b2 * Medium2.temperature(state_b2_inflow) else
     Medium2.temperature(state_a2_inflow)
     "Inlet temperature medium 2";
-  Modelica.Units.SI.ThermalConductance C1_flow=abs(m1_flow)*(if
+  Modelica.Units.SI.ThermalConductance C1_flow(
+    min=0,
+    nominal=m1_flow_nominal*cp1_default)=abs(m1_flow)*(if
       allowFlowReversal1 then fra_a1*Medium1.specificHeatCapacityCp(
       state_a1_inflow) + fra_b1*Medium1.specificHeatCapacityCp(state_b1_inflow)
        else Medium1.specificHeatCapacityCp(state_a1_inflow))
     "Heat capacity flow rate medium 1";
-  Modelica.Units.SI.ThermalConductance C2_flow=abs(m2_flow)*(if
+  Modelica.Units.SI.ThermalConductance C2_flow(
+    min=0,
+    nominal=m2_flow_nominal*cp2_default)=abs(m2_flow)*(if
       allowFlowReversal2 then fra_a2*Medium2.specificHeatCapacityCp(
       state_a2_inflow) + fra_b2*Medium2.specificHeatCapacityCp(state_b2_inflow)
        else Medium2.specificHeatCapacityCp(state_a2_inflow))
@@ -31,11 +35,20 @@ partial model PartialEffectiveness
 protected
   parameter Real delta=1E-3 "Parameter used for smoothing";
 
-  parameter Modelica.Units.SI.SpecificHeatCapacity cp1_default(fixed=false)
+  parameter Modelica.Units.SI.SpecificHeatCapacity cp1_default =
+    Medium1.specificHeatCapacityCp(Medium1.setState_pTX(
+      Medium1.p_default,
+      Medium1.T_default,
+      Medium1.X_default))
     "Specific heat capacity of medium 1 at default medium state";
-  parameter Modelica.Units.SI.SpecificHeatCapacity cp2_default(fixed=false)
+  parameter Modelica.Units.SI.SpecificHeatCapacity cp2_default =
+    Medium2.specificHeatCapacityCp(Medium2.setState_pTX(
+      Medium2.p_default,
+      Medium2.T_default,
+      Medium2.X_default))
     "Specific heat capacity of medium 2 at default medium state";
-  parameter Modelica.Units.SI.ThermalConductance CMin_flow_small(fixed=false)
+  parameter Modelica.Units.SI.ThermalConductance CMin_flow_small =
+    min(m1_flow_small*cp1_default, m2_flow_small*cp2_default)
     "Small value for smoothing of minimum heat capacity flow rate";
   Real fra_a1(min=0, max=1) = if allowFlowReversal1
     then Modelica.Fluid.Utilities.regStep(
@@ -61,16 +74,6 @@ protected
     then 1-fra_a2
     else 0
     "Fraction of incoming state taken from port b2 (used to avoid excessive calls to regStep)";
-initial equation
-  cp1_default = Medium1.specificHeatCapacityCp(Medium1.setState_pTX(
-    Medium1.p_default,
-    Medium1.T_default,
-    Medium1.X_default));
-  cp2_default = Medium2.specificHeatCapacityCp(Medium2.setState_pTX(
-    Medium2.p_default,
-    Medium2.T_default,
-    Medium2.X_default));
-  CMin_flow_small = min(m1_flow_small*cp1_default, m2_flow_small*cp2_default);
 
   annotation (
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
@@ -81,83 +84,91 @@ initial equation
           fillColor={95,95,95},
           fillPattern=FillPattern.Solid)}),
     Documentation(info="<html>
- <p>
- Partial model to implement heat exchanger models.
- </p>
- <p>
- Classes that extend this model need to implement heat and
- mass balance equations in a form like
- </p>
- <pre>
-   // transferred heat
-   Q1_flow = eps * QMax_flow;
-   // no heat loss to ambient
-   0 = Q1_flow + Q2_flow;
-   // no mass exchange
-   mXi1_flow = zeros(Medium1.nXi);
-   mXi2_flow = zeros(Medium2.nXi);
- </pre>
- <p>
- Thus, if medium 1 is heated in this device, then <code>Q1_flow &gt; 0</code>
- and <code>QMax_flow &gt; 0</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 21, 2019, by Filip Jorissen:<br/>
- Revised implementation of all equations
- such that a binding equation is used. 
- I.e. we set the variable value at the variable definition
- instead of using the equation section.
- This allows overwriting the equation
- when extending the model.<br/>
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1102\">#1102</a>.
- </li>
- <li>
- April 30, 2018, by Filip Jorissen:<br/>
- Set <code>prescribedHeatFlowRate1=true</code> and 
- <code>prescribedHeatFlowRate2=true</code>.<br/>
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/907\">#907</a>.
- </li>
- <li>
- June 9, 2015 by Michael Wetter:<br/>
- Changed type of <code>T_in1</code> and <code>T_in2</code>
- to <code>Medium1.Temperature</code> and <code>Medium2.Temperature</code>
- to avoid an error because of conflicting start values if
- <a href=\"modelica://AixLib.Examples.ChillerPlant.BaseClasses.Controls.Examples.ChillerSetPointControl\">
- Buildings.Examples.ChillerPlant.BaseClasses.Controls.Examples.ChillerSetPointControl</a>
- is translated using pedantic mode in Dymola 2016.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
- </li>
- <li>
- October 8, 2011, by Michael Wetter:<br/>
- Set <code>show_T=false</code> to avoid state events near zero flow.
- </li>
- <li>
- August 31, 2011, by Michael Wetter:<br/>
- Removed unused variables <code>gai1</code> and <code>gai2</code>.
- </li>
- <li>
- February 12, 2010, by Michael Wetter:<br/>
- Changed model structure to implement effectiveness-NTU model.
- </li>
- <li>
- January 28, 2010, by Michael Wetter:<br/>
- Added regularization near zero flow.
- </li>
- <li>
- October 2, 2009, by Michael Wetter:<br/>
- Changed computation of inlet temperatures to use
- <code>state_*_inflow</code> which is already known in base class.
- </li>
- <li>
- April 28, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model to implement heat exchanger models.
+</p>
+<p>
+Classes that extend this model need to implement heat and
+mass balance equations in a form like
+</p>
+<pre>
+  // transferred heat
+  Q1_flow = eps * QMax_flow;
+  // no heat loss to ambient
+  0 = Q1_flow + Q2_flow;
+  // no mass exchange
+  mXi1_flow = zeros(Medium1.nXi);
+  mXi2_flow = zeros(Medium2.nXi);
+</pre>
+<p>
+Thus, if medium 1 is heated in this device, then <code>Q1_flow &gt; 0</code>
+and <code>QMax_flow &gt; 0</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 27, 2023, by Michael Wetter:<br/>
+Set nominal and min attributes for capacity flow rates.<br/>
+Moved assignments from <code>initial equation</code> to parameter declaration.
+This avoids a warning in Dymola 2023x about non-literal nominal values.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3360\">#3360</a>.
+</li>
+<li>
+February 21, 2019, by Filip Jorissen:<br/>
+Revised implementation of all equations
+such that a binding equation is used.
+I.e. we set the variable value at the variable definition
+instead of using the equation section.
+This allows overwriting the equation
+when extending the model.<br/>
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1102\">#1102</a>.
+</li>
+<li>
+April 30, 2018, by Filip Jorissen:<br/>
+Set <code>prescribedHeatFlowRate1=true</code> and
+<code>prescribedHeatFlowRate2=true</code>.<br/>
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/907\">#907</a>.
+</li>
+<li>
+June 9, 2015 by Michael Wetter:<br/>
+Changed type of <code>T_in1</code> and <code>T_in2</code>
+to <code>Medium1.Temperature</code> and <code>Medium2.Temperature</code>
+to avoid an error because of conflicting start values if
+<a href=\"modelica://Buildings.Examples.ChillerPlant.BaseClasses.Controls.Examples.ChillerSetPointControl\">
+Buildings.Examples.ChillerPlant.BaseClasses.Controls.Examples.ChillerSetPointControl</a>
+is translated using pedantic mode in Dymola 2016.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
+</li>
+<li>
+October 8, 2011, by Michael Wetter:<br/>
+Set <code>show_T=false</code> to avoid state events near zero flow.
+</li>
+<li>
+August 31, 2011, by Michael Wetter:<br/>
+Removed unused variables <code>gai1</code> and <code>gai2</code>.
+</li>
+<li>
+February 12, 2010, by Michael Wetter:<br/>
+Changed model structure to implement effectiveness-NTU model.
+</li>
+<li>
+January 28, 2010, by Michael Wetter:<br/>
+Added regularization near zero flow.
+</li>
+<li>
+October 2, 2009, by Michael Wetter:<br/>
+Changed computation of inlet temperatures to use
+<code>state_*_inflow</code> which is already known in base class.
+</li>
+<li>
+April 28, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialEffectiveness;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/PartialEffectivenessNTU.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/PartialEffectivenessNTU.mo
index 3e166c6fff..9efc4e778c 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/PartialEffectivenessNTU.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/PartialEffectivenessNTU.mo
@@ -14,13 +14,20 @@ model PartialEffectivenessNTU
   parameter con configuration "Heat exchanger configuration"
     annotation (Evaluate=true);
 
+  constant Boolean use_dynamicFlowRegime = false
+    "If true, flow regime is determined using actual flow rates";
+  // This switch is declared as a constant instead of a parameter
+  //   as users typically need not to change this setting,
+  //   and setting it true may generate events.
+  //   See discussions in https://github.com/ibpsa/modelica-ibpsa/pull/1683
+
   parameter Boolean use_Q_flow_nominal = true
     "Set to true to specify Q_flow_nominal and temperatures, or to false to specify effectiveness"
     annotation (Evaluate=true,
                 Dialog(group="Nominal thermal performance"));
 
-  parameter Modelica.Units.SI.HeatFlowRate Q_flow_nominal(fixed=
-        use_Q_flow_nominal)
+  parameter Modelica.Units.SI.HeatFlowRate Q_flow_nominal(
+    fixed=use_Q_flow_nominal)
     "Nominal heat flow rate (positive for heat transfer from 1 to 2)"
     annotation (Dialog(group="Nominal thermal performance", enable=
           use_Q_flow_nominal));
@@ -54,7 +61,7 @@ protected
      p=Medium1.p_default,
      X=Medium1.X_default[1:Medium1.nXi]) "Default state for medium 1";
   final parameter Medium2.ThermodynamicState sta2_default = Medium2.setState_pTX(
-     T=Medium1.T_default,
+     T=Medium2.T_default,
      p=Medium2.p_default,
      X=Medium2.X_default[1:Medium2.nXi]) "Default state for medium 2";
 
@@ -83,10 +90,10 @@ protected
   flo flowRegime(fixed=false, start=flowRegime_nominal)
     "Heat exchanger flow regime";
 initial equation
-  assert(m1_flow_nominal > 0,
+  assert(m1_flow_nominal > Modelica.Constants.eps,
     "m1_flow_nominal must be positive, m1_flow_nominal = " + String(
     m1_flow_nominal));
-  assert(m2_flow_nominal > 0,
+  assert(m2_flow_nominal > Modelica.Constants.eps,
     "m2_flow_nominal must be positive, m2_flow_nominal = " + String(
     m2_flow_nominal));
 
@@ -153,19 +160,33 @@ initial equation
   UA_nominal = NTU_nominal*CMin_flow_nominal;
 equation
   // Assign the flow regime for the given heat exchanger configuration and capacity flow rates
-  if (configuration == con.ParallelFlow) then
-    flowRegime = if (C1_flow*C2_flow >= 0) then flo.ParallelFlow else flo.CounterFlow;
-  elseif (configuration == con.CounterFlow) then
-    flowRegime = if (C1_flow*C2_flow >= 0) then flo.CounterFlow else flo.ParallelFlow;
-  elseif (configuration == con.CrossFlowUnmixed) then
-    flowRegime = flo.CrossFlowUnmixed;
-  elseif (configuration == con.CrossFlowStream1MixedStream2Unmixed) then
-    flowRegime = if (C1_flow < C2_flow) then flo.CrossFlowCMinMixedCMaxUnmixed
-       else flo.CrossFlowCMinUnmixedCMaxMixed;
+  if use_dynamicFlowRegime then
+    if (configuration == con.ParallelFlow) then
+      flowRegime = if (C1_flow*C2_flow >= 0) then flo.ParallelFlow else flo.CounterFlow;
+    elseif (configuration == con.CounterFlow) then
+      flowRegime = if (C1_flow*C2_flow >= 0) then flo.CounterFlow else flo.ParallelFlow;
+    elseif (configuration == con.CrossFlowUnmixed) then
+      flowRegime = flo.CrossFlowUnmixed;
+    elseif (configuration == con.CrossFlowStream1MixedStream2Unmixed) then
+      flowRegime = if (C1_flow < C2_flow) then flo.CrossFlowCMinMixedCMaxUnmixed
+         else flo.CrossFlowCMinUnmixedCMaxMixed;
+    else
+      // have ( configuration == con.CrossFlowStream1UnmixedStream2Mixed)
+      flowRegime = if (C1_flow < C2_flow) then flo.CrossFlowCMinUnmixedCMaxMixed
+         else flo.CrossFlowCMinMixedCMaxUnmixed;
+    end if;
   else
-    // have ( configuration == con.CrossFlowStream1UnmixedStream2Mixed)
-    flowRegime = if (C1_flow < C2_flow) then flo.CrossFlowCMinUnmixedCMaxMixed
-       else flo.CrossFlowCMinMixedCMaxUnmixed;
+    flowRegime = flowRegime_nominal;
+    assert(noEvent(m1_flow > -0.1 * m1_flow_nominal)
+       and noEvent(m2_flow > -0.1 * m2_flow_nominal),
+"*** Warning in " + getInstanceName() +
+      ": The flow direction reversed.
+      However, because the constant use_dynamicFlowRegime is set to false,
+      the model does not change equations based on the actual flow regime.
+      To switch equations based on the actual flow regime during the simulation,
+      set the constant use_dynamicFlowRegime=true.
+      Note that this can lead to slow simulation because of events.",
+      level = AssertionLevel.warning);
   end if;
 
   // Effectiveness
@@ -188,80 +209,112 @@ equation
           fillPattern=FillPattern.Solid)}),
 defaultComponentName="hex",
     Documentation(info="<html>
- <p>
- Partial model of a heat exchanger without humidity condensation.
- This model transfers heat in the amount of
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   Q = Q<sub>max</sub>  &epsilon;<br/>
-   &epsilon; = f(NTU, Z, flowRegime),
- </p>
- <p>
- where
- <i>Q<sub>max</sub></i> is the maximum heat that can be transferred,
- <i>&epsilon;</i> is the heat transfer effectiveness,
- <i>NTU</i> is the Number of Transfer Units,
- <i>Z</i> is the ratio of minimum to maximum capacity flow rate and
- <i>flowRegime</i> is the heat exchanger flow regime.
- such as
- parallel flow, cross flow or counter flow.
- </p>
- <p>
- The flow regimes depend on the heat exchanger configuration. All configurations
- defined in
- <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerConfiguration\">
- AixLib.Fluid.Types.HeatExchangerConfiguration</a>
- are supported.
- </p>
- <p>
- Models that extend from this partial model need to provide an assignment
- for <code>UA</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 25, 2021 by Baptiste Ravache:<br/>
- Added a warning for when Q_flow_nominal is specified with the wrong sign.
- </li>
- <li>
- January 10, 2018 by Michael Wetter:<br/>
- Removed variable <code>Z</code> that is not used.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1328\">issue 1328</a>.
- </li>
- <li>
- January 10, 2018 by Filip Jorissen:<br/>
- Corrected an error where the value of NTU was assigned to Z.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1328\">issue 1328</a>.
- </li>
- <li>
- February 27, 2016 by Michael Wetter:<br/>
- Introduced <code>sta1_default</code> and <code>sta2_default</code>
- to enable translation under OpenModelica.
- Removed <code>max=1</code> attribute for <code>Z</code>. This is needed as near
- zero flow, <code>Z</code> can be larger than one due to the regularization.
- As <code>Z</code> is not used in this model other than for reporting, this bound
- need not be enforced (and the calculation of <code>eps</code> is fine at these small flow rates).
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/490\">issue 490</a>.
- </li>
- <li>
- April 29, 2014 by Michael Wetter:<br/>
- Changed <code>assert</code> statement to avoid comparing
- enumeration with an integer, which triggers a warning
- in Dymola 2015.
- </li>
- <li>
- July 30, 2013 by Michael Wetter:<br/>
- Updated model to use new variable <code>mWat_flow</code>
- in the base class.
- </li>
- <li>
- February 12, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model of a heat exchanger without humidity condensation.
+This model transfers heat in the amount of
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  Q = Q<sub>max</sub>  &epsilon;<br/>
+  &epsilon; = f(NTU, Z, flowRegime),
+</p>
+<p>
+where
+<i>Q<sub>max</sub></i> is the maximum heat that can be transferred,
+<i>&epsilon;</i> is the heat transfer effectiveness,
+<i>NTU</i> is the Number of Transfer Units,
+<i>Z</i> is the ratio of minimum to maximum capacity flow rate and
+<i>flowRegime</i> is the heat exchanger flow regime.
+such as
+parallel flow, cross flow or counter flow.
+</p>
+<p>
+The flow regimes depend on the heat exchanger configuration. All configurations
+defined in
+<a href=\"modelica://AixLib.Fluid.Types.HeatExchangerConfiguration\">
+AixLib.Fluid.Types.HeatExchangerConfiguration</a>
+are supported.
+</p>
+<p>
+By default, the flow regime, such as counter flow or parallel flow,
+is kept constant based on the parameter value <code>configuration</code>.
+If a flow reverses direction, it is not changed, e.g.,
+a heat exchanger does not change from counter flow to parallel flow
+if one flow changes direction.
+To dynamically change the flow regime,
+set the constant <code>use_dynamicFlowRegime</code> to
+<code>true</code>.
+However, <code>use_dynamicFlowRegime=true</code>
+can cause slower simulation due to events.
+</p>
+<p>
+Models that extend from this partial model need to provide an assignment
+for <code>UA</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 3, 2023, by Jianjun Hu:<br/>
+Added <code>noEvent()</code> in the assertion function to avoid Optimica to not converge.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1690\">issue 1690</a>.
+</li>
+<li>
+January 24, 2023, by Hongxiang Fu:<br/>
+Set <code>flowRegime</code> to be equal to <code>flowRegime_nominal</code>
+by default. Added an assertion warning to inform the user about how to change
+this behaviour if the flow direction does need to change.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1682\">issue 1682</a>.
+</li>
+<li>
+November 11, 2023, by Michael Wetter:<br/>
+Corrected wrong temperature in assignment of <code>sta2_default</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3151\">Buildings, issue 3151</a>.
+</li>
+<li>
+February 25, 2021 by Baptiste Ravache:<br/>
+Added a warning for when Q_flow_nominal is specified with the wrong sign.
+</li>
+<li>
+January 10, 2018 by Michael Wetter:<br/>
+Removed variable <code>Z</code> that is not used.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1328\">issue 1328</a>.
+</li>
+<li>
+January 10, 2018 by Filip Jorissen:<br/>
+Corrected an error where the value of NTU was assigned to Z.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1328\">issue 1328</a>.
+</li>
+<li>
+February 27, 2016 by Michael Wetter:<br/>
+Introduced <code>sta1_default</code> and <code>sta2_default</code>
+to enable translation under OpenModelica.
+Removed <code>max=1</code> attribute for <code>Z</code>. This is needed as near
+zero flow, <code>Z</code> can be larger than one due to the regularization.
+As <code>Z</code> is not used in this model other than for reporting, this bound
+need not be enforced (and the calculation of <code>eps</code> is fine at these small flow rates).
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/490\">issue 490</a>.
+</li>
+<li>
+April 29, 2014 by Michael Wetter:<br/>
+Changed <code>assert</code> statement to avoid comparing
+enumeration with an integer, which triggers a warning
+in Dymola 2015.
+</li>
+<li>
+July 30, 2013 by Michael Wetter:<br/>
+Updated model to use new variable <code>mWat_flow</code>
+in the base class.
+</li>
+<li>
+February 12, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialEffectivenessNTU;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/PartialPrescribedOutlet.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/PartialPrescribedOutlet.mo
index d958c33a5a..8a516a3fc6 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/PartialPrescribedOutlet.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/PartialPrescribedOutlet.mo
@@ -70,52 +70,52 @@ equation
           fillPattern=FillPattern.Solid)}),
 defaultComponentName="hea",
 Documentation(info="<html>
- <p>
- Base class for model for an ideal heater, cooler, humidifier or dehumidifier
- with a prescribed outlet conditions.
- </p>
- <p>
- Models that extend this model need to configure the instance <code>outCon</code>
- and connect its input signals, in they are enabled.
- </p>
- </html>",
+<p>
+Base class for model for an ideal heater, cooler, humidifier or dehumidifier
+with a prescribed outlet conditions.
+</p>
+<p>
+Models that extend this model need to configure the instance <code>outCon</code>
+and connect its input signals, in they are enabled.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 10, 2022, by Michael Wetter:<br/>
- Propagated <code>energyDynamics</code> from instance <code>outCon</code>.
- </li>
- <li>
- April 29, 2021, by Michael Wetter:<br/>
- Removed duplicate declaration of <code>m_flow_nominal</code> which is already
- declared in the base class.<br/>
- </li>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- Updated protected model for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- <li>
- November 11, 2014, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- March 19, 2014, by Christoph Nytsch-Geusen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 10, 2022, by Michael Wetter:<br/>
+Propagated <code>energyDynamics</code> from instance <code>outCon</code>.
+</li>
+<li>
+April 29, 2021, by Michael Wetter:<br/>
+Removed duplicate declaration of <code>m_flow_nominal</code> which is already
+declared in the base class.<br/>
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+Updated protected model for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+<li>
+November 11, 2014, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+March 19, 2014, by Christoph Nytsch-Geusen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialPrescribedOutlet;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilDryRegime.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilDryRegime.mo
index 7ec3871d00..d834f1d278 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilDryRegime.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilDryRegime.mo
@@ -79,19 +79,19 @@ equation
           fillPattern=FillPattern.Solid)}), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(revisions="<html>
- <ul>
- <li>
- Jan 21, 2021, by Donghun Kim:<br/>First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>This model implements the calculation for a 100% dry coil.</p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
- for documentation.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+Jan 21, 2021, by Donghun Kim:<br/>First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>This model implements the calculation for a 100% dry coil.</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
+for documentation.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WetCoilDryRegime;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilDryWetRegime.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilDryWetRegime.mo
index 3fcb5b4d84..a3b2ad4ec3 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilDryWetRegime.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilDryWetRegime.mo
@@ -163,12 +163,12 @@ model WetCoilDryWetRegime
   Real dryFra(final unit="1", min=0, max=1)
     "Dry fraction, 0.3 means condensation occurs at 30% heat exchange length from air inlet";
 protected
-  Modelica.Units.SI.MassFlowRate mAirNonZer_flow(min=Modelica.Constants.eps)=
+  Modelica.Units.SI.MassFlowRate mAirNonZer_flow(min=Modelica.Constants.eps) =
     AixLib.Utilities.Math.Functions.smoothMax(
     x1=mAir_flow,
     x2=1E-3*mAir_flow_nominal,
     deltaX=0.25E-3*mAir_flow_nominal) "Mass flow rate of air";
-  Modelica.Units.SI.MassFlowRate mWatNonZer_flow(min=Modelica.Constants.eps)=
+  Modelica.Units.SI.MassFlowRate mWatNonZer_flow(min=Modelica.Constants.eps) =
     AixLib.Utilities.Math.Functions.smoothMax(
     x1=mWat_flow,
     x2=1E-3*mWat_flow_nominal,
@@ -231,7 +231,7 @@ equation
           textStyle={TextStyle.Bold},
           pattern=LinePattern.None,
           textString="WET",
-          lineColor={0,0,0}),
+          textColor={0,0,0}),
         Line(
           points={{20,0},{120,0}},
           color={28,108,200},
@@ -375,47 +375,47 @@ equation
           textString="QSen")}),                                  Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-140,-120},{140,120}})),
     Documentation(revisions="<html>
- <ul>
- <li>
- Jan 21, 2021, by Donghun Kim:<br/>First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model implements the switching algorithm for the dry and wet regime.
- </p>
- <p>
- The switching criteria for (counter-flow) cooling coil modes are as follows.</p>
- <p>
- R1: If the coil surface temperature at the air inlet is lower than the dew-point
- temperature at the inlet to the coil, then the cooling coil surface is fully-wet.</p>
- <p>
- R2: If the surface temperature at the air outlet section is higher than
- the dew-point temperature of the air at the inlet, then the cooling coil surface is fully-dry.</p>
- <p>
- At each point of a simulation time step, the fuzzy-modeling approach determines
- the weights for R1 and R2 respectively (namely <i>&mu;<sub>FW</sub></i> and <i>&mu;<sub>FD</sub></i>)
- from the dew-point and coil surface temperatures.</p>
- <p>
- It calculates total and sensible heat transfer rates according to the weights as follows.
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q&#775;<sub>tot</sub>=&mu;<sub>FD</sub> Q&#775;<sub>tot,FD</sub>+&mu;<sub>FW</sub> Q<sub>tot,FW</sub>
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q&#775;<sub>sen</sub>=&mu;<sub>FD</sub> Q&#775;<sub>sen,FD</sub>+&mu;<sub>FW</sub> Q<sub>sen,FW</sub>
- </p>
- <p>
- The fuzzy-modeling ensures <i>&mu;<sub>FW</sub> + &mu;<sub>FD</sub> = 1</i>,
- <i>&mu;<sub>FW</sub> &gt;=0</i> and <i>&mu;<sub>FD</sub> &gt;=0</i>, which means the fuzzy
- model outcomes of <i>Q&#775;<sub>sen</sub></i> and <i>Q&#775;<sub>tot</sub></i> are always convex combinations of heat transfer
- rates for fully-dry and fully-wet modes and therefore are always bounded by them.
- </p>
- <p>
- The modeling approach also results in <i>n</i>-th order differentiable model
- depending on the selection of the underlying membership functions. This cooling
- coil model is once continuously differentiable at the mode switches.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+Jan 21, 2021, by Donghun Kim:<br/>First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model implements the switching algorithm for the dry and wet regime.
+</p>
+<p>
+The switching criteria for (counter-flow) cooling coil modes are as follows.</p>
+<p>
+R1: If the coil surface temperature at the air inlet is lower than the dew-point
+temperature at the inlet to the coil, then the cooling coil surface is fully-wet.</p>
+<p>
+R2: If the surface temperature at the air outlet section is higher than
+the dew-point temperature of the air at the inlet, then the cooling coil surface is fully-dry.</p>
+<p>
+At each point of a simulation time step, the fuzzy-modeling approach determines
+the weights for R1 and R2 respectively (namely <i>&mu;<sub>FW</sub></i> and <i>&mu;<sub>FD</sub></i>)
+from the dew-point and coil surface temperatures.</p>
+<p>
+It calculates total and sensible heat transfer rates according to the weights as follows.
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q&#775;<sub>tot</sub>=&mu;<sub>FD</sub> Q&#775;<sub>tot,FD</sub>+&mu;<sub>FW</sub> Q<sub>tot,FW</sub>
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q&#775;<sub>sen</sub>=&mu;<sub>FD</sub> Q&#775;<sub>sen,FD</sub>+&mu;<sub>FW</sub> Q<sub>sen,FW</sub>
+</p>
+<p>
+The fuzzy-modeling ensures <i>&mu;<sub>FW</sub> + &mu;<sub>FD</sub> = 1</i>,
+<i>&mu;<sub>FW</sub> &gt;=0</i> and <i>&mu;<sub>FD</sub> &gt;=0</i>, which means the fuzzy
+model outcomes of <i>Q&#775;<sub>sen</sub></i> and <i>Q&#775;<sub>tot</sub></i> are always convex combinations of heat transfer
+rates for fully-dry and fully-wet modes and therefore are always bounded by them.
+</p>
+<p>
+The modeling approach also results in <i>n</i>-th order differentiable model
+depending on the selection of the underlying membership functions. This cooling
+coil model is once continuously differentiable at the mode switches.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WetCoilDryWetRegime;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilUARated.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilUARated.mo
index bd987e22f4..18b006f83f 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilUARated.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilUARated.mo
@@ -73,7 +73,7 @@ protected
       MediumW.specificHeatCapacityCp(staWat)
     "Isobaric specific heat capacity of water";
   parameter Modelica.Units.SI.SpecificHeatCapacity cpEff(fixed=false, min=0) "Effective specific heat: change in saturated moist air enthalpy with respect to
-     temperature along the saturation line between inlet and outlet water temperatures";
+    temperature along the saturation line between inlet and outlet water temperatures";
   parameter Modelica.Units.SI.SpecificEnthalpy LMED(fixed=false)
     "Log mean enthalpy difference";
   parameter Modelica.Units.SI.MassFlowRate UASta(
@@ -194,23 +194,23 @@ initial equation
         fillPattern=FillPattern.Solid)}), Diagram(
       coordinateSystem(preserveAspectRatio=false)),
     Documentation(revisions="<html>
- <ul>
- <li>
- February 18, 2021 by Donghun Kim:<br/>
- First implementation
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model calculates the overall heat transfer coefficient, i.e.,
- <i>UA</i>-value, from cooling coil data at rated conditions.
- </p>
- <p>
- The main limitation of the current implementation is that the rated
- conditions should correspond to a fully-dry or a fully-wet coil regime.
- The modeling uncertainty yielded by partially-wet rated conditions
- has not been assessed yet.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 18, 2021 by Donghun Kim:<br/>
+First implementation
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model calculates the overall heat transfer coefficient, i.e.,
+<i>UA</i>-value, from cooling coil data at rated conditions.
+</p>
+<p>
+The main limitation of the current implementation is that the rated
+conditions should correspond to a fully-dry or a fully-wet coil regime.
+The modeling uncertainty yielded by partially-wet rated conditions
+has not been assessed yet.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WetCoilUARated;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilWetRegime.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilWetRegime.mo
index 7a3f740a67..8021545804 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilWetRegime.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/WetCoilWetRegime.mo
@@ -67,15 +67,19 @@ model WetCoilWetRegime
     "An object to calculate the saturated enthalpy of moist air at the coil surface temperature";
   AixLib.Utilities.Psychrometrics.hSat_pTSat hSatSurEffMinM(p=pAir,TSat=273.15+1)
     "An object to calculate a lower bound of the saturated enthalpy of moist
-     air at the coil surface temperature";
+    air at the coil surface temperature";
 
   Modelica.Units.SI.SpecificHeatCapacity cpEff "Effective specific heat: change in enthalpy with respect to temperature
-      along the saturation line at the local water temperature";
+     along the saturation line at the local water temperature";
 
   Modelica.Units.SI.MassFlowRate UASta
     "Overall mass transfer coefficient for dry coil";
 
-  Real NTUAirSta(unit="1")
+  // Set start value, otherwise OpenModelica has a division by zero in the expression
+  // (1 - exp(-NTUAirSta)) of hSatSurEff
+  Real NTUAirSta(
+    start=1,
+    unit="1")
     "Number of transfer units for air-side only (NTU_a*)";
 
   Real epsSta(start=0.66, unit="1")
@@ -166,91 +170,97 @@ annotation (Icon(graphics={
         lineColor={28,108,200},
         fillColor={170,213,255},
         fillPattern=FillPattern.Solid)}), Documentation(revisions="<html>
- <ul>
- <li>
- Jan 21, 2021, by Donghun Kim:<br/>First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model implements the calculation for a 100% wet coil.
- </p>
- <p>
- The equations from Braun (1988) and Mitchell and Braun (2012a and b),
- which are essentially the extension of the <i>&epsilon;-NTU</i> approach to
- simultaneous sensible and latent heat transfer, are utilized.
- </p>
- <p>
- The mathematical equations are analogous to that of the sensible heat exchanger.
- However, the key distinction is that the heat transfer is driven by an enthalpy difference
- not by an temperature difference. This change in the driving potential results in re-defining
- capacitances and heat transfer coefficients accordingly.
- </p>
- 
- <p>
- The total heat transfer rate is expressed as
- </p>
- <p align=\"center\">
- <i> Q<sub>tot</sub>=&epsilon;* C*<sub>min </sub>
- (h<sub>air,in</sub>-h<sub>sat</sub>(T<sub>wat,in</sub>))</i>,
- </p>
- <p>
- where <i>&epsilon;*=f(Cr*,NTU*)</i> and <i>f</i> is the same <i>&epsilon;-NTU</i> relationships
- (depending on the heat exchanger configuration) for the sensible heat exchanger.
- </p>
- <p>
- <i>h<sub>air,in</sub> </i> and <i>h<sub>sat</sub></i>(<i>T<sub>wat,in</sub></i>) are
- the specific enthalpies of the incoming moist air and saturated moist air
- at the water inlet temperature.
- </p>
- <p>
- The capacitances of water and air streams are defined as
- </p>
- <p align=\"center\"><i>C*<sub>air</sub>=m<sub>air</sub></i> and
- <i>C*<sub>wat</sub>=m<sub>wat</sub>c<sub>p,wat</sub>/csat</i>,
- </p>
- <p>
- where <i>csat</i> is an specific heat capacity, which indicates the sensitivity
- of the enthalpy of the staturated moist air w.r.t. the temperature, and is defined
- here as <i>csat=(h<sub>sat</sub>(T<sub>wat,out</sub>)-h<sub>sat</sub>(T<sub>wat,in</sub>))
- /(T<sub>wat,out</sub>-T<sub>wat,in</sub>)</i>.
- </p>
- <p>
- The capacitance ratio and minimum capacitance are naturally defined as
- </p>
- <p align=\"center\"> <i>Cr*=min(C*<sub>air</sub>,C*<sub>wat</sub>)/max(C*<sub>air</sub>,C*<sub>wat</sub>)</i>
- and <i>C*<sub>min</sub>=min(C*<sub>air</sub>,C*<sub>wat</sub>)</i>.
- </p>
- <p><br/>
- The number of transfer unit for the wet-coil is defined as <i>NTU*=UA*/C*<sub>min</sub></i>, where
- </p>
- <p align=\"center\">
- <i>UA*=1/(1/(UA<sub>air</sub>/c<sub>p,air</sub>)+1/(UA<sub>wat</sub>/csat)</i>.
- </p>
- 
- <h4>References </h4>
- <p>
- Braun, James E. 1988.
- &quot;Methodologies for the Design and Control of Central Cooling Plants&quot;.
- PhD Thesis. University of Wisconsin - Madison.
- Available
- <a href=\"https://minds.wisconsin.edu/handle/1793/46694\">
- online</a>.
- </p>
- <p>
- Mitchell, John W., and James E. Braun. 2012a.
- Principles of heating, ventilation, and air conditioning in buildings.
- Hoboken, N.J.: Wiley.
- </p>
- <p>
- Mitchell, John W., and James E. Braun. 2012b.
- &quot;Supplementary Material Chapter 2: Heat Exchangers for Cooling Applications&quot;.
- Excerpt from Principles of heating, ventilation, and air conditioning in buildings.
- Hoboken, N.J.: Wiley.
- Available
- <a href=\"http://bcs.wiley.com/he-bcs/Books?action=index&amp;itemId=0470624574&amp;bcsId=7185\">
- online</a>.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 18, 2023, by Michael Wetter:<br/>
+Set start value for <code>NTUAirSta</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1728\">IBPSA, #1728</a>.
+</li>
+<li>
+Jan 21, 2021, by Donghun Kim:<br/>First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model implements the calculation for a 100% wet coil.
+</p>
+<p>
+The equations from Braun (1988) and Mitchell and Braun (2012a and b),
+which are essentially the extension of the <i>&epsilon;-NTU</i> approach to
+simultaneous sensible and latent heat transfer, are utilized.
+</p>
+<p>
+The mathematical equations are analogous to that of the sensible heat exchanger.
+However, the key distinction is that the heat transfer is driven by an enthalpy difference
+not by an temperature difference. This change in the driving potential results in re-defining
+capacitances and heat transfer coefficients accordingly.
+</p>
+
+<p>
+The total heat transfer rate is expressed as
+</p>
+<p align=\"center\">
+<i> Q<sub>tot</sub>=&epsilon;* C*<sub>min </sub>
+(h<sub>air,in</sub>-h<sub>sat</sub>(T<sub>wat,in</sub>))</i>,
+</p>
+<p>
+where <i>&epsilon;*=f(Cr*,NTU*)</i> and <i>f</i> is the same <i>&epsilon;-NTU</i> relationships
+(depending on the heat exchanger configuration) for the sensible heat exchanger.
+</p>
+<p>
+<i>h<sub>air,in</sub> </i> and <i>h<sub>sat</sub></i>(<i>T<sub>wat,in</sub></i>) are
+the specific enthalpies of the incoming moist air and saturated moist air
+at the water inlet temperature.
+</p>
+<p>
+The capacitances of water and air streams are defined as
+</p>
+<p align=\"center\"><i>C*<sub>air</sub>=m<sub>air</sub></i> and
+<i>C*<sub>wat</sub>=m<sub>wat</sub>c<sub>p,wat</sub>/csat</i>,
+</p>
+<p>
+where <i>csat</i> is an specific heat capacity, which indicates the sensitivity
+of the enthalpy of the staturated moist air w.r.t. the temperature, and is defined
+here as <i>csat=(h<sub>sat</sub>(T<sub>wat,out</sub>)-h<sub>sat</sub>(T<sub>wat,in</sub>))
+/(T<sub>wat,out</sub>-T<sub>wat,in</sub>)</i>.
+</p>
+<p>
+The capacitance ratio and minimum capacitance are naturally defined as
+</p>
+<p align=\"center\"> <i>Cr*=min(C*<sub>air</sub>,C*<sub>wat</sub>)/max(C*<sub>air</sub>,C*<sub>wat</sub>)</i>
+and <i>C*<sub>min</sub>=min(C*<sub>air</sub>,C*<sub>wat</sub>)</i>.
+</p>
+<p><br/>
+The number of transfer unit for the wet-coil is defined as <i>NTU*=UA*/C*<sub>min</sub></i>, where
+</p>
+<p align=\"center\">
+<i>UA*=1/(1/(UA<sub>air</sub>/c<sub>p,air</sub>)+1/(UA<sub>wat</sub>/csat)</i>.
+</p>
+
+<h4>References </h4>
+<p>
+Braun, James E. 1988.
+&quot;Methodologies for the Design and Control of Central Cooling Plants&quot;.
+PhD Thesis. University of Wisconsin - Madison.
+Available
+<a href=\"https://minds.wisconsin.edu/handle/1793/46694\">
+online</a>.
+</p>
+<p>
+Mitchell, John W., and James E. Braun. 2012a.
+Principles of heating, ventilation, and air conditioning in buildings.
+Hoboken, N.J.: Wiley.
+</p>
+<p>
+Mitchell, John W., and James E. Braun. 2012b.
+&quot;Supplementary Material Chapter 2: Heat Exchangers for Cooling Applications&quot;.
+Excerpt from Principles of heating, ventilation, and air conditioning in buildings.
+Hoboken, N.J.: Wiley.
+Available
+<a href=\"http://bcs.wiley.com/he-bcs/Books?action=index&amp;itemId=0470624574&amp;bcsId=7185\">
+online</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WetCoilWetRegime;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/determineWaterIndex.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/determineWaterIndex.mo
index a4506dfb33..bc00600210 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/determineWaterIndex.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/determineWaterIndex.mo
@@ -22,27 +22,27 @@ algorithm
     "Did not find medium species 'water' in the medium model. " +
     "Change medium model.");
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- April 19, 2017, by Michael Wetter:<br/>
- Removed assertion as function is valid also for other values than <code>N==2</code>.
- </li>
- <li>
- March 17, 2017, by Michael O'Keefe:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Given an array of strings representing substance names, this function returns
- the integer index of the substance named \"water\" (case-insensitive).
- </p>
- 
- <p>
- This function is useful to automate lookup up the index of water within a media
- so as to avoid hard-coding or guessing what the index will be. Typically, this
- function would be run once at initialization time.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 19, 2017, by Michael Wetter:<br/>
+Removed assertion as function is valid also for other values than <code>N==2</code>.
+</li>
+<li>
+March 17, 2017, by Michael O'Keefe:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Given an array of strings representing substance names, this function returns
+the integer index of the substance named \"water\" (case-insensitive).
+</p>
+
+<p>
+This function is useful to automate lookup up the index of water within a media
+so as to avoid hard-coding or guessing what the index will be. Typically, this
+function would be run once at initialization time.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end determineWaterIndex;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/dynamicViscosityWater.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/dynamicViscosityWater.mo
index 4a835a6d89..4e2a8fc7ce 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/dynamicViscosityWater.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/dynamicViscosityWater.mo
@@ -10,23 +10,23 @@ algorithm
         //John Wiley & Sons, 1996
 
 annotation(Documentation(info = "<html>
- <p>
- This function is used to identify the dynamic viscosity of water at a given temperature.
- The function used is a fourth order polynomial fit to data from Incropera and Dewitt (1996).
- </p>
- <h4>References</h4>
- <p>
- Fundamentals of Heat and Mass Transfer (Fourth Edition), Frank Incropera and David P. Dewitt,
- John Wiley &amp; Sons, 1996
- </p>
- </html>",
+<p>
+This function is used to identify the dynamic viscosity of water at a given temperature.
+The function used is a fourth order polynomial fit to data from Incropera and Dewitt (1996).
+</p>
+<h4>References</h4>
+<p>
+Fundamentals of Heat and Mass Transfer (Fourth Edition), Frank Incropera and David P. Dewitt,
+John Wiley &amp; Sons, 1996
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 7, 2013 by Peter Grant:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 7, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end dynamicViscosityWater;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/epsilon_C.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/epsilon_C.mo
index cd216e2446..27bd3482a3 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/epsilon_C.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/epsilon_C.mo
@@ -78,48 +78,48 @@ algorithm
   Inline=false,
   smoothOrder=1,
   Documentation(info="<html>
- <p>
- This function computes the heat exchanger effectiveness,
- the Number of Transfer Units, and the capacity flow ratio
- for given capacity flow rates.
- </p>
- <p>
- The implementation allows for zero flow rate.
- As <code>CMin_flow</code> crosses <code>delta*CMin_flow_nominal</code> from above,
- the Number of Transfer Units and the heat exchanger effectiveness go to zero.
- </p>
- <p>
- The different options for the flow regime are declared in
- <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
- AixLib.Fluid.Types.HeatExchangerFlowRegime</a>.
- </p>
- </html>",
+<p>
+This function computes the heat exchanger effectiveness,
+the Number of Transfer Units, and the capacity flow ratio
+for given capacity flow rates.
+</p>
+<p>
+The implementation allows for zero flow rate.
+As <code>CMin_flow</code> crosses <code>delta*CMin_flow_nominal</code> from above,
+the Number of Transfer Units and the heat exchanger effectiveness go to zero.
+</p>
+<p>
+The different options for the flow regime are declared in
+<a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
+AixLib.Fluid.Types.HeatExchangerFlowRegime</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 10, 2018, by Michael Wetter:<br/>
- Removed outputs <code>Z</code> and <code>NTU</code> as they are not used by other models.
- Removed <code>if</code> statement that can cause a discontinuous derivative.
- </li>
- <li>
- July 7, 2014, by Michael Wetter:<br/>
- Changed the type of the input <code>flowRegime</code> from
- <code>AixLib.Fluid.Types.HeatExchangerFlowRegime</code>
- to <code>Integer</code>.
- This was done to have the same argument list as
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ\">
- AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ</a>,
- in which the type had to be changed.
- </li>
- <li>
- July 6, 2014, by Michael Wetter:<br/>
- Removed unused <code>import</code> statement.
- </li>
- <li>
- February 20, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 10, 2018, by Michael Wetter:<br/>
+Removed outputs <code>Z</code> and <code>NTU</code> as they are not used by other models.
+Removed <code>if</code> statement that can cause a discontinuous derivative.
+</li>
+<li>
+July 7, 2014, by Michael Wetter:<br/>
+Changed the type of the input <code>flowRegime</code> from
+<code>AixLib.Fluid.Types.HeatExchangerFlowRegime</code>
+to <code>Integer</code>.
+This was done to have the same argument list as
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ\">
+AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ</a>,
+in which the type had to be changed.
+</li>
+<li>
+July 6, 2014, by Michael Wetter:<br/>
+Removed unused <code>import</code> statement.
+</li>
+<li>
+February 20, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end epsilon_C;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/epsilon_ntuZ.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/epsilon_ntuZ.mo
index b4928f4c97..7f89d569fa 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/epsilon_ntuZ.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/epsilon_ntuZ.mo
@@ -49,40 +49,40 @@ algorithm
              inverse(NTU=AixLib.Fluid.HeatExchangers.BaseClasses.ntu_epsilonZ(eps=eps, Z=Z, flowRegime=flowRegime)),
            smoothOrder=1,
            Documentation(info="<html>
- <p>
- This function computes the heat exchanger effectiveness for a given number of transfer units, capacity flow ratio and heat exchanger flow regime.
- The different options for the flow regime are declared in
- <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
- AixLib.Fluid.Types.HeatExchangerFlowRegime</a>.
- </p>
- </html>",
+<p>
+This function computes the heat exchanger effectiveness for a given number of transfer units, capacity flow ratio and heat exchanger flow regime.
+The different options for the flow regime are declared in
+<a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
+AixLib.Fluid.Types.HeatExchangerFlowRegime</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 28, 2016, by Massimo Cimmino:<br/>
- Added case for constant temperature phase change on one side of
- the heat exchanger.
- </li>
- <li>
- July 7, 2014, by Michael Wetter:<br/>
- Changed the type of the input <code>flowRegime</code> from
- <code>AixLib.Fluid.Types.HeatExchangerFlowRegime</code>
- to <code>Integer</code>.
- This was required because this argument is passed in Dymola 2015 in the function
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_C\">
- AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_C</a>
- as an integer. Without this change, a translation warning occurs.
- </li>
- <li>
- September 25, 2013, by Michael Wetter:<br/>
- Changed test in the <code>assert</code> statement as OpenModelica
- had an error when comparing enumerations with integers.
- </li>
- <li>
- February 11, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 28, 2016, by Massimo Cimmino:<br/>
+Added case for constant temperature phase change on one side of
+the heat exchanger.
+</li>
+<li>
+July 7, 2014, by Michael Wetter:<br/>
+Changed the type of the input <code>flowRegime</code> from
+<code>AixLib.Fluid.Types.HeatExchangerFlowRegime</code>
+to <code>Integer</code>.
+This was required because this argument is passed in Dymola 2015 in the function
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_C\">
+AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_C</a>
+as an integer. Without this change, a translation warning occurs.
+</li>
+<li>
+September 25, 2013, by Michael Wetter:<br/>
+Changed test in the <code>assert</code> statement as OpenModelica
+had an error when comparing enumerations with integers.
+</li>
+<li>
+February 11, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end epsilon_ntuZ;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/isobaricExpansionCoefficientWater.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/isobaricExpansionCoefficientWater.mo
index baa9ad5a8d..dd63652f38 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/isobaricExpansionCoefficientWater.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/isobaricExpansionCoefficientWater.mo
@@ -11,24 +11,24 @@ algorithm
         //John Wiley & Sons, 1996
 
 annotation(Documentation(info = "<html>
- <p>
- This function is used to identify the isobaric expansion coefficient of water at a
- given temperature. The function used is a fourth order polynomial fit to data from
- Incropera and Dewitt (1996).
- </p>
- <h4>References</h4>
- <p>
- Fundamentals of Heat and Mass Transfer (Fourth Edition), Frank Incropera and David P.
- Dewitt, John Wiley &amp; Sons, 1996
- </p>
- </html>",
+<p>
+This function is used to identify the isobaric expansion coefficient of water at a
+given temperature. The function used is a fourth order polynomial fit to data from
+Incropera and Dewitt (1996).
+</p>
+<h4>References</h4>
+<p>
+Fundamentals of Heat and Mass Transfer (Fourth Edition), Frank Incropera and David P.
+Dewitt, John Wiley &amp; Sons, 1996
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 7, 2013 by Peter Grant:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 7, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end isobaricExpansionCoefficientWater;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/lmtd.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/lmtd.mo
index b03458c678..f995bda1ba 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/lmtd.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/lmtd.mo
@@ -15,27 +15,27 @@ algorithm
   lmtd :=(dT2 - dT1)/Modelica.Math.log(dT2/dT1);
 annotation (preferredView="info",
 Documentation(info="<html>
- <p>
- This function computes the log mean temperature difference of a heat exchanger.
- </p>
- <p>
- Note that the implementation requires the temperature differences <i>T<sub>a1</sub> - T<sub>b2</sub></i> and
- <i>T<sub>b1</sub> - T<sub>a2</sub></i> to be not equal to each other.
- </p>
- </html>",
+<p>
+This function computes the log mean temperature difference of a heat exchanger.
+</p>
+<p>
+Note that the implementation requires the temperature differences <i>T<sub>a1</sub> - T<sub>b2</sub></i> and
+<i>T<sub>b1</sub> - T<sub>a2</sub></i> to be not equal to each other.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 30, 2020, by Michael Wetter:<br/>
- Updated documentation.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2268\">Buildings, #2268</a>.
- </li>
- <li>
- May 28, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 30, 2020, by Michael Wetter:<br/>
+Updated documentation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2268\">Buildings, #2268</a>.
+</li>
+<li>
+May 28, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end lmtd;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/ntu_epsilonZ.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/ntu_epsilonZ.mo
index 6b17d827ef..b422f40208 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/ntu_epsilonZ.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/ntu_epsilonZ.mo
@@ -31,9 +31,9 @@ algorithm
     a := Z+1;
     assert(eps < 1/a,
       "Invalid input data. eps > 1/(1+Z) is physically not possible for parallel flow.
-   Received eps = "+ String(eps) + "
-              Z = "+ String(Z) + "
-        1/(Z+1) = "+ String(1/a));
+  Received eps = " + String(eps) + "
+             Z = " + String(Z) + "
+       1/(Z+1) = " + String(1/a));
     NTU := -(Modelica.Math.log(1-eps*a))/(a);
   elseif (flowRegime == Integer(f.CounterFlow)) then// counter flow
    // a is constraining Z since eps is not defined for Z=1.
@@ -86,61 +86,61 @@ algorithm
              inverse(eps=AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ(NTU=NTU, Z=Z, flowRegime=flowRegime)),
            smoothOrder=1,
 Documentation(info="<html>
- <p>
- This function computes the number of transfer units for a given heat exchanger effectiveness,
- capacity flow ratio and heat exchanger flow regime.
- The different options for the flow regime are declared in
- <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
- AixLib.Fluid.Types.HeatExchangerFlowRegime</a>.
- </p>
- <p>
- Note that for the flow regime <code>CrossFlowUnmixed</code>, computing the
- function requires the numerical solution of an equation in one variable.
- This is handled internally and not exposed to the global solver.
- </p>
- </html>",
+<p>
+This function computes the number of transfer units for a given heat exchanger effectiveness,
+capacity flow ratio and heat exchanger flow regime.
+The different options for the flow regime are declared in
+<a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
+AixLib.Fluid.Types.HeatExchangerFlowRegime</a>.
+</p>
+<p>
+Note that for the flow regime <code>CrossFlowUnmixed</code>, computing the
+function requires the numerical solution of an equation in one variable.
+This is handled internally and not exposed to the global solver.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 28, 2020, by Michael Wetter:<br/>
- Replaced call to <code>Media.Common.OneNonLinearEquation</code> to use
- <a href=\"modelica://Modelica.Math.Nonlinear.solveOneNonlinearEquation\">
- Modelica.Math.Nonlinear.solveOneNonlinearEquation</a>
- because <code>Media.Common.OneNonLinearEquation</code> will be obsolete in MSL 4.0.0.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1299\">issue 1299</a>.
- </li>
- <li>
- September 28, 2016, by Massimo Cimmino:<br/>
- Added case for constant temperature phase change on one side of
- the heat exchanger.
- </li>
- <li>
- July 7, 2014, by Michael Wetter:<br/>
- Changed the type of the input <code>flowRegime</code> from
- <code>AixLib.Fluid.Types.HeatExchangerFlowRegime</code>
- to <code>Integer</code>.
- This was done to have the same argument list as
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ\">
- AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ</a>,
- in which the type had to be changed.
- </li>
- <li>
- April 29, 2013, by Michael Wetter:<br/>
- Added dummy argument to function call of <code>Internal.solve</code>
- to avoid a warning during model check in Dymola 2015.
- </li>
- <li>
- August 10, 2011, by Michael Wetter:<br/>
- Changed implementation to use
- <code>Modelica.Media.Common.OneNonLinearEquation</code> instead of
- <code>AixLib.Utilities.Math.BaseClasses.OneNonLinearEquation</code>.
- </li>
- <li>
- February 11, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 28, 2020, by Michael Wetter:<br/>
+Replaced call to <code>Media.Common.OneNonLinearEquation</code> to use
+<a href=\"modelica://Modelica.Math.Nonlinear.solveOneNonlinearEquation\">
+Modelica.Math.Nonlinear.solveOneNonlinearEquation</a>
+because <code>Media.Common.OneNonLinearEquation</code> will be obsolete in MSL 4.0.0.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1299\">issue 1299</a>.
+</li>
+<li>
+September 28, 2016, by Massimo Cimmino:<br/>
+Added case for constant temperature phase change on one side of
+the heat exchanger.
+</li>
+<li>
+July 7, 2014, by Michael Wetter:<br/>
+Changed the type of the input <code>flowRegime</code> from
+<code>AixLib.Fluid.Types.HeatExchangerFlowRegime</code>
+to <code>Integer</code>.
+This was done to have the same argument list as
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ\">
+AixLib.Fluid.HeatExchangers.BaseClasses.epsilon_ntuZ</a>,
+in which the type had to be changed.
+</li>
+<li>
+April 29, 2013, by Michael Wetter:<br/>
+Added dummy argument to function call of <code>Internal.solve</code>
+to avoid a warning during model check in Dymola 2015.
+</li>
+<li>
+August 10, 2011, by Michael Wetter:<br/>
+Changed implementation to use
+<code>Modelica.Media.Common.OneNonLinearEquation</code> instead of
+<code>AixLib.Utilities.Math.BaseClasses.OneNonLinearEquation</code>.
+</li>
+<li>
+February 11, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ntu_epsilonZ;
diff --git a/AixLib/Fluid/HeatExchangers/BaseClasses/prandtlNumberWater.mo b/AixLib/Fluid/HeatExchangers/BaseClasses/prandtlNumberWater.mo
index df6cc8fd1e..5d373322e7 100644
--- a/AixLib/Fluid/HeatExchangers/BaseClasses/prandtlNumberWater.mo
+++ b/AixLib/Fluid/HeatExchangers/BaseClasses/prandtlNumberWater.mo
@@ -10,24 +10,24 @@ algorithm
         //John Wiley & Sons, 1996
 
 annotation(Documentation(info = "<html>
- <p>
- This function is used to identify the Prandtl number of water at a given temperature.
- The function used is a fourth order polynomial fit to data from Incropera and Dewitt
- (1996).
- </p>
- <h4>References</h4>
- <p>
- Fundamentals of Heat and Mass Transfer (Fourth Edition), Frank Incropera and David P.
- Dewitt, John Wiley &amp; Sons, 1996
- </p>
- </html>",
+<p>
+This function is used to identify the Prandtl number of water at a given temperature.
+The function used is a fourth order polynomial fit to data from Incropera and Dewitt
+(1996).
+</p>
+<h4>References</h4>
+<p>
+Fundamentals of Heat and Mass Transfer (Fourth Edition), Frank Incropera and David P.
+Dewitt, John Wiley &amp; Sons, 1996
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 7, 2013 by Peter Grant:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 7, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end prandtlNumberWater;
diff --git a/AixLib/Fluid/HeatExchangers/ConstantEffectiveness.mo b/AixLib/Fluid/HeatExchangers/ConstantEffectiveness.mo
index 01aa5f22cd..253f6307d4 100644
--- a/AixLib/Fluid/HeatExchangers/ConstantEffectiveness.mo
+++ b/AixLib/Fluid/HeatExchangers/ConstantEffectiveness.mo
@@ -26,51 +26,51 @@ model ConstantEffectiveness "Heat exchanger with constant effectiveness"
           preferredView="info",
 defaultComponentName="hex",
 Documentation(info="<html>
- <p>
- Model for a heat exchanger with constant effectiveness.
- </p>
- <p>
- This model transfers heat in the amount of
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   Q = Q<sub>max</sub> &epsilon;,
- </p>
- <p>
- where <i>&epsilon;</i> is a constant effectiveness and
- <i>Q<sub>max</sub></i> is the maximum heat that can be transferred.
- </p>
- <p>
- For a heat and moisture exchanger, use
- <a href=\"modelica://AixLib.Fluid.MassExchangers.ConstantEffectiveness\">
- AixLib.Fluid.MassExchangers.ConstantEffectiveness</a>
- instead of this model.
- </p>
- </html>",
+<p>
+Model for a heat exchanger with constant effectiveness.
+</p>
+<p>
+This model transfers heat in the amount of
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  Q = Q<sub>max</sub> &epsilon;,
+</p>
+<p>
+where <i>&epsilon;</i> is a constant effectiveness and
+<i>Q<sub>max</sub></i> is the maximum heat that can be transferred.
+</p>
+<p>
+For a heat and moisture exchanger, use
+<a href=\"modelica://AixLib.Fluid.MassExchangers.ConstantEffectiveness\">
+AixLib.Fluid.MassExchangers.ConstantEffectiveness</a>
+instead of this model.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 13, 2013 by Michael Wetter:<br/>
- Corrected error in the documentation.
- </li>
- <li>
- July 30, 2013 by Michael Wetter:<br/>
- Updated model to use new variable <code>mWat_flow</code>
- in the base class.
- </li>
- <li>
- January 28, 2010, by Michael Wetter:<br/>
- Added regularization near zero flow.
- </li>
- <li>
- October 2, 2009, by Michael Wetter:<br/>
- Changed computation of inlet temperatures to use
- <code>state_*_inflow</code> which is already known in base class.
- </li>
- <li>
- April 28, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+August 13, 2013 by Michael Wetter:<br/>
+Corrected error in the documentation.
+</li>
+<li>
+July 30, 2013 by Michael Wetter:<br/>
+Updated model to use new variable <code>mWat_flow</code>
+in the base class.
+</li>
+<li>
+January 28, 2010, by Michael Wetter:<br/>
+Added regularization near zero flow.
+</li>
+<li>
+October 2, 2009, by Michael Wetter:<br/>
+Changed computation of inlet temperatures to use
+<code>state_*_inflow</code> which is already known in base class.
+</li>
+<li>
+April 28, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantEffectiveness;
diff --git a/AixLib/Fluid/HeatExchangers/DryCoilEffectivenessNTU.mo b/AixLib/Fluid/HeatExchangers/DryCoilEffectivenessNTU.mo
index a0d470e938..15f312fb5e 100644
--- a/AixLib/Fluid/HeatExchangers/DryCoilEffectivenessNTU.mo
+++ b/AixLib/Fluid/HeatExchangers/DryCoilEffectivenessNTU.mo
@@ -36,50 +36,50 @@ equation
     preferredView="info",
 defaultComponentName="hex",
     Documentation(info="<html>
- <p>
- Model of a coil without humidity condensation.
- This model transfers heat in the amount of
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   Q&#775; = Q&#775;<sub>max</sub>  &epsilon;<br/>
-   &epsilon; = f(NTU, Z, flowRegime),
- </p>
- <p>
- where
- <i>Q&#775;<sub>max</sub></i> is the maximum heat that can be transferred,
- <i>&epsilon;</i> is the heat transfer effectiveness,
- <i>NTU</i> is the Number of Transfer Units,
- <i>Z</i> is the ratio of minimum to maximum capacity flow rate and
- <i>flowRegime</i> is the heat exchanger flow regime.
- such as
- parallel flow, cross flow or counter flow.
- </p>
- <p>
- The flow regimes depend on the heat exchanger configuration. All configurations
- defined in
- <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerConfiguration\">
- AixLib.Fluid.Types.HeatExchangerConfiguration</a>
- are supported.
- </p>
- <p>
- The convective heat transfer coefficients scale proportional to
- <i>(m&#775;/m&#775;<sub>0</sub>)<sup>n</sup></i>, where
- <i>m&#775;</i> is the mass flow rate,
- <i>m&#775;<sub>0</sub></i> is the nominal mass flow rate, and
- <i>n=0.8</i> on the air-side and <i>n=0.85</i> on the water side.
- </p>
- <p>
- For a heat and moisture exchanger, use
- <a href=\"modelica://AixLib.Fluid.MassExchangers.ConstantEffectiveness\">
- AixLib.Fluid.MassExchangers.ConstantEffectiveness</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 25, 2018, by Michael Wetter:<br/>
- Refactored model to use a common base class.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model of a coil without humidity condensation.
+This model transfers heat in the amount of
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  Q&#775; = Q&#775;<sub>max</sub>  &epsilon;<br/>
+  &epsilon; = f(NTU, Z, flowRegime),
+</p>
+<p>
+where
+<i>Q&#775;<sub>max</sub></i> is the maximum heat that can be transferred,
+<i>&epsilon;</i> is the heat transfer effectiveness,
+<i>NTU</i> is the Number of Transfer Units,
+<i>Z</i> is the ratio of minimum to maximum capacity flow rate and
+<i>flowRegime</i> is the heat exchanger flow regime.
+such as
+parallel flow, cross flow or counter flow.
+</p>
+<p>
+The flow regimes depend on the heat exchanger configuration. All configurations
+defined in
+<a href=\"modelica://AixLib.Fluid.Types.HeatExchangerConfiguration\">
+AixLib.Fluid.Types.HeatExchangerConfiguration</a>
+are supported.
+</p>
+<p>
+The convective heat transfer coefficients scale proportional to
+<i>(m&#775;/m&#775;<sub>0</sub>)<sup>n</sup></i>, where
+<i>m&#775;</i> is the mass flow rate,
+<i>m&#775;<sub>0</sub></i> is the nominal mass flow rate, and
+<i>n=0.8</i> on the air-side and <i>n=0.85</i> on the water side.
+</p>
+<p>
+For a heat and moisture exchanger, use
+<a href=\"modelica://AixLib.Fluid.MassExchangers.ConstantEffectiveness\">
+AixLib.Fluid.MassExchangers.ConstantEffectiveness</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 25, 2018, by Michael Wetter:<br/>
+Refactored model to use a common base class.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DryCoilEffectivenessNTU;
diff --git a/AixLib/Fluid/HeatExchangers/EvaporatorCondenser.mo b/AixLib/Fluid/HeatExchangers/EvaporatorCondenser.mo
index 7163b1475f..d26c16950a 100644
--- a/AixLib/Fluid/HeatExchangers/EvaporatorCondenser.mo
+++ b/AixLib/Fluid/HeatExchangers/EvaporatorCondenser.mo
@@ -46,7 +46,7 @@ model EvaporatorCondenser
 protected
   parameter Modelica.Units.SI.SpecificHeatCapacity cp_default=
       Medium.specificHeatCapacityCp(sta_default)
-    "Density, used to compute fluid volume";
+    "Specific heat capacity";
 
   Modelica.Thermal.HeatTransfer.Sensors.HeatFlowSensor heaFlo
     "Heat flow sensor"
@@ -93,53 +93,53 @@ equation
           textString="Q_flow")}),
 defaultComponentName="evaCon",
 Documentation(info="<html>
- <p>
- Model for a constant temperature evaporator or condenser based on a &epsilon;-NTU
- heat exchanger model.
- </p>
- <p>
- The heat exchanger effectiveness is calculated from the number of transfer units
- (NTU):
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &epsilon; = 1 - exp(UA &frasl; (m&#775; c<sub>p</sub>))
- </p>
- <p>
- Optionally, this model can have a flow resistance.
- If no flow resistance is requested, set <code>dp_nominal=0</code>.
- </p>
- <h4>Limitations</h4>
- <p>
- This model does not consider any superheating or supercooling on the refrigerant
- side. The refrigerant is considered to exchange heat at a constant temperature
- throughout the heat exchanger.
- </p>
- </html>",
+<p>
+Model for a constant temperature evaporator or condenser based on a &epsilon;-NTU
+heat exchanger model.
+</p>
+<p>
+The heat exchanger effectiveness is calculated from the number of transfer units
+(NTU):
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&epsilon; = 1 - exp(- UA &frasl; (m&#775; c<sub>p</sub>))
+</p>
+<p>
+Optionally, this model can have a flow resistance.
+If no flow resistance is requested, set <code>dp_nominal=0</code>.
+</p>
+<h4>Limitations</h4>
+<p>
+This model does not consider any superheating or supercooling on the refrigerant
+side. The refrigerant is considered to exchange heat at a constant temperature
+throughout the heat exchanger.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- May 27, 2017, by Filip Jorissen:<br/>
- Regularised heat transfer around zero flow.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
- </li>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Corrected invalid syntax for computing the specific heat capacity.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/707\">#707</a>.
- </li>
- <li>
- October 11, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+May 27, 2017, by Filip Jorissen:<br/>
+Regularised heat transfer around zero flow.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
+</li>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Corrected invalid syntax for computing the specific heat capacity.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/707\">#707</a>.
+</li>
+<li>
+October 11, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EvaporatorCondenser;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/AirHeater_T.mo b/AixLib/Fluid/HeatExchangers/Examples/AirHeater_T.mo
index be126c2e2b..a3d7bf053e 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/AirHeater_T.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/AirHeater_T.mo
@@ -32,47 +32,47 @@ equation
   connect(mov.port_b, hea.port_a) annotation (Line(points={{-50,-40},{-35,-40},
           {-20,-40}}, color={0,127,255}));
   annotation ( Documentation(info="<html>
- <p>
- This example illustrates how to use the heater model that takes as an
- input the leaving fluid temperature.
- </p>
- <p>
- The model consist of an air volume with heat loss to the ambient.
- The set point of the air temperature is different between night and day.
- The heater tracks the set point temperature, except for the periods in
- which the air temperature is above the set point.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.AirHeater_u\">
- AixLib.Fluid.HeatExchangers.Examples.AirHeater_u</a>
- for a model that takes the heating power as an input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- November 12, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example illustrates how to use the heater model that takes as an
+input the leaving fluid temperature.
+</p>
+<p>
+The model consist of an air volume with heat loss to the ambient.
+The set point of the air temperature is different between night and day.
+The heater tracks the set point temperature, except for the periods in
+which the air temperature is above the set point.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.AirHeater_u\">
+AixLib.Fluid.HeatExchangers.Examples.AirHeater_u</a>
+for a model that takes the heating power as an input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+November 12, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Examples/AirHeater_T.mos"
         "Simulate and plot"),
     experiment(
       StopTime=172800,
       Tolerance=1e-08),
     Diagram(coordinateSystem(extent={{-100,-100},{120,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{120,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{120,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirHeater_T;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/AirHeater_u.mo b/AixLib/Fluid/HeatExchangers/Examples/AirHeater_u.mo
index 39e4391735..1584143568 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/AirHeater_u.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/AirHeater_u.mo
@@ -25,41 +25,41 @@ equation
   connect(mov.port_b, hea.port_a) annotation (Line(points={{-50,-40},{-36,-40},
           {-20,-40}}, color={0,127,255}));
   annotation ( Documentation(info="<html>
- <p>
- This example illustrates how to use the heater model that takes as an
- input the heat added to the medium.
- </p>
- <p>
- The model consist of an air volume with heat loss to the ambient.
- The set point of the air temperature is different between night and day.
- The heater tracks the set point temperature, except for the periods in
- which the air temperature is above the set point.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.AirHeater_T\">
- AixLib.Fluid.HeatExchangers.Examples.AirHeater_T</a>
- for a model that takes the leaving air temperature as an input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- November 12, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example illustrates how to use the heater model that takes as an
+input the heat added to the medium.
+</p>
+<p>
+The model consist of an air volume with heat loss to the ambient.
+The set point of the air temperature is different between night and day.
+The heater tracks the set point temperature, except for the periods in
+which the air temperature is above the set point.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.AirHeater_T\">
+AixLib.Fluid.HeatExchangers.Examples.AirHeater_T</a>
+for a model that takes the leaving air temperature as an input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+November 12, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Examples/AirHeater_u.mos"
         "Simulate and plot"),
     experiment(
@@ -67,6 +67,6 @@ equation
       Tolerance=1e-6),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{
             120,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{120,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{120,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirHeater_u;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/BaseClasses/EffectivenessNTUMassFlow.mo b/AixLib/Fluid/HeatExchangers/Examples/BaseClasses/EffectivenessNTUMassFlow.mo
index 6ff9d74f17..1d98c25af6 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/BaseClasses/EffectivenessNTUMassFlow.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/BaseClasses/EffectivenessNTUMassFlow.mo
@@ -98,6 +98,6 @@ equation
       color={0,0,127},
       smooth=Smooth.None));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false,extent={{-100,
-            -100},{200,200}}), graphics),
-  __Dymola_LockedEditing="Model from IBPSA");
+            -100},{200,200}}), graphics), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end EffectivenessNTUMassFlow;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/BaseClasses/Heater.mo b/AixLib/Fluid/HeatExchangers/Examples/BaseClasses/Heater.mo
index ae3f30e873..3ff24838de 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/BaseClasses/Heater.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/BaseClasses/Heater.mo
@@ -106,56 +106,56 @@ equation
           -20},{52.6667,-10}},
                           color={0,127,255}));
   annotation ( Documentation(info="<html>
- <p>
- This partial model is used to construct the models
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.AirHeater_T\">
- AixLib.Fluid.HeatExchangers.Examples.AirHeater_T</a>
- and
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.AirHeater_u\">
- AixLib.Fluid.HeatExchangers.Examples.AirHeater_u</a> and
- the similar models
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_T\">
- AixLib.Fluid.HeatExchangers.Examples.WaterHeater_T</a>
- and
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u\">
- AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u</a>.
- It consists of a volume with heat loss to the ambient,
- a fan,
- a set point for the temperature of the volume and a PI controller.
- </p>
- <p>
- The instance <code>bou</code> is required to set a reference pressure
- for system models in which the fluid is modelled as an incompressible fluid,
- and it also is required to account for a variation of density of the fluid.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated model for new heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>February 20, 2016, by Ruben Baetens:<br/>
- Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- November 12, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+<p>
+This partial model is used to construct the models
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.AirHeater_T\">
+AixLib.Fluid.HeatExchangers.Examples.AirHeater_T</a>
+and
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.AirHeater_u\">
+AixLib.Fluid.HeatExchangers.Examples.AirHeater_u</a> and
+the similar models
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_T\">
+AixLib.Fluid.HeatExchangers.Examples.WaterHeater_T</a>
+and
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u\">
+AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u</a>.
+It consists of a volume with heat loss to the ambient,
+a fan,
+a set point for the temperature of the volume and a PI controller.
+</p>
+<p>
+The instance <code>bou</code> is required to set a reference pressure
+for system models in which the fluid is modelled as an incompressible fluid,
+and it also is required to account for a variation of density of the fluid.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated model for new heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>February 20, 2016, by Ruben Baetens:<br/>
+Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+November 12, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
             -100},{120,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{120,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{120,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Heater;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUMassFlow.mo b/AixLib/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUMassFlow.mo
index 56d1c2f6d3..259b5cc2b4 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUMassFlow.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUMassFlow.mo
@@ -58,19 +58,19 @@ __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUMassFlow.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model tests
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
- for different mass flow rates.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 12, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
+for different mass flow rates.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 12, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DryCoilEffectivenessNTUMassFlow;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUPControl.mo b/AixLib/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUPControl.mo
index 765883ef39..33746ea115 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUPControl.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUPControl.mo
@@ -130,33 +130,33 @@ __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Examples/DryCoilEffectivenessNTUPControl.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model demonstrates the use of
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>.
- The valve on the water-side is regulated to track a setpoint temperature
- for the air outlet.
- </p>
- </html>",
+<p>
+This model demonstrates the use of
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>.
+The valve on the water-side is regulated to track a setpoint temperature
+for the air outlet.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- July 3, 2014, by Michael Wetter:<br/>
- Changed pressure sink to mass flow rate sink to avoid an overdetermined
- by consistent set of initial conditions.
- </li>
- <li>
- March 1, 2013, by Michael Wetter:<br/>
- Added nominal pressure drop for valve as
- this parameter no longer has a default value.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+July 3, 2014, by Michael Wetter:<br/>
+Changed pressure sink to mass flow rate sink to avoid an overdetermined
+by consistent set of initial conditions.
+</li>
+<li>
+March 1, 2013, by Michael Wetter:<br/>
+Added nominal pressure drop for valve as
+this parameter no longer has a default value.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DryCoilEffectivenessNTUPControl;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/WaterCooler_T.mo b/AixLib/Fluid/HeatExchangers/Examples/WaterCooler_T.mo
index ea0ee28e4f..6cf92aa7f8 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/WaterCooler_T.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/WaterCooler_T.mo
@@ -40,37 +40,37 @@ equation
   connect(mov.port_b,coo. port_a) annotation (Line(points={{-50,-40},{-35,-40},
           {-20,-40}}, color={0,127,255}));
   annotation ( Documentation(info="<html>
- <p>
- This example illustrates how to use the sensible cooler model that takes as an
- input the leaving fluid temperature.
- </p>
- <p>
- The model consist of a water volume with heat gain from the ambient.
- The set point of the water temperature is different between night and day.
- The heater tracks the set point temperature, except for the periods in
- which the water temperature is above the set point.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u\">
- AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u</a>
- for a model that takes the heating power as an input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example illustrates how to use the sensible cooler model that takes as an
+input the leaving fluid temperature.
+</p>
+<p>
+The model consist of a water volume with heat gain from the ambient.
+The set point of the water temperature is different between night and day.
+The heater tracks the set point temperature, except for the periods in
+which the water temperature is above the set point.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u\">
+AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u</a>
+for a model that takes the heating power as an input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Examples/WaterCooler_T.mos"
         "Simulate and plot"),
     experiment(
@@ -78,6 +78,6 @@ equation
       Tolerance=1e-8),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{120,
             100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{120,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{120,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterCooler_T;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/WaterHeater_T.mo b/AixLib/Fluid/HeatExchangers/Examples/WaterHeater_T.mo
index f489f232d5..f1bcfbc3e6 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/WaterHeater_T.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/WaterHeater_T.mo
@@ -35,38 +35,38 @@ equation
   connect(mov.port_b, hea.port_a) annotation (Line(points={{-50,-40},{-20,-40}},
                       color={0,127,255}));
   annotation ( Documentation(info="<html>
- <p>
- This example illustrates how to use the heater model that takes as an
- input the leaving fluid temperature.
- </p>
- <p>
- The model consist of a water volume with heat loss to the ambient.
- The set point of the water temperature is different between night and day.
- The heater tracks the set point temperature, except for the periods in
- which the water temperature is above the set point.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u\">
- AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u</a>
- for a model that takes the heating power as an input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 27, 2016, by Michael Wetter;<br/>
- Removed algorithm specification in experiment annotation.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- March 16, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example illustrates how to use the heater model that takes as an
+input the leaving fluid temperature.
+</p>
+<p>
+The model consist of a water volume with heat loss to the ambient.
+The set point of the water temperature is different between night and day.
+The heater tracks the set point temperature, except for the periods in
+which the water temperature is above the set point.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u\">
+AixLib.Fluid.HeatExchangers.Examples.WaterHeater_u</a>
+for a model that takes the heating power as an input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 27, 2016, by Michael Wetter;<br/>
+Removed algorithm specification in experiment annotation.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+March 16, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Examples/WaterHeater_T.mos"
         "Simulate and plot"),
     experiment(
@@ -74,6 +74,6 @@ equation
       Tolerance=1e-6),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{
             120,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{120,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{120,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterHeater_T;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/WaterHeater_u.mo b/AixLib/Fluid/HeatExchangers/Examples/WaterHeater_u.mo
index 16d6bd46c5..e7a5c50b5e 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/WaterHeater_u.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/WaterHeater_u.mo
@@ -30,45 +30,45 @@ equation
   connect(mov.port_b, hea.port_a) annotation (Line(points={{-50,-40},{-20,-40}},
                       color={0,127,255}));
   annotation ( Documentation(info="<html>
- <p>
- This example illustrates how to use the heater model that takes as an
- input the heat added to the medium.
- </p>
- <p>
- The model consist of a water volume with heat loss to the ambient.
- The set point of the water temperature is different between night and day.
- The heater tracks the set point temperature, except for the periods in
- which the water temperature is above the set point.
- </p>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_T\">
- AixLib.Fluid.HeatExchangers.Examples.WaterHeater_T</a>
- for a model that takes the leaving water temperature as an input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 8, 2017, by Michael Wetter:<br/>
- Updated heater model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- <li>
- January 27, 2016, by Michael Wetter;<br/>
- Removed algorithm specification in experiment annotation.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- March 16, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example illustrates how to use the heater model that takes as an
+input the heat added to the medium.
+</p>
+<p>
+The model consist of a water volume with heat loss to the ambient.
+The set point of the water temperature is different between night and day.
+The heater tracks the set point temperature, except for the periods in
+which the water temperature is above the set point.
+</p>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.WaterHeater_T\">
+AixLib.Fluid.HeatExchangers.Examples.WaterHeater_T</a>
+for a model that takes the leaving water temperature as an input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 8, 2017, by Michael Wetter:<br/>
+Updated heater model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+<li>
+January 27, 2016, by Michael Wetter;<br/>
+Removed algorithm specification in experiment annotation.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+March 16, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Examples/WaterHeater_u.mos"
         "Simulate and plot"),
     experiment(
@@ -76,6 +76,6 @@ equation
       Tolerance=1e-6),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{
             120,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{120,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{120,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterHeater_u;
diff --git a/AixLib/Fluid/HeatExchangers/Examples/WetCoilEffectivenessNTUMassFlow.mo b/AixLib/Fluid/HeatExchangers/Examples/WetCoilEffectivenessNTUMassFlow.mo
index 41e1564cf3..09b88d00a8 100644
--- a/AixLib/Fluid/HeatExchangers/Examples/WetCoilEffectivenessNTUMassFlow.mo
+++ b/AixLib/Fluid/HeatExchangers/Examples/WetCoilEffectivenessNTUMassFlow.mo
@@ -61,24 +61,24 @@ equation
     Diagram(coordinateSystem(preserveAspectRatio=true,
       extent={{-100, -100},{200,200}})),
     Documentation(revisions="<html>
- <ul>
- <li>
- March 17, 2017, by Michael O'Keefe:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This example is similar to
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.DryCoilEffectivenessNTUMassFlow\">
- AixLib.Fluid.HeatExchangers.Examples.DryCoilEffectivenessNTUMassFlow</a>
- except that the coil model
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
- is replaced here by
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.WetCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.WetCoilEffectivenessNTU</a>.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 17, 2017, by Michael O'Keefe:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example is similar to
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Examples.DryCoilEffectivenessNTUMassFlow\">
+AixLib.Fluid.HeatExchangers.Examples.DryCoilEffectivenessNTUMassFlow</a>
+except that the coil model
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
+is replaced here by
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.WetCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.WetCoilEffectivenessNTU</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WetCoilEffectivenessNTUMassFlow;
diff --git a/AixLib/Fluid/HeatExchangers/HeaterCooler_u.mo b/AixLib/Fluid/HeatExchangers/HeaterCooler_u.mo
index f7b40ea489..42e1f060da 100644
--- a/AixLib/Fluid/HeatExchangers/HeaterCooler_u.mo
+++ b/AixLib/Fluid/HeatExchangers/HeaterCooler_u.mo
@@ -17,7 +17,10 @@ protected
     final alpha=0)
     "Prescribed heat flow"
     annotation (Placement(transformation(extent={{-40,50},{-20,70}})));
-  Modelica.Blocks.Math.Gain gai(k=Q_flow_nominal) "Gain"
+  Modelica.Blocks.Math.Gain gai(
+    k(final unit="W")=Q_flow_nominal,
+    y(final unit="W"))
+    "Gain"
     annotation (Placement(transformation(extent={{-80,50},{-60,70}})));
 equation
   connect(u, gai.u) annotation (Line(
@@ -77,106 +80,112 @@ equation
           textString="Q_flow")}),
 defaultComponentName="hea",
 Documentation(info="<html>
- <p>
- Model for an ideal heater or cooler with prescribed heat flow rate to the medium.
- </p>
- <p>
- This model adds heat in the amount of <code>Q_flow = u Q_flow_nominal</code> to the medium.
- The input signal <code>u</code> and the nominal heat flow rate <code>Q_flow_nominal</code>
- can be positive or negative. A positive value of <code>Q_flow</code> means
- heating, and negative means cooling.
- </p>
- <p>
- The outlet conditions at <code>port_a</code> are not affected by this model,
- other than for a possible pressure difference due to flow friction.
- </p>
- <p>
- Optionally, this model can have a flow resistance.
- Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
- </p>
- <p>
- For a model that uses as an input the fluid temperature leaving at
- <code>port_b</code>, use
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.PrescribedOutlet\">
- AixLib.Fluid.HeatExchangers.PrescribedOutlet</a>
- </p>
- <h4>Limitations</h4>
- <p>
- This model does not affect the humidity of the air. Therefore,
- if used to cool air below the dew point temperature, the water mass fraction
- will not change.
- </p>
- <h4>Validation</h4>
- <p>
- The model has been validated against the analytical solution in
- the example
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.HeaterCooler_u\">
- AixLib.Fluid.HeatExchangers.Validation.HeaterCooler_u</a>.
- </p>
- </html>",
+<p>
+Model for an ideal heater or cooler with prescribed heat flow rate to the medium.
+</p>
+<p>
+This model adds heat in the amount of <code>Q_flow = u Q_flow_nominal</code> to the medium.
+The input signal <code>u</code> and the nominal heat flow rate <code>Q_flow_nominal</code>
+can be positive or negative. A positive value of <code>Q_flow</code> means
+heating, and negative means cooling.
+</p>
+<p>
+The outlet conditions at <code>port_a</code> are not affected by this model,
+other than for a possible pressure difference due to flow friction.
+</p>
+<p>
+Optionally, this model can have a flow resistance.
+Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
+</p>
+<p>
+For a model that uses as an input the fluid temperature leaving at
+<code>port_b</code>, use
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.PrescribedOutlet\">
+AixLib.Fluid.HeatExchangers.PrescribedOutlet</a>
+</p>
+<h4>Limitations</h4>
+<p>
+This model does not affect the humidity of the air. Therefore,
+if used to cool air below the dew point temperature, the water mass fraction
+will not change.
+</p>
+<h4>Validation</h4>
+<p>
+The model has been validated against the analytical solution in
+the example
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.HeaterCooler_u\">
+AixLib.Fluid.HeatExchangers.Validation.HeaterCooler_u</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Set <code>preHea(final alpha=0)</code> as this allows to simplify the
- system of equations.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/570\">#570</a>.
- </li>
- <li>
- November 19, 2015, by Michael Wetter:<br/>
- Removed assignment of parameter
- <code>showDesignFlowDirection</code> in <code>extends</code> statement.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
- </li>
- <li>
- May 6, 2015, by Michael Wetter:<br/>
- Set <code>prescribedHeatFlowRate=true</code>.
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">
- #412</a>.
- </li>
- <li>
- May 1, 2015, by Marcus Fuchs:<br/>
- Corrected typo in documentation.
- </li>
- <li>
- November 12, 2014, by Michael Wetter:<br/>
- Added output signal <code>Q_flow</code> so that it has
- the same output ports as
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
- AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>.
- </li>
- <li>
- September 11, 2014, by Christoph Nytsch-Geusen:<br/>
- Renaming class to <code>HeaterCooler_u</code>.
- </li>
- <li>
- October 15, 2013, by Michael Wetter:<br/>
- Redeclared the control volume to be final so that it does not show
- anymore in the parameter window.
- </li>
- <li>
- July 11, 2011, by Michael Wetter:<br/>
- Redeclared fluid volume as final. This prevents the fluid volume model
- to appear in the dialog window.
- </li>
- <li>
- May 24, 2011, by Michael Wetter:<br/>
- Changed base class to allow using the model as a dynamic or a steady-state model.
- </li>
- <li>
- April 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 13, 2022, by Fabian Wuellhorst:<br/>
+Added unit to instance <code>gai</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1642\">#1642</a>.
+</li>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Set <code>preHea(final alpha=0)</code> as this allows to simplify the
+system of equations.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/570\">#570</a>.
+</li>
+<li>
+November 19, 2015, by Michael Wetter:<br/>
+Removed assignment of parameter
+<code>showDesignFlowDirection</code> in <code>extends</code> statement.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
+</li>
+<li>
+May 6, 2015, by Michael Wetter:<br/>
+Set <code>prescribedHeatFlowRate=true</code>.
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">
+#412</a>.
+</li>
+<li>
+May 1, 2015, by Marcus Fuchs:<br/>
+Corrected typo in documentation.
+</li>
+<li>
+November 12, 2014, by Michael Wetter:<br/>
+Added output signal <code>Q_flow</code> so that it has
+the same output ports as
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
+AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>.
+</li>
+<li>
+September 11, 2014, by Christoph Nytsch-Geusen:<br/>
+Renaming class to <code>HeaterCooler_u</code>.
+</li>
+<li>
+October 15, 2013, by Michael Wetter:<br/>
+Redeclared the control volume to be final so that it does not show
+anymore in the parameter window.
+</li>
+<li>
+July 11, 2011, by Michael Wetter:<br/>
+Redeclared fluid volume as final. This prevents the fluid volume model
+to appear in the dialog window.
+</li>
+<li>
+May 24, 2011, by Michael Wetter:<br/>
+Changed base class to allow using the model as a dynamic or a steady-state model.
+</li>
+<li>
+April 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeaterCooler_u;
diff --git a/AixLib/Fluid/HeatExchangers/Heater_T.mo b/AixLib/Fluid/HeatExchangers/Heater_T.mo
index 27c4a884fb..ef86b9e7c7 100644
--- a/AixLib/Fluid/HeatExchangers/Heater_T.mo
+++ b/AixLib/Fluid/HeatExchangers/Heater_T.mo
@@ -37,93 +37,93 @@ equation
     annotation (
     defaultComponentName="hea",
 Documentation(info="<html>
- <p>
- Model for an ideal heater that controls its outlet temperature to
- a prescribed outlet temperature.
- </p>
- <p>
- This model forces the outlet temperature at <code>port_b</code> to be
- no lower than the temperature of the input signal
- <code>TSet</code>, subject to optional limits on the
- capacity.
- By default, the model has unlimited heating capacity.
- </p>
- <p>
- The output signal <code>Q_flow</code> is the heat added
- to the medium if the mass flow rate is from <code>port_a</code> to <code>port_b</code>.
- If the flow is reversed, then <code>Q_flow=0</code>.
- </p>
- <p>
- The outlet conditions at <code>port_a</code> are not affected by this model,
- other than for a possible pressure difference due to flow friction.
- </p>
- <p>
- If the parameter <code>energyDynamics</code> is different from
- <code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
- the component models the dynamic response using a first order differential equation.
- The time constant of the component is equal to the parameter <code>tau</code>.
- This time constant is adjusted based on the mass flow rate using
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
- </p>
- <p>
- where
- <i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
- <i>m&#775;</i> and
- <i>&tau;</i> is the time constant at the nominal mass flow rate
- <i>m&#775;<sub>nom</sub></i>.
- This type of dynamics is equal to the dynamics that a completely mixed
- control volume would have.
- </p>
- <p>
- Optionally, this model can have a flow resistance.
- Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
- </p>
- <p>
- For a similar model that is a sensible cooling device, use
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.SensibleCooler_T\">
- AixLib.Fluid.HeatExchangers.SensibleCooler_T</a>.
- For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
- this with the nominal heating or cooling power, use
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
- AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>
- 
- </p>
- <h4>Limitations</h4>
- <p>
- If the flow is from <code>port_b</code> to <code>port_a</code>,
- then the enthalpy of the medium is not affected by this model.
- </p>
- <h4>Validation</h4>
- <p>
- The model has been validated against the analytical solution in
- the examples
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
- AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>
- and
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic\">
- AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic</a>.
- </p>
- </html>",
+<p>
+Model for an ideal heater that controls its outlet temperature to
+a prescribed outlet temperature.
+</p>
+<p>
+This model forces the outlet temperature at <code>port_b</code> to be
+no lower than the temperature of the input signal
+<code>TSet</code>, subject to optional limits on the
+capacity.
+By default, the model has unlimited heating capacity.
+</p>
+<p>
+The output signal <code>Q_flow</code> is the heat added
+to the medium if the mass flow rate is from <code>port_a</code> to <code>port_b</code>.
+If the flow is reversed, then <code>Q_flow=0</code>.
+</p>
+<p>
+The outlet conditions at <code>port_a</code> are not affected by this model,
+other than for a possible pressure difference due to flow friction.
+</p>
+<p>
+If the parameter <code>energyDynamics</code> is different from
+<code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
+the component models the dynamic response using a first order differential equation.
+The time constant of the component is equal to the parameter <code>tau</code>.
+This time constant is adjusted based on the mass flow rate using
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
+</p>
+<p>
+where
+<i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
+<i>m&#775;</i> and
+<i>&tau;</i> is the time constant at the nominal mass flow rate
+<i>m&#775;<sub>nom</sub></i>.
+This type of dynamics is equal to the dynamics that a completely mixed
+control volume would have.
+</p>
+<p>
+Optionally, this model can have a flow resistance.
+Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
+</p>
+<p>
+For a similar model that is a sensible cooling device, use
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.SensibleCooler_T\">
+AixLib.Fluid.HeatExchangers.SensibleCooler_T</a>.
+For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
+this with the nominal heating or cooling power, use
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
+AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>
+
+</p>
+<h4>Limitations</h4>
+<p>
+If the flow is from <code>port_b</code> to <code>port_a</code>,
+then the enthalpy of the medium is not affected by this model.
+</p>
+<h4>Validation</h4>
+<p>
+The model has been validated against the analytical solution in
+the examples
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
+AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>
+and
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic\">
+AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 10, 2018, by Michael Wetter:<br/>
- Corrected missing propagation of initial conditions.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1016\">
- AixLib, #1016</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+September 10, 2018, by Michael Wetter:<br/>
+Corrected missing propagation of initial conditions.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1016\">
+AixLib, #1016</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Rectangle(
           extent={{-70,60},{70,-60}},
@@ -172,6 +172,6 @@ revisions="<html>
           lineColor={0,0,0},
           fillColor={255,255,255},
           fillPattern=FillPattern.Solid),
-        Line(points={{-64,34},{-52,44},{-64,54}}, color={0,0,0})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        Line(points={{-64,34},{-52,44},{-64,54}}, color={0,0,0})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Heater_T;
diff --git a/AixLib/Fluid/HeatExchangers/PrescribedOutlet.mo b/AixLib/Fluid/HeatExchangers/PrescribedOutlet.mo
index 90fd439685..f8860ff02a 100644
--- a/AixLib/Fluid/HeatExchangers/PrescribedOutlet.mo
+++ b/AixLib/Fluid/HeatExchangers/PrescribedOutlet.mo
@@ -140,118 +140,118 @@ equation
           textString="Q_flow")}),
 defaultComponentName="preOut",
 Documentation(info="<html>
- <p>
- Model that allows specifying the temperature and mass fraction of the fluid
- that leaves the model from <code>port_b</code>.
- </p>
- <p>
- This model forces the outlet temperature at <code>port_b</code> to be equal to the temperature
- of the input signal <code>TSet</code>, subject to optional limits on the
- heating or cooling capacity <code>QMax_flow &ge; 0</code> and <code>QMin_flow &le; 0</code>.
- Similarly than for the temperature,
- this model also forces the outlet water mass fraction at <code>port_b</code> to be
- no lower than the
- input signal <code>X_wSet</code>, subject to optional limits on the
- maximum water vapor mass flow rate that is added, as
- described by the parameter <code>mWatMax_flow</code>.
- By default, the model has unlimited capacity, but control of temperature
- and humidity can be subject to capacity limits, or be disabled.
- </p>
- <p>
- The output signal <code>Q_flow</code> is the heat added (for heating) or subtracted (for cooling)
- to the medium if the flow rate is from <code>port_a</code> to <code>port_b</code>.
- If the flow is reversed, then <code>Q_flow=0</code>.
- </p>
- <p>
- The outlet conditions at <code>port_a</code> are not affected by this model.
- </p>
- <p>
- If the parameter <code>energyDynamics</code> is not equal to
- <code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
- the component models the dynamic response using a first order differential equation.
- The time constant of the component is equal to the parameter <code>tau</code>.
- This time constant is adjusted based on the mass flow rate using
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
- </p>
- <p>
- where
- <i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
- <i>m&#775;</i> and
- <i>&tau;</i> is the time constant at the nominal mass flow rate
- <i>m&#775;<sub>nom</sub></i>.
- This type of dynamics is equal to the dynamics that a completely mixed
- control volume would have.
- </p>
- <p>
- Optionally, this model can have a flow resistance.
- If no flow resistance is requested, set <code>dp_nominal=0</code>.
- </p>
- <p>
- For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
- this with the nominal heating or cooling power, use
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
- AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>
- 
- </p>
- <h4>Limitations</h4>
- <p>
- This model only adds or removes heat or water vapor for the flow from
- <code>port_a</code> to <code>port_b</code>.
- The enthalpy of the reverse flow is not affected by this model.
- </p>
- <p>
- If this model is used to cool air below the dew point temperature, the water mass fraction
- will not change.
- </p>
- <p>
- Note that for <code>use_TSet = false</code>, the enthalpy of the leaving fluid
- will not be changed, even if moisture is added. The enthalpy added (or removed)
- by the change in humidity is neglected. To properly account for change in enthalpy
- due to humidification, use instead
- <a href=\"AixLib.Fluid.Humidifiers.SprayAirWasher_X\">
- AixLib.Fluid.Humidifiers.SprayAirWasher_X</a>.
- </p>
- <h4>Validation</h4>
- <p>
- The model has been validated against the analytical solution in
- the examples
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
- AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>
- and
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic\">
- AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic</a>.
- </p>
- </html>",
+<p>
+Model that allows specifying the temperature and mass fraction of the fluid
+that leaves the model from <code>port_b</code>.
+</p>
+<p>
+This model forces the outlet temperature at <code>port_b</code> to be equal to the temperature
+of the input signal <code>TSet</code>, subject to optional limits on the
+heating or cooling capacity <code>QMax_flow &ge; 0</code> and <code>QMin_flow &le; 0</code>.
+Similarly than for the temperature,
+this model also forces the outlet water mass fraction at <code>port_b</code> to be
+no lower than the
+input signal <code>X_wSet</code>, subject to optional limits on the
+maximum water vapor mass flow rate that is added, as
+described by the parameter <code>mWatMax_flow</code>.
+By default, the model has unlimited capacity, but control of temperature
+and humidity can be subject to capacity limits, or be disabled.
+</p>
+<p>
+The output signal <code>Q_flow</code> is the heat added (for heating) or subtracted (for cooling)
+to the medium if the flow rate is from <code>port_a</code> to <code>port_b</code>.
+If the flow is reversed, then <code>Q_flow=0</code>.
+</p>
+<p>
+The outlet conditions at <code>port_a</code> are not affected by this model.
+</p>
+<p>
+If the parameter <code>energyDynamics</code> is not equal to
+<code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
+the component models the dynamic response using a first order differential equation.
+The time constant of the component is equal to the parameter <code>tau</code>.
+This time constant is adjusted based on the mass flow rate using
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
+</p>
+<p>
+where
+<i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
+<i>m&#775;</i> and
+<i>&tau;</i> is the time constant at the nominal mass flow rate
+<i>m&#775;<sub>nom</sub></i>.
+This type of dynamics is equal to the dynamics that a completely mixed
+control volume would have.
+</p>
+<p>
+Optionally, this model can have a flow resistance.
+If no flow resistance is requested, set <code>dp_nominal=0</code>.
+</p>
+<p>
+For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
+this with the nominal heating or cooling power, use
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
+AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>
+
+</p>
+<h4>Limitations</h4>
+<p>
+This model only adds or removes heat or water vapor for the flow from
+<code>port_a</code> to <code>port_b</code>.
+The enthalpy of the reverse flow is not affected by this model.
+</p>
+<p>
+If this model is used to cool air below the dew point temperature, the water mass fraction
+will not change.
+</p>
+<p>
+Note that for <code>use_TSet = false</code>, the enthalpy of the leaving fluid
+will not be changed, even if moisture is added. The enthalpy added (or removed)
+by the change in humidity is neglected. To properly account for change in enthalpy
+due to humidification, use instead
+<a href=\"modelica://AixLib.Fluid.Humidifiers.SprayAirWasher_X\">
+AixLib.Fluid.Humidifiers.SprayAirWasher_X</a>.
+</p>
+<h4>Validation</h4>
+<p>
+The model has been validated against the analytical solution in
+the examples
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
+AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>
+and
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic\">
+AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 3, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- Updated protected model for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- <li>
- November 11, 2014, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- March 19, 2014, by Christoph Nytsch-Geusen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 3, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+Updated protected model for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+<li>
+November 11, 2014, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+March 19, 2014, by Christoph Nytsch-Geusen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutlet;
diff --git a/AixLib/Fluid/HeatExchangers/Radiators/BaseClasses/package.order b/AixLib/Fluid/HeatExchangers/Radiators/BaseClasses/package.order
index 049da99ee9..e1338c0e42 100644
--- a/AixLib/Fluid/HeatExchangers/Radiators/BaseClasses/package.order
+++ b/AixLib/Fluid/HeatExchangers/Radiators/BaseClasses/package.order
@@ -5,3 +5,4 @@ PressureDropRadiator
 RadiatorTypes
 RadiatorWall
 calcHeaterExcessTemp
+RadiatorTypes
diff --git a/AixLib/Fluid/HeatExchangers/Radiators/Examples/RadiatorEN442_2.mo b/AixLib/Fluid/HeatExchangers/Radiators/Examples/RadiatorEN442_2.mo
index 041854850a..81a454be9c 100644
--- a/AixLib/Fluid/HeatExchangers/Radiators/Examples/RadiatorEN442_2.mo
+++ b/AixLib/Fluid/HeatExchangers/Radiators/Examples/RadiatorEN442_2.mo
@@ -105,29 +105,29 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=10800),
     Documentation(info="<html>
- This test model compares the radiator model when
- used as a steady-state and a dynamic model.
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- June 5, 2015 by Michael Wetter:<br/>
- Removed <code>annotation(Evaluate=true)</code> from instances
- <code>T_a_nominal</code> and <code>T_b_nominal</code>
- to avoid the warning about non-literal nominal values.
- This fixes
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/128\">#128</a>.
- </li>
- <li>
- January 30, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This test model compares the radiator model when
+used as a steady-state and a dynamic model.
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+June 5, 2015 by Michael Wetter:<br/>
+Removed <code>annotation(Evaluate=true)</code> from instances
+<code>T_a_nominal</code> and <code>T_b_nominal</code>
+to avoid the warning about non-literal nominal values.
+This fixes
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/128\">#128</a>.
+</li>
+<li>
+January 30, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RadiatorEN442_2;
diff --git a/AixLib/Fluid/HeatExchangers/Radiators/RadiatorEN442_2.mo b/AixLib/Fluid/HeatExchangers/Radiators/RadiatorEN442_2.mo
index ece7c91267..e5871abf8b 100644
--- a/AixLib/Fluid/HeatExchangers/Radiators/RadiatorEN442_2.mo
+++ b/AixLib/Fluid/HeatExchangers/Radiators/RadiatorEN442_2.mo
@@ -313,174 +313,174 @@ equation
           points={{66,60},{66,-60}})}),
     defaultComponentName="rad",
     Documentation(info="<html>
- <p>
- This is a model of a radiator that can be used as a dynamic or steady-state model.
- The required parameters are data that are typically available from
- manufacturers that follow the European Norm EN 442-2.
- </p>
- <p>
- However, to allow for varying mass flow rates, the transferred heat is computed
- using a discretization along the water flow path, and heat is exchanged between
- each compartment and a uniform room air and radiation temperature.
- This discretization is different from the computation in EN 442-2, which
- may yield water outlet temperatures that are below
- the room temperature at low mass flow rates.
- Furthermore, rather than using only one room temperature, this model uses
- a room air and room radiation temperature.
- </p>
- <p>
- The transferred heat is modeled as follows:
- Let <i>N</i> denote the number of elements used to discretize the radiator model.
- For each element <i>i &isin; {1, &hellip; , N}</i>,
- the convective and radiative heat transfer
- <i>Q<sup>i</sup><sub>c</sub></i> and
- <i>Q<sup>i</sup><sub>r</sub></i>
- from the radiator to the room is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   Q<sup>i</sup><sub>c</sub> = sign(T<sup>i</sup>-T<sub>a</sub>)
-      (1-f<sub>r</sub>) UA &frasl; N |T<sup>i</sup>-T<sub>a</sub>|<sup>n</sup>
-   <br/> <br/>
-   Q<sup>i</sup><sub>r</sub> = sign(T<sup>i</sup>-T<sub>r</sub>)
-      f<sub>r</sub> UA &frasl; N |T<sup>i</sup>-T<sub>r</sub>|<sup>n</sup>
- </p>
- <p>
- where
- <i>T<sup>i</sup></i> is the water temperature of the element,
- <i>T<sub>a</sub></i> is the temperature of the room air,
- <i>T<sub>r</sub></i> is the radiative temperature,
- <i>0 &lt; f<sub>r</sub> &lt; 1</i> is the fraction of radiant to total heat transfer,
- <i>UA</i> is the UA-value of the radiator,
- and
- <i>n</i> is an exponent for the heat transfer.
- The model computes the UA-value by numerically solving the above equations
- for given
- nominal heating power, nominal temperatures, fraction radiant to total heat transfer
- and exponent for heat transfer.
- </p>
- <p>
- The parameter <code>energyDynamics</code> (in the Assumptions tab),
- determines whether the model computes the dynamic or the steady-state response.
- For the transient response, heat storage is computed using a
- finite volume approach for the
- water and the metal mass, which are both assumed to be at the same
- temperature.
- </p>
- <p>
- The default parameters for the heat capacities are valid for a flat plate radiator without fins,
- with one plate of water carying fluid, and a height of 0.42 meters.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- November 17, 2016, by Filip Jorissen:<br/>
- Added pressure drop equations and parameters.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/586\">#586</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Set <code>preHea(final alpha=0)</code> as this allows to simplify the
- system of equations.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/570\">#570</a>.
- </li>
- <li>
- March 17, 2016, by Michael Wetter:<br/>
- Reformulated model to reduce the dimension of the nonlinear system of equations.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/435\">#435</a>.
- </li>
- <li>
- November 19, 2015, by Michael Wetter:<br/>
- Removed assignment of parameter
- <code>showDesignFlowDirection</code> in <code>extends</code> statement.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
- </li>
- <li>
- April 11, 2015, by Filip Jorissen:<br/>
- Propagated <code>vol.massDynamics</code> to
- top level parameter <code>massDynamics</code> instead of <code>energyDynamics</code>.
- </li>
- <li>
- November 25, 2014, by Carles Ribas Tugores:<br/>
- Interchange position of <code>fraRad</code> parameter and the complementary <code>(1-fraRad)</code>
- in the equation used to calculate the nominal heating power of each element, <code>QEle_flow_nominal[i]</code>.
- </li>
- <li>
- October 29, 2014, by Michael Wetter:<br/>
- Made assignment of <code>mFactor</code> final, and changed computation of
- density to use default medium states as are also used to compute the
- specific heat capacity.
- </li>
- <li>
- October 21, 2014, by Filip Jorissen:<br/>
- Added parameter <code>mFactor</code> and removed thermal capacity
- which can lead to an index reduction.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Removed conditional statement in the declaration of the parameter
- <code>mDry</code>, as this is incorrect syntax.
- </li>
- <li>
- September 26, 2013 by Michael Wetter:<br/>
- Reformulated implementation to avoid mixing textual and graphical
- declarations in the <code>equation</code> section.
- </li>
- <li>
- April 4, 2011 by Michael Wetter:<br/>
- Changed the implementation to use
- <a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
- AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
- This allows formulating the model without any non-differentiable function
- inside the equation section.
- </li>
- <li>
- April 2, 2011 by Michael Wetter:<br/>
- Added <code>homotopy</code> operator.
- </li>
- <li>
- February 11, 2011 by Michael Wetter:<br/>
- Revised the initialization to ensure that at the nominal conditions, the
- amount of transferred heat is excatly the same as the specified nominal power.
- In the previous implementation, the UA-value was computed using a simplified
- expression for the temperature difference, leading to a slightly different amount
- of heat transfer.
- </li>
- <li>
- February 4, 2011 by Michael Wetter:<br/>
- Simplified implementation.
- </li>
- <li>
- January 30, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    Diagram(graphics={Rectangle(extent={{-62,78},{-46,50}}, lineColor={28,108,200})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a model of a radiator that can be used as a dynamic or steady-state model.
+The required parameters are data that are typically available from
+manufacturers that follow the European Norm EN 442-2.
+</p>
+<p>
+However, to allow for varying mass flow rates, the transferred heat is computed
+using a discretization along the water flow path, and heat is exchanged between
+each compartment and a uniform room air and radiation temperature.
+This discretization is different from the computation in EN 442-2, which
+may yield water outlet temperatures that are below
+the room temperature at low mass flow rates.
+Furthermore, rather than using only one room temperature, this model uses
+a room air and room radiation temperature.
+</p>
+<p>
+The transferred heat is modeled as follows:
+Let <i>N</i> denote the number of elements used to discretize the radiator model.
+For each element <i>i &isin; {1, &hellip; , N}</i>,
+the convective and radiative heat transfer
+<i>Q<sup>i</sup><sub>c</sub></i> and
+<i>Q<sup>i</sup><sub>r</sub></i>
+from the radiator to the room is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  Q<sup>i</sup><sub>c</sub> = sign(T<sup>i</sup>-T<sub>a</sub>)
+     (1-f<sub>r</sub>) UA &frasl; N |T<sup>i</sup>-T<sub>a</sub>|<sup>n</sup>
+  <br/> <br/>
+  Q<sup>i</sup><sub>r</sub> = sign(T<sup>i</sup>-T<sub>r</sub>)
+     f<sub>r</sub> UA &frasl; N |T<sup>i</sup>-T<sub>r</sub>|<sup>n</sup>
+</p>
+<p>
+where
+<i>T<sup>i</sup></i> is the water temperature of the element,
+<i>T<sub>a</sub></i> is the temperature of the room air,
+<i>T<sub>r</sub></i> is the radiative temperature,
+<i>0 &lt; f<sub>r</sub> &lt; 1</i> is the fraction of radiant to total heat transfer,
+<i>UA</i> is the UA-value of the radiator,
+and
+<i>n</i> is an exponent for the heat transfer.
+The model computes the UA-value by numerically solving the above equations
+for given
+nominal heating power, nominal temperatures, fraction radiant to total heat transfer
+and exponent for heat transfer.
+</p>
+<p>
+The parameter <code>energyDynamics</code> (in the Assumptions tab),
+determines whether the model computes the dynamic or the steady-state response.
+For the transient response, heat storage is computed using a
+finite volume approach for the
+water and the metal mass, which are both assumed to be at the same
+temperature.
+</p>
+<p>
+The default parameters for the heat capacities are valid for a flat plate radiator without fins,
+with one plate of water carying fluid, and a height of 0.42 meters.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+November 17, 2016, by Filip Jorissen:<br/>
+Added pressure drop equations and parameters.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/586\">#586</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Set <code>preHea(final alpha=0)</code> as this allows to simplify the
+system of equations.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/570\">#570</a>.
+</li>
+<li>
+March 17, 2016, by Michael Wetter:<br/>
+Reformulated model to reduce the dimension of the nonlinear system of equations.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/435\">#435</a>.
+</li>
+<li>
+November 19, 2015, by Michael Wetter:<br/>
+Removed assignment of parameter
+<code>showDesignFlowDirection</code> in <code>extends</code> statement.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
+</li>
+<li>
+April 11, 2015, by Filip Jorissen:<br/>
+Propagated <code>vol.massDynamics</code> to
+top level parameter <code>massDynamics</code> instead of <code>energyDynamics</code>.
+</li>
+<li>
+November 25, 2014, by Carles Ribas Tugores:<br/>
+Interchange position of <code>fraRad</code> parameter and the complementary <code>(1-fraRad)</code>
+in the equation used to calculate the nominal heating power of each element, <code>QEle_flow_nominal[i]</code>.
+</li>
+<li>
+October 29, 2014, by Michael Wetter:<br/>
+Made assignment of <code>mFactor</code> final, and changed computation of
+density to use default medium states as are also used to compute the
+specific heat capacity.
+</li>
+<li>
+October 21, 2014, by Filip Jorissen:<br/>
+Added parameter <code>mFactor</code> and removed thermal capacity
+which can lead to an index reduction.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Removed conditional statement in the declaration of the parameter
+<code>mDry</code>, as this is incorrect syntax.
+</li>
+<li>
+September 26, 2013 by Michael Wetter:<br/>
+Reformulated implementation to avoid mixing textual and graphical
+declarations in the <code>equation</code> section.
+</li>
+<li>
+April 4, 2011 by Michael Wetter:<br/>
+Changed the implementation to use
+<a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
+AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
+This allows formulating the model without any non-differentiable function
+inside the equation section.
+</li>
+<li>
+April 2, 2011 by Michael Wetter:<br/>
+Added <code>homotopy</code> operator.
+</li>
+<li>
+February 11, 2011 by Michael Wetter:<br/>
+Revised the initialization to ensure that at the nominal conditions, the
+amount of transferred heat is excatly the same as the specified nominal power.
+In the previous implementation, the UA-value was computed using a simplified
+expression for the temperature difference, leading to a slightly different amount
+of heat transfer.
+</li>
+<li>
+February 4, 2011 by Michael Wetter:<br/>
+Simplified implementation.
+</li>
+<li>
+January 30, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Diagram(graphics={Rectangle(extent={{-62,78},{-46,50}}, lineColor={28,108,200})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end RadiatorEN442_2;
diff --git a/AixLib/Fluid/HeatExchangers/SensibleCooler_T.mo b/AixLib/Fluid/HeatExchangers/SensibleCooler_T.mo
index 0c34563a87..294f224934 100644
--- a/AixLib/Fluid/HeatExchangers/SensibleCooler_T.mo
+++ b/AixLib/Fluid/HeatExchangers/SensibleCooler_T.mo
@@ -37,97 +37,97 @@ equation
     annotation (
     defaultComponentName="coo",
 Documentation(info="<html>
- <p>
- Model for an ideal sensible-only cooler that controls its outlet temperature to
- a prescribed outlet temperature.
- </p>
- <p>
- This model forces the outlet temperature at <code>port_b</code> to be
- no higher than the temperature of the input signal
- <code>TSet</code>, subject to optional limits on the
- capacity.
- By default, the model has unlimited cooling capacity.
- </p>
- <p>
- The output signal <code>Q_flow &le; 0</code> is the heat added
- to the medium if the mass flow rate is from <code>port_a</code> to <code>port_b</code>.
- If the flow is reversed, then <code>Q_flow=0</code>.
- </p>
- <p>
- The outlet conditions at <code>port_a</code> are not affected by this model,
- other than for a possible pressure difference due to flow friction.
- </p>
- <p>
- If the parameter <code>energyDynamics</code> is different from
- <code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
- the component models the dynamic response using a first order differential equation.
- The time constant of the component is equal to the parameter <code>tau</code>.
- This time constant is adjusted based on the mass flow rate using
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
- </p>
- <p>
- where
- <i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
- <i>m&#775;</i> and
- <i>&tau;</i> is the time constant at the nominal mass flow rate
- <i>m&#775;<sub>nom</sub></i>.
- This type of dynamics is equal to the dynamics that a completely mixed
- control volume would have.
- </p>
- <p>
- Optionally, this model can have a flow resistance.
- Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
- </p>
- <p>
- For a similar model that is a heater, use
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Heater_T\">
- AixLib.Fluid.HeatExchangers.Heater_T</a>.
- For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
- this with the nominal heating or cooling power, use
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
- AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>.
- </p>
- <h4>Limitations</h4>
- <p>
- If the flow is from <code>port_b</code> to <code>port_a</code>,
- then the enthalpy of the medium is not affected by this model.
- </p>
- <p>
- This model does not affect the humidity of the air. Therefore,
- if used to cool air below the dew point temperature, the water mass fraction
- will not change.
- </p>
- <h4>Validation</h4>
- <p>
- The model has been validated against the analytical solution in
- the examples
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
- AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>
- and
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic\">
- AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic</a>.
- </p>
- </html>",
+<p>
+Model for an ideal sensible-only cooler that controls its outlet temperature to
+a prescribed outlet temperature.
+</p>
+<p>
+This model forces the outlet temperature at <code>port_b</code> to be
+no higher than the temperature of the input signal
+<code>TSet</code>, subject to optional limits on the
+capacity.
+By default, the model has unlimited cooling capacity.
+</p>
+<p>
+The output signal <code>Q_flow &le; 0</code> is the heat added
+to the medium if the mass flow rate is from <code>port_a</code> to <code>port_b</code>.
+If the flow is reversed, then <code>Q_flow=0</code>.
+</p>
+<p>
+The outlet conditions at <code>port_a</code> are not affected by this model,
+other than for a possible pressure difference due to flow friction.
+</p>
+<p>
+If the parameter <code>energyDynamics</code> is different from
+<code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
+the component models the dynamic response using a first order differential equation.
+The time constant of the component is equal to the parameter <code>tau</code>.
+This time constant is adjusted based on the mass flow rate using
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
+</p>
+<p>
+where
+<i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
+<i>m&#775;</i> and
+<i>&tau;</i> is the time constant at the nominal mass flow rate
+<i>m&#775;<sub>nom</sub></i>.
+This type of dynamics is equal to the dynamics that a completely mixed
+control volume would have.
+</p>
+<p>
+Optionally, this model can have a flow resistance.
+Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
+</p>
+<p>
+For a similar model that is a heater, use
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Heater_T\">
+AixLib.Fluid.HeatExchangers.Heater_T</a>.
+For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
+this with the nominal heating or cooling power, use
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
+AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>.
+</p>
+<h4>Limitations</h4>
+<p>
+If the flow is from <code>port_b</code> to <code>port_a</code>,
+then the enthalpy of the medium is not affected by this model.
+</p>
+<p>
+This model does not affect the humidity of the air. Therefore,
+if used to cool air below the dew point temperature, the water mass fraction
+will not change.
+</p>
+<h4>Validation</h4>
+<p>
+The model has been validated against the analytical solution in
+the examples
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
+AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>
+and
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic\">
+AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet_dynamic</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 10, 2018, by Michael Wetter:<br/>
- Corrected missing propagation of initial conditions.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1016\">
- AixLib, #1016</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
- AixLib, #763</a>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+September 10, 2018, by Michael Wetter:<br/>
+Corrected missing propagation of initial conditions.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1016\">
+AixLib, #1016</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">
+AixLib, #763</a>.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Rectangle(
           extent={{-70,60},{70,-60}},
@@ -176,6 +176,6 @@ revisions="<html>
         Text(
           extent={{-110,102},{-74,84}},
           textColor={0,0,127},
-          textString="T")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="T")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SensibleCooler_T;
diff --git a/AixLib/Fluid/HeatExchangers/Validation/ConstantEffectiveness.mo b/AixLib/Fluid/HeatExchangers/Validation/ConstantEffectiveness.mo
index ace9b8bbe4..a03ea04f74 100644
--- a/AixLib/Fluid/HeatExchangers/Validation/ConstantEffectiveness.mo
+++ b/AixLib/Fluid/HeatExchangers/Validation/ConstantEffectiveness.mo
@@ -114,19 +114,19 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/ConstantEffectiveness.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model tests
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ConstantEffectiveness\">
- AixLib.Fluid.HeatExchangers.ConstantEffectiveness</a>
- for different inlet conditions.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 28, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ConstantEffectiveness\">
+AixLib.Fluid.HeatExchangers.ConstantEffectiveness</a>
+for different inlet conditions.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 28, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantEffectiveness;
diff --git a/AixLib/Fluid/HeatExchangers/Validation/DryCoilEffectivenessNTU.mo b/AixLib/Fluid/HeatExchangers/Validation/DryCoilEffectivenessNTU.mo
index 25e0c05aa4..f01c80401f 100644
--- a/AixLib/Fluid/HeatExchangers/Validation/DryCoilEffectivenessNTU.mo
+++ b/AixLib/Fluid/HeatExchangers/Validation/DryCoilEffectivenessNTU.mo
@@ -252,25 +252,25 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/DryCoilEffectivenessNTU.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model tests
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
- for different inlet conditions.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- February 12, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
+for different inlet conditions.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+February 12, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DryCoilEffectivenessNTU;
diff --git a/AixLib/Fluid/HeatExchangers/Validation/EvaporatorCondenser.mo b/AixLib/Fluid/HeatExchangers/Validation/EvaporatorCondenser.mo
index 69ccbd1581..0de9dfef6d 100644
--- a/AixLib/Fluid/HeatExchangers/Validation/EvaporatorCondenser.mo
+++ b/AixLib/Fluid/HeatExchangers/Validation/EvaporatorCondenser.mo
@@ -68,24 +68,24 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=100),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.EvaporatorCondenser\">
- AixLib.Fluid.HeatExchangers.EvaporatorCondenser</a> model.
- </p>
- <p>
- The fluid flow rate is increased from <i>m&#775; = 0.01 kg/s</i> to
- <i>m&#775; = 0.10 kg/s</i> over 100 seconds. As a result, the heat exchanger
- effectiveness and the fluid temperature difference in the heat exchanger
- decrease.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 11, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.EvaporatorCondenser\">
+AixLib.Fluid.HeatExchangers.EvaporatorCondenser</a> model.
+</p>
+<p>
+The fluid flow rate is increased from <i>m&#775; = 0.01 kg/s</i> to
+<i>m&#775; = 0.10 kg/s</i> over 100 seconds. As a result, the heat exchanger
+effectiveness and the fluid temperature difference in the heat exchanger
+decrease.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 11, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EvaporatorCondenser;
diff --git a/AixLib/Fluid/HeatExchangers/Validation/HeaterCooler_u.mo b/AixLib/Fluid/HeatExchangers/Validation/HeaterCooler_u.mo
index 8a0189b4b5..cddaca05cf 100644
--- a/AixLib/Fluid/HeatExchangers/Validation/HeaterCooler_u.mo
+++ b/AixLib/Fluid/HeatExchangers/Validation/HeaterCooler_u.mo
@@ -108,33 +108,33 @@ equation
             200}}), graphics),
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/HeaterCooler_u.mos" "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of an ideal heater.
- Both heater models are identical, except that one model is configured
- as a steady-state model, whereas the other is configured as a dynamic model.
- Both heaters add heat to the medium to track a set-point for the outlet
- temperature.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 11, 2014, by Christoph Nytsch-Geusen:<br/>
- Rename experiment to HetaterColler_u
- in the Annex 60 library.
- </li>
- <li>
- September 19, 2013, by Michael Wetter:<br/>
- Removed fan with a prescribed mass flow source for inclusion of the test model
- in the Annex 60 library.
- </li>
- <li>
- July 11, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that demonstrates the use of an ideal heater.
+Both heater models are identical, except that one model is configured
+as a steady-state model, whereas the other is configured as a dynamic model.
+Both heaters add heat to the medium to track a set-point for the outlet
+temperature.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 11, 2014, by Christoph Nytsch-Geusen:<br/>
+Rename experiment to HetaterColler_u
+in the Annex 60 library.
+</li>
+<li>
+September 19, 2013, by Michael Wetter:<br/>
+Removed fan with a prescribed mass flow source for inclusion of the test model
+in the Annex 60 library.
+</li>
+<li>
+July 11, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=1200,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeaterCooler_u;
diff --git a/AixLib/Fluid/HeatExchangers/Validation/PrescribedOutlet.mo b/AixLib/Fluid/HeatExchangers/Validation/PrescribedOutlet.mo
index 6c0fda4036..f8c7988736 100644
--- a/AixLib/Fluid/HeatExchangers/Validation/PrescribedOutlet.mo
+++ b/AixLib/Fluid/HeatExchangers/Validation/PrescribedOutlet.mo
@@ -155,37 +155,37 @@ equation
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/PrescribedOutlet.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of an ideal heater and an ideal cooler.
- </p>
- <p>
- The heater model has a capacity of <code>Q_flow_max = 1.0e4</code> Watts and
- the cooler model has a capacitiy of <code>Q_flow_min = -1000</code> Watts.
- Hence, both only track their set point of the outlet temperature during certain times.
- There is also a heater and cooler with unlimited capacity.
- </p>
- <p>
- At <i>t=1000</i> second, the flow reverses its direction.
- </p>
- <p>
- Each flow leg has the same mass flow rate. There are three mass flow sources
- as using one source only would yield a nonlinear system of equations that
- needs to be solved to determine the mass flow rate distribution.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 21, 2014, by Michael Wetter:<br/>
- Revised example to test reverse flow and zero flow transition.
- </li>
- <li>
- March 19, 2014, by Christoph Nytsch-Geusen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that demonstrates the use of an ideal heater and an ideal cooler.
+</p>
+<p>
+The heater model has a capacity of <code>Q_flow_max = 1.0e4</code> Watts and
+the cooler model has a capacitiy of <code>Q_flow_min = -1000</code> Watts.
+Hence, both only track their set point of the outlet temperature during certain times.
+There is also a heater and cooler with unlimited capacity.
+</p>
+<p>
+At <i>t=1000</i> second, the flow reverses its direction.
+</p>
+<p>
+Each flow leg has the same mass flow rate. There are three mass flow sources
+as using one source only would yield a nonlinear system of equations that
+needs to be solved to determine the mass flow rate distribution.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 21, 2014, by Michael Wetter:<br/>
+Revised example to test reverse flow and zero flow transition.
+</li>
+<li>
+March 19, 2014, by Christoph Nytsch-Geusen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=1200,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutlet;
diff --git a/AixLib/Fluid/HeatExchangers/Validation/PrescribedOutlet_dynamic.mo b/AixLib/Fluid/HeatExchangers/Validation/PrescribedOutlet_dynamic.mo
index af6af897aa..d8f29478ec 100644
--- a/AixLib/Fluid/HeatExchangers/Validation/PrescribedOutlet_dynamic.mo
+++ b/AixLib/Fluid/HeatExchangers/Validation/PrescribedOutlet_dynamic.mo
@@ -10,27 +10,27 @@ model PrescribedOutlet_dynamic
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/PrescribedOutlet_dynamic.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of an ideal heater and an ideal cooler, configured as dynamic models.
- </p>
- <p>
- This example is identical to
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
- AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>
- except that the heater and cooler models are configured to have a
- time constant of <i>60</i> seconds at nominal flow rate.
- At lower flow rate, the time constant increases proportional to the mass flow rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 21, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that demonstrates the use of an ideal heater and an ideal cooler, configured as dynamic models.
+</p>
+<p>
+This example is identical to
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet\">
+AixLib.Fluid.HeatExchangers.Validation.PrescribedOutlet</a>
+except that the heater and cooler models are configured to have a
+time constant of <i>60</i> seconds at nominal flow rate.
+At lower flow rate, the time constant increases proportional to the mass flow rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 21, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=1200,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutlet_dynamic;
diff --git a/AixLib/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mo b/AixLib/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mo
index d56518e75e..e37e12353b 100644
--- a/AixLib/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mo
+++ b/AixLib/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mo
@@ -193,44 +193,44 @@ equation
     file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mos"
   "Simulate and plot"),
   Documentation(info="<html>
- <p>
- This model duplicates an example from Mitchell and Braun 2012, example SM-2-1
- (Mitchell and Braun 2012) to validate a single case for the
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.WetCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.WetCoilEffectivenessNTU</a>
- model.
- </p>
- <h4>Validation</h4>
- <p>
- The example simulates a wet coil with constant air
- and water inlet temperature and mass flow rate, and an increasing air inlet
- humidity which triggers the transition from a fully-dry to a fully-wet regime.
- The reference used for validation is the published experimental data.
- </p>
- <p>
- Note that the outlet air relative humidity may slightly exceed 100% when using
- the epsilon-NTU model.
- </p>
- <h4>References</h4>
- <p>
- Mitchell, John W., and James E. Braun. 2012.
- \"Supplementary Material Chapter 2: Heat Exchangers for Cooling Applications\".
- Excerpt from <i>Principles of heating, ventilation, and air conditioning in buildings</i>.
- Hoboken, N.J.: Wiley. Available online:
- <a href=\"http://bcs.wiley.com/he-bcs/Books?action=index&amp;itemId=0470624574&amp;bcsId=7185\">
- http://bcs.wiley.com/he-bcs/Books?action=index&amp;itemId=0470624574&amp;bcsId=7185</a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 19, 2017, by Michael Wetter:<br/>
- Revised model to avoid mixing textual equations and connect statements.
- </li>
- <li>
- March 17, 2017, by Michael O'Keefe:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model duplicates an example from Mitchell and Braun 2012, example SM-2-1
+(Mitchell and Braun 2012) to validate a single case for the
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.WetCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.WetCoilEffectivenessNTU</a>
+model.
+</p>
+<h4>Validation</h4>
+<p>
+The example simulates a wet coil with constant air
+and water inlet temperature and mass flow rate, and an increasing air inlet
+humidity which triggers the transition from a fully-dry to a fully-wet regime.
+The reference used for validation is the published experimental data.
+</p>
+<p>
+Note that the outlet air relative humidity may slightly exceed 100% when using
+the epsilon-NTU model.
+</p>
+<h4>References</h4>
+<p>
+Mitchell, John W., and James E. Braun. 2012.
+\"Supplementary Material Chapter 2: Heat Exchangers for Cooling Applications\".
+Excerpt from <i>Principles of heating, ventilation, and air conditioning in buildings</i>.
+Hoboken, N.J.: Wiley. Available online:
+<a href=\"http://bcs.wiley.com/he-bcs/Books?action=index&amp;itemId=0470624574&amp;bcsId=7185\">
+http://bcs.wiley.com/he-bcs/Books?action=index&amp;itemId=0470624574&amp;bcsId=7185</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 19, 2017, by Michael Wetter:<br/>
+Revised model to avoid mixing textual equations and connect statements.
+</li>
+<li>
+March 17, 2017, by Michael O'Keefe:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WetCoilEffectivenessNTU;
diff --git a/AixLib/Fluid/HeatExchangers/WetCoilEffectivenessNTU.mo b/AixLib/Fluid/HeatExchangers/WetCoilEffectivenessNTU.mo
index 0007ad10df..1d17ce8f3a 100644
--- a/AixLib/Fluid/HeatExchangers/WetCoilEffectivenessNTU.mo
+++ b/AixLib/Fluid/HeatExchangers/WetCoilEffectivenessNTU.mo
@@ -10,6 +10,13 @@ model WetCoilEffectivenessNTU
   import con = AixLib.Fluid.Types.HeatExchangerConfiguration;
   import flo = AixLib.Fluid.Types.HeatExchangerFlowRegime;
 
+  constant Boolean use_dynamicFlowRegime = false
+    "If true, flow regime is determined using actual flow rates";
+  // This switch is declared as a constant instead of a parameter
+  //   as users typically need not to change this setting,
+  //   and setting it true may generate events.
+  //   See discussions in https://github.com/ibpsa/modelica-ibpsa/pull/1683
+
   parameter AixLib.Fluid.Types.HeatExchangerConfiguration configuration=
     con.CounterFlow
     "Heat exchanger configuration";
@@ -72,6 +79,7 @@ model WetCoilEffectivenessNTU
 
   Real dryFra(final unit="1", min=0, max=1) = dryWetCalcs.dryFra
     "Dry fraction, 0.3 means condensation occurs at 30% heat exchange length from air inlet";
+
 protected
   final parameter Modelica.Units.SI.MassFraction X_w_a2_nominal=w_a2_nominal/(1
        + w_a2_nominal)
@@ -228,12 +236,12 @@ protected
       m1_flow_small)
     else 1
     "Fraction of incoming state taken from port a2
-     (used to avoid excessive calls to regStep)";
+    (used to avoid excessive calls to regStep)";
   Real fra_b1(min=0, max=1) = if allowFlowReversal1
     then 1-fra_a1
     else 0
     "Fraction of incoming state taken from port b2
-     (used to avoid excessive calls to regStep)";
+    (used to avoid excessive calls to regStep)";
   Real fra_a2(min=0, max=1) = if allowFlowReversal2
     then Modelica.Fluid.Utilities.regStep(
       m2_flow,
@@ -242,12 +250,12 @@ protected
       m2_flow_small)
     else 1
     "Fraction of incoming state taken from port a2
-     (used to avoid excessive calls to regStep)";
+    (used to avoid excessive calls to regStep)";
   Real fra_b2(min=0, max=1) = if allowFlowReversal2
     then 1-fra_a2
     else 0
     "Fraction of incoming state taken from port b2
-     (used to avoid excessive calls to regStep)";
+    (used to avoid excessive calls to regStep)";
 
   Modelica.Units.SI.ThermalConductance C1_flow=abs(m1_flow)*(if
       allowFlowReversal1 then fra_a1*Medium1.specificHeatCapacityCp(
@@ -277,6 +285,13 @@ protected
      X=Medium2.X_default[1:Medium2.nXi]) "Default state for medium 2";
 
 initial equation
+  assert(m1_flow_nominal > Modelica.Constants.eps,
+    "m1_flow_nominal must be positive, m1_flow_nominal = " + String(
+    m1_flow_nominal));
+  assert(m2_flow_nominal > Modelica.Constants.eps,
+    "m2_flow_nominal must be positive, m2_flow_nominal = " + String(
+    m2_flow_nominal));
+
   cp1_nominal = Medium1.specificHeatCapacityCp(sta1_default);
   cp2_nominal = Medium2.specificHeatCapacityCp(sta2_default);
   C1_flow_nominal = m1_flow_nominal*cp1_nominal;
@@ -310,33 +325,47 @@ initial equation
 equation
   // Assign the flow regime for the given heat exchanger configuration and
   // mass flow rates
-  if (configuration == con.ParallelFlow) then
-    flowRegime = if (C1_flow*C2_flow >= 0)
-      then
-        flo.ParallelFlow
-      else
-        flo.CounterFlow;
-  elseif (configuration == con.CounterFlow) then
-    flowRegime = if (C1_flow*C2_flow >= 0)
-      then
-        flo.CounterFlow
-      else
-        flo.ParallelFlow;
-  elseif (configuration == con.CrossFlowUnmixed) then
-    flowRegime = flo.CrossFlowUnmixed;
-  elseif (configuration == con.CrossFlowStream1MixedStream2Unmixed) then
-    flowRegime = if (C1_flow < C2_flow)
-      then
-        flo.CrossFlowCMinMixedCMaxUnmixed
-      else
-        flo.CrossFlowCMinUnmixedCMaxMixed;
+  if use_dynamicFlowRegime then
+    if (configuration == con.ParallelFlow) then
+      flowRegime = if (C1_flow*C2_flow >= 0)
+        then
+          flo.ParallelFlow
+        else
+          flo.CounterFlow;
+    elseif (configuration == con.CounterFlow) then
+      flowRegime = if (C1_flow*C2_flow >= 0)
+        then
+          flo.CounterFlow
+        else
+          flo.ParallelFlow;
+    elseif (configuration == con.CrossFlowUnmixed) then
+      flowRegime = flo.CrossFlowUnmixed;
+    elseif (configuration == con.CrossFlowStream1MixedStream2Unmixed) then
+      flowRegime = if (C1_flow < C2_flow)
+        then
+          flo.CrossFlowCMinMixedCMaxUnmixed
+        else
+          flo.CrossFlowCMinUnmixedCMaxMixed;
+    else
+      // have ( configuration == con.CrossFlowStream1UnmixedStream2Mixed)
+      flowRegime = if (C1_flow < C2_flow)
+        then
+          flo.CrossFlowCMinUnmixedCMaxMixed
+        else
+          flo.CrossFlowCMinMixedCMaxUnmixed;
+    end if;
   else
-    // have ( configuration == con.CrossFlowStream1UnmixedStream2Mixed)
-    flowRegime = if (C1_flow < C2_flow)
-      then
-        flo.CrossFlowCMinUnmixedCMaxMixed
-      else
-        flo.CrossFlowCMinMixedCMaxUnmixed;
+    flowRegime = flowRegime_nominal;
+    assert(noEvent(m1_flow > -0.1 * m1_flow_nominal)
+       and noEvent(m2_flow > -0.1 * m2_flow_nominal),
+"*** Warning in " + getInstanceName() +
+      ": The flow direction reversed.
+      However, because the constant use_dynamicFlowRegime is set to false,
+      the model does not change equations based on the actual flow regime.
+      To switch equations based on the actual flow regime during the simulation,
+      set the constant use_dynamicFlowRegime=true.
+      Note that this can lead to slow simulation because of events.",
+      level = AssertionLevel.warning);
   end if;
 
   connect(heaCoo.port_b, port_b1) annotation (Line(points={{80,60},{80,60},{100,60}},color={0,127,255},
@@ -508,125 +537,151 @@ equation
           horizontalAlignment=TextAlignment.Left,
           textString="Air Side")}),
     Documentation(info="<html>
- <p>
- This model describes a cooling coil applicable for fully-dry,
- partially-wet, and fully-wet regimes.
- The model is developed for counter flow heat exchangers but is also applicable
- for the cross-flow configuration, although in the latter case it is recommended
- to have more than four tube rows (Elmahdy and Mitalas, 1977 and Braun, 1988).
- The model can also be used for a heat exchanger which acts as both heating coil
- (for some period of time) and cooling coil (for the others).
- However, it is not recommended to use this model for heating coil only or for
- cooling coil with no water condensation because for these situations,
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
- computes faster.
- </p>
- <h4>Main equations</h4>
- <p>
- The coil model consists of two-equation sets, one for the fully-dry mode and
- the other for the fully-wet mode. For the fully-dry mode, the <i>&epsilon;-NTU</i>
- approach (Elmahdy and Mitalas, 1977) is used.
- For the fully-wet mode, equations from Braun (1988) and Mitchell and Braun (2012a and b),
- which are essentially the extension of the <i>&epsilon;-NTU</i> approach to simultaneous sensible
- and latent heat transfer, are utilized.
- The equation sets are switched depending on the switching criteria described below
- that determines the right mode based on a coil surface temperature and dew-point
- temperature for the air at the inlet of the coil.
- The transition regime between the two modes, which represents the partially-wet and
- partially-dry coil, is approximated by employing a fuzzy modeling approach,
- so-called Takagi-Sugeno fuzzy modeling (Takagi and Sugeno, 1985), which provides a
- continuously differentiable model that can cover all fully-dry, partially-wet,
- and fully-wet regimes.
- </p>
- <p>The switching rules are:</p>
- <ul>
- <li>R1: If the coil surface temperature at the air inlet is lower than the
- dew-point temperature of air at inlet, then the cooling coil surface is fully-wet.
- </li>
- <li>
- R2: If the coil surface temperature at the air outlet is higher than the
- dew-point temperature of air at inlet, then the cooling coil surface is fully-dry.
- </li>
- <li>
- R3: If any of the conditions in R1 or R2 is not satisfied, then the cooling coil
- surface is partially wet.
- </li>
- </ul>
- <p>
- For more detailed descriptions of the fully-wet coil model and the fuzzy modeling approach,
- see
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.WetCoilWetRegime\">
- AixLib.Fluid.HeatExchangers.BaseClasses.WetCoilWetRegime</a>.
- and
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.WetCoilDryWetRegime\">
- AixLib.Fluid.HeatExchangers.BaseClasses.WetCoilDryWetRegime</a>.
- </p>
- <h4>Assumptions and limitations</h4>
- <p>This model contains the following assumptions and limitations:</p>
- <p>Medium 2 must be air due to the use of various psychrometric functions.</p>
- <p>
- When parameterizing this model with rated conditions (with the parameter
- <code>use_UA_nominal</code> set to <code>false</code>), those should
- correspond to a fully-dry or a fully-wet coil regime, because
- the model uncertainty yielded by partially-wet rated conditions
- has not been assessed yet.
- </p>
- <p>The model uses steady-state physics. That is, no dynamics associated
- with water and coil materials are considered.</p>
- <p>The Lewis number, which relates the mass transfer coefficient to the heat transfer
- coefficient, is assumed to be <i>1</i>.</p>
- <p>The model is not suitable for a cross-flow heat exchanger of which the number
- of passes is less than four.</p>
- <h4>Validation</h4>
- <p>Validation results can be found in
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.WetCoilEffectivenessNTU\">
- AixLib.Fluid.HeatExchangers.Validation.WetCoilEffectivenessNTU</a>.
- <h4>References</h4>
- <p>Braun, James E. 1988.
- &quot;Methodologies for the Design and Control of
- Central Cooling Plants&quot;.
- PhD Thesis. University of Wisconsin - Madison.
- Available
- <a href=\"https://minds.wisconsin.edu/handle/1793/46694\">
- online</a>.
- </p>
- <p>Mitchell, John W., and James E. Braun. 2012a.
- Principles of heating, ventilation, and air conditioning in buildings.
- Hoboken, N.J.: Wiley.</p>
- <p>Mitchell, John W., and James E. Braun. 2012b.
- &quot;Supplementary Material Chapter 2: Heat Exchangers for Cooling Applications&quot;.
- Excerpt from Principles of heating, ventilation, and air conditioning in buildings.
- Hoboken, N.J.: Wiley.
- Available
- <a href=\"http://bcs.wiley.com/he-bcs/Books?action=index&amp;itemId=0470624574&amp;bcsId=7185\">
- online</a>.
- </p>
- <p>Elmahdy, A.H. and Mitalas, G.P. 1977.
- &quot;A Simple Model for Cooling and Dehumidifying Coils for Use
- In Calculating Energy Requirements for Buildings&quot;.
- ASHRAE Transactions. Vol.83. Part 2. pp. 103-117.</p>
- <p>Takagi, T. and Sugeno, M., 1985.
- Fuzzy identification of systems and its applications to modeling and control.
- &nbsp;IEEE transactions on systems, man, and cybernetics, (1), pp.116-132.</p>
- </html>",                   revisions="<html>
- <ul>
- <li>
- March 3, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
- </li>
- <li>
- November 2, 2021, by Michael Wetter:<br/>
- Corrected unit assignment during the model instantiation.<br/>
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2710\">issue 2710</a>.
- </li>
- <li>
- Jan 21, 2021, by Donghun Kim:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model describes a cooling coil applicable for fully-dry,
+partially-wet, and fully-wet regimes.
+The model is developed for counter flow heat exchangers but is also applicable
+for the cross-flow configuration, although in the latter case it is recommended
+to have more than four tube rows (Elmahdy and Mitalas, 1977 and Braun, 1988).
+The model can also be used for a heat exchanger which acts as both heating coil
+(for some period of time) and cooling coil (for the others).
+However, it is not recommended to use this model for heating coil only or for
+cooling coil with no water condensation because for these situations,
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.DryCoilEffectivenessNTU</a>
+computes faster.
+</p>
+<h4>Main equations</h4>
+<p>
+The coil model consists of two-equation sets, one for the fully-dry mode and
+the other for the fully-wet mode. For the fully-dry mode, the <i>&epsilon;-NTU</i>
+approach (Elmahdy and Mitalas, 1977) is used.
+For the fully-wet mode, equations from Braun (1988) and Mitchell and Braun (2012a and b),
+which are essentially the extension of the <i>&epsilon;-NTU</i> approach to simultaneous sensible
+and latent heat transfer, are utilized.
+The equation sets are switched depending on the switching criteria described below
+that determines the right mode based on a coil surface temperature and dew-point
+temperature for the air at the inlet of the coil.
+The transition regime between the two modes, which represents the partially-wet and
+partially-dry coil, is approximated by employing a fuzzy modeling approach,
+so-called Takagi-Sugeno fuzzy modeling (Takagi and Sugeno, 1985), which provides a
+continuously differentiable model that can cover all fully-dry, partially-wet,
+and fully-wet regimes.
+</p>
+<p>The switching rules are:</p>
+<ul>
+<li>R1: If the coil surface temperature at the air inlet is lower than the
+dew-point temperature of air at inlet, then the cooling coil surface is fully-wet.
+</li>
+<li>
+R2: If the coil surface temperature at the air outlet is higher than the
+dew-point temperature of air at inlet, then the cooling coil surface is fully-dry.
+</li>
+<li>
+R3: If any of the conditions in R1 or R2 is not satisfied, then the cooling coil
+surface is partially wet.
+</li>
+</ul>
+<p>
+For more detailed descriptions of the fully-wet coil model and the fuzzy modeling approach,
+see
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.WetCoilWetRegime\">
+AixLib.Fluid.HeatExchangers.BaseClasses.WetCoilWetRegime</a>.
+and
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.WetCoilDryWetRegime\">
+AixLib.Fluid.HeatExchangers.BaseClasses.WetCoilDryWetRegime</a>.
+</p>
+<h4>Assumptions and limitations</h4>
+<p>This model contains the following assumptions and limitations:</p>
+<p>Medium 2 must be air due to the use of various psychrometric functions.</p>
+<p>
+When parameterizing this model with rated conditions (with the parameter
+<code>use_UA_nominal</code> set to <code>false</code>), those should
+correspond to a fully-dry or a fully-wet coil regime, because
+the model uncertainty yielded by partially-wet rated conditions
+has not been assessed yet.
+</p>
+<p>The model uses steady-state physics. That is, no dynamics associated
+with water and coil materials are considered.</p>
+<p>The Lewis number, which relates the mass transfer coefficient to the heat transfer
+coefficient, is assumed to be <i>1</i>.</p>
+<p>The model is not suitable for a cross-flow heat exchanger of which the number
+of passes is less than four.</p>
+<p>
+By default, the flow regime, such as counter flow or parallel flow,
+is kept constant based on the parameter value <code>configuration</code>.
+If a flow reverses direction, it is not changed, e.g.,
+a heat exchanger does not change from counter flow to parallel flow
+if one flow changes direction.
+To dynamically change the flow regime,
+set the constant <code>use_dynamicFlowRegime</code> to
+<code>true</code>.
+However, <code>use_dynamicFlowRegime=true</code>
+can cause slower simulation due to events.
+</p>
+<h4>Validation</h4>
+<p>Validation results can be found in
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Validation.WetCoilEffectivenessNTU\">
+AixLib.Fluid.HeatExchangers.Validation.WetCoilEffectivenessNTU</a>.
+<h4>References</h4>
+<p>Braun, James E. 1988.
+&quot;Methodologies for the Design and Control of
+Central Cooling Plants&quot;.
+PhD Thesis. University of Wisconsin - Madison.
+Available
+<a href=\"https://minds.wisconsin.edu/handle/1793/46694\">
+online</a>.
+</p>
+<p>Mitchell, John W., and James E. Braun. 2012a.
+Principles of heating, ventilation, and air conditioning in buildings.
+Hoboken, N.J.: Wiley.</p>
+<p>Mitchell, John W., and James E. Braun. 2012b.
+&quot;Supplementary Material Chapter 2: Heat Exchangers for Cooling Applications&quot;.
+Excerpt from Principles of heating, ventilation, and air conditioning in buildings.
+Hoboken, N.J.: Wiley.
+Available
+<a href=\"http://bcs.wiley.com/he-bcs/Books?action=index&amp;itemId=0470624574&amp;bcsId=7185\">
+online</a>.
+</p>
+<p>Elmahdy, A.H. and Mitalas, G.P. 1977.
+&quot;A Simple Model for Cooling and Dehumidifying Coils for Use
+In Calculating Energy Requirements for Buildings&quot;.
+ASHRAE Transactions. Vol.83. Part 2. pp. 103-117.</p>
+<p>Takagi, T. and Sugeno, M., 1985.
+Fuzzy identification of systems and its applications to modeling and control.
+&nbsp;IEEE transactions on systems, man, and cybernetics, (1), pp.116-132.</p>
+</html>",                    revisions="<html>
+<ul>
+<li>
+February 3, 2023, by Jianjun Hu:<br/>
+Added <code>noEvent()</code> in the assertion function to avoid Optimica to not converge.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1690\">issue 1690</a>.
+</li>
+<li>
+January 24, 2023, by Hongxiang Fu:<br/>
+Set <code>flowRegime</code> to be equal to <code>flowRegime_nominal</code>
+by default. Added an assertion warning to inform the user about how to change
+this behaviour if the flow direction does need to change.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1682\">issue 1682</a>.
+</li>
+<li>
+March 3, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
+</li>
+<li>
+November 2, 2021, by Michael Wetter:<br/>
+Corrected unit assignment during the model instantiation.<br/>
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2710\">issue 2710</a>.
+</li>
+<li>
+Jan 21, 2021, by Donghun Kim:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WetCoilEffectivenessNTU;
diff --git a/AixLib/Fluid/HeatPumps/BaseClasses/PartialWaterToWater.mo b/AixLib/Fluid/HeatPumps/BaseClasses/PartialWaterToWater.mo
index 4fd7004a73..898b9976c2 100644
--- a/AixLib/Fluid/HeatPumps/BaseClasses/PartialWaterToWater.mo
+++ b/AixLib/Fluid/HeatPumps/BaseClasses/PartialWaterToWater.mo
@@ -166,8 +166,9 @@ equation
     annotation (Line(points={{-100,60},{40,60}},  color={0,127,255}));
   connect(con.port_b, port_b1)
     annotation (Line(points={{60,60},{60,60},{100,60}}, color={0,127,255}));
-  connect(con.Q_flow, QCon_flow) annotation (Line(points={{61,64},{60,64},{60,90},
-          {110,90}}, color={0,0,127}));
+  connect(con.Q_flow, QCon_flow) annotation (Line(points={{61,64},{80,64},{80,
+          90},{110,90}},
+                     color={0,0,127}));
   connect(eva.port_a, port_a2)
     annotation (Line(points={{60,-60},{100,-60}}, color={0,127,255}));
   connect(eva.port_b, port_b2)
@@ -302,41 +303,41 @@ equation
         Line(points={{62,0},{100,0}},                 color={0,0,255})}),
     defaultComponentName="heaPum",
     Documentation(info="<html>
- <p>
- Partial model for a water to water heat pump, as detailed in Jin (2002). The
- model for the compressor is a partial model and needs to be replaced by one of the
- compressor models in
- <a href = \"modelica://AixLib.Fluid.HeatPumps.Compressors\">
- AixLib.Fluid.HeatPumps.Compressors</a>.
- </p>
- <h4>References</h4>
- <p>
- H. Jin.
- <i>
- Parameter estimation based models of water source heat pumps.
- </i>
- PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- May 30, 2017, by Filip Jorissen:<br/>
- Added temperature protection block and
- set <code>energyDynamics=DynamicFreeInitial</code>.
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">
- #769</a>.
- </li>
- <li>
- October 17, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model for a water to water heat pump, as detailed in Jin (2002). The
+model for the compressor is a partial model and needs to be replaced by one of the
+compressor models in
+<a href = \"modelica://AixLib.Fluid.HeatPumps.Compressors\">
+AixLib.Fluid.HeatPumps.Compressors</a>.
+</p>
+<h4>References</h4>
+<p>
+H. Jin.
+<i>
+Parameter estimation based models of water source heat pumps.
+</i>
+PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+May 30, 2017, by Filip Jorissen:<br/>
+Added temperature protection block and
+set <code>energyDynamics=DynamicFreeInitial</code>.
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">
+#769</a>.
+</li>
+<li>
+October 17, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialWaterToWater;
diff --git a/AixLib/Fluid/HeatPumps/Calibration/BaseClasses/PartialWaterToWater.mo b/AixLib/Fluid/HeatPumps/Calibration/BaseClasses/PartialWaterToWater.mo
index 894b31244c..bb10c3d6a5 100644
--- a/AixLib/Fluid/HeatPumps/Calibration/BaseClasses/PartialWaterToWater.mo
+++ b/AixLib/Fluid/HeatPumps/Calibration/BaseClasses/PartialWaterToWater.mo
@@ -104,24 +104,24 @@ equation
             -100},{100,100}})),                                  Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-140,-100},{100,
             100}})),                                 preferredView="info",Documentation(info="<HTML>
- <p>
- Base class for the calibration of water to water heat pump models.
- </p>
- <p>
- Source and load temperatures and flow rates are read from an external time table.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- October 31, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Base class for the calibration of water to water heat pump models.
+</p>
+<p>
+Source and load temperatures and flow rates are read from an external time table.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+October 31, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialWaterToWater;
diff --git a/AixLib/Fluid/HeatPumps/Calibration/ScrollWaterToWater.mo b/AixLib/Fluid/HeatPumps/Calibration/ScrollWaterToWater.mo
index e9dfc672f4..38b397035c 100644
--- a/AixLib/Fluid/HeatPumps/Calibration/ScrollWaterToWater.mo
+++ b/AixLib/Fluid/HeatPumps/Calibration/ScrollWaterToWater.mo
@@ -53,38 +53,38 @@ model ScrollWaterToWater
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=142),
 Documentation(info="<HTML>
- <p>
- Calibration model for the calibration of models for water to water heat pump
- with scroll compressor.
- </p>
- <p>
- Source and load temperatures and flow rates are read from an external time
- table.
- </p>
- <p>
- This model is called from the Python code that computes heat pump model
- parameters from the performance data.
- Heat pump model parameters are obtained through an optimization procedure that
- minimizes the difference between the modeled and tabulated (from the
- manufacturers) capacity and power input of the heat pump.
- </p>
- <p>
- The optimization is done using a Python implementation of the heat pump model,
- found in AixLib/Resources/src/fluid/heatpumps/calibration/.
- Heat pump model parameters are verified using this modelica model after their
- evaluation by the Python code.
- </p>
- <p>
- Documentation for the Python code is in the directory
- <code>AixLib/Resources/src/fluid/heatpumps/calibration/doc/build/html</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 31, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibration model for the calibration of models for water to water heat pump
+with scroll compressor.
+</p>
+<p>
+Source and load temperatures and flow rates are read from an external time
+table.
+</p>
+<p>
+This model is called from the Python code that computes heat pump model
+parameters from the performance data.
+Heat pump model parameters are obtained through an optimization procedure that
+minimizes the difference between the modeled and tabulated (from the
+manufacturers) capacity and power input of the heat pump.
+</p>
+<p>
+The optimization is done using a Python implementation of the heat pump model,
+found in AixLib/Resources/src/fluid/heatpumps/calibration/.
+Heat pump model parameters are verified using this modelica model after their
+evaluation by the Python code.
+</p>
+<p>
+Documentation for the Python code is in the directory
+<code>AixLib/Resources/src/fluid/heatpumps/calibration/doc/build/html</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 31, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollWaterToWater;
diff --git a/AixLib/Fluid/HeatPumps/Carnot_TCon.mo b/AixLib/Fluid/HeatPumps/Carnot_TCon.mo
index bb4f501d79..576bebd6dd 100644
--- a/AixLib/Fluid/HeatPumps/Carnot_TCon.mo
+++ b/AixLib/Fluid/HeatPumps/Carnot_TCon.mo
@@ -74,108 +74,126 @@ equation
                                                     color={0,0,255})}),
 defaultComponentName="heaPum",
 Documentation(info="<html>
- <p>
- This is a model of a heat pump whose coefficient of performance COP changes
- with temperatures in the same way as the Carnot efficiency changes.
- The control input is the setpoint of the condenser leaving temperature, which
- is met exactly at steady state if the heat pump has sufficient capacity.
- </p>
- <p>
- The model allows to either specify the Carnot effectivness
- <i>&eta;<sub>Carnot,0</sub></i>, or
- a <i>COP<sub>0</sub></i>
- at the nominal conditions, together with
- the evaporator temperature <i>T<sub>eva,0</sub></i> and
- the condenser temperature <i>T<sub>con,0</sub></i>, in which
- case the model computes the Carnot effectivness as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &eta;<sub>Carnot,0</sub> =
-   COP<sub>0</sub>
- &frasl;  (T<sub>con,0</sub> &frasl; (T<sub>con,0</sub>-T<sub>eva,0</sub>)).
- </p>
- <p>
- The heat pump COP is computed as the product
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
- </p>
- <p>
- where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
- <i>&eta;<sub>PL</sub></i> is a polynomial in heating part load ratio <i>y<sub>PL</sub></i>
- that can be used to take into account a change in <i>COP</i> at part load
- conditions.
- This polynomial has the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y<sub>PL</sub> + a<sub>3</sub> y<sub>PL</sub><sup>2</sup> + ...
- </p>
- <p>
- where the coefficients <i>a<sub>i</sub></i>
- are declared by the parameter <code>a</code>.
- </p>
- <p>
- On the <code>Dynamics</code> tag, the model can be parametrized to compute a transient
- or steady-state response.
- The transient response of the model is computed using a first
- order differential equation for the evaporator and condenser fluid volumes.
- The heat pump outlet temperatures are equal to the temperatures of these lumped volumes.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- When using this component, make sure that the condenser has sufficient mass flow rate.
- Based on the evaporator mass flow rate, temperature difference and the efficiencies,
- the model computes how much heat will be removed by to the evaporator.
- If the mass flow rate is too small, very low outlet temperatures can result, possibly below freezing.
- </p>
- <p>
- The condenser heat flow rate <code>QCon_flow_nominal</code> is used to assign
- the default value for the mass flow rates, which are used for the pressure drop
- calculations.
- It is also used to compute the part load efficiency.
- Hence, make sure that <code>QCon_flow_nominal</code> is set to a reasonable value.
- </p>
- <p>
- The maximum heating capacity is set by the parameter <code>QCon_flow_max</code>,
- which is by default set to infinity.
- </p>
- <p>
- The coefficient of performance depends on the
- evaporator and condenser leaving temperature
- since otherwise the second law of thermodynamics may be violated.
- </p>
- <h4>Notes</h4>
- <p>
- For a similar model that can be used as a chiller, see
- <a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_TEva\">
- AixLib.Fluid.Chillers.Examples.Carnot_TEva</a>.
- </p>
- </html>",
+<p>
+This is a model of a heat pump whose coefficient of performance COP changes
+with temperatures in the same way as the Carnot efficiency changes.
+The control input is the setpoint of the condenser leaving temperature, which
+is met exactly at steady state if the heat pump has sufficient capacity.
+</p>
+<p>
+Set <code>use_eta_Carnot_nominal=true</code> to specify directly
+the Carnot effectiveness <i>&eta;<sub>Carnot,0</sub></i>,
+in which case the value of the parameter <code>COP_nominal</code>
+will not affect the simulation.
+If <code>use_eta_Carnot_nominal=false</code>, the model will use
+the value of the parameter <code>COP_nominal</code>
+together with the specified nominal temperatures
+to compute the Carnot effectiveness as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&eta;<sub>Carnot,0</sub> =
+  COP<sub>0</sub>
+&frasl;  (T<sub>con,0</sub> &frasl; (T<sub>con,0</sub> + T<sub>app,con,0</sub> - (T<sub>eva,0</sub>-T<sub>app,eva,0</sub>))),
+</p>
+<p>
+where
+<i>T<sub>eva,0</sub></i> is the evaporator temperature,
+<i>T<sub>con,0</sub></i> is the condenser temperature,
+<i>T<sub>app,eva,0</sub></i> is the evaporator approach temperature and
+<i>T<sub>app,con,0</sub></i> is the condenser approach temperature.
+</p>
+<p>
+The COP is computed as the product
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
+</p>
+<p>
+where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
+<i>&eta;<sub>PL</sub></i> is the part load efficiency, expressed using
+a polynomial.
+This polynomial has the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y + a<sub>3</sub> y<sup>2</sup> + ...,
+</p>
+<p>
+where <i>y &isin; [0, 1]</i> is
+the part load for heating and the coefficients <i>a<sub>i</sub></i>
+are declared by the parameter <code>a</code>.
+</p>
+<p>
+On the <code>Dynamics</code> tag, the model can be parametrized to compute a transient
+or steady-state response.
+The transient response of the model is computed using a first
+order differential equation for the evaporator and condenser fluid volumes.
+The heat pump outlet temperatures are equal to the temperatures of these lumped volumes.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+When using this component, make sure that the condenser has sufficient mass flow rate.
+Based on the evaporator mass flow rate, temperature difference and the efficiencies,
+the model computes how much heat will be removed by to the evaporator.
+If the mass flow rate is too small, very low outlet temperatures can result, possibly below freezing.
+</p>
+<p>
+The condenser heat flow rate <code>QCon_flow_nominal</code> is used to assign
+the default value for the mass flow rates, which are used for the pressure drop
+calculations.
+It is also used to compute the part load efficiency.
+Hence, make sure that <code>QCon_flow_nominal</code> is set to a reasonable value.
+</p>
+<p>
+The maximum heating capacity is set by the parameter <code>QCon_flow_max</code>,
+which is by default set to infinity.
+</p>
+<p>
+The coefficient of performance depends on the
+evaporator and condenser leaving temperature
+since otherwise the second law of thermodynamics may be violated.
+</p>
+<h4>Notes</h4>
+<p>
+For a similar model that can be used as a chiller, see
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_TEva\">
+AixLib.Fluid.Chillers.Examples.Carnot_TEva</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 3, 2017, by Michael Wetter:<br/>
- Removed parameters
- <code>effInpEva</code> and <code>effInpCon</code>
- and updated documentation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- issue 497</a>.
- </li>
- <li>
- August 8, 2016, by Michael Wetter:<br/>
- Changed default temperature to compute COP to be the leaving temperature as
- use of the entering temperature can violate the 2nd law if the temperature
- lift is small.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- Annex 60, issue 497</a>.
- </li>
- <li>
- November 25, 2015 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 3, 2023, by Michael Wetter:<br/>
+Changed in base class the parameter binding
+<code>etaCarnot_nominal(unit=\"1\") = COP_nominal/(TUseAct_nominal/(TCon_nominal+TAppCon_nominal - (TEva_nominal-TAppEva_nominal)))</code>
+to
+<code>etaCarnot_nominal(unit=\"1\") = 0.3</code> to avoid a circular assignment.<br/>
+Improved documentation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3226\">Buildings, #3226</a>.
+</li>
+<li>
+January 3, 2017, by Michael Wetter:<br/>
+Removed parameters
+<code>effInpEva</code> and <code>effInpCon</code>
+and updated documentation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+issue 497</a>.
+</li>
+<li>
+August 8, 2016, by Michael Wetter:<br/>
+Changed default temperature to compute COP to be the leaving temperature as
+use of the entering temperature can violate the 2nd law if the temperature
+lift is small.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+Annex 60, issue 497</a>.
+</li>
+<li>
+November 25, 2015 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TCon;
diff --git a/AixLib/Fluid/HeatPumps/Carnot_y.mo b/AixLib/Fluid/HeatPumps/Carnot_y.mo
index ce6b4561ba..6b261be2af 100644
--- a/AixLib/Fluid/HeatPumps/Carnot_y.mo
+++ b/AixLib/Fluid/HeatPumps/Carnot_y.mo
@@ -9,165 +9,184 @@ initial equation
   annotation (
 defaultComponentName="heaPum",
 Documentation(info="<html>
- <p>
- This is model of a heat pump whose coefficient of performance COP changes
- with temperatures in the same way as the Carnot efficiency changes.
- The input signal <i>y</i> is the control signal for the compressor.
- </p>
- <p>
- The model allows to either specify the Carnot effectivness
- <i>&eta;<sub>Carnot,0</sub></i>, or
- a <i>COP<sub>0</sub></i>
- at the nominal conditions, together with
- the evaporator temperature <i>T<sub>eva,0</sub></i> and
- the condenser temperature <i>T<sub>con,0</sub></i>, in which
- case the model computes the Carnot effectivness as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &eta;<sub>Carnot,0</sub> =
-   COP<sub>0</sub>
- &frasl;  (T<sub>con,0</sub> &frasl; (T<sub>con,0</sub>-T<sub>eva,0</sub>)).
- </p>
- <p>
- The heat pump COP is computed as the product
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
- </p>
- <p>
- where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
- <i>&eta;<sub>PL</sub></i> is a polynomial in the heating part load ratio <i>y<sub>PL</sub></i>
- that can be used to take into account a change in <i>COP</i> at part load
- conditions.
- This polynomial has the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y<sub>PL</sub> + a<sub>3</sub> y<sub>PL</sub><sup>2</sup> + ...
- </p>
- <p>
- where the coefficients <i>a<sub>i</sub></i> are declared by the parameter <code>a</code>.
- </p>
- <p>
- On the <code>Dynamics</code> tag, the model can be parametrized to compute a transient
- or steady-state response.
- The transient response of the model is computed using a first
- order differential equation for the evaporator and condenser fluid volumes.
- The heat pump outlet temperatures are equal to the temperatures of these lumped volumes.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- When using this component, make sure that the evaporator and the condenser have sufficient mass flow rate.
- Based on the mass flow rates, the compressor power, temperature difference and the efficiencies,
- the model computes how much heat will be added to the condenser and removed at the evaporator.
- If the mass flow rates are too small, very high temperature differences can result.
- </p>
- <p>
- The condenser heat flow rate <code>QCon_flow_nominal</code> is used to assign
- the default value for the mass flow rates, which are used for the pressure drop
- calculations.
- It is also used to compute the part load efficiency.
- Hence, make sure that <code>QCon_flow_nominal</code> is set to a reasonable value.
- </p>
- <p>
- The maximum heating capacity is set by the parameter <code>QCon_flow_max</code>,
- which is by default set to infinity.
- </p>
- <p>
- The coefficient of performance depends on the
- evaporator and condenser leaving temperature
- since otherwise the second law of thermodynamics may be violated.
- </p>
- <h4>Notes</h4>
- <p>
- For a similar model that can be used as a chiller, see
- <a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">AixLib.Fluid.Chillers.Carnot_y</a>.
- </p>
- </html>",
+<p>
+This is model of a heat pump whose coefficient of performance COP changes
+with temperatures in the same way as the Carnot efficiency changes.
+The input signal <i>y</i> is the control signal for the compressor.
+</p>
+<p>
+Set <code>use_eta_Carnot_nominal=true</code> to specify directly
+the Carnot effectiveness <i>&eta;<sub>Carnot,0</sub></i>,
+in which case the value of the parameter <code>COP_nominal</code>
+will not affect the simulation.
+If <code>use_eta_Carnot_nominal=false</code>, the model will use
+the value of the parameter <code>COP_nominal</code>
+together with the specified nominal temperatures
+to compute the Carnot effectiveness as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&eta;<sub>Carnot,0</sub> =
+  COP<sub>0</sub>
+&frasl;  (T<sub>con,0</sub> &frasl; (T<sub>con,0</sub> + T<sub>app,con,0</sub> - (T<sub>eva,0</sub>-T<sub>app,eva,0</sub>))),
+</p>
+<p>
+where
+<i>T<sub>eva,0</sub></i> is the evaporator temperature,
+<i>T<sub>con,0</sub></i> is the condenser temperature,
+<i>T<sub>app,eva,0</sub></i> is the evaporator approach temperature and
+<i>T<sub>app,con,0</sub></i> is the condenser approach temperature.
+</p>
+<p>
+The COP is computed as the product
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  COP = &eta;<sub>Carnot,0</sub> COP<sub>Carnot</sub> &eta;<sub>PL</sub>,
+</p>
+<p>
+where <i>COP<sub>Carnot</sub></i> is the Carnot efficiency and
+<i>&eta;<sub>PL</sub></i> is the part load efficiency, expressed using
+a polynomial.
+This polynomial has the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &eta;<sub>PL</sub> = a<sub>1</sub> + a<sub>2</sub> y + a<sub>3</sub> y<sup>2</sup> + ...,
+</p>
+<p>
+where <i>y &isin; [0, 1]</i> is
+the part load for heating and the coefficients <i>a<sub>i</sub></i>
+are declared by the parameter <code>a</code>.
+</p>
+<p>
+On the <code>Dynamics</code> tag, the model can be parametrized to compute a transient
+or steady-state response.
+The transient response of the model is computed using a first
+order differential equation for the evaporator and condenser fluid volumes.
+The heat pump outlet temperatures are equal to the temperatures of these lumped volumes.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+When using this component, make sure that the evaporator and the condenser have sufficient mass flow rate.
+Based on the mass flow rates, the compressor power, temperature difference and the efficiencies,
+the model computes how much heat will be added to the condenser and removed at the evaporator.
+If the mass flow rates are too small, very high temperature differences can result.
+</p>
+<p>
+The condenser heat flow rate <code>QCon_flow_nominal</code> is used to assign
+the default value for the mass flow rates, which are used for the pressure drop
+calculations.
+It is also used to compute the part load efficiency.
+Hence, make sure that <code>QCon_flow_nominal</code> is set to a reasonable value.
+</p>
+<p>
+The maximum heating capacity is set by the parameter <code>QCon_flow_max</code>,
+which is by default set to infinity.
+</p>
+<p>
+The coefficient of performance depends on the
+evaporator and condenser leaving temperature
+since otherwise the second law of thermodynamics may be violated.
+</p>
+<h4>Notes</h4>
+<p>
+For a similar model that can be used as a chiller, see
+<a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">AixLib.Fluid.Chillers.Carnot_y</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 3, 2017, by Michael Wetter:<br/>
- Removed parameters
- <code>effInpEva</code> and <code>effInpCon</code>
- and updated documentation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- issue 497</a>.
- </li>
- <li>
- August 8, 2016, by Michael Wetter:<br/>
- Changed default temperature to compute COP to be the leaving temperature as
- use of the entering temperature can violate the 2nd law if the temperature
- lift is small.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
- Annex 60, issue 497</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Refactored model to use the same base class as
- <a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">AixLib.Fluid.Chillers.Carnot_y</a>.<br/>
- Changed part load efficiency to depend on heating part load ratio rather than on the compressor
- part load ratio.
- </li>
- <li>
- January 20, 2015, by Damien Picard:<br/>
- Add Carnot model to Annex 60 from the Buildings library.<br/>
- Removed the flow direction dependency of
- <code>staA1</code>, <code>staB1</code>, <code>staA2</code> and <code>staB2</code> as the
- efficiency of the Carnot machine should only be computed in the design flow direction.<br/>
- </li>
- <li>
- December 18, 2015, by Michael Wetter:<br/>
- Corrected wrong computation of <code>staB1</code> and <code>staB2</code>
- which mistakenly used the <code>inStream</code> operator
- for the configuration without flow reversal.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/476\">
- issue 476</a>.
- </li>
- <li>
- November 25, 2015 by Michael Wetter:<br/>
- Changed sign convention for <code>dTEva_nominal</code> to be consistent with
- other models.
- The model will still work with the old values for <code>dTEva_nominal</code>,
- but it will write a warning so that users can transition their models.
- <br/>
- Corrected <code>assert</code> statement for the efficiency curve.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/468\">
- issue 468</a>.
- </li>
- <li>
- September 3, 2015 by Michael Wetter:<br/>
- Expanded documentation.
- </li>
- <li>
- May 6, 2015 by Michael Wetter:<br/>
- Added <code>prescribedHeatFlowRate=true</code> for <code>vol2</code>.
- </li>
- <li>
- October 9, 2013 by Michael Wetter:<br/>
- Reimplemented the computation of the port states to avoid using
- the conditionally removed variables <code>sta_a1</code>,
- <code>sta_a2</code>, <code>sta_b1</code> and <code>sta_b2</code>.
- </li>
- <li>
- May 10, 2013 by Michael Wetter:<br/>
- Added electric power <code>P</code> as an output signal.
- </li>
- <li>
- October 11, 2010 by Michael Wetter:<br/>
- Fixed bug in energy balance.
- </li>
- <li>
- March 3, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+February 3, 2023, by Michael Wetter:<br/>
+Changed in base class the parameter binding
+<code>etaCarnot_nominal(unit=\"1\") = COP_nominal/(TUseAct_nominal/(TCon_nominal+TAppCon_nominal - (TEva_nominal-TAppEva_nominal)))</code>
+to
+<code>etaCarnot_nominal(unit=\"1\") = 0.3</code> to avoid a circular assignment.<br/>
+Improved documentation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3226\">Buildings, #3226</a>.
+</li>
+<li>
+January 3, 2017, by Michael Wetter:<br/>
+Removed parameters
+<code>effInpEva</code> and <code>effInpCon</code>
+and updated documentation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+issue 497</a>.
+</li>
+<li>
+August 8, 2016, by Michael Wetter:<br/>
+Changed default temperature to compute COP to be the leaving temperature as
+use of the entering temperature can violate the 2nd law if the temperature
+lift is small.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/497\">
+Annex 60, issue 497</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Refactored model to use the same base class as
+<a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">AixLib.Fluid.Chillers.Carnot_y</a>.<br/>
+Changed part load efficiency to depend on heating part load ratio rather than on the compressor
+part load ratio.
+</li>
+<li>
+January 20, 2015, by Damien Picard:<br/>
+Add Carnot model to Annex 60 from the Buildings library.<br/>
+Removed the flow direction dependency of
+<code>staA1</code>, <code>staB1</code>, <code>staA2</code> and <code>staB2</code> as the
+efficiency of the Carnot machine should only be computed in the design flow direction.<br/>
+</li>
+<li>
+December 18, 2015, by Michael Wetter:<br/>
+Corrected wrong computation of <code>staB1</code> and <code>staB2</code>
+which mistakenly used the <code>inStream</code> operator
+for the configuration without flow reversal.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/476\">
+issue 476</a>.
+</li>
+<li>
+November 25, 2015 by Michael Wetter:<br/>
+Changed sign convention for <code>dTEva_nominal</code> to be consistent with
+other models.
+The model will still work with the old values for <code>dTEva_nominal</code>,
+but it will write a warning so that users can transition their models.
+<br/>
+Corrected <code>assert</code> statement for the efficiency curve.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/468\">
+issue 468</a>.
+</li>
+<li>
+September 3, 2015 by Michael Wetter:<br/>
+Expanded documentation.
+</li>
+<li>
+May 6, 2015 by Michael Wetter:<br/>
+Added <code>prescribedHeatFlowRate=true</code> for <code>vol2</code>.
+</li>
+<li>
+October 9, 2013 by Michael Wetter:<br/>
+Reimplemented the computation of the port states to avoid using
+the conditionally removed variables <code>sta_a1</code>,
+<code>sta_a2</code>, <code>sta_b1</code> and <code>sta_b2</code>.
+</li>
+<li>
+May 10, 2013 by Michael Wetter:<br/>
+Added electric power <code>P</code> as an output signal.
+</li>
+<li>
+October 11, 2010 by Michael Wetter:<br/>
+Fixed bug in energy balance.
+</li>
+<li>
+March 3, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Line(points={{0,68},{0,90},{90,90},{90,90},{100,90}},
-                                                 color={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+                                                 color={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_y;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/PartialCompressor.mo b/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/PartialCompressor.mo
index fb65b926b6..ed6b7d99a0 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/PartialCompressor.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/PartialCompressor.mo
@@ -84,10 +84,10 @@ equation
   // bounds of the property data in the refrigerant package
   assert(port_b.T > ref.T_min and port_b.T < ref.TCri,
     "Condensing temperature must be above the minimum refrigerant temperature
-     and below the critical temperature.");
+    and below the critical temperature.");
   assert(port_a.T > ref.T_min and port_a.T < ref.TCri,
     "Evaporating temperature must be above the minimum refrigerant temperature
-     and below the critical temperature.");
+    and below the critical temperature.");
 
   annotation (
   Icon(coordinateSystem(preserveAspectRatio=false,extent={{-100,-100},
@@ -117,54 +117,54 @@ equation
           textString="%name")}),
     defaultComponentName="com",
       Documentation(info="<html>
- <p>
- This is the base class for the compressor model.
- </p>
- <p>
- The model evaluates the evaporating pressure of the refrigerant <i>p<sub>eva</sub></i>,
- the specific enthalpy of the evaporating saturated refrigerant vapor <i>h<sub>eva</sub></i>,
- the condensing pressure of the refrigerant <i>p<sub>con</sub></i>
- and the specific enthalpy of the condensing saturated liquid refrigerant <i>h<sub>cond</sub></i>
- at the evaporating temperature <i>T<sub>eva</sub></i> = <code>port_a.T</code>
- and condensing temperature <i>T<sub>con</sub></i> = <code>port_b.T</code>.
- </p>
- <p>
- Thermodynamic properties are evaluated from functions contained in the specified refrigerant package.
- </p>
- <h4>Assumptions and limitations</h4>
- <p>
- The model assumes isothermal condensation and evaporation, therefore
- refrigerant mass flow is not accounted for and heat ports are used instead of fluid ports.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 30, 2017, by Filip Jorissen:<br/>
- Removed <code>pressure_error</code> as
- this is replaced by
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection\">
- AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection</a>.
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
- </li>
- <li>
- May 26, 2017, by Michael Wetter and Thierry Nouidui:<br/>
- Reformulated <code>isOn</code> to use the same construct as the hysteresis block,
- and to work around a JModelica limitation.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/774\">#774</a>.
- </li>
- <li>
- April 25, 2017, by Michael Wetter:<br/>
- Reformulated <code>when</code> conditions and moved common assignments
- to this base class.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/739\">#739</a>.
- </li>
- <li>
- November 11, 2016, by Massimo Cimmino:<br/>
- First implementation of this base class.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is the base class for the compressor model.
+</p>
+<p>
+The model evaluates the evaporating pressure of the refrigerant <i>p<sub>eva</sub></i>,
+the specific enthalpy of the evaporating saturated refrigerant vapor <i>h<sub>eva</sub></i>,
+the condensing pressure of the refrigerant <i>p<sub>con</sub></i>
+and the specific enthalpy of the condensing saturated liquid refrigerant <i>h<sub>cond</sub></i>
+at the evaporating temperature <i>T<sub>eva</sub></i> = <code>port_a.T</code>
+and condensing temperature <i>T<sub>con</sub></i> = <code>port_b.T</code>.
+</p>
+<p>
+Thermodynamic properties are evaluated from functions contained in the specified refrigerant package.
+</p>
+<h4>Assumptions and limitations</h4>
+<p>
+The model assumes isothermal condensation and evaporation, therefore
+refrigerant mass flow is not accounted for and heat ports are used instead of fluid ports.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 30, 2017, by Filip Jorissen:<br/>
+Removed <code>pressure_error</code> as
+this is replaced by
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection\">
+AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection</a>.
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
+</li>
+<li>
+May 26, 2017, by Michael Wetter and Thierry Nouidui:<br/>
+Reformulated <code>isOn</code> to use the same construct as the hysteresis block,
+and to work around a JModelica limitation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/774\">#774</a>.
+</li>
+<li>
+April 25, 2017, by Michael Wetter:<br/>
+Reformulated <code>when</code> conditions and moved common assignments
+to this base class.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/739\">#739</a>.
+</li>
+<li>
+November 11, 2016, by Massimo Cimmino:<br/>
+First implementation of this base class.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialCompressor;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/TemperatureProtection.mo b/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/TemperatureProtection.mo
index 196eabf41c..b3eaebf01c 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/TemperatureProtection.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/TemperatureProtection.mo
@@ -136,33 +136,33 @@ equation
   connect(notCon.u, hysHig.y) annotation (Line(points={{61.6,50},{14,50},{14,-30},
           {1,-30}}, color={255,0,255}));
   annotation (    Documentation(revisions="<html>
- <ul>
- <li>
- May 30, 2017, by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+May 30, 2017, by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
+</li>
+</ul>
+</html>",
 info="<html>
- <p>
- Temperature protection block for heat pumps.
- This block overrides the heat pump control
- signal when the condenser temperature is too high,
- the evaporator temperature is too low,
- or the temperature difference between
- the condenser and evaporator is negative.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- Temperature bounds are set using <code>TConMax</code>
- and <code>TEvaMin</code>.
- </p>
- <h4>Options</h4>
- <p>
- Parameter <code>dTHys</code> may be used
- to change the hysteresis interval.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Temperature protection block for heat pumps.
+This block overrides the heat pump control
+signal when the condenser temperature is too high,
+the evaporator temperature is too low,
+or the temperature difference between
+the condenser and evaporator is negative.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+Temperature bounds are set using <code>TConMax</code>
+and <code>TEvaMin</code>.
+</p>
+<h4>Options</h4>
+<p>
+Parameter <code>dTHys</code> may be used
+to change the hysteresis interval.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureProtection;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/Validation/TemperatureProtection.mo b/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/Validation/TemperatureProtection.mo
index 781a4cfe48..aa4245ef42 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/Validation/TemperatureProtection.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/BaseClasses/Validation/TemperatureProtection.mo
@@ -27,19 +27,19 @@ equation
     annotation (Line(points={{-59,10},{-40,10},{-22,10}}, color={0,0,127}));
   annotation (
     Documentation(info="<html>
- <p>
- Model that tests temperature protection functionality.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 31, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that tests temperature protection functionality.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 31, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/Compressors/BaseClasses/Validation/TemperatureProtection.mos"
         "Simulate and plot"),
-    experiment(StopTime=5, Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(StopTime=5, Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureProtection;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/ReciprocatingCompressor.mo b/AixLib/Fluid/HeatPumps/Compressors/ReciprocatingCompressor.mo
index 6dd8fc4d0d..9825593cc2 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/ReciprocatingCompressor.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/ReciprocatingCompressor.mo
@@ -74,57 +74,57 @@ equation
 
   annotation (defaultComponentName="scrCom",
     Documentation(info="<html>
- <p>
- Model for a reciprocating processor, as detailed in Jin (2002). The rate of heat transferred to the evaporator is given by:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q&#775;<sub>Eva</sub> = m&#775;<sub>ref</sub> ( h<sub>Vap</sub>(T<sub>Eva</sub>) - h<sub>Liq</sub>(T<sub>Con</sub>) ).
- </p>
- <p>
- The power consumed by the compressor is given by a linear efficiency relation:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- P = P<sub>Theoretical</sub> / &eta; + P<sub>Loss,constant</sub>.
- </p>
- <p>
- Variable speed is acheived by multiplying the full load piston displacement
- by the normalized compressor speed. The power and heat transfer rates are forced
- to zero if the resulting heat pump state has higher evaporating pressure than
- condensing pressure.
- </p>
- <h4>Assumptions and limitations</h4>
- <p>
- The compression process is assumed isentropic. The thermal energy
- of superheating is ignored in the evaluation of the heat transferred to the refrigerant
- in the evaporator. There is no supercooling.
- </p>
- <h4>References</h4>
- <p>
- H. Jin.
- <i>
- Parameter estimation based models of water source heat pumps.
- </i>
- PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 25, 2019, by Michael Wetter:<br/>
- Added start value to avoid warning in JModelica.
- </li>
- <li>
- May 30, 2017, by Filip Jorissen:<br/>
- Removed <code>pressure_error</code> as
- this is replaced by
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection\">
- AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection</a>.
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
- </li>
- <li>
- November 14, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model for a reciprocating processor, as detailed in Jin (2002). The rate of heat transferred to the evaporator is given by:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q&#775;<sub>Eva</sub> = m&#775;<sub>ref</sub> ( h<sub>Vap</sub>(T<sub>Eva</sub>) - h<sub>Liq</sub>(T<sub>Con</sub>) ).
+</p>
+<p>
+The power consumed by the compressor is given by a linear efficiency relation:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+P = P<sub>Theoretical</sub> / &eta; + P<sub>Loss,constant</sub>.
+</p>
+<p>
+Variable speed is acheived by multiplying the full load piston displacement
+by the normalized compressor speed. The power and heat transfer rates are forced
+to zero if the resulting heat pump state has higher evaporating pressure than
+condensing pressure.
+</p>
+<h4>Assumptions and limitations</h4>
+<p>
+The compression process is assumed isentropic. The thermal energy
+of superheating is ignored in the evaluation of the heat transferred to the refrigerant
+in the evaporator. There is no supercooling.
+</p>
+<h4>References</h4>
+<p>
+H. Jin.
+<i>
+Parameter estimation based models of water source heat pumps.
+</i>
+PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 25, 2019, by Michael Wetter:<br/>
+Added start value to avoid warning in JModelica.
+</li>
+<li>
+May 30, 2017, by Filip Jorissen:<br/>
+Removed <code>pressure_error</code> as
+this is replaced by
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection\">
+AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection</a>.
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
+</li>
+<li>
+November 14, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReciprocatingCompressor;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/ScrollCompressor.mo b/AixLib/Fluid/HeatPumps/Compressors/ScrollCompressor.mo
index ee83a308e5..3ad73c7b86 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/ScrollCompressor.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/ScrollCompressor.mo
@@ -37,7 +37,7 @@ protected
 
   Real v_norm
     "Normalized refrigerant volume flow rate at
-      suction at part load conditions";
+     suction at part load conditions";
 
   Real PRInt(start = 2.0)
     "Built-in pressure ratio";
@@ -97,57 +97,57 @@ equation
 
   annotation (    defaultComponentName="scrCom",
     Documentation(info="<html>
- <p>
- Model for a scroll processor, as detailed in Jin (2002). The rate of heat transferred to the evaporator is given by:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q&#775;<sub>Eva</sub> = m&#775;<sub>ref</sub> ( h<sub>Vap</sub>(T<sub>Eva</sub>) - h<sub>Liq</sub>(T<sub>Con</sub>) ).
- </p>
- <p>
- The power consumed by the compressor is given by a linear efficiency relation:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- P = P<sub>Theoretical</sub> / &eta; + P<sub>Loss,constant</sub>.
- </p>
- <p>
- Variable speed is achieved by multiplying the full load suction volume flow rate
- by the normalized compressor speed. The power and heat transfer rates are forced
- to zero if the resulting heat pump state has higher evaporating pressure than
- condensing pressure.
- </p>
- <h4>Assumptions and limitations</h4>
- <p>
- The compression process is assumed isentropic. The thermal energy
- of superheating is ignored in the evaluation of the heat transferred to the refrigerant
- in the evaporator. There is no supercooling.
- </p>
- <h4>References</h4>
- <p>
- H. Jin.
- <i>
- Parameter estimation based models of water source heat pumps.
- </i>
- PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 25, 2019, by Michael Wetter:<br/>
- Added start value to avoid warning in JModelica.
- </li>
- <li>
- May 30, 2017, by Filip Jorissen:<br/>
- Removed <code>pressure_error</code> as
- this is replaced by
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection\">
- AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection</a>.
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
- </li>
- <li>
- November 11, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model for a scroll processor, as detailed in Jin (2002). The rate of heat transferred to the evaporator is given by:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q&#775;<sub>Eva</sub> = m&#775;<sub>ref</sub> ( h<sub>Vap</sub>(T<sub>Eva</sub>) - h<sub>Liq</sub>(T<sub>Con</sub>) ).
+</p>
+<p>
+The power consumed by the compressor is given by a linear efficiency relation:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+P = P<sub>Theoretical</sub> / &eta; + P<sub>Loss,constant</sub>.
+</p>
+<p>
+Variable speed is achieved by multiplying the full load suction volume flow rate
+by the normalized compressor speed. The power and heat transfer rates are forced
+to zero if the resulting heat pump state has higher evaporating pressure than
+condensing pressure.
+</p>
+<h4>Assumptions and limitations</h4>
+<p>
+The compression process is assumed isentropic. The thermal energy
+of superheating is ignored in the evaluation of the heat transferred to the refrigerant
+in the evaporator. There is no supercooling.
+</p>
+<h4>References</h4>
+<p>
+H. Jin.
+<i>
+Parameter estimation based models of water source heat pumps.
+</i>
+PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 25, 2019, by Michael Wetter:<br/>
+Added start value to avoid warning in JModelica.
+</li>
+<li>
+May 30, 2017, by Filip Jorissen:<br/>
+Removed <code>pressure_error</code> as
+this is replaced by
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection\">
+AixLib.Fluid.HeatPumps.Compressors.BaseClasses.TemperatureProtection</a>.
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
+</li>
+<li>
+November 11, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollCompressor;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/Validation/ReciprocatingCompressor.mo b/AixLib/Fluid/HeatPumps/Compressors/Validation/ReciprocatingCompressor.mo
index e1d06756b7..bc3bf89163 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/Validation/ReciprocatingCompressor.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/Validation/ReciprocatingCompressor.mo
@@ -40,19 +40,19 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=100),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the ReciprocatingCompressor model.
- </p>
- <p>
- The compressor power, condenser heat transfer rate and evaporator heat transfer rate are calculated for given refrigerant temperatures.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 17, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the ReciprocatingCompressor model.
+</p>
+<p>
+The compressor power, condenser heat transfer rate and evaporator heat transfer rate are calculated for given refrigerant temperatures.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 17, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReciprocatingCompressor;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/Validation/ReciprocatingCompressor_ZeroInput.mo b/AixLib/Fluid/HeatPumps/Compressors/Validation/ReciprocatingCompressor_ZeroInput.mo
index c533e7cec3..0203ff5f6e 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/Validation/ReciprocatingCompressor_ZeroInput.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/Validation/ReciprocatingCompressor_ZeroInput.mo
@@ -40,20 +40,20 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=100),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the ReciprocatingCompressor model.
- </p>
- <p>
- The compressor power, condenser heat transfer rate and evaporator heat transfer
- rate are calculated for zero control input to compressor.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 5, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the ReciprocatingCompressor model.
+</p>
+<p>
+The compressor power, condenser heat transfer rate and evaporator heat transfer
+rate are calculated for zero control input to compressor.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 5, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReciprocatingCompressor_ZeroInput;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/Validation/ScrollCompressor.mo b/AixLib/Fluid/HeatPumps/Compressors/Validation/ScrollCompressor.mo
index eb862e5fb2..b311d5f34b 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/Validation/ScrollCompressor.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/Validation/ScrollCompressor.mo
@@ -40,19 +40,19 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=100),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the ScrollCompressor model.
- </p>
- <p>
- The compressor power, condenser heat transfer rate and evaporator heat transfer rate are calculated for given refrigerant temperatures.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 17, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the ScrollCompressor model.
+</p>
+<p>
+The compressor power, condenser heat transfer rate and evaporator heat transfer rate are calculated for given refrigerant temperatures.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 17, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollCompressor;
diff --git a/AixLib/Fluid/HeatPumps/Compressors/Validation/ScrollCompressor_ZeroInput.mo b/AixLib/Fluid/HeatPumps/Compressors/Validation/ScrollCompressor_ZeroInput.mo
index 0161742cce..451fdbb049 100644
--- a/AixLib/Fluid/HeatPumps/Compressors/Validation/ScrollCompressor_ZeroInput.mo
+++ b/AixLib/Fluid/HeatPumps/Compressors/Validation/ScrollCompressor_ZeroInput.mo
@@ -40,20 +40,20 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=100),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the ScrollCompressor model.
- </p>
- <p>
- The compressor power, condenser heat transfer rate and evaporator heat transfer
- rate are calculated for zero control input to compressor.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 5, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the ScrollCompressor model.
+</p>
+<p>
+The compressor power, condenser heat transfer rate and evaporator heat transfer
+rate are calculated for zero control input to compressor.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 5, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollCompressor_ZeroInput;
diff --git a/AixLib/Fluid/HeatPumps/Data/BaseClasses/HeatPumps.mo b/AixLib/Fluid/HeatPumps/Data/BaseClasses/HeatPumps.mo
index 1cad0f7642..ccb7990186 100644
--- a/AixLib/Fluid/HeatPumps/Data/BaseClasses/HeatPumps.mo
+++ b/AixLib/Fluid/HeatPumps/Data/BaseClasses/HeatPumps.mo
@@ -26,18 +26,18 @@ partial record HeatPumps
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- This is the base record for heat pump models.
- </p>
- </html>",
+<p>
+This is the base record for heat pump models.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 6, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+December 6, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Text(
           extent={{-95,53},{-12,-2}},
@@ -50,6 +50,6 @@ revisions="<html>
         Text(
           extent={{-95,-49},{-12,-104}},
           textColor={0,0,255},
-          textString="dTSup")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="dTSup")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeatPumps;
diff --git a/AixLib/Fluid/HeatPumps/Data/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/Data/BaseClasses/package.mo
index 49c44113ea..f59a16527f 100644
--- a/AixLib/Fluid/HeatPumps/Data/BaseClasses/package.mo
+++ b/AixLib/Fluid/HeatPumps/Data/BaseClasses/package.mo
@@ -6,7 +6,7 @@ package BaseClasses "Base classes for package Data"
   Documentation(info="<html>
 This package contains the common parameters that are used
 to specify the heat pump models in
-<a href=\"AixLib.Fluid.HeatPumps\">
+<a href=\"modelica://AixLib.Fluid.HeatPumps\">
 AixLib.Fluid.HeatPumps</a>.
 </html>", revisions="<html>
 <ul>
diff --git a/AixLib/Fluid/HeatPumps/Data/ReciprocatingWaterToWater/Generic.mo b/AixLib/Fluid/HeatPumps/Data/ReciprocatingWaterToWater/Generic.mo
index c6ba0c8983..ae16665742 100644
--- a/AixLib/Fluid/HeatPumps/Data/ReciprocatingWaterToWater/Generic.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ReciprocatingWaterToWater/Generic.mo
@@ -18,17 +18,17 @@ record Generic "Record for reciprocating water to water heat pump"
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- This is the base record for reciprocating water to water heat pump models.
- </p>
- </html>",
+<p>
+This is the base record for reciprocating water to water heat pump models.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 6, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 6, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Generic;
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Generic.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Generic.mo
index f58d8da1c1..1c9fe29c10 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Generic.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Generic.mo
@@ -20,17 +20,17 @@ record Generic "Record for scroll water to water heat pump"
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- This is the base record for scroll water to water heat pump models.
- </p>
- </html>",
+<p>
+This is the base record for scroll water to water heat pump models.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 6, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 6, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Generic;
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW122_38kW_4_29COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW122_38kW_4_29COP_R410A.mo
index 8fe564ee8a..c7b20777c9 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW122_38kW_4_29COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW122_38kW_4_29COP_R410A.mo
@@ -15,15 +15,15 @@ record Carrier_50PSW122_38kW_4_29COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Carrier 50PSW122.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Carrier 50PSW122.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW180_52kW_4_50COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW180_52kW_4_50COP_R410A.mo
index ab8387dc6b..c3cbad23ec 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW180_52kW_4_50COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW180_52kW_4_50COP_R410A.mo
@@ -15,15 +15,15 @@ record Carrier_50PSW180_52kW_4_50COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Carrier 50PSW180.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Carrier 50PSW180.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW210_70kW_4_40COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW210_70kW_4_40COP_R410A.mo
index d032af6abb..fed5af21fb 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW210_70kW_4_40COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW210_70kW_4_40COP_R410A.mo
@@ -15,15 +15,15 @@ record Carrier_50PSW210_70kW_4_40COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Carrier 50PSW210.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Carrier 50PSW210.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW240_93kW_4_40COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW240_93kW_4_40COP_R410A.mo
index 0da9959fb7..4a6e15ed17 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW240_93kW_4_40COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW240_93kW_4_40COP_R410A.mo
@@ -15,15 +15,15 @@ record Carrier_50PSW240_93kW_4_40COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Carrier 50PSW240.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Carrier 50PSW240.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW360_105kW_4_50COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW360_105kW_4_50COP_R410A.mo
index 612d068651..796428ad71 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW360_105kW_4_50COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW360_105kW_4_50COP_R410A.mo
@@ -15,15 +15,15 @@ record Carrier_50PSW360_105kW_4_50COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Carrier 50PSW360.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Carrier 50PSW360.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW420_140kW_4_40COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW420_140kW_4_40COP_R410A.mo
index 482b54d467..e4911dce72 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW420_140kW_4_40COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Carrier_50PSW420_140kW_4_40COP_R410A.mo
@@ -15,15 +15,15 @@ record Carrier_50PSW420_140kW_4_40COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Carrier 50PSW420.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Carrier 50PSW420.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW036_12kW_4_90COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW036_12kW_4_90COP_R410A.mo
index 007db3c2f8..95563bdf94 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW036_12kW_4_90COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW036_12kW_4_90COP_R410A.mo
@@ -15,15 +15,15 @@ record ClimateMaster_TMW036_12kW_4_90COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for ClimateMaster TMW036.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for ClimateMaster TMW036.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW060_21kW_4_60COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW060_21kW_4_60COP_R410A.mo
index ae7fb00c4f..233c40d8ce 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW060_21kW_4_60COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW060_21kW_4_60COP_R410A.mo
@@ -15,15 +15,15 @@ record ClimateMaster_TMW060_21kW_4_60COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for ClimateMaster TMW060.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for ClimateMaster TMW060.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW120_42kW_4_50COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW120_42kW_4_50COP_R410A.mo
index 66df55b680..b7e7b2396a 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW120_42kW_4_50COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW120_42kW_4_50COP_R410A.mo
@@ -15,15 +15,15 @@ record ClimateMaster_TMW120_42kW_4_50COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for ClimateMaster TMW120.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for ClimateMaster TMW120.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW170_48kW_4_30COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW170_48kW_4_30COP_R410A.mo
index 7bf709e16e..35e427c8a3 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW170_48kW_4_30COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW170_48kW_4_30COP_R410A.mo
@@ -15,15 +15,15 @@ record ClimateMaster_TMW170_48kW_4_30COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for ClimateMaster TMW170.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for ClimateMaster TMW170.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW340_98kW_4_40COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW340_98kW_4_40COP_R410A.mo
index a963f1e345..d41e802d0c 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW340_98kW_4_40COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/ClimateMaster_TMW340_98kW_4_40COP_R410A.mo
@@ -15,15 +15,15 @@ record ClimateMaster_TMW340_98kW_4_40COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for ClimateMaster TMW340.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for ClimateMaster TMW340.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA036_13kW_4_50COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA036_13kW_4_50COP_R410A.mo
index 8c0d61ef7a..ff38fb0549 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA036_13kW_4_50COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA036_13kW_4_50COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA036_13kW_4_50COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA036.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA036.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA048_16kW_4_60COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA048_16kW_4_60COP_R410A.mo
index a53ca3808d..03b87852f6 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA048_16kW_4_60COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA048_16kW_4_60COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA048_16kW_4_60COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA048.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA048.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA060_19kW_4_50COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA060_19kW_4_50COP_R410A.mo
index 8a27b05914..8d83f1aa5d 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA060_19kW_4_50COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA060_19kW_4_50COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA060_19kW_4_50COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA060.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA060.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA072_24kW_4_30COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA072_24kW_4_30COP_R410A.mo
index e27dc9ba1b..1bb55eef4e 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA072_24kW_4_30COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA072_24kW_4_30COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA072_24kW_4_30COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA072.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA072.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA120_37kW_4_40COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA120_37kW_4_40COP_R410A.mo
index adca2b1624..b56fb9ea2a 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA120_37kW_4_40COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA120_37kW_4_40COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA120_37kW_4_40COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA120.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA120.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA150_49kW_4_70COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA150_49kW_4_70COP_R410A.mo
index d16a8e15d8..89b94d30c7 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA150_49kW_4_70COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA150_49kW_4_70COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA150_49kW_4_70COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA150.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA150.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA180_63kW_4_50COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA180_63kW_4_50COP_R410A.mo
index 8e36c3888e..486967acfc 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA180_63kW_4_50COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA180_63kW_4_50COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA180_63kW_4_50COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA180.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA180.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA240_79kW_4_40COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA240_79kW_4_40COP_R410A.mo
index 5b4e745c35..58339c2b9e 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA240_79kW_4_40COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA240_79kW_4_40COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA240_79kW_4_40COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA240.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA240.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA300_93kW_4_60COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA300_93kW_4_60COP_R410A.mo
index 7338bed837..00a69a4c70 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA300_93kW_4_60COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA300_93kW_4_60COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA300_93kW_4_60COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA300.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA300.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA360_116kW_4_60COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA360_116kW_4_60COP_R410A.mo
index 5fda7313a0..d203c26701 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA360_116kW_4_60COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA360_116kW_4_60COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA360_116kW_4_60COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA360.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA360.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA420_137kW_4_50COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA420_137kW_4_50COP_R410A.mo
index 0221ac740e..ccc67d7bfe 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA420_137kW_4_50COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Daikin_WRA420_137kW_4_50COP_R410A.mo
@@ -15,15 +15,15 @@ record Daikin_WRA420_137kW_4_50COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Daikin WRA420.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Daikin WRA420.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW060_21kW_4_30COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW060_21kW_4_30COP_R410A.mo
index 4cdbf1695c..a04d960e16 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW060_21kW_4_30COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW060_21kW_4_30COP_R410A.mo
@@ -15,15 +15,15 @@ record Trane_EXW060_21kW_4_30COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Trane EXW060.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Trane EXW060.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW120_40kW_3_90COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW120_40kW_3_90COP_R410A.mo
index bcedaa5df2..82a8bcebc1 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW120_40kW_3_90COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW120_40kW_3_90COP_R410A.mo
@@ -15,15 +15,15 @@ record Trane_EXW120_40kW_3_90COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Trane EXW120.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Trane EXW120.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW240_76kW_4_10COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW240_76kW_4_10COP_R410A.mo
index 3f346d5141..82b610646e 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW240_76kW_4_10COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Trane_EXW240_76kW_4_10COP_R410A.mo
@@ -15,15 +15,15 @@ record Trane_EXW240_76kW_4_10COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Calibrated parameters for Trane EXW240.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 6, 2017, by Massimo Cimmino:<br/>
- Calibrated parameters.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Calibrated parameters for Trane EXW240.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 6, 2017, by Massimo Cimmino:<br/>
+Calibrated parameters.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A21_28kW_5_94COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A21_28kW_5_94COP_R410A.mo
index c1110d02c1..a5a1ae3114 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A21_28kW_5_94COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A21_28kW_5_94COP_R410A.mo
@@ -15,8 +15,8 @@ record Viessmann_BW301A21_28kW_5_94COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Generated by Filip Jorissen on 2017-05-19.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Generated by Filip Jorissen on 2017-05-19.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A29_37kW_6_0COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A29_37kW_6_0COP_R410A.mo
index 24a9159538..5ea0659073 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A29_37kW_6_0COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A29_37kW_6_0COP_R410A.mo
@@ -15,8 +15,8 @@ record Viessmann_BW301A29_37kW_6_0COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Generated by Filip Jorissen on 2017-05-19.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Generated by Filip Jorissen on 2017-05-19.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A45_58kW_5_50COP_R410A.mo b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A45_58kW_5_50COP_R410A.mo
index 2c00f46080..69f424682c 100644
--- a/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A45_58kW_5_50COP_R410A.mo
+++ b/AixLib/Fluid/HeatPumps/Data/ScrollWaterToWater/Heating/Viessmann_BW301A45_58kW_5_50COP_R410A.mo
@@ -15,8 +15,8 @@ record Viessmann_BW301A45_58kW_5_50COP_R410A =
     defaultComponentName="datHeaPum",
     preferredView="info",
   Documentation(info="<html>
- <p>
- Generated by Filip Jorissen on 2017-05-19.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Generated by Filip Jorissen on 2017-05-19.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/HeatPumps/Data/package.mo b/AixLib/Fluid/HeatPumps/Data/package.mo
index 1aac99391a..76d18c1d44 100644
--- a/AixLib/Fluid/HeatPumps/Data/package.mo
+++ b/AixLib/Fluid/HeatPumps/Data/package.mo
@@ -3,6 +3,8 @@ package Data "Package with model parameters for heat pumps"
   extends Modelica.Icons.MaterialPropertiesPackage;
 
   annotation (preferredView="info", Documentation(info="<html>
+  <p>
   Package with data for heat pump models.
+  </p>
 </html>"));
 end Data;
diff --git a/AixLib/Fluid/HeatPumps/Examples/Carnot_TCon.mo b/AixLib/Fluid/HeatPumps/Examples/Carnot_TCon.mo
index 3c0803290f..95a5ff8db7 100644
--- a/AixLib/Fluid/HeatPumps/Examples/Carnot_TCon.mo
+++ b/AixLib/Fluid/HeatPumps/Examples/Carnot_TCon.mo
@@ -24,7 +24,6 @@ model Carnot_TCon
     allowFlowReversal1=false,
     allowFlowReversal2=false,
     use_eta_Carnot_nominal=true,
-    etaCarnot_nominal=0.3,
     QCon_flow_nominal=QCon_flow_nominal,
     dp1_nominal=6000,
     dp2_nominal=6000) "Heat pump"
@@ -95,26 +94,32 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPum
         "Simulate and plot"),
     Documentation(
 info="<html>
- <p>
- Example that simulates a chiller whose efficiency is scaled based on the
- Carnot cycle.
- The chiller takes as an input the evaporator leaving water temperature.
- The condenser mass flow rate is computed in such a way that it has
- a temperature difference equal to <code>dTEva_nominal</code>.
- </p>
- </html>",
+<p>
+Example that simulates a chiller whose efficiency is scaled based on the
+Carnot cycle.
+The chiller takes as an input the evaporator leaving water temperature.
+The condenser mass flow rate is computed in such a way that it has
+a temperature difference equal to <code>dTEva_nominal</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 2, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 25, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 10, 2023, by Michael Wetter:<br/>
+Removed binding of parameter with same value as the default.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1692\">#1692</a>.
+</li>
+<li>
+May 2, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 25, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TCon;
diff --git a/AixLib/Fluid/HeatPumps/Examples/Carnot_y.mo b/AixLib/Fluid/HeatPumps/Examples/Carnot_y.mo
index 4739f81aa0..6b19646d75 100644
--- a/AixLib/Fluid/HeatPumps/Examples/Carnot_y.mo
+++ b/AixLib/Fluid/HeatPumps/Examples/Carnot_y.mo
@@ -116,37 +116,37 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/Examples/Carnot_y.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 25, 2015 by Michael Wetter:<br/>
- Changed sign of <code>dTEva_nominal</code> to be consistent.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- March 26, 2013 by Michael Wetter:<br/>
- Removed assignment of parameter that had attribute <code>fixed=false</code>.
- </li>
- <li>
- March 3, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Example that simulates a heat pump whose efficiency is scaled based on the
- Carnot cycle.
- The control signal of the heat pump is the compressor speed.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 25, 2015 by Michael Wetter:<br/>
+Changed sign of <code>dTEva_nominal</code> to be consistent.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+March 26, 2013 by Michael Wetter:<br/>
+Removed assignment of parameter that had attribute <code>fixed=false</code>.
+</li>
+<li>
+March 3, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example that simulates a heat pump whose efficiency is scaled based on the
+Carnot cycle.
+The control signal of the heat pump is the compressor speed.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_y;
diff --git a/AixLib/Fluid/HeatPumps/Examples/HeatPump.mo b/AixLib/Fluid/HeatPumps/Examples/HeatPump.mo
index 184793fe7a..6e941d37a5 100644
--- a/AixLib/Fluid/HeatPumps/Examples/HeatPump.mo
+++ b/AixLib/Fluid/HeatPumps/Examples/HeatPump.mo
@@ -103,8 +103,7 @@ model HeatPump "Example for the reversible heat pump model."
     amplitude=3000,
     offset=3000)
     annotation (Placement(transformation(extent={{76,26},{84,34}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm
-                                    pumSou(
+  Movers.SpeedControlled_y                                   pumSou(
     redeclare final AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to8 per,
     final allowFlowReversal=true,
     final addPowerToMedium=false,
@@ -128,7 +127,8 @@ model HeatPump "Example for the reversible heat pump model."
         rotation=270,
         origin={86,-20})));
 
-  Modelica.Blocks.Sources.Constant nIn(k=100) annotation (Placement(
+  Modelica.Blocks.Sources.Constant nIn(k=100/3040)
+                                              annotation (Placement(
         transformation(
         extent={{4,-4},{-4,4}},
         rotation=90,
@@ -174,8 +174,6 @@ equation
 
   connect(sourceSideMassFlowSource.ports[1], heatPump.port_a2) annotation (Line(
         points={{-34,-70},{-24,-70},{-24,-45},{-12.5,-45}}, color={0,127,255}));
-  connect(nIn.y, pumSou.Nrpm)
-    annotation (Line(points={{50,29.6},{50,24}}, color={0,0,127}));
   connect(Room.heatPort, heatFlowRateCon.port)
     annotation (Line(points={{86,-10},{86,0}},        color={191,0,0}));
   connect(sine.y, gain.u) annotation (Line(points={{84.4,30},{92,30},{92,24.8}},
@@ -186,8 +184,8 @@ equation
         points={{-12.5,3},{-70,3}},                   color={0,127,255}));
   connect(heatPump.port_b1, senTAct.port_a) annotation (Line(points={{16.5,-45},
           {30,-45},{30,-64},{44,-64}}, color={0,127,255}));
-  connect(Room.ports[1], pumSou.port_a) annotation (Line(points={{76,-18},{76,4},
-          {60,4},{60,12}}, color={0,127,255}));
+  connect(Room.ports[1], pumSou.port_a) annotation (Line(points={{76,-19},{76,
+          12},{60,12}},    color={0,127,255}));
   connect(pumSou.port_b, heatPump.port_a1) annotation (Line(points={{40,12},{28,
           12},{28,3},{16.5,3}}, color={0,127,255}));
   connect(senTAct.T, hysHeating.u) annotation (Line(points={{54,-53},{54,-54},{
@@ -197,7 +195,7 @@ equation
   connect(senTAct.port_b, sinkSideFixedBoundary.ports[1]) annotation (Line(
         points={{64,-64},{72,-64},{72,-64},{78,-64}}, color={0,127,255}));
   connect(senTAct.port_b, Room.ports[2]) annotation (Line(points={{64,-64},{66,
-          -64},{66,-22},{76,-22}}, color={0,127,255}));
+          -64},{66,-21},{76,-21}}, color={0,127,255}));
   connect(TsuSourceRamp.y, sourceSideMassFlowSource.T_in) annotation (Line(
         points={{-73,-80},{-66,-80},{-66,-66},{-56,-66}}, color={0,0,127},
         smooth=Smooth.None));
@@ -238,6 +236,8 @@ equation
       index=-1,
       extent={{-6,3},{-6,3}},
       horizontalAlignment=TextAlignment.Right));
+  connect(pumSou.y, nIn.y)
+    annotation (Line(points={{50,24},{50,29.6}}, color={0,0,127}));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
             -100},{100,100}})),
     experiment(Tolerance=1e-6, StopTime=3600),
diff --git a/AixLib/Fluid/HeatPumps/Examples/ScrollWaterToWater_OneRoomRadiator.mo b/AixLib/Fluid/HeatPumps/Examples/ScrollWaterToWater_OneRoomRadiator.mo
index f7c4fb8e3b..a73e485850 100644
--- a/AixLib/Fluid/HeatPumps/Examples/ScrollWaterToWater_OneRoomRadiator.mo
+++ b/AixLib/Fluid/HeatPumps/Examples/ScrollWaterToWater_OneRoomRadiator.mo
@@ -287,46 +287,46 @@ equation
   connect(preSou.ports[1], temRet.port_b) annotation (Line(points={{70,-120},{60,
           -120},{60,-30}}, color={0,127,255}));
   annotation (Documentation(info="<html>
- <p>
- Example that simulates one room equipped with a radiator. Hot water is produced
- by a <i>24</i> kW nominal capacity heat pump. The source side water temperature to the
- heat pump is constant at <i>10</i>&deg;C.
- </p>
- <p>
- The heat pump is turned on when the room temperature falls below
- <i>19</i>&deg;C and turned
- off when the room temperature rises above <i>21</i>&deg;C.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 22, 2021, by Michael Wetter:<br/>
- Removed assignments <code>pumHeaPum(y_start=1)</code> and <code>pumHeaPumSou(y_start=1)</code>.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1498\">#1498</a>.
- </li>
- <li>
- April 21, 2021, by Michael Wetter:<br/>
- Corrected error in calculation of design mass flow rate.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2458\">#2458</a>.
- </li>
- <li>
- May 2, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- March 3, 2017, by Michael Wetter:<br/>
- Changed mass flow test to use a hysteresis as a threshold test
- can cause chattering.
- </li>
- <li>
- January 27, 2017, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Example that simulates one room equipped with a radiator. Hot water is produced
+by a <i>24</i> kW nominal capacity heat pump. The source side water temperature to the
+heat pump is constant at <i>10</i>&deg;C.
+</p>
+<p>
+The heat pump is turned on when the room temperature falls below
+<i>19</i>&deg;C and turned
+off when the room temperature rises above <i>21</i>&deg;C.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 22, 2021, by Michael Wetter:<br/>
+Removed assignments <code>pumHeaPum(y_start=1)</code> and <code>pumHeaPumSou(y_start=1)</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1498\">#1498</a>.
+</li>
+<li>
+April 21, 2021, by Michael Wetter:<br/>
+Corrected error in calculation of design mass flow rate.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2458\">#2458</a>.
+</li>
+<li>
+May 2, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+March 3, 2017, by Michael Wetter:<br/>
+Changed mass flow test to use a hysteresis as a threshold test
+can cause chattering.
+</li>
+<li>
+January 27, 2017, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=false,extent={{-240,-220},{100,
             100}})),
     __Dymola_Commands(file=
@@ -334,6 +334,6 @@ equation
         "Simulate and plot"),
     experiment(
       StopTime=172800,
-      Tolerance=1e-08),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-08), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollWaterToWater_OneRoomRadiator;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/AirToWaterTableData2D.mo b/AixLib/Fluid/HeatPumps/ModularReversible/AirToWaterTableData2D.mo
new file mode 100644
index 0000000000..e66aaed01a
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/AirToWaterTableData2D.mo
@@ -0,0 +1,52 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+model AirToWaterTableData2D
+  "Reversible air to water heat pump based on 2D manufacturer data in Europe"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.TableData2D(
+    redeclare replaceable package MediumEva = AixLib.Media.Air,
+    redeclare replaceable package MediumCon = AixLib.Media.Water,
+    redeclare replaceable AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.GenericAirToWater datTabHea
+      constrainedby AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.GenericAirToWater,
+    redeclare replaceable AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic datTabCoo
+      constrainedby AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic);
+
+  annotation (Documentation(info="<html>
+<p>
+  Reversible air-to-water heat pump based on
+  two-dimensional data from manufacturer data, (e.g. based on EN 14511),
+  using the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a> approach.
+</p>
+<p>
+  For more information on the approach, see
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>.
+</p>
+<p>
+  Internal inertias and heat losses are neglected,
+  as these are implicitly obtained in measured
+  data from manufacturers.
+  Also, icing is disabled as the performance degradation
+  is already contained in the data.
+</p>
+<p>
+Please read the documentation of the model for heating at
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D</a>.
+</p>
+<p>
+For cooling, the assumptions are similar, and described at
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D\">
+  AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D</a>
+</p>
+<h4>References</h4>
+<p>
+EN 14511-2018: Air conditioners, liquid chilling packages and heat pumps for space
+heating and cooling and process chillers, with electrically driven compressors
+<a href=\"https://www.beuth.de/de/norm/din-en-14511-1/298537524\">
+https://www.beuth.de/de/norm/din-en-14511-1/298537524</a>
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end AirToWaterTableData2D;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/CalculateEfficiency.mo b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/CalculateEfficiency.mo
new file mode 100644
index 0000000000..451de930a6
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/CalculateEfficiency.mo
@@ -0,0 +1,117 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses;
+model CalculateEfficiency
+  "Calculate the COP or EER of a device"
+  extends Modelica.Blocks.Icons.Block;
+  parameter Modelica.Units.SI.Power PEleMin(min=Modelica.Constants.eps)
+    "If eletrical power consumption falls below this value, COP will be set to zero";
+
+  Modelica.Blocks.Interfaces.RealInput PEle(final unit="W", displayUnit="W")
+    "Electrical power consumed by the system" annotation (Placement(
+        transformation(extent={{-140,-90},{-100,-50}}), iconTransformation(extent={{-140,
+            -90},{-100,-50}})));
+  Modelica.Blocks.Interfaces.RealInput QUse_flow(final unit="W", displayUnit="W")
+    "Useful heat flow" annotation (Placement(transformation(
+          extent={{-140,50},{-100,90}}), iconTransformation(extent={{-140,50},{-100,
+            90}})));
+  Modelica.Blocks.Interfaces.RealOutput COP(min=0, final unit="1")
+    "Output for calculated COP value"
+    annotation (Placement(transformation(extent={{100,50},{120,70}})));
+  Modelica.Blocks.Logical.Hysteresis hys(
+    uLow=PEleMin,
+    uHigh=PEleMin*1.1)
+    "Hysteresis to switch between calculation and no calculation"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  Modelica.Blocks.Interfaces.BooleanInput hea
+    "=true for heating, false for cooling" annotation (Placement(transformation(
+          extent={{-140,-20},{-100,20}}), iconTransformation(extent={{-140,-20},{-100,
+            20}})));
+  Modelica.Blocks.Interfaces.RealOutput EER(min=0, final unit="1")
+    "Output for calculated EER value"
+    annotation (Placement(transformation(extent={{100,-70},{120,-50}})));
+  AixLib.Utilities.Math.InverseXRegularized invXReg(delta=PEleMin)
+    "Inverse of electrical power"
+    annotation (Placement(transformation(extent={{-40,20},{-20,40}})));
+protected
+  Modelica.Blocks.Math.Product  copCom "Computes COP"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  Modelica.Blocks.Logical.Switch swi
+    "Outputs COP or zero depending on electricity use"
+    annotation (Placement(transformation(extent={{-4,-50},{16,-30}})));
+  Modelica.Blocks.Sources.Constant zer(final k=0) "Outputs zero"
+    annotation (Placement(transformation(extent={{-40,-80},{-20,-60}})));
+  Modelica.Blocks.Logical.Switch swiCoo "Switch for cooling and EER calculation"
+    annotation (Placement(transformation(extent={{60,-70},{80,-50}})));
+  Modelica.Blocks.Logical.Switch swiHea "Switch for heating and COP calculation"
+    annotation (Placement(transformation(extent={{60,50},{80,70}})));
+protected
+  Modelica.Blocks.Math.Abs absQEva_flow
+    "Negates possibly negative usefule flow rates"
+    annotation (Placement(transformation(extent={{-40,60},{-20,80}})));
+initial equation
+  assert(PEleMin > 0,
+    "In " + getInstanceName() + ": PEleMin must be greater than zero. Disable efficiency calculation using
+    calEff=false to debug why PEle_nominal is lower than zero.",
+    AssertionLevel.error);
+
+equation
+
+  connect(hys.u, PEle)
+    annotation (Line(points={{-62,-40},{-80,-40},{-80,-70},{-120,-70}},
+                                                    color={0,0,127}));
+  connect(hys.y, swi.u2) annotation (Line(points={{-39,-40},{-6,-40}},
+        color={255,0,255}));
+  connect(copCom.y, swi.u1)
+    annotation (Line(points={{21,50},{34,50},{34,-20},{-20,-20},{-20,-32},{-6,
+          -32}},                                            color={0,0,127}));
+  connect(zer.y, swi.u3) annotation (Line(points={{-19,-70},{-14,-70},{-14,-48},{-6,
+          -48}},color={0,0,127}));
+  connect(swiCoo.y, EER)
+    annotation (Line(points={{81,-60},{110,-60}}, color={0,0,127}));
+  connect(swiHea.y, COP) annotation (Line(points={{81,60},{94,60},{94,60},{110,60}},
+        color={0,0,127}));
+  connect(hea, swiHea.u2) annotation (Line(points={{-120,0},{-90,0},{-90,92},{
+          40,92},{40,60},{58,60}},
+                            color={255,0,255}));
+  connect(swi.y, swiHea.u1) annotation (Line(points={{17,-40},{44,-40},{44,68},{58,
+          68}}, color={0,0,127}));
+  connect(swiHea.u3, zer.y) annotation (Line(points={{58,52},{48,52},{48,-70},{-19,
+          -70}}, color={0,0,127}));
+  connect(hea, swiCoo.u2) annotation (Line(points={{-120,0},{-90,0},{-90,-90},{40,
+          -90},{40,-60},{58,-60}}, color={255,0,255}));
+  connect(swi.y, swiCoo.u3) annotation (Line(points={{17,-40},{44,-40},{44,-68},
+          {58,-68}},
+                 color={0,0,127}));
+  connect(zer.y, swiCoo.u1) annotation (Line(points={{-19,-70},{48,-70},{48,-52},{
+          58,-52}}, color={0,0,127}));
+  connect(QUse_flow, absQEva_flow.u) annotation (Line(points={{-120,70},{-42,70}},
+                             color={0,0,127}));
+  connect(absQEva_flow.y, copCom.u1) annotation (Line(points={{-19,70},{-12,70},
+          {-12,56},{-2,56}},
+                       color={0,0,127}));
+  connect(copCom.u2, invXReg.y) annotation (Line(points={{-2,44},{-14,44},{-14,
+          30},{-19,30}}, color={0,0,127}));
+  connect(invXReg.u, PEle) annotation (Line(points={{-42,30},{-80,30},{-80,-70},
+          {-120,-70}},                     color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+  <li>
+    December 7, 2023, by Michael Wetter:<br/>
+    Reformulated to avoid mixing text and connect statements.
+  </li>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wüllhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">#577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This model is used to calculate the COP or the EER of a device. As
+  the electrical power can get zero, a lower boundary is used to
+  avoid division by zero.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CalculateEfficiency;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/EvaporatorCondenserWithCapacity.mo b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/EvaporatorCondenserWithCapacity.mo
new file mode 100644
index 0000000000..b8f5148133
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/EvaporatorCondenserWithCapacity.mo
@@ -0,0 +1,297 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses;
+model EvaporatorCondenserWithCapacity
+  "Evaporaotr or condenser model with added capacity for heat losses to the ambient"
+  extends AixLib.Fluid.Interfaces.TwoPortHeatMassExchanger(
+    redeclare final AixLib.Fluid.MixingVolumes.MixingVolume vol(final V=
+          m_flow_nominal*tau/rho_default,
+    final prescribedHeatFlowRate=true));
+
+  parameter Boolean isCon "=true for condenser, false for evaporator"
+    annotation (Dialog( descriptionLabel = true),
+      choices(
+        choice=true "Condenser",
+        choice=false "Evaporator",
+        radioButtons=true));
+  parameter Boolean use_cap=true
+    "False if capacity and heat losses are neglected"
+    annotation (Dialog(group="Heat losses"),choices(checkBox=true));
+  parameter Modelica.Units.SI.HeatCapacity C
+    "Capacity of heat exchanger, set to zero to ignore its dry mass"
+    annotation (Dialog(group="Heat losses", enable=use_cap));
+  parameter Modelica.Units.SI.Temperature TCap_start=Medium.T_default
+    "Initial temperature of heat capacity"
+    annotation (Dialog(tab="Initialization", group="Capacity"));
+  Modelica.Units.SI.ThermalConductance GOut
+    "Exterior heat transfer coefficient,
+    set to zero to ignore external heat loss but keep the dry mass"
+      annotation (Dialog(group="Heat losses", enable=use_cap));
+  Modelica.Blocks.Interfaces.RealOutput GInn
+    "Interior heat transfer coefficient"
+      annotation (Dialog(group="Heat losses", enable=use_cap));
+  Modelica.Thermal.HeatTransfer.Components.Convection conIns if use_cap
+    "Convection between the wall and the working fluid" annotation (Placement(transformation(
+        extent={{-12,-12},{12,12}},
+        rotation=90,
+        origin={-10,30})));
+  Modelica.Thermal.HeatTransfer.Components.Convection conOut if use_cap
+    "Convection and conduction between the wall and ambient air" annotation (
+      Placement(transformation(
+        extent={{12,12},{-12,-12}},
+        rotation=270,
+        origin={-10,70})));
+  Modelica.Thermal.HeatTransfer.Components.HeatCapacitor heaCap(
+    final C=C,
+    final T(final fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial),
+        final start=TCap_start),
+    final der_T(final fixed=(energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyStateInitial),
+        start=0)) if use_cap "Heat Capacity" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={30,50})));
+  Modelica.Blocks.Sources.RealExpression heaLosInt(final y=GInn) if use_cap
+    "Nominal heat loss coefficient to the interior" annotation (Placement(
+        transformation(
+        extent={{-20,-10},{20,10}},
+        rotation=0,
+        origin={-60,30})));
+  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a port_out if use_cap
+    "Temperature and heat flow to the ambient"
+    annotation (Placement(transformation(extent={{-5,105},{5,95}}),
+        iconTransformation(extent={{-5,105},{5,95}})));
+  Modelica.Blocks.Sources.RealExpression heaLosExt(final y=GOut) if use_cap
+    "Nominal heat loss coefficient to the exterior" annotation (Placement(
+        transformation(
+        extent={{-20,-10},{20,10}},
+        rotation=0,
+        origin={-60,70})));
+
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow preHea(final alpha=0,
+      final T_ref=293.15) "Heat flow rate of the condenser" annotation (
+      Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=270,
+        origin={0,-70})));
+  Modelica.Blocks.Interfaces.RealInput Q_flow
+    "Heat flow rate from the refrigerant to the medium"
+    annotation (
+      Placement(transformation(extent={{-20,-20},{20,20}},
+      rotation=90,
+        origin={0,-120})));
+
+  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor senT
+    "Temperature sensor for the condenser volume" annotation (Placement(transformation(
+        extent={{10,10},{-10,-10}},
+        rotation=180,
+        origin={50,-50})));
+  Modelica.Blocks.Interfaces.RealOutput T(
+    final unit="K",
+    displayUnit="degC")
+    "Temperature of the condenser volume" annotation (Placement(
+        transformation(extent={{100,-62},{124,-38}}), iconTransformation(extent=
+           {{100,-62},{124,-38}})));
+equation
+  connect(conIns.fluid, heaCap.port) annotation (Line(
+      points={{-10,42},{-10,50},{20,50}},
+      color={191,0,0},
+      pattern=LinePattern.Dash));
+  connect(heaCap.port, conOut.solid) annotation (Line(
+      points={{20,50},{-10,50},{-10,58}},
+      color={191,0,0},
+      pattern=LinePattern.Dash));
+  connect(conIns.Gc, heaLosInt.y) annotation (Line(
+      points={{-22,30},{-38,30}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(conOut.fluid, port_out)
+    annotation (Line(points={{-10,82},{-10,90},{0,90},{0,100}},
+                                                  color={191,0,0},
+      pattern=LinePattern.Dash));
+  connect(conOut.Gc, heaLosExt.y) annotation (Line(
+      points={{-22,70},{-38,70}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(vol.heatPort, conIns.solid) annotation (Line(
+      points={{-9,-10},{-14,-10},{-14,12},{-10,12},{-10,18}},
+      color={191,0,0},
+      pattern=LinePattern.Dash));
+  connect(vol.heatPort, preHea.port) annotation (Line(points={{-9,-10},{-14,-10},
+          {-14,-34},{0,-34},{0,-60},{1.77636e-15,-60}},   color={191,0,0}));
+  connect(preHea.Q_flow, Q_flow)
+  annotation (Line(points={{-1.77636e-15,-80},{-1.77636e-15,-100},{0,-100},{0,
+          -120}},              color={0,0,127}));
+  connect(senT.port, vol.heatPort) annotation (Line(points={{40,-50},{0,-50},{0,
+          -34},{-14,-34},{-14,-10},{-9,-10}}, color={191,0,0}));
+  connect(senT.T, T)
+    annotation (Line(points={{61,-50},{112,-50}}, color={0,0,127}));
+  annotation (Icon(graphics={ Ellipse(
+          extent={{-48,46},{46,-42}},
+          lineColor={0,0,0},
+          fillPattern=FillPattern.Sphere,
+          fillColor={170,213,255}),
+        Rectangle(
+          extent={{-18,100},{18,-100}},
+          lineColor={0,0,0},
+          fillColor={192,192,192},
+          fillPattern=FillPattern.Backward,
+          origin={0,68},
+          rotation=90,
+          visible=use_cap),
+        Text(
+          extent={{-36,52},{36,82}},
+          textColor={0,0,0},
+          pattern=LinePattern.Dash,
+          fillColor={255,215,136},
+          fillPattern=FillPattern.Solid,
+          textString="C",
+          visible=use_cap),
+        Text(
+          extent={{-36,-18},{36,12}},
+          textColor={0,0,0},
+          pattern=LinePattern.Dash,
+          fillColor={255,215,136},
+          fillPattern=FillPattern.Solid,
+          textString="V"),
+        Rectangle(
+          extent={{-107,5},{-44,-4}},
+          lineColor={0,0,255},
+          pattern=LinePattern.None,
+          fillColor={0,0,255},
+          fillPattern=FillPattern.Solid,
+          visible=isCon),
+        Rectangle(
+          extent={{44,-4},{100,5}},
+          lineColor={0,0,255},
+          pattern=LinePattern.None,
+          fillColor={255,0,0},
+          fillPattern=FillPattern.Solid,
+          visible=isCon),
+        Line(
+          points={{0,-96},{0,-50},{0,-46}},
+          color={0,0,0},
+          pattern=LinePattern.None),
+        Line(
+          points={{-12,-76},{-12,-122},{50,-80},{82,-64},{4,-100}},
+          color={0,0,0},
+          pattern=LinePattern.None),
+        Line(
+          points={{-18,-70},{42,-44}},
+          color={0,0,0},
+          pattern=LinePattern.None),
+        Rectangle(
+          extent={{0,-98},{0,-60}},
+          lineColor={238,46,47},
+          pattern=LinePattern.None,
+          fillColor={191,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-102,34},{-96,56},{-140,52},{-100,88},{-84,84},{-106,36}},
+          color={238,46,47},
+          pattern=LinePattern.None),
+        Line(
+          points={{-80,88},{-80,110},{-76,104},{-80,110},{-84,104}},
+          color={28,108,200},
+          visible=use_cap),
+        Line(
+          points={{-80,34},{-80,56},{-76,50},{-80,56},{-84,50}},
+          color={238,46,47},
+          visible=use_cap),
+        Line(
+          points={{-50,34},{-50,56},{-46,50},{-50,56},{-54,50}},
+          color={238,46,47},
+          visible=use_cap),
+        Line(
+          points={{-50,88},{-50,110},{-46,104},{-50,110},{-54,104}},
+          color={28,108,200},
+          visible=use_cap),
+        Line(
+          points={{80,34},{80,56},{84,50},{80,56},{76,50}},
+          color={238,46,47},
+          visible=use_cap),
+        Line(
+          points={{80,88},{80,110},{84,104},{80,110},{76,104}},
+          color={28,108,200},
+          visible=use_cap),
+        Line(
+          points={{50,88},{50,110},{54,104},{50,110},{46,104}},
+          color={28,108,200},
+          visible=use_cap),
+        Line(
+          points={{50,34},{50,56},{54,50},{50,56},{46,50}},
+          color={238,46,47},
+          visible=use_cap),
+        Line(
+          points={{20,34},{20,56},{24,50},{20,56},{16,50}},
+          color={238,46,47},
+          visible=use_cap),
+        Line(
+          points={{20,88},{20,110},{24,104},{20,110},{16,104}},
+          color={28,108,200},
+          visible=use_cap),
+        Line(
+          points={{-20,88},{-20,110},{-16,104},{-20,110},{-24,104}},
+          color={28,108,200},
+          visible=use_cap),
+        Line(
+          points={{-20,34},{-20,56},{-16,50},{-20,56},{-24,50}},
+          color={238,46,47},
+          visible=use_cap),
+        Rectangle(
+          extent={{-100,-4},{-44,5}},
+          lineColor={0,0,255},
+          pattern=LinePattern.None,
+          fillColor={255,0,0},
+          fillPattern=FillPattern.Solid,
+          visible=not isCon),
+        Rectangle(
+          extent={{43,5},{106,-4}},
+          lineColor={0,0,255},
+          pattern=LinePattern.None,
+          fillColor={0,0,255},
+          fillPattern=FillPattern.Solid,
+          visible=not isCon),
+        Text(
+          extent={{-100,-100},{100,-60}},
+          textColor={28,108,200},
+          pattern=LinePattern.Dash,
+          fillColor={255,215,136},
+          fillPattern=FillPattern.Solid,
+          textString="Q_flow")}),Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Model for an evaporator or condenser with the use of a capacity to
+  simulate heat losses.
+</p>
+<p>
+  Used in <a href=
+  \"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a> and <a href=
+  \"modelica://AixLib.Fluid.Chillers.ModularReversible.Modular\">
+  AixLib.Fluid.Chillers.ModularReversible.Modular</a>,
+  the heat flow to or from the volume is calculated in a black-box.
+  Thus the heat is directly added to the medium.
+</p>
+<p>
+  Transient heat losses are modelled by adding a capacity
+  and two convection components to
+  <a href=\"modelica://AixLib.Fluid.Interfaces.TwoPortHeatMassExchanger\">
+  AixLib.Fluid.Interfaces.TwoPortHeatMassExchanger</a>.
+  One of the convection component is between the capacity and the volume
+  (with thermal conductance <code>GInn</code>) and the other between
+  the capacity and the ambient heat port (with <code>GOut</code>).
+</p>
+<h4>Implementation</h4>
+<p>
+  Both <code>GInn</code> and <code>GOut</code> are constants
+  but declared without a <code>parameter</code> keyword so that
+  the calculation can follow a temperature or flow-rate based approach.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end EvaporatorCondenserWithCapacity;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/LargeScaleWaterToWaterDeclarations.mo b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/LargeScaleWaterToWaterDeclarations.mo
new file mode 100644
index 0000000000..38dcbce87f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/LargeScaleWaterToWaterDeclarations.mo
@@ -0,0 +1,68 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses;
+partial model LargeScaleWaterToWaterDeclarations
+  "Model with parameters for large scale water-to-water heat pump"
+
+  //Automatic calculation of mass flow rates and volumes of the evaporator
+  // and condenser using linear regressions from data sheets of
+  // heat pumps and chillers (water to water)
+
+protected
+  parameter Modelica.Units.SI.MassFlowRate autCalMMin_flow=0.3
+    "Realistic mass flow minimum for simulation plausibility";
+  parameter Modelica.Units.SI.Volume autCalVMin=0.003
+    "Realistic volume minimum for simulation plausibility";
+
+  parameter Modelica.Units.SI.MassFlowRate autCalMasEva_flow
+    "Automatically calculated evaporator mass flow rate";
+  parameter Modelica.Units.SI.MassFlowRate autCalMasCon_flow
+    "Automatically calculated condenser mass flow rate";
+  parameter Modelica.Units.SI.Volume autCalVEva
+    "Automatically calculated evaporator volume";
+  parameter Modelica.Units.SI.Volume autCalVCon
+    "Automatically calculated condenser volume";
+
+initial equation
+  //Control and feedback for the auto-calculation of condenser and evaporator data
+  assert(
+    autCalMasEva_flow > autCalMMin_flow and autCalMasEva_flow < 90,
+    "In " + getInstanceName() + ": Given nominal heat output for auto-calculation of
+    evaporator and condenser data is outside the range of data sheets
+    considered. Verify the auto-calculated mass flows.",
+    level=AssertionLevel.warning);
+  assert(
+    autCalVEva > autCalVMin and autCalVEva < 0.43,
+  "In " + getInstanceName() + ": Given nominal heat output for auto-calculation of evaporator
+  and condenser data is outside the range of data sheets considered.
+  Verify the auto-calculated volumes.",
+    level=AssertionLevel.warning);
+
+
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+  This model provides declarations that auto-populate nominal mass flow rates
+  and time constants (i.e. volumes) of the heat exchange based on
+  the nominal electric power consumption of the chiller or heat pump.
+  It is based on more than 20 datasets of water-to-water heat pumps
+  from multiple manufacturers ranging from about <i>25</i> kW
+  to <i>1</i> MW in nominal electric power consumption. The linear regressions with coefficients
+  of determination above <i>91</i>% give a good approximation of these
+  parameters. Nevertheless, estimates for machines outside
+  the given range should be checked for plausibility during simulation.
+</p>
+<p>
+For more information, see
+<a href=\"modelica://AixLib/Resources/Data/Fluid/HeatPumps/BaseClasses/LargeScaleWaterToWaterParameters.xlsx\">
+AixLib/Resources/Data/Fluid/HeatPumps/BaseClasses/LargeScaleWaterToWaterParameters.xlsx</a>.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>Novemeber 11, 2022</i> by Fabian Wuellhorst:<br/>
+    First implemented based on the discussion in this issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end LargeScaleWaterToWaterDeclarations;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/PartialModularRefrigerantCycle.mo b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/PartialModularRefrigerantCycle.mo
new file mode 100644
index 0000000000..a6b7ae2c3f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/PartialModularRefrigerantCycle.mo
@@ -0,0 +1,167 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses;
+partial model PartialModularRefrigerantCycle
+  "Partial refrigerant cycle model"
+
+  parameter Boolean use_rev=true
+    "True if the refrigerant machine is reversible";
+
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantMachineControlBus sigBus
+    "Signal bus with data for refrigerant models" annotation (Placement(
+        transformation(extent={{-18,84},{18,116}}), iconTransformation(extent={{-16,84},
+            {18,114}})));
+  Modelica.Blocks.Interfaces.RealOutput QCon_flow(
+    final unit="W")
+    "Heat flow rate from the refrigerant to the condenser medium"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  Modelica.Blocks.Interfaces.RealOutput QEva_flow(
+    final unit="W")
+    "Heat flow rate from the evaporator medium to the refrigerant"
+    annotation (Placement(transformation(extent={{-100,-10},{-120,10}})));
+  Modelica.Blocks.Logical.Switch swiQEva(
+    u1(final unit="W"),
+    u3(final unit="W"),
+    y(final unit="W"))
+    "Routing block that picks the component acting as evaporator"
+    annotation (Placement(transformation(extent={{-60,-10},{-80,10}})));
+  Modelica.Blocks.Logical.Switch swiQCon(
+    y(final unit="W"),
+    u1(final unit="W"),
+    u3(final unit="W"))
+    "Routing block that picks the component acting as condenser"
+    annotation (Placement(transformation(extent={{60,-10},{80,10}})));
+  Modelica.Blocks.Interfaces.RealOutput PEle(final unit="W")
+    "Routing block that picks the component for electric power consumption"
+    annotation (Placement(
+        transformation(
+        extent={{-10.5,-10.5},{10.5,10.5}},
+        rotation=-90,
+        origin={0.5,-110.5})));
+
+  Modelica.Blocks.Logical.Switch swiPEle(
+    u1(final unit="W"),
+    u3(final unit="W"),
+    y(final unit="W"))
+    "Whether to use cooling or heating power output" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-70})));
+protected
+  Modelica.Blocks.Routing.BooleanPassThrough pasTrhModSet
+    "Pass through to enable assertion for non-reversible device";
+equation
+  assert(
+    use_rev or (use_rev == false and pasTrhModSet.y == true),
+    "In " + getInstanceName() + ": Can't turn to reversible operation mode on
+    irreversible refrigerant machine.",
+    level=AssertionLevel.error);
+
+  connect(swiQEva.y, QEva_flow)
+    annotation (Line(points={{-81,0},{-110,0}}, color={0,0,127}));
+  connect(swiPEle.y, PEle) annotation (Line(points={{-1.9984e-15,-81},{-1.9984e-15,
+          -95.75},{0.5,-95.75},{0.5,-110.5}}, color={0,0,127}));
+  connect(swiQCon.y, QCon_flow)
+    annotation (Line(points={{81,0},{110,0}}, color={0,0,127}));
+
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-24,88},{22,44}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{-16,82},{20,74}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-18,52},{20,58}},
+          color={28,108,200},
+          thickness=0.5),
+        Rectangle(
+          extent={{-98,40},{-60,-28}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{-20,-60},{-20,-70},{-20,-80},{20,-60},{20,-80},{-20,-60}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-122,34},{-66,34},{-82,10},{-66,-22},{-120,-22}},
+          color={28,108,200},
+          thickness=0.5),
+        Rectangle(
+          extent={{60,40},{98,-28}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{120,34},{64,34},{80,10},{64,-22},{118,-22}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-80,40},{-80,68},{-24,68}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{22,66},{80,66},{80,40}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{78,-28},{78,-70}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{78,-70},{62,-70},{20,-70}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-80,-26},{-80,-68},{-20,-68}},
+          color={28,108,200},
+          thickness=0.5),
+        Text(
+          extent={{-151,147},{149,107}},
+          textColor={0,0,255},
+          fillPattern=FillPattern.HorizontalCylinder,
+          fillColor={0,127,255},
+          textString="%name")}),
+                          Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on the discussion in this issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>May 22, 2019</i> by Julian Matthes:<br/>
+    Rebuild due to the introducion of the refrigerant machine
+    partial model (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/715\">#715</a>)
+  </li>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">#577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Partial modular refrigerant cycle models for data and
+  equation based approaches used in the model
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialReversibleRefrigerantMachine\">
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialReversibleRefrigerantMachine</a>.
+</p>
+<p>
+  This partial container only adds outputs and switches
+  both relevant for heat pump and chiller applications.
+</p>
+<p>
+  For more information on the approach, please read the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  UsersGuide</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialModularRefrigerantCycle;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/PartialReversibleRefrigerantMachine.mo b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/PartialReversibleRefrigerantMachine.mo
new file mode 100644
index 0000000000..d738ed6edf
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/PartialReversibleRefrigerantMachine.mo
@@ -0,0 +1,748 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses;
+partial model PartialReversibleRefrigerantMachine
+  "Model for reversible heat pumps and chillers with a refrigerant cycle"
+  extends AixLib.Fluid.Interfaces.PartialFourPortInterface(
+    redeclare final package Medium1 = MediumCon,
+    redeclare final package Medium2 = MediumEva,
+    final m1_flow_nominal=mCon_flow_nominal,
+    final m2_flow_nominal=mEva_flow_nominal,
+    final allowFlowReversal1=allowFlowReversalCon,
+    final allowFlowReversal2=allowFlowReversalEva,
+    final m1_flow_small=1E-4*abs(mCon_flow_nominal),
+    final m2_flow_small=1E-4*abs(mEva_flow_nominal));
+
+  //General
+  replaceable package MediumCon =
+    Modelica.Media.Interfaces.PartialMedium "Medium on condenser side"
+    annotation (choicesAllMatching=true);
+  replaceable package MediumEva =
+    Modelica.Media.Interfaces.PartialMedium "Medium on evaporator side"
+    annotation (choicesAllMatching=true);
+  replaceable PartialModularRefrigerantCycle refCyc constrainedby
+    PartialModularRefrigerantCycle(final use_rev=use_rev)
+    "Model of the refrigerant cycle" annotation (Placement(transformation(
+          extent={{-18,-18},{18,18}}, rotation=90)));
+  parameter Modelica.Units.SI.HeatFlowRate PEle_nominal
+    "Nominal electrical power consumption"
+    annotation (Dialog(group="Nominal condition"));
+
+  replaceable model RefrigerantCycleInertia =
+     AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.NoInertia
+    constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.BaseClasses.PartialInertia
+      "Inertia between the refrigerant cycle outputs and the heat exchangers."
+    annotation (choicesAllMatching=true, Dialog(group="Inertia"));
+  parameter Boolean use_rev=true
+    "=true if the chiller or heat pump is reversible"
+    annotation(choices(checkBox=true));
+  parameter Boolean allowDifferentDeviceIdentifiers=false
+    "if use_rev=true, device data for cooling and heating need to entered. Set allowDifferentDeviceIdentifiers=true to allow different device identifiers devIde"
+    annotation(Dialog(tab="Advanced", enable=use_rev));
+
+  //Condenser
+  parameter Modelica.Units.SI.Time tauCon=30
+    "Condenser heat transfer time constant at nominal flow"
+    annotation (Dialog(tab="Condenser", group="Dynamics"));
+  parameter Modelica.Units.SI.TemperatureDifference dTCon_nominal
+    "Nominal temperature difference in condenser medium, used to calculate mass flow rate"
+    annotation (Dialog(group="Nominal condition - Pressure losses"));
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_nominal
+    "Nominal mass flow rate of the condenser medium"
+    annotation (Dialog(group="Nominal condition - Pressure losses"));
+
+  parameter Modelica.Units.SI.PressureDifference dpCon_nominal(displayUnit="Pa")
+    "Pressure drop at nominal mass flow rate"
+    annotation (Dialog(group="Nominal condition - Pressure losses"));
+  parameter Real deltaMCon=0.1
+    "Fraction of nominal mass flow rate where transition to turbulent occurs"
+    annotation (Dialog(tab="Condenser", group="Flow resistance"));
+  parameter Boolean use_conCap=true
+    "=true if using capacitor model for condenser heat loss estimation"
+    annotation (Dialog(group="Heat Losses", tab="Condenser"),
+                                          choices(checkBox=true));
+  parameter Modelica.Units.SI.HeatCapacity CCon=0
+    "Heat capacity of the condenser"
+    annotation (Dialog(
+      group="Heat Losses",
+      tab="Condenser",
+      enable=use_conCap));
+  parameter Modelica.Units.SI.ThermalConductance GConOut=0
+    "Outer thermal conductance for condenser heat loss calculations"
+    annotation (Dialog(
+      group="Heat Losses",
+      tab="Condenser",
+      enable=use_conCap));
+  parameter Modelica.Units.SI.ThermalConductance GConIns=0
+    "Inner thermal conductance for condenser heat loss calculations"
+    annotation (Dialog(
+      group="Heat Losses",
+      tab="Condenser",
+      enable=use_conCap));
+
+  final parameter Modelica.Units.SI.Density rhoCon=MediumCon.density(staCon_nominal)
+    "Condenser medium density";
+  final parameter Modelica.Units.SI.SpecificHeatCapacity cpCon=
+      MediumCon.specificHeatCapacityCp(staCon_nominal)
+    "Condenser medium specific heat capacity";
+
+  //Evaporator
+  parameter Modelica.Units.SI.Time tauEva=30
+    "Evaporator heat transfer time constant at nominal flow"
+    annotation (Dialog(tab="Evaporator", group="Dynamics"));
+  parameter Modelica.Units.SI.TemperatureDifference dTEva_nominal
+    "Nominal temperature difference in evaporator medium, used to calculate mass flow rate"
+    annotation (Dialog(group="Nominal condition - Pressure losses"));
+  parameter Modelica.Units.SI.MassFlowRate mEva_flow_nominal
+    "Nominal mass flow rate of the evaporator medium"
+    annotation (Dialog(group="Nominal condition - Pressure losses"));
+
+  parameter Modelica.Units.SI.PressureDifference dpEva_nominal(displayUnit="Pa")
+    "Pressure drop at nominal mass flow rate"
+    annotation (Dialog(group="Nominal condition - Pressure losses"));
+  parameter Real deltaMEva=0.1
+    "Fraction of nominal mass flow rate where transition to turbulent occurs"
+    annotation (Dialog(tab="Evaporator", group="Flow resistance"));
+  parameter Boolean use_evaCap=true
+    "=true if using capacitor model for evaporator heat loss estimation"
+    annotation (Dialog(group="Heat Losses", tab="Evaporator"),
+                                          choices(checkBox=true));
+  parameter Modelica.Units.SI.HeatCapacity CEva=0
+    "Heat capacity of the evaporator"
+    annotation ( Dialog(
+      group="Heat Losses",
+      tab="Evaporator",
+      enable=use_evaCap));
+  parameter Modelica.Units.SI.ThermalConductance GEvaOut=0
+    "Outer thermal conductance for evaporator heat loss calculations"
+    annotation ( Dialog(
+      group="Heat Losses",
+      tab="Evaporator",
+      enable=use_evaCap));
+  parameter Modelica.Units.SI.ThermalConductance GEvaIns=0
+    "Inner thermal conductance for evaporator heat loss calculations"
+    annotation ( Dialog(
+      group="Heat Losses",
+      tab="Evaporator",
+      enable=use_evaCap));
+  final parameter Modelica.Units.SI.Density rhoEva=MediumEva.density(staEva_nominal)
+    "Evaporator medium density";
+  final parameter Modelica.Units.SI.SpecificHeatCapacity cpEva=
+      MediumEva.specificHeatCapacityCp(staEva_nominal)
+    "Evaporator medium specific heat capacity";
+
+  // Safety control
+  parameter Boolean use_intSafCtr=true
+    "=true to enable internal safety control"
+    annotation (Dialog(group="Safety control"), choices(checkBox=true));
+  replaceable parameter
+    AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021 safCtrPar
+    constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Generic
+    "Safety control parameters" annotation (Dialog(enable=use_intSafCtr,
+    group="Safety control"),
+      choicesAllMatching=true,
+      Placement(transformation(extent={{42,-18},{58,-2}})));
+
+
+//Assumptions
+  parameter Boolean allowFlowReversalEva=true
+    "= false to simplify equations, assuming, but not enforcing, no flow reversal"
+    annotation (Dialog(group="Evaporator", tab="Assumptions"));
+  parameter Boolean allowFlowReversalCon=true
+    "= false to simplify equations, assuming, but not enforcing, no flow reversal"
+    annotation (Dialog(group="Condenser", tab="Assumptions"));
+
+//Initialization
+  parameter Modelica.Blocks.Types.Init initType=
+    Modelica.Blocks.Types.Init.InitialState
+    "Type of initialization for refrigerant cycle dynamics (InitialState and InitialOutput are identical)"
+    annotation (Dialog(tab="Initialization", group="Parameters"));
+  parameter Modelica.Media.Interfaces.Types.AbsolutePressure pCon_start=
+      MediumCon.p_default "Start value of pressure"
+    annotation (Dialog(tab="Initialization", group="Condenser"));
+  parameter Modelica.Media.Interfaces.Types.Temperature TCon_start=
+    MediumCon.T_default
+    "Start value of temperature"
+    annotation (Dialog(tab="Initialization", group="Condenser"));
+  parameter Modelica.Units.SI.Temperature TConCap_start=MediumCon.T_default
+    "Initial temperature of heat capacity of condenser" annotation (Dialog(
+      tab="Initialization",
+      group="Condenser",
+      enable=use_conCap));
+  parameter Modelica.Media.Interfaces.Types.MassFraction XCon_start[MediumCon.nX]=
+     MediumCon.X_default "Start value of mass fractions m_i/m"
+    annotation (Dialog(tab="Initialization", group="Condenser"));
+  parameter Modelica.Media.Interfaces.Types.AbsolutePressure pEva_start=
+      MediumEva.p_default "Start value of pressure"
+    annotation (Dialog(tab="Initialization", group="Evaporator"));
+  parameter Modelica.Media.Interfaces.Types.Temperature TEva_start=
+    MediumEva.T_default
+    "Start value of temperature"
+    annotation (Dialog(tab="Initialization", group="Evaporator"));
+  parameter Modelica.Units.SI.Temperature TEvaCap_start=MediumEva.T_default
+    "Initial temperature of heat capacity at evaporator" annotation (Dialog(
+      tab="Initialization",
+      group="Evaporator",
+      enable=use_evaCap));
+  parameter Modelica.Media.Interfaces.Types.MassFraction XEva_start[MediumEva.nX]=
+     MediumEva.X_default "Start value of mass fractions m_i/m"
+    annotation (Dialog(tab="Initialization", group="Evaporator"));
+
+//Dynamics
+  parameter Modelica.Fluid.Types.Dynamics energyDynamics=
+    Modelica.Fluid.Types.Dynamics.DynamicFreeInitial
+    "Type of energy balance: dynamic (3 initialization options)
+    or steady state (only affects fluid-models)"
+    annotation (Dialog(tab="Dynamics", group="Equation"));
+//Advanced
+  parameter Boolean from_dp=false
+    "= true, use m_flow = f(dp) else dp = f(m_flow)"
+    annotation (Dialog(tab="Advanced", group="Flow resistance"));
+  parameter Boolean linearized=false
+    "= true, use linear relation between m_flow and dp for any flow rate"
+    annotation (Dialog(tab="Advanced", group="Flow resistance"));
+  parameter Real ySet_small(min=0.002)=0.01
+    "Threshold for relative speed for the device to be considered on"
+    annotation (Dialog(tab="Advanced", group="Diagnostics"));
+  parameter Boolean calEff=true
+    "=false to disable efficiency calculation, may speed up the simulation"
+    annotation(Dialog(tab="Advanced"));
+  parameter Real limWarSca(final unit="1") = 0.05
+    "Allowed difference in scaling '|scaFacHea - scaFacCoo| / scaFacHea', if exceeded, a warning will be issued"
+    annotation(Dialog(tab="Advanced"));
+
+  Modelica.Units.SI.HeatFlowRate Q1_flow = QCon_flow
+    "Heat transferred into the medium 1";
+  Modelica.Units.SI.HeatFlowRate Q2_flow = QEva_flow
+    "Heat transferred into the medium 2";
+
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.EvaporatorCondenserWithCapacity con(
+    redeclare final package Medium = MediumCon,
+    final allowFlowReversal=allowFlowReversalCon,
+    final m_flow_small=1E-4*abs(mCon_flow_nominal),
+    final show_T=show_T,
+    final deltaM=deltaMCon,
+    final tau=tauCon,
+    final T_start=TCon_start,
+    final p_start=pCon_start,
+    final use_cap=use_conCap,
+    final X_start=XCon_start,
+    final from_dp=from_dp,
+    final energyDynamics=energyDynamics,
+    final isCon=true,
+    final C=CCon,
+    final TCap_start=TConCap_start,
+    final GOut=GConOut,
+    final m_flow_nominal=mCon_flow_nominal,
+    final dp_nominal=dpCon_nominal,
+    final GInn=GConIns) "Heat exchanger model for the condenser"
+    annotation (Placement(transformation(extent={{-20,80},{20,120}})));
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.EvaporatorCondenserWithCapacity eva(
+    redeclare final package Medium = MediumEva,
+    final deltaM=deltaMEva,
+    final tau=tauEva,
+    final use_cap=use_evaCap,
+    final allowFlowReversal=allowFlowReversalEva,
+    final m_flow_small=1E-4*abs(mEva_flow_nominal),
+    final show_T=show_T,
+    final T_start=TEva_start,
+    final p_start=pEva_start,
+    final X_start=XEva_start,
+    final from_dp=from_dp,
+    final energyDynamics=energyDynamics,
+    final isCon=false,
+    final C=CEva,
+    final m_flow_nominal=mEva_flow_nominal,
+    final dp_nominal=dpEva_nominal,
+    final TCap_start=TEvaCap_start,
+    final GOut=GEvaOut,
+    final GInn=GEvaIns) "Heat exchanger model for the evaporator"
+    annotation (Placement(transformation(extent={{20,-80},{-20,-120}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature varTOutEva
+    if use_evaCap "Forces heat losses according to ambient temperature"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-50,-130})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature varTOutCon
+    if use_conCap "Forces heat losses according to ambient temperature"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-50,130})));
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Safety safCtr(
+    final mEva_flow_nominal=mEva_flow_nominal,
+    final mCon_flow_nominal=mCon_flow_nominal,
+    safCtrPar=safCtrPar,
+    final ySet_small=ySet_small) if use_intSafCtr "Safety control models"
+    annotation (Placement(transformation(extent={{-112,-20},{-92,0}})));
+  Modelica.Blocks.Interfaces.RealInput ySet if not use_busConOnl
+    "Relative compressor speed between 0 and 1" annotation (Placement(
+        transformation(extent={{-164,8},{-140,32}}), iconTransformation(extent={{-120,10},
+            {-102,28}})));
+
+  Modelica.Blocks.Interfaces.RealInput TEvaAmb(final unit="K", displayUnit="degC")
+    if use_evaCap and not use_busConOnl
+    "Ambient temperature on the evaporator side" annotation (Placement(
+        transformation(
+        extent={{12,-12},{-12,12}},
+        rotation=180,
+        origin={-152,-130}),iconTransformation(extent={{9,-9},{-9,9}},
+          origin={-111,-91},
+        rotation=180)));
+  Modelica.Blocks.Interfaces.RealInput TConAmb(final unit="K", displayUnit="degC")
+    if use_conCap and not use_busConOnl
+    "Ambient temperature on the condenser side" annotation (Placement(
+        transformation(
+        extent={{-12,12},{12,-12}},
+        rotation=0,
+        origin={-152,120}),iconTransformation(
+        extent={{-9,9},{9,-9}},
+        rotation=0,
+        origin={-111,89})));
+
+  AixLib.Fluid.Sensors.MassFlowRate mEva_flow(redeclare final package Medium =
+        MediumEva, final allowFlowReversal=allowFlowReversalEva)
+    "Mass flow sensor at the evaporator" annotation (Placement(transformation(
+        origin={70,-60},
+        extent={{10,-10},{-10,10}},
+        rotation=0)));
+  AixLib.Fluid.Sensors.MassFlowRate mCon_flow(final allowFlowReversal=
+        allowFlowReversalEva, redeclare final package Medium = MediumCon)
+    "Mass flow sensor at the evaporator" annotation (Placement(transformation(
+        origin={-50,100},
+        extent={{-10,10},{10,-10}},
+        rotation=0)));
+
+  Modelica.Blocks.Logical.Hysteresis hys(
+    final uLow=0.001,
+    final uHigh=ySet_small,
+    final pre_y_start=false) "Use default ySet value" annotation (Placement(
+        transformation(extent={{10,10},{-10,-10}}, rotation=180,
+        origin={-110,-90})));
+
+  RefrigerantCycleInertia refCycIneCon "Inertia model for condenser side"
+      annotation(Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,50})));
+  RefrigerantCycleInertia refCycIneEva "Inertia model for evaporator side"
+      annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-50})));
+
+  Modelica.Blocks.Sources.RealExpression senTConIn(
+    final y(
+      final unit="K",
+      displayUnit="degC")=MediumCon.temperature(MediumCon.setState_phX(
+        port_a1.p,
+        inStream(port_a1.h_outflow),
+        inStream(port_a1.Xi_outflow))))
+    "Real expression for condenser inlet temperature" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-98,32})));
+  Modelica.Blocks.Sources.RealExpression senTEvaIn(
+    final y(
+      final unit="K",
+      displayUnit="degC")=MediumEva.temperature(MediumEva.setState_phX(
+        port_a2.p,
+        inStream(port_a2.h_outflow),
+        inStream(port_a2.Xi_outflow))))
+    "Real expression for evaporator inlet temperature" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-98,12})));
+  Modelica.Blocks.Interfaces.RealOutput QCon_flow(final quantity="HeatFlowRate",
+      final unit="W") "Actual heating heat flow rate added to fluid 1"
+    annotation (Placement(transformation(extent={{140,120},{160,140}}),
+        iconTransformation(extent={{100,80},{120,100}})));
+  Modelica.Blocks.Interfaces.RealOutput P(final quantity="Power", final unit="W")
+    "Electric power consumed by compressor"
+    annotation (Placement(transformation(extent={{140,-10},{160,10}}),
+        iconTransformation(extent={{100,-10},{120,10}})));
+  Modelica.Blocks.Interfaces.RealOutput QEva_flow(final quantity="HeatFlowRate",
+      final unit="W") "Actual cooling heat flow rate removed from fluid 2"
+    annotation (Placement(transformation(extent={{140,-140},{160,-120}}),
+        iconTransformation(extent={{100,-100},{120,-80}})));
+  Modelica.Blocks.Interfaces.RealOutput EER(unit="1") if use_EER
+    "Energy efficieny ratio" annotation (Placement(transformation(extent={{140,-40},
+            {160,-20}}), iconTransformation(extent={{100,-40},{120,-20}})));
+  Modelica.Blocks.Interfaces.RealOutput COP(unit="1") if use_COP
+    "Coefficient of performance" annotation (Placement(transformation(extent={{140,
+            20},{160,40}}), iconTransformation(extent={{100,20},{120,40}})));
+
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.CalculateEfficiency
+    eff(PEleMin=PEle_nominal*0.1) if calEff "Calculate efficiencies of device"
+    annotation (Placement(transformation(
+        extent={{10,10},{-10,-10}},
+        rotation=180,
+        origin={110,30})));
+// To avoid using the bus, set the section below to protected
+// <!-- @include_Buildings @include_IDEAS @include_BuildingSystems
+protected
+// -->
+  RefrigerantMachineControlBus sigBus
+    "Bus with model outputs and possibly inputs" annotation (Placement(transformation(
+          extent={{-156,-58},{-126,-24}}),iconTransformation(extent={{-108,-52},
+            {-90,-26}})));
+
+  parameter Boolean use_busConOnl=false
+    "=true to allow input to bus connector,
+    not applicable with internal safety control"
+    annotation(choices(checkBox=true), Dialog(group="Input Connectors", enable=not
+          use_intSafCtr));
+
+protected
+  parameter Boolean use_COP "=true to enable COP output";
+  parameter Boolean use_EER "=true to enable EER output";
+  parameter MediumCon.ThermodynamicState staCon_nominal=MediumCon.setState_pTX(
+      T=MediumCon.T_default, p=MediumCon.p_default, X=MediumCon.X_default)
+      "Nominal state of condenser medium";
+
+  parameter MediumEva.ThermodynamicState staEva_nominal=MediumEva.setState_pTX(
+      T=MediumEva.T_default, p=MediumEva.p_default, X=MediumEva.X_default)
+      "Nominal state of evaporator medium";
+
+equation
+
+  // Non bus connections
+  connect(safCtr.sigBus, sigBus) annotation (Line(
+      points={{-111.917,-16.0833},{-111.917,-16},{-116,-16},{-116,-40},{-140,
+          -40},{-140,-41},{-141,-41}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(safCtr.yOut, sigBus.yMea) annotation (Line(points={{-91.1667,-10},{
+          -84,-10},{-84,-40},{-138,-40},{-138,-42},{-140,-42},{-140,-41},{-141,
+          -41}},                                    color={0,0,127}));
+  connect(ySet, safCtr.ySet) annotation (Line(points={{-152,20},{-120,20},{-120,
+          -10},{-113.333,-10}},
+                       color={0,0,127}));
+  connect(TConAmb, varTOutCon.T) annotation (Line(
+      points={{-152,120},{-110,120},{-110,130},{-62,130}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(varTOutCon.port, con.port_out) annotation (Line(
+      points={{-40,130},{0,130},{0,120}},
+      color={191,0,0},
+      pattern=LinePattern.Dash));
+  connect(TEvaAmb, varTOutEva.T) annotation (Line(
+      points={{-152,-130},{-130,-130},{-130,-150},{-70,-150},{-70,-130},{-62,-130}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(eva.port_out, varTOutEva.port) annotation (Line(
+      points={{0,-120},{0,-130},{-40,-130}},
+      color={191,0,0},
+      pattern=LinePattern.Dash));
+  connect(mEva_flow.port_a, port_a2)
+    annotation (Line(points={{80,-60},{100,-60}}, color={0,127,255}));
+  connect(port_a1,mCon_flow. port_a)
+    annotation (Line(points={{-100,60},{-68,60},{-68,100},{-60,100}},
+                                                  color={0,127,255}));
+  connect(mEva_flow.port_b, eva.port_a) annotation (Line(points={{60,-60},{32,-60},
+          {32,-100},{20,-100}},
+                              color={0,127,255}));
+  connect(eva.port_b, port_b2) annotation (Line(points={{-20,-100},{-80,-100},{-80,
+          -60},{-100,-60}}, color={0,127,255}));
+  connect(refCyc.QEva_flow, refCycIneEva.u) annotation (Line(points={{-1.22125e-15,
+          -19.8},{-1.22125e-15,-28.9},{2.22045e-15,-28.9},{2.22045e-15,-38}},
+        color={0,0,127}));
+  connect(eva.Q_flow,refCycIneEva. y) annotation (Line(points={{0,-76},{0,-65.9},
+          {-1.9984e-15,-65.9},{-1.9984e-15,-61}},                     color={0,0,
+          127}));
+  connect(refCycIneCon.y, con.Q_flow) annotation (Line(points={{6.66134e-16,61},
+          {6.66134e-16,69.9},{0,69.9},{0,76}},                       color={0,0,
+          127}));
+  connect(refCycIneCon.u, refCyc.QCon_flow) annotation (Line(points={{-8.88178e-16,
+          38},{-8.88178e-16,28.9},{1.22125e-15,28.9},{1.22125e-15,19.8}}, color=
+         {0,0,127}));
+  connect(mCon_flow.port_b, con.port_a)
+    annotation (Line(points={{-40,100},{-20,100}},
+                                                 color={0,127,255}));
+  connect(con.port_b, port_b1) annotation (Line(points={{20,100},{100,100},{100,
+          60}},      color={0,127,255}));
+  // External bus connections
+  connect(mEva_flow.m_flow, sigBus.mEvaMea_flow) annotation (Line(points={{70,-49},
+          {70,-40},{26,-40},{26,-30},{-20,-30},{-20,-40},{-138,-40},{-138,-41},{-141,
+          -41}},                                                color={0,0,127}),
+      Text(
+      string="%second",
+      index=1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(mCon_flow.m_flow, sigBus.mConMea_flow) annotation (Line(points={{-50,89},
+          {-50,32},{-76,32},{-76,-40},{-134,-40},{-134,-42},{-138,-42},{-138,-41},
+          {-141,-41}},                           color={0,0,127}));
+  connect(refCyc.sigBus, sigBus) annotation (Line(
+      points={{-17.82,0.18},{-40,0.18},{-40,-40},{-138,-40},{-138,-42},{-140,-42},
+          {-140,-41},{-141,-41}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(refCyc.PEle, sigBus.PEleMea) annotation (Line(points={{19.89,0.09},{26,
+          0.09},{26,-30},{-20,-30},{-20,-40},{-138,-40},{-138,-41},{-141,-41}},
+        color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(hys.y, sigBus.onOffMea) annotation (Line(points={{-99,-90},{-88,-90},{
+          -88,-70},{-128,-70},{-128,-40},{-134,-40},{-134,-41},{-141,-41}},
+                                           color={255,0,255}));
+  connect(TConAmb, sigBus.TConAmbMea) annotation (Line(
+      points={{-152,120},{-128,120},{-128,50},{-76,50},{-76,-42},{-78,-42},{-78,
+          -41},{-141,-41}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(TEvaAmb, sigBus.TEvaAmbMea) annotation (Line(
+      points={{-152,-130},{-130,-130},{-130,-110},{-76,-110},{-76,-41},{-141,-41}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(hys.u, sigBus.yMea) annotation (Line(points={{-122,-90},{-132,-90},{-132,
+          -40},{-136,-40},{-136,-41},{-141,-41}},
+                       color={0,0,127}));
+  connect(con.T, sigBus.TConOutMea) annotation (Line(points={{22.4,90},{38,90},{
+          38,32},{-76,32},{-76,-40},{-140,-40},{-140,-41},{-141,-41}},
+                                                 color={0,0,127}));
+  connect(senTConIn.y, sigBus.TConInMea) annotation (Line(points={{-87,32},{-76,
+          32},{-76,-40},{-140,-40},{-140,-41},{-141,-41}},
+                                                       color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,-6},{-3,-6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(eva.T, sigBus.TEvaOutMea) annotation (Line(points={{-22.4,-90},{-76,-90},
+          {-76,-40},{-142,-40},{-142,-41},{-141,-41}},
+                                 color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(senTEvaIn.y, sigBus.TEvaInMea) annotation (Line(points={{-87,12},{-76,
+          12},{-76,-40},{-148,-40},{-148,-41},{-141,-41}},              color={0,
+          0,127}));
+  if not use_intSafCtr then
+    connect(ySet, sigBus.yMea) annotation (Line(points={{-152,20},{-120,20},{-120,
+            -40},{-136,-40},{-136,-41},{-141,-41}},
+                       color={0,0,127}));
+  end if;
+  connect(ySet, sigBus.ySet) annotation (Line(points={{-152,20},{-120,20},{-120,
+          -40},{-136,-40},{-136,-41},{-141,-41}},
+                     color={0,0,127}));
+  connect(refCyc.PEle, P) annotation (Line(points={{19.89,0.09},{26,0.09},{26,0},{
+          150,0}}, color={0,0,127}));
+  connect(refCycIneEva.y, QEva_flow) annotation (Line(points={{-1.9984e-15,-61},{-1.9984e-15,
+          -68},{50,-68},{50,-130},{150,-130}}, color={0,0,127}));
+  connect(refCycIneCon.y, QCon_flow) annotation (Line(points={{8.88178e-16,61},{8.88178e-16,
+          70},{70,70},{70,130},{150,130}}, color={0,0,127}));
+  connect(eff.PEle, refCyc.PEle) annotation (Line(points={{98,23},{48,23},{48,0.09},
+          {19.89,0.09}}, color={0,0,127}));
+  connect(eff.COP, COP) annotation (Line(points={{121,36},{130,36},{130,30},{150,30}},
+        color={0,0,127}));
+  connect(eff.EER, EER) annotation (Line(points={{121,24},{130,24},{130,-30},{150,
+          -30}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(extent={{-100,-100},{100,100}}),
+                   graphics={
+        Rectangle(
+          extent={{-102,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-16,60},{16,-60}},
+          fillColor={170,213,255},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0},
+          origin={0,-64},
+          rotation=90),
+        Rectangle(
+          extent={{-16,60},{16,-60}},
+          fillColor={238,46,47},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0},
+          origin={0,60},
+          rotation=90),
+        Line(
+          points={{-9,40},{9,40},{-5,-2},{9,-40},{-9,-40}},
+          color={0,0,0},
+          smooth=Smooth.None,
+          origin={-3,-60},
+          rotation=-90),
+        Line(
+          points={{9,40},{-9,40},{5,-2},{-9,-40},{9,-40}},
+          color={0,0,0},
+          smooth=Smooth.None,
+          origin={-5,56},
+          rotation=-90),
+        Rectangle(
+          extent={{-60,42},{60,-46}},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+    Line(
+    origin={-75.5,-80.333},
+    points={{43.5,8.3333},{37.5,0.3333},{25.5,-1.667},{33.5,-9.667},{17.5,-11.667},{27.5,-21.667},{13.5,-23.667},
+              {11.5,-31.667}},
+      smooth=Smooth.Bezier,
+      visible=use_evaCap),
+        Polygon(
+          points={{-70,-122},{-68,-108},{-58,-114},{-70,-122}},
+          lineColor={0,0,0},
+          fillPattern=FillPattern.Solid,
+          fillColor={0,0,0},
+          visible=use_evaCap),
+    Line( origin={24.5,93.667},
+          points={{39.5,6.333},{37.5,0.3333},{25.5,-1.667},{33.5,-9.667},{17.5,
+              -11.667},{27.5,-21.667},{13.5,-23.667},{11.5,-27.667}},
+          smooth=Smooth.Bezier,
+          visible=use_conCap),
+        Polygon(
+          points={{70,110},{68,96},{58,102},{70,110}},
+          lineColor={0,0,0},
+          fillPattern=FillPattern.Solid,
+          fillColor={0,0,0},
+          visible=use_conCap),
+        Line(
+          points={{-42,72},{34,72}},
+          color={0,0,0},
+          arrow={Arrow.None,Arrow.Filled},
+          thickness=0.5),
+        Line(
+          points={{-38,0},{38,0}},
+          color={0,0,0},
+          arrow={Arrow.None,Arrow.Filled},
+          thickness=0.5,
+          origin={0,-74},
+          rotation=180),
+        Text(
+          extent={{-96,100},{-68,78}},
+          textColor={0,0,127},
+          visible=use_conCap and not use_busConOnl,
+          textString="TConAmb"),
+        Text(
+          extent={{-96,28},{-74,10}},
+          textColor={0,0,127},
+          visible=not use_busConOnl,
+          textString="ySet"),
+        Text(
+          extent={{-96,-80},{-68,-102}},
+          textColor={0,0,127},
+          visible=use_evaCap and not use_busConOnl,
+          textString="TEvaAmb"),
+        Text(
+          extent={{64,104},{96,76}},
+          textColor={0,0,127},
+          textString="QCon_flow"),
+        Text(
+          extent={{64,-74},{96,-102}},
+          textColor={0,0,127},
+          textString="QEva_flow"),
+        Text(
+          extent={{72,10},{96,-6}},
+          textColor={0,0,127},
+          textString="P"),
+        Text(
+          extent={{72,40},{96,16}},
+          textColor={0,0,127},
+          visible=use_COP,
+          textString="COP"),
+        Text(
+          extent={{72,-18},{96,-42}},
+          textColor={0,0,127},
+          visible=use_EER,
+          textString="EER"),
+        Rectangle(
+          extent={{34,42},{38,-46}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{14,22},{58,-20}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Polygon(
+          points={{36,22},{18,-10},{54,-10},{36,22}},
+          lineColor={0,0,0},
+          smooth=Smooth.None,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-46,42},{-42,-46}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Polygon(
+          points={{-44,2},{-54,-10},{-34,-10},{-44,2}},
+          lineColor={0,0,0},
+          smooth=Smooth.None,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Polygon(
+          points={{-44,2},{-54,12},{-34,12},{-44,2}},
+          lineColor={0,0,0},
+          smooth=Smooth.None,
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}),
+       Diagram(coordinateSystem(extent={{-140,-160},{140,160}})),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>July 15, 2024</i> by Fabian Wuellhorst:<br/>
+    Adjust hysteresis bandwidth (see issue
+    <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1908\">IBPSA #1908</a>)
+  </li>
+  <li>
+    May 2, 2024, by Michael Wetter:<br/>
+    Refactored check for device identifiers.<br/>
+    This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">IBPSA, #1576</a>.
+  </li>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on the discussion in this issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>May 22, 2019</i> by Julian Matthes:<br/>
+    Rebuild due to the introducion of the thermal machine partial model
+    (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/715\">#715</a>)
+  </li>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">#577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This partial model defines all components which are equally required
+  for heat pump and chillers. This encompasses
+</p>
+<ul>
+<li>the heat exchangers (evaporator and condenser),</li>
+<li>sensors for temperature and mass flow rates,</li>
+<li>the replaceable model for refrigerant inertia,</li>
+<li>safety controls,</li>
+<li>connectors and parameters,</li>
+<li>and the replaceable refrigerant cycle model <code>refCyc</code></li>
+</ul>
+<p>
+  The model <code>refCyc</code> is replaced in the ModularReversible
+  model for heat pumps and chillers, e.g. by
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantCycle\">
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantCycle</a>
+  in <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a>.
+</p>
+<p>
+  For more information on the approach, please read the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  UsersGuide</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialReversibleRefrigerantMachine;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/RefrigerantCycle.mo b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/RefrigerantCycle.mo
new file mode 100644
index 0000000000..9f738162f6
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/RefrigerantCycle.mo
@@ -0,0 +1,197 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses;
+model RefrigerantCycle
+  "Refrigerant cycle model of a heat pump"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialModularRefrigerantCycle;
+
+  parameter Boolean allowDifferentDeviceIdentifiers=false
+    "if use_rev=true, device data for cooling and heating need to entered. Set allowDifferentDeviceIdentifiers=true to allow different device identifiers devIde"
+    annotation(Dialog(enable=use_rev));
+
+  replaceable model RefrigerantCycleHeatPumpHeating =
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.NoHeating(
+      useInHeaPum=true)
+      constrainedby
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle
+    "Replaceable model for refrigerant cycle of a heat pump in main operation mode"
+    annotation (choicesAllMatching=true);
+
+  replaceable model RefrigerantCycleHeatPumpCooling =
+      AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.NoCooling(
+        useInChi=true)
+      constrainedby
+        AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle
+    "Replaceable model for refrigerant cycle of a heat pump in reversed operation mode"
+    annotation (Dialog(enable=use_rev),choicesAllMatching=true);
+
+  RefrigerantCycleHeatPumpHeating refCycHeaPumHea
+    "Refrigerant cycle instance for heating"
+  annotation (Placement(transformation(extent={{20,40},{60,80}}, rotation=0)));
+  RefrigerantCycleHeatPumpCooling refCycHeaPumCoo
+    "Refrigerant cycle instance for cooling"
+  annotation (Placement(transformation(extent={{-60,40},{-19,80}}, rotation=0)));
+
+protected
+  parameter String devIde =
+    if use_rev then refCycHeaPumCoo.devIde else refCycHeaPumHea.devIde
+    "Data source for refrigerant cycle";
+
+initial algorithm
+  if not allowDifferentDeviceIdentifiers then
+    assert(
+      devIde == refCycHeaPumHea.devIde,
+      "In " + getInstanceName() + ": Device identifiers devIde for reversible operation are not equal.
+      Heating device identifier is '" + refCycHeaPumHea.devIde + "' but cooling is '"
+      + devIde + "'. To allow this, set 'allowDifferentDeviceIdentifiers=true'.",
+      AssertionLevel.error);
+  end if;
+
+equation
+  connect(pasTrhModSet.u, sigBus.hea);
+
+  connect(sigBus,refCycHeaPumCoo.sigBus)  annotation (Line(
+      points={{0,100},{0,90},{-40,90},{-40,86},{-39.3292,86},{-39.3292,80}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(sigBus,refCycHeaPumHea.sigBus)  annotation (Line(
+      points={{0,100},{0,90},{40.1667,90},{40.1667,80}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(swiQCon.u2, sigBus.hea) annotation (Line(points={{58,0},{0,0},{0,100}},
+        color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(swiPEle.u2, sigBus.hea) annotation (Line(points={{2.22045e-15,-58},{2.22045e-15,
+          22},{0,22},{0,100}}, color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(swiQEva.u2, sigBus.hea) annotation (Line(points={{-58,0},{0,0},{0,100},
+          {0,100}}, color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(refCycHeaPumHea.QCon_flow, swiQCon.u1) annotation (Line(points={{26.6667,
+          38.3333},{26.6667,8},{58,8}},         color={0,0,127}));
+  connect(refCycHeaPumHea.QEva_flow, swiQEva.u1) annotation (Line(points={{53.3333,
+          38.3333},{53.3333,28},{-12,28},{-12,8},{-58,8}},         color={0,0,127}));
+  connect(refCycHeaPumCoo.QEva_flow, swiQCon.u3) annotation (Line(points={{
+          -25.8333,38.3333},{-25.8333,-8},{58,-8}}, color={0,0,127}));
+  connect(refCycHeaPumCoo.QCon_flow, swiQEva.u3) annotation (Line(points={{
+          -53.1667,38.3333},{-53.1667,-8},{-58,-8}}, color={0,0,127}));
+  connect(refCycHeaPumCoo.PEle, swiPEle.u3) annotation (Line(points={{-39.5,
+          38.3333},{-39.5,-48},{-8,-48},{-8,-58}}, color={0,0,127}));
+  connect(refCycHeaPumHea.PEle, swiPEle.u1) annotation (Line(points={{40,
+          38.3333},{40,-48},{8,-48},{8,-58}},
+                                     color={0,0,127}));
+
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Ellipse(
+          extent={{-24,88},{22,44}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{-16,82},{20,74}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-18,52},{20,58}},
+          color={28,108,200},
+          thickness=0.5),
+        Rectangle(
+          extent={{-98,40},{-60,-28}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{-20,-60},{-20,-70},{-20,-80},{20,-60},{20,-80},{-20,-60}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-122,34},{-66,34},{-82,10},{-66,-22},{-120,-22}},
+          color={28,108,200},
+          thickness=0.5),
+        Rectangle(
+          extent={{60,40},{98,-28}},
+          lineColor={28,108,200},
+          lineThickness=0.5),
+        Line(
+          points={{120,34},{64,34},{80,10},{64,-22},{118,-22}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-80,40},{-80,68},{-24,68}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{22,66},{80,66},{80,40}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{78,-28},{78,-70}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{78,-70},{62,-70},{20,-70}},
+          color={28,108,200},
+          thickness=0.5),
+        Line(
+          points={{-80,-26},{-80,-68},{-20,-68}},
+          color={28,108,200},
+          thickness=0.5),
+        Text(
+          extent={{-151,147},{149,107}},
+          textColor={0,0,255},
+          fillPattern=FillPattern.HorizontalCylinder,
+          fillColor={0,127,255},
+          textString="%name")}),
+          Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html><ul>
+  <li>
+    May 2, 2024, by Michael Wetter:<br/>
+    Refactored check for device identifiers.<br/>
+    This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">IBPSA, #1576</a>.
+  </li>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on the discussion in this issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>May 22, 2019</i> by Julian Matthes:<br/>
+    Rebuild due to the introducion of the thermal machine partial model
+    (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/715\">AixLib #715</a>)
+  </li>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Modular refrigerant cycle model for heat pump applications used in
+  the model <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a> and extending models
+  of the modular approach.
+</p>
+<p>
+  This model adds the replaceable model approaches for cooling and heating data
+  to the partial refrigerant cylce.
+</p>
+<p>
+  Further, an asseration warning is raised if the model approaches or
+  sources for performance data differ. This indicates that they are not
+  for the same device.
+</p>
+<p>
+  For more information on the approach, please read the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  UsersGuide</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end RefrigerantCycle;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/RefrigerantMachineControlBus.mo b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/RefrigerantMachineControlBus.mo
new file mode 100644
index 0000000000..ed43046426
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/RefrigerantMachineControlBus.mo
@@ -0,0 +1,31 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses;
+expandable connector RefrigerantMachineControlBus
+  "Bus connector for reversible heat pump and chiller model"
+  extends Modelica.Icons.SignalBus;
+  annotation (Documentation(info="<html>
+<p>
+  Bus connector for a refrigerant machine.
+</p>
+<p>
+  Used in the reversbile modular approaches for chiller
+  and heat pump in the models
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.Modular\">
+  AixLib.Fluid.Chillers.ModularReversible.Modular</a> and
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a>.
+</p>
+</html>", revisions="<html><ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  Adapted based on AixLib implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+<li>
+  <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end RefrigerantMachineControlBus;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/package.mo
new file mode 100644
index 0000000000..d0254c46e7
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+package BaseClasses "Package with base classes for AixLib.Fluid.HeatPumps.ModularReversible"
+  extends Modelica.Icons.BasesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains base classes that are used to construct the models in
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible\">AixLib.Fluid.HeatPumps.ModularReversible</a>.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/package.order
new file mode 100644
index 0000000000..dec7694d55
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/BaseClasses/package.order
@@ -0,0 +1,7 @@
+CalculateEfficiency
+EvaporatorCondenserWithCapacity
+LargeScaleWaterToWaterDeclarations
+PartialModularRefrigerantCycle
+PartialReversibleRefrigerantMachine
+RefrigerantCycle
+RefrigerantMachineControlBus
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/CarnotWithLosses.mo b/AixLib/Fluid/HeatPumps/ModularReversible/CarnotWithLosses.mo
new file mode 100644
index 0000000000..c5019ee233
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/CarnotWithLosses.mo
@@ -0,0 +1,106 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+model CarnotWithLosses
+  "Heat pump using the Carnot approach, but with added reversibility and losses (heat, frost, inertia)"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.Modular(
+    QCoo_flow_nominal=-PEle_nominal*refCyc.refCycHeaPumCoo.EER_nominal,
+    redeclare model RefrigerantCycleHeatPumpCooling =
+        AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness
+        (
+        PEle_nominal=PEle_nominal,
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+          iceFacCal,
+        etaCarnot_nominal=etaCarnot_nominal,
+        use_constAppTem=true,
+        TAppCon_nominal=TAppCon_nominal,
+        TAppEva_nominal=TAppEva_nominal),
+    redeclare model RefrigerantCycleHeatPumpHeating =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness
+        (
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.FunctionalIcingFactor
+          iceFacCal(redeclare function icingFactor =
+              AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.Functions.wetterAfjei1997),
+        etaCarnot_nominal=etaCarnot_nominal,
+        TAppCon_nominal=TAppCon_nominal,
+        TAppEva_nominal=TAppEva_nominal),
+    final allowDifferentDeviceIdentifiers=false,
+    final use_evaCap,
+    final use_conCap,
+    redeclare model RefrigerantCycleInertia =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.VariableOrder
+        (
+        final refIneFreConst=1/refIneTimCon,
+        final nthOrd=nthOrd,
+        initType=Modelica.Blocks.Types.Init.InitialOutput));
+
+  parameter Real etaCarnot_nominal=0.3 "Constant Carnot effectiveness";
+  parameter Modelica.Units.SI.TemperatureDifference TAppCon_nominal=
+    if cpCon < 1500 then 5 else 2
+    "Temperature difference between refrigerant and working fluid outlet in condenser"
+    annotation(Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.TemperatureDifference TAppEva_nominal=
+    if cpEva < 1500 then 5 else 2
+    "Temperature difference between refrigerant and working fluid outlet in evaporator"
+    annotation(Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.Time refIneTimCon = 300
+    "Refrigerant cycle inertia time constant for first order delay"
+    annotation(Dialog(group="Refrigerant cycle inertia"));
+  parameter Integer nthOrd(min=1)=1 "Order of refrigerant cycle interia"
+    annotation(Dialog(group="Refrigerant cycle inertia"));
+
+initial algorithm
+  assert(use_rev and (abs(refCyc.refCycHeaPumCoo.PEle_nominal - PEle_nominal) / PEle_nominal < limWarSca),
+    "In " + getInstanceName() + ": Nominal electrical powers for heating and cooling
+    operation differ by " + String((refCyc.refCycHeaPumCoo.PEle_nominal - PEle_nominal) / PEle_nominal * 100) +
+    " %. The simulated nominal heating and cooling
+    capacities may not be realistic for a single device.",
+    AssertionLevel.warning);
+  annotation (Documentation(info="<html>
+<p>
+  Model of a reversible heat pump.
+</p>
+<p>
+  This model extends
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a> and selects the
+  constant Carnot effectiveness module for heat pumps
+  (<a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness</a>)
+  and chillers
+  (<a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness\">
+  AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness</a>)
+  to model a reversible heat pump.
+  For the heating operation, the approach temperatures are fixed
+  at nominal values to avoid nonlinear system of equations.
+</p>
+<p>
+  Furthermore, losses are enabled to model
+  the heat pump with a more realistic behaviour:
+</p>
+<ul>
+<li>Heat losses to the ambient (can be disabled)</li>
+<li>Refrigerant inertia using a first order delay</li>
+<li>Evaporator frosting assuming an air-sink chiller</li>
+</ul>
+<p>
+  For more information on the approach, see
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  May 2, 2024, by Michael Wetter:<br/>
+  Refactored check for device identifiers.<br/>
+  This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">IBPSA, #1576</a>.
+</li>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CarnotWithLosses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/AntiFreeze.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/AntiFreeze.mo
new file mode 100644
index 0000000000..01e8ef1dce
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/AntiFreeze.mo
@@ -0,0 +1,75 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety;
+model AntiFreeze "Model to prevent source from freezing"
+  extends BaseClasses.PartialSafetyWithCounter;
+
+  parameter Modelica.Units.SI.ThermodynamicTemperature TAntFre=276.15
+    "Limit temperature for anti freeze control";
+  parameter Real dTHys=2
+    "Hysteresis interval width";
+  Modelica.Blocks.Logical.Hysteresis hys(
+    final uLow=TAntFre,
+    final pre_y_start=true,
+    final uHigh=TAntFre + dTHys) "Hysteresis to indicate if freezing occurs"
+    annotation (Placement(transformation(extent={{-20,10},{0,30}})));
+
+  Modelica.Blocks.Math.Min min
+    "Minimum of evaporator outlet and condenser inlet temperatures"
+   annotation (Placement(transformation(extent={{-58,10},{-38,30}})));
+
+equation
+  connect(ySet,swiErr.u1)  annotation (Line(points={{-136,0},{-100,0},{-100,52},
+          {70,52},{70,8},{78,8}},
+                  color={0,0,127}));
+  connect(min.y, hys.u)
+    annotation (Line(points={{-37,20},{-22,20}},   color={0,0,127}));
+  connect(sigBus.TConInMea, min.u1) annotation (Line(
+      points={{-119,-61},{-119,-60},{-92,-60},{-92,26},{-60,26}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-3,-6},{-3,-6}},
+      horizontalAlignment=TextAlignment.Right));
+
+  connect(sigBus.TEvaOutMea, min.u2) annotation (Line(
+      points={{-119,-61},{-119,-60},{-92,-60},{-92,14},{-60,14}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+
+  connect(hys.y, booPasThr.u) annotation (Line(
+      points={{1,20},{20,20},{20,0},{38,0}},
+      color={255,0,255}));
+  annotation (Documentation(revisions="<html><ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  Adapted based on AixLib implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+<li>
+  <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+</li>
+</ul>
+</html>", info="<html>
+<p>
+  This model is used to prevent freezing of
+  the condenser or evaporator side.
+  A real device would shut off as well.
+</p>
+<p>
+  This models takes the minimum of the two temperatures evaporator
+  outlet and condenser inlet. If this minimal temperature falls below
+  the given lower boundary, the hystereses will trigger an error and cause
+  the device to switch off.
+</p>
+<h4>Assumptions</h4>
+  This block does not check the evaporator inlet or condenser outlet temperatures
+  because they are assumed to be always higher than the other side.
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end AntiFreeze;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/BoundaryMap.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/BoundaryMap.mo
new file mode 100644
index 0000000000..aedb46e032
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/BoundaryMap.mo
@@ -0,0 +1,192 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses;
+model BoundaryMap
+  "Block that checks if the inputs are within the characteristic map"
+  parameter Real tab[:,2]
+    "Table for boundary with second column as useful temperature side";
+  parameter Modelica.Units.SI.TemperatureDifference dT
+    "Delta value used to avoid state events when used as a safety control";
+  parameter Boolean isUppBou "=true if it is an upper boundary, false for lower";
+  Modelica.Blocks.Interfaces.BooleanOutput noErr
+    "=false when an error occurs"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  Modelica.Blocks.Interfaces.RealInput TAmbSid(unit="K", displayUnit="degC")
+    "Temperature at ambient side"
+    annotation (Placement(transformation(extent={{-130,-54},{-102,-26}})));
+
+  Modelica.Blocks.Tables.CombiTable1Ds tabBou(
+    final table=tab,
+    final smoothness=Modelica.Blocks.Types.Smoothness.LinearSegments,
+    final tableOnFile=false) "Table with envelope data"
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+  Modelica.Blocks.MathBoolean.Nor nor(nu=3)
+    "=true if the operational envelope is not violated"
+    annotation (Placement(transformation(extent={{60,-10},{80,10}})));
+  Modelica.Blocks.Logical.Hysteresis hysLef(
+    final uLow=-0.05,
+    final uHigh=0,
+    pre_y_start=false) "Hysteresis for left side of envelope"
+  annotation (Placement(transformation(extent={{20,-40},{40,-20}})));
+  Modelica.Blocks.Logical.Hysteresis hysRig(
+    final uLow=-0.05,
+    final uHigh=0,
+    pre_y_start=false) "Hysteresis for right side of envelope"
+    annotation (Placement(transformation(extent={{20,-80},{40,-60}})));
+  Modelica.Blocks.Sources.Constant conTAmbSidMin(k=TAmbSidMin)
+    "Constant minimal temperature of ambient temperature side"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  Modelica.Blocks.Sources.Constant conTAmbSidMax(k=TAmbSidMax)
+    "Constant maximal temperature of ambient temperature side"
+    annotation (Placement(transformation(extent={{-60,-90},{-40,-70}})));
+
+  Modelica.Blocks.Math.Add subMax(final k1=+1, final k2=-1)
+    "Actual minus maximal ambient side temperature"
+    annotation (Placement(transformation(extent={{-20,-80},{0,-60}})));
+  Modelica.Blocks.Math.Add sub(final k1=-1, final k2=+1)
+    "Minimal minus current ambient side temperature"
+    annotation (Placement(transformation(extent={{-20,-40},{0,-20}})));
+  Modelica.Blocks.Interfaces.RealInput TUseSid(unit="K", displayUnit="degC")
+    "Useful temperature side "
+    annotation (Placement(transformation(extent={{-128,26},{-100,54}})));
+  Modelica.Blocks.Math.Add subBou(final k1=if isUppBou then 1 else -1, final k2=
+       if isUppBou then -1 else 1)
+    "Subtract boundary from current value depending on lower or upper boundary"
+    annotation (Placement(transformation(extent={{-20,60},{0,80}})));
+  Modelica.Blocks.Logical.Hysteresis hysBou(
+    final uLow=-dT,
+    final uHigh=0,
+    pre_y_start=false) "Hysteresis for temperature limit"
+    annotation (Placement(transformation(extent={{20,0},{40,20}})));
+protected
+  parameter Real icoMin=-70
+    "Used to set the frame where the icon should appear";
+  parameter Real icoMax=70 "Used to set the frame where the icon should appear";
+  final parameter Modelica.Units.SI.Temperature TAmbSidMax=tab[end, 1]
+    "Maximal value of ambient side";
+  final parameter Modelica.Units.SI.Temperature TAmbSidMin=tab[1, 1]
+    "Minimal temperature at ambient side";
+  final parameter Modelica.Units.SI.Temperature TUseSidMax=max(tab[:, 2])
+    "Maximal temperature of useful side";
+  final parameter Modelica.Units.SI.Temperature TUseSidMin=0
+    "Minimal value of useful side";
+  final parameter Real poi[size(scaTAmbSid, 1),2]=transpose({scaTAmbSidToPoi,
+      scaTUseSidToPoi}) "Points for dynamic annotation"
+    annotation (Hide=false, HideResult=false);
+  final parameter Modelica.Units.SI.Temperature scaTAmbSid[:]=tab[:, 1]
+    "Helper array with only not ambient side temperature values";
+  final parameter Modelica.Units.SI.Temperature scaTUseSid[:]=tab[:, 2]
+    "Helper array with only useful side temperature values";
+  final parameter Real scaTAmbSidToPoi[size(scaTAmbSid, 1)](
+    each min=-100,
+    each max=100) = (scaTAmbSid - fill(TAmbSidMin, size(scaTAmbSid, 1)))*(icoMax -
+    icoMin)/(TAmbSidMax - TAmbSidMin) + fill(icoMin, size(scaTAmbSid, 1))
+    "Scale ambient side to icon size";
+  final parameter Real scaTUseSidToPoi[size(scaTAmbSid, 1)](
+    each min=-100,
+    each max=100) = (scaTUseSid - fill(TUseSidMin, size(scaTUseSid, 1)))*(icoMax -
+    icoMin)/(TUseSidMax - TUseSidMin) + fill(icoMin, size(scaTUseSid, 1))
+    "Scale useful side to icon size";
+
+equation
+  connect(nor.y, noErr)
+    annotation (Line(points={{81.5,0},{110,0}}, color={255,0,255}));
+  connect(hysLef.y, nor.u[1]) annotation (Line(points={{41,-30},{50,-30},{50,-2.33333},
+          {60,-2.33333}}, color={255,0,255}));
+  connect(hysRig.y, nor.u[2]) annotation (Line(points={{41,-70},{50,-70},{50,-5.55112e-16},
+          {60,-5.55112e-16}}, color={255,0,255}));
+  connect(subMax.u2,conTAmbSidMax.y)  annotation (Line(points={{-22,-76},{-32,-76},
+          {-32,-80},{-39,-80}}, color={0,0,127}));
+  connect(sub.u2,conTAmbSidMin.y)  annotation (Line(points={{-22,-36},{-32,-36},{
+          -32,-40},{-39,-40}},  color={0,0,127}));
+  connect(subMax.y, hysRig.u)
+    annotation (Line(points={{1,-70},{18,-70}}, color={0,0,127}));
+  connect(sub.y, hysLef.u)
+    annotation (Line(points={{1,-30},{18,-30}}, color={0,0,127}));
+  connect(hysBou.u, subBou.y)
+    annotation (Line(points={{18,10},{6,10},{6,70},{1,70}}, color={0,0,127}));
+  connect(hysBou.y, nor.u[3]) annotation (Line(points={{41,10},{50,10},{50,2.33333},
+          {60,2.33333}}, color={255,0,255}));
+  connect(tabBou.y[1], subBou.u2) annotation (Line(points={{-39,50},{-30,50},{-30,
+          64},{-22,64}}, color={0,0,127}));
+  connect(subBou.u1, TUseSid) annotation (Line(points={{-22,76},{-96,76},{-96,40},
+          {-114,40}}, color={0,0,127}));
+  connect(TAmbSid, tabBou.u) annotation (Line(points={{-116,-40},{-80,-40},{-80,50},
+          {-62,50}}, color={0,0,127}));
+  connect(TAmbSid, sub.u1) annotation (Line(points={{-116,-40},{-80,-40},{-80,-24},
+          {-22,-24}}, color={0,0,127}));
+  connect(TAmbSid, subMax.u1) annotation (Line(points={{-116,-40},{-80,-40},{-80,
+          -64},{-22,-64}},                color={0,0,127}));
+  annotation (Icon(
+    coordinateSystem(preserveAspectRatio=false,
+    extent={{-100,-100},{100,100}}), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+                                    Line(points=DynamicSelect(
+      {{-66,-66},{-66,50},{-44,66}, {68,66},{68,-66},{-66,-66}},poi),
+      color={238,46,47},
+      thickness=0.5),
+  Polygon(
+    points={{icoMin-20,icoMax},{icoMin-20,icoMax},
+            {icoMin-10,icoMax},{icoMin-15,icoMax+20}},
+    lineColor={95,95,95},
+    fillColor={95,95,95},
+    fillPattern=FillPattern.Solid),
+  Polygon(
+    points={{icoMax+20,icoMin-10},{icoMax,icoMin-4},
+            {icoMax,icoMin-16},{icoMax+20,icoMin-10}},
+    lineColor={95,95,95},
+    fillColor={95,95,95},
+    fillPattern=FillPattern.Solid),
+  Line(points={{icoMin-15,icoMax},
+              {icoMin-15,icoMin-15}}, color={95,95,95}),
+  Line(points={{icoMin-20,icoMin-10},
+              {icoMax+10,icoMin-10}}, color={95,95,95}),
+        Text(
+          extent={{-149,135},{151,95}},
+          textColor={0,0,255},
+          fillPattern=FillPattern.HorizontalCylinder,
+          fillColor={0,127,255},
+          textString="%name")}),
+      coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
+  Documentation(info="<html>
+<p>
+  Given an input of <code>TCon</code> and <code>TEva</code>,
+  the model returns false if the given
+  point is outside of the given operational envelope.
+</p>
+<p>
+  The maximal and minimal <code>TCon</code> depend on
+  <code>TEva</code> and are defined by the
+  upper and lower boundaries in form of 1Ds-Tables.</p>
+<p>
+  The maximal and minimal <code>TEva</code> values are obtained
+  trough the table and are constant.
+</p>
+<p>
+  For the boundaries of the <code>TCon</code> input value, a
+  dynamic hysteresis is used to ensure a used device will
+  stay off a certain time after shutdown.
+</p>
+<p>
+  This is similar to the hysteresis in a pressure-based safety control,
+  which prevents operation outside this envelope in real devices.
+</p>
+</html>",
+        revisions="<html>
+<ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on IPBSA guidelines <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>November 26, 2018;</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue
+    <a href=\"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BoundaryMap;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/CycleRateBoundary.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/CycleRateBoundary.mo
new file mode 100644
index 0000000000..89a5014ba4
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/CycleRateBoundary.mo
@@ -0,0 +1,92 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses;
+block CycleRateBoundary "Checks if the cycle rate is in boundary"
+  extends Modelica.Blocks.Interfaces.BooleanSISO;
+  parameter Integer maxCycRat "Maximal cycle rate";
+  parameter Modelica.Units.SI.Time delTim(displayUnit="h") = 3600
+    "Delay time of output with respect to input signal";
+  Modelica.Blocks.Logical.LessThreshold runCouLesMax(threshold=maxCycRat)
+    "Checks if the count of total runs is lower than the maximal value"
+    annotation (Placement(transformation(extent={{70,-10},{90,10}})));
+  Modelica.Blocks.MathInteger.TriggeredAdd triAdd "Count number of starts"
+    annotation (Placement(transformation(extent={{-50,-10},{-30,-30}})));
+  Modelica.Blocks.Sources.IntegerConstant intConPluOne(final k=1)
+    "Value for counting"
+    annotation (Placement(transformation(extent={{-90,-30},{-70,-10}})));
+  Modelica.Blocks.Math.IntegerToReal intToRea
+    "Convert to real in order to compare and delay"
+    annotation (Placement(transformation(extent={{-20,-30},{0,-10}})));
+  Modelica.Blocks.Math.Add sub(k2=-1)
+    "Difference of current and delayed starts"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+  Modelica.Blocks.Nonlinear.FixedDelay fixDel(final delayTime=delTim)
+    "Apply delay to enable starts per delay time"
+    annotation (Placement(transformation(extent={{20,-50},{40,-30}})));
+equation
+  connect(intConPluOne.y, triAdd.u) annotation (Line(points={{-69,-20},{-54,-20}},
+                            color={255,127,0}));
+  connect(intToRea.u, triAdd.y)
+    annotation (Line(points={{-22,-20},{-28,-20}},
+                                               color={255,127,0}));
+  connect(intToRea.y, sub.u1)
+    annotation (Line(points={{1,-20},{12,-20},{12,6},{38,6}},
+                                                          color={0,0,127}));
+  connect(intToRea.y, fixDel.u)
+    annotation (Line(points={{1,-20},{12,-20},{12,-40},{18,-40}},
+                                                           color={0,0,127}));
+  connect(fixDel.y, sub.u2)
+    annotation (Line(points={{41,-40},{50,-40},{50,-20},{28,-20},{28,-6},{38,-6}},
+                                                        color={0,0,127}));
+  connect(runCouLesMax.y, y)
+    annotation (Line(points={{91,0},{110,0}},           color={255,0,255}));
+  connect(u, triAdd.trigger) annotation (Line(points={{-120,0},{-46,0},{-46,-8}},
+                              color={255,0,255}));
+  connect(sub.y, runCouLesMax.u) annotation (Line(points={{61,0},{68,0}},
+                     color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+                                Rectangle(
+        extent={{-100,-100},{100,100}},
+        lineColor={0,0,127},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),
+        Ellipse(extent={{-80,80},{80,-80}}, lineColor={160,160,164}),
+        Line(points={{0,80},{0,60}}, color={160,160,164}),
+        Line(points={{80,0},{60,0}}, color={160,160,164}),
+        Line(points={{0,-80},{0,-60}}, color={160,160,164}),
+        Line(points={{-80,0},{-60,0}}, color={160,160,164}),
+        Line(points={{37,70},{26,50}}, color={160,160,164}),
+        Line(points={{70,38},{49,26}}, color={160,160,164}),
+        Line(points={{71,-37},{52,-27}}, color={160,160,164}),
+        Line(points={{39,-70},{29,-51}}, color={160,160,164}),
+        Line(points={{-39,-70},{-29,-52}}, color={160,160,164}),
+        Line(points={{-71,-37},{-50,-26}}, color={160,160,164}),
+        Line(points={{-71,37},{-54,28}}, color={160,160,164}),
+        Line(points={{-38,70},{-28,51}}, color={160,160,164}),
+        Line(
+          points={{0,0},{-50,50}},
+          thickness=0.5),
+        Line(
+          points={{0,0},{40,0}},
+          thickness=0.5)}), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+  The block counts the number of times the device is turned on
+  in a given time interval by tracking the rising edge of the boolean
+  input signal. If this number is higher than a set value, the block
+  indicates an error.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Renaming according to AixLib guideline (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CycleRateBoundary;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/OnOffFuzzyLogic.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/OnOffFuzzyLogic.mo
new file mode 100644
index 0000000000..591f2bcf91
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/OnOffFuzzyLogic.mo
@@ -0,0 +1,103 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses;
+model OnOffFuzzyLogic
+  "Fuzzy logic approach for on-off control"
+  parameter Real ySetRed
+    "Reduced relative compressor speed to allow longer on-time";
+  Modelica.Blocks.Interfaces.BooleanInput turOn(start=false, fixed=true)
+    "Indicates if device should turn on" annotation (Placement(transformation(
+          extent={{-132,-76},{-100,-44}})));
+  Modelica.Blocks.Interfaces.BooleanInput isAblToTurOn
+    "Indicates if the device can turn on" annotation (Placement(transformation(
+          extent={{-132,-106},{-100,-74}})));
+  Modelica.Blocks.Interfaces.BooleanInput turOff(start=false, fixed=true)
+    "Indicates if the device should turn off" annotation (Placement(
+        transformation(extent={{-132,14},{-100,46}})));
+  Modelica.Blocks.Interfaces.BooleanInput isAblToTurOff
+    "Indicates if the device can turn off"
+    annotation (Placement(transformation(extent={{-132,74},{-100,106}})));
+  Modelica.Blocks.Interfaces.BooleanInput staOff
+    "Indicates if the device has to stay off" annotation (Placement(
+        transformation(extent={{-132,-46},{-100,-14}})));
+  Modelica.Blocks.Interfaces.BooleanInput staOn
+    "Indicates if the device has to stay on" annotation (Placement(transformation(
+          extent={{-132,44},{-100,76}})));
+  Modelica.Blocks.Interfaces.RealOutput yOut
+    "Output for relative compressor speed from 0 to 1"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  Modelica.Blocks.Interfaces.RealInput ySet
+    "Input for relative compressor speed from 0 to 1"
+    annotation (Placement(transformation(extent={{-132,-16},{-100,16}})));
+protected
+  Integer devRunMin(start=0, fixed=true)
+    "Indicates if device needs to run at minimal limit";
+  Integer devTurOff(start=0, fixed=true)
+    "Indicates if device needs to turn off";
+  Integer devNorOpe(start=1, fixed=true)
+    "Indicates if device is at normal operation";
+equation
+  // The part "+ 0 * devTurOff" is implicitly included
+  yOut = ySet * devNorOpe + ySetRed  * devRunMin;
+  when edge(turOn) then
+    if isAblToTurOn then
+      devTurOff = 0;
+      devRunMin = 0;
+      devNorOpe = 1;
+   else
+      devTurOff = 1;
+      devRunMin = 0;
+      devNorOpe = 0;
+    end if;
+  elsewhen edge(turOff) then
+    if isAblToTurOff then
+      devTurOff = 0;
+      devRunMin = 0;
+      devNorOpe = 1;
+    else
+      devTurOff = 0;
+      devRunMin = 1;
+      devNorOpe = 0;
+    end if;
+  elsewhen isAblToTurOn and turOn then
+    devTurOff = 0;
+    devRunMin = 0;
+    devNorOpe = 1;
+  elsewhen isAblToTurOff and turOff then
+    devTurOff = 0;
+    devRunMin = 0;
+    devNorOpe = 1;
+  elsewhen staOff then
+    devTurOff = 0;
+    devRunMin = 0;
+    devNorOpe = 1;
+  elsewhen staOn then
+    devTurOff = 0;
+    devRunMin = 0;
+    devNorOpe = 1;
+  end when;
+
+  annotation (Documentation(info="<html>
+<p>
+The model uses a fuzzy logic approach to avoid the need for a state-machine.
+The device either has to turn off, run at the desired operating speed, or run
+at the minimal speed.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>December 06, 2023</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/1576\">IBPSA #1576</a>)
+  </li>
+</ul>
+</html>"), Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+          Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+                                        Text(
+        extent={{-154,138},{146,98}},
+        textString="%name",
+        textColor={0,0,255})}),                               Diagram(
+        coordinateSystem(preserveAspectRatio=false)), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end OnOffFuzzyLogic;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/OnPastThreshold.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/OnPastThreshold.mo
new file mode 100644
index 0000000000..3781e1a832
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/OnPastThreshold.mo
@@ -0,0 +1,72 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses;
+block OnPastThreshold
+  "Returns true if the device stays on for longer than a threshold time"
+  extends Modelica.Blocks.Interfaces.BooleanSISO;
+
+  parameter Modelica.Units.SI.Time minOnTime
+    "Minimal time the device is turned on or off";
+  Modelica.Blocks.Logical.Timer runTim
+    "Counts the seconds the heat pump is locked still"
+    annotation (Placement(transformation(extent={{-40,-10},{-20,10}})));
+  Modelica.Blocks.Logical.GreaterEqualThreshold runTimGreMin(final threshold=
+        minOnTime) "Checks if the on-time is greater than the minimal on-time"
+    annotation (Placement(transformation(extent={{20,-10},{40,10}})));
+equation
+  connect(runTimGreMin.y, y)
+    annotation (Line(points={{41,0},{110,0}}, color={255,0,255}));
+  connect(u,runTim. u) annotation (
+    Line(points={{-120,0},{-42,0}}, color={255,0,255}));
+  connect(runTim.y, runTimGreMin.u)
+    annotation (Line(points={{-19,0},{18,0}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false),
+    graphics={
+      Rectangle(
+        extent={{-100,-100},{100,100}},
+        lineColor={0,0,127},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),
+        Ellipse(extent={{-80,80},{80,-80}}, lineColor={160,160,164}),
+        Line(points={{0,80},{0,60}}, color={160,160,164}),
+        Line(points={{80,0},{60,0}}, color={160,160,164}),
+        Line(points={{0,-80},{0,-60}}, color={160,160,164}),
+        Line(points={{-80,0},{-60,0}}, color={160,160,164}),
+        Line(points={{37,70},{26,50}}, color={160,160,164}),
+        Line(points={{70,38},{49,26}}, color={160,160,164}),
+        Line(points={{71,-37},{52,-27}}, color={160,160,164}),
+        Line(points={{39,-70},{29,-51}}, color={160,160,164}),
+        Line(points={{-39,-70},{-29,-52}}, color={160,160,164}),
+        Line(points={{-71,-37},{-50,-26}}, color={160,160,164}),
+        Line(points={{-71,37},{-54,28}}, color={160,160,164}),
+        Line(points={{-38,70},{-28,51}}, color={160,160,164}),
+        Line(
+          points={{0,0},{-50,50}},
+          thickness=0.5),
+        Line(
+          points={{0,0},{40,0}},
+          thickness=0.5)}),
+    Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+  This block delays a true signal and only returns true
+  if the device stays on (true) for longer than a threshold time.
+  If the device is switched off before the threshold time,
+  this block continues returning false.
+</p>
+<p>
+  This block is used to check the mimimal on- or off-time of a device.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Renaming according to AixLib guideline (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end OnPastThreshold;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialOperationalEnvelope.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialOperationalEnvelope.mo
new file mode 100644
index 0000000000..4ca2f709d1
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialOperationalEnvelope.mo
@@ -0,0 +1,184 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses;
+partial model PartialOperationalEnvelope
+  "Indicates if the device operation is within a defined envelope"
+  extends BaseClasses.PartialSafetyWithCounter;
+  parameter Modelica.Units.SI.Temperature tabUppHea[:,2]
+    "Upper boundary for heating with second column as useful temperature side";
+  parameter Modelica.Units.SI.Temperature tabLowCoo[:,2]
+    "Lower boundary for cooling with second column as useful temperature side";
+  parameter Boolean use_TConOutHea=true
+    "=true to use condenser outlet temperature for envelope in heating mode, false for inlet"
+    annotation (Dialog(group="Operational Envelope"));
+  parameter Boolean use_TEvaOutHea=false
+    "=true to use evaporator outlet temperature for envelope in heating mode, false for inlet"
+    annotation (Dialog(group="Operational Envelope"));
+  parameter Boolean use_TConOutCoo=false
+    "=true to use useful side outlet temperature for envelope in cooling mode, false for inlet"
+    annotation (Dialog(group="Operational Envelope"));
+  parameter Boolean use_TEvaOutCoo=true
+    "=true to use evaporator outlet temperature for envelope in cooling mode, false for inlet"
+    annotation (Dialog(group="Operational Envelope"));
+
+  parameter Modelica.Units.SI.TemperatureDifference dTHys=5
+    "Temperature deadband in the operational envelope";
+
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.BoundaryMap bouMapHea(
+    final tab=tabUppHea,
+    final dT=dTHys,
+    final isUppBou=true) "Operational boundary map for heating operation"
+    annotation (Placement(transformation(extent={{-80,40},{-20,100}})));
+
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.BoundaryMap bouMapCoo(
+    final tab=tabLowCoo,
+    final dT=dTHys,
+    final isUppBou=false) "Operational boundary map for cooling operation"
+    annotation (Placement(transformation(extent={{-80,-80},{-20,-20}})));
+  Modelica.Blocks.Logical.LogicalSwitch swiHeaCoo
+    "Switch between heating and cooling envelope"
+    annotation (Placement(transformation(extent={{-4,-10},{16,10}})));
+equation
+  connect(ySet,swiErr.u1)  annotation (Line(points={{-136,0},{-80,0},{-80,20},{
+          70,20},{70,8},{78,8}},
+                  color={0,0,127}));
+  connect(swiHeaCoo.y, booPasThr.u)
+    annotation (Line(points={{17,0},{38,0}}, color={255,0,255}));
+  connect(bouMapCoo.noErr, swiHeaCoo.u3)
+    annotation (Line(points={{-17,-50},{-12,-50},{-12,-8},{-6,-8}},
+                                                          color={255,0,255}));
+  connect(bouMapHea.noErr, swiHeaCoo.u1)
+    annotation (Line(points={{-17,70},{-12,70},{-12,8},{-6,8}},
+                                                       color={255,0,255}));
+
+  annotation (Diagram(coordinateSystem(extent={{-120,-120},{120,120}})),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Model to check if the operating conditions are inside
+  the given boundaries. If not, the heat pump or chiller will switch off.
+</p>
+<p>
+  This safety control is mainly based on the operational
+  envelope of the compressor.
+  Refrigerant flowsheet and type will influence these values.
+</p>
+<h4>Limitations</h4>
+
+<ul>
+<li>
+  Only three sides of the real envelope are implemented (Figures 2 and 3).
+  The real operational envelope implies continuous operation.
+  This means start-up from e.g. a cold heat pump supply temperature
+  is possible. To avoid additional equations for startup and
+  continuous operation, we neither implement the
+  lower boundary for heating nor the upper boundary for cooling devices.
+  This avoids the situation where the device can never be turned on.
+</li>
+<li>
+  From all the influences on the real envelope, the compressor frequency
+  impacts the possible range of operation. However, the compressor
+  speed-dependent envelopes are typcially not provided in datasheets.
+  Further, including a third dimension requires 3D-table data. This is
+  currently not supported by AixLib or Modelica Standard Library.
+</li>
+</ul>
+
+<h4>Existing envelopes</h4>
+<p>
+  Technical datasheets often contain
+  information about the operational envelope.
+  The device records for heat pumps
+  (<a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2DData</a>)
+  and chillers
+  (<a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D\">
+  AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2DData</a>)
+  contain typical values. Older devices typically have lower limits
+  while new refrigerant machines based on propane or advanced flowsheets
+  are able to achieve temperature over 70 °C for heating.
+</p>
+<h4>Parameterization from datasheets</h4>
+<p>
+  Depending on the underlying datasheet in use, you have to think
+  thoroughly if you need inlet or outlet conditions, and if
+  you are modelling a heat pump or chiller.
+  Figure 1 depicts possible upper and lower boundaries as well as
+  what variables the boundaries are defined with.
+  Depending on your setup, you may have to transpose existing boundaries.
+  For instance, when using an envelope designed for a
+  heat pump in a chiller model, the useful side (column 2 of the data)
+  is not the condenser but the evaporator. Thus, you have to
+  switch columns 1 and 2.
+  The following examples aim to explain how to obtain the envelopes:
+</p>
+<p>
+  If the model in use is a heat pump,
+  the useful side is always the side of
+  <code>TConOutMea</code> and <code>TConInMea</code>.
+  In the chiller, the useful side is always the side of
+  <code>TEvaOutMea</code> or <code>TEvaInMea</code>.
+</p>
+<ol>
+<li>
+  The envelopes for air-to-water heat pumps
+  often contain water supply temperature (<code>TConOutMea</code>)
+  on the y-axis and ambient temperatures (<code>TEvaInMea</code>)
+  on the x-axis. In these cases, <code>tabUppHea</code> is based
+  on the y-axis maximal values and <code>tabLowCoo</code>
+  based on the y-axis minimal values.
+  Figure 2 depicts this setup.
+</li>
+<li>
+  The envelopes for air-to-air devices often
+  contain ambient inlet (<code>TConInMea</code>) as y and
+  room (<code>TEvaInMea</code>) inlet temperatures as x.
+  In these cases, <code>tabUppHea</code> is based on the x-axis maximal
+  values and tabLowCoo based on the x-axis minimal values.
+  Figure 3 depicts this setup.
+</li>
+<li>
+  Compressor datasheets often provide evaporating and condensing
+  temperatures or pressure levels. Those are not avaiable in the
+  simpified model approach. Thus, you have to assume pinch
+  temperatures to convert it to either in- or outflow temperature
+  levels of the secondary side temperatures
+  (i.e. <code>TConOutMea</code>, <code>TConInMea</code>,
+  <code>TEvaInMea</code>, <code>TEvaOutMea</code>).
+</li>
+</ol>
+
+<p align=\"center\">
+<img  style=\"width: 500\" alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/HeatPumps/ModularReversible/Controls/SafetyControls/OperationalEnvelope_1.png\" border=\"1\"/>
+</p>
+<p align=\"center\">
+  Figure 1: Possible upper and lower boundaries
+  as well as temperature specifications in datasheets
+</p>
+
+<p align=\"center\">
+<img  style=\"width: 500\" alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/HeatPumps/ModularReversible/Controls/SafetyControls/OperationalEnvelope_2.png\" border=\"1\"/>
+</p>
+<p align=\"center\">
+  Figure 2: Example for an air-to-water heat pump or chiller.
+  The supply temperature is the temperature leaving the device
+  into the hydraulic circuit of the building.
+  Red crosses indicate the point to write into the 2D table in Modelica.
+</p>
+
+<p align=\"center\">
+<img  style=\"width: 500\" alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/HeatPumps/ModularReversible/Controls/SafetyControls/OperationalEnvelope_3.png\" border=\"1\"/>
+</p>
+<p align=\"center\">
+  Figure 3: Example for an air-to-air heat pump or chiller.
+  The room temperature acts as an inflow to the device.
+  Red crosses indicate the point to write into the 2D table in Modelica.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialOperationalEnvelope;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialSafety.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialSafety.mo
new file mode 100644
index 0000000000..9dceff5a81
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialSafety.mo
@@ -0,0 +1,73 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses;
+partial model PartialSafety "Safety control with I/O"
+  Modelica.Blocks.Interfaces.RealInput ySet
+    "Input for relative compressor speed from 0 to 1"
+    annotation (Placement(transformation(extent={{-152,-16},{-120,16}}),
+        iconTransformation(extent={{-152,-16},{-120,16}})));
+  Modelica.Blocks.Interfaces.RealOutput yOut
+    "Output for relative compressor speed from 0 to 1"
+    annotation (Placement(transformation(extent={{120,-10},{140,10}}),
+        iconTransformation(extent={{120,-10},{140,10}})));
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantMachineControlBus sigBus
+    "Bus-connector for the heat pump" annotation (Placement(transformation(
+          extent={{-136,-76},{-102,-46}}), iconTransformation(extent={{-136,-88},
+            {-102,-58}})));
+  annotation (Icon(coordinateSystem(extent={{-120,-120},{120,120}}),
+                   graphics={   Rectangle(
+        extent={{-120,-120},{120,120}},
+        lineColor={0,0,127},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),
+        Polygon(
+          points={{-42,20},{0,62},{-42,20}},
+          lineColor={28,108,200},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-48,-26},{48,66}},
+          lineColor={0,0,0},
+          fillColor={91,91,91},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-36,-14},{36,54}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-60,20},{60,-80}},
+          lineColor={0,0,0},
+          fillColor={91,91,91},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-10,-30},{10,-70}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-14,-40},{16,-12}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Text(
+          extent={{-151,139},{149,99}},
+          textColor={0,0,255},
+          fillPattern=FillPattern.HorizontalCylinder,
+          fillColor={0,127,255},
+          textString="%name")}),     Diagram(coordinateSystem(
+          preserveAspectRatio=false, extent={{-120,-120},{120,120}})),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Partial block for a safety control. Based on the signals in the
+  <code>sigBus</code> either the input signals are equal to the output
+  signals or, if an error occurs, set to 0.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialSafety;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialSafetyWithCounter.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialSafetyWithCounter.mo
new file mode 100644
index 0000000000..5e548ae084
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/PartialSafetyWithCounter.mo
@@ -0,0 +1,70 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses;
+partial model PartialSafetyWithCounter
+   "Safety control which adds an error counter to the I/O"
+  extends PartialSafety;
+
+  Modelica.Blocks.Logical.Switch swiErr
+    "Switches to zero when an error occurs"
+    annotation (Placement(transformation(extent={{80,-10},{100,10}})));
+  Modelica.Blocks.Sources.Constant conZer(final k=0)
+    "Constant zero"
+    annotation (Placement(transformation(extent={{40,-40},{60,-20}})));
+  Modelica.Blocks.MathInteger.TriggeredAdd disErr(
+    y_start=0,
+    use_reset=false,
+    use_set=false) "Used to show if the error was triggered"
+                                                         annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={90,-100})));
+  Modelica.Blocks.Interfaces.IntegerOutput err
+    "Integer for displaying number of errors during simulation"
+                                               annotation (Placement(
+        transformation(extent={{-10,-10},{10,10}}, rotation=0,
+        origin={130,-100})));
+  Modelica.Blocks.Logical.Not notVal "=true indicates a error"
+                                     annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={10,-90})));
+  Modelica.Blocks.Sources.IntegerConstant intConOne(final k=1)
+    "Used for display of current error"
+    annotation (Placement(transformation(extent={{10,10},{-10,-10}},
+        rotation=180,
+        origin={48,-100})));
+  Modelica.Blocks.Routing.BooleanPassThrough booPasThr
+    "Used to keep the connection to the counter"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+equation
+  connect(conZer.y,swiErr. u3) annotation (Line(points={{61,-30},{70,-30},{70,
+          -8},{78,-8}},     color={0,0,127}));
+  connect(disErr.y,err)  annotation (Line(points={{102,-100},{130,-100}},
+                                                 color={255,127,0}));
+  connect(notVal.y, disErr.trigger) annotation (Line(points={{21,-90},{28,-90},
+          {28,-118},{84,-118},{84,-112}},
+                                  color={255,0,255}));
+  connect(intConOne.y, disErr.u) annotation (Line(points={{59,-100},{76,-100}},
+                   color={255,127,0}));
+  connect(booPasThr.y, swiErr.u2)
+    annotation (Line(points={{61,0},{78,0}}, color={255,0,255}));
+  connect(booPasThr.y, notVal.u) annotation (Line(points={{61,0},{68,0},{68,-12},
+          {-8,-12},{-8,-90},{-2,-90}},      color={255,0,255}));
+  connect(swiErr.y, yOut) annotation (Line(points={{101,0},{110,0},{110,0},{130,
+          0}},      color={0,0,127}));
+  annotation (Diagram(coordinateSystem(
+          preserveAspectRatio=false, extent={{-120,-120},{120,120}})),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This block counts the number of errors occurred in a specific safety block.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialSafetyWithCounter;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/package.mo
new file mode 100644
index 0000000000..99412cfd5b
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/package.mo
@@ -0,0 +1,33 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety;
+package BaseClasses "Package with base classes for AixLib.Fluid.HeatPump.Controls.Safety"
+
+annotation (Icon(graphics={
+        Rectangle(
+          lineColor={200,200,200},
+          fillColor={248,248,248},
+          fillPattern=FillPattern.HorizontalCylinder,
+          extent={{-100.0,-100.0},{100.0,100.0}},
+          radius=25.0),
+        Rectangle(
+          lineColor={128,128,128},
+          extent={{-100.0,-100.0},{100.0,100.0}},
+          radius=25.0),
+        Ellipse(
+          extent={{-30.0,-30.0},{30.0,30.0}},
+          lineColor={128,128,128},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This package contains base classes that are used to construct the
+  models in <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety</a>
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/package.order
new file mode 100644
index 0000000000..ae99a22fae
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/BaseClasses/package.order
@@ -0,0 +1,7 @@
+BoundaryMap
+CycleRateBoundary
+OnOffFuzzyLogic
+OnPastThreshold
+PartialOperationalEnvelope
+PartialSafety
+PartialSafetyWithCounter
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/Generic.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/Generic.mo
new file mode 100644
index 0000000000..51f1a09537
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/Generic.mo
@@ -0,0 +1,107 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data;
+record Generic "Generic record definition for safety control blocks"
+  extends Modelica.Icons.Record;
+  parameter Boolean use_minOnTime
+    "=false to ignore minimum on-time constraint"
+  annotation (Dialog(group="On/Off Control"), choices(checkBox=true));
+  parameter Modelica.Units.SI.Time minOnTime
+    "Mimimum on-time" annotation (Dialog(group=
+          "On/Off Control", enable=use_minOnTime));
+  parameter Real ySetRed(unit="1")
+    "Reduced relative compressor speed to allow longer on-time"
+        annotation (
+          Dialog(group="On/Off Control",
+          enable=use_minOnTime));
+  parameter Boolean use_minOffTime
+    "=false to ignore minimum off time"
+    annotation (Dialog(group="On/Off Control"),
+    choices(checkBox=true));
+  parameter Modelica.Units.SI.Time minOffTime
+    "Minimum off time" annotation (Dialog(group=
+          "On/Off Control", enable=use_minOffTime));
+  parameter Boolean use_maxCycRat
+    "=false to ignore maximum cycle rate constraint"
+    annotation (Dialog(group="On/Off Control"),
+    choices(checkBox=true));
+  parameter Integer maxCycRat "Maximum cycle rate"
+    annotation (Dialog(group="On/Off Control",
+    enable=use_maxCycRat));
+
+  parameter Boolean onOffMea_start=true
+    "Start value for the on-off signal of the device, true for on"
+    annotation (
+      Dialog(group="On/Off Control"),
+      choices(checkBox=true));
+
+  parameter Boolean use_opeEnv
+    "=true to use a the operational envelope"
+    annotation (
+      Dialog(group="Operational Envelope"),
+      choices(checkBox=true));
+  parameter Modelica.Units.SI.Temperature tabUppHea[:,2]
+    "Upper temperature boundary for heating with second column as useful temperature side"
+    annotation (
+      Dialog(group="Operational Envelope",
+      enable=use_opeEnv));
+  parameter Modelica.Units.SI.Temperature tabLowCoo[:,2]
+    "Lower temperature boundary for cooling with second column as useful temperature side"
+    annotation (
+      Dialog(group="Operational Envelope",
+      enable=use_opeEnv));
+  parameter Modelica.Units.SI.TemperatureDifference dTHysOpeEnv=5
+    "Hysteresis for operational envelopes of both upper and lower boundaries"
+    annotation (Dialog(group="Operational Envelope", enable=use_opeEnv));
+
+  parameter Boolean use_TConOutHea=true
+    "=true to use condenser outlet temperature for envelope in heating mode, false for inlet"
+    annotation (Dialog(group="Operational Envelope", enable=use_opeEnv));
+  parameter Boolean use_TEvaOutHea=false
+    "=true to use evaporator outlet temperature for envelope in heating mode, false for inlet"
+    annotation (Dialog(group="Operational Envelope", enable=use_opeEnv));
+  parameter Boolean use_TConOutCoo=false
+    "=true to use useful side outlet temperature for envelope in cooling mode, false for inlet"
+    annotation (Dialog(group="Operational Envelope", enable=use_opeEnv));
+  parameter Boolean use_TEvaOutCoo=true
+    "=true to use evaporator outlet temperature for envelope in cooling mode, false for inlet"
+    annotation (Dialog(group="Operational Envelope", enable=use_opeEnv));
+  parameter Boolean use_antFre
+    "=true to enable antifreeze control"
+    annotation (Dialog(group="Anti Freeze Control"), choices(checkBox=true));
+  parameter Modelica.Units.SI.ThermodynamicTemperature TAntFre
+    "Limit temperature for antifreeze control"
+    annotation (Dialog(group="Anti Freeze Control", enable=use_antFre));
+  parameter Modelica.Units.SI.TemperatureDifference dTHysAntFre
+    "Hysteresis interval width for antifreeze control"
+    annotation (Dialog(group="Anti Freeze Control", enable=use_antFre));
+  parameter Boolean use_minFlowCtr
+    "=false to disable minimum mass flow rate requirements"
+    annotation (choices(checkBox=true), Dialog(group="Minimal Flow Rates"));
+  parameter Real r_mEvaMinPer_flow
+    "Percentage of mass flow rate in evaporator required to operate the device"
+    annotation (Dialog(group="Minimal Flow Rates", enable=use_minFlowCtr));
+  parameter Real r_mConMinPer_flow
+    "Percentage of mass flow rate in condenser required to operate the device"
+    annotation (Dialog(group="Minimal Flow Rates", enable=use_minFlowCtr));
+    annotation (Icon(graphics, coordinateSystem(preserveAspectRatio=false)),
+     Diagram(graphics, coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+  Base data definitions with parameters relevant
+  to safety control of refrigerant machines.
+</p>
+<p>
+  Typically, datasheets of manufacturers provide
+  specific values for these assumptions. Some values are
+  harder to get, e.g. the minimum and maximum for on-time or off time.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generic;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/Wuellhorst2021.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/Wuellhorst2021.mo
new file mode 100644
index 0000000000..5f875e4f09
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/Wuellhorst2021.mo
@@ -0,0 +1,42 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data;
+record Wuellhorst2021
+  "Apply the default values according to the conference publication by Wuellhorst et al. (2021)"
+  extends Generic(
+    tabLowCoo=[263.15,283.15; 333.15,283.15],
+    dTHysAntFre=2,
+    onOffMea_start=false,
+    ySetRed=0.3,
+    r_mConMinPer_flow=0.1,
+    r_mEvaMinPer_flow=0.1,
+    use_minFlowCtr=true,
+    use_maxCycRat=true,
+    use_minOffTime=true,
+    use_minOnTime=true,
+    TAntFre=273.15,
+    use_antFre=false,
+    dTHysOpeEnv=5,
+    use_opeEnv=true,
+    tabUppHea=[233.15,343.15; 313.15,343.15],
+    maxCycRat=3,
+    minOffTime=1200,
+    minOnTime=600);
+  annotation (Documentation(info="<html>
+<p>
+  Default values according to the conference publication
+  by Wuellhorst et. al. <a href=\"https://doi.org/10.3384/ecp21181561\">
+  https://doi.org/10.3384/ecp21181561</a>.
+</p>
+<p>
+  These values are conservative estimates based on multiple datasheets.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Wuellhorst2021;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/package.mo
new file mode 100644
index 0000000000..00fc3befab
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety;
+package Data "Package with parameters for safety control blocks"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+  Package with record data to bundle the parameterization
+  of the safety controls into one class.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>
+"));
+end Data;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/package.order
new file mode 100644
index 0000000000..c831d0fb8e
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Data/package.order
@@ -0,0 +1,2 @@
+Generic
+Wuellhorst2021
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/AntiFreeze.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/AntiFreeze.mo
new file mode 100644
index 0000000000..921748cb37
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/AntiFreeze.mo
@@ -0,0 +1,80 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples;
+model AntiFreeze "Example for usage of antifreeze model"
+  extends BaseClasses.PartialSafety;
+  extends Modelica.Icons.Example;
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.AntiFreeze antFre
+    "Safety control for antifreeze"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Modelica.Blocks.Sources.Pulse ySetPul(amplitude=1, period=50)
+    "Pulse signal for ySet"
+    annotation (Placement(transformation(extent={{-90,20},{-70,40}})));
+  Modelica.Blocks.Sources.Pulse TConInEmu(
+    amplitude=-10,
+    period=20,
+    offset=283.15,
+    y(unit="K", displayUnit="K"))   "Emulator for condenser inlet temperature"
+    annotation (Placement(transformation(extent={{-90,-20},{-70,0}})));
+  Modelica.Blocks.Sources.Pulse TEvaOutEmu(
+    amplitude=-10,
+    period=15,
+    offset=283.15,
+    y(unit="K", displayUnit="K"))
+                   "Emulator for evaporator outlet temperature"
+    annotation (Placement(transformation(extent={{-90,-60},{-70,-40}})));
+equation
+  connect(antFre.sigBus, sigBus) annotation (Line(
+      points={{0.0833333,3.91667},{-50,3.91667},{-50,-50}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(ySetPul.y, antFre.ySet) annotation (Line(points={{-69,30},{-8,30},{-8,
+          11.6667},{-1.33333,11.6667}},
+                          color={0,0,127}));
+  connect(TEvaOutEmu.y, sigBus.TEvaOutMea) annotation (Line(points={{-69,-50},{
+          -50,-50}},                     color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(TConInEmu.y, sigBus.TConInMea) annotation (Line(points={{-69,-10},{-50,
+          -10},{-50,-50}},     color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(hys.u, antFre.yOut) annotation (Line(points={{22,-50},{44,-50},{44,
+          11.6667},{20.8333,11.6667}},
+                    color={0,0,127}));
+  connect(antFre.yOut, yOut) annotation (Line(points={{20.8333,11.6667},{44,
+          11.6667},{44,-40},{110,-40}},
+                      color={0,0,127}));
+  connect(ySetPul.y, ySet) annotation (Line(points={{-69,30},{-8,30},{-8,40},{110,
+          40}},     color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  This example shows the usage of the model
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.AntiFreeze\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.AntiFreeze</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),
+   __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/AntiFreeze.mos"
+        "Simulate and plot"),
+  experiment(
+      StartTime=0,
+      StopTime=100,
+      Interval=1,
+      Tolerance=1e-08), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end AntiFreeze;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/PartialSafety.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/PartialSafety.mo
new file mode 100644
index 0000000000..a5e8730604
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/PartialSafety.mo
@@ -0,0 +1,44 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples.BaseClasses;
+partial model PartialSafety
+
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantMachineControlBus sigBus
+    "Bus-connector for the heat pump"
+    annotation (Placement(transformation(extent={{-70,-70},{-30,-30}})));
+  Modelica.Blocks.Logical.Hysteresis hys(
+    pre_y_start=false,
+    uHigh=0.01,
+    uLow=0.01/2) "Check if onOffMea in heat pump model would be true"
+                 annotation (Placement(transformation(
+        extent={{-10,10},{10,-10}},
+        rotation=180,
+        origin={10,-50})));
+  Modelica.Blocks.Interfaces.RealOutput ySet
+    "Relative speed of compressor from 0 to 1"
+    annotation (Placement(transformation(extent={{100,30},{120,50}})));
+  Modelica.Blocks.Interfaces.RealOutput yOut
+    "Relative speed of compressor applied after safety control"
+    annotation (Placement(transformation(extent={{100,-50},{120,-30}})));
+equation
+  connect(hys.y, sigBus.onOffMea) annotation (Line(points={{-1,-50},{-50,-50}},
+                           color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Partial example providing interfaces to
+  show usage of safety control models.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialSafety;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/package.mo
new file mode 100644
index 0000000000..fe10e012a2
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/package.mo
@@ -0,0 +1,8 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples;
+package BaseClasses "Package with partial models for examples"
+extends Modelica.Icons.BasesPackage;
+
+annotation (Documentation(info="<html>
+<p>Package with basic models for safety control examples.</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/package.order
new file mode 100644
index 0000000000..a15c64c878
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/BaseClasses/package.order
@@ -0,0 +1 @@
+PartialSafety
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/MinimalFlowRate.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/MinimalFlowRate.mo
new file mode 100644
index 0000000000..091e5d15f6
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/MinimalFlowRate.mo
@@ -0,0 +1,76 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples;
+model MinimalFlowRate
+  "Example for usage of minimal flow rate safety control"
+  extends BaseClasses.PartialSafety;
+  extends Modelica.Icons.Example;
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.MinimalFlowRate minFloRatSaf(
+      mEvaMin_flow=0.1, mConMin_flow=0.1)
+    "Safety block for minimal flow rate safety"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Modelica.Blocks.Sources.Pulse ySetPul(amplitude=1, period=50)
+    "Pulse signal for ySet"
+    annotation (Placement(transformation(extent={{-90,20},{-70,40}})));
+  Modelica.Blocks.Sources.Pulse mConEmu_flow(amplitude=1, period=20)
+    "Emulator for condenser mass flow rate"
+    annotation (Placement(transformation(extent={{-90,-20},{-70,0}})));
+  Modelica.Blocks.Sources.Pulse mEvaEmu_flow(amplitude=1, period=15)
+    "Emulator for evaporator mass flow rate"
+    annotation (Placement(transformation(extent={{-90,-60},{-70,-40}})));
+equation
+  connect(sigBus, minFloRatSaf.sigBus) annotation (Line(
+      points={{-50,-50},{-46,-50},{-46,4},{0.0833333,4},{0.0833333,3.91667}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(minFloRatSaf.yOut, hys.u) annotation (Line(points={{20.8333,10},{46,
+          10},{46,-50},{22,-50}},
+                          color={0,0,127}));
+  connect(ySetPul.y, minFloRatSaf.ySet) annotation (Line(points={{-69,30},{-50,
+          30},{-50,10},{-1.33333,10}},
+                               color={0,0,127}));
+  connect(mConEmu_flow.y, sigBus.mConMea_flow) annotation (Line(points={{-69,-10},
+          {-50,-10},{-50,-50}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(mEvaEmu_flow.y, sigBus.mEvaMea_flow) annotation (Line(points={{-69,-50},
+          {-50,-50}},           color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(minFloRatSaf.yOut, yOut) annotation (Line(points={{20.8333,10},{46,10},
+          {46,-40},{110,-40}},
+                           color={0,0,127}));
+  connect(ySetPul.y, ySet) annotation (Line(points={{-69,30},{26,30},{26,40},{110,
+          40}}, color={0,0,127}));
+  annotation (
+      Documentation(info="<html>
+<p>
+  This example shows the usage of the model
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.MinimalFlowRate\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.MinimalFlowRate</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),
+   __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/MinimalFlowRate.mos"
+        "Simulate and plot"),
+  experiment(
+      StartTime=0,
+      StopTime=100,
+      Interval=1,
+      Tolerance=1e-08), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end MinimalFlowRate;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OnOff.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OnOff.mo
new file mode 100644
index 0000000000..0f4bbbd61c
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OnOff.mo
@@ -0,0 +1,65 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples;
+model OnOff "Example for on off controller"
+  extends BaseClasses.PartialSafety;
+  extends Modelica.Icons.Example;
+
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OnOff onOffCtr(
+    maxCycRat=2,
+    minOffTime(displayUnit="s") = 200,
+    minOnTime(displayUnit="s") = 300,
+    onOffMea_start=false,
+    use_minOffTime=true,
+    use_minOnTime=true,
+    use_maxCycRat=true,
+    ySet_small=hys.uHigh,
+    ySetRed=0.5) "Example case for on off control"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+
+  Modelica.Blocks.Sources.Sine ySetSin(
+    amplitude=0.5,
+    f=1/180,
+    offset=0.5) "Sine signal for ySet"
+    annotation (Placement(transformation(extent={{-90,0},{-70,20}})));
+equation
+  connect(onOffCtr.yOut, hys.u) annotation (Line(points={{20.8333,10},{40,10},{
+          40,-50},{22,-50}},  color={0,0,127}));
+  connect(onOffCtr.sigBus, sigBus) annotation (Line(
+      points={{0.0833333,3.91667},{-50,3.91667},{-50,-50}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%second",
+      index=1,
+      extent={{-3,-6},{-3,-6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(ySetSin.y, onOffCtr.ySet) annotation (Line(points={{-69,10},{-4,10},{
+          -4,10},{-1.33333,10}},
+                             color={0,0,127}));
+  connect(ySetSin.y, ySet) annotation (Line(points={{-69,10},{-56,10},{-56,40},{
+          110,40}},  color={0,0,127}));
+  connect(onOffCtr.yOut, yOut) annotation (Line(points={{20.8333,10},{40,10},{
+          40,-40},{110,-40}},
+                      color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  This example shows the usage of the model
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OnOff\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OnOff</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),
+   __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OnOff.mos"
+        "Simulate and plot"),
+  experiment(
+      StopTime=7200,
+      Interval=1,
+      Tolerance=1e-08), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end OnOff;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OperationalEnvelope.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OperationalEnvelope.mo
new file mode 100644
index 0000000000..267358542f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OperationalEnvelope.mo
@@ -0,0 +1,107 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples;
+model OperationalEnvelope "Example for usage of operational envelope model"
+  extends BaseClasses.PartialSafety;
+  extends Modelica.Icons.Example;
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OperationalEnvelope opeEnv(
+    tabUppHea=[233.15,333.15; 313.15,333.15],
+    tabLowCoo=[233.15,288.15; 313.15,288.15]) "Safety control for operational envelope"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Modelica.Blocks.Sources.Constant
+                                ySetPul(k=1) "Always on"
+    annotation (Placement(transformation(extent={{-90,20},{-70,40}})));
+  Modelica.Blocks.Sources.Trapezoid
+                                TConOutEmu(
+    amplitude=60,
+    rising=5,
+    width=20,
+    falling=5,
+    period=50,
+    offset=283.15,
+    y(unit="K", displayUnit="degC"))
+                   "Emulator for condenser outlet temperature"
+    annotation (Placement(transformation(extent={{-90,-20},{-70,0}})));
+  Modelica.Blocks.Sources.Pulse TEvaInEmu(
+    amplitude=-10,
+    period=15,
+    offset=283.15,
+    y(unit="K", displayUnit="degC"))
+                   "Emulator for evaporator inlet temperature"
+    annotation (Placement(transformation(extent={{-90,-60},{-70,-40}})));
+  Modelica.Blocks.Sources.BooleanStep hea(startTime=50, startValue=true)
+    "Heating mode"
+    annotation (Placement(transformation(extent={{-90,60},{-70,80}})));
+equation
+  connect(opeEnv.sigBus, sigBus) annotation (Line(
+      points={{0.0833333,3.91667},{-50,3.91667},{-50,-52}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(ySetPul.y, opeEnv.ySet) annotation (Line(points={{-69,30},{-8,30},{-8,
+          11.6667},{-1.33333,11.6667}},
+                          color={0,0,127}));
+  connect(hys.u, opeEnv.yOut) annotation (Line(points={{22,-50},{44,-50},{44,
+          11.6667},{20.8333,11.6667}},
+                    color={0,0,127}));
+  connect(opeEnv.yOut, yOut) annotation (Line(points={{20.8333,11.6667},{44,
+          11.6667},{44,-40},{110,-40}},
+                      color={0,0,127}));
+  connect(ySetPul.y, ySet) annotation (Line(points={{-69,30},{-8,30},{-8,40},{110,
+          40}},     color={0,0,127}));
+  connect(TConOutEmu.y, sigBus.TConOutMea) annotation (Line(points={{-69,-10},{
+          -50,-10},{-50,-52}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(TEvaInEmu.y, sigBus.TEvaInMea) annotation (Line(points={{-69,-50},{-52,
+          -50},{-52,-52},{-50,-52}},     color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(hea.y, sigBus.hea) annotation (Line(points={{-69,70},{-50,70},{-50,-52}},
+                 color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(TConOutEmu.y, sigBus.TConInMea) annotation (Line(points={{-69,-10},{-50,
+          -10},{-50,-52}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(TEvaInEmu.y, sigBus.TEvaOutMea) annotation (Line(points={{-69,-50},{-52,
+          -50},{-52,-52},{-50,-52}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  annotation (Documentation(info="<html>
+<p>
+  This example shows the usage of the model
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OperationalEnvelope\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OperationalEnvelope</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),
+   __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OperationalEnvelope.mos"
+        "Simulate and plot"),
+  experiment(
+      StartTime=0,
+      StopTime=100,
+      Interval=1,
+      Tolerance=1e-08), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end OperationalEnvelope;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/Safety.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/Safety.mo
new file mode 100644
index 0000000000..96cc44c4a1
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/Safety.mo
@@ -0,0 +1,148 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples;
+model Safety "Example for usage of all safety controls"
+  extends BaseClasses.PartialSafety;
+  extends Modelica.Icons.Example;
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Safety safCtr(
+    mEva_flow_nominal=0.01,
+    mCon_flow_nominal=0.01,
+    ySet_small=0.01,
+    redeclare AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021
+      safCtrPar(
+      minOnTime=5,
+      minOffTime=5,
+      use_antFre=true,
+      TAntFre=276.15)) "Safety control"
+    annotation (Placement(transformation(extent={{0,0},{20,20}})));
+  Modelica.Blocks.Sources.Pulse ySetPul(amplitude=1, period=50)
+    "Pulse signal for ySet"
+    annotation (Placement(transformation(extent={{-90,30},{-70,50}})));
+  Modelica.Blocks.Sources.Pulse TConInEmu(
+    amplitude=10,
+    period=20,
+    offset=303.15,
+    y(unit="K", displayUnit="degC"))
+                   "Emulator for condenser inlet temperature"
+    annotation (Placement(transformation(extent={{-90,-10},{-70,10}})));
+  Modelica.Blocks.Sources.Pulse TEvaOutEmu(
+    amplitude=-10,
+    period=15,
+    offset=287.15,
+    y(unit="K", displayUnit="degC"))
+                   "Emulator for evaporator outlet temperature"
+    annotation (Placement(transformation(extent={{-90,-50},{-70,-30}})));
+  Modelica.Blocks.Sources.Pulse TConOutEmu(
+    amplitude=40,
+    period=20,
+    offset=313.15,
+    y(unit="K", displayUnit="degC"))
+                   "Emulator for condenser outlet temperature"
+    annotation (Placement(transformation(extent={{-90,-90},{-70,-70}})));
+  Modelica.Blocks.Sources.Pulse TEvaInEmu(
+    amplitude=-10,
+    period=15,
+    offset=288.15,
+    y(unit="K", displayUnit="degC"))
+                   "Emulator for evaporator inlet temperature"
+    annotation (Placement(transformation(extent={{-58,-90},{-38,-70}})));
+  Modelica.Blocks.Sources.Pulse mConEmu_flow(
+    amplitude=1,
+    width=80,
+    period=100) "Emulator for condenser mass flow rate"
+    annotation (Placement(transformation(extent={{22,-90},{42,-70}})));
+  Modelica.Blocks.Sources.Pulse mEvaEmu_flow(amplitude=1, period=100)
+    "Emulator for evaporator mass flow rate"
+    annotation (Placement(transformation(extent={{-18,-90},{2,-70}})));
+  Modelica.Blocks.Sources.BooleanConstant conHea(final k=true)
+    "Constant heating mode" annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-80,80})));
+equation
+  connect(safCtr.sigBus, sigBus) annotation (Line(
+      points={{0.0833333,3.91667},{-50,3.91667},{-50,-50}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(ySetPul.y, safCtr.ySet) annotation (Line(points={{-69,40},{-8,40},{-8,
+          11.6667},{-1.33333,11.6667}},
+                          color={0,0,127}));
+  connect(TEvaOutEmu.y, sigBus.TEvaOutMea) annotation (Line(points={{-69,-40},{
+          -50,-40},{-50,-50}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(TConInEmu.y, sigBus.TConInMea) annotation (Line(points={{-69,0},{-50,0},
+          {-50,-50}},          color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(hys.u, safCtr.yOut) annotation (Line(points={{22,-50},{44,-50},{44,
+          11.6667},{20.8333,11.6667}},
+                    color={0,0,127}));
+  connect(safCtr.yOut, yOut) annotation (Line(points={{20.8333,11.6667},{44,
+          11.6667},{44,-40},{110,-40}},
+                      color={0,0,127}));
+  connect(ySetPul.y, ySet) annotation (Line(points={{-69,40},{110,40}},
+                    color={0,0,127}));
+  connect(TConOutEmu.y, sigBus.TConOutMea) annotation (Line(points={{-69,-80},{
+          -64,-80},{-64,-50},{-50,-50}},                     color={0,0,127}),
+      Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(TEvaInEmu.y, sigBus.TEvaInMea) annotation (Line(points={{-37,-80},{-34,
+          -80},{-34,-50},{-50,-50}},     color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(mEvaEmu_flow.y, sigBus.mEvaMea_flow) annotation (Line(points={{3,-80},{
+          4,-80},{4,-64},{-50,-64},{-50,-50}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(mConEmu_flow.y, sigBus.mConMea_flow) annotation (Line(points={{43,-80},
+          {50,-80},{50,-64},{-50,-64},{-50,-50}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(conHea.y, sigBus.hea) annotation (Line(points={{-69,80},{-50,80},{-50,
+          -50}}, color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  annotation (Documentation(info="<html>
+<p>
+  This example shows the usage and effect of
+  all safety controls aggregates into the model
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Safety\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Safety</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),
+   __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/Safety.mos"
+        "Simulate and plot"),
+  experiment(
+      StartTime=0,
+      StopTime=100,
+      Interval=1,
+      Tolerance=1e-08), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Safety;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/package.mo
new file mode 100644
index 0000000000..18adf3fece
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety;
+package Examples "Examples package"
+  extends Modelica.Icons.ExamplesPackage;
+
+  annotation (Documentation(info="<html>
+<p>
+  Package with examples showing the
+  use of single safety control.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/package.order
new file mode 100644
index 0000000000..fa38642331
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/package.order
@@ -0,0 +1,6 @@
+AntiFreeze
+MinimalFlowRate
+OnOff
+OperationalEnvelope
+Safety
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/MinimalFlowRate.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/MinimalFlowRate.mo
new file mode 100644
index 0000000000..486695e9fa
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/MinimalFlowRate.mo
@@ -0,0 +1,68 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety;
+model MinimalFlowRate "Safety control for minimum mass flow rate"
+  extends BaseClasses.PartialSafetyWithCounter;
+
+  parameter Modelica.Units.SI.MassFlowRate mEvaMin_flow
+    "Minimal mass flow rate in evaporator required to operate the device";
+  parameter Modelica.Units.SI.MassFlowRate mConMin_flow
+    "Minimal mass flow rate in condenser required to operate the device";
+  Modelica.Blocks.Logical.Hysteresis hysCon(
+    final uLow=mConMin_flow,
+    final uHigh=max(mConMin_flow*1.1, Modelica.Constants.eps),
+    final pre_y_start=false)
+    "Check if condenser mass flow rate is high enough"
+    annotation (Placement(transformation(extent={{-60,10},{-40,30}})));
+  Modelica.Blocks.Logical.Hysteresis hysEva(
+    final uLow=mEvaMin_flow,
+    final uHigh=max(mEvaMin_flow*1.1, Modelica.Constants.eps),
+    final pre_y_start=false)
+    "Check if evaporator mass flow rate is high enough"
+    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
+  Modelica.Blocks.Logical.And and1
+    "Both condenser and evaporator have sufficient flow"
+    annotation (Placement(transformation(extent={{-20,-10},{0,10}})));
+
+equation
+  connect(hysCon.y, and1.u1) annotation (Line(points={{-39,20},{-28,20},{-28,0},
+          {-22,0}},      color={255,0,255}));
+  connect(hysEva.y, and1.u2) annotation (Line(points={{-39,-20},{-30,-20},{-30,-8},
+          {-22,-8}},     color={255,0,255}));
+  connect(and1.y, booPasThr.u) annotation (Line(points={{1,0},{38,0}},
+             color={255,0,255}));
+  connect(hysEva.u, sigBus.mEvaMea_flow) annotation (Line(points={{-62,-20},{
+          -84,-20},{-84,-61},{-119,-61}},
+                                     color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(hysCon.u, sigBus.mConMea_flow) annotation (Line(points={{-62,20},{-94,
+          20},{-94,-52},{-119,-52},{-119,-61}},
+                                     color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(ySet, swiErr.u1) annotation (Line(points={{-136,0},{-100,0},{-100,40},
+          {68,40},{68,8},{78,8}}, color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  Safety control to prevent the device from turning on
+  if the mass flow rate is too low in either
+  condenser or evaporator.
+</p>
+<p>
+  Used in real devices to prevent overheating
+  or freezing of components.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end MinimalFlowRate;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/OnOff.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/OnOff.mo
new file mode 100644
index 0000000000..5be5ce4687
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/OnOff.mo
@@ -0,0 +1,215 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety;
+model OnOff
+  "Controlls if the Safety constraints for on-time, off-time, and cycle rate"
+  extends BaseClasses.PartialSafety;
+  parameter Boolean use_minOnTime=true
+    "=false to ignore minimum on-time constraint"
+    annotation(choices(checkBox=true));
+  parameter Modelica.Units.SI.Time minOnTime(displayUnit="min")
+    "Minimum on-time"
+    annotation (Dialog(enable=use_minOnTime));
+  parameter Boolean use_minOffTime=true
+    "=false to ignore minimum off time constraint"
+    annotation(choices(checkBox=true));
+  parameter Modelica.Units.SI.Time minOffTime(displayUnit="min")
+    "Minimum off time"
+     annotation (Dialog(enable=use_minOffTime));
+  parameter Boolean use_maxCycRat=true
+    "=false to ignore maximal cycle rate constraint"
+    annotation(choices(checkBox=true));
+  parameter Integer maxCycRat "Maximum cycle rate"
+    annotation (Dialog(enable=use_maxCycRat));
+  parameter Boolean onOffMea_start=true
+    "Start value for the on-off signal of the device, true for on";
+  parameter Real ySet_small
+    "Threshold for relative speed for the device to be considered on";
+  parameter Real ySetRed=ySet_small
+    "Reduced relative compressor speed to allow longer on-time";
+  Modelica.Blocks.Logical.Hysteresis ySetOn(
+    final pre_y_start=onOffMea_start,
+    final uHigh=ySet_small,
+    final uLow=ySet_small/2) "=true if device is set on"
+    annotation (Placement(transformation(extent={{-100,60},{-80,80}})));
+  Modelica.Blocks.Routing.BooleanPassThrough isAblToTurOff(
+    y(start=true, fixed=true))
+    "=true if the device is allowed to turn off, else false"
+    annotation (Placement(transformation(extent={{40,80},{60,100}})));
+  Modelica.Blocks.Logical.Pre preOnOff(final pre_u_start=onOffMea_start)
+    "On off signal of previous time step"
+    annotation (Placement(transformation(extent={{-100,-100},{-80,-80}})));
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.CycleRateBoundary
+    cycRatBou(final maxCycRat=maxCycRat, final delTim=3600) if use_maxCycRat
+    "Check cycle rate violations"
+    annotation (Placement(transformation(extent={{0,-60},{20,-40}})));
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.OnPastThreshold locTimCtr(
+   final minOnTime=minOffTime) if use_minOffTime
+    "Check if device should be locked"
+    annotation (Placement(transformation(extent={{0,10},{20,30}})));
+  Modelica.Blocks.Logical.Not notIsOn "=true if device is off"
+    annotation (Placement(transformation(extent={{-100,-60},{-80,-40}})));
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.OnPastThreshold runTimCtr(
+      final minOnTime=minOnTime) if use_minOnTime "Check if device needs to run"
+    annotation (Placement(transformation(extent={{0,90},{20,110}})));
+  Modelica.Blocks.Logical.And andIsAblToTurOn(
+    y(start=true, fixed=true))
+    "=false to lock the device off"
+    annotation (Placement(transformation(extent={{50,-70},{70,-50}})));
+
+  Modelica.Blocks.Sources.BooleanConstant booConstCycRat(final k=true)
+    if not use_maxCycRat "Constant value for disabled option"
+    annotation (Placement(transformation(extent={{0,-100},{20,-80}})));
+  Modelica.Blocks.Sources.BooleanConstant booConstLocTim(final k=true)
+    if not use_minOffTime "Constant value for disabled option"
+    annotation (Placement(transformation(extent={{0,-20},{20,0}})));
+  Modelica.Blocks.Sources.BooleanConstant booConstRunTim(final k=true)
+    if not use_minOnTime "Constant value for disabled option"
+    annotation (Placement(transformation(extent={{0,60},{20,80}})));
+  Modelica.Blocks.Logical.Not notSetOn "Device is not set to turn on"
+    annotation (Placement(transformation(extent={{-100,18},{-80,38}})));
+  Modelica.Blocks.Logical.And andTurOff
+    "Check if device is on and is set to be turned off"
+    annotation (Placement(transformation(extent={{-40,0},{-20,20}})));
+  Modelica.Blocks.Logical.And andTurOn
+    "Check if device is off and is set to be turned on"
+    annotation (Placement(transformation(extent={{-40,-100},{-20,-80}})));
+
+  Modelica.Blocks.Logical.And andStaOn
+    "=true if the device is on and wants to stay on"
+    annotation (Placement(transformation(extent={{-40,40},{-20,60}})));
+  Modelica.Blocks.Logical.And andStaOff
+    "=true if the device is off and wants to stay off"
+    annotation (Placement(transformation(extent={{-40,-40},{-20,-20}})));
+
+  BaseClasses.OnOffFuzzyLogic onOffFuzLog(ySetRed=ySetRed)
+    "Fuzzy logic to device for output"
+    annotation (Placement(transformation(extent={{74,-20},{114,20}})));
+equation
+  connect(preOnOff.y, cycRatBou.u) annotation (Line(points={{-79,-90},{-66,-90},{-66,
+          -50},{-2,-50}},                     color={255,0,255}));
+  connect(preOnOff.y, notIsOn.u) annotation (Line(points={{-79,-90},{-66,-90},{-66,
+          -66},{-108,-66},{-108,-50},{-102,-50}},     color={255,0,255}));
+  connect(notIsOn.y, locTimCtr.u) annotation (Line(points={{-79,-50},{-52,-50},{-52,
+          -30},{-48,-30},{-48,-4},{-8,-4},{-8,20},{-2,20}},
+                                color={255,0,255}));
+  connect(runTimCtr.u, preOnOff.y) annotation (Line(points={{-2,100},{-66,100},{
+          -66,-90},{-79,-90}}, color={255,0,255}));
+  connect(locTimCtr.y, andIsAblToTurOn.u1) annotation (Line(
+      points={{21,20},{26,20},{26,-10},{36,-10},{36,-60},{48,-60}},
+      color={255,0,255},
+      pattern=LinePattern.Dash));
+  connect(cycRatBou.y, andIsAblToTurOn.u2) annotation (Line(
+      points={{21,-50},{30,-50},{30,-68},{48,-68}},
+      color={255,0,255},
+      pattern=LinePattern.Dash));
+  connect(booConstCycRat.y, andIsAblToTurOn.u2) annotation (Line(
+      points={{21,-90},{32,-90},{32,-68},{48,-68}},
+      color={255,0,255},
+      pattern=LinePattern.Dash));
+
+  connect(ySetOn.y, notSetOn.u) annotation (Line(points={{-79,70},{-74,70},{-74,
+          52},{-110,52},{-110,28},{-102,28}},
+                         color={255,0,255}));
+  connect(notSetOn.y, andTurOff.u2) annotation (Line(points={{-79,28},{-70,28},{
+          -70,2},{-42,2}},    color={255,0,255}));
+  connect(preOnOff.y, andTurOff.u1) annotation (Line(points={{-79,-90},{-66,-90},
+          {-66,10},{-42,10}},                   color={255,0,255}));
+  connect(ySetOn.y, andTurOn.u2) annotation (Line(points={{-79,70},{-74,70},{-74,
+          -98},{-42,-98}},                       color={255,0,255}));
+  connect(notIsOn.y, andTurOn.u1) annotation (Line(points={{-79,-50},{-52,-50},{
+          -52,-90},{-42,-90}},                      color={255,0,255}));
+  connect(booConstLocTim.y, andIsAblToTurOn.u1) annotation (Line(
+      points={{21,-10},{36,-10},{36,-60},{48,-60}},
+      color={255,0,255},
+      pattern=LinePattern.Dash));
+
+  connect(preOnOff.u, sigBus.onOffMea) annotation (Line(points={{-102,-90},{
+          -108,-90},{-108,-61},{-119,-61}},
+                                       color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(ySetOn.u, ySet) annotation (Line(points={{-102,70},{-114,70},{-114,0},
+          {-136,0}},  color={0,0,127}));
+  connect(andStaOn.u1, ySetOn.y) annotation (Line(points={{-42,50},{-58,50},{-58,
+          52},{-74,52},{-74,70},{-79,70}},
+                         color={255,0,255}));
+  connect(andStaOn.u2, preOnOff.y) annotation (Line(points={{-42,42},{-66,42},{-66,
+          -90},{-79,-90}},                   color={255,0,255}));
+  connect(andStaOff.u1, notIsOn.y) annotation (Line(points={{-42,-30},{-52,-30},
+          {-52,-50},{-79,-50}}, color={255,0,255}));
+  connect(andStaOff.u2, notSetOn.y) annotation (Line(points={{-42,-38},{-70,-38},
+          {-70,28},{-79,28}}, color={255,0,255}));
+  connect(isAblToTurOff.u, runTimCtr.y) annotation (Line(points={{38,90},{28,90},
+          {28,100},{21,100}}, color={255,0,255}));
+  connect(booConstRunTim.y, isAblToTurOff.u) annotation (Line(points={{21,70},{28,
+          70},{28,90},{38,90}}, color={255,0,255}));
+  connect(onOffFuzLog.yOut, yOut)
+    annotation (Line(points={{116,0},{130,0}},   color={0,0,127}));
+  connect(onOffFuzLog.ySet, ySet) annotation (Line(points={{70.8,0},{56,0},{56,
+          36},{-58,36},{-58,6},{-114,6},{-114,0},{-136,0}},
+                                        color={0,0,127}));
+  connect(onOffFuzLog.staOff, andStaOff.y) annotation (Line(points={{70.8,-6},{
+          36,-6},{36,-30},{-19,-30}},
+                                   color={255,0,255}));
+  connect(onOffFuzLog.staOn, andStaOn.y) annotation (Line(points={{70.8,12},{42,
+          12},{42,50},{-19,50}},
+                             color={255,0,255}));
+  connect(onOffFuzLog.isAblToTurOff, isAblToTurOff.y) annotation (Line(points={{70.8,18},
+          {64,18},{64,90},{61,90}},     color={255,0,255}));
+  connect(andIsAblToTurOn.y, onOffFuzLog.isAblToTurOn) annotation (Line(points={{71,-60},
+          {80,-60},{80,-40},{54,-40},{54,-18},{70.8,-18}},  color={255,0,255}));
+  connect(onOffFuzLog.turOff, andTurOff.y) annotation (Line(points={{70.8,6},{
+          32,6},{32,40},{-12,40},{-12,10},{-19,10}},
+                                                   color={255,0,255}));
+  connect(onOffFuzLog.turOn, andTurOn.y) annotation (Line(points={{70.8,-12},{
+          34,-12},{34,-70},{-6,-70},{-6,-90},{-19,-90}},
+                                                   color={255,0,255}));
+  annotation (Documentation(info="<html>
+<p>
+  Checks if the <code>ySet</code> value is legal by checking if
+  the device can either be turned on or off,
+  depending on which state it was in. </p>
+<p>The output <code>yOut</code> equals <code>ySet</code>, if the device</p>
+<ul>
+<li>
+  is on and <code>ySet</code> is greater
+  than <code>ySet_small</code></li>
+<li>
+  or is off and <code>ySet</code> is 0
+</li>
+<li>
+  or is on and should turn off,
+  and exceeds the minimal on-time (if active)</li>
+<li>
+  or is off and should turn on, and does neither
+  exceed the maximal cycle rate (if active)
+  nor violates the minimal off-time (if active).
+</li>
+</ul>
+<p>
+  If the device is on and should turn off, but does not exceed
+  the minimal on-time (if active), <code>yOut</code>
+  equals <code>min(ySet, ySetMin)</code>.
+</p>
+<p>
+  If the device is off and should turn on, but exceeds the maximal
+  cycle rate (if active) or violates the minimal
+  off-time (if active), <code>yOut</code> equals 0.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on the discussion in this issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-120,-120},{120,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end OnOff;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/OperationalEnvelope.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/OperationalEnvelope.mo
new file mode 100644
index 0000000000..c7ebd71009
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/OperationalEnvelope.mo
@@ -0,0 +1,71 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety;
+model OperationalEnvelope
+  "Indicates if the heat pump operation is within a defined envelope"
+  extends BaseClasses.PartialOperationalEnvelope;
+equation
+  if use_TConOutHea then
+    connect(bouMapHea.TUseSid, sigBus.TConOutMea) annotation (Line(points={{-84.2,
+            82},{-104,82},{-104,-61},{-119,-61}},                       color={0,
+            0,127}));
+  else
+    connect(bouMapHea.TUseSid, sigBus.TConInMea) annotation (Line(points={{-84.2,
+            82},{-104,82},{-104,-61},{-119,-61}},                       color={0,
+            0,127}));
+  end if;
+  if use_TEvaOutCoo then
+    connect(bouMapCoo.TAmbSid, sigBus.TEvaOutMea) annotation (Line(points={{-84.8,
+            -62},{-104,-62},{-104,-61},{-119,-61}},
+                                                color={0,0,127}));
+  else
+    connect(bouMapCoo.TAmbSid, sigBus.TEvaInMea) annotation (Line(points={{-84.8,
+            -62},{-104,-62},{-104,-61},{-119,-61}},
+                                                color={0,0,127}));
+  end if;
+  if use_TEvaOutHea then
+    connect(bouMapHea.TAmbSid, sigBus.TEvaOutMea) annotation (Line(points={{-84.8,
+            58},{-104,58},{-104,-60},{-106,-60},{-106,-61},{-119,-61}},
+                                                color={0,0,127}));
+  else
+    connect(bouMapHea.TAmbSid, sigBus.TEvaInMea) annotation (Line(points={{-84.8,
+            58},{-104,58},{-104,-60},{-112,-60},{-112,-61},{-119,-61}},
+                                                color={0,0,127}));
+  end if;
+  if use_TConOutCoo then
+    connect(bouMapCoo.TUseSid, sigBus.TConOutMea) annotation (Line(points={{-84.2,
+            -38},{-104,-38},{-104,-60},{-112,-60},{-112,-61},{-119,-61}},
+                                                      color={0,0,127}));
+  else
+    connect(bouMapCoo.TUseSid, sigBus.TConInMea) annotation (Line(points={{-84.2,
+            -38},{-104,-38},{-104,-60},{-112,-60},{-112,-61},{-119,-61}},
+                                                      color={0,0,127}));
+  end if;
+  connect(swiHeaCoo.u2, sigBus.hea) annotation (Line(points={{-6,0},{-20,0},{
+          -20,-4},{-104,-4},{-104,-60},{-112,-60},{-112,-61},{-119,-61}},
+                            color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  annotation (Diagram(coordinateSystem(extent={{-120,-120},{120,120}})),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Model to check if the operating conditions of a heat pump are inside
+  the given boundaries. If not, the heat pump or chiller will switch off.
+</p>
+<p>
+  Read the documentation of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.PartialOperationalEnvelope\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.PartialOperationalEnvelope</a>
+  for more information.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end OperationalEnvelope;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Safety.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Safety.mo
new file mode 100644
index 0000000000..87d5277c83
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/Safety.mo
@@ -0,0 +1,239 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety;
+model Safety "Model including all safety levels"
+  extends BaseClasses.PartialSafety;
+  parameter Modelica.Units.SI.MassFlowRate mEva_flow_nominal
+    "Nominal mass flow rate in evaporator medium"
+    annotation (Dialog(group="Mass flow rates"));
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_nominal
+    "Nominal mass flow rate in condenser medium"
+    annotation (Dialog(group="Mass flow rates"));
+  parameter Real ySet_small
+    "Threshold for relative speed for the device to be considered on";
+
+  replaceable parameter AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Generic
+    safCtrPar constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Generic
+    "Safety control parameters" annotation (choicesAllMatching=true, Placement(
+        transformation(extent={{-106,92},{-92,108}})));
+  replaceable
+    AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OperationalEnvelope
+    opeEnv if safCtrPar.use_opeEnv constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.PartialOperationalEnvelope(
+      final use_TConOutHea=safCtrPar.use_TConOutHea,
+      final use_TEvaOutHea=safCtrPar.use_TEvaOutHea,
+      final use_TConOutCoo=safCtrPar.use_TConOutCoo,
+      final use_TEvaOutCoo=safCtrPar.use_TEvaOutCoo,
+      final tabUppHea=safCtrPar.tabUppHea,
+      final tabLowCoo=safCtrPar.tabLowCoo,
+      final dTHys=safCtrPar.dTHysOpeEnv) "Block for operational envelope"
+    annotation (Placement(transformation(extent={{-20,20},{0,40}})),
+      choicesAllMatching=true);
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OnOff onOffCtr(
+    final minOnTime=safCtrPar.minOnTime,
+    final minOffTime=safCtrPar.minOffTime,
+    final use_minOnTime=safCtrPar.use_minOnTime,
+    final use_minOffTime=safCtrPar.use_minOffTime,
+    final use_maxCycRat=safCtrPar.use_maxCycRat,
+    final maxCycRat=safCtrPar.maxCycRat,
+    final onOffMea_start=safCtrPar.onOffMea_start,
+    final ySet_small=ySet_small,
+    final ySetRed=safCtrPar.ySetRed) if safCtrPar.use_minOnTime or safCtrPar.use_minOffTime
+     or safCtrPar.use_maxCycRat "On off control block"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.AntiFreeze antFre(final TAntFre=
+        safCtrPar.TAntFre, final dTHys=safCtrPar.dTHysAntFre)
+    if safCtrPar.use_antFre "Antifreeze control"
+    annotation (Placement(transformation(extent={{20,20},{40,40}})));
+  Modelica.Blocks.Interfaces.IntegerOutput opeEnvErr if safCtrPar.use_opeEnv
+    "Number of errors from violating the operational envelope"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-10,-130})));
+  Modelica.Blocks.Interfaces.IntegerOutput antFreErr if safCtrPar.use_antFre
+    "Number of errors from antifreeze control"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={30,-130})));
+
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.MinimalFlowRate
+    minVolFloRatSaf(final mEvaMin_flow=safCtrPar.r_mEvaMinPer_flow*
+        mEva_flow_nominal, final mConMin_flow=safCtrPar.r_mConMinPer_flow*
+        mCon_flow_nominal) if safCtrPar.use_minFlowCtr
+    "Block to ensure minimal flow rates"
+    annotation (Placement(transformation(extent={{60,20},{80,40}})));
+
+  Modelica.Blocks.Interfaces.IntegerOutput minFlowErr
+    if safCtrPar.use_minFlowCtr
+    "Number of errors from violating minimum flow rates"
+    annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={70,-130})));
+  Modelica.Blocks.Routing.RealPassThrough reaPasThrOnOff if not (safCtrPar.use_minOnTime
+     or safCtrPar.use_minOffTime or safCtrPar.use_maxCycRat)
+    "No on off control" annotation (
+                         choicesAllMatching=true, Placement(transformation(
+          extent={{-60,60},{-40,80}})));
+  Modelica.Blocks.Routing.RealPassThrough reaPasThrOpeEnv
+    if not safCtrPar.use_opeEnv "No operational envelope control"  annotation (
+                                                           choicesAllMatching=true,
+      Placement(transformation(extent={{-20,60},{0,80}})));
+  Modelica.Blocks.Routing.RealPassThrough reaPasThrAntFre
+    if not safCtrPar.use_antFre "No antifreeze control"  annotation (
+                                                   choicesAllMatching=true,
+      Placement(transformation(extent={{20,60},{40,80}})));
+  Modelica.Blocks.Routing.RealPassThrough reaPasThrMinVolRat
+    if not safCtrPar.use_minFlowCtr  "No minimum flow rate control"
+    annotation (
+      choicesAllMatching=true, Placement(transformation(extent={{60,60},{80,80}})));
+equation
+
+  connect(sigBus, onOffCtr.sigBus) annotation (Line(
+      points={{-119,-61},{-112,-61},{-112,-10},{-66,-10},{-66,23.9167},{-59.9167,
+          23.9167}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-3,-6},{-3,-6}},
+      horizontalAlignment=TextAlignment.Right));
+
+  connect(sigBus, opeEnv.sigBus) annotation (Line(
+      points={{-119,-61},{-112,-61},{-112,-10},{-28,-10},{-28,23.9167},{-19.9167,
+          23.9167}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-3,-6},{-3,-6}},
+      horizontalAlignment=TextAlignment.Right));
+
+  connect(sigBus, antFre.sigBus) annotation (Line(
+      points={{-119,-61},{-112,-61},{-112,-10},{14,-10},{14,23.9167},{20.0833,
+          23.9167}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+
+  connect(antFre.err, antFreErr) annotation (Line(points={{40.8333,21.6667},{
+          40.8333,22},{46,22},{46,-54},{30,-54},{30,-130}},
+                                    color={255,127,0}));
+  connect(opeEnv.err, opeEnvErr) annotation (Line(points={{0.833333,21.6667},{
+          0.833333,22},{6,22},{6,-54},{-10,-54},{-10,-130}},
+                                      color={255,127,0}));
+  connect(minVolFloRatSaf.yOut, yOut) annotation (Line(
+      points={{80.8333,30},{92,30},{92,0},{130,0}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(sigBus, minVolFloRatSaf.sigBus) annotation (Line(
+      points={{-119,-61},{-112,-61},{-112,-10},{56,-10},{56,23.9167},{60.0833,
+          23.9167}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+
+  connect(minVolFloRatSaf.err, minFlowErr) annotation (Line(points={{80.8333,
+          21.6667},{80.8333,22},{84,22},{84,-54},{70,-54},{70,-130}},
+                                             color={255,127,0}));
+  connect(reaPasThrOnOff.y, reaPasThrOpeEnv.u)
+    annotation (Line(points={{-39,70},{-22,70}}, color={0,0,127}));
+  connect(reaPasThrOpeEnv.y, reaPasThrAntFre.u)
+    annotation (Line(points={{1,70},{18,70}}, color={0,0,127}));
+  connect(reaPasThrAntFre.y, reaPasThrMinVolRat.u)
+    annotation (Line(points={{41,70},{58,70}}, color={0,0,127}));
+  connect(reaPasThrMinVolRat.y, yOut) annotation (Line(
+      points={{81,70},{92,70},{92,0},{130,0}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(onOffCtr.yOut, opeEnv.ySet) annotation (Line(points={{-39.1667,30},{
+          -21.3333,30}},                          color={0,0,127}));
+  connect(opeEnv.yOut, antFre.ySet) annotation (Line(points={{0.833333,30},{
+          18.6667,30}},                                               color={0,0,
+          127}));
+  connect(antFre.yOut, minVolFloRatSaf.ySet) annotation (Line(points={{40.8333,30},
+          {58.6667,30}},                                                color={0,
+          0,127}));
+  connect(antFre.yOut, reaPasThrMinVolRat.u) annotation (Line(
+      points={{40.8333,30},{40.8333,30},{52,30},{52,70},{58,70}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(reaPasThrAntFre.y, minVolFloRatSaf.ySet) annotation (Line(
+      points={{41,70},{52,70},{52,30},{58.6667,30}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(opeEnv.yOut, reaPasThrAntFre.u) annotation (Line(
+      points={{0.833333,30},{12,30},{12,70},{18,70}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(reaPasThrOpeEnv.y, antFre.ySet) annotation (Line(
+      points={{1,70},{12,70},{12,30},{18.6667,30}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(onOffCtr.yOut, reaPasThrOpeEnv.u) annotation (Line(
+      points={{-39.1667,30},{-39.1667,30},{-32,30},{-32,70},{-22,70}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(reaPasThrOnOff.y, opeEnv.ySet) annotation (Line(
+      points={{-39,70},{-32,70},{-32,30},{-21.3333,30}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+
+  connect(ySet, onOffCtr.ySet) annotation (Line(
+      points={{-136,0},{-80,0},{-80,30},{-61.3333,30}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  connect(ySet, reaPasThrOnOff.u) annotation (Line(
+      points={{-136,0},{-80,0},{-80,70},{-62,70}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  annotation (Documentation(revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on the discussion in this issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Aggregation of the four main safety controls
+  of a refrigerant machine (heat pump or chiller).
+</p>
+<p>
+  The order is based on the relevance to a real system.
+  Antifreeze control and mininmum flow rate control are put
+  last because of the relevance for the simulation.
+  If the medium temperature falls below or rises above the
+  critical values, the simulation will fail.
+</p>
+<p>
+All used functions are optional. See the used models for more
+information on each safety function:
+</p>
+<ul>
+<li><a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OnOff\">
+AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OnOff</a> </li>
+<li><a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OperationalEnvelope\">
+AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.OperationalEnvelope</a> </li>
+<li><a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.AntiFreeze\">
+AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.AntiFreeze</a> </li>
+<li><a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.MinimalFlowRate\">
+AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.MinimalFlowRate</a> </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Safety;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/package.mo
new file mode 100644
index 0000000000..ced91ec35d
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/package.mo
@@ -0,0 +1,36 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Controls;
+package Safety "Contains typical safety controllers for heat pumps"
+  extends Modelica.Icons.Package;
+
+  annotation (Icon(graphics={
+        Ellipse(
+          extent={{-48,-12},{48,80}},
+          lineColor={0,0,0},
+          fillColor={91,91,91},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-36,0},{36,68}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-60,34},{60,-66}},
+          lineColor={0,0,0},
+          fillColor={91,91,91},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-10,-16},{10,-56}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-14,-26},{16,2}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Documentation(info="<html>
+<p>
+  Package with safety controls typically
+  applied in heat pumps and chiller devices.
+</p>
+</html>"));
+end Safety;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/package.order
new file mode 100644
index 0000000000..d22b818d75
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/Safety/package.order
@@ -0,0 +1,8 @@
+AntiFreeze
+MinimalFlowRate
+OnOff
+OperationalEnvelope
+Safety
+Data
+Examples
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/package.mo
new file mode 100644
index 0000000000..4ed58445f0
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/package.mo
@@ -0,0 +1,38 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+package Controls "Package of control sequences"
+  extends Modelica.Icons.Package;
+
+  annotation (
+    preferredView="info",
+    Documentation(
+      info="<html>
+<p>
+This package contains control logic for the heat pump internal controls.
+</p>
+</html>"),
+Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100.0,-100.0},{100.0,100.0}}), graphics={
+      Rectangle(
+        origin={0.0,35.1488},
+        fillColor={255,255,255},
+        extent={{-30.0,-20.1488},{30.0,20.1488}}),
+      Rectangle(
+        origin={0.0,-34.8512},
+        fillColor={255,255,255},
+        extent={{-30.0,-20.1488},{30.0,20.1488}}),
+      Line(
+        origin={-51.25,0.0},
+        points={{21.25,-35.0},{-13.75,-35.0},{-13.75,35.0},{6.25,35.0}}),
+      Polygon(
+        origin={-40.0,35.0},
+        pattern=LinePattern.None,
+        fillPattern=FillPattern.Solid,
+        points={{10.0,0.0},{-5.0,5.0},{-5.0,-5.0}}),
+      Line(
+        origin={51.25,0.0},
+        points={{-21.25,35.0},{13.75,35.0},{13.75,-35.0},{-6.25,-35.0}}),
+      Polygon(
+        origin={40.0,-35.0},
+        pattern=LinePattern.None,
+        fillPattern=FillPattern.Solid,
+        points={{-10.0,0.0},{5.0,5.0},{5.0,-5.0}})}));
+end Controls;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Controls/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/package.order
new file mode 100644
index 0000000000..64ee735bc3
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Controls/package.order
@@ -0,0 +1 @@
+Safety
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/SingleSplitRXM20R.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/SingleSplitRXM20R.mo
new file mode 100644
index 0000000000..58a39bcc94
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/SingleSplitRXM20R.mo
@@ -0,0 +1,58 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.EN14511;
+record SingleSplitRXM20R "Daikin_FTXM20R_RXM20R heating mode"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.GenericHeatPump(
+    use_TConOutForOpeEnv=true,
+    use_TEvaOutForOpeEnv=false,
+    dpEva_nominal=0,
+    dpCon_nominal=0,
+    tabQCon_flow=[0,258.15, 263.15, 268.15, 273.15, 280.15, 283.15;
+      288.15,1190,1430,1670,1940,2590,2810;
+      293.15,1120,1360,1600, 1860,2500,2730;
+      295.15,1090,1330,1570,1830,2470,2690;
+      297.15,1060,1300,1540,1800,2430,2660;
+      298.15,1040,1280,1520,1780,2410,2640;
+      300.15,1010,1250,1490,1760,2380,2610],
+    tabPEle=[0,258.15, 263.15, 268.15, 273.15, 280.15, 283.15;
+      288.15,320,340,360,460,490,510;
+      293.15,330,350,370,470,500,520;
+      295.15,340,360,370,480,500,520;
+      297.15,340,360,380,480,510,530;
+      298.15,340, 360,380,490,510,530;
+      300.15,350,370,380,490,520,540],
+    mCon_flow_nominal=(9.33*1.2)/60,
+    mEva_flow_nominal=(28.3*1.2)/60,
+    tabUppBou=[253.15,303.15; 291.15,303.15],
+    devIde="DaikinRXM20R",
+    use_TConOutForTab=false,
+    use_TEvaOutForTab=false);
+
+  annotation (
+    Icon(coordinateSystem(preserveAspectRatio=false)),
+    Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+  Performance data for Daikin FTXM20R_RXM20R for the heating mode.
+</p>
+<p>
+  Boundaries are for dry-bulb temperature. Pressure drops are not provided
+  in the datasheet.
+</p>
+<h4>References</h4>
+<p>
+Daikin, Technical data book RXM-R
+<a href=\"https://www.heizman24.de/media/pdf/fa/50/2c/Daikin-RXM-R-Produktdatenbuch.pdf\">
+https://www.heizman24.de/media/pdf/fa/50/2c/Daikin-RXM-R-Produktdatenbuch.pdf</a>
+</p>
+
+</html>", revisions="<html>
+<ul>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end SingleSplitRXM20R;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/Vitocal251A08.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/Vitocal251A08.mo
new file mode 100644
index 0000000000..62d9e8f475
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/Vitocal251A08.mo
@@ -0,0 +1,53 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.EN14511;
+record Vitocal251A08 "A2W Vitocal 251 by Viessmann"
+  extends GenericAirToWater(
+    dpEva_nominal=0,
+    dpCon_nominal=0,
+    tabUppBou=[253.15,333.15; 263.15,363.15; 313.15,363.15],
+    use_TConOutForOpeEnv=true,
+    use_TEvaOutForOpeEnv=false,
+    tabQCon_flow=[
+      0, 253.15, 258.15, 266.15, 275.15, 280.15, 283.15, 293.15, 303.15, 308.15;
+      308.15, 4490, 5170, 6470, 6790, 8000, 10210, 12330, 12310, 13090;
+      318.15, 4230, 4900, 6260, 6780, 8370, 9970, 11520, 13040, 12640;
+      328.15, 3780, 4710, 6030, 6830, 8380, 9940, 11500, 13070, 13110;
+      338.15, 0, 3170, 4610, 6320, 8140, 9550, 11290, 12100, 12180;
+      343.15, 0, 0, 3830, 5560, 7600, 8700, 11290, 12500, 12590],
+    tabPEle=[
+      0, 253.15, 258.15, 266.15, 275.15, 280.15, 283.15, 293.15, 303.15, 308.15;
+      308.15, 2128, 2238, 2396, 1835, 1633, 2006, 1720, 1465, 1558;
+      318.15, 2299, 2402, 2641, 2173, 2244, 2462, 2110, 1734, 1584;
+      328.15, 2305, 2631, 2899, 2493, 2669, 2915, 2556, 2164, 2081;
+      338.15, 0, 2032, 2478, 2760, 3095, 3375, 3085, 2521, 2511;
+      343.15, 0, 0, 2201, 2699, 3193, 3398, 3330, 2822, 2817],
+    mEva_flow_nominal=2125/3600/1.204,
+    mCon_flow_nominal=5600/5/4184,
+    use_TConOutForTab=true,
+    use_TEvaOutForTab=false,
+    devIde="Vitocal251A08");
+  annotation (Documentation(info="<html>
+<p>
+  Data from the planning book (Planungshandbuch) from Viessmann.
+</p>
+<p>
+  While the product exists in different sizes,
+  this record contains the data for the subtype 251-A08.
+  If you want to model the pressure losses of the device,
+  check out the data sheet and the installed pumps.
+  The pressure loss depends mostly on the hydraulic system
+  according to the datasheet.
+</p>
+<p>
+  The nominal mass flow rate is calculated for the nominal point A7/W35,
+  with a temperature spread of 5 K.
+</p>
+<h4>References</h4>
+<p>
+Viessmann, Planungshandbuch.
+<a href=\"https://www.haustechnik-handrich.de/media/pdf/54/c4/14/vie-pa-z022164.pdf\">
+https://www.haustechnik-handrich.de/media/pdf/54/c4/14/vie-pa-z022164.pdf</a>.
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Vitocal251A08;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/WAMAK_WaterToWater_220kW.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/WAMAK_WaterToWater_220kW.mo
new file mode 100644
index 0000000000..82b6982e8a
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/WAMAK_WaterToWater_220kW.mo
@@ -0,0 +1,91 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.EN14511;
+record WAMAK_WaterToWater_220kW "220 kW water to water with R513A"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.GenericHeatPump(
+    dpEva_nominal(displayUnit="kPa") = 40000,
+    dpCon_nominal(displayUnit="kPa") = 40000,
+    tabUppBou=[
+        268.15, 328.15;
+        273.15, 333.15;
+        283.15, 343.15;
+        293.15, 353.15],
+    mEva_flow_nominal=27.35/3600*997,
+    mCon_flow_nominal=29.07/3600*997,
+    tabPEle=[0, 268.15, 269.15, 270.15, 271.15, 272.15, 273.15, 274.15, 275.15,
+        276.15, 277.15, 278.15, 279.15, 280.15, 281.15, 282.15, 283.15, 284.15,
+        285.15, 286.15, 287.15, 288.15, 289.15, 290.15, 291.15, 292.15, 293.15,
+        294.15, 295.15, 296.15, 297.15, 298.15, 299.15, 300.15, 301.15, 302.15,
+        303.15, 304.15, 305.15, 306.15, 307.15, 308.15, 309.15, 310.15, 311.15,
+        312.15, 313.15, 314.15, 315.15, 316.15, 317.15, 318.15;
+      328.15, 30100, 30100, 30100, 30100, 30100, 30100, 30100, 30100, 30100,
+        30100, 30200, 30200, 30200, 30200, 30200, 30300, 30300, 30300, 30400,
+        30400, 30400, 30500, 30500, 30600, 30600, 30700, 30700, 30800, 30800,
+        30900, 31000, 31000, 31100, 31200, 31200, 31300, 31400, 31500, 31500,
+        31600, 31700, 31800, 31900, 32000, 32100, 32200, 32300, 32400, 32500,
+        32600, 32700;
+      333.15, 0, 0, 0, 0, 0, 33500, 33500, 33500, 33500, 33500, 33500, 33500,
+        33600, 33600, 33600, 33600, 33600, 33600, 33600, 33700, 33700, 33700,
+        33700, 33800, 33800, 33900, 33900, 33900, 34000, 34000, 34100, 34100,
+        34200, 34200, 34300, 34300, 34400, 34400, 34500, 34600, 34600, 34700,
+        34800, 34900, 34900, 35000, 35100, 35200, 35300, 35400, 35400;
+      343.15, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 41700, 41600, 41600,
+        41600, 41600, 41600, 41600, 41600, 41600, 41600, 41600, 41600, 41600,
+        41600, 41600, 41600, 41600, 41600, 41600, 41600, 41600, 41700, 41700,
+        41700, 41700, 41700, 41800, 41800, 41800, 41900, 41900, 41900, 42000,
+        42000, 42100, 42100;
+      353.15, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,
+        0, 0, 0, 0, 51400, 51400, 51300, 51300, 51200, 51200, 51200, 51100,
+        51100, 51000, 51000, 51000, 50900, 50900, 50900, 50800, 50800, 50800,
+        50800, 50700, 50700, 50700, 50700, 50600, 50600, 50600],
+    tabQCon_flow=[0, 268.15, 269.15, 270.15, 271.15, 272.15, 273.15, 274.15,
+        275.15, 276.15, 277.15, 278.15, 279.15, 280.15, 281.15, 282.15, 283.15,
+        284.15, 285.15, 286.15, 287.15, 288.15, 289.15, 290.15, 291.15, 292.15,
+        293.15, 294.15, 295.15, 296.15, 297.15, 298.15, 299.15, 300.15, 301.15,
+        302.15, 303.15, 304.15, 305.15, 306.15, 307.15, 308.15, 309.15, 310.15,
+        311.15, 312.15, 313.15, 314.15, 315.15, 316.15, 317.15, 318.15;
+      328.15, 65800, 68000, 70200, 72400, 74800, 77200, 79700, 82300, 84900,
+        87700, 90500, 93400, 96400, 99500, 102600, 105900, 109300, 112800,
+        116400, 120100, 123900, 127800, 131900, 136100, 140400, 144800, 149300,
+        154000, 158800, 163800, 168900, 174100, 179500, 185000, 190700, 196600,
+        202600, 208700, 215000, 221500, 228200, 235000, 242000, 249200, 256500,
+        264100, 271800, 279700, 287800, 296100, 304600;
+      333.15, 0, 0, 0, 0, 0, 75200, 77600, 80000, 82500, 85000, 87700, 90400,
+        93200, 96100, 99100, 102100, 105300, 108600, 111900, 115400, 119000,
+        122600, 126400, 130300, 134400, 138500, 142800, 147200, 151700, 156300,
+        161100, 166100, 171100, 176300, 181700, 187200, 192800, 198600, 204600,
+        210700, 217000, 223400, 230000, 236800, 243800, 250900, 258200, 265700,
+        273400, 281200, 289300;
+      343.15, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 95000, 97700, 100500,
+        103300, 106300, 109400, 112500, 115800, 119100, 122600, 126100, 129800,
+        133600, 137500, 141500, 145600, 149900, 154300, 158800, 163500, 168200,
+        173200, 178200, 183400, 188800, 194300, 199900, 205700, 211700, 217800,
+        224100, 230600, 237200, 244000, 250900, 258100;
+      353.15, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,
+        0, 0, 0, 114300, 117300, 120500, 123700, 127000, 130500, 134100, 137700,
+        141500, 145400, 149500, 153600, 157900, 162300, 166800, 171500, 176300,
+        181300, 186400, 191700, 197100, 202600, 208300, 214200, 220200, 226400],
+       devIde="WAMAK_TWW220_WHR_HeavyDuty",
+    use_TConOutForTab=true,
+    use_TEvaOutForTab=false);
+  annotation (Documentation(info="<html>
+<p>
+  Data for large scale (220 kW) water-to-water heat pump from WAMAK.
+  Nominal pressure losses are the maximal values given in the datasheet,
+  same for the nominal mass flow rates.
+</p>
+
+<h4>References</h4>
+<p>
+WAMAK, Produktblatt ver. 2023/24.
+<a href=\"https://products.wamak.eu/combine.php?&amp;ampcoverpg&amp;ampdescriptmrktadv&amp;amplang=de-DE&amp;ampcode_id=WAHDR2XE\">
+https://products.wamak.eu/combine.php?&amp;ampcoverpg&amp;ampdescriptmrktadv&amp;amplang=de-DE&amp;ampcode_id=WAHDR2XE</a>.
+</p>
+</html>", revisions="<html>
+<ul><li>
+<i>November 10, 2023</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li></ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WAMAK_WaterToWater_220kW;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/package.mo
new file mode 100644
index 0000000000..09d00fa782
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D;
+package EN14511 "Package for EN15411 data records"
+
+annotation (preferredVies="info",
+Documentation(info="<html>
+<p>
+  This package contains data records for heat pump
+  data according to European Norm 14511.
+</p>
+</html>"));
+end EN14511;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/package.order
new file mode 100644
index 0000000000..a3063bac81
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/EN14511/package.order
@@ -0,0 +1,3 @@
+SingleSplitRXM20R
+Vitocal251A08
+WAMAK_WaterToWater_220kW
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/Generic.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/Generic.mo
new file mode 100644
index 0000000000..0bef637e02
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/Generic.mo
@@ -0,0 +1,94 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D;
+record Generic "Partial two-dimensional data of refrigerant machines"
+    extends Modelica.Icons.Record;
+  parameter Real tabPEle[:,:]
+    "Electrical power consumption table, T in K, Q_flow in W";
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_nominal
+    "Nominal mass flow rate in condenser";
+  parameter Modelica.Units.SI.MassFlowRate mEva_flow_nominal
+    "Nominal mass flow rate in evaporator";
+  parameter Modelica.Units.SI.PressureDifference dpCon_nominal(displayUnit="Pa")
+    "Nominal pressure drop in condenser";
+  parameter Modelica.Units.SI.PressureDifference dpEva_nominal(displayUnit="Pa")
+    "Nominal pressure drop in evaporator";
+  parameter String devIde "Name of the device";
+  parameter Boolean use_TEvaOutForTab
+    "=true to use evaporator outlet temperature for table data, false for inlet";
+  parameter Boolean use_TConOutForTab
+    "=true to use condenser outlet temperature for table data, false for inlet";
+
+  annotation (Documentation(info="<html>
+<h4>Overview</h4>
+<p>
+  Base data definition used in the heat pump model.
+  It defines the table for <code>tab_PEle</code> which gives the electric power
+  consumption of the heat pump or chiller.
+  Information on heat flow rates are in the corresponding records for
+  heat pumps and chillers, as it is the condenser and evaporator heat flow rate,
+  respectively.
+</p>
+<p>
+  Both tables define the power values depending on the ambient side temperature
+  (defined in first row, in K) and the useful side temperature
+  (defined in first column, in K) in W.
+</p>
+<p>
+  Depending on the type of the device, either inlet or outlet conditions are used.
+  This feature could be required for air-air devices. Here, the room temperature
+  (inlet) and outdoor air temperature (inlet) are used. For air-to-water devices,
+  the outdoor air temperature (inlet) and the supply water temperature (outlet) are
+  used instead.
+  When adding new data, be sure to check if the datasheet uses inlet or outlet
+  conditions. Also, be sure to check if the data is for wet- or dry-bulb
+  temperatures. The measured temperatures of the modular approach are taken
+  directly from the fluid ports and are, thus, always dry bulb.
+</p>
+<p>
+  The nominal mass flow rates in the condenser and evaporator
+  are also defined as parameters. If nominal pressure curves are provided
+  in the datasheets, be sure to match the two parameters.
+  Aside from that, the nominal mass flow rates are compared to the values specified
+  by the user. If the deviation is too great, a warning indicates a possible mismatch of
+  system mass flow rate and table data.
+</p>
+<p>
+  The string <code>devIde</code> ensures that if data for heating and cooling are required,
+  matching records will be used. This parameter is mainly to avoid manual input
+  errors.
+</p>
+<h4>Where to get the data?</h4>
+<p>
+  Manufacturers often provide table data for heating or cooling capacity and
+  electrical power consumption, e.g. based on EN 14511.
+  While the usual datasheets only contain some nominal points,
+  the documents for installers and planners are often more specific.
+  Keywords for a search should be <i>technical guide</i>, <i>planning handbook</i>,
+  or similar, together with the manufacturer and possibly the device id.
+</p>
+<h4>References</h4>
+<p>
+EN 14511-2018: Air conditioners, liquid chilling packages and heat pumps for space
+heating and cooling and process chillers, with electrically driven compressors
+<a href=\"https://www.beuth.de/de/norm/din-en-14511-1/298537524\">
+https://www.beuth.de/de/norm/din-en-14511-1/298537524</a>
+</p>
+</html>",
+        revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on IPBSA guidelines <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>May 7, 2020</i> by Philipp Mehrfeld:<br/>
+    Add description of how to calculate m_flows
+  </li>
+  <li>
+    <i>December 10, 2013</i> by Ole Odendahl:<br/>
+    Formatted documentation appropriately
+  </li>
+</ul>
+</html>
+"),Icon, 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generic;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/GenericAirToWater.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/GenericAirToWater.mo
new file mode 100644
index 0000000000..c4fd7a0d87
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/GenericAirToWater.mo
@@ -0,0 +1,22 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D;
+record GenericAirToWater
+  "Partial record for air-to-water heat pump devices"
+  extends GenericHeatPump;
+  annotation (Documentation(revisions="<html>
+<ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Added to enable better selection <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This record allows specific selection using
+  <code>choicesAllMatching</code> for air-to-water heat pumps only in models such as
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.AirToWaterTableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.AirToWaterTableData2D</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GenericAirToWater;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/GenericHeatPump.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/GenericHeatPump.mo
new file mode 100644
index 0000000000..508b2d2f56
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/GenericHeatPump.mo
@@ -0,0 +1,44 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D;
+record GenericHeatPump "Partial heat pump data"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.Generic;
+  parameter Real tabQCon_flow[:,:]
+    "Heating output table, T in K, Q_flow in W";
+  parameter Real tabUppBou[:,2]
+    "Points to define upper boundary for sink temperature";
+  parameter Boolean use_TEvaOutForOpeEnv=false
+    "=true to use evaporator outlet temperature for operational envelope, false for inlet";
+  parameter Boolean use_TConOutForOpeEnv=true
+    "=true to use condenser outlet temperature for operational envelope, false for inlet";
+  annotation (Documentation(info="<html>
+<h4>Overview</h4>
+<p>
+  Base data definition used in the heat pump model.
+</p>
+<p>
+  This record extends <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.Generic\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2DData.RefrigerantCycle2DBaseDataDefinition</a>
+  to enable correct selection.</p>
+<p>
+  It adds the table data for upper temperature limits to
+  the partial record, which is the operational envelope of the compressor.
+</p>
+</html>",
+        revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on IPBSA guidelines <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>May 7, 2020</i> by Philipp Mehrfeld:<br/>
+    Add description of how to calculate m_flows
+  </li>
+  <li>
+    <i>December 10, 2013</i> by Ole Odendahl:<br/>
+    Formatted documentation appropriately
+  </li>
+</ul>
+</html>
+"),Icon, 
+   __Dymola_LockedEditing="Model from IBPSA");
+end GenericHeatPump;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/package.mo
new file mode 100644
index 0000000000..4029a04b9a
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Data;
+package TableData2D "Package with two-dimensional data"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+  annotation (preferredView="info",
+  Documentation(info="<html>
+<p>
+  This package contains data records for heat pump
+  data with two-dimensional tables.
+</p>
+</html>"));
+end TableData2D;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/package.order
new file mode 100644
index 0000000000..c031ee9a3f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/TableData2D/package.order
@@ -0,0 +1,4 @@
+Generic
+GenericAirToWater
+GenericHeatPump
+EN14511
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Data/package.mo
new file mode 100644
index 0000000000..331376d5d3
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/package.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+package Data "Package with data for modular reversible heat pump models"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+  annotation (preferredView="info", Documentation(info="<html>
+  <p>
+  Package with data for heat pump models.
+  </p>
+</html>"));
+end Data;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Data/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Data/package.order
new file mode 100644
index 0000000000..45578af2cf
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Data/package.order
@@ -0,0 +1 @@
+TableData2D
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/AirToWater2D_OneRoomRadiator.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/AirToWater2D_OneRoomRadiator.mo
new file mode 100644
index 0000000000..e5d4213887
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/AirToWater2D_OneRoomRadiator.mo
@@ -0,0 +1,114 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Examples;
+model AirToWater2D_OneRoomRadiator
+  "Reversible heat pump with EN 2D data connected to a simple room model with radiator"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator(
+    mEva_flow_nominal=heaPum.mEva_flow_nominal,
+    mCon_flow_nominal=heaPum.mCon_flow_nominal,
+    sin(nPorts=1, redeclare package Medium = MediumAir),
+    booToReaPumEva(realTrue=heaPum.mEva_flow_nominal),
+    pumHeaPumSou(
+      dp_nominal=heaPum.dpEva_nominal,
+      redeclare package Medium = MediumAir),
+    sou(use_T_in=true,
+      redeclare package Medium = MediumAir),
+    pumHeaPum(dp_nominal=heaPum.dpCon_nominal));
+
+  AixLib.Fluid.HeatPumps.ModularReversible.AirToWaterTableData2D
+    heaPum(
+    redeclare package MediumCon = MediumWat,
+    redeclare package MediumEva = MediumAir,
+    TCon_start=TRadSup_nominal,
+    QHea_flow_nominal=Q_flow_nominal,
+    use_intSafCtr=true,
+    dpCon_nominal(displayUnit="Pa") = 2000,
+    dpEva_nominal(displayUnit="Pa") = 200,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    TConHea_nominal=rad.TRad_nominal,
+    TEvaHea_nominal=283.15,
+    TConCoo_nominal=oneRooRadHeaPumCtr.TRadMinSup,
+    TEvaCoo_nominal=303.15,
+    redeclare
+      AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.EN14511.Vitocal251A08
+      datTabHea,
+    redeclare
+      AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.EN14511.Vitocal251A08
+      datTabCoo,
+    redeclare
+      AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021
+      safCtrPar(
+      use_minOnTime=true,
+      minOnTime=300,
+      use_minOffTime=true,
+      minOffTime=300,
+      use_maxCycRat=true)) "Reversible heat pump based on 2D table data"
+    annotation (Placement(transformation(extent={{20,-160},{0,-140}})));
+  extends Modelica.Icons.Example;
+
+  Modelica.Blocks.Sources.Pulse TAirSouSte(
+    amplitude=20,
+    width=10,
+    period=86400,
+    offset=283.15,
+    startTime=86400/2) if witCoo "Air source temperature step for cooling phase"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-150,-200})));
+equation
+  connect(heaPum.port_b2, sin.ports[1]) annotation (Line(points={{20,-156},{38,
+          -156},{38,-200},{60,-200}},           color={0,127,255}));
+  connect(heaPum.port_a2, pumHeaPumSou.port_b) annotation (Line(
+        points={{0,-156},{-30,-156},{-30,-170}}, color={0,127,255}));
+  connect(heaPum.port_b1, pumHeaPum.port_a) annotation (Line(points={{0,-144},{
+          -70,-144},{-70,-120}},           color={0,127,255}));
+  connect(heaPum.port_a1, temRet.port_b) annotation (Line(points={{20,-144},{60,
+          -144},{60,-30}},           color={0,127,255}));
+  connect(oneRooRadHeaPumCtr.ySet, heaPum.ySet) annotation (Line(
+        points={{-139.167,-66.6667},{28,-66.6667},{28,-148},{21.1,-148},{21.1,
+          -148.1}},                                                       color=
+         {0,0,127}));
+  connect(heaPum.hea, oneRooRadHeaPumCtr.hea) annotation (Line(
+        points={{21.1,-152.1},{24,-152.1},{24,-152},{26,-152},{26,-75},{
+          -139.167,-75}},                         color={255,0,255}));
+  connect(TAirSouSte.y, sou.T_in) annotation (Line(points={{-139,-200},{-94,
+          -200},{-94,-196},{-82,-196}},
+                                  color={0,0,127}));
+  annotation (
+   __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/AirToWater2D_OneRoomRadiator.mos"
+        "Simulate and plot"),
+  experiment(
+      StartTime=0,
+      StopTime=86400,
+      Tolerance=1e-08),
+    Documentation(info="<html>
+<p>
+  This example demonstrates how to use the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.AirToWaterTableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.AirToWaterTableData2D</a>
+  heat pump model. Please check the associated documentation for
+  further information.
+</p>
+<p>
+  Please check the documentation of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator</a>
+  for further information on the example.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>May 5, 2024</i> by Fabian Wuellhorst:<br/>
+  Updated documentation and changed default value (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1876\">#1576</a>)
+</li>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end AirToWater2D_OneRoomRadiator;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/OneRoomRadiatorHeatPumpControl.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/OneRoomRadiatorHeatPumpControl.mo
new file mode 100644
index 0000000000..76df51811a
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/OneRoomRadiatorHeatPumpControl.mo
@@ -0,0 +1,221 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses;
+model OneRoomRadiatorHeatPumpControl
+  "Helper model for the control of the system"
+  parameter Boolean witCoo=true
+    "=true to simulate cooling behaviour";
+  parameter Modelica.Units.SI.Temperature TRooSetHea=293.15
+    "Room set temperature for heating";
+  parameter Modelica.Units.SI.Temperature TRooSetCoo=296.15
+    "Room set temperature for cooling";
+  parameter Modelica.Units.SI.Temperature TRadMinSup=290.15
+    "Minimal radiator supply temperature to avoid condensation effects";
+  parameter Modelica.Units.SI.TemperatureDifference dTHysRoo=2
+    "Temperature hysteresis for room control";
+  Modelica.Blocks.Logical.Hysteresis hysHea(
+    final uLow=TRooSetHea - dTHysRoo,
+    final uHigh=TRooSetHea + dTHysRoo,
+    final pre_y_start=false)
+    "Hysteresis controller for heating" annotation (Placement(transformation(
+          extent={{-10,-10},{10,10}}, origin={-90,20})));
+  Modelica.Blocks.Logical.Hysteresis hysCoo(
+    final uLow=TRooSetCoo - dTHysRoo,
+    final uHigh=TRooSetCoo + dTHysRoo,
+    final pre_y_start=false)
+    if witCoo
+    "Hysteresis controller for cooling" annotation (Placement(transformation(
+          extent={{-10,-10},{10,10}}, origin={-90,-10})));
+  Modelica.Blocks.Sources.BooleanConstant conFal(final k=false)
+                                                          if not witCoo
+    "No cooling if witCoo=false"
+    annotation (Placement(transformation(extent={{-80,-50},{-60,-30}})));
+  Modelica.Blocks.Logical.Not heaIsOn
+    "If lower than hysteresis, heating demand" annotation (Placement(
+        transformation(extent={{-10,-10},{10,10}}, origin={-50,20})));
+  Modelica.Blocks.Logical.Switch swiHeaCooYSet if witCoo
+    "Switch ySet for heating and cooling" annotation (Placement(transformation(
+        extent={{-10,10},{10,-10}},
+        origin={30,70},
+        rotation=0)));
+  Modelica.Blocks.Continuous.LimPID PIDCoo(
+    controllerType=Modelica.Blocks.Types.SimpleController.PI,
+    k=0.01,
+    Ti=800,
+    yMax=1,
+    yMin=0.3,
+    I(use_reset=true, reset=booPasThrCoo.y)) if witCoo
+              "PI control for cooling, inverse"
+    annotation (Placement(transformation(extent={{-20,60},{0,80}})));
+  Modelica.Blocks.Continuous.LimPID PIDHea(
+    controllerType=Modelica.Blocks.Types.SimpleController.PI,
+    k=0.01,
+    Ti=800,
+    yMax=1,
+    yMin=0.3,
+    I(use_reset=true, reset=hysHea.y))
+              "PI control for heating"
+    annotation (Placement(transformation(extent={{-60,80},{-40,100}})));
+  Modelica.Blocks.Sources.Constant constTSetRooHea(final k=TRooSetHea)
+    "Room set point temperature for heating"
+    annotation (Placement(transformation(extent={{-100,80},{-80,100}})));
+  Modelica.Blocks.Sources.Constant constTSetRooCoo(final k=TRooSetCoo) if witCoo
+    "Room set point temperature for cooling"
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+  Modelica.Blocks.Sources.Constant constYSetZer(final k=0) "ySet equals zero"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={30,-18})));
+  Modelica.Blocks.Logical.Switch swiYSet "If no demand, switch heat pump off"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={70,50})));
+  Modelica.Blocks.Logical.Switch swiSecForCoo
+    "If in cooling mode, heat pump can't operate below condensing temperature of 15 °C"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={90,-10})));
+  Modelica.Blocks.Logical.Hysteresis hysSecCoo(
+    final uLow=TRadMinSup,
+    final uHigh=TRadMinSup + 4,
+    final pre_y_start=false)
+            if witCoo
+    "Hysteresis for avoiding temperatures below 15 °C when cooling"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-90,-70},
+        rotation=0)));
+  Modelica.Blocks.Sources.BooleanConstant conTru(final k=true)
+                                                         if not witCoo
+    "No cooling if witCoo=false, then no safety is necessary" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-50,-100})));
+  Modelica.Blocks.Interfaces.RealInput TRooMea(unit="K", displayUnit="degC")
+                                               "Room measurement temperature"
+    annotation (Placement(transformation(extent={{-160,-20},{-120,20}})));
+  Modelica.Blocks.Interfaces.RealInput TRadSup(displayUnit="degC", unit="K")
+                                               "Radiator supply temperature"
+    annotation (Placement(transformation(extent={{-160,-90},{-120,-50}})));
+  Modelica.Blocks.Interfaces.RealOutput ySet "Heat pump set speed"
+    annotation (Placement(transformation(extent={{120,30},{140,50}})));
+  Modelica.Blocks.Interfaces.BooleanOutput hea if witCoo
+    "Heat pump in normal mode"
+    annotation (Placement(transformation(extent={{120,-70},{140,-50}})));
+  Modelica.Blocks.Logical.Or heaOrCooIsOn "Heating or cooling is on"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}}, origin={-10,10})));
+
+  Modelica.Blocks.Logical.Or cooValOrHea
+    "Cooling safety control is used only when the device is not heating" annotation (
+      Placement(transformation(extent={{-10,-10},{10,10}}, origin={-10,-90})));
+  Modelica.Blocks.Routing.BooleanPassThrough booPasThrCoo "Used for reset of PID"
+    annotation (Placement(transformation(extent={{-40,-40},{-20,-20}})));
+equation
+  connect(hysHea.y, heaIsOn.u)
+    annotation (Line(points={{-79,20},{-62,20}}, color={255,0,255}));
+  connect(swiHeaCooYSet.u2, hysCoo.y)
+    annotation (Line(points={{18,70},{10,70},{10,-10},{-79,-10}},
+                                                          color={255,0,255}));
+  connect(swiYSet.u2, heaOrCooIsOn.y) annotation (Line(points={{58,50},{44,50},{44,
+          10},{1,10}},     color={255,0,255}));
+  connect(heaIsOn.y, heaOrCooIsOn.u1) annotation (Line(points={{-39,20},{-30,20},{
+          -30,10},{-22,10}},  color={255,0,255}));
+  connect(PIDHea.u_s,constTSetRooHea. y)
+    annotation (Line(points={{-62,90},{-79,90}},  color={0,0,127}));
+  connect(PIDHea.y, swiHeaCooYSet.u3) annotation (Line(points={{-39,90},{18,90},{18,
+          78}},             color={0,0,127}));
+  connect(constTSetRooCoo.y,PIDCoo. u_m) annotation (Line(points={{-39,50},{-10,50},
+          {-10,58}},                         color={0,0,127}));
+  connect(swiSecForCoo.u3, constYSetZer.y) annotation (Line(points={{78,-18},{
+          41,-18}},              color={0,0,127}));
+  connect(constYSetZer.y, swiYSet.u3) annotation (Line(points={{41,-18},{50,-18},
+          {50,42},{58,42}}, color={0,0,127}));
+  connect(hysCoo.u, TRooMea) annotation (Line(points={{-102,-10},{-108,-10},{-108,
+          0},{-140,0}},        color={0,0,127}));
+  connect(TRooMea, hysHea.u) annotation (Line(points={{-140,0},{-108,0},{-108,20},
+          {-102,20}},                                  color={0,0,127}));
+  connect(swiSecForCoo.y, ySet) annotation (Line(points={{101,-10},{110,-10},{110,
+          40},{130,40}},
+                     color={0,0,127}));
+  connect(hysSecCoo.u, TRadSup)
+    annotation (Line(points={{-102,-70},{-140,-70}},color={0,0,127}));
+  connect(swiYSet.y, swiSecForCoo.u1) annotation (Line(points={{81,50},{86,50},{86,
+          26},{58,26},{58,-2},{78,-2}},    color={0,0,127}));
+  connect(PIDCoo.u_s, TRooMea) annotation (Line(points={{-22,70},{-30,70},{-30,66},
+          {-108,66},{-108,0},{-140,0}},
+                                      color={0,0,127}));
+  connect(PIDHea.u_m, TRooMea) annotation (Line(points={{-50,78},{-50,66},{-108,66},
+          {-108,0},{-140,0}},color={0,0,127}));
+  connect(PIDCoo.y, swiHeaCooYSet.u1) annotation (Line(points={{1,70},{6,70},{6,62},
+          {18,62}},         color={0,0,127}));
+  connect(swiHeaCooYSet.y, swiYSet.u1) annotation (Line(points={{41,70},{50,70},{50,
+          58},{58,58}},                     color={0,0,127}));
+  connect(heaOrCooIsOn.u2, conFal.y) annotation (Line(points={{-22,2},{-26,2},{-26,
+          -10},{-50,-10},{-50,-40},{-59,-40}},
+                           color={255,0,255}));
+  connect(hysCoo.y, heaOrCooIsOn.u2) annotation (Line(points={{-79,-10},{-26,-10},
+          {-26,2},{-22,2}},color={255,0,255}));
+  connect(heaIsOn.y, hea) annotation (Line(points={{-39,20},{-30,20},{-30,-60},{130,
+          -60}},                        color={255,0,255}));
+  connect(cooValOrHea.y, swiSecForCoo.u2) annotation (Line(points={{1,-90},{70,
+          -90},{70,-10},{78,-10}},
+                                 color={255,0,255}));
+  connect(cooValOrHea.u2, conTru.y) annotation (Line(points={{-22,-98},{-32,-98},{
+          -32,-100},{-39,-100}},          color={255,0,255}));
+  connect(cooValOrHea.u2, hysSecCoo.y) annotation (Line(points={{-22,-98},{-32,-98},
+          {-32,-70},{-79,-70}},      color={255,0,255}));
+  connect(heaIsOn.y, cooValOrHea.u1) annotation (Line(points={{-39,20},{-30,20},{-30,
+          -90},{-22,-90}},     color={255,0,255}));
+  if not witCoo then
+    connect(PIDHea.y, swiYSet.u1) annotation (Line(
+      points={{-39,90},{50,90},{50,58},{58,58}},
+      color={0,0,127},
+      pattern=LinePattern.Dash));
+  end if;
+  connect(hysCoo.y, booPasThrCoo.u) annotation (Line(points={{-79,-10},{-49.5,-10},
+          {-49.5,-30},{-42,-30}}, color={255,0,255}));
+  connect(conFal.y, booPasThrCoo.u) annotation (Line(points={{-59,-40},{-50,-40},{
+          -50,-30},{-42,-30}}, color={255,0,255}));
+  annotation (                                                   Diagram(
+        coordinateSystem(extent={{-120,-120},{120,120}})),
+    Documentation(info="<html>
+<p>
+  Helper control model for the example
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator</a>
+  The control enables a PI control of the heat pumps compressor
+  speed for both heating and cooling. Depending on a hysteresis,
+  the heating or cooling mode is selected.
+  If the radiator supply temperature drops below a critical
+  value, the heat pump will turn to heating mode. This prohibits
+  possible freezing or water condensation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>July 15, 2024</i> by Fabian Wuellhorst:<br/>
+  Adjust hysteresis bandwidth (see issue
+  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1908\">IBPSA #1908</a>)
+</li>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(extent={{-120,-120},{120,120}}), graphics={
+      Text(
+          extent={{-153,163},{147,123}},
+          textColor={0,0,255},
+          fillPattern=FillPattern.HorizontalCylinder,
+          fillColor={0,127,255},
+          textString="%name"),
+        Rectangle(
+          extent={{-120,120},{120,-120}},
+          lineColor={0,0,0},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end OneRoomRadiatorHeatPumpControl;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/PartialOneRoomRadiator.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/PartialOneRoomRadiator.mo
new file mode 100644
index 0000000000..58b76dccad
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/PartialOneRoomRadiator.mo
@@ -0,0 +1,287 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses;
+partial model PartialOneRoomRadiator
+  "Simple room model with radiator, without a heat pump"
+  replaceable package MediumAir =
+      AixLib.Media.Air "Medium model for air";
+  replaceable package MediumWat =
+      AixLib.Media.Water "Medium model for water";
+
+  parameter Modelica.Units.SI.HeatFlowRate Q_flow_nominal=20000
+    "Nominal heat flow rate of radiator";
+  parameter Modelica.Units.SI.Temperature TRadSup_nominal=273.15 + 50
+    "Radiator nominal supply water temperature";
+  parameter Modelica.Units.SI.Temperature TRadRet_nominal=273.15 + 45
+    "Radiator nominal return water temperature";
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_nominal=Q_flow_nominal/4200
+      /5 "Heat pump nominal mass flow rate in condenser";
+  parameter Modelica.Units.SI.MassFlowRate mEva_flow_nominal(min=Modelica.Constants.eps)
+    "Heat pump nominal mass flow rate in evaporator";
+  parameter Modelica.Units.SI.Volume V=6*10*3 "Room volume";
+  parameter Modelica.Units.SI.MassFlowRate mAirRoo_flow_nominal=V*1.2*6/3600
+    "Nominal mass flow rate of room air";
+  parameter Modelica.Units.SI.HeatFlowRate QRooInt_flow=Q_flow_nominal/5
+    "Internal heat gains of the room";
+  parameter Boolean witCoo=true "=true to simulate cooling behaviour";
+//------------------------------------------------------------------------------//
+
+  AixLib.Fluid.MixingVolumes.MixingVolume vol(
+    redeclare package Medium = MediumAir,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    m_flow_nominal=mAirRoo_flow_nominal,
+    V=V) annotation (Placement(transformation(extent={{60,20},{80,40}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalConductor theCon(G=
+        Q_flow_nominal/40)
+    "Thermal conductance with the ambient"
+    annotation (Placement(transformation(extent={{20,40},{40,60}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow preHea
+    "Prescribed heat flow"
+    annotation (Placement(transformation(extent={{20,70},{40,90}})));
+  Modelica.Thermal.HeatTransfer.Components.HeatCapacitor heaCap(
+    C=2*V*1.2*1006)
+    "Heat capacity for furniture and walls"
+    annotation (Placement(transformation(extent={{60,50},{80,70}})));
+  Modelica.Blocks.Sources.CombiTimeTable timTab(
+      extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic,
+      smoothness=Modelica.Blocks.Types.Smoothness.ConstantSegments,
+      table=[-6*3600, 0;
+              8*3600, QRooInt_flow;
+             18*3600, 0]) "Time table for internal heat gain"
+    annotation (Placement(transformation(extent={{-20,70},{0,90}})));
+  AixLib.Fluid.HeatExchangers.Radiators.RadiatorEN442_2 rad(
+    redeclare package Medium = MediumWat,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    Q_flow_nominal=Q_flow_nominal,
+    T_a_nominal=TRadSup_nominal,
+    T_b_nominal=TRadRet_nominal,
+    m_flow_nominal=mCon_flow_nominal,
+    T_start=TRadSup_nominal) "Radiator"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort temSup(
+    redeclare package Medium = MediumWat,
+    m_flow_nominal=mCon_flow_nominal,
+    T_start=TRadSup_nominal) "Supply water temperature" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-70,-20})));
+  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor temRoo
+    "Room temperature" annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        origin={-38,30})));
+
+//----------------------------------------------------------------------------//
+
+  replaceable AixLib.Fluid.Movers.Preconfigured.FlowControlled_m_flow pumHeaPum(
+    redeclare package Medium = MediumWat,
+    m_flow_nominal=mCon_flow_nominal,
+    m_flow_start=mCon_flow_nominal,
+    T_start=TRadSup_nominal,
+    use_inputFilter=false,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
+    "Pump for radiator side" annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-70,-110})));
+//----------------------------------------------------------------------------//
+
+  AixLib.Fluid.Sensors.TemperatureTwoPort temRet(
+    redeclare package Medium = MediumWat,
+    m_flow_nominal=mCon_flow_nominal,
+    T_start=TRadSup_nominal) "Return water temperature" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={60,-20})));
+
+//------------------------------------------------------------------------------------//
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+    Modelica.Utilities.Files.loadResource(
+      "modelica://AixLib/Resources/weatherdata/USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos"))
+    "Weather data reader"
+    annotation (Placement(transformation(extent={{-220,40},{-200,60}})));
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather data bus"
+    annotation (Placement(transformation(extent={{-160,40},{-140,60}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature TOut
+    "Outside temperature"
+    annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+
+//--------------------------------------------------------------------------------------//
+
+  AixLib.Fluid.Movers.Preconfigured.FlowControlled_m_flow pumHeaPumSou(
+    redeclare package Medium = MediumWat,
+    m_flow_start=mEva_flow_nominal,
+    m_flow_nominal=mEva_flow_nominal,
+    use_inputFilter=false,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
+    "Pump for heat pump source side" annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-30,-180})));
+  Modelica.Blocks.Math.BooleanToReal booToReaPumCon(
+    realTrue=mCon_flow_nominal,
+    y(start=0)) "Pump signal" annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={-110,-110})));
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = MediumWat,
+    T=281.15,
+    nPorts=1) "Fluid source on source side"
+    annotation (Placement(transformation(extent={{-80,-210},{-60,-190}})));
+  AixLib.Fluid.Sources.Boundary_pT sin(
+    redeclare package Medium = MediumWat,
+    T=283.15) "Fluid sink on source side"
+    annotation (Placement(transformation(extent={{80,-210},{60,-190}})));
+  AixLib.Fluid.Sources.Boundary_pT preSou(
+    redeclare package Medium = MediumWat,
+    T=TRadSup_nominal,
+    nPorts=1)
+    "Source for pressure and to account for thermal expansion of water"
+    annotation (Placement(transformation(extent={{90,-130},{70,-110}})));
+
+  Modelica.Blocks.Math.BooleanToReal booToReaPumEva(realTrue=1, y(start=0))
+    "Pump signal" annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={-110,-180})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow preHeaCoo if witCoo
+    "Prescribed heat flow to trigger cooling"
+    annotation (Placement(transformation(extent={{-100,60},{-80,80}})));
+  Modelica.Blocks.Sources.Pulse cooLoa(
+    amplitude=Q_flow_nominal/2,
+    width=10,
+    period=86400,
+    startTime=86400/2) if witCoo "Cooling load with step" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-130,70})));
+  AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.OneRoomRadiatorHeatPumpControl oneRooRadHeaPumCtr(
+    final witCoo=witCoo)
+    "Control block for single room heat pump control"
+    annotation (Placement(transformation(extent={{-160,-80},{-140,-60}})));
+  Modelica.Blocks.Sources.BooleanConstant conPumAlwOn(final k=true)
+    "Let the pumps always run, due to inertia of the heat pump" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-154,-140})));
+equation
+  connect(theCon.port_b, vol.heatPort) annotation (Line(
+      points={{40,50},{50,50},{50,30},{60,30}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(preHea.port, vol.heatPort) annotation (Line(
+      points={{40,80},{50,80},{50,30},{60,30}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(heaCap.port, vol.heatPort) annotation (Line(
+      points={{70,50},{50,50},{50,30},{60,30}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(timTab.y[1], preHea.Q_flow) annotation (Line(
+      points={{1,80},{20,80}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(temSup.port_b, rad.port_a) annotation (Line(
+      points={{-70,-10},{-70,0},{0,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(temRoo.port, vol.heatPort) annotation (Line(
+      points={{-28,30},{60,30}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(rad.heatPortCon, vol.heatPort) annotation (Line(
+      points={{8,7.2},{8,30},{60,30}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(rad.heatPortRad, vol.heatPort) annotation (Line(
+      points={{12,7.2},{12,30},{60,30}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(weaDat.weaBus, weaBus) annotation (Line(
+      points={{-200,50},{-150,50}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(weaBus.TDryBul, TOut.T) annotation (Line(
+      points={{-149.95,50.05},{-86,50.05},{-86,50},{-22,50}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None), Text(
+      textString="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}}));
+  connect(TOut.port, theCon.port_a) annotation (Line(
+      points={{0,50},{20,50}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(pumHeaPum.port_b, temSup.port_a)
+    annotation (Line(points={{-70,-100},{-70,-30}},color={0,127,255}));
+  connect(temRet.port_a, rad.port_b)
+    annotation (Line(points={{60,-10},{60,0},{20,0}},     color={0,127,255}));
+  connect(booToReaPumCon.y, pumHeaPum.m_flow_in)
+    annotation (Line(points={{-99,-110},{-82,-110}}, color={0,0,127}));
+  connect(sou.ports[1], pumHeaPumSou.port_a) annotation (Line(points={{-60,-200},
+          {-30,-200},{-30,-190}}, color={0,127,255}));
+  connect(preSou.ports[1], temRet.port_b) annotation (Line(points={{70,-120},{60,
+          -120},{60,-30}}, color={0,127,255}));
+  connect(booToReaPumEva.y, pumHeaPumSou.m_flow_in)
+    annotation (Line(points={{-99,-180},{-42,-180}}, color={0,0,127}));
+
+  connect(cooLoa.y, preHeaCoo.Q_flow)
+    annotation (Line(points={{-119,70},{-100,70}}, color={0,0,127}));
+  connect(preHeaCoo.port, heaCap.port) annotation (Line(points={{-80,70},{-60,70},
+          {-60,66},{50,66},{50,50},{70,50}}, color={191,0,0}));
+  connect(conPumAlwOn.y, booToReaPumEva.u) annotation (Line(points={{-143,-140},
+          {-132,-140},{-132,-180},{-122,-180}}, color={255,0,255}));
+  connect(conPumAlwOn.y, booToReaPumCon.u) annotation (Line(points={{-143,-140},
+          {-132,-140},{-132,-110},{-122,-110}}, color={255,0,255}));
+  connect(oneRooRadHeaPumCtr.TRadSup, temSup.T) annotation (Line(points={{
+          -161.667,-75.8333},{-188,-75.8333},{-188,-20},{-81,-20}},    color={0,
+          0,127}));
+  connect(oneRooRadHeaPumCtr.TRooMea, temRoo.T) annotation (Line(points={{
+          -161.667,-70},{-180,-70},{-180,30},{-49,30}},          color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  Motivated by the example
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.ScrollWaterToWater_OneRoomRadiator\">
+  AixLib.Fluid.HeatPumps.Examples.ScrollWaterToWater_OneRoomRadiator</a>,
+  this example enables the use of the <code>ModularReversible</code>
+  approach for heat pumps and chillers.
+</p>
+<p>
+  Both heating and cooling of the room is possible by using
+  the reversible approach. For heating, 20 degC room temperature
+  is the set point, for cooling 23 degC.
+</p>
+<p>
+  The radiator minimal supply temperature is 23 degC.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+<li>
+January 27, 2017, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(preserveAspectRatio=false,extent={{-240,-220},{100,
+            100}})),
+    __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/Examples/ScrollWaterToWater_OneRoomRadiator.mos"
+        "Simulate and plot"),
+    experiment(
+      StopTime=172800,
+      Tolerance=1e-08), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialOneRoomRadiator;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/package.mo
new file mode 100644
index 0000000000..4ae0b59c95
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/package.mo
@@ -0,0 +1,6 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Examples;
+package BaseClasses "Bases package for examples"
+  extends Modelica.Icons.BasesPackage;
+
+
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/package.order
new file mode 100644
index 0000000000..f86d98d6b2
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/BaseClasses/package.order
@@ -0,0 +1,2 @@
+OneRoomRadiatorHeatPumpControl
+PartialOneRoomRadiator
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/CarnotWithLosses_OneRoomRadiator.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/CarnotWithLosses_OneRoomRadiator.mo
new file mode 100644
index 0000000000..63255a8601
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/CarnotWithLosses_OneRoomRadiator.mo
@@ -0,0 +1,101 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Examples;
+model CarnotWithLosses_OneRoomRadiator
+  "Reversible heat pump with Carnot approach connected to a simple room model with radiator"
+  extends Examples.BaseClasses.PartialOneRoomRadiator(
+    mEva_flow_nominal=heaPum.mEva_flow_nominal,
+    mCon_flow_nominal=heaPum.mCon_flow_nominal,
+    sin(nPorts=1),
+    booToReaPumEva(realTrue=heaPum.mEva_flow_nominal),
+    pumHeaPumSou(dp_nominal=heaPum.dpEva_nominal),
+    pumHeaPum(dp_nominal=heaPum.dpCon_nominal));
+  extends Modelica.Icons.Example;
+
+  parameter Real perHeaLos=0.01
+    "Percentage of heat losses in the heat exchangers to the nominal heating output";
+  AixLib.Fluid.HeatPumps.ModularReversible.CarnotWithLosses heaPum(
+    redeclare package MediumCon = MediumWat,
+    redeclare package MediumEva = MediumWat,
+    QHea_flow_nominal=Q_flow_nominal,
+    use_rev=true,
+    use_intSafCtr=true,
+    TConHea_nominal=TRadSup_nominal,
+    dTCon_nominal=TRadSup_nominal - TRadRet_nominal,
+    dpCon_nominal(displayUnit="Pa") = 2000,
+    CCon=5000,
+    GConOut=perHeaLos*Q_flow_nominal/(TRadSup_nominal - temAmbBas.k),
+    GConIns=20000,
+    TEvaHea_nominal=sou.T,
+    dTEva_nominal=5,
+    dpEva_nominal(displayUnit="Pa") = 2000,
+    CEva=5000,
+    GEvaOut=perHeaLos*Q_flow_nominal/(temAmbBas.k - sou.T),
+    GEvaIns=20000,
+    TConCoo_nominal=oneRooRadHeaPumCtr.TRadMinSup,
+    TEvaCoo_nominal=sou.T + 10,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    redeclare AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021 safCtrPar,
+    etaCarnot_nominal=0.4)
+      "Reversible heat pump with losses and Carnot approach"
+    annotation (Placement(transformation(extent={{20,-160},{0,-140}})));
+  Modelica.Blocks.Sources.Constant temAmbBas(final k(
+      final unit="K",
+      displayUnit="degC") = 291.15)
+    "Ambient temperature in basement of building" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={10,-190})));
+equation
+  connect(heaPum.port_b2, sin.ports[1]) annotation (Line(points={{20,-156},{38,
+          -156},{38,-200},{60,-200}},           color={0,127,255}));
+  connect(heaPum.port_a2, pumHeaPumSou.port_b) annotation (Line(
+        points={{0,-156},{-30,-156},{-30,-170}}, color={0,127,255}));
+  connect(heaPum.port_b1, pumHeaPum.port_a) annotation (Line(points={{0,-144},{
+          -70,-144},{-70,-120}},           color={0,127,255}));
+  connect(heaPum.port_a1, temRet.port_b) annotation (Line(points={{20,-144},{60,
+          -144},{60,-30}},           color={0,127,255}));
+  connect(temAmbBas.y, heaPum.TEvaAmb) annotation (Line(points={{21,-190},{28,-190},
+          {28,-159.1},{21.1,-159.1}},                     color={0,0,127}));
+  connect(temAmbBas.y, heaPum.TConAmb) annotation (Line(points={{21,-190},{28,-190},
+          {28,-141.1},{21.1,-141.1}},                     color={0,0,127}));
+
+  connect(oneRooRadHeaPumCtr.hea, heaPum.hea) annotation (Line(
+        points={{-139.167,-75},{-94,-75},{-94,-164},{30,-164},{30,-152.1},{21.1,
+          -152.1}},
+        color={255,0,255}));
+  connect(oneRooRadHeaPumCtr.ySet, heaPum.ySet) annotation (Line(
+        points={{-139.167,-66.6667},{30,-66.6667},{30,-148},{26,-148},{26,
+          -148.1},{21.1,-148.1}},                           color={0,0,127}));
+  annotation (
+   __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/CarnotWithLosses_OneRoomRadiator.mos"
+        "Simulate and plot"),
+  experiment(
+      StartTime=0,
+      StopTime=86400,
+      Tolerance=1e-08),
+    Documentation(info="<html>
+<p>
+  This example demonstrates how to use the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.CarnotWithLosses\">
+  AixLib.Fluid.HeatPumps.ModularReversible.CarnotWithLosses</a>
+  heat pump model. Please check the associated documentation for
+  further information.
+</p>
+<p>
+  Please check the documentation of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator</a>
+  for further information on the example.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end CarnotWithLosses_OneRoomRadiator;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/LargeScaleWaterToWater_OneRoomRadiator.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/LargeScaleWaterToWater_OneRoomRadiator.mo
new file mode 100644
index 0000000000..2b30301ee6
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/LargeScaleWaterToWater_OneRoomRadiator.mo
@@ -0,0 +1,117 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Examples;
+model LargeScaleWaterToWater_OneRoomRadiator
+  "Large scale water to water heat pump connected to a simple room model with radiator"
+  extends Modelica.Icons.Example;
+  extends BaseClasses.PartialOneRoomRadiator(
+    mEva_flow_nominal=heaPum.mEva_flow_nominal,
+    mCon_flow_nominal=heaPum.mCon_flow_nominal,
+    V=6*100*3,
+    witCoo=true,
+    mAirRoo_flow_nominal=V*1.2*6/3600*10,
+    Q_flow_nominal=200000,
+    sin(nPorts=1),
+    booToReaPumEva(realTrue=heaPum.mEva_flow_nominal),
+    pumHeaPumSou(dp_nominal=150000),
+    pumHeaPum(dp_nominal=150000),
+    sou(use_T_in=true));
+
+  AixLib.Fluid.HeatPumps.ModularReversible.LargeScaleWaterToWater heaPum(
+    allowDifferentDeviceIdentifiers=true,
+    QHea_flow_nominal=Q_flow_nominal,
+    use_intSafCtr=true,
+    QCoo_flow_nominal=-Q_flow_nominal/2,
+    TConHea_nominal=TRadSup_nominal,
+    dpCon_nominal(displayUnit="Pa"),
+    TEvaHea_nominal=sou.T,
+    dpEva_nominal(displayUnit="Pa"),
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    redeclare AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021
+      safCtrPar,
+    TConCoo_nominal=oneRooRadHeaPumCtr.TRadMinSup,
+    TEvaCoo_nominal=sou.T + 30,
+    redeclare
+      AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.EN14511.WAMAK_WaterToWater_220kW
+      datTabHea,
+    redeclare
+      AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.EN14511.Carrier30XWP1012_1MW
+      datTabCoo)
+    "Large scale water to water heat pump"
+    annotation (Placement(transformation(extent={{20,-160},{0,-140}})));
+  Modelica.Blocks.Sources.Pulse TAirSouSte(
+    amplitude=20,
+    width=10,
+    period=86400,
+    offset=283.15,
+    startTime=86400/2) if witCoo "Air source temperature step for cooling phase"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-150,-200})));
+equation
+  connect(heaPum.port_b2, sin.ports[1]) annotation (Line(points={{20,-156},{38,
+          -156},{38,-200},{60,-200}},               color={0,127,255}));
+  connect(heaPum.port_a2, pumHeaPumSou.port_b) annotation (Line(
+        points={{0,-156},{-30,-156},{-30,-170}}, color={0,127,255}));
+  connect(heaPum.port_b1, pumHeaPum.port_a) annotation (Line(
+        points={{0,-144},{-70,-144},{-70,-120}}, color={0,127,255}));
+  connect(heaPum.port_a1, temRet.port_b) annotation (Line(points={{20,-144},{60,
+          -144},{60,-30}},                color={0,127,255}));
+  connect(oneRooRadHeaPumCtr.ySet, heaPum.ySet) annotation (Line(
+        points={{-139.167,-66.6667},{26,-66.6667},{26,-148.1},{21.1,-148.1}},
+                                                                        color={
+          0,0,127}));
+  connect(oneRooRadHeaPumCtr.hea, heaPum.hea) annotation (Line(points={{
+          -139.167,-75},{32,-75},{32,-152.1},{21.1,-152.1}}, color={255,0,255}));
+  connect(TAirSouSte.y, sou.T_in) annotation (Line(points={{-139,-200},{-92,-200},
+          {-92,-196},{-82,-196}}, color={0,0,127}));
+  annotation (
+     __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/LargeScaleWaterToWater_OneRoomRadiator.mos"
+        "Simulate and plot"),
+  experiment(
+      StartTime=0,
+      StopTime=86400,
+      Tolerance=1e-08),
+  Documentation(
+   info="<html>
+<p>
+  This example demonstrates how to use the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.LargeScaleWaterToWater\">
+  AixLib.Fluid.HeatPumps.ModularReversible.LargeScaleWaterToWater</a>
+  heat pump model. Please check the associated documentation for
+  further information.
+</p>
+<p>
+  Contrary to the other models, parameters for heat exchanger
+  inertia (tau) and mass flow rates are calculated
+  automatically based on the heat demand.
+</p>
+<p>
+  Furthermore, this example demonstrates the warnings which
+  are raised if two devices are combined with different sizes, leading
+  to different scaling factors for heating and cooling operation.
+  If the default <code>QCoo_flow_nominal</code> is used (leading to
+  the same scaling factors), the mass flow rates will differ.
+  Setting the parameter <code>allowDifferentDeviceIdentifiers</code> to false,
+  an additional warning is raised, indicating that the table data for cooling and
+  heating operation do not originate from the same real device.
+</p>
+<p>
+  Please check the documentation of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator</a>
+  for further information on the example.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-240,-220},{100,100}})),
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end LargeScaleWaterToWater_OneRoomRadiator;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/Modular_OneRoomRadiator.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/Modular_OneRoomRadiator.mo
new file mode 100644
index 0000000000..ef079ac53f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/Modular_OneRoomRadiator.mo
@@ -0,0 +1,131 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Examples;
+model Modular_OneRoomRadiator
+  "Modular reversible heat pump connected to a simple room model with radiator"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator(
+    mEva_flow_nominal=heaPum.mEva_flow_nominal,
+    sin(nPorts=1, redeclare package Medium = MediumAir),
+    pumHeaPumSou(
+      dp_nominal=heaPum.dpEva_nominal,
+      redeclare package Medium = MediumAir),
+    sou(redeclare package Medium = MediumAir),
+    booToReaPumEva(realTrue=heaPum.mEva_flow_nominal),
+    pumHeaPum(dp_nominal=heaPum.dpCon_nominal));
+  extends Modelica.Icons.Example;
+
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular heaPum(
+    redeclare package MediumCon = MediumWat,
+    redeclare package MediumEva = MediumAir,
+    use_rev=true,
+    allowDifferentDeviceIdentifiers=true,
+    QHea_flow_nominal=Q_flow_nominal,
+    redeclare model RefrigerantCycleInertia =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.NoInertia,
+    use_intSafCtr=true,
+    TConHea_nominal=TRadSup_nominal,
+    TConCoo_nominal=oneRooRadHeaPumCtr.TRadMinSup,
+    dTCon_nominal=TRadSup_nominal - TRadRet_nominal,
+    dpCon_nominal(displayUnit="Pa") = 2000,
+    use_conCap=true,
+    CCon=3000,
+    GConOut=100,
+    GConIns=1000,
+    TEvaHea_nominal=sou.T,
+    TEvaCoo_nominal=sou.T,
+    dTEva_nominal=2,
+    dpEva_nominal(displayUnit="Pa") = 200,
+    use_evaCap=false,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    redeclare model RefrigerantCycleHeatPumpHeating =
+      AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness(
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+          iceFacCal,
+        TAppCon_nominal=0,
+        TAppEva_nominal=0),
+    redeclare model RefrigerantCycleHeatPumpCooling =
+      AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D(
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+          iceFacCal,
+        mCon_flow_nominal=heaPum.mCon_flow_nominal,
+        mEva_flow_nominal=heaPum.mEva_flow_nominal,
+        datTab=AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.EN14511.Vitocal251A08()),
+    redeclare AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021 safCtrPar(
+      use_TConOutHea=true,
+      use_TEvaOutHea=false,
+      use_antFre=true,
+      TAntFre=275.15),
+    QCoo_flow_nominal=-Q_flow_nominal*0.5)
+      "Modular reversible heat pump"
+    annotation (Placement(transformation(extent={{20,-160},{0,-140}})));
+
+  Modelica.Blocks.Sources.Constant temAmbBas(
+    final k(
+      final unit="K",
+      displayUnit="degC") = 291.15)
+    "Ambient temperature in basement of building" annotation (Placement(
+        transformation(
+        extent={{-10,10},{10,-10}},
+        rotation=180,
+        origin={70,-160})));
+equation
+  connect(heaPum.port_b2, sin.ports[1]) annotation (Line(points={{20,-156},{38,-156},
+          {38,-200},{60,-200}},           color={0,127,255}));
+  connect(heaPum.port_a2, pumHeaPumSou.port_b) annotation (Line(points={{0,-156},{
+          -30,-156},{-30,-170}},        color={0,127,255}));
+  connect(heaPum.port_b1, pumHeaPum.port_a) annotation (Line(points={{0,-144},{-70,
+          -144},{-70,-120}},      color={0,127,255}));
+  connect(heaPum.port_a1, temRet.port_b) annotation (Line(points={{20,-144},{60,-144},
+          {60,-30}},           color={0,127,255}));
+  connect(temAmbBas.y, heaPum.TConAmb) annotation (Line(points={{59,-160},{54,
+          -160},{54,-141.1},{21.1,-141.1}},
+                                          color={0,0,127}));
+  connect(heaPum.hea, oneRooRadHeaPumCtr.hea) annotation (Line(points={{21.1,
+          -152.1},{24,-152.1},{24,-75},{-139.167,-75}},
+                 color={255,0,255}));
+  connect(oneRooRadHeaPumCtr.ySet, heaPum.ySet) annotation (Line(points={{
+          -139.167,-66.6667},{30,-66.6667},{30,-148.1},{21.1,-148.1}},
+                                                      color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  This example demonstrates how to use the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a>
+  heat pump model directly. Please check the associated documentation for
+  further information.
+</p>
+<p>
+  Correct replacement of the replaceable submodels
+  and, thus, flexible aggregation to a new model
+  approach is demonstrated.
+</p>
+<p>
+  Please check the documentation of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Examples.BaseClasses.PartialOneRoomRadiator</a>
+  for further information on the example.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+  May 2, 2024, by Michael Wetter:<br/>
+  Refactored check for device identifiers.<br/>
+  This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">IBPSA, #1576</a>.
+</li>
+<li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li>
+</ul>
+</html>"),
+   __Dymola_Commands(file=
+     "modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/Modular_OneRoomRadiator.mos"
+        "Simulate and plot"),
+  experiment(
+      StartTime=0,
+      StopTime=86400,
+      Tolerance=1e-08), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Modular_OneRoomRadiator;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/package.mo
new file mode 100644
index 0000000000..13d2dd0cb8
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+package Examples "Collection of models that illustrate model use and test models"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible\">
+AixLib.Fluid.HeatPumps.ModularReversible</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Examples/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/package.order
new file mode 100644
index 0000000000..bf09de91d8
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Examples/package.order
@@ -0,0 +1,5 @@
+AirToWater2D_OneRoomRadiator
+CarnotWithLosses_OneRoomRadiator
+LargeScaleWaterToWater_OneRoomRadiator
+Modular_OneRoomRadiator
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/LargeScaleWaterToWater.mo b/AixLib/Fluid/HeatPumps/ModularReversible/LargeScaleWaterToWater.mo
new file mode 100644
index 0000000000..891188e7f5
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/LargeScaleWaterToWater.mo
@@ -0,0 +1,57 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+model LargeScaleWaterToWater
+  "Model with automatic parameter estimation for large scale water-to-water heat pumps"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.TableData2D(
+    redeclare replaceable package MediumCon = AixLib.Media.Water,
+    redeclare replaceable package MediumEva = AixLib.Media.Water,
+    final mCon_flow_nominal=autCalMasCon_flow,
+    final mEva_flow_nominal=autCalMasEva_flow,
+    final tauCon=autCalVCon*rhoCon/autCalMasCon_flow,
+    final tauEva=autCalVEva*rhoEva/autCalMasEva_flow);
+
+  extends AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.LargeScaleWaterToWaterDeclarations(
+    final autCalMasCon_flow=max(4E-5*QHea_flow_nominal - 0.6162, autCalMMin_flow),
+    final autCalMasEva_flow=max(4E-5*QHea_flow_nominal - 0.3177, autCalMMin_flow),
+    final autCalVCon=max(1E-7*QHea_flow_nominal - 94E-4, autCalVMin),
+    final autCalVEva=max(1E-7*QHea_flow_nominal - 75E-4, autCalVMin));
+
+  annotation (Documentation(info="<html>
+<p>
+  Model using parameters for a large scale water-to-water heat pump,
+  using the ModularReversible model approach.
+</p>
+<p>
+  Contrary to the standard sizing approach for the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a> models,
+  the parameters are based on an automatic estimation as described in
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.LargeScaleWaterToWaterDeclarations\">
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.LargeScaleWaterToWaterDeclarations</a>.
+</p>
+<p>
+  For more information on the approach, please read the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  UsersGuide</a>.
+</p>
+<p>
+  Please read the documentation of the model for heating here:
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D</a>.
+</p>
+<h4>Assumptions</h4>
+<ul>
+<li>
+  As heat losses are implicitly included in the table
+  data given by manufacturers, heat losses are disabled.
+</li>
+</ul>
+</html>", revisions="<html><ul>
+  <li>
+    <i>Novemeber 11, 2022</i> by Fabian Wuellhorst:<br/>
+    Implemented <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end LargeScaleWaterToWater;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Modular.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Modular.mo
new file mode 100644
index 0000000000..2f6eba1415
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Modular.mo
@@ -0,0 +1,147 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+model Modular
+  "Grey-box model for reversible and non-reversible heat pumps"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialReversibleRefrigerantMachine(
+    final use_COP=true,
+    final use_EER=use_rev,
+    con(preDro(m_flow(nominal=QHea_flow_nominal/1000/10))),
+    eva(preDro(m_flow(nominal=QHea_flow_nominal/1000/10))),
+    final PEle_nominal=refCyc.refCycHeaPumHea.PEle_nominal,
+    mCon_flow_nominal=QHea_flow_nominal/(dTCon_nominal*cpCon),
+    mEva_flow_nominal=(QHea_flow_nominal - PEle_nominal)/(dTEva_nominal*cpEva),
+    use_rev=false,
+    redeclare final AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantCycle refCyc(
+      redeclare model RefrigerantCycleHeatPumpHeating =
+          RefrigerantCycleHeatPumpHeating,
+      redeclare model RefrigerantCycleHeatPumpCooling =
+          RefrigerantCycleHeatPumpCooling,
+      final allowDifferentDeviceIdentifiers=allowDifferentDeviceIdentifiers));
+  parameter Modelica.Units.SI.HeatFlowRate QHea_flow_nominal(min=Modelica.Constants.eps)
+    "Nominal heating capacity"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.HeatFlowRate QCoo_flow_nominal(max=0)=0
+    "Nominal cooling capacity"
+      annotation(Dialog(group="Nominal condition - Cooling", enable=use_rev));
+
+  replaceable model RefrigerantCycleHeatPumpHeating =
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle
+      (PEle_nominal=0)
+       constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle(
+       final useInHeaPum=true,
+       final QHea_flow_nominal=QHea_flow_nominal,
+       final TCon_nominal=TConHea_nominal,
+       final TEva_nominal=TEvaHea_nominal,
+       final cpCon=cpCon,
+       final cpEva=cpEva)
+  "Refrigerant cycle module for the heating mode"
+    annotation (choicesAllMatching=true);
+
+  replaceable model RefrigerantCycleHeatPumpCooling =
+      AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.NoCooling
+      constrainedby
+    AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle(
+       final useInChi=false,
+       final cpCon=cpCon,
+       final cpEva=cpEva,
+       final TCon_nominal=TEvaCoo_nominal,
+       final TEva_nominal=TConCoo_nominal,
+       QCoo_flow_nominal=QCoo_flow_nominal)
+  "Refrigerant cycle module for the cooling mode"
+    annotation (Dialog(enable=use_rev),choicesAllMatching=true);
+  parameter Modelica.Units.SI.Temperature TConHea_nominal
+    "Nominal temperature of the heated fluid"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.Temperature TEvaHea_nominal
+    "Nominal temperature of the cooled fluid"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.Temperature TConCoo_nominal
+    "Nominal temperature of the cooled fluid"
+    annotation(Dialog(enable=use_rev, group="Nominal condition - Cooling"));
+  parameter Modelica.Units.SI.Temperature TEvaCoo_nominal
+    "Nominal temperature of the heated fluid"
+    annotation(Dialog(enable=use_rev, group="Nominal condition - Cooling"));
+
+  Modelica.Blocks.Sources.BooleanConstant conHea(final k=true)
+    if not use_busConOnl and not use_rev
+    "Locks the device in heating mode if designated to be not reversible" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-110,-130})));
+  Modelica.Blocks.Interfaces.BooleanInput hea if not use_busConOnl and use_rev
+    "=true for heating, =false for cooling"
+    annotation (Placement(transformation(extent={{-164,-82},{-140,-58}}),
+        iconTransformation(extent={{-120,-30},{-102,-12}})));
+equation
+  connect(conHea.y, sigBus.hea)
+    annotation (Line(points={{-99,-130},{-76,-130},{-76,-40},{-140,-40},{-140,-41},
+          {-141,-41}},          color={255,0,255}));
+  connect(hea, sigBus.hea)
+    annotation (Line(points={{-152,-70},{-128,-70},{-128,-40},{-134,-40},{-134,-41},
+          {-141,-41}}, color={255,0,255}));
+  connect(eff.QUse_flow, refCycIneCon.y) annotation (Line(points={{98,37},{48,37},
+          {48,66},{8.88178e-16,66},{8.88178e-16,61}}, color={0,0,127}));
+  connect(eff.hea, sigBus.hea) annotation (Line(points={{98,30},{48,30},{48,0},{
+          26,0},{26,-30},{-20,-30},{-20,-41},{-141,-41}}, color={255,0,255}),
+      Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  annotation (Icon(coordinateSystem(extent={{-100,-100},{100,100}}), graphics={
+          Text(
+          extent={{-100,-12},{-72,-30}},
+          textColor={255,85,255},
+          visible=not use_busConOnl and use_rev,
+          textString="hea")}),
+    Diagram(coordinateSystem(extent={{-140,-160},{140,160}})),
+    Documentation(revisions="
+<html>
+<ul>
+  <li>
+    May 2, 2024, by Michael Wetter:<br/>
+    Refactored check for device identifiers.<br/>
+    This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">IBPSA, #1576</a>.
+  </li>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adjusted based on the discussion in this issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>May 22, 2019</i> by Julian Matthes:<br/>
+    Rebuild due to the introducion of the thermal machine partial model
+    (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/715\">AixLib #715</a>)
+  </li>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Model of a reversible, modular heat pump.
+  This models allows combining any of the available modules
+  for refrigerant heating or cooling cycles, inertias,
+  heat losses, and safety controls.
+  All features are optional.
+</p>
+<p>
+  Adding to the partial model (
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialReversibleRefrigerantMachine\">
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.PartialReversibleRefrigerantMachine</a>),
+  this model has the <code>hea</code> signal to choose
+  the operation mode of the heat pump.
+</p>
+<p>
+  For more information on the approach, see
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Modular;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/NoHeating.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/NoHeating.mo
new file mode 100644
index 0000000000..b858bcd72f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/NoHeating.mo
@@ -0,0 +1,43 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses;
+model NoHeating
+  "Placeholder to disable heating"
+  extends PartialHeatPumpCycle(
+    TEva_nominal=273.15,
+    TCon_nominal=273.15,
+    cpEva=4184,
+    cpCon=4184,
+    PEle_nominal=0,
+    redeclare final
+      AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+      iceFacCal,
+    devIde="NoHeating",
+    QHea_flow_nominal=0);
+  Modelica.Blocks.Sources.Constant constZer(final k=0)
+    "No heating, hence, zero"
+    annotation (Placement(transformation(extent={{-100,20},{-80,40}})));
+equation
+  connect(constZer.y, feeHeaFloEva.u1) annotation (Line(points={{-79,30},{-62,30},
+          {-62,4},{-94,4},{-94,-10},{-78,-10}},     color={0,0,127}));
+  connect(constZer.y, feeHeaFloEva.u2) annotation (Line(points={{-79,30},{-62,
+          30},{-62,4},{-94,4},{-94,-24},{-70,-24},{-70,-18}},
+        color={0,0,127}));
+  connect(constZer.y, redQCon.u2) annotation (Line(points={{-79,30},{-62,30},{-62,
+          4},{64,4},{64,-78}}, color={0,0,127}));
+  connect(constZer.y, PEle)
+    annotation (Line(points={{-79,30},{0,30},{0,-130}}, color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  Using this model, the heat pump will always be off.
+  This option is mainly used to avoid warnings about
+  partial model which must be replaced.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end NoHeating;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialCarnot.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialCarnot.mo
new file mode 100644
index 0000000000..2c748611bf
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialCarnot.mo
@@ -0,0 +1,134 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses;
+partial model PartialCarnot
+  "Model with components for Carnot efficiency calculation"
+  parameter Boolean useForChi "=false to use in heat pump models";
+  parameter Real etaCarnot_nominal=0.3 "Constant Carnot effectiveness";
+  parameter Boolean use_constAppTem=false
+    "=true to fix approach temperatures at nominal values. This can improve simulation speed";
+  parameter Modelica.Units.SI.TemperatureDifference TAppCon_nominal(min=0)
+    "Temperature difference between refrigerant and working fluid outlet in condenser"
+    annotation (Dialog(group="Efficiency"));
+
+  parameter Modelica.Units.SI.TemperatureDifference TAppEva_nominal(min=0)
+    "Temperature difference between refrigerant and working fluid outlet in evaporator"
+    annotation (Dialog(group="Efficiency"));
+  parameter Modelica.Units.SI.TemperatureDifference dTCarMin=5
+    "Minimal temperature difference, used to avoid division errors"
+     annotation(Dialog(tab="Advanced"));
+  Modelica.Blocks.Sources.RealExpression reaCarnotCOP(final y=TUseSidAct/
+        AixLib.Utilities.Math.Functions.smoothMax(
+        x1=dTCarMin,
+        x2=(TConAct - TEvaAct),
+        deltaX=0.25)) "Internal calculation of Carnot COP"
+    annotation (Placement(transformation(extent={{-100,60},{-80,80}})));
+  Modelica.Blocks.Math.MultiProduct
+                               proQUse_flow(nu=3)
+                                            "Calculate QUse_flow" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-50,50})));
+  Modelica.Blocks.Math.Product proPEle "Calculate electrical power consumption" annotation (
+     Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={70,50})));
+  Modelica.Blocks.Sources.Constant constPEle
+    "Constant electrical power consumption" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={88,90})));
+  Modelica.Blocks.Routing.RealPassThrough pasThrYMea "From signal bus"
+    annotation (Placement(transformation(extent={{20,60},{40,80}})));
+  Modelica.Units.SI.Temperature TUseSidAct = if useForChi then TEvaAct else TConAct
+    "Useful side refrigerant temperature";
+  Modelica.Units.SI.Temperature TConAct = pasThrTCon.y + TAppCon
+    "Refrigerant condensation temperature";
+  Modelica.Units.SI.Temperature TEvaAct = pasThrTEva.y - TAppEva
+    "Refrigerant evaporation temperature";
+  Modelica.Units.SI.TemperatureDifference TAppCon = if use_constAppTem then TAppCon_nominal
+      else TAppCon_nominal * QCon_flow_internal/QCon_flow_nominal
+      "Condenser approach temperature";
+  Modelica.Units.SI.TemperatureDifference TAppEva = if use_constAppTem then TAppEva_nominal
+      else TAppEva_nominal * QEva_flow_internal/QEva_flow_nominal
+      "Evaporator approach temperature ";
+  Modelica.Blocks.Sources.Constant constZer(final k=0)
+    "Constant zero value if off" annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,10})));
+  Modelica.Blocks.Logical.Switch swiPEle
+    "If device is off, no heat exchange occurs" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=-90,
+        origin={50,10})));
+  Modelica.Blocks.Logical.Switch swiQUse
+    "If device is off, no heat exchange occurs" annotation (Placement(
+        transformation(
+        extent={{-10,10},{10,-10}},
+        rotation=-90,
+        origin={-50,10})));
+
+  Modelica.Blocks.Routing.RealPassThrough pasThrTEva
+    "Evaporator outlet pass through" annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-70,90})));
+  Modelica.Blocks.Routing.RealPassThrough pasThrTCon
+    "Condenser outlet pass through" annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-30,90})));
+  Modelica.Blocks.Sources.RealExpression reaCarnotEff(y=etaCarnot_nominal)
+    "Internal calculation of Carnot effectiveness"
+    annotation (Placement(transformation(extent={{-100,40},{-80,60}})));
+protected
+  parameter Modelica.Units.SI.HeatFlowRate QCon_flow_nominal
+    "Nominal condenser heat flow rate";
+  parameter Modelica.Units.SI.HeatFlowRate QEva_flow_nominal
+    "Nominal evaporator heat flow rate";
+  Modelica.Units.SI.HeatFlowRate QCon_flow_internal = if useForChi then
+    swiPEle.y - swiQUse.y else swiQUse.y
+    "Condenser heat flow rate";
+  Modelica.Units.SI.HeatFlowRate QEva_flow_internal = if useForChi then
+    swiQUse.y else swiPEle.y - swiQUse.y
+     "Evaporator heat flow rate";
+
+equation
+  connect(proPEle.u1, constPEle.y) annotation (Line(points={{76,62},{76,66},{88,
+          66},{88,79}}, color={0,0,127}));
+  connect(pasThrYMea.y, proPEle.u2)
+    annotation (Line(points={{41,70},{64,70},{64,62}}, color={0,0,127}));
+  connect(constZer.y, swiPEle.u3) annotation (Line(points={{8.88178e-16,21},{
+          8.88178e-16,28},{42,28},{42,22}}, color={0,0,127}));
+  connect(proPEle.y, swiPEle.u1) annotation (Line(points={{70,39},{70,34},{58,
+          34},{58,22}}, color={0,0,127}));
+  connect(proQUse_flow.y, swiQUse.u1) annotation (Line(points={{-50,38.3},{-50,36},
+          {-58,36},{-58,22}}, color={0,0,127}));
+  connect(swiQUse.u3, constZer.y) annotation (Line(points={{-42,22},{-42,28},{
+          8.88178e-16,28},{8.88178e-16,21}}, color={0,0,127}));
+  connect(reaCarnotCOP.y, proQUse_flow.u[1]) annotation (Line(points={{-79,70},{
+          -52.3333,70},{-52.3333,60}}, color={0,0,127}));
+  connect(proPEle.y, proQUse_flow.u[2]) annotation (Line(points={{70,39},{70,34},
+          {-26,34},{-26,70},{-50,70},{-50,60}}, color={0,0,127}));
+  connect(reaCarnotEff.y, proQUse_flow.u[3]) annotation (Line(points={{-79,50},{
+          -68,50},{-68,70},{-47.6667,70},{-47.6667,60}}, color={0,0,127}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,
+            -120},{120,120}})),
+      Documentation(info="<html>
+<p>
+  Partial model for equations and componenents used in both heat pump
+  and chiller with the Carnot approach.
+</p>
+</html>", revisions="<html>
+<ul><li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li></ul>
+</html>"),
+    Icon(coordinateSystem(extent={{-120,-120},{120,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialCarnot;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialHeatPumpCycle.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialHeatPumpCycle.mo
new file mode 100644
index 0000000000..06d6e5ca02
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialHeatPumpCycle.mo
@@ -0,0 +1,48 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses;
+partial model PartialHeatPumpCycle
+  "Partial model to allow selection of only heat pump options"
+  extends PartialRefrigerantCycle;
+  parameter Modelica.Units.SI.HeatFlowRate QHea_flow_nominal
+    "Nominal heating capacity"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Boolean useInHeaPum
+    "=false to indicate that this model is used in a chiller";
+  Modelica.Blocks.Math.Feedback feeHeaFloEva
+    "Calculates evaporator heat flow with total energy balance" annotation (
+      Placement(transformation(extent={{-80,-20},{-60,0}}, rotation=0)));
+equation
+  connect(iceFacCal.iceFac, sigBus.icefacHPMea) annotation (Line(points={{-81.2,
+          -50},{-64,-50},{-64,-28},{-110,-28},{-110,120},{1,120}},
+                                                              color={0,0,127}),
+      Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(feeHeaFloEva.y, proRedQEva.u2)
+    annotation (Line(points={{-61,-10},{-24,-10},{-24,-78}}, color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  Partial refrigerant cycle model for heat pumps.
+  It adds the specification for frosting calculation
+  and restricts to the intended choices under
+  <code>choicesAllMatching</code>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adapted based on AixLib implementation. Mainly, the iceFac is added directly
+    in this partial model (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialHeatPumpCycle;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialRefrigerantCycle.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialRefrigerantCycle.mo
new file mode 100644
index 0000000000..e7cad297bf
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialRefrigerantCycle.mo
@@ -0,0 +1,133 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses;
+partial model PartialRefrigerantCycle
+  "Partial model of refrigerant cycle"
+  parameter Modelica.Units.SI.Power PEle_nominal
+    "Nominal electrical power consumption"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.Temperature TCon_nominal
+    "Nominal temperature at secondary condenser side"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.Temperature TEva_nominal
+    "Nominal temperature at secondary evaporator side"
+    annotation (Dialog(group="Nominal condition"));
+  parameter String devIde=""
+    "Indicates the data source, used to warn users
+    about different vapor compression devices in reversible models";
+
+  replaceable AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting iceFacCal
+  constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.BaseClasses.PartialIcingFactor
+    "Replaceable model to calculate the icing factor" annotation (
+    choicesAllMatching=true,
+    Dialog(group="Frosting supression"),
+    Placement(transformation(extent={{-98,-58},{-82,-42}})));
+  parameter Modelica.Units.SI.SpecificHeatCapacity cpCon
+    "Evaporator medium specific heat capacity"
+    annotation (Dialog(tab="Advanced", group="Medium properties"));
+  parameter Modelica.Units.SI.SpecificHeatCapacity cpEva
+    "Evaporator medium specific heat capacity"
+    annotation (Dialog(tab="Advanced", group="Medium properties"));
+  Modelica.Blocks.Interfaces.RealOutput PEle(final unit="W")
+    "Electrical Power consumed by the device" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={0,-130})));
+  Modelica.Blocks.Interfaces.RealOutput QCon_flow(final unit="W")
+  "Heat flow rate through condenser" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-80,-130})));
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantMachineControlBus sigBus
+    "Bus-connector" annotation (Placement(transformation(
+        extent={{-15,-14},{15,14}},
+        rotation=0,
+        origin={1,120})));
+  Modelica.Blocks.Interfaces.RealOutput QEva_flow(final unit="W")
+    "Heat flow rate through evaporator" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={80,-130})));
+  Modelica.Blocks.Math.Add redQCon(final k1=-1, final k2=+1)
+    "Reduce heat flow to the condenser based on the reduction to the evaporator"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={70,-90})));
+  Modelica.Blocks.Math.Product proRedQEva
+    "Reduce heat flow to the evaporator based on the icing factor"
+    annotation (Placement(transformation(
+        extent={{-10,10},{10,-10}},
+        rotation=270,
+        origin={-30,-90})));
+
+equation
+  connect(proRedQEva.y, QEva_flow) annotation (Line(points={{-30,-101},{-30,-108},
+          {80,-108},{80,-130}},color={0,0,127}));
+  connect(proRedQEva.y, redQCon.u1) annotation (Line(points={{-30,-101},{-30,-108},
+          {2,-108},{2,-72},{76,-72},{76,-78}},color={0,0,127}));
+  connect(redQCon.y, QCon_flow) annotation (Line(points={{70,-101},{70,-116},{-80,
+          -116},{-80,-130}},color={0,0,127}));
+  connect(iceFacCal.iceFac, proRedQEva.u1)
+    annotation (Line(points={{-81.2,-50},{-36,-50},{-36,-78}},
+                                                             color={0,0,127}));
+  connect(iceFacCal.sigBus, sigBus) annotation (Line(
+      points={{-98.08,-50},{-110,-50},{-110,120},{1,120}},
+      color={255,204,51},
+      thickness=0.5));
+  annotation (Icon(coordinateSystem(extent={{-120,-120},
+            {120,120}}),                                        graphics={
+                                Rectangle(
+        extent={{-120,-120},{120,120}},
+        lineColor={0,0,255},
+        fillColor={255,255,255},
+        fillPattern=FillPattern.Solid),   Text(
+          extent={{-57.5,-35},{57.5,35}},
+          pattern=LinePattern.Dash,
+          textString="%name", origin={2.5,153},
+          rotation=180)}),Diagram(coordinateSystem(extent={
+            {-120,-120},{120,120}})),
+    Documentation(revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    Adapted based on AixLib implementation. Mainly, the iceFac is added directly
+    in this partial model (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+  <li>
+    November 26, 2018 by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Partial model for calculation of electrical power consumption
+  <code>PEle</code>, condenser heat flow <code>QCon_flow</code>
+  and evaporator heat flow <code>QEva_flow</code> based on the
+  values in the <code>sigBus</code> for a refrigerant machine.
+</p>
+<h4>Frosting performance</h4>
+<p>
+  To simulate possible icing of the evaporator on air-source devices, the
+  icing factor <code>iceFac</code> is used to influence the outputs.
+  The factor models the reduction of heat transfer between refrigerant
+  and source. Thus, the factor is implemented as follows:
+</p>
+<p>
+  <code>QEva_flow = iceFac * (QConNoIce_flow - PEle)</code>
+</p>
+<p>
+  With <code>iceFac</code> as a relative value between 0 and 1:</p>
+<p><code>iceFac = kA/kA_noIce</code></p>
+<p>Finally, the energy balance must still hold:</p>
+<p><code>QCon_flow = PEle + QEva_flow</code> </p>
+<p>
+  You can select different options for the modeling of the icing factor or
+  implement your own approach.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialRefrigerantCycle;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialTableData2D.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialTableData2D.mo
new file mode 100644
index 0000000000..256324c608
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/PartialTableData2D.mo
@@ -0,0 +1,190 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses;
+partial model PartialTableData2D
+  "Partial model with components for TableData2D approach for heat pumps and chillers"
+  parameter Real scaFac "Scaling factor";
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_nominal
+    "Nominal mass flow rate in secondary condenser side"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.MassFlowRate mEva_flow_nominal
+    "Nominal mass flow rate in secondary evaporator side"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Blocks.Types.Smoothness smoothness=
+    Modelica.Blocks.Types.Smoothness.LinearSegments
+    "Smoothness of table interpolation";
+  parameter Modelica.Blocks.Types.Extrapolation extrapolation=
+    Modelica.Blocks.Types.Extrapolation.LastTwoPoints
+    "Extrapolation of data outside the definition range";
+  parameter Boolean use_TEvaOutForTab=true
+    "=true to use evaporator outlet temperature, false for inlet";
+  parameter Boolean use_TConOutForTab=true
+    "=true to use condenser outlet temperature, false for inlet";
+  Modelica.Blocks.Tables.CombiTable2Ds tabPEle(
+    final tableOnFile=false,
+    final tableName="NoName",
+    final fileName="NoName",
+    final verboseRead=true,
+    final smoothness=smoothness,
+    final u1(unit="K", displayUnit="degC"),
+    final u2(unit="K", displayUnit="degC"),
+    final y(unit="W"),
+    final extrapolation=extrapolation) "Electrical power consumption table" annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=-90,
+        origin={90,50})));
+  Modelica.Blocks.Tables.CombiTable2Ds tabQUse_flow(
+    final tableOnFile=false,
+    final tableName="NoName",
+    final fileName="NoName",
+    final verboseRead=true,
+    final smoothness=smoothness,
+    final u1(unit="K", displayUnit="degC"),
+    final u2(unit="K", displayUnit="degC"),
+    final y(unit="W"),
+    final extrapolation=extrapolation) "Table for useful heat flow rate"
+                                       annotation (Placement(transformation(
+          extent={{-10,-10},{10,10}}, rotation=-90,
+        origin={50,50})));
+  Modelica.Blocks.Math.Product yMeaTimScaFac
+    "Create the product of the scaling factor and relative compressor speed"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=-90,
+        origin={-60,50})));
+
+
+  Modelica.Blocks.Math.Product scaFacTimPel "Scale electrical power consumption"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=-90,
+        origin={-40,2})));
+  Modelica.Blocks.Math.Product scaFacTimQUse_flow "Scale useful heat flow rate"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=-90,
+        origin={40,2})));
+  Modelica.Blocks.Sources.Constant constScaFac(final k=scaFac)
+    "Calculates correction of table output based on scaling factor"
+    annotation (Placement(
+        transformation(extent={{-10,-10},{10,10}}, rotation=0,
+        origin={-90,70})));
+
+
+  Modelica.Blocks.Routing.RealPassThrough reaPasThrTEvaIn if (not useInRevDev and not use_TEvaOutForTab) or (useInRevDev and not use_TConOutForTab)
+    "Used to enable conditional bus connection" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-50,90})));
+  Modelica.Blocks.Routing.RealPassThrough reaPasThrTConIn if (not useInRevDev and not use_TConOutForTab) or (useInRevDev and not use_TEvaOutForTab)
+    "Used to enable conditional bus connection" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={50,90})));
+  Modelica.Blocks.Routing.RealPassThrough reaPasThrTEvaOut if (not useInRevDev and use_TEvaOutForTab) or (useInRevDev and use_TConOutForTab)
+    "Used to enable conditional bus connection" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={-10,90})));
+  Modelica.Blocks.Routing.RealPassThrough reaPasThrTConOut if (not useInRevDev and use_TConOutForTab) or (useInRevDev and use_TEvaOutForTab)
+    "Used to enable conditional bus connection" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=270,
+        origin={90,90})));
+
+protected
+  parameter Boolean useInRevDev "=true to indicate usage in reversed operation";
+  parameter Integer numRow=size(tabPEle.table, 1) "Number of rows in table";
+  parameter Integer numCol=size(tabPEle.table, 2) "Number of columns in table";
+  parameter Modelica.Units.SI.TemperatureDifference dTMin=3
+    "Minimal temperature spread according to EN 14511";
+  parameter Modelica.Units.SI.TemperatureDifference dTMax=10
+    "Maximal temperature spread according to EN 14511";
+  parameter Modelica.Units.SI.Power valTabPEle[numRow-1, numCol - 1]=
+    {{tabPEle.table[j, i] for i in 2:numCol} for j in 2:numRow}
+    "Table with electrical power values only";
+  parameter Modelica.Units.SI.HeatFlowRate valTabQCon_flow[numRow-1, numCol - 1]
+    "Table with condenser heat flow values only";
+  parameter Modelica.Units.SI.HeatFlowRate valTabQEva_flow[numRow-1, numCol - 1]
+    "Table with evaporator heat flow values only";
+  parameter Modelica.Blocks.Types.ExternalCombiTable2D tabIdeQUse_flow=
+      Modelica.Blocks.Types.ExternalCombiTable2D(
+      "NoName",
+      "NoName",
+      tabQUse_flow.table,
+      smoothness,
+      extrapolation,
+      false) "External table object for nominal useful side conditions";
+  parameter Modelica.Blocks.Types.ExternalCombiTable2D tabIdePEle=
+      Modelica.Blocks.Types.ExternalCombiTable2D(
+      "NoName",
+      "NoName",
+      tabPEle.table,
+      smoothness,
+      extrapolation,
+      false) "External table object for nominal electrical power consumption";
+  parameter Modelica.Units.SI.MassFlowRate mEva_flow_min
+    "Minimal evaporator mass flow rate";
+  parameter Modelica.Units.SI.MassFlowRate mEva_flow_max
+    "Maximal evaporator mass flow rate";
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_min
+    "Minimal evaporator mass flow rate";
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_max
+    "Maximal evaporator mass flow rate";
+initial algorithm
+  assert(mCon_flow_nominal >= mCon_flow_min,
+    "In " + getInstanceName() + ": The nominal condenser mass flow rate ("
+    + String(mCon_flow_nominal) + " kg/s) is smaller than the 
+    minimal value (" + String(mCon_flow_min) + " kg/s) for the table data 
+    when assuming a temperature spread between 3 and 10 K, as in EN 14511.",
+    AssertionLevel.warning);
+  assert(mCon_flow_nominal <= mCon_flow_max,
+    "In " + getInstanceName() + ": The nominal condenser mass flow rate ("
+    + String(mCon_flow_nominal) + " kg/s) is bigger than the 
+    maximal value (" + String(mCon_flow_max) + " kg/s) for the table data 
+    when assuming a temperature spread between 3 and 10 K, as in EN 14511.",
+    AssertionLevel.warning);
+  assert(mEva_flow_nominal >= mEva_flow_min,
+    "In " + getInstanceName() + ": The nominal evaporator mass flow rate ("
+    + String(mEva_flow_nominal) + " kg/s) is smaller than the 
+    minimal value (" + String(mEva_flow_min) + " kg/s) for the table data 
+    when assuming a temperature spread between 3 and 10 K, as in EN 14511.",
+    AssertionLevel.warning);
+  assert(mEva_flow_nominal <= mEva_flow_max,
+    "In " + getInstanceName() + ": The nominal evaporator mass flow rate ("
+    + String(mEva_flow_nominal) + " kg/s) is bigger than the 
+    maximal value (" + String(mEva_flow_max) + " kg/s) for the table data 
+    when assuming a temperature spread between 3 and 10 K, as in EN 14511.",
+    AssertionLevel.warning);
+equation
+  connect(constScaFac.y,yMeaTimScaFac. u2)
+    annotation (Line(points={{-79,70},{-66,70},{-66,62}}, color={0,0,127}));
+  connect(scaFacTimPel.u2,yMeaTimScaFac. y) annotation (Line(points={{-46,14},{
+          -46,20},{-60,20},{-60,39}},
+                                  color={0,0,127}));
+  connect(tabQUse_flow.y, scaFacTimQUse_flow.u1) annotation (Line(points={{50,39},
+          {50,32},{46,32},{46,14}}, color={0,0,127}));
+  connect(scaFacTimQUse_flow.u2,yMeaTimScaFac. y) annotation (Line(points={{34,14},
+          {34,20},{-60,20},{-60,39}}, color={0,0,127}));
+  connect(tabPEle.y, scaFacTimPel.u1) annotation (Line(points={{90,39},{90,26},{
+          -34,26},{-34,14}}, color={0,0,127}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,
+            -120},{120,120}})),
+    Documentation(info="<html>
+<p>
+  Partial model for equations and componenents used in both heat pump
+  and chiller models using two-dimensional data.
+</p>
+</html>", revisions="<html>
+<ul><li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li></ul>
+</html>"),
+    Icon(coordinateSystem(extent={{-120,-120},{120,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialTableData2D;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/package.mo
new file mode 100644
index 0000000000..76679407f0
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/package.mo
@@ -0,0 +1,32 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle;
+package BaseClasses "Package with partial classes of Performance Data"
+annotation (Icon(graphics={
+        Rectangle(
+          lineColor={200,200,200},
+          fillColor={248,248,248},
+          fillPattern=FillPattern.HorizontalCylinder,
+          extent={{-100.0,-100.0},{100.0,100.0}},
+          radius=25.0),
+        Rectangle(
+          lineColor={128,128,128},
+          extent={{-100.0,-100.0},{100.0,100.0}},
+          radius=25.0),
+        Ellipse(
+          extent={{-30.0,-30.0},{30.0,30.0}},
+          lineColor={128,128,128},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid)}), Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This package contains base classes for the package <a href=
+  \"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle</a>.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/package.order
new file mode 100644
index 0000000000..473c08dd36
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/BaseClasses/package.order
@@ -0,0 +1,5 @@
+NoHeating
+PartialCarnot
+PartialHeatPumpCycle
+PartialRefrigerantCycle
+PartialTableData2D
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/ConstantCarnotEffectiveness.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/ConstantCarnotEffectiveness.mo
new file mode 100644
index 0000000000..b5892b74fe
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/ConstantCarnotEffectiveness.mo
@@ -0,0 +1,142 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle;
+model ConstantCarnotEffectiveness "Carnot COP with a constant Carnot effectiveness"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle(
+      useInHeaPum=true,
+      PEle_nominal=QHea_flow_nominal / COP_nominal,
+      devIde="ConstantCarnotEffectiveness");
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialCarnot(
+     TAppCon_nominal=if cpCon < 1500 then 5 else 2,
+     TAppEva_nominal=if cpEva < 1500 then 5 else 2,
+     final useForChi=false,
+     final QEva_flow_nominal=PEle_nominal-QHea_flow_nominal,
+     final QCon_flow_nominal=QHea_flow_nominal,
+     constPEle(final k=PEle_nominal));
+  parameter Real COP_nominal(
+    min=0,
+    final unit="1") = etaCarnot_nominal*(TCon_nominal + TAppCon_nominal)/(
+    TCon_nominal + TAppCon_nominal - (TEva_nominal - TAppEva_nominal))
+    "Nominal coefficient of performance";
+equation
+
+  connect(pasThrYMea.u, sigBus.yMea) annotation (Line(points={{18,70},{0,70},{0,
+          118},{2,118},{2,120},{1,120}},
+                 color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  if useInHeaPum then
+    connect(pasThrTCon.u, sigBus.TConOutMea) annotation (Line(points={{-30,102},{
+            -30,120},{1,120}},
+                           color={0,0,127}), Text(
+        string="%second",
+        index=1,
+        extent={{-6,3},{-6,3}},
+        horizontalAlignment=TextAlignment.Right));
+    connect(pasThrTEva.u, sigBus.TEvaOutMea) annotation (Line(points={{-70,102},{
+            -70,120},{1,120}},
+                           color={0,0,127}), Text(
+        string="%second",
+        index=1,
+        extent={{6,3},{6,3}},
+        horizontalAlignment=TextAlignment.Left));
+  else
+    connect(pasThrTCon.u, sigBus.TEvaOutMea) annotation (Line(points={{-30,102},{
+            -30,120},{1,120}},
+                           color={0,0,127}), Text(
+        string="%second",
+        index=1,
+        extent={{-6,3},{-6,3}},
+        horizontalAlignment=TextAlignment.Right));
+    connect(pasThrTEva.u, sigBus.TConOutMea) annotation (Line(points={{-70,102},{
+            -70,120},{1,120}},
+                           color={0,0,127}), Text(
+        string="%second",
+        index=1,
+        extent={{6,3},{6,3}},
+        horizontalAlignment=TextAlignment.Left));
+  end if;
+  connect(swiPEle.y, redQCon.u2) annotation (Line(points={{50,-1},{50,-26},{62,
+          -26},{62,-78},{64,-78}}, color={0,0,127}));
+  connect(swiPEle.y, PEle) annotation (Line(points={{50,-1},{50,-92},{0,-92},{0,
+          -130}}, color={0,0,127}));
+  connect(swiQUse.u2, sigBus.onOffMea) annotation (Line(points={{-50,22},{-50,30},
+          {0,30},{0,122},{1,122},{1,120}},
+                               color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(swiPEle.u2, sigBus.onOffMea) annotation (Line(points={{50,22},{50,46},{
+          0,46},{0,118},{2,118},{2,120},{1,120}},
+                           color={255,0,255}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(swiPEle.y, feeHeaFloEva.u1) annotation (Line(points={{50,-1},{50,-24},{
+          -90,-24},{-90,-10},{-78,-10}}, color={0,0,127}));
+  connect(feeHeaFloEva.u2, swiQUse.y)
+    annotation (Line(points={{-70,-18},{-50,-18},{-50,-1}}, color={0,0,127}));
+  annotation (Documentation(revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This model uses a constant Carnot effectiveness
+  to compute the efficiency of the heat pump.
+</p>
+<p>
+  <code>PEle_nominal</code> is computed from the provided
+  <code>QHea_flow_nominal</code> and other nominal conditions.
+  <code>PEle_nominal</code> stays constant over all boundary conditions
+  and is used to calculate <code>PEle</code> by multiplying it with the
+  relative compressor speed.
+  <code>QCon_flow</code> is computed using the Carnot approach:
+</p>
+<p>
+  <code>
+    QCon_flow = PEle_nominal * etaCarnot_nominal * yMea *
+    (TConOut + TAppCon) /
+    (TConOut + TAppCon - (TEvaOut - TAppEva))
+  </code>
+</p>
+<p>
+  <code>
+    PEle = PEle_nominal * yMea
+  </code>
+</p>
+<p>
+  This equations follows the Carnot approach of the AixLib library:
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">
+  AixLib.Fluid.HeatPumps.Carnot_y</a>
+  Similarly, the variables <code>TAppCon</code> and
+  <code>TAppEva</code> define the approach (pinch) temperature differences.
+</p>
+<p>
+  The approach temperatures
+  are calculated using the following equation:
+</p>
+<p>
+  <code>
+  TApp = TApp_nominal * Q_flow / Q_flow_nominal
+  </code>
+</p>
+<p>
+  This introduces nonlinear equations to the model, which
+  can lead to solver issues for reversible operation.
+  You can fix the approach temperature at the nominal value by
+  setting <code>use_constAppTem</code>
+</p>
+</html>"), Icon(graphics={Text(
+          extent={{-78,80},{74,-66}},
+          textColor={0,0,127},
+          textString="Carnot")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ConstantCarnotEffectiveness;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/PartialIcingFactor.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/PartialIcingFactor.mo
new file mode 100644
index 0000000000..915f427e4c
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/PartialIcingFactor.mo
@@ -0,0 +1,44 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.BaseClasses;
+partial model PartialIcingFactor "Partial model to calculate the icing factor"
+  extends Modelica.Blocks.Icons.Block;
+
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantMachineControlBus sigBus
+    "Bus-connector used in a heat pump" annotation (Placement(transformation(
+        extent={{-15,-14},{15,14}},
+        rotation=0,
+        origin={-101,0})));
+  Modelica.Blocks.Interfaces.RealOutput iceFac(final unit="1", min=0, max=1)
+    "Icing factor from 0 to 1 to estimate influence of icing"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={110,0})));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)),
+   Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+Partial model to calculate the icing factor based on the data available in the
+  signal bus <code>sigBus</code> of the heat pump.
+</p>
+<p>
+The icing factor is a heat transfer modifier between <i>0</i> and <i>1</i>, whereas
+<i>0</i> indicates no heat transfer occurs and
+<i>1</i> indicates the heat transfer is unaffected.
+</p>
+<p>
+  See the documentation of <a href=
+  \"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle</a>
+  for further information.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialIcingFactor;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/package.mo
new file mode 100644
index 0000000000..8a390c9f9f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/package.mo
@@ -0,0 +1,8 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting;
+package BaseClasses
+extends Modelica.Icons.BasesPackage;
+
+annotation (Documentation(info="<html>
+<p>Package with the partial icing factor model.</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/package.order
new file mode 100644
index 0000000000..4f0c4fa391
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/BaseClasses/package.order
@@ -0,0 +1 @@
+PartialIcingFactor
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/FunctionalIcingFactor.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/FunctionalIcingFactor.mo
new file mode 100644
index 0000000000..3e08420cc0
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/FunctionalIcingFactor.mo
@@ -0,0 +1,93 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting;
+model FunctionalIcingFactor
+  "Estimate the frosting supression using a function"
+  extends BaseClasses.PartialIcingFactor;
+
+  replaceable function icingFactor =
+      AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.Functions.partialIcingFactor
+    constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.Functions.partialIcingFactor
+    "Replaceable function to calculate current icing factor"
+    annotation(choicesAllMatching=true);
+protected
+  Modelica.Blocks.Routing.RealPassThrough pasThrTEvaIn
+    "Enable usage of bus variables in function call"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+  Modelica.Blocks.Routing.RealPassThrough pasThrTEvaOut
+    "Enable usage of bus variables in function call"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  Modelica.Blocks.Routing.RealPassThrough pasThrMasFlowEva
+    "Enable usage of bus variables in function call"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+
+  Modelica.Blocks.Sources.RealExpression ice(
+    final y=icingFactor(
+      pasThrTEvaIn.y,
+      pasThrTEvaOut.y,
+      pasThrMasFlowEva.y)) "Icing factor"
+    annotation (Placement(transformation(extent={{60,-10},{80,10}})));
+equation
+  connect(pasThrTEvaOut.u, sigBus.TEvaOutMea) annotation (Line(points={{-12,-30},
+          {-54,-30},{-54,0},{-101,0}},
+                            color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(pasThrTEvaIn.u, sigBus.TEvaInMea) annotation (Line(points={{-12,30},{-54,30},{
+          -54,0},{-101,0}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(pasThrMasFlowEva.u, sigBus.mEvaMea_flow) annotation (Line(points={{-12,0},
+          {-101,0}},        color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(ice.y, iceFac)
+    annotation (Line(points={{81,0},{110,0}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Text(
+          extent={{-151,147},{149,107}},
+          textColor={0,0,255},
+          fillPattern=FillPattern.HorizontalCylinder,
+          fillColor={0,127,255},
+          textString="%name"),
+        Ellipse(
+          lineColor = {108,88,49},
+          fillColor = {255,215,136},
+          fillPattern = FillPattern.Solid,
+          extent = {{-100,-100},{100,100}}),
+        Text(
+          textColor={108,88,49},
+          extent={{-90.0,-90.0},{90.0,90.0}},
+          textString="f")}),                                     Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+    <ul>
+    <li>
+    <>December 7, 2023, by Michael Wetter:<br/>
+    Changed implementation to use graphical models.
+    </li>
+    <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Model using functional approaches for calculation of the icing factor.
+  The replaceable function uses the inputs on the evaporator side to calculate
+  the resulting icing factor.
+</p>
+<p>
+  For more information, see the documentation of <a href=
+  \"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle</a>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FunctionalIcingFactor;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/package.mo
new file mode 100644
index 0000000000..1f52fd2e7d
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/package.mo
@@ -0,0 +1,19 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting;
+package Functions "Package with functions to calculate current icing factor on evaporator"
+
+annotation (Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This package contains functions for calculation of an icing factor
+  used in <a href=
+  \"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.FunctionalIcingFactor\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.FunctionalIcingFactor</a>.
+</p>
+</html>"));
+end Functions;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/package.order
new file mode 100644
index 0000000000..fd08706167
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/package.order
@@ -0,0 +1,2 @@
+partialIcingFactor
+wetterAfjei1997
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/partialIcingFactor.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/partialIcingFactor.mo
new file mode 100644
index 0000000000..e69c3c5b14
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/partialIcingFactor.mo
@@ -0,0 +1,43 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.Functions;
+partial function partialIcingFactor
+  "Base function for all icing factor functions"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.ThermodynamicTemperature TEvaInMea
+    "Evaporator supply temperature. Should be equal to outdoor air temperature";
+  input Modelica.Units.SI.ThermodynamicTemperature TEvaOutMea
+    "Evaporator return temperature";
+  input Modelica.Units.SI.MassFlowRate mEva_flow
+    "Mass flow rate at the evaporator";
+  output Real iceFac(final unit="1", min=0, max=1)
+    "Icing factor (0: no heat transfer; 1: no effect)";
+
+  annotation (Documentation(revisions="<html><ul>
+  <li>
+    <i>November 26, 2018,</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  Base function for calculation of the icing factor <code>iceFac</code>.
+  It represents the reduction of heat exchange as a result of icing of
+  the evaporator.
+</p>
+<p>
+  This function is used in the model <a href=
+  \"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.FunctionalIcingFactor\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.FunctionalIcingFactor</a>.
+</p>
+<p>
+  Typically, functions should only require evaporator side data for calculation of
+  the <code>iceFac</code>.
+</p>
+<p>
+For more information on the <code>iceFac</code>, see the documentation of <a href=
+\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle\">
+AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle</a>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end partialIcingFactor;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/wetterAfjei1997.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/wetterAfjei1997.mo
new file mode 100644
index 0000000000..13f052b703
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/Functions/wetterAfjei1997.mo
@@ -0,0 +1,57 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.Functions;
+function wetterAfjei1997
+  "Correction of COP for icing and defrost according to Wetter, Afjei and Glass"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.Functions.partialIcingFactor;
+protected
+  parameter Real offLin=0.03 "First factor for linear term, offset";
+  parameter Real sloLin=-0.004 "Second factor for linear term, slope";
+  parameter Real gauFac=0.1534 "Parameter for gaussian curve, factor";
+  parameter Real gauMea=0.8869 "Parameter for gaussian curve, mean";
+  parameter Real gauSig=26.06 "Parameter for gaussian curve, sigma";
+  Real fac "Probability of icing";
+  Real linTer "Linear part of equation";
+  Real gauTer "Gaussian part of equation";
+algorithm
+  linTer :=offLin + sloLin*TEvaInMea;
+  gauTer :=gauFac*Modelica.Math.exp(-(TEvaInMea - gauMea)*(TEvaInMea - gauMea)/
+    gauSig);
+  fac := gauTer + AixLib.Utilities.Math.Functions.smoothMax(
+    x1=1E-5,
+    x2= linTer,
+    deltaX=0.25E-5);
+  iceFac:=1 - fac;
+  annotation (Documentation(info="<html>
+<p>
+  Correction of the coefficient of performance due to
+  icing/frosting according to Wetter, Afjei and Glass (1997).
+</p>
+<p>
+  For more information on the <code>iceFac</code>, see the documentation of <a href=
+  \"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle</a>
+</p>
+<h4>References</h4>
+<p>
+Thomas Afjei, Michael Wetter and Andrew Glass.<br/>
+TRNSYS type: Dual-stage compressor heat pump including frost and cycle losses. Model description and implementation in TRNSYS.</br>
+TRNSYS user meeting, November 1997, Stuttgart, Germany.<br/>
+<a href=\"https://simulationresearch.lbl.gov/wetter/download/type204_hp.pdf\">
+https://simulationresearch.lbl.gov/wetter/download/type204_hp.pdf</a>
+</p>
+</html>",
+  revisions="<html><ul>
+  <li>
+  December 7, 2023, by Michael Wetter:<br/>
+  Reformulated to make function once continuously differentiable, and to avoid
+  an event that is triggered based on <code>TEvaInMea</code>).
+  </li>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end wetterAfjei1997;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/NoFrosting.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/NoFrosting.mo
new file mode 100644
index 0000000000..2ce46f506e
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/NoFrosting.mo
@@ -0,0 +1,19 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting;
+model NoFrosting "Placeholder block to ignore frosting"
+  extends BaseClasses.PartialIcingFactor;
+equation
+  iceFac = 1;
+  annotation (Documentation(info="<html>
+<p>
+This block is used to ignore frosting effects by setting the icing factor
+to constant <i>1</i>.
+</p>
+</html>", revisions="<html>
+<ul><li>
+  <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+  First implementation (see issue <a href=
+  \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+</li></ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end NoFrosting;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/package.mo
new file mode 100644
index 0000000000..dbf2701c7e
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle;
+package Frosting "Package for models and function to estimate influence of frosting on heat pump performance"
+annotation (Documentation(info="<html>
+<p>Package with models to account for frosting of an air-source evaporator.</p>
+<p>
+  For more information on the <code>iceFac</code>, see the documentation of <a href=
+  \"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialRefrigerantCycle</a>
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"));
+end Frosting;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/package.order
new file mode 100644
index 0000000000..7f95da56c1
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Frosting/package.order
@@ -0,0 +1,4 @@
+FunctionalIcingFactor
+NoFrosting
+Functions
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/PartialInertia.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/PartialInertia.mo
new file mode 100644
index 0000000000..e2cab967cb
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/PartialInertia.mo
@@ -0,0 +1,25 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.BaseClasses;
+partial model PartialInertia "Partial inertia model"
+  extends Modelica.Blocks.Interfaces.SISO;
+
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+  Partial model for inertia.
+  This block is identical to
+  <a href=\"Modelica://Modelica.Blocks.Interfaces.SISO\">
+  Modelica.Blocks.Interfaces.SISO</a>
+  and is made to constrain the replaceable inertia module
+  within other inertia models.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialInertia;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/package.mo
new file mode 100644
index 0000000000..9e1f35d81c
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/package.mo
@@ -0,0 +1,8 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias;
+package BaseClasses
+  extends Modelica.Icons.BasesPackage;
+
+annotation (Documentation(info="<html>
+<p>This package contains partial model for inertia models.</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/package.order
new file mode 100644
index 0000000000..b06d71ae52
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/BaseClasses/package.order
@@ -0,0 +1 @@
+PartialInertia
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/NoInertia.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/NoInertia.mo
new file mode 100644
index 0000000000..28c1acca1e
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/NoInertia.mo
@@ -0,0 +1,24 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias;
+model NoInertia "No inertia"
+  extends BaseClasses.PartialInertia;
+equation
+  connect(u, y) annotation (Line(points={{-120,0},{110,0}}, color={0,0,127}));
+  annotation (Icon(graphics={Line(points={{-100,0},{102,0}}, color={0,0,127})}),
+      Documentation(info="<html>
+<p>
+  Placeholder model for no inertia.
+  This block is identical to
+  <a href=\"Modelica://Modelica.Blocks.Routing.RealPassThrough\">
+  Modelica.Blocks.Routing.RealPassThrough</a>
+  and is replaceable but constrained by other inertia modules.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end NoInertia;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/VariableOrder.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/VariableOrder.mo
new file mode 100644
index 0000000000..da3e903a54
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/VariableOrder.mo
@@ -0,0 +1,77 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias;
+model VariableOrder
+  "Inertia using a critical damper with variable order"
+  extends BaseClasses.PartialInertia;
+
+  parameter Modelica.Units.SI.Frequency refIneFreConst
+    "Cut off frequency for inertia of refrigerant cycle" annotation (
+      Dialog(group="Refrigerant inertia"));
+  parameter Integer nthOrd=1 "Order of refrigerant cycle interia"
+    annotation (Dialog(group="Refrigerant inertia"));
+  parameter Real x_start[nthOrd]=zeros(nthOrd)
+    "Initial or guess values of states" annotation (Dialog(
+      tab="Initialization",
+      group="Refrigerant inertia"));
+  parameter Real yRefIne_start=0 "Initial or guess value of output (= state)"
+    annotation (Dialog(tab="Initialization", group="Refrigerant inertia",
+      enable=initType == Modelica.Blocks.Types.Init.InitialOutput));
+  parameter Modelica.Blocks.Types.Init initType=Modelica.Blocks.Types.Init.NoInit
+    "Type of initialization (1: no init, 2:
+    steady state, 3: initial state, 4: initial output)";
+  Modelica.Blocks.Continuous.CriticalDamping criDam(
+    final n=nthOrd,
+    final f=refIneFreConst,
+    initType=initType,
+    final x_start=x_start) "Variable order damping model"
+    annotation (Placement(transformation(extent={{-16,-16},{16,16}})));
+
+equation
+  connect(u, criDam.u)
+    annotation (Line(points={{-120,0},{-19.2,0}}, color={0,0,127}));
+  connect(criDam.y, y)
+    annotation (Line(points={{17.6,0},{110,0}}, color={0,0,127}));
+  annotation (Documentation(info="<html>
+<p>
+  Model that uses a variable order delay to account for inertia.
+</p>
+<p>
+Following the associated publication by Wuellhorst et al. (2021),
+  this model was used to calibrate the heat pump model.
+  If first order is selected, the frequency <code>refIneFreConst</code>
+  equals the inverse of the time constant of a first order delay element.
+</p>
+<p>
+  In usage, be careful with the order of the delay.
+  While a second or third order delay may result in a better fit
+  in calibration, simulation speed is impacted.
+  See the discussion in the paper for more information:
+  <a href=\"https://doi.org/10.3384/ecp21181561\">
+  https://doi.org/10.3384/ecp21181561 </a></p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"), Icon(graphics={
+        Line(origin={-15.976,-8.521},
+          points = {{96.962,55.158},{16.42,50.489},{-18.988,18.583},
+          {-32.024,-53.479},{-62.024,-73.479}},
+          color = {0,0,127},
+          smooth = Smooth.Bezier),
+        Polygon(lineColor={192,192,192},
+          fillColor={192,192,192},
+          fillPattern=FillPattern.Solid,
+          points={{-77.704,88.6305},{-85.704,66.6305},{-69.704,66.6305},
+          {-77.704,88.6305}}),
+        Line(points={{-78.69,75.6256},{-78.69,-92.374}},
+          color={192,192,192}),
+        Line(points={{-88,-82},{84,-82}},
+          color={192,192,192}),
+        Polygon(lineColor={192,192,192},
+          fillColor={192,192,192},
+          fillPattern=FillPattern.Solid,
+          points={{92,-82},{70,-74},{70,-90},{92,-82}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end VariableOrder;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/package.mo
new file mode 100644
index 0000000000..8a706d7324
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/package.mo
@@ -0,0 +1,8 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle;
+package Inertias "Package with modules to model inertia of refrigerant cycles"
+
+
+annotation (Documentation(info="<html>
+<p>This package contains models to account for inertia in the refrigerant cycle.</p>
+</html>"));
+end Inertias;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/package.order
new file mode 100644
index 0000000000..17f4d94b81
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/Inertias/package.order
@@ -0,0 +1,3 @@
+NoInertia
+VariableOrder
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/TableData2D.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/TableData2D.mo
new file mode 100644
index 0000000000..c9ef62c136
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/TableData2D.mo
@@ -0,0 +1,213 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle;
+model TableData2D "Performance data based on condenser outlet and evaporator inlet temperature"
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle(
+    final devIde=datTab.devIde,
+    PEle_nominal=Modelica.Blocks.Tables.Internal.getTable2DValueNoDer2(
+        tabIdePEle,
+        TCon_nominal,
+        TEva_nominal) * scaFac);
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialTableData2D(
+    final useInRevDev=not useInHeaPum,
+    scaFac=QHea_flow_nominal/QHeaNoSca_flow_nominal,
+    final valTabQEva_flow = valTabQCon_flow .- valTabPEle,
+    final valTabQCon_flow = {{tabQUse_flow.table[j, i] for i in 2:numCol} for j in 2:numRow},
+    final mCon_flow_max=max(valTabQCon_flow) * scaFac / cpCon / dTMin,
+    final mCon_flow_min=min(valTabQCon_flow) * scaFac / cpCon / dTMax,
+    final mEva_flow_min=min(valTabQEva_flow) * scaFac / cpEva / dTMax,
+    final mEva_flow_max=max(valTabQEva_flow) * scaFac / cpEva / dTMin,
+    mEva_flow_nominal=datTab.mEva_flow_nominal*scaFac,
+    mCon_flow_nominal=datTab.mCon_flow_nominal*scaFac,
+    final use_TConOutForTab=datTab.use_TConOutForTab,
+    final use_TEvaOutForTab=datTab.use_TEvaOutForTab,
+    tabQUse_flow(final table=datTab.tabQCon_flow),
+    tabPEle(final table=datTab.tabPEle));
+  parameter Modelica.Units.SI.HeatFlowRate QHeaNoSca_flow_nominal=Modelica.Blocks.Tables.Internal.getTable2DValueNoDer2(
+        tabIdeQUse_flow,
+        TCon_nominal,
+        TEva_nominal)
+    "Unscaled nominal heating capacity "
+    annotation (Dialog(group="Nominal condition"));
+
+  replaceable parameter AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.GenericHeatPump datTab
+    "Data Table of HP" annotation (choicesAllMatching=true);
+
+equation
+
+  connect(scaFacTimPel.y, PEle) annotation (Line(points={{-40,-9},{-40,-24},{0,
+          -24},{0,-130}}, color={0,0,127}));
+  connect(scaFacTimPel.y, redQCon.u2) annotation (Line(points={{-40,-9},{-40,-24},
+          {64,-24},{64,-78}}, color={0,0,127}));
+  connect(yMeaTimScaFac.u1, sigBus.yMea) annotation (Line(points={{-54,62},{-54,
+          74},{-70,74},{-70,120},{1,120}},
+                               color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,6},{-3,6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(reaPasThrTEvaOut.u, sigBus.TEvaOutMea) annotation (Line(points={{-10,102},
+          {-10,120},{1,120}},      color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(reaPasThrTEvaIn.u, sigBus.TEvaInMea) annotation (Line(points={{-50,102},
+          {-50,120},{1,120}},                      color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(reaPasThrTConIn.u, sigBus.TConInMea) annotation (Line(points={{50,102},
+          {50,120},{1,120}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(reaPasThrTConOut.u, sigBus.TConOutMea) annotation (Line(points={{90,102},
+          {90,120},{1,120}},      color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  if useInHeaPum then
+    connect(reaPasThrTConOut.y, tabPEle.u1)
+      annotation (Line(points={{90,79},{90,70},{96,70},{96,62}}, color={0,0,127}));
+    connect(reaPasThrTConIn.y, tabPEle.u1)
+      annotation (Line(points={{50,79},{50,70},{96,70},{96,62}}, color={0,0,127}));
+    connect(reaPasThrTConIn.y, tabQUse_flow.u1)
+      annotation (Line(points={{50,79},{50,70},{56,70},{56,62}}, color={0,0,127}));
+    connect(reaPasThrTConOut.y, tabQUse_flow.u1)
+      annotation (Line(points={{90,79},{90,70},{56,70},{56,62}}, color={0,0,127}));
+    connect(reaPasThrTEvaOut.y, tabPEle.u2) annotation (Line(points={{-10,79},{
+            -10,70},{84,70},{84,62}},
+                              color={0,0,127}));
+    connect(reaPasThrTEvaOut.y, tabQUse_flow.u2) annotation (Line(points={{-10,79},
+            {-10,70},{44,70},{44,62}},color={0,0,127}));
+    connect(reaPasThrTEvaIn.y, tabPEle.u2) annotation (Line(points={{-50,79},{-50,
+            70},{84,70},{84,62}},
+                              color={0,0,127}));
+    connect(reaPasThrTEvaIn.y, tabQUse_flow.u2) annotation (Line(points={{-50,79},
+            {-50,70},{44,70},{44,62}},
+                                  color={0,0,127}));
+  else
+    connect(reaPasThrTEvaOut.y, tabPEle.u1) annotation (Line(points={{-10,79},{
+            -10,70},{96,70},{96,62}},         color={0,0,127}));
+    connect(reaPasThrTEvaOut.y, tabQUse_flow.u1) annotation (Line(points={{-10,79},
+            {-10,70},{56,70},{56,62}},                color={0,0,127}));
+    connect(reaPasThrTEvaIn.y, tabPEle.u1) annotation (Line(points={{-50,79},{-50,
+            70},{96,70},{96,62}},             color={0,0,127}));
+    connect(reaPasThrTEvaIn.y, tabQUse_flow.u1) annotation (Line(points={{-50,79},
+            {-50,70},{56,70},{56,62}},            color={0,0,127}));
+    connect(reaPasThrTConOut.y, tabPEle.u2)
+      annotation (Line(points={{90,79},{90,70},{84,70},{84,62}}, color={0,0,127}));
+    connect(reaPasThrTConOut.y, tabQUse_flow.u2)
+      annotation (Line(points={{90,79},{90,70},{44,70},{44,62}}, color={0,0,127}));
+    connect(reaPasThrTConIn.y, tabPEle.u2)
+      annotation (Line(points={{50,79},{50,70},{84,70},{84,62}}, color={0,0,127}));
+    connect(reaPasThrTConIn.y, tabQUse_flow.u2)
+      annotation (Line(points={{50,79},{50,70},{44,70},{44,62}}, color={0,0,127}));
+  end if;
+  connect(scaFacTimPel.y, feeHeaFloEva.u1) annotation (Line(points={{-40,-9},{-40,
+          -24},{-86,-24},{-86,-10},{-78,-10}}, color={0,0,127}));
+  connect(scaFacTimQUse_flow.y, feeHeaFloEva.u2) annotation (Line(points={{40,-9},
+          {40,-26},{-70,-26},{-70,-18}}, color={0,0,127}));
+  annotation (Icon(graphics={
+    Line(points={
+          {-60.0,40.0},{-60.0,-40.0},{60.0,-40.0},{60.0,40.0},{30.0,40.0},
+          {30.0,-40.0},{-30.0,-40.0},{-30.0,40.0},{-60.0,40.0},{-60.0,20.0},
+          {60.0,20.0},{60.0,0.0},{-60.0,0.0},{-60.0,-20.0},{60.0,-20.0},
+          {60.0,-40.0},{-60.0,-40.0},{-60.0,40.0},{60.0,40.0},{60.0,-40.0}}),
+    Line(points={{0.0,40.0},{0.0,-40.0}}),
+    Rectangle(fillColor={255,215,136},
+      fillPattern=FillPattern.Solid,
+      extent={{-60.0,20.0},{-30.0,40.0}}),
+    Rectangle(fillColor={255,215,136},
+      fillPattern=FillPattern.Solid,
+      extent={{-60.0,0.0},{-30.0,20.0}}),
+    Rectangle(fillColor={255,215,136},
+      fillPattern=FillPattern.Solid,
+      extent={{-60.0,-20.0},{-30.0,0.0}}),
+    Rectangle(fillColor={255,215,136},
+      fillPattern=FillPattern.Solid,
+      extent={{-60.0,-40.0},{-30.0,-20.0}})}), Documentation(revisions="<html>
+<ul>
+  <li>
+    <i>May 21, 2021</i> by Fabian Wuellhorst:<br/>
+    Make use of BaseClasses (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/1092\">AixLib #1092</a>)
+  </li>
+  <li>
+    <i>November 26, 2018</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/577\">AixLib #577</a>)
+  </li>
+</ul>
+</html>", info="<html>
+<p>
+  This model uses two-dimensional table data typically given
+  by manufacturers as required by e.g. European Norm 14511
+  or ASHRAE 205 to calculate
+  <code>QCon_flow</code> and <code>PEle</code>.
+</p>
+<p>
+  For different condenser outlet and evaporator inlet temperatures,
+  the tables must provide two of the three following values:
+  electrical power consumption, evaporator heat flow rate, and COP.
+</p>
+<p>
+  Note that losses are often implicitly included in measured data.
+  In this case, the frosting modules should be disabled.
+</p>
+
+<h4>Scaling factor</h4>
+<p>
+For the scaling factor, the table data for condenser heat flow rate (<code>QConTabDat_flow</code>)
+is evaluated at nominal conditions. Hence, the scaling factor is
+</p>
+<pre>
+scaFac = QCon_flow_nominal/QConTabDat_flow(TEva_nominal, TCon_nominal).
+
+</pre>
+<p>
+Using <code>scaFac</code>, the table data is scaled linearly.
+This implies a constant COP over different design sizes:
+</p>
+<p><code>QCon_flow = scaFac * tabQCon_flow.y</code> </p>
+<p><code>PEle = scaFac * tabPel.y</code></p>
+
+
+<h4>Known Limitations </h4>
+<ul>
+<li>
+  Manufacturers are not required to provide the compressor speed at which
+  the data are measured. Thus, nominal values may be obtained at different
+  compressor speeds and, thus, efficiencies.
+  To accurately model the available thermal output,
+  please check that you use tables of the maximal thermal output,
+  which is often provided in the data sheets from the manufacturers.
+  This limitation only holds for inverter driven heat pumps.
+</li>
+<li>
+  We assume that the efficiency is contant over the whole
+  compressor speed range. Typically, effciencies will drop at minimal
+  and maximal compressor speeds.
+  To model an inverter controlled heat pump, the relative
+  compressor speed <code>yMea</code> is used to scale
+  the ouput of the tables linearly.
+  For models including the compressor speed, check the SDF-Library
+  dependent refrigerant cycle models in the
+  <a href=\"https://github.com/RWTH-EBC/AixLib\">AixLib</a> Library.
+</li>
+</ul>
+<h4>References</h4>
+<p>
+EN 14511-2018: Air conditioners, liquid chilling packages and heat pumps for space
+heating and cooling and process chillers, with electrically driven compressors
+<a href=\"https://www.beuth.de/de/norm/din-en-14511-1/298537524\">
+https://www.beuth.de/de/norm/din-en-14511-1/298537524</a>
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TableData2D;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/package.mo
new file mode 100644
index 0000000000..bf3fa223ae
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/package.mo
@@ -0,0 +1,16 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+package RefrigerantCycle "Package for heat pupmp refrigerant cycle modules"
+   extends Modelica.Icons.MaterialPropertiesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+  This package contains models and data to for
+  dynamic refrigerant cycles based on stationary data points,
+  evaporator frosting, and cycle inertia.
+</p>
+<p>
+  Besides, functional approaches for evaporator frosting and
+  refrigerant cycle inertia exist.
+</p>
+</html>"));
+end RefrigerantCycle;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/package.order
new file mode 100644
index 0000000000..96ca1f6e8f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/RefrigerantCycle/package.order
@@ -0,0 +1,5 @@
+ConstantCarnotEffectiveness
+TableData2D
+Frosting
+Inertias
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/TableData2D.mo b/AixLib/Fluid/HeatPumps/ModularReversible/TableData2D.mo
new file mode 100644
index 0000000000..ca3250f405
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/TableData2D.mo
@@ -0,0 +1,157 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+model TableData2D
+  "Reversible heat pump based on 2D manufacturer data"
+  extends AixLib.Fluid.HeatPumps.ModularReversible.Modular(
+    final use_rev=true,
+    QCoo_flow_nominal=refCyc.refCycHeaPumCoo.QCooNoSca_flow_nominal*scaFacHea,
+    dpEva_nominal=datTabHea.dpEva_nominal*scaFacHea^2,
+    dpCon_nominal=datTabHea.dpCon_nominal*scaFacHea^2,
+    redeclare replaceable
+      AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Wuellhorst2021
+      safCtrPar constrainedby
+      AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Data.Generic(
+      final tabUppHea=datTabHea.tabUppBou,
+      final tabLowCoo=datTabCoo.tabLowBou,
+      final use_TConOutHea=datTabHea.use_TConOutForOpeEnv,
+      final use_TEvaOutHea=datTabHea.use_TEvaOutForOpeEnv,
+      final use_TConOutCoo=datTabCoo.use_TConOutForOpeEnv,
+      final use_TEvaOutCoo=datTabCoo.use_TEvaOutForOpeEnv),
+    dTEva_nominal=(QHea_flow_nominal - PEle_nominal)/cpEva/mEva_flow_nominal,
+    mEva_flow_nominal=datTabHea.mEva_flow_nominal*scaFacHea,
+    mCon_flow_nominal=datTabHea.mCon_flow_nominal*scaFacHea,
+    dTCon_nominal=QHea_flow_nominal/cpCon/mCon_flow_nominal,
+    GEvaIns=0,
+    GEvaOut=0,
+    CEva=0,
+    use_evaCap=false,
+    GConIns=0,
+    GConOut=0,
+    CCon=0,
+    use_conCap=false,
+    redeclare model RefrigerantCycleHeatPumpCooling =
+        AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D (
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+          iceFacCal,
+        final mCon_flow_nominal=mCon_flow_nominal,
+        final mEva_flow_nominal=mEva_flow_nominal,
+        final smoothness=smoothness,
+        final extrapolation=extrapolation,
+        final datTab=datTabCoo),
+    redeclare model RefrigerantCycleHeatPumpHeating =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D (
+        redeclare
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.NoFrosting
+          iceFacCal,
+        final mCon_flow_nominal=mCon_flow_nominal,
+        final mEva_flow_nominal=mEva_flow_nominal,
+        final smoothness=smoothness,
+        final extrapolation=extrapolation,
+        final datTab=datTabHea),
+    redeclare model RefrigerantCycleInertia =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.NoInertia);
+  final parameter Real scaFacHea=refCyc.refCycHeaPumHea.scaFac
+    "Scaling factor of heat pump";
+  final parameter Real scaFacCoo=refCyc.refCycHeaPumCoo.scaFac
+    "Scaling factor for cooling mode";
+
+  replaceable parameter
+    AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.GenericHeatPump datTabHea
+    constrainedby
+    AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.GenericHeatPump
+    "Data table of heat pump"
+    annotation (choicesAllMatching=true,
+      Placement(transformation(extent={{82,-18},{98,-2}})));
+  replaceable parameter AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic datTabCoo(
+      use_TEvaOutForTab=true, use_TConOutForTab=true)
+    constrainedby
+    AixLib.Fluid.Chillers.ModularReversible.Data.TableData2D.Generic
+    "Data table of chiller"    annotation (choicesAllMatching=true,
+    Placement(transformation(extent={{114,-18},{130,-2}})));
+
+  parameter Modelica.Blocks.Types.Smoothness smoothness=Modelica.Blocks.Types.Smoothness.LinearSegments
+    "Smoothness of table interpolation" annotation (Dialog(tab="Advanced"));
+  parameter Modelica.Blocks.Types.Extrapolation extrapolation=Modelica.Blocks.Types.Extrapolation.LastTwoPoints
+    "Extrapolation of data outside the definition range"
+    annotation (Dialog(tab="Advanced"));
+initial algorithm
+  assert(use_rev and (abs(scaFacHea - scaFacCoo) / scaFacHea < limWarSca),
+    "In " + getInstanceName() + ": Scaling factors for heating and cooling
+    operation differ by " + String((scaFacHea - scaFacCoo) / scaFacHea * 100) +
+    " %. The simulated nominal heating and cooling
+    capacities may not be realistic for a single device",
+    AssertionLevel.warning);
+
+  annotation (Documentation(info="<html>
+<p>
+  Heat pump based on
+  two-dimensional data from manufacturer data, (e.g. based on EN 14511),
+  using the
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular</a> approach.
+</p>
+<p>
+  For more information on the approach, see
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">
+  AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>.
+</p>
+<p>
+  Internal inertias and heat losses are typically neglected,
+  as these are implicitly obtained in measured
+  data from manufacturers.
+  Also, icing is disabled as the performance degradation
+  is already contained in the data.
+</p>
+
+<h4>Sizing</h4>
+
+<p>
+  At the nominal conditions, the refrigerant cycle model will
+  calculate the unscaled nominal heat flow rate, which is
+  named <code>QHeaNoSca_flow_nominal</code> for heat pumps and
+  <code>QCooNoSca_flow_nominal</code> for chillers.
+  This value is probably
+  different from <code>QHea_flow_nominal</code> and
+  <code>QCoo_flow_nominal</code> which is for sizing.
+  For example, suppose you need a 7.6 kW heat pump,
+  but the datasheets only provides 5 kW and 10 kW options.
+  In such cases, the performance data and relevant parameters
+  are scaled using a scaling factor <code>scaFac</code>.
+  Resulting, the refrigerant machine can supply more or less heat with
+  the COP staying constant. However, one has to make sure
+  that the movers in use also scale with this factor.
+  Note that most parameters are scaled linearly. Only the
+  pressure differences are scaled quadratically due to
+  the linear scaling of the mass flow rates and the
+  basic assumption:
+  <p align=\"center\" style=\"font-style:italic;\">
+  k = m&#775; &frasl; &radic;<span style=\"text-decoration:overline;\">&nbsp;&Delta;p &nbsp;</span>
+</p>
+<p>
+  Both <code>QHeaNoSca_flow_nominal</code> or <code>QCooNoSca_flow_nominal</code>
+  and <code>scaFac</code>
+  are calculated in the refrigerant cycle models.
+</p>
+
+
+<p>
+Please read the documentation of the model for heating at
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D</a>.
+</p>
+<p>
+For cooling, the assumptions are similar, and described at
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D\">
+  AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D</a>
+</p>
+<h4>References</h4>
+<p>
+EN 14511-2018: Air conditioners, liquid chilling packages and heat pumps for space
+heating and cooling and process chillers, with electrically driven compressors
+<a href=\"https://www.beuth.de/de/norm/din-en-14511-1/298537524\">
+https://www.beuth.de/de/norm/din-en-14511-1/298537524</a>
+</p>
+
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TableData2D;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/UsersGuide.mo b/AixLib/Fluid/HeatPumps/ModularReversible/UsersGuide.mo
new file mode 100644
index 0000000000..f863da0f79
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/UsersGuide.mo
@@ -0,0 +1,560 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+package UsersGuide
+  "User's Guide for modular reversible heat pump and chiller models"
+  extends Modelica.Icons.Information;
+  annotation (preferredView="info",
+  Documentation(info="<html>
+<p>
+  The packages <a href=\"modelica://AixLib.Fluid.HeatPumps\">AixLib.Fluid.HeatPumps</a>
+  and <a href=\"modelica://AixLib.Fluid.Chillers\">AixLib.Fluid.Chillers</a> contain
+  models for both reversible and non-reversible refrigerant
+  machines (heat pumps and chillers) based on grey-box approaches.
+  Either empirical data or physical equations are used to model
+  the refrigerant cycle. The model for a refrigerant cycle calculates
+  the electrical power consumption <code>PEle</code>,
+  the condenser heat flow <code>QCon_flow</code>,
+  and the evaporator heat flow <code>QEva_flow</code>
+  based on available variables of the sink and source streams.
+  Thus, this model does not enable closed-loop simulations of
+  the refrigerant cycle. However, such models are
+  highly demanding in terms computation time, and commercial implementations exist.
+  When simulating the refrigerant machine in a more complex energy system,
+  this modular approach enables detailed performance and
+  dynamic behaviour and fast computating times.
+</p>
+<p>
+  This user guide will help understand how to use the models associated
+  with the modular approach.
+  The approach was presented at the Modelica Conference 2021, see the section <b>References</b>.
+</p>
+
+<h4>Why modular models?</h4>
+<p>
+  Heat pumps and chillers are versatile machines:
+</p>
+<ul>
+<li>
+  They may use various source or sink media (e.g. air, water, brine, etc.);
+</li>
+<li>
+  They may be on/off and inverter driven;
+</li>
+<li>
+  They are able reverse the operation between heating to cooling;
+</li>
+<li>
+  They operate in a limited characteristic range (operational envelope);
+</li>
+<li>
+  The design depends on various nominal boundary conditions;
+</li>
+<li>
+  Safety features are part of their control sequence.
+</li>
+</ul>
+<p>
+  To what extend all these effects need to be modeled depends
+  on the simulation aim. Sometimes a simple Carnot approach is
+  sufficient, sometimes a more detailed performance data
+  and a realistic control behaviour is required.
+</p>
+<p>
+  The modular approach allows to disable any irrelevant features,
+  select readily made functional modules, and
+  easily add new model modules.
+  Relevant components are declared as <code>replaceable</code>.
+  Replaceable models are <code>constrainedby</code> partial models
+  which one is free to extend. Thus, new model approaches can be inserted
+  into the framework of the modular reversible model approach.
+  For users not familiar with replaceable models,
+  there are readily assembled models as well.
+</p>
+
+<h4>Package and model structure</h4>
+
+<p>
+  This section explains the inheritance and model package structure
+  to help navigate through all options and to check out the
+  detailed documentation of each model for further information.
+</p>
+<p>
+  All modular heat pump or chiller models base on the model
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle</a>.
+  This partial model declares all common interfaces, parameters, etc.
+</p>
+
+<h5>Heat pump models</h5>
+<p>
+For heat pumps, the model <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Modular\">
+AixLib.Fluid.HeatPumps.ModularReversible.Modular</a> extends the partial model and adds
+the connector <code>hea</code> to choose
+between the operation modes of the heat pump:
+</p>
+<ul>
+<li><code>hea = true</code>: Main operation mode (heating) </li>
+<li><code>hea = false</code>: Reversed operation mode (cooling) </li>
+</ul>
+<p>
+Furthermore, the refrigerant cycle is redeclared to use the one for
+the heat pump
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantCycle\">
+AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.RefrigerantCycle</a>.
+This refrigerant cycle in turn contains replaceable models for the
+heating and cooling operation of the heat pump.
+Available modules can be found in the package:
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle\">
+AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle</a>
+For more information on the refrigerant cycle models, refer
+to the section <b>Refrigerant cycle models</b>.
+</p>
+<p>
+  There are a number of preconfigured models provided in the package.
+  Please check out the documentation of each approach
+  to check if this approach is suitable.
+</p>
+<ul>
+<li>
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.LargeScaleWaterToWater\">
+  AixLib.Fluid.HeatPumps.ModularReversible.LargeScaleWaterToWater</a>
+</li>
+<li>
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.AirToWaterTableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.AirToWaterTableData2D</a>
+</li>
+<li>
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.CarnotWithLosses\">
+  AixLib.Fluid.HeatPumps.ModularReversible.CarnotWithLosses</a>
+</li>
+</ul>
+
+<h5>Chiller models</h5>
+
+<p>
+For chillers, the model <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.Modular\">
+AixLib.Fluid.Chillers.ModularReversible.Modular</a> extends the partial model and adds
+the connector <code>coo</code> to choose
+between the operation mode of the chiller:
+</p>
+<ul>
+<li><code>coo = true</code>: Main operation mode (cooling) </li>
+<li><code>coo = false</code>: Reversed operation mode (heating) </li>
+</ul>
+<p>
+Furthermore, the refrigerant cycle is redeclared to use the one for
+the chiller
+<a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.BaseClasses.RefrigerantCycle\">
+AixLib.Fluid.Chillers.ModularReversible.BaseClasses.RefrigerantCycle</a>.
+This refrigerant cycle in turn contains replaceable models for the
+cooling and heating operation of the chiller.
+Available modules can be found in the package:
+<a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle\">
+AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle</a>.
+For more information on the refrigerant cycle models, refer
+to the section <b>Refrigerant cycle models</b>.
+</p>
+<p>
+  There are a number of preconfigured models provided in the package.
+  Please check out the documentation of each approach
+  to check if this approach is suitable.
+</p>
+<ul>
+<li>
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.LargeScaleWaterToWater\">
+  AixLib.Fluid.Chillers.ModularReversible.LargeScaleWaterToWater</a>
+</li>
+<li>
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.CarnotWithLosses\">
+  AixLib.Fluid.Chillers.ModularReversible.CarnotWithLosses</a>
+</li>
+</ul>
+
+
+<h4>Naming and reversible operation</h4>
+
+<p>
+Simulating reversible heat pumps and chillers can get confusing, as the same heat
+exchanger model has to be used for both condensation and evaporation.
+</p>
+
+<p>
+In most cases, heat pumps and chillers extract/exhaust heat from/to
+an ambient source (air, soil, ground-water, etc.),
+and, consuming electrical energy, provide heating or cooling
+on the <i>useful</i> or <i>load side</i>.
+For building applications, this <i>useful / load side</i> is inside the building.
+The ambient heat is outside of the building, on the <i>ambient / source side</i>.
+However, vapor compression machines can also be used to provide heating
+and cooling simultaneously.
+In this case, both sides provide utility to the energy system.
+Hence, both sides are <i>useful / load sides</i>.
+</p>
+<p>
+What always stays the same is that there is one heated fluid, and
+one cooled fluid. Thus, specifying the nominal temperatures, users have
+to specify the temperatures of both heated and cooled fluids, for both cooling
+and heating operation. Note, that the heated fluid will be the cooled fluid in
+reversed operation, and vice versa.
+</p>
+<p>
+Because of this, we decided on a naming scheme which is based on the main operation
+of the heat pump or chiller. The main operation of a heat pump is heating, for
+a chiller, it is cooling. When reversed, the condenser becomes the evaporator and
+vice versa. As renaming instances after translation is not possible, users always
+have to think about the names <code>con</code> and <code>eva</code> in terms of
+the main operation of the device.
+This applies to the instance and variable names,
+such as the heat exchangers <code>con</code> and <code>eva</code>,
+as well as sensors such as <code>TConOutMea</code> and <code>TEvaInMea</code>,
+or nominal conditions <code>TConHea_nominal</code> and <code>TConCoo_nominal</code>.
+
+As the nominal temperatures may be used table-based performance data
+and the operational envelope model,
+users also have to think about the <i>useful / load</i>
+and <i>ambient / source side</i> and how they translate to
+heat pumps and chillers in both main and reversed operation
+when adding new datasheets.
+Thinking about the heated and cooled fluid helps.
+</p>
+<p>
+The following tables summarizes the possible options.
+</p>
+
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+    <tr>
+      <th></th>
+      <th>Heat pump main</th>
+      <th>Heat pump reversed</th>
+      <th>Chiller main</th>
+      <th>Chiller reversed </th>
+    </tr>
+    <tr>
+      <td>Heating / cooling?</td>
+      <td>heating</td>
+      <td>cooling</td>
+      <td>cooling</td>
+      <td>heating  </td>
+    </tr>
+    <tr>
+      <td>Table-data: column 1: useful / load side</td>
+      <td><code>con</code></td>
+      <td><code>con</code> <sup>1</sup></td>
+      <td><code>eva</code></td>
+      <td><code>eva</code> <sup>2</sup>  </td>
+    </tr>
+    <tr>
+      <td>Table-data - row 1: ambient / source side</td>
+      <td><code>eva</code></td>
+      <td><code>eva</code> <sup>2</sup></td>
+      <td><code>con</code></td>
+      <td><code>con</code> <sup>1</sup>  </td>
+    </tr>
+    <tr>
+      <td>Operational envelope - column 1: ambient / source side</td>
+      <td><code>eva</code></td>
+      <td><code>eva</code> <sup>2</sup></td>
+      <td><code>con</code></td>
+      <td><code>con</code> <sup>1</sup>  </td>
+    </tr>
+    <tr>
+      <td>Operational envelope - column 2: useful / load side</td>
+      <td><code>con</code></td>
+      <td><code>con</code> <sup>1</sup></td>
+      <td><code>eva</code></td>
+      <td><code>eva</code> <sup>2</sup>  </td>
+    </tr>
+</table>
+<b>Footnotes:</b>
+<p>
+<sup>1</sup> In reality, the condenser, e.g. a plate heat exchanger, of the main operation is used for evaporation.
+<sup>2</sup> In reality, the evaporator, e.g. fin-tube heat exchanger, of the main operation is used for condensation.
+</p>
+
+<h4>Connectors</h4>
+
+<p>
+  Aside from the aforementioned Boolean signals
+  <code>hea</code> and <code>coo</code>, the following
+  connectors are relevant to understanding how the model works:
+  Compressor speed and the expandable bus connector.
+
+  The ambient temperatures <code>TEvaAmb</code> and <code>TConAmb</code> are
+  only relevant for the heat losses.
+  The fluid ports are explained in more detail here:
+<a href=\"modelica://AixLib.Fluid.UsersGuide\">AixLib.Fluid.UsersGuide</a>.
+</p>
+
+<h5>Compressor speed</h5>
+
+<p>
+  The input <code>ySet</code> represents the relative compressor speed.
+  To model both on/off and inverter controlled refrigerant machines,
+  the compressor speed is normalised to a relative value between <i>0</i> and <i>1</i>.
+  To model heat pumps other than inverter driven,
+  other signal limits can be used.
+
+
+  If data is in Hz or similar, consider converting
+  the input according to the maximum allowed value.
+</p>
+<p>
+  We use the notation <code>Set</code> to indicate a set value.
+  It may be modified by the safety control blocks which produces a signal
+  with the <code>Mea</code> notation. For example, the compressor
+  speed <code>ySet</code> is modified by the safety
+  control block to <code>yMea</code>. If no safety violations
+  occur, <code>ySet</code> equals <code>yMea</code>.
+</p>
+
+<h5>Expandable bus connector</h5>
+
+<p>
+  As the modular approach may require different information to model
+  the refrigerant cycle depending on configuration, all available states and outputs
+  are aggregated in the expandable bus connector <code>sigBus</code>.
+  For instance, in order to control both chillers and heat pumps,
+  both flow and return temperature are relevant.
+</p>
+
+<h4>Refrigerant cycle models</h4>
+
+<p>
+  A replaceable refrigerant cycle model for heating or
+  cooling calculates the electrical power consumption
+  <code>PEle</code>, condenser heat flow rate <code>QCon_flow</code>
+  and evaporator heat flow rate <code>QEva_flow</code> based on the
+  values in the <code>sigBus</code>.
+  Heat pumps models extend
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.BaseClasses.PartialHeatPumpCycle</a>
+  and chiller models extend
+  <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle\">
+  AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.PartialChillerCycle</a>.
+</p>
+<p>
+  Currently, two modules for refrigerant cycle are implemented.
+  First, the <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness</a> model
+  uses the same equations as the Carnot models, i.e.  <a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">
+  AixLib.Fluid.HeatPumps.Carnot_y</a>.
+  Second, the <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D</a> provides performance data
+  based on different condenser outlet and evaporator inlet temperatures using 2D-tables.
+</p>
+<p>
+  Two additional modules exist in the AixLib library.
+  These approaches require the use of the SDF-library, as
+  the compressor speed influences the model output as a third
+  dimension. Currently, tables with more than two dimensions are not supported in
+  the Modelica Standard Library.
+  The first approach is similar to <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D</a>
+  approach buts adds the 3rd dimension of compressor speed.
+  The second approach is based on white-box stationary Python models
+  for closed-loop refrigerant cycles. The model has been empirically
+  validated and can take up to n-dimensions.
+  If your simulation aim requires more detailed data, be sure
+  to check out the models in the AixLib.
+</p>
+
+
+<h4>Parameterization and naming</h4>
+<p>
+  The refrigerant cycle models will output
+  varying heat flow rates and electrical power consumptions.
+  This is based on the fact that refrigerant cycle performance
+  depend heavily on the boundary conditions.
+</p>
+<p>
+  Still, the user needs to size the device or the system
+  according to some reference points. Accordingly, we follow
+  the basic AixLib concept for nominal conditions, explained in
+  detail here:
+  <a href=\"modelica://AixLib.Fluid.UsersGuide\">AixLib.Fluid.UsersGuide</a>
+</p>
+<p>
+  The nominal heat flow rate of the device is distinct for
+  heat pumps and chillers.
+  For heat pumps, it is the nominal
+  condenser heat flow rate <code>QHea_flow_nominal</code>.
+  For chillers, it is the nominal
+  evaporator heat flow rate <code>QCoo_flow_nominal</code> (negative).
+  This nominal heat flow rate is only valid at the
+  nominal conditions. Whether parameters influence the nominal heat flow rates
+  depends on the model approach used to estimate the heat flow rate and efficiencies.
+  Typically, at least nominal source and sink temperatures will influence the
+  nominal conditions:
+</p>
+<ul>
+<li>
+  condenser temperature <code>TCon_nominal</code>,
+</li>
+<li>
+  evaporator temperature <code>TEva_nominal</code>,
+</li>
+</ul>
+<p>
+  Depending on the model in use, this may be inlet or outlet.
+</p>
+<p>
+  Another example would be inverter driven devices.
+  Here, the compressor speed influences the
+  refrigerant mass flow rate and compressor efficiencies.
+  If the performance data is dependent on the compressor speed,
+  <code>y_nominal</code> influences the nominal efficiencies.
+  In such cases, specifying additional nominal parameters will
+  be nessary.
+</p>
+<p>
+  Using the nominal conditions and the specified heat flow rate,
+  the nominal electrical power consumption <code>PEle_nominal</code> is calculated.
+  As reversible devices have typically a four-way-valve and a single
+  compressor, you have to make sure that the values for <code>PEle_nominal</code>
+  are similar between heating and cooling. The pre-configured models
+  warn about deviations if they are too large.
+</p>
+<p>
+  To change the capacity of the model, users should change
+  <code>QHea_flow_nominal</code> for heating operation and
+  <code>QCoo_flow_nominal</code> for cooling operation. This will then also
+  update the electricity use <code>PEle_nominal</code>.<br/>
+  For models with table-based performance curves, changing these values will also scale
+  the design mass flow rates and pressure drops.
+  The documentation of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.TableData2D\">
+  AixLib.Fluid.HeatPumps.ModularReversible.TableData2D</a>
+  further explains the scaling.
+</p>
+
+<h4>Safety controls</h4>
+
+<p>
+  Refrigerant machines contain internal safety controls,
+  prohibiting operations in possibly unsafe points.
+  All <code>ModularReversible</code> models account for those.
+  All options can be disabled as described in the model description
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Safety\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Safety</a>
+</p>
+
+<p>
+  An important safety control with regard to
+  system interaction is the operation envelope. Read the documentation of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.PartialOperationalEnvelope\">
+  AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.BaseClasses.PartialOperationalEnvelope</a>
+  for more information on this model and how it affects device operation.
+</p>
+
+
+<h4>Refrigerant cycle inertia</h4>
+
+<p>
+  The refrigerant cycle models
+  are based on stationary data points, any inertia
+  (mass and thermal) of components inside the refrigerant cycle
+  (compressor, pipes, expansion valve, fluid, etc.) is neglected.
+  To overcome this issue, replaceable SISO blocks that are connected to the
+  output of the refrigerant cycle (instance <code>refCyc</code>)
+  can approximate the refrigerant cycle inertia.
+</p>
+<p>
+  The package
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias</a>
+  contains implemented inertia models. In the
+  <a href=\"https://doi.org/10.1016/j.enconman.2021.114888\">contribution</a>, an empirical
+  validation showed that a third-order critical damping element
+  fits the inertia most closely. At the same time, models in literature
+  often use first-order delay blocks.
+  Additionally, higher-order elements require more computation time.
+  At the end, the requirements on the analysis will define the required level
+  of detail of the model.
+</p>
+<p>
+  The effect of the inertia can be removed by setting <code>NoInertia</code>.
+</p>
+<p>
+  If a user finds in real data that another approach might be better suited
+  (e.g. a deadband), then the model
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.BaseClasses.PartialInertia\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.BaseClasses.PartialInertia
+  </a>
+  can be extended to implement a costum model.
+</p>
+
+
+<h4>Frost</h4>
+
+<p>
+  To simulate possible icing of the evaporator on air-source devices, the
+  icing factor <code>iceFac</code> is used to modify the outputs.
+  The factor models the reduction of heat transfer between refrigerant
+  and source. Thus, the factor is implemented as follows:
+</p>
+<p>
+  <code>QEva_flow = iceFac * (QConNoIce_flow - PEle)</code>
+</p>
+<p>
+  With <code>iceFac</code> as a relative value between <i>0</i> and <i>1</i>:
+</p>
+<p><code>iceFac = kA/kA_noIce</code></p>
+<p>Finally, the energy balance must still hold:</p>
+<p><code>QCon_flow = PEle + QEva_flow</code> </p>
+<p>
+  Different options can be selected for the modeling of the icing factor, or
+  a custom model can be implemented by extending
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.BaseClasses.PartialIcingFactor\">
+  AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Frosting.BaseClasses.PartialIcingFactor</a>
+</p>
+<p>
+  Note however, that this only simulates the efficiency reduction
+  due to frost. If a user-provided frost module enables the simulation
+  of a defrost cycle, the user needs to implement the corresponding external controls.
+  The <code>iceFac</code> approach was already used by Vering et al., 2021,
+  to account for reverse cycle defrost based on validated literature-data.
+  However, as no empirical validation was performed, the model was not
+  added to the AixLib library.
+</p>
+
+<h4>Heat losses</h4>
+
+<p>
+  Most refrigerant cycle models that calculate
+  <code>PEle</code>, <code>QCon_flow</code>, and <code>QEva_flow</code>
+  assume the device to be adiabatic, following the equation:
+</p>
+<p>
+  <code>QCon_flow = PEle + QEva_flow</code>
+</p>
+<p>
+  Depending on the application, one may need to model
+  the heat losses to the ambient, as those may
+  impact the overall efficiency of the heat pump or chiller.
+  Thus, the heat exchangers in the models adds
+  thermal capacities to the adiabatic heat exchanger.
+  The parameterization may be challenging, as datasheets
+  do not contain parameters for the required values.
+  Besides empirical calibration, simplified
+  assumptions (e.g. <i>2%</i> heat loss) may be used to
+  parameterize the required values.
+  For more information, see the description of
+  <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.EvaporatorCondenserWithCapacity\">
+  AixLib.Fluid.HeatPumps.ModularReversible.BaseClasses.EvaporatorCondenserWithCapacity</a>
+</p>
+
+<h4>References</h4>
+<p>
+  Fabian Wuellhorst, David Jansen, Philipp Mehrfeld and Dirk Müller.<br/>
+  A Modular Model of Reversible Heat Pumps and Chillers for System Applications.<br/>
+  Proceedings of 14th Modelica Conference 2021. Linköping, Sweden, September, 2021.<br/>
+  <a href=\"https://doi.org/10.3384/ecp21181561\">doi:10.3384/ecp21181561</a>.
+</p>
+<p>
+Christian Vering, Fabian Wüllhorst, Philipp Mehrfeld and Dirk Müller.<br/>
+Towards an integrated design of heat pump systems: Application of process intensification using two-stage optimization.<br/>
+Energy Conversion and Management, Volume 250, 2021.<br/>
+<a href=\"https://doi.org/10.1016/j.enconman.2021.114888\">doi:10.1016/j.enconman.2021.114888</a>.
+</p>
+</html>"));
+
+end UsersGuide;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/PartialValidation.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/PartialValidation.mo
new file mode 100644
index 0000000000..297e89af06
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/PartialValidation.mo
@@ -0,0 +1,185 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation.BaseClasses;
+partial model PartialValidation
+  "Validation base case for the reversible heat pump model."
+
+  replaceable package MediumSin = AixLib.Media.Water
+    constrainedby Modelica.Media.Interfaces.PartialMedium
+      "Medium of sink side"
+      annotation (choicesAllMatching=true);
+  replaceable package MediumSou = AixLib.Media.Water
+    constrainedby Modelica.Media.Interfaces.PartialMedium
+      "Medium of source side"
+      annotation (choicesAllMatching=true);
+  AixLib.Fluid.Sources.MassFlowSource_T souSidMasFlowSou(
+    use_m_flow_in=true,
+    use_T_in=true,
+    m_flow=1,
+    nPorts=1,
+    redeclare final package Medium = MediumSou,
+    T=275.15) "Ideal mass flow source at the inlet of the source side"
+    annotation (Placement(transformation(extent={{-40,-82},{-20,-62}})));
+
+  AixLib.Fluid.Sources.Boundary_pT souSidFixBou(
+    nPorts=1,
+    redeclare package Medium = MediumSou)
+    "Fixed boundary at the outlet of the source side"
+    annotation (Placement(transformation(
+        extent={{-11,-11},{11,11}},
+        rotation=0,
+        origin={-33,-37})));
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular heaPum(
+    redeclare final package MediumCon = MediumSin,
+    redeclare final package MediumEva = MediumSou,
+    final use_intSafCtr=false,
+    TConHea_nominal=303.15,
+    dTCon_nominal=5,
+    CCon=0,
+    GConOut=0,
+    GConIns=0,
+    TEvaHea_nominal=290.15,
+    dTEva_nominal=5,
+    mEva_flow_nominal=0.8,
+    dpEva_nominal=0,
+    dpCon_nominal=0,
+    use_conCap=false,
+    final use_rev=false,
+    CEva=0,
+    GEvaOut=0,
+    GEvaIns=0,
+    TEva_start=290.15,
+    use_evaCap=false,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    TCon_start=303.15,
+    redeclare model RefrigerantCycleHeatPumpCooling =
+        AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.BaseClasses.NoCooling)
+    "Heat pump" annotation (Placement(transformation(
+        extent={{-10.5,-10.5},{10.5,10.5}},
+        rotation=0,
+        origin={10.5,-30.5})));
+
+  AixLib.Fluid.Sources.Boundary_pT sinSidFixBou(redeclare final package Medium =
+        MediumSin, nPorts=1) "Fixed boundary at the outlet of the sink side"
+    annotation (Placement(transformation(
+        extent={{10,10},{-10,-10}},
+        rotation=0,
+        origin={50,-24})));
+  AixLib.Fluid.Sources.MassFlowSource_T sinSidMasFlowSou(
+    use_m_flow_in=true,
+    use_T_in=true,
+    m_flow=1,
+    nPorts=1,
+    redeclare final package Medium = MediumSin,
+    T=275.15) "Ideal mass flow source at the inlet of the source side"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-30,0})));
+
+  Modelica.Blocks.Math.Gain mEva_flow(final k=heaPum.mEva_flow_nominal)
+    "Gain to scale the time table output to flow rate"
+    annotation (Placement(transformation(extent={{-80,-60},{-60,-40}})));
+  Modelica.Blocks.Math.Gain mCon_flow(final k=heaPum.mCon_flow_nominal)
+    "Gain to scale the time table output to flow rate" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-70,8})));
+  Modelica.Blocks.Sources.CombiTimeTable tabMea(
+    tableOnFile=true,
+    tableName="MeasuredData",
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/Data/Fluid/HeatPumps/Validation/MeasuredHeatPumpData.txt"),
+    columns=2:10,
+    extrapolation=Modelica.Blocks.Types.Extrapolation.HoldLastPoint)
+    "Table with measurement data"
+    annotation (Placement(transformation(extent={{-90,70},{-70,90}})));
+
+  Modelica.Blocks.Interfaces.RealOutput TConOutMea(unit="K", displayUnit="degC")
+    "Measured condenser outlet"
+    annotation (Placement(transformation(extent={{100,80},{120,100}})));
+  Modelica.Blocks.Interfaces.RealOutput TEvaOutMea(unit="K", displayUnit="degC")
+    "Measured evaporator outlet"
+    annotation (Placement(transformation(extent={{100,0},{120,20}})));
+  Modelica.Blocks.Interfaces.RealOutput PEleMea(unit="W")
+    "Measured electrical power consumption"
+    annotation (Placement(transformation(extent={{100,-78},{120,-58}})));
+  Modelica.Blocks.Interfaces.RealOutput PEleSim(unit="W")
+    "Simulated electrical power consumption"
+    annotation (Placement(transformation(extent={{100,-102},{120,-82}})));
+  Modelica.Blocks.Interfaces.RealOutput TConOutSim(unit="K", displayUnit="degC")
+    "Simulated condenser outlet"
+    annotation (Placement(transformation(extent={{100,60},{120,80}})));
+  Modelica.Blocks.Interfaces.RealOutput TEvaOutSim(unit="K", displayUnit="degC")
+    "Simulated evaporator outlet"
+    annotation (Placement(transformation(extent={{100,-20},{120,0}})));
+  Modelica.Blocks.Sources.RealExpression reaPEle(y=heaPum.refCyc.PEle)
+    "Use of internal heat pump state for PEle"
+    annotation (Placement(transformation(extent={{40,-100},{60,-80}})));
+  Modelica.Blocks.Sources.RealExpression reaTEvaOut(y=heaPum.eva.T)
+    "Use of internal heat pump state for TEvaOut"
+    annotation (Placement(transformation(extent={{60,-20},{80,0}})));
+  Modelica.Blocks.Sources.RealExpression reaTConOut(y=heaPum.con.T)
+    "Use of internal heat pump state for TConOut"
+    annotation (Placement(transformation(extent={{60,60},{80,80}})));
+equation
+
+  connect(souSidMasFlowSou.ports[1], heaPum.port_a2) annotation (Line(points={{-20,-72},
+          {32,-72},{32,-36.8},{21,-36.8}},           color={0,127,255}));
+  connect(heaPum.port_b2, souSidFixBou.ports[1]) annotation (Line(points={{0,-36.8},
+          {-8,-36.8},{-8,-37},{-22,-37}},color={0,127,255}));
+  connect(heaPum.port_b1, sinSidFixBou.ports[1]) annotation (Line(points={{21,
+          -24.2},{36,-24.2},{36,-24},{40,-24}},
+                                     color={0,127,255}));
+  connect(heaPum.port_a1, sinSidMasFlowSou.ports[1]) annotation (Line(points={{0,-24.2},
+          {0,-24},{-4,-24},{-4,0},{-20,0}},   color={0,127,255}));
+  connect(mEva_flow.y, souSidMasFlowSou.m_flow_in)
+    annotation (Line(points={{-59,-50},{-50,-50},{-50,-64},{-42,-64}},
+                                                             color={0,0,127}));
+  connect(sinSidMasFlowSou.m_flow_in, mCon_flow.y)
+    annotation (Line(points={{-42,8},{-59,8}},         color={0,0,127}));
+  connect(tabMea.y[5], mEva_flow.u) annotation (Line(points={{-69,80},{-54,80},
+          {-54,26},{-88,26},{-88,-50},{-82,-50}}, color={0,0,127}));
+  connect(tabMea.y[7], mCon_flow.u) annotation (Line(points={{-69,80},{-54,80},
+          {-54,26},{-88,26},{-88,8},{-82,8}},
+                             color={0,0,127}));
+  connect(tabMea.y[6], heaPum.ySet) annotation (Line(points={{-69,80},{-54,80},
+          {-54,26},{-12,26},{-12,-28},{-1.155,-28},{-1.155,-28.505}},
+                                                color={0,0,127}));
+  connect(tabMea.y[9], souSidMasFlowSou.T_in) annotation (Line(points={{-69,80},
+          {-54,80},{-54,26},{-88,26},{-88,-68},{-42,-68}}, color={0,0,127}));
+  connect(sinSidMasFlowSou.T_in, tabMea.y[1]) annotation (Line(points={{-42,4},
+          {-54,4},{-54,80},{-69,80}},          color={0,0,127}));
+  connect(tabMea.y[2], TConOutMea)
+    annotation (Line(points={{-69,80},{22,80},{22,90},{110,90}},
+                                                 color={0,0,127}));
+  connect(tabMea.y[8], TEvaOutMea) annotation (Line(points={{-69,80},{92,80},{92,
+          10},{110,10}}, color={0,0,127}));
+  connect(tabMea.y[3], PEleMea) annotation (Line(points={{-69,80},{92,80},{92,-68},
+          {110,-68}}, color={0,0,127}));
+  connect(reaPEle.y, PEleSim) annotation (Line(points={{61,-90},{82,-90},{82,
+          -92},{110,-92}}, color={0,0,127}));
+  connect(TEvaOutSim, reaTEvaOut.y)
+    annotation (Line(points={{110,-10},{81,-10}}, color={0,0,127}));
+  connect(TConOutSim, reaTConOut.y)
+    annotation (Line(points={{110,70},{81,70}}, color={0,0,127}));
+  annotation (Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-100,
+            -100},{100,100}})),
+    experiment(Tolerance=1e-6, StopTime=3600),
+    Documentation(info="<html>
+<p>
+  Partial model for the validation of different modular heat pump approaches
+  based on measured data of a brine-to-water heat pump at the Institute for
+  Energy Efficient Building and Indoor Climate.</p>
+<p>
+  If questions regarding the data or model
+  arises, please raise an issue and link FWuellhorst.
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialValidation;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/package.mo
new file mode 100644
index 0000000000..9b507f69d4
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/package.mo
@@ -0,0 +1,8 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation;
+package BaseClasses "Partial validation models"
+  extends Modelica.Icons.BasesPackage;
+
+annotation (Documentation(info="<html>
+<p>Package with partial models for heat pump validations.</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/package.order
new file mode 100644
index 0000000000..d3ef8abcd1
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/BaseClasses/package.order
@@ -0,0 +1 @@
+PartialValidation
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/PartialComparison.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/PartialComparison.mo
new file mode 100644
index 0000000000..66eae81252
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/PartialComparison.mo
@@ -0,0 +1,111 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative.BaseClasses;
+partial model PartialComparison
+  "Partial model to allow heat pump and chiller model comparison"
+  package Medium1 = AixLib.Media.Water "Medium model";
+  package Medium2 = AixLib.Media.Water "Medium model";
+
+  parameter Modelica.Units.SI.HeatFlowRate QUse_flow_nominal = 30E3
+    "Nominal capacity";
+
+  parameter Modelica.Units.SI.TemperatureDifference dTEva_nominal=10
+    "Temperature difference evaporator outlet-inlet";
+  parameter Modelica.Units.SI.TemperatureDifference dTCon_nominal=10
+    "Temperature difference condenser outlet-inlet";
+
+  parameter Modelica.Units.SI.Pressure dp1_nominal=6000
+    "Pressure difference over condenser";
+  parameter Modelica.Units.SI.Pressure dp2_nominal=6000
+    "Pressure difference over evaporator";
+  parameter Real etaCarnot_nominal=0.3
+    "Carnot effectiveness (=COP/COP_Carnot) used during simulation if use_eta_Carnot_nominal = true";
+  parameter Modelica.Units.SI.Time tau1=60
+    "Time constant at nominal flow rate (used if energyDynamics1 <> Modelica.Fluid.Types.Dynamics.SteadyState)";
+  parameter Modelica.Units.SI.Temperature T1_start=303.15
+    "Initial or guess value of set point";
+  parameter Modelica.Units.SI.Time tau2=60
+    "Time constant at nominal flow rate (used if energyDynamics2 <> Modelica.Fluid.Types.Dynamics.SteadyState)";
+  parameter Modelica.Units.SI.Temperature T2_start=278.15
+    "Initial or guess value of set point";
+
+  parameter Modelica.Units.SI.Temperature TConIn_nominal=303.15
+    "Nominal condenser inlet temperature";
+  parameter Modelica.Units.SI.Temperature TEvaIn_nominal=288.15
+    "Nominal condenser inlet temperature";
+
+  parameter Modelica.Units.SI.Temperature TCon_nominal=TConIn_nominal + dTCon_nominal
+    "Nominal condenser temperature";
+  parameter Modelica.Units.SI.Temperature TEva_nominal=TEvaIn_nominal -
+      dTEva_nominal
+    "Nominal evaporator temperature";
+  parameter Modelica.Units.SI.MassFlowRate m2_flow_nominal
+    "Nominal mass flow rate at chilled water side";
+  parameter Modelica.Units.SI.MassFlowRate m1_flow_nominal
+    "Nominal mass flow rate at condenser water wide";
+  AixLib.Fluid.Sources.MassFlowSource_T sou1(
+    redeclare package Medium = Medium1,
+    use_T_in=true,
+    m_flow=m1_flow_nominal,
+    T=298.15) "Condenser mass flow source"
+    annotation (Placement(transformation(extent={{-60,-4},{-40,16}})));
+  AixLib.Fluid.Sources.MassFlowSource_T sou2(
+    redeclare package Medium = Medium2,
+    use_T_in=true,
+    m_flow=m2_flow_nominal,
+    T=291.15) "Evaporator mass flow source"
+    annotation (Placement(transformation(extent={{60,-16},{40,4}})));
+  AixLib.Fluid.Sources.Boundary_pT sin1(redeclare package Medium = Medium1)
+    annotation (Placement(
+        transformation(
+        extent={{10,-10},{-10,10}},
+        origin={70,30})));
+  AixLib.Fluid.Sources.Boundary_pT sin2(redeclare package Medium = Medium2)
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        origin={-50,-30})));
+  Modelica.Blocks.Sources.Ramp uCom(
+    height=-1,
+    duration=60,
+    offset=1,
+    startTime=1800) "Compressor control signal"
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+  Modelica.Blocks.Sources.Ramp TCon_in(
+    height=10,
+    duration=60,
+    offset=TConIn_nominal - 10,
+    startTime=60) "Condenser inlet temperature"
+    annotation (Placement(transformation(extent={{-90,0},{-70,20}})));
+  Modelica.Blocks.Sources.Ramp TEva_in(
+    height=10,
+    duration=60,
+    startTime=900,
+    offset=TEvaIn_nominal) "Evaporator inlet temperature"
+    annotation (Placement(transformation(extent={{50,-50},{70,-30}})));
+equation
+  connect(TCon_in.y,sou1. T_in) annotation (Line(
+      points={{-69,10},{-62,10}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(TEva_in.y,sou2. T_in) annotation (Line(
+      points={{71,-40},{80,-40},{80,-2},{62,-2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model which is based on
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_y\">
+AixLib.Fluid.HeatPumps.Examples.Carnot_y</a>
+to validate the modular reversible models by means of
+comparison to the <a href=\"modelica://AixLib.Fluid.HeatPumps.Carnot_y\">
+AixLib.Fluid.HeatPumps.Carnot_y</a> model.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialComparison;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/PartialModularComparison.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/PartialModularComparison.mo
new file mode 100644
index 0000000000..d54cfdbb4c
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/PartialModularComparison.mo
@@ -0,0 +1,72 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative.BaseClasses;
+partial model PartialModularComparison
+  "Partial model for comparison to the Carnot model"
+  extends PartialComparison(
+    m1_flow_nominal=heaPum.mCon_flow_nominal,
+    m2_flow_nominal=heaPum.mEva_flow_nominal,
+    sou1(nPorts=1),
+    sin2(nPorts=1),
+    sou2(nPorts=1),
+    sin1(nPorts=1));
+
+  AixLib.Fluid.HeatPumps.ModularReversible.Modular heaPum(
+    redeclare final package MediumCon = Medium1,
+    redeclare final package MediumEva = Medium2,
+    QHea_flow_nominal=QUse_flow_nominal,
+    redeclare final model RefrigerantCycleInertia =
+        AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.NoInertia,
+    final use_rev=false,
+    final use_intSafCtr=false,
+    final tauCon=tau1,
+    final TConHea_nominal=TCon_nominal,
+    final dTCon_nominal=dTCon_nominal,
+    final dpCon_nominal=dp1_nominal,
+    final use_conCap=false,
+    final CCon=0,
+    final GConOut=0,
+    final GConIns=0,
+    final tauEva=tau2,
+    final TEvaHea_nominal=TEva_nominal,
+    final dTEva_nominal=dTEva_nominal,
+    final dpEva_nominal=dp2_nominal,
+    final TConCoo_nominal=0,
+    final TEvaCoo_nominal=0,
+    final use_evaCap=false,
+    final CEva=0,
+    final GEvaOut=0,
+    final GEvaIns=0,
+    final TCon_start=T1_start,
+    final TEva_start=T2_start,
+    final energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial)
+    "Modular heat pump model"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+
+equation
+  connect(heaPum.port_a1, sou1.ports[1])
+    annotation (Line(points={{-10,6},{-40,6}}, color={0,127,255}));
+  connect(heaPum.port_b2, sin2.ports[1]) annotation (Line(points={{-10,-6},{-32,
+          -6},{-32,-30},{-40,-30}},
+                                color={0,127,255}));
+  connect(heaPum.port_a2, sou2.ports[1])
+    annotation (Line(points={{10,-6},{40,-6}}, color={0,127,255}));
+  connect(heaPum.port_b1, sin1.ports[1])
+    annotation (Line(points={{10,6},{36,6},{36,30},{60,30}}, color={0,127,255}));
+  connect(heaPum.ySet, uCom.y) annotation (Line(points={{-11.2,2},{-34,2},{-34,50},
+          {-39,50}},             color={0,0,127}));
+
+  annotation (
+    Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model to have consitent parameterization of the
+modular reversible model approaches.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialModularComparison;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/package.mo
new file mode 100644
index 0000000000..4ac4141615
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/package.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative;
+package BaseClasses "Package with partial validation models"
+extends Modelica.Icons.BasesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains partial models for comparative validation.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/package.order
new file mode 100644
index 0000000000..15bbc82f11
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/BaseClasses/package.order
@@ -0,0 +1,2 @@
+PartialComparison
+PartialModularComparison
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/Carnot_y.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/Carnot_y.mo
new file mode 100644
index 0000000000..831d83149f
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/Carnot_y.mo
@@ -0,0 +1,62 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative;
+model Carnot_y "Example using the Carnot model approach"
+  extends BaseClasses.PartialComparison(
+    m1_flow_nominal=heaPum.m1_flow_nominal,
+    m2_flow_nominal=heaPum.m2_flow_nominal,
+    sin2(nPorts=1),
+    sou2(nPorts=1),
+    sin1(nPorts=1),
+    sou1(nPorts=1));
+  extends Modelica.Icons.Example;
+  AixLib.Fluid.HeatPumps.Carnot_y heaPum(
+    redeclare package Medium1 = Medium1,
+    redeclare package Medium2 = Medium2,
+    etaCarnot_nominal=etaCarnot_nominal,
+    TCon_nominal=TCon_nominal,
+    TEva_nominal=TEva_nominal,
+    tau1=tau1,
+    tau2=tau2,
+    P_nominal=QUse_flow_nominal/heaPum.COP_nominal,
+    dTEva_nominal=-dTEva_nominal,
+    dTCon_nominal=dTCon_nominal,
+    use_eta_Carnot_nominal=false,
+    dp1_nominal=dp1_nominal,
+    dp2_nominal=dp2_nominal,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    show_T=true,
+    T1_start=T1_start,
+    T2_start=T2_start) "Heat pump model"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+
+equation
+  connect(sin2.ports[1], heaPum.port_b2) annotation (Line(points={{-40,-30},{-16,
+          -30},{-16,-6},{-10,-6}}, color={0,127,255}));
+  connect(heaPum.port_a2, sou2.ports[1])
+    annotation (Line(points={{10,-6},{40,-6}},color={0,127,255}));
+  connect(heaPum.port_b1, sin1.ports[1])
+    annotation (Line(points={{10,6},{36,6},{36,30},{60,30}},color={0,127,255}));
+  connect(heaPum.port_a1, sou1.ports[1])
+    annotation (Line(points={{-10,6},{-40,6}}, color={0,127,255}));
+  connect(heaPum.y, uCom.y)
+    annotation (Line(points={{-12,9},{-12,50},{-39,50}}, color={0,0,127}));
+
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/Carnot_y.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Validation case for <a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">
+AixLib.Fluid.Chillers.Carnot_y</a>, duplicate of the example
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_y\">
+AixLib.Fluid.Chillers.Examples.Carnot_y</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Carnot_y;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/ConstantCarnotEffectiveness.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/ConstantCarnotEffectiveness.mo
new file mode 100644
index 0000000000..bebe8c53e3
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/ConstantCarnotEffectiveness.mo
@@ -0,0 +1,27 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative;
+model ConstantCarnotEffectiveness
+  "Validation case for modular Carnot approach"
+  extends BaseClasses.PartialModularComparison(heaPum(redeclare model
+        RefrigerantCycleHeatPumpHeating =
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness
+          (etaCarnot_nominal=etaCarnot_nominal)));
+  extends Modelica.Icons.Example;
+
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/ConstantCarnotEffectiveness.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Validation case for <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness\">
+AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ConstantCarnotEffectiveness;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/TableData2D.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/TableData2D.mo
new file mode 100644
index 0000000000..9629ea0c1c
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/TableData2D.mo
@@ -0,0 +1,43 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative;
+model TableData2D "Validation case for table data approach"
+  extends BaseClasses.PartialModularComparison(
+    TEva_nominal=TEvaIn_nominal,
+    TCon_nominal=TConIn_nominal,
+    heaPum(redeclare model RefrigerantCycleHeatPumpHeating =
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D (
+            datTab(
+            tabPEle=[0,288.15,298.15; 293.15,12375.1,12375.1; 303.15,12375.1,
+                12375.1],
+            mCon_flow_nominal=m1_flow_nominal,
+            mEva_flow_nominal=m2_flow_nominal,
+            dpCon_nominal=0,
+            dpEva_nominal=0,
+            devIde="CarnotTableData",
+            use_TEvaOutForTab=false,
+            use_TConOutForTab=false,
+            tabQCon_flow=[0,288.15,298.15; 293.15,34084.9,0; 303.15,30000,34620],
+
+            tabUppBou=[273.15,273.15; 273.15,273.15],
+            use_TEvaOutForOpeEnv=false,
+            use_TConOutForOpeEnv=false))));
+
+  extends Modelica.Icons.Example;
+
+  annotation (experiment(Tolerance=1e-6, StopTime=3600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/TableData2D.mos"
+        "Simulate and plot"),
+    Documentation(revisions="<html>
+<ul>
+<li>
+November 13, 2023 by Fabian Wuellhorst:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Validation case for <a href=\"modelica://AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D\">
+AixLib.Fluid.Chillers.ModularReversible.RefrigerantCycle.TableData2D</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TableData2D;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/package.mo
new file mode 100644
index 0000000000..1ddd9eec28
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation;
+package Comparative "Package for comparative model validation"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains models that validate the modular reversible chiller models
+using comparative validation against the Carnot model:
+<a href=\"modelica://AixLib.Fluid.Chillers.Examples.Carnot_y\">
+AixLib.Fluid.Chillers.Examples.Carnot_y</a>
+</p>
+</html>"));
+end Comparative;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/package.order
new file mode 100644
index 0000000000..bc40b5cefa
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/Comparative/package.order
@@ -0,0 +1,4 @@
+Carnot_y
+ConstantCarnotEffectiveness
+TableData2D
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/ConstantCarnotEffectiveness.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/ConstantCarnotEffectiveness.mo
new file mode 100644
index 0000000000..cb0654dc1c
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/ConstantCarnotEffectiveness.mo
@@ -0,0 +1,57 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation;
+model ConstantCarnotEffectiveness
+  extends Modelica.Icons.Example;
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.Validation.BaseClasses.PartialValidation(
+     heaPum(
+      QHea_flow_nominal=etaCarnot_nominal*PEle_nominal*heaPum.TConHea_nominal/(heaPum.TConHea_nominal
+           - heaPum.TEvaHea_nominal),
+      mCon_flow_nominal=mCon_flow_nominal,
+      tauCon=VCon*heaPum.rhoCon/mCon_flow_nominal,
+      redeclare model RefrigerantCycleInertia =
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.VariableOrder
+          (
+          refIneFreConst=refIneFreConst,
+          nthOrd=2,
+          initType=Modelica.Blocks.Types.Init.InitialState),
+      redeclare model RefrigerantCycleHeatPumpHeating =
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.ConstantCarnotEffectiveness
+          (TAppCon_nominal=0,
+           TAppEva_nominal=0,
+           etaCarnot_nominal=etaCarnot_nominal)));
+
+  parameter Real etaCarnot_nominal=0.4318 "Calibrated constant Carnot effectiveness";
+  parameter Modelica.Units.SI.Power PEle_nominal=1884.218212
+    "Calibrated nominal electrical power consumption";
+
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_nominal=0.407396
+    "Calibrated condenser nominal mass flow rate";
+  parameter Modelica.Units.SI.Volume VCon=0.0015972
+    "Calibrated condenser volume";
+  parameter Modelica.Units.SI.Frequency refIneFreConst=13.2e-3
+    "Calibrated cut off frequency for inertia of refrigerant cycle";
+
+annotation (experiment(Tolerance=1e-6, StopTime=14365),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/ConstantCarnotEffectiveness.mos"
+          "Simulate and plot"),
+  Documentation(info="<html>
+<p>
+  This validation case uses a constant Carnot effectiveness
+  to model the efficiency of the heat pump.
+</p>
+<p>
+  The approach was calibrated as a comparison to table-based data in
+  the conference paper for the heat pump model:
+  <a href=\"https://doi.org/10.3384/ecp21181561\">
+  https://doi.org/10.3384/ecp21181561 </a>
+</p>
+</html>",   revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ConstantCarnotEffectiveness;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/TableData2D.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/TableData2D.mo
new file mode 100644
index 0000000000..829503278d
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/TableData2D.mo
@@ -0,0 +1,60 @@
+within AixLib.Fluid.HeatPumps.ModularReversible.Validation;
+model TableData2D
+  extends Modelica.Icons.Example;
+  extends
+    AixLib.Fluid.HeatPumps.ModularReversible.Validation.BaseClasses.PartialValidation(
+      heaPum(
+      QHea_flow_nominal=heaPum.refCyc.refCycHeaPumHea.QHeaNoSca_flow_nominal,
+      mCon_flow_nominal=mCon_flow_nominal,
+      tauCon=VCon*heaPum.rhoCon/mCon_flow_nominal,
+      redeclare model RefrigerantCycleInertia =
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.Inertias.VariableOrder
+          (
+          refIneFreConst=refIneFreConst,
+          nthOrd=2,
+          initType=Modelica.Blocks.Types.Init.InitialState),
+      redeclare model RefrigerantCycleHeatPumpHeating =
+          AixLib.Fluid.HeatPumps.ModularReversible.RefrigerantCycle.TableData2D (
+            datTab=
+              AixLib.Fluid.HeatPumps.ModularReversible.Data.TableData2D.GenericHeatPump(
+              tabPEle=[0,273.15,283.15; 308.15,1300,1500; 328.15,1900,2300],
+              mCon_flow_nominal=6100/5/4184,
+              mEva_flow_nominal=4800/5/4184,
+              dpCon_nominal=0,
+              dpEva_nominal=0,
+              devIde="Vaillaint_VWL101",
+              use_TEvaOutForTab=false,
+              use_TConOutForTab=true,
+              tabQCon_flow=[0,273.15,283.15; 308.15,6100,8400; 328.15,5700,7600],
+              tabUppBou=[-40,70; 40,70]))));
+
+  parameter Modelica.Units.SI.MassFlowRate mCon_flow_nominal=0.404317
+    "Condenser nominal mass flow rate";
+  parameter Modelica.Units.SI.Volume VCon=0.004473
+    "Condenser volume";
+  parameter Modelica.Units.SI.Frequency refIneFreConst=0.011848
+    "Cut off frequency for inertia of refrigerant cycle";
+
+  annotation (experiment(Tolerance=1e-6, StopTime=14365),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/TableData2D.mos"
+            "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+  This validation case uses table-based data for the heat pump.
+</p>
+<p>
+  The approach was calibrated as a comparison to constant Carnot effectiveness
+  approach in the conference paper for the heat pump model:
+  <a href=\"https://doi.org/10.3384/ecp21181561\">
+  https://doi.org/10.3384/ecp21181561</a>
+</p>
+</html>", revisions="<html><ul>
+  <li>
+    <i>October 2, 2022</i> by Fabian Wuellhorst:<br/>
+    First implementation (see issue <a href=
+    \"https://github.com/ibpsa/modelica-ibpsa/issues/1576\">#1576</a>)
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TableData2D;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/package.mo
new file mode 100644
index 0000000000..93f34e2d09
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Fluid.HeatPumps.ModularReversible;
+package Validation "Collection of validation models"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains validation models for the classes in
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible\">
+AixLib.Fluid.HeatPumps.ModularReversible</a>.
+</p>
+<p>
+Note that most validation models contain simple input data
+which may not be realistic, but for which the correct
+output can be obtained through an analytic solution.
+The examples plot various outputs, which have been verified against these
+solutions. These model outputs are stored as reference data and
+used for continuous validation whenever models in the library change.
+</p>
+</html>"));
+end Validation;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/Validation/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/package.order
new file mode 100644
index 0000000000..ce7e44e6f4
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/Validation/package.order
@@ -0,0 +1,4 @@
+ConstantCarnotEffectiveness
+TableData2D
+Comparative
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/package.mo b/AixLib/Fluid/HeatPumps/ModularReversible/package.mo
new file mode 100644
index 0000000000..2e277d7796
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.HeatPumps;
+package ModularReversible "Package for reversible and non-reversible heat pumps using a modular model approach"
+  extends Modelica.Icons.VariantsPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+Package with models and packages for the modular reversible heat pump approach.
+See the <a href=\"modelica://AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide\">AixLib.Fluid.HeatPumps.ModularReversible.UsersGuide</a>
+for more information.
+</p>
+</html>"));
+end ModularReversible;
diff --git a/AixLib/Fluid/HeatPumps/ModularReversible/package.order b/AixLib/Fluid/HeatPumps/ModularReversible/package.order
new file mode 100644
index 0000000000..6daa6be60d
--- /dev/null
+++ b/AixLib/Fluid/HeatPumps/ModularReversible/package.order
@@ -0,0 +1,12 @@
+UsersGuide
+AirToWaterTableData2D
+CarnotWithLosses
+LargeScaleWaterToWater
+Modular
+TableData2D
+Controls
+RefrigerantCycle
+Data
+Examples
+Validation
+BaseClasses
diff --git a/AixLib/Fluid/HeatPumps/ReciprocatingWaterToWater.mo b/AixLib/Fluid/HeatPumps/ReciprocatingWaterToWater.mo
index 128bcc4d44..0edb721e28 100644
--- a/AixLib/Fluid/HeatPumps/ReciprocatingWaterToWater.mo
+++ b/AixLib/Fluid/HeatPumps/ReciprocatingWaterToWater.mo
@@ -23,78 +23,78 @@ model ReciprocatingWaterToWater
         iconTransformation(extent={{100,-100},{120,-80}})),
               defaultComponentName="heaPum",
     Documentation(info="<html>
- <p>
- Model for a water to water heat pump with a reciprocating compressor, as
- described in Jin (2002). The thermodynamic heat pump cycle is represented below.
- </p>
- <p align=\"center\">
- <img  alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/HeatPumps/WaterToWater_Cycle.png\" border=\"1\"/>
- </p>
- <p>
- The rate of heat transferred to the evaporator is given by:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q&#775;<sub>Eva</sub> = m&#775;<sub>ref</sub> ( h<sub>Vap</sub>(T<sub>Eva</sub>) - h<sub>Liq</sub>(T<sub>Con</sub>) ).
- </p>
- <p>
- The power consumed by the compressor is given by a linear efficiency relation:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- P = P<sub>Theoretical</sub> / &eta; + P<sub>Loss,constant</sub>.
- </p>
- <p>
- Heat transfer in the evaporator and condenser is calculated using an
- &epsilon;-NTU method, assuming constant refrigerant temperature and constant heat
- transfer coefficient between fluid and refrigerant.
- </p>
- <p>
- Variable speed is acheived by multiplying the full load piston displacement
- by the normalized compressor speed. The power and heat transfer rates are forced
- to zero if the resulting heat pump state has higher evaporating pressure than
- condensing pressure.
- </p>
- <h4>Options</h4>
- <p>
- Parameters <code>TConMax</code> and <code>TEvaMin</code>
- may be used to set an upper or lower bound for the
- condenser and evaporator.
- The compressor is disabled when these conditions
- are not satisfied, or when the
- evaporator temperature is larger
- than the condenser temperature.
- This mimics the temperature protection
- of heat pumps and moreover it avoids
- non-converging algebraic loops of equations,
- or freezing of evaporator medium.
- This option can be disabled by setting
- <code>enable_temperature_protection = false</code>.
- </p>
- <h4>Assumptions and limitations</h4>
- <p>
- The compression process is assumed isentropic. The thermal energy
- of superheating is ignored in the evaluation of the heat transferred to the refrigerant
- in the evaporator. There is no supercooling.
- </p>
- <h4>References</h4>
- <p>
- H. Jin.
- <i>
- Parameter estimation based models of water source heat pumps.
- </i>
- PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 30, 2017, by Filip Jorissen:<br/>
- Revised documentation for temperature protection.
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
- </li>
- <li>
- November 14, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model for a water to water heat pump with a reciprocating compressor, as
+described in Jin (2002). The thermodynamic heat pump cycle is represented below.
+</p>
+<p align=\"center\">
+<img  alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/HeatPumps/WaterToWater_Cycle.png\" border=\"1\"/>
+</p>
+<p>
+The rate of heat transferred to the evaporator is given by:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q&#775;<sub>Eva</sub> = m&#775;<sub>ref</sub> ( h<sub>Vap</sub>(T<sub>Eva</sub>) - h<sub>Liq</sub>(T<sub>Con</sub>) ).
+</p>
+<p>
+The power consumed by the compressor is given by a linear efficiency relation:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+P = P<sub>Theoretical</sub> / &eta; + P<sub>Loss,constant</sub>.
+</p>
+<p>
+Heat transfer in the evaporator and condenser is calculated using an
+&epsilon;-NTU method, assuming constant refrigerant temperature and constant heat
+transfer coefficient between fluid and refrigerant.
+</p>
+<p>
+Variable speed is acheived by multiplying the full load piston displacement
+by the normalized compressor speed. The power and heat transfer rates are forced
+to zero if the resulting heat pump state has higher evaporating pressure than
+condensing pressure.
+</p>
+<h4>Options</h4>
+<p>
+Parameters <code>TConMax</code> and <code>TEvaMin</code>
+may be used to set an upper or lower bound for the
+condenser and evaporator.
+The compressor is disabled when these conditions
+are not satisfied, or when the
+evaporator temperature is larger
+than the condenser temperature.
+This mimics the temperature protection
+of heat pumps and moreover it avoids
+non-converging algebraic loops of equations,
+or freezing of evaporator medium.
+This option can be disabled by setting
+<code>enable_temperature_protection = false</code>.
+</p>
+<h4>Assumptions and limitations</h4>
+<p>
+The compression process is assumed isentropic. The thermal energy
+of superheating is ignored in the evaluation of the heat transferred to the refrigerant
+in the evaporator. There is no supercooling.
+</p>
+<h4>References</h4>
+<p>
+H. Jin.
+<i>
+Parameter estimation based models of water source heat pumps.
+</i>
+PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 30, 2017, by Filip Jorissen:<br/>
+Revised documentation for temperature protection.
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
+</li>
+<li>
+November 14, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReciprocatingWaterToWater;
diff --git a/AixLib/Fluid/HeatPumps/ScrollWaterToWater.mo b/AixLib/Fluid/HeatPumps/ScrollWaterToWater.mo
index db0c74585f..21e5cb0330 100644
--- a/AixLib/Fluid/HeatPumps/ScrollWaterToWater.mo
+++ b/AixLib/Fluid/HeatPumps/ScrollWaterToWater.mo
@@ -21,88 +21,88 @@ model ScrollWaterToWater
         iconTransformation(extent={{100,-100},{120,-80}})),
               defaultComponentName="heaPum",
     Documentation(info="<html>
- <p>
- Model for a water to water heat pump with a scroll compressor, as described
- in Jin (2002). The thermodynamic heat pump cycle is represented below.
- </p>
- <p align=\"center\">
- <img  alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/HeatPumps/WaterToWater_Cycle.png\" border=\"1\"/>
- </p>
- <p>
- The rate of heat transferred to the evaporator is given by:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- Q&#775;<sub>Eva</sub> = m&#775;<sub>ref</sub> ( h<sub>Vap</sub>(T<sub>Eva</sub>) - h<sub>Liq</sub>(T<sub>Con</sub>) ).
- </p>
- <p>
- The power consumed by the compressor is given by a linear efficiency relation:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- P = P<sub>Theoretical</sub> / &eta; + P<sub>Loss,constant</sub>.
- </p>
- <p>
- Heat transfer in the evaporator and condenser is calculated using an
- &epsilon;-NTU method, assuming constant refrigerant temperature and constant heat
- transfer coefficient between fluid and refrigerant.
- </p>
- <p>
- Variable speed is achieved by multiplying the full load suction volume flow rate
- by the normalized compressor speed. The power and heat transfer rates are forced
- to zero if the resulting heat pump state has higher evaporating pressure than
- condensing pressure.
- </p>
- <p>
- The model parameters are obtained by calibration of the heat pump model to
- manufacturer performance data. Calibrated model parameters for various heat
- pumps from different manufacturers are found in
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Data.ScrollWaterToWater\">
- AixLib.Fluid.HeatPumps.Data.ScrollWaterToWater</a>. The calibrated model is
- located in
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Calibration.ScrollWaterToWater\">
- AixLib.Fluid.HeatPumps.Calibration.ScrollWaterToWater</a>.
- </p>
- <h4>Options</h4>
- <p>
- Parameters <code>TConMax</code> and <code>TEvaMin</code>
- may be used to set an upper or lower bound for the
- condenser and evaporator.
- The compressor is disabled when these conditions
- are not satisfied, or when the
- evaporator temperature is larger
- than the condenser temperature.
- This mimics the temperature protection
- of heat pumps and moreover it avoids
- non-converging algebraic loops of equations,
- or freezing of evaporator medium.
- This option can be disabled by setting
- <code>enable_temperature_protection = false</code>.
- </p>
- <h4>Assumptions and limitations</h4>
- <p>
- The compression process is assumed isentropic. The thermal energy
- of superheating is ignored in the evaluation of the heat transferred to the refrigerant
- in the evaporator. There is no supercooling.
- </p>
- <h4>References</h4>
- <p>
- H. Jin.
- <i>
- Parameter estimation based models of water source heat pumps.
- </i>
- PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 30, 2017, by Filip Jorissen:<br/>
- Revised documentation for temperature protection.
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
- </li>
- <li>
- November 11, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model for a water to water heat pump with a scroll compressor, as described
+in Jin (2002). The thermodynamic heat pump cycle is represented below.
+</p>
+<p align=\"center\">
+<img  alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/HeatPumps/WaterToWater_Cycle.png\" border=\"1\"/>
+</p>
+<p>
+The rate of heat transferred to the evaporator is given by:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q&#775;<sub>Eva</sub> = m&#775;<sub>ref</sub> ( h<sub>Vap</sub>(T<sub>Eva</sub>) - h<sub>Liq</sub>(T<sub>Con</sub>) ).
+</p>
+<p>
+The power consumed by the compressor is given by a linear efficiency relation:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+P = P<sub>Theoretical</sub> / &eta; + P<sub>Loss,constant</sub>.
+</p>
+<p>
+Heat transfer in the evaporator and condenser is calculated using an
+&epsilon;-NTU method, assuming constant refrigerant temperature and constant heat
+transfer coefficient between fluid and refrigerant.
+</p>
+<p>
+Variable speed is achieved by multiplying the full load suction volume flow rate
+by the normalized compressor speed. The power and heat transfer rates are forced
+to zero if the resulting heat pump state has higher evaporating pressure than
+condensing pressure.
+</p>
+<p>
+The model parameters are obtained by calibration of the heat pump model to
+manufacturer performance data. Calibrated model parameters for various heat
+pumps from different manufacturers are found in
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Data.ScrollWaterToWater\">
+AixLib.Fluid.HeatPumps.Data.ScrollWaterToWater</a>. The calibrated model is
+located in
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Calibration.ScrollWaterToWater\">
+AixLib.Fluid.HeatPumps.Calibration.ScrollWaterToWater</a>.
+</p>
+<h4>Options</h4>
+<p>
+Parameters <code>TConMax</code> and <code>TEvaMin</code>
+may be used to set an upper or lower bound for the
+condenser and evaporator.
+The compressor is disabled when these conditions
+are not satisfied, or when the
+evaporator temperature is larger
+than the condenser temperature.
+This mimics the temperature protection
+of heat pumps and moreover it avoids
+non-converging algebraic loops of equations,
+or freezing of evaporator medium.
+This option can be disabled by setting
+<code>enable_temperature_protection = false</code>.
+</p>
+<h4>Assumptions and limitations</h4>
+<p>
+The compression process is assumed isentropic. The thermal energy
+of superheating is ignored in the evaluation of the heat transferred to the refrigerant
+in the evaporator. There is no supercooling.
+</p>
+<h4>References</h4>
+<p>
+H. Jin.
+<i>
+Parameter estimation based models of water source heat pumps.
+</i>
+PhD Thesis. Oklahoma State University. Stillwater, Oklahoma, USA. 2002.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 30, 2017, by Filip Jorissen:<br/>
+Revised documentation for temperature protection.
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
+</li>
+<li>
+November 11, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollWaterToWater;
diff --git a/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_LimitedCapacity.mo b/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_LimitedCapacity.mo
index 9ef91665fb..85eccfe342 100644
--- a/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_LimitedCapacity.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_LimitedCapacity.mo
@@ -6,19 +6,19 @@ model Carnot_TCon_LimitedCapacity
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/Validation/Carnot_TCon_LimitedCapacity.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_TCon\">
- AixLib.Fluid.HeatPumps.Examples.Carnot_TCon</a>
- but limits the heating capacity.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 5, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_TCon\">
+AixLib.Fluid.HeatPumps.Examples.Carnot_TCon</a>
+but limits the heating capacity.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 5, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TCon_LimitedCapacity;
diff --git a/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_LowTemperature.mo b/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_LowTemperature.mo
index 2a700e7c2e..93cc92f915 100644
--- a/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_LowTemperature.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_LowTemperature.mo
@@ -15,24 +15,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/Validation/Carnot_TCon_LowTemperature.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_TCon\">
- AixLib.Fluid.HeatPumps.Examples.Carnot_TCon</a>
- but decreases the set point for the leaving condenser temperature
- to be below its inlet temperature, in which case the model provides no heating.
- Towards the end of the simulation, the inlet temperature of the condenser is decreased
- to be below the evaporator temperature. In this domain, the model requires cooling
- again. While this is not a meaningful operating point for the model, the example
- verifies that it robustly simulates this regime.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 10, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_TCon\">
+AixLib.Fluid.HeatPumps.Examples.Carnot_TCon</a>
+but decreases the set point for the leaving condenser temperature
+to be below its inlet temperature, in which case the model provides no heating.
+Towards the end of the simulation, the inlet temperature of the condenser is decreased
+to be below the evaporator temperature. In this domain, the model requires cooling
+again. While this is not a meaningful operating point for the model, the example
+verifies that it robustly simulates this regime.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 10, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TCon_LowTemperature;
diff --git a/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_etaPL.mo b/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_etaPL.mo
index 4aeda707ae..878c1255d4 100644
--- a/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_etaPL.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_etaPL.mo
@@ -8,19 +8,19 @@ model Carnot_TCon_etaPL
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/Validation/Carnot_TCon_etaPL.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_TCon\">
- AixLib.Fluid.HeatPumps.Examples.Carnot_TCon</a>
- but has a part load efficiency that varies with the load.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 10, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_TCon\">
+AixLib.Fluid.HeatPumps.Examples.Carnot_TCon</a>
+but has a part load efficiency that varies with the load.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 10, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TCon_etaPL;
diff --git a/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_reverseFlow.mo b/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_reverseFlow.mo
index 88c7d1ab9f..bd7024a965 100644
--- a/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_reverseFlow.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/Carnot_TCon_reverseFlow.mo
@@ -38,7 +38,6 @@ model Carnot_TCon_reverseFlow
     m1_flow_nominal=m1_flow_nominal,
     show_T=true,
     use_eta_Carnot_nominal=true,
-    etaCarnot_nominal=0.3,
     QCon_flow_nominal=QCon_flow_nominal,
     allowFlowReversal1=true,
     allowFlowReversal2=true,
@@ -101,29 +100,35 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPum
         "Simulate and plot"),
     Documentation(
 info="<html>
- <p>
- Example that simulates a heat pump whose efficiency is scaled based on the
- Carnot cycle.
- The heat pump takes as an input the condenser leaving water temperature.
- The condenser mass flow rate is computed in such a way that it has
- a temperature difference equal to <code>dTCon_nominal</code>.
- </p>
- <p>
- This example checks the correct behavior if a mass flow rate attains zero.
- </p>
- </html>",
+<p>
+Example that simulates a heat pump whose efficiency is scaled based on the
+Carnot cycle.
+The heat pump takes as an input the condenser leaving water temperature.
+The condenser mass flow rate is computed in such a way that it has
+a temperature difference equal to <code>dTCon_nominal</code>.
+</p>
+<p>
+This example checks the correct behavior if a mass flow rate attains zero.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 25, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 10, 2023, by Michael Wetter:<br/>
+Removed binding of parameter with same value as the default.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1692\">#1692</a>.
+</li>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\">#1072</a>.
+</li>
+<li>
+November 25, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_TCon_reverseFlow;
diff --git a/AixLib/Fluid/HeatPumps/Validation/Carnot_y_etaCar.mo b/AixLib/Fluid/HeatPumps/Validation/Carnot_y_etaCar.mo
index 5a16dc3585..120af1bb95 100644
--- a/AixLib/Fluid/HeatPumps/Validation/Carnot_y_etaCar.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/Carnot_y_etaCar.mo
@@ -9,19 +9,19 @@ model Carnot_y_etaCar
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/Validation/Carnot_y_etaCar.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_y\">
- AixLib.Fluid.HeatPumps.Examples.Carnot_y</a>
- but uses the parameter <code>etaCar</code> instead of <code>COP_nominal</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 5, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_y\">
+AixLib.Fluid.HeatPumps.Examples.Carnot_y</a>
+but uses the parameter <code>etaCar</code> instead of <code>COP_nominal</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 5, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_y_etaCar;
diff --git a/AixLib/Fluid/HeatPumps/Validation/Carnot_y_etaPL.mo b/AixLib/Fluid/HeatPumps/Validation/Carnot_y_etaPL.mo
index 7c5f12e860..71e289b89f 100644
--- a/AixLib/Fluid/HeatPumps/Validation/Carnot_y_etaPL.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/Carnot_y_etaPL.mo
@@ -9,19 +9,19 @@ model Carnot_y_etaPL
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/Validation/Carnot_y_etaPL.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example extends from
- <a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_y\">
- AixLib.Fluid.HeatPumps.Examples.Carnot_y</a>
- but uses a part load efficiency curve that is different from <i>1</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 10, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example extends from
+<a href=\"modelica://AixLib.Fluid.HeatPumps.Examples.Carnot_y\">
+AixLib.Fluid.HeatPumps.Examples.Carnot_y</a>
+but uses a part load efficiency curve that is different from <i>1</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 10, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Carnot_y_etaPL;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_Dynamic.mo b/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_Dynamic.mo
index 44716be078..4cd4c5b43e 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_Dynamic.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_Dynamic.mo
@@ -165,29 +165,29 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater\">
- AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater</a> heat pump model. This
- validation case also tests the stage input to the heat pump models.
- </p>
- <p>
- With constant inlet source and load water temperatures, the heat pumps cycle on
- and off. The apparent capacity of the dynamic model is compared to the
- steady-state model and to the condenser heat transfer rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 14, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater\">
+AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater</a> heat pump model. This
+validation case also tests the stage input to the heat pump models.
+</p>
+<p>
+With constant inlet source and load water temperatures, the heat pumps cycle on
+and off. The apparent capacity of the dynamic model is compared to the
+steady-state model and to the condenser heat transfer rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 14, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReciprocatingWaterToWater_Dynamic;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_ScalingFactor.mo b/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_ScalingFactor.mo
index 71ddbe670e..cc2505a884 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_ScalingFactor.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_ScalingFactor.mo
@@ -170,29 +170,29 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater\">
- AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater</a> heat pump model. This
- validation case also tests the stage input to the heat pump models.
- </p>
- <p>
- With constant inlet source and load water temperatures, the heat pumps cycle on
- and off. The capacity of the scaled heat pump model is compared to the
- capacity of the non-scaled heat pump model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- December 5, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater\">
+AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater</a> heat pump model. This
+validation case also tests the stage input to the heat pump models.
+</p>
+<p>
+With constant inlet source and load water temperatures, the heat pumps cycle on
+and off. The capacity of the scaled heat pump model is compared to the
+capacity of the non-scaled heat pump model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+December 5, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReciprocatingWaterToWater_ScalingFactor;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_Static.mo b/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_Static.mo
index 3c25b32b29..236d5a5960 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_Static.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_Static.mo
@@ -105,28 +105,28 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater\">
- AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater</a> heat pump model.
- </p>
- <p>
- The heat pump power, condenser heat transfer rate and evaporator heat transfer
- rate are calculated for given water temperatures and flow rates on the
- evaporator and condenser sides.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- October 18, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater\">
+AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater</a> heat pump model.
+</p>
+<p>
+The heat pump power, condenser heat transfer rate and evaporator heat transfer
+rate are calculated for given water temperatures and flow rates on the
+evaporator and condenser sides.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+October 18, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReciprocatingWaterToWater_Static;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_VariableSpeed.mo b/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_VariableSpeed.mo
index 637674ea28..08bd8184d1 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_VariableSpeed.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ReciprocatingWaterToWater_VariableSpeed.mo
@@ -107,31 +107,31 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=2000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater\">
- AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater</a> heat pump model.
- </p>
- <p>
- With constant inlet source and load water temperatures, the compressor frequency
- is increased linearly to its full load value and then ramped down to zero.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- April 25, 2017, by Michael Wetter:<br/>
- Changed input signal from ramp to a trapezoid to test switching it off.
- </li>
- <li>
- November 14, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater\">
+AixLib.Fluid.HeatPumps.ReciprocatingWaterToWater</a> heat pump model.
+</p>
+<p>
+With constant inlet source and load water temperatures, the compressor frequency
+is increased linearly to its full load value and then ramped down to zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+April 25, 2017, by Michael Wetter:<br/>
+Changed input signal from ramp to a trapezoid to test switching it off.
+</li>
+<li>
+November 14, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReciprocatingWaterToWater_VariableSpeed;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_Dynamic.mo b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_Dynamic.mo
index c1621f42b3..f95396bf16 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_Dynamic.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_Dynamic.mo
@@ -159,29 +159,29 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
- AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model. This
- validation case also tests the stage input to the heat pump models.
- </p>
- <p>
- With constant inlet source and load water temperatures, the heat pumps cycle on
- and off. The apparent capacity of the dynamic model is compared to the
- steady-state model and to the condenser heat transfer rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 11, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
+AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model. This
+validation case also tests the stage input to the heat pump models.
+</p>
+<p>
+With constant inlet source and load water temperatures, the heat pumps cycle on
+and off. The apparent capacity of the dynamic model is compared to the
+steady-state model and to the condenser heat transfer rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 11, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollWaterToWater_Dynamic;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_ScalingFactor.mo b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_ScalingFactor.mo
index 7d283c2787..5311e3a84d 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_ScalingFactor.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_ScalingFactor.mo
@@ -168,29 +168,29 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
- AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model. This
- validation case also tests the stage input to the heat pump models.
- </p>
- <p>
- With constant inlet source and load water temperatures, the heat pumps cycle on
- and off. The capacity of the scaled heat pump model is compared to the
- capacity of the non-scaled heat pump model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- December 5, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
+AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model. This
+validation case also tests the stage input to the heat pump models.
+</p>
+<p>
+With constant inlet source and load water temperatures, the heat pumps cycle on
+and off. The capacity of the scaled heat pump model is compared to the
+capacity of the non-scaled heat pump model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+December 5, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollWaterToWater_ScalingFactor;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_Static.mo b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_Static.mo
index fc1690a864..723c961084 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_Static.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_Static.mo
@@ -103,28 +103,28 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
- AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model.
- </p>
- <p>
- The heat pump power, condenser heat transfer rate and evaporator heat transfer
- rate are calculated for given water temperatures and flow rates on the
- evaporator and condenser sides.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- October 18, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
+AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model.
+</p>
+<p>
+The heat pump power, condenser heat transfer rate and evaporator heat transfer
+rate are calculated for given water temperatures and flow rates on the
+evaporator and condenser sides.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+October 18, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollWaterToWater_Static;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_TemperatureProtection.mo b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_TemperatureProtection.mo
index 663fb6bbfc..af512465f2 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_TemperatureProtection.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_TemperatureProtection.mo
@@ -104,28 +104,28 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the temperature protection implementation of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
- AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model.
- </p>
- <p>
- The heat pump is disabled when the evaporator and condenser temperature
- requirements are not satisfied.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- May 30, 2017, by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the temperature protection implementation of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
+AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model.
+</p>
+<p>
+The heat pump is disabled when the evaporator and condenser temperature
+requirements are not satisfied.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+May 30, 2017, by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/769\">#769</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollWaterToWater_TemperatureProtection;
diff --git a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_VariableSpeed.mo b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_VariableSpeed.mo
index 8177c4f72a..c84ccab482 100644
--- a/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_VariableSpeed.mo
+++ b/AixLib/Fluid/HeatPumps/Validation/ScrollWaterToWater_VariableSpeed.mo
@@ -99,27 +99,27 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=1000),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
- AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model.
- </p>
- <p>
- With constant inlet source and load water temperatures, the compressor frequency
- is increased linearly to its full load value.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 15, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 11, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.HeatPumps.ScrollWaterToWater\">
+AixLib.Fluid.HeatPumps.ScrollWaterToWater</a> heat pump model.
+</p>
+<p>
+With constant inlet source and load water temperatures, the compressor frequency
+is increased linearly to its full load value.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 11, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ScrollWaterToWater_VariableSpeed;
diff --git a/AixLib/Fluid/HeatPumps/package.order b/AixLib/Fluid/HeatPumps/package.order
index a374509e64..1a0ad34f84 100644
--- a/AixLib/Fluid/HeatPumps/package.order
+++ b/AixLib/Fluid/HeatPumps/package.order
@@ -5,6 +5,7 @@ ReciprocatingWaterToWater
 ScrollWaterToWater
 Calibration
 Compressors
+ModularReversible
 Data
 Examples
 Validation
diff --git a/AixLib/Fluid/Humidifiers/Examples/Humidifier_u.mo b/AixLib/Fluid/Humidifiers/Examples/Humidifier_u.mo
index 68b536f031..3bf438f414 100644
--- a/AixLib/Fluid/Humidifiers/Examples/Humidifier_u.mo
+++ b/AixLib/Fluid/Humidifiers/Examples/Humidifier_u.mo
@@ -105,30 +105,30 @@ equation
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Humidifiers/Examples/Humidifier_u.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that demonstrates the use of an ideal humidifier.
- Both humidifer models are identical, except that one model is configured
- as a steady-state model, whereas the other is configured as a dynamic model.
- Both humidifiers add water to the medium to track a set-point for the outlet
- temperature using adiabatic cooling.
- The temperature of the water that is added to the medium is determined by
- the parameter <code>T</code> of the humidifier models.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 23, 2013, by Michael Wetter:<br/>
- Added flow resistance at the outlet of the humidifier to avoid a numerical derivative,
- and changed model to use a prescribed mass flow rate.
- </li>
- <li>
- July 11, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that demonstrates the use of an ideal humidifier.
+Both humidifer models are identical, except that one model is configured
+as a steady-state model, whereas the other is configured as a dynamic model.
+Both humidifiers add water to the medium to track a set-point for the outlet
+temperature using adiabatic cooling.
+The temperature of the water that is added to the medium is determined by
+the parameter <code>T</code> of the humidifier models.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 23, 2013, by Michael Wetter:<br/>
+Added flow resistance at the outlet of the humidifier to avoid a numerical derivative,
+and changed model to use a prescribed mass flow rate.
+</li>
+<li>
+July 11, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=1200,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Humidifier_u;
diff --git a/AixLib/Fluid/Humidifiers/Humidifier_u.mo b/AixLib/Fluid/Humidifiers/Humidifier_u.mo
index 092715e3cc..3d16ad2b94 100644
--- a/AixLib/Fluid/Humidifiers/Humidifier_u.mo
+++ b/AixLib/Fluid/Humidifiers/Humidifier_u.mo
@@ -45,7 +45,7 @@ equation
           extent={{-52,-60},{58,-120}},
           textString="m=%m_flow_nominal",
           pattern=LinePattern.None,
-          lineColor={0,0,127}),
+          textColor={0,0,127}),
         Rectangle(
           extent={{-100,61},{-70,58}},
           lineColor={0,0,255},
@@ -56,13 +56,6 @@ equation
           extent={{-114,104},{-70,76}},
           textColor={0,0,127},
           textString="u"),
-        Rectangle(
-          visible=use_T_in,
-          extent={{-100,-59},{-70,-62}},
-          lineColor={0,0,0},
-          pattern=LinePattern.None,
-          fillColor={191,0,0},
-          fillPattern=FillPattern.Solid),
         Rectangle(
           extent={{-100,5},{101,-5}},
           lineColor={0,0,255},
@@ -107,93 +100,106 @@ equation
               {42,-28},{42,-26}},
           lineColor={255,255,255},
           fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-98,-57},{-70,-60}},
+          lineColor={0,0,255},
+          pattern=LinePattern.None,
+          fillColor={191,0,0},
           fillPattern=FillPattern.Solid)}),
 defaultComponentName="hum",
 Documentation(info="<html>
- <p>
- Model for an air humidifier or dehumidifier.
- </p>
- <p>
- This model adds (or removes) moisture from the air stream.
- The amount of exchanged moisture is equal to
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- m&#775;<sub>wat</sub> = u  m&#775;<sub>wat,nom</sub>,
- </p>
- <p>
- where <i>u</i> is the control input signal and
- <i>m&#775;<sub>wat,nom</sub></i> is equal to the parameter <code>mWat_flow_nominal</code>.
- The parameter <code>mWat_flow_nominal</code> can be positive or negative.
- If <i>m&#775;<sub>wat</sub></i> is positive, then moisture is added
- to the air stream, otherwise it is removed.
- </p>
- <p>
- If the heat port <code>heatPort</code> is unconnected, then the enthalpy of the
- air that flows through the device remains unchanged, e.g., the humidification
- is adiabatic. To change the enthalpy of the air, add heat flow to the connector
- <code>heatPort</code>.
- </p>
- </html>",
+<p>
+Model for an air humidifier or dehumidifier.
+</p>
+<p>
+This model adds (or removes) moisture from the air stream.
+The amount of exchanged moisture is equal to
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+m&#775;<sub>wat</sub> = u  m&#775;<sub>wat,nom</sub>,
+</p>
+<p>
+where <i>u</i> is the control input signal and
+<i>m&#775;<sub>wat,nom</sub></i> is equal to the parameter <code>mWat_flow_nominal</code>.
+The parameter <code>mWat_flow_nominal</code> can be positive or negative.
+If <i>m&#775;<sub>wat</sub></i> is positive, then moisture is added
+to the air stream, otherwise it is removed.
+</p>
+<p>
+If the heat port <code>heatPort</code> is unconnected, then the enthalpy of the
+air that flows through the device remains unchanged, e.g., the humidification
+is adiabatic. To change the enthalpy of the air, add heat flow to the connector
+<code>heatPort</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed parameters <code>use_T_in</code> and <code>T</code>.
- This removes the optional specification of temperature through the parameter <code>T</code>
- or the input connector <code>T_in</code>.
- Exposed the heat port of the control volume to allow adding heat,
- for example, to use the model as a steam humidifier.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">
- Buildings #704</a>.
- </li>
- <li>
- May 6, 2015, by Michael Wetter:<br/>
- Set <code>prescribedHeatFlowRate=true</code>.
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">
- #412</a>.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- February 11, 2014 by Michael Wetter:<br/>
- Corrected issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/197\">#197</a>
- which led to twice the amount of latent heat being added to the fluid stream.
- </li>
- <li>
- October 14, 2013 by Michael Wetter:<br/>
- Constrained medium to be a subclass of
- <code>Modelica.Media.Interfaces.PartialCondensingGases</code>,
- as this base class declares the function
- <code>enthalpyOfCondensingGas</code>.
- </li>
- <li>
- July 30, 2013 by Michael Wetter:<br/>
- Updated model to use new variable <code>mWat_flow</code>
- in the base class.
- </li>
- <li>
- May 24, 2011, by Michael Wetter:<br/>
- Changed base class to allow using the model as a dynamic or a steady-state model.
- </li>
- <li>
- April 14, 2010, by Michael Wetter:<br/>
- Converted temperature input to a conditional connector.
- </li>
- <li>
- April 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 9, 2023, by Michael Wetter:<br/>
+Removed access to parameter <code>use_T_in</code> which does not exist
+in this model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1697\">#1697</a>.
+</li>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed parameters <code>use_T_in</code> and <code>T</code>.
+This removes the optional specification of temperature through the parameter <code>T</code>
+or the input connector <code>T_in</code>.
+Exposed the heat port of the control volume to allow adding heat,
+for example, to use the model as a steam humidifier.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">
+Buildings #704</a>.
+</li>
+<li>
+May 6, 2015, by Michael Wetter:<br/>
+Set <code>prescribedHeatFlowRate=true</code>.
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">
+#412</a>.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+February 11, 2014 by Michael Wetter:<br/>
+Corrected issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/197\">#197</a>
+which led to twice the amount of latent heat being added to the fluid stream.
+</li>
+<li>
+October 14, 2013 by Michael Wetter:<br/>
+Constrained medium to be a subclass of
+<code>Modelica.Media.Interfaces.PartialCondensingGases</code>,
+as this base class declares the function
+<code>enthalpyOfCondensingGas</code>.
+</li>
+<li>
+July 30, 2013 by Michael Wetter:<br/>
+Updated model to use new variable <code>mWat_flow</code>
+in the base class.
+</li>
+<li>
+May 24, 2011, by Michael Wetter:<br/>
+Changed base class to allow using the model as a dynamic or a steady-state model.
+</li>
+<li>
+April 14, 2010, by Michael Wetter:<br/>
+Converted temperature input to a conditional connector.
+</li>
+<li>
+April 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Humidifier_u;
diff --git a/AixLib/Fluid/Humidifiers/SprayAirWasher_X.mo b/AixLib/Fluid/Humidifiers/SprayAirWasher_X.mo
index aa2d18e99c..a69005072b 100644
--- a/AixLib/Fluid/Humidifiers/SprayAirWasher_X.mo
+++ b/AixLib/Fluid/Humidifiers/SprayAirWasher_X.mo
@@ -116,90 +116,90 @@ equation
           fillPattern=FillPattern.Solid)}),
 defaultComponentName="hum",
 Documentation(info="<html>
- <p>
- Model for a spray air washer with a prescribed outlet water vapor mass fraction
- in kg/kg total air.
- </p>
- <p>
- This model forces the outlet water mass fraction at <code>port_b</code> to be
- no lower than the
- input signal <code>X_wSet</code>, subject to optional limits on the
- maximum water vapor mass flow rate that is added, as
- described by the parameter <code>mWatMax_flow</code>.
- By default, the model has unlimited capacity.
- </p>
- <p>
- The output signal <code>mWat_flow &ge; 0</code> is the moisture added
- to the medium if the flow rate is from <code>port_a</code> to <code>port_b</code>.
- If the flow is reversed, then <code>mWat_flow = 0</code>.
- The outlet specific enthalpy at <code>port_b</code> is increased by
- the enthalpy of liquid water at <i>10</i>&deg;C times the mass of water that was added.
- Therefore, the temperature of the leaving fluid is below the inlet temperature.
- </p>
- <p>
- The outlet conditions at <code>port_a</code> are not affected by this model,
- other than for a possible pressure difference due to flow friction.
- </p>
- <p>
- If the parameter <code>energyDynamics</code> is different from
- <code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
- the component models the dynamic response using a first order differential equation.
- The time constant of the component is equal to the parameter <code>tau</code>.
- This time constant is adjusted based on the mass flow rate using
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
- </p>
- <p>
- where
- <i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
- <i>m&#775;</i> and
- <i>&tau;</i> is the time constant at the nominal mass flow rate
- <i>m&#775;<sub>nom</sub></i>.
- This type of dynamics is equal to the dynamics that a completely mixed
- control volume would have.
- </p>
- <p>
- Optionally, this model can have a flow resistance.
- Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
- </p>
- <p>
- For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
- this with the nominal water mass flow rate, use
- <a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
- AixLib.Fluid.Humidifiers.Humidifier_u</a>
- 
- </p>
- <h4>Limitations</h4>
- <p>
- This model only adds water vapor for the flow from
- <code>port_a</code> to <code>port_b</code>.
- The water vapor of the reverse flow is not affected by this model.
- </p>
- <p>
- This model does not affect the enthalpy of the air. Therefore,
- if water is added, the temperature will decrease, e.g., the humidification
- is adiabatic.
- </p>
- </html>",
+<p>
+Model for a spray air washer with a prescribed outlet water vapor mass fraction
+in kg/kg total air.
+</p>
+<p>
+This model forces the outlet water mass fraction at <code>port_b</code> to be
+no lower than the
+input signal <code>X_wSet</code>, subject to optional limits on the
+maximum water vapor mass flow rate that is added, as
+described by the parameter <code>mWatMax_flow</code>.
+By default, the model has unlimited capacity.
+</p>
+<p>
+The output signal <code>mWat_flow &ge; 0</code> is the moisture added
+to the medium if the flow rate is from <code>port_a</code> to <code>port_b</code>.
+If the flow is reversed, then <code>mWat_flow = 0</code>.
+The outlet specific enthalpy at <code>port_b</code> is increased by
+the enthalpy of liquid water at <i>10</i>&deg;C times the mass of water that was added.
+Therefore, the temperature of the leaving fluid is below the inlet temperature.
+</p>
+<p>
+The outlet conditions at <code>port_a</code> are not affected by this model,
+other than for a possible pressure difference due to flow friction.
+</p>
+<p>
+If the parameter <code>energyDynamics</code> is different from
+<code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
+the component models the dynamic response using a first order differential equation.
+The time constant of the component is equal to the parameter <code>tau</code>.
+This time constant is adjusted based on the mass flow rate using
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
+</p>
+<p>
+where
+<i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
+<i>m&#775;</i> and
+<i>&tau;</i> is the time constant at the nominal mass flow rate
+<i>m&#775;<sub>nom</sub></i>.
+This type of dynamics is equal to the dynamics that a completely mixed
+control volume would have.
+</p>
+<p>
+Optionally, this model can have a flow resistance.
+Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
+</p>
+<p>
+For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
+this with the nominal water mass flow rate, use
+<a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
+AixLib.Fluid.Humidifiers.Humidifier_u</a>
+
+</p>
+<h4>Limitations</h4>
+<p>
+This model only adds water vapor for the flow from
+<code>port_a</code> to <code>port_b</code>.
+The water vapor of the reverse flow is not affected by this model.
+</p>
+<p>
+This model does not affect the enthalpy of the air. Therefore,
+if water is added, the temperature will decrease, e.g., the humidification
+is adiabatic.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 8, 2022, by Michael Wetter:<br/>
- Renamed parameter <code>massDynamics</code> to <code>energyDynamics</code> for consistency with other models.
- </li>
- <li>
- December 14, 2018, by Michael Wetter:<br/>
- Restricted base class for medium to one that implements
- the function <code>enthalpyOfLiquid</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1057\">#1057</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 8, 2022, by Michael Wetter:<br/>
+Renamed parameter <code>massDynamics</code> to <code>energyDynamics</code> for consistency with other models.
+</li>
+<li>
+December 14, 2018, by Michael Wetter:<br/>
+Restricted base class for medium to one that implements
+the function <code>enthalpyOfLiquid</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1057\">#1057</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SprayAirWasher_X;
diff --git a/AixLib/Fluid/Humidifiers/SteamHumidifier_X.mo b/AixLib/Fluid/Humidifiers/SteamHumidifier_X.mo
index f048679bb4..fb0098f64a 100644
--- a/AixLib/Fluid/Humidifiers/SteamHumidifier_X.mo
+++ b/AixLib/Fluid/Humidifiers/SteamHumidifier_X.mo
@@ -192,78 +192,78 @@ equation
           pattern=LinePattern.None)}),
 defaultComponentName="hum",
 Documentation(info="<html>
- <p>
- Model for a steam humidifier with a prescribed outlet water vapor mass fraction
- in kg/kg total air.
- </p>
- <p>
- This model forces the outlet water mass fraction at <code>port_b</code> to be
- no lower than the
- input signal <code>X_wSet</code>, subject to optional limits on the
- maximum water vapor mass flow rate that is added, as
- described by the parameter <code>mWatMax_flow</code>.
- By default, the model has unlimited capacity.
- </p>
- <p>
- The output signal <code>mWat_flow &ge; 0</code> is the moisture added
- to the medium if the flow rate is from <code>port_a</code> to <code>port_b</code>.
- If the flow is reversed, then <code>mWat_flow = 0</code>.
- The outlet specific enthalpy at <code>port_b</code> is increased by
- the enthalpy of steam at <i>100</i>&deg;C times the mass of steam that was added.
- Therefore, the temperature of the leaving fluid is slightly above the inlet temperature.
- </p>
- <p>
- The outlet conditions at <code>port_a</code> are not affected by this model,
- other than for a possible pressure difference due to flow friction.
- </p>
- <p>
- If the parameter <code>energyDynamics</code> is different from
- <code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
- the component models the dynamic response using a first order differential equation.
- The time constant of the component is equal to the parameter <code>tau</code>.
- This time constant is adjusted based on the mass flow rate using
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
- </p>
- <p>
- where
- <i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
- <i>m&#775;</i> and
- <i>&tau;</i> is the time constant at the nominal mass flow rate
- <i>m&#775;<sub>nom</sub></i>.
- This type of dynamics is equal to the dynamics that a completely mixed
- control volume would have.
- </p>
- <p>
- Optionally, this model can have a flow resistance.
- Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
- </p>
- <p>
- For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
- this with the nominal water mass flow rate, use
- <a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
- AixLib.Fluid.Humidifiers.Humidifier_u</a>
- 
- </p>
- <h4>Limitations</h4>
- <p>
- This model only adds water vapor for the flow from
- <code>port_a</code> to <code>port_b</code>.
- The water vapor of the reverse flow is not affected by this model.
- </p>
- </html>",
+<p>
+Model for a steam humidifier with a prescribed outlet water vapor mass fraction
+in kg/kg total air.
+</p>
+<p>
+This model forces the outlet water mass fraction at <code>port_b</code> to be
+no lower than the
+input signal <code>X_wSet</code>, subject to optional limits on the
+maximum water vapor mass flow rate that is added, as
+described by the parameter <code>mWatMax_flow</code>.
+By default, the model has unlimited capacity.
+</p>
+<p>
+The output signal <code>mWat_flow &ge; 0</code> is the moisture added
+to the medium if the flow rate is from <code>port_a</code> to <code>port_b</code>.
+If the flow is reversed, then <code>mWat_flow = 0</code>.
+The outlet specific enthalpy at <code>port_b</code> is increased by
+the enthalpy of steam at <i>100</i>&deg;C times the mass of steam that was added.
+Therefore, the temperature of the leaving fluid is slightly above the inlet temperature.
+</p>
+<p>
+The outlet conditions at <code>port_a</code> are not affected by this model,
+other than for a possible pressure difference due to flow friction.
+</p>
+<p>
+If the parameter <code>energyDynamics</code> is different from
+<code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
+the component models the dynamic response using a first order differential equation.
+The time constant of the component is equal to the parameter <code>tau</code>.
+This time constant is adjusted based on the mass flow rate using
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
+</p>
+<p>
+where
+<i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
+<i>m&#775;</i> and
+<i>&tau;</i> is the time constant at the nominal mass flow rate
+<i>m&#775;<sub>nom</sub></i>.
+This type of dynamics is equal to the dynamics that a completely mixed
+control volume would have.
+</p>
+<p>
+Optionally, this model can have a flow resistance.
+Set <code>dp_nominal = 0</code> to disable the flow friction calculation.
+</p>
+<p>
+For a model that uses a control signal <i>u &isin; [0, 1]</i> and multiplies
+this with the nominal water mass flow rate, use
+<a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
+AixLib.Fluid.Humidifiers.Humidifier_u</a>
+
+</p>
+<h4>Limitations</h4>
+<p>
+This model only adds water vapor for the flow from
+<code>port_a</code> to <code>port_b</code>.
+The water vapor of the reverse flow is not affected by this model.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 8, 2022, by Michael Wetter:<br/>
- Renamed parameter <code>massDynamics</code> to <code>energyDynamics</code> for consistency with other models.
- </li>
- <li>
- May 10, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 8, 2022, by Michael Wetter:<br/>
+Renamed parameter <code>massDynamics</code> to <code>energyDynamics</code> for consistency with other models.
+</li>
+<li>
+May 10, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SteamHumidifier_X;
diff --git a/AixLib/Fluid/Humidifiers/Validation/SprayAirWasher_X.mo b/AixLib/Fluid/Humidifiers/Validation/SprayAirWasher_X.mo
index 0e90f551af..69c6cb21e6 100644
--- a/AixLib/Fluid/Humidifiers/Validation/SprayAirWasher_X.mo
+++ b/AixLib/Fluid/Humidifiers/Validation/SprayAirWasher_X.mo
@@ -71,28 +71,28 @@ equation
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Humidifiers/Validation/SprayAirWasher_X.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that validates the use of a spray air washer
- configured as a steady-state model with limits on the maximum water mass flow rate
- that is added to the air stream.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 29, 2021, by Michael Wetter:<br/>
- Reformulated constraint of replaceable model to avoid access of
- component that is not in constraining type.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1473\">IBPSA, #1473</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that validates the use of a spray air washer
+configured as a steady-state model with limits on the maximum water mass flow rate
+that is added to the air stream.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 29, 2021, by Michael Wetter:<br/>
+Reformulated constraint of replaceable model to avoid access of
+component that is not in constraining type.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1473\">IBPSA, #1473</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=1080,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SprayAirWasher_X;
diff --git a/AixLib/Fluid/Humidifiers/Validation/SprayAirWasher_X_dynamic.mo b/AixLib/Fluid/Humidifiers/Validation/SprayAirWasher_X_dynamic.mo
index 7e3a52a1d5..d582fe47af 100644
--- a/AixLib/Fluid/Humidifiers/Validation/SprayAirWasher_X_dynamic.mo
+++ b/AixLib/Fluid/Humidifiers/Validation/SprayAirWasher_X_dynamic.mo
@@ -10,21 +10,21 @@ annotation (
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Humidifiers/Validation/SprayAirWasher_X_dynamic.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that validates the use of a spray air washer
- configured as a dynamic model with limits on the maximum water mass flow rate
- that is added to the air stream.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that validates the use of a spray air washer
+configured as a dynamic model with limits on the maximum water mass flow rate
+that is added to the air stream.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=1080,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SprayAirWasher_X_dynamic;
diff --git a/AixLib/Fluid/Humidifiers/Validation/SteamHumidifier_X.mo b/AixLib/Fluid/Humidifiers/Validation/SteamHumidifier_X.mo
index f9672d5cfc..49affd9ede 100644
--- a/AixLib/Fluid/Humidifiers/Validation/SteamHumidifier_X.mo
+++ b/AixLib/Fluid/Humidifiers/Validation/SteamHumidifier_X.mo
@@ -9,26 +9,26 @@ annotation (
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Humidifiers/Validation/SteamHumidifier_X.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that validates the use of a spray air washer
- configured as a steady-state model with limits on the maximum water mass flow rate
- that is added to the air stream.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 3, 2017, by Michael Wetter:<br/>
- Removed <code>import</code> statement.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/852\">#852</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that validates the use of a spray air washer
+configured as a steady-state model with limits on the maximum water mass flow rate
+that is added to the air stream.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 3, 2017, by Michael Wetter:<br/>
+Removed <code>import</code> statement.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/852\">#852</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=1080,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SteamHumidifier_X;
diff --git a/AixLib/Fluid/Humidifiers/Validation/SteamHumidifier_X_dynamic.mo b/AixLib/Fluid/Humidifiers/Validation/SteamHumidifier_X_dynamic.mo
index 2b5ca991f2..4200db54fe 100644
--- a/AixLib/Fluid/Humidifiers/Validation/SteamHumidifier_X_dynamic.mo
+++ b/AixLib/Fluid/Humidifiers/Validation/SteamHumidifier_X_dynamic.mo
@@ -10,21 +10,21 @@ annotation (
     __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Humidifiers/Validation/SteamHumidifier_X_dynamic.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that validates the use of a spray air washer
- configured as a dynamic model with limits on the maximum water mass flow rate
- that is added to the air stream.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Model that validates the use of a spray air washer
+configured as a dynamic model with limits on the maximum water mass flow rate
+that is added to the air stream.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=1080,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SteamHumidifier_X_dynamic;
diff --git a/AixLib/Fluid/Interfaces/ConservationEquation.mo b/AixLib/Fluid/Interfaces/ConservationEquation.mo
index 0a17baf0af..0612232521 100644
--- a/AixLib/Fluid/Interfaces/ConservationEquation.mo
+++ b/AixLib/Fluid/Interfaces/ConservationEquation.mo
@@ -35,7 +35,8 @@ model ConservationEquation "Lumped volume with mass and energy balance"
 
   // Outputs that are needed in models that use this model
   Modelica.Blocks.Interfaces.RealOutput hOut(unit="J/kg",
-                                             start=hStart)
+                                             start=hStart,
+                                             nominal=Medium.h_default)
     "Leaving specific enthalpy of the component"
      annotation (Placement(transformation(extent={{-10,-10},{10,10}},
         rotation=90,
@@ -56,8 +57,8 @@ model ConservationEquation "Lumped volume with mass and energy balance"
     "Internal energy of the component" annotation (Placement(transformation(
         extent={{-10,-10},{10,10}},
         origin={110,20})));
-  Modelica.Blocks.Interfaces.RealOutput mXiOut[Medium.nXi](each min=0, each unit=
-       "kg") "Species mass of the component"
+  Modelica.Blocks.Interfaces.RealOutput mXiOut[Medium.nXi](each min=0, each unit="kg")
+    "Species mass of the component"
     annotation (Placement(transformation(extent={{-10,-10},{10,10}},
         origin={110,-20})));
   Modelica.Blocks.Interfaces.RealOutput mOut(min=0, unit="kg")
@@ -70,7 +71,9 @@ model ConservationEquation "Lumped volume with mass and energy balance"
         origin={110,-60})));
 
   Modelica.Fluid.Vessels.BaseClasses.VesselFluidPorts_b ports[nPorts](
-      redeclare each final package Medium = Medium) "Fluid inlets and outlets"
+      redeclare each final package Medium = Medium,
+      each h_outflow(nominal=Medium.h_default),
+      each Xi_outflow(each nominal=0.01)) "Fluid inlets and outlets"
     annotation (Placement(transformation(extent={{-40,-10},{40,10}},
       origin={0,-100})));
 
@@ -79,11 +82,14 @@ model ConservationEquation "Lumped volume with mass and energy balance"
     p(start=p_start),
     h(start=hStart),
     T(start=T_start),
-    Xi(start=X_start[1:Medium.nXi]),
+    Xi(
+      each stateSelect=if medium.preferredMediumStates then StateSelect.prefer else StateSelect.default,
+      start=X_start[1:Medium.nXi]),
     X(start=X_start),
     d(start=rho_start)) "Medium properties";
 
-  Modelica.Units.SI.Energy U(start=fluidVolume*rho_start*
+  Modelica.Units.SI.Energy U(
+    start=fluidVolume*rho_start*
         Medium.specificInternalEnergy(Medium.setState_pTX(
         T=T_start,
         p=p_start,
@@ -94,8 +100,10 @@ model ConservationEquation "Lumped volume with mass and energy balance"
         massDynamics == Modelica.Fluid.Types.Dynamics.SteadyState then
         StateSelect.default else StateSelect.prefer) "Mass of fluid";
 
-  Modelica.Units.SI.Mass[Medium.nXi] mXi(start=fluidVolume*rho_start*X_start[1:
-        Medium.nXi]) "Masses of independent components in the fluid";
+  Modelica.Units.SI.Mass[Medium.nXi] mXi(
+    each stateSelect=StateSelect.never,
+    start=fluidVolume*rho_start*X_start[1:Medium.nXi])
+    "Masses of independent components in the fluid";
   Modelica.Units.SI.Mass[Medium.nC] mC(start=fluidVolume*rho_start*C_start)
     "Masses of trace substances in the fluid";
   // C need to be added here because unlike for Xi, which has medium.Xi,
@@ -165,21 +173,23 @@ protected
 
 initial equation
   // Assert that the substance with name 'water' has been found.
-  assert(Medium.nXi == 0 or abs(sum(s)-1) < 1e-5,
-      "In " + getInstanceName() + ":
-          If Medium.nXi > 1, then substance 'water' must be present for one component of '"
-         + Medium.mediumName + "'.
-          Check medium model.");
+  if use_mWat_flow then
+    assert(Medium.nXi == 0 or abs(sum(s) - 1) < 1e-5, "In " + getInstanceName()
+       + ":
+         If Medium.nXi > 1, then substance 'water' must be present for one component of '"
+       + Medium.mediumName + "'.
+         Check medium model.");
+  end if;
 
   // Make sure that if energyDynamics is SteadyState, then
   // massDynamics is also SteadyState.
   // Otherwise, the system of ordinary differential equations may be inconsistent.
   if energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState then
     assert(massDynamics == energyDynamics, "In " + getInstanceName() + ":
-          If 'massDynamics == Modelica.Fluid.Types.Dynamics.SteadyState', then it is
-          required that 'energyDynamics==Modelica.Fluid.Types.Dynamics.SteadyState'.
-          Otherwise, the system of equations may not be consistent.
-          You need to select other parameter values.");
+         If 'massDynamics == Modelica.Fluid.Types.Dynamics.SteadyState', then it is
+         required that 'energyDynamics==Modelica.Fluid.Types.Dynamics.SteadyState'.
+         Otherwise, the system of equations may not be consistent.
+         You need to select other parameter values.");
   end if;
 
   // initialization of balances
@@ -302,7 +312,7 @@ equation
   if substanceDynamics == Modelica.Fluid.Types.Dynamics.SteadyState then
     zeros(Medium.nXi) = mbXi_flow + mWat_flow_internal * s;
   else
-    der(mXi) = mbXi_flow + mWat_flow_internal * s;
+    der(medium.Xi) = (mbXi_flow + mWat_flow_internal * s)/m;
   end if;
 
   if traceDynamics == Modelica.Fluid.Types.Dynamics.SteadyState then
@@ -324,374 +334,393 @@ equation
   mCOut=mC;
   annotation (
     Documentation(info="<html>
- <p>
- Basic model for an ideally mixed fluid volume with the ability to store mass and energy.
- It implements a dynamic or a steady-state conservation equation for energy and mass fractions.
- The model has zero pressure drop between its ports.
- </p>
- <p>
- If the constant <code>simplify_mWat_flow = true</code> then adding
- moisture does not increase the mass of the volume or the leaving mass flow rate.
- It does however change the mass fraction <code>medium.Xi</code>.
- This allows to decouple the moisture balance from the pressure drop equations.
- If <code>simplify_mWat_flow = false</code>, then
- the outlet mass flow rate is
- <i>m<sub>out</sub> = m<sub>in</sub>  (1 + &Delta; X<sub>w</sub>)</i>,
- where
- <i>&Delta; X<sub>w</sub></i> is the change in water vapor mass
- fraction across the component. In this case,
- this component couples
- the energy calculation to the
- pressure drop versus mass flow rate calculations.
- However, in typical building HVAC systems,
- <i>&Delta; X<sub>w</sub></i> &lt; <i>0.005</i> kg/kg.
- Hence, by tolerating a relative error of <i>0.005</i> in the mass balance,
- one can decouple these equations.
- Decoupling these equations avoids having
- to compute the energy balance of the humidifier
- and its upstream components when solving for the
- pressure drop of downstream components.
- Therefore, the default value is <code>simplify_mWat_flow = true</code>.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- Set the parameter <code>use_mWat_flow_in=true</code> to enable an
- input connector for <code>mWat_flow</code>.
- Otherwise, the model uses <code>mWat_flow = 0</code>.
- </p>
- <p>
- If the constant <code>simplify_mWat_flow = true</code>, which is its default value,
- then the equation
- </p>
- <pre>
-   port_a.m_flow + port_b.m_flow = - mWat_flow;
- </pre>
- <p>
- is simplified as
- </p>
- <pre>
-   port_a.m_flow + port_b.m_flow = 0;
- </pre>
- <p>
- This causes an error in the mass balance of about <i>0.5%</i>, but generally leads to
- simpler equations because the pressure drop equations are then decoupled from the
- mass exchange in this component.
- The model
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeAdiabaticCooling\">
- AixLib.Fluid.MixingVolumes.Validation.MixingVolumeAdiabaticCooling</a>
- shows that the relative error on the temperature difference between these
- two options of <code>simplify_mWat_flow</code> is less than
- <i>0.1%</i>.
- </p>
- 
- <h4>Implementation</h4>
- <p>
- When extending or instantiating this model, the input
- <code>fluidVolume</code>, which is the actual volume occupied by the fluid,
- needs to be assigned.
- For most components, this can be set to a parameter.
- </p>
- Input connectors of the model are
- <ul>
- <li>
- <code>Q_flow</code>, which is the sensible plus latent heat flow rate added to the medium,
- </li>
- <li>
- <code>mWat_flow</code>, which is the moisture mass flow rate added to the medium, and
- </li>
- <li>
- <code>C_flow</code>, which is the trace substance mass flow rate added to the medium.
- </li>
- </ul>
- 
- <p>
- The model can be used as a dynamic model or as a steady-state model.
- However, for a steady-state model with exactly two fluid ports connected,
- the model
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- provides a more efficient implementation.
- </p>
- <p>
- For a model that instantiates this model, see
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
- AixLib.Fluid.MixingVolumes.MixingVolume</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 26, 2019, by Filip Jorissen:<br/>
- Returning <code>getInstanceName()</code> in asserts.
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1133\">1133</a>.
- </li>
- <li>
- April 16, 2019, by Michael Wetter:<br/>
- Changed computation of <code>computeCSen</code> to avoid the volume to become
- a structural parameter.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1122\">IBPSA, issue 1122</a>.
- </li>
- <li>
- April 16, 2018, by Michael Wetter:<br/>
- Reformulated mass calculation so that Dymola can differentiate the equations.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
- </li>
- <li>
- November 3, 2017, by Michael Wetter:<br/>
- Set <code>start</code> attributes.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/727\">727</a>.
- </li>
- <li>
- October 19, 2017, by Michael Wetter:<br/>
- Changed initialization of pressure from a <code>constant</code> to a <code>parameter</code>.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- <li>
- January 27, 2017, by Michael Wetter:<br/>
- Added <code>stateSelect</code> for mass <code>m</code>.<br/>
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/642\">
- Buildings, #642</a>.
- </li>
- <li>
- December 22, 2016, by Michael Wetter:<br/>
- Set nominal value for <code>U</code>.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/637\">637</a>.
- </li>
- <li>
- February 19, 2016 by Filip Jorissen:<br/>
- Added outputs UOut, mOut, mXiOut, mCOut for being able to
- check conservation of quantities.
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">
- issue 247</a>.
- </li>
- <li>
- January 17, 2016, by Michael Wetter:<br/>
- Added parameter <code>use_C_flow</code> and converted <code>C_flow</code>
- to a conditionally removed connector.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- December 16, 2015, by Michael Wetter:<br/>
- Added <code>C_flow</code> to the steady-state trace substance balance,
- and removed the units of <code>C_flow</code> to allow for PPM.
- </li>
- <li>
- December 2, 2015, by Filip Jorissen:<br/>
- Added input <code>C_flow</code> and code for handling trace substance insertions.
- </li>
- <li>
- September 3, 2015, by Filip Jorissen and Michael Wetter:<br/>
- Revised implementation for allowing moisture mass flow rate
- to be approximated using parameter <code>simplify_mWat_flow</code>.
- This may lead to smaller algebraic loops.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">#247</a>.
- </li>
- <li>
- July 17, 2015, by Michael Wetter:<br/>
- Added constant <code>simplify_mWat_flow</code> to remove dependencies of the pressure drop
- calculation on the moisture balance.
- </li>
- <li>
- June 5, 2015 by Michael Wetter:<br/>
- Removed <code>preferredMediumStates= false</code> in
- the instance <code>medium</code> as the default
- is already <code>false</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/260\">#260</a>.
- </li>
- <li>
- June 5, 2015 by Filip Jorissen:<br/>
- Removed <pre>
- Xi(start=X_start[1:Medium.nXi],
-        each stateSelect=if (not (substanceDynamics == Modelica.Fluid.Types.Dynamics.SteadyState))
-        then StateSelect.prefer else StateSelect.default),
- </pre>
- and set
- <code>preferredMediumStates = false</code>
- because the previous declaration led to more equations and
- translation problems in large models.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/260\">#260</a>.
- </li>
- <li>
- June 5, 2015, by Michael Wetter:<br/>
- Moved assignment of <code>dynBal.U.start</code>
- from instance <code>dynBal</code> of <code>PartialMixingVolume</code>
- to this model implementation.
- This is required for a pedantic model check in Dymola 2016.
- It addresses
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">
- issue 266</a>.
- This revison also renames the protected variable
- <code>rho_nominal</code> to <code>rho_start</code>
- as it depends on the start values and not the nominal values.
- </li>
- <li>
- May 22, 2015 by Michael Wetter:<br/>
- Removed <pre>
- p(stateSelect=if not (massDynamics == Modelica.Fluid.Types.Dynamics.SteadyState)
- then StateSelect.prefer else StateSelect.default)
- </pre>
- because the previous declaration led to the translation error
- <pre>
- The model requires derivatives of some inputs as listed below:
- 1 inlet.m_flow
- 1 inlet.p
- </pre>
- when translating
- <code>Buildings.Fluid.FMI.ExportContainers.Examples.FMUs.HeaterCooler_u</code>
- with a dynamic energy balance.
- </li>
- <li>
- May 6, 2015, by Michael Wetter:<br/>
- Corrected documentation.
- </li>
- <li>
- April 13, 2015, by Filip Jorissen:<br/>
- Now using <code>semiLinear()</code> function for calculation of
- <code>ports_H_flow</code>. This enables Dymola to simplify based on
- the <code>min</code> and <code>max</code> attribute of the mass flow rate.
- </li>
- <li>
- February 16, 2015, by Filip Jorissen:<br/>
- Fixed SteadyState massDynamics implementation for compressible media.
- Mass <code>m</code> is now constant.
- </li>
- <li>
- February 5, 2015, by Michael Wetter:<br/>
- Changed <code>initalize_p</code> from a <code>parameter</code> to a
- <code>constant</code>. This is only required in finite volume models
- of heat exchangers (to avoid consistent but redundant initial conditions)
- and hence it should be set as a <code>constant</code>.
- </li>
- <li>
- February 3, 2015, by Michael Wetter:<br/>
- Removed <code>stateSelect.prefer</code> for temperature.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/160\">#160</a>.
- </li>
- <li>
- October 21, 2014, by Filip Jorissen:<br/>
- Added parameter <code>mFactor</code> to increase the thermal capacity.
- </li>
- <li>
- October 6, 2014, by Michael Wetter:<br/>
- Changed medium declaration in ports to be final.
- </li>
- <li>
- October 6, 2014, by Michael Wetter:<br/>
- Set start attributes in <code>medium</code> to avoid in OpenModelica the warning
- alias set with several free start values.
- </li>
- <li>
- October 3, 2014, by Michael Wetter:<br/>
- Changed assignment of nominal value to avoid in OpenModelica the warning
- alias set with different nominal values.
- </li>
- <li>
- July 3, 2014, by Michael Wetter:<br/>
- Added parameter <code>initialize_p</code>. This is required
- to enable the coil models to initialize the pressure in the first
- volume, but not in the downstream volumes. Otherwise,
- the initial equations will be overdetermined, but consistent.
- This change was done to avoid a long information message that appears
- when translating models.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- February 11, 2014 by Michael Wetter:<br/>
- Improved documentation for <code>Q_flow</code> input.
- </li>
- <li>
- September 17, 2013 by Michael Wetter:<br/>
- Added start value for <code>hOut</code>.
- </li>
- <li>
- September 10, 2013 by Michael Wetter:<br/>
- Removed unrequired parameter <code>i_w</code>.<br/>
- Corrected the syntax error
- <code>Medium.ExtraProperty C[Medium.nC](each nominal=C_nominal)</code>
- to
- <code>Medium.ExtraProperty C[Medium.nC](nominal=C_nominal)</code>
- because <code>C_nominal</code> is a vector.
- This syntax error caused a compilation error in OpenModelica.
- </li>
- <li>
- July 30, 2013 by Michael Wetter:<br/>
- Changed connector <code>mXi_flow[Medium.nXi]</code>
- to a scalar input connector <code>mWat_flow</code>.
- The reason is that <code>mXi_flow</code> does not allow
- to compute the other components in <code>mX_flow</code> and
- therefore leads to an ambiguous use of the model.
- By only requesting <code>mWat_flow</code>, the mass balance
- and species balance can be implemented correctly.
- </li>
- <li>
- March 27, 2013 by Michael Wetter:<br/>
- Removed wrong unit attribute of <code>COut</code>,
- and added min and max attributes for <code>XiOut</code>.
- </li>
- <li>
- July 31, 2011 by Michael Wetter:<br/>
- Added test to stop model translation if the setting for
- <code>energyBalance</code> and <code>massBalance</code>
- can lead to inconsistent equations.
- </li>
- <li>
- July 26, 2011 by Michael Wetter:<br/>
- Removed the option to use <code>h_start</code>, as this
- is not needed for building simulation.
- Also removed the reference to <code>Modelica.Fluid.System</code>.
- Moved parameters and medium to
- <a href=\"AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
- AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
- </li>
- <li>
- July 14, 2011 by Michael Wetter:<br/>
- Added start value for medium density.
- </li>
- <li>
- March 29, 2011 by Michael Wetter:<br/>
- Changed default value for <code>substanceDynamics</code> and
- <code>traceDynamics</code> from <code>energyDynamics</code>
- to <code>massDynamics</code>.
- </li>
- <li>
- September 28, 2010 by Michael Wetter:<br/>
- Changed array index for nominal value of <code>Xi</code>.
- </li>
- <li>
- September 13, 2010 by Michael Wetter:<br/>
- Set nominal attributes for medium based on default medium values.
- </li>
- <li>
- July 30, 2010 by Michael Wetter:<br/>
- Added parameter <code>C_nominal</code> which is used as the nominal attribute for <code>C</code>.
- Without this value, the ODE solver gives wrong results for concentrations around 1E-7.
- </li>
- <li>
- March 21, 2010 by Michael Wetter:<br/>
- Changed pressure start value from <code>system.p_start</code>
- to <code>Medium.p_default</code> since HVAC models may have water and
- air, which are typically at different pressures.
- </li>
- <li><i>February 6, 2010</i> by Michael Wetter:<br/>
- Added to <code>Medium.BaseProperties</code> the initialization
- <code>X(start=X_start[1:Medium.nX])</code>. Previously, the initialization
- was only done for <code>Xi</code> but not for <code>X</code>, which caused the
- medium to be initialized to <code>reference_X</code>, ignoring the value of <code>X_start</code>.
- </li>
- <li><i>October 12, 2009</i> by Michael Wetter:<br/>
- Implemented first version in <code>Buildings</code> library, based on model from
- <code>Modelica.Fluid 1.0</code>.
- </li>
- </ul>
- </html>"),
+<p>
+Basic model for an ideally mixed fluid volume with the ability to store mass and energy.
+It implements a dynamic or a steady-state conservation equation for energy and mass fractions.
+The model has zero pressure drop between its ports.
+</p>
+<p>
+If the constant <code>simplify_mWat_flow = true</code> then adding
+moisture does not increase the mass of the volume or the leaving mass flow rate.
+It does however change the mass fraction <code>medium.Xi</code>.
+This allows to decouple the moisture balance from the pressure drop equations.
+If <code>simplify_mWat_flow = false</code>, then
+the outlet mass flow rate is
+<i>m<sub>out</sub> = m<sub>in</sub>  (1 + &Delta; X<sub>w</sub>)</i>,
+where
+<i>&Delta; X<sub>w</sub></i> is the change in water vapor mass
+fraction across the component. In this case,
+this component couples
+the energy calculation to the
+pressure drop versus mass flow rate calculations.
+However, in typical building HVAC systems,
+<i>&Delta; X<sub>w</sub></i> &lt; <i>0.005</i> kg/kg.
+Hence, by tolerating a relative error of <i>0.005</i> in the mass balance,
+one can decouple these equations.
+Decoupling these equations avoids having
+to compute the energy balance of the humidifier
+and its upstream components when solving for the
+pressure drop of downstream components.
+Therefore, the default value is <code>simplify_mWat_flow = true</code>.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+Set the parameter <code>use_mWat_flow_in=true</code> to enable an
+input connector for <code>mWat_flow</code>.
+Otherwise, the model uses <code>mWat_flow = 0</code>.
+</p>
+<p>
+If the constant <code>simplify_mWat_flow = true</code>, which is its default value,
+then the equation
+</p>
+<pre>
+  port_a.m_flow + port_b.m_flow = - mWat_flow;
+</pre>
+<p>
+is simplified as
+</p>
+<pre>
+  port_a.m_flow + port_b.m_flow = 0;
+</pre>
+<p>
+This causes an error in the mass balance of about <i>0.5%</i>, but generally leads to
+simpler equations because the pressure drop equations are then decoupled from the
+mass exchange in this component.
+The model
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeAdiabaticCooling\">
+AixLib.Fluid.MixingVolumes.Validation.MixingVolumeAdiabaticCooling</a>
+shows that the relative error on the temperature difference between these
+two options of <code>simplify_mWat_flow</code> is less than
+<i>0.1%</i>.
+</p>
+
+<h4>Implementation</h4>
+<p>
+When extending or instantiating this model, the input
+<code>fluidVolume</code>, which is the actual volume occupied by the fluid,
+needs to be assigned.
+For most components, this can be set to a parameter.
+</p>
+Input connectors of the model are
+<ul>
+<li>
+<code>Q_flow</code>, which is the sensible plus latent heat flow rate added to the medium,
+</li>
+<li>
+<code>mWat_flow</code>, which is the moisture mass flow rate added to the medium, and
+</li>
+<li>
+<code>C_flow</code>, which is the trace substance mass flow rate added to the medium.
+</li>
+</ul>
+
+<p>
+The model can be used as a dynamic model or as a steady-state model.
+However, for a steady-state model with exactly two fluid ports connected,
+the model
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+provides a more efficient implementation.
+</p>
+<p>
+For a model that instantiates this model, see
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
+AixLib.Fluid.MixingVolumes.MixingVolume</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+October 24, 2022, by Michael Wetter:<br/>
+Conditionally removed assertion that checks for water content as this is
+only required if water is added to the medium.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1650\">#1650</a>.
+</li>
+<li>
+September 9, 2022, by Michael Wetter:<br/>
+Changed state variable from <code>mXi</code> to <code>medium.Xi</code>
+as this allows setting a good nominal attribute without having to use the fluid volume,
+which is non-literal value that leads to a warning in Dymola.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1634\">1634</a>.
+</li>
+<li>
+April 26, 2019, by Filip Jorissen:<br/>
+Returning <code>getInstanceName()</code> in asserts.
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1133\">1133</a>.
+</li>
+<li>
+April 16, 2019, by Michael Wetter:<br/>
+Changed computation of <code>computeCSen</code> to avoid the volume to become
+a structural parameter.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1122\">IBPSA, issue 1122</a>.
+</li>
+<li>
+April 16, 2018, by Michael Wetter:<br/>
+Reformulated mass calculation so that Dymola can differentiate the equations.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
+</li>
+<li>
+November 3, 2017, by Michael Wetter:<br/>
+Set <code>start</code> attributes.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/727\">727</a>.
+</li>
+<li>
+October 19, 2017, by Michael Wetter:<br/>
+Changed initialization of pressure from a <code>constant</code> to a <code>parameter</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+<li>
+January 27, 2017, by Michael Wetter:<br/>
+Added <code>stateSelect</code> for mass <code>m</code>.<br/>
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/642\">
+Buildings, #642</a>.
+</li>
+<li>
+December 22, 2016, by Michael Wetter:<br/>
+Set nominal value for <code>U</code>.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/637\">637</a>.
+</li>
+<li>
+February 19, 2016 by Filip Jorissen:<br/>
+Added outputs UOut, mOut, mXiOut, mCOut for being able to
+check conservation of quantities.
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">
+issue 247</a>.
+</li>
+<li>
+January 17, 2016, by Michael Wetter:<br/>
+Added parameter <code>use_C_flow</code> and converted <code>C_flow</code>
+to a conditionally removed connector.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+December 16, 2015, by Michael Wetter:<br/>
+Added <code>C_flow</code> to the steady-state trace substance balance,
+and removed the units of <code>C_flow</code> to allow for PPM.
+</li>
+<li>
+December 2, 2015, by Filip Jorissen:<br/>
+Added input <code>C_flow</code> and code for handling trace substance insertions.
+</li>
+<li>
+September 3, 2015, by Filip Jorissen and Michael Wetter:<br/>
+Revised implementation for allowing moisture mass flow rate
+to be approximated using parameter <code>simplify_mWat_flow</code>.
+This may lead to smaller algebraic loops.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">#247</a>.
+</li>
+<li>
+July 17, 2015, by Michael Wetter:<br/>
+Added constant <code>simplify_mWat_flow</code> to remove dependencies of the pressure drop
+calculation on the moisture balance.
+</li>
+<li>
+June 5, 2015 by Michael Wetter:<br/>
+Removed <code>preferredMediumStates= false</code> in
+the instance <code>medium</code> as the default
+is already <code>false</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/260\">#260</a>.
+</li>
+<li>
+June 5, 2015 by Filip Jorissen:<br/>
+Removed <pre>
+Xi(start=X_start[1:Medium.nXi],
+       each stateSelect=if (not (substanceDynamics == Modelica.Fluid.Types.Dynamics.SteadyState))
+       then StateSelect.prefer else StateSelect.default),
+</pre>
+and set
+<code>preferredMediumStates = false</code>
+because the previous declaration led to more equations and
+translation problems in large models.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/260\">#260</a>.
+</li>
+<li>
+June 5, 2015, by Michael Wetter:<br/>
+Moved assignment of <code>dynBal.U.start</code>
+from instance <code>dynBal</code> of <code>PartialMixingVolume</code>
+to this model implementation.
+This is required for a pedantic model check in Dymola 2016.
+It addresses
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">
+issue 266</a>.
+This revison also renames the protected variable
+<code>rho_nominal</code> to <code>rho_start</code>
+as it depends on the start values and not the nominal values.
+</li>
+<li>
+May 22, 2015 by Michael Wetter:<br/>
+Removed <pre>
+p(stateSelect=if not (massDynamics == Modelica.Fluid.Types.Dynamics.SteadyState)
+then StateSelect.prefer else StateSelect.default)
+</pre>
+because the previous declaration led to the translation error
+<pre>
+The model requires derivatives of some inputs as listed below:
+1 inlet.m_flow
+1 inlet.p
+</pre>
+when translating
+<code>AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.HeaterCooler_u</code>
+with a dynamic energy balance.
+</li>
+<li>
+May 6, 2015, by Michael Wetter:<br/>
+Corrected documentation.
+</li>
+<li>
+April 13, 2015, by Filip Jorissen:<br/>
+Now using <code>semiLinear()</code> function for calculation of
+<code>ports_H_flow</code>. This enables Dymola to simplify based on
+the <code>min</code> and <code>max</code> attribute of the mass flow rate.
+</li>
+<li>
+February 16, 2015, by Filip Jorissen:<br/>
+Fixed SteadyState massDynamics implementation for compressible media.
+Mass <code>m</code> is now constant.
+</li>
+<li>
+February 5, 2015, by Michael Wetter:<br/>
+Changed <code>initalize_p</code> from a <code>parameter</code> to a
+<code>constant</code>. This is only required in finite volume models
+of heat exchangers (to avoid consistent but redundant initial conditions)
+and hence it should be set as a <code>constant</code>.
+</li>
+<li>
+February 3, 2015, by Michael Wetter:<br/>
+Removed <code>stateSelect.prefer</code> for temperature.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/160\">#160</a>.
+</li>
+<li>
+October 21, 2014, by Filip Jorissen:<br/>
+Added parameter <code>mFactor</code> to increase the thermal capacity.
+</li>
+<li>
+October 6, 2014, by Michael Wetter:<br/>
+Changed medium declaration in ports to be final.
+</li>
+<li>
+October 6, 2014, by Michael Wetter:<br/>
+Set start attributes in <code>medium</code> to avoid in OpenModelica the warning
+alias set with several free start values.
+</li>
+<li>
+October 3, 2014, by Michael Wetter:<br/>
+Changed assignment of nominal value to avoid in OpenModelica the warning
+alias set with different nominal values.
+</li>
+<li>
+July 3, 2014, by Michael Wetter:<br/>
+Added parameter <code>initialize_p</code>. This is required
+to enable the coil models to initialize the pressure in the first
+volume, but not in the downstream volumes. Otherwise,
+the initial equations will be overdetermined, but consistent.
+This change was done to avoid a long information message that appears
+when translating models.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+February 11, 2014 by Michael Wetter:<br/>
+Improved documentation for <code>Q_flow</code> input.
+</li>
+<li>
+September 17, 2013 by Michael Wetter:<br/>
+Added start value for <code>hOut</code>.
+</li>
+<li>
+September 10, 2013 by Michael Wetter:<br/>
+Removed unrequired parameter <code>i_w</code>.<br/>
+Corrected the syntax error
+<code>Medium.ExtraProperty C[Medium.nC](each nominal=C_nominal)</code>
+to
+<code>Medium.ExtraProperty C[Medium.nC](nominal=C_nominal)</code>
+because <code>C_nominal</code> is a vector.
+This syntax error caused a compilation error in OpenModelica.
+</li>
+<li>
+July 30, 2013 by Michael Wetter:<br/>
+Changed connector <code>mXi_flow[Medium.nXi]</code>
+to a scalar input connector <code>mWat_flow</code>.
+The reason is that <code>mXi_flow</code> does not allow
+to compute the other components in <code>mX_flow</code> and
+therefore leads to an ambiguous use of the model.
+By only requesting <code>mWat_flow</code>, the mass balance
+and species balance can be implemented correctly.
+</li>
+<li>
+March 27, 2013 by Michael Wetter:<br/>
+Removed wrong unit attribute of <code>COut</code>,
+and added min and max attributes for <code>XiOut</code>.
+</li>
+<li>
+July 31, 2011 by Michael Wetter:<br/>
+Added test to stop model translation if the setting for
+<code>energyBalance</code> and <code>massBalance</code>
+can lead to inconsistent equations.
+</li>
+<li>
+July 26, 2011 by Michael Wetter:<br/>
+Removed the option to use <code>h_start</code>, as this
+is not needed for building simulation.
+Also removed the reference to <code>Modelica.Fluid.System</code>.
+Moved parameters and medium to
+<a href=\"modelica://AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
+AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
+</li>
+<li>
+July 14, 2011 by Michael Wetter:<br/>
+Added start value for medium density.
+</li>
+<li>
+March 29, 2011 by Michael Wetter:<br/>
+Changed default value for <code>substanceDynamics</code> and
+<code>traceDynamics</code> from <code>energyDynamics</code>
+to <code>massDynamics</code>.
+</li>
+<li>
+September 28, 2010 by Michael Wetter:<br/>
+Changed array index for nominal value of <code>Xi</code>.
+</li>
+<li>
+September 13, 2010 by Michael Wetter:<br/>
+Set nominal attributes for medium based on default medium values.
+</li>
+<li>
+July 30, 2010 by Michael Wetter:<br/>
+Added parameter <code>C_nominal</code> which is used as the nominal attribute for <code>C</code>.
+Without this value, the ODE solver gives wrong results for concentrations around 1E-7.
+</li>
+<li>
+March 21, 2010 by Michael Wetter:<br/>
+Changed pressure start value from <code>system.p_start</code>
+to <code>Medium.p_default</code> since HVAC models may have water and
+air, which are typically at different pressures.
+</li>
+<li><i>February 6, 2010</i> by Michael Wetter:<br/>
+Added to <code>Medium.BaseProperties</code> the initialization
+<code>X(start=X_start[1:Medium.nX])</code>. Previously, the initialization
+was only done for <code>Xi</code> but not for <code>X</code>, which caused the
+medium to be initialized to <code>reference_X</code>, ignoring the value of <code>X_start</code>.
+</li>
+<li><i>October 12, 2009</i> by Michael Wetter:<br/>
+Implemented first version in <code>Buildings</code> library, based on model from
+<code>Modelica.Fluid 1.0</code>.
+</li>
+</ul>
+</html>"),
     Icon(graphics={            Rectangle(
           extent={{-100,100},{100,-100}},
           fillColor={135,135,135},
@@ -724,6 +753,6 @@ equation
         Text(
           extent={{-155,-120},{145,-160}},
           textColor={0,0,255},
-          textString="%name")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="%name")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConservationEquation;
diff --git a/AixLib/Fluid/Interfaces/EightPort.mo b/AixLib/Fluid/Interfaces/EightPort.mo
index 67d0abeb46..e0955817ed 100644
--- a/AixLib/Fluid/Interfaces/EightPort.mo
+++ b/AixLib/Fluid/Interfaces/EightPort.mo
@@ -144,20 +144,20 @@ partial model EightPort "Partial model with eight ports"
   annotation (
     preferredView="info",
     Documentation(info="<html>
- <p>This model defines an interface for components with eight ports. The parameters <code>allowFlowReversal1,
- </code> <code>allowFlowReversal2</code>, <code>allowFlowReversal3</code> and <code>allowFlowReversal4</code> 
- may be used by models that extend this model to treat flow reversal. </p>
- <p>This model is identical to <a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">Modelica.Fluid.Interfaces.PartialTwoPort</a>, except that it has eight ports. </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>July 2014, by Damien Picard:<br/>First implementation. </li>
- </ul>
- </html>"),
+<p>This model defines an interface for components with eight ports. The parameters <code>allowFlowReversal1,
+</code> <code>allowFlowReversal2</code>, <code>allowFlowReversal3</code> and <code>allowFlowReversal4</code> 
+may be used by models that extend this model to treat flow reversal. </p>
+<p>This model is identical to <a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">Modelica.Fluid.Interfaces.PartialTwoPort</a>, except that it has eight ports. </p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>July 2014, by Damien Picard:<br/>First implementation. </li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
           preserveAspectRatio=false,
           extent={{-100,-100},{100,100}},
@@ -169,6 +169,6 @@ partial model EightPort "Partial model with eight ports"
           textString="%name")}),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{
             100,100}}),
-                    graphics),
-  __Dymola_LockedEditing="Model from IBPSA");
+                    graphics), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end EightPort;
diff --git a/AixLib/Fluid/Interfaces/EightPortFlowResistanceParameters.mo b/AixLib/Fluid/Interfaces/EightPortFlowResistanceParameters.mo
index 28a8e6a72f..e9929eaa26 100644
--- a/AixLib/Fluid/Interfaces/EightPortFlowResistanceParameters.mo
+++ b/AixLib/Fluid/Interfaces/EightPortFlowResistanceParameters.mo
@@ -77,23 +77,23 @@ record EightPortFlowResistanceParameters
 
 annotation (preferredView="info",
 Documentation(info="<html>
- <p>
- This class contains parameters that are used to
- compute the pressure drop in components that have four fluid streams.
- Note that the nominal mass flow rate is not declared here because
- the model
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialEightPortInterface\">
- PartialHeightPortInterface</a>
- already declares it.
- </p>
- </html>",
+<p>
+This class contains parameters that are used to
+compute the pressure drop in components that have four fluid streams.
+Note that the nominal mass flow rate is not declared here because
+the model
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialEightPortInterface\">
+PartialHeightPortInterface</a>
+already declares it.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 28, 2015, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 28, 2015, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EightPortFlowResistanceParameters;
diff --git a/AixLib/Fluid/Interfaces/EightPortHeatMassExchanger.mo b/AixLib/Fluid/Interfaces/EightPortHeatMassExchanger.mo
index f807497f3b..fa7542207d 100644
--- a/AixLib/Fluid/Interfaces/EightPortHeatMassExchanger.mo
+++ b/AixLib/Fluid/Interfaces/EightPortHeatMassExchanger.mo
@@ -280,29 +280,29 @@ initial algorithm
   assert((energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState) or
           tau1 > Modelica.Constants.eps,
 "The parameter tau1, or the volume of the model from which tau may be derived, is unreasonably small.
-  You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
-  Received tau1 = "+ String(tau1) + "\n");
+ You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
+ Received tau1 = " + String(tau1) + "\n");
 
  // Check for tau2
   assert((energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState) or
           tau2 > Modelica.Constants.eps,
 "The parameter tau2, or the volume of the model from which tau may be derived, is unreasonably small.
-  You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
-  Received tau2 = "+ String(tau2) + "\n");
+ You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
+ Received tau2 = " + String(tau2) + "\n");
 
   // Check for tau1
   assert((energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState) or
           tau3 > Modelica.Constants.eps,
 "The parameter tau3, or the volume of the model from which tau may be derived, is unreasonably small.
-  You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
-  Received tau3 = "+ String(tau3) + "\n");
+ You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
+ Received tau3 = " + String(tau3) + "\n");
 
  // Check for tau2
   assert((energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState) or
           tau4 > Modelica.Constants.eps,
 "The parameter tau4, or the volume of the model from which tau may be derived, is unreasonably small.
-  You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
-  Received tau4 = "+ String(tau4) + "\n");
+ You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
+ Received tau4 = " + String(tau4) + "\n");
 
   assert(homotopyInitialization, "In " + getInstanceName() +
     ": The constant homotopyInitialization has been modified from its default value. This constant will be removed in future releases.",
@@ -359,27 +359,27 @@ equation
       smooth=Smooth.None));
   annotation (
     Documentation(info="<html>
- <p>This component transports four fluid streams between eight ports. It provides the basic model for implementing a dynamic heat exchanger. </p>
- <p>The model can be used as-is, although there will be no heat or mass transfer between the four fluid streams. To add heat transfer, heat flow can be added to the heat port of the four volumes.</p>
- <h4>Implementation</h4>
- <p>The variable names follow the conventions used in <a href=\"modelica://Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX\">Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX</a>. </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- July 18, 2018, by Massimo Cimmino:<br/>
- Remove start values of m_flow and dp variables.
- </li>
- </ul>
- <ul>
- <li>July 2014, by Damien Picard:<br/>First implementation. </li>
- </ul>
- </html>"),
+<p>This component transports four fluid streams between eight ports. It provides the basic model for implementing a dynamic heat exchanger. </p>
+<p>The model can be used as-is, although there will be no heat or mass transfer between the four fluid streams. To add heat transfer, heat flow can be added to the heat port of the four volumes.</p>
+<h4>Implementation</h4>
+<p>The variable names follow the conventions used in <a href=\"modelica://Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX\">Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX</a>. </p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+July 18, 2018, by Massimo Cimmino:<br/>
+Remove start values of m_flow and dp variables.
+</li>
+</ul>
+<ul>
+<li>July 2014, by Damien Picard:<br/>First implementation. </li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
         preserveAspectRatio=false,
         extent={{-100,-100},{100,100}},
@@ -415,6 +415,6 @@ equation
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid)}),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{
-            100,100}}), graphics),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100,100}}), graphics), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end EightPortHeatMassExchanger;
diff --git a/AixLib/Fluid/Interfaces/Examples/BaseClasses/PrescribedOutletState.mo b/AixLib/Fluid/Interfaces/Examples/BaseClasses/PrescribedOutletState.mo
index 96dd6f9d52..210517c902 100644
--- a/AixLib/Fluid/Interfaces/Examples/BaseClasses/PrescribedOutletState.mo
+++ b/AixLib/Fluid/Interfaces/Examples/BaseClasses/PrescribedOutletState.mo
@@ -148,38 +148,38 @@ equation
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-140,
             -120},{120,160}})),
     Documentation(info="<html>
- <p>
- Model that is used as the base class for models that
- demonstrates the use of an ideal heater and an ideal cooler,
- or an ideal humidifier and dehumidifier.
- </p>
- <p>
- The model on the top has almost unlimited positive capacity (<code>Q_flow_nominal = 1.0e10</code> Watts),
- and hence its outlet temperature always reaches the set points.
- </p>
- <p>
- The model in the middle has a limited negative capacitiy (<code>Q_flow_nominal = 1000</code> Watts), and hence
- its outlet state reaches only a limited value corresponding to its
- maximum negative capacity.
- </p>
- <p>
- The model at the bottom has unlimited capacity.
- </p>
- <p>
- At <i>t=1000</i> second, the flow reverses its direction.
- </p>
- <p>
- Each flow leg has the same mass flow rate. There are three mass flow sources
- as using one source only would yield a nonlinear system of equations that
- needs to be solved to determine the mass flow rate distribution.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that is used as the base class for models that
+demonstrates the use of an ideal heater and an ideal cooler,
+or an ideal humidifier and dehumidifier.
+</p>
+<p>
+The model on the top has almost unlimited positive capacity (<code>Q_flow_nominal = 1.0e10</code> Watts),
+and hence its outlet temperature always reaches the set points.
+</p>
+<p>
+The model in the middle has a limited negative capacitiy (<code>Q_flow_nominal = 1000</code> Watts), and hence
+its outlet state reaches only a limited value corresponding to its
+maximum negative capacity.
+</p>
+<p>
+The model at the bottom has unlimited capacity.
+</p>
+<p>
+At <i>t=1000</i> second, the flow reverses its direction.
+</p>
+<p>
+Each flow leg has the same mass flow rate. There are three mass flow sources
+as using one source only would yield a nonlinear system of equations that
+needs to be solved to determine the mass flow rate distribution.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutletState;
diff --git a/AixLib/Fluid/Interfaces/Examples/ConservationEquation.mo b/AixLib/Fluid/Interfaces/Examples/ConservationEquation.mo
index 13d3ea030e..0bf3fbd302 100644
--- a/AixLib/Fluid/Interfaces/Examples/ConservationEquation.mo
+++ b/AixLib/Fluid/Interfaces/Examples/ConservationEquation.mo
@@ -92,28 +92,28 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/ConservationEquation.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- Model that tests the conservation equations that are used
- for the heat and mass balance.
- </p>
- </html>",
+<p>
+Model that tests the conservation equations that are used
+for the heat and mass balance.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 23, 2018, by Filip Jorissen:<br/>
- Added <code>prescribedHeatFlowRate=true</code> since
- this model prescribes the heat flow rate.
- </li>
- <li>
- January 22, 2016 by Michael Wetter:<br/>
- Updated model to use the new parameter <code>use_mWat_flow</code>
- rather than <code>sensibleOnly</code>.
- </li>
- <li>
- September 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 23, 2018, by Filip Jorissen:<br/>
+Added <code>prescribedHeatFlowRate=true</code> since
+this model prescribes the heat flow rate.
+</li>
+<li>
+January 22, 2016 by Michael Wetter:<br/>
+Updated model to use the new parameter <code>use_mWat_flow</code>
+rather than <code>sensibleOnly</code>.
+</li>
+<li>
+September 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConservationEquation;
diff --git a/AixLib/Fluid/Interfaces/Examples/EightPortHeatMassExchanger.mo b/AixLib/Fluid/Interfaces/Examples/EightPortHeatMassExchanger.mo
index dcd6f08700..ac128bee19 100644
--- a/AixLib/Fluid/Interfaces/Examples/EightPortHeatMassExchanger.mo
+++ b/AixLib/Fluid/Interfaces/Examples/EightPortHeatMassExchanger.mo
@@ -101,20 +101,20 @@ equation
   connect(eigPor.port_a4, sin.ports[4]) annotation (Line(points={{10,2},{16,2},
           {16,-50},{3,-50}}, color={0,127,255}));
   annotation (    Documentation(info="<html>
- <p>
- This example model demonstrates the use of the
- <a href=\"modelica://AixLib.Fluid.Interfaces.EightPortHeatMassExchanger\">EightPortHeatMassExchanger</a> model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 18, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example model demonstrates the use of the
+<a href=\"modelica://AixLib.Fluid.Interfaces.EightPortHeatMassExchanger\">EightPortHeatMassExchanger</a> model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 18, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=5),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/EightPortHeatMassExchanger.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end EightPortHeatMassExchanger;
diff --git a/AixLib/Fluid/Interfaces/Examples/FourPortHeatMassExchanger.mo b/AixLib/Fluid/Interfaces/Examples/FourPortHeatMassExchanger.mo
index 62a75fec9b..45a3a90958 100644
--- a/AixLib/Fluid/Interfaces/Examples/FourPortHeatMassExchanger.mo
+++ b/AixLib/Fluid/Interfaces/Examples/FourPortHeatMassExchanger.mo
@@ -59,20 +59,20 @@ equation
   connect(ram_T.y, sou1.T_in) annotation (Line(points={{-69,0},{-66,0},{-66,14},
           {-62,14}},     color={0,0,127}));
   annotation (    Documentation(info="<html>
- <p>
- This example model demonstrates the used of the
- <a href=\"modelica://AixLib.Fluid.Interfaces.FourPortHeatMassExchanger\">FourPortHeatMassExchanger</a> model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 2, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example model demonstrates the used of the
+<a href=\"modelica://AixLib.Fluid.Interfaces.FourPortHeatMassExchanger\">FourPortHeatMassExchanger</a> model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 2, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=5),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/FourPortHeatMassExchanger.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end FourPortHeatMassExchanger;
diff --git a/AixLib/Fluid/Interfaces/Examples/HeaterCooler_u.mo b/AixLib/Fluid/Interfaces/Examples/HeaterCooler_u.mo
index 4a80ce8de9..b7bf8c3949 100644
--- a/AixLib/Fluid/Interfaces/Examples/HeaterCooler_u.mo
+++ b/AixLib/Fluid/Interfaces/Examples/HeaterCooler_u.mo
@@ -488,47 +488,47 @@ experiment(Tolerance=1e-6, StopTime=3600),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/HeaterCooler_u.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>Model that tests the basic class that is used for the heater models.
- It adds and removes heat for forward and reverse flow.
- The top and bottom models should give similar results,
- although the sign of the temperature difference over the components
- differ because of the reverse flow.
- The model computes differences in results that are expected to be
- close to each other after the initial transients decayed.
- All temperature sensors are configured as steady-state sensors to avoid
- differences in temperature due to the dynamic response of the sensor.
- </p>
- </html>",
+<p>Model that tests the basic class that is used for the heater models.
+It adds and removes heat for forward and reverse flow.
+The top and bottom models should give similar results,
+although the sign of the temperature difference over the components
+differ because of the reverse flow.
+The model computes differences in results that are expected to be
+close to each other after the initial transients decayed.
+All temperature sensors are configured as steady-state sensors to avoid
+differences in temperature due to the dynamic response of the sensor.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- May 30, 2014, by Michael Wetter:<br/>
- Changed initialization of mass dynamics to avoid overspecified system
- of equations if the medium model is incompressible.
- </li>
- <li>
- January 24, 2013, by Michael Wetter:<br/>
- Increased parameter <code>startTime</code> of the assert block
- and set initial conditions to
- <code>Modelica.Fluid.Types.Dynamics.FixedInitial</code>.
- </li>
- <li>
- July 11, 2011, by Michael Wetter:<br/>
- Changed model to sensors with two fluid ports.
- Moved model to <code>AixLib.Fluid.Interfaces.Examples</code>.
- </li>
- <li>
- April 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+May 30, 2014, by Michael Wetter:<br/>
+Changed initialization of mass dynamics to avoid overspecified system
+of equations if the medium model is incompressible.
+</li>
+<li>
+January 24, 2013, by Michael Wetter:<br/>
+Increased parameter <code>startTime</code> of the assert block
+and set initial conditions to
+<code>Modelica.Fluid.Types.Dynamics.FixedInitial</code>.
+</li>
+<li>
+July 11, 2011, by Michael Wetter:<br/>
+Changed model to sensors with two fluid ports.
+Moved model to <code>AixLib.Fluid.Interfaces.Examples</code>.
+</li>
+<li>
+April 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeaterCooler_u;
diff --git a/AixLib/Fluid/Interfaces/Examples/Humidifier_u.mo b/AixLib/Fluid/Interfaces/Examples/Humidifier_u.mo
index 819b90a419..bd936a3c75 100644
--- a/AixLib/Fluid/Interfaces/Examples/Humidifier_u.mo
+++ b/AixLib/Fluid/Interfaces/Examples/Humidifier_u.mo
@@ -546,51 +546,51 @@ experiment(Tolerance=1e-7, StopTime=3600),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/Humidifier_u.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- Model that tests the basic class that is used for the humidifier model.
- It adds and removes water for forward and reverse flow.
- The top and bottom models should give similar results, although
- the sign of the humidity difference over the components differ
- because of the reverse flow.
- The model computes differences of results that
- are expected to be close to each other after the
- initial transients decayed.</p>
- </html>",
+<p>
+Model that tests the basic class that is used for the humidifier model.
+It adds and removes water for forward and reverse flow.
+The top and bottom models should give similar results, although
+the sign of the humidity difference over the components differ
+because of the reverse flow.
+The model computes differences of results that
+are expected to be close to each other after the
+initial transients decayed.</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- May 30, 2014, by Michael Wetter:<br/>
- Changed initialization of mass dynamics to avoid overspecified system
- of equations if the medium model is incompressible.
- </li>
- <li>
- October 9, 2013, by Michael Wetter:<br/>
- Introduced protected model <code>Humidifier</code> so that states at
- the fluid ports can be computed without having to use a conditionally
- removed variable. This is required for the model to pass the model check in
- Dymola 2014 FD01 beta3 with <code>Advanced.PedanticModelica=true;</code>.
- </li>
- <li>
- January 24, 2013, by Michael Wetter:<br/>
- Set initial conditions to
- <code>Modelica.Fluid.Types.Dynamics.FixedInitial</code>.
- </li>
- <li>
- July 11, 2011, by Michael Wetter:<br/>
- Moved model to <code>AixLib.Fluid.Interfaces.Examples</code>.
- </li>
- <li>
- April 18, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+May 30, 2014, by Michael Wetter:<br/>
+Changed initialization of mass dynamics to avoid overspecified system
+of equations if the medium model is incompressible.
+</li>
+<li>
+October 9, 2013, by Michael Wetter:<br/>
+Introduced protected model <code>Humidifier</code> so that states at
+the fluid ports can be computed without having to use a conditionally
+removed variable. This is required for the model to pass the model check in
+Dymola 2014 FD01 beta3 with <code>Advanced.PedanticModelica=true;</code>.
+</li>
+<li>
+January 24, 2013, by Michael Wetter:<br/>
+Set initial conditions to
+<code>Modelica.Fluid.Types.Dynamics.FixedInitial</code>.
+</li>
+<li>
+July 11, 2011, by Michael Wetter:<br/>
+Moved model to <code>AixLib.Fluid.Interfaces.Examples</code>.
+</li>
+<li>
+April 18, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Humidifier_u;
diff --git a/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet.mo b/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet.mo
index 92269f5040..32c99f705f 100644
--- a/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet.mo
+++ b/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet.mo
@@ -26,25 +26,25 @@ equation
 __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/PrescribedOutlet.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that demonstrates
- <a href=\"modelica://AixLib.Fluid.Interfaces.PrescribedOutlet\">
- AixLib.Fluid.Interfaces.PrescribedOutlet</a>
- with mass fraction setpoint.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- Refactored model to allow <code>X_wSet</code> as an input.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
- </li>
- <li>
- November 11, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates
+<a href=\"modelica://AixLib.Fluid.Interfaces.PrescribedOutlet\">
+AixLib.Fluid.Interfaces.PrescribedOutlet</a>
+with mass fraction setpoint.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+Refactored model to allow <code>X_wSet</code> as an input.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
+</li>
+<li>
+November 11, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutlet;
diff --git a/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_TSetOnly.mo b/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_TSetOnly.mo
index 32928546f0..9d7f03cb1d 100644
--- a/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_TSetOnly.mo
+++ b/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_TSetOnly.mo
@@ -24,25 +24,25 @@ equation
 __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/PrescribedOutlet_TSetOnly.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that demonstrates
- <a href=\"modelica://AixLib.Fluid.Interfaces.PrescribedOutlet\">
- AixLib.Fluid.Interfaces.PrescribedOutlet</a>
- with temperature setpoint.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- Refactored model to allow <code>X_wSet</code> as an input.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
- </li>
- <li>
- November 11, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates
+<a href=\"modelica://AixLib.Fluid.Interfaces.PrescribedOutlet\">
+AixLib.Fluid.Interfaces.PrescribedOutlet</a>
+with temperature setpoint.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+Refactored model to allow <code>X_wSet</code> as an input.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
+</li>
+<li>
+November 11, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutlet_TSetOnly;
diff --git a/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_Water.mo b/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_Water.mo
index 167e4aee46..b3765b049f 100644
--- a/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_Water.mo
+++ b/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_Water.mo
@@ -26,25 +26,25 @@ equation
 __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/PrescribedOutlet_Water.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that demonstrates
- <a href=\"modelica://AixLib.Fluid.Interfaces.PrescribedOutlet\">
- AixLib.Fluid.Interfaces.PrescribedOutlet</a>
- with temperature setpoint and water as the medium.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- Refactored model to allow <code>X_wSet</code> as an input.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
- </li>
- <li>
- November 11, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates
+<a href=\"modelica://AixLib.Fluid.Interfaces.PrescribedOutlet\">
+AixLib.Fluid.Interfaces.PrescribedOutlet</a>
+with temperature setpoint and water as the medium.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+Refactored model to allow <code>X_wSet</code> as an input.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
+</li>
+<li>
+November 11, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutlet_Water;
diff --git a/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_X_wSetOnly.mo b/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_X_wSetOnly.mo
index 4439202fbf..735b36f6bf 100644
--- a/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_X_wSetOnly.mo
+++ b/AixLib/Fluid/Interfaces/Examples/PrescribedOutlet_X_wSetOnly.mo
@@ -26,25 +26,25 @@ equation
 __Dymola_Commands(file= "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/PrescribedOutlet_X_wSetOnly.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- Model that demonstrates
- <a href=\"modelica://AixLib.Fluid.Interfaces.PrescribedOutlet\">
- AixLib.Fluid.Interfaces.PrescribedOutlet</a>
- with mass fraction setpoint.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- Refactored model to allow <code>X_wSet</code> as an input.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
- </li>
- <li>
- November 11, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model that demonstrates
+<a href=\"modelica://AixLib.Fluid.Interfaces.PrescribedOutlet\">
+AixLib.Fluid.Interfaces.PrescribedOutlet</a>
+with mass fraction setpoint.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+Refactored model to allow <code>X_wSet</code> as an input.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
+</li>
+<li>
+November 11, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutlet_X_wSetOnly;
diff --git a/AixLib/Fluid/Interfaces/Examples/ReverseFlowHumidifier.mo b/AixLib/Fluid/Interfaces/Examples/ReverseFlowHumidifier.mo
index 8e8ef328de..5083f57c79 100644
--- a/AixLib/Fluid/Interfaces/Examples/ReverseFlowHumidifier.mo
+++ b/AixLib/Fluid/Interfaces/Examples/ReverseFlowHumidifier.mo
@@ -168,57 +168,57 @@ experiment(Tolerance=1e-6, StopTime=1),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/ReverseFlowHumidifier.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This model tests whether the results for a humidifer are
- identical for forward flow and reverse flow.
- </html>",revisions="<html>
- <ul>
- <li>
- September 20, 2020, by Michael Wetter:<br/>
- Updated model to use one port temperature sensor from Modelica Standard Library.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\"> #1399</a>.
- </li>
- <li>
- May 2, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed temperature connection that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- October 9, 2013, by Michael Wetter:<br/>
- Replaced
- <code>Modelica.Fluid.Sources.FixedBoundary</code>
- with
- <code>AixLib.Fluid.Sources.FixedBoundary</code>
- as otherwise, the pedantic model check fails in
- Dymola 2014 FD01 beta3.
- </li>
- <li>
- July 5, 2013, by Michael Wetter:<br/>
- Changed one instance of <code>Modelica.Fluid.Sources.MassFlowSource_T</code>,
- that was connected to the two fluid streams,
- to two instances, each having half the mass flow rate.
- This is required for the model to work with Modelica 3.2.1 due to the
- change introduced in
- ticket <a href=\"https://trac.modelica.org/Modelica/ticket/739\">#739</a>.
- </li>
- <li>
- August 19, 2010, by Michael Wetter:<br/>
- First implementation based on a model from Giuliano Fontanella.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This model tests whether the results for a humidifer are
+identical for forward flow and reverse flow.
+</html>", revisions="<html>
+<ul>
+<li>
+September 20, 2020, by Michael Wetter:<br/>
+Updated model to use one port temperature sensor from Modelica Standard Library.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\"> #1399</a>.
+</li>
+<li>
+May 2, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed temperature connection that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+October 9, 2013, by Michael Wetter:<br/>
+Replaced
+<code>Modelica.Fluid.Sources.FixedBoundary</code>
+with
+<code>AixLib.Fluid.Sources.FixedBoundary</code>
+as otherwise, the pedantic model check fails in
+Dymola 2014 FD01 beta3.
+</li>
+<li>
+July 5, 2013, by Michael Wetter:<br/>
+Changed one instance of <code>Modelica.Fluid.Sources.MassFlowSource_T</code>,
+that was connected to the two fluid streams,
+to two instances, each having half the mass flow rate.
+This is required for the model to work with Modelica 3.2.1 due to the
+change introduced in
+ticket <a href=\"https://trac.modelica.org/Modelica/ticket/739\">#739</a>.
+</li>
+<li>
+August 19, 2010, by Michael Wetter:<br/>
+First implementation based on a model from Giuliano Fontanella.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReverseFlowHumidifier;
diff --git a/AixLib/Fluid/Interfaces/Examples/ReverseFlowMassExchanger.mo b/AixLib/Fluid/Interfaces/Examples/ReverseFlowMassExchanger.mo
index acc0dff7bd..20c85bd0de 100644
--- a/AixLib/Fluid/Interfaces/Examples/ReverseFlowMassExchanger.mo
+++ b/AixLib/Fluid/Interfaces/Examples/ReverseFlowMassExchanger.mo
@@ -282,59 +282,59 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfa
     Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-400,-200},{200,
             200}})),
     Documentation(info="<html>
- <p>
- This model tests whether the results for a mass exchanger are
- identical for forward flow and reverse flow.
- </p>
- <p>
- Note that if the latent heat transfer effectiveness is non-zero, then
- the results will differ. The reason is that the maximum capacity stream
- is computed using the mass flow rates at <code>port_a1</code>
- and <code>port_a2</code>. For reverse flow, they are not equal if
- moisture is added to the mass flow rate. Using an average mass flow rate
- in computing the heat and moisture transfer would lead to identical results,
- but it would introduce additional nonlinear equations that need to be solved.
- Therefore, the model uses the mass flow rates at <code>port_a1</code>
- and <code>port_a2</code>.
- </p>
- <p>
- <b>Note:</b> This problem fails to translate in Dymola 2012 due to an error in Dymola's support
- of stream connector. This bug will be corrected in future versions of Dymola.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 20, 2020, by Michael Wetter:<br/>
- Updated model to use one port temperature sensor from Modelica Standard Library.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\"> #1399</a>.
- </li>
- <li>
- May 2, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- October 9, 2013, by Michael Wetter:<br/>
- Replaced
- <code>Modelica.Fluid.Sources.FixedBoundary</code>
- with
- <code>AixLib.Fluid.Sources.FixedBoundary</code>
- as otherwise, the pedantic model check fails in
- Dymola 2014 FD01 beta3.
- </li>
- <li>
- August 19, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the results for a mass exchanger are
+identical for forward flow and reverse flow.
+</p>
+<p>
+Note that if the latent heat transfer effectiveness is non-zero, then
+the results will differ. The reason is that the maximum capacity stream
+is computed using the mass flow rates at <code>port_a1</code>
+and <code>port_a2</code>. For reverse flow, they are not equal if
+moisture is added to the mass flow rate. Using an average mass flow rate
+in computing the heat and moisture transfer would lead to identical results,
+but it would introduce additional nonlinear equations that need to be solved.
+Therefore, the model uses the mass flow rates at <code>port_a1</code>
+and <code>port_a2</code>.
+</p>
+<p>
+<b>Note:</b> This problem fails to translate in Dymola 2012 due to an error in Dymola's support
+of stream connector. This bug will be corrected in future versions of Dymola.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 20, 2020, by Michael Wetter:<br/>
+Updated model to use one port temperature sensor from Modelica Standard Library.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\"> #1399</a>.
+</li>
+<li>
+May 2, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+October 9, 2013, by Michael Wetter:<br/>
+Replaced
+<code>Modelica.Fluid.Sources.FixedBoundary</code>
+with
+<code>AixLib.Fluid.Sources.FixedBoundary</code>
+as otherwise, the pedantic model check fails in
+Dymola 2014 FD01 beta3.
+</li>
+<li>
+August 19, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ReverseFlowMassExchanger;
diff --git a/AixLib/Fluid/Interfaces/Examples/StaticTwoPortConservationEquation.mo b/AixLib/Fluid/Interfaces/Examples/StaticTwoPortConservationEquation.mo
index 4fec280577..17d7a3c8be 100644
--- a/AixLib/Fluid/Interfaces/Examples/StaticTwoPortConservationEquation.mo
+++ b/AixLib/Fluid/Interfaces/Examples/StaticTwoPortConservationEquation.mo
@@ -105,26 +105,26 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Interfaces/Examples/StaticTwoPortConservationEquation.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- Model that tests the conservation equations that are used
- for the heat and mass balance.
- The instances have either water or air, and either allow or prohibit
- flow reversal.
- This example tests the implementation of the steady-state balance.
- </p>
- </html>",
+<p>
+Model that tests the conservation equations that are used
+for the heat and mass balance.
+The instances have either water or air, and either allow or prohibit
+flow reversal.
+This example tests the implementation of the steady-state balance.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 22, 2016 by Michael Wetter:<br/>
- Updated model to use the new parameter <code>use_mWat_flow</code>
- rather than <code>sensibleOnly</code>.
- </li>
- <li>
- July 17, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 22, 2016 by Michael Wetter:<br/>
+Updated model to use the new parameter <code>use_mWat_flow</code>
+rather than <code>sensibleOnly</code>.
+</li>
+<li>
+July 17, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end StaticTwoPortConservationEquation;
diff --git a/AixLib/Fluid/Interfaces/FourPortFlowResistanceParameters.mo b/AixLib/Fluid/Interfaces/FourPortFlowResistanceParameters.mo
index 25983fab91..db0329f6f7 100644
--- a/AixLib/Fluid/Interfaces/FourPortFlowResistanceParameters.mo
+++ b/AixLib/Fluid/Interfaces/FourPortFlowResistanceParameters.mo
@@ -10,8 +10,8 @@ record FourPortFlowResistanceParameters
     "= true, use m_flow = f(dp) else dp = f(m_flow)"
     annotation (Evaluate=true, Dialog(enable = computeFlowResistance1,
                 tab="Flow resistance", group="Medium 1"));
-  parameter Modelica.Units.SI.PressureDifference dp1_nominal(min=0, displayUnit=
-       "Pa") "Pressure difference"
+  parameter Modelica.Units.SI.PressureDifference dp1_nominal(min=0, displayUnit
+      ="Pa") "Pressure difference"
     annotation (Dialog(group="Nominal condition"));
   parameter Boolean linearizeFlowResistance1 = false
     "= true, use linear relation between m_flow and dp for any flow rate"
@@ -29,8 +29,8 @@ record FourPortFlowResistanceParameters
     "= true, use m_flow = f(dp) else dp = f(m_flow)"
     annotation (Evaluate=true, Dialog(enable = computeFlowResistance2,
                 tab="Flow resistance", group="Medium 2"));
-  parameter Modelica.Units.SI.PressureDifference dp2_nominal(min=0, displayUnit=
-       "Pa") "Pressure difference"
+  parameter Modelica.Units.SI.PressureDifference dp2_nominal(min=0, displayUnit
+      ="Pa") "Pressure difference"
     annotation (Dialog(group="Nominal condition"));
   parameter Boolean linearizeFlowResistance2 = false
     "= true, use linear relation between m_flow and dp for any flow rate"
@@ -42,29 +42,29 @@ record FourPortFlowResistanceParameters
                       tab="Flow resistance", group="Medium 2"));
 annotation (preferredView="info",
 Documentation(info="<html>
- <p>
- This class contains parameters that are used to
- compute the pressure drop in components that have two fluid streams.
- Note that the nominal mass flow rate is not declared here because
- the model
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPortInterface\">
- PartialFourPortInterface</a>
- already declares it.
- </p>
- </html>",
+<p>
+This class contains parameters that are used to
+compute the pressure drop in components that have two fluid streams.
+Note that the nominal mass flow rate is not declared here because
+the model
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPortInterface\">
+PartialFourPortInterface</a>
+already declares it.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FourPortFlowResistanceParameters;
diff --git a/AixLib/Fluid/Interfaces/FourPortHeatMassExchanger.mo b/AixLib/Fluid/Interfaces/FourPortHeatMassExchanger.mo
index 09760c7e06..9be3c9e13a 100644
--- a/AixLib/Fluid/Interfaces/FourPortHeatMassExchanger.mo
+++ b/AixLib/Fluid/Interfaces/FourPortHeatMassExchanger.mo
@@ -161,15 +161,15 @@ initial equation
   assert((energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState) or
           tau1 > Modelica.Constants.eps,
 "The parameter tau1, or the volume of the model from which tau may be derived, is unreasonably small.
-  You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
-  Received tau1 = "+ String(tau1) + "\n");
+ You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
+ Received tau1 = " + String(tau1) + "\n");
 
  // Check for tau2
   assert((energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState) or
           tau2 > Modelica.Constants.eps,
 "The parameter tau2, or the volume of the model from which tau may be derived, is unreasonably small.
-  You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
-  Received tau2 = "+ String(tau2) + "\n");
+ You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
+ Received tau2 = " + String(tau2) + "\n");
 
   assert(homotopyInitialization, "In " + getInstanceName() +
     ": The constant homotopyInitialization has been modified from its default value. This constant will be removed in future releases.",
@@ -196,163 +196,163 @@ equation
       color={0,127,255}));
   annotation (
     Documentation(info="<html>
- <p>
- This component transports two fluid streams between four ports.
- It provides the basic model for implementing a dynamic heat exchanger.
- </p>
- <p>
- The model can be used as-is, although there will be no heat or mass transfer
- between the two fluid streams.
- To add heat transfer, heat flow can be added to the heat port of the two volumes.
- See for example
- <a href=\"AixLib.Fluid.Chillers.Carnot_y\">
- AixLib.Fluid.Chillers.Carnot_y</a>.
- To add moisture input into (or moisture output from) volume <code>vol2</code>,
- the model can be replaced with
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir\">
- AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir</a>.
- </p>
- <h4>Implementation</h4>
- <p>
- The variable names follow the conventions used in
- <a href=\"modelica://Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX\">
- Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 3, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
- </li>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- October 23, 2017, by Michael Wetter:<br/>
- Made volume <code>vol1</code> replaceable. This is required for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Set <code>quantity</code> attributes.
- </li>
- <li>
- November 13, 2015, by Michael Wetter:<br/>
- Changed assignments of start values in <code>extends</code> statement.
- This is for issue
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/299\">#299</a>.
- </li>
- <li>
- June 2, 2015, by Filip Jorissen:<br/>
- Removed final modifier from <code>mSenFac</code> in
- <code>vol1</code> and <code>vol2</code>.
- This is for issue
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/258=\">#258</a>.
- </li>
- <li>
- May 6, 2015, by Michael Wetter:<br/>
- Added missing propagation of <code>allowFlowReversal</code> to
- instances <code>vol1</code> and <code>vol2</code>.
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">#412</a>.
- </li>
- <li>
- October 6, 2014, by Michael Wetter:<br/>
- Changed medium declaration in pressure drop elements to be final.
- </li>
- <li>
- May 28, 2014, by Michael Wetter:<br/>
- Removed <code>annotation(Evaluate=true)</code> for parameters <code>tau1</code>
- and <code>tau2</code>.
- This is needed to allow changing the time constant after translation.
- </li>
- <li>
- November 12, 2013, by Michael Wetter:<br/>
- Removed <code>import Modelica.Constants</code> statement.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Removed parameter <code>show_V_flow</code>.
- </li>
- <li>
- September 26, 2013, by Michael Wetter:<br/>
- Removed unrequired <code>sum</code> operator.
- </li>
- <li>
- February 6, 2012, by Michael Wetter:<br/>
- Updated documentation.
- </li>
- <li>
- February 3, 2012, by Michael Wetter:<br/>
- Removed assignment of <code>m_flow_small</code> as it is no
- longer used in its base class.
- </li>
- <li>
- July 29, 2011, by Michael Wetter:
- <ul>
- <li>
- Changed values of
- <code>h_outflow_a1_start</code>,
- <code>h_outflow_b1_start</code>,
- <code>h_outflow_a2_start</code> and
- <code>h_outflow_b2_start</code>, and
- declared them as final.
- </li>
- <li>
- Set nominal values for <code>vol1.C</code> and <code>vol2.C</code>.
- </li>
- </ul>
- </li>
- <li>
- July 11, 2011, by Michael Wetter:<br/>
- Changed parameterization of fluid volume so that steady-state balance is
- used when <code>tau = 0</code>.
- </li>
- <li>
- March 25, 2011, by Michael Wetter:<br/>
- Added homotopy operator.
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- Added model to compute flow friction.
- </li>
- <li>
- September 10, 2008 by Michael Wetter:<br/>
- Added <code>stateSelect=StateSelect.always</code> for temperature of volume 1.
- </li>
- <li>
- Changed temperature sensor from Celsius to Kelvin.
- Unit conversion should be made during output
- processing.
- </li>
- <li>
- August 5, 2008, by Michael Wetter:<br/>
- Replaced instances of <code>Delays.DelayFirstOrder</code> with instances of
- <code>MixingVolumes.MixingVolume</code>. This allows to extract liquid for a condensing cooling
- coil model.
- </li>
- <li>
- March 25, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component transports two fluid streams between four ports.
+It provides the basic model for implementing a dynamic heat exchanger.
+</p>
+<p>
+The model can be used as-is, although there will be no heat or mass transfer
+between the two fluid streams.
+To add heat transfer, heat flow can be added to the heat port of the two volumes.
+See for example
+<a href=\"modelica://AixLib.Fluid.Chillers.Carnot_y\">
+AixLib.Fluid.Chillers.Carnot_y</a>.
+To add moisture input into (or moisture output from) volume <code>vol2</code>,
+the model can be replaced with
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir\">
+AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir</a>.
+</p>
+<h4>Implementation</h4>
+<p>
+The variable names follow the conventions used in
+<a href=\"modelica://Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX\">
+Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 3, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+October 23, 2017, by Michael Wetter:<br/>
+Made volume <code>vol1</code> replaceable. This is required for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Set <code>quantity</code> attributes.
+</li>
+<li>
+November 13, 2015, by Michael Wetter:<br/>
+Changed assignments of start values in <code>extends</code> statement.
+This is for issue
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/299\">#299</a>.
+</li>
+<li>
+June 2, 2015, by Filip Jorissen:<br/>
+Removed final modifier from <code>mSenFac</code> in
+<code>vol1</code> and <code>vol2</code>.
+This is for issue
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/258=\">#258</a>.
+</li>
+<li>
+May 6, 2015, by Michael Wetter:<br/>
+Added missing propagation of <code>allowFlowReversal</code> to
+instances <code>vol1</code> and <code>vol2</code>.
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">#412</a>.
+</li>
+<li>
+October 6, 2014, by Michael Wetter:<br/>
+Changed medium declaration in pressure drop elements to be final.
+</li>
+<li>
+May 28, 2014, by Michael Wetter:<br/>
+Removed <code>annotation(Evaluate=true)</code> for parameters <code>tau1</code>
+and <code>tau2</code>.
+This is needed to allow changing the time constant after translation.
+</li>
+<li>
+November 12, 2013, by Michael Wetter:<br/>
+Removed <code>import Modelica.Constants</code> statement.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Removed parameter <code>show_V_flow</code>.
+</li>
+<li>
+September 26, 2013, by Michael Wetter:<br/>
+Removed unrequired <code>sum</code> operator.
+</li>
+<li>
+February 6, 2012, by Michael Wetter:<br/>
+Updated documentation.
+</li>
+<li>
+February 3, 2012, by Michael Wetter:<br/>
+Removed assignment of <code>m_flow_small</code> as it is no
+longer used in its base class.
+</li>
+<li>
+July 29, 2011, by Michael Wetter:
+<ul>
+<li>
+Changed values of
+<code>h_outflow_a1_start</code>,
+<code>h_outflow_b1_start</code>,
+<code>h_outflow_a2_start</code> and
+<code>h_outflow_b2_start</code>, and
+declared them as final.
+</li>
+<li>
+Set nominal values for <code>vol1.C</code> and <code>vol2.C</code>.
+</li>
+</ul>
+</li>
+<li>
+July 11, 2011, by Michael Wetter:<br/>
+Changed parameterization of fluid volume so that steady-state balance is
+used when <code>tau = 0</code>.
+</li>
+<li>
+March 25, 2011, by Michael Wetter:<br/>
+Added homotopy operator.
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+Added model to compute flow friction.
+</li>
+<li>
+September 10, 2008 by Michael Wetter:<br/>
+Added <code>stateSelect=StateSelect.always</code> for temperature of volume 1.
+</li>
+<li>
+Changed temperature sensor from Celsius to Kelvin.
+Unit conversion should be made during output
+processing.
+</li>
+<li>
+August 5, 2008, by Michael Wetter:<br/>
+Replaced instances of <code>Delays.DelayFirstOrder</code> with instances of
+<code>MixingVolumes.MixingVolume</code>. This allows to extract liquid for a condensing cooling
+coil model.
+</li>
+<li>
+March 25, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
         preserveAspectRatio=false,
         extent={{-100,-100},{100,100}},
@@ -374,6 +374,6 @@ equation
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,0},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end FourPortHeatMassExchanger;
diff --git a/AixLib/Fluid/Interfaces/LumpedVolumeDeclarations.mo b/AixLib/Fluid/Interfaces/LumpedVolumeDeclarations.mo
index 2f2cfcc8a0..07f5cd0932 100644
--- a/AixLib/Fluid/Interfaces/LumpedVolumeDeclarations.mo
+++ b/AixLib/Fluid/Interfaces/LumpedVolumeDeclarations.mo
@@ -48,10 +48,10 @@ block LumpedVolumeDeclarations "Declarations for lumped volumes"
     "Factor for scaling the sensible thermal mass of the volume"
     annotation(Dialog(tab="Dynamics"));
 
+protected
   // The parameter below is evaluated by OCT during compilation, and
   // if false, the assert statement won't be optimized away during
   // code generation.
-protected
   final parameter Boolean wrongEnergyMassBalanceConfiguration=
     not (energyDynamics <> Modelica.Fluid.Types.Dynamics.SteadyState or
          massDynamics == Modelica.Fluid.Types.Dynamics.SteadyState)
@@ -66,79 +66,79 @@ initial equation
 
 annotation (preferredView="info",
 Documentation(info="<html>
- <p>
- This class contains parameters and medium properties
- that are used in the lumped  volume model, and in models that extend the
- lumped volume model.
- </p>
- <p>
- These parameters are used for example by
- <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.ConservationEquation</a>,
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
- AixLib.Fluid.MixingVolumes.MixingVolume</a> and
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.Radiators.RadiatorEN442_2\">
- AixLib.Fluid.HeatExchangers.Radiators.RadiatorEN442_2</a>.
- </p>
- </html>",
+<p>
+This class contains parameters and medium properties
+that are used in the lumped  volume model, and in models that extend the
+lumped volume model.
+</p>
+<p>
+These parameters are used for example by
+<a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.ConservationEquation</a>,
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
+AixLib.Fluid.MixingVolumes.MixingVolume</a> and
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.Radiators.RadiatorEN442_2\">
+AixLib.Fluid.HeatExchangers.Radiators.RadiatorEN442_2</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 3, 2022, by Michael Wetter:<br/>
- Moved <code>massDynamics</code> to <code>Advanced</code> tab,
- added assertion for correct combination of energy and mass dynamics and
- changed type from <code>record</code> to <code>block</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- November 9, 2018 by Michael Wetter:<br/>
- Limited choices of media that are displayed in the pull down menu of
- graphical editors.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">issue 1050</a>.
- </li>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>quantity=Medium.substanceNames</code> for <code>X_start</code>.
- </li>
- <li>
- October 21, 2014, by Filip Jorissen:<br/>
- Added parameter <code>mFactor</code> to increase the thermal capacity.
- </li>
- <li>
- August 2, 2011, by Michael Wetter:<br/>
- Set <code>substanceDynamics</code> and <code>traceDynamics</code> to final
- and equal to <code>energyDynamics</code>,
- as there is no need to make them different from <code>energyDynamics</code>.
- </li>
- <li>
- August 1, 2011, by Michael Wetter:<br/>
- Changed default value for <code>energyDynamics</code> to
- <code>Modelica.Fluid.Types.Dynamics.DynamicFreeInitial</code> because
- <code>Modelica.Fluid.Types.Dynamics.SteadyStateInitial</code> leads
- to high order DAE that Dymola cannot reduce.
- </li>
- <li>
- July 31, 2011, by Michael Wetter:<br/>
- Changed default value for <code>energyDynamics</code> to
- <code>Modelica.Fluid.Types.Dynamics.SteadyStateInitial</code>.
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 3, 2022, by Michael Wetter:<br/>
+Moved <code>massDynamics</code> to <code>Advanced</code> tab,
+added assertion for correct combination of energy and mass dynamics and
+changed type from <code>record</code> to <code>block</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+November 9, 2018 by Michael Wetter:<br/>
+Limited choices of media that are displayed in the pull down menu of
+graphical editors.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">issue 1050</a>.
+</li>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>quantity=Medium.substanceNames</code> for <code>X_start</code>.
+</li>
+<li>
+October 21, 2014, by Filip Jorissen:<br/>
+Added parameter <code>mFactor</code> to increase the thermal capacity.
+</li>
+<li>
+August 2, 2011, by Michael Wetter:<br/>
+Set <code>substanceDynamics</code> and <code>traceDynamics</code> to final
+and equal to <code>energyDynamics</code>,
+as there is no need to make them different from <code>energyDynamics</code>.
+</li>
+<li>
+August 1, 2011, by Michael Wetter:<br/>
+Changed default value for <code>energyDynamics</code> to
+<code>Modelica.Fluid.Types.Dynamics.DynamicFreeInitial</code> because
+<code>Modelica.Fluid.Types.Dynamics.SteadyStateInitial</code> leads
+to high order DAE that Dymola cannot reduce.
+</li>
+<li>
+July 31, 2011, by Michael Wetter:<br/>
+Changed default value for <code>energyDynamics</code> to
+<code>Modelica.Fluid.Types.Dynamics.SteadyStateInitial</code>.
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LumpedVolumeDeclarations;
diff --git a/AixLib/Fluid/Interfaces/PartialEightPortInterface.mo b/AixLib/Fluid/Interfaces/PartialEightPortInterface.mo
index a51617d46a..62d03a73ca 100644
--- a/AixLib/Fluid/Interfaces/PartialEightPortInterface.mo
+++ b/AixLib/Fluid/Interfaces/PartialEightPortInterface.mo
@@ -1,6 +1,6 @@
 within AixLib.Fluid.Interfaces;
 partial model PartialEightPortInterface
-  "Partial model transporting fluid between eight ports without storing mass or energy"
+  "Partial model with eight ports and declaration of quantities that are used by many models"
   extends AixLib.Fluid.Interfaces.EightPort;
   parameter Modelica.Units.SI.MassFlowRate m1_flow_nominal(min=0)
     "Nominal mass flow rate" annotation (Dialog(group="Nominal condition"));
@@ -162,53 +162,60 @@ protected
   annotation (
   preferredView="info",
     Documentation(info="<html>
- <p>
- This component defines the interface for models that transport four fluid streams between eight ports.
- It is similar to <a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>,
- but it has eight ports instead of two. </p>
- <p>
- The model is used by other models in this package that add heat transfer,
- mass transfer and pressure drop equations.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 3, 2022, by Michael Wetter:<br/>
- If <code>allowFlowReversal==false</code>, removed <code>noEvent()</code> declaration
- for <code>sta_a</code> and for <code>sta_b</code> because the variable is either
- already used with <code>inStream()</code> in the computation of <code>state_*_inflow</code>,
- or the result of a variable of the model that already may generate an event.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
- </li>
- <li>
- February 2, 2022, by Hongxiang Fu:<br/>
- If <code>allowFlowReversal==false</code>, replaced <code>actualStream()</code>
- with <code>inStream()</code> for <code>sta_a</code> and
- removed <code>actualStream()</code> for <code>sta_b</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
- </li>
- <li>
- March 30, 2021, by Michael Wetter:<br/>
- Added annotation <code>HideResult=true</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
- </li>
- <li>
- July 12, 2019, by Michael Wetter:<br/>
- Corrected wrong medium in declaration of <code>m4_flow</code>.
- </li>
- <li>
- July 2014, by Damien Picard:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component defines the interface for models with eight fluid ports
+and four fluid streams.
+It is similar to <a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>,
+but it has eight ports instead of two. </p>
+<p>
+The model is used by other models in this package that add heat transfer,
+mass transfer and pressure drop equations.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2023, by Michael Wetter:<br/>
+Improved documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1796\">IBPSA, #1796</a>.
+</li>
+<li>
+February 3, 2022, by Michael Wetter:<br/>
+If <code>allowFlowReversal==false</code>, removed <code>noEvent()</code> declaration
+for <code>sta_a</code> and for <code>sta_b</code> because the variable is either
+already used with <code>inStream()</code> in the computation of <code>state_*_inflow</code>,
+or the result of a variable of the model that already may generate an event.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
+</li>
+<li>
+February 2, 2022, by Hongxiang Fu:<br/>
+If <code>allowFlowReversal==false</code>, replaced <code>actualStream()</code>
+with <code>inStream()</code> for <code>sta_a</code> and
+removed <code>actualStream()</code> for <code>sta_b</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
+</li>
+<li>
+March 30, 2021, by Michael Wetter:<br/>
+Added annotation <code>HideResult=true</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
+</li>
+<li>
+July 12, 2019, by Michael Wetter:<br/>
+Corrected wrong medium in declaration of <code>m4_flow</code>.
+</li>
+<li>
+July 2014, by Damien Picard:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{
             100,100}}),
                     graphics),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
-            100}}), graphics),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100}}), graphics), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialEightPortInterface;
diff --git a/AixLib/Fluid/Interfaces/PartialFourPort.mo b/AixLib/Fluid/Interfaces/PartialFourPort.mo
index f92c80d06d..1f6ff19ee1 100644
--- a/AixLib/Fluid/Interfaces/PartialFourPort.mo
+++ b/AixLib/Fluid/Interfaces/PartialFourPort.mo
@@ -58,92 +58,92 @@ partial model PartialFourPort "Partial model with four ports"
   annotation (
     preferredView="info",
     Documentation(info="<html>
- <p>
- This model defines an interface for components with four ports.
- The parameters <code>allowFlowReversal1</code> and
- <code>allowFlowReversal2</code> may be used by models that extend
- this model to treat flow reversal.
- </p>
- <p>
- This model is identical to
- <a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">
- Modelica.Fluid.Interfaces.PartialTwoPort</a>, except for the
- fowllowing:
- </p>
- <ol>
- <li>it has four ports, and
- </li>
- <li>
- the parameters <code>port_a_exposesState</code>,
- <code>port_b_exposesState</code> and
- <code>showDesignFlowDirection</code>
- are not implemented.
- </li>
- </ol>
- </html>",revisions="<html>
- <ul>
- <li>
- April 6, 2020, by Filip Jorissen:<br/>
- Added arrows to the icon indicating the intended flow direction
- when <code>allowFlowReversal=false</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1336\">#1336</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- July 8, 2018, by Filip Jorissen:<br/>
- Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
- </li>
- <li>
- November 12, 2015, by Michael Wetter:<br/>
- Renamed model from <code>FourPort</code> to
- <code>PartialFourPort</code>.
- Removed parameters
- <code>h_outflow_a1_start</code>,
- <code>h_outflow_b1_start</code>,
- <code>h_outflow_a2_start</code> and
- <code>h_outflow_b2_start</code>.
- This is for issue
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/299\">#299</a>.
- </li>
- <li>
- October 30, 2015, by Matthis Thorade:<br/>
- Added <code>partial</code> keyword to model declaration.
- </li>
- <li>
- October 6, 2014, by Michael Wetter:<br/>
- Changed medium declaration in ports to be final.
- </li>
- <li>
- October 3, 2014, by Michael Wetter:<br/>
- Changed assignment of nominal value to avoid in OpenModelica the warning
- alias set with different nominal values.
- </li>
- <li>
- November 12, 2013, by Michael Wetter:<br/>
- Removed <code>import Modelica.Constants</code> statement.
- </li>
- <li>
- September 26, 2013 by Michael Wetter:<br/>
- Added missing <code>each</code> keyword in declaration of nominal value for
- <code>Xi_outflow</code>.
- </li>
- <li>
- September 17, 2010 by Michael Wetter:<br/>
- Fixed bug: The start value for <code>port_b1.h_outflow</code>
- was set to <code>h_outflow_b2_start</code> instead of <code>h_outflow_b1_start</code>.
- </li>
- <li>
- February 26, 2010 by Michael Wetter:<br/>
- Added start values for outflowing enthalpy because they
- are often iteration variables in nonlinear equation systems.
- </li>
- </ul>
- </html>"),
+<p>
+This model defines an interface for components with four ports.
+The parameters <code>allowFlowReversal1</code> and
+<code>allowFlowReversal2</code> may be used by models that extend
+this model to treat flow reversal.
+</p>
+<p>
+This model is identical to
+<a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">
+Modelica.Fluid.Interfaces.PartialTwoPort</a>, except for the
+fowllowing:
+</p>
+<ol>
+<li>it has four ports, and
+</li>
+<li>
+the parameters <code>port_a_exposesState</code>,
+<code>port_b_exposesState</code> and
+<code>showDesignFlowDirection</code>
+are not implemented.
+</li>
+</ol>
+</html>", revisions="<html>
+<ul>
+<li>
+April 6, 2020, by Filip Jorissen:<br/>
+Added arrows to the icon indicating the intended flow direction
+when <code>allowFlowReversal=false</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1336\">#1336</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+July 8, 2018, by Filip Jorissen:<br/>
+Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
+</li>
+<li>
+November 12, 2015, by Michael Wetter:<br/>
+Renamed model from <code>FourPort</code> to
+<code>PartialFourPort</code>.
+Removed parameters
+<code>h_outflow_a1_start</code>,
+<code>h_outflow_b1_start</code>,
+<code>h_outflow_a2_start</code> and
+<code>h_outflow_b2_start</code>.
+This is for issue
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/299\">#299</a>.
+</li>
+<li>
+October 30, 2015, by Matthis Thorade:<br/>
+Added <code>partial</code> keyword to model declaration.
+</li>
+<li>
+October 6, 2014, by Michael Wetter:<br/>
+Changed medium declaration in ports to be final.
+</li>
+<li>
+October 3, 2014, by Michael Wetter:<br/>
+Changed assignment of nominal value to avoid in OpenModelica the warning
+alias set with different nominal values.
+</li>
+<li>
+November 12, 2013, by Michael Wetter:<br/>
+Removed <code>import Modelica.Constants</code> statement.
+</li>
+<li>
+September 26, 2013 by Michael Wetter:<br/>
+Added missing <code>each</code> keyword in declaration of nominal value for
+<code>Xi_outflow</code>.
+</li>
+<li>
+September 17, 2010 by Michael Wetter:<br/>
+Fixed bug: The start value for <code>port_b1.h_outflow</code>
+was set to <code>h_outflow_b2_start</code> instead of <code>h_outflow_b1_start</code>.
+</li>
+<li>
+February 26, 2010 by Michael Wetter:<br/>
+Added start values for outflowing enthalpy because they
+are often iteration variables in nonlinear equation systems.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
           preserveAspectRatio=true,
           extent={{-100,-100},{100,100}},
@@ -169,6 +169,6 @@ partial model PartialFourPort "Partial model with four ports"
           fillPattern=FillPattern.Solid,
           visible=not allowFlowReversal2,
           origin={-79,-50},
-          rotation=360)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          rotation=360)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialFourPort;
diff --git a/AixLib/Fluid/Interfaces/PartialFourPortInterface.mo b/AixLib/Fluid/Interfaces/PartialFourPortInterface.mo
index 3518c81456..9a5f3f4ee4 100644
--- a/AixLib/Fluid/Interfaces/PartialFourPortInterface.mo
+++ b/AixLib/Fluid/Interfaces/PartialFourPortInterface.mo
@@ -1,6 +1,6 @@
 within AixLib.Fluid.Interfaces;
 partial model PartialFourPortInterface
-  "Partial model transporting fluid between two ports without storing mass or energy"
+  "Partial model with four ports and declaration of quantities that are used by many models"
   extends AixLib.Fluid.Interfaces.PartialFourPort;
   parameter Modelica.Units.SI.MassFlowRate m1_flow_nominal(min=0)
     "Nominal mass flow rate" annotation (Dialog(group="Nominal condition"));
@@ -89,143 +89,149 @@ protected
   annotation (
   preferredView="info",
     Documentation(info="<html>
- <p>
- This component defines the interface for models that
- transport two fluid streams between four ports.
- It is similar to
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
- AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>,
- but it has four ports instead of two.
- </p>
- <p>
- The model is used by other models in this package that add heat transfer,
- mass transfer and pressure drop equations.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 3, 2022, by Michael Wetter:<br/>
- If <code>allowFlowReversal==false</code>, removed <code>noEvent()</code> declaration
- for <code>sta_a</code> and for <code>sta_b</code> because the variable is either
- already used with <code>inStream()</code> in the computation of <code>state_*_inflow</code>,
- or the result of a variable of the model that already may generate an event.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
- </li>
- <li>
- February 2, 2022, by Hongxiang Fu:<br/>
- If <code>allowFlowReversal==false</code>, replaced <code>actualStream()</code>
- with <code>inStream()</code> for <code>sta_a</code> and
- removed <code>actualStream()</code> for <code>sta_b</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
- </li>
- <li>
- March 30, 2021, by Michael Wetter:<br/>
- Added annotation <code>HideResult=true</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Moved computation of pressure drop to variable assignment so that
- the model won't mix graphical with textual modeling if used as a base
- class for a graphically implemented model.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Removed start values for mass flow rate and pressure difference
- to simplify the parameter window.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 13, 2013 by Michael Wetter:<br/>
- Removed assignment of <code>min</code> and <code>max</code>
- attributes of port mass flow rates, as this is already
- done in the base class.
- </li>
- <li>
- November 12, 2013 by Michael Wetter:<br/>
- Removed <code>import Modelica.Constants;</code> statement.
- </li>
- <li>
- November 11, 2013 by Michael Wetter:<br/>
- Removed the parameter <code>homotopyInitialization</code>
- as it is no longer used in this model.
- </li>
- <li>
- November 10, 2013 by Michael Wetter:<br/>
- In the computation of <code>sta_a1</code>,
- <code>sta_a2</code>, <code>sta_b1</code> and <code>sta_b2</code>,
- removed the branch that uses the homotopy operator.
- The rational is that these variables are conditionally enables (because
- of <code>... if show_T</code>). Therefore, the Modelica Language Specification
- does not allow for these variables to be used in any equation. Hence,
- the use of the homotopy operator is not needed here.
- </li>
- <li>
- October 10, 2013 by Michael Wetter:<br/>
- Added <code>noEvent</code> to the computation of the states at the port.
- This is correct, because the states are only used for reporting, but not
- to compute any other variable.
- Use of the states to compute other variables would violate the Modelica
- language, as conditionally removed variables must not be used in any equation.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Removed the computation of <code>V_flow</code> and removed the parameter
- <code>show_V_flow</code>.
- The reason is that the computation of <code>V_flow</code> required
- the use of <code>sta_a</code> (to compute the density),
- but <code>sta_a</code> is also a variable that is conditionally
- enabled. However, this was not correct Modelica syntax as conditional variables
- can only be used in a <code>connect</code>
- statement, not in an assignment. Dymola 2014 FD01 beta3 is checking
- for this incorrect syntax. Hence, <code>V_flow</code> was removed as its
- conditional implementation would require a rather cumbersome implementation
- that uses a new connector that carries the state of the medium.
- </li>
- <li>
- April 26, 2013 by Marco Bonvini:<br/>
- Moved the definitions of <code>dp1</code> and <code>dp2</code> because they cause some problem with PyFMI.
- </li>
- <li>
- March 27, 2012 by Michael Wetter:<br/>
- Replaced the erroneous function call <code>Medium.density</code> with
- <code>Medium1.density</code> and <code>Medium2.density</code>.
- Changed condition to remove <code>sta_a1</code> and <code>sta_a2</code> to also
- compute the states at the inlet port if <code>show_V_flow=true</code>.
- The previous implementation resulted in a translation error
- if <code>show_V_flow=true</code>, but worked correctly otherwise
- because the erroneous function call is removed if  <code>show_V_flow=false</code>.
- </li>
- <li>
- March 27, 2011 by Michael Wetter:<br/>
- Added <code>homotopy</code> operator.
- </li>
- <li>
- March 21, 2010 by Michael Wetter:<br/>
- Changed pressure start value from <code>system.p_start</code>
- to <code>Medium.p_default</code> since HVAC models may have water and
- air, which are typically at different pressures.
- </li>
- <li>
- September 19, 2008 by Michael Wetter:<br/>
- Added equations for the mass balance of extra species flow,
- i.e., <code>C</code> and <code>mC_flow</code>.
- </li>
- <li>
- April 28, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This component defines the interface for models with four fluid ports
+and two fluid streams.
+It is similar to
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>,
+but it has four ports instead of two.
+</p>
+<p>
+The model is used by other models in this package that add heat transfer,
+mass transfer and pressure drop equations.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2023, by Michael Wetter:<br/>
+Improved documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1796\">IBPSA, #1796</a>.
+</li>
+<li>
+February 3, 2022, by Michael Wetter:<br/>
+If <code>allowFlowReversal==false</code>, removed <code>noEvent()</code> declaration
+for <code>sta_a</code> and for <code>sta_b</code> because the variable is either
+already used with <code>inStream()</code> in the computation of <code>state_*_inflow</code>,
+or the result of a variable of the model that already may generate an event.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
+</li>
+<li>
+February 2, 2022, by Hongxiang Fu:<br/>
+If <code>allowFlowReversal==false</code>, replaced <code>actualStream()</code>
+with <code>inStream()</code> for <code>sta_a</code> and
+removed <code>actualStream()</code> for <code>sta_b</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
+</li>
+<li>
+March 30, 2021, by Michael Wetter:<br/>
+Added annotation <code>HideResult=true</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Moved computation of pressure drop to variable assignment so that
+the model won't mix graphical with textual modeling if used as a base
+class for a graphically implemented model.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Removed start values for mass flow rate and pressure difference
+to simplify the parameter window.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 13, 2013 by Michael Wetter:<br/>
+Removed assignment of <code>min</code> and <code>max</code>
+attributes of port mass flow rates, as this is already
+done in the base class.
+</li>
+<li>
+November 12, 2013 by Michael Wetter:<br/>
+Removed <code>import Modelica.Constants;</code> statement.
+</li>
+<li>
+November 11, 2013 by Michael Wetter:<br/>
+Removed the parameter <code>homotopyInitialization</code>
+as it is no longer used in this model.
+</li>
+<li>
+November 10, 2013 by Michael Wetter:<br/>
+In the computation of <code>sta_a1</code>,
+<code>sta_a2</code>, <code>sta_b1</code> and <code>sta_b2</code>,
+removed the branch that uses the homotopy operator.
+The rational is that these variables are conditionally enables (because
+of <code>... if show_T</code>). Therefore, the Modelica Language Specification
+does not allow for these variables to be used in any equation. Hence,
+the use of the homotopy operator is not needed here.
+</li>
+<li>
+October 10, 2013 by Michael Wetter:<br/>
+Added <code>noEvent</code> to the computation of the states at the port.
+This is correct, because the states are only used for reporting, but not
+to compute any other variable.
+Use of the states to compute other variables would violate the Modelica
+language, as conditionally removed variables must not be used in any equation.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Removed the computation of <code>V_flow</code> and removed the parameter
+<code>show_V_flow</code>.
+The reason is that the computation of <code>V_flow</code> required
+the use of <code>sta_a</code> (to compute the density),
+but <code>sta_a</code> is also a variable that is conditionally
+enabled. However, this was not correct Modelica syntax as conditional variables
+can only be used in a <code>connect</code>
+statement, not in an assignment. Dymola 2014 FD01 beta3 is checking
+for this incorrect syntax. Hence, <code>V_flow</code> was removed as its
+conditional implementation would require a rather cumbersome implementation
+that uses a new connector that carries the state of the medium.
+</li>
+<li>
+April 26, 2013 by Marco Bonvini:<br/>
+Moved the definitions of <code>dp1</code> and <code>dp2</code> because they cause some problem with PyFMI.
+</li>
+<li>
+March 27, 2012 by Michael Wetter:<br/>
+Replaced the erroneous function call <code>Medium.density</code> with
+<code>Medium1.density</code> and <code>Medium2.density</code>.
+Changed condition to remove <code>sta_a1</code> and <code>sta_a2</code> to also
+compute the states at the inlet port if <code>show_V_flow=true</code>.
+The previous implementation resulted in a translation error
+if <code>show_V_flow=true</code>, but worked correctly otherwise
+because the erroneous function call is removed if  <code>show_V_flow=false</code>.
+</li>
+<li>
+March 27, 2011 by Michael Wetter:<br/>
+Added <code>homotopy</code> operator.
+</li>
+<li>
+March 21, 2010 by Michael Wetter:<br/>
+Changed pressure start value from <code>system.p_start</code>
+to <code>Medium.p_default</code> since HVAC models may have water and
+air, which are typically at different pressures.
+</li>
+<li>
+September 19, 2008 by Michael Wetter:<br/>
+Added equations for the mass balance of extra species flow,
+i.e., <code>C</code> and <code>mC_flow</code>.
+</li>
+<li>
+April 28, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialFourPortInterface;
diff --git a/AixLib/Fluid/Interfaces/PartialFourPortParallel.mo b/AixLib/Fluid/Interfaces/PartialFourPortParallel.mo
index 8d64e8e4e8..77ee13909f 100644
--- a/AixLib/Fluid/Interfaces/PartialFourPortParallel.mo
+++ b/AixLib/Fluid/Interfaces/PartialFourPortParallel.mo
@@ -59,40 +59,40 @@ partial model PartialFourPortParallel
   annotation (
     preferredView="info",
     Documentation(info="<html>
- <p>
- This model defines an interface for components with four ports
- in which flows occur in parallel.
- The parameters <code>allowFlowReversal1</code> and <code>allowFlowReversal2</code>
- may be used by models that extend this model to treat flow reversal.
- </p>
- <p>
- This model is identical to
- <a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">Modelica.Fluid.Interfaces.PartialTwoPort</a>,
- except for the following: </p>
- <ol>
- <li>it has four ports, and </li>
- <li>the parameter <code>showDesignFlowDirection</code> is not implemented.
- </li>
- </ol>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- July 8, 2018, by Filip Jorissen:<br/>
- Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
- </li>
- <li>February 18, 2016 by Bram van der Heijde:<br/>
- First implementation, adapted from
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPort\">
- AixLib.Fluid.Interfaces.PartialFourPort</a>.
- </li>
- </ul>
- </html>"),
+<p>
+This model defines an interface for components with four ports
+in which flows occur in parallel.
+The parameters <code>allowFlowReversal1</code> and <code>allowFlowReversal2</code>
+may be used by models that extend this model to treat flow reversal.
+</p>
+<p>
+This model is identical to
+<a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">Modelica.Fluid.Interfaces.PartialTwoPort</a>,
+except for the following: </p>
+<ol>
+<li>it has four ports, and </li>
+<li>the parameter <code>showDesignFlowDirection</code> is not implemented.
+</li>
+</ol>
+</html>", revisions="<html>
+<ul>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+July 8, 2018, by Filip Jorissen:<br/>
+Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
+</li>
+<li>February 18, 2016 by Bram van der Heijde:<br/>
+First implementation, adapted from
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPort\">
+AixLib.Fluid.Interfaces.PartialFourPort</a>.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
           preserveAspectRatio=true,
           extent={{-100,-100},{100,100}},
@@ -101,6 +101,6 @@ partial model PartialFourPortParallel
           textColor={0,0,255},
           fillPattern=FillPattern.HorizontalCylinder,
           fillColor={0,127,255},
-          textString="%name")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="%name")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialFourPortParallel;
diff --git a/AixLib/Fluid/Interfaces/PartialTwoPort.mo b/AixLib/Fluid/Interfaces/PartialTwoPort.mo
index 6f3fecd40b..0233188f20 100644
--- a/AixLib/Fluid/Interfaces/PartialTwoPort.mo
+++ b/AixLib/Fluid/Interfaces/PartialTwoPort.mo
@@ -18,78 +18,90 @@ partial model PartialTwoPort "Partial component with two ports"
   Modelica.Fluid.Interfaces.FluidPort_a port_a(
     redeclare final package Medium = Medium,
      m_flow(min=if allowFlowReversal then -Modelica.Constants.inf else 0),
-     h_outflow(start = Medium.h_default, nominal = Medium.h_default))
+     h_outflow(
+       start = Medium.h_default,
+       nominal = Medium.h_default),
+     Xi_outflow(each nominal=0.01))
     "Fluid connector a (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{-110,-10},{-90,10}})));
   Modelica.Fluid.Interfaces.FluidPort_b port_b(
     redeclare final package Medium = Medium,
     m_flow(max=if allowFlowReversal then +Modelica.Constants.inf else 0),
-     h_outflow(start = Medium.h_default, nominal = Medium.h_default))
+     h_outflow(
+       start = Medium.h_default,
+       nominal = Medium.h_default),
+     Xi_outflow(each nominal=0.01))
     "Fluid connector b (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{110,-10},{90,10}})));
 
   annotation (
     Documentation(info="<html>
- <p>
- This partial model defines an interface for components with two ports.
- The treatment of the design flow direction and of flow reversal are predefined based on the parameter <code>allowFlowReversal</code>.
- The component may transport fluid and may have internal storage for a given fluid <code>Medium</code>.
- </p>
- <h4>Implementation</h4>
- <p>
- This model is similar to
- <a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">
- Modelica.Fluid.Interfaces.PartialTwoPort</a>
- but it does not use the <code>outer system</code> declaration.
- This declaration is omitted as in building energy simulation,
- many models use multiple media, an in practice,
- users have not used this global definition to assign parameters.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- July 8, 2018, by Filip Jorissen:<br/>
- Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
- </li>
- <li>
- November 19, 2015, by Michael Wetter:<br/>
- Removed parameters
- <code>port_a_exposesState</code> and
- <code>port_b_exposesState</code>
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/351\">#351</a>
- and
- <code>showDesignFlowDirection</code>
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
- </li>
- <li>
- November 13, 2015, by Michael Wetter:<br/>
- Assinged <code>start</code> attribute for leaving
- enthalpy at <code>port_a</code> and <code>port_b</code>.
- This was done to make the model similar to
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPort\">
- AixLib.Fluid.Interfaces.PartialFourPort</a>.
- </li>
- <li>
- November 12, 2015, by Michael Wetter:<br/>
- Removed import statement.
- </li>
- <li>
- October 21, 2014, by Michael Wetter:<br/>
- Revised implementation.
- Declared medium in ports to be <code>final</code>.
- </li>
- <li>
- October 20, 2014, by Filip Jorisson:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This partial model defines an interface for components with two ports.
+The treatment of the design flow direction and of flow reversal are predefined based on the parameter <code>allowFlowReversal</code>.
+The component may transport fluid and may have internal storage for a given fluid <code>Medium</code>.
+</p>
+<h4>Implementation</h4>
+<p>
+This model is similar to
+<a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">
+Modelica.Fluid.Interfaces.PartialTwoPort</a>
+but it does not use the <code>outer system</code> declaration.
+This declaration is omitted as in building energy simulation,
+many models use multiple media, an in practice,
+users have not used this global definition to assign parameters.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+July 8, 2018, by Filip Jorissen:<br/>
+Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
+</li>
+<li>
+November 19, 2015, by Michael Wetter:<br/>
+Removed parameters
+<code>port_a_exposesState</code> and
+<code>port_b_exposesState</code>
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/351\">#351</a>
+and
+<code>showDesignFlowDirection</code>
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
+</li>
+<li>
+November 13, 2015, by Michael Wetter:<br/>
+Assinged <code>start</code> attribute for leaving
+enthalpy at <code>port_a</code> and <code>port_b</code>.
+This was done to make the model similar to
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPort\">
+AixLib.Fluid.Interfaces.PartialFourPort</a>.
+</li>
+<li>
+November 12, 2015, by Michael Wetter:<br/>
+Removed import statement.
+</li>
+<li>
+October 21, 2014, by Michael Wetter:<br/>
+Revised implementation.
+Declared medium in ports to be <code>final</code>.
+</li>
+<li>
+October 20, 2014, by Filip Jorisson:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
           preserveAspectRatio=true,
           extent={{-100,-100},{100,100}}), graphics={
@@ -106,6 +118,6 @@ partial model PartialTwoPort "Partial component with two ports"
         Text(
           extent={{-149,-114},{151,-154}},
           textColor={0,0,255},
-          textString="%name")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="%name")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialTwoPort;
diff --git a/AixLib/Fluid/Interfaces/PartialTwoPortInterface.mo b/AixLib/Fluid/Interfaces/PartialTwoPortInterface.mo
index 0d032b82ac..70a521c2c4 100644
--- a/AixLib/Fluid/Interfaces/PartialTwoPortInterface.mo
+++ b/AixLib/Fluid/Interfaces/PartialTwoPortInterface.mo
@@ -1,6 +1,6 @@
 within AixLib.Fluid.Interfaces;
 partial model PartialTwoPortInterface
-  "Partial model transporting fluid between two ports without storing mass or energy"
+  "Partial model with two ports and declaration of quantities that are used by many models"
   extends AixLib.Fluid.Interfaces.PartialTwoPort(
     port_a(p(start=Medium.p_default)),
     port_b(p(start=Medium.p_default)));
@@ -57,146 +57,159 @@ protected
   annotation (
     preferredView="info",
     Documentation(info="<html>
- <p>
- This component defines the interface for models that
- transports a fluid between two ports. It is similar to
- <a href=\"Modelica://Modelica.Fluid.Interfaces.PartialTwoPortTransport\">
- Modelica.Fluid.Interfaces.PartialTwoPortTransport</a>, but it does not
- include the species balance
- </p>
- <pre>
-   port_b.Xi_outflow = inStream(port_a.Xi_outflow);
- </pre>
- <p>
- Thus, it can be used as a base class for a heat <i>and</i> mass transfer component
- </p>
- <p>
- The model is used by other models in this package that add heat transfer,
- mass transfer and pressure drop equations. See for example
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
- AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Hongxiang Fu:<br/>
- If <code>allowFlowReversal==false</code>, replaced <code>actualStream()</code>
- with <code>inStream()</code> for <code>sta_a</code> and
- removed <code>actualStream()</code> for <code>sta_b</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
- </li>
- <li>
- March 30, 2021, by Michael Wetter:<br/>
- Added annotation <code>HideResult=true</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Renamed protected parameter <code>m_flow_start</code> to avoid
- a name clash with
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
- AixLib.Fluid.Movers.FlowControlled_m_flow</a>
- which leads to an error as the definition were different,
- and also renamed protected parameter <code>dp_start</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>
- <br/>
- Moved computation of pressure drop to variable assignment so that
- the model won't mix graphical with textual modeling if used as a base
- class for a graphically implemented model.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Removed start values for mass flow rate and pressure difference
- to simplify the parameter window.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- October 3, 2014, by Michael Wetter:<br/>
- Changed assignment of nominal value to avoid in OpenModelica the warning
- alias set with different nominal values.
- </li>
- <li>
- November 12, 2013 by Michael Wetter:<br/>
- Removed <code>import Modelica.Constants;</code> statement.
- </li>
- <li>
- November 11, 2013 by Michael Wetter:<br/>
- Removed the parameter <code>homotopyInitialization</code>
- as it is no longer used in this model.
- </li>
- <li>
- November 10, 2013 by Michael Wetter:<br/>
- In the computation of <code>sta_a</code> and <code>sta_b</code>,
- removed the branch that uses the homotopy operator.
- The rational is that these variables are conditionally enables (because
- of <code>... if show_T</code>). Therefore, the Modelica Language Specification
- does not allow for these variables to be used in any equation. Hence,
- the use of the homotopy operator is not needed here.
- </li>
- <li>
- October 10, 2013 by Michael Wetter:<br/>
- Added <code>noEvent</code> to the computation of the states at the port.
- This is correct, because the states are only used for reporting, but not
- to compute any other variable.
- Use of the states to compute other variables would violate the Modelica
- language, as conditionally removed variables must not be used in any equation.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Removed the computation of <code>V_flow</code> and removed the parameter
- <code>show_V_flow</code>.
- The reason is that the computation of <code>V_flow</code> required
- the use of <code>sta_a</code> (to compute the density),
- but <code>sta_a</code> is also a variable that is conditionally
- enabled. However, this was not correct Modelica syntax as conditional variables
- can only be used in a <code>connect</code>
- statement, not in an assignment. Dymola 2014 FD01 beta3 is checking
- for this incorrect syntax. Hence, <code>V_flow</code> was removed as its
- conditional implementation would require a rather cumbersome implementation
- that uses a new connector that carries the state of the medium.
- </li>
- <li>
- April 26, 2013 by Marco Bonvini:<br/>
- Moved the definition of <code>dp</code> because it causes some problem with PyFMI.
- </li>
- <li>
- March 27, 2012 by Michael Wetter:<br/>
- Changed condition to remove <code>sta_a</code> to also
- compute the state at the inlet port if <code>show_V_flow=true</code>.
- The previous implementation resulted in a translation error
- if <code>show_V_flow=true</code>, but worked correctly otherwise
- because the erroneous function call is removed if  <code>show_V_flow=false</code>.
- </li>
- <li>
- March 27, 2011 by Michael Wetter:<br/>
- Added <code>homotopy</code> operator.
- </li>
- <li>
- March 21, 2010 by Michael Wetter:<br/>
- Changed pressure start value from <code>system.p_start</code>
- to <code>Medium.p_default</code> since HVAC models may have water and
- air, which are typically at different pressures.
- </li>
- <li>
- September 19, 2008 by Michael Wetter:<br/>
- Added equations for the mass balance of extra species flow,
- i.e., <code>C</code> and <code>mC_flow</code>.
- </li>
- <li>
- March 11, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This component defines the interface for models with two fluid ports.
+It is similar to
+<a href=\"Modelica://Modelica.Fluid.Interfaces.PartialTwoPortTransport\">
+Modelica.Fluid.Interfaces.PartialTwoPortTransport</a>, but it does not
+include the species balance
+</p>
+<pre>
+  port_b.Xi_outflow = inStream(port_a.Xi_outflow);
+</pre>
+<p>
+Thus, it can be used as a base class for a heat <i>and</i> mass transfer component
+</p>
+<p>
+The partial model extends
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPort\">
+AixLib.Fluid.Interfaces.PartialTwoPort</a>
+and adds quantities that are used by many models such as
+<code>m_flow_nominal</code>, <code>m_flow</code> and <code>dp</code>.
+</p>
+<p>
+The model is used by other models in this package that add heat transfer,
+mass transfer and pressure drop equations. See for example
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
+AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2023, by Michael Wetter:<br/>
+Improved documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1796\">IBPSA, #1796</a>.
+</li>
+<li>
+February 2, 2022, by Hongxiang Fu:<br/>
+If <code>allowFlowReversal==false</code>, replaced <code>actualStream()</code>
+with <code>inStream()</code> for <code>sta_a</code> and
+removed <code>actualStream()</code> for <code>sta_b</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1578\">IBPSA, #1578</a>.
+</li>
+<li>
+March 30, 2021, by Michael Wetter:<br/>
+Added annotation <code>HideResult=true</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Renamed protected parameter <code>m_flow_start</code> to avoid
+a name clash with
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.FlowControlled_m_flow</a>
+which leads to an error as the definition were different,
+and also renamed protected parameter <code>dp_start</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>
+<br/>
+Moved computation of pressure drop to variable assignment so that
+the model won't mix graphical with textual modeling if used as a base
+class for a graphically implemented model.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Removed start values for mass flow rate and pressure difference
+to simplify the parameter window.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/552\">#552</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+October 3, 2014, by Michael Wetter:<br/>
+Changed assignment of nominal value to avoid in OpenModelica the warning
+alias set with different nominal values.
+</li>
+<li>
+November 12, 2013 by Michael Wetter:<br/>
+Removed <code>import Modelica.Constants;</code> statement.
+</li>
+<li>
+November 11, 2013 by Michael Wetter:<br/>
+Removed the parameter <code>homotopyInitialization</code>
+as it is no longer used in this model.
+</li>
+<li>
+November 10, 2013 by Michael Wetter:<br/>
+In the computation of <code>sta_a</code> and <code>sta_b</code>,
+removed the branch that uses the homotopy operator.
+The rational is that these variables are conditionally enables (because
+of <code>... if show_T</code>). Therefore, the Modelica Language Specification
+does not allow for these variables to be used in any equation. Hence,
+the use of the homotopy operator is not needed here.
+</li>
+<li>
+October 10, 2013 by Michael Wetter:<br/>
+Added <code>noEvent</code> to the computation of the states at the port.
+This is correct, because the states are only used for reporting, but not
+to compute any other variable.
+Use of the states to compute other variables would violate the Modelica
+language, as conditionally removed variables must not be used in any equation.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Removed the computation of <code>V_flow</code> and removed the parameter
+<code>show_V_flow</code>.
+The reason is that the computation of <code>V_flow</code> required
+the use of <code>sta_a</code> (to compute the density),
+but <code>sta_a</code> is also a variable that is conditionally
+enabled. However, this was not correct Modelica syntax as conditional variables
+can only be used in a <code>connect</code>
+statement, not in an assignment. Dymola 2014 FD01 beta3 is checking
+for this incorrect syntax. Hence, <code>V_flow</code> was removed as its
+conditional implementation would require a rather cumbersome implementation
+that uses a new connector that carries the state of the medium.
+</li>
+<li>
+April 26, 2013 by Marco Bonvini:<br/>
+Moved the definition of <code>dp</code> because it causes some problem with PyFMI.
+</li>
+<li>
+March 27, 2012 by Michael Wetter:<br/>
+Changed condition to remove <code>sta_a</code> to also
+compute the state at the inlet port if <code>show_V_flow=true</code>.
+The previous implementation resulted in a translation error
+if <code>show_V_flow=true</code>, but worked correctly otherwise
+because the erroneous function call is removed if  <code>show_V_flow=false</code>.
+</li>
+<li>
+March 27, 2011 by Michael Wetter:<br/>
+Added <code>homotopy</code> operator.
+</li>
+<li>
+March 21, 2010 by Michael Wetter:<br/>
+Changed pressure start value from <code>system.p_start</code>
+to <code>Medium.p_default</code> since HVAC models may have water and
+air, which are typically at different pressures.
+</li>
+<li>
+September 19, 2008 by Michael Wetter:<br/>
+Added equations for the mass balance of extra species flow,
+i.e., <code>C</code> and <code>mC_flow</code>.
+</li>
+<li>
+March 11, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialTwoPortInterface;
diff --git a/AixLib/Fluid/Interfaces/PartialTwoPortTransport.mo b/AixLib/Fluid/Interfaces/PartialTwoPortTransport.mo
index 80ddcbf5d2..79a8910ff5 100644
--- a/AixLib/Fluid/Interfaces/PartialTwoPortTransport.mo
+++ b/AixLib/Fluid/Interfaces/PartialTwoPortTransport.mo
@@ -92,95 +92,95 @@ equation
 
   annotation (
     Documentation(info="<html>
- <p>
- This component transports fluid between its two ports, without storing mass or energy.
- Energy may be exchanged with the environment though, e.g., in the form of work.
- <code>PartialTwoPortTransport</code> is intended as base class for devices like orifices, valves and simple fluid machines.</p>
- <p>
- Three equations need to be added by an extending class using this component:
- </p>
- <ul>
- <li>The momentum balance specifying the relationship between the pressure drop <code>dp</code> and the mass flow rate <code>m_flow</code>,</li>
- <li><code>port_b.h_outflow</code> for flow in design direction, and</li>
- <li><code>port_a.h_outflow</code> for flow in reverse direction.</li>
- </ul>
- <p>
- Moreover appropriate values shall be assigned to the following parameters:
- </p>
- <ul>
- <li><code>dp_start</code> for a guess of the pressure drop</li>
- <li><code>m_flow_small</code> for regularization of zero flow.</li>
- </ul>
- <h4>Implementation</h4>
- <p>
- This is similar to
- <a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPortTransport\">
- Modelica.Fluid.Interfaces.PartialTwoPortTransport</a>
- except that it does not use the <code>outer system</code> declaration.
- This declaration is omitted as in building energy simulation,
- many models use multiple media, an in practice,
- users have not used this global definition to assign parameters.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 30, 2021, by Michael Wetter:<br/>
- Added annotation <code>HideResult=true</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
- </li>
- <li>
- September 15, 2016, by Michael Wetter:<br/>
- Removed wrong annotation, which caused an error in the pedantic model check
- of Dymola 2017 FD01.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/516\">#516</a>.
- </li>
- <li>
- January 22, 2016, by Henning Francke:<br/>
- Corrected type declaration of pressure.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 19, 2015, by Michael Wetter:<br/>
- Removed assignments of parameters
- <code>port_a_exposesState</code> and
- <code>port_b_exposesState</code> in base class.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/351\">#351</a>.
- </li>
- <li>
- August 15, 2015, by Filip Jorissen:<br/>
- Implemented more efficient computation of <code>port_a.Xi_outflow</code>
- and <code>port_a.C_outflow</code> when <code>allowFlowReversal=false</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/305\">#305</a>.
- </li>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Removed protected conditional variables <code>state_a</code> and <code>state_b</code>,
- as they were used outside of a connect statement, which causes an
- error during pedantic model check in Dymola 2016.
- This fixes
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/128\">#128</a>.
- </li>
- <li>
- April 1, 2015, by Michael Wetter:<br/>
- Made computation of <code>state_a</code> and <code>state_p</code>
- conditional on <code>show_T</code> or <code>show_V_flow</code>.
- This avoids computing temperature from enthalpy if temperature is
- a state of the medium, and the result is not used.
- </li>
- <li>
- October 21, 2014, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- <li>
- October 20, 2014, by Filip Jorisson:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This component transports fluid between its two ports, without storing mass or energy.
+Energy may be exchanged with the environment though, e.g., in the form of work.
+<code>PartialTwoPortTransport</code> is intended as base class for devices like orifices, valves and simple fluid machines.</p>
+<p>
+Three equations need to be added by an extending class using this component:
+</p>
+<ul>
+<li>The momentum balance specifying the relationship between the pressure drop <code>dp</code> and the mass flow rate <code>m_flow</code>,</li>
+<li><code>port_b.h_outflow</code> for flow in design direction, and</li>
+<li><code>port_a.h_outflow</code> for flow in reverse direction.</li>
+</ul>
+<p>
+Moreover appropriate values shall be assigned to the following parameters:
+</p>
+<ul>
+<li><code>dp_start</code> for a guess of the pressure drop</li>
+<li><code>m_flow_small</code> for regularization of zero flow.</li>
+</ul>
+<h4>Implementation</h4>
+<p>
+This is similar to
+<a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPortTransport\">
+Modelica.Fluid.Interfaces.PartialTwoPortTransport</a>
+except that it does not use the <code>outer system</code> declaration.
+This declaration is omitted as in building energy simulation,
+many models use multiple media, and in practice,
+users have not used this global definition to assign parameters.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 30, 2021, by Michael Wetter:<br/>
+Added annotation <code>HideResult=true</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
+</li>
+<li>
+September 15, 2016, by Michael Wetter:<br/>
+Removed wrong annotation, which caused an error in the pedantic model check
+of Dymola 2017 FD01.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/516\">#516</a>.
+</li>
+<li>
+January 22, 2016, by Henning Francke:<br/>
+Corrected type declaration of pressure.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 19, 2015, by Michael Wetter:<br/>
+Removed assignments of parameters
+<code>port_a_exposesState</code> and
+<code>port_b_exposesState</code> in base class.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/351\">#351</a>.
+</li>
+<li>
+August 15, 2015, by Filip Jorissen:<br/>
+Implemented more efficient computation of <code>port_a.Xi_outflow</code>
+and <code>port_a.C_outflow</code> when <code>allowFlowReversal=false</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/305\">#305</a>.
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Removed protected conditional variables <code>state_a</code> and <code>state_b</code>,
+as they were used outside of a connect statement, which causes an
+error during pedantic model check in Dymola 2016.
+This fixes
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/128\">#128</a>.
+</li>
+<li>
+April 1, 2015, by Michael Wetter:<br/>
+Made computation of <code>state_a</code> and <code>state_p</code>
+conditional on <code>show_T</code> or <code>show_V_flow</code>.
+This avoids computing temperature from enthalpy if temperature is
+a state of the medium, and the result is not used.
+</li>
+<li>
+October 21, 2014, by Michael Wetter:<br/>
+Revised implementation.
+</li>
+<li>
+October 20, 2014, by Filip Jorisson:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialTwoPortTransport;
diff --git a/AixLib/Fluid/Interfaces/PartialTwoPortVector.mo b/AixLib/Fluid/Interfaces/PartialTwoPortVector.mo
index 06fa0c526a..ba08ed752c 100644
--- a/AixLib/Fluid/Interfaces/PartialTwoPortVector.mo
+++ b/AixLib/Fluid/Interfaces/PartialTwoPortVector.mo
@@ -51,81 +51,81 @@ partial model PartialTwoPortVector "Partial component with two ports, one of whi
       if show_T "Medium properties in ports_b";
   annotation (
     Documentation(info="<html>
- <p>
- This partial model defines an interface for components with two ports,
- of which one is vectorized.
- </p>
- <p>
- The treatment of the design flow direction and of flow reversal are
- determined based on the parameter <code>allowFlowReversal</code>.
- The component may transport fluid and may have internal storage.
- </p>
- <h4>Implementation</h4>
- <p>
- This model is similar to
- <a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">
- Modelica.Fluid.Interfaces.PartialTwoPort</a>
- but it does not use the <code>outer system</code> declaration.
- This declaration is omitted as in building energy simulation,
- many models use multiple media, and in practice,
- users have not used this global definition to assign parameters.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 30, 2021, by Michael Wetter:<br/>
- Added annotation <code>HideResult=true</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
- </li>
- <li>
- January 31, 2019, by Michael Mans:<br/>
- Added optional temperature state calculation as diagnostics option.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1092\">#1092</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- July 8, 2018, by Filip Jorissen:<br/>
- Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
- </li>
- <li>
- November 19, 2015, by Michael Wetter:<br/>
- Removed parameters
- <code>port_a_exposesState</code> and
- <code>port_b_exposesState</code>
- for <a href=\"https://github.com/ibpsa/modelica/issues/351\">#351</a>
- and
- <code>showDesignFlowDirection</code>
- for <a href=\"https://github.com/ibpsa/modelica/issues/349\">#349</a>.
- </li>
- <li>
- November 13, 2015, by Michael Wetter:<br/>
- Assinged <code>start</code> attribute for leaving
- enthalpy at <code>port_a</code> and <code>port_b</code>.
- This was done to make the model similar to
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPort\">
- AixLib.Fluid.Interfaces.PartialFourPort</a>.
- </li>
- <li>
- November 12, 2015, by Michael Wetter:<br/>
- Removed import statement.
- </li>
- <li>
- October 21, 2014, by Michael Wetter:<br/>
- Revised implementation.
- Declared medium in ports to be <code>final</code>.
- </li>
- <li>
- October 20, 2014, by Filip Jorisson:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This partial model defines an interface for components with two ports,
+of which one is vectorized.
+</p>
+<p>
+The treatment of the design flow direction and of flow reversal are
+determined based on the parameter <code>allowFlowReversal</code>.
+The component may transport fluid and may have internal storage.
+</p>
+<h4>Implementation</h4>
+<p>
+This model is similar to
+<a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPort\">
+Modelica.Fluid.Interfaces.PartialTwoPort</a>
+but it does not use the <code>outer system</code> declaration.
+This declaration is omitted as in building energy simulation,
+many models use multiple media, and in practice,
+users have not used this global definition to assign parameters.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 30, 2021, by Michael Wetter:<br/>
+Added annotation <code>HideResult=true</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1459\">IBPSA, #1459</a>.
+</li>
+<li>
+January 31, 2019, by Michael Mans:<br/>
+Added optional temperature state calculation as diagnostics option.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1092\">#1092</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+July 8, 2018, by Filip Jorissen:<br/>
+Added nominal value of <code>h_outflow</code> in <code>FluidPorts</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/977\">#977</a>.
+</li>
+<li>
+November 19, 2015, by Michael Wetter:<br/>
+Removed parameters
+<code>port_a_exposesState</code> and
+<code>port_b_exposesState</code>
+for <a href=\"https://github.com/ibpsa/modelica/issues/351\">#351</a>
+and
+<code>showDesignFlowDirection</code>
+for <a href=\"https://github.com/ibpsa/modelica/issues/349\">#349</a>.
+</li>
+<li>
+November 13, 2015, by Michael Wetter:<br/>
+Assinged <code>start</code> attribute for leaving
+enthalpy at <code>port_a</code> and <code>port_b</code>.
+This was done to make the model similar to
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialFourPort\">
+AixLib.Fluid.Interfaces.PartialFourPort</a>.
+</li>
+<li>
+November 12, 2015, by Michael Wetter:<br/>
+Removed import statement.
+</li>
+<li>
+October 21, 2014, by Michael Wetter:<br/>
+Revised implementation.
+Declared medium in ports to be <code>final</code>.
+</li>
+<li>
+October 20, 2014, by Filip Jorisson:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{100,100}}),
         graphics={
         Polygon(
@@ -143,6 +143,6 @@ partial model PartialTwoPortVector "Partial component with two ports, one of whi
           textColor={0,0,255},
           textString="%name")}),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
-            100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialTwoPortVector;
diff --git a/AixLib/Fluid/Interfaces/PrescribedOutlet.mo b/AixLib/Fluid/Interfaces/PrescribedOutlet.mo
index 5e8ffe726b..6c72559a09 100644
--- a/AixLib/Fluid/Interfaces/PrescribedOutlet.mo
+++ b/AixLib/Fluid/Interfaces/PrescribedOutlet.mo
@@ -151,8 +151,8 @@ initial equation
   assert((energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState) or
           tau > Modelica.Constants.eps,
 "The parameter tau, or the volume of the model from which tau may be derived, is unreasonably small.
-  You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
-  Received tau = "+ String(tau) + "\n");
+ You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
+ Received tau = " + String(tau) + "\n");
 
  if use_X_wSet then
   assert(Medium.nX > 1, "If use_X_wSet = true, require a medium with water vapor, such as AixLib.Media.Air");
@@ -409,81 +409,81 @@ equation
           fillColor={0,0,127},
           fillPattern=FillPattern.Solid)}),
   Documentation(info="<html>
- <p>
- This model sets the temperature or the water vapor mass fraction
- of the medium that leaves <code>port_a</code>
- to the value given by the input <code>TSet</code> or <code>X_wSet</code>,
- subject to optional limitations on the capacity
- for heating and cooling, or limitations on the humidification or dehumidification
- moisture mass flow rate.
- Also, optionally the model allows to take into account first order dynamics.
- </p>
- <p>
- If the parameters <code>energyDynamics</code> is not equal to
- <code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
- the component models the dynamic response using a first order differential equation.
- The time constant of the component is equal to the parameter <code>tau</code>.
- This time constant is adjusted based on the mass flow rate using
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
- </p>
- <p>
- where
- <i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
- <i>m&#775;</i> and
- <i>&tau;</i> is the time constant at the nominal mass flow rate
- <i>m&#775;<sub>nom</sub></i>.
- This type of dynamics is equal to the dynamics that a completely mixed
- control volume would have.
- </p>
- <p>
- This model has no pressure drop.
- See <a href=\"modelica://AixLib.Fluid.HeatExchangers.PrescribedOutlet\">
- AixLib.Fluid.HeatExchangers.PrescribedOutlet</a>
- for a model that instantiates this model and that has a pressure drop.
- </p>
- <p>
- In case of reverse flow,
- the fluid that leaves <code>port_a</code> has the same
- properties as the fluid that enters <code>port_b</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 3, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
- </li>
- <li>
- April 29, 2021, by Michael Wetter:<br/>
- Removed duplicate declaration of <code>m_flow_nominal</code> which is already
- declared in the base class.<br/>
- </li>
- <li>
- March 19, 2018, by Michael Wetter:<br/>
- Added bugfix as the old model did not track <code>TSet</code> and <code>X_wSet</code>
- simultaneously.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/893\">#893</a>.
- </li>
- <li>
- May 3, 2017, by Michael Wetter:<br/>
- Refactored model to allow <code>X_wSet</code> as an input.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Removed inequality comparison of real numbers in <code>restrictCool</code>
- and in <code>restrictHeat</code> as this is not allowed in Modelica.
- </li>
- <li>
- November 10, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model sets the temperature or the water vapor mass fraction
+of the medium that leaves <code>port_a</code>
+to the value given by the input <code>TSet</code> or <code>X_wSet</code>,
+subject to optional limitations on the capacity
+for heating and cooling, or limitations on the humidification or dehumidification
+moisture mass flow rate.
+Also, optionally the model allows to take into account first order dynamics.
+</p>
+<p>
+If the parameters <code>energyDynamics</code> is not equal to
+<code>Modelica.Fluid.Types.Dynamics.SteadyState</code>,
+the component models the dynamic response using a first order differential equation.
+The time constant of the component is equal to the parameter <code>tau</code>.
+This time constant is adjusted based on the mass flow rate using
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&tau;<sub>eff</sub> = &tau; |m&#775;| &frasl; m&#775;<sub>nom</sub>
+</p>
+<p>
+where
+<i>&tau;<sub>eff</sub></i> is the effective time constant for the given mass flow rate
+<i>m&#775;</i> and
+<i>&tau;</i> is the time constant at the nominal mass flow rate
+<i>m&#775;<sub>nom</sub></i>.
+This type of dynamics is equal to the dynamics that a completely mixed
+control volume would have.
+</p>
+<p>
+This model has no pressure drop.
+See <a href=\"modelica://AixLib.Fluid.HeatExchangers.PrescribedOutlet\">
+AixLib.Fluid.HeatExchangers.PrescribedOutlet</a>
+for a model that instantiates this model and that has a pressure drop.
+</p>
+<p>
+In case of reverse flow,
+the fluid that leaves <code>port_a</code> has the same
+properties as the fluid that enters <code>port_b</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 3, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
+</li>
+<li>
+April 29, 2021, by Michael Wetter:<br/>
+Removed duplicate declaration of <code>m_flow_nominal</code> which is already
+declared in the base class.<br/>
+</li>
+<li>
+March 19, 2018, by Michael Wetter:<br/>
+Added bugfix as the old model did not track <code>TSet</code> and <code>X_wSet</code>
+simultaneously.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/893\">#893</a>.
+</li>
+<li>
+May 3, 2017, by Michael Wetter:<br/>
+Refactored model to allow <code>X_wSet</code> as an input.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/763\">#763</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Removed inequality comparison of real numbers in <code>restrictCool</code>
+and in <code>restrictHeat</code> as this is not allowed in Modelica.
+</li>
+<li>
+November 10, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PrescribedOutlet;
diff --git a/AixLib/Fluid/Interfaces/StaticFourPortHeatMassExchanger.mo b/AixLib/Fluid/Interfaces/StaticFourPortHeatMassExchanger.mo
index 80068b4c14..66b1d14835 100644
--- a/AixLib/Fluid/Interfaces/StaticFourPortHeatMassExchanger.mo
+++ b/AixLib/Fluid/Interfaces/StaticFourPortHeatMassExchanger.mo
@@ -74,131 +74,131 @@ equation
   annotation (
     preferredView="info",
     Documentation(info="<html>
- <p>
- This component transports two fluid streams between four ports, without
- storing mass or energy. It is similar to
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
- AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>,
- but it has four ports instead of two.
- </p>
- <p>
- If <code>dp<i>N</i>_nominal &gt; Modelica.Constants.eps</code>,
- where <code><i>N</i></code> denotes the fluid <i>1</i> or <i>2</i>,
- then the model computes
- pressure drop due to flow friction in the respective fluid stream.
- The pressure drop is defined by a quadratic function that goes through
- the point <code>(m<i>N</i>_flow_nominal, dp<i>N</i>_nominal)</code>.
- At <code>|m<i>N</i>_flow| &lt; deltaM<i>N</i> * m<i>N</i>_flow_nominal</code>,
- the pressure drop vs. flow relation is linearized.
- If the parameter <code>linearizeFlowResistance<i>N</i></code> is set to true,
- then the whole pressure drop vs. flow resistance curve is linearized.
- </p>
- 
- <h4>Implementation</h4>
- <p>
- This model uses inputs and constants that need to be set by models
- that extend or instantiate this model.
- The following inputs need to be assigned, where <code><i>N</i></code> denotes <code>1</code> or
- <code>2</code>:</p>
- <ul>
- <li>
- <code>Q<i>N</i>_flow</code>, which is the sensible and latent heat flow rate added to the medium <i>N</i>.
- </li>
- <li>
- <code>mWat<i>N</i>_flow</code>, which is the moisture mass flow rate added to the medium <i>N</i>.
- </li>
- </ul>
- <p>
- Set the constant <code>sensibleOnly<i>N</i>=true</code> if the model that extends
- or instantiates this model sets <code>mWat<i>N</i>_flow = 0</code>.
- </p>
- <p>
-      Note that the model does not implement <code>0 = Q1_flow + Q2_flow</code> or
-      <code>0 = mXi1_flow + mXi2_flow</code>. If there is no heat or mass transfer
-      with the environment, then a model that extends this model needs to provide these
-      equations.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- April 11, 2017, by Michael Wetter:<br/>
- Updated documentation to make clear that <code>Q1_flow</code> and <code>Q2_flow</code>
- include latent heat flow rate.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- January 22, 2016 by Michael Wetter:<br/>
- Removed assignment of <code>sensibleOnly</code> in <code>bal1</code> and <code>bal2</code>
- as this constant has been removed in
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
- AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>.
- </li>
- <li>
- November 13, 2013 by Michael Wetter:<br/>
- Added parameter <code>homotopyInitialization</code> as
- it has been removed in the base class.
- </li>
- <li>
- November 13, 2013, by Michael Wetter:<br/>
- Removed <code>import Modelica.Constants;</code> statement.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Removed parameter <code>show_V_flow</code>.
- </li>
- <li>
- July 30, 2013 by Michael Wetter:<br/>
- Changed connector <code>mXi_flow[Medium.nXi]</code>
- to a scalar input connector <code>mWat_flow</code>.
- The reason is that <code>mXi_flow</code> does not allow
- to compute the other components in <code>mX_flow</code> and
- therefore leads to an ambiguous use of the model.
- By only requesting <code>mWat_flow</code>, the mass balance
- and species balance can be implemented correctly.
- </li>
- <li>
- March 29, 2011, by Michael Wetter:<br/>
- Changed energy and mass balance to avoid a division by zero if <code>m_flow=0</code>.
- </li>
- <li>
- March 27, 2011, by Michael Wetter:<br/>
- Added <code>homotopy</code> operator.
- </li>
- <li>
- August 19, 2010, by Michael Wetter:<br/>
- Fixed bug in energy and moisture balance that affected results if a component
- adds or removes moisture to the air stream.
- In the old implementation, the enthalpy and species
- outflow at <code>port_b</code> was multiplied with the mass flow rate at
- <code>port_a</code>. The old implementation led to small errors that were proportional
- to the amount of moisture change. For example, if the moisture added by the component
- was <code>0.005 kg/kg</code>, then the error was <code>0.5%</code>.
- Also, the results for forward flow and reverse flow differed by this amount.
- With the new implementation, the energy and moisture balance is exact.
- </li>
- <li>
- March 22, 2010, by Michael Wetter:<br/>
- Added constants <code>sensibleOnly1</code> and
- <code>sensibleOnly2</code> to
- simplify species balance equations.
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- Added model to compute flow friction.
- </li>
- <li>
- March 25, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component transports two fluid streams between four ports, without
+storing mass or energy. It is similar to
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
+AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>,
+but it has four ports instead of two.
+</p>
+<p>
+If <code>dp<i>N</i>_nominal &gt; Modelica.Constants.eps</code>,
+where <code><i>N</i></code> denotes the fluid <i>1</i> or <i>2</i>,
+then the model computes
+pressure drop due to flow friction in the respective fluid stream.
+The pressure drop is defined by a quadratic function that goes through
+the point <code>(m<i>N</i>_flow_nominal, dp<i>N</i>_nominal)</code>.
+At <code>|m<i>N</i>_flow| &lt; deltaM<i>N</i> * m<i>N</i>_flow_nominal</code>,
+the pressure drop vs. flow relation is linearized.
+If the parameter <code>linearizeFlowResistance<i>N</i></code> is set to true,
+then the whole pressure drop vs. flow resistance curve is linearized.
+</p>
+
+<h4>Implementation</h4>
+<p>
+This model uses inputs and constants that need to be set by models
+that extend or instantiate this model.
+The following inputs need to be assigned, where <code><i>N</i></code> denotes <code>1</code> or
+<code>2</code>:</p>
+<ul>
+<li>
+<code>Q<i>N</i>_flow</code>, which is the sensible and latent heat flow rate added to the medium <i>N</i>.
+</li>
+<li>
+<code>mWat<i>N</i>_flow</code>, which is the moisture mass flow rate added to the medium <i>N</i>.
+</li>
+</ul>
+<p>
+Set the constant <code>sensibleOnly<i>N</i>=true</code> if the model that extends
+or instantiates this model sets <code>mWat<i>N</i>_flow = 0</code>.
+</p>
+<p>
+     Note that the model does not implement <code>0 = Q1_flow + Q2_flow</code> or
+     <code>0 = mXi1_flow + mXi2_flow</code>. If there is no heat or mass transfer
+     with the environment, then a model that extends this model needs to provide these
+     equations.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+April 11, 2017, by Michael Wetter:<br/>
+Updated documentation to make clear that <code>Q1_flow</code> and <code>Q2_flow</code>
+include latent heat flow rate.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+January 22, 2016 by Michael Wetter:<br/>
+Removed assignment of <code>sensibleOnly</code> in <code>bal1</code> and <code>bal2</code>
+as this constant has been removed in
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
+AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>.
+</li>
+<li>
+November 13, 2013 by Michael Wetter:<br/>
+Added parameter <code>homotopyInitialization</code> as
+it has been removed in the base class.
+</li>
+<li>
+November 13, 2013, by Michael Wetter:<br/>
+Removed <code>import Modelica.Constants;</code> statement.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Removed parameter <code>show_V_flow</code>.
+</li>
+<li>
+July 30, 2013 by Michael Wetter:<br/>
+Changed connector <code>mXi_flow[Medium.nXi]</code>
+to a scalar input connector <code>mWat_flow</code>.
+The reason is that <code>mXi_flow</code> does not allow
+to compute the other components in <code>mX_flow</code> and
+therefore leads to an ambiguous use of the model.
+By only requesting <code>mWat_flow</code>, the mass balance
+and species balance can be implemented correctly.
+</li>
+<li>
+March 29, 2011, by Michael Wetter:<br/>
+Changed energy and mass balance to avoid a division by zero if <code>m_flow=0</code>.
+</li>
+<li>
+March 27, 2011, by Michael Wetter:<br/>
+Added <code>homotopy</code> operator.
+</li>
+<li>
+August 19, 2010, by Michael Wetter:<br/>
+Fixed bug in energy and moisture balance that affected results if a component
+adds or removes moisture to the air stream.
+In the old implementation, the enthalpy and species
+outflow at <code>port_b</code> was multiplied with the mass flow rate at
+<code>port_a</code>. The old implementation led to small errors that were proportional
+to the amount of moisture change. For example, if the moisture added by the component
+was <code>0.005 kg/kg</code>, then the error was <code>0.5%</code>.
+Also, the results for forward flow and reverse flow differed by this amount.
+With the new implementation, the energy and moisture balance is exact.
+</li>
+<li>
+March 22, 2010, by Michael Wetter:<br/>
+Added constants <code>sensibleOnly1</code> and
+<code>sensibleOnly2</code> to
+simplify species balance equations.
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+Added model to compute flow friction.
+</li>
+<li>
+March 25, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
         preserveAspectRatio=false,
         extent={{-100,-100},{100,100}},
@@ -220,6 +220,6 @@ equation
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,0},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end StaticFourPortHeatMassExchanger;
diff --git a/AixLib/Fluid/Interfaces/StaticTwoPortConservationEquation.mo b/AixLib/Fluid/Interfaces/StaticTwoPortConservationEquation.mo
index c9c3f5e94a..83d14d5e66 100644
--- a/AixLib/Fluid/Interfaces/StaticTwoPortConservationEquation.mo
+++ b/AixLib/Fluid/Interfaces/StaticTwoPortConservationEquation.mo
@@ -40,7 +40,8 @@ model StaticTwoPortConservationEquation
 
   Modelica.Blocks.Interfaces.RealOutput XiOut[Medium.nXi](each unit="1",
                                                           each min=0,
-                                                          each max=1)
+                                                          each max=1,
+                                                          nominal=0.01*ones(Medium.nXi))
     "Leaving species concentration of the component"
     annotation (Placement(transformation(extent={{-10,-10},{10,10}},
         rotation=90,
@@ -107,11 +108,12 @@ protected
     "Needed to connect to conditional connector";
 initial equation
   // Assert that the substance with name 'water' has been found.
-  assert(Medium.nXi == 0 or abs(sum(s)-1) < 1e-5,
+  if use_mWat_flow then
+    assert(Medium.nXi == 0 or abs(sum(s)-1) < 1e-5,
       "If Medium.nXi > 1, then substance 'water' must be present for one component.'"
          + Medium.mediumName + "'.\n"
          + "Check medium model.");
-
+  end if;
 equation
   // Conditional connectors
   connect(mWat_flow, mWat_flow_internal);
@@ -143,13 +145,13 @@ equation
   if prescribedHeatFlowRate then
     assert(noEvent( abs(Q_flow) < dTMax*cp_default*max(m_flow_small/1E3, abs(m_flow))),
    "In " + getInstanceName() + ":
-    The heat flow rate equals "+ String(Q_flow) +
+   The heat flow rate equals " + String(Q_flow) +
    " W and the mass flow rate equals " + String(m_flow) + " kg/s,
-    which results in a temperature difference "+
+   which results in a temperature difference " +
    String(abs(Q_flow)/ (cp_default*max(m_flow_small/1E3, abs(m_flow)))) +
    " K > dTMax=" +String(dTMax) + " K.
-    This may indicate that energy is not conserved for small mass flow rates.
-    The implementation may require prescribedHeatFlowRate = false.");
+   This may indicate that energy is not conserved for small mass flow rates.
+   The implementation may require prescribedHeatFlowRate = false.");
   end if;
 
   if allowFlowReversal then
@@ -251,339 +253,350 @@ equation
   annotation (
     preferredView="info",
     Documentation(info="<html>
- <p>
- This model transports fluid between its two ports, without storing mass or energy.
- It implements a steady-state conservation equation for energy and mass fractions.
- The model has zero pressure drop between its ports.
- </p>
- 
- <h4>Typical use and important parameters</h4>
- <p>
- Set the parameter <code>use_mWat_flow_in=true</code> to enable an
- input connector for <code>mWat_flow</code>.
- Otherwise, the model uses <code>mWat_flow = 0</code>.
- </p>
- <p>
- If the constant <code>simplify_mWat_flow = true</code>, which is its default value,
- then the equation
- </p>
- <pre>
-   port_a.m_flow + port_b.m_flow = - mWat_flow;
- </pre>
- <p>
- is simplified as
- </p>
- <pre>
-   port_a.m_flow + port_b.m_flow = 0;
- </pre>
- <p>
- This causes an error in the mass balance of about <i>0.5%</i>, but generally leads to
- simpler equations because the pressure drop equations are then decoupled from the
- mass exchange in this component.
- </p>
- 
- <p>
- To increase the numerical robustness of the model, the constant
- <code>prescribedHeatFlowRate</code> can be set.
- Use the following settings:
- </p>
- <ul>
- <li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
- at the <code>heatPort</code> is a prescribed heat flow rate that
- is <i>not</i> a function of the temperature difference
- between the medium and an ambient temperature. Examples include an ideal electrical heater,
- a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
- If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
- in this case, <code>heatPort.Q_flow=0</code>.
- </li>
- <li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
- computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
- which may itself be a function of temperature or mass flow rate.<br/>
- If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
- for example a solar collector that dissipates heat to the ambient and receives heat from
- the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
- </li>
- </ul>
- <p>
- If <code>prescribedHeatFlow=true</code>, then energy and mass balance
- equations are formulated to guard against numerical problems near
- zero flow that can occur if <code>Q_flow</code> or <code>m_flow</code>
- are the results of an iterative solver.
- </p>
- <h4>Implementation</h4>
- <p>
- Input connectors of the model are
- </p>
- <ul>
- <li>
- <code>Q_flow</code>, which is the sensible plus latent heat flow rate added to the medium,
- </li>
- <li>
- <code>mWat_flow</code>, which is the moisture mass flow rate added to the medium, and
- </li>
- <li>
- <code>C_flow</code>, which is the trace substance mass flow rate added to the medium.
- </li>
- </ul>
- 
- <p>
- The model can only be used as a steady-state model with two fluid ports.
- For a model with a dynamic balance, and more fluid ports, use
- <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.ConservationEquation</a>.
- </p>
- </html>",
+<p>
+This model transports fluid between its two ports, without storing mass or energy.
+It implements a steady-state conservation equation for energy and mass fractions.
+The model has zero pressure drop between its ports.
+</p>
+
+<h4>Typical use and important parameters</h4>
+<p>
+Set the parameter <code>use_mWat_flow_in=true</code> to enable an
+input connector for <code>mWat_flow</code>.
+Otherwise, the model uses <code>mWat_flow = 0</code>.
+</p>
+<p>
+If the constant <code>simplify_mWat_flow = true</code>, which is its default value,
+then the equation
+</p>
+<pre>
+  port_a.m_flow + port_b.m_flow = - mWat_flow;
+</pre>
+<p>
+is simplified as
+</p>
+<pre>
+  port_a.m_flow + port_b.m_flow = 0;
+</pre>
+<p>
+This causes an error in the mass balance of about <i>0.5%</i>, but generally leads to
+simpler equations because the pressure drop equations are then decoupled from the
+mass exchange in this component.
+</p>
+
+<p>
+To increase the numerical robustness of the model, the constant
+<code>prescribedHeatFlowRate</code> can be set.
+Use the following settings:
+</p>
+<ul>
+<li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
+at the <code>heatPort</code> is a prescribed heat flow rate that
+is <i>not</i> a function of the temperature difference
+between the medium and an ambient temperature. Examples include an ideal electrical heater,
+a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
+If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
+in this case, <code>heatPort.Q_flow=0</code>.
+</li>
+<li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
+computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
+which may itself be a function of temperature or mass flow rate.<br/>
+If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
+for example a solar collector that dissipates heat to the ambient and receives heat from
+the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
+</li>
+</ul>
+<p>
+If <code>prescribedHeatFlow=true</code>, then energy and mass balance
+equations are formulated to guard against numerical problems near
+zero flow that can occur if <code>Q_flow</code> or <code>m_flow</code>
+are the results of an iterative solver.
+</p>
+<h4>Implementation</h4>
+<p>
+Input connectors of the model are
+</p>
+<ul>
+<li>
+<code>Q_flow</code>, which is the sensible plus latent heat flow rate added to the medium,
+</li>
+<li>
+<code>mWat_flow</code>, which is the moisture mass flow rate added to the medium, and
+</li>
+<li>
+<code>C_flow</code>, which is the trace substance mass flow rate added to the medium.
+</li>
+</ul>
+
+<p>
+The model can only be used as a steady-state model with two fluid ports.
+For a model with a dynamic balance, and more fluid ports, use
+<a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.ConservationEquation</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 18, 2020, by Michael Wetter:<br/>
- Removed start value for <code>hOut</code> as it will be set by
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume\">
- AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume</a>.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1397\">#1397</a>.
- </li>
- <li>
- February 12, 2019, by Filip Jorissen:<br/>
- Removed obsolete division by <code>TMax</code> in assert.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1097\">#1097</a>.
- </li>
- <li>
- June 23, 2018, by Filip Jorissen:<br/>
- Added more details to energy conservation assert to facilitate
- debugging.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/962\">#962</a>.
- </li>
- <li>
- March 30, 2018, by Filip Jorissen:<br/>
- Added <code>getInstanceName()</code> in asserts to facilitate
- debugging.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/901\">#901</a>.
- </li>
- <li>
- April 24, 2017, by Michael Wetter and Filip Jorissen:<br/>
- Reimplemented check for energy conversion.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/741\">#741</a>.
- </li>
- <li>
- April 24, 2017, by Michael Wetter:<br/>
- Reverted change from April 21, 2017.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/741\">#741</a>.
- </li>
- <li>
- April 21, 2017, by Filip Jorissen:<br/>
- Revised test for energy conservation at small mass flow rates.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/741\">#741</a>.
- </li>
- <li>
- October 23, 2016, by Filip Jorissen:<br/>
- Added test for energy conservation at small mass flow rates.
- </li>
- <li>
- March 17, 2016, by Michael Wetter:<br/>
- Refactored model and implmented <code>regStep</code> instead of <code>spliceFunction</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">#247</a>
- and for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">#300</a>.
- </li>
- <li>
- September 3, 2015, by Filip Jorissen:<br/>
- Revised implementation of conservation of vapor mass.
- Added new variable <code>mFlow_inv_b</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">#247</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Removed <code>constant sensibleOnly</code> as this is no longer used because
- the model uses <code>use_mWat_flow</code>.<br/>
- Changed condition that determines whether <code>m_flowInv</code> needs to be
- computed because the change from January 20 introduced an error in
- <a href=\"modelica://AixLib.Fluid.MassExchangers.Examples.ConstantEffectiveness\">
- AixLib.Fluid.MassExchangers.Examples.ConstantEffectiveness</a>.
- </li>
- <li>
- January 20, 2016, by Filip Jorissen:<br/>
- Removed if-else block in code for parameter <code>sensibleOnly</code>
- since this is no longer needed to simplify the equations.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- January 17, 2016, by Michael Wetter:<br/>
- Added parameter <code>use_C_flow</code> and converted <code>C_flow</code>
- to a conditionally removed connector.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- December 16, 2015, by Michael Wetter:<br/>
- Removed the units of <code>C_flow</code> to allow for PPM.
- </li>
- <li>
- December 2, 2015, by Filip Jorissen:<br/>
- Added input <code>C_flow</code> and code for handling trace substance insertions.
- November 19, 2015, by Michael Wetter:<br/>
- Removed assignment of parameter
- <code>showDesignFlowDirection</code> in <code>extends</code> statement.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
- </li>
- <li>
- September 14, 2015, by Filip Jorissen:<br/>
- Rewrote some equations for better readability.
- </li>
- <li>
- August 11, 2015, by Michael Wetter:<br/>
- Refactored implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
- AixLib.Utilities.Math.Functions.inverseXRegularized</a>
- to allow function to be inlined and to factor out the computation
- of arguments that only depend on parameters.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/302\">issue 302</a>.
- </li>
- <li>
- July 17, 2015, by Michael Wetter:<br/>
- Corrected bug for situation with latent heat exchange and flow reversal not
- allowed.
- The previous formulation was singular.
- This caused some models to not translate.
- The error was introduced in
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">#282</a>.
- </li>
- <li>
- July 17, 2015, by Michael Wetter:<br/>
- Added constant <code>simplify_mWat_flow</code> to remove dependencies of the pressure drop
- calculation on the moisture balance.
- </li>
- <li>
- July 2, 2015 by Michael Wetter:<br/>
- Revised implementation of conservation equations,
- added default values for outlet quantities at <code>port_a</code>
- if <code>allowFlowReversal=false</code> and
- updated documentation.
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/281\">
- issue 281</a> for a discussion.
- </li>
- <li>
- July 1, 2015, by Filip Jorissen:<br/>
- Revised implementation so that equations are always consistent
- and do not lead to division by zero,
- also when connecting a <code>prescribedHeatFlowRate</code>
- to <code>MixingVolume</code> instances.
- Renamed <code>use_safeDivision</code> into <code>prescribedHeatFlowRate</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">#282</a>
- for a discussion.
- </li>
- <li>
- May 6, 2015, by Michael Wetter:<br/>
- Corrected documentation.
- </li>
- <li>
- February 11, 2014 by Michael Wetter:<br/>
- Improved documentation for <code>Q_flow</code> input.
- </li>
- <li>
- October 21, 2013 by Michael Wetter:<br/>
- Corrected sign error in the equation that is used if <code>use_safeDivision=false</code>
- and <code>sensibleOnly=true</code>.
- This only affects internal numerical tests, but not any examples in the library
- as the constant <code>use_safeDivision</code> is set to <code>true</code> by default.
- </li>
- <li>
- September 25, 2013 by Michael Wetter:<br/>
- Reformulated computation of outlet properties to avoid an event at zero mass flow rate.
- </li>
- <li>
- September 17, 2013 by Michael Wetter:<br/>
- Added start value for <code>hOut</code>.
- </li>
- <li>September 10, 2013 by Michael Wetter:<br/>
- Removed unrequired parameter <code>i_w</code>.
- </li>
- <li>
- May 7, 2013 by Michael Wetter:<br/>
- Removed <code>for</code> loops for species balance and trace substance balance,
- as they cause the error <code>Error: Operand port_a.Xi_outflow[1] to operator inStream is not a stream variable.</code>
- in OpenModelica.
- </li>
- <li>
- March 27, 2013 by Michael Wetter:<br/>
- Removed wrong unit attribute of <code>COut</code>,
- and added min and max attributes for <code>XiOut</code>.
- </li>
- <li>
- June 22, 2012 by Michael Wetter:<br/>
- Reformulated implementation with <code>m_flowInv</code> to use <code>port_a.m_flow * ...</code>
- if <code>use_safeDivision=false</code>. This avoids a division by zero if
- <code>port_a.m_flow=0</code>.
- </li>
- <li>
- February 7, 2012 by Michael Wetter:<br/>
- Revised base classes for conservation equations in <code>AixLib.Fluid.Interfaces</code>.
- </li>
- <li>
- December 14, 2011 by Michael Wetter:<br/>
- Changed assignment of <code>hOut</code>, <code>XiOut</code> and
- <code>COut</code> to no longer declare that it is continuous.
- The declaration of continuity, i.e, the
- <code>smooth(0, if (port_a.m_flow >= 0) then ...)</code> declaration,
- was required for Dymola 2012 to simulate, but it is no longer needed
- for Dymola 2012 FD01.
- </li>
- <li>
- August 19, 2011, by Michael Wetter:<br/>
- Changed assignment of <code>hOut</code>, <code>XiOut</code> and
- <code>COut</code> to declare that it is not differentiable.
- </li>
- <li>
- August 4, 2011, by Michael Wetter:<br/>
- Moved linearized pressure drop equation from the function body to the equation
- section. With the previous implementation,
- the symbolic processor may not rearrange the equations, which can lead
- to coupled equations instead of an explicit solution.
- </li>
- <li>
- March 29, 2011, by Michael Wetter:<br/>
- Changed energy and mass balance to avoid a division by zero if <code>m_flow=0</code>.
- </li>
- <li>
- March 27, 2011, by Michael Wetter:<br/>
- Added <code>homotopy</code> operator.
- </li>
- <li>
- August 19, 2010, by Michael Wetter:<br/>
- Fixed bug in energy and moisture balance that affected results if a component
- adds or removes moisture to the air stream.
- In the old implementation, the enthalpy and species
- outflow at <code>port_b</code> was multiplied with the mass flow rate at
- <code>port_a</code>. The old implementation led to small errors that were proportional
- to the amount of moisture change. For example, if the moisture added by the component
- was <code>0.005 kg/kg</code>, then the error was <code>0.5%</code>.
- Also, the results for forward flow and reverse flow differed by this amount.
- With the new implementation, the energy and moisture balance is exact.
- </li>
- <li>
- March 22, 2010, by Michael Wetter:<br/>
- Added constant <code>sensibleOnly</code> to
- simplify species balance equation.
- </li>
- <li>
- April 10, 2009, by Michael Wetter:<br/>
- Added model to compute flow friction.
- </li>
- <li>
- April 22, 2008, by Michael Wetter:<br/>
- Revised to add mass balance.
- </li>
- <li>
- March 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+October 24, 2022, by Michael Wetter:<br/>
+Conditionally removed assertion that checks for water content as this is
+only required if water is added to the medium.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1650\">#1650</a>.
+</li>
+<li>
+September 9, 2022, by Michael Wetter:<br/>
+Set nominal attribute for <code>XiOut</code>.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1634\">1634</a>.
+</li>
+<li>
+September 18, 2020, by Michael Wetter:<br/>
+Removed start value for <code>hOut</code> as it will be set by
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume\">
+AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume</a>.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1397\">#1397</a>.
+</li>
+<li>
+February 12, 2019, by Filip Jorissen:<br/>
+Removed obsolete division by <code>TMax</code> in assert.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1097\">#1097</a>.
+</li>
+<li>
+June 23, 2018, by Filip Jorissen:<br/>
+Added more details to energy conservation assert to facilitate
+debugging.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/962\">#962</a>.
+</li>
+<li>
+March 30, 2018, by Filip Jorissen:<br/>
+Added <code>getInstanceName()</code> in asserts to facilitate
+debugging.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/901\">#901</a>.
+</li>
+<li>
+April 24, 2017, by Michael Wetter and Filip Jorissen:<br/>
+Reimplemented check for energy conversion.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/741\">#741</a>.
+</li>
+<li>
+April 24, 2017, by Michael Wetter:<br/>
+Reverted change from April 21, 2017.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/741\">#741</a>.
+</li>
+<li>
+April 21, 2017, by Filip Jorissen:<br/>
+Revised test for energy conservation at small mass flow rates.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/741\">#741</a>.
+</li>
+<li>
+October 23, 2016, by Filip Jorissen:<br/>
+Added test for energy conservation at small mass flow rates.
+</li>
+<li>
+March 17, 2016, by Michael Wetter:<br/>
+Refactored model and implmented <code>regStep</code> instead of <code>spliceFunction</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">#247</a>
+and for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">#300</a>.
+</li>
+<li>
+September 3, 2015, by Filip Jorissen:<br/>
+Revised implementation of conservation of vapor mass.
+Added new variable <code>mFlow_inv_b</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">#247</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Removed <code>constant sensibleOnly</code> as this is no longer used because
+the model uses <code>use_mWat_flow</code>.<br/>
+Changed condition that determines whether <code>m_flowInv</code> needs to be
+computed because the change from January 20 introduced an error in
+<a href=\"modelica://AixLib.Fluid.MassExchangers.Examples.ConstantEffectiveness\">
+AixLib.Fluid.MassExchangers.Examples.ConstantEffectiveness</a>.
+</li>
+<li>
+January 20, 2016, by Filip Jorissen:<br/>
+Removed if-else block in code for parameter <code>sensibleOnly</code>
+since this is no longer needed to simplify the equations.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+January 17, 2016, by Michael Wetter:<br/>
+Added parameter <code>use_C_flow</code> and converted <code>C_flow</code>
+to a conditionally removed connector.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+December 16, 2015, by Michael Wetter:<br/>
+Removed the units of <code>C_flow</code> to allow for PPM.
+</li>
+<li>
+December 2, 2015, by Filip Jorissen:<br/>
+Added input <code>C_flow</code> and code for handling trace substance insertions.
+November 19, 2015, by Michael Wetter:<br/>
+Removed assignment of parameter
+<code>showDesignFlowDirection</code> in <code>extends</code> statement.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
+</li>
+<li>
+September 14, 2015, by Filip Jorissen:<br/>
+Rewrote some equations for better readability.
+</li>
+<li>
+August 11, 2015, by Michael Wetter:<br/>
+Refactored implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
+AixLib.Utilities.Math.Functions.inverseXRegularized</a>
+to allow function to be inlined and to factor out the computation
+of arguments that only depend on parameters.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/302\">issue 302</a>.
+</li>
+<li>
+July 17, 2015, by Michael Wetter:<br/>
+Corrected bug for situation with latent heat exchange and flow reversal not
+allowed.
+The previous formulation was singular.
+This caused some models to not translate.
+The error was introduced in
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">#282</a>.
+</li>
+<li>
+July 17, 2015, by Michael Wetter:<br/>
+Added constant <code>simplify_mWat_flow</code> to remove dependencies of the pressure drop
+calculation on the moisture balance.
+</li>
+<li>
+July 2, 2015 by Michael Wetter:<br/>
+Revised implementation of conservation equations,
+added default values for outlet quantities at <code>port_a</code>
+if <code>allowFlowReversal=false</code> and
+updated documentation.
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/281\">
+issue 281</a> for a discussion.
+</li>
+<li>
+July 1, 2015, by Filip Jorissen:<br/>
+Revised implementation so that equations are always consistent
+and do not lead to division by zero,
+also when connecting a <code>prescribedHeatFlowRate</code>
+to <code>MixingVolume</code> instances.
+Renamed <code>use_safeDivision</code> into <code>prescribedHeatFlowRate</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">#282</a>
+for a discussion.
+</li>
+<li>
+May 6, 2015, by Michael Wetter:<br/>
+Corrected documentation.
+</li>
+<li>
+February 11, 2014 by Michael Wetter:<br/>
+Improved documentation for <code>Q_flow</code> input.
+</li>
+<li>
+October 21, 2013 by Michael Wetter:<br/>
+Corrected sign error in the equation that is used if <code>use_safeDivision=false</code>
+and <code>sensibleOnly=true</code>.
+This only affects internal numerical tests, but not any examples in the library
+as the constant <code>use_safeDivision</code> is set to <code>true</code> by default.
+</li>
+<li>
+September 25, 2013 by Michael Wetter:<br/>
+Reformulated computation of outlet properties to avoid an event at zero mass flow rate.
+</li>
+<li>
+September 17, 2013 by Michael Wetter:<br/>
+Added start value for <code>hOut</code>.
+</li>
+<li>September 10, 2013 by Michael Wetter:<br/>
+Removed unrequired parameter <code>i_w</code>.
+</li>
+<li>
+May 7, 2013 by Michael Wetter:<br/>
+Removed <code>for</code> loops for species balance and trace substance balance,
+as they cause the error <code>Error: Operand port_a.Xi_outflow[1] to operator inStream is not a stream variable.</code>
+in OpenModelica.
+</li>
+<li>
+March 27, 2013 by Michael Wetter:<br/>
+Removed wrong unit attribute of <code>COut</code>,
+and added min and max attributes for <code>XiOut</code>.
+</li>
+<li>
+June 22, 2012 by Michael Wetter:<br/>
+Reformulated implementation with <code>m_flowInv</code> to use <code>port_a.m_flow * ...</code>
+if <code>use_safeDivision=false</code>. This avoids a division by zero if
+<code>port_a.m_flow=0</code>.
+</li>
+<li>
+February 7, 2012 by Michael Wetter:<br/>
+Revised base classes for conservation equations in <code>AixLib.Fluid.Interfaces</code>.
+</li>
+<li>
+December 14, 2011 by Michael Wetter:<br/>
+Changed assignment of <code>hOut</code>, <code>XiOut</code> and
+<code>COut</code> to no longer declare that it is continuous.
+The declaration of continuity, i.e, the
+<code>smooth(0, if (port_a.m_flow >= 0) then ...)</code> declaration,
+was required for Dymola 2012 to simulate, but it is no longer needed
+for Dymola 2012 FD01.
+</li>
+<li>
+August 19, 2011, by Michael Wetter:<br/>
+Changed assignment of <code>hOut</code>, <code>XiOut</code> and
+<code>COut</code> to declare that it is not differentiable.
+</li>
+<li>
+August 4, 2011, by Michael Wetter:<br/>
+Moved linearized pressure drop equation from the function body to the equation
+section. With the previous implementation,
+the symbolic processor may not rearrange the equations, which can lead
+to coupled equations instead of an explicit solution.
+</li>
+<li>
+March 29, 2011, by Michael Wetter:<br/>
+Changed energy and mass balance to avoid a division by zero if <code>m_flow=0</code>.
+</li>
+<li>
+March 27, 2011, by Michael Wetter:<br/>
+Added <code>homotopy</code> operator.
+</li>
+<li>
+August 19, 2010, by Michael Wetter:<br/>
+Fixed bug in energy and moisture balance that affected results if a component
+adds or removes moisture to the air stream.
+In the old implementation, the enthalpy and species
+outflow at <code>port_b</code> was multiplied with the mass flow rate at
+<code>port_a</code>. The old implementation led to small errors that were proportional
+to the amount of moisture change. For example, if the moisture added by the component
+was <code>0.005 kg/kg</code>, then the error was <code>0.5%</code>.
+Also, the results for forward flow and reverse flow differed by this amount.
+With the new implementation, the energy and moisture balance is exact.
+</li>
+<li>
+March 22, 2010, by Michael Wetter:<br/>
+Added constant <code>sensibleOnly</code> to
+simplify species balance equation.
+</li>
+<li>
+April 10, 2009, by Michael Wetter:<br/>
+Added model to compute flow friction.
+</li>
+<li>
+April 22, 2008, by Michael Wetter:<br/>
+Revised to add mass balance.
+</li>
+<li>
+March 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
         preserveAspectRatio=true,
         extent={{-100,-100},{100,100}},
@@ -626,6 +639,6 @@ revisions="<html>
         Line(points={{-56,-73},{81,-73}}, color={255,255,255}),
         Line(points={{6,14},{6,-37}},     color={255,255,255}),
         Line(points={{54,14},{6,14}},     color={255,255,255}),
-        Line(points={{6,-37},{-42,-37}},  color={255,255,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        Line(points={{6,-37},{-42,-37}},  color={255,255,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end StaticTwoPortConservationEquation;
diff --git a/AixLib/Fluid/Interfaces/StaticTwoPortHeatMassExchanger.mo b/AixLib/Fluid/Interfaces/StaticTwoPortHeatMassExchanger.mo
index 81b9599509..f5fbea7ecb 100644
--- a/AixLib/Fluid/Interfaces/StaticTwoPortHeatMassExchanger.mo
+++ b/AixLib/Fluid/Interfaces/StaticTwoPortHeatMassExchanger.mo
@@ -90,211 +90,211 @@ equation
   annotation (
     preferredView="info",
     Documentation(info="<html>
- <p>
- This component transports fluid between its two ports, without
- storing mass or energy. It is based on
- <a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPortTransport\">
- Modelica.Fluid.Interfaces.PartialTwoPortTransport</a> but it does
- use a different implementation for handling reverse flow because
- in this component, mass flow rate can be added or removed from
- the medium.
- </p>
- <p>
- If <code>dp_nominal &gt; Modelica.Constants.eps</code>, this component computes
- pressure drop due to flow friction.
- The pressure drop is defined by a quadratic function that goes through
- the point <code>(m_flow_nominal, dp_nominal)</code>. At <code>|m_flow| &lt; deltaM * m_flow_nominal</code>,
- the pressure drop vs. flow relation is linearized.
- If the parameter <code>linearizeFlowResistance</code> is set to true,
- then the whole pressure drop vs. flow resistance curve is linearized.
- </p>
- <h4>Implementation</h4>
- This model uses inputs and constants that need to be set by models
- that extend or instantiate this model.
- The following inputs need to be assigned:
- <ul>
- <li>
- <code>Q_flow</code>, which is the sensible and latent heat flow rate added to the medium.
- </li>
- <li>
- <code>mWat_flow</code>, which is the moisture mass flow rate added to the medium.
- </li>
- </ul>
- 
- <p>
- Set the constant <code>sensibleOnly=true</code> if the model that extends
- or instantiates this model sets <code>mWat_flow = 0</code>.
- </p>
- <p>
- To increase the numerical robustness of the model, the constant
- <code>prescribedHeatFlowRate</code> can be set.
- Use the following settings:
- </p>
- <ul>
- <li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
- at the <code>heatPort</code> is a prescribed heat flow rate that
- is <i>not</i> a function of the temperature difference
- between the medium and an ambient temperature. Examples include an ideal electrical heater,
- a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
- If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
- in this case, <code>heatPort.Q_flow=0</code>.
- </li>
- <li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
- computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
- which may itself be a function of temperature or mass flow rate.<br/>
- If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
- for example a solar collector that dissipates heat to the ambient and receives heat from
- the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
- </li>
- </ul>
- <p>
- If <code>prescribedHeatFlow=true</code>, then energy and mass balance
- equations are formulated to guard against numerical problems near
- zero flow that can occur if <code>Q_flow</code> or <code>m_flow</code>
- are the results of an iterative solver.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- April 11, 2017, by Michael Wetter:<br/>
- Updated documentation to make clear that <code>Q_flow</code>
- includes latent heat flow rate.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- <li>
- January 22, 2016 by Michael Wetter:<br/>
- Removed assignment of <code>sensibleOnly</code> in <code>bal1</code> and <code>bal2</code>
- as this constant has been removed in
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
- AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>.
- </li>
- <li>
- November 19, 2015, by Michael Wetter:<br/>
- Removed assignment of parameter
- <code>showDesignFlowDirection</code> in <code>extends</code> statement.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
- </li>
- <li>
- July 2, 2015 by Michael Wetter:<br/>
- Revised implementation of conservation equations,
- added default values for outlet quantities at <code>port_a</code>
- if <code>allowFlowReversal=false</code> and
- updated documentation.
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/281\">
- issue 281</a> for a discussion.
- </li>
- <li>
- July 1, 2015 by Filip Jorissen:<br/>
- Renamed <code>use_safeDivision</code> into
- <code>prescribedHeatFlowRate</code>.
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">
- issue 282</a> for a discussion.
- </li>
- <li>
- November 13, 2013 by Michael Wetter:<br/>
- Added parameter <code>homotopyInitialization</code> as
- it has been removed in the base class.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Removed propagation of <code>show_V_flow</code>
- to pressure drop calculation, as this model no longer has
- that parameter.
- </li>
- <li>
- July 30, 2013 by Michael Wetter:<br/>
- Changed connector <code>mXi_flow[Medium.nXi]</code>
- to a scalar input connector <code>mWat_flow</code>.
- The reason is that <code>mXi_flow</code> does not allow
- to compute the other components in <code>mX_flow</code> and
- therefore leads to an ambiguous use of the model.
- By only requesting <code>mWat_flow</code>, the mass balance
- and species balance can be implemented correctly.
- </li>
- <li>
- March 27, 2013 by Michael Wetter:<br/>
- Removed wrong unit attribute of <code>COut</code>,
- and added min and max attributes for <code>XiOut</code>.
- </li>
- <li>
- February 8, 2012 by Michael Wetter:<br/>
- Changed model to use graphical modeling.
- </li>
- <li>
- December 14, 2011 by Michael Wetter:<br/>
- Changed assignment of <code>hOut</code>, <code>XiOut</code> and
- <code>COut</code> to no longer declare that it is continuous.
- The declaration of continuity, i.e, the
- <code>smooth(0, if (port_a.m_flow >= 0) then ...)</code> declaration,
- was required for Dymola 2012 to simulate, but it is no longer needed
- for Dymola 2012 FD01.
- </li>
- <li>
- August 19, 2011, by Michael Wetter:<br/>
- Changed assignment of <code>hOut</code>, <code>XiOut</code> and
- <code>COut</code> to declare that it is not differentiable.
- </li>
- <li>
- August 4, 2011, by Michael Wetter:<br/>
- Moved linearized pressure drop equation from the function body to the equation
- section. With the previous implementation,
- the symbolic processor may not rearrange the equations, which can lead
- to coupled equations instead of an explicit solution.
- </li>
- <li>
- March 29, 2011, by Michael Wetter:<br/>
- Changed energy and mass balance to avoid a division by zero if <code>m_flow=0</code>.
- </li>
- <li>
- March 27, 2011, by Michael Wetter:<br/>
- Added <code>homotopy</code> operator.
- </li>
- <li>
- August 19, 2010, by Michael Wetter:<br/>
- Fixed bug in energy and moisture balance that affected results if a component
- adds or removes moisture to the air stream.
- In the old implementation, the enthalpy and species
- outflow at <code>port_b</code> was multiplied with the mass flow rate at
- <code>port_a</code>. The old implementation led to small errors that were proportional
- to the amount of moisture change. For example, if the moisture added by the component
- was <code>0.005 kg/kg</code>, then the error was <code>0.5%</code>.
- Also, the results for forward flow and reverse flow differed by this amount.
- With the new implementation, the energy and moisture balance is exact.
- </li>
- <li>
- March 22, 2010, by Michael Wetter:<br/>
- Added constant <code>sensibleOnly</code> to
- simplify species balance equation.
- </li>
- <li>
- April 10, 2009, by Michael Wetter:<br/>
- Added model to compute flow friction.
- </li>
- <li>
- April 22, 2008, by Michael Wetter:<br/>
- Revised to add mass balance.
- </li>
- <li>
- March 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This component transports fluid between its two ports, without
+storing mass or energy. It is based on
+<a href=\"modelica://Modelica.Fluid.Interfaces.PartialTwoPortTransport\">
+Modelica.Fluid.Interfaces.PartialTwoPortTransport</a> but it does
+use a different implementation for handling reverse flow because
+in this component, mass flow rate can be added or removed from
+the medium.
+</p>
+<p>
+If <code>dp_nominal &gt; Modelica.Constants.eps</code>, this component computes
+pressure drop due to flow friction.
+The pressure drop is defined by a quadratic function that goes through
+the point <code>(m_flow_nominal, dp_nominal)</code>. At <code>|m_flow| &lt; deltaM * m_flow_nominal</code>,
+the pressure drop vs. flow relation is linearized.
+If the parameter <code>linearizeFlowResistance</code> is set to true,
+then the whole pressure drop vs. flow resistance curve is linearized.
+</p>
+<h4>Implementation</h4>
+This model uses inputs and constants that need to be set by models
+that extend or instantiate this model.
+The following inputs need to be assigned:
+<ul>
+<li>
+<code>Q_flow</code>, which is the sensible and latent heat flow rate added to the medium.
+</li>
+<li>
+<code>mWat_flow</code>, which is the moisture mass flow rate added to the medium.
+</li>
+</ul>
+
+<p>
+Set the constant <code>sensibleOnly=true</code> if the model that extends
+or instantiates this model sets <code>mWat_flow = 0</code>.
+</p>
+<p>
+To increase the numerical robustness of the model, the constant
+<code>prescribedHeatFlowRate</code> can be set.
+Use the following settings:
+</p>
+<ul>
+<li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
+at the <code>heatPort</code> is a prescribed heat flow rate that
+is <i>not</i> a function of the temperature difference
+between the medium and an ambient temperature. Examples include an ideal electrical heater,
+a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
+If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
+in this case, <code>heatPort.Q_flow=0</code>.
+</li>
+<li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
+computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
+which may itself be a function of temperature or mass flow rate.<br/>
+If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
+for example a solar collector that dissipates heat to the ambient and receives heat from
+the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
+</li>
+</ul>
+<p>
+If <code>prescribedHeatFlow=true</code>, then energy and mass balance
+equations are formulated to guard against numerical problems near
+zero flow that can occur if <code>Q_flow</code> or <code>m_flow</code>
+are the results of an iterative solver.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+April 11, 2017, by Michael Wetter:<br/>
+Updated documentation to make clear that <code>Q_flow</code>
+includes latent heat flow rate.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+<li>
+January 22, 2016 by Michael Wetter:<br/>
+Removed assignment of <code>sensibleOnly</code> in <code>bal1</code> and <code>bal2</code>
+as this constant has been removed in
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger\">
+AixLib.Fluid.Interfaces.StaticTwoPortHeatMassExchanger</a>.
+</li>
+<li>
+November 19, 2015, by Michael Wetter:<br/>
+Removed assignment of parameter
+<code>showDesignFlowDirection</code> in <code>extends</code> statement.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
+</li>
+<li>
+July 2, 2015 by Michael Wetter:<br/>
+Revised implementation of conservation equations,
+added default values for outlet quantities at <code>port_a</code>
+if <code>allowFlowReversal=false</code> and
+updated documentation.
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/281\">
+issue 281</a> for a discussion.
+</li>
+<li>
+July 1, 2015 by Filip Jorissen:<br/>
+Renamed <code>use_safeDivision</code> into
+<code>prescribedHeatFlowRate</code>.
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">
+issue 282</a> for a discussion.
+</li>
+<li>
+November 13, 2013 by Michael Wetter:<br/>
+Added parameter <code>homotopyInitialization</code> as
+it has been removed in the base class.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Removed propagation of <code>show_V_flow</code>
+to pressure drop calculation, as this model no longer has
+that parameter.
+</li>
+<li>
+July 30, 2013 by Michael Wetter:<br/>
+Changed connector <code>mXi_flow[Medium.nXi]</code>
+to a scalar input connector <code>mWat_flow</code>.
+The reason is that <code>mXi_flow</code> does not allow
+to compute the other components in <code>mX_flow</code> and
+therefore leads to an ambiguous use of the model.
+By only requesting <code>mWat_flow</code>, the mass balance
+and species balance can be implemented correctly.
+</li>
+<li>
+March 27, 2013 by Michael Wetter:<br/>
+Removed wrong unit attribute of <code>COut</code>,
+and added min and max attributes for <code>XiOut</code>.
+</li>
+<li>
+February 8, 2012 by Michael Wetter:<br/>
+Changed model to use graphical modeling.
+</li>
+<li>
+December 14, 2011 by Michael Wetter:<br/>
+Changed assignment of <code>hOut</code>, <code>XiOut</code> and
+<code>COut</code> to no longer declare that it is continuous.
+The declaration of continuity, i.e, the
+<code>smooth(0, if (port_a.m_flow >= 0) then ...)</code> declaration,
+was required for Dymola 2012 to simulate, but it is no longer needed
+for Dymola 2012 FD01.
+</li>
+<li>
+August 19, 2011, by Michael Wetter:<br/>
+Changed assignment of <code>hOut</code>, <code>XiOut</code> and
+<code>COut</code> to declare that it is not differentiable.
+</li>
+<li>
+August 4, 2011, by Michael Wetter:<br/>
+Moved linearized pressure drop equation from the function body to the equation
+section. With the previous implementation,
+the symbolic processor may not rearrange the equations, which can lead
+to coupled equations instead of an explicit solution.
+</li>
+<li>
+March 29, 2011, by Michael Wetter:<br/>
+Changed energy and mass balance to avoid a division by zero if <code>m_flow=0</code>.
+</li>
+<li>
+March 27, 2011, by Michael Wetter:<br/>
+Added <code>homotopy</code> operator.
+</li>
+<li>
+August 19, 2010, by Michael Wetter:<br/>
+Fixed bug in energy and moisture balance that affected results if a component
+adds or removes moisture to the air stream.
+In the old implementation, the enthalpy and species
+outflow at <code>port_b</code> was multiplied with the mass flow rate at
+<code>port_a</code>. The old implementation led to small errors that were proportional
+to the amount of moisture change. For example, if the moisture added by the component
+was <code>0.005 kg/kg</code>, then the error was <code>0.5%</code>.
+Also, the results for forward flow and reverse flow differed by this amount.
+With the new implementation, the energy and moisture balance is exact.
+</li>
+<li>
+March 22, 2010, by Michael Wetter:<br/>
+Added constant <code>sensibleOnly</code> to
+simplify species balance equation.
+</li>
+<li>
+April 10, 2009, by Michael Wetter:<br/>
+Added model to compute flow friction.
+</li>
+<li>
+April 22, 2008, by Michael Wetter:<br/>
+Revised to add mass balance.
+</li>
+<li>
+March 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end StaticTwoPortHeatMassExchanger;
diff --git a/AixLib/Fluid/Interfaces/TwoPortFlowResistanceParameters.mo b/AixLib/Fluid/Interfaces/TwoPortFlowResistanceParameters.mo
index 169cf32d1d..432f7d7c83 100644
--- a/AixLib/Fluid/Interfaces/TwoPortFlowResistanceParameters.mo
+++ b/AixLib/Fluid/Interfaces/TwoPortFlowResistanceParameters.mo
@@ -23,27 +23,27 @@ record TwoPortFlowResistanceParameters
 
 annotation (preferredView="info",
 Documentation(info="<html>
- This class contains parameters that are used to
- compute the pressure drop in models that have one fluid stream.
- Note that the nominal mass flow rate is not declared here because
- the model
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
- PartialTwoPortInterface</a>
- already declares it.
- </html>",
+This class contains parameters that are used to
+compute the pressure drop in models that have one fluid stream.
+Note that the nominal mass flow rate is not declared here because
+the model
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+PartialTwoPortInterface</a>
+already declares it.
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoPortFlowResistanceParameters;
diff --git a/AixLib/Fluid/Interfaces/TwoPortHeatMassExchanger.mo b/AixLib/Fluid/Interfaces/TwoPortHeatMassExchanger.mo
index 09aa0e113c..ae132e8221 100644
--- a/AixLib/Fluid/Interfaces/TwoPortHeatMassExchanger.mo
+++ b/AixLib/Fluid/Interfaces/TwoPortHeatMassExchanger.mo
@@ -77,8 +77,8 @@ initial algorithm
   assert((energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState) or
           tau > Modelica.Constants.eps,
 "The parameter tau, or the volume of the model from which tau may be derived, is unreasonably small.
-  You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
-  Received tau = "+ String(tau) + "\n");
+ You need to set energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState to model steady-state.
+ Received tau = " + String(tau) + "\n");
 
   assert(homotopyInitialization, "In " + getInstanceName() +
     ": The constant homotopyInitialization has been modified from its default value. This constant will be removed in future releases.",
@@ -96,153 +96,153 @@ equation
       color={0,127,255}));
   annotation (
     Documentation(info="<html>
- <p>
- This component transports one fluid stream.
- It provides the basic model for implementing dynamic and steady-state
- models that exchange heat and water vapor with the fluid stream.
- The model also computes the pressure drop due to the flow resistance.
- By setting the parameter <code>dp_nominal=0</code>, the computation
- of the pressure drop can be avoided.
- The variable <code>vol.heatPort.T</code> always has the value of
- the temperature of the medium that leaves the component.
- For the actual temperatures at the port, the variables <code>sta_a.T</code>
- and <code>sta_b.T</code> can be used. These two variables are provided by
- the base class
- <a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
- AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>.
- </p>
- 
- For models that extend this model, see for example
- <ul>
- <li>
- the ideal heater or cooler
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
- AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>, and
- </li>
- <li>
- the ideal humidifier
- <a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
- AixLib.Fluid.Humidifiers.Humidifier_u</a>.
- </li>
- </ul>
- 
- <h4>Implementation</h4>
- <p>
- The variable names follow the conventions used in
- <a href=\"modelica://Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX\">
- Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX
- </a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 3, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
- </li>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- December 1, 2016, by Michael Wetter:<br/>
- Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>final quantity=Medium.substanceNames</code> for <code>X_start</code>.
- </li>
- <li>
- May 6, 2015, by Michael Wetter:<br/>
- Added missing propagation of <code>allowFlowReversal</code> to
- instance <code>vol</code>.
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">#412</a>.
- </li>
- <li>
- May 1, 2015, by Marcus Fuchs:<br/>
- Fixed links in documentation.
- </li>
- <li>
- October 6, 2014, by Michael Wetter:<br/>
- Changed medium declaration in pressure drop element to be final.
- </li>
- <li>
- May 28, 2014, by Michael Wetter:<br/>
- Removed <code>annotation(Evaluate=true)</code> for parameter <code>tau</code>.
- This is needed to allow changing the time constant after translation.
- </li>
- <li>
- November 12, 2013, by Michael Wetter:<br/>
- Removed <code>import Modelica.Constants</code> statement.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Removed parameter <code>show_V_flow</code>.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with the naming conventions.
- </li>
- <li>
- October 17, 2012, by Michael Wetter:<br/>
- Fixed broken link in documentation.
- </li>
- <li>
- February 3, 2012, by Michael Wetter:<br/>
- Removed assignment of <code>m_flow_small</code> as it is no
- longer used in the pressure drop model.
- </li>
- <li>
- January 15, 2011, by Michael Wetter:<br/>
- Fixed wrong class reference in information section.
- </li>
- <li>
- September 13, 2011, by Michael Wetter:<br/>
- Changed assignment of <code>vol(mass/energyDynamics=...)</code> as the
- previous assignment caused a non-literal start value that was ignored.
- </li>
- <li>
- July 29, 2011, by Michael Wetter:<br/>
- Added start value for outflowing enthalpy.
- </li>
- <li>
- July 11, 2011, by Michael Wetter:<br/>
- Changed parameterization of fluid volume so that steady-state balance is
- used when <code>tau = 0</code>.
- </li>
- <li>
- May 25, 2011, by Michael Wetter:<br/>
- Removed temperature sensor and changed implementation of fluid volume
- to allow use of this model for the steady-state and dynamic humidifier
- <a href=\"modelica://AixLib.Fluid.MassExchangers.HumidifierPrescribed\">
- AixLib.Fluid.MassExchangers.HumidifierPrescribed</a>.
- </li>
- <li>
- March 25, 2011, by Michael Wetter:<br/>
- Added homotopy operator.
- </li>
- <li>
- March 21, 2010 by Michael Wetter:<br/>
- Changed pressure start value from <code>system.p_start</code>
- to <code>Medium.p_default</code> since HVAC models may have water and
- air, which are typically at different pressures.
- </li>
- <li>
- April 13, 2009, by Michael Wetter:<br/>
- Added model to compute flow friction.
- </li>
- <li>
- January 29, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This component transports one fluid stream.
+It provides the basic model for implementing dynamic and steady-state
+models that exchange heat and water vapor with the fluid stream.
+The model also computes the pressure drop due to the flow resistance.
+By setting the parameter <code>dp_nominal=0</code>, the computation
+of the pressure drop can be avoided.
+The variable <code>vol.heatPort.T</code> always has the value of
+the temperature of the medium that leaves the component.
+For the actual temperatures at the port, the variables <code>sta_a.T</code>
+and <code>sta_b.T</code> can be used. These two variables are provided by
+the base class
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>.
+</p>
+
+For models that extend this model, see for example
+<ul>
+<li>
+the ideal heater or cooler
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
+AixLib.Fluid.HeatExchangers.HeaterCooler_u</a>, and
+</li>
+<li>
+the ideal humidifier
+<a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
+AixLib.Fluid.Humidifiers.Humidifier_u</a>.
+</li>
+</ul>
+
+<h4>Implementation</h4>
+<p>
+The variable names follow the conventions used in
+<a href=\"modelica://Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX\">
+Modelica.Fluid.Examples.HeatExchanger.BaseClasses.BasicHX
+</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 3, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">issue 1542</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+December 1, 2016, by Michael Wetter:<br/>
+Updated model as <code>use_dh</code> is no longer a parameter in the pressure drop model.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/480\">#480</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>final quantity=Medium.substanceNames</code> for <code>X_start</code>.
+</li>
+<li>
+May 6, 2015, by Michael Wetter:<br/>
+Added missing propagation of <code>allowFlowReversal</code> to
+instance <code>vol</code>.
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">#412</a>.
+</li>
+<li>
+May 1, 2015, by Marcus Fuchs:<br/>
+Fixed links in documentation.
+</li>
+<li>
+October 6, 2014, by Michael Wetter:<br/>
+Changed medium declaration in pressure drop element to be final.
+</li>
+<li>
+May 28, 2014, by Michael Wetter:<br/>
+Removed <code>annotation(Evaluate=true)</code> for parameter <code>tau</code>.
+This is needed to allow changing the time constant after translation.
+</li>
+<li>
+November 12, 2013, by Michael Wetter:<br/>
+Removed <code>import Modelica.Constants</code> statement.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Removed parameter <code>show_V_flow</code>.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with the naming conventions.
+</li>
+<li>
+October 17, 2012, by Michael Wetter:<br/>
+Fixed broken link in documentation.
+</li>
+<li>
+February 3, 2012, by Michael Wetter:<br/>
+Removed assignment of <code>m_flow_small</code> as it is no
+longer used in the pressure drop model.
+</li>
+<li>
+January 15, 2011, by Michael Wetter:<br/>
+Fixed wrong class reference in information section.
+</li>
+<li>
+September 13, 2011, by Michael Wetter:<br/>
+Changed assignment of <code>vol(mass/energyDynamics=...)</code> as the
+previous assignment caused a non-literal start value that was ignored.
+</li>
+<li>
+July 29, 2011, by Michael Wetter:<br/>
+Added start value for outflowing enthalpy.
+</li>
+<li>
+July 11, 2011, by Michael Wetter:<br/>
+Changed parameterization of fluid volume so that steady-state balance is
+used when <code>tau = 0</code>.
+</li>
+<li>
+May 25, 2011, by Michael Wetter:<br/>
+Removed temperature sensor and changed implementation of fluid volume
+to allow use of this model for the steady-state and dynamic humidifier
+<a href=\"modelica://AixLib.Fluid.MassExchangers.HumidifierPrescribed\">
+AixLib.Fluid.MassExchangers.HumidifierPrescribed</a>.
+</li>
+<li>
+March 25, 2011, by Michael Wetter:<br/>
+Added homotopy operator.
+</li>
+<li>
+March 21, 2010 by Michael Wetter:<br/>
+Changed pressure start value from <code>system.p_start</code>
+to <code>Medium.p_default</code> since HVAC models may have water and
+air, which are typically at different pressures.
+</li>
+<li>
+April 13, 2009, by Michael Wetter:<br/>
+Added model to compute flow friction.
+</li>
+<li>
+January 29, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(
         preserveAspectRatio=true,
         extent={{-100,-100},{100,100}},
@@ -264,6 +264,6 @@ equation
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={255,0,0},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoPortHeatMassExchanger;
diff --git a/AixLib/Fluid/MassExchangers/ConstantEffectiveness.mo b/AixLib/Fluid/MassExchangers/ConstantEffectiveness.mo
index fbd5c21db7..8e286bfa1f 100644
--- a/AixLib/Fluid/MassExchangers/ConstantEffectiveness.mo
+++ b/AixLib/Fluid/MassExchangers/ConstantEffectiveness.mo
@@ -106,76 +106,76 @@ equation
           preferredView="info",
 defaultComponentName="masExc",
 Documentation(info="<html>
- <p>
- Model for a heat and moisture exchanger with constant effectiveness.
- </p>
- <p>
- This model transfers heat and moisture in the amount of </p>
- <pre>
-   QSen = epsS * Q_max,
-   m    = epsL * mWat_max,
- </pre>
- <p>
- where <code>epsS</code> and <code>epsL</code> are constant effectiveness
- for the sensible and latent heat transfer,
- <code>Q_max</code> is the maximum sensible heat that can be transferred and
- <code>mWat_max</code> is the maximum moisture that can be transferred.
- </p>
- <p>
- For a sensible heat exchanger, use
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ConstantEffectiveness\">
- AixLib.Fluid.HeatExchangers.ConstantEffectiveness</a>
- instead of this model.
- </p>
- <p>
- This model can only be used with medium models that define the integer constant
- <code>Water</code> which needs to be equal to the index of the water mass fraction
- in the species vector.
- </p>
- </html>",
+<p>
+Model for a heat and moisture exchanger with constant effectiveness.
+</p>
+<p>
+This model transfers heat and moisture in the amount of </p>
+<pre>
+  QSen = epsS * Q_max,
+  m    = epsL * mWat_max,
+</pre>
+<p>
+where <code>epsS</code> and <code>epsL</code> are constant effectiveness
+for the sensible and latent heat transfer,
+<code>Q_max</code> is the maximum sensible heat that can be transferred and
+<code>mWat_max</code> is the maximum moisture that can be transferred.
+</p>
+<p>
+For a sensible heat exchanger, use
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ConstantEffectiveness\">
+AixLib.Fluid.HeatExchangers.ConstantEffectiveness</a>
+instead of this model.
+</p>
+<p>
+This model can only be used with medium models that define the integer constant
+<code>Water</code> which needs to be equal to the index of the water mass fraction
+in the species vector.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 30, 2018, by Filip Jorissen:<br/>
- Set <code>final prescribedHeatFlowRate1=true</code> and 
- <code>final prescribedHeatFlowRate2=true</code>.<br/>
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/907\">#907</a>.
- </li>
- <li>
- April 11, 2017, by Michael Wetter:<br/>
- Corrected bug as <code>Q1_flow</code> did not include latent heat flow rate.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- October 14, 2013 by Michael Wetter:<br/>
- Replaced access to constant <code>Medium1.Water</code> by introducing
- the parameter <code>i1_w</code>, and used a similar construct for
- <code>Medium2</code>.
- This avoids an error during model check as these constants are not known
- in the partial medium model.
- </li>
- <li>
- August 13, 2013 by Michael Wetter:<br/>
- Corrected error in the documentation.
- </li>
- <li>
- July 30, 2013 by Michael Wetter:<br/>
- Updated model to use new variable <code>mWat_flow</code>
- in the base class.
- </li>
- <li>
- January 28, 2010, by Michael Wetter:<br/>
- Added regularization near zero flow.
- </li>
- <li>
- October 21, 2008, by Michael Wetter:<br/>
- First implementation, based on
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.ConstantEffectiveness\">
- AixLib.Fluid.HeatExchangers.ConstantEffectiveness</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 30, 2018, by Filip Jorissen:<br/>
+Set <code>final prescribedHeatFlowRate1=true</code> and 
+<code>final prescribedHeatFlowRate2=true</code>.<br/>
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/907\">#907</a>.
+</li>
+<li>
+April 11, 2017, by Michael Wetter:<br/>
+Corrected bug as <code>Q1_flow</code> did not include latent heat flow rate.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+October 14, 2013 by Michael Wetter:<br/>
+Replaced access to constant <code>Medium1.Water</code> by introducing
+the parameter <code>i1_w</code>, and used a similar construct for
+<code>Medium2</code>.
+This avoids an error during model check as these constants are not known
+in the partial medium model.
+</li>
+<li>
+August 13, 2013 by Michael Wetter:<br/>
+Corrected error in the documentation.
+</li>
+<li>
+July 30, 2013 by Michael Wetter:<br/>
+Updated model to use new variable <code>mWat_flow</code>
+in the base class.
+</li>
+<li>
+January 28, 2010, by Michael Wetter:<br/>
+Added regularization near zero flow.
+</li>
+<li>
+October 21, 2008, by Michael Wetter:<br/>
+First implementation, based on
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.ConstantEffectiveness\">
+AixLib.Fluid.HeatExchangers.ConstantEffectiveness</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantEffectiveness;
diff --git a/AixLib/Fluid/MassExchangers/Examples/ConstantEffectiveness.mo b/AixLib/Fluid/MassExchangers/Examples/ConstantEffectiveness.mo
index 04c6b5413b..b5193ee24d 100644
--- a/AixLib/Fluid/MassExchangers/Examples/ConstantEffectiveness.mo
+++ b/AixLib/Fluid/MassExchangers/Examples/ConstantEffectiveness.mo
@@ -97,10 +97,10 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MassExchangers/Examples/ConstantEffectiveness.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- <b>Note:</b> This problem fails to translate in Dymola 2012 due to an error in Dymola's support
- of stream connector. This bug will be corrected in future versions of Dymola.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+<b>Note:</b> This problem fails to translate in Dymola 2012 due to an error in Dymola's support
+of stream connector. This bug will be corrected in future versions of Dymola.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantEffectiveness;
diff --git a/AixLib/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlow.mo b/AixLib/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlow.mo
index 0a69e8ee9a..59c5b41efa 100644
--- a/AixLib/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlow.mo
+++ b/AixLib/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlow.mo
@@ -6,21 +6,21 @@ model ConstantEffectivenessZeroFlow
       height=0,
       offset=1E5), PIn(height=0, offset=101325));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- April 30, 2018, by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/907\">#907</a>.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model tests whether
- <a href=\"modelica://AixLib.Fluid.MassExchangers.ConstantEffectiveness\">ConstantEffectiveness</a>
- works correctly at zero flow if one stream is zero.
- </p>
- </html>"),experiment(Tolerance=1e-06, StopTime=1),
+<ul>
+<li>
+April 30, 2018, by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/907\">#907</a>.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model tests whether
+<a href=\"modelica://AixLib.Fluid.MassExchangers.ConstantEffectiveness\">ConstantEffectiveness</a>
+works correctly at zero flow if one stream is zero.
+</p>
+</html>"), experiment(Tolerance=1e-06, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlow.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantEffectivenessZeroFlow;
diff --git a/AixLib/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlowBothStreams.mo b/AixLib/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlowBothStreams.mo
index c89a4191a0..88c6ed7a99 100644
--- a/AixLib/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlowBothStreams.mo
+++ b/AixLib/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlowBothStreams.mo
@@ -9,21 +9,21 @@ model ConstantEffectivenessZeroFlowBothStreams
       height=0,
       offset=101325));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- May 7, 2018, by Michael Wetter:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/907\">#907</a>.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model tests whether
- <a href=\"modelica://AixLib.Fluid.MassExchangers.ConstantEffectiveness\">AixLib.Fluid.MassExchangers.ConstantEffectiveness</a>
- works correctly at zero flow if both streams are zero.
- </p>
- </html>"),experiment(Tolerance=1e-06, StopTime=1),
+<ul>
+<li>
+May 7, 2018, by Michael Wetter:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/907\">#907</a>.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model tests whether
+<a href=\"modelica://AixLib.Fluid.MassExchangers.ConstantEffectiveness\">AixLib.Fluid.MassExchangers.ConstantEffectiveness</a>
+works correctly at zero flow if both streams are zero.
+</p>
+</html>"), experiment(Tolerance=1e-06, StopTime=1),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MassExchangers/Validation/ConstantEffectivenessZeroFlowBothStreams.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ConstantEffectivenessZeroFlowBothStreams;
diff --git a/AixLib/Fluid/MixingVolumes/BaseClasses/MixingVolumeHeatMoisturePort.mo b/AixLib/Fluid/MixingVolumes/BaseClasses/MixingVolumeHeatMoisturePort.mo
index de60c9ffaf..519144ce62 100644
--- a/AixLib/Fluid/MixingVolumes/BaseClasses/MixingVolumeHeatMoisturePort.mo
+++ b/AixLib/Fluid/MixingVolumes/BaseClasses/MixingVolumeHeatMoisturePort.mo
@@ -45,40 +45,40 @@ equation
   annotation (
   defaultComponentName="vol",
   Documentation(info="<html>
- <p>
- Mixing volume with a heat port.
- </p>
- <p>
- This model is identical to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume\">
- AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume</a>,
- except that it has a heat and a moisture port.
- </p>
- <p>
- Note that this model is typically only used to implement new component models that
- have staggered volumes.
- In contrast to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir\">
- AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir</a>, it does
- not set <code>initialize_p</code> to <code>final</code> in order
- for this model to be usable in staggered volumes which require one
- pressure to be set to <code>initialize_p = not Medium.singleState</code>
- and all others to <code>false</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 9, 2021, by Michael Wetter:<br/>
- Corrected annotation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1547\">IBPSA, issue 1547</a>.
- </li>
- <li>
- October 23, 2017, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Mixing volume with a heat port.
+</p>
+<p>
+This model is identical to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume\">
+AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume</a>,
+except that it has a heat and a moisture port.
+</p>
+<p>
+Note that this model is typically only used to implement new component models that
+have staggered volumes.
+In contrast to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir\">
+AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir</a>, it does
+not set <code>initialize_p</code> to <code>final</code> in order
+for this model to be usable in staggered volumes which require one
+pressure to be set to <code>initialize_p = not Medium.singleState</code>
+and all others to <code>false</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 9, 2021, by Michael Wetter:<br/>
+Corrected annotation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1547\">IBPSA, issue 1547</a>.
+</li>
+<li>
+October 23, 2017, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeHeatMoisturePort;
diff --git a/AixLib/Fluid/MixingVolumes/BaseClasses/MixingVolumeHeatPort.mo b/AixLib/Fluid/MixingVolumes/BaseClasses/MixingVolumeHeatPort.mo
index 3822613fb5..26d515f556 100644
--- a/AixLib/Fluid/MixingVolumes/BaseClasses/MixingVolumeHeatPort.mo
+++ b/AixLib/Fluid/MixingVolumes/BaseClasses/MixingVolumeHeatPort.mo
@@ -12,40 +12,40 @@ equation
   annotation (
   defaultComponentName="vol",
   Documentation(info="<html>
- <p>
- Mixing volume with a heat port.
- </p>
- <p>
- This model is identical to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume\">
- AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume</a>,
- except that it has a heat port.
- </p>
- <p>
- Note that this model is typically only used to implement new component models that
- have staggered volumes.
- In contrast to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
- AixLib.Fluid.MixingVolumes.MixingVolume</a>, it does
- not set <code>initialize_p</code> to <code>final</code> in order
- for this model to be usable in staggered volumes which require one
- pressure to be set to <code>initialize_p = not Medium.singleState</code>
- and all others to <code>false</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 9, 2021, by Michael Wetter:<br/>
- Corrected annotation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1547\">IBPSA, issue 1547</a>.
- </li>
- <li>
- October 19, 2017, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Mixing volume with a heat port.
+</p>
+<p>
+This model is identical to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume\">
+AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume</a>,
+except that it has a heat port.
+</p>
+<p>
+Note that this model is typically only used to implement new component models that
+have staggered volumes.
+In contrast to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
+AixLib.Fluid.MixingVolumes.MixingVolume</a>, it does
+not set <code>initialize_p</code> to <code>final</code> in order
+for this model to be usable in staggered volumes which require one
+pressure to be set to <code>initialize_p = not Medium.singleState</code>
+and all others to <code>false</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 9, 2021, by Michael Wetter:<br/>
+Corrected annotation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1547\">IBPSA, issue 1547</a>.
+</li>
+<li>
+October 19, 2017, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeHeatPort;
diff --git a/AixLib/Fluid/MixingVolumes/BaseClasses/PartialMixingVolume.mo b/AixLib/Fluid/MixingVolumes/BaseClasses/PartialMixingVolume.mo
index 18a1a133fd..27529cc5dc 100644
--- a/AixLib/Fluid/MixingVolumes/BaseClasses/PartialMixingVolume.mo
+++ b/AixLib/Fluid/MixingVolumes/BaseClasses/PartialMixingVolume.mo
@@ -30,11 +30,17 @@ model PartialMixingVolume
     annotation(Dialog(tab="Assumptions"), Evaluate=true);
   parameter Modelica.Units.SI.Volume V "Volume";
   Modelica.Fluid.Vessels.BaseClasses.VesselFluidPorts_b ports[nPorts](
-      redeclare each package Medium = Medium) "Fluid inlets and outlets"
+      redeclare each package Medium = Medium,
+      each h_outflow(nominal=Medium.h_default),
+      each Xi_outflow(each nominal=0.01)
+      ) "Fluid inlets and outlets"
     annotation (Placement(transformation(extent={{-40,-10},{40,10}},
       origin={0,-100})));
 
-  Medium.Temperature T = Medium.temperature_phX(p=p, h=hOut_internal, X=cat(1,Xi,{1-sum(Xi)}))
+  Medium.Temperature T = Medium.temperature_phX(
+    p=p,
+    h=hOut_internal,
+    X=if Medium.reducedX then cat(1, Xi, {1-sum(Xi)}) else Xi)
     "Temperature of the fluid";
   Modelica.Blocks.Interfaces.RealOutput U(unit="J")
     "Internal energy of the component";
@@ -83,15 +89,15 @@ protected
     annotation (Placement(transformation(extent={{60,0},{80,20}})));
 
   // Density at start values, used to compute initial values and start guesses
-  parameter Modelica.Units.SI.Density rho_start=Medium.density(state=
-      state_start) "Density, used to compute start and guess values";
+  parameter Modelica.Units.SI.Density rho_start=Medium.density(
+    state=state_start) "Density, used to compute start and guess values";
   final parameter Medium.ThermodynamicState state_default = Medium.setState_pTX(
       T=Medium.T_default,
       p=Medium.p_default,
       X=Medium.X_default[1:Medium.nXi]) "Medium state at default values";
   // Density at medium default values, used to compute the size of control volumes
-  final parameter Modelica.Units.SI.Density rho_default=Medium.density(state=
-      state_default) "Density, used to compute fluid mass";
+  final parameter Modelica.Units.SI.Density rho_default=Medium.density(
+    state=state_default) "Density, used to compute fluid mass";
   final parameter Medium.ThermodynamicState state_start = Medium.setState_pTX(
       T=T_start,
       p=p_start,
@@ -116,12 +122,15 @@ protected
   Modelica.Blocks.Interfaces.RealOutput COut_internal[Medium.nC](each unit="1")
     "Internal connector for leaving trace substances of the component";
 
-  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature preTem
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature preTem(
+    port(T(start=T_start)))
     "Port temperature"
     annotation (Placement(transformation(extent={{-40,-10},{-60,10}})));
   Modelica.Blocks.Sources.RealExpression portT(y=T) "Port temperature"
     annotation (Placement(transformation(extent={{-10,-10},{-30,10}})));
-  Modelica.Thermal.HeatTransfer.Sensors.HeatFlowSensor heaFloSen
+  Modelica.Thermal.HeatTransfer.Sensors.HeatFlowSensor heaFloSen(
+    port_a(T(start=T_start)),
+    port_b(T(start=T_start)))
     "Heat flow sensor"
     annotation (Placement(transformation(extent={{-90,-10},{-70,10}})));
 equation
@@ -130,10 +139,10 @@ equation
   if not allowFlowReversal then
     assert(ports[1].m_flow > -m_flow_small,
   "In " + getInstanceName() + ": Model has flow reversal,
-   but the parameter allowFlowReversal is set to false.
-   m_flow_small    = "+ String(m_flow_small) + "
-   ports[1].m_flow = "+ String(ports[1].m_flow) + "
- ");
+  but the parameter allowFlowReversal is set to false.
+  m_flow_small    = " + String(m_flow_small) + "
+  ports[1].m_flow = " + String(ports[1].m_flow) + "
+");
   end if;
   // Actual definition of port variables.
   //
@@ -182,372 +191,384 @@ equation
   annotation (
 defaultComponentName="vol",
 Documentation(info="<html>
- <p>
- This is a partial model of an instantaneously mixed volume.
- It is used as the base class for all fluid volumes of the package
- <a href=\"modelica://AixLib.Fluid.MixingVolumes\">
- AixLib.Fluid.MixingVolumes</a>.
- </p>
- 
- 
- <h4>Typical use and important parameters</h4>
- <p>
- Set the constant <code>sensibleOnly=true</code> if the model that extends
- or instantiates this model sets <code>mWat_flow = 0</code>.
- </p>
- <p>
- Set the constant <code>simplify_mWat_flow = true</code> to simplify the equation
- </p>
- <pre>
-   port_a.m_flow + port_b.m_flow = - mWat_flow;
- </pre>
- <p>
- to
- </p>
- <pre>
-   port_a.m_flow + port_b.m_flow = 0;
- </pre>
- <p>
- This causes an error in the mass balance of about <i>0.5%</i>, but generally leads to
- simpler equations because the pressure drop equations are then decoupled from the
- mass exchange in this component.
- </p>
- 
- <p>
- To increase the numerical robustness of the model, the constant
- <code>prescribedHeatFlowRate</code> can be set by the user.
- This constant only has an effect if the model has exactly two fluid ports connected,
- and if it is used as a steady-state model.
- Use the following settings:
- </p>
- <ul>
- <li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
- at the <code>heatPort</code> is a prescribed heat flow rate that
- is <i>not</i> a function of the temperature difference
- between the medium and an ambient temperature. Examples include an ideal electrical heater,
- a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
- If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
- in this case, <code>heatPort.Q_flow=0</code>.
- </li>
- <li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
- computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
- which may itself be a function of temperature or mass flow rate.<br/>
- If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
- for example a solar collector that dissipates heat to the ambient and receives heat from
- the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
- </li>
- </ul>
- <p>
- Set the parameter <code>use_C_flow = true</code> to enable an input connector
- for the trace substance flow rate.
- </p>
- <h4>Implementation</h4>
- <p>
- If the model is (i) operated in steady-state,
- (ii) has two fluid ports connected, and
- (iii) <code>prescribedHeatFlowRate=true</code> or <code>allowFlowReversal=false</code>,
- then the model uses
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- in order to use
- the same energy and mass balance implementation as is used as in
- steady-state component models.
- In this situation, the functions <code>inStream</code> are used for the two
- flow directions rather than the function
- <code>actualStream</code>, which is less efficient.
- However, the use of <code>inStream</code> has the disadvantage
- that <code>hOut</code> has to be computed, in
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>,
- using
- </p>
- <pre>
- if allowFlowReversal then
-   hOut = AixLib.Utilities.Math.Functions.regStep(y1=port_b.h_outflow,
-                                                     y2=port_a.h_outflow,
-                                                     x=port_a.m_flow,
-                                                     x_small=m_flow_small/1E3);
- else
-   hOut = port_b.h_outflow;
- end if;
- </pre>
- <p>
- Hence, for <code>allowFlowReversal=true</code>, if <code>hOut</code>
- were to be used to compute the temperature that
- drives heat transfer such as by conduction,
- then the heat transfer would depend on upstream and the <i>downstream</i>
- temperatures for small mass flow rates.
- This can give wrong results. Consider for example a mass flow rate that is positive
- but very close to zero. Suppose the upstream temperature is <i>20</i>&deg;C,
- the downstream temperature is <i>10</i>&deg;C, and the heat port is
- connected through a heat conductor to a boundary condition of <i>20</i>&deg;C.
- Then, <code>hOut = (port_b.h_outflow + port_a.h_outflow)/2</code> and hence
- the temperature <code>heatPort.T</code>
- is <i>15</i>&deg;C. Therefore, heat is added to the component.
- As the mass flow rate is by assumption very small, the fluid that leaves the component
- will have a very high temperature, violating the 2nd law.
- To avoid this situation, if
- <code>prescribedHeatFlowRate=false</code>, then the model
- <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.ConservationEquation</a>
- is used instead of
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
- </p>
- <p>
- For simple models that uses this model, see
- <a href=\"modelica://AixLib.Fluid.MixingVolumes\">
- AixLib.Fluid.MixingVolumes</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 18, 2020, by Michael Wetter:<br/>
- Set start value for <code>steBal.hOut</code> so that <code>T_start</code>
- can be used which is not known in that instance.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1397\">#1397</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- October 30, 2019 by Filip Jorissen:<br/>
- Added <code>getInstanceName()</code> to flow
- reversal check.
- This if or <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1228\">
- issue 1228</a>.
- </li>
- <li>
- October 19, 2017, by Michael Wetter:<br/>
- Changed initialization of pressure from a <code>constant</code> to a <code>parameter</code>.<br/>
- Removed <code>partial</code> keyword as this model is not partial.<br/>
- Moved <code>C_flow</code> and <code>use_C_flow</code> to child classes.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- <li>
- April 11, 2017, by Michael Wetter:<br/>
- Moved heat port to the extending classes to provide better comment.
- Otherwise, the mixing volume without water input would have a comment
- that says latent heat can be added at this port.<br/>
- Removed blocks <code>QSen_flow</code> and
- <code>QLat_flow</code>.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- February 19, 2016 by Filip Jorissen:<br/>
- Added outputs U, m, mXi, mC for being able to
- check conservation of quantities.
- This if or <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">
- issue 247</a>.
- </li>
- <li>
- January 22, 2016 by Michael Wetter:<br/>
- Updated model to use the new parameter <code>use_mWat_flow</code>
- rather than <code>sensibleOnly</code>.
- </li>
- <li>
- January 17, 2016, by Michael Wetter:<br/>
- Removed <code>protected</code> block <code>masExc</code> as
- this revision introduces a conditional connector for the
- moisture flow rate in the energy and mass balance models.
- This change was done to use the same modeling concept for the
- moisture input as is used for the trace substance input.
- </li>
- <li>
- December 2, 2015, by Filip Jorissen:<br/>
- Added conditional input <code>C_flow</code> for
- handling trace substance insertions.
- </li>
- <li>
- July 17, 2015, by Michael Wetter:<br/>
- Added constant <code>simplify_mWat_flow</code> to remove dependencies of the pressure drop
- calculation on the moisture balance.
- </li>
- <li>
- July 1, 2015, by Filip Jorissen:<br/>
- Set <code>prescribedHeatFlowRate=prescribedHeatflowRate</code> for
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
- This results in equations that are solved more easily.
- See
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">
- issue 282</a> for a discussion.
- </li>
- <li>
- June 9, 2015 by Michael Wetter:<br/>
- Set start value for <code>heatPort.T</code> and changed
- type of <code>T</code> to <code>Medium.Temperature</code> rather than
- <code>Modelica.Units.SI.Temperature</code>
- to avoid an
- error because of conflicting start values if
- <code>AixLib.Fluid.Chillers.Carnot_y</code>
- is translated using pedantic mode in Dymola 2016.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
- </li>
- <li>
- June 5, 2015, by Michael Wetter:<br/>
- Moved assignment of <code>dynBal.U.start</code>
- from instance <code>dynBal</code> to the actual model implementation.
- This is required for a pedantic model check in Dymola 2016.
- It addresses
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">
- issue 266</a>.
- </li>
- <li>
- May 6, 2015, by Michael Wetter:<br/>
- Improved documentation and changed the test
- <pre>
-  final parameter Boolean useSteadyStateTwoPort=(nPorts == 2) and
-  prescribedHeatFlowRate and ...
- </pre>
- to
- <pre>
-  final parameter Boolean useSteadyStateTwoPort=(nPorts == 2) and
-  (prescribedHeatFlowRate or (not allowFlowReversal)) and ...
- </pre>
- The reason is that if there is no flow reversal, then
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- computes <code>hOut =  port_b.h_outflow;</code>, and hence
- it is correct to use <code>hOut</code> to compute
- temperature-driven heat flow, such as by conduction or convection.
- See also the model documentation.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">
- #412</a>.
- </li>
- <li>
- February 5, 2015, by Michael Wetter:<br/>
- Changed <code>initalize_p</code> from a <code>parameter</code> to a
- <code>constant</code>. This is only required in finite volume models
- of heat exchangers (to avoid consistent but redundant initial conditions)
- and hence it should be set as a <code>constant</code>.
- </li>
- <li>
- October 29, 2014, by Michael Wetter:<br/>
- Made assignment of <code>mFactor</code> final, and changed computation of
- density to use default medium states as are also used to compute the
- specific heat capacity.
- </li>
- <li>
- October 21, 2014, by Filip Jorissen:<br/>
- Added parameter <code>mFactor</code> to increase the thermal capacity.
- </li>
- <li>
- July 3, 2014, by Michael Wetter:<br/>
- Added parameter <code>initialize_p</code>. This is required
- to enable the coil models to initialize the pressure in the first
- volume, but not in the downstream volumes. Otherwise,
- the initial equations will be overdetermined, but consistent.
- This change was done to avoid a long information message that appears
- when translating models.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- February 11, 2014 by Michael Wetter:<br/>
- Removed <code>Q_flow</code> and added <code>QSen_flow</code>.
- This was done to clarify what is sensible and total heat flow rate
- as part of the correction of issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/197\">#197</a>.
- </li>
- <li>
- October 8, 2013 by Michael Wetter:<br/>
- Removed propagation of <code>show_V_flow</code>
- to instance <code>steBal</code> as it has no longer this parameter.
- </li>
- <li>
- September 13, 2013 by Michael Wetter:<br/>
- Renamed <code>rho_nominal</code> to <code>rho_start</code>
- because this quantity is computed using start values and not
- nominal values.
- </li>
- <li>
- April 18, 2013 by Michael Wetter:<br/>
- Removed the check of multiple connections to the same element
- of a fluid port, as this check required the use of the deprecated
- <code>cardinality</code> function.
- </li>
- <li>
- February 7, 2012 by Michael Wetter:<br/>
- Revised base classes for conservation equations in <code>AixLib.Fluid.Interfaces</code>.
- </li>
- <li>
- September 17, 2011 by Michael Wetter:<br/>
- Removed instance <code>medium</code> as this is already used in <code>dynBal</code>.
- Removing the base properties led to 30% faster computing time for a solar thermal system
- that contains many fluid volumes.
- </li>
- <li>
- September 13, 2011 by Michael Wetter:<br/>
- Changed in declaration of <code>medium</code> the parameter assignment
- <code>preferredMediumStates=true</code> to
- <code>preferredMediumStates= not (energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState)</code>.
- Otherwise, for a steady-state model, Dymola 2012 may differentiate the model to obtain <code>T</code>
- as a state. See ticket Dynasim #13596.
- </li>
- <li>
- July 26, 2011 by Michael Wetter:<br/>
- Revised model to use new declarations from
- <a href=\"AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
- AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
- </li>
- <li>
- July 14, 2011 by Michael Wetter:<br/>
- Added start values for mass and internal energy of dynamic balance
- model.
- </li>
- <li>
- May 25, 2011 by Michael Wetter:<br/>
- <ul>
- <li>
- Changed implementation of balance equation. The new implementation uses a different model if
- exactly two fluid ports are connected, and in addition, the model is used as a steady-state
- component. For this model configuration, the same balance equations are used as were used
- for steady-state component models, i.e., instead of <code>actualStream(...)</code>, the
- <code>inStream(...)</code> formulation is used.
- This changed required the introduction of a new parameter <code>m_flow_nominal</code> which
- is used for smoothing in the steady-state balance equations of the model with two fluid ports.
- This implementation also simplifies the implementation of
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort\">
- AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort</a>,
- which now uses the same equations as this model.
- </li>
- <li>
- Another revision was the removal of the parameter <code>use_HeatTransfer</code> as there is
- no noticeable overhead in always having the <code>heatPort</code> connector present.
- </li>
- </ul>
- </li>
- <li>
- July 30, 2010 by Michael Wetter:<br/>
- Added nominal value for <code>mC</code> to avoid wrong trajectory
- when concentration is around 1E-7.
- See also <a href=\"https://trac.modelica.org/Modelica/ticket/393\">
- https://trac.modelica.org/Modelica/ticket/393</a>.
- </li>
- <li>
- February 7, 2010 by Michael Wetter:<br/>
- Simplified model and its base classes by removing the port data
- and the vessel area.
- Eliminated the base class <code>PartialLumpedVessel</code>.
- </li>
- <li>
- October 12, 2009 by Michael Wetter:<br/>
- Changed base class to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.ClosedVolume\">
- AixLib.Fluid.MixingVolumes.BaseClasses.ClosedVolume</a>.
- </li>
- </ul>
- </html>"),
+<p>
+This is a partial model of an instantaneously mixed volume.
+It is used as the base class for all fluid volumes of the package
+<a href=\"modelica://AixLib.Fluid.MixingVolumes\">
+AixLib.Fluid.MixingVolumes</a>.
+</p>
+
+
+<h4>Typical use and important parameters</h4>
+<p>
+Set the constant <code>sensibleOnly=true</code> if the model that extends
+or instantiates this model sets <code>mWat_flow = 0</code>.
+</p>
+<p>
+Set the constant <code>simplify_mWat_flow = true</code> to simplify the equation
+</p>
+<pre>
+  port_a.m_flow + port_b.m_flow = - mWat_flow;
+</pre>
+<p>
+to
+</p>
+<pre>
+  port_a.m_flow + port_b.m_flow = 0;
+</pre>
+<p>
+This causes an error in the mass balance of about <i>0.5%</i>, but generally leads to
+simpler equations because the pressure drop equations are then decoupled from the
+mass exchange in this component.
+</p>
+
+<p>
+To increase the numerical robustness of the model, the constant
+<code>prescribedHeatFlowRate</code> can be set by the user.
+This constant only has an effect if the model has exactly two fluid ports connected,
+and if it is used as a steady-state model.
+Use the following settings:
+</p>
+<ul>
+<li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
+at the <code>heatPort</code> is a prescribed heat flow rate that
+is <i>not</i> a function of the temperature difference
+between the medium and an ambient temperature. Examples include an ideal electrical heater,
+a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
+If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
+in this case, <code>heatPort.Q_flow=0</code>.
+</li>
+<li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
+computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
+which may itself be a function of temperature or mass flow rate.<br/>
+If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
+for example a solar collector that dissipates heat to the ambient and receives heat from
+the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
+</li>
+</ul>
+<p>
+Set the parameter <code>use_C_flow = true</code> to enable an input connector
+for the trace substance flow rate.
+</p>
+<h4>Implementation</h4>
+<p>
+If the model is (i) operated in steady-state,
+(ii) has two fluid ports connected, and
+(iii) <code>prescribedHeatFlowRate=true</code> or <code>allowFlowReversal=false</code>,
+then the model uses
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+in order to use
+the same energy and mass balance implementation as is used as in
+steady-state component models.
+In this situation, the functions <code>inStream</code> are used for the two
+flow directions rather than the function
+<code>actualStream</code>, which is less efficient.
+However, the use of <code>inStream</code> has the disadvantage
+that <code>hOut</code> has to be computed, in
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>,
+using
+</p>
+<pre>
+if allowFlowReversal then
+  hOut = AixLib.Utilities.Math.Functions.regStep(y1=port_b.h_outflow,
+                                                    y2=port_a.h_outflow,
+                                                    x=port_a.m_flow,
+                                                    x_small=m_flow_small/1E3);
+else
+  hOut = port_b.h_outflow;
+end if;
+</pre>
+<p>
+Hence, for <code>allowFlowReversal=true</code>, if <code>hOut</code>
+were to be used to compute the temperature that
+drives heat transfer such as by conduction,
+then the heat transfer would depend on upstream and the <i>downstream</i>
+temperatures for small mass flow rates.
+This can give wrong results. Consider for example a mass flow rate that is positive
+but very close to zero. Suppose the upstream temperature is <i>20</i>&deg;C,
+the downstream temperature is <i>10</i>&deg;C, and the heat port is
+connected through a heat conductor to a boundary condition of <i>20</i>&deg;C.
+Then, <code>hOut = (port_b.h_outflow + port_a.h_outflow)/2</code> and hence
+the temperature <code>heatPort.T</code>
+is <i>15</i>&deg;C. Therefore, heat is added to the component.
+As the mass flow rate is by assumption very small, the fluid that leaves the component
+will have a very high temperature, violating the 2nd law.
+To avoid this situation, if
+<code>prescribedHeatFlowRate=false</code>, then the model
+<a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.ConservationEquation</a>
+is used instead of
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
+</p>
+<p>
+For simple models that uses this model, see
+<a href=\"modelica://AixLib.Fluid.MixingVolumes\">
+AixLib.Fluid.MixingVolumes</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+October 24, 2022, by Michael Wetter:<br/>
+Improved conversion from <code>Xi</code> to <code>X</code> so that it also works
+with media that have <code>reducedX=true</code>.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1650\">#1650</a>.
+</li>
+<li>
+September 18, 2020, by Michael Wetter:<br/>
+Set start value for <code>steBal.hOut</code> so that <code>T_start</code>
+can be used which is not known in that instance.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1397\">#1397</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+October 30, 2019 by Filip Jorissen:<br/>
+Added <code>getInstanceName()</code> to flow
+reversal check.
+This if or <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1228\">
+issue 1228</a>.
+</li>
+<li>
+October 19, 2017, by Michael Wetter:<br/>
+Changed initialization of pressure from a <code>constant</code> to a <code>parameter</code>.<br/>
+Removed <code>partial</code> keyword as this model is not partial.<br/>
+Moved <code>C_flow</code> and <code>use_C_flow</code> to child classes.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+<li>
+April 11, 2017, by Michael Wetter:<br/>
+Moved heat port to the extending classes to provide better comment.
+Otherwise, the mixing volume without water input would have a comment
+that says latent heat can be added at this port.<br/>
+Removed blocks <code>QSen_flow</code> and
+<code>QLat_flow</code>.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+February 19, 2016 by Filip Jorissen:<br/>
+Added outputs U, m, mXi, mC for being able to
+check conservation of quantities.
+This if or <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/247\">
+issue 247</a>.
+</li>
+<li>
+January 22, 2016 by Michael Wetter:<br/>
+Updated model to use the new parameter <code>use_mWat_flow</code>
+rather than <code>sensibleOnly</code>.
+</li>
+<li>
+January 17, 2016, by Michael Wetter:<br/>
+Removed <code>protected</code> block <code>masExc</code> as
+this revision introduces a conditional connector for the
+moisture flow rate in the energy and mass balance models.
+This change was done to use the same modeling concept for the
+moisture input as is used for the trace substance input.
+</li>
+<li>
+December 2, 2015, by Filip Jorissen:<br/>
+Added conditional input <code>C_flow</code> for
+handling trace substance insertions.
+</li>
+<li>
+July 17, 2015, by Michael Wetter:<br/>
+Added constant <code>simplify_mWat_flow</code> to remove dependencies of the pressure drop
+calculation on the moisture balance.
+</li>
+<li>
+July 1, 2015, by Filip Jorissen:<br/>
+Set <code>prescribedHeatFlowRate=prescribedHeatflowRate</code> for
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
+This results in equations that are solved more easily.
+See
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">
+issue 282</a> for a discussion.
+</li>
+<li>
+June 9, 2015 by Michael Wetter:<br/>
+Set start value for <code>heatPort.T</code> and changed
+type of <code>T</code> to <code>Medium.Temperature</code> rather than
+<code>Modelica.Units.SI.Temperature</code>
+to avoid an
+error because of conflicting start values if
+<code>AixLib.Fluid.Chillers.Carnot_y</code>
+is translated using pedantic mode in Dymola 2016.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/426\">#426</a>.
+</li>
+<li>
+June 5, 2015, by Michael Wetter:<br/>
+Moved assignment of <code>dynBal.U.start</code>
+from instance <code>dynBal</code> to the actual model implementation.
+This is required for a pedantic model check in Dymola 2016.
+It addresses
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">
+issue 266</a>.
+</li>
+<li>
+May 6, 2015, by Michael Wetter:<br/>
+Improved documentation and changed the test
+<pre>
+ final parameter Boolean useSteadyStateTwoPort=(nPorts == 2) and
+ prescribedHeatFlowRate and ...
+</pre>
+to
+<pre>
+ final parameter Boolean useSteadyStateTwoPort=(nPorts == 2) and
+ (prescribedHeatFlowRate or (not allowFlowReversal)) and ...
+</pre>
+The reason is that if there is no flow reversal, then
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+computes <code>hOut =  port_b.h_outflow;</code>, and hence
+it is correct to use <code>hOut</code> to compute
+temperature-driven heat flow, such as by conduction or convection.
+See also the model documentation.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/412\">
+#412</a>.
+</li>
+<li>
+February 5, 2015, by Michael Wetter:<br/>
+Changed <code>initalize_p</code> from a <code>parameter</code> to a
+<code>constant</code>. This is only required in finite volume models
+of heat exchangers (to avoid consistent but redundant initial conditions)
+and hence it should be set as a <code>constant</code>.
+</li>
+<li>
+October 29, 2014, by Michael Wetter:<br/>
+Made assignment of <code>mFactor</code> final, and changed computation of
+density to use default medium states as are also used to compute the
+specific heat capacity.
+</li>
+<li>
+October 21, 2014, by Filip Jorissen:<br/>
+Added parameter <code>mFactor</code> to increase the thermal capacity.
+</li>
+<li>
+July 3, 2014, by Michael Wetter:<br/>
+Added parameter <code>initialize_p</code>. This is required
+to enable the coil models to initialize the pressure in the first
+volume, but not in the downstream volumes. Otherwise,
+the initial equations will be overdetermined, but consistent.
+This change was done to avoid a long information message that appears
+when translating models.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+February 11, 2014 by Michael Wetter:<br/>
+Removed <code>Q_flow</code> and added <code>QSen_flow</code>.
+This was done to clarify what is sensible and total heat flow rate
+as part of the correction of issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/197\">#197</a>.
+</li>
+<li>
+October 8, 2013 by Michael Wetter:<br/>
+Removed propagation of <code>show_V_flow</code>
+to instance <code>steBal</code> as it has no longer this parameter.
+</li>
+<li>
+September 13, 2013 by Michael Wetter:<br/>
+Renamed <code>rho_nominal</code> to <code>rho_start</code>
+because this quantity is computed using start values and not
+nominal values.
+</li>
+<li>
+April 18, 2013 by Michael Wetter:<br/>
+Removed the check of multiple connections to the same element
+of a fluid port, as this check required the use of the deprecated
+<code>cardinality</code> function.
+</li>
+<li>
+February 7, 2012 by Michael Wetter:<br/>
+Revised base classes for conservation equations in <code>AixLib.Fluid.Interfaces</code>.
+</li>
+<li>
+September 17, 2011 by Michael Wetter:<br/>
+Removed instance <code>medium</code> as this is already used in <code>dynBal</code>.
+Removing the base properties led to 30% faster computing time for a solar thermal system
+that contains many fluid volumes.
+</li>
+<li>
+September 13, 2011 by Michael Wetter:<br/>
+Changed in declaration of <code>medium</code> the parameter assignment
+<code>preferredMediumStates=true</code> to
+<code>preferredMediumStates= not (energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState)</code>.
+Otherwise, for a steady-state model, Dymola 2012 may differentiate the model to obtain <code>T</code>
+as a state. See ticket Dynasim #13596.
+</li>
+<li>
+July 26, 2011 by Michael Wetter:<br/>
+Revised model to use new declarations from
+<a href=\"modelica://AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
+AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
+</li>
+<li>
+July 14, 2011 by Michael Wetter:<br/>
+Added start values for mass and internal energy of dynamic balance
+model.
+</li>
+<li>
+May 25, 2011 by Michael Wetter:<br/>
+<ul>
+<li>
+Changed implementation of balance equation. The new implementation uses a different model if
+exactly two fluid ports are connected, and in addition, the model is used as a steady-state
+component. For this model configuration, the same balance equations are used as were used
+for steady-state component models, i.e., instead of <code>actualStream(...)</code>, the
+<code>inStream(...)</code> formulation is used.
+This changed required the introduction of a new parameter <code>m_flow_nominal</code> which
+is used for smoothing in the steady-state balance equations of the model with two fluid ports.
+This implementation also simplifies the implementation of
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort\">
+AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort</a>,
+which now uses the same equations as this model.
+</li>
+<li>
+Another revision was the removal of the parameter <code>use_HeatTransfer</code> as there is
+no noticeable overhead in always having the <code>heatPort</code> connector present.
+</li>
+</ul>
+</li>
+<li>
+July 30, 2010 by Michael Wetter:<br/>
+Added nominal value for <code>mC</code> to avoid wrong trajectory
+when concentration is around 1E-7.
+See also <a href=\"https://trac.modelica.org/Modelica/ticket/393\">
+https://trac.modelica.org/Modelica/ticket/393</a>.
+</li>
+<li>
+February 7, 2010 by Michael Wetter:<br/>
+Simplified model and its base classes by removing the port data
+and the vessel area.
+Eliminated the base class <code>PartialLumpedVessel</code>.
+</li>
+<li>
+October 12, 2009 by Michael Wetter:<br/>
+Changed base class to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.ClosedVolume\">
+AixLib.Fluid.MixingVolumes.BaseClasses.ClosedVolume</a>.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={
        Text(
@@ -566,6 +587,6 @@ Documentation(info="<html>
         Text(
           extent={{62,28},{-58,-22}},
           textColor={255,255,255},
-          textString=DynamicSelect("", String(T-273.15, format=".1f")))}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString=DynamicSelect("", String(T-273.15, format=".1f")))}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialMixingVolume;
diff --git a/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatMoisturePort.mo b/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatMoisturePort.mo
index 8a6fb391b8..8afeea70b3 100644
--- a/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatMoisturePort.mo
+++ b/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatMoisturePort.mo
@@ -11,28 +11,28 @@ equation
   connect(const.y, vol.mWat_flow)
     annotation (Line(points={{-39,38},{-12,38}}, color={0,0,127}));
   annotation (Documentation(info="<html>
- <p>
- Model that validates that the initial conditions are uniquely set
- and not overdetermined.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 3, 2019 by Michael Wetter:<br/>
- Removed erroneous <code>each</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1068\">IBPSA, issue 1068</a>.
- </li>
- <li>
- October 23, 2017 by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Model that validates that the initial conditions are uniquely set
+and not overdetermined.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 3, 2019 by Michael Wetter:<br/>
+Removed erroneous <code>each</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1068\">IBPSA, issue 1068</a>.
+</li>
+<li>
+October 23, 2017 by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1E-6, StopTime=1.0),
 __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatMoisturePort.mos"
-  "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeHeatMoisturePort;
diff --git a/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortAir.mo b/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortAir.mo
index d7081c10dc..fe3ff6a4ab 100644
--- a/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortAir.mo
+++ b/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortAir.mo
@@ -5,22 +5,22 @@ model MixingVolumeHeatPortAir
     redeclare package Medium = AixLib.Media.Air);
 
   annotation (Documentation(info="<html>
- <p>
- Model that validates that the initial conditions are uniquely set
- and not overdetermined for water.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 23, 2017 by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Model that validates that the initial conditions are uniquely set
+and not overdetermined for water.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 23, 2017 by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1E-6, StopTime=1.0),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortAir.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeHeatPortAir;
diff --git a/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortWater.mo b/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortWater.mo
index 5671e54f02..58ed1b0800 100644
--- a/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortWater.mo
+++ b/AixLib/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortWater.mo
@@ -65,27 +65,27 @@ equation
                                                    color={0,127,255}));
 
   annotation (Documentation(info="<html>
- <p>
- Model that validates that the initial conditions are uniquely set
- and not overdetermined.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 3, 2017 by Michael Wetter:<br/>
- Corrected medium for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/850\">issue 850</a>.
- </li>
- <li>
- October 23, 2017 by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Model that validates that the initial conditions are uniquely set
+and not overdetermined.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 3, 2017 by Michael Wetter:<br/>
+Corrected medium for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/850\">issue 850</a>.
+</li>
+<li>
+October 23, 2017 by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1E-6, StopTime=1.0),
 __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/BaseClasses/Validation/MixingVolumeHeatPortWater.mos"
-  "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeHeatPortWater;
diff --git a/AixLib/Fluid/MixingVolumes/Examples/MixingVolumeHeatConduction.mo b/AixLib/Fluid/MixingVolumes/Examples/MixingVolumeHeatConduction.mo
index 64f4f5d1e4..0f0cf2b598 100644
--- a/AixLib/Fluid/MixingVolumes/Examples/MixingVolumeHeatConduction.mo
+++ b/AixLib/Fluid/MixingVolumes/Examples/MixingVolumeHeatConduction.mo
@@ -64,20 +64,20 @@ equation
       color={0,127,255}));
   annotation (Documentation(
         info="<html>
- <p>
- This model demonstrates the use of the mixing volume with heat conduction to the ambient.
- The mixing volume is configured as a steady-state model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 12, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the use of the mixing volume with heat conduction to the ambient.
+The mixing volume is configured as a steady-state model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 12, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1E-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Examples/MixingVolumeHeatConduction.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeHeatConduction;
diff --git a/AixLib/Fluid/MixingVolumes/Examples/MixingVolumeMoistAir.mo b/AixLib/Fluid/MixingVolumes/Examples/MixingVolumeMoistAir.mo
index 319e2ab52a..6afb4e1628 100644
--- a/AixLib/Fluid/MixingVolumes/Examples/MixingVolumeMoistAir.mo
+++ b/AixLib/Fluid/MixingVolumes/Examples/MixingVolumeMoistAir.mo
@@ -164,40 +164,40 @@ experiment(StopTime=600,
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Examples/MixingVolumeMoistAir.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir\">
- AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir</a>.
- After an initial transient, the temperature and humidity of the volume
- stabilizes.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 11, 2019 by Michael Wetter:<br/>
- Removed <code>each</code> statement.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1079\">#1079</a>.
- </li>
- <li>
- April 11, 2017, by Michael Wetter:<br/>
- Renamed variable used in result processing.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- February 11, 2014 by Michael Wetter:<br/>
- Changed
- <code>HWat_flow(y=vol1.HWat_flow)</code> to
- <code>QLat_flow(y=vol1.QLat_flow.y)</code>
- and
- <code>QWat</code> to <code>QLat</code>.
- </li>
- <li>
- October 12, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir\">
+AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir</a>.
+After an initial transient, the temperature and humidity of the volume
+stabilizes.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 11, 2019 by Michael Wetter:<br/>
+Removed <code>each</code> statement.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1079\">#1079</a>.
+</li>
+<li>
+April 11, 2017, by Michael Wetter:<br/>
+Renamed variable used in result processing.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+February 11, 2014 by Michael Wetter:<br/>
+Changed
+<code>HWat_flow(y=vol1.HWat_flow)</code> to
+<code>QLat_flow(y=vol1.QLat_flow.y)</code>
+and
+<code>QWat</code> to <code>QLat</code>.
+</li>
+<li>
+October 12, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeMoistAir;
diff --git a/AixLib/Fluid/MixingVolumes/Examples/MixingVolumePrescribedHeatFlowRate.mo b/AixLib/Fluid/MixingVolumes/Examples/MixingVolumePrescribedHeatFlowRate.mo
index d90e3086c0..2bd2a7b052 100644
--- a/AixLib/Fluid/MixingVolumes/Examples/MixingVolumePrescribedHeatFlowRate.mo
+++ b/AixLib/Fluid/MixingVolumes/Examples/MixingVolumePrescribedHeatFlowRate.mo
@@ -66,24 +66,24 @@ equation
       color={191,0,0}));
   annotation (Documentation(
         info="<html>
- <p>
- This model demonstrates the use of the mixing volume with a prescribed heat flow rate.
- The mixing volume is configured as a steady-state model.
- The heat flow rate is set to a very small value. This model is used to test
- convergence for the case the prescribed heat flow rate should be zero,
- but due to numerical solutions, it may have a small error that causes the signal to be
- non-zero.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 12, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the use of the mixing volume with a prescribed heat flow rate.
+The mixing volume is configured as a steady-state model.
+The heat flow rate is set to a very small value. This model is used to test
+convergence for the case the prescribed heat flow rate should be zero,
+but due to numerical solutions, it may have a small error that causes the signal to be
+non-zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 12, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1E-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Examples/MixingVolumePrescribedHeatFlowRate.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumePrescribedHeatFlowRate;
diff --git a/AixLib/Fluid/MixingVolumes/MixingVolume.mo b/AixLib/Fluid/MixingVolumes/MixingVolume.mo
index 5f9e4429f5..c92c756cef 100644
--- a/AixLib/Fluid/MixingVolumes/MixingVolume.mo
+++ b/AixLib/Fluid/MixingVolumes/MixingVolume.mo
@@ -28,228 +28,228 @@ equation
   annotation (
 defaultComponentName="vol",
 Documentation(info="<html>
- <p>
- This model represents an instantaneously mixed volume.
- Potential and kinetic energy at the port are neglected,
- and there is no pressure drop at the ports.
- The volume can exchange heat through its <code>heatPort</code>.
- </p>
- <p>
- The volume can be parameterized as a steady-state model or as
- dynamic model.</p>
- <p>
- To increase the numerical robustness of the model, the constant
- <code>prescribedHeatFlowRate</code> can be set by the user.
- This constant only has an effect if the model has exactly two fluid ports connected,
- and if it is used as a steady-state model.
- Use the following settings:
- </p>
- <ul>
- <li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
- at the <code>heatPort</code> is a prescribed heat flow rate that
- is <i>not</i> a function of the temperature difference
- between the medium and an ambient temperature. Examples include an ideal electrical heater,
- a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
- If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
- in this case, <code>heatPort.Q_flow=0</code>.
- </li>
- <li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
- computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
- which may itself be a function of temperature or mass flow rate.<br/>
- If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
- for example a solar collector that dissipates heat to the ambient and receives heat from
- the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
- </li>
- </ul>
- <h4>Options</h4>
- <p>
- The parameter <code>mSenFac</code> can be used to increase the thermal mass of this model
- without increasing its volume. This way, species concentrations are still calculated
- correctly even though the thermal mass increases. The additional thermal mass is calculated
- based on the density and the value of the function <code>HeatCapacityCp</code>
- of the medium state <code>state_default</code>. <br/>
- This parameter can for instance be useful in a pipe model when the developer wants to
- lump the pipe thermal mass to the fluid volume. By default <code>mSenFac = 1</code>, hence
- the mass is unchanged. For higher values of <code>mSenFac</code>, the mass will be scaled proportionally.
- </p>
- <p>
- Set the parameter <code>use_C_flow = true</code> to enable an input connector for the trace substance flow rate.
- This allows to directly add or subtract trace substances such as
- CO2 to the volume.
- See
- <a href=\"modelica://AixLib.Fluid.Sensors.Examples.PPM\">AixLib.Fluid.Sensors.Examples.PPM</a>
- for an example.
- </p>
- <h4>Implementation</h4>
- <p>
- If the model is operated in steady-state and has two fluid ports connected,
- then the same energy and mass balance implementation is used as in
- steady-state component models, i.e., the use of <code>actualStream</code>
- is not used for the properties at the port.
- </p>
- <p>
- The implementation of these balance equations is done in the instances
- <code>dynBal</code> for the dynamic balance and <code>steBal</code>
- for the steady-state balance. Both models use the same input variables:
- </p>
- <ul>
- <li>
- The variable <code>Q_flow</code> is used to add sensible <i>and</i> latent heat to the fluid.
- For example, <code>Q_flow</code> participates in the steady-state energy balance<pre>
-     port_b.h_outflow = inStream(port_a.h_outflow) + Q_flow * m_flowInv;
- </pre>
- where <code>m_flowInv</code> approximates the expression <code>1/m_flow</code>.
- </li>
- <li>
- The variable <code>mXi_flow</code> is used to add a species mass flow rate to the fluid.
- </li>
- </ul>
- <p>
- For the rationale of selecting different energy and mass balances, and for the
- use of <code>prescribedHeatFlowRate</code>, see the documentation of
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume\">
- AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume</a>.
- </p>
- <p>
- For simple models that uses this model, see
- <a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
- AixLib.Fluid.HeatExchangers.HeaterCooler_u</a> and
- <a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
- AixLib.Fluid.Humidifiers.Humidifier_u</a>.
- </p>
- 
- </html>",revisions="<html>
- <ul>
- <li>
- October 19, 2017, by Michael Wetter:<br/>
- Set <code>initialize_p</code> to <code>final</code> so that it does not
- appear as a user-selectable parameter. This is done because
- <code>initialize_p</code> has been changed from a <code>constant</code>
- to a <code>parameter</code> for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- <li>
- April 11, 2017, by Michael Wetter:<br/>
- Changed comment of heat port, as this needs to be the total heat flow
- rate in order to be able to use this model for modeling steam humidifiers
- and adiabatic humidifiers.<br/>
- Removed blocks <code>QSen_flow</code> and
- <code>QLat_flow</code>.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- January 19, 2016, by Michael Wetter:<br/>
- Updated documentation due to the addition of an input for trace substance
- in the mixing volume.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">
- issue 372</a>.
- </li>
- <li>
- January 17, 2016, by Michael Wetter:<br/>
- Removed <code>protected</code> block <code>masExc</code> as
- this revision introduces a conditional connector for the
- moisture flow rate in the energy and mass balance models.
- This change was done to use the same modeling concept for the
- moisture input as is used for the trace substance input.
- </li>
- <li>
- December 2, 2015, by Filip Jorissen:<br/>
- Changed code for handling trace substance insertions using input <code>C_flow</code>.
- </li>
- <li>
- May 1, 2015 by Michael Wetter<br/>
- Set <code>final</code> keyword for <code>masExc(final k=0)</code>.
- This addresses
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/230\">
- issue 230</a>.
- </li>
- <li>
- February 11, 2014 by Michael Wetter:<br/>
- Redesigned implementation of latent and sensible heat flow rates
- as port of the correction of issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/197\">#197</a>.
- </li>
- <li>
- February 7, 2012 by Michael Wetter:<br/>
- Revised base classes for conservation equations in <code>AixLib.Fluid.Interfaces</code>.
- </li>
- <li>
- September 17, 2011 by Michael Wetter:<br/>
- Removed instance <code>medium</code> as this is already used in <code>dynBal</code>.
- Removing the base properties led to 30% faster computing time for a solar thermal system
- that contains many fluid volumes.
- </li>
- <li>
- September 13, 2011 by Michael Wetter:<br/>
- Changed in declaration of <code>medium</code> the parameter assignment
- <code>preferredMediumStates=true</code> to
- <code>preferredMediumStates= not (energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState)</code>.
- Otherwise, for a steady-state model, Dymola 2012 may differentiate the model to obtain <code>T</code>
- as a state. See ticket Dynasim #13596.
- </li>
- <li>
- July 26, 2011 by Michael Wetter:<br/>
- Revised model to use new declarations from
- <a href=\"AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
- AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
- </li>
- <li>
- July 14, 2011 by Michael Wetter:<br/>
- Added start values for mass and internal energy of dynamic balance
- model.
- </li>
- <li>
- May 25, 2011 by Michael Wetter:<br/>
- <ul>
- <li>
- Changed implementation of balance equation. The new implementation uses a different model if
- exactly two fluid ports are connected, and in addition, the model is used as a steady-state
- component. For this model configuration, the same balance equations are used as were used
- for steady-state component models, i.e., instead of <code>actualStream(...)</code>, the
- <code>inStream(...)</code> formulation is used.
- This changed required the introduction of a new parameter <code>m_flow_nominal</code> which
- is used for smoothing in the steady-state balance equations of the model with two fluid ports.
- </li>
- <li>
- Another revision was the removal of the parameter <code>use_HeatTransfer</code> as there is
- no noticeable overhead in always having the <code>heatPort</code> connector present.
- </li>
- </ul>
- </li>
- <li>
- July 30, 2010 by Michael Wetter:<br/>
- Added nominal value for <code>mC</code> to avoid wrong trajectory
- when concentration is around 1E-7.
- See also <a href=\"https://trac.modelica.org/Modelica/ticket/393\">
- https://trac.modelica.org/Modelica/ticket/393</a>.
- </li>
- <li>
- February 7, 2010 by Michael Wetter:<br/>
- Simplified model and its base classes by removing the port data
- and the vessel area.
- Eliminated the base class <code>PartialLumpedVessel</code>.
- </li>
- <li>
- October 12, 2009 by Michael Wetter:<br/>
- Changed base class to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.ClosedVolume\">
- AixLib.Fluid.MixingVolumes.BaseClasses.ClosedVolume</a>.
- </li>
- </ul>
- </html>"),
+<p>
+This model represents an instantaneously mixed volume.
+Potential and kinetic energy at the port are neglected,
+and there is no pressure drop at the ports.
+The volume can exchange heat through its <code>heatPort</code>.
+</p>
+<p>
+The volume can be parameterized as a steady-state model or as
+dynamic model.</p>
+<p>
+To increase the numerical robustness of the model, the constant
+<code>prescribedHeatFlowRate</code> can be set by the user.
+This constant only has an effect if the model has exactly two fluid ports connected,
+and if it is used as a steady-state model.
+Use the following settings:
+</p>
+<ul>
+<li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
+at the <code>heatPort</code> is a prescribed heat flow rate that
+is <i>not</i> a function of the temperature difference
+between the medium and an ambient temperature. Examples include an ideal electrical heater,
+a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
+If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
+in this case, <code>heatPort.Q_flow=0</code>.
+</li>
+<li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
+computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
+which may itself be a function of temperature or mass flow rate.<br/>
+If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
+for example a solar collector that dissipates heat to the ambient and receives heat from
+the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
+</li>
+</ul>
+<h4>Options</h4>
+<p>
+The parameter <code>mSenFac</code> can be used to increase the thermal mass of this model
+without increasing its volume. This way, species concentrations are still calculated
+correctly even though the thermal mass increases. The additional thermal mass is calculated
+based on the density and the value of the function <code>HeatCapacityCp</code>
+of the medium state <code>state_default</code>. <br/>
+This parameter can for instance be useful in a pipe model when the developer wants to
+lump the pipe thermal mass to the fluid volume. By default <code>mSenFac = 1</code>, hence
+the mass is unchanged. For higher values of <code>mSenFac</code>, the mass will be scaled proportionally.
+</p>
+<p>
+Set the parameter <code>use_C_flow = true</code> to enable an input connector for the trace substance flow rate.
+This allows to directly add or subtract trace substances such as
+CO2 to the volume.
+See
+<a href=\"modelica://AixLib.Fluid.Sensors.Examples.PPM\">AixLib.Fluid.Sensors.Examples.PPM</a>
+for an example.
+</p>
+<h4>Implementation</h4>
+<p>
+If the model is operated in steady-state and has two fluid ports connected,
+then the same energy and mass balance implementation is used as in
+steady-state component models, i.e., the use of <code>actualStream</code>
+is not used for the properties at the port.
+</p>
+<p>
+The implementation of these balance equations is done in the instances
+<code>dynBal</code> for the dynamic balance and <code>steBal</code>
+for the steady-state balance. Both models use the same input variables:
+</p>
+<ul>
+<li>
+The variable <code>Q_flow</code> is used to add sensible <i>and</i> latent heat to the fluid.
+For example, <code>Q_flow</code> participates in the steady-state energy balance<pre>
+    port_b.h_outflow = inStream(port_a.h_outflow) + Q_flow * m_flowInv;
+</pre>
+where <code>m_flowInv</code> approximates the expression <code>1/m_flow</code>.
+</li>
+<li>
+The variable <code>mXi_flow</code> is used to add a species mass flow rate to the fluid.
+</li>
+</ul>
+<p>
+For the rationale of selecting different energy and mass balances, and for the
+use of <code>prescribedHeatFlowRate</code>, see the documentation of
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume\">
+AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolume</a>.
+</p>
+<p>
+For simple models that uses this model, see
+<a href=\"modelica://AixLib.Fluid.HeatExchangers.HeaterCooler_u\">
+AixLib.Fluid.HeatExchangers.HeaterCooler_u</a> and
+<a href=\"modelica://AixLib.Fluid.Humidifiers.Humidifier_u\">
+AixLib.Fluid.Humidifiers.Humidifier_u</a>.
+</p>
+
+</html>", revisions="<html>
+<ul>
+<li>
+October 19, 2017, by Michael Wetter:<br/>
+Set <code>initialize_p</code> to <code>final</code> so that it does not
+appear as a user-selectable parameter. This is done because
+<code>initialize_p</code> has been changed from a <code>constant</code>
+to a <code>parameter</code> for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+<li>
+April 11, 2017, by Michael Wetter:<br/>
+Changed comment of heat port, as this needs to be the total heat flow
+rate in order to be able to use this model for modeling steam humidifiers
+and adiabatic humidifiers.<br/>
+Removed blocks <code>QSen_flow</code> and
+<code>QLat_flow</code>.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+January 19, 2016, by Michael Wetter:<br/>
+Updated documentation due to the addition of an input for trace substance
+in the mixing volume.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">
+issue 372</a>.
+</li>
+<li>
+January 17, 2016, by Michael Wetter:<br/>
+Removed <code>protected</code> block <code>masExc</code> as
+this revision introduces a conditional connector for the
+moisture flow rate in the energy and mass balance models.
+This change was done to use the same modeling concept for the
+moisture input as is used for the trace substance input.
+</li>
+<li>
+December 2, 2015, by Filip Jorissen:<br/>
+Changed code for handling trace substance insertions using input <code>C_flow</code>.
+</li>
+<li>
+May 1, 2015 by Michael Wetter<br/>
+Set <code>final</code> keyword for <code>masExc(final k=0)</code>.
+This addresses
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/230\">
+issue 230</a>.
+</li>
+<li>
+February 11, 2014 by Michael Wetter:<br/>
+Redesigned implementation of latent and sensible heat flow rates
+as port of the correction of issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/197\">#197</a>.
+</li>
+<li>
+February 7, 2012 by Michael Wetter:<br/>
+Revised base classes for conservation equations in <code>AixLib.Fluid.Interfaces</code>.
+</li>
+<li>
+September 17, 2011 by Michael Wetter:<br/>
+Removed instance <code>medium</code> as this is already used in <code>dynBal</code>.
+Removing the base properties led to 30% faster computing time for a solar thermal system
+that contains many fluid volumes.
+</li>
+<li>
+September 13, 2011 by Michael Wetter:<br/>
+Changed in declaration of <code>medium</code> the parameter assignment
+<code>preferredMediumStates=true</code> to
+<code>preferredMediumStates= not (energyDynamics == Modelica.Fluid.Types.Dynamics.SteadyState)</code>.
+Otherwise, for a steady-state model, Dymola 2012 may differentiate the model to obtain <code>T</code>
+as a state. See ticket Dynasim #13596.
+</li>
+<li>
+July 26, 2011 by Michael Wetter:<br/>
+Revised model to use new declarations from
+<a href=\"modelica://AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
+AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
+</li>
+<li>
+July 14, 2011 by Michael Wetter:<br/>
+Added start values for mass and internal energy of dynamic balance
+model.
+</li>
+<li>
+May 25, 2011 by Michael Wetter:<br/>
+<ul>
+<li>
+Changed implementation of balance equation. The new implementation uses a different model if
+exactly two fluid ports are connected, and in addition, the model is used as a steady-state
+component. For this model configuration, the same balance equations are used as were used
+for steady-state component models, i.e., instead of <code>actualStream(...)</code>, the
+<code>inStream(...)</code> formulation is used.
+This changed required the introduction of a new parameter <code>m_flow_nominal</code> which
+is used for smoothing in the steady-state balance equations of the model with two fluid ports.
+</li>
+<li>
+Another revision was the removal of the parameter <code>use_HeatTransfer</code> as there is
+no noticeable overhead in always having the <code>heatPort</code> connector present.
+</li>
+</ul>
+</li>
+<li>
+July 30, 2010 by Michael Wetter:<br/>
+Added nominal value for <code>mC</code> to avoid wrong trajectory
+when concentration is around 1E-7.
+See also <a href=\"https://trac.modelica.org/Modelica/ticket/393\">
+https://trac.modelica.org/Modelica/ticket/393</a>.
+</li>
+<li>
+February 7, 2010 by Michael Wetter:<br/>
+Simplified model and its base classes by removing the port data
+and the vessel area.
+Eliminated the base class <code>PartialLumpedVessel</code>.
+</li>
+<li>
+October 12, 2009 by Michael Wetter:<br/>
+Changed base class to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.BaseClasses.ClosedVolume\">
+AixLib.Fluid.MixingVolumes.BaseClasses.ClosedVolume</a>.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}),
       graphics={
       Text(
           extent={{-152,100},{148,140}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolume;
diff --git a/AixLib/Fluid/MixingVolumes/MixingVolumeMoistAir.mo b/AixLib/Fluid/MixingVolumes/MixingVolumeMoistAir.mo
index 2fcab17643..ae9a158122 100644
--- a/AixLib/Fluid/MixingVolumes/MixingVolumeMoistAir.mo
+++ b/AixLib/Fluid/MixingVolumes/MixingVolumeMoistAir.mo
@@ -59,158 +59,158 @@ equation
           52,-60},{52,6},{58,6}}, color={0,0,127}));
   annotation (defaultComponentName="vol",
 Documentation(info="<html>
- <p>
- Model for an ideally mixed fluid volume and the ability
- to store mass and energy. The volume is fixed,
- and latent and sensible heat can be exchanged.
- </p>
- <p>
- This model represents the same physics as
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
- AixLib.Fluid.MixingVolumes.MixingVolume</a>, but in addition, it allows
- adding or subtracting water to the control volume.
- The mass flow rate of the added or subtracted water is
- specified at the port <code>mWat_flow</code>.
- Adding <code>mWat_flow</code> itself does not affect the energy balance
- in this model. Hence, the enthalpy that is added or removed with the
- flow of <code>mWat_flow</code> needs to be added to the heat port
- <code>heatPort</code>.
- </p>
- <p>
- To increase the numerical robustness of the model, the constant
- <code>prescribedHeatFlowRate</code> can be set by the user.
- This constant only has an effect if the model has exactly two fluid ports connected,
- and if it is used as a steady-state model.
- Use the following settings:
- </p>
- <ul>
- <li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
- at the <code>heatPort</code> is a prescribed heat flow rate that
- is <i>not</i> a function of the temperature difference
- between the medium and an ambient temperature. Examples include an ideal electrical heater,
- a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
- If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
- in this case, <code>heatPort.Q_flow=0</code>.
- </li>
- <li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
- computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
- which may itself be a function of temperature or mass flow rate.<br/>
- If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
- for example a solar collector that dissipates heat to the ambient and receives heat from
- the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
- </li>
- </ul>
- <h4>Options</h4>
- <p>
- The parameter <code>mSenFac</code> can be used to increase the thermal mass of this model
- without increasing its volume. This way, species concentrations are still calculated
- correctly even though the thermal mass increases. The additional thermal mass is calculated
- based on the density and the value of the function <code>HeatCapacityCp</code>
- of the medium state <code>state_default</code>. <br/>
- This parameter can for instance be useful in a pipe model when the developer wants to
- lump the pipe thermal mass to the fluid volume. By default <code>mSenFac = 1</code>, hence
- the mass is unchanged. For higher values of <code>mSenFac</code>, the mass will be scaled proportionally.
- </p>
- <p>
- Set the parameter <code>use_C_flow = true</code> to enable an input connector for the trace substance flow rate.
- This allows to directly add or subtract trace substances such as
- CO2 to the volume.
- See
- <a href=\"modelica://AixLib.Fluid.Sensors.Examples.PPM\">AixLib.Fluid.Sensors.Examples.PPM</a>
- for an example.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 19, 2017, by Michael Wetter:<br/>
- Set <code>initialize_p</code> to <code>final</code> so that it does not
- appear as a user-selectable parameter. This is done because
- <code>initialize_p</code> has been changed from a <code>constant</code>
- to a <code>parameter</code> for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
- </li>
- <li>
- April 11, 2017, by Michael Wetter:<br/>
- Changed comment of heat port, as this needs to be the total heat flow
- rate in order to be able to use this model for modeling steam humidifiers
- and adiabatic humidifiers.<br/>
- Removed blocks <code>QSen_flow</code> and
- <code>QLat_flow</code>.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- January 22, 2016 by Michael Wetter:<br/>
- Removed assignment of <code>sensibleOnly</code> in <code>steBal</code>
- as this constant is no longer used.
- </li>
- <li>
- January 19, 2016, by Michael Wetter:<br/>
- Updated documentation due to the addition of an input for trace substance
- in the mixing volume.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">
- issue 372</a>.
- </li>
- <li>
- February 11, 2014 by Michael Wetter:<br/>
- Redesigned implementation of latent and sensible heat flow rates
- as port of the correction of issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/197\">#197</a>.
- </li>
- <li>
- December 18, 2013 by Michael Wetter:<br/>
- Changed computation of <code>s</code> to allow this model to also be used
- with <code>AixLib.Media.Water</code>.
- </li>
- <li>
- October 21, 2013 by Michael Wetter:<br/>
- Removed dublicate declaration of medium model.
- </li>
- <li>
- September 27, 2013 by Michael Wetter:<br/>
- Reformulated assignment of <code>i_w</code> to avoid a warning in OpenModelica.
- </li>
- <li>
- September 17, 2013 by Michael Wetter:<br/>
- Changed model to no longer use the obsolete model <code>AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort</code>.
- </li>
- <li>
- July 30, 2013 by Michael Wetter:<br/>
- Changed connector <code>mXi_flow[Medium.nXi]</code>
- to a scalar input connector <code>mWat_flow</code>
- in the conservation equation model.
- The reason is that <code>mXi_flow</code> does not allow
- to compute the other components in <code>mX_flow</code> and
- therefore leads to an ambiguous use of the model.
- By only requesting <code>mWat_flow</code>, the mass balance
- and species balance can be implemented correctly.
- </li>
- <li>
- April 18, 2013 by Michael Wetter:<br/>
- Removed the use of the deprecated
- <code>cardinality</code> function.
- Therefore, all input signals must be connected.
- </li>
- <li>
- February 7, 2012 by Michael Wetter:<br/>
- Revised base classes for conservation equations in <code>AixLib.Fluid.Interfaces</code>.
- </li>
- <li>
- February 22, by Michael Wetter:<br/>
- Improved the code that searches for the index of 'water' in the medium model.
- </li>
- <li>
- May 29, 2010 by Michael Wetter:<br/>
- Rewrote computation of index of water substance.
- For the old formulation, Dymola 7.4 failed to differentiate the
- model when trying to reduce the index of the DAE.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Model for an ideally mixed fluid volume and the ability
+to store mass and energy. The volume is fixed,
+and latent and sensible heat can be exchanged.
+</p>
+<p>
+This model represents the same physics as
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
+AixLib.Fluid.MixingVolumes.MixingVolume</a>, but in addition, it allows
+adding or subtracting water to the control volume.
+The mass flow rate of the added or subtracted water is
+specified at the port <code>mWat_flow</code>.
+Adding <code>mWat_flow</code> itself does not affect the energy balance
+in this model. Hence, the enthalpy that is added or removed with the
+flow of <code>mWat_flow</code> needs to be added to the heat port
+<code>heatPort</code>.
+</p>
+<p>
+To increase the numerical robustness of the model, the constant
+<code>prescribedHeatFlowRate</code> can be set by the user.
+This constant only has an effect if the model has exactly two fluid ports connected,
+and if it is used as a steady-state model.
+Use the following settings:
+</p>
+<ul>
+<li>Set <code>prescribedHeatFlowRate=true</code> if the <i>only</i> means of heat transfer
+at the <code>heatPort</code> is a prescribed heat flow rate that
+is <i>not</i> a function of the temperature difference
+between the medium and an ambient temperature. Examples include an ideal electrical heater,
+a pump that rejects heat into the fluid stream, or a chiller that removes heat based on a performance curve.
+If the <code>heatPort</code> is not connected, then set <code>prescribedHeatFlowRate=true</code> as
+in this case, <code>heatPort.Q_flow=0</code>.
+</li>
+<li>Set <code>prescribedHeatFlowRate=false</code> if there is heat flow at the <code>heatPort</code>
+computed as <i>K * (T-heatPort.T)</i>, for some temperature <i>T</i> and some conductance <i>K</i>,
+which may itself be a function of temperature or mass flow rate.<br/>
+If there is a combination of <i>K * (T-heatPort.T)</i> and a prescribed heat flow rate,
+for example a solar collector that dissipates heat to the ambient and receives heat from
+the solar radiation, then set <code>prescribedHeatFlowRate=false</code>.
+</li>
+</ul>
+<h4>Options</h4>
+<p>
+The parameter <code>mSenFac</code> can be used to increase the thermal mass of this model
+without increasing its volume. This way, species concentrations are still calculated
+correctly even though the thermal mass increases. The additional thermal mass is calculated
+based on the density and the value of the function <code>HeatCapacityCp</code>
+of the medium state <code>state_default</code>. <br/>
+This parameter can for instance be useful in a pipe model when the developer wants to
+lump the pipe thermal mass to the fluid volume. By default <code>mSenFac = 1</code>, hence
+the mass is unchanged. For higher values of <code>mSenFac</code>, the mass will be scaled proportionally.
+</p>
+<p>
+Set the parameter <code>use_C_flow = true</code> to enable an input connector for the trace substance flow rate.
+This allows to directly add or subtract trace substances such as
+CO2 to the volume.
+See
+<a href=\"modelica://AixLib.Fluid.Sensors.Examples.PPM\">AixLib.Fluid.Sensors.Examples.PPM</a>
+for an example.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 19, 2017, by Michael Wetter:<br/>
+Set <code>initialize_p</code> to <code>final</code> so that it does not
+appear as a user-selectable parameter. This is done because
+<code>initialize_p</code> has been changed from a <code>constant</code>
+to a <code>parameter</code> for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1013\">Buildings, issue 1013</a>.
+</li>
+<li>
+April 11, 2017, by Michael Wetter:<br/>
+Changed comment of heat port, as this needs to be the total heat flow
+rate in order to be able to use this model for modeling steam humidifiers
+and adiabatic humidifiers.<br/>
+Removed blocks <code>QSen_flow</code> and
+<code>QLat_flow</code>.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+January 22, 2016 by Michael Wetter:<br/>
+Removed assignment of <code>sensibleOnly</code> in <code>steBal</code>
+as this constant is no longer used.
+</li>
+<li>
+January 19, 2016, by Michael Wetter:<br/>
+Updated documentation due to the addition of an input for trace substance
+in the mixing volume.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">
+issue 372</a>.
+</li>
+<li>
+February 11, 2014 by Michael Wetter:<br/>
+Redesigned implementation of latent and sensible heat flow rates
+as port of the correction of issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/197\">#197</a>.
+</li>
+<li>
+December 18, 2013 by Michael Wetter:<br/>
+Changed computation of <code>s</code> to allow this model to also be used
+with <code>AixLib.Media.Water</code>.
+</li>
+<li>
+October 21, 2013 by Michael Wetter:<br/>
+Removed dublicate declaration of medium model.
+</li>
+<li>
+September 27, 2013 by Michael Wetter:<br/>
+Reformulated assignment of <code>i_w</code> to avoid a warning in OpenModelica.
+</li>
+<li>
+September 17, 2013 by Michael Wetter:<br/>
+Changed model to no longer use the obsolete model <code>AixLib.Fluid.MixingVolumes.BaseClasses.PartialMixingVolumeWaterPort</code>.
+</li>
+<li>
+July 30, 2013 by Michael Wetter:<br/>
+Changed connector <code>mXi_flow[Medium.nXi]</code>
+to a scalar input connector <code>mWat_flow</code>
+in the conservation equation model.
+The reason is that <code>mXi_flow</code> does not allow
+to compute the other components in <code>mX_flow</code> and
+therefore leads to an ambiguous use of the model.
+By only requesting <code>mWat_flow</code>, the mass balance
+and species balance can be implemented correctly.
+</li>
+<li>
+April 18, 2013 by Michael Wetter:<br/>
+Removed the use of the deprecated
+<code>cardinality</code> function.
+Therefore, all input signals must be connected.
+</li>
+<li>
+February 7, 2012 by Michael Wetter:<br/>
+Revised base classes for conservation equations in <code>AixLib.Fluid.Interfaces</code>.
+</li>
+<li>
+February 22, by Michael Wetter:<br/>
+Improved the code that searches for the index of 'water' in the medium model.
+</li>
+<li>
+May 29, 2010 by Michael Wetter:<br/>
+Rewrote computation of index of water substance.
+For the old formulation, Dymola 7.4 failed to differentiate the
+model when trying to reduce the index of the DAE.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeMoistAir;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/MixingVolumeReverseFlow.mo b/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/MixingVolumeReverseFlow.mo
index 99d614dad9..3166ec9f02 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/MixingVolumeReverseFlow.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/MixingVolumeReverseFlow.mo
@@ -80,36 +80,36 @@ equation
           40}}, color={0,0,127}));
   annotation (Documentation(
         info="<html>
- <p>
- This model is the base class to validate
- the mixing volume with air flowing into and out of the volume
- and heat, moisture or trace substance added to the volume.
- </p>
- <p>
- The model <code>volDyn</code> uses a dynamic balance,
- whereas the model <code>volSte</code> uses a steady-state balance.
- The mass flow rate starts positive and reverses its direction at <i>t=5</i> seconds.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 29, 2021, by Michael Wetter:<br/>
- Reformulated constraint of replaceable model to avoid access of
- component that is not in constraining type.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1473\">IBPSA, #1473</a>.
- </li>
- <li>
- December 23, 2019, by Michael Wetter:<br/>
- Changed constraining clause to ensure that heat port is present.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1268\">IBPSA, #1268</a>.
- </li>
- <li>
- January 19, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model is the base class to validate
+the mixing volume with air flowing into and out of the volume
+and heat, moisture or trace substance added to the volume.
+</p>
+<p>
+The model <code>volDyn</code> uses a dynamic balance,
+whereas the model <code>volSte</code> uses a steady-state balance.
+The mass flow rate starts positive and reverses its direction at <i>t=5</i> seconds.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 29, 2021, by Michael Wetter:<br/>
+Reformulated constraint of replaceable model to avoid access of
+component that is not in constraining type.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1473\">IBPSA, #1473</a>.
+</li>
+<li>
+December 23, 2019, by Michael Wetter:<br/>
+Changed constraining clause to ensure that heat port is present.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1268\">IBPSA, #1268</a>.
+</li>
+<li>
+January 19, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeReverseFlow;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/MoistureMixingConservation.mo b/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/MoistureMixingConservation.mo
index 6fdcdca123..0d2ba8402c 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/MoistureMixingConservation.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/MoistureMixingConservation.mo
@@ -153,35 +153,35 @@ equation
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false,
           extent={{-100,-260},{160,100}})),
     Documentation(info="<html>
- <p>
- This is a partial model that is used in the validation tests
- of the mixing volume.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed temperature connection that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- November 15, 2016, by Michael Wetter:<br/>
- Changed model to be <code>partial</code> and removed the <code>experiment</code> annotation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/590\">issue 590</a>.
- </li>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- May 22 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a partial model that is used in the validation tests
+of the mixing volume.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed temperature connection that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+November 15, 2016, by Michael Wetter:<br/>
+Changed model to be <code>partial</code> and removed the <code>experiment</code> annotation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/590\">issue 590</a>.
+</li>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+May 22 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MoistureMixingConservation;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/TraceSubstanceConservation.mo b/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/TraceSubstanceConservation.mo
index 6f072ab455..267306d255 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/TraceSubstanceConservation.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/BaseClasses/TraceSubstanceConservation.mo
@@ -104,23 +104,23 @@ equation
       color={0,127,255},
       smooth=Smooth.None));
   annotation (    Documentation(info="<html>
- <p>
- This model is reconfigured to a steady state or
- dynamic check for conservation of trace substances.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed temperature connection that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- May 22 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model is reconfigured to a steady state or
+dynamic check for conservation of trace substances.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed temperature connection that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+May 22 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TraceSubstanceConservation;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesAir.mo b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesAir.mo
index 5867018bb8..bb62ad3901 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesAir.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesAir.mo
@@ -7,26 +7,26 @@ model CoupledVolumesAir
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Validation model for two directly coupled volumes.
- </p>
- <p>
- This tests whether a Modelica translator can perform the index reduction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 17, 2018, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for two directly coupled volumes.
+</p>
+<p>
+This tests whether a Modelica translator can perform the index reduction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 17, 2018, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=3600,
       Tolerance=1e-06),
     __Dymola_Commands(
       file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/CoupledVolumesAir.mos"
-           "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+           "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoupledVolumesAir;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesGlycol47.mo b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesGlycol47.mo
index efde3f0185..ed7b67a16f 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesGlycol47.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesGlycol47.mo
@@ -7,26 +7,26 @@ model CoupledVolumesGlycol47
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Validation model for two directly coupled volumes.
- </p>
- <p>
- This tests whether a Modelica translator can perform the index reduction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 17, 2018, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for two directly coupled volumes.
+</p>
+<p>
+This tests whether a Modelica translator can perform the index reduction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 17, 2018, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=3600,
       Tolerance=1e-06),
     __Dymola_Commands(
       file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/CoupledVolumesGlycol47.mos"
-           "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+           "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoupledVolumesGlycol47;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedAirPerfectGas.mo b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedAirPerfectGas.mo
index dae3f080b7..a32d1bea51 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedAirPerfectGas.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedAirPerfectGas.mo
@@ -8,26 +8,26 @@ model CoupledVolumesSpecializedAirPerfectGas
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Validation model for two directly coupled volumes.
- </p>
- <p>
- This tests whether a Modelica translator can perform the index reduction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 17, 2018, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for two directly coupled volumes.
+</p>
+<p>
+This tests whether a Modelica translator can perform the index reduction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 17, 2018, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=3600,
       Tolerance=1e-06),
     __Dymola_Commands(
       file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedAirPerfectGas.mos"
-           "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+           "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoupledVolumesSpecializedAirPerfectGas;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterConstantProperties_pT.mo b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterConstantProperties_pT.mo
index 9321503581..8df2b2dccd 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterConstantProperties_pT.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterConstantProperties_pT.mo
@@ -8,26 +8,26 @@ model CoupledVolumesSpecializedWaterConstantProperties_pT
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Validation model for two directly coupled volumes.
- </p>
- <p>
- This tests whether a Modelica translator can perform the index reduction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 17, 2018, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for two directly coupled volumes.
+</p>
+<p>
+This tests whether a Modelica translator can perform the index reduction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 17, 2018, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=3600,
       Tolerance=1e-06),
     __Dymola_Commands(
       file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterConstantProperties_pT.mos"
-           "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+           "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoupledVolumesSpecializedWaterConstantProperties_pT;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterTemperatureDependentDensity.mo b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterTemperatureDependentDensity.mo
index d5af933b6c..7ca4caf030 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterTemperatureDependentDensity.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterTemperatureDependentDensity.mo
@@ -8,26 +8,26 @@ model CoupledVolumesSpecializedWaterTemperatureDependentDensity
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Validation model for two directly coupled volumes.
- </p>
- <p>
- This tests whether a Modelica translator can perform the index reduction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 17, 2018, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for two directly coupled volumes.
+</p>
+<p>
+This tests whether a Modelica translator can perform the index reduction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 17, 2018, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=3600,
       Tolerance=1e-06),
     __Dymola_Commands(
       file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/CoupledVolumesSpecializedWaterTemperatureDependentDensity.mos"
-           "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+           "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoupledVolumesSpecializedWaterTemperatureDependentDensity;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesWater.mo b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesWater.mo
index 19ff7a8097..9f565e7035 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesWater.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/CoupledVolumesWater.mo
@@ -40,26 +40,26 @@ equation
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Validation model for two directly coupled volumes.
- </p>
- <p>
- This tests whether a Modelica translator can perform the index reduction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 17, 2018, by Michael Wetter:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for two directly coupled volumes.
+</p>
+<p>
+This tests whether a Modelica translator can perform the index reduction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 17, 2018, by Michael Wetter:<br/>
+First implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/910\">IBPSA, issue 910</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=3600,
       Tolerance=1e-06),
     __Dymola_Commands(
       file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/CoupledVolumesWater.mos"
-           "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+           "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CoupledVolumesWater;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MSLCombustionAir.mo b/AixLib/Fluid/MixingVolumes/Validation/MSLCombustionAir.mo
new file mode 100644
index 0000000000..90c72dd39a
--- /dev/null
+++ b/AixLib/Fluid/MixingVolumes/Validation/MSLCombustionAir.mo
@@ -0,0 +1,74 @@
+within AixLib.Fluid.MixingVolumes.Validation;
+model MSLCombustionAir
+  "Test model with medium for combustion air from the Modelica Standard Library"
+    extends Modelica.Icons.Example;
+
+  replaceable package Medium =
+      Modelica.Media.IdealGases.MixtureGases.CombustionAir;
+
+  parameter Modelica.Units.SI.PressureDifference dp_nominal=10
+    "Nominal pressure drop";
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=10
+    "Nominal mass flow rate";
+
+  AixLib.Fluid.FixedResistances.PressureDrop res(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dp_nominal=dp_nominal)
+    "Pressure drop"
+    annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  AixLib.Fluid.Sources.MassFlowSource_T masFloSou(
+    redeclare package Medium = Medium,
+    m_flow=m_flow_nominal,
+    nPorts=1) "Mass flow source"
+    annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
+  AixLib.Fluid.Sources.Boundary_pT bou(
+    redeclare package Medium = Medium,
+    p=Medium.p_default + dp_nominal,
+    nPorts=1)
+    "Pressure boundary condition"
+    annotation (Placement(transformation(extent={{60,-10},{40,10}})));
+  AixLib.Fluid.MixingVolumes.MixingVolume vol(
+    redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    m_flow_nominal=m_flow_nominal,
+    V=1,
+    nPorts=2)
+    "Control volume"
+    annotation (Placement(transformation(extent={{-40,20},{-20,40}})));
+equation
+  connect(res.port_b, bou.ports[1])
+    annotation (Line(points={{20,0},{40,0}}, color={0,127,255}));
+  connect(masFloSou.ports[1], vol.ports[1])
+    annotation (Line(points={{-60,0},{-31,0},{-31,20}}, color={0,127,255}));
+  connect(vol.ports[2], res.port_a) annotation (
+    Line(points = {{-29, 20}, {-29, 0}, {0, 0}}, color = {0, 127, 255}));
+  annotation (
+  experiment(
+    Tolerance=1E-6,
+    StopTime=1),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MSLCombustionAir.mos"
+        "Simulate and plot"),
+    Documentation(
+info = "<html>
+<p>
+This model verifies that basic fluid flow components also
+work with a medium model from the Modelica Standard Library
+for combustion air.
+</p>
+<p>
+This medium differs from media in the AixLib library in that it has no substance <code>water</code>
+and it sets <code>reducedX=false</code>.
+</p>
+</html>",
+revisions = "<html>
+<ul>
+<li>
+October 24, 2022, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1650\">#1650</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end MSLCombustionAir;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MSLFlueGasSixComponents.mo b/AixLib/Fluid/MixingVolumes/Validation/MSLFlueGasSixComponents.mo
new file mode 100644
index 0000000000..b4ca4a58bc
--- /dev/null
+++ b/AixLib/Fluid/MixingVolumes/Validation/MSLFlueGasSixComponents.mo
@@ -0,0 +1,35 @@
+within AixLib.Fluid.MixingVolumes.Validation;
+model MSLFlueGasSixComponents
+  "Test model with medium for flue gas from the Modelica Standard Library"
+    extends AixLib.Fluid.MixingVolumes.Validation.MSLCombustionAir(
+      redeclare package Medium =
+        Modelica.Media.IdealGases.MixtureGases.FlueGasSixComponents);
+
+  annotation (
+  experiment(
+    Tolerance=1E-6,
+    StopTime=1),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MSLFlueGasSixComponents.mos"
+        "Simulate and plot"),
+    Documentation(
+info = "<html>
+<p>
+This model verifies that basic fluid flow components also
+work with a medium model from the Modelica Standard Library
+for flue gas with six components.
+</p>
+<p>
+This medium differs from media in the AixLib library in that it sets <code>reducedX=false</code>.
+</p>
+</html>",
+revisions = "<html>
+<ul>
+<li>
+October 24, 2022, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1650\">#1650</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end MSLFlueGasSixComponents;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolume.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolume.mo
index 48d452a1ce..58e5c14f3d 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolume.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolume.mo
@@ -171,50 +171,50 @@ experiment(Tolerance=1E-9, StopTime=2),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolume.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of the mixing volumes.
- It compares the results from the mixing volume of the Modelica
- Standard Library with the implementation in the <code>Buildings</code>
- library.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed temperature connection that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- January 12, 2017, by Thierry S. Nouidui:<br/>
- Refactored difference blocks for checking integration errors.
- This is needed for the JModelica verification tests.
- </li>
- <li>
- November 4, 2016, by Michael Wetter:<br/>
- Removed wrong use of <code>each</code> keyword.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/575\">issue 575</a>.
- </li>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- October 24, 2013, by Michael Wetter:<br/>
- Set <code>vol(h_start=45300.945)</code>.
- This avoids a cyclic assignment of <code>vol.T_start</code>
- and <code>vol.h_start</code> in
- <code>Modelica.Fluid.Vessels.ClosedVolume</code>.
- </li>
- <li>
- October 12, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of the mixing volumes.
+It compares the results from the mixing volume of the Modelica
+Standard Library with the implementation in the <code>Buildings</code>
+library.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed temperature connection that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+January 12, 2017, by Thierry S. Nouidui:<br/>
+Refactored difference blocks for checking integration errors.
+This is needed for the JModelica verification tests.
+</li>
+<li>
+November 4, 2016, by Michael Wetter:<br/>
+Removed wrong use of <code>each</code> keyword.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/575\">issue 575</a>.
+</li>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+October 24, 2013, by Michael Wetter:<br/>
+Set <code>vol(h_start=45300.945)</code>.
+This avoids a cyclic assignment of <code>vol.T_start</code>
+and <code>vol.h_start</code> in
+<code>Modelica.Fluid.Vessels.ClosedVolume</code>.
+</li>
+<li>
+October 12, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolume;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeAdiabaticCooling.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeAdiabaticCooling.mo
index 4e190a9e54..8a42f9e6df 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeAdiabaticCooling.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeAdiabaticCooling.mo
@@ -43,38 +43,38 @@ equation
           {66,-2},{58,-2},{58,-48},{30,-48},{30,-38}}, color={0,127,255}));
 annotation (Documentation(
         info="<html>
- <p>
- This model validates the use of the mixing volume with adiabatic cooling.
- Water in liquid form at room temperature is added to the volume,
- which decreases its temperature.
- The instance <code>volSim</code> uses a simplified implementation of the
- mass balance that ignores the mass of the water added to the volume,
- whereas the instance <code>volExa</code> uses the exact formulation.
- The output of the instance <code>relErr</code>
- shows that the relative error on the temperature difference between these
- two options is less than <i>0.1%</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 2, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed temperature connection that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- May 2, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model validates the use of the mixing volume with adiabatic cooling.
+Water in liquid form at room temperature is added to the volume,
+which decreases its temperature.
+The instance <code>volSim</code> uses a simplified implementation of the
+mass balance that ignores the mass of the water added to the volume,
+whereas the instance <code>volExa</code> uses the exact formulation.
+The output of the instance <code>relErr</code>
+shows that the relative error on the temperature difference between these
+two options is less than <i>0.1%</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 2, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed temperature connection that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+May 2, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeAdiabaticCooling.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeAdiabaticCooling;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlow.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlow.mo
index 3abffb8a16..263d80a7f4 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlow.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlow.mo
@@ -22,25 +22,25 @@ equation
           40},{26,28},{-2,28},{-2,-40},{10,-40}}, color={191,0,0}));
 annotation (Documentation(
         info="<html>
- <p>
- This model validates the use of the mixing volume with air flowing into and out of the volume
- and sensible heat added to the volume.
- </p>
- <p>
- The model <code>volDyn</code> uses a dynamic balance,
- whereas the model <code>volSte</code> uses a steady-state balance.
- The mass flow rate starts positive and reverses its direction at <i>t=5</i> seconds.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 9, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model validates the use of the mixing volume with air flowing into and out of the volume
+and sensible heat added to the volume.
+</p>
+<p>
+The model <code>volDyn</code> uses a dynamic balance,
+whereas the model <code>volSte</code> uses a steady-state balance.
+The mass flow rate starts positive and reverses its direction at <i>t=5</i> seconds.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlow.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-08, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-08, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeHeatReverseFlow;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlowPrescribedHeatFlowRate.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlowPrescribedHeatFlowRate.mo
index fd2dbf0dce..b39394e407 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlowPrescribedHeatFlowRate.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlowPrescribedHeatFlowRate.mo
@@ -6,28 +6,28 @@ model MixingVolumeHeatReverseFlowPrescribedHeatFlowRate
 
   annotation (Documentation(
 info="<html>
- <p>
- This model is identical to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeHeatReverseFlow\">
- AixLib.Fluid.MixingVolumes.Validation.MixingVolumeHeatReverseFlow</a>,
- except that the steady state volume <code>volSte</code>
- is configured to have a prescribed heat flow rate,
- which is in this case zero as the heat port is not connected.
- This configures <code>volSte</code> to use the two port
- steady state heat and mass balance model
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 9, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model is identical to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeHeatReverseFlow\">
+AixLib.Fluid.MixingVolumes.Validation.MixingVolumeHeatReverseFlow</a>,
+except that the steady state volume <code>volSte</code>
+is configured to have a prescribed heat flow rate,
+which is in this case zero as the heat port is not connected.
+This configures <code>volSte</code> to use the two port
+steady state heat and mass balance model
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeHeatReverseFlowPrescribedHeatFlowRate.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeHeatReverseFlowPrescribedHeatFlowRate;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeInitialization.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeInitialization.mo
index 58d3005bfe..0b7a248f15 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeInitialization.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeInitialization.mo
@@ -55,24 +55,24 @@ experiment(StopTime=0.001,
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeInitialization.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the initialization of the mixing volume.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 24, 2013 by Michael Wetter:<br/>
- Set <code>flowModel(m_flow_nominal=2)</code> in the pipe models to
- avoid a cyclic definition of
- <code>pipe1.flowModel.m_flow_nominal</code>
- and
- <code>pipe2.flowModel.m_flow_nominal</code>.
- </li>
- <li>
- October 12, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the initialization of the mixing volume.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 24, 2013 by Michael Wetter:<br/>
+Set <code>flowModel(m_flow_nominal=2)</code> in the pipe models to
+avoid a cyclic definition of
+<code>pipe1.flowModel.m_flow_nominal</code>
+and
+<code>pipe2.flowModel.m_flow_nominal</code>.
+</li>
+<li>
+October 12, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeInitialization;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMFactor.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMFactor.mo
index cf3b98ff10..255b864a2f 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMFactor.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMFactor.mo
@@ -49,49 +49,49 @@ equation
   connect(bou.ports[3], vol1.ports[2]) annotation (Line(points={{40,1.33227e-15},
           {20,1.33227e-15},{20,-80},{2,-80}}, color={0,127,255}));
   annotation (Documentation(info="<html>
- <p>This model contains two verifications for the implementation of <code>mSenFac</code>:</p>
- <ol>
- <li>
- The mixingVolume temperature <code>vol.T</code> should be constant.
- This is to check the correct implementation of the parameter <code>mSenFac</code> for moist air media.
- </li>
- <li>
- The temperature response of <code>volMFactor.T</code> and <code>vol1.T</code> should be nearly identical.
- Furthermore the response of the species concentration <code>Xi</code> demonstrates the
- difference between using an <code>mSenFac = 10</code> and multiplying volume by <i>10</i>.
- </li>
- </ol>
- <p>
- See
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeMassFlow\">
- AixLib.Fluid.MixingVolumes.Validation.MixingVolumeMassFlow</a>
- for the rational of the selected initial conditions for the volumes.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 27, 2015 by Michael Wetter:<br/>
- Set the mass dynamics of the volume to
- <code>Modelica.Fluid.Types.Dynamics.DynamicFreeInitial</code>
- to avoid an overspecified but consistent initial value problem.
- The previous implementation caused a warning in Dymola 2015 FD01, and caused
- in Dymola 2016 beta 2 to not translate the model.
- The problem was that the boundary condition and the volume
- both declared an equation for the initial pressure.
- </li>
- <li>
- December, 2014 by Filip Jorissen:<br/>
- Added temperature verification.
- </li>
- <li>
- November 25, 2014 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>This model contains two verifications for the implementation of <code>mSenFac</code>:</p>
+<ol>
+<li>
+The mixingVolume temperature <code>vol.T</code> should be constant.
+This is to check the correct implementation of the parameter <code>mSenFac</code> for moist air media.
+</li>
+<li>
+The temperature response of <code>volMFactor.T</code> and <code>vol1.T</code> should be nearly identical.
+Furthermore the response of the species concentration <code>Xi</code> demonstrates the
+difference between using an <code>mSenFac = 10</code> and multiplying volume by <i>10</i>.
+</li>
+</ol>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeMassFlow\">
+AixLib.Fluid.MixingVolumes.Validation.MixingVolumeMassFlow</a>
+for the rational of the selected initial conditions for the volumes.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 27, 2015 by Michael Wetter:<br/>
+Set the mass dynamics of the volume to
+<code>Modelica.Fluid.Types.Dynamics.DynamicFreeInitial</code>
+to avoid an overspecified but consistent initial value problem.
+The previous implementation caused a warning in Dymola 2015 FD01, and caused
+in Dymola 2016 beta 2 to not translate the model.
+The problem was that the boundary condition and the volume
+both declared an equation for the initial pressure.
+</li>
+<li>
+December, 2014 by Filip Jorissen:<br/>
+Added temperature verification.
+</li>
+<li>
+November 25, 2014 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1E-6, StopTime=100),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeMFactor.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeMFactor;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMassFlow.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMassFlow.mo
index 28090d3a9b..550e5d648b 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMassFlow.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMassFlow.mo
@@ -41,46 +41,46 @@ equation
     annotation (Line(points={{40,0},{2,0}}, color={0,127,255}));
   annotation (Documentation(
         info="<html>
- <p>
- This model demonstrates the use of the mixing volume with air flowing into and out of the volume.
- </p>
- <p>
- The initial conditions for the volume is declared as fixed initial
- values for the energy dynamics, but free initial conditions
- for the mass dynamics. The reason for leaving the initial conditions
- unspecified for the mass dynamics is that the sink <code>bou</code>
- declares the pressure of the fluid. As there is no flow resistance
- between that boundary condition and the volume,
- the volume has the same pressure. Therefore, specifying an
- initial condition for the mass dynamics would yield to an overspecified
- initial value problem for the pressure of the medium.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- March 27, 2015 by Michael Wetter:<br/>
- Set the mass dynamics of the volume to
- <code>Modelica.Fluid.Types.Dynamics.DynamicFreeInitial</code>
- to avoid an overspecified but consistent initial value problem.
- The previous implementation caused a warning in Dymola 2015 FD01, and caused
- in Dymola 2016 beta 2 to not translate the model.
- The problem was that the boundary condition and the volume
- both declared an equation for the initial pressure.
- </li>
- <li>
- October 12, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the use of the mixing volume with air flowing into and out of the volume.
+</p>
+<p>
+The initial conditions for the volume is declared as fixed initial
+values for the energy dynamics, but free initial conditions
+for the mass dynamics. The reason for leaving the initial conditions
+unspecified for the mass dynamics is that the sink <code>bou</code>
+declares the pressure of the fluid. As there is no flow resistance
+between that boundary condition and the volume,
+the volume has the same pressure. Therefore, specifying an
+initial condition for the mass dynamics would yield to an overspecified
+initial value problem for the pressure of the medium.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+March 27, 2015 by Michael Wetter:<br/>
+Set the mass dynamics of the volume to
+<code>Modelica.Fluid.Types.Dynamics.DynamicFreeInitial</code>
+to avoid an overspecified but consistent initial value problem.
+The previous implementation caused a warning in Dymola 2015 FD01, and caused
+in Dymola 2016 beta 2 to not translate the model.
+The problem was that the boundary condition and the volume
+both declared an equation for the initial pressure.
+</li>
+<li>
+October 12, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeMassFlow.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1E-6, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1E-6, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeMassFlow;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlow.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlow.mo
index 34294e7ed5..3ce9d1bafd 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlow.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlow.mo
@@ -14,31 +14,31 @@ equation
           -10,-32},{8,-32}}, color={0,0,127}));
   annotation (Documentation(
         info="<html>
- <p>
- This model validates the use of the mixing volume with air flowing into and out of the volume
- and moisture added to the volume.
- </p>
- <p>
- The model <code>volDyn</code> uses a dynamic balance,
- whereas the model <code>volSte</code> uses a steady-state balance.
- The mass flow rate starts positive and reverses its direction at <i>t=5</i> seconds.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 12, 2017, by Michael Wetter:<br/>
- Removed temperature connection that is no longer needed.<br/>
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
- </li>
- <li>
- March 9, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model validates the use of the mixing volume with air flowing into and out of the volume
+and moisture added to the volume.
+</p>
+<p>
+The model <code>volDyn</code> uses a dynamic balance,
+whereas the model <code>volSte</code> uses a steady-state balance.
+The mass flow rate starts positive and reverses its direction at <i>t=5</i> seconds.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 12, 2017, by Michael Wetter:<br/>
+Removed temperature connection that is no longer needed.<br/>
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings #704</a>.
+</li>
+<li>
+March 9, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlow.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeMoistureReverseFlow;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlowPrescribedHeatFlowRate.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlowPrescribedHeatFlowRate.mo
index 1ee94dab6b..45deb4d019 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlowPrescribedHeatFlowRate.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlowPrescribedHeatFlowRate.mo
@@ -5,28 +5,28 @@ model MixingVolumeMoistureReverseFlowPrescribedHeatFlowRate
     prescribedHeatFlowRate=true);
   annotation (Documentation(
 info="<html>
- <p>
- This model is identical to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeMoistureReverseFlow\">
- AixLib.Fluid.MixingVolumes.Validation.MixingVolumeMoistureReverseFlow</a>,
- except that the steady state volume <code>volSte</code>
- is configured to have a prescribed heat flow rate,
- which is in this case zero as the heat port is not connected.
- This configures <code>volSte</code> to use the two port
- steady state heat and mass balance model
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 9, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model is identical to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeMoistureReverseFlow\">
+AixLib.Fluid.MixingVolumes.Validation.MixingVolumeMoistureReverseFlow</a>,
+except that the steady state volume <code>volSte</code>
+is configured to have a prescribed heat flow rate,
+which is in this case zero as the heat port is not connected.
+This configures <code>volSte</code> to use the two port
+steady state heat and mass balance model
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeMoistureReverseFlowPrescribedHeatFlowRate.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeMoistureReverseFlowPrescribedHeatFlowRate;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeSteadyStateMass.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeSteadyStateMass.mo
index 5027113874..39e33829f8 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeSteadyStateMass.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeSteadyStateMass.mo
@@ -57,22 +57,22 @@ equation
       color={0,127,255}));
   annotation (Documentation(
         info="<html>
- <p>
- This model shows that steady state mass dynamics are correctly simulated.
- A change in pressure does not lead to an exchange and/or creation of mass.
- The mixing volume temperature is also unaffected by a pressure change.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 9, 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model shows that steady state mass dynamics are correctly simulated.
+A change in pressure does not lead to an exchange and/or creation of mass.
+The mixing volume temperature is also unaffected by a pressure change.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1E-6, StopTime=1.0),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeSteadyStateMass.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeSteadyStateMass;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstance.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstance.mo
index 1b9ab5d643..641e94d2d6 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstance.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstance.mo
@@ -70,24 +70,24 @@ equation
           {20,-10},{20,-18},{40,-18}}, color={0,127,255}));
   annotation (Documentation(
         info="<html>
- <p>
- This model demonstrates the use of the mixing volume with air flowing into and out of the volume
- and trace substances added to the volume.
- </p>
- <p>
- The model <code>volDyn</code> uses a dynamic balance,
- whereas the model <code>volSte</code> uses a steady-state balance.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 19, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the use of the mixing volume with air flowing into and out of the volume
+and trace substances added to the volume.
+</p>
+<p>
+The model <code>volDyn</code> uses a dynamic balance,
+whereas the model <code>volSte</code> uses a steady-state balance.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 19, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstance.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeTraceSubstance;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlow.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlow.mo
index 4d8746bf82..9110ed6e34 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlow.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlow.mo
@@ -16,32 +16,32 @@ equation
           -10,4},{8,4}}, color={0,0,127}));
 annotation (Documentation(
         info="<html>
- <p>
- This model validates the use of the mixing volume with air flowing into and out of the volume
- and trace substances added to the volume.
- </p>
- <p>
- The model <code>volDyn</code> uses a dynamic balance,
- whereas the model <code>volSte</code> uses a steady-state balance.
- The mass flow rate starts positive and reverses its direction at <i>t=5</i> seconds.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 7, 2016, by Michael Wetter:<br/>
- Set <code>bou(C={0.003})</code> to avoid a negative value for
- <code>C_outflow</code> of the steady state volume.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/613\">#613</a>.
- </li>
- <li>
- January 19, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model validates the use of the mixing volume with air flowing into and out of the volume
+and trace substances added to the volume.
+</p>
+<p>
+The model <code>volDyn</code> uses a dynamic balance,
+whereas the model <code>volSte</code> uses a steady-state balance.
+The mass flow rate starts positive and reverses its direction at <i>t=5</i> seconds.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 7, 2016, by Michael Wetter:<br/>
+Set <code>bou(C={0.003})</code> to avoid a negative value for
+<code>C_outflow</code> of the steady state volume.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/613\">#613</a>.
+</li>
+<li>
+January 19, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlow.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-08, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-08, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeTraceSubstanceReverseFlow;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlowPrescribedHeatFlowRate.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlowPrescribedHeatFlowRate.mo
index e0baa51b64..ad393f5143 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlowPrescribedHeatFlowRate.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlowPrescribedHeatFlowRate.mo
@@ -5,28 +5,28 @@ model MixingVolumeTraceSubstanceReverseFlowPrescribedHeatFlowRate
     prescribedHeatFlowRate=true);
   annotation (Documentation(
 info="<html>
- <p>
- This model is identical to
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeTraceSubstanceReverseFlow\">
- AixLib.Fluid.MixingVolumes.Validation.MixingVolumeTraceSubstanceReverseFlow</a>,
- except that the steady state volume <code>volSte</code>
- is configured to have a prescribed heat flow rate,
- which is in this case zero as the heat port is not connected.
- This configures <code>volSte</code> to use the two port
- steady state heat and mass balance model
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 9, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model is identical to
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.Validation.MixingVolumeTraceSubstanceReverseFlow\">
+AixLib.Fluid.MixingVolumes.Validation.MixingVolumeTraceSubstanceReverseFlow</a>,
+except that the steady state volume <code>volSte</code>
+is configured to have a prescribed heat flow rate,
+which is in this case zero as the heat port is not connected.
+This configures <code>volSte</code> to use the two port
+steady state heat and mass balance model
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeTraceSubstanceReverseFlowPrescribedHeatFlowRate.mos"
         "Simulate and plot"),
-    experiment(Tolerance=1e-6, StopTime=10),
-  __Dymola_LockedEditing="Model from IBPSA");
+    experiment(Tolerance=1e-6, StopTime=10), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeTraceSubstanceReverseFlowPrescribedHeatFlowRate;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeZeroFlow.mo b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeZeroFlow.mo
index 7c0ac0b63f..4ff0fd3273 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeZeroFlow.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MixingVolumeZeroFlow.mo
@@ -173,58 +173,58 @@ equation
     experiment(
       Tolerance=1E-6, StopTime=2),
     Documentation(revisions="<html>
- <ul>
- <li>
- January 27, 2016, by Filip Jorissen:<br/>
- Changed heat flow rate at zero flow to avoid triggering of
- conservation of energy check.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/470\">
- issue 470</a>.
- </li>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Removed assertion as the variable that are tested are already
- part of the regression test.
- Also, the previous implementation mixed graphical with textual programming,
- which we try to avoid.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/441\">issue 441</a>.
- </li>
- <li>
- January 27, 2016, by Michael Wetter:<br/>
- Removed algorithm specification in experiment annotation.
- </li>
- <li>
- July 2, 2015 by Michael Wetter:<br/>
- Revised example.
- </li>
- <li>
- June 30, 2015 by Filip Jorissen:<br/>
- First implementation
- to test
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">
- issue 282</a>.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model verifies whether the equations in
- <a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- are consisent for all foreseeable cases.
- All <code>MixingVolume</code> instances contain the correct
- setting for <code>prescribedHeatFlowRate</code>.
- Switching the value will result in an error in each case.
- This error either is a non-physical solution to the (non-)linear system
- or a division by zero, which halts the simulation.
- </p>
- <p>
- If you use Dymola, set <code>Advanced.Define.AimForHighAccuracy = false</code> to
- increase the chance of the error being produced for this simple example.
- </p>
- </html>"),
+<ul>
+<li>
+January 27, 2016, by Filip Jorissen:<br/>
+Changed heat flow rate at zero flow to avoid triggering of
+conservation of energy check.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/470\">
+issue 470</a>.
+</li>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Removed assertion as the variable that are tested are already
+part of the regression test.
+Also, the previous implementation mixed graphical with textual programming,
+which we try to avoid.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/441\">issue 441</a>.
+</li>
+<li>
+January 27, 2016, by Michael Wetter:<br/>
+Removed algorithm specification in experiment annotation.
+</li>
+<li>
+July 2, 2015 by Michael Wetter:<br/>
+Revised example.
+</li>
+<li>
+June 30, 2015 by Filip Jorissen:<br/>
+First implementation
+to test
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/282\">
+issue 282</a>.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model verifies whether the equations in
+<a href=\"modelica://AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+are consisent for all foreseeable cases.
+All <code>MixingVolume</code> instances contain the correct
+setting for <code>prescribedHeatFlowRate</code>.
+Switching the value will result in an error in each case.
+This error either is a non-physical solution to the (non-)linear system
+or a division by zero, which halts the simulation.
+</p>
+<p>
+If you use Dymola, set <code>Advanced.Define.AimForHighAccuracy = false</code> to
+increase the chance of the error being produced for this simple example.
+</p>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MixingVolumeZeroFlow.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MixingVolumeZeroFlow;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MoistureMixingConservationDynamicBalance.mo b/AixLib/Fluid/MixingVolumes/Validation/MoistureMixingConservationDynamicBalance.mo
index 2622497360..004f5ebccb 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MoistureMixingConservationDynamicBalance.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MoistureMixingConservationDynamicBalance.mo
@@ -192,50 +192,50 @@ equation
                                                             color={0,0,127}));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,
             -280},{180,120}})),           Documentation(info="<html>
- <p>
- This model verifies if mass and energy are conserved,
- using a dynamic balance.
- Two air streams with different mass flow rate are humidified
- by a mixing volume with two different vapor mass flow rates.
- These flows are then mixed.
- Boundary integrals are used to verify if air mass,
- vapour mass and internal energy are conserved.
- </p>
- <p>
- Note, however, that there is some approximation error because
- in its default configuration, the conservation balance
- models simplify the treatment of the water that is added
- to the fluid.
- See <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- and
- <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- for a discussion.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 24, 2017, by Michael Wetter:<br/>
- Removed enthalpy of liquid from <code>entIn</code>.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings, #704</a>.
- </li>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- May 22 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model verifies if mass and energy are conserved,
+using a dynamic balance.
+Two air streams with different mass flow rate are humidified
+by a mixing volume with two different vapor mass flow rates.
+These flows are then mixed.
+Boundary integrals are used to verify if air mass,
+vapour mass and internal energy are conserved.
+</p>
+<p>
+Note, however, that there is some approximation error because
+in its default configuration, the conservation balance
+models simplify the treatment of the water that is added
+to the fluid.
+See <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+and
+<a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+for a discussion.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 24, 2017, by Michael Wetter:<br/>
+Removed enthalpy of liquid from <code>entIn</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/704\">Buildings, #704</a>.
+</li>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+May 22 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MoistureMixingConservationDynamicBalance.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MoistureMixingConservationDynamicBalance;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/MoistureMixingConservationSteadyState.mo b/AixLib/Fluid/MixingVolumes/Validation/MoistureMixingConservationSteadyState.mo
index fce4c3400c..b28cce870a 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/MoistureMixingConservationSteadyState.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/MoistureMixingConservationSteadyState.mo
@@ -24,43 +24,43 @@ equation
           extent={{-120,-280},{180,120}}), graphics),
     experiment(Tolerance=1e-6, StopTime=1),
     Documentation(info="<html>
- <p>
- This test checks if water vapour mass is conserved.
- Two air streams with different mass flow rate are humidified
- by a mixing volume with two different vapor mass flow rates.
- These flows are then mixed.
- Afterwards the added water is removed again.
- The final water concentration, mass flow rate and enthalpy
- flow rate should then be equal to the initial values.
- </p>
- <p>
- Note, however, that there is some approximation error because
- in its default configuration, the conservation balance
- models simplify the treatment of the water that is added
- to the fluid.
- See <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- and
- <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- for a discussion.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- May 22 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This test checks if water vapour mass is conserved.
+Two air streams with different mass flow rate are humidified
+by a mixing volume with two different vapor mass flow rates.
+These flows are then mixed.
+Afterwards the added water is removed again.
+The final water concentration, mass flow rate and enthalpy
+flow rate should then be equal to the initial values.
+</p>
+<p>
+Note, however, that there is some approximation error because
+in its default configuration, the conservation balance
+models simplify the treatment of the water that is added
+to the fluid.
+See <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+and
+<a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+for a discussion.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+May 22 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MoistureMixingConservationSteadyState.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MoistureMixingConservationSteadyState;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/TraceSubstanceConservationDynamicBalance.mo b/AixLib/Fluid/MixingVolumes/Validation/TraceSubstanceConservationDynamicBalance.mo
index e294b26953..6eee7bb6b2 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/TraceSubstanceConservationDynamicBalance.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/TraceSubstanceConservationDynamicBalance.mo
@@ -62,47 +62,47 @@ equation
       smooth=Smooth.None));
   annotation (    experiment(Tolerance=1e-08, StopTime=1),
     Documentation(info="<html>
- <p>
- This test checks if the trace substance flow rate is
- conserved when adding moisture to a mixing volume that is configured to steady state.<br/>
- The trace substance flow rate at the inlet and outlet should be equal
- since the trace substance concentration should not
- be affected by the independent mass fraction concentration.
- </p>
- <p>
- Note, however, that there is some approximation error because
- in its default configuration, the conservation balance
- models simplify the treatment of the water that is added
- to the fluid.
- See <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- and
- <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- for a discussion.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Removed wrong assignment for <code>C_nominal</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/568\">issue 568</a>.
- </li>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- May 22 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This test checks if the trace substance flow rate is
+conserved when adding moisture to a mixing volume that is configured to steady state.<br/>
+The trace substance flow rate at the inlet and outlet should be equal
+since the trace substance concentration should not
+be affected by the independent mass fraction concentration.
+</p>
+<p>
+Note, however, that there is some approximation error because
+in its default configuration, the conservation balance
+models simplify the treatment of the water that is added
+to the fluid.
+See <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+and
+<a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+for a discussion.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Removed wrong assignment for <code>C_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/568\">issue 568</a>.
+</li>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+May 22 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/TraceSubstanceConservationDynamicBalance.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TraceSubstanceConservationDynamicBalance;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/TraceSubstanceConservationSteadyState.mo b/AixLib/Fluid/MixingVolumes/Validation/TraceSubstanceConservationSteadyState.mo
index 77e7e0cd62..062331bf40 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/TraceSubstanceConservationSteadyState.mo
+++ b/AixLib/Fluid/MixingVolumes/Validation/TraceSubstanceConservationSteadyState.mo
@@ -32,41 +32,41 @@ equation
       smooth=Smooth.None));
   annotation (    experiment(Tolerance=1e-6, StopTime=2),
     Documentation(info="<html>
- <p>
- This test checks if the trace substance flow rate is conserved
- when adding moisture to a mixing volume that is configured to steady state.<br/>
- The trace substance flow rate at the inlet and outlet should be equal
- since the trace substance concentration should not
- be affected by the independent mass fraction concentration.
- </p>
- <p>
- Note, however, that there is some approximation error because
- in its default configuration, the conservation balance
- models simplify the treatment of the water that is added
- to the fluid.
- See <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- and
- <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
- AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
- for a discussion.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- May 22 2015 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This test checks if the trace substance flow rate is conserved
+when adding moisture to a mixing volume that is configured to steady state.<br/>
+The trace substance flow rate at the inlet and outlet should be equal
+since the trace substance concentration should not
+be affected by the independent mass fraction concentration.
+</p>
+<p>
+Note, however, that there is some approximation error because
+in its default configuration, the conservation balance
+models simplify the treatment of the water that is added
+to the fluid.
+See <a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+and
+<a href=\"modelica://AixLib.Fluid.Interfaces.ConservationEquation\">
+AixLib.Fluid.Interfaces.StaticTwoPortConservationEquation</a>
+for a discussion.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+May 22 2015 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/TraceSubstanceConservationSteadyState.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TraceSubstanceConservationSteadyState;
diff --git a/AixLib/Fluid/MixingVolumes/Validation/package.order b/AixLib/Fluid/MixingVolumes/Validation/package.order
index 3c4b18718d..9f3850820f 100644
--- a/AixLib/Fluid/MixingVolumes/Validation/package.order
+++ b/AixLib/Fluid/MixingVolumes/Validation/package.order
@@ -4,6 +4,8 @@ CoupledVolumesSpecializedAirPerfectGas
 CoupledVolumesSpecializedWaterConstantProperties_pT
 CoupledVolumesSpecializedWaterTemperatureDependentDensity
 CoupledVolumesWater
+MSLCombustionAir
+MSLFlueGasSixComponents
 MixingVolume
 MixingVolumeAdiabaticCooling
 MixingVolumeHeatReverseFlow
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiency.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiency.mo
index 9201eea99c..49365bb25b 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiency.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiency.mo
@@ -5,8 +5,8 @@ function efficiency "Flow vs. efficiency characteristics for fan or pump"
     "Efficiency performance data";
   input Modelica.Units.SI.VolumeFlowRate V_flow "Volumetric flow rate";
   input Real d[:] "Derivatives at support points for spline interpolation";
-  input Real r_N(unit="1") "Relative revolution, r_N=N/N_nominal";
-  input Real delta "Small value for switching implementation around zero rpm";
+  input Real r_N(unit="1") "Relative speed";
+  input Real delta "Small value for switching implementation around zero speed";
   output Real eta(unit="1", final quantity="Efficiency") "Efficiency";
 
 protected
@@ -17,8 +17,8 @@ algorithm
   if n == 1 then
     eta := per.eta[1];
   else
-    // The use of the max function to avoids problems for low speeds
-    // and turned off pumps
+    // The use of the max function avoids problems with low speeds
+    // and turned-off pumps
     rat:=V_flow/
             AixLib.Utilities.Math.Functions.smoothMax(
               x1=r_N,
@@ -43,59 +43,59 @@ algorithm
 
   annotation(smoothOrder=1,
               Documentation(info="<html>
- <p>
- This function computes the fan or pump efficiency for given normalized volume flow rate
- and performance data. The efficiency is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &eta; = s(V&#775;/r<sub>N</sub>, d),
- </p>
- <p>
- where
- <i>&eta;</i> is the efficiency,
- <i>r<sub>N</sub></i> is the normalized fan speed,
- <i>V&#775;</i> is the volume flow rate, and
- <i>d</i> are performance data for fan or pump efficiency.
- </p>
- <h4>Implementation</h4>
- <p>
- The function <i>s(&middot;, &middot;)</i> is a cubic hermite spline.
- If the data <i>d</i> define a monotone decreasing sequence, then
- <i>s(&middot;, d)</i> is a monotone decreasing function.
- </p>
- </html>",
+<p>
+This function computes the fan or pump efficiency for given normalized volume flow rate
+and performance data. The efficiency is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &eta; = s(V&#775;/r<sub>N</sub>, d),
+</p>
+<p>
+where
+<i>&eta;</i> is the efficiency,
+<i>r<sub>N</sub></i> is the normalized fan speed,
+<i>V&#775;</i> is the volume flow rate, and
+<i>d</i> are performance data for fan or pump efficiency.
+</p>
+<h4>Implementation</h4>
+<p>
+The function <i>s(&middot;, &middot;)</i> is a cubic hermite spline.
+If the data <i>d</i> define a monotone decreasing sequence, then
+<i>s(&middot;, d)</i> is a monotone decreasing function.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 2, 2016, by Michael Wetter:<br/>
- Removed <code>min</code> attribute as otherwise numerical noise can cause
- the assertion on the limit to fail.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
- </li>
- <li>
- November 22, 2014, by Michael Wetter:<br/>
- Corrected documentation as curve uses <i>V&#775;</i>
- as an independent variable.
- </li>
- <li>
- September 30, 2014, by Filip Jorissen:<br/>
- Changed polynomial to be evaluated at <code>V_flow</code>
- instead of <code>r_V</code>.
- </li>
- <li>
- April 19, 2014, by Filip Jorissen:<br/>
- Changed polynomial to be evaluated at <code>r_V/r_N</code>
- instead of <code>r_V</code> to properly account for the
- scaling law. See
- <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
- for a discussion and validation.
- </li>
- <li>
- September 28, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 2, 2016, by Michael Wetter:<br/>
+Removed <code>min</code> attribute as otherwise numerical noise can cause
+the assertion on the limit to fail.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
+</li>
+<li>
+November 22, 2014, by Michael Wetter:<br/>
+Corrected documentation as curve uses <i>V&#775;</i>
+as an independent variable.
+</li>
+<li>
+September 30, 2014, by Filip Jorissen:<br/>
+Changed polynomial to be evaluated at <code>V_flow</code>
+instead of <code>r_V</code>.
+</li>
+<li>
+April 19, 2014, by Filip Jorissen:<br/>
+Changed polynomial to be evaluated at <code>r_V/r_N</code>
+instead of <code>r_V</code> to properly account for the
+scaling law. See
+<a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
+for a discussion and validation.
+</li>
+<li>
+September 28, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end efficiency;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiencyParameters.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiencyParameters.mo
index 863111a11d..019586eceb 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiencyParameters.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiencyParameters.mo
@@ -1,27 +1,28 @@
 within AixLib.Fluid.Movers.BaseClasses.Characteristics;
-record efficiencyParameters "Record for efficiency parameters"
+record efficiencyParameters
+  "Record for efficiency parameters vs. volumetric flow rate"
   extends Modelica.Icons.Record;
   parameter Modelica.Units.SI.VolumeFlowRate V_flow[:](each min=0)
     "Volumetric flow rate at user-selected operating points";
   parameter Modelica.Units.SI.Efficiency eta[size(V_flow, 1)](each max=1)
     "Fan or pump efficiency at these flow rates";
   annotation (Documentation(info="<html>
- <p>
- Data record for performance data that describe volume flow rate versus
- efficiency.
- The volume flow rate <code>r_V</code> must be increasing, i.e.,
- <code>r_V[i] &lt; r_V[i+1]</code>.
- Both vectors, <code>r_V</code> and <code>eta</code>
- must have the same size.
- </p>
- </html>",
+<p>
+Data record for performance data that describe efficiency
+versus volumetric flow rate.
+The volume flow rate <code>r_V</code> must be increasing, i.e.,
+<code>V_flow[i] &lt; V_flow[i+1]</code>.
+Both vectors, <code>V_flow</code> and <code>eta</code>
+must have the same size.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 28, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 28, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end efficiencyParameters;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiencyParameters_yMot.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiencyParameters_yMot.mo
new file mode 100644
index 0000000000..6198add6a4
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiencyParameters_yMot.mo
@@ -0,0 +1,28 @@
+within AixLib.Fluid.Movers.BaseClasses.Characteristics;
+record efficiencyParameters_yMot
+  "Record for efficiency parameters vs. motor part load ratio"
+  extends Modelica.Icons.Record;
+  parameter Real y[:](each min=0)
+    "Part load ratio, y = PEle/PEle_nominal";
+  parameter Modelica.Units.SI.Efficiency eta[size(y, 1)](each max=1)
+    "Fan or pump efficiency at these part load ratios";
+  annotation (Documentation(info="<html>
+<p>
+Data record for performance data that describe efficiency versus part load ratio.
+This is used a method to describe the motor efficiency <code>etaMot</code>.
+The PLR <code>y</code> must be increasing, i.e.,
+<code>y[i] &lt; y[i+1]</code>.
+Both vectors, <code>y</code> and <code>eta</code>
+must have the same size.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+March 2, 2022, by Hongxiang Fu:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end efficiencyParameters_yMot;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiency_yMot.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiency_yMot.mo
new file mode 100644
index 0000000000..f27df78eff
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/efficiency_yMot.mo
@@ -0,0 +1,59 @@
+within AixLib.Fluid.Movers.BaseClasses.Characteristics;
+function efficiency_yMot
+  "Efficiency vs. motor PLR characteristics for fan or pump"
+  extends Modelica.Icons.Function;
+  input
+    AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiencyParameters_yMot
+    per "Efficiency performance data";
+  input Real y "Motor part load ratio, y = PEle/PEle_nominal";
+  input Real d[:] "Derivatives at support points for spline interpolation";
+  output Real eta(unit="1", final quantity="Efficiency") "Efficiency";
+
+protected
+  Integer n = size(per.y, 1) "Number of data points";
+  Integer i "Integer to select data interval";
+algorithm
+  if n == 1 then
+    eta := per.eta[1];
+  else
+    i :=1;
+    for j in 1:n-1 loop
+       if y > per.y[j] then
+         i := j;
+       end if;
+    end for;
+    // Extrapolate or interpolate the data
+    eta:=AixLib.Utilities.Math.Functions.cubicHermiteLinearExtrapolation(
+                x=y,
+                x1=per.y[i],
+                x2=per.y[i + 1],
+                y1=per.eta[i],
+                y2=per.eta[i + 1],
+                y1d=d[i],
+                y2d=d[i+1]);
+  end if;
+
+  annotation(smoothOrder=1,
+              Documentation(info="<html>
+<p>
+This function is similar to
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiency\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiency</a>,
+but takes the motor part load ratio
+<i>y=P<sub>ele</sub> &frasl; P<sub>ele,nominal</sub></i>
+instead of volumetric flow rate <i>V&#775;</i> as input
+and does not consider the speed of the mover.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+March 2, 2022, by Hongxiang Fu:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end efficiency_yMot;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/flowParameters.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/flowParameters.mo
index 3249130c6a..7f77ad1308 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Characteristics/flowParameters.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/flowParameters.mo
@@ -8,28 +8,28 @@ record flowParameters "Record for flow parameters"
       each displayUnit="Pa") "Fan or pump total pressure at these flow rates";
 
   annotation (Documentation(info="<html>
- <p>
- Data record for performance data that describe volume flow rate versus
- pressure rise.
- The volume flow rate <code>V_flow</code> must be increasing, i.e.,
- <code>V_flow[i] &lt; V_flow[i+1]</code>.
- Both vectors, <code>V_flow</code> and <code>dp</code>
- must have the same size.
- </p>
- </html>",
+<p>
+Data record for performance data that describe volume flow rate versus
+pressure rise.
+The volume flow rate <code>V_flow</code> must be increasing, i.e.,
+<code>V_flow[i] &lt; V_flow[i+1]</code>.
+Both vectors, <code>V_flow</code> and <code>dp</code>
+must have the same size.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- September 28, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+September 28, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end flowParameters;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/flowParametersInternal.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/flowParametersInternal.mo
index 3aceee6cbb..befa097fa2 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Characteristics/flowParametersInternal.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/flowParametersInternal.mo
@@ -8,43 +8,43 @@ record flowParametersInternal "Record for flow parameters with prescribed size"
   parameter Modelica.Units.SI.PressureDifference dp[n](each min=0, each
       displayUnit="Pa") "Fan or pump total pressure at these flow rates";
   annotation (Documentation(info="<html>
- <p>
- Data record for performance data that describe volume flow rate versus
- pressure rise.
- The volume flow rate <code>V_flow</code> must be increasing, i.e.,
- <code>V_flow[i] &lt; V_flow[i+1]</code>.
- Both vectors, <code>V_flow</code> and <code>dp</code>
- must have the same size.
- </p>
- <p>
- This record is identical to
- <a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters\">
- AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters</a>,
- except that it takes the size of the array as a parameter. This is required
- in Dymola 2014. Otherwise, the array size would need to be computed in
- <a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
- AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>
- in the <code>initial algorithm</code> section, which is not supported.
- </p>
- </html>",
+<p>
+Data record for performance data that describe volume flow rate versus
+pressure rise.
+The volume flow rate <code>V_flow</code> must be increasing, i.e.,
+<code>V_flow[i] &lt; V_flow[i+1]</code>.
+Both vectors, <code>V_flow</code> and <code>dp</code>
+must have the same size.
+</p>
+<p>
+This record is identical to
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters</a>,
+except that it takes the size of the array as a parameter. This is required
+in Dymola 2014. Otherwise, the array size would need to be computed in
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>
+in the <code>initial algorithm</code> section, which is not supported.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- March 22, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+March 22, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end flowParametersInternal;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/motorEfficiencyCurve.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/motorEfficiencyCurve.mo
new file mode 100644
index 0000000000..3bd874e1fb
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/motorEfficiencyCurve.mo
@@ -0,0 +1,71 @@
+within AixLib.Fluid.Movers.BaseClasses.Characteristics;
+function motorEfficiencyCurve
+  "This function generates the generic curve for motor efficiency based on rated motor power"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.Power P_nominal "Rated input power of the motor";
+  input Modelica.Units.SI.Efficiency eta_max "Maximum motor efficiency";
+  // Below, default values are assigned so that that dimensions are known.
+  output AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiencyParameters_yMot
+    motorEfficiency_yMot(
+        y={0, 0.1, 0.2, 0.3, 0.4, 0.6, 0.8, 1, 1.2},
+        eta=zeros(nPoi)) "Motor efficiency vs. motor part load ratio";
+
+protected
+  constant Modelica.Units.SI.Power u2[nSiz]={700, 2500, 7500, 15000, 35000, 70000, 80000, 90000}
+    "Rated motor input power";
+  constant Integer nSiz=8 "Number of motor sizes";
+  constant Integer nPoi=9 "Size";
+  // Two rows and two columns of 1 are added to the ends of the table in order to
+  //   prevent the lookup table from producing values larger than 1.
+  constant Real[nPoi, nSiz] tab=
+    [             1E-6,              1E-6,              1E-6,              1E-6,              1E-6,              1E-6, 1E-6, 1E-6;
+     0.319836509737628, 0.329886760993909, 0.458027464511497, 0.576112127457564, 0.643957112752703, 0.724359122802955,    1,    1;
+     0.551721742352314, 0.613279531297038, 0.752726767477942, 0.843179028784475, 0.903480536322164, 0.962525762452817,    1,    1;
+     0.716480140443274, 0.804199438688888, 0.886622050343885, 0.936873306625292, 0.956973809137855, 0.987124562906699,    1,    1;
+     0.816999745270129, 0.922527383461084, 0.950165574415858, 0.980316328184702,                 1,                 1,    1,    1;
+     0.906409929833499,                 1,                 1,                 1,                 1,                 1,    1,    1;
+     0.956863812148299,                 1,                 1,                 1,                 1,                 1,    1,    1;
+                     1,                 1,                 1,                 1,                 1,                 1,    1,    1;
+                     1,                 1,                 1,                 1,                 1,                 1,    1,    1]
+    "Generic motor efficiency table (eta / eta_max)";
+algorithm
+  if P_nominal>1E-6 then
+    for j in 1:nPoi loop
+      motorEfficiency_yMot.eta[j]:=eta_max * AixLib.Utilities.Math.Functions.smoothInterpolation(
+        x=P_nominal,
+        xSup=u2,
+        ySup=tab[j, :],
+        ensureMonotonicity=true);
+    end for;
+  else
+    motorEfficiency_yMot.eta := 0.7*ones(nPoi);
+  end if;
+
+annotation (Documentation(info="<html>
+<p>
+This function generates a generic motor efficiency curve based on the
+rated motor power input and maximum motor efficiency according to U.S. DOE (2014)
+(shown below). It returns a constant array if the rated power is unavailable.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/BaseClasses/Characteristics/MotorEfficiencyCurves.png\"
+width=\"500\"/>
+</p>
+<h4>References</h4>
+<p>
+U.S. DOE (2014).
+<i>Determining Electric Motor Load and Efficiency.</i>
+URL:
+<a href=\"https://www.energy.gov/sites/prod/files/2014/04/f15/10097517.pdf\">
+https://www.energy.gov/sites/prod/files/2014/04/f15/10097517.pdf</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>April 5, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end motorEfficiencyCurve;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/package.order b/AixLib/Fluid/Movers/BaseClasses/Characteristics/package.order
index 684a5a2891..7815f16ad3 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Characteristics/package.order
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/package.order
@@ -1,7 +1,10 @@
 efficiency
+efficiency_yMot
+motorEfficiencyCurve
 power
 pressure
 efficiencyParameters
+efficiencyParameters_yMot
 flowParameters
 flowParametersInternal
 powerParameters
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/power.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/power.mo
index 298f23ca68..5122c08226 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Characteristics/power.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/power.mo
@@ -4,9 +4,9 @@ function power "Flow vs. electrical power characteristics for fan or pump"
   input AixLib.Fluid.Movers.BaseClasses.Characteristics.powerParameters per
     "Pressure performance data";
   input Modelica.Units.SI.VolumeFlowRate V_flow "Volumetric flow rate";
-  input Real r_N(unit="1") "Relative revolution, r_N=N/N_nominal";
+  input Real r_N(unit="1") "Relative speed";
   input Real d[:] "Derivatives at support points for spline interpolation";
-  input Real delta "Small value for switching implementation around zero rpm";
+  input Real delta "Small value for switching implementation around zero speed";
   output Modelica.Units.SI.Power P "Power consumption";
 
 protected
@@ -44,42 +44,42 @@ algorithm
   end if;
   annotation(smoothOrder=1,
               Documentation(info="<html>
- <p>
- This function computes the fan power consumption for given volume flow rate,
- speed and performance data. The power consumption is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   P = r<sub>N</sub><sup>3</sup> &nbsp; s(V&#775;/r<sub>N</sub>, d),
- </p>
- <p>
- where
- <i>P</i> is the power consumption,
- <i>r<sub>N</sub></i> is the normalized fan speed,
- <i>V&#775;</i> is the volume flow rate and
- <i>d</i> are performance data for fan or pump power consumption at <i>r<sub>N</sub>=1</i>.
- </p>
- <h4>Implementation</h4>
- <p>
- The function <i>s(&middot;, &middot;)</i> is a cubic hermite spline.
- If the data <i>d</i> define a monotone decreasing sequence, then
- <i>s(&middot;, d)</i> is a monotone decreasing function.
- </p>
- </html>",
+<p>
+This function computes the fan power consumption for given volume flow rate,
+speed and performance data. The power consumption is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  P = r<sub>N</sub><sup>3</sup> &nbsp; s(V&#775;/r<sub>N</sub>, d),
+</p>
+<p>
+where
+<i>P</i> is the power consumption,
+<i>r<sub>N</sub></i> is the normalized fan speed,
+<i>V&#775;</i> is the volume flow rate and
+<i>d</i> are performance data for fan or pump power consumption at <i>r<sub>N</sub>=1</i>.
+</p>
+<h4>Implementation</h4>
+<p>
+The function <i>s(&middot;, &middot;)</i> is a cubic hermite spline.
+If the data <i>d</i> define a monotone decreasing sequence, then
+<i>s(&middot;, d)</i> is a monotone decreasing function.
+</p>
+</html>",
         revisions="<html>
- <ul>
- <li>
- February 26, 2014, by Filip Jorissen:<br/>
- Changed polynomial to be evaluated at <code>V_flow/r_N</code>
- instead of <code>V_flow</code> to properly account for the
- scaling law. See
- <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
- for a discussion and validation.
- </li>
- <li>
- September 28, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 26, 2014, by Filip Jorissen:<br/>
+Changed polynomial to be evaluated at <code>V_flow/r_N</code>
+instead of <code>V_flow</code> to properly account for the
+scaling law. See
+<a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
+for a discussion and validation.
+</li>
+<li>
+September 28, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end power;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/powerParameters.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/powerParameters.mo
index d338d21daa..1b9603d8af 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Characteristics/powerParameters.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/powerParameters.mo
@@ -6,27 +6,27 @@ record powerParameters "Record for electrical power parameters"
   parameter Modelica.Units.SI.Power P[size(V_flow, 1)](each min=0)
     "Fan or pump electrical power at these flow rates";
   annotation (Documentation(info="<html>
- <p>
- Data record for performance data that describe volume flow rate versus
- electrical power.
- The volume flow rate <code>V_flow</code> must be increasing, i.e.,
- <code>V_flow[i] &lt; V_flow[i+1]</code>.
- Both vectors, <code>V_flow</code> and <code>P</code>
- must have the same size.
- </p>
- </html>",
+<p>
+Data record for performance data that describe volume flow rate versus
+electrical power.
+The volume flow rate <code>V_flow</code> must be increasing, i.e.,
+<code>V_flow[i] &lt; V_flow[i+1]</code>.
+Both vectors, <code>V_flow</code> and <code>P</code>
+must have the same size.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 10, 2012, by Michael Wetter:<br/>
- Fixed wrong <code>displayUnit</code> and
- <code>max</code> attribute for power.
- </li>
- <li>
- September 28, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 10, 2012, by Michael Wetter:<br/>
+Fixed wrong <code>displayUnit</code> and
+<code>max</code> attribute for power.
+</li>
+<li>
+September 28, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end powerParameters;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Characteristics/pressure.mo b/AixLib/Fluid/Movers/BaseClasses/Characteristics/pressure.mo
index 17bda5dcf5..de1e6e987e 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Characteristics/pressure.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Characteristics/pressure.mo
@@ -69,46 +69,46 @@ algorithm
   end if;
 annotation(smoothOrder=1,
 Documentation(info="<html>
- <p>
- This function computes the fan static
- pressure raise as a function of volume flow rate and revolution in the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   &Delta;p = r<sub>N</sub><sup>2</sup> &nbsp; s(V&#775;/r<sub>N</sub>, d),
- </p>
- <p>
- where
- <i>&Delta;p</i> is the pressure rise,
- <i>r<sub>N</sub></i> is the normalized fan speed,
- <i>V&#775;</i> is the volume flow rate and
- <i>d</i> are performance data for fan or pump power consumption at <i>r<sub>N</sub>=1</i>.
- </p>
- <h4>Implementation</h4>
- <p>
- The function <i>s(&middot;, &middot;)</i> is a cubic hermite spline.
- If the data <i>d</i> define a monotone decreasing sequence, then
- <i>s(&middot;, d)</i> is a monotone decreasing function.
- </p>
- <p>
- The function allows <i>r<sub>N</sub></i> to be zero.
- </p>
- </html>",
+<p>
+This function computes the fan static
+pressure raise as a function of volume flow rate and revolution in the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  &Delta;p = r<sub>N</sub><sup>2</sup> &nbsp; s(V&#775;/r<sub>N</sub>, d),
+</p>
+<p>
+where
+<i>&Delta;p</i> is the pressure rise,
+<i>r<sub>N</sub></i> is the normalized fan speed,
+<i>V&#775;</i> is the volume flow rate and
+<i>d</i> are performance data for fan or pump power consumption at <i>r<sub>N</sub>=1</i>.
+</p>
+<h4>Implementation</h4>
+<p>
+The function <i>s(&middot;, &middot;)</i> is a cubic hermite spline.
+If the data <i>d</i> define a monotone decreasing sequence, then
+<i>s(&middot;, d)</i> is a monotone decreasing function.
+</p>
+<p>
+The function allows <i>r<sub>N</sub></i> to be zero.
+</p>
+</html>",
   revisions="<html>
- <ul>
- <li>
- September 8, 2016, by Michael Wetter and Filip Jorissen:<br/>
- Changed implementation to allow <code>r_N = 0</code>.<br/>
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/458\">#458</a>.
- </li>
- <li>
- September 7, 2016, by Michael Wetter:<br/>
- Moved function which was a protected function to make it public, as it
- is now called by
- <a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
- AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 8, 2016, by Michael Wetter and Filip Jorissen:<br/>
+Changed implementation to allow <code>r_N = 0</code>.<br/>
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/458\">#458</a>.
+</li>
+<li>
+September 7, 2016, by Michael Wetter:<br/>
+Moved function which was a protected function to make it public, as it
+is now called by
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end pressure;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Euler/correlation.mo b/AixLib/Fluid/Movers/BaseClasses/Euler/correlation.mo
new file mode 100644
index 0000000000..03d63b3a72
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Euler/correlation.mo
@@ -0,0 +1,151 @@
+within AixLib.Fluid.Movers.BaseClasses.Euler;
+function correlation
+  "Correlation of static efficiency ratio vs log of Euler number ratio"
+  extends Modelica.Icons.Function;
+  input Real x "log10(Eu/Eu_peak)";
+  output Real y "eta/eta_peak";
+
+protected
+  Real a "Polynomial coefficient";
+  Real b "Polynomial coefficient";
+  Real c "Polynomial coefficient";
+  Real d "Polynomial coefficient";
+  Real y1 "eta/eta_peak";
+algorithm
+  if x < -0.5 then
+    a := 0.05687322707407;
+    b := 0.493231336746;
+    c := 1.433531254001;
+    d := 1.407887300933;
+  elseif x > 0.5 then
+    a := -8.5494313567465000E-3;
+    b := 1.2957001502368300E-1;
+    c := -6.5997315029278200E-1;
+    d := 1.13993003013131;
+  else
+    a := 0.37824577860088;
+    b := -0.75988502317361;
+    c := -0.060614519563716;
+    d := 1.01426507307139;
+  end if;
+  y1 := (a*x^3 + b*x^2 + c*x + d) / 1.01545;
+  // y1 is almost always bounded away from zero,
+  // hence we make a test to see whether we indeed
+  // need to call smoothMax or can avoid its overhead
+  y := if y1 > 0.002 then y1 else
+    AixLib.Utilities.Math.Functions.smoothMax(
+      x1=y1,
+      x2=0.001,
+      deltaX=0.0005);
+
+  annotation(smoothOrder = 1,
+  Documentation(info="<html>
+<p>
+This function approximates the following correlation:
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/BaseClasses/Euler/eulerCorrelation.svg\"/>
+</p>
+<p>
+where <i>y=&eta; &frasl; &eta;<sub>p</sub></i> (note that <i>&eta;</i>
+refers to the hydraulic efficiency instead of total efficiency),
+<i>x=log<sub>10</sub>(Eu &frasl; Eu<sub>p</sub>)</i>,
+with the subscript <i>p</i> denoting the condition where
+the mover is operating at peak efficiency, and
+</p>
+<p align=\"center\">
+<i>Z<sub>1</sub>=(x-a) &frasl; b</i>
+</p>
+<p align=\"center\">
+<i>Z<sub>2</sub>=(e<sup>c&sdot;x</sup>&sdot;d&sdot;x-a) &frasl; b</i>
+</p>
+<p align=\"center\">
+<i>Z<sub>3</sub>=-a &frasl; b</i>
+</p>
+<p align=\"center\">
+<i>a=-2.732094</i>
+</p>
+<p align=\"center\">
+<i>b=2.273014</i>
+</p>
+<p align=\"center\">
+<i>c=0.196344</i>
+</p>
+<p align=\"center\">
+<i>d=5.267518</i>
+</p>
+<p>
+The approximation uses two simple polynomials stitched together by
+a third one of the same order.
+Care has been taken to ensure that, on the curve constructed by
+<code>if</code> statements, the differences of <i>dy &frasl; dx</i>
+evaluated by different groups of coefficients at the connecting points
+(i.e. at <i>x = - 0.5</i> and <i>x = + 0.5</i>) are less than <i>1E-14</i>.
+This way, the derivative is still continuous to the solver even if
+the solver requires a precision of <i>1E-10</i> when there are nested loops.
+</p>
+<p>
+The correlation and the approximation have the shape as shown below
+(plotted by 
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Validation.EulerCurve\">
+AixLib.Fluid.Movers.BaseClasses.Validation.EulerCurve</a>).
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/BaseClasses/Euler/EulerCurve.png\"/>
+</p>
+<p>
+The modified dimensionless Euler number is defined as
+</p>
+<p align=\"center\">
+<i>Eu=(&Delta;p&sdot;D<sup>4</sup>) &frasl; (&rho;&sdot;V&#775;<sup>2</sup>)</i>
+</p>
+<p>
+where <i>&Delta;p</i> is the fan pressure rise in Pa,
+<i>D</i> is the fan wheel outer diameter in m,
+<i>&rho;</i> is the inlet air density in kg/m<sup>3</sup>,
+and <i>V&#775;</i> is the volumetric flow rate in m<sup>3</sup>/s.
+Note that the units in the definition do not matter to this correlation
+because it is the ratio of the Euler numbers that is used.
+Since <i>D</i> is constant for the same mover
+and <i>&rho;</i> is approximately constant for common HVAC applications,
+the Euler number ratio can be simplified to
+</p>
+<p align=\"center\">
+<i>Eu &frasl; Eu<sub>p</sub>=(&Delta;p&sdot;V&#775;<sub>p</sub><sup>2</sup>)
+&frasl; (&Delta;p<sub>p</sub>&sdot;V&#775;<sup>2</sup>)</i>
+</p>
+<h4>References</h4>
+<p>
+For more information regarding the correlation curve refer to
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v9.6.0/EngineeringReference.pdf\">
+EnergyPlus 9.6.0 Engineering Reference</a>
+chapter 16.4 equations 16.209 through 16.218.
+Note that the formula is simplified here from the source document.
+</p>
+<h4>Resources</h4>
+<p>
+The svg file for the correlation equation was generated on
+<a href=\"https://viereck.ch/latex-to-svg/\">
+https://viereck.ch/latex-to-svg</a>
+using
+<a href=\"modelica://AixLib/Resources/Images/Fluid/Movers/BaseClasses/Euler/eulerCorrelation.txt\">
+this script</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 2, 2023, by Michael Wetter:<br/>
+Rewrote to reduce number of <code>if-then</code> statements and to use
+<code>smoothMax</code> rather than <code>max</code>.
+</li>
+<li>
+December 12, 2022, by Hongxiang Fu and Filip Jorissen:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a> and
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1645\">#1645</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end correlation;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Euler/efficiency.mo b/AixLib/Fluid/Movers/BaseClasses/Euler/efficiency.mo
new file mode 100644
index 0000000000..3b00c38a36
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Euler/efficiency.mo
@@ -0,0 +1,51 @@
+within AixLib.Fluid.Movers.BaseClasses.Euler;
+function efficiency
+  "Computes efficiency with the Euler number correlation"
+  extends Modelica.Icons.Function;
+  input AixLib.Fluid.Movers.BaseClasses.Euler.peak peak
+    "Operation point with maximum efficiency";
+  input Modelica.Units.SI.PressureDifference dp
+    "Pressure rise";
+  input Modelica.Units.SI.VolumeFlowRate V_flow
+    "Volumetric flow rate";
+  input Real V_flow_dp_small(
+    final unit="m3.Pa/s",
+    min = Modelica.Constants.eps)
+    "Small number for regularisation";
+  output Modelica.Units.SI.Efficiency eta
+    "Efficiency";
+
+protected
+  Real log_r_Eu "Log10 of Eu/Eu_peak";
+
+algorithm
+  log_r_Eu:= log10(
+               AixLib.Utilities.Math.Functions.smoothMax(
+                 x1=dp * peak.V_flow^2,
+                 x2=V_flow_dp_small,
+                 deltaX=V_flow_dp_small/2)
+              /AixLib.Utilities.Math.Functions.smoothMax(
+                 x1=peak.dp * V_flow^2,
+                 x2=V_flow_dp_small,
+                 deltaX=V_flow_dp_small/2));
+  eta:= peak.eta*
+          AixLib.Fluid.Movers.BaseClasses.Euler.correlation(x=log_r_Eu);
+
+          annotation(smoothOrder=1,
+              Documentation(info="<html>
+<p>
+This function uses the correlation of Euler number to compute
+the efficiency <i>&eta;</i>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+December 12, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end efficiency;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Euler/getPeak.mo b/AixLib/Fluid/Movers/BaseClasses/Euler/getPeak.mo
new file mode 100644
index 0000000000..152df7dba3
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Euler/getPeak.mo
@@ -0,0 +1,225 @@
+within AixLib.Fluid.Movers.BaseClasses.Euler;
+function getPeak
+  "Find peak condition from power characteristics"
+  extends Modelica.Icons.Function;
+  input AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters
+    pressure "Pressure vs. flow rate";
+  input BaseClasses.Characteristics.powerParameters
+    power "Power vs. flow rate";
+  output AixLib.Fluid.Movers.BaseClasses.Euler.peak
+    peak "Operation point at maximum efficiency";
+
+protected
+  parameter Integer nPre = size(pressure.V_flow, 1) "Size of the pressure array";
+  parameter Integer nPow = size(power.V_flow, 1) "Size of the power array";
+  parameter Integer n = max(nPre, nPow) "Bigger of the two arrays";
+  parameter Modelica.Units.SI.VolumeFlowRate V_flow_hal=
+    if max(pressure.V_flow) < 1E-6
+      then 0
+    else (pressure.V_flow[nPre]
+                -(pressure.V_flow[nPre] - pressure.V_flow[nPre - 1])
+                /(pressure.dp[nPre] - pressure.dp[nPre - 1])
+                * pressure.dp[nPre])/2
+    "Half of max flow, max flow is where dp=0";
+  parameter Modelica.Units.SI.PressureDifference dpHalFlo=
+    if max(pressure.V_flow) < 1E-6
+      then 0
+    else AixLib.Utilities.Math.Functions.smoothInterpolation(
+               x=V_flow_hal,
+               xSup=pressure.V_flow,
+               ySup=pressure.dp,
+               ensureMonotonicity=true)
+    "Pressure rise at half flow";
+
+  Modelica.Units.SI.VolumeFlowRate V_flow[n] "Flow rate";
+  Modelica.Units.SI.PressureDifference dp[n] "Pressure rise";
+  Modelica.Units.SI.Power P[n] "Power";
+
+  Real eta[n] "Efficiency series";
+  Boolean etaLes "Efficiency series has less than four points";
+  Boolean etaMon "Efficiency series is monotonic";
+
+  // A b = y
+  Real A[n,5] "Design matrix";
+  Real b[5] "Parameter vector";
+  Real r[3,2] "Roots";
+algorithm
+
+  if max(pressure.V_flow) < 1E-6 and
+     max(pressure.dp)     < 1E-6 then
+    // If there is no pressure curve, no estimation can be made
+    peak.V_flow:=0;
+    peak.dp:=0;
+    peak.eta:=0.7;
+
+  elseif max(power.P) < 1E-6 then
+    // If a pressure curve is available, but no power curve,
+    //   peak.V_flow = V_flow_max / 2,
+    //   peak.dp = dp(V_flow = V_flow_max / 2)
+    peak.V_flow:=V_flow_hal;
+    peak.dp:=dpHalFlo;
+    peak.eta:=0.7;
+
+  else
+    // Both a pressure curve and a power curve are available.
+
+    // Create arrays of the equal size
+    if nPre == nPow then
+      V_flow:= pressure.V_flow;
+      dp:= pressure.dp;
+      P:= power.P;
+    else
+      if nPre > nPow then
+        V_flow:= pressure.V_flow;
+        dp:= pressure.dp;
+        for i in 1:n loop
+          P[i]:= AixLib.Utilities.Math.Functions.smoothInterpolation(
+                   x=V_flow[i],
+                   xSup=power.V_flow,
+                   ySup=power.P,
+                   ensureMonotonicity=false);
+        end for;
+      else
+        V_flow:= power.V_flow;
+        P:= power.P;
+        for i in 1:n loop
+          dp[i]:= AixLib.Utilities.Math.Functions.smoothInterpolation(
+                    x=V_flow[i],
+                    xSup=pressure.V_flow,
+                    ySup=pressure.dp,
+                    ensureMonotonicity=true);
+        end for;
+      end if;
+    end if;
+
+    // Compute efficiency array
+    eta:=V_flow.*dp./P;
+    etaLes:=n<4;
+    etaMon:=AixLib.Utilities.Math.Functions.isMonotonic(
+      x=eta,
+      strict=false);
+
+    if etaLes or etaMon then
+    // If less than four data points are provided or the efficiency curve is
+    //   monotonic, use the one of two which has the higher efficiency:
+    //   1. the interpolated point at half of max flow;
+    //   2. the available point with the highest efficiency.
+      peak.eta:=AixLib.Utilities.Math.Functions.smoothInterpolation(
+               x=V_flow_hal,
+               xSup=V_flow,
+               ySup=eta,
+               ensureMonotonicity=
+                 AixLib.Utilities.Math.Functions.isMonotonic(eta, strict=false));
+      if peak.eta>max(eta) then
+             peak.V_flow:=V_flow_hal;
+             peak.dp:=dpHalFlo;
+      else
+        peak.eta:=max(eta);
+        for i in 1:n loop
+          if abs(eta[i]-peak.eta)<1E-6 then
+            peak.V_flow:=V_flow[i];
+            peak.dp:=dp[i];
+          end if;
+        end for;
+      end if;
+    else
+
+      // Constructs the matrix equation A b = y for quartic regression, where
+      //   A is a 5-by-n design matrix,
+      //   b is a parameter vector with length 5,
+      //   and y = eta is the response vector with length n.
+      A[:,1]:=ones(n); // Avoids 0^0
+      for i in 2:5 loop
+        A[:,i]:=V_flow[:].^(i-1);
+      end for;
+      b:=Modelica.Math.Matrices.leastSquares(A,eta);
+
+      // Solve the derivative for the max eta and corresponding V_flow.
+      // This assumes that there will only be one real solution
+      //   and it falls within the range of V_flow[:].
+      r:=Modelica.Math.Polynomials.roots({b[5]*4,b[4]*3,b[3]*2,b[2]});
+      for i in 1:3 loop
+        if abs(r[i,2])<=1E-6 and
+          r[i,1]>V_flow[1] and r[i,1]<V_flow[n] then
+          peak.V_flow:=r[i,1];
+        end if;
+      end for;
+      peak.eta:=AixLib.Utilities.Math.Functions.smoothInterpolation(
+        x=peak.V_flow,
+        xSup=V_flow,
+        ySup=eta,
+        ensureMonotonicity=false);
+      peak.dp:=AixLib.Utilities.Math.Functions.smoothInterpolation(
+        x=peak.V_flow,
+        xSup=V_flow,
+        ySup=dp,
+        ensureMonotonicity=false);
+    end if;
+  end if;
+
+  annotation(Documentation(info="<html>
+<p>
+This function finds or estimates the peak point
+<i>(V&#775;,&Delta;p,&eta;)|&eta;=&eta;<sub>max</sub></i>
+from the input power curve <i>P(V&#775;)</i>
+and pressure curve <i>&Delta;p(V&#775;)</i>
+which may or may not contain non-zero values.
+The results are output as an instance of
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Euler.peak\">
+AixLib.Fluid.Movers.BaseClasses.Euler.peak</a>.
+There are the following branches of computation based on information provided
+to the function:
+</p>
+<ul>
+<li>
+If <i>&Delta;p(V&#775;)</i> is unavailable, the function simply outputs
+<i>(0,0,0.7)</i>.
+</li>
+<li>
+If <i>&Delta;p(V&#775;)</i> is provided but <i>P(V&#775;)</i> is unavailable,
+the function provides an estimation of the peak point at half of max flow rate
+<i>(V&#775;<sub>max</sub> &frasl; 2,
+&Delta;p(V&#775;=V&#775;<sub>max</sub> &frasl; 2),
+0.7)</i>.
+</li>
+<li>
+If both <i>&Delta;p(V&#775;)</i> and <i>P(V&#775;)</i> are available,
+the function first computes
+<i>&eta;(V&#775;)=V&#775;&nbsp;&Delta;p &frasl; P</i>.
+<ul>
+<li>
+If <i>&eta;(V&#775;)</i> has less than four data points or is monotonic,
+use one of the two which ever produces a higher <i>&eta;</i>:
+<ul>
+<li>
+The interpolated point at half of max flow rate
+<i>(V&#775;<sub>max</sub> &frasl; 2,
+&Delta;p(V&#775;=V&#775;<sub>max</sub> &frasl; 2),
+&eta;(V&#775;=V&#775;<sub>max</sub> &frasl; 2))</i>
+</li>
+<li>
+The available point with the highest computed efficiency.
+</li>
+</ul>
+</li>
+<li>
+Otherwise, the function runs a quartic regression on <i>&eta;(V&#775;)</i>
+then solves its derivative to find an extremum.
+It assumes that there is only one extremum on the open interval
+<i>(0,V&#775;<sub>max</sub>)</i>.
+</li>
+</ul>
+</li>
+</ul>
+</html>",
+revisions="<html>
+<ul>
+<li>
+August 18, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end getPeak;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Euler/package.mo b/AixLib/Fluid/Movers/BaseClasses/Euler/package.mo
new file mode 100644
index 0000000000..b4b00043e8
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Euler/package.mo
@@ -0,0 +1,54 @@
+within AixLib.Fluid.Movers.BaseClasses;
+package Euler "Functions and data record templates for Euler number"
+
+  annotation (Documentation(info="<html>
+<p>
+This package implements a power computation using the Euler number
+and its correlation.
+</p>
+<ul>
+<li>
+The correlation function using the Euler number is implemented in
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Euler.correlation\">
+AixLib.Fluid.Movers.BaseClasses.Euler.correlation</a>.
+</li>
+<li>
+When curves of power and pressure against flow rate is available,
+the function
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Euler.getPeak\">
+AixLib.Fluid.Movers.BaseClasses.Euler.getPeak</a>
+can identify the peak operating condition from them.
+This is useful comparing power computation results
+against other methods.
+</li>
+<li>
+The peak operating condition (where the efficiency <i>&eta;</i> is
+at its maximum) which is used by the correlation is stored in an instance
+of the record
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Euler.peak\">
+AixLib.Fluid.Movers.BaseClasses.Euler.peak</a>.
+</li>
+<li>
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>
+uses the peak values and the correlation to generate a power curve against
+volumetric flow rate. This estimated power curve is used in place of the
+measured power that would otherwise be provided.
+</li>
+</ul>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
+User's Guide</a> for more information.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+October 13, 2021, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"));
+end Euler;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Euler/package.order b/AixLib/Fluid/Movers/BaseClasses/Euler/package.order
new file mode 100644
index 0000000000..47cec4d5b4
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Euler/package.order
@@ -0,0 +1,6 @@
+correlation
+efficiency
+getPeak
+power
+peak
+powerWithDerivative
diff --git a/AixLib/Fluid/Movers/BaseClasses/Euler/peak.mo b/AixLib/Fluid/Movers/BaseClasses/Euler/peak.mo
new file mode 100644
index 0000000000..16d3ae1695
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Euler/peak.mo
@@ -0,0 +1,31 @@
+within AixLib.Fluid.Movers.BaseClasses.Euler;
+record peak
+  "Record for the operation condition at peak efficiency"
+  extends Modelica.Icons.Record;
+  parameter Modelica.Units.SI.VolumeFlowRate
+    V_flow(min=0)
+    "Volume flow rate at peak efficiency";
+  parameter Modelica.Units.SI.PressureDifference
+    dp(
+      min=0,
+      displayUnit="Pa")
+    "Pressure rise at peak efficiency";
+  parameter Modelica.Units.SI.Efficiency eta=0.7
+    "Peak efficiency";
+  annotation (
+Documentation(info="<html>
+<p>
+Record for performance data that describe the operation at peak efficiency.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+October 15, 2021, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end peak;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Euler/power.mo b/AixLib/Fluid/Movers/BaseClasses/Euler/power.mo
new file mode 100644
index 0000000000..30778e609c
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Euler/power.mo
@@ -0,0 +1,110 @@
+within AixLib.Fluid.Movers.BaseClasses.Euler;
+function power
+  "Computes power as well as its derivative with respect to flow rate using Euler number"
+  extends Modelica.Icons.Function;
+  input AixLib.Fluid.Movers.BaseClasses.Euler.peak peak "Peak operation point";
+  input AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParametersInternal
+    pressure "Pressure curve with both max flow rate and max pressure";
+  output AixLib.Fluid.Movers.BaseClasses.Euler.powerWithDerivative power(
+    V_flow=zeros(11),P=zeros(11),d=zeros(11))
+    "Power and its derivative vs. flow rate";
+protected
+  Modelica.Units.SI.VolumeFlowRate V_flow[11]
+    "Volumetric flow rate";
+  Modelica.Units.SI.PressureDifference dp[11]
+    "Pressure rise";
+  Real V_flow_dp_small(
+    final unit="m3.Pa/s",
+    min = Modelica.Constants.eps) "Small value for regularisation";
+
+algorithm
+  // Construct pressure curve of 10% max flow rate increments
+  //   from the given pressure curve
+  V_flow:={pressure.V_flow[end]*i*0.1 for i in 0:10};
+  for i in 1:11 loop
+    dp[i]:=AixLib.Utilities.Math.Functions.smoothInterpolation(
+             x=V_flow[i],
+             xSup=pressure.V_flow,
+             ySup=pressure.dp,
+             ensureMonotonicity=false);
+  end for;
+
+  // Compute the power and derivative on non-boundary points
+  //   using efficiency estimated by Euler number method
+  power.V_flow:=V_flow;
+  V_flow_dp_small :=1E-4*max(pressure.V_flow)*max(pressure.dp);
+
+  for i in 2:10 loop
+    power.P[i]:=V_flow[i] * dp[i]
+                / AixLib.Fluid.Movers.BaseClasses.Euler.efficiency(
+                    peak=peak,
+                    dp=dp[i],
+                    V_flow=V_flow[i],
+                    V_flow_dp_small=V_flow_dp_small/2);
+  end for;
+
+  power.d[2:10]:=AixLib.Utilities.Math.Functions.splineDerivatives(
+                   x=V_flow[2:10],
+                   y=power.P[2:10],
+                   ensureMonotonicity=false);
+
+  // Use linear extrapolation to find the boundary points
+  power.d[1]:=power.d[2];
+  power.d[11]:=power.d[10];
+  power.P[1]:=power.P[2]-power.d[2]*V_flow[2];
+  power.P[11]:=power.P[10]+power.d[10]*(V_flow[11]-V_flow[10]);
+
+annotation(smoothOrder=1,
+              Documentation(info="<html>
+<p>
+This function outputs power values as well as its derivative versus
+volumetric flow rate in the following steps:
+</p>
+<ul>
+<li>
+It first interpolates the input pressure curve to find a new pressure curve of
+11 points on 10% increments of max flow rate.
+It assumes that the last point on the input pressure curve corresponds to
+<i>&Delta;p = 0</i>, which is ensured when this function is called by
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>.
+</li>
+<li>
+It then computes power using efficiency evaluated with the Euler number
+from 10% to 90% of max flow rate on 10% increments.
+</li>
+<li>
+With the incomplete power curve it computes the spline derivatives
+with respect to flow rate at the same points.
+</li>
+<li>
+Once the derivatives are available, the power values at the two boundary points
+are found through linear extrapolation.
+</li>
+</ul>
+<p>
+These steps are designed to ensure that power and efficiency computation with
+the Euler number is handled correctly near zero flow or zero pressure, where<br/>
+<p align=\"center\" style=\"font-style:italic;\">
+W&#775;<sub>flo</sub> = 0,<br/>
+&eta; = 0,<br/>
+P &gt; 0
+</p>
+<p>
+in the equation
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&eta; = W&#775;<sub>flo</sub> &frasl; P.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+December 13, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end power;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Euler/powerWithDerivative.mo b/AixLib/Fluid/Movers/BaseClasses/Euler/powerWithDerivative.mo
new file mode 100644
index 0000000000..e0adb04c6f
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Euler/powerWithDerivative.mo
@@ -0,0 +1,30 @@
+within AixLib.Fluid.Movers.BaseClasses.Euler;
+record powerWithDerivative
+  "Record for electrical power and its derivative with respect to flow rate"
+  extends Modelica.Icons.Record;
+  parameter Modelica.Units.SI.VolumeFlowRate V_flow[11](each min=0)
+    "Volume flow rate at user-selected operating points";
+  parameter Modelica.Units.SI.Power P[11](each min=0)
+    "Fan or pump electrical power at these flow rates";
+  parameter Real d[11](each unit="J/m3")
+    "Derivative of power with respect to volume flow rate";
+  annotation (Documentation(info="<html>
+<p>
+Data record for performance data that describe electrical power and its derivative
+versus volumetric flow rate.
+This record is specifically constructed for the Euler number method
+and is the output type of function
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler.power\">
+AixLib.Fluid.Movers.BaseClasses.Euler.power</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+December 13, 2022, by Hongxiang Fu:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end powerWithDerivative;
diff --git a/AixLib/Fluid/Movers/BaseClasses/FlowMachineInterface.mo b/AixLib/Fluid/Movers/BaseClasses/FlowMachineInterface.mo
index a954f62e76..f7ce0b1764 100644
--- a/AixLib/Fluid/Movers/BaseClasses/FlowMachineInterface.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/FlowMachineInterface.mo
@@ -24,10 +24,14 @@ model FlowMachineInterface
   parameter Modelica.Units.SI.Density rho_default
     "Fluid density at medium default state";
 
-  parameter Boolean haveVMax
+  final parameter Boolean haveVMax = (abs(per.pressure.dp[nOri]) < Modelica.Constants.eps)
     "Flag, true if user specified data that contain V_flow_max";
 
-  parameter Modelica.Units.SI.VolumeFlowRate V_flow_max
+  final parameter Modelica.Units.SI.VolumeFlowRate V_flow_max=
+    if per.V_flow_max>Modelica.Constants.eps
+      then per.V_flow_max
+    else
+      V_flow_nominal
     "Maximum volume flow rate, used for smoothing";
 
   parameter Integer nOri(min=1) "Number of data points for pressure curve"
@@ -60,8 +64,8 @@ model FlowMachineInterface
   Modelica.Blocks.Interfaces.RealOutput V_flow(
     quantity="VolumeFlowRate",
     final unit="m3/s") "Volume flow rate"
-    annotation (Placement(transformation(extent={{100,38},{120,58}}),
-        iconTransformation(extent={{100,38},{120,58}})));
+    annotation (Placement(transformation(extent={{100,50},{120,70}}),
+        iconTransformation(extent={{100,50},{120,70}})));
 
   Modelica.Blocks.Interfaces.RealInput dp_in(
     quantity="PressureDifference",
@@ -80,27 +84,40 @@ model FlowMachineInterface
     final unit="W") "Flow work"
     annotation (Placement(transformation(extent={{100,10},{120,30}})));
 
+  Modelica.Blocks.Interfaces.RealOutput WHyd(
+    quantity="Power",
+    final unit="W") "Hydraulic work (shaft work, brake horsepower)"
+    annotation (Placement(
+        transformation(extent={{100,-10},{120,10}}), iconTransformation(extent={
+            {100,-10},{120,10}})));
+
   Modelica.Blocks.Interfaces.RealOutput PEle(
     quantity="Power",
     final unit="W") "Electrical power consumed"
-    annotation (Placement(transformation(extent={{100,-20},{120,0}}),
-        iconTransformation(extent={{100,-20},{120,0}})));
+    annotation (Placement(transformation(extent={{100,-30},{120,-10}}),
+        iconTransformation(extent={{100,-30},{120,-10}})));
 
   Modelica.Blocks.Interfaces.RealOutput eta(
     final quantity="Efficiency",
-    final unit="1") "Overall efficiency"
-    annotation (Placement(transformation(extent={{100,-50},{120,-30}}),
-        iconTransformation(extent={{100,-50},{120,-30}})));
+    final unit="1",
+    start = 0.49) "Overall efficiency"
+    annotation (Placement(transformation(extent={{100,-70},{120,-50}}),
+        iconTransformation(extent={{100,-70},{120,-50}})));
+  // A start value is given to suppress the following translation warning:
+  //   "Some variables are iteration variables of the initialization problem:
+  //   but they are not given any explicit start values. Zero will be used."
 
   Modelica.Blocks.Interfaces.RealOutput etaHyd(
     final quantity="Efficiency",
-    final unit="1") "Hydraulic efficiency"
-    annotation (Placement(transformation(extent={{100,-80},{120,-60}}),
-        iconTransformation(extent={{100,-80},{120,-60}})));
+    final unit="1",
+    start = 0.7) "Hydraulic efficiency"
+    annotation (Placement(transformation(extent={{100,-90},{120,-70}}),
+        iconTransformation(extent={{100,-90},{120,-70}})));
 
   Modelica.Blocks.Interfaces.RealOutput etaMot(
     final quantity="Efficiency",
-    final unit="1") "Motor efficiency"
+    final unit="1",
+    start = 0.7) "Motor efficiency"
     annotation (Placement(transformation(extent={{100,-110},{120,-90}}),
         iconTransformation(extent={{100,-110},{120,-90}})));
 
@@ -119,27 +136,74 @@ protected
     "True if pressure head is a prescribed variable of this block";
 
   // Derivatives for cubic spline
-  final parameter Real motDer[size(per.motorEfficiency.V_flow, 1)](each fixed=false)
-    "Coefficients for polynomial of motor efficiency vs. volume flow rate";
-  final parameter Real hydDer[size(per.hydraulicEfficiency.V_flow,1)](each fixed=false)
-    "Coefficients for polynomial of hydraulic efficiency vs. volume flow rate";
-
-  parameter Modelica.Units.SI.PressureDifference dpMax(displayUnit="Pa") = if
-    haveDPMax then per.pressure.dp[1] else per.pressure.dp[1] - ((per.pressure.dp[
-    2] - per.pressure.dp[1])/(per.pressure.V_flow[2] - per.pressure.V_flow[1]))
-    *per.pressure.V_flow[1] "Maximum head";
+  final parameter Real etaDer[size(per.efficiency.V_flow,1)]=
+    if not per.etaHydMet==AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate
+      then zeros(size(per.efficiency.V_flow,1))
+    elseif (size(per.efficiency.V_flow, 1) == 1)
+      then {0}
+    else
+      AixLib.Utilities.Math.Functions.splineDerivatives(
+        x=per.efficiency.V_flow,
+        y=per.efficiency.eta,
+        ensureMonotonicity=AixLib.Utilities.Math.Functions.isMonotonic(
+          x=per.efficiency.eta,
+          strict=false))
+    "Coefficients for cubic spline of total or hydraulic efficiency vs. volume flow rate";
+  final parameter Real motDer[size(per.motorEfficiency.V_flow, 1)]=
+    if not per.etaMotMet==AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_VolumeFlowRate
+      then zeros(size(per.motorEfficiency.V_flow,1))
+    elseif (size(per.motorEfficiency.V_flow, 1) == 1)
+      then {0}
+    else
+      AixLib.Utilities.Math.Functions.splineDerivatives(
+        x=per.motorEfficiency.V_flow,
+        y=per.motorEfficiency.eta,
+        ensureMonotonicity=AixLib.Utilities.Math.Functions.isMonotonic(
+          x=per.motorEfficiency.eta,
+          strict=false))
+    "Coefficients for cubic spline of motor efficiency vs. volume flow rate";
+  final parameter Real motDer_yMot[size(per.motorEfficiency_yMot.y,1)]=
+    if not per.etaMotMet==
+      AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio
+      then zeros(size(per.motorEfficiency_yMot.y,1))
+    elseif (size(per.motorEfficiency_yMot.y,1) == 1)
+      then {0}
+    else
+      AixLib.Utilities.Math.Functions.splineDerivatives(
+        x=per.motorEfficiency_yMot.y,
+        y=per.motorEfficiency_yMot.eta,
+        ensureMonotonicity=AixLib.Utilities.Math.Functions.isMonotonic(
+          x=per.motorEfficiency_yMot.eta,
+          strict=false))
+    "Coefficients for cubic spline of motor efficiency vs. motor PLR";
+  final parameter Real motDer_yMot_generic[9]=
+    if per.etaMotMet==
+      AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve
+      or  (per.etaMotMet==
+      AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided
+           and per.haveWMot_nominal)
+      then AixLib.Utilities.Math.Functions.splineDerivatives(
+             x=per.motorEfficiency_yMot_generic.y,
+             y=per.motorEfficiency_yMot_generic.eta,
+             ensureMonotonicity=true)
+    else zeros(9)
+    "Coefficients for cubic spline of motor efficiency vs. motor PLR with generic curves";
+
+  final parameter Modelica.Units.SI.PressureDifference dpMax(
+    displayUnit="Pa")=
+    per.dpMax "Maximum head";
 
   parameter Real delta = 0.05
     "Small value used to for regularization and to approximate an internal flow resistance of the fan";
 
   parameter Real kRes(min=0, unit="kg/(s.m4)") =  dpMax/V_flow_max*delta^2/10
-    "Coefficient for internal pressure drop of fan or pump";
+    "Coefficient for internal pressure drop of the fan or pump";
 
   parameter Integer curve=
      if (haveVMax and haveDPMax) or (nOri == 2) then 1
      elseif haveVMax or haveDPMax then 2
      else 3
-    "Flag, used to pick the right representatio of the fan or pump pressure curve";
+    "Flag, used to pick the right representation of the fan or pump's pressure curve";
 
   final parameter
     AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParametersInternal pCur1(
@@ -152,7 +216,7 @@ protected
              {(per.pressure.dp[i] + per.pressure.V_flow[i] * kRes) for i in 1:nOri}
              else
              zeros(nOri))
-    "Volume flow rate vs. total pressure rise with correction for pump resistance added";
+    "Volume flow rate vs. total pressure rise with correction for fan or pump's resistance added";
 
   parameter
     AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParametersInternal pCur2(
@@ -173,7 +237,7 @@ protected
               cat(1, {per.pressure.dp[i] + per.pressure.V_flow[i] * kRes for i in 1:nOri}, {0})
              else
                zeros(nOri+1))
-    "Volume flow rate vs. total pressure rise with correction for pump resistance added";
+    "Volume flow rate vs. total pressure rise with correction for fan or pump's resistance added";
   parameter
     AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParametersInternal pCur3(
     final n = nOri + 2,
@@ -189,7 +253,7 @@ protected
                zeros(nOri + 2)
              else
                cat(1, {dpMax}, {per.pressure.dp[i] + per.pressure.V_flow[i] * kRes for i in 1:nOri}, {0}))
-    "Volume flow rate vs. total pressure rise with correction for pump resistance added";
+    "Volume flow rate vs. total pressure rise with correction for fan or pump's resistance added";
 
   parameter Real preDer1[nOri](each fixed=false)
     "Derivatives of flow rate vs. pressure at the support points";
@@ -198,7 +262,8 @@ protected
   parameter Real preDer3[nOri+2](each fixed=false)
     "Derivatives of flow rate vs. pressure at the support points";
   parameter Real powDer[size(per.power.V_flow,1)]=
-   if per.use_powerCharacteristic then
+   if per.etaHydMet==
+      AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate then
      AixLib.Utilities.Math.Functions.splineDerivatives(
                    x=per.power.V_flow,
                    y=per.power.P,
@@ -208,16 +273,49 @@ protected
      zeros(size(per.power.V_flow,1))
     "Coefficients for polynomial of power vs. flow rate";
 
+  final parameter AixLib.Fluid.Movers.BaseClasses.Euler.powerWithDerivative powEu_internal=
+    if (curve == 1) then
+      AixLib.Fluid.Movers.BaseClasses.Euler.power(peak=per.peak,pressure=pCur1)
+    elseif (curve == 2) then
+      AixLib.Fluid.Movers.BaseClasses.Euler.power(peak=per.peak,pressure=pCur2)
+    else
+      AixLib.Fluid.Movers.BaseClasses.Euler.power(peak=per.peak,pressure=pCur3)
+    "Intermediate parameter";
+  final parameter AixLib.Fluid.Movers.BaseClasses.Characteristics.powerParameters powEu(
+    V_flow = powEu_internal.V_flow,
+    P = powEu_internal.P)
+    "Power vs. volumetric flow rate computed from Euler number";
+  final parameter Real powEuDer[:] = powEu_internal.d
+    "Power derivative with respect to volumetric flow rate computed from Euler number";
+
   parameter Boolean haveMinimumDecrease=
-    Modelica.Math.BooleanVectors.allTrue({(per.pressure.dp[i + 1] -
-    per.pressure.dp[i])/(per.pressure.V_flow[i + 1] - per.pressure.V_flow[
-    i]) < -kRes for i in 1:nOri - 1}) "Flag used for reporting";
+    if nOri<2 then false
+    else
+      Modelica.Math.BooleanVectors.allTrue({(per.pressure.dp[i + 1] -
+      per.pressure.dp[i])/(per.pressure.V_flow[i + 1] - per.pressure.V_flow[
+      i]) < -kRes for i in 1:nOri - 1}) "Flag used for reporting";
 
   parameter Boolean haveDPMax = (abs(per.pressure.V_flow[1])  < Modelica.Constants.eps)
     "Flag, true if user specified data that contain dpMax";
 
   Modelica.Blocks.Interfaces.RealOutput dp_internal
     "If dp is prescribed, use dp_in and solve for r_N, otherwise compute dp using r_N";
+
+  Modelica.Units.SI.Efficiency eta_internal
+    "Either eta or etaHyd";
+
+  Modelica.Units.SI.Power P_internal
+    "Either PEle or WHyd";
+
+  parameter Real deltaP = 1E-4 * V_flow_max * dpMax
+    "Small value for regularisation of power";
+
+  Real yMot(final min=0, final start=0.833)=
+    if per.haveWMot_nominal
+      then WHyd/per.WMot_nominal
+    else 1
+    "Motor part load ratio";
+
 function getPerformanceDataAsString
   input AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters pressure
       "Performance data";
@@ -265,49 +363,52 @@ initial equation
   assert(AixLib.Utilities.Math.Functions.isMonotonic(x=per.pressure.V_flow, strict=true) and
   per.pressure.V_flow[1] > -Modelica.Constants.eps,
   "The fan pressure rise must be a strictly decreasing sequence with respect to the volume flow rate,
-   with the first element for the fan pressure raise being non-zero.
- The following performance data have been entered:
- "+ getArrayAsString(per.pressure.V_flow, "pressure.V_flow"));
+  with the first element for the fan pressure raise being non-zero.
+The following performance data have been entered:
+" + getArrayAsString(per.pressure.V_flow, "pressure.V_flow"));
 
   if not haveVMax then
-    assert((per.pressure.V_flow[nOri]-per.pressure.V_flow[nOri-1])
-         /((per.pressure.dp[nOri]-per.pressure.dp[nOri-1]))<0,
-    "The last two pressure points for the fan or pump performance curve must be decreasing.
-     You need to set more reasonable parameters.
- Received
- "+ getArrayAsString(per.pressure.dp, "dp"));
-
+    assert(nOri>=2,
+      "When the maximum flow is not specified,
+      at least two points are needed for the power curve.");
+    if nOri>=2 then
+      assert((per.pressure.V_flow[nOri]-per.pressure.V_flow[nOri-1])
+           /((per.pressure.dp[nOri]-per.pressure.dp[nOri-1]))<0,
+    "The last two pressure points for the fan or pump's performance curve must be decreasing.
+Received
+" + getArrayAsString(per.pressure.dp, "dp"));
+    end if;
   end if;
 
   // Write warning if the volumetric flow rate versus pressure curve does not satisfy
   // the minimum decrease condition
   if (not haveMinimumDecrease) then
     Modelica.Utilities.Streams.print("
- Warning:
- ========
- It is recommended that the volume flow rate versus pressure relation
- of the fan or pump satisfies the minimum decrease condition
- 
-         (per.pressure.dp[i+1]-per.pressure.dp[i])
- d[i] = ------------------------------------------------- < "+ String(-kRes) + "
-        (per.pressure.V_flow[i+1]-per.pressure.V_flow[i])
- 
-  is
- "+ getArrayAsString({(per.pressure.dp[i+1]-per.pressure.dp[i])
+Warning:
+========
+It is recommended that the volume flow rate versus pressure relation
+of the fan or pump satisfy the minimum decrease condition
+
+        (per.pressure.dp[i+1]-per.pressure.dp[i])
+d[i] = ------------------------------------------------- < " + String(-kRes) + "
+       (per.pressure.V_flow[i+1]-per.pressure.V_flow[i])
+
+ is
+" + getArrayAsString({(per.pressure.dp[i+1]-per.pressure.dp[i])
         /(per.pressure.V_flow[i+1]-per.pressure.V_flow[i]) for i in 1:nOri-1}, "d") + "
- Otherwise, a solution to the equations may not exist if the fan or pump speed is reduced.
- In this situation, the solver will fail due to non-convergence and
- the simulation stops.");
+Otherwise, a solution to the equations may not exist if the fan or pump's speed is reduced.
+In this situation, the solver will fail due to non-convergence and
+the simulation stops.");
   end if;
 
-  // Correction for flow resistance of pump or fan
-  if (haveVMax and haveDPMax) or (nOri == 2) then  // ----- Curve 1
+  // Correction for flow resistance of the fan or pump
+  if curve == 1 then  // ----- Curve 1
     // V_flow_max and dpMax are provided by the user, or we only have two data points
     preDer1= AixLib.Utilities.Math.Functions.splineDerivatives(x=pCur1.V_flow,
       y=pCur1.dp);
     preDer2= zeros(nOri + 1);
     preDer3= zeros(nOri + 2);
-  elseif haveVMax or haveDPMax then  // ----- Curve 2
+  elseif curve == 2 then  // ----- Curve 2
     // V_flow_max or dpMax is provided by the user, but not both
     preDer1= zeros(nOri);
     preDer2= AixLib.Utilities.Math.Functions.splineDerivatives(x=pCur2.V_flow,
@@ -321,31 +422,36 @@ initial equation
       y=pCur3.dp);
   end if;
 
- // Compute derivatives for cubic spline
- motDer = if per.use_powerCharacteristic then zeros(size(per.motorEfficiency.V_flow,
-    1)) elseif (size(per.motorEfficiency.V_flow, 1) == 1) then {0} else
-    AixLib.Utilities.Math.Functions.splineDerivatives(
-    x=per.motorEfficiency.V_flow,
-    y=per.motorEfficiency.eta,
-    ensureMonotonicity=AixLib.Utilities.Math.Functions.isMonotonic(x=per.motorEfficiency.eta,
-      strict=false));
-  hydDer = if per.use_powerCharacteristic then zeros(size(per.hydraulicEfficiency.V_flow,
-    1)) elseif (size(per.hydraulicEfficiency.V_flow, 1) == 1) then {0}
-     else AixLib.Utilities.Math.Functions.splineDerivatives(x=per.hydraulicEfficiency.V_flow,
-    y=per.hydraulicEfficiency.eta);
+  assert(not ((per.etaMotMet==
+           AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio
+           or  per.etaMotMet==
+           AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve)
+         and not per.haveWMot_nominal),
+         "In " + getInstanceName() + ": etaMotMet is set to
+         .Efficiency_MotorPartLoadRatio or .GenericCurve which requires
+         the motor's rated power, but per.WMot_nominal is not assigned or
+         cannot be estimated because no power curve is provided.");
+
+  assert(max(per.power.P)<1E-6 or per.WMot_nominal>max(per.power.P)*0.99,
+         "In " + getInstanceName() + ": The rated motor power provided in
+         per.WMot_nominal is smaller than the maximum power provided in per.power.
+         Use a larger value for per.WMot_nominal or leave it blank to allow the
+         model to assume a default value.");
 
   assert(homotopyInitialization, "In " + getInstanceName() +
-    ": The constant homotopyInitialization has been modified from its default value. This constant will be removed in future releases.",
-    level = AssertionLevel.warning);
+         ": The constant homotopyInitialization has been modified from its default
+         value. This constant will be removed in future releases.",
+         level = AssertionLevel.warning);
 
 equation
-  //assign values of dp and r_N, depending on which variable exists and is prescribed
+  // Assign values of dp and r_N, depending on which variable exists and is prescribed
   connect(dp_internal,dp);
   connect(dp_internal,dp_in);
   connect(r_N, y_in);
   y_out=r_N;
 
-  V_flow = m_flow/rho;
+  // Flow rate conversion
+  V_flow = m_flow / rho;
 
   // Hydraulic equations
   r_V = V_flow/V_flow_max;
@@ -483,66 +589,132 @@ equation
     // end of if/else choosing between exact/simplified power computation
   end if;
 
-  // Flow work
-  WFlo = dp_internal*V_flow;
+  // Power and efficiency
+  WFlo = AixLib.Utilities.Math.Functions.smoothMax(
+           x1=dp_internal*V_flow,
+           x2=0,
+           deltaX=deltaP/2);
+  if per.powerOrEfficiencyIsHydraulic then
+    eta = etaHyd * etaMot;
+  else
+    etaHyd = AixLib.Utilities.Math.Functions.smoothMin(
+               x1=eta/etaMot, x2=1, deltaX=1E-3);
+  end if;
 
-  // Power consumption
-  if per.use_powerCharacteristic then
-    // For the homotopy, we want P/V_flow to be bounded as V_flow -> 0 to avoid a very high medium
-    // temperature near zero flow.
+  // Hydraulic efficiency etaHyd and hydraulic work WHyd
+  //   or total efficiency eta and total electric power PEle
+  //   depending on the information provided
+  if per.powerOrEfficiencyIsHydraulic then
+    P_internal=WHyd;
+    eta_internal=etaHyd;
+    PEle = WFlo / AixLib.Utilities.Math.Functions.smoothMax(
+                    x1=eta, x2=1E-2, deltaX=1E-3);
+  else
+    P_internal=PEle;
+    eta_internal=eta;
+    WHyd = WFlo / AixLib.Utilities.Math.Functions.smoothMax(
+                    x1=etaHyd, x2=1E-2, deltaX=1E-3);
+  end if;
+  if per.etaHydMet==
+       AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate then
     if homotopyInitialization then
-      PEle = homotopy(actual=cha.power(per=per.power, V_flow=V_flow, r_N=r_N, d=powDer, delta=delta),
+      P_internal = homotopy(actual=cha.power(per=per.power, V_flow=V_flow, r_N=r_N, d=powDer, delta=delta),
                       simplified=V_flow/V_flow_nominal*
                             cha.power(per=per.power, V_flow=V_flow_nominal, r_N=1, d=powDer, delta=delta));
     else
-      PEle = (rho/rho_default)*cha.power(per=per.power, V_flow=V_flow, r_N=r_N, d=powDer, delta=delta);
+      P_internal = (rho/rho_default)*cha.power(per=per.power, V_flow=V_flow, r_N=r_N, d=powDer, delta=delta);
     end if;
-    // To compute the efficiency, we set a lower bound on the electricity consumption.
-    // This is needed because WFlo can be close to zero when P is zero, thereby
-    // causing a division by zero.
-    // Earlier versions of the model computed WFlo = eta * P, but this caused
-    // a division by zero.
-    eta = WFlo / AixLib.Utilities.Math.Functions.smoothMax(x1=PEle, x2=1E-5, deltaX=1E-6);
-    // In this configuration, we only know the total power consumption.
-    // Because nothing is known about etaMot versus etaHyd, we set etaHyd=1. This will
-    // cause etaMot=eta, because eta=etaHyd*etaMot.
-    // Earlier versions used etaMot=sqrt(eta), but as eta->0, this function has
-    // and infinite derivative.
-    etaHyd = 1;
-    etaMot = eta;
-  else
+    eta_internal = WFlo/AixLib.Utilities.Math.Functions.smoothMax(
+                     x1=P_internal, x2=deltaP, deltaX=deltaP/2);
+  elseif per.etaHydMet==
+       AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber then
+    if homotopyInitialization then
+      P_internal = homotopy(actual=cha.power(per=powEu, V_flow=V_flow, r_N=r_N, d=powEuDer, delta=delta),
+                      simplified=V_flow/V_flow_nominal*
+                            cha.power(per=powEu, V_flow=V_flow_nominal, r_N=1, d=powEuDer, delta=delta));
+    else
+      P_internal = (rho/rho_default)*cha.power(per=powEu, V_flow=V_flow, r_N=r_N, d=powEuDer, delta=delta);
+    end if;
+    eta_internal = WFlo / AixLib.Utilities.Math.Functions.smoothMax(
+                            x1=P_internal, x2=deltaP, deltaX=deltaP/2);
+  elseif per.etaHydMet == AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate then
+    if homotopyInitialization then
+      eta_internal = homotopy(actual=cha.efficiency(per=per.efficiency,     V_flow=V_flow, d=etaDer, r_N=r_N, delta=delta),
+                        simplified=cha.efficiency(per=per.efficiency, V_flow=V_flow_max,   d=etaDer, r_N=r_N, delta=delta));
+    else
+      eta_internal = cha.efficiency(per=per.efficiency, V_flow=V_flow, d=etaDer, r_N=r_N, delta=delta);
+    end if;
+    P_internal=WFlo/AixLib.Utilities.Math.Functions.smoothMax(
+                      x1=eta_internal, x2=1E-2, deltaX=1E-3);
+  else // Not provided
+    if per.powerOrEfficiencyIsHydraulic then
+      eta_internal=0.7;
+    else
+      eta_internal=0.49;
+    end if;
+    P_internal=WFlo/eta_internal;
+  end if;
+
+  // Motor efficiency etaMot
+  if per.etaMotMet == AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_VolumeFlowRate then
     if homotopyInitialization then
-      etaHyd = homotopy(actual=cha.efficiency(per=per.hydraulicEfficiency,     V_flow=V_flow, d=hydDer, r_N=r_N, delta=delta),
-                        simplified=cha.efficiency(per=per.hydraulicEfficiency, V_flow=V_flow_max,   d=hydDer, r_N=r_N, delta=delta));
       etaMot = homotopy(actual=cha.efficiency(per=per.motorEfficiency,     V_flow=V_flow, d=motDer, r_N=r_N, delta=delta),
                         simplified=cha.efficiency(per=per.motorEfficiency, V_flow=V_flow_max,   d=motDer, r_N=r_N, delta=delta));
     else
-      etaHyd = cha.efficiency(per=per.hydraulicEfficiency, V_flow=V_flow, d=hydDer, r_N=r_N, delta=delta);
       etaMot = cha.efficiency(per=per.motorEfficiency,     V_flow=V_flow, d=motDer, r_N=r_N, delta=delta);
     end if;
-    // To compute the electrical power, we set a lower bound for eta to avoid
-    // a division by zero.
-    PEle = WFlo / AixLib.Utilities.Math.Functions.smoothMax(x1=eta, x2=1E-5, deltaX=1E-6);
-    eta = etaHyd * etaMot;
-
+  elseif per.etaMotMet==
+       AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio then
+    if homotopyInitialization then
+      etaMot =homotopy(actual=cha.efficiency_yMot(
+        per=per.motorEfficiency_yMot,
+        y=yMot,
+        d=motDer_yMot), simplified=cha.efficiency_yMot(
+        per=per.motorEfficiency_yMot,
+        y=1,
+        d=motDer_yMot));
+    else
+      etaMot =cha.efficiency_yMot(
+        per=per.motorEfficiency_yMot,
+        y=yMot,
+        d=motDer_yMot);
+    end if;
+  elseif per.etaMotMet==
+       AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve then
+      if homotopyInitialization then
+        etaMot =homotopy(actual=cha.efficiency_yMot(
+          per=per.motorEfficiency_yMot_generic,
+          y=yMot,
+          d=motDer_yMot_generic), simplified=cha.efficiency_yMot(
+          per=per.motorEfficiency_yMot_generic,
+          y=1,
+          d=motDer_yMot_generic));
+      else
+        etaMot =cha.efficiency_yMot(
+          per=per.motorEfficiency_yMot_generic,
+          y=yMot,
+          d=motDer_yMot_generic);
+      end if;
+  else // Not provided
+    etaMot = 0.7;
   end if;
 
   annotation (
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
                     graphics={
-        Text(extent={{56,66},{106,52}},
+        Text(extent={{56,84},{106,70}},
           textColor={0,0,127},
           textString="dp"),
-        Text(extent={{56,8},{106,-6}},
+        Text(extent={{56,-10},{106,-24}},
           textColor={0,0,127},
           textString="PEle"),
-        Text(extent={{52,-22},{102,-36}},
+        Text(extent={{48,-48},{98,-62}},
           textColor={0,0,127},
           textString="eta"),
-        Text(extent={{50,-52},{100,-66}},
+        Text(extent={{50,-68},{100,-82}},
           textColor={0,0,127},
           textString="etaHyd"),
-        Text(extent={{50,-72},{100,-86}},
+        Text(extent={{50,-86},{100,-100}},
           textColor={0,0,127},
           textString="etaMot"),
         Ellipse(
@@ -592,10 +764,10 @@ equation
           smooth=Smooth.Bezier,
           origin={-43,-31},
           rotation=90),
-        Text(extent={{56,36},{106,22}},
+        Text(extent={{56,28},{106,14}},
           textColor={0,0,127},
           textString="WFlo"),
-        Text(extent={{56,94},{106,80}},
+        Text(extent={{56,66},{106,52}},
           textColor={0,0,127},
           textString="V_flow"),
         Line(
@@ -609,166 +781,233 @@ equation
         Line(
           points={{-70,86},{-40,84},{8,68},{36,42}},
           color={0,0,0},
-          smooth=Smooth.Bezier)}),
+          smooth=Smooth.Bezier),
+        Text(extent={{56,102},{106,88}},
+          textColor={0,0,127},
+          textString="y_out"),
+        Text(extent={{56,8},{106,-6}},
+          textColor={0,0,127},
+          textString="WHyd")}),
     Documentation(info="<html>
- <p>
- This is an interface that implements the functions to compute the head, power draw
- and efficiency of fans and pumps.
- </p>
- <p>
- The nominal hydraulic characteristic (volume flow rate versus total pressure)
- is given by a set of data points
- using the data record <code>per</code>, which is an instance of
- <a href=\"modelica://AixLib.Fluid.Movers.Data.Generic\">
- AixLib.Fluid.Movers.Data.Generic</a>.
- A cubic hermite spline with linear extrapolation is used to compute
- the performance at other operating points.
- </p>
- <p>
- The fan or pump energy balance can be specified in two alternative ways:
- </p>
- <ul>
- <li>
- If <code>per.use_powerCharacteristic = false</code>, then the data points for
- normalized volume flow rate versus efficiency is used to determine the efficiency,
- and then the power consumption. The default is a constant efficiency of <i>0.7</i>.
- </li>
- <li>
- If <code>per.use_powerCharacteristic = true</code>, then the data points for
- normalized volume flow rate versus power consumption
- is used to determine the power consumption, and then the efficiency
- is computed based on the actual power consumption and the flow work.
- </li>
- </ul>
- <p>
- For exceptions to this general rule, check the
- <a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
- User's Guide</a> for more information.
- </p>
- 
- <h4>Implementation</h4>
- <p>
- For numerical reasons, the user-provided data points for volume flow rate
- versus pressure rise are modified to add a fan internal flow resistance.
- Because this flow resistance is subtracted during the simulation when
- computing the fan pressure rise, the model reproduces the exact points
- that were provided by the user.
- </p>
- <p>
- Also for numerical reasons, the pressure rise at zero flow rate and
- the flow rate at zero pressure rise is added to the user-provided data,
- unless the user already provides these data points.
- Since Modelica 3.2 does not allow dynamic memory allocation, this
- implementation required the use of three different arrays for the
- situation where no additional point is added, where one additional
- point is added and where two additional points are added.
- The parameter <code>curve</code> causes the correct data record
- to be used during the simulation.
- </p>
- </html>",
+<p>
+This is an interface that implements the functions to compute the head, power draw
+and efficiency of fans and pumps.
+</p>
+<p>
+The nominal hydraulic characteristic (total pressure rise versus volume flow rate)
+is given by a set of data points
+using the data record <code>per</code>, which is an instance of
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Generic\">
+AixLib.Fluid.Movers.Data.Generic</a>.
+A cubic hermite spline with linear extrapolation is used to compute
+the performance at other operating points.
+</p>
+<p>
+The model computes the power and efficiency items in the list below.
+</p>
+<ul>
+<li>
+Flow work:<br/>
+<i>W&#775;<sub>flo</sub> = V&#775; &sdot; &Delta;p</i>
+</li>
+<li>
+Total efficiency and consumed electric power:<br/>
+<i>&eta; = W&#775;<sub>flo</sub> &frasl; P<sub>ele</sub></i>
+</li>
+<li>
+Hydraulic effiency and hydraulic work (shaft work, brake horsepower):<br/>
+<i>&eta;<sub>hyd</sub> = W&#775;<sub>flo</sub> &frasl; W&#775;<sub>hyd</sub></i>
+</li>
+<li>
+Motor efficiency:<br/>
+<i>&eta;<sub>mot</sub> = W&#775;<sub>hyd</sub> &frasl; P<sub>ele</sub></i>
+</li>
+</ul>
+<p>
+See
+<a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
+AixLib.Fluid.Movers.UsersGuide</a>
+for how the user can provide power and efficiency information to the model.
+</p>
+<h4>Implementation</h4>
+<p>
+For numerical reasons, the user-provided data points for volume flow rate
+versus pressure rise are modified to add a fan internal flow resistance.
+Because this flow resistance is subtracted during the simulation when
+computing the fan pressure rise, the model reproduces the exact points
+that were provided by the user.
+</p>
+<p>
+Also for numerical reasons, the pressure rise at zero flow rate and
+the flow rate at zero pressure rise is added to the user-provided data,
+unless the user already provides these data points.
+Since Modelica 3.2 does not allow dynamic memory allocation, this
+implementation required the use of three different arrays for the
+situation where no additional point is added, where one additional
+point is added and where two additional points are added.
+The parameter <code>curve</code> causes the correct data record
+to be used during the simulation.
+</p>
+<p>
+In order to prevent the model from producing negative mover power
+when either the flow rate or pressure rise is forced to be negative,
+the flow work <i>W&#775;<sub>flo</sub></i> is constrained to be non-negative.
+The regularisation starts around 0.01% of the characteristic maximum power
+<i>W&#775;<sub>max</sub> = V&#775;<sub>max</sub> &Delta;p<sub>max</sub></i>.
+See discussions and an example of this situation in
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1621\">IBPSA, #1621</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- December 2, 2016, by Michael Wetter:<br/>
- Removed <code>min</code> attribute as otherwise numerical noise can cause
- the assertion on the limit to fail.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
- </li>
- <li>
- February 19, 2016, by Michael Wetter and Filip Jorissen:<br/>
- Refactored model to make implementation clearer.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference and reformatted code.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- September 2, 2015, by Michael Wetter:<br/>
- Corrected computation of
- <code>etaMot = cha.efficiency(per=per.motorEfficiency, V_flow=V_flow, d=motDer, r_N=r_N, delta=1E-4)</code>
- which previously used <code>V_flow_max</code> instead of <code>V_flow</code>.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised model for OpenModelica.
- </li>
- <li>
- November 22, 2014, by Michael Wetter:<br/>
- Removed in <code>N_actual</code> and <code>N_filtered</code>
- the <code>max</code> attribute to
- avoid a translation warning.
- </li>
- <li>
- April 21, 2014, by Filip Jorissen and Michael Wetter:<br/>
- Changed model to use
- <a href=\"modelica://AixLib.Fluid.Movers.Data.Generic\">
- AixLib.Fluid.Movers.Data.Generic</a>.
- April 19, 2014, by Filip Jorissen:<br/>
- Passed extra parameters to power() and efficiency()
- to be able to properly evaluate the
- scaling law. See
- <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
- for a discussion and validation.
- </li>
- <li>
- September 27, 2013, by Michael Wetter:<br/>
- Reformulated <code>per=if (curve == 1) then pCur1 elseif (curve == 2) then pCur2 else pCur3</code>
- by moving the computation into the idividual logical branches because OpenModelica generates an
- error when assign the statement to <code>data</code>
- as <code>pCur1</code>, <code>pCur2</code> and <code>pCur3</code> have different dimensions.
- </li>
- <li>
- September 17, 2013, by Michael Wetter:<br/>
- Added missing <code>each</code> keyword in declaration of parameters
- that are an array.
- </li>
- <li>
- March 20, 2013, by Michael Wetter:<br/>
- Removed assignment in declaration of <code>pCur?.V_flow</code> as
- these parameters have the attribute <code>fixed=false</code> set.
- </li>
- <li>
- October 11, 2012, by Michael Wetter:<br/>
- Added implementation of <code>WFlo = eta * P</code> with
- guard against division by zero.
- Changed implementation of <code>etaMot=sqrt(eta)</code> to
- <code>etaHyd = 1</code> to avoid infinite derivative as <code>eta</code>
- converges to zero.
- </li>
- <li>
- February 20, 2012, by Michael Wetter:<br/>
- Assigned value to nominal attribute of <code>V_flow</code>.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- October 4 2011, by Michael Wetter:<br/>
- Revised the implementation of the pressure drop computation as a function
- of speed and volume flow rate.
- The new implementation avoids a singularity near zero volume flow rate and zero speed.
- </li>
- <li>
- March 28 2011, by Michael Wetter:<br/>
- Added <code>homotopy</code> operator.
- </li>
- <li>
- March 23 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 15, 2024, by Hongxiang Fu:<br/>
+Corrected efficiency equations if
+<code>powerOrEfficiencyIsHydraulic=false</code>
+and specified the <code>start</code> attribute for <code>etaHyd</code>
+and <code>etaMot</code> to suppress a warning.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1880\">IBPSA, #1880</a>.
+</li>
+<li>
+August 8, 2022, by Hongxiang Fu:<br/>
+<ul>
+<li>
+Modified the power and efficiency computation to allow computing
+the hydraulic efficiency <code>etaHyd</code> and
+the motor efficiency <code>etaMot</code> separately;
+</li>
+<li>
+Implemented the option to compute the total efficiency <code>eta</code>
+or the hydraulic efficiency <code>etaHyd</code> using the Euler number.
+</li>
+<li>
+Implemented the option for the user to provide the motor efficiency
+<code>etaMot</code> as a function of part load ratio <i>y</i>. Also allowed generic
+curves to be used.
+</li>
+<li>
+Moved <code>haveVMax</code> here from
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine\">
+AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine</a>.
+</li>
+<li>
+Now it passes <code>WHyd</code> instead of <code>etaHyd</code> to
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.PowerInterface\">
+AixLib.Fluid.Movers.BaseClasses.PowerInterface</a>.
+</li>
+<li>
+Now the flow work <code>WFlo</code> is bounded to be non-negative.
+</li>
+</ul>
+These are for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+June 6, 2022, by Hongxiang Fu:<br/>
+Added a constraint that <i>W<sub>flo</sub> = V&#775; &Delta;p &ge; 0</i>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1621\">IBPSA, #1621</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+December 2, 2016, by Michael Wetter:<br/>
+Removed <code>min</code> attribute as otherwise numerical noise can cause
+the assertion on the limit to fail.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
+</li>
+<li>
+February 19, 2016, by Michael Wetter and Filip Jorissen:<br/>
+Refactored model to make implementation clearer.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference and reformatted code.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+September 2, 2015, by Michael Wetter:<br/>
+Corrected computation of
+<code>etaMot = cha.efficiency(per=per.motorEfficiency, V_flow=V_flow, d=motDer, r_N=r_N, delta=1E-4)</code>
+which previously used <code>V_flow_max</code> instead of <code>V_flow</code>.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised model for OpenModelica.
+</li>
+<li>
+November 22, 2014, by Michael Wetter:<br/>
+Removed in <code>N_actual</code> and <code>N_filtered</code>
+the <code>max</code> attribute to
+avoid a translation warning.
+</li>
+<li>
+April 21, 2014, by Filip Jorissen and Michael Wetter:<br/>
+Changed model to use
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Generic\">
+AixLib.Fluid.Movers.Data.Generic</a>.
+April 19, 2014, by Filip Jorissen:<br/>
+Passed extra parameters to power() and efficiency()
+to be able to properly evaluate the
+scaling law. See
+<a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
+for a discussion and validation.
+</li>
+<li>
+September 27, 2013, by Michael Wetter:<br/>
+Reformulated <code>per=if (curve == 1) then pCur1 elseif (curve == 2) then pCur2 else pCur3</code>
+by moving the computation into the idividual logical branches because OpenModelica generates an
+error when assign the statement to <code>data</code>
+as <code>pCur1</code>, <code>pCur2</code> and <code>pCur3</code> have different dimensions.
+</li>
+<li>
+September 17, 2013, by Michael Wetter:<br/>
+Added missing <code>each</code> keyword in declaration of parameters
+that are an array.
+</li>
+<li>
+March 20, 2013, by Michael Wetter:<br/>
+Removed assignment in declaration of <code>pCur?.V_flow</code> as
+these parameters have the attribute <code>fixed=false</code> set.
+</li>
+<li>
+October 11, 2012, by Michael Wetter:<br/>
+Added implementation of <code>WFlo = eta * P</code> with
+guard against division by zero.
+Changed implementation of <code>etaMot=sqrt(eta)</code> to
+<code>etaHyd = 1</code> to avoid infinite derivative as <code>eta</code>
+converges to zero.
+</li>
+<li>
+February 20, 2012, by Michael Wetter:<br/>
+Assigned value to nominal attribute of <code>V_flow</code>.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+October 4 2011, by Michael Wetter:<br/>
+Revised the implementation of the pressure drop computation as a function
+of speed and volume flow rate.
+The new implementation avoids a singularity near zero volume flow rate and zero speed.
+</li>
+<li>
+March 28 2011, by Michael Wetter:<br/>
+Added <code>homotopy</code> operator.
+</li>
+<li>
+March 23 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowMachineInterface;
diff --git a/AixLib/Fluid/Movers/BaseClasses/IdealSource.mo b/AixLib/Fluid/Movers/BaseClasses/IdealSource.mo
index 16a162a1ba..5dc69db9ed 100644
--- a/AixLib/Fluid/Movers/BaseClasses/IdealSource.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/IdealSource.mo
@@ -79,75 +79,75 @@ equation
           textColor={255,255,255},
           textString="m")}),
     Documentation(info="<html>
- <p>
- Model of a fictitious pipe that is used as a base class
- for a pressure source or to prescribe a mass flow rate.
- </p>
- <p>
- Note that for fans and pumps with dynamic balance,
- both the heat and the flow work are added to the volume of
- air or water. This simplifies the equations compared to
- adding heat to the volume, and flow work to this model.
- </p>
- <p>
- Typically either <code>control_m_flow</code> or
- <code>control_dp</code> should be <code>true</code> to avoid a
- singular system.
- If <code>control_m_flow = true</code>, then the mass flow rate
- is set to the value of the input connector <code>m_flow_in</code>.
- Otherwise, this model does not specify the mass flow rate.
- Similarly, if <code>control_dp = true</code>, the head is equal to the
- value of the input connector <code>dp_in</code>.
- Otherwise, this model does not specify the head.
- </p>
- </html>",
+<p>
+Model of a fictitious pipe that is used as a base class
+for a pressure source or to prescribe a mass flow rate.
+</p>
+<p>
+Note that for fans and pumps with dynamic balance,
+both the heat and the flow work are added to the volume of
+air or water. This simplifies the equations compared to
+adding heat to the volume, and flow work to this model.
+</p>
+<p>
+Typically either <code>control_m_flow</code> or
+<code>control_dp</code> should be <code>true</code> to avoid a
+singular system.
+If <code>control_m_flow = true</code>, then the mass flow rate
+is set to the value of the input connector <code>m_flow_in</code>.
+Otherwise, this model does not specify the mass flow rate.
+Similarly, if <code>control_dp = true</code>, the head is equal to the
+value of the input connector <code>dp_in</code>.
+Otherwise, this model does not specify the head.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 4, 2017, by Filip Jorissen:<br/>
- Implemented option to set <code>control_dp</code>
- independently from <code>control_m_flow</code>.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/770\">#770</a>.
- </li>
- <li>
- March 2, 2017, by Filip Jorissen:<br/>
- Implemented simplification when <code>allowFlowReversal=false</code>.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/673\">#673</a>.
- </li>
- <li>
- March 20, 2016, by Michael Wetter:<br/>
- Corrected documentation for <code>dp_in</code>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Added units to the signal connectors.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- October 8, 2013, by Michael Wetter:<br/>
- Removed parameter <code>show_V_flow</code>.
- </li>
- <li>
- May 25, 2011 by Michael Wetter:<br/>
- Removed the option to add power to the medium, as this is dealt with in the volume
- that is used in the mover model.
- </li>
- <li>
- July 27, 2010 by Michael Wetter:<br/>
- Redesigned model to fix bug in medium balance.
- </li>
- <li>
- April 13, 2010 by Michael Wetter:<br/>
- Made heat connector optional.
- </li>
- <li>
- March 23, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 4, 2017, by Filip Jorissen:<br/>
+Implemented option to set <code>control_dp</code>
+independently from <code>control_m_flow</code>.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/770\">#770</a>.
+</li>
+<li>
+March 2, 2017, by Filip Jorissen:<br/>
+Implemented simplification when <code>allowFlowReversal=false</code>.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/673\">#673</a>.
+</li>
+<li>
+March 20, 2016, by Michael Wetter:<br/>
+Corrected documentation for <code>dp_in</code>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Added units to the signal connectors.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Removed parameter <code>show_V_flow</code>.
+</li>
+<li>
+May 25, 2011 by Michael Wetter:<br/>
+Removed the option to add power to the medium, as this is dealt with in the volume
+that is used in the mover model.
+</li>
+<li>
+July 27, 2010 by Michael Wetter:<br/>
+Redesigned model to fix bug in medium balance.
+</li>
+<li>
+April 13, 2010 by Michael Wetter:<br/>
+Made heat connector optional.
+</li>
+<li>
+March 23, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IdealSource;
diff --git a/AixLib/Fluid/Movers/BaseClasses/PartialFlowMachine.mo b/AixLib/Fluid/Movers/BaseClasses/PartialFlowMachine.mo
index 38749d6189..fde5094a05 100644
--- a/AixLib/Fluid/Movers/BaseClasses/PartialFlowMachine.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/PartialFlowMachine.mo
@@ -4,15 +4,13 @@ partial model PartialFlowMachine
   extends AixLib.Fluid.Interfaces.LumpedVolumeDeclarations(
     final massDynamics=energyDynamics,
     final mSenFac=1);
-  extends AixLib.Fluid.Interfaces.PartialTwoPortInterface(
-    m_flow_nominal(final min=Modelica.Constants.small),
-    show_T=false,
+  extends AixLib.Fluid.Interfaces.PartialTwoPort(
     port_a(
+      p(start=Medium.p_default),
       h_outflow(start=h_outflow_start)),
     port_b(
-      h_outflow(start=h_outflow_start),
       p(start=p_start),
-      final m_flow(max = if allowFlowReversal then +Modelica.Constants.inf else 0)));
+      h_outflow(start=h_outflow_start)));
 
   replaceable parameter AixLib.Fluid.Movers.Data.Generic per
     constrainedby AixLib.Fluid.Movers.Data.Generic
@@ -65,7 +63,7 @@ partial model PartialFlowMachine
     annotation(Dialog(tab="Dynamics", group="Filtered speed",enable=use_inputFilter));
 
   // Connectors and ports
-    Modelica.Blocks.Interfaces.IntegerInput stage
+  Modelica.Blocks.Interfaces.IntegerInput stage
     if inputType == AixLib.Fluid.Types.InputType.Stages
     "Stage input signal for the pressure head"
     annotation (Placement(
@@ -76,7 +74,7 @@ partial model PartialFlowMachine
 
   Modelica.Blocks.Interfaces.RealOutput y_actual(
     final unit="1")
-    "Actual normalised pump speed that is used for computations"
+    "Actual normalised fan or pump speed that is used for computations"
     annotation (Placement(transformation(extent={{100,60},{120,80}}),
         iconTransformation(extent={{100,60},{120,80}})));
 
@@ -86,7 +84,8 @@ partial model PartialFlowMachine
     annotation (Placement(transformation(extent={{100,80},{120,100}}),
         iconTransformation(extent={{100,80},{120,100}})));
 
-  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a heatPort
+  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a heatPort(
+    T(start=293.15))
     "Heat dissipation to environment"
     annotation (Placement(transformation(extent={{-70,-110},{-50,-90}}),
         iconTransformation(extent={{-10,-78},{10,-58}})));
@@ -102,11 +101,66 @@ partial model PartialFlowMachine
   Real etaMot(unit="1", final quantity="Efficiency") = eff.etaMot "Motor efficiency";
 
   // Quantity to control
+
+  // Copied from Fluid.Interfaces.PartialTwoPortInterface
+  parameter Modelica.Units.SI.MassFlowRate m_flow_small(min=0) = 1E-4*abs(
+    _m_flow_nominal) "Small mass flow rate for regularization of zero flow"
+    annotation (Dialog(tab="Advanced"));
+  // Diagnostics
+   parameter Boolean show_T = false
+    "= true, if actual temperature at port is computed"
+    annotation (
+      Dialog(tab="Advanced", group="Diagnostics"),
+      HideResult=true);
+
+  Modelica.Units.SI.MassFlowRate m_flow(start=_m_flow_start) = port_a.m_flow
+    "Mass flow rate from port_a to port_b (m_flow > 0 is design flow direction)";
+
+  Modelica.Units.SI.PressureDifference dp(
+    start=_dp_start,
+    displayUnit="Pa") = port_a.p - port_b.p
+    "Pressure difference between port_a and port_b";
+
+  Medium.ThermodynamicState sta_a=
+    if allowFlowReversal then
+      Medium.setState_phX(port_a.p,
+                          noEvent(actualStream(port_a.h_outflow)),
+                          noEvent(actualStream(port_a.Xi_outflow)))
+    else
+      Medium.setState_phX(port_a.p,
+                          noEvent(inStream(port_a.h_outflow)),
+                          noEvent(inStream(port_a.Xi_outflow)))
+      if show_T "Medium properties in port_a";
+
+  Medium.ThermodynamicState sta_b=
+    if allowFlowReversal then
+      Medium.setState_phX(port_b.p,
+                          noEvent(actualStream(port_b.h_outflow)),
+                          noEvent(actualStream(port_b.Xi_outflow)))
+    else
+      Medium.setState_phX(port_b.p,
+                          noEvent(port_b.h_outflow),
+                          noEvent(port_b.Xi_outflow))
+       if show_T "Medium properties in port_b";
+  // - Copy continues in protected section
+
 protected
+  parameter Modelica.Units.SI.MassFlowRate _m_flow_nominal=
+    max(eff.per.pressure.V_flow)*rho_default
+    "Nominal mass flow rate";
+
+  // Copied from Fluid.Interfaces.PartialTwoPortInterface
+  final parameter Modelica.Units.SI.MassFlowRate _m_flow_start=0
+    "Start value for m_flow, used to avoid a warning if not set in m_flow, and to avoid m_flow.start in parameter window";
+  final parameter Modelica.Units.SI.PressureDifference _dp_start(displayUnit=
+        "Pa") = 0
+    "Start value for dp, used to avoid a warning if not set in dp, and to avoid dp.start in parameter window";
+  // - End of copy
+
   final parameter Modelica.Units.SI.VolumeFlowRate _VMachine_flow=0
     "Start value for VMachine_flow, used to avoid a warning if not specified";
 
-  parameter Types.PrescribedVariable preVar "Type of prescribed variable";
+  parameter AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable preVar "Type of prescribed variable";
 
   // The parameter speedIsInput is required to conditionally remove the instance gain.
   // If the conditional removal of this instance where to use the test
@@ -123,15 +177,12 @@ protected
     "Number of data points for pressure curve"
     annotation(Evaluate=true);
 
-  final parameter Boolean haveVMax = (abs(per.pressure.dp[nOri]) < Modelica.Constants.eps)
+  final parameter Boolean haveVMax = eff.haveVMax
     "Flag, true if user specified data that contain V_flow_max";
 
-  final parameter Modelica.Units.SI.VolumeFlowRate V_flow_max=if per.havePressureCurve
-       then (if haveVMax then per.pressure.V_flow[nOri] else per.pressure.V_flow[
-      nOri] - (per.pressure.V_flow[nOri] - per.pressure.V_flow[nOri - 1])/((per.pressure.dp[
-      nOri] - per.pressure.dp[nOri - 1]))*per.pressure.dp[nOri]) else
-      m_flow_nominal/rho_default "Maximum volume flow rate, used for smoothing";
-  final parameter Modelica.Units.SI.Density rho_default=Medium.density_pTX(
+  final parameter Modelica.Units.SI.VolumeFlowRate V_flow_max=eff.V_flow_max;
+  final parameter Modelica.Units.SI.Density rho_default=
+    Medium.density_pTX(
       p=Medium.p_default,
       T=Medium.T_default,
       X=Medium.X_default) "Default medium density";
@@ -175,7 +226,7 @@ protected
     final T_start=T_start,
     final X_start=X_start,
     final C_start=C_start,
-    final m_flow_nominal=m_flow_nominal,
+    final m_flow_nominal=_m_flow_nominal,
     final m_flow_small=m_flow_small,
     final p_start=p_start,
     final prescribedHeatFlowRate=true,
@@ -188,15 +239,9 @@ protected
     final f=fCut,
     final normalized=true,
     final initType=init) if use_inputFilter
-    "Second order filter to approximate dynamics of pump speed, and to improve numerics"
+    "Second order filter to approximate dynamics of the fan or pump's speed, and to improve numerics"
     annotation (Placement(transformation(extent={{20,61},{40,80}})));
 
-  Modelica.Blocks.Math.Gain gaiSpe(y(final unit="1"))
- if inputType == AixLib.Fluid.Types.InputType.Continuous and
-    speedIsInput
-    "Gain to normalized speed using speed_nominal or speed_rpm_nominal"
-    annotation (Placement(transformation(extent={{-4,74},{-16,86}})));
-
   AixLib.Fluid.Movers.BaseClasses.IdealSource preSou(
     redeclare final package Medium = Medium,
     final m_flow_small=m_flow_small,
@@ -216,7 +261,8 @@ protected
     annotation (Placement(transformation(extent={{50,-90},{70,-70}})));
 
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow prePow(
-    final alpha=0)
+    final alpha=0,
+    port(T(start=293.15)))
  if addPowerToMedium
     "Prescribed power (=heat and flow work) flow for dynamic model"
     annotation (Placement(transformation(extent={{-14,-104},{-34,-84}})));
@@ -233,27 +279,28 @@ protected
     redeclare final package Medium = Medium) "Mass flow rate sensor"
     annotation (Placement(transformation(extent={{-50,10},{-30,-10}})));
 
-  Sensors.RelativePressure senRelPre(
+  AixLib.Fluid.Sensors.RelativePressure senRelPre(
     redeclare final package Medium = Medium) "Head of mover"
     annotation (Placement(transformation(extent={{58,-27},{43,-14}})));
 
   // Because the speed data are not used by FlowMachineInterface, we set them
   // to zero.
-  FlowMachineInterface eff(
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff(
     per(
-      final hydraulicEfficiency = per.hydraulicEfficiency,
-      final motorEfficiency =     per.motorEfficiency,
-      final motorCooledByFluid =  per.motorCooledByFluid,
-      final speed_nominal =       0,
-      final constantSpeed =       0,
-      final speeds =              {0},
-      final power =               per.power),
+      final powerOrEfficiencyIsHydraulic = per.powerOrEfficiencyIsHydraulic,
+      final efficiency =           per.efficiency,
+      final motorEfficiency =      per.motorEfficiency,
+      final motorEfficiency_yMot = per.motorEfficiency_yMot,
+      final motorCooledByFluid =   per.motorCooledByFluid,
+      final speed_nominal =        0,
+      final constantSpeed =        0,
+      final speeds =               {0},
+      final power =                per.power,
+      final peak =                 per.peak),
     final nOri = nOri,
     final rho_default=rho_default,
     final computePowerUsingSimilarityLaws=computePowerUsingSimilarityLaws,
-    final haveVMax=haveVMax,
-    final V_flow_max=V_flow_max,
-    r_V(start=m_flow_nominal/rho_default),
+    r_V(start=_m_flow_nominal/rho_default),
     final preVar=preVar) "Flow machine"
     annotation (Placement(transformation(extent={{-32,-68},{-12,-48}})));
 
@@ -337,44 +384,72 @@ protected
             fillPattern=FillPattern.Solid)}));
   end Extractor;
 
-initial equation
-  // Check incorrect value of m_flow_nominal
-  assert(m_flow_nominal >= Modelica.Constants.small, "In "+ getInstanceName()+
-  ": The value of parameter m_flow_nominal should be greater or equal than " +
-  String(Modelica.Constants.small) + " but it equals " + String(m_flow_nominal));
-  // The control signal is dp or m_flow but the user did not provide a pump curve.
+initial algorithm
+  // The control signal is dp or m_flow but the user did not provide a fan or pump curve.
   // Hence, the speed is computed using default values, which likely are wrong.
   // Therefore, scaling the power using the speed is inaccurate.
   assert(nominalValuesDefineDefaultPressureCurve or
          per.havePressureCurve or
          (preVar == AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed),
-"*** Warning: You are using a flow or pressure controlled mover with the
-              default pressure curve.
-              This leads to approximate calculations of the electrical power
-              consumption. Add the correct pressure curve in the record per
-              to obtain an accurate computation.
-              Setting nominalValuesDefineDefaultPressureCurve=true will suppress this warning.",
+"*** Warning in " + getInstanceName() +
+": Mover is flow or pressure controlled and uses default pressure curve.
+This leads to an approximate power consumption.
+Set nominalValuesDefineDefaultPressureCurve=true to suppress this warning.",
          level=AssertionLevel.warning);
 
-  // The control signal is dp or m_flow but the user did not provide a pump curve.
+  // The control signal is dp or m_flow but the user did not provide a fan or pump curve.
   // Hence, the speed is computed using default values, which likely are wrong.
   // In addition, the user wants to use (V_flow, P) to compute the power.
   // This can lead to using a power that is less than the flow work. We avoid
-  // this by ignoring the setting of per.use_powerCharacteristics.
+  // this by ignoring the setting of per.etaHydMet.
   // The comment is split into two parts since otherwise the JModelica C-compiler
   // throws warnings.
   assert(nominalValuesDefineDefaultPressureCurve or
          (per.havePressureCurve or
            (preVar == AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed)) or
-         per.use_powerCharacteristic == false,
-"*** Warning: You are using a flow or pressure controlled mover with the
-              default pressure curve and you set use_powerCharacteristic = true.
-              Since this can cause wrong power consumption, the model will overwrite
-              this setting and use instead use_powerCharacteristic = false."+
-             "Since this causes the efficiency curve to be used,
-              make sure that the efficiency curves in the performance record per
-              are correct or add the pressure curve of the mover.
-              Setting nominalValuesDefineDefaultPressureCurve=true will suppress this warning.",
+         per.etaHydMet<>
+      AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+"*** Warning in " + getInstanceName() +
+": Mover is flow or pressure controlled, uses default pressure curve and
+has per.etaHydMet=.Power_VolumeFlowRate.
+As this can cause wrong power consumption, the model overrides this setting by using per.etaHydMet=.NotProvided.
+Set nominalValuesDefineDefaultPressureCurve=true to suppress this warning.",
+         level=AssertionLevel.warning);
+
+  assert(per.havePressureCurve or
+          not (per.etaHydMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate
+            or per.etaHydMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber),
+"*** Warning in " + getInstanceName() +
+": Mover has per.etaHydMet=.Power_VolumeFlowRate or per.etaHydMet=.EulerNumber.
+This requires per.pressure to be provided.
+Because it is not, the model overrides this setting by using per.etaHydMet=.NotProvided.
+Also consider using models under Movers.Preconfigured which autopopulate a pressure curve.",
+         level=AssertionLevel.warning);
+
+  assert(per.havePressureCurve or per.haveWMot_nominal or
+          not (per.etaMotMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio
+            or per.etaMotMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve),
+"*** Warning in " + getInstanceName() +
+": Mover has per.etaMotMet=.Efficiency_MotorPartLoadRatio or per.etaMotMet=.GenericCurve.
+This requires per.WMot_nominal or per.pressure to be provided. Because neither is provided,
+the model overrides this setting and by using per.etaMotMet=.NotProvided.
+Also consider using models under Movers.Preconfigured which autopopulate a pressure curve.",
+         level=AssertionLevel.warning);
+
+  assert(per.powerOrEfficiencyIsHydraulic or
+          not (per.etaMotMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio
+            or per.etaMotMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve),
+"*** Warning in " + getInstanceName() +
+": Mover has per.etaMotMet=.Efficiency_MotorPartLoadRatio or per.etaMotMet=.GenericCurve
+and provides information for total electric power instead of hydraulic power.
+This forms an algebraic loop. If simulation fails to converge,
+see the \"Motor efficiency\" section in the users guide for how to correct it.",
          level=AssertionLevel.warning);
 
 equation
@@ -418,24 +493,18 @@ equation
   connect(senRelPre.port_a, preSou.port_b) annotation (Line(points={{58,-20.5},{
           80,-20.5},{80,0},{60,0}},
                                color={0,127,255}));
-  connect(heaDis.etaHyd,eff. etaHyd) annotation (Line(points={{18,-60},{10,-60},
-          {10,-65},{-11,-65}},                     color={0,0,127}));
-  connect(heaDis.V_flow,eff. V_flow) annotation (Line(points={{18,-66},{14,-66},
-          {14,-53.2},{-6,-53.2},{-11,-53.2}},
-                                     color={0,0,127}));
-  connect(eff.PEle, heaDis.PEle) annotation (Line(points={{-11,-59},{0,-59},{0,-80},
-          {18,-80}},      color={0,0,127}));
-  connect(eff.WFlo, heaDis.WFlo) annotation (Line(points={{-11,-56},{-8,-56},{-8,
-          -74},{18,-74}}, color={0,0,127}));
+  connect(heaDis.V_flow,eff. V_flow) annotation (Line(points={{18,-60},{14,-60},
+          {14,-52},{-11,-52}},       color={0,0,127}));
+  connect(eff.PEle, heaDis.PEle) annotation (Line(points={{-11,-60},{0,-60},{0,
+          -80},{18,-80}}, color={0,0,127}));
+  connect(eff.WFlo, heaDis.WFlo) annotation (Line(points={{-11,-56},{4,-56},{4,
+          -66},{18,-66}}, color={0,0,127}));
   connect(rho_inlet.y,eff. rho) annotation (Line(points={{-69,-64},{-69,-64},{-34,
           -64}},                          color={0,0,127}));
   connect(eff.m_flow, senMasFlo.m_flow) annotation (Line(points={{-34,-54},{-34,
           -54},{-40,-54},{-40,-11}},               color={0,0,127}));
-  connect(eff.PEle, P) annotation (Line(points={{-11,-59},{0,-59},{0,-50},{90,
-          -50},{90,90},{110,90}},
-                             color={0,0,127}));
-  connect(eff.WFlo, PToMed.u2) annotation (Line(points={{-11,-56},{-8,-56},{-8,-86},
-          {48,-86}},      color={0,0,127}));
+  connect(eff.WFlo, PToMed.u2) annotation (Line(points={{-11,-56},{4,-56},{4,
+          -86},{48,-86}}, color={0,0,127}));
   connect(inputSwitch.y, filter.u) annotation (Line(points={{1,50},{12,50},{12,70.5},
           {18,70.5}},     color={0,0,127}));
 
@@ -445,11 +514,16 @@ equation
           70},{110,70}},
                      color={0,0,127}));
   connect(port_a, vol.ports[1])
-    annotation (Line(points={{-100,0},{-78,0},{-78,0}}, color={0,127,255}));
+    annotation (Line(points={{-100,0},{-79,0},{-79,0}}, color={0,127,255}));
   connect(vol.ports[2], senMasFlo.port_a)
-    annotation (Line(points={{-82,0},{-82,0},{-50,0}}, color={0,127,255}));
+    annotation (Line(points={{-81,0},{-81,0},{-50,0}}, color={0,127,255}));
   connect(senMasFlo.port_b, preSou.port_a)
     annotation (Line(points={{-30,0},{40,0},{40,0}}, color={0,127,255}));
+  connect(eff.WHyd, heaDis.WHyd) annotation (Line(points={{-11,-58},{2,-58},{2,
+          -74},{18,-74}}, color={0,0,127}));
+  connect(eff.PEle, P) annotation (Line(points={{-11,-60},{0,-60},{0,-50},{90,
+          -50},{90,90},{110,90}},
+                             color={0,0,127}));
    annotation(Icon(coordinateSystem(preserveAspectRatio=false,
     extent={{-100,-100},{100,100}}),
     graphics={
@@ -517,142 +591,217 @@ equation
           textString="M",
           textStyle={TextStyle.Bold})}),
     Documentation(info="<html>
- <p>
- This is the base model for fans and pumps.
- It provides an interface
- between the equations that compute head and power consumption,
- and the implementation of the energy and pressure balance
- of the fluid.
- </p>
- <p>
- Optionally, the fluid volume
- is computed using a dynamic balance or a steady-state balance.
- </p>
- <p>
- The parameter <code>addPowerToMedium</code> determines whether
- any power is added to the fluid. The default is <code>addPowerToMedium=true</code>,
- and hence the outlet enthalpy is higher than the inlet enthalpy if the
- flow device is operating.
- The setting <code>addPowerToMedium=false</code> is physically incorrect
- (since the flow work, the flow friction and the fan heat do not increase
- the enthalpy of the medium), but this setting does in some cases lead to simpler equations
- and more robust simulation, in particular if the mass flow is equal to zero.
- </p>
- </html>",
+<p>
+This is the base model for fans and pumps.
+It provides an interface
+between the equations that compute head and power consumption,
+and the implementation of the energy and pressure balance
+of the fluid.
+</p>
+<p>
+Optionally, the fluid volume
+is computed using a dynamic balance or a steady-state balance.
+</p>
+<p>
+The parameter <code>addPowerToMedium</code> determines whether
+any power is added to the fluid. The default is <code>addPowerToMedium=true</code>,
+and hence the outlet enthalpy is higher than the inlet enthalpy if the
+flow device is operating.
+The setting <code>addPowerToMedium=false</code> is physically incorrect
+(since the flow work, the flow friction and the fan heat do not increase
+the enthalpy of the medium), but this setting does in some cases lead to simpler equations
+and more robust simulation, in particular if the mass flow is equal to zero.
+</p>
+<p>
+In the previous implementation, this model extends from
+<a href=\"Modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>.
+Now it copies much of the code instead.
+This is to resolve a potential circular parameter binding that occurs when
+<a href=\"Modelica://AixLib.Fluid.Movers.Preconfigured.SpeedControlled_y\">
+AixLib.Fluid.Movers.Preconfigured.SpeedControlled_y</a>
+extends from
+<a href=\"Modelica://AixLib.Fluid.Movers.SpeedControlled_y\">
+AixLib.Fluid.Movers.SpeedControlled_y</a>.
+The former uses the nominal flow rate provided by user to construct
+the pressure curve, whilst the latter uses the user-provided pressure curve
+to determine the nominal flow rate. The new implementation removes the
+original declaration of nominal flow rate from
+<a href=\"Modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>
+and hides it (<code>protected _m_flow_nominal</code>) from the user.
+This way, A higher-level model (e.g.
+<a href=\"Modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
+AixLib.Fluid.Movers.FlowControlled_dp</a>),
+can still provide a default but not the other way around.
+See discussions in
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1705\">#1705</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 17, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- October 25, 2019, by Jianjun Hu:<br/>
- Improved icon graphics annotation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
- </li>
- <li>
- January 22, 2019, by Filip Jorissen:<br/>
- Split long assert output string into two strings to avoid compiler warnings
- in JModelica.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1081\">#1081</a>.
- </li>
- <li>
- January 8, 2019, by Filip Jorissen:<br/>
- Added assert for value of <code>m_flow_nominal</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/908\">#908</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredSpeed</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- December 2, 2016, by Michael Wetter:<br/>
- Removed <code>min</code> attribute as otherwise numerical noise can cause
- the assertion on the limit to fail.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Set start value for <code>VMachine_flow</code> to avoid a warning in
- <a href=\"modelica://AixLib.Fluid.Movers.Examples.MoverContinuous\">
- AixLib.Fluid.Movers.Examples.MoverContinuous</a>.
- </li>
- <li>
- July 29, 2016, by Michael Wetter:<br/>
- Made <code>Extractor</code> protected so that it can be removed later
- with a backwards compatible change.
- </li>
- <li>
- July 19, 2016, by Filip Jorissen:<br/>
- Created custom implementation for extractor.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/498\">#498</a>.
- </li>
- <li>
- June 16, 2016, by Filip Jorissen:<br/>
- Switched position of mixing volume and mass flow rate sensor.
- This is to have a consistent operating point tuple
- of <code>dp</code> and <code>m_flow</code> when having
- compressible flow.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/458\">#458</a>.
- </li>
- <li>
- February 19, 2016, by Michael Wetter and Filip Jorissen:<br/>
- Refactored model to make implementation clearer.
- This model now includes code for both speed and flow prescribed models,
- eliminating the need for an additional level of partial models.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- <li>
- Removed the parameter <code>dynamicBalance</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/411\">#411</a>.
- </li>
- <li>
- November 19, 2015, by Michael Wetter:<br/>
- Removed assignment of parameter
- <code>showDesignFlowDirection</code> in <code>extends</code> statement.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
- Removed assignment of <code>min</code> and <code>max</code> attributes
- of the port mass flow rate as this is already done in the base class.
- Removed <code>import</code> statement.
- </li>
- <li>
- April 2, 2015, by Filip Jorissen:<br/>
- Added code for supporting stage input and constant input.
- Added code for displaying constant set point in symbol.
- </li>
- <li>
- January 24, 2015, by Michael Wetter:<br/>
- Propagated <code>m_flow_small</code> of instance <code>vol</code> and made
- all its parameters final.
- </li>
- <li>
- May 25, 2011, by Michael Wetter:<br/>
- Revised implementation of energy balance to avoid having to use conditionally removed models.
- </li>
- <li>
- July 29, 2010, by Michael Wetter:<br/>
- Reduced fan time constant from 10 to 1 second.
- </li>
- <li>
- July 27, 2010, by Michael Wetter:<br/>
- Redesigned model to fix bug in medium balance.
- </li>
- <li>March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Removed the gain block that normalised the speed input
+because it is no longer needed. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+March 1, 2023, by Hongxiang Fu:<br/>
+Instead of extending
+<a href=\"Modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>,
+this model now has its code copied, then rewrote <code>m_flow_nominal</code>
+as <code>protected _m_flow_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1705\">#1705</a>.
+</li>
+<li>
+May 6, 2022, by Hongxiang Fu:<br/>
+<ul>
+<li>
+Moved <code>haveVMax</code> from here to
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>
+and <code>V_flow_max</code> from here to
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Generic\">
+AixLib.Fluid.Movers.Data.Generic</a>.
+</li>
+<li>
+Added <code>per.peak</code>, <code>per.totalEfficiency,</code>,
+<code>per.motorEfficiency_yMot</code>to be also passed down to <code>eff.per</code>
+at instantiation.
+</li>
+<li>
+Added an <code>assert()</code> warning when the model has to make an unreliable
+guess for efficiency computation using <code>.EulerNumber</code>.
+</li>
+<li>
+Added an <code>assert()</code> warning when the model has to override
+<code>per.etaMotMet</code>.
+</li>
+</ul>
+These are for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+June 17, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+October 25, 2019, by Jianjun Hu:<br/>
+Improved icon graphics annotation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1225\">#1225</a>.
+</li>
+<li>
+January 22, 2019, by Filip Jorissen:<br/>
+Split long assert output string into two strings to avoid compiler warnings
+in JModelica.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1081\">#1081</a>.
+</li>
+<li>
+January 8, 2019, by Filip Jorissen:<br/>
+Added assert for value of <code>m_flow_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/908\">#908</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredSpeed</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+December 2, 2016, by Michael Wetter:<br/>
+Removed <code>min</code> attribute as otherwise numerical noise can cause
+the assertion on the limit to fail.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Set start value for <code>VMachine_flow</code> to avoid a warning in
+<a href=\"modelica://AixLib.Fluid.Movers.Examples.MoverContinuous\">
+AixLib.Fluid.Movers.Examples.MoverContinuous</a>.
+</li>
+<li>
+July 29, 2016, by Michael Wetter:<br/>
+Made <code>Extractor</code> protected so that it can be removed later
+with a backwards compatible change.
+</li>
+<li>
+July 19, 2016, by Filip Jorissen:<br/>
+Created custom implementation for extractor.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/498\">#498</a>.
+</li>
+<li>
+June 16, 2016, by Filip Jorissen:<br/>
+Switched position of mixing volume and mass flow rate sensor.
+This is to have a consistent operating point tuple
+of <code>dp</code> and <code>m_flow</code> when having
+compressible flow.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/458\">#458</a>.
+</li>
+<li>
+February 19, 2016, by Michael Wetter and Filip Jorissen:<br/>
+Refactored model to make implementation clearer.
+This model now includes code for both speed and flow prescribed models,
+eliminating the need for an additional level of partial models.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
+</li>
+<li>
+Removed the parameter <code>dynamicBalance</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/411\">#411</a>.
+</li>
+<li>
+November 19, 2015, by Michael Wetter:<br/>
+Removed assignment of parameter
+<code>showDesignFlowDirection</code> in <code>extends</code> statement.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/349\">#349</a>.
+Removed assignment of <code>min</code> and <code>max</code> attributes
+of the port mass flow rate as this is already done in the base class.
+Removed <code>import</code> statement.
+</li>
+<li>
+April 2, 2015, by Filip Jorissen:<br/>
+Added code for supporting stage input and constant input.
+Added code for displaying constant set point in symbol.
+</li>
+<li>
+January 24, 2015, by Michael Wetter:<br/>
+Propagated <code>m_flow_small</code> of instance <code>vol</code> and made
+all its parameters final.
+</li>
+<li>
+May 25, 2011, by Michael Wetter:<br/>
+Revised implementation of energy balance to avoid having to use conditionally removed models.
+</li>
+<li>
+July 29, 2010, by Michael Wetter:<br/>
+Reduced fan time constant from 10 to 1 second.
+</li>
+<li>
+July 27, 2010, by Michael Wetter:<br/>
+Redesigned model to fix bug in medium balance.
+</li>
+<li>March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialFlowMachine;
diff --git a/AixLib/Fluid/Movers/BaseClasses/PowerInterface.mo b/AixLib/Fluid/Movers/BaseClasses/PowerInterface.mo
index 69ad4737ad..b68b97c24d 100644
--- a/AixLib/Fluid/Movers/BaseClasses/PowerInterface.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/PowerInterface.mo
@@ -12,23 +12,22 @@ model PowerInterface
   parameter Modelica.Units.SI.VolumeFlowRate delta_V_flow
     "Factor used for setting heat input into medium to zero at very small flows";
 
-  Modelica.Blocks.Interfaces.RealInput etaHyd(
-    final quantity="Efficiency",
-    final unit="1") "Hydraulic efficiency"
-    annotation (Placement(transformation(extent={{-140,80},{-100,120}}),
-        iconTransformation(extent={{-140,80},{-100,120}})));
-
   Modelica.Blocks.Interfaces.RealInput V_flow(
     final quantity="VolumeFlowRate",
     final unit="m3/s") "Volume flow rate"
-    annotation (Placement(transformation(extent={{-140,20},{-100,60}}),
-        iconTransformation(extent={{-140,20},{-100,60}})));
+    annotation (Placement(transformation(extent={{-140,80},{-100,120}}),
+        iconTransformation(extent={{-140,80},{-100,120}})));
 
   Modelica.Blocks.Interfaces.RealInput WFlo(
     final quantity="Power",
     final unit="W") "Flow work"
-    annotation (Placement(transformation(extent={{-140,-60},{-100,-20}}),
-        iconTransformation(extent={{-140,-60},{-100,-20}})));
+    annotation (Placement(transformation(extent={{-140,20},{-100,60}}),
+        iconTransformation(extent={{-140,20},{-100,60}})));
+
+  Modelica.Blocks.Interfaces.RealInput WHyd(final quantity="Power", final unit="W")
+    "Hydraulic work (converted to flow work and heat)" annotation (Placement(
+        transformation(extent={{-140,-60},{-100,-20}}), iconTransformation(
+          extent={{-140,-60},{-100,-20}})));
 
   Modelica.Blocks.Interfaces.RealInput PEle(
     final quantity="Power",
@@ -40,13 +39,13 @@ model PowerInterface
     final unit="W") "Heat input from fan or pump to medium"
     annotation (Placement(transformation(extent={{100,-10},{120,10}})));
 
-  Modelica.Units.SI.Power WHyd
-    "Hydraulic power input (converted to flow work and heat)";
-
 protected
   Modelica.Units.SI.HeatFlowRate QThe_flow
     "Heat input from fan or pump to medium";
 
+  Modelica.Units.SI.Efficiency etaHyd
+    "Hydraulic efficiency";
+
 initial equation
   assert(homotopyInitialization, "In " + getInstanceName() +
     ": The constant homotopyInitialization has been modified from its default value. This constant will be removed in future releases.",
@@ -54,7 +53,8 @@ initial equation
 
 equation
   // Hydraulic power (transmitted by shaft), etaHyd = WFlo/WHyd
-  etaHyd * WHyd   = WFlo;
+  etaHyd = WFlo / AixLib.Utilities.Math.Functions.smoothMax(
+                     x1=WHyd, x2=1E-5, deltaX=1E-6);
   // Heat input into medium
   QThe_flow +  WFlo = if motorCooledByFluid then PEle else WHyd;
   // At m_flow = 0, the solver may still obtain positive values for QThe_flow.
@@ -113,40 +113,49 @@ equation
           lineColor={0,0,0},
           fillColor={255,0,0})}),
     Documentation(info="<html>
- <p>Block that implements the functions to compute the
- heat dissipation of fans and pumps. It is used by the model
- <a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine\">
- AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine</a>.
- </p>
- </html>",
+<p>Block that implements the functions to compute the
+heat dissipation of fans and pumps. It is used by the model
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine\">
+AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine</a>.
+</p>
+</html>",
       revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- December 2, 2016, by Michael Wetter:<br/>
- Removed <code>min</code> attribute as otherwise numerical noise can cause
- the assertion on the limit to fail.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
- </li>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- February 19, 2016, by Michael Wetter:<br/>
- First implementation during refactoring of mover models to make implementation clearer.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 8, 2022, by Hongxiang Fu:<br/>
+This model no longer computes <code>WHyd</code>.
+It now takes <code>WHyd</code> instead of <code>etaHyd</code> as an input from
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+December 2, 2016, by Michael Wetter:<br/>
+Removed <code>min</code> attribute as otherwise numerical noise can cause
+the assertion on the limit to fail.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
+</li>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+February 19, 2016, by Michael Wetter:<br/>
+First implementation during refactoring of mover models to make implementation clearer.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerInterface;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Types.mo b/AixLib/Fluid/Movers/BaseClasses/Types.mo
index 17da7bfd40..2680464170 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Types.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Types.mo
@@ -7,11 +7,60 @@ package Types "Package with type definitions"
       FlowRate "Flow rate is prescribed",
       PressureDifference "Pressure difference is prescribed")
     "Enumeration to choose what variable is prescribed";
+  type HydraulicEfficiencyMethod = enumeration(
+      NotProvided
+        "Not provided, computed from other efficiency terms",
+      Efficiency_VolumeFlowRate "Array of efficiency vs. volumetric flow rate",
+      Power_VolumeFlowRate
+        "Array of power vs. volumetric flow rate",
+      EulerNumber
+        "One peak point to be used for the Euler number")
+    "Enumeration to choose the computation method for total efficiency and hydraulic efficiency"
+    annotation (Documentation(info="<html>
+<p>
+Enumeration to specify the calculation of the hydraulic efficiency.
+See <a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">AixLib.Fluid.Movers.UsersGuide</a>
+for instructions.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 15, 2021, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"));
+
+  type MotorEfficiencyMethod = enumeration(
+      NotProvided
+        "Not provided, computed from other efficiency terms",
+      Efficiency_VolumeFlowRate "Array of efficiency vs. volumetric flow rate",
+      Efficiency_MotorPartLoadRatio
+        "Rated input and array of efficiency vs. motor part load ratio yMot=WHyd/WMot_nominal",
+      GenericCurve
+        "Rated input and maximum efficiency to be used for generic curves")
+    "Enumeration to choose the computation method for motor efficiency"
+    annotation (Documentation(info="<html>
+<p>
+Enumeration to specify the calculation of the motor efficiency.
+See <a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">AixLib.Fluid.Movers.UsersGuide</a>
+for instructions.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 15, 2021, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"));
 
  annotation (preferredView="info", Documentation(info="<html>
- <p>
- This package contains type definitions for movers.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This package contains type definitions for movers.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Types;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/EulerComparison.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/EulerComparison.mo
new file mode 100644
index 0000000000..65c6bd85a7
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/EulerComparison.mo
@@ -0,0 +1,116 @@
+within AixLib.Fluid.Movers.BaseClasses.Validation;
+model EulerComparison
+  "Validates the Euler number method at nominal mover speed"
+  extends Modelica.Icons.Example;
+
+  parameter Integer nOri(min=1)=size(per1.power.V_flow,1)
+    "Number of data points for pressure curve"
+    annotation(Evaluate=true);
+  parameter Modelica.Units.SI.Density rhoCon=1.2
+    "Constant density";
+
+  parameter AixLib.Fluid.Movers.Data.Fans.Greenheck.BIDW13 per1
+    "Mover performance curves with flow rate, pressure rise, and power";
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff1(
+    per=per1,
+    rho_default=rhoCon,
+    nOri=nOri,
+    computePowerUsingSimilarityLaws=false)
+    "Flow machine interface using power characteristic"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  parameter AixLib.Fluid.Movers.Data.Generic per2(
+    final powerOrEfficiencyIsHydraulic=per1.powerOrEfficiencyIsHydraulic,
+    final etaHydMet=
+           AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber,
+    final etaMotMet=
+           AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided,
+    pressure=per1.pressure,
+    power=per1.power)
+    "Peak condition";
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff2(
+    per=per2,
+    rho_default=rhoCon,
+    nOri=nOri,
+    computePowerUsingSimilarityLaws=false)
+    "Flow machine interface using power Euler correlation"
+    annotation (Placement(transformation(extent={{-10,-44},{10,-24}})));
+
+  Modelica.Blocks.Sources.Constant y(k=1) "Control signal"
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+  Modelica.Blocks.Sources.Constant rho(k=rhoCon) "Density"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+
+  Modelica.Units.SI.VolumeFlowRate V_flow = m_flow.y/rhoCon "Volumetric flow rate";
+  Modelica.Units.SI.Power P1(displayUnit="W")=
+    if per1.powerOrEfficiencyIsHydraulic
+    then eff1.WHyd
+    else eff1.PEle
+    "Power from interpolation (total or hydraulic depending on data)";
+  Modelica.Units.SI.Power P2(displayUnit="W")=
+    if per1.powerOrEfficiencyIsHydraulic
+    then eff2.WHyd
+    else eff2.PEle
+    "Power from Euler number (total or hydraulic depending on data)";
+  Modelica.Units.SI.Efficiency eta1=
+    if per1.powerOrEfficiencyIsHydraulic
+    then eff1.etaHyd
+    else eff1.eta
+    "Efficiency from interpolation (total or hydraulic depending on data)";
+  Modelica.Units.SI.Efficiency eta2=
+    if per1.powerOrEfficiencyIsHydraulic
+    then eff2.etaHyd
+    else eff2.eta
+    "Efficiency from Euler number (total or hydraulic depending on data)";
+
+  Modelica.Blocks.Sources.Ramp m_flow(
+    height=eff1.V_flow_max*rhoCon,
+    duration=1)
+    "Mass flow rate"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+equation
+  connect(eff1.rho, rho.y)
+    annotation (Line(points={{-12,-6},{-26,-6},{-26,10},{-39,10}},
+                                               color={0,0,127}));
+  connect(y.y, eff1.y_in)
+    annotation (Line(points={{-39,50},{-4,50},{-4,12}},   color={0,0,127}));
+  connect(m_flow.y, eff1.m_flow) annotation (Line(points={{-39,-30},{-18,-30},{-18,
+          4},{-12,4}}, color={0,0,127}));
+  connect(y.y, eff2.y_in) annotation (Line(points={{-39,50},{-4,50},{-4,18},{18,
+          18},{18,-14},{-4,-14},{-4,-22}}, color={0,0,127}));
+  connect(rho.y, eff2.rho) annotation (Line(points={{-39,10},{-26,10},{-26,-40},
+          {-12,-40}},               color={0,0,127}));
+  connect(m_flow.y, eff2.m_flow) annotation (Line(points={{-39,-30},{-12,-30}},
+                           color={0,0,127}));
+  annotation (experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerComparison.mos"
+ "Simulate and plot"),
+Documentation(
+info="<html>
+<p>
+This model validates the power and efficiency computation using the Euler number
+and its correlation as implemented in
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+AixLib.Fluid.Movers.BaseClasses.Euler</a>.
+Its results of calculated efficiency and power are compared with those obtained
+using power curves.
+</p>
+<p>
+Note that the power curve is still provided because it is required by
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>.
+See <a href=\"modelica://AixLib.Fluid.Movers.Validation.ComparePowerHydraulic\">
+AixLib.Fluid.Movers.Validation.ComparePowerHydraulic</a>
+for a use case where the mover model is agnostic to the power curve and
+only the peak values are provided.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 21, 2021, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end EulerComparison;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/EulerCurve.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/EulerCurve.mo
new file mode 100644
index 0000000000..9d72d6db9f
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/EulerCurve.mo
@@ -0,0 +1,53 @@
+within AixLib.Fluid.Movers.BaseClasses.Validation;
+model EulerCurve "Displays the curve of the Euler number's correlation"
+  extends Modelica.Icons.Example;
+  Real x "log10(Eu/Eu_peak)";
+  Real etaApp "eta/eta_peak from polynomial approximation";
+  Real etaOri "eta/eta_peak from original correlation";
+
+function correlation
+  input Real x "log10(Eu/Eu_peak)";
+  output Real y "eta/eta_peak";
+  protected
+  constant Real a=-2.732094, b=2.273014, c=0.196344, d=5.267518;
+  Real Z1, Z2, Z3;
+algorithm
+  Z1:=(x-a)/b;
+  Z2:=((exp(c*x)*d*x)-a)/b;
+  Z3:=-a/b;
+  y:=(exp(-0.5*Z1^2)*(1+sign(Z2)*Modelica.Math.Special.erf(u=abs(Z2)/sqrt(2))))
+    /(exp(-0.5*Z3^2)*(1+Modelica.Math.Special.erf(u=Z3/sqrt(2))));
+end correlation;
+
+initial equation
+  x = -4;
+equation
+  der(x)=1;
+  etaApp = AixLib.Fluid.Movers.BaseClasses.Euler.correlation(x);
+  etaOri = correlation(x);
+
+  annotation (experiment(Tolerance=1e-6, StopTime=10.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerCurve.mos"
+ "Simulate and plot"),
+ Documentation(
+info="<html>
+<p>
+This validation model plots and compares out the original correlation function
+of Euler number and its polynomial approximation.
+</p>
+<p>
+See details of this function in the documentation of
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Euler.correlation\">
+AixLib.Fluid.Movers.BaseClasses.Euler.correlation</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 13, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end EulerCurve;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/EulerReducedSpeed.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/EulerReducedSpeed.mo
new file mode 100644
index 0000000000..8a83632a39
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/EulerReducedSpeed.mo
@@ -0,0 +1,158 @@
+within AixLib.Fluid.Movers.BaseClasses.Validation;
+model EulerReducedSpeed
+  "Validates the Euler number method at reduced mover speed"
+  extends Modelica.Icons.Example;
+
+  parameter Integer nOri(min=1)=size(per1.power.V_flow,1)
+    "Number of data points for pressure curve"
+    annotation(Evaluate=true);
+  parameter Modelica.Units.SI.Density rhoCon=1.2
+    "Constant density";
+
+  parameter AixLib.Fluid.Movers.Data.Fans.Greenheck.BIDW13 per1(
+    final etaHydMet=
+            AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber,
+    final etaMotMet=
+            AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided)
+    "Mover performance curves with flow rate, pressure rise, and power";
+  parameter AixLib.Fluid.Movers.Data.Generic per2(
+    power(V_flow={0.939939939939939,1.88588588588588,2.83183183183181,
+         3.77177177177175,4.46546546546544}, P={4332.517,5801.546,6651.644,
+         6800.784,6502.504}),
+    pressure(V_flow={0.939939939939939,1.88588588588588,2.83183183183181,
+            3.77177177177175,4.46546546546544}, dp={2081.78137651821,
+            2008.90688259109,1474.4939271255,704.453441295546,0}))
+    "Mover performance curves at reduced speed N=3400";
+  parameter AixLib.Fluid.Movers.Data.Generic per3(
+    power(V_flow={0.939939939939939,1.88588588588588,2.83183183183181,
+         3.28228228228228}, P={1998.476,2535.38,2714.348,2550.294}),
+    pressure(V_flow={0.939939939939939,1.88588588588588,2.83183183183181,
+            3.28228228228228}, dp={1127.12550607287,903.643724696356,
+            340.080971659919,0}))
+    "Mover performance curves at reduced speed N=2500";
+
+  Modelica.Units.SI.Power pow1=
+    AixLib.Utilities.Math.Functions.smoothInterpolation(
+      x=m1_flow.y/rhoCon,
+      xSup=per1.power.V_flow,
+      ySup=per1.power.P,
+      ensureMonotonicity=false) "Measured power";
+  Modelica.Units.SI.Power pow2=
+    AixLib.Utilities.Math.Functions.smoothInterpolation(
+      x=m2_flow.y/rhoCon,
+      xSup=per2.power.V_flow,
+      ySup=per2.power.P,
+      ensureMonotonicity=false) "Measured power";
+  Modelica.Units.SI.Power pow3=
+    AixLib.Utilities.Math.Functions.smoothInterpolation(
+      x=m3_flow.y/rhoCon,
+      xSup=per3.power.V_flow,
+      ySup=per3.power.P,
+      ensureMonotonicity=false) "Measured power";
+
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff1(
+    per=per1,
+    rho_default=rhoCon,
+    nOri=nOri,
+    computePowerUsingSimilarityLaws=false)
+    "Flow machine interface using power characteristic"
+    annotation (Placement(transformation(extent={{20,40},{40,60}})));
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff2(
+    per=per1,
+    rho_default=rhoCon,
+    nOri=nOri,
+    computePowerUsingSimilarityLaws=false)
+    "Flow machine interface using power Euler correlation"
+    annotation (Placement(transformation(extent={{20,-20},{40,0}})));
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff3(
+    per=per1,
+    rho_default=rhoCon,
+    nOri=nOri,
+    computePowerUsingSimilarityLaws=false)
+    "Flow machine interface using power Euler correlation"
+    annotation (Placement(transformation(extent={{20,-68},{40,-48}})));
+
+  Modelica.Blocks.Sources.Constant y1(k=1) "Control signal"
+    annotation (Placement(transformation(extent={{-60,70},{-40,90}})));
+  Modelica.Blocks.Sources.Constant rho(k=rhoCon) "Density"
+    annotation (Placement(transformation(extent={{-20,-80},{0,-60}})));
+  Modelica.Blocks.Sources.Constant y2(k=3400/4100)
+    "Reduced speed y = 3400/4100 = 0.829"
+    annotation (Placement(transformation(extent={{-60,10},{-40,30}})));
+  Modelica.Blocks.Sources.Constant y3(k=2500/4100)
+    "Reduced speed y = 2500/4100 = 0.610"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+
+  Modelica.Blocks.Sources.Ramp m1_flow(
+    height=0.98*max(per1.pressure.V_flow)*rhoCon,
+    duration=1,
+    offset=0.01*max(per1.pressure.V_flow)*rhoCon)
+    "Mass flow rate"
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+  Modelica.Blocks.Sources.Ramp m2_flow(
+    height=0.98*max(per2.pressure.V_flow)*rhoCon,
+    duration=1,
+    offset=0.01*max(per2.pressure.V_flow)*rhoCon) "Mass flow rate"
+    annotation (Placement(transformation(extent={{-60,-20},{-40,0}})));
+  Modelica.Blocks.Sources.Ramp m3_flow(
+    height=0.98*max(per3.pressure.V_flow)*rhoCon,
+    duration=1,
+    offset=0.01*max(per3.pressure.V_flow)*rhoCon) "Mass flow rate"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+
+equation
+  connect(eff1.rho, rho.y)
+    annotation (Line(points={{18,44},{10,44},{10,-70},{1,-70}},
+                                               color={0,0,127}));
+  connect(y1.y, eff1.y_in)
+    annotation (Line(points={{-39,80},{26,80},{26,62}}, color={0,0,127}));
+  connect(m1_flow.y, eff1.m_flow) annotation (Line(points={{-39,50},{-20,50},{-20,
+          54},{18,54}}, color={0,0,127}));
+  connect(rho.y, eff2.rho) annotation (Line(points={{1,-70},{10,-70},{10,-16},{
+          18,-16}},                 color={0,0,127}));
+  connect(y2.y, eff2.y_in)
+    annotation (Line(points={{-39,20},{26,20},{26,2}}, color={0,0,127}));
+  connect(m2_flow.y, eff2.m_flow) annotation (Line(points={{-39,-10},{-20,-10},{
+          -20,-6},{18,-6}}, color={0,0,127}));
+  connect(y3.y, eff3.y_in)
+    annotation (Line(points={{-39,-40},{26,-40},{26,-46}}, color={0,0,127}));
+  connect(m3_flow.y, eff3.m_flow) annotation (Line(points={{-39,-70},{-30,-70},
+          {-30,-54},{18,-54}},color={0,0,127}));
+  connect(rho.y, eff3.rho) annotation (Line(points={{1,-70},{10,-70},{10,-64},{
+          18,-64}},
+                 color={0,0,127}));
+  annotation (experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerReducedSpeed.mos"
+ "Simulate and plot"),
+Documentation(
+info="<html>
+<p>
+Similar to
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Validation.EulerComparison\">
+AixLib.Fluid.Movers.BaseClasses.Validation.EulerComparison</a>,
+this model compares the power computed from the Euler number method with measured
+values. The power data at speeds N=4100, 3400, and 2500 RPM from the power map of
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Fans.Greenheck.BIDW13\">
+AixLib.Fluid.Movers.Data.Fans.Greenheck.BIDW13</a>
+(shown below) was used.
+Note that the pressure curves in the figure do not seem to be independently
+measured but rather simply scaled from the nominal curve.
+However, because the Euler number method also does not account for the efficiency
+degradation along any curve <i>&Delta;p=kV&#775;<sup>2</sup></i>,
+using the Euler number method has equivalent accuracy to using such power maps.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/BaseClasses/Validation/BIDW13.png\"
+width=\"1000\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 18, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end EulerReducedSpeed;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/FlowMachineInterface.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/FlowMachineInterface.mo
index e72ac68264..e9d093a595 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Validation/FlowMachineInterface.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/FlowMachineInterface.mo
@@ -4,8 +4,6 @@ model FlowMachineInterface "Simple model to validate FlowMachineInterface"
   AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff(
     per(pressure(V_flow={0,1}, dp={1000,0})),
     rho_default=1.2,
-    haveVMax=true,
-    V_flow_max=1,
     nOri=2,
     preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
     computePowerUsingSimilarityLaws=true) "Flow machine interface model"
@@ -13,33 +11,41 @@ model FlowMachineInterface "Simple model to validate FlowMachineInterface"
   Modelica.Blocks.Sources.Constant y(k=1) "Control signal"
     annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
   Modelica.Blocks.Sources.Constant rho(k=1.2) "Density"
-    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
-  Modelica.Blocks.Sources.Ramp m_flow(height=1.2, duration=1) "Mass flow rate"
     annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+  Modelica.Blocks.Sources.Ramp m_flow(height=1.2, duration=1) "Mass flow rate"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
 equation
   connect(eff.rho, rho.y)
-    annotation (Line(points={{-12,-6},{-26,-6},{-26,0},{-39,0}},
+    annotation (Line(points={{-12,-6},{-20,-6},{-20,-30},{-39,-30}},
                                                color={0,0,127}));
-  connect(m_flow.y, eff.m_flow) annotation (Line(points={{-39,-30},{-26,-30},{
-          -26,4},{-12,4}},
-                         color={0,0,127}));
+  connect(m_flow.y, eff.m_flow) annotation (Line(points={{-39,0},{-20,0},{-20,4},
+          {-12,4}},      color={0,0,127}));
   connect(y.y, eff.y_in)
     annotation (Line(points={{-39,30},{-4,30},{-4,12}},   color={0,0,127}));
   annotation (
     Documentation(info="<html>
- <p>
- Simple validation model for the flow machine interface model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 19, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Simple validation model for the flow machine interface model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 1, 2021, by Hongxiang Fu:<br/>
+Removed assignments for <code>eff.haveVMax</code> 
+and <code>eff.V_flow_max</code> as they are now assigned inside 
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>.<br/>
+This is for 
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 19, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/FlowMachineInterface.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowMachineInterface;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/HydraulicEfficiencyMethods.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/HydraulicEfficiencyMethods.mo
new file mode 100644
index 0000000000..e0a28fba17
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/HydraulicEfficiencyMethods.mo
@@ -0,0 +1,128 @@
+within AixLib.Fluid.Movers.BaseClasses.Validation;
+model HydraulicEfficiencyMethods
+  "Validation model for different hydraulic efficiency options"
+  extends Modelica.Icons.Example;
+
+  AixLib.Fluid.Movers.Data.Generic per(
+    powerOrEfficiencyIsHydraulic=true,
+    final pressure(V_flow={0,1}, dp={1000,0}),
+    final etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided)
+    "Performance record";
+  parameter Modelica.Units.SI.Density rhoFlu=1.2 "Fluid density";
+
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff1(
+    per(
+      powerOrEfficiencyIsHydraulic=per.powerOrEfficiencyIsHydraulic,
+      pressure=per.pressure,
+      etaMotMet=per.etaMotMet,
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.NotProvided),
+    rho_default=rhoFlu,
+    nOri=2,
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
+    computePowerUsingSimilarityLaws=true)
+    "FlowMachineInterface with per.etaHydMet=.NotProvided"
+    annotation (Placement(transformation(extent={{40,40},{60,60}})));
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff2(
+    per(
+      powerOrEfficiencyIsHydraulic=per.powerOrEfficiencyIsHydraulic,
+      pressure=per.pressure,
+      etaMotMet=per.etaMotMet,
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate,
+      efficiency(V_flow={0,0.3,0.6,0.8,1}, eta={0,0.5,0.7,0.5,0})),
+    rho_default=rhoFlu,
+    nOri=2,
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
+    computePowerUsingSimilarityLaws=true)
+    "FlowMachineInterface with per.etaHydMet=.Efficiency_VolumeFlowRate"
+    annotation (Placement(transformation(extent={{40,0},{60,20}})));
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff3(
+    per(
+      powerOrEfficiencyIsHydraulic=per.powerOrEfficiencyIsHydraulic,
+      pressure=per.pressure,
+      etaMotMet=per.etaMotMet,
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+      power(V_flow={0,0.25,0.5,0.75,1}, P={480,540,510,550,710})),
+    rho_default=rhoFlu,
+    nOri=2,
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
+    computePowerUsingSimilarityLaws=true)
+    "FlowMachineInterface with per.etaHydMet=.Power_VolumeFlowRate"
+    annotation (Placement(transformation(extent={{40,-40},{60,-20}})));
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff4(
+    per(
+      powerOrEfficiencyIsHydraulic=per.powerOrEfficiencyIsHydraulic,
+      pressure=per.pressure,
+      etaMotMet=per.etaMotMet,
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber,
+      peak(
+        V_flow=0.5,
+        dp=500,
+        eta=0.7)),
+    rho_default=rhoFlu,
+    nOri=2,
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
+    computePowerUsingSimilarityLaws=true)
+    "FlowMachineInterface with per.etaHydMet=.EulerNumber"
+    annotation (Placement(transformation(extent={{40,-80},{60,-60}})));
+
+  Modelica.Blocks.Sources.Constant y(k=1) "Relative speed"
+    annotation (Placement(transformation(extent={{-60,70},{-40,90}})));
+  Modelica.Blocks.Sources.Ramp m_flow(height=rho.k, duration=1) "Mass flow rate"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Modelica.Blocks.Sources.Constant rho(k=rhoFlu) "Density"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+
+equation
+  connect(eff3.rho, rho.y) annotation (Line(points={{38,-36},{-20,-36},{-20,-30},
+          {-39,-30}},
+                 color={0,0,127}));
+  connect(rho.y,eff4. rho) annotation (Line(points={{-39,-30},{-20,-30},{-20,-76},
+          {38,-76}}, color={0,0,127}));
+  connect(m_flow.y,eff3. m_flow) annotation (Line(points={{-39,30},{0,30},{0,-26},
+          {38,-26}},color={0,0,127}));
+  connect(m_flow.y,eff4. m_flow) annotation (Line(points={{-39,30},{0,30},{0,-66},
+          {38,-66}}, color={0,0,127}));
+  connect(m_flow.y, eff1.m_flow) annotation (Line(points={{-39,30},{0,30},{0,54},
+          {38,54}}, color={0,0,127}));
+  connect(m_flow.y, eff2.m_flow) annotation (Line(points={{-39,30},{0,30},{0,14},
+          {38,14}}, color={0,0,127}));
+  connect(rho.y, eff2.rho) annotation (Line(points={{-39,-30},{-20,-30},{-20,4},
+          {38,4}}, color={0,0,127}));
+  connect(rho.y, eff1.rho) annotation (Line(points={{-39,-30},{-20,-30},{-20,44},
+          {38,44}}, color={0,0,127}));
+  connect(y.y, eff1.y_in) annotation (Line(points={{-39,80},{68,80},{68,70},{46,
+          70},{46,62}}, color={0,0,127}));
+  connect(y.y, eff2.y_in) annotation (Line(points={{-39,80},{68,80},{68,30},{46,
+          30},{46,22}}, color={0,0,127}));
+  connect(y.y, eff3.y_in) annotation (Line(points={{-39,80},{68,80},{68,-10},{
+          46,-10},{46,-18}},
+                          color={0,0,127}));
+  connect(y.y, eff4.y_in) annotation (Line(points={{-39,80},{68,80},{68,-50},{
+          46,-50},{46,-58}},
+                          color={0,0,127}));
+  annotation (
+    Documentation(info="<html>
+<p>
+This is a simple validation model for
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>
+where its hydraulic efficiency <i>&eta;<sub>hyd</sub></i> is specified with
+different methods defined in
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod\">
+AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Aug 5, 2022, by Hongxiang Fu:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/HydraulicEfficiencyMethods.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end HydraulicEfficiencyMethods;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/MotorEfficiencyMethods.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/MotorEfficiencyMethods.mo
new file mode 100644
index 0000000000..b3156974be
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/MotorEfficiencyMethods.mo
@@ -0,0 +1,128 @@
+within AixLib.Fluid.Movers.BaseClasses.Validation;
+model MotorEfficiencyMethods
+  "Validation model for different motor efficiency options"
+  extends Modelica.Icons.Example;
+
+  AixLib.Fluid.Movers.Data.Generic per(
+    final pressure(V_flow={0,1}, dp={1000,0}),
+    final etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.NotProvided)
+    "Performance record";
+  parameter Modelica.Units.SI.Density rhoFlu=1.2 "Fluid density";
+
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff1(
+    per(
+      pressure=per.pressure,
+      etaHydMet=per.etaHydMet,
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided),
+    rho_default=rhoFlu,
+    nOri=2,
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
+    computePowerUsingSimilarityLaws=true)
+    "FlowMachineInterface with per.etaMotMet=.NotProvided"
+    annotation (Placement(transformation(extent={{40,40},{60,60}})));
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff2(
+    per(
+      pressure=per.pressure,
+      etaHydMet=per.etaHydMet,
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_VolumeFlowRate,
+      motorEfficiency(V_flow={0,0.3,0.6,1}, eta={0,0.4,0.6,0.7})),
+    rho_default=rhoFlu,
+    nOri=2,
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
+    computePowerUsingSimilarityLaws=true)
+    "FlowMachineInterface with per.etaMotMet=.Efficiency_VolumeFlowRate"
+    annotation (Placement(transformation(extent={{40,0},{60,20}})));
+
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff3(
+    per(
+      pressure=per.pressure,
+      etaHydMet=per.etaHydMet,
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio,
+      motorEfficiency_yMot(y={0,0.25,0.5,1}, eta={0,0.56,0.7,0.7}),
+      WMot_nominal=500),
+    rho_default=rhoFlu,
+    nOri=2,
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
+    computePowerUsingSimilarityLaws=true)
+    "FlowMachineInterface with per.etaMotMet=.Efficiency_MotorPartLoadRatio"
+    annotation (Placement(transformation(extent={{40,-40},{60,-20}})));
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff4(
+    per(
+      pressure=per.pressure,
+      etaHydMet=per.etaHydMet,
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve,
+      etaMot_max=0.7,
+      WMot_nominal=500),
+    rho_default=rhoFlu,
+    nOri=2,
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
+    computePowerUsingSimilarityLaws=true)
+    "FlowMachineInterface with per.etaMotMet=.GenericCurve"
+    annotation (Placement(transformation(extent={{40,-80},{60,-60}})));
+
+  Modelica.Blocks.Sources.Constant y(k=1) "Relative speed"
+    annotation (Placement(transformation(extent={{-60,70},{-40,90}})));
+  Modelica.Blocks.Sources.Ramp m_flow(height=1*rhoFlu, duration=1) "Mass flow rate"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Modelica.Blocks.Sources.Constant rho(k=rhoFlu) "Density"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+
+equation
+  connect(eff3.rho, rho.y) annotation (Line(points={{38,-36},{-20,-36},{-20,-30},
+          {-39,-30}},
+                 color={0,0,127}));
+  connect(rho.y,eff4. rho) annotation (Line(points={{-39,-30},{-20,-30},{-20,-76},
+          {38,-76}}, color={0,0,127}));
+  connect(m_flow.y,eff3. m_flow) annotation (Line(points={{-39,30},{0,30},{0,-26},
+          {38,-26}},color={0,0,127}));
+  connect(m_flow.y,eff4. m_flow) annotation (Line(points={{-39,30},{0,30},{0,-66},
+          {38,-66}}, color={0,0,127}));
+  connect(m_flow.y, eff1.m_flow) annotation (Line(points={{-39,30},{0,30},{0,54},
+          {38,54}}, color={0,0,127}));
+  connect(m_flow.y, eff2.m_flow) annotation (Line(points={{-39,30},{0,30},{0,14},
+          {38,14}}, color={0,0,127}));
+  connect(rho.y, eff2.rho) annotation (Line(points={{-39,-30},{-20,-30},{-20,4},
+          {38,4}}, color={0,0,127}));
+  connect(rho.y, eff1.rho) annotation (Line(points={{-39,-30},{-20,-30},{-20,44},
+          {38,44}}, color={0,0,127}));
+  connect(y.y, eff1.y_in) annotation (Line(points={{-39,80},{68,80},{68,70},{46,
+          70},{46,62}}, color={0,0,127}));
+  connect(y.y, eff2.y_in) annotation (Line(points={{-39,80},{68,80},{68,30},{46,
+          30},{46,22}}, color={0,0,127}));
+  connect(y.y, eff3.y_in) annotation (Line(points={{-39,80},{68,80},{68,-10},{
+          46,-10},{46,-18}},
+                          color={0,0,127}));
+  connect(y.y, eff4.y_in) annotation (Line(points={{-39,80},{68,80},{68,-50},{
+          46,-50},{46,-58}},
+                          color={0,0,127}));
+  annotation (
+    Documentation(info="<html>
+<p>
+This is a simple validation model for
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>
+where its motor efficiency <i>&eta;<sub>mot</sub></i> is specified with
+different methods defined in
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod\">
+AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod</a>.
+The instance <code>eff4</code> specifies <i>&eta;<sub>mot</sub></i> as
+a function of motor PLR by finding a generic curve with the maximum motor
+efficiency and rated motor input power. The generic curve is generated by
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Apr 6, 2022, by Hongxiang Fu:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/MotorEfficiencyMethods.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end MotorEfficiencyMethods;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/NegativePressureOrFlow.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/NegativePressureOrFlow.mo
new file mode 100644
index 0000000000..dd28c20ee4
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/NegativePressureOrFlow.mo
@@ -0,0 +1,90 @@
+within AixLib.Fluid.Movers.BaseClasses.Validation;
+model NegativePressureOrFlow
+  "A validation model that tests the mover behaviour when the pressure rise or flow is negative"
+  extends Modelica.Icons.Example;
+
+  package Medium = AixLib.Media.Air;
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=0.1
+    "Nominal mass flow rate";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal=10000
+    "Nominal pressure difference";
+  parameter Modelica.Units.SI.Density rho_default=1.2
+    "Fluid density at medium default state";
+
+  AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface eff(
+    per(pressure(V_flow=m_flow_nominal/rho_default*{0,2},
+                 dp=dp_nominal*{2,0}),
+        etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.NotProvided,
+        etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided),
+    preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.PressureDifference,
+    computePowerUsingSimilarityLaws=true,
+    rho_default=rho_default,
+    nOri=2)
+    "FlowMachineInterface model with prescribed pressure"
+    annotation (Placement(transformation(extent={{-20,-20},{0,0}})));
+  Modelica.Blocks.Sources.Constant rho(k=rho_default) "Density"
+    annotation (Placement(transformation(extent={{-80,-60},{-60,-40}})));
+  Modelica.Blocks.Sources.Ramp m_flow(
+    height=2*m_flow_nominal,
+    duration=3600,
+    offset=-0.5*m_flow_nominal) "Mass flow rate"
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+  Modelica.Blocks.Sources.Ramp dp(
+    height=-2*dp_nominal,
+    duration=3600,
+    offset=1.5*dp_nominal) "Pressure rise"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+equation
+
+  connect(eff.m_flow, m_flow.y) annotation (Line(points={{-22,-6},{-52,-6},{-52,
+          -10},{-59,-10}}, color={0,0,127}));
+  connect(rho.y, eff.rho) annotation (Line(points={{-59,-50},{-28,-50},{-28,-16},
+          {-22,-16}}, color={0,0,127}));
+  connect(dp.y, eff.dp_in)
+    annotation (Line(points={{-59,30},{-6,30},{-6,2}}, color={0,0,127}));
+annotation(__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/NegativePressureOrFlow.mos"
+        "Simulate and plot"),
+   experiment(
+      StopTime=3600,
+      Tolerance=1e-06),
+   Documentation(info="<html>
+<p>
+Without the constraint that
+<i>W<sub>flo</sub> = V&#775; &Delta;p &ge; 0</i>,
+this validation model would produce negative computed mover power
+when the pressure rise or the flow rate is forced to be negative,
+as shown below.
+</p>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/BaseClasses/Validation/NegativePressureOrFlow.png\"/>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 5, 2022, by Hongxiang Fu:<br/>
+<ul>
+<li>
+Remade this model with
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>
+instead of using a full mover model so that forcing a flow rate and a pressure rise
+is more straightforward.
+</li>
+<li>
+Changed parameterisation so that the result curve is clearer.
+</li>
+</ul>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+June 6, 2022, by Hongxiang Fu:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1621\">IBPSA, #1621</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end NegativePressureOrFlow;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/PowerInterface.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/PowerInterface.mo
index 19077d4935..53ec350f47 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Validation/PowerInterface.mo
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/PowerInterface.mo
@@ -6,13 +6,13 @@ model PowerInterface "Simple model to validate PowerInterface"
     delta_V_flow=0.05) "Power interface model"
     annotation (Placement(transformation(extent={{-10,10},{10,30}})));
   Modelica.Blocks.Sources.Constant WFlo(k=1*1000) "Flow work"
-    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
   Modelica.Blocks.Sources.Ramp V_flow(
     duration=1,
     height=1) "Volume flow rate"
-    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
-  Modelica.Blocks.Sources.Constant etaHyd(k=0.8) "Efficiency"
     annotation (Placement(transformation(extent={{-60,60},{-40,80}})));
+  Modelica.Blocks.Sources.Constant WHyd(k=1250) "Hydraulic work"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
   Modelica.Blocks.Sources.Constant PEle(k=1*1000*4) "Electrical work"
     annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
   AixLib.Fluid.Movers.BaseClasses.PowerInterface powNonCoo(
@@ -20,37 +20,45 @@ model PowerInterface "Simple model to validate PowerInterface"
     delta_V_flow=0.05) "Power interface model"
     annotation (Placement(transformation(extent={{-10,-30},{10,-10}})));
 equation
-  connect(powCoo.etaHyd, etaHyd.y) annotation (Line(points={{-12,30},{-26,30},{-26,
-          70},{-39,70}}, color={0,0,127}));
-  connect(V_flow.y, powCoo.V_flow) annotation (Line(points={{-39,30},{-30,30},{-30,
-          24},{-12,24}}, color={0,0,127}));
-  connect(powCoo.WFlo, WFlo.y) annotation (Line(points={{-12,16},{-26,16},{-26,-30},
-          {-39,-30}}, color={0,0,127}));
+  connect(V_flow.y, powCoo.V_flow) annotation (Line(points={{-39,70},{-30,70},{
+          -30,36},{-12,36},{-12,30}},
+                         color={0,0,127}));
+  connect(powCoo.WFlo, WFlo.y) annotation (Line(points={{-12,24},{-34,24},{-34,
+          30},{-39,30}},
+                      color={0,0,127}));
   connect(PEle.y, powCoo.PEle) annotation (Line(points={{-39,-70},{-20,-70},{-20,
           10},{-12,10}}, color={0,0,127}));
-  connect(powNonCoo.etaHyd, etaHyd.y) annotation (Line(points={{-12,-10},{-26,-10},
-          {-26,70},{-39,70}}, color={0,0,127}));
-  connect(V_flow.y, powNonCoo.V_flow) annotation (Line(points={{-39,30},{-30,30},
-          {-30,-16},{-12,-16}}, color={0,0,127}));
-  connect(powNonCoo.WFlo, WFlo.y) annotation (Line(points={{-12,-24},{-26,-24},{
-          -26,-30},{-39,-30}}, color={0,0,127}));
+  connect(V_flow.y, powNonCoo.V_flow) annotation (Line(points={{-39,70},{-30,70},
+          {-30,-10},{-12,-10}}, color={0,0,127}));
+  connect(powNonCoo.WFlo, WFlo.y) annotation (Line(points={{-12,-16},{-34,-16},
+          {-34,30},{-39,30}},  color={0,0,127}));
   connect(PEle.y, powNonCoo.PEle) annotation (Line(points={{-39,-70},{-20,-70},{
           -20,-30},{-12,-30}}, color={0,0,127}));
+  connect(WHyd.y, powCoo.WHyd) annotation (Line(points={{-39,-30},{-24,-30},{
+          -24,16},{-12,16}}, color={0,0,127}));
+  connect(WHyd.y, powNonCoo.WHyd) annotation (Line(points={{-39,-30},{-24,-30},
+          {-24,-24},{-12,-24}}, color={0,0,127}));
   annotation (
     Documentation(info="<html>
- <p>
- Simple validation model for the power interface model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 19, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Simple validation model for the power interface model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 8, 2022, by Hongxiang Fu:<br/>
+Changed the source for <code>etaHyd</code> to <code>WHyd</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 19, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-6, StopTime=1),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/PowerInterface.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerInterface;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/TotalEfficiencyMethods.mo b/AixLib/Fluid/Movers/BaseClasses/Validation/TotalEfficiencyMethods.mo
new file mode 100644
index 0000000000..9ecb3ce609
--- /dev/null
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/TotalEfficiencyMethods.mo
@@ -0,0 +1,33 @@
+within AixLib.Fluid.Movers.BaseClasses.Validation;
+model TotalEfficiencyMethods
+  "Validation model for total efficiency specified via hydraulic efficiency options"
+  extends HydraulicEfficiencyMethods(
+    per(powerOrEfficiencyIsHydraulic=false),
+    eff2(per(efficiency(eta={0,0.35,0.49,0.35,0}))),
+    eff3(per(power(P={680,771,730,780,1010}))),
+    eff4(per(peak(eta=0.49))));
+
+annotation (
+    Documentation(info="<html>
+<p>
+This model is the same as
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Validation.HydraulicEfficiencyMethods\">
+AixLib.Fluid.Movers.BaseClasses.Validation.HydraulicEfficiencyMethods</a>
+except that the enumeration is used for total efficiency <i>&eta;</i>
+via the parameter <code>per.powerOrEfficiencyIsHydraulic</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Aug 5, 2022, by Hongxiang Fu:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),
+experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/TotalEfficiencyMethods.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end TotalEfficiencyMethods;
diff --git a/AixLib/Fluid/Movers/BaseClasses/Validation/package.order b/AixLib/Fluid/Movers/BaseClasses/Validation/package.order
index 4bd6b34d90..0b11f3b287 100644
--- a/AixLib/Fluid/Movers/BaseClasses/Validation/package.order
+++ b/AixLib/Fluid/Movers/BaseClasses/Validation/package.order
@@ -1,2 +1,9 @@
+EulerComparison
+EulerCurve
+EulerReducedSpeed
 FlowMachineInterface
+HydraulicEfficiencyMethods
+MotorEfficiencyMethods
+NegativePressureOrFlow
 PowerInterface
+TotalEfficiencyMethods
diff --git a/AixLib/Fluid/Movers/BaseClasses/package.order b/AixLib/Fluid/Movers/BaseClasses/package.order
index 5eef704ec5..c35a84de69 100644
--- a/AixLib/Fluid/Movers/BaseClasses/package.order
+++ b/AixLib/Fluid/Movers/BaseClasses/package.order
@@ -3,5 +3,6 @@ IdealSource
 PartialFlowMachine
 PowerInterface
 Characteristics
+Euler
 Types
 Validation
diff --git a/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW12.mo b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW12.mo
new file mode 100644
index 0000000000..e90c78a34f
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW12.mo
@@ -0,0 +1,31 @@
+within AixLib.Fluid.Movers.Data.Fans.Greenheck;
+record BIDW12 "Fan data for Greenheck 12 BIDW fan"
+  extends Generic(
+    final powerOrEfficiencyIsHydraulic=true,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={0.941802252816019, 1.41392017800028, 1.88603810318454,
+                   2.36058962592129, 2.82784035600056, 3.30239187873731,
+                   3.77450980392156, 4.17118620497844},
+               P={         5309.384,         6323.536,         7188.548,
+                           7673.253,         7889.506,         8090.845,
+                           7785.108,         7740.366}),
+    pressure(V_flow={0.941802252816019, 1.41392017800028, 1.88603810318454,
+                      2.36058962592129, 2.82784035600056, 3.30239187873731,
+                      3.77450980392156, 4.17118620497844},
+                 dp={ 2684.68468468468, 2671.17117117117, 2536.03603603603,
+                      2186.93693693693, 1698.19819819819, 1191.44144144144,
+                      581.081081081081, 0}));
+
+  annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="per",
+Documentation(info="<html>
+<p>
+Fan performance data.
+See the documentation of
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Fans.Greenheck\">
+AixLib.Fluid.Movers.Data.Fans.Greenheck</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BIDW12;
diff --git a/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW13.mo b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW13.mo
new file mode 100644
index 0000000000..b1e39d3810
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW13.mo
@@ -0,0 +1,26 @@
+within AixLib.Fluid.Movers.Data.Fans.Greenheck;
+record BIDW13 "Fan data for Greenheck 13 BIDW fan"
+  extends Generic(
+    final powerOrEfficiencyIsHydraulic=true,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={0.945419103313839, 1.89083820662768, 2.83300844704353,
+                   3.77517868745939, 4.71734892787522, 5.38011695906431},
+               P={         7091.607,         9492.761,        10954.333,
+                          11610.549,        11849.173,        11252.613}),
+    pressure(V_flow={0.945419103313839, 1.89083820662768, 2.83300844704353,
+                      3.77517868745939, 4.71734892787522, 5.38011695906431},
+                 dp={ 3010.50788091068, 3005.25394045534, 2632.22416812609,
+                      1802.10157618213, 830.122591943958,                0}));
+  annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="per",
+Documentation(info="<html>
+<p>
+Fan performance data.
+See the documentation of
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Fans.Greenheck\">
+AixLib.Fluid.Movers.Data.Fans.Greenheck</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BIDW13;
diff --git a/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW15.mo b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW15.mo
new file mode 100644
index 0000000000..c1aee2e7b0
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW15.mo
@@ -0,0 +1,30 @@
+within AixLib.Fluid.Movers.Data.Fans.Greenheck;
+record BIDW15 "Fan data for Greenheck 15 BIDW fan"
+  extends Generic(
+    final powerOrEfficiencyIsHydraulic=true,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={1.88566375364128, 2.82632820086003, 3.77132750728255,
+                   4.7119919545013, 5.66132612012761, 6.60199056734636,
+                  7.02680676931611},
+               P={       12199.652,        14630.634,        16136.948,
+                         16808.078,        17195.842,        17285.326,
+                         16517.255}),
+    pressure(V_flow={1.88566375364128, 2.82632820086003, 3.77132750728255,
+                      4.7119919545013, 5.66132612012761, 6.60199056734636,
+                     7.02680676931611},
+                 dp={3389.81562774363, 3300.26338893766, 2894.64442493415,
+                     2183.49429323968,  1409.1308165057, 479.367866549604,
+                                    0}));
+  annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="per",
+Documentation(info="<html>
+<p>
+Fan performance data.
+See the documentation of
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Fans.Greenheck\">
+AixLib.Fluid.Movers.Data.Fans.Greenheck</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BIDW15;
diff --git a/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW16.mo b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW16.mo
new file mode 100644
index 0000000000..a98358dce5
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW16.mo
@@ -0,0 +1,30 @@
+within AixLib.Fluid.Movers.Data.Fans.Greenheck;
+record BIDW16 "Fan data for Greenheck 16 BIDW fan"
+  extends Generic(
+    final powerOrEfficiencyIsHydraulic=true,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={2.83018867924528, 3.77358490566036, 4.71698113207544,
+                  5.66037735849056, 6.60377358490564, 7.54716981132075,
+                  8.49056603773583, 8.99776831000203},
+               P={       18642.500,        21327.020,        22960.103,
+                         23884.771,        24496.245,        24749.783,
+                         24466.417,        23519.378}),
+    pressure(V_flow={2.83018867924528, 3.77358490566036, 4.71698113207544,
+                     5.66037735849056, 6.60377358490564, 7.54716981132075,
+                     8.49056603773583, 8.99776831000203},
+                 dp={3781.57683024939, 3663.31456154465, 3302.89621882542,
+                     2705.95333869670, 2047.06355591311, 1323.41110217216,
+                     504.022526146420, 0}));
+  annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="per",
+Documentation(info="<html>
+<p>
+Fan performance data.
+See the documentation of
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Fans.Greenheck\">
+AixLib.Fluid.Movers.Data.Fans.Greenheck</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BIDW16;
diff --git a/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW18.mo b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW18.mo
new file mode 100644
index 0000000000..81b323e981
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/Greenheck/BIDW18.mo
@@ -0,0 +1,34 @@
+within AixLib.Fluid.Movers.Data.Fans.Greenheck;
+record BIDW18 "Fan data for Greenheck 18 BIDW fan"
+  extends Generic(
+    final powerOrEfficiencyIsHydraulic=true,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={2.83387830993139, 3.77636725011219,   4.718856190293,
+                  5.66134513047381, 6.60383407065461, 7.55273450022439,
+                  8.49522344040519,   9.437712380586, 10.3802013207668,
+                  10.8546515355517},
+               P={       23966.798,        27486.502,        30163.565,
+                         32236.611,        33996.463,        35167.212,
+                         35965.111,        35883.084,        35308.895,
+                         34167.974}),
+    pressure(V_flow={2.83387830993139, 3.77636725011219,   4.718856190293,
+                     5.66134513047381, 6.60383407065461, 7.55273450022439,
+                     8.49522344040519,   9.437712380586, 10.3802013207668,
+                     10.8546515355517},
+                 dp={4223.51959966638, 4203.50291909924,  4106.7556296914,
+                     3913.26105087572, 3532.94412010008,  2855.7130942452,
+                     2105.08757297748,  1274.3953294412, 457.047539616347,
+                                    0}));
+  annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="per",
+Documentation(info="<html>
+<p>
+Fan performance data.
+See the documentation of
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Fans.Greenheck\">
+AixLib.Fluid.Movers.Data.Fans.Greenheck</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end BIDW18;
diff --git a/AixLib/Fluid/Movers/Data/Fans/Greenheck/package.mo b/AixLib/Fluid/Movers/Data/Fans/Greenheck/package.mo
new file mode 100644
index 0000000000..499dfc197a
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/Greenheck/package.mo
@@ -0,0 +1,27 @@
+within AixLib.Fluid.Movers.Data.Fans;
+package Greenheck "Package with performance data for fans of Greenheck"
+  extends Modelica.Icons.Package;
+
+  annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains performance data for Greenheck fans.
+The data points are digitised from
+<a href=\"https://content.greenheck.com/public/DAMProd/Original/10002/CentrifugalDWPerfSuppl_catalog.pdf\">
+https://content.greenheck.com/public/DAMProd/Original/10002/CentrifugalDWPerfSuppl_catalog.pdf</a>.
+The highest available speeds on the graphs were selected as nominal.
+The volumetric flow rates and static pressures were extracted by plot digitiser
+(<a href=\"https://apps.automeris.io/wpd/\">https://apps.automeris.io/wpd/</a>).
+The powers were read from the graphs approximately using
+<a href=\"https://eleif.net/photo_measure.html\">
+https://eleif.net/photo_measure.html</a>.
+For each pressure-flow rate curve, the points to the left of the highest point
+were abandoned to ensure convergence.
+See <a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">AixLib.Fluid.Movers.UsersGuide</a>
+and <a href=\"modelica://AixLib/Resources/Images/Fluid/Movers/UsersGuide/2013-IBPSA-Wetter.pdf\">Wetter (2013)</a>
+for more information on the convergence considerations.
+Also note that in the actual names of each fan,
+the number precedes the letters (e.g. \"12 BIDW\").
+They had to be reversed in class names of the records.
+</p>
+</html>"));
+end Greenheck;
diff --git a/AixLib/Fluid/Movers/Data/Fans/Greenheck/package.order b/AixLib/Fluid/Movers/Data/Fans/Greenheck/package.order
new file mode 100644
index 0000000000..9a6eef5bdf
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/Greenheck/package.order
@@ -0,0 +1,5 @@
+BIDW12
+BIDW13
+BIDW15
+BIDW16
+BIDW18
diff --git a/AixLib/Fluid/Movers/Data/Fans/package.mo b/AixLib/Fluid/Movers/Data/Fans/package.mo
new file mode 100644
index 0000000000..81f92c8cbd
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/package.mo
@@ -0,0 +1,15 @@
+within AixLib.Fluid.Movers.Data;
+package Fans "Package of fan performance data"
+  extends Modelica.Icons.Package;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains performance data for fans.
+</p>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
+User's Guide</a> for more information.
+</p>
+</html>"));
+end Fans;
diff --git a/AixLib/Fluid/Movers/Data/Fans/package.order b/AixLib/Fluid/Movers/Data/Fans/package.order
new file mode 100644
index 0000000000..27e8e2af3b
--- /dev/null
+++ b/AixLib/Fluid/Movers/Data/Fans/package.order
@@ -0,0 +1 @@
+Greenheck
diff --git a/AixLib/Fluid/Movers/Data/Generic.mo b/AixLib/Fluid/Movers/Data/Generic.mo
index eaa371d054..fc355c9078 100644
--- a/AixLib/Fluid/Movers/Data/Generic.mo
+++ b/AixLib/Fluid/Movers/Data/Generic.mo
@@ -9,71 +9,146 @@ record Generic "Generic data record for movers"
     dp =     {0, 0}) "Volume flow rate vs. total pressure rise"
     annotation(Evaluate=true,
                Dialog(group="Pressure curve"));
+  final parameter Modelica.Units.SI.VolumeFlowRate V_flow_max=
+    if havePressureCurve
+      then (pressure.V_flow[end]
+                -(pressure.V_flow[end] - pressure.V_flow[end - 1])
+                /(pressure.dp[end] - pressure.dp[end - 1])
+                * pressure.dp[end])
+    else 0
+      "Volume flow rate on the curve when pressure rise is zero";
+  final parameter Modelica.Units.SI.PressureDifference dpMax(
+    displayUnit="Pa")=
+    if havePressureCurve
+      then (pressure.dp[1]
+                -(pressure.dp[1] - pressure.dp[2])
+                /(pressure.V_flow[1] - pressure.V_flow[2])
+                * pressure.V_flow[1])
+    else 0
+      "Pressure rise on the curve when flow rate is zero";
 
-  parameter Boolean use_powerCharacteristic=false
-    "Use power data instead of motor efficiency"
+  // Efficiency computation choices
+  parameter AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod etaHydMet=
+    if havePressureCurve
+    then AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber
+    else AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.NotProvided
+    "Efficiency computation method for the hydraulic efficiency etaHyd"
     annotation (Dialog(group="Power computation"));
+  parameter AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod etaMotMet=
+    if powerOrEfficiencyIsHydraulic and havePressureCurve
+    then AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve
+    else AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided
+    "Efficiency computation method for the motor efficiency etaMot"
+    annotation (Dialog(group="Power computation"));
+
+  parameter Boolean powerOrEfficiencyIsHydraulic=true
+    "=true if hydraulic power or efficiency is provided, instead of total"
+    annotation (Dialog(group="Power computation",
+    enable=max(power.P)>Modelica.Constants.eps
+    or max(efficiency.eta)>Modelica.Constants.eps));
 
+  // Arrays for efficiency values
   parameter
     AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiencyParameters
-    hydraulicEfficiency(
+    efficiency(
       V_flow={0},
-      eta={0.7}) "Hydraulic efficiency (used if use_powerCharacteristic=false)"
+      eta={0.7}) "Total or hydraulic efficiency vs. volumetric flow rate"
     annotation (Dialog(group="Power computation",
-                       enable=not use_powerCharacteristic));
+                       enable=etaHydMet == AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate));
   parameter
     AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiencyParameters
     motorEfficiency(
       V_flow={0},
       eta={0.7})
-    "Electric motor efficiency (used if use_powerCharacteristic=false)"
+    "Motor efficiency vs. volumetric flow rate"
     annotation (Dialog(group="Power computation",
-                       enable=not use_powerCharacteristic));
+                       enable=etaMotMet == AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_VolumeFlowRate));
+  parameter
+    AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiencyParameters_yMot
+    motorEfficiency_yMot(y={0}, eta={0.7})
+    "Motor efficiency vs. part load ratio yMot, where yMot = WHyd/WMot_nominal"
+    annotation (Dialog(group="Power computation", enable=etaMotMet ==
+      AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio));
 
-  // Power requires default values to avoid in Dymola the message
-  // Failed to expand the variable Power.V_flow
-  parameter BaseClasses.Characteristics.powerParameters power(
+  // Power curve
+  //   It requires default values to suppress Dymola message
+  //   "Failed to expand the variable Power.V_flow"
+  parameter AixLib.Fluid.Movers.BaseClasses.Characteristics.powerParameters power(
     V_flow={0},
     P={0})
-    "Volume flow rate vs. electrical power consumption (used if use_powerCharacteristic=true)"
+    "Power (either consumed or hydraulic) vs. volumetric flow rate"
    annotation (Dialog(group="Power computation",
-                      enable=use_powerCharacteristic));
+                      enable =   etaHydMet==
+      AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate));
 
+  // Peak condition
+  parameter AixLib.Fluid.Movers.BaseClasses.Euler.peak peak(
+    V_flow=peak_internal.V_flow,
+    dp=peak_internal.dp,
+    eta=peak_internal.eta)
+    "Volume flow rate, pressure rise, and efficiency (either total or hydraulic) at peak condition"
+    annotation (Dialog(group="Power computation",
+                       enable =  etaHydMet==
+      AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber));
+  final parameter AixLib.Fluid.Movers.BaseClasses.Euler.peak peak_internal=
+    AixLib.Fluid.Movers.BaseClasses.Euler.getPeak(pressure=pressure,power=power)
+    "Internal peak variable";
+  // The getPeak() function automatically handles the estimation of peak point
+  //   when insufficient information is provided from the pressure curve.
+
+  // Motor
   parameter Boolean motorCooledByFluid=true
     "If true, then motor heat is added to fluid stream"
     annotation(Dialog(group="Motor heat rejection"));
+  parameter Modelica.Units.SI.Power WMot_nominal=
+    if max(power.P)>Modelica.Constants.eps
+    then
+      if powerOrEfficiencyIsHydraulic
+        then max(power.P)*1.2
+      else max(power.P)
+    else
+      if havePressureCurve
+        then V_flow_max/2 * dpMax/2 /0.7*1.2
+      else 0
+    "Rated motor power"
+      annotation(Dialog(group="Power computation",
+                        enable= etaMotMet==
+        AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio
+                        or      etaMotMet==
+        AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve));
+  parameter Modelica.Units.SI.Efficiency etaMot_max(max=1)= 0.7
+    "Maximum motor efficiency"
+    annotation (Dialog(group="Power computation", enable=etaMotMet ==
+      AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve));
+  final parameter
+    AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiencyParameters_yMot
+      motorEfficiency_yMot_generic=
+        AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve(
+          P_nominal=WMot_nominal,
+          eta_max=etaMot_max)
+    "Motor efficiency  vs. part load ratio"
+    annotation (Dialog(enable=false));
+  final parameter Boolean haveWMot_nominal=WMot_nominal > Modelica.Constants.eps
+    "= true, if the rated motor power is provided";
 
+  // Speed
   parameter Real speed_nominal(
     final min=0,
     final unit="1") = 1 "Nominal rotational speed for flow characteristic"
-    annotation (Dialog(group="Normalized speeds (used in model, default values assigned from speeds in rpm)"));
+    annotation (Dialog(group="Normalized speeds"));
 
-  parameter Real constantSpeed(final min=0, final unit="1") = constantSpeed_rpm/speed_rpm_nominal
+  parameter Real constantSpeed(final min=0, final unit="1") = 1
     "Normalized speed set point, used if inputType = AixLib.Fluid.Types.InputType.Constant"
-    annotation (Dialog(group="Normalized speeds (used in model, default values assigned from speeds in rpm)"));
+    annotation (Dialog(group="Normalized speeds"));
 
-  parameter Real[:] speeds(each final min = 0, each final unit="1") = speeds_rpm/speed_rpm_nominal
+  parameter Real[:] speeds(each final min = 0, each final unit="1") = {1}
     "Vector of normalized speed set points, used if inputType = AixLib.Fluid.Types.InputType.Stages"
-    annotation (Dialog(group="Normalized speeds (used in model, default values assigned from speeds in rpm)"));
-
-  parameter Modelica.Units.NonSI.AngularVelocity_rpm speed_rpm_nominal=1500
-    "Nominal rotational speed for flow characteristic"
-    annotation (Dialog(group="Speeds in RPM"));
-
-  parameter Modelica.Units.NonSI.AngularVelocity_rpm constantSpeed_rpm=
-      speed_rpm_nominal
-    "Speed set point, used if inputType = AixLib.Fluid.Types.InputType.Constant"
-    annotation (Dialog(group="Speeds in RPM"));
-
-  parameter Modelica.Units.NonSI.AngularVelocity_rpm[:] speeds_rpm={
-      speed_rpm_nominal}
-    "Vector of speed set points, used if inputType = AixLib.Fluid.Types.InputType.Stages"
-    annotation (Dialog(group="Speeds in RPM"));
+    annotation (Dialog(group="Normalized speeds"));
 
   // Set a parameter in order for
-  // (a) FlowControlled_m_flow and FlowControlled_dp being able to set a reasonable
+  // (a) FlowControlled_m_flow and FlowControlled_dp to be able to set a reasonable
   //     default pressure curve if it is not specified here, and
-  // (b) SpeedControlled_y and SpeedControlled_Nrpm being able to issue an assert
+  // (b) SpeedControlled_y to be able to issue an assert
   //     if no pressure curve is specified.
   final parameter Boolean havePressureCurve=
     sum(pressure.V_flow) > Modelica.Constants.eps and
@@ -84,89 +159,124 @@ record Generic "Generic data record for movers"
   defaultComponentPrefixes = "parameter",
   defaultComponentName = "per",
   Documentation(revisions="<html>
- <ul>
- <li>
- February 19, 2016, by Filip Jorissen:<br/>
- Refactored model such that <code>SpeedControlled_Nrpm</code>,
- <code>SpeedControlled_y</code> and <code>FlowControlled</code>
- are integrated into one record.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Changed parameter <code>N_nominal</code> to
- <code>speed_rpm_nominal</code> as it is the same quantity as <code>speeds_rmp</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- January 19, 2016, by Filip Jorissen:<br/>
- Added parameter <code>speeds_rpm</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- February 13, 2015, by Michael Wetter:<br/>
- Updated documentation.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised record for OpenModelica.
- </li>
- <li>
- November 22, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Record containing parameters for pumps or fans.
- </p>
- <h4>Typical use</h4>
- <p>
- This record may be used to assign for example fan performance data using
- declaration such as
- </p>
- <pre>
-   AixLib.Fluid.Movers.SpeedControlled_y fan(
-     redeclare package Medium = Medium,
-       per(pressure(V_flow={0,m_flow_nominal,2*m_flow_nominal}/1.2,
-                    dp={2*dp_nominal,dp_nominal,0}))) \"Fan\";
- </pre>
- <p>
- This data record can be used with
- <a href=\"modelica://AixLib.Fluid.Movers.SpeedControlled_Nrpm\">
- AixLib.Fluid.Movers.SpeedControlled_Nrpm</a>,
- <a href=\"modelica://AixLib.Fluid.Movers.SpeedControlled_y\">
- AixLib.Fluid.Movers.SpeedControlled_y</a>,
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
- AixLib.Fluid.Movers.FlowControlled_dp</a>,
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
- AixLib.Fluid.Movers.FlowControlled_m_flow</a>.
- </p>
- <p>
- An example that uses manufacturer data can be found in
- <a href=\"modelica://AixLib.Fluid.Movers.Validation.Pump_Nrpm_stratos\">
- AixLib.Fluid.Movers.Validation.Pump_Nrpm_stratos</a>.
- </p>
- <h4>Parameters in RPM</h4>
- <p>
- The parameters <code>speed_rpm_nominal</code>,
- <code>constantSpeed_rpm</code> and
- <code>speeds_rpm</code> are used to assign the non-dimensional speeds
- </p>
- <pre>
-   parameter Real constantSpeed(final min=0, final unit=\"1\") = constantSpeed_rpm/speed_rpm_nominal;
-   parameter Real[:] speeds(each final min = 0, each final unit=\"1\") = speeds_rpm/speed_rpm_nominal;
- </pre>
- <p>
- In addition, <code>speed_rpm_nominal</code> is used in
- <a href=\"modelica://AixLib.Fluid.Movers.SpeedControlled_Nrpm\">
- AixLib.Fluid.Movers.SpeedControlled_Nrpm</a>
- to normalize the control input signal.
- Otherwise, these speed parameters in RPM are not used in the models.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 8, 2024, by Hongxiang Fu:<br/>
+Default efficiency methods now depend on whether a pressure curve is available.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+March 1, 2022, by Hongxiang Fu:<br/>
+<ul>
+<li>
+Modified the record to allow separate specifications of different
+efficiency variables.
+</li>
+<li>
+Added parameters for computation using Euler number.
+</li>
+<li>
+Added parameters for providing the motor efficiency as an array
+vs. motor part load ratio.
+</li>
+<li>
+Moved the computation of <code>V_flow_max</code> here from
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine\">
+AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine</a>
+and <code>dpMax</code> here from
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface\">
+AixLib.Fluid.Movers.BaseClasses.FlowMachineInterface</a>
+</li>
+</ul>
+These are for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 19, 2016, by Filip Jorissen:<br/>
+Refactored model such that <code>SpeedControlled_Nrpm</code>,
+<code>SpeedControlled_y</code> and <code>FlowControlled</code>
+are integrated into one record.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Changed parameter <code>N_nominal</code> to
+<code>speed_rpm_nominal</code> as it is the same quantity as <code>speeds_rmp</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+January 19, 2016, by Filip Jorissen:<br/>
+Added parameter <code>speeds_rpm</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+February 13, 2015, by Michael Wetter:<br/>
+Updated documentation.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised record for OpenModelica.
+</li>
+<li>
+November 22, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Record containing parameters for pumps or fans.
+</p>
+<h4>Typical use</h4>
+<p>
+This record may be used to assign for example fan performance data using
+declaration such as
+</p>
+<pre>
+  AixLib.Fluid.Movers.SpeedControlled_y fan(
+    redeclare package Medium = Medium,
+      per(pressure(V_flow={0,m_flow_nominal,2*m_flow_nominal}/1.2,
+                   dp={2*dp_nominal,dp_nominal,0}))) \"Fan\";
+</pre>
+<p>
+This data record can be used with
+<a href=\"modelica://AixLib.Fluid.Movers.SpeedControlled_y\">
+AixLib.Fluid.Movers.SpeedControlled_y</a>,
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
+AixLib.Fluid.Movers.FlowControlled_dp</a>,
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.FlowControlled_m_flow</a>.
+</p>
+<p>
+An example that uses manufacturer data can be found in
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.Pump_y_stratos\">
+AixLib.Fluid.Movers.Validation.Pump_y_stratos</a>.
+</p>
+<h4>Declaration of the peak condition</h4>
+<p>
+The variable <code>peak</code> is intentionally declared in a way that each of its
+element is declared individually. If it was delcared the same way as does
+<code>peak_internal</code>, Modelica would prevent the modification of its
+specific elements with the following error message:<br/>
+<code>
+Record has a value, and attempt to modify specific elements.<br/>
+The element modification of e.g. V_flow will be ignored.<br/>
+</code>
+The other variable <code>peak_internal</code> uses a function call to compute its
+default values. By passing them to <code>peak</code> one by one, the model can
+both have default values and also allow the user to override them easily.
+See <a href=\"https://github.com/modelica/ModelicaSpecification/issues/791\">
+Modelica Specification issue #791</a>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Generic;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/CronolineIL80slash220dash4slash4.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/CronolineIL80slash220dash4slash4.mo
index 02d59c149b..4b1dbadf2e 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/CronolineIL80slash220dash4slash4.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/CronolineIL80slash220dash4slash4.mo
@@ -2,38 +2,67 @@ within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record CronolineIL80slash220dash4slash4
   "Pump data for a Wilo Cronoline-IL 80/220-4/4 pump"
   extends Generic(
-    use_powerCharacteristic=true,
-    speed_rpm_nominal=1450,
-    power(V_flow={0.00303454715219,0.00578898225957,0.00863678804855,0.0113912231559,0.0146125116713,0.0181605975724,0.0214285714286,0.0248366013072,0.0274042950514,0.0282446311858}, P={1905.29339941,2202.03582759,2548.86483304,2812.07908132,3146.06691483,3435.07911022,3592.75276695,3710.09774539,3774.78991597,3793.34692457}),
-    pressure(V_flow={0.00303454715219,0.00578898225957,0.00863678804855,0.0113912231559,0.0146125116713,0.0181605975724,0.0214285714286,0.0248366013072,0.0274042950514,0.0282446311858}, dp={168215.17064,166653.242326,164291.843595,161128.282627,154367.77774,142807.085577,128439.498542,108468.216086,92889.3102384,86895.3009775}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={0.00303454715219, 0.00578898225957, 0.00863678804855,
+                   0.0113912231559,  0.0146125116713,  0.0181605975724,
+                   0.0214285714286,  0.0248366013072,  0.0274042950514,
+                   0.0282446311858},
+               P={   1905.29339941,    2202.03582759,    2548.86483304,
+                     2812.07908132,    3146.06691483,    3435.07911022,
+                     3592.75276695,    3710.09774539,    3774.78991597,
+                     3793.34692457}),
+    pressure(V_flow={0.00303454715219, 0.00578898225957, 0.00863678804855,
+                      0.0113912231559,  0.0146125116713,  0.0181605975724,
+                      0.0214285714286,  0.0248366013072,  0.0274042950514,
+                      0.0282446311858},
+                 dp={    168215.17064,    166653.242326,    164291.843595,
+                        161128.282627,     154367.77774,    142807.085577,
+                        128439.498542,    108468.216086,    92889.3102384,
+                        86895.3009775}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
- <p>Data from: <a href=\"http://productfinder.wilo.com/com/en/c000000220003ab4800010023/_000000100002c2550002003a/product.html\">http://productfinder.wilo.com/com/en/c000000220003ab4800010023/_000000100002c2550002003a/product.html</a></p>
- <p>See <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 </a>for more information about how the data is derived. </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- June 01, 2017, by Iago Cupeiro:
- <br/>
- Changed data link to English version
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>Data from: <a href=\"http://productfinder.wilo.com/com/en/c000000220003ab4800010023/_000000100002c2550002003a/product.html\">http://productfinder.wilo.com/com/en/c000000220003ab4800010023/_000000100002c2550002003a/product.html</a></p>
+<p>See <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 </a>for more information about how the data is derived. </p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+June 01, 2017, by Iago Cupeiro:
+<br/>
+Changed data link to English version
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CronolineIL80slash220dash4slash4;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to4.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to4.mo
index 0632255259..1ffc1de173 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to4.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to4.mo
@@ -1,51 +1,68 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos25slash1to4 "Pump data for a Wilo Stratos 25/1-4 pump"
   extends Generic(
-    speed_rpm_nominal=1800,
-    use_powerCharacteristic = true,
-    power(V_flow={5.55555555556e-07,0.000402190923318,0.00052269170579,
-          0.000643192488263,0.000752738654147,0.000866979655712,
-          0.000973395931142,0.00108607198748,0.00115962441315}, P={
-          14.2085618951,21.2596204596,23.3573239437,25.1349149442,26.581943662,
-          27.9121571534,28.8498841148,29.4981726255,29.7520982304}),
-    pressure(V_flow={5.55555555556e-07,0.000402190923318,0.00052269170579,
-          0.000643192488263,0.000752738654147,0.000866979655712,
-          0.000973395931142,0.00108607198748,0.00115962441315}, dp={
-          17066.9518717,16997.0053476,16437.4331551,15528.1283422,14408.9839572,
-          13149.9465241,11681.0695187,9932.40641711,8533.47593583}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={5.55555555556e-07, 0.000402190923318,  0.00052269170579,
+                  0.000643192488263, 0.000752738654147, 0.000866979655712,
+                  0.000973395931142,  0.00108607198748,  0.00115962441315},
+               P={    14.2085618951,     21.2596204596,     23.3573239437,
+                      25.1349149442,      26.581943662,     27.9121571534,
+                      28.8498841148,     29.4981726255,     29.7520982304}),
+    pressure(V_flow={5.55555555556e-07, 0.000402190923318,  0.00052269170579,
+                     0.000643192488263, 0.000752738654147, 0.000866979655712,
+                     0.000973395931142,  0.00108607198748,  0.00115962441315},
+                 dp={    17066.9518717,     16997.0053476,     16437.4331551,
+                         15528.1283422,     14408.9839572,     13149.9465241,
+                         11681.0695187,     9932.40641711,     8533.47593583}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>",
   revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 17, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 17, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos25slash1to4;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to6.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to6.mo
index 6b567b2b73..3b0f6f344f 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to6.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to6.mo
@@ -1,64 +1,79 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos25slash1to6 "Pump data for a Wilo Stratos 25/1-6 pump"
   extends Generic(
-    speed_rpm_nominal=2540,
-    use_powerCharacteristic=true,
-    power(V_flow={8.4618254914e-06,0.000274485730449,0.000555832400486,
-          0.000837082776634,0.00110292011218,0.00138657181719,0.00166761756882,
-          0.00187198329301}, P={27.7850423935,35.9020280633,46.212011386,
-          55.5493899809,62.3704820257,68.7045763872,73.3263927089,75.1773568358}),
-    pressure(V_flow={8.4618254914e-06,0.000274485730449,0.000555832400486,
-          0.000837082776634,0.00110292011218,0.00138657181719,0.00166761756882,
-          0.00187198329301}, dp={34808.1176471,34738.9411765,34508.1176471,
-          32430.7058824,29083.7647059,24005.6470588,18004.2352941,13041.5294118}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={8.4618254914e-06, 0.000274485730449, 0.000555832400486,
+                 0.000837082776634,  0.00110292011218,  0.00138657181719,
+                  0.00166761756882,  0.00187198329301},
+               P={   27.7850423935,     35.9020280633,      46.212011386,
+                     55.5493899809,     62.3704820257,     68.7045763872,
+                     73.3263927089,     75.1773568358}),
+    pressure(V_flow={8.4618254914e-06, 0.000274485730449, 0.000555832400486,
+                    0.000837082776634,  0.00110292011218,  0.00138657181719,
+                     0.00166761756882,  0.00187198329301},
+                 dp={   34808.1176471,     34738.9411765,     34508.1176471,
+                        32430.7058824,     29083.7647059,     24005.6470588,
+                        18004.2352941,     13041.5294118}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
- <p>Data from
- <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000028040002003a/fc_product_datasheet\">
- http://productfinder.wilo.com/en/COM/product/00000018000028040002003a/fc_product_datasheet</a>
- </p>
- <p>
- The nominal rpm is arbitrarily chosen as the rpm of the pump curve
- in the data sheet that has the highest rpm,
- without being limited by the maximum power limitation
- (see dotted curve on figure below).
- Pump curves (H(m_flow) and P(m_flow)) from the data sheets
- are digitized using
- <a href=\"https://automeris.io/WebPlotDigitizer/\">web plot digitizer</a>.
- </p>
- <h4>Limitations:</h4>
- <ul>
- <li>The pump curve cap at high rpm that can be seen is not enforced
- by the model.
- </li>
- <li>
- The pump curve may be altered slightly to guarantee that <i>dp/dm&lt;0</i>
- </li>
- </ul>
- <p>
- The figure below illustrates a digitized pump curve.
- </p>
- <p align=\"center\">
- <img alt=\"Pump curve\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Data/stratoscurve.png\"/></p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 17, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>Data from
+<a href=\"http://productfinder.wilo.com/en/COM/product/00000018000028040002003a/fc_product_datasheet\">
+http://productfinder.wilo.com/en/COM/product/00000018000028040002003a/fc_product_datasheet</a>
+</p>
+<p>
+Pump curves (H(m_flow) and P(m_flow)) from the data sheets
+are digitized using
+<a href=\"https://automeris.io/WebPlotDigitizer/\">web plot digitizer</a>.
+</p>
+<h4>Limitations:</h4>
+<ul>
+<li>The pump curve cap at high speed that can be seen is not enforced
+by the model.
+</li>
+<li>
+The pump curve may be altered slightly to guarantee that <i>dp/dm&lt;0</i>
+</li>
+</ul>
+<p>
+The figure below illustrates a digitized pump curve.
+</p>
+<p align=\"center\">
+<img alt=\"Pump curve\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Data/stratoscurve.png\"/></p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 17, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos25slash1to6;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to8.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to8.mo
index d636272275..555fe2844f 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to8.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos25slash1to8.mo
@@ -1,48 +1,67 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos25slash1to8 "Pump data for a Wilo Stratos 25/1-8 pump"
   extends Generic(
-    speed_rpm_nominal=3040,
-    use_powerCharacteristic=true,
-    power(V_flow={2.66111582909e-06,0.000621486635037,0.000887056469533,
-          0.0011525489114,0.00140859349908,0.00168018209891,0.00191740837085,
-          0.00219831980599}, P={42.7878285797,72.7712666315,87.0576021552,
-          99.7562542248,108.565085499,117.461493336,123.188074537,128.511579716}),
-    pressure(V_flow={2.66111582909e-06,0.000621486635037,0.000887056469533,
-          0.0011525489114,0.00140859349908,0.00168018209891,0.00191740837085,
-          0.00219831980599}, dp={50002.7035151,49603.919395,47783.2940685,
-          44505.1908368,39882.6694921,33688.9797121,27835.1000463,20631.4409942}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={2.66111582909e-06, 0.000621486635037, 0.000887056469533,
+                    0.0011525489114,  0.00140859349908,  0.00168018209891,
+                   0.00191740837085,  0.00219831980599},
+               P={    42.7878285797,     72.7712666315,     87.0576021552,
+                      99.7562542248,     108.565085499,     117.461493336,
+                      123.188074537,     128.511579716}),
+    pressure(V_flow={2.66111582909e-06, 0.000621486635037, 0.000887056469533,
+                       0.0011525489114,  0.00140859349908,  0.00168018209891,
+                      0.00191740837085,  0.00219831980599},
+                 dp={    50002.7035151,      49603.919395,     47783.2940685,
+                         44505.1908368,     39882.6694921,     33688.9797121,
+                         27835.1000463,     20631.4409942}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000028650002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000028650002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos25slash1to8;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos30slash1to4.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos30slash1to4.mo
index e4d12f8eed..79da724aca 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos30slash1to4.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos30slash1to4.mo
@@ -1,50 +1,67 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos30slash1to4 "Pump data for a Wilo Stratos 30/1-4 pump"
   extends Generic(
-    speed_rpm_nominal=1800,
-    use_powerCharacteristic=true,
-    power(V_flow={5.55555555556e-07,0.000402190923318,0.00052269170579,
-          0.000643192488263,0.000752738654147,0.000866979655712,
-          0.000973395931142,0.00108607198748,0.00115962441315}, P={
-          14.2085618951,21.2596204596,23.3573239437,25.1349149442,26.581943662,
-          27.9121571534,28.8498841148,29.4981726255,29.7520982304}),
-    pressure(V_flow={5.55555555556e-07,0.000402190923318,0.00052269170579,
-          0.000643192488263,0.000752738654147,0.000866979655712,
-          0.000973395931142,0.00108607198748,0.00115962441315}, dp={
-          17066.9518717,16997.0053476,16437.4331551,15528.1283422,14408.9839572,
-          13149.9465241,11681.0695187,9932.40641711,8533.47593583}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={5.55555555556e-07, 0.000402190923318,  0.00052269170579,
+                  0.000643192488263, 0.000752738654147, 0.000866979655712,
+                  0.000973395931142,  0.00108607198748,  0.00115962441315},
+               P={    14.2085618951,     21.2596204596,     23.3573239437,
+                      25.1349149442,      26.581943662,     27.9121571534,
+                      28.8498841148,     29.4981726255,     29.7520982304}),
+    pressure(V_flow={5.55555555556e-07, 0.000402190923318,  0.00052269170579,
+                     0.000643192488263, 0.000752738654147, 0.000866979655712,
+                     0.000973395931142,  0.00108607198748,  0.00115962441315},
+                 dp={    17066.9518717,     16997.0053476,     16437.4331551,
+                         15528.1283422,     14408.9839572,     13149.9465241,
+                         11681.0695187,     9932.40641711,     8533.47593583}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/0000000e000379ac0002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/0000000e000379ac0002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos30slash1to4;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos30slash1to8.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos30slash1to8.mo
index b1e84404b9..ce25936308 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos30slash1to8.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos30slash1to8.mo
@@ -1,48 +1,67 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos30slash1to8 "Pump data for a Wilo Stratos 30/1-8 pump"
   extends Generic(
-    speed_rpm_nominal=3040,
-    use_powerCharacteristic=true,
-    power(V_flow={2.66111582909e-06,0.000621486635037,0.000887056469533,
-          0.0011525489114,0.00140859349908,0.00168018209891,0.00191740837085,
-          0.00219831980599}, P={42.7878285797,72.7712666315,87.0576021552,
-          99.7562542248,108.565085499,117.461493336,123.188074537,128.511579716}),
-    pressure(V_flow={2.66111582909e-06,0.000621486635037,0.000887056469533,
-          0.0011525489114,0.00140859349908,0.00168018209891,0.00191740837085,
-          0.00219831980599}, dp={50002.7035151,49603.919395,47783.2940685,
-          44505.1908368,39882.6694921,33688.9797121,27835.1000463,20631.4409942}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={2.66111582909e-06, 0.000621486635037, 0.000887056469533,
+                    0.0011525489114,  0.00140859349908,  0.00168018209891,
+                   0.00191740837085,  0.00219831980599},
+               P={    42.7878285797,     72.7712666315,     87.0576021552,
+                      99.7562542248,     108.565085499,     117.461493336,
+                      123.188074537,     128.511579716}),
+    pressure(V_flow={2.66111582909e-06, 0.000621486635037, 0.000887056469533,
+                       0.0011525489114,  0.00140859349908,  0.00168018209891,
+                      0.00191740837085,  0.00219831980599},
+                 dp={    50002.7035151,      49603.919395,     47783.2940685,
+                         44505.1908368,     39882.6694921,     33688.9797121,
+                         27835.1000463,     20631.4409942}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000029420002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000029420002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos30slash1to8;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos32slash1to12.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos32slash1to12.mo
index f7a5144488..937edbf4f3 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos32slash1to12.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos32slash1to12.mo
@@ -1,50 +1,67 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos32slash1to12 "Pump data for a Wilo Stratos 32/1-12 pump"
   extends Generic(
-    speed_rpm_nominal=3580,
-    use_powerCharacteristic=true,
-    power(V_flow={2.11830535572e-05,0.000167865707434,0.000700939248601,
-          0.0012450039968,0.00177258193445,0.00227268185452,0.00272332134293,
-          0.00312450039968,0.00345423661071}, P={103.427852653,110.225580543,
-          135.414121033,162.955749719,191.043411366,216.051565678,230.204882307,
-          236.346847436,239.552825212}),
-    pressure(V_flow={2.11830535572e-05,0.000167865707434,0.000700939248601,
-          0.0012450039968,0.00177258193445,0.00227268185452,0.00272332134293,
-          0.00312450039968,0.00345423661071}, dp={59279.4925671,59115.2927989,
-          59000.1476354,57351.238791,54446.2693068,50284.7374612,44865.6398104,
-          38328.4550274,32066.9663984}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={2.11830535572e-05, 0.000167865707434, 0.000700939248601,
+                    0.0012450039968,  0.00177258193445,  0.00227268185452,
+                   0.00272332134293,  0.00312450039968,  0.00345423661071},
+               P={    103.427852653,     110.225580543,     135.414121033,
+                      162.955749719,     191.043411366,     216.051565678,
+                      230.204882307,     236.346847436,     239.552825212}),
+    pressure(V_flow={2.11830535572e-05, 0.000167865707434, 0.000700939248601,
+                       0.0012450039968,  0.00177258193445,  0.00227268185452,
+                      0.00272332134293,  0.00312450039968,  0.00345423661071},
+                 dp={    59279.4925671,     59115.2927989,     59000.1476354,
+                          57351.238791,     54446.2693068,     50284.7374612,
+                         44865.6398104,     38328.4550274,     32066.9663984}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000029770002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000029770002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos32slash1to12;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos40slash1to12.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos40slash1to12.mo
index 71cb6a0409..e33038d8ee 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos40slash1to12.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos40slash1to12.mo
@@ -1,48 +1,67 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos40slash1to12 "Pump data for a Wilo Stratos 40/1-12 pump"
   extends Generic(
-    speed_rpm_nominal=3690,
-    use_powerCharacteristic=true,
-    power(V_flow={2.05415499533e-05,0.0012380952381,0.00197759103641,0.00261998132586,
-          0.00315779645191,0.00385247432306,0.00436788048553,0.00493557422969},
-        P={195.711338777,254.50525152,302.203269367,339.387400348,367.008331835,
-          392.162896856,397.658764999,404.489181997}),
-    pressure(V_flow={2.05415499533e-05,0.0012380952381,0.00197759103641,0.00261998132586,
-          0.00315779645191,0.00385247432306,0.00436788048553,0.00493557422969},
-        dp={78528.2698296,78278.944236,77854.9591567,74108.1678158,68408.8742011,
-          57809.9050693,48393.0944907,37408.2956474}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={2.05415499533e-05,  0.0012380952381, 0.00197759103641,
+                   0.00261998132586, 0.00315779645191, 0.00385247432306,
+                   0.00436788048553, 0.00493557422969},
+               P={    195.711338777,     254.50525152,    302.203269367,
+                      339.387400348,    367.008331835,    392.162896856,
+                      397.658764999,    404.489181997}),
+    pressure(V_flow={2.05415499533e-05,  0.0012380952381, 0.00197759103641,
+                      0.00261998132586, 0.00315779645191, 0.00385247432306,
+                      0.00436788048553, 0.00493557422969},
+              dp={       78528.2698296,     78278.944236,    77854.9591567,
+                         74108.1678158,    68408.8742011,    57809.9050693,
+                         48393.0944907,    37408.2956474}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000029380002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000029380002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos40slash1to12;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos40slash1to8.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos40slash1to8.mo
index 180878cbad..7cd544ee85 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos40slash1to8.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos40slash1to8.mo
@@ -1,48 +1,67 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos40slash1to8 "Pump data for a Wilo Stratos 40/1-8 pump"
   extends Generic(
-    speed_rpm_nominal=3830,
-    use_powerCharacteristic=true,
-    power(V_flow={4.03163741226e-06,0.00188290448506,0.00245068662086,
-          0.00286231420438,0.00325508173616,0.00357919645424,0.00394696189973},
-        P={99.4470603052,175.709481933,197.426392754,209.437047607,213.2290948,
-          215.740841723,218.557203232}),
-    pressure(V_flow={4.03163741226e-06,0.00188290448506,0.00245068662086,
-          0.00286231420438,0.00325508173616,0.00357919645424,0.00394696189973},
-        dp={50361.3292164,50002.6907452,46761.3220062,42267.4693149,
-          36095.691563,30066.6880748,23476.280464}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={4.03163741226e-06, 0.00188290448506, 0.00245068662086,
+                   0.00286231420438, 0.00325508173616, 0.00357919645424,
+                   0.00394696189973},
+               P={    99.4470603052,    175.709481933,    197.426392754,
+                      209.437047607,      213.2290948,    215.740841723,
+                      218.557203232}),
+    pressure(V_flow={4.03163741226e-06, 0.00188290448506, 0.00245068662086,
+                      0.00286231420438, 0.00325508173616, 0.00357919645424,
+                      0.00394696189973},
+                 dp={    50361.3292164,    50002.6907452,    46761.3220062,
+                         42267.4693149,     36095.691563,    30066.6880748,
+                          23476.280464}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000028050002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000028050002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos40slash1to8;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos50slash1to12.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos50slash1to12.mo
index 0bf6615b6f..79ae0632a4 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos50slash1to12.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos50slash1to12.mo
@@ -1,50 +1,67 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos50slash1to12 "Pump data for a Wilo Stratos 50/1-12 pump"
   extends Generic(
-    speed_rpm_nominal=3690,
-    use_powerCharacteristic=true,
-    power(V_flow={5.55555555556e-07,0.00209948320413,0.00303617571059,
-          0.00389750215332,0.0046188630491,0.00546942291128,0.00621231696813,
-          0.00695521102498,0.00755813953488}, P={205.291823945,337.504763698,
-          400.584905585,453.68913657,488.040727585,515.872422868,528.307902115,
-          531.276246541,523.90128749}),
-    pressure(V_flow={5.55555555556e-07,0.00209948320413,0.00303617571059,
-          0.00389750215332,0.0046188630491,0.00546942291128,0.00621231696813,
-          0.00695521102498,0.00755813953488}, dp={74298.6885246,74154.3248189,
-          73404.0823485,70722.2584827,66879.2916508,59372.6282882,49547.6683187,
-          37985.8558902,27964.6709874}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={5.55555555556e-07, 0.00209948320413, 0.00303617571059,
+                   0.00389750215332,  0.0046188630491, 0.00546942291128,
+                   0.00621231696813, 0.00695521102498, 0.00755813953488},
+               P={    205.291823945,    337.504763698,    400.584905585,
+                       453.68913657,    488.040727585,    515.872422868,
+                      528.307902115,    531.276246541,     523.90128749}),
+    pressure(V_flow={5.55555555556e-07, 0.00209948320413, 0.00303617571059,
+                      0.00389750215332,  0.0046188630491, 0.00546942291128,
+                      0.00621231696813, 0.00695521102498, 0.00755813953488},
+                 dp={    74298.6885246,    74154.3248189,    73404.0823485,
+                         70722.2584827,    66879.2916508,    59372.6282882,
+                         49547.6683187,    37985.8558902,    27964.6709874}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000029520002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/00000018000029520002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos50slash1to12;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos80slash1to12.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos80slash1to12.mo
index c3b31c5342..e3141d94ce 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos80slash1to12.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/Stratos80slash1to12.mo
@@ -1,50 +1,67 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record Stratos80slash1to12 "Pump data for a Wilo Stratos 80/1-12 pump"
   extends Generic(
-    speed_rpm_nominal=2610,
-    use_powerCharacteristic=true,
-    power(V_flow={8.79043600562e-06,0.00277777777778,0.00556874120956,
-          0.00776635021097,0.00978815049226,0.0113484528833,0.0127329465541,
-          0.013985583685,0.0154360056259}, P={437.425146701,588.954435301,
-          792.603370491,931.705429399,1048.15648043,1115.77190985,1154.92222088,
-          1171.51603429,1166.47479929}),
-    pressure(V_flow={8.79043600562e-06,0.00277777777778,0.00556874120956,
-          0.00776635021097,0.00978815049226,0.0113484528833,0.0127329465541,
-          0.013985583685,0.0154360056259}, dp={78355.8975904,78243.6144578,
-          78054.5060241,75596.0963855,70490.1686747,63682.2650602,55361.4939759,
-          45527.8554217,30966.5060241}));
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={8.79043600562e-06, 0.00277777777778, 0.00556874120956,
+                   0.00776635021097, 0.00978815049226,  0.0113484528833,
+                    0.0127329465541,   0.013985583685,  0.0154360056259},
+               P={    437.425146701,    588.954435301,    792.603370491,
+                      931.705429399,    1048.15648043,    1115.77190985,
+                      1154.92222088,    1171.51603429,    1166.47479929}),
+    pressure(V_flow={8.79043600562e-06, 0.00277777777778, 0.00556874120956,
+                      0.00776635021097, 0.00978815049226,  0.0113484528833,
+                       0.0127329465541,   0.013985583685,  0.0154360056259},
+                 dp={    78355.8975904,    78243.6144578,    78054.5060241,
+                         75596.0963855,    70490.1686747,    63682.2650602,
+                         55361.4939759,    45527.8554217,    30966.5060241}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/0000001700017d670001003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/0000001700017d670001003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000000e000379df0002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>", revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratos80slash1to12;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS25slash10.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS25slash10.mo
index 965ab81658..0342cae1ad 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS25slash10.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS25slash10.mo
@@ -1,56 +1,71 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record TopS25slash10 "Pump data for a staged Wilo-Top-S 25/10 pump"
   extends Generic(
-    speed_rpm_nominal=2650,
-    use_powerCharacteristic = true,
-    power(V_flow={3.51617440225e-06,0.000523909985935,0.000847398030942,
-                  0.00115682137834,0.00148382559775,0.00177918424754,
-                  0.00206047819972,0.00229254571027,0.0025,0.00271097046414,
-                  0.00282700421941},
-          P={192.787993617,238.762280675,272.937843988,301.381574494,
-             326.18493197,344.613937245,359.220335761,369.040720135,
-             376.979332273,382.887700535,382.887700535}),
-    pressure(V_flow={3.51617440225e-06,0.000523909985935,0.000847398030942,
-                     0.00115682137834,0.00148382559775,0.00177918424754,
-                     0.00206047819972,0.00229254571027,0.0025,0.00271097046414,
-                     0.00282700421941},
-             dp={110125.414283,106765.16619,100392.787862,92220.6199738,
-                 81651.34693,70879.932776,60307.3708281,50930.4520427,
-                 41152.0339559,29575.0912725,22388.3296727}),
-    speeds_rpm = {0, 1950, 2250, 2650});
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={3.51617440225e-06, 0.000523909985935, 0.000847398030942,
+                   0.00115682137834,  0.00148382559775,  0.00177918424754,
+                   0.00206047819972,  0.00229254571027,            0.0025,
+                   0.00271097046414,  0.00282700421941},
+               P={    192.787993617,     238.762280675,     272.937843988,
+                      301.381574494,      326.18493197,     344.613937245,
+                      359.220335761,     369.040720135,     376.979332273,
+                      382.887700535,     382.887700535}),
+    pressure(V_flow={3.51617440225e-06, 0.000523909985935, 0.000847398030942,
+                      0.00115682137834,  0.00148382559775,  0.00177918424754,
+                      0.00206047819972,  0.00229254571027,            0.0025,
+                      0.00271097046414,  0.00282700421941},
+                 dp={    110125.414283,      106765.16619,     100392.787862,
+                         92220.6199738,       81651.34693,      70879.932776,
+                         60307.3708281,     50930.4520427,     41152.0339559,
+                         29575.0912725,     22388.3296727}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/0000001000029c210002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/0000001000029c210002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",
-           revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- January 19, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/0000001000029c210002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/0000001000029c210002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>",revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+January 19, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TopS25slash10;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS30slash10.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS30slash10.mo
index 5aec506469..f28b58db37 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS30slash10.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS30slash10.mo
@@ -1,57 +1,72 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record TopS30slash10 "Pump data for a staged Wilo-Top-S 30/10 pump"
   extends Generic(
-    speed_rpm_nominal=2650,
-    use_powerCharacteristic = true,
-    power(V_flow={3.51617440225e-06,0.000523909985935,0.000847398030942,
-                  0.00115682137834,0.00148382559775,0.00177918424754,
-                  0.00206047819972,0.00229254571027,0.0025,
-                  0.00271097046414,0.00282700421941},
-          P={192.787993617,238.762280675,272.937843988,
-             301.381574494,326.18493197,344.613937245,
-             359.220335761,369.040720135,376.979332273,
-             382.887700535,382.887700535}),
-    pressure(V_flow={3.51617440225e-06,0.000523909985935,0.000847398030942,
-                     0.00115682137834,0.00148382559775,0.00177918424754,
-                     0.00206047819972,0.00229254571027,0.0025,0.00271097046414,
-                     0.00282700421941},
-             dp={110125.414283,106765.16619,100392.787862,92220.6199738,
-                 81651.34693,70879.932776,60307.3708281,50930.4520427,
-                 41152.0339559,29575.0912725,22388.3296727}),
-    speeds_rpm = {0, 1950, 2250, 2650});
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={3.51617440225e-06, 0.000523909985935, 0.000847398030942,
+                   0.00115682137834,  0.00148382559775,  0.00177918424754,
+                   0.00206047819972,  0.00229254571027,            0.0025,
+                   0.00271097046414,  0.00282700421941},
+               P={    192.787993617,     238.762280675,     272.937843988,
+                      301.381574494,      326.18493197,     344.613937245,
+                      359.220335761,     369.040720135,     376.979332273,
+                      382.887700535,     382.887700535}),
+    pressure(V_flow={3.51617440225e-06, 0.000523909985935, 0.000847398030942,
+                      0.00115682137834,  0.00148382559775,  0.00177918424754,
+                      0.00206047819972,  0.00229254571027,            0.0025,
+                      0.00271097046414,  0.00282700421941},
+                 dp={    110125.414283,      106765.16619,     100392.787862,
+                         92220.6199738,       81651.34693,      70879.932776,
+                         60307.3708281,     50930.4520427,     41152.0339559,
+                         29575.0912725,     22388.3296727}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/00000009000287740001003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/00000009000287740001003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/00000009000287740001003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/00000009000287740001003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>",
   revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- January 19, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+January 19, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TopS30slash10;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS30slash5.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS30slash5.mo
index 36823f8f82..56183d1f0d 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS30slash5.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS30slash5.mo
@@ -1,56 +1,72 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record TopS30slash5 "Pump data for a staged Wilo-Top-S 30/5 pump"
   extends Generic(
-    speed_rpm_nominal=2650,
-    use_powerCharacteristic = true,
-    power(V_flow={4.24448217317e-06,0.000275419732126,0.000501792114695,
-                  0.000688077721185,0.000827202414639,0.00101584606678,
-                  0.0011714770798,0.00132710809281,0.00148981324278,
-                  0.00166195057536},
-          P={83.0171256559,101.117659669,113.263045942,122.28302674,
-             128.764680916,135.257448954,139.852003784,143.350736549,
-             145.269964752,146.115128625}),
-    pressure(V_flow={4.24448217317e-06,0.000275419732126,0.000501792114695,
-                     0.000688077721185,0.000827202414639,0.00101584606678,
-                     0.0011714770798,0.00132710809281,0.00148981324278,
-                     0.00166195057536},
-             dp={52688.1456954,49223.2450331,45151.986755,40994.1059603,
-                 37269.3377483,31205.7615894,25661.9205298,19598.3443709,
-                 12755.1655629,4699.27152318}),
-    speeds_rpm = {0, 1890, 2190, 2650});
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={4.24448217317e-06, 0.000275419732126, 0.000501792114695,
+                  0.000688077721185, 0.000827202414639,  0.00101584606678,
+                    0.0011714770798,  0.00132710809281,  0.00148981324278,
+                   0.00166195057536},
+               P={    83.0171256559,     101.117659669,     113.263045942,
+                       122.28302674,     128.764680916,     135.257448954,
+                      139.852003784,     143.350736549,     145.269964752,
+                      146.115128625}),
+    pressure(V_flow={4.24448217317e-06, 0.000275419732126, 0.000501792114695,
+                     0.000688077721185, 0.000827202414639,  0.00101584606678,
+                       0.0011714770798,  0.00132710809281,  0.00148981324278,
+                      0.00166195057536},
+                 dp={    52688.1456954,     49223.2450331,      45151.986755,
+                         40994.1059603,     37269.3377483,     31205.7615894,
+                         25661.9205298,     19598.3443709,     12755.1655629,
+                         4699.27152318}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/00000000000296670002003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/00000000000296670002003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/00000000000296670002003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/00000000000296670002003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>",
   revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- January 19, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+January 19, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TopS30slash5;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS40slash10.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS40slash10.mo
index 3d87d1e083..8970c8de52 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS40slash10.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS40slash10.mo
@@ -1,54 +1,68 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record TopS40slash10 "Pump data for a staged Wilo-Top-S 40/10 pump"
   extends Generic(
-    speed_rpm_nominal=2900,
-    use_powerCharacteristic = true,
-    power(V_flow={2.29252636405e-05,0.00110041265475,0.00221610881858,
-                  0.00334708849152,0.00417239798258,0.0048448723827,
-                  0.00537979520098,0.00605991135565,0.00625859697387},
-          P={432.950095719,492.916811695,565.94308364,630.111524164,
-             658.215613383,671.6839839,676.925957128,671.543363813,
-             668.661679135}),
-    pressure(V_flow={2.29252636405e-05,0.00110041265475,0.00221610881858,
-                     0.00334708849152,0.00417239798258,0.0048448723827,
-                     0.00537979520098,0.00605991135565,0.00625859697387},
-             dp={98785.5232361,97106.6860151,91320.1257409,79370.6856694,
-                 66042.1923274,53051.3974809,40227.5679296,25353.7625039,
-                 20566.1680722}),
-    speeds_rpm = {0, 2600, 2800});
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={2.29252636405e-05, 0.00110041265475, 0.00221610881858,
+                   0.00334708849152, 0.00417239798258,  0.0048448723827,
+                   0.00537979520098, 0.00605991135565, 0.00625859697387},
+               P={    432.950095719,    492.916811695,     565.94308364,
+                      630.111524164,    658.215613383,      671.6839839,
+                      676.925957128,    671.543363813,    668.661679135}),
+    pressure(V_flow={2.29252636405e-05, 0.00110041265475, 0.00221610881858,
+                      0.00334708849152, 0.00417239798258,  0.0048448723827,
+                      0.00537979520098, 0.00605991135565, 0.00625859697387},
+                 dp={    98785.5232361,    97106.6860151,    91320.1257409,
+                         79370.6856694,    66042.1923274,    53051.3974809,
+                         40227.5679296,    25353.7625039,    20566.1680722}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/000000120001ad890001003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/000000120001ad890001003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/000000120001ad890001003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/000000120001ad890001003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>",
   revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- January 19, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+January 19, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TopS40slash10;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS40slash7.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS40slash7.mo
index f781fe54ff..8d65264396 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS40slash7.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/TopS40slash7.mo
@@ -1,55 +1,72 @@
 within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record TopS40slash7 "Pump data for a staged Wilo-Top-S 40/7 pump"
   extends Generic(
-    speed_rpm_nominal=2800,
-    use_powerCharacteristic = true,
-    power(V_flow={9.97406742472e-07,0.000621384400559,0.00113006183922,
-                  0.00162078595651,0.00206961899062,0.00244663873928,
-                  0.0029074406543,0.00330241372432,0.00375723119888,
-                  0.00418212647117,0.00466686614802},
-          P={254.806788065,282.40881459,303.06122449,330.952380952,
-             347.819548872,360.093167702,372.657450077,380.261136713,
-             386.328725038,390.607012036,391.047619048}),
-    pressure(V_flow={9.97406742472e-07,0.000621384400559,0.00113006183922,0.00162078595651,
-                     0.00206961899062,0.00244663873928,0.0029074406543,0.00330241372432,
-                     0.00375723119888,0.00418212647117,0.00466686614802},
-             dp={70951.3953488,69946.0659263,67225.7989228,63706.4291679,
-                 59843.4165588,54951.3185253,48807.3201536,42775.1388251,
-                 34577.6798464,26835.4759718,17270.2037493}),
-    speeds_rpm = {0, 2200, 2450, 2650});
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={9.97406742472e-07, 0.000621384400559, 0.00113006183922,
+                   0.00162078595651,  0.00206961899062, 0.00244663873928,
+                    0.0029074406543,  0.00330241372432, 0.00375723119888,
+                   0.00418212647117,  0.00466686614802},
+               P={    254.806788065,      282.40881459,     303.06122449,
+                      330.952380952,     347.819548872,    360.093167702,
+                      372.657450077,     380.261136713,    386.328725038,
+                      390.607012036,     391.047619048}),
+    pressure(V_flow={9.97406742472e-07, 0.000621384400559, 0.00113006183922,
+                      0.00162078595651,  0.00206961899062, 0.00244663873928,
+                       0.0029074406543,  0.00330241372432, 0.00375723119888,
+                      0.00418212647117,  0.00466686614802},
+                 dp={    70951.3953488,     69946.0659263,    67225.7989228,
+                         63706.4291679,     59843.4165588,    54951.3185253,
+                         48807.3201536,     42775.1388251,    34577.6798464,
+                         26835.4759718,     17270.2037493}));
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
-   <p>Data from:
-   <a href=\"http://productfinder.wilo.com/en/COM/product/000000120001ad1f0001003a/fc_product_datasheet\">
-   http://productfinder.wilo.com/en/COM/product/000000120001ad1f0001003a/fc_product_datasheet
-   </a>
-   </p>
-   <p>See
-   <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
-   AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
-   </a>
-   for more information about how the data is derived.
-   </p>
-   </html>",
+  <p>Data from:
+  <a href=\"http://productfinder.wilo.com/en/COM/product/000000120001ad1f0001003a/fc_product_datasheet\">
+  http://productfinder.wilo.com/en/COM/product/000000120001ad1f0001003a/fc_product_datasheet
+  </a>
+  </p>
+  <p>See
+  <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">
+  AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6
+  </a>
+  for more information about how the data is derived.
+  </p>
+  </html>",
   revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- January 19, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+January 19, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TopS40slash7;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/VeroLine50slash150dash4slash2.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/VeroLine50slash150dash4slash2.mo
index f8fe2a014a..48d68b1bf5 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/VeroLine50slash150dash4slash2.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/VeroLine50slash150dash4slash2.mo
@@ -2,25 +2,46 @@ within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record VeroLine50slash150dash4slash2
   "Pump data for a Wilo Veroline IP-E 50/150-4/2 pump"
   extends Generic(
-    speed_rpm_nominal=2900,
-    use_powerCharacteristic=true,
-    power(V_flow={0.0,0.00277777, 0.00555555, 0.00833333, 0.01111111, 0.01388888, 0.01666666}, P={1607.8, 2235.3, 2862.7, 3529.4, 4078.4, 4392.2, 4666.7}),
-    pressure(V_flow={0.0,0.00277777, 0.00555555, 0.00833333, 0.01111111, 0.01388888, 0.01666666}, dp={255400, 253000, 250600, 248200, 232010, 199640, 156470}),
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={       0.0, 0.00277777, 0.00555555, 0.00833333, 0.01111111,
+                  0.01388888, 0.01666666},
+               P={    1607.8,     2235.3,     2862.7,     3529.4,     4078.4,
+                      4392.2,     4666.7}),
+    pressure(V_flow={       0.0, 0.00277777, 0.00555555, 0.00833333, 0.01111111,
+                     0.01388888, 0.01666666},
+                 dp={    255400,     253000,     250600,     248200,     232010,
+                         199640,     156470}),
     motorCooledByFluid=true);
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
- <p>Data from:<a href=\"http://productfinder.wilo.com/com/en/c0000002200012eb000020023/_0000004f0003f94e0001003a/product.html\"> http://productfinder.wilo.com/com/en/c0000002200012eb000020023/_0000004f0003f94e0001003a/product.html</a></p>
- <p>See <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6</a>for more information about how the data is derived.</p>
- </html>",  revisions="<html>
- <ul>
- <li>
- May 28, 2017, by Iago Cupeiro:
- <br/>
- Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>Data from:<a href=\"http://productfinder.wilo.com/com/en/c0000002200012eb000020023/_0000004f0003f94e0001003a/product.html\"> http://productfinder.wilo.com/com/en/c0000002200012eb000020023/_0000004f0003f94e0001003a/product.html</a></p>
+<p>See <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6</a>for more information about how the data is derived.</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+May 28, 2017, by Iago Cupeiro:
+<br/>
+Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VeroLine50slash150dash4slash2;
diff --git a/AixLib/Fluid/Movers/Data/Pumps/Wilo/VeroLine80slash115dash2comma2slash2.mo b/AixLib/Fluid/Movers/Data/Pumps/Wilo/VeroLine80slash115dash2comma2slash2.mo
index 2577e9347b..e7396aa99f 100644
--- a/AixLib/Fluid/Movers/Data/Pumps/Wilo/VeroLine80slash115dash2comma2slash2.mo
+++ b/AixLib/Fluid/Movers/Data/Pumps/Wilo/VeroLine80slash115dash2comma2slash2.mo
@@ -2,39 +2,64 @@ within AixLib.Fluid.Movers.Data.Pumps.Wilo;
 record VeroLine80slash115dash2comma2slash2
   "Pump data for a Wilo Veroline IP-E 80/115-2,2/2 pump"
   extends Generic(
-    speed_rpm_nominal=2900,
-    use_powerCharacteristic=true,
-    power(V_flow={0.0,0.00381944444444,0.00770833333333,0.0111111111111,0.014375,0.0171527777778,0.0197916666667,0.0220138888889}, P={1712.23021583,1939.82995422,2319.7768316,2599.92683819,2775.17985612,2815.09529219,2709.57970466,2571.61543492}),
-    pressure(V_flow={0.0,0.00381944444444,0.00770833333333,0.0111111111111,0.014375,0.0171527777778,0.0197916666667,0.0220138888889}, dp={157548.6,150053.76,139302.0,127431.9,113011.2,97943.04,76596.48,57133.44}),
+    final powerOrEfficiencyIsHydraulic=false,
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={            0.0, 0.00381944444444, 0.00770833333333,
+                  0.0111111111111,         0.014375,  0.0171527777778,
+                  0.0197916666667,  0.0220138888889},
+               P={  1712.23021583,    1939.82995422,     2319.7768316,
+                    2599.92683819,    2775.17985612,    2815.09529219,
+                    2709.57970466,    2571.61543492}),
+    pressure(V_flow={            0.0, 0.00381944444444, 0.00770833333333,
+                     0.0111111111111,         0.014375,  0.0171527777778,
+                     0.0197916666667,  0.0220138888889},
+                 dp={       157548.6,        150053.76,         139302.0,
+                            127431.9,         113011.2,         97943.04,
+                            76596.48,         57133.44}),
     motorCooledByFluid=true);
   annotation (
 defaultComponentPrefixes="parameter",
 defaultComponentName="per",
 Documentation(info="<html>
- <p>Data from:<a href=\"http://productfinder.wilo.com/com/en/c0000002200012eb000020023/_0000001d000149e80001003a/product.html\"> http://productfinder.wilo.com/com/en/c0000002200012eb000020023/_0000001d000149e80001003a/product.html</a></p>
- <p>See <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 </a>for more information about how the data is derived. </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- June 01, 2017, by Iago Cupeiro:
- <br/>
- Changed data link to the English version
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- December 12, 2014, by Michael Wetter:<br/>
- Added <code>defaultComponentPrefixes</code> and
- <code>defaultComponentName</code> annotations.
- </li>
- <li>April 22, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>Data from:<a href=\"http://productfinder.wilo.com/com/en/c0000002200012eb000020023/_0000001d000149e80001003a/product.html\"> http://productfinder.wilo.com/com/en/c0000002200012eb000020023/_0000001d000149e80001003a/product.html</a></p>
+<p>See <a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6\">AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 </a>for more information about how the data is derived. </p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Deleted angular speed parameters with the unit rpm.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+October 14, 2021, by Hongxiang Fu:<br/>
+Rewrote the statements using <code>use_powerCharacteristic</code>
+to support the implementation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+<code>AixLib.Fluid.Movers.BaseClasses.Euler</code></a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+June 01, 2017, by Iago Cupeiro:
+<br/>
+Changed data link to the English version
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+December 12, 2014, by Michael Wetter:<br/>
+Added <code>defaultComponentPrefixes</code> and
+<code>defaultComponentName</code> annotations.
+</li>
+<li>April 22, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VeroLine80slash115dash2comma2slash2;
diff --git a/AixLib/Fluid/Movers/Data/package.order b/AixLib/Fluid/Movers/Data/package.order
index 7bbde5448e..ebf620a7b7 100644
--- a/AixLib/Fluid/Movers/Data/package.order
+++ b/AixLib/Fluid/Movers/Data/package.order
@@ -1,2 +1,3 @@
 Generic
+Fans
 Pumps
diff --git a/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpConst.mo b/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpConst.mo
similarity index 97%
rename from AixLib/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpConst.mo
rename to AixLib/Fluid/Movers/DpControlledMovers/Examples/DpConst.mo
index 4b0c467c3b..170daa89ea 100644
--- a/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpConst.mo
+++ b/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpConst.mo
@@ -1,5 +1,5 @@
 within AixLib.Fluid.Movers.DpControlledMovers.Examples;
-model DpControlled_dpConst
+model DpConst
   extends Modelica.Icons.Example;
   package Medium = AixLib.Media.Water "Medium model";
 
@@ -68,9 +68,9 @@ equation
   connect(dpControlled_dp.P, integrator.u) annotation (Line(points={{1,9},{8,9},{8,70},{38,70}},   color={0,0,127}));
   connect(integrator.y, elEnergy) annotation (Line(points={{61,70},{110,70}}, color={0,0,127}));
   annotation (
-    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpConst.mos"
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpConst.mos"
         "Simulate and plot"),
     experiment(
       StopTime=3600,
       Tolerance=1e-06));
-end DpControlled_dpConst;
+end DpConst;
diff --git a/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpVar.mo b/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpVar.mo
deleted file mode 100644
index 22a74be94f..0000000000
--- a/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpVar.mo
+++ /dev/null
@@ -1,10 +0,0 @@
-within AixLib.Fluid.Movers.DpControlledMovers.Examples;
-model DpControlled_dpVar
-  extends DpControlled_dpConst(dpControlled_dp(ctrlType=AixLib.Fluid.Movers.DpControlledMovers.Types.CtrlType.dpVar));
-  annotation (
-    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpVar.mos"
-        "Simulate and plot"),
-    experiment(
-      StopTime=3600,
-      Tolerance=1e-06));
-end DpControlled_dpVar;
diff --git a/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpVar.mo b/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpVar.mo
new file mode 100644
index 0000000000..e9ba316b2b
--- /dev/null
+++ b/AixLib/Fluid/Movers/DpControlledMovers/Examples/DpVar.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.Movers.DpControlledMovers.Examples;
+model DpVar
+  extends DpConst(dpControlled_dp(ctrlType=AixLib.Fluid.Movers.DpControlledMovers.Types.CtrlType.dpVar));
+  annotation (
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpVar.mos"
+        "Simulate and plot"),
+    experiment(
+      StopTime=3600,
+      Tolerance=1e-06));
+end DpVar;
diff --git a/AixLib/Fluid/Movers/DpControlledMovers/Examples/package.order b/AixLib/Fluid/Movers/DpControlledMovers/Examples/package.order
index 380a5ad3d2..20a82b4711 100644
--- a/AixLib/Fluid/Movers/DpControlledMovers/Examples/package.order
+++ b/AixLib/Fluid/Movers/DpControlledMovers/Examples/package.order
@@ -1,2 +1,2 @@
-DpControlled_dpConst
-DpControlled_dpVar
+DpConst
+DpVar
diff --git a/AixLib/Fluid/Movers/Examples/ClosedLoop_y.mo b/AixLib/Fluid/Movers/Examples/ClosedLoop_y.mo
index 8e7777ede0..28dce230c8 100644
--- a/AixLib/Fluid/Movers/Examples/ClosedLoop_y.mo
+++ b/AixLib/Fluid/Movers/Examples/ClosedLoop_y.mo
@@ -21,7 +21,7 @@ model ClosedLoop_y "Flow machine with feedback control"
     p=101325,
     T=293.15,
     nPorts=2) annotation (Placement(transformation(extent={{-82,10},{-62,30}})));
-  FixedResistances.PressureDrop dp1(
+  AixLib.Fluid.FixedResistances.PressureDrop dp1(
     redeclare package Medium = Medium,
     m_flow_nominal=m_flow_nominal,
     dp_nominal=dp_nominal/2) "Pressure drop"
@@ -78,28 +78,28 @@ equation
     Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{160,
             160}})),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of a fan with closed loop control.
- The fan is controlled to track a required mass flow rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates the use of a fan with closed loop control.
+The fan is controlled to track a required mass flow rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/ClosedLoop_y.mos"
         "Simulate and plot"),
     experiment(
       StopTime=3600,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ClosedLoop_y;
diff --git a/AixLib/Fluid/Movers/Examples/Data/EnglanderNorford1992.mo b/AixLib/Fluid/Movers/Examples/Data/EnglanderNorford1992.mo
new file mode 100644
index 0000000000..60badb9ca2
--- /dev/null
+++ b/AixLib/Fluid/Movers/Examples/Data/EnglanderNorford1992.mo
@@ -0,0 +1,42 @@
+within AixLib.Fluid.Movers.Examples.Data;
+record EnglanderNorford1992 "Data for the supply fan in Englander and Norford (1992)"
+  extends AixLib.Fluid.Movers.Data.Generic(
+    etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+    power(V_flow={5.44049459041731, 8.71715610510046, 15.6826378155589,
+                  19.9484801648634, 22.5450798557444, 25.6362699639361,
+                  27.8619268418341, 29.8402885110767, 32.9314786192684,
+                   36.764554353426, 40.1648634724368, 42.9057187017001},
+          P={              18642.5,            22371,            29828,
+                         34652.679,            37285,         39149.25,
+                         39454.987,        38612.346,            37285,
+                         35912.912,        35308.895,        36002.396}),
+    pressure(V_flow={5.44049459041731, 8.71715610510046, 15.6826378155589,
+                     19.9484801648634, 22.5450798557444, 25.6362699639361,
+                     27.8619268418341, 29.8402885110767, 32.9314786192684,
+                      36.764554353426, 40.1648634724368, 42.9057187017001},
+             dp={    1430.48245810056, 1404.41681564246,  1332.4756424581,
+                      1280.3443575419,  1224.0425698324, 1128.12100558659,
+                     1034.28469273743, 909.169608938547,  702.72972067039,
+                     433.732290502792,  197.05625698324, 6.25575418994417}));
+  annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="per",
+Documentation(info="<html>
+<p>
+Performance data for the supply fan used in Englander and Norford (1992)
+(figure below). See the documentation of
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Fans.Greenheck\">
+AixLib.Fluid.Movers.Data.Fans.Greenheck</a>
+for the methods used to extract data.
+</p>
+<p align=\"center\">
+<img alt=\"Fan curve\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Examples/Supply.png\"/></p>
+<h4>References</h4>
+<p>
+Englander, S. L., and L. K. Norford. 
+\"Saving fan energy in VAV systems- part 1: analysis of a variable-speed-drive retrofit.\" 
+<i>ASHRAE Winter Meeting, Anaheim, CA, USA, 01/25-29/92.</i> 1992.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end EnglanderNorford1992;
diff --git a/AixLib/Fluid/Movers/Examples/Data/package.mo b/AixLib/Fluid/Movers/Examples/Data/package.mo
new file mode 100644
index 0000000000..b9d7f0dd03
--- /dev/null
+++ b/AixLib/Fluid/Movers/Examples/Data/package.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.Movers.Examples;
+package Data "Package containing data for examples"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains data that are exclusively useful for the example models.
+</p>
+</html>"));
+end Data;
diff --git a/AixLib/Fluid/Movers/Examples/Data/package.order b/AixLib/Fluid/Movers/Examples/Data/package.order
new file mode 100644
index 0000000000..c0d5a91c43
--- /dev/null
+++ b/AixLib/Fluid/Movers/Examples/Data/package.order
@@ -0,0 +1 @@
+EnglanderNorford1992
diff --git a/AixLib/Fluid/Movers/Examples/MoverContinuous.mo b/AixLib/Fluid/Movers/Examples/MoverContinuous.mo
index f5028e48dd..951268d923 100644
--- a/AixLib/Fluid/Movers/Examples/MoverContinuous.mo
+++ b/AixLib/Fluid/Movers/Examples/MoverContinuous.mo
@@ -2,51 +2,50 @@ within AixLib.Fluid.Movers.Examples;
 model MoverContinuous
   "Example model of movers using a real input for setting the stage"
   extends MoverParameter(
-    pump_Nrpm(inputType=AixLib.Fluid.Types.InputType.Continuous),
     pump_m_flow(inputType=AixLib.Fluid.Types.InputType.Continuous),
     pump_y(inputType=AixLib.Fluid.Types.InputType.Continuous),
     pump_dp(inputType=AixLib.Fluid.Types.InputType.Continuous));
   Modelica.Blocks.Sources.Ramp ramp(duration=1) "Ramp input for all movers"
     annotation (Placement(transformation(extent={{-80,60},{-60,80}})));
-  Modelica.Blocks.Math.Gain gaiNrpm(k=2000) "Nominal rpm"
-    annotation (Placement(transformation(extent={{-40,60},{-20,80}})));
   Modelica.Blocks.Math.Gain gai_m_flow(k=m_flow_nominal)
     "Nominal mass flow rate"
     annotation (Placement(transformation(extent={{-40,10},{-20,30}})));
   Modelica.Blocks.Math.Gain gai_dp(k=dp_nominal) "Nominal pressure drop"
     annotation (Placement(transformation(extent={{-40,-70},{-20,-50}})));
 equation
-  connect(gaiNrpm.y, pump_Nrpm.Nrpm)
-    annotation (Line(points={{-19,70},{0,70},{0,52}}, color={0,0,127}));
   connect(gai_dp.y, pump_dp.dp_in) annotation (Line(points={{-19,-60},{-10,-60},
-          {-0.2,-60},{-0.2,-68}}, color={0,0,127}));
+          {0,-60},{0,-68}},       color={0,0,127}));
   connect(gai_m_flow.y, pump_m_flow.m_flow_in)
-    annotation (Line(points={{-19,20},{-0.2,20},{-0.2,12}}, color={0,0,127}));
-  connect(gaiNrpm.u, ramp.y)
-    annotation (Line(points={{-42,70},{-59,70}}, color={0,0,127}));
+    annotation (Line(points={{-19,20},{0,20},{0,12}},       color={0,0,127}));
   connect(gai_m_flow.u, ramp.y) annotation (Line(points={{-42,20},{-50,20},{-50,
           70},{-59,70}}, color={0,0,127}));
   connect(gai_dp.u, ramp.y) annotation (Line(points={{-42,-60},{-50,-60},{-50,
           70},{-59,70}}, color={0,0,127}));
-  connect(pump_y.y, ramp.y) annotation (Line(points={{-0.2,-28},{-0.2,-20},{-50,
-          -20},{-50,70},{-59,70}}, color={0,0,127}));
+  connect(pump_y.y, ramp.y) annotation (Line(points={{0,-28},{0,-20},{-50,-20},{
+          -50,70},{-59,70}},       color={0,0,127}));
   annotation (
     Documentation(info="<html>
- <p>
- This example demonstrates the use of a <code>RealInput</code>
- connector for a mover model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 24, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example demonstrates the use of a <code>RealInput</code>
+connector for a mover model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Deleted the mover with <code>Nrpm</code> signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+August 24, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 experiment(Tolerance=1e-06, StopTime=1),
 __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverContinuous.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MoverContinuous;
diff --git a/AixLib/Fluid/Movers/Examples/MoverParameter.mo b/AixLib/Fluid/Movers/Examples/MoverParameter.mo
index 64a1beca6b..1169969887 100644
--- a/AixLib/Fluid/Movers/Examples/MoverParameter.mo
+++ b/AixLib/Fluid/Movers/Examples/MoverParameter.mo
@@ -7,8 +7,9 @@ model MoverParameter
   parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=2
     "Nominal mass flow rate";
 
-  FlowControlled_m_flow pump_m_flow(
+  AixLib.Fluid.Movers.FlowControlled_m_flow pump_m_flow(
     redeclare package Medium = Medium,
+    nominalValuesDefineDefaultPressureCurve=true,
     m_flow_nominal=m_flow_nominal,
     use_inputFilter=false,
     massFlowRates={0,0.5,1}*m_flow_nominal,
@@ -19,22 +20,22 @@ model MoverParameter
 
   AixLib.Fluid.Sources.Boundary_pT sou(
     redeclare package Medium = Medium,
-    nPorts=4) "Fluid source"
+    nPorts=3) "Fluid source"
               annotation (Placement(transformation(extent={{-80,-10},{-60,10}})));
 
   AixLib.Fluid.Sources.Boundary_pT sin(redeclare package Medium = Medium,
-      nPorts=4) "Fluid sink"
+      nPorts=3) "Fluid sink"
     annotation (Placement(transformation(extent={{80,-10},{60,10}})));
-  SpeedControlled_y pump_y(
+  AixLib.Fluid.Movers.SpeedControlled_y pump_y(
     redeclare package Medium = Medium,
     redeclare AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to4 per(
-        speeds_rpm=1800*{0,0.5,1}, constantSpeed_rpm=1800),
+        speeds={0,0.5,1}, constantSpeed=1),
     use_inputFilter=false,
     inputType=AixLib.Fluid.Types.InputType.Constant,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
     "Pump with normalised speed input"
     annotation (Placement(transformation(extent={{-10,-50},{10,-30}})));
-  FlowControlled_dp pump_dp(
+  AixLib.Fluid.Movers.FlowControlled_dp pump_dp(
     redeclare package Medium = Medium,
     m_flow_nominal=m_flow_nominal,
     redeclare AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to4 per,
@@ -45,74 +46,78 @@ model MoverParameter
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
     "Pump with pressure head input"
     annotation (Placement(transformation(extent={{-10,-90},{10,-70}})));
-  FixedResistances.PressureDrop res(
+  AixLib.Fluid.FixedResistances.PressureDrop res(
     redeclare package Medium = Medium,
     m_flow_nominal=m_flow_nominal,
     dp_nominal=dp_nominal)
     "Pressure drop component for avoiding singular system"
     annotation (Placement(transformation(extent={{26,-90},{46,-70}})));
-  SpeedControlled_Nrpm pump_Nrpm(
-    redeclare package Medium = Medium,
-    use_inputFilter=false,
-    redeclare AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to4 per(
-        speeds_rpm={0,1000,2000}, constantSpeed_rpm=2000),
-    inputType=AixLib.Fluid.Types.InputType.Constant,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
-    "Pump with speed input"
-    annotation (Placement(transformation(extent={{-10,30},{10,50}})));
   parameter Modelica.Units.SI.PressureDifference dp_nominal=10000
     "Nominal pressure raise";
 equation
   connect(sou.ports[1], pump_m_flow.port_a) annotation (Line(
-      points={{-60,3},{-60,0},{-10,0}},
+      points={{-60,-1.33333},{-60,0},{-10,0}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(pump_m_flow.port_b, sin.ports[1]) annotation (Line(
-      points={{10,0},{60,0},{60,3}},
+      points={{10,0},{60,0},{60,-1.33333}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(res.port_a, pump_dp.port_b)
     annotation (Line(points={{26,-80},{18,-80},{10,-80}}, color={0,127,255}));
   connect(pump_y.port_b, sin.ports[2])
-    annotation (Line(points={{10,-40},{60,-40},{60,1}}, color={0,127,255}));
+    annotation (Line(points={{10,-40},{60,-40},{60,2.22045e-16}},
+                                                        color={0,127,255}));
   connect(res.port_b, sin.ports[3])
-    annotation (Line(points={{46,-80},{60,-80},{60,-1}}, color={0,127,255}));
+    annotation (Line(points={{46,-80},{60,-80},{60,1.33333}},
+                                                         color={0,127,255}));
   connect(pump_dp.port_a, sou.ports[2])
-    annotation (Line(points={{-10,-80},{-60,-80},{-60,1}}, color={0,127,255}));
+    annotation (Line(points={{-10,-80},{-60,-80},{-60,2.22045e-16}},
+                                                           color={0,127,255}));
   connect(pump_y.port_a, sou.ports[3]) annotation (Line(points={{-10,-40},{-20,-40},
-          {-60,-40},{-60,-1}}, color={0,127,255}));
-  connect(sou.ports[4], pump_Nrpm.port_a) annotation (Line(points={{-60,-3},{-60,
-          -3},{-60,34},{-60,40},{-10,40}}, color={0,127,255}));
-  connect(pump_Nrpm.port_b, sin.ports[4]) annotation (Line(points={{10,40},{24,40},
-          {60,40},{60,-3}}, color={0,127,255}));
+          {-60,-40},{-60,1.33333}},
+                               color={0,127,255}));
   annotation (
     __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverParameter.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of a <code>Parameter</code>
- set point for a mover model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- August 24, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    experiment(Tolerance=1e-06, StopTime=1),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of a <code>Parameter</code>
+set point for a mover model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 8, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Deleted the mover with <code>Nrpm</code> signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+August 24, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-06, StopTime=1), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MoverParameter;
diff --git a/AixLib/Fluid/Movers/Examples/MoverStages.mo b/AixLib/Fluid/Movers/Examples/MoverStages.mo
index a62d4e5671..149496c7ff 100644
--- a/AixLib/Fluid/Movers/Examples/MoverStages.mo
+++ b/AixLib/Fluid/Movers/Examples/MoverStages.mo
@@ -2,7 +2,6 @@ within AixLib.Fluid.Movers.Examples;
 model MoverStages
   "Example model of movers using an integer input for setting the stage"
   extends AixLib.Fluid.Movers.Examples.MoverParameter(
-    pump_Nrpm(inputType=AixLib.Fluid.Types.InputType.Stages),
     pump_m_flow(inputType=AixLib.Fluid.Types.InputType.Stages),
     pump_y(inputType=AixLib.Fluid.Types.InputType.Stages),
     pump_dp(inputType=AixLib.Fluid.Types.InputType.Stages));
@@ -17,8 +16,6 @@ model MoverStages
   parameter Modelica.Units.SI.PressureDifference dp_nominal=10000
     "Nominal pressure raise";
 equation
-  connect(integerTable.y, pump_Nrpm.stage)
-    annotation (Line(points={{-39,80},{0,80},{0,52}}, color={255,127,0}));
   connect(integerTable.y, pump_m_flow.stage)
     annotation (Line(points={{-39,80},{-30,80},{-30,20},{-30,20},{-30,20},{0,20},
           {0,12}},                                    color={255,127,0}));
@@ -33,30 +30,36 @@ equation
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverStages.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the <code>Integer</code>
- stage connector for a mover model.
- Note that integer input <i>1</i> refers to the first stage, whereas
- input <i>0</i> switches the mover off.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- August 24, 2015, by Filip Jorissen:<br/>
- Extended implementation with more movers.
- </li>
- <li>
- April 2, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    experiment(Tolerance=1e-06, StopTime=1),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the <code>Integer</code>
+stage connector for a mover model.
+Note that integer input <i>1</i> refers to the first stage, whereas
+input <i>0</i> switches the mover off.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Deleted the mover with <code>Nrpm</code> signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+August 24, 2015, by Filip Jorissen:<br/>
+Extended implementation with more movers.
+</li>
+<li>
+April 2, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-06, StopTime=1), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MoverStages;
diff --git a/AixLib/Fluid/Movers/Examples/PumpsParallel.mo b/AixLib/Fluid/Movers/Examples/PumpsParallel.mo
index 48965fb194..3112d2721f 100644
--- a/AixLib/Fluid/Movers/Examples/PumpsParallel.mo
+++ b/AixLib/Fluid/Movers/Examples/PumpsParallel.mo
@@ -116,39 +116,39 @@ equation
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/PumpsParallel.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This example tests the configuration of two flow machines that are installed in parallel.
- Both flow machines start with full speed.
- At <i>t=150</i> second, the speed of the flow machine on the top is reduced to zero.
- As its speed is reduced, the mass flow rate changes its direction in such a way that the flow machine
- at the top has reverse flow.
- </html>",revisions="<html>
- <ul>
- <li>February 20, 2016, by Ruben Baetens:<br/>
- Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
- </li>
- <li>
- April 2, 2015, by Filip Jorissen:<br/>
- Set constant speed for pump using a <code>parameter</code>
- instead of a <code>realInput</code>.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>,
- and set <code>rho_nominal</code> to a constant to avoid a non-literal
- nominal value for <code>V_flow_max</code> and <code>VMachine_flow</code>.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+This example tests the configuration of two flow machines that are installed in parallel.
+Both flow machines start with full speed.
+At <i>t=150</i> second, the speed of the flow machine on the top is reduced to zero.
+As its speed is reduced, the mass flow rate changes its direction in such a way that the flow machine
+at the top has reverse flow.
+</html>", revisions="<html>
+<ul>
+<li>February 20, 2016, by Ruben Baetens:<br/>
+Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
+</li>
+<li>
+April 2, 2015, by Filip Jorissen:<br/>
+Set constant speed for pump using a <code>parameter</code>
+instead of a <code>realInput</code>.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>,
+and set <code>rho_nominal</code> to a constant to avoid a non-literal
+nominal value for <code>V_flow_max</code> and <code>VMachine_flow</code>.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=300,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PumpsParallel;
diff --git a/AixLib/Fluid/Movers/Examples/PumpsSeries.mo b/AixLib/Fluid/Movers/Examples/PumpsSeries.mo
index 485413ef62..c7cc4b778d 100644
--- a/AixLib/Fluid/Movers/Examples/PumpsSeries.mo
+++ b/AixLib/Fluid/Movers/Examples/PumpsSeries.mo
@@ -65,35 +65,35 @@ equation
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/PumpsSeries.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This example tests the configuration of two flow machines that are installed in series.
- Both flow machines start with full speed.
- At <i>t=150</i> seconds, the speed of the flow machine on the left is reduced to zero.
- As its speed is reduced, the mass flow rate is reduced. Note that even at zero input, the mass flow rate is non-zero,
- but the pressure drop of the pump <code>floMac1.dp</code> is positive, which means that this pump has a flow resistance.
- However, <code>flowMac2.dp</code> is always negative, as this pump has a constant control input of 1.
- </html>",revisions="<html>
- <ul>
- <li>
- April 2, 2015, by Filip Jorissen:<br/>
- Set constant speed for pump using a <code>parameter</code>
- instead of a <code>realInput</code>.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+This example tests the configuration of two flow machines that are installed in series.
+Both flow machines start with full speed.
+At <i>t=150</i> seconds, the speed of the flow machine on the left is reduced to zero.
+As its speed is reduced, the mass flow rate is reduced. Note that even at zero input, the mass flow rate is non-zero,
+but the pressure drop of the pump <code>floMac1.dp</code> is positive, which means that this pump has a flow resistance.
+However, <code>flowMac2.dp</code> is always negative, as this pump has a constant control input of 1.
+</html>", revisions="<html>
+<ul>
+<li>
+April 2, 2015, by Filip Jorissen:<br/>
+Set constant speed for pump using a <code>parameter</code>
+instead of a <code>realInput</code>.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=300,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PumpsSeries;
diff --git a/AixLib/Fluid/Movers/Examples/SpeedControlled_y_pumpCurves.mo b/AixLib/Fluid/Movers/Examples/SpeedControlled_y_pumpCurves.mo
index ebea5f6ab5..990c025aee 100644
--- a/AixLib/Fluid/Movers/Examples/SpeedControlled_y_pumpCurves.mo
+++ b/AixLib/Fluid/Movers/Examples/SpeedControlled_y_pumpCurves.mo
@@ -162,41 +162,41 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/SpeedControlled_y_pumpCurves.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example demonstrates how the pump curves changes for different (constant) input
- signal <code>y</code>.
- If <code>y &ge; delta = 0.05</code>, the pump curves are polynomials.
- For <code>y &lt; delta = 0.05</code>, the pump curves convert to linear functions to
- avoid a singularity at the origin.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 2, 2016, by Michael Wetter:<br/>
- Changed the valve opening signal to not take on zero as otherwise <code>pum.port_a.p</code>
- is negative, violating the <code>min</code> attribute on the pressure variable.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
- </li>
- <li>
- March 11, 2016, by Michael Wetter:<br/>
- Reformulated model for OpenModelica.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- June 14, 2015, by Filip Jorissen:<br/>
- Set constant speed for pump using a <code>parameter</code>
- instead of a <code>realInput</code>.
- </li>
- <li>March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates how the pump curves changes for different (constant) input
+signal <code>y</code>.
+If <code>y &ge; delta = 0.05</code>, the pump curves are polynomials.
+For <code>y &lt; delta = 0.05</code>, the pump curves convert to linear functions to
+avoid a singularity at the origin.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 2, 2016, by Michael Wetter:<br/>
+Changed the valve opening signal to not take on zero as otherwise <code>pum.port_a.p</code>
+is negative, violating the <code>min</code> attribute on the pressure variable.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
+</li>
+<li>
+March 11, 2016, by Michael Wetter:<br/>
+Reformulated model for OpenModelica.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+June 14, 2015, by Filip Jorissen:<br/>
+Set constant speed for pump using a <code>parameter</code>
+instead of a <code>realInput</code>.
+</li>
+<li>March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpeedControlled_y_pumpCurves;
diff --git a/AixLib/Fluid/Movers/Examples/StaticReset.mo b/AixLib/Fluid/Movers/Examples/StaticReset.mo
new file mode 100644
index 0000000000..ec7357d447
--- /dev/null
+++ b/AixLib/Fluid/Movers/Examples/StaticReset.mo
@@ -0,0 +1,335 @@
+within AixLib.Fluid.Movers.Examples;
+model StaticReset
+  "Comparing different computation paths with a static pressure reset"
+  extends Modelica.Icons.Example;
+
+  package Medium = AixLib.Media.Air;
+
+  // Fans and their performance records
+  AixLib.Fluid.Movers.SpeedControlled_y fan1(
+    redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    redeclare AixLib.Fluid.Movers.Examples.Data.EnglanderNorford1992 per(
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate,
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided))
+    "Fan using power curves"
+    annotation (Placement(transformation(extent={{-10,170},{10,190}})));
+  AixLib.Fluid.Movers.SpeedControlled_y fan2(
+    redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    per(
+      powerOrEfficiencyIsHydraulic=fan1.per.powerOrEfficiencyIsHydraulic,
+      pressure=fan1.per.pressure,
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber,
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided,
+      peak(
+        V_flow=23.022856,
+        dp=1211.1604,
+        eta=0.74030644)))
+    "Fan using the Euler number"
+    annotation (Placement(transformation(extent={{-10,70},{10,90}})));
+  AixLib.Fluid.Movers.SpeedControlled_y fan3(
+    redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    per(
+      powerOrEfficiencyIsHydraulic=fan1.per.powerOrEfficiencyIsHydraulic,
+      pressure=fan1.per.pressure,
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate,
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided,
+      efficiency(eta={0.7}))) "Fan using constant efficiency"
+    annotation (Placement(transformation(extent={{-10,-30},{10,-10}})));
+
+  // Define the system curve
+  parameter Modelica.Units.SI.VolumeFlowRate V_flow_nominal=21.8
+    "Nominal volumetric flow rate of the system";
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=V_flow_nominal/1.2
+    "Nominal mass flow rate of the system";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal=1244.2
+    "Nominal pressure rise of the system";
+
+  // Boundaries
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p=101325,
+    T=293.15,
+    nPorts=6) "Boundary"
+    annotation (Placement(transformation(extent={{-100,-90},{-80,-70}})));
+  AixLib.Fluid.Sources.Boundary_pT sin(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p=101325,
+    T=293.15,
+    nPorts=3) "Boundary"
+    annotation (Placement(transformation(extent={{160,-90},{140,-70}})));
+
+  // Duct pressure drops
+  AixLib.Fluid.FixedResistances.PressureDrop dp11(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dp_nominal=dp_nominal/3)
+    "Duct pressure drop before the static pressure measurement point"
+    annotation (Placement(transformation(extent={{20,170},{40,190}})));
+  AixLib.Fluid.FixedResistances.PressureDrop dp12(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dp_nominal=dp_nominal/3)
+    "Duct pressure drop after the static pressure measurement point"
+    annotation (Placement(transformation(extent={{60,170},{80,190}})));
+  AixLib.Fluid.FixedResistances.PressureDrop dp21(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dp_nominal=dp_nominal/3)
+    "Duct pressure drop before the static pressure measurement point"
+    annotation (Placement(transformation(extent={{20,70},{40,90}})));
+  AixLib.Fluid.FixedResistances.PressureDrop dp22(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dp_nominal=dp_nominal/3)
+    "Duct pressure drop after the static pressure measurement point"
+    annotation (Placement(transformation(extent={{60,70},{80,90}})));
+  AixLib.Fluid.FixedResistances.PressureDrop dp31(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dp_nominal=dp_nominal/3)
+    "Duct pressure drop before the static pressure measurement point"
+    annotation (Placement(transformation(extent={{20,-30},{40,-10}})));
+  AixLib.Fluid.FixedResistances.PressureDrop dp32(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dp_nominal=dp_nominal/3)
+    "Duct pressure drop after the static pressure measurement point"
+    annotation (Placement(transformation(extent={{60,-30},{80,-10}})));
+
+  // PI controllers and components
+  AixLib.Fluid.Sensors.RelativePressure pDucSta1(
+    redeclare package Medium = Medium)
+    "Duct static pressure"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=180,
+        origin={-50,152})));
+  AixLib.Fluid.Sensors.RelativePressure pDucSta2(
+    redeclare package Medium = Medium)
+    "Duct static pressure"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=180,
+        origin={-50,50})));
+  AixLib.Fluid.Sensors.RelativePressure pDucSta3(
+    redeclare package Medium = Medium)
+    "Duct static pressure"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=180,
+        origin={-50,-50})));
+  AixLib.Controls.Continuous.LimPID conPID1(
+    Td=1,
+    k=0.5,
+    Ti=15) "PI controller"
+    annotation (Placement(transformation(extent={{-60,200},{-40,220}})));
+  AixLib.Controls.Continuous.LimPID conPID2(
+    Td=1,
+    k=0.5,
+    Ti=15) "PI controller"
+    annotation (Placement(transformation(extent={{-60,100},{-40,120}})));
+  AixLib.Controls.Continuous.LimPID conPID3(
+    Td=1,
+    k=0.5,
+    Ti=15) "PI controller"
+    annotation (Placement(transformation(extent={{-60,0},{-40,20}})));
+  Modelica.Blocks.Math.Gain gai1(k=2/dp_nominal) "Gain"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-50,180})));
+  Modelica.Blocks.Math.Gain gai2(k=2/dp_nominal) "Gain"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-50,78})));
+  Modelica.Blocks.Math.Gain gai3(k=2/dp_nominal) "Gain"
+    annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-50,-22})));
+  Modelica.Blocks.Sources.Constant y(k=1)
+    "Duct static pressure setpoint (normalised)"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-90,220})));
+
+  // VAV boxes
+  Actuators.Dampers.Exponential damExp1(
+    redeclare final package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dpDamper_nominal=dp_nominal/3,
+    y_start=0) "Damper representing a VAV box"
+    annotation (Placement(transformation(extent={{100,170},{120,190}})));
+  Actuators.Dampers.Exponential damExp2(
+    redeclare final package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dpDamper_nominal=dp_nominal/3,
+    y_start=0) "Damper representing a VAV box"
+    annotation (Placement(transformation(extent={{100,70},{120,90}})));
+  Actuators.Dampers.Exponential damExp3(
+    redeclare final package Medium = Medium,
+    m_flow_nominal=m_flow_nominal,
+    dpDamper_nominal=dp_nominal/3,
+    y_start=0) "Damper representing a VAV box"
+    annotation (Placement(transformation(extent={{100,-30},{120,-10}})));
+  Modelica.Blocks.Sources.Ramp yDam(
+    height=1,
+    duration=3600,
+    offset=0) "Ramp input for damper position"
+    annotation (Placement(transformation(extent={{60,200},{80,220}})));
+
+equation
+  connect(y.y, conPID3.u_s) annotation (Line(points={{-79,220},{-68,220},{-68,10},
+          {-62,10}}, color={0,0,127}));
+  connect(pDucSta3.p_rel, gai3.u)
+    annotation (Line(points={{-50,-41},{-50,-34}}, color={0,0,127}));
+  connect(gai3.y, conPID3.u_m)
+    annotation (Line(points={{-50,-11},{-50,-2}}, color={0,0,127}));
+  connect(conPID3.y, fan3.y)
+    annotation (Line(points={{-39,10},{0,10},{0,-8}}, color={0,0,127}));
+  connect(fan3.port_b, dp31.port_a)
+    annotation (Line(points={{10,-20},{20,-20}}, color={0,127,255}));
+  connect(dp31.port_b, dp32.port_a)
+    annotation (Line(points={{40,-20},{60,-20}}, color={0,127,255}));
+  connect(fan2.port_b, dp21.port_a)
+    annotation (Line(points={{10,80},{20,80}}, color={0,127,255}));
+  connect(dp21.port_b, dp22.port_a)
+    annotation (Line(points={{40,80},{60,80}}, color={0,127,255}));
+  connect(pDucSta2.p_rel, gai2.u)
+    annotation (Line(points={{-50,59},{-50,66}}, color={0,0,127}));
+  connect(gai2.y, conPID2.u_m)
+    annotation (Line(points={{-50,89},{-50,98}}, color={0,0,127}));
+  connect(pDucSta2.port_a, dp22.port_a) annotation (Line(
+      points={{-40,50},{60,50},{60,80}},
+      color={0,127,255},
+      pattern=LinePattern.Dot));
+  connect(y.y, conPID2.u_s) annotation (Line(points={{-79,220},{-68,220},{-68,110},
+          {-62,110}}, color={0,0,127}));
+  connect(conPID2.y, fan2.y)
+    annotation (Line(points={{-39,110},{0,110},{0,92}}, color={0,0,127}));
+  connect(fan1.port_b, dp11.port_a)
+    annotation (Line(points={{10,180},{20,180}}, color={0,127,255}));
+  connect(dp11.port_b, dp12.port_a)
+    annotation (Line(points={{40,180},{60,180}}, color={0,127,255}));
+  connect(pDucSta1.p_rel,gai1. u)
+    annotation (Line(points={{-50,161},{-50,168}},
+                                                 color={0,0,127}));
+  connect(gai1.y,conPID1. u_m)
+    annotation (Line(points={{-50,191},{-50,198}},
+                                                 color={0,0,127}));
+  connect(y.y, conPID1.u_s) annotation (Line(points={{-79,220},{-68,220},{-68,
+          210},{-62,210}},
+                      color={0,0,127}));
+  connect(pDucSta1.port_a, dp12.port_a) annotation (Line(
+      points={{-40,152},{60,152},{60,180}},
+      color={0,127,255},
+      pattern=LinePattern.Dot));
+  connect(conPID1.y, fan1.y)
+    annotation (Line(points={{-39,210},{0,210},{0,192}}, color={0,0,127}));
+  connect(pDucSta3.port_a, dp32.port_a) annotation (Line(
+      points={{-40,-50},{60,-50},{60,-20}},
+      color={0,127,255},
+      pattern=LinePattern.Dot));
+  connect(fan3.port_a, sou.ports[1]) annotation (Line(points={{-10,-20},{-18,
+          -20},{-18,-81.6667},{-80,-81.6667}},
+                                          color={0,127,255}));
+  connect(fan2.port_a, sou.ports[2]) annotation (Line(points={{-10,80},{-18,80},
+          {-18,-81},{-80,-81}}, color={0,127,255}));
+  connect(fan1.port_a, sou.ports[3]) annotation (Line(points={{-10,180},{-18,
+          180},{-18,-80.3333},{-80,-80.3333}},
+                                          color={0,127,255}));
+  connect(pDucSta3.port_b, sou.ports[4]) annotation (Line(
+      points={{-60,-50},{-78,-50},{-78,-79.6667},{-80,-79.6667}},
+      color={0,127,255},
+      pattern=LinePattern.Dot));
+  connect(pDucSta2.port_b, sou.ports[5]) annotation (Line(
+      points={{-60,50},{-78,50},{-78,-79},{-80,-79}},
+      color={0,127,255},
+      pattern=LinePattern.Dot));
+  connect(pDucSta1.port_b, sou.ports[6]) annotation (Line(
+      points={{-60,152},{-78,152},{-78,-78},{-80,-78},{-80,-78.3333}},
+      color={0,127,255},
+      pattern=LinePattern.Dot));
+  connect(dp12.port_b, damExp1.port_a)
+    annotation (Line(points={{80,180},{100,180}}, color={0,127,255}));
+  connect(damExp1.port_b, sin.ports[1]) annotation (Line(points={{120,180},{134,
+          180},{134,-81.3333},{140,-81.3333}}, color={0,127,255}));
+  connect(yDam.y, damExp1.y)
+    annotation (Line(points={{81,210},{92,210},{92,202},{110,202},{110,192}},
+                                                            color={0,0,127}));
+  connect(dp22.port_b,damExp2. port_a)
+    annotation (Line(points={{80,80},{100,80}}, color={0,127,255}));
+  connect(damExp2.port_b, sin.ports[2]) annotation (Line(points={{120,80},{134,80},
+          {134,-80},{140,-80}}, color={0,127,255}));
+  connect(dp32.port_b,damExp3. port_a)
+    annotation (Line(points={{80,-20},{100,-20}}, color={0,127,255}));
+  connect(damExp3.port_b, sin.ports[3]) annotation (Line(points={{120,-20},{134,
+          -20},{134,-78.6667},{140,-78.6667}}, color={0,127,255}));
+  connect(yDam.y, damExp2.y) annotation (Line(points={{81,210},{92,210},{92,100},
+          {110,100},{110,92}},                     color={0,0,127}));
+  connect(yDam.y, damExp3.y) annotation (Line(points={{81,210},{92,210},{92,0},
+          {110,0},{110,-8}},                   color={0,0,127}));
+  annotation (
+    Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{160,
+            240}})),
+    Documentation(info="<html>
+<p>
+This example model compares the three power computation methods in a scenario
+where the fan performance (<i>P</i> vs. <i>V&#775;</i>) is examined
+to verify savings of a static pressure reset. The fan speed is controlled
+to track the duct static pressure at a point downstream while the damper
+(representing a VAV box) moves from fully closed to fully open.
+The system was described in Englander and Norford (1992).
+The fan data are implemented in
+<a href=\"Modelica://AixLib.Fluid.Movers.Examples.Data.EnglanderNorford1992\">
+AixLib.Fluid.Movers.Examples.Data.EnglanderNorford1992</a>.
+</p>
+<ul>
+<li>
+The first fan uses the fan curve to estimate the shaft power at reduced speed.
+</li>
+<li>
+The second fan uses the Euler number and its correlation to estimate
+the hydraulic efficiency.
+</li>
+<li>
+The third fan assumes a constant hydraulic efficiency.
+</li>
+</ul>
+<p>
+In the results, <i>P</i> computed from the Euler number and from the power curve
+agree on the trend of <i>P</i> vs. <i>V&#775;</i>. Both of them are also able
+to prevent <i>P</i> from incorrectly going to zero as <i>V&#775;</i> approaches
+zero, which the method with constant efficiency failed.
+</p>
+<h4>References</h4>
+<p>
+Englander, S. L., and L. K. Norford.
+\"Saving fan energy in VAV systems- part 1: analysis of a variable-speed-drive retrofit.\"
+<i>ASHRAE Winter Meeting, Anaheim, CA, USA, 01/25-29/92.</i> 1992.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 24, 2022, by Hongxiang Fu and David Blum:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/StaticReset.mos"
+        "Simulate and plot"),
+    experiment(
+      StopTime=3600,
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end StaticReset;
diff --git a/AixLib/Fluid/Movers/Examples/package.order b/AixLib/Fluid/Movers/Examples/package.order
index efb6874d3d..85e40ce061 100644
--- a/AixLib/Fluid/Movers/Examples/package.order
+++ b/AixLib/Fluid/Movers/Examples/package.order
@@ -5,3 +5,5 @@ MoverStages
 PumpsParallel
 PumpsSeries
 SpeedControlled_y_pumpCurves
+StaticReset
+Data
diff --git a/AixLib/Fluid/Movers/FlowControlled_dp.mo b/AixLib/Fluid/Movers/FlowControlled_dp.mo
index fcb8254f2a..3f270c0fb0 100644
--- a/AixLib/Fluid/Movers/FlowControlled_dp.mo
+++ b/AixLib/Fluid/Movers/FlowControlled_dp.mo
@@ -7,6 +7,7 @@ model FlowControlled_dp
     preSou(dp_start=dp_start, control_dp= not prescribeSystemPressure),
     final stageInputs(each final unit="Pa") = heads,
     final constInput(final unit="Pa") = constantHead,
+    final _m_flow_nominal = m_flow_nominal,
     filter(
       final y_start=dp_start,
       u(final unit="Pa"),
@@ -15,13 +16,29 @@ model FlowControlled_dp
       u_nominal=dp_nominal),
     eff(
       per(
-        final pressure = if per.havePressureCurve then
-          per.pressure
-        else
-          AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters(
-            V_flow = {i/(nOri-1)*2.0*m_flow_nominal/rho_default for i in 0:(nOri-1)},
-            dp =     {i/(nOri-1)*2.0*dp_nominal for i in (nOri-1):-1:0}),
-      final use_powerCharacteristic = if per.havePressureCurve then per.use_powerCharacteristic else false),
+        final pressure=
+          if per.havePressureCurve then
+            per.pressure
+          else
+            AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters(
+              V_flow = {i/(nOri-1)*2.0*m_flow_nominal/rho_default for i in 0:(nOri-1)},
+              dp =     {i/(nOri-1)*2.0*dp_nominal for i in (nOri-1):-1:0}),
+        final etaHydMet=
+          if (per.etaHydMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate
+            or per.etaHydMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber)
+            and not per.havePressureCurve then
+              AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.NotProvided
+          else per.etaHydMet,
+        final etaMotMet=
+          if (per.etaMotMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio
+            or per.etaMotMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve)
+            and (not per.haveWMot_nominal and not per.havePressureCurve) then
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided
+          else per.etaMotMet),
       r_N(start=if abs(dp_nominal) > 1E-8 then dp_start/dp_nominal else 0)));
 
   parameter Modelica.Units.SI.PressureDifference dp_start(
@@ -29,12 +46,16 @@ model FlowControlled_dp
     displayUnit="Pa") = 0 "Initial value of pressure raise"
     annotation (Dialog(tab="Dynamics", group="Filtered speed"));
 
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal(
+    final min=Modelica.Constants.small)
+    "Nominal mass flow rate" annotation (Dialog(group="Nominal condition"));
+
   // For air, we set dp_nominal = 600 as default, for water we set 10000
   parameter Modelica.Units.SI.PressureDifference dp_nominal(
-    min=0,
+    final min=Modelica.Constants.small,
     displayUnit="Pa") = if rho_default < 500 then 500 else 10000 "Nominal pressure raise, used to normalized the filter if use_inputFilter=true,
-         to set default values of constantHead and heads, and
-         and for default pressure curve if not specified in record per"
+        to set default values of constantHead and heads, and
+        and for default pressure curve if not specified in record per"
     annotation (Dialog(group="Nominal condition"));
 
   parameter Modelica.Units.SI.PressureDifference constantHead(
@@ -56,7 +77,7 @@ model FlowControlled_dp
 
   Modelica.Blocks.Interfaces.RealInput dpMea(
     final quantity="PressureDifference",
-    final displayUnit="Pa",
+    displayUnit="Pa",
     final unit="Pa")=gain.u if prescribeSystemPressure
     "Measurement of pressure difference between two points where the set point should be obtained"
     annotation (Placement(transformation(
@@ -65,7 +86,7 @@ model FlowControlled_dp
         origin={-80,120})));
 
   Modelica.Blocks.Interfaces.RealInput dp_in(final unit="Pa")
- if inputType == AixLib.Fluid.Types.InputType.Continuous
+    if inputType == AixLib.Fluid.Types.InputType.Continuous
     "Prescribed pressure rise"
     annotation (Placement(transformation(
         extent={{-20,-20},{20,20}},
@@ -119,167 +140,179 @@ equation
           textColor={0,0,127},
           visible=inputType == AixLib.Fluid.Types.InputType.Continuous or inputType == AixLib.Fluid.Types.InputType.Stages,
           textString=DynamicSelect("dp", if inputType == AixLib.Fluid.Types.InputType.Continuous then String(dp_in, format=".0f") else String(stage)))}),
-  defaultComponentName="fan",
+  defaultComponentName="mov",
   Documentation(info="<html>
- <p>
- This model describes a fan or pump with prescribed head.
- The input connector provides the difference between
- outlet minus inlet pressure.
- The efficiency of the device is computed based
- on the efficiency and pressure curves that are defined
- in record <code>per</code>, which is of type
- <a href=\"modelica://AixLib.Fluid.Movers.SpeedControlled_Nrpm\">
- AixLib.Fluid.Movers.SpeedControlled_Nrpm</a>.
- </p>
- <h4>Main equations</h4>
- <p>
- See the
- <a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
- User's Guide</a>.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- If <code>use_inputFilter=true</code>, then the parameter <code>dp_nominal</code> is
- used to normalize the filter. This is used to improve the numerics of the transient response.
- The actual pressure raise of the mover at steady-state is independent
- of the value of <code>dp_nominal</code>. It is recommended to set
- <code>dp_nominal</code> to approximately the pressure raise that the mover has during
- full speed.
- </p>
- <h4>Options</h4>
- <p>
- Parameter <code>prescribeSystemPressure</code>
- can be used to control the mover such that the pressure
- difference set point is obtained across two points
- in the system, instead of across the fan.
- This allows an efficient implementation of
- static pressure reset controllers.
- A measurement of the pressure difference between the
- two points in system then needs to be connected
- to <code>RealInput dpMea</code>.
- This functionality is demonstrated in
- <a href=\"modelica://AixLib.Fluid.Movers.Validation.FlowControlled_dpSystem\">
- AixLib.Fluid.Movers.Validation.FlowControlled_dpSystem</a>.
- </p>
- </html>",
+<p>
+This model describes a fan or pump with prescribed head.
+The input connector provides the pressure rise from the inlet to the outlet.
+</p>
+<h4>Main equations</h4>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
+User's Guide</a>.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+If <code>use_inputFilter=true</code>, then the parameter <code>dp_nominal</code> is
+used to normalize the filter. This is used to improve the numerics of the transient response.
+The actual pressure raise of the mover at steady-state is independent
+of the value of <code>dp_nominal</code>. It is recommended to set
+<code>dp_nominal</code> to approximately the pressure raise that the mover has during
+full speed.
+</p>
+<h4>Options</h4>
+<p>
+Parameter <code>prescribeSystemPressure</code>
+can be used to control the mover such that the pressure
+difference set point is obtained across two points
+in the system, instead of across the fan.
+This allows an efficient implementation of
+static pressure reset controllers.
+A measurement of the pressure difference between the
+two points in system then needs to be connected
+to <code>RealInput dpMea</code>.
+This functionality is demonstrated in
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.FlowControlled_dpSystem\">
+AixLib.Fluid.Movers.Validation.FlowControlled_dpSystem</a>.
+</p>
+</html>",
       revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 17, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter.<br/>
- Removed parameter <code>y_start</code> which is not used because <code>dp_start</code> is used.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating stage.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- May 5, 2017, by Filip Jorissen:<br/>
- Added parameters, documentation and functionality for
- <code>prescribeSystemPressure</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/770\">#770</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredSpeed</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- December 2, 2016, by Michael Wetter:<br/>
- Removed <code>min</code> attribute as otherwise numerical noise can cause
- the assertion on the limit to fail.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
- </li>
- <li>
- November 14, 2016, by Michael Wetter:<br/>
- Changed default values for <code>heads</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/583\">#583</a>.
- </li>
- <li>
- March 2, 2016, by Filip Jorissen:<br/>
- Refactored model such that it directly extends <code>PartialFlowMachine</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- November 5, 2015, by Michael Wetter:<br/>
- Removed the parameters <code>use_powerCharacteristics</code> and <code>power</code>
- from the performance data record <code>per</code>
- because
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
- AixLib.Fluid.Movers.FlowControlled_dp</a>
- and
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
- AixLib.Fluid.Movers.FlowControlled_m_flow</a>
- fix the flow rate or head, which can give a flow work that is higher
- than the power consumption specified in this record.
- Hence, users should use the efficiency data for this model.
- The record has been moved to
- <a href=\"modelica://AixLib.Fluid.Movers.Data.SpeedControlled_y\">
- AixLib.Fluid.Movers.Data.SpeedControlled_y</a>
- as it makes sense to use it for the movers
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_Nrpm\">
- AixLib.Fluid.Movers.FlowControlled_Nrpm</a>
- and
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_y\">
- AixLib.Fluid.Movers.FlowControlled_y</a>.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/457\">
- issue 457</a>.
- </li>
- <li>
- April 2, 2015, by Filip Jorissen:<br/>
- Added code for supporting stage input and constant input.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised model for OpenModelica.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- May 25, 2011, by Michael Wetter:<br/>
- Revised implementation of energy balance to avoid having to use conditionally removed models.
- </li>
- <li>
- July 27, 2010, by Michael Wetter:<br/>
- Redesigned model to fix bug in medium balance.
- </li>
- <li>July 5, 2010, by Michael Wetter:<br/>
- Changed <code>assert(dp_in >= 0, ...)</code> to <code>assert(dp_in >= -0.1, ...)</code>.
- The former implementation triggered the assert if <code>dp_in</code> was solved for
- in a nonlinear equation since the solution can be slightly negative while still being
- within the solver tolerance.
- </li>
- <li>March 24, 2010, by Michael Wetter:<br/>
- Revised implementation to allow zero flow rate.
- </li>
- <li>October 1, 2009,
-     by Michael Wetter:<br/>
-        Added model to the AixLib library.
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 1, 2023, by Hongxiang Fu:<br/>
+Refactored the model with a new declaration for
+<code>m_flow_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1705\">#1705</a>.
+</li>
+<li>
+April 27, 2022, by Hongxiang Fu:<br/>
+Replaced <code>not use_powerCharacteristic</code> with the enumerations
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod\">
+AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod</a>
+and
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod\">
+AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod</a>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 17, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter.<br/>
+Removed parameter <code>y_start</code> which is not used because <code>dp_start</code> is used.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating stage.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+May 5, 2017, by Filip Jorissen:<br/>
+Added parameters, documentation and functionality for
+<code>prescribeSystemPressure</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/770\">#770</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredSpeed</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+December 2, 2016, by Michael Wetter:<br/>
+Removed <code>min</code> attribute as otherwise numerical noise can cause
+the assertion on the limit to fail.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
+</li>
+<li>
+November 14, 2016, by Michael Wetter:<br/>
+Changed default values for <code>heads</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/583\">#583</a>.
+</li>
+<li>
+March 2, 2016, by Filip Jorissen:<br/>
+Refactored model such that it directly extends <code>PartialFlowMachine</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+November 5, 2015, by Michael Wetter:<br/>
+Removed the parameters <code>use_powerCharacteristics</code> and <code>power</code>
+from the performance data record <code>per</code>
+because
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
+AixLib.Fluid.Movers.FlowControlled_dp</a>
+and
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.FlowControlled_m_flow</a>
+fix the flow rate or head, which can give a flow work that is higher
+than the power consumption specified in this record.
+Hence, users should use the efficiency data for this model.
+The record has been moved to
+<a href=\"modelica://AixLib.Fluid.Movers.Data.SpeedControlled_y\">
+AixLib.Fluid.Movers.Data.SpeedControlled_y</a>
+as it makes sense to use it for the movers
+<a href=\"modelica://AixLib.Obsolete.Fluid.Movers.FlowControlled_Nrpm\">
+AixLib.Obsolete.Fluid.Movers.FlowControlled_Nrpm</a>
+and
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_y\">
+AixLib.Fluid.Movers.FlowControlled_y</a>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/457\">
+issue 457</a>.
+</li>
+<li>
+April 2, 2015, by Filip Jorissen:<br/>
+Added code for supporting stage input and constant input.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised model for OpenModelica.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+May 25, 2011, by Michael Wetter:<br/>
+Revised implementation of energy balance to avoid having to use conditionally removed models.
+</li>
+<li>
+July 27, 2010, by Michael Wetter:<br/>
+Redesigned model to fix bug in medium balance.
+</li>
+<li>July 5, 2010, by Michael Wetter:<br/>
+Changed <code>assert(dp_in >= 0, ...)</code> to <code>assert(dp_in >= -0.1, ...)</code>.
+The former implementation triggered the assert if <code>dp_in</code> was solved for
+in a nonlinear equation since the solution can be slightly negative while still being
+within the solver tolerance.
+</li>
+<li>March 24, 2010, by Michael Wetter:<br/>
+Revised implementation to allow zero flow rate.
+</li>
+<li>October 1, 2009,
+    by Michael Wetter:<br/>
+       Added model to the AixLib library.
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowControlled_dp;
diff --git a/AixLib/Fluid/Movers/FlowControlled_m_flow.mo b/AixLib/Fluid/Movers/FlowControlled_m_flow.mo
index 2350b56ed7..13a8089188 100644
--- a/AixLib/Fluid/Movers/FlowControlled_m_flow.mo
+++ b/AixLib/Fluid/Movers/FlowControlled_m_flow.mo
@@ -6,6 +6,7 @@ model FlowControlled_m_flow
     final computePowerUsingSimilarityLaws=per.havePressureCurve,
     final stageInputs(each final unit="kg/s")=massFlowRates,
     final constInput(final unit="kg/s")=constantMassFlowRate,
+    final _m_flow_nominal = m_flow_nominal,
     filter(
       final y_start=m_flow_start,
       u(final unit="kg/s"),
@@ -20,13 +21,32 @@ model FlowControlled_m_flow
           AixLib.Fluid.Movers.BaseClasses.Characteristics.flowParameters(
             V_flow = {i/(nOri-1)*2.0*m_flow_nominal/rho_default for i in 0:(nOri-1)},
             dp =     {i/(nOri-1)*2.0*dp_nominal for i in (nOri-1):-1:0}),
-      final use_powerCharacteristic = if per.havePressureCurve then per.use_powerCharacteristic else false),
+        final etaHydMet=
+          if (per.etaHydMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Power_VolumeFlowRate
+            or per.etaHydMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber)
+            and not per.havePressureCurve then
+              AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.NotProvided
+          else per.etaHydMet,
+        final etaMotMet=
+          if (per.etaMotMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_MotorPartLoadRatio
+            or per.etaMotMet ==
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve)
+            and (not per.haveWMot_nominal and not per.havePressureCurve) then
+               AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided
+          else per.etaMotMet),
       r_N(start=if abs(m_flow_nominal) > 1E-8 then m_flow_start/m_flow_nominal else 0)),
     preSou(m_flow_start=m_flow_start));
 
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal(
+    final min=Modelica.Constants.small)
+    "Nominal mass flow rate" annotation (Dialog(group="Nominal condition"));
+
   // For air, we set dp_nominal = 600 as default, for water we set 10000
   parameter Modelica.Units.SI.PressureDifference dp_nominal(
-    min=0,
+    final min=Modelica.Constants.small,
     displayUnit="Pa") = if rho_default < 500 then 500 else 10000
     "Nominal pressure raise, used for default pressure curve if not specified in record per"
     annotation (Dialog(group="Nominal condition"));
@@ -45,6 +65,12 @@ model FlowControlled_m_flow
     "Vector of mass flow rate set points, used when inputType=Stage"
     annotation (Dialog(enable=inputType == AixLib.Fluid.Types.InputType.Stages));
 
+  parameter Modelica.Units.SI.Pressure dpMax(
+    min=0,
+    displayUnit="Pa") = 2*max(eff.per.pressure.dp)
+   "Maximum pressure allowed to operate the model, if exceeded, the simulation stops with an error"
+   annotation(Dialog(tab="Advanced"));
+
   Modelica.Blocks.Interfaces.RealInput m_flow_in(
     final unit="kg/s",
     nominal=m_flow_nominal)
@@ -64,6 +90,13 @@ model FlowControlled_m_flow
         iconTransformation(extent={{100,40},{120,60}})));
 
 equation
+  assert(-dp <= dpMax,
+    "In " + getInstanceName() + ": Model operates with head -dp = " + String(-dp) + " Pa,
+    exceeding the pressure allowed by the parameter " + getInstanceName() + ".dpMax.
+    This can happen if the model forces a high mass flow rate through a closed actuator,
+    or if the performance record is unreasonable. Please verify your model, and
+    consider using one of the other pump or fan models.");
+
   if use_inputFilter then
     connect(filter.y, m_flow_actual) annotation (Line(
       points={{41,70.5},{44,70.5},{44,50},{110,50}},
@@ -80,13 +113,11 @@ equation
       smooth=Smooth.None));
   end if;
 
-
   connect(inputSwitch.u, m_flow_in) annotation (Line(
       points={{-22,50},{-26,50},{-26,80},{0,80},{0,120}},
       color={0,0,127},
       smooth=Smooth.None));
 
-
   annotation (
       Icon(graphics={
         Text(
@@ -94,89 +125,115 @@ equation
           textColor={0,0,127},
           visible=inputType == AixLib.Fluid.Types.InputType.Continuous or inputType == AixLib.Fluid.Types.InputType.Stages,
           textString=DynamicSelect("m_flow", if inputType == AixLib.Fluid.Types.InputType.Continuous then String(m_flow_in, leftJustified=false, significantDigits=3) else String(stage)))}),
-  defaultComponentName="fan",
+  defaultComponentName="mov",
   Documentation(
    info="<html>
- <p>
- This model describes a fan or pump with prescribed mass flow rate.
- The efficiency of the device is computed based
- on the efficiency and pressure curves that are defined
- in record <code>per</code>, which is of type
- <a href=\"modelica://AixLib.Fluid.Movers.SpeedControlled_Nrpm\">
- AixLib.Fluid.Movers.SpeedControlled_Nrpm</a>.
- </p>
- <p>
- See the
- <a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
- User's Guide</a> for more information.
- </p>
- </html>",
+<p>
+This model describes a fan or pump with prescribed mass flow rate.
+</p>
+<p>
+Note that if the model operates with a head that is larger than <code>dpMax</code>, which by default is
+two times larger than the largest head declared in <code>eff.per.pressure.dp</code>,
+the simulation will stop with an error message.
+This guards against unreasonably high pressure drops and electrical power use,
+which can happen if the model is forcing mass flow rate through a closed actuator.
+</p>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
+User's Guide</a> for more information.
+</p>
+</html>",
       revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 17, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter.<br/>
- Removed parameter <code>y_start</code> which is not used because <code>m_flow_start</code> is used.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating stage.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredSpeed</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- November 10, 2016, by Michael Wetter:<br/>
- Changed default values for <code>massFlowRates</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/583\">#583</a>.
- </li>
- <li>
- March 2, 2016, by Filip Jorissen:<br/>
- Refactored model such that it directly extends <code>PartialFlowMachine</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- <li>
- April 2, 2015, by Filip Jorissen:<br/>
- Added code for supporting stage input and constant input.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised model for OpenModelica.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- May 25, 2011, by Michael Wetter:<br/>
- Revised implementation of energy balance to avoid having to use conditionally removed models.
- </li>
- <li>
- July 27, 2010, by Michael Wetter:<br/>
- Redesigned model to fix bug in medium balance.
- </li>
- <li>March 24, 2010, by Michael Wetter:<br/>
- Revised implementation to allow zero flow rate.
- </li>
- <li>October 1, 2009
-     by Michael Wetter:<br/>
-        Model added to the AixLib library.
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 1, 2023, by Hongxiang Fu:<br/>
+Refactored the model with a new declaration for
+<code>m_flow_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1705\">#1705</a>.
+</li>
+<li>
+April 27, 2022, by Hongxiang Fu:<br/>
+Replaced <code>not use_powerCharacteristic</code> with the enumerations
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod\">
+AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod</a>
+and
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod\">
+AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod</a>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+<li>
+November 15, 2022, by Michael Wetter:<br/>
+Added assertion if model operates with a pressure higher than <code>dpMax</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1659\">#1659</a>.
+</li>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 17, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter.<br/>
+Removed parameter <code>y_start</code> which is not used because <code>m_flow_start</code> is used.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating stage.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredSpeed</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+November 10, 2016, by Michael Wetter:<br/>
+Changed default values for <code>massFlowRates</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/583\">#583</a>.
+</li>
+<li>
+March 2, 2016, by Filip Jorissen:<br/>
+Refactored model such that it directly extends <code>PartialFlowMachine</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
+</li>
+<li>
+April 2, 2015, by Filip Jorissen:<br/>
+Added code for supporting stage input and constant input.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised model for OpenModelica.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+May 25, 2011, by Michael Wetter:<br/>
+Revised implementation of energy balance to avoid having to use conditionally removed models.
+</li>
+<li>
+July 27, 2010, by Michael Wetter:<br/>
+Redesigned model to fix bug in medium balance.
+</li>
+<li>March 24, 2010, by Michael Wetter:<br/>
+Revised implementation to allow zero flow rate.
+</li>
+<li>October 1, 2009
+    by Michael Wetter:<br/>
+       Model added to the AixLib library.
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowControlled_m_flow;
diff --git a/AixLib/Fluid/Movers/Preconfigured/FlowControlled_dp.mo b/AixLib/Fluid/Movers/Preconfigured/FlowControlled_dp.mo
new file mode 100644
index 0000000000..a1f0e5053e
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/FlowControlled_dp.mo
@@ -0,0 +1,37 @@
+within AixLib.Fluid.Movers.Preconfigured;
+model FlowControlled_dp "Fan or pump with ideally controlled head dp as input signal and pre-configured parameters"
+  extends AixLib.Fluid.Movers.FlowControlled_dp(
+    final per(
+            pressure(
+              V_flow=m_flow_nominal/rho_default*{0, 1, 2},
+              dp=if rho_default < 500
+                   then dp_nominal*{1.12, 1, 0}
+                   else dp_nominal*{1.14, 1, 0.42}),
+            powerOrEfficiencyIsHydraulic=true,
+            etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber,
+            etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve),
+    final constantHead,
+    final heads,
+    final nominalValuesDefineDefaultPressureCurve=true,
+    final inputType=AixLib.Fluid.Types.InputType.Continuous,
+    final prescribeSystemPressure=false,
+    final init=Modelica.Blocks.Types.Init.InitialOutput,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial);
+    annotation (
+defaultComponentName="mov",
+Documentation(info="<html>
+<p>
+This model is the preconfigured version for
+<a href=\"Modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
+AixLib.Fluid.Movers.FlowControlled_dp</a>.
+</html>", revisions="<html>
+<ul>
+<li>
+August 17, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FlowControlled_dp;
diff --git a/AixLib/Fluid/Movers/Preconfigured/FlowControlled_m_flow.mo b/AixLib/Fluid/Movers/Preconfigured/FlowControlled_m_flow.mo
new file mode 100644
index 0000000000..d00053a00f
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/FlowControlled_m_flow.mo
@@ -0,0 +1,36 @@
+within AixLib.Fluid.Movers.Preconfigured;
+model FlowControlled_m_flow "Fan or pump with ideally controlled mass flow rate as input signal and pre-configured parameters"
+  extends AixLib.Fluid.Movers.FlowControlled_m_flow(
+    final per(
+            pressure(
+              V_flow=m_flow_nominal/rho_default*{0, 1, 2},
+              dp=if rho_default < 500
+                   then dp_nominal*{1.12, 1, 0}
+                   else dp_nominal*{1.14, 1, 0.42}),
+            powerOrEfficiencyIsHydraulic=true,
+            etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber,
+            etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve),
+    final constantMassFlowRate,
+    final massFlowRates,
+    final nominalValuesDefineDefaultPressureCurve=true,
+    final inputType=AixLib.Fluid.Types.InputType.Continuous,
+    final init=Modelica.Blocks.Types.Init.InitialOutput,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial);
+annotation (
+defaultComponentName="mov",
+Documentation(info="<html>
+<p>
+This model is the preconfigured version for
+<a href=\"Modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.FlowControlled_m_flow</a>.
+</html>", revisions="<html>
+<ul>
+<li>
+August 17, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FlowControlled_m_flow;
diff --git a/AixLib/Fluid/Movers/Preconfigured/SpeedControlled_y.mo b/AixLib/Fluid/Movers/Preconfigured/SpeedControlled_y.mo
new file mode 100644
index 0000000000..f68d418f6a
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/SpeedControlled_y.mo
@@ -0,0 +1,49 @@
+within AixLib.Fluid.Movers.Preconfigured;
+model SpeedControlled_y "Fan or pump with ideally controlled normalized speed y as input signal and pre-configured parameters"
+  extends AixLib.Fluid.Movers.SpeedControlled_y(
+    final per(
+            pressure(
+              V_flow=m_flow_nominal/rho_default*{0, 1, 2},
+              dp=if rho_default < 500
+                   then dp_nominal*{1.12, 1, 0}
+                   else dp_nominal*{1.14, 1, 0.42}),
+            powerOrEfficiencyIsHydraulic=true,
+            etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber,
+            etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.GenericCurve),
+    final inputType=AixLib.Fluid.Types.InputType.Continuous,
+    final init=Modelica.Blocks.Types.Init.InitialOutput,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial);
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal(
+    final min=Modelica.Constants.small)
+    "Nominal mass flow rate for configuration of pressure curve"
+    annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(
+    final min=Modelica.Constants.small)
+    "Nominal pressure head for configuration of pressure curve"
+    annotation(Dialog(group="Nominal condition"));
+annotation (
+defaultComponentName="mov",
+Documentation(info="<html>
+<p>
+This model is the preconfigured version for
+<a href=\"Modelica://AixLib.Fluid.Movers.SpeedControlled_y\">
+AixLib.Fluid.Movers.SpeedControlled_y</a>.
+</html>", revisions="<html>
+<ul>
+<li>
+March 1, 2023, by Hongxiang Fu:<br/>
+Refactored the model with a new declaration for
+<code>m_flow_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1705\">#1705</a>.
+</li>
+<li>
+August 17, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end SpeedControlled_y;
diff --git a/AixLib/Fluid/Movers/Preconfigured/UsersGuide.mo b/AixLib/Fluid/Movers/Preconfigured/UsersGuide.mo
new file mode 100644
index 0000000000..582f1bdab0
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/UsersGuide.mo
@@ -0,0 +1,47 @@
+within AixLib.Fluid.Movers.Preconfigured;
+package UsersGuide "User's Guide"
+  extends Modelica.Icons.Information;
+
+  annotation (preferredView="info",
+  Documentation(info="<html>
+<p>
+This package contains preconfigured versions of the mover models.
+They automatically configure a mover model based on
+<code>m_flow_nominal</code> and <code>dp_nominal</code>.
+</p>
+<p>
+The configuration is as follows:
+</p>
+<ul>
+<li>
+The parameters <code>m_flow_nominal</code> and <code>dp_nominal</code>
+are used to construct the pressure curve <i>&Delta; p = f(m&#775;,  y)</i>
+where <i>m&#775;</i> is the mass flow rate and <i>y</i> is the speed.
+This curve is based on a least squares polynomial fit of all pressure curves from
+<a href=\"Modelica://AixLib.Fluid.Movers.Data.Pumps\">
+AixLib.Fluid.Movers.Data.Pumps</a>
+for pumps and
+<a href=\"Modelica://AixLib.Fluid.Movers.Data.Fans\">
+AixLib.Fluid.Movers.Data.Fans</a>
+for fans.
+(See also
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1884\">#1884</a>.)
+The model identifies itself as a fan or pump based on the default density of
+the medium.
+</li>
+<li>
+The hydraulic efficiency is computed based on the Euler number.
+See <a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
+AixLib.Fluid.Movers.UsersGuide</a>
+for details.
+</li>
+<li>
+The motor efficiency is computed based on a generic curve.
+See <a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve</a>
+for details.
+</li>
+</ul>
+</html>"));
+
+end UsersGuide;
diff --git a/AixLib/Fluid/Movers/Preconfigured/Validation/ControlledFlowMachinePreconfigured.mo b/AixLib/Fluid/Movers/Preconfigured/Validation/ControlledFlowMachinePreconfigured.mo
new file mode 100644
index 0000000000..00c5a65870
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/Validation/ControlledFlowMachinePreconfigured.mo
@@ -0,0 +1,56 @@
+within AixLib.Fluid.Movers.Preconfigured.Validation;
+model ControlledFlowMachinePreconfigured
+  "Preconfigured fans with different control signals"
+  extends Modelica.Icons.Example;
+  extends AixLib.Fluid.Movers.Validation.BaseClasses.ControlledFlowMachine(
+    redeclare AixLib.Fluid.Movers.Preconfigured.SpeedControlled_y fan1(
+      redeclare package Medium = Medium,
+      m_flow_nominal=m_flow_nominal,
+      dp_nominal=dp_nominal),
+    redeclare AixLib.Fluid.Movers.Preconfigured.FlowControlled_m_flow fan2(
+      redeclare package Medium = Medium,
+      m_flow_nominal=m_flow_nominal,
+      dp_nominal=dp_nominal),
+    redeclare AixLib.Fluid.Movers.Preconfigured.FlowControlled_dp fan3(
+      redeclare package Medium = Medium,
+      m_flow_nominal=m_flow_nominal,
+      dp_nominal=dp_nominal),
+    dp1(m_flow_nominal=m_flow_nominal, dp_nominal=dp_nominal),
+    dp2(m_flow_nominal=m_flow_nominal, dp_nominal=dp_nominal),
+    dp3(m_flow_nominal=m_flow_nominal, dp_nominal=dp_nominal));
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=2
+    "Nominal mass flow rate for each fan";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal=500
+    "Nominal pressure head for each fan";
+
+      annotation (
+experiment(Tolerance=1e-6, StopTime=600),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Preconfigured/Validation/ControlledFlowMachinePreconfigured.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+This model validates the preconfigured mover models.
+It is based on
+<a href=\"Modelica://AixLib.Fluid.Movers.Validation.ControlledFlowMachineDynamic\">
+AixLib.Fluid.Movers.Validation.ControlledFlowMachineDynamic</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Deleted the mover with <code>Nrpm</code> signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+August 17, 2022, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-160,-80},{160,160}})),
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ControlledFlowMachinePreconfigured;
diff --git a/AixLib/Fluid/Movers/Preconfigured/Validation/package.mo b/AixLib/Fluid/Movers/Preconfigured/Validation/package.mo
new file mode 100644
index 0000000000..01e8194953
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/Validation/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.Movers.Preconfigured;
+package Validation "Package for validation models"
+extends Modelica.Icons.ExamplesPackage;
+
+  annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains validation models for the classes in
+<a href=\"modelica://AixLib.Fluid.Movers.Preconfigured\">
+AixLib.Fluid.Movers.Preconfigured</a>.
+</p>
+</html>"));
+end Validation;
diff --git a/AixLib/Fluid/Movers/Preconfigured/Validation/package.order b/AixLib/Fluid/Movers/Preconfigured/Validation/package.order
new file mode 100644
index 0000000000..799d7b6441
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/Validation/package.order
@@ -0,0 +1 @@
+ControlledFlowMachinePreconfigured
diff --git a/AixLib/Fluid/Movers/Preconfigured/package.mo b/AixLib/Fluid/Movers/Preconfigured/package.mo
new file mode 100644
index 0000000000..1faceda3db
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/package.mo
@@ -0,0 +1,17 @@
+within AixLib.Fluid.Movers;
+package Preconfigured "Preconfigured mover models"
+  extends Modelica.Icons.Package;
+
+    annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains preconfigured versions for the mover models.
+The models are identical to the ones in the package
+<a href=\"Modelica://AixLib.Fluid.Movers\">AixLib.Fluid.Movers</a>
+except that most parameters are set to default values.
+</p>
+</html>"),
+    Icon(graphics={       Line(
+          points={{-60,0},{-20,-40},{60,40}},
+          color={0,140,72},
+          thickness=10)}));
+end Preconfigured;
diff --git a/AixLib/Fluid/Movers/Preconfigured/package.order b/AixLib/Fluid/Movers/Preconfigured/package.order
new file mode 100644
index 0000000000..96cea4f048
--- /dev/null
+++ b/AixLib/Fluid/Movers/Preconfigured/package.order
@@ -0,0 +1,5 @@
+UsersGuide
+FlowControlled_dp
+FlowControlled_m_flow
+SpeedControlled_y
+Validation
diff --git a/AixLib/Fluid/Movers/PumpsPolynomialBased/Examples/PumpHeadControlled.mo b/AixLib/Fluid/Movers/PumpsPolynomialBased/Examples/PumpHeadControlled.mo
index 2ac51e5a7c..1d8a9a86c2 100644
--- a/AixLib/Fluid/Movers/PumpsPolynomialBased/Examples/PumpHeadControlled.mo
+++ b/AixLib/Fluid/Movers/PumpsPolynomialBased/Examples/PumpHeadControlled.mo
@@ -24,7 +24,7 @@ model PumpHeadControlled "testing the head controlled pump model."
         extent={{-10,-10},{10,10}},
         rotation=-90,
         origin={-36,20})));
-  parameter Modelica.SIunits.MassFlowRate m_flow_nominal=0.1 "Nominal mass flow rate";
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=0.1 "Nominal mass flow rate";
   Modelica.Blocks.Sources.BooleanPulse    PumpOn1(period=600, width=500/600*100,
     startTime=0)
     annotation (Placement(transformation(extent={{-70,30},{-50,50}})));
@@ -66,9 +66,9 @@ equation
   connect(pump.port_b, simpleValve.port_a) annotation (Line(points={{10,10},{40,
           10},{40,-30},{-20,-30}}, color={0,127,255}));
   connect(vessle.ports[1], pump.port_a)
-    annotation (Line(points={{-34,10},{-10,10}}, color={0,127,255}));
+    annotation (Line(points={{-37,10},{-10,10}}, color={0,127,255}));
   connect(simpleValve.port_b, vessle.ports[2]) annotation (Line(points={{-40,-30},
-          {-60,-30},{-60,10},{-38,10}}, color={0,127,255}));
+          {-60,-30},{-60,10},{-35,10}}, color={0,127,255}));
   connect(rampValvePosition.y, simpleValve.y)
     annotation (Line(points={{-21,-60},{-30,-60},{-30,-42}}, color={0,0,127}));
   annotation (
@@ -77,7 +77,7 @@ equation
       Tolerance=1e-06,
       __Dymola_Algorithm="Dassl"),
     Documentation(revisions="<html><ul>
-  <li>2019-09-18 by Alexander Kümpel:<br/>
+  <li>2019-09-18 by Alexander Kuempel:<br/>
     Renaming and restructuring.
   </li>
   <li>2018-03-01 by Peter Matthes:<br/>
diff --git a/AixLib/Fluid/Movers/PumpsPolynomialBased/Examples/package.mo b/AixLib/Fluid/Movers/PumpsPolynomialBased/Examples/package.mo
index 5107cdd1f6..110bb3f200 100644
--- a/AixLib/Fluid/Movers/PumpsPolynomialBased/Examples/package.mo
+++ b/AixLib/Fluid/Movers/PumpsPolynomialBased/Examples/package.mo
@@ -2,117 +2,5 @@
 package Examples
 extends Modelica.Icons.ExamplesPackage;
 
-  model PumpHeadControlled "testing the head controlled pump model."
-    extends Modelica.Icons.Example;
-
-    replaceable package Medium =
-      Modelica.Media.Water.ConstantPropertyLiquidWater;
-
-    .AixLib.Fluid.Movers.PumpsPolynomialBased.PumpHeadControlled pump(
-      m_flow_nominal=m_flow_nominal,
-      calculatePower=true,
-      calculateEfficiency=true,
-      redeclare package Medium = Medium,
-      pumpParam=DataBase.Pumps.PumpPolynomialBased.Pump_DN25_H1_8_V9())
-                 annotation (Placement(transformation(extent={{-10,0},{10,20}})));
-
-    Modelica.Blocks.Sources.Ramp rampValvePosition(
-      offset=0.5,
-      height=0.5,
-      duration(displayUnit="s") = 120,
-      startTime(displayUnit="min") = 120)
-      annotation (Placement(transformation(extent={{0,-70},{-20,-50}})));
-    AixLib.Fluid.Sources.Boundary_pT vessle(
-      redeclare package Medium = Medium, nPorts=2)
-                annotation (Placement(transformation(
-          extent={{-10,-10},{10,10}},
-          rotation=-90,
-          origin={-36,20})));
-  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=0.1
-    "Nominal mass flow rate";
-    Modelica.Blocks.Sources.BooleanPulse    PumpOn1(period=600, width=500/600*100,
-      startTime=0)
-      annotation (Placement(transformation(extent={{-70,30},{-50,50}})));
-    Modelica.Blocks.Sources.Ramp rampPumpDp(
-      height=2,
-      offset=2,
-      duration(displayUnit="s") = 100,
-      startTime(displayUnit="s") = 100)
-      annotation (Placement(transformation(extent={{46,30},{26,50}})));
-    BaseClasses.PumpBus                                          pumpBus
-      annotation (Placement(transformation(extent={{-10,30},{10,50}})));
-    Actuators.Valves.TwoWayLinear             simpleValve(
-      redeclare package Medium = Medium,
-      m_flow_nominal=m_flow_nominal,
-      CvData=AixLib.Fluid.Types.CvTypes.Kv,
-      Kv=6.3,
-      dpFixed_nominal=1000)
-      annotation (Placement(transformation(extent={{-20,-20},{-40,-40}})));
-  equation
-    connect(PumpOn1.y, pumpBus.onSet) annotation (Line(points={{-49,40},{-28,40},{
-            -28,40},{-14,40},{-14,40.05},{0.05,40.05}}, color={255,0,255}), Text(
-        string="%second",
-        index=2,
-        extent={{6,3},{6,3}}));
-    connect(pumpBus, pump.pumpBus) annotation (Line(
-        points={{0,40},{0,20}},
-        color={255,204,51},
-        thickness=0.5), Text(
-        string="%first",
-        index=-1,
-        extent={{-3,6},{-3,6}},
-        horizontalAlignment=TextAlignment.Right));
-    connect(rampPumpDp.y, pumpBus.dpSet) annotation (Line(points={{25,40},{12,40},
-            {12,40.05},{0.05,40.05}}, color={0,0,127}), Text(
-        string="%second",
-        index=1,
-        extent={{-6,3},{-6,3}},
-        horizontalAlignment=TextAlignment.Right));
-    connect(pump.port_b, simpleValve.port_a) annotation (Line(points={{10,10},{40,
-            10},{40,-30},{-20,-30}}, color={0,127,255}));
-    connect(vessle.ports[1], pump.port_a)
-      annotation (Line(points={{-34,10},{-10,10}}, color={0,127,255}));
-    connect(simpleValve.port_b, vessle.ports[2]) annotation (Line(points={{-40,-30},
-            {-60,-30},{-60,10},{-38,10}}, color={0,127,255}));
-    connect(rampValvePosition.y, simpleValve.y)
-      annotation (Line(points={{-21,-60},{-30,-60},{-30,-42}}, color={0,0,127}));
-    annotation (
-        experiment(
-        StopTime=600,
-        Tolerance=1e-06,
-        __Dymola_Algorithm="Dassl"),
-      Documentation(revisions="<html><ul>
-  <li>2019-09-18 by Alexander Kümpel:<br/>
-    Renaming and restructuring.
-  </li>
-  <li>2018-03-01 by Peter Matthes:<br/>
-    Adjusted parameter settings. From pump model removed Nstart (became
-    Nnom in pump model) and m_flow_start (should be used as output from
-    pump rather than a setting). Changed setting of system.m_flow_start
-    to become pump.m_flow_start.
-  </li>
-  <li>2018-02-01 by Peter Matthes<br/>
-    Switches pump off near end of simulation to check for handling of
-    power and efficiency calculation. Improves plot script.
-  </li>
-  <li>2018-01-29 by Peter Matthes:<br/>
-    * Removes parameter useABCformula in pump model and changes pump
-    record to Stratos_Pico_25_1_6.<br/>
-    * The selectable function for efficiency calculation could be
-    removed from the parameter dialog.
-  </li>
-  <li>2018-01-26 by Peter Matthes:<br/>
-    Changes parameter name n_start into Nstart in the pump models.
-  </li>
-  <li>2017-11-22 by Peter Matthes<br/>
-    Implemented
-  </li>
-</ul>
-</html>"),
-      __Dymola_Commands(file=
-            "Resources/Scripts/Dymola/Fluid/Movers/PumpsPolynomialBased/Examples/PumpHeadControlled.mos"
-          "Simulate and plot"));
-  end PumpHeadControlled;
-
   annotation(preferredView="info");
 end Examples;
diff --git a/AixLib/Fluid/Movers/SpeedControlled_y.mo b/AixLib/Fluid/Movers/SpeedControlled_y.mo
index 0eb439c36a..0565718830 100644
--- a/AixLib/Fluid/Movers/SpeedControlled_y.mo
+++ b/AixLib/Fluid/Movers/SpeedControlled_y.mo
@@ -5,7 +5,6 @@ model SpeedControlled_y
     final preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
     final nominalValuesDefineDefaultPressureCurve=false,
     final computePowerUsingSimilarityLaws=true,
-    final m_flow_nominal = max(per.pressure.V_flow)*rho_default,
     final stageInputs(each final unit="1") = per.speeds,
     final constInput(final unit="1") =       per.constantSpeed,
     filter(
@@ -14,10 +13,9 @@ model SpeedControlled_y
       y(final unit="1")),
     eff(
       per(final pressure = per.pressure,
-          final use_powerCharacteristic = per.use_powerCharacteristic),
-          r_N(start=y_start)),
-    gaiSpe(u(final unit="1"),
-           final k=1/per.speed_nominal));
+          final etaHydMet = per.etaHydMet,
+          final etaMotMet = per.etaMotMet),
+      r_N(start=y_start)));
 
   parameter Real y_start(min=0, max=1, unit="1")=0 "Initial value of speed"
     annotation(Dialog(tab="Dynamics", group="Filtered speed", enable=use_inputFilter));
@@ -38,20 +36,19 @@ protected
   Modelica.Blocks.Math.Gain gain(final k=-1) "Pressure gain"
     annotation (Placement(transformation(extent={{10,-10},{-10,10}},
         rotation=270,
-        origin={10,-20})));
+        origin={-10,-20})));
 initial equation
   assert(per.havePressureCurve,
    "SpeedControlled_y requires to set the pressure vs. flow rate curve in record 'per'.");
 
 equation
-  connect(gaiSpe.u, y)
-    annotation (Line(points={{-2.8,80},{0,80},{0,120}}, color={0,0,127}));
-  connect(gaiSpe.y, inputSwitch.u) annotation (Line(points={{-16.6,80},{-26,80},
-          {-26,50},{-22,50}}, color={0,0,127}));
+  connect(inputSwitch.u, y) annotation (Line(points={{-22,50},{-26,50},{-26,80},
+          {0,80},{0,120}}, color={0,0,127}));
   connect(eff.dp, gain.u)
-    annotation (Line(points={{-11,-50},{10,-50},{10,-32}}, color={0,0,127}));
+    annotation (Line(points={{-11,-50},{-6,-50},{-6,-42},{-10,-42},{-10,-32}},
+                                                           color={0,0,127}));
   connect(gain.y, preSou.dp_in)
-    annotation (Line(points={{10,-9},{10,14},{56,14},{56,8},{56,8}},
+    annotation (Line(points={{-10,-9},{-10,14},{56,14},{56,8}},
                                                      color={0,0,127}));
 
   if use_inputFilter then
@@ -63,7 +60,7 @@ equation
                                    color={0,0,127}));
   end if;
 
-    annotation (defaultComponentName="fan",
+    annotation (defaultComponentName="mov",
     Icon(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{100,
             100}}),
          graphics={
@@ -73,102 +70,117 @@ equation
           visible=inputType == AixLib.Fluid.Types.InputType.Continuous or inputType == AixLib.Fluid.Types.InputType.Stages,
           textString=DynamicSelect("y", if inputType == AixLib.Fluid.Types.InputType.Continuous then String(y, format=".2f") else String(stage)))}),
     Documentation(info="<html>
- <p>
- This model describes a fan or pump with prescribed normalized speed.
- The input connector provides the normalized rotational speed (between 0 and 1).
- The head is computed based on the performance curve that take as an argument
- the actual volume flow rate divided by the maximum flow rate and the relative
- speed of the fan.
- The efficiency of the device is computed based
- on the efficiency curves that take as an argument
- the actual volume flow rate divided by the maximum possible volume flow rate, or
- based on the motor performance curves.
- </p>
- <p>
- See the
- <a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
- User's Guide</a> for more information.
- </p>
- </html>",
+<p>
+This model describes a fan or pump with prescribed normalized speed.
+The input connector provides the normalized rotational speed (between 0 and 1).
+The head is computed based on the performance curve that take as an argument
+the actual volume flow rate divided by the maximum flow rate and the relative
+speed of the fan.
+</p>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Movers.UsersGuide\">
+User's Guide</a> for more information.
+</p>
+</html>",
       revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 17, 2021, by Michael Wetter:<br/>
- Changed implementation of the filter.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating stage.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- March 24, 2017, by Michael Wetter:<br/>
- Renamed <code>filteredSpeed</code> to <code>use_inputFilter</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
- </li>
- <li>
- December 2, 2016, by Michael Wetter:<br/>
- Removed <code>min</code> attribute as otherwise numerical noise can cause
- the assertion on the limit to fail.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
- </li>
- <li>
- March 2, 2016, by Filip Jorissen:<br/>
- Refactored model such that it directly extends <code>PartialFlowMachine</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>
- April 2, 2015, by Filip Jorissen:<br/>
- Added code for supporting stage input and constant input.
- </li>
- <li>
- January 6, 2015, by Michael Wetter:<br/>
- Revised model for OpenModelica.
- </li>
- <li>
- November 22, 2014, by Michael Wetter:<br/>
- Revised implementation that uses the new performance data as a record.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- May 25, 2011, by Michael Wetter:<br/>
- Revised implementation of energy balance to avoid having to use conditionally removed models.
- </li>
- <li>
- July 27, 2010, by Michael Wetter:<br/>
- Redesigned model to fix bug in medium balance.
- </li>
- <li>March 24, 2010, by Michael Wetter:<br/>
- Revised implementation to allow zero flow rate.
- </li>
- <li>
- October 1, 2009, by Michael Wetter:<br/>
- Model added to the AixLib library. Changed control signal from rpm to normalized value between 0 and 1</li>
- <li>
- October 31, 2005 by <a href=\"mailto:francesco.casella@polimi.it\">Francesco Casella</a>:<br/>
- Model added to the Fluid library
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 29, 2023, by Hongxiang Fu:<br/>
+Removed the modification that normalised the speed input
+because it is no longer needed. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+March 1, 2023, by Hongxiang Fu:<br/>
+Removed the modification of <code>m_flow_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1705\">#1705</a>.
+</li>
+<li>
+March 8, 2022, by Hongxiang Fu:<br/>
+Refactored the model by replacing <code>not use_powerCharacteristic</code>
+with the enumeration
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod\">
+AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod</a>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2668\">#2668</a>.
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 17, 2021, by Michael Wetter:<br/>
+Changed implementation of the filter.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1498\">#1498</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating stage.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+March 24, 2017, by Michael Wetter:<br/>
+Renamed <code>filteredSpeed</code> to <code>use_inputFilter</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/665\">#665</a>.
+</li>
+<li>
+December 2, 2016, by Michael Wetter:<br/>
+Removed <code>min</code> attribute as otherwise numerical noise can cause
+the assertion on the limit to fail.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
+</li>
+<li>
+March 2, 2016, by Filip Jorissen:<br/>
+Refactored model such that it directly extends <code>PartialFlowMachine</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>
+April 2, 2015, by Filip Jorissen:<br/>
+Added code for supporting stage input and constant input.
+</li>
+<li>
+January 6, 2015, by Michael Wetter:<br/>
+Revised model for OpenModelica.
+</li>
+<li>
+November 22, 2014, by Michael Wetter:<br/>
+Revised implementation that uses the new performance data as a record.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+May 25, 2011, by Michael Wetter:<br/>
+Revised implementation of energy balance to avoid having to use conditionally removed models.
+</li>
+<li>
+July 27, 2010, by Michael Wetter:<br/>
+Redesigned model to fix bug in medium balance.
+</li>
+<li>March 24, 2010, by Michael Wetter:<br/>
+Revised implementation to allow zero flow rate.
+</li>
+<li>
+October 1, 2009, by Michael Wetter:<br/>
+Model added to the AixLib library. Changed control signal from rpm to normalized value between 0 and 1</li>
+<li>
+October 31, 2005 by <a href=\"mailto:francesco.casella@polimi.it\">Francesco Casella</a>:<br/>
+Model added to the Fluid library
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpeedControlled_y;
diff --git a/AixLib/Fluid/Movers/UsersGuide.mo b/AixLib/Fluid/Movers/UsersGuide.mo
index 63c1037263..a4fa767f98 100644
--- a/AixLib/Fluid/Movers/UsersGuide.mo
+++ b/AixLib/Fluid/Movers/UsersGuide.mo
@@ -4,11 +4,33 @@ package UsersGuide "User's Guide"
   annotation (preferredView="info",
   Documentation(info="<html>
 <p>
-This package contains models for fans and pumps. The same models
-are used for fans or pumps.
+This package contains models for fans and pumps (movers).
+The same models can be used for fans or pumps.
 </p>
 
 <h4>Model description</h4>
+<p>
+The models consider the pressure rise, flow rate, speed, power consumption, and
+heat dissipation based on the user's specification.
+They can take pressure rise (head), mass flow rate, or speed (absolute or relative)
+as control signal, and compute resulting quantities based on user-provided
+performance curves.
+</p>
+<p>
+While the models in the package
+<a href=\"modelica://AixLib.Fluid.Movers\">AixLib.Fluid.Movers</a>
+allow full customization,
+preconfigured models that use the same underlying physical equations
+are available in the package
+<a href=\"modelica://AixLib.Fluid.Movers.Preconfigured\">
+AixLib.Fluid.Movers.Preconfigured</a>.
+The models in
+<a href=\"modelica://AixLib.Fluid.Movers\">AixLib.Fluid.Movers</a>
+can also be parameterized with the data records from
+<a href=\"modelica://AixLib.Fluid.Movers.Data\">
+AixLib.Fluid.Movers.Data</a>.
+</p>
+
 <p>A detailed description of the fan and pump models can be
 found in
 <a href=\"modelica://AixLib/Resources/Images/Fluid/Movers/UsersGuide/2013-IBPSA-Wetter.pdf\">Wetter (2013)</a>.
@@ -56,43 +78,54 @@ pressure</a></td>
 </tr>
 <tr>
 <td>Volume flow rate</td>
-<td>Efficiency</td>
+<td>Efficiency<br/>
+    (hydraulic or motor)</td>
 <td><a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiencyParameters\">
 efficiencyParameters</a></td>
 <td><a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiency\">
 efficiency</a></td>
 </tr>
 <tr>
+<td>Motor part load ratio</td>
+<td>Motor efficiency*</td>
+<td><a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiencyParameters_yMot\">
+efficiencyParameters_yMot</a></td>
+<td><a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiency_yMot\">
+efficiency_yMot</a></td>
+</tr>
+<tr>
 <td>Volume flow rate</td>
-<td>Power*</td>
+<td>Power**</td>
 <td><a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.powerParameters\">
 powerParameters</a></td>
 <td><a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.power\">
 power</a></td>
 </tr>
 </table>
-<p>*Note: This record should not be used
-(i.e. <code>use_powerCharacteristic</code> should be <code>false</code>)
-for the movers that take as a control signal
-the mass flow rate or the head,
-unless also values for the record <code>pressure</code> are provided.
-The reason is that for these movers the record <code>pressure</code>
-is required to be able to compute the mover speed,
-which is required to be able to compute the electrical power
-correctly using similarity laws.
-If a <code>Pressure</code> record is not provided,
-the model will internally override <code>use_powerCharacteristic=false</code>.
-In this case the efficiency records will be used.
-Note that in this case an error is still introduced,
-but it is smaller than when using the power records.
-Compare
-<a href=\"modelica://AixLib.Fluid.Movers.Validation.PowerSimplified\">
-AixLib.Fluid.Movers.Validation.PowerSimplified</a>
-with
-<a href=\"modelica://AixLib.Fluid.Movers.Validation.PowerExact\">
-AixLib.Fluid.Movers.Validation.PowerExact</a>
-for an illustration of this error.
+<p>
+Notes (applicable to
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
+AixLib.Fluid.Movers.FlowControlled_dp</a>
+and
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.FlowControlled_m_flow</a>):
 </p>
+<ul>
+<li>
+* The models will ignore this record if the nominal motor power is not provided
+and cannot be estimated from the pressure curve. This is because calculating the
+motor part load ratio requires knowing the nominal power.
+</li>
+<li>
+** The models will ignore this record if the pressure curve is not provided
+and the speed is unknown. This is because the models wouldn't be able
+to compute the elctrical power correctly using similarity laws without speed.
+In this case the user should consider using the preconfigured mover models in
+<a href=\"modelica://AixLib.Fluid.Movers.Preconfigured\">
+AixLib.Fluid.Movers.Preconfigured</a>
+which will auto-populate a pressure curve from nominal flow rate and pressure.
+</li>
+</ul>
 <p>
 These performance curves are implemented in
 <a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics\">
@@ -107,13 +140,11 @@ contains different data records.
 </p>
 <h5>Models that use performance curves for pressure rise</h5>
 <p>
-The models
+The model
 <a href=\"modelica://AixLib.Fluid.Movers.SpeedControlled_y\">
-AixLib.Fluid.Movers.SpeedControlled_y</a> and
-<a href=\"modelica://AixLib.Fluid.Movers.SpeedControlled_Nrpm\">
-AixLib.Fluid.Movers.SpeedControlled_Nrpm</a>
-take as an input either a control signal between <i>0</i> and <i>1</i>, or the
-rotational speed in units of <i>[1/min]</i>. From this input and the current flow rate,
+AixLib.Fluid.Movers.SpeedControlled_y</a>
+takes as an input a control signal between <i>0</i> and <i>1</i>.
+From this input and the current flow rate,
 they compute the pressure rise.
 This pressure rise is computed using a user-provided list of operating points that
 defines the fan or pump curve at full speed.
@@ -162,7 +193,11 @@ This will model the following pump curve for the pump input signal <code>y=1</co
 <p align=\"center\">
 <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/UsersGuide/pumpCurve.png\"/>
 </p>
-
+<p>
+See <a href=\"modelica://AixLib.Fluid.Movers.Validation.PressureCurve\">
+AixLib.Fluid.Movers.Validation.PressureCurve</a>
+for a small example that validates the pressure curve specification.
+</p>
 <h5>Models that directly control the head or the mass flow rate</h5>
 <p>
 The models <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
@@ -175,6 +210,11 @@ i.e., the fan or pump has idealized perfect control and infinite capacity.
 Using these models that take as an input the head or the mass flow rate often leads
 to smaller system of equations compared to using the models that take
 as an input the speed.
+The validation model
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.ComparePowerInput\">
+AixLib.Fluid.Movers.Validation.ComparePowerInput</a>
+demonstrates that the models with different input signals produce the same
+power consumption estimates.
 </p>
 <p>
 These models can be configured for three different control inputs.
@@ -312,7 +352,7 @@ to be enabled and a differential pressure measurement
 must be connected to
 the pump input <code>dpMea</code>.
 This functionality is demonstrated in
-<a href=\"AixLib.Fluid.Movers.Validation.FlowControlled_dpSystem\">
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.FlowControlled_dpSystem\">
 AixLib.Fluid.Movers.Validation.FlowControlled_dpSystem</a>.
 </p>
 <p>
@@ -351,6 +391,335 @@ robust model.
 However, otherwise <code>m_flow_nominal</code> does not affect the mass flow rate of the mover as
 the mass flow rate is determined by the input signal or the above explained parameters.
 </p>
+
+<h5>Electrical power consumption</h5>
+<p>
+All models compute the motor power draw <i>P<sub>ele</sub></i>,
+the hydraulic power input <i>W&#775;<sub>hyd</sub></i>, the flow work
+<i>W&#775;<sub>flo</sub></i> and the heat dissipated into the medium
+<i>Q&#775;</i>. Based on the first law, the flow work is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  W&#775;<sub>flo</sub> = | V&#775; &Delta;p |,
+</p>
+<p>
+where <i>V&#775;</i> is the volume flow rate and
+<i>&Delta;p</i> is the pressure rise.
+In order to prevent the model from producing negative mover power
+when either the flow rate or pressure rise is forced to be negative,
+the flow work <i>W&#775;<sub>flo</sub></i> is constrained to be non-negative.
+The regularisation starts around 0.01% of the characteristic maximum power
+<i>W&#775;<sub>max</sub> = V&#775;<sub>max</sub> &Delta;p<sub>max</sub></i>.
+See discussions and an example of this situation in
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1621\">IBPSA, #1621</a>.
+</p>
+<p>
+The heat dissipated into the medium is as follows:
+If the motor is cooled by the fluid, as indicated by
+<code>per.motorCooledByFluid=true</code>, then the heat dissipated into the medium is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q&#775; = P<sub>ele</sub> - W&#775;<sub>flo</sub>.
+</p>
+
+<p>
+If <code>per.motorCooledByFluid=false</code>, then the motor is outside the fluid stream,
+and only the shaft, or hydraulic, work <i>W&#775;<sub>hyd</sub></i> enters the thermodynamic
+control volume. Hence,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q&#775; = W&#775;<sub>hyd</sub> - W&#775;<sub>flo</sub>.
+</p>
+<p>The efficiencies are defined as</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&eta; = W&#775;<sub>flo</sub> &frasl; P<sub>ele</sub> = &eta;<sub>hyd</sub> &nbsp; &eta;<sub>mot</sub> <br/>
+&eta;<sub>hyd</sub> = W&#775;<sub>flo</sub> &frasl; W&#775;<sub>hyd</sub> <br/>
+&eta;<sub>mot</sub> = W&#775;<sub>hyd</sub> &frasl; P<sub>ele</sub> <br/>
+</p>
+<p>where
+<i>&eta;</i> is the total efficiency,
+<i>&eta;<sub>hyd</sub></i> is the hydraulic efficiency, and
+<i>&eta;<sub>mot</sub></i> is the motor efficiency.
+From the definition one has
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+<i>&eta; = &eta;<sub>hyd</sub> &nbsp; &eta;<sub>mot</sub></i>.
+</p>
+
+<h5>Hydraulic efficiency</h5>
+<p>
+The following options are used to specify how <i>&eta;<sub>hyd</sub></i>
+is computed.
+</p>
+<ul>
+<li>
+<code>Efficiency_VolumeFlowRate</code> -
+The user provides an array of <i>&eta;<sub>hyd</sub></i> vs. <i>V&#775;</i>.
+If the array has only one element, <i>&eta;<sub>hyd</sub></i> is considered
+constant. If the array has more than one element, the efficiency is interpolated
+or extrapolated using
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiency\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiency</a>.
+</li>
+<li>
+<code>Power_VolumeFlowRate</code> -
+The user provides an array of <i>W&#775;<sub>hyd</sub></i> vs. <i>V&#775;</i>.
+The power is interpolated or extrapolated using
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.power\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.power</a>.
+<i>&eta;<sub>hyd</sub></i> is then computed from <i>W&#775;<sub>hyd</sub></i>.
+</li>
+<li>
+<b><code>EulerNumber</code> (default 1)</b> -
+The model uses a triple <i>(&eta;<sub>hyd</sub>, V&#775;, &Delta;p)</i>
+corresponding to the operating point at which the peak efficiency is attained.
+It computes <i>&eta;<sub>hyd</sub></i> and <i>W&#775;<sub>hyd</sub></i>
+using the package
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler\">
+AixLib.Fluid.Movers.BaseClasses.Euler</a>.
+The model finds <i>&eta;<sub>hyd</sub></i> by evaluating the following correlation:
+<br/>
+<p align=\"center\">
+<img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/BaseClasses/Euler/eulerCorrelation.svg\"/>
+<br/>
+</p>
+where <i>x=log10(Eu &frasl; Eu<sub>p</sub>)</i>,
+with the subscript <i>p</i> denoting the condition where
+the mover is operating at peak efficiency.
+The Euler number is defined as
+<br/>
+<p align=\"center\" style=\"font-style:italic;\">
+Eu=(pressure forces)/(inertial forces)
+</p>
+from which one can derive the ratio of Euler numbers as<br/>
+<p align=\"center\" style=\"font-style:italic;\">
+Eu &frasl; Eu<sub>p</sub>
+=(&Delta;p &frasl; V&#775;<sup>2</sup>)
+&frasl; (&Delta;p<sub>p</sub> &frasl; V&#775;<sub>p</sub><sup>2</sup>).
+</p>
+<p>
+The peak point can be provided directly by the user or computed by calling
+the function
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Euler.getPeak\">
+AixLib.Fluid.Movers.BaseClasses.Euler.getPeak</a>.
+This function finds the peak point when both pressure and power curves are provided.
+When only the pressure curve is available, the function estimates the peak point to be at
+<i>V&#775;=V&#775;<sub>max</sub> &frasl; 2</i>.
+Examples:
+</p>
+<ul>
+<li>
+<a href=\"modelica://AixLib.Fluid.Movers.Examples.StaticReset\">
+AixLib.Fluid.Movers.Examples.StaticReset</a>
+specifies the peak point directly.
+</li>
+<li>
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Validation.EulerComparison\">
+AixLib.Fluid.Movers.BaseClasses.Validation.EulerComparison</a>
+implicitly calls the function when
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Generic\">
+AixLib.Fluid.Movers.Data.Generic</a>
+is instantiated.
+</li>
+</ul>
+<p>
+For simplicity, the implementation does not directly use this method to estimate
+<i>&eta;<sub>hyd</sub></i> at any operation point.
+Rather, it only computes a power curve at nominal speed and then uses similarity
+laws to estimate power at reduced speeds.
+Because the Euler number method does not account for the efficiency
+degradation along any curve <i>&Delta;p=kV&#775;<sup>2</sup></i>,
+these two methods are equivalent.
+See the documentation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler.power\">
+AixLib.Fluid.Movers.BaseClasses.Euler.power</a>
+for more details.
+Also see
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Validation.EulerReducedSpeed\">
+AixLib.Fluid.Movers.BaseClasses.Validation.EulerReducedSpeed</a>
+for demonstration.
+</p>
+<p>
+For more information on the Euler number method, see the documentation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Euler.correlation\">
+AixLib.Fluid.Movers.BaseClasses.Euler.correlation</a>,
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v9.6.0/EngineeringReference.pdf\">
+EnergyPlus 9.6.0 Engineering Reference</a>
+chapter 16.4 equations 16.209 through 16.218, and
+<a href=\"https://2022.american.conference.modelica.org/documents/NA_Modelica_2022_Proceedings.pdf\">
+Fu et al. (2022)</a>
+</p>
+</li>
+<li>
+<code>NotProvided</code> (default 2) - The information of this efficiency item is not provided.
+The model uses a constant value <i>&eta;<sub>hyd</sub>=0.7</i>.
+</li>
+</ul>
+
+<p>
+These options are validated in
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Validation.HydraulicEfficiencyMethods\">
+AixLib.Fluid.Movers.BaseClasses.Validation.HydraulicEfficiencyMethods</a> and
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.ComparePowerHydraulic\">
+AixLib.Fluid.Movers.Validation.ComparePowerHydraulic</a>.
+</p>
+<p>
+The model uses <code>EulerNumber</code> as the default option
+unless a pressure curve is not provided.
+In this case, the model overrides it and uses <code>NotProvided</code> instead.
+</p>
+<p>
+The user can use the same options to specify the total efficiency <i>&eta;</i>
+instead by setting <code>per.powerOrEfficiencyIsHydraulic=false</code>.
+This changes the default constant value to <i>&eta;=0.49</i> and also imposes
+an additional constraint of <i>&eta;<sub>hyd</sub> &le; 1</i> to prevent the division
+<i>&eta;<sub>hyd</sub> = &eta; &frasl; &eta;<sub>mot</sub></i>
+from producing efficiency values larger than one.
+This configuration is validated in
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Validation.TotalEfficiencyMethods\">
+AixLib.Fluid.Movers.BaseClasses.Validation.TotalEfficiencyMethods</a> and
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.ComparePowerTotal\">
+AixLib.Fluid.Movers.Validation.ComparePowerTotal</a>.
+</p>
+<p>
+Although the Euler number method is defined for <i>&eta;<sub>hyd</sub></i>,
+this implementation applies it also to <i>&eta;</i> and <i>P<sub>ele</sub></i>
+as an approximation. The basis is that <i>&eta;<sub>mot</sub></i> is mostly
+constant for motors larger than about 3.5 kW or 5 HP except when the motor
+part load drops below around 40%, (see the documentation of
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve</a>)
+which shows that <i>&eta;</i> and <i>&eta;<sub>hyd</sub></i> are roughly linear
+to each other for motors of this size.
+</p>
+
+<h5>Motor efficiency</h5>
+<p>
+The following options are used to specify how <i>&eta;<sub>mot</sub></i>
+is computed.
+</p>
+<ul>
+<li>
+<code>Efficiency_VolumeFlowRate</code> - This is same as the option for
+<i>&eta;<sub>hyd</sub></i> with the same name.
+</li>
+<li>
+<code>Efficiency_MotorPartLoadRatio</code> -
+The user provides an array of <i>&eta;<sub>mot</sub></i> vs. motor part load ratio
+<i>y<sub>mot</sub>=W<sub>hyd</sub> &frasl; P<sub>mot,nominal</sub></i>.
+The efficiency is interpolated or extrapolated using
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiency_yMot\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.efficiency_yMot</a>.
+See
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Validation.MotorEfficiencyMethods\">
+AixLib.Fluid.Movers.BaseClasses.Validation.MotorEfficiencyMethods</a>
+as an example.
+</li>
+<li>
+<b><code>GenericCurve</code> (default 1)</b> -
+The user provides the rated motor power <i>P<sub>mot,nominal</sub></i>
+and maximum motor efficiency <i>&eta;<sub>mot,max</sub></i>.
+The model then uses a generic motor efficiency curve as a function of motor PLR
+generated using
+<a href=\"Modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve\">
+AixLib.Fluid.Movers.BaseClasses.Characteristics.motorEfficiencyCurve</a>.
+The <i>&eta;<sub>mot,max</sub></i> is assumed to be 0.7 if not specified by user.
+If <i>P<sub>mot,nominal</sub></i> is unspecified, the model estimates it
+in the following ways:
+<ul>
+<li>
+If a power curve is provided,
+<ul>
+<li>
+If the curve refers to total electric power <i>P<sub>ele</sub></i>,
+<p align=\"center\" style=\"font-style:italic;\">
+P<sub>mot,nominal</sub>=
+W&#775;<sub>max</sub>,
+</p>
+where <i>W&#775;<sub>max</sub></i> is the maximum value on the provided power curve.
+</li>
+<li>
+If the curve refers to hydraulic power <i>W&#775;<sub>hyd</sub></i>,
+<p align=\"center\" style=\"font-style:italic;\">
+P<sub>mot,nominal</sub>=
+1.2 &nbsp; W&#775;<sub>max</sub>,
+</p>
+where the factor <i>1.2</i> accounts for a 20% oversize of the motor.
+</li>
+</ul>
+</li>
+<li>
+Otherwise, if only a pressure curve is provided,
+<p align=\"center\" style=\"font-style:italic;\">
+P<sub>mot,nominal</sub>=
+1.2 &nbsp; (V&#775;<sub>max</sub> &frasl; 2) &nbsp; (&Delta;p<sub>max</sub> &frasl; 2)
+&frasl; &eta;<sub>hyd,p</sub>,
+</p>
+where the factor <i>1.2</i> also assumes a 20% oversize
+and the assumed peak hydraulic efficiency <i>&eta;<sub>hyd,p</sub>=0.7</i>.
+</li>
+</ul>
+The model then computes the efficiency the same way as in the option of
+<code>Efficiency_MotorPartLoadRatio</code>.
+</li>
+<li>
+<code>NotProvided</code> (default 2) -
+The information of this efficiency item is not provided.
+The model uses a constant value <i>&eta;<sub>mot</sub>=0.7</i>.
+</li>
+</ul>
+<p>
+These options are tested in
+<a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Validation.MotorEfficiencyMethods\">
+AixLib.Fluid.Movers.BaseClasses.Validation.MotorEfficiencyMethods</a>.
+</p>
+<p>
+By default, the model uses the <code>GenericCurve</code> to obtain more accurate
+results with variable <i>&eta;<sub>mot</sub></i>. There are two exceptions:
+</p>
+<ul>
+<li>
+When neither pressure curve nor nominal motor power is provided,
+the model overrides it and uses <code>NotProvided</code> instead.
+</li>
+<li>
+When the user specifies that the provided power is total power instead of
+hydraulic power, i.e. <code>per.powerOrEfficiencyIsHydraulic==false</code>,
+the model uses <code>NotProvided</code> as default.
+The user can still mannually set it to <code>GenericCurve</code>, but this is
+not recommended. There are two reasons:
+<ol>
+<li>
+Consider the following two equations:
+<p align=\"center\" style=\"font-style:italic;\">
+&eta;<sub>mot</sub> = f(W&#775;<sub>hyd</sub>), <br/>
+P<sub>ele</sub> = W&#775;<sub>hyd</sub> &frasl; &eta;<sub>mot</sub>,
+</p>
+where <i>f(&sdot;)</i> refers to the curve of motor efficiency vs. motor PLR.
+When <i>W&#775;<sub>hyd</sub></i> is known
+(i.e. <code>per.powerOrEfficiencyIsHydraulic=true</code>),
+the unknowns are <i>&eta;<sub>mot</sub></i> and <i>P<sub>ele</sub></i>
+which can be solved explicitly. Otherwise, the unknowns are
+<i>&eta;<sub>mot</sub></i> and <i>W&#775;<sub>hyd</sub></i>,
+and an iterative solution would be required which may not converge
+for some values.
+</li>
+<li>
+If the power data provided refer to the total electric power instead of
+the hydraulic power of the mover, it is likely that the mover comes with
+built-in motors. This is often the case for small pumps whose motor is inside
+the fluid stream (such as the pumps whose data are provided in
+<a href=\"modelica://AixLib.Fluid.Movers.Data.Pumps.Wilo\">
+AixLib.Fluid.Movers.Data.Pumps.Wilo</a>).
+Because the models only use the two efficiencies to differentiate mover heat
+carried away by the fluid and dissipated to the ambient and now only a negligible
+amount of heat dissipates into the ambient, the separation of
+<i>&eta;<sub>hyd</sub></i> and <i>&eta;<sub>mot</sub></i> is then not important.
+</li>
+</ol>
+</li>
+</ul>
+
 <h5>Start-up and shut-down transients</h5>
 <p>
 All models have a parameter <code>use_inputFilter</code>. This
@@ -358,8 +727,8 @@ parameter affects the fan output as follows:
 </p>
 <ol>
 <li>
-If <code>use_inputFilter=false</code>, then the input signal <code>y</code> (or
-<code>Nrpm</code>, <code>m_flow_in</code>, or <code>dp_in</code>)
+If <code>use_inputFilter=false</code>, then the input signal <code>y</code>
+(or <code>m_flow_in</code>, or <code>dp_in</code>)
 is equal to the fan speed (or the mass flow rate or pressure rise).
 Thus, a step change in the input signal causes a step change in the fan speed (or mass flow rate or pressure rise).
 </li>
@@ -419,82 +788,6 @@ If the control loop shows oscillatory behavior, then reduce <code>k</code> and/o
 If the control loop reacts too slow, do the opposite.
 </p>
 
-<h5>Efficiency and electrical power consumption</h5>
-<p>
-All models compute the motor power draw <i>P<sub>ele</sub></i>,
-the hydraulic power input <i>W<sub>hyd</sub></i>, the flow work
-<i>W<sub>flo</sub></i> and the heat dissipated into the medium
-<i>Q</i>. Based on the first law, the flow work is
-</p>
-<p align=\"center\" style=\"font-style:italic;\">
-  W<sub>flo</sub> = | V&#775; &Delta;p |,
-</p>
-<p>
-where <i>V&#775;</i> is the volume flow rate and
-<i>&Delta;p</i> is the pressure rise.
-The heat dissipated into the medium is as follows:
-If the motor is cooled by the fluid, as indicated by
-<code>per.motorCooledByFluid=true</code>, then the heat dissipated into the medium is
-</p>
-<p align=\"center\" style=\"font-style:italic;\">
-  Q = P<sub>ele</sub> - W<sub>flo</sub>.
-</p>
-
-<p>
-If <code>per.motorCooledByFluid=false</code>, then the motor is outside the fluid stream,
-and only the shaft, or hydraulic, work <i>W<sub>hyd</sub></i> enters the thermodynamic
-control volume. Hence,
-</p>
-<p align=\"center\" style=\"font-style:italic;\">
-  Q = W<sub>hyd</sub> - W<sub>flo</sub>.
-</p>
-<p>The efficiencies are computed as</p>
-<p align=\"center\" style=\"font-style:italic;\">
-  &eta; = W<sub>flo</sub> &frasl; P<sub>ele</sub> = &eta;<sub>hyd</sub> &nbsp; &eta;<sub>mot</sub> <br/>
-  &eta;<sub>hyd</sub> = W<sub>flo</sub> &frasl; W<sub>hyd</sub> <br/>
-  &eta;<sub>mot</sub> = W<sub>hyd</sub> &frasl; P<sub>ele</sub> <br/>
-</p>
-<p>where
-<i>&eta;<sub>hyd</sub></i> is the hydraulic efficiency,
-<i>&eta;<sub>mot</sub></i> is the motor efficiency and
-<i>Q</i> is the heat released by the motor.
-</p>
-<p>
-If <code>per.use_powerCharacteristic=true</code>,
-then a set of data points for the power <i>P<sub>ele</sub></i> for different
-volume flow rates at full speed needs to be provided by the user.
-Using the flow work <i>W<sub>flo</sub></i> and the electrical power input
-<i>P<sub>ele</sub></i>, the total efficiency is computed as
-</p>
-<p align=\"center\" style=\"font-style:italic;\">
-  &eta; = W<sub>flo</sub> &frasl; P<sub>ele</sub>, <br/>
-</p>
-<p>
-and the two efficiencies
-<i>&eta;<sub>hyd</sub></i>
-and <i>&eta;<sub>mot</sub></i> are computed as
-</p>
-<p align=\"center\" style=\"font-style:italic;\">
-  &eta;<sub>hyd</sub> = 1,<br/>
-  &eta;<sub>mot</sub> = &eta;.
-</p>
-<p>
-However, if <code>per.use_powerCharacteristic=false</code>, then
-performance data for
-<i>&eta;<sub>hyd</sub></i> and
- <i>&eta;<sub>mot</sub></i> need to be provided by the user, and hence
-the model computes
-</p>
-<p align=\"center\" style=\"font-style:italic;\">
-  &eta; = &eta;<sub>hyd</sub> &nbsp; &eta;<sub>mot</sub><br/>
-  P<sub>ele</sub> = W<sub>flo</sub> &frasl; &eta;.
-</p>
-
-<p>
-The efficiency data for the motor are a list of points
-<i>V&#775;</i> and <i>&eta;<sub>mot</sub></i>.
-</p>
-
 <h5>Fluid volume of the component</h5>
 <p>
 All models can be configured to have a fluid volume at the low-pressure side.
@@ -550,6 +843,10 @@ These functions are implemented in
 <a href=\"modelica://AixLib.Fluid.Movers.BaseClasses.Characteristics\">
 AixLib.Fluid.Movers.BaseClasses.Characteristics</a>.
 </li>
+<li>
+The efficiency calculation is different, in particular, the models in this package allow
+use of the Euler number to compute the hydraulic efficiency.
+</li>
 </ul>
 <h4>References</h4>
 <p>
@@ -560,6 +857,17 @@ boundary condition and control signal.</a>
 <i>Proc. of the 13th Conference of the International Building Performance
 Simulation Association</i>, p. 3505-3512. Chambery, France. August 2013.
 </p>
+<p>
+Hongxiang Fu, David Blum, Michael Wetter.
+Fan and Pump Efficiency in Modelica based on the Euler Number.
+<i>Proc. of the American Modelica Conference 2022</i>, p. 19-25.
+Dallas, TX, USA. October 2022.
+<a href=\"https://doi.org/10.3384/ECP2118619\">https://doi.org/10.3384/ECP2118619</a>
+</p>
+<p>
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v9.6.0/EngineeringReference.pdf\">
+EnergyPlus 9.6.0 Engineering Reference</a>
+</p>
 </html>"));
 
 end UsersGuide;
diff --git a/AixLib/Fluid/Movers/Validation/BaseClasses/ComparePower.mo b/AixLib/Fluid/Movers/Validation/BaseClasses/ComparePower.mo
new file mode 100644
index 0000000000..e1397370de
--- /dev/null
+++ b/AixLib/Fluid/Movers/Validation/BaseClasses/ComparePower.mo
@@ -0,0 +1,126 @@
+within AixLib.Fluid.Movers.Validation.BaseClasses;
+model ComparePower
+  "Base class for validation models that compare power estimation methods"
+
+  package Medium = AixLib.Media.Water "Medium model";
+
+  replaceable parameter AixLib.Fluid.Movers.Data.Generic per
+    constrainedby AixLib.Fluid.Movers.Data.Generic
+    "Performance records"
+    annotation (Placement(transformation(extent={{60,60},{80,80}})));
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal =
+    per.peak.V_flow * rho_default
+    "Nominal mass flow rate";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal =
+    per.peak.dp
+    "Nominal pressure drop";
+  final parameter Modelica.Units.SI.Density rho_default=
+    Medium.density_pTX(
+      p=Medium.p_default,
+      T=Medium.T_default,
+      X=Medium.X_default) "Default medium density";
+
+  replaceable AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine mov1
+    constrainedby AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine
+    "Mover (fan or pump)"
+    annotation (Placement(transformation(extent={{-40,30},{-20,50}})));
+  replaceable AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine mov2
+    constrainedby AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine
+    "Mover (fan or pump)"
+    annotation (Placement(transformation(extent={{-40,-30},{-20,-10}})));
+  replaceable AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine mov3
+    constrainedby AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine
+    "Mover (fan or pump)"
+    annotation (Placement(transformation(extent={{-40,-80},{-20,-60}})));
+
+  AixLib.Fluid.Actuators.Dampers.Exponential damExp1(
+    redeclare final package Medium = Medium,
+    final m_flow_nominal=m_flow_nominal,
+    use_inputFilter=false,
+    final dpDamper_nominal=dp_nominal/2,
+    y_start=1,
+    final dpFixed_nominal=dp_nominal/2) "Damper"
+    annotation (Placement(transformation(extent={{40,30},{60,50}})));
+  AixLib.Fluid.Actuators.Dampers.Exponential damExp2(
+    redeclare final package Medium = Medium,
+    final m_flow_nominal=m_flow_nominal,
+    use_inputFilter=false,
+    final dpDamper_nominal=dp_nominal/2,
+    y_start=1,
+    final dpFixed_nominal=dp_nominal/2) "Damper"
+    annotation (Placement(transformation(extent={{40,-30},{60,-10}})));
+  AixLib.Fluid.Actuators.Dampers.Exponential damExp3(
+    redeclare final package Medium = Medium,
+    final m_flow_nominal=m_flow_nominal,
+    use_inputFilter=false,
+    final dpDamper_nominal=dp_nominal/2,
+    y_start=1,
+    final dpFixed_nominal=dp_nominal/2) "Damper"
+    annotation (Placement(transformation(extent={{40,-80},{60,-60}})));
+
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare final package Medium = Medium,
+    nPorts=3)
+    "Source"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  AixLib.Fluid.Sources.Boundary_pT sin(
+    redeclare final package Medium = Medium,
+    nPorts=3)
+    "Sink" annotation (Placement(transformation(extent={{100,-10},{80,10}})));
+  Modelica.Blocks.Sources.Ramp ramSpe(
+    height=1,
+    duration=60,
+    startTime=20) "Ramp signal for mover speed"
+    annotation (Placement(transformation(extent={{-80,70},{-60,90}})));
+  Modelica.Blocks.Sources.Ramp ramDam(
+    height=-1,
+    duration=60,
+    offset=1,
+    startTime=120) "Ramp signal for damper position"
+    annotation (Placement(transformation(extent={{0,70},{20,90}})));
+
+equation
+  connect(sou.ports[1], mov1.port_a)
+    annotation (Line(points={{-80,-1.33333},{-80,40},{-40,40}},
+                                                         color={0,127,255}));
+  connect(sou.ports[2], mov2.port_a)
+    annotation (Line(points={{-80,0},{-80,-20},{-40,-20}}, color={0,127,255}));
+  connect(sou.ports[3], mov3.port_a) annotation (Line(points={{-80,1.33333},{-78,
+          1.33333},{-78,0},{-80,0},{-80,-70},{-40,-70}}, color={0,127,255}));
+  connect(damExp1.port_b, sin.ports[1]) annotation (Line(points={{60,40},{80,40},
+          {80,-1.33333}},color={0,127,255}));
+  connect(ramDam.y, damExp1.y)
+    annotation (Line(points={{21,80},{50,80},{50,52}}, color={0,0,127}));
+  connect(mov2.port_b, damExp2.port_a)
+    annotation (Line(points={{-20,-20},{40,-20}}, color={0,127,255}));
+  connect(damExp2.port_b, sin.ports[2])
+    annotation (Line(points={{60,-20},{80,-20},{80,0}}, color={0,127,255}));
+  connect(mov3.port_b, damExp3.port_a)
+    annotation (Line(points={{-20,-70},{40,-70}}, color={0,127,255}));
+  connect(damExp3.port_b, sin.ports[3]) annotation (Line(points={{60,-70},{80,-70},
+          {80,1.33333}}, color={0,127,255}));
+  connect(ramDam.y, damExp2.y) annotation (Line(points={{21,80},{30,80},{30,0},
+          {50,0},{50,-8}}, color={0,0,127}));
+  connect(ramDam.y, damExp3.y) annotation (Line(points={{21,80},{30,80},{30,-50},
+          {50,-50},{50,-58}}, color={0,0,127}));
+  connect(mov1.port_b, damExp1.port_a)
+    annotation (Line(points={{-20,40},{40,40}}, color={0,127,255}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+        Documentation(info="<html>
+<p>
+This is the base class for a number of validation models that compare
+power computation of different mover model configurations.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2024, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1880\">IBPSA, #1880</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ComparePower;
diff --git a/AixLib/Fluid/Movers/Validation/BaseClasses/ControlledFlowMachine.mo b/AixLib/Fluid/Movers/Validation/BaseClasses/ControlledFlowMachine.mo
index bb93be78ab..0b0f07ecac 100644
--- a/AixLib/Fluid/Movers/Validation/BaseClasses/ControlledFlowMachine.mo
+++ b/AixLib/Fluid/Movers/Validation/BaseClasses/ControlledFlowMachine.mo
@@ -14,7 +14,7 @@ model ControlledFlowMachine
     use_p_in=false,
     p=101325,
     T=293.15,
-    nPorts=4) annotation (Placement(transformation(extent={{-90,20},{-70,40}})));
+    nPorts=3) annotation (Placement(transformation(extent={{-90,20},{-70,40}})));
 
   AixLib.Fluid.Sensors.MassFlowRate masFloRat1(redeclare package Medium =
         Medium)
@@ -23,18 +23,21 @@ model ControlledFlowMachine
         Medium) annotation (Placement(transformation(
         extent={{10,-10},{-10,10}},
         origin={-10,32})));
+  replaceable
   AixLib.Fluid.Movers.SpeedControlled_y fan1(
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     redeclare AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos32slash1to12 per)
+    constrainedby AixLib.Fluid.Movers.SpeedControlled_y
+    "Fan with normalized control input between 0 and 1"
     annotation (Placement(transformation(extent={{-20,50},{0,70}})));
-  FixedResistances.PressureDrop dp1(
+  AixLib.Fluid.FixedResistances.PressureDrop dp1(
     redeclare package Medium = Medium,
     from_dp=true,
     m_flow_nominal=0.006,
     dp_nominal=50000) "Pressure drop"
     annotation (Placement(transformation(extent={{16,50},{36,70}})));
-  FixedResistances.PressureDrop dp2(
+  AixLib.Fluid.FixedResistances.PressureDrop dp2(
     redeclare package Medium = Medium,
     from_dp=true,
     m_flow_nominal=0.006,
@@ -43,7 +46,7 @@ model ControlledFlowMachine
   AixLib.Fluid.Sensors.MassFlowRate masFloRat2(
     redeclare package Medium = Medium)
     annotation (Placement(transformation(extent={{60,-30},{80,-10}})));
-  FixedResistances.PressureDrop dp3(
+  AixLib.Fluid.FixedResistances.PressureDrop dp3(
     redeclare package Medium = Medium,
     from_dp=true,
     m_flow_nominal=0.006,
@@ -52,64 +55,48 @@ model ControlledFlowMachine
   AixLib.Fluid.Sensors.MassFlowRate masFloRat3(
     redeclare package Medium = Medium)
     annotation (Placement(transformation(extent={{60,-70},{80,-50}})));
+  replaceable
   AixLib.Fluid.Movers.FlowControlled_dp fan3(
     redeclare package Medium = Medium,
     m_flow_nominal=6000/3600*1.2,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     redeclare AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos32slash1to12 per)
+    constrainedby AixLib.Fluid.Movers.FlowControlled_dp
+    "Fan with head as input"
     annotation (Placement(transformation(extent={{-20,-70},{0,-50}})));
+  replaceable
   AixLib.Fluid.Movers.FlowControlled_m_flow fan2(
     redeclare package Medium = Medium,
     m_flow_nominal=6000/3600*1.2,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     redeclare AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos32slash1to12 per)
+    constrainedby AixLib.Fluid.Movers.FlowControlled_m_flow
+    "Fan with mass flow rate as input"
     annotation (Placement(transformation(extent={{-20,-30},{0,-10}})));
-  FixedResistances.PressureDrop dp4(
-    redeclare package Medium = Medium,
-    from_dp=true,
-    m_flow_nominal=0.006,
-    dp_nominal=50000) "Pressure drop"
-    annotation (Placement(transformation(extent={{16,100},{36,120}})));
-  AixLib.Fluid.Sensors.MassFlowRate masFloRat4(
-    redeclare package Medium = Medium)
-    annotation (Placement(transformation(extent={{60,100},{80,120}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm fan4(
-    redeclare package Medium = Medium,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
-    redeclare AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos32slash1to12 per)
-    annotation (Placement(transformation(extent={{-20,100},{0,120}})));
-  Modelica.Blocks.Math.Gain gain(k=3580) "Converts y to nominal rpm"
-    annotation (Placement(transformation(extent={{-60,130},{-40,150}})));
-  FixedResistances.PressureDrop dp5(
+  AixLib.Fluid.FixedResistances.PressureDrop dp5(
     m_flow_nominal=6000/3600*1.2,
     redeclare package Medium = Medium,
     dp_nominal=300,
     from_dp=true) "Pressure drop"
     annotation (Placement(transformation(extent={{-52,50},{-32,70}})));
-  FixedResistances.PressureDrop dp6(
+  AixLib.Fluid.FixedResistances.PressureDrop dp6(
     m_flow_nominal=6000/3600*1.2,
     redeclare package Medium = Medium,
     dp_nominal=300,
     from_dp=true) "Pressure drop"
     annotation (Placement(transformation(extent={{-52,-30},{-32,-10}})));
-  FixedResistances.PressureDrop dp7(
+  AixLib.Fluid.FixedResistances.PressureDrop dp7(
     m_flow_nominal=6000/3600*1.2,
     redeclare package Medium = Medium,
     dp_nominal=300,
     from_dp=true) "Pressure drop"
     annotation (Placement(transformation(extent={{-52,-70},{-32,-50}})));
-  FixedResistances.PressureDrop dp8(
-    m_flow_nominal=6000/3600*1.2,
-    redeclare package Medium = Medium,
-    dp_nominal=300,
-    from_dp=true) "Pressure drop"
-    annotation (Placement(transformation(extent={{-52,100},{-32,120}})));
   AixLib.Fluid.Sources.Boundary_pT sin(
     redeclare package Medium = Medium,
     use_p_in=false,
     p=101325,
     T=293.15,
-    nPorts=4) annotation (Placement(transformation(extent={{142,20},{122,40}})));
+    nPorts=3) annotation (Placement(transformation(extent={{142,20},{122,40}})));
 equation
 
   connect(fan1.port_a, relPre.port_b) annotation (Line(
@@ -127,21 +114,12 @@ equation
   connect(fan3.port_b, dp3.port_a) annotation (Line(
       points={{5.55112e-16,-60},{16,-60}},
       color={0,127,255}));
-  connect(fan4.port_b, dp4.port_a) annotation (Line(
-      points={{5.55112e-16,110},{16,110}},
-      color={0,127,255}));
-  connect(gain.y, fan4.Nrpm) annotation (Line(
-      points={{-39,140},{-10,140},{-10,122}},
-      color={0,0,127}));
   connect(masFloRat1.m_flow, fan2.m_flow_in) annotation (Line(
-      points={{70,71},{70,86},{42,86},{42,4},{-10.2,4},{-10.2,-8}},
+      points={{70,71},{70,86},{42,86},{42,4},{-10,4},{-10,-8}},
       color={0,0,127}));
   connect(relPre.p_rel, fan3.dp_in) annotation (Line(
       points={{-10,23},{-10,8},{-24,8},{-24,-40},{-10,-40},{-10,-48}},
       color={0,0,127}));
-  connect(dp8.port_b, fan4.port_a) annotation (Line(
-      points={{-32,110},{-20,110}},
-      color={0,127,255}));
   connect(dp5.port_b, fan1.port_a) annotation (Line(
       points={{-32,60},{-20,60}},
       color={0,127,255}));
@@ -154,23 +132,14 @@ equation
   connect(y.y, fan1.y) annotation (Line(
       points={{-119,80},{-10,80},{-10,72}},
       color={0,0,127}));
-  connect(y.y, gain.u) annotation (Line(
-      points={{-119,80},{-80,80},{-80,140},{-62,140}},
-      color={0,0,127}));
-  connect(dp8.port_a, sou.ports[1]) annotation (Line(
-      points={{-52,110},{-62,110},{-62,33},{-70,33}},
-      color={0,127,255}));
-  connect(dp5.port_a, sou.ports[2]) annotation (Line(
-      points={{-52,60},{-60,60},{-60,31},{-70,31}},
+  connect(dp5.port_a, sou.ports[1]) annotation (Line(
+      points={{-52,60},{-60,60},{-60,28.6667},{-70,28.6667}},
       color={0,127,255}));
-  connect(dp6.port_a, sou.ports[3]) annotation (Line(
-      points={{-52,-20},{-60,-20},{-60,29},{-70,29}},
+  connect(dp6.port_a, sou.ports[2]) annotation (Line(
+      points={{-52,-20},{-60,-20},{-60,30},{-70,30}},
       color={0,127,255}));
-  connect(dp7.port_a, sou.ports[4]) annotation (Line(
-      points={{-52,-60},{-62,-60},{-62,27},{-70,27}},
-      color={0,127,255}));
-  connect(dp4.port_b, masFloRat4.port_a) annotation (Line(
-      points={{36,110},{60,110}},
+  connect(dp7.port_a, sou.ports[3]) annotation (Line(
+      points={{-52,-60},{-62,-60},{-62,31.3333},{-70,31.3333}},
       color={0,127,255}));
   connect(dp1.port_b, masFloRat1.port_a) annotation (Line(
       points={{36,60},{60,60}},
@@ -181,25 +150,31 @@ equation
   connect(dp3.port_b, masFloRat3.port_a) annotation (Line(
       points={{36,-60},{60,-60}},
       color={0,127,255}));
-  connect(masFloRat4.port_b, sin.ports[1]) annotation (Line(
-      points={{80,110},{102,110},{102,33},{122,33}},
-      color={0,127,255}));
-  connect(masFloRat1.port_b, sin.ports[2]) annotation (Line(
-      points={{80,60},{100,60},{100,31},{122,31}},
+  connect(masFloRat1.port_b, sin.ports[1]) annotation (Line(
+      points={{80,60},{100,60},{100,28.6667},{122,28.6667}},
       color={0,127,255}));
-  connect(masFloRat2.port_b, sin.ports[3]) annotation (Line(
-      points={{80,-20},{100,-20},{100,29},{122,29}},
+  connect(masFloRat2.port_b, sin.ports[2]) annotation (Line(
+      points={{80,-20},{100,-20},{100,30},{122,30}},
       color={0,127,255}));
-  connect(masFloRat3.port_b, sin.ports[4]) annotation (Line(
-      points={{80,-60},{102,-60},{102,27},{122,27}},
+  connect(masFloRat3.port_b, sin.ports[3]) annotation (Line(
+      points={{80,-60},{102,-60},{102,31.3333},{122,31.3333}},
       color={0,127,255}));
   annotation (
     Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-160,-100},{160,
             160}})),
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-160,-100},{160,160}})),
     Documentation(info="<html>
- This example demonstrates the use of the flow model with four different configuration.
- At steady-state, all flow models have the same mass flow rate and pressure difference.
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This example demonstrates the use of the flow model with four different configuration.
+At steady-state, all flow models have the same mass flow rate and pressure difference.
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Deleted the mover with <code>Nrpm</code> signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ControlledFlowMachine;
diff --git a/AixLib/Fluid/Movers/Validation/BaseClasses/FlowMachine_ZeroFlow.mo b/AixLib/Fluid/Movers/Validation/BaseClasses/FlowMachine_ZeroFlow.mo
index 4aac99fb14..6c45287b79 100644
--- a/AixLib/Fluid/Movers/Validation/BaseClasses/FlowMachine_ZeroFlow.mo
+++ b/AixLib/Fluid/Movers/Validation/BaseClasses/FlowMachine_ZeroFlow.mo
@@ -93,34 +93,32 @@ equation
     Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},{160,
             160}})),
     Documentation(info="<html>
- <p>
- This is the base class for examples that demonstrates the use of a flow machine whose flow rate transitions to zero.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- September 20, 2014, by Michael Wetter:<br/>
- Added <code>constrainedby</code> declaration for medium.
- Otherwise, the pedantic model check of
- <a href=\"modelica://AixLib.Fluid.Movers.Validation.SpeedControlled_Nrpm_Data\">
- AixLib.Fluid.Movers.Validation.SpeedControlled_Nrpm_Data</a>
- fails because water does not implemented the function
- <code>Xsaturation</code>.
- </li>
- <li>February 20, 2016, by Ruben Baetens:<br/>
- Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
- </li>
- <li>
- March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is the base class for examples that demonstrates the use of a flow machine whose flow rate transitions to zero.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>February 20, 2016, by Ruben Baetens:<br/>
+Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+September 20, 2014, by Michael Wetter:<br/>
+Added <code>constrainedby</code> declaration for medium.
+Otherwise, a pedantic model check
+fails because water does not implement the function
+<code>Xsaturation</code>.
+</li>
+<li>
+March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowMachine_ZeroFlow;
diff --git a/AixLib/Fluid/Movers/Validation/BaseClasses/package.order b/AixLib/Fluid/Movers/Validation/BaseClasses/package.order
index 6288e83081..ff75cdea3d 100644
--- a/AixLib/Fluid/Movers/Validation/BaseClasses/package.order
+++ b/AixLib/Fluid/Movers/Validation/BaseClasses/package.order
@@ -1,2 +1,3 @@
+ComparePower
 ControlledFlowMachine
 FlowMachine_ZeroFlow
diff --git a/AixLib/Fluid/Movers/Validation/ComparePowerHydraulic.mo b/AixLib/Fluid/Movers/Validation/ComparePowerHydraulic.mo
new file mode 100644
index 0000000000..a674b7357d
--- /dev/null
+++ b/AixLib/Fluid/Movers/Validation/ComparePowerHydraulic.mo
@@ -0,0 +1,96 @@
+within AixLib.Fluid.Movers.Validation;
+model ComparePowerHydraulic
+  "Compare power estimation with hydraulic power curve"
+  extends Modelica.Icons.Example;
+  extends AixLib.Fluid.Movers.Validation.BaseClasses.ComparePower(
+    redeclare replaceable AixLib.Fluid.Movers.Data.Fans.Greenheck.BIDW15 per(
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_VolumeFlowRate,
+      motorEfficiency(V_flow={0}, eta={0.7}))
+      constrainedby AixLib.Fluid.Movers.Data.Generic,
+    redeclare AixLib.Fluid.Movers.SpeedControlled_y mov1(
+      redeclare final package Medium = Medium,
+      per=per,
+      energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+      addPowerToMedium=false,
+      use_inputFilter=false),
+    redeclare AixLib.Fluid.Movers.SpeedControlled_y mov2(
+      redeclare final package Medium = Medium,
+      per(
+        powerOrEfficiencyIsHydraulic=per.powerOrEfficiencyIsHydraulic,
+        pressure=per.pressure,
+        etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.EulerNumber,
+        peak=per.peak,
+        etaMotMet=per.etaMotMet),
+      energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+      addPowerToMedium=false,
+      use_inputFilter=false),
+    redeclare AixLib.Fluid.Movers.SpeedControlled_y mov3(
+      redeclare final package Medium = Medium,
+      per(
+        powerOrEfficiencyIsHydraulic=per.powerOrEfficiencyIsHydraulic,
+        pressure=per.pressure,
+        etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate,
+        efficiency(V_flow={per.peak.V_flow}, eta={per.peak.eta}),
+        etaMotMet=per.etaMotMet),
+      energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+      addPowerToMedium=false,
+      use_inputFilter=false));
+
+equation
+  connect(ramSpe.y, mov2.y) annotation (Line(points={{-59,80},{-52,80},{-52,0},
+          {-30,0},{-30,-8}},    color={0,0,127}));
+  connect(ramSpe.y, mov3.y) annotation (Line(points={{-59,80},{-52,80},{-52,-50},
+          {-30,-50},{-30,-58}}, color={0,0,127}));
+  connect(ramSpe.y, mov1.y)
+    annotation (Line(points={{-59,80},{-30,80},{-30,52}}, color={0,0,127}));
+  annotation(experiment(Tolerance=1e-6, StopTime=200),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerHydraulic.mos"
+        "Simulate and plot"),
+        Documentation(info="<html>
+<p>
+The purpose of this validation is two-fold.
+</p>
+<p>
+First, it validates that efficiency computation is implemented correctly
+for <code>per.powerOrEfficiencyIsHydraulic=true</code>.
+The results should show that
+<i>&eta; = &eta;<sub>hyd</sub>&nbsp;&eta;<sub>mot</sub></i>
+holds.
+</p>
+<p>
+Second, it compares the power estimation results using different selections
+of <code>per.etaHydMet</code>.
+</p>
+<ul>
+<li>
+The fan <code>mov1</code> directly uses the power curve of the fan.
+</li>
+<li>
+The fan <code>mov2</code> uses the Euler number method to estimate
+the hydraulic efficiency and computer the power consumption.
+</li>
+<li>
+The fan <code>mov3</code> assumes a constant hydraulic efficiency
+to compute the power consumption.
+</li>
+</ul>
+<p>
+The three methods agree with each other when the three fans operate
+at different speeds under constant system condition.
+Their power estimates diverge when the damper closes and the system curve is
+changed. The Euler number method was able to produce results close
+to the power curves and maintained positive power consumption as the flow rate
+approached zero. However, the constant efficiency assumption was not able
+to capture this characteristic.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2024, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1880\">IBPSA, #1880</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ComparePowerHydraulic;
diff --git a/AixLib/Fluid/Movers/Validation/ComparePowerInput.mo b/AixLib/Fluid/Movers/Validation/ComparePowerInput.mo
new file mode 100644
index 0000000000..e75a69ec14
--- /dev/null
+++ b/AixLib/Fluid/Movers/Validation/ComparePowerInput.mo
@@ -0,0 +1,66 @@
+within AixLib.Fluid.Movers.Validation;
+model ComparePowerInput
+  "Compare power estimation with different input signal"
+  extends Modelica.Icons.Example;
+  extends AixLib.Fluid.Movers.Validation.BaseClasses.ComparePower(
+    redeclare AixLib.Fluid.Movers.Data.Fans.Greenheck.BIDW15 per(
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_VolumeFlowRate,
+      motorEfficiency(V_flow={0}, eta={0.7})),
+    redeclare AixLib.Fluid.Movers.SpeedControlled_y mov1(
+      redeclare final package Medium = Medium,
+      per=per,
+      energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+      addPowerToMedium=false,
+      use_inputFilter=false),
+    redeclare AixLib.Fluid.Movers.FlowControlled_dp mov2(
+      redeclare final package Medium = Medium,
+      energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+      per=per,
+      addPowerToMedium=false,
+      use_inputFilter=false,
+      m_flow_nominal=m_flow_nominal,
+      dp_nominal=dp_nominal),
+    redeclare AixLib.Fluid.Movers.FlowControlled_m_flow mov3(
+      redeclare final package Medium = Medium,
+      energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+      per=per,
+      addPowerToMedium=false,
+      use_inputFilter=false,
+      m_flow_nominal=m_flow_nominal,
+      dp_nominal=dp_nominal),
+    ramDam(height=-0.5));
+  Modelica.Blocks.Sources.RealExpression exp_dp(y=mov1.dpMachine)
+    "Expression to impose the same pressure rise"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+  Modelica.Blocks.Sources.RealExpression exp_m_flow(y=mov1.m_flow)
+    "Expression to impose the same mass flow rate"
+    annotation (Placement(transformation(extent={{-58,-60},{-38,-40}})));
+equation
+  connect(exp_dp.y, mov2.dp_in)
+    annotation (Line(points={{-39,0},{-30,0},{-30,-8}}, color={0,0,127}));
+  connect(exp_m_flow.y, mov3.m_flow_in)
+    annotation (Line(points={{-37,-50},{-30,-50},{-30,-58}}, color={0,0,127}));
+  connect(ramSpe.y, mov1.y)
+    annotation (Line(points={{-59,80},{-30,80},{-30,52}}, color={0,0,127}));
+  annotation(experiment(Tolerance=1e-6, StopTime=200),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerInput.mos"
+        "Simulate and plot"),
+        Documentation(info="<html>
+<p>
+This validation model is similar to
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.ComparePowerHydraulic\">
+AixLib.Fluid.Movers.Validation.ComparePowerHydraulic</a>.
+It demonstrates that the mover models with different input signals
+should produce the same power computation results.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2024, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1880\">IBPSA, #1880</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ComparePowerInput;
diff --git a/AixLib/Fluid/Movers/Validation/ComparePowerTotal.mo b/AixLib/Fluid/Movers/Validation/ComparePowerTotal.mo
new file mode 100644
index 0000000000..2aa4bc79cc
--- /dev/null
+++ b/AixLib/Fluid/Movers/Validation/ComparePowerTotal.mo
@@ -0,0 +1,27 @@
+within AixLib.Fluid.Movers.Validation;
+model ComparePowerTotal
+  "Compare power estimation with total power curve"
+  extends AixLib.Fluid.Movers.Validation.ComparePowerHydraulic(
+    redeclare AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos40slash1to12 per);
+annotation(experiment(Tolerance=1e-6, StopTime=200),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerTotal.mos"
+        "Simulate and plot"),
+        Documentation(info="<html>
+<p>
+This validation model is similar to
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.ComparePowerHydraulic\">
+AixLib.Fluid.Movers.Validation.ComparePowerHydraulic</a>,
+with the difference being the fan components are replaced with pump components
+with <code>per.powerOrEfficiencyIsHydraulic=false</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 15, 2024, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1880\">IBPSA, #1880</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ComparePowerTotal;
diff --git a/AixLib/Fluid/Movers/Validation/ControlledFlowMachine.mo b/AixLib/Fluid/Movers/Validation/ControlledFlowMachine.mo
index 686ba97be2..92bd3bb04a 100644
--- a/AixLib/Fluid/Movers/Validation/ControlledFlowMachine.mo
+++ b/AixLib/Fluid/Movers/Validation/ControlledFlowMachine.mo
@@ -2,13 +2,14 @@ within AixLib.Fluid.Movers.Validation;
 model ControlledFlowMachine "Fans with different control signals as input"
   extends Modelica.Icons.Example;
   extends AixLib.Fluid.Movers.Validation.BaseClasses.ControlledFlowMachine(
-    fan4(addPowerToMedium=false, use_inputFilter=false,
+    fan1(addPowerToMedium=false, energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial),
+    fan2(
+      addPowerToMedium=false,
+      use_inputFilter=false,
       energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial),
-    fan1(addPowerToMedium=false,
-      energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial),
-    fan2(addPowerToMedium=false, use_inputFilter=false,
-      energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial),
-    fan3(addPowerToMedium=false, use_inputFilter=false,
+    fan3(
+      addPowerToMedium=false,
+      use_inputFilter=false,
       energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial));
 
   annotation (
@@ -16,14 +17,22 @@ experiment(Tolerance=1e-6, StopTime=600),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachine.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This example demonstrates the use of the flow model with four different configurations.
- At steady-state, all flow models have the same mass flow rate and pressure difference.
- Note that <code>addPowerToMedium=false</code> since otherwise,
- Dymola computes the enthalpy change of the component as a fraction <code>(k*m_flow+P_internal)/m_flow</code>
- which leads to an error because of <code>0/0</code> at zero flow rate.
- </html>",revisions="<html>
- </html>"),
+This example demonstrates the use of the flow model with four different configurations.
+At steady-state, all flow models have the same mass flow rate and pressure difference.
+Note that <code>addPowerToMedium=false</code> since otherwise,
+Dymola computes the enthalpy change of the component as a fraction <code>(k*m_flow+P_internal)/m_flow</code>
+which leads to an error because of <code>0/0</code> at zero flow rate.
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Deleted the mover with <code>Nrpm</code> signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-160,-100},{160,
-            160}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+            160}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ControlledFlowMachine;
diff --git a/AixLib/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mo b/AixLib/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mo
index 8936c2eeae..8ba864738d 100644
--- a/AixLib/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mo
+++ b/AixLib/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mo
@@ -3,7 +3,6 @@ model ControlledFlowMachineDynamic
   "Fans with different control signals as input and a dynamic speed signal"
   extends Modelica.Icons.Example;
   extends AixLib.Fluid.Movers.Validation.BaseClasses.ControlledFlowMachine(
-    fan4(energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial),
     fan1(energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial),
     fan2(energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial),
     fan3(energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial));
@@ -12,9 +11,18 @@ experiment(Tolerance=1e-6, StopTime=600),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This example demonstrates the use of the flow model with four different configurations.
- At steady-state, all flow models have the same mass flow rate and pressure difference.
- </html>"),
-Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-160,-100},{160, 160}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+This example demonstrates the use of the flow model with four different configurations.
+At steady-state, all flow models have the same mass flow rate and pressure difference.
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Deleted the mover with <code>Nrpm</code> signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+</ul>
+</html>"),
+Diagram(coordinateSystem(preserveAspectRatio=true, extent={{-160,-100},{160, 160}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ControlledFlowMachineDynamic;
diff --git a/AixLib/Fluid/Movers/Validation/FlowControlled_dp.mo b/AixLib/Fluid/Movers/Validation/FlowControlled_dp.mo
index e0afa9e192..f579f5813f 100644
--- a/AixLib/Fluid/Movers/Validation/FlowControlled_dp.mo
+++ b/AixLib/Fluid/Movers/Validation/FlowControlled_dp.mo
@@ -4,11 +4,13 @@ model FlowControlled_dp "Fan with zero mass flow rate and head as input"
  extends AixLib.Fluid.Movers.Validation.BaseClasses.FlowMachine_ZeroFlow(
     gain(k=dp_nominal),
     redeclare AixLib.Fluid.Movers.FlowControlled_dp floMacSta(
+      nominalValuesDefineDefaultPressureCurve=true,
       redeclare package Medium = Medium,
       m_flow_nominal=m_flow_nominal,
       use_inputFilter=false,
       energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState),
     redeclare AixLib.Fluid.Movers.FlowControlled_dp floMacDyn(
+      nominalValuesDefineDefaultPressureCurve=true,
       redeclare package Medium = Medium,
       m_flow_nominal=m_flow_nominal,
       use_inputFilter=false,
@@ -28,37 +30,44 @@ experiment(Tolerance=1e-06, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/FlowControlled_dp.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example demonstrates and tests the use of a flow machine whose mass flow rate is reduced to zero.
- </p>
- <p>
- The fans have been configured as steady-state models.
- This ensures that the actual speed is equal to the input signal.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 5, 2015, by Michael Wetter:<br/>
- Changed parameters of fan since the power is no longer a parameter.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/457\">issue 457</a>.
- </li>
- <li>
- September 2, 2015, by Michael Wetter:<br/>
- Changed example so that the fans use different powers, one being computed
- based on efficiency, the other based on the specified power.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/457\">issue 457</a>.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates and tests the use of a flow machine whose mass flow rate is reduced to zero.
+</p>
+<p>
+The fans have been configured as steady-state models.
+This ensures that the actual speed is equal to the input signal.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 8, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+November 5, 2015, by Michael Wetter:<br/>
+Changed parameters of fan since the power is no longer a parameter.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/457\">issue 457</a>.
+</li>
+<li>
+September 2, 2015, by Michael Wetter:<br/>
+Changed example so that the fans use different powers, one being computed
+based on efficiency, the other based on the specified power.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/457\">issue 457</a>.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowControlled_dp;
diff --git a/AixLib/Fluid/Movers/Validation/FlowControlled_dpSystem.mo b/AixLib/Fluid/Movers/Validation/FlowControlled_dpSystem.mo
index fc77ce1648..564a1ca747 100644
--- a/AixLib/Fluid/Movers/Validation/FlowControlled_dpSystem.mo
+++ b/AixLib/Fluid/Movers/Validation/FlowControlled_dpSystem.mo
@@ -23,6 +23,7 @@ model FlowControlled_dpSystem
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     allowFlowReversal=false,
+    nominalValuesDefineDefaultPressureCurve=true,
     m_flow_nominal=1,
     use_inputFilter=false) "Regular dp controlled fan"
     annotation (Placement(transformation(extent={{-80,50},{-60,70}})));
@@ -30,6 +31,7 @@ model FlowControlled_dpSystem
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     allowFlowReversal=false,
+    nominalValuesDefineDefaultPressureCurve=true,
     m_flow_nominal=1,
     use_inputFilter=false,
     prescribeSystemPressure=true)
@@ -215,26 +217,33 @@ __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/FlowControlled_dpSystem.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example demonstrates and tests the use of
- <a href=\"modelica://AixLib.Fluid.Movers.Validation.FlowControlled_dp\">
- AixLib.Fluid.Movers.Validation.FlowControlled_dp</a>
- movers that use parameter
- <code>prescribeSystemPressure</code>.
- </p>
- <p>
- The mass flow rates and actual pressure heads of the two configurations are compared.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 4 2017, by Filip Jorissen:<br/>
- First implementation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/770\">#770</a>.
- </li>
- </ul>
- </html>"),
-    Icon(coordinateSystem(extent={{-120,-120},{120,120}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates and tests the use of
+<a href=\"modelica://AixLib.Fluid.Movers.Validation.FlowControlled_dp\">
+AixLib.Fluid.Movers.Validation.FlowControlled_dp</a>
+movers that use parameter
+<code>prescribeSystemPressure</code>.
+</p>
+<p>
+The mass flow rates and actual pressure heads of the two configurations are compared.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 9, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+May 4 2017, by Filip Jorissen:<br/>
+First implementation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/770\">#770</a>.
+</li>
+</ul>
+</html>"),
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowControlled_dpSystem;
diff --git a/AixLib/Fluid/Movers/Validation/FlowControlled_m_flow.mo b/AixLib/Fluid/Movers/Validation/FlowControlled_m_flow.mo
index 48206a6637..7acc50428b 100644
--- a/AixLib/Fluid/Movers/Validation/FlowControlled_m_flow.mo
+++ b/AixLib/Fluid/Movers/Validation/FlowControlled_m_flow.mo
@@ -5,11 +5,13 @@ model FlowControlled_m_flow
  extends AixLib.Fluid.Movers.Validation.BaseClasses.FlowMachine_ZeroFlow(
     gain(k=m_flow_nominal),
     redeclare AixLib.Fluid.Movers.FlowControlled_m_flow floMacSta(
+      nominalValuesDefineDefaultPressureCurve=true,
       redeclare package Medium = Medium,
       m_flow_nominal=m_flow_nominal,
       use_inputFilter=false,
       energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState),
     redeclare AixLib.Fluid.Movers.FlowControlled_m_flow floMacDyn(
+      nominalValuesDefineDefaultPressureCurve=true,
       redeclare package Medium = Medium,
       m_flow_nominal=m_flow_nominal,
       use_inputFilter=false,
@@ -29,24 +31,31 @@ experiment(Tolerance=1e-06, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/FlowControlled_m_flow.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example demonstrates and tests the use of a flow machine whose mass flow rate is reduced to zero.
- </p>
- <p>
- The fans have been configured as steady-state models.
- This ensures that the actual speed is equal to the input signal.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates and tests the use of a flow machine whose mass flow rate is reduced to zero.
+</p>
+<p>
+The fans have been configured as steady-state models.
+This ensures that the actual speed is equal to the input signal.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 8, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FlowControlled_m_flow;
diff --git a/AixLib/Fluid/Movers/Validation/PowerExact.mo b/AixLib/Fluid/Movers/Validation/PowerExact.mo
deleted file mode 100644
index 4e0a342818..0000000000
--- a/AixLib/Fluid/Movers/Validation/PowerExact.mo
+++ /dev/null
@@ -1,44 +0,0 @@
-within AixLib.Fluid.Movers.Validation;
-model PowerExact
-  "Power calculation comparison among three mover types, using exact power computation for m_flow and dp"
-  extends PowerSimplified(
-    pump_dp(per=per),
-    pump_m_flow(per=per));
-  annotation (
-    experiment(Tolerance=1e-6, StopTime=200),
-    __Dymola_Commands(file=
-          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PowerExact.mos"
-        "Simulate and plot"),
-        Documentation(
-info="<html>
- <p>
- This example is identical to
- <a href=\"modelica://AixLib.Fluid.Movers.Validation.PowerSimplified\">
- AixLib.Fluid.Movers.Validation.PowerSimplified</a>, except that the
- performance data for the flow controlled pumps
- <code>pump_dp</code> and <code>pump_m_flow</code> contain
- the pressure curves and efficiency curves.
- The plot below shows that this leads to a computation of the power consumption
- that is identical to the one from the speed controlled pump <code>pump_Nrpm</code>.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Validation/PowerExact.png\"/>
- </p>
- </html>",
-revisions="<html>
- <ul>
- <li>
- October 15, 2021, by Hongxiang Fu:<br/>
- Fixed the image in the documentation which was cut off
- at the <i>y</i>-axis. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1533\">IBPSA, #1533</a>.
- </li>
- <li>
- March 2, 2016, by Filip Jorissen:<br/>
- First implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
-end PowerExact;
diff --git a/AixLib/Fluid/Movers/Validation/PowerSimplified.mo b/AixLib/Fluid/Movers/Validation/PowerSimplified.mo
deleted file mode 100644
index 6c38fa9d70..0000000000
--- a/AixLib/Fluid/Movers/Validation/PowerSimplified.mo
+++ /dev/null
@@ -1,182 +0,0 @@
-within AixLib.Fluid.Movers.Validation;
-model PowerSimplified
-  "Power calculation comparison among three mover types, using simplified power computation for m_flow and dp"
-  extends Modelica.Icons.Example;
-
-  package Medium = AixLib.Media.Water "Medium model";
-
-  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=3
-    "Nominal mass flow rate";
-
-  parameter Data.Pumps.Wilo.Stratos30slash1to8 per "Pump performance data"
-    annotation (Placement(transformation(extent={{50,60},{70,80}})));
-
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pump_Nrpm(
-    redeclare package Medium = Medium,
-    per=per,
-    use_inputFilter=false,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial)
-    "Pump with RPM as control signal"
-    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
-  AixLib.Fluid.Movers.FlowControlled_dp pump_dp(
-    redeclare package Medium = Medium,
-    redeclare Data.Pumps.Wilo.Stratos30slash1to8 per(
-      pressure(V_flow={0,0}, dp={0,0}),
-      use_powerCharacteristic=false,
-      hydraulicEfficiency(V_flow={0}, eta={0.3577})),
-    use_inputFilter=false,
-    m_flow_nominal=m_flow_nominal,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial)
-    "Pump with pressure rise as control signal"
-    annotation (Placement(transformation(extent={{-60,10},{-40,30}})));
-  AixLib.Fluid.Movers.FlowControlled_m_flow pump_m_flow(
-    redeclare package Medium = Medium,
-    m_flow_nominal=m_flow_nominal,
-    redeclare Data.Pumps.Wilo.Stratos30slash1to8 per(
-      pressure(V_flow={0,0}, dp={0,0}),
-      use_powerCharacteristic=false,
-      hydraulicEfficiency(V_flow={0}, eta={0.3577})),
-    use_inputFilter=false,
-    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial)
-    "Pump with mass flow rate as control signal"
-    annotation (Placement(transformation(extent={{-60,-30},{-40,-10}})));
-
-  AixLib.Fluid.Sources.Boundary_pT bou(
-    nPorts=3,
-    redeclare package Medium = Medium) "Pressure source"
-    annotation (Placement(transformation(extent={{-102,10},{-82,30}})));
-
-  AixLib.Fluid.FixedResistances.PressureDrop[3] res(
-    redeclare each package Medium = Medium,
-    each m_flow_nominal=m_flow_nominal,
-    each dp_nominal=40000) "Flow resistance"
-    annotation (Placement(transformation(extent={{20,10},{40,30}})));
-  AixLib.Fluid.Sources.Boundary_pT sink(
-    nPorts=3,
-    redeclare package Medium = Medium)
-    annotation (Placement(transformation(extent={{100,10},{80,30}})));
-  Modelica.Blocks.Sources.Ramp ramp(
-    duration=100,
-    startTime=10,
-    height=1000,
-    offset=2400) "Ramp for pump speed control signal"
-    annotation (Placement(transformation(extent={{-80,70},{-60,90}})));
-  Modelica.Blocks.Sources.RealExpression dpSet(y=pump_Nrpm.port_b.p - pump_Nrpm.port_a.p)
-    "Pressure rise across pump"
-    annotation (Placement(transformation(extent={{82,30},{6,50}})));
-  Modelica.Blocks.Sources.RealExpression m_flowSet(y=pump_Nrpm.port_a.m_flow)
-    "Pump mass flow rate"
-    annotation (Placement(transformation(extent={{82,-10},{6,10}})));
-  Modelica.Blocks.Routing.Multiplex3 result
-    annotation (Placement(transformation(extent={{20,-60},{40,-40}})));
-equation
-  connect(bou.ports[1], pump_Nrpm.port_a) annotation (Line(
-      points={{-82,22.6667},{-82,60},{-60,60}},
-      color={0,127,255}));
-  connect(pump_dp.port_a, bou.ports[2]) annotation (Line(
-      points={{-60,20},{-82,20}},
-      color={0,127,255}));
-  connect(pump_m_flow.port_a, bou.ports[3]) annotation (Line(
-      points={{-60,-20},{-82,-20},{-82,17.3333}},
-      color={0,127,255}));
-  connect(pump_Nrpm.port_b, res[1].port_a) annotation (Line(
-      points={{-40,60},{0,60},{0,20},{20,20}},
-      color={0,127,255}));
-  connect(pump_dp.port_b, res[2].port_a) annotation (Line(
-      points={{-40,20},{20,20}},
-      color={0,127,255}));
-  connect(pump_m_flow.port_b, res[3].port_a) annotation (Line(
-      points={{-40,-20},{0,-20},{0,20},{20,20}},
-      color={0,127,255}));
-  connect(sink.ports[1:3], res.port_b) annotation (Line(
-      points={{80,17.3333},{60,17.3333},{60,20},{40,20}},
-      color={0,127,255}));
-  connect(ramp.y, pump_Nrpm.Nrpm) annotation (Line(
-      points={{-59,80},{-50,80},{-50,72}},
-      color={0,0,127}));
-  connect(m_flowSet.y, pump_m_flow.m_flow_in) annotation (Line(
-      points={{2.2,0},{-50,0},{-50,-8}},
-      color={0,0,127}));
-  connect(result.u1[1], pump_Nrpm.P) annotation (Line(
-      points={{18,-43},{-30,-43},{-30,69},{-39,69}},
-      color={0,0,127}));
-  connect(result.u2[1], pump_dp.P) annotation (Line(
-      points={{18,-50},{-30,-50},{-30,29},{-39,29}},
-      color={0,0,127}));
-  connect(result.u3[1], pump_m_flow.P) annotation (Line(
-      points={{18,-57},{-30,-57},{-30,-11},{-39,-11}},
-      color={0,0,127}));
-  connect(dpSet.y, pump_dp.dp_in) annotation (Line(
-      points={{2.2,40},{-50,40},{-50,32}},
-      color={0,0,127}));
-  annotation (    experiment(Tolerance=1e-6, StopTime=200),
-    __Dymola_Commands(file=
-          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PowerSimplified.mos"
-        "Simulate and plot"),
-    Documentation(info="<html>
- <p>
- This example compares the power consumed by pumps that
- take three different control signals.
- Each pump has identical mass flow rate and pressure rise.
- </p>
- <p>
- Note that for the instances
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_dp\">
- AixLib.Fluid.Movers.FlowControlled_dp</a>
- and
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
- AixLib.Fluid.Movers.FlowControlled_m_flow</a>,
- we had to assign the efficiencies (otherwise the default constant
- efficiency of <i>0.7</i> would have been used).
- In these models, the power consumption is computed
- using similarity laws, but using the mass flow rate as opposed
- to the speed, because speed is not known in these two models.
- This is an approximation at operating points in which
- the speed is different from the nominal speed <code>N_nominal</code>
- because similarity laws are valid for speed and not for
- mass flow rate.
- </p>
- <p>
- The figure below shows the approximation error for the
- power calculation where the speed <i>N<sub>rpm</sub></i> differs from
- the nominal speed <i>N<sub>nominal</sub></i>.
- </p>
- <p align=\"center\">
- <img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Validation/PowerSimplified.png\"/>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 15, 2021, by Hongxiang Fu:<br/>
- Fixed the image in the documentation which was cut off
- at the <i>y</i>-axis. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1533\">IBPSA, #1533</a>.
- </li>
- <li>
- March 11, 2016, by Michael Wetter:<br/>
- Revised implementation by assigning the data record directly in the
- instances <code>pump_dp</code> and <code>pump_m_flow</code>, because
- using a <code>parameter</code> and assigning this <code>parameter</code> leads
- in OpenModelica to the error message
- <code>expected subtype of record AixLib.Fluid.Movers.Data.Generic</code>.
- </li>
- <li>
- March 2, 2016, by Filip Jorissen:<br/>
- Revised implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">#417</a>.
- </li>
- <li>
- November 5, 2015, by Michael Wetter:<br/>
- Changed parameters since the power is no longer a parameter for the movers
- that take mass flow rate or head as an input.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/457\">issue 457</a>.
- </li>
- <li>
- November 22, 2014, by Michael Wetter:<br/>
- Revised implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
-end PowerSimplified;
diff --git a/AixLib/Fluid/Movers/Validation/PressureCurve.mo b/AixLib/Fluid/Movers/Validation/PressureCurve.mo
new file mode 100644
index 0000000000..7cb1e059ff
--- /dev/null
+++ b/AixLib/Fluid/Movers/Validation/PressureCurve.mo
@@ -0,0 +1,71 @@
+within AixLib.Fluid.Movers.Validation;
+model PressureCurve "Displays the pressure curve of the mover"
+  extends Modelica.Icons.Example;
+
+  package Medium = AixLib.Media.Air "Medium model";
+
+  parameter Modelica.Units.SI.Density rho_default=
+    Medium.density_pTX(
+      p=Medium.p_default,
+      T=Medium.T_default,
+      X=Medium.X_default) "Default medium density";
+  parameter AixLib.Fluid.Movers.Data.Generic per(
+    pressure(V_flow={0.945419103313839, 2.83300844704353, 4.71734892787522},
+                 dp={ 3010.50788091068, 2632.22416812609, 830.122591943958}))
+    "Performance data"
+    annotation (Placement(transformation(extent={{60,60},{80,80}})));
+
+  AixLib.Fluid.Movers.SpeedControlled_y mov(
+    redeclare final package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    per=per,
+    addPowerToMedium=false,
+    y_start=1) "Mover"
+    annotation (Placement(transformation(extent={{0,-20},{20,0}})));
+  Modelica.Blocks.Sources.Constant one(final k=1) "Constant one"
+    annotation (Placement(transformation(extent={{-40,20},{-20,40}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou1(
+    redeclare final package Medium = Medium,
+    final use_m_flow_in=true,
+    nPorts=1) "Boundary that forces a mass flow rate"
+    annotation (Placement(transformation(extent={{-60,-20},{-40,0}})));
+  Modelica.Blocks.Sources.Ramp ram(
+    height=per.V_flow_max*rho_default,
+    duration=1,
+    offset=0) "Ramp signal"
+    annotation (Placement(transformation(extent={{-100,20},{-80,40}})));
+  AixLib.Fluid.Sources.Boundary_pT bou2(
+    redeclare final package Medium = Medium,
+    nPorts=1) "Boundary"
+    annotation (Placement(transformation(extent={{80,-20},{60,0}})));
+
+equation
+  connect(one.y, mov.y)
+    annotation (Line(points={{-19,30},{10,30},{10,2}},   color={0,0,127}));
+  connect(ram.y, bou1.m_flow_in) annotation (Line(points={{-79,30},{-70,30},{-70,
+          -2},{-62,-2}}, color={0,0,127}));
+  connect(bou1.ports[1], mov.port_a)
+    annotation (Line(points={{-40,-10},{0,-10}}, color={0,127,255}));
+  connect(mov.port_b, bou2.ports[1])
+    annotation (Line(points={{20,-10},{60,-10}}, color={0,127,255}));
+  annotation (experiment(Tolerance=1e-6, StopTime=1),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PressureCurve.mos"
+        "Simulate and plot"),
+        Documentation(info="
+<html>
+<p>
+This model validates the pressure curve that is specified in the instance <code>per</code>
+and provided to the mover.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 1, 2023, by Hongxiang Fu:<br/>
+First implementation. This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3371\">#3371</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PressureCurve;
diff --git a/AixLib/Fluid/Movers/Validation/PumpCurveConstruction.mo b/AixLib/Fluid/Movers/Validation/PumpCurveConstruction.mo
index 42974c0e87..2b74eb3383 100644
--- a/AixLib/Fluid/Movers/Validation/PumpCurveConstruction.mo
+++ b/AixLib/Fluid/Movers/Validation/PumpCurveConstruction.mo
@@ -154,45 +154,45 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PumpCurveConstruction.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests whether the construction of the pump curve is correct implemented
- for the cases where no data point is given at zero head, zero mass flow rate, or both.
- </p>
- <p>
- Each pump is identical, but different points on the pump curve are specified.
- However, the pump curves are linear and hence, because the pump curves are linearly
- extrapolated, all four pumps need to give the same flow rate.
- </p>
- <h4>Implementation</h4>
- <p>
- The pump curves are such that the protected parameter <code>curve</code>
- of the pumps have different values. This then tests the correct extrapolation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 6, 2016, by Michael Wetter:<br/>
- Relaxed input signal to allow simulation if bounds on min and max values are checked in Dymola.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
- </li>
- <li>February 20, 2016, by Ruben Baetens:<br/>
- Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- January 7, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example tests whether the construction of the pump curve is correct implemented
+for the cases where no data point is given at zero head, zero mass flow rate, or both.
+</p>
+<p>
+Each pump is identical, but different points on the pump curve are specified.
+However, the pump curves are linear and hence, because the pump curves are linearly
+extrapolated, all four pumps need to give the same flow rate.
+</p>
+<h4>Implementation</h4>
+<p>
+The pump curves are such that the protected parameter <code>curve</code>
+of the pumps have different values. This then tests the correct extrapolation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 6, 2016, by Michael Wetter:<br/>
+Relaxed input signal to allow simulation if bounds on min and max values are checked in Dymola.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/606\">#606</a>.
+</li>
+<li>February 20, 2016, by Ruben Baetens:<br/>
+Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+January 7, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(extent={{-100,-100},{100,120}},
           preserveAspectRatio=false), graphics),
-    Icon(coordinateSystem(extent={{-100,-100},{100,120}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{100,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PumpCurveConstruction;
diff --git a/AixLib/Fluid/Movers/Validation/PumpCurveDerivatives.mo b/AixLib/Fluid/Movers/Validation/PumpCurveDerivatives.mo
index 32a9b077e1..13b70235cf 100644
--- a/AixLib/Fluid/Movers/Validation/PumpCurveDerivatives.mo
+++ b/AixLib/Fluid/Movers/Validation/PumpCurveDerivatives.mo
@@ -1,6 +1,6 @@
 within AixLib.Fluid.Movers.Validation;
 model PumpCurveDerivatives
-  "Check for monotoneously increasing pump curve relations between Nrpm, dp and m_flow"
+  "Check for monotoneously increasing pump curve relations between y, dp and m_flow"
   extends Modelica.Icons.Example;
   package Medium = Modelica.Media.Water.ConstantPropertyLiquidWater;
 
@@ -24,14 +24,14 @@ model PumpCurveDerivatives
     startTime=0) "Ramp signal for forced mass flow rate"
     annotation (Placement(transformation(extent={{-36,60},{-24,72}})));
 
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pump1(
+  AixLib.Fluid.Movers.SpeedControlled_y pump1(
     y_start=1,
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     per=per,
     use_inputFilter=false) "Wilo Stratos pump"
     annotation (Placement(transformation(extent={{-60,30},{-40,50}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pump2(
+  AixLib.Fluid.Movers.SpeedControlled_y pump2(
     y_start=1,
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
@@ -41,12 +41,13 @@ model PumpCurveDerivatives
 
   AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump1(
     redeclare package Medium = Medium,
+    nominalValuesDefineDefaultPressureCurve=true,
     m_flow_nominal=3,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     use_inputFilter=false) "Pump for forcing a certain mass flow rate"
     annotation (Placement(transformation(extent={{38,30},{58,50}})));
 
-  Modelica.Blocks.Sources.Constant rpm1(k=1000) "Pump speed control signal"
+  Modelica.Blocks.Sources.Constant y1(k=1000/2610) "Pump speed control signal"
     annotation (Placement(transformation(extent={{-90,54},{-78,66}})));
 
   Modelica.Blocks.Math.Min min1
@@ -56,7 +57,7 @@ model PumpCurveDerivatives
         origin={35,63})));
 
   Modelica.Blocks.Sources.Constant mMax_flow(k=40/3.6)
-    "Maximum flow rate of the pump at given rpm"
+    "Maximum flow rate of the pump at given speed"
     annotation (Placement(transformation(extent={{0,46},{12,58}})));
 
   FixedResistances.PressureDrop res(
@@ -64,10 +65,10 @@ model PumpCurveDerivatives
     m_flow_nominal=40/3.6,
     dp_nominal=7e4) "Pressure drop component"
     annotation (Placement(transformation(extent={{40,-50},{60,-30}})));
-  Modelica.Blocks.Sources.Ramp m_flow1(
+  Modelica.Blocks.Sources.Ramp y2(
     duration=1,
     startTime=0,
-    height=100,
+    height=100/2610,
     offset=0) "Ramp signal for speed"
     annotation (Placement(transformation(extent={{-100,-32},{-88,-20}})));
   Sensors.RelativePressure relPre(redeclare package Medium =
@@ -83,29 +84,26 @@ model PumpCurveDerivatives
     redeclare package Medium = Medium) annotation (Placement(transformation(
         extent={{10,-10},{-10,10}},
         origin={-50,-70})));
-  Modelica.Blocks.Continuous.Derivative ddp_dNrpm(
-    initType=Modelica.Blocks.Types.Init.InitialState)
-    "Derivative of dp for changing rpm"
+  Modelica.Blocks.Continuous.Derivative ddp_dy(initType=Modelica.Blocks.Types.Init.InitialState)
+    "Derivative of dp for changing speed"
     annotation (Placement(transformation(extent={{0,-120},{20,-100}})));
   Sensors.MassFlowRate senMasFlo(redeclare package Medium = Medium)
     "Mass flow rate sensor"
     annotation (Placement(transformation(extent={{-30,-30},{-10,-50}})));
-  Modelica.Blocks.Continuous.Derivative dm_flow_dNrpm(
-    initType=Modelica.Blocks.Types.Init.InitialState)
-    "Derivative of m_flow for changing rpm"
+  Modelica.Blocks.Continuous.Derivative dm_flow_dy(initType=Modelica.Blocks.Types.Init.InitialState)
+    "Derivative of m_flow for changing speed"
     annotation (Placement(transformation(extent={{0,-80},{20,-60}})));
 equation
   connect(sou.ports[1], pump1.port_a) annotation (Line(
-      points={{-100,2},{-70,2},{-70,40},{-60,40}},
+      points={{-100,-1},{-70,-1},{-70,40},{-60,40}},
       color={0,127,255}));
   connect(forcedPump1.port_a, pump1.port_b) annotation (Line(
       points={{38,40},{-40,40}},
       color={0,127,255}));
-  connect(pump1.Nrpm, rpm1.y) annotation (Line(
-      points={{-50,52},{-50,60},{-77.4,60}},
-      color={0,0,127}));
+  connect(pump1.y, y1.y)
+    annotation (Line(points={{-50,52},{-50,60},{-77.4,60}}, color={0,0,127}));
   connect(pump2.port_a, sou.ports[2]) annotation (Line(
-      points={{-60,-40},{-70,-40},{-70,-2},{-100,-2}},
+      points={{-60,-40},{-70,-40},{-70,1},{-100,1}},
       color={0,127,255}));
 
   connect(forcedPump1.m_flow_in, min1.y) annotation (Line(
@@ -117,26 +115,26 @@ equation
   connect(mMax_flow.y, min1.u2) annotation (Line(points={{12.6,52},{18,52},{18,60},
           {29,60}}, color={0,0,127}));
   connect(forcedPump1.port_b, sin.ports[1]) annotation (Line(
-      points={{58,40},{94,40},{94,2},{110,2}},
+      points={{58,40},{94,40},{94,-1},{110,-1}},
       color={0,127,255}));
 
   connect(res.port_b, sin.ports[2]) annotation (Line(points={{60,-40},{94,-40},{
-          94,-2},{110,-2}},  color={0,127,255}));
-  connect(m_flow1.y, pump2.Nrpm) annotation (Line(points={{-87.4,-26},{-87.4,-26},
-          {-50,-26},{-50,-28}},      color={0,0,127}));
+          94,1},{110,1}},    color={0,127,255}));
+  connect(y2.y, pump2.y) annotation (Line(points={{-87.4,-26},{-87.4,-26},{-50,-26},
+          {-50,-28}}, color={0,0,127}));
   connect(ddp_dm_flow.u, relPre.p_rel) annotation (Line(points={{-2,-10},{-50,
           -10},{-50,1}},           color={0,0,127}));
   connect(relPre1.port_b, pump2.port_a) annotation (Line(points={{-60,-70},{-60,
           -70},{-60,-40}}, color={0,127,255}));
   connect(relPre1.port_a, pump2.port_b) annotation (Line(points={{-40,-70},{-40,
           -70},{-40,-40}}, color={0,127,255}));
-  connect(ddp_dNrpm.u, relPre1.p_rel) annotation (Line(points={{-2,-110},{-2,-110},
-          {-50,-110},{-50,-79}},       color={0,0,127}));
+  connect(ddp_dy.u, relPre1.p_rel) annotation (Line(points={{-2,-110},{-2,-110},
+          {-50,-110},{-50,-79}}, color={0,0,127}));
   connect(senMasFlo.port_a, pump2.port_b) annotation (Line(points={{-30,-40},{-36,
           -40},{-40,-40}},     color={0,127,255}));
   connect(senMasFlo.port_b, res.port_a)
     annotation (Line(points={{-10,-40},{14,-40},{40,-40}}, color={0,127,255}));
-  connect(senMasFlo.m_flow, dm_flow_dNrpm.u)
+  connect(senMasFlo.m_flow, dm_flow_dy.u)
     annotation (Line(points={{-20,-51},{-20,-70},{-2,-70}}, color={0,0,127}));
   connect(relPre.port_b, pump1.port_b) annotation (Line(points={{-40,10},{-40,10},
           {-40,40}},              color={0,127,255}));
@@ -148,44 +146,58 @@ __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PumpCurveDerivatives.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example checks if the pump similarity law implementation results in
- monotoneously increasing or decreasing relations between <code>dp</code>,
- <code>m_flow</code> and <code>Nrpm</code>.
- </p>
- </html>",
+<p>
+This example checks if the pump similarity law implementation results in
+monotoneously increasing or decreasing relations between <code>dp</code>,
+<code>m_flow</code> and <code>y</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- July 5, 2017, by Michael Wetter:<br/>
- Replaced exact derivative with derivative approximation, and removed the assertions.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/807\">#807</a>.
- </li>
- <li>
- April 6, 2017, by Thierry S. Nouidui:<br/>
- Added <code>experiment</code> annotation
- for JModelica verification.
- </li>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Removed duplicate <code>experiment</code> annotation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- November 26, 2014, by Filip Jorissen:<br/>
- Cleaned up implementation
- </li>
- <li>
- February 27, 2014, by Filip Jorissen:<br/>
- First implementation. See
- <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
- for a discussion and validation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 8, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Replaced the pump with <code>Nrpm</code> signal with one with <code>y</code>
+signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+July 5, 2017, by Michael Wetter:<br/>
+Replaced exact derivative with derivative approximation, and removed the assertions.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/807\">#807</a>.
+</li>
+<li>
+April 6, 2017, by Thierry S. Nouidui:<br/>
+Added <code>experiment</code> annotation
+for JModelica verification.
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Removed duplicate <code>experiment</code> annotation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+November 26, 2014, by Filip Jorissen:<br/>
+Cleaned up implementation
+</li>
+<li>
+February 27, 2014, by Filip Jorissen:<br/>
+First implementation. See
+<a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
+for a discussion and validation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(extent={{-140,-140},{140,120}},
-          preserveAspectRatio=false)),
-  __Dymola_LockedEditing="Model from IBPSA");
+          preserveAspectRatio=false)), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PumpCurveDerivatives;
diff --git a/AixLib/Fluid/Movers/Validation/Pump_stratos.mo b/AixLib/Fluid/Movers/Validation/Pump_stratos.mo
index 383b3fcd7b..658164e571 100644
--- a/AixLib/Fluid/Movers/Validation/Pump_stratos.mo
+++ b/AixLib/Fluid/Movers/Validation/Pump_stratos.mo
@@ -3,24 +3,24 @@ model Pump_stratos "Stratos pumps with speed as input"
   extends Modelica.Icons.Example;
  extends AixLib.Fluid.Movers.Validation.BaseClasses.FlowMachine_ZeroFlow(
     redeclare package Medium = AixLib.Media.Water,
-    gain(k=floMacSta.per.speed_rpm_nominal),
+    gain(k=1),
     m_flow_nominal=floMacSta.per.pressure.V_flow[3]*1000,
     dp_nominal=floMacSta.per.pressure.dp[3]/2,
-    redeclare AixLib.Fluid.Movers.SpeedControlled_Nrpm floMacSta(
+    redeclare AixLib.Fluid.Movers.SpeedControlled_y floMacSta(
       redeclare package Medium = Medium,
       use_inputFilter=false,
       per=per),
-    redeclare AixLib.Fluid.Movers.SpeedControlled_Nrpm floMacDyn(
+    redeclare AixLib.Fluid.Movers.SpeedControlled_y floMacDyn(
       redeclare package Medium = Medium,
       use_inputFilter=false,
       per=per));
   parameter Data.Pumps.Wilo.Stratos25slash1to6 per
     annotation (Placement(transformation(extent={{100,100},{120,120}})));
 equation
-  connect(gain.y, floMacSta.Nrpm) annotation (Line(
+  connect(gain.y, floMacSta.y) annotation (Line(
       points={{-25,100},{30,100},{30,92}},
       color={0,0,127}));
-  connect(gain.y, floMacDyn.Nrpm) annotation (Line(
+  connect(gain.y, floMacDyn.y) annotation (Line(
       points={{-25,100},{10,100},{10,30},{30,30},{30,12}},
       color={0,0,127}));
 
@@ -31,20 +31,27 @@ experiment(Tolerance=1e-06, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_stratos.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>This example demonstrates and tests the use of a flow machine that uses
- a performance data from a Stratos pump.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 17, 2016, by Michael Wetter:<br/>
- Updated parameter names for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
- </li>
- <li>April 18, 2014
-     by Filip Jorissen:<br/>
-        Initial version
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>This example demonstrates and tests the use of a flow machine that uses
+a performance data from a Stratos pump.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Replaced the pump with <code>Nrpm</code> signal with one with <code>y</code>
+signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+February 17, 2016, by Michael Wetter:<br/>
+Updated parameter names for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/396\">#396</a>.
+</li>
+<li>April 18, 2014
+    by Filip Jorissen:<br/>
+       Initial version
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Pump_stratos;
diff --git a/AixLib/Fluid/Movers/Validation/Pump_Nrpm_stratos.mo b/AixLib/Fluid/Movers/Validation/Pump_y_stratos.mo
similarity index 63%
rename from AixLib/Fluid/Movers/Validation/Pump_Nrpm_stratos.mo
rename to AixLib/Fluid/Movers/Validation/Pump_y_stratos.mo
index 8dd8f2fbc0..6851c79061 100644
--- a/AixLib/Fluid/Movers/Validation/Pump_Nrpm_stratos.mo
+++ b/AixLib/Fluid/Movers/Validation/Pump_y_stratos.mo
@@ -1,5 +1,5 @@
 within AixLib.Fluid.Movers.Validation;
-model Pump_Nrpm_stratos "Model validation using a Wilo Stratos 80/1-12 pump"
+model Pump_y_stratos "Model validation using a Wilo Stratos 80/1-12 pump"
   extends Modelica.Icons.Example;
   package Medium = Modelica.Media.Water.ConstantPropertyLiquidWater;
 
@@ -23,72 +23,82 @@ model Pump_Nrpm_stratos "Model validation using a Wilo Stratos 80/1-12 pump"
     offset=0) "Ramp signal for forced mass flow rate"
     annotation (Placement(transformation(extent={{-36,88},{-24,100}})));
 
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pump1(
+  AixLib.Fluid.Movers.SpeedControlled_y pump1(
     y_start=1,
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     per=per) "Wilo Stratos pump"
     annotation (Placement(transformation(extent={{-60,60},{-40,80}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pump2(
+  AixLib.Fluid.Movers.SpeedControlled_y pump2(
     y_start=1,
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     per=per) "Wilo Stratos pump"
     annotation (Placement(transformation(extent={{-60,10},{-40,30}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pump3(
+  AixLib.Fluid.Movers.SpeedControlled_y pump3(
     y_start=1,
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     per=per) "Wilo Stratos pump"
     annotation (Placement(transformation(extent={{-60,-36},{-40,-16}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pump4(
+  AixLib.Fluid.Movers.SpeedControlled_y pump4(
     y_start=1,
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     per=per) "Wilo Stratos pump"
     annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pump5(
+  AixLib.Fluid.Movers.SpeedControlled_y pump5(
     y_start=1,
     redeclare package Medium = Medium,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
     per=per) "Wilo Stratos pump"
     annotation (Placement(transformation(extent={{-60,-130},{-40,-110}})));
 
-  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump1(redeclare package
-      Medium = Medium, m_flow_nominal=3,
+  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump1(
+    redeclare package Medium = Medium,
+    nominalValuesDefineDefaultPressureCurve=true,
+    m_flow_nominal=3,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
     "Pump for forcing a certain mass flow rate"
     annotation (Placement(transformation(extent={{38,60},{58,80}})));
-  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump2(redeclare package
-      Medium = Medium, m_flow_nominal=3,
+  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump2(
+    redeclare package Medium = Medium,
+    nominalValuesDefineDefaultPressureCurve=true,
+    m_flow_nominal=3,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
     "Pump for forcing a certain mass flow rate"
     annotation (Placement(transformation(extent={{38,10},{58,30}})));
-  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump3(redeclare package
-      Medium = Medium, m_flow_nominal=3,
+  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump3(
+    redeclare package Medium = Medium,
+    nominalValuesDefineDefaultPressureCurve=true,
+    m_flow_nominal=3,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
     "Pump for forcing a certain mass flow rate"
     annotation (Placement(transformation(extent={{38,-36},{58,-16}})));
-  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump4(redeclare package
-      Medium = Medium, m_flow_nominal=3,
+  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump4(
+    redeclare package Medium = Medium,
+    nominalValuesDefineDefaultPressureCurve=true,
+    m_flow_nominal=3,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
     "Pump for forcing a certain mass flow rate"
     annotation (Placement(transformation(extent={{38,-80},{58,-60}})));
-  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump5(redeclare package
-      Medium = Medium, m_flow_nominal=3,
+  AixLib.Fluid.Movers.FlowControlled_m_flow forcedPump5(
+    redeclare package Medium = Medium,
+    nominalValuesDefineDefaultPressureCurve=true,
+    m_flow_nominal=3,
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
     "Pump for forcing a certain mass flow rate"
     annotation (Placement(transformation(extent={{38,-130},{58,-110}})));
 
-  Modelica.Blocks.Sources.Constant rpm1(k=2960) "Pump speed control signal"
+  Modelica.Blocks.Sources.Constant y1(k=2960/2610) "Pump speed control signal"
     annotation (Placement(transformation(extent={{-90,84},{-78,96}})));
-  Modelica.Blocks.Sources.Constant rpm2(k=2610) "Pump speed control signal"
+  Modelica.Blocks.Sources.Constant y2(k=2610/2610) "Pump speed control signal"
     annotation (Placement(transformation(extent={{-90,34},{-78,46}})));
-  Modelica.Blocks.Sources.Constant rpm3(k=1930) "Pump speed control signal"
+  Modelica.Blocks.Sources.Constant y3(k=1930/2610) "Pump speed control signal"
     annotation (Placement(transformation(extent={{-90,-6},{-78,6}})));
-  Modelica.Blocks.Sources.Constant rpm4(k=3300) "Pump speed control signal"
+  Modelica.Blocks.Sources.Constant y4(k=3300/2610) "Pump speed control signal"
     annotation (Placement(transformation(extent={{-90,-56},{-78,-44}})));
-  Modelica.Blocks.Sources.Constant rpm5(k=900) "Pump speed control signal"
+  Modelica.Blocks.Sources.Constant y5(k=900/2610) "Pump speed control signal"
     annotation (Placement(transformation(extent={{-90,-108},{-78,-96}})));
 
   Modelica.Blocks.Math.Min min1
@@ -118,43 +128,42 @@ model Pump_Nrpm_stratos "Model validation using a Wilo Stratos 80/1-12 pump"
         origin={35,-97})));
 
   Modelica.Blocks.Sources.Constant mMax_flow1(k=40/3.6)
-    "Maximum flow rate of the pump at given rpm"
+    "Maximum flow rate of the pump at given speed"
     annotation (Placement(transformation(extent={{2,76},{14,88}})));
   Modelica.Blocks.Sources.Constant mMax_flow2(k=55/3.6)
-    "Maximum flow rate of the pump at given rpm"
+    "Maximum flow rate of the pump at given speed"
     annotation (Placement(transformation(extent={{0,30},{12,42}})));
   Modelica.Blocks.Sources.Constant mMax_flow3(k=40/3.6)
-    "Maximum flow rate of the pump at given rpm"
+    "Maximum flow rate of the pump at given speed"
     annotation (Placement(transformation(extent={{0,-20},{12,-8}})));
   Modelica.Blocks.Sources.Constant mMax_flow4(k=22/3.6)
-    "Maximum flow rate of the pump at given rpm"
+    "Maximum flow rate of the pump at given speed"
     annotation (Placement(transformation(extent={{0,-64},{12,-52}})));
   Modelica.Blocks.Sources.Constant mMax_flow5(k=16/3.6)
-    "Maximum flow rate of the pump at given rpm"
+    "Maximum flow rate of the pump at given speed"
     annotation (Placement(transformation(extent={{0,-112},{12,-100}})));
 
 equation
   connect(sou.ports[1], pump1.port_a) annotation (Line(
-      points={{-100,-18.8},{-70,-18.8},{-70,70},{-60,70}},
+      points={{-100,-23.6},{-70,-23.6},{-70,70},{-60,70}},
       color={0,127,255}));
   connect(forcedPump1.port_a, pump1.port_b) annotation (Line(
       points={{38,70},{-40,70}},
       color={0,127,255}));
-  connect(pump1.Nrpm, rpm1.y) annotation (Line(
-      points={{-50,82},{-50,90},{-77.4,90}},
-      color={0,0,127}));
+  connect(pump1.y, y1.y)
+    annotation (Line(points={{-50,82},{-50,90},{-77.4,90}}, color={0,0,127}));
   connect(pump2.port_a, sou.ports[2]) annotation (Line(
-      points={{-60,20},{-70,20},{-70,-20.4},{-100,-20.4}},
+      points={{-60,20},{-70,20},{-70,-22.8},{-100,-22.8}},
       color={0,127,255}));
   connect(pump3.port_a, sou.ports[3]) annotation (Line(
       points={{-60,-26},{-70,-26},{-70,-22},{-100,-22}},
       color={0,127,255}));
   connect(pump4.port_a, sou.ports[4]) annotation (Line(
-      points={{-60,-70},{-70,-70},{-70,-24},{-96,-24},{-96,-23.6},{-100,-23.6}},
+      points={{-60,-70},{-70,-70},{-70,-24},{-96,-24},{-96,-21.2},{-100,-21.2}},
       color={0,127,255}));
 
   connect(pump5.port_a, sou.ports[5]) annotation (Line(
-      points={{-60,-120},{-70,-120},{-70,-25.2},{-100,-25.2}},
+      points={{-60,-120},{-70,-120},{-70,-20.4},{-100,-20.4}},
       color={0,127,255}));
   connect(pump2.port_b, forcedPump2.port_a) annotation (Line(
       points={{-40,20},{38,20}},
@@ -168,38 +177,34 @@ equation
   connect(pump5.port_b, forcedPump5.port_a) annotation (Line(
       points={{-40,-120},{38,-120}},
       color={0,127,255}));
-  connect(rpm2.y, pump2.Nrpm) annotation (Line(
-      points={{-77.4,40},{-50,40},{-50,32}},
-      color={0,0,127}));
-  connect(rpm3.y, pump3.Nrpm) annotation (Line(
-      points={{-77.4,0},{-50,0},{-50,-14}},
-      color={0,0,127}));
-  connect(rpm4.y, pump4.Nrpm) annotation (Line(
-      points={{-77.4,-50},{-50,-50},{-50,-58}},
-      color={0,0,127}));
-  connect(rpm5.y, pump5.Nrpm) annotation (Line(
-      points={{-77.4,-102},{-50,-102},{-50,-108}},
-      color={0,0,127}));
+  connect(y2.y, pump2.y)
+    annotation (Line(points={{-77.4,40},{-50,40},{-50,32}}, color={0,0,127}));
+  connect(y3.y, pump3.y)
+    annotation (Line(points={{-77.4,0},{-50,0},{-50,-14}}, color={0,0,127}));
+  connect(y4.y, pump4.y) annotation (Line(points={{-77.4,-50},{-50,-50},{-50,-58}},
+        color={0,0,127}));
+  connect(y5.y, pump5.y) annotation (Line(points={{-77.4,-102},{-50,-102},{-50,-108}},
+        color={0,0,127}));
   connect(forcedPump1.m_flow_in, min1.y) annotation (Line(
-      points={{47.8,82},{48,82},{48,91},{40.5,91}},
+      points={{48,82},{48,82},{48,91},{40.5,91}},
       color={0,0,127}));
   connect(min1.u1, m_flow.y) annotation (Line(
       points={{29,94},{-23.4,94}},
       color={0,0,127}));
   connect(min2.y, forcedPump2.m_flow_in) annotation (Line(
-      points={{40.5,45},{48,45},{48,32},{47.8,32}},
+      points={{40.5,45},{48,45},{48,32},{48,32}},
       color={0,0,127}));
   connect(min2.u1, m_flow.y) annotation (Line(
       points={{29,48},{-14,48},{-14,94},{-23.4,94}},
       color={0,0,127}));
   connect(min3.y, forcedPump3.m_flow_in) annotation (Line(
-      points={{40.5,-5},{44.25,-5},{44.25,-14},{47.8,-14}},
+      points={{40.5,-5},{44.25,-5},{44.25,-14},{48,-14}},
       color={0,0,127}));
   connect(min5.y, forcedPump5.m_flow_in) annotation (Line(
-      points={{40.5,-97},{44.25,-97},{44.25,-108},{47.8,-108}},
+      points={{40.5,-97},{44.25,-97},{44.25,-108},{48,-108}},
       color={0,0,127}));
   connect(min4.y, forcedPump4.m_flow_in) annotation (Line(
-      points={{40.5,-49},{44.25,-49},{44.25,-58},{47.8,-58}},
+      points={{40.5,-49},{44.25,-49},{44.25,-58},{48,-58}},
       color={0,0,127}));
   connect(min3.u1, m_flow.y) annotation (Line(
       points={{29,-2},{-14,-2},{-14,94},{-23.4,94}},
@@ -226,65 +231,79 @@ equation
       points={{12.6,-106},{20,-106},{20,-100},{29,-100}},
       color={0,0,127}));
   connect(forcedPump1.port_b, sin.ports[1]) annotation (Line(
-      points={{58,70},{100,70},{100,3.2},{110,3.2}},
+      points={{58,70},{100,70},{100,-1.6},{110,-1.6}},
       color={0,127,255}));
   connect(forcedPump2.port_b, sin.ports[2]) annotation (Line(
-      points={{58,20},{100,20},{100,1.6},{110,1.6}},
+      points={{58,20},{100,20},{100,-0.8},{110,-0.8}},
       color={0,127,255}));
   connect(forcedPump3.port_b, sin.ports[3]) annotation (Line(
       points={{58,-26},{100,-26},{100,0},{110,0}},
       color={0,127,255}));
   connect(forcedPump4.port_b, sin.ports[4]) annotation (Line(
-      points={{58,-70},{100,-70},{100,-2.66667},{110,-2.66667},{110,-1.6}},
+      points={{58,-70},{100,-70},{100,-2.66667},{110,-2.66667},{110,0.8}},
       color={0,127,255}));
   connect(forcedPump5.port_b, sin.ports[5]) annotation (Line(
-      points={{58,-120},{100,-120},{100,-1},{110,-1},{110,-3.2}},
+      points={{58,-120},{100,-120},{100,-1},{110,-1},{110,1.6}},
       color={0,127,255}));
 
   annotation (experiment(Tolerance=1e-08, StopTime=1000),
-__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_Nrpm_stratos.mos"
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_y_stratos.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>This example provides a validation for the Nrpm model.
- A Wilo Stratos 80/1-12 pump is simulated for five different RPMs for load
- that changes with time.
- The resulting curves for the pump head and mass flow rate are plotted
- using colored lines over the pump data sheet.
- The resulting figures are shown below.
- </p>
- <p>Pump heads:</p>
- <p><img src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Examples/PumpValidationHead.png\"
- alt=\"Pump head.\"/>
- </p>
- <p>Pump electrical power:</p>
- <p><img src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Examples/PumpValidationPower.png\"
- alt=\"Pump power.\"/></p>
- <p>The figures are adapted from the
- <a href=\"http://productfinder.wilo.com/en/COM/product/0000001700017d670001003a/fc_product_datasheet\">
- Wilo Stratos 80/1-12 data sheet</a>.
- </p>
- </html>",
+<p>This example provides a validation for the speed-controlled model.
+A Wilo Stratos 80/1-12 pump is simulated for five different speeds for load
+that changes with time.
+The resulting curves for the pump head and mass flow rate are plotted
+using colored lines over the pump data sheet.
+The resulting figures are shown below.
+</p>
+<p>Pump heads:</p>
+<p><img src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Validation/PumpValidationHead.png\"
+alt=\"Pump head.\"/>
+</p>
+<p>Pump electrical power:</p>
+<p><img src=\"modelica://AixLib/Resources/Images/Fluid/Movers/Validation/PumpValidationPower.png\"
+alt=\"Pump power.\"/></p>
+<p>The figures are adapted from the
+<a href=\"http://productfinder.wilo.com/en/COM/product/0000001700017d670001003a/fc_product_datasheet\">
+Wilo Stratos 80/1-12 data sheet</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Removed dublicate <code>experiment</code> annotation.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- November 26, 2014, by Filip Jorissen:<br/>
- Cleaned up implementation
- </li>
- <li>
- February 27, 2014, by Filip Jorissen:<br/>
- First implementation. See
- <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
- for a discussion and validation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 8, 2024, by Hongxiang Fu:<br/>
+Specified <code>nominalValuesDefineDefaultPressureCurve=true</code>
+in the mover component to suppress a warning.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3819\">#3819</a>.
+</li>
+<li>
+March 21, 2023, by Hongxiang Fu:<br/>
+Replaced the pumps with <code>Nrpm</code> signal with ones with <code>y</code>
+signal.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1704\">IBPSA, #1704</a>.
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Removed dublicate <code>experiment</code> annotation.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+November 26, 2014, by Filip Jorissen:<br/>
+Cleaned up implementation
+</li>
+<li>
+February 27, 2014, by Filip Jorissen:<br/>
+First implementation. See
+<a href=\"https://github.com/lbl-srg/modelica-buildings/pull/202\">#202</a>
+for a discussion and validation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(extent={{-140,-140},{140,120}},
-          preserveAspectRatio=false)),
-  __Dymola_LockedEditing="Model from IBPSA");
-end Pump_Nrpm_stratos;
+          preserveAspectRatio=false)), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Pump_y_stratos;
diff --git a/AixLib/Fluid/Movers/Validation/SpeedControlled_Nrpm.mo b/AixLib/Fluid/Movers/Validation/SpeedControlled_Nrpm.mo
deleted file mode 100644
index 889abafb11..0000000000
--- a/AixLib/Fluid/Movers/Validation/SpeedControlled_Nrpm.mo
+++ /dev/null
@@ -1,53 +0,0 @@
-within AixLib.Fluid.Movers.Validation;
-model SpeedControlled_Nrpm "Fan with zero mass flow rate and speed as input"
-  extends Modelica.Icons.Example;
- extends AixLib.Fluid.Movers.Validation.BaseClasses.FlowMachine_ZeroFlow(
-    gain(k=1500),
-    redeclare AixLib.Fluid.Movers.SpeedControlled_Nrpm floMacSta(
-      redeclare package Medium = Medium,
-      per(pressure(V_flow={0,m_flow_nominal,2*m_flow_nominal}/1.2,
-                  dp={2*dp_nominal,dp_nominal,0})),
-      use_inputFilter=false,
-      energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState),
-    redeclare AixLib.Fluid.Movers.SpeedControlled_Nrpm floMacDyn(
-      redeclare package Medium = Medium,
-      per(pressure(V_flow={0,m_flow_nominal,2*m_flow_nominal}/1.2,
-                   dp={2*dp_nominal,dp_nominal,0})),
-      use_inputFilter=false,
-      energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial));
-
-equation
-  connect(gain.y, floMacSta.Nrpm) annotation (Line(
-      points={{-25,100},{30,100},{30,92}},
-      color={0,0,127}));
-  connect(gain.y, floMacDyn.Nrpm) annotation (Line(
-      points={{-25,100},{10,100},{10,30},{30,30},{30,12}},
-      color={0,0,127}));
-  annotation (
-    Diagram(coordinateSystem(preserveAspectRatio=false,extent={{-100,-100},{160,
-            160}}), graphics),
-experiment(Tolerance=1e-08, StopTime=1.0),
-__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/SpeedControlled_Nrpm.mos"
-        "Simulate and plot"),
-    Documentation(info="<html>
- <p>
- This example demonstrates and tests the use of a flow machine whose mass flow rate is reduced to zero.
- </p>
- <p>
- The fans have been configured as steady-state models.
- This ensures that the actual speed is equal to the input signal.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
-end SpeedControlled_Nrpm;
diff --git a/AixLib/Fluid/Movers/Validation/SpeedControlled_y.mo b/AixLib/Fluid/Movers/Validation/SpeedControlled_y.mo
index 7e62c60920..bc913d29ec 100644
--- a/AixLib/Fluid/Movers/Validation/SpeedControlled_y.mo
+++ b/AixLib/Fluid/Movers/Validation/SpeedControlled_y.mo
@@ -31,24 +31,24 @@ experiment(Tolerance=1e-08, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/SpeedControlled_y.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example demonstrates and tests the use of a flow machine whose mass flow rate is reduced to zero.
- </p>
- <p>
- The fans have been configured as steady-state models.
- This ensures that the actual speed is equal to the input signal.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates and tests the use of a flow machine whose mass flow rate is reduced to zero.
+</p>
+<p>
+The fans have been configured as steady-state models.
+This ensures that the actual speed is equal to the input signal.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpeedControlled_y;
diff --git a/AixLib/Fluid/Movers/Validation/SpeedControlled_y_linear.mo b/AixLib/Fluid/Movers/Validation/SpeedControlled_y_linear.mo
index 362646de63..ba33406836 100644
--- a/AixLib/Fluid/Movers/Validation/SpeedControlled_y_linear.mo
+++ b/AixLib/Fluid/Movers/Validation/SpeedControlled_y_linear.mo
@@ -89,38 +89,38 @@ experiment(Tolerance=1e-06, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/SpeedControlled_y_linear.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example demonstrates and tests the use of a flow machine whose speed is reduced to zero.
- In the top model, the pressure drop across the pump is constant, and in the bottom model,
- the mass flow rate across the pump is constant.
- In the top model, a small flow resistance has been added since a pump with zero speed cannot
- produce a non-zero pressure raise. For this operating region, the pressure drop ensures that
- the model is non-singular.
- </p>
- <p>
- The fans have been configured as steady-state models.
- This ensures that the actual speed is equal to the input signal.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>February 20, 2016, by Ruben Baetens:<br/>
- Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- February 14, 2012, by Michael Wetter:<br/>
- Added filter for start-up and shut-down transient.
- </li>
- <li>
- March 24 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates and tests the use of a flow machine whose speed is reduced to zero.
+In the top model, the pressure drop across the pump is constant, and in the bottom model,
+the mass flow rate across the pump is constant.
+In the top model, a small flow resistance has been added since a pump with zero speed cannot
+produce a non-zero pressure raise. For this operating region, the pressure drop ensures that
+the model is non-singular.
+</p>
+<p>
+The fans have been configured as steady-state models.
+This ensures that the actual speed is equal to the input signal.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>February 20, 2016, by Ruben Baetens:<br/>
+Removal of <code>dynamicBalance</code> as parameter for <code>massDynamics</code> and <code>energyDynamics</code>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+February 14, 2012, by Michael Wetter:<br/>
+Added filter for start-up and shut-down transient.
+</li>
+<li>
+March 24 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpeedControlled_y_linear;
diff --git a/AixLib/Fluid/Movers/Validation/package.order b/AixLib/Fluid/Movers/Validation/package.order
index ebfb64c51f..94d372bb3e 100644
--- a/AixLib/Fluid/Movers/Validation/package.order
+++ b/AixLib/Fluid/Movers/Validation/package.order
@@ -1,15 +1,16 @@
+ComparePowerHydraulic
+ComparePowerInput
+ComparePowerTotal
 ControlledFlowMachine
 ControlledFlowMachineDynamic
 FlowControlled_dp
 FlowControlled_dpSystem
 FlowControlled_m_flow
-PowerExact
-PowerSimplified
+PressureCurve
 PumpCurveConstruction
 PumpCurveDerivatives
-Pump_Nrpm_stratos
 Pump_stratos
-SpeedControlled_Nrpm
+Pump_y_stratos
 SpeedControlled_y
 SpeedControlled_y_linear
 BaseClasses
diff --git a/AixLib/Fluid/Movers/package.order b/AixLib/Fluid/Movers/package.order
index 11de6715f7..032f8db4cc 100644
--- a/AixLib/Fluid/Movers/package.order
+++ b/AixLib/Fluid/Movers/package.order
@@ -1,10 +1,10 @@
 UsersGuide
 FlowControlled_dp
 FlowControlled_m_flow
-SpeedControlled_Nrpm
 SpeedControlled_y
 Compressors
 DpControlledMovers
+Preconfigured
 PumpsPolynomialBased
 Data
 Examples
diff --git a/AixLib/Fluid/Pools/BaseClasses/AirFlowMoistureToROM.mo b/AixLib/Fluid/Pools/BaseClasses/AirFlowMoistureToROM.mo
new file mode 100644
index 0000000000..a2b3409041
--- /dev/null
+++ b/AixLib/Fluid/Pools/BaseClasses/AirFlowMoistureToROM.mo
@@ -0,0 +1,93 @@
+within AixLib.Fluid.Pools.BaseClasses;
+model AirFlowMoistureToROM
+
+    replaceable package AirMedium =
+    Modelica.Media.Interfaces.PartialMedium "Medium in the component"
+      annotation (choices(
+        choice(redeclare package Medium = AixLib.Media.Air "Moist air"),
+        choice(redeclare package Medium = AixLib.Media.Water "Water"),
+        choice(redeclare package Medium =
+            AixLib.Media.Antifreeze.PropyleneGlycolWater (
+              property_T=293.15,
+              X_a=0.40)
+              "Propylene glycol water, 40% mass fraction")));
+
+  parameter Modelica.Fluid.Types.Dynamics energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState
+    "Type of energy balance: dynamic (3 initialization options) or steady state"
+    annotation(Evaluate=true, Dialog(tab="Dynamics", group="Equations"));
+
+  parameter Integer nPools = 1;
+
+    //Parameters to enable addition of evaporation mass flow to ROM
+  parameter Modelica.Units.SI.MassFlowRate m_flow_air_nominal=1
+    "air flow rate between swimming hall and air layer above swimming pool";
+  parameter Modelica.Units.SI.Volume VAirLay = 7500
+    "volume of air layer above pool for mass exchange due to evaporation";
+
+  Modelica.Blocks.Interfaces.RealInput QEva[nPools](final quantity=
+        "HeatFlowRate", final unit="W") "Heat due to evaporation" annotation (
+      Placement(transformation(extent={{118,26},{88,56}}), iconTransformation(
+          extent={{106,24},{82,48}})));
+  Modelica.Blocks.Interfaces.RealInput m_flow_eva[nPools]
+    "Water mass flow due to evaporation" annotation (Placement(transformation(
+          extent={{120,-44},{88,-12}}), iconTransformation(extent={{108,-50},{
+            82,-24}})));
+  MixingVolumes.MixingVolumeMoistAir AirLay(
+    redeclare package Medium = AirMedium,
+    T_start=303.15,
+    V=VAirLay,
+    energyDynamics=energyDynamics,
+    m_flow_nominal=m_flow_air_nominal,
+    nPorts=2) "Air layer above swimming pool, relevant for evaporation"
+    annotation (Placement(transformation(extent={{-4,42},{-24,62}})));
+  Movers.FlowControlled_m_flow          sou(
+    redeclare package Medium = AirMedium,
+    energyDynamics=energyDynamics,
+    m_flow_nominal=m_flow_air_nominal,
+    addPowerToMedium=false,
+    nominalValuesDefineDefaultPressureCurve=true)
+                 annotation (Placement(transformation(extent={{-24,-42},{-46,
+            -16}})));
+  Modelica.Fluid.Interfaces.FluidPort_a port_a(redeclare package Medium =
+        AirMedium)
+    "Fluid connector a (positive design flow direction is from port_a to port_b)"
+    annotation (Placement(transformation(extent={{-118,8},{-90,34}}),
+        iconTransformation(extent={{-110,14},{-90,34}})));
+  Modelica.Fluid.Interfaces.FluidPort_b port_b(redeclare package Medium =
+        AirMedium)
+    "Fluid connector a (positive design flow direction is from port_a to port_b)"
+    annotation (Placement(transformation(extent={{-112,-42},{-84,-14}}),
+        iconTransformation(extent={{-108,-34},{-88,-14}})));
+  Modelica.Blocks.Math.MultiSum Sum_m_flow_eva(nu=nPools)
+    annotation (Placement(transformation(extent={{76,-34},{64,-22}})));
+  Modelica.Blocks.Math.MultiSum SumQEva(nu=nPools)
+    annotation (Placement(transformation(extent={{76,34},{60,50}})));
+  Modelica.Blocks.Sources.RealExpression mAirExc(y=m_flow_air_nominal)
+    "Set point for water mass fraction"
+    annotation (Placement(transformation(extent={{-84,0},{-66,18}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow prescribedHeatFlow
+    annotation (Placement(transformation(extent={{48,32},{28,52}})));
+equation
+  connect(m_flow_eva, Sum_m_flow_eva.u)
+    annotation (Line(points={{104,-28},{76,-28}}, color={0,0,127}));
+  connect(Sum_m_flow_eva.y, AirLay.mWat_flow) annotation (Line(points={{62.98,
+          -28},{6,-28},{6,60},{-2,60}},
+                                     color={0,0,127}));
+  connect(sou.port_a, AirLay.ports[1])
+    annotation (Line(points={{-24,-29},{-13,-29},{-13,42}},
+                                                          color={0,127,255}));
+  connect(sou.port_b, port_b) annotation (Line(points={{-46,-29},{-72,-29},{-72,
+          -28},{-98,-28}}, color={0,127,255}));
+  connect(port_a, AirLay.ports[2]) annotation (Line(points={{-104,21},{-104,26},
+          {-15,26},{-15,42}}, color={0,127,255}));
+  connect(mAirExc.y, sou.m_flow_in)
+    annotation (Line(points={{-65.1,9},{-35,9},{-35,-13.4}}, color={0,0,127}));
+  connect(prescribedHeatFlow.port, AirLay.heatPort) annotation (Line(points={{
+          28,42},{14,42},{14,52},{-4,52}}, color={191,0,0}));
+  connect(SumQEva.y, prescribedHeatFlow.Q_flow)
+    annotation (Line(points={{58.64,42},{48,42}}, color={0,0,127}));
+  connect(QEva, SumQEva.u) annotation (Line(points={{103,41},{89.5,41},{89.5,42},
+          {76,42}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)));
+end AirFlowMoistureToROM;
diff --git a/AixLib/Fluid/Pools/BaseClasses/HeatTransferConduction.mo b/AixLib/Fluid/Pools/BaseClasses/HeatTransferConduction.mo
new file mode 100644
index 0000000000..e1500a0602
--- /dev/null
+++ b/AixLib/Fluid/Pools/BaseClasses/HeatTransferConduction.mo
@@ -0,0 +1,169 @@
+within AixLib.Fluid.Pools.BaseClasses;
+model HeatTransferConduction
+  "Heat transfer due to conduction through pool walls"
+
+  parameter Modelica.Fluid.Types.Dynamics energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState
+    "Type of energy balance: dynamic (3 initialization options) or steady state"
+    annotation(Evaluate=true, Dialog(tab="Dynamics", group="Equations"));
+
+  parameter Modelica.Units.SI.Area AWalInt "Area of pool walls which is connected to inner rooms (inner pool walls)";
+  parameter Modelica.Units.SI.Area AWalExt "Area of pool walls which is connected to the ground (pool wall with earth contact)";
+  parameter Modelica.Units.SI.Area AFloInt "Area of pool floors which is connected to inner rooms (inner pool floor)";
+  parameter Modelica.Units.SI.Area AFloExt "Area of pool floors which is connected to teh ground (pool floor with earth contact)";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConWaterHorizontal "Mean value for the heat transfer coefficient of free convection on horizontal pool floors";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConWaterVertical "Mean value for the heat transfer coefficient of free convection on vertical pool walls";
+
+  parameter Modelica.Units.SI.Temperature TPool "Set temperature for pool";
+
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature HeatFlowOuter
+    "Generate Heat Flow for earth contact" annotation (Placement(transformation(
+        extent={{-6,-6},{6,6}},
+        rotation=180,
+        origin={74,-28})));
+
+  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a heatport_a
+    "Inlet for heattransfer"  annotation (Placement(transformation(extent={{-116,
+            -14},{-90,12}}),
+        iconTransformation(extent={{-116,-14},{-90,12}})));
+
+  Modelica.Blocks.Interfaces.RealInput TSoil "Temperature of Soil" annotation (Placement(transformation(extent={{130,-48},
+            {90,-8}}),
+        iconTransformation(extent={{126,16},{86,56}})));
+
+  AixLib.ThermalZones.HighOrder.Components.Walls.BaseClasses.SimpleNLayer
+    InnerPoolFloor(
+    A=AFloInt,
+    wallRec=PoolWall,
+    T_start=fill(TPool, PoolWall.n),
+    energyDynamics=energyDynamics)
+             annotation (Placement(transformation(extent={{-2,-32},{22,-8}})));
+  AixLib.Utilities.HeatTransfer.HeatConvInside HeatConvWaterHorizontalInner(
+    hCon_const=hConWaterHorizontal,
+    A=AFloInt,
+    calcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon,
+    surfaceOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall)
+                  annotation (Placement(transformation(
+        origin={-50,-20},
+        extent={{-10,-10},{10,10}},
+        rotation=180)));
+  AixLib.Utilities.HeatTransfer.HeatConvInside HeatConvWaterVerticalOuter(
+    hCon_const=hConWaterVertical,
+    A=AWalExt,
+    calcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon,
+    surfaceOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall)  annotation (Placement(transformation(
+        origin={-50,40},
+        extent={{-10,-10},{10,10}},
+        rotation=180)));
+  AixLib.ThermalZones.HighOrder.Components.Walls.BaseClasses.SimpleNLayer
+    PoolWallWithEarthContact(
+    A=AWalExt,
+    wallRec=PoolWall,
+    T_start=fill(TPool, PoolWall.n),
+    energyDynamics=energyDynamics)
+             annotation (Placement(transformation(extent={{-2,28},{22,52}})));
+  AixLib.Utilities.HeatTransfer.HeatConvInside HeatConvWaterHorizontalOuter(
+    hCon_const=hConWaterHorizontal,
+    A=AFloExt,
+    calcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon,
+    surfaceOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall)  annotation (Placement(transformation(
+        origin={-50,-60},
+        extent={{-10,-10},{10,10}},
+        rotation=180)));
+  AixLib.ThermalZones.HighOrder.Components.Walls.BaseClasses.SimpleNLayer
+    PoolFloorWithEarthContact(
+    A=AFloExt,
+    wallRec=PoolWall,
+    T_start=fill(TPool, PoolWall.n),
+    energyDynamics=energyDynamics)
+             annotation (Placement(transformation(extent={{-2,-72},{22,-50}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow
+    prescribedHeatFlow1 "Generate Heat Flow for earth contact"
+                           annotation (Placement(transformation(
+        extent={{-6,-6},{6,6}},
+        rotation=180,
+        origin={44,12})));
+  AixLib.ThermalZones.HighOrder.Components.Walls.BaseClasses.SimpleNLayer
+    InnerPoolWall(
+    A=AWalInt,
+    wallRec=PoolWall,
+    T_start=fill(TPool, PoolWall.n),
+    energyDynamics=energyDynamics)
+             annotation (Placement(transformation(extent={{-2,68},{22,92}})));
+  Modelica.Blocks.Sources.RealExpression HeatFlowInner(y=0)
+    "Inner pool walls are not connected to other zones, only outer pool walls have earth contact"
+    annotation (Placement(transformation(extent={{96,2},{76,22}})));
+  AixLib.Utilities.HeatTransfer.HeatConvInside HeatConvWaterVerticalInner(
+    hCon_const=hConWaterVertical,
+    A=AWalInt,
+    calcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon,
+    surfaceOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall)  annotation (Placement(transformation(
+        origin={-50,80},
+        extent={{-10,-10},{10,10}},
+        rotation=180)));
+  replaceable parameter AixLib.DataBase.Walls.WallBaseDataDefinition PoolWall
+    "Wall type for pool walls, record contains all wall layers"
+    annotation (Placement(transformation(extent={{76,-98},{96,-78}})));
+equation
+  connect(HeatFlowOuter.T, TSoil)
+    annotation (Line(points={{81.2,-28},{110,-28}}, color={0,0,127}));
+  connect(heatport_a, heatport_a)
+    annotation (Line(points={{-103,-1},{-103,-1}}, color={191,0,0}));
+  connect(HeatConvWaterHorizontalInner.port_a, InnerPoolFloor.port_a)
+    annotation (Line(points={{-40,-20},{-2,-20}},  color={191,0,0}));
+  connect(PoolFloorWithEarthContact.port_b, HeatFlowOuter.port) annotation (
+      Line(points={{22,-61},{58,-61},{58,-28},{68,-28}}, color={191,0,0}));
+  connect(PoolFloorWithEarthContact.port_a, HeatConvWaterHorizontalOuter.port_a)
+    annotation (Line(points={{-2,-61},{-2,-60},{-40,-60}},   color={191,0,0}));
+  connect(InnerPoolWall.port_b, prescribedHeatFlow1.port) annotation (Line(
+        points={{22,80},{30,80},{30,12},{38,12}}, color={191,0,0}));
+  connect(HeatConvWaterVerticalOuter.port_b, heatport_a) annotation (Line(
+        points={{-60,40},{-72,40},{-72,-1},{-103,-1}}, color={191,0,0}));
+  connect(HeatConvWaterHorizontalInner.port_b, heatport_a) annotation (Line(
+        points={{-60,-20},{-72,-20},{-72,-1},{-103,-1}}, color={191,0,0}));
+  connect(HeatConvWaterHorizontalOuter.port_b, heatport_a) annotation (Line(
+        points={{-60,-60},{-72,-60},{-72,-1},{-103,-1}}, color={191,0,0}));
+  connect(prescribedHeatFlow1.Q_flow, HeatFlowInner.y)
+    annotation (Line(points={{50,12},{75,12}}, color={0,0,127}));
+  connect(HeatFlowOuter.port, PoolWallWithEarthContact.port_b) annotation (Line(
+        points={{68,-28},{58,-28},{58,40},{22,40}}, color={191,0,0}));
+  connect(InnerPoolFloor.port_b, prescribedHeatFlow1.port) annotation (Line(
+        points={{22,-20},{30,-20},{30,12},{38,12}}, color={191,0,0}));
+  connect(HeatConvWaterVerticalOuter.port_a, PoolWallWithEarthContact.port_a)
+    annotation (Line(points={{-40,40},{-2,40}}, color={191,0,0}));
+  connect(InnerPoolWall.port_a, HeatConvWaterVerticalInner.port_a) annotation (
+      Line(points={{-2,80},{-40,80}},                   color={191,0,0}));
+  connect(HeatConvWaterVerticalInner.port_b, heatport_a) annotation (Line(
+        points={{-60,80},{-72,80},{-72,-1},{-103,-1}},color={191,0,0}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-80,58},{28,-26}},
+          lineColor={28,108,200},
+          fillColor={28,108,200},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{28,68},{48,-46}},
+          lineColor={135,135,135},
+          fillColor={175,175,175},
+          fillPattern=FillPattern.Forward),
+        Rectangle(
+          extent={{-86,-26},{30,-46}},
+          lineColor={135,135,135},
+          fillColor={175,175,175},
+          fillPattern=FillPattern.Forward),
+        Polygon(
+          points={{-16,-10},{-4,6},{58,-52},{46,-62},{-16,-10}},
+          lineColor={238,46,47},
+          fillColor={238,46,47},
+          fillPattern=FillPattern.Solid),
+        Polygon(
+          points={{32,-68},{36,-66},{62,-38},{76,-78},{32,-68}},
+          lineColor={238,46,47},
+          fillColor={238,46,47},
+          fillPattern=FillPattern.Solid),
+        Rectangle(extent={{-100,100},{100,-100}}, lineColor={0,0,0})}),
+                                                                 Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+    <p>This model is a base model to calculate the heat transfer through pool walls. The pool walls are  divided in: vertical walls without earth contact, vertical walls with earth contact, pool floor without earth contact, pool floor with earth contact.</p>
+</html>"));
+end HeatTransferConduction;
diff --git a/AixLib/Fluid/Pools/BaseClasses/package.mo b/AixLib/Fluid/Pools/BaseClasses/package.mo
new file mode 100644
index 0000000000..fb7f0d7029
--- /dev/null
+++ b/AixLib/Fluid/Pools/BaseClasses/package.mo
@@ -0,0 +1,6 @@
+within AixLib.Fluid.Pools;
+package BaseClasses
+    extends Modelica.Icons.BasesPackage;
+
+
+end BaseClasses;
diff --git a/AixLib/Fluid/Pools/BaseClasses/package.order b/AixLib/Fluid/Pools/BaseClasses/package.order
new file mode 100644
index 0000000000..670c315541
--- /dev/null
+++ b/AixLib/Fluid/Pools/BaseClasses/package.order
@@ -0,0 +1,3 @@
+AirFlowMoistureToROM
+HeatTransferConduction
+waveMachine
diff --git a/AixLib/Fluid/Pools/BaseClasses/waveMachine.mo b/AixLib/Fluid/Pools/BaseClasses/waveMachine.mo
new file mode 100644
index 0000000000..e498df7091
--- /dev/null
+++ b/AixLib/Fluid/Pools/BaseClasses/waveMachine.mo
@@ -0,0 +1,93 @@
+within AixLib.Fluid.Pools.BaseClasses;
+model waveMachine "Calculate energy demands of a wave machine"
+
+  parameter Modelica.Units.SI.Length heightWave "Height of generated wave";
+  parameter Modelica.Units.SI.Length widthWave
+    "Width of generated wave/ width of wave machineoutlet";
+  parameter Modelica.Units.SI.Time timeWavePul_start
+    "Start time of first wave cycle";
+  parameter Modelica.Units.SI.Time periodeWavePul "Time of cycling period";
+  parameter Real widthWavePul "Fraction of time of wave generation within cycling period";
+
+  Modelica.Blocks.Math.RealToBoolean useWavePool(threshold=1)
+    "If input = 1, then true, else no waves generated"
+    annotation (Placement(transformation(extent={{-58,-8},{-42,8}})));
+  Modelica.Blocks.Tables.CombiTable1Dv tablePWave(
+    y(unit="W/m"),
+    tableOnFile=false,
+    table=[0,0; 0.7,3500; 0.9,6000; 1.3,12000],
+    extrapolation=Modelica.Blocks.Types.Extrapolation.LastTwoPoints)
+    "Estimate consumed power per width to generate wave of a certain heigth; "
+    annotation (Placement(transformation(extent={{-46,50},{-26,70}})));
+  Modelica.Blocks.Sources.RealExpression get_heightWave(y=heightWave)
+    "Get height of generated wave"
+    annotation (Placement(transformation(extent={{-90,50},{-70,70}})));
+  Modelica.Blocks.Interfaces.RealInput open "Input profil of wave machine"
+    annotation (Placement(transformation(extent={{-136,-20},{-96,20}})));
+  Modelica.Blocks.Interfaces.RealOutput PWaveMachine( final unit="W", final quantity="Power")
+    "Power consumption of wave machine"
+    annotation (Placement(transformation(extent={{96,-10},{116,10}})));
+  Modelica.Blocks.Math.Gain multiply(k=widthWave) "Multply by width of wave"
+    annotation (Placement(transformation(extent={{0,52},{16,68}})));
+  Modelica.Blocks.Sources.Constant zero(k=0)
+    "no output if wave machine is off"
+    annotation (Placement(transformation(extent={{-14,-78},{0,-64}})));
+  Modelica.Blocks.Logical.Switch switchWaveMachine
+    annotation (Placement(transformation(extent={{60,-10},{80,10}})));
+  Modelica.Blocks.Logical.And and1
+    annotation (Placement(transformation(extent={{-8,-10},{12,10}})));
+  Modelica.Blocks.Sources.BooleanPulse wavePoolCycle(
+    width=widthWavePul,
+    period=periodeWavePul,
+    startTime=timeWavePul_start)
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+equation
+  connect(get_heightWave.y, tablePWave.u[1]) annotation (Line(points={{-69,60},{-48,
+          60}},                  color={0,0,127}));
+  connect(multiply.u, tablePWave.y[1]) annotation (Line(points={{-1.6,60},{-25,60}},
+                              color={0,0,127}));
+  connect(open, useWavePool.u)
+    annotation (Line(points={{-116,0},{-59.6,0}}, color={0,0,127}));
+  connect(switchWaveMachine.y, PWaveMachine) annotation (Line(points={{81,0},{
+          106,0}},                     color={0,0,127}));
+  connect(multiply.y, switchWaveMachine.u1)
+    annotation (Line(points={{16.8,60},{42,60},{42,8},{58,8}},
+                                                             color={0,0,127}));
+  connect(zero.y, switchWaveMachine.u3) annotation (Line(points={{0.7,-71},{52,-71},
+          {52,-8},{58,-8}},         color={0,0,127}));
+  connect(PWaveMachine, PWaveMachine) annotation (Line(
+      points={{106,0},{101,0},{101,0},{106,0}},
+      color={0,0,127},
+      smooth=Smooth.Bezier));
+  connect(useWavePool.y, and1.u1)
+    annotation (Line(points={{-41.2,0},{-10,0}}, color={255,0,255}));
+  connect(and1.y, switchWaveMachine.u2)
+    annotation (Line(points={{13,0},{58,0}}, color={255,0,255}));
+  connect(wavePoolCycle.y, and1.u2) annotation (Line(points={{-39,-40},{-24,-40},
+          {-24,-8},{-10,-8}}, color={255,0,255}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(extent={{-100,100},{100,-100}}, lineColor={0,0,0}),
+        Line(
+          points={{-98,0},{-52,62},{-2,-24},{50,60},{100,-2}},
+          color={28,108,200},
+          smooth=Smooth.Bezier,
+          thickness=1),
+        Line(
+          points={{-98,-18},{-52,44},{-2,-42},{50,42},{98,-20}},
+          color={28,108,200},
+          smooth=Smooth.Bezier,
+          thickness=1),
+        Line(
+          points={{-98,-36},{-52,26},{-2,-60},{50,24},{96,-36}},
+          color={28,108,200},
+          smooth=Smooth.Bezier,
+          thickness=1)}),                                        Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>Model to calculate the energy demand of a wavemachine. Based on values of:</p>
+<ul>
+<li>German Association for the Recreational and Medicinal Bath Industry (Deutsche Gesellschaft f&uuml;r das Badewesen DGfdB), April 2015 : Richtlinien f&uuml;r den B&auml;derbau</li>
+<li>Chroistoph Saunus, 2005: Schwimmb&auml;der Planung - Ausf&uuml;hrung - Betrieb</li>
+</ul>
+</html>"));
+end waveMachine;
diff --git a/AixLib/Fluid/Pools/Examples/IndoorSwimmingPool.mo b/AixLib/Fluid/Pools/Examples/IndoorSwimmingPool.mo
new file mode 100644
index 0000000000..1fe527ebb6
--- /dev/null
+++ b/AixLib/Fluid/Pools/Examples/IndoorSwimmingPool.mo
@@ -0,0 +1,66 @@
+within AixLib.Fluid.Pools.Examples;
+model IndoorSwimmingPool "Example of an indoor swimming pool"
+    extends Modelica.Icons.Example;
+  .AixLib.Fluid.Pools.IndoorSwimmingPool indoorSwimming(poolParam=
+        AixLib.DataBase.Pools.SportPool(),
+    poolWallParam=
+        AixLib.DataBase.Pools.SwimmingPoolWalls.ConcreteInsulationConstruction(),
+                                           redeclare package WaterMedium =
+        WaterMedium)
+    annotation (Placement(transformation(extent={{-20,-40},{30,16}})));
+
+    replaceable package WaterMedium = AixLib.Media.Water annotation (choicesAllMatching=true);
+
+  Modelica.Blocks.Sources.RealExpression TSoil(y=273.15 + 8)
+    annotation (Placement(transformation(extent={{96,44},{80,60}})));
+  Modelica.Blocks.Sources.RealExpression X_W(y=14.3/1000)
+    annotation (Placement(transformation(extent={{-84,32},{-68,48}})));
+  Modelica.Blocks.Sources.RealExpression T_Air(y=273.15 + 30)
+    annotation (Placement(transformation(extent={{-84,56},{-68,72}})));
+  Modelica.Blocks.Sources.Pulse timeOpe(
+    amplitude=1,
+    width=(13/15)*100,
+    period=(24 - 7)*3600,
+    offset=0,
+    startTime=3600*7)
+    annotation (Placement(transformation(extent={{-88,-48},{-74,-34}})));
+  Modelica.Blocks.Sources.Trapezoid uRelPer(
+    amplitude=0.5,
+    rising=7*3600,
+    width=1*3600,
+    falling=7*3600,
+    period=17*3600,
+    offset=0.3,
+    startTime=7*3600)
+    annotation (Placement(transformation(extent={{-86,-6},{-72,8}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature
+    prescribedTemperature
+    annotation (Placement(transformation(extent={{-16,74},{-4,86}})));
+equation
+  connect(TSoil.y, indoorSwimming.TSoil) annotation (Line(points={{79.2,52},{38,
+          52},{38,1.16},{30.75,1.16}},   color={0,0,127}));
+  connect(indoorSwimming.X_w, X_W.y) annotation (Line(points={{-2.25,16.84},{
+          -2.25,24},{-62,24},{-62,40},{-67.2,40}},
+                                       color={0,0,127}));
+  connect(indoorSwimming.TAir, T_Air.y) annotation (Line(points={{-11.75,16.84},
+          {-10,16.84},{-10,64},{-67.2,64}},
+                                   color={0,0,127}));
+  connect(timeOpe.y, indoorSwimming.timeOpe) annotation (Line(points={{-73.3,
+          -41},{-30,-41},{-30,-28.24},{-21.5,-28.24}}, color={0,0,127}));
+  connect(uRelPer.y, indoorSwimming.uRelPer) annotation (Line(points={{-71.3,1},
+          {-30,1},{-30,-19.56},{-21.75,-19.56}}, color={0,0,127}));
+  connect(prescribedTemperature.T, T_Air.y)
+    annotation (Line(points={{-17.2,80},{-58,80},{-58,64},{-67.2,64}},
+                                                     color={0,0,127}));
+  connect(prescribedTemperature.port, indoorSwimming.convPool) annotation (Line(
+        points={{-4,80},{23.5,80},{23.5,17.12}}, color={191,0,0}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    experiment(Tolerance=1e-6,StopTime=604800,Interval=900),
+        __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Pools/Examples/IndoorSwimmingPool.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>Example model for an sport oriented indoor swimming pool with an integrated ideal heat exchanger. </p>
+</html>"));
+end IndoorSwimmingPool;
diff --git a/AixLib/Fluid/Pools/Examples/IndoorSwimmingPoolExternalHeatingSystem.mo b/AixLib/Fluid/Pools/Examples/IndoorSwimmingPoolExternalHeatingSystem.mo
new file mode 100644
index 0000000000..1a6e345c88
--- /dev/null
+++ b/AixLib/Fluid/Pools/Examples/IndoorSwimmingPoolExternalHeatingSystem.mo
@@ -0,0 +1,100 @@
+within AixLib.Fluid.Pools.Examples;
+model IndoorSwimmingPoolExternalHeatingSystem
+    extends Modelica.Icons.Example;
+  .AixLib.Fluid.Pools.IndoorSwimmingPool indoorSwimming(poolParam=
+        AixLib.DataBase.Pools.SportPool(use_ideHeaExc=false),
+    poolWallParam=
+        AixLib.DataBase.Pools.SwimmingPoolWalls.ConcreteInsulationConstruction(),
+                                                              redeclare package
+      WaterMedium = WaterMedium)
+    annotation (Placement(transformation(extent={{-32,-38},{16,28}})));
+
+    replaceable package WaterMedium = AixLib.Media.Water annotation (choicesAllMatching=true);
+
+  Modelica.Blocks.Sources.RealExpression TSoil(y=273.15 + 8)
+    annotation (Placement(transformation(extent={{74,80},{58,96}})));
+  Modelica.Blocks.Sources.RealExpression X_W(y=14.3/1000)
+    annotation (Placement(transformation(extent={{-88,48},{-72,64}})));
+  Modelica.Blocks.Sources.RealExpression T_Air(y=273.15 + 30)
+    annotation (Placement(transformation(extent={{-86,72},{-70,88}})));
+  Modelica.Blocks.Sources.Pulse Opening(
+    amplitude=1,
+    width=(13/15)*100,
+    period=(24 - 7)*3600,
+    offset=0,
+    startTime=3600*7)
+    annotation (Placement(transformation(extent={{-94,-44},{-80,-30}})));
+  Modelica.Blocks.Sources.Trapezoid Person(
+    amplitude=0.5,
+    rising=7*3600,
+    width=1*3600,
+    falling=7*3600,
+    period=17*3600,
+    offset=0.3,
+    startTime=7*3600)
+    annotation (Placement(transformation(extent={{-94,-8},{-80,6}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature
+    prescribedTemperature
+    annotation (Placement(transformation(extent={{-16,74},{-4,86}})));
+  Controls.Continuous.LimPID        PI(
+    k=1000,
+    yMax=10000000,
+    yMin=0,
+    controllerType=Modelica.Blocks.Types.SimpleController.PI,
+    Ti=1)                                                                                                                                                                                                         annotation(Placement(transformation(extent={{-8,-8},
+            {8,8}},
+        rotation=180,
+        origin={82,4})));
+  Modelica.Blocks.Sources.RealExpression SetTemperature(y=273.15 + 28)
+    annotation (Placement(transformation(extent={{96,34},{78,50}})));
+  MixingVolumes.MixingVolume vol(
+    redeclare package Medium = AixLib.Media.Water,
+    energyDynamics=indoorSwimming.energyDynamics,
+    p_start=100000,
+    m_flow_nominal=indoorSwimming.m_flow_nominal,
+    V=2,
+    nPorts=2) annotation (Placement(transformation(
+        extent={{-10,10},{10,-10}},
+        rotation=90,
+        origin={44,-12})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow prescribedHeatFlow
+    annotation (Placement(transformation(extent={{62,-50},{42,-30}})));
+equation
+  connect(TSoil.y, indoorSwimming.TSoil) annotation (Line(points={{57.2,88},{36,
+          88},{36,10.51},{16.72,10.51}}, color={0,0,127}));
+  connect(indoorSwimming.X_w, X_W.y) annotation (Line(points={{-14.96,28.99},{
+          -14.96,38},{-64,38},{-64,56},{-71.2,56}},
+                                       color={0,0,127}));
+  connect(indoorSwimming.TAir, T_Air.y) annotation (Line(points={{-24.08,28.99},
+          {-24.08,80},{-69.2,80}}, color={0,0,127}));
+  connect(Opening.y, indoorSwimming.timeOpe) annotation (Line(points={{-79.3,
+          -37},{-50,-37},{-50,-24.14},{-33.44,-24.14}}, color={0,0,127}));
+  connect(Person.y, indoorSwimming.uRelPer) annotation (Line(points={{-79.3,-1},
+          {-50,-1},{-50,-13.91},{-33.68,-13.91}}, color={0,0,127}));
+  connect(prescribedTemperature.T, T_Air.y)
+    annotation (Line(points={{-17.2,80},{-69.2,80}}, color={0,0,127}));
+  connect(prescribedTemperature.port, indoorSwimming.convPool) annotation (Line(
+        points={{-4,80},{9.76,80},{9.76,29.32}}, color={191,0,0}));
+  connect(PI.u_s, SetTemperature.y) annotation (Line(points={{91.6,4},{98,4},{
+          98,30},{70,30},{70,42},{77.1,42}},
+                             color={0,0,127}));
+  connect(indoorSwimming.TPool, PI.u_m) annotation (Line(points={{17.92,0.28},{
+          62,0.28},{62,18},{82,18},{82,13.6}}, color={0,0,127}));
+  connect(vol.ports[1], indoorSwimming.port_a1) annotation (Line(points={{34,
+          -13},{16,-13},{16,-14.9}}, color={0,127,255}));
+  connect(vol.ports[2], indoorSwimming.port_b1) annotation (Line(points={{34,
+          -11},{20,-11},{20,-22.82},{16,-22.82}}, color={0,127,255}));
+  connect(prescribedHeatFlow.port, vol.heatPort)
+    annotation (Line(points={{42,-40},{42,-22},{44,-22}}, color={191,0,0}));
+  connect(PI.y, prescribedHeatFlow.Q_flow) annotation (Line(points={{73.2,4},{
+          66,4},{66,-20},{70,-20},{70,-40},{62,-40}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+        experiment(Tolerance=1e-6,StopTime=604800,Interval=900),
+        __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/Fluid/Pools/Examples/IndoorSwimmingPoolExternalHeatingSystem.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>Example model for an sport oriented indoor swimming pool with an external heat source. </p>
+</html>"));
+end IndoorSwimmingPoolExternalHeatingSystem;
diff --git a/AixLib/Fluid/Pools/Examples/package.mo b/AixLib/Fluid/Pools/Examples/package.mo
new file mode 100644
index 0000000000..30e5b78435
--- /dev/null
+++ b/AixLib/Fluid/Pools/Examples/package.mo
@@ -0,0 +1,4 @@
+within AixLib.Fluid.Pools;
+package Examples
+      extends Modelica.Icons.ExamplesPackage;
+end Examples;
diff --git a/AixLib/Fluid/Pools/Examples/package.order b/AixLib/Fluid/Pools/Examples/package.order
new file mode 100644
index 0000000000..1736d4cc6d
--- /dev/null
+++ b/AixLib/Fluid/Pools/Examples/package.order
@@ -0,0 +1,2 @@
+IndoorSwimmingPool
+IndoorSwimmingPoolExternalHeatingSystem
diff --git a/AixLib/Fluid/Pools/IndoorSwimmingPool.mo b/AixLib/Fluid/Pools/IndoorSwimmingPool.mo
new file mode 100644
index 0000000000..2e5997cb64
--- /dev/null
+++ b/AixLib/Fluid/Pools/IndoorSwimmingPool.mo
@@ -0,0 +1,655 @@
+within AixLib.Fluid.Pools;
+model IndoorSwimmingPool
+  parameter AixLib.DataBase.Pools.IndoorSwimmingPoolBaseDataDefinition
+    poolParam "Choose setup for this pool" annotation (choicesAllMatching=true);
+
+   parameter AixLib.DataBase.Walls.WallBaseDataDefinition
+    poolWallParam "Choose setup for this pool" annotation (choicesAllMatching=true);
+
+  replaceable package WaterMedium = AixLib.Media.Water annotation (choicesAllMatching=true);
+
+  parameter Modelica.Fluid.Types.Dynamics energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState
+    "Type of energy balance: dynamic (3 initialization options) or steady state"
+    annotation(Evaluate=true, Dialog(tab="Dynamics", group="Equations"));
+
+  parameter Modelica.Fluid.Types.Dynamics massDynamics=energyDynamics
+  "Type of energy balance: dynamic (3 initialization options) or steady state"
+    annotation(Evaluate=true, Dialog(tab="Advanced", group="Dynamics"));
+
+  // Water transfer coefficients according to VDI 2089 Blatt 1
+  parameter Real betaNonUse(unit="m/s")=7/3600 "Water transfer coefficient during non opening hours" annotation (Dialog(group="Water transfer coefficients"));
+  parameter Real betaCover(unit="m/s")=0.7/3600 "Water transfer coefficient during non opening hours with pool cover" annotation (Dialog(group="Water transfer coefficients"));
+  parameter Real betaWavePool(unit="m/s")=50/3600 "Water transfer coefficient during wave pool operation" annotation (Dialog(group="Water transfer coefficients"));
+
+  // Parameter and variables for evaporation
+  final constant Modelica.Units.SI.SpecificHeatCapacity RD=461.52
+    "Specific gas constant for steam";                                // Source: Klaus Lucas, Thermodynamik (2008)
+  final parameter Modelica.Units.SI.SpecificEnergy hVap=
+      AixLib.Media.Air.enthalpyOfCondensingGas(poolParam.TPool)
+    "Latent heat of evaporating water";
+  Modelica.Units.SI.MassFlowRate m_flow_evap(start=0.0)
+    "mass flow rate between pool water and air due to evaporation";
+  Modelica.Units.SI.Pressure psat_TPool=
+      Modelica.Media.Air.ReferenceMoistAir.Utilities.Water95_Utilities.psat(
+      poolWat.T) "Saturation pressure at pool temperature";
+  Modelica.Units.SI.Pressure psat_TAir=
+      Modelica.Media.Air.ReferenceMoistAir.Utilities.Water95_Utilities.psat(
+      TAir) "Saturation pressure at air temperature";
+  Real phi "Relative humidity";
+
+  // Pump
+  parameter Modelica.Units.SI.Pressure pumpHead=170000
+    "Expected average flow resistance of water cycle";    //Source: Saunus 2005
+
+  // Pool circulation flow rate
+  final parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=
+      poolParam.V_flow_nominal*rhoWater_default
+      "Nominal circulation mass flow rate to the pool";
+  final parameter Modelica.Units.SI.MassFlowRate m_flow_partial=
+      poolParam.V_flow_par*rhoWater_default
+    "Partial circulation mass flow rate to pool during non operating hours";
+  Modelica.Units.SI.MassFlowRate m_flow_toPool(start=0.0)
+     "Actual circulation mass flow rate to the pool";
+
+  // Fresh water and water recycling
+  final parameter Modelica.Units.SI.Efficiency eta=if poolParam.use_HRS then
+      poolParam.etaHRS else 0;
+  Modelica.Units.SI.MassFlowRate m_flow_add(start=0.0)
+  "Mass flow of fresh water supplied to pool circulation system";
+  parameter Modelica.Media.Interfaces.Types.Temperature TFreWater=283.15
+    "Temperature of fresh water";
+
+  // Convection and Radiation at pool water surface
+  final parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConvAir=3.5
+    "Coefficient of heat transfer between the water surface and the room air";
+    // approximated for free and forced convection at velocities between 0,05 to 0,2 m/s  above a plane area
+  parameter Real eps = 0.9*0.95
+    "Product of expected emission coefficients of water (0.95) and the surrounding wall surfaces (0.95)";
+
+  AixLib.Fluid.MixingVolumes.MixingVolume poolSto(
+    redeclare package Medium = WaterMedium,
+    energyDynamics=energyDynamics,
+    massDynamics=massDynamics,
+    T_start=poolParam.TPool,
+    m_flow_nominal=m_flow_nominal,
+    V=poolParam.VSto,
+    nPorts=4) "water storage for pool "
+    annotation (Placement(transformation(extent={{-38,-56},{-18,-36}})));
+
+  AixLib.Fluid.Sources.Boundary_pT Sinc(
+    redeclare package Medium = WaterMedium, nPorts=1)
+    annotation (Placement(transformation(extent={{30,-92},{22,-84}})));
+  AixLib.Fluid.MixingVolumes.MixingVolume poolWat(
+    redeclare package Medium = WaterMedium,
+    energyDynamics=energyDynamics,
+    massDynamics=massDynamics,
+    T_start=poolParam.TPool,
+    m_flow_nominal=m_flow_nominal,
+    V=poolParam.VPool,
+    nPorts=3) "water volume of pool"
+    annotation (Placement(transformation(extent={{14,-10},{-6,10}})));
+
+  Modelica.Blocks.Sources.RealExpression getSetMasFlo(y=m_flow_toPool)
+    "set circulating mass flow of pool water"
+    annotation (Placement(transformation(extent={{42,-56},{28,-42}})));
+
+  AixLib.Fluid.Movers.BaseClasses.IdealSource setEva(
+    redeclare package Medium = WaterMedium,
+    m_flow_small=0.00001,
+    control_m_flow=true) annotation (Placement(transformation(
+        extent={{6,-6},{-6,6}},
+        rotation=0,
+        origin={-30,26})));
+  Modelica.Blocks.Sources.RealExpression getEva(y=m_flow_evap) annotation (
+      Placement(transformation(
+        extent={{9,-9},{-9,9}},
+        rotation=180,
+        origin={-81,41})));
+  AixLib.Fluid.HeatExchangers.ConstantEffectiveness heatExchanger(
+    redeclare package Medium1 = WaterMedium,
+    redeclare package Medium2 = WaterMedium,
+    m1_flow_nominal=poolParam.m_flow_out*1.5,
+    m2_flow_nominal=poolParam.m_flow_out,
+    dp1_nominal(displayUnit="bar") = 20000,
+    dp2_nominal(displayUnit="bar") = 20000,
+    eps=eps)
+     annotation (Placement(transformation(
+        extent={{-5,-5},{5,5}},
+        rotation=90,
+        origin={-33,-73})));
+  Modelica.Blocks.Interfaces.RealInput timeOpe
+    "Input profile for opening hours (0: closed, 1: open)" annotation (
+      Placement(transformation(extent={{-118,-70},{-94,-46}}),
+        iconTransformation(extent={{-118,-70},{-94,-46}})));
+  Modelica.Blocks.Interfaces.RealInput uRelPer
+    "relative number of people related to max. value" annotation (Placement(
+        transformation(extent={{-120,-40},{-94,-14}}), iconTransformation(
+          extent={{-120,-40},{-94,-14}})));
+
+  Modelica.Blocks.Interfaces.RealInput TAir(
+    final quantity="ThermodynamicTemperature",
+    final unit="K",
+    displayUnit="degC") "Temperature of the surrounding room air" annotation (
+      Placement(transformation(
+        extent={{-15,-15},{15,15}},
+        rotation=-90,
+        origin={-67,103}),iconTransformation(
+        extent={{-15,-15},{15,15}},
+        rotation=-90,
+        origin={-67,103})));
+  Modelica.Blocks.Interfaces.RealInput X_w "Absolute humidty of the room Air"  annotation (Placement(transformation(
+        extent={{-15,-15},{15,15}},
+        rotation=-90,
+        origin={-29,103}), iconTransformation(
+        extent={{-15,-15},{15,15}},
+        rotation=-90,
+        origin={-29,103})));
+
+  AixLib.ThermalZones.ReducedOrder.Multizone.BaseClasses.AbsToRelHum absToRelHum
+    "Calculation of the relative humidity of the room air " annotation (Placement(transformation(
+        extent={{-5,-5},{5,5}},
+        rotation=-90,
+        origin={-59,77})));
+
+  Modelica.Blocks.Sources.RealExpression getAddWat(y=m_flow_add)
+    "requried added fresh warter to the pool circulation"
+    annotation (Placement(transformation(extent={{-62,-78},{-48,-62}})));
+
+  AixLib.Fluid.Sources.Boundary_pT sincEva(redeclare package Medium =
+        WaterMedium, nPorts=1) annotation (Placement(transformation(
+        extent={{6,-6},{-6,6}},
+        rotation=180,
+        origin={-64,26})));
+
+  Modelica.Fluid.Interfaces.FluidPort_b port_b1(redeclare package Medium =
+        WaterMedium) if not poolParam.use_ideHeaExc
+    "Fluid connector b1 (positive design flow direction is from port_a1 to port_b1)"
+    annotation (Placement(transformation(extent={{90,-64},{110,-44}}),
+        iconTransformation(extent={{90,-64},{110,-44}})));
+
+  Modelica.Fluid.Interfaces.FluidPort_a port_a1(redeclare package Medium =
+        WaterMedium) if not poolParam.use_ideHeaExc
+    "Fluid connector a1 (positive design flow direction is from port_a1 to port_b1)"
+    annotation (Placement(transformation(extent={{90,-40},{110,-20}}),
+        iconTransformation(extent={{90,-40},{110,-20}})));
+
+  AixLib.Fluid.Pools.BaseClasses.waveMachine waveMachine(
+    heightWave=poolParam.heiWav,
+    widthWave=poolParam.widWav,
+    timeWavePul_start=poolParam.timeWavPul_start,
+    periodeWavePul=poolParam.perWavPul,
+    widthWavePul=poolParam.widWavPul) if poolParam.use_wavPool
+    annotation (Placement(transformation(extent={{-92,-94},{-76,-80}})));
+
+  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a convPool
+    "Air temperature in zone" annotation (Placement(transformation(extent={{56,86},
+            {80,110}}), iconTransformation(extent={{64,94},{84,114}})));
+
+  AixLib.Utilities.Interfaces.RadPort radPool
+    "Mean Radiation Temperature of surrounding walls " annotation (Placement(
+        transformation(
+        extent={{-8,-9},{8,9}},
+        rotation=-90,
+        origin={39,100}), iconTransformation(
+        extent={{-11,-11},{11,11}},
+        rotation=-90,
+        origin={30,100})));
+
+  Modelica.Thermal.HeatTransfer.Components.BodyRadiation radWaterSurface(
+  final Gr=eps*poolParam.APool)
+  "Model to depict the heat flow rate due to radiation between the pool surface an the surrounding walls" annotation (Placement(transformation(
+      extent={{-7,-7},{7,7}},
+      rotation=90,
+      origin={39,73})));
+
+  Modelica.Thermal.HeatTransfer.Components.Convection convWaterSurface
+  "Convection at the watersurface" annotation (Placement(transformation(
+      extent={{-7,7},{7,-7}},
+      rotation=90,
+      origin={67,75})));
+
+  Modelica.Blocks.Sources.RealExpression getHeatCoefConv(y=hConvAir*poolParam.APool)
+    "Coefficient of heat transfer between water surface and room air" annotation (Placement(transformation(extent={{100,66},
+            {82,84}})));
+
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow preHeatFlowEvapLoss annotation (Placement(transformation(extent={{-4,52},
+            {12,68}})));
+
+  Modelica.Blocks.Math.Gain hEva(final k=hVap)
+    "Calculation of heat flow rate due to evaporation" annotation (Placement(
+        transformation(
+        extent={{-4,-4},{4,4}},
+        rotation=0,
+        origin={-44,52})));
+
+  Modelica.Blocks.Interfaces.RealOutput m_flow_add_out(
+    final quantity="MassFlowRate",
+    final unit= "kg/s")
+    "Flow rate of added fresh water to the pool and water treatment system"
+    annotation (Placement(transformation(extent={{98,-102},{118,-82}}),
+        iconTransformation(extent={{98,-102},{118,-82}})));
+
+  AixLib.Fluid.Pools.BaseClasses.HeatTransferConduction heatTraCond(
+    AWalInt=poolParam.AWalInt,
+    AWalExt=poolParam.AWalExt,
+    AFloInt=poolParam.AFloInt,
+    AFloExt=poolParam.AFloExt,
+    hConWaterHorizontal=poolParam.hConWatHor,
+    hConWaterVertical=poolParam.hConWatVer,
+    TPool=poolParam.TPool,
+    PoolWall=poolWallParam)
+    "Model to depict the heat flow rate through the pool walls to the bordering room/soil"
+    annotation (Placement(transformation(extent={{64,32},{80,48}})));
+
+  Modelica.Blocks.Math.Gain minusGain(final k=-1) annotation (Placement(
+        transformation(
+        extent={{-4,-4},{4,4}},
+        rotation=0,
+        origin={-20,60})));
+
+  Modelica.Blocks.Interfaces.RealOutput QEva(
+    final quantity="HeatFlowRate",
+    final unit="W") "Heat due to evaporation" annotation (Placement(
+        transformation(extent={{-94,52},{-124,82}}), iconTransformation(extent={{-94,60},
+            {-114,80}})));
+
+   Modelica.Blocks.Interfaces.RealOutput QPool(
+     final quantity="HeatFlowRate",
+     final unit="W")
+     if poolParam.use_ideHeaExc
+   "Heat flow rate to maintain the pool at the set temperature" annotation (
+      Placement(transformation(extent={{98,-16},{118,4}}),  iconTransformation(
+          extent={{98,-16},{118,4}})));
+
+  Modelica.Blocks.Interfaces.RealInput TSoil(
+    final quantity="ThermodynamicTemperature",
+    final unit="K",
+    displayUnit="degC") "Temperature of Soil" annotation (Placement(
+        transformation(
+        extent={{-13,-13},{13,13}},
+        rotation=180,
+        origin={105,49}), iconTransformation(
+      extent={{-11,-11},{11,11}},
+      rotation=180,
+      origin={103,47})));
+
+  Modelica.Blocks.Interfaces.RealOutput PPool(
+    final quantity="Power",
+    final unit="W")
+    "Output eletric energy needed for pool operation" annotation (Placement(transformation(extent={{98,-86},
+            {118,-66}}),
+      iconTransformation(extent={{98,-86},{118,-66}})));
+
+  Modelica.Blocks.Interfaces.RealOutput TPool(
+    final quantity="ThermodynamicTemperature",
+    final unit="K")
+    "current temperature of pool"
+    annotation (Placement(transformation(extent={{98,6},{118,26}}),
+        iconTransformation(extent={{98,6},{118,26}})));
+
+  Modelica.Blocks.Math.MultiSum elPower(nu=if poolParam.use_wavPool then 2 else 1)
+    "Add electric power of pump and the optional wave pool"
+    annotation (Placement(transformation(extent={{72,-72},{80,-80}})));
+  Sources.MassFlowSource_T bou(
+    redeclare package Medium = WaterMedium,
+    use_m_flow_in=true,
+    T=TFreWater,
+    nPorts=1)
+    annotation (Placement(transformation(extent={{-52,-94},{-40,-82}})));
+  Modelica.Blocks.Sources.RealExpression getMeaTPool(y=poolWat.T) annotation (
+      Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={72,16})));
+
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow idealHeater
+    if poolParam.use_ideHeaExc
+    annotation (Placement(transformation(extent={{48,-20},{32,-4}})));
+  AixLib.Controls.Continuous.LimPID        PI(
+    k=poolParam.KHeat,
+    yMax=poolParam.QMaxHeat,
+    yMin=poolParam.QMinHeat,
+    controllerType=Modelica.Blocks.Types.SimpleController.PI,
+    Ti=poolParam.timeHea) if poolParam.use_ideHeaExc                                                                                                                                                                 annotation(Placement(transformation(extent={{-4,-4},
+            {4,4}},
+        rotation=180,
+        origin={66,-16})));
+  Modelica.Blocks.Sources.RealExpression getSetTPool(y=poolParam.TPool)
+    if poolParam.use_ideHeaExc
+    annotation (Placement(transformation(extent={{96,-24},{78,-8}})));
+  AixLib.Fluid.Movers.FlowControlled_m_flow cirPump(
+    redeclare package Medium = WaterMedium,
+    redeclare Movers.Data.Generic per(
+      pressure(V_flow={m_flow_nominal/1000/100,m_flow_nominal/1000,
+            m_flow_nominal/1000/0.7}, dp={pumpHead/0.7,pumpHead,0}),
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate,
+
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.Efficiency_VolumeFlowRate,
+
+      efficiency(V_flow={m_flow_nominal/1000/100,m_flow_nominal/1000,
+            m_flow_nominal/1000/0.7}, eta={0.7,0.8,0.7}),
+      motorEfficiency(V_flow={m_flow_nominal/1000/100,m_flow_nominal/1000,
+            m_flow_nominal/1000/0.7}, eta={0.9,0.9,0.9})),
+    inputType=AixLib.Fluid.Types.InputType.Continuous,
+    energyDynamics=energyDynamics,
+    T_start=poolParam.TPool,
+    allowFlowReversal=false,
+    m_flow_nominal=m_flow_nominal,
+    addPowerToMedium=false,
+    dp_nominal=pumpHead,
+    m_flow_start=m_flow_nominal)
+    "circulation pump for permanent pool circulation " annotation (Placement(
+        transformation(
+        extent={{-8,-8},{8,8}},
+        rotation=0,
+        origin={0,-68})));
+
+  FixedResistances.PressureDrop              res(
+    redeclare package Medium = WaterMedium,
+    allowFlowReversal=false,
+    m_flow_nominal=m_flow_nominal,
+    show_T=false,
+    from_dp=false,
+    dp_nominal=pumpHead - poolParam.dpHeaExcPool,
+    homotopyInitialization=true,
+    linearized=false,
+    deltaM=0.3) "representative resistance for whole system "
+    annotation (Placement(transformation(extent={{32,-76},{44,-60}})));
+
+
+  Modelica.Blocks.Interfaces.RealOutput m_flow_eva(final quantity=
+        "MassFlowRate", final unit="kg/s") "Evaporation mass flow" annotation (
+      Placement(transformation(extent={{-94,34},{-122,62}}), iconTransformation(
+          extent={{-96,36},{-116,56}})));
+protected
+  final parameter Modelica.Units.SI.Density rhoWater_default=
+      WaterMedium.density_pTX(
+      p=WaterMedium.p_default,
+      T=273.15 + 30,
+      X=WaterMedium.X_default) "Default medium density";
+
+equation
+  // Fresh water and water recycling
+  if poolParam.use_watRec then
+    m_flow_add=(1-poolParam.x_rec)*(poolParam.m_flow_out + m_flow_evap);
+  else
+    m_flow_add=poolParam.m_flow_out + m_flow_evap;
+  end if;
+
+  // Pool circulation flow rate
+  if poolParam.use_parLoa then
+    if timeOpe > 0 then
+      m_flow_toPool = m_flow_nominal;
+    else
+      m_flow_toPool = m_flow_partial;
+    end if;
+  else
+    m_flow_toPool = m_flow_nominal;
+  end if;
+
+  // Evaporation according to VDI 2089 sheet 1, formula (1)
+   phi=absToRelHum.relHum;
+   if psat_TPool-phi*psat_TAir<0 then
+     m_flow_evap=0.0;
+   else
+    if timeOpe > 0 then
+      if uRelPer > 0 then
+         m_flow_evap =uRelPer*(poolParam.betaInUse/(RD*0.5*(poolWat.T + TAir))*(
+          psat_TPool - phi*psat_TAir)*poolParam.APool);
+       else
+         m_flow_evap =betaNonUse/(RD*0.5*(poolWat.T + TAir))*(psat_TPool - phi*
+          psat_TAir)*poolParam.APool;
+       end if;
+     else
+       if poolParam.use_poolCov then
+         m_flow_evap =betaCover/(RD*0.5*(poolWat.T + TAir))*(psat_TPool - phi*
+          psat_TAir)*poolParam.APool;
+       else
+         m_flow_evap =betaNonUse/(RD*0.5*(poolWat.T + TAir))*(psat_TPool - phi*
+          psat_TAir)*poolParam.APool;
+       end if;
+     end if;
+   end if;
+
+  if poolParam.use_ideHeaExc then
+    connect(res.port_b, poolWat.ports[1]) annotation (Line(points={{44,-68},{54,
+            -68},{54,-24},{6,-24},{6,-10},{5.33333,-10}}, color={0,127,255}));
+  else
+    connect(poolWat.ports[1], port_a1) annotation (Line(
+        points={{5.33333,-10},{6,-10},{6,-22},{56,-22},{56,-30},{100,-30}},
+        color={0,127,255},
+        pattern=LinePattern.Dash));
+    connect(port_b1, res.port_b) annotation (Line(
+        points={{100,-54},{78,-54},{78,-68},{44,-68}},
+        color={0,127,255},
+        pattern=LinePattern.Dash));
+  end if;
+
+  connect(poolWat.ports[3], setEva.port_a) annotation (Line(points={{2.66667,-10},
+          {2,-10},{2,-18},{-12,-18},{-12,26},{-24,26}}, color={0,127,255}));
+
+  connect(poolSto.ports[2],heatExchanger. port_b1) annotation (Line(points={{-28.5,
+          -56},{-28.5,-64},{-36,-64},{-36,-68}}, color={0,127,255}));
+  connect(poolSto.ports[3],heatExchanger. port_a2) annotation (Line(points={{-27.5,
+          -56},{-28,-56},{-28,-64},{-30,-64},{-30,-68}}, color={0,127,255}));
+  connect(poolSto.ports[4], cirPump.port_a) annotation (Line(points={{-26.5,-56},
+          {-14,-56},{-14,-68},{-8,-68}}, color={0,127,255}));
+  connect(poolSto.ports[1], poolWat.ports[2]) annotation (Line(points={{-29.5,-56},
+          {-29.5,-60},{-60,-60},{-60,-24},{4,-24},{4,-10}}, color={0,127,255}));
+
+  connect(absToRelHum.TDryBul, TAir) annotation (Line(points={{-61.8,83},{-62,83},
+          {-62,88},{-67,88},{-67,103}},color={0,0,127}));
+  connect(absToRelHum.absHum, X_w) annotation (Line(points={{-56.4,83},{-56,83},
+          {-56,88},{-29,88},{-29,103}},  color={0,0,127}));
+  connect(heatExchanger.port_b2, Sinc.ports[1]) annotation (Line(points={{-30,-78},
+          {-30,-88},{22,-88}},                    color={0,127,255}));
+  connect(setEva.port_b, sincEva.ports[1])
+    annotation (Line(points={{-36,26},{-58,26}}, color={0,127,255}));
+  connect(getEva.y, setEva.m_flow_in) annotation (Line(points={{-71.1,41},{-26.4,
+          41},{-26.4,30.8}}, color={0,0,127}));
+  connect(radWaterSurface.port_b, radPool)
+    annotation (Line(points={{39,80},{39,100}}, color={191,0,0}));
+  connect(convWaterSurface.fluid, convPool)
+    annotation (Line(points={{67,82},{68,82},{68,98}}, color={191,0,0}));
+  connect(convWaterSurface.solid, poolWat.heatPort) annotation (Line(points={{67,
+          68},{66,68},{66,52},{38,52},{38,0},{14,0}}, color={191,0,0}));
+  connect(radWaterSurface.port_a, poolWat.heatPort)
+    annotation (Line(points={{39,66},{38,66},{38,0},{14,0}}, color={191,0,0}));
+  connect(preHeatFlowEvapLoss.port, poolWat.heatPort)
+    annotation (Line(points={{12,60},{26,60},{26,0},{14,0}}, color={191,0,0}));
+  connect(getEva.y, hEva.u) annotation (Line(points={{-71.1,41},{-58,41},{-58,52},
+          {-48.8,52}}, color={0,0,127}));
+  connect(heatTraCond.heatport_a, poolWat.heatPort) annotation (Line(points={{63.76,
+          39.92},{38,39.92},{38,0},{14,0}}, color={191,0,0}));
+  connect(hEva.y, minusGain.u) annotation (Line(points={{-39.6,52},{-34,52},{-34,
+          60},{-24.8,60}}, color={0,0,127}));
+  connect(hEva.y, QEva) annotation (Line(points={{-39.6,52},{-34,52},{-34,67},{
+          -109,67}},
+                color={0,0,127}));
+  connect(heatTraCond.TSoil, TSoil) annotation (Line(points={{80.48,42.88},{82,42.88},
+          {82,49},{105,49}}, color={0,0,127}));
+  connect(convPool, convPool)
+    annotation (Line(points={{68,98},{68,98}}, color={191,0,0}));
+  connect(getHeatCoefConv.y, convWaterSurface.Gc) annotation (Line(points={{81.1,75},
+          {74,75}},                                                                              color={0,0,127}));
+  connect(minusGain.y, preHeatFlowEvapLoss.Q_flow)
+    annotation (Line(points={{-15.6,60},{-4,60}}, color={0,0,127}));
+
+  connect(bou.ports[1],heatExchanger. port_a1) annotation (Line(points={{-40,-88},
+          {-40,-78},{-36,-78}}, color={0,127,255}));
+  connect(waveMachine.open, timeOpe) annotation (Line(points={{-93.28,-87},{-98,
+          -87},{-98,-74},{-90,-74},{-90,-58},{-106,-58}}, color={0,0,127}));
+  connect(getMeaTPool.y, TPool)
+    annotation (Line(points={{83,16},{108,16}}, color={0,0,127}));
+
+  connect(PI.y, idealHeater.Q_flow) annotation (Line(points={{61.6,-16},{54,-16},
+          {54,-12},{48,-12}}, color={0,0,127}));
+  connect(idealHeater.port, poolWat.heatPort) annotation (Line(points={{32,-12},
+          {24,-12},{24,0},{14,0}}, color={191,0,0}));
+  connect(getSetTPool.y, PI.u_s)
+    annotation (Line(points={{77.1,-16},{70.8,-16}}, color={0,0,127}));
+  connect(QPool, PI.y) annotation (Line(points={{108,-6},{58,-6},{58,-16},{61.6,
+          -16}}, color={0,0,127}));
+  connect(bou.m_flow_in, getAddWat.y) annotation (Line(points={{-53.2,-83.2},{-60,
+          -83.2},{-60,-76},{-42,-76},{-42,-70},{-47.3,-70}}, color={0,0,127}));
+  connect(getAddWat.y, m_flow_add_out) annotation (Line(points={{-47.3,-70},{-42,-70},
+          {-42,-76},{-60,-76},{-60,-96},{94,-96},{94,-92},{108,-92}}, color={0,0,
+          127}));
+  connect(setEva.port_b, setEva.port_a) annotation (Line(
+      points={{-36,26},{-30,26},{-24,26}},
+      color={0,127,255},
+      smooth=Smooth.Bezier));
+
+  connect(elPower.u[1], cirPump.P) annotation (Line(points={{72,-76},{62,-76},{62,
+          -60.8},{8.8,-60.8}}, color={0,0,127}));
+  connect(elPower.y, PPool)  annotation (Line(points={{80.68,-76},{108,-76}}, color={0,0,127}));
+  connect(waveMachine.PWaveMachine, elPower.u[2]) annotation (Line(points={{-75.52,
+          -87},{-72,-87},{-72,-100},{64,-100},{64,-76},{72,-76}},
+                                                       color={0,0,127}));
+
+  connect(PI.u_m,getMeaTPool. y) annotation (Line(points={{66,-11.2},{66,4},{92,
+          4},{92,16},{83,16}}, color={0,0,127}));
+  connect(getEva.y, m_flow_eva) annotation (Line(points={{-71.1,41},{-68,41},{
+          -68,48},{-108,48}}, color={0,0,127}));
+  connect(getSetMasFlo.y, cirPump.m_flow_in)
+    annotation (Line(points={{27.3,-49},{0,-49},{0,-58.4}}, color={0,0,127}));
+  connect(cirPump.port_b, res.port_a)
+    annotation (Line(points={{8,-68},{32,-68}}, color={0,127,255}));
+  annotation (Line(
+        points={{47,-32},{47,-14},{-25,-14},{-25,-6}}, color={0,127,255}),
+             Line(points={{18.4,-40},
+          {18,-40},{18,-44},{-100,-44}}, color={0,127,255}),
+                Placement(transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=-90,
+        origin={-50,82}), iconTransformation(
+        extent={{-20,-20},{20,20}},
+        rotation=-90,
+        origin={-60,80})),
+         Icon(coordinateSystem(preserveAspectRatio=false),
+         graphics={
+         Rectangle(
+          extent={{98,98},{-98,-98}},
+          fillColor={215,215,215},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+          Bitmap(extent={{-94,-150},{96,58}}, fileName="modelica://AixLib/Resources/Images/Fluid/Pools/icon_schwimmbecken.jpg")}),
+          Diagram(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-100,2},{100,100}},
+          lineColor={0,128,255},
+          fillColor={170,213,255},
+          fillPattern=FillPattern.Solid,
+          lineThickness=0.5),
+        Text(
+          extent={{-98,12},{-6,0}},
+          textColor={85,85,255},
+          textStyle={TextStyle.Bold},
+          horizontalAlignment=TextAlignment.Left,
+          textString="Heat and mass exchange 
+at pool surface or pool walls 
+"),     Rectangle(
+          extent={{-66,-98},{100,-2}},
+          lineColor={0,0,127},
+          fillColor={155,195,232},
+          fillPattern=FillPattern.Solid,
+          lineThickness=0.5),
+        Rectangle(
+          extent={{-100,-98},{-68,-2}},
+          lineColor={95,95,95},
+          fillColor={215,215,215},
+          fillPattern=FillPattern.Solid,
+          lineThickness=0.5),
+        Text(
+          extent={{-98,-6},{-72,-14}},
+          textColor={95,95,95},
+          horizontalAlignment=TextAlignment.Left,
+          textStyle={TextStyle.Bold},
+          textString="Pool 
+operation"),
+        Text(
+          extent={{-64,-2},{-22,-24}},
+          textColor={0,0,127},
+          horizontalAlignment=TextAlignment.Left,
+          textStyle={TextStyle.Bold},
+          textString="Water treatment 
+circuit
+")}),
+Documentation(info="<html><p>
+  <b><span style=\"color: #008000;\">Overview</span></b>
+</p>
+<p>
+  Model for indoor swimming pools to calculate energy and water
+  demands. Optional use of a wave machine, pool cover, partial load for
+  the circulation pump and heat recovery from wastewater or recycling.
+  In addition, an ideal heater can be used to heat the pool.
+</p>
+<p>
+  <br/>
+  <br/>
+  <img src=
+  \"modelica://AixLib/Resources/Images/Fluid/Pools/PoolAndWaterCuircut.png\"
+  alt=\"1\">
+</p>
+<p>
+  <b><span style=\"color: #008000;\">Important parameters and
+  Inputs</span></b>
+</p>
+<ul>
+  <li>All pool specific parameters are collected in one <a href=
+  \"AixLib.DataBase.Pools.IndoorSwimmingPoolBaseRecord\">AixLib.DataBase.Pools.IndoorSwimmingPoolBaseRecord</a>
+  record.
+  </li>
+  <li>openingHours: Input profile for the opening hours to consider a
+  pool cover or a reduced circulation flow during non-operating hours.
+  Also, during non-opening hours pool occupancy is set to 0.
+  </li>
+  <li>persons: Input profile for occupancy of the pool to consider
+  occupancy level for evaportaion.
+  </li>
+</ul>
+<p>
+  <b><span style=\"color: #008000;\">Assumptions</span></b>
+</p>
+<ul>
+  <li>Evaporation is determined according to VDI 2089.
+  </li>
+  <li>Filter and disinfection units are not explicitly modeled and have
+  to be considered within the pump delivery head (pumpHead). According
+  to Saunus 1.7 bar is a good estimation for swimming pools in sport
+  oriented swimming facilities.
+  </li>
+  <li>The type of the filter should be taken into account within the
+  determination of the volume flow and storage capacities. DIN 19643
+  provides standards for the volume flow and storage capacities, taking
+  into account the pool size and type as well as the filter type.
+  </li>
+  <li>There are no water losses or heat gains due to people entering or
+  leaving the swimming pool.
+  </li>
+</ul>
+<p>
+  <b><span style=\"color: #008000;\">References</span></b>
+</p>
+<p>
+  For automatic generation of a swimming pool within a thermal zone and
+  multizone model as well as for datasets, see
+  https://github.com/RWTH-EBC/TEASER
+</p>
+<p>
+  References for implemented constants (use also for parametrization):
+</p>
+<ul>
+  <li>German Association of Engineers: Guideline VDI 2089-1, January
+  2010: Building Services in swimming baths - Indoor Pools
+  </li>
+  <li>German Institute for Standardization DIN 19643-1, November 2012:
+  Treatment of water of swimming pools and baths - Part 1 General
+  Requirements
+  </li>
+  <li>Chroistoph Saunus, 2005: Schwimmbäder Planung - Ausführung -
+  Betrieb
+  </li>
+</ul>
+</html>"));
+end IndoorSwimmingPool;
diff --git a/AixLib/Fluid/Pools/package.mo b/AixLib/Fluid/Pools/package.mo
new file mode 100644
index 0000000000..ed22197509
--- /dev/null
+++ b/AixLib/Fluid/Pools/package.mo
@@ -0,0 +1,33 @@
+within AixLib.Fluid;
+package Pools
+
+   extends Modelica.Icons.Package;
+
+
+annotation (Icon(graphics={
+      Rectangle(
+        extent={{-66,-2},{68,-42}},
+        lineColor={0,0,0},
+        lineThickness=0.5,
+        fillColor={170,213,255},
+        fillPattern=FillPattern.Solid,
+        pattern=LinePattern.None),
+      Line(
+        points={{-66,20},{-66,-42}},
+        color={0,0,0},
+        thickness=1),
+      Line(
+        points={{-66,-42},{68,-42}},
+        color={0,0,0},
+        thickness=1),
+      Line(
+        points={{68,20},{68,-42}},
+        color={0,0,0},
+        thickness=1),            Line(
+        points={{-66,-4},{-60,2},{-56,-4},{-50,2},{-44,-4},{-36,2},{-30,-4},{
+            -24,2},{-18,-4},{-12,2},{-6,-4},{0,2},{6,-4},{10,2},{16,-4},{22,2},
+            {28,-4},{34,2},{40,-4},{44,2},{50,-4},{56,2},{62,-4},{68,2}},
+        color={0,0,0},
+        smooth=Smooth.Bezier,
+        thickness=0.5)}));
+end Pools;
diff --git a/AixLib/Fluid/Pools/package.order b/AixLib/Fluid/Pools/package.order
new file mode 100644
index 0000000000..92ca0d4d74
--- /dev/null
+++ b/AixLib/Fluid/Pools/package.order
@@ -0,0 +1,3 @@
+IndoorSwimmingPool
+Examples
+BaseClasses
diff --git a/AixLib/Fluid/Sensors/BaseClasses/PartialAbsoluteSensor.mo b/AixLib/Fluid/Sensors/BaseClasses/PartialAbsoluteSensor.mo
index 9afd1786b1..03b80428c3 100644
--- a/AixLib/Fluid/Sensors/BaseClasses/PartialAbsoluteSensor.mo
+++ b/AixLib/Fluid/Sensors/BaseClasses/PartialAbsoluteSensor.mo
@@ -27,9 +27,9 @@ protected
 initial equation
   assert(not warnAboutOnePortConnection,
   "Sensor " + instanceName + " can lead to numerical problems if connected to a scalar fluid port.
-   Only connect it to a vectorized fluid port, such as used in 'AixLib.Fluid.MixingVolumes`.
-   See AixLib.Fluid.Sensors.UsersGuide for more information.
-   To disable this warning, set 'warnAboutOnePortConnection = false' in "+ instanceName + ".",
+  Only connect it to a vectorized fluid port, such as used in 'AixLib.Fluid.MixingVolumes`.
+  See AixLib.Fluid.Sensors.UsersGuide for more information.
+  To disable this warning, set 'warnAboutOnePortConnection = false' in " + instanceName + ".",
   level=AssertionLevel.warning);
 equation
   port.m_flow = 0;
@@ -37,56 +37,56 @@ equation
   port.Xi_outflow = zeros(Medium.nXi);
   port.C_outflow = zeros(Medium.nC);
   annotation (Documentation(info="<html>
- <p>
- Partial component to model an absolute sensor.
- The component can be used for pressure sensor models.
- Use for other properties such as temperature or density is discouraged, because the enthalpy at the connector can have different meanings, depending on the connection topology. For these properties, use
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialFlowSensor\">
- AixLib.Fluid.Sensors.BaseClasses.PartialFlowSensor</a>.
- </p>
- </html>",
+<p>
+Partial component to model an absolute sensor.
+The component can be used for pressure sensor models.
+Use for other properties such as temperature or density is discouraged, because the enthalpy at the connector can have different meanings, depending on the connection topology. For these properties, use
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialFlowSensor\">
+AixLib.Fluid.Sensors.BaseClasses.PartialFlowSensor</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 20, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and added assertion with level set to warning.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\"> #1399</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- September 7, 2018, by Michael Wetter:<br/>
- Changed
- <code>port(redeclare package Medium=Medium, m_flow(min=0, max=0))</code>
- to
- <code>port(redeclare package Medium=Medium, m_flow(min=0))</code>
- to avoid in Dymola 2019FD01 beta1 the message
- \"port.m_flow has the range [0,0] - which is suspicious since the max-value should be above the min-value\"
- which causes an error in pedantic mode.
- Note that the MSL also uses only a <code>min</code> value.
- </li>
- <li>
- March 22, 2017, by Filip Jorissen:<br/>
- Set <code>m_flow(max=0)</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/687\">#687</a>.
- </li>
- <li>
- February 12, 2011, by Michael Wetter:<br/>
- First implementation.
- Implementation is based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+September 20, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and added assertion with level set to warning.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\"> #1399</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+September 7, 2018, by Michael Wetter:<br/>
+Changed
+<code>port(redeclare package Medium=Medium, m_flow(min=0, max=0))</code>
+to
+<code>port(redeclare package Medium=Medium, m_flow(min=0))</code>
+to avoid in Dymola 2019FD01 beta1 the message
+\"port.m_flow has the range [0,0] - which is suspicious since the max-value should be above the min-value\"
+which causes an error in pedantic mode.
+Note that the MSL also uses only a <code>min</code> value.
+</li>
+<li>
+March 22, 2017, by Filip Jorissen:<br/>
+Set <code>m_flow(max=0)</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/687\">#687</a>.
+</li>
+<li>
+February 12, 2011, by Michael Wetter:<br/>
+First implementation.
+Implementation is based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),
 Icon(
   graphics={
     Bitmap(
       visible = warnAboutOnePortConnection,
       extent={{-96,-82},{-64,-50}},
-      fileName="modelica://AixLib/Resources/Images/Fluid/Sensors/warningIcon.png")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+      fileName="modelica://AixLib/Resources/Images/Fluid/Sensors/warningIcon.png")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialAbsoluteSensor;
diff --git a/AixLib/Fluid/Sensors/BaseClasses/PartialDynamicFlowSensor.mo b/AixLib/Fluid/Sensors/BaseClasses/PartialDynamicFlowSensor.mo
index ef3138cc96..958f648a05 100644
--- a/AixLib/Fluid/Sensors/BaseClasses/PartialDynamicFlowSensor.mo
+++ b/AixLib/Fluid/Sensors/BaseClasses/PartialDynamicFlowSensor.mo
@@ -29,45 +29,52 @@ equation
     k = 1;
   end if;
   annotation (Icon(graphics={
-        Line(visible=(tau <> 0),
+        Line(visible=(tau > 0),
         points={{52,60},{58,74},{66,86},{76,92},{88,96},{98,96}}, color={0,
               0,127})}), Documentation(info="<html>
- <p>
- Partial component to model a sensor that measures any intensive properties
- of a flow, e.g., to get temperature or density in the flow
- between fluid connectors.</p>
- <p>
- The sensor computes a gain that is zero at zero mass flow rate.
- This avoids fast transients if the flow is close to zero, thereby
- improving the numerical efficiency.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 9, 2016, by Michael Wetter:<br/>
- Improved documentation for <code>tau</code>.
- </li>
- <li>
- January 12, 2016, by Filip Jorissen:<br/>
- Added optional parameter <code>tauInv</code>.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- March 29, 2013, by Michael Wetter:<br/>
- Changed the parameter <code>initType</code> to
- <code>Modelica.Blocks.Types.Init.InitialState</code>.
- This allows a pedantic model check in Dymola 2014 of models that instanciate sensors
- but do not set this parameter. It also ensures that different Modelica simulators solve
- the same initialization problem.
- </li>
- <li>
- July 7, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial component to model a sensor that measures any intensive properties
+of a flow, e.g., to get temperature or density in the flow
+between fluid connectors.</p>
+<p>
+The sensor computes a gain that is zero at zero mass flow rate.
+This avoids fast transients if the flow is close to zero, thereby
+improving the numerical efficiency.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 10, 2022, by Michael Wetter:<br/>
+Corrected annotation to avoid comparing a real-valued parameter
+for equality.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1671\">IBPSA, #1671</a>.
+</li>
+<li>
+August 9, 2016, by Michael Wetter:<br/>
+Improved documentation for <code>tau</code>.
+</li>
+<li>
+January 12, 2016, by Filip Jorissen:<br/>
+Added optional parameter <code>tauInv</code>.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+March 29, 2013, by Michael Wetter:<br/>
+Changed the parameter <code>initType</code> to
+<code>Modelica.Blocks.Types.Init.InitialState</code>.
+This allows a pedantic model check in Dymola 2014 of models that instanciate sensors
+but do not set this parameter. It also ensures that different Modelica simulators solve
+the same initialization problem.
+</li>
+<li>
+July 7, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialDynamicFlowSensor;
diff --git a/AixLib/Fluid/Sensors/BaseClasses/PartialFlowSensor.mo b/AixLib/Fluid/Sensors/BaseClasses/PartialFlowSensor.mo
index adf353fe89..6c9d787794 100644
--- a/AixLib/Fluid/Sensors/BaseClasses/PartialFlowSensor.mo
+++ b/AixLib/Fluid/Sensors/BaseClasses/PartialFlowSensor.mo
@@ -22,35 +22,35 @@ equation
   port_a.C_outflow = if allowFlowReversal then inStream(port_b.C_outflow) else zeros(Medium.nC);
   port_b.C_outflow = inStream(port_a.C_outflow);
   annotation (Documentation(info="<html>
- <p>
- Partial component to model a sensor.
- The sensor is ideal. It does not influence mass, energy,
- species or substance balance, and it has no flow friction.
- </p>
- </html>",
+<p>
+Partial component to model a sensor.
+The sensor is ideal. It does not influence mass, energy,
+species or substance balance, and it has no flow friction.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 15, 2015, by Filip Jorissen:<br/>
- Implemented more efficient computation of <code>port_a.Xi_outflow</code>,
- <code>port_a.h_outflow</code>
- and <code>port_a.C_outflow</code> when <code>allowFlowReversal=false</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/281\">#281</a>.
- </li>
- <li>
- June 19, 2015, by Michael Wetter:<br/>
- Moved <code>m_flow_small</code> to the <code>Advanced</code> tab
- as it usually need not be changed by the user.
- Other models such as heat exchangers also have this parameter
- on the <code>Advanced</code> tab.
- </li>
- <li>
- February 12, 2011, by Michael Wetter:<br/>
- First implementation.
- Implementation is based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+August 15, 2015, by Filip Jorissen:<br/>
+Implemented more efficient computation of <code>port_a.Xi_outflow</code>,
+<code>port_a.h_outflow</code>
+and <code>port_a.C_outflow</code> when <code>allowFlowReversal=false</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/281\">#281</a>.
+</li>
+<li>
+June 19, 2015, by Michael Wetter:<br/>
+Moved <code>m_flow_small</code> to the <code>Advanced</code> tab
+as it usually need not be changed by the user.
+Other models such as heat exchangers also have this parameter
+on the <code>Advanced</code> tab.
+</li>
+<li>
+February 12, 2011, by Michael Wetter:<br/>
+First implementation.
+Implementation is based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialFlowSensor;
diff --git a/AixLib/Fluid/Sensors/Conversions/Examples/To_VolumeFraction.mo b/AixLib/Fluid/Sensors/Conversions/Examples/To_VolumeFraction.mo
index 8895085183..33fdc89824 100644
--- a/AixLib/Fluid/Sensors/Conversions/Examples/To_VolumeFraction.mo
+++ b/AixLib/Fluid/Sensors/Conversions/Examples/To_VolumeFraction.mo
@@ -16,8 +16,10 @@ model To_VolumeFraction "Example problem for conversion model"
     k=2,
     Td=1)
     annotation (Placement(transformation(extent={{-100,-20},{-80,0}})));
-  AixLib.Fluid.Sensors.TraceSubstances senCO2(redeclare package Medium =
-        Medium, substanceName="CO2") "CO2 sensor"
+  AixLib.Fluid.Sensors.TraceSubstances senCO2(
+    redeclare package Medium = Medium,
+    substanceName="CO2",
+    warnAboutOnePortConnection = false) "CO2 sensor"
     annotation (Placement(transformation(extent={{120,0},{140,20}})));
   AixLib.Fluid.MixingVolumes.MixingVolume vol(
     nPorts=4,
@@ -143,37 +145,43 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors
         "Simulate and plot"),
   Diagram(coordinateSystem(preserveAspectRatio=false,extent={{-200,-100},{200,100}})),
     Documentation(info="<html>
- This example demonstrates the modeling of a room with one person and CO<sub>2</sub> control.
- The room has a volume of <i>4*4*2.7 m<sup>3</sup></i>, and the CO<sub>2</sub> inflow is from
- one person.
- A control system regulates the outside air to maintain a CO<sub>2</sub> concentration of 1000 PPM
- in the room. The outside air has a CO<sub>2</sub> concentration of 300 PPM.
- Note that for simplicity, we allow zero outside air flow rate if the CO<sub>2</sub> concentration is below
- the setpoint, which does not comply with ASHRAE regulations.
- </html>",revisions="<html>
- <ul>
- <li>
- May 2, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- April 25, 2017 by Filip Jorissen:<br/>
- Increased model tolerance for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/750\">#750</a>.
- </li>
- <li>
- March 27, 2013 by Michael Wetter:<br/>
- Added a flow resistance between the volume and the ambient to decouple the
- state of the volume from the boundary conditions. This is needed to allow
- a pedantic model check in Dymola 2014, as otherwise, the initial conditions of
- the volume could not be specified without introducing redundant equations.
- </li>
- <li>
- February 13, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
-end To_VolumeFraction;
+This example demonstrates the modeling of a room with one person and CO<sub>2</sub> control.
+The room has a volume of <i>4*4*2.7 m<sup>3</sup></i>, and the CO<sub>2</sub> inflow is from
+one person.
+A control system regulates the outside air to maintain a CO<sub>2</sub> concentration of 1000 PPM
+in the room. The outside air has a CO<sub>2</sub> concentration of 300 PPM.
+Note that for simplicity, we allow zero outside air flow rate if the CO<sub>2</sub> concentration is below
+the setpoint, which does not comply with ASHRAE regulations.
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2024, by Michael Wetter:<br/>
+Configured the sensor parameter to suppress the warning about being a one-port connection.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1857\">IBPSA, #1857</a>.
+</li>
+<li>
+May 2, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+April 25, 2017 by Filip Jorissen:<br/>
+Increased model tolerance for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/750\">#750</a>.
+</li>
+<li>
+March 27, 2013 by Michael Wetter:<br/>
+Added a flow resistance between the volume and the ambient to decouple the
+state of the volume from the boundary conditions. This is needed to allow
+a pedantic model check in Dymola 2014, as otherwise, the initial conditions of
+the volume could not be specified without introducing redundant equations.
+</li>
+<li>
+February 13, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end To_VolumeFraction;
\ No newline at end of file
diff --git a/AixLib/Fluid/Sensors/Conversions/To_VolumeFraction.mo b/AixLib/Fluid/Sensors/Conversions/To_VolumeFraction.mo
index 005c12411e..67c616580e 100644
--- a/AixLib/Fluid/Sensors/Conversions/To_VolumeFraction.mo
+++ b/AixLib/Fluid/Sensors/Conversions/To_VolumeFraction.mo
@@ -58,33 +58,33 @@ equation
           textString=DynamicSelect("", String(V, leftJustified=false, significantDigits=3)))}),
 defaultComponentName="toVolFra",
 Documentation(info="<html>
- <p>
- This component converts mass fraction to volume fraction for an ideal gas.
- The default value for the parameter <code>MMBul</code>
- assumes that the bulk medium is air.
- The model assumes that the concentration
- of the measured substance is small enough to be neglected in the molar mass
- of the mixture.
- </p>
- </html>",
+<p>
+This component converts mass fraction to volume fraction for an ideal gas.
+The default value for the parameter <code>MMBul</code>
+assumes that the bulk medium is air.
+The model assumes that the concentration
+of the measured substance is small enough to be neglected in the molar mass
+of the mixture.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- February 13, 2011 by Michael Wetter:<br/>
- Changed connectors from the obsolete <code>RealSignal</code>
- to <code>RealInput</code> and <code>RealOutput</code>.
- </li>
- <li>
- September 22, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+February 13, 2011 by Michael Wetter:<br/>
+Changed connectors from the obsolete <code>RealSignal</code>
+to <code>RealInput</code> and <code>RealOutput</code>.
+</li>
+<li>
+September 22, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end To_VolumeFraction;
diff --git a/AixLib/Fluid/Sensors/Density.mo b/AixLib/Fluid/Sensors/Density.mo
index f9f244dd58..0da7b84f3e 100644
--- a/AixLib/Fluid/Sensors/Density.mo
+++ b/AixLib/Fluid/Sensors/Density.mo
@@ -31,40 +31,40 @@ annotation (defaultComponentName="senDen",
           textColor={0,0,0},
           textString=DynamicSelect("", String(d, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the density of the fluid connected to its port.
- The sensor is ideal, i.e. it does not influence the fluid.
- </p>
- <p>
- To measure density in a duct or pipe, use
- <a href=\"modelica://AixLib.Fluid.Sensors.DensityTwoPort\">AixLib.Fluid.Sensors.DensityTwoPort</a>
- rather than this sensor.
- Read the
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a>
- prior to using this model to see about potential numerical problems if this sensor is used incorrectly
- in a system model.
- </p>
- </html>",
+<p>
+This model outputs the density of the fluid connected to its port.
+The sensor is ideal, i.e. it does not influence the fluid.
+</p>
+<p>
+To measure density in a duct or pipe, use
+<a href=\"modelica://AixLib.Fluid.Sensors.DensityTwoPort\">AixLib.Fluid.Sensors.DensityTwoPort</a>
+rather than this sensor.
+Read the
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a>
+prior to using this model to see about potential numerical problems if this sensor is used incorrectly
+in a system model.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 21, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 21, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Density;
diff --git a/AixLib/Fluid/Sensors/DensityTwoPort.mo b/AixLib/Fluid/Sensors/DensityTwoPort.mo
index 7ea258b317..6644af6177 100644
--- a/AixLib/Fluid/Sensors/DensityTwoPort.mo
+++ b/AixLib/Fluid/Sensors/DensityTwoPort.mo
@@ -74,46 +74,46 @@ annotation (defaultComponentName="senDen",
           textColor={0,0,0},
           textString=DynamicSelect("", String(d, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the density of the fluid flowing from
- <code>port_a</code> to <code>port_b</code>.
- </p>
- <p>
- The sensor is ideal, i.e., it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then its output
- is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",
+<p>
+This model outputs the density of the fluid flowing from
+<code>port_a</code> to <code>port_b</code>.
+</p>
+<p>
+The sensor is ideal, i.e., it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then its output
+is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation, based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation, based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DensityTwoPort;
diff --git a/AixLib/Fluid/Sensors/EnthalpyFlowRate.mo b/AixLib/Fluid/Sensors/EnthalpyFlowRate.mo
index 2cbd825da9..525ab7b7a6 100644
--- a/AixLib/Fluid/Sensors/EnthalpyFlowRate.mo
+++ b/AixLib/Fluid/Sensors/EnthalpyFlowRate.mo
@@ -62,69 +62,69 @@ annotation (defaultComponentName="senEntFlo",
           textColor={0,0,0},
           textString=DynamicSelect("", String(H_flow, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the enthalphy flow rate of the medium in the flow
- between fluid ports. The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- <p>
- If the parameter <code>tau</code> is non-zero, then the measured
- specific enthalpy <i>h<sub>out</sub></i> that is used to
- compute the enthalpy flow rate
- <i>H&#775; = m&#775; h<sub>out</sub></i>
- is computed using a first order differential equation.
- See <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- <p>
- For a sensor that measures the latent enthalpy flow rate, use
- <a href=\"modelica://AixLib.Fluid.Sensors.LatentEnthalpyFlowRate\">
- AixLib.Fluid.Sensors.LatentEnthalpyFlowRate</a>.
- </p>
- </html>",
+<p>
+This model outputs the enthalphy flow rate of the medium in the flow
+between fluid ports. The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+<p>
+If the parameter <code>tau</code> is non-zero, then the measured
+specific enthalpy <i>h<sub>out</sub></i> that is used to
+compute the enthalpy flow rate
+<i>H&#775; = m&#775; h<sub>out</sub></i>
+is computed using a first order differential equation.
+See <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+<p>
+For a sensor that measures the latent enthalpy flow rate, use
+<a href=\"modelica://AixLib.Fluid.Sensors.LatentEnthalpyFlowRate\">
+AixLib.Fluid.Sensors.LatentEnthalpyFlowRate</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 19, 2020, by Antoine Gautier:<br/>
- Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Made unit assignment of output signal final.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Removed default value <code>tau=0</code> as the base class
- already sets <code>tau=1</code>.
- This change was made so that all sensors use the same default value.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This can improve the numerics.
- </li>
- <li>
- April 9, 2008 by Michael Wetter:<br/>
- First implementation.
- Implementation is based on enthalpy sensor of <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 19, 2020, by Antoine Gautier:<br/>
+Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Made unit assignment of output signal final.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Removed default value <code>tau=0</code> as the base class
+already sets <code>tau=1</code>.
+This change was made so that all sensors use the same default value.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This can improve the numerics.
+</li>
+<li>
+April 9, 2008 by Michael Wetter:<br/>
+First implementation.
+Implementation is based on enthalpy sensor of <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EnthalpyFlowRate;
diff --git a/AixLib/Fluid/Sensors/EntropyFlowRate.mo b/AixLib/Fluid/Sensors/EntropyFlowRate.mo
index 10211b7590..851d362a73 100644
--- a/AixLib/Fluid/Sensors/EntropyFlowRate.mo
+++ b/AixLib/Fluid/Sensors/EntropyFlowRate.mo
@@ -73,41 +73,41 @@ annotation (defaultComponentName="senS_flow",
           textColor={0,0,0},
           textString=DynamicSelect("", String(S_flow, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the entropy flow rate of the medium in the flow
- between fluid ports. The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- <p>
- If the parameter <code>tau</code> is non-zero, then the measured
- specific entropy <i>s<sub>out</sub></i> that is used to
- compute the entropy flow rate
- <i>S&#775; = m&#775; s<sub>out</sub></i>
- is computed using a first order differential equation.
- See <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",
+<p>
+This model outputs the entropy flow rate of the medium in the flow
+between fluid ports. The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+<p>
+If the parameter <code>tau</code> is non-zero, then the measured
+specific entropy <i>s<sub>out</sub></i> that is used to
+compute the entropy flow rate
+<i>S&#775; = m&#775; s<sub>out</sub></i>
+is computed using a first order differential equation.
+See <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 19, 2020, by Antoine Gautier:<br/>
- Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- July 29, 2016, by Michael Wetter:<br/>
- First implementation based on
- <a href=\"modelica://AixLib.Fluid.Sensors.EnthalpyFlowRate\">
- AixLib.Fluid.Sensors.EnthalpyFlowRate</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 19, 2020, by Antoine Gautier:<br/>
+Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+July 29, 2016, by Michael Wetter:<br/>
+First implementation based on
+<a href=\"modelica://AixLib.Fluid.Sensors.EnthalpyFlowRate\">
+AixLib.Fluid.Sensors.EnthalpyFlowRate</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EntropyFlowRate;
diff --git a/AixLib/Fluid/Sensors/Examples/Density.mo b/AixLib/Fluid/Sensors/Examples/Density.mo
index b77d515998..26b1273f16 100644
--- a/AixLib/Fluid/Sensors/Examples/Density.mo
+++ b/AixLib/Fluid/Sensors/Examples/Density.mo
@@ -67,21 +67,21 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/Density.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the density sensors.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 10, 2013 by Michael Wetter:<br/>
- Changed initialization of volume to fixed initial values to avoid
- a translation warning in OpenModelica.
- </li>
- <li>
- August 31, 2013 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the density sensors.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 10, 2013 by Michael Wetter:<br/>
+Changed initialization of volume to fixed initial values to avoid
+a translation warning in OpenModelica.
+</li>
+<li>
+August 31, 2013 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Density;
diff --git a/AixLib/Fluid/Sensors/Examples/EnthalpyFlowRate.mo b/AixLib/Fluid/Sensors/Examples/EnthalpyFlowRate.mo
index 051c174ae9..6244b5b1fb 100644
--- a/AixLib/Fluid/Sensors/Examples/EnthalpyFlowRate.mo
+++ b/AixLib/Fluid/Sensors/Examples/EnthalpyFlowRate.mo
@@ -73,32 +73,32 @@ equation
 experiment(Tolerance=1e-6, StopTime=60),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/EnthalpyFlowRate.mos"
         "Simulate and plot"),    Documentation(info="<html>
- <p>
- This example tests the enthalpy flow rate sensor and the
- specific enthalpy sensor.
- The model compares the output of the enthalpy flow rate sensor with
- the product of the output of the enthalpy and the mass flow rate sensor.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Changed assertions to blocks that compute the difference,
- and added the difference to the regression results.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Change <code>tau=0</code> to <code>tau=1</code> for sensors.
- Changed source model to use temperature instead of specific enthalpy
- as a parameter.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the enthalpy flow rate sensor and the
+specific enthalpy sensor.
+The model compares the output of the enthalpy flow rate sensor with
+the product of the output of the enthalpy and the mass flow rate sensor.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Changed assertions to blocks that compute the difference,
+and added the difference to the regression results.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Change <code>tau=0</code> to <code>tau=1</code> for sensors.
+Changed source model to use temperature instead of specific enthalpy
+as a parameter.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EnthalpyFlowRate;
diff --git a/AixLib/Fluid/Sensors/Examples/EntropyFlowRate.mo b/AixLib/Fluid/Sensors/Examples/EntropyFlowRate.mo
index e93e754139..5c104db110 100644
--- a/AixLib/Fluid/Sensors/Examples/EntropyFlowRate.mo
+++ b/AixLib/Fluid/Sensors/Examples/EntropyFlowRate.mo
@@ -71,19 +71,19 @@ equation
 experiment(Tolerance=1e-6, StopTime=60),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/EntropyFlowRate.mos"
         "Simulate and plot"),    Documentation(info="<html>
- <p>
- This example tests the entropy flow rate sensor and the
- specific entropy sensor.
- The model compares the output of the entropy flow rate sensor with
- the product of the output of the entropy and the mass flow rate sensor.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 29, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the entropy flow rate sensor and the
+specific entropy sensor.
+The model compares the output of the entropy flow rate sensor with
+the product of the output of the entropy and the mass flow rate sensor.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 29, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EntropyFlowRate;
diff --git a/AixLib/Fluid/Sensors/Examples/HeatMeter.mo b/AixLib/Fluid/Sensors/Examples/HeatMeter.mo
new file mode 100644
index 0000000000..18b406de93
--- /dev/null
+++ b/AixLib/Fluid/Sensors/Examples/HeatMeter.mo
@@ -0,0 +1,78 @@
+within AixLib.Fluid.Sensors.Examples;
+model HeatMeter
+  extends Modelica.Icons.Example;
+
+  package Medium = AixLib.Media.Water
+    "Medium model";
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal = 10 "Nominal mass flow rate";
+
+  Sources.MassFlowSource_T sou(
+    redeclare package Medium = Medium,
+    m_flow=m_flow_nominal,
+    nPorts=1) "Mass flow source"
+    annotation (Placement(transformation(extent={{-70,-10},{-50,10}})));
+  Sources.Boundary_pT sin(
+    redeclare package Medium = Medium,
+    nPorts=1)
+    "Sink"
+    annotation (Placement(transformation(extent={{70,-10},{50,10}})));
+  Modelica.Thermal.HeatTransfer.Sources.FixedHeatFlow heaFloRat(Q_flow=
+        m_flow_nominal*10*4200) "Heat flow rate"
+    annotation (Placement(transformation(extent={{-50,30},{-30,50}})));
+  MixingVolumes.MixingVolume vol(
+    redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    m_flow_nominal=m_flow_nominal,
+    V=0.1,
+    nPorts=2)
+    "Mixing volume"
+    annotation (Placement(transformation(extent={{-10,30},{10,50}})));
+  TemperatureTwoPort senT(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal)
+    annotation (Placement(transformation(extent={{-30,-10},{-10,10}})));
+  AixLib.Fluid.Sensors.HeatMeter senHeaFlo(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal)
+    annotation (Placement(transformation(extent={{10,-10},{30,10}})));
+equation
+  connect(sou.ports[1], senT.port_a)
+    annotation (Line(points={{-50,0},{-30,0}},   color={0,127,255}));
+  connect(senT.port_b, vol.ports[1]) annotation (Line(points={{-10,0},{-2,0},{
+          -2,30},{-1,30}},    color={0,127,255}));
+  connect(vol.ports[2], senHeaFlo.port_a) annotation (Line(points={{1,30},{2,30},
+          {2,0},{10,0}},       color={0,127,255}));
+  connect(senHeaFlo.port_b, sin.ports[1])
+    annotation (Line(points={{30,0},{50,0}},   color={0,127,255}));
+  connect(senT.T, senHeaFlo.TExt) annotation (Line(points={{-20,11},{-20,18},{
+          -6,18},{-6,6},{8,6}},     color={0,0,127}));
+  connect(heaFloRat.port, vol.heatPort)
+    annotation (Line(points={{-30,40},{-10,40}}, color={191,0,0}));
+    annotation (
+experiment(Tolerance=1e-6, StopTime=60),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/HeatMeter.mos"
+        "Simulate and plot"),
+  Documentation(info="<html>
+<p>
+This example tests the heat meter sensor for the situation where heat is exchanged with a control volume.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 1, 2024, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1831\">IBPSA, #1831</a>.
+</li>
+<li>
+February 1, 2024, by Jan Gall:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1831\">IBPSA, #1831</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end HeatMeter;
diff --git a/AixLib/Fluid/Sensors/Examples/MassFraction.mo b/AixLib/Fluid/Sensors/Examples/MassFraction.mo
index 6696e0c665..7c37075c0b 100644
--- a/AixLib/Fluid/Sensors/Examples/MassFraction.mo
+++ b/AixLib/Fluid/Sensors/Examples/MassFraction.mo
@@ -59,16 +59,16 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/MassFraction.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the mass fraction sensors.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 7, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the mass fraction sensors.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 7, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFraction;
diff --git a/AixLib/Fluid/Sensors/Examples/MoistAirEnthalpyFlowRate.mo b/AixLib/Fluid/Sensors/Examples/MoistAirEnthalpyFlowRate.mo
index 36b958c469..88a3491590 100644
--- a/AixLib/Fluid/Sensors/Examples/MoistAirEnthalpyFlowRate.mo
+++ b/AixLib/Fluid/Sensors/Examples/MoistAirEnthalpyFlowRate.mo
@@ -89,27 +89,27 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors
         "Simulate and plot"),
     Documentation(
     info="<html>
- <p>
- This example tests the sensible and latent enthalpy sensors.
- It compares the output from the enthalpy sensor with the sum of the
- sensible and latent enthalpy sensors.
- </p>
- </html>",
+<p>
+This example tests the sensible and latent enthalpy sensors.
+It compares the output from the enthalpy sensor with the sum of the
+sensible and latent enthalpy sensors.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 2, 2016, by Michael Wetter:<br/>
- Removed assertion and added the enthalpy flow rates instead
- to the plot window so that they become part of the regression tests.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
- </li>
- <li>
- January 23 2013, by Michael Wetter:<br/>
- Changed time constant of <code>senH</code> so that it has
- the same transient response model as <code>senH_flow</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 2, 2016, by Michael Wetter:<br/>
+Removed assertion and added the enthalpy flow rates instead
+to the plot window so that they become part of the regression tests.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/564\">issue 564</a>.
+</li>
+<li>
+January 23 2013, by Michael Wetter:<br/>
+Changed time constant of <code>senH</code> so that it has
+the same transient response model as <code>senH_flow</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MoistAirEnthalpyFlowRate;
diff --git a/AixLib/Fluid/Sensors/Examples/PPM.mo b/AixLib/Fluid/Sensors/Examples/PPM.mo
index 378be41b6c..5b5acccd81 100644
--- a/AixLib/Fluid/Sensors/Examples/PPM.mo
+++ b/AixLib/Fluid/Sensors/Examples/PPM.mo
@@ -4,8 +4,8 @@ model PPM "Test model for the extra property sensor outputting PPM"
   package Medium = AixLib.Media.Air(extraPropertiesNames={"CO2"})
     "Medium model";
 
-  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=volDyn.V*
-      senPPMTwoPort.tau*3*rho_default
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=
+    volDyn.V*senPPMTwoPort.tau*3*rho_default
     "Mass flow rate into and out of the volume";
 
   AixLib.Fluid.MixingVolumes.MixingVolume volDyn(
@@ -20,7 +20,7 @@ model PPM "Test model for the extra property sensor outputting PPM"
     redeclare package Medium = Medium,
     nPorts=2,
     m_flow=m_flow_nominal) "Fresh air supply"
-    annotation (Placement(transformation(extent={{-40,30},{-20,50}})));
+    annotation (Placement(transformation(origin = {-28, 0}, extent = {{-40, 30}, {-20, 50}})));
 
   AixLib.Fluid.Sensors.PPM senPPMVol(
     redeclare package Medium = Medium,
@@ -82,32 +82,44 @@ model PPM "Test model for the extra property sensor outputting PPM"
     redeclare package Medium = Medium,
     nPorts=1,
     m_flow=m_flow_nominal) "Fresh air supply for steady state volume"
-    annotation (Placement(transformation(extent={{-40,110},{-20,130}})));
+    annotation (Placement(transformation(origin = {-28, 0}, extent = {{-40, 110}, {-20, 130}})));
   AixLib.Fluid.Sources.Boundary_pT sin(
     redeclare package Medium = Medium,
     nPorts=2) "Exhaust air"
-    annotation (Placement(transformation(extent={{-40,-60},{-20,-40}})));
+    annotation (Placement(transformation(origin = {-30, 0}, extent = {{-40, -60}, {-20, -40}})));
+
+  AixLib.Fluid.FixedResistances.PressureDrop dp(
+     redeclare package Medium = Medium,
+     dp_nominal = 200,
+     m_flow_nominal = m_flow_nominal)
+     "Pressure drop to decouple volume pressure from boundary pressure"
+     annotation (
+    Placement(transformation(origin = {-28, -50}, extent = {{-2, -10}, {18, 10}})));
 
 protected
   final parameter Medium.ThermodynamicState state_default = Medium.setState_pTX(
       T=Medium.T_default,
       p=Medium.p_default,
-      X=Medium.X_default[1:Medium.nXi]) "Medium state at default values";
+      X=Medium.X_default[1:Medium.nXi]) "Medium state at default values"
+    annotation(Evaluate=true);
   // Density at medium default values, used to compute the size of control volumes
-  final parameter Modelica.Units.SI.Density rho_default=Medium.density(state=
-      state_default) "Density, used to compute fluid mass";
+  final parameter Modelica.Units.SI.Density rho_default=Medium.density(
+    state=state_default)
+    "Density, used to compute fluid mass"
+    annotation(Evaluate=true);
 
 equation
-  connect(mSou.ports[1], volDyn.ports[1]) annotation (Line(points={{-20,42},{
-          77.3333,42},{77.3333,50}},       color={0,127,255}));
+  connect(mSou.ports[1], volDyn.ports[1]) annotation (Line(points={{-48,39},{
+          -48,50},{78.6667,50}},
+                            color={0,127,255}));
   connect(CO2In.y, volDyn.C_flow[1]) annotation (Line(points={{21,70},{32,70},{32,
           54},{68,54}}, color={0,0,127}));
   connect(senPPMVol.port, volDyn.ports[2]) annotation (Line(points={{130,40},{80,
-          40},{80,50}},         color={0,127,255}));
+          40},{80,50}},color={0,127,255}));
   connect(senPPMIn.port, mSou.ports[2])
-    annotation (Line(points={{-10,80},{-10,38},{-20,38}}, color={0,127,255}));
+    annotation (Line(points={{-10,80},{-10,41},{-48,41}}, color={0,127,255}));
   connect(senPPMTwoPort.port_a, volDyn.ports[3]) annotation (Line(points={{80,20},
-          {80,50},{82.6667,50}},         color={0,127,255}));
+          {80,50},{81.3333,50}},         color={0,127,255}));
   connect(senPPMNoRev.port_a, senPPMTwoPort.port_b)
     annotation (Line(points={{80,-20},{80,0}}, color={0,127,255}));
   connect(senPPMRev.port_b, senPPMNoRev.port_b) annotation (Line(points={{60,-50},
@@ -116,15 +128,17 @@ equation
     annotation (Line(points={{20,-50},{30,-50},{40,-50}}, color={0,127,255}));
   connect(CO2In.y,volSte. C_flow[1]) annotation (Line(points={{21,70},{32,70},{32,
           84},{68,84}}, color={0,0,127}));
-  connect(volSte.ports[1], senPPMVol2.port) annotation (Line(points={{77.3333,
+  connect(volSte.ports[1], senPPMVol2.port) annotation (Line(points={{78.6667,
           80},{130,80}},          color={0,127,255}));
-  connect(mSouSta.ports[1], volSte.ports[2]) annotation (Line(points={{-20,120},
+  connect(mSouSta.ports[1], volSte.ports[2]) annotation (Line(points={{-48,120},
           {54,120},{54,80},{80,80}},      color={0,127,255}));
-  connect(sin.ports[1], senPPMSta.port_b) annotation (Line(points={{-20,-48},{-10,
-          -48},{-10,-50},{0,-50}}, color={0,127,255}));
-  connect(sin.ports[2], volSte.ports[3]) annotation (Line(points={{-20,-52},{
-          -20,-80},{110,-80},{110,80},{82.6667,80}},
-                                                 color={0,127,255}));
+  connect(sin.ports[1], volSte.ports[3]) annotation (
+    Line(points={{-50,-51},{-50,-80},{110,-80},{110,80},{81.3333,80}},            color = {0, 127, 255}));
+  connect(dp.port_b, senPPMSta.port_b) annotation (
+    Line(points = {{-10, -50}, {0, -50}}, color = {0, 127, 255}));
+  connect(dp.port_a, sin.ports[2]) annotation (
+    Line(points={{-30,-50},{-40,-50},{-40,-49},{-50,-49}},
+                                            color = {0, 127, 255}));
     annotation (
 experiment(Tolerance=1e-6, StopTime=3),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/PPM.mos"
@@ -132,27 +146,32 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors
     Diagram(coordinateSystem(preserveAspectRatio=false,extent={{-100,-100},{180,
             180}})),
     Documentation(info="<html>
- <p>
- This example tests the sensors that measure trace substances
- using an output in parts per million.
- Various configurations with and without flow reversal
- and with or without dynamics are tested.
- </p>
- </html>",
+<p>
+This example tests the sensors that measure trace substances
+using an output in parts per million.
+Various configurations with and without flow reversal
+and with or without dynamics are tested.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 2, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- January 12, 2016, by Filip Jorissen:<br/>
- First implementation.
- See issue
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 1, 2024, by Michael Wetter:<br/>
+Added pressure drop to avoid redundant initial conditions for pressure of control volume.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1830\"> #1830</a>.
+</li>
+<li>
+May 2, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+January 12, 2016, by Filip Jorissen:<br/>
+First implementation.
+See issue
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PPM;
diff --git a/AixLib/Fluid/Sensors/Examples/Pressure.mo b/AixLib/Fluid/Sensors/Examples/Pressure.mo
index 451e157b80..f98625952f 100644
--- a/AixLib/Fluid/Sensors/Examples/Pressure.mo
+++ b/AixLib/Fluid/Sensors/Examples/Pressure.mo
@@ -65,16 +65,16 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/Pressure.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the pressure sensors.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 31, 2013 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the pressure sensors.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 31, 2013 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Pressure;
diff --git a/AixLib/Fluid/Sensors/Examples/RelativeHumidity.mo b/AixLib/Fluid/Sensors/Examples/RelativeHumidity.mo
index 6a763390f4..f2b021a771 100644
--- a/AixLib/Fluid/Sensors/Examples/RelativeHumidity.mo
+++ b/AixLib/Fluid/Sensors/Examples/RelativeHumidity.mo
@@ -67,18 +67,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/RelativeHumidity.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the relative humidity sensors.
- Note that the sensor with one port always measures the humidity
- as if the flow would be leaving the source.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 12, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the relative humidity sensors.
+Note that the sensor with one port always measures the humidity
+as if the flow would be leaving the source.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 12, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RelativeHumidity;
diff --git a/AixLib/Fluid/Sensors/Examples/SpecificEnthalpy.mo b/AixLib/Fluid/Sensors/Examples/SpecificEnthalpy.mo
index c106649faa..75806abf11 100644
--- a/AixLib/Fluid/Sensors/Examples/SpecificEnthalpy.mo
+++ b/AixLib/Fluid/Sensors/Examples/SpecificEnthalpy.mo
@@ -50,20 +50,20 @@ equation
 experiment(Tolerance=1e-6, StopTime=60),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/SpecificEnthalpy.mos"
         "Simulate and plot"),    Documentation(info="<html>
- <p>
- This example tests the specific enthalpy sensors.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 8, 2014, by Michael Wetter:<br/>
- Set species concentration to the default value of the medium.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the specific enthalpy sensors.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 8, 2014, by Michael Wetter:<br/>
+Set species concentration to the default value of the medium.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpecificEnthalpy;
diff --git a/AixLib/Fluid/Sensors/Examples/SpecificEntropy.mo b/AixLib/Fluid/Sensors/Examples/SpecificEntropy.mo
index ef756f2949..4a3fd00af8 100644
--- a/AixLib/Fluid/Sensors/Examples/SpecificEntropy.mo
+++ b/AixLib/Fluid/Sensors/Examples/SpecificEntropy.mo
@@ -50,16 +50,16 @@ equation
 experiment(Tolerance=1e-6, StopTime=60),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/SpecificEntropy.mos"
         "Simulate and plot"),    Documentation(info="<html>
- <p>
- This example tests the specific entropy sensors.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the specific entropy sensors.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpecificEntropy;
diff --git a/AixLib/Fluid/Sensors/Examples/TemperatureDryBulb.mo b/AixLib/Fluid/Sensors/Examples/TemperatureDryBulb.mo
index 58559f4a01..3283372288 100644
--- a/AixLib/Fluid/Sensors/Examples/TemperatureDryBulb.mo
+++ b/AixLib/Fluid/Sensors/Examples/TemperatureDryBulb.mo
@@ -97,26 +97,26 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/TemperatureDryBulb.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the dry bulb temperature sensors.
- One sensor is configured to be a steady-state model,
- a second sensor is configured to be a dynamic sensor and
- the third sensors is a dynamic sensor with heat transfer.
- There is also a sensor that measures the temperature difference.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 19, 2015 by Filip Jorissen:<br/>
- Extended example with demonstration of thermal losses.
- </li>
- <li>
- September 10, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example tests the dry bulb temperature sensors.
+One sensor is configured to be a steady-state model,
+a second sensor is configured to be a dynamic sensor and
+the third sensors is a dynamic sensor with heat transfer.
+There is also a sensor that measures the temperature difference.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 19, 2015 by Filip Jorissen:<br/>
+Extended example with demonstration of thermal losses.
+</li>
+<li>
+September 10, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-120,-100},{120,
-            100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureDryBulb;
diff --git a/AixLib/Fluid/Sensors/Examples/TemperatureWetBulb.mo b/AixLib/Fluid/Sensors/Examples/TemperatureWetBulb.mo
index 74ba16e1fe..4214a9fbbc 100644
--- a/AixLib/Fluid/Sensors/Examples/TemperatureWetBulb.mo
+++ b/AixLib/Fluid/Sensors/Examples/TemperatureWetBulb.mo
@@ -56,23 +56,23 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/TemperatureWetBulb.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the wet bulb temperature sensor.
- The problem setup is such that the moisture concentration and
- the dry bulb temperature are varied simultaneously in such a way
- that the wet bulb temperature remains close to a constant value.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 4, 2011 by Michael Wetter:<br/>
- Adjusted parameters and simulation stop time since the sensor was changed to a dynamic sensor.
- </li>
- <li>
- May 6, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the wet bulb temperature sensor.
+The problem setup is such that the moisture concentration and
+the dry bulb temperature are varied simultaneously in such a way
+that the wet bulb temperature remains close to a constant value.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 4, 2011 by Michael Wetter:<br/>
+Adjusted parameters and simulation stop time since the sensor was changed to a dynamic sensor.
+</li>
+<li>
+May 6, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureWetBulb;
diff --git a/AixLib/Fluid/Sensors/Examples/TraceSubstances.mo b/AixLib/Fluid/Sensors/Examples/TraceSubstances.mo
index 764a31299c..3666a32070 100644
--- a/AixLib/Fluid/Sensors/Examples/TraceSubstances.mo
+++ b/AixLib/Fluid/Sensors/Examples/TraceSubstances.mo
@@ -113,57 +113,57 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors
     Diagram(coordinateSystem(preserveAspectRatio=false,extent={{-100,-100},{180,
             180}})),
     Documentation(info="<html>
- <p>
- This example tests the sensors that measure trace substances.
- A CO<sub>2</sub> mass flow rate of <i>8.18E-8</i> kg/kg is added to the
- volume. The volume also has a fresh air mass flow rate and
- an exhaust air mass flow rate. The initial CO<sub>2</sub> concentration
- of the volume is <i>0</i> kg/kg.
- Note that the fresh air supply has zero carbon dioxide concentration.
- Therefore, if it were outside air, then all concentrations are relative
- to the outside air concentration.
- </p>
- </html>",
+<p>
+This example tests the sensors that measure trace substances.
+A CO<sub>2</sub> mass flow rate of <i>8.18E-8</i> kg/kg is added to the
+volume. The volume also has a fresh air mass flow rate and
+an exhaust air mass flow rate. The initial CO<sub>2</sub> concentration
+of the volume is <i>0</i> kg/kg.
+Note that the fresh air supply has zero carbon dioxide concentration.
+Therefore, if it were outside air, then all concentrations are relative
+to the outside air concentration.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 2, 2019, by Jianjun Hu:<br/>
- Replaced fluid source. This is for 
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
- </li>
- <li>
- May 22, 2015, by Michael Wetter:<br/>
- Updated example to test the correction for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/249\">issue 249</a>.
- </li>
- <li>
- May 8, 2014, by Michael Wetter:<br/>
- Added a pressure drop element, as otherwise the initialization problem
- is overspecified for incompressible media.
- </li>
- <li>
- November 27, 2013 by Michael Wetter:<br/>
- Changed sink model from a prescribed flow source to a pressure
- boundary condition. This is required for the new air model,
- which is incompressible. Otherwise, there will be no pressure reference
- in the system.
- </li>
- <li>
- September 10, 2013 by Michael Wetter:<br/>
- Changed initialization of volume to fixed initial values to avoid
- a translation warning in OpenModelica.
- </li>
- <li>
- August 30, 2013 by Michael Wetter:<br/>
- Renamed example and added an instance of
- <a href=\"modelica://AixLib.Fluid.Sensors.TraceSubstancesTwoPort\">
- AixLib.Fluid.Sensors.TraceSubstancesTwoPort</a>.
- </li>
- <li>
- September 29, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 2, 2019, by Jianjun Hu:<br/>
+Replaced fluid source. This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\"> #1072</a>.
+</li>
+<li>
+May 22, 2015, by Michael Wetter:<br/>
+Updated example to test the correction for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/249\">issue 249</a>.
+</li>
+<li>
+May 8, 2014, by Michael Wetter:<br/>
+Added a pressure drop element, as otherwise the initialization problem
+is overspecified for incompressible media.
+</li>
+<li>
+November 27, 2013 by Michael Wetter:<br/>
+Changed sink model from a prescribed flow source to a pressure
+boundary condition. This is required for the new air model,
+which is incompressible. Otherwise, there will be no pressure reference
+in the system.
+</li>
+<li>
+September 10, 2013 by Michael Wetter:<br/>
+Changed initialization of volume to fixed initial values to avoid
+a translation warning in OpenModelica.
+</li>
+<li>
+August 30, 2013 by Michael Wetter:<br/>
+Renamed example and added an instance of
+<a href=\"modelica://AixLib.Fluid.Sensors.TraceSubstancesTwoPort\">
+AixLib.Fluid.Sensors.TraceSubstancesTwoPort</a>.
+</li>
+<li>
+September 29, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TraceSubstances;
diff --git a/AixLib/Fluid/Sensors/Examples/Velocity.mo b/AixLib/Fluid/Sensors/Examples/Velocity.mo
index 7156188778..3f582ddbbc 100644
--- a/AixLib/Fluid/Sensors/Examples/Velocity.mo
+++ b/AixLib/Fluid/Sensors/Examples/Velocity.mo
@@ -54,23 +54,23 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/Velocity.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the flow velocity sensor.
- One sensor is configured to be steady-state, and the other is
- configured to be dynamic.
- Note that steady-state sensors can lead to numerical problems
- if used incorrectly.
- See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 20, 2016 by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the flow velocity sensor.
+One sensor is configured to be steady-state, and the other is
+configured to be dynamic.
+Note that steady-state sensors can lead to numerical problems
+if used incorrectly.
+See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 20, 2016 by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Velocity;
diff --git a/AixLib/Fluid/Sensors/Examples/VolumeFlowRate.mo b/AixLib/Fluid/Sensors/Examples/VolumeFlowRate.mo
index 04b2b44662..e982b70816 100644
--- a/AixLib/Fluid/Sensors/Examples/VolumeFlowRate.mo
+++ b/AixLib/Fluid/Sensors/Examples/VolumeFlowRate.mo
@@ -52,23 +52,23 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/VolumeFlowRate.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the volume flow rate sensor.
- One sensor is configured to be steady-state, and the other is
- configured to be dynamic.
- Note that steady-state sensors can lead to numerical problems
- if used incorrectly.
- See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 31, 2013 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the volume flow rate sensor.
+One sensor is configured to be steady-state, and the other is
+configured to be dynamic.
+Note that steady-state sensors can lead to numerical problems
+if used incorrectly.
+See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 31, 2013 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VolumeFlowRate;
diff --git a/AixLib/Fluid/Sensors/Examples/package.order b/AixLib/Fluid/Sensors/Examples/package.order
index 6e4c242734..9288f23614 100644
--- a/AixLib/Fluid/Sensors/Examples/package.order
+++ b/AixLib/Fluid/Sensors/Examples/package.order
@@ -1,6 +1,7 @@
 Density
 EnthalpyFlowRate
 EntropyFlowRate
+HeatMeter
 MassFraction
 MoistAirEnthalpyFlowRate
 PPM
diff --git a/AixLib/Fluid/Sensors/HeatMeter.mo b/AixLib/Fluid/Sensors/HeatMeter.mo
new file mode 100644
index 0000000000..621cbea5b0
--- /dev/null
+++ b/AixLib/Fluid/Sensors/HeatMeter.mo
@@ -0,0 +1,127 @@
+within AixLib.Fluid.Sensors;
+model HeatMeter "Measures thermal energy provided between supply and return pipes"
+  extends BaseClasses.PartialDynamicFlowSensor;
+  extends Modelica.Icons.RoundSensor;
+  Modelica.Blocks.Interfaces.RealInput TExt(
+    final unit="K",
+    displayUnit="degC") "External temperature measurement to calculate temperature difference"
+    annotation (Placement(transformation(extent={{-140,40},{-100,80}}),
+        iconTransformation(extent={{-140,40},{-100,80}})));
+  Modelica.Blocks.Interfaces.RealOutput Q_flow(
+    final quantity="HeatFlowRate",
+    final unit="W") "Heat flow rate"
+    annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={0,110})));
+  parameter Modelica.Units.SI.Temperature T_start=Medium.T_default
+    "Initial or guess value of temperature"
+    annotation (Dialog(group="Initialization"));
+  Medium.Temperature T(start=T_start) "Temperature of the passing fluid";
+protected
+  Medium.Temperature TMed(start=T_start) "Medium temperature to which the sensor is exposed";
+  Medium.Temperature T_a_inflow "Temperature of inflowing fluid at port_a";
+  Medium.Temperature T_b_inflow "Temperature of inflowing fluid at port_b, or T_a_inflow if uni-directional flow";
+initial equation
+  if dynamic then
+    if initType == Modelica.Blocks.Types.Init.SteadyState then
+      der(T) = 0;
+    elseif initType == Modelica.Blocks.Types.Init.InitialState or
+           initType == Modelica.Blocks.Types.Init.InitialOutput then
+      T = T_start;
+    end if;
+  end if;
+equation
+  if allowFlowReversal then
+     T_a_inflow = Medium.temperature(state=
+                    Medium.setState_phX(p=port_b.p, h=port_b.h_outflow, X=port_b.Xi_outflow));
+     T_b_inflow = Medium.temperature(state=
+                    Medium.setState_phX(p=port_a.p, h=port_a.h_outflow, X=port_a.Xi_outflow));
+     TMed = Modelica.Fluid.Utilities.regStep(
+              x=port_a.m_flow,
+              y1=T_a_inflow,
+              y2=T_b_inflow,
+              x_small=m_flow_small);
+  else
+     TMed = Medium.temperature(state=
+              Medium.setState_phX(p=port_b.p, h=port_b.h_outflow, X=port_b.Xi_outflow));
+     T_a_inflow = TMed;
+     T_b_inflow = TMed;
+  end if;
+  if dynamic then
+    der(T) = (TMed-T)*k*tauInv;
+  else
+    T = TMed;
+  end if;
+  Q_flow = port_a.m_flow * Medium.cp_const * (T - TExt);
+
+annotation (defaultComponentName="senHeaFlo",
+  Icon(graphics={
+        Ellipse(
+          fillColor={245,222,222},
+          fillPattern=FillPattern.Solid,
+          extent={{-70,-70},{70,70}}),
+        Line(points={{-100,0},{-70,0}}, color={0,128,255}),
+        Line(points={{70,0},{100,0}}, color={0,128,255}),
+        Line(points={{0,100},{0,70}}, color={0,0,127}),
+        Text(
+          extent={{180,151},{20,99}},
+          textColor={0,0,0},
+          textString="Q_flow"),
+        Text(
+          extent={{-20,120},{-140,70}},
+          textColor={0,0,0},
+          textString=DynamicSelect("", String(Q_flow, leftJustified=false, significantDigits=3))),
+        Text(
+          extent={{-22,120},{-100,48}},
+          textColor={0,0,127},
+          textString="TExt"),
+        Line(points={{37.6,13.7},{65.8,23.9}}),
+        Line(points={{22.9,32.8},{40.2,57.3}}),
+        Line(points={{0,70},{0,40}}),
+        Line(points={{-22.9,32.8},{-40.2,57.3}}),
+        Line(points={{-37.6,13.7},{-65.8,23.9}}),
+        Ellipse(
+          fillColor={64,64,64},
+          pattern=LinePattern.None,
+          fillPattern=FillPattern.Solid,
+          extent={{-7,-7},{7,7}}),
+        Polygon(
+          rotation=-17.5,
+          fillColor={64,64,64},
+          pattern=LinePattern.None,
+          fillPattern=FillPattern.Solid,
+          points={{-5.0,0.0},{-2.0,60.0},{0.0,65.0},{2.0,60.0},{5.0,0.0}}),
+        Ellipse(
+          lineColor={64,64,64},
+          fillColor={255,255,255},
+          extent={{-12,-12},{12,12}})}),
+Documentation(info="<html>
+<p>
+This model measures thermal energy provided between a supply and return pipe.
+It measures the capacity flow rate of the heat transfer fluid and the change in its
+temperature compared to an external temperature measurement that is input into the port
+<code>TExt</code>. The sensor does not influence the fluid.
+</p>
+<p>
+The rate of heat flow is calculated as <i>Q&#775; = m&#775; c<sub>p</sub> (T - T<sub>Ext</sub>)</i>.</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 1, 2024, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1831\">IBPSA, #1831</a>.
+</li>
+<li>
+February 1, 2024, by Jan Gall:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1831\">IBPSA, #1831</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end HeatMeter;
diff --git a/AixLib/Fluid/Sensors/LatentEnthalpyFlowRate.mo b/AixLib/Fluid/Sensors/LatentEnthalpyFlowRate.mo
index 28b818380a..a20ff97250 100644
--- a/AixLib/Fluid/Sensors/LatentEnthalpyFlowRate.mo
+++ b/AixLib/Fluid/Sensors/LatentEnthalpyFlowRate.mo
@@ -106,113 +106,113 @@ annotation (defaultComponentName="senLatEnt",
           textColor={0,0,0},
           textString=DynamicSelect("", String(H_flow, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the <i>latent</i> enthalphy flow rate of the medium in the flow
- between its fluid ports. In particular, if the total enthalpy flow rate is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   H&#775;<sub>tot</sub> = H&#775;<sub>sen</sub> + H&#775;<sub>lat</sub>,
- </p>
- <p>
- where
- <i>H&#775;<sub>sen</sub> = m&#775; (1-X<sub>w</sub>) c<sub>p,air</sub></i>,
- then this sensor outputs <i>H&#775; = H&#775;<sub>lat</sub></i>.
- </p>
- <p>
- If the parameter <code>tau</code> is non-zero, then the measured
- specific latent enthalpy <i>h<sub>out</sub></i> that is used to
- compute the latent enthalpy flow rate
- <i>H&#775;<sub>lat</sub> = m&#775; h<sub>out</sub></i>
- is computed using a first order differential equation.
- See <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- <p>
- For a sensor that measures
- <i>H&#775;<sub>tot</sub></i>, use
- <a href=\"modelica://AixLib.Fluid.Sensors.EnthalpyFlowRate\">
- AixLib.Fluid.Sensors.EnthalpyFlowRate</a>.<br/>
- For a sensor that measures
- <i>H&#775;<sub>sen</sub></i>, use
- <a href=\"modelica://AixLib.Fluid.Sensors.SensibleEnthalpyFlowRate\">
- AixLib.Fluid.Sensors.SensibleEnthalpyFlowRate</a>.
- </p>
- <p>
- The sensor is ideal, i.e., it does not influence the fluid.
- The sensor can only be used with medium models that implement the function
- <code>enthalpyOfNonCondensingGas(T)</code>.
- </p>
- </html>",
+<p>
+This model outputs the <i>latent</i> enthalphy flow rate of the medium in the flow
+between its fluid ports. In particular, if the total enthalpy flow rate is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  H&#775;<sub>tot</sub> = H&#775;<sub>sen</sub> + H&#775;<sub>lat</sub>,
+</p>
+<p>
+where
+<i>H&#775;<sub>sen</sub> = m&#775; (1-X<sub>w</sub>) c<sub>p,air</sub></i>,
+then this sensor outputs <i>H&#775; = H&#775;<sub>lat</sub></i>.
+</p>
+<p>
+If the parameter <code>tau</code> is non-zero, then the measured
+specific latent enthalpy <i>h<sub>out</sub></i> that is used to
+compute the latent enthalpy flow rate
+<i>H&#775;<sub>lat</sub> = m&#775; h<sub>out</sub></i>
+is computed using a first order differential equation.
+See <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+<p>
+For a sensor that measures
+<i>H&#775;<sub>tot</sub></i>, use
+<a href=\"modelica://AixLib.Fluid.Sensors.EnthalpyFlowRate\">
+AixLib.Fluid.Sensors.EnthalpyFlowRate</a>.<br/>
+For a sensor that measures
+<i>H&#775;<sub>sen</sub></i>, use
+<a href=\"modelica://AixLib.Fluid.Sensors.SensibleEnthalpyFlowRate\">
+AixLib.Fluid.Sensors.SensibleEnthalpyFlowRate</a>.
+</p>
+<p>
+The sensor is ideal, i.e., it does not influence the fluid.
+The sensor can only be used with medium models that implement the function
+<code>enthalpyOfNonCondensingGas(T)</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 19, 2020, by Antoine Gautier:<br/>
- Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Changed medium declaration in the <code>extends</code> statement
- to <code>replaceable</code> to avoid a translation error in
- OpenModelica.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Removed default value <code>tau=0</code> as the base class
- already sets <code>tau=1</code>.
- This change was made so that all sensors use the same default value.
- </li>
- <li>
- December 18, 2012, by Michael Wetter:<br/>
- Moved computation of <code>i_w</code> to new base class
- <a href=\"modelica://AixLib.Fluid.BaseClasses.IndexWater\">
- AixLib.Fluid.BaseClasses.IndexWater</a>.
- The value of this parameter is now assigned dynamically and does not require to be specified
- by the user.
- </li>
- <li>
- November 3, 2011, by Michael Wetter:<br/>
- Moved <code>der(h_out) := 0;</code> from the initial algorithm section to
- the initial equation section
- as this assignment does not conform to the Modelica specification.
- </li>
- <li>
- August 10, 2011 by Michael Wetter:<br/>
- Added parameter <code>i_w</code> and an assert statement to
- make sure it is set correctly. Without this change, Dymola
- cannot differentiate the model when reducing the index of the DAE.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This can improve the numerics.
- </li>
- <li>
- February 22, by Michael Wetter:<br/>
- Improved code that searches for index of 'water' in medium model.
- </li>
- <li>
- September 9, 2009 by Michael Wetter:<br/>
- First implementation.
- Implementation is based on enthalpy sensor of <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 19, 2020, by Antoine Gautier:<br/>
+Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Changed medium declaration in the <code>extends</code> statement
+to <code>replaceable</code> to avoid a translation error in
+OpenModelica.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Removed default value <code>tau=0</code> as the base class
+already sets <code>tau=1</code>.
+This change was made so that all sensors use the same default value.
+</li>
+<li>
+December 18, 2012, by Michael Wetter:<br/>
+Moved computation of <code>i_w</code> to new base class
+<a href=\"modelica://AixLib.Fluid.BaseClasses.IndexWater\">
+AixLib.Fluid.BaseClasses.IndexWater</a>.
+The value of this parameter is now assigned dynamically and does not require to be specified
+by the user.
+</li>
+<li>
+November 3, 2011, by Michael Wetter:<br/>
+Moved <code>der(h_out) := 0;</code> from the initial algorithm section to
+the initial equation section
+as this assignment does not conform to the Modelica specification.
+</li>
+<li>
+August 10, 2011 by Michael Wetter:<br/>
+Added parameter <code>i_w</code> and an assert statement to
+make sure it is set correctly. Without this change, Dymola
+cannot differentiate the model when reducing the index of the DAE.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This can improve the numerics.
+</li>
+<li>
+February 22, by Michael Wetter:<br/>
+Improved code that searches for index of 'water' in medium model.
+</li>
+<li>
+September 9, 2009 by Michael Wetter:<br/>
+First implementation.
+Implementation is based on enthalpy sensor of <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end LatentEnthalpyFlowRate;
diff --git a/AixLib/Fluid/Sensors/MassFlowRate.mo b/AixLib/Fluid/Sensors/MassFlowRate.mo
index 8b98b24a35..be2d05c642 100644
--- a/AixLib/Fluid/Sensors/MassFlowRate.mo
+++ b/AixLib/Fluid/Sensors/MassFlowRate.mo
@@ -30,31 +30,31 @@ Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}})
         textColor={0,0,0},
         textString=DynamicSelect("", String(m_flow, leftJustified=false, significantDigits=3)))}),
 Documentation(info="<html>
- <p>
- This model outputs the mass flow rate flowing from
- <code>port_a</code> to <code>port_b</code>.
- The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- Implementation is based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the mass flow rate flowing from
+<code>port_a</code> to <code>port_b</code>.
+The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+Implementation is based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFlowRate;
diff --git a/AixLib/Fluid/Sensors/MassFraction.mo b/AixLib/Fluid/Sensors/MassFraction.mo
index 9f15b87ebe..dd291dd8aa 100644
--- a/AixLib/Fluid/Sensors/MassFraction.mo
+++ b/AixLib/Fluid/Sensors/MassFraction.mo
@@ -36,68 +36,68 @@ annotation (defaultComponentName="senMasFra",
           textColor={0,0,0},
           textString=DynamicSelect("", String(X, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the mass fraction of the fluid connected to its port.
- The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- <p>
- To measure mass fraction in a duct or pipe, use
- <a href=\"modelica://AixLib.Fluid.Sensors.MassFractionTwoPort\">AixLib.Fluid.Sensors.MassFractionTwoPort</a>
- rather than this sensor.
- Read the
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a>
- prior to using this model to see about potential numerical problems if this sensor is used incorrectly
- in a system model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Corrected wrong assignment
- <code>XiVec[Medium.nXi](quantity=Medium.extraPropertiesNames)</code>
- to
- <code>XiVec[Medium.nXi](quantity=Medium.substanceNames[1:Medium.nXi])</code>.<br/>
- Changed unit of output signal from <code>1</code> to <code>kg/kg</code>
- to indicate that it is a mass fraction, and declared the assignment final.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Changed <code>min</code> and <code>max</code> values for
- output signals to allow for numerical approximation error
- without violating these bounds.<br/>
- Changed medium declaration in the <code>extends</code> statement
- to <code>replaceable</code> to avoid a translation error in
- OpenModelica.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Revised model to use base class
- <a href=\"modelica://AixLib.Fluid.BaseClasses.IndexMassFraction\">
- AixLib.Fluid.BaseClasses.IndexMassFraction</a>.
- </li>
- <li>
- February 22, by Michael Wetter:<br/>
- Improved the code that searches for the index of the substance in the medium model.
- </li>
- <li>
- April 7, 2009 by Michael Wetter:<br/>
- First implementation.
- Implementation is based on enthalpy sensor of <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the mass fraction of the fluid connected to its port.
+The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+<p>
+To measure mass fraction in a duct or pipe, use
+<a href=\"modelica://AixLib.Fluid.Sensors.MassFractionTwoPort\">AixLib.Fluid.Sensors.MassFractionTwoPort</a>
+rather than this sensor.
+Read the
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a>
+prior to using this model to see about potential numerical problems if this sensor is used incorrectly
+in a system model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Corrected wrong assignment
+<code>XiVec[Medium.nXi](quantity=Medium.extraPropertiesNames)</code>
+to
+<code>XiVec[Medium.nXi](quantity=Medium.substanceNames[1:Medium.nXi])</code>.<br/>
+Changed unit of output signal from <code>1</code> to <code>kg/kg</code>
+to indicate that it is a mass fraction, and declared the assignment final.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Changed <code>min</code> and <code>max</code> values for
+output signals to allow for numerical approximation error
+without violating these bounds.<br/>
+Changed medium declaration in the <code>extends</code> statement
+to <code>replaceable</code> to avoid a translation error in
+OpenModelica.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Revised model to use base class
+<a href=\"modelica://AixLib.Fluid.BaseClasses.IndexMassFraction\">
+AixLib.Fluid.BaseClasses.IndexMassFraction</a>.
+</li>
+<li>
+February 22, by Michael Wetter:<br/>
+Improved the code that searches for the index of the substance in the medium model.
+</li>
+<li>
+April 7, 2009 by Michael Wetter:<br/>
+First implementation.
+Implementation is based on enthalpy sensor of <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFraction;
diff --git a/AixLib/Fluid/Sensors/MassFractionTwoPort.mo b/AixLib/Fluid/Sensors/MassFractionTwoPort.mo
index 6fb9da10ca..ccf3f77281 100644
--- a/AixLib/Fluid/Sensors/MassFractionTwoPort.mo
+++ b/AixLib/Fluid/Sensors/MassFractionTwoPort.mo
@@ -68,77 +68,77 @@ annotation (defaultComponentName="senMasFra",
           textColor={0,0,0},
           textString=DynamicSelect("", String(X, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the mass fraction of the passing fluid.
- The sensor is ideal, i.e. it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then its output
- is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",
+<p>
+This model outputs the mass fraction of the passing fluid.
+The sensor is ideal, i.e. it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then its output
+is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Corrected wrong assignment
- <code>XiVec[Medium.nXi](quantity=Medium.extraPropertiesNames)</code>
- to
- <code>XiVec[Medium.nXi](quantity=Medium.substanceNames[1:Medium.nXi])</code>.<br/>
- Changed unit of output signal from <code>1</code> to <code>kg/kg</code>
- to indicate that it is a mass fraction, and declared the assignment final.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Changed <code>min</code> and <code>max</code> values for
- output signals to allow for numerical approximation error
- without violating these bounds.<br/>
- Changed medium declaration in the <code>extends</code> statement
- to <code>replaceable</code> to avoid a translation error in
- OpenModelica.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Revised model to use base class
- <a href=\"modelica://AixLib.Fluid.BaseClasses.IndexMassFraction\">
- AixLib.Fluid.BaseClasses.IndexMassFraction</a>.
- </li>
- <li>
- November 3, 2011, by Michael Wetter:<br/>
- Moved <code>der(X) := 0;</code> from the initial algorithm section to
- the initial equation section
- as this assignment does not conform to the Modelica specification.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- February 22, by Michael Wetter:<br/>
- Improved code that searches for index of the substance name in the medium model.
- </li>
- <li>
- Feb. 8, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Corrected wrong assignment
+<code>XiVec[Medium.nXi](quantity=Medium.extraPropertiesNames)</code>
+to
+<code>XiVec[Medium.nXi](quantity=Medium.substanceNames[1:Medium.nXi])</code>.<br/>
+Changed unit of output signal from <code>1</code> to <code>kg/kg</code>
+to indicate that it is a mass fraction, and declared the assignment final.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Changed <code>min</code> and <code>max</code> values for
+output signals to allow for numerical approximation error
+without violating these bounds.<br/>
+Changed medium declaration in the <code>extends</code> statement
+to <code>replaceable</code> to avoid a translation error in
+OpenModelica.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Revised model to use base class
+<a href=\"modelica://AixLib.Fluid.BaseClasses.IndexMassFraction\">
+AixLib.Fluid.BaseClasses.IndexMassFraction</a>.
+</li>
+<li>
+November 3, 2011, by Michael Wetter:<br/>
+Moved <code>der(X) := 0;</code> from the initial algorithm section to
+the initial equation section
+as this assignment does not conform to the Modelica specification.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+February 22, by Michael Wetter:<br/>
+Improved code that searches for index of the substance name in the medium model.
+</li>
+<li>
+Feb. 8, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFractionTwoPort;
diff --git a/AixLib/Fluid/Sensors/PPM.mo b/AixLib/Fluid/Sensors/PPM.mo
index 9046bc4d0b..3f35a9c4f3 100644
--- a/AixLib/Fluid/Sensors/PPM.mo
+++ b/AixLib/Fluid/Sensors/PPM.mo
@@ -70,59 +70,59 @@ annotation (defaultComponentName="senPPM",
           textColor={0,0,0},
           textString=DynamicSelect("", String(ppm, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the trace substance concentration in ppm contained in the fluid connected to its port.
- The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- <p>
- The parameter <code>MM</code> is the molar mass of the trace substance.
- For a list of molar masses, see
- <a href=\"modelica://Modelica.Media.IdealGases.Common.SingleGasesData\">
- Modelica.Media.IdealGases.Common.SingleGasesData</a>
- and
- <a href=\"modelica://Modelica.Media.IdealGases.Common.FluidData\">
- Modelica.Media.IdealGases.Common.FluidData</a>.
- </p>
- <p>
- To measure PPM in a duct or pipe, use
- <a href=\"modelica://AixLib.Fluid.Sensors.PPMTwoPort\">AixLib.Fluid.Sensors.PPMTwoPort</a>
- rather than this sensor.
- Read the
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a>
- prior to using this model to see about potential numerical problems if this sensor is used incorrectly
- in a system model.
- </p>
- <h4>Assumptions</h4>
- <p>
- This sensor assumes that the concentration <i>C</i> of the medium
- is in mass fraction. Otherwise, the conversion to <i>ppm</i> will be
- wrong.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- December 16, 2015, by Michael Wetter:<br/>
- Revised implementation, corrected error in the molar fraction which
- used the inverse ratio.
- </li>
- <li>
- December 2, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the trace substance concentration in ppm contained in the fluid connected to its port.
+The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+<p>
+The parameter <code>MM</code> is the molar mass of the trace substance.
+For a list of molar masses, see
+<a href=\"modelica://Modelica.Media.IdealGases.Common.SingleGasesData\">
+Modelica.Media.IdealGases.Common.SingleGasesData</a>
+and
+<a href=\"modelica://Modelica.Media.IdealGases.Common.FluidData\">
+Modelica.Media.IdealGases.Common.FluidData</a>.
+</p>
+<p>
+To measure PPM in a duct or pipe, use
+<a href=\"modelica://AixLib.Fluid.Sensors.PPMTwoPort\">AixLib.Fluid.Sensors.PPMTwoPort</a>
+rather than this sensor.
+Read the
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a>
+prior to using this model to see about potential numerical problems if this sensor is used incorrectly
+in a system model.
+</p>
+<h4>Assumptions</h4>
+<p>
+This sensor assumes that the concentration <i>C</i> of the medium
+is in mass fraction. Otherwise, the conversion to <i>ppm</i> will be
+wrong.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+December 16, 2015, by Michael Wetter:<br/>
+Revised implementation, corrected error in the molar fraction which
+used the inverse ratio.
+</li>
+<li>
+December 2, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PPM;
diff --git a/AixLib/Fluid/Sensors/PPMTwoPort.mo b/AixLib/Fluid/Sensors/PPMTwoPort.mo
index cb8e1de21e..7902cf3387 100644
--- a/AixLib/Fluid/Sensors/PPMTwoPort.mo
+++ b/AixLib/Fluid/Sensors/PPMTwoPort.mo
@@ -100,31 +100,31 @@ annotation (defaultComponentName="senPPM",
           textColor={0,0,0},
           textString=DynamicSelect("", String(ppm, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the trace substance of the passing fluid
- in parts per million.
- The sensor is ideal, i.e., it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then its output
- is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 12, 2016, by Filip Jorissen:<br/>
- First implementation.
- See issue
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the trace substance of the passing fluid
+in parts per million.
+The sensor is ideal, i.e., it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then its output
+is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 12, 2016, by Filip Jorissen:<br/>
+First implementation.
+See issue
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PPMTwoPort;
diff --git a/AixLib/Fluid/Sensors/Pressure.mo b/AixLib/Fluid/Sensors/Pressure.mo
index aea775c809..df49889a17 100644
--- a/AixLib/Fluid/Sensors/Pressure.mo
+++ b/AixLib/Fluid/Sensors/Pressure.mo
@@ -30,29 +30,29 @@ equation
           textColor={0,0,0},
           textString=DynamicSelect("", String(p, leftJustified=false, significantDigits=5)))}),
     Documentation(info="<html>
- <p>
- This model outputs the absolute pressure of the fluid connected to its port.
- The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- </html>",
+<p>
+This model outputs the absolute pressure of the fluid connected to its port.
+The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- May 9, 2017, by Filip Jorissen:<br/>
- Changed output quantity to <code>AbsolutePressure</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/770\">#770</a>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation, based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+May 9, 2017, by Filip Jorissen:<br/>
+Changed output quantity to <code>AbsolutePressure</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/770\">#770</a>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation, based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Pressure;
diff --git a/AixLib/Fluid/Sensors/RelativeHumidity.mo b/AixLib/Fluid/Sensors/RelativeHumidity.mo
index 1b7a14efa0..453b3cae99 100644
--- a/AixLib/Fluid/Sensors/RelativeHumidity.mo
+++ b/AixLib/Fluid/Sensors/RelativeHumidity.mo
@@ -41,48 +41,48 @@ annotation (defaultComponentName="senRelHum",
           textColor={0,0,0},
           textString=DynamicSelect("", String(phi, leftJustified=false, significantDigits=2)))}),
   Documentation(info="<html>
- <p>
- This model outputs the relative humidity of the fluid connected to its port.
- The sensor is ideal, i.e. it does not influence the fluid.
- </p>
- <p>
- Note that this sensor can only be used with media that contain the variable <code>phi</code>,
- which is typically the case for moist air models.
- </p>
- <p>
- To measure relative humidity in a duct or pipe, use
- <a href=\"modelica://AixLib.Fluid.Sensors.RelativeHumidityTwoPort\">AixLib.Fluid.Sensors.RelativeHumidityTwoPort</a>
- rather than this sensor.
- Read the
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a>
- prior to using this model to see about potential numerical problems if this sensor is used incorrectly
- in a system model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 26, 2016 by Michael Wetter:<br/>
- Added <code>quantity</code> attribute for mass fraction variables.<br/>
- Made unit assignment of output signal final.
- </li>
- <li>
- May 12, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the relative humidity of the fluid connected to its port.
+The sensor is ideal, i.e. it does not influence the fluid.
+</p>
+<p>
+Note that this sensor can only be used with media that contain the variable <code>phi</code>,
+which is typically the case for moist air models.
+</p>
+<p>
+To measure relative humidity in a duct or pipe, use
+<a href=\"modelica://AixLib.Fluid.Sensors.RelativeHumidityTwoPort\">AixLib.Fluid.Sensors.RelativeHumidityTwoPort</a>
+rather than this sensor.
+Read the
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a>
+prior to using this model to see about potential numerical problems if this sensor is used incorrectly
+in a system model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 26, 2016 by Michael Wetter:<br/>
+Added <code>quantity</code> attribute for mass fraction variables.<br/>
+Made unit assignment of output signal final.
+</li>
+<li>
+May 12, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RelativeHumidity;
diff --git a/AixLib/Fluid/Sensors/RelativeHumidityTwoPort.mo b/AixLib/Fluid/Sensors/RelativeHumidityTwoPort.mo
index 406f3a0803..68764f428d 100644
--- a/AixLib/Fluid/Sensors/RelativeHumidityTwoPort.mo
+++ b/AixLib/Fluid/Sensors/RelativeHumidityTwoPort.mo
@@ -100,54 +100,54 @@ annotation (defaultComponentName="senRelHum",
           textColor={0,0,0},
           textString=DynamicSelect("", String(phi, leftJustified=false, significantDigits=2)))}),
   Documentation(info="<html>
- <p>
- This model outputs the relative humidity of the fluid flowing from
- <code>port_a</code> to <code>port_b</code>.
- The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- <p>
- Note that this sensor can only be used with media that contain the variable <code>phi</code>,
- which is typically the case for moist air models.
- </p>
- <p>
- If the parameter <code>tau</code> is non-zero, then its output
- is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 26, 2016 by Michael Wetter:<br/>
- Added <code>quantity</code> attribute for mass fraction variables.<br/>
- Made unit assignment of output signal final.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- Feb. 5, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the relative humidity of the fluid flowing from
+<code>port_a</code> to <code>port_b</code>.
+The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+<p>
+Note that this sensor can only be used with media that contain the variable <code>phi</code>,
+which is typically the case for moist air models.
+</p>
+<p>
+If the parameter <code>tau</code> is non-zero, then its output
+is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 26, 2016 by Michael Wetter:<br/>
+Added <code>quantity</code> attribute for mass fraction variables.<br/>
+Made unit assignment of output signal final.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+Feb. 5, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RelativeHumidityTwoPort;
diff --git a/AixLib/Fluid/Sensors/RelativePressure.mo b/AixLib/Fluid/Sensors/RelativePressure.mo
index 69b28b4264..7985ce2c01 100644
--- a/AixLib/Fluid/Sensors/RelativePressure.mo
+++ b/AixLib/Fluid/Sensors/RelativePressure.mo
@@ -71,42 +71,42 @@ equation
           textColor={0,0,0},
           textString=DynamicSelect("", String(p_rel, leftJustified=false, significantDigits=3)))}),
     Documentation(info="<html>
- <p>
- The relative pressure <code>port_a.p - port_b.p</code> is determined between
- the two ports of this component and is provided as output signal. The
- sensor should be connected in parallel with other equipment, no flow
- through the sensor is allowed.
- </p>
- </html>",
+<p>
+The relative pressure <code>port_a.p - port_b.p</code> is determined between
+the two ports of this component and is provided as output signal. The
+sensor should be connected in parallel with other equipment, no flow
+through the sensor is allowed.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- February 19, 2016, by Michael Wetter:<br/>
- Corrected the quantity of the output signal from <code>Pressure</code>
- to <code>PressureDifference</code>.
- This was needed for the model
- <a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
- AixLib.Fluid.Movers.FlowControlled_m_flow</a>
- when revising it for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">
- issue 417</a>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation, based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+February 19, 2016, by Michael Wetter:<br/>
+Corrected the quantity of the output signal from <code>Pressure</code>
+to <code>PressureDifference</code>.
+This was needed for the model
+<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.FlowControlled_m_flow</a>
+when revising it for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/417\">
+issue 417</a>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation, based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RelativePressure;
diff --git a/AixLib/Fluid/Sensors/RelativeTemperature.mo b/AixLib/Fluid/Sensors/RelativeTemperature.mo
index b4a35b844d..823ac8fe54 100644
--- a/AixLib/Fluid/Sensors/RelativeTemperature.mo
+++ b/AixLib/Fluid/Sensors/RelativeTemperature.mo
@@ -71,40 +71,40 @@ equation
           textColor={0,0,0},
           textString=DynamicSelect("", String(T_rel, leftJustified=false, significantDigits=3)))}),
     Documentation(info="<html>
- <p>
- The relative temperature <code>T(port_a) - T(port_b)</code> is determined between
- the two ports of this component and is provided as output signal. The
- sensor should be connected in parallel with other equipment.
- There is no flow through the sensor.
- </p>
- <p>
- Note that this sensor should only be connected to fluid volumes, such as
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
- AixLib.Fluid.MixingVolumes.MixingVolume</a>. Otherwise, numerical
- problems may occur if one of the mass flow rates are close to zero.
- See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",
+<p>
+The relative temperature <code>T(port_a) - T(port_b)</code> is determined between
+the two ports of this component and is provided as output signal. The
+sensor should be connected in parallel with other equipment.
+There is no flow through the sensor.
+</p>
+<p>
+Note that this sensor should only be connected to fluid volumes, such as
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolume\">
+AixLib.Fluid.MixingVolumes.MixingVolume</a>. Otherwise, numerical
+problems may occur if one of the mass flow rates are close to zero.
+See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation, based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation, based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RelativeTemperature;
diff --git a/AixLib/Fluid/Sensors/SensibleEnthalpyFlowRate.mo b/AixLib/Fluid/Sensors/SensibleEnthalpyFlowRate.mo
index 35b500b084..0d67a40976 100644
--- a/AixLib/Fluid/Sensors/SensibleEnthalpyFlowRate.mo
+++ b/AixLib/Fluid/Sensors/SensibleEnthalpyFlowRate.mo
@@ -97,116 +97,116 @@ annotation (defaultComponentName="senEntFlo",
           textColor={0,0,0},
           textString=DynamicSelect("", String(H_flow, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the <i>sensible</i> enthalphy flow rate of the medium in the flow
- between its fluid ports. In particular, if the total enthalpy flow rate is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   H&#775;<sub>tot</sub> = H&#775;<sub>sen</sub> + H&#775;<sub>lat</sub>,
- </p>
- <p>
- where
- <i>H&#775;<sub>sen</sub> = m&#775; (1-X<sub>w</sub>) c<sub>p,air</sub></i>,
- then this sensor outputs <i>H&#775; = H&#775;<sub>sen</sub></i>.
- </p>
- 
- <p>
- If the parameter <code>tau</code> is non-zero, then the measured
- specific sensible enthalpy <i>h<sub>out</sub></i> that is used to
- compute the sensible enthalpy flow rate
- <i>H&#775;<sub>sen</sub> = m&#775; h<sub>out</sub></i>
- is computed using a first order differential equation.
- See <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- 
- <p>
- For a sensor that measures
- <i>H&#775;<sub>tot</sub></i>, use
- <a href=\"modelica://AixLib.Fluid.Sensors.EnthalpyFlowRate\">
- AixLib.Fluid.Sensors.EnthalpyFlowRate</a>.<br/>
- For a sensor that measures
- <i>H&#775;<sub>lat</sub></i>, use
- <a href=\"modelica://AixLib.Fluid.Sensors.LatentEnthalpyFlowRate\">
- AixLib.Fluid.Sensors.LatentEnthalpyFlowRate</a>.
- </p>
- 
- <p>
- The sensor is ideal, i.e., it does not influence the fluid.
- The sensor can only be used with medium models that implement the function
- <code>enthalpyOfNonCondensingGas(T)</code>.</p>
- 
- </html>",
+<p>
+This model outputs the <i>sensible</i> enthalphy flow rate of the medium in the flow
+between its fluid ports. In particular, if the total enthalpy flow rate is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  H&#775;<sub>tot</sub> = H&#775;<sub>sen</sub> + H&#775;<sub>lat</sub>,
+</p>
+<p>
+where
+<i>H&#775;<sub>sen</sub> = m&#775; (1-X<sub>w</sub>) c<sub>p,air</sub></i>,
+then this sensor outputs <i>H&#775; = H&#775;<sub>sen</sub></i>.
+</p>
+
+<p>
+If the parameter <code>tau</code> is non-zero, then the measured
+specific sensible enthalpy <i>h<sub>out</sub></i> that is used to
+compute the sensible enthalpy flow rate
+<i>H&#775;<sub>sen</sub> = m&#775; h<sub>out</sub></i>
+is computed using a first order differential equation.
+See <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+
+<p>
+For a sensor that measures
+<i>H&#775;<sub>tot</sub></i>, use
+<a href=\"modelica://AixLib.Fluid.Sensors.EnthalpyFlowRate\">
+AixLib.Fluid.Sensors.EnthalpyFlowRate</a>.<br/>
+For a sensor that measures
+<i>H&#775;<sub>lat</sub></i>, use
+<a href=\"modelica://AixLib.Fluid.Sensors.LatentEnthalpyFlowRate\">
+AixLib.Fluid.Sensors.LatentEnthalpyFlowRate</a>.
+</p>
+
+<p>
+The sensor is ideal, i.e., it does not influence the fluid.
+The sensor can only be used with medium models that implement the function
+<code>enthalpyOfNonCondensingGas(T)</code>.</p>
+
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 19, 2020, by Antoine Gautier:<br/>
- Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Changed medium declaration in the <code>extends</code> statement
- to <code>replaceable</code> to avoid a translation error in
- OpenModelica.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Removed default value <code>tau=0</code> as the base class
- already sets <code>tau=1</code>.
- This change was made so that all sensors use the same default value.
- </li>
- <li>
- December 18, 2012, by Michael Wetter:<br/>
- Moved computation of <code>i_w</code> to new base class
- <a href=\"modelica://AixLib.Fluid.BaseClasses.IndexWater\">
- AixLib.Fluid.BaseClasses.IndexWater</a>.
- The value of this parameter is now assigned dynamically and does not require to be specified
- by the user.
- </li>
- <li>
- November 3, 2011, by Michael Wetter:<br/>
- Moved <code>der(h_out) := 0;</code> from the initial algorithm section to
- the initial equation section
- as this assignment does not conform to the Modelica specification.
- </li>
- <li>
- August 10, 2011 by Michael Wetter:<br/>
- Added parameter <code>i_w</code> and an assert statement to
- make sure it is set correctly. Without this change, Dymola
- cannot differentiate the model when reducing the index of the DAE.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This can improve the numerics.
- </li>
- <li>
- February 22, by Michael Wetter:<br/>
- Improved code that searches for index of 'water' in the medium model.
- </li>
- <li>
- September 9, 2009 by Michael Wetter:<br/>
- First implementation.
- Implementation is based on enthalpy sensor of <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 19, 2020, by Antoine Gautier:<br/>
+Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Changed medium declaration in the <code>extends</code> statement
+to <code>replaceable</code> to avoid a translation error in
+OpenModelica.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Removed default value <code>tau=0</code> as the base class
+already sets <code>tau=1</code>.
+This change was made so that all sensors use the same default value.
+</li>
+<li>
+December 18, 2012, by Michael Wetter:<br/>
+Moved computation of <code>i_w</code> to new base class
+<a href=\"modelica://AixLib.Fluid.BaseClasses.IndexWater\">
+AixLib.Fluid.BaseClasses.IndexWater</a>.
+The value of this parameter is now assigned dynamically and does not require to be specified
+by the user.
+</li>
+<li>
+November 3, 2011, by Michael Wetter:<br/>
+Moved <code>der(h_out) := 0;</code> from the initial algorithm section to
+the initial equation section
+as this assignment does not conform to the Modelica specification.
+</li>
+<li>
+August 10, 2011 by Michael Wetter:<br/>
+Added parameter <code>i_w</code> and an assert statement to
+make sure it is set correctly. Without this change, Dymola
+cannot differentiate the model when reducing the index of the DAE.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This can improve the numerics.
+</li>
+<li>
+February 22, by Michael Wetter:<br/>
+Improved code that searches for index of 'water' in the medium model.
+</li>
+<li>
+September 9, 2009 by Michael Wetter:<br/>
+First implementation.
+Implementation is based on enthalpy sensor of <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SensibleEnthalpyFlowRate;
diff --git a/AixLib/Fluid/Sensors/SpecificEnthalpy.mo b/AixLib/Fluid/Sensors/SpecificEnthalpy.mo
index d62b78151e..b36db9d9e6 100644
--- a/AixLib/Fluid/Sensors/SpecificEnthalpy.mo
+++ b/AixLib/Fluid/Sensors/SpecificEnthalpy.mo
@@ -26,40 +26,40 @@ annotation (defaultComponentName="senSpeEnt",
           textColor={0,0,0},
           textString=DynamicSelect("", String(h_out, format=".0f")))}),
   Documentation(info="<html>
- <p>
- This model outputs the specific enthalpy of the fluid connected to its port.
- The sensor is ideal, i.e. it does not influence the fluid.
- </p>
- <p>
- To measure specific enthalpy in a duct or pipe, use
- <a href=\"modelica://AixLib.Fluid.Sensors.SpecificEnthalpyTwoPort\">AixLib.Fluid.Sensors.SpecificEnthalpyTwoPort</a>
- rather than this sensor.
- Read the
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a>
- prior to using this model to see about potential numerical problems if this sensor is used incorrectly
- in a system model.
- </p>
- </html>",
+<p>
+This model outputs the specific enthalpy of the fluid connected to its port.
+The sensor is ideal, i.e. it does not influence the fluid.
+</p>
+<p>
+To measure specific enthalpy in a duct or pipe, use
+<a href=\"modelica://AixLib.Fluid.Sensors.SpecificEnthalpyTwoPort\">AixLib.Fluid.Sensors.SpecificEnthalpyTwoPort</a>
+rather than this sensor.
+Read the
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a>
+prior to using this model to see about potential numerical problems if this sensor is used incorrectly
+in a system model.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 21, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 21, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpecificEnthalpy;
diff --git a/AixLib/Fluid/Sensors/SpecificEnthalpyTwoPort.mo b/AixLib/Fluid/Sensors/SpecificEnthalpyTwoPort.mo
index 183c2d922e..9cb80b860c 100644
--- a/AixLib/Fluid/Sensors/SpecificEnthalpyTwoPort.mo
+++ b/AixLib/Fluid/Sensors/SpecificEnthalpyTwoPort.mo
@@ -59,43 +59,43 @@ annotation (defaultComponentName="senSpeEnt",
           textColor={0,0,0},
           textString=DynamicSelect("", String(h_out, format=".0f")))}),
   Documentation(info="<html>
- <p>
- This model outputs the specific enthalpy of a passing fluid.
- The sensor is ideal, i.e. it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then its output
- is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",
+<p>
+This model outputs the specific enthalpy of a passing fluid.
+The sensor is ideal, i.e. it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then its output
+is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpecificEnthalpyTwoPort;
diff --git a/AixLib/Fluid/Sensors/SpecificEntropy.mo b/AixLib/Fluid/Sensors/SpecificEntropy.mo
index daa67f561c..321496d4c7 100644
--- a/AixLib/Fluid/Sensors/SpecificEntropy.mo
+++ b/AixLib/Fluid/Sensors/SpecificEntropy.mo
@@ -29,40 +29,40 @@ annotation (defaultComponentName="senSpeEnt",
           textColor={0,0,0},
           textString=DynamicSelect("", String(s, format=".0f")))}),
   Documentation(info="<html>
- <p>
- This model outputs the specific entropy of the fluid connected to its port.
- The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- <p>
- To measure specific entropy in a duct or pipe, use
- <a href=\"modelica://AixLib.Fluid.Sensors.SpecificEntropyTwoPort\">AixLib.Fluid.Sensors.SpecificEntropyTwoPort</a>
- rather than this sensor.
- Read the
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a>
- prior to using this model to see about potential numerical problems if this sensor is used incorrectly
- in a system model.
- </p>
- </html>",
+<p>
+This model outputs the specific entropy of the fluid connected to its port.
+The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+<p>
+To measure specific entropy in a duct or pipe, use
+<a href=\"modelica://AixLib.Fluid.Sensors.SpecificEntropyTwoPort\">AixLib.Fluid.Sensors.SpecificEntropyTwoPort</a>
+rather than this sensor.
+Read the
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a>
+prior to using this model to see about potential numerical problems if this sensor is used incorrectly
+in a system model.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 21, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 21, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpecificEntropy;
diff --git a/AixLib/Fluid/Sensors/SpecificEntropyTwoPort.mo b/AixLib/Fluid/Sensors/SpecificEntropyTwoPort.mo
index a0924dfdbd..19cd3abeb0 100644
--- a/AixLib/Fluid/Sensors/SpecificEntropyTwoPort.mo
+++ b/AixLib/Fluid/Sensors/SpecificEntropyTwoPort.mo
@@ -71,46 +71,46 @@ annotation (defaultComponentName="senSpeEnt",
           textColor={0,0,0},
           textString=DynamicSelect("", String(s, format=".0f")))}),
   Documentation(info="<html>
- <p>
- This model outputs the specific entropy of the passing fluid.
- The sensor is ideal, i.e., it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then its output
- is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Corrected wrong computation of <code>s</code> and <code>sMed</code>.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the specific entropy of the passing fluid.
+The sensor is ideal, i.e., it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then its output
+is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Corrected wrong computation of <code>s</code> and <code>sMed</code>.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpecificEntropyTwoPort;
diff --git a/AixLib/Fluid/Sensors/Temperature.mo b/AixLib/Fluid/Sensors/Temperature.mo
index eb9fcb40b0..0165ff739e 100644
--- a/AixLib/Fluid/Sensors/Temperature.mo
+++ b/AixLib/Fluid/Sensors/Temperature.mo
@@ -16,42 +16,42 @@ equation
 annotation (
   defaultComponentName="senTem",
   Documentation(info="<html>
- <p>
- This model outputs the temperature of the fluid connected to its port.
- The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- <p>
- To measure temperature in a duct or pipe, use
- <a href=\"modelica://AixLib.Fluid.Sensors.TemperatureTwoPort\">AixLib.Fluid.Sensors.TemperatureTwoPort</a>
- rather than this sensor.
- Read the
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a>
- prior to using this model to see about potential numerical problems if this sensor is used incorrectly
- in a system model.
- </p>
- </html>",
+<p>
+This model outputs the temperature of the fluid connected to its port.
+The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+<p>
+To measure temperature in a duct or pipe, use
+<a href=\"modelica://AixLib.Fluid.Sensors.TemperatureTwoPort\">AixLib.Fluid.Sensors.TemperatureTwoPort</a>
+rather than this sensor.
+Read the
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a>
+prior to using this model to see about potential numerical problems if this sensor is used incorrectly
+in a system model.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 21, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
- </li>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- Implementation is based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+September 21, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+Implementation is based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),
   Diagram(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{100,100}}),
                         graphics={
         Line(points={{0,-70},{0,-100}}, color={0,0,127}),
@@ -120,6 +120,6 @@ revisions="<html>
         Text(
           extent={{180,90},{60,40}},
           textColor={0,0,0},
-          textString=DynamicSelect("", String(T-273.15, format=".1f")))}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString=DynamicSelect("", String(T-273.15, format=".1f")))}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Temperature;
diff --git a/AixLib/Fluid/Sensors/TemperatureTwoPort.mo b/AixLib/Fluid/Sensors/TemperatureTwoPort.mo
index f4344f11b0..fe996e9819 100644
--- a/AixLib/Fluid/Sensors/TemperatureTwoPort.mo
+++ b/AixLib/Fluid/Sensors/TemperatureTwoPort.mo
@@ -123,86 +123,86 @@ annotation (defaultComponentName="senTem",
           textColor={0,0,0},
           textString=DynamicSelect("", String(T-273.15, format=".1f")))}),
     Documentation(info="<html>
- <p>
- This model outputs the temperature of the medium in the flow
- between its fluid ports. The sensor does not influence the fluid.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- If the parameter <code>tau</code> is non-zero, then its output <i>T</i>
- converges to the temperature of the incoming fluid using
- a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- <p>
- If <code>transferHeat = true</code>, then heat transfer with the ambient is
- approximated and <i>T</i> converges towards the fixed ambient
- temperature <i>T<sub>Amb</sub></i> using a first order approximation
- with a time constant of <code>tauHeaTra</code>
- when the flow rate is small.
- Note that no energy is exchanged with the fluid as the
- sensor does not influence the fluid temperature.
- </p>
- <p>
- Setting <code>transferHeat = true</code> is useful, for example,
- if the sensor is used to measure the fluid temperature in
- a system with on/off control on the mass flow rate.
- If <code>transferHeat</code> were <code>false</code>, then the sensor output <i>T</i>
- would remain constant if the mass flow rate is set to zero, and hence
- the controller may never switch the mass flow rate on again.
- </p>
- <p>
- In general, applications in which the sensor output is not used to switch
- the mass flow rate on should set <code>transferHeat=false</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- October 23, 2017 by Filip Jorissen:<br/>
- Revised implementation of equations
- when <code>transferHeat=true</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/840\">#840</a>.
- </li>
- <li>
- January 12, 2016 by Filip Jorissen:<br/>
- Removed parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- </li>
- <li>
- June 19, 2015 by Michael Wetter:<br/>
- Revised model and documentation.
- </li>
- <li>
- June 18, 2015 by Filip Jorissen:<br/>
- Added option for simulating thermal losses.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- February 26, 2010 by Michael Wetter:<br/>
- Set start attribute for temperature output. Prior to this change,
- the output was 0 at initial time, which caused the plot of the output to
- use 0 Kelvin as the lower value of the ordinate.
- </li>
- <li>
- September 10, 2008, by Michael Wetter:<br/>
- First implementation, based on
- <a href=\"modelica://AixLib.Fluid.Sensors.Temperature\">AixLib.Fluid.Sensors.Temperature</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the temperature of the medium in the flow
+between its fluid ports. The sensor does not influence the fluid.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+If the parameter <code>tau</code> is non-zero, then its output <i>T</i>
+converges to the temperature of the incoming fluid using
+a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+<p>
+If <code>transferHeat = true</code>, then heat transfer with the ambient is
+approximated and <i>T</i> converges towards the fixed ambient
+temperature <i>T<sub>Amb</sub></i> using a first order approximation
+with a time constant of <code>tauHeaTra</code>
+when the flow rate is small.
+Note that no energy is exchanged with the fluid as the
+sensor does not influence the fluid temperature.
+</p>
+<p>
+Setting <code>transferHeat = true</code> is useful, for example,
+if the sensor is used to measure the fluid temperature in
+a system with on/off control on the mass flow rate.
+If <code>transferHeat</code> were <code>false</code>, then the sensor output <i>T</i>
+would remain constant if the mass flow rate is set to zero, and hence
+the controller may never switch the mass flow rate on again.
+</p>
+<p>
+In general, applications in which the sensor output is not used to switch
+the mass flow rate on should set <code>transferHeat=false</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+October 23, 2017 by Filip Jorissen:<br/>
+Revised implementation of equations
+when <code>transferHeat=true</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/840\">#840</a>.
+</li>
+<li>
+January 12, 2016 by Filip Jorissen:<br/>
+Removed parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+</li>
+<li>
+June 19, 2015 by Michael Wetter:<br/>
+Revised model and documentation.
+</li>
+<li>
+June 18, 2015 by Filip Jorissen:<br/>
+Added option for simulating thermal losses.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+February 26, 2010 by Michael Wetter:<br/>
+Set start attribute for temperature output. Prior to this change,
+the output was 0 at initial time, which caused the plot of the output to
+use 0 Kelvin as the lower value of the ordinate.
+</li>
+<li>
+September 10, 2008, by Michael Wetter:<br/>
+First implementation, based on
+<a href=\"modelica://AixLib.Fluid.Sensors.Temperature\">AixLib.Fluid.Sensors.Temperature</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureTwoPort;
diff --git a/AixLib/Fluid/Sensors/TemperatureWetBulbTwoPort.mo b/AixLib/Fluid/Sensors/TemperatureWetBulbTwoPort.mo
index 2ed4373229..01bd567670 100644
--- a/AixLib/Fluid/Sensors/TemperatureWetBulbTwoPort.mo
+++ b/AixLib/Fluid/Sensors/TemperatureWetBulbTwoPort.mo
@@ -53,7 +53,10 @@ equation
     Xi = port_b.Xi_outflow;
   end if;
   // Compute wet bulb temperature
-  wetBulMod.TDryBul = Medium.temperature_phX(p=port_a.p, h=h, X=cat(1,Xi,{1-sum(Xi)}));
+  wetBulMod.TDryBul = Medium.temperature_phX(
+    p=port_a.p,
+    h=h,
+    X=if Medium.reducedX then cat(1, Xi, {1-sum(Xi)}) else Xi);
   wetBulMod.Xi = Xi;
   wetBulMod.p  = port_a.p;
   TMedWetBul = wetBulMod.TWetBul;
@@ -101,58 +104,64 @@ annotation (defaultComponentName="senWetBul",
           textColor={0,0,0},
           textString=DynamicSelect("", String(T-273.15, format=".1f")))}),
     Documentation(info="<html>
- <p>
- This sensor outputs the wet bulb temperature of the medium in the flow
- between its fluid ports. The sensor is ideal, i.e., it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then its output
- is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",
+<p>
+This sensor outputs the wet bulb temperature of the medium in the flow
+between its fluid ports. The sensor is ideal, i.e., it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then its output
+is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 21, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- September 10, 2013 by Michael Wetter:<br/>
- Set <code>start</code> attribute for <code>wetBulMod</code>
- to use consistent start values within this model.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- February 18, 2010, by Michael Wetter:<br/>
- Revised model to use new block for computing the wet bulb temperature.
- </li>
- <li>
- September 10, 2008, by Michael Wetter:<br/>
- Renamed output port to have the same interfaces as the dry bulb temperature sensor.
- </li>
- <li>
- May 5, 2008, by Michael Wetter:<br/>
- First implementation.
- Implementation is based on
- <a href=\"modelica://AixLib.Fluid.Sensors.Temperature\">AixLib.Fluid.Sensors.Temperature</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 24, 2022, by Michael Wetter:<br/>
+Improved conversion from <code>Xi</code> to <code>X</code> so that it also works
+with media that have <code>reducedX=true</code>.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1650\">#1650</a>.
+</li>
+<li>
+February 21, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+September 10, 2013 by Michael Wetter:<br/>
+Set <code>start</code> attribute for <code>wetBulMod</code>
+to use consistent start values within this model.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+February 18, 2010, by Michael Wetter:<br/>
+Revised model to use new block for computing the wet bulb temperature.
+</li>
+<li>
+September 10, 2008, by Michael Wetter:<br/>
+Renamed output port to have the same interfaces as the dry bulb temperature sensor.
+</li>
+<li>
+May 5, 2008, by Michael Wetter:<br/>
+First implementation.
+Implementation is based on
+<a href=\"modelica://AixLib.Fluid.Sensors.Temperature\">AixLib.Fluid.Sensors.Temperature</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureWetBulbTwoPort;
diff --git a/AixLib/Fluid/Sensors/TraceSubstances.mo b/AixLib/Fluid/Sensors/TraceSubstances.mo
index e38e29b6c4..f26b1b7b69 100644
--- a/AixLib/Fluid/Sensors/TraceSubstances.mo
+++ b/AixLib/Fluid/Sensors/TraceSubstances.mo
@@ -45,61 +45,61 @@ annotation (defaultComponentName="senTraSub",
           textColor={0,0,0},
           textString=DynamicSelect("", String(C, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the trace substances contained in the fluid connected to its port.
- The sensor is ideal, i.e., it does not influence the fluid.
- </p>
- <p>
- To measure trace substances in a duct or pipe, use
- <a href=\"modelica://AixLib.Fluid.Sensors.TraceSubstancesTwoPort\">AixLib.Fluid.Sensors.TraceSubstancesTwoPort</a>
- rather than this sensor.
- Read the
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a>
- prior to using this model to see about potential numerical problems if this sensor is used incorrectly
- in a system model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2020, by Michael Wetter:<br/>
- Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- June 10, 2015, by Michael Wetter:<br/>
- Reformulated assignment of <code>s</code> and <code>assert</code>
- statement. The reformulation of the assignment of <code>s</code> was
- done to allow a model check in non-pedantic mode.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/268\">issue 268</a>.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Corrected a syntax error in setting the nominal value for the output signal.
- This eliminates a compilation error in OpenModelica.
- </li>
- <li>
- February 22, by Michael Wetter:<br/>
- Improved code that searches for index of trace substance in medium model.
- </li>
- <li>
- March 22, 2010 by Michael Wetter:<br/>
- Changed assignment for <code>C</code> so that Dymola 7.4 can find
- the analytic derivative.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the trace substances contained in the fluid connected to its port.
+The sensor is ideal, i.e., it does not influence the fluid.
+</p>
+<p>
+To measure trace substances in a duct or pipe, use
+<a href=\"modelica://AixLib.Fluid.Sensors.TraceSubstancesTwoPort\">AixLib.Fluid.Sensors.TraceSubstancesTwoPort</a>
+rather than this sensor.
+Read the
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a>
+prior to using this model to see about potential numerical problems if this sensor is used incorrectly
+in a system model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2020, by Michael Wetter:<br/>
+Introduced parameter <code>warnAboutOnePortConnection</code> and updated documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1399\">#1399</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+June 10, 2015, by Michael Wetter:<br/>
+Reformulated assignment of <code>s</code> and <code>assert</code>
+statement. The reformulation of the assignment of <code>s</code> was
+done to allow a model check in non-pedantic mode.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/268\">issue 268</a>.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Corrected a syntax error in setting the nominal value for the output signal.
+This eliminates a compilation error in OpenModelica.
+</li>
+<li>
+February 22, by Michael Wetter:<br/>
+Improved code that searches for index of trace substance in medium model.
+</li>
+<li>
+March 22, 2010 by Michael Wetter:<br/>
+Changed assignment for <code>C</code> so that Dymola 7.4 can find
+the analytic derivative.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TraceSubstances;
diff --git a/AixLib/Fluid/Sensors/TraceSubstancesTwoPort.mo b/AixLib/Fluid/Sensors/TraceSubstancesTwoPort.mo
index 1f1bd65d3e..d791be9fe7 100644
--- a/AixLib/Fluid/Sensors/TraceSubstancesTwoPort.mo
+++ b/AixLib/Fluid/Sensors/TraceSubstancesTwoPort.mo
@@ -70,82 +70,82 @@ annotation (defaultComponentName="senTraSub",
           textColor={0,0,0},
           textString=DynamicSelect("", String(C, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the trace substance of the passing fluid.
- The sensor is ideal, i.e., it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then its output
- is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Avoided assignment of <code>CMed(nominal=0)</code> as this is
- not allowed.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- June 10, 2015, by Michael Wetter:<br/>
- Reformulated assignment of <code>s</code> and <code>assert</code>
- statement. The reformulation of the assignment of <code>s</code> was
- done to allow a model check in non-pedantic mode.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/268\">issue 268</a>.
- </li>
- <li>
- May 22, 2015, by Michael Wetter:<br/>
- Corrected wrong sensor signal if <code>allowFlowReversal=false</code>.
- For this setting, the sensor output was for the wrong flow direction.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/249\">issue 249</a>.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Corrected syntax errors in setting nominal value for output signal
- and for state variable.
- This eliminates a compilation error in OpenModelica.
- </li>
- <li>
- August 30, 2013, by Michael Wetter:<br/>
- Added default value <code>C_start=0</code>.
- </li>
- <li>
- November 3, 2011, by Michael Wetter:<br/>
- Moved <code>der(C) := 0;</code> from the initial algorithm section to
- the initial equation section
- as this assignment does not conform to the Modelica specification.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- February 22, by Michael Wetter:<br/>
- Improved code that searches for index of trace substance in medium model.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the trace substance of the passing fluid.
+The sensor is ideal, i.e., it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then its output
+is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Avoided assignment of <code>CMed(nominal=0)</code> as this is
+not allowed.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+June 10, 2015, by Michael Wetter:<br/>
+Reformulated assignment of <code>s</code> and <code>assert</code>
+statement. The reformulation of the assignment of <code>s</code> was
+done to allow a model check in non-pedantic mode.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/268\">issue 268</a>.
+</li>
+<li>
+May 22, 2015, by Michael Wetter:<br/>
+Corrected wrong sensor signal if <code>allowFlowReversal=false</code>.
+For this setting, the sensor output was for the wrong flow direction.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/249\">issue 249</a>.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Corrected syntax errors in setting nominal value for output signal
+and for state variable.
+This eliminates a compilation error in OpenModelica.
+</li>
+<li>
+August 30, 2013, by Michael Wetter:<br/>
+Added default value <code>C_start=0</code>.
+</li>
+<li>
+November 3, 2011, by Michael Wetter:<br/>
+Moved <code>der(C) := 0;</code> from the initial algorithm section to
+the initial equation section
+as this assignment does not conform to the Modelica specification.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+February 22, by Michael Wetter:<br/>
+Improved code that searches for index of trace substance in medium model.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TraceSubstancesTwoPort;
diff --git a/AixLib/Fluid/Sensors/UsersGuide.mo b/AixLib/Fluid/Sensors/UsersGuide.mo
index b910f2792a..bfe6f893b1 100644
--- a/AixLib/Fluid/Sensors/UsersGuide.mo
+++ b/AixLib/Fluid/Sensors/UsersGuide.mo
@@ -60,7 +60,7 @@ Sensors for quantities that depend on the direction of the mass flow rate but
 not of its magnitude:
 </em>
 Such quantities include density, mass fraction, PPM, relative humidity, specific enthalpy, specific entropy and trace substances.
-Not that these are all quantities that are carried by the fluid that flows through the sensor.
+Note that these are all quantities that are carried by the fluid that flows through the sensor.
 For these sensors, if the parameter <code>allowFlowReversal=true</code> is set (which is the default setting),
 then it is strongly recommended to configure them
 as a dynamic sensor. This is the default setting.<br/>
diff --git a/AixLib/Fluid/Sensors/Velocity.mo b/AixLib/Fluid/Sensors/Velocity.mo
index 4abedbeaa9..13ed468114 100644
--- a/AixLib/Fluid/Sensors/Velocity.mo
+++ b/AixLib/Fluid/Sensors/Velocity.mo
@@ -89,46 +89,46 @@ annotation (defaultComponentName="senVel",
           textColor={0,0,0},
           textString=DynamicSelect("", String(v, format=".3g")))}),
   Documentation(info="<html>
- <p>
- This model outputs the flow velocity flowing from
- <code>port_a</code> to <code>port_b</code>.
- </p>
- <p>
- The sensor is ideal, i.e., it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then the measured
- density that is used to convert the mass flow rate into
- volumetric flow rate is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- In order to use the flow velocity sensor, the cross sectional area of the flow
- channel <code>crossSection</code> must be specified in <code>m<sub>2</sub></code>. For a
- circular flow channel (e.g. a round pipe) of diameter <code>diameter</code>, the
- cross sectional area can be specified as <code>crossSection = diameter *
- diameter / 4 * Modelica.Constants.pi</code>. See
- <a href=\"modelica://AixLib.Fluid.Sensors.Examples.Velocity\">
- AixLib.Fluid.Sensors.Examples.Velocity</a> for an example implementation
- with <code>diameter = 0.1</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- May 20, 2016, by Marcus Fuchs:<br/>
- First implementation.
- Implementation is based on
- <a href=\"modelica://AixLib.Fluid.Sensors.VolumeFlowRate\">
- AixLib.Fluid.Sensors.VolumeFlowRate</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the flow velocity flowing from
+<code>port_a</code> to <code>port_b</code>.
+</p>
+<p>
+The sensor is ideal, i.e., it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then the measured
+density that is used to convert the mass flow rate into
+volumetric flow rate is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+In order to use the flow velocity sensor, the cross sectional area of the flow
+channel <code>crossSection</code> must be specified in <code>m<sub>2</sub></code>. For a
+circular flow channel (e.g. a round pipe) of diameter <code>diameter</code>, the
+cross sectional area can be specified as <code>crossSection = diameter *
+diameter / 4 * Modelica.Constants.pi</code>. See
+<a href=\"modelica://AixLib.Fluid.Sensors.Examples.Velocity\">
+AixLib.Fluid.Sensors.Examples.Velocity</a> for an example implementation
+with <code>diameter = 0.1</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+May 20, 2016, by Marcus Fuchs:<br/>
+First implementation.
+Implementation is based on
+<a href=\"modelica://AixLib.Fluid.Sensors.VolumeFlowRate\">
+AixLib.Fluid.Sensors.VolumeFlowRate</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Velocity;
diff --git a/AixLib/Fluid/Sensors/VolumeFlowRate.mo b/AixLib/Fluid/Sensors/VolumeFlowRate.mo
index 62693635b4..777264e9d2 100644
--- a/AixLib/Fluid/Sensors/VolumeFlowRate.mo
+++ b/AixLib/Fluid/Sensors/VolumeFlowRate.mo
@@ -25,7 +25,7 @@ model VolumeFlowRate "Ideal sensor for volume flow rate"
         rotation=270)));
 protected
   Medium.Density dMed(start=d_start)
-    "Medium temperature to which the sensor is exposed";
+    "Medium density to which the sensor is exposed";
 
   Medium.Density d_a_inflow(start=d_start)
     "Density of inflowing fluid at port_a";
@@ -84,57 +84,57 @@ annotation (defaultComponentName="senVolFlo",
           textColor={0,0,0},
           textString=DynamicSelect("", String(V_flow, leftJustified=false, significantDigits=3)))}),
   Documentation(info="<html>
- <p>
- This model outputs the volume flow rate flowing from
- <code>port_a</code> to <code>port_b</code>.
- The sensor is ideal, i.e., it does not influence the fluid.
- If the parameter <code>tau</code> is non-zero, then the measured
- density that is used to convert the mass flow rate into
- volumetric flow rate is computed using a first order differential equation.
- Setting <code>tau=0</code> is <i>not</i> recommend. See
- <a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
- AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 19, 2020, by Antoine Gautier:<br/>
- Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
- </li>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- January 18, 2016 by Filip Jorissen:<br/>
- Using parameter <code>tauInv</code>
- since this now exists in
- <a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
- </li>
- <li>
- August 31, 2013, by Michael Wetter:<br/>
- Removed default value <code>tau=0</code> as the base class
- already sets <code>tau=1</code>.
- This change was made so that all sensors use the same default value.
- </li>
- <li>
- June 3, 2011 by Michael Wetter:<br/>
- Revised implementation to add dynamics in such a way that
- the time constant increases as the mass flow rate tends to zero.
- This significantly improves the numerics.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- Implementation is based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model outputs the volume flow rate flowing from
+<code>port_a</code> to <code>port_b</code>.
+The sensor is ideal, i.e., it does not influence the fluid.
+If the parameter <code>tau</code> is non-zero, then the measured
+density that is used to convert the mass flow rate into
+volumetric flow rate is computed using a first order differential equation.
+Setting <code>tau=0</code> is <i>not</i> recommend. See
+<a href=\"modelica://AixLib.Fluid.Sensors.UsersGuide\">
+AixLib.Fluid.Sensors.UsersGuide</a> for an explanation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 19, 2020, by Antoine Gautier:<br/>
+Changed default value for <code>tau</code> from <code>1</code> to <code>0</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1406\">#1406</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+January 18, 2016 by Filip Jorissen:<br/>
+Using parameter <code>tauInv</code>
+since this now exists in
+<a href=\"modelica://AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor\">AixLib.Fluid.Sensors.BaseClasses.PartialDynamicFlowSensor</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">#372</a>.
+</li>
+<li>
+August 31, 2013, by Michael Wetter:<br/>
+Removed default value <code>tau=0</code> as the base class
+already sets <code>tau=1</code>.
+This change was made so that all sensors use the same default value.
+</li>
+<li>
+June 3, 2011 by Michael Wetter:<br/>
+Revised implementation to add dynamics in such a way that
+the time constant increases as the mass flow rate tends to zero.
+This significantly improves the numerics.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+Implementation is based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VolumeFlowRate;
diff --git a/AixLib/Fluid/Sensors/package.order b/AixLib/Fluid/Sensors/package.order
index 1dda995259..ed40f550b7 100644
--- a/AixLib/Fluid/Sensors/package.order
+++ b/AixLib/Fluid/Sensors/package.order
@@ -3,6 +3,7 @@ Density
 DensityTwoPort
 EnthalpyFlowRate
 EntropyFlowRate
+HeatMeter
 LatentEnthalpyFlowRate
 MassFlowRate
 MassFraction
diff --git a/AixLib/Fluid/Solar/Thermal/SolarThermal.mo b/AixLib/Fluid/Solar/Thermal/SolarThermal.mo
index b7e970049b..ffd7328557 100644
--- a/AixLib/Fluid/Solar/Thermal/SolarThermal.mo
+++ b/AixLib/Fluid/Solar/Thermal/SolarThermal.mo
@@ -3,7 +3,7 @@ model SolarThermal "Model of a solar thermal panel"
   extends AixLib.Fluid.BoilerCHP.BaseClasses.PartialHeatGenerator(
     vol(final V=volPip),
     a=pressureDropCoeff,
-    dp_start=pressureDropCoeff*(m_flow_start *
+    dp_start=pressureDropCoeff*(m_flow_start /
       Medium.density(Medium.setState_pTX(
                        p_start,
                        T_start,
diff --git a/AixLib/Fluid/SolarCollectors/ASHRAE93.mo b/AixLib/Fluid/SolarCollectors/ASHRAE93.mo
new file mode 100644
index 0000000000..592efa134b
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/ASHRAE93.mo
@@ -0,0 +1,210 @@
+within AixLib.Fluid.SolarCollectors;
+model ASHRAE93 "Model of a solar thermal collector according to the ASHRAE Standard 93"
+  extends AixLib.Fluid.SolarCollectors.BaseClasses.PartialSolarCollector(
+    redeclare AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 per);
+
+  BaseClasses.ASHRAESolarGain solGai(
+    redeclare package Medium = Medium,
+    final nSeg=nSeg,
+    final til=til,
+    final incAngDat=per.incAngDat,
+    final incAngModDat=per.incAngModDat,
+    final y_intercept=per.y_intercept,
+    final use_shaCoe_in=use_shaCoe_in,
+    final shaCoe=shaCoe,
+    final A_c=ATot_internal)
+    "Identifies heat gained from the sun using the ASHRAE Standard 93 calculations"
+             annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+
+  BaseClasses.ASHRAEHeatLoss heaLos(
+    redeclare package Medium = Medium,
+    final nSeg=nSeg,
+    final slope=per.slope,
+    final A_c=ATot_internal)
+    "Calculates the heat lost to the surroundings using the ASHRAE Standard 93 calculations"
+        annotation (Placement(transformation(extent={{-20,10},{0,30}})));
+
+equation
+  // Make sure the model is only used with the ASHRAE ratings data, and slope < 0
+  assert(per.slope < 0,
+    "In " + getInstanceName() + ": The heat loss coefficient from the ASHRAE ratings data must be strictly negative. Obtained slope = " + String(per.slope));
+
+  connect(weaBus.TDryBul, heaLos.TEnv) annotation (Line(
+      points={{-99.95,80.05},{-90,80.05},{-90,26},{-22,26}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None), Text(
+      textString="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}}));
+  connect(HDirTil.inc, solGai.incAng)    annotation (Line(
+      points={{-59,46},{-50,46},{-50,48},{-22,48}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HDirTil.H, solGai.HDirTil)    annotation (Line(
+      points={{-59,50},{-50,50},{-50,52},{-22,52}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HDifTilIso.HGroDifTil, solGai.HGroDifTil) annotation (Line(
+      points={{-59,74},{-40,74},{-40,55},{-22,55}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HDifTilIso.HSkyDifTil, solGai.HSkyDifTil) annotation (Line(
+      points={{-59,86},{-30,86},{-30,58},{-22,58}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(shaCoe_in, solGai.shaCoe_in) annotation (Line(
+      points={{-120,40},{-40,40},{-40,45},{-22,45}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(solGai.QSol_flow, QGai.Q_flow) annotation (Line(
+      points={{1,50},{50,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(temSen.T, heaLos.TFlu) annotation (Line(
+      points={{-11,-20},{-30,-20},{-30,14},{-22,14}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(temSen.T, solGai.TFlu) annotation (Line(
+      points={{-11,-20},{-30,-20},{-30,42},{-22,42}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(heaLos.QLos_flow, QLos.Q_flow) annotation (Line(
+      points={{1,20},{50,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+annotation (
+    Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
+            100}}),
+         graphics={
+        Rectangle(
+          extent={{-84,100},{84,-100}},
+          lineColor={27,0,55},
+          fillColor={26,0,55},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-100,0},{-76,0},{-76,-90},{66,-90},{66,-60},{-64,-60},{-64,
+              -30},{66,-30},{66,0},{-64,0},{-64,28},{66,28},{66,60},{-64,60},{
+              -64,86},{78,86},{78,0},{98,0},{100,0}},
+          color={0,128,255},
+          thickness=1,
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-24,26},{28,-26}},
+          lineColor={255,255,0},
+          fillColor={255,255,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-6,-6},{8,8}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={-24,30},
+          rotation=90),
+        Line(
+          points={{-50,0},{-30,0}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1),
+        Line(
+          points={{-36,-40},{-20,-24}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1),
+        Line(
+          points={{-10,0},{10,0}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={2,-40},
+          rotation=90),
+        Line(
+          points={{-8,-8},{6,6}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={30,-30},
+          rotation=90),
+        Line(
+          points={{32,0},{52,0}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1),
+        Line(
+          points={{-8,-8},{6,6}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={28,32},
+          rotation=180),
+        Line(
+          points={{-10,0},{10,0}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={0,40},
+          rotation=90)}),
+  defaultComponentName="solCol",
+  Documentation(info="<html>
+<p>
+This component models a solar thermal collector according to the ASHRAE93
+test standard.
+</p>
+
+<h4>References</h4>
+<p>
+ASHRAE 93-2010 -- Methods of Testing to Determine the Thermal Performance of
+Solar Collectors (ANSI approved).
+</p>
+<p>
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v23.2.0/EngineeringReference.pdf\">
+EnergyPlus 23.2.0 Engineering Reference</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 28, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+December 11, 2023, by Michael Wetter:<br/>
+Corrected implementation of pressure drop calculation for the situation where the collectors are in parallel,
+e.g., if <code>sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Parallel</code>.<br/>
+Changed assignment of <code>computeFlowResistance</code> to <code>final</code> based on
+<code>dp_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3597\">Buildings, #3597</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+December 17, 2017, by Michael Wetter:<br/>
+Revised computation of heat loss.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1100\">
+issue 1100</a>.
+</li>
+<li>
+November 21, 2017, by Michael Wetter:<br/>
+Corrected error in heat loss calculations that did not scale correctly with <code>nPanels</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1073\">issue 1073</a>.
+</li>
+<li>
+October 18, 2013, by Michael Wetter:<br/>
+Removed duplicate connection.
+</li>
+<li>
+January 4, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ASHRAE93;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/ASHRAEHeatLoss.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/ASHRAEHeatLoss.mo
new file mode 100644
index 0000000000..c61e720641
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/ASHRAEHeatLoss.mo
@@ -0,0 +1,88 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+block ASHRAEHeatLoss
+  "Calculate the heat loss of a solar collector per ASHRAE standard 93"
+  extends AixLib.Fluid.SolarCollectors.BaseClasses.PartialHeatLoss(
+    QLos_internal = -slope * A_c/nSeg * {dT[i] for i in 1:nSeg});
+
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer slope(final max=0)
+    "Slope from ratings data";
+
+annotation (
+defaultComponentName="heaLos",
+Documentation(info="<html>
+<p>
+This component computes the heat loss from the solar thermal collector to the
+environment.
+It is designed for use with ratings data collected in accordance with
+ASHRAE Standard 93.
+A negative heat loss indicates that heat is being lost to the environment.
+</p>
+
+<h4> Model description </h4>
+<p>
+This model calculates the heat loss to the ambient, for each segment
+<i>i &isin; {1, ..., n<sub>seg</sub>}</i> where <i>n<sub>seg</sub></i> is
+the number of segments, as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>los,i</sub> = -slope A<sub>c</sub> &frasl; n<sub>seg</sub>
+  (T<sub>env</sub>-T<sub>flu,i</sub>)
+</p>
+<p>
+where
+<i>slope &lt; 0</i> is the slope for the heat loss as specified in the ratings
+data, <i>A<sub>c</sub></i> is the collector area, <i>T<sub>env</sub></i> is
+the environment temperature, and <i>T<sub>flu,i</sub></i> is the
+fluid temperature in segment <i>i &isin; {1, ..., n<sub>seg</sub>}</i>.
+</p>
+<p>
+This model reduces the heat loss rate to <i>0</i> when the fluid temperature
+is within <i>1</i> Kelvin of the minimum temperature of the medium model.
+The calculation is performed using the
+<a href=\"modelica://AixLib.Utilities.Math.Functions.smoothHeaviside\">
+AixLib.Utilities.Math.Functions.smoothHeaviside</a> function.
+</p>
+
+<h4>Implementation</h4>
+<p>
+ASHRAE uses the collector fluid inlet temperature to compute the heat loss
+(see Duffie and Beckmann, p. 293).
+However, unless the environment temperature which was present during the
+collector rating is known, which is not the case, one cannot compute a
+log mean temperature difference that would improve the <i>UA</i> calculation.
+Hence, this model is using the fluid temperature of each segment
+to compute the heat loss to the environment.
+</p>
+
+<h4>References</h4>
+<p>
+ASHRAE 93-2010 -- Methods of Testing to Determine the Thermal Performance of Solar
+Collectors (ANSI approved).
+</p>
+<p>
+J.A. Duffie and W.A. Beckman 2006, Solar Engineering of Thermal Processes (3rd Edition),
+John Wiley &amp; Sons, Inc.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+December 17, 2017, by Michael Wetter:<br/>
+Revised computation of heat loss.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1100\">
+issue 1100</a>.
+</li>
+<li>
+Jan 16, 2012, by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ASHRAEHeatLoss;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/ASHRAESolarGain.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/ASHRAESolarGain.mo
new file mode 100644
index 0000000000..0b73f5fadf
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/ASHRAESolarGain.mo
@@ -0,0 +1,290 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+block ASHRAESolarGain
+  "Calculate the solar heat gain of a solar collector per ASHRAE Standard 93"
+  extends Modelica.Blocks.Icons.Block;
+  extends SolarCollectors.BaseClasses.PartialParameters;
+
+  replaceable package Medium = Modelica.Media.Interfaces.PartialMedium
+    "Medium in the system";
+
+  parameter Real y_intercept(final unit="1") "y intercept(maximum efficiency)";
+  parameter Modelica.Units.SI.Angle[:] incAngDat "Incidence angle modifier spline derivative coefficients";
+  parameter Real[size(incAngDat,1)] incAngModDat(
+    each final unit="1") "Incidence angle modifier spline derivative coefficients";
+  parameter Boolean use_shaCoe_in = false "Enable input connector for shaCoe"
+    annotation(Dialog(group="Shading"));
+
+  parameter Real shaCoe(
+    min=0.0,
+    max=1.0) = 0 "Shading coefficient 0.0: no shading, 1.0: full shading"
+    annotation(Dialog(enable = not use_shaCoe_in, group = "Shading"));
+
+  parameter Modelica.Units.SI.Angle til "Surface tilt";
+
+  Modelica.Blocks.Interfaces.RealInput shaCoe_in if use_shaCoe_in
+    "Shading coefficient"
+    annotation(Placement(transformation(extent={{-140,-70},{-100,-30}})));
+   Modelica.Blocks.Interfaces.RealInput TFlu[nSeg](
+   each unit = "K",
+   each displayUnit="degC",
+   each quantity="ThermodynamicTemperature")
+   annotation (Placement(transformation(extent={{-140,-100},{-100,-60}})));
+   Modelica.Blocks.Interfaces.RealInput HSkyDifTil(
+     unit="W/m2", quantity="RadiantEnergyFluenceRate")
+    "Diffuse solar irradiation on a tilted surfce from the sky"
+     annotation (Placement(transformation(extent={{-140,60},{-100,100}})));
+  Modelica.Blocks.Interfaces.RealInput HGroDifTil(
+    unit="W/m2", quantity="RadiantEnergyFluenceRate")
+    "Diffuse solar irradiation on a tilted surfce from the ground"
+    annotation (Placement(transformation(extent={{-140,30},{-100,70}})));
+  Modelica.Blocks.Interfaces.RealInput incAng(
+    quantity="Angle",
+    unit="rad",
+    displayUnit="deg") "Incidence angle of the sun beam on a tilted surface"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+  Modelica.Blocks.Interfaces.RealInput HDirTil(
+    unit="W/m2", quantity="RadiantEnergyFluenceRate")
+    "Direct solar irradiation on a tilted surfce"
+    annotation (Placement(transformation(extent={{-140,0},{-100,40}})));
+  Modelica.Blocks.Interfaces.RealOutput QSol_flow[nSeg](each final unit="W")
+    "Solar heat gain"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+
+protected
+  constant Modelica.Units.SI.TemperatureDifference dTMax=1
+    "Safety temperature difference to prevent TFlu > Medium.T_max";
+  final parameter Modelica.Units.SI.Temperature TMedMax=Medium.T_max - dTMax
+    "Fluid temperature above which there will be no heat gain computed to prevent TFlu > Medium.T_max";
+  final parameter Modelica.Units.SI.Temperature TMedMax2=TMedMax - dTMax
+    "Fluid temperature above which there will be no heat gain computed to prevent TFlu > Medium.T_max";
+
+  final parameter Real iamSky(fixed=false)
+    "Incident angle modifier for diffuse solar radiation from the sky";
+  final parameter Real iamGro(fixed=false)
+    "Incident angle modifier for diffuse solar radiation from the ground";
+  final parameter Modelica.Units.SI.Angle incAngSky(fixed=false)
+    "Incident angle of diffuse radiation from the sky";
+  final parameter Modelica.Units.SI.Angle incAngGro(fixed=false)
+    "Incident angle of diffuse radiation from the ground";
+  final parameter Real tilDeg(
+    unit = "deg") = Modelica.Units.Conversions.to_deg(til)
+    "Surface tilt angle in degrees";
+  final parameter Modelica.Units.SI.HeatFlux HTotMin=1
+    "Minimum HTot to avoid div/0";
+  final parameter Real HMinDel = 0.001
+    "Delta of the smoothing function for HTot";
+
+  Real iamBea "Incident angle modifier for direct solar radiation";
+  Real iam "Weighted incident angle modifier";
+
+  Modelica.Blocks.Interfaces.RealInput shaCoe_internal
+    "Internally used shading coefficient";
+
+  parameter Real[size(incAngDat, 1)] dMonotone(each fixed=false) "Derivatives";
+
+initial algorithm
+  dMonotone := AixLib.Utilities.Math.Functions.splineDerivatives(
+    x=incAngDat,
+    y=incAngModDat,
+    ensureMonotonicity=false);
+
+initial equation
+  // EnergyPlus 23.2.0 Engineering Reference Eq 18.300
+  incAngSky =Modelica.Units.Conversions.from_deg(59.68 - 0.1388*(tilDeg) +
+    0.001497*(tilDeg)^2);
+  // Diffuse radiation from the sky
+  // EnergyPlus 23.2.0 Engineering Reference Eq 18.298
+  iamSky = SolarCollectors.BaseClasses.IAM(incAngSky, incAngDat, incAngModDat, dMonotone);
+  // EnergyPlus 23.2.0 Engineering Reference Eq 18.301
+  incAngGro =Modelica.Units.Conversions.from_deg(90 - 0.5788*(tilDeg) +
+    0.002693*(tilDeg)^2);
+  // Diffuse radiation from the ground
+  // EnergyPlus 23.2.0 Engineering Reference Eq 18.298
+  iamGro = SolarCollectors.BaseClasses.IAM(incAngGro, incAngDat, incAngModDat, dMonotone);
+
+equation
+
+  connect(shaCoe_internal, shaCoe_in);
+
+  if not use_shaCoe_in then
+    shaCoe_internal = shaCoe;
+  end if;
+
+  // EnergyPlus 23.2.0 Engineering Reference Eq 18.298
+  iamBea = SolarCollectors.BaseClasses.IAM(incAng, incAngDat, incAngModDat, dMonotone);
+  // EnergyPlus 23.2.0 Engineering Reference Eq 18.299
+  iam = (HDirTil*iamBea + HSkyDifTil*iamSky + HGroDifTil*iamGro)/
+      AixLib.Utilities.Math.Functions.smoothMax((
+        HDirTil + HSkyDifTil + HGroDifTil), HTotMin, HMinDel);
+  // Modified from EnergyPlus 23.2.0 Engineering Reference Eq 18.302
+  // by applying shade effect for direct solar radiation
+  // Only solar heat gain is considered here
+  for i in 1 : nSeg loop
+    QSol_flow[i] = A_c/nSeg*(y_intercept*iam*
+      (HDirTil*(1.0 - shaCoe_internal) + HSkyDifTil + HGroDifTil))*
+      smooth(1, if TFlu[i] < TMedMax2
+        then 1
+        else AixLib.Utilities.Math.Functions.smoothHeaviside(TMedMax-TFlu[i], dTMax));
+  end for;
+
+  annotation (
+    defaultComponentName="solGai",
+    Documentation(info="<html>
+<p>
+This component computes the solar heat gain of the solar thermal collector.
+It only calculates the solar heat gain without considering the heat loss
+to the environment.
+This model uses ratings data according to ASHRAE93.
+The solar heat gain is calculated using Equations 18.298-18.302 in the
+referenced EnergyPlus documentation.
+</p>
+<p>
+The solar radiation absorbed by the panel is identified using Eq 18.302 from
+the EnergyPlus documentation. It is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>flow</sub>[i]=A<sub>c</sub>/nSeg (F<sub>R</sub>(&tau;&alpha;)
+  K<sub>(&tau;&alpha;)<sub>net</sub></sub> (G<sub>dir</sub>
+  (1-shaCoe)+G<sub>dif</sub>+G<sub>gnd</sub>))
+</p>
+<p>
+where <i>Q<sub>flow</sub>[i]</i> is the heat gain in each segment,
+<i>A<sub>c</sub></i> is the area of the collector,
+<i>nSeg</i> is the user-specified number of segments in the simulation,
+<i>F<sub>R</sub>(&tau;&alpha;)</i> is the maximum collector efficiency,
+<i>K<sub>(&tau;&alpha;)<sub>net</sub></sub></i> is the incidence angle modifier,
+<i>G<sub>dir</sub></i> is the direct solar radiation,
+<i>shaCoe</i> is the user-specified shading coefficient,
+<i>G<sub>sky</sub></i> is the diffuse solar radiation from the sky,
+and <i>G<sub>gnd</sub></i> is the diffuse radiation from the ground.
+</p>
+<p>
+The solar radiation equation indicates that the collector is divided into
+multiple segments.
+The number of segments used in the simulation is specified by the user via <code>nSeg</code>.
+The area of an individual segment is identified by dividing the collector area
+by the total number of segments.
+The term <code>shaCoe</code> is used to define the percentage of the collector
+that is shaded.
+</p>
+<p>
+The incidence angle modifier used in the solar radiation equation is found using
+Eq 18.299 from the EnergyPlus documentation. It is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+K<sub>(&tau;&alpha;),net</sub>=(G<sub>dir</sub> K<sub>(&tau;&alpha;),dir</sub>
+  +G<sub>sky</sub> K<sub>(&tau;&alpha;),sky</sub>
+  +G<sub>gnd</sub> K<sub>(&tau;&alpha;),gnd</sub>)
+  /(G<sub>dir</sub>+G<sub>sky</sub>+G<sub>gnd</sub>)
+</p>
+<p>
+where <i>K<sub>(&tau;&alpha;),net</sub></i> is the net incidence angle modified,
+<i>G<sub>dir</sub></i> is the (direct) beam radiation,
+<i>K<sub>(&tau;&alpha;),dir</sub></i> is the incidence angle modifier
+for (direct) beam radiation,
+<i>G<sub>sky</sub></i> is the diffuse radiation from the sky,
+<i>K<sub>(&tau;&alpha;),sky</sub></i> is the incidence angle modifier
+for radiation from the sky,
+<i>G<sub>gnd</sub></i> is the diffuse radiation from the ground,
+and <i>K<sub>(&tau;&alpha;),gnd</sub></i> is the incidence angle modifier
+for diffuse radiation from the ground.
+</p>
+<p>
+Each incidence angle modifier is calculated using Eq 18.298 from the EnergyPlus
+documentation. It is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+K<sub>(&tau;&alpha;),x</sub>=1+b<sub>0</sub> (1/cos(&theta;)-1)+b<sub>1</sub>
+  (1/cos(&theta;)-1)<sup>2</sup>
+</p>
+<p>
+where x can refer to beam, sky or ground.
+<i>&theta;</i> is the incidence angle.
+For beam radiation <i>&theta;</i> is found via standard geometry.
+The incidence angle for sky and ground diffuse radiation are found using,
+respectively, Eq 18.300 and 18.301 from the EnergyPlus documentation.
+They are
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&theta;<sub>sky</sub>=59.68-0.1388 til+0.001497 til<sup>2</sup><br/>
+&theta;<sub>gnd</sub>=90.0-0.5788 til+0.002693 til<sup>2</sup>
+</p>
+<p>
+where <i>&theta;<sub>sky</sub></i> is the incidence angle
+for diffuse radiation from the sky,
+<i>til</i> is the tilt of the solar thermal collector,
+and <i>&theta;<sub>gnd</sub></i> is the incidence angle
+for diffuse radiation from the ground.
+</p>
+<p>
+These two equations must be evaluated in degrees.
+The necessary unit conversions are made internally.
+</p>
+<p>
+This model reduces the heat gain rate to 0 W when the fluid temperature is
+within 1 degree C of the maximum temperature of the medium model.
+The calculation is performed using the
+<a href=\"modelica://AixLib.Utilities.Math.Functions.smoothHeaviside\">
+AixLib.Utilities.Math.Functions.smoothHeaviside</a> function.
+</p>
+
+<h4>References</h4>
+<p>
+ASHRAE 93-2010 -- Methods of Testing to Determine the Thermal Performance of Solar
+Collectors (ANSI approved).
+</p>
+<p>
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v23.2.0/EngineeringReference.pdf\">
+EnergyPlus 23.2.0 Engineering Reference</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 28, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+April 27, 2018, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">Buildings, issue 912</a>.
+</li>
+<li>
+May 31, 2017, by Michael Wetter and Filip Jorissen:<br/>
+Change limits for incident angle modifier to avoid dip in temperature
+at shallow incidence angles.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/785\">issue 785</a>.
+</li>
+<li>
+September 17, 2016, by Michael Wetter:<br/>
+Corrected quantity from <code>Temperature</code> to <code>ThermodynamicTemperature</code>
+to avoid an error in the pedantic model check in Dymola 2017 FD01 beta2.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/557\">issue 557</a>.
+</li>
+<li>
+June 29, 2015, by Michael Wetter:<br/>
+Revised implementation of heat loss near <code>Medium.T_max</code>
+to make it more efficient.
+</li>
+<li>
+June 29, 2015, by Filip Jorissen:<br/>
+Fixed sign mistake causing model to fail under high
+solar irradiation because temperature goes above medium
+temperature bound.
+</li>
+<li>
+November 20, 2014, by Michael Wetter:<br/>
+Added missing <code>each</code> keyword.
+</li>
+<li>
+Jan 15, 2013, by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end ASHRAESolarGain;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/EN12975HeatLoss.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/EN12975HeatLoss.mo
new file mode 100644
index 0000000000..ffce68b0ec
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/EN12975HeatLoss.mo
@@ -0,0 +1,89 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+block EN12975HeatLoss "Calculate the heat loss of a solar collector per EN12975"
+  extends AixLib.Fluid.SolarCollectors.BaseClasses.PartialHeatLoss(
+    QLos_internal = A_c/nSeg * {dT[i] * (a1 - a2 * dT[i]) for i in 1:nSeg});
+
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer a1(final min=0)
+    "a1 from ratings data";
+
+  parameter Real a2(final unit = "W/(m2.K2)", final min=0)
+    "a2 from ratings data";
+
+annotation (
+defaultComponentName="heaLos",
+Documentation(info="<html>
+<p>
+This component computes the heat loss from the solar thermal collector
+to the environment. It is designed anticipating ratings data collected in
+accordance with EN12975. A negative heat loss indicates that heat
+is being lost to the environment.
+</p>
+<p>
+This model calculates the heat loss to the ambient, for each
+segment <i>i &isin; {1, ..., n<sub>seg</sub>}</i>
+where <i>n<sub>seg</sub></i> is the number of segments, as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>los,i</sub> = A<sub>c</sub> &frasl; n<sub>seg</sub>
+(T<sub>env</sub>-T<sub>flu,i</sub>) (a<sub>1</sub> - a<sub>2</sub>
+  (T<sub>env</sub>-T<sub>flu,i</sub>))
+</p>
+<p>
+where
+<i>a<sub>1</sub> &gt; 0</i> is the heat loss coefficient
+from EN12975 ratings data,
+<i>a<sub>2</sub> &ge; 0</i> is the temperature dependence of heat loss
+from EN12975 ratings data,
+<i>A<sub>c</sub></i> is the collector area,
+<i>T<sub>env</sub></i> is the environment temperature and
+<i>T<sub>flu,i</sub></i> is the fluid temperature in segment
+<i>i &isin; {1, ..., n<sub>seg</sub>}</i>.
+</p>
+<p>
+This model reduces the heat loss rate to <i>0</i> when the fluid temperature is within
+<i>1</i> Kelvin of the minimum temperature of the medium model. The calculation is
+performed using the
+<a href=\"modelica://AixLib.Utilities.Math.Functions.smoothHeaviside\">
+AixLib.Utilities.Math.Functions.smoothHeaviside</a> function.
+</p>
+<h4>Implementation</h4>
+<p>
+EN 12975 uses the arithmetic average temperature of the collector fluid inlet
+and outlet temperature to compute the heat loss (see Duffie and Beckmann, p. 293).
+However, unless the environment temperature that was present during the collector rating
+is known, which is not the case, one cannot compute
+a log mean temperature difference that would improve the <i>UA</i> calculation. Hence,
+this model is using the fluid temperature of each segment
+to compute the heat loss to the environment.
+If the arithmetic average temperature were used, then segments at the collector
+outlet could be cooled below the ambient temperature, which violates the 2nd law
+of Thermodynamics.
+</p>
+
+<h4>References</h4>
+<p>
+CEN 2006, European Standard 12975-1:2006, European Committee for Standardization
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+December 17, 2017, by Michael Wetter:<br/>
+Revised computation of heat loss.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1100\">
+issue 1100</a>.
+</li>
+<li>
+Jan 16, 2012, by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end EN12975HeatLoss;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/EN12975SolarGain.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/EN12975SolarGain.mo
new file mode 100644
index 0000000000..d3e26ee268
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/EN12975SolarGain.mo
@@ -0,0 +1,219 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+model EN12975SolarGain "Model calculating solar gains per the EN12975 standard"
+  extends Modelica.Blocks.Icons.Block;
+  extends SolarCollectors.BaseClasses.PartialParameters;
+
+  replaceable package Medium = Modelica.Media.Interfaces.PartialMedium
+    "Medium in the system";
+
+  parameter Real eta0(final unit="1") "Optical efficiency (maximum efficiency)";
+  parameter Modelica.Units.SI.Angle[:] incAngDat "Incidence angle modifier spline derivative coefficients";
+  parameter Real[size(incAngDat,1)] incAngModDat(each final unit="1") "Incidence angle modifier spline derivative coefficients";
+  parameter Boolean use_shaCoe_in = false
+    "Enables an input connector for shaCoe"
+    annotation(Dialog(group="Shading"));
+  parameter Real shaCoe(
+    min=0.0,
+    max=1.0) = 0 "Shading coefficient 0.0: no shading, 1.0: full shading"
+    annotation(Dialog(enable = not use_shaCoe_in,group="Shading"));
+
+  parameter Real iamDiff "Incidence angle modifier for diffuse radiation";
+
+  Modelica.Blocks.Interfaces.RealInput shaCoe_in if use_shaCoe_in
+    "Time varying input for the shading coefficient"
+    annotation(Placement(transformation(extent={{-140,-70},{-100,-30}})));
+
+  Modelica.Blocks.Interfaces.RealInput HSkyDifTil(
+    unit="W/m2",
+    quantity="RadiantEnergyFluenceRate")
+    "Diffuse solar irradiation on a tilted surfce from the sky"
+    annotation (Placement(transformation(extent={{-140,60},{-100,100}})));
+  Modelica.Blocks.Interfaces.RealInput incAng(
+    quantity="Angle",
+    unit="rad",
+    displayUnit="deg") "Incidence angle of the sun beam on a tilted surface"
+    annotation (Placement(transformation(extent={{-140,-40},{-100,0}})));
+  Modelica.Blocks.Interfaces.RealInput HDirTil(
+    unit="W/m2",
+    quantity="RadiantEnergyFluenceRate")
+    "Direct solar irradiation on a tilted surfce"
+    annotation (Placement(transformation(extent={{-140,0},{-100,40}})));
+  Modelica.Blocks.Interfaces.RealOutput QSol_flow[nSeg](each final unit="W")
+    "Solar heat gain"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  Modelica.Blocks.Interfaces.RealInput TFlu[nSeg](
+     each final unit="K",
+     each displayUnit="degC",
+     each final quantity="ThermodynamicTemperature")
+    annotation (Placement(transformation(extent={{-140,-100},{-100,-60}})));
+
+protected
+  constant Modelica.Units.SI.TemperatureDifference dTMax=1
+    "Safety temperature difference to prevent TFlu > Medium.T_max";
+  final parameter Modelica.Units.SI.Temperature TMedMax=Medium.T_max - dTMax
+    "Fluid temperature above which there will be no heat gain computed to prevent TFlu > Medium.T_max";
+  final parameter Modelica.Units.SI.Temperature TMedMax2=TMedMax - dTMax
+    "Fluid temperature above which there will be no heat gain computed to prevent TFlu > Medium.T_max";
+  Real iamBea "Incidence angle modifier for director solar radiation";
+  Modelica.Blocks.Interfaces.RealInput shaCoe_internal "Internally used shaCoe";
+
+  parameter Real[size(incAngDat, 1)] dMonotone(each fixed=false) "Derivatives";
+
+initial algorithm
+  dMonotone := AixLib.Utilities.Math.Functions.splineDerivatives(
+    x=incAngDat,
+    y=incAngModDat,
+    ensureMonotonicity=false);
+
+equation
+  connect(shaCoe_internal, shaCoe_in);
+
+  if not use_shaCoe_in then
+    shaCoe_internal = shaCoe;
+  end if;
+
+  // EnergyPlus 23.2.0 Engineering Reference Eq 18.298
+  iamBea = SolarCollectors.BaseClasses.IAM(incAng, incAngDat, incAngModDat, dMonotone);
+  // Modified from EnergyPlus 23.2.0 Engineering Reference Eq 18.302
+  // by applying shade effect for direct solar radiation
+  // Only solar heat gain is considered here
+  for i in 1 : nSeg loop
+  QSol_flow[i] = A_c/nSeg*(eta0*(iamBea*HDirTil*(1.0 - shaCoe_internal) + iamDiff *
+  HSkyDifTil))*
+      smooth(1, if TFlu[i] < TMedMax2
+        then 1
+        else AixLib.Utilities.Math.Functions.smoothHeaviside(TMedMax-TFlu[i], dTMax));
+  end for;
+  annotation (
+    defaultComponentName="solGai",
+    Documentation(info="<html>
+<p>
+This component computes the solar heat gain of the solar thermal collector.
+It only calculates the solar heat gain without considering the heat loss
+to the environment.
+This model uses ratings data according to EN12975.
+The solar heat gain is calculated using Equations 18.298 and 18.302 in the
+referenced EnergyPlus documentation.
+The calculation is modified to use coefficients from EN12975.
+</p>
+<p>
+The equation used to calculate solar gain is a modified version of Eq 18.302
+from the EnergyPlus documentation.
+It is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+Q<sub>flow</sub>[i] = A<sub>c</sub>/nSeg &eta;<sub>0</sub> (K<sub>
+(&tau;&alpha;),dir</sub> G<sub>dir</sub> (1-shaCoe)+K<sub>dif</sub> G<sub>
+dif</sub>),
+</p>
+<p>
+where <i>Q<sub>flow</sub>[i]</i> is the heat gained in each segment,
+<i>A<sub>c</sub></i> is the area of the collector,
+<code>nSeg</code> is the number of segments in the collector,
+<i>&eta;<sub>0</sub></i> is the maximum efficiency of the collector,
+<i>K<sub>(&tau;&alpha;),dir</sub> </i>is the incidence angle modifier
+for (direct) beam radiation,
+<i>G<sub>dir</sub></i> is the current beam radiation on the collector,
+<code>shaCoe</code> is the shading coefficient,
+<i>K<sub>dif</sub></i> is the incidence angle modifier
+for diffuse radiation,
+and <i>G<sub>dif</sub></i> is the diffuse radiation striking the surface.
+</p>
+<p>
+The solar radiation equation indicates that the collector is divided into
+multiple segments.
+The number of segments used in the simulation is specified by the user via <code>nSeg</code>.
+The area of an individual segment is identified by dividing the collector area
+by the total number of segments.
+The term <code>shaCoe</code> is used to define the percentage of the collector
+that is shaded.
+</p>
+<p>
+The main difference between this model and the ASHRAE model is the handling of
+diffuse radiation.
+The ASHRAE model contains calculated incidence angle modifiers for
+both sky and ground diffuse radiation,
+while this model uses a coefficient from test data for diffuse radiation.
+</p>
+<p>
+The incidence angle modifier is calculated using Eq 18.298 from the EnergyPlus
+documentation. It is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+K<sub>(&tau;&alpha;),x</sub>=1+b<sub>0</sub> (1/cos(&theta;)-1)+b<sub>1</sub>
+  (1/cos(&theta;)-1)<sup>2</sup>
+</p>
+<p>
+where <i>K<sub>(&tau;&alpha;),dir</sub></i> is the incidence angle modifier
+for beam radiation,
+<i>b<sub>0</sub></i> is the first incidence angle modifier coefficient,
+<i>b<sub>1</sub></i> is the second incidence angle modifier coefficient,
+and <i>&theta;</i> is the incidence angle.
+</p>
+<p>
+This model reduces the heat gain rate to 0 W when the fluid temperature is
+within 1 degree C of the maximum temperature of the medium model.
+The calculation is performed using the
+<a href=\"modelica://AixLib.Utilities.Math.Functions.smoothHeaviside\">
+AixLib.Utilities.Math.Functions.smoothHeaviside</a> function.
+</p>
+
+<h4>References</h4>
+<p>
+CEN 2022, European Standard 12975:2022, European Committee for Standardization
+</p>
+<p>
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v23.2.0/EngineeringReference.pdf\">
+EnergyPlus 23.2.0 Engineering Reference</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 28, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+January 12, 2019, by Michael Wetter:<br/>
+Added missing <code>each</code>.
+</li>
+<li>
+April 27, 2018, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">Buildings, issue 912</a>.
+</li>
+<li>
+May 31, 2017, by Michael Wetter and Filip Jorissen:<br/>
+Change limits for incident angle modifier to avoid dip in temperature
+at shallow incidence angles.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/785\">issue 785</a>.
+</li>
+<li>
+September 17, 2016, by Michael Wetter:<br/>
+Corrected quantity from <code>Temperature</code> to <code>ThermodynamicTemperature</code>
+to avoid an error in the pedantic model check in Dymola 2017 FD01 beta2.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/557\">issue 557</a>.
+</li>
+<li>
+June 29, 2015, by Michael Wetter:<br/>
+Revised implementation of heat loss near <code>Medium.T_max</code>
+to make it more efficient.
+</li>
+<li>
+June 29, 2015, by Filip Jorissen:<br/>
+Fixed sign mistake causing model to fail under high
+solar irradiation because temperature goes above
+medium temperature bound.
+</li>
+<li>
+Jan 15, 2013, by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end EN12975SolarGain;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAEHeatLoss.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAEHeatLoss.mo
new file mode 100644
index 0000000000..700f7c3f52
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAEHeatLoss.mo
@@ -0,0 +1,74 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses.Examples;
+model ASHRAEHeatLoss "Example showing the use of ASHRAEHeatLoss"
+  extends Modelica.Icons.Example;
+  parameter AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 per=
+    AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_SolahartKf()
+    "Performance data"
+    annotation (choicesAllMatching=true);
+  Modelica.Blocks.Sources.Sine TEnv(
+    f=0.01,
+    offset=273.15 + 10,
+    amplitude=7.5) "Temperature of the surrounding environment"
+    annotation (Placement(transformation(extent={{30,70},{50,90}})));
+  Modelica.Blocks.Sources.Sine T1(
+    amplitude=15,
+    f=0.1,
+    offset=273.15 + 10) "Temperature of the first segment"
+    annotation (Placement(transformation(extent={{30,-90},{50,-70}})));
+  Modelica.Blocks.Sources.Sine T2(
+    f=0.1,
+    amplitude=15,
+    offset=273.15 + 15) "Temperature of the second segment"
+    annotation (Placement(transformation(extent={{-10,-70},{10,-50}})));
+  Modelica.Blocks.Sources.Sine T3(
+    f=0.1,
+    amplitude=15,
+    offset=273.15 + 20) "Temperature of the third segment"
+    annotation (Placement(transformation(extent={{-50,-50},{-30,-30}})));
+  AixLib.Fluid.SolarCollectors.BaseClasses.ASHRAEHeatLoss  heaLos(
+    nSeg=3,
+    redeclare package Medium = AixLib.Media.Water,
+    A_c=per.A,
+    slope=per.slope) "Heat loss model using EN12975 calculations"
+    annotation (Placement(transformation(extent={{70,-10},{90,10}})));
+equation
+  connect(TEnv.y, heaLos.TEnv) annotation (Line(
+      points={{51,80},{60,80},{60,6},{68,6}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T3.y, heaLos.TFlu[3]) annotation (Line(
+      points={{-29,-40},{-20,-40},{-20,-6},{68,-6},{68,-5.33333}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T2.y, heaLos.TFlu[2]) annotation (Line(
+      points={{11,-60},{20,-60},{20,-6},{68,-6}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T1.y, heaLos.TFlu[1]) annotation (Line(
+      points={{51,-80},{60,-80},{60,-6.66667},{68,-6.66667}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (
+    Documentation(info="<html>
+<p>
+This examples demonstrates the implementation of
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.BaseClasses.ASHRAEHeatLoss\">
+AixLib.Fluid.SolarCollectors.BaseClasses.ASHRAEHeatLoss</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+</ul>
+  </html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAEHeatLoss.mos"
+        "Simulate and plot"),
+        experiment(Tolerance=1e-6, StopTime=100), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ASHRAEHeatLoss;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAESolarGain.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAESolarGain.mo
new file mode 100644
index 0000000000..12fee03141
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAESolarGain.mo
@@ -0,0 +1,117 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses.Examples;
+model ASHRAESolarGain "Example showing the use of ASHRAESolarGain"
+  extends Modelica.Icons.Example;
+  parameter AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 per=
+    AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_ThermaLiteHS20()
+    "Performance data"
+    annotation (choicesAllMatching=true);
+  AixLib.Fluid.SolarCollectors.BaseClasses.ASHRAESolarGain solGai(
+    nSeg=3,
+    incAngDat=per.incAngDat,
+    incAngModDat=per.incAngModDat,
+    shaCoe=0,
+    use_shaCoe_in=true,
+    A_c=per.A,
+    y_intercept=per.y_intercept,
+    redeclare package Medium = AixLib.Media.Water,
+    til=0.78539816339745) "Solar heat gain model using ASHRAE 93 calculations"
+    annotation (Placement(transformation(extent={{70,-10},{90,10}})));
+  Modelica.Blocks.Sources.Sine HGroDifTil(
+    amplitude=50,
+    f=4/86400,
+    offset=100) "Diffuse radiation from the ground, tilted surface"
+    annotation (Placement(transformation(extent={{-10,50},{10,70}})));
+  Modelica.Blocks.Sources.Ramp incAng(duration=86400, height=60*(2*Modelica.Constants.pi
+        /360)) "Incidence angle"
+    annotation (Placement(transformation(extent={{-90,10},{-70,30}})));
+  Modelica.Blocks.Sources.Sine HDirTil(
+    offset=400,
+    amplitude=300,
+    f=2/86400) "Direct beam radiation, tilted surface"
+    annotation (Placement(transformation(extent={{-50,30},{-30,50}})));
+  Modelica.Blocks.Sources.Sine HSkyDifTil(
+    f=1/86400,
+    amplitude=100,
+    offset=100) "Diffuse radiation, tilted surface"
+    annotation (Placement(transformation(extent={{30,70},{50,90}})));
+  Modelica.Blocks.Sources.Ramp shaCoe(
+    height=-1,
+    duration=86400,
+    offset=1) "Shading coefficient"
+    annotation (Placement(transformation(extent={{-90,-30},{-70,-10}})));
+  Modelica.Blocks.Sources.Sine T3(
+    f=2/86400,
+    amplitude=50,
+    offset=273.15 + 110)
+    annotation (Placement(transformation(extent={{-50,-50},{-30,-30}})));
+  Modelica.Blocks.Sources.Sine T2(
+    f=2/86400,
+    amplitude=50,
+    offset=273.15 + 100)
+    annotation (Placement(transformation(extent={{-10,-70},{10,-50}})));
+  Modelica.Blocks.Sources.Sine T1(
+    f=2/86400,
+    amplitude=50,
+    offset=273.15 + 90)
+    annotation (Placement(transformation(extent={{30,-90},{50,-70}})));
+equation
+  connect(HGroDifTil.y,solGai. HGroDifTil) annotation (Line(
+      points={{11,60},{20,60},{20,5},{68,5}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(shaCoe.y,solGai. shaCoe_in) annotation (Line(
+      points={{-69,-20},{-60,-20},{-60,-5},{68,-5}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(incAng.y,solGai. incAng) annotation (Line(
+      points={{-69,20},{-60,20},{-60,-2},{68,-2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HDirTil.y,solGai. HDirTil) annotation (Line(
+      points={{-29,40},{-20,40},{-20,2},{68,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HSkyDifTil.y,solGai. HSkyDifTil) annotation (Line(
+      points={{51,80},{60,80},{60,8},{68,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T3.y,solGai. TFlu[3]) annotation (Line(
+      points={{-29,-40},{-20,-40},{-20,-8},{68,-8},{68,-7.33333}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T2.y,solGai. TFlu[2]) annotation (Line(
+      points={{11,-60},{20,-60},{20,-8},{68,-8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T1.y,solGai. TFlu[1]) annotation (Line(
+      points={{51,-80},{60,-80},{60,-8.66667},{68,-8.66667}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (
+    Documentation(info="<html>
+<p>
+This examples demonstrates the implementation of
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.BaseClasses.ASHRAESolarGain\">
+AixLib.Fluid.SolarCollectors.BaseClasses.ASHRAESolarGain</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+Mar 27, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAESolarGain.mos"
+        "Simulate and plot"),
+        experiment(Tolerance=1e-6, StopTime=86400), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ASHRAESolarGain;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/EN12975HeatLoss.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/EN12975HeatLoss.mo
new file mode 100644
index 0000000000..011df421a2
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/EN12975HeatLoss.mo
@@ -0,0 +1,79 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses.Examples;
+model EN12975HeatLoss "Example showing the use of EN12975HeatLoss"
+  extends Modelica.Icons.Example;
+  parameter AixLib.Fluid.SolarCollectors.Data.GenericEN12975 per=
+    AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_VerificationModel()
+    "Performance data"
+    annotation (choicesAllMatching=true);
+  Modelica.Blocks.Sources.Sine TEnv(
+    f=0.01,
+    offset=273.15 + 10,
+    amplitude=15) "Temperature of the surrounding environment"
+    annotation (Placement(transformation(extent={{30,70},{50,90}})));
+  Modelica.Blocks.Sources.Sine T1(
+    amplitude=15,
+    f=0.1,
+    offset=273.15 + 10) "Temperature of the first segment"
+    annotation (Placement(transformation(extent={{30,-90},{50,-70}})));
+  Modelica.Blocks.Sources.Sine T2(
+    f=0.1,
+    amplitude=15,
+    offset=273.15 + 15) "Temperature of the second segment"
+    annotation (Placement(transformation(extent={{-10,-70},{10,-50}})));
+  Modelica.Blocks.Sources.Sine T3(
+    f=0.1,
+    amplitude=15,
+    offset=273.15 + 20) "Temperature of the third segment"
+    annotation (Placement(transformation(extent={{-50,-50},{-30,-30}})));
+  AixLib.Fluid.SolarCollectors.BaseClasses.EN12975HeatLoss heaLos(
+    nSeg=3,
+    redeclare package Medium = AixLib.Media.Water,
+    a1=per.a1,
+    a2=per.a2,
+    A_c=per.A)       "Heat loss model using EN12975 calculations"
+    annotation (Placement(transformation(extent={{70,-10},{90,10}})));
+equation
+  connect(TEnv.y, heaLos.TEnv) annotation (Line(
+      points={{51,80},{60,80},{60,6},{68,6}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T3.y, heaLos.TFlu[3]) annotation (Line(
+      points={{-29,-40},{-20,-40},{-20,-6},{68,-6},{68,-5.33333}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T2.y, heaLos.TFlu[2]) annotation (Line(
+      points={{11,-60},{20,-60},{20,-6},{68,-6}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T1.y, heaLos.TFlu[1]) annotation (Line(
+      points={{51,-80},{60,-80},{60,-6.66667},{68,-6.66667}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (
+    Documentation(info="<html>
+<p>
+This examples demonstrates the implementation of
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.BaseClasses.EN12975HeatLoss\">
+AixLib.Fluid.SolarCollectors.BaseClasses.EN12975HeatLoss</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+Mar 27, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+  </html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/EN12975HeatLoss.mos"
+        "Simulate and plot"),
+        experiment(Tolerance=1e-6, StopTime=100), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end EN12975HeatLoss;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/EN12975SolarGain.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/EN12975SolarGain.mo
new file mode 100644
index 0000000000..8e384fff03
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/EN12975SolarGain.mo
@@ -0,0 +1,108 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses.Examples;
+model EN12975SolarGain "Example showing the use of EN12975SolarGain"
+  extends Modelica.Icons.Example;
+  parameter AixLib.Fluid.SolarCollectors.Data.GenericEN12975 per=
+    AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_VerificationModel()
+    "Performance data"
+    annotation (choicesAllMatching=true);
+  AixLib.Fluid.SolarCollectors.BaseClasses.EN12975SolarGain solGai(
+    eta0=per.eta0,
+    incAngDat=per.incAngDat,
+    incAngModDat=per.incAngModDat,
+    nSeg=3,
+    A_c=per.A,
+    iamDiff=per.IAMDiff,
+    shaCoe=0,
+    use_shaCoe_in=true,
+    redeclare package Medium = AixLib.Media.Water)
+    "Solar heat gain model using EN12975 calculations"
+    annotation (Placement(transformation(extent={{70,-10},{90,10}})));
+  Modelica.Blocks.Sources.Ramp incAng(duration=86400,
+    height=60*(2*Modelica.Constants.pi/360)) "Incidence angle"
+    annotation (Placement(transformation(extent={{-90,10},{-70,30}})));
+  Modelica.Blocks.Sources.Sine HDirTil(
+    offset=400,
+    amplitude=300,
+    f=2/86400) "Direct beam radiation, tilted surface"
+    annotation (Placement(transformation(extent={{-50,30},{-30,50}})));
+  Modelica.Blocks.Sources.Sine HDifTil(
+    amplitude=200,
+    f=1/86400,
+    offset=300) "Diffuse radiation, tilted surface"
+    annotation (Placement(transformation(extent={{30,70},{50,90}})));
+  Modelica.Blocks.Sources.Ramp shaCoe(
+    duration=86400,
+    offset=1,
+    height=-1) "Shading coefficient"
+    annotation (Placement(transformation(extent={{-90,-30},{-70,-10}})));
+  Modelica.Blocks.Sources.Sine T3(
+    f=2/86400,
+    amplitude=50,
+    offset=273.15 + 110)
+    annotation (Placement(transformation(extent={{-50,-50},{-30,-30}})));
+  Modelica.Blocks.Sources.Sine T2(
+    f=2/86400,
+    amplitude=50,
+    offset=273.15 + 100)
+    annotation (Placement(transformation(extent={{-10,-70},{10,-50}})));
+  Modelica.Blocks.Sources.Sine T1(
+    f=2/86400,
+    amplitude=50,
+    offset=273.15 + 90)
+    annotation (Placement(transformation(extent={{30,-90},{50,-70}})));
+equation
+  connect(incAng.y, solGai.incAng) annotation (Line(
+      points={{-69,20},{-60,20},{-60,-2},{68,-2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(shaCoe.y, solGai.shaCoe_in) annotation (Line(
+      points={{-69,-20},{-60,-20},{-60,-5},{68,-5}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HDirTil.y, solGai.HDirTil) annotation (Line(
+      points={{-29,40},{-20,40},{-20,2},{68,2}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HDifTil.y, solGai.HSkyDifTil) annotation (Line(
+      points={{51,80},{60,80},{60,8},{68,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T3.y, solGai.TFlu[3]) annotation (Line(
+      points={{-29,-40},{-20,-40},{-20,-7.33333},{68,-7.33333}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T2.y, solGai.TFlu[2]) annotation (Line(
+      points={{11,-60},{20,-60},{20,-8},{68,-8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(T1.y, solGai.TFlu[1]) annotation (Line(
+      points={{51,-80},{60,-80},{60,-8},{68,-8},{68,-8.66667}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (
+    Documentation(info="<html>
+<p>
+This examples demonstrates the implementation of
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.BaseClasses.EN12975SolarGain\">
+AixLib.Fluid.SolarCollectors.BaseClasses.EN12975SolarGain</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+Mar 27, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/EN12975SolarGain.mos"
+        "Simulate and plot"),
+        experiment(Tolerance=1e-6, StopTime=86400), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end EN12975SolarGain;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/package.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/package.mo
new file mode 100644
index 0000000000..7aced36f44
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+package Examples "Collection of models that illustrate model use and test models"
+extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains examples for the use of models that can be found in
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.BaseClasses\">
+AixLib.Fluid.SolarCollectors.BaseClasses.</a>
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/package.order b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/package.order
new file mode 100644
index 0000000000..d5f4209aa5
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/Examples/package.order
@@ -0,0 +1,4 @@
+ASHRAEHeatLoss
+ASHRAESolarGain
+EN12975HeatLoss
+EN12975SolarGain
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/IAM.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/IAM.mo
new file mode 100644
index 0000000000..7d826cb24f
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/IAM.mo
@@ -0,0 +1,80 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+function IAM "Function for incident angle modifier"
+  extends Modelica.Icons.Function;
+
+  input Modelica.Units.SI.Angle incAng "Incident angle";
+  input Modelica.Units.SI.Angle[:] incAngDat "Incident angle data";
+  input Real[size(incAngDat,1)] incAngModDat(
+    each final min=0,
+    each final max=1,
+    each final unit="1") "Incident angle modifier data";
+  input Real[size(incAngDat,1)] dMonotone "Incident angle modifier spline derivatives";
+  output Real incAngMod "Incident angle modifier coefficient";
+protected
+  Integer i "Counter to pick the interpolation interval";
+  constant Real delta = 0.0001 "Width of the smoothing function";
+
+algorithm
+  i := 1;
+  for j in 1:size(incAngDat, 1) - 1 loop
+    if incAng > incAngDat[j] then
+      i := j;
+    end if;
+  end for;
+  // Extrapolate or interpolate the data and sets its value to 0 if
+  // the incident angle modifier becomes negative.
+  incAngMod := AixLib.Utilities.Math.Functions.smoothMax(
+    x1 = AixLib.Utilities.Math.Functions.cubicHermiteLinearExtrapolation(
+      x=incAng,
+      x1=incAngDat[i],
+      x2=incAngDat[i + 1],
+      y1=incAngModDat[i],
+      y2=incAngModDat[i + 1],
+      y1d=dMonotone[i],
+      y2d=dMonotone[i + 1]),
+    x2 = 0,
+    deltaX = delta);
+
+  annotation (
+  smoothOrder=1,
+    Documentation(info="<html>
+<h4>Overview</h4>
+<p>
+This function computes the incidence angle modifier for solar irradiation
+striking the surface of the solar thermal collector.
+It is calculated using cubic spline interpolation and
+measurement data for the incident angle modifier provided in data sheets.
+</p>
+
+<h4>References</h4>
+<p>
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v23.2.0/EngineeringReference.pdf\">
+EnergyPlus 23.2.0 Engineering Reference</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 28, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+May 31, 2017, by Michael Wetter and Filip Jorissen:<br/>
+Change limits for incident angle modifier to avoid dip in temperature
+at shallow incidence angles.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/785\">issue 785</a>.
+</li>
+<li>
+November 20, 2014, by Michael Wetter:<br/>
+Added missing <code>protected</code> keyword.
+</li>
+<li>
+May 22, 2012, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end IAM;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/PartialHeatLoss.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/PartialHeatLoss.mo
new file mode 100644
index 0000000000..20d821456a
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/PartialHeatLoss.mo
@@ -0,0 +1,87 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+block PartialHeatLoss
+  "Partial heat loss model on which ASHRAEHeatLoss and EN12975HeatLoss are based"
+  extends Modelica.Blocks.Icons.Block;
+  extends SolarCollectors.BaseClasses.PartialParameters;
+
+  replaceable package Medium = Modelica.Media.Interfaces.PartialMedium
+    "Medium in the component";
+
+  Modelica.Blocks.Interfaces.RealInput TEnv(
+    quantity="ThermodynamicTemperature",
+    unit="K",
+    displayUnit="degC") "Temperature of surrounding environment"
+    annotation (Placement(transformation(extent={{-140,40},{-100,80}})));
+
+  Modelica.Blocks.Interfaces.RealInput TFlu[nSeg](
+    each quantity="ThermodynamicTemperature",
+    each unit = "K",
+    each displayUnit="degC") "Temperature of the heat transfer fluid"
+    annotation (Placement(transformation(extent={{-140,-80},{-100,-40}})));
+  Modelica.Blocks.Interfaces.RealOutput QLos_flow[nSeg](
+    each quantity="HeatFlowRate",
+    each unit="W",
+    each displayUnit="W") = {QLos_internal[i]*smooth(1, if TFlu[i] > TMedMin2
+     then 1 else AixLib.Utilities.Math.Functions.smoothHeaviside(TFlu[i] -
+    TMedMin, dTMin)) for i in 1:nSeg}
+    "Limited heat loss rate at current conditions"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+
+protected
+  constant Modelica.Units.SI.Temperature dTMin=1
+    "Safety temperature difference to prevent TFlu < Medium.T_min";
+  final parameter Modelica.Units.SI.Temperature TMedMin=Medium.T_min + dTMin
+    "Fluid temperature below which there will be no heat loss computed to prevent TFlu < Medium.T_min";
+  final parameter Modelica.Units.SI.Temperature TMedMin2=TMedMin + dTMin
+    "Fluid temperature below which there will be no heat loss computed to prevent TFlu < Medium.T_min";
+
+  input Modelica.Units.SI.HeatFlowRate QLos_internal[nSeg]
+    "Heat loss rate at current conditions for each segment";
+
+  Modelica.Units.SI.TemperatureDifference dT[nSeg]={TEnv - TFlu[i] for i in 1:
+      nSeg} "Environment minus collector fluid temperature";
+
+  annotation (
+defaultComponentName="heaLos",
+Documentation(info="<html>
+<p>
+This component is a partial model used as the base for
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.BaseClasses.ASHRAEHeatLoss\">
+AixLib.Fluid.SolarCollectors.BaseClasses.ASHRAEHeatLoss</a> and
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.BaseClasses.EN12975HeatLoss\">
+AixLib.Fluid.SolarCollectors.BaseClasses.EN12975HeatLoss</a>. It contains the
+input, output and parameter declarations which are common to both models. More
+detailed information is available in the documentation of the extending classes.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+December 17, 2017, by Michael Wetter:<br/>
+Revised computation of heat loss.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1100\">
+issue 1100</a>.
+</li>
+<li>
+June 29, 2015, by Michael Wetter:<br/>
+Revised implementation of heat loss near <code>Medium.T_min</code>
+to make it more efficient.
+</li>
+<li>
+November 20, 2014, by Michael Wetter:<br/>
+Added missing <code>each</code> keyword.
+</li>
+<li>
+Apr 17, 2013, by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialHeatLoss;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/PartialParameters.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/PartialParameters.mo
new file mode 100644
index 0000000000..5e400e6b2d
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/PartialParameters.mo
@@ -0,0 +1,26 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+block PartialParameters "Partial model for parameters"
+
+  parameter Modelica.Units.SI.Area A_c "Area of the collector";
+  parameter Integer nSeg=3 "Number of segments";
+
+  annotation(Documentation(info="<html>
+<p>
+Partial parameters used in all solar collector models
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+Apr 17, 2013, by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialParameters;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/PartialSolarCollector.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/PartialSolarCollector.mo
new file mode 100644
index 0000000000..ede1f50862
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/PartialSolarCollector.mo
@@ -0,0 +1,337 @@
+within AixLib.Fluid.SolarCollectors.BaseClasses;
+partial model PartialSolarCollector "Partial model for solar collectors"
+ extends AixLib.Fluid.Interfaces.LumpedVolumeDeclarations;
+  extends AixLib.Fluid.Interfaces.TwoPortFlowResistanceParameters(
+    final dp_nominal = dp_nominal_final,
+    final computeFlowResistance=(abs(dp_nominal) > Modelica.Constants.eps));
+  extends AixLib.Fluid.Interfaces.PartialTwoPortInterface(
+    final m_flow_nominal=m_flow_nominal_final);
+
+  constant Boolean homotopyInitialization = true "= true, use homotopy method"
+    annotation(HideResult=true);
+
+  parameter Integer nSeg = 3
+    "Number of segments used to discretize the collector model";
+
+  parameter Modelica.Units.SI.Angle azi(displayUnit="deg")
+    "Surface azimuth (0 for south-facing; -90 degree for east-facing; +90 degree for west facing";
+  parameter Modelica.Units.SI.Angle til(displayUnit="deg")
+    "Surface tilt (0 for horizontally mounted collector)";
+  parameter Real rho(
+    final min=0,
+    final max=1,
+    final unit = "1") "Ground reflectance";
+
+  parameter Modelica.Units.SI.HeatCapacity CTot=
+    if per.CTyp==AixLib.Fluid.SolarCollectors.Types.HeatCapacity.TotalCapacity then
+      per.C
+    elseif per.CTyp==AixLib.Fluid.SolarCollectors.Types.HeatCapacity.DryCapacity then
+      per.C+rho_default*per.V*cp_default
+    else
+      385*per.mDry+rho_default*per.V*cp_default
+    "Heat capacity of solar collector with fluid";
+
+  parameter Boolean use_shaCoe_in = false
+    "Enables an input connector for shaCoe"
+    annotation(Dialog(group="Shading"));
+  parameter Real shaCoe(
+    min=0.0,
+    max=1.0) = 0 "Shading coefficient. 0.0: no shading, 1.0: full shading"
+    annotation(Dialog(enable = not use_shaCoe_in, group = "Shading"));
+
+  parameter AixLib.Fluid.SolarCollectors.Types.NumberSelection nColType=
+  AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number
+    "Selection of area specification format"
+    annotation(Dialog(group="Area declarations"));
+  parameter Integer nPanels= 0 "Desired number of panels in the simulation"
+    annotation(Dialog(group="Area declarations", enable= (nColType == AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number)));
+
+  parameter Modelica.Units.SI.Area totalArea=0
+    "Total area of panels in the simulation" annotation (Dialog(group=
+          "Area declarations", enable=(nColType == AixLib.Fluid.SolarCollectors.Types.NumberSelection.Area)));
+
+  parameter AixLib.Fluid.SolarCollectors.Types.SystemConfiguration sysConfig=
+  AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series
+    "Selection of system configuration"
+    annotation(Dialog(group="Configuration declarations"));
+  parameter Integer nPanelsSer=0 "Number of array panels in series"
+    annotation(Dialog(group="Configuration declarations", enable= (sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Array)));
+  parameter Integer nPanelsPar=0 "Number of array panels in parallel"
+    annotation(Dialog(group="Configuration declarations", enable= (sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Array)));
+
+  Modelica.Blocks.Interfaces.RealInput shaCoe_in if use_shaCoe_in
+    "Shading coefficient"
+    annotation(Placement(transformation(extent={{-140,60},{-100,20}})));
+
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather data bus"
+    annotation (Placement(
+    transformation(extent={{-110,70},{-90,90}})));
+  AixLib.BoundaryConditions.SolarIrradiation.DiffusePerez HDifTilIso(
+    final outSkyCon=true,
+    final outGroCon=true,
+    final til=til,
+    final azi=azi,
+    final rho=rho) "Diffuse solar irradiation on a tilted surface"
+    annotation (Placement(transformation(extent={{-80,70},{-60,90}})));
+
+  AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTil(
+    final til=til,
+    final azi=azi) "Direct solar irradiation on a tilted surface"
+    annotation (Placement(transformation(extent={{-80,40},{-60,60}})));
+
+  AixLib.Fluid.Sensors.MassFlowRate senMasFlo(redeclare package Medium =
+    Medium, allowFlowReversal=allowFlowReversal) "Mass flow rate sensor"
+    annotation (Placement(transformation(extent={{-90,-11},{-70,11}})));
+  AixLib.Fluid.FixedResistances.PressureDrop res(
+    redeclare final package Medium = Medium,
+    final from_dp=from_dp,
+    final show_T=show_T,
+    final m_flow_nominal=m_flow_nominal,
+    final allowFlowReversal=allowFlowReversal,
+    final linearized=linearizeFlowResistance,
+    final homotopyInitialization=homotopyInitialization,
+    deltaM=deltaM,
+    final dp_nominal=dp_nominal_final) "Flow resistance"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+
+  // The size of the liquid volume has been increased to also add
+  // the heat capacity of the metal.
+  AixLib.Fluid.MixingVolumes.MixingVolume vol[nSeg](
+    each nPorts=2,
+    redeclare package Medium = Medium,
+    each final m_flow_nominal=m_flow_nominal,
+    each final energyDynamics=energyDynamics,
+    each final p_start=p_start,
+    each final T_start=T_start,
+    each final m_flow_small=m_flow_small,
+    each final V=CTot/cp_default/rho_default*nPanels_internal/nSeg,
+    each final massDynamics=massDynamics,
+    each final X_start=X_start,
+    each final C_start=C_start,
+    each final C_nominal=C_nominal,
+    each final mSenFac=mSenFac,
+    each final allowFlowReversal=allowFlowReversal,
+    each final prescribedHeatFlowRate=false)
+    "Volume of fluid in one segment of the solar collector"
+    annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={50,-20})));
+
+  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor temSen[nSeg]
+    "Temperature sensor"
+    annotation (Placement(transformation(
+      extent={{-10,10},{10,-10}},
+      rotation=180,
+      origin={0,-20})));
+
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow QGai[nSeg]
+    "Rate of solar heat gain"
+    annotation (Placement(transformation(extent={{50,40},{70,60}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow QLos[nSeg]
+    "Rate of heat loss"
+    annotation (Placement(transformation(extent={{50,10},{70,30}})));
+  replaceable parameter AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 per
+    constrainedby AixLib.Fluid.SolarCollectors.Data.BaseClasses.Generic
+    "Performance data"
+    annotation(Placement(transformation(extent={{60,-80},{80,-60}})),choicesAllMatching=true);
+
+protected
+  Modelica.Blocks.Interfaces.RealInput shaCoe_internal
+    "Internally used shading coefficient";
+
+  final parameter Modelica.Units.SI.MassFlowRate m_flow_nominal_final(
+      displayUnit="kg/s") = nPanelsPar_internal*per.mperA_flow_nominal*per.A
+    "Nominal mass flow rate through the system of collectors";
+
+  final parameter Modelica.Units.SI.PressureDifference dp_nominal_final(
+      displayUnit="Pa") = nPanelsSer_internal*per.dp_nominal
+    "Nominal pressure loss across the system of collectors";
+
+  parameter Modelica.Units.SI.Area ATot_internal=nPanels_internal*per.A
+    "Area used in the simulation";
+
+  parameter Real nPanels_internal=
+    if nColType == AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number then
+      nPanels
+    else
+      totalArea/per.A "Number of panels used in the simulation";
+  parameter Real nPanelsSer_internal=
+    if sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series then
+      nPanels
+    else if sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Parallel then
+      1
+    else
+      nPanelsSer "Number of panels in series";
+  parameter Real nPanelsPar_internal=
+    if sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Parallel then
+      nPanels
+    else if sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series then
+      1
+    else
+      nPanelsPar "Number of panels in parallel";
+
+  parameter Medium.ThermodynamicState sta_default = Medium.setState_pTX(
+    T=Medium.T_default,
+    p=Medium.p_default,
+    X=Medium.X_default[1:Medium.nXi]) "Medium state at default properties";
+  parameter Modelica.Units.SI.SpecificHeatCapacity cp_default=
+      Medium.specificHeatCapacityCp(sta_default)
+    "Specific heat capacity of the fluid";
+  parameter Modelica.Units.SI.Density rho_default=Medium.density(sta_default)
+    "Density, used to compute fluid mass";
+
+initial equation
+  assert(homotopyInitialization, "In " + getInstanceName() +
+    ": The constant homotopyInitialization has been modified from its default value. This constant will be removed in future releases.",
+    level = AssertionLevel.warning);
+
+  if sysConfig==AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Array then
+    assert(abs(nPanelsPar_internal*nPanelsSer_internal-nPanels_internal) < 1E-6,
+      "In " + getInstanceName() +
+      ": The product of the number of panels in series and parallel is not equal to the total number of panels in the array.",
+      level = AssertionLevel.error);
+  end if;
+
+equation
+  connect(shaCoe_internal,shaCoe_in);
+
+  if not use_shaCoe_in then
+    shaCoe_internal=shaCoe;
+  end if;
+
+  connect(weaBus, HDifTilIso.weaBus) annotation (Line(
+      points={{-100,80},{-80,80}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(weaBus, HDirTil.weaBus) annotation (Line(
+      points={{-100,80},{-90,80},{-90,50},{-80,50}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(port_a, senMasFlo.port_a) annotation (Line(
+      points={{-100,0},{-90,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(senMasFlo.port_b, res.port_a) annotation (Line(
+      points={{-70,0},{-60,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(vol[nSeg].ports[2], port_b) annotation (Line(
+      points={{51,-10},{51,0},{100,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(vol[1].ports[1], res.port_b) annotation (Line(
+      points={{49,-10},{49,0},{-40,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+      for i in 1:(nSeg - 1) loop
+    connect(vol[i].ports[2], vol[i + 1].ports[1]);
+  end for;
+  connect(vol.heatPort, temSen.port)            annotation (Line(
+      points={{40,-20},{10,-20}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(QGai.port, vol.heatPort) annotation (Line(
+      points={{70,50},{90,50},{90,-40},{30,-40},{30,-20},{40,-20}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(QLos.port, vol.heatPort) annotation (Line(
+      points={{70,20},{90,20},{90,-40},{30,-40},{30,-20},{40,-20}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  annotation (
+    defaultComponentName="solCol",
+    Documentation(info="<html>
+<p>
+This component is a partial model of a solar thermal collector.
+It can be expanded to create solar collector models based on either ASHRAE93 or
+EN12975 ratings data.
+</p>
+
+<h4>References</h4>
+<p>
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v23.2.0/EngineeringReference.pdf\">
+EnergyPlus 23.2.0 Engineering Reference</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 27, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+December 11, 2023, by Michael Wetter:<br/>
+Corrected implementation of pressure drop calculation for the situation where the collectors are in parallel,
+e.g., if <code>sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Parallel</code>.<br/>
+Changed assignment of <code>computeFlowResistance</code> to <code>final</code> based on
+<code>dp_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3597\">Buildings, #3597</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+November 12, 2019, by Filip Jorissen:<br/>
+Set <code>prescribedHeatFlowRate=false</code>
+to avoid a division by zero at zero flow when using SteadyState dynamics.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1636\">Buildings, issue 1636</a>.
+</li>
+<li>
+April 27, 2018, by Michael Wetter:<br/>
+Corrected <code>displayUnit</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/912\">Buildings, issue 912</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+February 8, 2015, by Filip Jorissen:<br/>
+Propagated multiple parameters from <code>LumpedVolumeDeclarations</code>,
+set <code>prescribedHeatFlowRate = true</code> in <code>vol</code>.
+</li>
+<li>
+September 18, 2014, by Michael Wetter:<br/>
+Removed the separate instance of
+<code>Modelica.Thermal.HeatTransfer.Components.HeatCapacitor</code> and
+added this capacity to the volume.
+This is in response to
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/276\">
+https://github.com/lbl-srg/modelica-buildings/issues/276</a>.
+</li>
+<li>
+June 25, 2014, by Michael Wetter:<br/>
+Improved comments for tilt to address
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/246\">
+https://github.com/lbl-srg/modelica-buildings/issues/246</a>.
+</li>
+<li>
+October 8, 2013, by Michael Wetter:<br/>
+Removed parameter <code>show_V_flow</code> in declaration of instance <code>res</code>.
+</li>
+<li>
+January 4, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialSolarCollector;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/package.mo b/AixLib/Fluid/SolarCollectors/BaseClasses/package.mo
new file mode 100644
index 0000000000..dc7c4ab7f6
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Fluid.SolarCollectors;
+package BaseClasses "Package with base classes for AixLib.Fluid.SolarCollectors"
+extends Modelica.Icons.BasesPackage;
+
+
+
+
+
+
+
+
+
+
+annotation (preferredView="info", Documentation(info="<html>
+  <p>
+    This package contains base classes that are used to construct the models in
+    <a href=\"modelica://AixLib.Fluid.SolarCollectors\">AixLib.Fluid.SolarCollectors</a>.
+   </p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/SolarCollectors/BaseClasses/package.order b/AixLib/Fluid/SolarCollectors/BaseClasses/package.order
new file mode 100644
index 0000000000..67be4c23c7
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/BaseClasses/package.order
@@ -0,0 +1,9 @@
+ASHRAEHeatLoss
+ASHRAESolarGain
+EN12975HeatLoss
+EN12975SolarGain
+IAM
+PartialHeatLoss
+PartialParameters
+PartialSolarCollector
+Examples
diff --git a/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/GCritCalc.mo b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/GCritCalc.mo
new file mode 100644
index 0000000000..44f5efd3b9
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/GCritCalc.mo
@@ -0,0 +1,48 @@
+within AixLib.Fluid.SolarCollectors.Controls.BaseClasses.Examples;
+model GCritCalc "Example showing the use of GCritCalc"
+  extends Modelica.Icons.Example;
+  AixLib.Fluid.SolarCollectors.Controls.BaseClasses.GCritCalc criSol(slope=-3.764,
+      y_intercept=0.602)
+    "Calculates the critical insolation based on collector design and current weather conditions"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  Modelica.Blocks.Sources.Sine TEnv(
+    amplitude=10,
+    f=0.1,
+    offset=10)
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  Modelica.Blocks.Sources.Sine TIn(
+    amplitude=10,
+    f=0.01,
+    offset=30)
+    annotation (Placement(transformation(extent={{-80,-40},{-60,-20}})));
+equation
+  connect(TEnv.y, criSol.TEnv)    annotation (Line(
+      points={{-59,30},{-20,30},{-20,5},{-12,5}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(TIn.y, criSol.TIn)    annotation (Line(
+      points={{-59,-30},{-20,-30},{-20,-5},{-12,-5}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (
+  Documentation(info="<html>
+<p>
+This model provides an example of how to use the
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.Controls.BaseClasses.GCritCalc\">
+AixLib.Fluid.SolarCollectors.Controls.BaseClasses.GCritCalc</a> model.<br/>
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+  Mar 27, 2013 by Peter Grant:<br/>
+  First implementation
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Controls/BaseClasses/Examples/GCritCalc.mos"
+        "Simulate and plot"),
+   experiment(Tolerance=1e-6, StopTime=100), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end GCritCalc;
diff --git a/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/package.mo b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/package.mo
new file mode 100644
index 0000000000..4a0223c814
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/package.mo
@@ -0,0 +1,15 @@
+within AixLib.Fluid.SolarCollectors.Controls.BaseClasses;
+package Examples "Package containing examples demonstrating the use of Controls.BaseClasses models"
+
+
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+  This package contains examples demonstrating the use of models that can be found in
+  <a href=\"modelica://AixLib.Fluid.SolarCollectors.Controls.BaseClasses\">
+  AixLib.Fluid.SolarCollectors.Controls.BaseClasses</a>.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/package.order b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/package.order
new file mode 100644
index 0000000000..ee6264ef23
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/Examples/package.order
@@ -0,0 +1 @@
+GCritCalc
diff --git a/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/GCritCalc.mo b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/GCritCalc.mo
new file mode 100644
index 0000000000..aa493d658c
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/GCritCalc.mo
@@ -0,0 +1,74 @@
+within AixLib.Fluid.SolarCollectors.Controls.BaseClasses;
+model GCritCalc "Model calculating the critical insolation level"
+
+  extends Modelica.Blocks.Icons.Block;
+
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer slope
+    "Slope from ratings data";
+  parameter Real y_intercept(final unit="1") "y_intercept from ratings data";
+
+  Modelica.Blocks.Interfaces.RealInput TIn(
+    final unit="K",
+    displayUnit = "degC",
+    quantity = "ThermodynamicTemperature")
+    "Temperature of water entering the collector"
+    annotation (Placement(transformation(extent={{-140,-70},{-100,-30}})));
+  Modelica.Blocks.Interfaces.RealOutput G_TC(
+    final unit="W/m2",
+    quantity = "RadiantEnergyFluenceRate") "Critical radiation level"
+    annotation (Placement(transformation(extent={{100,-16},{132,16}})));
+  Modelica.Blocks.Interfaces.RealInput TEnv(
+    final unit="K",
+    displayUnit = "degC",
+    quantity = "ThermodynamicTemperature")
+    "Ambient temperature at the collector"
+    annotation (Placement(transformation(extent={{-140,30},{-100,70}})));
+
+equation
+  G_TC = -slope * (TIn - TEnv) / y_intercept;
+  annotation (defaultComponentName="criSol",
+  Documentation(info="<html>
+<p>
+This component calculates the solar radiation necessary for the fluid
+in the collector to gain heat. It is used in the model
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.Controls.CollectorPump\">
+AixLib.Fluid.SolarCollectors.Controls.CollectorPump</a>.
+</p>
+<p>
+The critical solar radiation level is calculated using Equation 6.8.2 in
+Duffie and Beckman (2006).
+It is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+G<sub>TC</sub>=F<sub>R</sub>U<sub>L</sub> (T<sub>In</sub>-T<sub>Env</sub>)
+/(F<sub>R</sub>(&tau;&alpha;))
+</p>
+<p>
+where <i>G<sub>TC</sub></i> is the critical solar radiation,
+<i>F<sub>R</sub>U<sub>L</sub></i> is the heat loss coefficient,
+<i>T<sub>In</sub></i> is the inlet temperature, <i>T<sub>Env</sub></i> is the
+ambient temperature, and <i>F<sub>R</sub>(&tau;&alpha;)</i> is the maximum
+efficiency.
+</p>
+<h4>References</h4>
+<p>
+J.A. Duffie and W.A. Beckman 2006, Solar Engineering of Thermal Processes (3rd
+Edition), John Wiley &amp; Sons, Inc.<br/>
+</p>
+</html>",
+revisions = "<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+  February 15, 2013 by Peter Grant <br/>
+  First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GCritCalc;
diff --git a/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/package.mo b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/package.mo
new file mode 100644
index 0000000000..fda641fadb
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Fluid.SolarCollectors.Controls;
+package BaseClasses "Package of BaseClass models used to create the models in the Controls package"
+extends Modelica.Icons.Package;
+
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains base classes that are used in the
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.Controls\">
+AixLib.Fluid.SolarCollectors.Controls</a> package.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/package.order b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/package.order
new file mode 100644
index 0000000000..2e6b137706
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/BaseClasses/package.order
@@ -0,0 +1,2 @@
+GCritCalc
+Examples
diff --git a/AixLib/Fluid/SolarCollectors/Controls/CollectorPump.mo b/AixLib/Fluid/SolarCollectors/Controls/CollectorPump.mo
new file mode 100644
index 0000000000..4abacc35cf
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/CollectorPump.mo
@@ -0,0 +1,164 @@
+within AixLib.Fluid.SolarCollectors.Controls;
+model CollectorPump
+  "Controller which activates a circulation pump when solar radiation is above a critical level"
+  extends Modelica.Blocks.Icons.Block;
+
+  parameter Modelica.Units.SI.HeatFlowRate delQ_flow(min=1)=10
+    "Required estimated heat gain per unit area of collector to switch system on";
+  parameter Modelica.Units.SI.Angle azi(displayUnit="deg")
+    "Surface azimuth (0 for south-facing; -90 degree for east-facing; +90 degree for west facing";
+  parameter Modelica.Units.SI.Angle til(displayUnit="deg")
+    "Surface tilt (0 for horizontally mounted collector)";
+  parameter Real rho(
+    final min=0,
+    final max=1,
+    final unit = "1") = 0.2 "Ground reflectance";
+
+  parameter AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 per
+    "Performance data"
+    annotation (choicesAllMatching=true, Placement(transformation(extent={{60,60},{80,80}})));
+
+  Modelica.Blocks.Interfaces.RealInput TIn(
+    final unit = "K",
+    final displayUnit = "degC",
+    quantity = "ThermodynamicTemperature")
+    "Fluid temperature entering the collector"
+    annotation (Placement(transformation(extent={{-140,-60},{-100,-20}})));
+
+  Modelica.Blocks.Interfaces.BooleanOutput on
+    "Ouputs true if collector pump should be on"
+    annotation (Placement(transformation(extent={{100,-20},{140,20}})));
+
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather data input"
+    annotation (Placement(transformation(extent={{-110,40},{-90,60}})));
+
+  AixLib.Fluid.SolarCollectors.Controls.BaseClasses.GCritCalc criSol(
+    final slope=per.slope,
+    final y_intercept=per.y_intercept)
+    "Calculates the critical insolation based on collector design and current weather conditions"
+    annotation (Placement(visible = true, transformation(origin={-2,0},    extent = {{-58, -20}, {-38, 0}}, rotation = 0)));
+  BoundaryConditions.SolarIrradiation.DiffusePerez HDifTilIso(
+    final til=til,
+    final azi=azi,
+    final rho=rho) "Diffuse solar irradiation on a tilted surface"
+    annotation (Placement(transformation(extent={{-60,50},{-40,70}})));
+  BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTil(
+    final til=til,
+    final azi=azi)
+      "Direct solar irradiation on a tilted surface"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Modelica.Blocks.Math.Add HTotTil(
+    u1(final unit="W/m2"),
+    u2(final unit="W/m2"),
+    y(final unit="W/m2"))
+    "Total irradiation on tilted surface"
+    annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+
+  Modelica.Blocks.Logical.Hysteresis hys(
+    final uLow=0,
+    final uHigh=delQ_flow)
+    annotation (Placement(transformation(extent={{60,-10},{80,10}})));
+protected
+  Modelica.Blocks.Math.Add sub(
+    final k2=-1)
+    "Difference between incident solar and required incident to compensate thermal losses"
+    annotation (Placement(transformation(extent={{20,-10},{40,10}})));
+equation
+  connect(TIn, criSol.TIn)    annotation (Line(
+      points={{-120,-40},{-80,-40},{-80,-15},{-62,-15}},
+      color={0,0,127}));
+  connect(weaBus.TDryBul, criSol.TEnv)    annotation (Line(points={{-99.95,
+          50.05},{-80,50.05},{-80,-5},{-62,-5}},
+                                  color = {255, 204, 51}, thickness = 0.5));
+  connect(HDirTil.weaBus, weaBus) annotation (Line(
+      points={{-60,30},{-80,30},{-80,50},{-100,50}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(HDifTilIso.weaBus, weaBus) annotation (Line(
+      points={{-60,60},{-80,60},{-80,50},{-100,50}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(HDifTilIso.H, HTotTil.u1) annotation (Line(points={{-39,60},{-30,60},{
+          -30,56},{-22,56}}, color={0,0,127}));
+  connect(HDirTil.H, HTotTil.u2) annotation (Line(points={{-39,30},{-30,30},{-30,
+          44},{-22,44}}, color={0,0,127}));
+  connect(HTotTil.y, sub.u1)
+    annotation (Line(points={{1,50},{10,50},{10,6},{18,6}}, color={0,0,127}));
+  connect(criSol.G_TC, sub.u2) annotation (Line(points={{-38.4,-10},{10,-10},{10,
+          -6},{18,-6}}, color={0,0,127}));
+  connect(hys.u, sub.y)
+    annotation (Line(points={{58,0},{41,0}}, color={0,0,127}));
+  connect(on, hys.y) annotation (Line(points={{120,0},{81,0}},
+        color={255,0,255}));
+  annotation (
+  defaultComponentName = "pumCon",
+Documentation(info="<html>
+<p>
+Pump on/off controller for a solar thermal system.
+</p>
+<p>
+This controller outputs whether the pump should be commanded on or off
+based on the incident solar radiation, the collector inlet temperature,
+and the system parameters.
+The pump is commanded on when the incident solar radiation is greater than
+the critical radiation plus the offset <code>delQ_flow</code>,
+and it is switched off if the incident solar radiation is
+below the critical radiation.
+</p>
+<p>
+The critical radiation is defined per Equation 6.8.2 in
+Duffie and Beckman (2006).
+It is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+G<sub>TC</sub>=(F<sub>R</sub>U<sub>L</sub> (T<sub>In</sub>-T<sub>Env</sub>))
+  /(F<sub>R</sub>(&tau;&alpha;))
+</p>
+<p>
+where <i>G<sub>TC</sub></i> is the critical solar radiation,
+<i>F<sub>R</sub>U<sub>L</sub></i> is the heat loss coefficient,
+<i>T<sub>In</sub></i> is the inlet temperature,
+<i>T<sub>Env</sub></i> is the ambient temperature,
+and <i>F<sub>R</sub>(&tau;&alpha;)</i> is the maximum efficiency.
+</p>
+
+<h4>References</h4>
+<p>
+J.A. Duffie and W.A. Beckman 2006, Solar Engineering of Thermal Processes (3rd Edition),
+John Wiley &amp; Sons, Inc.<br/>
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+November 7, 2022, by Michael Wetter:<br/>
+Corrected implementation to make comparison based on total irradiation on tilted surface
+rather than the direct normal irradiation.
+This required adding parameters for the azimuth, tilt and ground reflectance.<br/>
+Changed output from continuous signal to boolean on/off signal as the old implementation run the pump
+possibly at very small flow rates.
+Moved old model to <code>AixLib.Obsolete</code> package.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3074\">issue 3074</a>.
+</li>
+<li>
+January 15, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Icon(graphics={
+      Text(
+        extent={{226,60},{106,10}},
+        textColor={0,0,0},
+        textString=DynamicSelect("",String(y,
+          leftJustified=false,
+          significantDigits=3)))}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end CollectorPump;
diff --git a/AixLib/Fluid/SolarCollectors/Controls/Examples/SolarPumpController.mo b/AixLib/Fluid/SolarCollectors/Controls/Examples/SolarPumpController.mo
new file mode 100644
index 0000000000..9332493934
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/Examples/SolarPumpController.mo
@@ -0,0 +1,56 @@
+within AixLib.Fluid.SolarCollectors.Controls.Examples;
+model SolarPumpController "Example for the solar pump controller"
+  extends Modelica.Icons.Example;
+  AixLib.Fluid.SolarCollectors.Controls.CollectorPump pumCon(
+    azi=0,
+    til=0.78539816339745,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_ThermaLiteHS20())
+    "Model controlling the on/off status of the pump"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
+     filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data input file"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  Modelica.Blocks.Sources.Sine sine(
+    amplitude=20,
+    f=0.0001,
+    offset=273.15 + 40) "Water inlet temperature"
+    annotation (Placement(transformation(extent={{-80,-40},{-60,-20}})));
+equation
+  connect(weaDat.weaBus, pumCon.weaBus)  annotation (Line(
+      points={{-60,30},{-20,30},{-20,5},{-10,5}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(sine.y, pumCon.TIn)  annotation (Line(
+      points={{-59,-30},{-20,-30},{-20,-4},{-12,-4}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation ( __Dymola_Commands(file=
+    "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Controls/Examples/SolarPumpController.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=86400.0),
+    Documentation(info="<html>
+<p>
+This model illustrates the use of the
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.Controls.CollectorPump\">
+AixLib.Fluid.SolarCollectors.Controls.CollectorPump</a> model.
+Based on weather data and inlet temperature, the controller switches the pump on
+and off.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 7, 2022, by Michael Wetter:<br/>
+Revised example to provide values for new parameters.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3074\">issue 3074</a>.
+</li>
+<li>
+Mar 27, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end SolarPumpController;
diff --git a/AixLib/Fluid/SolarCollectors/Controls/Examples/package.mo b/AixLib/Fluid/SolarCollectors/Controls/Examples/package.mo
new file mode 100644
index 0000000000..5662fe029f
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/Examples/package.mo
@@ -0,0 +1,13 @@
+within AixLib.Fluid.SolarCollectors.Controls;
+package Examples "Examples for solar thermal collector controller models"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+annotation (preferredView="info", Documentation(info="<html>
+  <p>
+    This package contains examples demonstrating the use of models that can be found in
+    <a href=\"modelica://AixLib.Fluid.SolarCollectors.Controls\">
+    AixLib.Fluid.SolarCollectors.Controls</a>.
+  </p>
+</html>"));
+end Examples;
diff --git a/AixLib/Fluid/SolarCollectors/Controls/Examples/package.order b/AixLib/Fluid/SolarCollectors/Controls/Examples/package.order
new file mode 100644
index 0000000000..2bfd2ecd8f
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/Examples/package.order
@@ -0,0 +1 @@
+SolarPumpController
diff --git a/AixLib/Fluid/SolarCollectors/Controls/package.mo b/AixLib/Fluid/SolarCollectors/Controls/package.mo
new file mode 100644
index 0000000000..50d17b2347
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/package.mo
@@ -0,0 +1,17 @@
+within AixLib.Fluid.SolarCollectors;
+package Controls "Package for solar thermal collector controllers"
+  extends Modelica.Icons.Package;
+
+  annotation(Documentation(info = "<html>
+  <p>
+    This package contains a controller for solar thermal collectors.
+  </p>
+  </html>"),
+    Icon(graphics={
+      Polygon(origin = {40, -35}, pattern = LinePattern.None, fillPattern = FillPattern.Solid, points = {{-10, 0}, {5, 5}, {5, -5}, {-10, 0}}),
+      Line(origin = {-51.25, 0}, points = {{21.25, -35}, {-13.75, -35}, {-13.75, 35}, {6.25, 35}}),
+      Rectangle(origin = {0, 35.1488}, fillColor = {255, 255, 255}, extent = {{-30, -20.1488}, {30, 20.1488}}),
+      Rectangle(origin = {0, -34.8512}, fillColor = {255, 255, 255}, extent = {{-30, -20.1488}, {30, 20.1488}}),
+      Polygon(origin = {-40, 35}, pattern = LinePattern.None, fillPattern = FillPattern.Solid, points = {{10, 0}, {-5, 5}, {-5, -5}, {10, 0}}),
+      Line(origin = {51.25, 0}, points = {{-21.25, 35}, {13.75, 35}, {13.75, -35}, {-6.25, -35}})}));
+end Controls;
diff --git a/AixLib/Fluid/SolarCollectors/Controls/package.order b/AixLib/Fluid/SolarCollectors/Controls/package.order
new file mode 100644
index 0000000000..5afc6704b9
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Controls/package.order
@@ -0,0 +1,3 @@
+CollectorPump
+Examples
+BaseClasses
diff --git a/AixLib/Fluid/SolarCollectors/Data/BaseClasses/Generic.mo b/AixLib/Fluid/SolarCollectors/Data/BaseClasses/Generic.mo
new file mode 100644
index 0000000000..55fa5d17c0
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/BaseClasses/Generic.mo
@@ -0,0 +1,86 @@
+within AixLib.Fluid.SolarCollectors.Data.BaseClasses;
+record Generic
+  "Generic data record providing common inputs for ASHRAE93 and EN12975 solar collector models"
+  extends Modelica.Icons.Record;
+
+  parameter Modelica.Units.SI.Area A "Area";
+  parameter AixLib.Fluid.SolarCollectors.Types.HeatCapacity CTyp
+    "Total thermal capacity or fluid volume and 'dry' thermal capacity or mass";
+  parameter Modelica.Units.SI.HeatCapacity C
+    "Dry or total thermal capacity of the solar thermal collector";
+  parameter Modelica.Units.SI.Volume V "Fluid volume ";
+  parameter Modelica.Units.SI.Mass mDry "Dry mass";
+  parameter Real mperA_flow_nominal(final unit="kg/(s.m2)")
+    "Nominal mass flow rate per unit area of collector";
+  parameter Modelica.Units.SI.PressureDifference dp_nominal(displayUnit="Pa")
+    "Nominal pressure drop";
+  parameter Modelica.Units.SI.Angle[:] incAngDat=Modelica.Units.Conversions.from_deg({0,10,20,30,40,50,60,70,80,90})
+    "Incident angle data";
+  parameter Real[size(incAngDat,1)] incAngModDat(
+    each final min=0,
+    each final unit="1")
+    "Incident angle modifier data";
+
+  final parameter Boolean validated = validateAngles(
+    incAngDat=incAngDat,
+    incAngModDat=incAngModDat)
+    "True if data are valid, otherwise an assertion is issued";
+
+annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info="<html>
+<p>
+Partial record containing common performance parameters for ASHRAE93 and EN12975
+solar collector models.
+</p>
+<p>
+Depending on the data source that is used, different parameters are available to
+model the thermal capacity of the solar collector.
+The choice of CTyp determines which parameters are used to calculate the
+representative heat capacity of the entire solar collector (including fluid).
+When the dry mass of the solar collector is used to calculate the heat capacity,
+the collector is assumed to be made fully out of copper
+(specific heat capacity of <i>385 J/kg/K</i>).
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<th>CTyp</th>
+<th> C </th>
+<th> V </th>
+<th> mDry </th>
+</tr>
+<tr>
+<td> TotalCapacity </td>
+<td> CTot </td>
+<td> / </td>
+<td> / </td>
+</tr>
+<tr>
+<td> DryCapacity </td>
+<td> CDry </td>
+<td> V </td>
+<td> / </td>
+</tr>
+<tr>
+<td> DryMass </td>
+<td> / </td>
+<td> V </td>
+<td> mDry </td>
+</tr>
+</table>
+</html>", revisions="<html>
+<ul>
+<li>
+February 28, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+January 4, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generic;
diff --git a/AixLib/Fluid/SolarCollectors/Data/BaseClasses/package.mo b/AixLib/Fluid/SolarCollectors/Data/BaseClasses/package.mo
new file mode 100644
index 0000000000..ae735617e7
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/BaseClasses/package.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.SolarCollectors.Data;
+package BaseClasses "Package with base classes for data records of solar thermal collectors"
+  extends Modelica.Icons.BasesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+Package with base classes for performance data for solar thermal collectors.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/Fluid/SolarCollectors/Data/BaseClasses/package.order b/AixLib/Fluid/SolarCollectors/Data/BaseClasses/package.order
new file mode 100644
index 0000000000..ae8758dabb
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/BaseClasses/package.order
@@ -0,0 +1,2 @@
+validateAngles
+Generic
diff --git a/AixLib/Fluid/SolarCollectors/Data/BaseClasses/validateAngles.mo b/AixLib/Fluid/SolarCollectors/Data/BaseClasses/validateAngles.mo
new file mode 100644
index 0000000000..a49a4c4ef0
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/BaseClasses/validateAngles.mo
@@ -0,0 +1,38 @@
+within AixLib.Fluid.SolarCollectors.Data.BaseClasses;
+function validateAngles "Function to validate the provided angles"
+  extends Modelica.Icons.Function;
+  input Modelica.Units.SI.Angle[:] incAngDat(
+    each final min=0,
+    each final max=Modelica.Constants.pi/2)
+    "Incident angle data in degrees";
+  input Real[:] incAngModDat(
+    each final min=0,
+    each final unit="1")
+    "Incident angle modifier data";
+  output Boolean valid;
+protected
+  Integer n = size(incAngDat,1) "Number of elements";
+algorithm
+  assert(size(incAngModDat, 1) == n, "Both arguments incAngDat and incAngModDat must have the same size.");
+  assert(abs(incAngDat[1]) < 1E-4, "First element of incAngDat must be zero.");
+  assert(abs(Modelica.Constants.pi/2-incAngDat[n]) < 1E-4, "Last element of incAngDat must be pi/2.");
+  assert(abs(1-incAngModDat[1]) < 1E-4, "First element of incAngModDat must be 1.");
+  assert(abs(incAngModDat[n]) < 1E-4, "Last element of incAngModDat must be 0.");
+  valid := true;
+
+  annotation (Documentation(info="<html>
+<p>
+Function that validates the incidence angle modifiers.
+If the data are invalid, the function issues an assertion and stops the simulation.
+Otherwise it returns <code>true</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 14, 2023, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end validateAngles;
diff --git a/AixLib/Fluid/SolarCollectors/Data/GenericASHRAE93.mo b/AixLib/Fluid/SolarCollectors/Data/GenericASHRAE93.mo
new file mode 100644
index 0000000000..3c0010ff8e
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GenericASHRAE93.mo
@@ -0,0 +1,29 @@
+within AixLib.Fluid.SolarCollectors.Data;
+record GenericASHRAE93
+  "Generic data record for ASHRAE93 solar collector models"
+  extends AixLib.Fluid.SolarCollectors.Data.BaseClasses.Generic;
+
+  parameter Real y_intercept(final min=0, final max=1, final unit="1")
+    "y intercept (Maximum efficiency)";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer slope(final max=0)
+    "Slope from rating data";
+
+annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info="<html>
+<p>
+Record containing performance parameters for ASHRAE93 solar collector models.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GenericASHRAE93;
diff --git a/AixLib/Fluid/SolarCollectors/Data/GenericEN12975.mo b/AixLib/Fluid/SolarCollectors/Data/GenericEN12975.mo
new file mode 100644
index 0000000000..19f0101e8e
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GenericEN12975.mo
@@ -0,0 +1,33 @@
+within AixLib.Fluid.SolarCollectors.Data;
+record GenericEN12975
+  "Generic data record for EN12975 solar collector models"
+  extends AixLib.Fluid.SolarCollectors.Data.BaseClasses.Generic;
+
+  parameter Real IAMDiff(final min=0, final max=1, final unit="1")
+    "Incidence angle modifier for diffuse irradiance (incidence angle of 50°)";
+  parameter Real eta0(final min=0, final max=1, final unit="1")
+    "Optical efficiency (Maximum efficiency)";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer a1(final min=0)
+    "First order heat loss coefficient";
+  parameter Real a2(final unit="W/(m2.K2)", final min=0)
+    "Second order heat loss coefficient";
+
+annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info="<html>
+<p>
+Record containing performance parameters for EN12975 solar collector models.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GenericEN12975;
diff --git a/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_GuangdongFSPTY95.mo b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_GuangdongFSPTY95.mo
new file mode 100644
index 0000000000..0839374a8e
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_GuangdongFSPTY95.mo
@@ -0,0 +1,26 @@
+within AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate;
+record FP_GuangdongFSPTY95 =
+    AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 (
+    final A=2,
+    final mDry=35,
+    final CTyp=AixLib.Fluid.SolarCollectors.Types.HeatCapacity.DryMass,
+    final C=0,
+    final V=1.7/1000,
+    final dp_nominal=235,
+    final mperA_flow_nominal=0.02,
+    final incAngDat=Modelica.Units.Conversions.from_deg({0,10,20,30,40,50,60,70,80,90}),
+    final incAngModDat={1.0,0.9967,0.9862,0.9671,0.9360,0.8868,0.8065,0.6686,0.4906,0.0},
+    final y_intercept=0.678,
+    final slope=-4.426)
+  "FP - Guandong Fivestar Solar Energy Co, FS-PTY95-2.0"
+    annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info = "<html>
+<h4>References</h4>
+<p>
+Ratings data taken from the <a href=\"http://www.solar-rating.org\">
+Solar Rating and Certification Corporation website</a>. SRCC# = 2012043A.<br/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_SolahartKf.mo b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_SolahartKf.mo
new file mode 100644
index 0000000000..8a4e0a0db0
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_SolahartKf.mo
@@ -0,0 +1,25 @@
+within AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate;
+record FP_SolahartKf =
+    AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 (
+    final A=2.003,
+    final CTyp=AixLib.Fluid.SolarCollectors.Types.HeatCapacity.DryMass,
+    final C=0,
+    final mDry=42,
+    final V=3.8/1000,
+    final dp_nominal=93.89,
+    final mperA_flow_nominal=0.0194,
+    final incAngDat=Modelica.Units.Conversions.from_deg({0,10,20,30,40,50,60,70,80,90}),
+    final incAngModDat={1.0,0.9979,0.9913,0.9792,0.9597,0.929,0.8796,0.7979,0.724,0.0},
+    final y_intercept=0.775,
+    final slope=-5.103) "FP - Solahart Kf"
+    annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info = "<html>
+<h4>References</h4>
+<p>
+Ratings data taken from the <a href=\"http://www.solar-rating.org\">
+Solar Rating and Certification Corporation website</a>. SRCC# = 2012021A.<br/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_TRNSYSValidation.mo b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_TRNSYSValidation.mo
new file mode 100644
index 0000000000..21068c6ff3
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_TRNSYSValidation.mo
@@ -0,0 +1,26 @@
+within AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate;
+record FP_TRNSYSValidation =
+    AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 (
+    A=5,
+    CTyp=AixLib.Fluid.SolarCollectors.Types.HeatCapacity.DryMass,
+    C=0,
+    mDry=8.6,
+    V=0.6/1000,
+    dp_nominal=100,
+    mperA_flow_nominal=0.0111,
+    incAngDat=Modelica.Units.Conversions.from_deg({0,10,20,30,40,50,60,70,80,90}),
+    incAngModDat={1.0,0.9969,0.9872,0.9691,0.9389,0.8889,0.8,0.6152,0.0482,0.0},
+    y_intercept=0.8,
+    slope=-3.6111)
+  "Default values in the TRNSYS Simulation Studio SDHW example"
+    annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info="<html>
+<p>
+Default values in the TRNSYS Simualtion Studio SDHW example.
+No value for <code>dp_nominal</code> was provided in TRNSYS, so 100
+Pascal was used as a placeholder.<br/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_ThermaLiteHS20.mo b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_ThermaLiteHS20.mo
new file mode 100644
index 0000000000..0fd355a5cc
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_ThermaLiteHS20.mo
@@ -0,0 +1,25 @@
+within AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate;
+record FP_ThermaLiteHS20 =
+    AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 (
+    final A=1.97,
+    final CTyp=AixLib.Fluid.SolarCollectors.Types.HeatCapacity.DryMass,
+    final C=0,
+    final mDry=26,
+    final V=2.8/1000,
+    final dp_nominal=242.65,
+    final mperA_flow_nominal=0.1777,
+    final incAngDat=Modelica.Units.Conversions.from_deg({0,10,20,30,40,50,60,70,80,90}),
+    final incAngModDat={1.0,0.9989,0.9946,0.9836,0.9567,0.8882,0.6935,0.0,0.0,0.0},
+    final y_intercept=0.762,
+    final slope=-3.710) "FP - Therma-Lite, HS-20"
+    annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info = "<html>
+<h4>References</h4>
+<p>
+Ratings data taken from the <a href=\"http://www.solar-rating.org\">
+Solar Rating and Certification Corporation website</a>. SRCC# = 2012047A.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_VerificationModel.mo b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_VerificationModel.mo
new file mode 100644
index 0000000000..d00689f92c
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/FP_VerificationModel.mo
@@ -0,0 +1,30 @@
+within AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate;
+record FP_VerificationModel =
+  AixLib.Fluid.SolarCollectors.Data.GenericEN12975 (
+    final A=4.302,
+    final CTyp=AixLib.Fluid.SolarCollectors.Types.HeatCapacity.DryMass,
+    final C=0,
+    final V=4.4/1000,
+    final dp_nominal = 100,
+    final mperA_flow_nominal=0.0241,
+    final eta0=0.720,
+    final IAMDiff=0.133,
+    final a1=2.8312,
+    final a2=0.00119,
+    final incAngDat=Modelica.Units.Conversions.from_deg({0,10,20,30,40,50,60,70,80,90}),
+    final incAngModDat={1.0,0.9967,0.9862,0.9671,0.9360,0.8868,0.8065,0.6686,0.4906,0.0},
+    final mDry=484)
+  "FP - All inputs necessary for verification of EN12975 models"
+    annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info = "<html>
+<p>
+No model on the <a href=\"http://www.solar-rating.org\"> Solar Rating and
+Certification Corporation </a> website tested to EN12975 standards provides all
+of the necessary information for modeling.
+This data record was created to allow verification of EN12975 base classes
+despite the limitations in available data.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/package.mo b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/package.mo
new file mode 100644
index 0000000000..8aae94f16f
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Fluid.SolarCollectors.Data;
+package GlazedFlatPlate "Package with SRCC rating information for glazed flat-plate solar thermal collectors"
+extends Modelica.Icons.MaterialPropertiesPackage;
+
+
+annotation (Documentation(info="<html>
+  <p>
+    Package with records for SRCC rating information for glazed flat-plate solar thermal collector.
+    All models in the GlazedFlatPlate package are tested according to the ASHRAE Standard 93.
+  </p>
+  </html>",
+  revisions="<html>
+    <ul>
+      <li>
+        June 8, 2012, by Wangda Zuo:<br/>
+        First implementation.
+      </li>
+    </ul>
+  </html>"));
+end GlazedFlatPlate;
diff --git a/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/package.order b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/package.order
new file mode 100644
index 0000000000..8cdac5e8e9
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/GlazedFlatPlate/package.order
@@ -0,0 +1,5 @@
+FP_GuangdongFSPTY95
+FP_SolahartKf
+FP_TRNSYSValidation
+FP_ThermaLiteHS20
+FP_VerificationModel
diff --git a/AixLib/Fluid/SolarCollectors/Data/Tubular/T_AMKCollectraAGOWR20.mo b/AixLib/Fluid/SolarCollectors/Data/Tubular/T_AMKCollectraAGOWR20.mo
new file mode 100644
index 0000000000..997c51f7f4
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/Tubular/T_AMKCollectraAGOWR20.mo
@@ -0,0 +1,30 @@
+within AixLib.Fluid.SolarCollectors.Data.Tubular;
+record T_AMKCollectraAGOWR20 =
+    AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 (
+    final A=3.457,
+    final CTyp=AixLib.Fluid.SolarCollectors.Types.HeatCapacity.DryMass,
+    final C=0,
+    final mDry=73,
+    final V=3.5/1000,
+    final dp_nominal=100,
+    final mperA_flow_nominal=0.0201,
+    final incAngDat=Modelica.Units.Conversions.from_deg({0,10,20,30,40,50,60,70,80,90}),
+    final incAngModDat={1.0,1.0088,1.0367,1.0884,1.1743,1.3164,1.567,2.0816,3.6052,0.0},
+    final y_intercept=0.446,
+    final slope=-1.432) "T - AMG Collectra AG, OWR 20"
+    annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info = "<html>
+<h4>References</h4>
+<p>
+Ratings data taken from the <a href=\"http://www.solar-rating.org\">
+Solar Rating and Certification Corporation website</a>.
+SRCC# = 2012018A.
+</p>
+<p>
+The ratings provided for <code>dp_nominal</code> were suspicious
+so 100 Pa is used instead.<br/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Data/Tubular/T_JiaxingDiyiC0130.mo b/AixLib/Fluid/SolarCollectors/Data/Tubular/T_JiaxingDiyiC0130.mo
new file mode 100644
index 0000000000..72196970cd
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/Tubular/T_JiaxingDiyiC0130.mo
@@ -0,0 +1,30 @@
+within AixLib.Fluid.SolarCollectors.Data.Tubular;
+record T_JiaxingDiyiC0130 =
+    AixLib.Fluid.SolarCollectors.Data.GenericASHRAE93 (
+    final A=4.650,
+    final CTyp=AixLib.Fluid.SolarCollectors.Types.HeatCapacity.DryMass,
+    final C=0,
+    final mDry=95,
+    final V=1.7/1000,
+    final dp_nominal=100,
+    final mperA_flow_nominal=0.0142,
+    final incAngDat=Modelica.Units.Conversions.from_deg({0,10,20,30,40,50,60,70,80,90}),
+    final incAngModDat={1.0,1.0222,1.0897,1.2034,1.3596,1.5272,1.5428,0.4206,0.0,0.0},
+    final y_intercept=0.388,
+    final slope=-1.453) "T - Jiaxing Diyi New Energy Co., Ltd., DIYI-C01-30"
+    annotation (
+defaultComponentPrefixes="parameter",
+defaultComponentName="datSolCol",
+Documentation(info = "<html>
+<h4>References</h4>
+<p>
+Ratings data taken from the <a href=\"http://www.solar-rating.org\">
+Solar Rating and Certification Corporation website</a>.
+SRCC# = 2012036A.
+</p>
+<p>
+The ratings provided for <code>dp_nominal</code> were suspicious
+so 100 Pa is used instead.<br/>
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Data/Tubular/package.mo b/AixLib/Fluid/SolarCollectors/Data/Tubular/package.mo
new file mode 100644
index 0000000000..e145fd550c
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/Tubular/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Fluid.SolarCollectors.Data;
+package Tubular "Package with SRCC rating information for tubular solar thermal collectors"
+extends Modelica.Icons.MaterialPropertiesPackage;
+
+    annotation(Documentation(info="<html>
+      <p>
+        Package with data describing tubular solar collectors. All models in the Tubular
+        pacakage use ASHRAE93 test data.
+      </p>
+    </html>"));
+end Tubular;
diff --git a/AixLib/Fluid/SolarCollectors/Data/Tubular/package.order b/AixLib/Fluid/SolarCollectors/Data/Tubular/package.order
new file mode 100644
index 0000000000..bd5f3c83ca
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/Tubular/package.order
@@ -0,0 +1,2 @@
+T_AMKCollectraAGOWR20
+T_JiaxingDiyiC0130
diff --git a/AixLib/Fluid/SolarCollectors/Data/package.mo b/AixLib/Fluid/SolarCollectors/Data/package.mo
new file mode 100644
index 0000000000..cb962d6300
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/package.mo
@@ -0,0 +1,17 @@
+within AixLib.Fluid.SolarCollectors;
+package Data "Data for solar thermal collectors"
+extends Modelica.Icons.MaterialPropertiesPackage;
+
+annotation (Documentation(info="<html>
+  <p>
+    Package with performance data for solar thermal collectors. All solar collector data package
+    names begin with an abbreviation of the type of collector it is.  The abbreviations are as
+    follows:
+  </p>
+  <ul>
+    <li>C: Concentrating</li>
+    <li>FP: Flat Plate</li>
+    <li>T: Tubular</li>
+  </ul>
+</html>"));
+end Data;
diff --git a/AixLib/Fluid/SolarCollectors/Data/package.order b/AixLib/Fluid/SolarCollectors/Data/package.order
new file mode 100644
index 0000000000..361d653672
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Data/package.order
@@ -0,0 +1,5 @@
+GenericASHRAE93
+GenericEN12975
+GlazedFlatPlate
+Tubular
+BaseClasses
diff --git a/AixLib/Fluid/SolarCollectors/EN12975.mo b/AixLib/Fluid/SolarCollectors/EN12975.mo
new file mode 100644
index 0000000000..b3e4c470d9
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/EN12975.mo
@@ -0,0 +1,203 @@
+within AixLib.Fluid.SolarCollectors;
+model EN12975 "Model of a solar thermal collector according to the ASHRAE Standard 93"
+  extends AixLib.Fluid.SolarCollectors.BaseClasses.PartialSolarCollector(
+    redeclare AixLib.Fluid.SolarCollectors.Data.GenericEN12975 per);
+
+  AixLib.Fluid.SolarCollectors.BaseClasses.EN12975SolarGain solGai(
+    redeclare package Medium = Medium,
+    final nSeg=nSeg,
+    final incAngDat=per.incAngDat,
+    final incAngModDat=per.incAngModDat,
+    final iamDiff=per.IAMDiff,
+    final eta0=per.eta0,
+    final use_shaCoe_in=use_shaCoe_in,
+    final shaCoe=shaCoe,
+    final A_c=ATot_internal)
+    "Identifies heat gained from the sun using the EN12975 standard calculations"
+     annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+  AixLib.Fluid.SolarCollectors.BaseClasses.EN12975HeatLoss heaLos(
+    redeclare package Medium = Medium,
+    final nSeg=nSeg,
+    final a1=per.a1,
+    final a2=per.a2,
+    final A_c=ATot_internal)
+    "Calculates the heat lost to the surroundings using the EN12975 standard calculations"
+      annotation (Placement(transformation(extent={{-20,10},{0,30}})));
+
+equation
+  // Make sure the model is only used with the EN ratings data, and hence a1 > 0
+  assert(per.a1 > 0,
+    "In " + getInstanceName() + ": The heat loss coefficient from the EN 12975 ratings data must be strictly positive. Obtained a1 = " + String(per.a1));
+  connect(shaCoe_internal, solGai.shaCoe_in);
+
+  connect(weaBus.TDryBul, heaLos.TEnv) annotation (Line(
+      points={{-99.95,80.05},{-90,80.05},{-90,26},{-22,26}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None), Text(
+      textString="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}}));
+  connect(HDirTil.inc, solGai.incAng)    annotation (Line(
+      points={{-59,46},{-50,46},{-50,48},{-22,48}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HDifTilIso.H, solGai.HSkyDifTil) annotation (Line(
+      points={{-59,80},{-30,80},{-30,58},{-22,58}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(HDirTil.H, solGai.HDirTil) annotation (Line(
+      points={{-59,50},{-50,50},{-50,52},{-22,52}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(shaCoe_in, solGai.shaCoe_in) annotation (Line(
+      points={{-120,40},{-40,40},{-40,45},{-22,45}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(heaLos.TFlu, temSen.T) annotation (Line(
+      points={{-22,14},{-30,14},{-30,-20},{-11,-20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(heaLos.QLos_flow, QLos.Q_flow) annotation (Line(
+      points={{1,20},{50,20}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(solGai.QSol_flow, QGai.Q_flow) annotation (Line(
+      points={{1,50},{50,50}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(temSen.T, solGai.TFlu) annotation (Line(
+      points={{-11,-20},{-30,-20},{-30,42},{-22,42}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  annotation (
+  defaultComponentName="solCol",
+  Documentation(info="<html>
+<p>
+This component models a solar thermal collector according to the EN12975
+test standard.
+</p>
+
+<h4>References</h4>
+<p>
+CEN 2022, European Standard 12975:2022, European Committee for Standardization
+</p>
+<p>
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v23.2.0/EngineeringReference.pdf\">
+EnergyPlus 23.2.0 Engineering Reference</a>
+</p>
+</html>",
+      revisions="<html>
+<ul>
+<li>
+February 28, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+December 11, 2023, by Michael Wetter:<br/>
+Corrected implementation of pressure drop calculation for the situation where the collectors are in parallel,
+e.g., if <code>sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Parallel</code>.<br/>
+Changed assignment of <code>computeFlowResistance</code> to <code>final</code> based on
+<code>dp_nominal</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3597\">Buildings, #3597</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+December 17, 2017, by Michael Wetter:<br/>
+Revised computation of heat loss.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1100\">
+issue 1100</a>.
+</li>
+<li>
+November 21, 2017, by Michael Wetter:<br/>
+Corrected error in heat loss calculations that did not scale correctly with <code>nPanels</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1073\">issue 1073</a>.
+</li>
+<li>
+January 4, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+      Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
+            100}}),
+      graphics={
+        Rectangle(
+          extent={{-84,100},{84,-100}},
+          lineColor={27,0,55},
+          fillColor={26,0,55},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-100,0},{-76,0},{-76,-90},{66,-90},{66,-60},{-64,-60},{-64,
+              -30},{66,-30},{66,0},{-64,0},{-64,28},{66,28},{66,60},{-64,60},{
+              -64,86},{78,86},{78,0},{98,0},{100,0}},
+          color={0,128,255},
+          thickness=1,
+          smooth=Smooth.None),
+        Ellipse(
+          extent={{-24,26},{28,-26}},
+          lineColor={255,255,0},
+          fillColor={255,255,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-6,-6},{8,8}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={-24,30},
+          rotation=90),
+        Line(
+          points={{-50,0},{-30,0}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1),
+        Line(
+          points={{-36,-40},{-20,-24}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1),
+        Line(
+          points={{-10,0},{10,0}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={2,-40},
+          rotation=90),
+        Line(
+          points={{-8,-8},{6,6}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={30,-30},
+          rotation=90),
+        Line(
+          points={{32,0},{52,0}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1),
+        Line(
+          points={{-8,-8},{6,6}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={28,32},
+          rotation=180),
+        Line(
+          points={{-10,0},{10,0}},
+          color={255,255,0},
+          smooth=Smooth.None,
+          thickness=1,
+          origin={0,40},
+          rotation=90)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end EN12975;
diff --git a/AixLib/Fluid/SolarCollectors/Examples/FlatPlate.mo b/AixLib/Fluid/SolarCollectors/Examples/FlatPlate.mo
new file mode 100644
index 0000000000..33f31b71a7
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Examples/FlatPlate.mo
@@ -0,0 +1,120 @@
+within AixLib.Fluid.SolarCollectors.Examples;
+model FlatPlate "Test model for FlatPlate"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = Modelica.Media.Incompressible.Examples.Glycol47
+    "Medium in the system";
+
+  AixLib.Fluid.SolarCollectors.ASHRAE93 solCol(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    rho=0.2,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Array,
+    nPanelsSer=5,
+    nPanelsPar=5,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_GuangdongFSPTY95(),
+    nPanels=25,
+    nSeg=9,
+    azi=0.3,
+    til=0.5,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    massDynamics=Modelica.Fluid.Types.Dynamics.SteadyState)
+    "Flat plate solar collector model"
+    annotation (Placement(transformation(extent={{2,-10},{22,10}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+    Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data input file"
+    annotation (Placement(transformation(extent={{-28,60},{-8,80}})));
+  AixLib.Fluid.Sources.Boundary_pT sin(
+    redeclare package Medium = Medium,
+    p(displayUnit="bar") = 100000,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{82,-10},{62,10}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TOut(
+    redeclare package Medium = Medium,
+    T_start(displayUnit="K"),
+    m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{32,-10},{52,10}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TIn(redeclare package Medium =
+    Medium, m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{-28,-10},{-8,10}})));
+  Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    T=273.15 + 10,
+    nPorts=1,
+    use_p_in=true) "Inlet for water flow"
+    annotation (Placement(
+      transformation(
+      extent={{10,-10},{-10,10}},
+      rotation=180,
+      origin={-48,0})));
+  Modelica.Blocks.Sources.Sine sine(
+    f=3/86400,
+    amplitude=-solCol.dp_nominal,
+    offset=1E5) "Pressure source"
+    annotation (Placement(transformation(extent={{-88,-18},{-68,2}})));
+equation
+  connect(solCol.port_b, TOut.port_a) annotation (Line(
+      points={{22,0},{32,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(sou.ports[1], TIn.port_a) annotation (Line(
+      points={{-38,0},{-28,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(weaDat.weaBus, solCol.weaBus) annotation (Line(
+      points={{-8,70},{2,70},{2,8}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(TIn.port_b, solCol.port_a)
+    annotation (Line(points={{-8,0},{2,0}},               color={0,127,255}));
+  connect(TOut.port_b, sin.ports[1])
+    annotation (Line(points={{52,0},{62,0}},              color={0,127,255}));
+  connect(sine.y, sou.p_in) annotation (Line(points={{-67,-8},{-60,-8}},
+                           color={0,0,127}));
+  annotation (
+    Documentation(info="<html>
+<p>
+This example demonstrates the implementation of
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.ASHRAE93\">
+AixLib.Fluid.SolarCollectors.ASHRAE93</a>
+for a variable fluid flow rate and weather data from San Francisco, CA, USA.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+September 18, 2014, by Michael Wetter:<br/>
+Changed medium from water to glycol.
+</li>
+<li>
+Mar 27, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlate.mos"
+        "Simulate and plot"),
+ experiment(Tolerance=1e-6, StopTime=86400.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end FlatPlate;
diff --git a/AixLib/Fluid/SolarCollectors/Examples/FlatPlateShaCoeTrue.mo b/AixLib/Fluid/SolarCollectors/Examples/FlatPlateShaCoeTrue.mo
new file mode 100644
index 0000000000..c19077b511
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Examples/FlatPlateShaCoeTrue.mo
@@ -0,0 +1,122 @@
+within AixLib.Fluid.SolarCollectors.Examples;
+model FlatPlateShaCoeTrue "Test model for FlatPlate with use_shaCoe_in = true"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Water "Medium in the system";
+  AixLib.Fluid.SolarCollectors.ASHRAE93          solCol(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    from_dp=true,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    use_shaCoe_in=true,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_GuangdongFSPTY95(),
+    rho=0.2,
+    azi=0,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nPanels=5,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series,
+    nSeg=9,
+    til=0.5235987755983) "Flat plate solar collector with 3 segments"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+    Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data input file"
+    annotation (Placement(transformation(extent={{-40,60},{-20,80}})));
+  AixLib.Fluid.Sources.Boundary_pT sin(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{70,-10},{50,10}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TOut(
+    redeclare package Medium = Medium,
+    T_start(displayUnit="K"),
+    m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{20,-10},{40,10}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TIn(redeclare package Medium =
+    Medium, m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{-40,-10},{-20,10}})));
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    nPorts=1,
+    T=273.15 + 10,
+    p(displayUnit="Pa") = 101325 + 5*solCol.per.dp_nominal)
+    "Inlet for water flow"
+    annotation (Placement(
+        transformation(
+        extent={{10,10},{-10,-10}},
+        rotation=180,
+        origin={-60,0})));
+  Modelica.Blocks.Sources.Ramp shaCoe(
+    startTime=34040,
+    height=1,
+    duration=24193) "Varying shading coefficient"
+    annotation (Placement(transformation(extent={{-58,30},{-38,50}})));
+equation
+  connect(solCol.port_b, TOut.port_a) annotation (Line(
+      points={{10,0},{20,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TOut.port_b, sin.ports[1]) annotation (Line(
+      points={{40,0},{50,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TIn.port_b, solCol.port_a) annotation (Line(
+      points={{-20,0},{-10,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(sou.ports[1], TIn.port_a) annotation (Line(
+      points={{-50,0},{-50,0},{-40,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(shaCoe.y, solCol.shaCoe_in) annotation (Line(
+      points={{-37,40},{-16,40},{-16,4},{-12,4},{-12,4}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(weaDat.weaBus, solCol.weaBus) annotation (Line(
+      points={{-20,70},{-10,70},{-10,8}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  annotation (
+    Documentation(info="<html>
+<p>
+This example demonstrates the use of <code>use_shaCoe_in</code>.
+Aside from changed use of <code>use_shaCoe_in</code> it is identical to
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.Examples.FlatPlate\">
+AixLib.Fluid.SolarCollectors.Examples.FlatPlate</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+May 13, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateShaCoeTrue.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=86400.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end FlatPlateShaCoeTrue;
diff --git a/AixLib/Fluid/SolarCollectors/Examples/FlatPlateTotalArea.mo b/AixLib/Fluid/SolarCollectors/Examples/FlatPlateTotalArea.mo
new file mode 100644
index 0000000000..d9de3b9a3c
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Examples/FlatPlateTotalArea.mo
@@ -0,0 +1,161 @@
+within AixLib.Fluid.SolarCollectors.Examples;
+model FlatPlateTotalArea "Example showing the use of TotalArea and nSeg"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Water "Medium in the system";
+
+  AixLib.Fluid.SolarCollectors.ASHRAE93          solCol(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    from_dp=true,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    rho=0.2,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_SolahartKf(),
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nPanels=10,
+    nSeg=9,
+    azi=0.3,
+    til=0.5) "Flat plate solar collector model"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+    Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data input file"
+    annotation (Placement(transformation(extent={{-60,60},{-40,80}})));
+  AixLib.Fluid.Sources.Boundary_pT sin(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=2) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{70,-10},{50,10}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TOut(
+    redeclare package Medium = Medium,
+    T_start(displayUnit="K"),
+    m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{20,20},{40,40}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TIn(redeclare package Medium =
+    Medium, m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{-40,20},{-20,40}})));
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    T=273.15 + 10,
+    use_p_in=false,
+    nPorts=2,
+    p(displayUnit="Pa") = 101325 + solCol.dp_nominal) "Inlet for water flow"
+    annotation (Placement(
+        transformation(
+        extent={{10,10},{-10,-10}},
+        rotation=180,
+        origin={-60,0})));
+
+  AixLib.Fluid.SolarCollectors.ASHRAE93 solCol1(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    from_dp=true,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    rho=0.2,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_SolahartKf(),
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nPanels=10,
+    nSeg=27,
+    azi=0.3,
+    til=0.5) "Flat plate solar collector model"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TOut1(
+    redeclare package Medium = Medium,
+    T_start(displayUnit="K"),
+    m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{20,-40},{40,-20}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TIn1(
+    redeclare package Medium =
+    Medium, m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{-40,-40},{-20,-20}})));
+equation
+  connect(solCol.port_b, TOut.port_a) annotation (Line(
+      points={{10,30},{20,30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TOut.port_b, sin.ports[1]) annotation (Line(
+      points={{40,30},{50,30},{50,-1}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TIn.port_b, solCol.port_a) annotation (Line(
+      points={{-20,30},{-10,30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(sou.ports[1], TIn.port_a) annotation (Line(
+      points={{-50,-1},{-50,30},{-40,30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(weaDat.weaBus, solCol.weaBus) annotation (Line(
+      points={{-40,70},{-14,70},{-14,38},{-10,38},{-10,38}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(solCol1.port_b, TOut1.port_a)
+                                      annotation (Line(
+      points={{10,-30},{20,-30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TIn1.port_b, solCol1.port_a)
+                                     annotation (Line(
+      points={{-20,-30},{-10,-30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(weaDat.weaBus, solCol1.weaBus)
+                                        annotation (Line(
+      points={{-40,70},{-14,70},{-14,-22},{-10,-22}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(sou.ports[2], TIn1.port_a) annotation (Line(
+      points={{-50,1},{-50,-30},{-40,-30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TOut1.port_b, sin.ports[2]) annotation (Line(
+      points={{40,-30},{50,-30},{50,1}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  annotation (
+    Documentation(info="<html>
+<p>
+This model uses <code>TotalArea</code> instead of <code>nPanels</code> to
+define the system size.
+Aside from that change, this model is identical to
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.Examples.FlatPlate\">
+AixLib.Fluid.SolarCollectors.Examples.FlatPlate</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+Mar 27, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateTotalArea.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=86400.0), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end FlatPlateTotalArea;
diff --git a/AixLib/Fluid/SolarCollectors/Examples/FlatPlateWithTank.mo b/AixLib/Fluid/SolarCollectors/Examples/FlatPlateWithTank.mo
new file mode 100644
index 0000000000..a015bc6c4b
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Examples/FlatPlateWithTank.mo
@@ -0,0 +1,285 @@
+within AixLib.Fluid.SolarCollectors.Examples;
+model FlatPlateWithTank
+  "Example showing use of the flat plate solar collector in a complete solar thermal system"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Water
+    "Fluid in the storage tank";
+  replaceable package Medium_2 = AixLib.Media.Water "Fluid flowing through the collector";
+
+  parameter Modelica.Units.SI.Angle azi=0.3
+    "Surface azimuth (0 for south-facing; -90 degree for east-facing; +90 degree for west facing";
+  parameter Modelica.Units.SI.Angle til=0.78539816339745
+    "Surface tilt (0 for horizontally mounted collector)";
+  parameter Real rho=0.2 "Ground reflectance";
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal = solCol.m_flow_nominal
+    "Nominal mass flow rate";
+
+  AixLib.Fluid.SolarCollectors.ASHRAE93 solCol(
+    redeclare package Medium = Medium_2,
+    shaCoe=0,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nPanels=5,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_SolahartKf(),
+    nSeg=9,
+    final azi=azi,
+    final til=til,
+    final rho=rho) "Flat plate solar collector model"
+    annotation (Placement(transformation(extent={{-2,46},{18,66}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+    Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"),
+    computeWetBulbTemperature=false) "Weather data file reader"
+    annotation (Placement(transformation(extent={{-180,60},{-160,80}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TOut(
+    T_start(displayUnit="K"),
+    m_flow_nominal=m_flow_nominal,
+    redeclare package Medium = Medium_2) "Temperature sensor"
+    annotation (Placement(transformation(extent={{30,46},{50,66}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TIn(m_flow_nominal=m_flow_nominal,
+    redeclare package Medium = Medium_2) "Temperature sensor"
+    annotation (Placement(transformation(extent={{-34,46},{-14,66}})));
+  AixLib.Fluid.Storage.StratifiedEnhancedInternalHex
+   tan(
+    nSeg=4,
+    redeclare package Medium = Medium,
+    hTan=1.8,
+    m_flow_nominal=m_flow_nominal,
+    VTan=1.5,
+    dIns=0.07,
+    redeclare package MediumHex = Medium_2,
+    CHex=200,
+    dExtHex=0.01905,
+    hHex_a=0.9,
+    hHex_b=0.65,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    Q_flow_nominal=3000,
+    mHex_flow_nominal=3000/20/4200,
+    T_start=293.15,
+    TTan_nominal=293.15,
+    THex_nominal=323.15,
+    energyDynamicsHex=Modelica.Fluid.Types.Dynamics.FixedInitial)
+    "Storage tank model"
+    annotation (Placement(transformation(
+      extent={{-20,-20},{20,20}},
+      origin={100,-20})));
+  AixLib.Fluid.SolarCollectors.Controls.CollectorPump pumCon(
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_ThermaLiteHS20(),
+    final azi=azi,
+    final til=til,
+    final rho=rho)
+    "Pump controller"
+    annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={-130,0})));
+  Modelica.Thermal.HeatTransfer.Sources.FixedTemperature rooT(T=293.15)
+    "Room temperature"
+    annotation (Placement(transformation(extent={{20,-90},{40,-70}})));
+  AixLib.Fluid.Sources.Boundary_pT bou(redeclare package Medium =
+    Medium, nPorts=1) "Outlet for hot water draw"
+    annotation (Placement(transformation(
+      extent={{-10,-10},{10,10}},
+      rotation=180,
+      origin={150,20})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou1(
+    redeclare package Medium = Medium,
+    use_m_flow_in=false,
+    nPorts=1,
+    m_flow=0.001,
+    T=288.15) "Inlet and flow rate for hot water draw"
+    annotation (Placement(transformation(
+      extent={{10,-10},{-10,10}},
+      origin={150,-20})));
+  AixLib.Fluid.Movers.FlowControlled_m_flow pum(
+    redeclare package Medium = Medium_2,
+    m_flow_nominal=m_flow_nominal,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    nominalValuesDefineDefaultPressureCurve=true)
+    "Pump forcing circulation through the system" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-50,0})));
+  AixLib.Fluid.Storage.ExpansionVessel exp(
+    redeclare package Medium = Medium_2,
+    V_start=0.1) "Expansion tank"
+    annotation (Placement(transformation(
+      extent={{-10,-10},{10,10}},
+      origin={0,-20})));
+  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor TTan
+    "Temperature in the tank water that surrounds the heat exchanger"
+    annotation (Placement(transformation(extent={{-80,20},{-100,40}})));
+
+  Modelica.Blocks.Math.BooleanToReal booToRea(
+    realTrue=m_flow_nominal)
+    "Conversion of control signal to real-valued signal"
+	annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+equation
+  connect(solCol.port_b,TOut. port_a) annotation (Line(
+      points={{18,56},{30,56}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TIn.port_b,solCol. port_a) annotation (Line(
+      points={{-14,56},{-2,56}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(weaDat.weaBus,solCol. weaBus) annotation (Line(
+      points={{-160,70},{-2,70},{-2,64}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(weaDat.weaBus, pumCon.weaBus) annotation (Line(
+      points={{-160,70},{-152,70},{-152,5},{-140,5}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(rooT.port, tan.heaPorTop)                  annotation (Line(
+      points={{40,-80},{48,-80},{48,0},{104,0},{104,-5.2}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(rooT.port, tan.heaPorSid)                  annotation (Line(
+      points={{40,-80},{111.2,-80},{111.2,-20}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(pum.port_b, TIn.port_a) annotation (Line(
+      points={{-50,10},{-50,56},{-34,56}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(pum.port_a, exp.port_a) annotation (Line(
+      points={{-50,-10},{-50,-36},{0,-36},{0,-30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(exp.port_a, tan.portHex_b) annotation (Line(
+      points={{0,-30},{0,-36},{80,-36}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TOut.port_b, tan.portHex_a) annotation (Line(
+      points={{50,56},{68,56},{68,-27.6},{80,-27.6}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(bou.ports[1], tan.port_a) annotation (Line(
+      points={{140,20},{100,20},{100,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(bou1.ports[1], tan.port_b) annotation (Line(
+      points={{140,-20},{120,-20},{120,-40},{100,-40}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(tan.heaPorVol[3], TTan.port) annotation (Line(
+      points={{100,-19.85},{98,-19.85},{98,-20},{96,-20},{96,30},{-80,30}},
+      color={191,0,0},
+      smooth=Smooth.None));
+  connect(TTan.T, pumCon.TIn) annotation (Line(
+      points={{-101,30},{-160,30},{-160,-4},{-142,-4}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(pumCon.on, booToRea.u)
+    annotation (Line(points={{-118,0},{-102,0}}, color={255,0,255}));
+  connect(pum.m_flow_in, booToRea.y) annotation (Line(points={{-62,7.77156e-16},
+          {-70,7.77156e-16},{-70,0},{-78,0}}, color={0,0,127}));
+    annotation(
+   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateWithTank.mos"
+        "Simulate and plot"),
+   experiment(Tolerance=1e-6, StopTime=86400.0),
+        Documentation(info="<html>
+<p>
+This example shows how several different models can be combined to create
+an entire solar water heating system.
+The
+<a href=\"modelica://AixLib.Fluid.Storage.StratifiedEnhancedInternalHex\">
+AixLib.Fluid.Storage.StratifiedEnhancedInternalHex</a> (tan) model is
+used to represent the tank filled with hot water.
+A loop, powered by a pump
+(<a href=\"modelica://AixLib.Fluid.Movers.FlowControlled_m_flow\">
+AixLib.Fluid.Movers.FlowControlled_m_flow</a>, pum), 
+passes the water through an expansion tank
+(<a href=\"modelica://AixLib.Fluid.Storage.ExpansionVessel\">
+AixLib.Fluid.Storage.ExpansionVessel</a>, exp),
+a temperature sensor
+(<a href=\"modelica://AixLib.Fluid.Sensors.TemperatureTwoPort\">
+AixLib.Fluid.Sensors.TemperatureTwoPort</a>, TIn),
+the solar collector
+(<a href=\"modelica://AixLib.Fluid.SolarCollectors.ASHRAE93\">
+AixLib.Fluid.SolarCollectors.ASHRAE93,</a> solCol),
+and a second temperature sensor
+(<a href=\"modelica://AixLib.Fluid.Sensors.TemperatureTwoPort\">
+AixLib.Fluid.Sensors.TemperatureTwoPort</a>, TOut)
+before re-entering the tank.
+</p>
+<p>
+The solar collector is connected to the weather model
+(<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>, weaDat) which passes
+information for the San Francisco, CA, USA climate.
+This information is used to identify both the heat gain in the water 
+from the sun and the heat loss to the ambient conditions.
+</p>
+<p>
+The flow rate through the pump is controlled by a solar pump controller model
+(<a href=\"modelica://AixLib.Fluid.SolarCollectors.Controls.CollectorPump\">
+AixLib.Fluid.SolarCollectors.Controls.CollectorPump</a>, pumCon)
+and a gain model.
+The controller outputs a binary on (1) / off (0) signal.
+The on/off signal is passed through a boolean to real signal converter 
+to set the pump mass flow rate.
+</p>
+<p>
+The heat ports for the tank are connected to an ambient temperature of 
+20 degrees C representing the temperature of the room the tank is stored in.
+</p>
+<p>
+bou1 (<a href=\"modelica://AixLib.Fluid.Sources.MassFlowSource_T\">
+AixLib.Fluid.Sources.MassFlowSource_T)</a> provides a constant mass flow
+rate for a hot water draw while bou
+(<a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT)</a> 
+provides a boundary condition for the outlet of the draw.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+November 7, 2022, by Michael Wetter:<br/>
+Revised example to provide values for new parameters and to integrate the revised solar pump controller.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3074\">issue 3074</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+April 18, 2014, by Michael Wetter:<br/>
+Updated model to use the revised tank and increased the tank height.
+</li>
+<li>
+March 25, 2014, by Michael Wetter:<br/>
+Updated model with new expansion vessel.
+</li>
+<li>
+March 27, 2013 by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-200,-100},{180,100}})),
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end FlatPlateWithTank;
diff --git a/AixLib/Fluid/SolarCollectors/Examples/Tubular.mo b/AixLib/Fluid/SolarCollectors/Examples/Tubular.mo
new file mode 100644
index 0000000000..b5dd9d8a4f
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Examples/Tubular.mo
@@ -0,0 +1,128 @@
+within AixLib.Fluid.SolarCollectors.Examples;
+model Tubular "Example showing the use of Tubular"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Water "Medium in the system";
+  AixLib.Fluid.SolarCollectors.ASHRAE93 solCol(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    use_shaCoe_in=false,
+    per=AixLib.Fluid.SolarCollectors.Data.Tubular.T_AMKCollectraAGOWR20(),
+    nPanels=10,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Parallel,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    rho=0.2,
+    nSeg=9,
+    azi=0.3,
+    til=0.5) "Tubular solar collector model"
+             annotation (Placement(transformation(extent={{10,-10},{30,10}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+    Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data input file"
+    annotation (Placement(transformation(extent={{-20,60},{0,80}})));
+  AixLib.Fluid.Sources.Boundary_pT sin(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Inlet for fluid flow" annotation (Placement(transformation(extent={{90,-10},
+            {70,10}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TOut(
+    redeclare package Medium = Medium,
+    T_start(displayUnit="K"),
+    m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort TIn(redeclare package Medium =
+    Medium, m_flow_nominal=solCol.m_flow_nominal) "Temperature sensor"
+    annotation (Placement(transformation(extent={{-20,-10},{0,10}})));
+  Modelica.Blocks.Sources.Sine sine(
+    f=3/86400,
+    offset=101325,
+    amplitude=-0.1*solCol.dp_nominal)
+    annotation (Placement(transformation(extent={{-80,-18},{-60,2}})));
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    T=273.15 + 10,
+    nPorts=1,
+    use_p_in=true,
+    p(displayUnit="Pa")) "Inlet for water flow"
+    annotation (Placement(
+        transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=180,
+        origin={-40,0})));
+equation
+  connect(solCol.port_b,TOut. port_a) annotation (Line(
+      points={{30,0},{40,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TOut.port_b,sin. ports[1]) annotation (Line(
+      points={{60,0},{70,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(TIn.port_b,solCol. port_a) annotation (Line(
+      points={{0,0},{10,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(weaDat.weaBus, solCol.weaBus) annotation (Line(
+      points={{0,70},{10,70},{10,8}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(sine.y, sou.p_in) annotation (Line(
+      points={{-59,-8},{-52,-8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou.ports[1], TIn.port_a) annotation (Line(
+      points={{-30,0},{-20,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  annotation (__Dymola_Commands(file=
+    "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/Tubular.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=86400.0),
+    Documentation(info="<html>
+<p>
+  This example models a tubular solar thermal collector. It uses the
+  <a href=\"modelica://AixLib.Fluid.SolarCollectors.ASHRAE93\">
+  AixLib.Fluid.SolarCollectors.ASHRAE93</a> model and references
+  data in the <a href=\"modelica://AixLib.Fluid.SolarCollectors.Data.Tubular\">
+  AixLib.Fluid.SolarCollectors.Data.Tubular</a> package.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+December 11, 2023, by Michael Wetter:<br/>
+Changed design flow rate. This is due to correction for the
+implementation of the pressure drop calculation for the situation where collectors are in parallel,
+e.g., if <code>sysConfig == AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Parallel</code>.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3597\">Buildings, #3597</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+March 27, 2013 by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Tubular;
diff --git a/AixLib/Fluid/SolarCollectors/Examples/package.mo b/AixLib/Fluid/SolarCollectors/Examples/package.mo
new file mode 100644
index 0000000000..d294e5880f
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Examples/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Fluid.SolarCollectors;
+package Examples "Examples demonstrating the use of models in the SolarCollectors package"
+  extends Modelica.Icons.ExamplesPackage;
+
+
+
+
+
+
+
+
+
+
+  annotation(Documentation(info="<html>
+    <p>
+      This package contains example model demonstrating the use of models in
+      the SolarCollectors package.
+    </p>
+  </html>"));
+end Examples;
diff --git a/AixLib/Fluid/SolarCollectors/Examples/package.order b/AixLib/Fluid/SolarCollectors/Examples/package.order
new file mode 100644
index 0000000000..6a925c587c
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Examples/package.order
@@ -0,0 +1,5 @@
+FlatPlate
+FlatPlateShaCoeTrue
+FlatPlateTotalArea
+FlatPlateWithTank
+Tubular
diff --git a/AixLib/Fluid/SolarCollectors/Types/HeatCapacity.mo b/AixLib/Fluid/SolarCollectors/Types/HeatCapacity.mo
new file mode 100644
index 0000000000..ab61adab9a
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Types/HeatCapacity.mo
@@ -0,0 +1,15 @@
+within AixLib.Fluid.SolarCollectors.Types;
+type HeatCapacity = enumeration(
+    TotalCapacity
+      "Total thermal capacity of the solar collector (i.e. including fluid)",
+    DryCapacity
+      "Dry thermal capacity and fluid volume of the solar collector",
+    DryMass
+      "Dry mass and fluid volume of the solar collector")
+  "Enumeration to define how the heat capacity of the solar collector is calculated"
+  annotation(Documentation(info="<html>
+<p>
+Enumeration used to define the different types of solar collector capacity specification.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Types/NumberSelection.mo b/AixLib/Fluid/SolarCollectors/Types/NumberSelection.mo
new file mode 100644
index 0000000000..e966af87a0
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Types/NumberSelection.mo
@@ -0,0 +1,12 @@
+within AixLib.Fluid.SolarCollectors.Types;
+type NumberSelection = enumeration(
+    Number "Number of panels",
+    Area "Total panel area") "Enumeration of options for how users will specify
+      the number of solar collectors in a system"
+  annotation(Documentation(info="<html>
+<p>
+Enumeration used to define the different methods of declaring solar thermal
+system size.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Types/SystemConfiguration.mo b/AixLib/Fluid/SolarCollectors/Types/SystemConfiguration.mo
new file mode 100644
index 0000000000..d9e4f4d9c8
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Types/SystemConfiguration.mo
@@ -0,0 +1,13 @@
+within AixLib.Fluid.SolarCollectors.Types;
+type SystemConfiguration = enumeration(
+    Parallel "Panels connected in parallel",
+    Series "Panels connected in series",
+    Array "Rectangular array of panels")
+  "Enumeration of options for how the panels are connected"
+  annotation(Documentation(info="<html>
+<p>
+Enumeration used to define the different configurations of
+solar thermal systems.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Fluid/SolarCollectors/Types/package.mo b/AixLib/Fluid/SolarCollectors/Types/package.mo
new file mode 100644
index 0000000000..da04bed7c3
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Types/package.mo
@@ -0,0 +1,10 @@
+within AixLib.Fluid.SolarCollectors;
+package Types "Package with type definitions used in solar collector data records"
+  extends Modelica.Icons.TypesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+  <p>
+    This package contains type definitions used in solar thermal collector models.
+  </p>
+</html>"));
+end Types;
diff --git a/AixLib/Fluid/SolarCollectors/Types/package.order b/AixLib/Fluid/SolarCollectors/Types/package.order
new file mode 100644
index 0000000000..a75bffc197
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Types/package.order
@@ -0,0 +1,3 @@
+HeatCapacity
+NumberSelection
+SystemConfiguration
diff --git a/AixLib/Fluid/SolarCollectors/UsersGuide.mo b/AixLib/Fluid/SolarCollectors/UsersGuide.mo
new file mode 100644
index 0000000000..c0ccb924cb
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/UsersGuide.mo
@@ -0,0 +1,234 @@
+within AixLib.Fluid.SolarCollectors;
+package UsersGuide "User's Guide"
+  extends Modelica.Icons.Information;
+  annotation(preferredView="info",
+  Documentation(info="<html>
+<p>
+This package contains models for solar thermal systems.
+Top-level models are available for solar thermal collectors based on the
+ASHRAE93 (American) and EN12975 (European) test protocols.
+The two models use different models for solar gain, heat loss, and use
+different data packages.
+The model applied to (un)glazed flat-plate solar thermal collectors, as well as
+evacuated tube collectors.
+</p>
+
+<h4>Model description</h4>
+<p>
+The solar thermal collector model is developed based on the
+flat-plate solar thermal collector model of EnergyPlus.
+The model determines the solar heat gain and heat loss of the collector
+seperately, and the difference of both is transferred to the collector.
+The ASHRAE93 and EN12975 collector model calculate the heat gain and heat loss
+differently.
+The details of these calculations can be found in
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.BaseClasses\">
+AixLib.Fluid.SolarCollectors.BaseClasses</a>.
+Accordingly, data records for both test methods are available in
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.Data\">
+AixLib.Fluid.SolarCollectors.Data</a>.
+</p>
+
+<h5>Performance data</h5>
+<p>
+Different sources exist to find ratings data of individual collectors.
+However, not all data might be available in one single data sheet.
+The table below specifies which input data of the model can be found in several
+well-known data sources:
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr>
+<th>Input data</th>
+<th> <a href=\"http://www.solar-rating.org\"> SRCC</a> </th>
+<th> <a href=\"https://solarkeymark.eu/\"> Solar Keymark</a> </th>
+<th> <a href=\"https://www.spftesting.info/\"> SPF</a> </th>
+</tr>
+<tr>
+<td> A </td>
+<td> Gross area </td>
+<td> Gross area </td>
+<td> Gross, aperture, or absorber area </td>
+</tr>
+<tr>
+<td> C </td>
+<td> (mDry*385, V) </td>
+<td> C </td>
+<td> (CDry or mDry*385, V) </td>
+</tr>
+<tr>
+<td> mperA_flow_nominal </td>
+<td> mperA_flow_nominal </td>
+<td> mperA_flow_nominal </td>
+<td> m_flow_nominal/A </td>
+</tr>
+<tr>
+<td> dp_nominal </td>
+<td> / </td>
+<td> / </td>
+<td> dp_nominal </td>
+</tr>
+<tr>
+<td> incAngDat, incAngModDat </td>
+<td> IAM({0°,10°,...,90°}) </td>
+<td> IAM({10°,20°,...,90°}) </td>
+<td> IAM(angle)-plot </td>
+</tr>
+<tr>
+<td> y_intercept, slope (ASHRAE93) </td>
+<td> y_intercept, slope </td>
+<td> / </td>
+<td> / </td>
+</tr>
+<tr>
+<td> IAMDiff, eta0, a1, a2 (EN12975) </td>
+<td> IAM(50°), eta0, a1, a2 </td>
+<td> Kd or IAM(50°), eta0, a1, a2 </td>
+<td> IAM(50°), eta0, a1, a2 </td>
+</tr>
+</table>
+<p>
+Some extra important remarks regarding the performance data:
+</p>
+<ul>
+<li>
+Different areas can be defined for a solar collector: the gross, absorber, and
+aperture area.
+The performance parameters of the solar collector vary depending on the area
+for which they are defined.
+Therefore, the performance parameters used in the data record should match the
+area that is used.
+</li>
+<li>
+When the thermal capacity of the solar collector without fluid is not known,
+the thermal capacity is calculated based on the dry mass of the collector
+and the specific heat capacity of copper (<i>385 J/kg/K</i>).
+</li>
+<li>
+All data sources report a nominal mass flow rate (per unit area of collector),
+but only SPF reports a corresponding nominal pressure drop.
+If a specific collector is used that is not included in the SPF database, one
+can likely find this via the manufacturer (website or on request).
+Some examples of (<code>mperA_flow_nominal</code>, <code>dp_nominal</code> can
+be found in <a href=\"modelica://AixLib.Fluid.SolarCollectors.Data\">
+AixLib.Fluid.SolarCollectors.BaseClasses</a>.
+</li>
+<li>
+Pressure drops depend on the medium that is used in the collectors.
+If the modelled solar thermal collector uses a different medium than the medium
+that was used to determine the nominal pressure drop in a data sheet, one should
+therefore correctly take this into account (e.g. using an empirical correction
+factor).
+</li>
+<li>
+<p>
+The relation between the incidence angle modifier (IAM) and incidence angle
+<code>&theta;</code> is calculated using cubic splines and measurement data
+provided in the data sheets.
+</p>
+</li>
+<li>
+Evacuated tube collectors have bi-axial IAMs due to its axisymetric geometry.
+Therefore, data sheets report both a longitudinal and transversal IAM.
+The model however only allows the definition of one (symmetrical) IAM.
+Two possible approaches to deal with this are:
+<ul>
+<li>
+multiplying the longitudinal and transversal IAM;
+</li>
+<li>
+using either the longitudinal or transversal IAM.
+</li>
+</ul>
+The model should therefore be used with care when dealing with
+evacuated tube collectors.
+</li>
+<li>
+The Solar Keymark database sometimes reports a value for <i>Kd</i> which is
+the incident angle modifier for diffuse irradiance.
+This value differs from the IAM at an incidence angle of 50 degrees because
+the former is determined by integrating the values of the IAM
+for all incidence angles over the hemisphere.
+</li>
+</ul>
+
+<h5> Other model parameters </h5>
+<p>
+Apart from the performance parameters, several other parameters must be defined.
+Most of the parameters are self-explanatory.
+The complex parameters are used as follows:
+</p>
+<ul>
+<li>
+<code>nSeg</code>: This parameter refers to the number of segments between
+the inlet and outlet of the system, not the number of segments in each solar
+thermal collector.
+</li>
+<li>
+<code>nColType</code>: This parameter allows the user to specify how the
+number of collectors in the system is defined. Options are
+<code>Number</code>, allowing the user to enter a number of panels, or
+<code>TotalArea</code>, allowing the user to enter a system area.
+<ul>
+<li>
+<code>Number</code>: If <code>Number</code> is selected for
+<code>nColType</code> the user enters a number of panels. The simulation then
+identifies the area of the system and uses that in solar gain and heat loss
+computations.
+</li>
+<li>
+<code>TotalArea</code>: If <code>TotalArea</code> is selected for
+<code>nColType</code> the user enters a desired surface area of panels. The
+model then uses this specified area in solar gain and heat loss computations.
+The number of panels in the system is identified by dividing the specified
+area by the area of each panel.
+</li>
+</ul>
+</li>
+<li>
+<code>SysConfig</code>: This parameter allows the user to specify the
+installation configuration of the system. Options are <code>Series</code> and
+<code>Parallel</code>. The handling of <code>dp_nominal</code> is changed
+depending on the selection.
+<ul>
+<li>
+<code>Series</code>: If <code>Series</code> is selected it is assumed that all
+panels in the system are connected in series. As a result there is a pressure
+drop corresponding to <code>dp_nominal</code> for each panel and the effective
+<code>dp_nominal</code> for the system is <code>dp_nominal</code> *
+<code>nPanels</code>.
+</li>
+<li>
+<code>Parallel</code>: If <code>Parallel</code> is selected it is assumed that
+all panels in the system are connected in parallel. As a result the fluid
+flows through only a single panel and the <code>dp_nominal</code> for the
+system is <code>dp_nominal</code> specified in the collector data package if
+the collector field has a mass flow rate equal to
+<code>m_flow_nominal</code>.
+</li>
+<li>
+<code>Array</code>: If <code>Array</code> is selected it is assumed that the
+panels are mounted as a rectangular array with <code>nPanelsPar</code> rows,
+each having <code>nPanelsSer</code> panels in series. As a result there is a
+pressure drop corresponding to <code>dp_nominal</code> for each panel per row
+and the effective <code>dp_nominal</code> for the system is
+<code>dp_nominal</code> * <code>nPanelsSer</code>.
+</li>
+</ul>
+</li>
+</ul>
+
+<h4>References</h4>
+<p>
+ASHRAE 93-2010 -- Methods of Testing to Determine the Thermal Performance of
+Solar Collectors (ANSI approved).
+</p>
+<p>
+CEN 2022, European Standard 12975:2022, European Committee for Standardization.
+</p>
+<p>
+<a href=\"https://energyplus.net/assets/nrel_custom/pdfs/pdfs_v23.2.0/EngineeringReference.pdf\">
+EnergyPlus 23.2.0 Engineering Reference</a>.
+</p>
+</html>"));
+
+end UsersGuide;
diff --git a/AixLib/Fluid/SolarCollectors/Validation/EN12975NPanels.mo b/AixLib/Fluid/SolarCollectors/Validation/EN12975NPanels.mo
new file mode 100644
index 0000000000..e39d1fe6be
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Validation/EN12975NPanels.mo
@@ -0,0 +1,146 @@
+within AixLib.Fluid.SolarCollectors.Validation;
+model EN12975NPanels
+  "Validation model for collector according to EN12975 with different settings for nPanel"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Water "Medium in the system";
+
+  parameter Integer nPanels=10 "Number of panels";
+
+  AixLib.Fluid.SolarCollectors.EN12975 solCol(
+    redeclare package Medium = Medium,
+    per=datSolCol,
+    shaCoe=0,
+    azi=0,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    rho=0.2,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nPanels=1,
+    nSeg=30,
+    til=0.78539816339745)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{30,20},{50,40}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+        Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"),
+      computeWetBulbTemperature=false)
+    "Weather data file reader"
+    annotation (Placement(transformation(extent={{-40,60},{-20,80}})));
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{90,20},{70,40}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_m_flow_in=true,
+    use_T_in=false,
+    T=303.15) "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+
+  AixLib.Fluid.SolarCollectors.EN12975 solCol1(
+    redeclare package Medium = Medium,
+    per=datSolCol,
+    shaCoe=0,
+    azi=0,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    rho=0.2,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nSeg=30,
+    til=0.78539816339745,
+    nPanels=nPanels)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{30,-40},{50,-20}})));
+  AixLib.Fluid.Sources.Boundary_pT sou1(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{90,-40},{70,-20}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou1(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_m_flow_in=true,
+    use_T_in=false,
+    T=303.15) "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  Modelica.Blocks.Math.Gain gaiNPan(k=nPanels) "Gain for number of panels"
+    annotation (Placement(transformation(extent={{-50,-30},{-30,-10}})));
+  Modelica.Blocks.Sources.RealExpression difHeaGai(y=solCol.QGai[30].Q_flow -
+        solCol1.QGai[30].Q_flow/nPanels)
+    "Difference in heat gain at last panel between model with 1 and with 30 panels"
+    annotation (Placement(transformation(extent={{-70,-70},{-50,-50}})));
+  Modelica.Blocks.Sources.RealExpression difHeaLos(y=solCol.QLos[30].Q_flow -
+        solCol1.QLos[30].Q_flow/nPanels)
+    "Difference in heat loss at last panel between model with 1 and with 30 panels"
+    annotation (Placement(transformation(extent={{-70,-90},{-50,-70}})));
+  Modelica.Blocks.Sources.Constant m_flow_nominal(k=datSolCol.A*datSolCol.mperA_flow_nominal)
+    "Nominal flow rate for one panel"
+    annotation (Placement(transformation(extent={{-90,30},{-70,50}})));
+  parameter Data.GlazedFlatPlate.FP_VerificationModel datSolCol
+    annotation (Placement(transformation(extent={{60,60},{80,80}})));
+equation
+  connect(weaDat.weaBus, solCol1.weaBus) annotation (Line(
+      points={{-20,70},{20,70},{20,-22},{30,-22}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(bou1.ports[1], solCol1.port_a) annotation (Line(
+      points={{10,-30},{30,-30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(sou1.ports[1], solCol1.port_b) annotation (Line(
+      points={{70,-30},{50,-30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(gaiNPan.y, bou1.m_flow_in)
+    annotation (Line(points={{-29,-20},{-20,-20},{-20,-22},{-12,-22}},
+                                                   color={0,0,127}));
+  connect(solCol.port_a, bou.ports[1])
+    annotation (Line(points={{30,30},{10,30}},color={0,127,255}));
+  connect(solCol.port_b, sou.ports[1])
+    annotation (Line(points={{50,30},{70,30}}, color={0,127,255}));
+  connect(solCol.weaBus, weaDat.weaBus) annotation (Line(
+      points={{30,38},{20,38},{20,70},{-20,70}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(m_flow_nominal.y, bou.m_flow_in) annotation (Line(points={{-69,40},{
+          -20,40},{-20,38},{-12,38}},
+                                  color={0,0,127}));
+  connect(gaiNPan.u, m_flow_nominal.y) annotation (Line(points={{-52,-20},{-60,
+          -20},{-60,40},{-69,40}}, color={0,0,127}));
+  annotation (
+    Documentation(info="<html>
+<p>
+This model validates the solar collector model
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.EN12975\">
+AixLib.Fluid.SolarCollectors.EN12975</a>
+for the case
+where the number of panels is <i>1</i> for the instance <code>solCol</code>
+and <i>10</i> for the instance <code>solCol1</code>.
+The instances <code>difHeaGai</code> and <code>difHeaLos</code>
+compare the heat gain and heat loss between the two models.
+The output of these blocks should be zero, except for rounding errors.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+November 21, 2017, by Michael Wetter:<br/>
+First implementation to validate
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1073\">#1073</a>.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975NPanels.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=86400), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end EN12975NPanels;
diff --git a/AixLib/Fluid/SolarCollectors/Validation/EN12975_Array.mo b/AixLib/Fluid/SolarCollectors/Validation/EN12975_Array.mo
new file mode 100644
index 0000000000..db79f52859
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Validation/EN12975_Array.mo
@@ -0,0 +1,162 @@
+within AixLib.Fluid.SolarCollectors.Validation;
+model EN12975_Array
+  "Validation model for collector according to EN12975 in array configuration"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Water "Medium in the system";
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=solCol.per.A*
+      solCol.per.mperA_flow_nominal "Nominal mass flow rate";
+
+  model Collector
+    extends AixLib.Fluid.SolarCollectors.EN12975(
+    redeclare final package Medium = AixLib.Media.Water,
+    final show_T = true,
+    final per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_VerificationModel(),
+    final shaCoe=0,
+    final azi=0,
+    final energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    final rho=0.2,
+    final nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nPanels=1,
+    final til=0.78539816339745,
+    final use_shaCoe_in=false,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series);
+
+  end Collector;
+
+  Collector solCol(
+    nPanels=4,
+    nSeg=3,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Array,
+    nPanelsSer=2,
+    nPanelsPar=2)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{-20,20},{0,40}})));
+
+  Collector solCol1(nSeg=3, nPanels=2)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{-50,-40},{-30,-20}})));
+
+  Collector solCol2(nSeg=3, nPanels=2)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{-50,-80},{-30,-60}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+        Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"),
+      computeWetBulbTemperature=false)
+    "Weather data file reader"
+    annotation (Placement(transformation(extent={{-88,60},{-68,80}})));
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{80,20},{60,40}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_T_in=false,
+    m_flow=m_flow_nominal,
+    T=303.15) "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+
+  AixLib.Fluid.Sources.Boundary_pT sou1(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{80,-40},{60,-20}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou1(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_T_in=false,
+    m_flow=m_flow_nominal/2,
+    T=303.15) "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-80,-40},{-60,-20}})));
+
+  Sensors.TemperatureTwoPort senTem(
+     redeclare package Medium = Medium,
+     tau=0,
+     m_flow_nominal=m_flow_nominal)
+    "Temperature sensor"
+    annotation (Placement(transformation(extent={{20,40},{40,20}})));
+  Sensors.TemperatureTwoPort senTem1(
+    redeclare package Medium = Medium,
+    tau=0,
+    m_flow_nominal=m_flow_nominal)
+    "Temperature sensor"
+    annotation (Placement(transformation(extent={{20,-20},{40,-40}})));
+  Modelica.Blocks.Math.Add dT(final k2=-1) "Temperature difference (must be zero)"
+    annotation (Placement(transformation(extent={{60,-80},{80,-60}})));
+  Sources.MassFlowSource_T                 bou2(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_T_in=false,
+    m_flow=m_flow_nominal/2,
+    T=303.15) "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-80,-80},{-60,-60}})));
+equation
+  connect(weaDat.weaBus, solCol1.weaBus) annotation (Line(
+      points={{-68,70},{-50,70},{-50,-22}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(bou1.ports[1], solCol1.port_a) annotation (Line(
+      points={{-60,-30},{-50,-30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(solCol.port_a, bou.ports[1]) annotation (Line(points={{-20,30},{-60,30}},
+                           color={0,127,255}));
+  connect(solCol.weaBus, weaDat.weaBus) annotation (Line(
+      points={{-20,38},{-24,38},{-24,70},{-68,70}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(weaDat.weaBus, solCol2.weaBus) annotation (Line(
+      points={{-68,70},{-50,70},{-50,-62}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(solCol.port_b, senTem.port_a)
+    annotation (Line(points={{0,30},{20,30}}, color={0,127,255}));
+  connect(senTem.port_b, sou.ports[1])
+    annotation (Line(points={{40,30},{60,30}}, color={0,127,255}));
+  connect(sou1.ports[1], senTem1.port_b)
+    annotation (Line(points={{60,-30},{40,-30}}, color={0,127,255}));
+  connect(dT.u1, senTem.T) annotation (Line(points={{58,-64},{50,-64},{50,0},{30,
+          0},{30,19}},  color={0,0,127}));
+  connect(senTem1.T, dT.u2) annotation (Line(points={{30,-41},{30,-76},{58,-76}},
+                                       color={0,0,127}));
+  connect(bou2.ports[1], solCol2.port_a)
+    annotation (Line(points={{-60,-70},{-50,-70}}, color={0,127,255}));
+  connect(solCol1.port_b, senTem1.port_a)
+    annotation (Line(points={{-30,-30},{20,-30}}, color={0,127,255}));
+  connect(solCol2.port_b, senTem1.port_a) annotation (Line(points={{-30,-70},{-20,
+          -70},{-20,-30},{20,-30}}, color={0,127,255}));
+  annotation (
+    Documentation(info="<html>
+<p>
+This model validates the solar collector model
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.EN12975\">
+AixLib.Fluid.SolarCollectors.EN12975</a>
+for the case where one model has multiple panels in a 2x2 array,
+versus the case where two models are in parallel,
+each having two panels in series.
+The output of the block <code>dT</code> must be zero,
+as both cases must have the same outlet temperatures.
+Furthermore, the pressure drops over all models should be the same.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 27, 2024, by Jelger Jansen:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975_Array.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=86400), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end EN12975_Array;
diff --git a/AixLib/Fluid/SolarCollectors/Validation/EN12975_Series.mo b/AixLib/Fluid/SolarCollectors/Validation/EN12975_Series.mo
new file mode 100644
index 0000000000..52f7458814
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Validation/EN12975_Series.mo
@@ -0,0 +1,158 @@
+within AixLib.Fluid.SolarCollectors.Validation;
+model EN12975_Series
+  "Validation model for collector according to EN12975 with different panels in series"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Water "Medium in the system";
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal=solCol.per.A*
+      solCol.per.mperA_flow_nominal "Nominal mass flow rate";
+
+  model Collector
+    extends AixLib.Fluid.SolarCollectors.EN12975(
+    redeclare final package Medium = AixLib.Media.Water,
+    final show_T = true,
+    final per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_VerificationModel(),
+    final shaCoe=0,
+    final azi=0,
+    final energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    final rho=0.2,
+    final nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nPanels=1,
+    final til=0.78539816339745,
+    final use_shaCoe_in=false,
+    final sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series);
+
+  end Collector;
+
+  Collector solCol(nPanels=2, nSeg=6)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{-20,20},{0,40}})));
+
+  Collector solCol1(nSeg=3, nPanels=1)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{-50,-40},{-30,-20}})));
+
+  Collector solCol2(nSeg=3, nPanels=1)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{-20,-40},{0,-20}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+        Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"),
+      computeWetBulbTemperature=false)
+    "Weather data file reader"
+    annotation (Placement(transformation(extent={{-88,60},{-68,80}})));
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{80,20},{60,40}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_T_in=false,
+    m_flow=m_flow_nominal,
+    T=303.15) "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+
+  AixLib.Fluid.Sources.Boundary_pT sou1(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{80,-40},{60,-20}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou1(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_T_in=false,
+    m_flow=m_flow_nominal,
+    T=303.15) "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-80,-40},{-60,-20}})));
+
+  Sensors.TemperatureTwoPort senTem(
+     redeclare package Medium = Medium,
+     tau=0,
+     m_flow_nominal=m_flow_nominal)
+    "Temperature sensor"
+    annotation (Placement(transformation(extent={{20,40},{40,20}})));
+  Sensors.TemperatureTwoPort senTem1(
+    redeclare package Medium = Medium,
+    tau=0,
+    m_flow_nominal=m_flow_nominal)
+    "Temperature sensor"
+    annotation (Placement(transformation(extent={{20,-20},{40,-40}})));
+  Modelica.Blocks.Math.Add dT(final k2=-1) "Temperature difference (must be zero)"
+    annotation (Placement(transformation(extent={{60,-80},{80,-60}})));
+equation
+  connect(weaDat.weaBus, solCol1.weaBus) annotation (Line(
+      points={{-68,70},{-50,70},{-50,-22}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(bou1.ports[1], solCol1.port_a) annotation (Line(
+      points={{-60,-30},{-50,-30}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(solCol.port_a, bou.ports[1]) annotation (Line(points={{-20,30},{-60,30}},
+                           color={0,127,255}));
+  connect(solCol.weaBus, weaDat.weaBus) annotation (Line(
+      points={{-20,38},{-24,38},{-24,70},{-68,70}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(solCol2.port_a, solCol1.port_b)
+    annotation (Line(points={{-20,-30},{-30,-30}},
+                                                color={0,127,255}));
+  connect(weaDat.weaBus, solCol2.weaBus) annotation (Line(
+      points={{-68,70},{-24,70},{-24,-22},{-20,-22}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(solCol.port_b, senTem.port_a)
+    annotation (Line(points={{0,30},{20,30}}, color={0,127,255}));
+  connect(senTem.port_b, sou.ports[1])
+    annotation (Line(points={{40,30},{60,30}}, color={0,127,255}));
+  connect(sou1.ports[1], senTem1.port_b)
+    annotation (Line(points={{60,-30},{40,-30}}, color={0,127,255}));
+  connect(senTem1.port_a, solCol2.port_b)
+    annotation (Line(points={{20,-30},{0,-30}}, color={0,127,255}));
+  connect(dT.u1, senTem.T) annotation (Line(points={{58,-64},{50,-64},{50,0},{30,
+          0},{30,19}},  color={0,0,127}));
+  connect(senTem1.T, dT.u2) annotation (Line(points={{30,-41},{30,-76},{58,-76}},
+                                       color={0,0,127}));
+  annotation (
+    Documentation(info="<html>
+<p>
+This model validates the solar collector model
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.EN12975\">
+AixLib.Fluid.SolarCollectors.EN12975</a>
+for the case where one model has multiple panels in series,
+versus the case where two models are in series, each having one panel.
+The output of the block <code>dT</code> must be zero, as both
+cases must have the same outlet temperatures.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 15, 2024, by Jelger Jansen:<br/>
+Refactor model.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3604\">Buildings, #3604</a>.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+December 12, 2017, by Michael Wetter:<br/>
+First implementation to validate
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1100\">#1100</a>.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975_Series.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=86400), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end EN12975_Series;
diff --git a/AixLib/Fluid/SolarCollectors/Validation/ExtremeAmbientConditions.mo b/AixLib/Fluid/SolarCollectors/Validation/ExtremeAmbientConditions.mo
new file mode 100644
index 0000000000..b4306a3c61
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Validation/ExtremeAmbientConditions.mo
@@ -0,0 +1,220 @@
+within AixLib.Fluid.SolarCollectors.Validation;
+model ExtremeAmbientConditions
+  "Validation model for to ensure that collectors do not freeze or boil"
+  extends Modelica.Icons.Example;
+
+  replaceable package Medium = AixLib.Media.Water(T_min=273.15, T_max=273.15+100)
+    "Medium in the system";
+
+  ASHRAE93 solAsh(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    rho=0.2,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_GuangdongFSPTY95(),
+    nPanels=1,
+    azi=0.3,
+    til=0.5,
+    T_start=313.15) "Flat plate solar collector model using the ASHRAE model"
+    annotation (Placement(transformation(extent={{20,-50},{40,-30}})));
+  EN12975 solEn(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    rho=0.2,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    sysConfig=AixLib.Fluid.SolarCollectors.Types.SystemConfiguration.Series,
+    nPanels=1,
+    azi=0.3,
+    til=0.5,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_VerificationModel(),
+    T_start=313.15) "Flat plate solar collector model using the EN 12975 model"
+    annotation (Placement(transformation(extent={{20,-90},{40,-70}})));
+
+  Sources.MassFlowSource_T sou(
+    redeclare package Medium = Medium,
+    nPorts=1,
+    m_flow=0) "Inlet boundary conditions"
+    annotation (Placement(
+      transformation(
+      extent={{10,10},{-10,-10}},
+      rotation=180,
+      origin={-10,-40})));
+  Sources.Boundary_pT sou1(
+    redeclare package Medium = Medium,
+    p(displayUnit="Pa"),
+    use_p_in=false,
+    nPorts=2) "Inlet boundary conditions"
+    annotation (Placement(
+      transformation(
+      extent={{-10,10},{10,-10}},
+      rotation=180,
+      origin={80,-60})));
+  Modelica.Blocks.Sources.Ramp TAmb(
+    offset=273.15 + 40,
+    height=-100,
+    duration=10*3600) "Ambient temperature"
+    annotation (Placement(transformation(extent={{-80,90},{-60,110}})));
+  Modelica.Blocks.Sources.Ramp HSol(
+    duration=12*3600,
+    height=1000,
+    startTime=10*3600) "Solar irradiation"
+    annotation (Placement(transformation(extent={{-80,60},{-60,80}})));
+
+  Sources.MassFlowSource_T sou2(
+    redeclare package Medium = Medium,
+    nPorts=1,
+    m_flow=0) "Inlet boundary conditions"
+    annotation (Placement(
+      transformation(
+      extent={{10,10},{-10,-10}},
+      rotation=180,
+      origin={-10,-80})));
+  BoundaryConditions.WeatherData.Bus weaBus annotation (Placement(
+        transformation(extent={{-10,-10},{10,10}}),iconTransformation(extent={{-154,
+            16},{-134,36}})));
+  Modelica.Blocks.Sources.Constant const(k=0) "Constant that outputs zero"
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  Modelica.Blocks.Sources.Constant solTim(k=12*3600) "Solar time"
+    annotation (Placement(transformation(extent={{-80,-50},{-60,-30}})));
+  Modelica.Blocks.Sources.Constant lat(k=0.656593) "Location latitude"
+    annotation (Placement(transformation(extent={{-80,-80},{-60,-60}})));
+  Modelica.Blocks.Sources.Constant alt(k=2) "Location altitude"
+    annotation (Placement(transformation(extent={{-80,-110},{-60,-90}})));
+  Modelica.Blocks.Sources.Constant const1(k=0)
+                                              "Constant that outputs zero"
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+equation
+  connect(sou.ports[1], solAsh.port_a)
+    annotation (Line(points={{1.77636e-15,-40},{20,-40}}, color={0,127,255}));
+  connect(sou2.ports[1], solEn.port_a)
+    annotation (Line(points={{1.77636e-15,-80},{20,-80}}, color={0,127,255}));
+  connect(solAsh.port_b, sou1.ports[1])
+    annotation (Line(points={{40,-40},{70,-40},{70,-61}},
+                                                       color={0,127,255}));
+  connect(solEn.port_b, sou1.ports[2]) annotation (Line(points={{40,-80},{70,
+          -80},{70,-59}},     color={0,127,255}));
+  connect(weaBus, solAsh.weaBus) annotation (Line(
+      points={{0,0},{16,0},{16,-32},{20,-32}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      textString="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}}));
+  connect(TAmb.y, weaBus.TDryBul) annotation (Line(points={{-59,100},{0,100},{0,
+          50},{0.05,50},{0.05,0.05}},
+                      color={0,0,127}), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(HSol.y, weaBus.HDifHor) annotation (Line(points={{-59,70},{-28,70},{-28,
+          0.05},{0.05,0.05}},
+                     color={0,0,127}), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(HSol.y, weaBus.HGloHor) annotation (Line(points={{-59,70},{-28,70},{-28,
+          0.05},{0.05,0.05}},
+                     color={0,0,127}), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(const.y, weaBus.solZen) annotation (Line(points={{-59,30},{-28,30},{-28,
+          0.05},{0.05,0.05}},
+                     color={0,0,127}), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(solTim.y, weaBus.solTim) annotation (Line(points={{-59,-40},{-28,-40},
+          {-28,0.05},{0.05,0.05}},
+                          color={0,0,127}), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(HSol.y, weaBus.HDirNor) annotation (Line(points={{-59,70},{-28,70},{-28,
+          0.05},{0.05,0.05}},
+                     color={0,0,127}), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(solEn.weaBus, weaBus) annotation (Line(
+      points={{20,-72},{16,-72},{16,0},{0,0}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      textString="%second",
+      index=1,
+      extent={{6,3},{6,3}}));
+  connect(lat.y, weaBus.lat) annotation (Line(points={{-59,-70},{-28,-70},{-28,0.05},
+          {0.05,0.05}},
+                     color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(alt.y, weaBus.alt) annotation (Line(points={{-59,-100},{-28,-100},{-28,
+          0.05},{0.05,0.05}},
+                     color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(const1.y, weaBus.cloTim) annotation (Line(points={{-59,-10},{-28,-10},
+          {-28,0.05},{0.05,0.05}}, color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  annotation (
+    Documentation(info="<html>
+<p>
+This model validates the correct implementation of the heat transfer
+to the collector when ambient temperatures are very low or irradiation is very
+large.
+It applies a ramp boundary condition that reduces the ambient temperature
+to <i>-60</i>&deg;C to verify that the collector fluid temperature does not
+drop below <code>Medium.T_min</code>.
+Afterwards, the solar irradiation is increased to overheat the collector.
+If the fluid temperature approaches <code>Medium.T_max</code>,
+then the solar heat gain is reduced to zero.
+Ensuring these bounds is important as otherwise, the collector model
+would trigger an assertion and the simulation would stop.
+The tested collector models are
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.ASHRAE93\">
+AixLib.Fluid.SolarCollectors.ASHRAE93</a>
+and
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.EN12975\">
+AixLib.Fluid.SolarCollectors.EN12975</a>.
+</p>
+<p>
+Note that the medium has been declared
+as <code>AixLib.Media.Water(T_min=273.15, T_max=273.15+100)</code>
+to set the two bounds for the water temperature.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+September 25, 2023, by Michael Wetter:<br/>
+Corrected <code>connect</code> statement with wrong quantity.
+</li>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+June 30, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/ExtremeAmbientConditions.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-06, StopTime=86400),
+    Diagram(coordinateSystem(extent={{-100,-120},{100,120}})),
+    Icon(coordinateSystem(extent={{-100,-120},{100,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ExtremeAmbientConditions;
diff --git a/AixLib/Fluid/SolarCollectors/Validation/FlatPlate.mo b/AixLib/Fluid/SolarCollectors/Validation/FlatPlate.mo
new file mode 100644
index 0000000000..f59df25dca
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Validation/FlatPlate.mo
@@ -0,0 +1,135 @@
+within AixLib.Fluid.SolarCollectors.Validation;
+model FlatPlate "Validation model for FlatPlate"
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Water "Medium in the system";
+  AixLib.Fluid.SolarCollectors.ASHRAE93
+   solCol(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    azi=0,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_TRNSYSValidation(),
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    rho=0.2,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nPanels=1,
+    nSeg=30,
+    til=0.78539816339745)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{30,-10},{50,10}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+    Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"),
+      computeWetBulbTemperature=false)
+    "Weather data file reader"
+    annotation (Placement(transformation(extent={{-40,60},{-20,80}})));
+  AixLib.Fluid.Sources.Boundary_pT sou(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{90,-10},{70,10}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_m_flow_in=true,
+    use_T_in=true)
+    "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  Modelica.Blocks.Math.Add add
+    "Converts TRNSYS data from degree Celsius to Kelving"
+    annotation (Placement(transformation(extent={{-50,0},{-30,20}})));
+  Modelica.Blocks.Sources.CombiTimeTable datRea(
+    tableOnFile=true,
+    tableName="TRNSYS",
+    columns=2:5,
+    fileName=Modelica.Utilities.Files.loadResource(
+       "modelica://AixLib/Resources/Data/Fluid/SolarCollectors/Validation/FlatPlate/TRNSYSAnnualData.txt"),
+    smoothness=Modelica.Blocks.Types.Smoothness.ConstantSegments)
+    "Data reader with inlet conditions from TRNSYS"
+    annotation (Placement(transformation(extent={{-90,20},{-70,40}})));
+
+  Modelica.Blocks.Sources.Constant const(k=273.15)
+    "Used to convert TRNSYS data from degree Celsius to Kelving"
+    annotation (Placement(transformation(extent={{-90,-40},{-70,-20}})));
+
+equation
+  connect(weaDat.weaBus, solCol.weaBus) annotation (Line(
+      points={{-20,70},{20,70},{20,8},{30,8}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(bou.ports[1], solCol.port_a)      annotation (Line(
+      points={{10,0},{30,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(const.y, add.u2) annotation (Line(
+      points={{-69,-30},{-60,-30},{-60,4},{-52,4}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(add.y, bou.T_in)      annotation (Line(
+      points={{-29,10},{-24,10},{-24,4},{-12,4}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(datRea.y[1], add.u1)        annotation (Line(
+      points={{-69,30},{-60,30},{-60,16},{-52,16}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(datRea.y[4], bou.m_flow_in)             annotation (Line(
+      points={{-69,30},{-20,30},{-20,8},{-12,8}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou.ports[1], solCol.port_b) annotation (Line(
+      points={{70,0},{50,0}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  annotation (
+    Documentation(info="<html>
+<p>
+This model was used to validate the
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.ASHRAE93\">
+AixLib.Fluid.SolarCollectors.ASHRAE93</a> solar collector model
+against TRNSYS data. Data files are used to ensure that the
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.ASHRAE93\">
+AixLib.Fluid.SolarCollectors.ASHRAE93</a> solar collector model and
+the TRNSYS model use the same inlet and weather conditions. The
+solar collector model must reference the
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_TRNSYSValidation\">
+AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_TRNSYSValidation</a>
+data record when comparing model results to the stored TRNSYS results.
+</p>
+<p>
+The solar collector temperature of the Modelica model has a spike
+in the morning. At this time, there is solar irradiation on the collector
+but no mass flow rate, which leads to an increase in temperature.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+April 21, 2016, by Michael Wetter:<br/>
+Replaced <code>ModelicaServices.ExternalReferences.loadResource</code> with
+<code>Modelica.Utilities.Files.loadResource</code>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+March 27, 2013, by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/FlatPlate.mos"
+    "Simulate and plot"),
+  experiment(Tolerance=1e-6, StopTime=86400), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end FlatPlate;
diff --git a/AixLib/Fluid/SolarCollectors/Validation/FlatPlateNPanels.mo b/AixLib/Fluid/SolarCollectors/Validation/FlatPlateNPanels.mo
new file mode 100644
index 0000000000..6ba75b9db2
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Validation/FlatPlateNPanels.mo
@@ -0,0 +1,99 @@
+within AixLib.Fluid.SolarCollectors.Validation;
+model FlatPlateNPanels
+  "Validation model for flat plate collector with different settings for nPanel"
+  extends AixLib.Fluid.SolarCollectors.Validation.FlatPlate;
+  parameter Integer nPanels = 10 "Number of panels";
+  AixLib.Fluid.SolarCollectors.ASHRAE93
+   solCol1(
+    redeclare package Medium = Medium,
+    shaCoe=0,
+    azi=0,
+    per=AixLib.Fluid.SolarCollectors.Data.GlazedFlatPlate.FP_TRNSYSValidation(),
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    rho=0.2,
+    nColType=AixLib.Fluid.SolarCollectors.Types.NumberSelection.Number,
+    nSeg=30,
+    til=0.78539816339745,
+    nPanels=nPanels)
+    "Flat plate solar collector model, has been modified for validation purposes"
+    annotation (Placement(transformation(extent={{30,-50},{50,-30}})));
+  AixLib.Fluid.Sources.Boundary_pT sou1(
+    redeclare package Medium = Medium,
+    use_p_in=false,
+    p(displayUnit="Pa") = 101325,
+    nPorts=1) "Outlet for water flow"
+    annotation (Placement(transformation(extent={{90,-50},{70,-30}})));
+  AixLib.Fluid.Sources.MassFlowSource_T bou1(
+    nPorts=1,
+    redeclare package Medium = Medium,
+    use_m_flow_in=true,
+    use_T_in=true)
+    "Inlet for water flow, at a prescribed flow rate and temperature"
+    annotation (Placement(transformation(extent={{-10,-50},{10,-30}})));
+  Modelica.Blocks.Math.Gain gaiNPan(k=nPanels) "Gain for number of panels"
+    annotation (Placement(transformation(extent={{-50,-30},{-30,-10}})));
+  Modelica.Blocks.Sources.RealExpression difHeaGai(y=solCol.QGai[30].Q_flow -
+        solCol1.QGai[30].Q_flow/nPanels)
+    "Difference in heat gain at last panel between model with 1 and with 30 panels"
+    annotation (Placement(transformation(extent={{-70,-70},{-50,-50}})));
+  Modelica.Blocks.Sources.RealExpression difHeaLos(y=solCol.QLos[30].Q_flow -
+        solCol1.QLos[30].Q_flow/nPanels)
+    "Difference in heat loss at last panel between model with 1 and with 30 panels"
+    annotation (Placement(transformation(extent={{-70,-90},{-50,-70}})));
+equation
+  connect(weaDat.weaBus, solCol1.weaBus) annotation (Line(
+      points={{-20,70},{20,70},{20,-32},{30,-32}},
+      color={255,204,51},
+      thickness=0.5,
+      smooth=Smooth.None));
+  connect(bou1.ports[1], solCol1.port_a) annotation (Line(
+      points={{10,-40},{30,-40}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(add.y, bou1.T_in) annotation (Line(
+      points={{-29,10},{-24,10},{-24,-36},{-12,-36}},
+      color={0,0,127},
+      smooth=Smooth.None));
+  connect(sou1.ports[1], solCol1.port_b) annotation (Line(
+      points={{70,-40},{50,-40}},
+      color={0,127,255},
+      smooth=Smooth.None));
+  connect(gaiNPan.y, bou1.m_flow_in)
+    annotation (Line(points={{-29,-20},{-20,-20},{-20,-32},{-12,-32}},
+                                                   color={0,0,127}));
+  connect(gaiNPan.u, datRea.y[4]) annotation (Line(points={{-52,-20},{-64,-20},
+          {-64,30},{-69,30}},color={0,0,127}));
+  annotation (
+    Documentation(info="<html>
+<p>
+This model validates the solar collector model
+<a href=\"modelica://AixLib.Fluid.SolarCollectors.ASHRAE93\">
+AixLib.Fluid.SolarCollectors.ASHRAE93</a>
+for the case
+where the number of panels is <i>1</i> for the instance <code>solCol</code>
+and <i>10</i> for the instance <code>solCol1</code>.
+The instances <code>difHeaGai</code> and <code>difHeaLos</code>
+compare the heat gain and heat loss between the two models.
+The output of these blocks should be zero, except for rounding errors.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+September 16, 2021, by Michael Wetter:<br/>
+Removed parameter assignment for <code>lat</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+November 21, 2017, by Michael Wetter:<br/>
+First implementation to validate
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1073\">#1073</a>.
+</li>
+</ul>
+</html>"),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/FlatPlateNPanels.mos"
+    "Simulate and plot"),
+  experiment(Tolerance=1e-6, StopTime=86400), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end FlatPlateNPanels;
diff --git a/AixLib/Fluid/SolarCollectors/Validation/package.mo b/AixLib/Fluid/SolarCollectors/Validation/package.mo
new file mode 100644
index 0000000000..d27a88be83
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Validation/package.mo
@@ -0,0 +1,20 @@
+within AixLib.Fluid.SolarCollectors;
+package Validation "Collection of validation models"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains validation models for the classes in
+<a href=\"modelica://AixLib.Fluid.SolarCollectors\">
+AixLib.Fluid.SolarCollectors</a>.
+</p>
+<p>
+Note that most validation models contain simple input data
+which may not be realistic, but for which the correct
+output can be obtained through an analytic solution.
+The examples plot various outputs, which have been verified against these
+solutions. These model outputs are stored as reference data and
+used for continuous validation whenever models in the library change.
+</p>
+</html>"));
+end Validation;
diff --git a/AixLib/Fluid/SolarCollectors/Validation/package.order b/AixLib/Fluid/SolarCollectors/Validation/package.order
new file mode 100644
index 0000000000..72f0e83363
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/Validation/package.order
@@ -0,0 +1,6 @@
+EN12975NPanels
+EN12975_Array
+EN12975_Series
+ExtremeAmbientConditions
+FlatPlate
+FlatPlateNPanels
diff --git a/AixLib/Fluid/SolarCollectors/package.mo b/AixLib/Fluid/SolarCollectors/package.mo
new file mode 100644
index 0000000000..54a8c89986
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/package.mo
@@ -0,0 +1,18 @@
+within AixLib.Fluid;
+package SolarCollectors "Package with models for solar collectors"
+  extends Modelica.Icons.Package;
+
+  annotation (
+    Documentation(info = "<html>
+  This package contains models which can be used to simulate solar thermal
+  systems and examples describing their use.
+  </html>"),
+    Icon(
+      graphics={
+        Polygon(origin = {14, -34}, fillColor = {136, 138, 133}, pattern = LinePattern.None, fillPattern = FillPattern.Solid,
+          points = {{-70, -20}, {-32, -48}, {74, 28}, {30, 48}, {-70, -20}}),
+        Ellipse(origin = {-59, 59}, fillColor = {255, 255, 255}, fillPattern = FillPattern.Solid, extent = {{-19, 19}, {19, -19}}),
+        Line(origin = {-20.0398, 44.6215}, points = {{-16, 8}, {26, -4}}),
+        Line(origin = {-48.3585, 20.4861}, points = {{-6, 16}, {0, -18}}),
+        Line(origin = {-35.6812, 25.8008}, points = {{-6, 16}, {14, -12}})}));
+end SolarCollectors;
diff --git a/AixLib/Fluid/SolarCollectors/package.order b/AixLib/Fluid/SolarCollectors/package.order
new file mode 100644
index 0000000000..0b4645fa88
--- /dev/null
+++ b/AixLib/Fluid/SolarCollectors/package.order
@@ -0,0 +1,9 @@
+UsersGuide
+ASHRAE93
+EN12975
+Controls
+Data
+Types
+Examples
+Validation
+BaseClasses
diff --git a/AixLib/Fluid/Sources/BaseClasses/Outside.mo b/AixLib/Fluid/Sources/BaseClasses/Outside.mo
index ec4823fab0..4130cffe8a 100644
--- a/AixLib/Fluid/Sources/BaseClasses/Outside.mo
+++ b/AixLib/Fluid/Sources/BaseClasses/Outside.mo
@@ -1,11 +1,11 @@
 within AixLib.Fluid.Sources.BaseClasses;
 partial model Outside
   "Boundary that takes weather data, and optionally trace substances, as an input"
-  extends AixLib.Fluid.Sources.BaseClasses.PartialSource(final verifyInputs=true);
+  extends AixLib.Fluid.Sources.BaseClasses.PartialAirSource(final verifyInputs=true);
 
   parameter Boolean use_C_in = false
     "Get the trace substances from the input connector"
-    annotation(Evaluate=true, HideResult=true);
+    annotation(Evaluate=true);
   parameter Medium.ExtraProperty C[Medium.nC](
     final quantity=Medium.extraPropertiesNames)=fill(0, Medium.nC)
     "Fixed values of trace substances"
@@ -108,77 +108,89 @@ equation
           textColor={255,255,255},
           textString=DynamicSelect("", String(weaBus.TDryBul-273.15, format=".1f")))}),
     Documentation(info="<html>
- <p>
- This is the base class for models that describes boundary conditions for
- pressure, enthalpy, and species concentration that can be obtained
- from weather data, and that may be modified based on the wind pressure.
- </p>
- <p>If the parameter <code>use_C_in</code> is <code>false</code> (default option),
- the <code>C</code> parameter
- is used as the trace substance for flow that leaves the component, and the
- <code>C_in</code> input connector is disabled; if <code>use_C_in</code> is <code>true</code>,
- then the <code>C</code> parameter is ignored, and the value provided by the input connector is used instead.</p>
- <p>
- Note that boundary temperature,
- mass fractions and trace substances have only an effect if the mass flow
- is from the boundary into the port. If mass is flowing from
- the port into the boundary, the boundary definitions,
- with exception of boundary pressure, do not have an effect.
- </p>
- </html>",
+<p>
+This is the base class for models that describes boundary conditions for
+pressure, enthalpy, and species concentration that can be obtained
+from weather data, and that may be modified based on the wind pressure.
+</p>
+<p>If the parameter <code>use_C_in</code> is <code>false</code> (default option),
+the <code>C</code> parameter
+is used as the trace substance for flow that leaves the component, and the
+<code>C_in</code> input connector is disabled; if <code>use_C_in</code> is <code>true</code>,
+then the <code>C</code> parameter is ignored, and the value provided by the input connector is used instead.</p>
+<p>
+Note that boundary temperature,
+mass fractions and trace substances have only an effect if the mass flow
+is from the boundary into the port. If mass is flowing from
+the port into the boundary, the boundary definitions,
+with exception of boundary pressure, do not have an effect.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- November 14, 2019, by Michael Wetter:<br/>
- Removed duplicate connector.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1248\"> #1248</a>.
- </li>
- <li>
- January 14, 2019 by Jianjun Hu:<br/>
- Changed to extend <a href=\"modelica://AixLib.Fluid.Sources.BaseClasses.PartialSource\">
- AixLib.Fluid.Sources.BaseClasses.PartialSource</a>. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\"> #1050</a>.
- </li>
- <li>
- May 30, 2017 by Jianjun Hu:<br/>
- Corrected <code>X_in_internal = zeros()</code> to be <code>X_in_internal = ones()</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/787\"> #787</a>.
- </li>
- <li>
- April, 25, 2016 by Marcus Fuchs:<br/>
- Introduced missing <code>each</code> keyword. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/454\"> #454</a>,
- to prevent a warning in OpenModelica.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>unit</code> and <code>quantity</code> attributes.
- </li>
- <li>
- May 30, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- October 26, 2011 by Michael Wetter:<br/>
- Introduced new base class to allow implementation of wind pressure for natural ventilation.
- </li>
- <li>
- April 27, 2011 by Michael Wetter:<br/>
- Revised implementation to allow medium model that do not have water vapor.
- </li>
- <li>
- Feb. 9, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+January 09, 2023, by Jianjun Hu:<br/>
+Changed base class to constrain medium to moist air.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1681\">IBPSA, #1681</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+November 14, 2019, by Michael Wetter:<br/>
+Removed duplicate connector.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1248\"> #1248</a>.
+</li>
+<li>
+January 14, 2019 by Jianjun Hu:<br/>
+Changed to extend <a href=\"modelica://AixLib.Fluid.Sources.BaseClasses.PartialSource\">
+AixLib.Fluid.Sources.BaseClasses.PartialSource</a>. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\"> #1050</a>.
+</li>
+<li>
+May 30, 2017 by Jianjun Hu:<br/>
+Corrected <code>X_in_internal = zeros()</code> to be <code>X_in_internal = ones()</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/787\"> #787</a>.
+</li>
+<li>
+April, 25, 2016 by Marcus Fuchs:<br/>
+Introduced missing <code>each</code> keyword. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/454\"> #454</a>,
+to prevent a warning in OpenModelica.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>unit</code> and <code>quantity</code> attributes.
+</li>
+<li>
+May 30, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+October 26, 2011 by Michael Wetter:<br/>
+Introduced new base class to allow implementation of wind pressure for natural ventilation.
+</li>
+<li>
+April 27, 2011 by Michael Wetter:<br/>
+Revised implementation to allow medium model that do not have water vapor.
+</li>
+<li>
+Feb. 9, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside;
diff --git a/AixLib/Fluid/Sources/BaseClasses/PartialAirSource.mo b/AixLib/Fluid/Sources/BaseClasses/PartialAirSource.mo
new file mode 100644
index 0000000000..4417c63db8
--- /dev/null
+++ b/AixLib/Fluid/Sources/BaseClasses/PartialAirSource.mo
@@ -0,0 +1,101 @@
+within AixLib.Fluid.Sources.BaseClasses;
+partial model PartialAirSource
+  "Partial component air source with one fluid connector"
+
+  replaceable package Medium =
+    Modelica.Media.Interfaces.PartialMedium "Medium in the component"
+      annotation (choices(
+        choice(redeclare package Medium = AixLib.Media.Air "Moist air")));
+
+  parameter Integer nPorts=0 "Number of ports" annotation(Dialog(connectorSizing=true));
+  parameter Boolean verifyInputs = false
+    "Set to true to stop the simulation with an error if the medium temperature is outside its allowable range"
+    annotation(Evaluate=true, Dialog(tab="Advanced"));
+
+  Modelica.Fluid.Interfaces.FluidPorts_b ports[nPorts](
+    redeclare each package Medium = Medium,
+    each m_flow(max=if flowDirection == Modelica.Fluid.Types.PortFlowDirection.Leaving
+                    then 0 else +Modelica.Constants.inf,
+                min=if flowDirection == Modelica.Fluid.Types.PortFlowDirection.Entering
+                    then 0 else -Modelica.Constants.inf),
+    each h_outflow(nominal=Medium.h_default),
+    each Xi_outflow(each nominal=0.01))
+    "Fluid ports"
+    annotation (Placement(transformation(extent={{90,40},{110,-40}})));
+
+protected
+  parameter Modelica.Fluid.Types.PortFlowDirection flowDirection=Modelica.Fluid.Types.PortFlowDirection.Bidirectional
+    "Allowed flow direction" annotation (Evaluate=true, Dialog(tab="Advanced"));
+  Modelica.Blocks.Interfaces.RealInput p_in_internal(final unit="Pa")
+    "Needed to connect to conditional connector";
+  Medium.BaseProperties medium(
+      T(start=Medium.T_default)
+    ) if verifyInputs "Medium in the source";
+  Modelica.Blocks.Interfaces.RealInput Xi_in_internal[Medium.nXi](
+    each final unit = "kg/kg")
+    "Needed to connect to conditional connector";
+  Modelica.Blocks.Interfaces.RealInput X_in_internal[Medium.nX](
+    each final unit = "kg/kg")
+    "Needed to connect to conditional connector";
+  Modelica.Blocks.Interfaces.RealInput C_in_internal[Medium.nC](
+    final quantity=Medium.extraPropertiesNames)
+    "Needed to connect to conditional connector";
+
+initial equation
+  // Only one connection allowed to a port to avoid unwanted ideal mixing
+  for i in 1:nPorts loop
+    assert(cardinality(ports[i]) <= 1,"
+Each ports[i] of boundary shall at most be connected to one component.
+If two or more connections are present, ideal mixing takes
+place in these connections, which is usually not the intention
+of the modeller. Increase nPorts to add an additional port.
+");
+  end for;
+
+equation
+  connect(medium.p, p_in_internal);
+
+  annotation (defaultComponentName="bou",
+  Documentation(info="<html>
+<p>
+Partial model for a moist air source that either prescribes
+pressure or mass flow rate.
+Models that extend this partial model need to prescribe the outflowing
+specific enthalpy, composition and trace substances.
+This partial model only declares the <code>ports</code>
+and ensures that the pressures at all ports are equal.
+</p>
+<h4>Implementation</h4>
+<p>
+If the parameter <code>verifyInputs</code> is set to <code>true</code>,
+then a protected instance of medium base properties is enabled.
+This instance verifies that the
+medium temperature is within the bounds <code>T_min</code> and <code>T_max</code>,
+where <code>T_min</code> and <code>T_max</code> are constants of the <code>Medium</code>.
+If the temperature is outside these bounds, the simulation will stop with an error.
+</p>
+<h4>Usage</h4>
+<p>
+This partial model provides medium selection for moist air.
+For a model that only provides for water, moist air and glycol as a selection, use
+<a href=\"modelica://AixLib.Fluid.Sources.BaseClasses.PartialSource\">
+AixLib.Fluid.Sources.BaseClasses.PartialSource</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+January 09, 2023, by Jianjun Hu:<br/>
+First implementation, specifically for the moist air source.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1681\">IBPSA, #1681</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialAirSource;
diff --git a/AixLib/Fluid/Sources/BaseClasses/PartialPropertySource.mo b/AixLib/Fluid/Sources/BaseClasses/PartialPropertySource.mo
index 32efb66122..d581300001 100644
--- a/AixLib/Fluid/Sources/BaseClasses/PartialPropertySource.mo
+++ b/AixLib/Fluid/Sources/BaseClasses/PartialPropertySource.mo
@@ -102,32 +102,32 @@ equation
           fillPattern=FillPattern.HorizontalCylinder,
           fillColor={0,127,255})}),
     Documentation(info="<html>
- <p>
- Model that changes the properties, 
- but not the mass flow rate,
- of the fluid that passes through it.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- If <code>allowFlowReversal=true</code>, then the properties are changed for both flow directions,
- i.e., from <code>port_a</code> to <code>port_b</code> and
- from <code>port_b</code> to <code>port_a</code>.
- </p>
- <h4>Dynamics</h4>
- <p>
- This model has no dynamics.
- </p>
- </html>",
+<p>
+Model that changes the properties, 
+but not the mass flow rate,
+of the fluid that passes through it.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+If <code>allowFlowReversal=true</code>, then the properties are changed for both flow directions,
+i.e., from <code>port_a</code> to <code>port_b</code> and
+from <code>port_b</code> to <code>port_a</code>.
+</p>
+<h4>Dynamics</h4>
+<p>
+This model has no dynamics.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 30, 2018, by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 30, 2018, by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{
-            100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialPropertySource;
diff --git a/AixLib/Fluid/Sources/BaseClasses/PartialSource.mo b/AixLib/Fluid/Sources/BaseClasses/PartialSource.mo
index 1ff0dd59ff..265597c756 100644
--- a/AixLib/Fluid/Sources/BaseClasses/PartialSource.mo
+++ b/AixLib/Fluid/Sources/BaseClasses/PartialSource.mo
@@ -23,7 +23,9 @@ partial model PartialSource
     each m_flow(max=if flowDirection == Modelica.Fluid.Types.PortFlowDirection.Leaving
                     then 0 else +Modelica.Constants.inf,
                 min=if flowDirection == Modelica.Fluid.Types.PortFlowDirection.Entering
-                    then 0 else -Modelica.Constants.inf))
+                    then 0 else -Modelica.Constants.inf),
+    each h_outflow(nominal=Medium.h_default),
+    each Xi_outflow(each nominal=0.01))
     "Fluid ports"
     annotation (Placement(transformation(extent={{90,40},{110,-40}})));
 
@@ -48,11 +50,11 @@ initial equation
   // Only one connection allowed to a port to avoid unwanted ideal mixing
   for i in 1:nPorts loop
     assert(cardinality(ports[i]) <= 1,"
- Each ports[i] of boundary shall at most be connected to one component.
- If two or more connections are present, ideal mixing takes
- place in these connections, which is usually not the intention
- of the modeller. Increase nPorts to add an additional port.
- ");
+Each ports[i] of boundary shall at most be connected to one component.
+If two or more connections are present, ideal mixing takes
+place in these connections, which is usually not the intention
+of the modeller. Increase nPorts to add an additional port.
+");
   end for;
 
 equation
@@ -60,45 +62,58 @@ equation
 
   annotation (defaultComponentName="bou",
   Documentation(info="<html>
- <p>
- Partial model for a fluid source that either prescribes
- pressure or mass flow rate.
- Models that extend this partial model need to prescribe the outflowing
- specific enthalpy, composition and trace substances.
- This partial model only declares the <code>ports</code>
- and ensures that the pressures at all ports are equal.
- </p>
- <h4>Implementation</h4>
- <p>
- If the parameter <code>verifyInputs</code> is set to <code>true</code>,
- then a protected instance of medium base properties is enabled.
- This instance verifies that the
- medium temperature is within the bounds <code>T_min</code> and <code>T_max</code>,
- where <code>T_min</code> and <code>T_max</code> are constants of the <code>Medium</code>.
- If the temperature is outside these bounds, the simulation will stop with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 1, 2021, by Michael Wetter:<br/>
- Corrected misplaced <code>each</code> and added missing instance comment.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1462\">IBPSA, #1462</a>.
- </li>
- <li>
- January 18, 2019, by Jianjun Hu:<br/>
- Limited the media choice.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">IBPSA, #1050</a>.
- </li>
- <li>
- May 30, 2018, by Michael Wetter:<br/>
- Improved documentation.
- </li>
- <li>
- February 2nd, 2018 by Filip Jorissen<br/>
- Initial version for refactoring inputs of sources.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">IBPSA, #882</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model for a fluid source that either prescribes
+pressure or mass flow rate.
+Models that extend this partial model need to prescribe the outflowing
+specific enthalpy, composition and trace substances.
+This partial model only declares the <code>ports</code>
+and ensures that the pressures at all ports are equal.
+</p>
+<h4>Implementation</h4>
+<p>
+If the parameter <code>verifyInputs</code> is set to <code>true</code>,
+then a protected instance of medium base properties is enabled.
+This instance verifies that the
+medium temperature is within the bounds <code>T_min</code> and <code>T_max</code>,
+where <code>T_min</code> and <code>T_max</code> are constants of the <code>Medium</code>.
+If the temperature is outside these bounds, the simulation will stop with an error.
+</p>
+<h4>Usage</h4>
+<p>
+This partial model provides medium selection for water, moist air and glycol.
+For a model that only provides moist air as a selection, use
+<a href=\"modelica://AixLib.Fluid.Sources.BaseClasses.PartialAirSource\">
+AixLib.Fluid.Sources.BaseClasses.PartialAirSource</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+April 1, 2021, by Michael Wetter:<br/>
+Corrected misplaced <code>each</code> and added missing instance comment.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1462\">IBPSA, #1462</a>.
+</li>
+<li>
+January 18, 2019, by Jianjun Hu:<br/>
+Limited the media choice.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">IBPSA, #1050</a>.
+</li>
+<li>
+May 30, 2018, by Michael Wetter:<br/>
+Improved documentation.
+</li>
+<li>
+February 2nd, 2018 by Filip Jorissen<br/>
+Initial version for refactoring inputs of sources.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">IBPSA, #882</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialSource;
diff --git a/AixLib/Fluid/Sources/BaseClasses/PartialSource_Xi_C.mo b/AixLib/Fluid/Sources/BaseClasses/PartialSource_Xi_C.mo
index 53f424f09f..0323cf0169 100644
--- a/AixLib/Fluid/Sources/BaseClasses/PartialSource_Xi_C.mo
+++ b/AixLib/Fluid/Sources/BaseClasses/PartialSource_Xi_C.mo
@@ -5,13 +5,13 @@ partial model PartialSource_Xi_C
 
   parameter Boolean use_X_in = false
     "Get the composition (all fractions) from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(tab="Advanced"));
+    annotation(Evaluate=true, Dialog(tab="Advanced"));
   parameter Boolean use_Xi_in = false
     "Get the composition (independent fractions) from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Boolean use_C_in = false
     "Get the trace substances from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Medium.MassFraction X[Medium.nX](
     final quantity=Medium.substanceNames) = Medium.X_default
     "Fixed value of composition"
@@ -111,36 +111,42 @@ equation
           fillPattern=FillPattern.Solid,
           textString="C")}),
           Documentation(info="<html>
- <p>
- Partial model that defines outflowing properties
- <code>ports.Xi_outflow</code> and <code>ports.C_outflow</code>
- using an optional input for both.
- Otherwise the parameter value is used.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 19, 2019, by Michael Wetter:<br/>
- Refactored handling of mass fractions which was needed to handle media such as
- <a href=\"modelica://Modelica.Media.IdealGases.MixtureGases.FlueGasSixComponents\">
- Modelica.Media.IdealGases.MixtureGases.FlueGasSixComponents</a> and
- <a href=\"modelica://Modelica.Media.IdealGases.MixtureGases.SimpleNaturalGas\">
- Modelica.Media.IdealGases.MixtureGases.SimpleNaturalGas</a>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
- </li>
- <li>
- February 13, 2018, by Michael Wetter:<br/>
- Corrected error in quantity assignment for <code>Xi_in</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
- </li>
- <li>
- February 2nd, 2018 by Filip Jorissen<br/>
- Initial version for refactoring inputs of sources.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Partial model that defines outflowing properties
+<code>ports.Xi_outflow</code> and <code>ports.C_outflow</code>
+using an optional input for both.
+Otherwise the parameter value is used.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+September 19, 2019, by Michael Wetter:<br/>
+Refactored handling of mass fractions which was needed to handle media such as
+<a href=\"modelica://Modelica.Media.IdealGases.MixtureGases.FlueGasSixComponents\">
+Modelica.Media.IdealGases.MixtureGases.FlueGasSixComponents</a> and
+<a href=\"modelica://Modelica.Media.IdealGases.MixtureGases.SimpleNaturalGas\">
+Modelica.Media.IdealGases.MixtureGases.SimpleNaturalGas</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
+</li>
+<li>
+February 13, 2018, by Michael Wetter:<br/>
+Corrected error in quantity assignment for <code>Xi_in</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
+</li>
+<li>
+February 2nd, 2018 by Filip Jorissen<br/>
+Initial version for refactoring inputs of sources.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialSource_Xi_C;
diff --git a/AixLib/Fluid/Sources/BaseClasses/package.order b/AixLib/Fluid/Sources/BaseClasses/package.order
index 1d1d51704f..761832f71a 100644
--- a/AixLib/Fluid/Sources/BaseClasses/package.order
+++ b/AixLib/Fluid/Sources/BaseClasses/package.order
@@ -1,4 +1,5 @@
 Outside
+PartialAirSource
 PartialPropertySource
 PartialSource
 PartialSource_Xi_C
diff --git a/AixLib/Fluid/Sources/Boundary_pT.mo b/AixLib/Fluid/Sources/Boundary_pT.mo
index 21a5d4c5c0..d2061f36e9 100644
--- a/AixLib/Fluid/Sources/Boundary_pT.mo
+++ b/AixLib/Fluid/Sources/Boundary_pT.mo
@@ -5,14 +5,14 @@ model Boundary_pT
 
   parameter Boolean use_p_in = false
     "Get the pressure from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Medium.AbsolutePressure p = Medium.p_default
     "Fixed value of pressure"
     annotation (Dialog(enable = not use_p_in, group="Fixed inputs"));
 
   parameter Boolean use_T_in= false
     "Get the temperature from the input connector"
-    annotation(Evaluate=true, HideResult=true,Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Medium.Temperature T = Medium.T_default
     "Fixed value of temperature"
     annotation (Dialog(enable = not use_T_in,group="Fixed inputs"));
@@ -82,101 +82,107 @@ equation
   connect(medium.h, h_internal);
   annotation (defaultComponentName="bou",
     Documentation(info="<html>
- <p>
- Defines prescribed values for boundary conditions:
- </p>
- <ul>
- <li> Prescribed boundary pressure.</li>
- <li> Prescribed boundary temperature.</li>
- <li> Boundary composition (only for multi-substance or trace-substance flow).</li>
- </ul>
- <h4>Typical use and important parameters</h4>
- <p>
- If <code>use_p_in</code> is false (default option),
- the <code>p</code> parameter is used as boundary pressure,
- and the <code>p_in</code> input connector is disabled;
- if <code>use_p_in</code> is true, then the <code>p</code>
- parameter is ignored, and the value provided by the
- input connector is used instead.
- </p>
- <p>
- The same applies to the temperature <i>T</i>, composition <i>X<sub>i</sub></i> or <i>X</i> and trace substances <i>C</i>.
- </p>
- <h4>Options</h4>
- <p>
- Instead of using <code>Xi_in</code> (the <i>independent</i> composition fractions),
- the advanced tab provides an option for setting all
- composition fractions using <code>X_in</code>.
- <code>use_X_in</code> and <code>use_Xi_in</code> cannot be used
- at the same time.
- </p>
- <p>
- Parameter <code>verifyInputs</code> can be set to <code>true</code>
- to enable a check that verifies the validity of the used temperatures
- and pressures.
- This removes the corresponding overhead from the model, which is
- a substantial part of the overhead of this model.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>
- for more information.
- </p>
- <p>
- Note, that boundary temperature,
- mass fractions and trace substances have only an effect if the mass flow
- is from the boundary into the port. If mass is flowing from
- the port into the boundary, the boundary definitions,
- with exception of boundary pressure, do not have an effect.
- </p>
- </html>",
+<p>
+Defines prescribed values for boundary conditions:
+</p>
+<ul>
+<li> Prescribed boundary pressure.</li>
+<li> Prescribed boundary temperature.</li>
+<li> Boundary composition (only for multi-substance or trace-substance flow).</li>
+</ul>
+<h4>Typical use and important parameters</h4>
+<p>
+If <code>use_p_in</code> is false (default option),
+the <code>p</code> parameter is used as boundary pressure,
+and the <code>p_in</code> input connector is disabled;
+if <code>use_p_in</code> is true, then the <code>p</code>
+parameter is ignored, and the value provided by the
+input connector is used instead.
+</p>
+<p>
+The same applies to the temperature <i>T</i>, composition <i>X<sub>i</sub></i> or <i>X</i> and trace substances <i>C</i>.
+</p>
+<h4>Options</h4>
+<p>
+Instead of using <code>Xi_in</code> (the <i>independent</i> composition fractions),
+the advanced tab provides an option for setting all
+composition fractions using <code>X_in</code>.
+<code>use_X_in</code> and <code>use_Xi_in</code> cannot be used
+at the same time.
+</p>
+<p>
+Parameter <code>verifyInputs</code> can be set to <code>true</code>
+to enable a check that verifies the validity of the used temperatures
+and pressures.
+This removes the corresponding overhead from the model, which is
+a substantial part of the overhead of this model.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>
+for more information.
+</p>
+<p>
+Note, that boundary temperature,
+mass fractions and trace substances have only an effect if the mass flow
+is from the boundary into the port. If mass is flowing from
+the port into the boundary, the boundary definitions,
+with exception of boundary pressure, do not have an effect.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 25, 2020, by Michael Wetter:<br/>
- Changed icon to display its operating state.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
- </li>
- <li>
- Juni 7, 2019, by Michael Wetter:<br/>
- Added constant boolean expressions to avoid a potential string comparison in an equation section.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1148\">#1148</a>.
- </li>
- <li>
- Juni 4, 2019, by Filip Jorissen:<br/>
- Added check for the value of <code>p</code> and <code>p_in</code>.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1148\">#1148</a>.
- </li>
- <li>
- January 25, 2019, by Michael Wetter:<br/>
- Refactored use of base classes.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\">#1072</a>.
- </li>
- <li>
- February 2nd, 2018 by Filip Jorissen<br/>
- Made <code>medium</code> conditional and refactored inputs.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
- </li>
- <li>
- April 18, 2017, by Filip Jorissen:<br/>
- Changed <code>checkBoundary</code> implementation
- such that it is run as an initial equation
- when it depends on parameters only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/728\">#728</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>unit</code> and <code>quantity</code> attributes.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- Implementation is based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+February 25, 2020, by Michael Wetter:<br/>
+Changed icon to display its operating state.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1294\">#1294</a>.
+</li>
+<li>
+Juni 7, 2019, by Michael Wetter:<br/>
+Added constant boolean expressions to avoid a potential string comparison in an equation section.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1148\">#1148</a>.
+</li>
+<li>
+Juni 4, 2019, by Filip Jorissen:<br/>
+Added check for the value of <code>p</code> and <code>p_in</code>.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1148\">#1148</a>.
+</li>
+<li>
+January 25, 2019, by Michael Wetter:<br/>
+Refactored use of base classes.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\">#1072</a>.
+</li>
+<li>
+February 2nd, 2018 by Filip Jorissen<br/>
+Made <code>medium</code> conditional and refactored inputs.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
+</li>
+<li>
+April 18, 2017, by Filip Jorissen:<br/>
+Changed <code>checkBoundary</code> implementation
+such that it is run as an initial equation
+when it depends on parameters only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/728\">#728</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>unit</code> and <code>quantity</code> attributes.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+Implementation is based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Text(
           visible=use_p_in,
@@ -206,6 +212,6 @@ revisions="<html>
         Text(
           extent={{62,28},{-58,-22}},
           textColor={255,255,255},
-          textString=DynamicSelect("", String((if use_T_in then T_in else T)-273.15, format=".1f")))}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString=DynamicSelect("", String((if use_T_in then T_in else T)-273.15, format=".1f")))}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Boundary_pT;
diff --git a/AixLib/Fluid/Sources/Boundary_ph.mo b/AixLib/Fluid/Sources/Boundary_ph.mo
index ab5a0b06ef..7a8a24a0fb 100644
--- a/AixLib/Fluid/Sources/Boundary_ph.mo
+++ b/AixLib/Fluid/Sources/Boundary_ph.mo
@@ -5,14 +5,14 @@ model Boundary_ph
 
   parameter Boolean use_p_in = false
     "Get the pressure from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Medium.AbsolutePressure p = Medium.p_default
     "Fixed value of pressure"
     annotation (Dialog(enable = not use_p_in, group="Fixed inputs"));
 
   parameter Boolean use_h_in= false
     "Get the specific enthalpy from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Medium.SpecificEnthalpy h = Medium.h_default
     "Fixed value of specific enthalpy"
     annotation (Dialog(enable = not use_h_in, group="Fixed inputs"));
@@ -77,95 +77,101 @@ equation
 
   annotation (defaultComponentName="bou",
     Documentation(info="<html>
- <p>
- Defines prescribed values for boundary conditions:
- </p>
- <ul>
- <li> Prescribed boundary pressure.</li>
- <li> Prescribed boundary specific enthalpy.</li>
- <li> Boundary composition (only for multi-substance or trace-substance flow).</li>
- </ul>
- <h4>Typical use and important parameters</h4>
- <p>
- If <code>use_p_in</code> is false (default option),
- the <code>p</code> parameter is used as boundary pressure,
- and the <code>p_in</code> input connector is disabled;
- if <code>use_p_in</code> is true, then the <code>p</code>
- parameter is ignored, and the value provided by the
- input connector is used instead.
- </p>
- <p>
- The same applies to the specific enthalpy <i>h</i>, composition <i>X<sub>i</sub></i> or <i>X</i> and trace substances <i>C</i>.
- </p>
- <h4>Options</h4>
- <p>
- Instead of using <code>Xi_in</code> (the <i>independent</i> composition fractions),
- the advanced tab provides an option for setting all
- composition fractions using <code>X_in</code>.
- <code>use_X_in</code> and <code>use_Xi_in</code> cannot be used
- at the same time.
- </p>
- <p>
- Parameter <code>verifyInputs</code> can be set to <code>true</code>
- to enable a check that verifies the validity of the used specific enthalpy
- and pressures.
- This removes the corresponding overhead from the model, which is
- a substantial part of the overhead of this model.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>
- for more information.
- </p>
- <p>
- Note, that boundary specific enthalpy,
- mass fractions and trace substances have only an effect if the mass flow
- is from the boundary into the port. If mass is flowing from
- the port into the boundary, the boundary definitions,
- with exception of boundary pressure, do not have an effect.
- </p>
- </html>",
+<p>
+Defines prescribed values for boundary conditions:
+</p>
+<ul>
+<li> Prescribed boundary pressure.</li>
+<li> Prescribed boundary specific enthalpy.</li>
+<li> Boundary composition (only for multi-substance or trace-substance flow).</li>
+</ul>
+<h4>Typical use and important parameters</h4>
+<p>
+If <code>use_p_in</code> is false (default option),
+the <code>p</code> parameter is used as boundary pressure,
+and the <code>p_in</code> input connector is disabled;
+if <code>use_p_in</code> is true, then the <code>p</code>
+parameter is ignored, and the value provided by the
+input connector is used instead.
+</p>
+<p>
+The same applies to the specific enthalpy <i>h</i>, composition <i>X<sub>i</sub></i> or <i>X</i> and trace substances <i>C</i>.
+</p>
+<h4>Options</h4>
+<p>
+Instead of using <code>Xi_in</code> (the <i>independent</i> composition fractions),
+the advanced tab provides an option for setting all
+composition fractions using <code>X_in</code>.
+<code>use_X_in</code> and <code>use_Xi_in</code> cannot be used
+at the same time.
+</p>
+<p>
+Parameter <code>verifyInputs</code> can be set to <code>true</code>
+to enable a check that verifies the validity of the used specific enthalpy
+and pressures.
+This removes the corresponding overhead from the model, which is
+a substantial part of the overhead of this model.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>
+for more information.
+</p>
+<p>
+Note, that boundary specific enthalpy,
+mass fractions and trace substances have only an effect if the mass flow
+is from the boundary into the port. If mass is flowing from
+the port into the boundary, the boundary definitions,
+with exception of boundary pressure, do not have an effect.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- Juni 7, 2019, by Michael Wetter:<br/>
- Added constant boolean expressions to avoid a potential string comparison in an equation section.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1148\">#1148</a>.
- </li>
- <li>
- Juni 4, 2019, by Filip Jorissen:<br/>
- Added check for the value of <code>p</code> and <code>p_in</code>.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1148\">#1148</a>.
- </li>
- <li>
- January 25, 2019, by Michael Wetter:<br/>
- Refactored use of base classes.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\">#1072</a>.
- </li>
- <li>
- February 2nd, 2018 by Filip Jorissen<br/>
- Made <code>medium</code> conditional and refactored inputs.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
- </li>
- <li>
- April 18, 2017, by Filip Jorissen:<br/>
- Changed <code>checkBoundary</code> implementation
- such that it is run as an initial equation
- when it depends on parameters only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/728\">#728</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>unit</code> and <code>quantity</code> attributes.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- Implementation is based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+Juni 7, 2019, by Michael Wetter:<br/>
+Added constant boolean expressions to avoid a potential string comparison in an equation section.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1148\">#1148</a>.
+</li>
+<li>
+Juni 4, 2019, by Filip Jorissen:<br/>
+Added check for the value of <code>p</code> and <code>p_in</code>.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1148\">#1148</a>.
+</li>
+<li>
+January 25, 2019, by Michael Wetter:<br/>
+Refactored use of base classes.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\">#1072</a>.
+</li>
+<li>
+February 2nd, 2018 by Filip Jorissen<br/>
+Made <code>medium</code> conditional and refactored inputs.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
+</li>
+<li>
+April 18, 2017, by Filip Jorissen:<br/>
+Changed <code>checkBoundary</code> implementation
+such that it is run as an initial equation
+when it depends on parameters only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/728\">#728</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>unit</code> and <code>quantity</code> attributes.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+Implementation is based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Text(
           visible=use_h_in,
@@ -189,6 +195,6 @@ revisions="<html>
         Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Boundary_ph;
diff --git a/AixLib/Fluid/Sources/Examples/MassFlowSource_WeatherData.mo b/AixLib/Fluid/Sources/Examples/MassFlowSource_WeatherData.mo
index 240755ac81..a48193b8f9 100644
--- a/AixLib/Fluid/Sources/Examples/MassFlowSource_WeatherData.mo
+++ b/AixLib/Fluid/Sources/Examples/MassFlowSource_WeatherData.mo
@@ -11,7 +11,7 @@ model MassFlowSource_WeatherData
     redeclare package Medium = Medium,
     m_flow=-1,
     nPorts=1) "Mass flow source model receiving h and X from weather data through
-      weather bus"
+     weather bus"
     annotation (Placement(transformation(extent={{96,-10},{76,10}})));
   AixLib.Fluid.Sources.Outside bou(redeclare package Medium = Medium, nPorts=1)
     "Model with outside conditions"
@@ -50,20 +50,20 @@ experiment(Tolerance=1e-6, StopTime=3.1536e+07),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/MassFlowSource_WeatherData.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates how to connect fluid flow components to a
- boundary condition that has environmental conditions as
- obtained from a weather file.
- The model draws a constant mass flow rate of outside air through
- its components.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 21, 2017 by Jianjun Hu:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model demonstrates how to connect fluid flow components to a
+boundary condition that has environmental conditions as
+obtained from a weather file.
+The model draws a constant mass flow rate of outside air through
+its components.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 21, 2017 by Jianjun Hu:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFlowSource_WeatherData;
diff --git a/AixLib/Fluid/Sources/Examples/Outside.mo b/AixLib/Fluid/Sources/Examples/Outside.mo
index 79b0851dbb..a04654fed6 100644
--- a/AixLib/Fluid/Sources/Examples/Outside.mo
+++ b/AixLib/Fluid/Sources/Examples/Outside.mo
@@ -54,20 +54,20 @@ experiment(Tolerance=1e-6, StopTime=3.1536e+07),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates how to connect fluid flow component to a
- boundary condition that has environmental conditions as
- obtained from a weather file.
- The model draws a constant mass flow rate of outside air through
- its components.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- Feb. 9, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model demonstrates how to connect fluid flow component to a
+boundary condition that has environmental conditions as
+obtained from a weather file.
+The model draws a constant mass flow rate of outside air through
+its components.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Feb. 9, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside;
diff --git a/AixLib/Fluid/Sources/Examples/Outside_CpData.mo b/AixLib/Fluid/Sources/Examples/Outside_CpData.mo
index 0124a35c1d..de303a6872 100644
--- a/AixLib/Fluid/Sources/Examples/Outside_CpData.mo
+++ b/AixLib/Fluid/Sources/Examples/Outside_CpData.mo
@@ -60,32 +60,32 @@ equation
   annotation (__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates the use of a source for ambient conditions that computes
- the wind pressure on a facade of a building using a user-defined wind pressure profile.
- Weather data are used for San Francisco, for a period of a week
- where the wind blows primarily from North-West.
- The plot shows that the wind pressure on the north- and west-facing
- facade is positive,
- whereas it is negative for the south- and east-facing facades.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Jun 28, 2021 by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the use of a source for ambient conditions that computes
+the wind pressure on a facade of a building using a user-defined wind pressure profile.
+Weather data are used for San Francisco, for a period of a week
+where the wind blows primarily from North-West.
+The plot shows that the wind pressure on the north- and west-facing
+facade is positive,
+whereas it is negative for the south- and east-facing facades.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Jun 28, 2021 by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StartTime=1.728e+07,
       StopTime=1.78848e+07,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside_CpData;
diff --git a/AixLib/Fluid/Sources/Examples/Outside_CpData_Angles.mo b/AixLib/Fluid/Sources/Examples/Outside_CpData_Angles.mo
index 30a504df66..d08968684f 100644
--- a/AixLib/Fluid/Sources/Examples/Outside_CpData_Angles.mo
+++ b/AixLib/Fluid/Sources/Examples/Outside_CpData_Angles.mo
@@ -77,35 +77,35 @@ equation
   annotation (__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData_Angles.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates the use of a source for ambient conditions that computes
- the wind pressure on a facade of a building using a user-defined wind pressure profile.
- </p>
- <p>
- The model showcases the possibility to use asymmetrical wind pressure profiles.
- It also shows how <i>C<sub>p,act</sub></i> shifts with regards to the wind direction and azimuth
- based on the <i>C<sub>p</sub></i> values which are defined relative to the surface normal.
- </p>
- <p>
- The plot shows <i>C<sub>p,act</sub></i> of each boundary for each wind direction.
- Notice how the profile is shifted based on the surface azimuth.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Jun 28, 2021 by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the use of a source for ambient conditions that computes
+the wind pressure on a facade of a building using a user-defined wind pressure profile.
+</p>
+<p>
+The model showcases the possibility to use asymmetrical wind pressure profiles.
+It also shows how <i>C<sub>p,act</sub></i> shifts with regards to the wind direction and azimuth
+based on the <i>C<sub>p</sub></i> values which are defined relative to the surface normal.
+</p>
+<p>
+The plot shows <i>C<sub>p,act</sub></i> of each boundary for each wind direction.
+Notice how the profile is shifted based on the surface azimuth.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Jun 28, 2021 by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=20,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside_CpData_Angles;
diff --git a/AixLib/Fluid/Sources/Examples/Outside_CpData_Specification.mo b/AixLib/Fluid/Sources/Examples/Outside_CpData_Specification.mo
index cda1c7d973..616bf44a6e 100644
--- a/AixLib/Fluid/Sources/Examples/Outside_CpData_Specification.mo
+++ b/AixLib/Fluid/Sources/Examples/Outside_CpData_Specification.mo
@@ -35,24 +35,24 @@ equation
   annotation (__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData_Specification.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model validates the specification of the wind pressure profile
- in the information section of the model
- <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">AixLib.Fluid.Sources.Outside_CpData</a>.
- The surface is configured to be facing North.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 11, 2022, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- </ul>
- </html>"),
+<p>
+This model validates the specification of the wind pressure profile
+in the information section of the model
+<a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">AixLib.Fluid.Sources.Outside_CpData</a>.
+The surface is configured to be facing North.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 11, 2022, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=86400,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside_CpData_Specification;
diff --git a/AixLib/Fluid/Sources/Examples/Outside_CpLowRise.mo b/AixLib/Fluid/Sources/Examples/Outside_CpLowRise.mo
index 650fc304b1..d5eff0880f 100644
--- a/AixLib/Fluid/Sources/Examples/Outside_CpLowRise.mo
+++ b/AixLib/Fluid/Sources/Examples/Outside_CpLowRise.mo
@@ -54,32 +54,32 @@ equation
   annotation (__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpLowRise.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates the use of a source for ambient conditions that computes
- the wind pressure on a facade of a low-rise building using the equation from Swami and Chandra (1987).
- Weather data are used for San Francisco, for a period of a week
- where the wind blows primarily from North-West.
- The plot shows that the wind pressure on the north- and west-facing
- facade is positive,
- whereas it is negative for the south- and east-facing facades.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-Buildings/issues/311\">#311</a>.
- </li>
- <li>
- October 26, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the use of a source for ambient conditions that computes
+the wind pressure on a facade of a low-rise building using the equation from Swami and Chandra (1987).
+Weather data are used for San Francisco, for a period of a week
+where the wind blows primarily from North-West.
+The plot shows that the wind pressure on the north- and west-facing
+facade is positive,
+whereas it is negative for the south- and east-facing facades.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-Buildings/issues/311\">#311</a>.
+</li>
+<li>
+October 26, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     experiment(
       StartTime=1.728e+07,
       StopTime=1.78848e+07,
-      Tolerance=1e-6),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-6), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside_CpLowRise;
diff --git a/AixLib/Fluid/Sources/Examples/PropertySource_T.mo b/AixLib/Fluid/Sources/Examples/PropertySource_T.mo
index 3c492524cf..352e55070e 100644
--- a/AixLib/Fluid/Sources/Examples/PropertySource_T.mo
+++ b/AixLib/Fluid/Sources/Examples/PropertySource_T.mo
@@ -109,24 +109,24 @@ equation
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Example model that illustrates the use of
- the <a href=\"modelica://AixLib.Fluid.Sources.PropertySource_T\">
- AixLib.Fluid.Sources.PropertySource_T</a> model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 30, 2018, by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Example model that illustrates the use of
+the <a href=\"modelica://AixLib.Fluid.Sources.PropertySource_T\">
+AixLib.Fluid.Sources.PropertySource_T</a> model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 30, 2018, by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/PropertySource_T.mos"
         "Simulate and plot"),
     experiment(
       StopTime=1,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropertySource_T;
diff --git a/AixLib/Fluid/Sources/Examples/PropertySource_h.mo b/AixLib/Fluid/Sources/Examples/PropertySource_h.mo
index 39349f0cde..43274da1aa 100644
--- a/AixLib/Fluid/Sources/Examples/PropertySource_h.mo
+++ b/AixLib/Fluid/Sources/Examples/PropertySource_h.mo
@@ -85,24 +85,24 @@ equation
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Example model that illustrates the use of
- the <a href=\"modelica://AixLib.Fluid.Sources.PropertySource_h\">
- AixLib.Fluid.Sources.PropertySource_h</a> model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 30, 2018, by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Example model that illustrates the use of
+the <a href=\"modelica://AixLib.Fluid.Sources.PropertySource_h\">
+AixLib.Fluid.Sources.PropertySource_h</a> model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 30, 2018, by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/PropertySource_h.mos"
         "Simulate and plot"),
     experiment(
       StopTime=1,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropertySource_h;
diff --git a/AixLib/Fluid/Sources/Examples/TraceSubstancesFlowSource.mo b/AixLib/Fluid/Sources/Examples/TraceSubstancesFlowSource.mo
index 54c6571999..9113d890fd 100644
--- a/AixLib/Fluid/Sources/Examples/TraceSubstancesFlowSource.mo
+++ b/AixLib/Fluid/Sources/Examples/TraceSubstancesFlowSource.mo
@@ -11,11 +11,13 @@ model TraceSubstancesFlowSource
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial) "Mixing volume"
                           annotation (Placement(transformation(extent={{100,120},
             {120,140}})));
-  Sources.TraceSubstancesFlowSource sou(redeclare package Medium = Medium,
-      use_m_flow_in=true,
+  Sources.TraceSubstancesFlowSource sou(
+    redeclare package Medium = Medium,
+    use_m_flow_in=true,
     nPorts=1)
     annotation (Placement(transformation(extent={{-46,110},{-26,130}})));
-  Modelica.Blocks.Sources.Step step(          startTime=0.5,
+  Modelica.Blocks.Sources.Step step(
+    startTime=0.5,
     height=-2,
     offset=2)
     annotation (Placement(transformation(extent={{-92,30},{-72,50}})));
@@ -106,16 +108,24 @@ model TraceSubstancesFlowSource
     "Resistance, used to check if species are transported between ports"
     annotation (Placement(transformation(extent={{-28,-80},{-6,-60}})));
 
-  Sensors.TraceSubstances C(redeclare package Medium = Medium)
+  Sensors.TraceSubstances C(
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "Trace substance sensor"
     annotation (Placement(transformation(extent={{120,134},{140,154}})));
-  Sensors.TraceSubstances C1(redeclare package Medium = Medium)
+  Sensors.TraceSubstances C1(
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "Trace substance sensor"
     annotation (Placement(transformation(extent={{120,90},{140,110}})));
-  Sensors.TraceSubstances C2(redeclare package Medium = Medium)
+  Sensors.TraceSubstances C2(
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "Trace substance sensor"
     annotation (Placement(transformation(extent={{168,6},{188,26}})));
-  Sensors.TraceSubstances C3(redeclare package Medium = Medium)
+  Sensors.TraceSubstances C3(
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "Trace substance sensor"
     annotation (Placement(transformation(extent={{188,-50},{208,-30}})));
   FixedResistances.PressureDrop res4(
@@ -242,41 +252,47 @@ equation
              __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/TraceSubstancesFlowSource.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This model demonstrates the use of trace substances that are added
- to a volume of air.
- The source is a step function of <i>2</i> kg/s CO<sub>2</sub> from <i>t=0</i> second
- to <i>t=0.5</i> second.
- The sensors <code>C</code> and <code>C1</code> measure the same concentration that initially increases
- and then remains constant as there is no flow through the volumes <code>vol</code> and <code>vol1</code>.
- The sensors
- <code>C2</code> and
- <code>C3</code> first meaure an increase in concentration, which then decays to zero
- as there is a mass flow rate with zero CO<sub>2</sub> from the source <code>bou</code> to the sink <code>sin</code>.
- </html>",revisions="<html>
- <ul>
- <li>
- November 27, 2013 by Michael Wetter:<br/>
- Added pressure boundary condition to model.
- This is required for the new air model,
- which is incompressible. Otherwise, there will be no pressure reference
- in the system.
- </li>
- <li>
- September 19, 2013, by Michael Wetter:<br/>
- Simplified example.
- </li>
- <li>
- April 29, 2013, by Michael Wetter:<br/>
- Changed the initialization of the medium volumes from free initial conditions
- to <code>Modelica.Fluid.Types.Dynamics.FixedInitial</code>.
- This was required for <code>vol</code> and <code>vol1</code> to have the same
- computations for the initial states.
- </li>
- <li>
- September 18, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
-end TraceSubstancesFlowSource;
+This model demonstrates the use of trace substances that are added
+to a volume of air.
+The source is a step function of <i>2</i> kg/s CO<sub>2</sub> from <i>t=0</i> second
+to <i>t=0.5</i> second.
+The sensors <code>C</code> and <code>C1</code> measure the same concentration that initially increases
+and then remains constant as there is no flow through the volumes <code>vol</code> and <code>vol1</code>.
+The sensors
+<code>C2</code> and
+<code>C3</code> first meaure an increase in concentration, which then decays to zero
+as there is a mass flow rate with zero CO<sub>2</sub> from the source <code>bou</code> to the sink <code>sin</code>.
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2024, by Michael Wetter:<br/>
+Configured the sensor parameter to suppress the warning about being a one-port connection.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1857\">IBPSA, #1857</a>.
+</li>
+<li>
+November 27, 2013 by Michael Wetter:<br/>
+Added pressure boundary condition to model.
+This is required for the new air model,
+which is incompressible. Otherwise, there will be no pressure reference
+in the system.
+</li>
+<li>
+September 19, 2013, by Michael Wetter:<br/>
+Simplified example.
+</li>
+<li>
+April 29, 2013, by Michael Wetter:<br/>
+Changed the initialization of the medium volumes from free initial conditions
+to <code>Modelica.Fluid.Types.Dynamics.FixedInitial</code>.
+This was required for <code>vol</code> and <code>vol1</code> to have the same
+computations for the initial states.
+</li>
+<li>
+September 18, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end TraceSubstancesFlowSource;
\ No newline at end of file
diff --git a/AixLib/Fluid/Sources/MassFlowSource_T.mo b/AixLib/Fluid/Sources/MassFlowSource_T.mo
index f22590b37d..ba33612050 100644
--- a/AixLib/Fluid/Sources/MassFlowSource_T.mo
+++ b/AixLib/Fluid/Sources/MassFlowSource_T.mo
@@ -5,13 +5,13 @@ model MassFlowSource_T
 
   parameter Boolean use_m_flow_in = false
     "Get the mass flow rate from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Modelica.Units.SI.MassFlowRate m_flow=0
     "Fixed mass flow rate going out of the fluid port"
     annotation (Dialog(enable=not use_m_flow_in, group="Fixed inputs"));
   parameter Boolean use_T_in= false
     "Get the temperature from the input connector"
-    annotation(Evaluate=true, HideResult=true,Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Medium.Temperature T = Medium.T_default
     "Fixed value of temperature"
     annotation (Dialog(enable = not use_T_in,group="Fixed inputs"));
@@ -58,79 +58,85 @@ equation
 
   annotation (defaultComponentName="boundary",
     Documentation(info="<html>
- <p>
- Models an ideal flow source, with prescribed values of flow rate, temperature, composition and trace substances:
- </p>
- <ul>
- <li> Prescribed mass flow rate.</li>
- <li> Prescribed temperature.</li>
- <li> Boundary composition (only for multi-substance or trace-substance flow).</li>
- </ul>
- <p>
- If <code>use_m_flow_in</code> is false (default option),
- the <code>m_flow</code> parameter
- is used as boundary pressure, and the <code>m_flow_in</code>
- input connector is disabled; if <code>use_m_flow_in</code>
- is true, then the <code>m_flow</code> parameter is ignored,
- and the value provided by the input connector is used instead.
- </p>
- <p>
- The same applies to the temperature <i>T</i>, composition <i>X<sub>i</sub></i> or <i>X</i> and trace substances <i>C</i>.
- </p>
- <h4>Options</h4>
- <p>
- Instead of using <code>Xi_in</code> (the <i>independent</i> composition fractions),
- the advanced tab provides an option for setting all
- composition fractions using <code>X_in</code>.
- <code>use_X_in</code> and <code>use_Xi_in</code> cannot be used
- at the same time.
- </p>
- <p>
- Parameter <code>verifyInputs</code> can be set to <code>true</code>
- to enable a check that verifies the validity of the used temperature
- and pressures.
- This removes the corresponding overhead from the model, which is
- a substantial part of the overhead of this model.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>
- for more information.
- </p>
- <p>
- Note, that boundary temperature,
- mass fractions and trace substances have only an effect if the mass flow
- is from the boundary into the port. If mass is flowing from
- the port into the boundary, the boundary definitions,
- with exception of boundary flow rate, do not have an effect.
- </p>
- </html>",
+<p>
+Models an ideal flow source, with prescribed values of flow rate, temperature, composition and trace substances:
+</p>
+<ul>
+<li> Prescribed mass flow rate.</li>
+<li> Prescribed temperature.</li>
+<li> Boundary composition (only for multi-substance or trace-substance flow).</li>
+</ul>
+<p>
+If <code>use_m_flow_in</code> is false (default option),
+the <code>m_flow</code> parameter
+is used as boundary pressure, and the <code>m_flow_in</code>
+input connector is disabled; if <code>use_m_flow_in</code>
+is true, then the <code>m_flow</code> parameter is ignored,
+and the value provided by the input connector is used instead.
+</p>
+<p>
+The same applies to the temperature <i>T</i>, composition <i>X<sub>i</sub></i> or <i>X</i> and trace substances <i>C</i>.
+</p>
+<h4>Options</h4>
+<p>
+Instead of using <code>Xi_in</code> (the <i>independent</i> composition fractions),
+the advanced tab provides an option for setting all
+composition fractions using <code>X_in</code>.
+<code>use_X_in</code> and <code>use_Xi_in</code> cannot be used
+at the same time.
+</p>
+<p>
+Parameter <code>verifyInputs</code> can be set to <code>true</code>
+to enable a check that verifies the validity of the used temperature
+and pressures.
+This removes the corresponding overhead from the model, which is
+a substantial part of the overhead of this model.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>
+for more information.
+</p>
+<p>
+Note, that boundary temperature,
+mass fractions and trace substances have only an effect if the mass flow
+is from the boundary into the port. If mass is flowing from
+the port into the boundary, the boundary definitions,
+with exception of boundary flow rate, do not have an effect.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 25, 2019, by Michael Wetter:<br/>
- Refactored use of base classes.<br/>
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\">#1072</a>.
- </li>
- <li>
- February 2nd, 2018 by Filip Jorissen<br/>
- Made <code>medium</code> conditional and refactored inputs.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
- </li>
- <li>
- April 18, 2017, by Filip Jorissen:<br/>
- Changed <code>checkBoundary</code> implementation
- such that it is run as an initial equation
- when it depends on parameters only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/728\">#728</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>unit</code> and <code>quantity</code> attributes.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+January 25, 2019, by Michael Wetter:<br/>
+Refactored use of base classes.<br/>
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1072\">#1072</a>.
+</li>
+<li>
+February 2nd, 2018 by Filip Jorissen<br/>
+Made <code>medium</code> conditional and refactored inputs.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
+</li>
+<li>
+April 18, 2017, by Filip Jorissen:<br/>
+Changed <code>checkBoundary</code> implementation
+such that it is run as an initial equation
+when it depends on parameters only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/728\">#728</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>unit</code> and <code>quantity</code> attributes.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Text(
           visible=use_m_flow_in,
@@ -175,6 +181,6 @@ revisions="<html>
                                   Text(
           extent={{-161,110},{139,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFlowSource_T;
diff --git a/AixLib/Fluid/Sources/MassFlowSource_WeatherData.mo b/AixLib/Fluid/Sources/MassFlowSource_WeatherData.mo
index 36e0b5ee32..778aacf941 100644
--- a/AixLib/Fluid/Sources/MassFlowSource_WeatherData.mo
+++ b/AixLib/Fluid/Sources/MassFlowSource_WeatherData.mo
@@ -1,14 +1,14 @@
 within AixLib.Fluid.Sources;
 model MassFlowSource_WeatherData
   "Ideal flow source that produces a prescribed mass flow with prescribed
-   trace substances, outside specific enthalpy and mass fraction "
-  extends AixLib.Fluid.Sources.BaseClasses.PartialSource(final verifyInputs=true);
+  trace substances, outside specific enthalpy and mass fraction "
+  extends AixLib.Fluid.Sources.BaseClasses.PartialAirSource(final verifyInputs=true);
   parameter Boolean use_m_flow_in = false
     "Get the mass flow rate from the input connector"
-    annotation(Evaluate=true, HideResult=true);
+    annotation(Evaluate=true);
   parameter Boolean use_C_in = false
     "Get the trace substances from the input connector"
-    annotation(Evaluate=true, HideResult=true);
+    annotation(Evaluate=true);
   parameter Modelica.Units.SI.MassFlowRate m_flow=0
     "Fixed mass flow rate going out of the fluid port"
     annotation (Dialog(enable=not use_m_flow_in));
@@ -155,56 +155,68 @@ equation
           textString="%name",
           textColor={0,0,255})}),
     Documentation(info="<html>
- <p>
- Models an ideal flow source, with prescribed values of flow rate and trace
- substances, with temperature and specific enthalpy from outside:
- </p>
- <ul>
- <li> Prescribed mass flow rate.</li>
- <li> Boundary composition (trace-substance flow).</li>
- <li> Outside specific enthalpy.</li>
- <li> Multi-substance composition (e.g. water vapor) from outside.</li>
- </ul>
- <p>If <code>use_m_flow_in</code> is false (default option), the <code>m_flow
- </code> parameter is used as boundary flow rate, and the <code>m_flow_in</code>
- input connector is disabled;
- if <code>use_m_flow_in</code> is true, then the <code>m_flow</code> parameter
- is ignored, and the value provided by the input connector is used instead.</p>
- <p>The same applies to the trace substances.</p>
- <p>The <a href=\"modelica://AixLib.Utilities.Psychrometrics.X_pTphi\">
- AixLib.Utilities.Psychrometrics.X_pTphi</a> block is used with the input data
- including <code>pAtm</code>, <code>TDryBul</code>, <code>relHum</code> from
- weather bus <code>weaBus</code>, to calculate <code>X</code>.</p>
- <p>The same applies to the specific enthalpy.</p>
- <p>
- Note, that boundary temperature,
- mass fractions and trace substances have only an effect if the mass flow
- is from the boundary into the port. If mass is flowing from
- the port into the boundary, the boundary definitions,
- with exception of boundary flow rate, do not have an effect.
- </p>
- </html>",
+<p>
+Models an ideal flow source, with prescribed values of flow rate and trace
+substances, with temperature and specific enthalpy from outside:
+</p>
+<ul>
+<li> Prescribed mass flow rate.</li>
+<li> Boundary composition (trace-substance flow).</li>
+<li> Outside specific enthalpy.</li>
+<li> Multi-substance composition (e.g. water vapor) from outside.</li>
+</ul>
+<p>If <code>use_m_flow_in</code> is false (default option), the <code>m_flow
+</code> parameter is used as boundary flow rate, and the <code>m_flow_in</code>
+input connector is disabled;
+if <code>use_m_flow_in</code> is true, then the <code>m_flow</code> parameter
+is ignored, and the value provided by the input connector is used instead.</p>
+<p>The same applies to the trace substances.</p>
+<p>The <a href=\"modelica://AixLib.Utilities.Psychrometrics.X_pTphi\">
+AixLib.Utilities.Psychrometrics.X_pTphi</a> block is used with the input data
+including <code>pAtm</code>, <code>TDryBul</code>, <code>relHum</code> from
+weather bus <code>weaBus</code>, to calculate <code>X</code>.</p>
+<p>The same applies to the specific enthalpy.</p>
+<p>
+Note, that boundary temperature,
+mass fractions and trace substances have only an effect if the mass flow
+is from the boundary into the port. If mass is flowing from
+the port into the boundary, the boundary definitions,
+with exception of boundary flow rate, do not have an effect.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 14, 2019, by Michael Wetter:<br/>
- Removed duplicate connector.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1248\"> #1248</a>.
- </li>
- <li>
- January 14, 2019 by Jianjun Hu:<br/>
- Changed to extend <a href=\"modelica://AixLib.Fluid.Sources.BaseClasses.PartialSource\">
- AixLib.Fluid.Sources.BaseClasses.PartialSource</a>. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\"> #1050</a>.
- </li>
- <li>
- May 21, 2017, by Jianjun Hu:<br/>
- First implementation. Created flow source with prescribed mass flow and trace
- substances, outside enthalpy and composition. Weather bus is used.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/777\">#777</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+January 09, 2023, by Jianjun Hu:<br/>
+Changed base class to constrain medium to moist air.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1681\">IBPSA, #1681</a>.
+</li>
+<li>
+November 14, 2019, by Michael Wetter:<br/>
+Removed duplicate connector.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1248\"> #1248</a>.
+</li>
+<li>
+January 14, 2019 by Jianjun Hu:<br/>
+Changed to extend <a href=\"modelica://AixLib.Fluid.Sources.BaseClasses.PartialSource\">
+AixLib.Fluid.Sources.BaseClasses.PartialSource</a>. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\"> #1050</a>.
+</li>
+<li>
+May 21, 2017, by Jianjun Hu:<br/>
+First implementation. Created flow source with prescribed mass flow and trace
+substances, outside enthalpy and composition. Weather bus is used.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/777\">#777</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFlowSource_WeatherData;
diff --git a/AixLib/Fluid/Sources/MassFlowSource_h.mo b/AixLib/Fluid/Sources/MassFlowSource_h.mo
index 42f1f26fd5..64b8e72f6b 100644
--- a/AixLib/Fluid/Sources/MassFlowSource_h.mo
+++ b/AixLib/Fluid/Sources/MassFlowSource_h.mo
@@ -5,14 +5,14 @@ model MassFlowSource_h
 
   parameter Boolean use_m_flow_in = false
     "Get the mass flow rate from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Modelica.Units.SI.MassFlowRate m_flow=0
     "Fixed mass flow rate going out of the fluid port"
     annotation (Dialog(enable=not use_m_flow_in, group="Fixed inputs"));
 
   parameter Boolean use_h_in= false
     "Get the specific enthalpy from the input connector"
-    annotation(Evaluate=true, HideResult=true, Dialog(group="Conditional inputs"));
+    annotation(Evaluate=true, Dialog(group="Conditional inputs"));
   parameter Medium.SpecificEnthalpy h = Medium.h_default
     "Fixed value of specific enthalpy"
     annotation (Dialog(enable = not use_h_in, group="Fixed inputs"));
@@ -54,79 +54,85 @@ equation
 
   annotation (defaultComponentName="boundary",
     Documentation(info="<html>
- <p>
- Models an ideal flow source, with prescribed values of flow rate, specific enthalpy, composition and trace substances:
- </p>
- <ul>
- <li> Prescribed mass flow rate.</li>
- <li> Prescribed specific enthalpy.</li>
- <li> Boundary composition (only for multi-substance or trace-substance flow).</li>
- </ul>
- <p>
- If <code>use_m_flow_in</code> is false (default option),
- the <code>m_flow</code> parameter
- is used as boundary pressure, and the <code>m_flow_in</code>
- input connector is disabled; if <code>use_m_flow_in</code>
- is true, then the <code>m_flow</code> parameter is ignored,
- and the value provided by the input connector is used instead.
- </p>
- <p>
- The same applies to the specific enthalpy <i>h</i>, composition <i>X<sub>i</sub></i> or <i>X</i> and trace substances <i>C</i>.
- </p>
- <h4>Options</h4>
- <p>
- Instead of using <code>Xi_in</code> (the <i>independent</i> composition fractions),
- the advanced tab provides an option for setting all
- composition fractions using <code>X_in</code>.
- <code>use_X_in</code> and <code>use_Xi_in</code> cannot be used
- at the same time.
- </p>
- <p>
- Parameter <code>verifyInputs</code> can be set to <code>true</code>
- to enable a check that verifies the validity of the used specific enthalpy
- and pressures.
- This removes the corresponding overhead from the model, which is
- a substantial part of the overhead of this model.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>
- for more information.
- </p>
- <p>
- Note, that boundary specific enthalpy,
- mass fractions and trace substances have only an effect if the mass flow
- is from the boundary into the port. If mass is flowing from
- the port into the boundary, the boundary definitions,
- with exception of boundary flow rate, do not have an effect.
- </p>
- </html>",
+<p>
+Models an ideal flow source, with prescribed values of flow rate, specific enthalpy, composition and trace substances:
+</p>
+<ul>
+<li> Prescribed mass flow rate.</li>
+<li> Prescribed specific enthalpy.</li>
+<li> Boundary composition (only for multi-substance or trace-substance flow).</li>
+</ul>
+<p>
+If <code>use_m_flow_in</code> is false (default option),
+the <code>m_flow</code> parameter
+is used as boundary pressure, and the <code>m_flow_in</code>
+input connector is disabled; if <code>use_m_flow_in</code>
+is true, then the <code>m_flow</code> parameter is ignored,
+and the value provided by the input connector is used instead.
+</p>
+<p>
+The same applies to the specific enthalpy <i>h</i>, composition <i>X<sub>i</sub></i> or <i>X</i> and trace substances <i>C</i>.
+</p>
+<h4>Options</h4>
+<p>
+Instead of using <code>Xi_in</code> (the <i>independent</i> composition fractions),
+the advanced tab provides an option for setting all
+composition fractions using <code>X_in</code>.
+<code>use_X_in</code> and <code>use_Xi_in</code> cannot be used
+at the same time.
+</p>
+<p>
+Parameter <code>verifyInputs</code> can be set to <code>true</code>
+to enable a check that verifies the validity of the used specific enthalpy
+and pressures.
+This removes the corresponding overhead from the model, which is
+a substantial part of the overhead of this model.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>
+for more information.
+</p>
+<p>
+Note, that boundary specific enthalpy,
+mass fractions and trace substances have only an effect if the mass flow
+is from the boundary into the port. If mass is flowing from
+the port into the boundary, the boundary definitions,
+with exception of boundary flow rate, do not have an effect.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 2nd, 2018 by Filip Jorissen<br/>
- Made <code>medium</code> conditional and refactored inputs.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
- </li>
- <li>
- April 18, 2017, by Filip Jorissen:<br/>
- Changed <code>checkBoundary</code> implementation
- such that it is run as an initial equation
- when it depends on parameters only.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/728\">#728</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>unit</code> and <code>quantity</code> attributes.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- September 29, 2009, by Michael Wetter:<br/>
- First implementation.
- Implemenation is based on <code>Modelica.Fluid</code>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+February 2nd, 2018 by Filip Jorissen<br/>
+Made <code>medium</code> conditional and refactored inputs.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/882\">#882</a>.
+</li>
+<li>
+April 18, 2017, by Filip Jorissen:<br/>
+Changed <code>checkBoundary</code> implementation
+such that it is run as an initial equation
+when it depends on parameters only.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/728\">#728</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>unit</code> and <code>quantity</code> attributes.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+September 29, 2009, by Michael Wetter:<br/>
+First implementation.
+Implemenation is based on <code>Modelica.Fluid</code>.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Text(
           visible=use_m_flow_in,
@@ -171,6 +177,6 @@ revisions="<html>
                                   Text(
           extent={{-161,110},{139,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFlowSource_h;
diff --git a/AixLib/Fluid/Sources/Outside.mo b/AixLib/Fluid/Sources/Outside.mo
index 351807d3aa..c584186976 100644
--- a/AixLib/Fluid/Sources/Outside.mo
+++ b/AixLib/Fluid/Sources/Outside.mo
@@ -8,49 +8,49 @@ equation
   connect(weaBus.TDryBul, T_in_internal);
   annotation (defaultComponentName="out",
     Documentation(info="<html>
- <p>
- This model describes boundary conditions for
- pressure, enthalpy, and species concentration that can be obtained
- from weather data.
- </p>
- <p>
- To use this model, connect weather data from
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
- AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a> to the port
- <code>weaBus</code> of this model.
- This will cause the medium of this model to be
- at the pressure that is obtained from the weather file, and any flow that
- leaves this model to be at the temperature and humidity that are obtained
- from the weather data.
- </p>
- <p>If the parameter <code>use_C_in</code> is <code>false</code> (default option),
- the <code>C</code> parameter
- is used as the trace substance for flow that leaves the component, and the
- <code>C_in</code> input connector is disabled; if <code>use_C_in</code> is <code>true</code>,
- then the <code>C</code> parameter is ignored, and the value provided by the input connector is used instead.</p>
- <p>
- Note that boundary temperature,
- mass fractions and trace substances have only an effect if the mass flow
- is from the boundary into the port. If mass is flowing from
- the port into the boundary, the boundary definitions,
- with exception of boundary pressure, do not have an effect.
- </p>
- </html>",
+<p>
+This model describes boundary conditions for
+pressure, enthalpy, and species concentration that can be obtained
+from weather data.
+</p>
+<p>
+To use this model, connect weather data from
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a> to the port
+<code>weaBus</code> of this model.
+This will cause the medium of this model to be
+at the pressure that is obtained from the weather file, and any flow that
+leaves this model to be at the temperature and humidity that are obtained
+from the weather data.
+</p>
+<p>If the parameter <code>use_C_in</code> is <code>false</code> (default option),
+the <code>C</code> parameter
+is used as the trace substance for flow that leaves the component, and the
+<code>C_in</code> input connector is disabled; if <code>use_C_in</code> is <code>true</code>,
+then the <code>C</code> parameter is ignored, and the value provided by the input connector is used instead.</p>
+<p>
+Note that boundary temperature,
+mass fractions and trace substances have only an effect if the mass flow
+is from the boundary into the port. If mass is flowing from
+the port into the boundary, the boundary definitions,
+with exception of boundary pressure, do not have an effect.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 26, 2011 by Michael Wetter:<br/>
- Introduced new base class to allow implementation of wind pressure for natural ventilation.
- </li>
- <li>
- April 27, 2011 by Michael Wetter:<br/>
- Revised implementation to allow medium model that do not have water vapor.
- </li>
- <li>
- Feb. 9, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 26, 2011 by Michael Wetter:<br/>
+Introduced new base class to allow implementation of wind pressure for natural ventilation.
+</li>
+<li>
+April 27, 2011 by Michael Wetter:<br/>
+Revised implementation to allow medium model that do not have water vapor.
+</li>
+<li>
+Feb. 9, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside;
diff --git a/AixLib/Fluid/Sources/Outside_CpData.mo b/AixLib/Fluid/Sources/Outside_CpData.mo
index b52d18ce3a..185587fee5 100644
--- a/AixLib/Fluid/Sources/Outside_CpData.mo
+++ b/AixLib/Fluid/Sources/Outside_CpData.mo
@@ -90,104 +90,104 @@ equation
 
   annotation (defaultComponentName="out",
     Documentation(info="<html>
- <p>
- This model describes boundary conditions for
- pressure, enthalpy, and species concentration that can be obtained
- from weather data. The model is identical to
- <a href=\"modelica://AixLib.Fluid.Sources.Outside\">
- AixLib.Fluid.Sources.Outside</a>,
- except that it adds the wind pressure to the
- pressure at the fluid ports <code>ports</code>.
- </p>
- <p>
- The pressure <i>p</i> at the fluid ports is computed as:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- p = p<sub>w</sub> + C<sub>p,act</sub> C<sub>s</sub> v<sup>2</sup> &rho; &frasl; 2,
- </p>
- <p>
- where <i>p<sub>w</sub></i> is the atmospheric pressure from the weather bus,
- <i>v</i> is the wind speed from the weather bus, and
- <i>&rho;</i> is the fluid density.
- </p>
- <p>
- The wind pressure coefficient <i>C<sub>p,act</sub></i> is a function of the surface wind incidence
- angle and is defined relative to the surface azimuth (normal to the surface is <i>0</i>).
- The wind incidence angle <code>incAng</code> is computed from the wind direction obtained from the weather file 
- with the surface azimuth <code>azi</code> as the base of the angle.
- The relation between the wind pressure coefficient <i>C<sub>p,act</sub></i> and the incidence angle <code>incAng</code>
- is defined by a cubic hermite interpolation of the users table input.
- Typical table values can be obtained from the &quot;AIVC guide to energy efficient ventilation&quot;,
- appendix 2 (1996). The default table is appendix 2, table 2.2, face 1.
- </p>
- <p>
- The wind speed modifier <i>C<sub>s</sub></i> can be used to incorporate the effect of the surroundings on the local wind speed.
- </p>
- <h4>Definition of angles</h4>
- <p>
- The angles <code>incAngSurNor</code> for the wind incidence angle relative to the surface normal
- are measured counter-clock wise.
- The figure below shows an example entry, which is also used in the model
- <a href=\"modelica://AixLib.Fluid.Sources.Examples.Outside_CpData_Specification\">
- AixLib.Fluid.Sources.Examples.Outside_CpData_Specification</a>.
- </p>
- <p align=\"center\"><img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Sources/Outside_CpData.png\"/> </p>
- 
- <p>
- The wind incidence angle and surface azimuths are defined as follows:
- The wind indicience angle is obtained directly from the weather data bus <code>weaBus.winDir</code>.
- This variable contains the data from the weather data file that was read, such as a TMY3 file.
- In accordance to TMY3, the data is as shown in the table below.
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <caption>Value of <code>winDir</code> if the wind blows from different directions.</caption>
- <tr><td></td>  <td style=\"text-align: center\">Wind from North:<br/>0 <br/> 0&deg;</td>  <td></td> </tr>
- <tr><td style=\"text-align: center\">Wind from West:<br/>3&pi;/2 <br/> 270&deg;</td>  <td></td>  <td style=\"text-align: center\">Wind from East:<br/>&pi;/2 <br/> 90&deg;</td></tr>
- <tr><td></td>  <td style=\"text-align: center\">Wind from South:<br/>&pi; <br/> 180&deg;</td>  <td></td></tr>
- </table>
- <p>
- For the surface azimuth <code>azi</code>, the specification from
- <a href=\"modelica://AixLib.Types.Azimuth\">AixLib.Types.Azimuth</a> is
- used, which is as shown in the table below.
- </p>
- 
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <caption>Value of <code>azi</code> if the exterior wall faces in the different directions.</caption>
- <tr><td></td>  <td style=\"text-align: center\">Wall facing north:<br> &pi; <br/> 180&deg;</td>  <td></td> </tr>
- <tr><td style=\"text-align: center\">Wall facing West:<br/> &pi;/2 <br/> 90&deg;</td>  <td></td>  <td style=\"text-align: center\">Wall facing east:<br/> 3&pi;/2 <br/> 270&deg;</td></tr>
- <tr><td></td>  <td style=\"text-align: center\">Wall facing South:<br/>0; <br/> 0&deg;</td>  <td></td></tr>
- </table>
- 
- <h4>Related model</h4>
- <p>
- This model differs from <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpLowRise\">
- AixLib.Fluid.Sources.Outside_CpLowRise</a> by the calculation of the wind pressure coefficient
- <i>C<sub>p,act</sub></i>.
- The wind pressure coefficient is defined by a user-defined table instead of a generalized equation
- such that it can be used for all building sizes and situations, for shielded buildings,
- and for buildings with non-rectangular shapes.
- </p>
- <p>
- <b>References</b>
- </p>
- <ul>
- <li>M. W. Liddament, 1996, <i>A guide to energy efficient ventilation</i>. AIVC Annex V. </li>
- </ul>
- </html>",
+<p>
+This model describes boundary conditions for
+pressure, enthalpy, and species concentration that can be obtained
+from weather data. The model is identical to
+<a href=\"modelica://AixLib.Fluid.Sources.Outside\">
+AixLib.Fluid.Sources.Outside</a>,
+except that it adds the wind pressure to the
+pressure at the fluid ports <code>ports</code>.
+</p>
+<p>
+The pressure <i>p</i> at the fluid ports is computed as:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+p = p<sub>w</sub> + C<sub>p,act</sub> C<sub>s</sub> v<sup>2</sup> &rho; &frasl; 2,
+</p>
+<p>
+where <i>p<sub>w</sub></i> is the atmospheric pressure from the weather bus,
+<i>v</i> is the wind speed from the weather bus, and
+<i>&rho;</i> is the fluid density.
+</p>
+<p>
+The wind pressure coefficient <i>C<sub>p,act</sub></i> is a function of the surface wind incidence
+angle and is defined relative to the surface azimuth (normal to the surface is <i>0</i>).
+The wind incidence angle <code>incAng</code> is computed from the wind direction obtained from the weather file 
+with the surface azimuth <code>azi</code> as the base of the angle.
+The relation between the wind pressure coefficient <i>C<sub>p,act</sub></i> and the incidence angle <code>incAng</code>
+is defined by a cubic hermite interpolation of the users table input.
+Typical table values can be obtained from the &quot;AIVC guide to energy efficient ventilation&quot;,
+appendix 2 (1996). The default table is appendix 2, table 2.2, face 1.
+</p>
+<p>
+The wind speed modifier <i>C<sub>s</sub></i> can be used to incorporate the effect of the surroundings on the local wind speed.
+</p>
+<h4>Definition of angles</h4>
+<p>
+The angles <code>incAngSurNor</code> for the wind incidence angle relative to the surface normal
+are measured counter-clock wise.
+The figure below shows an example entry, which is also used in the model
+<a href=\"modelica://AixLib.Fluid.Sources.Examples.Outside_CpData_Specification\">
+AixLib.Fluid.Sources.Examples.Outside_CpData_Specification</a>.
+</p>
+<p align=\"center\"><img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Fluid/Sources/Outside_CpData.png\"/> </p>
+
+<p>
+The wind incidence angle and surface azimuths are defined as follows:
+The wind indicience angle is obtained directly from the weather data bus <code>weaBus.winDir</code>.
+This variable contains the data from the weather data file that was read, such as a TMY3 file.
+In accordance to TMY3, the data is as shown in the table below.
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<caption>Value of <code>winDir</code> if the wind blows from different directions.</caption>
+<tr><td></td>  <td style=\"text-align: center\">Wind from North:<br/>0 <br/> 0&deg;</td>  <td></td> </tr>
+<tr><td style=\"text-align: center\">Wind from West:<br/>3&pi;/2 <br/> 270&deg;</td>  <td></td>  <td style=\"text-align: center\">Wind from East:<br/>&pi;/2 <br/> 90&deg;</td></tr>
+<tr><td></td>  <td style=\"text-align: center\">Wind from South:<br/>&pi; <br/> 180&deg;</td>  <td></td></tr>
+</table>
+<p>
+For the surface azimuth <code>azi</code>, the specification from
+<a href=\"modelica://AixLib.Types.Azimuth\">AixLib.Types.Azimuth</a> is
+used, which is as shown in the table below.
+</p>
+
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<caption>Value of <code>azi</code> if the exterior wall faces in the different directions.</caption>
+<tr><td></td>  <td style=\"text-align: center\">Wall facing north:<br> &pi; <br/> 180&deg;</td>  <td></td> </tr>
+<tr><td style=\"text-align: center\">Wall facing West:<br/> &pi;/2 <br/> 90&deg;</td>  <td></td>  <td style=\"text-align: center\">Wall facing east:<br/> 3&pi;/2 <br/> 270&deg;</td></tr>
+<tr><td></td>  <td style=\"text-align: center\">Wall facing South:<br/>0; <br/> 0&deg;</td>  <td></td></tr>
+</table>
+
+<h4>Related model</h4>
+<p>
+This model differs from <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpLowRise\">
+AixLib.Fluid.Sources.Outside_CpLowRise</a> by the calculation of the wind pressure coefficient
+<i>C<sub>p,act</sub></i>.
+The wind pressure coefficient is defined by a user-defined table instead of a generalized equation
+such that it can be used for all building sizes and situations, for shielded buildings,
+and for buildings with non-rectangular shapes.
+</p>
+<p>
+<b>References</b>
+</p>
+<ul>
+<li>M. W. Liddament, 1996, <i>A guide to energy efficient ventilation</i>. AIVC Annex V. </li>
+</ul>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Apr 6, 2021, by Klaas De Jonge:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, by Klaas De Jonge:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Line(points={{-56,54},{-56,-44},{52,-44}}, color={255,255,255}),
         Line(points={{-56,16},{-50,16},{-44,12},{-38,-2},{-28,-24},{-20,-40},
@@ -198,6 +198,6 @@ revisions="<html>
         Text(
           extent={{-54,66},{2,22}},
           textColor={255,255,255},
-          textString="Cp")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="Cp")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside_CpData;
diff --git a/AixLib/Fluid/Sources/Outside_CpLowRise.mo b/AixLib/Fluid/Sources/Outside_CpLowRise.mo
index 2af27a1548..516b5165d8 100644
--- a/AixLib/Fluid/Sources/Outside_CpLowRise.mo
+++ b/AixLib/Fluid/Sources/Outside_CpLowRise.mo
@@ -51,135 +51,137 @@ equation
   connect(weaBus.TDryBul, T_in_internal);
   annotation (defaultComponentName="out",
     Documentation(info="<html>
- <p>
- This model describes boundary conditions for
- pressure, enthalpy, and species concentration that can be obtained
- from weather data. The model is identical to
- <a href=\"modelica://AixLib.Fluid.Sources.Outside\">
- AixLib.Fluid.Sources.Outside</a>,
- except that it adds the wind pressure to the
- pressure at the fluid port <code>ports</code>.
- The correlation that is used to compute the wind pressure is based
- on Swami and Chandra (1987) and valid for low-rise buildings
- with rectangular shape.
- The same correlation is also implemented in CONTAM (Persily and Ivy, 2001).
- <!-- @include_Buildings
- For other buildings, the model
- <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">
- AixLib.Fluid.Sources.Outside_CpData</a> or
- <a href=\"modelica://AixLib.Fluid.Sources.Outside_Cp\">
- AixLib.Fluid.Sources.Outside_Cp</a>
- should be used that takes
- the wind pressure coefficient as a parameter or an input.
- -->
- </p>
- <p>
- The wind pressure coefficient is computed based on the
- side ratio of the walls, which is defined as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- s = x &frasl; y
- </p>
- <p>
- where <i>x</i> is the length of the wall that will be connected to
- this model, and <i>y</i> is the length of the adjacent wall.
- The wind direction is computed relative to the azimuth of this surface,
- which is equal to the parameter <code>azi</code>.
- The surface azimuth is defined in
- <a href=\"modelica://AixLib.Types.Azimuth\">
- AixLib.Types.Azimuth</a>.
- For example, if an exterior wall is South oriented, i.e., its outside-facing
- surface is towards South, use
- <code>AixLib.Types.Azimuth.S</code>.
- </p>
- <p>
- Based on the surface azimuth, the wind direction and the side ratio
- of the walls, the model computes how much the wind pressure
- is attenuated compared to the reference wind pressure <code>Cp0</code>.
- The reference wind pressure <code>Cp0</code> is a user-defined parameter,
- and must be equal to the wind pressure at zero wind incidence angle.
- Swami and Chandra (1987) recommend <i>C<sub>p0</sub> = 0.6</i> for
- all low-rise buildings as this represents the average of
- various values reported in the literature.
- The computation of the actual wind pressure coefficient <i>C<sub>p</sub></i>
- is explained in the function
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise\">
- Buildings.Airflow.Multizone.BaseClasses.windPressureLowRise</a>
- that is called by this model.
- </p>
- <p>
- The pressure <i>p</i> at the port <code>ports</code> is computed as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   p = p<sub>w</sub> + C<sub>p</sub> 1 &frasl; 2 v<sup>2</sup> &rho;,
- </p>
- <p>
- where
- <i>p<sub>w</sub></i> is the atmospheric pressure from the weather bus,
- <i>v</i> is the wind speed from the weather bus, and
- <i>&rho;</i> is the fluid density.
- </p>
- 
- <p>
- This model differs from <a href=\"AixLib.Fluid.Sources.Outside_CpData\">
- AixLib.Fluid.Sources.Outside_CpData</a> by the calculation of the wind pressure coefficient C<sub>p,act</sub>.
- The wind pressure coefficient is defined by an equation in stead of a user-defined table.
- This model is only suited for low-rise rectangular buildings.
- </p>
- 
- <h4>References</h4>
- <ul>
- <li>
- Muthusamy V. Swami and
- Subrato Chandra.
- <i>
- <a href=\"http://www.fsec.ucf.edu/en/publications/pdf/FSEC-CR-163-86.pdf\">
- Procedures for
- Calculating Natural
- Ventilation Airflow
- Rates in Buildings.</a></i>
- Florida Solar Energy Center, FSEC-CR-163-86. March, 1987.
- Cape Canaveral, Florida.
- </li>
- <li>
- Andrew K. Persily and Elizabeth M. Ivy.
- <i>
- <a href=\"http://ws680.nist.gov/publication/get_pdf.cfm?pub_id=860831\">
- Input Data for Multizone Airflow and IAQ Analysis.</a></i>
- NIST, NISTIR 6585.
- January, 2001.
- Gaithersburg, MD.
- </li>
- </ul>
- </html>",
+<p>
+This model describes boundary conditions for
+pressure, enthalpy, and species concentration that can be obtained
+from weather data. The model is identical to
+<a href=\"modelica://AixLib.Fluid.Sources.Outside\">
+AixLib.Fluid.Sources.Outside</a>,
+except that it adds the wind pressure to the
+pressure at the fluid port <code>ports</code>.
+The correlation that is used to compute the wind pressure is based
+on Swami and Chandra (1987) and valid for low-rise buildings
+with rectangular shape.
+The same correlation is also implemented in CONTAM (Persily and Ivy, 2001).
+<!-- @include_Buildings
+For other buildings, the model
+<a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">
+AixLib.Fluid.Sources.Outside_CpData</a> or
+<a href=\"modelica://AixLib.Fluid.Sources.Outside_Cp\">
+AixLib.Fluid.Sources.Outside_Cp</a>
+should be used that takes
+the wind pressure coefficient as a parameter or an input.
+-->
+</p>
+<p>
+The wind pressure coefficient is computed based on the
+side ratio of the walls, which is defined as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+s = x &frasl; y
+</p>
+<p>
+where <i>x</i> is the length of the wall that will be connected to
+this model, and <i>y</i> is the length of the adjacent wall.
+The wind direction is computed relative to the azimuth of this surface,
+which is equal to the parameter <code>azi</code>.
+The surface azimuth is defined in
+<a href=\"modelica://AixLib.Types.Azimuth\">
+AixLib.Types.Azimuth</a>.
+For example, if an exterior wall is South oriented, i.e., its outside-facing
+surface is towards South, use
+<code>AixLib.Types.Azimuth.S</code>.
+</p>
+<p>
+Based on the surface azimuth, the wind direction and the side ratio
+of the walls, the model computes how much the wind pressure
+is attenuated compared to the reference wind pressure <code>Cp0</code>.
+The reference wind pressure <code>Cp0</code> is a user-defined parameter,
+and must be equal to the wind pressure at zero wind incidence angle.
+Swami and Chandra (1987) recommend <i>C<sub>p0</sub> = 0.6</i> for
+all low-rise buildings as this represents the average of
+various values reported in the literature.
+The computation of the actual wind pressure coefficient <i>C<sub>p</sub></i>
+is explained in the function
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise\">
+Buildings.Airflow.Multizone.BaseClasses.windPressureLowRise</a>
+that is called by this model.
+</p>
+<p>
+The pressure <i>p</i> at the port <code>ports</code> is computed as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  p = p<sub>w</sub> + C<sub>p</sub> 1 &frasl; 2 v<sup>2</sup> &rho;,
+</p>
+<p>
+where
+<i>p<sub>w</sub></i> is the atmospheric pressure from the weather bus,
+<i>v</i> is the wind speed from the weather bus, and
+<i>&rho;</i> is the fluid density.
+</p>
+
+<p>
+This model differs from <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">
+AixLib.Fluid.Sources.Outside_CpData</a> by the calculation of the wind pressure coefficient C<sub>p,act</sub>.
+The wind pressure coefficient is defined by an equation in stead of a user-defined table.
+This model is only suited for low-rise rectangular buildings.
+</p>
+
+<h4>References</h4>
+<ul>
+<li>
+Muthusamy V. Swami and
+Subrato Chandra.
+<i>
+<a href=\"http://www.fsec.ucf.edu/en/publications/pdf/FSEC-CR-163-86.pdf\">
+Procedures for
+Calculating Natural
+Ventilation Airflow
+Rates in Buildings.</a></i>
+Florida Solar Energy Center, FSEC-CR-163-86. March, 1987.
+Cape Canaveral, Florida.
+</li>
+<li>
+Andrew K. Persily and Elizabeth M. Ivy.
+<i>
+<a href=\"http://ws680.nist.gov/publication/get_pdf.cfm?pub_id=860831\">
+Input Data for Multizone Airflow and IAQ Analysis.</a></i>
+NIST, NISTIR 6585.
+January, 2001.
+Gaithersburg, MD.
+</li>
+</ul>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 2, 2022, by Michael Wetter:<br/>
- Revised implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- <li>
- Jun 28, 2021, by Klaas De Jonge:<br/>
- Documentation changes to explain the difference with <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">
- AixLib.Fluid.Sources.Outside_CpData</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>unit</code> and <code>quantity</code> attributes.
- </li>
- <li>
- October 26, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    Icon(graphics={Text(
-          visible=use_Cp_in,
-          extent={{-140,92},{-92,62}},
-          textColor={0,0,255},
-          textString="C_p"),
+<ul>
+<li>
+April 4, 2023, by Michael Wetter:<br/>
+Removed use of non-existent parameter in annotation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1724\">IBPSA, #1724</a>.
+</li>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Jun 28, 2021, by Klaas De Jonge:<br/>
+Documentation changes to explain the difference with <a href=\"modelica://AixLib.Fluid.Sources.Outside_CpData\">
+AixLib.Fluid.Sources.Outside_CpData</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>unit</code> and <code>quantity</code> attributes.
+</li>
+<li>
+October 26, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Icon(graphics={
           Text(
           visible=use_C_in,
           extent={{-154,-28},{-102,-62}},
@@ -188,6 +190,6 @@ revisions="<html>
         Text(
           extent={{-28,22},{28,-22}},
           textColor={255,255,255},
-          textString="Cp")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="Cp")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside_CpLowRise;
diff --git a/AixLib/Fluid/Sources/PropertySource_T.mo b/AixLib/Fluid/Sources/PropertySource_T.mo
index 028c0d8f8f..9e5348dd19 100644
--- a/AixLib/Fluid/Sources/PropertySource_T.mo
+++ b/AixLib/Fluid/Sources/PropertySource_T.mo
@@ -46,38 +46,38 @@ annotation (defaultComponentName="proSou",
           fillPattern=FillPattern.Solid,
           textString="T")}),
     Documentation(info="<html>
- <p>
- Model that changes the properties,
- but not the mass flow rate,
- of the fluid that passes through it.
- </p>
- <p>
- If <code>allowFlowReversal=true</code>, then the properties are changed for both flow directions,
- i.e., from <code>port_a</code> to <code>port_b</code> and
- from <code>port_b</code> to <code>port_a</code>.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The fluid properties <code>h</code>, <code>Xi</code> and <code>C</code>
- are only modified when the corresponding boolean parameter
- <code>use_T_in</code>, <code>use_Xi_in</code> or <code>use_C_in</code>
- is set to <code>true</code>.
- </p>
- <h4>Dynamics</h4>
- <p>
- This model has no dynamics.
- </p>
- </html>",
+<p>
+Model that changes the properties,
+but not the mass flow rate,
+of the fluid that passes through it.
+</p>
+<p>
+If <code>allowFlowReversal=true</code>, then the properties are changed for both flow directions,
+i.e., from <code>port_a</code> to <code>port_b</code> and
+from <code>port_b</code> to <code>port_a</code>.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The fluid properties <code>h</code>, <code>Xi</code> and <code>C</code>
+are only modified when the corresponding boolean parameter
+<code>use_T_in</code>, <code>use_Xi_in</code> or <code>use_C_in</code>
+is set to <code>true</code>.
+</p>
+<h4>Dynamics</h4>
+<p>
+This model has no dynamics.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 30, 2018, by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 30, 2018, by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{
-            100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropertySource_T;
diff --git a/AixLib/Fluid/Sources/PropertySource_h.mo b/AixLib/Fluid/Sources/PropertySource_h.mo
index 255339bc51..20a82429ff 100644
--- a/AixLib/Fluid/Sources/PropertySource_h.mo
+++ b/AixLib/Fluid/Sources/PropertySource_h.mo
@@ -33,38 +33,38 @@ annotation (defaultComponentName="proSou",
           fillPattern=FillPattern.Solid,
           textString="h")}),
     Documentation(info="<html>
- <p>
- Model that changes the properties,
- but not the mass flow rate,
- of the fluid that passes through it.
- </p>
- <p>
- If <code>allowFlowReversal=true</code>, then the properties are changed for both flow directions,
- i.e., from <code>port_a</code> to <code>port_b</code> and
- from <code>port_b</code> to <code>port_a</code>.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The fluid properties <code>h</code>, <code>Xi</code> and <code>C</code>
- are only modified when the corresponding boolean parameter
- <code>use_h_in</code>, <code>use_Xi_in</code> or <code>use_C_in</code>
- is set to <code>true</code>.
- </p>
- <h4>Dynamics</h4>
- <p>
- This model has no dynamics.
- </p>
- </html>",
+<p>
+Model that changes the properties,
+but not the mass flow rate,
+of the fluid that passes through it.
+</p>
+<p>
+If <code>allowFlowReversal=true</code>, then the properties are changed for both flow directions,
+i.e., from <code>port_a</code> to <code>port_b</code> and
+from <code>port_b</code> to <code>port_a</code>.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The fluid properties <code>h</code>, <code>Xi</code> and <code>C</code>
+are only modified when the corresponding boolean parameter
+<code>use_h_in</code>, <code>use_Xi_in</code> or <code>use_C_in</code>
+is set to <code>true</code>.
+</p>
+<h4>Dynamics</h4>
+<p>
+This model has no dynamics.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 30, 2018, by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 30, 2018, by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/881\">#881</a>.
+</li>
+</ul>
+</html>"),
     Diagram(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{
-            100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+            100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropertySource_h;
diff --git a/AixLib/Fluid/Sources/TraceSubstancesFlowSource.mo b/AixLib/Fluid/Sources/TraceSubstancesFlowSource.mo
index a2e45a161b..d93280e9c7 100644
--- a/AixLib/Fluid/Sources/TraceSubstancesFlowSource.mo
+++ b/AixLib/Fluid/Sources/TraceSubstancesFlowSource.mo
@@ -13,7 +13,7 @@ model TraceSubstancesFlowSource
   parameter String substanceName = "CO2" "Name of trace substance";
   parameter Boolean use_m_flow_in = false
     "Get the trace substance mass flow rate from the input connector"
-    annotation(Evaluate=true, HideResult=true);
+    annotation(Evaluate=true);
 
   parameter Modelica.Units.SI.MassFlowRate m_flow=0
     "Fixed mass flow rate going out of the fluid port"
@@ -53,11 +53,11 @@ initial equation
   // Only one connection allowed to a port to avoid unwanted ideal mixing
   for i in 1:nPorts loop
     assert(cardinality(ports[i]) <= 1,"
- Each ports[i] of boundary shall at most be connected to one component.
- If two or more connections are present, ideal mixing takes
- place in these connections, which is usually not the intention
- of the modeller. Increase nPorts to add an additional port.
- ");
+Each ports[i] of boundary shall at most be connected to one component.
+If two or more connections are present, ideal mixing takes
+place in these connections, which is usually not the intention
+of the modeller. Increase nPorts to add an additional port.
+");
   end for;
 
 equation
@@ -81,84 +81,90 @@ equation
   annotation (
 defaultComponentName="souTraSub",
 Documentation(info="<html>
- <p>
- This model can be used to inject trace substances into a system.
- The model adds a mass flow rate to its port with a
- trace substance concentration of <i>1</i>.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- A typical use of this model is to add carbon dioxide to room air, since the
- carbon dioxide concentration is typically so small that it need not be
- added to the room mass balance, and since the mass flow rate can be
- made small compared to the room volume if the medium that leaves this
- component has a carbon dioxide concentration of <i>1</i>.
- The parameter <code>substanceName</code> must be set to the name of the substance
- that is injected into the fluid.
- </p>
- <p>
- Note however that mixing volumes from the package
- <a href=\"modelica://AixLib.Fluid.MixingVolumes\">AixLib.Fluid.MixingVolumes</a>
- allow to directly add a trace substance mass flow rate,
- which is more efficient than using this model.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 14, 2019, by Michael Wetter:<br/>
- Rewrote assignment of <code>C_in_internal</code> to avoid an initial algorithm section.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1250\">#1250</a>.
- </li>
- <li>
- January 23, 2019, by Michael Wetter:<br/>
- Refactored implementation to provide default medium choice.
- This refactoring removes the dependency of the base class but is
- compatible with the previous implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
- </li>
- <li>
- January 26, 2016, by Michael Wetter:<br/>
- Added <code>unit</code> and <code>quantity</code> attributes.
- </li>
- <li>
- January 19, 2016, by Michael Wetter:<br/>
- Updated documentation due to the addition of an input for trace substance
- in the mixing volume.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">
- issue 372</a>.
- </li>
- <li>
- October 30, 2015, by Matthis Thorade:<br/>
- Removed <code>nPorts=1</code> in extension of the base class
- as the default must be <i>0</i>.
- This avoids a warning in the pedantic model check of Dymola 2016.
- </li>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Added missing <code>each</code> in declaration of
- <code>C_in_internal</code>.
- This eliminates a compilation error in OpenModelica.
- </li>
- <li>
- March 27, 2013, by Michael Wetter:<br/>
- Removed binding for <code>C_in_internal</code> to allow pedantic check in Dymola 2014.
- </li>
- <li>
- February 22, by Michael Wetter:<br/>
- Improved code that searches for the index of the trace substance in the medium model.
- </li>
- <li>
- September 18, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),                      Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,
+<p>
+This model can be used to inject trace substances into a system.
+The model adds a mass flow rate to its port with a
+trace substance concentration of <i>1</i>.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+A typical use of this model is to add carbon dioxide to room air, since the
+carbon dioxide concentration is typically so small that it need not be
+added to the room mass balance, and since the mass flow rate can be
+made small compared to the room volume if the medium that leaves this
+component has a carbon dioxide concentration of <i>1</i>.
+The parameter <code>substanceName</code> must be set to the name of the substance
+that is injected into the fluid.
+</p>
+<p>
+Note however that mixing volumes from the package
+<a href=\"modelica://AixLib.Fluid.MixingVolumes\">AixLib.Fluid.MixingVolumes</a>
+allow to directly add a trace substance mass flow rate,
+which is more efficient than using this model.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+November 14, 2019, by Michael Wetter:<br/>
+Rewrote assignment of <code>C_in_internal</code> to avoid an initial algorithm section.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1250\">#1250</a>.
+</li>
+<li>
+January 23, 2019, by Michael Wetter:<br/>
+Refactored implementation to provide default medium choice.
+This refactoring removes the dependency of the base class but is
+compatible with the previous implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1050\">#1050</a>.
+</li>
+<li>
+January 26, 2016, by Michael Wetter:<br/>
+Added <code>unit</code> and <code>quantity</code> attributes.
+</li>
+<li>
+January 19, 2016, by Michael Wetter:<br/>
+Updated documentation due to the addition of an input for trace substance
+in the mixing volume.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/372\">
+issue 372</a>.
+</li>
+<li>
+October 30, 2015, by Matthis Thorade:<br/>
+Removed <code>nPorts=1</code> in extension of the base class
+as the default must be <i>0</i>.
+This avoids a warning in the pedantic model check of Dymola 2016.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Added missing <code>each</code> in declaration of
+<code>C_in_internal</code>.
+This eliminates a compilation error in OpenModelica.
+</li>
+<li>
+March 27, 2013, by Michael Wetter:<br/>
+Removed binding for <code>C_in_internal</code> to allow pedantic check in Dymola 2014.
+</li>
+<li>
+February 22, by Michael Wetter:<br/>
+Improved code that searches for the index of the trace substance in the medium model.
+</li>
+<li>
+September 18, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),                       Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,
             -100},{100,100}}), graphics={
         Rectangle(
           extent={{20,60},{100,-60}},
@@ -207,6 +213,6 @@ Documentation(info="<html>
         Text(
           extent={{-150,110},{150,150}},
           textString="%name",
-          textColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TraceSubstancesFlowSource;
diff --git a/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystem.mo b/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystem.mo
index 633d36b380..ec43b55265 100644
--- a/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystem.mo
+++ b/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystem.mo
@@ -30,24 +30,24 @@ equation
   connect(sin.ports[1], senTem.port_b)
     annotation (Line(points={{40,0},{10,0}}, color={0,127,255}));
   annotation (Documentation(info="<html>
- <p>
- System model used to test the boundary conditions for different media.
- This model has been introduced to get access to the medium mass fraction,
- which is a protected variable in
- <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
- AixLib.Fluid.Sources.Boundary_pT</a>.
- Therefore, this model has been created so that the boundary model has a port which
- is used to access the mass fraction.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 13, 2019 by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+System model used to test the boundary conditions for different media.
+This model has been introduced to get access to the medium mass fraction,
+which is a protected variable in
+<a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a>.
+Therefore, this model has been created so that the boundary model has a port which
+is used to access the mass fraction.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 13, 2019 by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BoundarySystem;
diff --git a/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystemWithX_in.mo b/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystemWithX_in.mo
index 2283ca4323..60099fd5d3 100644
--- a/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystemWithX_in.mo
+++ b/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystemWithX_in.mo
@@ -12,19 +12,19 @@ equation
   connect(sou.X_in, X_in) annotation (Line(points={{-62,-4},{-82,-4},{-82,0},{-120,
           0}},      color={0,0,127}));
   annotation (Documentation(info="<html>
- <p>
- System model used to test the boundary conditions for different media
- with prescribed mass fraction <code>X</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 13, 2019 by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+System model used to test the boundary conditions for different media
+with prescribed mass fraction <code>X</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 13, 2019 by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BoundarySystemWithX_in;
diff --git a/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystemWithXi_in.mo b/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystemWithXi_in.mo
index 527b141d6e..df86b50744 100644
--- a/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystemWithXi_in.mo
+++ b/AixLib/Fluid/Sources/Validation/BaseClasses/BoundarySystemWithXi_in.mo
@@ -12,19 +12,19 @@ equation
   connect(sou.Xi_in, Xi_in) annotation (Line(points={{-62,-4},{-82,-4},{-82,0},{
           -120,0}}, color={0,0,127}));
   annotation (Documentation(info="<html>
- <p>
- System model used to test the boundary conditions for different media
- with independent prescribed mass fraction <code>Xi</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 13, 2019 by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+System model used to test the boundary conditions for different media
+with independent prescribed mass fraction <code>Xi</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 13, 2019 by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BoundarySystemWithXi_in;
diff --git a/AixLib/Fluid/Sources/Validation/Boundary.mo b/AixLib/Fluid/Sources/Validation/Boundary.mo
index 746f2e790b..c0b98fcfb0 100644
--- a/AixLib/Fluid/Sources/Validation/Boundary.mo
+++ b/AixLib/Fluid/Sources/Validation/Boundary.mo
@@ -38,25 +38,25 @@ model Boundary "Validation model for boundary with different media"
     annotation (Placement(transformation(extent={{20,-60},{40,-40}})));
 
     annotation (Documentation(info="<html>
- <p>
- Validation model for <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
- AixLib.Fluid.Sources.Boundary_pT</a>
- for different media.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 13, 2019 by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a>
+for different media.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 13, 2019 by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Validation/Boundary.mos"
         "Simulate and plot"),
 experiment(
       StopTime=1,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Boundary;
diff --git a/AixLib/Fluid/Sources/Validation/BoundaryWithX_in.mo b/AixLib/Fluid/Sources/Validation/BoundaryWithX_in.mo
index 45b7b83ab3..f6f39c3397 100644
--- a/AixLib/Fluid/Sources/Validation/BoundaryWithX_in.mo
+++ b/AixLib/Fluid/Sources/Validation/BoundaryWithX_in.mo
@@ -42,25 +42,25 @@ equation
   connect(X_2.y, bouMoiAirCO2.X_in) annotation (Line(points={{1,76},{10,76},{10,
           40},{18,40}}, color={0,0,127}));
   annotation (Documentation(info="<html>
- <p>
- Validation model for <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
- AixLib.Fluid.Sources.Boundary_pT</a>
- for different media and with mass fraction <code>X</code> prescribed by an input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 13, 2019 by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a>
+for different media and with mass fraction <code>X</code> prescribed by an input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 13, 2019 by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Validation/BoundaryWithX_in.mos"
         "Simulate and plot"),
 experiment(
       StopTime=1,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BoundaryWithX_in;
diff --git a/AixLib/Fluid/Sources/Validation/BoundaryWithXi_in.mo b/AixLib/Fluid/Sources/Validation/BoundaryWithXi_in.mo
index a88f81ceb6..d30fd038f1 100644
--- a/AixLib/Fluid/Sources/Validation/BoundaryWithXi_in.mo
+++ b/AixLib/Fluid/Sources/Validation/BoundaryWithXi_in.mo
@@ -42,25 +42,25 @@ equation
   connect(Xi_1.y, bouMoiAirCO2.Xi_in) annotation (Line(points={{1,76},{10,76},{10,
           40},{18,40}}, color={0,0,127}));
   annotation (Documentation(info="<html>
- <p>
- Validation model for <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
- AixLib.Fluid.Sources.Boundary_pT</a>
- for different media and with independent mass fraction <code>Xi</code> prescribed by an input.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 13, 2019 by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Validation model for <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a>
+for different media and with independent mass fraction <code>Xi</code> prescribed by an input.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 13, 2019 by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1205\">IBPSA, #1205</a>.
+</li>
+</ul>
+</html>"),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Validation/BoundaryWithXi_in.mos"
         "Simulate and plot"),
 experiment(
       StopTime=1,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BoundaryWithXi_in;
diff --git a/AixLib/Fluid/Sources/Validation/Outside_CpData_Directions.mo b/AixLib/Fluid/Sources/Validation/Outside_CpData_Directions.mo
index 5cb4668ee6..30f3213e2a 100644
--- a/AixLib/Fluid/Sources/Validation/Outside_CpData_Directions.mo
+++ b/AixLib/Fluid/Sources/Validation/Outside_CpData_Directions.mo
@@ -74,24 +74,24 @@ equation
   annotation (__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Sources/Validation/Outside_CpData_Directions.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates the use of a source for ambient conditions that computes
- the wind pressure on a facade of a building using a user-defined wind pressure profile.
- In this model, the wind pressure profile is not realistic, but rather it is set to <i>1</i>
- if the wind strikes the surface perpendicular, and otherwise it goes back to <i>0</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 11, 2022, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
- </li>
- </ul>
- </html>"),
+<p>
+This model demonstrates the use of a source for ambient conditions that computes
+the wind pressure on a facade of a building using a user-defined wind pressure profile.
+In this model, the wind pressure profile is not realistic, but rather it is set to <i>1</i>
+if the wind strikes the surface perpendicular, and otherwise it goes back to <i>0</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 11, 2022, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=86400,
-      Tolerance=1e-06),
-  __Dymola_LockedEditing="Model from IBPSA");
+      Tolerance=1e-06), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Outside_CpData_Directions;
diff --git a/AixLib/Fluid/Storage/BaseClasses/Buoyancy.mo b/AixLib/Fluid/Storage/BaseClasses/Buoyancy.mo
index 9a29029420..ceabc7d4e7 100644
--- a/AixLib/Fluid/Storage/BaseClasses/Buoyancy.mo
+++ b/AixLib/Fluid/Storage/BaseClasses/Buoyancy.mo
@@ -39,46 +39,46 @@ equation
   end for;
   heatPort[nSeg].Q_flow = Q_flow[nSeg-1];
   annotation (Documentation(info="<html>
- <p>
- This model outputs a heat flow rate that can be added to fluid volumes
- in order to emulate buoyancy during a temperature inversion.
- For simplicity, this model does not compute a buoyancy induced mass flow rate,
- but rather a heat flow that has the same magnitude as the enthalpy flow
- associated with the buoyancy induced mass flow rate.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Renamed protected parameters for consistency with naming convention.
- </li>
- <li>
- October 8, 2011 by Michael Wetter:<br/>
- Added <code>noEvent(...)</code> to
- <code>Q_flow[i] = k*smooth(1, if dT[i]>0 then dT[i]^2 else 0);</code>
- since the equation returns the same value to the left and right of
- <code>dT[i]>0</code>.
- </li>
- <li>
- September 16, 2011 by Michael Wetter:<br/>
- Changed the implementation from <code>Q_flow[i] = k*max(heatPort[i+1].T-heatPort[i].T, 0);</code> to
- <code>Q_flow[i] = k*smooth(1, if dT[i]>0 then dT[i]^2 else 0);</code>.
- The previous implementation was not differentiable. In modeling a solar system, this
- change reduced the computing time by a factor of 20 during the time when the pumps
- were almost switched off and colder temperature was fed from the collector to the tank.
- </li>
- <li>
- October 28, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model outputs a heat flow rate that can be added to fluid volumes
+in order to emulate buoyancy during a temperature inversion.
+For simplicity, this model does not compute a buoyancy induced mass flow rate,
+but rather a heat flow that has the same magnitude as the enthalpy flow
+associated with the buoyancy induced mass flow rate.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Renamed protected parameters for consistency with naming convention.
+</li>
+<li>
+October 8, 2011 by Michael Wetter:<br/>
+Added <code>noEvent(...)</code> to
+<code>Q_flow[i] = k*smooth(1, if dT[i]>0 then dT[i]^2 else 0);</code>
+since the equation returns the same value to the left and right of
+<code>dT[i]>0</code>.
+</li>
+<li>
+September 16, 2011 by Michael Wetter:<br/>
+Changed the implementation from <code>Q_flow[i] = k*max(heatPort[i+1].T-heatPort[i].T, 0);</code> to
+<code>Q_flow[i] = k*smooth(1, if dT[i]>0 then dT[i]^2 else 0);</code>.
+The previous implementation was not differentiable. In modeling a solar system, this
+change reduced the computing time by a factor of 20 during the time when the pumps
+were almost switched off and colder temperature was fed from the collector to the tank.
+</li>
+<li>
+October 28, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
         graphics={
         Rectangle(
@@ -115,6 +115,6 @@ Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}})
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,127},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Buoyancy;
diff --git a/AixLib/Fluid/Storage/BaseClasses/Examples/IndirectTankHeatExchanger.mo b/AixLib/Fluid/Storage/BaseClasses/Examples/IndirectTankHeatExchanger.mo
index 0b6f56ad97..9dbb796498 100644
--- a/AixLib/Fluid/Storage/BaseClasses/Examples/IndirectTankHeatExchanger.mo
+++ b/AixLib/Fluid/Storage/BaseClasses/Examples/IndirectTankHeatExchanger.mo
@@ -59,40 +59,40 @@ equation
         "Simulate and plot"),
         experiment(Tolerance=1e-6, StopTime=15),
 Documentation(info="<html>
- <p>
- This model provides an example of how the
- <a href=\"modelica://AixLib.Fluid.Storage.BaseClasses.IndirectTankHeatExchanger\">
- AixLib.Fluid.Storage.BaseClasses.IndirectTankHeatExchanger</a>
- model is used. In the model water flows from a flow source through
- the heat exchanger to a low pressure environment. The stagnant fluid on the outside
- of the heat exchanger is modeled as a constant temperature.<br/>
- </p>
- </html>",
+<p>
+This model provides an example of how the
+<a href=\"modelica://AixLib.Fluid.Storage.BaseClasses.IndirectTankHeatExchanger\">
+AixLib.Fluid.Storage.BaseClasses.IndirectTankHeatExchanger</a>
+model is used. In the model water flows from a flow source through
+the heat exchanger to a low pressure environment. The stagnant fluid on the outside
+of the heat exchanger is modeled as a constant temperature.<br/>
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- February 27, 2016 by Michael Wetter:<br/>
- Stored example in a single file rather than a file with multiple examples.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/488\">#488</a>.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- March 27, 2013 by Peter Grant:<br/>
- First implementation
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+February 27, 2016 by Michael Wetter:<br/>
+Stored example in a single file rather than a file with multiple examples.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/488\">#488</a>.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+March 27, 2013 by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IndirectTankHeatExchanger;
diff --git a/AixLib/Fluid/Storage/BaseClasses/IndirectTankHeatExchanger.mo b/AixLib/Fluid/Storage/BaseClasses/IndirectTankHeatExchanger.mo
index 9bb763b758..5c07fea586 100644
--- a/AixLib/Fluid/Storage/BaseClasses/IndirectTankHeatExchanger.mo
+++ b/AixLib/Fluid/Storage/BaseClasses/IndirectTankHeatExchanger.mo
@@ -169,7 +169,7 @@ equation
       color={191,0,0},
       smooth=Smooth.None));
   connect(vol[1].ports[1],senMasFlo.port_b) annotation (Line(
-      points={{-24,-40},{-24,-50},{-60,-50}},
+      points={{-23,-40},{-23,-50},{-60,-50}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(cap.port,HexToTan.solid) annotation (Line(
@@ -185,7 +185,7 @@ equation
       color={191,0,0},
       smooth=Smooth.None));
   connect(temSenHex.T, hAPipIns.T)     annotation (Line(
-      points={{-10,-70},{0,-70},{0,-76},{9,-76}},
+      points={{-9,-70},{0,-70},{0,-76},{9,-76}},
       color={0,0,127},
       smooth=Smooth.None));
   connect(hAPipIns.hA, htfToHex.Gc)     annotation (Line(
@@ -202,12 +202,12 @@ equation
       smooth=Smooth.None));
   connect(temSenSur.T, hANatCyl.TSur)
                                      annotation (Line(
-      points={{20,52},{20,70},{-40,70},{-40,114},{-2,114}},
+      points={{20,53},{20,70},{-40,70},{-40,114},{-2,114}},
       color={0,0,127},
       smooth=Smooth.None));
   connect(hANatCyl.TFlu, temSenWat.T)
                                      annotation (Line(
-      points={{-2,106},{-36,106},{-36,76},{68,76},{68,50}},
+      points={{-2,106},{-36,106},{-36,76},{68,76},{68,51}},
       color={0,0,127},
       smooth=Smooth.None));
   connect(port_a, senMasFlo.port_a) annotation (Line(
@@ -215,7 +215,7 @@ equation
       color={0,127,255},
       smooth=Smooth.None));
   connect(vol[nSeg].ports[2], res.port_a) annotation (Line(
-      points={{-20,-40},{-20,-50},{46,-50}},
+      points={{-21,-40},{-21,-50},{46,-50}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(res.port_b, port_b) annotation (Line(
@@ -238,7 +238,7 @@ equation
             -150},{100,150}}), graphics), Icon(coordinateSystem(
           preserveAspectRatio=false, extent={{-100,-150},{100,150}}), graphics={
         Rectangle(
-          extent={{-66,64},{74,-96}},
+          extent={{-70,64},{70,-96}},
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={95,95,95},
@@ -250,126 +250,126 @@ equation
           fillColor={0,0,255},
           fillPattern=FillPattern.Solid),
         Rectangle(
-          extent={{-66,-12},{74,-18}},
+          extent={{-70,-12},{70,-18}},
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid),
         Rectangle(
-          extent={{-36,64},{-32,-96}},
+          extent={{-40,64},{-36,-96}},
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid),
         Rectangle(
-          extent={{2,64},{6,-96}},
+          extent={{-2,64},{2,-96}},
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid),
         Rectangle(
-          extent={{40,64},{44,-96}},
+          extent={{36,64},{40,-96}},
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid)}),
           defaultComponentName="indTanHex",
         Documentation(info = "<html>
-           <p>
-           This model is a heat exchanger with a moving fluid on one side and a stagnant fluid on the other.
-           It is intended for use when a heat exchanger is submerged in a stagnant fluid.
-           For example, the heat exchanger in a storage tank which is part of a solar thermal system.
-           </p>
-           <p>
-           This component models the fluid in the heat exchanger, convection between the fluid and
-           the heat exchanger, and convection from the heat exchanger to the surrounding fluid.
-           </p>
-           <p>
-           The model is based on <a href=\"AixLib.Fluid.HeatExchangers.BaseClasses.HACoilInside\">
-           AixLib.Fluid.HeatExchangers.BaseClasses.HACoilInside</a> and
-           <a href=\"AixLib.Fluid.HeatExchangers.BaseClasses.HANaturalCylinder\">
-           AixLib.Fluid.HeatExchangers.BaseClasses.HANaturalCylinder</a>.
-           </p>
-           <p>
-           The fluid ports are intended to be connected to a circulated heat transfer fluid
-           while the heat port is intended to be connected to a stagnant fluid.
-           </p>
-           </html>",
+          <p>
+          This model is a heat exchanger with a moving fluid on one side and a stagnant fluid on the other.
+          It is intended for use when a heat exchanger is submerged in a stagnant fluid.
+          For example, the heat exchanger in a storage tank which is part of a solar thermal system.
+          </p>
+          <p>
+          This component models the fluid in the heat exchanger, convection between the fluid and
+          the heat exchanger, and convection from the heat exchanger to the surrounding fluid.
+          </p>
+          <p>
+          The model is based on <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.HACoilInside\">
+          AixLib.Fluid.HeatExchangers.BaseClasses.HACoilInside</a> and
+          <a href=\"modelica://AixLib.Fluid.HeatExchangers.BaseClasses.HANaturalCylinder\">
+          AixLib.Fluid.HeatExchangers.BaseClasses.HANaturalCylinder</a>.
+          </p>
+          <p>
+          The fluid ports are intended to be connected to a circulated heat transfer fluid
+          while the heat port is intended to be connected to a stagnant fluid.
+          </p>
+          </html>",
           revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- April 9, 2021, by Michael Wetter:<br/>
- Corrected placement of <code>each</code> keyword.<br/>
- See <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/2440\">Buildings, PR #2440</a>.
- </li>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- Changed <code>homotopyInitialization</code> to a constant.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
- </li>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- January 7, 2016, by Filip Jorissen:<br/>
- Propagated <code>flowDependent</code> and <code>temperatureDependent</code>
- in <code>hAPipIns</code>.
- This is for issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/454\">#454</a>.
- </li>
- <li>
- September 24, 2015 by Michael Wetter:<br/>
- Set <code>fixed</code> attribute in <code>cap.T</code> to avoid
- unspecified initial conditions.
- </li>
- <li>
- July 2, 2015, by Michael Wetter:<br/>
- Set <code>prescribedHeatFlowRate=false</code> in control volume.
- </li>
- <li>
- July 1, 2015, by Filip Jorissen:<br/>
- Added parameter <code>energyDynamicsSolid</code>.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/434\">
- #434</a>.
- </li>
- <li>
- March 28, 2015, by Filip Jorissen:<br/>
- Propagated <code>allowFlowReversal</code>.
- </li>
-           <li>
-           August 29, 2014, by Michael Wetter:<br/>
-           Introduced <code>MediumTan</code> for the tank medium, and assigned <code>Medium</code>
-           to be equal to <code>MediumHex</code>.
-           This is to correct issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/271\">
-           #271</a>.
-           </li>
-           <li>
-           June 18, 2014, by Michael Wetter:<br/>
-           Set initial equations for <code>cap</code>, and renamed this instance from
-           <code>Cap</code> to <code>cap</code>.
-           This was done to avoid a warning during translation, and to comply with
-           the coding convention.
-           </li>
-           <li>
-           October 8, 2013, by Michael Wetter:<br/>
-           Removed parameter <code>show_V_flow</code>.
-           </li>
-           <li>
-           January 29, 2013, by Peter Grant:<br/>
-           First implementation.
-           </li>
-           </ul>
-           </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+April 9, 2021, by Michael Wetter:<br/>
+Corrected placement of <code>each</code> keyword.<br/>
+See <a href=\"https://github.com/lbl-srg/modelica-buildings/pull/2440\">Buildings, PR #2440</a>.
+</li>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+Changed <code>homotopyInitialization</code> to a constant.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1341\">IBPSA, #1341</a>.
+</li>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+January 7, 2016, by Filip Jorissen:<br/>
+Propagated <code>flowDependent</code> and <code>temperatureDependent</code>
+in <code>hAPipIns</code>.
+This is for issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/454\">#454</a>.
+</li>
+<li>
+September 24, 2015 by Michael Wetter:<br/>
+Set <code>fixed</code> attribute in <code>cap.T</code> to avoid
+unspecified initial conditions.
+</li>
+<li>
+July 2, 2015, by Michael Wetter:<br/>
+Set <code>prescribedHeatFlowRate=false</code> in control volume.
+</li>
+<li>
+July 1, 2015, by Filip Jorissen:<br/>
+Added parameter <code>energyDynamicsSolid</code>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/434\">
+#434</a>.
+</li>
+<li>
+March 28, 2015, by Filip Jorissen:<br/>
+Propagated <code>allowFlowReversal</code>.
+</li>
+          <li>
+          August 29, 2014, by Michael Wetter:<br/>
+          Introduced <code>MediumTan</code> for the tank medium, and assigned <code>Medium</code>
+          to be equal to <code>MediumHex</code>.
+          This is to correct issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/271\">
+          #271</a>.
+          </li>
+          <li>
+          June 18, 2014, by Michael Wetter:<br/>
+          Set initial equations for <code>cap</code>, and renamed this instance from
+          <code>Cap</code> to <code>cap</code>.
+          This was done to avoid a warning during translation, and to comply with
+          the coding convention.
+          </li>
+          <li>
+          October 8, 2013, by Michael Wetter:<br/>
+          Removed parameter <code>show_V_flow</code>.
+          </li>
+          <li>
+          January 29, 2013, by Peter Grant:<br/>
+          First implementation.
+          </li>
+          </ul>
+          </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IndirectTankHeatExchanger;
diff --git a/AixLib/Fluid/Storage/BaseClasses/PartialHeatTransferLayers.mo b/AixLib/Fluid/Storage/BaseClasses/PartialHeatTransferLayers.mo
index 3814f72a48..e5878c71f1 100644
--- a/AixLib/Fluid/Storage/BaseClasses/PartialHeatTransferLayers.mo
+++ b/AixLib/Fluid/Storage/BaseClasses/PartialHeatTransferLayers.mo
@@ -8,7 +8,7 @@ partial model PartialHeatTransferLayers "Partial for storage heat transfer model
       Modelica.Media.Interfaces.PartialMedium "Medium model" annotation(choicesAllMatching);
 
   replaceable parameter
-    AixLib.DataBase.Storage.BufferStorageBaseDataDefinition data=
+    AixLib.DataBase.Storage.StorageDetailedBaseDataDefinition data=
       AixLib.DataBase.Storage.Generic_New_2000l()
       "Storage data record"
     annotation (choicesAllMatching);
diff --git a/AixLib/Fluid/Storage/BaseClasses/PartialStratified.mo b/AixLib/Fluid/Storage/BaseClasses/PartialStratified.mo
index 328ba467d3..0dd1e77e99 100644
--- a/AixLib/Fluid/Storage/BaseClasses/PartialStratified.mo
+++ b/AixLib/Fluid/Storage/BaseClasses/PartialStratified.mo
@@ -1,10 +1,11 @@
 within AixLib.Fluid.Storage.BaseClasses;
 model PartialStratified
   "Partial model of a stratified tank for thermal energy storage"
-  extends AixLib.Fluid.Interfaces.PartialTwoPortInterface;
+  extends AixLib.Fluid.Storage.BaseClasses.PartialTwoPortInterface;
 
   import Modelica.Fluid.Types;
   import Modelica.Fluid.Types.Dynamics;
+
   parameter Modelica.Units.SI.Volume VTan "Tank volume";
   parameter Modelica.Units.SI.Length hTan "Height of tank (without insulation)";
   parameter Modelica.Units.SI.Length dIns "Thickness of insulation";
@@ -76,6 +77,7 @@ model PartialStratified
     each final m_flow_small=m_flow_small,
     each final allowFlowReversal=allowFlowReversal) "Tank segment"
     annotation (Placement(transformation(extent={{6,-16},{26,4}})));
+
 protected
   parameter Medium.ThermodynamicState sta_default = Medium.setState_pTX(
     T=Medium.T_default,
@@ -165,11 +167,11 @@ equation
           {52,74},{20,74}}, color={191,0,0}));
   connect(heaFloBot.port_b, heaPorBot) annotation (Line(points={{42,20},{44,20},
           {44,-74},{20,-74}}, color={191,0,0}));
-  connect(heaFloTop.Q_flow, mul.u1[1]) annotation (Line(points={{36,54},{50,54},
+  connect(heaFloTop.Q_flow, mul.u1[1]) annotation (Line(points={{36,53.4},{50,53.4},
           {50,52.5},{61.2,52.5}}, color={0,0,127}));
-  connect(heaFloSid.Q_flow, mul.u2) annotation (Line(points={{36,34},{50,34},{
-          50,49},{61.2,49}}, color={0,0,127}));
-  connect(heaFloBot.Q_flow, mul.u3[1]) annotation (Line(points={{36,14},{36,10},
+  connect(heaFloSid.Q_flow, mul.u2) annotation (Line(points={{36,33.4},{50,33.4},
+          {50,49},{61.2,49}},color={0,0,127}));
+  connect(heaFloBot.Q_flow, mul.u3[1]) annotation (Line(points={{36,13.4},{36,10},
           {58,10},{58,45.5},{61.2,45.5}}, color={0,0,127}));
   connect(mul.y, sum1.u) annotation (Line(points={{70.4,49},{76.8,49}}, color={
           0,0,127}));
@@ -185,139 +187,139 @@ equation
       smooth=Smooth.None));
   annotation (
 Documentation(info="<html>
- <p>
- This is a partial model of a stratified storage tank.
- </p>
- <p>
- See the
- <a href=\"modelica://AixLib.Fluid.Storage.UsersGuide\">
- AixLib.Fluid.Storage.UsersGuide</a>
- for more information.
- </p>
- <h4>Implementation</h4>
- <p>
- This model does not include the ports that connect to the fluid from
- the outside, because these ports cannot be used for the models that
- contain the
- <a href=\"modelica://AixLib.Fluid.Storage.BaseClasses.ThirdOrderStratifier\">
- AixLib.Fluid.Storage.BaseClasses.ThirdOrderStratifier</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- November 13, 2019 by Jianjun Hu:<br/>
- Added parameter <code>TFlu_start</code> and changed the initial tank segments
- temperature to <code>TFlu_start</code> so each segment could have different
- temperature.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1246\">#1246</a>.
- </li>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- June 1, 2018, by Michael Wetter:<br/>
- Refactored model to allow a fluid port in the tank that do not have
- the enhanced stratification model.<br/>
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1182\">
- issue 1182</a>.
- </li>
- <li>
- July 29, 2017, by Michael Wetter:<br/>
- Removed medium declaration, which is not needed and inconsistent with
- the declaration in the base class.
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/544\">
- issue 544</a>.
- </li>
- <li>
- March 28, 2015, by Filip Jorissen:<br/>
- Propagated <code>allowFlowReversal</code> and <code>m_flow_small</code>
- and set <code>mSenFac=1</code>.
- </li>
- <li>
- January 26, 2015, by Michael Wetter:<br/>
- Renamed
- <code>hA_flow</code> to <code>H_a_flow</code>,
- <code>hB_flow</code> to <code>H_b_flow</code> and
- <code>hVol_flow</code> to <code>H_vol_flow</code>
- as they output enthalpy flow rate, and not specific enthalpy.
- Made various models <code>protected</code>.
- </li>
- <li>
- January 25, 2015, by Michael Wetter:<br/>
- Added <code>final</code> to <code>tau = 0</code> in <code>EnthalpyFlowRate</code>.
- These sensors do not need dynamics as the enthalpy flow rate
- is used to compute a heat flow which is then added to the volume of the tank.
- Thus, if there were high frequency oscillations of small mass flow rates,
- then they have a small effect on <code>H_flow</code>, and they are
- not used in any control loop. Rather, the oscillations are further damped
- by the differential equation of the fluid volume.
- </li>
- <li>
- January 25, 2015, by Filip Jorissen:<br/>
- Set <code>tau = 0</code> in <code>EnthalpyFlowRate</code>
- sensors for increased simulation speed.
- </li>
- <li>
- August 29, 2014, by Michael Wetter:<br/>
- Replaced the use of <code>Medium.lambda_const</code> with
- <code>Medium.thermalConductivity(sta_default)</code> as
- <code>lambda_const</code> is not declared for all media.
- This avoids a translation error if certain media are used.
- </li>
- <li>
- June 18, 2014, by Michael Wetter:<br/>
- Changed the default value for the energy balance initialization to avoid
- a dependency on the global <code>system</code> declaration.
- </li>
- <li>
- July 29, 2011, by Michael Wetter:<br/>
- Removed <code>use_T_start</code> and <code>h_start</code>.
- </li>
- <li>
- February 18, 2011, by Michael Wetter:<br/>
- Changed default start values for temperature and pressure.
- </li>
- <li>
- October 25, 2009 by Michael Wetter:<br/>
- Changed computation of heat transfer through top (and bottom) of tank. Now,
- the thermal resistance of the fluid is not taken into account, i.e., the
- top (and bottom) element is assumed to be mixed.
- </li>
- <li>
- October 23, 2009 by Michael Wetter:<br/>
- Fixed bug in computing heat conduction of top and bottom segment.
- In the previous version,
- for computing the heat conduction between the top (or bottom) segment and
- the outside,
- the whole thickness of the water volume was used
- instead of only half the thickness.
- </li>
- <li>
- February 19, 2009 by Michael Wetter:<br/>
- Changed declaration that constrains the medium. The earlier
- declaration caused the medium model to be not shown in the parameter
- window.
- </li>
- <li>
- October 31, 2008 by Michael Wetter:<br/>
- Added heat conduction.
- </li>
- <li>
- October 23, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This is a partial model of a stratified storage tank.
+</p>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Storage.UsersGuide\">
+AixLib.Fluid.Storage.UsersGuide</a>
+for more information.
+</p>
+<h4>Implementation</h4>
+<p>
+This model does not include the ports that connect to the fluid from
+the outside, because these ports cannot be used for the models that
+contain the
+<a href=\"modelica://AixLib.Fluid.Storage.BaseClasses.ThirdOrderStratifier\">
+AixLib.Fluid.Storage.BaseClasses.ThirdOrderStratifier</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+November 13, 2019 by Jianjun Hu:<br/>
+Added parameter <code>TFlu_start</code> and changed the initial tank segments
+temperature to <code>TFlu_start</code> so each segment could have different
+temperature.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1246\">#1246</a>.
+</li>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+June 1, 2018, by Michael Wetter:<br/>
+Refactored model to allow a fluid port in the tank that do not have
+the enhanced stratification model.<br/>
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1182\">
+issue 1182</a>.
+</li>
+<li>
+July 29, 2017, by Michael Wetter:<br/>
+Removed medium declaration, which is not needed and inconsistent with
+the declaration in the base class.
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/544\">
+issue 544</a>.
+</li>
+<li>
+March 28, 2015, by Filip Jorissen:<br/>
+Propagated <code>allowFlowReversal</code> and <code>m_flow_small</code>
+and set <code>mSenFac=1</code>.
+</li>
+<li>
+January 26, 2015, by Michael Wetter:<br/>
+Renamed
+<code>hA_flow</code> to <code>H_a_flow</code>,
+<code>hB_flow</code> to <code>H_b_flow</code> and
+<code>hVol_flow</code> to <code>H_vol_flow</code>
+as they output enthalpy flow rate, and not specific enthalpy.
+Made various models <code>protected</code>.
+</li>
+<li>
+January 25, 2015, by Michael Wetter:<br/>
+Added <code>final</code> to <code>tau = 0</code> in <code>EnthalpyFlowRate</code>.
+These sensors do not need dynamics as the enthalpy flow rate
+is used to compute a heat flow which is then added to the volume of the tank.
+Thus, if there were high frequency oscillations of small mass flow rates,
+then they have a small effect on <code>H_flow</code>, and they are
+not used in any control loop. Rather, the oscillations are further damped
+by the differential equation of the fluid volume.
+</li>
+<li>
+January 25, 2015, by Filip Jorissen:<br/>
+Set <code>tau = 0</code> in <code>EnthalpyFlowRate</code>
+sensors for increased simulation speed.
+</li>
+<li>
+August 29, 2014, by Michael Wetter:<br/>
+Replaced the use of <code>Medium.lambda_const</code> with
+<code>Medium.thermalConductivity(sta_default)</code> as
+<code>lambda_const</code> is not declared for all media.
+This avoids a translation error if certain media are used.
+</li>
+<li>
+June 18, 2014, by Michael Wetter:<br/>
+Changed the default value for the energy balance initialization to avoid
+a dependency on the global <code>system</code> declaration.
+</li>
+<li>
+July 29, 2011, by Michael Wetter:<br/>
+Removed <code>use_T_start</code> and <code>h_start</code>.
+</li>
+<li>
+February 18, 2011, by Michael Wetter:<br/>
+Changed default start values for temperature and pressure.
+</li>
+<li>
+October 25, 2009 by Michael Wetter:<br/>
+Changed computation of heat transfer through top (and bottom) of tank. Now,
+the thermal resistance of the fluid is not taken into account, i.e., the
+top (and bottom) element is assumed to be mixed.
+</li>
+<li>
+October 23, 2009 by Michael Wetter:<br/>
+Fixed bug in computing heat conduction of top and bottom segment.
+In the previous version,
+for computing the heat conduction between the top (or bottom) segment and
+the outside,
+the whole thickness of the water volume was used
+instead of only half the thickness.
+</li>
+<li>
+February 19, 2009 by Michael Wetter:<br/>
+Changed declaration that constrains the medium. The earlier
+declaration caused the medium model to be not shown in the parameter
+window.
+</li>
+<li>
+October 31, 2008 by Michael Wetter:<br/>
+Added heat conduction.
+</li>
+<li>
+October 23, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 Icon(graphics={
         Rectangle(
           extent={{-40,60},{40,20}},
@@ -331,49 +333,13 @@ Icon(graphics={
           fillColor={0,0,127},
           fillPattern=FillPattern.Solid),
         Rectangle(
-          extent={{-76,2},{-90,-2}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{0,84},{-80,80}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{-76,84},{-80,-2}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{82,0},{78,-86}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{0,84},{-4,60}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{82,-84},{2,-88}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{6,-60},{2,-84}},
+          extent={{2,100},{-2,60}},
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,127},
           fillPattern=FillPattern.Solid),
         Rectangle(
-          extent={{92,2},{78,-2}},
+          extent={{2,-60},{-2,-100}},
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={0,0,127},
@@ -428,6 +394,9 @@ Icon(graphics={
         Line(
           points={{22,-74},{70,-74},{70,72}},
           color={127,0,0},
-          pattern=LinePattern.Dot)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          pattern=LinePattern.Dot),     Text(
+        extent={{-100,100},{-8,70}},
+        textString="%name",
+        textColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialStratified;
diff --git a/AixLib/Fluid/Storage/BaseClasses/PartialTwoPortInterface.mo b/AixLib/Fluid/Storage/BaseClasses/PartialTwoPortInterface.mo
new file mode 100644
index 0000000000..4b13d45bdf
--- /dev/null
+++ b/AixLib/Fluid/Storage/BaseClasses/PartialTwoPortInterface.mo
@@ -0,0 +1,114 @@
+within AixLib.Fluid.Storage.BaseClasses;
+partial model PartialTwoPortInterface
+  "Partial model transporting fluid between two ports without storing mass or energy"
+
+  replaceable package Medium =
+    Modelica.Media.Interfaces.PartialMedium "Medium in the component"
+      annotation (choices(
+        choice(redeclare package Medium = AixLib.Media.Air "Moist air"),
+        choice(redeclare package Medium = AixLib.Media.Water "Water"),
+        choice(redeclare package Medium =
+            AixLib.Media.Antifreeze.PropyleneGlycolWater (
+              property_T=293.15,
+              X_a=0.40)
+              "Propylene glycol water, 40% mass fraction")));
+
+  parameter Boolean allowFlowReversal = true
+    "= false to simplify equations, assuming, but not enforcing, no flow reversal"
+    annotation(Dialog(tab="Assumptions"), Evaluate=true);
+
+  Modelica.Fluid.Interfaces.FluidPort_a port_a(
+    redeclare final package Medium = Medium,
+    m_flow(min=if allowFlowReversal then -Modelica.Constants.inf else 0),
+    p(start=Medium.p_default),
+    h_outflow(start = Medium.h_default, nominal = Medium.h_default))
+    "Fluid connector a (positive design flow direction is from port_a to port_b)"
+    annotation (Placement(transformation(extent={{-10,90},{10,110}})));
+  Modelica.Fluid.Interfaces.FluidPort_b port_b(
+    redeclare final package Medium = Medium,
+    m_flow(max=if allowFlowReversal then +Modelica.Constants.inf else 0),
+    p(start=Medium.p_default),
+    h_outflow(start = Medium.h_default, nominal = Medium.h_default))
+    "Fluid connector b (positive design flow direction is from port_a to port_b)"
+    annotation (Placement(transformation(extent={{10,-110},{-10,-90}})));
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal
+    "Nominal mass flow rate" annotation (Dialog(group="Nominal condition"));
+  parameter Modelica.Units.SI.MassFlowRate m_flow_small(min=0) = 1E-4*abs(
+    m_flow_nominal) "Small mass flow rate for regularization of zero flow"
+    annotation (Dialog(tab="Advanced"));
+  // Diagnostics
+   parameter Boolean show_T = false
+    "= true, if actual temperature at port is computed"
+    annotation (
+      Dialog(tab="Advanced", group="Diagnostics"),
+      HideResult=true);
+
+  Modelica.Units.SI.MassFlowRate m_flow(start=_m_flow_start) = port_a.m_flow
+    "Mass flow rate from port_a to port_b (m_flow > 0 is design flow direction)";
+
+  Modelica.Units.SI.PressureDifference dp(
+    start=_dp_start,
+    displayUnit="Pa") = port_a.p - port_b.p
+    "Pressure difference between port_a and port_b";
+
+  Medium.ThermodynamicState sta_a=
+    if allowFlowReversal then
+      Medium.setState_phX(port_a.p,
+                          noEvent(actualStream(port_a.h_outflow)),
+                          noEvent(actualStream(port_a.Xi_outflow)))
+    else
+      Medium.setState_phX(port_a.p,
+                          noEvent(inStream(port_a.h_outflow)),
+                          noEvent(inStream(port_a.Xi_outflow)))
+      if show_T "Medium properties in port_a";
+
+  Medium.ThermodynamicState sta_b=
+    if allowFlowReversal then
+      Medium.setState_phX(port_b.p,
+                          noEvent(actualStream(port_b.h_outflow)),
+                          noEvent(actualStream(port_b.Xi_outflow)))
+    else
+      Medium.setState_phX(port_b.p,
+                          noEvent(port_b.h_outflow),
+                          noEvent(port_b.Xi_outflow))
+       if show_T "Medium properties in port_b";
+
+protected
+  final parameter Modelica.Units.SI.MassFlowRate _m_flow_start=0
+    "Start value for m_flow, used to avoid a warning if not set in m_flow, and to avoid m_flow.start in parameter window";
+  final parameter Modelica.Units.SI.PressureDifference _dp_start(displayUnit=
+        "Pa") = 0
+    "Start value for dp, used to avoid a warning if not set in dp, and to avoid dp.start in parameter window";
+
+  annotation (
+    preferredView="info",
+    Documentation(info="<html>
+<p>
+This partial class implements the same functionality as 
+<a href=\"modelica://AixLib.Fluid.Interfaces.PartialTwoPortInterface\">
+AixLib.Fluid.Interfaces.PartialTwoPortInterface</a>,
+except that <code>port_a</code> and <code>port_b</code> are placed at the top and bottom
+of the component.
+</p>
+<h4>Implementation</h4>
+<p>
+The implementation is done in this package as opposed to
+<a href=\"modelica://AixLib.Fluid.Interfaces\">
+AixLib.Fluid.Interfaces</a>
+as it is only used by the storage model, and may be removed when the tool limitations
+that are discussed in
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1794\">IBPSA, #1794</a>.
+are removed.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 20, 2023, by Michael Wetter:<br/>
+First implementation to address
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1794\">IBPSA, #1794</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end PartialTwoPortInterface;
diff --git a/AixLib/Fluid/Storage/BaseClasses/ThirdOrderStratifier.mo b/AixLib/Fluid/Storage/BaseClasses/ThirdOrderStratifier.mo
index 484fa40f1a..c1a8027831 100644
--- a/AixLib/Fluid/Storage/BaseClasses/ThirdOrderStratifier.mo
+++ b/AixLib/Fluid/Storage/BaseClasses/ThirdOrderStratifier.mo
@@ -103,68 +103,68 @@ equation
     heatPort[i].Q_flow = Q_flow[i]*alpha;
   end for;
   annotation (Documentation(info="<html>
- <p>
- This model reduces the numerical dissipation that is introduced
- by the standard first-order upwind discretization scheme which is
- created when connecting fluid volumes in series.
- </p>
- <p>
- The model is used in conjunction with
- <a href=\"modelica://AixLib.Fluid.Storage.Stratified\">
- AixLib.Fluid.Storage.Stratified</a>.
- It computes a heat flux that needs to be added to each volume of <a href=\"modelica://AixLib.Fluid.Storage.Stratified\">
- AixLib.Fluid.Storage.Stratified</a> in order to give the results that a third-order upwind discretization scheme (QUICK) would give.
- </p>
- <p>
- The QUICK method can cause oscillations in the tank temperatures since the high order method introduces numerical dispersion.
- There are two ways to reduce the oscillations:</p>
- <ul>
- <li>
- To use an under-relaxation coefficient <code>alpha</code> when adding the heat flux into the volume.
- </li>
- <li>
- To use the first-order upwind for <code>hOut[2]</code> and <code>hOut[nSeg]</code>. Note: Using it requires <code>nSeg &ge; 4</code>.
- </li>
- </ul>
- <p>
- Both approaches are implemented in the model.
- </p>
- <p>
- The model is used by
- <a href=\"modelica://AixLib.Fluid.Storage.StratifiedEnhanced\">
- AixLib.Fluid.Storage.StratifiedEnhanced</a>.
- </p>
- <h4>Limitations</h4>
- <p>
- The model requires at least 4 fluid segments. Hence, set <code>nSeg</code> to 4 or higher.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- December 14, 2012 by Michael Wetter:<br/>
- Removed unused protected parameters <code>sta0</code> and <code>cp0</code>.
- </li>
- <li>
- March 29, 2012 by Wangda Zuo:<br/>
- Revised the implementation to reduce the temperature overshoot.
- </li>
- <li>
- July 28, 2010 by Wangda Zuo:<br/>
- Rewrote third order upwind scheme to avoid state events.
- This leads to more robust and faster simulation.
- </li>
- <li>
- June 23, 2010 by Michael Wetter and Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},
+<p>
+This model reduces the numerical dissipation that is introduced
+by the standard first-order upwind discretization scheme which is
+created when connecting fluid volumes in series.
+</p>
+<p>
+The model is used in conjunction with
+<a href=\"modelica://AixLib.Fluid.Storage.Stratified\">
+AixLib.Fluid.Storage.Stratified</a>.
+It computes a heat flux that needs to be added to each volume of <a href=\"modelica://AixLib.Fluid.Storage.Stratified\">
+AixLib.Fluid.Storage.Stratified</a> in order to give the results that a third-order upwind discretization scheme (QUICK) would give.
+</p>
+<p>
+The QUICK method can cause oscillations in the tank temperatures since the high order method introduces numerical dispersion.
+There are two ways to reduce the oscillations:</p>
+<ul>
+<li>
+To use an under-relaxation coefficient <code>alpha</code> when adding the heat flux into the volume.
+</li>
+<li>
+To use the first-order upwind for <code>hOut[2]</code> and <code>hOut[nSeg]</code>. Note: Using it requires <code>nSeg &ge; 4</code>.
+</li>
+</ul>
+<p>
+Both approaches are implemented in the model.
+</p>
+<p>
+The model is used by
+<a href=\"modelica://AixLib.Fluid.Storage.StratifiedEnhanced\">
+AixLib.Fluid.Storage.StratifiedEnhanced</a>.
+</p>
+<h4>Limitations</h4>
+<p>
+The model requires at least 4 fluid segments. Hence, set <code>nSeg</code> to 4 or higher.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+December 14, 2012 by Michael Wetter:<br/>
+Removed unused protected parameters <code>sta0</code> and <code>cp0</code>.
+</li>
+<li>
+March 29, 2012 by Wangda Zuo:<br/>
+Revised the implementation to reduce the temperature overshoot.
+</li>
+<li>
+July 28, 2010 by Wangda Zuo:<br/>
+Rewrote third order upwind scheme to avoid state events.
+This leads to more robust and faster simulation.
+</li>
+<li>
+June 23, 2010 by Michael Wetter and Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,-100},
             {100,100}}),graphics={
         Rectangle(
           extent={{-48,66},{48,34}},
@@ -182,6 +182,6 @@ equation
           fillColor={0,0,255},
           fillPattern=FillPattern.Solid,
           pattern=LinePattern.None,
-          lineColor={0,0,0})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          lineColor={0,0,0})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThirdOrderStratifier;
diff --git a/AixLib/Fluid/Storage/BaseClasses/package.order b/AixLib/Fluid/Storage/BaseClasses/package.order
index a8d48dfa71..732be0f162 100644
--- a/AixLib/Fluid/Storage/BaseClasses/package.order
+++ b/AixLib/Fluid/Storage/BaseClasses/package.order
@@ -9,6 +9,7 @@ HeatingCoil
 IndirectTankHeatExchanger
 PartialHeatTransferLayers
 PartialStratified
+PartialTwoPortInterface
 StorageCover
 StorageMantle
 ThirdOrderStratifier
diff --git a/AixLib/Fluid/Storage/Examples/ExpansionVessel.mo b/AixLib/Fluid/Storage/Examples/ExpansionVessel.mo
index 94847a3504..523f6003dc 100644
--- a/AixLib/Fluid/Storage/Examples/ExpansionVessel.mo
+++ b/AixLib/Fluid/Storage/Examples/ExpansionVessel.mo
@@ -44,12 +44,18 @@ equation
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/ExpansionVessel.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This model tests a pressure expansion vessel. The medium model that is used in this
- example changes its density as a function of temperature.
- To see the effect of the expansion vessel, delete the connecting line between
- the volume and the expansion vessel and check how much more the pressure increases
- as the fluid is heated.
- </html>"),
-    experiment(Tolerance=1e-6, StopTime=7200),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests a pressure expansion vessel.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 19, 2022 by Hongxiang Fu:<br/>
+Deleted outdated comment in documentation regarding compressible fluid.
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3198\">#3198</a>.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=7200), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ExpansionVessel;
diff --git a/AixLib/Fluid/Storage/Examples/StorageBoiler.mo b/AixLib/Fluid/Storage/Examples/StorageBoiler.mo
index 86243dbfa9..264d6730ad 100644
--- a/AixLib/Fluid/Storage/Examples/StorageBoiler.mo
+++ b/AixLib/Fluid/Storage/Examples/StorageBoiler.mo
@@ -1,14 +1,13 @@
 within AixLib.Fluid.Storage.Examples;
 model StorageBoiler
   extends Modelica.Icons.Example;
-  import AixLib;
 
   replaceable package Medium =
      Modelica.Media.Water.ConstantPropertyLiquidWater
      constrainedby Modelica.Media.Interfaces.PartialMedium;
 
-  AixLib.Fluid.Storage.BufferStorage
-                               bufferStorage(
+  AixLib.Fluid.Storage.StorageDetailed bufferStorage(
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     redeclare package MediumHC1 = Medium,
     redeclare package MediumHC2 = Medium,
     m1_flow_nominal=pipe1.m_flow_nominal,
@@ -16,6 +15,7 @@ model StorageBoiler
     mHC1_flow_nominal=pipe1.m_flow_nominal,
     useHeatingCoil2=false,
     useHeatingRod=false,
+    TStart=fill(343.15, 10),
     redeclare AixLib.DataBase.Storage.Generic_New_2000l data(
       hTank=2,
       hUpperPortDemand=1.95,
@@ -27,89 +27,103 @@ model StorageBoiler
     hConIn=1500,
     hConOut=15,
     redeclare package Medium = Medium,
-    hConHC1=300)                       annotation (Placement(transformation(extent={{6,8},{
-            -18,38}})));
-  Modelica.Thermal.HeatTransfer.Sources.FixedTemperature fixedTemperature(T = 283.15) annotation(Placement(transformation(extent={{-56,12},
-            {-36,32}})));
-  AixLib.Obsolete.Year2021.Fluid.Movers.Pump pump(redeclare package Medium = Medium, m_flow_small=1e-4) annotation (Placement(transformation(
-        extent={{-10,-10},{10,10}},
-        rotation=270,
-        origin={6,60})));
-  AixLib.Fluid.Sources.Boundary_pT
-                     boundary_p(nPorts=1, redeclare package Medium = Medium)
-                                annotation(Placement(transformation(extent={{-48,68},
-            {-28,88}})));
-  Modelica.Blocks.Sources.BooleanExpression booleanExpression annotation(Placement(transformation(extent = {{-10, -10}, {10, 10}}, rotation = 180, origin={46,48})));
-  Modelica.Blocks.Sources.Constant const(k = 273.15 + 80) annotation(Placement(transformation(extent = {{-3, -3}, {3, 3}}, rotation = 180, origin={61,67})));
+    hConHC1=300) annotation (Placement(transformation(extent={{6,-14},{-18,16}})));
+  Modelica.Thermal.HeatTransfer.Sources.FixedTemperature fixedTemperature(T = 283.15)
+  annotation(Placement(transformation(extent={{-56,-10},{-36,10}})));
+  AixLib.Fluid.Sources.Boundary_pT boundary_p(redeclare package Medium = Medium,nPorts=1)
+	annotation(Placement(transformation(extent={{-48,46},{-28,66}})));
+  Modelica.Blocks.Sources.Constant SetTemp(k=273.15 + 80) annotation (Placement(
+        transformation(
+        extent={{-7,-7},{7,7}},
+        rotation=180,
+        origin={65,69})));
   AixLib.Fluid.FixedResistances.PressureDrop pipe(
     redeclare package Medium = Medium,
     m_flow_nominal=0.5,
     dp_nominal=200)
-    annotation (Placement(transformation(extent={{12,-12},{32,8}})));
-  AixLib.Fluid.FixedResistances.HydraulicResistance
-                                           hydraulicResistance(zeta = 1000,
+    annotation (Placement(transformation(extent={{18,-34},{38,-14}})));
+  AixLib.Fluid.FixedResistances.HydraulicResistance hydraulicResistance(zeta = 1000,
     redeclare package Medium = Medium,
     diameter=0.05,
-    m_flow_nominal=0.001)                                                   annotation(Placement(transformation(extent={{46,-12},
-            {66,8}})));
-  AixLib.Fluid.Sources.Boundary_ph
-                      boundary_ph1(use_p_in = true, h = 0.8e5,
+    m_flow_nominal=0.001) annotation(Placement(transformation(extent={{46,-34},
+            {66,-14}})));
+  AixLib.Fluid.Sources.Boundary_ph boundary_ph1(use_p_in = true,
+	h = 0.8e5,
     nPorts=1,
-    redeclare package Medium = Medium)                         annotation(Placement(transformation(extent={{-66,-22},
-            {-46,-2}})));
-  Modelica.Blocks.Sources.Ramp ramp(duration = 1000,               height = 0.00001e5,
-    offset=101325)                                                                     annotation(Placement(transformation(extent={{-96,-14},
-            {-76,6}})));
-  AixLib.Fluid.Sources.Boundary_pT
-                      boundary_ph2(nPorts=1, redeclare package Medium = Medium)
-                                                     annotation(Placement(transformation(extent = {{10, -10}, {-10, 10}}, rotation = 180, origin={-38,56})));
+    redeclare package Medium = Medium)
+	annotation(Placement(transformation(extent={{-66,-44},{-46,-24}})));
+  Modelica.Blocks.Sources.Ramp ramp(duration = 1000,
+	height = 0.00001e5,
+    offset=101325) annotation(Placement(transformation(extent={{-96,-36},{-76,-16}})));
+  AixLib.Fluid.Sources.Boundary_pT boundary_ph2(nPorts=1,
+					  redeclare package Medium = Medium)
+					  annotation(Placement(transformation(extent = {{10, -10}, {-10, 10}}, rotation = 180, origin={-38,34})));
   AixLib.Fluid.FixedResistances.PressureDrop pipe1(
     redeclare package Medium = Medium,
     m_flow_nominal=0.5,
     dp_nominal=200)
-    annotation (Placement(transformation(extent={{-36,-22},{-16,-2}})));
+    annotation (Placement(transformation(extent={{-36,-44},{-16,-24}})));
   AixLib.Fluid.HeatExchangers.Heater_T       hea(
     redeclare package Medium = Medium,
     m_flow_nominal=0.01,
     dp_nominal=0)
-    annotation (Placement(transformation(extent={{42,68},{22,88}})));
+    annotation (Placement(transformation(extent={{42,46},{22,66}})));
+  AixLib.Fluid.Movers.FlowControlled_dp pump(redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+    T_start=298.15,
+      m_flow_nominal=pipe1.m_flow_nominal,
+    per(pressure(V_flow={0,pipe.m_flow_nominal/1000,pipe.m_flow_nominal/(1000*
+            0.8)}, dp={dpSet.k/0.8,dpSet.k,0}), motorCooledByFluid=false))
+		annotation (Placement(transformation(extent={{10,10},{-10,-10}},rotation=90,origin={2,42})));
+  Modelica.Blocks.Sources.Constant dpSet(k=40000)
+    "Constant set pressure difference for pump" annotation (Placement(
+        transformation(
+        extent={{-7,-7},{7,7}},
+        rotation=180,
+        origin={37,27})));
 equation
-  connect(booleanExpression.y, pump.IsNight) annotation(Line(points={{35,48},{
-          24,48},{24,60},{16.2,60}},                                                                                 color = {255, 0, 255}));
-  connect(pipe.port_b, hydraulicResistance.port_a) annotation(Line(points={{32,-2},
-          {46,-2}},                                                                            color = {0, 127, 255}));
-  connect(ramp.y, boundary_ph1.p_in) annotation(Line(points={{-75,-4},{-68,-4}},        color = {0, 0, 127}));
+  connect(pipe.port_b, hydraulicResistance.port_a) annotation(Line(points={{38,-24},
+          {46,-24}},color = {0, 127, 255}));
+  connect(ramp.y, boundary_ph1.p_in) annotation(Line(points={{-75,-26},{-68,-26}},color = {0, 0, 127}));
   connect(boundary_ph1.ports[1], pipe1.port_a) annotation (Line(
-      points={{-46,-12},{-36,-12}},
+      points={{-46,-34},{-36,-34}},
       color={0,127,255}));
-  connect(boundary_p.ports[1], pump.port_a) annotation (Line(
-      points={{-28,78},{6,78},{6,70}},
-      color={0,127,255}));
-  connect(pump.port_a, hea.port_b) annotation (Line(points={{6,70},{6,70},{6,78},
-          {6,78},{22,78}}, color={0,127,255}));
-  connect(hydraulicResistance.port_b, hea.port_a) annotation (Line(points={{66,
-          -2},{80,-2},{80,78},{42,78}}, color={0,127,255}));
-  connect(const.y, hea.TSet) annotation (Line(points={{57.7,67},{52,67},{52,86},
-          {44,86}}, color={0,0,127}));
+  connect(hydraulicResistance.port_b, hea.port_a) annotation (Line(points={{66,-24},
+          {80,-24},{80,56},{42,56}},    color={0,127,255}));
+  connect(SetTemp.y, hea.TSet) annotation (Line(points={{57.3,69},{52,69},{52,
+          64},{44,64}}, color={0,0,127}));
   connect(boundary_ph2.ports[1], bufferStorage.fluidportTop2) annotation (Line(
-        points={{-28,56},{-9.75,56},{-9.75,38.15}}, color={0,127,255}));
-  connect(bufferStorage.fluidportBottom2, pipe1.port_b) annotation (Line(points=
-         {{-9.45,7.85},{-9.45,-2},{-10,-2},{-10,-12},{-16,-12}}, color={0,127,
+        points={{-28,34},{-9.75,34},{-9.75,16.15}}, color={0,127,255}));
+  connect(bufferStorage.fluidportBottom2, pipe1.port_b) annotation (Line(points={{-9.45,
+          -14.15},{-9.45,-24},{-10,-24},{-10,-34},{-16,-34}},    color={0,127,
           255}));
-  connect(pipe.port_a, bufferStorage.portHC1Out) annotation (Line(points={{12,
-          -2},{14,-2},{14,26.9},{6.15,26.9}}, color={0,127,255}));
-  connect(pump.port_b, bufferStorage.portHC1In) annotation (Line(points={{6,50},
-          {6,44},{12,44},{12,31.55},{6.3,31.55}}, color={0,127,255}));
+  connect(pipe.port_a, bufferStorage.portHC1Out) annotation (Line(points={{18,-24},
+          {18,4.9},{6.15,4.9}},               color={0,127,255}));
   connect(fixedTemperature.port, bufferStorage.heatportOutside) annotation (
-      Line(points={{-36,22},{-28,22},{-28,23.9},{-17.7,23.9}}, color={191,0,0}));
+      Line(points={{-36,0},{-28,0},{-28,1.9},{-17.7,1.9}},     color={191,0,0}));
+  connect(pump.port_b, bufferStorage.portHC1In) annotation (Line(points={{2,32},
+          {2,26},{14,26},{14,9.55},{6.3,9.55}}, color={0,127,255}));
+  connect(pump.port_a, hea.port_b)
+    annotation (Line(points={{2,52},{2,56},{22,56}}, color={0,127,255}));
+  connect(boundary_p.ports[1], pump.port_a) annotation (Line(points={{-28,56},{
+          -18,56},{-18,58},{0,58},{0,52},{2,52}}, color={0,127,255}));
+  connect(dpSet.y, pump.dp_in) annotation (Line(points={{29.3,27},{30,27},{30,
+          28},{24,28},{24,42},{14,42}}, color={0,0,127}));
   annotation (experiment(Tolerance=1e-6, StopTime=86400, Interval=60),
-    Documentation(info = "<html><h4>
-  <span style=\"color:#008000\">Overview</span>
-</h4>
+   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageBoiler.mos" "Simulate and plot"),
+    Documentation(
+    info="<html>
 <p>
-  This is a simple example of a storage and a boiler.
+  This is a simple example of a storage and an ideal heater.<br/>
+  The ideal heater has a constant supply temperature and supplies heat
+  to a thermal energy water storage.<br/>
+  The pressure boundary is an idealized consumer with a pressure ramp.
 </p>
 <ul>
+  <li>
+    <i>November 14, 2022</i> by Laura Maier:<br/>
+    Added simulate and plot scripts, add docu and adapt parameters.
+  </li>
   <li>
     <i>December 08, 2016&#160;</i> by Moritz Lauster:<br/>
     Adapted to AixLib conventions
diff --git a/AixLib/Fluid/Storage/Examples/BufferStorage.mo b/AixLib/Fluid/Storage/Examples/StorageDetailedExample.mo
similarity index 82%
rename from AixLib/Fluid/Storage/Examples/BufferStorage.mo
rename to AixLib/Fluid/Storage/Examples/StorageDetailedExample.mo
index 2fad30207e..430be90748 100644
--- a/AixLib/Fluid/Storage/Examples/BufferStorage.mo
+++ b/AixLib/Fluid/Storage/Examples/StorageDetailedExample.mo
@@ -1,12 +1,11 @@
 within AixLib.Fluid.Storage.Examples;
-model BufferStorage
+model StorageDetailedExample "Simple usage example for StorageDetailed"
 
   extends Modelica.Icons.Example;
-  import AixLib;
   replaceable package Medium =
      Modelica.Media.Water.ConstantPropertyLiquidWater
      constrainedby Modelica.Media.Interfaces.PartialMedium;
-  AixLib.Fluid.Storage.BufferStorage bufferStorage(
+  AixLib.Fluid.Storage.StorageDetailed bufferStorage(
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     massDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial,
     m1_flow_nominal=const.k,
@@ -24,7 +23,8 @@ model BufferStorage
         AixLib.Fluid.Storage.BaseClasses.HeatTransferBuoyancyWetter,
     redeclare package MediumHC1 = Medium,
     redeclare package MediumHC2 = Medium,
-    TStart=303.15) annotation (Placement(transformation(extent={{0,0},{-20,24}})));
+    TStart={333.15,328.15,323.15,318.15,313.15,308.15,303.15,298.15,293.15,293.15})
+    annotation (Placement(transformation(extent={{0,0},{-20,24}})));
   Modelica.Thermal.HeatTransfer.Sources.FixedTemperature fixedTemperature(T=283.15)   annotation(Placement(transformation(extent={{-58,4},
             {-38,24}})));
   AixLib.Fluid.Sources.MassFlowSource_T boundary(
@@ -37,8 +37,8 @@ model BufferStorage
         rotation=180,
         origin={22,46})));
   AixLib.Fluid.Sources.Boundary_pT
-                      boundary_ph5(          redeclare package Medium = Medium,
-      nPorts=1)                                      annotation(Placement(transformation(extent = {{10, -10}, {-10, 10}}, rotation=0,     origin={12,-20})));
+                      boundary_ph5(redeclare package Medium = Medium,
+      nPorts=1) annotation(Placement(transformation(extent = {{10, -10}, {-10, 10}}, rotation=0,     origin={12,-20})));
   AixLib.Fluid.Sources.MassFlowSource_T boundary1(
     m_flow=0,
     redeclare package Medium = Medium,
@@ -70,11 +70,12 @@ model BufferStorage
         origin={14,20})));
   AixLib.Fluid.Sources.Boundary_pT
                       boundary_ph1(redeclare package Medium = Medium, nPorts=1)
-                                                     annotation(Placement(transformation(extent={{5,-5},{-5,5}},          rotation=0,     origin={13,7})));
+    annotation(Placement(transformation(extent={{5,-5},{-5,5}},rotation=0,origin={13,7})));
 equation
   connect(boundary.m_flow_in, const.y)
     annotation (Line(points={{34,38},{34,38},{51,38}}, color={0,0,127}));
-  connect(boundary1.ports[1], bufferStorage.fluidportTop2) annotation (Line(points={{-34,46},{-14,46},{-14,24.12},{-13.125,24.12}}, color={0,127,255}));
+  connect(boundary1.ports[1], bufferStorage.fluidportTop2) annotation (Line(points={{-34,46},
+          {-14,46},{-14,24.12},{-13.125,24.12}},color={0,127,255}));
   connect(bufferStorage.fluidportTop1, boundary.ports[1]) annotation (Line(points={{-6.5,24.12},{-6.5,45.06},{12,45.06},{12,46}}, color={0,127,255}));
   connect(bufferStorage.fluidportBottom1, boundary_ph5.ports[1]) annotation (Line(points={{-6.625,-0.24},{-6.625,-20.12},{2,-20.12},{2,-20}}, color={0,127,255}));
   connect(boundary2.ports[1], bufferStorage.fluidportBottom2) annotation (Line(points={{-36,-20},{-14,-20},{-14,-0.12},{-12.875,-0.12}}, color={0,127,255}));
@@ -85,7 +86,7 @@ equation
     Icon(coordinateSystem(preserveAspectRatio=false)),
     Diagram(coordinateSystem(preserveAspectRatio=false)),
     experiment(Tolerance=1e-6, StopTime=86400, Interval=60),
-    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/BufferStorage.mos" "Simulate and plot"),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageDetailedExample.mos" "Simulate and plot"),
     Documentation(info="<html><p>
   <b><span style=\"color: #008000;\">Overview</span></b>
 </p>
@@ -94,6 +95,10 @@ equation
   mass flow with a higher temperature than the initial temperature.
 </p>
 <ul>
+  <li>November 14, 2022, by Laura Maier:<br/>
+    <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1223\">#1223</a>:
+    Parameter tuning and refactoring.
+  </li>
   <li>November 27, 2019, by Philipp Mehrfeld:<br/>
     <a href=\"https://github.com/RWTH-EBC/AixLib/issues/793\">#793</a>:
     Add one heating coil to example.
@@ -104,4 +109,4 @@ equation
   </li>
 </ul>
 </html>"));
-end BufferStorage;
+end StorageDetailedExample;
diff --git a/AixLib/Fluid/Storage/Examples/StorageSimpleExample.mo b/AixLib/Fluid/Storage/Examples/StorageSimpleExample.mo
new file mode 100644
index 0000000000..06091af0e3
--- /dev/null
+++ b/AixLib/Fluid/Storage/Examples/StorageSimpleExample.mo
@@ -0,0 +1,288 @@
+within AixLib.Fluid.Storage.Examples;
+model StorageSimpleExample "Example model with simple storage"
+  extends Modelica.Icons.Example;
+  StorageSimple storageSimple(
+    redeclare package Medium = Medium,
+    use_TOut=true,
+    n=3,
+    d=0.7,
+    h=0.78,
+    lambda_ins=0.032,
+    s_ins=0.01,
+    hConIn=1500,
+    hConOut=15,
+    V_HE=0.04,
+    k_HE=1500,
+    A_HE=10,
+    m_flow_nominal_layer=m_flow_nominal_gen,
+    m_flow_nominal_HE=m_flow_nominal_gen,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    T_start=fill(308.15, 3))
+    "300 l storage"
+    annotation (Placement(transformation(extent={{22,-22},{-20,22}})));
+  HeatExchangers.HeatingRod heatingRod(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal_gen,
+    dp_nominal=dp_nominal_hr,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    Q_flow_nominal=8000,
+    V=0.01,
+    eta=0.98,
+    use_countNumSwi=false)
+              annotation (Placement(transformation(extent={{-70,12},{-50,32}})));
+  replaceable package Medium = AixLib.Media.Water
+    annotation (choicesAllMatching=true);
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal_gen=
+  heatingRod.Q_flow_nominal/(dT_gen*Medium.cp_const)
+  "Nominal mass flow rate in generation cycle";
+
+  parameter Modelica.Units.SI.PressureDifference dp_nominal_hr = 1000
+    "Pressure difference in heating rod";
+
+  parameter Modelica.Units.SI.TemperatureDifference dT_gen = 8
+  "Temperature difference in generation cycle";
+
+  parameter Real bandwidth=5 "Bandwidth around reference signal";
+
+  AixLib.Systems.HydraulicModules.SimpleConsumer simpleConsumer(
+    redeclare package Medium = Medium,
+    kA=heatingRod.Q_flow_nominal/dT_gen,
+    V=0.2,
+    m_flow_nominal=m_flow_nominal_gen,
+    functionality="Q_flow_input") annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=-90,
+        origin={62,4})));
+  AixLib.Fluid.Sources.Boundary_pT pressureBoundary(
+    redeclare package Medium = Medium,
+    p=200000,
+    nPorts=1)
+    annotation (Placement(transformation(extent={{-24,-52},{-38,-38}})));
+  AixLib.Fluid.Movers.SpeedControlled_y pumpGen(redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+      redeclare
+      AixLib.Fluid.Movers.Data.Pumps.Wilo.CronolineIL80slash220dash4slash4 per)
+    annotation (Placement(transformation(extent={{-48,-20},{-68,-40}})));
+  AixLib.Fluid.Movers.SpeedControlled_y pumpCon(redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+      redeclare
+      AixLib.Fluid.Movers.Data.Pumps.Wilo.CronolineIL80slash220dash4slash4 per)
+    "Consumer pump"
+    annotation (Placement(transformation(extent={{44,-20},{24,-40}})));
+  AixLib.Fluid.Sources.Boundary_pT pressureBoundary1(
+    redeclare package Medium = Medium,
+    p=200000,
+    nPorts=1) annotation (Placement(transformation(extent={{70,-52},{56,-38}})));
+  Modelica.Blocks.Logical.OnOffController storageHysteresis(bandwidth=bandwidth,
+      pre_y_start=true)
+    annotation (Placement(transformation(extent={{-72,54},{-60,66}})));
+  AixLib.Controls.Continuous.LimPID PIDHR(
+    controllerType=Modelica.Blocks.Types.SimpleController.PI,
+    Ti=10,
+    yMax=1,
+    yMin=0,
+    initType=Modelica.Blocks.Types.Init.InitialOutput,
+    xi_start=1) "PID controller for heating rod"
+    annotation (Placement(transformation(extent={{-54,78},{-38,94}})));
+  Modelica.Blocks.Logical.Switch HROffOrPI
+    annotation (Placement(transformation(extent={{-22,62},{-12,72}})));
+  Modelica.Blocks.Sources.Constant TUpperHysteresis(k=273.15 + 40)
+    annotation (Placement(transformation(extent={{-98,60},{-84,74}})));
+  Modelica.Blocks.Interfaces.RealOutput PelHR
+    "Electrical power used to provide current heat flow"
+    annotation (Placement(transformation(extent={{76,46},{96,66}})));
+  Modelica.Blocks.Sources.Cosine dailyHeatDemand(
+    amplitude=-2000,
+    f=1/86400,
+    phase=3.1415926535898,
+    offset=-4000)
+                 annotation (Placement(transformation(extent={{96,10},{82,24}})));
+  Modelica.Blocks.Sources.Constant Off(k=0)
+    annotation (Placement(transformation(extent={{-44,52},{-36,60}})));
+  Modelica.Thermal.HeatTransfer.Celsius.FixedTemperature fixedTemperature(T=18)
+    annotation (Placement(transformation(extent={{40,-6},{28,6}})));
+  Modelica.Blocks.Logical.LessThreshold    greaterZero
+    annotation (Placement(transformation(extent={{18,-88},{30,-76}})));
+  AixLib.Fluid.Sensors.MassFlowRate senMasFlo_gen(redeclare package Medium = Medium)
+    "Mass flow rate sensor at generation side" annotation (Placement(
+        transformation(
+        extent={{-7,-7},{7,7}},
+        rotation=90,
+        origin={-87,-17})));
+  Controls.Continuous.LimPID PIDPumpGen(
+    controllerType=Modelica.Blocks.Types.SimpleController.PI,
+    k=0.5,
+    Ti=10,
+    yMax=1,
+    yMin=0,
+    initType=Modelica.Blocks.Types.Init.InitialOutput,
+    xi_start=1) "PID controller for generation system pump"
+    annotation (Placement(transformation(extent={{-68,-86},{-56,-74}})));
+  AixLib.Fluid.Sensors.MassFlowRate senMasFlo_con(redeclare package Medium = Medium)
+    "Mass fow rate sensor at consumer side" annotation (Placement(
+        transformation(
+        extent={{-7,-7},{7,7}},
+        rotation=0,
+        origin={47,37})));
+  Modelica.Blocks.Sources.Constant m_flow_set(k=m_flow_nominal_gen)
+    "Set mass flow rate"
+    annotation (Placement(transformation(extent={{-96,-88},{-82,-74}})));
+  Controls.Continuous.LimPID PIDPumpCon(
+    controllerType=Modelica.Blocks.Types.SimpleController.PI,
+    yMax=1,
+    yMin=0,
+    initType=Modelica.Blocks.Types.Init.InitialOutput,
+    xi_start=1) "PID controller for consumer pump"
+    annotation (Placement(transformation(extent={{44,-64},{56,-76}})));
+  Modelica.Blocks.Logical.Switch PumpOnOffCon
+    annotation (Placement(transformation(extent={{70,-90},{84,-76}})));
+  Modelica.Blocks.Sources.Constant Offpump(k=0)
+    annotation (Placement(transformation(extent={{48,-94},{56,-86}})));
+  Modelica.Blocks.Logical.Switch PumpOnOffGen
+    annotation (Placement(transformation(extent={{-28,-90},{-14,-76}})));
+  Modelica.Blocks.Math.Add add
+    annotation (Placement(transformation(extent={{-72,80},{-62,90}})));
+  Modelica.Blocks.Sources.Constant addToSetTemp(k=bandwidth/2)
+    annotation (Placement(transformation(extent={{-96,82},{-88,90}})));
+
+  FixedResistances.PressureDrop res(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal_gen,
+    dp_nominal=20000) annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={-88,6})));
+  FixedResistances.PressureDrop res1(
+    redeclare package Medium = Medium,
+    m_flow_nominal=m_flow_nominal_gen,
+    dp_nominal=20000) annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=0,
+        origin={22,36})));
+equation
+  connect(heatingRod.port_b, storageSimple.port_a_heatGenerator) annotation (
+      Line(points={{-50,22},{-30,22},{-30,19.36},{-16.64,19.36}}, color={0,127,255}));
+  connect(pumpGen.port_a, storageSimple.port_b_heatGenerator) annotation (Line(
+        points={{-48,-30},{-26,-30},{-26,-17.6},{-16.64,-17.6}}, color={0,127,255}));
+  connect(pressureBoundary.ports[1], pumpGen.port_a) annotation (Line(points={{-38,
+          -45},{-42,-45},{-42,-30},{-48,-30}}, color={0,127,255}));
+  connect(pumpCon.port_b, storageSimple.port_a_consumer)
+    annotation (Line(points={{24,-30},{1,-30},{1,-22}}, color={0,127,255}));
+  connect(pressureBoundary1.ports[1], pumpCon.port_a)
+    annotation (Line(points={{56,-45},{56,-30},{44,-30}}, color={0,127,255}));
+  connect(simpleConsumer.port_b, pumpCon.port_a)
+    annotation (Line(points={{62,-6},{62,-30},{44,-30}}, color={0,127,255}));
+  connect(storageHysteresis.y, HROffOrPI.u2) annotation (Line(points={{-59.4,60},
+          {-59.4,67},{-23,67}}, color={255,0,255}));
+  connect(HROffOrPI.y, heatingRod.u) annotation (Line(points={{-11.5,67},{-8,67},
+          {-8,38},{-84,38},{-84,28},{-72,28}}, color={0,0,127}));
+  connect(PIDHR.y, HROffOrPI.u1) annotation (Line(points={{-37.2,86},{-32,86},{
+          -32,71},{-23,71}}, color={0,0,127}));
+  connect(TUpperHysteresis.y, storageHysteresis.reference) annotation (Line(
+        points={{-83.3,67},{-83.3,64},{-74,64},{-74,63.6},{-73.2,63.6}},
+                                                                color={0,0,127}));
+  connect(heatingRod.Pel, PelHR) annotation (Line(points={{-49,28},{-2,28},{-2,56},
+          {86,56}}, color={0,0,127}));
+  connect(dailyHeatDemand.y, simpleConsumer.Q_flow) annotation (Line(points={{81.3,17},
+          {75.65,17},{75.65,10},{72,10}},   color={0,0,127}));
+  connect(Off.y, HROffOrPI.u3) annotation (Line(points={{-35.6,56},{-35.6,63},{-23,
+          63}}, color={0,0,127}));
+  connect(fixedTemperature.port, storageSimple.heatPort)
+    annotation (Line(points={{28,0},{17.8,0}}, color={191,0,0}));
+  connect(dailyHeatDemand.y, greaterZero.u) annotation (Line(points={{81.3,17},{
+          68,17},{68,34},{100,34},{100,-100},{12,-100},{12,-82},{16.8,-82}},
+        color={0,0,127}));
+  connect(pumpGen.port_b, senMasFlo_gen.port_a) annotation (Line(points={{-68,-30},
+          {-87,-30},{-87,-24}}, color={0,127,255}));
+  connect(senMasFlo_con.port_b, simpleConsumer.port_a)
+    annotation (Line(points={{54,37},{62,37},{62,14}}, color={0,127,255}));
+  connect(m_flow_set.y, PIDPumpGen.u_s) annotation (Line(points={{-81.3,-81},{-76,
+          -81},{-76,-80},{-69.2,-80}}, color={0,0,127}));
+  connect(senMasFlo_gen.m_flow, PIDPumpGen.u_m) annotation (Line(points={{-94.7,
+          -17},{-100,-17},{-100,-100},{-62,-100},{-62,-87.2}}, color={0,0,127}));
+  connect(m_flow_set.y, PIDPumpCon.u_s) annotation (Line(points={{-81.3,-81},{-40,
+          -81},{-40,-66},{2,-66},{2,-70},{42.8,-70}}, color={0,0,127}));
+  connect(PIDPumpCon.y, PumpOnOffCon.u1) annotation (Line(points={{56.6,-70},{
+          60,-70},{60,-77.4},{68.6,-77.4}}, color={0,0,127}));
+  connect(greaterZero.y, PumpOnOffCon.u2) annotation (Line(points={{30.6,-82},{68.6,
+          -82},{68.6,-83}}, color={255,0,255}));
+  connect(Offpump.y, PumpOnOffCon.u3) annotation (Line(points={{56.4,-90},{62,-90},
+          {62,-88.6},{68.6,-88.6}}, color={0,0,127}));
+  connect(PumpOnOffCon.y, pumpCon.y) annotation (Line(points={{84.7,-83},{90,-83},
+          {90,-60},{34,-60},{34,-42}}, color={0,0,127}));
+  connect(senMasFlo_con.m_flow, PIDPumpCon.u_m) annotation (Line(points={{47,
+          44.7},{47,40},{100,40},{100,-60},{50,-60},{50,-62.8}}, color={0,0,127}));
+  connect(PIDPumpGen.y, PumpOnOffGen.u1) annotation (Line(points={{-55.4,-80},{
+          -52,-80},{-52,-72},{-38,-72},{-38,-76},{-29.4,-76},{-29.4,-77.4}},
+        color={0,0,127}));
+  connect(storageHysteresis.y, PumpOnOffGen.u2) annotation (Line(points={{-59.4,
+          60},{-58,60},{-58,50},{-100,50},{-100,-100},{-40,-100},{-40,-83},{-29.4,
+          -83}}, color={255,0,255}));
+  connect(PumpOnOffGen.y, pumpGen.y) annotation (Line(points={{-13.3,-83},{-8,-83},
+          {-8,-60},{-58,-60},{-58,-42}}, color={0,0,127}));
+  connect(Offpump.y, PumpOnOffGen.u3) annotation (Line(points={{56.4,-90},{60,-90},
+          {60,-100},{-44,-100},{-44,-88.6},{-29.4,-88.6}}, color={0,0,127}));
+  connect(add.y, PIDHR.u_s) annotation (Line(points={{-61.5,85},{-61.5,86},{-55.6,
+          86}}, color={0,0,127}));
+  connect(TUpperHysteresis.y, add.u2) annotation (Line(points={{-83.3,67},{-82,67},
+          {-82,82},{-73,82}}, color={0,0,127}));
+  connect(addToSetTemp.y, add.u1) annotation (Line(points={{-87.6,86},{-87.6,88},
+          {-73,88}}, color={0,0,127}));
+  connect(senMasFlo_gen.port_b, res.port_a) annotation (Line(points={{-87,-10},
+          {-87,-7},{-88,-7},{-88,-4}}, color={0,127,255}));
+  connect(res.port_b, heatingRod.port_a)
+    annotation (Line(points={{-88,16},{-88,22},{-70,22}}, color={0,127,255}));
+  connect(storageSimple.port_b_consumer, res1.port_a) annotation (Line(points={
+          {1,22},{2,22},{2,36},{12,36}}, color={0,127,255}));
+  connect(res1.port_b, senMasFlo_con.port_a) annotation (Line(points={{32,36},{
+          36,36},{36,37},{40,37}}, color={0,127,255}));
+  connect(storageSimple.TLayer[3], PIDHR.u_m) annotation (Line(points={{19.165,
+          7.04},{26,7.04},{26,42},{-46,42},{-46,76.4}}, color={0,0,127}));
+  connect(storageSimple.TLayer[3], storageHysteresis.u) annotation (Line(points
+        ={{19.165,7.04},{24,7.04},{24,40},{-74,40},{-74,50},{-73.2,50},{-73.2,
+          56.4}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-100,-60},{100,-100}},
+          fillColor={215,215,215},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None),
+        Text(
+          extent={{-98,-60},{-68,-66}},
+          textString="Pump control",
+          textColor={0,0,0}),
+        Rectangle(
+          extent={{-100,100},{0,52}},
+          fillColor={170,255,255},
+          fillPattern=FillPattern.Solid,
+          pattern=LinePattern.None,
+          lineColor={0,0,0}),
+        Text(
+          extent={{-96,98},{-66,92}},
+          textColor={0,0,0},
+          textString="HR control")}),
+    experiment(
+      StopTime=38200,
+      Interval=900,
+      Tolerance=1e-06,
+      __Dymola_Algorithm="Dassl"),
+          __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageSimpleExample.mos" "Simulate and plot"),
+    Documentation(info="<html><p>
+  This is an example of the simple storage model with two hydronic
+  circuits.<br/>
+  A heating rod indirectly supplies heat to the thermal energy
+  storage.<br/>
+  A simplified consumer extracts heat from the consumer water
+  circuit<br/>
+  based on a daily load profile.
+</p>
+</html>",revisions="<html>
+<ul>
+  <li>
+    <i>November 14 2022</i> by Laura Maier:<br/>
+    First implementation
+  </li>
+</ul>
+</html>"));
+end StorageSimpleExample;
diff --git a/AixLib/Fluid/Storage/Examples/StorageSolarCollector.mo b/AixLib/Fluid/Storage/Examples/StorageSolarCollector.mo
index fc2ba7fcac..7da7c25c65 100644
--- a/AixLib/Fluid/Storage/Examples/StorageSolarCollector.mo
+++ b/AixLib/Fluid/Storage/Examples/StorageSolarCollector.mo
@@ -1,12 +1,11 @@
 within AixLib.Fluid.Storage.Examples;
 model StorageSolarCollector
   extends Modelica.Icons.Example;
-  import AixLib;
 
   replaceable package Medium = AixLib.Media.Water;
 
-  AixLib.Fluid.Storage.BufferStorage
-                               bufferStorage(
+  AixLib.Fluid.Storage.StorageDetailed bufferStorage(
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     redeclare package MediumHC1 = Medium,
     redeclare package MediumHC2 = Medium,
     m1_flow_nominal=solarThermal.m_flow_nominal,
@@ -14,73 +13,69 @@ model StorageSolarCollector
     mHC1_flow_nominal=solarThermal.m_flow_nominal,
     useHeatingCoil2=false,
     useHeatingRod=false,
+    TStart=fill(333.15, 10),
     redeclare AixLib.DataBase.Storage.Generic_New_2000l data(hHC1Up=2.1),
     n=10,
     hConIn=1500,
     hConOut=15,
     redeclare package Medium = Medium,
-    hConHC1=1500)                      annotation (Placement(transformation(extent={{-10,14},
-            {-30,34}})));
-  Modelica.Thermal.HeatTransfer.Sources.FixedTemperature fixedTemperature(T = 283.15) annotation(Placement(transformation(extent={{-60,14},
+    hConHC1=1500)
+		annotation (Placement(transformation(extent={{-10,14},{-30,34}})));
+  Modelica.Thermal.HeatTransfer.Sources.FixedTemperature fixedTemperature(T = 283.15)
+	annotation(Placement(transformation(extent={{-60,14},
             {-40,34}})));
-  AixLib.Obsolete.Year2021.Fluid.Movers.Pump pump(
-    ControlStrategy=1,
+  AixLib.Fluid.Sources.Boundary_pT boundary_p(redeclare package Medium = Medium,nPorts=1)
+	annotation(Placement(transformation(extent={{86,74},
+            {66,94}})));
+  AixLib.Fluid.FixedResistances.PressureDrop
+                   res1(
     redeclare package Medium = Medium,
-    m_flow_small=1e-4) annotation (Placement(transformation(
-        extent={{-10,-10},{10,10}},
-        rotation=270,
-        origin={-8,70})));
-  AixLib.Fluid.Sources.Boundary_pT
-                     boundary_p(nPorts=1, redeclare package Medium = Medium)
-                                annotation(Placement(transformation(extent = {{-86, 70}, {-66, 90}})));
-  Modelica.Blocks.Sources.BooleanExpression booleanExpression annotation(Placement(transformation(extent = {{-10, -10}, {10, 10}}, rotation = 180, origin={36,70})));
-  Modelica.Fluid.Pipes.DynamicPipe
-                   pipe(
+    m_flow_nominal=solarThermal.m_flow_nominal,
+    dp_nominal=2000)
+	annotation(Placement(transformation(extent={{-6,-10},{14,10}})));
+  AixLib.Fluid.Sources.Boundary_pT boundary_ph2(nPorts=1, redeclare package Medium = Medium)
+	annotation(Placement(transformation(extent = {{10, -10}, {-10, 10}}, rotation = 180, origin={-76,52})));
+  AixLib.Fluid.FixedResistances.PressureDrop
+                   res(
     redeclare package Medium = Medium,
-    length=10,
-    diameter=0.05)                       annotation(Placement(transformation(extent={{-6,-10},
-            {14,10}})));
-  AixLib.Fluid.Sources.Boundary_ph
-                      boundary_ph1(use_p_in = true, h = 42e3,
-    nPorts=1,
-    redeclare package Medium = Medium)                        annotation(Placement(transformation(extent={{-66,-26},
-            {-46,-6}})));
-  AixLib.Fluid.Sources.Boundary_pT
-                      boundary_ph2(nPorts=1, redeclare package Medium = Medium)
-                                                     annotation(Placement(transformation(extent = {{10, -10}, {-10, 10}}, rotation = 180, origin={-76,52})));
-  Modelica.Fluid.Pipes.DynamicPipe
-                   pipe1(
-    redeclare package Medium = Medium,
-    length=10,
-    diameter=0.05)                        annotation(Placement(transformation(extent={{-40,-26},
-            {-20,-6}})));
+    allowFlowReversal=true,
+    m_flow_nominal=solarThermal.m_flow_nominal,
+    dp_nominal=2000)
+	annotation(Placement(transformation(extent={{-40,-26},{-20,-6}})));
   AixLib.Fluid.Solar.Thermal.SolarThermal solarThermal(
+    vol(T(start=298.15, fixed=true)),
     Collector=AixLib.DataBase.SolarThermal.FlatCollector(),
     A=20,
     redeclare package Medium = Medium,
-    m_flow_nominal=0.01,
+    m_flow_nominal=0.04,
     volPip=1)
     annotation (Placement(transformation(extent={{24,-10},{44,10}})));
-  Modelica.Blocks.Sources.Pulse pulse(period = 3600,               width = 1, amplitude = 60,
-    offset=101325)                                                                            annotation(Placement(transformation(extent={{-96,-18},
-            {-76,2}})));
-  AixLib.Obsolete.Year2021.Fluid.Actuators.Valves.SimpleValve simpleValve(
-    Kvs=2,
+  Modelica.Blocks.Sources.Pulse pulse(period = 3600,
+    width=10,
+    amplitude=0.05,
+    offset=0)
+	annotation(Placement(transformation(extent={{-96,-14},{-76,6}})));
+  AixLib.Fluid.Actuators.Valves.TwoWayEqualPercentage valve(
     redeclare package Medium = Medium,
-    m_flow_small=1e-4) annotation (Placement(transformation(
+    m_flow_nominal=solarThermal.m_flow_nominal,
+    dpValve_nominal=2000) annotation (Placement(transformation(
         extent={{-10,9},{10,-9}},
         rotation=90,
         origin={69,42})));
-  AixLib.Fluid.Sensors.TemperatureTwoPort
-                            temperatureSensor(redeclare package Medium = Medium,
-      m_flow_nominal=0.01)                    annotation(Placement(transformation(extent={{48,-10},
-            {68,10}})));
-  Modelica.Blocks.Continuous.LimPID PI(controllerType = Modelica.Blocks.Types.SimpleController.PI, k = 0.05, Ti = 60, yMax = 0.999, yMin = 0) annotation(Placement(transformation(extent = {{-6, 6}, {6, -6}}, rotation = 90, origin={90,14})));
-  Modelica.Blocks.Sources.Constant const(k = 273.15 + 70) annotation(Placement(transformation(extent={{74,-10},
-            {80,-4}})));
-  Modelica.Blocks.Math.Add add(k2 = -1) annotation(Placement(transformation(extent = {{-4, -4}, {4, 4}}, rotation = 90, origin={88,30})));
-  Modelica.Blocks.Sources.Constant const1(k = 1) annotation(Placement(transformation(extent={{70,20},
-            {78,28}})));
+  AixLib.Fluid.Sensors.TemperatureTwoPort temperatureSensor(redeclare package Medium = Medium,
+      m_flow_nominal=0.01)
+	  annotation(Placement(transformation(extent={{48,-10},{68,10}})));
+  Modelica.Blocks.Continuous.LimPID PI(controllerType = Modelica.Blocks.Types.SimpleController.PI,
+    k=0.005,
+    Ti=60,
+	yMax = 0.999,
+	yMin = 0) annotation(Placement(transformation(extent = {{-6, 6}, {6, -6}}, rotation = 90, origin={90,14})));
+  Modelica.Blocks.Sources.Constant const(k = 273.15 + 70)
+	annotation(Placement(transformation(extent={{74,-10},{80,-4}})));
+  Modelica.Blocks.Math.Add add(k2 = -1)
+	annotation(Placement(transformation(extent = {{-4, -4}, {4, 4}}, rotation = 90, origin={88,30})));
+  Modelica.Blocks.Sources.Constant const1(k = 1)
+	annotation(Placement(transformation(extent={{70,20},{78,28}})));
   Modelica.Blocks.Sources.CombiTimeTable hotSummerDay(
     extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic,
     table=[0,21,0; 3600,20.6,0; 7200,20.5,0; 10800,20.4,0; 14400,20,6; 18000,20.5,
@@ -90,32 +85,34 @@ model StorageSolarCollector
         5; 72000,22.9,0; 75600,21.2,0; 79200,20.6,0; 82800,20.3,0],
     offset={273.15,0.01})
     annotation (Placement(transformation(extent={{10,32},{30,52}})));
+  AixLib.Fluid.Movers.FlowControlled_dp pump(redeclare package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyState,
+      m_flow_nominal=solarThermal.m_flow_nominal,
+    per(pressure(V_flow={0,solarThermal.m_flow_nominal/1000,solarThermal.m_flow_nominal
+            /(1000*0.8)}, dp={dpPumpInput.k/0.8,dpPumpInput.k,0})))
+    annotation (Placement(transformation(extent={{6,60},{-14,80}})));
+  Modelica.Blocks.Sources.Constant dpPumpInput(k=55000)
+    annotation (Placement(transformation(extent={{32,80},{12,100}})));
+  AixLib.Fluid.Sources.MassFlowSource_T boundary(
+    redeclare package Medium = Medium,
+    use_m_flow_in=true,
+    use_T_in=false,
+    T=283.15,
+    nPorts=1)
+    annotation (Placement(transformation(extent={{-68,-26},{-48,-6}})));
 equation
-  connect(booleanExpression.y, pump.IsNight) annotation(Line(points={{25,70},{
-          2.2,70}},                                                                             color = {255, 0, 255}));
   connect(hotSummerDay.y[2], solarThermal.Irradiation) annotation(Line(points={{31,42},
-          {31,10},{34,10}},                                                                                           color = {0, 0, 127}));
+          {31,10},{34,10}},color = {0, 0, 127}));
   connect(hotSummerDay.y[1], solarThermal.T_air) annotation(Line(points={{31,42},
-          {31,22},{28,22},{28,10}},                                                                 color = {0, 0, 127}));
-  connect(pulse.y, boundary_ph1.p_in) annotation(Line(points={{-75,-8},{-68,-8}},        color = {0, 0, 127}));
-  connect(simpleValve.port_b, pump.port_a) annotation(Line(points={{69,52},{68,
-          52},{68,80},{-8,80}},                                                                                color = {0, 127, 255}));
+          {31,22},{28,22},{28,10}},color = {0, 0, 127}));
   connect(solarThermal.port_b, temperatureSensor.port_a) annotation(Line(points={{44,0},{
-          48,0}},                                                                                     color = {0, 127, 255}));
-  connect(solarThermal.port_a, pipe.port_b) annotation(Line(points={{24,0},{14,
-          0}},                                                                            color = {0, 127, 255}));
-  connect(temperatureSensor.port_b, simpleValve.port_a) annotation(Line(points={{68,0},{
-          68,32},{69,32}},                                                                                      color = {0, 127, 255}));
-  connect(const.y, PI.u_s) annotation(Line(points={{80.3,-7},{90,-7},{90,6.8}},          color = {0, 0, 127}));
-  connect(PI.y, add.u2) annotation(Line(points={{90,20.6},{90,25.2},{90.4,25.2}},           color = {0, 0, 127}));
-  connect(add.y, simpleValve.opening) annotation(Line(points={{88,34.4},{88,42},
-          {76.2,42}},                                                                              color = {0, 0, 127}));
-  connect(boundary_ph1.ports[1], pipe1.port_a) annotation (Line(
-      points={{-46,-16},{-40,-16}},
-      color={0,127,255}));
-  connect(boundary_p.ports[1], pump.port_a) annotation (Line(
-      points={{-66,80},{-36,80},{-8,80}},
-      color={0,127,255}));
+          48,0}},color = {0, 127, 255}));
+  connect(solarThermal.port_a,res1. port_b) annotation(Line(points={{24,0},{14,
+          0}},color = {0, 127, 255}));
+  connect(temperatureSensor.port_b, valve.port_a)
+    annotation (Line(points={{68,0},{68,32},{69,32}}, color={0,127,255}));
+  connect(const.y, PI.u_s) annotation(Line(points={{80.3,-7},{90,-7},{90,6.8}},color = {0, 0, 127}));
+  connect(PI.y, add.u2) annotation(Line(points={{90,20.6},{90,25.2},{90.4,25.2}},color = {0, 0, 127}));
   connect(temperatureSensor.T, PI.u_m) annotation (Line(
       points={{58,11},{58,14},{82.8,14}},
       color={0,0,127}));
@@ -124,23 +121,39 @@ equation
   connect(boundary_ph2.ports[1], bufferStorage.fluidportTop2) annotation (Line(
         points={{-66,52},{-50,52},{-50,50},{-23.125,50},{-23.125,34.1}}, color=
           {0,127,255}));
-  connect(pipe1.port_b, bufferStorage.fluidportBottom2) annotation (Line(points=
-         {{-20,-16},{-16,-16},{-16,0},{-22.875,0},{-22.875,13.9}}, color={0,127,
-          255}));
+  connect(res.port_b, bufferStorage.fluidportBottom2) annotation (Line(points={{
+          -20,-16},{-16,-16},{-16,0},{-22.875,0},{-22.875,13.9}}, color={0,127,255}));
   connect(fixedTemperature.port, bufferStorage.heatportOutside) annotation (
       Line(points={{-40,24},{-34,24},{-34,24.6},{-29.75,24.6}}, color={191,0,0}));
-  connect(pipe.port_a, bufferStorage.portHC1Out) annotation (Line(points={{-6,0},
+  connect(res1.port_a, bufferStorage.portHC1Out) annotation (Line(points={{-6,0},
           {-6,26.6},{-9.875,26.6}}, color={0,127,255}));
-  connect(bufferStorage.portHC1In, pump.port_b) annotation (Line(points={{-9.75,
-          29.7},{-9.75,44.85},{-8,44.85},{-8,60}}, color={0,127,255}));
+  connect(valve.port_b, pump.port_a) annotation (Line(points={{69,52},{68,52},{
+          68,70},{6,70}}, color={0,127,255}));
+  connect(dpPumpInput.y, pump.dp_in)
+    annotation (Line(points={{11,90},{-4,90},{-4,82}}, color={0,0,127}));
+  connect(pump.port_a, boundary_p.ports[1]) annotation (Line(points={{6,70},{36,
+          70},{36,84},{66,84}}, color={0,127,255}));
+  connect(add.y, valve.y)
+    annotation (Line(points={{88,34.4},{88,42},{79.8,42}}, color={0,0,127}));
+  connect(pump.port_b, bufferStorage.portHC1In) annotation (Line(points={{-14,
+          70},{-16,70},{-16,46},{-6,46},{-6,29.7},{-9.75,29.7}}, color={0,127,
+          255}));
+  connect(boundary.ports[1], res.port_a)
+    annotation (Line(points={{-48,-16},{-40,-16}}, color={0,127,255}));
+  connect(pulse.y, boundary.m_flow_in) annotation (Line(points={{-75,-4},{-72,
+          -4},{-72,-8},{-70,-8}}, color={0,0,127}));
   annotation (experiment(Tolerance=1e-6, StopTime = 172800, Interval = 60),
-  Documentation(info = "<html><h4>
-  <span style=\"color:#008000\">Overview</span>
-</h4>
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageSolarCollector.mos" "Simulate and plot"),
+  Documentation(info = "<html>
 <p>
   This is a simple example of a storage and a solar collector.
 </p>
 <ul>
+  <li>
+    <i>November 17, 2022</i> by Laura Maier:<br/>
+    Replace pump, polish example to make it more realistic, and add
+    simulate and plot script.
+  </li>
   <li>
     <i>October 11, 2016</i> by Marcus Fuchs:<br/>
     Replace pipe
diff --git a/AixLib/Fluid/Storage/Examples/Stratified.mo b/AixLib/Fluid/Storage/Examples/Stratified.mo
index 00ee065e49..616123377f 100644
--- a/AixLib/Fluid/Storage/Examples/Stratified.mo
+++ b/AixLib/Fluid/Storage/Examples/Stratified.mo
@@ -27,14 +27,14 @@ model Stratified "Test model for stratified tank"
     T=273.15 + 20,
     use_p_in=true,
     p=300000,
-    nPorts=2)             annotation (Placement(transformation(extent={{90,-2},
-            {70,18}})));
+    nPorts=2)             annotation (Placement(transformation(extent={{90,-18},
+            {70,2}})));
   AixLib.Fluid.FixedResistances.PressureDrop res_1(
     from_dp=true,
     redeclare package Medium = Medium,
     dp_nominal=5000,
     m_flow_nominal=0.1)
-    annotation (Placement(transformation(extent={{36,0},{56,20}})));
+    annotation (Placement(transformation(extent={{34,-18},{54,2}})));
   AixLib.Fluid.Storage.StratifiedEnhanced tanEnh(
     redeclare package Medium = Medium,
     hTan=3,
@@ -42,21 +42,21 @@ model Stratified "Test model for stratified tank"
     nSeg=10,
     m_flow_nominal=0.1,
     VTan=3) "Tank"
-    annotation (Placement(transformation(extent={{-18,-38},{2,-18}})));
+    annotation (Placement(transformation(extent={{-20,-70},{0,-50}})));
   AixLib.Fluid.FixedResistances.PressureDrop res_2(
     from_dp=true,
     redeclare package Medium = Medium,
     dp_nominal=5000,
     m_flow_nominal=0.1)
-    annotation (Placement(transformation(extent={{38,-38},{58,-18}})));
+    annotation (Placement(transformation(extent={{40,-90},{60,-70}})));
   AixLib.Fluid.Sensors.EnthalpyFlowRate HOut_flow(redeclare package Medium =
         Medium, m_flow_nominal=0.1) "Enthalpy flow rate"
                                      annotation (Placement(transformation(
-          extent={{6,2},{22,18}})));
+          extent={{4,-16},{20,0}})));
   AixLib.Fluid.Sensors.EnthalpyFlowRate HOut_flow1(redeclare package Medium =
         Medium, m_flow_nominal=0.1) "Enthalpy flow rate"
                                      annotation (Placement(transformation(
-          extent={{18,-36},{34,-20}})));
+          extent={{20,-88},{36,-72}})));
   Modelica.Blocks.Continuous.Integrator dH
     "Differenz in enthalpy (should be zero at steady-state)"
     annotation (Placement(transformation(extent={{68,30},{88,50}})));
@@ -87,25 +87,23 @@ equation
   connect(TWat.y, sou_1.T_in) annotation (Line(
       points={{-79,12},{-62,12}},
       color={0,0,127}));
-  connect(tanSim.port_b, HOut_flow.port_a) annotation (Line(points={{
-          5.55112e-16,10},{5.55112e-16,10},{6,10}},
-                                     color={0,127,255}));
+  connect(tanSim.port_b, HOut_flow.port_a) annotation (Line(points={{-10,0},{
+          -10,-8},{4,-8}},           color={0,127,255}));
   connect(HOut_flow.port_b, res_1.port_a)
-    annotation (Line(points={{22,10},{30,10},{36,10}},
-                                               color={0,127,255}));
+    annotation (Line(points={{20,-8},{34,-8}}, color={0,127,255}));
   connect(tanEnh.port_b, HOut_flow1.port_a)
-    annotation (Line(points={{2,-28},{2,-28},{18,-28}},
+    annotation (Line(points={{-10,-70},{-10,-80},{20,-80}},
                                                color={0,127,255}));
-  connect(HOut_flow1.port_b, res_2.port_a) annotation (Line(points={{34,-28},{
-          38,-28}}, color={0,127,255}));
+  connect(HOut_flow1.port_b, res_2.port_a) annotation (Line(points={{36,-80},{
+          40,-80}}, color={0,127,255}));
   connect(add.y, dH.u)
     annotation (Line(points={{53,40},{66,40}},   color={0,0,127}));
-  connect(HOut_flow.H_flow, add.u1) annotation (Line(points={{14,18.8},{14,46},
-          {30,46}},  color={0,0,127}));
-  connect(HOut_flow1.H_flow, add.u2) annotation (Line(points={{26,-19.2},{26,34},
+  connect(HOut_flow.H_flow, add.u1) annotation (Line(points={{12,0.8},{12,46},{
+          30,46}},   color={0,0,127}));
+  connect(HOut_flow1.H_flow, add.u2) annotation (Line(points={{28,-71.2},{28,34},
           {30,34}},       color={0,0,127}));
   connect(P.y, sin_1.p_in) annotation (Line(
-      points={{41,70},{100,70},{100,16},{92,16}},
+      points={{41,70},{100,70},{100,0},{92,0}},
       color={0,0,127}));
   connect(sine.y, TBCSid1.T) annotation (Line(points={{-69,72},{-55.5,72},{
           -55.5,90},{-41.2,90}}, color={0,0,127}));
@@ -116,23 +114,23 @@ equation
   connect(sine.y, TBCTop2.T) annotation (Line(points={{-69,72},{-56,72},{-56,38},
           {-41.2,38}}, color={0,0,127}));
   connect(TBCSid2.port, tanEnh.heaPorSid) annotation (Line(points={{-28,56},{
-          -24,56},{-24,-12},{-2,-12},{-2,-28},{-2.4,-28}}, color={191,0,0}));
+          -24,56},{-24,-12},{-4.4,-12},{-4.4,-60}},        color={191,0,0}));
   connect(TBCTop2.port, tanEnh.heaPorTop) annotation (Line(points={{-28,38},{
-          -26,38},{-26,-14},{-6,-14},{-6,-20.6}}, color={191,0,0}));
+          -26,38},{-26,-14},{-8,-14},{-8,-52.6}}, color={191,0,0}));
   connect(sin_1.ports[1], res_1.port_b) annotation (Line(
-      points={{70,10},{56,10}},
+      points={{70,-9},{64,-9},{64,-8},{54,-8}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(sin_1.ports[2], res_2.port_b) annotation (Line(
-      points={{70,6},{64,6},{64,-28},{58,-28}},
+      points={{70,-7},{64,-7},{64,-80},{60,-80}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(sou_1.ports[1], tanSim.port_a) annotation (Line(
-      points={{-40,10},{-20,10}},
+      points={{-40,7},{-30,7},{-30,20},{-10,20}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(sou_1.ports[2], tanEnh.port_a) annotation (Line(
-      points={{-40,6},{-30,6},{-30,-28},{-18,-28}},
+      points={{-40,9},{-30,9},{-30,-40},{-10,-40},{-10,-50}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(TBCSid1.port, tanSim.heaPorSid) annotation (Line(
@@ -147,19 +145,19 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/Stratified.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This test model compares two tank models. The only difference between
- the two tank models is that one uses the third order upwind discretization
- scheme that reduces numerical diffusion that is induced when connecting
- volumes in series.
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This test model compares two tank models. The only difference between
+the two tank models is that one uses the third order upwind discretization
+scheme that reduces numerical diffusion that is induced when connecting
+volumes in series.
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratified;
diff --git a/AixLib/Fluid/Storage/Examples/StratifiedEnhancedInternalHex.mo b/AixLib/Fluid/Storage/Examples/StratifiedEnhancedInternalHex.mo
index 008e19c659..7e018b6ad2 100644
--- a/AixLib/Fluid/Storage/Examples/StratifiedEnhancedInternalHex.mo
+++ b/AixLib/Fluid/Storage/Examples/StratifiedEnhancedInternalHex.mo
@@ -18,7 +18,7 @@ model StratifiedEnhancedInternalHex
         transformation(
         extent={{-10,10},{10,-10}},
         rotation=180,
-        origin={70,-12})));
+        origin={72,-78})));
   AixLib.Fluid.Sources.Boundary_pT solColSup(
     redeclare package Medium = MediumHex,
     nPorts=3,
@@ -116,37 +116,39 @@ model StratifiedEnhancedInternalHex
     m_flow_nominal=mHex_flow_nominal,
     tau=0)
     "Temperature sensor for outlet of steady state heat exchanger with solid configured dynamic"
-    annotation (Placement(transformation(extent={{-22,-80},{-42,-60}})));
+    annotation (Placement(transformation(extent={{-20,-82},{-40,-62}})));
 equation
   connect(solColSup.ports[1], tanSte.portHex_a) annotation (Line(
-      points={{-20,42.6667},{-4,42.6667},{-4,65.92},{6,65.92}},
+      points={{-20,38.6667},{-4,38.6667},{-4,65.92},{6,65.92}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(senTemSte.port_b, toSolCol.ports[1])
-    annotation (Line(points={{-40,10},{-40,10},{-50,10},{-50,-17.3333},{-62,
-          -17.3333}},                          color={0,127,255}));
+    annotation (Line(points={{-40,10},{-40,10},{-50,10},{-50,-21.3333},{-62,
+          -21.3333}},                          color={0,127,255}));
   connect(senTemSte.port_a, tanSte.portHex_b) annotation (Line(points={{-20,10},
           {0,10},{0,59.2},{6,59.2}}, color={0,127,255}));
   connect(senTemDyn.port_a, tanDyn.portHex_b) annotation (Line(points={{-22,-20},
           {0,-20},{0,-24.8},{4,-24.8}}, color={0,127,255}));
   connect(senTemDyn.port_b, toSolCol.ports[2]) annotation (Line(points={{-42,-20},
           {-52,-20},{-62,-20}},           color={0,127,255}));
-  connect(tanDynSol.portHex_b, senTemDynSol.port_a) annotation (Line(points={{6,
-          -72.8},{-8,-72.8},{-8,-70},{-22,-70}}, color={0,127,255}));
-  connect(senTemDynSol.port_b, toSolCol.ports[3]) annotation (Line(points={{-42,-70},
-          {-42,-70},{-50,-70},{-50,-22.6667},{-62,-22.6667}},      color={0,127,
+  connect(tanDynSol.portHex_b, senTemDynSol.port_a) annotation (Line(points={{6,-72.8},
+          {-8,-72.8},{-8,-72},{-20,-72}},        color={0,127,255}));
+  connect(senTemDynSol.port_b, toSolCol.ports[3]) annotation (Line(points={{-40,-72},
+          {-50,-72},{-50,-18.6667},{-62,-18.6667}},                color={0,127,
           255}));
   connect(solColSup.ports[2], tanDyn.portHex_a) annotation (Line(points={{-20,40},
           {-14,40},{-4,40},{-4,-18.08},{4,-18.08}}, color={0,127,255}));
   connect(solColSup.ports[3], tanDynSol.portHex_a) annotation (Line(points={{-20,
-          37.3333},{-12,37.3333},{-4,37.3333},{-4,-66.08},{6,-66.08}}, color={0,
+          41.3333},{-6,41.3333},{-6,-66.08},{6,-66.08}},               color={0,
           127,255}));
-  connect(bouWat.ports[1], tanSte.port_b) annotation (Line(points={{60,-9.33333},
-          {52,-9.33333},{52,72},{40,72}}, color={0,127,255}));
+  connect(bouWat.ports[1], tanSte.port_b) annotation (Line(points={{62,-79.3333},
+          {52,-79.3333},{52,40},{22,40},{22,56},{23,56}},
+                                          color={0,127,255}));
   connect(bouWat.ports[2], tanDyn.port_b)
-    annotation (Line(points={{60,-12},{52,-12},{38,-12}}, color={0,127,255}));
-  connect(bouWat.ports[3], tanDynSol.port_b) annotation (Line(points={{60,
-          -14.6667},{52,-14.6667},{52,-60},{40,-60}},
+    annotation (Line(points={{62,-78},{52,-78},{52,-36},{21,-36},{21,-28}},
+                                                          color={0,127,255}));
+  connect(bouWat.ports[3], tanDynSol.port_b) annotation (Line(points={{62,
+          -76.6667},{24,-76.6667},{24,-76},{23,-76}},
                                             color={0,127,255}));
   connect(step.y, solColSup.p_in)
     annotation (Line(points={{-59,48},{-52,48},{-42,48}}, color={0,0,127}));
@@ -155,74 +157,74 @@ equation
         "Simulate and plot"),
 experiment(Tolerance=1e-6, StopTime=1200),
 Documentation(info="<html>
- <p>
- This model provides an example for the
- <a href=\"modelica://AixLib.Fluid.Storage.StratifiedEnhancedInternalHex\">
- AixLib.Fluid.Storage.StratifiedEnhancedInternalHex</a> model.
- There are three tanks.
- In the tank on top, the fluid in the heat exchanger and the metal of the
- heat exchanger use a steady-state energy balance.
- In the middle tank, both use a dynamic balance.
- In the bottom tank, the fluid uses a steady-state heat balance
- but the metal of the heat exchanger uses a dynamic balance.
- </p>
- <p>
- Each tank starts at the same water temperature, and there is no
- water flow through the tank.
- The glycol that flows through the heat exchanger starts with zero
- mass flow rate, and is set to its design flow rate at <i>t=300</i> seconds.
- </p>
- </html>",
+<p>
+This model provides an example for the
+<a href=\"modelica://AixLib.Fluid.Storage.StratifiedEnhancedInternalHex\">
+AixLib.Fluid.Storage.StratifiedEnhancedInternalHex</a> model.
+There are three tanks.
+In the tank on top, the fluid in the heat exchanger and the metal of the
+heat exchanger use a steady-state energy balance.
+In the middle tank, both use a dynamic balance.
+In the bottom tank, the fluid uses a steady-state heat balance
+but the metal of the heat exchanger uses a dynamic balance.
+</p>
+<p>
+Each tank starts at the same water temperature, and there is no
+water flow through the tank.
+The glycol that flows through the heat exchanger starts with zero
+mass flow rate, and is set to its design flow rate at <i>t=300</i> seconds.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- September 28, 2015 by Michael Wetter:<br/>
- Changed medium in heat exchanger from
- <a href=\"modelica://Modelica.Media.Incompressible.Examples.Glycol47\">
- Modelica.Media.Incompressible.Examples.Glycol47</a> to
- <a href=\"modelica://AixLib.Media.Water\">
- AixLib.Media.Water</a>
- to avoid numerical derivative in regression tests.
- </li>
- <li>
- July 2, 2015 by Michael Wetter:<br/>
- Modified example to test dynamic versus steady-state heat exchanger
- configuration.
- </li>
- <li>
- December 22, 2014 by Michael Wetter:<br/>
- Removed <code>Modelica.Fluid.System</code>
- to address issue
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
- </li>
- <li>
- August 29, 2014 by Michael Wetter:<br/>
- Revised example to use a different media in the tank and in the
- heat exchanger. This is to provide a unit test for
- issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/271\">#271</a>.
- </li>
- <li>
- April 18, 2014 by Michael Wetter:<br/>
- Revised example for new connectors and parameters, and provided
- more interesting parameter values that cause a tank stratification.
- </li>
- <li>
- Mar 27, 2013 by Peter Grant:<br/>
- First implementation
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+September 28, 2015 by Michael Wetter:<br/>
+Changed medium in heat exchanger from
+<a href=\"modelica://Modelica.Media.Incompressible.Examples.Glycol47\">
+Modelica.Media.Incompressible.Examples.Glycol47</a> to
+<a href=\"modelica://AixLib.Media.Water\">
+AixLib.Media.Water</a>
+to avoid numerical derivative in regression tests.
+</li>
+<li>
+July 2, 2015 by Michael Wetter:<br/>
+Modified example to test dynamic versus steady-state heat exchanger
+configuration.
+</li>
+<li>
+December 22, 2014 by Michael Wetter:<br/>
+Removed <code>Modelica.Fluid.System</code>
+to address issue
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/311\">#311</a>.
+</li>
+<li>
+August 29, 2014 by Michael Wetter:<br/>
+Revised example to use a different media in the tank and in the
+heat exchanger. This is to provide a unit test for
+issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/271\">#271</a>.
+</li>
+<li>
+April 18, 2014 by Michael Wetter:<br/>
+Revised example for new connectors and parameters, and provided
+more interesting parameter values that cause a tank stratification.
+</li>
+<li>
+Mar 27, 2013 by Peter Grant:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end StratifiedEnhancedInternalHex;
diff --git a/AixLib/Fluid/Storage/Examples/StratifiedUnloadAtMinimumTemperature.mo b/AixLib/Fluid/Storage/Examples/StratifiedUnloadAtMinimumTemperature.mo
index 6558c99595..63bc57141e 100644
--- a/AixLib/Fluid/Storage/Examples/StratifiedUnloadAtMinimumTemperature.mo
+++ b/AixLib/Fluid/Storage/Examples/StratifiedUnloadAtMinimumTemperature.mo
@@ -20,7 +20,7 @@ model StratifiedUnloadAtMinimumTemperature
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     nSeg=nSeg,
     T_start=353.15) "Hot water storage tank"
-    annotation (Placement(transformation(extent={{-120,-130},{-100,-110}})));
+    annotation (Placement(transformation(extent={{-120,-128},{-100,-108}})));
   AixLib.Fluid.Sources.Boundary_pT loa(redeclare package Medium = Medium,
       nPorts=1)
     "Load (imposed by a constant pressure boundary condition and the flow of masSou)"
@@ -38,18 +38,18 @@ model StratifiedUnloadAtMinimumTemperature
     use_inputFilter=false) "Control valve at top"
     annotation (Placement(transformation(extent={{112,-30},{132,-10}})));
 
-  AixLib.Fluid.Actuators.Valves.TwoWayLinear valMed(
+  AixLib.Fluid.Actuators.Valves.TwoWayLinear valMid(
     redeclare package Medium = Medium,
     m_flow_nominal=m_flow_nominal,
     dpValve_nominal=3000,
-    use_inputFilter=false) "Control valve at top"
+    use_inputFilter=false) "Control valve at middle"
     annotation (Placement(transformation(extent={{132,-70},{152,-50}})));
 
   AixLib.Fluid.Actuators.Valves.TwoWayLinear valBot(
     redeclare package Medium = Medium,
     m_flow_nominal=m_flow_nominal,
     dpValve_nominal=3000,
-    use_inputFilter=false) "Control valve at top"
+    use_inputFilter=false) "Control valve at bottom"
     annotation (Placement(transformation(extent={{150,-110},{170,-90}})));
 
   Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor TMid
@@ -103,18 +103,19 @@ model StratifiedUnloadAtMinimumTemperature
     "Boolean to real conversion for valve at bottom"
     annotation (Placement(transformation(extent={{80,30},{100,50}})));
 equation
-  connect(masSou.ports[1], tan.port_b) annotation (Line(points={{222,-120},{-100,
-          -120}},             color={0,127,255}));
+  connect(masSou.ports[1], tan.port_b) annotation (Line(points={{222,-120},{56,
+          -120},{56,-128},{-110,-128}},
+                              color={0,127,255}));
   connect(TMid.port, tan.heaPorVol[3])
-    annotation (Line(points={{-100,80},{-110,80},{-110,-120}},
+    annotation (Line(points={{-100,80},{-100,-118},{-110,-118}},
                                                              color={191,0,0}));
   connect(TBot.port, tan.heaPorVol[5])
-    annotation (Line(points={{-100,40},{-110,40},{-110,-120}},
+    annotation (Line(points={{-100,40},{-100,-117.76},{-110,-117.76}},
                                                            color={191,0,0}));
   connect(valTop.port_b, senTem.port_a) annotation (Line(points={{132,-20},{182,
           -20},{182,-60},{190,-60}},
                                    color={0,127,255}));
-  connect(valMed.port_b, senTem.port_a)
+  connect(valMid.port_b, senTem.port_a)
     annotation (Line(points={{152,-60},{190,-60}},
                                                  color={0,127,255}));
   connect(valBot.port_b, senTem.port_a) annotation (Line(points={{170,-100},{182,
@@ -123,12 +124,14 @@ equation
   connect(senTem.port_b,loa. ports[1])
     annotation (Line(points={{210,-60},{222,-60}},
                                                  color={0,127,255}));
-  connect(valTop.port_a, tan.fluPorVol[1]) annotation (Line(points={{112,-20},{-112.6,
-          -20},{-112.6,-120}}, color={0,127,255}));
-  connect(valMed.port_a, tan.fluPorVol[3]) annotation (Line(points={{132,-60},{-112.6,
-          -60},{-112.6,-120}},color={0,127,255}));
-  connect(valBot.port_a, tan.fluPorVol[5]) annotation (Line(points={{150,-100},{
-          -112.6,-100},{-112.6,-120}},
+  connect(valTop.port_a, tan.fluPorVol[1]) annotation (Line(points={{112,-20},{
+          -116,-20},{-116,-118},{-112.6,-118},{-112.6,-118.4}},
+                               color={0,127,255}));
+  connect(valMid.port_a, tan.fluPorVol[3]) annotation (Line(points={{132,-60},{
+          -116,-60},{-116,-118},{-112.6,-118}},
+                              color={0,127,255}));
+  connect(valBot.port_a, tan.fluPorVol[5]) annotation (Line(points={{150,-100},
+          {-116,-100},{-116,-118},{-112.6,-118},{-112.6,-117.6}},
                               color={0,127,255}));
   connect(onOffMid.y, and2.u1)
     annotation (Line(points={{-29,80},{8,80}},     color={255,0,255}));
@@ -144,18 +147,20 @@ equation
           {48,112}},color={255,0,255}));
   connect(yTop.y, valTop.y) annotation (Line(points={{101,120},{122,120},{122,-8}},
                                color={0,0,127}));
-  connect(yMid.y, valMed.y) annotation (Line(points={{101,80},{142,80},{142,-48}},
+  connect(yMid.y, valMid.y) annotation (Line(points={{101,80},{142,80},{142,-48}},
                               color={0,0,127}));
   connect(not1.u, onOffBot.y) annotation (Line(points={{-22,60},{-26,60},{-26,40},
           {-29,40}},       color={255,0,255}));
   connect(not1.y, and2.u2) annotation (Line(points={{1,60},{4,60},{4,72},{8,72}},
         color={255,0,255}));
-  connect(hea.port, tan.heaPorVol[5]) annotation (Line(points={{-130,-124},{-110,
-          -124},{-110,-120}}, color={191,0,0}));
-  connect(TTop.port, tan.heaPorVol[1]) annotation (Line(points={{-160,-90},{-110,
-          -90},{-110,-120}}, color={191,0,0}));
+  connect(hea.port, tan.heaPorVol[5]) annotation (Line(points={{-130,-124},{
+          -110,-124},{-110,-117.76}},
+                              color={191,0,0}));
+  connect(TTop.port, tan.heaPorVol[1]) annotation (Line(points={{-160,-90},{
+          -120,-90},{-120,-120},{-110,-120},{-110,-118.24}},
+                             color={191,0,0}));
   connect(onOffHea.u, TTop.T) annotation (Line(points={{-212,-124},{-230,-124},
-          {-230,-90},{-180,-90}},color={0,0,127}));
+          {-230,-90},{-181,-90}},color={0,0,127}));
   connect(onOffHea.y, yHea.u)
     annotation (Line(points={{-189,-124},{-182,-124}}, color={255,0,255}));
   connect(hea.Q_flow, yHea.y)
@@ -165,9 +170,9 @@ equation
   connect(yBot.y, valBot.y)
     annotation (Line(points={{101,40},{160,40},{160,-88}}, color={0,0,127}));
   connect(TBot.T, onOffBot.u)
-    annotation (Line(points={{-80,40},{-52,40}}, color={0,0,127}));
+    annotation (Line(points={{-79,40},{-52,40}}, color={0,0,127}));
   connect(onOffMid.u, TMid.T)
-    annotation (Line(points={{-52,80},{-80,80}}, color={0,0,127}));
+    annotation (Line(points={{-52,80},{-79,80}}, color={0,0,127}));
   annotation (Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-300,-140},{260,140}})),
        __Dymola_Commands(file=
@@ -177,33 +182,33 @@ equation
       StopTime=21600,
       Tolerance=1e-06),
     Documentation(info="<html>
- <p>
- Example for tank model that has three outlets, each with a valve.
- The valve at the bottom opens when the temperature in that tank segment
- is sufficiently warm to serve the load.
- The tank in the middle also opens when its tank temperature is sufficiently high,
- but only if the valve below is closed.
- Finally, the valve at the top only opens if no other valve is open.
- Hence, there is always exactly one valve open.
- On the right-hand side of the model is a heater that adds heat to the bottom of the
- tank if the top tank segment is below the set point temperature.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly
- by removing CDL blocks.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- June 1, 2018, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1182\">
- issue 1182</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Example for tank model that has three outlets, each with a valve.
+The valve at the bottom opens when the temperature in that tank segment
+is sufficiently warm to serve the load.
+The tank in the middle also opens when its tank temperature is sufficiently high,
+but only if the valve below is closed.
+Finally, the valve at the top only opens if no other valve is open.
+Hence, there is always exactly one valve open.
+On the right-hand side of the model is a heater that adds heat to the bottom of the
+tank if the top tank segment is below the set point temperature.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly
+by removing CDL blocks.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+June 1, 2018, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1182\">
+issue 1182</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end StratifiedUnloadAtMinimumTemperature;
diff --git a/AixLib/Fluid/Storage/Examples/package.order b/AixLib/Fluid/Storage/Examples/package.order
index 865913b956..fe5f06d624 100644
--- a/AixLib/Fluid/Storage/Examples/package.order
+++ b/AixLib/Fluid/Storage/Examples/package.order
@@ -1,6 +1,7 @@
-BufferStorage
 ExpansionVessel
 StorageBoiler
+StorageDetailedExample
+StorageSimpleExample
 StorageSolarCollector
 Stratified
 StratifiedEnhancedInternalHex
diff --git a/AixLib/Fluid/Storage/ExpansionVessel.mo b/AixLib/Fluid/Storage/ExpansionVessel.mo
index a453979ad5..c38b30fcbe 100644
--- a/AixLib/Fluid/Storage/ExpansionVessel.mo
+++ b/AixLib/Fluid/Storage/ExpansionVessel.mo
@@ -6,8 +6,6 @@ model ExpansionVessel "Expansion vessel with fixed pressure"
    final mSenFac=1);
   parameter Modelica.Units.SI.Volume V_start(start=1)
     "Volume of liquid stored in the vessel at the start of the simulation";
-  parameter Modelica.Units.SI.Pressure p=Medium.p_default
-    "Constant pressure of the expansion vessel";
 
   Modelica.Fluid.Interfaces.FluidPort_a port_a(
     redeclare package Medium = Medium) "Fluid port"
@@ -82,71 +80,77 @@ equation
           fillPattern=FillPattern.Solid)}),
 defaultComponentName="exp",
 Documentation(info="<html>
- <p>
- This is a model of a pressure expansion vessel. The vessel has a constant pressure
- that is equal to the value of the parameter <code>p_start</code>.
- The model takes into account the energy and mass balance of the medium.
- It has no heat exchange with the ambient.
- </p>
- <p>
- The expansion vessel needs to be used in closed loops that contain
- water to set a reference pressure and, for liquids where the
- density is modeled as a function of temperature, to allow for
- the thermal expansion of the liquid.
- </p>
- <p>
- Note that alternatively, the model
- <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
- AixLib.Fluid.Sources.Boundary_pT</a> may be used to set
- a reference pressure. The main difference between these two models
- is that in this model, there is an energy and mass balance for the volume.
- In contrast, for
- <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
- AixLib.Fluid.Sources.Boundary_pT</a>,
- any mass flow rate that flows out of the model will be at a user-specified temperature.
- Therefore, <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
- AixLib.Fluid.Sources.Boundary_pT</a> leads to smaller systems
- of equations, which may result in faster simulation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- March 25, 2014 by Michael Wetter:<br/>
- Revised the model to use a constant pressure rather than a constant volume of
- water and gas. This leads to a simpler model.
- </li>
- <li>
- August 1, 2013 by Michael Wetter:<br/>
- Updated model to use new connector <code>mWat_flow</code>.
- </li>
- <li>
- February 7, 2012 by Michael Wetter:<br/>
- Revised due to changes in conservation equations in <code>AixLib.Fluid.Interfaces</code>.
- </li>
- <li>
- September 16, 2011 by Michael Wetter:<br/>
- Set <code>m(stateSelect=StateSelect.always)</code>, since
- setting the <code>stateSelect</code> attribute leads to smaller systems of equations.
- </li>
- <li>
- July 26, 2011 by Michael Wetter:<br/>
- Revised model to use new declarations from
- <a href=\"AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
- AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
- </li>
- <li>
- May 25, 2011 by Michael Wetter:<br/>
- Revised model due to a change in the fluid volume model.
- </li>
- <li>
- Nov. 4, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a model of a pressure expansion vessel. The vessel has a constant pressure
+that is equal to the value of the parameter <code>p_start</code>.
+The model takes into account the energy and mass balance of the medium.
+It has no heat exchange with the ambient.
+</p>
+<p>
+The expansion vessel needs to be used in closed loops that contain
+water to set a reference pressure and, for liquids where the
+density is modeled as a function of temperature, to allow for
+the thermal expansion of the liquid.
+</p>
+<p>
+Note that alternatively, the model
+<a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a> may be used to set
+a reference pressure. The main difference between these two models
+is that in this model, there is an energy and mass balance for the volume.
+In contrast, for
+<a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a>,
+any mass flow rate that flows out of the model will be at a user-specified temperature.
+Therefore, <a href=\"modelica://AixLib.Fluid.Sources.Boundary_pT\">
+AixLib.Fluid.Sources.Boundary_pT</a> leads to smaller systems
+of equations, which may result in faster simulation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 11, 2022, by Michael Wetter:<br/>
+Removed nonused parameter <code>p</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1614\">IBPSA, #1614</a>.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+March 25, 2014 by Michael Wetter:<br/>
+Revised the model to use a constant pressure rather than a constant volume of
+water and gas. This leads to a simpler model.
+</li>
+<li>
+August 1, 2013 by Michael Wetter:<br/>
+Updated model to use new connector <code>mWat_flow</code>.
+</li>
+<li>
+February 7, 2012 by Michael Wetter:<br/>
+Revised due to changes in conservation equations in <code>AixLib.Fluid.Interfaces</code>.
+</li>
+<li>
+September 16, 2011 by Michael Wetter:<br/>
+Set <code>m(stateSelect=StateSelect.always)</code>, since
+setting the <code>stateSelect</code> attribute leads to smaller systems of equations.
+</li>
+<li>
+July 26, 2011 by Michael Wetter:<br/>
+Revised model to use new declarations from
+<a href=\"modelica://AixLib.Fluid.Interfaces.LumpedVolumeDeclarations\">
+AixLib.Fluid.Interfaces.LumpedVolumeDeclarations</a>.
+</li>
+<li>
+May 25, 2011 by Michael Wetter:<br/>
+Revised model due to a change in the fluid volume model.
+</li>
+<li>
+Nov. 4, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ExpansionVessel;
diff --git a/AixLib/Fluid/Storage/Storage.mo b/AixLib/Fluid/Storage/Storage.mo
deleted file mode 100644
index bf4626fa8e..0000000000
--- a/AixLib/Fluid/Storage/Storage.mo
+++ /dev/null
@@ -1,213 +0,0 @@
-within AixLib.Fluid.Storage;
-model Storage
-
-  replaceable package Medium =
-     Modelica.Media.Water.ConstantPropertyLiquidWater
-     constrainedby Modelica.Media.Interfaces.PartialMedium;
-
-  parameter Integer n(min = 3) "number of layers";
-  parameter Modelica.Units.SI.Length d "storage diameter";
-  parameter Modelica.Units.SI.Length h "storage height";
-  parameter Modelica.Units.SI.ThermalConductivity lambda_ins
-    "thermal conductivity of insulation"
-    annotation (Dialog(group="Heat losses"));
-  parameter Modelica.Units.SI.Length s_ins "thickness of insulation"
-    annotation (Dialog(group="Heat losses"));
-  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConIn
-    "Iinternal heat transfer coefficient"
-    annotation (Dialog(group="Heat losses"));
-  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConOut
-    "External heat transfer coefficient"
-    annotation (Dialog(group="Heat losses"));
-  parameter Modelica.Units.SI.Volume V_HE "heat exchanger volume"
-    annotation (Dialog(group="Heat exchanger"));
-  parameter Modelica.Units.SI.CoefficientOfHeatTransfer k_HE
-    "heat exchanger heat transfer coefficient"
-    annotation (Dialog(group="Heat exchanger"));
-  parameter Modelica.Units.SI.Area A_HE "heat exchanger area"
-    annotation (Dialog(group="Heat exchanger"));
-  parameter Modelica.Units.SI.RelativePressureCoefficient beta=350e-6
-    annotation (Dialog(group="Bouyancy"));
-  parameter Real kappa = 0.4 annotation(Dialog(group = "Bouyancy"));
-  Modelica.Fluid.Interfaces.FluidPort_a
-                    port_a_consumer(redeclare final package Medium = Medium)
-                                    annotation(Placement(transformation(extent = {{-10, -108}, {10, -88}}), iconTransformation(extent = {{-10, -110}, {10, -90}})));
-  Modelica.Fluid.Interfaces.FluidPort_b
-                    port_b_consumer(redeclare final package Medium = Medium)
-                                    annotation(Placement(transformation(extent = {{-10, 82}, {10, 102}}), iconTransformation(extent = {{-10, 90}, {10, 110}})));
-  Fluid.MixingVolumes.MixingVolume
-                     layer[n](
-    each final energyDynamics=energyDynamics,
-    each final p_start=p_start,
-    each final T_start=T_start,
-    each final m_flow_small=m_flow_small_layer,
-    each final V = V / n,
-    redeclare final package Medium = Medium,
-    each final nPorts=2,
-    each final m_flow_nominal=m_flow_nominal_layer)      annotation(Placement(transformation(extent = {{-10, -10}, {10, 10}}, rotation = 90, origin = {0, 0})));
-  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a heatPort
-    "connect to ambient temperature around the storage"                                                            annotation(Placement(transformation(extent = {{-116, -10}, {-96, 10}}), iconTransformation(extent = {{-90, -10}, {-70, 10}})));
-  Modelica.Fluid.Interfaces.FluidPort_b
-                    port_b_heatGenerator(redeclare final package Medium = Medium)
-                                         annotation(Placement(transformation(extent = {{74, -98}, {94, -78}}), iconTransformation(extent = {{74, -90}, {94, -70}})));
-  Modelica.Fluid.Interfaces.FluidPort_a
-                    port_a_heatGenerator(redeclare final package Medium = Medium)
-                                         annotation(Placement(transformation(extent = {{74, 78}, {94, 98}}), iconTransformation(extent = {{74, 78}, {94, 98}})));
-  Fluid.MixingVolumes.MixingVolume
-                     layer_HE[n](
-    each final energyDynamics=energyDynamics,
-    each final p_start=p_start,
-    each final T_start=T_start,
-    each final m_flow_small=m_flow_small_layer_HE,
-    each final V = V_HE / n,
-    redeclare final package Medium = Medium,
-    each final nPorts=2,
-    each final m_flow_nominal=m_flow_nominal_HE)               annotation(Placement(transformation(extent = {{-10, -10}, {10, 10}}, rotation = 90, origin = {84, 0})));
-
-  Modelica.Thermal.HeatTransfer.Components.ThermalConductor heatTransfer_HE[n](each final G = k_HE * A_HE / n) annotation(Placement(transformation(extent = {{32, -10}, {52, 10}})));
-  Modelica.Thermal.HeatTransfer.Components.ThermalConductor heatTransfer[n](final G = cat(1, {G_top_bottom}, array(G_middle for k in 2:n - 1), {G_top_bottom})) annotation(Placement(transformation(extent = {{-80, -10}, {-60, 10}})));
-  BaseClasses.Bouyancy bouyancy[n - 1](
-    each final rho=Medium.density(Medium.setState_phX(
-        port_a_consumer.p,
-        inStream(port_a_consumer.h_outflow),
-        inStream(port_a_consumer.Xi_outflow))),
-    each final lambda=Medium.thermalConductivity(Medium.setState_phX(
-        port_a_consumer.p,
-        inStream(port_a_consumer.h_outflow),
-        inStream(port_a_consumer.Xi_outflow))),
-    each final g=Modelica.Constants.g_n,
-    each final cp=Medium.specificHeatCapacityCp(Medium.setState_phX(
-        port_a_consumer.p,
-        inStream(port_a_consumer.h_outflow),
-        inStream(port_a_consumer.Xi_outflow))),
-    each final A=A,
-    each final beta=beta,
-    each final dx=dx,
-    each final kappa=kappa) annotation (Placement(transformation(extent={{-10,-10},{
-            10,10}}, origin={-28,0})));
-  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal_layer
-    "Nominal mass flow rate in layers";
-  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal_HE
-    "Nominal mass flow rate of heat exchanger layers";
-
-  parameter Modelica.Fluid.Types.Dynamics energyDynamics=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial
-    "Type of energy balance: dynamic (3 initialization options) or steady state in layers and layers_HE";
-
-  //Initialization parameters
-  parameter Modelica.Media.Interfaces.Types.Temperature T_start=Medium.T_default
-    "Start value of temperature" annotation(Dialog(tab="Initialization"));
-  parameter Modelica.Media.Interfaces.Types.AbsolutePressure p_start=Medium.p_default
-    "Start value of pressure" annotation(Dialog(tab="Initialization"));
-
-  //Mass flow rates to regulate zero flow
-  parameter Modelica.Units.SI.MassFlowRate m_flow_small_layer=1E-4*abs(
-      m_flow_nominal_layer)
-    "Small mass flow rate for regularization of zero flow"
-    annotation (Dialog(tab="Advanced"));
-  parameter Modelica.Units.SI.MassFlowRate m_flow_small_layer_HE=1E-4*abs(
-      m_flow_nominal_HE) "Small mass flow rate for regularization of zero flow"
-    annotation (Dialog(tab="Advanced"));
-
-protected
-  parameter Modelica.Units.SI.Volume V=A*h;
-  parameter Modelica.Units.SI.Area A=Modelica.Constants.pi*d^2/4;
-  parameter Modelica.Units.SI.Length dx=V/A/n;
-  parameter Modelica.Units.SI.ThermalConductance G_middle=2*Modelica.Constants.pi
-      *h/n/(1/(hConIn*d/2) + 1/lambda_ins*log((d/2 + s_ins)/(d/2)) + 1/(hConOut
-      *(d/2 + s_ins)));
-  parameter Modelica.Units.SI.ThermalConductance G_top_bottom=G_middle +
-      lambda_ins/s_ins*A;
-equation
-  //Connect layers to the upper and lower ports
-  connect(port_a_consumer, layer[1].ports[1]) annotation (Line(
-      points={{0,-98},{0,-34},{20,-34},{20,-2},{10,-2}},
-      color={0,127,255}));
-  connect(layer[n].ports[2], port_b_consumer) annotation (Line(
-      points={{10,2},{16,2},{20,2},{20,40},{0,40},{0,92}},
-      color={0,127,255}));
-
-  //Connect layers
-  for k in 1:n - 1 loop
-    connect(layer[k].ports[2], layer[k + 1].ports[1]);
-  end for;
-  //Connect Heat Transfer to the Outside
-  for k in 1:n loop
-    connect(heatTransfer[k].port_a, layer[k].heatPort);
-    connect(heatTransfer[k].port_b, heatPort);
-  end for;
-  //Connect layers of Heat Exchanger
-  connect(port_a_heatGenerator, layer_HE[n].ports[2]) annotation (Line(
-      points={{84,88},{84,36},{96,22},{94,2}},
-      color={0,127,255}));
-  connect(port_b_heatGenerator, layer_HE[1].ports[1]) annotation (Line(
-      points={{84,-88},{84,-26},{96,-16},{94,-2}},
-      color={0,127,255}));
-  for k in 1:n - 1 loop
-    connect(layer_HE[k].ports[2], layer_HE[k + 1].ports[1]);
-  end for;
-  //Connect heat exchanger to storage layers
-  for k in 1:n loop
-    connect(heatTransfer_HE[k].port_a, layer[k].heatPort);
-    connect(heatTransfer_HE[k].port_b, layer_HE[k].heatPort);
-  end for;
-  //Connect bouyancy element
-  for k in 1:n - 1 loop
-    connect(bouyancy[k].port_a, layer[k + 1].heatPort);
-    connect(bouyancy[k].port_b, layer[k].heatPort);
-  end for;
-  connect(heatPort, heatPort) annotation(Line(points = {{-106, 0}, {-106, 0}}, color = {191, 0, 0}));
-
-  annotation (Icon(coordinateSystem(preserveAspectRatio = false, extent = {{-100, -100}, {100, 100}}), graphics={  Polygon(points = {{-154, 3}, {-136, -7}, {-110, -3}, {-84, -7}, {-48, -5}, {-18, -9}, {6, -3}, {6, -41}, {-154, -41}, {-154, 3}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {0, 0, 255},
-            fillPattern =                                                                                                   FillPattern.Solid, origin = {78, -59}, rotation = 360), Polygon(points = {{-154, 3}, {-134, -3}, {-110, 1}, {-84, -1}, {-56, -5}, {-30, -11}, {6, -3}, {6, -41}, {-154, -41}, {-154, 3}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {14, 110, 255},
-            fillPattern =                                                                                                   FillPattern.Solid, origin = {78, -27}, rotation = 360), Rectangle(extent = {{-80, -71}, {80, 71}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {85, 170, 255},
-            fillPattern =                                                                                                   FillPattern.Solid, origin = {4, 1}, rotation = 360), Polygon(points = {{-24, -67}, {-16, -67}, {-8, -67}, {4, -67}, {12, -67}, {36, -67}, {76, -67}, {110, -67}, {136, -67}, {136, 39}, {-24, 35}, {-24, -67}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {170, 213, 255},
-            fillPattern =                                                                                                   FillPattern.Solid, origin = {-52, 33}, rotation = 360), Polygon(points = {{-39, -30}, {-31, -30}, {-11, -30}, {23, -30}, {67, -30}, {93, -30}, {121, -30}, {121, 24}, {-39, 26}, {-39, -30}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {255, 170, 170},
-            fillPattern =                                                                                                   FillPattern.Solid, origin = {-37, 38}, rotation = 360), Polygon(points = {{-80, 100}, {-80, 54}, {-62, 54}, {-30, 54}, {32, 54}, {80, 54}, {80, 82}, {80, 100}, {-80, 100}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {255, 62, 62},
-            fillPattern =                                                                                                   FillPattern.Solid, origin = {4, 0}, rotation = 360), Rectangle(extent = {{-76, 100}, {84, -100}}, lineColor = {0, 0, 0},
-            lineThickness =                                                                                                   1), Line(points = {{-21, 94}, {-21, 132}}, color = {0, 0, 0}, smooth = Smooth.Bezier, thickness = 1, arrow = {Arrow.Filled, Arrow.None}, origin = {-56, 67}, rotation = 270, visible = use_heatingCoil1), Line(points = {{-54, 88}, {68, 56}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{68, 56}, {-48, 44}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{-48, 44}, {62, 6}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{62, 6}, {-44, -16}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{76, -81}, {-26, -81}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{0, -9}, {0, 9}}, color = {0, 0, 0}, smooth = Smooth.Bezier, thickness = 1, arrow = {Arrow.Filled, Arrow.None}, origin = {-34, -81}, rotation = 90, visible = use_heatingCoil1), Line(points = {{62, -42}, {-44, -16}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{62, -42}, {-42, -80}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{48, 88}, {-54, 88}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1)}), Documentation(info = "<html><h4>
-  <span style=\"color:#008000\">Overview</span>
-</h4>
-<p>
-  Simple model for a buffer storage.
-</p>
-<h4>
-  <span style=\"color:#008000\">Concept</span>
-</h4>
-<p>
-  The water volume can be discretised in several layers.
-</p>
-<p>
-  The following physical processes are modelled
-</p>
-<ul>
-  <li>heat exchange with the environment
-  </li>
-  <li>heat exchange over the heat exchanger
-  </li>
-  <li>a bouyancy model for the heat transfer between the layers
-  </li>
-</ul>
-<p>
-  <br/>
-  <b><span style=\"color: #008000\">Example Results</span></b>
-</p>
-<p>
-  <a href=
-  \"AixLib.HVAC.Storage.Examples.StorageBoiler\">AixLib.HVAC.Storage.Examples.StorageBoiler</a>
-</p>
-<p>
-  <a href=
-  \"AixLib.HVAC.Storage.Examples.StorageSolarCollector\">AixLib.HVAC.Storage.Examples.StorageSolarCollector</a>
-</p>
-<ul>
-  <li>
-    <i>November 2014&#160;</i> by Marcus Fuchs:<br/>
-    Changed model to use Annex 60 base class
-  </li>
-  <li>
-    <i>13.12.2013</i> by Sebastian Stinner:<br/>
-    implemented
-  </li>
-</ul>
-</html>"));
-end Storage;
diff --git a/AixLib/Fluid/Storage/BufferStorage.mo b/AixLib/Fluid/Storage/StorageDetailed.mo
similarity index 91%
rename from AixLib/Fluid/Storage/BufferStorage.mo
rename to AixLib/Fluid/Storage/StorageDetailed.mo
index d8a0760406..7762529b6e 100644
--- a/AixLib/Fluid/Storage/BufferStorage.mo
+++ b/AixLib/Fluid/Storage/StorageDetailed.mo
@@ -1,13 +1,9 @@
 within AixLib.Fluid.Storage;
-model BufferStorage
+model StorageDetailed
   "Buffer Storage Model with support for heating rod and two heating coils"
-  import      Modelica.Units.SI;
 
-  extends AixLib.Fluid.Interfaces.LumpedVolumeDeclarations(final T_start = TStart);
-
-  replaceable package Medium =
-      Modelica.Media.Interfaces.PartialMedium "Medium model"
-                 annotation (Dialog(group="Medium"),choicesAllMatching = true);
+  extends AixLib.Fluid.Interfaces.LumpedVolumeDeclarations(
+    final T_start=sum(TStart)/n);
 
   replaceable package MediumHC1 =
       Modelica.Media.Interfaces.PartialMedium "Medium model for HC1"
@@ -18,45 +14,41 @@ model BufferStorage
                  annotation (choicesAllMatching = true, Dialog(group="Medium"));
   parameter Modelica.Units.SI.MassFlowRate m1_flow_nominal(min=0)
     "Nominal mass flow rate of fluid 1 ports"
-    annotation (Dialog(group="Nominal condition"));
+    annotation(Dialog(group = "Nominal condition"));
   parameter Modelica.Units.SI.MassFlowRate m2_flow_nominal(min=0)
     "Nominal mass flow rate of fluid 2 ports"
-    annotation (Dialog(group="Nominal condition"));
-
-  parameter Modelica.Units.SI.MassFlowRate mHC1_flow_nominal(min=0)
-    if useHeatingCoil1 "Nominal mass flow rate of fluid 1 ports" annotation (
-      Dialog(
-      tab="Heating Coils and Rod",
-      group="Nominal condition",
-      enable=useHeatingCoil1));
-  parameter Modelica.Units.SI.MassFlowRate mHC2_flow_nominal(min=0)
-    if useHeatingCoil2 "Nominal mass flow rate of fluid 1 ports" annotation (
-      Dialog(
-      tab="Heating Coils and Rod",
-      group="Nominal condition",
-      enable=useHeatingCoil2));
+    annotation(Dialog(group = "Nominal condition"));
+
+  parameter Modelica.Units.SI.MassFlowRate mHC1_flow_nominal(min=0) if useHeatingCoil1
+    "Nominal mass flow rate of fluid 1 ports"
+    annotation(Dialog(tab="Heating Coils and Rod", group = "Nominal condition", enable=useHeatingCoil1));
+  parameter Modelica.Units.SI.MassFlowRate mHC2_flow_nominal(min=0) if useHeatingCoil2
+    "Nominal mass flow rate of fluid 1 ports"
+    annotation(Dialog(tab="Heating Coils and Rod", group = "Nominal condition", enable=useHeatingCoil2));
 
   parameter Boolean useHeatingCoil1=true "Use Heating Coil1?" annotation(Dialog(tab="Heating Coils and Rod"));
   parameter Boolean useHeatingCoil2=true "Use Heating Coil2?" annotation(Dialog(tab="Heating Coils and Rod"));
   parameter Boolean useHeatingRod=true "Use Heating Rod?" annotation(Dialog(tab="Heating Coils and Rod"));
 
-  parameter SI.Temperature TStart=298.15 "Start Temperature of fluid" annotation (Dialog(tab="Initialization", group="Storage specific"));
-
-  replaceable parameter DataBase.Storage.BufferStorageBaseDataDefinition data constrainedby DataBase.Storage.BufferStorageBaseDataDefinition "Data record for Storage"
-  annotation (choicesAllMatching);
+  parameter Integer n(min=3)=5 "Number of Layers";
+  parameter Modelica.Units.SI.Temperature TStart[n]=fill(298.15,n)
+    "Start Temperature of fluid in each layer. e.g. for a 3 layer model: {20, 20, 20}"
+    annotation (Dialog(tab="Initialization", group="Storage specific"));
 
-  parameter Integer n(min=3)=5 " Model assumptions Number of Layers";
+  replaceable parameter AixLib.DataBase.Storage.StorageDetailedBaseDataDefinition data
+    constrainedby AixLib.DataBase.Storage.StorageDetailedBaseDataDefinition
+    "Data record for Storage" annotation (choicesAllMatching);
 
 ////////////////////////////////////////////////////////////////////////////////////////////////////
 /////////////CONVECTION/////////////////////////////////////////////////////////////////////////////
 ////////////////////////////////////////////////////////////////////////////////////////////////////
 
-  parameter SI.CoefficientOfHeatTransfer hConIn=100 "Model assumptions heat transfer coefficient water <-> wall";
-  parameter SI.CoefficientOfHeatTransfer hConOut=10 "Model assumptions heat transfer coefficient insulation <-> air";
-  parameter SI.CoefficientOfHeatTransfer hConHC1=100 "Model assumptions Coefficient of Heat Transfer HC1 <-> Heating Water"
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConIn=100 "Model assumptions heat transfer coefficient water <-> wall";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConOut=10 "Model assumptions heat transfer coefficient insulation <-> air";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConHC1=100 "Model assumptions Coefficient of Heat Transfer HC1 <-> Heating Water"
                                                                            annotation(Dialog(enable=useHeatingCoil1,  tab=
           "Heating Coils and Rod"));
-  parameter SI.CoefficientOfHeatTransfer hConHC2=100 " Model assumptions Coefficient of Heat Transfer HC2 <-> Heating Water"
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConHC2=100 " Model assumptions Coefficient of Heat Transfer HC2 <-> Heating Water"
                                                                             annotation(Dialog(enable=useHeatingCoil2,  tab=
           "Heating Coils and Rod"));
   parameter Boolean upToDownHC1 = true
@@ -67,11 +59,9 @@ model BufferStorage
                                                  annotation(Dialog(enable = useHeatingCoil2,tab="Heating Coils and Rod"));
 
   parameter Modelica.Units.SI.Temperature TStartWall=293.15
-    "Starting Temperature of wall in K"
-    annotation (Dialog(tab="Initialization", group="Storage specific"));
+    "Starting Temperature of wall in K" annotation(Dialog(tab="Initialization", group="Storage specific"));
   parameter Modelica.Units.SI.Temperature TStartIns=293.15
-    "Starting Temperature of insulation in K"
-    annotation (Dialog(tab="Initialization", group="Storage specific"));
+    "Starting Temperature of insulation in K" annotation(Dialog(tab="Initialization", group="Storage specific"));
 
 ////////////////////////////////////////////////////////////////////////////////////////////////////
 ////////////Advanced parameters/////////////////////////////////////////////////////////////////////
@@ -147,24 +137,25 @@ model BufferStorage
         extent={{-5,5},{5,-5}},
         rotation=0,
         origin={-80,-80})));
-  Modelica.Fluid.Interfaces.FluidPort_a fluidportTop1(redeclare final package Medium =
-                Medium)
+  Modelica.Fluid.Interfaces.FluidPort_a fluidportTop1(redeclare final package
+      Medium =  Medium)
     "Fluid connector a (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{-38,92},{-18,110}},rotation=
            0), iconTransformation(extent={{-38,92},{-18,110}})));
   Modelica.Fluid.Interfaces.FluidPort_a fluidportBottom2(redeclare final
-      package                                                                    Medium =
+      package Medium =
                Medium)
     "Fluid connector a (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{14,-110},{32,-92}},rotation=
            0), iconTransformation(extent={{14,-110},{32,-92}})));
   Modelica.Fluid.Interfaces.FluidPort_b fluidportBottom1(redeclare final
-      package                                                                    Medium =
+      package Medium =
                  Medium)
     "Fluid connector b (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{-36,-112},{-18,-92}},
           rotation=0), iconTransformation(extent={{-36,-112},{-18,-92}})));
-  Modelica.Fluid.Interfaces.FluidPort_b fluidportTop2(redeclare final package Medium =
+  Modelica.Fluid.Interfaces.FluidPort_b fluidportTop2(redeclare final package
+      Medium =
         Medium)
     "Fluid connector b (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{14,92},{36,110}},rotation=0),
@@ -176,7 +167,7 @@ model BufferStorage
       "Heat transfer model" annotation (Placement(transformation(extent={{-34,0},
             {-14,20}}, rotation=0)));
 
-  AixLib.Fluid.MixingVolumes.MixingVolume          layer[n](
+  AixLib.Fluid.MixingVolumes.MixingVolume layer[n](
     each final energyDynamics=energyDynamics,
     each final massDynamics=massDynamics,
     each final p_start=p_start,
@@ -188,7 +179,7 @@ model BufferStorage
     each final m_flow_small=m_flow_small,
     final V=fill(data.hTank/n*Modelica.Constants.pi/4*data.dTank^2,n),
     final nPorts = portsLayer,
-    final T_start=fill(TStart,n),
+    final T_start=TStart,
     redeclare each final package Medium = Medium,
     each final m_flow_nominal=m1_flow_nominal + m2_flow_nominal)
     "Layer volumes"
@@ -207,12 +198,14 @@ model BufferStorage
 /////HEATING COIL 1 ////////////////////////////////////////////////////////////////////
 ////////////////////////////////////////////////////////////////////////////////////////
 
-  Modelica.Fluid.Interfaces.FluidPort_a portHC1In(redeclare final package Medium =
+  Modelica.Fluid.Interfaces.FluidPort_a portHC1In(redeclare final package
+      Medium =
         MediumHC1) if useHeatingCoil1
     "Fluid connector a (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{-92,36},{-72,56}}),
         iconTransformation(extent={{-90,50},{-74,64}})));
-  Modelica.Fluid.Interfaces.FluidPort_b portHC1Out(redeclare final package Medium =
+  Modelica.Fluid.Interfaces.FluidPort_b portHC1Out(redeclare final package
+      Medium =
         MediumHC1) if useHeatingCoil1
     "Fluid connector b (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{-90,2},{-70,22}}),
@@ -222,12 +215,14 @@ model BufferStorage
 /////HEATING COIL 2 ////////////////////////////////////////////////////////////////////
 ////////////////////////////////////////////////////////////////////////////////////////
 
-  Modelica.Fluid.Interfaces.FluidPort_a portHC2In(redeclare final package Medium =
+  Modelica.Fluid.Interfaces.FluidPort_a portHC2In(redeclare final package
+      Medium =
         MediumHC2) if useHeatingCoil2
     "Fluid connector a (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{-92,-30},{-72,-10}}),
         iconTransformation(extent={{-88,-32},{-74,-18}})));
-  Modelica.Fluid.Interfaces.FluidPort_b portHC2Out(redeclare final package Medium =
+  Modelica.Fluid.Interfaces.FluidPort_b portHC2Out(redeclare final package
+      Medium =
         MediumHC2) if useHeatingCoil2
     "Fluid connector b (positive design flow direction is from port_a to port_b)"
     annotation (Placement(transformation(extent={{-92,-68},{-72,-48}}),
@@ -310,7 +305,7 @@ model BufferStorage
     pipeHC=data.pipeHC1,
     allowFlowReversal=allowFlowReversal_HC1,
     final m_flow_nominal=mHC1_flow_nominal,
-    TStart=TStart) if useHeatingCoil1
+    TStart=sum(TStart)/n) if useHeatingCoil1
     annotation (Placement(transformation(
         extent={{-10,-10},{10,10}},
         rotation=270,
@@ -324,17 +319,17 @@ model BufferStorage
     redeclare package Medium = MediumHC2,
     allowFlowReversal=allowFlowReversal_HC2,
     final m_flow_nominal=mHC2_flow_nominal,
-    TStart=TStart) if useHeatingCoil2
+    TStart=sum(TStart)/n) if useHeatingCoil2
     annotation (Placement(transformation(
         extent={{-10,-10},{10,10}},
         rotation=270,
         origin={-56,-39})));
 
-  parameter SI.MassFlowRate m_flow_small_HC1=1E-4*abs(mHC1_flow_nominal) if useHeatingCoil1
+  parameter Modelica.Units.SI.MassFlowRate m_flow_small_HC1=1E-4*abs(mHC1_flow_nominal) if useHeatingCoil1
     "Small mass flow rate for regularization of zero flow" annotation(Dialog(tab="Advanced", enable=useHeatingCoil1));
-  parameter SI.MassFlowRate m_flow_small_HC2=1E-4*abs(mHC2_flow_nominal) if useHeatingCoil2
+  parameter Modelica.Units.SI.MassFlowRate m_flow_small_HC2=1E-4*abs(mHC2_flow_nominal) if useHeatingCoil2
     "Small mass flow rate for regularization of zero flow" annotation(Dialog(tab="Advanced", enable=useHeatingCoil2));
-  parameter SI.MassFlowRate m_flow_small=1E-4*abs(m1_flow_nominal + m2_flow_nominal)
+  parameter Modelica.Units.SI.MassFlowRate m_flow_small=1E-4*abs(m1_flow_nominal + m2_flow_nominal)
     "Small mass flow rate for regularization of zero flow" annotation(Dialog(tab="Advanced"));
   parameter Boolean allowFlowReversal_layers=true
     "= false to simplify equations, assuming, but not enforcing, no flow reversal. Used only if model has two ports."
@@ -783,6 +778,9 @@ for i in 2:(n-1) loop
                  Diagram(coordinateSystem(preserveAspectRatio=false,
           extent={{-80,-100},{80,100}})),
     Documentation(revisions="<html><ul>
+  <li>November 14, 2022, by Laura Maier:<br/>
+  Add adapt name and do some spring cleaning
+  </li>
   <li>November 27, 2019, by Philipp Mehrfeld:<br/>
     - <a href=
     \"https://github.com/RWTH-EBC/AixLib/issues/793\">#793</a><br/>
@@ -822,16 +820,16 @@ for i in 2:(n-1) loop
   </li>
 </ul>
 </html>",
-        info="<html><h4>
-  <span style=\"color: #008000\">Overview</span>
-</h4>
+        info="<html><p>
+  <b><span style=\"color: #008000;\">Overview</span></b>
+</p>
+<p>
+  Detailed thermal energy storage model with optional heating rod and
+  two heating coils based on a pipe model.
+</p>
 <p>
-  Buffer Storage Model with support for heating rod and two heating
-  coils.
+  <b><span style=\"color: #008000;\">Concept</span></b>
 </p>
-<h4>
-  <span style=\"color: #008000\">Concept</span>
-</h4>
 <p>
   It represents a buffer storage stratified into n layers where 1
   represents the bottom layer and n represents the top layer. The
@@ -883,9 +881,9 @@ for i in 2:(n-1) loop
   included. Thus external pressure loss models are required for the use
   of the model.
 </p>
-<h4>
-  <span style=\"color: #008000\">Sources</span>
-</h4>
+<p>
+  <b><span style=\"color: #008000;\">Sources</span></b>
+</p>
 <ul>
   <li>R. Viskanta, A. KaraIds: Interferometric observations of the
   temperature structure in water cooled or heated from above.
@@ -893,12 +891,20 @@ for i in 2:(n-1) loop
   Bibtex-Key [R.VISKANTA1977]
   </li>
 </ul>
-<h4>
-  <span style=\"color: #008000;\">Example Results</span>
-</h4>
+<p>
+  <b><span style=\"color: #008000;\">Example Results</span></b>
+</p>
+<p>
+  <a href=
+  \"AixLib.Fluid.Storage.Examples.StorageDetailed\">AixLib.Fluid.Storage.Examples.StorageDetailed</a>
+</p>
+<p>
+  <a href=
+  \"AixLib.Fluid.Storage.Examples.StorageBoiler\">AixLib.Fluid.Storage.Examples.StorageBoiler</a>
+</p>
 <p>
   <a href=
-  \"AixLib.Fluid.Storage.Examples.BufferStorageCharging\">AixLib.Fluid.Storage.Examples.BufferStorageCharging</a>
+  \"AixLib.Fluid.Storage.Examples.StorageSolarCollector\">AixLib.Fluid.Storage.Examples.StorageSolarCollector</a>
 </p>
 </html>"));
-end BufferStorage;
+end StorageDetailed;
diff --git a/AixLib/Fluid/Storage/StorageSimple.mo b/AixLib/Fluid/Storage/StorageSimple.mo
new file mode 100644
index 0000000000..e6b49327b0
--- /dev/null
+++ b/AixLib/Fluid/Storage/StorageSimple.mo
@@ -0,0 +1,271 @@
+within AixLib.Fluid.Storage;
+model StorageSimple
+  "Simplified multi-layer storage model with volumes as heat exchangers without pressure losses"
+
+  replaceable package Medium =
+     Modelica.Media.Water.ConstantPropertyLiquidWater
+     constrainedby Modelica.Media.Interfaces.PartialMedium;
+
+  parameter Integer n(min = 3) "number of layers";
+  parameter Modelica.Units.SI.Length d "storage diameter";
+  parameter Modelica.Units.SI.Length h "storage height";
+  parameter Modelica.Units.SI.ThermalConductivity lambda_ins
+    "thermal conductivity of insulation"
+ annotation(Dialog(group = "Heat losses"));
+  parameter Modelica.Units.SI.Length s_ins "thickness of insulation" annotation(Dialog(group = "Heat losses"));
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConIn "Iinternal heat transfer coefficient"
+  annotation(Dialog(group="Heat losses"));
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConOut "External heat transfer coefficient"
+  annotation(Dialog(group="Heat losses"));
+  parameter Modelica.Units.SI.Volume V_HE "heat exchanger volume" annotation(Dialog(group = "Heat exchanger"));
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer k_HE
+    "heat exchanger heat transfer coefficient" annotation(Dialog(group = "Heat exchanger"));
+  parameter Modelica.Units.SI.Area A_HE "heat exchanger area"
+  annotation(Dialog(group = "Heat exchanger"));
+  parameter Modelica.Units.SI.RelativePressureCoefficient beta = 350e-6
+  annotation(Dialog(group = "Bouyancy"));
+  parameter Real kappa = 0.4 annotation(Dialog(group = "Bouyancy"));
+
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal_layer
+    "Nominal mass flow rate in layers";
+  parameter Modelica.Units.SI.MassFlowRate m_flow_nominal_HE
+    "Nominal mass flow rate of heat exchanger layers";
+
+  //Optional temperature outputs
+  parameter Boolean use_TOut = true "Use temperature real outputs";
+
+  parameter Modelica.Fluid.Types.Dynamics energyDynamics=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial
+    "Type of energy balance: dynamic (3 initialization options) or steady state in layers and layers_HE";
+
+  //Initialization parameters
+  parameter Modelica.Units.SI.Temperature T_start[n]
+    "Start value of temperature of each layer, e.g. for 3 layers: {20, 20, 20}" annotation(Dialog(tab="Initialization"));
+  parameter Modelica.Media.Interfaces.Types.AbsolutePressure p_start=Medium.p_default
+    "Start value of pressure" annotation(Dialog(tab="Initialization"));
+
+  //Mass flow rates to regulate zero flow
+  parameter Modelica.Units.SI.MassFlowRate m_flow_small_layer=1E-4*abs(m_flow_nominal_layer)
+    "Small mass flow rate for regularization of zero flow" annotation(Dialog(tab="Advanced"));
+   parameter Modelica.Units.SI.MassFlowRate m_flow_small_layer_HE=1E-4*abs(m_flow_nominal_HE)
+    "Small mass flow rate for regularization of zero flow" annotation(Dialog(tab="Advanced"));
+
+  Modelica.Fluid.Interfaces.FluidPort_a
+                    port_a_consumer(redeclare final package Medium = Medium)
+                                    annotation(Placement(transformation(extent = {{-10, -108}, {10, -88}}), iconTransformation(extent = {{-10, -110}, {10, -90}})));
+  Modelica.Fluid.Interfaces.FluidPort_b
+                    port_b_consumer(redeclare final package Medium = Medium)
+                                    annotation(Placement(transformation(extent = {{-10, 82}, {10, 102}}), iconTransformation(extent = {{-10, 90}, {10, 110}})));
+  Fluid.MixingVolumes.MixingVolume
+                     layer[n](
+    each final energyDynamics=energyDynamics,
+    each final p_start=p_start,
+    T_start=T_start,
+    each final m_flow_small=m_flow_small_layer,
+    each final V = V / n,
+    redeclare final package Medium = Medium,
+    each final nPorts=2,
+    each final m_flow_nominal=m_flow_nominal_layer)
+  annotation(Placement(transformation(extent = {{-10, -10}, {10, 10}}, rotation = 90, origin = {0, 0})));
+  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a heatPort
+    "connect to ambient temperature around the storage"
+  annotation(Placement(transformation(extent = {{-116, -10}, {-96, 10}}),
+       iconTransformation(extent = {{-90, -10}, {-70, 10}})));
+  Modelica.Fluid.Interfaces.FluidPort_b
+    port_b_heatGenerator(redeclare final package Medium = Medium)
+  annotation(Placement(transformation(extent = {{74, -98}, {94, -78}}), iconTransformation(extent = {{74, -90}, {94, -70}})));
+  Modelica.Fluid.Interfaces.FluidPort_a
+    port_a_heatGenerator(redeclare final package Medium = Medium)
+        annotation(Placement(transformation(extent = {{74, 78}, {94, 98}}), iconTransformation(extent = {{74, 78}, {94, 98}})));
+  Fluid.MixingVolumes.MixingVolume
+    layer_HE[n](
+    each final energyDynamics=energyDynamics,
+    each final p_start=p_start,
+    T_start=T_start,
+    each final m_flow_small=m_flow_small_layer_HE,
+    each final V = V_HE / n,
+    redeclare final package Medium = Medium,
+    each final nPorts=2,
+    each final m_flow_nominal=m_flow_nominal_HE) annotation(Placement(transformation(extent = {{-10, -10}, {10, 10}}, rotation = 90, origin = {84, 0})));
+
+  Modelica.Thermal.HeatTransfer.Components.ThermalConductor heatTransfer_HE[n](each final G = k_HE * A_HE / n) annotation(Placement(transformation(extent = {{32, -10}, {52, 10}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalConductor heatTransfer[n](final G = cat(1, {G_top_bottom}, array(G_middle for k in 2:n - 1), {G_top_bottom})) annotation(Placement(transformation(extent = {{-80, -10}, {-60, 10}})));
+  BaseClasses.Bouyancy bouyancy[n - 1](
+    each final rho=Medium.density(Medium.setState_phX(
+        port_a_consumer.p,
+        inStream(port_a_consumer.h_outflow),
+        inStream(port_a_consumer.Xi_outflow))),
+    each final lambda=Medium.thermalConductivity(Medium.setState_phX(
+        port_a_consumer.p,
+        inStream(port_a_consumer.h_outflow),
+        inStream(port_a_consumer.Xi_outflow))),
+    each final g=Modelica.Constants.g_n,
+    each final cp=Medium.specificHeatCapacityCp(Medium.setState_phX(
+        port_a_consumer.p,
+        inStream(port_a_consumer.h_outflow),
+        inStream(port_a_consumer.Xi_outflow))),
+    each final A=A,
+    each final beta=beta,
+    each final dx=dx,
+    each final kappa=kappa) annotation (Placement(transformation(extent={{-10,-10},{
+            10,10}}, origin={-28,0})));
+
+  Modelica.Blocks.Interfaces.RealOutput TLayer[n](
+    each final quantity="ThermodynamicTemperature",
+    each final unit="K",
+    each min=0,
+    each displayUnit="degC") if use_TOut "Temperature in the top layer" annotation (Placement(
+        transformation(
+        origin={-112,30},
+        extent={{12,12},{-12,-12}},
+        rotation=0), iconTransformation(
+        extent={{7.5,7.5},{-7.5,-7.5}},
+        rotation=0,
+        origin={-86.5,29.5})));
+  Modelica.Blocks.Interfaces.RealOutput TLayer_HE[n](
+    each final quantity="ThermodynamicTemperature",
+    each final unit="K",
+    each min=0,
+    each displayUnit="degC") if use_TOut "Temperature in the top layer" annotation (Placement(
+        transformation(
+        origin={112,30},
+        extent={{-12,12},{12,-12}},
+        rotation=0), iconTransformation(
+        extent={{-7.5,7.5},{7.5,-7.5}},
+        rotation=0,
+        origin={94.5,29.5})));
+protected
+  parameter Modelica.Units.SI.Volume V = A * h;
+  parameter Modelica.Units.SI.Area A = Modelica.Constants.pi * d ^ 2 / 4;
+  parameter Modelica.Units.SI.Length dx = V / A / n;
+  parameter Modelica.Units.SI.ThermalConductance G_middle=
+  2*Modelica.Constants.pi*h/n/(1/(hConIn*d/2) + 1/lambda_ins*
+  log((d/2 + s_ins)/(d/2)) + 1/(hConOut*(d/2 + s_ins)));
+  parameter Modelica.Units.SI.ThermalConductance G_top_bottom=
+   G_middle + lambda_ins / s_ins * A;
+
+equation
+  //Connect layers to the upper and lower ports
+  connect(port_a_consumer, layer[1].ports[1]) annotation (Line(
+      points={{0,-98},{0,-34},{20,-34},{20,-1},{10,-1}},
+      color={0,127,255}));
+  connect(layer[n].ports[2], port_b_consumer) annotation (Line(
+      points={{10,1},{16,1},{20,1},{20,40},{0,40},{0,92}},
+      color={0,127,255}));
+
+  //Connect layers
+  for k in 1:n - 1 loop
+    connect(layer[k].ports[2], layer[k + 1].ports[1]);
+  end for;
+  //Connect Heat Transfer to the Outside
+  for k in 1:n loop
+    connect(heatTransfer[k].port_a, layer[k].heatPort);
+    connect(heatTransfer[k].port_b, heatPort);
+  end for;
+  //Connect layers of Heat Exchanger
+  connect(port_a_heatGenerator, layer_HE[n].ports[2]) annotation (Line(
+      points={{84,88},{94,36},{94,22},{94,1}},
+      color={0,127,255}));
+  connect(port_b_heatGenerator, layer_HE[1].ports[1]) annotation (Line(
+      points={{84,-88},{84,-26},{94,-26},{94,-1}},
+      color={0,127,255}));
+  for k in 1:n - 1 loop
+    connect(layer_HE[k].ports[2], layer_HE[k + 1].ports[1]);
+  end for;
+  //Connect heat exchanger to storage layers
+  for k in 1:n loop
+    connect(heatTransfer_HE[k].port_a, layer[k].heatPort);
+    connect(heatTransfer_HE[k].port_b, layer_HE[k].heatPort);
+  end for;
+  //Connect bouyancy element
+  for k in 1:n - 1 loop
+    connect(bouyancy[k].port_a, layer[k + 1].heatPort);
+    connect(bouyancy[k].port_b, layer[k].heatPort);
+  end for;
+  connect(heatPort, heatPort) annotation(Line(points={{-106,0},{-106,0}},      color = {191, 0, 0}));
+
+///////////////////////////////////////////////////////////////////////////////
+///////////////////  connection of Temperature Sensor//////////////////////////
+///////////////////////////////////////////////////////////////////////////////
+
+  if use_TOut then
+    for k in 1:n loop
+
+      TLayer[k] = layer[k].heatPort.T;
+
+      TLayer_HE[k] = layer_HE[k].heatPort.T;
+
+    end for;
+  end if;
+  annotation (Icon(coordinateSystem(preserveAspectRatio = false, extent = {{-100, -100}, {100, 100}}), graphics={  Polygon(points = {{-154, 3}, {-136, -7}, {-110, -3}, {-84, -7}, {-48, -5}, {-18, -9}, {6, -3}, {6, -41}, {-154, -41}, {-154, 3}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {0, 0, 255},
+            fillPattern = FillPattern.Solid, origin = {78, -59}, rotation = 360), Polygon(points = {{-154, 3}, {-134, -3}, {-110, 1}, {-84, -1}, {-56, -5}, {-30, -11}, {6, -3}, {6, -41}, {-154, -41}, {-154, 3}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {14, 110, 255},
+            fillPattern = FillPattern.Solid, origin = {78, -27}, rotation = 360), Rectangle(extent = {{-80, -71}, {80, 71}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {85, 170, 255},
+            fillPattern = FillPattern.Solid, origin = {4, 1}, rotation = 360), Polygon(points = {{-24, -67}, {-16, -67}, {-8, -67}, {4, -67}, {12, -67}, {36, -67}, {76, -67}, {110, -67}, {136, -67}, {136, 39}, {-24, 35}, {-24, -67}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {170, 213, 255},
+            fillPattern = FillPattern.Solid, origin = {-52, 33}, rotation = 360), Polygon(points = {{-39, -30}, {-31, -30}, {-11, -30}, {23, -30}, {67, -30}, {93, -30}, {121, -30}, {121, 24}, {-39, 26}, {-39, -30}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {255, 170, 170},
+            fillPattern = FillPattern.Solid, origin = {-37, 38}, rotation = 360), Polygon(points = {{-80, 100}, {-80, 54}, {-62, 54}, {-30, 54}, {32, 54}, {80, 54}, {80, 82}, {80, 100}, {-80, 100}}, lineColor = {0, 0, 255}, pattern = LinePattern.None, fillColor = {255, 62, 62},
+            fillPattern = FillPattern.Solid, origin = {4, 0}, rotation = 360), Rectangle(extent = {{-76, 100}, {84, -100}}, lineColor = {0, 0, 0},
+            lineThickness = 1), Line(points = {{-21, 94}, {-21, 132}}, color = {0, 0, 0}, smooth = Smooth.Bezier, thickness = 1, arrow = {Arrow.Filled, Arrow.None}, origin = {-56, 67}, rotation = 270, visible = use_heatingCoil1), Line(points = {{-54, 88}, {68, 56}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{68, 56}, {-48, 44}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{-48, 44}, {62, 6}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{62, 6}, {-44, -16}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{76, -81}, {-26, -81}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{0, -9}, {0, 9}}, color = {0, 0, 0}, smooth = Smooth.Bezier, thickness = 1, arrow = {Arrow.Filled, Arrow.None}, origin = {-34, -81}, rotation = 90, visible = use_heatingCoil1), Line(points = {{62, -42}, {-44, -16}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{62, -42}, {-42, -80}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1), Line(points = {{48, 88}, {-54, 88}}, color = {0, 0, 0}, thickness = 1, smooth = Smooth.Bezier, visible = use_heatingCoil1)}), Documentation(info="<html><p>
+  <b><span style=\"color: #008000;\">Overview</span></b>
+</p>
+<p>
+  Simple multi-layer thermal energy storage model with volumes as heat
+  exchangers (no pressure losses).
+</p>
+<p>
+  <b><span style=\"color: #008000;\">Concept</span></b>
+</p>
+<p>
+  The water volume of the thermal energy storage can be discretised in
+  several layers.
+</p>
+<p>
+  The following physical processes are modelled
+</p>
+<ul>
+  <li>heat exchange with the environment
+  </li>
+  <li>heat exchange over the heat exchanger
+  </li>
+  <li>a bouyancy model for the heat transfer between the layers
+  </li>
+</ul>
+<p>
+  <br/>
+  In contrast to the StorageDetailed model, the following
+  simplifications are taken as a basis:
+</p>
+<ul>
+  <li>Only indirect charging and discharging using a heat exchanger is
+  possible. Thus, there are two separated hydraulic circuits.
+  </li>
+  <li>The heat exchanger is an array of volumes without any pressure
+  losses
+  </li>
+  <li>There is no optional heating coil and no second heating coil.
+  Hence, the StorageSimple model is limited to a two-circuit
+  application.
+  </li>
+</ul>
+<p>
+  <br/>
+  <b><span style=\"color: #008000;\">Example Results</span></b>
+</p>
+<p>
+  <a href=\"modelica://AixLib.Fluid.Storage.Examples.StorageSimpleExample\">AixLib.Fluid.Storage.Examples.StorageSimpleExample</a>
+</p>
+<ul>
+  <li>
+    <i>November 2022</i> by Laura Maier:<br/>
+      Rename model and specify difference compared to detailed thermal
+      energy storage model
+  </li>
+  <li>
+    <i>November 2014&#160;</i> by Marcus Fuchs:<br/>
+    Changed model to use Annex 60 base class
+  </li>
+  <li>
+    <i>13.12.2013</i> by Sebastian Stinner:<br/>
+    implemented
+  </li>
+</ul>
+</html>"));
+end StorageSimple;
diff --git a/AixLib/Fluid/Storage/Stratified.mo b/AixLib/Fluid/Storage/Stratified.mo
index 6d8ead735d..108b4a7e63 100644
--- a/AixLib/Fluid/Storage/Stratified.mo
+++ b/AixLib/Fluid/Storage/Stratified.mo
@@ -2,149 +2,150 @@ within AixLib.Fluid.Storage;
 model Stratified "Model of a stratified tank for thermal energy storage"
   extends AixLib.Fluid.Storage.BaseClasses.PartialStratified(vol(each nPorts=3));
 
-  Modelica.Fluid.Interfaces.FluidPort_a fluPorVol[nSeg](
+  Modelica.Fluid.Interfaces.FluidPorts_a fluPorVol[nSeg](
     redeclare each final package Medium = Medium)
     "Fluid port that connects to the control volumes of the tank"
-    annotation (Placement(transformation(extent={{-30,-10},{-10,10}}),
-        iconTransformation(extent={{-36,-10},{-16,10}})));
+    annotation (Placement(transformation(extent={{-110,-40},{-90,40}}),
+        iconTransformation(extent={{-60,-40},{-40,40}})));
 equation
-  connect(port_a, vol[1].ports[1]) annotation (Line(points={{-100,0},{-88,0},{
-          -88,-20},{16,-20},{16,-16}}, color={0,127,255}));
+  connect(port_a, vol[1].ports[1]) annotation (Line(points={{0,0},{-80,0},{-80,
+          -20},{16,-20},{16,-16}},     color={0,127,255}));
   connect(vol[nSeg].ports[2], port_b) annotation (Line(points={{16,-16},{20,-16},
-          {20,-20},{90,-20},{90,0},{100,0}}, color={0,127,255}));
+          {20,-20},{90,-20},{90,0},{0,0}},   color={0,127,255}));
   for i in 1:(nSeg-1) loop
     connect(vol[i].ports[2], vol[i + 1].ports[1]) annotation (Line(points={{16,-16},
             {16,-32},{14,-32},{14,-16},{16,-16}}, color={0,127,255}));
   end for;
   for i in 1:nSeg loop
-    connect(fluPorVol[i], vol[i].ports[3]) annotation (Line(points={{-20,0},{-20,-36},
-          {16,-36},{16,-16}}, color={0,127,255}));
+    connect(fluPorVol[i], vol[i].ports[3]) annotation (Line(points={{-100,0},{
+            -88,0},{-88,-36},{16,-36},{16,-16}},
+                              color={0,127,255}));
   end for;
   annotation (
 defaultComponentName="tan",
 Documentation(info="<html>
- <p>
- This is a model of a stratified storage tank.
- </p>
- <p>
- See the
- <a href=\"modelica://AixLib.Fluid.Storage.UsersGuide\">
- AixLib.Fluid.Storage.UsersGuide</a>
- for more information.
- </p>
- <p>
- For a model with enhanced stratification, use
- <a href=\"modelica://AixLib.Fluid.Storage.StratifiedEnhanced\">
- AixLib.Fluid.Storage.StratifiedEnhanced</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- June 1, 2018, by Michael Wetter:<br/>
- Refactored model to allow a fluid port in the tank that do not have
- the enhanced stratification model.<br/>
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1182\">
- issue 1182</a>.
- </li>
- <li>
- July 29, 2017, by Michael Wetter:<br/>
- Removed medium declaration, which is not needed and inconsistent with
- the declaration in the base class.
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/544\">
- issue 544</a>.
- </li>
- <li>
- March 28, 2015, by Filip Jorissen:<br/>
- Propagated <code>allowFlowReversal</code> and <code>m_flow_small</code>
- and set <code>mSenFac=1</code>.
- </li>
- <li>
- January 26, 2015, by Michael Wetter:<br/>
- Renamed
- <code>hA_flow</code> to <code>H_a_flow</code>,
- <code>hB_flow</code> to <code>H_b_flow</code> and
- <code>hVol_flow</code> to <code>H_vol_flow</code>
- as they output enthalpy flow rate, and not specific enthalpy.
- Made various models <code>protected</code>.
- </li>
- <li>
- January 25, 2015, by Michael Wetter:<br/>
- Added <code>final</code> to <code>tau = 0</code> in <code>EnthalpyFlowRate</code>.
- These sensors do not need dynamics as the enthalpy flow rate
- is used to compute a heat flow which is then added to the volume of the tank.
- Thus, if there were high frequency oscillations of small mass flow rates,
- then they have a small effect on <code>H_flow</code>, and they are
- not used in any control loop. Rather, the oscillations are further damped
- by the differential equation of the fluid volume.
- </li>
- <li>
- January 25, 2015, by Filip Jorissen:<br/>
- Set <code>tau = 0</code> in <code>EnthalpyFlowRate</code>
- sensors for increased simulation speed.
- </li>
- <li>
- August 29, 2014, by Michael Wetter:<br/>
- Replaced the use of <code>Medium.lambda_const</code> with
- <code>Medium.thermalConductivity(sta_default)</code> as
- <code>lambda_const</code> is not declared for all media.
- This avoids a translation error if certain media are used.
- </li>
- <li>
- June 18, 2014, by Michael Wetter:<br/>
- Changed the default value for the energy balance initialization to avoid
- a dependency on the global <code>system</code> declaration.
- </li>
- <li>
- July 29, 2011, by Michael Wetter:<br/>
- Removed <code>use_T_start</code> and <code>h_start</code>.
- </li>
- <li>
- February 18, 2011, by Michael Wetter:<br/>
- Changed default start values for temperature and pressure.
- </li>
- <li>
- October 25, 2009 by Michael Wetter:<br/>
- Changed computation of heat transfer through top (and bottom) of tank. Now,
- the thermal resistance of the fluid is not taken into account, i.e., the
- top (and bottom) element is assumed to be mixed.
- </li>
- <li>
- October 23, 2009 by Michael Wetter:<br/>
- Fixed bug in computing heat conduction of top and bottom segment.
- In the previous version,
- for computing the heat conduction between the top (or bottom) segment and
- the outside,
- the whole thickness of the water volume was used
- instead of only half the thickness.
- </li>
- <li>
- February 19, 2009 by Michael Wetter:<br/>
- Changed declaration that constrains the medium. The earlier
- declaration caused the medium model to be not shown in the parameter
- window.
- </li>
- <li>
- October 31, 2008 by Michael Wetter:<br/>
- Added heat conduction.
- </li>
- <li>
- October 23, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This is a model of a stratified storage tank.
+</p>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Storage.UsersGuide\">
+AixLib.Fluid.Storage.UsersGuide</a>
+for more information.
+</p>
+<p>
+For a model with enhanced stratification, use
+<a href=\"modelica://AixLib.Fluid.Storage.StratifiedEnhanced\">
+AixLib.Fluid.Storage.StratifiedEnhanced</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+June 1, 2018, by Michael Wetter:<br/>
+Refactored model to allow a fluid port in the tank that do not have
+the enhanced stratification model.<br/>
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1182\">
+issue 1182</a>.
+</li>
+<li>
+July 29, 2017, by Michael Wetter:<br/>
+Removed medium declaration, which is not needed and inconsistent with
+the declaration in the base class.
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/544\">
+issue 544</a>.
+</li>
+<li>
+March 28, 2015, by Filip Jorissen:<br/>
+Propagated <code>allowFlowReversal</code> and <code>m_flow_small</code>
+and set <code>mSenFac=1</code>.
+</li>
+<li>
+January 26, 2015, by Michael Wetter:<br/>
+Renamed
+<code>hA_flow</code> to <code>H_a_flow</code>,
+<code>hB_flow</code> to <code>H_b_flow</code> and
+<code>hVol_flow</code> to <code>H_vol_flow</code>
+as they output enthalpy flow rate, and not specific enthalpy.
+Made various models <code>protected</code>.
+</li>
+<li>
+January 25, 2015, by Michael Wetter:<br/>
+Added <code>final</code> to <code>tau = 0</code> in <code>EnthalpyFlowRate</code>.
+These sensors do not need dynamics as the enthalpy flow rate
+is used to compute a heat flow which is then added to the volume of the tank.
+Thus, if there were high frequency oscillations of small mass flow rates,
+then they have a small effect on <code>H_flow</code>, and they are
+not used in any control loop. Rather, the oscillations are further damped
+by the differential equation of the fluid volume.
+</li>
+<li>
+January 25, 2015, by Filip Jorissen:<br/>
+Set <code>tau = 0</code> in <code>EnthalpyFlowRate</code>
+sensors for increased simulation speed.
+</li>
+<li>
+August 29, 2014, by Michael Wetter:<br/>
+Replaced the use of <code>Medium.lambda_const</code> with
+<code>Medium.thermalConductivity(sta_default)</code> as
+<code>lambda_const</code> is not declared for all media.
+This avoids a translation error if certain media are used.
+</li>
+<li>
+June 18, 2014, by Michael Wetter:<br/>
+Changed the default value for the energy balance initialization to avoid
+a dependency on the global <code>system</code> declaration.
+</li>
+<li>
+July 29, 2011, by Michael Wetter:<br/>
+Removed <code>use_T_start</code> and <code>h_start</code>.
+</li>
+<li>
+February 18, 2011, by Michael Wetter:<br/>
+Changed default start values for temperature and pressure.
+</li>
+<li>
+October 25, 2009 by Michael Wetter:<br/>
+Changed computation of heat transfer through top (and bottom) of tank. Now,
+the thermal resistance of the fluid is not taken into account, i.e., the
+top (and bottom) element is assumed to be mixed.
+</li>
+<li>
+October 23, 2009 by Michael Wetter:<br/>
+Fixed bug in computing heat conduction of top and bottom segment.
+In the previous version,
+for computing the heat conduction between the top (or bottom) segment and
+the outside,
+the whole thickness of the water volume was used
+instead of only half the thickness.
+</li>
+<li>
+February 19, 2009 by Michael Wetter:<br/>
+Changed declaration that constrains the medium. The earlier
+declaration caused the medium model to be not shown in the parameter
+window.
+</li>
+<li>
+October 31, 2008 by Michael Wetter:<br/>
+Added heat conduction.
+</li>
+<li>
+October 23, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 Icon(graphics={
         Rectangle(
           extent={{-40,60},{40,20}},
@@ -157,54 +158,6 @@ Icon(graphics={
           pattern=LinePattern.None,
           fillColor={0,0,127},
           fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{-76,2},{-90,-2}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{0,84},{-80,80}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{-76,84},{-80,-2}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{82,0},{78,-86}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{0,84},{-4,60}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{82,-84},{2,-88}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{6,-60},{2,-84}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
-        Rectangle(
-          extent={{92,2},{78,-2}},
-          lineColor={0,0,255},
-          pattern=LinePattern.None,
-          fillColor={0,0,127},
-          fillPattern=FillPattern.Solid),
         Rectangle(
           extent={{-40,20},{40,-20}},
           lineColor={255,0,0},
@@ -255,6 +208,6 @@ Icon(graphics={
         Line(
           points={{22,-74},{70,-74},{70,72}},
           color={127,0,0},
-          pattern=LinePattern.Dot)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          pattern=LinePattern.Dot)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Stratified;
diff --git a/AixLib/Fluid/Storage/StratifiedEnhanced.mo b/AixLib/Fluid/Storage/StratifiedEnhanced.mo
index 4dc0313fc4..6246115eee 100644
--- a/AixLib/Fluid/Storage/StratifiedEnhanced.mo
+++ b/AixLib/Fluid/Storage/StratifiedEnhanced.mo
@@ -43,16 +43,16 @@ equation
           {-40,-80},{14,-80},{14,-16},{16,-16}},color={0,127,255}));
   connect(vol[nSeg].ports[2], H_b_flow.port_a) annotation (Line(points={{16,-16},
           {14,-16},{14,-80},{50,-80}}, color={0,127,255}));
-  connect(H_b_flow.port_b, port_b) annotation (Line(points={{70,-80},{80,-80},{80,
-          0},{100,0}}, color={0,127,255}));
+  connect(H_b_flow.port_b, port_b) annotation (Line(points={{70,-80},{80,-80},{
+          80,-100},{0,-100}}, color={0,127,255}));
   for i in 1:(nSeg-1) loop
     connect(vol[i].ports[2], H_vol_flow[i].port_a) annotation (Line(points={{16,
             -16},{16,-20},{-28,-20},{-28,-40},{-20,-40}}, color={0,127,255}));
     connect(H_vol_flow[i].port_b, vol[i + 1].ports[1]) annotation (Line(points={{0,-40},
             {4,-40},{4,-16},{16,-16}},         color={0,127,255}));
   end for;
-  connect(port_a, H_a_flow.port_a) annotation (Line(points={{-100,0},{
-          -80,0},{-80,-80},{-60,-80}}, color={0,127,255}));
+  connect(port_a, H_a_flow.port_a) annotation (Line(points={{0,100},{-96,100},{
+          -96,-80},{-60,-80}}, color={0,127,255}));
 
   connect(vol[1:nSeg].ports[3], str.fluidPort[2:nSeg+1])
    annotation (Line(points={{16,-16},{16,-18},{-66,-18},{-66,-40},{-60,-40}},
@@ -69,76 +69,76 @@ equation
                                                   color={0,0,127}));
   connect(str.heatPort, vol.heatPort)    annotation (Line(points={{-40,-40},{
           -32,-40},{-32,10},{6,10},{6,-6}},      color={191,0,0}));
-  connect(port_a, str.fluidPort[1]) annotation (Line(points={{-100,5.55112e-16},
-          {-100,0},{-72,0},{-72,-40},{-60,-40}}, color={0,127,255}));
-  connect(port_b, str.fluidPort[nSeg + 2]) annotation (Line(points={{100,
-          5.55112e-16},{100,0},{80,0},{80,-88},{-72,-88},{-72,-40},{-60,-40}},
+  connect(port_a, str.fluidPort[1]) annotation (Line(points={{0,100},{0,92},{
+          -72,92},{-72,-40},{-60,-40}},          color={0,127,255}));
+  connect(port_b, str.fluidPort[nSeg + 2]) annotation (Line(points={{0,-100},{
+          -72,-100},{-72,-40},{-60,-40}},
                            color={0,127,255}));
   connect(mTan_flow.y, str.m_flow) annotation (Line(points={{-73,-32},{-68.5,
           -32},{-68.5,-31.8},{-62,-31.8}}, color={0,0,127}));
   annotation (
 defaultComponentName="tan",
 Documentation(info="<html>
- <p>
- This is a model of a stratified storage tank for thermal energy storage.
- </p>
- <p>
- See the
- <a href=\"modelica://AixLib.Fluid.Storage.UsersGuide\">
- AixLib.Fluid.Storage.UsersGuide</a>
- for more information.
- </p>
- <h4>Limitations</h4>
- <p>
- The model requires at least 4 fluid segments. Hence, set <code>nSeg</code> to 4 or higher.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Set <code>final massDynamics=energyDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- June 1, 2018, by Michael Wetter:<br/>
- Refactored model to allow a fluid port in the tank that do not have
- the enhanced stratification model.<br/>
- This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1182\">
- issue 1182</a>.
- </li>
- <li>
- March 29, 2012 by Wangda Zuo:<br/>
- Revised the implementation to reduce the temperature overshoot.
- </li>
- <li>
- June 23, 2010 by Michael Wetter and Wangda Zuo:<br/>
- Changed model that is used to correct the numerical diffusion.
- The previous version used the model from Stefan Wischhusen,
- <a href=\"http://www.modelica.org/events/modelica2006/Proceedings/sessions/Session3a2.pdf\">
- An Enhanced Discretization Method for Storage
- Tank Models within Energy Systems</a>,
- <i>Modelica Conference</i>,
- Vienna, Austria, September 2006. However, for situations where there is a strong stratification,
- this model can lead to a large overshoot in tank temperatures, leading to a violation of the
- second law.
- In this revision, the model that computes the volume outlet temperatures has been changed to a third order upwind scheme,
- which is implemented in
- <a href=\"modelica://AixLib.Fluid.Storage.BaseClasses.ThirdOrderStratifier\">
- AixLib.Fluid.Storage.BaseClasses.ThirdOrderStratifier</a>.
- </li>
- <li>
- October 23, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This is a model of a stratified storage tank for thermal energy storage.
+</p>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Storage.UsersGuide\">
+AixLib.Fluid.Storage.UsersGuide</a>
+for more information.
+</p>
+<h4>Limitations</h4>
+<p>
+The model requires at least 4 fluid segments. Hence, set <code>nSeg</code> to 4 or higher.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Set <code>final massDynamics=energyDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+June 1, 2018, by Michael Wetter:<br/>
+Refactored model to allow a fluid port in the tank that do not have
+the enhanced stratification model.<br/>
+This is for <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/1182\">
+issue 1182</a>.
+</li>
+<li>
+March 29, 2012 by Wangda Zuo:<br/>
+Revised the implementation to reduce the temperature overshoot.
+</li>
+<li>
+June 23, 2010 by Michael Wetter and Wangda Zuo:<br/>
+Changed model that is used to correct the numerical diffusion.
+The previous version used the model from Stefan Wischhusen,
+<a href=\"http://www.modelica.org/events/modelica2006/Proceedings/sessions/Session3a2.pdf\">
+An Enhanced Discretization Method for Storage
+Tank Models within Energy Systems</a>,
+<i>Modelica Conference</i>,
+Vienna, Austria, September 2006. However, for situations where there is a strong stratification,
+this model can lead to a large overshoot in tank temperatures, leading to a violation of the
+second law.
+In this revision, the model that computes the volume outlet temperatures has been changed to a third order upwind scheme,
+which is implemented in
+<a href=\"modelica://AixLib.Fluid.Storage.BaseClasses.ThirdOrderStratifier\">
+AixLib.Fluid.Storage.BaseClasses.ThirdOrderStratifier</a>.
+</li>
+<li>
+October 23, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
  Icon(graphics={
         Rectangle(
           extent={{-40,20},{40,-20}},
@@ -162,6 +162,6 @@ Documentation(info="<html>
           lineColor={0,0,255},
           pattern=LinePattern.None,
           fillColor={255,255,0},
-          fillPattern=FillPattern.Solid)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end StratifiedEnhanced;
diff --git a/AixLib/Fluid/Storage/StratifiedEnhancedInternalHex.mo b/AixLib/Fluid/Storage/StratifiedEnhancedInternalHex.mo
index c02ba504c8..947b39f37d 100644
--- a/AixLib/Fluid/Storage/StratifiedEnhancedInternalHex.mo
+++ b/AixLib/Fluid/Storage/StratifiedEnhancedInternalHex.mo
@@ -95,13 +95,13 @@ model StratifiedEnhancedInternalHex
     redeclare final package Medium =MediumHex,
      m_flow(min=if allowFlowReversalHex then -Modelica.Constants.inf else 0))
     "Heat exchanger inlet"
-   annotation (Placement(transformation(extent={{-110,-48},{-90,-28}}),
+   annotation (Placement(transformation(extent={{-150,-30},{-130,-10}}),
                    iconTransformation(extent={{-110,-48},{-90,-28}})));
   Modelica.Fluid.Interfaces.FluidPort_b portHex_b(
      redeclare final package Medium = MediumHex,
      m_flow(max=if allowFlowReversalHex then Modelica.Constants.inf else 0))
     "Heat exchanger outlet"
-   annotation (Placement(transformation(extent={{-110,-90},{-90,-70}}),
+   annotation (Placement(transformation(extent={{-150,-90},{-130,-70}}),
         iconTransformation(extent={{-110,-90},{-90,-70}})));
 
   BaseClasses.IndirectTankHeatExchanger indTanHex(
@@ -126,11 +126,10 @@ model StratifiedEnhancedInternalHex
     final allowFlowReversal=allowFlowReversalHex,
     final m_flow_small=1e-4*abs(mHex_flow_nominal))
     "Heat exchanger inside the tank"
-     annotation (Placement(
-        transformation(
-        extent={{-10,-15},{10,15}},
+     annotation (Placement(transformation(
+        extent={{10,-15},{-10,15}},
         rotation=180,
-        origin={-87,32})));
+        origin={-120,-20})));
 
   Modelica.Units.SI.HeatFlowRate QHex_flow=-sum(indTanHex.port.Q_flow)
     "Heat transferred from the heat exchanger to the tank";
@@ -173,17 +172,17 @@ equation
     for i in 1:hexSegMult loop
       connect(indTanHex.port[j*hexSegMult+i], heaPorVol[segHex_a + (if hHex_a > hHex_b then j else -j)])
         annotation (Line(
-       points={{-87,41.8},{-20,41.8},{-20,-2.22045e-16},{0,-2.22045e-16}},
+       points={{-120,-10.2},{-120,0},{0,0}},
        color={191,0,0},
        smooth=Smooth.None));
     end for;
   end for;
   connect(portHex_a, indTanHex.port_a) annotation (Line(
-      points={{-100,-38},{-68,-38},{-68,32},{-77,32}},
+      points={{-140,-20},{-130,-20}},
       color={0,127,255},
       smooth=Smooth.None));
   connect(indTanHex.port_b, portHex_b) annotation (Line(
-      points={{-97,32},{-98,32},{-98,18},{-70,18},{-70,-80},{-100,-80}},
+      points={{-110,-20},{-100,-20},{-100,-80},{-140,-80}},
       color={0,127,255},
       smooth=Smooth.None));
 
@@ -229,114 +228,115 @@ equation
           fillPattern=FillPattern.Solid)}),
 defaultComponentName = "tan",
 Documentation(info = "<html>
- <p>
- This is a model of a stratified storage tank for thermal energy storage with built-in heat exchanger.
- </p>
- <p>
- See the
- <a href=\"modelica://AixLib.Fluid.Storage.UsersGuide\">
- AixLib.Fluid.Storage.UsersGuide</a>
- for more information.
- </p>
- <h4>Limitations</h4>
- <p>
- The model requires at least 4 fluid segments. Hence, set <code>nSeg</code> to 4 or higher.
- </p>
- </html>",
+<p>
+This is a model of a stratified storage tank for thermal energy storage with built-in heat exchanger.
+</p>
+<p>
+See the
+<a href=\"modelica://AixLib.Fluid.Storage.UsersGuide\">
+AixLib.Fluid.Storage.UsersGuide</a>
+for more information.
+</p>
+<h4>Limitations</h4>
+<p>
+The model requires at least 4 fluid segments. Hence, set <code>nSeg</code> to 4 or higher.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code> and <code>massDynamicsHex</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- June 23, 2016, by Michael Wetter:<br/>
- Corrected computation of the heat exchanger location which was wrong
- if <code>hHex_a &lt; hHex_b</code>, e.g., the port a of the heat exchanger
- is below the port b.
- This closes
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/531\">issue 531</a>.
- </li>
- <li>
- January 22, 2016, by Michael Wetter:<br/>
- Corrected type declaration of pressure difference.
- This is
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
- </li>
- <li>
- July 2, 2015, by Michael Wetter:<br/>
- Set the default value <code>energyDynamicsHexSolid=energyDynamicsHex</code>
- rather than
- <code>energyDynamicsHexSolid=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial</code>
- as users are not likely to want different settings.
- </li>
- <li>
- July 1, 2015, by Filip Jorissen:<br/>
- Added parameter <code>energyDynamicsHexSolid</code>.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/434\">
- #434</a>.
- </li>
- <li>
- March 28, 2015, by Filip Jorissen:<br/>
- Propagated <code>allowFlowReversal</code> and <code>m_flow_small</code>.
- </li>
- <li>
- September 2, 2014 by Michael Wetter:<br/>
- Replaced the <code>abs()</code> function in the assignment of the parameter
- <code>nSegHexTan</code> as the return value of <code>abs()</code>
- is a <code>Real</code> which causes a type error during model check.
- </li>
- <li>
- August 29, 2014 by Michael Wetter:<br/>
- Corrected issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/271\">#271</a>
- which led to a compilation error if the heat exchanger and the tank
- had different media.
- </li>
- <li>
- April 18, 2014 by Michael Wetter:<br/>
- Added missing ceiling function in computation of <code>botHexSeg</code>.
- Without this function, this parameter can take on zero, which is wrong
- because the Modelica uses one-based arrays.
- 
- Revised the model as the old version required the port<sub>a</sub>
- of the heat exchanger to be located higher than port<sub>b</sub>.
- This makes sense if the heat exchanger is used to heat up the tank,
- but not if it is used to cool down a tank, such as in a cooling plant.
- The following parameters were changed:
- <ol>
- <li>Changed <code>hexTopHeight</code> to <code>hHex_a</code>.</li>
- <li>Changed <code>hexBotHeight</code> to <code>hHex_b</code>.</li>
- <li>Changed <code>topHexSeg</code> to <code>segHex_a</code>,
-  and made it protected as this is deduced from <code>hHex_a</code>.</li>
- <li>Changed <code>botHexSeg</code> to <code>segHex_b</code>,
-  and made it protected as this is deduced from <code>hHex_b</code>.</li>
- </ol>
- The names of the following ports have been changed:
- <ol>
- <li>Changed <code>port_a1</code> to <code>portHex_a</code>.</li>
- <li>Changed <code>port_b1</code> to <code>portHex_b</code>.</li>
- </ol>
- The conversion script should update old instances of
- this model automatically in Dymola for all of the above changes.
- </li>
- <li>
- May 10, 2013 by Michael Wetter:<br/>
- Removed <code>m_flow_nominal_tank</code> which was not used.
- </li>
- <li>
- January 29, 2013 by Peter Grant:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code> and <code>massDynamicsHex</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+June 23, 2016, by Michael Wetter:<br/>
+Corrected computation of the heat exchanger location which was wrong
+if <code>hHex_a &lt; hHex_b</code>, e.g., the port a of the heat exchanger
+is below the port b.
+This closes
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/531\">issue 531</a>.
+</li>
+<li>
+January 22, 2016, by Michael Wetter:<br/>
+Corrected type declaration of pressure difference.
+This is
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/404\">#404</a>.
+</li>
+<li>
+July 2, 2015, by Michael Wetter:<br/>
+Set the default value <code>energyDynamicsHexSolid=energyDynamicsHex</code>
+rather than
+<code>energyDynamicsHexSolid=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial</code>
+as users are not likely to want different settings.
+</li>
+<li>
+July 1, 2015, by Filip Jorissen:<br/>
+Added parameter <code>energyDynamicsHexSolid</code>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/434\">
+#434</a>.
+</li>
+<li>
+March 28, 2015, by Filip Jorissen:<br/>
+Propagated <code>allowFlowReversal</code> and <code>m_flow_small</code>.
+</li>
+<li>
+September 2, 2014 by Michael Wetter:<br/>
+Replaced the <code>abs()</code> function in the assignment of the parameter
+<code>nSegHexTan</code> as the return value of <code>abs()</code>
+is a <code>Real</code> which causes a type error during model check.
+</li>
+<li>
+August 29, 2014 by Michael Wetter:<br/>
+Corrected issue <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/271\">#271</a>
+which led to a compilation error if the heat exchanger and the tank
+had different media.
+</li>
+<li>
+April 18, 2014 by Michael Wetter:<br/>
+Added missing ceiling function in computation of <code>botHexSeg</code>.
+Without this function, this parameter can take on zero, which is wrong
+because the Modelica uses one-based arrays.
+
+Revised the model as the old version required the port<sub>a</sub>
+of the heat exchanger to be located higher than port<sub>b</sub>.
+This makes sense if the heat exchanger is used to heat up the tank,
+but not if it is used to cool down a tank, such as in a cooling plant.
+The following parameters were changed:
+<ol>
+<li>Changed <code>hexTopHeight</code> to <code>hHex_a</code>.</li>
+<li>Changed <code>hexBotHeight</code> to <code>hHex_b</code>.</li>
+<li>Changed <code>topHexSeg</code> to <code>segHex_a</code>,
+ and made it protected as this is deduced from <code>hHex_a</code>.</li>
+<li>Changed <code>botHexSeg</code> to <code>segHex_b</code>,
+ and made it protected as this is deduced from <code>hHex_b</code>.</li>
+</ol>
+The names of the following ports have been changed:
+<ol>
+<li>Changed <code>port_a1</code> to <code>portHex_a</code>.</li>
+<li>Changed <code>port_b1</code> to <code>portHex_b</code>.</li>
+</ol>
+The conversion script should update old instances of
+this model automatically in Dymola for all of the above changes.
+</li>
+<li>
+May 10, 2013 by Michael Wetter:<br/>
+Removed <code>m_flow_nominal_tank</code> which was not used.
+</li>
+<li>
+January 29, 2013 by Peter Grant:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Diagram(coordinateSystem(extent={{-140,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end StratifiedEnhancedInternalHex;
diff --git a/AixLib/Fluid/Storage/UsersGuide.mo b/AixLib/Fluid/Storage/UsersGuide.mo
index 22aa4931e6..95a1aa73c3 100644
--- a/AixLib/Fluid/Storage/UsersGuide.mo
+++ b/AixLib/Fluid/Storage/UsersGuide.mo
@@ -172,7 +172,7 @@ as this seems to be the typical configuration.
 </p>
 <p>
 The heat exchanger is implemented in
-<a href=\"AixLib.Fluid.Storage.BaseClasses.IndirectTankHeatExchanger\">
+<a href=\"modelica://AixLib.Fluid.Storage.BaseClasses.IndirectTankHeatExchanger\">
 AixLib.Fluid.Storage.BaseClasses.IndirectTankHeatExchanger</a>.
 </p>
 </td>
diff --git a/AixLib/Fluid/Storage/Validation/HeatExchangerDynamics.mo b/AixLib/Fluid/Storage/Validation/HeatExchangerDynamics.mo
index f76ac818b0..66f2af7e0f 100644
--- a/AixLib/Fluid/Storage/Validation/HeatExchangerDynamics.mo
+++ b/AixLib/Fluid/Storage/Validation/HeatExchangerDynamics.mo
@@ -87,11 +87,11 @@ model HeatExchangerDynamics
   AixLib.Fluid.Sources.MassFlowSource_T mWatTanDyn_flow(
     redeclare package Medium = Medium,
     nPorts=1) "Mass flow rate through the tank"
-    annotation (Placement(transformation(extent={{88,20},{68,40}})));
+    annotation (Placement(transformation(extent={{82,10},{62,30}})));
   AixLib.Fluid.Sources.MassFlowSource_T mWatTanSte_flow(
     redeclare package Medium = Medium,
     nPorts=1) "Mass flow rate through the tank"
-    annotation (Placement(transformation(extent={{88,-20},{68,0}})));
+    annotation (Placement(transformation(extent={{82,-30},{62,-10}})));
 equation
   connect(mHex_flow_in.y, mHex_flow1.m_flow_in) annotation (Line(
       points={{-79,20},{-70,20},{-70,28},{-62,28}},
@@ -101,57 +101,58 @@ equation
           {-70,-2},{-70,20},{-79,20}}, color={0,0,127}));
   connect(mHex_flow2.ports[1], tanSte.portHex_a) annotation (Line(points={{-40,-10},
           {-32,-10},{-30,-10},{-30,-13.8},{32,-13.8}},  color={0,127,255}));
-  connect(watInTan.ports[1], tanSte.port_a) annotation (Line(points={{-40,62},{
-          -40,59},{-22,59},{-22,-10},{32,-10}},
-                                             color={0,127,255}));
+  connect(watInTan.ports[1], tanSte.port_a) annotation (Line(points={{-40,59},{
+          -40,59},{-22,59},{-22,0},{42,0}},  color={0,127,255}));
   connect(mHex_flow1.ports[1], tanDyn.portHex_a) annotation (Line(points={{-40,
           20},{-30,20},{-30,26.2},{32,26.2}}, color={0,127,255}));
-  connect(watInTan.ports[2], tanDyn.port_a) annotation (Line(points={{-40,58},{
-          -30,58},{-20,58},{-20,30},{32,30}},
+  connect(watInTan.ports[2], tanDyn.port_a) annotation (Line(points={{-40,61},{
+          -30,61},{-20,61},{-20,40},{42,40}},
                                            color={0,127,255}));
   connect(senTanDyn.port_a, tanDyn.portHex_b) annotation (Line(points={{10,10},{
           20,10},{20,22},{32,22}}, color={0,127,255}));
   connect(senTanSte.port_a, tanSte.portHex_b) annotation (Line(points={{10,-40},
           {20,-40},{20,-18},{32,-18}}, color={0,127,255}));
-  connect(senTanDyn.port_b, sin.ports[1]) annotation (Line(points={{-10,10},{-20,
-          10},{-20,-36},{-42,-36}}, color={0,127,255}));
-  connect(senTanSte.port_b, sin.ports[2]) annotation (Line(points={{-10,-40},{-16,
-          -40},{-42,-40}}, color={0,127,255}));
+  connect(senTanDyn.port_b, sin.ports[1]) annotation (Line(points={{-10,10},{
+          -20,10},{-20,-39},{-42,-39}},
+                                    color={0,127,255}));
+  connect(senTanSte.port_b, sin.ports[2]) annotation (Line(points={{-10,-40},{
+          -42,-40},{-42,-37}},
+                           color={0,127,255}));
   connect(mWatTanDyn_flow.ports[1], tanDyn.port_b)
-    annotation (Line(points={{68,30},{52,30}}, color={0,127,255}));
+    annotation (Line(points={{62,20},{42,20}}, color={0,127,255}));
   connect(mWatTanSte_flow.ports[1], tanSte.port_b)
-    annotation (Line(points={{68,-10},{52,-10}}, color={0,127,255}));
+    annotation (Line(points={{62,-20},{42,-20}}, color={0,127,255}));
   annotation (
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Validation/HeatExchangerDynamics.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This validation model compares two tank models. The only difference between
- the two tank models is that one uses a dynamic energy balance, whereas
- the other uses a steady-state energy balance for the heat exchanger.
- The mass flow rate through the heat exchanger is varied from zero to
- the design flow rate and back to zero to test the model under conditions in
- which no water flows through the heat exchanger.
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- July 5, 2017, by Michael Wetter:<br/>
- Added zero mass flow rate boundary conditions to avoid a translation error in Dymola 2018.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/834\">issue 834</a>.
- </li>
- <li>
- January 8, 2016 by Michael Wetter:<br/>
- First implementation to test
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/434\">issue 434</a>.
- </li>
- </ul>
- </html>"),
-    experiment(Tolerance=1e-6, StopTime=14400),
-  __Dymola_LockedEditing="Model from IBPSA");
+This validation model compares two tank models. The only difference between
+the two tank models is that one uses a dynamic energy balance, whereas
+the other uses a steady-state energy balance for the heat exchanger.
+The mass flow rate through the heat exchanger is varied from zero to
+the design flow rate and back to zero to test the model under conditions in
+which no water flows through the heat exchanger.
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+July 5, 2017, by Michael Wetter:<br/>
+Added zero mass flow rate boundary conditions to avoid a translation error in Dymola 2018.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/834\">issue 834</a>.
+</li>
+<li>
+January 8, 2016 by Michael Wetter:<br/>
+First implementation to test
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/434\">issue 434</a>.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=14400), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeatExchangerDynamics;
diff --git a/AixLib/Fluid/Storage/Validation/HeatExchangerLocation.mo b/AixLib/Fluid/Storage/Validation/HeatExchangerLocation.mo
index c4b2e3d10b..fe51a4cebf 100644
--- a/AixLib/Fluid/Storage/Validation/HeatExchangerLocation.mo
+++ b/AixLib/Fluid/Storage/Validation/HeatExchangerLocation.mo
@@ -104,34 +104,34 @@ equation
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Validation/HeatExchangerLocation.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This validation model compares two tank models. The only difference between
- the two tank models is that <code>tan_aTop</code> has the hot water inlet
- for the heat exchanger above its outlet, whereas <code>tan_bTop</code>
- has the hot water inlet below its outlet. In both models, the heat exchanger
- extends from element <i>9</i> to element <i>11</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- <li>
- July 5, 2017, by Michael Wetter:<br/>
- Added zero mass flow rate boundary conditions to avoid a translation error in Dymola 2018.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/834\">issue 834</a>.
- </li>
- <li>
- June 23, 2016 by Michael Wetter:<br/>
- First implementation to test
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/531\">issue 531</a>.
- </li>
- </ul>
- </html>"),
-    experiment(Tolerance=1e-6, StopTime=600000),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This validation model compares two tank models. The only difference between
+the two tank models is that <code>tan_aTop</code> has the hot water inlet
+for the heat exchanger above its outlet, whereas <code>tan_bTop</code>
+has the hot water inlet below its outlet. In both models, the heat exchanger
+extends from element <i>9</i> to element <i>11</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+<li>
+July 5, 2017, by Michael Wetter:<br/>
+Added zero mass flow rate boundary conditions to avoid a translation error in Dymola 2018.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/834\">issue 834</a>.
+</li>
+<li>
+June 23, 2016 by Michael Wetter:<br/>
+First implementation to test
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/531\">issue 531</a>.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=600000), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HeatExchangerLocation;
diff --git a/AixLib/Fluid/Storage/Validation/StratifiedLoadingUnloading.mo b/AixLib/Fluid/Storage/Validation/StratifiedLoadingUnloading.mo
index 927fe263e2..40bd61f6a2 100644
--- a/AixLib/Fluid/Storage/Validation/StratifiedLoadingUnloading.mo
+++ b/AixLib/Fluid/Storage/Validation/StratifiedLoadingUnloading.mo
@@ -147,20 +147,20 @@ equation
   annotation (                     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Validation/StratifiedLoadingUnloading.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This test model compares two tank models. The only difference between
- the two tank models is that one uses the third order upwind discretization
- scheme that reduces numerical diffusion that is induced when connecting
- volumes in series.
- </html>",revisions="<html>
- <ul>
- <li>
- June 7, 2018 by Filip Jorissen:<br/>
- Copied model from Buildings and update the model accordingly.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
- </li>
- </ul>
- </html>"),
-    experiment(Tolerance=1e-6, StopTime=14400),
-  __Dymola_LockedEditing="Model from IBPSA");
+This test model compares two tank models. The only difference between
+the two tank models is that one uses the third order upwind discretization
+scheme that reduces numerical diffusion that is induced when connecting
+volumes in series.
+</html>", revisions="<html>
+<ul>
+<li>
+June 7, 2018 by Filip Jorissen:<br/>
+Copied model from Buildings and update the model accordingly.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/314\">#314</a>.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=14400), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end StratifiedLoadingUnloading;
diff --git a/AixLib/Fluid/Storage/Validation/StratifiedNonUniformInitial.mo b/AixLib/Fluid/Storage/Validation/StratifiedNonUniformInitial.mo
index 861b72b2ab..b9e758f541 100644
--- a/AixLib/Fluid/Storage/Validation/StratifiedNonUniformInitial.mo
+++ b/AixLib/Fluid/Storage/Validation/StratifiedNonUniformInitial.mo
@@ -131,19 +131,19 @@ annotation (experiment(Tolerance=1e-6, StopTime=3600),
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Fluid/Storage/Validation/StratifiedNonUniformInitial.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- This test model validates
- <a href=\"modelica://AixLib.Fluid.Storage.Stratified\">
- AixLib.Fluid.Storage.Stratified</a> by specifying a non-uniform initial 
- temperature. 
- </html>",revisions="<html>
- <ul>
- <li>
- November 13, 2019 by Jianjun Hu:<br/>
- Changed the uniform initial tank temperature to be non-uniform.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1246\">#1246</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This test model validates
+<a href=\"modelica://AixLib.Fluid.Storage.Stratified\">
+AixLib.Fluid.Storage.Stratified</a> by specifying a non-uniform initial 
+temperature. 
+</html>", revisions="<html>
+<ul>
+<li>
+November 13, 2019 by Jianjun Hu:<br/>
+Changed the uniform initial tank temperature to be non-uniform.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1246\">#1246</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end StratifiedNonUniformInitial;
diff --git a/AixLib/Fluid/Storage/package.order b/AixLib/Fluid/Storage/package.order
index 36d4bed7bb..9ad0ec530e 100644
--- a/AixLib/Fluid/Storage/package.order
+++ b/AixLib/Fluid/Storage/package.order
@@ -1,7 +1,7 @@
 UsersGuide
-BufferStorage
 ExpansionVessel
-Storage
+StorageDetailed
+StorageSimple
 Stratified
 StratifiedEnhanced
 StratifiedEnhancedInternalHex
diff --git a/AixLib/Fluid/Types.mo b/AixLib/Fluid/Types.mo
index 02490d0759..250cfa6c42 100644
--- a/AixLib/Fluid/Types.mo
+++ b/AixLib/Fluid/Types.mo
@@ -14,37 +14,37 @@ package Types "Package with type definitions"
       Av "Av (metric) flow coefficient")
     "Enumeration to define the choice of valve flow coefficient" annotation (
       Documentation(info="<html>
- 
- <p>
- Enumeration to define the choice of valve flow coefficient
- (to be selected via choices menu):
- </p>
- 
- <table summary=\"summary\"  border=\"1\">
- <tr><th>Enumeration</th>
-     <th>Description</th></tr>
- 
- <tr><td>OpPoint</td>
-     <td>flow coefficient defined by ratio m_flow_nominal/sqrt(dp_nominal)</td></tr>
- 
- <tr><td>Kv</td>
-     <td>Kv (metric) flow coefficient</td></tr>
- 
- <tr><td>Cv</td>
-     <td>Cv (US) flow coefficient</td></tr>
- 
- <tr><td>Av</td>
-     <td>Av (metric) flow coefficient</td></tr>
- 
- </table>
- 
- <p>
- The details of the coefficients are explained in the
- <a href=\"modelica://Modelica.Fluid.UsersGuide.ComponentDefinition.ValveCharacteristics\">
- Users Guide</a>.
- </p>
- 
- </html>"));
+
+<p>
+Enumeration to define the choice of valve flow coefficient
+(to be selected via choices menu):
+</p>
+
+<table summary=\"summary\"  border=\"1\">
+<tr><th>Enumeration</th>
+    <th>Description</th></tr>
+
+<tr><td>OpPoint</td>
+    <td>flow coefficient defined by ratio m_flow_nominal/sqrt(dp_nominal)</td></tr>
+
+<tr><td>Kv</td>
+    <td>Kv (metric) flow coefficient</td></tr>
+
+<tr><td>Cv</td>
+    <td>Cv (US) flow coefficient</td></tr>
+
+<tr><td>Av</td>
+    <td>Av (metric) flow coefficient</td></tr>
+
+</table>
+
+<p>
+The details of the coefficients are explained in the
+<a href=\"modelica://Modelica.Fluid.UsersGuide.ComponentDefinition.ValveCharacteristics\">
+Users Guide</a>.
+</p>
+
+</html>"));
   type HeatExchangerConfiguration = enumeration(
       ParallelFlow "Parallel flow",
       CounterFlow "Counter flow",
@@ -56,48 +56,48 @@ package Types "Package with type definitions"
       ConstantTemperaturePhaseChange "Constant temperature phase change in one stream")
     "Enumeration for heat exchanger construction"
   annotation(Documentation(info="<html>
- <p>
-  Enumeration that defines the heat exchanger construction.
+<p>
+ Enumeration that defines the heat exchanger construction.
+</p>
+<p>
+The following heat exchanger configurations are available in this enumeration:
+</p>
+<table summary=\"summary\" border=\"1\">
+<tr><th>Enumeration</th><th>Description</th></tr>
+<tr><td>ParallelFlow</td><td>Parallel flow</td></tr>
+<tr><td>CounterFlow</td><td>Counter flow</td></tr>
+<tr><td>CrossFlowUnmixed</td><td>Cross flow, both streams unmixed</td></tr>
+<tr><td>CrossFlowStream1MixedStream2Unmixed</td><td>Cross flow, stream 1 mixed, stream 2 unmixed</td></tr>
+<tr><td>CrossFlowStream1UnmixedStream2Mixed</td><td>Cross flow, stream 1 unmixed, stream 2 mixed</td></tr>
+<tr><td>ConstantTemperaturePhaseChange</td><td>Constant temperature phase change in one stream</td></tr>
+</table>
+<p>
+Note that for a given heat exchanger, the
+ <code>HeatExchangerConfiguration</code> is fixed. However, if the capacity
+ flow rates change, then the
+ <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
+ AixLib.Fluid.Types.HeatExchangerFlowRegime</a> may change. For example,
+ a counter flow heat exchanger has <code>HeatExchangerConfiguration=CounterFlow</code>,
+ but the <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
+ AixLib.Fluid.Types.HeatExchangerFlowRegime</a> can change to parallel flow if one of the two capacity flow rates reverts
+ its direction.
  </p>
- <p>
- The following heat exchanger configurations are available in this enumeration:
- </p>
- <table summary=\"summary\" border=\"1\">
- <tr><th>Enumeration</th><th>Description</th></tr>
- <tr><td>ParallelFlow</td><td>Parallel flow</td></tr>
- <tr><td>CounterFlow</td><td>Counter flow</td></tr>
- <tr><td>CrossFlowUnmixed</td><td>Cross flow, both streams unmixed</td></tr>
- <tr><td>CrossFlowStream1MixedStream2Unmixed</td><td>Cross flow, stream 1 mixed, stream 2 unmixed</td></tr>
- <tr><td>CrossFlowStream1UnmixedStream2Mixed</td><td>Cross flow, stream 1 unmixed, stream 2 mixed</td></tr>
- <tr><td>ConstantTemperaturePhaseChange</td><td>Constant temperature phase change in one stream</td></tr>
- </table>
- <p>
- Note that for a given heat exchanger, the
-  <code>HeatExchangerConfiguration</code> is fixed. However, if the capacity
-  flow rates change, then the
-  <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
-  AixLib.Fluid.Types.HeatExchangerFlowRegime</a> may change. For example,
-  a counter flow heat exchanger has <code>HeatExchangerConfiguration=CounterFlow</code>,
-  but the <a href=\"modelica://AixLib.Fluid.Types.HeatExchangerFlowRegime\">
-  AixLib.Fluid.Types.HeatExchangerFlowRegime</a> can change to parallel flow if one of the two capacity flow rates reverts
-  its direction.
-  </p>
- </html>",revisions=
+</html>", revisions=
           "<html>
- <ul>
- <li>
- March 27, 2017, by Michael Wetter:<br/>
- Added <code>ConstantTemperaturePhaseChange</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/694\">
- AixLib #694</a>.
- </li>
- <li>
- February 18, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+March 27, 2017, by Michael Wetter:<br/>
+Added <code>ConstantTemperaturePhaseChange</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/694\">
+AixLib #694</a>.
+</li>
+<li>
+February 18, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 
   type HeatExchangerFlowRegime = enumeration(
       ParallelFlow "Parallel flow",
@@ -108,74 +108,74 @@ package Types "Package with type definitions"
       ConstantTemperaturePhaseChange "Constant temperature phase change in one stream")
     "Enumeration for heat exchanger flow configuration"
   annotation(Documentation(info="<html>
- <p>
-  Enumeration to define the heat exchanger flow regime.
- </p>
- <p>
- This enumeration defines for the current capacity flow rate the kind of
- heat transfer relation that will be used to compute the relation between
- effectiveness and Number of Transfer Units.
- </p>
- <p>
- The following heat exchanger flow regimes are available in this enumeration:
- </p>
- <table summary=\"summary\" border=\"1\">
- <tr><th>Enumeration</th><th>Description</th></tr>
- <tr><td>ParallelFlow</td><td>Parallel flow</td></tr>
- <tr><td>CounterFlow</td><td>Counter flow</td></tr>
- <tr><td>CrossFlowUnmixed</td><td>Cross flow, both streams unmixed</td></tr>
- <tr><td>CrossFlowCMinMixedCMaxUnmixed</td><td>Cross flow, CMin mixed,   CMax unmixed</td></tr>
- <tr><td>CrossFlowCMinUnmixedCMaxMixed</td><td>Cross flow, CMin unmixed, CMax mixed</td></tr>
- <tr><td>ConstantTemperaturePhaseChange</td><td>Constant temperature phase change in one stream</td></tr>
- </table>
- </html>",revisions="<html>
- <ul>
- <li>
- March 27, 2017, by Michael Wetter:<br/>
- Added <code>ConstantTemperaturePhaseChange</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/694\">
- AixLib #694</a>.
- </li>
- <li>
- February 18, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+ Enumeration to define the heat exchanger flow regime.
+</p>
+<p>
+This enumeration defines for the current capacity flow rate the kind of
+heat transfer relation that will be used to compute the relation between
+effectiveness and Number of Transfer Units.
+</p>
+<p>
+The following heat exchanger flow regimes are available in this enumeration:
+</p>
+<table summary=\"summary\" border=\"1\">
+<tr><th>Enumeration</th><th>Description</th></tr>
+<tr><td>ParallelFlow</td><td>Parallel flow</td></tr>
+<tr><td>CounterFlow</td><td>Counter flow</td></tr>
+<tr><td>CrossFlowUnmixed</td><td>Cross flow, both streams unmixed</td></tr>
+<tr><td>CrossFlowCMinMixedCMaxUnmixed</td><td>Cross flow, CMin mixed,   CMax unmixed</td></tr>
+<tr><td>CrossFlowCMinUnmixedCMaxMixed</td><td>Cross flow, CMin unmixed, CMax mixed</td></tr>
+<tr><td>ConstantTemperaturePhaseChange</td><td>Constant temperature phase change in one stream</td></tr>
+</table>
+</html>", revisions="<html>
+<ul>
+<li>
+March 27, 2017, by Michael Wetter:<br/>
+Added <code>ConstantTemperaturePhaseChange</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/694\">
+AixLib #694</a>.
+</li>
+<li>
+February 18, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   type InputType = enumeration(
       Constant "Use parameter to set stage",
       Stages "Use integer input to select stage",
       Continuous "Use continuous, real input") "Input options for movers"
     annotation (Documentation(info="<html>
- <p>
- This type allows defining which type of input should be used for movers.
- This can either be
- </p>
- <ol>
- <li>
- a constant set point declared by a parameter,
- </li>
- <li>
- a series of possible set points that can be switched using an integer input, or
- </li>
- <li>
- a continuously variable set point.
- </li>
- </ol>
- </html>",revisions="<html>
- <ul>
- <li>
- April 2, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+This type allows defining which type of input should be used for movers.
+This can either be
+</p>
+<ol>
+<li>
+a constant set point declared by a parameter,
+</li>
+<li>
+a series of possible set points that can be switched using an integer input, or
+</li>
+<li>
+a continuously variable set point.
+</li>
+</ol>
+</html>", revisions="<html>
+<ul>
+<li>
+April 2, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 
  annotation (preferredView="info", Documentation(info="<html>
- <p>
- This package contains type definitions.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This package contains type definitions.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Types;
diff --git a/AixLib/Fluid/package.order b/AixLib/Fluid/package.order
index aa0e98cd8f..516433de38 100644
--- a/AixLib/Fluid/package.order
+++ b/AixLib/Fluid/package.order
@@ -13,8 +13,10 @@ Humidifiers
 MassExchangers
 MixingVolumes
 Movers
+Pools
 Sensors
 Solar
+SolarCollectors
 Sources
 Storage
 Types
diff --git a/AixLib/Media/Air.mo b/AixLib/Media/Air.mo
index 321828b7d8..ddbb56f765 100644
--- a/AixLib/Media/Air.mo
+++ b/AixLib/Media/Air.mo
@@ -52,7 +52,7 @@ package Air
   end ThermodynamicState;
   // There must not be any stateSelect=StateSelect.prefer for
   // the pressure.
-  // Otherwise, translateModel("Buildings.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume")
+  // Otherwise, translateModel("AixLib.Fluid.FMI.ExportContainers.Examples.FMUs.ResistanceVolume")
   // will fail as Dymola does an index reduction and outputs
   //   Differentiated the equation
   //   vol.dynBal.medium.p+res.dp-inlet.p = 0.0;
@@ -76,6 +76,7 @@ package Air
   InputAbsolutePressure p "Absolute pressure of medium";
   InputMassFraction[1] Xi(
     start=reference_X[1:1],
+    nominal={0.01},
     each stateSelect=if preferredMediumStates then StateSelect.prefer else StateSelect.default)
     "Structurally independent mass fractions";
   InputSpecificEnthalpy h "Specific enthalpy of medium";
@@ -83,7 +84,9 @@ package Air
   Modelica.Media.Interfaces.Types.Temperature T(
    stateSelect=if preferredMediumStates then StateSelect.prefer else StateSelect.default)
    "Temperature of medium";
-  Modelica.Media.Interfaces.Types.MassFraction[2] X(start=reference_X)
+  Modelica.Media.Interfaces.Types.MassFraction[2] X(
+    start=reference_X,
+    nominal={0.01, 1})
     "Mass fractions (= (component mass)/total mass  m_i/m)";
   Modelica.Media.Interfaces.Types.SpecificInternalEnergy u
     "Specific internal energy of medium";
@@ -91,7 +94,8 @@ package Air
     "Gas constant (of mixture if applicable)";
   Modelica.Media.Interfaces.Types.MolarMass MM
     "Molar mass (of mixture or single fluid)";
-  ThermodynamicState state
+  ThermodynamicState state(
+    X(nominal={0.01, 1}))
     "Thermodynamic state record for optional functions";
 
     Modelica.Units.NonSI.Temperature_degC T_degC=
@@ -143,9 +147,9 @@ package Air
       + "\nof medium \"AixLib.Media.Air\" is not in the range 0..1");
 
     assert(noEvent(T >= 200.0), "In "   + getInstanceName() + ": Temperature T exceeded its minimum allowed value of -73.15 degC (200 Kelvin)
- as required from medium model \"AixLib.Media.Air\".");
+as required from medium model \"AixLib.Media.Air\".");
     assert(noEvent(T <= 423.15), "In "   + getInstanceName() + ": Temperature T exceeded its maximum allowed value of 150 degC (423.15 Kelvin)
- as required from medium model \"AixLib.Media.Air\".");
+as required from medium model \"AixLib.Media.Air\".");
 
   assert(noEvent(p >= 0.0), "Pressure (= " + String(p) + " Pa) of medium \"AixLib.Media.Air\" is negative\n(Temperature = " + String(T) + " K)");
   annotation (Icon(coordinateSystem(preserveAspectRatio=true, extent={{-100,
@@ -157,50 +161,50 @@ package Air
           extent={{-152,164},{152,102}},
           textString="%name",
           textColor={0,0,255})}), Documentation(info="<html>
- <p>
- Model with basic thermodynamic properties.
- </p>
- <p>
- This model provides equation for the following thermodynamic properties:
- </p>
- <table border=\"1\" cellspacing=\"0\" cellpadding=\"2\" summary=\"Thermodynamic properties\">
-   <tr><td><strong>Variable</strong></td>
-       <td><strong>Unit</strong></td>
-       <td><strong>Description</strong></td></tr>
-   <tr><td>T</td>
-       <td>K</td>
-       <td>temperature</td></tr>
-   <tr><td>p</td>
-       <td>Pa</td>
-       <td>absolute pressure</td></tr>
-   <tr><td>d</td>
-       <td>kg/m3</td>
-       <td>density</td></tr>
-   <tr><td>h</td>
-       <td>J/kg</td>
-       <td>specific enthalpy</td></tr>
-   <tr><td>u</td>
-       <td>J/kg</td>
-       <td>specific internal energy</td></tr>
-   <tr><td>Xi[nXi]</td>
-       <td>kg/kg</td>
-       <td>independent mass fractions m_i/m</td></tr>
-   <tr><td>R</td>
-       <td>J/kg.K</td>
-       <td>gas constant</td></tr>
-   <tr><td>M</td>
-       <td>kg/mol</td>
-       <td>molar mass</td></tr>
- </table>
- </html>",revisions="<html>
- <ul>
- <li>
- September 22, 2020, by Michael Wetter:<br/>
- First implementation based on Modelica Standard Library,
- but with <code>noEvent</code> added to check of bounds.
- </li>
- </ul>
- </html>"));
+<p>
+Model with basic thermodynamic properties.
+</p>
+<p>
+This model provides equation for the following thermodynamic properties:
+</p>
+<table border=\"1\" cellspacing=\"0\" cellpadding=\"2\" summary=\"Thermodynamic properties\">
+  <tr><td><strong>Variable</strong></td>
+      <td><strong>Unit</strong></td>
+      <td><strong>Description</strong></td></tr>
+  <tr><td>T</td>
+      <td>K</td>
+      <td>temperature</td></tr>
+  <tr><td>p</td>
+      <td>Pa</td>
+      <td>absolute pressure</td></tr>
+  <tr><td>d</td>
+      <td>kg/m3</td>
+      <td>density</td></tr>
+  <tr><td>h</td>
+      <td>J/kg</td>
+      <td>specific enthalpy</td></tr>
+  <tr><td>u</td>
+      <td>J/kg</td>
+      <td>specific internal energy</td></tr>
+  <tr><td>Xi[nXi]</td>
+      <td>kg/kg</td>
+      <td>independent mass fractions m_i/m</td></tr>
+  <tr><td>R</td>
+      <td>J/kg.K</td>
+      <td>gas constant</td></tr>
+  <tr><td>M</td>
+      <td>kg/mol</td>
+      <td>molar mass</td></tr>
+</table>
+</html>", revisions="<html>
+<ul>
+<li>
+September 22, 2020, by Michael Wetter:<br/>
+First implementation based on Modelica Standard Library,
+but with <code>noEvent</code> added to check of bounds.
+</li>
+</ul>
+</html>"));
   end BaseProperties;
 
 redeclare function density "Gas density"
@@ -212,8 +216,8 @@ algorithm
   annotation(smoothOrder=5,
   Inline=true,
   Documentation(info="<html>
- Density is computed from pressure, temperature and composition in the thermodynamic state record applying the ideal gas law.
- </html>"));
+Density is computed from pressure, temperature and composition in the thermodynamic state record applying the ideal gas law.
+</html>"));
 end density;
 
 redeclare function extends dynamicViscosity
@@ -224,33 +228,33 @@ algorithm
   smoothOrder=99,
   Inline=true,
 Documentation(info="<html>
- <p>
- This function returns the dynamic viscosity.
- </p>
- <h4>Implementation</h4>
- <p>
- The function is based on the 5th order polynomial
- of
- <a href=\"modelica://Modelica.Media.Air.MoistAir.dynamicViscosity\">
- Modelica.Media.Air.MoistAir.dynamicViscosity</a>.
- However, for the typical range of temperatures encountered
- in building applications, a linear function sufficies.
- This implementation is therefore the above 5th order polynomial,
- linearized around <i>20</i>&deg;C.
- The relative error of this linearization is
- <i>0.4</i>% at <i>-20</i>&deg;C,
- and less then
- <i>0.2</i>% between  <i>-5</i>&deg;C and  <i>+50</i>&deg;C.
- </p>
- </html>",
+<p>
+This function returns the dynamic viscosity.
+</p>
+<h4>Implementation</h4>
+<p>
+The function is based on the 5th order polynomial
+of
+<a href=\"modelica://Modelica.Media.Air.MoistAir.dynamicViscosity\">
+Modelica.Media.Air.MoistAir.dynamicViscosity</a>.
+However, for the typical range of temperatures encountered
+in building applications, a linear function sufficies.
+This implementation is therefore the above 5th order polynomial,
+linearized around <i>20</i>&deg;C.
+The relative error of this linearization is
+<i>0.4</i>% at <i>-20</i>&deg;C,
+and less then
+<i>0.2</i>% between  <i>-5</i>&deg;C and  <i>+50</i>&deg;C.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 19, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 19, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end dynamicViscosity;
 
 redeclare function enthalpyOfCondensingGas
@@ -316,8 +320,8 @@ algorithm
     smoothOrder=2,
     Inline=true,
     Documentation(info="<html>
- The ideal gas constant for moist air is computed from <a href=\"modelica://Modelica.Media.Air.MoistAir.ThermodynamicState\">thermodynamic state</a> assuming that all water is in the gas phase.
- </html>"));
+The ideal gas constant for moist air is computed from <a href=\"modelica://Modelica.Media.Air.MoistAir.ThermodynamicState\">thermodynamic state</a> assuming that all water is in the gas phase.
+</html>"));
 end gasConstant;
 
 redeclare function extends pressure
@@ -329,8 +333,8 @@ algorithm
   smoothOrder=2,
   Inline=true,
   Documentation(info="<html>
- Pressure is returned from the thermodynamic state record input as a simple assignment.
- </html>"));
+Pressure is returned from the thermodynamic state record input as a simple assignment.
+</html>"));
 end pressure;
 
 redeclare function extends isobaricExpansionCoefficient
@@ -341,29 +345,29 @@ algorithm
     smoothOrder=5,
     Inline=true,
 Documentation(info="<html>
- <p>
- This function returns the isobaric expansion coefficient at constant pressure,
- which is zero for this medium.
- The isobaric expansion coefficient at constant pressure is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &beta;<sub>p</sub> = - 1 &frasl; v &nbsp; (&part; v &frasl; &part; T)<sub>p</sub> = 0,
- </p>
- <p>
- where
- <i>v</i> is the specific volume,
- <i>T</i> is the temperature and
- <i>p</i> is the pressure.
- </p>
- </html>",
+<p>
+This function returns the isobaric expansion coefficient at constant pressure,
+which is zero for this medium.
+The isobaric expansion coefficient at constant pressure is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&beta;<sub>p</sub> = - 1 &frasl; v &nbsp; (&part; v &frasl; &part; T)<sub>p</sub> = 0,
+</p>
+<p>
+where
+<i>v</i> is the specific volume,
+<i>T</i> is the temperature and
+<i>p</i> is the pressure.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end isobaricExpansionCoefficient;
 
 redeclare function extends isothermalCompressibility
@@ -374,29 +378,29 @@ algorithm
     smoothOrder=5,
     Inline=true,
     Documentation(info="<html>
- <p>
- This function returns the isothermal compressibility coefficient.
- The isothermal compressibility is
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &kappa;<sub>T</sub> = -1 &frasl; v &nbsp; (&part; v &frasl; &part; p)<sub>T</sub>
-   = -1 &frasl; p,
- </p>
- <p>
- where
- <i>v</i> is the specific volume,
- <i>T</i> is the temperature and
- <i>p</i> is the pressure.
- </p>
- </html>",
+<p>
+This function returns the isothermal compressibility coefficient.
+The isothermal compressibility is
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&kappa;<sub>T</sub> = -1 &frasl; v &nbsp; (&part; v &frasl; &part; p)<sub>T</sub>
+  = -1 &frasl; p,
+</p>
+<p>
+where
+<i>v</i> is the specific volume,
+<i>T</i> is the temperature and
+<i>p</i> is the pressure.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end isothermalCompressibility;
 
 redeclare function extends saturationPressure
@@ -424,68 +428,68 @@ algorithm
   annotation (
   Inline=true,
     Documentation(info="<html>
- <p>
- This function computes the specific entropy.
- </p>
- <p>
- The specific entropy of the mixture is obtained from
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- s = s<sub>s</sub> + s<sub>m</sub>,
- </p>
- <p>
- where
- <i>s<sub>s</sub></i> is the entropy change due to the state change
- (relative to the reference temperature) and
- <i>s<sub>m</sub></i> is the entropy change due to mixing
- of the dry air and water vapor.
- </p>
- <p>
- The entropy change due to change in state is obtained from
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- s<sub>s</sub> = c<sub>v</sub> ln(T/T<sub>0</sub>) + R ln(v/v<sub>0</sub>) <br/>
- = c<sub>v</sub> ln(T/T<sub>0</sub>) + R ln(&rho;<sub>0</sub>/&rho;)
- </p>
- <p>If we assume <i>&rho; = p<sub>0</sub>/(R T)</i>,
- and because <i>c<sub>p</sub> = c<sub>v</sub> + R</i>,
- we can write
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- s<sub>s</sub> = c<sub>v</sub> ln(T/T<sub>0</sub>) + R ln(T/T<sub>0</sub>) <br/>
- =c<sub>p</sub> ln(T/T<sub>0</sub>).
- </p>
- <p>
- Next, the entropy of mixing is obtained from a reversible isothermal
- expansion process. Hence,
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   s<sub>m</sub> = -R &sum;<sub>i</sub>( X<sub>i</sub> &frasl; M<sub>i</sub>
-   ln(Y<sub>i</sub> p/p<sub>0</sub>)),
- </p>
- <p>
- where <i>R</i> is the gas constant,
- <i>X</i> is the mass fraction,
- <i>M</i> is the molar mass, and
- <i>Y</i> is the mole fraction.
- </p>
- <p>
- To obtain the state for a given pressure, entropy and mass fraction, use
- <a href=\"modelica://AixLib.Media.Air.setState_psX\">
- AixLib.Media.Air.setState_psX</a>.
- </p>
- <h4>Limitations</h4>
- <p>
- This function is only valid for a relative humidity below 100%.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 27, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+This function computes the specific entropy.
+</p>
+<p>
+The specific entropy of the mixture is obtained from
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+s = s<sub>s</sub> + s<sub>m</sub>,
+</p>
+<p>
+where
+<i>s<sub>s</sub></i> is the entropy change due to the state change
+(relative to the reference temperature) and
+<i>s<sub>m</sub></i> is the entropy change due to mixing
+of the dry air and water vapor.
+</p>
+<p>
+The entropy change due to change in state is obtained from
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+s<sub>s</sub> = c<sub>v</sub> ln(T/T<sub>0</sub>) + R ln(v/v<sub>0</sub>) <br/>
+= c<sub>v</sub> ln(T/T<sub>0</sub>) + R ln(&rho;<sub>0</sub>/&rho;)
+</p>
+<p>If we assume <i>&rho; = p<sub>0</sub>/(R T)</i>,
+and because <i>c<sub>p</sub> = c<sub>v</sub> + R</i>,
+we can write
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+s<sub>s</sub> = c<sub>v</sub> ln(T/T<sub>0</sub>) + R ln(T/T<sub>0</sub>) <br/>
+=c<sub>p</sub> ln(T/T<sub>0</sub>).
+</p>
+<p>
+Next, the entropy of mixing is obtained from a reversible isothermal
+expansion process. Hence,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  s<sub>m</sub> = -R &sum;<sub>i</sub>( X<sub>i</sub> &frasl; M<sub>i</sub>
+  ln(Y<sub>i</sub> p/p<sub>0</sub>)),
+</p>
+<p>
+where <i>R</i> is the gas constant,
+<i>X</i> is the mass fraction,
+<i>M</i> is the molar mass, and
+<i>Y</i> is the mole fraction.
+</p>
+<p>
+To obtain the state for a given pressure, entropy and mass fraction, use
+<a href=\"modelica://AixLib.Media.Air.setState_psX\">
+AixLib.Media.Air.setState_psX</a>.
+</p>
+<h4>Limitations</h4>
+<p>
+This function is only valid for a relative humidity below 100%.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 27, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificEntropy;
 
 redeclare function extends density_derp_T
@@ -495,19 +499,19 @@ algorithm
   annotation (
   Inline=true,
 Documentation(info="<html>
- <p>
- This function returns the partial derivative of density
- with respect to pressure at constant temperature.
- </p>
- </html>",
+<p>
+This function returns the partial derivative of density
+with respect to pressure at constant temperature.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end density_derp_T;
 
 redeclare function extends density_derT_p
@@ -520,19 +524,19 @@ algorithm
   Inline=true,
   Documentation(info=
 "<html>
- <p>
- This function computes the derivative of density with respect to temperature
- at constant pressure.
- </p>
- </html>",revisions=
+<p>
+This function computes the derivative of density with respect to temperature
+at constant pressure.
+</p>
+</html>", revisions=
 "<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end density_derT_p;
 
 redeclare function extends density_derX
@@ -543,21 +547,21 @@ annotation (
   smoothOrder=99,
   Inline=true,
   Documentation(info="<html>
- <p>
- This function returns the partial derivative of density
- with respect to mass fraction.
- This value is zero because in this medium, density is proportional
- to pressure, but independent of the species concentration.
- </p>
- </html>",
+<p>
+This function returns the partial derivative of density
+with respect to mass fraction.
+This value is zero because in this medium, density is proportional
+to pressure, but independent of the species concentration.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end density_derX;
 
 redeclare replaceable function extends specificHeatCapacityCp
@@ -600,11 +604,11 @@ algorithm
     smoothOrder=2,
     Inline=true,
     Documentation(info="<html>
- <p>
- The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
-     is computed from density <code>d</code>, temperature <code>T</code> and composition <code>X</code>.
- </p>
- </html>"));
+<p>
+The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
+    is computed from density <code>d</code>, temperature <code>T</code> and composition <code>X</code>.
+</p>
+</html>"));
 end setState_dTX;
 
 redeclare function extends setState_phX
@@ -618,9 +622,9 @@ algorithm
   smoothOrder=2,
   Inline=true,
   Documentation(info="<html>
- The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">
- thermodynamic state record</a> is computed from pressure p, specific enthalpy h and composition X.
- </html>"));
+The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">
+thermodynamic state record</a> is computed from pressure p, specific enthalpy h and composition X.
+</html>"));
 end setState_phX;
 
 redeclare function extends setState_pTX
@@ -634,9 +638,9 @@ algorithm
   smoothOrder=2,
   Inline=true,
   Documentation(info="<html>
- The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">
- thermodynamic state record</a> is computed from pressure p, temperature T and composition X.
- </html>"));
+The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">
+thermodynamic state record</a> is computed from pressure p, temperature T and composition X.
+</html>"));
 end setState_pTX;
 
 redeclare function extends setState_psX
@@ -674,24 +678,24 @@ algorithm
 annotation (
 Inline=true,
 Documentation(info="<html>
- <p>
- This function returns the thermodynamic state based on pressure,
- specific entropy and mass fraction.
- </p>
- <p>
- The state is computed by symbolically solving
- <a href=\"modelica://AixLib.Media.Air.specificEntropy\">
- AixLib.Media.Air.specificEntropy</a>
- for temperature.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 27, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+This function returns the thermodynamic state based on pressure,
+specific entropy and mass fraction.
+</p>
+<p>
+The state is computed by symbolically solving
+<a href=\"modelica://AixLib.Media.Air.specificEntropy\">
+AixLib.Media.Air.specificEntropy</a>
+for temperature.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 27, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end setState_psX;
 
 redeclare replaceable function extends specificEnthalpy
@@ -717,20 +721,20 @@ algorithm
              Inline=true,
              inverse(T=temperature_phX(p, h, X)),
              Documentation(info="<html>
- Specific enthalpy as a function of temperature and species concentration.
- The pressure is input for compatibility with the medium models, but the specific enthalpy
- is independent of the pressure.
- </html>",
+Specific enthalpy as a function of temperature and species concentration.
+The pressure is input for compatibility with the medium models, but the specific enthalpy
+is independent of the pressure.
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 30, 2015, by Filip Jorissen and Michael Wetter:<br/>
- Added <code>Inline=true</code> for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
- issue 227</a>.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+April 30, 2015, by Filip Jorissen and Michael Wetter:<br/>
+Added <code>Inline=true</code> for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
+issue 227</a>.
+</li>
+</ul>
+</html>"));
 end specificEnthalpy_pTX;
 
 redeclare replaceable function extends specificGibbsEnergy
@@ -758,21 +762,21 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function computes the specific enthalpy for
- an isentropic state change from the temperature
- that corresponds to the state <code>refState</code>
- to <code>reference_T</code>.
- </p>
- </html>",
+<p>
+This function computes the specific enthalpy for
+an isentropic state change from the temperature
+that corresponds to the state <code>refState</code>
+to <code>reference_T</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end isentropicEnthalpy;
 
 redeclare function extends specificInternalEnergy "Specific internal energy"
@@ -791,8 +795,8 @@ algorithm
   smoothOrder=2,
   Inline=true,
   Documentation(info="<html>
- Temperature is returned from the thermodynamic state record input as a simple assignment.
- </html>"));
+Temperature is returned from the thermodynamic state record input as a simple assignment.
+</html>"));
 end temperature;
 
 redeclare function extends molarMass "Return the molar mass"
@@ -802,18 +806,18 @@ algorithm
 Inline=true,
 smoothOrder=99,
 Documentation(info="<html>
- <p>
- This function returns the molar mass.
- </p>
- </html>",
+<p>
+This function returns the molar mass.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end molarMass;
 
 redeclare replaceable function temperature_phX
@@ -830,20 +834,20 @@ algorithm
              Inline=true,
              inverse(h=specificEnthalpy_pTX(p, T, X)),
              Documentation(info="<html>
- Temperature as a function of specific enthalpy and species concentration.
- The pressure is input for compatibility with the medium models, but the temperature
- is independent of the pressure.
- </html>",
+Temperature as a function of specific enthalpy and species concentration.
+The pressure is input for compatibility with the medium models, but the temperature
+is independent of the pressure.
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 30, 2015, by Filip Jorissen and Michael Wetter:<br/>
- Added <code>Inline=true</code> for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
- issue 227</a>.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+April 30, 2015, by Filip Jorissen and Michael Wetter:<br/>
+Added <code>Inline=true</code> for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
+issue 227</a>.
+</li>
+</ul>
+</html>"));
 end temperature_phX;
 
 redeclare function extends thermalConductivity
@@ -875,24 +879,23 @@ protected
     annotation (
       preferredView="info",
       Documentation(info="<html>
- <p>
- This data record contains the coefficients for perfect gases.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 12, 2014, by Michael Wetter:<br/>
- Corrected the wrong location of the <code>preferredView</code>
- and the <code>revisions</code> annotation.
- </li>
- <li>
- November 21, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+This data record contains the coefficients for perfect gases.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 12, 2014, by Michael Wetter:<br/>
+Corrected the wrong location of the <code>preferredView</code>
+and the <code>revisions</code> annotation.
+</li>
+<li>
+November 21, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end GasProperties;
-
   constant Modelica.Units.SI.SpecificEnergy h_fg=AixLib.Utilities.Psychrometrics.Constants.h_fg
     "Latent heat of evaporation of water";
   constant Modelica.Units.SI.SpecificHeatCapacity cpWatLiq=AixLib.Utilities.Psychrometrics.Constants.cpWatLiq
@@ -986,222 +989,234 @@ algorithm
     Inline=true);
 end der_specificHeatCapacityCv;
   annotation(Documentation(info="<html>
- <p>
- This medium package models moist air using a gas law in which pressure and temperature
- are independent, which often leads to significantly faster and more robust computations.
- The specific heat capacities at constant pressure and at constant volume are constant.
- The air is assumed to be not saturated.
- </p>
- <p>
- This medium uses the gas law
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &rho;/&rho;<sub>stp</sub> = p/p<sub>stp</sub>,
- </p>
- <p>
- where
- <i>p<sub>std</sub></i> and <i>&rho;<sub>stp</sub></i> are constant reference
- temperature and density, rathern than the ideal gas law
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &rho; = p &frasl;(R T),
- </p>
- <p>
- where <i>R</i> is the gas constant and <i>T</i> is the temperature.
- </p>
- <p>
- This formulation often leads to smaller systems of nonlinear equations
- because equations for pressure and temperature are decoupled.
- Therefore, if air inside a control volume such as room air is heated, it
- does not increase its specific volume. Consequently, merely heating or cooling
- a control volume does not affect the air flow calculations in a duct network
- that may be connected to that volume.
- Note that multizone air exchange simulation in which buoyancy drives the
- air flow is still possible as the models in
- <a href=\"modelica://AixLib.Airflow.Multizone\">
- AixLib.Airflow.Multizone</a> compute the mass density using the function
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.density_pTX\">
- AixLib.Utilities.Psychrometrics.Functions.density_pTX</a> in which density
- is a function of temperature.
- </p>
- <p>
- Note that models in this package implement the equation for the internal energy as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   u = h - p<sub>stp</sub> &frasl; &rho;<sub>stp</sub>,
- </p>
- <p>
- where
- <i>u</i> is the internal energy per unit mass,
- <i>h</i> is the enthalpy per unit mass,
- <i>p<sub>stp</sub></i> is the static pressure and
- <i>&rho;<sub>stp</sub></i> is the mass density at standard pressure and temperature.
- The reason for this implementation is that in general,
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   h = u + p v,
- </p>
- <p>
- from which follows that
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   u = h - p v = h - p &frasl; &rho; = h - p<sub>stp</sub> &frasl; &rho;<sub>std</sub>,
- </p>
- <p>
- because <i>p &frasl; &rho; = p<sub>stp</sub> &frasl; &rho;<sub>stp</sub></i> in this medium model.
- </p>
- <p>
- The enthalpy is computed using the convention that <i>h=0</i>
- if <i>T=0</i> &deg;C and no water vapor is present.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 28, 2020, by Michael Wetter:<br/>
- Reformulated <code>BaseProperties</code> to avoid event-triggering assertions.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1401\">#1401</a>.
- </li>
- <li>
- January 11, 2019 by Michael Wetter:<br/>
- Reforulated assignment of <code>X_int</code> in <code>setState_psX</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1079\">#1079</a>.
- </li>
- <li>
- October 26, 2018, by Filip Jorissen and Michael Wetter:<br/>
- Now printing different messages if temperature is above or below its limit,
- and adding instance name as JModelica does not print the full instance name in the assertion.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1045\">#1045</a>.
- </li>
- <li>
- November 4, 2016, by Michael Wetter:<br/>
- Set default value for <code>dT.start</code> in base properties.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/575\">#575</a>.
- </li>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Set <code>AbsolutePressure(start=p_default)</code> to avoid
- a translation error if
- <a href=\"modelica://AixLib.Fluid.Sources.Examples.TraceSubstancesFlowSource\">
- AixLib.Fluid.Sources.Examples.TraceSubstancesFlowSource</a>
- is translated in pedantic mode in Dymola 2016.
- The reason is that pressures use <code>Medium.p_default</code> as start values,
- but
- <a href=\"modelica://Modelica.Media.Interfaces.Types\">
- Modelica.Media.Interfaces.Types</a>
- sets a default value of <i>1E-5</i>.
- A similar change has been done for pressure.
- This fixes
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- June 5, 2015, by Michael Wetter:<br/>
- Added <code>stateSelect</code> attribute in <code>BaseProperties.T</code>
- to allow correct use of <code>preferredMediumState</code> as
- described in
- <a href=\"modelica://Modelica.Media.Interfaces.PartialMedium\">
- Modelica.Media.Interfaces.PartialMedium</a>.
- Note that the default is <code>preferredMediumState=false</code>
- and hence the same states are used as were used before.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/260\">#260</a>.
- </li>
- <li>
- May 11, 2015, by Michael Wetter:<br/>
- Removed
- <code>p(stateSelect=if preferredMediumStates then StateSelect.prefer else StateSelect.default)</code>
- in declaration of <code>BaseProperties</code>.
- Otherwise, when models that contain a fluid volume
- are exported as an FMU, their pressure would be
- differentiated with respect to time. This would require
- the time derivative of the inlet pressure, which is not available,
- causing the translation to stop with an error.
- </li>
- <li>
- May 1, 2015, by Michael Wetter:<br/>
- Added <code>Inline=true</code> for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
- issue 227</a>.
- </li>
- <li>
- March 20, 2015, by Michael Wetter:<br/>
- Added missing term <code>state.p/reference_p</code> in function
- <code>specificEntropy</code>.
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/193\">#193</a>.
- </li>
- <li>
- February 3, 2015, by Michael Wetter:<br/>
- Removed <code>stateSelect.prefer</code> for temperature.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/160\">#160</a>.
- </li>
- <li>
- July 24, 2014, by Michael Wetter:<br/>
- Changed implementation to use
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Constants\">
- AixLib.Utilities.Psychrometrics.Constants</a>.
- This was done to use consistent values throughout the library.
- </li>
- <li>
- November 16, 2013, by Michael Wetter:<br/>
- Revised and simplified the implementation.
- </li>
- <li>
- November 14, 2013, by Michael Wetter:<br/>
- Removed function
- <code>HeatCapacityOfWater</code>
- which is neither needed nor implemented in the
- Modelica Standard Library.
- </li>
- <li>
- November 13, 2013, by Michael Wetter:<br/>
- Removed non-used computations in <code>specificEnthalpy_pTX</code> and
- in <code>temperature_phX</code>.
- </li>
- <li>
- March 29, 2013, by Michael Wetter:<br/>
- Added <code>final standardOrderComponents=true</code> in the
- <code>BaseProperties</code> declaration. This avoids an error
- when models are checked in Dymola 2014 in the pedenatic mode.
- </li>
- <li>
- April 12, 2012, by Michael Wetter:<br/>
- Added keyword <code>each</code> to <code>Xi(stateSelect=...)</code>.
- </li>
- <li>
- April 4, 2012, by Michael Wetter:<br/>
- Added redeclaration of <code>ThermodynamicState</code> to avoid a warning
- during model check and translation.
- </li>
- <li>
- August 3, 2011, by Michael Wetter:<br/>
- Fixed bug in <code>u=h-R*T</code>, which is only valid for ideal gases.
- For this medium, the function is <code>u=h-pStd/dStp</code>.
- </li>
- <li>
- January 27, 2010, by Michael Wetter:<br/>
- Fixed bug in <code>else</code> branch of function <code>setState_phX</code>
- that lead to a run-time error when the constructor of this function was called.
- </li>
- <li>
- January 22, 2010, by Michael Wetter:<br/>
- Added implementation of function
- <a href=\"modelica://AixLib.Media.GasesPTDecoupled.MoistAirUnsaturated.enthalpyOfNonCondensingGas\">
- enthalpyOfNonCondensingGas</a> and its derivative.
- </li>
- <li>
- January 13, 2010, by Michael Wetter:<br/>
- Fixed implementation of derivative functions.
- </li>
- <li>
- August 28, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This medium package models moist air using a gas law in which pressure and temperature
+are independent, which often leads to significantly faster and more robust computations.
+The specific heat capacities at constant pressure and at constant volume are constant.
+The air is assumed to be not saturated.
+</p>
+<p>
+This medium uses the gas law
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&rho;/&rho;<sub>stp</sub> = p/p<sub>stp</sub>,
+</p>
+<p>
+where
+<i>p<sub>std</sub></i> and <i>&rho;<sub>stp</sub></i> are constant reference
+temperature and density, rathern than the ideal gas law
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&rho; = p &frasl;(R T),
+</p>
+<p>
+where <i>R</i> is the gas constant and <i>T</i> is the temperature.
+</p>
+<p>
+This formulation often leads to smaller systems of nonlinear equations
+because equations for pressure and temperature are decoupled.
+Therefore, if air inside a control volume such as room air is heated, it
+does not increase its specific volume. Consequently, merely heating or cooling
+a control volume does not affect the air flow calculations in a duct network
+that may be connected to that volume.
+Note that multizone air exchange simulation in which buoyancy drives the
+air flow is still possible as the models in
+<a href=\"modelica://AixLib.Airflow.Multizone\">
+AixLib.Airflow.Multizone</a> compute the mass density using the function
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.density_pTX\">
+AixLib.Utilities.Psychrometrics.Functions.density_pTX</a> in which density
+is a function of temperature.
+</p>
+<p>
+Note that models in this package implement the equation for the internal energy as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  u = h - p<sub>stp</sub> &frasl; &rho;<sub>stp</sub>,
+</p>
+<p>
+where
+<i>u</i> is the internal energy per unit mass,
+<i>h</i> is the enthalpy per unit mass,
+<i>p<sub>stp</sub></i> is the static pressure and
+<i>&rho;<sub>stp</sub></i> is the mass density at standard pressure and temperature.
+The reason for this implementation is that in general,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  h = u + p v,
+</p>
+<p>
+from which follows that
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  u = h - p v = h - p &frasl; &rho; = h - p<sub>stp</sub> &frasl; &rho;<sub>std</sub>,
+</p>
+<p>
+because <i>p &frasl; &rho; = p<sub>stp</sub> &frasl; &rho;<sub>stp</sub></i> in this medium model.
+</p>
+<p>
+The enthalpy is computed using the convention that <i>h=0</i>
+if <i>T=0</i> &deg;C and no water vapor is present.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+September 9, 2022, by Michael Wetter:<br/>
+Set nominal attribute for <code>BaseProperties.Xi</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1634\">#1634</a>.
+</li>
+<li>
+September 28, 2020, by Michael Wetter:<br/>
+Reformulated <code>BaseProperties</code> to avoid event-triggering assertions.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1401\">#1401</a>.
+</li>
+<li>
+January 11, 2019 by Michael Wetter:<br/>
+Reforulated assignment of <code>X_int</code> in <code>setState_psX</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1079\">#1079</a>.
+</li>
+<li>
+October 26, 2018, by Filip Jorissen and Michael Wetter:<br/>
+Now printing different messages if temperature is above or below its limit,
+and adding instance name as JModelica does not print the full instance name in the assertion.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1045\">#1045</a>.
+</li>
+<li>
+November 4, 2016, by Michael Wetter:<br/>
+Set default value for <code>dT.start</code> in base properties.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/575\">#575</a>.
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Set <code>AbsolutePressure(start=p_default)</code> to avoid
+a translation error if
+<a href=\"modelica://AixLib.Fluid.Sources.Examples.TraceSubstancesFlowSource\">
+AixLib.Fluid.Sources.Examples.TraceSubstancesFlowSource</a>
+is translated in pedantic mode in Dymola 2016.
+The reason is that pressures use <code>Medium.p_default</code> as start values,
+but
+<a href=\"modelica://Modelica.Media.Interfaces.Types\">
+Modelica.Media.Interfaces.Types</a>
+sets a default value of <i>1E-5</i>.
+A similar change has been done for pressure.
+This fixes
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+June 5, 2015, by Michael Wetter:<br/>
+Added <code>stateSelect</code> attribute in <code>BaseProperties.T</code>
+to allow correct use of <code>preferredMediumState</code> as
+described in
+<a href=\"modelica://Modelica.Media.Interfaces.PartialMedium\">
+Modelica.Media.Interfaces.PartialMedium</a>.
+Note that the default is <code>preferredMediumState=false</code>
+and hence the same states are used as were used before.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/260\">#260</a>.
+</li>
+<li>
+May 11, 2015, by Michael Wetter:<br/>
+Removed
+<code>p(stateSelect=if preferredMediumStates then StateSelect.prefer else StateSelect.default)</code>
+in declaration of <code>BaseProperties</code>.
+Otherwise, when models that contain a fluid volume
+are exported as an FMU, their pressure would be
+differentiated with respect to time. This would require
+the time derivative of the inlet pressure, which is not available,
+causing the translation to stop with an error.
+</li>
+<li>
+May 1, 2015, by Michael Wetter:<br/>
+Added <code>Inline=true</code> for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
+issue 227</a>.
+</li>
+<li>
+March 20, 2015, by Michael Wetter:<br/>
+Added missing term <code>state.p/reference_p</code> in function
+<code>specificEntropy</code>.
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/193\">#193</a>.
+</li>
+<li>
+February 3, 2015, by Michael Wetter:<br/>
+Removed <code>stateSelect.prefer</code> for temperature.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/160\">#160</a>.
+</li>
+<li>
+July 24, 2014, by Michael Wetter:<br/>
+Changed implementation to use
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Constants\">
+AixLib.Utilities.Psychrometrics.Constants</a>.
+This was done to use consistent values throughout the library.
+</li>
+<li>
+November 16, 2013, by Michael Wetter:<br/>
+Revised and simplified the implementation.
+</li>
+<li>
+November 14, 2013, by Michael Wetter:<br/>
+Removed function
+<code>HeatCapacityOfWater</code>
+which is neither needed nor implemented in the
+Modelica Standard Library.
+</li>
+<li>
+November 13, 2013, by Michael Wetter:<br/>
+Removed non-used computations in <code>specificEnthalpy_pTX</code> and
+in <code>temperature_phX</code>.
+</li>
+<li>
+March 29, 2013, by Michael Wetter:<br/>
+Added <code>final standardOrderComponents=true</code> in the
+<code>BaseProperties</code> declaration. This avoids an error
+when models are checked in Dymola 2014 in the pedenatic mode.
+</li>
+<li>
+April 12, 2012, by Michael Wetter:<br/>
+Added keyword <code>each</code> to <code>Xi(stateSelect=...)</code>.
+</li>
+<li>
+April 4, 2012, by Michael Wetter:<br/>
+Added redeclaration of <code>ThermodynamicState</code> to avoid a warning
+during model check and translation.
+</li>
+<li>
+August 3, 2011, by Michael Wetter:<br/>
+Fixed bug in <code>u=h-R*T</code>, which is only valid for ideal gases.
+For this medium, the function is <code>u=h-pStd/dStp</code>.
+</li>
+<li>
+January 27, 2010, by Michael Wetter:<br/>
+Fixed bug in <code>else</code> branch of function <code>setState_phX</code>
+that lead to a run-time error when the constructor of this function was called.
+</li>
+<li>
+January 22, 2010, by Michael Wetter:<br/>
+Added implementation of function
+<a href=\"modelica://AixLib.Media.GasesPTDecoupled.MoistAirUnsaturated.enthalpyOfNonCondensingGas\">
+enthalpyOfNonCondensingGas</a> and its derivative.
+</li>
+<li>
+January 13, 2010, by Michael Wetter:<br/>
+Fixed implementation of derivative functions.
+</li>
+<li>
+August 28, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Ellipse(
           extent={{-78,78},{-34,34}},
@@ -1237,6 +1252,6 @@ end der_specificHeatCapacityCv;
           extent={{-90,-6},{-46,-50}},
           lineColor={0,0,0},
           fillPattern=FillPattern.Sphere,
-          fillColor={120,120,120})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={120,120,120})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Air;
diff --git a/AixLib/Media/Antifreeze/BaseClasses/PropertyCoefficients.mo b/AixLib/Media/Antifreeze/BaseClasses/PropertyCoefficients.mo
index 1967d1fb9c..363091909f 100644
--- a/AixLib/Media/Antifreeze/BaseClasses/PropertyCoefficients.mo
+++ b/AixLib/Media/Antifreeze/BaseClasses/PropertyCoefficients.mo
@@ -17,25 +17,25 @@ record PropertyCoefficients
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(info="<html>
- <p>
- Record that is used by media packages in 
- <a href=\"modelica://AixLib.Media.Antifreeze\">
- AixLib.Media.Antifreeze</a> to implement the thermophysical properties
- based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 11, 2018, by Michael Wetter:
- Added documentation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Record that is used by media packages in 
+<a href=\"modelica://AixLib.Media.Antifreeze\">
+AixLib.Media.Antifreeze</a> to implement the thermophysical properties
+based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 11, 2018, by Michael Wetter:
+Added documentation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropertyCoefficients;
diff --git a/AixLib/Media/Antifreeze/EthyleneGlycolWater.mo b/AixLib/Media/Antifreeze/EthyleneGlycolWater.mo
index dd3da5b6d5..ba0293571f 100644
--- a/AixLib/Media/Antifreeze/EthyleneGlycolWater.mo
+++ b/AixLib/Media/Antifreeze/EthyleneGlycolWater.mo
@@ -69,20 +69,20 @@ package EthyleneGlycolWater
 
   equation
   assert(T >= T_min, "
- In "  + getInstanceName() + ": Temperature T exceeded its minimum allowed value of " + String(T_min-273.15)
+In "   + getInstanceName() + ": Temperature T exceeded its minimum allowed value of " + String(T_min-273.15)
     + " degC (" + String(T_min) + " Kelvin)
- as required from medium model \""+ mediumName + "\".");
+as required from medium model \"" + mediumName + "\".");
   assert(T <= T_max, "
- In "  + getInstanceName() + ": Temperature T exceeded its maximum allowed value of " + String(T_max-273.15)
+In "   + getInstanceName() + ": Temperature T exceeded its maximum allowed value of " + String(T_max-273.15)
     + " degC (" + String(T_max) + " Kelvin)
- as required from medium model \""+ mediumName + "\".");
+as required from medium model \"" + mediumName + "\".");
 
   assert(X_a >= X_a_min, "
- In "  + getInstanceName() + ": Mass fraction x_a exceeded its minimum allowed value of " + String(X_a_min) + "
- as required from medium model \""+ mediumName + "\".");
+In "   + getInstanceName() + ": Mass fraction x_a exceeded its minimum allowed value of " + String(X_a_min) + "
+as required from medium model \"" + mediumName + "\".");
   assert(X_a <= X_a_max, "
- In "  + getInstanceName() + ": Mass fraction x_a exceeded its maximum allowed value of " + String(X_a_max) + "
- as required from medium model \""+ mediumName + "\".");
+In "   + getInstanceName() + ": Mass fraction x_a exceeded its maximum allowed value of " + String(X_a_max) + "
+as required from medium model \"" + mediumName + "\".");
 
     h = cp_const*(T-reference_T);
     u = h;
@@ -90,18 +90,18 @@ package EthyleneGlycolWater
     state.p = p;
 
     annotation(Documentation(info="<html>
-     <p>
-     This base properties model is identical to
-     <a href=\"modelica://Modelica.Media.Water.ConstantPropertyLiquidWater\">
-     Modelica.Media.Water.ConstantPropertyLiquidWater</a>,
-     except that the equation
-     <code>u = cv_const*(T - reference_T)</code>
-     has been replaced by <code>u=h</code> because
-     <code>cp_const=cv_const</code>.
-     Also, the model checks if the mass fraction of the mixture is within the
-     allowed limits.
-     </p>
- </html>"));
+    <p>
+    This base properties model is identical to
+    <a href=\"modelica://Modelica.Media.Water.ConstantPropertyLiquidWater\">
+    Modelica.Media.Water.ConstantPropertyLiquidWater</a>,
+    except that the equation
+    <code>u = cv_const*(T - reference_T)</code>
+    has been replaced by <code>u=h</code> because
+    <code>cp_const=cv_const</code>.
+    Also, the model checks if the mass fraction of the mixture is within the
+    allowed limits.
+    </p>
+</html>"));
   end BaseProperties;
 protected
   constant Modelica.Units.SI.MassFraction X_a_min=0.
@@ -156,28 +156,28 @@ protected
         proCoe.a_d)
     annotation (
     Documentation(info="<html>
-   <p>
-   Density of propylene antifreeze-water mixture at specified mass fraction
-   and temperature, based on Melinder (2010).
-   </p>
-   <h4>References</h4>
-   <p>
-   Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
-   Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
-   IIR/IIF.
-   </p>
-   </html>",
+  <p>
+  Density of propylene antifreeze-water mixture at specified mass fraction
+  and temperature, based on Melinder (2010).
+  </p>
+  <h4>References</h4>
+  <p>
+  Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+  Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+  IIR/IIF.
+  </p>
+  </html>",
   revisions="<html>
-   <ul>
-   <li>
-   May 2, 2018 by Massimo Cimmino:<br/>
-   First implementation.
-   This function is used by
-   <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
-   AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
-   </li>
-   </ul>
-   </html>"));
+  <ul>
+  <li>
+  May 2, 2018 by Massimo Cimmino:<br/>
+  First implementation.
+  This function is used by
+  <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
+  AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
+  </li>
+  </ul>
+  </html>"));
 
   end density_TX_a;
 
@@ -197,27 +197,27 @@ protected
 
   annotation (
   Documentation(info="<html>
- <p>
- Dynamic viscosity of antifreeze-water mixture at specified mass fraction and
- temperature, based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- May 2, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Dynamic viscosity of antifreeze-water mixture at specified mass fraction and
+temperature, based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+May 2, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
+</li>
+</ul>
+</html>"));
   end dynamicViscosity_TX_a;
 
   replaceable function fusionTemperature_TX_a
@@ -236,27 +236,27 @@ protected
 
   annotation (
   Documentation(info="<html>
- <p>
- Fusion temperature of antifreeze-water mixture at specified mass fraction and
- temperature, based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- May 2, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Fusion temperature of antifreeze-water mixture at specified mass fraction and
+temperature, based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+May 2, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
+</li>
+</ul>
+</html>"));
   end fusionTemperature_TX_a;
 
   replaceable function polynomialProperty
@@ -287,41 +287,41 @@ protected
     end for;
   annotation (
   Documentation(info="<html>
- <p>
- Evaluates a thermophysical property of a mixture, based on correlations proposed
- by Melinder (2010).
- </p>
- <p>
- The polynomial has the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- f = a<sub>1</sub> (x-xm)<sup>0</sup>(y-ym)<sup>0</sup>
- + a<sub>2</sub> (x-xm)<sup>0</sup>(y-ym)<sup>1</sup>
- + ... +
- a<sub>ny[1]</sub> (x-xm)<sup>0</sup>(y-ym)<sup>ny[1]-1</sup>
- + ... +
- a<sub>ny[1])+1</sub> (x-xm)<sup>1</sup>(y-ym)<sup>0</sup>
- + ... +
- a<sub>ny[1]+ny[2]</sub> (x-xm)<sup>1</sup>(y-ym)<sup>ny[2]-1</sup>
- + ...
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 16, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used models in
- <a href=\"modelica://AixLib.Media.Antifreeze\">
- AixLib.Media.Antifreeze</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Evaluates a thermophysical property of a mixture, based on correlations proposed
+by Melinder (2010).
+</p>
+<p>
+The polynomial has the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+f = a<sub>1</sub> (x-xm)<sup>0</sup>(y-ym)<sup>0</sup>
++ a<sub>2</sub> (x-xm)<sup>0</sup>(y-ym)<sup>1</sup>
++ ... +
+a<sub>ny[1]</sub> (x-xm)<sup>0</sup>(y-ym)<sup>ny[1]-1</sup>
++ ... +
+a<sub>ny[1])+1</sub> (x-xm)<sup>1</sup>(y-ym)<sup>0</sup>
++ ... +
+a<sub>ny[1]+ny[2]</sub> (x-xm)<sup>1</sup>(y-ym)<sup>ny[2]-1</sup>
++ ...
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 16, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used models in
+<a href=\"modelica://AixLib.Media.Antifreeze\">
+AixLib.Media.Antifreeze</a>.
+</li>
+</ul>
+</html>"));
   end polynomialProperty;
 
   replaceable function specificHeatCapacityCp_TX_a
@@ -340,27 +340,27 @@ protected
 
   annotation (
   Documentation(info="<html>
- <p>
- Specific heat capacity of antifreeze-water mixture at specified mass fraction
- and temperature, based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 16, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Specific heat capacity of antifreeze-water mixture at specified mass fraction
+and temperature, based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 16, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
+</li>
+</ul>
+</html>"));
   end specificHeatCapacityCp_TX_a;
 
   replaceable function thermalConductivity_TX_a
@@ -379,96 +379,96 @@ protected
 
   annotation (
   Documentation(info="<html>
- <p>
- Thermal conductivity of antifreeze-water mixture at specified mass fraction and
- temperature, based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 16, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Thermal conductivity of antifreeze-water mixture at specified mass fraction and
+temperature, based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 16, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater</a>.
+</li>
+</ul>
+</html>"));
   end thermalConductivity_TX_a;
 annotation(preferredView="info", Documentation(info="<html>
- <p>
- This medium package models ethylene glycol - water mixtures.
- </p>
- <p>
- The mass density, specific heat capacity, thermal conductivity and viscosity
- are assumed constant and evaluated at a set temperature and mass fraction of
- ethylene glycol within the mixture. The dependence of the four properties
- are shown on the figure below.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/EthyleneGlycolWaterProperties.png\" border=\"1\"
- alt=\"Relative variation of specific heat capacity with temperature\"/>
- </p>
- <p>
- The accuracy of the thermophysical properties is dependent on the temperature
- variations encountered during simulations.
- The figure below shows the relative error of the the four properties over a
- <i>10</i> &deg;C range around the temperature used to evaluate the constant
- properties. The maximum errors are <i>0.8</i> % for mass density, <i>2.7</i> %
- for specific heat capacity, <i>3.2</i> % for thermal conductivity and <i>160</i>
- % for dynamic viscosity.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/EthyleneGlycolWaterError10degC.png\" border=\"1\"
- alt=\"Relative variation of specific heat capacity with temperature\"/>
- </p>
- <p>
- The figure below shows the relative error of the the four properties over a
- <i>20</i> &deg;C range around the temperature used to evaluate the constant
- proepties. The maximum errors are <i>1.5</i> % for mass density, <i>5.3</i> %
- for specific heat capacity, <i>5.9</i> % for thermal conductivity and <i>500</i>
- % for dynamic viscosity.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/EthyleneGlycolWaterError20degC.png\" border=\"1\"
- alt=\"Relative variation of specific heat capacity with temperature\"/>
- </p>
- <p>
- The enthalpy is computed using the convention that <i>h=0</i>
- if <i>T=0</i> &deg;C.
- </p>
- <h4>Limitations</h4>
- <p>
- Density, specific heat capacity, thermal conductivity and viscosity are constant.
- The ethylene glycol/water mixture is modeled as an incompressible liquid.
- There are no phase changes. The medium is limited to temperatures below
- <i>100</i> &deg;C and mass fractions below <i>0.60</i>.
- As is the case for <a href=\"modelica://AixLib.Media.Water\">AixLib.Media.Water</a>,
- this medium package should not be used if
- the simulation relies on the dynamic viscosity.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The temperature and mass fraction must be specified for the evaluation of the
- constant thermophysical properties. A typical use of the package is (e.g. for
- a temperature of <i>20</i> &deg;C and a mass fraction of <i>0.40</i>):
- </p>
- <p>
- <code>Medium = AixLib.Media.Antifreeze.EthyleneGlycolWater(property_T=293.15, X_a=0.40)</code>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 05, 2020, by Wen HU:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This medium package models ethylene glycol - water mixtures.
+</p>
+<p>
+The mass density, specific heat capacity, thermal conductivity and viscosity
+are assumed constant and evaluated at a set temperature and mass fraction of
+ethylene glycol within the mixture. The dependence of the four properties
+are shown on the figure below.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/EthyleneGlycolWaterProperties.png\" border=\"1\"
+alt=\"Relative variation of specific heat capacity with temperature\"/>
+</p>
+<p>
+The accuracy of the thermophysical properties is dependent on the temperature
+variations encountered during simulations.
+The figure below shows the relative error of the the four properties over a
+<i>10</i> &deg;C range around the temperature used to evaluate the constant
+properties. The maximum errors are <i>0.8</i> % for mass density, <i>2.7</i> %
+for specific heat capacity, <i>3.2</i> % for thermal conductivity and <i>160</i>
+% for dynamic viscosity.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/EthyleneGlycolWaterError10degC.png\" border=\"1\"
+alt=\"Relative variation of specific heat capacity with temperature\"/>
+</p>
+<p>
+The figure below shows the relative error of the the four properties over a
+<i>20</i> &deg;C range around the temperature used to evaluate the constant
+proepties. The maximum errors are <i>1.5</i> % for mass density, <i>5.3</i> %
+for specific heat capacity, <i>5.9</i> % for thermal conductivity and <i>500</i>
+% for dynamic viscosity.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/EthyleneGlycolWaterError20degC.png\" border=\"1\"
+alt=\"Relative variation of specific heat capacity with temperature\"/>
+</p>
+<p>
+The enthalpy is computed using the convention that <i>h=0</i>
+if <i>T=0</i> &deg;C.
+</p>
+<h4>Limitations</h4>
+<p>
+Density, specific heat capacity, thermal conductivity and viscosity are constant.
+The ethylene glycol/water mixture is modeled as an incompressible liquid.
+There are no phase changes. The medium is limited to temperatures below
+<i>100</i> &deg;C and mass fractions below <i>0.60</i>.
+As is the case for <a href=\"modelica://AixLib.Media.Water\">AixLib.Media.Water</a>,
+this medium package should not be used if
+the simulation relies on the dynamic viscosity.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The temperature and mass fraction must be specified for the evaluation of the
+constant thermophysical properties. A typical use of the package is (e.g. for
+a temperature of <i>20</i> &deg;C and a mass fraction of <i>0.40</i>):
+</p>
+<p>
+<code>Medium = AixLib.Media.Antifreeze.EthyleneGlycolWater(property_T=293.15, X_a=0.40)</code>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 05, 2020, by Wen HU:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EthyleneGlycolWater;
diff --git a/AixLib/Media/Antifreeze/PropyleneGlycolWater.mo b/AixLib/Media/Antifreeze/PropyleneGlycolWater.mo
index 3eb87344e9..3fd21ee112 100644
--- a/AixLib/Media/Antifreeze/PropyleneGlycolWater.mo
+++ b/AixLib/Media/Antifreeze/PropyleneGlycolWater.mo
@@ -69,20 +69,20 @@ package PropyleneGlycolWater
 
   equation
   assert(T >= T_min, "
- In "  + getInstanceName() + ": Temperature T exceeded its minimum allowed value of " + String(T_min-273.15)
+In "   + getInstanceName() + ": Temperature T exceeded its minimum allowed value of " + String(T_min-273.15)
     + " degC (" + String(T_min) + " Kelvin)
- as required from medium model \""+ mediumName + "\".");
+as required from medium model \"" + mediumName + "\".");
   assert(T <= T_max, "
- In "  + getInstanceName() + ": Temperature T exceeded its maximum allowed value of " + String(T_max-273.15)
+In "   + getInstanceName() + ": Temperature T exceeded its maximum allowed value of " + String(T_max-273.15)
     + " degC (" + String(T_max) + " Kelvin)
- as required from medium model \""+ mediumName + "\".");
+as required from medium model \"" + mediumName + "\".");
 
   assert(X_a >= X_a_min, "
- In "  + getInstanceName() + ": Mass fraction x_a exceeded its minimum allowed value of " + String(X_a_min) + "
- as required from medium model \""+ mediumName + "\".");
+In "   + getInstanceName() + ": Mass fraction x_a exceeded its minimum allowed value of " + String(X_a_min) + "
+as required from medium model \"" + mediumName + "\".");
   assert(X_a <= X_a_max, "
- In "  + getInstanceName() + ": Mass fraction x_a exceeded its maximum allowed value of " + String(X_a_max) + "
- as required from medium model \""+ mediumName + "\".");
+In "   + getInstanceName() + ": Mass fraction x_a exceeded its maximum allowed value of " + String(X_a_max) + "
+as required from medium model \"" + mediumName + "\".");
 
     h = cp_const*(T-reference_T);
     u = h;
@@ -90,18 +90,18 @@ package PropyleneGlycolWater
     state.p = p;
 
     annotation(Documentation(info="<html>
-     <p>
-     This base properties model is identical to
-     <a href=\"modelica://Modelica.Media.Water.ConstantPropertyLiquidWater\">
-     Modelica.Media.Water.ConstantPropertyLiquidWater</a>,
-     except that the equation
-     <code>u = cv_const*(T - reference_T)</code>
-     has been replaced by <code>u=h</code> because
-     <code>cp_const=cv_const</code>.
-     Also, the model checks if the mass fraction of the mixture is within the
-     allowed limits.
-     </p>
- </html>"));
+    <p>
+    This base properties model is identical to
+    <a href=\"modelica://Modelica.Media.Water.ConstantPropertyLiquidWater\">
+    Modelica.Media.Water.ConstantPropertyLiquidWater</a>,
+    except that the equation
+    <code>u = cv_const*(T - reference_T)</code>
+    has been replaced by <code>u=h</code> because
+    <code>cp_const=cv_const</code>.
+    Also, the model checks if the mass fraction of the mixture is within the
+    allowed limits.
+    </p>
+</html>"));
   end BaseProperties;
 protected
   constant Modelica.Units.SI.MassFraction X_a_min=0.
@@ -156,28 +156,28 @@ protected
         proCoe.a_d)
     annotation (
     Documentation(info="<html>
-   <p>
-   Density of propylene antifreeze-water mixture at specified mass fraction
-   and temperature, based on Melinder (2010).
-   </p>
-   <h4>References</h4>
-   <p>
-   Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
-   Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
-   IIR/IIF.
-   </p>
-   </html>",
+  <p>
+  Density of propylene antifreeze-water mixture at specified mass fraction
+  and temperature, based on Melinder (2010).
+  </p>
+  <h4>References</h4>
+  <p>
+  Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+  Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+  IIR/IIF.
+  </p>
+  </html>",
   revisions="<html>
-   <ul>
-   <li>
-   May 2, 2018 by Massimo Cimmino:<br/>
-   First implementation.
-   This function is used by
-   <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
-   AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
-   </li>
-   </ul>
-   </html>"));
+  <ul>
+  <li>
+  May 2, 2018 by Massimo Cimmino:<br/>
+  First implementation.
+  This function is used by
+  <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
+  AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
+  </li>
+  </ul>
+  </html>"));
 
   end density_TX_a;
 
@@ -197,27 +197,27 @@ protected
 
   annotation (
   Documentation(info="<html>
- <p>
- Dynamic viscosity of antifreeze-water mixture at specified mass fraction and
- temperature, based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- May 2, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Dynamic viscosity of antifreeze-water mixture at specified mass fraction and
+temperature, based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+May 2, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
+</li>
+</ul>
+</html>"));
   end dynamicViscosity_TX_a;
 
   replaceable function fusionTemperature_TX_a
@@ -236,27 +236,27 @@ protected
 
   annotation (
   Documentation(info="<html>
- <p>
- Fusion temperature of antifreeze-water mixture at specified mass fraction and
- temperature, based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- May 2, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Fusion temperature of antifreeze-water mixture at specified mass fraction and
+temperature, based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+May 2, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
+</li>
+</ul>
+</html>"));
   end fusionTemperature_TX_a;
 
   replaceable function polynomialProperty
@@ -287,41 +287,41 @@ protected
     end for;
   annotation (
   Documentation(info="<html>
- <p>
- Evaluates a thermophysical property of a mixture, based on correlations proposed
- by Melinder (2010).
- </p>
- <p>
- The polynomial has the form
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- f = a<sub>1</sub> (x-xm)<sup>0</sup>(y-ym)<sup>0</sup>
- + a<sub>2</sub> (x-xm)<sup>0</sup>(y-ym)<sup>1</sup>
- + ... +
- a<sub>ny[1]</sub> (x-xm)<sup>0</sup>(y-ym)<sup>ny[1]-1</sup>
- + ... +
- a<sub>ny[1])+1</sub> (x-xm)<sup>1</sup>(y-ym)<sup>0</sup>
- + ... +
- a<sub>ny[1]+ny[2]</sub> (x-xm)<sup>1</sup>(y-ym)<sup>ny[2]-1</sup>
- + ...
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 16, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used models in
- <a href=\"modelica://AixLib.Media.Antifreeze\">
- AixLib.Media.Antifreeze</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Evaluates a thermophysical property of a mixture, based on correlations proposed
+by Melinder (2010).
+</p>
+<p>
+The polynomial has the form
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+f = a<sub>1</sub> (x-xm)<sup>0</sup>(y-ym)<sup>0</sup>
++ a<sub>2</sub> (x-xm)<sup>0</sup>(y-ym)<sup>1</sup>
++ ... +
+a<sub>ny[1]</sub> (x-xm)<sup>0</sup>(y-ym)<sup>ny[1]-1</sup>
++ ... +
+a<sub>ny[1])+1</sub> (x-xm)<sup>1</sup>(y-ym)<sup>0</sup>
++ ... +
+a<sub>ny[1]+ny[2]</sub> (x-xm)<sup>1</sup>(y-ym)<sup>ny[2]-1</sup>
++ ...
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 16, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used models in
+<a href=\"modelica://AixLib.Media.Antifreeze\">
+AixLib.Media.Antifreeze</a>.
+</li>
+</ul>
+</html>"));
   end polynomialProperty;
 
   replaceable function specificHeatCapacityCp_TX_a
@@ -340,27 +340,27 @@ protected
 
   annotation (
   Documentation(info="<html>
- <p>
- Specific heat capacity of antifreeze-water mixture at specified mass fraction
- and temperature, based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 16, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Specific heat capacity of antifreeze-water mixture at specified mass fraction
+and temperature, based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 16, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
+</li>
+</ul>
+</html>"));
   end specificHeatCapacityCp_TX_a;
 
   replaceable function thermalConductivity_TX_a
@@ -379,103 +379,103 @@ protected
 
   annotation (
   Documentation(info="<html>
- <p>
- Thermal conductivity of antifreeze-water mixture at specified mass fraction and
- temperature, based on Melinder (2010).
- </p>
- <h4>References</h4>
- <p>
- Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
- Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
- IIR/IIF.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 16, 2018 by Massimo Cimmino:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Thermal conductivity of antifreeze-water mixture at specified mass fraction and
+temperature, based on Melinder (2010).
+</p>
+<h4>References</h4>
+<p>
+Melinder, &#197;ke. 2010. Properties of Secondary Working Fluids (Secondary
+Refrigerants or Coolants, Heat Transfer Fluids) for Indirect Systems. Paris:
+IIR/IIF.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 16, 2018 by Massimo Cimmino:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater</a>.
+</li>
+</ul>
+</html>"));
   end thermalConductivity_TX_a;
 annotation(preferredView="info", Documentation(info="<html>
- <p>
- This medium package models propylene glycol - water mixtures.
- </p>
- <p>
- The mass density, specific heat capacity, thermal conductivity and viscosity
- are assumed constant and evaluated at a set temperature and mass fraction of
- propylene glycol within the mixture. The dependence of the four properties
- are shown on the figure below.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/PropyleneGlycolWaterProperties.png\" border=\"1\"
- alt=\"Relative variation of specific heat capacity with temperature\"/>
- </p>
- <p>
- The accuracy of the thermophysical properties is dependent on the temperature
- variations encountered during simulations.
- The figure below shows the relative error of the the four properties over a
- <i>10</i> &deg;C range around the temperature used to evaluate the constant
- properties. The maximum errors are <i>0.8</i> % for mass density, <i>1.5</i> %
- for specific heat capacity, <i>3.2</i> % for thermal conductivity and <i>250</i>
- % for dynamic viscosity.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/PropyleneGlycolWaterError10degC.png\" border=\"1\"
- alt=\"Relative variation of specific heat capacity with temperature\"/>
- </p>
- <p>
- The figure below shows the relative error of the the four properties over a
- <i>20</i> &deg;C range around the temperature used to evaluate the constant
- proepties. The maximum errors are <i>1.6</i> % for mass density, <i>3.0</i> %
- for specific heat capacity, <i>6.2</i> % for thermal conductivity and <i>950</i>
- % for dynamic viscosity.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/PropyleneGlycolWaterError20degC.png\" border=\"1\"
- alt=\"Relative variation of specific heat capacity with temperature\"/>
- </p>
- <p>
- The enthalpy is computed using the convention that <i>h=0</i>
- if <i>T=0</i> &deg;C.
- </p>
- <h4>Limitations</h4>
- <p>
- Density, specific heat capacity, thermal conductivity and viscosity are constant.
- The propylene glycol/water mixture is modeled as an incompressible liquid.
- There are no phase changes. The medium is limited to temperatures below
- <i>100</i> &deg;C and mass fractions below <i>0.60</i>.
- As is the case for <a href=\"modelica://AixLib.Media.Water\">AixLib.Media.Water</a>,
- this medium package should not be used if
- the simulation relies on the dynamic viscosity.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The temperature and mass fraction must be specified for the evaluation of the
- constant thermophysical properties. A typical use of the package is (e.g. for
- a temperature of <i>20</i> &deg;C and a mass fraction of <i>0.40</i>):
- </p>
- <p>
- <code>Medium = AixLib.Media.Antifreeze.PropyleneGlycolWater(property_T=293.15, X_a=0.40)</code>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 26, 2018, by Filip Jorissen and Michael Wetter:<br/>
- Now printing different messages if temperature or mass fraction is above or below its limit,
- and adding instance name as JModelica does not print the full instance name in the assertion.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1045\">#1045</a>.
- </li>
- <li>
- March 16, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This medium package models propylene glycol - water mixtures.
+</p>
+<p>
+The mass density, specific heat capacity, thermal conductivity and viscosity
+are assumed constant and evaluated at a set temperature and mass fraction of
+propylene glycol within the mixture. The dependence of the four properties
+are shown on the figure below.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/PropyleneGlycolWaterProperties.png\" border=\"1\"
+alt=\"Relative variation of specific heat capacity with temperature\"/>
+</p>
+<p>
+The accuracy of the thermophysical properties is dependent on the temperature
+variations encountered during simulations.
+The figure below shows the relative error of the the four properties over a
+<i>10</i> &deg;C range around the temperature used to evaluate the constant
+properties. The maximum errors are <i>0.8</i> % for mass density, <i>1.5</i> %
+for specific heat capacity, <i>3.2</i> % for thermal conductivity and <i>250</i>
+% for dynamic viscosity.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/PropyleneGlycolWaterError10degC.png\" border=\"1\"
+alt=\"Relative variation of specific heat capacity with temperature\"/>
+</p>
+<p>
+The figure below shows the relative error of the the four properties over a
+<i>20</i> &deg;C range around the temperature used to evaluate the constant
+proepties. The maximum errors are <i>1.6</i> % for mass density, <i>3.0</i> %
+for specific heat capacity, <i>6.2</i> % for thermal conductivity and <i>950</i>
+% for dynamic viscosity.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Antifreeze/PropyleneGlycolWaterError20degC.png\" border=\"1\"
+alt=\"Relative variation of specific heat capacity with temperature\"/>
+</p>
+<p>
+The enthalpy is computed using the convention that <i>h=0</i>
+if <i>T=0</i> &deg;C.
+</p>
+<h4>Limitations</h4>
+<p>
+Density, specific heat capacity, thermal conductivity and viscosity are constant.
+The propylene glycol/water mixture is modeled as an incompressible liquid.
+There are no phase changes. The medium is limited to temperatures below
+<i>100</i> &deg;C and mass fractions below <i>0.60</i>.
+As is the case for <a href=\"modelica://AixLib.Media.Water\">AixLib.Media.Water</a>,
+this medium package should not be used if
+the simulation relies on the dynamic viscosity.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The temperature and mass fraction must be specified for the evaluation of the
+constant thermophysical properties. A typical use of the package is (e.g. for
+a temperature of <i>20</i> &deg;C and a mass fraction of <i>0.40</i>):
+</p>
+<p>
+<code>Medium = AixLib.Media.Antifreeze.PropyleneGlycolWater(property_T=293.15, X_a=0.40)</code>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 26, 2018, by Filip Jorissen and Michael Wetter:<br/>
+Now printing different messages if temperature or mass fraction is above or below its limit,
+and adding instance name as JModelica does not print the full instance name in the assertion.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1045\">#1045</a>.
+</li>
+<li>
+March 16, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropyleneGlycolWater;
diff --git a/AixLib/Media/Antifreeze/Validation/BaseClasses/EthyleneGlycolWater.mo b/AixLib/Media/Antifreeze/Validation/BaseClasses/EthyleneGlycolWater.mo
index 14b7791bce..89fec6c20f 100644
--- a/AixLib/Media/Antifreeze/Validation/BaseClasses/EthyleneGlycolWater.mo
+++ b/AixLib/Media/Antifreeze/Validation/BaseClasses/EthyleneGlycolWater.mo
@@ -14,22 +14,22 @@ package EthyleneGlycolWater
     d := density_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.density_TX_a\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater.density_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.density_TX_a\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater.density_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
     end testDensity_TX_a;
 
   function testDynamicViscosity_TX_a
@@ -44,22 +44,22 @@ package EthyleneGlycolWater
     eta := dynamicViscosity_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.dynamicViscosity_TX_a\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater.dynamicViscosity_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.dynamicViscosity_TX_a\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater.dynamicViscosity_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end testDynamicViscosity_TX_a;
 
   function testFusionTemperature_TX_a
@@ -74,22 +74,22 @@ package EthyleneGlycolWater
     Tf := fusionTemperature_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.fusionTemperature_TX_a\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater.fusionTemperature_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.fusionTemperature_TX_a\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater.fusionTemperature_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end testFusionTemperature_TX_a;
 
   function testSpecificHeatCapacityCp_TX_a
@@ -104,22 +104,22 @@ package EthyleneGlycolWater
     cp := specificHeatCapacityCp_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.specificHeatCapacityCp_TX_a\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater.specificHeatCapacityCp_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.specificHeatCapacityCp_TX_a\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater.specificHeatCapacityCp_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end testSpecificHeatCapacityCp_TX_a;
 
   function testThermalConductivity_TX_a
@@ -134,41 +134,41 @@ package EthyleneGlycolWater
     lambda := thermalConductivity_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.thermalConductivity_TX_a\">
- AixLib.Media.Antifreeze.EthyleneGlycolWater.thermalConductivity_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.EthyleneGlycolWater.thermalConductivity_TX_a\">
+AixLib.Media.Antifreeze.EthyleneGlycolWater.thermalConductivity_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end testThermalConductivity_TX_a;
 annotation (Documentation(info="<html>
- <p>
- Media implementation that extends
- <a href=\"modelica://AixLib.Media.Antifreeze\">
- AixLib.Media.Antifreeze</a>
- in order to make its thermophysical property functions
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",
+<p>
+Media implementation that extends
+<a href=\"modelica://AixLib.Media.Antifreeze\">
+AixLib.Media.Antifreeze</a>
+in order to make its thermophysical property functions
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>",
       revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EthyleneGlycolWater;
diff --git a/AixLib/Media/Antifreeze/Validation/BaseClasses/FluidProperties.mo b/AixLib/Media/Antifreeze/Validation/BaseClasses/FluidProperties.mo
index f04728604f..403426c4f5 100644
--- a/AixLib/Media/Antifreeze/Validation/BaseClasses/FluidProperties.mo
+++ b/AixLib/Media/Antifreeze/Validation/BaseClasses/FluidProperties.mo
@@ -46,24 +46,24 @@ equation
 
    annotation (
 Documentation(info="<html>
- <p>
- This example checks the implementation of functions that evaluate the
- temperature- and concentration-dependent thermophysical properties of the
- medium.
- </p>
- <p>
- Thermophysical properties (density, specific heat capacity, thermal conductivity
- and dynamic viscosity) are shown as 0 if the temperature is below the fusion
- temperature.
- </p>
- </html>",
+<p>
+This example checks the implementation of functions that evaluate the
+temperature- and concentration-dependent thermophysical properties of the
+medium.
+</p>
+<p>
+Thermophysical properties (density, specific heat capacity, thermal conductivity
+and dynamic viscosity) are shown as 0 if the temperature is below the fusion
+temperature.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 14, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 14, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FluidProperties;
diff --git a/AixLib/Media/Antifreeze/Validation/BaseClasses/PropyleneGlycolWater.mo b/AixLib/Media/Antifreeze/Validation/BaseClasses/PropyleneGlycolWater.mo
index e59e4629f2..501da8ed01 100644
--- a/AixLib/Media/Antifreeze/Validation/BaseClasses/PropyleneGlycolWater.mo
+++ b/AixLib/Media/Antifreeze/Validation/BaseClasses/PropyleneGlycolWater.mo
@@ -14,22 +14,22 @@ package PropyleneGlycolWater
     d := density_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.density_TX_a\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater.density_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.density_TX_a\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater.density_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
     end testDensity_TX_a;
 
   function testDynamicViscosity_TX_a
@@ -44,22 +44,22 @@ package PropyleneGlycolWater
     eta := dynamicViscosity_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.dynamicViscosity_TX_a\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater.dynamicViscosity_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.dynamicViscosity_TX_a\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater.dynamicViscosity_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end testDynamicViscosity_TX_a;
 
   function testFusionTemperature_TX_a
@@ -74,22 +74,22 @@ package PropyleneGlycolWater
     Tf := fusionTemperature_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.fusionTemperature_TX_a\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater.fusionTemperature_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.fusionTemperature_TX_a\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater.fusionTemperature_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end testFusionTemperature_TX_a;
 
   function testSpecificHeatCapacityCp_TX_a
@@ -104,22 +104,22 @@ package PropyleneGlycolWater
     cp := specificHeatCapacityCp_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.specificHeatCapacityCp_TX_a\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater.specificHeatCapacityCp_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.specificHeatCapacityCp_TX_a\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater.specificHeatCapacityCp_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end testSpecificHeatCapacityCp_TX_a;
 
   function testThermalConductivity_TX_a
@@ -134,41 +134,41 @@ package PropyleneGlycolWater
     lambda := thermalConductivity_TX_a(T = T, X_a = X_a);
 
     annotation (Documentation(info="<html>
- <p>
- Function that makes
- <a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.thermalConductivity_TX_a\">
- AixLib.Media.Antifreeze.PropyleneGlycolWater.thermalConductivity_TX_a</a>
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Function that makes
+<a href=\"modelica://AixLib.Media.Antifreeze.PropyleneGlycolWater.thermalConductivity_TX_a\">
+AixLib.Media.Antifreeze.PropyleneGlycolWater.thermalConductivity_TX_a</a>
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end testThermalConductivity_TX_a;
 annotation (Documentation(info="<html>
- <p>
- Media implementation that extends
- <a href=\"modelica://AixLib.Media.Antifreeze\">
- AixLib.Media.Antifreeze</a>
- in order to make its thermophysical property functions
- publicly accessible as needed for the validation model
- <a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
- AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
- </p>
- </html>",
+<p>
+Media implementation that extends
+<a href=\"modelica://AixLib.Media.Antifreeze\">
+AixLib.Media.Antifreeze</a>
+in order to make its thermophysical property functions
+publicly accessible as needed for the validation model
+<a href=\"modelica://AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties\">
+AixLib.Media.Antifreeze.Validation.BaseClasses.FluidProperties</a>.
+</p>
+</html>",
       revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 14, 2018 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropyleneGlycolWater;
diff --git a/AixLib/Media/Antifreeze/Validation/EthyleneGlycolWater.mo b/AixLib/Media/Antifreeze/Validation/EthyleneGlycolWater.mo
index 4b800c2804..e6f360e888 100644
--- a/AixLib/Media/Antifreeze/Validation/EthyleneGlycolWater.mo
+++ b/AixLib/Media/Antifreeze/Validation/EthyleneGlycolWater.mo
@@ -16,24 +16,24 @@ model EthyleneGlycolWater
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Antifreeze/Validation/EthyleneGlycolWater.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks the implementation of functions that evaluate the
- temperature- and concentration-dependent thermophysical properties of the
- medium.
- </p>
- <p>
- Thermophysical properties (density, specific heat capacity, thermal conductivity
- and dynamic viscosity) are shown as 0 if the temperature is below the fusion
- temperature.
- </p>
- </html>",
+<p>
+This example checks the implementation of functions that evaluate the
+temperature- and concentration-dependent thermophysical properties of the
+medium.
+</p>
+<p>
+Thermophysical properties (density, specific heat capacity, thermal conductivity
+and dynamic viscosity) are shown as 0 if the temperature is below the fusion
+temperature.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2020, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 18, 2020, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end EthyleneGlycolWater;
diff --git a/AixLib/Media/Antifreeze/Validation/PropyleneGlycolWater.mo b/AixLib/Media/Antifreeze/Validation/PropyleneGlycolWater.mo
index 4a79b54037..cb8bbf684d 100644
--- a/AixLib/Media/Antifreeze/Validation/PropyleneGlycolWater.mo
+++ b/AixLib/Media/Antifreeze/Validation/PropyleneGlycolWater.mo
@@ -16,24 +16,24 @@ model PropyleneGlycolWater
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Antifreeze/Validation/PropyleneGlycolWater.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks the implementation of functions that evaluate the
- temperature- and concentration-dependent thermophysical properties of the
- medium.
- </p>
- <p>
- Thermophysical properties (density, specific heat capacity, thermal conductivity
- and dynamic viscosity) are shown as 0 if the temperature is below the fusion
- temperature.
- </p>
- </html>",
+<p>
+This example checks the implementation of functions that evaluate the
+temperature- and concentration-dependent thermophysical properties of the
+medium.
+</p>
+<p>
+Thermophysical properties (density, specific heat capacity, thermal conductivity
+and dynamic viscosity) are shown as 0 if the temperature is below the fusion
+temperature.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 14, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 14, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropyleneGlycolWater;
diff --git a/AixLib/Media/Examples/AirDerivativeCheck.mo b/AixLib/Media/Examples/AirDerivativeCheck.mo
index 95dbe95a37..14bc61d5cc 100644
--- a/AixLib/Media/Examples/AirDerivativeCheck.mo
+++ b/AixLib/Media/Examples/AirDerivativeCheck.mo
@@ -61,29 +61,29 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/AirDerivativeCheck.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- August 17, 2015, by Michael Wetter:<br/>
- Changed regression test to have slope different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- November 20, 2013, by Michael Wetter:<br/>
- Removed check of <code>enthalpyOfDryAir</code> as this function
- is protected and should therefore not be accessed from outside the class.
- </li>
- <li>
- May 12, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+August 17, 2015, by Michael Wetter:<br/>
+Changed regression test to have slope different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+November 20, 2013, by Michael Wetter:<br/>
+Removed check of <code>enthalpyOfDryAir</code> as this function
+is protected and should therefore not be accessed from outside the class.
+</li>
+<li>
+May 12, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirDerivativeCheck;
diff --git a/AixLib/Media/Examples/AirProperties.mo b/AixLib/Media/Examples/AirProperties.mo
index 36bed8355c..f4ff983fc8 100644
--- a/AixLib/Media/Examples/AirProperties.mo
+++ b/AixLib/Media/Examples/AirProperties.mo
@@ -23,17 +23,17 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/AirProperties.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks thermophysical properties of the medium.
- </p>
- </html>",
+<p>
+This example checks thermophysical properties of the medium.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 19, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 19, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirProperties;
diff --git a/AixLib/Media/Examples/AirTemperatureEnthalpyInversion.mo b/AixLib/Media/Examples/AirTemperatureEnthalpyInversion.mo
index c55cd3c2b0..84494753e3 100644
--- a/AixLib/Media/Examples/AirTemperatureEnthalpyInversion.mo
+++ b/AixLib/Media/Examples/AirTemperatureEnthalpyInversion.mo
@@ -9,18 +9,18 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/AirTemperatureEnthalpyInversion.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests whether the inversion of temperature and enthalpy
- is implemented correctly.
- If <i>T &ne; T(h(T))</i>, the model stops with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 21, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the inversion of temperature and enthalpy
+is implemented correctly.
+If <i>T &ne; T(h(T))</i>, the model stops with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 21, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AirTemperatureEnthalpyInversion;
diff --git a/AixLib/Media/Examples/BaseClasses/FluidProperties.mo b/AixLib/Media/Examples/BaseClasses/FluidProperties.mo
index 709f1a76ad..e5c9659be0 100644
--- a/AixLib/Media/Examples/BaseClasses/FluidProperties.mo
+++ b/AixLib/Media/Examples/BaseClasses/FluidProperties.mo
@@ -27,34 +27,34 @@ equation
     ddTp = Medium.density_derT_p(state_pTX);
     dddX   = Medium.density_derX(state_pTX);
    annotation (Documentation(info="<html>
- <p>
- This example checks thermophysical properties of the medium.
- </p>
- </html>",
+<p>
+This example checks thermophysical properties of the medium.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Changed type of <code>T</code> from
- <code>Modelica.Units.SI.Temperature</code> to <code>Medium.Temperature</code>.
- Otherwise, it has a different start value than <code>BaseProperties.T</code>, which
- causes an error if
- <a href=\"AixLib.Media.Examples.WaterProperties\">
- AixLib.Media.Examples.WaterProperties</a>
- is translated in pedantic mode.
- This fixes
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- October 16, 2014, by Michael Wetter:<br/>
- Removed call to <code>setState_dTX</code> as this
- function is physically not defined for incompressible media.
- </li>
- <li>
- December 19, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Changed type of <code>T</code> from
+<code>Modelica.Units.SI.Temperature</code> to <code>Medium.Temperature</code>.
+Otherwise, it has a different start value than <code>BaseProperties.T</code>, which
+causes an error if
+<a href=\"modelica://AixLib.Media.Examples.WaterProperties\">
+AixLib.Media.Examples.WaterProperties</a>
+is translated in pedantic mode.
+This fixes
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+October 16, 2014, by Michael Wetter:<br/>
+Removed call to <code>setState_dTX</code> as this
+function is physically not defined for incompressible media.
+</li>
+<li>
+December 19, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FluidProperties;
diff --git a/AixLib/Media/Examples/BaseClasses/PartialProperties.mo b/AixLib/Media/Examples/BaseClasses/PartialProperties.mo
index a0b4dd0722..c6d128c6cf 100644
--- a/AixLib/Media/Examples/BaseClasses/PartialProperties.mo
+++ b/AixLib/Media/Examples/BaseClasses/PartialProperties.mo
@@ -48,7 +48,7 @@ protected
     extends Modelica.Icons.Function;
     input Medium.ThermodynamicState state1 "Medium state";
     input Medium.ThermodynamicState state2 "Medium state";
-    input Real errAbs=errAbs "Absolute error threshold";
+    input Real errAbs "Absolute error threshold";
     input String message "Message for error reporting";
 
   protected
@@ -96,43 +96,49 @@ equation
 
    annotation (
 Documentation(info="<html>
- <p>
- This example checks thermophysical properties of the medium.
- </p>
- </html>",
+<p>
+This example checks thermophysical properties of the medium.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 24, 2020, by Kathryn Hinkelman:<br/>
- Expand error message for checkState and added absolute error as input.
- </li>
- <li>
- September 16, 2019, by Yangyang Fu:<br/>
- Reconstruct the implementation structure to avoid duplicated codes for different media.
- This fixes <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1206\">#1206</a>.
- </li>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Changed type of <code>T</code> from
- <code>Modelica.Units.SI.Temperature</code> to <code>Medium.Temperature</code>.
- Otherwise, it has a different start value than <code>BaseProperties.T</code>, which
- causes an error if
- <a href=\"AixLib.Media.Examples.WaterProperties\">
- AixLib.Media.Examples.WaterProperties</a>
- is translated in pedantic mode.
- This fixes
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- October 16, 2014, by Michael Wetter:<br/>
- Removed call to <code>setState_dTX</code> as this
- function is physically not defined for incompressible media.
- </li>
- <li>
- December 19, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 5, 2023 by Hongxiang Fu:<br/>
+Removed a self-dependent input binding in the function <code>checkState</code>.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3384\">#3384</a>.
+</li>
+<li>
+March 24, 2020, by Kathryn Hinkelman:<br/>
+Expand error message for checkState and added absolute error as input.
+</li>
+<li>
+September 16, 2019, by Yangyang Fu:<br/>
+Reconstruct the implementation structure to avoid duplicated codes for different media.
+This fixes <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1206\">#1206</a>.
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Changed type of <code>T</code> from
+<code>Modelica.Units.SI.Temperature</code> to <code>Medium.Temperature</code>.
+Otherwise, it has a different start value than <code>BaseProperties.T</code>, which
+causes an error if
+<a href=\"modelica://AixLib.Media.Examples.WaterProperties\">
+AixLib.Media.Examples.WaterProperties</a>
+is translated in pedantic mode.
+This fixes
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+October 16, 2014, by Michael Wetter:<br/>
+Removed call to <code>setState_dTX</code> as this
+function is physically not defined for incompressible media.
+</li>
+<li>
+December 19, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialProperties;
diff --git a/AixLib/Media/Examples/BaseClasses/TestTemperatureEnthalpyInversion.mo b/AixLib/Media/Examples/BaseClasses/TestTemperatureEnthalpyInversion.mo
index 572db99860..882f8b06f0 100644
--- a/AixLib/Media/Examples/BaseClasses/TestTemperatureEnthalpyInversion.mo
+++ b/AixLib/Media/Examples/BaseClasses/TestTemperatureEnthalpyInversion.mo
@@ -11,46 +11,52 @@ partial model TestTemperatureEnthalpyInversion
 equation
     h = Medium.specificEnthalpy_pTX(p=101325, T=T0, X=Xi);
     T = Medium.temperature_phX(p=101325, h=h,  X=Xi);
-    if (time>0.1) then
+    if (time>=0.1) then
     assert(abs(T-T0)<tol, "Error in implementation of functions.\n"
        + "   T0 = " + String(T0) + "\n"
        + "   T  = " + String(T) + "\n"
        + "   Absolute error: " + String(abs(T-T0)) + " K");
     end if;
     annotation (preferredView="info", Documentation(info="<html>
- This model computes <code>h=f(T0)</code> and
- <code>T=g(h)</code>. It then checks whether <code>T=T0</code>.
- Hence, it checks whether the function <code>T_phX</code> is
- implemented correctly.
- </html>",revisions="<html>
- <ul>
- <li>
- March 24, 2020 by Kathryn Hinkelman:<br/>
- Expanded the assert message to include absolute error value.
- </li>
- <li>
- September 16, 2019 by Yangyang Fu:<br/>
- Added a parameter <code>tol</code> to control numerical errors.
- </li>
- <li>
- June 6, 2015 by Michael Wetter:<br/>
- Changed <code>Medium</code> base class to avoid a translation error
- in Dymola 2016 using pedantic mode.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- February 12, 2015 by Michael Wetter:<br/>
- Replaced <code>h_pTX</code> with <code>specificEnthalpy_pTX</code>
- and
- <code>T_phX</code> with <code>temperature_phX</code>
- as the old names are not present in all media.
- </li>
- <li>
- January 21, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This model computes <code>h=f(T0)</code> and
+<code>T=g(h)</code>. It then checks whether <code>T=T0</code>.
+Hence, it checks whether the function <code>T_phX</code> is
+implemented correctly.
+</html>", revisions="<html>
+<ul>
+<li>
+November 14, 2022, by Michael Wetter:<br/>
+Reformulated <code>if</code>-expression to avoid warning about state event.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1657\">#1657</a>.
+</li>
+<li>
+March 24, 2020 by Kathryn Hinkelman:<br/>
+Expanded the assert message to include absolute error value.
+</li>
+<li>
+September 16, 2019 by Yangyang Fu:<br/>
+Added a parameter <code>tol</code> to control numerical errors.
+</li>
+<li>
+June 6, 2015 by Michael Wetter:<br/>
+Changed <code>Medium</code> base class to avoid a translation error
+in Dymola 2016 using pedantic mode.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+February 12, 2015 by Michael Wetter:<br/>
+Replaced <code>h_pTX</code> with <code>specificEnthalpy_pTX</code>
+and
+<code>T_phX</code> with <code>temperature_phX</code>
+as the old names are not present in all media.
+</li>
+<li>
+January 21, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestTemperatureEnthalpyInversion;
diff --git a/AixLib/Media/Examples/PropyleneGlycolWaterDerivativeCheck.mo b/AixLib/Media/Examples/PropyleneGlycolWaterDerivativeCheck.mo
index 1a5155b419..a30979bdf8 100644
--- a/AixLib/Media/Examples/PropyleneGlycolWaterDerivativeCheck.mo
+++ b/AixLib/Media/Examples/PropyleneGlycolWaterDerivativeCheck.mo
@@ -48,18 +48,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/PropyleneGlycolWaterDerivativeCheck.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 13, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 13, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropyleneGlycolWaterDerivativeCheck;
diff --git a/AixLib/Media/Examples/PropyleneGlycolWaterProperties.mo b/AixLib/Media/Examples/PropyleneGlycolWaterProperties.mo
index 0fdf075f5e..1a4604283b 100644
--- a/AixLib/Media/Examples/PropyleneGlycolWaterProperties.mo
+++ b/AixLib/Media/Examples/PropyleneGlycolWaterProperties.mo
@@ -16,17 +16,17 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/PropyleneGlycolWaterProperties.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks thermophysical properties of the medium.
- </p>
- </html>",
+<p>
+This example checks thermophysical properties of the medium.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 13, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 13, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropyleneGlycolWaterProperties;
diff --git a/AixLib/Media/Examples/PropyleneGlycolWaterTemperatureEnthalpyInversion.mo b/AixLib/Media/Examples/PropyleneGlycolWaterTemperatureEnthalpyInversion.mo
index 81d381141f..a90753a758 100644
--- a/AixLib/Media/Examples/PropyleneGlycolWaterTemperatureEnthalpyInversion.mo
+++ b/AixLib/Media/Examples/PropyleneGlycolWaterTemperatureEnthalpyInversion.mo
@@ -11,18 +11,18 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/PropyleneGlycolWaterTemperatureEnthalpyInversion.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests whether the inversion of temperature and enthalpy
- is implemented correctly.
- If <i>T &ne; T(h(T))</i>, the model stops with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 13, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the inversion of temperature and enthalpy
+is implemented correctly.
+If <i>T &ne; T(h(T))</i>, the model stops with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 13, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PropyleneGlycolWaterTemperatureEnthalpyInversion;
diff --git a/AixLib/Media/Examples/SteamDerivativeCheck.mo b/AixLib/Media/Examples/SteamDerivativeCheck.mo
index ec30a63398..27db608c24 100644
--- a/AixLib/Media/Examples/SteamDerivativeCheck.mo
+++ b/AixLib/Media/Examples/SteamDerivativeCheck.mo
@@ -49,24 +49,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/SteamDerivativeCheck.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- March 16, 2020, by Michael Wetter:<br/>
- Changed to relative plus absolute error check in assertion because the specific enthalpy has a
- magnitude of <i>1E6</i>, which causes the assertion to fail in JModelica if an absolute accuracy
- of <i>1E-2</i> is requested.
- </li>
- <li>
- March 6, 2020, by Kathryn Hinkelman:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+March 16, 2020, by Michael Wetter:<br/>
+Changed to relative plus absolute error check in assertion because the specific enthalpy has a
+magnitude of <i>1E6</i>, which causes the assertion to fail in JModelica if an absolute accuracy
+of <i>1E-2</i> is requested.
+</li>
+<li>
+March 6, 2020, by Kathryn Hinkelman:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SteamDerivativeCheck;
diff --git a/AixLib/Media/Examples/SteamProperties.mo b/AixLib/Media/Examples/SteamProperties.mo
index ae5258007a..4184ebd387 100644
--- a/AixLib/Media/Examples/SteamProperties.mo
+++ b/AixLib/Media/Examples/SteamProperties.mo
@@ -38,22 +38,22 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/SteamProperties.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks thermophysical properties of the medium.
- </p>
- </html>",
+<p>
+This example checks thermophysical properties of the medium.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 30, 2020, by Kathryn Hinkelman:<br/>
- Rebased steam medium to PartialMedium and improved steam property consistency
- and efficiency.
- </li>
- <li>
- September 12, 2019, by Yangyang Fu:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 30, 2020, by Kathryn Hinkelman:<br/>
+Rebased steam medium to PartialMedium and improved steam property consistency
+and efficiency.
+</li>
+<li>
+September 12, 2019, by Yangyang Fu:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SteamProperties;
diff --git a/AixLib/Media/Examples/SteamSaturationConsistencyCheck.mo b/AixLib/Media/Examples/SteamSaturationConsistencyCheck.mo
index 7d33d3fb45..cd1ab09641 100644
--- a/AixLib/Media/Examples/SteamSaturationConsistencyCheck.mo
+++ b/AixLib/Media/Examples/SteamSaturationConsistencyCheck.mo
@@ -101,22 +101,22 @@ equation
   Icon(coordinateSystem(preserveAspectRatio=false)),
   Diagram(coordinateSystem(preserveAspectRatio=false)),
     Documentation(revisions="<html>
- <ul>
- <li>
- November 8, 2020, by Kathryn Hinkelman:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This example checks the consistency of satuated property functions across the steam and liquid water mediums. 
- It also checks if the inversion of saturated temperature and saturated pressure is implemented correctly 
- for the steam model.
- </p>
- <p>
- Errors are presented as percent differences between the standard property functions - 
- e.g medium.specificEnthalpy(saturatedState) - and the IF97 saturated property functions as the baseline.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 8, 2020, by Kathryn Hinkelman:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This example checks the consistency of satuated property functions across the steam and liquid water mediums. 
+It also checks if the inversion of saturated temperature and saturated pressure is implemented correctly 
+for the steam model.
+</p>
+<p>
+Errors are presented as percent differences between the standard property functions - 
+e.g medium.specificEnthalpy(saturatedState) - and the IF97 saturated property functions as the baseline.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SteamSaturationConsistencyCheck;
diff --git a/AixLib/Media/Examples/SteamTemperatureEnthalpyInversion.mo b/AixLib/Media/Examples/SteamTemperatureEnthalpyInversion.mo
index f76f0d2aa3..e13a2eade9 100644
--- a/AixLib/Media/Examples/SteamTemperatureEnthalpyInversion.mo
+++ b/AixLib/Media/Examples/SteamTemperatureEnthalpyInversion.mo
@@ -10,25 +10,25 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/SteamTemperatureEnthalpyInversion.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests whether the inversion of temperature and enthalpy
- is implemented correctly for the steam model. 
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 24, 2020, by Kathryn Hinkelman:<br/>
- Relaxed absolute error tolerance.
- </li>
- <li>
- January 16, 2020, by Kathryn Hinkelman:<br/>
- Change medium to ideal steam to eliminate property discontinuities.
- </li>
- <li>
- September 12, 2019, by Yangyang Fu:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the inversion of temperature and enthalpy
+is implemented correctly for the steam model. 
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 24, 2020, by Kathryn Hinkelman:<br/>
+Relaxed absolute error tolerance.
+</li>
+<li>
+January 16, 2020, by Kathryn Hinkelman:<br/>
+Change medium to ideal steam to eliminate property discontinuities.
+</li>
+<li>
+September 12, 2019, by Yangyang Fu:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SteamTemperatureEnthalpyInversion;
diff --git a/AixLib/Media/Examples/WaterDerivativeCheck.mo b/AixLib/Media/Examples/WaterDerivativeCheck.mo
index 3b02e5037c..8ee577c6dd 100644
--- a/AixLib/Media/Examples/WaterDerivativeCheck.mo
+++ b/AixLib/Media/Examples/WaterDerivativeCheck.mo
@@ -45,24 +45,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/WaterDerivativeCheck.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- August 17, 2015, by Michael Wetter:<br/>
- Changed regression test to have slope different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+August 17, 2015, by Michael Wetter:<br/>
+Changed regression test to have slope different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterDerivativeCheck;
diff --git a/AixLib/Media/Examples/WaterProperties.mo b/AixLib/Media/Examples/WaterProperties.mo
index e1a5726295..edfc688612 100644
--- a/AixLib/Media/Examples/WaterProperties.mo
+++ b/AixLib/Media/Examples/WaterProperties.mo
@@ -14,17 +14,17 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/WaterProperties.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks thermophysical properties of the medium.
- </p>
- </html>",
+<p>
+This example checks thermophysical properties of the medium.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 19, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 19, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterProperties;
diff --git a/AixLib/Media/Examples/WaterTemperatureEnthalpyInversion.mo b/AixLib/Media/Examples/WaterTemperatureEnthalpyInversion.mo
index 35b89300d6..86d6a697cd 100644
--- a/AixLib/Media/Examples/WaterTemperatureEnthalpyInversion.mo
+++ b/AixLib/Media/Examples/WaterTemperatureEnthalpyInversion.mo
@@ -9,18 +9,18 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Examples/WaterTemperatureEnthalpyInversion.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests whether the inversion of temperature and enthalpy
- is implemented correctly.
- If <i>T &ne; T(h(T))</i>, the model stops with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 21, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the inversion of temperature and enthalpy
+is implemented correctly.
+If <i>T &ne; T(h(T))</i>, the model stops with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 21, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterTemperatureEnthalpyInversion;
diff --git a/AixLib/Media/Refrigerants/R410A/dPressureVap_dSpecificVolume_Tv.mo b/AixLib/Media/Refrigerants/R410A/dPressureVap_dSpecificVolume_Tv.mo
index e3d54abab8..76e1d491b8 100644
--- a/AixLib/Media/Refrigerants/R410A/dPressureVap_dSpecificVolume_Tv.mo
+++ b/AixLib/Media/Refrigerants/R410A/dPressureVap_dSpecificVolume_Tv.mo
@@ -22,30 +22,30 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the derivative of the Martin-Hou equation of for R410A
- state with regards to specific volume.
- </p>
- <h4>References</h4>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- November 8, 2020, by Michael Wetter:<br/>
- Corrected use of dimension <code>n</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
- </li>
- <li>
- November 30, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the derivative of the Martin-Hou equation of for R410A
+state with regards to specific volume.
+</p>
+<h4>References</h4>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+November 8, 2020, by Michael Wetter:<br/>
+Corrected use of dimension <code>n</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
+</li>
+<li>
+November 30, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end dPressureVap_dSpecificVolume_Tv;
diff --git a/AixLib/Media/Refrigerants/R410A/dPressureVap_dTemperature_Tv.mo b/AixLib/Media/Refrigerants/R410A/dPressureVap_dTemperature_Tv.mo
index 7d13919779..608e1cf028 100644
--- a/AixLib/Media/Refrigerants/R410A/dPressureVap_dTemperature_Tv.mo
+++ b/AixLib/Media/Refrigerants/R410A/dPressureVap_dTemperature_Tv.mo
@@ -21,30 +21,30 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the derivative of the Martin-Hou equation of for R410A
- state with regards to temperature.
- </p>
- <h4>References</h4>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- November 8, 2020, by Michael Wetter:<br/>
- Corrected use of dimension <code>n</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
- </li>
- <li>
- November 30, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the derivative of the Martin-Hou equation of for R410A
+state with regards to temperature.
+</p>
+<h4>References</h4>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+November 8, 2020, by Michael Wetter:<br/>
+Corrected use of dimension <code>n</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
+</li>
+<li>
+November 30, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end dPressureVap_dTemperature_Tv;
diff --git a/AixLib/Media/Refrigerants/R410A/dSpecificVolumeVap_pT.mo b/AixLib/Media/Refrigerants/R410A/dSpecificVolumeVap_pT.mo
index c9d832938b..45323d4496 100644
--- a/AixLib/Media/Refrigerants/R410A/dSpecificVolumeVap_pT.mo
+++ b/AixLib/Media/Refrigerants/R410A/dSpecificVolumeVap_pT.mo
@@ -33,18 +33,18 @@ algorithm
   dv := dp/dpdv + dT*(dpdT/dpdv);
 
 annotation (preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the derivatives of
- <a href=\"modelica://AixLib.Media.Refrigerants.R410A.specificVolumeVap_pT\">
- AixLib.Media.Refrigerants.R410A.specificVolumeVap_pT</a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 30, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the derivatives of
+<a href=\"modelica://AixLib.Media.Refrigerants.R410A.specificVolumeVap_pT\">
+AixLib.Media.Refrigerants.R410A.specificVolumeVap_pT</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 30, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end dSpecificVolumeVap_pT;
diff --git a/AixLib/Media/Refrigerants/R410A/enthalpySatLiq_T.mo b/AixLib/Media/Refrigerants/R410A/enthalpySatLiq_T.mo
index e9d078a2b5..66fb8f5608 100644
--- a/AixLib/Media/Refrigerants/R410A/enthalpySatLiq_T.mo
+++ b/AixLib/Media/Refrigerants/R410A/enthalpySatLiq_T.mo
@@ -23,24 +23,24 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the enthalpy of saturated liquid R410A based on
- temperature.
- </p>
- <h4>References</h4>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 17, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the enthalpy of saturated liquid R410A based on
+temperature.
+</p>
+<h4>References</h4>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 17, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end enthalpySatLiq_T;
diff --git a/AixLib/Media/Refrigerants/R410A/enthalpySatVap_T.mo b/AixLib/Media/Refrigerants/R410A/enthalpySatVap_T.mo
index a084570bff..425f43123c 100644
--- a/AixLib/Media/Refrigerants/R410A/enthalpySatVap_T.mo
+++ b/AixLib/Media/Refrigerants/R410A/enthalpySatVap_T.mo
@@ -20,24 +20,24 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the specific enthalpy of saturated R410A vapor based
- on temperature.
- </p>
- <h4>References</h4>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 17, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the specific enthalpy of saturated R410A vapor based
+on temperature.
+</p>
+<h4>References</h4>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 17, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end enthalpySatVap_T;
diff --git a/AixLib/Media/Refrigerants/R410A/isentropicExponentVap_Tv.mo b/AixLib/Media/Refrigerants/R410A/isentropicExponentVap_Tv.mo
index f12988c704..7870ed79d2 100644
--- a/AixLib/Media/Refrigerants/R410A/isentropicExponentVap_Tv.mo
+++ b/AixLib/Media/Refrigerants/R410A/isentropicExponentVap_Tv.mo
@@ -20,37 +20,37 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the isentropic exponent of R410A vapor based on temperature and specific volume. The isentropic exponent is equal to the ratio of specific heat capacities:
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- k = c<sub>p</sub>/c<sub>v</sub>
- </p>
- <h4>References</h4>
- <p>
- F. de Monte. (2002).
- Calculation of thermodynamic properties of R407C and
- R410A by the Martin-Hou equation of state, part I:
- theoretical development.
- <i>
- International Journal of Refrigeration.
- </i>
- 25. 306-313.
- </p>
- <p>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 31, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the isentropic exponent of R410A vapor based on temperature and specific volume. The isentropic exponent is equal to the ratio of specific heat capacities:
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+k = c<sub>p</sub>/c<sub>v</sub>
+</p>
+<h4>References</h4>
+<p>
+F. de Monte. (2002).
+Calculation of thermodynamic properties of R407C and
+R410A by the Martin-Hou equation of state, part I:
+theoretical development.
+<i>
+International Journal of Refrigeration.
+</i>
+25. 306-313.
+</p>
+<p>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 31, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end isentropicExponentVap_Tv;
diff --git a/AixLib/Media/Refrigerants/R410A/pressureSatVap_T.mo b/AixLib/Media/Refrigerants/R410A/pressureSatVap_T.mo
index 462adebcf3..399c8a9511 100644
--- a/AixLib/Media/Refrigerants/R410A/pressureSatVap_T.mo
+++ b/AixLib/Media/Refrigerants/R410A/pressureSatVap_T.mo
@@ -23,23 +23,23 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the pressure of saturated R410A vapor based on temperature.
- </p>
- <h4>References</h4>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 17, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the pressure of saturated R410A vapor based on temperature.
+</p>
+<h4>References</h4>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 17, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end pressureSatVap_T;
diff --git a/AixLib/Media/Refrigerants/R410A/pressureVap_Tv.mo b/AixLib/Media/Refrigerants/R410A/pressureVap_Tv.mo
index 9a1812feb0..93e6eb50f5 100644
--- a/AixLib/Media/Refrigerants/R410A/pressureVap_Tv.mo
+++ b/AixLib/Media/Refrigerants/R410A/pressureVap_Tv.mo
@@ -18,31 +18,31 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the pressure R410A vapor based on temperature and
- specific volume. The pressure is calculated from the Martin-Hou equation of
- state.
- </p>
- <h4>References</h4>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- November 8, 2020, by Michael Wetter:<br/>
- Corrected use of dimension <code>n</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
- </li>
- <li>
- October 17, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the pressure R410A vapor based on temperature and
+specific volume. The pressure is calculated from the Martin-Hou equation of
+state.
+</p>
+<h4>References</h4>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+November 8, 2020, by Michael Wetter:<br/>
+Corrected use of dimension <code>n</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
+</li>
+<li>
+October 17, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end pressureVap_Tv;
diff --git a/AixLib/Media/Refrigerants/R410A/specificIsobaricHeatCapacityVap_Tv.mo b/AixLib/Media/Refrigerants/R410A/specificIsobaricHeatCapacityVap_Tv.mo
index 6485091e8e..d50a533adc 100644
--- a/AixLib/Media/Refrigerants/R410A/specificIsobaricHeatCapacityVap_Tv.mo
+++ b/AixLib/Media/Refrigerants/R410A/specificIsobaricHeatCapacityVap_Tv.mo
@@ -24,43 +24,43 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the specific isobaric heat capacity (<i>c<sub>p</sub></i>) of R410A vapor based on temperature and specific volume.
- </p>
- <p>
- The specific isobaric heat capacity is evaluated from the partial derivatives of the Martin-Hou equation of state.
- </p>
- <h4>References</h4>
- <p>
- F. de Monte. (2002).
- Calculation of thermodynamic properties of R407C and
- R410A by the Martin-Hou equation of state, part I:
- theoretical development.
- <i>
- International Journal of Refrigeration.
- </i>
- 25. 306-313.
- </p>
- <p>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 8, 2020, by Michael Wetter:<br/>
- Removed non-used parameters.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
- </li>
- <li>
- October 31, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the specific isobaric heat capacity (<i>c<sub>p</sub></i>) of R410A vapor based on temperature and specific volume.
+</p>
+<p>
+The specific isobaric heat capacity is evaluated from the partial derivatives of the Martin-Hou equation of state.
+</p>
+<h4>References</h4>
+<p>
+F. de Monte. (2002).
+Calculation of thermodynamic properties of R407C and
+R410A by the Martin-Hou equation of state, part I:
+theoretical development.
+<i>
+International Journal of Refrigeration.
+</i>
+25. 306-313.
+</p>
+<p>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2020, by Michael Wetter:<br/>
+Removed non-used parameters.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
+</li>
+<li>
+October 31, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end specificIsobaricHeatCapacityVap_Tv;
diff --git a/AixLib/Media/Refrigerants/R410A/specificIsochoricHeatCapacityVap_Tv.mo b/AixLib/Media/Refrigerants/R410A/specificIsochoricHeatCapacityVap_Tv.mo
index 847c24eabf..d9db785e63 100644
--- a/AixLib/Media/Refrigerants/R410A/specificIsochoricHeatCapacityVap_Tv.mo
+++ b/AixLib/Media/Refrigerants/R410A/specificIsochoricHeatCapacityVap_Tv.mo
@@ -1,7 +1,7 @@
 within AixLib.Media.Refrigerants.R410A;
 function specificIsochoricHeatCapacityVap_Tv
   "Function that calculates the specific isochoric heat capacity of R410A vapor
-   based on temperature and specific volume"
+  based on temperature and specific volume"
   input Modelica.Units.SI.Temperature T "Temperature of refrigerant";
   input Modelica.Units.SI.SpecificVolume v "Specific volume of refrigerant";
   output Modelica.Units.SI.SpecificHeatCapacity cv
@@ -32,45 +32,45 @@ algorithm
 
 annotation (smoothOrder=1,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the specific isochoric heat capacity
- (<i>c<sub>v</sub></i>) of R410A vapor based on temperature and specific volume.
- </p>
- <p>
- The specific isochoric heat capacity is evaluated from the partial derivatives
- of the Martin-Hou equation of state.
- </p>
- <h4>References</h4>
- <p>
- F. de Monte. (2002).
- Calculation of thermodynamic properties of R407C and
- R410A by the Martin-Hou equation of state, part I:
- theoretical development.
- <i>
- International Journal of Refrigeration.
- </i>
- 25. 306-313.
- </p>
- <p>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 8, 2020, by Michael Wetter:<br/>
- Removed non-used parameters and reformulated integral as a sum, and multiplied sum with common factors.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
- </li>
- <li>
- October 31, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the specific isochoric heat capacity
+(<i>c<sub>v</sub></i>) of R410A vapor based on temperature and specific volume.
+</p>
+<p>
+The specific isochoric heat capacity is evaluated from the partial derivatives
+of the Martin-Hou equation of state.
+</p>
+<h4>References</h4>
+<p>
+F. de Monte. (2002).
+Calculation of thermodynamic properties of R407C and
+R410A by the Martin-Hou equation of state, part I:
+theoretical development.
+<i>
+International Journal of Refrigeration.
+</i>
+25. 306-313.
+</p>
+<p>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2020, by Michael Wetter:<br/>
+Removed non-used parameters and reformulated integral as a sum, and multiplied sum with common factors.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
+</li>
+<li>
+October 31, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end specificIsochoricHeatCapacityVap_Tv;
diff --git a/AixLib/Media/Refrigerants/R410A/specificVolumeVap_pT.mo b/AixLib/Media/Refrigerants/R410A/specificVolumeVap_pT.mo
index e238cb735e..c9ba74c319 100644
--- a/AixLib/Media/Refrigerants/R410A/specificVolumeVap_pT.mo
+++ b/AixLib/Media/Refrigerants/R410A/specificVolumeVap_pT.mo
@@ -37,35 +37,35 @@ end while;
 
 annotation (derivative=AixLib.Media.Refrigerants.R410A.dSpecificVolumeVap_pT,
 preferredView="info",Documentation(info="<HTML>
- <p>
- Function that calculates the specific volume R410A vapor based on pressure and
- temperature. The specific volume is evaluated iteratively by succesive
- evaluations of the vapor pressure.
- </p>
- <p>
- The initial guess is estimated by the first term in the Martin-Hou equation of
- state.
- </p>
- <h4>References</h4>
- <p>
- Thermodynamic properties of DuPont Suva 410A:
- <a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
- https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
- </a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 8, 2020, by Michael Wetter:<br/>
- Removed non-used parameters.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
- </li>
- <li>
- October 17, 2016, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that calculates the specific volume R410A vapor based on pressure and
+temperature. The specific volume is evaluated iteratively by succesive
+evaluations of the vapor pressure.
+</p>
+<p>
+The initial guess is estimated by the first term in the Martin-Hou equation of
+state.
+</p>
+<h4>References</h4>
+<p>
+Thermodynamic properties of DuPont Suva 410A:
+<a href=\"https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf\">
+https://www.chemours.com/Refrigerants/en_US/assets/downloads/h64423_Suva410A_thermo_prop_si.pdf
+</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 8, 2020, by Michael Wetter:<br/>
+Removed non-used parameters.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1414\">#1414</a>.
+</li>
+<li>
+October 17, 2016, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end specificVolumeVap_pT;
diff --git a/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_340_Formula/package.order b/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_340_Formula/package.order
index f547d28437..e69de29bb2 100644
--- a/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_340_Formula/package.order
+++ b/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_340_Formula/package.order
@@ -1,30 +0,0 @@
-refrigerantConstants
-SmoothTransition
-f_Idg
-f_Res
-t_fIdg_t
-tt_fIdg_tt
-t_fRes_t
-tt_fRes_tt
-d_fRes_d
-dd_fRes_dd
-td_fRes_td
-ttt_fIdg_ttt
-ttt_fRes_ttt
-ddd_fRes_ddd
-tdd_fRes_tdd
-ttd_fRes_ttd
-saturationPressure
-saturationTemperature
-bubbleDensity
-dewDensity
-bubbleEnthalpy
-dewEnthalpy
-bubbleEntropy
-dewEntropy
-temperature_ph
-temperature_ps
-density_pT
-dynamicViscosity
-thermalConductivity
-surfaceTension
diff --git a/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_340_Record/package.order b/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_340_Record/package.order
index b433689bb9..e69de29bb2 100644
--- a/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_340_Record/package.order
+++ b/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_340_Record/package.order
@@ -1,8 +0,0 @@
-refrigerantConstants
-EoS
-BDSP
-TSP
-SmoothTransition
-dynamicViscosity
-thermalConductivity
-surfaceTension
diff --git a/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_473_Formula/package.order b/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_473_Formula/package.order
index f547d28437..e69de29bb2 100644
--- a/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_473_Formula/package.order
+++ b/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_473_Formula/package.order
@@ -1,30 +0,0 @@
-refrigerantConstants
-SmoothTransition
-f_Idg
-f_Res
-t_fIdg_t
-tt_fIdg_tt
-t_fRes_t
-tt_fRes_tt
-d_fRes_d
-dd_fRes_dd
-td_fRes_td
-ttt_fIdg_ttt
-ttt_fRes_ttt
-ddd_fRes_ddd
-tdd_fRes_tdd
-ttd_fRes_ttd
-saturationPressure
-saturationTemperature
-bubbleDensity
-dewDensity
-bubbleEnthalpy
-dewEnthalpy
-bubbleEntropy
-dewEntropy
-temperature_ph
-temperature_ps
-density_pT
-dynamicViscosity
-thermalConductivity
-surfaceTension
diff --git a/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_473_Horner/package.order b/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_473_Horner/package.order
index f547d28437..e69de29bb2 100644
--- a/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_473_Horner/package.order
+++ b/AixLib/Media/Refrigerants/R410A_HEoS/R410a_IIR_P1_48_T233_473_Horner/package.order
@@ -1,30 +0,0 @@
-refrigerantConstants
-SmoothTransition
-f_Idg
-f_Res
-t_fIdg_t
-tt_fIdg_tt
-t_fRes_t
-tt_fRes_tt
-d_fRes_d
-dd_fRes_dd
-td_fRes_td
-ttt_fIdg_ttt
-ttt_fRes_ttt
-ddd_fRes_ddd
-tdd_fRes_tdd
-ttd_fRes_ttd
-saturationPressure
-saturationTemperature
-bubbleDensity
-dewDensity
-bubbleEnthalpy
-dewEnthalpy
-bubbleEntropy
-dewEntropy
-temperature_ph
-temperature_ps
-density_pT
-dynamicViscosity
-thermalConductivity
-surfaceTension
diff --git a/AixLib/Media/Refrigerants/Validation/R410A_dSpecificVolumeVap_pT.mo b/AixLib/Media/Refrigerants/Validation/R410A_dSpecificVolumeVap_pT.mo
index caba063e50..06140da2ed 100644
--- a/AixLib/Media/Refrigerants/Validation/R410A_dSpecificVolumeVap_pT.mo
+++ b/AixLib/Media/Refrigerants/Validation/R410A_dSpecificVolumeVap_pT.mo
@@ -42,12 +42,12 @@ protected
   Real dv_p_num(
     final unit="m3/(kg)")
     "Numerical delta of specific volume of refrigerant with regards to
-     pressure";
+    pressure";
 
   Real dv_T_num(
     final unit="m3/(kg)")
     "Numerical delta of specific volume of refrigerant with regards to
-     temperature";
+    temperature";
 
   constant Modelica.Units.SI.Time oneSec=1.0
     "Unit time variable for unit conversion of time derivatives";
@@ -80,21 +80,21 @@ equation
     experiment(
       Tolerance=1e-6, StopTime=100),
     Documentation(info="<html>
- <p>
- Validation case for evaluation of derivatives of the Martin-Hou equation of
- state with regards to pressure and temperature.
- </p>
- <p>
- The analytical implementation of derivatives is compared to a numerical
- evaluation of the derivatives.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 25, 2017, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Validation case for evaluation of derivatives of the Martin-Hou equation of
+state with regards to pressure and temperature.
+</p>
+<p>
+The analytical implementation of derivatives is compared to a numerical
+evaluation of the derivatives.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 25, 2017, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end R410A_dSpecificVolumeVap_pT;
diff --git a/AixLib/Media/Specialized/Air/Examples/PerfectGasDerivativeCheck.mo b/AixLib/Media/Specialized/Air/Examples/PerfectGasDerivativeCheck.mo
index 90842673fb..fb9ae106d7 100644
--- a/AixLib/Media/Specialized/Air/Examples/PerfectGasDerivativeCheck.mo
+++ b/AixLib/Media/Specialized/Air/Examples/PerfectGasDerivativeCheck.mo
@@ -38,24 +38,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Specialized/Air/Examples/PerfectGasDerivativeCheck.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- August 17, 2015, by Michael Wetter:<br/>
- Changed regression test to have slope different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- May 12, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+August 17, 2015, by Michael Wetter:<br/>
+Changed regression test to have slope different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+May 12, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PerfectGasDerivativeCheck;
diff --git a/AixLib/Media/Specialized/Air/Examples/PerfectGasTemperatureEnthalpyInversion.mo b/AixLib/Media/Specialized/Air/Examples/PerfectGasTemperatureEnthalpyInversion.mo
index 6d97395044..c45d6f66bd 100644
--- a/AixLib/Media/Specialized/Air/Examples/PerfectGasTemperatureEnthalpyInversion.mo
+++ b/AixLib/Media/Specialized/Air/Examples/PerfectGasTemperatureEnthalpyInversion.mo
@@ -9,18 +9,18 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Specialized/Air/Examples/PerfectGasTemperatureEnthalpyInversion.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests whether the inversion of temperature and enthalpy
- is implemented correctly.
- If <i>T &ne; T(h(T))</i>, the model stops with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 21, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the inversion of temperature and enthalpy
+is implemented correctly.
+If <i>T &ne; T(h(T))</i>, the model stops with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 21, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PerfectGasTemperatureEnthalpyInversion;
diff --git a/AixLib/Media/Specialized/Air/PerfectGas.mo b/AixLib/Media/Specialized/Air/PerfectGas.mo
index 77a0ea86d6..d0f5d7e197 100644
--- a/AixLib/Media/Specialized/Air/PerfectGas.mo
+++ b/AixLib/Media/Specialized/Air/PerfectGas.mo
@@ -28,14 +28,16 @@ package PerfectGas "Model for air as a perfect gas"
 
   redeclare replaceable model extends BaseProperties(
     p(stateSelect=if preferredMediumStates then StateSelect.prefer else StateSelect.default),
-    Xi(each stateSelect=if preferredMediumStates then StateSelect.prefer else StateSelect.default),
+    Xi(
+      nominal={0.01},
+      each stateSelect=if preferredMediumStates then StateSelect.prefer else StateSelect.default),
     final standardOrderComponents=true)
 
     /* p, T, X = X[Water] are used as preferred states, since only then all
-      other quantities can be computed in a recursive sequence.
-      If other variables are selected as states, static state selection
-      is no longer possible and non-linear algebraic equations occur.
-       */
+     other quantities can be computed in a recursive sequence.
+     If other variables are selected as states, static state selection
+     is no longer possible and non-linear algebraic equations occur.
+      */
   protected
     constant Modelica.Units.SI.MolarMass[2] MMX={steam.MM,dryair.MM}
       "Molar masses of components";
@@ -44,11 +46,11 @@ package PerfectGas "Model for air as a perfect gas"
     MassFraction X_air "Mass fraction of air";
   equation
     assert(T >= 200.0, "
- In "  + getInstanceName() + ": Temperature T exceeded its minimum allowed value of -73.15 degC (200 Kelvin)
- as required from medium model \""+ mediumName + "\".");
+In "   + getInstanceName() + ": Temperature T exceeded its minimum allowed value of -73.15 degC (200 Kelvin)
+as required from medium model \"" + mediumName + "\".");
     assert(T <= 423.15, "
- In "  + getInstanceName() + ": Temperature T exceeded its maximum allowed value of 150 degC (423.15 Kelvin)
- as required from medium model \""+ mediumName + "\".");
+In "   + getInstanceName() + ": Temperature T exceeded its maximum allowed value of 150 degC (423.15 Kelvin)
+as required from medium model \"" + mediumName + "\".");
 
     MM = 1/(Xi[Water]/MMX[Water]+(1.0-Xi[Water])/MMX[Air]);
 
@@ -63,8 +65,8 @@ package PerfectGas "Model for air as a perfect gas"
     u =h - R_s*T;
     d =p/(R_s*T);
     /* Note, u and d are computed under the assumption that the volume of the liquid
-          water is negligible with respect to the volume of air and of steam
-       */
+         water is negligible with respect to the volume of air and of steam
+      */
     state.p = p;
     state.T = T;
     state.X = X;
@@ -95,8 +97,8 @@ package PerfectGas "Model for air as a perfect gas"
     annotation (
   Inline=true,
   Documentation(info="<html>
- Function to set the state for given pressure, enthalpy and species concentration.
- </html>"));
+Function to set the state for given pressure, enthalpy and species concentration.
+</html>"));
   end setState_phX;
 
   redeclare function setState_dTX
@@ -124,9 +126,9 @@ package PerfectGas "Model for air as a perfect gas"
     smoothOrder=2,
     Inline=true,
     Documentation(info="<html>
-   The thermodynamic state record
-   is computed from density d, temperature T and composition X.
- </html>"));
+  The thermodynamic state record
+  is computed from density d, temperature T and composition X.
+</html>"));
   end setState_dTX;
 
 redeclare function extends gasConstant "Gas constant"
@@ -152,9 +154,9 @@ algorithm
     Inline=true,
     derivative=AixLib.Media.Specialized.Air.PerfectGas.saturationPressureLiquid_der,
     Documentation(info="<html>
- Saturation pressure of water above the triple point temperature is computed from temperature. It's range of validity is between
- 273.16 and 373.16 K. Outside these limits a less accurate result is returned.
- </html>"));
+Saturation pressure of water above the triple point temperature is computed from temperature. It's range of validity is between
+273.16 and 373.16 K. Outside these limits a less accurate result is returned.
+</html>"));
 end saturationPressureLiquid;
 
 function saturationPressureLiquid_der
@@ -172,10 +174,10 @@ algorithm
     smoothOrder=5,
     Inline=true,
 Documentation(info="<html>
- Derivative function of
- <a href=\"modelica://AixLib.Media.Specialized.Air.PerfectGas.saturationPressureLiquid\">
- AixLib.Media.Specialized.Air.PerfectGas.saturationPressureLiquid</a>
- </html>"));
+Derivative function of
+<a href=\"modelica://AixLib.Media.Specialized.Air.PerfectGas.saturationPressureLiquid\">
+AixLib.Media.Specialized.Air.PerfectGas.saturationPressureLiquid</a>
+</html>"));
 end saturationPressureLiquid_der;
 
   function sublimationPressureIce =
@@ -209,8 +211,8 @@ end saturationPressure;
     smoothOrder=2,
     Inline=true,
     Documentation(info="<html>
- Pressure is returned from the thermodynamic state record input as a simple assignment.
- </html>"));
+Pressure is returned from the thermodynamic state record input as a simple assignment.
+</html>"));
  end pressure;
 
  redeclare function extends temperature "Gas temperature"
@@ -220,8 +222,8 @@ end saturationPressure;
     smoothOrder=2,
     Inline=true,
     Documentation(info="<html>
- Temperature is returned from the thermodynamic state record input as a simple assignment.
- </html>"));
+Temperature is returned from the thermodynamic state record input as a simple assignment.
+</html>"));
  end temperature;
 
  redeclare function extends density "Gas density"
@@ -231,8 +233,8 @@ end saturationPressure;
     smoothOrder=2,
     Inline=true,
     Documentation(info="<html>
- Density is computed from pressure, temperature and composition in the thermodynamic state record applying the ideal gas law.
- </html>"));
+Density is computed from pressure, temperature and composition in the thermodynamic state record applying the ideal gas law.
+</html>"));
  end density;
 
  redeclare function extends specificEntropy
@@ -246,8 +248,8 @@ end saturationPressure;
     smoothOrder=2,
     Inline=true,
     Documentation(info="<html>
- Specific entropy is calculated from the thermodynamic state record, assuming ideal gas behavior and including entropy of mixing. Liquid or solid water is not taken into account, the entire water content X[1] is assumed to be in the vapor state (relative humidity below 1.0).
- </html>"));
+Specific entropy is calculated from the thermodynamic state record, assuming ideal gas behavior and including entropy of mixing. Liquid or solid water is not taken into account, the entire water content X[1] is assumed to be in the vapor state (relative humidity below 1.0).
+</html>"));
  end specificEntropy;
 
  redeclare function extends enthalpyOfVaporization
@@ -495,10 +497,10 @@ algorithm
              Inline=true,
              inverse(h=specificEnthalpy_pTX(p, T, X)),
              Documentation(info="<html>
- Temperature as a function of specific enthalpy and species concentration.
- The pressure is input for compatibility with the medium models, but the temperature
- is independent of the pressure.
- </html>"));
+Temperature as a function of specific enthalpy and species concentration.
+The pressure is input for compatibility with the medium models, but the temperature
+is independent of the pressure.
+</html>"));
 end temperature_phX;
 //////////////////////////////////////////////////////////////////////
 // Protected classes.
@@ -521,39 +523,39 @@ protected
     annotation (
       preferredView="info",
       Documentation(info="<html>
- <p>
- This data record contains the coefficients for perfect gases.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Set <code>AbsolutePressure(start=p_default)</code>
- and <code>Temperature(start=T_default)</code>
- to have to have conistent start values.
- See also revision notes of
- <a href=\"modelica://AixLib.Media.Water\">
- AixLib.Media.Water</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- May 1, 2015, by Michael Wetter:<br/>
- Added <code>Inline=true</code> for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
- issue 227</a>.
- </li>
- <li>
- September 12, 2014, by Michael Wetter:<br/>
- Corrected the wrong location of the <code>preferredView</code>
- and the <code>revisions</code> annotation.
- </li>
- <li>
- November 21, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+This data record contains the coefficients for perfect gases.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Set <code>AbsolutePressure(start=p_default)</code>
+and <code>Temperature(start=T_default)</code>
+to have to have conistent start values.
+See also revision notes of
+<a href=\"modelica://AixLib.Media.Water\">
+AixLib.Media.Water</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+May 1, 2015, by Michael Wetter:<br/>
+Added <code>Inline=true</code> for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
+issue 227</a>.
+</li>
+<li>
+September 12, 2014, by Michael Wetter:<br/>
+Corrected the wrong location of the <code>preferredView</code>
+and the <code>revisions</code> annotation.
+</li>
+<li>
+November 21, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end GasProperties;
   // In the assignments below, we compute cv as OpenModelica
   // cannot evaluate cv=cp-R as defined in GasProperties.
@@ -583,101 +585,107 @@ protected
   function s_pTX_der = Modelica.Media.Air.MoistAir.s_pTX_der
     "Return specific entropy of moist air as a function of pressure p, temperature T and composition X (only valid for phi<1)";
   annotation(preferredView="info", Documentation(info="<html>
- <p>
- This package contains a <i>thermally perfect</i> model of moist air.
- </p>
- <p>
- A medium is called thermally perfect if
- </p>
- <ul>
- <li>
- it is in thermodynamic equilibrium,
- </li><li>
- it is chemically not reacting, and
- </li><li>
- internal energy and enthalpy are functions of temperature only.
- </li>
- </ul>
- <p>
- In addition, this medium model is <i>calorically perfect</i>, i.e., the
- specific heat capacities at constant pressure <i>c<sub>p</sub></i>
- and constant volume <i>c<sub>v</sub></i> are both constant (Bower 1998).
- </p>
- <p>
- This medium uses the ideal gas law
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &rho; = p &frasl;(R T),
- </p>
- <p>
- where
- <i>&rho;</i> is the density,
- <i>p</i> is the pressure,
- <i>R</i> is the gas constant and
- <i>T</i> is the temperature.
- </p>
- <p>
- The enthalpy is computed using the convention that <i>h=0</i>
- if <i>T=0</i> &deg;C and no water vapor is present.
- </p>
- <p>
- Note that for typical building simulations, the media
- <a href=\"modelica://AixLib.Media.Air\">AixLib.Media.Air</a>
- should be used as it leads generally to faster simulation.
- </p>
- <h4>References</h4>
- <p>
- Bower, William B. <i>A primer in fluid mechanics: Dynamics of flows in one
- space dimension</i>. CRC Press. 1998.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 26, 2018, by Filip Jorissen and Michael Wetter:<br/>
- Now printing different messages if temperature is above or below its limit,
- and adding instance name as JModelica does not print the full instance name in the assertion.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1045\">#1045</a>.
- </li>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- November 13, 2014, by Michael Wetter:<br/>
- Removed <code>phi</code> and removed non-required computations.
- </li>
- <li>
- March 29, 2013, by Michael Wetter:<br/>
- Added <code>final standardOrderComponents=true</code> in the
- <code>BaseProperties</code> declaration. This avoids an error
- when models are checked in Dymola 2014 in the pedenatic mode.
- </li>
- <li>
- April 12, 2012, by Michael Wetter:<br/>
- Added keyword <code>each</code> to <code>Xi(stateSelect=...)</code>.
- </li>
- <li>
- April 4, 2012, by Michael Wetter:<br/>
- Added redeclaration of <code>ThermodynamicState</code> to avoid a warning
- during model check and translation.
- </li>
- <li>
- January 27, 2010, by Michael Wetter:<br/>
- Added function <code>enthalpyOfNonCondensingGas</code> and its derivative.
- </li>
- <li>
- January 27, 2010, by Michael Wetter:<br/>
- Fixed bug with temperature offset in <code>T_phX</code>.
- </li>
- <li>
- August 18, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This package contains a <i>thermally perfect</i> model of moist air.
+</p>
+<p>
+A medium is called thermally perfect if
+</p>
+<ul>
+<li>
+it is in thermodynamic equilibrium,
+</li><li>
+it is chemically not reacting, and
+</li><li>
+internal energy and enthalpy are functions of temperature only.
+</li>
+</ul>
+<p>
+In addition, this medium model is <i>calorically perfect</i>, i.e., the
+specific heat capacities at constant pressure <i>c<sub>p</sub></i>
+and constant volume <i>c<sub>v</sub></i> are both constant (Bower 1998).
+</p>
+<p>
+This medium uses the ideal gas law
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&rho; = p &frasl;(R T),
+</p>
+<p>
+where
+<i>&rho;</i> is the density,
+<i>p</i> is the pressure,
+<i>R</i> is the gas constant and
+<i>T</i> is the temperature.
+</p>
+<p>
+The enthalpy is computed using the convention that <i>h=0</i>
+if <i>T=0</i> &deg;C and no water vapor is present.
+</p>
+<p>
+Note that for typical building simulations, the media
+<a href=\"modelica://AixLib.Media.Air\">AixLib.Media.Air</a>
+should be used as it leads generally to faster simulation.
+</p>
+<h4>References</h4>
+<p>
+Bower, William B. <i>A primer in fluid mechanics: Dynamics of flows in one
+space dimension</i>. CRC Press. 1998.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 9, 2022, by Michael Wetter:<br/>
+Set nominal attribute for <code>BaseProperties.Xi</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1634\">#1634</a>.
+</li>
+<li>
+October 26, 2018, by Filip Jorissen and Michael Wetter:<br/>
+Now printing different messages if temperature is above or below its limit,
+and adding instance name as JModelica does not print the full instance name in the assertion.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1045\">#1045</a>.
+</li>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+November 13, 2014, by Michael Wetter:<br/>
+Removed <code>phi</code> and removed non-required computations.
+</li>
+<li>
+March 29, 2013, by Michael Wetter:<br/>
+Added <code>final standardOrderComponents=true</code> in the
+<code>BaseProperties</code> declaration. This avoids an error
+when models are checked in Dymola 2014 in the pedenatic mode.
+</li>
+<li>
+April 12, 2012, by Michael Wetter:<br/>
+Added keyword <code>each</code> to <code>Xi(stateSelect=...)</code>.
+</li>
+<li>
+April 4, 2012, by Michael Wetter:<br/>
+Added redeclaration of <code>ThermodynamicState</code> to avoid a warning
+during model check and translation.
+</li>
+<li>
+January 27, 2010, by Michael Wetter:<br/>
+Added function <code>enthalpyOfNonCondensingGas</code> and its derivative.
+</li>
+<li>
+January 27, 2010, by Michael Wetter:<br/>
+Fixed bug with temperature offset in <code>T_phX</code>.
+</li>
+<li>
+August 18, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Ellipse(
           extent={{-78,78},{-34,34}},
@@ -713,6 +721,6 @@ protected
           extent={{-90,-6},{-46,-50}},
           lineColor={0,0,0},
           fillPattern=FillPattern.Sphere,
-          fillColor={120,120,120})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={120,120,120})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end PerfectGas;
diff --git a/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityDerivativeCheck.mo b/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityDerivativeCheck.mo
index 3e6c7c8245..f34c1d6d06 100644
--- a/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityDerivativeCheck.mo
+++ b/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityDerivativeCheck.mo
@@ -49,24 +49,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Specialized/Water/Examples/TemperatureDependentDensityDerivativeCheck.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- August 17, 2015, by Michael Wetter:<br/>
- Changed regression test to have slope different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+August 17, 2015, by Michael Wetter:<br/>
+Changed regression test to have slope different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureDependentDensityDerivativeCheck;
diff --git a/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityProperties.mo b/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityProperties.mo
index 3d2eecf710..b65d1fd25d 100644
--- a/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityProperties.mo
+++ b/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityProperties.mo
@@ -15,17 +15,17 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Specialized/Water/Examples/TemperatureDependentDensityProperties.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks thermophysical properties of the medium.
- </p>
- </html>",
+<p>
+This example checks thermophysical properties of the medium.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 19, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 19, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureDependentDensityProperties;
diff --git a/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityTemperatureEnthalpyInversion.mo b/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityTemperatureEnthalpyInversion.mo
index cb2671461d..9720c14741 100644
--- a/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityTemperatureEnthalpyInversion.mo
+++ b/AixLib/Media/Specialized/Water/Examples/TemperatureDependentDensityTemperatureEnthalpyInversion.mo
@@ -10,18 +10,18 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Specialized/Water/Examples/TemperatureDependentDensityTemperatureEnthalpyInversion.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests whether the inversion of temperature and enthalpy
- is implemented correctly.
- If <i>T &ne; T(h(T))</i>, the model stops with an error.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 21, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests whether the inversion of temperature and enthalpy
+is implemented correctly.
+If <i>T &ne; T(h(T))</i>, the model stops with an error.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 21, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureDependentDensityTemperatureEnthalpyInversion;
diff --git a/AixLib/Media/Specialized/Water/Examples/WaterProperties_pT.mo b/AixLib/Media/Specialized/Water/Examples/WaterProperties_pT.mo
index 46afca52f3..070eeea24f 100644
--- a/AixLib/Media/Specialized/Water/Examples/WaterProperties_pT.mo
+++ b/AixLib/Media/Specialized/Water/Examples/WaterProperties_pT.mo
@@ -17,19 +17,19 @@ equation
    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Media/Specialized/Water/Examples/WaterProperties_pT.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This example checks the thermophysical properties of the medium
- <a href=\"modelica://AixLib.Media.Specialized.Water.Examples.WaterProperties_pT\">
- AixLib.Media.Specialized.Water.Examples.WaterProperties_pT</a>.
- </p>
- </html>",
+<p>
+This example checks the thermophysical properties of the medium
+<a href=\"modelica://AixLib.Media.Specialized.Water.Examples.WaterProperties_pT\">
+AixLib.Media.Specialized.Water.Examples.WaterProperties_pT</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 12, 2016, by Marcus Fuchs:<br/>
- First implementation
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 12, 2016, by Marcus Fuchs:<br/>
+First implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterProperties_pT;
diff --git a/AixLib/Media/Specialized/Water/TemperatureDependentDensity.mo b/AixLib/Media/Specialized/Water/TemperatureDependentDensity.mo
index 4d871622cc..b7f883c80f 100644
--- a/AixLib/Media/Specialized/Water/TemperatureDependentDensity.mo
+++ b/AixLib/Media/Specialized/Water/TemperatureDependentDensity.mo
@@ -38,10 +38,10 @@ package TemperatureDependentDensity
     R_s = 0;
     MM=MM_const;
     annotation(Documentation(info="<html>
-     <p>
-     Base properties of the medium.
-     </p>
- </html>"));
+    <p>
+    Base properties of the medium.
+    </p>
+</html>"));
   end BaseProperties;
 
 redeclare function extends density "Return the density"
@@ -58,34 +58,34 @@ algorithm
   smoothOrder=1,
   Inline=true,
 Documentation(info="<html>
- <p>
- This function computes the density as a function of temperature.
- </p>
- <h4>Implementation</h4>
- <p>
- The function is based on the IDA implementation in <code>therpro.nmf</code>, which
- implements
- </p>
- <pre>
- d := 1000.12 + 1.43711e-2*T_degC -
-  5.83576e-3*T_degC^2 + 1.5009e-5*T_degC^3;
-  </pre>
- <p>
- This has been converted to Kelvin, which resulted in the above expression.
- In addition, below 5 &deg;C and above 100 &deg;C, the density is replaced
- by a linear function to avoid inflection points.
- This linear extension is such that the density is once continuously differentiable.
- </p>
- </html>",
+<p>
+This function computes the density as a function of temperature.
+</p>
+<h4>Implementation</h4>
+<p>
+The function is based on the IDA implementation in <code>therpro.nmf</code>, which
+implements
+</p>
+<pre>
+d := 1000.12 + 1.43711e-2*T_degC -
+ 5.83576e-3*T_degC^2 + 1.5009e-5*T_degC^3;
+ </pre>
+<p>
+This has been converted to Kelvin, which resulted in the above expression.
+In addition, below 5 &deg;C and above 100 &deg;C, the density is replaced
+by a linear function to avoid inflection points.
+This linear extension is such that the density is once continuously differentiable.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation, based on the IDA implementation in <code>therpro.nmf</code>,
- but converted from Celsius to Kelvin and linearly extended.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation, based on the IDA implementation in <code>therpro.nmf</code>,
+but converted from Celsius to Kelvin and linearly extended.
+</li>
+</ul>
+</html>"));
 end density;
 
 redeclare function extends dynamicViscosity "Return the dynamic viscosity"
@@ -94,18 +94,18 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function computes the dynamic viscosity.
- </p>
- </html>",
+<p>
+This function computes the dynamic viscosity.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 2, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 2, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end dynamicViscosity;
 
 redeclare function extends specificEnthalpy "Return the specific enthalpy"
@@ -115,18 +115,18 @@ annotation (
   smoothOrder=5,
   Inline=true,
   Documentation(info="<html>
- <p>
- This function computes the specific enthalpy.
- </p>
- </html>",
+<p>
+This function computes the specific enthalpy.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificEnthalpy;
 
 function enthalpyOfLiquid "Return the specific enthalpy of liquid"
@@ -140,18 +140,18 @@ algorithm
     Inline=true,
     derivative=der_enthalpyOfLiquid,
 Documentation(info="<html>
- <p>
- This function computes the specific enthalpy of liquid water.
- </p>
- </html>",
+<p>
+This function computes the specific enthalpy of liquid water.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 2, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 2, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end enthalpyOfLiquid;
 
 redeclare function extends specificInternalEnergy
@@ -162,18 +162,18 @@ annotation (
   smoothOrder=5,
   Inline=true,
   Documentation(info="<html>
- <p>
- This function computes the specific internal energy.
- </p>
- </html>",
+<p>
+This function computes the specific internal energy.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificInternalEnergy;
 
 redeclare function extends specificEntropy "Return the specific entropy"
@@ -183,23 +183,23 @@ algorithm
   annotation (
     Inline=true,
     Documentation(info="<html>
- <p>
- This function computes the specific entropy.
- </p>
- <p>
- To obtain the state for a given pressure, entropy and mass fraction, use
- <a href=\"modelica://AixLib.Media.Air.setState_psX\">
- AixLib.Media.Air.setState_psX</a>.
- </p>
- </html>",
+<p>
+This function computes the specific entropy.
+</p>
+<p>
+To obtain the state for a given pressure, entropy and mass fraction, use
+<a href=\"modelica://AixLib.Media.Air.setState_psX\">
+AixLib.Media.Air.setState_psX</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificEntropy;
 
 redeclare function extends specificGibbsEnergy
@@ -210,18 +210,18 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function computes the specific Gibbs energy.
- </p>
- </html>",
+<p>
+This function computes the specific Gibbs energy.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 2, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 2, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificGibbsEnergy;
 
 redeclare function extends specificHelmholtzEnergy
@@ -232,18 +232,18 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function computes the specific Helmholtz energy.
- </p>
- </html>",
+<p>
+This function computes the specific Helmholtz energy.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 2, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 2, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificHelmholtzEnergy;
 
 redeclare function extends isentropicEnthalpy "Return the isentropic enthalpy"
@@ -255,21 +255,21 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function computes the specific enthalpy for
- an isentropic state change from the temperature
- that corresponds to the state <code>refState</code>
- to <code>reference_T</code>.
- </p>
- </html>",
+<p>
+This function computes the specific enthalpy for
+an isentropic state change from the temperature
+that corresponds to the state <code>refState</code>
+to <code>reference_T</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end isentropicEnthalpy;
 
 redeclare function extends isobaricExpansionCoefficient
@@ -292,27 +292,27 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function returns the isobaric expansion coefficient,
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &beta;<sub>p</sub> = - 1 &frasl; v &nbsp; (&part; v &frasl; &part; T)<sub>p</sub>,
- </p>
- <p>
- where
- <i>v</i> is the specific volume,
- <i>T</i> is the temperature and
- <i>p</i> is the pressure.
- </p>
- </html>",
+<p>
+This function returns the isobaric expansion coefficient,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&beta;<sub>p</sub> = - 1 &frasl; v &nbsp; (&part; v &frasl; &part; T)<sub>p</sub>,
+</p>
+<p>
+where
+<i>v</i> is the specific volume,
+<i>T</i> is the temperature and
+<i>p</i> is the pressure.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end isobaricExpansionCoefficient;
 
 redeclare function extends isothermalCompressibility
@@ -322,29 +322,29 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function returns the isothermal compressibility coefficient,
- which is zero as this medium is incompressible.
- The isothermal compressibility is defined as
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
- &kappa;<sub>T</sub> = - 1 &frasl; v &nbsp; (&part; v &frasl; &part; p)<sub>T</sub>,
- </p>
- <p>
- where
- <i>v</i> is the specific volume,
- <i>T</i> is the temperature and
- <i>p</i> is the pressure.
- </p>
- </html>",
+<p>
+This function returns the isothermal compressibility coefficient,
+which is zero as this medium is incompressible.
+The isothermal compressibility is defined as
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&kappa;<sub>T</sub> = - 1 &frasl; v &nbsp; (&part; v &frasl; &part; p)<sub>T</sub>,
+</p>
+<p>
+where
+<i>v</i> is the specific volume,
+<i>T</i> is the temperature and
+<i>p</i> is the pressure.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end isothermalCompressibility;
 
 redeclare function extends density_derp_T
@@ -354,20 +354,20 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function returns the partial derivative of density
- with respect to pressure at constant temperature,
- which is zero as the medium is incompressible.
- </p>
- </html>",
+<p>
+This function returns the partial derivative of density
+with respect to pressure at constant temperature,
+which is zero as the medium is incompressible.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end density_derp_T;
 
 redeclare function extends density_derT_p
@@ -385,26 +385,26 @@ algorithm
   Inline=true,
   Documentation(info=
                    "<html>
- <p>
- This function computes the derivative of density with respect to temperature
- at constant pressure.
- </p>
- </html>",revisions=
+<p>
+This function computes the derivative of density with respect to temperature
+at constant pressure.
+</p>
+</html>", revisions=
 "<html>
- <ul>
- <li>
- August 17, 2015, by Michael Wetter:<br/>
- Removed dublicate entry of <code>smooth</code> and <code>smoothOrder</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation, based on the IDA implementation in <code>therpro.nmf</code>,
- but converted from Celsius to Kelvin.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+August 17, 2015, by Michael Wetter:<br/>
+Removed dublicate entry of <code>smooth</code> and <code>smoothOrder</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation, based on the IDA implementation in <code>therpro.nmf</code>,
+but converted from Celsius to Kelvin.
+</li>
+</ul>
+</html>"));
 end density_derT_p;
 
 redeclare function extends density_derX
@@ -414,20 +414,20 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function returns the partial derivative of density
- with respect to mass fraction,
- which is zero as the medium is a single substance.
- </p>
- </html>",
+<p>
+This function returns the partial derivative of density
+with respect to mass fraction,
+which is zero as the medium is a single substance.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end density_derX;
 
 redeclare replaceable function extends specificHeatCapacityCp
@@ -438,18 +438,18 @@ algorithm
     Inline=true,
     derivative=der_specificHeatCapacityCp,
 Documentation(info="<html>
- <p>
- This function returns the specific heat capacity at constant pressure.
- </p>
- </html>",
+<p>
+This function returns the specific heat capacity at constant pressure.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificHeatCapacityCp;
 
 redeclare replaceable function extends specificHeatCapacityCv
@@ -460,18 +460,18 @@ algorithm
     Inline=true,
     derivative=der_specificHeatCapacityCp,
 Documentation(info="<html>
- <p>
- This function computes the specific heat capacity at constant volume.
- </p>
- </html>",
+<p>
+This function computes the specific heat capacity at constant volume.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificHeatCapacityCv;
 
 redeclare function extends thermalConductivity
@@ -481,27 +481,27 @@ algorithm
   annotation (
     Inline=true,
     Documentation(info="<html>
- <p>
- This function returns the thermal conductivity.
- The expression is obtained from Ramires et al. (1995).
- </p>
- <h4>References</h4>
- <p>
- Ramires, Maria L. V. and Nieto de Castro, Carlos A. and Nagasaka, Yuchi
- and Nagashima, Akira and Assael, Marc J. and Wakeham, William A.
- Standard Reference Data for the Thermal Conductivity of Water.
- <i>Journal of Physical and Chemical Reference Data</i>, 24, p. 1377-1381, 1995.
- <a href=\"http://dx.doi.org/10.1063/1.555963\">DOI:10.1063/1.555963</a>.
- </p>
- </html>",
+<p>
+This function returns the thermal conductivity.
+The expression is obtained from Ramires et al. (1995).
+</p>
+<h4>References</h4>
+<p>
+Ramires, Maria L. V. and Nieto de Castro, Carlos A. and Nagasaka, Yuchi
+and Nagashima, Akira and Assael, Marc J. and Wakeham, William A.
+Standard Reference Data for the Thermal Conductivity of Water.
+<i>Journal of Physical and Chemical Reference Data</i>, 24, p. 1377-1381, 1995.
+<a href=\"http://dx.doi.org/10.1063/1.555963\">DOI:10.1063/1.555963</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end thermalConductivity;
 
 redeclare function extends pressure "Return the pressure"
@@ -511,18 +511,18 @@ annotation (
   Inline=true,
   smoothOrder=99,
 Documentation(info="<html>
- <p>
- This function returns the pressure.
- </p>
- </html>",
+<p>
+This function returns the pressure.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end pressure;
 
 redeclare function extends temperature "Return the temperature"
@@ -532,18 +532,18 @@ annotation (
   Inline=true,
   smoothOrder=99,
 Documentation(info="<html>
- <p>
- This function returns the temperature.
- </p>
- </html>",
+<p>
+This function returns the temperature.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end temperature;
 
 redeclare function extends molarMass "Return the molar mass"
@@ -553,19 +553,19 @@ algorithm
     Inline=true,
     smoothOrder=99,
     Documentation(info="<html>
- <p>
- This function returns the molar mass,
- which is assumed to be constant.
- </p>
- </html>",
+<p>
+This function returns the molar mass,
+which is assumed to be constant.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end molarMass;
 
 redeclare function setState_dTX
@@ -588,19 +588,19 @@ algorithm
     Inline=true,
     smoothOrder=99,
     Documentation(info="<html>
- <p>
- This function returns the thermodynamic state for a given pressure,
- specific enthalpy and composition.
- </p>
- </html>",
+<p>
+This function returns the thermodynamic state for a given pressure,
+specific enthalpy and composition.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end setState_phX;
 
 redeclare function extends setState_pTX
@@ -611,19 +611,19 @@ annotation (
   smoothOrder=99,
   Inline=true,
   Documentation(info="<html>
- <p>
- This function returns the thermodynamic state for a given pressure,
- temperature and composition.
- </p>
- </html>",
+<p>
+This function returns the thermodynamic state for a given pressure,
+temperature and composition.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end setState_pTX;
 
 redeclare function extends setState_psX
@@ -636,29 +636,29 @@ algorithm
   annotation (
     Inline=true,
     Documentation(info="<html>
- <p>
- This function returns the thermodynamic state based on pressure,
- specific entropy and mass fraction.
- </p>
- <p>
- The state is computed by symbolically solving
- <a href=\"modelica://AixLib.Media.Specialized.Water.TemperatureDependentDensity.specificEntropy\">
- AixLib.Media.Specialized.Water.TemperatureDependentDensity.specificEntropy</a>
- for temperature.
-   </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+This function returns the thermodynamic state based on pressure,
+specific entropy and mass fraction.
+</p>
+<p>
+The state is computed by symbolically solving
+<a href=\"modelica://AixLib.Media.Specialized.Water.TemperatureDependentDensity.specificEntropy\">
+AixLib.Media.Specialized.Water.TemperatureDependentDensity.specificEntropy</a>
+for temperature.
+  </p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end setState_psX;
 //////////////////////////////////////////////////////////////////////
 // Protected classes.
@@ -686,19 +686,19 @@ algorithm
 annotation (
   Inline=true,
   Documentation(info="<html>
- <p>
- This function computes the derivative of the specific heat capacity
- at constant pressure with respect to the state.
- </p>
- </html>",
+<p>
+This function computes the derivative of the specific heat capacity
+at constant pressure with respect to the state.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end der_specificHeatCapacityCp;
 
 replaceable function der_enthalpyOfLiquid
@@ -713,19 +713,19 @@ annotation (
   Inline=true,
   Documentation(info=
 "<html>
- <p>
- This function computes the temperature derivative of the enthalpy of liquid water
- per unit mass.
- </p>
- </html>",revisions=
+<p>
+This function computes the temperature derivative of the enthalpy of liquid water
+per unit mass.
+</p>
+</html>", revisions=
 "<html>
- <ul>
- <li>
- December 11, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 11, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end der_enthalpyOfLiquid;
 
 function kinematicViscosity "Return the kinematic viscosity"
@@ -746,181 +746,181 @@ annotation (
   Inline=true,
   smoothOrder=1,
   Documentation(info="<html>
- <p>
- This function computes the kinematic viscosity as a function of temperature.
- </p>
- <h4>Implementation</h4>
- <p>
- The function is based on the IDA implementation in <code>therpro.nmf</code>.
- The original equation is
- </p>
- <pre>
- kinVis :=1E-6*Modelica.Math.exp(0.577449 - 3.253945e-2*T_degC + 2.17369e-4*
-       T_degC^2 - 7.22111e-7*T_degC^3);
-       </pre>
- <p>
- This has been converted to Kelvin, which resulted in the above expression.
- In addition, at 5 &deg;C the kinematic viscosity is linearly extrapolated
- to avoid a large gradient at very low temperatures.
- We selected the same point for the linearization as we used for the density,
- as the density and the kinematic viscosity are combined in
- <a href=\"modelica://AixLib.Media.Specialized.Water.TemperatureDependentDensity.dynamicViscosity\">
- AixLib.Media.Specialized.Water.TemperatureDependentDensity.dynamicViscosity</a>.
- </p>
- </html>",
+<p>
+This function computes the kinematic viscosity as a function of temperature.
+</p>
+<h4>Implementation</h4>
+<p>
+The function is based on the IDA implementation in <code>therpro.nmf</code>.
+The original equation is
+</p>
+<pre>
+kinVis :=1E-6*Modelica.Math.exp(0.577449 - 3.253945e-2*T_degC + 2.17369e-4*
+      T_degC^2 - 7.22111e-7*T_degC^3);
+      </pre>
+<p>
+This has been converted to Kelvin, which resulted in the above expression.
+In addition, at 5 &deg;C the kinematic viscosity is linearly extrapolated
+to avoid a large gradient at very low temperatures.
+We selected the same point for the linearization as we used for the density,
+as the density and the kinematic viscosity are combined in
+<a href=\"modelica://AixLib.Media.Specialized.Water.TemperatureDependentDensity.dynamicViscosity\">
+AixLib.Media.Specialized.Water.TemperatureDependentDensity.dynamicViscosity</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation, based on the IDA implementation in <code>therpro.nmf</code>,
- but converted from Celsius to Kelvin.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation, based on the IDA implementation in <code>therpro.nmf</code>,
+but converted from Celsius to Kelvin.
+</li>
+</ul>
+</html>"));
 end kinematicViscosity;
 annotation(preferredView="info", Documentation(info="<html>
- <p>
- This medium package models liquid water.
- </p>
- <p>
- The mass density is computed using a 3rd order polynomial, which yields the
- density as a function of temperature as shown in the figure below. Note, however,
- that computing density as a function of temperature can lead to considerably
- slower computing time compared to using
- <a href=\"modelica://AixLib.Media.Water\">
- AixLib.Media.Water</a>
- in which the density is a constant. We therefore recommend to use
- <a href=\"modelica://AixLib.Media.Water\">
- AixLib.Media.Water</a>
- for typical building energy simulations.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Water/plotRho.png\" border=\"1\"
- alt=\"Mass density as a function of temperature\"/>
- </p>
- <p>
- For the specific heat capacities at constant pressure and at constant volume,
- a constant value of <i>4184</i> J/(kg K), which corresponds to <i>20</i>&deg;C
- is used.
- The figure below shows the relative error of the specific heat capacity that
- is introduced by this simplification.
- Using a constant value for the specific heat capacity allows to compute
- temperature from enthalpy without having to solve an implicit equation,
- and therefore leads to faster simulation.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Water/plotCp.png\" border=\"1\"
- alt=\"Relative variation of specific heat capacity with temperature\"/>
- </p>
- 
- 
- <p>
- Thermal conductivity is calculated as a function of temperature as shown in the figure below.
- The correlation used to calculate the thermal conductivity is
- </p>
- 
- <p align=\"center\" style=\"font-style:italic;\">
- &lambda;(T) = &lambda;(298.15 K) &sdot; (-1.48445+4.12292&sdot;(T/298.15)-1.63866&sdot;(T/298.15)<sup>2</sup>),
- </p>
- <p>
- where <i>&lambda;(298.15 K) = 0.6065</i>  W/(m &sdot; K) is the adopted standard value
- of the thermal conductivity of water at <i>298.15</i> K and <i>0.1</i> MPa.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Water/plotLambda.png\" border=\"1\"
- alt=\"Thermal conductivity as a function of temperature\"/>
- </p>
- 
- <p>
- Dynamic viscosity is calculated as the product of density and kinematic viscosity,
- both temperature dependent. However, the kinematic viscosity
- has its own temperature dependent correlation, implemented at
- <a href=\"modelica://AixLib.Media.Specialized.Water.TemperatureDependentDensity.kinematicViscosity\">
- AixLib.Media.Specialized.Water.TemperatureDependentDensity.kinematicViscosity</a>.
- Results of the kinematic viscosity as a function of temperature are shown in the figure below.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Water/plotkinVis.png\" border=\"1\"
- alt=\"Kinematic viscosity as a function of temperature\"/>
- </p>
- 
- <p>
- The enthalpy is computed using the convention that <i>h=0</i>
- if <i>T=0</i> &deg;C.
- </p>
- <h4>Limitations</h4>
- <p>
- Phase changes are not modeled.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 5, 2022, by Michael Wetter:<br/>
- Corrected assignment of <code>R_s</code> in <code>BaseProperties</code> to avoid a unit error.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1603\">#1603</a>.
- </li>
- <li>
- July 7, 2016, by Carles Ribas Tugores:<br/>
- Correct Documentation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/487\">#487</a>.
- </li>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Set <code>AbsolutePressure(start=p_default)</code>
- and <code>Temperature(start=T_default)</code>
- to have to have conistent start values.
- See also revision notes of
- <a href=\"modelica://AixLib.Media.Water\">
- AixLib.Media.Water</a>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- May 1, 2015, by Michael Wetter:<br/>
- Added <code>Inline=true</code> for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
- issue 227</a>.
- </li>
- <li>
- February 25, 2015, by Michael Wetter:<br/>
- Removed <code>stateSelect</code> attribute on pressure as this caused
- <a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
- AixLib.Examples.Tutorial.SpaceCooling.System3</a>
- to fail with the error message
- \"differentiated if-then-else was not continuous\".
- </li>
- <li>
- February 3, 2015, by Michael Wetter:<br/>
- Removed <code>stateSelect.prefer</code> for temperature.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/160\">#160</a>.
- </li>
- <li>
- October 15, 2014, by Michael Wetter:<br/>
- Renamed from <code>AixLib.Media.Water</code> to
- <code>AixLib.Media.Water.Detailed</code> to allow addition of
- <code>AixLib.Media.Water.Simple</code>.
- </li>
- <li>
- September 12, 2014, by Michael Wetter:<br/>
- Set <code>T(start=T_default)</code> and <code>p(start=p_default)</code> in the
- <code>ThermodynamicState</code> record. Setting the start value for
- <code>T</code> is required to avoid an error due to conflicting start values
- when checking <a href=\"modelica://AixLib.Examples.VAVReheat.ClosedLoop\">
- AixLib.Examples.VAVReheat.ClosedLoop</a> in pedantic mode.
- </li>
- <li>
- December 18, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This medium package models liquid water.
+</p>
+<p>
+The mass density is computed using a 3rd order polynomial, which yields the
+density as a function of temperature as shown in the figure below. Note, however,
+that computing density as a function of temperature can lead to considerably
+slower computing time compared to using
+<a href=\"modelica://AixLib.Media.Water\">
+AixLib.Media.Water</a>
+in which the density is a constant. We therefore recommend to use
+<a href=\"modelica://AixLib.Media.Water\">
+AixLib.Media.Water</a>
+for typical building energy simulations.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Water/plotRho.png\" border=\"1\"
+alt=\"Mass density as a function of temperature\"/>
+</p>
+<p>
+For the specific heat capacities at constant pressure and at constant volume,
+a constant value of <i>4184</i> J/(kg K), which corresponds to <i>20</i>&deg;C
+is used.
+The figure below shows the relative error of the specific heat capacity that
+is introduced by this simplification.
+Using a constant value for the specific heat capacity allows to compute
+temperature from enthalpy without having to solve an implicit equation,
+and therefore leads to faster simulation.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Water/plotCp.png\" border=\"1\"
+alt=\"Relative variation of specific heat capacity with temperature\"/>
+</p>
+
+
+<p>
+Thermal conductivity is calculated as a function of temperature as shown in the figure below.
+The correlation used to calculate the thermal conductivity is
+</p>
+
+<p align=\"center\" style=\"font-style:italic;\">
+&lambda;(T) = &lambda;(298.15 K) &sdot; (-1.48445+4.12292&sdot;(T/298.15)-1.63866&sdot;(T/298.15)<sup>2</sup>),
+</p>
+<p>
+where <i>&lambda;(298.15 K) = 0.6065</i>  W/(m &sdot; K) is the adopted standard value
+of the thermal conductivity of water at <i>298.15</i> K and <i>0.1</i> MPa.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Water/plotLambda.png\" border=\"1\"
+alt=\"Thermal conductivity as a function of temperature\"/>
+</p>
+
+<p>
+Dynamic viscosity is calculated as the product of density and kinematic viscosity,
+both temperature dependent. However, the kinematic viscosity
+has its own temperature dependent correlation, implemented at
+<a href=\"modelica://AixLib.Media.Specialized.Water.TemperatureDependentDensity.kinematicViscosity\">
+AixLib.Media.Specialized.Water.TemperatureDependentDensity.kinematicViscosity</a>.
+Results of the kinematic viscosity as a function of temperature are shown in the figure below.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Water/plotkinVis.png\" border=\"1\"
+alt=\"Kinematic viscosity as a function of temperature\"/>
+</p>
+
+<p>
+The enthalpy is computed using the convention that <i>h=0</i>
+if <i>T=0</i> &deg;C.
+</p>
+<h4>Limitations</h4>
+<p>
+Phase changes are not modeled.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 5, 2022, by Michael Wetter:<br/>
+Corrected assignment of <code>R_s</code> in <code>BaseProperties</code> to avoid a unit error.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1603\">#1603</a>.
+</li>
+<li>
+July 7, 2016, by Carles Ribas Tugores:<br/>
+Correct Documentation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/487\">#487</a>.
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Set <code>AbsolutePressure(start=p_default)</code>
+and <code>Temperature(start=T_default)</code>
+to have to have conistent start values.
+See also revision notes of
+<a href=\"modelica://AixLib.Media.Water\">
+AixLib.Media.Water</a>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+May 1, 2015, by Michael Wetter:<br/>
+Added <code>Inline=true</code> for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
+issue 227</a>.
+</li>
+<li>
+February 25, 2015, by Michael Wetter:<br/>
+Removed <code>stateSelect</code> attribute on pressure as this caused
+<a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
+AixLib.Examples.Tutorial.SpaceCooling.System3</a>
+to fail with the error message
+\"differentiated if-then-else was not continuous\".
+</li>
+<li>
+February 3, 2015, by Michael Wetter:<br/>
+Removed <code>stateSelect.prefer</code> for temperature.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/160\">#160</a>.
+</li>
+<li>
+October 15, 2014, by Michael Wetter:<br/>
+Renamed from <code>AixLib.Media.Water</code> to
+<code>AixLib.Media.Water.Detailed</code> to allow addition of
+<code>AixLib.Media.Water.Simple</code>.
+</li>
+<li>
+September 12, 2014, by Michael Wetter:<br/>
+Set <code>T(start=T_default)</code> and <code>p(start=p_default)</code> in the
+<code>ThermodynamicState</code> record. Setting the start value for
+<code>T</code> is required to avoid an error due to conflicting start values
+when checking <a href=\"modelica://AixLib.Examples.VAVReheat.ClosedLoop\">
+AixLib.Examples.VAVReheat.ClosedLoop</a> in pedantic mode.
+</li>
+<li>
+December 18, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}),
         graphics={
@@ -952,6 +952,6 @@ annotation(preferredView="info", Documentation(info="<html>
         Text(
           extent={{-64,88},{-42,58}},
           textColor={255,0,0},
-          textString="T")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="T")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TemperatureDependentDensity;
diff --git a/AixLib/Media/Steam.mo b/AixLib/Media/Steam.mo
index 10c85d6c56..8df8f22301 100644
--- a/AixLib/Media/Steam.mo
+++ b/AixLib/Media/Steam.mo
@@ -8,6 +8,7 @@ package Steam
     reducedX=true,
     fixedX=true,
     FluidConstants={Modelica.Media.IdealGases.Common.FluidData.H2O},
+    ThermoStates=Modelica.Media.Interfaces.Choices.IndependentVariables.pTX,
     reference_T=273.15,
     reference_p=101325,
     reference_X={1},
@@ -44,11 +45,11 @@ redeclare replaceable function extends density
 algorithm
   d := rho_pT(state.p, state.T);
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Density is computed from temperature and pressure using the
- IAPWS-IF97 relationship via the Gibbs free energy for region 2.
- </p>
- </html>"));
+<p>
+Density is computed from temperature and pressure using the
+IAPWS-IF97 relationship via the Gibbs free energy for region 2.
+</p>
+</html>"));
 end density;
 
 redeclare replaceable function extends dynamicViscosity
@@ -59,11 +60,11 @@ algorithm
           T=state.T,
           p=state.p);
     annotation (Inline=true, Documentation(info="<html>
- <p>
- Dynamic viscosity is computed from density, temperature and pressure
- using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Dynamic viscosity is computed from density, temperature and pressure
+using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end dynamicViscosity;
 
 redeclare replaceable function extends molarMass
@@ -71,10 +72,10 @@ redeclare replaceable function extends molarMass
 algorithm
   MM := steam.MM;
     annotation (Documentation(info="<html>
- <p>
- Returns the molar mass.
- </p>
- </html>"));
+<p>
+Returns the molar mass.
+</p>
+</html>"));
 end molarMass;
 
 redeclare function extends pressure
@@ -82,10 +83,10 @@ redeclare function extends pressure
 algorithm
   p := state.p;
     annotation (Documentation(info="<html>
- <p>
- Pressure is returned from the thermodynamic state record input as a simple assignment.
- </p>
- </html>"));
+<p>
+Pressure is returned from the thermodynamic state record input as a simple assignment.
+</p>
+</html>"));
 end pressure;
 
 replaceable function saturationPressure
@@ -96,11 +97,11 @@ replaceable function saturationPressure
 algorithm
    psat := Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.psat(Tsat);
  annotation (Inline=true, Documentation(info="<html>
- <p>
- Saturation pressure is computed from temperature
- using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Saturation pressure is computed from temperature
+using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end saturationPressure;
 
 replaceable function saturationTemperature
@@ -110,11 +111,11 @@ replaceable function saturationTemperature
 algorithm
     Tsat := Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.tsat(psat);
     annotation (Inline=true, Documentation(info="<html>
- <p>
- Saturation temperature is computed from pressure
- using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Saturation temperature is computed from pressure
+using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end saturationTemperature;
 
 redeclare replaceable function extends specificEnthalpy
@@ -125,41 +126,41 @@ redeclare replaceable function extends specificEnthalpy
     constant Temperature TMean =  4.15555698340926E+02 "Mean temperature";
     constant Real pSD = 1.13236055019318E+05 "Normalization value";
     constant Real TSD = 1.32971013463839E+01 "Normalization value";
-    AbsolutePressure pHat;
-    Temperature THat;
+    Modelica.Units.SI.PressureDifference pHat;
+    Modelica.Units.SI.TemperatureDifference THat;
 algorithm
   pHat := (state.p - pMean)/pSD;
   THat := (state.T - TMean)/TSD;
   h := a[1] + a[2]*pHat + a[3]*THat;
 annotation (Inline=true,smoothOrder=2,
     Documentation(info="<html>
- <p>
- Returns the specific enthalpy.
- </p>
- <h4>Implementation</h4>
- <p>
- The function is based on
- <a href=\"modelica://Modelica.Media.Water.WaterIF97_base.specificEnthalpy_pT\">
- Modelica.Media.Water.WaterIF97_base.specificEnthalpy_pT</a>.
- However, for the typical range of temperatures and pressures
- encountered in building and district energy applications,
- a linear function sufficies. This implementation is therefore a linear
- surface fit of the IF97 formulation <i>h(p,T)</i> in the ranges of
- <i>100&deg;C &le; T &le; 160&deg;C</i> and
- <i>100 kPa &le; p &le; 550</i> kPa. The fit is scaled by the dataset's
- mean and standard deviation values to improve conditioning.
- The largest error of this linearization is  <i>2.42 kJ/kg</i> (<i>0.09</i>%),
- which occurs at <i>100.6&deg;C</i> and <i>100 kPa</i>.
- The root mean square error (RMSE) is <i>0.76 kJ/kg</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 30, 2020, by Kathryn Hinkelman:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Returns the specific enthalpy.
+</p>
+<h4>Implementation</h4>
+<p>
+The function is based on
+<a href=\"modelica://Modelica.Media.Water.WaterIF97_base.specificEnthalpy_pT\">
+Modelica.Media.Water.WaterIF97_base.specificEnthalpy_pT</a>.
+However, for the typical range of temperatures and pressures
+encountered in building and district energy applications,
+a linear function sufficies. This implementation is therefore a linear
+surface fit of the IF97 formulation <i>h(p,T)</i> in the ranges of
+<i>100&deg;C &le; T &le; 160&deg;C</i> and
+<i>100 kPa &le; p &le; 550</i> kPa. The fit is scaled by the dataset's
+mean and standard deviation values to improve conditioning.
+The largest error of this linearization is  <i>2.42 kJ/kg</i> (<i>0.09</i>%),
+which occurs at <i>100.6&deg;C</i> and <i>100 kPa</i>.
+The root mean square error (RMSE) is <i>0.76 kJ/kg</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 30, 2020, by Kathryn Hinkelman:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end specificEnthalpy;
 
 redeclare replaceable function extends specificEntropy
@@ -170,35 +171,35 @@ redeclare replaceable function extends specificEntropy
     constant Temperature TMean =  4.15555698340926E+02 "Mean temperature";
     constant Real pSD = 1.13236055019318E+05 "Normalization value";
     constant Real TSD = 1.32971013463839E+01 "Normalization value";
-    AbsolutePressure pHat;
-    Temperature THat;
+    Modelica.Units.SI.PressureDifference pHat;
+    Modelica.Units.SI.TemperatureDifference THat;
 algorithm
   pHat := (state.p - pMean)/pSD;
   THat := (state.T - TMean)/TSD;
   s := a[1] + a[2]*pHat + a[3]*THat + pHat*(a[4]*pHat + a[5]*THat);
 annotation (Inline=true,smoothOrder=2,
     Documentation(info="<html>
- <p>
- Returns the specific entropy.
- </p>
- <h4>Implementation</h4>
- <p>
- The function is based on
- <a href=\"modelica://Modelica.Media.Water.WaterIF97_base.specificEntropy\">
- Modelica.Media.Water.WaterIF97_base.specificEntropy</a>.
- However, for the typical range of temperatures and pressures
- encountered in building and district energy applications,
- an invertible polynomial fit sufficies. This implementation is therefore
- a polynomial fit (quadratic in pressure, linear in temperature) of the
- IF97 formulation <i>s(p,T)</i> in the ranges of
- <i>100&deg;C &le; T &le; 160&deg;C</i> and
- <i>100 kPa &le; p &le; 550 kPa</i>. The fit is scaled by the dataset's
- mean and standard deviation values to improve conditioning.
- The largest error of this approximation is <i>0.047 kJ/kg-K</i> (<i>0.70</i>%),
- which occurs at <i>160&deg;C</i> and <i>550 kPa</i>.
- The root mean square error (RMSE) is <i>12.56 J/kg-K</i>.
- </p>
- </html>"));
+<p>
+Returns the specific entropy.
+</p>
+<h4>Implementation</h4>
+<p>
+The function is based on
+<a href=\"modelica://Modelica.Media.Water.WaterIF97_base.specificEntropy\">
+Modelica.Media.Water.WaterIF97_base.specificEntropy</a>.
+However, for the typical range of temperatures and pressures
+encountered in building and district energy applications,
+an invertible polynomial fit sufficies. This implementation is therefore
+a polynomial fit (quadratic in pressure, linear in temperature) of the
+IF97 formulation <i>s(p,T)</i> in the ranges of
+<i>100&deg;C &le; T &le; 160&deg;C</i> and
+<i>100 kPa &le; p &le; 550 kPa</i>. The fit is scaled by the dataset's
+mean and standard deviation values to improve conditioning.
+The largest error of this approximation is <i>0.047 kJ/kg-K</i> (<i>0.70</i>%),
+which occurs at <i>160&deg;C</i> and <i>550 kPa</i>.
+The root mean square error (RMSE) is <i>12.56 J/kg-K</i>.
+</p>
+</html>"));
 end specificEntropy;
 
 redeclare replaceable function extends specificInternalEnergy
@@ -206,10 +207,10 @@ redeclare replaceable function extends specificInternalEnergy
 algorithm
   u := specificEnthalpy(state) - state.p/density(state);
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Returns the specific internal energy for a given state.
- </p>
- </html>"));
+<p>
+Returns the specific internal energy for a given state.
+</p>
+</html>"));
 end specificInternalEnergy;
 
 redeclare replaceable function extends specificHeatCapacityCp
@@ -228,12 +229,12 @@ algorithm
     smoothOrder=2,
     Inline=true,
       Documentation(info="<html>
- <p>
- Specific heat at constant pressure is computed from temperature and
- pressure using the IAPWS-IF97 relationship via the Gibbs
- free energy for region 2.
- </p>
- </html>"));
+<p>
+Specific heat at constant pressure is computed from temperature and
+pressure using the IAPWS-IF97 relationship via the Gibbs
+free energy for region 2.
+</p>
+</html>"));
 end specificHeatCapacityCp;
 
 redeclare replaceable function extends specificHeatCapacityCv
@@ -254,24 +255,24 @@ algorithm
     Inline=true,
     LateInline = true,
       Documentation(info="<html>
- <p>
- Specific heat at constant volume is computed from temperature and
- pressure using the IAPWS-IF97 relationship via the Gibbs
- free energy for region 2.
- </p>
- </html>",
+<p>
+Specific heat at constant volume is computed from temperature and
+pressure using the IAPWS-IF97 relationship via the Gibbs
+free energy for region 2.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 6, 2020, by Michael Wetter:<br/>
- Added <code>LateInline=true</code>.
- This is required for OCT-r17595_JM-r14295, otherwise
- <a href=\"modelica://AixLib.Media.Examples.SteamDerivativeCheck\">
- AixLib.Media.Examples.SteamDerivativeCheck</a>
- does not translate.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+December 6, 2020, by Michael Wetter:<br/>
+Added <code>LateInline=true</code>.
+This is required for OCT-r17595_JM-r14295, otherwise
+<a href=\"modelica://AixLib.Media.Examples.SteamDerivativeCheck\">
+AixLib.Media.Examples.SteamDerivativeCheck</a>
+does not translate.
+</li>
+</ul>
+</html>"));
 end specificHeatCapacityCv;
 
 redeclare replaceable function extends specificGibbsEnergy
@@ -286,10 +287,10 @@ redeclare replaceable function extends specificHelmholtzEnergy
 algorithm
   f := specificEnthalpy(state) - steam.R*state.T - state.T*specificEntropy(state);
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Returns the specific Helmholtz energy for a given state.
- </p>
- </html>"));
+<p>
+Returns the specific Helmholtz energy for a given state.
+</p>
+</html>"));
 end specificHelmholtzEnergy;
 
 redeclare replaceable function extends setState_dTX
@@ -298,11 +299,11 @@ algorithm
   state := ThermodynamicState(p=pressure_dT(d,T), T=T);
 annotation (Inline=true,
       Documentation(info="<html>
- <p>
- The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
- is computed from density <code>d</code> and temperature <code>T</code>.
- </p>
- </html>"));
+<p>
+The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
+is computed from density <code>d</code> and temperature <code>T</code>.
+</p>
+</html>"));
 end setState_dTX;
 
 redeclare replaceable function extends setState_pTX
@@ -311,11 +312,11 @@ algorithm
   state := ThermodynamicState(p=p, T=T);
 annotation (Inline=true,smoothOrder=2,
     Documentation(info="<html>
- <p>
- The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
- is computed from pressure <code>p</code> and temperature <code>T</code>.
- </p>
- </html>"));
+<p>
+The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
+is computed from pressure <code>p</code> and temperature <code>T</code>.
+</p>
+</html>"));
 end setState_pTX;
 
 redeclare replaceable function extends setState_phX
@@ -324,11 +325,11 @@ algorithm
   state := ThermodynamicState(p=p, T=temperature_ph(p,h));
 annotation (Inline=true,smoothOrder=2,
       Documentation(info="<html>
- <p>
- The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
- is computed from pressure <code>p</code> and specific enthalpy <code>h</code>.
- </p>
- </html>"));
+<p>
+The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
+is computed from pressure <code>p</code> and specific enthalpy <code>h</code>.
+</p>
+</html>"));
 end setState_phX;
 
 redeclare replaceable function extends setState_psX
@@ -337,11 +338,11 @@ algorithm
   state := ThermodynamicState(p=p, T=temperature_ps(p,s));
 annotation (Inline=true,smoothOrder=2,
     Documentation(info="<html>
- <p>
- The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
- is computed from pressure <code>p</code> and specific entropy <code>s</code>.
- </p>
- </html>"));
+<p>
+The <a href=\"modelica://Modelica.Media.Interfaces.PartialMixtureMedium.ThermodynamicState\">thermodynamic state record</a>
+is computed from pressure <code>p</code> and specific entropy <code>s</code>.
+</p>
+</html>"));
 end setState_psX;
 
 redeclare function extends temperature
@@ -349,10 +350,10 @@ redeclare function extends temperature
 algorithm
   T := state.T;
     annotation (Documentation(info="<html>
- <p>
- Temperature is returned from the thermodynamic state record input as a simple assignment.
- </p>
- </html>"));
+<p>
+Temperature is returned from the thermodynamic state record input as a simple assignment.
+</p>
+</html>"));
 end temperature;
 
 redeclare replaceable function extends thermalConductivity
@@ -363,11 +364,11 @@ algorithm
         state.T,
         state.p);
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Thermal conductivity is computed from density, temperature and pressure
- using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Thermal conductivity is computed from density, temperature and pressure
+using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end thermalConductivity;
 
 redeclare function extends density_derh_p
@@ -379,11 +380,11 @@ algorithm
         phase = 1,
         region = 2);
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Returns the partial derivative of density with respect
- to specific enthalpy at constant pressure using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Returns the partial derivative of density with respect
+to specific enthalpy at constant pressure using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end density_derh_p;
 
 redeclare function extends density_derp_h
@@ -395,11 +396,11 @@ algorithm
         phase = 1,
         region = 2);
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Returns the partial derivative of density with respect
- to pressure at constant specific enthalpy using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Returns the partial derivative of density with respect
+to pressure at constant specific enthalpy using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end density_derp_h;
 
 redeclare replaceable function extends isentropicExponent
@@ -410,11 +411,11 @@ algorithm
         T = state.T,
         region = 2);
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Isentropic exponent is computed from temperature and pressure
- using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Isentropic exponent is computed from temperature and pressure
+using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end isentropicExponent;
 
 redeclare replaceable function extends isothermalCompressibility
@@ -425,11 +426,11 @@ algorithm
         T = state.T,
         region = 2);
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Isothermal compressibility is computed from temperature and pressure
- using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Isothermal compressibility is computed from temperature and pressure
+using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end isothermalCompressibility;
 
 redeclare replaceable function extends isobaricExpansionCoefficient
@@ -440,11 +441,11 @@ algorithm
         T = state.T,
         region = 2);
     annotation (Documentation(info="<html>
- <p>
- Isobaric expansion coefficient is computed from temperature and
- pressure using the IAPWS-IF97 formulation.
- </p>
- </html>"));
+<p>
+Isobaric expansion coefficient is computed from temperature and
+pressure using the IAPWS-IF97 formulation.
+</p>
+</html>"));
 end isobaricExpansionCoefficient;
 
 redeclare replaceable function extends isentropicEnthalpy
@@ -455,17 +456,17 @@ algorithm
         s = specificEntropy(refState),
         phase = 0); // phase 0 means unknown
   annotation (Inline=true, Documentation(info="<html>
- <p>
- Isentropic enthalpy is computed using the IAPWS-IF97 formulation:
- </p>
- <ol>
- <li> A medium is in a particular state, <code>refState</code>.</li>
- <li> The enthalpy at another state <code>h_is</code> shall be computed
-      under the assumption that the state transformation from <code>refState</code> to <code>h_is</code>
-      is performed with a change of specific entropy <i>ds = 0</i> and the pressure of state <code>h_is</code>
-      is <code>p_downstream</code> and the composition <code>X</code> upstream and downstream is assumed to be the same.</li>
- </ol>
- </html>"));
+<p>
+Isentropic enthalpy is computed using the IAPWS-IF97 formulation:
+</p>
+<ol>
+<li> A medium is in a particular state, <code>refState</code>.</li>
+<li> The enthalpy at another state <code>h_is</code> shall be computed
+     under the assumption that the state transformation from <code>refState</code> to <code>h_is</code>
+     is performed with a change of specific entropy <i>ds = 0</i> and the pressure of state <code>h_is</code>
+     is <code>p_downstream</code> and the composition <code>X</code> upstream and downstream is assumed to be the same.</li>
+</ol>
+</html>"));
 end isentropicEnthalpy;
 //////////////////////////////////////////////////////////////////////
 // Protected classes
@@ -684,36 +685,36 @@ algorithm
     1.02325742818280e-7 + o[44])*tau2)));
 annotation(smoothOrder = 2,
 Documentation(info="<html>
- <p>
- This function is identical to
- <a href=\"modelica://Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.g2\">
- Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.g2</a>
- except that
- </p>
- <ul>
- <li>it contains the <code>smoothOrder</code> annotation, and
- </li>
- <li>
- it removes the assertions on the temperature and pressure because the applicability of
- this medium is steam heating which has medium states that are inside these values.
- </li>
- </ul>
- <p>
- The <code>smoothOrder</code> is needed for Optimica to differentiate the specific heat capacity,
- which is used in
- <a href=\"modelica://AixLib.Media.Examples.SteamDerivativeCheck\">
- AixLib.Media.Examples.SteamDerivativeCheck</a>.
- The function is differentiable except at <code>p=0</code>, which is far away from the state for which
- this function is used.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 11, 2021, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+This function is identical to
+<a href=\"modelica://Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.g2\">
+Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.g2</a>
+except that
+</p>
+<ul>
+<li>it contains the <code>smoothOrder</code> annotation, and
+</li>
+<li>
+it removes the assertions on the temperature and pressure because the applicability of
+this medium is steam heating which has medium states that are inside these values.
+</li>
+</ul>
+<p>
+The <code>smoothOrder</code> is needed for Optimica to differentiate the specific heat capacity,
+which is used in
+<a href=\"modelica://AixLib.Media.Examples.SteamDerivativeCheck\">
+AixLib.Media.Examples.SteamDerivativeCheck</a>.
+The function is differentiable except at <code>p=0</code>, which is far away from the state for which
+this function is used.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 11, 2021, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end g2;
 
 function temperature_ph
@@ -728,38 +729,38 @@ function temperature_ph
     constant Temperature TMean =  4.15555698340926E+02 "Mean temperature";
     constant Real pSD = 1.13236055019318E+05 "Normalization value";
     constant Real TSD = 1.32971013463839E+01 "Normalization value";
-    AbsolutePressure pHat;
+    Modelica.Units.SI.PressureDifference pHat;
 algorithm
   pHat := (p - pMean)/pSD;
   T := b[1] + b[2]*pHat + b[3]*h;
 annotation (Inline=true,smoothOrder=2,
       Documentation(info="<html>
- <p>
- Returns temperature from specific enthalpy and pressure.
- </p>
- <h4>Implementation</h4>
- <p>
- This linear approximation is the inverse or backward function of
- <a href=\"modelica://AixLib.Media.Steam.specificEnthalpy\">
- AixLib.Media.Steam.specificEnthalpy</a> and is numerically
- consistent with that forward function.
- </p>
- <p>
- The largest error of this linearization is  <i>1.17&deg;C</i> (<i>0.31</i>%),
- which occurs at <i>100&deg;C</i> and <i>100 kPa</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 13, 2021, by Kathryn Hinkelman:<br/>
- Added pressure as a variable.
- </li>
- <li>
- October 30, 2020, by Kathryn Hinkelman:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Returns temperature from specific enthalpy and pressure.
+</p>
+<h4>Implementation</h4>
+<p>
+This linear approximation is the inverse or backward function of
+<a href=\"modelica://AixLib.Media.Steam.specificEnthalpy\">
+AixLib.Media.Steam.specificEnthalpy</a> and is numerically
+consistent with that forward function.
+</p>
+<p>
+The largest error of this linearization is  <i>1.17&deg;C</i> (<i>0.31</i>%),
+which occurs at <i>100&deg;C</i> and <i>100 kPa</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 13, 2021, by Kathryn Hinkelman:<br/>
+Added pressure as a variable.
+</li>
+<li>
+October 30, 2020, by Kathryn Hinkelman:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end temperature_ph;
 
 function temperature_ps
@@ -773,40 +774,40 @@ function temperature_ps
     constant Temperature TMean =  4.15555698340926E+02 "Mean temperature";
     constant Real pSD = 1.13236055019318E+05 "Normalization value";
     constant Real TSD = 1.32971013463839E+01 "Normalization value";
-    AbsolutePressure pHat;
-    Temperature THat;
+    Modelica.Units.SI.PressureDifference pHat;
+    Modelica.Units.SI.TemperatureDifference THat;
 algorithm
   pHat := (p - pMean)/pSD;
   THat := (s - a[1] - pHat*(a[2] + a[4]*pHat))/(a[3] + a[5]*pHat);
   T := THat*TSD + TMean;
 annotation (Inline=true,smoothOrder=2,
     Documentation(info="<html>
- <p>
- Returns temperature from specific entropy and pressure.
- </p>
- <h4>Implementation</h4>
- <p>
- This polynomial approximation is the inverse or backward function of
- <a href=\"modelica://AixLib.Media.Steam.specificEntropy\">
- AixLib.Media.Steam.specificEntropy</a> and is numerically
- consistent with that forward function.
- </p>
- <p>
- The largest error of this linearization is  <i>7.70&deg;C</i> (<i>1.86</i>%),
- which occurs at <i>137.4&deg;C</i> and <i>100 kPa</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 13, 2021, by Kathryn Hinkelman:<br/>
- Added pressure as a variable.
- </li>
- <li>
- October 30, 2020, by Kathryn Hinkelman:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<p>
+Returns temperature from specific entropy and pressure.
+</p>
+<h4>Implementation</h4>
+<p>
+This polynomial approximation is the inverse or backward function of
+<a href=\"modelica://AixLib.Media.Steam.specificEntropy\">
+AixLib.Media.Steam.specificEntropy</a> and is numerically
+consistent with that forward function.
+</p>
+<p>
+The largest error of this linearization is  <i>7.70&deg;C</i> (<i>1.86</i>%),
+which occurs at <i>137.4&deg;C</i> and <i>100 kPa</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 13, 2021, by Kathryn Hinkelman:<br/>
+Added pressure as a variable.
+</li>
+<li>
+October 30, 2020, by Kathryn Hinkelman:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
 end temperature_ps;
 
 function rho_pT "Density as function of temperature and pressure"
@@ -818,20 +819,24 @@ function rho_pT "Density as function of temperature and pressure"
   Modelica.Media.Common.GibbsDerivs g
     "Dimensionless Gibbs function and derivatives w.r.t. pi and tau";
   SpecificHeatCapacity R "Specific gas constant of water vapor";
+  function g2_smooth
+    extends Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.g2;
+    annotation(smoothOrder=2);
+  end g2_smooth;
 algorithm
   R := Modelica.Media.Water.IF97_Utilities.BaseIF97.data.RH2O;
   // Region 2 properties
-  g := Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.g2(p, T);
+  g := g2_smooth(p, T);
   rho := p/(R*T*g.pi*g.gpi);
   annotation (
     Inline=true,
     smoothOrder=2,
     Documentation(info="<html>
- <p>
- Density is computed from temperature and pressure using the
- IAPWS-IF97 relationship via the Gibbs free energy for region 2.
- </p>
- </html>"));
+<p>
+Density is computed from temperature and pressure using the
+IAPWS-IF97 relationship via the Gibbs free energy for region 2.
+</p>
+</html>"));
 end rho_pT;
 
 function pressure_dT
@@ -847,7 +852,6 @@ algorithm
         region=2);
   annotation (Inline=true);
 end pressure_dT;
-
   annotation (Icon(graphics={
       Line(
         points={{50,30},{30,10},{50,-10},{30,-30}},
@@ -861,71 +865,104 @@ end pressure_dT;
         points={{-30,30},{-50,10},{-30,-10},{-50,-30}},
         color={0,0,0},
         smooth=Smooth.Bezier)}), Documentation(info="<html>
- <p>
- This medium package models water vapor (pure steam, region 2, quality=1).
- </p>
- <p>
- Thermodynamic properties are calculated primarily in terms of pressure
- and temperature.
- For thermodynamic property functions, the IAPWS-IF97 formulations are adapted,
- and approximate relationships are provided for commonly used functions to improve
- computational efficiency and provide backward compatability.
- </p>
- <p>
- Detailed functions from <a href=\"modelica://Modelica.Media.Water.WaterIF97_R2pT\">
- Modelica.Media.Water.WaterIF97_R2pT</a> are generally used, expect for
- <a href=\"modelica://AixLib.Media.Steam.specificEnthalpy\">AixLib.Media.Steam.specificEnthalpy</a> and
- <a href=\"modelica://AixLib.Media.Steam.specificEntropy\">AixLib.Media.Steam.specificEntropy</a>
- (both \"forward\" functions), as well as their \"backward\" inverse functions
- <a href=\"modelica://AixLib.Media.Steam.temperature_ph\">AixLib.Media.Steam.temperature_ph</a> and
- <a href=\"modelica://AixLib.Media.Steam.temperature_ps\">AixLib.Media.Steam.temperature_ps</a>,
- which are numerically consistent with the forward functions.
- The following modifications were made relative to the
- <a href=\"modelica://Modelica.Media.Water.WaterIF97_R2pT\">
- Modelica.Media.Water.WaterIF97_R2pT</a> medium package:
- </p>
- <ol>
- <li>Analytic expressions for the derivatives are provided for all thermodynamic property functions.</li>
- <li>The implementation is generally simplier in order to increase the likelyhood
- of more efficient simulations. </li>
- </ol>
- <h4>Limitations </h4>
- <ul>
- <li>
- The valid temperature range is <i>100&deg;C &le; T &le; 160&deg;C</i>, and the valid
- pressure range is <i>100 kPa &le; p &le; 550 kPa</i>.
- </li>
- <li>When phase change is required, this model is to be used in combination with
- <a href=\"modelica://AixLib.Media.Water\">AixLib.Media.Water</a>
- for the liquid phase (quality=0). Please note that the maximum temperature for liquid
- water is <code>T_max=130&deg;C</code>. This is suitable for real-world condensate
- return and boiler feedwater systems, which are typically vented to the atmosphere
- with steam contained via steam traps (thus, <code>T_max=100&deg;C</code> for the
- condensate or feedwater in properly functioning systems).</li>
- </ul>
- <h4>Applications </h4>
- <p>
- This model is intended for first generation district heating systems and other
- steam heating processes involving low and medium pressure steam.
- </p>
- <h4>References </h4>
- <p>W. Wagner et al., &ldquo;The IAPWS industrial formulation 1997 for the thermodynamic
- properties of water and steam,&rdquo; <i>J. Eng. Gas Turbines Power</i>, vol. 122, no.
- 1, pp. 150&ndash;180, 2000.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 13, 2021, by Kathryn Hinkelman:<br/>
- Changed pressure from constant to variable and reduced applicable
- pressure-temperature range to improve accuracy of polynomial approximations.
- </li>
- <li>
- October 30, 2020, by Kathryn Hinkelman:<br/>
- Complete new reimplementation to eliminate numerical inefficiencies
- and improve accuracy of property function calculations.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This medium package models water vapor (pure steam, region 2, quality=1).
+</p>
+<p>
+Thermodynamic properties are calculated primarily in terms of pressure
+and temperature.
+For thermodynamic property functions, the IAPWS-IF97 formulations are adapted,
+and approximate relationships are provided for commonly used functions to improve
+computational efficiency and provide backward compatability.
+</p>
+<p>
+Detailed functions from <a href=\"modelica://Modelica.Media.Water.WaterIF97_R2pT\">
+Modelica.Media.Water.WaterIF97_R2pT</a> are generally used, except for
+<a href=\"modelica://AixLib.Media.Steam.specificEnthalpy\">AixLib.Media.Steam.specificEnthalpy</a> and
+<a href=\"modelica://AixLib.Media.Steam.specificEntropy\">AixLib.Media.Steam.specificEntropy</a>
+(both \"forward\" functions), as well as their \"backward\" inverse functions
+<a href=\"modelica://AixLib.Media.Steam.temperature_ph\">AixLib.Media.Steam.temperature_ph</a> and
+<a href=\"modelica://AixLib.Media.Steam.temperature_ps\">AixLib.Media.Steam.temperature_ps</a>,
+which are numerically consistent with the forward functions.
+The following modifications were made relative to the
+<a href=\"modelica://Modelica.Media.Water.WaterIF97_R2pT\">
+Modelica.Media.Water.WaterIF97_R2pT</a> medium package:
+</p>
+<ol>
+<li>Analytic expressions for the derivatives are provided for all thermodynamic property functions.</li>
+<li>The implementation is generally simpler in order to increase the likelihood
+of more efficient simulations. </li>
+</ol>
+<h4>Limitations </h4>
+<ul>
+<li>
+The valid temperature range is <i>100&deg;C &le; T &le; 160&deg;C</i>, and the valid
+pressure range is <i>100 kPa &le; p &le; 550 kPa</i>.
+</li>
+<li>When phase change is required, this model is to be used in combination with
+<a href=\"modelica://AixLib.Media.Water\">AixLib.Media.Water</a>
+for the liquid phase (quality=0). Please note that the maximum temperature for liquid
+water is <code>T_max=130&deg;C</code>. This is suitable for real-world condensate
+return and boiler feedwater systems, which are typically vented to the atmosphere
+with steam contained via steam traps (thus, <code>T_max=100&deg;C</code> for the
+condensate or feedwater in properly functioning systems).</li>
+</ul>
+<h4>Applications </h4>
+<p>
+This model is intended for first generation district heating systems and other
+steam heating processes involving low and medium pressure steam.
+</p>
+<h4>References </h4>
+<p>W. Wagner et al., &ldquo;The IAPWS industrial formulation 1997 for the thermodynamic
+properties of water and steam,&rdquo; <i>J. Eng. Gas Turbines Power</i>, vol. 122, no.
+1, pp. 150&ndash;180, 2000.
+</p>
+<p>
+Kathryn Hinkelman, Saranya Anbarasu, Michael Wetter, Antoine Gautier, Wangda Zuo. 2022.
+&ldquo;A Fast and Accurate Modeling Approach for Water and Steam
+Thermodynamics with Practical Applications in District Heating System Simulation,&rdquo;
+<i>Energy</i>, 254(A), pp. 124227.
+<a href=\"https://doi.org/10.1016/j.energy.2022.124227\">10.1016/j.energy.2022.124227</a>
+</p>
+<p>
+Kathryn Hinkelman, Saranya Anbarasu, Michael Wetter, Antoine Gautier, Baptiste Ravache, Wangda Zuo 2022.
+&ldquo;Towards Open-Source Modelica Models For Steam-Based District Heating Systems.&rdquo;
+<i>Proc. of the 1st International Workshop On Open Source Modelling And Simulation Of
+Energy Systems (OSMSES 2022)</i>, Aachen, German, April 4-5, 2022.
+<a href=\"https://doi.org/10.1109/OSMSES54027.2022.9769121\">10.1109/OSMSES54027.2022.9769121</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 29, 2023, by Kathryn Hinkelman:<br/>
+Added publication references.
+</li>
+<li>
+March 10, 2023, by Saranya Anbarasu:<br/>
+Changed the variable type definition of <code>pHat</code> and <code>THat</code>
+from absolute to <code>Modelica.Units.SI.PressureDifference</code> and
+<code>Modelica.Units.SI.TemperatureDifference</code> to prevent min/max
+assertion errors during initilization.
+</li>
+<li>
+May 9, 2022, by David Blum:<br/>
+In function <code>rho_pT</code>, created and used new function extending
+<code>Modelica.Media.Water.IF97_Utilities.BaseIF97.Basic.g2</code> with an
+annotation <code>smoothOrder=2</code>. This is to specifically pass on the
+<code>smoothOrder=2</code> annotion placed on <code>rho_pT</code> to
+the <code>g2</code> function.
+</li>
+<li>
+April 13, 2021, by Kathryn Hinkelman:<br/>
+Changed pressure from constant to variable and reduced applicable
+pressure-temperature range to improve accuracy of polynomial approximations.
+</li>
+<li>
+October 30, 2020, by Kathryn Hinkelman:<br/>
+Complete new reimplementation to eliminate numerical inefficiencies
+and improve accuracy of property function calculations.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Steam;
diff --git a/AixLib/Media/Water.mo b/AixLib/Media/Water.mo
index b45c41c41d..93aadc2b88 100644
--- a/AixLib/Media/Water.mo
+++ b/AixLib/Media/Water.mo
@@ -19,8 +19,9 @@ package Water "Package with model for liquid water with constant density"
     final parameter Boolean standardOrderComponents=true
       "If true, and reducedX = true, the last element of X will be computed from the other ones";
     Modelica.Units.SI.Density d=d_const "Density of medium";
-    Temperature T(stateSelect=
-      if preferredMediumStates then StateSelect.prefer else StateSelect.default)
+    Temperature T(
+      start=293.15,
+      stateSelect=if preferredMediumStates then StateSelect.prefer else StateSelect.default)
       "Temperature of medium";
     InputAbsolutePressure p "Absolute pressure of medium";
     InputMassFraction[nXi] Xi=fill(0, 0)
@@ -68,51 +69,51 @@ package Water "Package with model for liquid water with constant density"
     assert(noEvent(p >= 0.0), "Pressure (= " + String(p) + " Pa) of medium \"AixLib.Media.Water\" is negative\n(Temperature = " + String(T) + " K)");
 
     annotation(Documentation(info="<html>
- <p>
- Model with basic thermodynamic properties.
- </p>
- <p>
- This base properties model is identical to
- <a href=\"modelica://Modelica.Media.Water.ConstantPropertyLiquidWater\">
- Modelica.Media.Water.ConstantPropertyLiquidWater</a>,
- except that the equation
- <code>u = cv_const*(T - reference_T)</code>
- has been replaced by <code>u=h</code> because
- <code>cp_const=cv_const</code>.
- </p>
- <p>
- This model provides equation for the following thermodynamic properties:
- </p>
- <table border=\"1\" cellspacing=\"0\" cellpadding=\"2\" summary=\"Thermodynamic properties\">
-   <tr><td><strong>Variable</strong></td>
-       <td><strong>Unit</strong></td>
-       <td><strong>Description</strong></td></tr>
-   <tr><td>T</td>
-       <td>K</td>
-       <td>temperature</td></tr>
-   <tr><td>p</td>
-       <td>Pa</td>
-       <td>absolute pressure</td></tr>
-   <tr><td>d</td>
-       <td>kg/m3</td>
-       <td>density</td></tr>
-   <tr><td>h</td>
-       <td>J/kg</td>
-       <td>specific enthalpy</td></tr>
-   <tr><td>u</td>
-       <td>J/kg</td>
-       <td>specific internal energy</td></tr>
-   <tr><td>Xi[nXi]</td>
-       <td>kg/kg</td>
-       <td>independent mass fractions m_i/m</td></tr>
-   <tr><td>R</td>
-       <td>J/kg.K</td>
-       <td>gas constant</td></tr>
-   <tr><td>M</td>
-       <td>kg/mol</td>
-       <td>molar mass</td></tr>
- </table>
- </html>"));
+<p>
+Model with basic thermodynamic properties.
+</p>
+<p>
+This base properties model is identical to
+<a href=\"modelica://Modelica.Media.Water.ConstantPropertyLiquidWater\">
+Modelica.Media.Water.ConstantPropertyLiquidWater</a>,
+except that the equation
+<code>u = cv_const*(T - reference_T)</code>
+has been replaced by <code>u=h</code> because
+<code>cp_const=cv_const</code>.
+</p>
+<p>
+This model provides equation for the following thermodynamic properties:
+</p>
+<table border=\"1\" cellspacing=\"0\" cellpadding=\"2\" summary=\"Thermodynamic properties\">
+  <tr><td><strong>Variable</strong></td>
+      <td><strong>Unit</strong></td>
+      <td><strong>Description</strong></td></tr>
+  <tr><td>T</td>
+      <td>K</td>
+      <td>temperature</td></tr>
+  <tr><td>p</td>
+      <td>Pa</td>
+      <td>absolute pressure</td></tr>
+  <tr><td>d</td>
+      <td>kg/m3</td>
+      <td>density</td></tr>
+  <tr><td>h</td>
+      <td>J/kg</td>
+      <td>specific enthalpy</td></tr>
+  <tr><td>u</td>
+      <td>J/kg</td>
+      <td>specific internal energy</td></tr>
+  <tr><td>Xi[nXi]</td>
+      <td>kg/kg</td>
+      <td>independent mass fractions m_i/m</td></tr>
+  <tr><td>R</td>
+      <td>J/kg.K</td>
+      <td>gas constant</td></tr>
+  <tr><td>M</td>
+      <td>kg/mol</td>
+      <td>molar mass</td></tr>
+</table>
+</html>"));
   end BaseProperties;
 
 function enthalpyOfLiquid "Return the specific enthalpy of liquid"
@@ -125,142 +126,148 @@ annotation (
   smoothOrder=5,
   Inline=true,
 Documentation(info="<html>
- <p>
- Enthalpy of the water.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 16, 2014 by Michael Wetter:<br/>
- First implementation.
- This function is used by
- <a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir\">
- AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir</a>.
- </li>
- </ul>
- </html>"));
+<p>
+Enthalpy of the water.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 16, 2014 by Michael Wetter:<br/>
+First implementation.
+This function is used by
+<a href=\"modelica://AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir\">
+AixLib.Fluid.MixingVolumes.MixingVolumeMoistAir</a>.
+</li>
+</ul>
+</html>"));
 end enthalpyOfLiquid;
   annotation(Documentation(info="<html>
- <p>
- This medium package models liquid water.
- </p>
- <p>
- The mass density is computed using a constant value of <i>995.586</i> kg/s.
- For a medium model in which the density is a function of temperature, use
- <a href=\"modelica://AixLib.Media.Specialized.Water.TemperatureDependentDensity\">
- AixLib.Media.Specialized.Water.TemperatureDependentDensity</a> which may have considerably higher computing time.
- </p>
- <p>
- For the specific heat capacities at constant pressure and at constant volume,
- a constant value of <i>4184</i> J/(kg K), which corresponds to <i>20</i>&deg;C
- is used.
- The figure below shows the relative error of the specific heat capacity that
- is introduced by this simplification.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/Media/Water/plotCp.png\" border=\"1\"
- alt=\"Relative variation of specific heat capacity with temperature\"/>
- </p>
- <p>
- The enthalpy is computed using the convention that <i>h=0</i>
- if <i>T=0</i> &deg;C.
- </p>
- <h4>Limitations</h4>
- <p>
- Density, specific heat capacity, thermal conductivity and viscosity are constant.
- Water is modeled as an incompressible liquid.
- There are no phase changes.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 28, 2020, by Michael Wetter:<br/>
- Reformulated <code>BaseProperties</code> to avoid event-triggering assertions.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1401\">#1401</a>.
- </li>
- <li>
- October 26, 2018, by Filip Jorissen and Michael Wetter:<br/>
- Now printing different messages if temperature is above or below its limit,
- and adding instance name as JModelica does not print the full instance name in the assertion.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1045\">#1045</a>.
- </li>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Set <code>AbsolutePressure(start=p_default)</code> to avoid
- a translation error if
- <a href=\"modelica://AixLib.Fluid.Sources.Examples.TraceSubstancesFlowSource\">
- AixLib.Fluid.Sources.Examples.TraceSubstancesFlowSource</a>
- (if used with water instead of air)
- is translated in pedantic mode in Dymola 2016.
- The reason is that pressures use <code>Medium.p_default</code> as start values,
- but
- <a href=\"modelica://Modelica.Media.Interfaces.Types\">
- Modelica.Media.Interfaces.Types</a>
- sets a default value of <i>1E-5</i>.
- A similar change has been done for pressure and density.
- This fixes
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- June 6, 2015, by Michael Wetter:<br/>
- Changed type of <code>BaseProperties.T</code> from
- <code>Modelica.Units.SI.Temperature</code> to <code>Temperature</code>.
- Otherwise, it has a different start value than <code>Medium.T</code>, which
- causes an error if
- <a href=\"AixLib.Media.Examples.WaterProperties\">
- AixLib.Media.Examples.WaterProperties</a>
- is translated in pedantic mode.
- This fixes
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
- </li>
- <li>
- June 5, 2015, by Michael Wetter:<br/>
- Added <code>stateSelect</code> attribute in <code>BaseProperties.T</code>
- to allow correct use of <code>preferredMediumState</code> as
- described in
- <a href=\"modelica://Modelica.Media.Interfaces.PartialMedium\">
- Modelica.Media.Interfaces.PartialMedium</a>,
- and set <code>preferredMediumState=false</code>
- to keep the same states as were used before.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/260\">#260</a>.
- </li>
- <li>
- June 5, 2015, by Michael Wetter:<br/>
- Removed <code>ThermodynamicState</code> declaration as this lead to
- the error
- \"Attempting to redeclare record ThermodynamicState when the original was not replaceable.\"
- in Dymola 2016 using the pedantic model check.
- </li>
- <li>
- May 1, 2015, by Michael Wetter:<br/>
- Added <code>Inline=true</code> for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
- issue 227</a>.
- </li>
- <li>
- February 25, 2015, by Michael Wetter:<br/>
- Removed <code>stateSelect</code> attribute on pressure as this caused
- <a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
- AixLib.Examples.Tutorial.SpaceCooling.System3</a>
- to fail with the error message
- \"differentiated if-then-else was not continuous\".
- </li>
- <li>
- October 15, 2014, by Michael Wetter:<br/>
- Reimplemented media based on
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/blob/446aa83720884052476ad6d6d4f90a6a29bb8ec9/AixLib/Media/Water.mo\">446aa83</a>.
- </li>
- <li>
- November 15, 2013, by Michael Wetter:<br/>
- Complete new reimplementation because the previous version
- had the option to add a compressibility to the medium, which
- has never been used.
- </li>
- </ul>
- </html>"),
+<p>
+This medium package models liquid water.
+</p>
+<p>
+The mass density is computed using a constant value of <i>995.586</i> kg/s.
+For a medium model in which the density is a function of temperature, use
+<a href=\"modelica://AixLib.Media.Specialized.Water.TemperatureDependentDensity\">
+AixLib.Media.Specialized.Water.TemperatureDependentDensity</a> which may have considerably higher computing time.
+</p>
+<p>
+For the specific heat capacities at constant pressure and at constant volume,
+a constant value of <i>4184</i> J/(kg K), which corresponds to <i>20</i>&deg;C
+is used.
+The figure below shows the relative error of the specific heat capacity that
+is introduced by this simplification.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/Media/Water/plotCp.png\" border=\"1\"
+alt=\"Relative variation of specific heat capacity with temperature\"/>
+</p>
+<p>
+The enthalpy is computed using the convention that <i>h=0</i>
+if <i>T=0</i> &deg;C.
+</p>
+<h4>Limitations</h4>
+<p>
+Density, specific heat capacity, thermal conductivity and viscosity are constant.
+Water is modeled as an incompressible liquid.
+There are no phase changes.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+September 28, 2020, by Michael Wetter:<br/>
+Reformulated <code>BaseProperties</code> to avoid event-triggering assertions.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1401\">#1401</a>.
+</li>
+<li>
+October 26, 2018, by Filip Jorissen and Michael Wetter:<br/>
+Now printing different messages if temperature is above or below its limit,
+and adding instance name as JModelica does not print the full instance name in the assertion.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1045\">#1045</a>.
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Set <code>AbsolutePressure(start=p_default)</code> to avoid
+a translation error if
+<a href=\"modelica://AixLib.Fluid.Sources.Examples.TraceSubstancesFlowSource\">
+AixLib.Fluid.Sources.Examples.TraceSubstancesFlowSource</a>
+(if used with water instead of air)
+is translated in pedantic mode in Dymola 2016.
+The reason is that pressures use <code>Medium.p_default</code> as start values,
+but
+<a href=\"modelica://Modelica.Media.Interfaces.Types\">
+Modelica.Media.Interfaces.Types</a>
+sets a default value of <i>1E-5</i>.
+A similar change has been done for pressure and density.
+This fixes
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+June 6, 2015, by Michael Wetter:<br/>
+Changed type of <code>BaseProperties.T</code> from
+<code>Modelica.Units.SI.Temperature</code> to <code>Temperature</code>.
+Otherwise, it has a different start value than <code>Medium.T</code>, which
+causes an error if
+<a href=\"modelica://AixLib.Media.Examples.WaterProperties\">
+AixLib.Media.Examples.WaterProperties</a>
+is translated in pedantic mode.
+This fixes
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/266\">#266</a>.
+</li>
+<li>
+June 5, 2015, by Michael Wetter:<br/>
+Added <code>stateSelect</code> attribute in <code>BaseProperties.T</code>
+to allow correct use of <code>preferredMediumState</code> as
+described in
+<a href=\"modelica://Modelica.Media.Interfaces.PartialMedium\">
+Modelica.Media.Interfaces.PartialMedium</a>,
+and set <code>preferredMediumState=false</code>
+to keep the same states as were used before.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/260\">#260</a>.
+</li>
+<li>
+June 5, 2015, by Michael Wetter:<br/>
+Removed <code>ThermodynamicState</code> declaration as this lead to
+the error
+\"Attempting to redeclare record ThermodynamicState when the original was not replaceable.\"
+in Dymola 2016 using the pedantic model check.
+</li>
+<li>
+May 1, 2015, by Michael Wetter:<br/>
+Added <code>Inline=true</code> for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/227\">
+issue 227</a>.
+</li>
+<li>
+February 25, 2015, by Michael Wetter:<br/>
+Removed <code>stateSelect</code> attribute on pressure as this caused
+<a href=\"modelica://AixLib.Examples.Tutorial.SpaceCooling.System3\">
+AixLib.Examples.Tutorial.SpaceCooling.System3</a>
+to fail with the error message
+\"differentiated if-then-else was not continuous\".
+</li>
+<li>
+October 15, 2014, by Michael Wetter:<br/>
+Reimplemented media based on
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/blob/446aa83720884052476ad6d6d4f90a6a29bb8ec9/Annex60/Media/Water.mo\">446aa83</a>.
+</li>
+<li>
+November 15, 2013, by Michael Wetter:<br/>
+Complete new reimplementation because the previous version
+had the option to add a compressibility to the medium, which
+has never been used.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
         graphics={
         Polygon(
@@ -287,6 +294,6 @@ end enthalpyOfLiquid;
           extent={{20,-30},{78,-88}},
           lineColor={0,0,0},
           fillPattern=FillPattern.Sphere,
-          fillColor={95,95,95})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={95,95,95})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Water;
diff --git a/AixLib/Obsolete/Year2019/Fluid/HeatPumps/Examples/HeatPumpDetailed.mo b/AixLib/Obsolete/Year2019/Fluid/HeatPumps/Examples/HeatPumpDetailed.mo
index 17281fc51d..96f8bf20e8 100644
--- a/AixLib/Obsolete/Year2019/Fluid/HeatPumps/Examples/HeatPumpDetailed.mo
+++ b/AixLib/Obsolete/Year2019/Fluid/HeatPumps/Examples/HeatPumpDetailed.mo
@@ -68,10 +68,10 @@ model HeatPumpDetailed
     amplitude=3000,
     offset=3000)
     annotation (Placement(transformation(extent={{76,26},{84,34}})));
-  AixLib.Fluid.Movers.SpeedControlled_Nrpm pumSou(
+  AixLib.Obsolete.Year2024.Fluid.Movers.SpeedControlled_Nrpm pumSou(
     redeclare final package Medium = Medium_sin,
-    redeclare final AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to8
-      per,
+    redeclare final AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to8 per,
+
     final allowFlowReversal=true,
     final addPowerToMedium=false) "Fan or pump at source side of HP"
     annotation (Placement(transformation(
diff --git a/AixLib/Obsolete/Year2021/Electrical/PVSystem.mo b/AixLib/Obsolete/Year2021/Electrical/PVSystem.mo
index ed2dd7ecfd..7a3d0d05d6 100644
--- a/AixLib/Obsolete/Year2021/Electrical/PVSystem.mo
+++ b/AixLib/Obsolete/Year2021/Electrical/PVSystem.mo
@@ -428,7 +428,7 @@ package PVSystem
     model PVInverterRMS "Inverter model including system management"
       extends AixLib.Obsolete.BaseClasses.ObsoleteModel;
 
-      parameter Modelica.Units.SI.Power uMax2
+      parameter Modelica.Units.SI.Power uMax2=3800
         "Upper limits of input signals (MaxOutputPower)";
      Modelica.Blocks.Interfaces.RealOutput PVPowerRmsW(
       final quantity="Power",
diff --git a/AixLib/Obsolete/Year2021/Fluid/Examples/package.order b/AixLib/Obsolete/Year2021/Fluid/Examples/package.order
index b0a86450d4..1666453594 100644
--- a/AixLib/Obsolete/Year2021/Fluid/Examples/package.order
+++ b/AixLib/Obsolete/Year2021/Fluid/Examples/package.order
@@ -1,3 +1,3 @@
+PumpHydraulicResistance_closedLoop
 PumpRadiatorThermostaticValve
 PumpRadiatorValve
-PumpHydraulicResistance_closedLoop
diff --git a/AixLib/Obsolete/Year2022/ThermalZones/HighOrder/House/MFD/package.order b/AixLib/Obsolete/Year2022/ThermalZones/HighOrder/House/MFD/package.order
index bb59d56e3b..ce59e42a6d 100644
--- a/AixLib/Obsolete/Year2022/ThermalZones/HighOrder/House/MFD/package.order
+++ b/AixLib/Obsolete/Year2022/ThermalZones/HighOrder/House/MFD/package.order
@@ -1,3 +1,3 @@
-BuildingEnvelope
 BuildingAndEnergySystem
+BuildingEnvelope
 EnergySystem
diff --git a/AixLib/Obsolete/Year2022/ThermalZones/HighOrder/package.order b/AixLib/Obsolete/Year2022/ThermalZones/HighOrder/package.order
index 037743e3c6..5ea3a55ff7 100644
--- a/AixLib/Obsolete/Year2022/ThermalZones/HighOrder/package.order
+++ b/AixLib/Obsolete/Year2022/ThermalZones/HighOrder/package.order
@@ -1,3 +1,3 @@
-Rooms
 House
+Rooms
 Examples
diff --git a/AixLib/Obsolete/Year2022/package.order b/AixLib/Obsolete/Year2022/package.order
index 66f8377bcc..fef9d04c12 100644
--- a/AixLib/Obsolete/Year2022/package.order
+++ b/AixLib/Obsolete/Year2022/package.order
@@ -1,3 +1,3 @@
+ThermalZones
 Utilities
 Examples
-ThermalZones
diff --git a/AixLib/Airflow/Multizone/BaseClasses/Examples/Interpolate.mo b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/Interpolate.mo
similarity index 76%
rename from AixLib/Airflow/Multizone/BaseClasses/Examples/Interpolate.mo
rename to AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/Interpolate.mo
index dfddc29793..329f83cdc6 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/Examples/Interpolate.mo
+++ b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/Interpolate.mo
@@ -1,4 +1,4 @@
-within AixLib.Airflow.Multizone.BaseClasses.Examples;
+within AixLib.Obsolete.Year2024.Airflow.Multizone.BaseClasses.Examples;
 model Interpolate "Test model for the function flowElementData"
   extends Modelica.Icons.Example;
 
@@ -28,17 +28,19 @@ initial equation
     ensureMonotonicity=true);
 equation
    dp=ramp.y;
-   m_flow =AixLib.Airflow.Multizone.BaseClasses.interpolate(u=dp,xd=xd,yd=yd,d=d);
+   m_flow =AixLib.Obsolete.Year2024.Airflow.Multizone.BaseClasses.interpolate(
+    u=dp,
+    xd=xd,
+    yd=yd,
+    d=d);
 
   annotation (
 experiment(
       StopTime=500,
-      Tolerance=1e-06),
-  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Airflow/Multizone/BaseClasses/Examples/Interpolate.mos"
-        "Simulate and plot"), Documentation(info="<html>
+      Tolerance=1e-06), Documentation(info="<html>
  <p>
  This example demonstrates the function
- <a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.interpolate\">
+ <a href=\"modelica://AixLib.Obsolete.Year2024.Airflow.Multizone.BaseClasses.interpolate\">
  AixLib.Airflow.Multizone.BaseClasses.interpolate</a>.
  </p>
  </html>",revisions="<html>
@@ -55,6 +57,5 @@ experiment(
  </li>
  </ul>
  </html>
- "),
-  __Dymola_LockedEditing="Model from IBPSA");
+ "));
 end Interpolate;
diff --git a/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/package.mo b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/package.mo
new file mode 100644
index 0000000000..6dbe9c258d
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/package.mo
@@ -0,0 +1,3 @@
+within AixLib.Obsolete.Year2024.Airflow.Multizone.BaseClasses;
+package Examples
+end Examples;
diff --git a/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/package.order b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/package.order
new file mode 100644
index 0000000000..37396855ae
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/Examples/package.order
@@ -0,0 +1 @@
+Interpolate
diff --git a/AixLib/Airflow/Multizone/BaseClasses/interpolate.mo b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/interpolate.mo
similarity index 92%
rename from AixLib/Airflow/Multizone/BaseClasses/interpolate.mo
rename to AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/interpolate.mo
index 24ea877e03..75bfd77537 100644
--- a/AixLib/Airflow/Multizone/BaseClasses/interpolate.mo
+++ b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/interpolate.mo
@@ -1,8 +1,8 @@
-within AixLib.Airflow.Multizone.BaseClasses;
+within AixLib.Obsolete.Year2024.Airflow.Multizone.BaseClasses;
 function interpolate
   "Function for the interpolation of table data for airflow models"
   extends Modelica.Icons.Function;
-
+  extends AixLib.Obsolete.BaseClasses.ObsoleteModel;
   input Real u "Independent variable";
   input Real[:] xd "X-axis support points";
   input Real[size(xd, 1)] yd "Y-axis support points";
@@ -38,7 +38,7 @@ algorithm
         y2d=d[i + 1]);
   end if;
 
-  annotation (
+  annotation (Diagram(obsolete = "Obsolete model"),
     Documentation(info="<html>
  <p>
  This function returns the value on a cubic hermite spline through the given support points
@@ -77,6 +77,5 @@ algorithm
  First Implementation.
  </li>
  </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+ </html>"));
 end interpolate;
diff --git a/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/package.mo b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/package.mo
new file mode 100644
index 0000000000..c922277642
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/package.mo
@@ -0,0 +1,3 @@
+within AixLib.Obsolete.Year2024.Airflow.Multizone;
+package BaseClasses
+end BaseClasses;
diff --git a/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/package.order b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/package.order
new file mode 100644
index 0000000000..9abc91405e
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Airflow/Multizone/BaseClasses/package.order
@@ -0,0 +1,2 @@
+interpolate
+Examples
diff --git a/AixLib/Obsolete/Year2024/Airflow/Multizone/package.mo b/AixLib/Obsolete/Year2024/Airflow/Multizone/package.mo
new file mode 100644
index 0000000000..f08aa93178
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Airflow/Multizone/package.mo
@@ -0,0 +1,3 @@
+within AixLib.Obsolete.Year2024.Airflow;
+package Multizone
+end Multizone;
diff --git a/AixLib/Obsolete/Year2024/Airflow/Multizone/package.order b/AixLib/Obsolete/Year2024/Airflow/Multizone/package.order
new file mode 100644
index 0000000000..7d7064fc3e
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Airflow/Multizone/package.order
@@ -0,0 +1 @@
+BaseClasses
diff --git a/AixLib/Obsolete/Year2024/Airflow/package.mo b/AixLib/Obsolete/Year2024/Airflow/package.mo
new file mode 100644
index 0000000000..fd0ded3ea2
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Airflow/package.mo
@@ -0,0 +1,3 @@
+within AixLib.Obsolete.Year2024;
+package Airflow
+end Airflow;
diff --git a/AixLib/Obsolete/Year2024/Airflow/package.order b/AixLib/Obsolete/Year2024/Airflow/package.order
new file mode 100644
index 0000000000..89df8286e7
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Airflow/package.order
@@ -0,0 +1 @@
+Multizone
diff --git a/AixLib/Fluid/Movers/SpeedControlled_Nrpm.mo b/AixLib/Obsolete/Year2024/Fluid/Movers/SpeedControlled_Nrpm.mo
similarity index 88%
rename from AixLib/Fluid/Movers/SpeedControlled_Nrpm.mo
rename to AixLib/Obsolete/Year2024/Fluid/Movers/SpeedControlled_Nrpm.mo
index f235a5a49b..4c70866ea9 100644
--- a/AixLib/Fluid/Movers/SpeedControlled_Nrpm.mo
+++ b/AixLib/Obsolete/Year2024/Fluid/Movers/SpeedControlled_Nrpm.mo
@@ -1,11 +1,10 @@
-within AixLib.Fluid.Movers;
+within AixLib.Obsolete.Year2024.Fluid.Movers;
 model SpeedControlled_Nrpm
   "Fan or pump with ideally controlled speed Nrpm as input signal"
   extends AixLib.Fluid.Movers.BaseClasses.PartialFlowMachine(
     final preVar=AixLib.Fluid.Movers.BaseClasses.Types.PrescribedVariable.Speed,
     final nominalValuesDefineDefaultPressureCurve=false,
     final computePowerUsingSimilarityLaws=true,
-    final m_flow_nominal = max(per.pressure.V_flow)*rho_default,
     final stageInputs(each final unit="1") = per.speeds,
     final constInput(final unit="1") =       per.constantSpeed,
     filter(
@@ -13,12 +12,9 @@ model SpeedControlled_Nrpm
       u(final unit="1"),
       y(final unit="1")),
     eff(
-      per(final pressure = per.pressure,
-          final use_powerCharacteristic = per.use_powerCharacteristic),
-          r_N(start=y_start)),
-    gaiSpe(u(final unit="rev/min"),
-           final k=1/per.speed_rpm_nominal));
-
+      per(final pressure = per.pressure)));
+ extends AixLib.Obsolete.BaseClasses.ObsoleteModel;
+  parameter Modelica.Units.NonSI.AngularVelocity_rpm speed_rpm_nominal=1500 "Nominal rotational speed";
   parameter Real y_start(min=0, max=1, unit="1")=0 "Initial value of speed"
     annotation(Dialog(tab="Dynamics", group="Filtered speed", enable=use_inputFilter));
 
@@ -38,15 +34,21 @@ protected
     annotation (Placement(transformation(extent={{10,-10},{-10,10}},
         rotation=270,
         origin={10,-20})));
+protected
+  Modelica.Blocks.Math.Gain gaiSpe(final k=1/speed_rpm_nominal) "Pressure gain"
+    annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=0,
+        origin={-12,80})));
 initial equation
   assert(per.havePressureCurve,
    "SpeedControlled_Nrpm model requires to set the pressure vs. flow rate curve in record 'per'.");
 
 equation
   connect(Nrpm, gaiSpe.u)
-    annotation (Line(points={{0,120},{0,80},{-2.8,80}}, color={0,0,127}));
-  connect(gaiSpe.y, inputSwitch.u) annotation (Line(points={{-16.6,80},{-26,80},
-          {-26,50},{-22,50}}, color={0,0,127}));
+    annotation (Line(points={{0,120},{0,80}},           color={0,0,127}));
+  connect(gaiSpe.y, inputSwitch.u) annotation (Line(points={{-23,80},{-26,80},{-26,
+          50},{-22,50}},      color={0,0,127}));
   connect(eff.dp, gain.u) annotation (Line(points={{-11,-50},{2,-50},{10,-50},{10,
           -32}}, color={0,0,127}));
   connect(gain.y, preSou.dp_in)
@@ -60,7 +62,7 @@ equation
             26},{-26,26},{-26,-46}},
                                    color={0,0,127}));
   end if;
-  annotation (defaultComponentName="pump",
+  annotation (Diagram(obsolete = "Obsolete model - use AixLib.Fluid.Movers.SpeedControlled_y instead"), defaultComponentName="pump",
     Icon(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{100,
             100}}),
       graphics={
@@ -176,6 +178,5 @@ equation
      by <a href=\"mailto:francesco.casella@polimi.it\">Francesco Casella</a>:<br/>
         Model added to the Fluid library</li>
  </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+ </html>"));
 end SpeedControlled_Nrpm;
diff --git a/AixLib/Obsolete/Year2024/Fluid/Movers/package.mo b/AixLib/Obsolete/Year2024/Fluid/Movers/package.mo
new file mode 100644
index 0000000000..70a0987726
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Fluid/Movers/package.mo
@@ -0,0 +1,3 @@
+within AixLib.Obsolete.Year2024.Fluid;
+package Movers
+end Movers;
diff --git a/AixLib/Obsolete/Year2024/Fluid/Movers/package.order b/AixLib/Obsolete/Year2024/Fluid/Movers/package.order
new file mode 100644
index 0000000000..9986a873f8
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Fluid/Movers/package.order
@@ -0,0 +1 @@
+SpeedControlled_Nrpm
diff --git a/AixLib/Obsolete/Year2024/Fluid/package.mo b/AixLib/Obsolete/Year2024/Fluid/package.mo
new file mode 100644
index 0000000000..a2505b1231
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Fluid/package.mo
@@ -0,0 +1,3 @@
+within AixLib.Obsolete.Year2024;
+package Fluid
+end Fluid;
diff --git a/AixLib/Obsolete/Year2024/Fluid/package.order b/AixLib/Obsolete/Year2024/Fluid/package.order
new file mode 100644
index 0000000000..1fa2c6d10b
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/Fluid/package.order
@@ -0,0 +1 @@
+Movers
diff --git a/AixLib/Obsolete/Year2024/package.mo b/AixLib/Obsolete/Year2024/package.mo
new file mode 100644
index 0000000000..976477b445
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/package.mo
@@ -0,0 +1,3 @@
+within AixLib.Obsolete;
+package Year2024
+end Year2024;
diff --git a/AixLib/Obsolete/Year2024/package.order b/AixLib/Obsolete/Year2024/package.order
new file mode 100644
index 0000000000..47994bd685
--- /dev/null
+++ b/AixLib/Obsolete/Year2024/package.order
@@ -0,0 +1,2 @@
+Airflow
+Fluid
diff --git a/AixLib/Obsolete/YearIndependent/FastHVAC/Components/Chiller/Chiller.mo b/AixLib/Obsolete/YearIndependent/FastHVAC/Components/Chiller/Chiller.mo
index 39b236e878..3c3289041b 100644
--- a/AixLib/Obsolete/YearIndependent/FastHVAC/Components/Chiller/Chiller.mo
+++ b/AixLib/Obsolete/YearIndependent/FastHVAC/Components/Chiller/Chiller.mo
@@ -68,7 +68,7 @@ model Chiller "Base model of FastHVAC Chiller"
       group="Heat Losses",
       tab="Condenser",
       enable=use_ConCap));
-  parameter Modelica.Units.SI.ThermalConductance GConIns
+  parameter Modelica.Units.SI.ThermalConductance GConIns=0
     "Constant thermal conductance of condenser material" annotation (Evaluate=
         true, Dialog(
       group="Heat Losses",
@@ -101,7 +101,7 @@ model Chiller "Base model of FastHVAC Chiller"
       group="Heat Losses",
       tab="Evaporator",
       enable=use_EvaCap));
-  parameter Modelica.Units.SI.ThermalConductance GEvaIns
+  parameter Modelica.Units.SI.ThermalConductance GEvaIns=0
     "Constant thermal conductance of Evaporator material" annotation (Evaluate=
         true, Dialog(
       group="Heat Losses",
@@ -381,12 +381,6 @@ equation
           -16,-86},{-30,-86},{-30,-86.1},{-43.2,-86.1}}, color={176,0,0}));
   connect(senT_b2.enthalpyPort_b, enthalpyPort_b1) annotation (Line(points={{-61,
           -86.1},{-82,-86.1},{-82,-60},{-100,-60}}, color={176,0,0}));
-  connect(iceFac_in, sigBus.iceFacMeas) annotation (Line(points={{-76,-136},{-76,-43},
-          {-105,-43}},         color={0,0,127}), Text(
-      string="%second",
-      index=1,
-      extent={{-3,6},{-3,6}},
-      horizontalAlignment=TextAlignment.Right));
   connect(innerCycle.QEva, realPassThroughnSetEva.u) annotation (Line(points={{0,
           -30.7},{0,-40},{16,-40},{16,-44.8}}, color={0,0,127}));
   connect(innerCycle.QEva, heatFlowIneEva.u) annotation (Line(points={{0,-30.7},
diff --git a/AixLib/Obsolete/YearIndependent/FastHVAC/Components/HeatExchangers/RadiatorMultiLayer.mo b/AixLib/Obsolete/YearIndependent/FastHVAC/Components/HeatExchangers/RadiatorMultiLayer.mo
index 62a511a3f9..9927290929 100644
--- a/AixLib/Obsolete/YearIndependent/FastHVAC/Components/HeatExchangers/RadiatorMultiLayer.mo
+++ b/AixLib/Obsolete/YearIndependent/FastHVAC/Components/HeatExchangers/RadiatorMultiLayer.mo
@@ -1,4 +1,4 @@
-within AixLib.Obsolete.YearIndependent.FastHVAC.Components.HeatExchangers;
+within AixLib.Obsolete.YearIndependent.FastHVAC.Components.HeatExchangers;
 model RadiatorMultiLayer "Simple radiator multilayer model"
 extends AixLib.Obsolete.BaseClasses.ObsoleteModel;
 
@@ -283,618 +283,563 @@ equation
   T_source output is relevant for exergy analysis. It describes
   the&#160;logarithmic&#160;mean&#160;temperature&#160;is&#160;calculated&#160;from&#160;the&#160;temperatures&#160;at&#160;in-&#160;and&#160;outlet&#160;of&#160;the&#160;radiator.
 </p>
-<table>
+<table cellspacing=\"0\" cellpadding=\"2\" border=\"1\">
+  <tr>
+    <td>
+      <h4>
+        Type
+      </h4>
+    </td>
+    <td>
+      <h4>
+        Fraction of convective transport
+      </h4>
+    </td>
+    <td>
+      <h4>
+        Fraction of radiative transport
+      </h4>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>SectionalRadiator</i>
+      </p>
+      <p>
+        Simple (vertical) sectional radiator
+      </p>
+    </td>
+    <td>
+      <p>
+        0.70
+      </p>
+    </td>
+    <td>
+      <p>
+        0.30
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator10</i>
+      </p>
+      <p>
+        10 -- Panel radiator (single panel) without convection device
+      </p>
+    </td>
+    <td>
+      <p>
+        0.50
+      </p>
+    </td>
+    <td>
+      <p>
+        0.50
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator11</i>
+      </p>
+      <p>
+        11 -- Panel radiator (single panel) with one convection device
+      </p>
+    </td>
+    <td>
+      <p>
+        0.65
+      </p>
+    </td>
+    <td>
+      <p>
+        0.35
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator12</i>
+      </p>
+      <p>
+        12 -- Panel radiator (single panel) with two convection devices
+      </p>
+    </td>
+    <td>
+      <p>
+        0.75
+      </p>
+    </td>
+    <td>
+      <p>
+        0.25
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator20</i>
+      </p>
+      <p>
+        20 -- Panel radiator (two panels) without convection device
+      </p>
+    </td>
+    <td>
+      <p>
+        0.65
+      </p>
+    </td>
+    <td>
+      <p>
+        0.35
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator21</i>
+      </p>
+      <p>
+        21 -- Panel radiator (two panels) with one convection device
+      </p>
+    </td>
+    <td>
+      <p>
+        0.80
+      </p>
+    </td>
+    <td>
+      <p>
+        0.20
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator22</i>
+      </p>
+      <p>
+        22 -- Panel radiator (two panels) with two convection devices
+      </p>
+    </td>
+    <td>
+      <p>
+        0.85
+      </p>
+    </td>
+    <td>
+      <p>
+        0.15
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator30</i>
+      </p>
+      <p>
+        30 -- Panel radiator (three panels) without convection device
+      </p>
+    </td>
+    <td>
+      <p>
+        0.80
+      </p>
+    </td>
+    <td>
+      <p>
+        0.20
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator31</i>
+      </p>
+      <p>
+        31 -- Panel radiator (three panels) with one convection device
+      </p>
+    </td>
+    <td>
+      <p>
+        0.85
+      </p>
+    </td>
+    <td>
+      <p>
+        0.15
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>PanelRadiator32</i>
+      </p>
+      <p>
+        32 -- Panel radiator (three panels) with two or more convection
+        devices
+      </p>
+    </td>
+    <td>
+      <p>
+        0.90
+      </p>
+    </td>
+    <td>
+      <p>
+        0.10
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>ConvectorHeaterUncovered</i>
+      </p>
+      <p>
+        Convector heater without cover
+      </p>
+    </td>
+    <td>
+      <p>
+        0.95
+      </p>
+    </td>
+    <td>
+      <p>
+        0.05
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <i>ConvectorHeaterCovered</i>
+      </p>
+      <p>
+        Convector heater with cover
+      </p>
+    </td>
+    <td>
+      <p>
+        1.00
+      </p>
+    </td>
+    <td>
+      <p>
+        - no radiative transport -
+      </p>
+    </td>
+  </tr>
+</table>
+<p>
+  <br/>
+  The Height H of the radiator is discretized in N single Layers, as
+  shown in Figure 1
+</p>
+<p>
+  <br/>
+  <img src=
+  \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Schichtenmodell.png\"
+  alt=\"Multilayer Model of radiator \">
+</p>
+<p>
+  Figure 1: Multilayer Model of radiator
+</p>
+<p>
+  For every layer the equation (1) is solved.
+</p>
+<table cellspacing=\"0\" cellpadding=\"2\" border=\"1\">
   <caption>
-    \"equation for multilayer\" cellspacing=\"0\" cellpadding= \"2\"
-    border=\"1\"&gt;
-    <table>
-      <tr>
-        <td>
-          <h4>
-            Type
-          </h4>
-        </td>
-        <td>
-          <h4>
-            Fraction of convective transport
-          </h4>
-        </td>
-        <td>
-          <h4>
-            Fraction of radiative transport
-          </h4>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>SectionalRadiator</i>
-          </p>
-          <p>
-            Simple (vertical) sectional radiator
-          </p>
-        </td>
-        <td>
-          <p>
-            0.70
-          </p>
-        </td>
-        <td>
-          <p>
-            0.30
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator10</i>
-          </p>
-          <p>
-            10 -- Panel radiator (single panel) without convection
-            device
-          </p>
-        </td>
-        <td>
-          <p>
-            0.50
-          </p>
-        </td>
-        <td>
-          <p>
-            0.50
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator11</i>
-          </p>
-          <p>
-            11 -- Panel radiator (single panel) with one convection
-            device
-          </p>
-        </td>
-        <td>
-          <p>
-            0.65
-          </p>
-        </td>
-        <td>
-          <p>
-            0.35
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator12</i>
-          </p>
-          <p>
-            12 -- Panel radiator (single panel) with two convection
-            devices
-          </p>
-        </td>
-        <td>
-          <p>
-            0.75
-          </p>
-        </td>
-        <td>
-          <p>
-            0.25
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator20</i>
-          </p>
-          <p>
-            20 -- Panel radiator (two panels) without convection device
-          </p>
-        </td>
-        <td>
-          <p>
-            0.65
-          </p>
-        </td>
-        <td>
-          <p>
-            0.35
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator21</i>
-          </p>
-          <p>
-            21 -- Panel radiator (two panels) with one convection
-            device
-          </p>
-        </td>
-        <td>
-          <p>
-            0.80
-          </p>
-        </td>
-        <td>
-          <p>
-            0.20
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator22</i>
-          </p>
-          <p>
-            22 -- Panel radiator (two panels) with two convection
-            devices
-          </p>
-        </td>
-        <td>
-          <p>
-            0.85
-          </p>
-        </td>
-        <td>
-          <p>
-            0.15
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator30</i>
-          </p>
-          <p>
-            30 -- Panel radiator (three panels) without convection
-            device
-          </p>
-        </td>
-        <td>
-          <p>
-            0.80
-          </p>
-        </td>
-        <td>
-          <p>
-            0.20
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator31</i>
-          </p>
-          <p>
-            31 -- Panel radiator (three panels) with one convection
-            device
-          </p>
-        </td>
-        <td>
-          <p>
-            0.85
-          </p>
-        </td>
-        <td>
-          <p>
-            0.15
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>PanelRadiator32</i>
-          </p>
-          <p>
-            32 -- Panel radiator (three panels) with two or more
-            convection devices
-          </p>
-        </td>
-        <td>
-          <p>
-            0.90
-          </p>
-        </td>
-        <td>
-          <p>
-            0.10
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>ConvectorHeaterUncovered</i>
-          </p>
-          <p>
-            Convector heater without cover
-          </p>
-        </td>
-        <td>
-          <p>
-            0.95
-          </p>
-        </td>
-        <td>
-          <p>
-            0.05
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <i>ConvectorHeaterCovered</i>
-          </p>
-          <p>
-            Convector heater with cover
-          </p>
-        </td>
-        <td>
-          <p>
-            1.00
-          </p>
-        </td>
-        <td>
-          <p>
-            - no radiative transport -
-          </p>
-        </td>
-      </tr>
-    </table>
-    <p>
-      <br/>
-      The Height H of the radiator is discretized in N single Layers,
-      as shown in Figure 1
-    </p>
-    <p>
-      <br/>
-      <img src=
-      \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Schichtenmodell.png\"
-      alt=\"Multilayer Model of radiator \">
-    </p>
-    <p>
-      Figure 1: Multilayer Model of radiator
-    </p>
-    <p>
-      For every layer the equation (1) is solved.
-    </p>
-    <table>
-      <caption>
-        \"\" cellspacing=\"0\" cellpadding=\"2\" border=\"1\
-      </caption>
-      <tr>
-        <td>
-          <p>
-            <br/>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/DGL_HK.png\"
-            alt=\"Equation for every layer\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (1)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td></td>
-        <td></td>
-      </tr>
-    </table>
-    <p>
-      The total heat emission consists of a convective and a radiative
-      part.
-    </p>
-    <table>
-      <caption>
-        \"\" cellspacing=\"0\" cellpadding=\"2\" border=\"1\
-      </caption>
-      <tr>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_ab.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (2)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_K1.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (3)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_R1.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (4)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td></td>
-        <td></td>
-      </tr>
-    </table>
-    <p>
-      The convective heat emission is proportional to <img src=
-      \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/deltaT.png\"
-      alt=\"\"> &#160;.
-    </p>
-    <p>
-      The radiative heat emission is proportional to <img src=
-      \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/delta.png\"
-      alt=\"\"> &#160;=(T_L + DeltaT)^4-TR^4 (T_L: Room Temperature,
-      DeltaT: heater excess temperature, T_R: radiative temperature).
-    </p>
-    <table>
-      <caption>
-        \"\" cellspacing=\"0\" cellpadding=\"2\" border=\"1\
-      </caption>
-      <tr>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_K.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (5)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_R.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (6)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td></td>
-        <td></td>
-      </tr>
-    </table>
-    <p>
-      The heat emission of the radiator depends on the heater excess
-      temperature. In the model it is possible to choose between:
-    </p>
-    <table>
-      <caption>
-        \"\" cellspacing=\"0\" cellpadding=\"2\" border=\"1\
-      </caption>
-      <tr>
-        <td>
-          <h4>
-            Method
-          </h4>
-        </td>
-        <td>
-          <h4>
-            Formula
-          </h4>
-        </td>
-        <td></td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            arithmetic heater excess temperature
-          </p>
-        </td>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Delta_T_ari.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (7)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            logarithmic heater excess temperature
-          </p>
-        </td>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Delta_T_log.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (8)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            exponential heater excess temperature according to [2]
-          </p>
-        </td>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Delta_T_exp.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (9)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td></td>
-        <td></td>
-        <td></td>
-      </tr>
-    </table>
-    <p>
-      Due to stability reasons and accuracy at small heating medium
-      flow, an exponential calculation of the heater excess temperture
-      is recommended. The function \"calcHeaterExcessTemp \" regularize
-      the discontinuities in equation (9).
-    </p>
-    <p>
-      The radiator exponent according to DIN 442 is valid for the total
-      heat emission. the radiative heat emission part grows larger.
-      This is considered by the following formulas:
-    </p>
-    <table>
-      <caption>
-        \"\" cellspacing=\"0\" cellpadding=\"2\" border=\"1\
-      </caption>
-      <tr>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/n_K1.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (10)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            <img src=
-            \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/n_K2.png\"
-            alt=\"\">
-          </p>
-        </td>
-        <td>
-          <p>
-            <br/>
-            (11)
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td></td>
-        <td></td>
-      </tr>
-    </table>
-    <p>
-      The modified convective exponent is calculated by (11). The
-      region of discontinuity in eq. (11) has not yet been regulized,
-      so a constant radiator exponent is used for now.
-    </p>
-    <p>
-      In the model the heat emission is calculated according to eq.
-      (5), (6) for every layer and the respective power is connected to
-      the romm via the thermal ports. A varHeatSource (inPort=total
-      heat emission) is connected via a thermal port to the enthalpie
-      flow of the heating medium and the stored heat in the radiator
-      mass.
-    </p>
-    <table>
-      <caption>
-        \"\" cellspacing=\"0\" cellpadding=\"2\" border=\"1\
-      </caption>
-      <tr>
-        <td></td>
-      </tr>
-    </table>
-    <h4>
-      <span style=\"color:#008000\">References</span>
-    </h4>
-    <p>
-      Knowing the heat load of the room, an appropriate radiator can be
-      choosen out of a Radiator DataBase via a record. But it is also
-      possible to simulate with arbitrary parameters.
-    </p>
-    <p>
-      The thermal part of the model is adapted from [3] and [1].
-    </p>
-    <ul>
-      <li>[1] Glück, Bernd: Wärmeübertragung - Wärmeabgabe von
-      Raumheizflächen und Rohren, 1990
-      </li>
-      <li>[2] Nadler,Norbert: Die Wärmeleistung von Raumheizkörpern in
-      expliziter Darstellung, In: HLH Lüftung/Klima - Heizung/Sanitär -
-      Gebäudetechnik 11, S.621 - 624, 1991
-      </li>
-      <li>[3] Tritschler, Markus: Bewertung der Genauigkeit von
-      Heizkostenverteilern, Dissertation, Uni Stuttart, 1999
-      </li>
-    </ul>
-    <h4>
-      <span style=\"color:#008000\">Example Results</span>
-    </h4>
-    <p>
-      <a href=
-      \"AixLib.FastHVAC.Examples.HeatExchangers.RadiatorMultiLayer.ValidationRadiator\">
-      ValidationRadiator</a>
-    </p>
+    Equation for multilayer:
   </caption>
+  <tr>
+    <td>
+      <p>
+        <br/>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/DGL_HK.png\"
+        alt=\"Equation for every layer\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (1)
+      </p>
+    </td>
+  </tr>
+</table>
+<p>
+  The total heat emission consists of a convective and a radiative
+  part.
+</p>
+<table cellspacing=\"0\" cellpadding=\"2\" border=\"1\">
+  <tr>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_ab.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (2)
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_K1.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (3)
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_R1.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (4)
+      </p>
+    </td>
+  </tr>
+</table>
+<p>
+  The convective heat emission is proportional to <img src=
+  \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/deltaT.png\"
+  alt=\"\"> &#160;.
+</p>
+<p>
+  The radiative heat emission is proportional to <img src=
+  \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/delta.png\"
+  alt=\"\"> &#160;=(T_L + DeltaT)^4-TR^4 (T_L: Room Temperature, DeltaT:
+  heater excess temperature, T_R: radiative temperature).
+</p>
+<table cellspacing=\"0\" cellpadding=\"2\" border=\"1\">
+  <tr>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_K.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (5)
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Q_R.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (6)
+      </p>
+    </td>
+  </tr>
 </table>
+<p>
+  The heat emission of the radiator depends on the heater excess
+  temperature. In the model it is possible to choose between:
+</p>
+<table cellspacing=\"0\" cellpadding=\"2\" border=\"1\">
+  <tr>
+    <td>
+      <h4>
+        Method
+      </h4>
+    </td>
+    <td>
+      <h4>
+        Formula
+      </h4>
+    </td>
+    <td></td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        arithmetic heater excess temperature
+      </p>
+    </td>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Delta_T_ari.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (7)
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        logarithmic heater excess temperature
+      </p>
+    </td>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Delta_T_log.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (8)
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        exponential heater excess temperature according to [2]
+      </p>
+    </td>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/Delta_T_exp.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (9)
+      </p>
+    </td>
+  </tr>
+</table>
+<p>
+  Due to stability reasons and accuracy at small heating medium flow,
+  an exponential calculation of the heater excess temperture is
+  recommended. The function \"calcHeaterExcessTemp \" regularize the
+  discontinuities in equation (9).
+</p>
+<p>
+  The radiator exponent according to DIN 442 is valid for the total
+  heat emission. the radiative heat emission part grows larger. This is
+  considered by the following formulas:
+</p>
+<table cellspacing=\"0\" cellpadding=\"2\" border=\"1\">
+  <tr>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/n_K1.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (10)
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        <img src=
+        \"modelica://AixLib/Resources/Images//Fluid/HeatExchanger/Radiator/n_K2.png\"
+        alt=\"\">
+      </p>
+    </td>
+    <td>
+      <p>
+        <br/>
+        (11)
+      </p>
+    </td>
+  </tr>
+</table>
+<p>
+  The modified convective exponent is calculated by (11). The region of
+  discontinuity in eq. (11) has not yet been regulized, so a constant
+  radiator exponent is used for now.
+</p>
+<p>
+  In the model the heat emission is calculated according to eq. (5),
+  (6) for every layer and the respective power is connected to the romm
+  via the thermal ports. A varHeatSource (inPort=total heat emission)
+  is connected via a thermal port to the enthalpie flow of the heating
+  medium and the stored heat in the radiator mass.
+</p>
+<h4>
+  <span style=\"color:#008000\">References</span>
+</h4>
+<p>
+  Knowing the heat load of the room, an appropriate radiator can be
+  choosen out of a Radiator DataBase via a record. But it is also
+  possible to simulate with arbitrary parameters.
+</p>
+<p>
+  The thermal part of the model is adapted from [3] and [1].
+</p>
+<ul>
+  <li>[1] Glück, Bernd: Wärmeübertragung - Wärmeabgabe von
+  Raumheizflächen und Rohren, 1990
+  </li>
+  <li>[2] Nadler,Norbert: Die Wärmeleistung von Raumheizkörpern in
+  expliziter Darstellung, In: HLH Lüftung/Klima - Heizung/Sanitär -
+  Gebäudetechnik 11, S.621 - 624, 1991
+  </li>
+  <li>[3] Tritschler, Markus: Bewertung der Genauigkeit von
+  Heizkostenverteilern, Dissertation, Uni Stuttart, 1999
+  </li>
+</ul>
+<h4>
+  <span style=\"color:#008000\">Example Results</span>
+</h4>
+<p>
+  <a href=
+  \"AixLib.FastHVAC.Examples.HeatExchangers.RadiatorMultiLayer.ValidationRadiator\">
+  ValidationRadiator</a>
+</p>
 </html>",
 revisions="<html><ul>
   <li>
diff --git a/AixLib/Obsolete/YearIndependent/FastHVAC/Components/HeatGenerators/HeatPump/HeatPump.mo b/AixLib/Obsolete/YearIndependent/FastHVAC/Components/HeatGenerators/HeatPump/HeatPump.mo
index 25ceeb0a0c..aa9dbb4fe4 100644
--- a/AixLib/Obsolete/YearIndependent/FastHVAC/Components/HeatGenerators/HeatPump/HeatPump.mo
+++ b/AixLib/Obsolete/YearIndependent/FastHVAC/Components/HeatGenerators/HeatPump/HeatPump.mo
@@ -70,7 +70,7 @@ model HeatPump "Base model of FastHVAC Heat Pump"
       group="Heat Losses",
       tab="Condenser",
       enable=use_ConCap));
-  parameter Modelica.Units.SI.ThermalConductance GConIns
+  parameter Modelica.Units.SI.ThermalConductance GConIns=0
     "Constant thermal conductance of condenser material" annotation (Evaluate=
         true, Dialog(
       group="Heat Losses",
@@ -103,7 +103,7 @@ model HeatPump "Base model of FastHVAC Heat Pump"
       group="Heat Losses",
       tab="Evaporator",
       enable=use_EvaCap));
-  parameter Modelica.Units.SI.ThermalConductance GEvaIns
+  parameter Modelica.Units.SI.ThermalConductance GEvaIns=0
     "Constant thermal conductance of Evaporator material" annotation (Evaluate=
         true, Dialog(
       group="Heat Losses",
diff --git a/AixLib/Obsolete/YearIndependent/FastHVAC/Components/Pipes/BaseClasses/PipeBase.mo b/AixLib/Obsolete/YearIndependent/FastHVAC/Components/Pipes/BaseClasses/PipeBase.mo
index 226d4a097f..12a678ab07 100644
--- a/AixLib/Obsolete/YearIndependent/FastHVAC/Components/Pipes/BaseClasses/PipeBase.mo
+++ b/AixLib/Obsolete/YearIndependent/FastHVAC/Components/Pipes/BaseClasses/PipeBase.mo
@@ -24,7 +24,7 @@ model PipeBase
 
     parameter Integer nParallel(min=1)=1 "Number of identical parallel pipes"
     annotation(Dialog(group="Geometry"));
-  parameter Modelica.Units.SI.Length length "Length of pipe"
+  parameter Modelica.Units.SI.Length length=0 "Length of pipe"
     annotation (Dialog(group="Geometry"));
 
     parameter AixLib.DataBase.Pipes.PipeBaseDataDefinition parameterPipe=
diff --git a/AixLib/Obsolete/YearIndependent/FastHVAC/Examples/Chiller/Chiller.mo b/AixLib/Obsolete/YearIndependent/FastHVAC/Examples/Chiller/Chiller.mo
index e758410d0a..9d82bcb625 100644
--- a/AixLib/Obsolete/YearIndependent/FastHVAC/Examples/Chiller/Chiller.mo
+++ b/AixLib/Obsolete/YearIndependent/FastHVAC/Examples/Chiller/Chiller.mo
@@ -123,6 +123,9 @@ model Chiller
     annotation (Placement(transformation(extent={{46,-82},{34,-70}})));
   Modelica.Blocks.Logical.LogicalSwitch logicalSwitch
     annotation (Placement(transformation(extent={{10,-78},{0,-88}})));
+  Controls.Interfaces.VapourCompressionMachineControlBus sigBus1
+    annotation (Placement(transformation(extent={{18,-28},{30,-16}}),
+        iconTransformation(extent={{18,-28},{30,-16}})));
 equation
   connect(dotm_sink.y, fluidSource.dotm) annotation (Line(points={{-77,-72},{-64,
           -72},{-64,-36.6},{-48,-36.6}}, color={0,0,127}));
@@ -146,9 +149,6 @@ equation
     annotation (Line(points={{-30,-33},{-5,-33},{-5,-15}}, color={176,0,0}));
   connect(vessel_ev.enthalpyPort_a, chiller.enthalpyPort_b) annotation (Line(
         points={{-27.3,57},{-20,57},{-20,18},{-5,18},{-5,11}}, color={176,0,0}));
-  connect(iceFac.y, chiller.iceFac_in) annotation (Line(points={{29.4,-12},{
-          26.75,-12},{26.75,-11.88},{21.1333,-11.88}},
-                                                 color={0,0,127}));
   connect(hysHeating.y,not2. u)
     annotation (Line(points={{33.4,-76},{28.8,-76}}, color={255,0,255}));
   connect(logicalSwitch.y,booleanToReal. u) annotation (Line(points={{-0.5,-83},
@@ -170,6 +170,19 @@ equation
           -54},{12,-36},{5.4,-36},{5.4,-17.08}}, color={255,0,255}));
   connect(chiller.nSet, booleanToReal.y) annotation (Line(points={{0.333333,-17.08},
           {0.333333,-38},{-3,-38},{-3,-45.3}}, color={0,0,127}));
+  connect(chiller.sigBus, sigBus1) annotation (Line(
+      points={{8.2,-14.87},{8.2,-22},{24,-22}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(iceFac.y, sigBus1.iceFacMea) annotation (Line(points={{29.6,-14},{
+          24.03,-14},{24.03,-21.97}},
+                          color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(iceFac.y, chiller.iceFac_in) annotation (Line(points={{29.4,-12},{
+          25.2667,-12},{25.2667,-11.88},{21.1333,-11.88}}, color={0,0,127}));
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
             -100},{100,100}}),      graphics={
         Rectangle(
diff --git a/AixLib/Obsolete/package.order b/AixLib/Obsolete/package.order
index a17dc4be9c..d4a1fb12a0 100644
--- a/AixLib/Obsolete/package.order
+++ b/AixLib/Obsolete/package.order
@@ -3,5 +3,6 @@ Year2019
 Year2020
 Year2021
 Year2022
+Year2024
 YearIndependent
 BaseClasses
diff --git a/AixLib/Resources/C-Sources/WeeklySchedule.c b/AixLib/Resources/C-Sources/WeeklySchedule.c
new file mode 100644
index 0000000000..519af8d833
--- /dev/null
+++ b/AixLib/Resources/C-Sources/WeeklySchedule.c
@@ -0,0 +1,439 @@
+/*
+
+  This code implements a weekly schedule.
+
+  Changelog:
+    June 15, 2024 by Filip Jorissen, Builtwins
+          Revisions for #1891: compliance with Modelica include annotation rules.
+    April 9, 2024 by Filip Jorissen, Builtwins
+          Revisions for #1869 to remove a header requirement that contains the number of rows/columns.
+    March 30, 2024 by Filip Jorissen, Builtwins
+          Revisions for #1860 to avoid memory leaks when calling ModelicaFormatError.
+    May 25, 2022 by Michael Wetter, LBNL
+          Refactored to comply with C89.
+    March 9, 2022 by Filip Jorissen, KU Leuven
+         Initial version.
+    April 10, 2022 by Filip Jorissen, KU Leuven
+        Added tableOnFile option.
+
+*/
+
+#include <stdio.h>
+#include <stdlib.h>
+#include <string.h>
+#include <math.h>
+#include "WeeklySchedule.h"
+#include "ModelicaUtilities.h"
+
+#ifndef WEEKCAL_c
+#define WEEKCAL_c
+
+
+int cmpfun(const void * tuple1, const void * tuple2) {
+  const double time1 = (*(const TimeDataTuple **)tuple1)->time;
+  const double time2 = (*(const TimeDataTuple **)tuple2)->time;
+  return  (time1 - time2);
+}
+
+void* weeklyScheduleInit(const int tableOnFile, const char* name, const double t_offset, const char* stringData) {
+  const int bufLen = 255;
+  const int allocSize = 50;
+  WeeklySchedule* scheduleID = NULL;
+
+
+  int i = 0;              /* iterator */
+  int j = 0;              /* iterator */
+  int k = 0;              /* iterator */
+  int index = 0;          /* index in the token buffer where we are currently writing */
+  int line = 0;           /* number of parsed lines */
+  int rule_i = 0;         /* rule index where we are currently writing */
+  int foundHeader = 0;    /* indicates whether a header has been found */
+  int isHeaderLine = 0;   /* indicates whether we are currently parsing the header line */
+  int tokensInLine = 0;   /* keeps track of the number of tokens in the current line: column index and sanity check */
+  int tokensInFirstLine = 0;
+  int comment = 0;        /* we are parsing a comment */
+  int n_reservedRules = 0;/* number of rules for which we have allocated memory */
+  int n_reservedColumns = allocSize;/* number of columns for which we have allocated memory */
+  int n_rulesInRow = 0;   /* number of rules that exist in the current row */
+  int n_newLines = 0;     /* number of newlines */
+  int mustHaveNewLine = 0;/* The next character must be a newline */
+  char c;                 /* the character that is being parsed in this iteration */
+
+
+  int parseToken = 0;
+  double timeStamp;
+  int tokenLen;
+  int offset = 0;
+
+  scheduleID = (WeeklySchedule*)calloc(1, sizeof(WeeklySchedule));
+  if ( scheduleID == NULL){
+    ModelicaFormatError("Failed to allocate memory for scheduleID in WeeklySchedule.c.");
+  }
+
+  scheduleID->n_allocatedRules = 0;
+  scheduleID->n_allocatedRulesData = 0;
+  scheduleID->lastData = NULL;
+  scheduleID->token = NULL;
+  scheduleID->fp = NULL;
+  scheduleID->buff2 = NULL;
+  scheduleID->rules = NULL;
+
+  scheduleID->token = (char*)calloc(sizeof(char), bufLen);
+  if ( scheduleID->token == NULL){
+      weeklyScheduleFreeInit(scheduleID);
+      weeklyScheduleFree(scheduleID);
+      ModelicaFormatError("Failed to allocate memory for token in WeeklySchedule.c.");
+  }
+
+  if (tableOnFile){
+      scheduleID->fp = fopen(name, "r");
+    if (scheduleID->fp == NULL) {
+      weeklyScheduleFreeInit(scheduleID);
+      weeklyScheduleFree(scheduleID);
+      ModelicaFormatError("Failed to open weekly schedule '%s'.", name);
+    }
+  }
+
+  scheduleID->buff2 = (char*)calloc(sizeof(char), bufLen);
+  if (scheduleID->buff2 == NULL){
+      weeklyScheduleFreeInit(scheduleID);
+      weeklyScheduleFree(scheduleID);
+      ModelicaFormatError("Failed to allocate memory for buff in WeeklySchedule.c.");
+  }
+
+  scheduleID->rules = (TimeDataTuple**)calloc(sizeof(TimeDataTuple *), allocSize);
+  if ( scheduleID->rules == NULL){
+    weeklyScheduleFreeInit(scheduleID);
+    weeklyScheduleFree(scheduleID);
+    ModelicaFormatError("Failed to allocate memory for rules in WeeklySchedule.c.");
+  }
+  n_reservedRules = allocSize;
+
+  /* Identify 'tokens' by splitting on (one or more) whitespace characters. */
+  /* Each token is parsed and special behaviour is created for comments and the header. */
+  /* The first column is analysed and split in (one or more) days (which can be comma separated), and hours, minutes, seconds. */
+  /* The format is day1,day2,day3:23:59:59 where day* is one of mon, tue, wed, thu, fri, sat, sun. */
+  /* All later columns contain data, where '-' serves as a wildcard, where data from the previous rule is reused. */
+  /* Rules are sorted by timestamp and then expanded, where '-' is filled in. */
+  while ( 1 ) {
+    parseToken = 0;
+
+    if (tableOnFile){
+      c = fgetc( scheduleID->fp ); /* read a character from the file */
+    }else{
+      c = stringData[j]; /* read a character from the string */
+      j++;
+    }
+    if ( c == EOF || c == '\0') {
+      if (!tableOnFile && c == '\0'){
+        break;
+      }else if (tableOnFile && feof(scheduleID->fp)) {
+        break; /* exit the while loop */
+      } else {
+        weeklyScheduleFreeInit(scheduleID);
+        weeklyScheduleFree(scheduleID);
+        ModelicaFormatError("Error while reading file '%s'.", name);
+      }
+    }{
+      if (index >= bufLen - 2) {
+        weeklyScheduleFreeInit(scheduleID);
+        weeklyScheduleFree(scheduleID);
+        ModelicaFormatError("Buffer overflow when reading weekly schedule '%s'.", name);
+      }
+
+
+      if (c == '\n') { /* Check whether a token ends */
+        parseToken = 1;
+        mustHaveNewLine = 0;
+        n_newLines++;
+      } else if (mustHaveNewLine == 1){
+        weeklyScheduleFreeInit(scheduleID);
+        weeklyScheduleFree(scheduleID);
+        ModelicaFormatError("Error while reading weekly schedule '%s'. Inconsistent line endings: \\r must be followed by \\n.", name);
+      } else if (c == '\r') { /* Check whether a token ends */
+        mustHaveNewLine = 1;
+      } else if (comment == 1 || c == '#') {
+        comment = 1;
+        continue; /* ignore this character and the next characters until a newline is detected, then parse the token */
+      } else if ( isHeaderLine == 0 && (c == ' ' || c == '\t' ) && index > 0) { /* parse token when reaching a space or tab, unless buffer is empty */
+        parseToken = 1;
+      } else if (c != ' ' && c != '\t' ) { /* build up the token by copying a character */
+        scheduleID->token[index] = c;
+        index++;
+      }
+
+
+      /* Parse a token if needed. */
+      if (parseToken == 1 && index > 0) {
+        /* shouldn't require an overflow check since token is already checked */
+
+        offset = 0;
+
+        scheduleID->token[index] = '\0';
+        index++;
+        tokenLen = strlen(scheduleID->token);
+        index = 0;
+
+        if (foundHeader == 0 && strcmp("double", scheduleID->token) == 0) {
+		  /* we found a header line, we expect a specific format after the whitespace */
+          foundHeader = 1; /* Avoid checking header line again */
+          comment = 1; /* Ignore the rest of the line */
+          ModelicaFormatWarning("Detected header line when reading weekly schedule '%s'. This is deprecated. Consider removing the line that starts with 'double tab1'.", name);
+        } else if (tokensInLine == 0) {
+          /* 0 tokens have been found on this line, so we're parsing a date/time */
+          const int ncharsDays = strcspn(scheduleID->token, ":");
+          timeStamp = 0;
+          if (tokenLen  != ncharsDays) {
+            double val;
+            const int ncharsHour = strcspn(scheduleID->token + ncharsDays + 1, ":");
+
+            strncpy(scheduleID->buff2, scheduleID->token + ncharsDays + 1, ncharsHour);
+            scheduleID->buff2[ncharsHour] = '\0';
+            if (sscanf(scheduleID->buff2, "%lf", &val) != 1) {
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Error in float conversion in hours when reading weekly schedule '%s'. Found token %s with length %i", name, scheduleID->buff2, ncharsHour);
+            }
+            if (val > 24 || val < 0) {
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Unexpected value for hour: '%f' when reading weekly schedule '%s', should be between 0 and 24.", val, name);
+            }
+            timeStamp += val * 3600;
+
+            if (tokenLen != ncharsHour + ncharsDays + 1) {
+              const int ncharsMinutes = strcspn(scheduleID->token + ncharsDays + ncharsHour + 2, ":");
+              strncpy(scheduleID->buff2, scheduleID->token + ncharsDays + ncharsHour + 2, ncharsMinutes);
+              scheduleID->buff2[ncharsMinutes] = '\0';
+              if (sscanf(scheduleID->buff2, "%lf", &val) != 1) {
+                weeklyScheduleFreeInit(scheduleID);
+                weeklyScheduleFree(scheduleID);
+                ModelicaFormatError("Error in float conversion in minutes when reading weekly schedule '%s'.", name);
+              }
+              if (val > 60 || val < 0) {
+                weeklyScheduleFreeInit(scheduleID);
+                weeklyScheduleFree(scheduleID);
+                ModelicaFormatError("Unexpected value for minute: '%f' when reading weekly schedule '%s', should be between 0 and 60.", val, name);
+              }
+              timeStamp += val * 60;
+
+              if (tokenLen != ncharsMinutes + ncharsHour + ncharsDays + 2) {
+                const int ncharsSeconds = tokenLen - ncharsMinutes - ncharsHour - ncharsDays - 2;
+                strncpy(scheduleID->buff2, scheduleID->token + ncharsDays + ncharsHour + ncharsMinutes + 3, ncharsSeconds);
+                scheduleID->buff2[ncharsSeconds] = '\0';
+                if (sscanf(scheduleID->buff2, "%lf", &val) != 1) {
+                  weeklyScheduleFreeInit(scheduleID);
+                  weeklyScheduleFree(scheduleID);
+                  ModelicaFormatError("Error in float conversion in seconds when reading weekly schedule '%s'.", name);
+                }
+                if (val > 60 || val < 0) {
+                  weeklyScheduleFreeInit(scheduleID);
+                  weeklyScheduleFree(scheduleID);
+                  ModelicaFormatError("Unexpected value for seconds: '%f' when reading weekly schedule '%s', should be between 0 and 60.", val, name);
+                }
+                timeStamp += val;
+              }
+            }
+          }
+          strncpy(scheduleID->buff2, scheduleID->token, ncharsDays);
+          scheduleID->buff2[ncharsDays] = '\0';
+
+
+          /* loop over all days (comma separated) and for each date, add a rule */
+          while ( 1 ) {
+            char * startIndex = scheduleID->buff2 + offset;
+            double t_day, time_i;
+            int nchars = strcspn(startIndex, ",");
+
+            if (nchars != 3 ) {
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Unexpected day format when reading weekly schedule '%s': %s.", name, startIndex);
+            }
+
+            if (strncmp("mon", startIndex, 3) == 0) {
+              t_day = 0;
+            } else if (strncmp("tue", startIndex, 3) == 0) {
+              t_day = 1 * 3600 * 24;
+            } else if (strncmp("wed", startIndex, 3) == 0) {
+              t_day = 2 * 3600 * 24;
+            } else if (strncmp("thu", startIndex, 3) == 0) {
+              t_day = 3 * 3600 * 24;
+            } else if (strncmp("fri", startIndex, 3) == 0) {
+              t_day = 4 * 3600 * 24;
+            } else if (strncmp("sat", startIndex, 3) == 0) {
+              t_day = 5 * 3600 * 24;
+            } else if (strncmp("sun", startIndex, 3) == 0) {
+              t_day = 6 * 3600 * 24;
+            } else {
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Unexpected day format when parsing weekday '%s': %s.", name, startIndex);
+            }
+
+            /* expand the memory if the initially assigned memory block does not suffice*/
+            if (rule_i >= n_reservedRules) {
+              n_reservedRules += allocSize;
+              scheduleID->rules = (TimeDataTuple**)realloc(scheduleID->rules, sizeof(TimeDataTuple*) * n_reservedRules);
+              if (scheduleID->rules == NULL) {
+                weeklyScheduleFreeInit(scheduleID);
+                weeklyScheduleFree(scheduleID);
+                ModelicaFormatError("Failed to reallocate memory when reading weekly schedule '%s'.", name);
+              }
+            }
+
+            time_i = timeStamp + t_day;
+            scheduleID->rules[rule_i] = (TimeDataTuple*)calloc(sizeof(TimeDataTuple), 1);
+            if ( scheduleID->rules[rule_i] == NULL){
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Failed to allocate memory for rules[rule_i] in WeeklySchedule.c.");
+            }
+            scheduleID->n_allocatedRules++;
+
+            scheduleID->rules[rule_i]->time = time_i;
+            scheduleID->rules[rule_i]->data = (double*)calloc(sizeof(double), n_reservedColumns);
+            if ( scheduleID->rules[rule_i]->data == NULL){
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Failed to allocate memory for rules[rule_i]->data in WeeklySchedule.c.");
+            }
+            scheduleID->n_allocatedRulesData++;
+
+            rule_i++;
+            n_rulesInRow++;
+
+            if (strlen(startIndex) == 3) { /*reached the end of the substring*/
+              break;
+            }
+            offset = offset + 4; /* the length of a token and a comma*/
+          }
+
+          tokensInLine++;
+        } else if (tokensInLine > 0) {
+          double val;
+
+          /* a token has been found on this line before, so we're parsing some numerical data*/
+          if (tokensInFirstLine != 0 && tokensInLine + 1 > tokensInFirstLine){
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Too many columns on data line %i when reading weekly schedule '%s'. %i instead of %i.", line, name, tokensInLine + 1, tokensInFirstLine);
+          }else if (tokensInLine >= n_reservedColumns) { /* This code should only be reached upon passing the first line of data */
+            n_reservedColumns += allocSize;
+            scheduleID->rules[rule_i-1]->data = (double*)realloc(scheduleID->rules[rule_i-1]->data, sizeof(double)*n_reservedColumns);
+            if ( scheduleID->rules[rule_i-1]->data == NULL){
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Failed to reallocate memory for rules[rule_i-1]->data in WeeklySchedule.c.");
+            }
+          }
+
+          if (sscanf(scheduleID->token, "%lf", &val) != 1) {
+            if (scheduleID->token[0] == '-') {
+              val = HUGE_VAL; /*convert the wildcard in a double representation*/
+            } else {
+              weeklyScheduleFreeInit(scheduleID);
+              weeklyScheduleFree(scheduleID);
+              ModelicaFormatError("Invalid format for float %s  when reading weekly schedule '%s'.", scheduleID->token, name);
+            }
+
+          }
+          /* Set the data for all rules that result from this row.*/
+          for (i = rule_i - n_rulesInRow; i < rule_i; ++i) {
+            scheduleID->rules[i]->data[tokensInLine - 1] = val;
+          }
+
+          tokensInLine++;
+        } else {
+          weeklyScheduleFreeInit(scheduleID);
+          weeklyScheduleFree(scheduleID);
+          ModelicaFormatError("Logic error when reading weekly schedule '%s'.", name); /*should not be able to end up here*/
+        }
+      }
+      if (c == '\n') { 
+        if (tokensInFirstLine == 0 && tokensInLine > 0){
+          tokensInFirstLine = tokensInLine;
+        }else if (tokensInLine > 0 && tokensInLine != tokensInFirstLine) {
+          weeklyScheduleFreeInit(scheduleID);
+          weeklyScheduleFree(scheduleID);
+          ModelicaFormatError("Too few columns on data line %i when reading weekly schedule '%s'. %i instead of %i", line, name, tokensInLine, tokensInFirstLine);
+        }
+
+        /*reset some internal variables*/
+        line++;
+        tokensInLine = 0;
+        comment = 0;
+        n_rulesInRow = 0;
+      }
+    }
+  }
+
+  if (n_newLines==0){
+    weeklyScheduleFreeInit(scheduleID);
+    weeklyScheduleFree(scheduleID);
+    ModelicaFormatError("In weekly schedule '%s': The provided %s is incorrectly formatted since it does not contain newline characters.", name, tableOnFile ? "file": "string parameter");
+  }
+
+  /* sort all data by time stamp*/
+  qsort(scheduleID->rules, rule_i, sizeof(TimeDataTuple*), cmpfun);
+
+  {
+    /* working vector with zero initial value*/
+    scheduleID->lastData = (double*)calloc(sizeof(double), tokensInFirstLine - 1);
+    if (scheduleID->lastData == NULL){
+      weeklyScheduleFreeInit(scheduleID);
+      weeklyScheduleFree(scheduleID);
+      ModelicaFormatError("Failed to allocate memory for lastData in WeeklySchedule.c., tokensInFirstLine - 1 = %d", tokensInFirstLine - 1);
+    }
+
+    memset(scheduleID->lastData, (char)(double)0, tokensInFirstLine - 1); /* set vector to zero initial guess*/
+
+    /* Loop over all data and fill in wildcards using the last preceeding value.*/
+    /* This may wrap back to the end of last week, therefore loop the data twice.*/
+    /* If an entire column contains wildcards then use a default value of zero.*/
+
+    for (i = 0; i < 2; ++i) {
+      for (j = 0; j < rule_i; ++j) {
+        for (k = 0; k < tokensInFirstLine - 1; ++k) {
+          if ( scheduleID->rules[j]->data[k] != HUGE_VAL ) {
+            scheduleID->lastData[k] = scheduleID->rules[j]->data[k];
+          } else if (i > 0) {
+            /* only on the second pass, since otherwise the default value is filled in permanently and
+               information from the back of the domain can't be recycled */
+            scheduleID->rules[j]->data[k] = scheduleID->lastData[k];
+          }
+        }
+      }
+    }
+  }
+
+  /* store data for later use */
+  scheduleID->t_offset = t_offset;
+  scheduleID->previousIndex = 0;
+  scheduleID->previousTimestamp = HUGE_VAL;
+  scheduleID->n_data_cols = tokensInFirstLine - 1;
+
+  weeklyScheduleFreeInit(scheduleID);
+
+  return (void*) scheduleID;
+}
+
+
+void weeklyScheduleFreeInit(void * ID) {
+  WeeklySchedule* scheduleID = (WeeklySchedule*)ID;
+
+  if (scheduleID->lastData != NULL)
+    free(scheduleID->lastData);
+
+  if (scheduleID->token != NULL)
+    free(scheduleID->token);
+
+  if (scheduleID->fp != NULL)
+    fclose(scheduleID->fp);
+
+  if (scheduleID->buff2 != NULL)
+    free(scheduleID->buff2);
+
+}
+
+#endif
diff --git a/AixLib/Resources/C-Sources/WeeklySchedule.h b/AixLib/Resources/C-Sources/WeeklySchedule.h
new file mode 100644
index 0000000000..0c7e7229c1
--- /dev/null
+++ b/AixLib/Resources/C-Sources/WeeklySchedule.h
@@ -0,0 +1,54 @@
+/*
+
+  This code implements a weekly schedule.
+  See modelica model for documentation.
+
+
+  Changelog:
+    March 9, 2022 by Filip Jorissen, KU Leuven
+        Initial version.
+    April 10, 2022 by Filip Jorissen, KU Leuven
+        Added tableOnFile option.
+
+*/
+
+
+#ifndef WEEKCAL_h
+#define WEEKCAL_h
+
+
+typedef struct TimeDataTuple {
+  double time;	/* Time relative to monday midnight. */
+  double *data; /* Corresponding column data */
+} TimeDataTuple;
+
+
+typedef struct WeeklySchedule {
+  double t_offset;      /* Time offset for monday, midnight. */
+  int n_data_cols;      /* Number of used input columns */
+  int n_allocatedRules; /* Number rules for which a struct was allocated */
+  int n_allocatedRulesData; /* Number rules for which a data vector was allocated */
+
+  double previousTimestamp; /* Time where the schedule was called the previous time */
+  int previousIndex;        /* Index where the schedule was called the previous time */
+
+
+  double * lastData;    /* A work vector */
+  char * token;         /* A piece of input string that is being parsed */
+  FILE* fp;             /* A file pointer */
+  char* buff2;          /* A text buffer */
+  struct TimeDataTuple **rules; /* An array of rule pointers */
+
+} WeeklySchedule;
+
+
+
+void* weeklyScheduleInit(const int tableOnFile, const char* name, const double t_offset, const char* stringData);
+
+void weeklyScheduleFree(void * ID);
+
+void weeklyScheduleFreeInit(void * ID);
+
+double getScheduleValue(void * ID, const int column, const double time);
+
+#endif
diff --git a/AixLib/Resources/C-Sources/WeeklyScheduleFree.c b/AixLib/Resources/C-Sources/WeeklyScheduleFree.c
new file mode 100644
index 0000000000..63f863b7e5
--- /dev/null
+++ b/AixLib/Resources/C-Sources/WeeklyScheduleFree.c
@@ -0,0 +1,44 @@
+/*
+
+  This code implements a weekly schedule.
+
+  Changelog:
+    June 15, 2024 by Filip Jorissen, Builtwins
+          Initial version for #1891: compliance with Modelica include annotation rules.
+
+*/
+
+#include <stdio.h>
+#include <stdlib.h>
+#include <string.h>
+#include <math.h>
+#include "WeeklySchedule.h"
+#include "ModelicaUtilities.h"
+
+#ifndef WEEKCALFREE_c
+#define WEEKCALFREE_c
+
+
+void weeklyScheduleFree(void * ID) {
+  int i;
+  WeeklySchedule* scheduleID = (WeeklySchedule*)ID;
+
+  if (ID == NULL) /* Otherwise OM segfaults when IBPSA.Utilities.IO.Files.Examples.WeeklySchedule triggers an error */
+    return;
+
+  for (i = 0; i < scheduleID->n_allocatedRulesData; ++i) {
+    free(scheduleID->rules[i]->data);
+  }
+ 
+  for (i = 0; i < scheduleID->n_allocatedRules; ++i) {
+    free(scheduleID->rules[i]);
+  }
+
+  if (scheduleID->rules != NULL)
+    free(scheduleID->rules);
+
+  free(ID);
+  ID = NULL;
+}
+
+#endif
diff --git a/AixLib/Resources/C-Sources/WeeklyScheduleGetValue.c b/AixLib/Resources/C-Sources/WeeklyScheduleGetValue.c
new file mode 100644
index 0000000000..96098df26d
--- /dev/null
+++ b/AixLib/Resources/C-Sources/WeeklyScheduleGetValue.c
@@ -0,0 +1,69 @@
+/*
+
+  This code implements a weekly schedule.
+
+  Changelog:
+    June 15, 2024 by Filip Jorissen, Builtwins
+          Initial version for #1891: compliance with Modelica include annotation rules.
+
+*/
+
+
+#include <stdio.h>
+#include <stdlib.h>
+#include <string.h>
+#include <math.h>
+#include "WeeklySchedule.h"
+#include "ModelicaUtilities.h"
+
+#ifndef WEEKCALGET_c
+#define WEEKCALGET_c
+
+
+/* Get a column value. Cache the last used row internally to speed up lookup. */
+double getScheduleValue(void * ID, const int column, const double modelicaTime) {
+  WeeklySchedule* scheduleID = (WeeklySchedule*)ID;
+  /* extrapolation for weeks that are outside of the user-defined range */
+  double t = modelicaTime - scheduleID->t_offset;
+  const double weekLen = 7 * 24 * 3600;
+  double time = fmod(t - weekLen * floor(t / weekLen), weekLen);
+  int i;
+  const int columnIndex = column - 1; /* Since we do not store the time indices in the data table */
+
+  /* Not calling weeklyScheduleFreeInit() or weeklyScheduleFree() since weeklyScheduleFreeInit() has already been called at the end of the
+  initialization and Modelica will call weeklyScheduleFree() upon a call of ModelicaFormatError) */
+  if (column < 0 || column > scheduleID->n_data_cols) {
+    ModelicaFormatError("The requested column index '%i' is outside of the table range '%i'.", column + 1, scheduleID->n_data_cols);
+  }
+  if (column == 0 ) {
+    ModelicaFormatError("The column index 1 is not a data column and is reserved for 'time'. It should not be read.");
+  }
+
+
+  if (time == scheduleID->previousTimestamp) {
+    i = scheduleID->previousIndex;
+  } else if (time > scheduleID->rules[scheduleID->previousIndex]->time) {
+    for (i = scheduleID->previousIndex; i < scheduleID->n_allocatedRules - 1; i ++) {
+      if (scheduleID->rules[i + 1]->time > time) {
+        break;
+      }
+    }
+  } else {
+    for (i = scheduleID->previousIndex; i > 0; i--) {
+      if (scheduleID->rules[i - 1]->time < time) {
+        i = i - 1;
+        break;
+      }
+    }
+    /* if time is smaller than the first row, wrap back to the end of the week */
+    if (i == 0 && scheduleID->rules[0]->time > time) {
+      i = scheduleID->n_allocatedRules - 1;
+    }
+  }
+  scheduleID->previousIndex = i;
+  scheduleID->previousTimestamp = time;
+
+  return scheduleID->rules[i]->data[columnIndex];
+}
+
+#endif
diff --git a/AixLib/Resources/C-Sources/fileWriterFree.c b/AixLib/Resources/C-Sources/fileWriterFree.c
index 414ed1fc71..0c4ac49c91 100644
--- a/AixLib/Resources/C-Sources/fileWriterFree.c
+++ b/AixLib/Resources/C-Sources/fileWriterFree.c
@@ -2,6 +2,10 @@
  *
  * Michael Wetter, LBNL                     2018-05-12
  */
+
+#ifndef IBPSA_FILEWRITERFree_c
+#define IBPSA_FILEWRITERFree_c
+
 #include <stdlib.h>
 #include <stdio.h>
 #include "ModelicaUtilities.h"
@@ -22,7 +26,7 @@ void prependString(const char* fileName, const char* string){
   if(fseek(fr, 0, SEEK_SET)!=0)
     ModelicaFormatError("The file %s could not be read.", fileName);
 
-  origString = malloc(fsize + 1);
+  origString = (char *)malloc((fsize + 1) * sizeof(char));
   if ( origString == NULL ){
     /* not enough memory is available: file too large */
     ModelicaError("Not enough memory in fileWriterInit.c for prepending string.");
@@ -62,3 +66,5 @@ void fileWriterFree(void* ptrFileWriter){
 
   return;
 }
+
+#endif
diff --git a/AixLib/Resources/C-Sources/fileWriterStructure.c b/AixLib/Resources/C-Sources/fileWriterStructure.c
index cb32894d11..fafbbc18b8 100644
--- a/AixLib/Resources/C-Sources/fileWriterStructure.c
+++ b/AixLib/Resources/C-Sources/fileWriterStructure.c
@@ -1,6 +1,9 @@
 #ifndef IBPSA_FILEWRITERStructure_c
 #define IBPSA_FILEWRITERStructure_c
 
+#include <stdlib.h>
+#include <string.h>
+
 #include "ModelicaUtilities.h"
 
 #include "fileWriterStructure.h"
@@ -23,8 +26,8 @@ void* allocateFileWriter(
 
   if ( FileWriterNames_n == 0 ){
     /* Allocate memory for array of file names */
-    FileWriterNames = malloc(sizeof(char*));
-    InstanceNames = malloc(sizeof(char*));
+    FileWriterNames = (char **)malloc(sizeof(char*));
+    InstanceNames = (char **)malloc(sizeof(char*));
     if ( FileWriterNames == NULL || InstanceNames == NULL)
       ModelicaError("Not enough memory in fileWriterStructure.c for allocating FileWriterNames and InstanceNames.");
   }
@@ -36,14 +39,14 @@ void* allocateFileWriter(
       instanceName, fileName, InstanceNames[index]);
     }
     /* Reallocate memory for array of file names */
-    FileWriterNames = realloc(FileWriterNames, (FileWriterNames_n+1) * sizeof(char*));
-    InstanceNames = realloc(InstanceNames, (FileWriterNames_n+1) * sizeof(char*));
+    FileWriterNames = (char **)realloc(FileWriterNames, (FileWriterNames_n+1) * sizeof(char*));
+    InstanceNames = (char **)realloc(InstanceNames, (FileWriterNames_n+1) * sizeof(char*));
     if ( FileWriterNames == NULL || InstanceNames == NULL )
       ModelicaError("Not enough memory in fileWriterStructure.c for reallocating FileWriterNames and InstanceNames.");
   }
   /* Allocate memory for this file name */
-  FileWriterNames[FileWriterNames_n] = malloc((strlen(fileName)+1) * sizeof(char));
-  InstanceNames[FileWriterNames_n] = malloc((strlen(instanceName)+1) * sizeof(char));
+  FileWriterNames[FileWriterNames_n] = (char *)malloc((strlen(fileName)+1) * sizeof(char));
+  InstanceNames[FileWriterNames_n] = (char *)malloc((strlen(instanceName)+1) * sizeof(char));
   if ( FileWriterNames[FileWriterNames_n] == NULL || InstanceNames[FileWriterNames_n] == NULL)
     ModelicaError("Not enough memory in fileWriterStructure.c for allocating FileWriterNames[] and InstanceNames[].");
   /* Copy the file name */
@@ -55,12 +58,12 @@ void* allocateFileWriter(
   if ( ID == NULL )
     ModelicaFormatError("Not enough memory in fileWriterStructure.c for allocating ID of FileWriter %s.", instanceName);
 
-  ID->fileWriterName = malloc((strlen(fileName)+1) * sizeof(char));
+  ID->fileWriterName = (char *)malloc((strlen(fileName)+1) * sizeof(char));
   if ( ID->fileWriterName == NULL )
     ModelicaFormatError("Not enough memory in fileWriterStructure.c for allocating ID->fileWriterName in FileWriter %s.", instanceName);
   strcpy(ID->fileWriterName, fileName);
 
-  ID->instanceName = malloc((strlen(instanceName)+1) * sizeof(char));
+  ID->instanceName = (char *)malloc((strlen(instanceName)+1) * sizeof(char));
   if ( ID->instanceName == NULL )
     ModelicaFormatError("Not enough memory in fileWriterStructure.c for allocating ID->instanceName in FileWriter %s.", instanceName);
   strcpy(ID->instanceName, instanceName);
diff --git a/AixLib/Resources/C-Sources/getTimeSpan.c b/AixLib/Resources/C-Sources/getTimeSpan.c
index 63cab8d20b..755d7aae4d 100644
--- a/AixLib/Resources/C-Sources/getTimeSpan.c
+++ b/AixLib/Resources/C-Sources/getTimeSpan.c
@@ -6,6 +6,9 @@
 #define GETTIMESPAN_C_
 
 #include <stdio.h>
+#include <stdlib.h>
+#include <string.h>
+
 #include "ModelicaUtilities.h"
 
 #include "getTimeSpan.h"
@@ -24,7 +27,7 @@
 char *concat(const char *s1, const char *s2) {
   const size_t len1 = strlen(s1);
   const size_t len2 = strlen(s2);
-  char *result = malloc(len1 + len2 + 1);
+  char *result = (char *)malloc((len1 + len2 + 1) * sizeof(char));
   if (result == NULL) {
     ModelicaError("Failed to allocate memory in getTimeSpan.c");
   }
diff --git a/AixLib/Resources/C-Sources/jsonWriterInit.c b/AixLib/Resources/C-Sources/jsonWriterInit.c
index 8970dc4521..5e19354b49 100644
--- a/AixLib/Resources/C-Sources/jsonWriterInit.c
+++ b/AixLib/Resources/C-Sources/jsonWriterInit.c
@@ -5,6 +5,12 @@
  * Filip Jorissen, KU Leuven
  */
 
+#ifndef IBPSA_JSONWRITERINIT_c
+#define IBPSA_JSONWRITERINIT_c
+
+#include <stdlib.h>
+#include <string.h>
+
 #include "fileWriterStructure.c"
 #include "ModelicaUtilities.h"
 
@@ -26,16 +32,16 @@ void* jsonWriterInit(
 
   ID->numKeys=numKeys;
 
-  ID-> varKeys = malloc(numKeys * sizeof(char*));
+  ID-> varKeys = (char **)malloc(numKeys * sizeof(char*));
   if ( ID->varKeys == NULL )
     ModelicaError("Not enough memory in jsonWriterInit.c for allocating varKeys[].");
-  ID-> varVals = malloc(numKeys * sizeof(double));
+  ID-> varVals = (double *)malloc(numKeys * sizeof(double));
   if ( ID->varVals == NULL )
     ModelicaError("Not enough memory in jsonWriterInit.c for allocating varVals[].");
 
   for (i = 0; i < numKeys; ++i)
   {
-    ID-> varKeys[i] = malloc((strlen(varKeys[i])+1) * sizeof(char*));
+    ID-> varKeys[i] = (char *)malloc((strlen(varKeys[i])+1) * sizeof(char));
     if ( ID->varKeys[i] == NULL )
       ModelicaError("Not enough memory in jsonWriterInit.c for allocating varKeys.");
       strcpy(ID->varKeys[i], varKeys[i]);
@@ -90,3 +96,5 @@ void writeJson(void *ptrFileWriter,  const double* varVals, const int numVals){
   if (fclose(fOut) == EOF)
     ModelicaFormatError("In writeJson.c: Returned an error when closing %s.", ID->fileWriterName);
 }
+
+#endif
diff --git a/AixLib/Resources/Data/Fluid/HeatPumps/ModularReversible/BaseClasses/LargeScaleWaterToWaterDeclarations.xlsx b/AixLib/Resources/Data/Fluid/HeatPumps/ModularReversible/BaseClasses/LargeScaleWaterToWaterDeclarations.xlsx
new file mode 100644
index 0000000000..c609e812af
Binary files /dev/null and b/AixLib/Resources/Data/Fluid/HeatPumps/ModularReversible/BaseClasses/LargeScaleWaterToWaterDeclarations.xlsx differ
diff --git a/AixLib/Resources/Data/Fluid/HeatPumps/Validation/MeasuredHeatPumpData.txt b/AixLib/Resources/Data/Fluid/HeatPumps/Validation/MeasuredHeatPumpData.txt
new file mode 100644
index 0000000000..69cf3ff528
--- /dev/null
+++ b/AixLib/Resources/Data/Fluid/HeatPumps/Validation/MeasuredHeatPumpData.txt
@@ -0,0 +1,14369 @@
+#1
+double MeasuredData(14366, 10)
+#time_in_s	HP/Temperatures/T_Water_return	HP/Temperatures/T_Water_supply	HP/Power/Total_effPow	HP/Temperatures/T_Amb	HP/Status/Status_Pump_Brine_Run	HP/Status/Status_Compressor_Run	HP/Status/Status_Pump_IntHeat_Run	HP/Temperatures/T_Brine_out	HP/Temperatures/T_Brine_in
+0.0	297.85000076293943	300.85000076293943	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.45000019073484	288.7500003814697
+1.0	297.85000076293943	300.85000076293943	0.0799999982118606	294.04999961853025	0.0	0.0	0.0	288.45000019073484	288.7500003814697
+2.0	297.85000076293943	300.85000076293943	0.0799999237060546	294.04999961853025	0.0	0.0	0.0	288.45000019073484	288.7500003814697
+3.0	297.85000076293943	300.85000076293943	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+4.0	297.85000076293943	300.85000076293943	0.0799999982118606	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+5.0	297.85000076293943	300.85000076293943	-5.279999732971191	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+6.0	297.85000076293943	300.85000076293943	-5.599999904632568	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+7.0	297.85000076293943	300.85000076293943	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+8.0	297.85000076293943	300.85000076293943	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+9.0	297.85000076293943	300.85000076293943	0.0799999982118606	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+10.0	297.85000076293943	300.85000076293943	0.0799999237060546	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+11.0	297.85000076293943	300.85000076293943	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+12.0	297.85000076293943	300.85000076293943	-4.080655895343408	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+13.0	297.85000076293943	300.85000076293943	-2.7339317240684733	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+14.0	297.85000076293943	300.85000076293943	-4.938813518428267	294.1321004121713	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+15.0	297.85000076293943	300.85000076293943	-5.440000057220459	294.07020576003043	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+16.0	297.85000076293943	300.85000076293943	-1.0301650504618136	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+17.0	297.85000076293943	300.85000076293943	-4.335045572580593	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+18.0	297.85000076293943	300.85000076293943	-1.0197436975857537	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+19.0	297.85000076293943	300.85000076293943	0.07999998343846727	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+20.0	297.85000076293943	300.85000076293943	-4.350676703639641	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+21.0	297.85000076293943	300.85000076293943	-1.0041170534967545	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+22.0	297.85000076293943	300.85000076293943	-8.287273705531558	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+23.0	297.85000076293943	300.85000076293943	-6.389211146772471	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+24.0	297.85000076293943	300.85000076293943	-5.3754854544242106	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+25.0	297.85000076293943	300.85000076293943	-5.42459025181343	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+26.0	297.85000076293943	300.85000076293943	-5.375334419450671	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+27.0	297.85000076293943	300.85000076293943	-0.9575983244706947	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+28.0	297.85000076293943	300.85000076293943	0.07999998407126546	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+29.0	297.85000076293943	300.85000076293943	-8.810223128414973	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+30.0	297.85000076293943	300.85000076293943	-1.9794313407095814	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+31.0	297.85000076293943	300.85000076293943	-4.407979063739552	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+32.0	297.85000076293943	300.85000076293943	-9.933188755687567	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+33.0	297.85000076293943	300.85000076293943	2.5351978132209005	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+34.0	297.85000076293943	300.85000076293943	1.096390926421516	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+35.0	297.85000076293943	300.85000076293943	0.014654841670447921	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+36.0	297.85000076293943	300.85000076293943	-4.289725960312569	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+37.0	297.85000076293943	300.77183396563055	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+38.0	297.85000076293943	300.7500003814697	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+39.0	297.85000076293943	300.7500003814697	-1.1147890405548093	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+40.0	297.85000076293943	300.7500003814697	-4.250421635238898	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+41.0	297.85000076293943	300.7500003814697	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+42.0	297.85000076293943	300.7500003814697	-5.440000057220459	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+43.0	297.85000076293943	300.7500003814697	-1.0939529665828687	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+44.0	297.85000076293943	300.7500003814697	-4.271256825956794	294.04999961853025	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+45.0	297.85000076293943	300.7500003814697	-5.440000057220459	283.4829682548144	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+46.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+47.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+48.0	297.85000076293943	300.7500003814697	-8.15999984741211	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+49.0	297.85000076293943	300.7500003814697	-2.720000028610229	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+50.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+51.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+52.0	297.85000076293943	300.7500003814697	2.879999876022339	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+53.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+54.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+55.0	297.85000076293943	300.7500003814697	0.0799999982118606	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+56.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+57.0	297.85000076293943	300.7500003814697	-4.800000190734863	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+58.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+59.0	297.85000076293943	300.7500003814697	0.0799999982118606	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+60.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+61.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+62.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+63.0	297.85000076293943	300.7500003814697	0.0799999237060546	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+64.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+65.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.7500003814697
+66.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.8499998092651
+67.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	0.0	0.0	0.0	288.55000057220457	288.8499998092651
+68.0	297.85000076293943	300.7500003814697	0.0799999237060546	272.15	0.0	0.0	0.0	288.55000057220457	288.8499998092651
+69.0	297.85000076293943	300.7500003814697	0.0799999982118606	272.15	0.0	0.0	0.0	288.55000057220457	288.8499998092651
+70.0	297.85000076293943	300.7500003814697	-5.440000057220459	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+71.0	297.85000076293943	300.7500003814697	0.0799999237060546	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+72.0	297.85000076293943	300.7500003814697	5.599999904632568	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+73.0	297.85000076293943	300.7500003814697	5.679999828338623	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+74.0	297.85000076293943	300.7500003814697	16.15999984741211	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+75.0	297.85000076293943	300.7500003814697	16.8799991607666	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+76.0	297.85000076293943	300.7500003814697	44.880001068115234	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+77.0	297.85000076293943	300.7500003814697	72.87999725341797	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+78.0	297.85000076293943	300.7500003814697	100.87999725341795	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+79.0	297.85000076293943	300.7500003814697	128.8000030517578	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+80.0	297.85000076293943	300.7500003814697	128.95999145507812	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+81.0	297.85000076293943	300.7500003814697	123.36000061035156	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+82.0	297.95000114440916	300.65	117.84000396728516	272.15	1.0	0.0	1.0	288.55000057220457	288.8499998092651
+83.0	298.18909919850273	300.65	122.23941667543787	272.15	1.0	0.0	1.0	288.55000057220457	288.77030071125864
+84.0	298.4156439595996	300.5947851229113	123.35999639780682	272.15	1.0	0.0	1.0	288.55000057220457	288.7500003814697
+85.0	298.54999961853025	300.54999961853025	123.35999298095705	272.15	1.0	0.0	1.0	288.55000057220457	288.7500003814697
+86.0	298.95000114440916	300.45000114440916	123.27999877929688	272.15	1.0	0.0	1.0	288.55000057220457	288.65
+87.0	299.35000076293943	300.45000114440916	123.43999481201172	272.15	1.0	0.0	1.0	288.45000019073484	288.65
+88.0	299.7500003814697	300.35000076293943	123.36000061035156	272.15	1.0	0.0	1.0	288.45000019073484	288.65
+89.0	300.15	300.2500003814697	123.35999298095705	272.15	1.0	0.0	1.0	288.45000019073484	288.55000057220457
+90.0	300.54999961853025	300.15	132.47999572753906	272.15	1.0	0.0	1.0	288.3499998092651	288.55000057220457
+91.0	300.85000076293943	300.15	123.36000061035156	272.15	1.0	0.0	1.0	288.3499998092651	288.55000057220457
+92.0	301.2500003814697	300.15	129.0399932861328	272.15	1.0	0.0	1.0	288.3499998092651	288.45000019073484
+93.0	301.54999961853025	300.15	128.8000030517578	272.15	1.0	0.0	1.0	288.2500003814697	288.45000019073484
+94.0	301.95000114440916	300.2500003814697	126.07999420166016	272.15	1.0	0.0	1.0	288.2500003814697	288.45000019073484
+95.0	302.2500003814697	300.2500003814697	128.8000030517578	272.15	1.0	0.0	1.0	288.2500003814697	288.45000019073484
+96.0	302.65	300.45000114440916	120.55999755859376	272.15	1.0	0.0	1.0	288.2500003814697	288.3499998092651
+97.0	302.95000114440916	300.54999961853025	128.87998962402344	272.15	1.0	0.0	1.0	288.2500003814697	288.3499998092651
+98.0	303.35000076293943	300.85000076293943	123.27999877929688	272.15	1.0	0.0	1.0	288.2500003814697	288.3499998092651
+99.0	303.65	301.04999961853025	120.55999755859376	272.15	1.0	0.0	1.0	288.15	288.3499998092651
+100.0	303.85000076293943	301.2500003814697	128.87998962402344	272.15	1.0	0.0	1.0	288.15	288.3499998092651
+101.0	304.04999961853025	301.45000114440916	126.15999603271484	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+102.0	304.2500003814697	301.7500003814697	128.95999145507812	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+103.0	304.2500003814697	302.04999961853025	126.15999603271484	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+104.0	304.35000076293943	302.35000076293943	123.44000244140624	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+105.0	304.35000076293943	302.54999961853025	123.36000061035156	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+106.0	304.2500003814697	302.85000076293943	126.15999603271484	272.15	1.0	0.0	1.0	288.05000057220457	288.2500003814697
+107.0	304.15	303.15	126.15999603271484	272.15	1.0	0.0	1.0	288.05000057220457	288.15
+108.0	304.04999961853025	303.45000114440916	123.36000061035156	272.15	1.0	0.0	1.0	288.05000057220457	288.15
+109.0	303.95000114440916	303.65	128.239990234375	272.15	1.0	0.0	1.0	288.05000057220457	288.15
+110.0	303.7500003814697	303.95000114440916	120.55999755859376	272.15	1.0	0.0	1.0	288.05000057220457	288.15
+111.0	303.65	304.15	123.36000061035156	272.15	1.0	0.0	1.0	288.05000057220457	288.15
+112.0	303.54999961853025	304.35000076293943	126.15999603271484	272.15	1.0	0.0	1.0	288.05000057220457	288.15
+113.0	303.35000076293943	304.45000114440916	117.84000396728516	272.15	1.0	0.0	1.0	288.05000057220457	288.15
+114.0	303.2500003814697	304.54999961853025	126.16000366210938	272.15	1.0	0.0	1.0	288.05000057220457	288.2500003814697
+115.0	303.15	304.65	123.36000061035156	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+116.0	303.15	304.65	117.84000396728516	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+117.0	303.04999961853025	304.65	126.15999603271484	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+118.0	303.04999961853025	304.65	128.3876525157989	272.15	1.0	0.0	1.0	288.15	288.2500003814697
+119.0	303.04999961853025	304.5773857566444	122.85279140959358	272.15	1.0	0.0	1.0	288.22261424335557	288.32261393232454
+120.0	303.11958308395003	304.4804174803047	120.58433155555726	272.15	1.0	0.0	1.0	288.2500003814697	288.3499998092651
+121.0	303.21967785741424	304.3803232869949	122.51097225021526	272.15	1.0	0.0	1.0	288.2500003814697	288.3499998092651
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+905.0	317.25000228881834	321.65	2178.18122678433	272.15	1.0	1.0	1.0	280.8500002861023	283.45000019073484
+906.0	317.25000228881834	321.65	2177.2039078644475	272.15	1.0	1.0	1.0	280.8500002861023	283.4032353195729
+907.0	317.25000228881834	321.65	2176.1050849468193	272.15	1.0	1.0	1.0	280.8500002861023	283.3499998092651
+908.0	317.25000228881834	321.65	2174.703377497882	272.15	1.0	1.0	1.0	280.8500002861023	283.3499998092651
+909.0	317.25000228881834	321.65	2175.5948071818866	272.15	1.0	1.0	1.0	280.8029522532545	283.3499998092651
+910.0	317.25000228881834	321.65	2175.8411325035536	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+911.0	317.25000228881834	321.65	2176.925456737721	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+912.0	317.25000228881834	321.65	2176.6641412285417	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+913.0	317.25000228881834	321.65	2175.5787505415756	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+914.0	317.25000228881834	321.65	2177.9494545876714	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+915.0	317.25000228881834	321.65	2174.8039554604857	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
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+917.0	317.25000228881834	321.65	2173.202525031696	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+918.0	317.25000228881834	321.65	2167.43994140625	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
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+926.0	317.25000228881834	321.65	2170.0822551870083	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+927.0	317.25000228881834	321.65	2168.127278289706	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+928.0	317.25000228881834	321.65	2167.9984799952276	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+929.0	317.25000228881834	321.65	2169.8775640771914	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
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+931.0	317.25000228881834	321.65	2167.68553850373	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+932.0	317.25000228881834	321.65	2170.0767313959705	272.15	1.0	1.0	1.0	280.74999990463255	283.30078163977686
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+934.0	317.25000228881834	321.65	2167.4408908366618	272.15	1.0	1.0	1.0	280.65	283.2500003814697
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+947.0	316.2571258960293	321.55712513308987	2056.146324300447	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+948.0	316.1570295084953	321.5500015258789	2044.9473090985514	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+949.0	316.056936370039	321.5500015258789	2039.0228252417642	272.15	1.0	1.0	1.0	280.65	283.2500003814697
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+954.0	315.55646452721703	321.25000228881834	2022.196608129962	272.15	1.0	1.0	1.0	280.5564631891609	283.15646312461195
+955.0	315.4563680899819	321.15636885292133	2011.353184669562	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+956.0	315.35627499894184	321.0562757618813	2020.9872429654931	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+957.0	315.2561821284404	320.9561793124284	2013.9491673577818	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+958.0	315.15608569784405	320.8560862286379	2015.9943866995109	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+959.0	315.0559925951486	320.75599335808806	2021.2739378846647	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+960.0	314.9558961332858	320.6558968962253	2008.5761123101993	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+961.0	314.9499992370605	320.55580391985734	2005.1978648870243	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+962.0	314.8557087663639	320.45570745823136	2005.0400390625	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+963.0	314.75561591844007	320.35561439256117	1999.7543149440864	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+964.0	314.6556139150466	320.25561598971603	2004.6500788230953	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+965.0	314.55552647163717	320.15552515652143	2004.8843071529807	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+966.0	314.5500015258789	320.0554320750648	1999.659635231125	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+967.0	314.4553355918195	319.9553355918195	1999.2841738676364	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+968.0	314.3921727792385	319.8921727792385	1996.0878267532723	272.15	1.0	1.0	1.0	280.5500000953674	283.15
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+970.0	314.25000228881834	319.65	1993.7598876953125	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+971.0	314.15	319.65	1988.159912109375	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+972.0	314.0500015258789	319.5500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+973.0	313.9499992370605	319.4499992370605	1982.39990234375	272.15	1.0	1.0	1.0	280.5500000953674	283.15
+974.0	313.85000076293943	319.35000076293943	1979.760009765625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+975.0	313.85000076293943	319.25000228881834	1974.239990234375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+976.0	313.75000228881834	319.15	1968.639892578125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
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+979.0	313.4499992370605	318.9499992370605	1960.159912109375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
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+981.0	313.35000076293943	318.75000228881834	1960.0799560546875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+982.0	313.25000228881834	318.65	1957.3599853515625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+983.0	313.15	318.65	1954.6400146484373	272.15	1.0	1.0	1.0	280.65	283.2500003814697
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+985.0	313.0500015258789	318.4499992370605	1954.4000244140625	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+986.0	312.9499992370605	318.35000076293943	1949.1199951171875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
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+1026.0	311.4499992370605	316.15	1959.3359182938916	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1027.0	311.51959627605174	316.15	1968.0378330260496	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1028.0	311.5500015258789	316.0803112490395	1977.1654401134829	272.15	1.0	1.0	1.0	280.65	283.3499998092651
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+1030.0	311.65	316.0500015258789	1979.2220855741452	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1031.0	311.65	316.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
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+1033.0	311.75000228881834	316.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
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+1036.0	311.85000076293943	316.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
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+1039.0	311.9499992370605	316.15	1988.080078125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1040.0	311.9499992370605	316.25000228881834	1982.56005859375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1041.0	311.9499992370605	316.25000228881834	1988.080078125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1042.0	312.0359626780505	316.33596245063836	1988.080078125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1043.0	312.0500015258789	316.35000076293943	1983.863382720765	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1044.0	312.0500015258789	316.35000076293943	1986.8617503938058	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1045.0	312.0500015258789	316.4277002292258	1983.790959743093	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1046.0	312.12779530470334	316.4499992370605	1986.7920591547136	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1047.0	312.15	316.4499992370605	1988.0	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1048.0	312.15	316.51126769767563	1984.5689849027776	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1049.0	312.15	316.5500015258789	1982.4490393902788	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1050.0	312.15	316.5500015258789	1985.8723495825056	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1051.0	312.2115515371861	316.61155071511394	1988.0	272.15	1.0	1.0	1.0	280.65	283.4115501724757
+1052.0	312.25000228881834	316.65	1988.09865229869	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1053.0	312.25000228881834	316.65	1991.089911778574	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1054.0	312.25000228881834	316.65	1993.679931640625	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1055.0	312.35000076293943	316.75000228881834	1993.7598876953125	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1056.0	312.35000076293943	316.75000228881834	2004.7999267578125	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1057.0	312.35000076293943	316.75000228881834	2004.719970703125	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1058.0	312.4499992370605	316.75000228881834	1999.52001953125	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1059.0	312.4499992370605	316.85000076293943	2004.8798828125	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1060.0	312.4499992370605	316.85000076293943	2010.1394325738202	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1061.0	312.5422250027903	316.85000076293943	2005.3892167059573	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1062.0	312.5500015258789	316.85000076293943	2007.5449115358115	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1063.0	312.6424124511339	316.94241168819445	2015.4487792396837	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1064.0	312.65	316.9499992370605	2010.9736888338339	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1065.0	312.7426032202336	316.9499992370605	2015.6714313650948	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1066.0	312.75000228881834	316.9499992370605	2016.0800602917438	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1067.0	312.75000228881834	317.0427912585765	2021.3504808851121	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1068.0	312.84288514486815	317.0500015258789	2029.488044803567	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1069.0	312.85000076293943	317.0500015258789	2025.550235683712	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1070.0	312.85000076293943	317.0500015258789	2022.56005859375	272.15	1.0	1.0	1.0	280.65	283.45000019073484
+1071.0	312.9499992370605	317.15	2021.83984375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1072.0	312.9499992370605	317.15	2035.679931640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1073.0	312.9499992370605	317.15	2027.35986328125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1074.0	313.0500015258789	317.25000228881834	2021.83984375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1075.0	313.0500015258789	317.25000228881834	2021.679931640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1076.0	313.0500015258789	317.25000228881834	2027.280029296875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1077.0	313.0500015258789	317.35000076293943	2016.159912109375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1078.0	313.0500015258789	317.35000076293943	2016.159912109375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1079.0	313.0500015258789	317.4499992370605	2010.719970703125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1080.0	313.0500015258789	317.4499992370605	2015.9200439453125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1081.0	313.0500015258789	317.4499992370605	2011.199951171875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1082.0	313.0500015258789	317.5375515013559	2005.8069320779246	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1083.0	313.0500015258789	317.5500015258789	2005.0400390625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1084.0	313.0500015258789	317.5500015258789	2005.0400390625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1085.0	313.0500015258789	317.5500015258789	2004.9743941470176	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1086.0	313.0500015258789	317.6320707625891	2009.2932066174276	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1087.0	313.0500015258789	317.65	2005.835943607227	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1088.0	313.0500015258789	317.65	2000.3392775409434	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1089.0	313.0500015258789	317.65	1997.0540432039954	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1090.0	313.0500015258789	317.65	2003.353639631449	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1091.0	313.0500015258789	317.65	2000.243473127887	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1092.0	313.0500015258789	317.65	1999.345959084706	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1093.0	313.0500015258789	317.65	2002.3217359308542	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1094.0	313.0500015258789	317.65	2004.7999267578125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1095.0	312.9499992370605	317.65	2002.159912109375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1096.0	312.9499992370605	317.65	2004.239990234375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1097.0	312.9499992370605	317.65	2003.5198974609373	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1098.0	312.9499992370605	317.65	1995.199951171875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1099.0	312.9499992370605	317.65	2001.43994140625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1100.0	312.9499992370605	317.65	1999.2799072265625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1101.0	312.9499992370605	317.65	1994.39990234375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1102.0	312.9499992370605	317.65	1994.39990234375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1103.0	312.9499992370605	317.65	1990.239990234375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1104.0	312.9499992370605	317.65	1995.840087890625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1105.0	312.9499992370605	317.65	1997.919921875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1106.0	312.9499992370605	317.65	1993.919921875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1107.0	312.9499992370605	317.65	1994.079833984375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1108.0	312.85000076293943	317.5500015258789	1990.9598388671875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1109.0	312.85000076293943	317.5500015258789	1988.2398681640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1110.0	312.85000076293943	317.5500015258789	1990.9598388671875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1111.0	312.85000076293943	317.5500015258789	1988.1600341796875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1112.0	312.85000076293943	317.5500015258789	1988.1600341796875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1113.0	312.85000076293943	317.5500015258789	1990.8800048828125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1114.0	312.85000076293943	317.5500015258789	1990.8800048828125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1115.0	312.75000228881834	317.5500015258789	1985.3599853515625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1116.0	312.75000228881834	317.5500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1117.0	312.75000228881834	317.5500015258789	1988.080078125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1118.0	312.75000228881834	317.4499992370605	1988.080078125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1119.0	312.75000228881834	317.4499992370605	1977.679931640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1120.0	312.75000228881834	317.4499992370605	1982.56005859375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1121.0	312.65	317.4499992370605	1979.7598876953125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1122.0	312.65	317.4499992370605	1982.64013671875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1123.0	312.65	317.4499992370605	1982.64013671875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1124.0	312.65	317.4499992370605	1982.31982421875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1125.0	312.65	317.35000076293943	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1126.0	312.65	317.35000076293943	1986.639892578125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1127.0	312.65	317.35000076293943	1992.239990234375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1128.0	312.65	317.35000076293943	1983.8399658203125	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1129.0	312.5500015258789	317.35000076293943	1985.27978515625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1130.0	312.5500015258789	317.35000076293943	1977.1850582881486	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1131.0	312.5500015258789	317.2885023031888	1980.2562445975034	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1132.0	312.5500015258789	317.25000228881834	1982.31982421875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1133.0	312.5500015258789	317.25000228881834	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1134.0	312.5500015258789	317.25000228881834	1988.0	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1135.0	312.5500015258789	317.25000228881834	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1136.0	312.5500015258789	317.25000228881834	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1137.0	312.5500015258789	317.25000228881834	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1138.0	312.5500015258789	317.25000228881834	1971.43994140625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1139.0	312.5500015258789	317.15	1981.83984375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1140.0	312.5500015258789	317.15	1977.599853515625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1141.0	312.4499992370605	317.15	1979.679931640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1142.0	312.4499992370605	317.15	1979.760009765625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1143.0	312.4499992370605	317.15	1987.83984375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1144.0	312.4499992370605	317.15	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1145.0	312.4499992370605	317.15	1977.1201171875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1146.0	312.4499992370605	317.15	1971.52001953125	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1147.0	312.4499992370605	317.15	1976.8798828125	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1148.0	312.4499992370605	317.15	1977.0400390625	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1149.0	312.4499992370605	317.15	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1150.0	312.4499992370605	317.15	1971.43994140625	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1151.0	312.4499992370605	317.15	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1152.0	312.4499992370605	317.0500015258789	1971.43994140625	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1153.0	312.4499992370605	317.0500015258789	1987.679931640625	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1154.0	312.4499992370605	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1155.0	312.4499992370605	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1156.0	312.4499992370605	317.0500015258789	1977.280029296875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1157.0	312.35000076293943	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1158.0	312.35000076293943	317.0500015258789	1971.760009765625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1159.0	312.35000076293943	317.0500015258789	1981.8399658203125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1160.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1161.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1162.0	312.35000076293943	317.0500015258789	1971.43994140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1163.0	312.35000076293943	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1164.0	312.35000076293943	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1165.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1166.0	312.35000076293943	317.0500015258789	1971.43994140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1167.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1168.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1169.0	312.35000076293943	316.98830549416823	1979.9134632049943	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1170.0	312.35000076293943	316.9499992370605	1978.3199462890625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1171.0	312.35000076293943	316.9499992370605	1977.597270150183	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1172.0	312.35000076293943	316.9499992370605	1977.280029296875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1173.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1174.0	312.35000076293943	316.9499992370605	1971.43994140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1175.0	312.35000076293943	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1176.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1177.0	312.35000076293943	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1178.0	312.35000076293943	316.9499992370605	1982.1600341796875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1179.0	312.35000076293943	316.9499992370605	1977.2799072265625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1180.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1181.0	312.35000076293943	316.9499992370605	1971.760009765625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1182.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1183.0	312.35000076293943	316.9499992370605	1977.9200439453125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1184.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1185.0	312.35000076293943	316.9499992370605	1981.8399658203125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1186.0	312.35000076293943	316.9499992370605	1982.159912109375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1187.0	312.35000076293943	316.9499992370605	1981.8399658203125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1188.0	312.35000076293943	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1189.0	312.35000076293943	316.9499992370605	1981.8399658203125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1190.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1191.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1192.0	312.35000076293943	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1193.0	312.35000076293943	316.9499992370605	1971.43994140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1194.0	312.35000076293943	316.9499992370605	1971.43994140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1195.0	312.35000076293943	316.9499992370605	1977.1062664056471	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1196.0	312.35000076293943	316.9499992370605	1979.3687119436936	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1197.0	312.35000076293943	316.9499992370605	1981.9868193117059	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1198.0	312.35000076293943	316.9499992370605	1979.6210473477379	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1199.0	312.35000076293943	316.9499992370605	1979.3314811458354	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1200.0	312.35000076293943	316.9499992370605	1982.0365897752133	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1201.0	312.35000076293943	316.9499992370605	1981.8161330495695	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1202.0	312.35000076293943	316.9499992370605	1982.1600341796875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1203.0	312.35000076293943	316.9499992370605	1982.1600341796875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1204.0	312.35000076293943	316.9499992370605	1981.119873046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1205.0	312.35000076293943	316.9499992370605	1977.9200439453125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1206.0	312.35000076293943	316.9499992370605	1981.5198974609373	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1207.0	312.35000076293943	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1208.0	312.35000076293943	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1209.0	312.42895590240585	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1210.0	312.4499992370605	316.9499992370605	1981.3092401744098	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1211.0	312.4499992370605	316.9499992370605	1979.679931640625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1212.0	312.4499992370605	316.9499992370605	1978.320068359375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1213.0	312.4499992370605	316.9499992370605	1988.0	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1214.0	312.4499992370605	316.9499992370605	1971.43994140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1215.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1216.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1217.0	312.4499992370605	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1218.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1219.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1220.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1221.0	312.4499992370605	316.9499992370605	1988.0	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1222.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1223.0	312.4499992370605	316.9499992370605	1988.0	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1224.0	312.4499992370605	316.9499992370605	1985.199951171875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1225.0	312.4499992370605	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1226.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1227.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1228.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1229.0	312.4499992370605	316.9499992370605	1988.0	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1230.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1231.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1232.0	312.4499992370605	316.9499992370605	1971.760009765625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1233.0	312.4499992370605	316.9499992370605	1982.4798583984373	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1234.0	312.4499992370605	316.9499992370605	1982.4798583984373	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1235.0	312.4499992370605	316.9499992370605	1987.679931640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1236.0	312.4499992370605	316.9499992370605	1987.679931640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1237.0	312.4499992370605	316.9499992370605	1987.679931640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1238.0	312.4499992370605	316.9499992370605	1982.4798583984373	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1239.0	312.4499992370605	316.9499992370605	1987.679931640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1240.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1241.0	312.4499992370605	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1242.0	312.4499992370605	316.9499992370605	1978.6562944764041	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1243.0	312.4499992370605	316.9499992370605	1979.4740751325944	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1244.0	312.4499992370605	316.9499992370605	1982.2466458828549	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1245.0	312.4499992370605	317.0416719693766	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1246.0	312.4499992370605	317.0500015258789	1985.0494462158615	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1247.0	312.4499992370605	317.0500015258789	1985.280029296875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1248.0	312.4499992370605	317.0500015258789	1987.781145902325	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1249.0	312.4499992370605	317.0500015258789	1977.8378446796805	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1250.0	312.4499992370605	317.0500015258789	1982.0462441388033	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1251.0	312.4499992370605	317.0500015258789	1977.3884868451225	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1252.0	312.4499992370605	317.0500015258789	1982.0566641220291	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1253.0	312.4499992370605	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1254.0	312.4499992370605	317.0500015258789	1977.3728569675711	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1255.0	312.4499992370605	317.0500015258789	1987.184629462034	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1256.0	312.4499992370605	317.0500015258789	1982.8824548708435	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1257.0	312.4499992370605	317.0500015258789	1985.0785126776866	272.15	1.0	1.0	1.0	280.7428030148861	283.3499998092651
+1258.0	312.4499992370605	317.0500015258789	1987.8068139066727	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1259.0	312.4499992370605	317.0500015258789	1985.5450010313198	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1260.0	312.4499992370605	317.0500015258789	1985.3600989822594	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1261.0	312.4499992370605	317.0500015258789	1987.8945942450985	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1262.0	312.4499992370605	317.0500015258789	1985.4683314105212	272.15	1.0	1.0	1.0	280.74999990463255	283.4432752068678
+1263.0	312.4499992370605	317.0500015258789	1982.6656394005563	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1264.0	312.4499992370605	317.0500015258789	1987.7140413568313	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1265.0	312.4499992370605	317.0500015258789	1982.9156520762288	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1266.0	312.4499992370605	317.0500015258789	1987.7296954182927	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1267.0	312.4499992370605	317.0500015258789	1987.7799095708979	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1268.0	312.4499992370605	317.0500015258789	1982.8803013583572	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1269.0	312.4499992370605	317.0500015258789	1987.7453252758207	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1270.0	312.4499992370605	317.0500015258789	1988.080078125	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1271.0	312.4499992370605	317.0500015258789	1983.1854276163988	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1272.0	312.4499992370605	317.0500015258789	1982.729215656586	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1273.0	312.4499992370605	317.0500015258789	1982.8707888127874	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1274.0	312.4499992370605	317.0500015258789	1987.7892585393856	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1275.0	312.4499992370605	317.0500015258789	1988.080078125	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1276.0	312.4499992370605	317.0500015258789	1977.63660976947	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1277.0	312.4499992370605	317.0500015258789	1982.2669827677937	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1278.0	312.4499992370605	317.0500015258789	1987.7922077280564	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1279.0	312.4499992370605	317.0500015258789	1982.8427184188618	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1280.0	312.4499992370605	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1281.0	312.4499992370605	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1282.0	312.4499992370605	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1283.0	312.4499992370605	317.0500015258789	1985.1549437529075	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1284.0	312.4499992370605	317.0500015258789	1985.4825832945348	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1285.0	312.4499992370605	317.0500015258789	1985.1598384459028	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1286.0	312.4499992370605	317.0500015258789	1988.080078125	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1287.0	312.4499992370605	317.0500015258789	1988.080078125	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1288.0	312.4499992370605	317.0500015258789	1985.4646697673445	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1289.0	312.4499992370605	317.0500015258789	1985.1806168885726	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1290.0	312.4499992370605	317.0500015258789	1986.7480546595584	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1291.0	312.4499992370605	317.0500015258789	1983.9835368639567	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1292.0	312.4499992370605	317.0500015258789	1982.5599365234373	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1293.0	312.4499992370605	317.0500015258789	1982.5599365234373	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1294.0	312.4499992370605	317.0500015258789	1984.89979623849	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1295.0	312.4499992370605	317.0500015258789	1989.630645511023	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1296.0	312.4499992370605	317.0500015258789	1985.41499075907	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1297.0	312.4499992370605	317.0500015258789	1982.5641893998786	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1298.0	312.4499992370605	317.0500015258789	1987.2746654437663	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1299.0	312.4499992370605	317.0500015258789	1985.5420349082901	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1300.0	312.4499992370605	317.0500015258789	1983.0543142544611	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1301.0	312.4499992370605	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1302.0	312.4499992370605	317.0500015258789	1985.2483999362717	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1303.0	312.4499992370605	317.0500015258789	1985.3865295435587	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1304.0	312.4499992370605	317.0500015258789	1985.2588180420807	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1305.0	312.4499992370605	317.0500015258789	1985.3761085026495	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1306.0	312.4499992370605	317.0500015258789	1985.2692383614005	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1307.0	312.4499992370605	317.0500015258789	1988.080078125	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1308.0	312.4499992370605	317.0500015258789	1983.2714619163817	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1309.0	312.4499992370605	317.0500015258789	1980.5314275875517	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1310.0	312.4499992370605	317.0500015258789	1985.0552396205658	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1311.0	312.4499992370605	317.0500015258789	1984.941893480165	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1312.0	312.4499992370605	317.0500015258789	1982.5197355742716	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1313.0	312.4499992370605	317.0500015258789	1982.5997678472058	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1314.0	312.4499992370605	317.0500015258789	1982.5602016800703	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1315.0	312.4499992370605	317.0500015258789	1982.200691975263	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1316.0	312.4499992370605	317.0500015258789	1982.2395569783007	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1317.0	312.4499992370605	317.0500015258789	1985.3210153394207	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1318.0	312.4499992370605	317.0500015258789	1988.0541250732363	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1319.0	312.4499992370605	317.0500015258789	1988.0022856161738	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1320.0	312.4499992370605	317.0500015258789	1984.1116721463482	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1321.0	312.4499992370605	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1322.0	312.4499992370605	317.0500015258789	1982.5103295545944	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1323.0	312.4499992370605	317.0500015258789	1980.7882936763035	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1324.0	312.4499992370605	317.0500015258789	1978.0158753946482	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1325.0	312.4499992370605	317.0500015258789	1977.0597202047006	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1326.0	312.4499992370605	317.0500015258789	1980.3188301158325	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1327.0	312.4499992370605	317.0500015258789	1982.3400512958374	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1328.0	312.4499992370605	317.0500015258789	1979.0409667263648	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1329.0	312.4499992370605	317.0500015258789	1983.6675439211547	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1330.0	312.4499992370605	317.0500015258789	1984.3816916314668	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1331.0	312.4499992370605	317.0500015258789	1982.479935241764	272.15	1.0	1.0	1.0	280.74999990463255	283.38704989746776
+1332.0	312.4499992370605	317.0500015258789	1975.9737508475068	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1333.0	312.4499992370605	317.0500015258789	1981.959070285438	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1334.0	312.4499992370605	317.0500015258789	1981.1036684481592	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1335.0	312.4499992370605	317.0500015258789	1980.674252659255	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1336.0	312.4499992370605	317.0500015258789	1982.5892603512561	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1337.0	312.4499992370605	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1338.0	312.4499992370605	317.0500015258789	1982.5091203622403	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1339.0	312.4499992370605	317.0500015258789	1982.5309942860852	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1340.0	312.4499992370605	317.0500015258789	1980.72255317554	272.15	1.0	1.0	1.0	280.6862005063513	283.3499998092651
+1341.0	312.4499992370605	317.0500015258789	1979.7310965789918	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1342.0	312.4499992370605	317.0500015258789	1978.172960421728	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1343.0	312.4499992370605	317.0500015258789	1980.5096470628075	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1344.0	312.4499992370605	317.0500015258789	1985.7598188939883	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1345.0	312.4499992370605	317.0500015258789	1984.2758897921249	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1346.0	312.4499992370605	317.0500015258789	1985.756132489568	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1347.0	312.4499992370605	317.0500015258789	1984.4199244561844	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1348.0	312.4499992370605	317.0500015258789	1985.8757039766806	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1349.0	312.4499992370605	317.0500015258789	1984.286837492649	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1350.0	312.4499992370605	317.0500015258789	1982.2398681640625	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1351.0	312.4499992370605	317.0500015258789	1979.5518019764838	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1352.0	312.4499992370605	317.0500015258789	1978.398513147989	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1353.0	312.4499992370605	317.0500015258789	1980.8158325236104	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1354.0	312.4499992370605	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1355.0	312.4499992370605	317.0500015258789	1988.0	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1356.0	312.4499992370605	317.0500015258789	1988.0	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1357.0	312.4499992370605	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1358.0	312.4499992370605	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1359.0	312.4499992370605	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1360.0	312.4499992370605	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1361.0	312.4499992370605	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1362.0	312.4499992370605	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1363.0	312.4499992370605	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1364.0	312.4499992370605	317.0500015258789	1988.0	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1365.0	312.4499992370605	317.0500015258789	1977.0399169921875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1366.0	312.4499992370605	317.0500015258789	1986.719970703125	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1367.0	312.4499992370605	317.0500015258789	1973.0399169921875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1368.0	312.4499992370605	317.0500015258789	1982.1600341796875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1369.0	312.4499992370605	317.0500015258789	1973.0399169921875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1370.0	312.4499992370605	317.0500015258789	1976.9599609375	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1371.0	312.4499992370605	317.0500015258789	1974.159912109375	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1372.0	312.4499992370605	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1373.0	312.4499992370605	317.0500015258789	1979.760009765625	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1374.0	312.4499992370605	317.0500015258789	1984.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1375.0	312.4499992370605	317.0500015258789	1976.8798828125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1376.0	312.4499992370605	317.0500015258789	1971.599853515625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1377.0	312.4499992370605	317.0500015258789	1977.119873046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1378.0	312.4499992370605	317.0500015258789	1978.12080016549	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1379.0	312.4499992370605	317.0500015258789	1980.3388012782157	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1380.0	312.4499992370605	317.0500015258789	1982.0906932153541	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1381.0	312.4499992370605	317.0500015258789	1981.5078764663895	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1382.0	312.4499992370605	317.0500015258789	1979.1160502711723	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1383.0	312.4499992370605	317.0500015258789	1980.3264119756273	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1384.0	312.4499992370605	317.0500015258789	1981.119960639269	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1385.0	312.4499992370605	317.0500015258789	1974.1648725311425	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1386.0	312.4499992370605	317.0500015258789	1976.389721942792	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1387.0	312.4499992370605	317.0500015258789	1977.3402289650742	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1388.0	312.4499992370605	317.0500015258789	1980.9417280367284	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1389.0	312.4499992370605	317.0500015258789	1978.4930025026322	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1390.0	312.4499992370605	317.0500015258789	1972.9099473199483	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1391.0	312.4499992370605	317.0500015258789	1975.3573795398045	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1392.0	312.4499992370605	317.0500015258789	1972.8774013883215	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1393.0	312.4499992370605	317.0500015258789	1974.3222397760658	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1394.0	312.4065368507796	317.0500015258789	1976.1700909263516	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1395.0	312.35000076293943	317.0500015258789	1977.119873046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1396.0	312.35000076293943	317.0500015258789	1981.8399658203125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1397.0	312.35000076293943	317.0500015258789	1977.5198974609373	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1398.0	312.35000076293943	317.0500015258789	1977.5198974609373	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1399.0	312.35000076293943	317.0500015258789	1981.8399658203125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1400.0	312.35000076293943	317.0500015258789	1972.4000244140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1401.0	312.35000076293943	317.0500015258789	1982.7999267578125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1402.0	312.35000076293943	317.0500015258789	1987.0399169921875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1403.0	312.35000076293943	317.0500015258789	1972.719970703125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1404.0	312.35000076293943	317.0500015258789	1972.4000244140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1405.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1406.0	312.35000076293943	317.0500015258789	1983.37693521578	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1407.0	312.35000076293943	317.0500015258789	1983.83984375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1408.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1409.0	312.35000076293943	317.0500015258789	1979.679931640625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1410.0	312.35000076293943	317.0500015258789	1987.8399658203125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1411.0	312.35000076293943	317.0500015258789	1987.919921875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1412.0	312.35000076293943	317.0500015258789	1972.4000244140625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1413.0	312.35000076293943	317.0500015258789	1978.0	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1414.0	312.35000076293943	317.0500015258789	1975.3669762090033	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1415.0	312.35000076293943	317.0500015258789	1974.957576098505	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1416.0	312.35000076293943	317.0500015258789	1979.5481186427357	272.15	1.0	1.0	1.0	280.595946927582	283.2500003814697
+1417.0	312.35000076293943	317.0500015258789	1979.7036470126786	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1418.0	312.35000076293943	317.0500015258789	1979.709700445454	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1419.0	312.35000076293943	317.0500015258789	1982.3071066887399	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1420.0	312.35000076293943	317.00367609850235	1979.7705865262665	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1421.0	312.35000076293943	316.9499992370605	1979.5452107062729	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1422.0	312.35000076293943	316.98158843372573	1980.6184316123927	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1423.0	312.35000076293943	317.0495670716845	1977.3012296671948	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1424.0	312.35000076293943	316.9570572842854	1983.0796081538992	272.15	1.0	1.0	1.0	280.65	283.34294196396803
+1425.0	312.35000076293943	316.9499992370605	1982.5575470158208	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1426.0	312.35000076293943	317.0426376913202	1977.3664367398974	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1427.0	312.35000076293943	317.0500015258789	1978.2209721059269	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1428.0	312.35000076293943	317.0500015258789	1982.1814947056328	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1429.0	312.35000076293943	317.0500015258789	1985.0817720235889	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1430.0	312.35000076293943	316.9569854927745	1981.41050554855	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1431.0	312.35000076293943	316.9499992370605	1983.7269483389287	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1432.0	312.35000076293943	317.0432039469612	1987.7226598173636	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1433.0	312.35000076293943	317.0500015258789	1977.699977587663	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1434.0	312.35000076293943	317.0500015258789	1979.5001782926029	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1435.0	312.35000076293943	317.0500015258789	1983.643718208655	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1436.0	312.35000076293943	317.0500015258789	1982.5724225901595	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1437.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1438.0	312.35000076293943	317.0500015258789	1977.3788969146428	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1439.0	312.35000076293943	317.0500015258789	1987.3274008723515	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1440.0	312.35000076293943	317.0500015258789	1991.5328145963897	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1441.0	312.35000076293943	317.0500015258789	1979.0441622928852	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1442.0	312.35000076293943	317.0500015258789	1977.0348891713104	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1443.0	312.35000076293943	317.0500015258789	1974.3966397760594	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1444.0	312.35000076293943	317.0500015258789	1974.239990234375	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1445.0	312.35000076293943	316.9555699244736	1979.452513770423	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1446.0	312.35000076293943	317.04452523434514	1979.8355872938755	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1447.0	312.35000076293943	317.0500015258789	1979.6885443457218	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1448.0	312.35000076293943	316.9552867510408	1984.908086047709	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1449.0	312.35000076293943	316.9499992370605	1982.621229032238	272.15	1.0	1.0	1.0	280.7448068917585	283.3499998092651
+1450.0	312.35000076293943	316.9499992370605	1982.7077345136884	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1451.0	312.35000076293943	316.9499992370605	1988.7236529570296	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1452.0	312.35000076293943	316.9499992370605	1991.0178644730959	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1453.0	312.35000076293943	316.9499992370605	1991.8052952742569	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1454.0	312.35000076293943	316.9499992370605	1980.4063904591503	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1455.0	312.35000076293943	316.9499992370605	1982.3578272479338	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1456.0	312.35000076293943	316.9499992370605	1985.2294526754547	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1457.0	312.35000076293943	316.9499992370605	1987.9593603543665	272.15	1.0	1.0	1.0	280.74999990463255	283.44556217184396
+1458.0	312.35000076293943	316.9499992370605	1982.799826364694	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1459.0	312.35000076293943	316.9499992370605	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1460.0	312.35000076293943	317.03135135363533	1982.4949148351714	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1461.0	312.35000076293943	317.0500015258789	1980.1921977603158	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1462.0	312.35000076293943	317.0500015258789	1977.52001953125	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1463.0	312.35000076293943	317.0500015258789	1988.080078125	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1464.0	312.35000076293943	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1465.0	312.35000076293943	317.0500015258789	1988.0	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1466.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1467.0	312.35000076293943	317.0500015258789	1988.0	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1468.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1469.0	312.35000076293943	317.0500015258789	1982.47998046875	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1470.0	312.35000076293943	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1471.0	312.35000076293943	317.0500015258789	1988.0	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1472.0	312.35000076293943	317.0500015258789	1982.56005859375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1473.0	312.35000076293943	317.0500015258789	1988.0	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1474.0	312.35000076293943	317.0500015258789	1988.0	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1475.0	312.35000076293943	317.0500015258789	1983.1199951171875	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1476.0	312.35000076293943	317.0500015258789	1986.0	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1477.0	312.35000076293943	317.0500015258789	1977.0400390625	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1478.0	312.35000076293943	317.0500015258789	1984.8784472235009	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1479.0	312.35000076293943	317.0500015258789	1987.2441418601618	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1480.0	312.35000076293943	317.0500015258789	1988.0509284568313	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1481.0	312.41369263733645	317.0500015258789	1984.5132165336825	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1482.0	312.39169874465307	317.0500015258789	1984.1124476326688	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1483.0	312.4044720918723	317.0500015258789	1983.7984025004669	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1484.0	312.4499992370605	317.0500015258789	1984.0879485132048	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1485.0	312.4499992370605	317.0500015258789	1985.360040697103	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1486.0	312.4499992370605	317.0500015258789	1986.8493139797683	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1487.0	312.4499992370605	317.0500015258789	1988.0799560546875	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1488.0	312.4499992370605	317.0500015258789	1986.5415629055822	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1489.0	312.4499992370605	317.0500015258789	1986.8211310584636	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1490.0	312.4499992370605	317.0500015258789	1986.5363334559152	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1491.0	312.4499992370605	317.0500015258789	1985.280029296875	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1492.0	312.4499992370605	317.0500015258789	1983.7309985645345	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1493.0	312.4499992370605	317.0500015258789	1985.5389516992534	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1494.0	312.4499992370605	317.0500015258789	1986.534519034953	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1495.0	312.4499992370605	317.0500015258789	1986.4735981434317	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1496.0	312.4499992370605	317.0500015258789	1987.83984375	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1497.0	312.4499992370605	317.0500015258789	1988.0494849861914	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1498.0	312.4499992370605	317.0500015258789	1984.0018211032084	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1499.0	312.4499992370605	317.0500015258789	1987.122786642386	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1500.0	312.4499992370605	317.0500015258789	1983.6680023851504	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1501.0	312.4499992370605	317.0500015258789	1990.1749016244216	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1502.0	312.4499992370605	317.0500015258789	1988.8634963675106	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1503.0	312.4499992370605	317.0500015258789	1986.3369247152655	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1504.0	312.4499992370605	317.0500015258789	1984.7466712824569	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1505.0	312.4499992370605	317.0500015258789	1982.9138347158591	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1506.0	312.4499992370605	317.0500015258789	1985.6959747087817	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1507.0	312.4499992370605	317.0500015258789	1987.732253892288	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1508.0	312.4499992370605	317.0500015258789	1981.4007142117305	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1509.0	312.4499992370605	317.0500015258789	1985.9969670503942	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1510.0	312.4499992370605	317.0500015258789	1984.9601762809664	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1511.0	312.4499992370605	317.0500015258789	1986.1167421171967	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1512.0	312.4499992370605	317.0500015258789	1984.525382675503	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1513.0	312.4499992370605	317.0500015258789	1982.4788463605878	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1514.0	312.4499992370605	317.0500015258789	1982.4376057754446	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1515.0	312.4499992370605	317.0500015258789	1984.8952659528982	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1516.0	312.4499992370605	317.0500015258789	1985.9756550611908	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1517.0	312.4499992370605	317.0500015258789	1980.6475467055132	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1518.0	312.4499992370605	317.0500015258789	1978.3199462890625	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1519.0	312.4499992370605	317.0500015258789	1984.1900251503857	272.15	1.0	1.0	1.0	280.74999990463255	283.45000019073484
+1520.0	312.4499992370605	317.0500015258789	1985.9921922449112	272.15	1.0	1.0	1.0	280.74999990463255	283.38002385420003
+1521.0	312.4499992370605	317.0500015258789	1988.5387756703024	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1522.0	312.4499992370605	317.0500015258789	1981.0595223989242	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1523.0	312.4499992370605	317.0500015258789	1984.385813554945	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1524.0	312.4499992370605	317.0500015258789	1983.757851784612	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1525.0	312.4499992370605	317.0500015258789	1979.1965914606303	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1526.0	312.4499992370605	317.0500015258789	1980.9673979876954	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1527.0	312.4499992370605	317.0500015258789	1978.6270115142293	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1528.0	312.4499992370605	317.0500015258789	1977.2329425073524	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1529.0	312.4499992370605	317.0500015258789	1977.439275001948	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1530.0	312.4499992370605	317.0500015258789	1977.5999755859373	272.15	1.0	1.0	1.0	280.74999990463255	283.3499998092651
+1531.0	312.4499992370605	317.0500015258789	1977.1089298230484	272.15	1.0	1.0	1.0	280.6732758334273	283.3499998092651
+1532.0	312.4499992370605	317.0500015258789	1980.510165615077	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1533.0	312.4016198582006	317.0500015258789	1983.2490625278663	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1534.0	312.35000076293943	317.0500015258789	1980.1290072941442	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1535.0	312.35000076293943	317.0500015258789	1977.119873046875	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1536.0	312.35000076293943	317.0500015258789	1980.8961401618344	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1537.0	312.35000076293943	317.0500015258789	1981.1743795948435	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1538.0	312.35000076293943	317.0500015258789	1979.1558682480932	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1539.0	312.35000076293943	317.0500015258789	1981.6681294963719	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1540.0	312.35000076293943	317.0500015258789	1979.846859898833	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1541.0	312.35000076293943	317.00086528071506	1979.5612912464228	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1542.0	312.35000076293943	316.9499992370605	1984.0847977869241	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1543.0	312.35000076293943	316.9499992370605	1981.8226991033778	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1544.0	312.35000076293943	316.9499992370605	1978.8989775903794	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1545.0	312.35000076293943	316.9499992370605	1984.839328894813	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1546.0	312.35000076293943	316.9499992370605	1983.0871418883676	272.15	1.0	1.0	1.0	280.65	283.3499998092651
+1547.0	312.35000076293943	316.9499992370605	1979.624485012063	272.15	1.0	1.0	1.0	280.65	283.3002987433162
+1548.0	312.35000076293943	316.9499992370605	1979.6107600578787	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1549.0	312.35000076293943	316.9499992370605	1982.188432130653	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1550.0	312.35000076293943	316.9499992370605	1979.6024184398027	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1551.0	312.35000076293943	316.9499992370605	1974.5644725871048	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1552.0	312.35000076293943	316.9499992370605	1974.550358860188	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1553.0	312.35000076293943	316.9499992370605	1974.3739000656476	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1554.0	312.35000076293943	316.9499992370605	1979.5787592906647	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1555.0	312.35000076293943	316.9499992370605	1979.6170147177359	272.15	1.0	1.0	1.0	280.59954368171793	283.2500003814697
+1556.0	312.35000076293943	316.9499992370605	1977.2009539005883	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1557.0	312.35000076293943	316.9499992370605	1977.0773749106547	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1558.0	312.35000076293943	316.9499992370605	1976.9205140019374	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1559.0	312.35000076293943	316.9499992370605	1979.6847084552476	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1560.0	312.35000076293943	316.9499992370605	1982.4015087339305	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1561.0	312.35000076293943	316.9499992370605	1979.6635224740744	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1562.0	312.35000076293943	316.9499992370605	1976.8782186716555	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1563.0	312.35000076293943	316.9499992370605	1979.053223432294	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1564.0	312.35000076293943	316.9499992370605	1982.159912109375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1565.0	312.35000076293943	316.9499992370605	1986.1704774420843	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1566.0	312.35000076293943	316.9499992370605	1988.0	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1567.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1568.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1569.0	312.35000076293943	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1570.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1571.0	312.35000076293943	316.9499992370605	1982.47998046875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1572.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1573.0	312.35000076293943	316.9499992370605	1977.1201171875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1574.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1575.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1576.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1577.0	312.35000076293943	316.9499992370605	1976.9599609375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1578.0	312.35000076293943	316.9499992370605	1977.679931640625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1579.0	312.35000076293943	316.9499992370605	1974.1600341796875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1580.0	312.35000076293943	316.9499992370605	1981.760009765625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1581.0	312.35000076293943	316.9499992370605	1982.56005859375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
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+1583.0	312.35000076293943	316.9499992370605	1982.639892578125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
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+1585.0	312.35000076293943	316.9499992370605	1980.079833984375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
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+1590.0	312.35000076293943	316.9499992370605	1977.52001953125	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
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+1594.0	312.35000076293943	316.9499992370605	1988.0799560546875	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1595.0	312.35000076293943	316.9499992370605	1982.56005859375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
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+1597.0	312.35000076293943	316.9499992370605	1983.83984375	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1598.0	312.35000076293943	316.9499992370605	1977.0400390625	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
+1599.0	312.35000076293943	316.9499992370605	1990.0	272.15	1.0	1.0	1.0	280.5500000953674	283.2500003814697
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+1603.0	312.35000076293943	316.9499992370605	1979.840087890625	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1604.0	312.35000076293943	316.9499992370605	1984.1155081816037	272.15	1.0	1.0	1.0	280.65	283.2500003814697
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+1607.0	312.35000076293943	316.9499992370605	1986.1117057050544	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1608.0	312.35000076293943	316.9499992370605	1986.4017008501557	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1609.0	312.35000076293943	316.9499992370605	1983.691148040982	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1610.0	312.30086108801163	316.9008595621327	1978.0115354524282	272.15	1.0	1.0	1.0	280.65	283.2500003814697
+1611.0	312.25000228881834	316.85000076293943	1967.5156598960668	272.15	1.0	1.0	1.0	280.65	283.2500003814697
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+4603.0	313.0349187867798	316.5349187867798	1975.21479904656	272.15	1.0	1.0	1.0	275.8500000476837	278.45000019073484
+4604.0	313.0500015258789	316.6305188785318	1972.4352414001671	272.15	1.0	1.0	1.0	275.8500000476837	278.45000019073484
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+4620.0	313.25000228881834	317.25000228881834	1965.5999755859373	272.15	1.0	1.0	1.0	275.94999995231626	278.5500000953674
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+14325.0	300.65	302.65	-5.171908646366068	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14326.0	300.65	302.65	-8.149839481722694	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14327.0	300.65	302.65	-10.31999969482422	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14328.0	300.5632834265106	302.65	-10.87498394577697	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14329.0	300.54999961853025	302.65	-8.083157329156116	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
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+14331.0	300.54999961853025	302.65	-1.6902360179635716	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
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+14333.0	300.54999961853025	302.65	-4.079999923706055	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14334.0	300.54999961853025	302.65	-4.905478795745632	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14335.0	300.54999961853025	302.65	-5.440000057220459	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14336.0	300.54999961853025	302.65	-5.440000057220459	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
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+14339.0	300.54999961853025	302.65	-2.7233843087583787	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
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+14346.0	300.54999961853025	302.65	-0.35860701294120245	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14347.0	300.54999961853025	302.65	3.5999999046325684	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
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+14351.0	300.54999961853025	302.65	-5.440000057220459	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14352.0	300.54999961853025	302.65	-5.440000057220459	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14353.0	300.54999961853025	302.65	-1.6709130484564878	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14354.0	300.54999961853025	302.65	-2.060624829082768	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
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+14356.0	300.54999961853025	302.65	-2.4361473334938935	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14357.0	300.54999961853025	302.65	-0.2400002479553222	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14358.0	300.54999961853025	302.65	-7.467487212169159	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14359.0	300.54999961853025	302.65	-10.960000038146973	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14360.0	300.54999961853025	302.65	-5.952448423069965	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14361.0	300.54999961853025	302.65	-3.075346351139208	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14362.0	300.54999961853025	302.65	-1.2799999713897705	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14363.0	300.54999961853025	302.65	-1.28000018286967	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14364.0	300.54999961853025	302.65	-3.42719728468254	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
+14365.0	300.54999961853025	302.65	-5.440000057220459	272.15	0.0	0.0	0.0	294.2500003814697	294.45000114440916
diff --git a/AixLib/Resources/Data/Fluid/SolarCollectors/Validation/FlatPlate/TRNSYSAnnualData.txt b/AixLib/Resources/Data/Fluid/SolarCollectors/Validation/FlatPlate/TRNSYSAnnualData.txt
new file mode 100644
index 0000000000..46c282819a
--- /dev/null
+++ b/AixLib/Resources/Data/Fluid/SolarCollectors/Validation/FlatPlate/TRNSYSAnnualData.txt
@@ -0,0 +1,35043 @@
+#1
+double TRNSYS(35041,5)
+0	20	20	0	0.0277777778
+900	15.0005988236	10.6125	0	0
+1800	15.0004256659	9.6375	0	0
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+3600	15.0004480672	7.6875	0	0
+4500	15.0004480672	7.2	0	0
+5400	15.0004480672	7.2	0	0
+6300	15.0004480672	7.2	0	0
+7200	15.0004480672	7.2	0	0
+8100	15.0004480672	7.1375	0	0
+9000	15.0004480672	7.0125	0	0
+9900	15.0004480672	6.8875	0	0
+10800	15.0004480672	6.7625	0	0
+11700	15.0004480672	6.625	0	0
+12600	15.0004480672	6.475	0	0
+13500	15.0004480672	6.325	0	0
+14400	15.0004480672	6.175	0	0
+15300	15.0004480672	5.8875	0	0
+16200	15.0004480672	5.4625	0	0
+17100	15.0004480672	5.0375	0	0
+18000	15.0004480672	4.6125	0	0
+18900	15.0004480672	4.4	0	0
+19800	15.0004480672	4.4	0	0
+20700	15.0004480672	4.4	0	0
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+22500	15.0004480672	4.6125	0	0
+23400	15.0004480672	5.0375	0	0
+24300	15.0004480672	5.4625	0	0
+25200	15.0004480672	5.8875	0	0
+26100	15.0004480672	5.9625	0	0
+27000	15.0004480672	5.7049826667	0.1417052078	0
+27900	15.0004480672	9.6348665652	32.4339226689	0
+28800	15.0004480672	10.7005458155	37.2487345827	0
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+58500	15.001502075	13.55	0	0
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diff --git a/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat b/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat
deleted file mode 100644
index 69d94cfa2e..0000000000
Binary files a/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat and /dev/null differ
diff --git a/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt b/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt
new file mode 100644
index 0000000000..478bbaab53
--- /dev/null
+++ b/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt
@@ -0,0 +1,5908 @@
+#1
+double measurement(5905, 35)
+#time_in_s	N2_attic_east_AT N2_attic_west_AT N2_cellar_AT N2_living_AT_h67cm N2_living_AT_h125cm N2_living_AT_h187cm N2_corridor_AT N2_bath_AT N2_child_AT N2_kitchen_AT N2_doorway_AT N2_bedroom_AT N2_living_rH_h125cm N2_westfacade_S_IS_T N2_westfacade_S_IS_HF N2_westfacade_S_BL1_T N2_westfacade_S_BL1_HF N2_westfacade_S_ES_T N2_heat_elP_living_room N2_heat_elP_bath_room N2_heat_elP_children_room N2_heat_elP_kitchen N2-Heat-Input-Kitchen N2_heat_elP_doorway N2_heat_elP_bedroom N2_vent_ODA_AT N2_vent_SUA_AT N2_vent_SUA_corr_AT N2_vent_EHA_AT N2_vent_SUA_VFR N2_vent_EHA_VFR N2_vent_SUA_fan_elP  N2_vent_EHA_fan_elP N2_vent_thP
+0.0	24.135921	24.057659	20.144239	29.531048	29.986008	31.134912	30.049305	29.979389	29.99707	29.986731	30.012228	30.000942	32.82666	29.403091	-5.42798	23.11824	-8.122489	7.441233	1148.295898	195.525391	362.478455	316.952423	-147.4558946	181.835098	262.006775	12.0888	14.122999	17.60345897	30.50737	120.032494	120.069397	51.31963	62.448448	-661.163208
+600.0	24.12431	24.038069	20.13871	29.547962	30.000132	31.15799	30.057949	30.0056	30.006847	29.99439	29.999079	29.998449	32.73769	29.403967	-5.436573	23.088718	-8.203476	7.30115	1159.407959	197.555878	362.155701	323.893127	-148.8728733	181.458313	266.2659	11.94253	13.998851	17.50940971	30.539021	120.024002	119.975388	51.350929	62.469982	-667.194641
+1200.0	24.110592	24.020189	20.131298	29.54632	29.972891	31.184851	30.067911	30.00235	30.002213	30.00835	29.985352	30.000271	32.673229	29.420502	-5.588989	23.06073	-8.235997	7.364199	1174.606934	192.249298	356.349487	318.024597	-149.8112527	184.004181	261.460388	11.87324	13.926028	17.45614642	30.520077	120.045204	119.9879	51.047638	62.144032	-669.467102
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+3540600.0	15.017011	14.881419	15.85874	15.04997	15.061041	15.116321	15.69326	15.53668	15.573151	15.26026	15.601132	16.118481	59.219856	14.85663	0.240544	13.53981	-2.650355	8.666048	0.058167	0.0	0.042533	0.042867	-32.62650917	0.03005	0.061433	9.385233	11.135651	12.12354344	15.780539	120.003197	120.011093	50.561451	33.969521	-187.390594
+3541200.0	15.010271	14.877378	15.859459	15.03124	15.060422	15.117849	15.690831	15.532349	15.57149	15.25688	15.59886	16.11301	59.26828	14.85358	0.217709	13.533701	-2.644409	8.704334	0.044	0.0	0.042633	0.04335	-32.35891928	0.03055	0.070117	9.40355	11.164009	12.14467267	15.77657	120.025291	119.979813	50.609673	33.96273	-186.05899
+3541800.0	15.00654	14.874141	15.854889	15.033789	15.05421	15.108339	15.68703	15.531809	15.5603	15.253	15.593478	16.107492	59.333443	14.84716	0.234826	13.52841	-2.630306	8.702632	0.052	0.0	0.04205	0.04215	-32.6332428	0.029717	0.059283	9.36025	11.1275	12.11566692	15.76861	120.005104	120.009506	50.721916	34.032867	-187.228104
+3542400.0	15.00783	14.869951	15.85607	15.023169	15.050229	15.10068	15.676419	15.524359	15.56313	15.24169	15.591321	16.104549	59.355064	14.84269	0.23548	13.522591	-2.624223	8.721666	0.045167	0.0	0.043067	0.035367	-32.47012674	0.030033	0.0673	9.376049	11.13527	12.11929474	15.766521	119.995895	119.9944	50.662163	33.944786	-186.805817
diff --git a/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseO5.mat b/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseO5.mat
deleted file mode 100644
index 12a3c0b42e..0000000000
Binary files a/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseO5.mat and /dev/null differ
diff --git a/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mat b/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mat
deleted file mode 100644
index 8aaf86ed0e..0000000000
Binary files a/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mat and /dev/null differ
diff --git a/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.txt b/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.txt
new file mode 100644
index 0000000000..0a2d9a05a5
--- /dev/null
+++ b/AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.txt
@@ -0,0 +1,8763 @@
+#1
+double Table(8760, 5)
+#time_in_s	1	2	3	4
+0.0	10.375	10.455	11.25	0.0
+3600.0	10.5	10.425	11.235	0.0
+7200.0	10.5	10.425	11.235	0.0
+10800.0	10.375	10.425	11.235	0.0
+14400.0	10.5	10.44	11.205	0.0
+18000.0	10.5	10.41	11.25	0.0
+21600.0	10.375	10.41	11.145	0.0
+25200.0	10.125	10.38	11.145	0.0
+28800.0	10.125	10.3925	11.1125	0.0
+32400.0	10.25	10.395	11.145	0.0
+36000.0	10.5	10.3125	11.08	0.0
+39600.0	10.5	10.295	11.1125	0.0
+43200.0	10.5	10.33	11.145	0.0
+46800.0	10.5	10.4075	11.19	0.0
+50400.0	10.25	10.41	11.205	0.0
+54000.0	10.375	10.4525	11.25	0.0
+57600.0	10.375	10.3775	11.22	0.0
+61200.0	10.625	10.395	11.19	0.0
+64800.0	10.25	10.31	11.1275	0.0
+68400.0	10.0	10.28	11.095	0.0
+72000.0	10.25	10.345	11.1125	0.0
+75600.0	10.25	10.265	11.0625	0.0
+79200.0	10.375	10.235	11.03	0.0
+82800.0	10.25	10.28	11.0625	0.0
+86400.0	10.25	10.28	11.045	0.0
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+97200.0	10.25	10.25	11.0625	0.0
+100800.0	10.25	10.235	11.015	0.0
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+108000.0	10.125	10.19	11.03	0.0
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+176400.0	11.0	10.8775	10.955	0.0
+180000.0	10.875	10.845	10.91	0.0
+183600.0	10.75	10.8775	10.895	0.0
+187200.0	10.75	10.8775	10.955	0.0
+190800.0	10.75	10.8625	10.925	0.0
+194400.0	10.375	10.8125	10.955	0.0
+198000.0	10.625	10.55	11.0325	0.0
+201600.0	10.75	10.485	11.25	0.0
+205200.0	10.625	10.53	11.265	0.0
+208800.0	10.75	10.6125	11.28	0.0
+212400.0	10.625	10.58	11.28	0.0
+216000.0	10.625	10.595	11.2975	0.0
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+223200.0	10.625	10.515	11.395	0.0
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+237600.0	10.875	10.94	11.2675	0.0
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+288000.0	10.75	10.455	11.265	0.0
+291600.0	10.625	10.61	11.395	0.0
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+370800.0	10.375	10.515	11.25	0.0
+374400.0	10.75	10.595	11.36	0.0
+378000.0	10.625	10.735	11.44	0.0
+381600.0	10.5	10.72	11.455	0.0
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+406800.0	11.125	11.1275	11.455	0.0
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+417600.0	10.75	10.485	11.235	0.0
+421200.0	10.75	10.5	11.25	0.0
+424800.0	10.375	10.455	11.22	0.0
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+432000.0	10.375	10.425	11.205	0.0
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+453600.0	10.25	10.295	11.095	0.0
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diff --git a/AixLib/Resources/Data/schedule.txt b/AixLib/Resources/Data/schedule.txt
new file mode 100644
index 0000000000..799c8329bb
--- /dev/null
+++ b/AixLib/Resources/Data/schedule.txt
@@ -0,0 +1,5 @@
+# Comments start with a #
+mon:0:0:10          -  3   1  -
+# Comments can be added in the table too
+tue,thu:20:30:59  123  -  45  -
+wed                12  1   4  -
diff --git a/AixLib/Resources/Data/scheduleWindows.txt b/AixLib/Resources/Data/scheduleWindows.txt
new file mode 100644
index 0000000000..799c8329bb
--- /dev/null
+++ b/AixLib/Resources/Data/scheduleWindows.txt
@@ -0,0 +1,5 @@
+# Comments start with a #
+mon:0:0:10          -  3   1  -
+# Comments can be added in the table too
+tue,thu:20:30:59  123  -  45  -
+wed                12  1   4  -
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diff --git a/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix.png b/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix.png
new file mode 100644
index 0000000000..f4b13f5f4c
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diff --git a/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix.tex b/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix.tex
new file mode 100644
index 0000000000..294629c73b
--- /dev/null
+++ b/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix.tex
@@ -0,0 +1,16 @@
+\begin{pmatrix}
+  V_1^p - V_1^n \\
+  V_2^p - V_2^n \\
+  V_3^p - V_3^n
+ \end{pmatrix}
+ =
+ \begin{pmatrix}
+  Z_{1,1} & Z_{1,2} & Z_{1,3} \\
+  \cdot & Z_{2,2} & Z_{2,3} \\
+  \cdot & \cdot & Z_{3,3}
+ \end{pmatrix}
+ \begin{pmatrix}
+  I_1^p \\
+  I_2^p \\
+  I_3^p
+ \end{pmatrix}
diff --git a/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix_N.png b/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix_N.png
new file mode 100644
index 0000000000..6b5cd12c06
Binary files /dev/null and b/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix_N.png differ
diff --git a/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix_N.tex b/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix_N.tex
new file mode 100644
index 0000000000..a18a40d9e3
--- /dev/null
+++ b/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRLMatrix_N.tex
@@ -0,0 +1,19 @@
+\begin{pmatrix}
+  V_1^p - V_1^n \\
+  V_2^p - V_2^n \\
+  V_3^p - V_3^n \\
+  V_4^p - V_4^n
+ \end{pmatrix}
+ =
+ \begin{pmatrix}
+  Z_{1,1} & Z_{1,2} & Z_{1,3} & Z_{1,4} \\
+  \cdot & Z_{2,2} & Z_{2,3} & Z_{2,4}\\
+  \cdot & \cdot & Z_{3,3} & Z_{3,4}\\
+  \cdot & \cdot & \cdot & Z_{4,4}
+ \end{pmatrix}
+ \begin{pmatrix}
+  I_1^p \\
+  I_2^p \\
+  I_3^p \\
+  I_4^p
+ \end{pmatrix}
diff --git a/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRL_N.png b/AixLib/Resources/Images/Electrical/AC/ThreePhasesUnbalanced/Lines/twoPortRL_N.png
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index 0000000000..c36c196299
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index 0000000000..206b48fb3e
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diff --git a/AixLib/Resources/LowOrder_ExampleData/AHU_Input_SwimmingFacility_6Zones.txt b/AixLib/Resources/LowOrder_ExampleData/AHU_Input_SwimmingFacility_6Zones.txt
new file mode 100644
index 0000000000..8748e37370
--- /dev/null
+++ b/AixLib/Resources/LowOrder_ExampleData/AHU_Input_SwimmingFacility_6Zones.txt
@@ -0,0 +1,8762 @@
+#1
+double AHU(8760, 5)
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diff --git a/AixLib/Resources/LowOrder_ExampleData/InternalGains_SwimmingFacility_6Zones.txt b/AixLib/Resources/LowOrder_ExampleData/InternalGains_SwimmingFacility_6Zones.txt
new file mode 100644
index 0000000000..c446165bb5
--- /dev/null
+++ b/AixLib/Resources/LowOrder_ExampleData/InternalGains_SwimmingFacility_6Zones.txt
@@ -0,0 +1,8762 @@
+#1																		
+double Internals(8760, 19)																		
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diff --git a/AixLib/Resources/LowOrder_ExampleData/OpeningHours_SwimmingFacility.txt b/AixLib/Resources/LowOrder_ExampleData/OpeningHours_SwimmingFacility.txt
new file mode 100644
index 0000000000..80f261a651
--- /dev/null
+++ b/AixLib/Resources/LowOrder_ExampleData/OpeningHours_SwimmingFacility.txt
@@ -0,0 +1,17522 @@
+#1 
+double openingHours(17520,2)
+0    0
+1800    0
+1800	0
+3600	0
+5400	0
+7200	0
+9000	0
+10800	0
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diff --git a/AixLib/Resources/LowOrder_ExampleData/Tset_SwimmingFacility.txt b/AixLib/Resources/LowOrder_ExampleData/Tset_SwimmingFacility.txt
new file mode 100644
index 0000000000..d6f12febd0
--- /dev/null
+++ b/AixLib/Resources/LowOrder_ExampleData/Tset_SwimmingFacility.txt
@@ -0,0 +1,8762 @@
+#1						
+double Tset(8760,7)						
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_OpeningArea.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_OpeningArea.txt
new file mode 100644
index 0000000000..36ae2bc662
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_OpeningArea.txt
@@ -0,0 +1,38 @@
+last-generated=2024-07-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_VentilationFlowRateSashOpening.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_VentilationFlowRateSashOpening.txt
new file mode 100644
index 0000000000..68fdf70236
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_VentilationFlowRateSashOpening.txt
@@ -0,0 +1,25 @@
+last-generated=2024-07-15
+statistics-simulation=
+{
+  "linear": "0",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_VentilationFlowRateSimpleOpening.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_VentilationFlowRateSimpleOpening.txt
new file mode 100644
index 0000000000..1b4ff8e3c2
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_WindowVentilation_Examples_VentilationFlowRateSimpleOpening.txt
@@ -0,0 +1,23 @@
+last-generated=2024-07-15
+statistics-simulation=
+{
+  "linear": "0",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1.8e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_BoundaryConditions_SolarIrradiation_Examples_GlobalPerezTiltedSurface.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_BoundaryConditions_SolarIrradiation_Examples_GlobalPerezTiltedSurface.txt
new file mode 100644
index 0000000000..f7c1bec2ba
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_BoundaryConditions_SolarIrradiation_Examples_GlobalPerezTiltedSurface.txt
@@ -0,0 +1,11 @@
+last-generated=2022-11-11
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACConverter.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACConverter.txt
new file mode 100644
index 0000000000..c262c9ec38
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACConverter.txt
@@ -0,0 +1,13 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACTransformer.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACTransformer.txt
new file mode 100644
index 0000000000..27c3ce6232
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACTransformer.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACTransformerFull.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACTransformerFull.txt
new file mode 100644
index 0000000000..7ee65c49d8
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACACTransformerFull.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACDCConverter.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACDCConverter.txt
new file mode 100644
index 0000000000..a85d68dbdb
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Conversion_Examples_ACDCConverter.txt
@@ -0,0 +1,6 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Examples_GeneratorLoadGrid.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Examples_GeneratorLoadGrid.txt
new file mode 100644
index 0000000000..ef10afff27
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Examples_GeneratorLoadGrid.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Examples_GridDCLoad.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Examples_GridDCLoad.txt
new file mode 100644
index 0000000000..8badc28341
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Examples_GridDCLoad.txt
@@ -0,0 +1,8 @@
+last-generated=2015-05-08
+statistics-initialization={'numerical Jacobians': '0', 'nonlinear': '1', 'linear': '2'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine.txt
new file mode 100644
index 0000000000..abdc8530dc
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine.txt
@@ -0,0 +1,26 @@
+last-generated=2019-02-01
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+{
+  "linear": "2, 2, 3, 2, 2, 2, 3, 2"
+}
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+{
+  "linear": " ",
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_L.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_L.txt
new file mode 100644
index 0000000000..469530e0d9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_L.txt
@@ -0,0 +1,18 @@
+last-generated=2015-05-08
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_R.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_R.txt
new file mode 100644
index 0000000000..0d4fa0f0bf
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_R.txt
@@ -0,0 +1,18 @@
+last-generated=2015-05-08
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_RL.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_RL.txt
new file mode 100644
index 0000000000..6bb6a7db48
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACLine_RL.txt
@@ -0,0 +1,16 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACSimpleGrid.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACSimpleGrid.txt
new file mode 100644
index 0000000000..1e0864b9c7
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Lines_Examples_ACSimpleGrid.txt
@@ -0,0 +1,8 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_DynamicLoads.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_DynamicLoads.txt
new file mode 100644
index 0000000000..dcae360485
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_DynamicLoads.txt
@@ -0,0 +1,19 @@
+last-generated=2019-02-01
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+{
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+}
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+  "number of continuous time states": "4",
+  "numerical Jacobians": "0"
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_ParallelLoads.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_ParallelLoads.txt
new file mode 100644
index 0000000000..9f54b941bd
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_ParallelLoads.txt
@@ -0,0 +1,17 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_ParallelResistors.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_ParallelResistors.txt
new file mode 100644
index 0000000000..b2fee9bc16
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_ParallelResistors.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_TestImpedance.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_TestImpedance.txt
new file mode 100644
index 0000000000..f318457be5
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_TestImpedance.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_ThreePhases.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Loads_Examples_ThreePhases.txt
new file mode 100644
index 0000000000..60969f3d2c
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index 0000000000..58cf97f4ce
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sensors_Examples_GeneralizedSensor.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sensors_Examples_GeneralizedSensor.txt
new file mode 100644
index 0000000000..6c80e46251
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sensors_Examples_GeneralizedSensor.txt
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new file mode 100644
index 0000000000..7a2c6fc3e9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sensors_Examples_Probe.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sources_Examples_FixedVoltageSource.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sources_Examples_FixedVoltageSource.txt
new file mode 100644
index 0000000000..e79fdcc1d7
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sources_Examples_FixedVoltageSource.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sources_Examples_VariablePowerSource.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sources_Examples_VariablePowerSource.txt
new file mode 100644
index 0000000000..fb47906594
--- /dev/null
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new file mode 100644
index 0000000000..919bb9079a
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_OnePhase_Sources_Examples_WindTurbine.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Conversion_Examples_ACACConverter.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Conversion_Examples_ACACConverter.txt
new file mode 100644
index 0000000000..b4e8f95ebe
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Conversion_Examples_ACACConverter.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Conversion_Examples_ACACTransformer.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Conversion_Examples_ACACTransformer.txt
new file mode 100644
index 0000000000..680b66de1b
--- /dev/null
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Conversion_Examples_ACACTransformerFull.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Conversion_Examples_ACACTransformerFull.txt
new file mode 100644
index 0000000000..4aede3103d
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new file mode 100644
index 0000000000..d82d53408b
--- /dev/null
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine.txt
new file mode 100644
index 0000000000..f88b13c3f3
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLineMedium.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLineMedium.txt
new file mode 100644
index 0000000000..2371a4e64d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLineMedium.txt
@@ -0,0 +1,26 @@
+last-generated=2019-02-01
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+{
+  "linear": "3, 6, 7, 3, 4, 2, 6, 3"
+}
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+{
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_L.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_L.txt
new file mode 100644
index 0000000000..00343bea10
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_L.txt
@@ -0,0 +1,18 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_R.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_R.txt
new file mode 100644
index 0000000000..aa03fa3fae
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_R.txt
@@ -0,0 +1,18 @@
+last-generated=2015-05-08
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_RL.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_RL.txt
new file mode 100644
index 0000000000..dfa2342864
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACLine_RL.txt
@@ -0,0 +1,25 @@
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+{
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACSimpleGrid.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACSimpleGrid.txt
new file mode 100644
index 0000000000..92624c4aea
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Lines_Examples_ACSimpleGrid.txt
@@ -0,0 +1,18 @@
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index 0000000000..3406578f37
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Loads_Examples_ParallelLoads.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Loads_Examples_ParallelLoads.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Loads_Examples_ThreePhases.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Loads_Examples_ThreePhases.txt
new file mode 100644
index 0000000000..2240e3e780
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Loads_Examples_ThreePhases.txt
@@ -0,0 +1,18 @@
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sensors_Examples_GeneralizedSensor.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sensors_Examples_GeneralizedSensor.txt
new file mode 100644
index 0000000000..d19ca65963
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sensors_Examples_GeneralizedSensor.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sensors_Examples_Probe.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sensors_Examples_Probe.txt
new file mode 100644
index 0000000000..0e58a9d8b9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sensors_Examples_Probe.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sources_Examples_FixedVoltageSource.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sources_Examples_FixedVoltageSource.txt
new file mode 100644
index 0000000000..f5c3aeb1b4
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sources_Examples_FixedVoltageSource.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sources_Examples_VariablePowerSource.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesBalanced_Sources_Examples_VariablePowerSource.txt
new file mode 100644
index 0000000000..04da0af097
--- /dev/null
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_Converter.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_Converter.txt
new file mode 100644
index 0000000000..4323a219c2
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_Converter.txt
@@ -0,0 +1,21 @@
+last-generated=2015-05-08
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+probe_D_1.V[3]=[480., 480.]
+probe_D_1.V[2]=[480., 480.]
+probe_Y_1.V[2]=[277.128143310546875, 277.128143310546875]
+probe_D_1.V[1]=[480., 480.]
+probe_Y_1.V[3]=[277.128143310546875, 277.128143310546875]
+probe_Y_1.V[1]=[277.128143310546875, 277.128143310546875]
+time=[0., 1.]
+probe_2.V[2]=[138.5640716552734375, 138.5640716552734375]
+probe_2.V[3]=[138.5640716552734375, 138.5640716552734375]
+probe_2.V[1]=[138.5640716552734375, 138.5640716552734375]
+probe_Y_1.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
+probe_Y_1.theta[1]=[0., 0.]
+probe_Y_1.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_D_1.theta[2]=[-1.57079637050628662109, -1.57079637050628662109]
+probe_D_1.theta[1]=[0.52359879016876220703, 0.52359879016876220703]
+probe_D_1.theta[3]=[2.61799383163452148438, 2.61799383163452148438]
+probe_2.theta[1]=[0., 0.]
+probe_2.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_2.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_Transformer.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_Transformer.txt
new file mode 100644
index 0000000000..8b195f5bfa
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_Transformer.txt
@@ -0,0 +1,30 @@
+last-generated=2016-11-03
+statistics-initialization=
+{
+  "linear": "2, 2, 2"
+}
+statistics-simulation=
+{
+  "numerical Jacobians": "0", 
+  "nonlinear": " ", 
+  "linear": " "
+}
+probe_D_1.V[3]=[12470., 12470.]
+probe_D_1.V[2]=[12470., 12470.]
+probe_Y_1.V[2]=[7199.5576171875, 7199.5576171875]
+probe_D_1.V[1]=[12470., 12470.]
+probe_Y_1.V[3]=[7199.5576171875, 7199.5576171875]
+probe_Y_1.V[1]=[7199.5576171875, 7199.5576171875]
+time=[0., 1.]
+probe_2.V[2]=[2376.952392578125, 2376.952392578125]
+probe_2.V[3]=[2376.952392578125, 2376.952392578125]
+probe_2.V[1]=[2376.952392578125, 2376.952392578125]
+probe_Y_1.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
+probe_Y_1.theta[1]=[0., 0.]
+probe_Y_1.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_D_1.theta[2]=[-1.57079637050628662109, -1.57079637050628662109]
+probe_D_1.theta[1]=[0.52359879016876220703, 0.52359879016876220703]
+probe_D_1.theta[3]=[2.61799383163452148438, 2.61799383163452148438]
+probe_2.theta[1]=[-0.05346732586622238159, -0.05346732586622238159]
+probe_2.theta[2]=[-2.14786243438720703125, -2.14786243438720703125]
+probe_2.theta[3]=[2.040927886962890625, 2.040927886962890625]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerDD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerDD.txt
new file mode 100644
index 0000000000..72719c8e30
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerDD.txt
@@ -0,0 +1,30 @@
+last-generated=2016-11-03
+statistics-initialization=
+{
+  "linear": "8"
+}
+statistics-simulation=
+{
+  "numerical Jacobians": "0", 
+  "nonlinear": " ", 
+  "linear": " "
+}
+probe_D_1.V[3]=[12470., 12470.]
+probe_D_1.V[2]=[12470., 12470.]
+probe_Y_1.V[2]=[7199.5576171875, 7199.5576171875]
+probe_D_1.V[1]=[12470., 12470.]
+probe_Y_1.V[3]=[7199.5576171875, 7199.5576171875]
+probe_Y_1.V[1]=[7199.5576171875, 7199.5576171875]
+time=[0., 1.]
+probe_2.V[2]=[4117.001953125, 4117.001953125]
+probe_2.V[3]=[4117.001953125, 4117.001953125]
+probe_2.V[1]=[4117.001953125, 4117.001953125]
+probe_Y_1.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
+probe_Y_1.theta[1]=[0., 0.]
+probe_Y_1.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_D_1.theta[2]=[-1.57079637050628662109, -1.57079637050628662109]
+probe_D_1.theta[1]=[0.52359879016876220703, 0.52359879016876220703]
+probe_D_1.theta[3]=[2.61799383163452148438, 2.61799383163452148438]
+probe_2.theta[1]=[0.47013145685195922852, 0.47013145685195922852]
+probe_2.theta[2]=[-1.62426364421844482422, -1.62426364421844482422]
+probe_2.theta[3]=[2.56452655792236328125, 2.56452655792236328125]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerFull.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerFull.txt
new file mode 100644
index 0000000000..e91e57320e
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerFull.txt
@@ -0,0 +1,30 @@
+last-generated=2016-11-03
+statistics-initialization=
+{
+  "linear": "2, 2, 2, 2, 2, 2"
+}
+statistics-simulation=
+{
+  "numerical Jacobians": "0", 
+  "nonlinear": " ", 
+  "linear": " "
+}
+probe_D_1.V[3]=[12470., 12470.]
+probe_D_1.V[2]=[12470., 12470.]
+probe_Y_1.V[2]=[7199.5576171875, 7199.5576171875]
+probe_D_1.V[1]=[12470., 12470.]
+probe_Y_1.V[3]=[7199.5576171875, 7199.5576171875]
+probe_Y_1.V[1]=[7199.5576171875, 7199.5576171875]
+time=[0., 1.]
+probe_2.V[2]=[2385.810791015625, 2385.810791015625]
+probe_2.V[3]=[2385.810791015625, 2385.810791015625]
+probe_2.V[1]=[2385.810791015625, 2385.810791015625]
+probe_Y_1.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
+probe_Y_1.theta[1]=[0., 0.]
+probe_Y_1.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_D_1.theta[2]=[-1.57079637050628662109, -1.57079637050628662109]
+probe_D_1.theta[1]=[0.52359879016876220703, 0.52359879016876220703]
+probe_D_1.theta[3]=[2.61799383163452148438, 2.61799383163452148438]
+probe_2.theta[1]=[-0.02040015161037445068, -0.02040015161037445068]
+probe_2.theta[2]=[-2.11479520797729492188, -2.11479520797729492188]
+probe_2.theta[3]=[2.07399487495422363281, 2.07399487495422363281]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepDownDY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepDownDY.txt
new file mode 100644
index 0000000000..92629b9234
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepDownDY.txt
@@ -0,0 +1,30 @@
+last-generated=2016-11-03
+statistics-initialization=
+{
+  "linear": "2, 2, 2"
+}
+statistics-simulation=
+{
+  "numerical Jacobians": "0", 
+  "nonlinear": " ", 
+  "linear": " "
+}
+probe_D_1.V[3]=[12470., 12470.]
+probe_D_1.V[2]=[12470., 12470.]
+probe_Y_1.V[2]=[7199.5576171875, 7199.5576171875]
+probe_D_1.V[1]=[12470., 12470.]
+probe_Y_1.V[3]=[7199.5576171875, 7199.5576171875]
+probe_Y_1.V[1]=[7199.5576171875, 7199.5576171875]
+time=[0., 1.]
+probe_2.V[2]=[2376.952392578125, 2376.952392578125]
+probe_2.V[3]=[2376.952392578125, 2376.952392578125]
+probe_2.V[1]=[2376.952392578125, 2376.952392578125]
+probe_Y_1.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
+probe_Y_1.theta[1]=[0., 0.]
+probe_Y_1.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_D_1.theta[2]=[-1.57079637050628662109, -1.57079637050628662109]
+probe_D_1.theta[1]=[0.52359879016876220703, 0.52359879016876220703]
+probe_D_1.theta[3]=[2.61799383163452148438, 2.61799383163452148438]
+probe_2.theta[1]=[-0.57706612348556518555, -0.57706612348556518555]
+probe_2.theta[2]=[-2.6714611053466796875, -2.6714611053466796875]
+probe_2.theta[3]=[1.51732897758483886719, 1.51732897758483886719]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepDownYD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepDownYD.txt
new file mode 100644
index 0000000000..05d835473b
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepDownYD.txt
@@ -0,0 +1,30 @@
+last-generated=2016-11-03
+statistics-initialization=
+{
+  "linear": "8"
+}
+statistics-simulation=
+{
+  "numerical Jacobians": "0", 
+  "nonlinear": " ", 
+  "linear": " "
+}
+probe_D_1.V[3]=[12470., 12470.]
+probe_D_1.V[2]=[12470., 12470.]
+probe_Y_1.V[2]=[7199.5576171875, 7199.5576171875]
+probe_D_1.V[1]=[12470., 12470.]
+probe_Y_1.V[3]=[7199.5576171875, 7199.5576171875]
+probe_Y_1.V[1]=[7199.5576171875, 7199.5576171875]
+time=[0., 1.]
+probe_2.V[2]=[4117.001953125, 4117.001953125]
+probe_2.V[3]=[4117.001953125, 4117.001953125]
+probe_2.V[1]=[4117.001953125, 4117.001953125]
+probe_Y_1.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
+probe_Y_1.theta[1]=[0., 0.]
+probe_Y_1.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_D_1.theta[2]=[-1.57079637050628662109, -1.57079637050628662109]
+probe_D_1.theta[1]=[0.52359879016876220703, 0.52359879016876220703]
+probe_D_1.theta[3]=[2.61799383163452148438, 2.61799383163452148438]
+probe_2.theta[1]=[-0.05346732586622238159, -0.05346732586622238159]
+probe_2.theta[2]=[-2.14786243438720703125, -2.14786243438720703125]
+probe_2.theta[3]=[2.040927886962890625, 2.040927886962890625]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepUpDY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepUpDY.txt
new file mode 100644
index 0000000000..c3a669cbce
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepUpDY.txt
@@ -0,0 +1,30 @@
+last-generated=2016-11-03
+statistics-initialization=
+{
+  "linear": "2, 2, 2"
+}
+statistics-simulation=
+{
+  "numerical Jacobians": "0", 
+  "nonlinear": " ", 
+  "linear": " "
+}
+probe_D_1.V[3]=[4160., 4160.]
+probe_D_1.V[2]=[4160., 4160.]
+probe_Y_1.V[2]=[2401.777099609375, 2401.777099609375]
+probe_D_1.V[1]=[4160., 4160.]
+probe_Y_1.V[3]=[2401.777099609375, 2401.777099609375]
+probe_Y_1.V[1]=[2401.777099609375, 2401.777099609375]
+time=[0., 1.]
+probe_2.V[2]=[7125.14306640625, 7125.14306640625]
+probe_2.V[3]=[7125.14306640625, 7125.14306640625]
+probe_2.V[1]=[7125.14306640625, 7125.14306640625]
+probe_Y_1.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
+probe_Y_1.theta[1]=[0., 0.]
+probe_Y_1.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_D_1.theta[2]=[-1.57079637050628662109, -1.57079637050628662109]
+probe_D_1.theta[1]=[0.52359879016876220703, 0.52359879016876220703]
+probe_D_1.theta[3]=[2.61799383163452148438, 2.61799383163452148438]
+probe_2.theta[1]=[0.47013145685195922852, 0.47013145685195922852]
+probe_2.theta[2]=[-1.62426364421844482422, -1.62426364421844482422]
+probe_2.theta[3]=[2.56452655792236328125, 2.56452655792236328125]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepUpYD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepUpYD.txt
new file mode 100644
index 0000000000..e3a8bb88ed
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Conversion_Examples_TransformerStepUpYD.txt
@@ -0,0 +1,30 @@
+last-generated=2016-11-03
+statistics-initialization=
+{
+  "linear": "8"
+}
+statistics-simulation=
+{
+  "numerical Jacobians": "0", 
+  "nonlinear": " ", 
+  "linear": " "
+}
+probe_D_1.V[3]=[4160., 4160.]
+probe_D_1.V[2]=[4160., 4160.]
+probe_Y_1.V[2]=[2401.777099609375, 2401.777099609375]
+probe_D_1.V[1]=[4160., 4160.]
+probe_Y_1.V[3]=[2401.777099609375, 2401.777099609375]
+probe_Y_1.V[1]=[2401.777099609375, 2401.777099609375]
+time=[0., 1.]
+probe_2.V[2]=[12341.1103515625, 12341.1103515625]
+probe_2.V[3]=[12341.1103515625, 12341.1103515625]
+probe_2.V[1]=[12341.1103515625, 12341.1103515625]
+probe_Y_1.theta[3]=[2.09439516067504882812, 2.09439516067504882812]
+probe_Y_1.theta[1]=[0., 0.]
+probe_Y_1.theta[2]=[-2.09439516067504882812, -2.09439516067504882812]
+probe_D_1.theta[2]=[-1.57079637050628662109, -1.57079637050628662109]
+probe_D_1.theta[1]=[0.52359879016876220703, 0.52359879016876220703]
+probe_D_1.theta[3]=[2.61799383163452148438, 2.61799383163452148438]
+probe_2.theta[1]=[0.99373024702072143555, 0.99373024702072143555]
+probe_2.theta[2]=[-1.10066485404968261719, -1.10066485404968261719]
+probe_2.theta[3]=[3.0881252288818359375, 3.0881252288818359375]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Interfaces_Examples_WyeToDelta.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Interfaces_Examples_WyeToDelta.txt
new file mode 100644
index 0000000000..9438df3544
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Interfaces_Examples_WyeToDelta.txt
@@ -0,0 +1,9 @@
+last-generated=2015-05-08
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+probe_Y.V[1]=[277.128143310546875, 277.128143310546875]
+probeD.V[2]=[480., 480.]
+probeD.V[3]=[480., 480.]
+time=[0., 1.]
+probeD.V[1]=[480., 480.]
+probe_Y.V[3]=[277.128143310546875, 277.128143310546875]
+probe_Y.V[2]=[277.128143310546875, 277.128143310546875]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine.txt
new file mode 100644
index 0000000000..df1aa71362
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine.txt
@@ -0,0 +1,10 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '2, 2, 2, 2, 2, 2, 4, 4, 4, 2, 2, 2, 2, 2, 2, 4, 4, 4'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+R2.load1.i[1]=[26.1357288360595703125, 26.1357288360595703125]
+R2.load1.i[2]=[-0.07493173331022262573, -0.07493173331022262573]
+R1.load1.i[2]=[-0.07493173331022262573, -0.07493173331022262573]
+R3.load1.i[1]=[26.1357288360595703125, 26.1357288360595703125]
+R3.load1.i[2]=[-0.07493173331022262573, -0.07493173331022262573]
+R1.load1.i[1]=[26.1357288360595703125, 26.1357288360595703125]
+time=[0., 1.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RL.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RL.txt
new file mode 100644
index 0000000000..f42a4ccc5b
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RL.txt
@@ -0,0 +1,12 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '6, 6, 12, 6, 6, 12'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+Rline_1.terminal_n.phase[1].i[2]=[-5., -5.]
+Rline_1.terminal_n.phase[1].i[1]=[5., 5.]
+Rline_2a.terminal_n.phase[1].i[2]=[-5., -5.]
+Rline_2a.terminal_n.phase[1].i[1]=[5., 5.]
+time=[0., 1.]
+Rline_3a.terminal_n.phase[1].i[2]=[-2.5, -2.5]
+Rline_3a.terminal_n.phase[1].i[1]=[2.5, 2.5]
+Rline_3b.terminal_n.phase[1].i[1]=[2.5, 2.5]
+Rline_3b.terminal_n.phase[1].i[2]=[-2.5, -2.5]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RLC.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RLC.txt
new file mode 100644
index 0000000000..cd5ef49b58
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RLC.txt
@@ -0,0 +1,8 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '6, 12, 6'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+Rline_1.terminal_n.phase[1].i[2]=[-5., -5.]
+Rline_1.terminal_n.phase[1].i[1]=[5., 5.]
+time=[0., 1.]
+Rline_2.terminal_n.phase[1].i[1]=[0., 0.]
+Rline_2.terminal_n.phase[1].i[2]=[10., 10.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RLC_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RLC_N.txt
new file mode 100644
index 0000000000..cc345952f6
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RLC_N.txt
@@ -0,0 +1,8 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '8, 14, 14'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+Rline_1.terminal_n.phase[1].i[2]=[-5., -5.]
+Rline_1.terminal_n.phase[1].i[1]=[5., 5.]
+time=[0., 1.]
+Rline_2.terminal_n.phase[1].i[1]=[0., 0.]
+Rline_2.terminal_n.phase[1].i[2]=[10., 10.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RL_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RL_N.txt
new file mode 100644
index 0000000000..386077f50e
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLineMatrix_RL_N.txt
@@ -0,0 +1,12 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '6, 6, 14, 6, 6, 14'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+Rline_1.terminal_n.phase[1].i[2]=[-5., -5.]
+Rline_1.terminal_n.phase[1].i[1]=[5., 5.]
+Rline_2a.terminal_n.phase[1].i[2]=[-5., -5.]
+Rline_2a.terminal_n.phase[1].i[1]=[5., 5.]
+time=[0., 1.]
+Rline_3a.terminal_n.phase[1].i[2]=[-2.5, -2.5]
+Rline_3a.terminal_n.phase[1].i[1]=[2.5, 2.5]
+Rline_3b.terminal_n.phase[1].i[1]=[2.5, 2.5]
+Rline_3b.terminal_n.phase[1].i[2]=[-2.5, -2.5]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_L.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_L.txt
new file mode 100644
index 0000000000..8294483fce
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_L.txt
@@ -0,0 +1,12 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '2, 2, 2, 4, 2, 2, 2, 4, 2, 2, 2, 4'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+E.vPhase[1].terminal.v[1]=[277.128143310546875, 277.128143310546875]
+L3.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+L2.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+L1.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+time=[0., 1.]
+L3.load1.i[2]=[-13.85640621185302734375, -13.85640621185302734375]
+L2.load1.i[2]=[-13.85640621185302734375, -13.85640621185302734375]
+sc_load.load1.i[2]=[-13.85640621185302734375, -13.85640621185302734375]
+L1.load1.i[2]=[-13.85640621185302734375, -13.85640621185302734375]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_L_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_L_N.txt
new file mode 100644
index 0000000000..fb6cada1c4
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_L_N.txt
@@ -0,0 +1,12 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '6, 6, 6, 14'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+E.vPhase[1].terminal.v[1]=[277.128143310546875, 277.128143310546875]
+L3.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+L2.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+L1.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+time=[0., 1.]
+L3.load1.i[2]=[-13.85640621185302734375, -13.85640621185302734375]
+L2.load1.i[2]=[-13.85640621185302734375, -13.85640621185302734375]
+sc_load.load1.i[2]=[-13.85640621185302734375, -13.85640621185302734375]
+L1.load1.i[2]=[-13.85640621185302734375, -13.85640621185302734375]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_N.txt
new file mode 100644
index 0000000000..a9a0bcdb8d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_N.txt
@@ -0,0 +1,10 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '6, 6, 11, 6, 6, 11'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+R2.load1.i[1]=[26.1357288360595703125, 26.1357288360595703125]
+R2.load1.i[2]=[-0.07493173331022262573, -0.07493173331022262573]
+R1.load1.i[2]=[-0.07493173331022262573, -0.07493173331022262573]
+R3.load1.i[1]=[26.1357288360595703125, 26.1357288360595703125]
+R3.load1.i[2]=[-0.07493173331022262573, -0.07493173331022262573]
+R1.load1.i[1]=[26.1357288360595703125, 26.1357288360595703125]
+time=[0., 1.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_R.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_R.txt
new file mode 100644
index 0000000000..9c45239fd5
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_R.txt
@@ -0,0 +1,12 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '2, 2, 4, 2, 2, 2, 4, 2, 2, 2, 4, 2'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+E.vPhase[1].terminal.v[1]=[277.128143310546875, 277.128143310546875]
+R2.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+R1.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+R3.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
+time=[0., 1.]
+R2.load1.i[1]=[13.85640621185302734375, 13.85640621185302734375]
+R1.load1.i[1]=[13.85640621185302734375, 13.85640621185302734375]
+sc_load.load1.i[1]=[13.85640621185302734375, 13.85640621185302734375]
+R3.load1.i[1]=[13.85640621185302734375, 13.85640621185302734375]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RL.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RL.txt
new file mode 100644
index 0000000000..c2e68b9966
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RL.txt
@@ -0,0 +1,25 @@
+last-generated=2017-04-05
+statistics-initialization=
+{
+  "linear": "2, 2, 2, 2, 2, 2, 2, 2, 2"
+}
+statistics-simulation=
+{
+  "numerical Jacobians": "0", 
+  "nonlinear": " ", 
+  "number of continuous time states": "6", 
+  "linear": " "
+}
+load_sc_3.load1.v[2]=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -0e+00]
+load_sc_2.load1.v[1]=[0e+00, 0e+00]
+load_sc_1.load1.v[1]=[0e+00, 0e+00]
+load_sc_3.load1.v[1]=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+load_sc_1.load1.v[2]=[0e+00, 0e+00]
+time=[0e+00, 1e+00]
+load_sc_2.load1.v[2]=[-0e+00, -0e+00]
+load_sc_1.load1.i[1]=[5e+00, 5e+00]
+load_sc_2.load1.i[1]=[5e+00, 5e+00]
+load_sc_3.load1.i[1]=[0e+00, 5.025498382528636e+00, 5.001641750364364e+00, 4.999895095846938e+00, 5.000010490415775e+00, 4.99999713897634e+00, 5.000000953674316e+00, 5.000000476837158e+00, 4.999999523162842e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00, 5e+00]
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+load_sc_2.load1.i[2]=[-5e+00, -5e+00]
+load_sc_1.load1.i[2]=[-5e+00, -5e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RLC.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RLC.txt
new file mode 100644
index 0000000000..e37516ad0f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RLC.txt
@@ -0,0 +1,23 @@
+last-generated=2019-02-01
+statistics-initialization=
+{
+  "linear": "3, 3, 3, 6, 6, 6, 7, 7, 7, 2, 2, 2, 4, 4, 4, 6, 6, 6"
+}
+statistics-simulation=
+{
+  "linear": "0, 2, 0, 2, 0, 2",
+  "nonlinear": " ",
+  "number of continuous time states": "6",
+  "numerical Jacobians": "0"
+}
+RLCLine_sc.terminal_n.phase[1].i[2]=[1.771281242370605e+01, -2.001048802951823e+00, -2.000007867811991e+00, -2.000000238418579e+00, -1.999999880790764e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00]
+RLCLine_1.terminal_n.phase[1].i[1]=[6e+00, 6e+00]
+RLCLine_1.terminal_n.phase[1].i[2]=[-2e+00, -2e+00]
+RLCLine_sc.terminal_n.phase[1].i[1]=[-1.771281242370605e+01, 6.016360281381189e+00, 5.999994277955594e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00, 6e+00]
+time=[0e+00, 1e+00]
+RLCLine_2a.terminal_n.phase[1].i[1]=[5.444247722625732e+00, 5.444247722625732e+00]
+RLCLine_2a.terminal_n.phase[1].i[2]=[-1.536283135414124e+00, -1.536283135414124e+00]
+RLCLine_3a.terminal_n.phase[1].i[1]=[3e+00, 3e+00]
+RLCLine_3b.terminal_n.phase[1].i[1]=[3e+00, 3e+00]
+RLCLine_3b.terminal_n.phase[1].i[2]=[-1e+00, -1e+00]
+RLCLine_3a.terminal_n.phase[1].i[2]=[-1e+00, -1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RLC_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RLC_N.txt
new file mode 100644
index 0000000000..6e63486467
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RLC_N.txt
@@ -0,0 +1,23 @@
+last-generated=2019-02-01
+statistics-initialization=
+{
+  "linear": "14, 22, 27, 8, 12, 23"
+}
+statistics-simulation=
+{
+  "linear": "0, 6, 0, 0, 0",
+  "nonlinear": " ",
+  "number of continuous time states": "8",
+  "numerical Jacobians": "0"
+}
+RLCLine_sc.terminal_n.phase[1].i[2]=[1.771281242370605e+01, -2.001103639223165e+00, -2.000000953674423e+00, -1.99999988079075e+00, -2e+00, -1.999999999999956e+00, -2e+00, -2e+00, -1.99999988079071e+00, -1.99999988079071e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00, -2e+00]
+RLCLine_1.terminal_n.phase[1].i[1]=[6e+00, 6e+00]
+RLCLine_1.terminal_n.phase[1].i[2]=[-2e+00, -2e+00]
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+time=[0e+00, 1e+00]
+RLCLine_2a.terminal_n.phase[1].i[1]=[5.444247722625732e+00, 5.444247722625732e+00]
+RLCLine_2a.terminal_n.phase[1].i[2]=[-1.536283135414124e+00, -1.536283135414124e+00]
+RLCLine_3a.terminal_n.phase[1].i[1]=[3e+00, 3e+00]
+RLCLine_3b.terminal_n.phase[1].i[1]=[3e+00, 3e+00]
+RLCLine_3b.terminal_n.phase[1].i[2]=[-1e+00, -1e+00]
+RLCLine_3a.terminal_n.phase[1].i[2]=[-1e+00, -1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RL_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RL_N.txt
new file mode 100644
index 0000000000..8cf13be996
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_RL_N.txt
@@ -0,0 +1,12 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '6, 6, 6'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+load_sc_1.load1.v[1]=[0., 0.]
+load_sc_2.load1.v[2]=[-0., -0.]
+load_sc_2.load1.v[1]=[0., 0.]
+load_sc_1.load1.v[2]=[0., 0.]
+time=[0., 1.]
+load_sc_2.load1.i[2]=[-5., -5.]
+load_sc_1.load1.i[2]=[-5., -5.]
+load_sc_2.load1.i[1]=[5., 5.]
+load_sc_1.load1.i[1]=[5., 5.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_R_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_R_N.txt
new file mode 100644
index 0000000000..185a7adb3f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACLine_R_N.txt
@@ -0,0 +1,12 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '6, 6, 14, 6'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+E.vPhase[1].terminal.v[1]=[277.128143310546875, 277.128143310546875]
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+R3.terminal.phase[1].v[1]=[138.5640716552734375, 138.5640716552734375]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACSimpleGrid.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACSimpleGrid.txt
new file mode 100644
index 0000000000..fbbb2b712f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACSimpleGrid.txt
@@ -0,0 +1,10 @@
+last-generated=2015-05-08
+statistics-initialization={'numerical Jacobians': '0', 'nonlinear': '2, 2', 'linear': '2, 2'}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACSimpleGrid_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACSimpleGrid_N.txt
new file mode 100644
index 0000000000..848a1a37ee
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Lines_Examples_ACSimpleGrid_N.txt
@@ -0,0 +1,14 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Impedances.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Impedances.txt
new file mode 100644
index 0000000000..376acffcd9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Impedances.txt
@@ -0,0 +1,10 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_LoadCtrl.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_LoadCtrl.txt
new file mode 100644
index 0000000000..39dd2ed4df
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_LoadCtrl.txt
@@ -0,0 +1,23 @@
+last-generated=2017-04-05
+statistics-initialization=
+{
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+  "nonlinear": "2, 2", 
+  "linear": "2, 2"
+}
+statistics-simulation=
+{
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+  "nonlinear": "3, 2", 
+  "number of continuous time states": "1", 
+  "linear": "2, 2"
+}
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+time=[0e+00, 1e+01]
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+load_ctrl.vCTRL_1.Vmin=[2.63271728515625e+02, 2.63271728515625e+02]
+load_ctrl.vCTRL_1.V_nominal=[2.771281433105469e+02, 2.771281433105469e+02]
+load_ctrl.vCTRL_1.terminal.v[1]=[2.872103576660156e+02, 2.876683044365495e+02, 2.881230468614986e+02, 2.885728454056517e+02, 2.890159301495514e+02, 2.894506530761719e+02, 2.898753966282895e+02, 2.902885132319424e+02, 2.906885375506537e+02, 2.784761338667478e+02, 2.77128173828125e+02, 2.771281127929688e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.838973080517237e+02, 2.7712841796875e+02, 2.771281127929688e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.771281433105469e+02, 2.827389109008705e+02, 2.872101745605469e+02, 2.867510066419196e+02, 2.862921133844057e+02, 2.858353585347658e+02, 2.853826298242497e+02, 2.849357299804688e+02, 2.84496551100106e+02, 2.840669242417782e+02, 2.836485908763141e+02, 2.832432865139275e+02, 2.828528137207031e+02, 2.824787289014199e+02, 2.821227410420536e+02, 2.817863165439928e+02, 2.814709780756969e+02, 2.811781311035156e+02, 2.80908965822018e+02, 2.806648250031863e+02, 2.804467167041152e+02, 2.802556154060878e+02, 2.800924377441406e+02, 2.799578856305742e+02, 2.798525999306001e+02, 2.797770386955818e+02, 2.797315674146813e+02, 2.797164001464844e+02, 2.797315674146813e+02, 2.797770386955818e+02, 2.798525999308911e+02, 2.799579161480068e+02, 2.800924377441406e+02, 2.802556450860727e+02, 2.804467167043968e+02, 2.806648555207748e+02, 2.809090280885349e+02, 2.811781616210938e+02, 2.81471007148878e+02, 2.817863775791341e+02, 2.821228020772256e+02, 2.824787611660693e+02, 2.828528442382812e+02, 2.832433151376081e+02, 2.836485908765864e+02, 2.840669547593755e+02, 2.844965531754626e+02, 2.849356994628906e+02, 2.853825361276205e+02, 2.858352669820107e+02, 2.862920218316922e+02, 2.867510088326707e+02, 2.872103576660156e+02]
+load_ctrl.vCTRL_1.Vmax=[2.909845275878906e+02, 2.909845275878906e+02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Loads.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Loads.txt
new file mode 100644
index 0000000000..543c4d06a6
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Loads.txt
@@ -0,0 +1,15 @@
+last-generated=2015-05-08
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+sen.S[2, 2]=[0., 0.]
+sen.S[2, 1]=[0., 0.]
+sen.S[1, 1]=[7500., 3973.28850933486273788731, 1793.6608467882047079911, 1793.66098166956157911045, 3973.28885861755134101259, 7499.99971985839874832891, 11026.71230336516782699618, 13206.33882585504397866316, 13206.33861919368064263836, 11026.71295220101455925032, 7500.00056028179551503854, 3973.28840119537335340283, 1793.66063737032209246536, 1793.66154998814363352722, 3973.28840119537744612899, 7499.99775887135092489189, 11026.71295220101455925032, 13206.33861919368246162776, 13206.33953732628651778214, 11026.71115566710977873299, 7500.00112056359193957178, 3973.28667096160961591522, 1793.66077698229560155596, 1793.66049775834835600108, 3973.29028060837526936666, 7500., 11026.71468243187155167107, 13206.33737922458931279834, 13206.33897887729472131468, 11026.70925967864059202839, 7500.00448225438685767585, 3973.28933261414113076171, 1793.66021853439860933577, 1793.65966008650434559968, 3973.28753607849739637459, 7500.00224112718296964886, 11026.70736369015321542975, 13206.33820587064838036895, 13206.33820587064838036895, 11026.70736369015321542975, 7500.00224112718296964886, 3973.28753607849739637459, 1793.65966008650434559968, 1793.66021853439860933577, 3973.28933261414113076171, 7500.00448225438685767585, 11026.70925967864059202839, 13206.33897887729472131468, 13206.33737922458931279834, 11026.71468243187155167107, 7500., 3973.28580588597287714947, 1793.65910166523303814756, 1793.66485651036214221676, 3973.28234547001738974359, 7499.99551780951333057601, 11026.71115565582476847339, 13206.33953731629480898846, 13206.33655261302010330837, 11026.70357183752457785886, 7500.00896437519440951291, 3973.29312452329168081633, 1793.66154997828948580718, 1793.66154997828948580718, 3973.29312452329168081633, 7500.00896437519440951291, 11026.70357183752457785886, 13206.33655261302010330837, 13206.33953731629480898846, 11026.71115565582476847339, 7499.99551780951333057601, 3973.28234547001738974359, 1793.66485651036214221676, 1793.65910166523303814756, 3973.28580588597287714947, 7500., 11026.71468239062050997745, 13206.34065419763464888092, 13206.33489934552017075475, 11026.71814280075523129199, 7500.00448218757628637832, 3973.2893326254243220319, 1793.66021854438940863474, 1793.66320324431808330701, 3973.29691644372542214114, 7499.99103561898482439574, 11026.70736375795786443632, 13206.33820588050366495736, 13206.33820588050366495736, 11026.70736375795786443632, 7499.99103561898482439574, 3973.29691644372542214114, 1793.66320324431808330701, 1793.66021854438940863474, 3973.2893326254243220319, 7500.00448218757628637832, 11026.71814280075523129199, 13206.33489934552017075475, 13206.34065419763464888092, 11026.71468239062050997745, 7500.]
+time=[0., 1.]
+sen.S[3, 1]=[-0., -0.]
+sen.S[3, 2]=[-0., -0.]
+sen.S[1, 2]=[0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0., 0.]
+senSingleConn.S[3, 1]=[0., 0.]
+senSingleConn.S[2, 2]=[0., 0.]
+senSingleConn.S[3, 2]=[0., 0.]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Loads_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Loads_N.txt
new file mode 100644
index 0000000000..d6089fce41
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Loads_Examples_Loads_N.txt
@@ -0,0 +1,7 @@
+last-generated=2015-05-08
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
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+time=[0., 1.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sensors_Examples_Sensors.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sensors_Examples_Sensors.txt
new file mode 100644
index 0000000000..e10f948c4e
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sensors_Examples_Sensors.txt
@@ -0,0 +1,32 @@
+last-generated=2015-05-08
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+probeWye.V[2]=[1., 1.]
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+time=[0., 1.]
+probeDelta.V[1]=[1., 1.]
+probeDelta.V[2]=[1., 1.]
+probeDelta.V[3]=[1., 1.]
+probeWye_N.V[3]=[1., 1.]
+probeWye_N.V[2]=[1., 1.]
+probeWye_N.V[1]=[1., 1.]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_FixedVoltageSource.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_FixedVoltageSource.txt
new file mode 100644
index 0000000000..f324cf672b
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_FixedVoltageSource.txt
@@ -0,0 +1,15 @@
+last-generated=2015-05-08
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+sen_N.V[1]=[1., 1.]
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+sen_N.V[2]=[1., 1.]
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+sen.V[3]=[1., 1.]
+sen.V[2]=[1., 1.]
+sen_N.theta[3]=[-1.91986215114593505859, -1.91986215114593505859]
+sen_N.theta[2]=[2.26892805099487304688, 2.26892805099487304688]
+sen.theta[1]=[0.17453292012214660645, 0.17453292012214660645]
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+sen.theta[3]=[2.26892805099487304688, 2.26892805099487304688]
+sen.theta[2]=[-1.91986215114593505859, -1.91986215114593505859]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_WindTurbine.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_WindTurbine.txt
new file mode 100644
index 0000000000..4a1dd71181
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_WindTurbine.txt
@@ -0,0 +1,23 @@
+last-generated=2019-06-13
+statistics-initialization=
+{
+  "linear": "2, 2, 2",
+  "nonlinear": "2, 2, 2",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "2, 2, 2",
+  "nonlinear": "2, 2, 2",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_WindTurbine_N.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_WindTurbine_N.txt
new file mode 100644
index 0000000000..a626f4d637
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Sources_Examples_WindTurbine_N.txt
@@ -0,0 +1,23 @@
+last-generated=2019-06-13
+statistics-initialization=
+{
+  "linear": "4",
+  "nonlinear": "3",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "4",
+  "nonlinear": "4",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_DD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_DD.txt
new file mode 100644
index 0000000000..a887979f60
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_DD.txt
@@ -0,0 +1,31 @@
+last-generated=2022-08-05
+statistics-initialization=
+{
+  "nonlinear": "8",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_DY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_DY.txt
new file mode 100644
index 0000000000..f1be70fbb9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_DY.txt
@@ -0,0 +1,22 @@
+last-generated=2015-05-08
+statistics-initialization={'numerical Jacobians': '0', 'nonlinear': '12'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+err_V3[3]=[0.23434446752071380615, 0.23434446752071380615]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_YD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_YD.txt
new file mode 100644
index 0000000000..069a709a4e
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_YD.txt
@@ -0,0 +1,31 @@
+last-generated=2022-08-05
+statistics-initialization=
+{
+  "nonlinear": "8",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
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+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_YY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_YY.txt
new file mode 100644
index 0000000000..79e175c090
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepDown_YY.txt
@@ -0,0 +1,22 @@
+last-generated=2015-05-08
+statistics-initialization={'numerical Jacobians': '0', 'nonlinear': '12'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_DD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_DD.txt
new file mode 100644
index 0000000000..408e1814e3
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_DD.txt
@@ -0,0 +1,31 @@
+last-generated=2022-08-05
+statistics-initialization=
+{
+  "nonlinear": "8",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_DY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_DY.txt
new file mode 100644
index 0000000000..b172326299
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_DY.txt
@@ -0,0 +1,22 @@
+last-generated=2015-05-08
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_YD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_YD.txt
new file mode 100644
index 0000000000..d54fb0669d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_YD.txt
@@ -0,0 +1,31 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_YY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_YY.txt
new file mode 100644
index 0000000000..c88576b21a
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_BalancedStepUp_YY.txt
@@ -0,0 +1,22 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_DD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_DD.txt
new file mode 100644
index 0000000000..f785ff4d84
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_DD.txt
@@ -0,0 +1,31 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_DY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_DY.txt
new file mode 100644
index 0000000000..1c02e5045b
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_DY.txt
@@ -0,0 +1,22 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_YD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_YD.txt
new file mode 100644
index 0000000000..f994f8a75f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_YD.txt
@@ -0,0 +1,31 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_YY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_YY.txt
new file mode 100644
index 0000000000..081f41ac57
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepDown_YY.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_DD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_DD.txt
new file mode 100644
index 0000000000..ba892d1ec6
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_DD.txt
@@ -0,0 +1,31 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_DY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_DY.txt
new file mode 100644
index 0000000000..ab7433573c
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_DY.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_YD.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_YD.txt
new file mode 100644
index 0000000000..338991e468
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_YD.txt
@@ -0,0 +1,31 @@
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+err_V4[3]=[-5.498391389846802e-01, -5.498391389846802e-01]
+err_Theta2[1]=[2.314654120709747e-04, 2.314654120709747e-04]
+err_Theta2[2]=[7.110466249287128e-04, 7.110466249287128e-04]
+err_Theta2[3]=[7.122518727555871e-04, 7.122518727555871e-04]
+err_Theta3[1]=[3.787593741435558e-04, 3.787593741435558e-04]
+err_Theta3[2]=[-7.20113484931062e-06, -7.20113484931062e-06]
+err_Theta3[3]=[-2.180294723075349e-05, -2.180294723075349e-05]
+err_Theta4[1]=[7.338505238294601e-04, 7.338505238294601e-04]
+err_Theta4[2]=[8.281824411824346e-04, 8.281824411824346e-04]
+err_Theta4[3]=[6.261589005589485e-04, 6.261589005589485e-04]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_YY.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_YY.txt
new file mode 100644
index 0000000000..ad028d4ef0
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_AC_ThreePhasesUnbalanced_Validation_IEEETests_Test4NodesFeeder_UnbalancedStepUp_YY.txt
@@ -0,0 +1,22 @@
+last-generated=2015-05-08
+statistics-initialization={'numerical Jacobians': '0', 'nonlinear': '12'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+err_V3[3]=[0.16021563112735748291, 0.16021563112735748291]
+err_V4[1]=[0.37761300802230834961, 0.37761300802230834961]
+err_V4[3]=[-0.06358843296766281128, -0.06358843296766281128]
+err_V4[2]=[0.20272503793239593506, 0.20272503793239593506]
+err_V2[3]=[-0.49103468656539916992, -0.49103468656539916992]
+err_V2[1]=[-0.11977462470531463623, -0.11977462470531463623]
+time=[0., 1.]
+err_V3[2]=[-0.30366429686546325684, -0.30366429686546325684]
+err_V2[2]=[0.18549895286560058594, 0.18549895286560058594]
+err_V3[1]=[0.32745033502578735352, 0.32745033502578735352]
+err_Theta4[1]=[0.00049209891585633159, 0.00049209891585633159]
+err_Theta4[3]=[-0.00038532013422809541, -0.00038532013422809541]
+err_Theta3[2]=[0.00018433525110594928, 0.00018433525110594928]
+err_Theta4[2]=[0.000266846182057634, 0.000266846182057634]
+err_Theta3[3]=[0.00068887084489688277, 0.00068887084489688277]
+err_Theta3[1]=[-0.00070652569411322474, -0.00070652569411322474]
+err_Theta2[3]=[-0.00089562020730227232, -0.00089562020730227232]
+err_Theta2[2]=[0.00078997417585924268, 0.00078997417585924268]
+err_Theta2[1]=[0.00026117765810340643, 0.00026117765810340643]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Conversion_Examples_DCDCConverter.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Conversion_Examples_DCDCConverter.txt
new file mode 100644
index 0000000000..7ac51b8e99
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Conversion_Examples_DCDCConverter.txt
@@ -0,0 +1,10 @@
+last-generated=2024-01-08
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
+sen.I=[2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.75e+01, 2.566666646798378e+01, 2.383333265781623e+01, 2.200000240404997e+01, 2.016666668653378e+01, 1.833333287636623e+01, 1.650000262259997e+01, 1.466666785875809e+01, 1.283333214124191e+01, 1.099999737740003e+01, 9.166668077308087e+00, 7.333332836629066e+00, 5.499997595950036e+00, 3.666668057438657e+00, 1.833332935969911e+00, -1.806197763700692e-06, -1.515150236363731e+00, -3.030303182023544e+00, -4.545456127684645e+00, -6.060604557850836e+00, -7.575757503509521e+00, -9.090910449146675e+00, -1.060606387162099e+01, -1.212121634042098e+01, -1.363636073203976e+01, -1.515151320084999e+01, -1.666666566963922e+01, -1.818181909212428e+01, -1.969697251459859e+01, -2.12121259370729e+01, -2.272726842135328e+01, -2.42424218438276e+01, -2.575757526630191e+01, -2.727272868877622e+01, -2.878788020391554e+01, -3.030303362637621e+01, -3.181817801800522e+01, -3.333332953314682e+01, -3.484848295561203e+01, -3.636363637809254e+01, -3.787878980056519e+01, -3.939394322300767e+01, -4.090908761462986e+01, -4.242424103711326e+01, -4.393939064491759e+01, -4.545454406738281e+01, -4.696969748986622e+01, -4.848485091234963e+01, -5.000000433483303e+01, -5.15151487264143e+01, -5.30303021488977e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01, -5.303030395507812e+01]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLine.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLine.txt
new file mode 100644
index 0000000000..3df09f30ad
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLine.txt
@@ -0,0 +1,21 @@
+last-generated=2019-02-01
+statistics-initialization=
+{
+  "linear": "0",
+  "nonlinear": "2, 2, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0",
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
+line1.R=[2.105000019073486e-01, 2.105000019073486e-01]
+line.R=[2.105000019073486e-01, 2.105000019073486e-01]
+line2.R=[2.105000019073486e-01, 2.105000019073486e-01]
+time=[0e+00, 1e+00]
+load2.i[1]=[3.038878440856934e+00, 3.038878440856934e+00]
+load3.i[1]=[4.069728851318359e+00, 4.069728851318359e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLines.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLines.txt
new file mode 100644
index 0000000000..80648476c4
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLines.txt
@@ -0,0 +1,16 @@
+last-generated=2019-02-01
+statistics-initialization=
+{
+  "linear": "15",
+  "nonlinear": "16",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "14",
+  "nonlinear": "17",
+  "numerical Jacobians": "0"
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLinesLinearized.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLinesLinearized.txt
new file mode 100644
index 0000000000..efa6a53c37
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_DCLinesLinearized.txt
@@ -0,0 +1,10 @@
+last-generated=2019-02-01
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_RCModel.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_RCModel.txt
new file mode 100644
index 0000000000..f0cb301ec4
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_RCModel.txt
@@ -0,0 +1,8 @@
+last-generated=2015-05-08
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_Resistance.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_Resistance.txt
new file mode 100644
index 0000000000..36ecbd62f2
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Lines_Examples_Resistance.txt
@@ -0,0 +1,5 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '0'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+sen.I=[5., 5.]
+time=[0., 1.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_LinearizedLoad.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_LinearizedLoad.txt
new file mode 100644
index 0000000000..93debd3ae7
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_LinearizedLoad.txt
@@ -0,0 +1,11 @@
+last-generated=2015-05-08
+statistics-initialization={'numerical Jacobians': '0', 'nonlinear': '1'}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_Resistor.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_Resistor.txt
new file mode 100644
index 0000000000..3e7266d5c1
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_Resistor.txt
@@ -0,0 +1,6 @@
+last-generated=2015-05-08
+statistics-initialization={'linear': '0'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+sen.I=[3., 3.]
+sen1.I=[6., 6.]
+time=[0., 1.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_VariableLoad.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_VariableLoad.txt
new file mode 100644
index 0000000000..0b9784f024
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Loads_Examples_VariableLoad.txt
@@ -0,0 +1,7 @@
+last-generated=2015-05-08
+statistics-initialization={'numerical Jacobians': '0', 'nonlinear': '1'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sensors_Examples_GeneralizedSensor.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sensors_Examples_GeneralizedSensor.txt
new file mode 100644
index 0000000000..fc6ff017db
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sensors_Examples_GeneralizedSensor.txt
@@ -0,0 +1,5 @@
+last-generated=2015-05-08
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'linear': ' '}
+sen.I=[-1., -1.]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sources_Examples_VoltageSource.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sources_Examples_VoltageSource.txt
new file mode 100644
index 0000000000..9fd88bcab8
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sources_Examples_VoltageSource.txt
@@ -0,0 +1,5 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sources_Examples_WindTurbine.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sources_Examples_WindTurbine.txt
new file mode 100644
index 0000000000..89e1fc5b68
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_DC_Sources_Examples_WindTurbine.txt
@@ -0,0 +1,9 @@
+last-generated=2015-05-08
+statistics-initialization={'numerical Jacobians': '0', 'nonlinear': '1'}
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': '1', 'linear': ' '}
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+tur.vIn=[3.5, 3.5]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Transmission_Functions_Validation_SelectCable_low.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Transmission_Functions_Validation_SelectCable_low.txt
new file mode 100644
index 0000000000..38ed4f0999
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Transmission_Functions_Validation_SelectCable_low.txt
@@ -0,0 +1,15 @@
+last-generated=2020-08-25
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
+cab[1].Amp=[6.5e+01, 6.5e+01]
+cab[2].Amp=[9.5e+01, 9.5e+01]
+cab[3].Amp=[1.1e+02, 1.1e+02]
+cab[4].Amp=[1.3e+02, 1.3e+02]
+cab[5].Amp=[1.7e+02, 1.7e+02]
+cab[6].Amp=[2.2e+02, 2.2e+02]
+cab[7].Amp=[2.3e+02, 2.3e+02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Transmission_Functions_Validation_SelectCable_med.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Transmission_Functions_Validation_SelectCable_med.txt
new file mode 100644
index 0000000000..dca75c8310
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Transmission_Functions_Validation_SelectCable_med.txt
@@ -0,0 +1,15 @@
+last-generated=2020-08-25
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
+cab[1].Amp=[1.95e+02, 1.95e+02]
+cab[2].Amp=[2.5e+02, 2.5e+02]
+cab[3].Amp=[2.85e+02, 2.85e+02]
+cab[4].Amp=[3.75e+02, 3.75e+02]
+cab[5].Amp=[4.5e+02, 4.5e+02]
+cab[6].Amp=[6.4e+02, 6.4e+02]
+cab[7].Amp=[8e+02, 8e+02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Utilities_Examples_TestVoltageCTRL.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Utilities_Examples_TestVoltageCTRL.txt
new file mode 100644
index 0000000000..14de4da44f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Electrical_Utilities_Examples_TestVoltageCTRL.txt
@@ -0,0 +1,7 @@
+last-generated=2015-05-08
+statistics-simulation={'numerical Jacobians': '0', 'nonlinear': ' ', 'number of continuous time states': '1', 'linear': ' '}
+voltageControl.V_nominal=[120., 120.]
+Vtr_high.y=[132., 132.]
+sou.V_in=[120., 121.25581357993701203668, 122.50666805363560740716, 123.74762711097636724844, 124.97380058651565093442, 126.1803436279296875, 127.36248751371806520183, 128.51557935877434601935, 129.63507066905938813761, 130.71653772753364819437, 131.755706787109375, 132.74847388906323431002, 133.69094804693523315109, 134.57937662811832524312, 135.4102632510441139857, 136.1803436279296875, 136.88655074121183474745, 137.52613801368133295, 138.09654261010894060746, 138.59553538685952389642, 139.0211334228515625, 139.37165861594286297986, 139.64575183714612194308, 139.84230048637988375049, 139.96054068868389208546, 140., 139.96054068868389208546, 139.84230048637988375049, 139.64575183714612194308, 139.37165861594286297986, 139.0211334228515625, 138.59553483012089714066, 138.09654261011041853635, 137.52613801367959922572, 136.88655153909408568325, 136.1803436279296875, 135.41026229187190210723, 134.57937662812076951013, 133.69094804693261835382, 132.74847503968427986365, 131.755706787109375, 130.71653645971576906959, 129.63506869322534953426, 128.51558138590397106782, 127.36248890444508674591, 126.1803436279296875, 124.97379949655331188296, 123.74762490110654766795, 122.50667046678654514835, 121.25581479418292474293, 120., 118.74418520581707525707, 117.49332953321345485165, 116.25237509889345233205, 115.02620050344668811704, 113.8196563720703125, 112.63751109555489904324, 111.48441098470151189304, 110.36493130677465046574, 109.28346354028424514127, 108.244293212890625, 107.25151733095758288528, 106.30905740614814192213, 105.42062543101359040065, 104.58973770816446346998, 103.8196563720703125, 103.1134408315113688559, 102.47386818220438442495, 101.90345867573439875287, 101.40447279923725432127, 100.9788665771484375, 100.62833375469899976906, 100.3542552419672091446, 100.15770752969577017666, 100.03946694067425937646, 100., 100.03946694067425937646, 100.15770752969577017666, 100.3542552419672091446, 100.62833375469899976906, 100.9788665771484375, 101.40447061448840315734, 101.90345867570974291993, 102.47386818223159821173, 103.11344406110468696625, 103.8196563720703125, 104.58973390621787302734, 105.42062543097419791138, 106.30905740618956656363, 107.25152196220240341518, 108.244293212890625, 109.28345849333476280663, 110.36493130672440088347, 111.48441098475306887394, 112.63751667494902619637, 113.8196563720703125, 115.02619470555931968647, 116.25237509883724840165, 117.4933295332701135294, 118.74419118738256884171, 120.]
+time=[0., 10.]
+voltageControl.y=[1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 0.0005271651905829765, 0.00000207342437772649, -0.00000018538743579552, 0.00000003026889962182, -0.00000002865619208592, 0.00000001020258143561, 0.00000000419408057236, -0.00000000054440306095, -0.00000000193695547326, -0.00000000127042665277, 0.00000000016834330877, 0.0000000010925076667, 0.00000000021946796741, 0.00000000002757091178, -0.00000000005858833557, -0.00000000006971035691, -0.00000000003649653492, 0.0000000000103521348, 0.00000000004013434625, 0.00000000002214907945, 0.0000000000038522843, 0.00000000000066830073, -0.00000000000131187454, -0.00000000000229454806, -0.00000000000248604132, -0.00000000000209266808, -0.00000000000132074742, -0.00000000000037659232, 0.00000000000053347653, 0.00000000000120314696, 0.00000000000142609934, 0.00000000000099601663, 0.00000000000002831139, -0.00000000000057438969, -0.00000000000145708142, -0.00000000000268032155, -0.00000000000430466744, -0.00000000000639066575, -0.00000000000899889355, -0.00000000001218989926, 0.99942326809355364059, 1.00000298020495392848, 1.00000011920587894565, 0.99999994039620787589, 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1., 1.]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_SimpleHouse.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_SimpleHouse.txt
new file mode 100644
index 0000000000..c7c87ba983
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_SimpleHouse.txt
@@ -0,0 +1,19 @@
+last-generated=2022-12-19
+statistics-initialization=
+{
+  "nonlinear": "5",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0",
+  "nonlinear": "1",
+  "number of continuous time states": "10",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.1536e+07]
+zon.T=[2.931499938964844e+02, 2.938165893554688e+02, 2.948394775390625e+02, 2.951160888671875e+02, 2.933800964355469e+02, 2.949007263183594e+02, 2.937331848144531e+02, 2.949746704101562e+02, 2.94963623046875e+02, 2.944449768066406e+02, 2.949704284667969e+02, 2.932081604003906e+02, 2.945489196777344e+02, 2.949959106445312e+02, 2.950682983398438e+02, 2.951320190429688e+02, 2.94079345703125e+02, 2.940500793457031e+02, 2.93251708984375e+02, 2.933990783691406e+02, 2.932026672363281e+02, 2.936112365722656e+02, 2.94181396484375e+02, 2.951331481933594e+02, 2.93716552734375e+02, 2.932184143066406e+02, 2.950964050292969e+02, 2.934932556152344e+02, 2.940997009277344e+02, 2.96098876953125e+02, 2.970375061035156e+02, 2.962566223144531e+02, 2.963293762207031e+02, 2.957511291503906e+02, 2.968561096191406e+02, 2.973106079101562e+02, 2.972330017089844e+02, 2.974053955078125e+02, 2.972986145019531e+02, 2.974791564941406e+02, 2.975252075195312e+02, 2.975371398925781e+02, 2.97523681640625e+02, 2.975829772949219e+02, 2.975098876953125e+02, 2.974816284179688e+02, 2.975858459472656e+02, 2.975862426757812e+02, 2.97521728515625e+02, 2.975988159179688e+02, 2.974871520996094e+02, 2.975801086425781e+02, 2.97568115234375e+02, 2.975059204101562e+02, 2.975872802734375e+02, 2.97644775390625e+02, 2.975877075195312e+02, 2.975962524414062e+02, 2.976087341308594e+02, 2.975819396972656e+02, 2.975243835449219e+02, 2.975371398925781e+02, 2.974706420898438e+02, 2.975225830078125e+02, 2.975242614746094e+02, 2.97474609375e+02, 2.974830017089844e+02, 2.974789428710938e+02, 2.974937438964844e+02, 2.974887390136719e+02, 2.974450988769531e+02, 2.974119873046875e+02, 2.970668029785156e+02, 2.966719360351562e+02, 2.971568603515625e+02, 2.972576599121094e+02, 2.966737670898438e+02, 2.959289245605469e+02, 2.957213745117188e+02, 2.9481201171875e+02, 2.944169616699219e+02, 2.947103271484375e+02, 2.939195556640625e+02, 2.940602722167969e+02, 2.940169677734375e+02, 2.937295227050781e+02, 2.931671142578125e+02, 2.933880310058594e+02, 2.950133056640625e+02, 2.940987243652344e+02, 2.951145935058594e+02, 2.951122131347656e+02, 2.931902465820312e+02, 2.951495361328125e+02, 2.950298767089844e+02, 2.942200012207031e+02, 2.936318054199219e+02, 2.943542785644531e+02, 2.931622009277344e+02, 2.951441650390625e+02, 2.932530822753906e+02]
+heaWat.u=[1e+00, 0e+00, 1e+00, 1e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 0e+00, 1e+00, 1e+00, 0e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 1e+00, 0e+00]
+vavDam.y=[2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.554025948047638e-01, 2.5e-01, 3.29160213470459e-01, 3.752192556858063e-01, 3.871423006057739e-01, 3.736800849437714e-01, 4.329911172389984e-01, 3.599009811878204e-01, 3.316185176372528e-01, 4.358335733413696e-01, 4.362431168556213e-01, 3.717152774333954e-01, 4.48826789855957e-01, 3.371655642986298e-01, 4.301155805587769e-01, 4.181102514266968e-01, 3.559122383594513e-01, 4.37283456325531e-01, 4.947710633277893e-01, 4.377006590366364e-01, 4.462576806545258e-01, 4.58719402551651e-01, 4.31939035654068e-01, 3.743763864040375e-01, 3.871388733386993e-01, 3.206299543380737e-01, 3.725927770137787e-01, 3.742593824863434e-01, 3.246186673641205e-01, 3.33006888628006e-01, 3.289314806461334e-01, 3.437333405017853e-01, 3.387492895126343e-01, 2.950859367847443e-01, 2.619776129722595e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01, 2.5e-01]
+fan.sta_a.T=[2.883200073242188e+02, 2.90562744140625e+02, 2.883319396972656e+02, 2.920919799804688e+02, 2.906665649414062e+02, 2.918930969238281e+02, 2.898759155273438e+02, 2.901109619140625e+02, 2.89111572265625e+02, 2.908656616210938e+02, 2.898673706054688e+02, 2.899195861816406e+02, 2.912050170898438e+02, 2.915523681640625e+02, 2.904037475585938e+02, 2.919996948242188e+02, 2.906729431152344e+02, 2.909330749511719e+02, 2.910764465332031e+02, 2.914588623046875e+02, 2.901047668457031e+02, 2.916375122070312e+02, 2.910815734863281e+02, 2.919293212890625e+02, 2.92504638671875e+02, 2.907031555175781e+02, 2.918236694335938e+02, 2.916273803710938e+02, 2.919345703125e+02, 2.964934997558594e+02, 2.946243896484375e+02, 2.942006225585938e+02, 2.941107788085938e+02, 2.946829528808594e+02, 2.956533813476562e+02, 2.953515014648438e+02, 2.958345642089844e+02, 2.946706848144531e+02, 2.963741760253906e+02, 2.969334106445312e+02, 2.952789306640625e+02, 2.982248229980469e+02, 2.966036376953125e+02, 2.979476318359375e+02, 2.962223205566406e+02, 2.965768737792969e+02, 2.962604675292969e+02, 2.985108032226562e+02, 2.948568725585938e+02, 2.9739111328125e+02, 2.97256591796875e+02, 2.973014831542969e+02, 2.968691101074219e+02, 2.978995361328125e+02, 2.976356811523438e+02, 2.979755554199219e+02, 2.981031188964844e+02, 2.967643127441406e+02, 2.979931640625e+02, 2.976788024902344e+02, 2.957882080078125e+02, 2.974443054199219e+02, 2.967668151855469e+02, 2.963309020996094e+02, 2.979713745117188e+02, 2.966609191894531e+02, 2.968990478515625e+02, 2.969129638671875e+02, 2.965253295898438e+02, 2.967495727539062e+02, 2.962158203125e+02, 2.966826782226562e+02, 2.9535986328125e+02, 2.960602416992188e+02, 2.956841430664062e+02, 2.958915100097656e+02, 2.955003356933594e+02, 2.934600830078125e+02, 2.941224365234375e+02, 2.925818786621094e+02, 2.921419067382812e+02, 2.928599243164062e+02, 2.915148315429688e+02, 2.920691223144531e+02, 2.939436645507812e+02, 2.926375732421875e+02, 2.904195556640625e+02, 2.91980224609375e+02, 2.920718688964844e+02, 2.905301208496094e+02, 2.907398986816406e+02, 2.901202697753906e+02, 2.900093688964844e+02, 2.924759521484375e+02, 2.906303100585938e+02, 2.909695129394531e+02, 2.895492553710938e+02, 2.903458862304688e+02, 2.896872253417969e+02, 2.911193237304688e+02, 2.893901062011719e+02]
+fan.sta_b.T=[2.886552734375e+02, 2.908980102539062e+02, 2.886672058105469e+02, 2.924272155761719e+02, 2.910018310546875e+02, 2.922283630371094e+02, 2.90211181640625e+02, 2.904462280273438e+02, 2.894468383789062e+02, 2.91200927734375e+02, 2.9020263671875e+02, 2.902548522949219e+02, 2.91540283203125e+02, 2.918876342773438e+02, 2.90739013671875e+02, 2.923349609375e+02, 2.910082092285156e+02, 2.91268310546875e+02, 2.914117126464844e+02, 2.917941284179688e+02, 2.904400329589844e+02, 2.919727783203125e+02, 2.914168395996094e+02, 2.922645874023438e+02, 2.928399047851562e+02, 2.910384216308594e+02, 2.92158935546875e+02, 2.91962646484375e+02, 2.922698364257812e+02, 2.968287353515625e+02, 2.949596252441406e+02, 2.94535888671875e+02, 2.944460144042969e+02, 2.950182189941406e+02, 2.959886474609375e+02, 2.95686767578125e+02, 2.961697998046875e+02, 2.950059509277344e+02, 2.967094421386719e+02, 2.972686767578125e+02, 2.956141967773438e+02, 2.9856005859375e+02, 2.969389038085938e+02, 2.982828979492188e+02, 2.965575866699219e+02, 2.969121398925781e+02, 2.965957336425781e+02, 2.988460693359375e+02, 2.95192138671875e+02, 2.977263793945312e+02, 2.975918579101562e+02, 2.976367492675781e+02, 2.972043762207031e+02, 2.982347717285156e+02, 2.97970947265625e+02, 2.983108215332031e+02, 2.984383850097656e+02, 2.970995788574219e+02, 2.983284301757812e+02, 2.980140686035156e+02, 2.961234741210938e+02, 2.977795715332031e+02, 2.971020812988281e+02, 2.966661682128906e+02, 2.98306640625e+02, 2.969961853027344e+02, 2.972343139648438e+02, 2.972482299804688e+02, 2.968605651855469e+02, 2.970848388671875e+02, 2.965510864257812e+02, 2.970179443359375e+02, 2.956951293945312e+02, 2.963955078125e+02, 2.960194091796875e+02, 2.962267761230469e+02, 2.958355712890625e+02, 2.937953491210938e+02, 2.944577026367188e+02, 2.929171447753906e+02, 2.924771728515625e+02, 2.931951904296875e+02, 2.918500671386719e+02, 2.924043884277344e+02, 2.942789306640625e+02, 2.929728393554688e+02, 2.907548217773438e+02, 2.923154907226562e+02, 2.924071350097656e+02, 2.908653869628906e+02, 2.910751647949219e+02, 2.904555358886719e+02, 2.903446350097656e+02, 2.928112182617188e+02, 2.90965576171875e+02, 2.913047790527344e+02, 2.89884521484375e+02, 2.906811218261719e+02, 2.900224914550781e+02, 2.9145458984375e+02, 2.897253723144531e+02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse0.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse0.txt
new file mode 100644
index 0000000000..edb3888914
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse0.txt
@@ -0,0 +1,9 @@
+last-generated=2023-09-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+06]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse1.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse1.txt
new file mode 100644
index 0000000000..f7f50b5866
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse1.txt
@@ -0,0 +1,10 @@
+last-generated=2023-09-08
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "number of continuous time states": "1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+06]
+walCap.T=[2.931499938964844e+02, 2.930488891601562e+02, 2.929534912109375e+02, 2.928625793457031e+02, 2.927890625e+02, 2.927221069335938e+02, 2.926539916992188e+02, 2.925841979980469e+02, 2.925122985839844e+02, 2.924403991699219e+02, 2.923712768554688e+02, 2.923157653808594e+02, 2.9226025390625e+02, 2.922047119140625e+02, 2.921505126953125e+02, 2.920964660644531e+02, 2.920424194335938e+02, 2.919769897460938e+02, 2.919044799804688e+02, 2.918319702148438e+02, 2.917594604492188e+02, 2.916893310546875e+02, 2.916217041015625e+02, 2.915540466308594e+02, 2.914863586425781e+02, 2.914178771972656e+02, 2.91349365234375e+02, 2.912808837890625e+02, 2.912074890136719e+02, 2.911309814453125e+02, 2.91054443359375e+02, 2.909779357910156e+02, 2.909013977050781e+02, 2.908248596191406e+02, 2.907483520507812e+02, 2.906789855957031e+02, 2.906123962402344e+02, 2.905458068847656e+02, 2.904791870117188e+02, 2.9041259765625e+02, 2.903459777832031e+02, 2.902665405273438e+02, 2.901768493652344e+02, 2.90087158203125e+02, 2.899946594238281e+02, 2.898983154296875e+02, 2.89802001953125e+02, 2.89703369140625e+02, 2.895991516113281e+02, 2.894949340820312e+02, 2.893912353515625e+02, 2.892901611328125e+02, 2.891891174316406e+02, 2.890880432128906e+02, 2.889869689941406e+02, 2.888859252929688e+02, 2.887772521972656e+02, 2.8866162109375e+02, 2.885459899902344e+02, 2.884303283691406e+02, 2.88314697265625e+02, 2.881990661621094e+02, 2.880933837890625e+02, 2.87989013671875e+02, 2.878941650390625e+02, 2.878175659179688e+02, 2.877409362792969e+02, 2.876662292480469e+02, 2.875919799804688e+02, 2.875189208984375e+02, 2.874469909667969e+02, 2.873750305175781e+02, 2.87322509765625e+02, 2.872810363769531e+02, 2.872395629882812e+02, 2.8719775390625e+02, 2.871559143066406e+02, 2.8711181640625e+02, 2.87065673828125e+02, 2.8701953125e+02, 2.86973388671875e+02, 2.8692724609375e+02, 2.868709716796875e+02, 2.8681298828125e+02, 2.867549743652344e+02, 2.866969604492188e+02, 2.86641357421875e+02, 2.865965576171875e+02, 2.865517272949219e+02, 2.865069274902344e+02, 2.864621276855469e+02, 2.864214782714844e+02, 2.863848266601562e+02, 2.863481750488281e+02, 2.863114929199219e+02, 2.862760925292969e+02, 2.862434387207031e+02, 2.862107849121094e+02, 2.861781311035156e+02, 2.861456604003906e+02, 2.861146240234375e+02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse2.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse2.txt
new file mode 100644
index 0000000000..8f376300c9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse2.txt
@@ -0,0 +1,10 @@
+last-generated=2023-09-08
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "number of continuous time states": "1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+06]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse3.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse3.txt
new file mode 100644
index 0000000000..067c1f0e8d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse3.txt
@@ -0,0 +1,10 @@
+last-generated=2023-09-08
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "number of continuous time states": "4",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+06]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse4.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse4.txt
new file mode 100644
index 0000000000..142a5fe719
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse4.txt
@@ -0,0 +1,16 @@
+last-generated=2023-09-22
+statistics-initialization=
+{
+  "nonlinear": "5, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0",
+  "nonlinear": "1",
+  "number of continuous time states": "9",
+  "numerical Jacobians": "0"
+}
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+heaWat.u=[1e+00, 1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse5.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse5.txt
new file mode 100644
index 0000000000..f5c54c97ce
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse5.txt
@@ -0,0 +1,16 @@
+last-generated=2023-09-22
+statistics-initialization=
+{
+  "nonlinear": "5, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0",
+  "nonlinear": "1, 1",
+  "number of continuous time states": "9",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse6.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse6.txt
new file mode 100644
index 0000000000..6461262282
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Examples_Tutorial_SimpleHouse_SimpleHouse6.txt
@@ -0,0 +1,19 @@
+last-generated=2024-06-05
+statistics-initialization=
+{
+  "nonlinear": "5, 1, 1, 1",
+  "numerical Jacobians": "0"
+}
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+{
+  "linear": "0, 0, 0, 0, 0",
+  "nonlinear": "1, 0, 1, 1, 1",
+  "number of continuous time states": "11",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_BoilerCHP_Examples_CHPSystem.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_BoilerCHP_Examples_CHPSystem.txt
new file mode 100644
index 0000000000..ef2923d060
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_BoilerCHP_Examples_CHPSystem.txt
@@ -0,0 +1,15 @@
+last-generated=2024-07-19
+statistics-initialization=
+{
+  "linear": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 1",
+  "number of continuous time states": "6",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_CarnotWithLosses.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_CarnotWithLosses.txt
new file mode 100644
index 0000000000..48ba580932
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_CarnotWithLosses.txt
@@ -0,0 +1,18 @@
+last-generated=2024-07-16
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "2, 2",
+  "number of continuous time states": "4",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_LargeScaleWaterToWater.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_LargeScaleWaterToWater.txt
new file mode 100644
index 0000000000..cf74cadfae
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_LargeScaleWaterToWater.txt
@@ -0,0 +1,18 @@
+last-generated=2023-11-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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+chi.refCyc.sigBus.yMea=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 9.599999785423279e-01, 9.200000166893005e-01, 8.799999952316284e-01, 8.399999737739561e-01, 8.000000119209287e-01, 7.599999904632566e-01, 7.200000286102295e-01, 6.800000071525574e-01, 6.399999856948853e-01, 6.000000238418579e-01, 5.600000023841858e-01, 5.199999809265137e-01, 4.799999892711639e-01, 4.399999976158142e-01, 4.000000059604645e-01, 3.600000143051147e-01, 3.199999928474426e-01, 2.800000011920929e-01, 2.39999994635582e-01, 2.000000029802322e-01, 1.599999964237213e-01, 1.19999997317791e-01, 7.999999821186066e-02, 3.999999910593033e-02, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_Modular.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_Modular.txt
new file mode 100644
index 0000000000..fa16a5849d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Examples_Modular.txt
@@ -0,0 +1,18 @@
+last-generated=2024-07-16
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "2",
+  "number of continuous time states": "5",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_Carnot_y.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_Carnot_y.txt
new file mode 100644
index 0000000000..9b147dcaeb
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_Carnot_y.txt
@@ -0,0 +1,20 @@
+last-generated=2023-11-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_ConstantCarnotEffectiveness.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_ConstantCarnotEffectiveness.txt
new file mode 100644
index 0000000000..2f10d0063e
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_ConstantCarnotEffectiveness.txt
@@ -0,0 +1,20 @@
+last-generated=2023-11-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "2",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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+chi.P=[1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 1.4122759765625e+04, 5.649103515625e+03, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+chi.dp1=[6e+03, 6e+03]
+chi.dp2=[6e+03, 6e+03]
+chi.refCyc.refCycChiCoo.EER_nominal=[2.124230861663818e+00, 2.124230861663818e+00]
+chi.EER=[2.755671262741089e+00, 2.601786375045776e+00, 2.534570693969727e+00, 2.38344669342041e+00, 2.230450391769409e+00, 2.167744159698486e+00, 2.142425775527954e+00, 2.131905078887939e+00, 2.127480268478394e+00, 2.125609397888184e+00, 2.124817132949829e+00, 2.124480009078979e+00, 2.124336719512939e+00, 2.124275922775269e+00, 2.124249935150146e+00, 2.124239206314087e+00, 2.124234437942505e+00, 2.124232292175293e+00, 2.124231576919556e+00, 2.124231100082397e+00, 2.124230861663818e+00, 2.124230861663818e+00, 2.124230623245239e+00, 2.124230623245239e+00, 2.124230623245239e+00, 2.124230623245239e+00, 2.204912900924683e+00, 2.38360619544983e+00, 2.491180181503296e+00, 2.535692691802979e+00, 2.553391456604004e+00, 2.560320854187012e+00, 2.563015937805176e+00, 2.564061164855957e+00, 2.564467668533325e+00, 2.564625978469849e+00, 2.564687490463257e+00, 2.564711570739746e+00, 2.564720392227173e+00, 2.564723968505859e+00, 2.564725637435913e+00, 2.56472635269165e+00, 2.564726591110229e+00, 2.564726591110229e+00, 2.564726829528809e+00, 2.564726829528809e+00, 2.564727067947388e+00, 2.564727067947388e+00, 2.564727067947388e+00, 2.564726829528809e+00, 2.564726829528809e+00, 3.104876279830933e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_TableData2D.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_TableData2D.txt
new file mode 100644
index 0000000000..96577fb07a
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Chillers_ModularReversible_Validation_TableData2D.txt
@@ -0,0 +1,19 @@
+last-generated=2023-11-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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+chi.dp1=[6e+03, 6e+03]
+chi.dp2=[6e+03, 6e+03]
+chi.EER=[2.513644695281982e+00, 2.513644695281982e+00, 2.435760498046875e+00, 2.20210862159729e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.124224662780762e+00, 2.388512134552002e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 2.564703941345215e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Examples_GeothermalHeatPump.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Examples_GeothermalHeatPump.txt
index 0992023f63..6d5e6d8535 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Examples_GeothermalHeatPump.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Examples_GeothermalHeatPump.txt
@@ -1,19 +1,19 @@
-last-generated=2022-07-06
+last-generated=2024-07-19
 statistics-initialization=
 {
-  "nonlinear": "1, 0, 1, 0, 1, 0, 1, 0, 1, 0",
+  "nonlinear": "1, 0, 2, 0, 1, 0, 1, 0, 1, 0",
   "numerical Jacobians": "0"
 }
 statistics-simulation=
 {
-  "linear": "0, 0, 0, 0, 0, 8, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 8, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0",
-  "nonlinear": "2, 1, 1, 1, 1, 0, 0, 1, 1, 1, 1, 1, 1, 1, 1, 1",
+  "linear": "0, 0, 0, 0, 0, 0, 8, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 8, 0, 0, 0, 0, 0, 0,   0, 0, 0",
+  "nonlinear": "1, 1, 1, 1, 1, 1, 1, 0, 0, 1, 1, 1, 1, 1, 1, 1",
   "number of continuous time states": "113",
   "numerical Jacobians": "0"
 }
 time=[0e+00, 8.64e+04]
-heatPumpPower=[1.4345e+03, 3.896387451171875e+03, 3.948070556640625e+03, 3.981284423828125e+03, 4.0029033203125e+03, 4.017043212890625e+03, 4.026296875e+03, 4.01835791015625e+03, 4.062794677734375e+03, 6.257839965820312e+02, 8.745105590820312e+02, 3.966314697265625e+03, 3.988554443359375e+03, 3.992769287109375e+03, 4.050381591796875e+03, 4.044908935546875e+03, 8.746222534179688e+02, 6.600349731445311e+02, 3.916833740234375e+03, 3.947125732421875e+03, 4.019474853515625e+03, 4.024126220703125e+03, 4.016660400390625e+03, 4.055726318359375e+03, 6.267014770507812e+02, 8.745106201171875e+02, 3.961543212890625e+03, 3.98491748046875e+03, 3.990190673828125e+03, 4.047609130859375e+03, 4.04412744140625e+03, 9.539927978515625e+02, 6.602987060546875e+02, 3.87441162109375e+03, 3.94232958984375e+03, 4.016078857421874e+03, 4.022084716796875e+03, 4.015318359375e+03, 4.052810302734375e+03, 6.270133056640625e+02, 8.745106201171875e+02, 3.957061279296875e+03, 3.982141357421875e+03, 3.988316650390625e+03, 4.045515625e+03, 4.04343359375e+03, 1.4332451171875e+03, 6.643651123046875e+02, 3.8370849609375e+03, 3.938772705078125e+03, 4.01360693359375e+03, 4.020560791015625e+03, 4.014320068359375e+03, 4.051552734375e+03, 6.27177001953125e+02, 8.745106811523438e+02, 3.953599609375e+03, 3.980117919921875e+03, 3.9869697265625e+03, 4.04405224609375e+03, 4.042918212890625e+03, 2.80371337890625e+03, 6.677594604492188e+02, 3.78389306640625e+03, 3.936125e+03, 4.0120146484375e+03, 4.019367431640625e+03, 4.01354150390625e+03, 4.053092529296875e+03, 6.271268310546877e+02, 8.74510681152344e+02, 3.951143310546875e+03, 3.9786376953125e+03, 3.9860146484375e+03, 4.043724609375e+03, 4.04250146484375e+03, 4.02937939453125e+03, 6.646435546875e+02, 3.436643310546875e+03, 3.934267822265625e+03, 4.01107080078125e+03, 4.01845556640625e+03, 4.012952880859375e+03, 4.056391845703125e+03, 6.268676147460938e+02, 8.745106201171875e+02, 3.949607666015625e+03, 3.97762451171875e+03, 3.98540087890625e+03, 4.044221435546875e+03, 4.04216455078125e+03, 4.02912158203125e+03, 6.599116821289062e+02, 2.955962890625e+03, 3.933100830078125e+03, 4.0103681640625e+03, 4.0177841796875e+03, 4.01255126953125e+03, 4.0600634765625e+03, 6.264298095703125e+02, 8.745106201171875e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Examples_SimpleHouse.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Examples_SimpleHouse.txt
deleted file mode 100644
index b258794031..0000000000
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Examples_SimpleHouse.txt
+++ /dev/null
@@ -1,19 +0,0 @@
-last-generated=2022-07-06
-statistics-initialization=
-{
-  "nonlinear": "5",
-  "numerical Jacobians": "0"
-}
-statistics-simulation=
-{
-  "linear": "0, 0, 0, 0, 0",
-  "nonlinear": "1",
-  "number of continuous time states": "10",
-  "numerical Jacobians": "0"
-}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Examples_CoolingOffice.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Examples_CoolingOffice.txt
new file mode 100644
index 0000000000..82c2f157b6
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Examples_CoolingOffice.txt
@@ -0,0 +1,15 @@
+last-generated=2023-09-22
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+{
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Validation_NumberWells.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Validation_NumberWells.txt
new file mode 100644
index 0000000000..222c96cf1d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Validation_NumberWells.txt
@@ -0,0 +1,15 @@
+last-generated=2023-09-22
+statistics-initialization=
+{
+  "nonlinear": "1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
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+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Validation_SimulationTest.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Validation_SimulationTest.txt
new file mode 100644
index 0000000000..32b7832e9f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Aquifer_Validation_SimulationTest.txt
@@ -0,0 +1,15 @@
+last-generated=2023-09-22
+statistics-initialization=
+{
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_ClusterBoreholes_100boreholes.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_ClusterBoreholes_100boreholes.txt
new file mode 100644
index 0000000000..6333f3e424
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_ClusterBoreholes_100boreholes.txt
@@ -0,0 +1,9 @@
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_Equivalent.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_Equivalent.txt
new file mode 100644
index 0000000000..e84530a5d7
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_Equivalent.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_Integrand_Equivalent.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_Integrand_Equivalent.txt
new file mode 100644
index 0000000000..d0016b5331
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_Integrand_Equivalent.txt
@@ -0,0 +1,11 @@
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_SteadyState.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_SteadyState.txt
new file mode 100644
index 0000000000..7577fd5e13
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Geothermal_Borefields_BaseClasses_HeatTransfer_ThermalResponseFactors_Validation_FiniteLineSource_SteadyState.txt
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_AntiFreeze.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_AntiFreeze.txt
new file mode 100644
index 0000000000..58a9a7c671
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_AntiFreeze.txt
@@ -0,0 +1,13 @@
+last-generated=2023-07-31
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+02]
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+antFre.TAntFre=[2.761499938964844e+02, 2.761499938964844e+02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_MinimalFlowRate.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_MinimalFlowRate.txt
new file mode 100644
index 0000000000..4f68f957ba
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_MinimalFlowRate.txt
@@ -0,0 +1,14 @@
+last-generated=2023-07-31
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+02]
+ySet=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
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+minFloRatSaf.mEvaMin_flow=[1.000000014901161e-01, 1.000000014901161e-01]
+minFloRatSaf.mConMin_flow=[1.000000014901161e-01, 1.000000014901161e-01]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_OnOff.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_OnOff.txt
new file mode 100644
index 0000000000..ede7f41ba4
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_OnOff.txt
@@ -0,0 +1,10 @@
+last-generated=2023-07-31
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 7.2e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_OperationalEnvelope.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_OperationalEnvelope.txt
new file mode 100644
index 0000000000..f47c5a13cc
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_OperationalEnvelope.txt
@@ -0,0 +1,13 @@
+last-generated=2024-04-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+02]
+ySet=[1e+00, 1e+00]
+yOut=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+sigBus.TConInMea=[2.831499938964844e+02, 2.951499938964844e+02, 3.071499938964844e+02, 3.191499938964844e+02, 3.311499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.311499938964844e+02, 3.191499938964844e+02, 3.071499938964843e+02, 2.951499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.951499938964844e+02, 3.071499938964844e+02, 3.191499938964844e+02, 3.311499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.431499938964844e+02, 3.311499938964844e+02, 3.191499938964844e+02, 3.071499938964844e+02, 2.951499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02]
+opeEnv.bouMapHea.tabBou.y[1]=[3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02, 3.331499938964844e+02]
+opeEnv.bouMapCoo.tab[2, 2]=[2.881499938964844e+02, 2.881499938964844e+02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_Safety.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_Safety.txt
new file mode 100644
index 0000000000..1f1214a3c7
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Controls_Safety_Examples_Safety.txt
@@ -0,0 +1,13 @@
+last-generated=2024-03-06
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+02]
+ySet=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+yOut=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+safCtr.minFlowErr=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00]
+safCtr.opeEnvErr=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 2e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 3e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00, 4e+00]
+safCtr.antFreErr=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_AirToWater2D_OneRoomRadiator.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_AirToWater2D_OneRoomRadiator.txt
new file mode 100644
index 0000000000..9cc49d2b88
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_AirToWater2D_OneRoomRadiator.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-15
+statistics-initialization=
+{
+  "nonlinear": "5, 1, 1, 1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0",
+  "nonlinear": "1",
+  "number of continuous time states": "15",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
+vol.T_start=[2.931499938964844e+02, 2.931499938964844e+02]
+vol.T=[2.931499938964844e+02, 2.926033935546875e+02, 2.872524108886719e+02, 2.843258056640625e+02, 2.830519104003906e+02, 2.83083740234375e+02, 2.840514526367188e+02, 2.855957641601562e+02, 2.874038391113281e+02, 2.892298278808594e+02, 2.9090380859375e+02, 2.923201904296875e+02, 2.934297485351562e+02, 2.942312316894531e+02, 2.947184753417969e+02, 2.949185485839844e+02, 2.948959045410156e+02, 2.947317504882812e+02, 2.945032958984375e+02, 2.942562561035156e+02, 2.940097961425781e+02, 2.937659301757812e+02, 2.935325927734375e+02, 2.933323974609375e+02, 2.931742248535156e+02, 2.930597534179688e+02, 2.92986328125e+02, 2.92948486328125e+02, 2.929392700195312e+02, 2.929511413574219e+02, 2.929819946289062e+02, 2.930473937988281e+02, 2.931455078125e+02, 2.932619934082031e+02, 2.95337158203125e+02, 2.918630981445312e+02, 2.889076843261719e+02, 2.879935302734375e+02, 2.879578552246094e+02, 2.885302124023438e+02, 2.894996032714844e+02, 2.906563720703125e+02, 2.918136291503906e+02, 2.92850341796875e+02, 2.9371337890625e+02, 2.943753967285156e+02, 2.948340454101562e+02, 2.951057739257812e+02, 2.936395874023438e+02, 2.905567321777344e+02, 2.89898681640625e+02, 2.969423217773438e+02, 2.982201232910156e+02, 2.971582946777344e+02, 2.957851867675781e+02, 2.961087036132812e+02, 2.961149597167969e+02, 2.96105224609375e+02, 2.966309509277344e+02, 2.9614892578125e+02, 2.967032775878906e+02, 2.893049011230469e+02, 2.892781677246094e+02, 2.906144409179688e+02, 2.919315795898438e+02, 2.930139770507812e+02, 2.938160705566406e+02, 2.94340576171875e+02, 2.946160583496094e+02, 2.946858520507812e+02, 2.945997924804688e+02, 2.944077758789062e+02, 2.941411437988281e+02, 2.938178405761719e+02, 2.934757690429688e+02, 2.931576538085938e+02, 2.902052612304688e+02, 2.891943359375e+02, 2.888721008300781e+02, 2.890093078613281e+02, 2.894812927246094e+02, 2.902332458496094e+02, 2.911415405273438e+02, 2.920470275878906e+02, 2.927953491210938e+02, 2.933131103515625e+02, 2.936116027832031e+02, 2.937445068359375e+02, 2.937903747558594e+02, 2.938132629394531e+02, 2.938274841308594e+02, 2.938176879882812e+02, 2.937514038085938e+02, 2.936143188476562e+02, 2.934307861328125e+02, 2.932322998046875e+02, 2.930537719726562e+02, 2.929295654296875e+02, 2.92872314453125e+02, 2.928668518066406e+02, 2.928837280273438e+02]
+temSup.T=[3.231499938964844e+02, 3.077752380371094e+02, 3.03253662109375e+02, 3.008519897460938e+02, 3.00715576171875e+02, 3.0222998046875e+02, 3.047685546875e+02, 3.077805786132812e+02, 3.108355102539062e+02, 3.13632080078125e+02, 3.159883117675781e+02, 3.17819580078125e+02, 3.191369934082031e+02, 3.199720458984375e+02, 3.203635559082031e+02, 3.203818054199219e+02, 3.201213684082031e+02, 3.19685791015625e+02, 3.191717224121094e+02, 3.186518859863281e+02, 3.181692504882812e+02, 3.177525024414062e+02, 3.174043884277344e+02, 3.171282043457031e+02, 3.169266357421875e+02, 3.16795654296875e+02, 3.167262878417969e+02, 3.16706787109375e+02, 3.16724365234375e+02, 3.167667541503906e+02, 3.168233642578125e+02, 3.168904418945312e+02, 3.169649963378906e+02, 3.170367126464844e+02, 3.10512451171875e+02, 3.020683898925782e+02, 3.016178283691406e+02, 3.013190612792969e+02, 3.019627380371094e+02, 3.032536926269531e+02, 3.048780517578125e+02, 3.065636291503906e+02, 3.080995178222656e+02, 3.093460998535156e+02, 3.102420349121094e+02, 3.107803039550781e+02, 3.109878234863281e+02, 3.10912353515625e+02, 3.027415466308594e+02, 3.003910217285156e+02, 3.009700317382812e+02, 2.99920654296875e+02, 2.962229614257812e+02, 2.918811340332031e+02, 2.923125305175781e+02, 2.937986145019531e+02, 2.903401184082031e+02, 2.932470092773438e+02, 2.914586486816406e+02, 2.927693176269531e+02, 2.918222351074219e+02, 2.963103637695312e+02, 3.000172424316406e+02, 3.025484313964844e+02, 3.045316162109375e+02, 3.059948120117188e+02, 3.069560241699219e+02, 3.074682922363281e+02, 3.076089477539062e+02, 3.07466552734375e+02, 3.071301574707031e+02, 3.066816101074219e+02, 3.061895446777344e+02, 3.057030029296875e+02, 3.052622985839844e+02, 3.049023742675781e+02, 3.041956176757812e+02, 3.037523498535156e+02, 3.040432434082031e+02, 3.048883361816406e+02, 3.060660400390625e+02, 3.073977661132812e+02, 3.087383117675781e+02, 3.099522399902344e+02, 3.109291381835938e+02, 3.116071472167969e+02, 3.119927673339844e+02, 3.121397399902344e+02, 3.121233520507812e+02, 3.120174560546875e+02, 3.118695983886719e+02, 3.116984252929688e+02, 3.115054626464844e+02, 3.112892150878906e+02, 3.110640258789062e+02, 3.108548278808594e+02, 3.106866455078125e+02, 3.105792236328125e+02, 3.105411987304688e+02, 3.105635375976562e+02, 3.106248779296875e+02]
+temRet.T=[3.231499938964844e+02, 3.073618774414062e+02, 3.001544189453125e+02, 2.967893676757812e+02, 2.956328735351562e+02, 2.961915893554688e+02, 2.979190979003906e+02, 3.003036804199219e+02, 3.029212036132812e+02, 3.054551391601562e+02, 3.076964721679688e+02, 3.095286560058594e+02, 3.109138488769531e+02, 3.118744812011719e+02, 3.124266052246094e+02, 3.126145935058594e+02, 3.125148620605469e+02, 3.122208557128906e+02, 3.118260192871094e+02, 3.114025573730469e+02, 3.109935913085938e+02, 3.106215515136719e+02, 3.102966613769531e+02, 3.100271301269531e+02, 3.098198852539062e+02, 3.096750183105469e+02, 3.095870971679688e+02, 3.0954736328125e+02, 3.095453186035156e+02, 3.095702209472656e+02, 3.096130065917969e+02, 3.096741333007812e+02, 3.097535705566406e+02, 3.098418579101562e+02, 3.103954467773437e+02, 3.018144226074219e+02, 2.985887756347656e+02, 2.977553405761719e+02, 2.979024963378906e+02, 2.987799072265625e+02, 3.001029052734375e+02, 3.016069030761719e+02, 3.030709228515625e+02, 3.043371276855469e+02, 3.053252563476562e+02, 3.060082702636719e+02, 3.063941040039062e+02, 3.065142822265625e+02, 3.025225830078125e+02, 2.975263671875e+02, 2.9791748046875e+02, 2.998484802246094e+02, 2.99001220703125e+02, 2.942681884765625e+02, 2.923887023925781e+02, 2.93837890625e+02, 2.926290893554688e+02, 2.932986755371094e+02, 2.938765258789062e+02, 2.928361206054688e+02, 2.943052368164062e+02, 2.93109375e+02, 2.963419494628906e+02, 2.986748962402344e+02, 3.005951538085938e+02, 3.020895080566406e+02, 3.031460571289062e+02, 3.0379150390625e+02, 3.040811767578125e+02, 3.040862426757812e+02, 3.038832702636719e+02, 3.035462036132812e+02, 3.031378173828125e+02, 3.027017211914062e+02, 3.022779541015625e+02, 3.019055480957031e+02, 3.007247619628906e+02, 2.99856201171875e+02, 2.997262268066406e+02, 3.001844482421875e+02, 3.010359497070312e+02, 3.021274719238281e+02, 3.03322509765625e+02, 3.044764709472656e+02, 3.054555053710938e+02, 3.061719665527344e+02, 3.066129150390625e+02, 3.0681982421875e+02, 3.068640441894531e+02, 3.0682080078125e+02, 3.067372131347656e+02, 3.066286010742188e+02, 3.064892883300781e+02, 3.0631005859375e+02, 3.061023559570312e+02, 3.058912963867188e+02, 3.0570556640625e+02, 3.055716857910156e+02, 3.055052185058594e+02, 3.055011596679688e+02, 3.055386352539062e+02]
+heaPum.refCyc.sigBus.hea=[1e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00]
+heaPum.refCyc.sigBus.onOffMea=[1e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 1e+00, 1e+00, 0e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 0e+00, 1e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_CarnotWithLosses_OneRoomRadiator.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_CarnotWithLosses_OneRoomRadiator.txt
new file mode 100644
index 0000000000..14b6894cf5
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_CarnotWithLosses_OneRoomRadiator.txt
@@ -0,0 +1,20 @@
+last-generated=2024-05-16
+statistics-initialization=
+{
+  "nonlinear": "5, 1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0",
+  "nonlinear": "1, 2, 2",
+  "number of continuous time states": "18",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
+vol.T_start=[2.931499938964844e+02, 2.931499938964844e+02]
+vol.T=[2.931499938964844e+02, 2.917251892089844e+02, 2.886861877441406e+02, 2.866962585449219e+02, 2.860060424804688e+02, 2.8624169921875e+02, 2.869993591308594e+02, 2.879870910644531e+02, 2.890218505859375e+02, 2.899991149902344e+02, 2.908689270019531e+02, 2.916096801757812e+02, 2.922152404785156e+02, 2.926876220703125e+02, 2.930194091796875e+02, 2.932230834960938e+02, 2.93335205078125e+02, 2.9340087890625e+02, 2.934582214355469e+02, 2.935157775878906e+02, 2.935619812011719e+02, 2.935757446289062e+02, 2.93549560546875e+02, 2.935038146972656e+02, 2.934499206542969e+02, 2.933947448730469e+02, 2.933426513671875e+02, 2.93296142578125e+02, 2.932564697265625e+02, 2.932239074707031e+02, 2.932032470703125e+02, 2.932161254882812e+02, 2.932645874023438e+02, 2.933365783691406e+02, 2.95460693359375e+02, 2.925295104980469e+02, 2.896095886230469e+02, 2.89629638671875e+02, 2.902962646484375e+02, 2.911327514648438e+02, 2.919900207519531e+02, 2.92771484375e+02, 2.934074096679688e+02, 2.938790893554688e+02, 2.942116088867188e+02, 2.9442724609375e+02, 2.945483093261719e+02, 2.945964050292969e+02, 2.945913391113281e+02, 2.945502624511719e+02, 2.945060119628906e+02, 3.001047058105469e+02, 2.982427368164062e+02, 2.940140991210938e+02, 2.943144836425781e+02, 2.951688537597656e+02, 2.960208129882812e+02, 2.967854614257812e+02, 2.974311828613281e+02, 2.979300537109375e+02, 2.967666625976562e+02, 2.856502990722656e+02, 2.835823974609375e+02, 2.883830871582031e+02, 2.929782409667969e+02, 2.956009826660156e+02, 2.936690673828125e+02, 2.910787963867188e+02, 2.912563781738281e+02, 2.928034362792969e+02, 2.939569396972656e+02, 2.946380920410156e+02, 2.950357666015625e+02, 2.945670471191406e+02, 2.919860534667969e+02, 2.906861877441406e+02, 2.892413330078125e+02, 2.897418518066406e+02, 2.904535522460938e+02, 2.911250610351562e+02, 2.917194519042969e+02, 2.922969055175781e+02, 2.928437805175781e+02, 2.932951049804688e+02, 2.935728149414062e+02, 2.936619567871094e+02, 2.936131286621094e+02, 2.934982604980469e+02, 2.93396240234375e+02, 2.933577270507812e+02, 2.933752746582031e+02, 2.934109497070312e+02, 2.934136352539062e+02, 2.933562622070312e+02, 2.932557678222656e+02, 2.931380004882812e+02, 2.9303271484375e+02, 2.929696350097656e+02, 2.92957275390625e+02, 2.929777526855469e+02, 2.930016784667969e+02]
+temSup.T=[3.231499938964844e+02, 3.12006103515625e+02, 3.078103637695312e+02, 3.061668090820312e+02, 3.063213500976562e+02, 3.074601135253906e+02, 3.090391540527344e+02, 3.107222595214844e+02, 3.123187561035156e+02, 3.137315979003906e+02, 3.149217529296875e+02, 3.158841552734375e+02, 3.1663134765625e+02, 3.171847839355469e+02, 3.175671691894531e+02, 3.178028259277344e+02, 3.179252624511719e+02, 3.179720153808594e+02, 3.179771118164062e+02, 3.179610290527344e+02, 3.17928955078125e+02, 3.178775634765625e+02, 3.178033447265625e+02, 3.177141418457031e+02, 3.176211242675781e+02, 3.175321655273438e+02, 3.174520568847656e+02, 3.173831481933594e+02, 3.173262023925781e+02, 3.172808227539062e+02, 3.172464294433594e+02, 3.172268676757812e+02, 3.172238159179688e+02, 3.172308349609375e+02, 3.139916687011718e+02, 3.047022705078126e+02, 3.043235473632812e+02, 3.055128784179688e+02, 3.066809997558594e+02, 3.078085632324219e+02, 3.088002319335938e+02, 3.095927429199219e+02, 3.101542663574219e+02, 3.104814758300781e+02, 3.106004943847656e+02, 3.105482788085938e+02, 3.103622131347656e+02, 3.100768127441406e+02, 3.097225646972656e+02, 3.093250122070312e+02, 3.090281066894531e+02, 3.04449951171875e+02, 2.851360168457031e+02, 2.884064025878906e+02, 2.905628662109375e+02, 2.920706787109375e+02, 2.933028869628906e+02, 2.943565063476562e+02, 2.952657470703125e+02, 2.960379638671875e+02, 2.835398559570312e+02, 2.837323608398438e+02, 2.929266662597656e+02, 3.037991943359375e+02, 3.09487060546875e+02, 3.083078308105469e+02, 3.022742614746094e+02, 2.984705810546875e+02, 3.039081420898438e+02, 3.063138732910156e+02, 3.076370849609375e+02, 3.083343505859375e+02, 3.088277893066406e+02, 3.045819702148438e+02, 2.996817016601562e+02, 3.0260546875e+02, 3.0505322265625e+02, 3.065571594238281e+02, 3.078487243652344e+02, 3.089518127441406e+02, 3.098542175292969e+02, 3.10576171875e+02, 3.111401672363281e+02, 3.115458068847656e+02, 3.117832946777344e+02, 3.1185791015625e+02, 3.118078308105469e+02, 3.11688232421875e+02, 3.115538024902344e+02, 3.114443054199219e+02, 3.113700561523438e+02, 3.113177490234375e+02, 3.112651062011719e+02, 3.111953735351562e+02, 3.111118774414062e+02, 3.110299987792969e+02, 3.109668579101562e+02, 3.109361572265625e+02, 3.109426879882812e+02, 3.109779968261719e+02, 3.110260009765625e+02]
+temRet.T=[3.231499938964844e+02, 3.099340209960938e+02, 3.055309448242188e+02, 3.033744201660156e+02, 3.031017761230469e+02, 3.039298400878906e+02, 3.052975158691406e+02, 3.068433837890625e+02, 3.083556213378906e+02, 3.097214660644531e+02, 3.108910827636719e+02, 3.118515625e+02, 3.12609375e+02, 3.131811218261719e+02, 3.135843200683594e+02, 3.13839111328125e+02, 3.139778442382812e+02, 3.140392150878906e+02, 3.140596618652344e+02, 3.140607299804688e+02, 3.140469665527344e+02, 3.140127258300781e+02, 3.139521484375e+02, 3.138734130859375e+02, 3.137881164550781e+02, 3.137046203613281e+02, 3.136281127929688e+02, 3.135614013671875e+02, 3.13505615234375e+02, 3.134606628417969e+02, 3.134265441894531e+02, 3.134095153808594e+02, 3.134131164550781e+02, 3.134311828613281e+02, 3.135132446289062e+02, 3.044541015625001e+02, 3.019859924316406e+02, 3.029919128417969e+02, 3.040614624023438e+02, 3.051487731933594e+02, 3.061451416015625e+02, 3.069747924804688e+02, 3.075936889648438e+02, 3.079889831542969e+02, 3.0818212890625e+02, 3.082066955566406e+02, 3.080974426269531e+02, 3.0788720703125e+02, 3.076052551269531e+02, 3.072766418457031e+02, 3.069886474609375e+02, 3.043913879394531e+02, 2.905680541992188e+02, 2.885044250488281e+02, 2.906229858398438e+02, 2.9211962890625e+02, 2.933461608886719e+02, 2.943958129882812e+02, 2.95301513671875e+02, 2.960699768066406e+02, 2.885525817871094e+02, 2.837503051757812e+02, 2.884703063964844e+02, 3.000557250976562e+02, 3.062027893066406e+02, 3.08029296875e+02, 3.021154174804688e+02, 2.979242553710938e+02, 3.015198669433594e+02, 3.040516662597656e+02, 3.055120239257812e+02, 3.062846984863281e+02, 3.067979125976562e+02, 3.043900146484375e+02, 2.995418701171875e+02, 3.002327270507812e+02, 3.024449462890625e+02, 3.038230590820312e+02, 3.050406188964844e+02, 3.061009521484375e+02, 3.069825744628906e+02, 3.077070617675781e+02, 3.082954406738281e+02, 3.087396850585938e+02, 3.090178833007812e+02, 3.09125e+02, 3.09095458984375e+02, 3.089856262207031e+02, 3.088555603027344e+02, 3.08751708984375e+02, 3.086875610351562e+02, 3.086488647460938e+02, 3.086089172363281e+02, 3.085459289550781e+02, 3.084616088867188e+02, 3.083719482421875e+02, 3.082964172363281e+02, 3.082525634765625e+02, 3.0824853515625e+02, 3.082766723632812e+02, 3.083194885253906e+02]
+heaPum.refCyc.sigBus.hea=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00]
+heaPum.refCyc.sigBus.onOffMea=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 0e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_LargeScaleWaterToWater_OneRoomRadiator.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_LargeScaleWaterToWater_OneRoomRadiator.txt
new file mode 100644
index 0000000000..7e4b3acbb6
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_LargeScaleWaterToWater_OneRoomRadiator.txt
@@ -0,0 +1,19 @@
+last-generated=2024-07-15
+statistics-initialization=
+{
+  "nonlinear": "5, 1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0",
+  "nonlinear": "1",
+  "number of continuous time states": "14",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
+vol.T_start=[2.931499938964844e+02, 2.931499938964844e+02]
+vol.T=[2.931499938964844e+02, 2.93133544921875e+02, 2.893275146484375e+02, 2.865391235351562e+02, 2.85306884765625e+02, 2.853642883300781e+02, 2.862884521484375e+02, 2.876766967773438e+02, 2.892074890136719e+02, 2.906585083007812e+02, 2.919026794433594e+02, 2.92882080078125e+02, 2.935859375e+02, 2.940323181152344e+02, 2.942413024902344e+02, 2.942566528320312e+02, 2.941459045410156e+02, 2.939813842773438e+02, 2.9382275390625e+02, 2.936928405761719e+02, 2.9358740234375e+02, 2.934868469238281e+02, 2.933814086914062e+02, 2.932872314453125e+02, 2.932109375e+02, 2.93154296875e+02, 2.931163940429688e+02, 2.930946960449219e+02, 2.930859680175781e+02, 2.930867004394531e+02, 2.930986633300781e+02, 2.931412048339844e+02, 2.932147216796875e+02, 2.933056945800781e+02, 2.952909851074219e+02, 2.91727783203125e+02, 2.889950561523438e+02, 2.887469482421875e+02, 2.892843627929688e+02, 2.902214660644531e+02, 2.913283081054688e+02, 2.924151000976562e+02, 2.933390502929688e+02, 2.940355224609375e+02, 2.945091247558594e+02, 2.94781982421875e+02, 2.948889770507812e+02, 2.948707885742188e+02, 2.947679443359375e+02, 2.946170349121094e+02, 2.944482421875e+02, 2.995169677734375e+02, 2.997100524902344e+02, 2.988101806640625e+02, 2.977340393066406e+02, 2.968164978027344e+02, 2.9615869140625e+02, 2.957342224121094e+02, 2.954729919433594e+02, 2.959471130371094e+02, 2.967270202636719e+02, 2.894002990722656e+02, 2.881305541992188e+02, 2.905759887695312e+02, 2.929897766113281e+02, 2.947109680175781e+02, 2.943995056152344e+02, 2.916976928710938e+02, 2.907207641601562e+02, 2.916838684082031e+02, 2.926928405761719e+02, 2.934634704589844e+02, 2.939512939453125e+02, 2.941632995605469e+02, 2.9421484375e+02, 2.942047119140625e+02, 2.913815612792969e+02, 2.904150085449219e+02, 2.90102783203125e+02, 2.902085571289062e+02, 2.906024780273438e+02, 2.91230712890625e+02, 2.919742736816406e+02, 2.92682373046875e+02, 2.932145690917969e+02, 2.935168151855469e+02, 2.936214294433594e+02, 2.935989074707031e+02, 2.935372924804688e+02, 2.935013427734375e+02, 2.934981994628906e+02, 2.935015258789062e+02, 2.934678649902344e+02, 2.933747863769531e+02, 2.932420959472656e+02, 2.930984191894531e+02, 2.929757995605469e+02, 2.929054870605469e+02, 2.928961486816406e+02, 2.92928466796875e+02, 2.929700927734375e+02]
+temSup.T=[3.231499938964844e+02, 3.132603454589844e+02, 3.07589599609375e+02, 3.049389343261719e+02, 3.0469482421875e+02, 3.060532836914062e+02, 3.082928466796875e+02, 3.108318176269531e+02, 3.132659301757812e+02, 3.153562622070312e+02, 3.169946594238281e+02, 3.181632995605469e+02, 3.188988647460938e+02, 3.192674560546875e+02, 3.193446960449219e+02, 3.192078857421875e+02, 3.189385070800781e+02, 3.186126098632812e+02, 3.182906494140625e+02, 3.180069885253906e+02, 3.177703857421875e+02, 3.175743713378906e+02, 3.174088134765625e+02, 3.1727392578125e+02, 3.171723937988281e+02, 3.171031494140625e+02, 3.170623168945312e+02, 3.170444030761719e+02, 3.170434875488281e+02, 3.170539245605469e+02, 3.170711364746094e+02, 3.170960998535156e+02, 3.171278991699219e+02, 3.171575622558594e+02, 3.121260681152343e+02, 3.025603637695313e+02, 3.029165649414062e+02, 3.0366650390625e+02, 3.049569091796875e+02, 3.065069580078125e+02, 3.080377197265625e+02, 3.093494873046875e+02, 3.103242492675781e+02, 3.1091845703125e+02, 3.111548767089844e+02, 3.110906677246094e+02, 3.107955627441406e+02, 3.103405151367188e+02, 3.097904968261719e+02, 3.092001647949219e+02, 3.086117248535156e+02, 3.030996704101562e+02, 2.994584655761719e+02, 2.964105834960938e+02, 2.941552734375e+02, 2.925123596191406e+02, 2.913623962402344e+02, 2.906131591796875e+02, 2.901717529296875e+02, 2.929496154785156e+02, 2.929772644042969e+02, 2.932011413574219e+02, 2.991383666992188e+02, 3.042302856445312e+02, 3.075304260253906e+02, 3.094901123046875e+02, 3.034314270019531e+02, 2.985845336914062e+02, 3.018729553222656e+02, 3.039779357910156e+02, 3.054502258300781e+02, 3.064117736816406e+02, 3.069237976074219e+02, 3.071089477539062e+02, 3.072250061035156e+02, 3.072765808105469e+02, 3.065417175292969e+02, 3.060611572265625e+02, 3.062565002441406e+02, 3.069412231445312e+02, 3.078926086425781e+02, 3.08939208984375e+02, 3.099480590820312e+02, 3.108040771484375e+02, 3.114244995117188e+02, 3.117790832519531e+02, 3.119013977050781e+02, 3.118616027832031e+02, 3.117386474609375e+02, 3.115975341796875e+02, 3.114691772460938e+02, 3.113538818359375e+02, 3.112379455566406e+02, 3.111100463867188e+02, 3.109785766601562e+02, 3.108635864257812e+02, 3.107852478027344e+02, 3.107577819824219e+02, 3.107837219238281e+02, 3.108494262695312e+02, 3.109322204589844e+02]
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+heaPum.refCyc.sigBus.onOffMea=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 1e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_Modular_OneRoomRadiator.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_Modular_OneRoomRadiator.txt
new file mode 100644
index 0000000000..790ae52b44
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Examples_Modular_OneRoomRadiator.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-15
+statistics-initialization=
+{
+  "nonlinear": "5, 1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0",
+  "nonlinear": "1",
+  "number of continuous time states": "16",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
+vol.T_start=[2.931499938964844e+02, 2.931499938964844e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_Carnot_y.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_Carnot_y.txt
new file mode 100644
index 0000000000..c63fd87bfa
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_Carnot_y.txt
@@ -0,0 +1,20 @@
+last-generated=2023-11-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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+heaPum.dp2=[6e+03, 6e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_ConstantCarnotEffectiveness.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_ConstantCarnotEffectiveness.txt
new file mode 100644
index 0000000000..ad504e5c54
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_ConstantCarnotEffectiveness.txt
@@ -0,0 +1,20 @@
+last-generated=2023-11-16
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "2",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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+heaPum.P=[1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 1.23750595703125e+04, 4.95002392578125e+03, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+heaPum.dp1=[6e+03, 6e+03]
+heaPum.dp2=[6e+03, 6e+03]
+heaPum.refCyc.refCycHeaPumHea.COP_nominal=[2.424230813980103e+00, 2.424230813980103e+00]
+heaPum.COP=[3.022756576538086e+00, 2.841303110122681e+00, 2.772667646408081e+00, 2.637427091598511e+00, 2.504878282546997e+00, 2.454448699951172e+00, 2.435764312744141e+00, 2.428664922714233e+00, 2.425941228866577e+00, 2.424896478652954e+00, 2.424487590789795e+00, 2.424330711364746e+00, 2.424269199371338e+00, 2.424245595932007e+00, 2.424236059188843e+00, 2.424232721328735e+00, 2.42423152923584e+00, 2.424231052398682e+00, 2.424230813980103e+00, 2.424230813980103e+00, 2.424230575561523e+00, 2.424230575561523e+00, 2.424230575561523e+00, 2.424230813980103e+00, 2.424230813980103e+00, 2.424230813980103e+00, 2.499832391738892e+00, 2.659942865371705e+00, 2.747552394866943e+00, 2.77983832359314e+00, 2.791336297988892e+00, 2.795384168624878e+00, 2.796802520751953e+00, 2.797298669815063e+00, 2.797469854354858e+00, 2.797532320022583e+00, 2.797554731369019e+00, 2.797562837600708e+00, 2.797565698623657e+00, 2.797566413879395e+00, 2.797566890716553e+00, 2.797567129135132e+00, 2.797567129135132e+00, 2.797566890716553e+00, 2.797566652297974e+00, 2.797566652297974e+00, 2.797566652297974e+00, 2.797567129135132e+00, 2.797567367553711e+00, 2.797567367553711e+00, 2.797567367553711e+00, 3.30132269859314e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_TableData2D.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_TableData2D.txt
new file mode 100644
index 0000000000..bfcecfedac
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_Comparative_TableData2D.txt
@@ -0,0 +1,19 @@
+last-generated=2023-11-15
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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+heaPum.dp1=[6e+03, 6e+03]
+heaPum.dp2=[6e+03, 6e+03]
+heaPum.COP=[2.754312992095947e+00, 2.754312992095947e+00, 2.688295125961304e+00, 2.490240812301636e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.424222946166992e+00, 2.648221015930176e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 2.797553062438965e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_ConstantCarnotEffectiveness.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_ConstantCarnotEffectiveness.txt
new file mode 100644
index 0000000000..3321be56cf
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_ConstantCarnotEffectiveness.txt
@@ -0,0 +1,15 @@
+last-generated=2023-11-17
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "2",
+  "number of continuous time states": "6",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1.4365e+04]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_TableData2D.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_TableData2D.txt
new file mode 100644
index 0000000000..80ac91bddc
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_HeatPumps_ModularReversible_Validation_TableData2D.txt
@@ -0,0 +1,15 @@
+last-generated=2023-06-22
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "6",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1.4365e+04]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_MixingVolumes_Validation_MSLCombustionAir.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_MixingVolumes_Validation_MSLCombustionAir.txt
new file mode 100644
index 0000000000..f9e235b238
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_MixingVolumes_Validation_MSLCombustionAir.txt
@@ -0,0 +1,10 @@
+last-generated=2022-10-24
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 1, 0",
+  "number of continuous time states": "4",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_MixingVolumes_Validation_MSLFlueGasSixComponents.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_MixingVolumes_Validation_MSLFlueGasSixComponents.txt
new file mode 100644
index 0000000000..70386fe3d9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_MixingVolumes_Validation_MSLFlueGasSixComponents.txt
@@ -0,0 +1,10 @@
+last-generated=2022-10-24
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 1, 0",
+  "number of continuous time states": "8",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerComparison.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerComparison.txt
new file mode 100644
index 0000000000..b5039b1074
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerComparison.txt
@@ -0,0 +1,14 @@
+last-generated=2022-12-22
+statistics-simulation=
+{
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+  "numerical Jacobians": "0"
+}
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+eff1.r_N=[1e+00, 1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerCurve.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerCurve.txt
new file mode 100644
index 0000000000..06ad95459b
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerCurve.txt
@@ -0,0 +1,11 @@
+last-generated=2024-07-18
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+01]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerReducedSpeed.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerReducedSpeed.txt
new file mode 100644
index 0000000000..430171914d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_EulerReducedSpeed.txt
@@ -0,0 +1,14 @@
+last-generated=2022-12-22
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_HydraulicEfficiencyMethods.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_HydraulicEfficiencyMethods.txt
new file mode 100644
index 0000000000..e6001f1d05
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_HydraulicEfficiencyMethods.txt
@@ -0,0 +1,20 @@
+last-generated=2022-12-14
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
+eff1.eta=[4.900000095367432e-01, 4.900000095367432e-01]
+eff1.etaHyd=[6.99999988079071e-01, 6.99999988079071e-01]
+eff1.etaMot=[6.99999988079071e-01, 6.99999988079071e-01]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_MotorEfficiencyMethods.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_MotorEfficiencyMethods.txt
new file mode 100644
index 0000000000..5f6dc81aca
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_MotorEfficiencyMethods.txt
@@ -0,0 +1,20 @@
+last-generated=2022-10-19
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_NegativePressureOrFlow.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_NegativePressureOrFlow.txt
new file mode 100644
index 0000000000..c89b308d3b
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_NegativePressureOrFlow.txt
@@ -0,0 +1,16 @@
+last-generated=2022-10-19
+statistics-initialization=
+{
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_TotalEfficiencyMethods.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_TotalEfficiencyMethods.txt
new file mode 100644
index 0000000000..61e75faae7
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_BaseClasses_Validation_TotalEfficiencyMethods.txt
@@ -0,0 +1,20 @@
+last-generated=2022-12-14
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
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+eff4.etaMot=[6.99999988079071e-01, 6.99999988079071e-01]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpConst.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpConst.txt
new file mode 100644
index 0000000000..0b31c0eae6
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpConst.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-25
+statistics-initialization=
+{
+  "nonlinear": "1, 0, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 1",
+  "number of continuous time states": "5",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
+dpControlled_dp.mov.dpMachine=[0e+00, 9.999103125e+04, 9.9999984375e+04, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 1e+05, 9.98264296875e+04, 9.80484453125e+04, 9.63080234375e+04, 9.463771875e+04, 9.30351953125e+04, 9.14981171875e+04, 9.0024140625e+04, 8.86109375e+04, 8.7256203125e+04, 8.595767187499999e+04, 8.471310156249999e+04, 8.352031249999999e+04, 8.2377171875e+04, 8.128159375e+04, 8.02315703125e+04, 7.92251484375e+04, 7.82604375e+04, 7.73356015625e+04, 7.6448890625e+04, 7.55986171875e+04, 7.45276953125e+04, 7.3137421875e+04, 7.18191484375e+04, 7.05687734375e+04, 6.93820546875e+04, 6.82550390625e+04, 6.71840546875e+04, 6.61656796875e+04, 6.519675390625e+04, 6.42743203125e+04, 6.339560546875e+04, 6.278280859375e+04, 6.26391484375e+04, 6.2616984375e+04, 6.26140546875e+04, 6.26136875e+04, 6.261365625e+04, 6.26136484375e+04, 6.26136484375e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04]
+dpControlled_dp.mov.m_flow=[0e+00, 2.812247430483694e-06, 2.81249913314241e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 2.812499587889761e-06, 1.184053532779217e-02, 6.628159433603303e-02, 1.212379187345507e-01, 1.771624833345413e-01, 2.330515831708908e-01, 2.887530028820038e-01, 3.442236185073853e-01, 3.994203507900238e-01, 4.542765021324158e-01, 5.086791515350342e-01, 5.624399185180664e-01, 6.153948903083801e-01, 6.676467657089233e-01, 7.191846370697021e-01, 7.699679136276245e-01, 8.199595808982849e-01, 8.691262006759644e-01, 9.174379706382751e-01, 9.648687839508057e-01, 1.010517954826355e+00, 1.046635866165161e+00, 1.081138849258423e+00, 1.114249706268311e+00, 1.146014809608459e+00, 1.176481127738953e+00, 1.205695509910583e+00, 1.233704209327698e+00, 1.260553479194641e+00, 1.286288380622864e+00, 1.310953378677368e+00, 1.33459210395813e+00, 1.357246994972229e+00, 1.378959178924561e+00, 1.399768829345703e+00, 1.41971480846405e+00, 1.438834547996521e+00, 1.457164287567139e+00, 1.474738955497742e+00, 1.491592168807983e+00, 1.505178570747375e+00, 1.514347910881042e+00, 1.523036360740662e+00, 1.531278491020203e+00, 1.53910219669342e+00, 1.546533465385437e+00, 1.553596138954163e+00, 1.560312509536743e+00, 1.56670355796814e+00, 1.572788834571838e+00, 1.578586101531982e+00, 1.581841588020325e+00, 1.582470417022705e+00, 1.58256196975708e+00, 1.582574129104614e+00, 1.582575440406799e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00]
+m_flow_nominal=[1e+00, 1e+00]
+dp_nominal=[1e+05, 1e+05]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpControlled_dpConst.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpControlled_dpConst.txt
deleted file mode 100644
index 2f4d93f9ba..0000000000
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpControlled_dpConst.txt
+++ /dev/null
@@ -1,20 +0,0 @@
-last-generated=2022-05-23
-statistics-initialization=
-{
-  "nonlinear": "1, 0, 1",
-  "numerical Jacobians": "0"
-}
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-{
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-  "numerical Jacobians": "0"
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-time=[0e+00, 3.6e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpControlled_dpVar.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpControlled_dpVar.txt
deleted file mode 100644
index 65c313d5b9..0000000000
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpControlled_dpVar.txt
+++ /dev/null
@@ -1,20 +0,0 @@
-last-generated=2022-05-23
-statistics-initialization=
-{
-  "nonlinear": "1, 0, 1",
-  "numerical Jacobians": "0"
-}
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-{
-  "linear": " ",
-  "nonlinear": "1, 1",
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-  "numerical Jacobians": "0"
-}
-time=[0e+00, 3.6e+03]
-dpControlled_dp.mov.dpMachine=[0e+00, 4.999550390625e+04, 5.00000390625e+04, 5.000006640625e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.013146875e+04, 5.195680078125001e+04, 5.399589843750001e+04, 5.615390625e+04, 5.839734765625e+04, 6.07192734375e+04, 6.3119484375e+04, 6.5598421875e+04, 6.81555703125e+04, 7.07892265625e+04, 7.3494921875e+04, 7.6263296875e+04, 7.9077640625e+04, 8.19307890625e+04, 8.4831078125e+04, 8.77740390625e+04, 9.0755203125e+04, 9.37696796875e+04, 9.681259375e+04, 9.96583828125e+04, 9.80484375e+04, 9.6308015625e+04, 9.463771875e+04, 9.30351953125e+04, 9.14981171875e+04, 9.0024140625e+04, 8.86109375e+04, 8.7256203125e+04, 8.595767187499999e+04, 8.471310156249999e+04, 8.352031249999999e+04, 8.2377171875e+04, 8.128159375e+04, 8.02315703125e+04, 7.92251484375e+04, 7.82604296875e+04, 7.73356015625e+04, 7.6448890625e+04, 7.55986171875e+04, 7.4527625e+04, 7.31374140625e+04, 7.18191328125e+04, 7.05687734375e+04, 6.9382046875e+04, 6.825503125e+04, 6.71840390625e+04, 6.6165671875e+04, 6.519674609375e+04, 6.42743046875e+04, 6.3395609375e+04, 6.278280078125e+04, 6.263912890625e+04, 6.2617e+04, 6.261405859375e+04, 6.2613703125e+04, 6.261365625e+04, 6.26136484375e+04, 6.26136484375e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04]
-dpControlled_dp.mov.m_flow=[0e+00, 1.406123260494496e-06, 1.40625081712642e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 6.017619278281927e-03, 4.774345457553876e-02, 8.89835506677629e-02, 1.325507164001465e-01, 1.777599304914474e-01, 2.245334684848785e-01, 2.728754580020905e-01, 3.227908909320831e-01, 3.74267041683197e-01, 4.272601902484894e-01, 4.816660284996033e-01, 5.37266731262207e-01, 5.937086343765259e-01, 6.50974452495575e-01, 7.091696262359619e-01, 7.682020664215088e-01, 8.279775977134705e-01, 8.883987665176392e-01, 9.493671059608459e-01, 1.009667038917542e+00, 1.046635746955872e+00, 1.081138849258423e+00, 1.114249706268311e+00, 1.146014809608459e+00, 1.176481127738953e+00, 1.205695509910583e+00, 1.233704209327698e+00, 1.260553479194641e+00, 1.286288380622864e+00, 1.310953378677368e+00, 1.33459210395813e+00, 1.357246994972229e+00, 1.378959178924561e+00, 1.399768829345703e+00, 1.41971480846405e+00, 1.438834547996521e+00, 1.457164287567139e+00, 1.474738955497742e+00, 1.491592049598694e+00, 1.505177736282349e+00, 1.514347910881042e+00, 1.523036122322083e+00, 1.531278491020203e+00, 1.53910219669342e+00, 1.546533346176147e+00, 1.553595900535583e+00, 1.560312390327454e+00, 1.56670355796814e+00, 1.572788715362549e+00, 1.578586101531982e+00, 1.581841707229614e+00, 1.582470297813416e+00, 1.58256208896637e+00, 1.582574009895325e+00, 1.582575440406799e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00]
-m_flow_nominal=[1e+00, 1e+00]
-dp_nominal=[1e+05, 1e+05]
-val.y_actual=[0e+00, -9.110714831768838e-27, 2.054392167979787e-27, 7.147010467824369e-28, 3.010373910788051e-28, 9.089485955993214e-29, 6.776033027111639e-29, 4.462579797303508e-29, 2.14912656749538e-29, 1.082622623480205e-29, 1.262591673754939e-29, 1.442560648798035e-29, 1.622529774304408e-29, 1.802498749347504e-29, 1.982467874853877e-29, 2.162436849896973e-29, 2.122785262534131e-29, 1.840601016348052e-29, 1.558416770161972e-29, 1.276232523975892e-29, 9.940482025581742e-30, 7.118639563720945e-30, 4.296796725701956e-30, 1.474953981722515e-30, -1.346888762256926e-30, -4.168731412196819e-30, 6.45081140100956e-03, 2.337789162993437e-02, 4.290840402245528e-02, 6.284619867801666e-02, 8.28385204076767e-02, 1.028376296162605e-01, 1.228375285863876e-01, 1.428375244140625e-01, 1.628374755382538e-01, 1.82837501168251e-01, 2.028374820947647e-01, 2.228374928236008e-01, 2.428374886512756e-01, 2.628374993801117e-01, 2.828374803066254e-01, 3.028374910354614e-01, 3.228374719619751e-01, 3.428374826908112e-01, 3.628374934196472e-01, 3.828374743461609e-01, 4.028374850749969e-01, 4.22837495803833e-01, 4.428374767303467e-01, 4.628374874591827e-01, 4.828374981880188e-01, 5.028374791145325e-01, 5.228374600410461e-01, 5.428375005722046e-01, 5.628374814987184e-01, 5.82837462425232e-01, 6.028375029563905e-01, 6.228374838829041e-01, 6.428374648094177e-01, 6.628375053405762e-01, 6.828374862670898e-01, 7.028374671936035e-01, 7.22837507724762e-01, 7.428374886512756e-01, 7.628374695777893e-01, 7.828375101089478e-01, 8.028374910354614e-01, 8.228374719619751e-01, 8.428375124931335e-01, 8.628374934196472e-01, 8.828374743461609e-01, 9.028375148773193e-01, 9.22837495803833e-01, 9.428374767303467e-01, 9.628374576568604e-01, 9.828374981880188e-01, 9.963869452476501e-01, 9.994602203369141e-01, 9.999291896820068e-01, 9.999912977218628e-01, 9.999988079071045e-01, 9.999998211860657e-01, 9.999999403953552e-01, 9.999999403953552e-01, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00]
-elEnergy=[0e+00, 4.353961907327175e-03, 9.542594663798809e-03, 1.473132707178593e-02, 1.992006041109562e-02, 2.510879375040531e-02, 3.0297527089715e-02, 3.548625856637955e-02, 4.067499190568924e-02, 4.586372524499893e-02, 5.105245858430862e-02, 5.624119192361832e-02, 6.142992526292801e-02, 6.66186586022377e-02, 7.180739194154741e-02, 7.699612528085709e-02, 8.218485862016678e-02, 8.737359195947647e-02, 9.256232529878616e-02, 9.775105863809586e-02, 1.029397919774055e-01, 1.081285253167152e-01, 1.133172586560249e-01, 1.185059919953346e-01, 1.236947253346443e-01, 1.288834512233734e-01, 4.330331802368164e+00, 1.039218139648444e+02, 3.706001892089856e+02, 8.20700927734375e+02, 1.476484497070312e+03, 2.360545166015625e+03, 3.496956787109375e+03, 4.91147265625e+03, 6.6315380859375e+03, 8.6861826171875e+03, 1.11057431640625e+04, 1.3921201171875e+04, 1.716294140625e+04, 2.0860490234375e+04, 2.50454375e+04, 2.9750376953125e+04, 3.500816796875e+04, 4.08517734375e+04, 4.73140625e+04, 5.4426578125e+04, 6.19365390625e+04, 6.9565984375e+04, 7.72997421875e+04, 8.51255625e+04, 9.30323125e+04, 1.01009875e+05, 1.090491015625e+05, 1.17141734375e+05, 1.252803046875001e+05, 1.334580781250001e+05, 1.416689843750001e+05, 1.499075625e+05, 1.58168921875e+05, 1.664486875e+05, 1.7474290625e+05, 1.83048109375e+05, 1.913611875e+05, 1.9967934375e+05, 2.08000140625e+05, 2.16312921875e+05, 2.24538328125e+05, 2.32660671875e+05, 2.4068353125e+05, 2.4861053125e+05, 2.5644521875e+05, 2.64191e+05, 2.7185125e+05, 2.7942909375e+05, 2.8692765625e+05, 2.9434990625e+05, 3.0170246875e+05, 3.09022375e+05, 3.1633584375e+05, 3.2364840625e+05, 3.3096084375e+05, 3.3827328125e+05, 3.455856875e+05, 3.52898125e+05, 3.6021053125e+05, 3.6752296875e+05, 3.74835375e+05, 3.8214778125e+05, 3.8946021875e+05, 3.96772625e+05, 4.040850625e+05, 4.1139746875e+05, 4.1870990625e+05, 4.260223125e+05, 4.3333475e+05, 4.4064715625e+05, 4.479595625e+05, 4.55272e+05, 4.6258440625e+05, 4.6989684375e+05, 4.7720925e+05]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpVar.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpVar.txt
new file mode 100644
index 0000000000..bad54dc64c
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_DpControlledMovers_Examples_DpVar.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-25
+statistics-initialization=
+{
+  "nonlinear": "1, 0, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 1",
+  "number of continuous time states": "5",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
+dpControlled_dp.mov.dpMachine=[0e+00, 4.999569921875e+04, 5.000008984375e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.00000703125e+04, 5.013146875e+04, 5.195672656250001e+04, 5.399590625000001e+04, 5.615389453125e+04, 5.839734765625e+04, 6.071926171875e+04, 6.311950390625e+04, 6.559840625e+04, 6.8155578125e+04, 7.078921875e+04, 7.34949296875e+04, 7.62632890625e+04, 7.9077578125e+04, 8.19309296875e+04, 8.48310625e+04, 8.77740390625e+04, 9.07551953125e+04, 9.37696796875e+04, 9.681259375e+04, 9.96584375e+04, 9.80484609375e+04, 9.63080234375e+04, 9.463771875e+04, 9.30351953125e+04, 9.14981171875e+04, 9.0024140625e+04, 8.86109375e+04, 8.7256203125e+04, 8.595767187499999e+04, 8.471310156249999e+04, 8.352031249999999e+04, 8.2377171875e+04, 8.128159375e+04, 8.0231578125e+04, 7.92251484375e+04, 7.82604375e+04, 7.73356015625e+04, 7.6448890625e+04, 7.55986171875e+04, 7.4527609375e+04, 7.31374140625e+04, 7.1819109375e+04, 7.05687421875e+04, 6.9382046875e+04, 6.82550234375e+04, 6.718403125e+04, 6.61656640625e+04, 6.5196734375e+04, 6.4274296875e+04, 6.3395609375e+04, 6.278281640625e+04, 6.263915234375e+04, 6.261698828125e+04, 6.26140546875e+04, 6.26136875e+04, 6.261365625e+04, 6.26136484375e+04, 6.26136484375e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04, 6.261364453125e+04]
+dpControlled_dp.mov.m_flow=[0e+00, 1.406128831149545e-06, 1.40625229505531e-06, 1.406251840307959e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 1.406251726621122e-06, 6.017664447426796e-03, 4.774333536624921e-02, 8.89835283160211e-02, 1.325505375862122e-01, 1.777598708868027e-01, 2.245333939790726e-01, 2.728754281997681e-01, 3.227907717227936e-01, 3.742671012878418e-01, 4.27260160446167e-01, 4.816660583019257e-01, 5.37266731262207e-01, 5.937083959579468e-01, 6.509750485420227e-01, 7.091695070266724e-01, 7.682020664215088e-01, 8.279775977134705e-01, 8.883987665176392e-01, 9.493671059608459e-01, 1.009667277336121e+00, 1.046635866165161e+00, 1.081138849258423e+00, 1.114249706268311e+00, 1.146014809608459e+00, 1.176481127738953e+00, 1.205695509910583e+00, 1.233704209327698e+00, 1.260553479194641e+00, 1.286288380622864e+00, 1.310953378677368e+00, 1.33459210395813e+00, 1.357246994972229e+00, 1.378959178924561e+00, 1.399768829345703e+00, 1.41971480846405e+00, 1.438834547996521e+00, 1.457164287567139e+00, 1.474738955497742e+00, 1.491592049598694e+00, 1.505177736282349e+00, 1.514347910881042e+00, 1.523035883903503e+00, 1.531278133392334e+00, 1.539102077484131e+00, 1.546533226966858e+00, 1.553595781326294e+00, 1.560312271118164e+00, 1.566703319549561e+00, 1.572788596153259e+00, 1.578586101531982e+00, 1.581841707229614e+00, 1.582470417022705e+00, 1.58256208896637e+00, 1.582574129104614e+00, 1.582575559616089e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00, 1.582575678825378e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Examples_StaticReset.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Examples_StaticReset.txt
new file mode 100644
index 0000000000..5242279cde
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Examples_StaticReset.txt
@@ -0,0 +1,20 @@
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+{
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+  "numerical Jacobians": "0"
+}
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Preconfigured_Validation_ControlledFlowMachinePreconfigured.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Preconfigured_Validation_ControlledFlowMachinePreconfigured.txt
new file mode 100644
index 0000000000..860d1f9cca
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Preconfigured_Validation_ControlledFlowMachinePreconfigured.txt
@@ -0,0 +1,20 @@
+last-generated=2024-06-05
+statistics-initialization=
+{
+  "nonlinear": "1, 1, 0, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 1, 0, 1",
+  "number of continuous time states": "15",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerHydraulic.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerHydraulic.txt
new file mode 100644
index 0000000000..cd090ef000
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerHydraulic.txt
@@ -0,0 +1,27 @@
+last-generated=2024-05-15
+statistics-initialization=
+{
+  "nonlinear": "1, 1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 1, 1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 2e+02]
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+ramSpe.y=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.333333507180214e-02, 6.666667014360428e-02, 1.000000014901161e-01, 1.333333402872086e-01, 1.666666716337204e-01, 2.000000029802322e-01, 2.333333343267441e-01, 2.666666805744171e-01, 3.00000011920929e-01, 3.333333432674408e-01, 3.666666746139526e-01, 4.000000059604645e-01, 4.333333373069763e-01, 4.666666686534882e-01, 5e-01, 5.333333611488342e-01, 5.666666626930237e-01, 6.00000023841858e-01, 6.333333253860473e-01, 6.666666865348816e-01, 6.99999988079071e-01, 7.333333492279053e-01, 7.666666507720947e-01, 8.00000011920929e-01, 8.333333134651184e-01, 8.666666746139526e-01, 8.999999761581421e-01, 9.333333373069763e-01, 9.666666388511658e-01, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00]
+ramDam.y=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 9.666666388511658e-01, 9.333333373069763e-01, 8.999999761581421e-01, 8.666666746139526e-01, 8.333333134651184e-01, 8.00000011920929e-01, 7.666666507720947e-01, 7.333333492279053e-01, 6.99999988079071e-01, 6.666666865348816e-01, 6.333333253860474e-01, 6.000000238418579e-01, 5.666666626930237e-01, 5.333333611488342e-01, 5e-01, 4.666666686534882e-01, 4.333333373069763e-01, 4.000000059604645e-01, 3.666666746139526e-01, 3.333333432674408e-01, 3.00000011920929e-01, 2.666666805744171e-01, 2.333333343267441e-01, 2.000000029802322e-01, 1.666666716337204e-01, 1.333333402872086e-01, 1.000000014901161e-01, 6.666667014360428e-02, 3.333333507180214e-02, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+mov1.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.583001613616943e+00, 4.784634113311768e+00, 2.153220748901367e+01, 5.322282409667977e+01, 1.047782287597656e+02, 1.820938262939453e+02, 2.897984619140625e+02, 4.328740539550781e+02, 6.163928833007812e+02, 8.455368041992188e+02, 1.125414672851562e+03, 1.461099853515625e+03, 1.857665893554688e+03, 2.320186279296875e+03, 2.853734619140625e+03, 3.463384033203125e+03, 4.15420849609375e+03, 4.931280761718753e+03, 5.799675292968746e+03, 6.76446435546875e+03, 7.83072265625e+03, 9.0035224609375e+03, 1.02879384765625e+04, 1.16890439453125e+04, 1.32119111328125e+04, 1.4861615234375e+04, 1.6643228515625e+04, 1.856182421875e+04, 2.06224765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2562322265625e+04, 2.2222333984375e+04, 2.17934296875e+04, 2.1258087890625e+04, 2.059309375e+04, 1.97520625e+04, 1.880525e+04, 1.7863771484375e+04, 1.7009693359375e+04, 1.6212673828125e+04, 1.54711806640625e+04, 1.47925595703125e+04, 1.41923935546875e+04, 1.36617255859375e+04, 1.3185326171875e+04, 1.2753912109375e+04, 1.23623388671875e+04, 1.200891796875e+04, 1.169495703125e+04, 1.1423541015625e+04, 1.11971806640625e+04, 1.1015421875e+04, 1.0874197265625e+04, 1.07670966796875e+04, 1.0687154296875e+04, 1.05992001953125e+04, 2.43349658203125e+03, 2.56244140625e+02, 7.136455059051514e+00, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01]
+mov2.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.583001613616943e+00, 4.898924350738525e+00, 2.16268424987793e+01, 5.33353576660157e+01, 1.049069595336914e+02, 1.821174468994141e+02, 2.896756286621094e+02, 4.326127319335938e+02, 6.160057373046875e+02, 8.450044555664062e+02, 1.12470458984375e+03, 1.460176513671875e+03, 1.856490356445312e+03, 2.31871630859375e+03, 2.851924560546875e+03, 3.461185546875e+03, 4.1515693359375e+03, 4.928145507812503e+03, 5.795985351562496e+03, 6.76015869140625e+03, 7.8257353515625e+03, 8.9977861328125e+03, 1.0281380859375e+04, 1.168158984375e+04, 1.32034833984375e+04, 1.4852130859375e+04, 1.6632603515625e+04, 1.854997265625e+04, 2.06093046875e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2815673828125e+04, 2.2598779296875e+04, 2.2287890625e+04, 2.1879923828125e+04, 2.1359462890625e+04, 2.0709966796875e+04, 1.9886181640625e+04, 1.8975267578125e+04, 1.810778125e+04, 1.7311208984375e+04, 1.6531923828125e+04, 1.5739392578125e+04, 1.49410966796875e+04, 1.419896875e+04, 1.35336044921875e+04, 1.2942490234375e+04, 1.2417359375e+04, 1.1941337890625e+04, 1.15116962890625e+04, 1.11300244140625e+04, 1.080007421875e+04, 1.05248955078125e+04, 1.03039375e+04, 1.0132255859375e+04, 1.0002056640625e+04, 9.904873046875e+03, 9.7790146484375e+03, 2.43349658203125e+03, 2.56244140625e+02, 7.136455059051514e+00, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01, 1.394233703613281e-01]
+mov3.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 2.012787908315659e-01, 4.933322429656982e+00, 2.078840065002441e+01, 5.238673019409188e+01, 1.044012451171875e+02, 1.817397918701172e+02, 2.89380859375e+02, 4.32327880859375e+02, 6.156624755859375e+02, 8.445794067382812e+02, 1.124188842773438e+03, 1.459560791015625e+03, 1.855765625e+03, 2.317873291015625e+03, 2.8509541015625e+03, 3.460077880859375e+03, 4.15031494140625e+03, 4.926735839843753e+03, 5.794409667968746e+03, 6.75840771484375e+03, 7.82379931640625e+03, 8.9956552734375e+03, 1.0279044921875e+04, 1.16790390625e+04, 1.32007080078125e+04, 1.48491201171875e+04, 1.662934765625e+04, 1.85464609375e+04, 2.060552734375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.281162109375e+04, 2.247336328125e+04, 2.1970287109375e+04, 2.1264125e+04, 2.0324251953125e+04, 1.9124876953125e+04, 1.761944140625e+04, 1.5945466796875e+04, 1.42762890625e+04, 1.271678515625e+04, 1.1235283203125e+04, 9.8401826171875e+03, 8.549171875e+03, 7.3961025390625e+03, 6.367712890625e+03, 5.4374208984375e+03, 4.58920166015625e+03, 3.81456689453125e+03, 3.11152734375e+03, 2.483894287109375e+03, 1.938971557617188e+03, 1.482845947265625e+03, 1.1155009765625e+03, 8.294064331054688e+02, 6.120479125976562e+02, 4.495857238769531e+02, 2.241946105957031e+02, 5.13458137512207e+01, 5.406650066375732e+00, 1.505763828754425e-01, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03, 2.941777929663658e-03]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerInput.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerInput.txt
new file mode 100644
index 0000000000..a6dbfa4c77
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerInput.txt
@@ -0,0 +1,27 @@
+last-generated=2024-05-15
+statistics-initialization=
+{
+  "nonlinear": "1, 1, 1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 0, 1, 1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 2e+02]
+mov1.eta=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 2.662420831620693e-02, 4.886708855628967e-01, 4.575706720352173e-01, 4.664972424507141e-01, 4.722372889518738e-01, 4.730210602283478e-01, 4.732595980167389e-01, 4.733445346355438e-01, 4.733809530735016e-01, 4.734058976173401e-01, 4.734263122081757e-01, 4.734432995319366e-01, 4.734576940536499e-01, 4.734700322151184e-01, 4.734807312488556e-01, 4.734900891780853e-01, 4.734983444213867e-01, 4.735057055950165e-01, 4.735122621059418e-01, 4.735181629657745e-01, 4.735235273838043e-01, 4.735283851623535e-01, 4.735328257083893e-01, 4.73536878824234e-01, 4.735406339168549e-01, 4.735440909862518e-01, 4.735472798347473e-01, 4.735502600669861e-01, 4.735530316829681e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.730305075645447e-01, 4.720738530158997e-01, 4.706114828586578e-01, 4.685670733451843e-01, 4.658646285533905e-01, 4.624316990375519e-01, 4.582027494907379e-01, 4.531229436397552e-01, 4.471518993377686e-01, 4.401520192623138e-01, 4.319839179515839e-01, 4.22771155834198e-01, 4.126746654510498e-01, 4.018683433532715e-01, 3.905176222324371e-01, 3.787632882595062e-01, 3.667131364345551e-01, 3.543288707733154e-01, 3.415527045726776e-01, 3.284392654895782e-01, 3.150481879711151e-01, 3.014431297779083e-01, 2.876905202865601e-01, 2.739090621471405e-01, 2.603259384632111e-01, 2.469863593578339e-01, 2.338569611310959e-01, 2.209040075540543e-01, 2.081050276756287e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01, 1.954464465379715e-01]
+mov1.etaHyd=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.80345806479454e-02, 6.981012225151062e-01, 6.536723971366882e-01, 6.664246320724487e-01, 6.746246814727783e-01, 6.75744354724884e-01, 6.760851144790649e-01, 6.762064695358276e-01, 6.762585043907166e-01, 6.762941479682922e-01, 6.763232946395874e-01, 6.763476133346558e-01, 6.763681769371033e-01, 6.76385760307312e-01, 6.764010787010193e-01, 6.76414430141449e-01, 6.764262318611145e-01, 6.76436722278595e-01, 6.764460802078247e-01, 6.764545440673828e-01, 6.764621734619141e-01, 6.76469087600708e-01, 6.76475465297699e-01, 6.764812469482422e-01, 6.76486611366272e-01, 6.764915585517883e-01, 6.764960885047913e-01, 6.765003800392151e-01, 6.765043139457703e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.75757884979248e-01, 6.743912100791931e-01, 6.723021268844604e-01, 6.693814992904663e-01, 6.655209064483643e-01, 6.606167554855347e-01, 6.545753479003906e-01, 6.473184823989868e-01, 6.387884020805359e-01, 6.287885904312134e-01, 6.171198487281799e-01, 6.03958785533905e-01, 5.895352363586426e-01, 5.740976333618164e-01, 5.578823089599609e-01, 5.410903692245483e-01, 5.238759517669678e-01, 5.061841011047363e-01, 4.879324436187744e-01, 4.691989421844482e-01, 4.50068861246109e-01, 4.306330382823944e-01, 4.10986453294754e-01, 3.912986516952515e-01, 3.718942105770111e-01, 3.528376519680023e-01, 3.340813517570496e-01, 3.155771493911743e-01, 2.972928881645203e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01, 2.792091965675354e-01]
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+mov2.eta=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1.302249170839787e-02, 3.376121520996094e-01, 3.689912557601929e-01, 4.125420749187471e-01, 4.502602219581604e-01, 4.660475254058838e-01, 4.718737602233887e-01, 4.732204079627991e-01, 4.733809530735016e-01, 4.734058976173401e-01, 4.734263122081757e-01, 4.734432995319366e-01, 4.734576940536499e-01, 4.734700322151184e-01, 4.734807312488556e-01, 4.734900891780853e-01, 4.734983444213867e-01, 4.735057055950165e-01, 4.735122621059418e-01, 4.735181629657745e-01, 4.735235273838043e-01, 4.735283851623535e-01, 4.735328257083893e-01, 4.73536878824234e-01, 4.735406339168549e-01, 4.735440909862518e-01, 4.735472798347473e-01, 4.735502600669861e-01, 4.735530316829681e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.735555946826935e-01, 4.730305075645447e-01, 4.720738530158997e-01, 4.706114828586578e-01, 4.685670733451843e-01, 4.658646285533905e-01, 4.624316990375519e-01, 4.582027494907379e-01, 4.531229436397552e-01, 4.471518993377686e-01, 4.401520192623138e-01, 4.319839179515839e-01, 4.22771155834198e-01, 4.126746654510498e-01, 4.018683433532715e-01, 3.905176222324371e-01, 3.787632882595062e-01, 3.667131364345551e-01, 3.543288707733154e-01, 3.415527045726776e-01, 3.284392654895782e-01, 3.150481879711151e-01, 3.014431297779083e-01, 2.876905202865601e-01, 2.739090621471405e-01, 2.603258490562439e-01, 2.465216070413589e-01, 2.313000857830048e-01, 2.14568093419075e-01, 1.968347430229187e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01, 1.787372678518295e-01]
+mov2.etaHyd=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1.860355958342552e-02, 4.823030531406403e-01, 5.271303653717041e-01, 5.893458127975465e-01, 6.432288885116577e-01, 6.657821536064148e-01, 6.741054058074951e-01, 6.760291457176208e-01, 6.762585043907166e-01, 6.762941479682922e-01, 6.763232946395874e-01, 6.763476133346558e-01, 6.763681769371033e-01, 6.76385760307312e-01, 6.764010787010193e-01, 6.76414430141449e-01, 6.764262318611145e-01, 6.76436722278595e-01, 6.764460802078247e-01, 6.764545440673828e-01, 6.764621734619141e-01, 6.76469087600708e-01, 6.76475465297699e-01, 6.764812469482422e-01, 6.76486611366272e-01, 6.764915585517883e-01, 6.764960885047913e-01, 6.765003800392151e-01, 6.765043139457703e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.765080094337463e-01, 6.75757884979248e-01, 6.743912100791931e-01, 6.723021268844604e-01, 6.693814992904663e-01, 6.655209064483643e-01, 6.606167554855347e-01, 6.545753479003906e-01, 6.473184823989868e-01, 6.387884020805359e-01, 6.287885904312134e-01, 6.171198487281799e-01, 6.03958785533905e-01, 5.895352363586426e-01, 5.740976333618164e-01, 5.578823089599609e-01, 5.410903692245483e-01, 5.238759517669678e-01, 5.061841011047363e-01, 4.879324436187744e-01, 4.691989421844482e-01, 4.50068861246109e-01, 4.306330382823944e-01, 4.10986453294754e-01, 3.912986516952515e-01, 3.718940615653992e-01, 3.521737158298492e-01, 3.304286897182465e-01, 3.06525856256485e-01, 2.811924815177917e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01, 2.553389668464661e-01]
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+ramDam.y=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 9.833333492279053e-01, 9.666666388511658e-01, 9.49999988079071e-01, 9.333333373069763e-01, 9.166666865348816e-01, 8.999999761581421e-01, 8.833333253860474e-01, 8.666666746139526e-01, 8.500000238418579e-01, 8.333333134651184e-01, 8.166666626930237e-01, 8.00000011920929e-01, 7.833333611488342e-01, 7.666666507720947e-01, 7.5e-01, 7.333333492279053e-01, 7.166666388511658e-01, 6.99999988079071e-01, 6.833333373069763e-01, 6.666666865348816e-01, 6.499999761581421e-01, 6.333333253860474e-01, 6.166666746139526e-01, 6.000000238418579e-01, 5.833333134651184e-01, 5.666666626930237e-01, 5.50000011920929e-01, 5.333333611488342e-01, 5.166666507720947e-01, 5e-01, 5e-01, 5e-01, 5e-01, 5e-01, 5e-01, 5e-01, 5e-01, 5e-01, 5e-01, 5e-01]
+mov1.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.583001613616943e+00, 4.784634113311768e+00, 2.153220748901367e+01, 5.322282409667977e+01, 1.047782287597656e+02, 1.820938262939453e+02, 2.897984619140625e+02, 4.328740539550781e+02, 6.163928833007812e+02, 8.455368041992188e+02, 1.125414672851562e+03, 1.461099853515625e+03, 1.857665893554688e+03, 2.320186279296875e+03, 2.853734619140625e+03, 3.463384033203125e+03, 4.15420849609375e+03, 4.931280761718753e+03, 5.799675292968746e+03, 6.76446435546875e+03, 7.83072265625e+03, 9.0035224609375e+03, 1.02879384765625e+04, 1.16890439453125e+04, 1.32119111328125e+04, 1.4861615234375e+04, 1.6643228515625e+04, 1.856182421875e+04, 2.06224765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.27043125e+04, 2.2562322265625e+04, 2.2402353515625e+04, 2.2222333984375e+04, 2.2020099609375e+04, 2.17934296875e+04, 2.1540125e+04, 2.1258087890625e+04, 2.0945421875e+04, 2.059309375e+04, 2.019223828125e+04, 1.97520625e+04, 1.9285013671875e+04, 1.880525e+04, 1.832712109375e+04, 1.7863771484375e+04, 1.74261875e+04, 1.7009693359375e+04, 1.66047578125e+04, 1.6212673828125e+04, 1.58345244140625e+04, 1.54711806640625e+04, 1.51233076171875e+04, 1.47925595703125e+04, 1.4482583984375e+04, 1.41923935546875e+04, 1.39194921875e+04, 1.36617255859375e+04, 1.341743359375e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04]
+mov2.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.583001613616943e+00, 3.79670524597168e+00, 1.615411186218262e+01, 4.153712844848639e+01, 8.657707214355469e+01, 1.628532867431641e+02, 2.77126953125e+02, 4.296744995117188e+02, 6.163928833007812e+02, 8.455368041992188e+02, 1.125414672851562e+03, 1.461099853515625e+03, 1.857665893554688e+03, 2.320186279296875e+03, 2.853734619140625e+03, 3.463384033203125e+03, 4.15420849609375e+03, 4.931280761718753e+03, 5.799675292968746e+03, 6.76446435546875e+03, 7.83072265625e+03, 9.0035224609375e+03, 1.02879384765625e+04, 1.16890439453125e+04, 1.32119111328125e+04, 1.4861615234375e+04, 1.6643228515625e+04, 1.856182421875e+04, 2.06224765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.27043125e+04, 2.2562322265625e+04, 2.2402353515625e+04, 2.2222333984375e+04, 2.2020099609375e+04, 2.17934296875e+04, 2.1540125e+04, 2.1258087890625e+04, 2.0945421875e+04, 2.059309375e+04, 2.019223828125e+04, 1.97520625e+04, 1.9285013671875e+04, 1.880525e+04, 1.832712109375e+04, 1.7863771484375e+04, 1.74261875e+04, 1.7009693359375e+04, 1.66047578125e+04, 1.6212673828125e+04, 1.58345244140625e+04, 1.54711806640625e+04, 1.51233076171875e+04, 1.47925595703125e+04, 1.44825810546875e+04, 1.418096484375e+04, 1.385976171875e+04, 1.352121484375e+04, 1.318010546875e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04, 1.28507724609375e+04]
+mov3.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.583001613616943e+00, 4.784634113311768e+00, 2.153220748901367e+01, 5.322282409667977e+01, 1.047782287597656e+02, 1.820938262939453e+02, 2.897984619140625e+02, 4.328740539550781e+02, 6.163928833007812e+02, 8.455368041992188e+02, 1.125414672851562e+03, 1.461099853515625e+03, 1.857665893554688e+03, 2.320186279296875e+03, 2.853734619140625e+03, 3.463384033203125e+03, 4.15420849609375e+03, 4.931280761718753e+03, 5.799675292968746e+03, 6.76446435546875e+03, 7.83072265625e+03, 9.0035224609375e+03, 1.02879384765625e+04, 1.16890439453125e+04, 1.32119111328125e+04, 1.4861615234375e+04, 1.6643228515625e+04, 1.856182421875e+04, 2.06224765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.2830259765625e+04, 2.27043125e+04, 2.2562322265625e+04, 2.2402353515625e+04, 2.2222333984375e+04, 2.2020099609375e+04, 2.17934296875e+04, 2.1540125e+04, 2.1258087890625e+04, 2.0945421875e+04, 2.059309375e+04, 2.019223828125e+04, 1.97520625e+04, 1.9285013671875e+04, 1.880525e+04, 1.832712109375e+04, 1.7863771484375e+04, 1.74261875e+04, 1.7009693359375e+04, 1.66047578125e+04, 1.6212673828125e+04, 1.58345244140625e+04, 1.54711806640625e+04, 1.51233076171875e+04, 1.47925595703125e+04, 1.4482583984375e+04, 1.41923935546875e+04, 1.39194921875e+04, 1.36617255859375e+04, 1.341743359375e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04, 1.3185326171875e+04]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerTotal.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerTotal.txt
new file mode 100644
index 0000000000..fc49867833
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_ComparePowerTotal.txt
@@ -0,0 +1,27 @@
+last-generated=2024-05-15
+statistics-initialization=
+{
+  "nonlinear": "1, 1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1, 1, 1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 2e+02]
+mov1.eta=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.492167964577675e-02, 6.11555814743042e-01, 5.761631727218628e-01, 5.817868113517761e-01, 5.880606770515442e-01, 5.883736610412598e-01, 5.883923768997192e-01, 5.884082913398743e-01, 5.884376764297485e-01, 5.884642004966736e-01, 5.884859561920166e-01, 5.885040760040283e-01, 5.885193943977356e-01, 5.885325074195862e-01, 5.885439515113831e-01, 5.885539054870605e-01, 5.885626673698425e-01, 5.885704755783081e-01, 5.885775089263916e-01, 5.88583767414093e-01, 5.885894894599915e-01, 5.885946750640869e-01, 5.885993838310242e-01, 5.886037349700928e-01, 5.886076688766479e-01, 5.88611364364624e-01, 5.886147618293762e-01, 5.886179208755493e-01, 5.886209011077881e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.886236429214478e-01, 5.881841778755188e-01, 5.859197378158569e-01, 5.808865427970886e-01, 5.715749263763428e-01, 5.577517747879028e-01, 5.388244390487671e-01, 5.128459334373474e-01, 4.812151193618774e-01, 4.474658071994781e-01, 4.11169171333313e-01, 3.724821209907532e-01, 3.330301940441132e-01, 2.952267229557037e-01, 2.595611214637756e-01, 2.257571220397949e-01, 1.936779171228409e-01, 1.633393317461014e-01, 1.349484473466873e-01, 1.089258715510368e-01, 8.583158254623413e-02, 6.615643203258514e-02, 5.008816719055176e-02, 3.743508085608482e-02, 2.773764170706272e-02, 2.043944224715233e-02, 1.023917552083731e-02, 2.353599993512034e-03, 2.480772382114083e-04, 6.800326900702203e-06, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07, 1.349403788708514e-07]
+mov1.etaHyd=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 4.988811537623405e-02, 8.736511468887329e-01, 8.230902552604675e-01, 8.311240077018738e-01, 8.400866985321045e-01, 8.405337929725647e-01, 8.405605554580688e-01, 8.405832648277283e-01, 8.406252264976501e-01, 8.406631946563721e-01, 8.406942486763e-01, 8.407201170921326e-01, 8.407419919967651e-01, 8.407607674598694e-01, 8.407770395278931e-01, 8.407912850379944e-01, 8.408038020133972e-01, 8.40815007686615e-01, 8.408249616622925e-01, 8.408339619636536e-01, 8.408421277999878e-01, 8.408495187759399e-01, 8.408562541007996e-01, 8.408624529838562e-01, 8.408681154251099e-01, 8.408733606338501e-01, 8.408782482147217e-01, 8.408827781677246e-01, 8.408869504928589e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.408908843994141e-01, 8.402630686759949e-01, 8.370281457901001e-01, 8.298378586769104e-01, 8.165356516838074e-01, 7.96788215637207e-01, 7.697492241859436e-01, 7.326370477676392e-01, 6.874501705169678e-01, 6.392368674278259e-01, 5.873845219612122e-01, 5.321173071861267e-01, 4.757574200630188e-01, 4.217524826526642e-01, 3.708015978336334e-01, 3.225101828575134e-01, 2.766827344894409e-01, 2.333419024944305e-01, 1.927835047245026e-01, 1.556083858013153e-01, 1.226165443658829e-01, 9.450918436050415e-02, 7.15545266866684e-02, 5.347868800163269e-02, 3.962520137429237e-02, 2.919920347630978e-02, 1.462739333510399e-02, 3.362285671755672e-03, 3.543960629031062e-04, 9.714752195577603e-06, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07, 1.927719637251357e-07]
+mov1.etaMot=[6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01, 6.99999988079071e-01]
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+ramDam.y=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 9.666666388511658e-01, 9.333333373069763e-01, 8.999999761581421e-01, 8.666666746139526e-01, 8.333333134651184e-01, 8.00000011920929e-01, 7.666666507720947e-01, 7.333333492279053e-01, 6.99999988079071e-01, 6.666666865348816e-01, 6.333333253860474e-01, 6.000000238418579e-01, 5.666666626930237e-01, 5.333333611488342e-01, 5e-01, 4.666666686534882e-01, 4.333333373069763e-01, 4.000000059604645e-01, 3.666666746139526e-01, 3.333333432674408e-01, 3.00000011920929e-01, 2.666666805744171e-01, 2.333333343267441e-01, 2.000000029802322e-01, 1.666666716337204e-01, 1.333333402872086e-01, 1.000000014901161e-01, 6.666667014360428e-02, 3.333333507180214e-02, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+mov1.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 7.849041372537613e-03, 7.902026921510696e-02, 3.437995910644531e-01, 8.583009839057935e-01, 1.693686008453369e+00, 2.948226690292358e+00, 4.695231437683105e+00, 7.014782428741455e+00, 9.989002227783203e+00, 1.370242309570312e+01, 1.823802185058594e+01, 2.367801666259766e+01, 3.010462951660156e+01, 3.760007476806641e+01, 4.624657821655273e+01, 5.61263542175293e+01, 6.732162475585938e+01, 7.991460418701176e+01, 9.398751831054682e+01, 1.096225814819336e+02, 1.269020156860352e+02, 1.459080352783203e+02, 1.667228698730469e+02, 1.894287414550781e+02, 2.141078491210938e+02, 2.408424224853516e+02, 2.697146911621094e+02, 3.008068542480469e+02, 3.34201171875e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.699797973632812e+02, 3.643883056640625e+02, 3.573406982421875e+02, 3.48763671875e+02, 3.38936767578125e+02, 3.281545715332031e+02, 3.163817749023438e+02, 3.036598815917969e+02, 2.89926513671875e+02, 2.759512329101562e+02, 2.631422424316406e+02, 2.524350738525391e+02, 2.435967864990234e+02, 2.362706604003906e+02, 2.300823822021484e+02, 2.246943969726562e+02, 2.199074401855469e+02, 2.156072540283203e+02, 2.117416229248047e+02, 2.083073577880859e+02, 2.053318328857422e+02, 2.028424377441406e+02, 2.008367004394531e+02, 1.992728118896484e+02, 1.980828247070312e+02, 1.9719189453125e+02, 1.959530334472656e+02, 1.950016326904297e+02, 1.947491302490234e+02, 1.947208557128906e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02, 1.947194519042969e+02]
+mov2.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 6.876427680253983e-03, 8.141607046127319e-02, 3.501363396644592e-01, 8.627013564109814e-01, 1.698006272315979e+00, 2.950947761535645e+00, 4.69660758972168e+00, 7.015505790710449e+00, 9.989782333374023e+00, 1.37034740447998e+01, 1.823940086364746e+01, 2.367978477478027e+01, 3.010685157775879e+01, 3.760282516479492e+01, 4.624993133544922e+01, 5.613039398193359e+01, 6.732643890380859e+01, 7.992028808593754e+01, 9.399416351318354e+01, 1.096303024291992e+02, 1.269109191894531e+02, 1.459182281494141e+02, 1.667344818115234e+02, 1.894418792724609e+02, 2.141226654052734e+02, 2.408590393066406e+02, 2.697332458496094e+02, 3.008275146484375e+02, 3.342240600585938e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.700050964355469e+02, 3.656661682128906e+02, 3.604568481445312e+02, 3.540480346679688e+02, 3.462041931152344e+02, 3.371627502441406e+02, 3.266574096679688e+02, 3.142793579101562e+02, 3.001557922363281e+02, 2.852984008789062e+02, 2.705143432617188e+02, 2.560456237792969e+02, 2.421462707519531e+02, 2.296561737060547e+02, 2.186748962402344e+02, 2.090027618408203e+02, 2.003047332763672e+02, 1.924244995117188e+02, 1.853288879394531e+02, 1.790464019775391e+02, 1.736392822265625e+02, 1.691530151367188e+02, 1.655690765380859e+02, 1.627964172363281e+02, 1.607005767822266e+02, 1.591397705078125e+02, 1.569818878173828e+02, 1.553323516845703e+02, 1.548946533203125e+02, 1.548456573486328e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02, 1.548432159423828e+02]
+mov3.P=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 3.201681189239025e-03, 8.204033225774765e-02, 3.366678059101105e-01, 8.487000465393079e-01, 1.692800521850586e+00, 2.948253631591797e+00, 4.69542407989502e+00, 7.0152587890625e+00, 9.990180015563965e+00, 1.370465755462646e+01, 1.824166870117188e+01, 2.368348121643066e+01, 3.011236000061035e+01, 3.761057281494141e+01, 4.626038360595703e+01, 5.614405822753906e+01, 6.734386444091797e+01, 7.994207000732426e+01, 9.402093505859369e+01, 1.09662727355957e+02, 1.269497222900391e+02, 1.459641723632812e+02, 1.667883605957031e+02, 1.895045318603516e+02, 2.141949768066406e+02, 2.409419403076172e+02, 2.698276977539062e+02, 3.009345092773438e+02, 3.343446350097656e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.70140380859375e+02, 3.642742614746094e+02, 3.558535766601562e+02, 3.443287353515625e+02, 3.292627563476562e+02, 3.1107861328125e+02, 2.897406921386719e+02, 2.646824035644531e+02, 2.371253356933594e+02, 2.098664093017578e+02, 1.838915863037109e+02, 1.598107147216797e+02, 1.378814697265625e+02, 1.185540008544922e+02, 1.015017929077148e+02, 8.621531677246094e+01, 7.238870239257812e+01, 5.985561370849609e+01, 4.856516647338867e+01, 3.856438446044922e+01, 2.995395278930664e+01, 2.280770683288574e+01, 1.709735679626465e+01, 1.267878341674805e+01, 9.338284492492676e+00, 6.850287914276123e+00, 3.410104990005493e+00, 7.800485491752625e-01, 8.211324363946915e-02, 2.250572433695197e-03, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05, 4.465828169486485e-05]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PowerExact.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PowerExact.txt
deleted file mode 100644
index 3afcc4d44e..0000000000
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PowerExact.txt
+++ /dev/null
@@ -1,20 +0,0 @@
-last-generated=2019-08-15
-statistics-initialization=
-{
-  "linear": "0, 0, 0",
-  "nonlinear": "1, 0, 1, 1",
-  "numerical Jacobians": "0"
-}
-statistics-simulation=
-{
-  "linear": " ",
-  "nonlinear": "1, 0, 1, 1",
-  "number of continuous time states": "3",
-  "numerical Jacobians": "0"
-}
-pump_m_flow.P=[6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.468942260742188e+01, 6.630660247802734e+01, 6.795051574707031e+01, 6.962137603759766e+01, 7.131940460205078e+01, 7.304482269287109e+01, 7.479784393310547e+01, 7.657869720458984e+01, 7.838758850097656e+01, 8.022474670410156e+01, 8.209038543701172e+01, 8.398472595214844e+01, 8.590798950195312e+01, 8.786038970947266e+01, 8.984215545654297e+01, 9.185349273681641e+01, 9.389463043212891e+01, 9.596578216552734e+01, 9.806717681884766e+01, 1.001990203857422e+02, 1.023615341186523e+02, 1.045549468994141e+02, 1.067794723510742e+02, 1.090353240966797e+02, 1.113227310180664e+02, 1.136419067382812e+02, 1.159930648803711e+02, 1.183764343261719e+02, 1.207922286987305e+02, 1.232406768798828e+02, 1.257219772338867e+02, 1.282363739013672e+02, 1.307840728759766e+02, 1.333652801513672e+02, 1.359802398681641e+02, 1.38629150390625e+02, 1.41312255859375e+02, 1.440297546386719e+02, 1.467818603515625e+02, 1.495688171386719e+02, 1.523908233642578e+02, 1.552480926513672e+02, 1.58140869140625e+02, 1.610693664550781e+02, 1.640337829589844e+02, 1.670343475341797e+02, 1.700712890625e+02, 1.731448211669922e+02, 1.762551727294922e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02]
-pump_Nrpm.P=[6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.468942260742188e+01, 6.630660247802734e+01, 6.795051574707031e+01, 6.962137603759766e+01, 7.131940460205078e+01, 7.304482269287109e+01, 7.479784393310547e+01, 7.657869720458984e+01, 7.838758850097656e+01, 8.022474670410156e+01, 8.209038543701172e+01, 8.398472595214844e+01, 8.590798950195312e+01, 8.786038970947266e+01, 8.984215545654297e+01, 9.185349273681641e+01, 9.389463043212891e+01, 9.596578216552734e+01, 9.806717681884766e+01, 1.001990203857422e+02, 1.023615341186523e+02, 1.045549468994141e+02, 1.067794723510742e+02, 1.090353240966797e+02, 1.113227310180664e+02, 1.136419067382812e+02, 1.159930648803711e+02, 1.183764343261719e+02, 1.207922286987305e+02, 1.232406768798828e+02, 1.257219772338867e+02, 1.282363739013672e+02, 1.307840728759766e+02, 1.333652801513672e+02, 1.359802398681641e+02, 1.38629150390625e+02, 1.41312255859375e+02, 1.440297546386719e+02, 1.467818603515625e+02, 1.495688171386719e+02, 1.523908233642578e+02, 1.552480926513672e+02, 1.58140869140625e+02, 1.610693664550781e+02, 1.640337829589844e+02, 1.670343475341797e+02, 1.700712890625e+02, 1.731448211669922e+02, 1.762551727294922e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02]
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-time=[0e+00, 2e+02]
-pump_Nrpm.per.speed_rpm_nominal=[3.04e+03, 3.04e+03]
-pump_Nrpm.Nrpm=[2.4e+03, 2.4e+03, 2.4e+03, 2.4e+03, 2.4e+03, 2.4e+03, 2.42e+03, 2.44e+03, 2.46e+03, 2.48e+03, 2.5e+03, 2.52e+03, 2.54e+03, 2.56e+03, 2.58e+03, 2.6e+03, 2.62e+03, 2.64e+03, 2.66e+03, 2.68e+03, 2.7e+03, 2.72e+03, 2.74e+03, 2.76e+03, 2.78e+03, 2.8e+03, 2.82e+03, 2.84e+03, 2.86e+03, 2.88e+03, 2.9e+03, 2.92e+03, 2.94e+03, 2.96e+03, 2.98e+03, 3e+03, 3.02e+03, 3.04e+03, 3.06e+03, 3.08e+03, 3.1e+03, 3.12e+03, 3.14e+03, 3.16e+03, 3.18e+03, 3.2e+03, 3.22e+03, 3.24e+03, 3.26e+03, 3.28e+03, 3.3e+03, 3.32e+03, 3.34e+03, 3.36e+03, 3.38e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PowerSimplified.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PowerSimplified.txt
deleted file mode 100644
index f62e6cd698..0000000000
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PowerSimplified.txt
+++ /dev/null
@@ -1,20 +0,0 @@
-last-generated=2019-08-15
-statistics-initialization=
-{
-  "linear": "0, 0, 0",
-  "nonlinear": "1, 0",
-  "numerical Jacobians": "0"
-}
-statistics-simulation=
-{
-  "linear": " ",
-  "nonlinear": "1, 0",
-  "number of continuous time states": "3",
-  "numerical Jacobians": "0"
-}
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-pump_Nrpm.P=[6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.30987548828125e+01, 6.468942260742188e+01, 6.630660247802734e+01, 6.795051574707031e+01, 6.962137603759766e+01, 7.131940460205078e+01, 7.304482269287109e+01, 7.479784393310547e+01, 7.657869720458984e+01, 7.838758850097656e+01, 8.022474670410156e+01, 8.209038543701172e+01, 8.398472595214844e+01, 8.590798950195312e+01, 8.786038970947266e+01, 8.984215545654297e+01, 9.185349273681641e+01, 9.389463043212891e+01, 9.596578216552734e+01, 9.806717681884766e+01, 1.001990203857422e+02, 1.023615341186523e+02, 1.045549468994141e+02, 1.067794723510742e+02, 1.090353240966797e+02, 1.113227310180664e+02, 1.136419067382812e+02, 1.159930648803711e+02, 1.183764343261719e+02, 1.207922286987305e+02, 1.232406768798828e+02, 1.257219772338867e+02, 1.282363739013672e+02, 1.307840728759766e+02, 1.333652801513672e+02, 1.359802398681641e+02, 1.38629150390625e+02, 1.41312255859375e+02, 1.440297546386719e+02, 1.467818603515625e+02, 1.495688171386719e+02, 1.523908233642578e+02, 1.552480926513672e+02, 1.58140869140625e+02, 1.610693664550781e+02, 1.640337829589844e+02, 1.670343475341797e+02, 1.700712890625e+02, 1.731448211669922e+02, 1.762551727294922e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02, 1.794025421142578e+02]
-pump_dp.P=[9.013990020751953e+01, 9.013990020751953e+01, 9.013990020751953e+01, 9.013990020751953e+01, 9.013990020751953e+01, 9.013990020751953e+01, 9.241249847412109e+01, 9.472297668457031e+01, 9.707164764404297e+01, 9.945882415771484e+01, 1.018848266601562e+02, 1.043499526977539e+02, 1.068545303344727e+02, 1.093988647460938e+02, 1.11983268737793e+02, 1.146080627441406e+02, 1.17273551940918e+02, 1.199800491333008e+02, 1.227278747558594e+02, 1.25517333984375e+02, 1.283487396240234e+02, 1.312224273681641e+02, 1.34138671875e+02, 1.370978240966797e+02, 1.401001586914062e+02, 1.431460266113281e+02, 1.462357177734375e+02, 1.493695526123047e+02, 1.525478363037109e+02, 1.557708892822266e+02, 1.590390319824219e+02, 1.623525543212891e+02, 1.657117919921875e+02, 1.691170501708984e+02, 1.725686492919922e+02, 1.7606689453125e+02, 1.796120910644531e+02, 1.832045593261719e+02, 1.868446197509766e+02, 1.905325775146484e+02, 1.942687530517578e+02, 1.980534515380859e+02, 2.018869934082031e+02, 2.057696685791016e+02, 2.097018280029297e+02, 2.136837615966797e+02, 2.177157745361328e+02, 2.217982025146484e+02, 2.259313507080078e+02, 2.301155242919922e+02, 2.343510284423828e+02, 2.386381988525391e+02, 2.429773406982422e+02, 2.473687744140625e+02, 2.518127899169922e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02, 2.563097229003906e+02]
-time=[0e+00, 2e+02]
-pump_Nrpm.per.speed_rpm_nominal=[3.04e+03, 3.04e+03]
-pump_Nrpm.Nrpm=[2.4e+03, 2.4e+03, 2.4e+03, 2.4e+03, 2.4e+03, 2.4e+03, 2.42e+03, 2.44e+03, 2.46e+03, 2.48e+03, 2.5e+03, 2.52e+03, 2.54e+03, 2.56e+03, 2.58e+03, 2.6e+03, 2.62e+03, 2.64e+03, 2.66e+03, 2.68e+03, 2.7e+03, 2.72e+03, 2.74e+03, 2.76e+03, 2.78e+03, 2.8e+03, 2.82e+03, 2.84e+03, 2.86e+03, 2.88e+03, 2.9e+03, 2.92e+03, 2.94e+03, 2.96e+03, 2.98e+03, 3e+03, 3.02e+03, 3.04e+03, 3.06e+03, 3.08e+03, 3.1e+03, 3.12e+03, 3.14e+03, 3.16e+03, 3.18e+03, 3.2e+03, 3.22e+03, 3.24e+03, 3.26e+03, 3.28e+03, 3.3e+03, 3.32e+03, 3.34e+03, 3.36e+03, 3.38e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03, 3.4e+03]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PressureCurve.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PressureCurve.txt
new file mode 100644
index 0000000000..671a5d27cf
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_PressureCurve.txt
@@ -0,0 +1,15 @@
+last-generated=2023-05-01
+statistics-initialization=
+{
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
+mov.dpMachine=[3.199975341796875e+03, 3.188406249741149e+03, 3.176818847137893e+03, 3.165218016799853e+03, 3.153608397399257e+03, 3.141994629771543e+03, 3.130381346099214e+03, 3.118773437845827e+03, 3.107175290896198e+03, 3.095591801014866e+03, 3.084027345472034e+03, 3.072487059859953e+03, 3.06097485043299e+03, 3.04949608828664e+03, 3.038054932321581e+03, 3.026656012642737e+03, 3.015303951029063e+03, 3.004199953088358e+03, 2.99417871778358e+03, 2.985234128868386e+03, 2.977249513992482e+03, 2.970109126476638e+03, 2.963696776625323e+03, 2.957895998423362e+03, 2.952590817598864e+03, 2.9476650390625e+03, 2.943002681202264e+03, 2.938487553638542e+03, 2.934003418505133e+03, 2.929434566415214e+03, 2.924665044877434e+03, 2.919579102811925e+03, 2.914061275128633e+03, 2.907996102027258e+03, 2.901269045479387e+03, 2.893765620220433e+03, 2.885371838728988e+03, 2.875974369920082e+03, 2.865460688003117e+03, 2.853718976220851e+03, 2.840638435865969e+03, 2.826108881195e+03, 2.810022194415784e+03, 2.792270765144991e+03, 2.772748530237713e+03, 2.751351291457304e+03, 2.727976338545605e+03, 2.702522946030432e+03, 2.674891570470941e+03, 2.644986357533779e+03, 2.612692626953125e+03, 2.577931606109606e+03, 2.540819994995681e+03, 2.501487920931178e+03, 2.460064055458447e+03, 2.41667510145278e+03, 2.371446544155037e+03, 2.324501918849708e+03, 2.275962808110926e+03, 2.22594981782853e+03, 2.174581666663757e+03, 2.12197492943692e+03, 2.068244654727896e+03, 2.013505100586374e+03, 1.957868083774831e+03, 1.901444444545336e+03, 1.844343656253201e+03, 1.786672704007122e+03, 1.72853861591321e+03, 1.670046372732579e+03, 1.611299978670164e+03, 1.552402095202839e+03, 1.493455002618427e+03, 1.434558705998082e+03, 1.37581316629458e+03, 1.317317626953125e+03, 1.259170232873413e+03, 1.201468762606838e+03, 1.144310018188858e+03, 1.087791380440723e+03, 1.032008244830083e+03, 9.77057080887731e+02, 9.230339583710224e+02, 8.700349468256555e+02, 8.181248037663067e+02, 7.66591004168835e+02, 7.151021244093479e+02, 6.636588990325905e+02, 6.122618163260703e+02, 5.609112425020343e+02, 5.096076353205164e+02, 4.583516053202501e+02, 4.071430297658023e+02, 3.559825805236241e+02, 3.048706543247062e+02, 2.53807632645829e+02, 2.02793927467534e+02, 1.51830208615654e+02, 1.00916265283436e+02, 5.005277141792394e+01, -7.598958015441895e-01]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_Pump_Nrpm_stratos.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_Pump_Nrpm_stratos.txt
deleted file mode 100644
index ff27e992c6..0000000000
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_Pump_Nrpm_stratos.txt
+++ /dev/null
@@ -1,24 +0,0 @@
-last-generated=2022-05-23
-statistics-simulation=
-{
-  "linear": " ",
-  "nonlinear": " ",
-  "number of continuous time states": "20",
-  "numerical Jacobians": "0"
-}
-time=[0e+00, 1e+03]
-pump1.m_flow=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 7.514491677284241e-02, 2.590211033821106e-01, 4.644336700439453e-01, 6.724663376808167e-01, 8.807709813117981e-01, 1.089101672172546e+00, 1.29743480682373e+00, 1.505768179893494e+00, 1.714101552963257e+00, 1.92243480682373e+00, 2.130768060684204e+00, 2.339101552963257e+00, 2.54743480682373e+00, 2.755768060684204e+00, 2.964101552963257e+00, 3.17243480682373e+00, 3.380768060684204e+00, 3.589101552963257e+00, 3.79743480682373e+00, 4.005768299102783e+00, 4.214101314544678e+00, 4.42243480682373e+00, 4.630768299102783e+00, 4.839101314544678e+00, 5.04743480682373e+00, 5.255768299102783e+00, 5.464101314544678e+00, 5.67243480682373e+00, 5.880768299102783e+00, 6.089101314544678e+00, 6.29743480682373e+00, 6.505768299102783e+00, 6.714101314544678e+00, 6.92243480682373e+00, 7.130768299102783e+00, 7.339101314544678e+00, 7.54743480682373e+00, 7.755768299102783e+00, 7.964101314544678e+00, 8.17243480682373e+00, 8.380767822265625e+00, 8.589101791381836e+00, 8.79743480682373e+00, 9.005767822265625e+00, 9.214101791381836e+00, 9.42243480682373e+00, 9.630767822265625e+00, 9.839101791381836e+00, 1.004743480682373e+01, 1.025576782226562e+01, 1.046410179138184e+01, 1.067243480682373e+01, 1.088076782226562e+01, 1.105775451660156e+01, 1.1104323387146e+01, 1.111039257049561e+01, 1.111104106903076e+01, 1.111110496520996e+01, 1.111110973358154e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01]
-pump2.m_flow=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 7.514491677284241e-02, 2.590211033821106e-01, 4.644336700439453e-01, 6.724663376808167e-01, 8.807709813117981e-01, 1.089101672172546e+00, 1.29743480682373e+00, 1.505768179893494e+00, 1.714101552963257e+00, 1.92243480682373e+00, 2.130768060684204e+00, 2.339101552963257e+00, 2.54743480682373e+00, 2.755768060684204e+00, 2.964101552963257e+00, 3.17243480682373e+00, 3.380768060684204e+00, 3.589101552963257e+00, 3.79743480682373e+00, 4.005768299102783e+00, 4.214101314544678e+00, 4.42243480682373e+00, 4.630768299102783e+00, 4.839101314544678e+00, 5.04743480682373e+00, 5.255768299102783e+00, 5.464101314544678e+00, 5.67243480682373e+00, 5.880768299102783e+00, 6.089101314544678e+00, 6.29743480682373e+00, 6.505768299102783e+00, 6.714101314544678e+00, 6.92243480682373e+00, 7.130768299102783e+00, 7.339101314544678e+00, 7.54743480682373e+00, 7.755768299102783e+00, 7.964101314544678e+00, 8.17243480682373e+00, 8.380767822265625e+00, 8.589101791381836e+00, 8.79743480682373e+00, 9.005767822265625e+00, 9.214101791381836e+00, 9.42243480682373e+00, 9.630767822265625e+00, 9.839101791381836e+00, 1.004743480682373e+01, 1.025576782226562e+01, 1.046410179138184e+01, 1.067243480682373e+01, 1.088076782226562e+01, 1.108910179138184e+01, 1.129743480682373e+01, 1.150576782226562e+01, 1.171410179138184e+01, 1.192243480682373e+01, 1.213076782226562e+01, 1.233910179138184e+01, 1.254743480682373e+01, 1.275576782226562e+01, 1.296410179138184e+01, 1.317243480682373e+01, 1.338076782226562e+01, 1.358910179138184e+01, 1.379743480682373e+01, 1.400576782226562e+01, 1.421410179138184e+01, 1.442243480682373e+01, 1.463076782226562e+01, 1.483910179138184e+01, 1.504743480682373e+01, 1.522443866729736e+01, 1.527099323272705e+01, 1.527705955505371e+01, 1.527770805358887e+01, 1.527777099609375e+01, 1.527777671813965e+01, 1.527777671813965e+01, 1.527777767181396e+01, 1.527777767181396e+01, 1.527777767181396e+01, 1.527777767181396e+01, 1.527777767181396e+01, 1.527777767181396e+01, 1.527777767181396e+01, 1.527777767181396e+01, 1.527777767181396e+01, 1.527777767181396e+01]
-pump3.m_flow=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 7.514491677284241e-02, 2.590211033821106e-01, 4.644336700439453e-01, 6.724663376808167e-01, 8.807709813117981e-01, 1.089101672172546e+00, 1.29743480682373e+00, 1.505768179893494e+00, 1.714101552963257e+00, 1.92243480682373e+00, 2.130768060684204e+00, 2.339101552963257e+00, 2.54743480682373e+00, 2.755768060684204e+00, 2.964101552963257e+00, 3.17243480682373e+00, 3.380768060684204e+00, 3.589101552963257e+00, 3.79743480682373e+00, 4.005768299102783e+00, 4.214101314544678e+00, 4.42243480682373e+00, 4.630768299102783e+00, 4.839101314544678e+00, 5.04743480682373e+00, 5.255768299102783e+00, 5.464101314544678e+00, 5.67243480682373e+00, 5.880768299102783e+00, 6.089101314544678e+00, 6.29743480682373e+00, 6.505768299102783e+00, 6.714101314544678e+00, 6.92243480682373e+00, 7.130768299102783e+00, 7.339101314544678e+00, 7.54743480682373e+00, 7.755768299102783e+00, 7.964101314544678e+00, 8.17243480682373e+00, 8.380767822265625e+00, 8.589101791381836e+00, 8.79743480682373e+00, 9.005767822265625e+00, 9.214101791381836e+00, 9.42243480682373e+00, 9.630767822265625e+00, 9.839101791381836e+00, 1.004743480682373e+01, 1.025576782226562e+01, 1.046410179138184e+01, 1.067243480682373e+01, 1.088076782226562e+01, 1.105775451660156e+01, 1.1104323387146e+01, 1.111039257049561e+01, 1.111104106903076e+01, 1.111110496520996e+01, 1.111110973358154e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01, 1.111111068725586e+01]
-pump4.m_flow=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 7.514491677284241e-02, 2.590211033821106e-01, 4.644336700439453e-01, 6.724663376808167e-01, 8.807709813117981e-01, 1.089101672172546e+00, 1.29743480682373e+00, 1.505768179893494e+00, 1.714101552963257e+00, 1.92243480682373e+00, 2.130768060684204e+00, 2.339101552963257e+00, 2.54743480682373e+00, 2.755768060684204e+00, 2.964101552963257e+00, 3.17243480682373e+00, 3.380768060684204e+00, 3.589101552963257e+00, 3.79743480682373e+00, 4.005768299102783e+00, 4.214101314544678e+00, 4.42243480682373e+00, 4.630768299102783e+00, 4.839101314544678e+00, 5.04743480682373e+00, 5.255768299102783e+00, 5.464101314544678e+00, 5.67243480682373e+00, 5.880768299102783e+00, 6.057771682739258e+00, 6.104327201843262e+00, 6.110393047332764e+00, 6.111041069030762e+00, 6.111104488372803e+00, 6.111110687255859e+00, 6.111110687255859e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00, 6.111111164093018e+00]
-pump5.m_flow=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 7.514491677284241e-02, 2.590211033821106e-01, 4.644336700439453e-01, 6.724663376808167e-01, 8.807709813117981e-01, 1.089101672172546e+00, 1.29743480682373e+00, 1.505768179893494e+00, 1.714101552963257e+00, 1.92243480682373e+00, 2.130768060684204e+00, 2.339101552963257e+00, 2.54743480682373e+00, 2.755768060684204e+00, 2.964101552963257e+00, 3.17243480682373e+00, 3.380768060684204e+00, 3.589101552963257e+00, 3.79743480682373e+00, 4.005768299102783e+00, 4.214101314544678e+00, 4.391105651855469e+00, 4.437659740447998e+00, 4.443726062774658e+00, 4.444374561309814e+00, 4.444437980651855e+00, 4.444443702697754e+00, 4.444444179534912e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00, 4.44444465637207e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_Pump_y_stratos.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_Pump_y_stratos.txt
new file mode 100644
index 0000000000..806384f990
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_Pump_y_stratos.txt
@@ -0,0 +1,24 @@
+last-generated=2020-08-17
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "20",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_SpeedControlled_Nrpm.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_SpeedControlled_Nrpm.txt
deleted file mode 100644
index db12f04375..0000000000
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Movers_Validation_SpeedControlled_Nrpm.txt
+++ /dev/null
@@ -1,19 +0,0 @@
-last-generated=2019-08-15
-statistics-initialization=
-{
-  "nonlinear": "1, 2",
-  "numerical Jacobians": "0"
-}
-statistics-simulation=
-{
-  "linear": " ",
-  "nonlinear": "1, 0, 1",
-  "number of continuous time states": "3",
-  "numerical Jacobians": "0"
-}
-gain.u=[1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 1e+00, 9.8e-01, 9.6e-01, 9.399999999999999e-01, 9.2e-01, 9e-01, 8.8e-01, 8.6e-01, 8.4e-01, 8.2e-01, 8e-01, 7.8e-01, 7.6e-01, 7.4e-01, 7.2e-01, 7e-01, 6.8e-01, 6.6e-01, 6.4e-01, 6.2e-01, 6e-01, 5.8e-01, 5.600000000000001e-01, 5.4e-01, 5.2e-01, 5e-01, 4.799999701981039e-01, 4.59999970198246e-01, 4.399999403962078e-01, 4.200000298016828e-01, 4.00000029801967e-01, 3.800000000000709e-01, 3.600000000002133e-01, 3.399999701981751e-01, 3.199999403965277e-01, 3.00000059603579e-01, 2.800000298018961e-01, 2.599999999998579e-01, 2.399999850990164e-01, 2.199999701982105e-01, 1.999999552972269e-01, 1.800000596036677e-01, 1.600000298018249e-01, 1.400000149008946e-01, 1.199999925493573e-01, 9.999997764865798e-02, 7.99999552972359e-02, 6.00000558784486e-02, 4.000003725226355e-02, 2.000001862613177e-02, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
-time=[0e+00, 1e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Pools_Examples_IndoorSwimmingPool.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Pools_Examples_IndoorSwimmingPool.txt
new file mode 100644
index 0000000000..1365fa4dcd
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Pools_Examples_IndoorSwimmingPool.txt
@@ -0,0 +1,18 @@
+last-generated=2024-07-23
+statistics-initialization=
+{
+  "nonlinear": "0, 16, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "13",
+  "nonlinear": "16, 0, 1",
+  "number of continuous time states": "3",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 6.048e+05]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Pools_Examples_IndoorSwimmingPoolExternalHeatingSystem.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Pools_Examples_IndoorSwimmingPoolExternalHeatingSystem.txt
new file mode 100644
index 0000000000..3b6ba2a343
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Pools_Examples_IndoorSwimmingPoolExternalHeatingSystem.txt
@@ -0,0 +1,18 @@
+last-generated=2024-07-23
+statistics-initialization=
+{
+  "nonlinear": "0, 17, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "13",
+  "nonlinear": "17, 0, 1",
+  "number of continuous time states": "3",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 6.048e+05]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Sensors_Examples_HeatMeter.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Sensors_Examples_HeatMeter.txt
new file mode 100644
index 0000000000..e6493018ae
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Sensors_Examples_HeatMeter.txt
@@ -0,0 +1,11 @@
+last-generated=2024-02-01
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "3",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 6e+01]
+senHeaFlo.Q_flow=[0e+00, 6.135302814887254e+03, 2.024211004943313e+04, 3.806596635045912e+04, 5.735886017640069e+04, 7.69003203125e+04, 9.605505767047344e+04, 1.145098494566929e+05, 1.321029788968033e+05, 1.487847005315746e+05, 1.645585e+05, 1.794507366602567e+05, 1.934949730579872e+05, 2.067290271429792e+05, 2.191943982694409e+05, 2.30933234375e+05, 2.41987868139305e+05, 2.523970031914593e+05, 2.621994657085459e+05, 2.714292556591234e+05, 2.8011971875e+05, 2.883016199230112e+05, 2.960048461113893e+05, 3.032570914998232e+05, 3.100849416862036e+05, 3.16513375e+05, 3.225658712441389e+05, 3.282644616773623e+05, 3.336297565791147e+05, 3.38681284347135e+05, 3.4343725e+05, 3.479150597213503e+05, 3.521309010177422e+05, 3.561000986168839e+05, 3.598370335411865e+05, 3.6335534375e+05, 3.666678729444488e+05, 3.697867773791028e+05, 3.727235973512874e+05, 3.754886266952436e+05, 3.780919375e+05, 3.805429672290988e+05, 3.828506533860168e+05, 3.85023346414309e+05, 3.870689075040729e+05, 3.8899471875e+05, 3.908079051247715e+05, 3.925150603812684e+05, 3.941224394709131e+05, 3.956357509278391e+05, 3.97060625e+05, 3.984022804174283e+05, 3.996654359322101e+05, 4.008547202083168e+05, 4.019744347208977e+05, 4.0302865625e+05, 4.040212211838006e+05, 4.04955686340282e+05, 4.058354698288537e+05, 4.066638104436868e+05, 4.0744371875e+05, 4.081780018008138e+05, 4.088693741418842e+05, 4.09520344548312e+05, 4.101332484785269e+05, 4.107103125e+05, 4.11253626332332e+05, 4.117651556152049e+05, 4.122467818404886e+05, 4.127002176242927e+05, 4.13127125e+05, 4.135290322358382e+05, 4.139074682803112e+05, 4.142637504369059e+05, 4.145992179171435e+05, 4.149150625e+05, 4.152124382295441e+05, 4.154924371525018e+05, 4.157560628232587e+05, 4.160042806340994e+05, 4.1623796875e+05, 4.164580005396084e+05, 4.16665155992903e+05, 4.168601564892154e+05, 4.170437807942336e+05, 4.172166875e+05, 4.17379437899342e+05, 4.175326873098595e+05, 4.176770001768287e+05, 4.178128434126455e+05, 4.1794075e+05, 4.180611877956323e+05, 4.181745936091331e+05, 4.182813438809327e+05, 4.183818435008583e+05, 4.1847646875e+05, 4.185655627185454e+05, 4.186494373958896e+05, 4.187283750967591e+05, 4.188026873156272e+05, 4.1887265625e+05]
+heaFloRat.Q_flow=[4.2e+05, 4.2e+05]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_ASHRAEHeatLoss.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_ASHRAEHeatLoss.txt
new file mode 100644
index 0000000000..cd4d310e59
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_ASHRAEHeatLoss.txt
@@ -0,0 +1,15 @@
+last-generated=2019-10-21
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_ASHRAESolarGain.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_ASHRAESolarGain.txt
new file mode 100644
index 0000000000..95a8ea7499
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_ASHRAESolarGain.txt
@@ -0,0 +1,14 @@
+last-generated=2024-04-26
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_EN12975HeatLoss.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_EN12975HeatLoss.txt
new file mode 100644
index 0000000000..85891c41e9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_EN12975HeatLoss.txt
@@ -0,0 +1,15 @@
+last-generated=2024-01-17
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_EN12975SolarGain.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_EN12975SolarGain.txt
new file mode 100644
index 0000000000..53a1b80f0c
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_BaseClasses_Examples_EN12975SolarGain.txt
@@ -0,0 +1,14 @@
+last-generated=2024-04-26
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Controls_BaseClasses_Examples_GCritCalc.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Controls_BaseClasses_Examples_GCritCalc.txt
new file mode 100644
index 0000000000..86d0f3b742
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Controls_BaseClasses_Examples_GCritCalc.txt
@@ -0,0 +1,11 @@
+last-generated=2024-01-17
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Controls_Examples_SolarPumpController.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Controls_Examples_SolarPumpController.txt
new file mode 100644
index 0000000000..6875218f93
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Controls_Examples_SolarPumpController.txt
@@ -0,0 +1,11 @@
+last-generated=2024-01-17
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_Concentrating.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_Concentrating.txt
new file mode 100644
index 0000000000..a82b56c816
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_Concentrating.txt
@@ -0,0 +1,13 @@
+last-generated=2021-09-16
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "0, 1",
+  "number of continuous time states": "11",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlate.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlate.txt
new file mode 100644
index 0000000000..06d35493f0
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlate.txt
@@ -0,0 +1,18 @@
+last-generated=2024-06-05
+statistics-initialization=
+{
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "0, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1",
+  "number of continuous time states": "11",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateShaCoeTrue.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateShaCoeTrue.txt
new file mode 100644
index 0000000000..837b7363bd
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateShaCoeTrue.txt
@@ -0,0 +1,13 @@
+last-generated=2021-09-16
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "number of continuous time states": "11",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateTotalArea.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateTotalArea.txt
new file mode 100644
index 0000000000..be63ae4c3f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateTotalArea.txt
@@ -0,0 +1,19 @@
+last-generated=2021-09-17
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "1",
+  "number of continuous time states": "40",
+  "numerical Jacobians": "0"
+}
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+solCol1.m_flow=[3.885820135474205e-02, 3.885820135474205e-02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateWithTank.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateWithTank.txt
new file mode 100644
index 0000000000..10944bb9a5
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_FlatPlateWithTank.txt
@@ -0,0 +1,13 @@
+last-generated=2022-11-08
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "27",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_Tubular.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_Tubular.txt
new file mode 100644
index 0000000000..25d3f35646
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Examples_Tubular.txt
@@ -0,0 +1,18 @@
+last-generated=2024-06-05
+statistics-initialization=
+{
+  "nonlinear": "1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "0, 1",
+  "number of continuous time states": "11",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975NPanels.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975NPanels.txt
new file mode 100644
index 0000000000..cc58283089
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975NPanels.txt
@@ -0,0 +1,17 @@
+last-generated=2024-04-26
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "60",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975_Array.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975_Array.txt
new file mode 100644
index 0000000000..1e0eadf5b3
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975_Array.txt
@@ -0,0 +1,19 @@
+last-generated=2024-04-26
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "9",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
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+solCol.m_flow=[1.036781966686249e-01, 1.036781966686249e-01]
+solCol1.m_flow=[5.183909833431244e-02, 5.183909833431244e-02]
+solCol2.m_flow=[5.183909833431244e-02, 5.183909833431244e-02]
+solCol.dp=[5e+01, 5e+01]
+solCol1.dp=[5e+01, 5e+01]
+solCol2.dp=[5e+01, 5e+01]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975_Series.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975_Series.txt
new file mode 100644
index 0000000000..a2d7e2c981
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_EN12975_Series.txt
@@ -0,0 +1,12 @@
+last-generated=2024-04-26
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "12",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_ExtremeAmbientConditions.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_ExtremeAmbientConditions.txt
new file mode 100644
index 0000000000..72271ecc44
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_ExtremeAmbientConditions.txt
@@ -0,0 +1,23 @@
+last-generated=2024-04-26
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "6",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_FlatPlate.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_FlatPlate.txt
new file mode 100644
index 0000000000..8b287c8ef5
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_FlatPlate.txt
@@ -0,0 +1,11 @@
+last-generated=2021-09-16
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "30",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_FlatPlateNPanels.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_FlatPlateNPanels.txt
new file mode 100644
index 0000000000..e9cd7286ee
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_SolarCollectors_Validation_FlatPlateNPanels.txt
@@ -0,0 +1,17 @@
+last-generated=2024-04-26
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "number of continuous time states": "60",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_BufferStorage.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_BufferStorage.txt
deleted file mode 100644
index d900fc152b..0000000000
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_BufferStorage.txt
+++ /dev/null
@@ -1,13 +0,0 @@
-last-generated=2022-05-23
-statistics-simulation=
-{
-  "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0",
-  "nonlinear": "1, 1, 1, 1, 1, 1, 1, 1",
-  "number of continuous time states": "66",
-  "numerical Jacobians": "0"
-}
-time=[0e+00, 8.64e+04]
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-bufferStorage.portHC1Out.p=[1.01325e+05, 1.01325e+05]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageBoiler.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageBoiler.txt
new file mode 100644
index 0000000000..076f52238e
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageBoiler.txt
@@ -0,0 +1,18 @@
+last-generated=2022-11-14
+statistics-initialization=
+{
+  "nonlinear": "1, 0, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
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+  "nonlinear": "1, 0, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1",
+  "number of continuous time states": "76",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+04]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageDetailedExample.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageDetailedExample.txt
new file mode 100644
index 0000000000..8d50b2fce9
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageDetailedExample.txt
@@ -0,0 +1,13 @@
+last-generated=2024-07-19
+statistics-simulation=
+{
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageSimpleExample.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageSimpleExample.txt
new file mode 100644
index 0000000000..019bccd2d0
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageSimpleExample.txt
@@ -0,0 +1,19 @@
+last-generated=2024-07-19
+statistics-initialization=
+{
+  "nonlinear": "1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0",
+  "nonlinear": "1, 1",
+  "number of continuous time states": "17",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageSolarCollector.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageSolarCollector.txt
new file mode 100644
index 0000000000..bb6a7887ea
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Fluid_Storage_Examples_StorageSolarCollector.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-23
+statistics-initialization=
+{
+  "nonlinear": "1, 0, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0",
+  "nonlinear": "1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1, 1",
+  "number of continuous time states": "83",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1.728e+05]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Admix.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Admix.txt
new file mode 100644
index 0000000000..2a3f29f9ee
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Admix.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "3, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
+  "nonlinear": "2",
+  "number of continuous time states": "56",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Injection.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Injection.txt
new file mode 100644
index 0000000000..5130443426
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Injection.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "4, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
+  "nonlinear": "3",
+  "number of continuous time states": "79",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Injection2WayValve.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Injection2WayValve.txt
new file mode 100644
index 0000000000..35c5b3d25f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Injection2WayValve.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "3, 0, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
+  "nonlinear": "2",
+  "number of continuous time states": "63",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Pump.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Pump.txt
new file mode 100644
index 0000000000..f18f6cb0d6
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Pump.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "1, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0",
+  "nonlinear": "1, 1, 1, 1",
+  "number of continuous time states": "26",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Throttle.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Throttle.txt
new file mode 100644
index 0000000000..722ae4b6e7
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_Throttle.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "1, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0",
+  "nonlinear": "1",
+  "number of continuous time states": "30",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_ThrottlePump.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_ThrottlePump.txt
new file mode 100644
index 0000000000..4d9881115e
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_HydraulicModules_Examples_ThrottlePump.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "1, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0, 0, 0",
+  "nonlinear": "1",
+  "number of continuous time states": "40",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 6e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_DemandControlledAHU.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_DemandControlledAHU.txt
new file mode 100644
index 0000000000..a024d33bed
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_DemandControlledAHU.txt
@@ -0,0 +1,20 @@
+last-generated=2024-07-25
+statistics-initialization=
+{
+  "linear": "4, 0",
+  "nonlinear": "4, 0, 4, 0, 3, 0, 0, 1, 0, 1, 0, 0, 0, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 4, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
+  "nonlinear": "0, 1, 1, 0, 0, 0, 0, 0, 2, 1, 1, 1, 1, 1, 1, 2, 1, 1, 1, 1, 1, 1, 2, 1, 1, 1, 1,   1, 1, 0, 1, 0, 1, 0, 1",
+  "number of continuous time states": "272",
+  "numerical Jacobians": "0"
+}
+time=[5.9616e+06, 6.5664e+06]
+genericAHU.genericAHUBus.TSupMea=[3.031499938964844e+02, 2.931525085449219e+02, 2.931464233398438e+02, 2.931482971191406e+02, 2.931467529296875e+02, 2.931530151367188e+02, 2.931550659179687e+02, 2.931567687988281e+02, 2.931459167480469e+02, 2.931519653320312e+02, 2.931468200683594e+02, 2.931435424804687e+02, 2.931444396972656e+02, 2.931422302246094e+02, 2.93148095703125e+02, 2.931452941894531e+02, 2.9314453125e+02, 2.931453063964844e+02, 2.931523559570313e+02, 2.931512451171875e+02, 2.921061401367188e+02, 2.932062805175781e+02, 2.931635620117187e+02, 2.930996276855469e+02, 2.931445251464844e+02, 2.931529541015625e+02, 2.931467529296875e+02, 2.931463195800781e+02, 2.931401916503906e+02, 2.931448791503906e+02, 2.931481628417969e+02, 2.931456909179688e+02, 2.931497131347656e+02, 2.931717468261719e+02, 2.931677978515625e+02, 2.931574096679688e+02, 2.929947204589844e+02, 2.929675903320312e+02, 2.931598510742188e+02, 2.930356140136719e+02, 2.931483154296875e+02, 2.931512390136719e+02, 2.931463256835938e+02, 2.931496398925781e+02, 2.931450256347656e+02, 2.931466674804688e+02, 2.931465270996094e+02, 2.931481689453125e+02, 2.931563903808594e+02, 2.931296508789063e+02, 2.931705322265625e+02, 2.931882568359375e+02, 2.93135791015625e+02, 2.937101745605469e+02, 2.931428039550781e+02, 2.931470642089844e+02, 2.931428833007812e+02, 2.931418640136719e+02, 2.931496643066406e+02, 2.931432250976562e+02, 2.931478881835938e+02, 2.931449157714844e+02, 2.931734802246094e+02, 2.932702270507813e+02, 2.932194702148437e+02, 2.931085510253906e+02, 2.934374084472656e+02, 2.931758850097656e+02, 2.925652587890625e+02, 2.931372497558594e+02, 2.931415710449219e+02, 2.931428100585937e+02, 2.931434997558594e+02, 2.931406616210937e+02, 2.931445495605469e+02, 2.931371154785156e+02, 2.931534790039062e+02, 2.931725402832031e+02, 2.941346862792969e+02, 2.931924743652344e+02, 2.931701049804688e+02, 2.938579528808594e+02, 2.931154418945313e+02, 2.931359436035156e+02, 2.931460510253906e+02, 2.931474304199219e+02, 2.931450866699219e+02, 2.931465209960937e+02, 2.931467041015625e+02, 2.931476928710937e+02, 2.931481018066406e+02, 2.93150537109375e+02, 2.931482238769531e+02, 2.931499145507813e+02, 2.931501037597656e+02, 2.931523742675781e+02, 2.931496887207031e+02, 2.931495910644531e+02, 2.93150537109375e+02, 2.931531494140625e+02, 2.931556396484375e+02]
+genericAHU.genericAHUBus.TOdaMea=[3.031499938964844e+02, 2.816510437011719e+02, 2.812721008300781e+02, 2.810447387695312e+02, 2.806353942871094e+02, 2.806245727539062e+02, 2.813888671875e+02, 2.823677001953125e+02, 2.825362915039062e+02, 2.827453186035156e+02, 2.824911193847656e+02, 2.819651428222656e+02, 2.811151550292969e+02, 2.794293579101562e+02, 2.794889770507813e+02, 2.785244445800781e+02, 2.781871215820312e+02, 2.778995727539062e+02, 2.785819702148438e+02, 2.786313537597656e+02, 2.820504760742188e+02, 2.853292114257812e+02, 2.864217895507812e+02, 2.868355102539062e+02, 2.87213037109375e+02, 2.875488891601562e+02, 2.866647033691406e+02, 2.85530322265625e+02, 2.847202209472656e+02, 2.835629028320312e+02, 2.836711120605469e+02, 2.83335107421875e+02, 2.831687866210938e+02, 2.828631103515625e+02, 2.837184204101562e+02, 2.843091125488281e+02, 2.845592834472656e+02, 2.850676513671875e+02, 2.853401550292969e+02, 2.850943969726562e+02, 2.850019836425781e+02, 2.846758361816406e+02, 2.832384338378906e+02, 2.834480712890625e+02, 2.830691284179687e+02, 2.827716674804688e+02, 2.823108764648438e+02, 2.821388366699219e+02, 2.826403381347656e+02, 2.829925048828125e+02, 2.836463317871094e+02, 2.854063049316406e+02, 2.854196472167969e+02, 2.856457336425781e+02, 2.847413879394531e+02, 2.841886291503906e+02, 2.836947021484375e+02, 2.82323583984375e+02, 2.812730895996094e+02, 2.804439819335938e+02, 2.803667907714844e+02, 2.803451293945312e+02, 2.806056823730469e+02, 2.844159973144531e+02, 2.878858947753906e+02, 2.906085510253906e+02, 2.91112646484375e+02, 2.911349182128906e+02, 2.89287939453125e+02, 2.874098022460938e+02, 2.862945861816406e+02, 2.850127746582031e+02, 2.841727661132812e+02, 2.828424438476562e+02, 2.819891967773438e+02, 2.80355224609375e+02, 2.796067687988281e+02, 2.81635107421875e+02, 2.834853271484375e+02, 2.859810302734375e+02, 2.873733520507812e+02, 2.854789916992187e+02, 2.835642944335938e+02, 2.810159118652344e+02, 2.804072143554687e+02, 2.799130249023438e+02, 2.791451416015625e+02, 2.786036560058594e+02, 2.78099658203125e+02, 2.778919067382812e+02, 2.775111083984375e+02, 2.773408386230469e+02, 2.774520690917969e+02, 2.776192810058594e+02, 2.78026513671875e+02, 2.786343688964844e+02, 2.789421203613281e+02, 2.788549865722656e+02, 2.782231201171875e+02, 2.780323059082031e+02, 2.794450073242188e+02]
+genericAHU.genericAHUBus.heaterBus.hydraulicBus.valveSet=[0e+00, 4.353749930858612e-01, 4.389260828495026e-01, 4.417324483394623e-01, 4.44546240568161e-01, 4.462419152259827e-01, 4.409913957118988e-01, 4.309958875179291e-01, 4.287210881710052e-01, 4.296214699745178e-01, 4.315162599086761e-01, 4.358306348323822e-01, 4.424919962882995e-01, 4.535297989845276e-01, 4.554321706295014e-01, 4.616130888462067e-01, 4.642196297645569e-01, 4.67069810628891e-01, 4.649906098842621e-01, 4.523712992668152e-01, 5.981433391571045e-01, 5.182182550430298e-01, 3.897131383419037e-01, 5.016682386398316e-01, 4.30000239610672e-01, 3.724558353424072e-01, 3.9695925116539e-01, 4.078249037265778e-01, 4.135084748268127e-01, 4.25180983543396e-01, 4.256089925765991e-01, 4.287417471408844e-01, 4.325169086456299e-01, 4.219634473323822e-01, 4.093535721302032e-01, 5.763819217681885e-01, 4.082461893558502e-01, 5.547938466072082e-01, 5.160202503204345e-01, 3.978763103485107e-01, 4.126027822494507e-01, 4.167377293109894e-01, 4.283762633800506e-01, 4.281341671943665e-01, 4.316097915172577e-01, 4.347160160541534e-01, 4.39115959405899e-01, 4.412565290927887e-01, 4.179922342300415e-01, 6.051241755485535e-01, 5.467936992645264e-01, 4.673546135425568e-01, 5.130228161811828e-01, 4.384145379066468e-01, 4.129826486110687e-01, 4.188401699066162e-01, 4.228028237819672e-01, 4.342906534671783e-01, 4.437309861183166e-01, 4.484700560569763e-01, 4.500316679477692e-01, 4.501384377479553e-01, 4.37259715795517e-01, 5.771345853805542e-01, 4.544011235237121e-01, 3.392685353755951e-01, 1.881531178951263e-01, 8.703893721103668e-02, 3.438824355602265e-01, 3.772744297981262e-01, 3.894599080085754e-01, 4.008763551712036e-01, 4.084188997745514e-01, 4.184819400310517e-01, 4.263796389102936e-01, 4.376241266727448e-01, 4.313414990901947e-01, 4.103860318660736e-01, 5.424436569213867e-01, 3.802259087562561e-01, 4.57478791475296e-01, 4.35078102350235e-01, 3.856487691402435e-01, 4.223862588405609e-01, 4.298744082450867e-01, 4.352738857269287e-01, 4.410141527652741e-01, 4.460964202880859e-01, 4.50242692232132e-01, 4.523450791835785e-01, 4.537136852741241e-01, 4.543777704238892e-01, 4.557966649532318e-01, 4.569764077663422e-01, 4.582026302814484e-01, 4.568041861057281e-01, 4.55569738149643e-01, 4.57279235124588e-01, 4.612696826457977e-01, 4.632321655750274e-01, 4.577629268169403e-01]
+genericAHU.genericAHUBus.heaterBus.VFlowAirMea=[0e+00, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 7.301835417747498e-01, 5.449817538261413e-01, 1.840522557497025e-01, 7.11042070388794e-01, 3.58930641412735e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 7.112767696380615e-01, 1.839792758226395e-01, 7.446747422218323e-01, 5.359786629676819e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 7.118768811225891e-01, 5.360565185546875e-01, 3.598538041114807e-01, 5.230319380760193e-01, 1.670225977897644e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 7.275366663932801e-01, 5.39739453792572e-01, 3.63675057888031e-01, 7.059062957763672e-01, 3.598480343818665e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 5.278637528419494e-01, 1.840484768152237e-01, 7.397847771644592e-01, 3.954299688339233e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01, 1.666666716337204e-01]
+thermalZone.CO2Con=[4e+02, 4.200032592773438e+02, 4.345891845703125e+02, 4.420400817871094e+02, 4.458450256347656e+02, 4.477870178222656e+02, 4.487790954589844e+02, 4.492855712890625e+02, 4.49544140625e+02, 4.496761779785156e+02, 4.497435913085938e+02, 4.497779846191406e+02, 4.497955444335938e+02, 4.498045288085938e+02, 4.498091186523437e+02, 4.498114318847656e+02, 4.498126342773438e+02, 4.498132568359375e+02, 4.498135681152344e+02, 5.226792846679688e+02, 8.998889770507812e+02, 9.000609130859375e+02, 9e+02, 8.99948876953125e+02, 8.999955444335938e+02, 8.290685424804688e+02, 6.434911254882812e+02, 5.487060424804688e+02, 5.00308251953125e+02, 4.756022521972656e+02, 4.629825439453125e+02, 4.565390930175781e+02, 4.53247607421875e+02, 4.897243774414063e+02, 7.791283569335938e+02, 9.000065307617188e+02, 8.999966674804688e+02, 9.001863525390625e+02, 8.999999755859375e+02, 8.59250537109375e+02, 6.84522705078125e+02, 5.696478881835938e+02, 5.10993896484375e+02, 4.81053076171875e+02, 4.657656860351562e+02, 4.579599609375e+02, 4.539727966308594e+02, 4.519380859375e+02, 6.717307495117187e+02, 8.999711791992188e+02, 9e+02, 9.000000610351562e+02, 9.000001586914062e+02, 8.958544189453125e+02, 7.341894409179688e+02, 5.949932861328125e+02, 5.239372436523438e+02, 4.876567016601563e+02, 4.69137109375e+02, 4.596778076171875e+02, 4.548511352539062e+02, 4.523864990234375e+02, 5.681602905273437e+02, 9.000591674804688e+02, 9.000090087890625e+02, 9.00029052734375e+02, 8.999982055664062e+02, 8.999997924804687e+02, 7.94417529296875e+02, 6.2571728515625e+02, 5.396390380859375e+02, 4.957082885742187e+02, 4.732465515136719e+02, 4.617792297363281e+02, 4.559232482910156e+02, 4.529327392578125e+02, 5.077596740722656e+02, 8.57424853515625e+02, 9.00306396484375e+02, 8.999998291015625e+02, 8.999732666015625e+02, 8.99992578125e+02, 8.43434619140625e+02, 6.629959350585938e+02, 5.586784423828125e+02, 5.053997497558594e+02, 4.781988586425781e+02, 4.643093383789063e+02, 4.572218505859375e+02, 4.53594677734375e+02, 4.517444458007812e+02, 4.508002502441406e+02, 4.503176025390625e+02, 4.500711303710938e+02, 4.499452453613281e+02, 4.498809814453125e+02, 4.498481750488281e+02, 4.498314086914062e+02, 4.498228515625e+02, 4.498184448242188e+02, 4.498162231445312e+02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_GenericAHU.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_GenericAHU.txt
index 5676e3c614..452d0569e1 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_GenericAHU.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_GenericAHU.txt
@@ -1,4 +1,4 @@
-last-generated=2022-10-13
+last-generated=2024-07-25
 statistics-initialization=
 {
   "nonlinear": "0, 0, 0, 1, 0, 1, 0, 0, 3, 0, 3, 0, 3, 0",
@@ -13,9 +13,9 @@ statistics-simulation=
 }
 time=[0e+00, 7.2e+03]
 ctrAHUBasic.genericAHUBus.TOdaMea=[2.931499938964844e+02, 2.83256103515625e+02, 2.8315087890625e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02]
-ctrAHUBasic.genericAHUBus.TSupMea=[2.931499938964844e+02, 2.932666931152344e+02, 2.93436279296875e+02, 2.934192199707031e+02, 2.931875305175781e+02, 2.928282165527344e+02, 2.924723815917969e+02, 2.924530029296875e+02, 2.926907958984375e+02, 2.92909423828125e+02, 2.930338439941406e+02, 2.930841369628906e+02, 2.930950012207031e+02, 2.930905151367188e+02, 2.930831604003906e+02, 2.930778198242188e+02, 2.930756530761719e+02, 2.930762634277344e+02, 2.930789184570312e+02, 2.93082763671875e+02, 2.930872802734375e+02, 2.930920104980469e+02, 2.930967102050781e+02, 2.931012268066406e+02, 2.9310546875e+02, 2.931094055175781e+02, 2.93113037109375e+02, 2.931163635253906e+02, 2.93119384765625e+02, 2.931221313476562e+02, 2.931246643066406e+02, 2.931269226074219e+02, 2.931289978027344e+02, 2.931308898925781e+02, 2.931325988769531e+02, 2.931341552734375e+02, 2.931355895996094e+02, 2.931368713378906e+02, 2.931380615234375e+02, 2.931391296386719e+02, 2.931400756835938e+02, 2.931409606933594e+02, 2.931417846679688e+02, 2.931425170898438e+02, 2.931431579589844e+02, 2.931437683105469e+02, 2.931443176269531e+02, 2.931448364257812e+02, 2.931452941894531e+02, 2.931457214355469e+02, 2.931460876464844e+02, 2.931464233398438e+02, 2.931467590332031e+02, 2.931470336914062e+02, 2.931473083496094e+02, 2.931475524902344e+02, 2.931477661132812e+02, 2.9314794921875e+02, 2.931481323242188e+02, 2.931482849121094e+02, 2.931484375e+02, 2.931485900878906e+02, 2.931487121582031e+02, 2.931488342285156e+02, 2.9314892578125e+02, 2.931490173339844e+02, 2.931491088867188e+02, 2.931492004394531e+02, 2.931492614746094e+02, 2.931493225097656e+02, 2.931493835449219e+02, 2.931494445800781e+02, 2.931495056152344e+02, 2.931495361328125e+02, 2.931495666503906e+02, 2.931496276855469e+02, 2.93149658203125e+02, 2.931496887207031e+02, 2.931497192382812e+02, 2.931497192382812e+02, 2.931497497558594e+02, 2.931497802734375e+02, 2.931498107910156e+02, 2.931498107910156e+02, 2.931498413085938e+02, 2.931498413085938e+02, 2.931498718261719e+02, 2.931498718261719e+02, 2.931498718261719e+02, 2.9314990234375e+02, 2.9314990234375e+02, 2.9314990234375e+02, 2.931499328613281e+02, 2.931499328613281e+02, 2.931499328613281e+02, 2.931499328613281e+02, 2.931499328613281e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499633789062e+02]
+ctrAHUBasic.genericAHUBus.TSupMea=[2.931499938964844e+02, 2.933804321289062e+02, 2.935948791503906e+02, 2.93597412109375e+02, 2.933819274902344e+02, 2.930357666015625e+02, 2.926546020507812e+02, 2.924460144042969e+02, 2.926290893554688e+02, 2.92911865234375e+02, 2.931109619140625e+02, 2.932099304199219e+02, 2.932431335449219e+02, 2.93243408203125e+02, 2.932309875488281e+02, 2.932146911621094e+02, 2.931976928710938e+02, 2.93182373046875e+02, 2.931704406738281e+02, 2.931622009277344e+02, 2.931570434570312e+02, 2.931540222167969e+02, 2.931523132324219e+02, 2.931513977050781e+02, 2.931508483886719e+02, 2.931505126953125e+02, 2.931503295898438e+02, 2.931502075195312e+02, 2.931501159667969e+02, 2.931500854492188e+02, 2.931500549316406e+02, 2.931500244140625e+02, 2.931500244140625e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02]
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-ctrAHUBasic.genericAHUBus.TEhaMea=[2.931499938964844e+02, 2.92551025390625e+02, 2.910286865234375e+02, 2.897292785644531e+02, 2.888068237304688e+02, 2.881987915039062e+02, 2.878167419433594e+02, 2.875845031738281e+02, 2.874466857910156e+02, 2.873663024902344e+02, 2.873200378417969e+02, 2.87293701171875e+02, 2.8727880859375e+02, 2.872704467773438e+02, 2.872657775878906e+02, 2.8726318359375e+02, 2.872617492675781e+02, 2.872609558105469e+02, 2.872605285644531e+02, 2.872602844238281e+02, 2.872601623535156e+02, 2.872601013183594e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.87260009765625e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02, 2.872600402832031e+02]
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-ctrAHUBasic.genericAHUBus.coolerBus.hydraulicBus.valveMea=[0e+00, 7.029999438495156e-27, 3.50058134101542e-28, 1.753732247133019e-29, 8.808416454609906e-31, 4.38553050369115e-32, 2.182656257567893e-33, 1.087222645887075e-34, 5.30552351263113e-36, 2.509498651358404e-37, 3.993924550820328e-38, 8.154822781975129e-39, 1.791966463193933e-40, -8.238317749673459e-40, -1.734176914525185e-40, 1.047274420297795e-40, 4.689585440709433e-41, -3.71807922837768e-40, -1.243876594842567e-40, 5.242537814732006e-41, -2.844916142272244e-41, 8.947290694713957e-42, 8.35173884737591e-41, 1.987461611951888e-41, -9.552231241762981e-41, -1.698934258147408e-41, 4.102301254310902e-41, 1.394291972003181e-41, -1.99390758488779e-41, -1.178211748804306e-41, 7.845870101754651e-42, 9.209333507542698e-42, -2.122967173452098e-42, -2.380525831194999e-41, -5.279812353883046e-41, -7.065627116818593e-41, -4.777867243961896e-41, 1.148364091514188e-41, 4.730923745407015e-41, 2.130394055313019e-41, 6.364697624963319e-42, -1.747419185013047e-42, -1.908708638256833e-41, -1.509758965463558e-41, -2.505521654212773e-42, 5.530925038690053e-42, 7.966381769686585e-42, 9.434942560298993e-42, 1.922581493053649e-42, -4.393070685658302e-42, -3.40935916370228e-42, -3.962872057110583e-42, -1.56805298157947e-42, 4.21510578068905e-42, 1.176670320493553e-41, 1.751763210252455e-41, 1.552078179086161e-41, 7.599241572033483e-42, 4.763013480240053e-42, 1.534421818435675e-42, 4.848492686563867e-43, 2.480298281854926e-43, -2.916102104259944e-42, -4.789638151062225e-42, -3.884399343108393e-42, -1.56805298157947e-42, -3.152921544730838e-43, 9.34666075704653e-43, 1.223333559355565e-42, 1.318621854929653e-42, 2.090737308772627e-42, 2.239274945991058e-42, 1.339641331894525e-42, 7.006492321624085e-44, -8.407790785948902e-43, -1.432127030539963e-42, -1.104223189887956e-42, -6.516037859110399e-43, -5.563154903369524e-43, -3.321077360449816e-43, -6.445972935894159e-44, 2.802596928649634e-43, 6.27781712017518e-43, 7.637076630570253e-43, 4.638297916915145e-43, 1.471363387541058e-43, -5.324934164434305e-44, -2.087934711843977e-43, -1.793662034335766e-43, -2.284116496849452e-43, -3.671401976531021e-43, -5.002635517639597e-43, -6.249791150888684e-43, -7.440894845564779e-43, -8.646011524884121e-43, -1.003329700456569e-42, -1.18409720235447e-42, -1.156071233067974e-42, -9.739024327057479e-43, -6.572089797683392e-43, -1.793662034335766e-43]
-ctrAHUBasic.genericAHUBus.heaterBus.hydraulicBus.valveMea=[0e+00, 2.059059909242933e-07, 1.025306772817203e-08, 5.136614467105005e-10, 2.579951183245832e-11, 2.59646656922996e-03, 8.410798385739326e-03, 1.359828002750874e-02, 1.541061978787184e-02, 1.541553065180779e-02, 1.509681344032288e-02, 1.498161163181067e-02, 1.51224797591567e-02, 1.543798763304949e-02, 1.584309153258801e-02, 1.627932861447334e-02, 1.671280339360237e-02, 1.712609082460403e-02, 1.751141250133514e-02, 1.786637119948864e-02, 1.819122023880482e-02, 1.848744228482246e-02, 1.875706948339939e-02, 1.90022885799408e-02, 1.92252155393362e-02, 1.942784339189529e-02, 1.961204409599304e-02, 1.977954246103764e-02, 1.993188820779324e-02, 2.007047459483147e-02, 2.019656449556351e-02, 2.031130343675613e-02, 2.041573449969292e-02, 2.051079459488392e-02, 2.059733495116234e-02, 2.067612670361996e-02, 2.074788510799408e-02, 2.081324905157089e-02, 2.087277360260487e-02, 2.092698961496353e-02, 2.097637578845024e-02, 2.102136984467506e-02, 2.106235921382904e-02, 2.109971083700657e-02, 2.113374508917332e-02, 2.116475999355316e-02, 2.119302377104759e-02, 2.121878229081631e-02, 2.124225348234177e-02, 2.126364409923553e-02, 2.128313668072224e-02, 2.130090072751045e-02, 2.131709270179272e-02, 2.133184671401978e-02, 2.134529128670692e-02, 2.135753631591797e-02, 2.136868983507156e-02, 2.137884870171547e-02, 2.138810604810715e-02, 2.139654569327831e-02, 2.140424959361553e-02, 2.141127921640873e-02, 2.141767740249634e-02, 2.142350934445858e-02, 2.142882719635963e-02, 2.143367752432823e-02, 2.143809571862221e-02, 2.144212462007999e-02, 2.144579775631428e-02, 2.144914492964745e-02, 2.145219407975674e-02, 2.145497314631939e-02, 2.145750634372234e-02, 2.145981602370739e-02, 2.146191708743572e-02, 2.146383188664913e-02, 2.146557904779911e-02, 2.14671678841114e-02, 2.146861515939236e-02, 2.146993204951286e-02, 2.147113345563412e-02, 2.147222682833672e-02, 2.147321961820126e-02, 2.147412486374378e-02, 2.147495001554489e-02, 2.147569879889488e-02, 2.14763805270195e-02, 2.147700078785419e-02, 2.147756703197956e-02, 2.147808112204075e-02, 2.147854678332806e-02, 2.147896774113178e-02, 2.147934958338737e-02, 2.147969417273998e-02, 2.14800052344799e-02, 2.148028649389744e-02, 2.148053608834743e-02, 2.148076705634594e-02, 2.148097567260265e-02, 2.148116379976273e-02, 2.148133330047131e-02]
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+ctrAHUBasic.genericAHUBus.coolerBus.hydraulicBus.valveMea=[0e+00, 4.87638297459455e-27, 2.428189603465337e-28, 1.216473701372179e-29, 6.109849119754871e-31, 3.057478145030444e-32, 1.522150206273673e-33, 7.56756343779576e-35, 3.779620781710635e-36, 1.825884388055468e-37, 9.246629066170703e-39, 4.744586405434182e-40, 2.235631569983813e-41, 1.538625713828649e-42, 7.567011707353973e-44, 2.802596928649634e-44, -3.643376007244524e-44, -3.503246160812043e-44, 1.541428310757299e-44, -4.203895392974451e-45, 1.401298464324817e-45, 1.401298464324817e-45, -1.401298464324817e-45, 1.401298464324817e-45, -1.401298464324817e-45, 0e+00, 0e+00, 0e+00, 0e+00, -0e+00, 0e+00, 0e+00, -0e+00, 0e+00, 0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -0e+00, -0e+00, -0e+00, -0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, -0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
+ctrAHUBasic.genericAHUBus.heaterBus.hydraulicBus.valveMea=[0e+00, 1.055693132911983e-08, 5.256812207754535e-10, 2.633556393794034e-11, 1.322727517794053e-12, 5.846770945936441e-04, 5.080480128526688e-03, 1.093213818967343e-02, 1.391268149018288e-02, 1.383071299642324e-02, 1.267784368246794e-02, 1.151747442781925e-02, 1.063982024788857e-02, 1.0033312253654e-02, 9.619647637009621e-03, 9.338960982859135e-03, 9.165868163108826e-03, 9.075815789401531e-03, 9.038357064127922e-03, 9.026726707816124e-03, 9.024623781442642e-03, 9.024909697473049e-03, 9.025014936923981e-03, 9.024491533637047e-03, 9.023820050060749e-03, 9.023254737257957e-03, 9.022855199873447e-03, 9.022566489875317e-03, 9.022373706102371e-03, 9.022257290780544e-03, 9.022188372910023e-03, 9.022143669426441e-03, 9.02211107313633e-03, 9.022087790071964e-03, 9.022067300975323e-03, 9.022049605846405e-03, 9.02203656733036e-03, 9.022027254104614e-03, 9.022019803524017e-03, 9.022015146911144e-03, 9.02201235294342e-03, 9.022008627653122e-03, 9.022004902362823e-03, 9.021999314427376e-03, 9.021993726491928e-03, 9.02198813855648e-03, 9.021981619298458e-03, 9.021974168717861e-03, 9.021967649459839e-03, 9.021961130201817e-03, 9.021954610943794e-03, 9.021949023008347e-03, 9.021943435072899e-03, 9.021938778460026e-03, 9.021933190524578e-03, 9.021928533911705e-03, 9.021923877298832e-03, 9.021919220685959e-03, 9.021914564073086e-03, 9.021909907460213e-03, 9.02190525084734e-03, 9.021901525557041e-03, 9.021896868944168e-03, 9.021892212331295e-03, 9.021887555718422e-03, 9.021882899105549e-03, 9.021877311170101e-03, 9.021872654557228e-03, 9.02186706662178e-03, 9.021861478686333e-03, 9.021855890750885e-03, 9.021850302815437e-03, 9.021845646202564e-03, 9.021840058267117e-03, 9.021835401654243e-03, 9.02183074504137e-03, 9.021826088428497e-03, 9.021821431815624e-03, 9.021816775202751e-03, 9.021812118589878e-03, 9.021807461977005e-03, 9.021802805364132e-03, 9.021799080073833e-03, 9.02179442346096e-03, 9.021789766848087e-03, 9.021785110235214e-03, 9.021780453622341e-03, 9.021775797009468e-03, 9.021771140396595e-03, 9.021766483783722e-03, 9.021761827170849e-03, 9.02175810188055e-03, 9.021753445267677e-03, 9.021748788654804e-03, 9.021744132041931e-03, 9.021739475429058e-03, 9.021734818816185e-03, 9.021730162203312e-03, 9.021725505590439e-03, 9.021720848977566e-03, 9.021717123687267e-03]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_Heater.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_Heater.txt
new file mode 100644
index 0000000000..e15e493f31
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Examples_Heater.txt
@@ -0,0 +1,18 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "linear": "2, 59, 2",
+  "nonlinear": "0, 3, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
+  "nonlinear": "2",
+  "number of continuous time states": "70",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.6e+03]
+ctrBasic.registerBus.TAirInMea=[2.931499938964844e+02, 2.840595092773438e+02, 2.832325134277344e+02, 2.83157470703125e+02, 2.831506652832031e+02, 2.831500549316406e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02, 2.831499938964844e+02]
+ctrBasic.registerBus.TAirOutMea=[2.931499938964844e+02, 2.860477294921875e+02, 2.844830932617188e+02, 2.849703979492188e+02, 2.868435974121094e+02, 2.885881042480469e+02, 2.89514892578125e+02, 2.900386047363281e+02, 2.904998168945312e+02, 2.909453735351562e+02, 2.913321533203125e+02, 2.916411743164062e+02, 2.918876953125e+02, 2.920899047851562e+02, 2.922577514648438e+02, 2.923970642089844e+02, 2.925128784179688e+02, 2.926094970703125e+02, 2.926905212402344e+02, 2.927586669921875e+02, 2.928161926269531e+02, 2.928648376464844e+02, 2.929060974121094e+02, 2.929411926269531e+02, 2.929710388183594e+02, 2.929965209960938e+02, 2.930182800292969e+02, 2.93036865234375e+02, 2.930527954101562e+02, 2.930664367675781e+02, 2.930781555175781e+02, 2.930881958007812e+02, 2.930968017578125e+02, 2.931042175292969e+02, 2.93110595703125e+02, 2.931160888671875e+02, 2.931208190917969e+02, 2.931248779296875e+02, 2.931283569335938e+02, 2.9313134765625e+02, 2.931339111328125e+02, 2.931361694335938e+02, 2.931380615234375e+02, 2.931397399902344e+02, 2.931411437988281e+02, 2.931423645019531e+02, 2.931434326171875e+02, 2.931443176269531e+02, 2.931451110839844e+02, 2.931457824707031e+02, 2.931463623046875e+02, 2.931468811035156e+02, 2.931473083496094e+02, 2.931476745605469e+02, 2.931480102539062e+02, 2.931482849121094e+02, 2.931484985351562e+02, 2.931487121582031e+02, 2.931488952636719e+02, 2.931490478515625e+02, 2.93149169921875e+02, 2.931492919921875e+02, 2.931493835449219e+02, 2.931494750976562e+02, 2.931495666503906e+02, 2.931496276855469e+02, 2.93149658203125e+02, 2.931497192382812e+02, 2.931497497558594e+02, 2.931497802734375e+02, 2.931498107910156e+02, 2.931498413085938e+02, 2.931498718261719e+02, 2.931498718261719e+02, 2.9314990234375e+02, 2.9314990234375e+02, 2.931499328613281e+02, 2.931499328613281e+02, 2.931499328613281e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02]
+ctrBasic.registerBus.hydraulicBus.valveSet=[0e+00, 3.494245409965515e-01, 5.256073474884033e-01, 6.276180148124695e-01, 6.570575833320618e-01, 6.654150485992432e-01, 6.872996687889099e-01, 7.149211168289185e-01, 7.379586100578308e-01, 7.550886869430542e-01, 7.685712575912476e-01, 7.801552414894104e-01, 7.902421355247498e-01, 7.988734245300293e-01, 8.062137365341187e-01, 8.124842643737793e-01, 8.178587555885315e-01, 8.224705457687378e-01, 8.264287114143372e-01, 8.298268914222717e-01, 8.327468037605286e-01, 8.35256814956665e-01, 8.374144434928894e-01, 8.39270293712616e-01, 8.408676385879517e-01, 8.422420024871826e-01, 8.434247374534607e-01, 8.444433808326721e-01, 8.453206419944763e-01, 8.460757732391357e-01, 8.467262387275696e-01, 8.472869396209717e-01, 8.47770094871521e-01, 8.481862545013428e-01, 8.485446572303772e-01, 8.488531708717346e-01, 8.491191267967224e-01, 8.493485450744629e-01, 8.495464324951172e-01, 8.497169613838196e-01, 8.498637676239014e-01, 8.499900698661804e-01, 8.500989079475403e-01, 8.501927852630615e-01, 8.502738475799561e-01, 8.50343644618988e-01, 8.504037261009216e-01, 8.504554033279419e-01, 8.504999279975891e-01, 8.505383729934692e-01, 8.505716919898987e-01, 8.506004214286804e-01, 8.506250977516174e-01, 8.506461977958679e-01, 8.506643772125244e-01, 8.506801724433899e-01, 8.506938815116882e-01, 8.507057428359985e-01, 8.507159948348999e-01, 8.507248163223267e-01, 8.507323861122131e-01, 8.507388830184937e-01, 8.507444262504578e-01, 8.50749135017395e-01, 8.507531881332397e-01, 8.507567048072815e-01, 8.507598638534546e-01, 8.507625460624695e-01, 8.507649302482605e-01, 8.507669568061829e-01, 8.507686853408813e-01, 8.50770115852356e-01, 8.507713079452515e-01, 8.507723808288574e-01, 8.507732152938843e-01, 8.507739901542664e-01, 8.507746458053589e-01, 8.507752418518066e-01, 8.507757782936096e-01, 8.507762551307678e-01, 8.507766127586365e-01, 8.507769107818604e-01, 8.507771492004395e-01, 8.507773280143738e-01, 8.507774472236633e-01, 8.507776260375977e-01, 8.50777804851532e-01, 8.507779836654663e-01, 8.507781028747559e-01, 8.507782220840454e-01, 8.50778341293335e-01, 8.507784008979797e-01, 8.507784008979797e-01, 8.507784605026245e-01, 8.507784605026245e-01, 8.507785201072693e-01, 8.507785201072693e-01, 8.507785797119141e-01, 8.507786393165588e-01, 8.507786393165588e-01, 8.507786989212036e-01]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Cooler.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Cooler.txt
new file mode 100644
index 0000000000..59bd9fd5e0
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Cooler.txt
@@ -0,0 +1,26 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "3, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0",
+  "nonlinear": "2, 1, 1, 1, 1, 1, 1",
+  "number of continuous time states": "62",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 2.7e+03]
+registerModule.registerBus.TAirInMea=[2.936499938964844e+02, 2.944480285644531e+02, 2.952676086425781e+02, 2.96085205078125e+02, 2.968776245117188e+02, 2.976463012695312e+02, 2.983805541992188e+02, 2.99074462890625e+02, 2.997355041503906e+02, 3.003439636230469e+02, 3.009241027832031e+02, 3.014602661132812e+02, 3.019753723144531e+02, 3.024494323730469e+02, 3.028904418945312e+02, 3.032985534667969e+02, 3.036838989257812e+02, 3.040399780273438e+02, 3.043752136230469e+02, 3.046864318847656e+02, 3.049853820800781e+02, 3.052636413574219e+02, 3.055229187011719e+02, 3.057688903808594e+02, 3.060007934570312e+02, 3.062103881835938e+02, 3.063927001953125e+02, 3.065473327636719e+02, 3.066889343261719e+02, 3.068114624023438e+02, 3.069253845214844e+02, 3.07029296875e+02, 3.071211242675781e+02, 3.072143859863281e+02, 3.073046875e+02, 3.0738623046875e+02, 3.074523010253906e+02, 3.075103454589844e+02, 3.075734252929688e+02, 3.076388244628906e+02, 3.077059326171875e+02, 3.0776904296875e+02, 3.078240356445312e+02, 3.078670654296875e+02, 3.078916931152344e+02, 3.0789111328125e+02, 3.078703918457031e+02, 3.078473510742188e+02, 3.078283386230469e+02, 3.078198852539062e+02, 3.078257141113281e+02, 3.0784130859375e+02, 3.078588562011719e+02, 3.078689270019531e+02, 3.078612060546875e+02, 3.078359680175781e+02, 3.078094787597656e+02, 3.077905578613281e+02, 3.077819519042969e+02, 3.077730102539062e+02, 3.077566528320312e+02, 3.077353210449219e+02, 3.077147827148438e+02, 3.0768798828125e+02, 3.076477661132812e+02, 3.075938110351562e+02, 3.075341186523438e+02, 3.074731750488281e+02, 3.074212341308594e+02, 3.073898620605469e+02, 3.073850402832031e+02, 3.074035949707031e+02, 3.074239196777344e+02, 3.074326782226562e+02, 3.074338073730469e+02, 3.074334411621094e+02, 3.074185791015625e+02, 3.073830261230469e+02, 3.073384094238281e+02, 3.072871398925781e+02, 3.072327575683594e+02, 3.071730041503906e+02, 3.071109619140625e+02, 3.070484008789062e+02, 3.069862670898438e+02, 3.069236450195312e+02, 3.06859619140625e+02, 3.068023376464844e+02, 3.067530517578125e+02, 3.067050170898438e+02, 3.066617431640625e+02, 3.06625e+02, 3.065984191894531e+02, 3.065780944824219e+02, 3.065611572265625e+02, 3.065442810058594e+02, 3.0653125e+02, 3.065216369628906e+02, 3.065160522460938e+02, 3.065094299316406e+02, 3.065018005371094e+02]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Heater.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Heater.txt
new file mode 100644
index 0000000000..7aa29a5d75
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Heater.txt
@@ -0,0 +1,26 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "3, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0",
+  "nonlinear": "2, 1, 1, 1, 1, 1, 1",
+  "number of continuous time states": "62",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 4.32e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Preheater.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Preheater.txt
new file mode 100644
index 0000000000..50597633bd
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Systems_ModularAHU_Validation_AHU2_Preheater.txt
@@ -0,0 +1,26 @@
+last-generated=2024-07-24
+statistics-initialization=
+{
+  "nonlinear": "3, 0",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "0, 0, 0, 0, 0, 0",
+  "nonlinear": "2, 1, 1, 1, 1, 1, 1",
+  "number of continuous time states": "66",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 7.2e+03]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Examples_OFDHeatLoad.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Examples_OFDHeatLoad.txt
index 3e459e9728..58d420aeab 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Examples_OFDHeatLoad.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Examples_OFDHeatLoad.txt
@@ -7,7 +7,7 @@ statistics-initialization=
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,   0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
-  "nonlinear": "5, 9, 5, 8, 5, 7, 5, 8, 5, 7, 5, 8, 5, 9, 5, 8, 5, 9, 5, 8, 10",
+  "nonlinear": "4, 9, 4, 8, 4, 7, 4, 8, 4, 7, 4, 8, 4, 9, 4, 8, 4, 9, 4, 8, 10",
   "number of continuous time states": "251",
   "numerical Jacobians": "0"
 }
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case210.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case210.txt
index 24445ced09..82f35ebbd3 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case210.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case210.txt
@@ -1,4 +1,4 @@
-last-generated=2022-07-06
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,13 +8,13 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAEHeatingOrTempMax.lowerLimit=[6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03, 6.456e+03]
-AnnualHeatingLoad=[0e+00, 2.072945153808594e+02, 3.456739978027344e+02, 4.472299206542968e+02, 5.6456294921875e+02, 6.928199645996094e+02, 8.661484960937501e+02, 9.670370629882813e+02, 1.095395107421875e+03, 1.238005085449219e+03, 1.415879711914062e+03, 1.5510164453125e+03, 1.642815952148437e+03, 1.789832041015625e+03, 1.928484921875e+03, 2.062509790039062e+03, 2.166970986328125e+03, 2.298949560546875e+03, 2.44203869140625e+03, 2.562404560546875e+03, 2.64721708984375e+03, 2.753580971679688e+03, 2.8516298828125e+03, 2.953412661132812e+03, 3.0142398046875e+03, 3.073531127929688e+03, 3.1812435546875e+03, 3.249796586914063e+03, 3.320664228515625e+03, 3.419539677734375e+03, 3.4657056640625e+03, 3.515920356445312e+03, 3.537368408203125e+03, 3.60675021484375e+03, 3.6616890625e+03, 3.720703857421875e+03, 3.77892595703125e+03, 3.820805747070312e+03, 3.83617626953125e+03, 3.865548735351562e+03, 3.885744535385884e+03, 3.9208310546875e+03, 3.9483782421875e+03, 3.963972287557041e+03, 4.0067916015625e+03, 4.036176025390625e+03, 4.056240087890625e+03, 4.0781787109375e+03, 4.093774169921875e+03, 4.101822265625e+03, 4.1059375e+03, 4.123328154296875e+03, 4.13505419921875e+03, 4.1380166015625e+03, 4.14451419921875e+03, 4.1508369140625e+03, 4.1531416015625e+03, 4.15534375e+03, 4.15759765625e+03, 4.15918701171875e+03, 4.164898121083092e+03, 4.1777392578125e+03, 4.187983046875e+03, 4.1912744140625e+03, 4.20755419921875e+03, 4.223548291015625e+03, 4.22839306640625e+03, 4.232259765625e+03, 4.24893318359375e+03, 4.25866064453125e+03, 4.28477685546875e+03, 4.31216125e+03, 4.3515439453125e+03, 4.39396166015625e+03, 4.44033140625e+03, 4.4833017578125e+03, 4.547461484375e+03, 4.595531337890625e+03, 4.6602826953125e+03, 4.71548646484375e+03, 4.76851259765625e+03, 4.821610673828125e+03, 4.89399203125e+03, 4.99475998046875e+03, 5.11385673828125e+03, 5.212416162109375e+03, 5.29535015625e+03, 5.4064671875e+03, 5.51377173828125e+03, 5.614054462890625e+03, 5.737233189174107e+03, 5.833771240234375e+03, 5.93496455078125e+03, 6.071136259765625e+03, 6.2463415234375e+03, 6.39224638671875e+03, 6.5513843359375e+03, 6.649684833984375e+03, 6.74195576171875e+03, 6.846482080078125e+03, 6.97142919921875e+03]
+AnnualHeatingLoad=[0e+00, 2.072945153808594e+02, 3.456739978027344e+02, 4.472299206542968e+02, 5.6456294921875e+02, 6.928199645996094e+02, 8.661484960937501e+02, 9.670370629882813e+02, 1.095395107421875e+03, 1.238005085449219e+03, 1.415879711914062e+03, 1.5510164453125e+03, 1.642815952148437e+03, 1.789832041015625e+03, 1.928484921875e+03, 2.062509790039062e+03, 2.166970869140625e+03, 2.29894931640625e+03, 2.442038447265625e+03, 2.562404516601563e+03, 2.64721708984375e+03, 2.753581123046875e+03, 2.851630087890625e+03, 2.953412661132812e+03, 3.014240048828125e+03, 3.07353076171875e+03, 3.181243134765625e+03, 3.249796342773438e+03, 3.320663740234375e+03, 3.419539189453125e+03, 3.465704931640625e+03, 3.515919868164062e+03, 3.537367919921875e+03, 3.606749790039063e+03, 3.66168857421875e+03, 3.720703369140625e+03, 3.778925244140625e+03, 3.820805258789062e+03, 3.836174560546875e+03, 3.86554712890625e+03, 3.885742826401509e+03, 3.92082958984375e+03, 3.948376533203125e+03, 3.963970578572666e+03, 4.006789404296875e+03, 4.036174072265625e+03, 4.05623810546875e+03, 4.0781767578125e+03, 4.09377197265625e+03, 4.1018203125e+03, 4.105935546875e+03, 4.123326201171875e+03, 4.13505224609375e+03, 4.13801416015625e+03, 4.14451224609375e+03, 4.1508349609375e+03, 4.1531396484375e+03, 4.155341796875e+03, 4.157595703125e+03, 4.15918505859375e+03, 4.164896167958092e+03, 4.1777373046875e+03, 4.18798109375e+03, 4.1912724609375e+03, 4.20755224609375e+03, 4.223546337890625e+03, 4.22839111328125e+03, 4.2322578125e+03, 4.24893123046875e+03, 4.25865869140625e+03, 4.28477490234375e+03, 4.312159296875e+03, 4.3515419921875e+03, 4.39395970703125e+03, 4.440329453125e+03, 4.4832998046875e+03, 4.5474598828125e+03, 4.5955294140625e+03, 4.66028115234375e+03, 4.715484814453125e+03, 4.7685111328125e+03, 4.821609208984375e+03, 4.89399056640625e+03, 4.994758515625e+03, 5.1138550390625e+03, 5.21241435546875e+03, 5.29534869140625e+03, 5.4064662109375e+03, 5.5137702734375e+03, 5.614053486328125e+03, 5.737231724330357e+03, 5.833769775390625e+03, 5.9349630859375e+03, 6.071134794921875e+03, 6.24634005859375e+03, 6.392244921875e+03, 6.55138287109375e+03, 6.64968353515625e+03, 6.741954296875e+03, 6.846480615234375e+03, 6.971427734375e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.upperLimit=[6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03, 6.967e+03]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02, -6.68e+02]
-AnnualCoolingLoad=[0e+00, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -1.122336834669113e-01, -3.439573764801025e+00, -5.350968837738037e+00, -5.350968837738037e+00, -5.350968837738037e+00, -5.52509880065918e+00, -5.52509880065918e+00, -6.411886692047119e+00, -7.480137825012207e+00, -1.614482502821015e+01, -1.614720726013184e+01, -1.725870895385742e+01, -1.739229393005371e+01, -1.739642906188965e+01, -2.212619018554688e+01, -3.358353515625e+01, -4.137648010253906e+01, -5.077560424804688e+01, -5.09579222869873e+01, -5.937957000732422e+01, -7.339310455322266e+01, -7.67874755859375e+01, -8.644706802368164e+01, -9.374903869628906e+01, -1.008560256958008e+02, -1.139522247314453e+02, -1.419720022583008e+02, -1.779326477050781e+02, -1.883226776123047e+02, -2.051777941894531e+02, -2.242893350219726e+02, -2.463250579833984e+02, -2.734994110107422e+02, -3.073361096191406e+02, -3.463339874267578e+02, -3.804419799804688e+02, -3.976769744873047e+02, -4.217657775878906e+02, -4.350347686767578e+02, -4.500419616699219e+02, -4.842037744140625e+02, -4.897124377441406e+02, -5.017265319824219e+02, -5.331839990234375e+02, -5.566427136230469e+02, -5.780570678710938e+02, -6.050080346679688e+02, -6.08532470703125e+02, -6.144929809570312e+02, -6.229655151367188e+02, -6.252633666992188e+02, -6.315123291015625e+02, -6.4000390625e+02, -6.42372802734375e+02, -6.471512451171875e+02, -6.480831298828125e+02, -6.4998583984375e+02, -6.563046264648438e+02, -6.58427978515625e+02, -6.585819702148438e+02, -6.585819702148438e+02, -6.585819702148438e+02, -6.585819702148438e+02, -6.585819702148438e+02, -6.585819702148438e+02, -6.585819702148438e+02, -6.585819702148438e+02, -6.585819702148438e+02, -6.588099365234375e+02, -6.588099365234375e+02, -6.588099365234375e+02, -6.588099365234375e+02, -6.588099365234375e+02, -6.588099365234375e+02, -6.588099365234375e+02, -6.588099365234375e+02, -6.588099365234375e+02, -6.588099365234375e+02]
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 checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[-1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02, -1.62e+02]
 checkResultsAccordingToASHRAEHeatingOrTempMax.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
 checkResultsAccordingToASHRAECoolingOrTempMin.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
 Room.thermRoom.T=[2.941499938964844e+02, 2.930499572753906e+02, 2.930499877929688e+02, 2.930499774169922e+02, 2.930499914550781e+02, 2.930499908447266e+02, 2.930499572753906e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.93050048828125e+02, 2.930499749755859e+02, 2.930499572753906e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.930499786376953e+02, 2.930500646972656e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930500183105469e+02, 2.930500164794922e+02, 2.930500183105469e+02, 2.930500335693359e+02, 2.930499877929688e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.930500183105469e+02, 2.930499572753906e+02, 2.931499633789062e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.931499725341797e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.931499938964844e+02, 2.93050048828125e+02, 2.930499850537171e+02, 2.93150023803711e+02, 2.93050048828125e+02, 2.93050012105494e+02, 2.930500183105469e+02, 2.931499938964844e+02, 2.930499877929688e+02, 2.931386173875299e+02, 2.930500048828125e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.93049994506836e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.930499877929688e+02, 2.931499633789062e+02, 2.931500451660156e+02, 2.931499774169922e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.930499877929688e+02, 2.9314990234375e+02, 2.93050048828125e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.93050048828125e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.930499877929688e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930500793457031e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.930500793457031e+02, 2.930500061035156e+02, 2.930499932861328e+02, 2.9305001953125e+02, 2.930499877929688e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930499700927734e+02, 2.930500215328998e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930500183105469e+02, 2.930499975585938e+02, 2.930499877929688e+02, 2.930500793457031e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.93050103149414e+02, 2.930499877929688e+02]
-Room.starRoom.T=[2.875967712402344e+02, 2.852758868408203e+02, 2.874619873046875e+02, 2.880939379882813e+02, 2.873018237304688e+02, 2.878247497558594e+02, 2.873042419433594e+02, 2.8833423828125e+02, 2.862878186035156e+02, 2.884177624511719e+02, 2.878858093261719e+02, 2.881799957275391e+02, 2.901536779785156e+02, 2.87212314453125e+02, 2.873885827636719e+02, 2.911388427734375e+02, 2.900407971191406e+02, 2.879688555908203e+02, 2.87681943359375e+02, 2.890208996582031e+02, 2.884875732421875e+02, 2.884977844238281e+02, 2.8769083984375e+02, 2.898796746826172e+02, 2.917958068847656e+02, 2.897962036132812e+02, 2.892560510253906e+02, 2.931156481933594e+02, 2.883018615722656e+02, 2.905329278564453e+02, 2.908593444824219e+02, 2.901405297851563e+02, 2.9296062041492e+02, 2.903031072998047e+02, 2.906805871582031e+02, 2.930369537353516e+02, 2.909181823730469e+02, 2.911156451416016e+02, 2.932716955566406e+02, 2.915373907470703e+02, 2.914066083018307e+02, 2.937351843261719e+02, 2.917318957519531e+02, 2.925554510599584e+02, 2.903329675292969e+02, 2.935151245117187e+02, 2.91102158203125e+02, 2.932981330747137e+02, 2.917342211914063e+02, 2.935734442138672e+02, 2.96608154296875e+02, 2.913393634033203e+02, 2.956720788574219e+02, 2.941462023925781e+02, 2.918596789550782e+02, 2.960479888916016e+02, 2.951302819824219e+02, 2.935190325927734e+02, 2.955852624511719e+02, 2.939150189208984e+02, 2.921358120906564e+02, 2.942664617919922e+02, 2.929643566894531e+02, 2.932825946044922e+02, 2.942904919433594e+02, 2.923388580322265e+02, 2.943480310058594e+02, 2.961890161132812e+02, 2.913203698730469e+02, 2.940015118408203e+02, 2.951195678710938e+02, 2.902300439453125e+02, 2.921978625488281e+02, 2.920310888671875e+02, 2.898207434082031e+02, 2.889718627929688e+02, 2.922028759765625e+02, 2.891967846679688e+02, 2.924012707519531e+02, 2.910114379882813e+02, 2.899469055175781e+02, 2.920475598144531e+02, 2.899107629394532e+02, 2.883421862792969e+02, 2.887763073730468e+02, 2.888184539794922e+02, 2.888555981445313e+02, 2.885231396484375e+02, 2.876802038574219e+02, 2.897154595947266e+02, 2.931877299243619e+02, 2.906510479736328e+02, 2.874745080566406e+02, 2.886516094970703e+02, 2.878699206542969e+02, 2.878377197265625e+02, 2.886688024902344e+02, 2.877155187988281e+02, 2.89783720703125e+02, 2.876301477050781e+02, 2.880650939941406e+02]
+Room.starRoom.T=[2.875967712402344e+02, 2.852758868408203e+02, 2.874619873046875e+02, 2.880939379882813e+02, 2.873018237304688e+02, 2.878247497558594e+02, 2.873042419433594e+02, 2.8833423828125e+02, 2.862878186035156e+02, 2.884177624511719e+02, 2.878858093261719e+02, 2.881799957275391e+02, 2.901536779785156e+02, 2.87212314453125e+02, 2.873885827636719e+02, 2.911388427734375e+02, 2.900407971191406e+02, 2.879688555908203e+02, 2.876819128417969e+02, 2.890208996582031e+02, 2.884875732421875e+02, 2.884977844238281e+02, 2.8769083984375e+02, 2.898796746826172e+02, 2.917958068847656e+02, 2.897962036132812e+02, 2.892560510253906e+02, 2.931156481933594e+02, 2.883018615722656e+02, 2.905329278564453e+02, 2.90859326171875e+02, 2.901405297851563e+02, 2.9296062041492e+02, 2.903031072998047e+02, 2.906805871582031e+02, 2.930369537353516e+02, 2.909181823730469e+02, 2.911156451416016e+02, 2.932716955566406e+02, 2.915373907470703e+02, 2.914066083018307e+02, 2.937351843261719e+02, 2.917318957519531e+02, 2.925554510599584e+02, 2.903329675292969e+02, 2.935151245117187e+02, 2.91102158203125e+02, 2.932981330747137e+02, 2.917342211914063e+02, 2.935734442138672e+02, 2.96608154296875e+02, 2.913393634033203e+02, 2.95672109375e+02, 2.941462023925781e+02, 2.918596789550782e+02, 2.960479888916016e+02, 2.951302819824219e+02, 2.935190325927734e+02, 2.955852624511719e+02, 2.939150189208984e+02, 2.921358120906564e+02, 2.942664617919922e+02, 2.929643566894531e+02, 2.932825946044922e+02, 2.942904919433594e+02, 2.923388580322265e+02, 2.943480310058594e+02, 2.961890161132812e+02, 2.913203698730469e+02, 2.940015118408203e+02, 2.951195678710938e+02, 2.902300439453125e+02, 2.921978576660156e+02, 2.920310888671875e+02, 2.898207214355469e+02, 2.889718627929688e+02, 2.922028759765625e+02, 2.891967846679688e+02, 2.924012707519531e+02, 2.910114263916016e+02, 2.899469055175781e+02, 2.920475598144531e+02, 2.899107629394532e+02, 2.883421862792969e+02, 2.887763073730468e+02, 2.888184326171875e+02, 2.888555981445313e+02, 2.885231396484375e+02, 2.876802038574219e+02, 2.897154772949219e+02, 2.931877299243619e+02, 2.906510479736328e+02, 2.874745080566406e+02, 2.886516094970703e+02, 2.878699206542969e+02, 2.878377197265625e+02, 2.886688024902344e+02, 2.877155187988281e+02, 2.89783720703125e+02, 2.876301477050781e+02, 2.880650939941406e+02]
 TransmittedSolarRadiation_room=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case220.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case220.txt
index 8e9c7a6058..c95e9576b2 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case220.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case220.txt
@@ -1,4 +1,4 @@
-last-generated=2022-07-06
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,13 +8,13 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAEHeatingOrTempMax.lowerLimit=[6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03, 6.944e+03]
-AnnualHeatingLoad=[0e+00, 2.137208517456055e+02, 3.570928637695313e+02, 4.625357537841797e+02, 5.84133828125e+02, 7.170767700195313e+02, 8.963080468749999e+02, 1.001054970703125e+03, 1.134040219726563e+03, 1.281758051757813e+03, 1.465471557617188e+03, 1.605409873046875e+03, 1.700832319335937e+03, 1.8527978125e+03, 1.996418745117187e+03, 2.135362548828125e+03, 2.243664755859375e+03, 2.38023349609375e+03, 2.528331611328125e+03, 2.652966303710938e+03, 2.74104677734375e+03, 2.851487270507812e+03, 2.953152001953125e+03, 3.058717900390625e+03, 3.121816748046875e+03, 3.1833720703125e+03, 3.295155048828125e+03, 3.36653912109375e+03, 3.44008623046875e+03, 3.542797182617187e+03, 3.590831787109375e+03, 3.64308408203125e+03, 3.665386962890625e+03, 3.737438935546875e+03, 3.79456775390625e+03, 3.8560537109375e+03, 3.91657732421875e+03, 3.96016681640625e+03, 3.97613623046875e+03, 4.006591826171875e+03, 4.027543388511378e+03, 4.06419189453125e+03, 4.09277900390625e+03, 4.10897314453125e+03, 4.153458359375e+03, 4.1840908203125e+03, 4.2049436328125e+03, 4.2277783203125e+03, 4.2439243359375e+03, 4.252228515625e+03, 4.25642919921875e+03, 4.274504404296875e+03, 4.28671728515625e+03, 4.289771484375e+03, 4.29645921875e+03, 4.30297705078125e+03, 4.30531298828125e+03, 4.30757763671875e+03, 4.30989013671875e+03, 4.31152294921875e+03, 4.317369844069747e+03, 4.330763671875e+03, 4.3413841796875e+03, 4.34475390625e+03, 4.361673828125e+03, 4.37822529296875e+03, 4.383212890625e+03, 4.38717529296875e+03, 4.404323046875e+03, 4.414349609375e+03, 4.44145751953125e+03, 4.46985576171875e+03, 4.51078947265625e+03, 4.554768349609375e+03, 4.60287826171875e+03, 4.647316162109375e+03, 4.7139035546875e+03, 4.7636677734375e+03, 4.83100279296875e+03, 4.888223193359375e+03, 4.94309794921875e+03, 4.99825708984375e+03, 5.0733490234375e+03, 5.17780609375e+03, 5.3010703125e+03, 5.40315361328125e+03, 5.4893051171875e+03, 5.6044330078125e+03, 5.7156987109375e+03, 5.81980080078125e+03, 5.9473185546875e+03, 6.04722271484375e+03, 6.15200275390625e+03, 6.29295126953125e+03, 6.4739084765625e+03, 6.62488447265625e+03, 6.78935822265625e+03, 6.89140375e+03, 6.9872108203125e+03, 7.095428984375e+03, 7.2249052734375e+03]
+AnnualHeatingLoad=[0e+00, 2.137208517456055e+02, 3.570928637695313e+02, 4.625357537841797e+02, 5.84133828125e+02, 7.170767700195313e+02, 8.963080468749999e+02, 1.001054970703125e+03, 1.134040219726563e+03, 1.281758051757813e+03, 1.465471557617188e+03, 1.605409873046875e+03, 1.700832319335937e+03, 1.8527978125e+03, 1.996418745117187e+03, 2.135362548828125e+03, 2.243664755859375e+03, 2.38023349609375e+03, 2.528331611328125e+03, 2.652966303710938e+03, 2.74104677734375e+03, 2.851487270507812e+03, 2.953152001953125e+03, 3.058717900390625e+03, 3.121816748046875e+03, 3.1833720703125e+03, 3.295155048828125e+03, 3.36653912109375e+03, 3.44008623046875e+03, 3.542797182617187e+03, 3.590831787109375e+03, 3.64308408203125e+03, 3.665386962890625e+03, 3.737438935546875e+03, 3.79456775390625e+03, 3.8560537109375e+03, 3.91657732421875e+03, 3.96016681640625e+03, 3.97613623046875e+03, 4.006591826171875e+03, 4.027543388511378e+03, 4.06419189453125e+03, 4.09277900390625e+03, 4.10897314453125e+03, 4.153458359375e+03, 4.1840908203125e+03, 4.2049436328125e+03, 4.2277783203125e+03, 4.2439243359375e+03, 4.252228515625e+03, 4.25642919921875e+03, 4.274504404296875e+03, 4.28671728515625e+03, 4.289771484375e+03, 4.29645921875e+03, 4.30297705078125e+03, 4.30531298828125e+03, 4.30757763671875e+03, 4.30989013671875e+03, 4.31152294921875e+03, 4.317369844069747e+03, 4.33076416015625e+03, 4.3413838671875e+03, 4.34475390625e+03, 4.361673828125e+03, 4.37822529296875e+03, 4.383212890625e+03, 4.38717529296875e+03, 4.40432306640625e+03, 4.414349609375e+03, 4.44145751953125e+03, 4.46985576171875e+03, 4.51078947265625e+03, 4.554767890625e+03, 4.60287826171875e+03, 4.64731591796875e+03, 4.7139035546875e+03, 4.76366728515625e+03, 4.8310023828125e+03, 4.888223193359375e+03, 4.94309521484375e+03, 4.998254248046875e+03, 5.07334658203125e+03, 5.17780365234375e+03, 5.30106787109375e+03, 5.403151171875e+03, 5.48930267578125e+03, 5.60443056640625e+03, 5.71569626953125e+03, 5.819798359375e+03, 5.94731611328125e+03, 6.04722076171875e+03, 6.152001171875e+03, 6.292949580078125e+03, 6.47390685546875e+03, 6.6248830078125e+03, 6.78935669921875e+03, 6.89140228515625e+03, 6.987209140625e+03, 7.09542703125e+03, 7.2249033203125e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.upperLimit=[8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03, 8.787e+03]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02, -8.35e+02]
-AnnualCoolingLoad=[0e+00, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -3.458089828491211e+00, -5.352277755737305e+00, -5.352277755737305e+00, -5.352277755737305e+00, -5.500625610351562e+00, -5.500625610351562e+00, -6.387824058532715e+00, -7.459638595581055e+00, -1.631673468686222e+01, -1.632031440734863e+01, -1.741679954528809e+01, -1.752539958953857e+01, -1.752933120727539e+01, -2.235028266906738e+01, -3.411346160888672e+01, -4.214949035644531e+01, -5.174369812011719e+01, -5.190860656738281e+01, -6.05566520690918e+01, -7.497373962402344e+01, -7.846428680419922e+01, -8.843743896484375e+01, -9.594685363769531e+01, -1.032265319824219e+02, -1.167155838012695e+02, -1.456850628662109e+02, -1.828849945068359e+02, -1.936869812011719e+02, -2.109842626953125e+02, -2.309005221557617e+02, -2.536859283447266e+02, -2.816975250244141e+02, -3.168697814941406e+02, -3.573291595458984e+02, -3.926827685546875e+02, -4.106820843505859e+02, -4.355733947753906e+02, -4.492047973632813e+02, -4.648028869628906e+02, -5.001869061279297e+02, -5.0576162109375e+02, -5.181173095703125e+02, -5.50651806640625e+02, -5.749521545410156e+02, -5.970709838867188e+02, -6.248659692382812e+02, -6.284072631835937e+02, -6.345343627929688e+02, -6.43205078125e+02, -6.455068969726562e+02, -6.519122314453125e+02, -6.605376586914062e+02, -6.62873779296875e+02, -6.67686767578125e+02, -6.686028442382812e+02, -6.704877319335938e+02, -6.76827880859375e+02, -6.789241943359375e+02, -6.790614013671875e+02, -6.790614013671875e+02, -6.790614013671875e+02, -6.790614013671875e+02, -6.790614013671875e+02, -6.790614013671875e+02, -6.790614013671875e+02, -6.790614013671875e+02, -6.790614013671875e+02, -6.79267578125e+02, -6.79267578125e+02, -6.79267578125e+02, -6.79267578125e+02, -6.79267578125e+02, -6.79267578125e+02, -6.79267578125e+02, -6.79267578125e+02, -6.79267578125e+02, -6.79267578125e+02]
+AnnualCoolingLoad=[0e+00, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -1.12454429268837e-01, -3.458089828491211e+00, -5.352277755737305e+00, -5.352277755737305e+00, -5.352277755737305e+00, -5.500625610351562e+00, -5.500625610351562e+00, -6.387824058532715e+00, -7.459638595581055e+00, -1.631673468686222e+01, -1.632031440734863e+01, -1.741679954528809e+01, -1.752539958953857e+01, -1.752933120727539e+01, -2.235028266906738e+01, -3.411346160888672e+01, -4.214949035644531e+01, -5.174369812011719e+01, -5.190860656738281e+01, -6.05566520690918e+01, -7.497373962402344e+01, -7.846428680419922e+01, -8.843743896484375e+01, -9.594685363769531e+01, -1.032265319824219e+02, -1.167155838012695e+02, -1.456850628662109e+02, -1.828849945068359e+02, -1.936869812011719e+02, -2.109842626953125e+02, -2.309005221557617e+02, -2.536859283447266e+02, -2.816975250244141e+02, -3.168697814941406e+02, -3.573291595458984e+02, -3.926827612304688e+02, -4.106821142578125e+02, -4.355733947753906e+02, -4.492048455810547e+02, -4.648029174804688e+02, -5.001868713378906e+02, -5.0576162109375e+02, -5.181173095703125e+02, -5.50651806640625e+02, -5.749522155761719e+02, -5.970711669921875e+02, -6.248660803222656e+02, -6.284073608398437e+02, -6.345344848632812e+02, -6.43205322265625e+02, -6.45507080078125e+02, -6.519124145507812e+02, -6.60537841796875e+02, -6.628739013671875e+02, -6.676869506835938e+02, -6.686029663085938e+02, -6.704879150390625e+02, -6.768280029296875e+02, -6.7892431640625e+02, -6.790615234375e+02, -6.790615234375e+02, -6.790615234375e+02, -6.790615234375e+02, -6.790615234375e+02, -6.790615234375e+02, -6.790615234375e+02, -6.790615234375e+02, -6.790615234375e+02, -6.792677001953125e+02, -6.792677001953125e+02, -6.792677001953125e+02, -6.792677001953125e+02, -6.792677001953125e+02, -6.792677001953125e+02, -6.792677001953125e+02, -6.792677001953125e+02, -6.792677001953125e+02, -6.792677001953125e+02]
 checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[-1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02, -1.86e+02]
 checkResultsAccordingToASHRAEHeatingOrTempMax.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
 checkResultsAccordingToASHRAECoolingOrTempMin.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
 Room.thermRoom.T=[2.941499938964844e+02, 2.930499572753906e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.930499914550781e+02, 2.930499908447266e+02, 2.930499572753906e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.93050048828125e+02, 2.930499749755859e+02, 2.930499572753906e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.930500646972656e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930500183105469e+02, 2.930500164794922e+02, 2.930500183105469e+02, 2.930500335693359e+02, 2.930499877929688e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.930500183105469e+02, 2.930499572753906e+02, 2.931499633789062e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.931499725341797e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.931499938964844e+02, 2.930500665283203e+02, 2.930499850537171e+02, 2.93150023803711e+02, 2.93050048828125e+02, 2.930609466939033e+02, 2.930500183105469e+02, 2.931499938964844e+02, 2.930499877929688e+02, 2.931206776647804e+02, 2.930500048828125e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.93049994506836e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.930499877929688e+02, 2.931499633789062e+02, 2.931500451660156e+02, 2.931499774169922e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.930499877929688e+02, 2.9314990234375e+02, 2.93050048828125e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.93050048828125e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.930499877929688e+02, 2.931499633789062e+02, 2.931500427246094e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930500793457031e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.930500793457031e+02, 2.930500061035156e+02, 2.930499932861328e+02, 2.9305001953125e+02, 2.930499877929688e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.930499853515625e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930499700927734e+02, 2.930500244140625e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930500183105469e+02, 2.930499975585938e+02, 2.930499877929688e+02, 2.930500793457031e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930500793457031e+02, 2.930499877929688e+02]
-Room.starRoom.T=[2.894175109863281e+02, 2.88675498046875e+02, 2.898958715820312e+02, 2.90374263305664e+02, 2.898571020507812e+02, 2.901259796142578e+02, 2.899448583984375e+02, 2.903491949462891e+02, 2.891812377929688e+02, 2.905830651855469e+02, 2.899963439941406e+02, 2.903646539306641e+02, 2.916037524414062e+02, 2.897439819335938e+02, 2.899138134765625e+02, 2.921112976074219e+02, 2.912236047363281e+02, 2.90234970703125e+02, 2.900992919921875e+02, 2.906921954345703e+02, 2.904945434570312e+02, 2.905455157470703e+02, 2.899885388183594e+02, 2.912790148925781e+02, 2.924037854003906e+02, 2.911511993408203e+02, 2.909665148925781e+02, 2.929476611328125e+02, 2.904434606933594e+02, 2.918353332519531e+02, 2.918414916992188e+02, 2.915233959960938e+02, 2.931850561934911e+02, 2.914560125732422e+02, 2.917908325195312e+02, 2.931683197021484e+02, 2.918550378417969e+02, 2.920802319335937e+02, 2.932768896484375e+02, 2.920608520507812e+02, 2.922477390757101e+02, 2.934889331054687e+02, 2.922204626464843e+02, 2.929990686344195e+02, 2.91526962890625e+02, 2.933963195800781e+02, 2.92049951171875e+02, 2.931526070515242e+02, 2.92365517578125e+02, 2.934961364746094e+02, 2.950800476074219e+02, 2.92114326171875e+02, 2.946367224121093e+02, 2.936502728271485e+02, 2.92489482421875e+02, 2.948910949707031e+02, 2.941212878417969e+02, 2.934346765136719e+02, 2.946315417480469e+02, 2.934882263183594e+02, 2.925883826116585e+02, 2.94143154296875e+02, 2.928589880371094e+02, 2.932848181152344e+02, 2.938146350097657e+02, 2.925441131591797e+02, 2.938894067382813e+02, 2.948023651123047e+02, 2.921531652832031e+02, 2.937510949707032e+02, 2.94125e+02, 2.915137408447266e+02, 2.927386462402344e+02, 2.924098028564453e+02, 2.9130673828125e+02, 2.907805480957031e+02, 2.9237328125e+02, 2.908251965332031e+02, 2.927157641601563e+02, 2.917182965087891e+02, 2.913261535644531e+02, 2.925723852539062e+02, 2.913036083984375e+02, 2.903975201416015e+02, 2.9061888671875e+02, 2.905832183837891e+02, 2.907925854492187e+02, 2.905048602294922e+02, 2.900315698242188e+02, 2.913239739990235e+02, 2.930156799316406e+02, 2.917483245849609e+02, 2.8992654296875e+02, 2.904973822021485e+02, 2.901367919921875e+02, 2.901581268310547e+02, 2.903918078613281e+02, 2.900873760986328e+02, 2.912270190429688e+02, 2.897540686035156e+02, 2.902552490234375e+02]
+Room.starRoom.T=[2.894175109863281e+02, 2.88675498046875e+02, 2.898958715820312e+02, 2.90374263305664e+02, 2.898571020507812e+02, 2.901259796142578e+02, 2.899448583984375e+02, 2.903491949462891e+02, 2.891812377929688e+02, 2.905830651855469e+02, 2.899963439941406e+02, 2.903646539306641e+02, 2.916037524414062e+02, 2.897439819335938e+02, 2.899138134765625e+02, 2.921112976074219e+02, 2.912236047363281e+02, 2.90234970703125e+02, 2.900992919921875e+02, 2.906921954345703e+02, 2.904945434570312e+02, 2.905455157470703e+02, 2.899885388183594e+02, 2.912790148925781e+02, 2.924037854003906e+02, 2.911511993408203e+02, 2.909665148925781e+02, 2.929476611328125e+02, 2.904434606933594e+02, 2.918353332519531e+02, 2.918414916992188e+02, 2.915233959960938e+02, 2.931850561934911e+02, 2.914560125732422e+02, 2.917908325195312e+02, 2.931683197021484e+02, 2.918550378417969e+02, 2.920802319335937e+02, 2.932768896484375e+02, 2.920608520507812e+02, 2.922477390757101e+02, 2.934889331054687e+02, 2.922204626464843e+02, 2.929990686344195e+02, 2.91526962890625e+02, 2.933963195800781e+02, 2.92049951171875e+02, 2.931526070515242e+02, 2.92365517578125e+02, 2.934961364746094e+02, 2.950800476074219e+02, 2.92114326171875e+02, 2.946367224121093e+02, 2.936502728271485e+02, 2.92489482421875e+02, 2.948910949707031e+02, 2.941212878417969e+02, 2.934346765136719e+02, 2.946315417480469e+02, 2.934882562255859e+02, 2.925883826116585e+02, 2.94143154296875e+02, 2.928589880371094e+02, 2.932848181152344e+02, 2.938146350097657e+02, 2.925441131591797e+02, 2.938894067382813e+02, 2.948023651123047e+02, 2.921531652832031e+02, 2.937510949707032e+02, 2.94125e+02, 2.915137408447266e+02, 2.927386462402344e+02, 2.924098028564453e+02, 2.913067297363281e+02, 2.907805480957031e+02, 2.9237328125e+02, 2.908251965332031e+02, 2.927157641601563e+02, 2.917182965087891e+02, 2.913261535644531e+02, 2.925723602294922e+02, 2.913036083984375e+02, 2.903975201416015e+02, 2.9061888671875e+02, 2.905831878662109e+02, 2.907925854492187e+02, 2.905048602294922e+02, 2.900315698242188e+02, 2.913239739990235e+02, 2.930156799316406e+02, 2.917483245849609e+02, 2.8992654296875e+02, 2.904973822021485e+02, 2.901367919921875e+02, 2.901581268310547e+02, 2.903918078613281e+02, 2.900873760986328e+02, 2.912270190429688e+02, 2.897540686035156e+02, 2.902552490234375e+02]
 TransmittedSolarRadiation_room=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case250.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case250.txt
index 5026197a64..830aba65a7 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case250.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case250.txt
@@ -1,4 +1,4 @@
-last-generated=2022-07-06
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,13 +8,13 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAEHeatingOrTempMax.lowerLimit=[4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03, 4.751e+03]
-AnnualHeatingLoad=[0e+00, 2.077252581787109e+02, 3.427198852539062e+02, 4.373985247802734e+02, 5.494172949218751e+02, 6.731013671875e+02, 8.433904565429688e+02, 9.394499780273437e+02, 1.061702573242188e+03, 1.196093881835938e+03, 1.373303955078125e+03, 1.503725424804687e+03, 1.588585712890625e+03, 1.733256357421875e+03, 1.862964877929687e+03, 1.990625024414062e+03, 2.086949609375e+03, 2.208633217773438e+03, 2.34357384765625e+03, 2.45316056640625e+03, 2.526212744140625e+03, 2.6242885546875e+03, 2.712508671875e+03, 2.802309077148438e+03, 2.855398193359375e+03, 2.908419311523438e+03, 3.005597109375e+03, 3.06564111328125e+03, 3.12956767578125e+03, 3.214280405273437e+03, 3.254305908203125e+03, 3.29603232421875e+03, 3.3145986328125e+03, 3.37585505859375e+03, 3.419370859375e+03, 3.466736572265625e+03, 3.516447890625e+03, 3.55136052734375e+03, 3.565138916015625e+03, 3.590566162109375e+03, 3.607054881948286e+03, 3.63518017578125e+03, 3.658752498246844e+03, 3.670716796875e+03, 3.70952435546875e+03, 3.735108154296875e+03, 3.7516191796875e+03, 3.77076708984375e+03, 3.78491654296875e+03, 3.79200927734375e+03, 3.79552978515625e+03, 3.809757768554688e+03, 3.819568115234375e+03, 3.822045654296875e+03, 3.827876025390625e+03, 3.8334013671875e+03, 3.835388916015625e+03, 3.83741650390625e+03, 3.83938525390625e+03, 3.840820556640625e+03, 3.845995554842045e+03, 3.856703369140625e+03, 3.86573095703125e+03, 3.868804443359375e+03, 3.882697265625e+03, 3.89739638671875e+03, 3.9017041015625e+03, 3.904870849609375e+03, 3.91903228515625e+03, 3.927376708984375e+03, 3.9498427734375e+03, 3.9737673828125e+03, 4.008265138725385e+03, 4.044638916015625e+03, 4.086367587890625e+03, 4.124947998046875e+03, 4.18552783203125e+03, 4.23063798828125e+03, 4.28873974609375e+03, 4.340060888671875e+03, 4.38806318359375e+03, 4.4346162109375e+03, 4.50058240234375e+03, 4.59461931640625e+03, 4.70487673828125e+03, 4.79438115234375e+03, 4.87065533203125e+03, 4.97646630859375e+03, 5.07637107421875e+03, 5.1688616015625e+03, 5.2863583984375e+03, 5.377340390625e+03, 5.47566607421875e+03, 5.607231328125e+03, 5.78005154296875e+03, 5.9201990234375e+03, 6.0753791796875e+03, 6.16933001953125e+03, 6.25686341796875e+03, 6.357868017578125e+03, 6.47828662109375e+03]
+AnnualHeatingLoad=[0e+00, 2.077252581787109e+02, 3.427198852539062e+02, 4.373985247802734e+02, 5.494172338867188e+02, 6.731012390136718e+02, 8.4339029296875e+02, 9.394497619628906e+02, 1.061702451171875e+03, 1.196093759765625e+03, 1.373303833007812e+03, 1.503725302734375e+03, 1.588585668945313e+03, 1.733256252441406e+03, 1.862964765625e+03, 1.99062490234375e+03, 2.086949609375e+03, 2.208633217773438e+03, 2.343573857421875e+03, 2.453160766601562e+03, 2.526212890625e+03, 2.624288647460938e+03, 2.712508671875e+03, 2.802309077148438e+03, 2.855398193359375e+03, 2.90841943359375e+03, 3.00559728515625e+03, 3.065641357421875e+03, 3.12956767578125e+03, 3.214280405273437e+03, 3.254305908203125e+03, 3.29603232421875e+03, 3.31459765625e+03, 3.375854389648438e+03, 3.419370126953125e+03, 3.46673583984375e+03, 3.516447158203125e+03, 3.551359794921875e+03, 3.56513818359375e+03, 3.5905654296875e+03, 3.607054149526411e+03, 3.635179443359375e+03, 3.6587515956456e+03, 3.6707158203125e+03, 3.70952345703125e+03, 3.735107421875e+03, 3.751618447265625e+03, 3.77076611328125e+03, 3.78491556640625e+03, 3.792008544921875e+03, 3.79552880859375e+03, 3.809756791992188e+03, 3.819567138671875e+03, 3.822044677734375e+03, 3.827875048828125e+03, 3.833400390625e+03, 3.835387939453125e+03, 3.83741552734375e+03, 3.83938427734375e+03, 3.840819580078125e+03, 3.84599458260946e+03, 3.856702392578125e+03, 3.86572998046875e+03, 3.868803466796875e+03, 3.8826962890625e+03, 3.897395581054688e+03, 3.901703369140625e+03, 3.9048701171875e+03, 3.919031064453125e+03, 3.92737548828125e+03, 3.949841552734375e+03, 3.973766254882813e+03, 4.00826391802226e+03, 4.044637451171875e+03, 4.086366298828125e+03, 4.124946533203125e+03, 4.18552685546875e+03, 4.230636552734375e+03, 4.28873876953125e+03, 4.340059423828125e+03, 4.38806171875e+03, 4.434615234375e+03, 4.50058140625e+03, 4.5946178515625e+03, 4.7048752734375e+03, 4.794379541015625e+03, 4.8706538671875e+03, 4.97646435546875e+03, 5.07636943359375e+03, 5.168859931640625e+03, 5.28635693359375e+03, 5.3773384375e+03, 5.47566423828125e+03, 5.60722986328125e+03, 5.780050078125e+03, 5.9201970703125e+03, 6.0753772265625e+03, 6.1693285546875e+03, 6.25686146484375e+03, 6.357866064453125e+03, 6.47828466796875e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.upperLimit=[7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03, 7.024e+03]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03, -3.38e+03]
-AnnualCoolingLoad=[0e+00, -1.12454429268837e-01, -1.12454429268837e-01, -1.505186408758163e-01, -3.073258996009827e-01, -3.073258996009827e-01, -3.073258996009827e-01, -7.756425738334656e-01, -7.756425738334656e-01, -7.756425738334656e-01, -7.756425738334656e-01, -7.756425738334656e-01, -1.374441385269165e+00, -1.374441385269165e+00, -1.374441385269165e+00, -1.374441385269165e+00, -1.374441385269165e+00, -1.374441385269165e+00, -1.374441385269165e+00, -1.374441385269165e+00, -6.743113040924072e+00, -6.901308059692383e+00, -9.888031959533691e+00, -9.923163414001465e+00, -2.079652252197265e+01, -3.222150802612305e+01, -3.222150802612305e+01, -3.537313003540039e+01, -3.741098022460938e+01, -3.954879379272461e+01, -4.939302444458008e+01, -5.867255401611328e+01, -8.573245239257812e+01, -8.936476135253906e+01, -1.008019180297852e+02, -1.044574600219727e+02, -1.047924423217773e+02, -1.213687973022461e+02, -1.502066003417969e+02, -1.700025177001953e+02, -1.986484222412109e+02, -2.064571810913086e+02, -2.302737884521484e+02, -2.625987854003906e+02, -2.709682312011719e+02, -2.935995941162109e+02, -3.137989807128906e+02, -3.326087744140625e+02, -3.623649597167969e+02, -4.11906996459961e+02, -4.7070654296875e+02, -4.92816650390625e+02, -5.307880737304688e+02, -5.662221838378906e+02, -6.0876416015625e+02, -6.608154113769531e+02, -7.150101147460938e+02, -7.770914306640625e+02, -8.322504833984375e+02, -8.644269030761719e+02, -9.126723022460938e+02, -9.408464978027343e+02, -9.718578932682217e+02, -1.031251970214844e+03, -1.054973520507813e+03, -1.084231201171875e+03, -1.138923232421875e+03, -1.179763937988281e+03, -1.221048950195312e+03, -1.267053154296875e+03, -1.282398681640625e+03, -1.300123901367188e+03, -1.322419921875e+03, -1.337690705566406e+03, -1.35515380859375e+03, -1.377057006835938e+03, -1.390264892578125e+03, -1.403892944335938e+03, -1.409464672851562e+03, -1.422087524414062e+03, -1.440074829101562e+03, -1.448469282226562e+03, -1.451125e+03, -1.451707397460938e+03, -1.451707397460938e+03, -1.454401000976562e+03, -1.454901245117188e+03, -1.454901245117188e+03, -1.454901245117188e+03, -1.454980102539062e+03, -1.455254516601562e+03, -1.45649169921875e+03, -1.45649169921875e+03, -1.45649169921875e+03, -1.45649169921875e+03, -1.45649169921875e+03, -1.45649169921875e+03, -1.45649169921875e+03, -1.456923217773438e+03, -1.457067749023438e+03, -1.457067749023438e+03]
+AnnualCoolingLoad=[0e+00, -1.12454429268837e-01, -1.12454429268837e-01, -1.505186408758163e-01, -3.073259890079498e-01, -3.073259890079498e-01, -3.073259890079498e-01, -7.756415605545044e-01, -7.756415605545044e-01, -7.756415605545044e-01, -7.756415605545044e-01, -7.756415605545044e-01, -1.374434232711792e+00, -1.374434232711792e+00, -1.374434232711792e+00, -1.374434232711792e+00, -1.374434232711792e+00, -1.374434232711792e+00, -1.374434232711792e+00, -1.374434232711792e+00, -6.743105411529541e+00, -6.901290893554688e+00, -9.888066291809082e+00, -9.923197746276855e+00, -2.079653015136719e+01, -3.222151947021484e+01, -3.222151947021484e+01, -3.537314910888672e+01, -3.741099166870117e+01, -3.954880905151367e+01, -4.939306259155273e+01, -5.867259216308594e+01, -8.573248321533202e+01, -8.936480712890625e+01, -1.008019332885742e+02, -1.044574851989746e+02, -1.047924652099609e+02, -1.213690567016602e+02, -1.50206875e+02, -1.700032501220703e+02, -1.986491088867188e+02, -2.064578524780273e+02, -2.302746429443359e+02, -2.625996704101562e+02, -2.709691162109375e+02, -2.936004791259766e+02, -3.137996826171875e+02, -3.326094458007813e+02, -3.623656311035156e+02, -4.119077593994141e+02, -4.707071838378906e+02, -4.928172912597656e+02, -5.307888061523438e+02, -5.662229162597656e+02, -6.087649536132812e+02, -6.608161437988281e+02, -7.150106640625e+02, -7.770919189453125e+02, -8.322510327148437e+02, -8.644275134277344e+02, -9.126729125976562e+02, -9.408471081542968e+02, -9.718584809155469e+02, -1.03125259765625e+03, -1.054974130859375e+03, -1.084231811523438e+03, -1.138923901367187e+03, -1.179764548339844e+03, -1.221049560546875e+03, -1.267053642578125e+03, -1.282399169921875e+03, -1.300124389648438e+03, -1.32242041015625e+03, -1.337691071777344e+03, -1.355154174804688e+03, -1.377057250976562e+03, -1.390265380859375e+03, -1.403893310546875e+03, -1.409465161132812e+03, -1.422088012695312e+03, -1.4400751953125e+03, -1.448469548339844e+03, -1.451125244140625e+03, -1.451707763671875e+03, -1.451707763671875e+03, -1.4544013671875e+03, -1.454901611328125e+03, -1.454901611328125e+03, -1.454901611328125e+03, -1.45498046875e+03, -1.455254858398438e+03, -1.456492065429688e+03, -1.456492065429688e+03, -1.456492065429688e+03, -1.456492065429688e+03, -1.456492065429688e+03, -1.456492065429688e+03, -1.456492065429688e+03, -1.456923461914062e+03, -1.457068115234375e+03, -1.457068115234375e+03]
 checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[-2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03, -2.177e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
 checkResultsAccordingToASHRAECoolingOrTempMin.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
 Room.thermRoom.T=[2.941499938964844e+02, 2.930499505615234e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.930499914550781e+02, 2.930499908447266e+02, 2.930499572753906e+02, 2.93050034790039e+02, 2.930499877929688e+02, 2.930499572753906e+02, 2.93050048828125e+02, 2.930499749755859e+02, 2.930499572753906e+02, 2.930500183105469e+02, 2.930499877929688e+02, 2.93049935913086e+02, 2.930500793457031e+02, 2.930499877929688e+02, 2.930499584960937e+02, 2.930500793457031e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930500183105469e+02, 2.930500164794922e+02, 2.931500244140625e+02, 2.930500335693359e+02, 2.930499877929688e+02, 2.931500549316406e+02, 2.930499877929688e+02, 2.930499267578125e+02, 2.930500061035156e+02, 2.930499572753906e+02, 2.931499328613281e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.931499420166016e+02, 2.93050048828125e+02, 2.930499877929688e+02, 2.931499938964844e+02, 2.930500793457031e+02, 2.930499850537171e+02, 2.931499938964844e+02, 2.930501098632812e+02, 2.930759626270395e+02, 2.93050048828125e+02, 2.931499938964844e+02, 2.930499877929688e+02, 2.931500549316406e+02, 2.930500219726562e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.93049994506836e+02, 2.931499328613281e+02, 2.931499938964844e+02, 2.930499877929688e+02, 2.931499298095703e+02, 2.931500451660156e+02, 2.931499774169922e+02, 2.931499328613281e+02, 2.931500549316406e+02, 2.930499877929688e+02, 2.931498718261719e+02, 2.931500592062038e+02, 2.931499938964844e+02, 2.931499914550781e+02, 2.930500793457031e+02, 2.931499633789062e+02, 2.931500323486328e+02, 2.930499877929688e+02, 2.931499633789062e+02, 2.931500366210938e+02, 2.930499877929688e+02, 2.93049944399481e+02, 2.931500799560547e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.930574129544772e+02, 2.930500183105469e+02, 2.931499890136719e+02, 2.930501098632812e+02, 2.930500061035156e+02, 2.931499688720703e+02, 2.930500500488281e+02, 2.930499877929688e+02, 2.930500341796875e+02, 2.930499877929688e+02, 2.930499853515625e+02, 2.930500140380859e+02, 2.930499877929688e+02, 2.930499700927734e+02, 2.931500244140625e+02, 2.930499877929688e+02, 2.930499877929688e+02, 2.93050048828125e+02, 2.930499975585938e+02, 2.930499877929688e+02, 2.930501062011719e+02, 2.930499877929688e+02, 2.930499743652344e+02, 2.930501165771485e+02, 2.930499877929688e+02]
-Room.starRoom.T=[2.894175109863281e+02, 2.894480603027343e+02, 2.898966540527344e+02, 2.903787292480469e+02, 2.906642858886719e+02, 2.901260070800781e+02, 2.899604382324219e+02, 2.904754229736328e+02, 2.891813061523437e+02, 2.906036999511718e+02, 2.908070373535156e+02, 2.903648291015625e+02, 2.916479846191406e+02, 2.898422094726562e+02, 2.899141723632812e+02, 2.923518676757812e+02, 2.917293798828125e+02, 2.902364562988281e+02, 2.909978186035156e+02, 2.91086875e+02, 2.904976379394531e+02, 2.909368267822265e+02, 2.900038134765625e+02, 2.912882531738281e+02, 2.936120678710938e+02, 2.911571807861328e+02, 2.909926098632812e+02, 2.937247503662109e+02, 2.904435217285156e+02, 2.919255255126953e+02, 2.925319213867188e+02, 2.915239892578125e+02, 2.934171899414063e+02, 2.923561077880859e+02, 2.917922766113281e+02, 2.936820098876953e+02, 2.929077685546875e+02, 2.920842724609375e+02, 2.937812390136719e+02, 2.927151293945312e+02, 2.922578142361454e+02, 2.948387390136719e+02, 2.928287062892405e+02, 2.930174497891317e+02, 2.920591101074219e+02, 2.934431671142578e+02, 2.920577416992188e+02, 2.939883911132812e+02, 2.923773522949219e+02, 2.935665521240234e+02, 2.959344482421875e+02, 2.921146618652344e+02, 2.950236840820313e+02, 2.947348547363281e+02, 2.924908264160156e+02, 2.955486511230469e+02, 2.951032739257813e+02, 2.934362884521485e+02, 2.951609033203125e+02, 2.942512426757813e+02, 2.925937914672685e+02, 2.948361712646484e+02, 2.9346648129311e+02, 2.932955139160156e+02, 2.950617517089844e+02, 2.926178344726562e+02, 2.939074548339844e+02, 2.959095458984375e+02, 2.921534375e+02, 2.937735638427735e+02, 2.951225158691406e+02, 2.915141650390625e+02, 2.929182971693065e+02, 2.940650708007813e+02, 2.913078344726562e+02, 2.908383636474609e+02, 2.930349357978448e+02, 2.908255737304688e+02, 2.9324513671875e+02, 2.921233117675781e+02, 2.913285766601563e+02, 2.93577177734375e+02, 2.914763000488281e+02, 2.904028210449219e+02, 2.91833974609375e+02, 2.905832183837891e+02, 2.907979113769532e+02, 2.914403778076172e+02, 2.90031630859375e+02, 2.913337408447265e+02, 2.937075622558594e+02, 2.917484460449219e+02, 2.899633544921875e+02, 2.908791265869141e+02, 2.901370043945312e+02, 2.901760467529297e+02, 2.907920617675781e+02, 2.900876806640625e+02, 2.914196362304688e+02, 2.90118032836914e+02, 2.902564392089844e+02]
+Room.starRoom.T=[2.894175109863281e+02, 2.894480603027343e+02, 2.898966540527344e+02, 2.903787292480469e+02, 2.906642858886719e+02, 2.901260070800781e+02, 2.899604382324219e+02, 2.904754089355469e+02, 2.891813061523437e+02, 2.906036999511718e+02, 2.908070373535156e+02, 2.903648291015625e+02, 2.916479846191406e+02, 2.898422094726562e+02, 2.899141723632812e+02, 2.923518676757812e+02, 2.917293798828125e+02, 2.902364562988281e+02, 2.909978186035156e+02, 2.91086875e+02, 2.904976379394531e+02, 2.909368267822265e+02, 2.900038134765625e+02, 2.912882513427734e+02, 2.936120678710938e+02, 2.911571960449219e+02, 2.909926098632812e+02, 2.937247503662109e+02, 2.904435217285156e+02, 2.919255255126953e+02, 2.925319213867188e+02, 2.915239892578125e+02, 2.934171899414063e+02, 2.923561077880859e+02, 2.917922766113281e+02, 2.936820098876953e+02, 2.929077685546875e+02, 2.920842724609375e+02, 2.937812390136719e+02, 2.927151293945312e+02, 2.922578142361454e+02, 2.948387390136719e+02, 2.928287062892405e+02, 2.930174497891317e+02, 2.920591101074219e+02, 2.934431671142578e+02, 2.920577416992188e+02, 2.939883911132812e+02, 2.923773522949219e+02, 2.935665521240234e+02, 2.959344482421875e+02, 2.921146618652344e+02, 2.950236840820313e+02, 2.947348547363281e+02, 2.924908264160156e+02, 2.955486511230469e+02, 2.951032739257813e+02, 2.934362884521485e+02, 2.951609033203125e+02, 2.942512127685547e+02, 2.925937914672685e+02, 2.948361712646484e+02, 2.9346648129311e+02, 2.932955139160156e+02, 2.950617517089844e+02, 2.926178344726562e+02, 2.939074548339844e+02, 2.959095458984375e+02, 2.921534375e+02, 2.937735638427735e+02, 2.951225158691406e+02, 2.915141650390625e+02, 2.929182971693065e+02, 2.940650708007813e+02, 2.913078344726562e+02, 2.908383636474609e+02, 2.930349357978448e+02, 2.908255737304688e+02, 2.932451416015625e+02, 2.921233117675781e+02, 2.913285766601563e+02, 2.93577177734375e+02, 2.914763000488281e+02, 2.904028210449219e+02, 2.91833974609375e+02, 2.905832489013672e+02, 2.907979113769532e+02, 2.914403778076172e+02, 2.90031630859375e+02, 2.913337408447265e+02, 2.937075622558594e+02, 2.917484460449219e+02, 2.899633544921875e+02, 2.908791265869141e+02, 2.901370043945312e+02, 2.901760467529297e+02, 2.907920617675781e+02, 2.900876806640625e+02, 2.914196362304688e+02, 2.90118032836914e+02, 2.902564392089844e+02]
 TransmittedSolarRadiation_room=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case400.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case400.txt
index adabd80e89..6d64641c26 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case400.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case400.txt
@@ -1,4 +1,4 @@
-last-generated=2022-07-06
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,7 +8,7 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAEHeatingOrTempMax.lowerLimit=[6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03, 6.9e+03]
-AnnualHeatingLoad=[0e+00, 2.143581787109375e+02, 3.584226428222656e+02, 4.64551098022461e+02, 5.868380102539063e+02, 7.204745666503907e+02, 9.004019067382812e+02, 1.005836926269531e+03, 1.139515478515625e+03, 1.287922768554688e+03, 1.472328442382812e+03, 1.612952702636719e+03, 1.709058862304687e+03, 1.861711450195312e+03, 2.006023935546875e+03, 2.145659448242187e+03, 2.254648232421875e+03, 2.391901118164063e+03, 2.540689111328125e+03, 2.666000698242187e+03, 2.754755126953125e+03, 2.86588779296875e+03, 2.9682292578125e+03, 3.07446837890625e+03, 3.136772119140625e+03, 3.198097045898438e+03, 3.310568505859375e+03, 3.382629248046875e+03, 3.456751689453125e+03, 3.560144033203125e+03, 3.608418603515625e+03, 3.660774604492187e+03, 3.680958984375e+03, 3.753301948242187e+03, 3.810528046875e+03, 3.872652099609375e+03, 3.933785263671875e+03, 3.976484189453125e+03, 3.9895078125e+03, 4.017838334960938e+03, 4.03619354178601e+03, 4.07338037109375e+03, 4.09968205078125e+03, 4.113322265625e+03, 4.155996171875e+03, 4.18635693359375e+03, 4.20523408203125e+03, 4.22626171875e+03, 4.2400791015625e+03, 4.24445458984375e+03, 4.24563037109375e+03, 4.261815703125e+03, 4.27217822265625e+03, 4.27355322265625e+03, 4.27724609375e+03, 4.27952099609375e+03, 4.27952099609375e+03, 4.2803818359375e+03, 4.28050537109375e+03, 4.28050537109375e+03, 4.28241162109375e+03, 4.2943701171875e+03, 4.3021226171875e+03, 4.30326416015625e+03, 4.3181591796875e+03, 4.33153828125e+03, 4.33338525390625e+03, 4.33474462890625e+03, 4.34633265625e+03, 4.352201171875e+03, 4.3771279296875e+03, 4.403831025390625e+03, 4.44273890625e+03, 4.486326689453125e+03, 4.5331353515625e+03, 4.57484423828125e+03, 4.64081701171875e+03, 4.68893267578125e+03, 4.75640185546875e+03, 4.8132528125e+03, 4.86578486328125e+03, 4.920467900390625e+03, 4.996133359375e+03, 5.10127146484375e+03, 5.2252076953125e+03, 5.32795615234375e+03, 5.41478572265625e+03, 5.53059322265625e+03, 5.64254271484375e+03, 5.7473250390625e+03, 5.8755185546875e+03, 5.97594251953125e+03, 6.08140115234375e+03, 6.223032919921875e+03, 6.4046766015625e+03, 6.556338671875e+03, 6.721496875e+03, 6.8242263671875e+03, 6.92071126953125e+03, 7.02960732421875e+03, 7.1597685546875e+03]
+AnnualHeatingLoad=[0e+00, 2.143581787109375e+02, 3.584226428222656e+02, 4.64551098022461e+02, 5.868380102539063e+02, 7.204745666503907e+02, 9.004019067382812e+02, 1.005836926269531e+03, 1.139515478515625e+03, 1.287922768554688e+03, 1.472328442382812e+03, 1.612952702636719e+03, 1.709058862304687e+03, 1.861711450195312e+03, 2.006023935546875e+03, 2.145659448242187e+03, 2.254648232421875e+03, 2.391901118164063e+03, 2.540689111328125e+03, 2.666000698242187e+03, 2.754755126953125e+03, 2.86588779296875e+03, 2.9682292578125e+03, 3.07446837890625e+03, 3.136772119140625e+03, 3.198097045898438e+03, 3.310568505859375e+03, 3.382629248046875e+03, 3.456751689453125e+03, 3.560144033203125e+03, 3.608418603515625e+03, 3.660774604492187e+03, 3.680958984375e+03, 3.753301948242187e+03, 3.810528046875e+03, 3.872652099609375e+03, 3.933785263671875e+03, 3.976484189453125e+03, 3.9895078125e+03, 4.017838334960938e+03, 4.03619354178601e+03, 4.07338037109375e+03, 4.09968205078125e+03, 4.113322265625e+03, 4.155996171875e+03, 4.18635693359375e+03, 4.20523408203125e+03, 4.22626171875e+03, 4.2400791015625e+03, 4.24445458984375e+03, 4.24563037109375e+03, 4.261815703125e+03, 4.27217822265625e+03, 4.27355322265625e+03, 4.27724609375e+03, 4.27952099609375e+03, 4.27952099609375e+03, 4.2803818359375e+03, 4.28050537109375e+03, 4.28050537109375e+03, 4.28241162109375e+03, 4.2943701171875e+03, 4.3021226171875e+03, 4.30326416015625e+03, 4.3181591796875e+03, 4.33153828125e+03, 4.33338525390625e+03, 4.33474462890625e+03, 4.34633265625e+03, 4.352201171875e+03, 4.3771279296875e+03, 4.403831025390625e+03, 4.44273890625e+03, 4.486326689453125e+03, 4.5331353515625e+03, 4.57484423828125e+03, 4.64081701171875e+03, 4.68893267578125e+03, 4.75640185546875e+03, 4.8132528125e+03, 4.86578486328125e+03, 4.920467900390625e+03, 4.996133828125e+03, 5.101271591796875e+03, 5.22520818359375e+03, 5.327956298828125e+03, 5.41478625e+03, 5.53059419921875e+03, 5.64254337890625e+03, 5.747325732421875e+03, 5.87551943359375e+03, 5.975943984375e+03, 6.0814025e+03, 6.22303412109375e+03, 6.404677734375e+03, 6.55634013671875e+03, 6.7214978515625e+03, 6.82422734375e+03, 6.92071224609375e+03, 7.02960830078125e+03, 7.15976904296875e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.upperLimit=[8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03, 8.77e+03]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01, -6.1e+01]
 AnnualCoolingLoad=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -5.624511977657676e-04, -1.37129008769989e+00, -6.907763004302979e+00, -9.551223754882812e+00, -1.074156463623047e+01, -1.223206520080566e+01, -1.259947395324707e+01, -1.419630241394043e+01, -1.888622856140137e+01, -2.632191467285156e+01, -2.94926050567627e+01, -2.974195289611816e+01, -3.001294326782227e+01, -3.062193298339844e+01, -3.080928993225098e+01, -3.412953186035156e+01, -3.412953186035156e+01, -3.415247344970703e+01, -3.599963760375977e+01, -3.681404876708984e+01, -3.831153106689453e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01, -3.856275939941406e+01]
@@ -16,5 +16,5 @@ checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[0e+00, 0e+00, 0e+00, 0
 checkResultsAccordingToASHRAEHeatingOrTempMax.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
 checkResultsAccordingToASHRAECoolingOrTempMin.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
 Room.thermRoom.T=[2.941499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500549316406e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500299072266e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500244140625e+02, 2.931500396728516e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500122070312e+02, 2.931499633789062e+02, 2.941629833984375e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.933988708496094e+02, 2.931500244140625e+02, 2.931499371337891e+02, 2.942939440917969e+02, 2.931500549316406e+02, 2.931499633789062e+02, 2.937941088867187e+02, 2.931500549316406e+02, 2.96046752319336e+02, 2.931500244140625e+02, 2.963847045898438e+02, 2.931499938964844e+02, 2.932057745361328e+02, 2.936198327636719e+02, 2.986464862060547e+02, 3.001501159667969e+02, 2.931499938964844e+02, 3.001499633789062e+02, 2.941156927490234e+02, 2.9465490234375e+02, 3.001499633789062e+02, 2.959303649902344e+02, 2.981262561035156e+02, 3.001499633789062e+02, 2.938199847412109e+02, 2.937602338803904e+02, 3.000584920247396e+02, 2.931500549316406e+02, 2.967592419433594e+02, 2.947254113769531e+02, 2.931500244140625e+02, 2.99553271484375e+02, 2.994756286621094e+02, 2.931499633789062e+02, 2.993903387451172e+02, 2.951084411621094e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500549316406e+02, 2.931499719238281e+02, 2.931499938964844e+02, 2.931500634765625e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02, 2.931499993896484e+02, 2.931499963378906e+02, 2.931499938964844e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499914550781e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500244140625e+02, 2.931500036621094e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02]
-Room.starRoom.T=[2.894175109863281e+02, 2.887623004150391e+02, 2.899824401855469e+02, 2.904606481933594e+02, 2.899437182617187e+02, 2.902123718261719e+02, 2.900313452148437e+02, 2.904356372070313e+02, 2.892679919433594e+02, 2.906694598388672e+02, 2.900828491210938e+02, 2.904513415527344e+02, 2.916898205566406e+02, 2.898305078125e+02, 2.900000891113281e+02, 2.921970306396485e+02, 2.913096313476562e+02, 2.903214880371094e+02, 2.901859912109375e+02, 2.907788403320312e+02, 2.905809692382812e+02, 2.906316668701172e+02, 2.900752136230469e+02, 2.913651696777344e+02, 2.924897229003906e+02, 2.912373199462891e+02, 2.910531762695313e+02, 2.930326043701172e+02, 2.905297802734375e+02, 2.91921591796875e+02, 2.919273803710938e+02, 2.916154028320312e+02, 2.941052209472657e+02, 2.915421252441406e+02, 2.918858471679687e+02, 2.933731353759766e+02, 2.919412573242187e+02, 2.924810064697265e+02, 2.942697473144531e+02, 2.921467315673828e+02, 2.924667363799779e+02, 2.938418499755859e+02, 2.923098449707031e+02, 2.959363787841797e+02, 2.916131848144531e+02, 2.963305633544922e+02, 2.921357702636719e+02, 2.9323439453125e+02, 2.935168334960937e+02, 2.985529876708985e+02, 3.004659118652344e+02, 2.922004162597656e+02, 3.006186181640625e+02, 2.941907733154297e+02, 2.945386340332032e+02, 3.008549835205078e+02, 2.960486535644531e+02, 2.980430505371094e+02, 3.006187194824219e+02, 2.938888110351563e+02, 2.936753108296518e+02, 2.99993896484375e+02, 2.929780163574219e+02, 2.966835748291016e+02, 2.947925e+02, 2.927014678955078e+02, 2.994921325683594e+02, 2.996004815673828e+02, 2.924660668945313e+02, 2.993108947753906e+02, 2.952344482421875e+02, 2.916014086914063e+02, 2.928512951660156e+02, 2.924961779785156e+02, 2.913930505371094e+02, 2.908669738769531e+02, 2.924589038085937e+02, 2.909118591308594e+02, 2.928013342285156e+02, 2.91804370727539e+02, 2.914287536621094e+02, 2.926582452392578e+02, 2.913902380371094e+02, 2.904842724609375e+02, 2.907057092285156e+02, 2.906704681396484e+02, 2.908789831542969e+02, 2.905919140625e+02, 2.901182592773437e+02, 2.914102392578125e+02, 2.931005676269531e+02, 2.91834384765625e+02, 2.900133654785157e+02, 2.90583916015625e+02, 2.902231958007812e+02, 2.902445465087891e+02, 2.904780700683594e+02, 2.901739642333985e+02, 2.913139074707031e+02, 2.898407855224609e+02, 2.903420104980469e+02]
+Room.starRoom.T=[2.894175109863281e+02, 2.887623004150391e+02, 2.899824401855469e+02, 2.904606481933594e+02, 2.899437182617187e+02, 2.902123718261719e+02, 2.900313452148437e+02, 2.904356372070313e+02, 2.892679919433594e+02, 2.906694598388672e+02, 2.900828491210938e+02, 2.904513415527344e+02, 2.916898205566406e+02, 2.898305078125e+02, 2.900000891113281e+02, 2.921970306396485e+02, 2.913096313476562e+02, 2.903214880371094e+02, 2.901859912109375e+02, 2.907788403320312e+02, 2.905809692382812e+02, 2.906316668701172e+02, 2.900752136230469e+02, 2.913651696777344e+02, 2.924897229003906e+02, 2.912373199462891e+02, 2.910531762695313e+02, 2.930326043701172e+02, 2.905297802734375e+02, 2.91921591796875e+02, 2.919273803710938e+02, 2.916154028320312e+02, 2.941052209472657e+02, 2.915421252441406e+02, 2.918858471679687e+02, 2.933731353759766e+02, 2.919412573242187e+02, 2.924810064697265e+02, 2.942697473144531e+02, 2.921467315673828e+02, 2.924667363799779e+02, 2.938418499755859e+02, 2.923098449707031e+02, 2.959363787841797e+02, 2.916131848144531e+02, 2.963305633544922e+02, 2.921357702636719e+02, 2.9323439453125e+02, 2.935168334960937e+02, 2.985529876708985e+02, 3.004659118652344e+02, 2.922004162597656e+02, 3.006186181640625e+02, 2.941907733154297e+02, 2.945386340332032e+02, 3.008549835205078e+02, 2.960486535644531e+02, 2.980430505371094e+02, 3.006187194824219e+02, 2.938888110351563e+02, 2.936753108296518e+02, 2.99993896484375e+02, 2.929780163574219e+02, 2.966835748291016e+02, 2.947925e+02, 2.927014678955078e+02, 2.994921325683594e+02, 2.996004815673828e+02, 2.924660668945313e+02, 2.993108947753906e+02, 2.952344482421875e+02, 2.916014086914063e+02, 2.928512951660156e+02, 2.924961779785156e+02, 2.913930505371094e+02, 2.908669738769531e+02, 2.924589038085937e+02, 2.909118591308594e+02, 2.928013342285156e+02, 2.91804370727539e+02, 2.914287536621094e+02, 2.926582452392578e+02, 2.913902380371094e+02, 2.904842724609375e+02, 2.907057092285156e+02, 2.906704681396484e+02, 2.908789831542969e+02, 2.905919140625e+02, 2.901182592773437e+02, 2.914102392578125e+02, 2.931005676269531e+02, 2.91834384765625e+02, 2.900133654785157e+02, 2.90583916015625e+02, 2.902231958007812e+02, 2.902445465087891e+02, 2.904780700683594e+02, 2.901739642333985e+02, 2.913139074707031e+02, 2.898407922363281e+02, 2.903420104980469e+02]
 TransmittedSolarRadiation_room=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case410.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case410.txt
index d4a9f3a4ff..be61fdcb11 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case410.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case410.txt
@@ -1,4 +1,4 @@
-last-generated=2022-07-06
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,13 +8,13 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAEHeatingOrTempMax.lowerLimit=[8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03, 8.596e+03]
-AnnualHeatingLoad=[0e+00, 2.65960463256836e+02, 4.44919658203125e+02, 5.770879760742188e+02, 7.293674072265625e+02, 8.954924499511719e+02, 1.119113315429687e+03, 1.250254692382812e+03, 1.416668002929687e+03, 1.601396398925781e+03, 1.83082841796875e+03, 2.005953181152344e+03, 2.125647958984375e+03, 2.316016176757812e+03, 2.495701337890625e+03, 2.6692525390625e+03, 2.80527767578125e+03, 2.976740854492187e+03, 3.1620768359375e+03, 3.318797080078125e+03, 3.43004501953125e+03, 3.568355922851562e+03, 3.6963953515625e+03, 3.829333564453125e+03, 3.907784306640625e+03, 3.9848193359375e+03, 4.125059375e+03, 4.215031591796875e+03, 4.30800125e+03, 4.43709541015625e+03, 4.49787998046875e+03, 4.5638812109375e+03, 4.589845703125e+03, 4.680665869140625e+03, 4.75282369140625e+03, 4.83070654296875e+03, 4.90761857421875e+03, 4.96150666015625e+03, 4.97871533203125e+03, 5.01524953125e+03, 5.039220048791087e+03, 5.08621875e+03, 5.1201656640625e+03, 5.138119140625e+03, 5.19231146484375e+03, 5.23043994140625e+03, 5.2549882421875e+03, 5.28195361328125e+03, 5.29988994140625e+03, 5.30666552734375e+03, 5.3086279296875e+03, 5.32983e+03, 5.34343798828125e+03, 5.34569091796875e+03, 5.3511826171875e+03, 5.35534912109375e+03, 5.35569091796875e+03, 5.357142578125e+03, 5.35790185546875e+03, 5.35830322265625e+03, 5.36167919921875e+03, 5.3772958984375e+03, 5.388065859375e+03, 5.3900224609375e+03, 5.40971923828125e+03, 5.42763310546875e+03, 5.4307939453125e+03, 5.433259765625e+03, 5.44973205078125e+03, 5.45856103515625e+03, 5.49086279296875e+03, 5.52537451171875e+03, 5.5748280859375e+03, 5.63028849609375e+03, 5.6896327734375e+03, 5.7428173828125e+03, 5.82545275390625e+03, 5.886361669921875e+03, 5.9708994140625e+03, 6.042636845703125e+03, 6.109096875e+03, 6.17771587890625e+03, 6.27259212890625e+03, 6.40386677734375e+03, 6.55905171875e+03, 6.687909130859375e+03, 6.79639419921875e+03, 6.9410419921875e+03, 7.0807226171875e+03, 7.211400341796875e+03, 7.37123583984375e+03, 7.4972753515625e+03, 7.62918552734375e+03, 7.8057625e+03, 8.0321290234375e+03, 8.2212119140625e+03, 8.427161796875e+03, 8.555261757812499e+03, 8.675578085937501e+03, 8.811753281249999e+03, 8.973943359375e+03]
+AnnualHeatingLoad=[0e+00, 2.65960463256836e+02, 4.44919658203125e+02, 5.770879760742188e+02, 7.293674072265625e+02, 8.954924499511719e+02, 1.119113315429687e+03, 1.250254692382812e+03, 1.416667880859375e+03, 1.601396157226563e+03, 1.830828076171875e+03, 2.005952885742187e+03, 2.12564771484375e+03, 2.316015932617187e+03, 2.49570107421875e+03, 2.669252124023437e+03, 2.8052771875e+03, 2.976740546875e+03, 3.16207634765625e+03, 3.318796547851563e+03, 3.430044287109375e+03, 3.568355434570312e+03, 3.6963944140625e+03, 3.82933283203125e+03, 3.90778357421875e+03, 3.984818603515625e+03, 4.12505853515625e+03, 4.21503064453125e+03, 4.30800076171875e+03, 4.437094921875e+03, 4.4978794921875e+03, 4.56388072265625e+03, 4.58984521484375e+03, 4.680665380859375e+03, 4.752823203125e+03, 4.83070654296875e+03, 4.907618046875e+03, 4.961506171875e+03, 4.97871484375e+03, 5.015248759765625e+03, 5.039219072228587e+03, 5.08621826171875e+03, 5.12016505859375e+03, 5.1381181640625e+03, 5.19231064453125e+03, 5.230439453125e+03, 5.254987265625e+03, 5.281953125e+03, 5.2998891796875e+03, 5.3066650390625e+03, 5.30862744140625e+03, 5.3298290234375e+03, 5.3434375e+03, 5.3456904296875e+03, 5.35118212890625e+03, 5.3553486328125e+03, 5.3556904296875e+03, 5.3571416015625e+03, 5.3579013671875e+03, 5.358302734375e+03, 5.3616787109375e+03, 5.377294921875e+03, 5.38806537109375e+03, 5.390021484375e+03, 5.40971875e+03, 5.4276326171875e+03, 5.43079345703125e+03, 5.4332587890625e+03, 5.4497315625e+03, 5.458560546875e+03, 5.4908623046875e+03, 5.525373720703125e+03, 5.57482759765625e+03, 5.6302880078125e+03, 5.68963228515625e+03, 5.742816650390625e+03, 5.825452265625e+03, 5.886361181640625e+03, 5.97089892578125e+03, 6.042636357421875e+03, 6.10909638671875e+03, 6.177715390625e+03, 6.27259166015625e+03, 6.4038662890625e+03, 6.55905123046875e+03, 6.687908642578125e+03, 6.79639318359375e+03, 6.941040595703125e+03, 7.08072146484375e+03, 7.211399365234375e+03, 7.37123486328125e+03, 7.497274375e+03, 7.629184921875e+03, 7.80576201171875e+03, 8.032128203125e+03, 8.2212109375e+03, 8.427161679687501e+03, 8.555261425781249e+03, 8.675577109375001e+03, 8.811753066406251e+03, 8.973943359375e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.upperLimit=[1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04, 1.0506e+04]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01, -8.4e+01]
-AnnualCoolingLoad=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -3.002009391784668e-01, -3.031482696533203e+00, -1.095425224304199e+01, -1.428366184234619e+01, -1.619326637268066e+01, -1.820087623596191e+01, -1.932974815368652e+01, -2.199979496002197e+01, -2.855017852783203e+01, -3.868256378173828e+01, -4.358632080078125e+01, -4.384432601928711e+01, -4.476755142211914e+01, -4.587932968139648e+01, -4.638987350463867e+01, -5.133343887329102e+01, -5.133343887329102e+01, -5.166058731079102e+01, -5.488337707519531e+01, -5.65267219543457e+01, -5.898796081542969e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01, -6.033815002441406e+01]
+AnnualCoolingLoad=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -3.002009391784668e-01, -3.031456708908081e+00, -1.095422554016113e+01, -1.428363132476807e+01, -1.619324348449707e+01, -1.820087814331055e+01, -1.932978630065918e+01, -2.19998405456543e+01, -2.855023002624512e+01, -3.86826057434082e+01, -4.35863542175293e+01, -4.384435653686523e+01, -4.476758193969727e+01, -4.587936782836914e+01, -4.63899040222168e+01, -5.133347702026367e+01, -5.133347702026367e+01, -5.166062545776367e+01, -5.488343811035156e+01, -5.652678298950195e+01, -5.898830032348633e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01, -6.03385009765625e+01]
 checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
 checkResultsAccordingToASHRAEHeatingOrTempMax.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
 checkResultsAccordingToASHRAECoolingOrTempMin.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
-Room.thermRoom.T=[2.941499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499670410156e+02, 2.931499938964844e+02, 2.931499328613281e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499627685547e+02, 2.931500549316406e+02, 2.931499633789062e+02, 2.931499328613281e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500854492188e+02, 2.931499713134766e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500207519532e+02, 2.931500244140625e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499328613281e+02, 2.931500244140625e+02, 2.931499633789062e+02, 2.941240661621094e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.933658264160156e+02, 2.931500244140625e+02, 2.931499633789062e+02, 2.942942846679687e+02, 2.931500854492188e+02, 2.931499606396546e+02, 2.938946362304687e+02, 2.931500622558594e+02, 2.957719573974609e+02, 2.931500244140625e+02, 2.961396850585937e+02, 2.931499938964844e+02, 2.932323034667968e+02, 2.9314998046875e+02, 2.983138293457031e+02, 3.001500549316406e+02, 2.931500006103516e+02, 3.001499633789062e+02, 2.943134106445312e+02, 2.937861767578125e+02, 3.001499633789062e+02, 2.960052661132813e+02, 2.9770998046875e+02, 3.001499633789062e+02, 2.938883343505859e+02, 2.932493576683556e+02, 2.999356140136719e+02, 2.931500549316406e+02, 2.964994122314453e+02, 2.949767724609375e+02, 2.931500549316406e+02, 2.994837158203125e+02, 2.999446966552734e+02, 2.931499633789062e+02, 2.992171990966797e+02, 2.955826477050781e+02, 2.931499938964844e+02, 2.931499584960937e+02, 2.931500549316406e+02, 2.931499719238281e+02, 2.931499938964844e+02, 2.931500939941406e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931501159667969e+02, 2.931499938964844e+02, 2.931499743652344e+02, 2.931500268554688e+02, 2.931499938964844e+02, 2.93150009765625e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499456787109e+02, 2.931500305175781e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500384521485e+02, 2.931500036621094e+02, 2.931499938964844e+02, 2.931500891113281e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931501159667969e+02, 2.931499938964844e+02]
-Room.starRoom.T=[2.894175109863281e+02, 2.88762269897461e+02, 2.899824536132812e+02, 2.904606176757812e+02, 2.899437182617187e+02, 2.9021240234375e+02, 2.900313452148437e+02, 2.904356536865234e+02, 2.892679846191406e+02, 2.906694598388672e+02, 2.900828552246094e+02, 2.904513415527344e+02, 2.916898205566406e+02, 2.89830503540039e+02, 2.900000891113281e+02, 2.921970306396485e+02, 2.913096472167969e+02, 2.903214575195312e+02, 2.901859912109375e+02, 2.907788458251953e+02, 2.9058095703125e+02, 2.906316668701172e+02, 2.900752087402344e+02, 2.913651373291016e+02, 2.924897229003906e+02, 2.912373352050781e+02, 2.91053154296875e+02, 2.930326043701172e+02, 2.905297802734375e+02, 2.91921591796875e+02, 2.91927392578125e+02, 2.916146514892578e+02, 2.941295104980469e+02, 2.915421557617187e+02, 2.918844189453125e+02, 2.933660247802734e+02, 2.91941259765625e+02, 2.923913391113281e+02, 2.943009851074219e+02, 2.921467315673828e+02, 2.924380617780722e+02, 2.939029241943359e+02, 2.923089416503906e+02, 2.958294494628906e+02, 2.916131848144531e+02, 2.961497009277344e+02, 2.921357971191406e+02, 2.932425866699219e+02, 2.929591088867188e+02, 2.9835373046875e+02, 3.006168212890625e+02, 2.922004162597656e+02, 3.006304321289062e+02, 2.943074139404297e+02, 2.938581872558594e+02, 3.008688201904297e+02, 2.959674169921875e+02, 2.977439013671875e+02, 3.006222387695312e+02, 2.938869250488281e+02, 2.932910588176106e+02, 2.999843280029297e+02, 2.929631701660156e+02, 2.965263610839844e+02, 2.949710302734375e+02, 2.926673034667969e+02, 2.994963903808594e+02, 2.999006866455078e+02, 2.923578991699219e+02, 2.992453350830078e+02, 2.955341430664063e+02, 2.916012329101562e+02, 2.928414123535156e+02, 2.924961187744141e+02, 2.913930200195313e+02, 2.908669586181641e+02, 2.924589123535156e+02, 2.909118591308594e+02, 2.928013391113281e+02, 2.918043591308594e+02, 2.914272277832031e+02, 2.926582702636719e+02, 2.913902673339844e+02, 2.904842724609375e+02, 2.907057238769531e+02, 2.906704376220703e+02, 2.908789831542969e+02, 2.90591918334961e+02, 2.901182397460938e+02, 2.914102087402344e+02, 2.931005737304687e+02, 2.918343548583985e+02, 2.900133422851562e+02, 2.905839324951172e+02, 2.902231860351562e+02, 2.902445495605469e+02, 2.904781005859375e+02, 2.901739440917969e+02, 2.913139074707031e+02, 2.898407922363281e+02, 2.903420104980469e+02]
+Room.thermRoom.T=[2.941499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499670410156e+02, 2.931499938964844e+02, 2.931499328613281e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499627685547e+02, 2.931500549316406e+02, 2.931499633789062e+02, 2.931499328613281e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500854492188e+02, 2.931499713134766e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500207519532e+02, 2.931500244140625e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499328613281e+02, 2.931500244140625e+02, 2.931499633789062e+02, 2.941240661621094e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.933658264160156e+02, 2.931500244140625e+02, 2.931499633789062e+02, 2.942942846679687e+02, 2.931500854492188e+02, 2.931499606396546e+02, 2.938946362304687e+02, 2.931500622558594e+02, 2.957719573974609e+02, 2.931500244140625e+02, 2.961396850585937e+02, 2.931499938964844e+02, 2.932323034667968e+02, 2.9314998046875e+02, 2.983138293457031e+02, 3.001500549316406e+02, 2.931500006103516e+02, 3.001499633789062e+02, 2.943134106445312e+02, 2.937861767578125e+02, 3.001499633789062e+02, 2.960052661132813e+02, 2.9770998046875e+02, 3.001499633789062e+02, 2.938883343505859e+02, 2.932493576683556e+02, 2.999356140136719e+02, 2.931500549316406e+02, 2.964994122314453e+02, 2.949767724609375e+02, 2.931500549316406e+02, 2.994837158203125e+02, 2.999446887207031e+02, 2.931499633789062e+02, 2.992171990966797e+02, 2.955826477050781e+02, 2.931499938964844e+02, 2.931499584960937e+02, 2.931500549316406e+02, 2.931499719238281e+02, 2.931499938964844e+02, 2.931500939941406e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931501159667969e+02, 2.931499938964844e+02, 2.931499743652344e+02, 2.931500268554688e+02, 2.931499938964844e+02, 2.93150009765625e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499456787109e+02, 2.931500305175781e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500384521485e+02, 2.931500036621094e+02, 2.931499938964844e+02, 2.931500891113281e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931501159667969e+02, 2.931499938964844e+02]
+Room.starRoom.T=[2.894175109863281e+02, 2.88762269897461e+02, 2.899824536132812e+02, 2.904606176757812e+02, 2.899437182617187e+02, 2.9021240234375e+02, 2.900313452148437e+02, 2.904356536865234e+02, 2.892679614257813e+02, 2.906694598388672e+02, 2.900828552246094e+02, 2.904513415527344e+02, 2.916898205566406e+02, 2.89830503540039e+02, 2.900000891113281e+02, 2.921970306396485e+02, 2.913096472167969e+02, 2.903214575195312e+02, 2.901859912109375e+02, 2.907788458251953e+02, 2.9058095703125e+02, 2.906316668701172e+02, 2.900752087402344e+02, 2.913651373291016e+02, 2.924897229003906e+02, 2.912373352050781e+02, 2.91053154296875e+02, 2.930326043701172e+02, 2.905297802734375e+02, 2.91921591796875e+02, 2.91927392578125e+02, 2.916146514892578e+02, 2.941295104980469e+02, 2.915421557617187e+02, 2.918844189453125e+02, 2.933660247802734e+02, 2.91941259765625e+02, 2.92391343383789e+02, 2.943009851074219e+02, 2.921467315673828e+02, 2.924380617780722e+02, 2.939029241943359e+02, 2.923089416503906e+02, 2.958294494628906e+02, 2.916131848144531e+02, 2.961497009277344e+02, 2.921357971191406e+02, 2.932425866699219e+02, 2.92959091796875e+02, 2.9835373046875e+02, 3.006168212890625e+02, 2.922004162597656e+02, 3.006304321289062e+02, 2.943074139404297e+02, 2.938581872558594e+02, 3.008688201904297e+02, 2.959674169921875e+02, 2.977439013671875e+02, 3.006222387695312e+02, 2.938869250488281e+02, 2.932910588176106e+02, 2.999843280029297e+02, 2.929631701660156e+02, 2.965263610839844e+02, 2.949710302734375e+02, 2.926673034667969e+02, 2.994963903808594e+02, 2.999006866455078e+02, 2.923578991699219e+02, 2.992453350830078e+02, 2.955341430664063e+02, 2.916012329101562e+02, 2.928414123535156e+02, 2.924961187744141e+02, 2.913930200195313e+02, 2.908669586181641e+02, 2.924589123535156e+02, 2.90911860961914e+02, 2.928013391113281e+02, 2.918043780517578e+02, 2.914272277832031e+02, 2.926582702636719e+02, 2.913902673339844e+02, 2.904842724609375e+02, 2.907057238769531e+02, 2.90670458984375e+02, 2.908789831542969e+02, 2.90591918334961e+02, 2.901182397460938e+02, 2.914102087402344e+02, 2.931005737304687e+02, 2.918343548583985e+02, 2.900133422851562e+02, 2.905839324951172e+02, 2.902232067871093e+02, 2.902445495605469e+02, 2.904781005859375e+02, 2.901739440917969e+02, 2.913139074707031e+02, 2.898407922363281e+02, 2.903420104980469e+02]
 TransmittedSolarRadiation_room=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case420.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case420.txt
index c2b70a3c74..c010264ee5 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case420.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case420.txt
@@ -1,4 +1,4 @@
-last-generated=2022-07-06
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,13 +8,13 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAEHeatingOrTempMax.lowerLimit=[7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03, 7.298e+03]
-AnnualHeatingLoad=[0e+00, 2.499427896118164e+02, 4.1280951171875e+02, 5.28901962890625e+02, 6.6509865234375e+02, 8.151403198242188e+02, 1.022650632324219e+03, 1.137723676757812e+03, 1.288047758789063e+03, 1.456673017578125e+03, 1.669986572265625e+03, 1.829011691894531e+03, 1.932635517578125e+03, 2.106896005859375e+03, 2.27048232421875e+03, 2.42794560546875e+03, 2.547889248046875e+03, 2.703250805664063e+03, 2.872486513671875e+03, 3.013094965820313e+03, 3.10825830078125e+03, 3.230499204101563e+03, 3.342511884765625e+03, 3.459348090820312e+03, 3.52390125e+03, 3.586439208984375e+03, 3.710595048828125e+03, 3.78458740234375e+03, 3.861954619140625e+03, 3.974967021484375e+03, 4.02139697265625e+03, 4.072776430664062e+03, 4.089546875e+03, 4.16405228515625e+03, 4.22182666015625e+03, 4.28432177734375e+03, 4.34494912109375e+03, 4.38635986328125e+03, 4.39490771484375e+03, 4.419676064453125e+03, 4.434580078125e+03, 4.46595947265625e+03, 4.4885825e+03, 4.49840966796875e+03, 4.53834083984375e+03, 4.56678759765625e+03, 4.58094646484375e+03, 4.597234375e+03, 4.60735986328125e+03, 4.6103359375e+03, 4.610865234375e+03, 4.622408544921875e+03, 4.62874169921875e+03, 4.628935546875e+03, 4.6304462890625e+03, 4.63067919921875e+03, 4.63067919921875e+03, 4.630705078125e+03, 4.630705078125e+03, 4.630705078125e+03, 4.631033203125e+03, 4.637830078125e+03, 4.6420615234375e+03, 4.642494140625e+03, 4.65244189453125e+03, 4.66103905957616e+03, 4.661287109375e+03, 4.66136376953125e+03, 4.67045548828125e+03, 4.67379541015625e+03, 4.69405810546875e+03, 4.715998515625e+03, 4.7540341796875e+03, 4.795120390625e+03, 4.8418212890625e+03, 4.883313720703125e+03, 4.9515707421875e+03, 4.9992641796875e+03, 5.06841158203125e+03, 5.125616611328125e+03, 5.17921298828125e+03, 5.233668349609375e+03, 5.313003515625e+03, 5.428196787109375e+03, 5.5672615625e+03, 5.6800994140625e+03, 5.7725133203125e+03, 5.901060810546875e+03, 6.02465033203125e+03, 6.139241142578125e+03, 6.2830595703125e+03, 6.39330623046875e+03, 6.50913103515625e+03, 6.66959576171875e+03, 6.87983564453125e+03, 7.0528060546875e+03, 7.24263265625e+03, 7.35465453125e+03, 7.4589192578125e+03, 7.579001015625e+03, 7.72509130859375e+03]
+AnnualHeatingLoad=[0e+00, 2.499427896118164e+02, 4.1280951171875e+02, 5.28901962890625e+02, 6.6509865234375e+02, 8.151403198242188e+02, 1.022650632324219e+03, 1.137723610839844e+03, 1.288048002929688e+03, 1.45667375e+03, 1.669987548828125e+03, 1.829012790527344e+03, 1.932636572265625e+03, 2.106897192382813e+03, 2.270483544921875e+03, 2.427946752929688e+03, 2.5478903515625e+03, 2.703251782226563e+03, 2.8724875e+03, 3.013096186523438e+03, 3.108259521484375e+03, 3.230500424804688e+03, 3.34251408203125e+03, 3.459350532226562e+03, 3.52390369140625e+03, 3.586441650390625e+03, 3.710597490234375e+03, 3.78458984375e+03, 3.861957060546875e+03, 3.974969462890625e+03, 4.0213994140625e+03, 4.072778872070312e+03, 4.089549072265625e+03, 4.16405423828125e+03, 4.2218291015625e+03, 4.28432373046875e+03, 4.34495107421875e+03, 4.38636181640625e+03, 4.39490966796875e+03, 4.41967822265625e+03, 4.43458251953125e+03, 4.4659619140625e+03, 4.48858482421875e+03, 4.49841162109375e+03, 4.53834279296875e+03, 4.5667900390625e+03, 4.58094841796875e+03, 4.59723583984375e+03, 4.607361328125e+03, 4.610337890625e+03, 4.6108671875e+03, 4.622410498046875e+03, 4.62874365234375e+03, 4.6289375e+03, 4.6304482421875e+03, 4.6306806640625e+03, 4.6306806640625e+03, 4.63070703125e+03, 4.63070703125e+03, 4.63070703125e+03, 4.63103515625e+03, 4.63783154296875e+03, 4.64206298828125e+03, 4.64249609375e+03, 4.652443359375e+03, 4.66104101270116e+03, 4.6612890625e+03, 4.66136572265625e+03, 4.670456953125e+03, 4.67379736328125e+03, 4.69406005859375e+03, 4.71600046875e+03, 4.7540361328125e+03, 4.795122373046875e+03, 4.84182359375e+03, 4.883315673828125e+03, 4.951573046875e+03, 4.999266591796875e+03, 5.06841361328125e+03, 5.125618564453125e+03, 5.17921513671875e+03, 5.233670302734375e+03, 5.31300546875e+03, 5.4281988671875e+03, 5.56726400390625e+03, 5.6801013671875e+03, 5.7725152734375e+03, 5.901062763671875e+03, 6.02465228515625e+03, 6.139243583984375e+03, 6.2830615234375e+03, 6.39330818359375e+03, 6.50913298828125e+03, 6.66959771484375e+03, 6.87983775390625e+03, 7.052808056640625e+03, 7.242634609375e+03, 7.354656650390625e+03, 7.45892142578125e+03, 7.57900296875e+03, 7.72509326171875e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.upperLimit=[9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03, 9.151e+03]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02, -1.89e+02]
-AnnualCoolingLoad=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -1.983975321054459e-01, -5.740681886672974e-01, -5.740681886672974e-01, -1.322022318840027e+00, -1.731423020362854e+00, -1.805977582931519e+00, -3.646051645278931e+00, -1.145280170440674e+01, -2.694634056091309e+01, -3.187973213195801e+01, -3.651271377563477e+01, -4.110701370239258e+01, -4.600626373291016e+01, -5.276364669799805e+01, -6.639449310302734e+01, -8.495280456542969e+01, -9.743771759033203e+01, -9.876436614990234e+01, -1.032137298583984e+02, -1.060069882935582e+02, -1.094411087036133e+02, -1.213094711303711e+02, -1.213094711303711e+02, -1.229147109985352e+02, -1.321975250244141e+02, -1.379770315551758e+02, -1.435431823730469e+02, -1.497616271972656e+02, -1.497616271972656e+02, -1.502259979248047e+02, -1.502628173828125e+02, -1.502628173828125e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02, -1.506912841796875e+02]
+AnnualCoolingLoad=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -1.983975768089294e-01, -5.740669965744019e-01, -5.740669965744019e-01, -1.322022318840027e+00, -1.731422901153564e+00, -1.805977463722229e+00, -3.646050930023193e+00, -1.145280075073242e+01, -2.694633483886719e+01, -3.187972450256348e+01, -3.65126985168457e+01, -4.110694885253906e+01, -4.600616836547852e+01, -5.276361083984375e+01, -6.639444732666016e+01, -8.495264434814453e+01, -9.743752685546875e+01, -9.876416015625e+01, -1.032135162353516e+02, -1.060067670411168e+02, -1.094408798217773e+02, -1.213092727661133e+02, -1.213092727661133e+02, -1.229145050048828e+02, -1.321973266601562e+02, -1.379768179321289e+02, -1.4354296875e+02, -1.497613830566406e+02, -1.497613830566406e+02, -1.502257690429688e+02, -1.502625732421875e+02, -1.502625732421875e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02, -1.506910247802734e+02]
 checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[-1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01, -1.1e+01]
 checkResultsAccordingToASHRAEHeatingOrTempMax.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
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-Room.starRoom.T=[2.895909423828125e+02, 2.890937384033203e+02, 2.903125390625e+02, 2.907900140380859e+02, 2.9027392578125e+02, 2.905419891357422e+02, 2.903612390136719e+02, 2.907652600097656e+02, 2.895990393066406e+02, 2.909988323974609e+02, 2.90412744140625e+02, 2.907814324951172e+02, 2.920183288574219e+02, 2.901606292724609e+02, 2.903295922851563e+02, 2.925249603271484e+02, 2.916381628417969e+02, 2.906512609863281e+02, 2.905161560058594e+02, 2.911087463378906e+02, 2.909104553222656e+02, 2.909604748535156e+02, 2.904055151367187e+02, 2.916938494873047e+02, 2.928185534667969e+02, 2.915660400390625e+02, 2.913829711914062e+02, 2.934430413818359e+02, 2.908590502929687e+02, 2.922506292724609e+02, 2.922555786132813e+02, 2.919628582763672e+02, 2.956550146484375e+02, 2.918707531738281e+02, 2.922435717773437e+02, 2.945154388427734e+02, 2.922702465820312e+02, 2.934020384361302e+02, 2.958406286621094e+02, 2.924754187011719e+02, 2.933600733934251e+02, 2.948833319091797e+02, 2.926484875488281e+02, 2.976861065673828e+02, 2.919420727539062e+02, 2.979268249511719e+02, 2.924641662597656e+02, 2.939546820068359e+02, 2.944490368652343e+02, 2.993437915039062e+02, 3.012408752441406e+02, 2.925295007324219e+02, 3.0095904296875e+02, 2.953878448486328e+02, 2.953400280761718e+02, 3.01208154296875e+02, 2.978615979003906e+02, 2.989588763427735e+02, 3.009513354492187e+02, 2.957592510986328e+02, 2.95192380272838e+02, 3.004091518676083e+02, 2.933953210449219e+02, 2.981255932617187e+02, 2.961388842773438e+02, 2.930976763513988e+02, 3.001549561888307e+02, 3.009617724609375e+02, 2.929483972167969e+02, 2.999946478271484e+02, 2.96518701171875e+02, 2.919362615966797e+02, 2.939181127929688e+02, 2.928262646484375e+02, 2.917236755371094e+02, 2.911963500976562e+02, 2.9278783203125e+02, 2.912417681884766e+02, 2.931305297851562e+02, 2.921331671142578e+02, 2.917823791503906e+02, 2.929873468017578e+02, 2.917200866699219e+02, 2.9081453125e+02, 2.910359106445313e+02, 2.910017578125e+02, 2.9120830078125e+02, 2.909226379394531e+02, 2.904485009765625e+02, 2.917390631103515e+02, 2.935951110839844e+02, 2.921629693603516e+02, 2.903439538574219e+02, 2.909136798095703e+02, 2.905528552246094e+02, 2.905741851806641e+02, 2.908073864746094e+02, 2.905039508056641e+02, 2.916442700195312e+02, 2.901714691162109e+02, 2.906723022460938e+02]
+Room.thermRoom.T=[2.941499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499670410156e+02, 2.931499938964844e+02, 2.931499328613281e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499627685547e+02, 2.931500549316406e+02, 2.931499633789062e+02, 2.931499328613281e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500854492188e+02, 2.931499713134766e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500207519532e+02, 2.931500244140625e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.934115441894531e+02, 2.931499938964844e+02, 2.931499328613281e+02, 2.931500244140625e+02, 2.931499633789062e+02, 2.956171643066406e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.944913940429688e+02, 2.931500244140625e+02, 2.9326771414226e+02, 2.958058129882813e+02, 2.931500854492188e+02, 2.932425838812865e+02, 2.948553863525391e+02, 2.931500549316406e+02, 2.975843859863281e+02, 2.931500244140625e+02, 2.978838989257812e+02, 2.931499938964844e+02, 2.939263977050781e+02, 2.943406750488281e+02, 2.992805059814453e+02, 3.001500244140625e+02, 2.931500006103516e+02, 3.001499633789062e+02, 2.953695471191406e+02, 2.952278503417969e+02, 3.001499603271484e+02, 2.978617065429688e+02, 2.988977624511719e+02, 3.001499633789062e+02, 2.957317956542969e+02, 2.951054500980559e+02, 3.001498718261719e+02, 2.933602844238281e+02, 2.980647833251953e+02, 2.96121748046875e+02, 2.931500342820219e+02, 3.001163866650927e+02, 3.001500549316406e+02, 2.9314994140625e+02, 2.999477001953125e+02, 2.965405212402344e+02, 2.931499938964844e+02, 2.938622082519531e+02, 2.931500549316406e+02, 2.931499719238281e+02, 2.931499938964844e+02, 2.931500939941406e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931501159667969e+02, 2.931499938964844e+02, 2.931499743652344e+02, 2.931500268554688e+02, 2.931499938964844e+02, 2.93150009765625e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499456787109e+02, 2.935695434570313e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500384521485e+02, 2.931500036621094e+02, 2.931499938964844e+02, 2.931500891113281e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931501159667969e+02, 2.931499938964844e+02]
+Room.starRoom.T=[2.895909423828125e+02, 2.890937384033203e+02, 2.903125390625e+02, 2.907900140380859e+02, 2.9027392578125e+02, 2.905419891357422e+02, 2.903612390136719e+02, 2.907652600097656e+02, 2.895990393066406e+02, 2.909988323974609e+02, 2.90412744140625e+02, 2.907814324951172e+02, 2.920183288574219e+02, 2.90160625e+02, 2.903295922851563e+02, 2.925249603271484e+02, 2.916381628417969e+02, 2.906512609863281e+02, 2.905161560058594e+02, 2.911087463378906e+02, 2.909104553222656e+02, 2.909604748535156e+02, 2.904055151367187e+02, 2.9169384765625e+02, 2.928185754394531e+02, 2.915660705566406e+02, 2.913829711914062e+02, 2.934430413818359e+02, 2.908590502929687e+02, 2.922506292724609e+02, 2.922555786132813e+02, 2.919628582763672e+02, 2.956550146484375e+02, 2.918707531738281e+02, 2.922435717773437e+02, 2.945154388427734e+02, 2.922702465820312e+02, 2.934020384361302e+02, 2.958406286621094e+02, 2.924754187011719e+02, 2.933600733934251e+02, 2.948833319091797e+02, 2.926484875488281e+02, 2.976861065673828e+02, 2.919420727539062e+02, 2.979268249511719e+02, 2.924641662597656e+02, 2.939546820068359e+02, 2.944490368652343e+02, 2.993437915039062e+02, 3.012408752441406e+02, 2.925295007324219e+02, 3.0095904296875e+02, 2.953878448486328e+02, 2.953400280761718e+02, 3.012081817626953e+02, 2.978615979003906e+02, 2.989588763427735e+02, 3.009513354492187e+02, 2.957592510986328e+02, 2.95192380272838e+02, 3.004091518676083e+02, 2.933953210449219e+02, 2.981255932617187e+02, 2.961388842773438e+02, 2.930976763513988e+02, 3.001549561888307e+02, 3.009617724609375e+02, 2.929483679199218e+02, 2.999946478271484e+02, 2.96518701171875e+02, 2.919362426757813e+02, 2.939181079101563e+02, 2.928262646484375e+02, 2.917236840820312e+02, 2.911963500976562e+02, 2.9278783203125e+02, 2.912417681884766e+02, 2.931305249023437e+02, 2.921331671142578e+02, 2.917823791503906e+02, 2.929873468017578e+02, 2.917201184082031e+02, 2.908145538330078e+02, 2.910359106445313e+02, 2.910017669677734e+02, 2.9120830078125e+02, 2.909226379394531e+02, 2.904485009765625e+02, 2.917390631103515e+02, 2.935951110839844e+02, 2.921629693603516e+02, 2.903439538574219e+02, 2.909136798095703e+02, 2.905528552246094e+02, 2.905741851806641e+02, 2.908073864746094e+02, 2.905039508056641e+02, 2.916442700195312e+02, 2.901714691162109e+02, 2.906723022460938e+02]
 TransmittedSolarRadiation_room=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case430.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case430.txt
index d5d257e202..7ebefec199 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case430.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case430.txt
@@ -1,4 +1,4 @@
-last-generated=2022-06-02
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,13 +8,13 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAEHeatingOrTempMax.lowerLimit=[5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03, 5.429e+03]
-AnnualHeatingLoad=[0e+00, 2.461959606933594e+02, 4.038277954101562e+02, 5.13162568359375e+02, 6.4332044921875e+02, 7.875749450683594e+02, 9.89496572265625e+02, 1.099031516113281e+03, 1.242647734375e+03, 1.402945073242187e+03, 1.612191772460938e+03, 1.765271091308594e+03, 1.862001694335938e+03, 2.03169302734375e+03, 2.186584130859375e+03, 2.336986767578125e+03, 2.44943685546875e+03, 2.595496962890625e+03, 2.756507216796875e+03, 2.887715395507812e+03, 2.97176240234375e+03, 3.086191127929687e+03, 3.1888547265625e+03, 3.295807719726562e+03, 3.353209228515625e+03, 3.409009887695312e+03, 3.52403921875e+03, 3.590449462890625e+03, 3.661425078125e+03, 3.762454204101562e+03, 3.80292509765625e+03, 3.846594458007813e+03, 3.86030517578125e+03, 3.926913237304687e+03, 3.9744351171875e+03, 4.02760693359375e+03, 4.080846201171875e+03, 4.1162119140625e+03, 4.122873046875e+03, 4.143706171875e+03, 4.1552705078125e+03, 4.18038916015625e+03, 4.198684926531917e+03, 4.2054638671875e+03, 4.2415716015625e+03, 4.266125e+03, 4.27737404296875e+03, 4.29123193359375e+03, 4.29926171875e+03, 4.30188525390625e+03, 4.302314453125e+03, 4.311028662109375e+03, 4.315546875e+03, 4.31556005859375e+03, 4.31662353515625e+03, 4.316728515625e+03, 4.316728515625e+03, 4.316728515625e+03, 4.316728515625e+03, 4.316728515625e+03, 4.31698095703125e+03, 4.3220732421875e+03, 4.3253994140625e+03, 4.32577490234375e+03, 4.33311962890625e+03, 4.340016156033987e+03, 4.3401650390625e+03, 4.34018603515625e+03, 4.34750248046875e+03, 4.3501337890625e+03, 4.36654833984375e+03, 4.38485693359375e+03, 4.4184716796875e+03, 4.4521025390625e+03, 4.49337173828125e+03, 4.530490966796875e+03, 4.59288232421875e+03, 4.63663625e+03, 4.699392578125e+03, 4.75068138671875e+03, 4.7987974609375e+03, 4.8469755859375e+03, 4.9196977734375e+03, 5.028330322265625e+03, 5.15926521484375e+03, 5.263463671875e+03, 5.34960095703125e+03, 5.47232130859375e+03, 5.58881341796875e+03, 5.69613328125e+03, 5.83378125e+03, 5.93811921875e+03, 6.049937265625e+03, 6.20453734375e+03, 6.40968916015625e+03, 6.575891845703125e+03, 6.759911640625e+03, 6.86686986328125e+03, 6.9659306640625e+03, 7.08148271484375e+03, 7.221912109375e+03]
+AnnualHeatingLoad=[0e+00, 2.461959606933594e+02, 4.038279174804687e+02, 5.131626696777344e+02, 6.433206860351562e+02, 7.875751892089844e+02, 9.894965112304687e+02, 1.099031459960938e+03, 1.242647856445313e+03, 1.4029451953125e+03, 1.612192016601562e+03, 1.765271335449219e+03, 1.862001938476563e+03, 2.031693271484375e+03, 2.18658435546875e+03, 2.336986767578125e+03, 2.44943697265625e+03, 2.595496962890625e+03, 2.7565074609375e+03, 2.887715395507812e+03, 2.971762646484375e+03, 3.086191279296875e+03, 3.188854931640625e+03, 3.295807963867187e+03, 3.35320947265625e+03, 3.409010131835938e+03, 3.524039462890625e+03, 3.590449462890625e+03, 3.661425078125e+03, 3.762454204101562e+03, 3.802924951171875e+03, 3.846594213867188e+03, 3.860304931640625e+03, 3.926913056640625e+03, 3.974434873046875e+03, 4.02760693359375e+03, 4.08084595703125e+03, 4.11621142578125e+03, 4.122873046875e+03, 4.14370568359375e+03, 4.15527001953125e+03, 4.18038916015625e+03, 4.198684438250667e+03, 4.2054638671875e+03, 4.24157111328125e+03, 4.26612451171875e+03, 4.27737361328125e+03, 4.2912314453125e+03, 4.29926123046875e+03, 4.30188525390625e+03, 4.30231396484375e+03, 4.3110285546875e+03, 4.315546875e+03, 4.31556005859375e+03, 4.31662353515625e+03, 4.316728515625e+03, 4.316728515625e+03, 4.316728515625e+03, 4.316728515625e+03, 4.316728515625e+03, 4.31698046875e+03, 4.32207275390625e+03, 4.32539892578125e+03, 4.3257744140625e+03, 4.333119140625e+03, 4.340015667752737e+03, 4.3401650390625e+03, 4.340185546875e+03, 4.3475019921875e+03, 4.3501337890625e+03, 4.3665478515625e+03, 4.384856630859375e+03, 4.4184716796875e+03, 4.4521025390625e+03, 4.49337125e+03, 4.530490478515625e+03, 4.59288134765625e+03, 4.63663576171875e+03, 4.69939208984375e+03, 4.750680712890625e+03, 4.79879677734375e+03, 4.846974609375e+03, 4.9196962890625e+03, 5.02832849609375e+03, 5.15926326171875e+03, 5.263461865234375e+03, 5.34959900390625e+03, 5.47231984375e+03, 5.588811953125e+03, 5.696131611328125e+03, 5.833779296875e+03, 5.93811775390625e+03, 6.04993580078125e+03, 6.204535615234375e+03, 6.40968736328125e+03, 6.57588994140625e+03, 6.75990974609375e+03, 6.866868076171875e+03, 6.965928984375e+03, 7.081480869140625e+03, 7.22191064453125e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.upperLimit=[7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03, 7.827e+03]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02, -8.75e+02]
-AnnualCoolingLoad=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -1.906495541334152e-01, -6.585839986801147e-01, -6.585839986801147e-01, -6.585839986801147e-01, -6.585839986801147e-01, -6.585839986801147e-01, -6.585839986801147e-01, -6.585839986801147e-01, -1.495771169662476e+00, -1.495771169662476e+00, -1.495771169662476e+00, -1.495771169662476e+00, -1.495771169662476e+00, -2.890789031982422e+00, -5.484135627746582e+00, -7.513307094573975e+00, -9.272046089172363e+00, -9.272046089172363e+00, -1.211132049560547e+01, -1.619174003601074e+01, -1.648847007751465e+01, -1.877862167358398e+01, -2.158172225952148e+01, -2.325775337219238e+01, -2.77004508972168e+01, -4.484724807739258e+01, -7.204277801513672e+01, -7.879960632324219e+01, -8.925372406005859e+01, -9.832605743408203e+01, -1.116427841186523e+02, -1.296491851806641e+02, -1.532925720214844e+02, -1.838416900634766e+02, -2.070857366943359e+02, -2.135506591796875e+02, -2.2907421875e+02, -2.365525381469727e+02, -2.460142059326172e+02, -2.702948913574219e+02, -2.717400817871094e+02, -2.781832885742188e+02, -2.988557434082031e+02, -3.108449755859375e+02, -3.248339233398438e+02, -3.398744506835938e+02, -3.398744506835938e+02, -3.424156799316406e+02, -3.45586181640625e+02, -3.456663818359375e+02, -3.474822998046875e+02, -3.49486083984375e+02, -3.49486083984375e+02, -3.495873413085938e+02, -3.495873413085938e+02, -3.495873413085938e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02, -3.50538330078125e+02]
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 checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[-4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02, -4.22e+02]
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 TransmittedSolarRadiation_room=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case600FF.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case600FF.txt
index 24d5ca6435..1de621b4c1 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case600FF.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case600FF.txt
@@ -3,7 +3,7 @@ statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
   "nonlinear": "13",
-  "number of continuous time states": "23",
+  "number of continuous time states": "21",
   "numerical Jacobians": "0"
 }
 time=[0e+00, 3.15396e+07]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case650FF.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case650FF.txt
index c6a33bc250..db47833cd3 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case650FF.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case650FF.txt
@@ -3,7 +3,7 @@ statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
   "nonlinear": "13",
-  "number of continuous time states": "23",
+  "number of continuous time states": "21",
   "numerical Jacobians": "0"
 }
 time=[0e+00, 3.15396e+07]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case800.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case800.txt
index 5509dd3ba8..e190a972b5 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case800.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case800.txt
@@ -1,4 +1,4 @@
-last-generated=2022-07-06
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,13 +8,13 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAEHeatingOrTempMax.lowerLimit=[4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03, 4.868e+03]
-AnnualHeatingLoad=[0e+00, 2.419274752807617e+02, 4.067510314941406e+02, 5.194193994140625e+02, 6.444752758789062e+02, 7.911325561523438e+02, 9.918129907226562e+02, 1.101696496582031e+03, 1.24273880859375e+03, 1.4066748828125e+03, 1.607335498046875e+03, 1.767361953125e+03, 1.8677171875e+03, 2.030192192382812e+03, 2.187883369140625e+03, 2.341243481445313e+03, 2.451160556640625e+03, 2.596563198242187e+03, 2.75473166015625e+03, 2.888201767578125e+03, 2.971117822265625e+03, 3.083801030273437e+03, 3.186530205078125e+03, 3.295537807617187e+03, 3.345710107421875e+03, 3.394532348632812e+03, 3.509539287109375e+03, 3.575627768554687e+03, 3.642770576171875e+03, 3.74621240234375e+03, 3.779342431640625e+03, 3.820803852539063e+03, 3.824384521484375e+03, 3.881074721679688e+03, 3.927506142578125e+03, 3.976850830078125e+03, 4.027670458984375e+03, 4.06151220703125e+03, 4.06154345703125e+03, 4.066718466796875e+03, 4.071315185546875e+03, 4.086733154296875e+03, 4.09302294921875e+03, 4.093121337890625e+03, 4.11625890625e+03, 4.13954833984375e+03, 4.13985943359375e+03, 4.14558203125e+03, 4.1464375e+03, 4.1464375e+03, 4.1464375e+03, 4.1464375e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14647998046875e+03, 4.14648193359375e+03, 4.14648193359375e+03, 4.14648193359375e+03, 4.14648193359375e+03, 4.14648193359375e+03, 4.14866259765625e+03, 4.156067041015625e+03, 4.1761005859375e+03, 4.200221807462032e+03, 4.23024443359375e+03, 4.252304931640625e+03, 4.3082319921875e+03, 4.3409935546875e+03, 4.4038283203125e+03, 4.447647568359375e+03, 4.48527431640625e+03, 4.5260245703125e+03, 4.59778712890625e+03, 4.70181986328125e+03, 4.831525703125e+03, 4.9377703125e+03, 5.02457193359375e+03, 5.142765966796875e+03, 5.26046162109375e+03, 5.3703707421875e+03, 5.508051171875e+03, 5.609557021484375e+03, 5.717878515625e+03, 5.8723162890625e+03, 6.0760662109375e+03, 6.242725341796875e+03, 6.425038203125e+03, 6.535844033203125e+03, 6.63570763671875e+03, 6.746373291015625e+03, 6.88904541015625e+03]
+AnnualHeatingLoad=[0e+00, 2.419274752807617e+02, 4.067510314941406e+02, 5.194193994140625e+02, 6.44475390625e+02, 7.911326171875e+02, 9.918130712890625e+02, 1.101696618652344e+03, 1.242738959960938e+03, 1.406675490722656e+03, 1.607335986328125e+03, 1.767362197265625e+03, 1.867717475585938e+03, 2.030192436523437e+03, 2.18788361328125e+03, 2.341244140625e+03, 2.451161044921875e+03, 2.596563930664062e+03, 2.7547321484375e+03, 2.888202255859375e+03, 2.971118310546875e+03, 3.0838019140625e+03, 3.1865309375e+03, 3.295538310546875e+03, 3.345711328125e+03, 3.394533325195312e+03, 3.509540263671875e+03, 3.575628745117187e+03, 3.642771552734375e+03, 3.746213286132812e+03, 3.779343408203125e+03, 3.820804541015625e+03, 3.82438525390625e+03, 3.881075209960938e+03, 3.927506630859375e+03, 3.976851318359375e+03, 4.027670947265625e+03, 4.0615126953125e+03, 4.0615439453125e+03, 4.066719096679687e+03, 4.071315673828125e+03, 4.086733642578125e+03, 4.09302294921875e+03, 4.093121337890625e+03, 4.1162590625e+03, 4.13954833984375e+03, 4.13985986328125e+03, 4.14558251953125e+03, 4.14643798828125e+03, 4.14643798828125e+03, 4.14643798828125e+03, 4.14643798828125e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648046875e+03, 4.14648193359375e+03, 4.14648193359375e+03, 4.14648193359375e+03, 4.14648193359375e+03, 4.14648193359375e+03, 4.1486630859375e+03, 4.156067529296875e+03, 4.17610107421875e+03, 4.200221380786361e+03, 4.2302439453125e+03, 4.25230517578125e+03, 4.30823380859375e+03, 4.340995048828125e+03, 4.4038301953125e+03, 4.447649521484375e+03, 4.48527646484375e+03, 4.5260275e+03, 4.59779005859375e+03, 4.701822666015625e+03, 4.8315286328125e+03, 4.9377732421875e+03, 5.02457486328125e+03, 5.14276931640625e+03, 5.26046455078125e+03, 5.370373955078125e+03, 5.50805419921875e+03, 5.609559951171875e+03, 5.71788107421875e+03, 5.872318955078125e+03, 6.07606865234375e+03, 6.242727783203125e+03, 6.42504064453125e+03, 6.535846474609375e+03, 6.63570986328125e+03, 6.746375732421875e+03, 6.8890478515625e+03]
 checkResultsAccordingToASHRAEHeatingOrTempMax.upperLimit=[7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03, 7.228e+03]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02, -3.25e+02]
-AnnualCoolingLoad=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -1.001171231269836e+00, -1.677864456176758e+01, -2.188740730285645e+01, -2.188740730285645e+01, -2.465415000915527e+01, -2.563814353942871e+01, -3.052769145965576e+01, -4.736412139892578e+01, -6.644913482666016e+01, -8.061882995605468e+01, -8.343758392333984e+01, -8.621833801269531e+01, -8.621833801269531e+01, -8.621833801269531e+01, -9.669728851318359e+01, -9.669728851318359e+01, -9.669728851318359e+01, -9.896501159667969e+01, -1.02013885345459e+02, -1.046993942260742e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02, -1.047727127075195e+02]
+AnnualCoolingLoad=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, -1.001171231269836e+00, -1.677866554260254e+01, -2.188739967346191e+01, -2.188739967346191e+01, -2.46541862487793e+01, -2.563819313049316e+01, -3.052772960662842e+01, -4.73641455078125e+01, -6.644937896728516e+01, -8.061918090820312e+01, -8.343796539306641e+01, -8.621878051757812e+01, -8.621878051757812e+01, -8.621878051757812e+01, -9.669796752929688e+01, -9.669796752929688e+01, -9.669796752929688e+01, -9.896570587158203e+01, -1.020145948791504e+02, -1.047001113891602e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02, -1.047734146118164e+02]
 checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[-5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01, -5.5e+01]
 checkResultsAccordingToASHRAEHeatingOrTempMax.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
 checkResultsAccordingToASHRAECoolingOrTempMin.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
-Room.thermRoom.T=[2.941499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500103759765e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500549316406e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499920654297e+02, 2.931500244140625e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500122070312e+02, 2.931499633789062e+02, 2.947706750488281e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.934412689208984e+02, 2.931500244140625e+02, 2.940896697998047e+02, 2.960121423339844e+02, 2.931500549316406e+02, 2.946215678334387e+02, 2.942469537353516e+02, 2.933939685058594e+02, 2.96273671875e+02, 2.931500244140625e+02, 2.965344146728515e+02, 2.931499938964844e+02, 2.949113537597656e+02, 2.9603931640625e+02, 2.996921484375e+02, 3.001500244140625e+02, 2.932536315917969e+02, 2.998504565429687e+02, 2.983524694824219e+02, 2.983426611328125e+02, 3.001499633789062e+02, 3.001499829101563e+02, 3.001234939804181e+02, 3.001499865722656e+02, 2.986131744384766e+02, 2.981911565720791e+02, 2.992444519042969e+02, 2.974835083007812e+02, 2.993481530761719e+02, 2.961250451660156e+02, 2.958270935058594e+02, 3.000228601074219e+02, 3.001500323486328e+02, 2.96667861328125e+02, 2.993100799560547e+02, 2.951132507324219e+02, 2.931499938964844e+02, 2.931985571289063e+02, 2.931500549316406e+02, 2.931499719238281e+02, 2.931499938964844e+02, 2.931500634765625e+02, 2.931500225830078e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02, 2.931499993896484e+02, 2.931500256347656e+02, 2.931499938964844e+02, 2.93150009765625e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499761962891e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02]
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+Room.thermRoom.T=[2.941499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500103759765e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500549316406e+02, 2.931499633789062e+02, 2.931499633789062e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499920654297e+02, 2.931500244140625e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931500549316406e+02, 2.931499938964844e+02, 2.931499633789062e+02, 2.931500122070312e+02, 2.931499633789062e+02, 2.947706750488281e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.934412689208984e+02, 2.931500244140625e+02, 2.940896697998047e+02, 2.960121228027344e+02, 2.931500549316406e+02, 2.946215678334387e+02, 2.942469537353516e+02, 2.933939685058594e+02, 2.96273671875e+02, 2.931500244140625e+02, 2.965344146728515e+02, 2.931499938964844e+02, 2.949113537597656e+02, 2.9603931640625e+02, 2.996921484375e+02, 3.001500244140625e+02, 2.932536315917969e+02, 2.998504565429687e+02, 2.983524694824219e+02, 2.983426611328125e+02, 3.001499633789062e+02, 3.001499829101563e+02, 3.001234939804181e+02, 3.001499865722656e+02, 2.986131750488281e+02, 2.981911565720791e+02, 2.992444519042969e+02, 2.974835083007812e+02, 2.993481530761719e+02, 2.961250427246094e+02, 2.958271545410156e+02, 3.000228601074219e+02, 3.001500323486328e+02, 2.96667861328125e+02, 2.993100799560547e+02, 2.951132507324219e+02, 2.931499938964844e+02, 2.931985571289063e+02, 2.931500549316406e+02, 2.931499719238281e+02, 2.931499938964844e+02, 2.931500634765625e+02, 2.931500225830078e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02, 2.931499993896484e+02, 2.931500256347656e+02, 2.931499938964844e+02, 2.93150009765625e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931499761962891e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500244140625e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02, 2.931499938964844e+02, 2.931500854492188e+02, 2.931499938964844e+02]
+Room.starRoom.T=[2.896538391113281e+02, 2.888715002441406e+02, 2.905432922363281e+02, 2.913104321289063e+02, 2.904584655761719e+02, 2.908516876220703e+02, 2.905632824707031e+02, 2.909565759277344e+02, 2.900165856933594e+02, 2.912172174072265e+02, 2.89824853515625e+02, 2.909685778808594e+02, 2.921366687011719e+02, 2.902150573730469e+02, 2.907582141113281e+02, 2.922640594482422e+02, 2.916231945800781e+02, 2.909733422851563e+02, 2.906192602539062e+02, 2.912544177246094e+02, 2.911871704101562e+02, 2.91011284790039e+02, 2.909500439453125e+02, 2.918632885742188e+02, 2.92670107421875e+02, 2.917692108154297e+02, 2.916747009277344e+02, 2.930442645263672e+02, 2.91284345703125e+02, 2.924066241455078e+02, 2.9247744140625e+02, 2.92712836303711e+02, 2.947988232421875e+02, 2.921386254882813e+02, 2.929278540039062e+02, 2.934357604980469e+02, 2.924859143066406e+02, 2.943155328369141e+02, 2.96054326171875e+02, 2.927882769775391e+02, 2.948357040077335e+02, 2.942356457519531e+02, 2.935401843261719e+02, 2.963885797119141e+02, 2.920494787597656e+02, 2.965610900878906e+02, 2.930568603515625e+02, 2.949384490966797e+02, 2.962519201660156e+02, 2.997986798095703e+02, 3.011384887695312e+02, 2.934230639648438e+02, 2.997712243652344e+02, 2.98380166015625e+02, 2.986091918945312e+02, 3.009836975097656e+02, 3.002514025878907e+02, 3.002580872831045e+02, 3.010014172363281e+02, 2.986720550537109e+02, 2.984121430151134e+02, 2.992664190673828e+02, 2.976045764160156e+02, 2.994752014160156e+02, 2.961015844726563e+02, 2.959528564453125e+02, 3.000564306640625e+02, 3.007563873291016e+02, 2.969493225097656e+02, 2.993572839355469e+02, 2.949848388671875e+02, 2.926445959472656e+02, 2.932595239257813e+02, 2.931641268150829e+02, 2.921788208007812e+02, 2.917840423583984e+02, 2.928265710449219e+02, 2.914941217041016e+02, 2.929453283691406e+02, 2.924530773925781e+02, 2.923274536132812e+02, 2.927246203613281e+02, 2.9214224609375e+02, 2.910301025390625e+02, 2.912134716796875e+02, 2.915342987060547e+02, 2.917353552246093e+02, 2.911154962158203e+02, 2.909307922363281e+02, 2.919272290039062e+02, 2.930031982421875e+02, 2.919163299560547e+02, 2.9056921875e+02, 2.909428344726563e+02, 2.904810009765625e+02, 2.905968231201172e+02, 2.905952319335938e+02, 2.910154779052734e+02, 2.917597229003906e+02, 2.904255401611328e+02, 2.909460144042969e+02]
 TransmittedSolarRadiation_room=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case900FF.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case900FF.txt
index 7d2ad9e164..a2fd90d09d 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case900FF.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case900FF.txt
@@ -3,7 +3,7 @@ statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
   "nonlinear": "13",
-  "number of continuous time states": "23",
+  "number of continuous time states": "21",
   "numerical Jacobians": "0"
 }
 time=[0e+00, 3.15396e+07]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case950.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case950.txt
index 345cc15492..39d5b5ebd0 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case950.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case950.txt
@@ -1,4 +1,4 @@
-last-generated=2022-07-06
+last-generated=2024-01-15
 statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -8,9 +8,9 @@ statistics-simulation=
 }
 time=[0e+00, 3.15396e+07]
 checkResultsAccordingToASHRAECoolingOrTempMin.lowerLimit=[-9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02, -9.21e+02]
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 checkResultsAccordingToASHRAECoolingOrTempMin.upperLimit=[-3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02, -3.87e+02]
 checkResultsAccordingToASHRAECoolingOrTempMin.satisfied=[0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case950FF.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case950FF.txt
index aeffb0c6ca..46c2700c3c 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case950FF.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_HighOrder_Validation_ASHRAE140_Case950FF.txt
@@ -3,7 +3,7 @@ statistics-simulation=
 {
   "linear": "0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
   "nonlinear": "13",
-  "number of continuous time states": "23",
+  "number of continuous time states": "21",
   "numerical Jacobians": "0"
 }
 time=[0e+00, 3.15396e+07]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_FreeFloating.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_FreeFloating.txt
new file mode 100644
index 0000000000..2d2f13970f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_FreeFloating.txt
@@ -0,0 +1,10 @@
+last-generated=2023-02-13
+statistics-simulation=
+{
+  "linear": "2",
+  "nonlinear": "1",
+  "number of continuous time states": "1",
+  "numerical Jacobians": "0"
+}
+time=[8.64e+06, 9.504e+06]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_FreeFloatingHVAC.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_FreeFloatingHVAC.txt
new file mode 100644
index 0000000000..5a0a4c66ed
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_FreeFloatingHVAC.txt
@@ -0,0 +1,10 @@
+last-generated=2023-02-13
+statistics-simulation=
+{
+  "linear": "0",
+  "nonlinear": "1",
+  "number of continuous time states": "4",
+  "numerical Jacobians": "0"
+}
+time=[8.64e+06, 9.504e+06]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_HeatingCooling.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_HeatingCooling.txt
new file mode 100644
index 0000000000..7b646388b3
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_HeatingCooling.txt
@@ -0,0 +1,10 @@
+last-generated=2023-02-13
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "2, 1",
+  "number of continuous time states": "3",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_HeatingCoolingHVAC.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_HeatingCoolingHVAC.txt
new file mode 100644
index 0000000000..85ea848678
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Examples_HeatingCoolingHVAC.txt
@@ -0,0 +1,10 @@
+last-generated=2023-02-13
+statistics-simulation=
+{
+  "linear": "0",
+  "nonlinear": "1",
+  "number of continuous time states": "5",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case600.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case600.txt
new file mode 100644
index 0000000000..bbdaaed85d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case600.txt
@@ -0,0 +1,11 @@
+last-generated=2023-01-16
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": "2, 1",
+  "number of continuous time states": "5",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case600FF.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case600FF.txt
new file mode 100644
index 0000000000..9f3eef498d
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case600FF.txt
@@ -0,0 +1,14 @@
+last-generated=2023-01-16
+statistics-initialization=
+{
+  "linear": "2"
+}
+statistics-simulation=
+{
+  "linear": "2",
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+  "number of continuous time states": "2",
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case900.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case900.txt
new file mode 100644
index 0000000000..b9a65b3c2f
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case900.txt
@@ -0,0 +1,11 @@
+last-generated=2023-01-16
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+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case900FF.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case900FF.txt
new file mode 100644
index 0000000000..977f8edc39
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ISO13790_Validation_BESTEST_Case900FF.txt
@@ -0,0 +1,14 @@
+last-generated=2023-01-16
+statistics-initialization=
+{
+  "linear": "2"
+}
+statistics-simulation=
+{
+  "linear": "2",
+  "nonlinear": "1",
+  "number of continuous time states": "2",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_Multizone.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_Multizone.txt
new file mode 100644
index 0000000000..cd1398fdc0
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_Multizone.txt
@@ -0,0 +1,19 @@
+last-generated=2024-07-19
+statistics-initialization=
+{
+  "linear": "5, 5, 5, 5, 5"
+}
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+  "nonlinear": "0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0,   1, 0, 1",
+  "number of continuous time states": "35",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneEquipped.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneEquipped.txt
new file mode 100644
index 0000000000..b9efb51967
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneEquipped.txt
@@ -0,0 +1,23 @@
+last-generated=2024-07-25
+statistics-initialization=
+{
+  "linear": "5, 5, 5, 5, 5"
+}
+statistics-simulation=
+{
+  "linear": "0, 4, 0, 0, 4, 0, 0, 4, 0, 0, 4, 0, 0, 4, 0",
+  "nonlinear": "1, 1, 0, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1,   0, 1, 0, 1, 0, 1",
+  "number of continuous time states": "35",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 8.64e+05]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneMoistAirCO2Equipped.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneMoistAirCO2Equipped.txt
index a2bc301a6c..fd60f1ff92 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneMoistAirCO2Equipped.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneMoistAirCO2Equipped.txt
@@ -1,7 +1,7 @@
-last-generated=2022-01-27
+last-generated=2024-07-25
 statistics-initialization=
 {
-  "linear": "5, 4, 4, 4, 4"
+  "linear": "5, 5, 5, 5, 5"
 }
 statistics-simulation=
 {
@@ -10,6 +10,14 @@ statistics-simulation=
   "number of continuous time states": "45",
   "numerical Jacobians": "0"
 }
-time=[0e+00, 3.1536e+07]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneMoistAirCO2EquippedSwimmingFacility.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneMoistAirCO2EquippedSwimmingFacility.txt
new file mode 100644
index 0000000000..2edd47372a
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizoneMoistAirCO2EquippedSwimmingFacility.txt
@@ -0,0 +1,17 @@
+last-generated=2023-09-21
+statistics-initialization=
+{
+  "linear": "0, 0, 0, 0, 0",
+  "nonlinear": "0, 0, 9, 1, 1",
+  "numerical Jacobians": "0"
+}
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+  "number of continuous time states": "86",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizonePartlyCooled.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizonePartlyCooled.txt
new file mode 100644
index 0000000000..9bd12370a3
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_MultizonePartlyCooled.txt
@@ -0,0 +1,23 @@
+last-generated=2024-07-19
+statistics-initialization=
+{
+  "linear": "5, 5, 5, 5, 5"
+}
+statistics-simulation=
+{
+  "linear": "0, 4, 0, 0, 4, 0, 0, 4, 0, 0, 4, 0, 0, 4, 0",
+  "nonlinear": "0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0, 1, 0,   1, 0, 1",
+  "number of continuous time states": "39",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_SimpleRoomTwoElementsNonConstantTGround.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_SimpleRoomTwoElementsNonConstantTGround.txt
new file mode 100644
index 0000000000..00558d83d5
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_SimpleRoomTwoElementsNonConstantTGround.txt
@@ -0,0 +1,14 @@
+last-generated=2023-09-14
+statistics-initialization=
+{
+  "linear": "5"
+}
+statistics-simulation=
+{
+  "linear": "0, 3, 0",
+  "nonlinear": " ",
+  "number of continuous time states": "4",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 3.1536e+07]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_ThermalZoneMoistAirSwimmingPool.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_ThermalZoneMoistAirSwimmingPool.txt
new file mode 100644
index 0000000000..8fc82a2edf
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_ThermalZones_ReducedOrder_Examples_ThermalZoneMoistAirSwimmingPool.txt
@@ -0,0 +1,16 @@
+last-generated=2023-09-21
+statistics-initialization=
+{
+  "nonlinear": "0, 0, 8, 1, 1",
+  "numerical Jacobians": "0"
+}
+statistics-simulation=
+{
+  "linear": "13, 6, 6, 0, 0, 13, 6, 6",
+  "nonlinear": "6, 0, 1, 0, 1, 0, 1, 1, 1",
+  "number of continuous time states": "25",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Clustering_Validation_KMeans_1d.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Clustering_Validation_KMeans_1d.txt
new file mode 100644
index 0000000000..0d077bdb12
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Clustering_Validation_KMeans_1d.txt
@@ -0,0 +1,9 @@
+last-generated=2022-09-12
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
+cmp=[1e+00, 1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Clustering_Validation_KMeans_2d.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Clustering_Validation_KMeans_2d.txt
new file mode 100644
index 0000000000..0d077bdb12
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Clustering_Validation_KMeans_2d.txt
@@ -0,0 +1,9 @@
+last-generated=2022-09-12
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
+cmp=[1e+00, 1e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Examples_WeeklySchedule.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Examples_WeeklySchedule.txt
new file mode 100644
index 0000000000..29cae8c8ac
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Examples_WeeklySchedule.txt
@@ -0,0 +1,12 @@
+last-generated=2023-05-09
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Examples_WeeklySchedule7to19.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Examples_WeeklySchedule7to19.txt
new file mode 100644
index 0000000000..e0ff80ae88
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Examples_WeeklySchedule7to19.txt
@@ -0,0 +1,9 @@
+last-generated=2022-04-26
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1.2096e+06]
+sch.y[1]=[0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 1e+00, 1e+00, 1e+00, 1e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00, 0e+00]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Validation_WeeklyScheduleWindowsLineEndings.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Validation_WeeklyScheduleWindowsLineEndings.txt
new file mode 100644
index 0000000000..cb6e638234
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_IO_Files_Validation_WeeklyScheduleWindowsLineEndings.txt
@@ -0,0 +1,12 @@
+last-generated=2024-04-02
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[-1e+04, 1e+06]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Math_Examples_Interpolate.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Math_Examples_Interpolate.txt
new file mode 100644
index 0000000000..b7c14e9f57
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Math_Examples_Interpolate.txt
@@ -0,0 +1,9 @@
+last-generated=2024-02-29
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 5e+02]
+int.y=[-8.709000051021576e-02, -8.607897162437439e-02, -8.508513867855072e-02, -8.410613983869553e-02, -8.313964307308197e-02, -8.218330889940262e-02, -8.123478293418884e-02, -8.029171824455261e-02, -7.935179024934769e-02, -7.841263711452484e-02, -7.747191935777664e-02, -7.652729749679565e-02, -7.557642459869385e-02, -7.461696118116379e-02, -7.364656031131744e-02, -7.266288250684738e-02, -7.166357338428497e-02, -7.064630091190338e-02, -6.960871070623398e-02, -6.854847073554993e-02, -6.74632266163826e-02, -6.635063886642456e-02, -6.520836800336838e-02, -6.403406709432602e-02, -6.282539665699005e-02, -6.157999858260155e-02, -6.03080615401268e-02, -5.901877209544182e-02, -5.770833417773247e-02, -5.637295171618462e-02, -5.500881373882294e-02, -5.36121279001236e-02, -5.217909067869186e-02, -5.070589855313301e-02, -4.918875172734261e-02, -4.762385040521622e-02, -4.600739479064941e-02, -4.433558508753777e-02, -4.260461404919624e-02, -4.081068560481071e-02, -3.894999995827675e-02, -3.698130697011948e-02, -3.486191853880882e-02, -3.258588165044785e-02, -3.014722652733326e-02, -2.754000015556812e-02, -2.463850006461143e-02, -2.133000083267689e-02, -1.741999946534634e-02, -1.231999974697828e-02, 0e+00, 1.231999974697828e-02, 1.741999946534634e-02, 2.133000083267689e-02, 2.528040856122971e-02, 2.613032609224319e-02, 2.613095752894878e-02, 2.613155916333199e-02, 2.61321347206831e-02, 2.613268233835697e-02, 2.613320574164391e-02, 2.613370306789875e-02, 2.613417431712151e-02, 2.613462321460247e-02, 2.613504603505135e-02, 2.613544836640358e-02, 2.613582648336887e-02, 2.613618411123753e-02, 2.613652125000954e-02, 2.613683789968491e-02, 2.613713406026363e-02, 2.613740973174572e-02, 2.613766863942146e-02, 2.613791078329086e-02, 2.613813430070877e-02, 2.613834105432034e-02, 2.613853104412556e-02, 2.613870799541473e-02, 2.613886818289757e-02, 2.613901719450951e-02, 2.61391494423151e-02, 2.61392705142498e-02, 2.613938041031361e-02, 2.613947726786137e-02, 2.613956481218338e-02, 2.61396411806345e-02, 2.613970823585987e-02, 2.61397659778595e-02, 2.613981626927853e-02, 2.613985724747181e-02, 2.613989263772964e-02, 2.613992244005203e-02, 2.613994479179382e-02, 2.613996341824532e-02, 2.613997645676136e-02, 2.613998576998711e-02, 2.61399932205677e-02, 2.6139996945858e-02, 2.613999880850315e-02, 2.61400006711483e-02, 2.61400006711483e-02]
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_Multizone_BaseClasses_Examples_Interpolate.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Math_Functions_Examples_Interpolate.txt
similarity index 100%
rename from AixLib/Resources/ReferenceResults/Dymola/AixLib_Airflow_Multizone_BaseClasses_Examples_Interpolate.txt
rename to AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Math_Functions_Examples_Interpolate.txt
diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Math_Functions_Examples_SmoothInterpolation.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Math_Functions_Examples_SmoothInterpolation.txt
new file mode 100644
index 0000000000..3d5f847c71
--- /dev/null
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Math_Functions_Examples_SmoothInterpolation.txt
@@ -0,0 +1,14 @@
+last-generated=2022-10-19
+statistics-simulation=
+{
+  "linear": " ",
+  "nonlinear": " ",
+  "numerical Jacobians": "0"
+}
+time=[0e+00, 1e+00]
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diff --git a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Sensors_Examples_ExergyMeters.txt b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Sensors_Examples_ExergyMeters.txt
index cd2d84490d..15c418f932 100644
--- a/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Sensors_Examples_ExergyMeters.txt
+++ b/AixLib/Resources/ReferenceResults/Dymola/AixLib_Utilities_Sensors_Examples_ExergyMeters.txt
@@ -1,4 +1,4 @@
-last-generated=2022-05-19
+last-generated=2024-07-19
 statistics-simulation=
 {
   "linear": "0, 0, 0, 13, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0",
@@ -7,5 +7,5 @@ statistics-simulation=
   "numerical Jacobians": "0"
 }
 time=[0e+00, 7.2e+03]
-calcExergyDestructionLoss_1.y=[-2.809915161132812e+01, 8.47181396484375e+02, 4.796566162109375e+02, 3.260004272460938e+02, 2.576920166015625e+02, 2.231594696044922e+02, 2.021144409179688e+02, 1.834994201660156e+02, 1.646245269775391e+02, 1.443641510009766e+02, 1.229949111938477e+02, 9.982244873046875e+01, 7.537297821044922e+01, 5.028591156005859e+01, 2.531649398803707e+01, -2.157377898693085e-01, -2.555892372131348e+01, -5.01982421875e+01, -7.373641204833984e+01, -9.586761474609375e+01, -1.160231552124023e+02, -1.338829345703125e+02, -1.495463104248047e+02, -1.624952392578125e+02, -1.721825408935547e+02, -1.784967346191406e+02, -1.819301452636719e+02, -1.822144012451172e+02, -1.79369140625e+02, -1.734698181152344e+02, -1.644579925537109e+02, -1.525889282226562e+02, -1.380698547363281e+02, -1.211239776611328e+02, -1.020287704467773e+02, -8.110501861572266e+01, -5.866793060302734e+01, -3.503179931640625e+01, -1.054138469696045e+01, 1.443301105499268e+01, 3.952675247192383e+01, 6.436393737792969e+01, 8.857762145996094e+01, 1.11791618347168e+02, 1.336641693115234e+02, 1.538517761230469e+02, 1.720440216064453e+02, 1.879901733398438e+02, 2.013853607177734e+02, 2.119829406738281e+02, 2.196073913574219e+02, 2.241714935302734e+02, 2.255471496582031e+02, 2.236181335449219e+02, 2.184808349609374e+02, 2.101358032226562e+02, 1.986631622314452e+02, 1.842591400146484e+02, 1.671931915283203e+02, 1.477256927490234e+02, 1.265347747802734e+02, 1.037881927490234e+02, 7.932408905029297e+01, 5.379601287841797e+01, 2.764523315429688e+01, 1.357666254043579e+00, -2.461800003051758e+01, -4.983815765380859e+01, -7.405979156494141e+01, -9.668334197998047e+01, -1.17383056640625e+02, -1.358478393554688e+02, -1.519288024902344e+02, -1.651790161132812e+02, -1.750903778076172e+02, -1.818320770263672e+02, -1.8538330078125e+02, -1.857389221191406e+02, -1.828680572509766e+02, -1.768624725341797e+02, -1.678009490966797e+02, -1.558663330078125e+02, -1.412315521240234e+02, -1.241742324829102e+02, -1.049456329345703e+02, -8.383344268798828e+01, -6.118498992919922e+01, -3.733578109741211e+01, -1.264315319061279e+01, 1.252662086486816e+01, 3.778979110717773e+01, 6.278577423095703e+01, 8.714192199707031e+01, 1.104809799194336e+02, 1.324539337158203e+02, 1.527316284179688e+02, 1.710111999511719e+02, 1.86972900390625e+02, 2.0039208984375e+02, 2.110257720947266e+02, 2.187105255126953e+02]
-calcExergyDestructionLoss_2.y=[-2.809915161132812e+01, 8.622514038085938e+02, 4.989183654785156e+02, 3.490438232421875e+02, 2.845926513671875e+02, 2.541740570068359e+02, 2.360304107666016e+02, 2.205071563720703e+02, 2.044441070556641e+02, 1.865298004150391e+02, 1.669261016845703e+02, 1.448824615478516e+02, 1.208854904174805e+02, 9.552924346923828e+01, 6.958940124511714e+01, 4.241501617431641e+01, 1.481691932678223e+01, -1.261092090606689e+01, -3.937111282348633e+01, -6.505409240722656e+01, -8.896519470214844e+01, -1.106668548583984e+02, -1.301229095458984e+02, -1.46681640625e+02, -1.597450103759766e+02, -1.691152648925781e+02, -1.752163391113281e+02, -1.777585296630859e+02, -1.767468414306641e+02, -1.722724761962891e+02, -1.642881011962891e+02, -1.531078643798828e+02, -1.389845581054688e+02, -1.222003936767578e+02, -1.031001510620117e+02, -8.205540466308594e+01, -5.942817687988281e+01, -3.557367324829102e+01, -1.085197257995605e+01, 1.43596658706665e+01, 3.970915222167969e+01, 6.485508728027344e+01, 8.946418762207031e+01, 1.132248611450195e+02, 1.358383483886719e+02, 1.570177612304688e+02, 1.765024719238281e+02, 1.940748901367188e+02, 2.094540405273438e+02, 2.224116821289062e+02, 2.327558898925781e+02, 2.403565216064453e+02, 2.450279388427734e+02, 2.465868682861328e+02, 2.45028823852539e+02, 2.402498168945312e+02, 2.321867065429687e+02, 2.209736175537109e+02, 2.067260437011719e+02, 1.89601806640625e+02, 1.701785430908203e+02, 1.485802307128906e+02, 1.245701065063477e+02, 9.878471374511719e+01, 7.168146514892578e+01, 4.376366424560547e+01, 1.554234027862549e+01, -1.246404647827148e+01, -3.990685653686523e+01, -6.6071044921875e+01, -9.050305938720703e+01, -1.12770133972168e+02, -1.325677947998047e+02, -1.494968566894531e+02, -1.627771301269531e+02, -1.725706481933594e+02, -1.787881622314453e+02, -1.813877563476562e+02, -1.803478851318359e+02, -1.757490539550781e+02, -1.677048492431641e+02, -1.564477233886719e+02, -1.422055358886719e+02, -1.253022308349609e+02, -1.060629348754883e+02, -8.482801818847656e+01, -6.198830795288086e+01, -3.791233825683594e+01, -1.298471164703369e+01, 1.242741680145264e+01, 3.796009063720703e+01, 6.3273681640625e+01, 8.803018951416016e+01, 1.119176712036133e+02, 1.346383209228516e+02, 1.559082641601562e+02, 1.754772338867188e+02, 1.930710906982422e+02, 2.084809417724609e+02, 2.214705505371094e+02, 2.318709411621094e+02]
+calcExergyDestructionLoss_1.y=[-2.809915161132812e+01, 8.47181396484375e+02, 4.796634826660156e+02, 3.259949035644531e+02, 2.576996154785156e+02, 2.231523590087891e+02, 2.021178131103516e+02, 1.834868774414062e+02, 1.646134033203125e+02, 1.443696136474609e+02, 1.230537261962891e+02, 9.99530029296875e+01, 7.556234741210938e+01, 5.026644515991211e+01, 2.448601341247555e+01, -1.204262375831604e+00, -2.582668113708496e+01, -5.035812759399414e+01, -7.385865020751953e+01, -9.596932983398438e+01, -1.160789260864258e+02, -1.3404248046875e+02, -1.494683990478516e+02, -1.621127471923828e+02, -1.719203491210938e+02, -1.785994262695312e+02, -1.820501251220703e+02, -1.822846069335938e+02, -1.793245849609375e+02, -1.732821960449219e+02, -1.642214965820312e+02, -1.523199462890625e+02, -1.377820739746094e+02, -1.208354339599609e+02, -1.019171905517578e+02, -8.157322692871094e+01, -5.942579650878906e+01, -3.591634368896484e+01, -1.151514530181885e+01, 1.339921188354492e+01, 3.84677619934082e+01, 6.329604721069336e+01, 8.751224517822266e+01, 1.108303833007812e+02, 1.329167175292969e+02, 1.532299957275391e+02, 1.716201477050781e+02, 1.875839385986328e+02, 2.014080047607422e+02, 2.123533935546875e+02, 2.199942169189453e+02, 2.243719482421875e+02, 2.256347045898438e+02, 2.236702423095703e+02, 2.184777069091796e+02, 2.101208953857421e+02, 1.986841735839843e+02, 1.8434912109375e+02, 1.673193511962891e+02, 1.478686676025391e+02, 1.263147277832031e+02, 1.029880218505859e+02, 7.828522491455078e+01, 5.261427688598633e+01, 2.639907455444336e+01, 8.36091935634613e-02, -2.590721130371094e+01, -5.112687683105469e+01, -7.516878509521484e+01, -9.763808441162109e+01, -1.181710968017578e+02, -1.364338684082031e+02, -1.521454772949219e+02, -1.650689849853516e+02, -1.750023956298828e+02, -1.818078002929688e+02, -1.854102172851562e+02, -1.857574157714844e+02, -1.828742828369141e+02, -1.768378601074219e+02, -1.677526397705078e+02, -1.557853088378906e+02, -1.411383209228516e+02, -1.240469589233398e+02, -1.047922286987305e+02, -8.36636962890625e+01, -6.099855422973633e+01, -3.713516235351562e+01, -1.243287658691406e+01, 1.273874568939209e+01, 3.801607131958008e+01, 6.301175689697266e+01, 8.735373687744141e+01, 1.106902236938477e+02, 1.326552124023438e+02, 1.529287872314453e+02, 1.7118212890625e+02, 1.871344299316406e+02, 2.005378112792969e+02, 2.111460113525391e+02, 2.187969055175781e+02]
+calcExergyDestructionLoss_2.y=[-2.809915161132812e+01, 8.622514038085938e+02, 4.989249267578125e+02, 3.490461120605469e+02, 2.845937805175781e+02, 2.541727294921875e+02, 2.360346374511719e+02, 2.204941253662109e+02, 2.044332275390625e+02, 1.865338745117188e+02, 1.669810638427734e+02, 1.450214996337891e+02, 1.210759124755859e+02, 9.551406860351562e+01, 6.876628875732418e+01, 4.142972183227539e+01, 1.454091739654541e+01, -1.277441310882568e+01, -3.949267578125e+01, -6.515564727783203e+01, -8.902238464355469e+01, -1.108181610107422e+02, -1.300212097167969e+02, -1.462823944091797e+02, -1.594745635986328e+02, -1.692169799804688e+02, -1.753429870605469e+02, -1.778391876220703e+02, -1.767054901123047e+02, -1.720782012939453e+02, -1.640472106933594e+02, -1.528288269042969e+02, -1.386859588623047e+02, -1.219052658081055e+02, -1.029802322387695e+02, -8.251397705078125e+01, -6.018574142456055e+01, -3.64642448425293e+01, -1.183643627166748e+01, 1.331779003143311e+01, 3.865212249755859e+01, 6.379570388793945e+01, 8.841100311279297e+01, 1.122660675048828e+02, 1.350898132324219e+02, 1.563933715820312e+02, 1.760798797607422e+02, 1.937059020996094e+02, 2.095054168701172e+02, 2.227671051025391e+02, 2.331306915283203e+02, 2.405553283691406e+02, 2.451112518310547e+02, 2.466316986083984e+02, 2.450201416015625e+02, 2.402198486328125e+02, 2.322183074951171e+02, 2.210651397705078e+02, 2.068520660400391e+02, 1.897458343505859e+02, 1.699668273925781e+02, 1.477844696044922e+02, 1.235369110107422e+02, 9.761115264892578e+01, 7.043798828125e+01, 4.248730850219727e+01, 1.425081729888916e+01, -1.375411605834961e+01, -4.101377868652344e+01, -6.70220947265625e+01, -9.129151916503906e+01, -1.133701553344727e+02, -1.328534545898438e+02, -1.493925323486328e+02, -1.626988830566406e+02, -1.725513458251953e+02, -1.7881298828125e+02, -1.814105529785156e+02, -1.803551788330078e+02, -1.757235565185547e+02, -1.676592864990234e+02, -1.563698120117188e+02, -1.421101226806641e+02, -1.251781234741211e+02, -1.059103012084961e+02, -8.466011810302734e+01, -6.180182647705078e+01, -3.771475601196289e+01, -1.277590942382812e+01, 1.264320278167725e+01, 3.818407440185547e+01, 6.349774932861328e+01, 8.824974060058594e+01, 1.12130973815918e+02, 1.348414154052734e+02, 1.561047515869141e+02, 1.756492462158203e+02, 1.932305145263672e+02, 2.086177673339844e+02, 2.215928802490234e+02, 2.319580078125e+02]
diff --git a/AixLib/Resources/Scripts/ConvertAixLib_from_1.4.0_to_1.4.1.mos b/AixLib/Resources/Scripts/ConvertAixLib_from_1.4.0_to_1.4.1.mos
new file mode 100644
index 0000000000..59309f1506
--- /dev/null
+++ b/AixLib/Resources/Scripts/ConvertAixLib_from_1.4.0_to_1.4.1.mos
@@ -0,0 +1,19 @@
+clear
+
+convertClear();
+
+
+// Rename Buffer and standard storage
+//convertClass("AixLib.Fluid.Storage.BufferStorage", "AixLib.Fluid.Storage.StorageDetailed");
+convertClass("AixLib.Fluid.Storage.Storage", "AixLib.Fluid.Storage.StorageSimple");
+
+//Rename data base due to renaming of buffer storage
+convertClass("AixLib.DataBase.Storage.BufferStorageBaseDataDefinition", "AixLib.DataBase.Storage.StorageDetailedBaseDataDefinition");
+convertClass("AixLib.Fluid.Storage.Examples.BufferStorage", "AixLib.Fluid.Storage.Examples.StorageDetailedExample");
+
+// add the parameters heaLoadFacOut and heaLoadFacGrd for dynamic heat load calculation with dummy values of zero
+convertElement("AixLib.Fluid.DistrictHeatingCooling.Pipes.DHCPipe", "pipCor", "floPip");
+
+
+// T_start array: Does not work
+//convertModifiers("AixLib.Fluid.Storage.Examples.StorageDetailed", {"TStart=293.15"}, {"TStart=fill(%TStart%, 5)"});
diff --git a/AixLib/Resources/Scripts/ConvertAixLib_from_1.4.1_to_2.0.0.mos b/AixLib/Resources/Scripts/ConvertAixLib_from_1.4.1_to_2.0.0.mos
new file mode 100644
index 0000000000..af88ce0527
--- /dev/null
+++ b/AixLib/Resources/Scripts/ConvertAixLib_from_1.4.1_to_2.0.0.mos
@@ -0,0 +1,22 @@
+clear
+
+convertClear();
+
+// Changes from IBPSA
+
+// Conversion for https://github.com/ibpsa/modelica-ibpsa/issues/1885
+convertModifiers("AixLib.Fluid.Geothermal.Borefields.BaseClasses.PartialBorefield",
+                {"dynFil"}, fill("",0), true);
+convertModifiers("AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.OneUTube",
+                {"dynFil"}, fill("",0), true);
+convertModifiers("AixLib.Fluid.Geothermal.Borefields.BaseClasses.Boreholes.TwoUTube",
+                {"dynFil"}, fill("",0), true);
+
+
+// Conversion for https://github.com/ibpsa/modelica-ibpsa/issues/1614
+convertModifiers("AixLib.Fluid.Storage.ExpansionVessel", {"p"}, fill("",0), true);
+
+
+// Moved models due to deletion in IBPSA
+convertClass("AixLib.Airflow.Multizone.BaseClasses", "AixLib.Obsolete.Year2024.Airflow.Multizone.BaseClasses.interpolate");
+convertClass("AixLib.Fluid.Movers.SpeedControlled_Nrpm", "AixLib.Obsolete.Year2024.Fluid.Movers.SpeedControlled_Nrpm");
diff --git a/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/OneOpenDoor.mos b/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/OneOpenDoor.mos
index 57274c2560..8f37a7fcc3 100644
--- a/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/OneOpenDoor.mos
+++ b/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/OneOpenDoor.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.Airflow.Multizone.Examples.OneOpenDoor", stopTime=7200, method="dassl", tolerance=1e-06, resultFile="OneOpenDoor");
+simulateModel("AixLib.Airflow.Multizone.Examples.OneOpenDoor", stopTime=7200, method="CVode", tolerance=1e-06, resultFile="OneOpenDoor");
 removePlots();
 createPlot(id = 4,
  position = {73, 34, 537, 565},
diff --git a/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/TrickleVent.mos b/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/TrickleVent.mos
index 014630b1d1..aa380e7711 100644
--- a/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/TrickleVent.mos
+++ b/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/Examples/TrickleVent.mos
@@ -1,3 +1,3 @@
-simulateModel("AixLib.Airflow.Multizone.Examples.TrickleVent", stopTime=2592000, numberOfIntervals=0, outputInterval=600, tolerance=1e-06, resultFile="TrickleVent");
+simulateModel("AixLib.Airflow.Multizone.Examples.TrickleVent", stopTime=2592000, numberOfIntervals=0, outputInterval=600, tolerance=1e-06, resultFile="TrickleVent");
 createPlot(id=1, position={55, 55, 584, 361}, y={"tabDat_m_flow.m_flow", "tabDat_V_flow.V_flow"}, range={0.0, 2600000.0, -0.08, 0.039999999999999994}, grid=true, filename="TrickleVent.mat", colors={{28,108,200}, {0,0,0}}, displayUnits={"kg/s", "m3/s"});
 createPlot(id=1, position={55, 55, 584, 361}, x="tabDat_m_flow.dp", y={"tabDat_V_flow.V_flow", "tabDat_m_flow.m_flow"}, range={-35.0, 45.0, -0.08, 0.039999999999999994}, grid=true, subPlot=102, colors={{238,46,47}, {28,108,200}}, patterns={LinePattern.None, LinePattern.None}, markers={MarkerStyle.Cross, MarkerStyle.Cross}, timeUnit="Pa", displayUnits={"m3/s", "kg/s"});
diff --git a/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/OpeningArea.mos b/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/OpeningArea.mos
new file mode 100644
index 0000000000..018a35b9d3
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/OpeningArea.mos
@@ -0,0 +1,134 @@
+simulateModel("AixLib.Airflow.WindowVentilation.Examples.OpeningArea", startTime=0, stopTime=60, outputInterval=1, method="dassl", tolerance=1e-6, resultFile="OpeningArea");
+createPlot(
+	id=1,
+	position={0, 0, 1200, 600},
+	y={"opnSimp.A", "opnSimpVDI2078.A"},
+	heading="Simple opening",
+	range={0.0, 60.0, 0.4, 1.6},
+	grid=true,
+	colors={{28,108,200}, {238,46,47}},
+	timeUnit="s",
+	displayUnits={"m2", "m2"});
+createPlot(
+	id=2,
+	position={50, 50, 1200, 600},
+	y={"opnSasSdHunInGeo.A", "opnSasSdHunInPrj.A", "opnSasSdHunInEqv.A", "opnSasSdHunInEff.A", "opnSasSdHunOutGeo.A"},
+	heading="Sash opening common 1",
+	range={0.0, 60.0, -0.5, 1.5},
+	grid=true,
+	subPlot=101,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}},
+	timeUnit="s",
+	displayUnits={"m2", "m2", "m2", "m2", "m2"});
+createPlot(
+	id=2,
+	position={50, 50, 1200, 600},
+	y={"opnSasBtmHunInGeo.A", "opnSasBtmHunInPrj.A", "opnSasBtmHunInEqv.A", "opnSasBtmHunInEff.A", "opnSasTopHunOutPrj.A"},
+	range={0.0, 60.0, -0.5, 1.5},
+	grid=true,
+	subPlot=102,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}},
+	timeUnit="s",
+	displayUnits={"m2", "m2", "m2", "m2", "m2"});
+createPlot(
+	id=2,
+	position={50, 50, 1200, 600},
+	y={"opnSasPivVerGeo.A", "opnSasPivVerPrj.A", "opnSasPivVerEqv.A", "opnSasPivVerEff.A"},
+	range={0.0, 60.0, -1.0, 2.0},
+	grid=true,
+	subPlot=103,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}},
+	timeUnit="s",
+	displayUnits={"m2", "m2", "m2", "m2"});
+createPlot(
+	id=2,
+	position={50, 50, 1200, 600},
+	y={"opnSasPivHorGeo.A", "opnSasPivHorPrj.A", "opnSasPivHorEqv.A", "opnSasPivHorEff.A"},
+	range={0.0, 60.0, -1.0, 2.0},
+	grid=true,
+	subPlot=104,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}},
+	timeUnit="s",
+	displayUnits={"m2", "m2", "m2", "m2"});
+createPlot(
+	id=3,
+	position={100, 100, 1200, 600},
+	y={"opnSasSldVerGeo.A"},
+	heading="Sash opening common 2",
+	range={0.0, 60.0, -0.2, 0.6},
+	grid=true,
+	subPlot=101,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m2"});
+createPlot(
+	id=3,
+	position={100, 100, 1200, 600},
+	y={"opnSasSldHorGeo.A"},
+	range={0.0, 60.0, -0.5, 1.0},
+	grid=true,
+	subPlot=102,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m2"});
+createPlot(
+	id=3,
+	position={100, 100, 1200, 600},
+	y={"opnSasPivHorEffPre.A"},
+	range={0.0, 60.0, 1.1, 1.4},
+	grid=true,
+	subPlot=103,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m2"});
+createPlot(
+	id=3,
+	position={100, 100, 1200, 600},
+	y={"opnSasAngBtmHunInGeo.A"},
+	range={0.0, 60.0, -1.0, 2.0},
+	grid=true,
+	subPlot=104,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m2"});
+createPlot(
+	id=4,
+	position={150, 150, 1200, 600},
+	y={"opnSasBtmHunInDIN16798.A"},
+	heading="Sash opening special",
+	range={0.0, 60.0, -0.2, 0.6},
+	grid=true,
+	subPlot=101,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m2"});
+createPlot(
+	id=4,
+	position={150, 150, 1200, 600},
+	y={"opnSasSdHunInDIN4108.A", "opnSasBtmHunInDIN4108.A", "opnSasPivHorDIN4108.A"},
+	range={0.0, 60.0, -0.5, 1.5},
+	grid=true,
+	subPlot=102,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}},
+	timeUnit="s",
+	displayUnits={"m2", "m2", "m2"});
+createPlot(
+	id=4,
+	position={150, 150, 1200, 600},
+	y={"opnSasBtmHunInHall.A"},
+	range={0.0, 60.0, -0.1, 0.2},
+	grid=true,
+	subPlot=103,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m2"});
+createPlot(
+	id=4,
+	position={150, 150, 1200, 600},
+	y={"opnSasBtmHunInVDI2078.A"},
+	range={0.0, 60.0, -0.1, 0.3},
+	grid=true,
+	subPlot=104,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m2"});
diff --git a/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/VentilationFlowRateSashOpening.mos b/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/VentilationFlowRateSashOpening.mos
new file mode 100644
index 0000000000..43cf733f87
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/VentilationFlowRateSashOpening.mos
@@ -0,0 +1,72 @@
+simulateModel("AixLib.Airflow.WindowVentilation.Examples.VentilationFlowRateSashOpening", startTime=0, stopTime=180, outputInterval=0.1, method="dassl", tolerance=1e-6, resultFile="VentilationFlowRateSashOpening");
+createPlot(
+	id=1,
+	position={10, 24, 600, 400},
+	y={"TRoomSet.y", "TAmbSet.y"},
+	heading="Boundary conditions",
+	range={0.0, 180.0, -10.0, 50.0},
+	grid=true,
+	subPlot=101,
+	colors={{28,108,200}, {238,46,47}},
+	timeUnit="s",
+	displayUnits={"degC", "degC"});
+createPlot(
+	id=1,
+	position={10, 24, 600, 400},
+	y={"winSpe10Set.y"},
+	range={0.0, 180.0, -5.0, 25.0},
+	grid=true,
+	subPlot=102,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m/s"});
+createPlot(
+	id=1,
+	position={10, 24, 600, 400},
+	y={"winDirSet.y"},
+	range={0.0, 180.0, -400.0, 400.0},
+	grid=true,
+	subPlot=103,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"deg"});
+createPlot(
+	id=2,
+	position={20, 48, 600, 400},
+	y={"warrenParkins.V_flow", "gidsPhaff.V_flow", "larsenHeiselberg.V_flow", "caciolo.V_flow", "tang.V_flow"},
+	heading="Volume flow 1",
+	range={0.0, 180.0, -0.05, 0.55},
+	grid=true,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}},
+	timeUnit="s",
+	displayUnits={"m3/s", "m3/s", "m3/s", "m3/s", "m3/s"});
+createPlot(
+	id=3,
+	position={30, 72, 600, 400},
+	y={"maas.V_flow", "hall.V_flow", "jiang.V_flow", "din16798_1.V_flow", "din4108_1.V_flow"},
+	heading="Volume flow 2",
+	range={0.0, 180.0, -0.1, 0.7},
+	grid=true,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}},
+	timeUnit="s",
+	displayUnits={"m3/s", "m3/s", "m3/s", "m3/s", "m3/s"});
+createPlot(
+	id=4,
+	position={40, 96, 600, 400},
+	y={"din16798_1.V_flow", "vdi2078_2.V_flow", "vdi2078_3.V_flow"},
+	heading="Volume flow VDI 2078",
+	range={0.0, 180.0, -0.01, 0.08},
+	grid=true,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}},
+	timeUnit="s",
+	displayUnits={"m3/s", "m3/s", "m3/s"});
+createPlot(
+	id=5,
+	position={50, 120, 600, 400},
+	y={"ashrae.V_flow"},
+	heading="Volume flow ASHRAE",
+	range={0.0, 180.0, -0.5, 6.0},
+	grid=true,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m3/s"});
diff --git a/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/VentilationFlowRateSimpleOpening.mos b/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/VentilationFlowRateSimpleOpening.mos
new file mode 100644
index 0000000000..16748a5259
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Airflow/WindowVentilation/Examples/VentilationFlowRateSimpleOpening.mos
@@ -0,0 +1,62 @@
+simulateModel("AixLib.Airflow.WindowVentilation.Examples.VentilationFlowRateSimpleOpening", startTime=0, stopTime=180, outputInterval=0.1, method="dassl", tolerance=1e-6, resultFile="VentilationFlowRateSimpleOpening");
+createPlot(
+	id=1,
+	position={10, 24, 600, 400},
+	y={"TRoomSet.y", "TAmbSet.y"},
+	heading="Boundary conditions",
+	range={0.0, 180.0, -20.0, 60.0},
+	grid=true,
+	subPlot=101,
+	colors={{28,108,200}, {238,46,47}},
+	timeUnit="s",
+	displayUnits={"degC", "degC"});
+createPlot(
+	id=1,
+	position={10, 24, 600, 400},
+	y={"winSpe10Set.y"},
+	range={0.0, 180.0, -10.0, 30.0},
+	grid=true,
+	subPlot=102,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m/s"});
+createPlot(
+	id=1,
+	position={10, 24, 600, 400},
+	y={"winDirSet.y"},
+	range={0.0, 180.0, -400.0, 400.0},
+	grid=true,
+	subPlot=103,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"deg"});
+createPlot(
+	id=2,
+	position={20, 48, 600, 400},
+	y={"warrenParkins.V_flow", "gidsPhaff.V_flow", "larsenHeiselberg.V_flow", "caciolo.V_flow", "tang.V_flow"},
+	heading="Volume flow 1",
+	range={0.0, 180.0, -0.1, 1.2},
+	grid=true,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}},
+	timeUnit="s",
+	displayUnits={"m3/s", "m3/s", "m3/s", "m3/s", "m3/s"});
+createPlot(
+	id=3,
+	position={30, 72, 600, 400},
+	y={"vdi2078_1.V_flow", "vdi2078_2.V_flow", "vdi2078_3.V_flow", "din16798_1.V_flow", "din4108_1.V_flow"},
+	heading="Volume flow 2",
+	range={0.0, 180.0, -0.1, 1.2},
+	grid=true,
+	colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}},
+	timeUnit="s",
+	displayUnits={"m3/s", "m3/s", "m3/s", "m3/s", "m3/s"});
+createPlot(
+	id=4,
+	position={40, 96, 600, 400},
+	y={"ashrae.V_flow"},
+	heading="Volume flow ASHRAE",
+	range={0.0, 180.0, -2.0, 14.0},
+	grid=true,
+	colors={{28,108,200}},
+	timeUnit="s",
+	displayUnits={"m3/s"});
diff --git a/AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/Examples/GlobalPerezTiltedSurface.mos b/AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/Examples/GlobalPerezTiltedSurface.mos
new file mode 100644
index 0000000000..fe7f5f01f0
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/BoundaryConditions/SolarIrradiation/Examples/GlobalPerezTiltedSurface.mos
@@ -0,0 +1,14 @@
+removePlots();
+simulateModel("AixLib.BoundaryConditions.SolarIrradiation.Examples.GlobalPerezTiltedSurface", startTime=1.82304e+07, tolerance=1e-6, stopTime=1.83168e+07, method="CVode", resultFile="GlobalPerezTiltedSurface");
+createPlot(id = 1,
+ position = {7, 7, 746, 517},
+ y = {"HGloRoo.H", "HGloWal.H", "HGloFlo.H"},
+ range = {0, 90000.0, 100000.0, -20000.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ filename = "GlobalPerezTiltedSurface.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACConverter.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACConverter.mos
new file mode 100644
index 0000000000..6a5da7fbe0
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACConverter.mos
@@ -0,0 +1,48 @@
+// Script generated by Dymola Mon Feb  3 17:04:42 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Conversion.Examples.ACACConverter", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACACConverter");
+createPlot(id = 1,
+ position = {0, 0, 1674, 725},
+ y = {"load.S[1]", "load.S[2]", "sou.S[1]", "sou.S[2]"},
+ range = {0.0, 1.0, -1500.0, 1500.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ACACConverter.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 237},
+ y = {"load.i[1]", "load.i[2]"},
+ range = {0.0, 1.0, -10.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 238},
+ y = {"conACAC.terminal_n.v[1]", "conACAC.terminal_n.v[2]", "conACAC.terminal_p.v[1]", "conACAC.terminal_p.v[2]"},
+ range = {0.0, 1.0, -50.0, 250.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformer.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformer.mos
new file mode 100644
index 0000000000..ee6ad034aa
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformer.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 17:57:41 2014
+// Plot commands
+removePlots();
+simulateModel("AixLib.Electrical.AC.OnePhase.Conversion.Examples.ACACTransformer", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACACTransformer");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1674, 725},
+y={"load.S[1]", "load.S[2]", "sou.S[1]", "sou.S[2]"},
+range={0.0, 1.0, -4000.0, 1000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACACTransformer.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 1674, 237},
+y={"load.i[1]", "load.i[2]"},
+range={0.0, 1.0, -60.0, 60.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+ bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformerFull.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformerFull.mos
new file mode 100644
index 0000000000..b3ecaab3e9
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACACTransformerFull.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Sun Aug 24 15:47:09 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Conversion.Examples.ACACTransformerFull", method="dassl", tolerance=1e-6, stopTime=1.0, resultFile="ACACTransformerFull");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1674, 725},
+y={"load.S[1]", "load.S[2]", "sou.S[1]", "sou.S[2]"},
+range={0.0, 1.0, -4000.0, 1000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACACTransformerFull.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 1674, 237},
+y={"load.i[1]", "load.i[2]"},
+range={0.0, 1.0, -60.0, 60.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+ bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACDCConverter.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACDCConverter.mos
new file mode 100644
index 0000000000..d8941ee8af
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Conversion/Examples/ACDCConverter.mos
@@ -0,0 +1,33 @@
+// Script generated by Dymola Mon Feb  3 18:00:58 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Conversion.Examples.ACDCConverter", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACDCConverter");
+createPlot(id = 1,
+ position = {0, 0, 1674, 725},
+ y = {"load.S[1]", "res.S[1]"},
+ range = {0.0, 1.0, -6000.0, 4000.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ACDCConverter.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 359},
+ y = {"sou.S[1]"},
+ range = {0.0, 1.0, -5000.0, 2000.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Examples/GeneratorLoadGrid.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Examples/GeneratorLoadGrid.mos
new file mode 100644
index 0000000000..a4640cb37d
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Examples/GeneratorLoadGrid.mos
@@ -0,0 +1,19 @@
+// Script generated by Dymola Fri Mar 27 11:33:03 2015
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Examples.GeneratorLoadGrid",tolerance=1e-6, stopTime=1.0, method="Radau", resultFile="AcGeneratorLoadGrid");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+Advanced.DefaultAutoErase = true;
+Advanced.Legend.Horizontal = true;
+createPlot(id=1,
+position={43, 20, 982, 708},
+y={"grid.P.real", "grid.P.apparent"},
+range={0.0, 1.0, -6000.0, 8000.0},
+grid=true,
+filename="AcGeneratorLoadGrid.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Examples/GridDCLoad.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Examples/GridDCLoad.mos
new file mode 100644
index 0000000000..761ccd4b70
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Examples/GridDCLoad.mos
@@ -0,0 +1,28 @@
+// Script generated by Dymola Fri Mar 27 11:38:36 2015
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Examples.GridDCLoad",tolerance=1e-6, stopTime=1.0, method="Radau", resultFile="AcGridDCLoad");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+Advanced.DefaultAutoErase = true;
+Advanced.Legend.Horizontal = true;
+createPlot(id=1,
+position={43, 20, 982, 708},
+y={"grid.P.real", "grid.P.apparent"},
+range={0.0, 1.0, 140.0, 180.0},
+grid=true,
+filename="AcGridDCLoad.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={43, 20, 982, 351},
+y={"resistor.S[1]", "resistor.S[2]"},
+range={0.0, 1.0, -160.0, 20.0},
+grid=true,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine.mos
new file mode 100644
index 0000000000..e1aa6db4db
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine.mos
@@ -0,0 +1,42 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Lines.Examples.ACLine", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACline");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, 0, 1674, 904},
+y={"R1.v[1]", "R1.v[2]", "R2.v[1]", "R2.v[2]", "R3.v[1]", "R3.v[2]"},
+range={0.0, 1.0, -5.0, 65.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACline.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={-6, 0, 1674, 449},
+y={"R1.i[1]", "R1.i[2]", "load_sc.i[1]", "load_sc.i[2]", "R2.i[1]", "R2.i[2]", "R3.i[1]", "R3.i[2]"},
+range={0.0, 1.0, -1.0, 13.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0},
+{0,128,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_L.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_L.mos
new file mode 100644
index 0000000000..ad67ce28f2
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_L.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb 10 12:05:07 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Lines.Examples.ACLine_L", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="ACline_L");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, 0, 1674, 904},
+y={"R1.v[1]", "R1.v[2]", "R2.v[1]", "R2.v[2]", "R3.v[1]", "R3.v[2]"},
+range={0.0, 1.0, -5.0, 65.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACline_L.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={-6, 0, 1674, 449},
+y={"R1.i[1]", "R1.i[2]", "load_sc.i[1]", "load_sc.i[2]", "R2.i[1]", "R2.i[2]", "R3.i[1]", "R3.i[2]"},
+range={0.0, 1.0, -1.0, 13.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_R.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_R.mos
new file mode 100644
index 0000000000..59dfa92802
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_R.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb 10 11:59:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Lines.Examples.ACLine_R", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACline_R");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, 0, 1674, 904},
+y={"R1.v[1]", "R1.v[2]", "R2.v[1]", "R2.v[2]", "R3.v[1]", "R3.v[2]"},
+range={0.0, 1.0, -5.0, 65.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACline_R.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={-6, 0, 1674, 449},
+y={"R1.i[1]", "R1.i[2]", "sc_load.i[1]", "sc_load.i[2]", "R2.i[1]", "R2.i[2]", "R3.i[1]", "R3.i[2]"},
+range={0.0, 1.0, -1.0, 13.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_RL.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_RL.mos
new file mode 100644
index 0000000000..10e53f116e
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACLine_RL.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Lines.Examples.ACLine_RL", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="ACline_RL");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, -484, 1674, 904},
+ y={"load_sc_1.v[1]", "load_sc_1.v[2]", "load_sc_2.v[1]", "load_sc_2.v[2]", "load_sc_3.v[1]", "load_sc_3.v[2]"},
+ range={0.0, 1.0, -1.2000000000000002, 1.4},
+ autoscale=true,
+ autoerase=true,
+ autoreplot=true,
+ description=false,
+ grid=true,
+ color=true,
+ online=false,
+ filename="ACline_RL.mat",
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+ markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+ position={-6, -484, 1674, 449},
+ y={"load_sc_1.i[1]", "load_sc_1.i[2]", "load_sc_2.i[1]", "load_sc_2.i[2]", "load_sc_3.i[1]", "load_sc_3.i[2]"},
+ range={0.0, 1.0, -7.0, 8.0},
+ autoscale=true,
+ autoerase=true,
+ autoreplot=true,
+ description=false,
+ grid=true,
+ color=true,
+ online=false,
+ subPlot=2,
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+ markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACSimpleGrid.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACSimpleGrid.mos
new file mode 100644
index 0000000000..f7f6706d94
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Lines/Examples/ACSimpleGrid.mos
@@ -0,0 +1,22 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Lines.Examples.ACSimpleGrid", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACSimpleGrid");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1016, 317},
+y={"load.v[1]", "load.v[2]", "E.terminal.v[1]", "E.terminal.v[2]"},
+range={0.0, 3.0, -20.0, 140.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACSimpleGrid.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ParallelLoads.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ParallelLoads.mos
new file mode 100644
index 0000000000..7f2b141590
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ParallelLoads.mos
@@ -0,0 +1,63 @@
+// Script generated by Dymola Mon Feb  3 11:32:00 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Loads.Examples.ParallelLoads", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ParallelLoads");
+createPlot(id = 2,
+ position = {0, 0, 1482, 904},
+ y = {"varRL.i[1]", "varRL.i[2]", "RL.i[1]", "RL.i[2]"},
+ range = {0.0, 1.0, -6.0, 6.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ParallelLoads.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 221},
+ y = {"varRC.i[1]", "varRC.i[2]", "RC.i[1]", "RC.i[2]"},
+ range = {0.0, 1.0, -1.0, 5.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 222},
+ y = {"R.i[1]", "R.i[2]"},
+ range = {0.0, 1.0, -1.0, 5.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 221},
+ y = {"RL.S[1]", "RL.S[2]", "RC.S[1]", "RC.S[2]"},
+ range = {0.0, 1.0, -1000.0, 1500.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 4,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ParallelResistors.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ParallelResistors.mos
new file mode 100644
index 0000000000..cc9c61d47e
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ParallelResistors.mos
@@ -0,0 +1,33 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Loads.Examples.ParallelResistors", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ParallelResistors");
+createPlot(id = 2,
+ position = {0, 0, 1482, 844},
+ y = {"R.i[1]", "R.i[2]", "R1.i[1]", "R1.i[2]"},
+ range = {0.0, 1.0, -5.0, 5.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ParallelResistors.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 419},
+ y = {"source.S[1]", "source.S[2]"},
+ range = {0.0, 1.0, -2200.0, 200.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/TestImpedance.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/TestImpedance.mos
new file mode 100644
index 0000000000..3d01731221
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/TestImpedance.mos
@@ -0,0 +1,78 @@
+// Script generated by Dymola Mon Feb  3 13:07:22 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Loads.Examples.TestImpedance", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="TestImpedance");
+createPlot(id = 2,
+ position = {0, 0, 1482, 844},
+ y = {"Z1.i[1]", "Z1.i[2]"},
+ range = {0.0, 1.0, -300.0, 100.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "TestImpedance.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 164},
+ y = {"Z2.i[1]", "Z2.i[2]"},
+ range = {0.0, 1.0, -100.0, 300.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 164},
+ y = {"Z3.i[1]", "Z3.i[2]"},
+ range = {0.0, 1.0, -100.0, 300.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 164},
+ y = {"Z4.i[1]", "Z4.i[2]"},
+ range = {0.0, 1.0, -200.0, 200.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 4,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 164},
+ y = {"Z5.i[1]", "Z5.i[2]"},
+ range = {0.0, 1.0, 90.0, 130.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 5,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ThreePhases.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ThreePhases.mos
new file mode 100644
index 0000000000..d9d78ce367
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/ThreePhases.mos
@@ -0,0 +1,48 @@
+// Script generated by Dymola Mon Feb  3 13:11:10 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Loads.Examples.ThreePhases", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="ThreePhases");
+createPlot(id = 2,
+ position = {0, 0, 1482, 844},
+ y = {"Za.i[1]", "Za.i[2]"},
+ range = {0.0, 1.0, -5.0, 25.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ThreePhases.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 278},
+ y = {"Zb.i[1]", "Zb.i[2]"},
+ range = {0.0, 1.0, -10.0, 25.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1482, 277},
+ y = {"Zc.i[1]", "Zc.i[2]"},
+ range = {0.0, 1.0, -18.0, -12.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/VariableImpedance.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/VariableImpedance.mos
new file mode 100644
index 0000000000..b2708bc544
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Loads/Examples/VariableImpedance.mos
@@ -0,0 +1,53 @@
+// Script generated by Dymola Mon Feb  3 13:07:22 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Loads.Examples.VariableImpedance", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="VariableImpedance");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=2,
+position={3, -39, 1482, 661},
+y={"Z_L.i[1]", "Z_L.i[2]"},
+range={0.0, 1.0, -150.0, 50.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="VariableImpedance.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=2,
+position={3, -39, 1482, 217},
+y={"Z_C.i[1]", "Z_C.i[2]"},
+range={0.0, 1.0, -50.0, 250.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=2,
+position={3, -39, 1482, 216},
+y={"Z_R.i[1]", "Z_R.i[2]"},
+range={0.0, 1.0, -50.0, 150.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sensors/Examples/GeneralizedSensor.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sensors/Examples/GeneralizedSensor.mos
new file mode 100644
index 0000000000..085c6334f4
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sensors/Examples/GeneralizedSensor.mos
@@ -0,0 +1,48 @@
+// Script generated by Dymola Mon Feb  3 18:10:17 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Sensors.Examples.GeneralizedSensor", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="GeneralizedSensorAc1ph");
+createPlot(id = 1,
+ position = {0, 0, 1674, 725},
+ y = {"sen.I"},
+ range = {0.0, 0.10200000000000001, -0.2, 1.4000000000000001},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "GeneralizedSensorAc1ph.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 237},
+ y = {"sen.V"},
+ range = {0.0, 0.10200000000000001, 119.95, 120.02},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 238},
+ y = {"loa.S[1]", "loa.S[2]"},
+ range = {0.0, 0.10200000000000001, -100.0, 150.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sensors/Examples/Probe.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sensors/Examples/Probe.mos
new file mode 100644
index 0000000000..f4fd6b6a93
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sensors/Examples/Probe.mos
@@ -0,0 +1,18 @@
+// Script generated by Dymola Mon Feb  3 18:10:17 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Sensors.Examples.Probe", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ProbeAcOnePhase");
+createPlot(id = 1,
+ position = {0, 0, 1674, 725},
+ y = {"probe_source.V", "probe_loadRC.V", "probe_loadRL.V"},
+ range = {0.0, 1.0, 0.9, 1.1},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ProbeAcOnePhase.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/FixedVoltageSource.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/FixedVoltageSource.mos
new file mode 100644
index 0000000000..a10f968caf
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/FixedVoltageSource.mos
@@ -0,0 +1,48 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Sources.Examples.FixedVoltageSource", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="FixedVoltageSource");
+createPlot(id=1,
+position={0, 0, 1535, 702},
+y={"RL.i[1]", "RL.i[2]"},
+range={0.0, 21.0, -1.0, 4.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="FixedVoltageSource.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={0, 0, 1535, 230},
+y={"sen.V"},
+range={0.0, 21.0, 0.8500000000000001, 1.1500000000000001},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
+createPlot(id=1,
+position={0, 0, 1535, 230},
+y={"sen.theta"},
+range={0.0, 21.0, 17.0, 23.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/VariablePowerSource.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/VariablePowerSource.mos
new file mode 100644
index 0000000000..5c37962d46
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/VariablePowerSource.mos
@@ -0,0 +1,63 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Sources.Examples.VariablePowerSource", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="VariablePowerSource");
+createPlot(id = 2,
+ position = {0, 0, 1603, 844},
+ y = {"RL.i[1]", "RL.i[2]"},
+ range = {0.0, 21.0, -2.0, 2.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "VariablePowerSource.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1603, 206},
+ y = {"RL.S[1]", "RL.S[2]"},
+ range = {0.0, 21.0, 0.0, 0.4},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1603, 207},
+ y = {"generator.S[1]", "generator.S[2]"},
+ range = {0.0, 21.0, -0.4, 0.1},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1603, 206},
+ y = {"grid.sou.S[1]", "grid.sou.S[2]"},
+ range = {0.0, 21.0, -0.4, 0.4},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 4,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/WindTurbine.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/WindTurbine.mos
new file mode 100644
index 0000000000..263617d2bd
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/OnePhase/Sources/Examples/WindTurbine.mos
@@ -0,0 +1,53 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.OnePhase.Sources.Examples.WindTurbine", tolerance=1e-6, stopTime = 172800, method="Radau", resultFile="WindTurbineAC");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1535, 702},
+y={"tur.P", "res.P"},
+range={0.0, 175000.0, -1000.0, 2000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="WindTurbineAC.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={0, 0, 1535, 230},
+y={"sen.V"},
+range={0.0, 175000.0, 119.8, 121.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
+createPlot(id=1,
+position={0, 0, 1535, 230},
+y={"sou.P.real", "sou.P.apparent"},
+range={0.0, 175000.0, -1500.0, 2000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACConverter.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACConverter.mos
new file mode 100644
index 0000000000..6d9aa9cbd2
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACConverter.mos
@@ -0,0 +1,48 @@
+// Script generated by Dymola Mon Feb  3 17:04:42 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples.ACACConverter", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACACConverter3ph");
+createPlot(id = 1,
+ position = {0, 0, 1674, 725},
+ y = {"load.S[1]", "load.S[2]", "sou.S[1]", "sou.S[2]"},
+ range = {0.0, 1.0, -1500.0, 1500.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ACACConverter3ph.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 237},
+ y = {"load.i[1]", "load.i[2]"},
+ range = {0.0, 1.0, -10.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 238},
+ y = {"conACAC.terminal_n.v[1]", "conACAC.terminal_n.v[2]", "conACAC.terminal_p.v[1]", "conACAC.terminal_p.v[2]"},
+ range = {0.0, 1.0, -50.0, 250.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformer.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformer.mos
new file mode 100644
index 0000000000..85209959e8
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformer.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 17:57:41 2014
+// Plot commands
+removePlots();
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples.ACACTransformer", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACACTransformer3ph");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1674, 725},
+y={"load.S[1]", "load.S[2]", "sou.S[1]", "sou.S[2]"},
+range={0.0, 1.0, -4000.0, 1000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACACTransformer3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 1674, 237},
+y={"load.i[1]", "load.i[2]"},
+range={0.0, 1.0, -60.0, 60.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+ bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformerFull.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformerFull.mos
new file mode 100644
index 0000000000..465bc1dd56
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACACTransformerFull.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Sun Aug 24 15:47:09 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples.ACACTransformerFull", method="dassl", tolerance=1e-6, stopTime=1.0, resultFile="ACACTransformerFull3ph");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1674, 725},
+y={"load.S[1]", "load.S[2]", "sou.S[1]", "sou.S[2]"},
+range={0.0, 1.0, -4000.0, 1000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACACTransformerFull3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 1674, 237},
+y={"load.i[1]", "load.i[2]"},
+range={0.0, 1.0, -60.0, 60.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+ bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACDCConverter.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACDCConverter.mos
new file mode 100644
index 0000000000..462161796d
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Conversion/Examples/ACDCConverter.mos
@@ -0,0 +1,33 @@
+// Script generated by Dymola Mon Feb  3 18:00:58 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples.ACDCConverter", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACDCConverter3ph");
+createPlot(id = 1,
+ position = {0, 0, 1674, 725},
+ y = {"load.S[1]", "res.S[1]"},
+ range = {0.0, 1.0, -6000.0, 4000.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ACDCConverter3ph.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 359},
+ y = {"sou.S[1]"},
+ range = {0.0, 1.0, -5000.0, 2000.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine.mos
new file mode 100644
index 0000000000..e39cb5335d
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine.mos
@@ -0,0 +1,42 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLine", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACline3ph");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, 0, 1674, 904},
+y={"R1.v[1]", "R1.v[2]", "R2.v[1]", "R2.v[2]", "R3.v[1]", "R3.v[2]"},
+range={0.0, 1.0, -5.0, 65.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACline3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={-6, 0, 1674, 449},
+y={"R1.i[1]", "R1.i[2]", "load_sc.i[1]", "load_sc.i[2]", "R2.i[1]", "R2.i[2]", "R3.i[1]", "R3.i[2]"},
+range={0.0, 1.0, -1.0, 13.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0},
+{0,128,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLineMedium.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLineMedium.mos
new file mode 100644
index 0000000000..cf557d878e
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLineMedium.mos
@@ -0,0 +1,42 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLineMedium", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="AClineMedium3ph");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, 0, 1674, 904},
+y={"R1.v[1]", "R1.v[2]", "R2.v[1]", "R2.v[2]", "R3.v[1]", "R3.v[2]"},
+range={0.0, 1.0, -5.0, 65.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="AClineMedium3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={-6, 0, 1674, 449},
+y={"R1.i[1]", "R1.i[2]", "load_sc.i[1]", "load_sc.i[2]", "R2.i[1]", "R2.i[2]", "R3.i[1]", "R3.i[2]"},
+range={0.0, 1.0, -1.0, 13.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0},
+{0,128,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_L.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_L.mos
new file mode 100644
index 0000000000..314eb5ec5f
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_L.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb 10 12:05:07 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLine_L", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="ACline_L3ph");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, 0, 1674, 904},
+y={"R1.v[1]", "R1.v[2]", "R2.v[1]", "R2.v[2]", "R3.v[1]", "R3.v[2]"},
+range={0.0, 1.0, -5.0, 65.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACline_L3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={-6, 0, 1674, 449},
+y={"R1.i[1]", "R1.i[2]", "load_sc.i[1]", "load_sc.i[2]", "R2.i[1]", "R2.i[2]", "R3.i[1]", "R3.i[2]"},
+range={0.0, 1.0, -1.0, 13.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_R.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_R.mos
new file mode 100644
index 0000000000..2bf55106c0
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_R.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb 10 11:59:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLine_R", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACline_R3ph");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, 0, 1674, 904},
+y={"R1.v[1]", "R1.v[2]", "R2.v[1]", "R2.v[2]", "R3.v[1]", "R3.v[2]"},
+range={0.0, 1.0, -5.0, 65.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACline_R3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={-6, 0, 1674, 449},
+y={"R1.i[1]", "R1.i[2]", "sc_load.i[1]", "sc_load.i[2]", "R2.i[1]", "R2.i[2]", "R3.i[1]", "R3.i[2]"},
+range={0.0, 1.0, -1.0, 13.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_RL.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_RL.mos
new file mode 100644
index 0000000000..13ac4cc491
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACLine_RL.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLine_RL", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACline_RL3ph");
+removePlots();
+createPlot(id=1,
+position={-6, -484, 1674, 904},
+ y={"load_sc_1.v[1]", "load_sc_1.v[2]", "load_sc_2.v[1]", "load_sc_2.v[2]", "load_sc_3.v[1]", "load_sc_3.v[2]"},
+ range={0.0, 1.0, -1.2000000000000002, 1.4},
+ autoscale=true,
+ autoerase=true,
+ autoreplot=true,
+ description=false,
+ grid=true,
+ color=true,
+ online=false,
+ filename="ACline_RL3ph.mat",
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+ markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+ position={-6, -484, 1674, 449},
+ y={"load_sc_1.i[1]", "load_sc_1.i[2]", "load_sc_2.i[1]", "load_sc_2.i[2]", "load_sc_3.i[1]", "load_sc_3.i[2]"},
+ range={0.0, 1.0, -7.0, 8.0},
+ autoscale=true,
+ autoerase=true,
+ autoreplot=true,
+ description=false,
+ grid=true,
+ color=true,
+ online=false,
+ subPlot=2,
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+ markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGrid.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGrid.mos
new file mode 100644
index 0000000000..14f557292e
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGrid.mos
@@ -0,0 +1,22 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACSimpleGrid", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACSimpleGrid3ph");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1016, 317},
+y={"load.v[1]", "load.v[2]", "E.terminal.v[1]", "E.terminal.v[2]"},
+range={0.0, 3.0, -20.0, 140.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACSimpleGrid3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGridMedium.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGridMedium.mos
new file mode 100644
index 0000000000..37def1f106
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Lines/Examples/ACSimpleGridMedium.mos
@@ -0,0 +1,22 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACSimpleGridMedium", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACSimpleGridMedium3ph");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1016, 317},
+y={"load.v[1]", "load.v[2]", "E.terminal.v[1]", "E.terminal.v[2]"},
+range={0.0, 3.0, -20.0, 140.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACSimpleGridMedium3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/Impedances.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/Impedances.mos
new file mode 100644
index 0000000000..0e584eb641
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/Impedances.mos
@@ -0,0 +1,25 @@
+// Script generated by Dymola Mon Feb  3 11:32:00 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Examples.Impedances", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="Impedances3ph");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1535, 703},
+y={"Z1.i[1]", "Z1.i[2]", "Z2.i[1]", "Z2.i[2]", "Z3.i[1]", "Z3.i[2]", "Z4.i[1]", "Z4.i[2]", "Z5.i[1]", "Z5.i[2]"},
+range={0.0, 1.0, -500.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Impedances3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross,MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ParallelLoads.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ParallelLoads.mos
new file mode 100644
index 0000000000..c09ea53836
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ParallelLoads.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 11:32:00 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Examples.ParallelLoads", method="Dassl", tolerance=1e-6, stopTime=1.0, resultFile="ParallelLoads3ph");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1535, 703},
+y={"RL_pf.S[1]", "RL_pf.S[2]", "varRL_y.S[1]", "varRL_y.S[2]", "varRC_y.S[1]", "varRC_y.S[2]", "varRL_P.S[1]", "varRL_P.S[2]"},
+range={0.0, 0.00028500000000000004, -2500.0, 2500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ParallelLoads3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={0, 0, 1535, 348},
+y={"E.S[1]", "E.S[2]"},
+range={0.0, 1.0, -7000.0, 2000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ThreePhases.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ThreePhases.mos
new file mode 100644
index 0000000000..2d7c4cf19d
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Loads/Examples/ThreePhases.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb  3 11:32:00 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Loads.Examples.ThreePhases", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ThreePhases3ph");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1535, 703},
+y={"sen_Y.S[1]", "sen_Y.S[2]", "sen_D.S[1]", "sen_D.S[2]"},
+range={0.0, 1.0, 100000.0, 400000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ThreePhases3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 1535, 348},
+y={"errorY", "errorD"},
+range={0.0, 1.0, 0.0, 1.2E-10},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/GeneralizedSensor.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/GeneralizedSensor.mos
new file mode 100644
index 0000000000..df8ebc938f
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/GeneralizedSensor.mos
@@ -0,0 +1,48 @@
+// Script generated by Dymola Mon Feb  3 18:10:17 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Sensors.Examples.GeneralizedSensor", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="GeneralizedSensorAc3ph");
+createPlot(id = 1,
+ position = {0, 0, 1674, 725},
+ y = {"sen.I"},
+ range = {0.0, 0.10200000000000001, -0.2, 1.4000000000000001},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "GeneralizedSensorAc3ph.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 237},
+ y = {"sen.V"},
+ range = {0.0, 0.10200000000000001, 119.95, 120.02},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1674, 238},
+ y = {"loa.S[1]", "loa.S[2]"},
+ range = {0.0, 0.10200000000000001, -100.0, 150.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/Probe.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/Probe.mos
new file mode 100644
index 0000000000..56127a30ec
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sensors/Examples/Probe.mos
@@ -0,0 +1,21 @@
+// Script generated by Dymola Mon Feb  3 18:10:17 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Sensors.Examples.Probe", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ProbeAcOnePhase3ph");
+createPlot(id=1,
+ position={0, 0, 1200, 781},
+ y={"probe_source.V", "probe_loadRC.V", "probe_loadRL.V"},
+ range={0.0, 1.0, 0.9950000000000001, 1.0005000000000002},
+ grid=true,
+ filename="ProbeAcOnePhase3ph.mat",
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=1,
+ position={0, 0, 1200, 387},
+ y={"probe_source.theta", "probe_loadRC.theta", "probe_loadRL.theta"},
+ range={0.0, 1.0, -0.2, 0.2},
+ grid=true,
+ subPlot=2,
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sources/Examples/FixedVoltageSource.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sources/Examples/FixedVoltageSource.mos
new file mode 100644
index 0000000000..cc72b4ca34
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sources/Examples/FixedVoltageSource.mos
@@ -0,0 +1,48 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Sources.Examples.FixedVoltageSource", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="FixedVoltageSource3ph");
+createPlot(id=1,
+position={20, 20, 600, 400},
+y={"RL.i[1]", "RL.i[2]"},
+range={0.0, 21.0, -1.0, 4.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="FixedVoltageSource3ph.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={20, 20, 600, 400},
+y={"sen.V"},
+range={0.0, 21.0, 0.8500000000000001, 1.1500000000000001},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
+createPlot(id=1,
+position={20, 20, 600, 400},
+y={"sen.theta"},
+range={0.0, 21.0, 17.0, 23.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sources/Examples/VariablePowerSource.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sources/Examples/VariablePowerSource.mos
new file mode 100644
index 0000000000..9885551e08
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesBalanced/Sources/Examples/VariablePowerSource.mos
@@ -0,0 +1,63 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesBalanced.Sources.Examples.VariablePowerSource", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="VariablePowerSource3ph");
+createPlot(id = 2,
+ position = {0, 0, 1603, 844},
+ y = {"RL.i[1]", "RL.i[2]"},
+ range = {0.0, 21.0, -2.0, 2.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "VariablePowerSource3ph.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1603, 206},
+ y = {"RL.S[1]", "RL.S[2]"},
+ range = {0.0, 21.0, 0.0, 0.4},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1603, 207},
+ y = {"generator.S[1]", "generator.S[2]"},
+ range = {0.0, 21.0, -0.4, 0.1},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 2,
+ position = {0, 0, 1603, 206},
+ y = {"grid.sou.S[1]", "grid.sou.S[2]"},
+ range = {0.0, 21.0, -0.4, 0.4},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 4,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Converter.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Converter.mos
new file mode 100644
index 0000000000..80517194f5
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Converter.mos
@@ -0,0 +1,84 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.Converter", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="Converter3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={15, 10, 853, 509},
+y={"probe_Y_1.V[1]", "probe_Y_1.V[2]", "probe_Y_1.V[3]", "probe_D_1.V[1]", "probe_D_1.V[2]", "probe_D_1.V[3]"},
+range={0.0, 1.0, 250.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 853, 251},
+y={"probe_2.V[1]", "probe_2.V[2]", "probe_2.V[3]"},
+range={0.0, 1.0, 120.0, 160.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 500},
+y={"probe_Y_1.theta[1]", "probe_Y_1.theta[2]", "probe_Y_1.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 162},
+y={"probe_D_1.theta[1]", "probe_D_1.theta[2]", "probe_D_1.theta[3]"},
+range={0.0, 1.0, -100.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 163},
+y={"probe_2.theta[1]", "probe_2.theta[2]", "probe_2.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Transformer.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Transformer.mos
new file mode 100644
index 0000000000..99e96591c5
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/Transformer.mos
@@ -0,0 +1,80 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.Transformer", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="Transformer3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1, position={15, 10, 853, 509},
+y={"probe_Y_1.V[1]", "probe_Y_1.V[2]", "probe_Y_1.V[3]", "probe_D_1.V[1]", "probe_D_1.V[2]", "probe_D_1.V[3]"},
+range={0.0, 1.0, 250.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Transformer3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 853, 251},
+y={"probe_2.V[1]", "probe_2.V[2]", "probe_2.V[3]"},
+range={0.0, 1.0, 120.0, 160.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 500},
+y={"probe_Y_1.theta[1]", "probe_Y_1.theta[2]", "probe_Y_1.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 162},
+y={"probe_D_1.theta[1]", "probe_D_1.theta[2]", "probe_D_1.theta[3]"},
+range={0.0, 1.0, -100.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 163},
+y={"probe_2.theta[1]", "probe_2.theta[2]", "probe_2.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false, subPlot=3, leftTitleType=1, bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerDD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerDD.mos
new file mode 100644
index 0000000000..66619644f7
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerDD.mos
@@ -0,0 +1,80 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.TransformerDD", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="TransformerDD3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={15, 10, 853, 509},
+y={"probe_Y_1.V[1]", "probe_Y_1.V[2]", "probe_Y_1.V[3]", "probe_D_1.V[1]", "probe_D_1.V[2]", "probe_D_1.V[3]"},
+range={0.0, 1.0, 250.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="TransformerDD3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 853, 251},
+y={"probe_2.V[1]", "probe_2.V[2]", "probe_2.V[3]"},
+range={0.0, 1.0, 120.0, 160.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true, color=true, online=false, subPlot=2,
+leftTitleType=1, bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 500},
+y={"probe_Y_1.theta[1]", "probe_Y_1.theta[2]", "probe_Y_1.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 162},
+y={"probe_D_1.theta[1]", "probe_D_1.theta[2]", "probe_D_1.theta[3]"},
+range={0.0, 1.0, -100.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 163},
+y={"probe_2.theta[1]", "probe_2.theta[2]", "probe_2.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerFull.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerFull.mos
new file mode 100644
index 0000000000..5473016599
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerFull.mos
@@ -0,0 +1,82 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.TransformerFull", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="TransformerFull3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={15, 10, 853, 509},
+y={"probe_Y_1.V[1]", "probe_Y_1.V[2]", "probe_Y_1.V[3]", "probe_D_1.V[1]", "probe_D_1.V[2]", "probe_D_1.V[3]"},
+range={0.0, 1.0, 250.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false, grid=true, color=true,
+online=false,
+filename="TransformerFull3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 853, 251},
+y={"probe_2.V[1]", "probe_2.V[2]", "probe_2.V[3]"},
+range={0.0, 1.0, 120.0, 160.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 500},
+y={"probe_Y_1.theta[1]", "probe_Y_1.theta[2]", "probe_Y_1.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 162},
+y={"probe_D_1.theta[1]", "probe_D_1.theta[2]", "probe_D_1.theta[3]"},
+range={0.0, 1.0, -100.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 163},
+y={"probe_2.theta[1]", "probe_2.theta[2]", "probe_2.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownDY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownDY.mos
new file mode 100644
index 0000000000..1b6da01f6a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownDY.mos
@@ -0,0 +1,81 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.TransformerStepDownDY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="TransformerStepDownDY3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1, position={15, 10, 853, 509},
+y={"probe_Y_1.V[1]", "probe_Y_1.V[2]", "probe_Y_1.V[3]", "probe_D_1.V[1]", "probe_D_1.V[2]", "probe_D_1.V[3]"},
+range={0.0, 1.0, 250.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false, grid=true, color=true,
+online=false,
+filename="TransformerStepDownDY3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 853, 251},
+y={"probe_2.V[1]", "probe_2.V[2]", "probe_2.V[3]"},
+range={0.0, 1.0, 120.0, 160.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 500},
+y={"probe_Y_1.theta[1]", "probe_Y_1.theta[2]", "probe_Y_1.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 162},
+y={"probe_D_1.theta[1]", "probe_D_1.theta[2]", "probe_D_1.theta[3]"},
+range={0.0, 1.0, -100.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 163},
+y={"probe_2.theta[1]", "probe_2.theta[2]", "probe_2.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownYD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownYD.mos
new file mode 100644
index 0000000000..8f92a946f7
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepDownYD.mos
@@ -0,0 +1,84 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.TransformerStepDownYD", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="TransformerStepDownYD3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={15, 10, 853, 509},
+y={"probe_Y_1.V[1]", "probe_Y_1.V[2]", "probe_Y_1.V[3]", "probe_D_1.V[1]", "probe_D_1.V[2]", "probe_D_1.V[3]"},
+range={0.0, 1.0, 250.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="TransformerStepDownYD3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 853, 251},
+y={"probe_2.V[1]", "probe_2.V[2]", "probe_2.V[3]"},
+range={0.0, 1.0, 120.0, 160.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 500},
+y={"probe_Y_1.theta[1]", "probe_Y_1.theta[2]", "probe_Y_1.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 162},
+y={"probe_D_1.theta[1]", "probe_D_1.theta[2]", "probe_D_1.theta[3]"},
+range={0.0, 1.0, -100.0, 200.0},
+autoscale=true,
+autoerase=true,
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+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 163},
+y={"probe_2.theta[1]", "probe_2.theta[2]", "probe_2.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
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+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpDY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpDY.mos
new file mode 100644
index 0000000000..486f34dcf6
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpDY.mos
@@ -0,0 +1,84 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.TransformerStepUpDY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="TransformerStepUpDY3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={15, 10, 853, 509},
+y={"probe_Y_1.V[1]", "probe_Y_1.V[2]", "probe_Y_1.V[3]", "probe_D_1.V[1]", "probe_D_1.V[2]", "probe_D_1.V[3]"},
+range={0.0, 1.0, 250.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="TransformerStepUpDY3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 853, 251},
+y={"probe_2.V[1]", "probe_2.V[2]", "probe_2.V[3]"},
+range={0.0, 1.0, 120.0, 160.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 500},
+y={"probe_Y_1.theta[1]", "probe_Y_1.theta[2]", "probe_Y_1.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 162},
+y={"probe_D_1.theta[1]", "probe_D_1.theta[2]", "probe_D_1.theta[3]"},
+range={0.0, 1.0, -100.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 163},
+y={"probe_2.theta[1]", "probe_2.theta[2]", "probe_2.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpYD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpYD.mos
new file mode 100644
index 0000000000..b8bb66c819
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Conversion/Examples/TransformerStepUpYD.mos
@@ -0,0 +1,82 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Conversion.Examples.TransformerStepUpYD", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="TransformerStepUpYD3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={15, 10, 853, 509},
+y={"probe_Y_1.V[1]", "probe_Y_1.V[2]", "probe_Y_1.V[3]", "probe_D_1.V[1]", "probe_D_1.V[2]", "probe_D_1.V[3]"},
+range={0.0, 1.0, 250.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false, grid=true, color=true,
+online=false,
+filename="TransformerStepUpYD3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 853, 251},
+y={"probe_2.V[1]", "probe_2.V[2]", "probe_2.V[3]"},
+range={0.0, 1.0, 120.0, 160.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 500},
+y={"probe_Y_1.theta[1]", "probe_Y_1.theta[2]", "probe_Y_1.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Converter.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 162},
+y={"probe_D_1.theta[1]", "probe_D_1.theta[2]", "probe_D_1.theta[3]"},
+range={0.0, 1.0, -100.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={225, 80, 863, 163},
+y={"probe_2.theta[1]", "probe_2.theta[2]", "probe_2.theta[3]"},
+range={0.0, 1.0, -200.0, 200.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/WyeToDelta.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/WyeToDelta.mos
new file mode 100644
index 0000000000..4d7cf7dfad
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Interfaces/Examples/WyeToDelta.mos
@@ -0,0 +1,25 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Interfaces.Examples.WyeToDelta", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="WyeToDelta");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, 5, 1234, 528},
+y={"probe_Y.V[1]", "probe_Y.V[2]", "probe_Y.V[3]", "probeD.V[1]", "probeD.V[2]", "probeD.V[3]"},
+range={0.0, 1.0, 260.0, 500.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="WyeToDelta.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine.mos
new file mode 100644
index 0000000000..b311177082
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine.mos
@@ -0,0 +1,25 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, -43, 920, 323},
+y={"R1.load1.i[1]", "R1.load1.i[2]", "R2.load1.i[1]", "R2.load1.i[2]", "R3.load1.i[1]", "R3.load1.i[2]"},
+range={0.0, 1.0, -5.0, 30.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLine_3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL.mos
new file mode 100644
index 0000000000..21d857116c
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLineMatrix_RL", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLineMatrix_RL3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, -43, 920, 323},
+y={"Rline_1.terminal_n.phase[1].i[1]", "Rline_1.terminal_n.phase[1].i[2]", "Rline_2a.terminal_n.phase[1].i[1]", "Rline_2a.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -10.0, 10.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLineMatrix_RL3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={11, -43, 920, 158},
+y={"Rline_3a.terminal_n.phase[1].i[1]", "Rline_3a.terminal_n.phase[1].i[2]", "Rline_3b.terminal_n.phase[1].i[1]", "Rline_3b.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -4.0, 4.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC.mos
new file mode 100644
index 0000000000..6afe6743aa
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC.mos
@@ -0,0 +1,40 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLineMatrix_RLC", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLineMatrix_RLC3phu");
+// Script generated by Dymola Wed Oct  8 15:30:37 2014
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, -43, 920, 323},
+y={"Rline_1.terminal_n.phase[1].i[1]", "Rline_1.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -10.0, 10.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLineMatrix_RLC3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={11, -43, 920, 158},
+y={"Rline_2.terminal_n.phase[1].i[1]", "Rline_2.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -5.0, 15.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC_N.mos
new file mode 100644
index 0000000000..3f53c9d525
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RLC_N.mos
@@ -0,0 +1,40 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLineMatrix_RLC_N", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLineMatrix_RLC3phu_N");
+// Script generated by Dymola Wed Oct  8 15:30:37 2014
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, -43, 920, 323},
+y={"Rline_1.terminal_n.phase[1].i[1]", "Rline_1.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -10.0, 10.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLineMatrix_RLC3phu_N.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={11, -43, 920, 158},
+y={"Rline_2.terminal_n.phase[1].i[1]", "Rline_2.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -5.0, 15.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL_N.mos
new file mode 100644
index 0000000000..a7b0a03299
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLineMatrix_RL_N.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLineMatrix_RL_N", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLineMatrix_RL3phu_N");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, -43, 920, 323},
+y={"Rline_1.terminal_n.phase[1].i[1]", "Rline_1.terminal_n.phase[1].i[2]", "Rline_2a.terminal_n.phase[1].i[1]", "Rline_2a.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -10.0, 10.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLineMatrix_RL3phu_N.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={11, -43, 920, 158},
+y={"Rline_3a.terminal_n.phase[1].i[1]", "Rline_3a.terminal_n.phase[1].i[2]", "Rline_3b.terminal_n.phase[1].i[1]", "Rline_3b.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -4.0, 4.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L.mos
new file mode 100644
index 0000000000..6438b50129
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb 10 11:59:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_L", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_L3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 920, 323},
+y={"L1.terminal.phase[1].v[1]", "L2.terminal.phase[1].v[1]", "L3.terminal.phase[1].v[1]", "E.vPhase[1].terminal.v[1]"},
+range={0.0, 1.0, 100.0, 300.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLine_L3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 920, 158},
+y={"L1.load1.i[2]", "L2.load1.i[2]", "L3.load1.i[2]", "sc_load.load1.i[2]"},
+range={0.0, 1.0, 12.0, 16.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L_N.mos
new file mode 100644
index 0000000000..e8fd73fa22
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_L_N.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb 10 11:59:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_L_N", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_L3phu_N");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 920, 323},
+y={"L1.terminal.phase[1].v[1]", "L2.terminal.phase[1].v[1]", "L3.terminal.phase[1].v[1]", "E.vPhase[1].terminal.v[1]"},
+range={0.0, 1.0, 100.0, 300.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLine_L3phu_N.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 920, 158},
+y={"L1.load1.i[2]", "L2.load1.i[2]", "L3.load1.i[2]", "sc_load.load1.i[2]"},
+range={0.0, 1.0, 12.0, 16.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_N.mos
new file mode 100644
index 0000000000..c7716b3a3a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_N.mos
@@ -0,0 +1,23 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_N", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_N_3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, -43, 920, 323},
+y={"R1.load1.i[1]", "R1.load1.i[2]", "R2.load1.i[1]", "R2.load1.i[2]", "R3.load1.i[1]", "R3.load1.i[2]"},
+range={0.0, 1.0, -5.0, 30.0}, autoscale=true, autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLine_N_3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R.mos
new file mode 100644
index 0000000000..3ddf089db1
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R.mos
@@ -0,0 +1,37 @@
+// Script generated by Dymola Mon Feb 10 11:59:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_R", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_R3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 920, 323},
+y={"R1.terminal.phase[1].v[1]", "R2.terminal.phase[1].v[1]", "R3.terminal.phase[1].v[1]", "E.vPhase[1].terminal.v[1]"},
+range={0.0, 1.0, 100.0, 300.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true, color=true,
+online=false,
+filename="ACLine_R3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 920, 158},
+y={"R1.load1.i[1]", "R2.load1.i[1]", "R3.load1.i[1]", "sc_load.load1.i[1]"},
+range={0.0, 1.0, 12.0, 16.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL.mos
new file mode 100644
index 0000000000..4682c19ae8
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_RL", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_RL3phu");
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={-6, -484, 1674, 904},
+ y={"load_sc_1.load1.v[1]", "load_sc_1.load1.v[2]", "load_sc_2.load1.v[1]", "load_sc_2.load1.v[2]", "load_sc_3.load1.v[1]", "load_sc_3.load1.v[2]"},
+ range={0.0, 1.0, -1.2000000000000002, 1.4},
+ autoscale=true,
+ autoerase=true,
+ autoreplot=true,
+ description=false,
+ grid=true,
+ color=true,
+ online=false,
+ filename="ACLine_RL3phu.mat",
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+ markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+ position={-6, -484, 1674, 449},
+ y={"load_sc_1.load1.i[1]", "load_sc_1.load1.i[2]", "load_sc_2.load1.i[1]", "load_sc_2.load1.i[2]", "load_sc_3.load1.i[1]", "load_sc_3.load1.i[2]"},
+ range={0.0, 1.0, -7.0, 8.0},
+ autoscale=true,
+ autoerase=true,
+ autoreplot=true,
+ description=false,
+ grid=true,
+ color=true,
+ online=false,
+ subPlot=2,
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+ markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC.mos
new file mode 100644
index 0000000000..db85594964
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC.mos
@@ -0,0 +1,53 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_RLC", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_RLC3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 920, 323},
+y={"RLCLine_1.terminal_n.phase[1].i[1]", "RLCLine_1.terminal_n.phase[1].i[2]", "RLCLine_sc.terminal_n.phase[1].i[1]","RLCLine_sc.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -20.0, 20.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLine_RLC3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 920, 103},
+y={"RLCLine_2a.terminal_n.phase[1].i[1]", "RLCLine_2a.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -10.0, 10.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={0, 0, 920, 104},
+y={"RLCLine_3a.terminal_n.phase[1].i[1]", "RLCLine_3a.terminal_n.phase[1].i[2]", "RLCLine_3b.terminal_n.phase[1].i[1]", "RLCLine_3b.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -5.0, 5.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC_N.mos
new file mode 100644
index 0000000000..5329ec7ec1
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RLC_N.mos
@@ -0,0 +1,53 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_RLC_N", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_RLC3phu_N");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 920, 323},
+y={"RLCLine_1.terminal_n.phase[1].i[1]", "RLCLine_1.terminal_n.phase[1].i[2]", "RLCLine_sc.terminal_n.phase[1].i[1]","RLCLine_sc.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -20.0, 20.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLine_RLC3phu_N.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 920, 103},
+y={"RLCLine_2a.terminal_n.phase[1].i[1]", "RLCLine_2a.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -10.0, 10.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={0, 0, 920, 104},
+y={"RLCLine_3a.terminal_n.phase[1].i[1]", "RLCLine_3a.terminal_n.phase[1].i[2]", "RLCLine_3b.terminal_n.phase[1].i[1]", "RLCLine_3b.terminal_n.phase[1].i[2]"},
+range={0.0, 1.0, -5.0, 5.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL_N.mos
new file mode 100644
index 0000000000..46d1485560
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_RL_N.mos
@@ -0,0 +1,9 @@
+// Script generated by Dymola Mon Feb 10 12:23:40 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_RL_N", method="Radau", stopTime=1.0, tolerance=1e-06, resultFile="ACLine_RL3phu_N");
+createPlot(id=1, position={15, 10, 799, 555},
+y={"load_sc_1.load1.v[1]", "load_sc_1.load1.v[2]", "load_sc_2.load1.v[1]", "load_sc_2.load1.v[2]"},
+range={0.0, 1.0, -1.5, 1.5}, grid=true, filename="ACLine_RL3phu_N.mat", leftTitleType=1, bottomTitleType=1, colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1, position={15, 10, 799, 274},
+y={"load_sc_1.load1.i[1]", "load_sc_1.load1.i[2]", "load_sc_2.load1.i[1]", "load_sc_2.load1.i[2]"},
+range={0.0, 1.0, -6.0, 6.0}, grid=true, subPlot=2, leftTitleType=1, bottomTitleType=1, colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R_N.mos
new file mode 100644
index 0000000000..5c06c12452
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACLine_R_N.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb 10 11:59:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACLine_R_N", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACLine_R3phu_N");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 920, 323},
+y={"R1.terminal.phase[1].v[1]", "R2.terminal.phase[1].v[1]", "R3.terminal.phase[1].v[1]", "E.vPhase[1].terminal.v[1]"},
+range={0.0, 1.0, 100.0, 300.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACLine_R3phu_N.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={0, 0, 920, 158},
+y={"R1.load1.i[1]", "R2.load1.i[1]", "R3.load1.i[1]", "sc_load.load1.i[1]"},
+range={0.0, 1.0, 12.0, 16.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid.mos
new file mode 100644
index 0000000000..411568bd01
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid.mos
@@ -0,0 +1,53 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACSimpleGrid", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACSimpleGrid_3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, -43, 920, 509},
+y={"E.vPhase[1].S[1]", "E.vPhase[1].S[2]"},
+range={0.0, 1.0, -4000.0, 4000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACSimpleGrid_3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={11, -43, 920, 165},
+y={"E.vPhase[2].S[1]", "E.vPhase[2].S[2]"},
+range={0.0, 1.0, -4000.0, 4000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={11, -43, 920, 166},
+y={"E.vPhase[3].S[1]", "E.vPhase[3].S[2]"},
+range={0.0, 1.0, -2.0, 2.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid_N.mos
new file mode 100644
index 0000000000..39494aa554
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Lines/Examples/ACSimpleGrid_N.mos
@@ -0,0 +1,82 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Lines.Examples.ACSimpleGrid_N", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="ACSimpleGrid_N_3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={11, -236, 920, 509},
+y={"E.vPhase[1].S[1]", "E.vPhase[1].S[2]"}, range={0.0, 1.0, -4000.0, 4000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACSimpleGrid_N_3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={11, -236, 920, 165},
+y={"E.vPhase[2].S[1]", "E.vPhase[2].S[2]"},
+range={0.0, 1.0, -4000.0, 4000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+position={11, -236, 920, 166},
+y={"E.vPhase[3].S[1]", "E.vPhase[3].S[2]"},
+range={0.0, 1.0, -1.5, 1.5},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=2,
+position={80, 7, 407, 281},
+y={"load.terminal.phase[4].v[1]", "load.terminal.phase[4].v[2]"},
+range={0.0, 1.0, -0.5, 0.5},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="ACSimpleGrid_N_3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
+createPlot(id=2,
+position={80, 7, 407, 137},
+y={"load.terminal.phase[4].i[1]", "load.terminal.phase[4].i[2]"},
+range={0.0, 1.0, -10.0, 20.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Impedances.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Impedances.mos
new file mode 100644
index 0000000000..87bb1e44e9
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Impedances.mos
@@ -0,0 +1,37 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Examples.Impedances", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="Impedances3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={68, 4, 1044, 646},
+y={"sen_N.I[1]", "sen_N.I[2]", "sen_N.I[3]", "sen_N.I[4]"}, range={0.0, 1.0, -1.0, 8.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Impedances.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=1,
+position={68, 4, 1044, 320},
+y={"sen.I[1]", "sen.I[2]", "sen.I[3]"},
+range={0.0, 1.0, -1.0, 8.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/LoadCtrl.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/LoadCtrl.mos
new file mode 100644
index 0000000000..4ab08c8e04
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/LoadCtrl.mos
@@ -0,0 +1,32 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Examples.LoadCtrl", tolerance=1e-6, stopTime=10.0, method="dassl", resultFile="LoadCtrl3phu");
+createPlot(id=1,
+position={15, 9, 923, 622},
+y={"load.load1.S[1]", "load.load1.S[2]", "load_ctrl.load1.S[1]"}, range={0.0, 10.0, -2000.0, 12000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="LoadCtrl3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=1,
+position={15, 9, 923, 308},
+y={"load_ctrl.vCTRL_1.V_nominal", "load_ctrl.vCTRL_1.Vmin", "load_ctrl.vCTRL_1.Vmax", "load.load1.v[1]","load_ctrl.vCTRL_1.terminal.v[1]"},
+range={0.0, 10.0, 260.0, 295.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {0,0,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads.mos
new file mode 100644
index 0000000000..df0c0d869c
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Examples.Loads", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="Loads3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={15, 10, 1073, 624},
+y={"sen.S[1, 1]", "sen.S[1, 2]", "sen.S[2, 1]", "sen.S[2, 2]", "sen.S[3, 1]", "sen.S[3, 2]"},
+range={0.0, 1.0, -2000.0, 14000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Loads3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 1073, 309},
+y={"senSingleConn.S[1, 1]", "senSingleConn.S[1, 2]", "senSingleConn.S[2, 1]", "senSingleConn.S[2, 2]", "senSingleConn.S[3, 1]", "senSingleConn.S[3, 2]"},
+range={0.0, 1.0, -2000.0, 14000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads_N.mos
new file mode 100644
index 0000000000..cbc2a2f8a6
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Loads/Examples/Loads_N.mos
@@ -0,0 +1,23 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Loads.Examples.Loads_N", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="Loads_N3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={9, 24, 810, 474},
+y={"sen.I[1]", "sen.I[2]", "sen.I[3]", "sen.I[4]"},
+range={0.0, 1.0, -2.0, 18.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Loads_N3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/Sensors.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/Sensors.mos
new file mode 100644
index 0000000000..926251ad42
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sensors/Examples/Sensors.mos
@@ -0,0 +1,129 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Sensors.Examples.Sensors", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="Sensors3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={14, 19, 874, 577},
+y={"probeWye.V[1]", "probeWye.V[2]", "probeWye.V[3]"},
+range={0.0, 1.0, 0.8, 1.2000000000000002},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Sensors3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=1,
+position={14, 19, 874, 189},
+y={"probeDelta.V[1]", "probeDelta.V[2]", "probeDelta.V[3]"},
+range={0.0, 1.0, 0.8, 1.2000000000000002},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=1,
+position={14, 19, 874, 188},
+y={"probeWye_N.V[1]", "probeWye_N.V[2]", "probeWye_N.V[3]"},
+range={0.0, 1.0, 0.8, 1.2000000000000002},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={185, 7, 979, 631},
+y={"sen.I[1]", "sen.I[2]", "sen.I[3]"},
+range={0.0, 1.0, -10.0, 40.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Sensors3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=2,
+position={185, 7, 979, 207},
+y={"sen_N.I[1]", "sen_N.I[2]", "sen_N.I[3]", "sen_N.I[4]"},
+range={0.0, 1.0, -10.0, 40.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
+createPlot(id=2,
+position={185, 7, 979, 206},
+y={"sen.S[1, 1]", "sen.S[2, 1]", "sen.S[3, 1]", "sen_N.S[1, 1]", "sen_N.S[2, 1]", "sen_N.S[3, 1]", "sen_N.S[4, 1]"},
+range={0.0, 1.0, -15000.0, 15000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=3,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=3,
+position={394, 51, 845, 518},
+y={"source.vPhase[1].S[1]", "source.vPhase[2].S[1]", "source.vPhase[3].S[1]"},
+range={0.0, 1.0, -15000.0, 15000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Sensors3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=3,
+position={394, 51, 845, 256},
+y={"source_N.vPhase[1].S[1]", "source_N.vPhase[2].S[1]", "source_N.vPhase[3].S[1]"},
+range={0.0, 1.0, -15000.0, 15000.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/FixedVoltageSource.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/FixedVoltageSource.mos
new file mode 100644
index 0000000000..50fb606e59
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/FixedVoltageSource.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.Examples.FixedVoltageSource", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="FixedVoltageSource3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={15, 10, 948, 614},
+y={"sen.V[1]", "sen.V[2]", "sen.V[3]", "sen_N.V[1]", "sen_N.V[2]", "sen_N.V[3]"},
+range={0.0, 1.0, 0.8500000000000001, 1.1500000000000001}, autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="FixedVoltageSource3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id=1,
+position={15, 10, 948, 304},
+y={"sen.theta[1]", "sen.theta[2]", "sen.theta[3]", "sen_N.theta[1]", "sen_N.theta[2]", "sen_N.theta[3]"},
+range={0.0, 1.0, -150.0, 150.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine.mos
new file mode 100644
index 0000000000..155059450b
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb  3 15:31:44 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.Examples.WindTurbine", tolerance=1e-6, stopTime = 172800, method="Radau", resultFile="WindTurbineAC3phu");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={17, 15, 914, 619},
+y={"sen.V[1]", "sen.V[2]", "sen.V[3]"}, range={0.0, 180000.0, 277.1, 277.55},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="WindTurbineAC3phu.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=1,
+position={17, 15, 914, 306},
+y={"sen.S[1, 1]", "sen.S[1, 2]", "sen.S[2, 1]", "sen.S[2, 2]", "sen.S[3, 1]", "sen.S[3, 2]"},
+range={0.0, 180000.0, -1000.0, 600.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine_N.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine_N.mos
new file mode 100644
index 0000000000..eb0eb3dc7c
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Sources/Examples/WindTurbine_N.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Tue Jan 13 11:25:50 2015
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Sources.Examples.WindTurbine_N", tolerance=1e-6, stopTime = 172800, method="Radau", resultFile="WindTurbineAC3phu_N");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={4, 3, 914, 619},
+y={"sen.V[1]", "sen.V[2]", "sen.V[3]"},
+range={0.0, 180000.0, 277.1, 277.6},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="WindTurbineAC3phu_N.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=1,
+position={4, 3, 914, 306},
+y={"sen.S[1, 1]", "sen.S[1, 2]", "sen.S[2, 1]", "sen.S[2, 2]", "sen.S[3, 1]", "sen.S[3, 2]"},
+range={0.0, 180000.0, -1200.0, 600.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DD.mos
new file mode 100644
index 0000000000..aafb4fa325
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DD.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.DD", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="BalancedStepDown_DD");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1, position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true, color=true,
+online=false,
+filename="BalancedStepDown_DD.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DY.mos
new file mode 100644
index 0000000000..acc5caca92
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/DY.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.DY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="BalancedStepDown_DY");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="BalancedStepDown_DY.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YD.mos
new file mode 100644
index 0000000000..6373aec329
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YD.mos
@@ -0,0 +1,40 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.YD", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="BalancedStepDown_YD");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1, position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="BalancedStepDown_YD.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YY.mos
new file mode 100644
index 0000000000..7d9eb3e39b
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepDown/YY.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepDown.YY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="BalancedStepDown_YY");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="BalancedStepDown_YY.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DD.mos
new file mode 100644
index 0000000000..7e81a9c33f
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DD.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepUp.DD", method="Dassl", tolerance=1e-6, stopTime=1.0, resultFile="BalancedStepUp_DD");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false, grid=true, color=true,
+online=false,
+filename="BalancedStepUp_DD.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DY.mos
new file mode 100644
index 0000000000..73ecc87e93
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/DY.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepUp.DY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="BalancedStepUp_DY");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="BalancedStepUp_DY.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2, leftTitleType=1, bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YD.mos
new file mode 100644
index 0000000000..1e2b46858f
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YD.mos
@@ -0,0 +1,40 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepUp.YD", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="BalancedStepUp_YD");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1, position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="BalancedStepUp_YD.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YY.mos
new file mode 100644
index 0000000000..e1c4e968ea
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/BalancedStepUp/YY.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.BalancedStepUp.YY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="BalancedStepUp_YY");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="BalancedStepUp_YY.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DD.mos
new file mode 100644
index 0000000000..6d193dd664
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DD.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepDown.DD", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="UnbalancedStepDown_DD");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false, grid=true, color=true,
+online=false,
+filename="UnbalancedStepDown_DD.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DY.mos
new file mode 100644
index 0000000000..9e6617f558
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/DY.mos
@@ -0,0 +1,40 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepDown.DY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="UnbalancedStepDown_DY");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1, position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="UnbalancedStepDown_DY.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YD.mos
new file mode 100644
index 0000000000..55c4fb21d1
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YD.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepDown.YD", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="UnbalancedStepDown_YD");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false, grid=true, color=true,
+online=false,
+filename="UnbalancedStepDown_YD.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YY.mos
new file mode 100644
index 0000000000..73535cbb84
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepDown/YY.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepDown.YY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="UnbalancedStepDown_YY");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="UnbalancedStepDown_YY.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DD.mos
new file mode 100644
index 0000000000..4c629cf7de
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DD.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.DD", method="Dassl", tolerance=1e-6, stopTime=1.0, resultFile="UnbalancedStepUp_DD");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="UnbalancedStepUp_DD.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DY.mos
new file mode 100644
index 0000000000..a3c3ac249a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/DY.mos
@@ -0,0 +1,41 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.DY", method="Dassl", tolerance=1e-6, stopTime=1.0, resultFile="UnbalancedStepUp_DY");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="UnbalancedStepUp_DY.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YD.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YD.mos
new file mode 100644
index 0000000000..19a0b3f43a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YD.mos
@@ -0,0 +1,34 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.YD", method="Dassl", tolerance=1e-6, stopTime=1.0, resultFile="UnbalancedStepUp_YD");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true, color=true,
+online=false,
+filename="UnbalancedStepUp_YD.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true, description=false, grid=true, color=true, online=false,
+subPlot=2, leftTitleType=1, bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YY.mos b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YY.mos
new file mode 100644
index 0000000000..fe0da0e88f
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/AC/ThreePhasesUnbalanced/Validation/IEEETests/Test4NodesFeeder/UnbalancedStepUp/YY.mos
@@ -0,0 +1,39 @@
+// Script generated by Dymola Mon Feb  3 11:58:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.AC.ThreePhasesUnbalanced.Validation.IEEETests.Test4NodesFeeder.UnbalancedStepUp.YY", method="Radau", tolerance=1e-6, stopTime=1.0, resultFile="UnbalancedStepUp_YY");
+// Plot commands
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={13, 7, 1366, 618},
+y={"err_V2[1]", "err_V2[2]", "err_V2[3]", "err_V3[1]", "err_V3[2]", "err_V3[3]", "err_V4[1]", "err_V4[2]", "err_V4[3]"},
+range={0.0, 1.0, -0.5, 0.4},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false, grid=true, color=true,
+online=false,
+filename="UnbalancedStepUp_YY.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
+createPlot(id=1,
+position={13, 7, 1366, 306},
+y={"err_Theta2[1]", "err_Theta2[2]", "err_Theta2[3]", "err_Theta3[1]", "err_Theta3[2]", "err_Theta3[3]", "err_Theta4[1]", "err_Theta4[2]", "err_Theta4[3]"},
+range={0.0, 1.0, -0.06, 0.060000000000000005},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}},
+markers={MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross, MarkerStyle.Cross});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Conversion/Examples/DCDCConverter.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Conversion/Examples/DCDCConverter.mos
new file mode 100644
index 0000000000..7f43088ae1
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Conversion/Examples/DCDCConverter.mos
@@ -0,0 +1,33 @@
+// Script generated by Dymola Mon Feb  3 08:48:49 2014
+// Plot commands
+simulateModel("AixLib.Electrical.DC.Conversion.Examples.DCDCConverter", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="DCDCConverter");
+createPlot(id = 1,
+ position = {0, 0, 1603, 904},
+ y = {"sen.I"},
+ range = {0.0, 1.0, -60.0, 30.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "DCDCConverter.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 449},
+ y = {"sen.P"},
+ range = {0.0, 1.0, -7000.0, 4000.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLine.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLine.mos
new file mode 100644
index 0000000000..0603797bdc
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLine.mos
@@ -0,0 +1,48 @@
+// Script generated by Dymola Mon Feb  3 09:22:32 2014
+// Plot commands
+simulateModel("AixLib.Electrical.DC.Lines.Examples.DCLine", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="DCLine");
+createPlot(id = 1,
+ position = {0, 0, 1603, 904},
+ y = {"line1.R", "line.R", "line2.R"},
+ range = {0.0, 1.0, 0.18, 0.24},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "DCLine.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 298},
+ y = {"load1.i[1]", "load2.i[1]", "load3.i[1]"},
+ range = {0.0, 1.0, 0.0, 4.5},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 297},
+ y = {"E.S[1]"},
+ range = {0.0, 1.0, -410.0, -360.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLines.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLines.mos
new file mode 100644
index 0000000000..86695276f7
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLines.mos
@@ -0,0 +1,33 @@
+// Script generated by Dymola Mon Feb  3 09:41:06 2014
+// Plot commands
+simulateModel("AixLib.Electrical.DC.Lines.Examples.DCLines", stopTime=4000, method="Radau", tolerance=1e-06, resultFile="DCLines");
+createPlot(id = 1,
+ position = {0, 0, 1603, 904},
+ y = {"Sloads"},
+ range = {0.0, 4000.0, 650.0, 1200.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "DCLines.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 449},
+ y = {"E.S[1]"},
+ range = {0.0, 4000.0, -1250.0, -650.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLinesLinearized.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLinesLinearized.mos
new file mode 100644
index 0000000000..82e67702e5
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/DCLinesLinearized.mos
@@ -0,0 +1,33 @@
+// Script generated by Dymola Mon Feb  3 09:41:06 2014
+// Plot commands
+simulateModel("AixLib.Electrical.DC.Lines.Examples.DCLinesLinearized", stopTime=4000, method="Radau", tolerance=1e-06, resultFile="DCLinesLinearized");
+createPlot(id = 1,
+ position = {0, 0, 1603, 904},
+ y = {"Sloads"},
+ range = {0.0, 4000.0, 650.0, 1200.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "DCLinesLinearized.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 449},
+ y = {"E.S[1]"},
+ range = {0.0, 4000.0, -1250.0, -650.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/RCModel.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/RCModel.mos
new file mode 100644
index 0000000000..5703c3aef0
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/RCModel.mos
@@ -0,0 +1,31 @@
+// Script generated by Dymola Wed Jun  4 12:25:18 2014
+simulateModel("AixLib.Electrical.DC.Lines.Examples.RCModel", stopTime=15.0, tolerance=1e-06, method="Radau", resultFile="RCModel");
+createPlot(id=1,
+ y={"sen_ss.I", "sen_dyn.I"},
+ range={0.0, 15.5, 6.0, 13.0},
+ autoscale=true,
+ autoerase=true,
+ autoreplot=true,
+ description=false,
+ grid=true,
+ color=true,
+ online=false,
+ filename="RCModel.mat",
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255}, {255,0,0}});
+createPlot(id=1,
+ y={"RC_ss.Vc", "RC_dyn.Vc"},
+ range={0.0, 15.5, 24.0, 52.0},
+ autoscale=true,
+ autoerase=true,
+ autoreplot=true,
+ description=false,
+ grid=true,
+ color=true,
+ online=false,
+ subPlot=2,
+ leftTitleType=1,
+ bottomTitleType=1,
+ colors={{0,0,255},
+  {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/Resistance.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/Resistance.mos
new file mode 100644
index 0000000000..bf5734e6e7
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Lines/Examples/Resistance.mos
@@ -0,0 +1,17 @@
+// Script generated by Dymola Wed Jun  4 12:25:18 2014
+simulateModel("AixLib.Electrical.DC.Lines.Examples.Resistance", stopTime=1.0, tolerance=1e-06, method="Radau", resultFile="Resistance");
+createPlot(id=1,
+position={15, 10, 876, 544},
+y={"sen.I"},
+range={0.0, 1.0, 4.0, 6.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="Resistance.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/LinearizedLoad.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/LinearizedLoad.mos
new file mode 100644
index 0000000000..058e44f0e2
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/LinearizedLoad.mos
@@ -0,0 +1,63 @@
+// Script generated by Dymola Mon Feb 10 13:39:25 2014
+// Plot commands
+simulateModel("AixLib.Electrical.DC.Loads.Examples.LinearizedLoad", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="LinearizedLoad");
+createPlot(id = 1,
+ position = {0, 0, 1603, 904},
+ y = {"error"},
+ range = {0.0, 1.0, -0.5, 1.5},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "LinearizedLoad.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 221},
+ y = {"sen_nlin.I", "sen_lin.I"},
+ range = {0.0, 1.0, 0.0, 15.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 222},
+ y = {"sen_nlin.V", "sen_lin.V"},
+ range = {0.0, 1.0, 70.0, 100.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 221},
+ y = {"sen_nlin.P", "sen_lin.P"},
+ range = {0.0, 1.0, 0.0, 1200.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 4,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/Resistor.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/Resistor.mos
new file mode 100644
index 0000000000..25efa55aec
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/Resistor.mos
@@ -0,0 +1,18 @@
+// Script generated by Dymola Fri Jan 31 18:12:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.DC.Loads.Examples.Resistor", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="Resistor");
+createPlot(id = 1,
+ position = {0, 0, 1603, 904},
+ y = {"sen.I", "sen1.I"},
+ range = {0.0, 1.0, 2.9000000000000004, 6.1000000000000005},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "Resistor.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/VariableLoad.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/VariableLoad.mos
new file mode 100644
index 0000000000..ef3fb8e40e
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Loads/Examples/VariableLoad.mos
@@ -0,0 +1,17 @@
+// Script generated by Dymola Fri Jan 31 17:04:12 2014
+simulateModel("AixLib.Electrical.DC.Loads.Examples.VariableLoad", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="VariableLoad");
+createPlot(id = 1,
+ position = {0, 0, 1603, 904},
+ y = {"loa1.i[1]", "loa2.i[1]", "loa3.i[1]"},
+ range = {0.0, 1.0, -2.0, 9.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "VariableLoad.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Sensors/Examples/GeneralizedSensor.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Sensors/Examples/GeneralizedSensor.mos
new file mode 100644
index 0000000000..3bc9f65f13
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Sensors/Examples/GeneralizedSensor.mos
@@ -0,0 +1,33 @@
+// Script generated by Dymola Mon Feb  3 09:01:29 2014
+// Plot commands
+simulateModel("AixLib.Electrical.DC.Sensors.Examples.GeneralizedSensor", method="Radau", tolerance=1e-06, stopTime=1.0, resultFile="GeneralizedSensor");
+createPlot(id = 1,
+ position = {0, 0, 1603, 904},
+ y = {"sen.I"},
+ range = {0.0, 1.0, -1.12, -0.8800000000000001},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "GeneralizedSensor.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1603, 449},
+ y = {"sen.V"},
+ range = {0.0, 1.0, 106.0, 134.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/DC/Sources/Examples/VoltageSource.mos b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Sources/Examples/VoltageSource.mos
new file mode 100644
index 0000000000..3cc2079d19
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/DC/Sources/Examples/VoltageSource.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Fri Jan 31 18:53:29 2014
+// Plot commands
+simulateModel("AixLib.Electrical.DC.Sources.Examples.VoltageSource", stopTime=1, method="dassl", tolerance=1e-6, resultFile="VoltageSourceDC");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1340, 565},
+y={"sen.V"},
+range={0.0, 1.0, 4.0, 8.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="VoltageSourceDC.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
+createPlot(id=1,
+position={0, 0, 1340, 279},
+y={"sen.I"},
+range={0.0, 1.0, 8.0, 16.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/Transmission/Functions/Validation/SelectCable_low.mos b/AixLib/Resources/Scripts/Dymola/Electrical/Transmission/Functions/Validation/SelectCable_low.mos
new file mode 100644
index 0000000000..b83b437c18
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/Transmission/Functions/Validation/SelectCable_low.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Electrical.Transmission.Functions.Validation.SelectCable_low", stopTime=1, method="Cvode", tolerance=1e-6, resultFile="SelectCable_low");
+createPlot(id=2, position={55, 55, 1034, 602}, y={"cab[1].Amp", "cab[2].Amp", "cab[3].Amp", "cab[4].Amp", "cab[5].Amp", "cab[6].Amp", "cab[7].Amp"}, range={0.0, 1.0, 40.0, 260.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}, {162,29,33}, {244,125,35}}, displayUnits={"A", "A", "A", "A", "A", "A", "A"});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/Transmission/Functions/Validation/SelectCable_med.mos b/AixLib/Resources/Scripts/Dymola/Electrical/Transmission/Functions/Validation/SelectCable_med.mos
new file mode 100644
index 0000000000..7f3d8293e3
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/Transmission/Functions/Validation/SelectCable_med.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Electrical.Transmission.Functions.Validation.SelectCable_med", stopTime=1, method="Cvode", tolerance=1e-6, resultFile="SelectCable_med");
+createPlot(id=2, position={55, 55, 1034, 602}, y={"cab[1].Amp", "cab[2].Amp", "cab[3].Amp", "cab[4].Amp", "cab[5].Amp", "cab[6].Amp", "cab[7].Amp"}, range={0.0, 1.0, 40.0, 260.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}, {162,29,33}, {244,125,35}}, displayUnits={"A", "A", "A", "A", "A", "A", "A"});
diff --git a/AixLib/Resources/Scripts/Dymola/Electrical/Utilities/Examples/TestVoltageCTRL.mos b/AixLib/Resources/Scripts/Dymola/Electrical/Utilities/Examples/TestVoltageCTRL.mos
new file mode 100644
index 0000000000..3321fc3cdf
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Electrical/Utilities/Examples/TestVoltageCTRL.mos
@@ -0,0 +1,38 @@
+// Script generated by Dymola Mon Feb 10 11:19:50 2014
+// Plot commands
+simulateModel("AixLib.Electrical.Utilities.Examples.TestVoltageCTRL", stopTime=10, method="Radau", tolerance=1e-6, resultFile="TestVoltageCTRL");
+removePlots();
+Advanced.FilenameInLegend = false;
+Advanced.SequenceInLegend = true;
+Advanced.PlotLegendTooltip = true;
+Advanced.FullPlotTooltip = true;
+createPlot(id=1,
+position={0, 0, 1340, 565},
+y={"voltageControl.V_nominal", "sou.V_in", "Vtr_high.y"},
+range={0.0, 10.0, 90.0, 150.0},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+filename="TestVoltageCTRL.mat",
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id=1,
+position={0, 0, 1340, 279},
+y={"voltageControl.y"},
+range={0.0, 10.0, -0.5, 1.5},
+autoscale=true,
+autoerase=true,
+autoreplot=true,
+description=false,
+grid=true,
+color=true,
+online=false,
+subPlot=2,
+leftTitleType=1,
+bottomTitleType=1,
+colors={{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Examples/SimpleHouse.mos b/AixLib/Resources/Scripts/Dymola/Examples/SimpleHouse.mos
similarity index 62%
rename from AixLib/Resources/Scripts/Dymola/Fluid/Examples/SimpleHouse.mos
rename to AixLib/Resources/Scripts/Dymola/Examples/SimpleHouse.mos
index 2972e08e47..1b3d4876a0 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Examples/SimpleHouse.mos
+++ b/AixLib/Resources/Scripts/Dymola/Examples/SimpleHouse.mos
@@ -1,5 +1,5 @@
-simulateModel("AixLib.Fluid.Examples.SimpleHouse", stopTime=3.1536e+07, method="Lsodar", tolerance=1e-06, resultFile="SimpleHouse");
-createPlot(id=1, position={0, 0, 792, 1247}, y={"zone.T"}, range={0.0, 32000000.0, 19.5, 24.5}, grid=true, colors={{28,108,200}});
+simulateModel("AixLib.Examples.SimpleHouse", stopTime=3.1536e+07, method="Lsodar", tolerance=1e-06, resultFile="SimpleHouse");
+createPlot(id=1, position={0, 0, 792, 1247}, y={"zon.T"}, range={0.0, 32000000.0, 19.5, 24.5}, grid=true, colors={{28,108,200}});
 createPlot(id=1, position={0, 0, 792, 413}, y={"heaWat.u"}, range={0.0, 32000000.0, -0.1, 1.1}, grid=true, subPlot=2, colors={{28,108,200}});
 createPlot(id=1, position={0, 0, 792, 413}, y={"vavDam.y"}, range={0.0, 380.0, 0.098, 0.124}, grid=true, subPlot=3, colors={{28,108,200}});
 createPlot(id=2, position={818, 10, 662, 377}, y={"fan.sta_a.T", "fan.sta_b.T"}, range={0.0, 380.0, 18.0, 22.5}, grid=true, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse0.mos b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse0.mos
new file mode 100644
index 0000000000..62fc94cc74
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse0.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse0", stopTime=1e+06, method="CVode", tolerance=1e-06, resultFile="SimpleHouse0");
+createPlot(id=1,position={0, 0, 792, 1247}, y={"TOut.T"}, range={0.0, 1e+06, 12.5, 20.5}, grid=true, colors={{28,108,200}});
\ No newline at end of file
diff --git a/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse1.mos b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse1.mos
new file mode 100644
index 0000000000..407ee3c4e0
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse1.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse1", stopTime=1e+06, method="CVode", tolerance=1e-06, resultFile="SimpleHouse1");
+createPlot(id=1,position={0, 0, 792, 1247}, y={"walCap.T"}, range={0.0, 1e+06, 12.5, 20.5}, grid=true, colors={{28,108,200}});
\ No newline at end of file
diff --git a/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse2.mos b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse2.mos
new file mode 100644
index 0000000000..cfea483dea
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse2.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse2", stopTime=1e+06, method="CVode", tolerance=1e-06, resultFile="SimpleHouse2");
+createPlot(id=1,position={0, 0, 792, 1247}, y={"walCap.T"}, range={0.0, 1e+06, 16.5, 20.5}, grid=true, colors={{28,108,200}});
\ No newline at end of file
diff --git a/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse3.mos b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse3.mos
new file mode 100644
index 0000000000..f41b87b0df
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse3.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse3", stopTime=1e+06, method="CVode", tolerance=1e-06, resultFile="SimpleHouse3");
+createPlot(id=1,position={0, 0, 792, 1247}, y={"zon.T"}, range={0.0, 1e+06, 16.5, 20.5}, grid=true, colors={{28,108,200}});
\ No newline at end of file
diff --git a/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse4.mos b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse4.mos
new file mode 100644
index 0000000000..df312ffec5
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse4.mos
@@ -0,0 +1,3 @@
+simulateModel("AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse4", stopTime=1e+06, method="CVode", tolerance=1e-06, resultFile="SimpleHouse4");
+createPlot(id=1,position={0, 0, 792, 1247}, y={"zon.T"}, range={0.0, 1e+06, 20, 80}, grid=true, colors={{28,108,200}});
+createPlot(id=1, position={0, 0, 792, 413}, y={"heaWat.u"}, range={0.0, 1e+06, -0.1, 1.1}, grid=true, subPlot=2, colors={{28,108,200}});
\ No newline at end of file
diff --git a/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse5.mos b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse5.mos
new file mode 100644
index 0000000000..fab0b7b4b3
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse5.mos
@@ -0,0 +1,3 @@
+simulateModel("AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse5", stopTime=1e+06, method="CVode", tolerance=1e-06, resultFile="SimpleHouse5");
+createPlot(id=1,position={0, 0, 792, 1247}, y={"zon.T"}, range={0.0, 1e+06, 20, 24}, grid=true, colors={{28,108,200}});
+createPlot(id=1, position={0, 0, 792, 413}, y={"heaWat.u"}, range={0.0, 1e+06, -0.1, 1.1}, grid=true, subPlot=2, colors={{28,108,200}});
\ No newline at end of file
diff --git a/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse6.mos b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse6.mos
new file mode 100644
index 0000000000..b8c9e992b9
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Examples/Tutorial/SimpleHouse/SimpleHouse6.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Examples.Tutorial.SimpleHouse.SimpleHouse6", stopTime=1e+06, method="CVode", tolerance=1e-06, resultFile="SimpleHouse6");
+createPlot(id=1,position={0, 0, 792, 1247}, y={"zon.T"}, range={0.0, 1e+06, 20, 26}, grid=true, colors={{28,108,200}});
+createPlot(id=1, position={0, 0, 792, 413}, y={"heaWat.u"}, range={0.0, 1e+06, -0.1, 1.1}, grid=true, subPlot=2, colors={{28,108,200}});
+createPlot(id=1, position={0, 0, 792, 413}, y={"vavDam.y"}, range={0.0, 1e+06, -0.1, 1.1}, grid=true, subPlot=3, colors={{28,108,200}});
+createPlot(id=2, position={818, 10, 662, 377}, y={"fan.sta_a.T", "fan.sta_b.T"}, range={0.0, 380.0, 18.0, 22.5}, grid=true, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mos b/AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mos
index 906effbc5f..8aa40c8086 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/BaseClasses/Validation/MassFlowRateMultiplier.mos
@@ -4,7 +4,7 @@ createPlot(
   id   = 1,
   position = {35, 30, 631, 456},
   x    = "time",
-  y    = {"ram_m_flow.y", "massFlowRateMultiplier.port_a.m_flow", "massFlowRateMultiplier.port_b.m_flow"},
+  y    = {"ram_m_flow.y", "gaiMasFlo.y", "massFlowRateMultiplier.port_a.m_flow", "massFlowRateMultiplier.port_b.m_flow", "massFlowRateMultiplier1.port_b.m_flow"},
   autoscale = true,
   autoerase = true,
   autoreplot = true,
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/BoilerCHP/Examples/CHPSystem.mos b/AixLib/Resources/Scripts/Dymola/Fluid/BoilerCHP/Examples/CHPSystem.mos
new file mode 100644
index 0000000000..9afef7b876
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/BoilerCHP/Examples/CHPSystem.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Fluid.BoilerCHP.Examples.CHPSystem", tolerance=1e-06, stopTime=1200, method="dassl",  resultFile="CHPSystem");
+createPlot(id=1, position={15, 10, 1039, 644}, y={"TSet.y", "combinedHeatPower.senTHot.T"}, range={0.0, 300.0, -0.2, 1.2000000000000002}, grid=true, filename="CHPSystem.mat", colors={{238,46,47},{28,108,200}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/CarnotWithLosses.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/CarnotWithLosses.mos
new file mode 100644
index 0000000000..cc1e481d5f
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/CarnotWithLosses.mos
@@ -0,0 +1,4 @@
+simulateModel("AixLib.Fluid.Chillers.ModularReversible.Examples.CarnotWithLosses", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="CarnotWithLosses");
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.sigBus.TConInMea", "chi.refCyc.sigBus.TConOutMea", "chi.refCyc.sigBus.TEvaOutMea", "chi.refCyc.sigBus.TEvaInMea"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="CarnotWithLosses.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.QCon_flow", "chi.QEva_flow", "chi.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.sigBus.ySet", "chi.refCyc.sigBus.yMea"}, range={0.0, 3600.0, 0.0, 1.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/LargeScaleWaterToWater.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/LargeScaleWaterToWater.mos
new file mode 100644
index 0000000000..dd64203254
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/LargeScaleWaterToWater.mos
@@ -0,0 +1,4 @@
+simulateModel("AixLib.Fluid.Chillers.ModularReversible.Examples.LargeScaleWaterToWater", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="LargeScaleWaterToWater");
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.sigBus.TConInMea", "chi.refCyc.sigBus.TConOutMea", "chi.refCyc.sigBus.TEvaOutMea", "chi.refCyc.sigBus.TEvaInMea"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="LargeScaleWaterToWater.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.QCon_flow", "chi.QEva_flow", "chi.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.sigBus.ySet", "chi.refCyc.sigBus.yMea"}, range={0.0, 3600.0, 0.0, 1.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/Modular.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/Modular.mos
new file mode 100644
index 0000000000..cfeb4ef15b
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Examples/Modular.mos
@@ -0,0 +1,4 @@
+simulateModel("AixLib.Fluid.Chillers.ModularReversible.Examples.Modular", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="Modular");
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.sigBus.TConInMea", "chi.refCyc.sigBus.TConOutMea", "chi.refCyc.sigBus.TEvaOutMea", "chi.refCyc.sigBus.TEvaInMea"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="Modular.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.QCon_flow", "chi.QEva_flow", "chi.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.sigBus.ySet", "chi.refCyc.sigBus.yMea"}, range={0.0, 3600.0, 0.0, 1.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/Carnot_y.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/Carnot_y.mos
new file mode 100644
index 0000000000..3d76085882
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/Carnot_y.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Fluid.Chillers.ModularReversible.Validation.Carnot_y", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="Chiller_Carnot_y");
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.sta_a1.T", "chi.sta_b1.T", "chi.sta_a2.T", "chi.sta_b2.T"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="Chiller_Carnot_y.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.QEva_flow", "chi.QCon_flow", "chi.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.dp1", "chi.dp2"}, range={0.0, 3600.0, 0.0, 14000.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.COP_nominal", "chi.COP"}, range={0.0, 3600.0, 3.0, 10.0}, grid=true, subPlot=4, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/ConstantCarnotEffectiveness.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/ConstantCarnotEffectiveness.mos
new file mode 100644
index 0000000000..c4702e0f71
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/ConstantCarnotEffectiveness.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Fluid.Chillers.ModularReversible.Validation.ConstantCarnotEffectiveness", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="Chiller_ConstantCarnotEffectiveness");
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.sigBus.TConInMea", "chi.refCyc.sigBus.TConOutMea", "chi.refCyc.sigBus.TEvaInMea", "chi.refCyc.sigBus.TEvaOutMea"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="Chiller_ConstantCarnotEffectiveness.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.QEva_flow", "chi.QCon_flow", "chi.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.dp1", "chi.dp2"}, range={0.0, 3600.0, 0.0, 14000.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.refCycChiCoo.EER_nominal", "chi.EER"}, range={0.0, 3600.0, 3.0, 10.0}, grid=true, subPlot=4, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/TableData2D.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/TableData2D.mos
new file mode 100644
index 0000000000..639871a471
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Chillers/ModularReversible/Validation/TableData2D.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Fluid.Chillers.ModularReversible.Validation.TableData2D", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="TableData2D");
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.refCyc.sigBus.TConInMea", "chi.refCyc.sigBus.TConOutMea", "chi.refCyc.sigBus.TEvaInMea", "chi.refCyc.sigBus.TEvaOutMea"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="TableData2D.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.QEva_flow", "chi.QCon_flow", "chi.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.dp1", "chi.dp2"}, range={0.0, 3600.0, 0.0, 14000.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"chi.EER"}, range={0.0, 3600.0, 3.0, 10.0}, grid=true, subPlot=4, colors={{238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Examples/PlugFlowPipe.mos b/AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Examples/PlugFlowPipe.mos
index ba7a170e00..63b181f9b8 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Examples/PlugFlowPipe.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/FixedResistances/Examples/PlugFlowPipe.mos
@@ -1,3 +1,3 @@
-translateModel("AixLib.Fluid.FixedResistances.Examples.PlugFlowPipe");
+translateModel("AixLib.Fluid.FixedResistances.Examples.PlugFlowPipe");
 simulateModel("AixLib.Fluid.FixedResistances.Examples.PlugFlowPipe", stopTime=1000, method="CVode", tolerance=1e-006, resultFile="PlugFlowPipe");
 createPlot(id=1, position={15, 10, 584, 397}, y={"senTemIn.T", "senTemInNoMix.T", "senTemOutNoMix.T", "senTemOut.T"}, range={0.0, 1000.0, 45.0, 75.0}, grid=true, colors={{28,108,200}, {0,140,72}, {217,67,180}, {238,46,47}}, timeUnit="s", displayUnits={"degC", "degC", "degC", "degC"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Examples/CoolingOffice.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Examples/CoolingOffice.mos
new file mode 100644
index 0000000000..e93dfa1c41
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Examples/CoolingOffice.mos
@@ -0,0 +1,13 @@
+simulateModel("AixLib.Fluid.Geothermal.Aquifer.Examples.CoolingOffice", tolerance=1e-6, startTime=0, stopTime=7776000, method="CVode", resultFile="CoolingOffice");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"aquWel.TAquHot[50]"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ filename = "CoolingOffice.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Validation/NumberWells.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Validation/NumberWells.mos
new file mode 100644
index 0000000000..8df8a88c0c
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Validation/NumberWells.mos
@@ -0,0 +1,13 @@
+simulateModel("AixLib.Fluid.Geothermal.Aquifer.Validation.NumberWells", tolerance=1e-6, startTime=0, stopTime=31536000, method="CVode", resultFile="NumberWells");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"cheEqu.y"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ filename = "NumberWells.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Validation/SimulationTest.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Validation/SimulationTest.mos
new file mode 100644
index 0000000000..f6c583b94e
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Aquifer/Validation/SimulationTest.mos
@@ -0,0 +1,13 @@
+simulateModel("AixLib.Fluid.Geothermal.Aquifer.Validation.SimulationTest", tolerance=1e-6, startTime=0, stopTime=31536000, method="CVode", resultFile="SimulationTest");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"aquWel.TAquCol[150]"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ filename = "SimulationTest.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ClusterBoreholes_100boreholes.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ClusterBoreholes_100boreholes.mos
new file mode 100644
index 0000000000..4be8503d59
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/ClusterBoreholes_100boreholes.mos
@@ -0,0 +1,15 @@
+simulateModel("AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation.ClusterBoreholes_100boreholes", startTime=0, stopTime=1.0, tolerance=1E-6, method="CVode", resultFile="ClusterBoreholes_100boreholes");
+
+createPlot(
+  id   = 1,
+  position = {35, 30, 631, 456},
+  x    = "time",
+  y    = {"cmp"},
+  autoscale = true,
+  autoerase = true,
+  autoreplot = true,
+  grid=true,
+  color=true,
+  filename="ClusterBoreholes_100boreholes.mat",
+  leftTitleType = 1,
+  bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Equivalent.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Equivalent.mos
new file mode 100644
index 0000000000..4e51f9c3bd
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Equivalent.mos
@@ -0,0 +1,14 @@
+simulateModel("AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation.FiniteLineSource_Equivalent", startTime=0, stopTime=20.0, tolerance=1E-6, method="CVode", resultFile="FiniteLineSource_Equivalent");
+createPlot(
+  id   = 1,
+  position = {35, 30, 631, 456},
+  x    = "t",
+  y    = {"hRea", "hMir", "h"},
+  autoscale = true,
+  autoerase = true,
+  autoreplot = true,
+  grid=true,
+  color=true,
+  filename="FiniteLineSource_Equivalent.mat",
+  leftTitleType = 1,
+  bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Equivalent.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Equivalent.mos
new file mode 100644
index 0000000000..a2b59fed35
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_Integrand_Equivalent.mos
@@ -0,0 +1,14 @@
+simulateModel("AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation.FiniteLineSource_Integrand_Equivalent", startTime=0.01, stopTime=1.0, tolerance=1E-6, method="CVode", resultFile="FiniteLineSource_Integrand_Equivalent");
+createPlot(
+  id   = 1,
+  position = {35, 30, 631, 456},
+  x    = "u",
+  y    = {"yRea", "yMir", "y"},
+  autoscale = true,
+  autoerase = true,
+  autoreplot = true,
+  grid=true,
+  color=true,
+  filename="FiniteLineSource_Integrand_Equivalent.mat",
+  leftTitleType = 1,
+  bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_SteadyState.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_SteadyState.mos
new file mode 100644
index 0000000000..7c2c3f3529
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Geothermal/Borefields/BaseClasses/HeatTransfer/ThermalResponseFactors/Validation/FiniteLineSource_SteadyState.mos
@@ -0,0 +1,14 @@
+simulateModel("AixLib.Fluid.Geothermal.Borefields.BaseClasses.HeatTransfer.ThermalResponseFactors.Validation.FiniteLineSource_SteadyState", startTime=0.0, stopTime=50.0, tolerance=1E-6, method="CVode", resultFile="FiniteLineSource_SteadyState");
+createPlot(
+  id   = 1,
+  position = {35, 30, 631, 456},
+  x    = "dis",
+  y    = {"hRea", "hMir", "h"},
+  autoscale = true,
+  autoerase = true,
+  autoreplot = true,
+  grid=true,
+  color=true,
+  filename="FiniteLineSource_SteadyState.mat",
+  leftTitleType = 1,
+  bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/HeaterCooler_u.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/HeaterCooler_u.mos
index 0d75ad9a0c..3480a22076 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/HeaterCooler_u.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/HeaterCooler_u.mos
@@ -1,24 +1,18 @@
 simulateModel("AixLib.Fluid.HeatExchangers.Validation.HeaterCooler_u", method="CVode", tolerance=1e-6, stopTime=1200, resultFile="HeaterCooler_u");
-createPlot(id = 1,
- position = {78, 39, 400, 444},
- y = {"con1.u_s", "con1.u_m", "con2.u_m"},
- range = {0.0, 1200.0, 35.0, 15.0},
- autoscale = true,
- autoerase = true,
- autoreplot = true,
- grid = true,
- color = true,
- leftTitleType = 1,
- bottomTitleType = 1);
-createPlot(id = 20,
- position = {78, 39, 400, 219},
- y = {"con1.y", "con2.y"},
- range = {0.0, 1200.0, 1.5, -0.5},
- autoscale = true,
- autoerase = true,
- autoreplot = true,
- grid = true,
- color = true,
- subPlot = 2,
- leftTitleType = 1,
- bottomTitleType = 1);
+createPlot(id=1,
+ position={125, 65, 400, 447},
+ y={"con1.u_s", "con1.u_m", "con2.u_m"},
+ range={0.0, 1200.0, 290.0, 305.0},
+ grid=true,
+ subPlot=101,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s");
+createPlot(id=1,
+ position={125, 65, 400, 447},
+ y={"con1.y", "con2.y"},
+ range={0.0, 1200.0, -0.5, 1.5},
+ grid=true,
+ subPlot=102,
+ colors={{28,108,200}, {238,46,47}},
+ timeUnit="s");
+
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mos
index de53eb913d..2e83368bfe 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatExchangers/Validation/WetCoilEffectivenessNTU.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.Fluid.HeatExchangers.Validation.WetCoilEffectivenessNTU",
+simulateModel("AixLib.Fluid.HeatExchangers.Validation.WetCoilEffectivenessNTU",
     stopTime=1000,
     method="cvode",
     tolerance=1e-6,
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/AntiFreeze.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/AntiFreeze.mos
new file mode 100644
index 0000000000..c4a586e535
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/AntiFreeze.mos
@@ -0,0 +1,31 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples.AntiFreeze", stopTime=100, method="CVode", tolerance=1e-08, resultFile="AntiFreeze");
+createPlot(id = 1,
+ position = {19, 32, 826, 408},
+ y = {"ySet", "yOut"},
+ range = {0.0, 100.0, 0.0, 1.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "AntiFreeze.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 826, 408},
+ y = {"antFre.sigBus.TConInMea", "antFre.sigBus.TEvaOutMea", "antFre.TAntFre"},
+ range = {0.0, 100.0, 0.0, 15.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}, {0, 0, 0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/MinimalFlowRate.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/MinimalFlowRate.mos
new file mode 100644
index 0000000000..70e98819aa
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/MinimalFlowRate.mos
@@ -0,0 +1,31 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples.MinimalFlowRate", stopTime=100, method="CVode", tolerance=1e-08, resultFile="MinimalFlowRate");
+createPlot(id = 1,
+ position = {19, 32, 826, 408},
+ y = {"ySet", "yOut"},
+ range = {0.0, 100.0, 0.0, 1.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "MinimalFlowRate.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 826, 408},
+ y = {"minFloRatSaf.sigBus.mEvaMea_flow", "minFloRatSaf.sigBus.mConMea_flow", "minFloRatSaf.mEvaMin_flow", "minFloRatSaf.mConMin_flow"},
+ range = {0.0, 100.0, 0.0, 1.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}, {0, 0, 0}, {0, 0, 0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OnOff.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OnOff.mos
new file mode 100644
index 0000000000..6a016483a4
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OnOff.mos
@@ -0,0 +1,16 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples.OnOff", stopTime=7200, method="CVode", tolerance=1e-08, resultFile="OnOff");
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"ySet", "yOut"},
+ range = {0.0, 7200.0, 0.0, 1.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "OnOff.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OperationalEnvelope.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OperationalEnvelope.mos
new file mode 100644
index 0000000000..dff0319d08
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/OperationalEnvelope.mos
@@ -0,0 +1,32 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples.OperationalEnvelope", stopTime=100, method="CVode", tolerance=1e-08, resultFile="OperationalEnvelope");
+createPlot(id = 1,
+ position = {19, 32, 826, 408},
+ y = {"ySet", "yOut"},
+ range = {0.0, 100.0, 0.0, 1.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "OperationalEnvelope.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 826, 408},
+ y = {"sigBus.TConInMea", "opeEnv.bouMapHea.tabBou.y[1]", "opeEnv.bouMapCoo.tab[2, 2]"},
+ range = {0.0, 100.0, 0.0, 15.0},
+ displayUnits = {"K", "", ""},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {0, 0, 0}, {0, 0, 0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/Safety.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/Safety.mos
new file mode 100644
index 0000000000..246d5a4daa
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Controls/Safety/Examples/Safety.mos
@@ -0,0 +1,31 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Controls.Safety.Examples.Safety", stopTime=100, method="CVode", tolerance=1e-08, resultFile="Safety");
+createPlot(id = 1,
+ position = {19, 32, 826, 408},
+ y = {"ySet", "yOut"},
+ range = {0.0, 100.0, 0.0, 1.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "Safety.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 826, 408},
+ y = {"safCtr.minFlowErr", "safCtr.opeEnvErr", "safCtr.antFreErr"},
+ range = {0.0, 100.0, 0.0, 15.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {0, 0, 255}, {0, 0, 255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/AirToWater2D_OneRoomRadiator.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/AirToWater2D_OneRoomRadiator.mos
new file mode 100644
index 0000000000..1a31cdb1a4
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/AirToWater2D_OneRoomRadiator.mos
@@ -0,0 +1,46 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Examples.AirToWater2D_OneRoomRadiator", stopTime=86400, method="CVode", tolerance=1e-08, resultFile="AirToWater2D_OneRoomRadiator");
+createPlot(id = 1,
+ position = {19, 32, 809, 500},
+ y = {"vol.T_start", "vol.T"},
+ range = {0.0, 180000.0, 100.0, -20.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "AirToWater2D_OneRoomRadiator.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 809, 500},
+ y = {"temSup.T", "temRet.T"},
+ range = {0.0, 180000.0, 80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 809, 500},
+ y = {"heaPum.refCyc.sigBus.hea", "heaPum.refCyc.sigBus.onOffMea"},
+ range = {0.0, 180000.0, 80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/CarnotWithLosses_OneRoomRadiator.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/CarnotWithLosses_OneRoomRadiator.mos
new file mode 100644
index 0000000000..8055ab0a71
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/CarnotWithLosses_OneRoomRadiator.mos
@@ -0,0 +1,46 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Examples.CarnotWithLosses_OneRoomRadiator", stopTime=86400, method="CVode", tolerance=1e-08, resultFile="CarnotWithLosses_OneRoomRadiator");
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"vol.T_start", "vol.T"},
+ range = {0.0, 180000.0, 100.0, -20.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "CarnotWithLosses_OneRoomRadiator.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"temSup.T", "temRet.T"},
+ range = {0.0, 180000.0, 80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"heaPum.refCyc.sigBus.hea", "heaPum.refCyc.sigBus.onOffMea"},
+ range = {0.0, 180000.0, 80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/LargeScaleWaterToWater_OneRoomRadiator.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/LargeScaleWaterToWater_OneRoomRadiator.mos
new file mode 100644
index 0000000000..e7dc6e9466
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/LargeScaleWaterToWater_OneRoomRadiator.mos
@@ -0,0 +1,46 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Examples.LargeScaleWaterToWater_OneRoomRadiator", stopTime=86400, method="CVode", tolerance=1e-08, resultFile="LargeScaleWaterToWater_OneRoomRadiator");
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"vol.T_start", "vol.T"},
+ range = {0.0, 180000.0, 100.0, -20.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "LargeScaleWaterToWater_OneRoomRadiator.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"temSup.T", "temRet.T"},
+ range = {0.0, 180000.0, 80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"heaPum.refCyc.sigBus.onOffMea"},
+ range = {0.0, 180000.0, 80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/Modular_OneRoomRadiator.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/Modular_OneRoomRadiator.mos
new file mode 100644
index 0000000000..79d3483750
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Examples/Modular_OneRoomRadiator.mos
@@ -0,0 +1,46 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Examples.Modular_OneRoomRadiator", stopTime=86400, method="CVode", tolerance=1e-08, resultFile="Modular_OneRoomRadiator");
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"vol.T_start", "vol.T"},
+ range = {0.0, 180000.0, 100.0, -20.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "Modular_OneRoomRadiator.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"temSup.T", "temRet.T"},
+ range = {0.0, 180000.0, 80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
+createPlot(id = 1,
+ position = {19, 32, 798, 500},
+ y = {"heaPum.refCyc.sigBus.hea", "heaPum.refCyc.sigBus.onOffMea"},
+ range = {0.0, 180000.0, 80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 3,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0, 0, 255}, {255, 0, 0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/Carnot_y.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/Carnot_y.mos
new file mode 100644
index 0000000000..1144d87c9a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/Carnot_y.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative.Carnot_y", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="HeatPump_Carnot_y");
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.sta_a1.T", "heaPum.sta_b1.T", "heaPum.sta_a2.T", "heaPum.sta_b2.T"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="HeatPump_Carnot_y.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.QEva_flow", "heaPum.QCon_flow", "heaPum.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.dp1", "heaPum.dp2"}, range={0.0, 3600.0, 0.0, 14000.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.COP_nominal", "heaPum.COP"}, range={0.0, 3600.0, 3.0, 10.0}, grid=true, subPlot=4, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/ConstantCarnotEffectiveness.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/ConstantCarnotEffectiveness.mos
new file mode 100644
index 0000000000..84fde5f216
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/ConstantCarnotEffectiveness.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative.ConstantCarnotEffectiveness", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="HeatPump_ConstantCarnotEffectiveness");
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.refCyc.sigBus.TConInMea", "heaPum.refCyc.sigBus.TConOutMea", "heaPum.refCyc.sigBus.TEvaInMea", "heaPum.refCyc.sigBus.TEvaOutMea"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="HeatPump_ConstantCarnotEffectiveness.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.QEva_flow", "heaPum.QCon_flow", "heaPum.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.dp1", "heaPum.dp2"}, range={0.0, 3600.0, 0.0, 14000.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.refCyc.refCycHeaPumHea.COP_nominal", "heaPum.COP"}, range={0.0, 3600.0, 3.0, 10.0}, grid=true, subPlot=4, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/TableData2D.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/TableData2D.mos
new file mode 100644
index 0000000000..889e6eb08a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/Comparative/TableData2D.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Validation.Comparative.TableData2D", tolerance=1e-6, stopTime=3600, method="CVode", resultFile="HeatPump_TableData2D");
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.refCyc.sigBus.TConInMea", "heaPum.refCyc.sigBus.TConOutMea", "heaPum.refCyc.sigBus.TEvaInMea", "heaPum.refCyc.sigBus.TEvaOutMea"}, range={0.0, 3600.0, 5.0, 40.0}, grid=true, filename="HeatPump_TableData2D.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.QEva_flow", "heaPum.QCon_flow", "heaPum.P"}, range={0.0, 3600.0, -200000.0, 300000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.dp1", "heaPum.dp2"}, range={0.0, 3600.0, 0.0, 14000.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"heaPum.COP"}, range={0.0, 3600.0, 3.0, 10.0}, grid=true, subPlot=4, colors={{238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/ConstantCarnotEffectiveness.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/ConstantCarnotEffectiveness.mos
new file mode 100644
index 0000000000..67ba252da6
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/ConstantCarnotEffectiveness.mos
@@ -0,0 +1,4 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Validation.ConstantCarnotEffectiveness", tolerance=1e-6, stopTime=14365, method="CVode", resultFile="ConstantCarnotEffectiveness");
+createPlot(id=2, position={39, 13, 913, 546}, y={"TConOutMea", "TConOutSim"}, range={0.0, 14365.0, 293.15, 363.15}, grid=true, filename="ConstantCarnotEffectiveness.mat", colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"PEleMea", "PEleSim"}, range={0.0, 14365.0, 0.0, 3000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"TEvaOutMea", "TEvaOutSim"}, range={0.0, 14365.0, 273.15, 303.15}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/TableData2D.mos b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/TableData2D.mos
new file mode 100644
index 0000000000..0cd00bac1a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/HeatPumps/ModularReversible/Validation/TableData2D.mos
@@ -0,0 +1,4 @@
+simulateModel("AixLib.Fluid.HeatPumps.ModularReversible.Validation.TableData2D", tolerance=1e-6, stopTime=14365, method="CVode", resultFile="TableData2D");
+createPlot(id=2, position={39, 13, 913, 546}, y={"TConOutMea", "TConOutSim"}, range={0.0, 14365.0, 293.15, 363.15}, grid=true, filename="TableData2D.mat", colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"PEleMea", "PEleSim"}, range={0.0, 14365.0, 0.0, 3000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}});
+createPlot(id=2, position={39, 13, 913, 546}, y={"TEvaOutMea", "TEvaOutSim"}, range={0.0, 14365.0, 273.15, 303.15}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MSLCombustionAir.mos b/AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MSLCombustionAir.mos
new file mode 100644
index 0000000000..4496b196dd
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MSLCombustionAir.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Fluid.MixingVolumes.Validation.MSLCombustionAir", method="Cvode", tolerance=1e-06, resultFile="MSLCombustionAir");
+createPlot(id=1, position={15, 15, 930, 581}, y={"vol.T"}, range={0.0, 1.0, 19.95, 20.0}, grid=true, colors={{28,108,200}}, timeUnit="s", displayUnits={"degC"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MSLFlueGasSixComponents.mos b/AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MSLFlueGasSixComponents.mos
new file mode 100644
index 0000000000..330c75ccdb
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/MixingVolumes/Validation/MSLFlueGasSixComponents.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Fluid.MixingVolumes.Validation.MSLFlueGasSixComponents", method="Cvode", tolerance=1e-06, resultFile="MSLFlueGasSixComponents");
+createPlot(id=1, position={15, 15, 930, 581}, y={"vol.T"}, range={0.0, 1.0, 19.95, 20.0}, grid=true, colors={{28,108,200}}, timeUnit="s", displayUnits={"degC"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerComparison.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerComparison.mos
new file mode 100644
index 0000000000..3e76a430ce
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerComparison.mos
@@ -0,0 +1,78 @@
+simulateModel("AixLib.Fluid.Movers.BaseClasses.Validation.EulerComparison",
+  method="Dassl",
+  tolerance=1e-06,
+  resultFile="EulerComparison");
+// Plot commands
+createPlot(id=1, 
+ position={1, 2, 499, 568},
+ x="V_flow",
+ y={"eta1", "eta2"},
+ grid=true,
+ legends={"Power Curve", "Euler Number"},
+ leftTitleType=2,
+ leftTitle="Efficiency [1]",
+ colors={{28,108,200}, {238,46,47}},
+ patterns={LinePattern.Solid, LinePattern.Dash},
+ thicknesses={0.5, 0.5},
+ timeUnit="m3/s",
+ displayUnits={"1", "1"});
+createPlot(id=1,
+ position={1, 2, 499, 568},
+ x="V_flow",
+ y={"P1", "P2"},
+ grid=true,
+ legends={"Power Curve", "Euler Number"},
+ subPlot=102,
+ leftTitleType=2,
+ leftTitle="Power [W]",
+ colors={{28,108,200}, {238,46,47}},
+ patterns={LinePattern.Solid, LinePattern.Dash},
+ thicknesses={0.5, 0.5},
+ timeUnit="m3/s",
+ displayUnits={"W", "W"});
+createPlot(id=2,
+ position={482, 2, 489, 565},
+ x="eff1.dp",
+ y={"eta1", "eta2"},
+ grid=true,
+ legends={"Power Curve", "Euler Number"},
+ leftTitleType=2,
+ leftTitle="Efficiency [1]",
+ colors={{28,108,200}, {238,46,47}},
+ patterns={LinePattern.Solid, LinePattern.Dash},
+ thicknesses={0.5, 0.5},
+ timeUnit="Pa",
+ displayUnits={"1", "1"});
+createPlot(id=2,
+ position={482, 2, 489, 565},
+ x="eff1.dp",
+ y={"P1", "P2"},
+ grid=true,
+ legends={"Power Curve", "Euler Number"},
+ leftTitleType=2,
+ leftTitle="Power [W]",
+ subPlot=102,
+ colors={{28,108,200}, {238,46,47}},
+ patterns={LinePattern.Solid, LinePattern.Dash},
+ thicknesses={0.5, 0.5},
+ timeUnit="Pa",
+ displayUnits={"W", "W"});
+createPlot(id=3,
+ position={964, 4, 488, 563},
+ x="V_flow",
+ y={"eff1.dp"},
+ grid=true,
+ legends={"Pressure Rise"},
+ colors={{28,108,200}},
+ timeUnit="m3/s",
+ displayUnits={"Pa"});
+createPlot(id=3,
+ position={964, 4, 488, 563},
+ y={"eff1.r_N"},
+ grid=true, 
+ legends={"Relative Speed"},
+ subPlot=102,
+ colors={{28,108,200}},
+ timeUnit="s",
+ displayUnits={"1"});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerCurve.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerCurve.mos
new file mode 100644
index 0000000000..d2e6442c83
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerCurve.mos
@@ -0,0 +1,18 @@
+simulateModel("AixLib.Fluid.Movers.BaseClasses.Validation.EulerCurve",
+ stopTime=10,
+ tolerance=1e-06,
+ resultFile="EulerCurve");
+// Plot commands
+createPlot(id=1,
+ position={294, 80, 535, 374},
+ x="x",
+ y={"etaApp", "etaOri"},
+ range={-4.0, 6.0, 0.0, 1.0},
+ autoscale=false,
+ grid=true,
+ legends={"Approximation", "Original"},
+ leftTitleType=2,
+ leftTitle="Ratio of Efficiency",
+ bottomTitleType=2,
+ bottomTitle="Log10 of Ratio of Euler Number",
+ colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerReducedSpeed.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerReducedSpeed.mos
new file mode 100644
index 0000000000..e412114ed5
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/EulerReducedSpeed.mos
@@ -0,0 +1,20 @@
+simulateModel("AixLib.Fluid.Movers.BaseClasses.Validation.EulerReducedSpeed",
+  method="Dassl",
+  tolerance=1e-06, 
+  resultFile="EulerReducedSpeed");
+// Plot commands
+createPlot(
+ id=1,
+ position={53, 37, 881, 372},
+ y={"pow1", "eff1.WHyd", "pow2", "eff2.WHyd", "pow3", "eff3.WHyd"},
+ range={0.0, 1.0, 0.0, 14000.0},
+ grid=true,
+ legends={"Measured y=1", "Euler", "Measured y=0.83", "Euler", "Measured y=0.61", "Euler"},
+ leftTitleType=2,
+ leftTitle="Hydraulic Work [W]",
+ colors={{238,46,47}, {238,46,47}, {28,108,200}, {28,108,200}, {0,140,72}, {0,140,72}},
+ patterns={LinePattern.Dash, LinePattern.Solid, LinePattern.Solid,
+           LinePattern.Dash, LinePattern.Solid, LinePattern.Dash},
+ thicknesses={0.5, 0.5, 0.5, 0.5, 0.5, 0.5},
+ timeUnit="s",
+ displayUnits={"W", "W", "W", "W", "W", "W"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/HydraulicEfficiencyMethods.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/HydraulicEfficiencyMethods.mos
new file mode 100644
index 0000000000..6be331d2a4
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/HydraulicEfficiencyMethods.mos
@@ -0,0 +1,43 @@
+simulateModel("AixLib.Fluid.Movers.BaseClasses.Validation.HydraulicEfficiencyMethods",
+ method="CVode",
+ tolerance=1e-6,
+ stopTime=1.0,
+ resultFile="HydraulicEfficiencyMethods");
+// Plot commands
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff1.eta", "eff1.etaHyd", "eff1.etaMot"},
+ range={0.0, 1.0, 0.0, 1.0},
+ grid=true,
+ subPlot=101,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff2.eta", "eff2.etaHyd", "eff2.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=102,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff3.eta", "eff3.etaHyd", "eff3.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=103,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff4.eta", "eff4.etaHyd", "eff4.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=104,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/MotorEfficiencyMethods.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/MotorEfficiencyMethods.mos
new file mode 100644
index 0000000000..b6b0bac439
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/MotorEfficiencyMethods.mos
@@ -0,0 +1,43 @@
+simulateModel("AixLib.Fluid.Movers.BaseClasses.Validation.MotorEfficiencyMethods",
+ method="CVode",
+ tolerance=1e-6,
+ stopTime=1.0,
+ resultFile="MotorEfficiencyMethods");
+// Plot commands
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff1.eta", "eff1.etaHyd", "eff1.etaMot"},
+ range={0.0, 1.0, 0.0, 1.0},
+ grid=true,
+ subPlot=101,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff2.eta", "eff2.etaHyd", "eff2.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=102,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff3.eta", "eff3.etaHyd", "eff3.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=103,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff4.eta", "eff4.etaHyd", "eff4.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=104,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/NegativePressureOrFlow.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/NegativePressureOrFlow.mos
new file mode 100644
index 0000000000..b35a3b7cfd
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/NegativePressureOrFlow.mos
@@ -0,0 +1,37 @@
+simulateModel("AixLib.Fluid.Movers.BaseClasses.Validation.NegativePressureOrFlow",
+ tolerance=1e-6,
+ stopTime=3600,
+ method="CVode",
+ resultFile="NegativePressureOrFlow");
+// Plot commands
+createPlot(id=1,
+ position={93, 33, 666, 645},
+ y={"eff.PEle"},
+ range={0.0, 4000.0, -500.0, 1000.0},
+ autoscale=false,
+ grid=true,
+ subPlot=101,
+ colors={{28,108,200}},
+ timeUnit="s",
+ displayUnits={"W"});
+createPlot(id=1,
+ position={93, 33, 666, 645},
+ y={"eff.dp_in"},
+ range={0.0, 4000.0, -10000.0, 20000.0},
+ autoscale=false,
+ grid=true,
+ subPlot=102,
+ colors={{28,108,200}},
+ timeUnit="s",
+ displayUnits={"Pa"});
+createPlot(id=1,
+ position={93, 33, 666, 645},
+ y={"eff.V_flow"},
+ range={0.0, 4000.0, -0.1, 0.2},
+ autoscale=false,
+ grid=true,
+ subPlot=103,
+ colors={{28,108,200}},
+ timeUnit="s",
+ displayUnits={"m3/s"});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/TotalEfficiencyMethods.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/TotalEfficiencyMethods.mos
new file mode 100644
index 0000000000..311c0602b3
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/BaseClasses/Validation/TotalEfficiencyMethods.mos
@@ -0,0 +1,43 @@
+simulateModel("AixLib.Fluid.Movers.BaseClasses.Validation.TotalEfficiencyMethods",
+ method="CVode",
+ tolerance=1e-6,
+ stopTime=1.0,
+ resultFile="TotalEfficiencyMethods");
+// Plot commands
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff1.eta", "eff1.etaHyd", "eff1.etaMot"},
+ range={0.0, 1.0, 0.0, 1.0},
+ grid=true,
+ subPlot=101,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff2.eta", "eff2.etaHyd", "eff2.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=102,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff3.eta", "eff3.etaHyd", "eff3.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=103,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+createPlot(id=1,
+ position={68, 1, 583, 554},
+ y={"eff4.eta", "eff4.etaHyd", "eff4.etaMot"},
+ range={0.0, 1.0, -1.0, 1.0},
+ grid=true,
+ subPlot=104,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpVar.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpConst.mos
similarity index 84%
rename from AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpVar.mos
rename to AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpConst.mos
index c785e2f6ed..9b23edae3b 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpVar.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpConst.mos
@@ -1,5 +1,5 @@
 removePlots();
-simulateModel("AixLib.Fluid.Movers.DpControlledMovers.Examples.DpControlled_dpVar", startTime=0, stopTime=3600, tolerance=1e-6, method="dassl", resultFile="DpControlled_dpVar");
+simulateModel("AixLib.Fluid.Movers.DpControlledMovers.Examples.DpConst", startTime=0, stopTime=3600, tolerance=1e-6, method="dassl", resultFile="DpConst");
 
 createPlot(id=1,
  x="dpControlled_dp.mov.VMachine_flow",
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpConst.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpVar.mos
similarity index 84%
rename from AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpConst.mos
rename to AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpVar.mos
index 82cadd26ca..1cc6743ca7 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpControlled_dpConst.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/DpControlledMovers/Examples/DpVar.mos
@@ -1,5 +1,5 @@
 removePlots();
-simulateModel("AixLib.Fluid.Movers.DpControlledMovers.Examples.DpControlled_dpConst", startTime=0, stopTime=3600, tolerance=1e-6, method="dassl", resultFile="DpControlled_dpConst");
+simulateModel("AixLib.Fluid.Movers.DpControlledMovers.Examples.DpVar", startTime=0, stopTime=3600, tolerance=1e-6, method="dassl", resultFile="DpVar");
 
 createPlot(id=1,
  x="dpControlled_dp.mov.VMachine_flow",
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverContinuous.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverContinuous.mos
index 44fc3c93c6..5030cf31c3 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverContinuous.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverContinuous.mos
@@ -1,7 +1,7 @@
 simulateModel("AixLib.Fluid.Movers.Examples.MoverContinuous", stopTime=1, method="CVode", tolerance=1e-06, resultFile="MoverContinuous");
 createPlot(id=1,
 position={15, 10, 586, 422},
-y={"pump_Nrpm.m_flow", "pump_dp.m_flow", "pump_m_flow.m_flow", "pump_y.m_flow"},
+y={"pump_dp.m_flow", "pump_m_flow.m_flow", "pump_y.m_flow"},
 range={0.0, 1.0, -0.2, 2.2},
 grid=true,
-colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+colors={{28,108,200}, {238,46,47}, {0,140,72}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverParameter.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverParameter.mos
index 48228c8b69..82e67b1bfb 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverParameter.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverParameter.mos
@@ -1,7 +1,7 @@
 simulateModel("AixLib.Fluid.Movers.Examples.MoverParameter", stopTime=1, method="CVode", tolerance=1e-06, resultFile="MoverParameter");
 createPlot(id=1,
 position={15, 10, 586, 422},
-y={"pump_Nrpm.m_flow", "pump_dp.m_flow", "pump_m_flow.m_flow", "pump_y.m_flow"},
+y={"pump_dp.m_flow", "pump_m_flow.m_flow", "pump_y.m_flow"},
 range={0.0, 1.0, -0.2, 2.2},
 grid=true,
-colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+colors={{28,108,200}, {238,46,47}, {0,140,72}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverStages.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverStages.mos
index 845bf63fff..d4a84ef11e 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverStages.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/MoverStages.mos
@@ -1,7 +1,7 @@
 simulateModel("AixLib.Fluid.Movers.Examples.MoverStages", stopTime=1, method="CVode", tolerance=1e-06, resultFile="MoverStages");
 createPlot(id=1,
 position={15, 10, 586, 422},
-y={"pump_Nrpm.m_flow", "pump_dp.m_flow", "pump_m_flow.m_flow", "pump_y.m_flow"},
+y={"pump_dp.m_flow", "pump_m_flow.m_flow", "pump_y.m_flow"},
 range={0.0, 1.0, -0.2, 2.2},
 grid=true,
-colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}});
+colors={{28,108,200}, {238,46,47}, {0,140,72}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/StaticReset.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/StaticReset.mos
new file mode 100644
index 0000000000..7d83e600da
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Examples/StaticReset.mos
@@ -0,0 +1,32 @@
+simulateModel("AixLib.Fluid.Movers.Examples.StaticReset",
+  method="Dassl",
+  stopTime=3600,
+  tolerance=1e-06,
+  resultFile="StaticReset");
+// Plot commands
+createPlot(id=1,
+ position={15, 15, 647, 371},
+ x="fan1.VMachine_flow",
+ y={"fan1.P", "fan2.P", "fan3.P"},
+ range={0.0, 14.0, -5000.0, 25000.0},
+ grid=true,
+ legends={"Power Curve", "Euler Number", "Constant Efficiency"},
+ leftTitleType=2,
+ leftTitle="Power [W]",
+ bottomTitleType=2, 
+ bottomTitle="Flow [m3/s]",
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ patterns={LinePattern.Solid, LinePattern.Dash, LinePattern.DashDot},
+ thicknesses={0.5, 0.5, 0.5},
+ timeUnit="m3/s",
+ displayUnits={"W", "W", "W"});
+createPlot(id=2,
+ position={680, 17, 592, 372},
+ y={"fan1.y_actual", "fan2.y_actual", "fan3.y_actual"},
+ range={0.0, 4000.0, -0.2, 1.0000000000000002},
+ grid=true,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}},
+ patterns={LinePattern.Solid, LinePattern.Dash, LinePattern.DashDot},
+ timeUnit="s",
+ displayUnits={"1", "1", "1"});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Preconfigured/Validation/ControlledFlowMachinePreconfigured.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Preconfigured/Validation/ControlledFlowMachinePreconfigured.mos
new file mode 100644
index 0000000000..17de592516
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Preconfigured/Validation/ControlledFlowMachinePreconfigured.mos
@@ -0,0 +1,24 @@
+simulateModel("AixLib.Fluid.Movers.Preconfigured.Validation.ControlledFlowMachinePreconfigured", method="CVode", tolerance=1e-6, stopTime=600, resultFile="ControlledFlowMachinePreconfigured");
+createPlot(id = 3,
+ position = {55, 50, 750, 480},
+ y = {"fan1.m_flow", "fan2.m_flow", "fan3.m_flow"},
+ range = {0, 600, 2.5, 0.5},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
+createPlot(id = 3,
+ position = {55, 50, 750, 237},
+ y = {"fan1.dp", "fan2.dp", "fan3.dp"},
+ range = {0, 600, 700.0, 0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerHydraulic.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerHydraulic.mos
new file mode 100644
index 0000000000..d9e820669c
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerHydraulic.mos
@@ -0,0 +1,6 @@
+simulateModel("AixLib.Fluid.Movers.Validation.ComparePowerHydraulic", method="dassl", tolerance=1e-6, stopTime=200, resultFile="ComparePowerHydraulic");
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov1.eta", "mov1.etaHyd", "mov1.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=101, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov2.eta", "mov2.etaHyd", "mov2.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov3.eta", "mov3.etaHyd", "mov3.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=103, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=2, position={607, 91, 601, 428}, y={"ramSpe.y", "ramDam.y"}, range={0.0, 200.0, -0.5, 1.5}, grid=true, subPlot=101, colors={{28,108,200}, {238,46,47}}, timeUnit="s", displayUnits={"1", "1"});
+createPlot(id=2, position={607, 91, 601, 428}, y={"mov1.P", "mov2.P", "mov3.P"}, range={0.0, 200.0, -10000.0, 30000.0}, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"W", "W", "W"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerInput.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerInput.mos
new file mode 100644
index 0000000000..ae873299e8
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerInput.mos
@@ -0,0 +1,6 @@
+simulateModel("AixLib.Fluid.Movers.Validation.ComparePowerInput", method="dassl", tolerance=1e-6, stopTime=200, resultFile="ComparePowerInput");
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov1.eta", "mov1.etaHyd", "mov1.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=101, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov2.eta", "mov2.etaHyd", "mov2.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov3.eta", "mov3.etaHyd", "mov3.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=103, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=2, position={607, 91, 601, 428}, y={"ramSpe.y", "ramDam.y"}, range={0.0, 200.0, -0.5, 1.5}, grid=true, subPlot=101, colors={{28,108,200}, {238,46,47}}, timeUnit="s", displayUnits={"1", "1"});
+createPlot(id=2, position={607, 91, 601, 428}, y={"mov1.P", "mov2.P", "mov3.P"}, range={0.0, 200.0, -10000.0, 30000.0}, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"W", "W", "W"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerTotal.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerTotal.mos
new file mode 100644
index 0000000000..494a1f6d46
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ComparePowerTotal.mos
@@ -0,0 +1,6 @@
+simulateModel("AixLib.Fluid.Movers.Validation.ComparePowerTotal", method="dassl", tolerance=1e-6, stopTime=200, resultFile="ComparePowerTotal");
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov1.eta", "mov1.etaHyd", "mov1.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=101, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov2.eta", "mov2.etaHyd", "mov2.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=1, position={26, -4, 656, 575}, y={"mov3.eta", "mov3.etaHyd", "mov3.etaMot"}, range={0.0, 200.0, -0.5, 1.0}, grid=true, subPlot=103, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"1", "1", "1"});
+createPlot(id=2, position={607, 91, 601, 428}, y={"ramSpe.y", "ramDam.y"}, range={0.0, 200.0, -0.5, 1.5}, grid=true, subPlot=101, colors={{28,108,200}, {238,46,47}}, timeUnit="s", displayUnits={"1", "1"});
+createPlot(id=2, position={607, 91, 601, 428}, y={"mov1.P", "mov2.P", "mov3.P"}, range={0.0, 200.0, -10000.0, 30000.0}, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}}, timeUnit="s", displayUnits={"W", "W", "W"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachine.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachine.mos
index 0757bc93aa..b884cd1ba0 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachine.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachine.mos
@@ -1,7 +1,7 @@
 simulateModel("AixLib.Fluid.Movers.Validation.ControlledFlowMachine", method="CVode", tolerance=1e-6, stopTime=600, resultFile="ControlledFlowMachine");
 createPlot(id = 3,
  position = {55, 50, 750, 480},
- y = {"fan1.m_flow", "fan2.m_flow", "fan3.m_flow", "fan4.m_flow"},
+ y = {"fan1.m_flow", "fan2.m_flow", "fan3.m_flow"},
  range = {0, 600, 2.5, 0.5},
  autoscale = true,
  autoerase = true,
@@ -12,7 +12,7 @@ createPlot(id = 3,
  bottomTitleType = 1);
 createPlot(id = 3,
  position = {55, 50, 750, 237},
- y = {"fan1.dp", "fan2.dp", "fan3.dp", "fan4.dp"},
+ y = {"fan1.dp", "fan2.dp", "fan3.dp"},
  range = {0, 1, 600.0, 0},
  autoscale = true,
  autoerase = true,
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mos
index 8ba3b17e2c..55e54eb627 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/ControlledFlowMachineDynamic.mos
@@ -1,7 +1,7 @@
 simulateModel("AixLib.Fluid.Movers.Validation.ControlledFlowMachineDynamic", method="CVode", tolerance=1e-6, stopTime=600, resultFile="ControlledFlowMachineDynamic");
 createPlot(id = 3,
  position = {55, 50, 750, 480},
- y = {"fan1.m_flow", "fan2.m_flow", "fan3.m_flow", "fan4.m_flow"},
+ y = {"fan1.m_flow", "fan2.m_flow", "fan3.m_flow"},
  range = {0, 600, 2.5, 0.5},
  autoscale = true,
  autoerase = true,
@@ -12,7 +12,7 @@ createPlot(id = 3,
  bottomTitleType = 1);
 createPlot(id = 3,
  position = {55, 50, 750, 237},
- y = {"fan1.dp", "fan2.dp", "fan3.dp", "fan4.dp"},
+ y = {"fan1.dp", "fan2.dp", "fan3.dp"},
  range = {0, 600, 700.0, 0},
  autoscale = true,
  autoerase = true,
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PowerExact.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PowerExact.mos
deleted file mode 100644
index c644ff936a..0000000000
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PowerExact.mos
+++ /dev/null
@@ -1,3 +0,0 @@
-simulateModel("AixLib.Fluid.Movers.Validation.PowerExact", tolerance=1e-6, stopTime=200, method="CVode", resultFile="PowerExact");
-createPlot(id=1, position={137, 58, 814, 653}, y={"pump_Nrpm.P", "pump_dp.P", "pump_m_flow.P"}, range={0.0, 200.0, 60.0, 200.0}, grid=true, filename="PowerExact.mat", colors={{0,0,255}, {255,0,0}, {0,128,0}}, patterns={LinePattern.Solid, LinePattern.Dash, LinePattern.DashDot});
-createPlot(id=1, position={137, 58, 814, 323}, y={"pump_Nrpm.per.speed_rpm_nominal", "pump_Nrpm.Nrpm"}, range={0.0, 200.0, 2200.0, 3600.0}, grid=true, subPlot=2, colors={{0,0,255}, {255,0,0}}, displayUnits={"rev/min", "rev/min"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PowerSimplified.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PowerSimplified.mos
deleted file mode 100644
index 4ccec78c6b..0000000000
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PowerSimplified.mos
+++ /dev/null
@@ -1,3 +0,0 @@
-simulateModel("AixLib.Fluid.Movers.Validation.PowerSimplified", tolerance=1e-6, stopTime=200, method="CVode", resultFile="PowerSimplified");
-createPlot(id=1, position={137, 58, 814, 653}, y={"pump_Nrpm.P", "pump_dp.P", "pump_m_flow.P"}, range={0.0, 200.0, 60.0, 200.0}, grid=true, filename="PowerSimplified.mat", colors={{0,0,255}, {255,0,0}, {0,128,0}}, patterns={LinePattern.Solid, LinePattern.Dash, LinePattern.DashDot});
-createPlot(id=1, position={137, 58, 814, 323}, y={"pump_Nrpm.per.speed_rpm_nominal", "pump_Nrpm.Nrpm"}, range={0.0, 200.0, 2200.0, 3600.0}, grid=true, subPlot=2, colors={{0,0,255}, {255,0,0}}, displayUnits={"rev/min", "rev/min"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PressureCurve.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PressureCurve.mos
new file mode 100644
index 0000000000..2d581ebe63
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PressureCurve.mos
@@ -0,0 +1,10 @@
+simulateModel("AixLib.Fluid.Movers.Validation.PressureCurve", tolerance=1e-6, stopTime=1, method="CVode", resultFile="PressureCurve");
+createPlot(id=1,
+ position={35, 35, 592, 371},
+ x="mov.VMachine_flow",
+ y={"mov.dpMachine"},
+ range={0.0, 6.0, -500.0, 3500.0},
+ grid=true,
+ colors={{238,46,47}},
+ timeUnit="m3/s",
+ displayUnits={"Pa"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PumpCurveDerivatives.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PumpCurveDerivatives.mos
index 41a8702934..fb4b7bb3f4 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PumpCurveDerivatives.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/PumpCurveDerivatives.mos
@@ -1,7 +1,7 @@
 simulateModel("AixLib.Fluid.Movers.Validation.PumpCurveDerivatives", numberOfIntervals=500, method="CVode", tolerance=1e-6, stopTime=1.0, resultFile="PumpCurveDerivatives");
 createPlot(id=1,
 position={0, 0, 1532, 801},
-y={"ddp_dNrpm.y"},
+y={"ddp_dy.y"},
 range={0.0, 1.0, -50.0, 250.0},
 grid=true,
 colors={{28,108,200}});
@@ -14,7 +14,7 @@ subPlot=2,
 colors={{28,108,200}});
 createPlot(id=1,
 position={0, 0, 1532, 263},
-y={"dm_flow_dNrpm.y"},
+y={"dm_flow_dy.y"},
 range={0.0, 1.0, -0.05, 0.25000000000000006},
 grid=true,
 subPlot=3,
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_Nrpm_stratos.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_y_stratos.mos
similarity index 76%
rename from AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_Nrpm_stratos.mos
rename to AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_y_stratos.mos
index 81374e0737..edb48b6a7c 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_Nrpm_stratos.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/Pump_y_stratos.mos
@@ -1,7 +1,7 @@
-simulateModel("AixLib.Fluid.Movers.Validation.Pump_Nrpm_stratos", stopTime=1000, method="CVode", tolerance=1e-08, resultFile="Pump_Nrpm_stratos");
+simulateModel("AixLib.Fluid.Movers.Validation.Pump_y_stratos", stopTime=1000, method="CVode", tolerance=1e-08, resultFile="Pump_y_stratos");
 removePlots();
 createPlot(id=1,
-filename = "Pump_Nrpm_stratos.mat",
+filename = "Pump_y_stratos.mat",
 position={0, 0, 1010, 701},
 y={"pump1.m_flow", "pump2.m_flow", "pump3.m_flow", "pump4.m_flow", "pump5.m_flow"},
 range={0.0, 1000.0, -2.0, 16.0},
@@ -15,7 +15,6 @@ y={"forcedPump1.dp", "forcedPump2.dp", "forcedPump3.dp", "forcedPump4.dp", "forc
 range={0.0, 1000.0, 0.0, 140000.0},
 autoscale=false,
 grid=true,
-subPlot=2,
 leftTitleType=1,
 bottomTitleType=1);
 createPlot(id=3,
@@ -24,6 +23,5 @@ y={"pump1.P", "pump2.P", "pump3.P", "pump4.P", "pump5.P"},
 range={0.0, 1000.0, 0.0, 1600.0},
 autoscale=false,
 grid=true,
-subPlot=2,
 leftTitleType=1,
 bottomTitleType=1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/SpeedControlled_Nrpm.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/SpeedControlled_Nrpm.mos
deleted file mode 100644
index 91da60e92b..0000000000
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Movers/Validation/SpeedControlled_Nrpm.mos
+++ /dev/null
@@ -1,40 +0,0 @@
-simulateModel("AixLib.Fluid.Movers.Validation.SpeedControlled_Nrpm", method="CVode", tolerance=1e-08, stopTime=1.0, resultFile="SpeedControlled_Nrpm");
-removePlots();
-createPlot(id = 4,
- filename = "SpeedControlled_Nrpm.mat",
- position = {441, 13, 281, 255},
- y = {"gain.u"},
- range = {0, 1, 1, -0.2},
- autoscale = true,
- autoerase = true,
- autoreplot = true,
- grid = true,
- color = true,
- leftTitleType = 1,
- bottomTitleType = 1);
-createPlot(id = 5,
- filename = "SpeedControlled_Nrpm.mat",
- position = {13, 10, 300, 280},
- x = "floMacSta.VMachine_flow",
- y = {"floMacSta.dpMachine", "floMacDyn.dpMachine"},
- range = {0, 0.0009, 2050.0, 1550.0},
- autoscale = true,
- autoerase = true,
- autoreplot = true,
- grid = true,
- color = true,
- leftTitleType = 1,
- bottomTitleType = 1);
-createPlot(id = 6,
- filename = "SpeedControlled_Nrpm.mat",
- position = {200, 10, 400, 280},
- x = "time",
- y = {"floMacSta.VMachine_flow", "floMacDyn.VMachine_flow"},
- range = {0, 0.001, 2100.0, 1500.0},
- autoscale = true,
- autoerase = true,
- autoreplot = true,
- grid = true,
- color = true,
- leftTitleType = 1,
- bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Pools/Examples/IndoorSwimmingPool.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Pools/Examples/IndoorSwimmingPool.mos
new file mode 100644
index 0000000000..87b121615d
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Pools/Examples/IndoorSwimmingPool.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.Fluid.Pools.Examples.IndoorSwimmingPool", tolerance=1e-6, stopTime=604800, numberOfIntervals=0, outputInterval=900, method="CVode", resultFile="IndoorSwimmingPool");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"indoorSwimming.TPool","indoorSwimming.QPool","indoorSwimming.PPool","indoorSwimming.QEva"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Pools/Examples/IndoorSwimmingPoolExternalHeatingSystem.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Pools/Examples/IndoorSwimmingPoolExternalHeatingSystem.mos
new file mode 100644
index 0000000000..00a125c746
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Pools/Examples/IndoorSwimmingPoolExternalHeatingSystem.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.Fluid.Pools.Examples.IndoorSwimmingPoolExternalHeatingSystem", tolerance=1e-6, stopTime=604800, numberOfIntervals=0, outputInterval=900, method="CVode", resultFile="IndoorSwimmingPoolExternalHeatingSystem");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"indoorSwimming.TPool","prescribedHeatFlow.Q_flow","indoorSwimming.PPool","indoorSwimming.QEva"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/HeatMeter.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/HeatMeter.mos
new file mode 100644
index 0000000000..76fd960eb3
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Sensors/Examples/HeatMeter.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Fluid.Sensors.Examples.HeatMeter", stopTime=60, tolerance=1e-06, resultFile="HeatMeter");
+createPlot(id=1, position={551, 169, 592, 371}, y={"senHeaFlo.Q_flow", "heaFloRat.Q_flow"}, range={0.0, 60.0, -50000.0, 450000.0}, grid=true, colors={{28,108,200}, {238,46,47}}, timeUnit="s", displayUnits={"W", "W"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAEHeatLoss.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAEHeatLoss.mos
new file mode 100644
index 0000000000..1c8895cd47
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAEHeatLoss.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.BaseClasses.Examples.ASHRAEHeatLoss", tolerance=1e-6, stopTime=100, method="dassl", resultFile="ASHRAEHeatLoss");
+createPlot(id = 11,
+ position = {0, 0, 1000, 500},
+ y = {"heaLos.QLos_flow[1]", "heaLos.QLos_flow[2]", "heaLos.QLos_flow[3]"},
+ range = {0.0, 100.0, -80.0, 10.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ASHRAEHeatLoss.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 11,
+ position = {0, 0, 1000, 500},
+ y = {"TEnv.y", "T1.y", "T2.y", "T3.y"},
+ range = {0.0, 100.0, 275.0, 310.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAESolarGain.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAESolarGain.mos
new file mode 100644
index 0000000000..e208ca85bf
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/ASHRAESolarGain.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.BaseClasses.Examples.ASHRAESolarGain", tolerance=1e-6, stopTime=86400, method="dassl", resultFile="ASHRAESolarGain");
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solGai.TFlu[1]", "solGai.TFlu[2]", "solGai.TFlu[3]"},
+ range = {0.0, 88000.0, 310.0, 440.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ASHRAESolarGain.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solGai.QSol_flow[1]", "solGai.QSol_flow[2]", "solGai.QSol_flow[3]"},
+ range = {0.0, 88000.0, -20.0, 240.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/EN12975HeatLoss.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/EN12975HeatLoss.mos
new file mode 100644
index 0000000000..3793a364c3
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/EN12975HeatLoss.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.BaseClasses.Examples.EN12975HeatLoss", tolerance=1e-6, stopTime=100, method="dassl", resultFile="EN12975HeatLoss");
+createPlot(id = 11,
+ position = {0, 0, 1000, 500},
+ y = {"heaLos.QLos_flow[1]", "heaLos.QLos_flow[2]", "heaLos.QLos_flow[3]"},
+ range = {0.0, 100.0, -160.0, 20.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "EN12975HeatLoss.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 11,
+ position = {0, 0, 1000, 500},
+ y = {"TEnv.y", "T1.y", "T2.y", "T3.y"},
+ range = {0.0, 100.0, 275.0, 310.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/EN12975SolarGain.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/EN12975SolarGain.mos
new file mode 100644
index 0000000000..2895b77329
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/BaseClasses/Examples/EN12975SolarGain.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.BaseClasses.Examples.EN12975SolarGain", tolerance=1e-6, stopTime=86400, method="dassl", resultFile="EN12975SolarGain");
+createPlot(id = 11,
+ position = {0, 0, 1000, 500},
+ y = {"solGai.TFlu[1]", "solGai.TFlu[2]", "solGai.TFlu[3]"},
+ range = {0.0, 88000.0, 310.0, 440.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "EN12975SolarGain.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 11,
+ position = {0, 0, 1000, 500},
+ y = {"solGai.QSol_flow[1]", "solGai.QSol_flow[2]", "solGai.QSol_flow[3]"},
+ range = {0.0, 88000.0, -50.0, 500.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Controls/BaseClasses/Examples/GCritCalc.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Controls/BaseClasses/Examples/GCritCalc.mos
new file mode 100644
index 0000000000..979207f3c0
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Controls/BaseClasses/Examples/GCritCalc.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.Controls.BaseClasses.Examples.GCritCalc", tolerance=1e-6, stopTime=100, method="dassl", resultFile="GCritCalc");
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"criSol.G_TC"},
+ range = {0.0, 100.0, -50.0, 300.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "GCritCalc.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"criSol.TEnv", "criSol.TIn"},
+ range = {0.0, 88000.0, -100.0, 700.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Controls/Examples/SolarPumpController.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Controls/Examples/SolarPumpController.mos
new file mode 100644
index 0000000000..bb1b73839a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Controls/Examples/SolarPumpController.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.Controls.Examples.SolarPumpController", tolerance=1e-6, stopTime = 86400, method = "dassl", resultFile = "SolarPumpController");
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"pumCon.on"},
+ range = {0.0, 88000.0, -0.1, 1.2000000000000002},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "SolarPumpController.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"pumCon.criSol.G_TC", "pumCon.weaBus.HDirNor"},
+ range = {0.0, 88000.0, -100.0, 700.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlate.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlate.mos
new file mode 100644
index 0000000000..632b6c2eb5
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlate.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.Examples.FlatPlate", tolerance=1e-6, stopTime = 86400, method = "dassl", resultFile = "FlatPlate");
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solCol.vol[3].T", "solCol.vol[6].T", "solCol.vol[9].T"},
+ range = {0.0, 88000.0, 8.0, 28.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "FlatPlate.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solCol.m_flow"},
+ range = {0.0, 88000.0, 0.092, 0.11599999999999999},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateShaCoeTrue.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateShaCoeTrue.mos
new file mode 100644
index 0000000000..f9909856b1
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateShaCoeTrue.mos
@@ -0,0 +1,31 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.Examples.FlatPlateShaCoeTrue", tolerance=1e-6, stopTime = 86400, method = "dassl", resultFile = "FlatPlateShaCoeTrue");
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solCol.vol[3].T", "solCol.vol[6].T", "solCol.vol[9].T"},
+ range = {0,86400,0, 20},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ subPlot = 1,
+ filename = "FlatPlateShaCoeTrue.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"shaCoe.y"},
+ range = {0.0, 86400.0, 0, 1},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateTotalArea.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateTotalArea.mos
new file mode 100644
index 0000000000..c6d174e611
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateTotalArea.mos
@@ -0,0 +1,34 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.Examples.FlatPlateTotalArea", tolerance=1e-6, stopTime = 86400, method = "dassl", resultFile = "FlatPlateTotalArea");
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solCol.vol[3].T", "solCol.vol[6].T", "solCol.vol[9].T", "solCol1.vol[9].T","solCol1.vol[18].T", "solCol1.vol[27].T"},
+ range = {0.0, 88000.0, 9.0, 21.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "FlatPlateTotalArea.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}, {255,0,255}, {0,0,0}, {0,0,255}},
+ markers = {MarkerStyle.None, MarkerStyle.None, MarkerStyle.None, MarkerStyle.None,
+MarkerStyle.None, MarkerStyle.Cross});
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solCol.m_flow", "solCol.m_flow_nominal", "solCol1.m_flow", "solCol1.m_flow_nominal"},
+ range = {0.0, 88000.0, 0.31, 0.4},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0},{255,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateWithTank.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateWithTank.mos
new file mode 100644
index 0000000000..0a6b3104cc
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/FlatPlateWithTank.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.Examples.FlatPlateWithTank", tolerance=1e-6, stopTime = 86400, method = "dassl", resultFile = "FlatPlateWithTank");
+createPlot(id = 1,
+ position = {0, 0, 1000, 600},
+ y = {"solCol.vol[9].T", "tan.vol[1].T", "TIn.T"},
+ range = {0.0, 90000.0, 0.0, 40.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "FlatPlateWithTank.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 1,
+ position = {0, 0, 1000, 600},
+ y = {"pumCon.on"},
+ range = {0.0, 88000.0, -0.1, 1.2000000000000002},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/Tubular.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/Tubular.mos
new file mode 100644
index 0000000000..d831756162
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Examples/Tubular.mos
@@ -0,0 +1,32 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.Examples.Tubular", tolerance=1e-6, stopTime = 86400, method = "dassl", resultFile = "Tubular");
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solCol.vol[3].T", "solCol.vol[6].T", "solCol.vol[9].T"},
+ range = {0.0, 88000.0, 8.0, 28.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "Tubular.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}, {0,128,0}});
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solCol.m_flow"},
+ range = {0.0, 88000.0, 0.092, 0.11599999999999999},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ subPlot = 2,
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975NPanels.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975NPanels.mos
new file mode 100644
index 0000000000..86e7fe94e3
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975NPanels.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Fluid.SolarCollectors.Validation.EN12975NPanels", tolerance=1e-6, stopTime=86400, method="dassl", resultFile="EN12975NPanels");
+createPlot(id=1, position={210, 54, 1727, 864}, y={"solCol.vol[30].T", "solCol1.vol[30].T"}, range={0.0, 90000.0, 0.0, 100.0}, grid=true, colors={{0,0,255}, {255,0,0}});
+createPlot(id=1, position={210, 54, 1727, 213}, y={"solCol.solGai.QSol_flow[30]", "solCol1.solGai.QSol_flow[30]"}, range={0.0, 90000.0, -1000.0, 1000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}});
+createPlot(id=1, position={210, 54, 1727, 212}, y={"solCol.heaLos.QLos_flow[30]", "solCol1.heaLos.QLos_flow[30]"}, range={0.0, 90000.0, -200.0, 200.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
+createPlot(id=1, position={210, 54, 1727, 212}, y={"difHeaGai.y", "difHeaLos.y"}, range={0.0, 90000.0, -2.0000000000000003E-13, 2.0000000000000003E-13}, grid=true, subPlot=4, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975_Array.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975_Array.mos
new file mode 100644
index 0000000000..d84db8300e
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975_Array.mos
@@ -0,0 +1,6 @@
+simulateModel("AixLib.Fluid.SolarCollectors.Validation.EN12975_Array", stopTime=86400, method="Cvode", tolerance=1e-06, resultFile="EN12975_Array");
+createPlot(id=1, position = {39, -2, 802, 524}, y={"solCol.sta_b.T","solCol1.sta_b.T","solCol2.sta_b.T"}, range={0.0, 86400.0, 15.0, 45.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=1, position = {39, -2, 802, 524}, y={"dT.y"}, range={0.0, 86400.0, -0.025, 0.005}, grid=true, subPlot=2, colors={{28,108,200}});
+createPlot(id=1, position = {39, -2, 802, 524}, y={"solCol.m_flow","solCol1.m_flow","solCol2.m_flow"}, range={0.0, 86400.0, 0.0, 0.15}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+createPlot(id=1, position = {39, -2, 802, 524}, y={"solCol.dp","solCol1.dp","solCol2.dp"}, range={0.0, 86400.0, 0.0, 50.0}, grid=true, subPlot=4, colors={{28,108,200}, {238,46,47}, {0,140,72}});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975_Series.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975_Series.mos
new file mode 100644
index 0000000000..b693440e4f
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/EN12975_Series.mos
@@ -0,0 +1,3 @@
+simulateModel("AixLib.Fluid.SolarCollectors.Validation.EN12975_Series", stopTime=86400, method="Cvode", tolerance=1e-06, resultFile="EN12975_Series");
+createPlot(id=1, position={15, 10, 1358, 844}, y={"solCol.sta_b.T", "solCol2.sta_b.T"}, range={0.0, 1.0, 15.0, 40.0}, grid=true, colors={{28,108,200}, {238,46,47}});
+createPlot(id=1, position={15, 10, 1358, 419}, y={"dT.y"}, range={0.0, 1.0, -0.025, 0.005}, grid=true, subPlot=2, colors={{28,108,200}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/ExtremeAmbientConditions.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/ExtremeAmbientConditions.mos
new file mode 100644
index 0000000000..7f1737d5d9
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/ExtremeAmbientConditions.mos
@@ -0,0 +1,11 @@
+simulateModel("AixLib.Fluid.SolarCollectors.Validation.ExtremeAmbientConditions", stopTime=86400, numberOfIntervals=50000, method="dassl", tolerance=1e-06, resultFile="ExtremeAmbientConditions");
+createPlot(id=1, position={81, 14, 592, 445},
+y={"solAsh.vol[1].T", "solAsh.vol[2].T", "solAsh.vol[3].T", "solEn.vol[1].T", "solEn.vol[2].T", "solEn.vol[3].T", "weaBus.TDryBul"},
+range={0.0, 90000.0, -100.0, 150.0}, grid=true, filename="ExtremeAmbientConditions.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}, {0,0,0}, {162,29,33},
+{244,125,35}});
+createPlot(id=1, position={81, 14, 592, 219},
+y={"solAsh.QLos[1].Q_flow", "solAsh.QLos[2].Q_flow", "solAsh.QLos[3].Q_flow", "solEn.QLos[1].Q_flow", "solEn.QLos[2].Q_flow", "solEn.QLos[3].Q_flow"},
+range={0.0, 90000.0, -600.0, 200.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}, {0,0,0}, {162,29,33}});
+createPlot(id=2, position={82, 498, 592, 228},
+y={"weaBus.HDifHor"},
+range={0.0, 90000.0, -200.0, 1200.0}, grid=true, filename="ExtremeAmbientConditions.mat", colors={{28,108,200}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/FlatPlate.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/FlatPlate.mos
new file mode 100644
index 0000000000..1facd1f4b9
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/FlatPlate.mos
@@ -0,0 +1,17 @@
+removePlots();
+simulateModel("AixLib.Fluid.SolarCollectors.Validation.FlatPlate", tolerance=1e-6, stopTime=86400, method="dassl", resultFile="ValidationFlatPlate");
+createPlot(id = 1,
+ position = {0, 0, 1000, 500},
+ y = {"solCol.vol[30].T", "datRea.y[2]"},
+ range = {0.0, 88000.0, 3.0, 29.0},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ description = false,
+ grid = true,
+ color = true,
+ online = false,
+ filename = "ValidationFlatPlate.mat",
+ leftTitleType = 1,
+ bottomTitleType = 1,
+ colors = {{0,0,255}, {255,0,0}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/FlatPlateNPanels.mos b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/FlatPlateNPanels.mos
new file mode 100644
index 0000000000..70024240d8
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/SolarCollectors/Validation/FlatPlateNPanels.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Fluid.SolarCollectors.Validation.FlatPlateNPanels", tolerance=1e-6, stopTime=86400, method="dassl", resultFile="ValidationFlatPlateNPanels");
+createPlot(id=1, position={210, 54, 1727, 864}, y={"solCol.vol[30].T", "solCol1.vol[30].T"}, range={0.0, 90000.0, 0.0, 100.0}, grid=true, colors={{0,0,255}, {255,0,0}});
+createPlot(id=1, position={210, 54, 1727, 213}, y={"solCol.solGai.QSol_flow[30]", "solCol1.solGai.QSol_flow[30]"}, range={0.0, 90000.0, -1000.0, 1000.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}});
+createPlot(id=1, position={210, 54, 1727, 212}, y={"solCol.heaLos.QLos_flow[30]", "solCol1.heaLos.QLos_flow[30]"}, range={0.0, 90000.0, -200.0, 200.0}, grid=true, subPlot=3, colors={{28,108,200}, {238,46,47}});
+createPlot(id=1, position={210, 54, 1727, 212}, y={"difHeaGai.y", "difHeaLos.y"}, range={0.0, 90000.0, -2.0000000000000003E-13, 2.0000000000000003E-13}, grid=true, subPlot=4, colors={{28,108,200}, {238,46,47}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData.mos
index c22293e551..3359ddd445 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.Fluid.Sources.Examples.Outside_CpData", startTime=1.728e+07, stopTime=1.78848e+07, method="CVode", tolerance=1e-6, resultFile="Outside_CpData");
+simulateModel("AixLib.Fluid.Sources.Examples.Outside_CpData", startTime=1.728e+07, stopTime=1.78848e+07, method="CVode", tolerance=1e-6, resultFile="Outside_CpData");
 createPlot(id = 3,
  position = {55, 24, 679, 513},
  y = {"weaDat.weaBus.winDir"},
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData_Angles.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData_Angles.mos
index f3a90582c0..9e7f8ec736 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData_Angles.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Sources/Examples/Outside_CpData_Angles.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.Fluid.Sources.Examples.Outside_CpData_Angles", startTime=0, stopTime=20, method="CVode", tolerance=1e-6, resultFile="Outside_CpData_Angles");
+simulateModel("AixLib.Fluid.Sources.Examples.Outside_CpData_Angles", startTime=0, stopTime=20, method="CVode", tolerance=1e-6, resultFile="Outside_CpData_Angles");
 createPlot(id = 3,
  position = {55, 24, 679, 513},
  y = {"weaDat.weaBus.winDir"},
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/BufferStorage.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/BufferStorage.mos
deleted file mode 100644
index e9ff7959d6..0000000000
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/BufferStorage.mos
+++ /dev/null
@@ -1,4 +0,0 @@
-simulateModel("AixLib.Fluid.Storage.Examples.BufferStorage", tolerance=1e-6, stopTime=86400, method="dassl", resultFile="BufferStorage");
-createPlot(id=1, position={405, 134, 811, 420}, y={"bufferStorage.heatingCoil1.Therm1[4].Q_flow"}, range={0.0, 90000.0, -200.0, 1800.0}, grid=true, filename="BufferStorage.mat", colors={{28,108,200}});
-createPlot(id=2, position={104, 0, 742, 420}, y={"bufferStorage.layer[4].T"}, range={0.0, 90000.0, 25.0, 65.0}, grid=true, filename="BufferStorage.mat", colors={{28,108,200}}, displayUnits={"degC"});
-createPlot(id=3, position={235, 62, 807, 420}, y={"bufferStorage.portHC1In.p", "bufferStorage.portHC1Out.p"}, range={0.0, 90000.0, 1.0, 1.16}, grid=true, filename="BufferStorage.mat", colors={{28,108,200}, {238,46,47}}, displayUnits={"bar", "bar"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageBoiler.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageBoiler.mos
new file mode 100644
index 0000000000..4646f88499
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageBoiler.mos
@@ -0,0 +1,6 @@
+simulateModel("AixLib.Fluid.Storage.Examples.StorageBoiler", tolerance=1e-6, stopTime=86400, method="dassl", resultFile="StorageBoiler");
+createPlot(id=1, position={104, 0, 742, 420}, y={"bufferStorage.layer[10].T","bufferStorage.layer[5].T","bufferStorage.layer[1].T"}, 
+range={0.0, 90000.0, 25.0, 65.0}, grid=true, filename="StorageBoiler.mat", subPlot=1, colors={{28,108,200},{238,46,47},{110,110,110}},
+displayUnits={"degC","degC","degC"});
+createPlot(id=1, position={104, 0, 742, 420}, y={"hea.Q_flow"}, 
+range={0.0, 90000.0, 25.0, 65.0}, grid=true, filename="StorageBoiler.mat", subPlot=2, colors={{28,108,200}}, displayUnits={"W"});
\ No newline at end of file
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageDetailedExample.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageDetailedExample.mos
new file mode 100644
index 0000000000..48026162a0
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageDetailedExample.mos
@@ -0,0 +1,7 @@
+simulateModel("AixLib.Fluid.Storage.Examples.StorageDetailedExample", tolerance=1e-6, stopTime=86400, method="dassl", resultFile="StorageDetailed");
+createPlot(id=1, position={405, 134, 811, 420}, y={"bufferStorage.heatingCoil1.Therm1[4].Q_flow"},
+range={0.0, 90000.0, -200.0, 1800.0}, grid=true, filename="StorageDetailed.mat", subPlot=1, colors={{28,108,200}});
+createPlot(id=1, position={104, 0, 742, 420}, y={"bufferStorage.layer[4].T"},
+range={0.0, 90000.0, 25.0, 65.0}, grid=true, filename="StorageDetailed.mat", subPlot=2, colors={{28,108,200}}, displayUnits={"degC"});
+createPlot(id=1, position={235, 62, 807, 420}, y={"bufferStorage.portHC1In.p", "bufferStorage.portHC1Out.p"},
+range={0.0, 90000.0, 1.0, 1.16}, grid=true, filename="StorageDetailed.mat", subPlot=3, colors={{28,108,200}, {238,46,47}}, displayUnits={"bar", "bar"});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageSimpleExample.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageSimpleExample.mos
new file mode 100644
index 0000000000..95c521556b
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageSimpleExample.mos
@@ -0,0 +1,7 @@
+simulateModel("AixLib.Fluid.Storage.Examples.StorageSimpleExample", tolerance=1e-6, stopTime=38200, method="dassl", resultFile="StorageSimple");
+createPlot(id=1, position={104, 0, 742, 420}, y={"storageSimple.layer[1].T","storageSimple.layer[2].T","storageSimple.layer[3].T"}, 
+grid=true, filename="StorageSimple.mat", subPlot=1, colors={{28,108,200},{100,108,150},{50,70,20}});
+createPlot(id=1, position={104, 0, 742, 420}, y={"heatingRod.Pel"}, 
+grid=true, filename="StorageSimple.mat", subPlot=2, colors={{28,108,200}});
+createPlot(id=1, position={104, 0, 742, 420}, y={"simpleConsumer.Q_flow"}, 
+grid=true, filename="StorageSimple.mat", subPlot=3, colors={{28,108,200}});
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageSolarCollector.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageSolarCollector.mos
new file mode 100644
index 0000000000..03f2ed4c41
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Examples/StorageSolarCollector.mos
@@ -0,0 +1,10 @@
+simulateModel("AixLib.Fluid.Storage.Examples.StorageSolarCollector", tolerance=1e-6, stopTime=172800, method="dassl", resultFile="StorageSolarCollector");
+createPlot(id=1, position={104, 0, 742, 420}, y={"bufferStorage.layer[10].T","bufferStorage.layer[5].T","bufferStorage.layer[1].T"},
+range={0.0, 90000.0, 25.0, 65.0}, grid=true, filename="StorageSolarCollector.mat", subPlot=1,
+colors={{110,110,110},{28,108,200},{238,46,47}}, displayUnits={"degC","degC","degC"});
+createPlot(id=1, position={104, 0, 742, 420}, y={"temperatureSensor.T"}, 
+range={0.0, 90000.0, 25.0, 65.0}, grid=true, filename="StorageSolarCollector.mat", subPlot=2,
+colors={{28,108,200}}, displayUnits={"degC"});
+createPlot(id=1, position={104, 0, 742, 420}, y={"solarThermal.Irradiation","solarThermal.heater.Q_flow"}, 
+range={0.0, 90000.0, 25.0, 65.0}, grid=true, filename="StorageSolarCollector.mat", subPlot=3, 
+colors={{28,108,200},{238,46,47}});
\ No newline at end of file
diff --git a/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Validation/StratifiedLoadingUnloading.mos b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Validation/StratifiedLoadingUnloading.mos
index 52456ab853..04c385fa3d 100644
--- a/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Validation/StratifiedLoadingUnloading.mos
+++ b/AixLib/Resources/Scripts/Dymola/Fluid/Storage/Validation/StratifiedLoadingUnloading.mos
@@ -1,9 +1,12 @@
 simulateModel("AixLib.Fluid.Storage.Validation.StratifiedLoadingUnloading", tolerance=1e-6, stopTime=14400, method="CVode", resultFile="StratifiedLoadingUnloading");
-createPlot(id = 1,
- position = {10, 30, 719, 600},
- filename = "StratifiedLoadingUnloading.mat",
- y = {"tanEnh.vol[1].T", "tanEnh.vol[2].T", "tanEnh.vol[3].T", "tanEnh.vol[4].T", "tanEnh.vol[5].T", "tanEnh.vol[6].T", "tanEnh.vol[7].T"},
- range = {0, 15000.0, 55.0, 15.0},
+createPlot(id=1,
+ position={10, 30, 719, 603},
+ y={"tanEnh.vol[1].T", "tanEnh.vol[2].T", "tanEnh.vol[3].T", "tanEnh.vol[4].T", "tanEnh.vol[5].T", "tanEnh.vol[6].T", "tanEnh.vol[7].T"},
+ range={0.0, 15000.0, 10.0, 50.0},
+ subPlot=101,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}, {162,29,33}, {244,125,35}},
+ timeUnit="s",
+ displayUnits={"degC", "degC", "degC", "degC", "degC", "degC", "degC"},
  autoscale = true,
  autoerase = true,
  autoreplot = true,
@@ -11,27 +14,32 @@ createPlot(id = 1,
  color = true,
  leftTitleType = 1,
  bottomTitleType = 1);
-createPlot(id = 1,
- position = {10, 30, 719, 200},
- y = {"dHTan.y", "dHTanEnh.y"},
- range = {0, 14500.0, 60.0, 10.0},
+createPlot(id=1,
+ position={10, 30, 719, 603},
+ y={"dHTan.y", "dHTanEnh.y"},
+ range={0.0, 15000.0, -5000000.0, 10000000.0},
+ subPlot=102,
+ colors={{28,108,200}, {238,46,47}},
+ timeUnit="s",
  autoscale = true,
  autoerase = true,
  autoreplot = true,
  grid = true,
  color = true,
- subPlot = 3,
  leftTitleType = 1,
  bottomTitleType = 1);
-createPlot(id = 1,
-  position = {10, 30, 719, 200},
- y = {"tan.vol[1].T", "tan.vol[2].T", "tan.vol[3].T", "tan.vol[4].T", "tan.vol[5].T", "tan.vol[6].T", "tan.vol[7].T"},
- range = {0, 14500.0, 60.0, 10.0},
+createPlot(id=1,
+ position={10, 30, 719, 603},
+ y={"tan.vol[1].T", "tan.vol[2].T", "tan.vol[3].T", "tan.vol[4].T", "tan.vol[5].T","tan.vol[6].T", "tan.vol[7].T"},
+ range={0.0, 15000.0, 10.0, 50.0},
+ subPlot=103,
+ colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}, {162,29,33}, {244,125,35}},
+ timeUnit="s",
+ displayUnits={"degC", "degC", "degC", "degC", "degC", "degC", "degC"},
  autoscale = true,
  autoerase = true,
  autoreplot = true,
  grid = true,
  color = true,
- subPlot = 2,
  leftTitleType = 1,
  bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamDerivativeCheck.mos b/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamDerivativeCheck.mos
index ca87b8cead..7ecde00897 100644
--- a/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamDerivativeCheck.mos
+++ b/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamDerivativeCheck.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.Media.Examples.SteamDerivativeCheck", startTime=0, stopTime=1, tolerance=1E-10, method="dassl", resultFile="MediaExamplesSteamDerivativeCheck");
+simulateModel("AixLib.Media.Examples.SteamDerivativeCheck", startTime=0, stopTime=1, tolerance=1E-10, method="dassl", resultFile="MediaExamplesSteamDerivativeCheck");
 createPlot(id=1, 
   position={34, 26, 626, 458}, 
   y={"der(hVapSym)", "der(hVapCod)"}, 
diff --git a/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamProperties.mos b/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamProperties.mos
index 6989f0f8a7..d0a3de0ff7 100644
--- a/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamProperties.mos
+++ b/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamProperties.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.Media.Examples.SteamProperties", method="dassl", startTime=0, stopTime=1.0, tolerance=1e-06, resultFile="SteamProperties");
+simulateModel("AixLib.Media.Examples.SteamProperties", method="dassl", startTime=0, stopTime=1.0, tolerance=1e-06, resultFile="SteamProperties");
 createPlot(
   id   = 1,
   x    = "T_degC",
diff --git a/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamSaturationConsistencyCheck.mos b/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamSaturationConsistencyCheck.mos
index 7e136c86f8..b38ead1609 100644
--- a/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamSaturationConsistencyCheck.mos
+++ b/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamSaturationConsistencyCheck.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.Media.Examples.SteamSaturationConsistencyCheck", method="dassl", startTime=0, stopTime=1.0, tolerance=1e-06, resultFile="SteamSaturationConsistencyCheck");
+simulateModel("AixLib.Media.Examples.SteamSaturationConsistencyCheck", method="dassl", startTime=0, stopTime=1.0, tolerance=1e-06, resultFile="SteamSaturationConsistencyCheck");
 createPlot(id=1, position={15, 10, 498, 544}, 
   x="TSat_degC", 
   y={"TSat0", "TSat"}, 
diff --git a/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamTemperatureEnthalpyInversion.mos b/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamTemperatureEnthalpyInversion.mos
index 67443cf84a..04c3694b22 100644
--- a/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamTemperatureEnthalpyInversion.mos
+++ b/AixLib/Resources/Scripts/Dymola/Media/Examples/SteamTemperatureEnthalpyInversion.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.Media.Examples.SteamTemperatureEnthalpyInversion", method="dassl", tolerance=1e-6, stopTime=1.0, resultFile="MediaExamplesSteamTemperatureEnthalpyInversion");
+simulateModel("AixLib.Media.Examples.SteamTemperatureEnthalpyInversion", method="dassl", tolerance=1e-6, stopTime=1.0, resultFile="MediaExamplesSteamTemperatureEnthalpyInversion");
 createPlot(id = 1,
  position = {31, 30, 400, 280},
  y = {"T"},
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Admix.mos b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Admix.mos
index c7afbcd4fa..f080757dc0 100644
--- a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Admix.mos
+++ b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Admix.mos
@@ -1,7 +1,4 @@
-// Script generated by Dymola Thu May 28 19:09:18 2020
-// Plot commands
-removePlots(false);
-createPlot(id=1, position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea",
- "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
+simulateModel("AixLib.Systems.HydraulicModules.Example.Admix", tolerance=1e-6, stopTime=800, resultFile="Admix");
+createPlot(id=1, filename="Admix.mat", position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea","hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
 createPlot(id=1, position={0, 0, 1577, 303}, y={"hydraulicBus.VFlowInMea", "hydraulicBus.VFlowOutMea"}, range={0.0, 800.0, -5.0, 35.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}}, displayUnits={"l/min", "l/min"});
 
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection.mos b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection.mos
index c7afbcd4fa..4f4a43e3e2 100644
--- a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection.mos
+++ b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection.mos
@@ -1,7 +1,3 @@
-// Script generated by Dymola Thu May 28 19:09:18 2020
-// Plot commands
-removePlots(false);
-createPlot(id=1, position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea",
- "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
+simulateModel("AixLib.Systems.HydraulicModules.Example.Injection", tolerance=1e-6, stopTime=800, resultFile="Injection");
+createPlot(id=1, filename="Injection.mat", position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea", "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
 createPlot(id=1, position={0, 0, 1577, 303}, y={"hydraulicBus.VFlowInMea", "hydraulicBus.VFlowOutMea"}, range={0.0, 800.0, -5.0, 35.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}}, displayUnits={"l/min", "l/min"});
-
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection2WayValve.mos b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection2WayValve.mos
index c7afbcd4fa..67907d2d3e 100644
--- a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection2WayValve.mos
+++ b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection2WayValve.mos
@@ -1,7 +1,4 @@
-// Script generated by Dymola Thu May 28 19:09:18 2020
-// Plot commands
-removePlots(false);
-createPlot(id=1, position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea",
- "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
-createPlot(id=1, position={0, 0, 1577, 303}, y={"hydraulicBus.VFlowInMea", "hydraulicBus.VFlowOutMea"}, range={0.0, 800.0, -5.0, 35.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}}, displayUnits={"l/min", "l/min"});
+simulateModel("AixLib.Systems.HydraulicModules.Example.Injection2WayValve", tolerance=1e-6, stopTime=800, resultFile="Injection2WayValve");
 
+createPlot(id=1, filename="Injection2WayValve.mat", position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea", "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
+createPlot(id=1, position={0, 0, 1577, 303}, y={"hydraulicBus.VFlowInMea", "hydraulicBus.VFlowOutMea"}, range={0.0, 800.0, -5.0, 35.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}}, displayUnits={"l/min", "l/min"});
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Pump.mos b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Pump.mos
index c7afbcd4fa..8d18c723ef 100644
--- a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Pump.mos
+++ b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Pump.mos
@@ -1,7 +1,4 @@
-// Script generated by Dymola Thu May 28 19:09:18 2020
-// Plot commands
-removePlots(false);
-createPlot(id=1, position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea",
- "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
+simulateModel("AixLib.Systems.HydraulicModules.Example.Pump", tolerance=1e-6, outputInterval=5, stopTime=800, resultFile="Pump");
+createPlot(id=1, filename="Pump.mat", position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea", "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
 createPlot(id=1, position={0, 0, 1577, 303}, y={"hydraulicBus.VFlowInMea", "hydraulicBus.VFlowOutMea"}, range={0.0, 800.0, -5.0, 35.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}}, displayUnits={"l/min", "l/min"});
 
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Throttle.mos b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Throttle.mos
index c7afbcd4fa..b822515386 100644
--- a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Throttle.mos
+++ b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Throttle.mos
@@ -1,7 +1,4 @@
-// Script generated by Dymola Thu May 28 19:09:18 2020
-// Plot commands
-removePlots(false);
-createPlot(id=1, position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea",
- "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
+simulateModel("AixLib.Systems.HydraulicModules.Example.Throttle", tolerance=1e-6, stopTime=1000, resultFile="Throttle");
+createPlot(id=1, filename="Throttle.mat", position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea", "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
 createPlot(id=1, position={0, 0, 1577, 303}, y={"hydraulicBus.VFlowInMea", "hydraulicBus.VFlowOutMea"}, range={0.0, 800.0, -5.0, 35.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}}, displayUnits={"l/min", "l/min"});
 
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/ThrottlePump.mos b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/ThrottlePump.mos
index c7afbcd4fa..c932fae6a3 100644
--- a/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/ThrottlePump.mos
+++ b/AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/ThrottlePump.mos
@@ -1,7 +1,4 @@
-// Script generated by Dymola Thu May 28 19:09:18 2020
-// Plot commands
-removePlots(false);
-createPlot(id=1, position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea",
- "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
+simulateModel("AixLib.Systems.HydraulicModules.Example.ThrottlePump", tolerance=1e-6, stopTime=600, resultFile="ThrottlePump");
+createPlot(id=1, filename="ThrottlePump.mat", position={0, 0, 1577, 612}, y={"hydraulicBus.TFwrdInMea", "hydraulicBus.TFwrdOutMea", "hydraulicBus.TRtrnInMea", "hydraulicBus.TRtrnOutMea"}, range={0.0, 800.0, -20.0, 60.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, displayUnits={"degC", "degC", "degC", "degC"});
 createPlot(id=1, position={0, 0, 1577, 303}, y={"hydraulicBus.VFlowInMea", "hydraulicBus.VFlowOutMea"}, range={0.0, 800.0, -5.0, 35.0}, grid=true, subPlot=2, colors={{28,108,200}, {238,46,47}}, displayUnits={"l/min", "l/min"});
 
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/DemandControlledAHU.mos b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/DemandControlledAHU.mos
index 2e00e05f93..3f0b7e2677 100644
--- a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/DemandControlledAHU.mos
+++ b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/DemandControlledAHU.mos
@@ -1,7 +1,5 @@
-// Script generated by Dymola Mon Oct 17 16:29:35 2022
-// Plot commands
-removePlots(false);
-createPlot(id=1, position={0, 0, 1167, 585}, y={"genericAHU.genericAHUBus.TSupMea", "genericAHU.genericAHUBus.TOdaMea"}, range={69.0, 71.0, 0.0, 40.0}, grid=true, subPlot=101, colors={{28,108,200}, {238,46,47}}, timeUnit="d", displayUnits={"degC", "degC"});
+simulateModel("AixLib.Systems.ModularAHU.Examples.DemandControlledAHU", tolerance=1e-5, startTime=5961600, stopTime=6566400, outputInterval=120, resultFile="DemandControlledAHU");
+createPlot(id=1, filename="DemandControlledAHU.mat", position={0, 0, 1167, 585}, y={"genericAHU.genericAHUBus.TSupMea", "genericAHU.genericAHUBus.TOdaMea"}, range={69.0, 71.0, 0.0, 40.0}, grid=true, subPlot=101, colors={{28,108,200}, {238,46,47}}, timeUnit="d", displayUnits={"degC", "degC"});
 createPlot(id=1, position={0, 0, 1167, 585}, y={"genericAHU.genericAHUBus.heaterBus.hydraulicBus.valveSet"}, range={69.0, 71.0, -0.5, 1.0}, grid=true, subPlot=102, colors={{28,108,200}}, timeUnit="d");
 createPlot(id=1, position={0, 0, 1167, 585}, y={"genericAHU.genericAHUBus.heaterBus.VFlowAirMea"}, range={69.0, 71.0, -0.5, 1.0}, autoscale=false, grid=true, subPlot=103, colors={{28,108,200}}, timeUnit="d", displayUnits={"m3/s"});
 createPlot(id=1, position={0, 0, 1167, 585}, y={"thermalZone.CO2Con"}, range={69.0, 71.0, 0.0, 1000.0}, grid=true, subPlot=104, colors={{28,108,200}}, timeUnit="d");
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/Heater.mos b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/Heater.mos
index bd928df2bb..2edfc554f0 100644
--- a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/Heater.mos
+++ b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/Heater.mos
@@ -1,6 +1,3 @@
-// Script generated by Dymola Mon Apr 26 15:37:32 2021
-// Plot commands
-removePlots(false);
-createPlot(id=1, position={0, 0, 2559, 1770}, y={"ctrBasic.registerBus.TAirInMea", "ctrBasic.registerBus.TAirOutMea"}, heading="Air temperatures", range={0.0, 3600.0, 9.5, 20.5}, grid=true, colors={{28,108,200}, {238,46,47}}, displayUnits={"degC", "degC"});
+simulateModel("AixLib.Systems.ModularAHU.Examples.Heater", tolerance=1e-6, stopTime=3600, resultFile="Heater");
+createPlot(id=1, filename="Heater.mat", position={0, 0, 2559, 1770}, y={"ctrBasic.registerBus.TAirInMea", "ctrBasic.registerBus.TAirOutMea"}, heading="Air temperatures", range={0.0, 3600.0, 9.5, 20.5}, grid=true, colors={{28,108,200}, {238,46,47}}, displayUnits={"degC", "degC"});
 createPlot(id=1, position={0, 0, 2559, 882}, y={"ctrBasic.registerBus.hydraulicBus.valveSet"}, heading="Valve opening", range={0.0, 3600.0, -0.05, 0.95}, grid=true, subPlot=2, leftTitleType=2, leftTitle="Opening", colors={{28,108,200}});
-
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Cooler.mos b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Cooler.mos
new file mode 100644
index 0000000000..ef0b01ff03
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Cooler.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Systems.ModularAHU.Validation.AHU2_Cooler", tolerance=1e-6, outputInterval=1, stopTime=2700, resultFile="AHU2_Cooler");
+createPlot(id=1, filename="AHU2_Cooler.mat", position={0, 0, 1590, 731}, y={"registerModule.registerBus.TAirInMea", "registerModule.registerBus.TAirOutMea", "combiTimeTable.y[6]", "combiTimeTable.y[5]"}, heading="Air temperature [°C]", range={0.0, 2700.0, 10.0, 70.0}, grid=true, legends={"Simulation.TairIn", "Simulation.TairOut", "Data.TairOut", "Data.TairIn"}, colors={{28,108,200}, {238,46,47}, {238,46,47}, {28,108,200}}, patterns={LinePattern.Solid, LinePattern.Solid, LinePattern.Dash, LinePattern.Dash}, displayUnits={"degC", "degC", "", ""});
+createPlot(id=1, position={0, 0, 1590, 241}, y={"combiTimeTable.y[3]", "combiTimeTable.y[4]", "registerModule.registerBus.hydraulicBus.TFwrdOutMea", "registerModule.registerBus.hydraulicBus.TRtrnInMea"}, heading="Water temperature at register entry and exit [°C]", range={0.0, 2700.0, 0.0, 100.0}, grid=true, legends={"Data.TfwrdOut", "Data.TrtrnIn", "Simulation.TfwrdOut", "Simulation.TrtrnIn"}, subPlot=2, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid}, displayUnits={"", "", "degC", "degC"});
+createPlot(id=1, position={0, 0, 1590, 240}, y={"combiTimeTable.y[9]", "combiTimeTable.y[8]", "Simulation_VF_in_m3h.y", "Simulation_VF_out_m3h.y"}, heading="Water volume flow rate in m3/h", range={0.0, 2700.0, -1.0, 5.0}, grid=true, legends={"Data.VFlowIn", "Data.VFlowOut", "Simulation.VFlowIn", "Simulation.VFlowOut"}, subPlot=3, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Heater.mos b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Heater.mos
new file mode 100644
index 0000000000..bc57e77e62
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Heater.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Systems.ModularAHU.Validation.AHU2_Heater", tolerance=1e-6, outputInterval=1, stopTime=4320, resultFile="AHU2_Heater");
+createPlot(id=1, filename="AHU2_Heater.mat", position={0, 0, 1590, 731}, y={"registerModule.registerBus.TAirInMea", "registerModule.registerBus.TAirOutMea", "combiTimeTable.y[6]", "combiTimeTable.y[5]"}, heading="Air temperature [°C]", range={0.0, 4320.0, 10.0, 70.0}, grid=true, legends={"Simulation.TairIn", "Simulation.TairOut", "Data.TairOut", "Data.TairIn"}, colors={{28,108,200}, {238,46,47}, {238,46,47}, {28,108,200}}, patterns={LinePattern.Solid, LinePattern.Solid, LinePattern.Dash, LinePattern.Dash}, displayUnits={"degC", "degC", "", ""});
+createPlot(id=1, position={0, 0, 1590, 241}, y={"combiTimeTable.y[3]", "combiTimeTable.y[4]", "registerModule.registerBus.hydraulicBus.TFwrdOutMea", "registerModule.registerBus.hydraulicBus.TRtrnInMea"}, heading="Water temperature at register entry and exit [°C]", range={0.0, 4320.0, 0.0, 100.0}, grid=true, legends={"Data.TfwrdOut", "Data.TrtrnIn", "Simulation.TfwrdOut", "Simulation.TrtrnIn"}, subPlot=2, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid}, displayUnits={"", "", "degC", "degC"});
+createPlot(id=1, position={0, 0, 1590, 240}, y={"combiTimeTable.y[9]", "combiTimeTable.y[8]", "Simulation_VF_in_m3h.y", "Simulation_VF_out_m3h.y"}, heading="Water volume flow rate in m3/h", range={0.0, 4320.0, -1.0, 5.0}, grid=true, legends={"Data.VFlowIn", "Data.VFlowOut", "Simulation.VFlowIn", "Simulation.VFlowOut"}, subPlot=3, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Preheater.mos b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Preheater.mos
new file mode 100644
index 0000000000..d9abfbd525
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Preheater.mos
@@ -0,0 +1,5 @@
+simulateModel("AixLib.Systems.ModularAHU.Validation.AHU2_Preheater", tolerance=1e-6, outputInterval=1, stopTime=7200, resultFile="AHU2_Preheater");
+createPlot(id=1, filename="AHU2_Preheater.mat", position={0, 0, 1590, 731}, y={"registerModule.registerBus.TAirInMea", "registerModule.registerBus.TAirOutMea", "combiTimeTable.y[6]", "combiTimeTable.y[5]"}, heading="Air temperature [°C]", range={0.0, 7200.0, 10.0, 70.0}, grid=true, legends={"Simulation.TairIn", "Simulation.TairOut", "Data.TairOut", "Data.TairIn"}, colors={{28,108,200}, {238,46,47}, {238,46,47}, {28,108,200}}, patterns={LinePattern.Solid, LinePattern.Solid, LinePattern.Dash, LinePattern.Dash}, displayUnits={"degC", "degC", "", ""});
+createPlot(id=1, position={0, 0, 1590, 241}, y={"combiTimeTable.y[3]", "combiTimeTable.y[4]", "registerModule.registerBus.hydraulicBus.TFwrdOutMea", "registerModule.registerBus.hydraulicBus.TRtrnInMea"}, heading="Water temperature at register entry and exit [°C]", range={0.0, 7200.0, 0.0, 100.0}, grid=true, legends={"Data.TfwrdOut", "Data.TrtrnIn", "Simulation.TfwrdOut", "Simulation.TrtrnIn"}, subPlot=2, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid}, displayUnits={"", "", "degC", "degC"});
+createPlot(id=1, position={0, 0, 1590, 240}, y={"combiTimeTable.y[9]", "combiTimeTable.y[8]", "Simulation_VF_in_m3h.y", "Simulation_VF_out_m3h.y"}, heading="Water volume flow rate in m3/h", range={0.0, 7200.0, -1.0, 5.0}, grid=true, legends={"Data.VFlowIn", "Data.VFlowIn", "Simulation.VFlowIn", "Simulation.VFlowOut"}, subPlot=3, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid});
+
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Cooler.mos b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Cooler.mos
deleted file mode 100644
index 5a8ba2e09b..0000000000
--- a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Cooler.mos
+++ /dev/null
@@ -1,21 +0,0 @@
-// Script generated by Dymola Tue May 15 11:15:38 2018
-// Plot commands
-removePlots(false);
-Advanced.FilenameInLegend = false;
-Advanced.SequenceInLegend = true;
-Advanced.PlotLegendTooltip = true;
-Advanced.ShowPlotTooltip = true;
-Advanced.FullPlotTooltip = true;
-Advanced.DefaultAutoErase = true;
-Advanced.Legend.Horizontal = true;
-Advanced.Legend.Frame = false;
-Advanced.Legend.Transparent = true;
-Advanced.Legend.Location = 1;
-Advanced.FilesToKeep = 2;
-createPlot(id=1, position={0, 0, 1590, 731}, y={"registerModule.registerBus.TAirInMea", "registerModule.registerBus.TAirOutMea", 
-"combiTimeTable.y[6]", "combiTimeTable.y[5]"}, heading="Air temperature [°C]", range={0.0, 4000.0, 10.0, 70.0}, grid=true, legends={"Simulation.TairIn", "Simulation.TairOut", "Data.TairOut", "Data.TairIn"}, colors={{28,108,200}, {238,46,47}, {238,46,47}, {28,108,200}}, patterns={LinePattern.Solid, LinePattern.Solid, LinePattern.Dash, LinePattern.Dash}, displayUnits={"degC", "degC", "", ""});
-createPlot(id=1, position={0, 0, 1590, 241}, y={"combiTimeTable.y[3]", "combiTimeTable.y[4]", "registerModule.registerBus.hydraulicBus.TFwrdOutMea",
- "registerModule.registerBus.hydraulicBus.TRtrnInMea"}, heading="Water temperature at register entry and exit [°C]", range={0.0, 4000.0, 0.0, 100.0}, grid=true, legends={"Data.TfwrdOut", "Data.TrtrnIn", "Simulation.TfwrdOut", "Simulation.TrtrnIn"}, subPlot=2, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid}, displayUnits={"", "", "degC", "degC"});
-createPlot(id=1, position={0, 0, 1590, 240}, y={"combiTimeTable.y[9]", "combiTimeTable.y[8]", "Simulation_VF_in_m3h.y", 
-"Simulation_VF_out_m3h.y"}, heading="Water volume flow rate in m3/h", range={0.0, 4000.0, -1.0, 5.0}, grid=true, legends={"Data.VFlowIn", "Data.VFlowOut", "Simulation.VFlowIn", "Simulation.VFlowOut"}, subPlot=3, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid});
-
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Heater.mos b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Heater.mos
deleted file mode 100644
index 5a8ba2e09b..0000000000
--- a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Heater.mos
+++ /dev/null
@@ -1,21 +0,0 @@
-// Script generated by Dymola Tue May 15 11:15:38 2018
-// Plot commands
-removePlots(false);
-Advanced.FilenameInLegend = false;
-Advanced.SequenceInLegend = true;
-Advanced.PlotLegendTooltip = true;
-Advanced.ShowPlotTooltip = true;
-Advanced.FullPlotTooltip = true;
-Advanced.DefaultAutoErase = true;
-Advanced.Legend.Horizontal = true;
-Advanced.Legend.Frame = false;
-Advanced.Legend.Transparent = true;
-Advanced.Legend.Location = 1;
-Advanced.FilesToKeep = 2;
-createPlot(id=1, position={0, 0, 1590, 731}, y={"registerModule.registerBus.TAirInMea", "registerModule.registerBus.TAirOutMea", 
-"combiTimeTable.y[6]", "combiTimeTable.y[5]"}, heading="Air temperature [°C]", range={0.0, 4000.0, 10.0, 70.0}, grid=true, legends={"Simulation.TairIn", "Simulation.TairOut", "Data.TairOut", "Data.TairIn"}, colors={{28,108,200}, {238,46,47}, {238,46,47}, {28,108,200}}, patterns={LinePattern.Solid, LinePattern.Solid, LinePattern.Dash, LinePattern.Dash}, displayUnits={"degC", "degC", "", ""});
-createPlot(id=1, position={0, 0, 1590, 241}, y={"combiTimeTable.y[3]", "combiTimeTable.y[4]", "registerModule.registerBus.hydraulicBus.TFwrdOutMea",
- "registerModule.registerBus.hydraulicBus.TRtrnInMea"}, heading="Water temperature at register entry and exit [°C]", range={0.0, 4000.0, 0.0, 100.0}, grid=true, legends={"Data.TfwrdOut", "Data.TrtrnIn", "Simulation.TfwrdOut", "Simulation.TrtrnIn"}, subPlot=2, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid}, displayUnits={"", "", "degC", "degC"});
-createPlot(id=1, position={0, 0, 1590, 240}, y={"combiTimeTable.y[9]", "combiTimeTable.y[8]", "Simulation_VF_in_m3h.y", 
-"Simulation_VF_out_m3h.y"}, heading="Water volume flow rate in m3/h", range={0.0, 4000.0, -1.0, 5.0}, grid=true, legends={"Data.VFlowIn", "Data.VFlowOut", "Simulation.VFlowIn", "Simulation.VFlowOut"}, subPlot=3, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid});
-
diff --git a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Preheater.mos b/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Preheater.mos
deleted file mode 100644
index d96740fd3d..0000000000
--- a/AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Preheater.mos
+++ /dev/null
@@ -1,21 +0,0 @@
-// Script generated by Dymola Tue May 15 11:15:38 2018
-// Plot commands
-removePlots(false);
-Advanced.FilenameInLegend = false;
-Advanced.SequenceInLegend = true;
-Advanced.PlotLegendTooltip = true;
-Advanced.ShowPlotTooltip = true;
-Advanced.FullPlotTooltip = true;
-Advanced.DefaultAutoErase = true;
-Advanced.Legend.Horizontal = true;
-Advanced.Legend.Frame = false;
-Advanced.Legend.Transparent = true;
-Advanced.Legend.Location = 1;
-Advanced.FilesToKeep = 2;
-createPlot(id=1, position={0, 0, 1590, 731}, y={"registerModule.registerBus.TAirInMea", "registerModule.registerBus.TAirOutMea", 
-"combiTimeTable.y[6]", "combiTimeTable.y[5]"}, heading="Air temperature [°C]", range={0.0, 4000.0, 10.0, 70.0}, grid=true, legends={"Simulation.TairIn", "Simulation.TairOut", "Data.TairOut", "Data.TairIn"}, colors={{28,108,200}, {238,46,47}, {238,46,47}, {28,108,200}}, patterns={LinePattern.Solid, LinePattern.Solid, LinePattern.Dash, LinePattern.Dash}, displayUnits={"degC", "degC", "", ""});
-createPlot(id=1, position={0, 0, 1590, 241}, y={"combiTimeTable.y[3]", "combiTimeTable.y[4]", "registerModule.registerBus.hydraulicBus.TFwrdOutMea",
- "registerModule.registerBus.hydraulicBus.TRtrnInMea"}, heading="Water temperature at register entry and exit [°C]", range={0.0, 4000.0, 0.0, 100.0}, grid=true, legends={"Data.TfwrdOut", "Data.TrtrnIn", "Simulation.TfwrdOut", "Simulation.TrtrnIn"}, subPlot=2, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid}, displayUnits={"", "", "degC", "degC"});
-createPlot(id=1, position={0, 0, 1590, 240}, y={"combiTimeTable.y[9]", "combiTimeTable.y[8]", "Simulation_VF_in_m3h.y", 
-"Simulation_VF_out_m3h.y"}, heading="Water volume flow rate in m3/h", range={0.0, 4000.0, -1.0, 5.0}, grid=true, legends={"Data.VFlowIn", "Data.VFlowIn", "Simulation.VFlowIn", "Simulation.VFlowOut"}, subPlot=3, colors={{28,108,200}, {238,46,47}, {28,108,200}, {238,46,47}}, patterns={LinePattern.Dash, LinePattern.Dash, LinePattern.Solid, LinePattern.Solid});
-
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/FreeFloating.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/FreeFloating.mos
new file mode 100644
index 0000000000..958da4ae35
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/FreeFloating.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ISO13790.Examples.FreeFloating", tolerance=1e-6, startTime=8640000, stopTime=9504000, method="CVode", resultFile="FreeFloating");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"zon5R1C.TAir"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/FreeFloatingHVAC.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/FreeFloatingHVAC.mos
new file mode 100644
index 0000000000..e4f0c6a0af
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/FreeFloatingHVAC.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ISO13790.Examples.FreeFloatingHVAC", tolerance=1e-6, startTime=8640000, stopTime=9504000, method="CVode", resultFile="FreeFloatingHVAC");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"zonHVAC.TAir"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/HeatingCooling.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/HeatingCooling.mos
new file mode 100644
index 0000000000..aa6191f8c4
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/HeatingCooling.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ISO13790.Examples.HeatingCooling", tolerance=1e-6, startTime=8640000, stopTime=9504000, method="CVode", resultFile="HeatingCooling");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"zon5R1C.TAir"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/HeatingCoolingHVAC.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/HeatingCoolingHVAC.mos
new file mode 100644
index 0000000000..3817ddef23
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/HeatingCoolingHVAC.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ISO13790.Examples.HeatingCoolingHVAC", tolerance=1e-6, startTime=8640000, stopTime=9504000, method="CVode", resultFile="HeatingCoolingHVAC");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"zonHVAC.TAir"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case600.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case600.mos
new file mode 100644
index 0000000000..304c27ec63
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case600.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ISO13790.Validation.BESTEST.Case600", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Dassl", resultFile="Case600");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"EHea.y", "ECoo.y"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case600FF.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case600FF.mos
new file mode 100644
index 0000000000..04de584e04
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case600FF.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ISO13790.Validation.BESTEST.Case600FF", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Dassl", resultFile="Case600FF");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"zon5R1C.TAir"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case900.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case900.mos
new file mode 100644
index 0000000000..8ec7f01de5
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case900.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ISO13790.Validation.BESTEST.Case900", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Dassl", resultFile="Case900");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"EHea.y", "ECoo.y"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case900FF.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case900FF.mos
new file mode 100644
index 0000000000..8459dd026e
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case900FF.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ISO13790.Validation.BESTEST.Case900FF", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Dassl", resultFile="Case900FF");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"zon5R1C.TAir"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ComparisonThermalZoneMoistAndDryAir.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ComparisonThermalZoneMoistAndDryAir.mos
index eaf6d8c900..dbfa68a3d9 100644
--- a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ComparisonThermalZoneMoistAndDryAir.mos
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ComparisonThermalZoneMoistAndDryAir.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ComparisonThermalZoneMoistAndDryAir", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Radau", resultFile="ComparisonThermalZoneMoistAndDryAir");
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ComparisonThermalZoneMoistAndDryAir", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="ComparisonThermalZoneMoistAndDryAir");
 createPlot(id = 1,
  position = {55, 50, 697, 502},
  x = "time",
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/Multizone.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/Multizone.mos
new file mode 100644
index 0000000000..80226099ab
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/Multizone.mos
@@ -0,0 +1,3 @@
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.Multizone", tolerance=1e-6, stopTime=864000, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="Multizone");
+createPlot(id=1, position={0, 0, 1617, 533}, y={"multizone.TAir[1]", "multizone.TAir[2]", "multizone.TAir[3]", "multizone.TAir[4]", "multizone.TAir[5]"}, range={0.0, 10.200000000000001, 19.5, 23.0}, erase=true, autoscale=true, grid=true, filename="Multizone.mat", subPlot=101, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}}, timeUnit="d", displayUnits={"degC", "degC", "degC", "degC", "degC"});
+createPlot(id=1, position={0, 0, 1617, 533}, y={"weaDat.weaBus.TDryBul"}, range={0.0, 10.200000000000001, -10000.0, 80000.0}, erase=true, grid=true, subPlot=102, colors={{28,108,200}}, timeUnit="d");
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneEquipped.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneEquipped.mos
new file mode 100644
index 0000000000..3847654cce
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneEquipped.mos
@@ -0,0 +1,3 @@
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.MultizoneEquipped", tolerance=1e-6, stopTime=864000, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="MultizoneEquipped");
+createPlot(id=1, position={0, 0, 1617, 533}, y={"multizone.TAir[1]", "multizone.TAir[2]", "multizone.TAir[3]", "multizone.TAir[4]", "multizone.TAir[5]"}, range={0.0, 10.200000000000001, 19.5, 23.0}, erase=false, autoscale=false, grid=true, filename="MultizoneEquipped.mat", subPlot=101, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}}, timeUnit="d", displayUnits={"degC", "degC", "degC", "degC", "degC"});
+createPlot(id=1, position={0, 0, 1617, 533}, y={"multizone.PHeater[1]", "multizone.PHeater[2]", "multizone.PHeater[3]", "multizone.PHeater[4]", "multizone.PHeater[5]"}, range={0.0, 10.200000000000001, -10000.0, 80000.0}, erase=false, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}}, timeUnit="d", displayUnits={"W", "W", "W", "W", "W"});
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2.mos
index b8d7074b10..7ba59e1819 100644
--- a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2.mos
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.MultizoneMoistAirCO2", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Radau", resultFile="MultizoneMoistAirCO2");
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.MultizoneMoistAirCO2", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="MultizoneMoistAirCO2");
 createPlot(id = 1,
  position = {55, 50, 697, 502},
  x = "time",
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2Equipped.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2Equipped.mos
new file mode 100644
index 0000000000..e547507fbc
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2Equipped.mos
@@ -0,0 +1,3 @@
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.MultizoneMoistAirCO2Equipped", tolerance=1e-6, stopTime=864000, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="MultizoneEquipped");
+createPlot(id=1, position={0, 0, 1617, 533}, y={"multizone.TAir[1]", "multizone.TAir[2]", "multizone.TAir[3]", "multizone.TAir[4]", "multizone.TAir[5]"}, range={0.0, 10.200000000000001, 19.5, 23.0}, erase=false, autoscale=false, grid=true, filename="MultizoneMoistAirCO2Equipped.mat", subPlot=101, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}}, timeUnit="d", displayUnits={"degC", "degC", "degC", "degC", "degC"});
+createPlot(id=1, position={0, 0, 1617, 533}, y={"multizone.PHeater[1]", "multizone.PHeater[2]", "multizone.PHeater[3]", "multizone.PHeater[4]", "multizone.PHeater[5]"}, range={0.0, 10.200000000000001, -10000.0, 80000.0}, erase=false, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}}, timeUnit="d", displayUnits={"W", "W", "W", "W", "W"});
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2EquippedSwimmingFacility.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2EquippedSwimmingFacility.mos
new file mode 100644
index 0000000000..0c9a56ac0a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2EquippedSwimmingFacility.mos
@@ -0,0 +1,23 @@
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.MultizoneMoistAirCO2EquippedSwimmingFacility", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="MultizoneMoistAirCO2EquippedSwimmingFacility");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"multizone.TAir[1]"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
+createPlot(id = 2,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"multizone.zone[1].X_w"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizonePartlyCooled.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizonePartlyCooled.mos
new file mode 100644
index 0000000000..aa11860e5c
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizonePartlyCooled.mos
@@ -0,0 +1,3 @@
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.MultizonePartlyCooled", tolerance=1e-6, startTime=14688000, stopTime=15552000, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="MultizonePartlyCooled");
+createPlot(id=1, position={0, 0, 1617, 533}, y={"multizone.TAir[1]", "multizone.TAir[2]", "multizone.TAir[3]", "multizone.TAir[4]", "multizone.TAir[5]"}, range={0.0, 10.200000000000001, 19.5, 23.0}, erase=false, autoscale=false, grid=true, filename="MultizonePartlyCooled.mat", subPlot=101, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}}, timeUnit="d", displayUnits={"degC", "degC", "degC", "degC", "degC"});
+createPlot(id=1, position={0, 0, 1617, 533}, y={"multizone.PCooler[1]", "multizone.PCooler[2]", "multizone.PCooler[3]", "multizone.PCooler[4]", "multizone.PCooler[5]"}, range={0.0, 10.200000000000001, -10000.0, 80000.0}, erase=false, grid=true, subPlot=102, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}, {0,0,0}}, timeUnit="d", displayUnits={"W", "W", "W", "W", "W"});
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElementsNonConstantTGround.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElementsNonConstantTGround.mos
new file mode 100644
index 0000000000..e0e6bbd980
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElementsNonConstantTGround.mos
@@ -0,0 +1,12 @@
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.SimpleRoomTwoElementsNonConstantTGround", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="SimpleRoomTwoElementsNonConstantTGround");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"eqAirTemp.TEqAir"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZone.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZone.mos
index 4e42ff7637..e4d9f2d71d 100644
--- a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZone.mos
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZone.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZone", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Radau", resultFile="ThermalZone");
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZone", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="ThermalZone");
 createPlot(id = 1,
  position = {55, 50, 697, 502},
  x = "time",
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneAirExchange.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneAirExchange.mos
index 49c4435541..6a8faea054 100644
--- a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneAirExchange.mos
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneAirExchange.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZoneAirExchange", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Radau", resultFile="ThermalZoneAirExchange");
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZoneAirExchange", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="ThermalZoneAirExchange");
 createPlot(id = 1,
  position = {55, 50, 697, 502},
  x = "time",
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAir.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAir.mos
index 12019c6741..fea96504a8 100644
--- a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAir.mos
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAir.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZoneMoistAir", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Radau", resultFile="ThermalZoneMoistAir");
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZoneMoistAir", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="ThermalZoneMoistAir");
 createPlot(id = 1,
  position = {55, 50, 697, 502},
  x = "time",
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAirSwimmingPool.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAirSwimmingPool.mos
new file mode 100644
index 0000000000..d851e723fb
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAirSwimmingPool.mos
@@ -0,0 +1,27 @@
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZoneMoistAirSwimmingPool", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="ThermalZoneMoistAirSwimmingPool");
+createPlot(id = 1,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"thermalZone.TAir"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
+ createPlot(id = 2,
+ position = {55, 50, 697, 502},
+ x = "time",
+ y = {"thermalZone.X_w"},
+ autoscale = true,
+ autoerase = true,
+ autoreplot = true,
+ grid = true,
+ color = true,
+ leftTitleType = 1,
+ bottomTitleType = 1);
+
+
+
+
diff --git a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistCO2AirExchange.mos b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistCO2AirExchange.mos
index 4591ef1fee..bb389c5086 100644
--- a/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistCO2AirExchange.mos
+++ b/AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistCO2AirExchange.mos
@@ -1,4 +1,4 @@
-simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZoneMoistCO2AirExchange", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="Radau", resultFile="ThermalZoneMoistAirCO2AirExchange");
+simulateModel("AixLib.ThermalZones.ReducedOrder.Examples.ThermalZoneMoistCO2AirExchange", tolerance=1e-6, stopTime=3.1536e+007, numberOfIntervals=0, outputInterval=3600, method="CVode", resultFile="ThermalZoneMoistAirCO2AirExchange");
 createPlot(id = 1,
  position = {55, 50, 697, 502},
  x = "time",
diff --git a/AixLib/Resources/Scripts/Dymola/Utilities/Clustering/Validation/KMeans_1d.mos b/AixLib/Resources/Scripts/Dymola/Utilities/Clustering/Validation/KMeans_1d.mos
new file mode 100644
index 0000000000..e1138a7ff4
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/Clustering/Validation/KMeans_1d.mos
@@ -0,0 +1,6 @@
+simulateModel("AixLib.Utilities.Clustering.Validation.KMeans_1d", tolerance=1e-6, stopTime=1, method="CVode", resultFile="KMeans_1d");
+createPlot(id = 1,
+ position = {50, 50, 700, 500},
+ x = "time",
+ y = {"cmp"},
+ filename="KMeans_1d.mat");
diff --git a/AixLib/Resources/Scripts/Dymola/Utilities/Clustering/Validation/KMeans_2d.mos b/AixLib/Resources/Scripts/Dymola/Utilities/Clustering/Validation/KMeans_2d.mos
new file mode 100644
index 0000000000..79b4b0a26a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/Clustering/Validation/KMeans_2d.mos
@@ -0,0 +1,6 @@
+simulateModel("AixLib.Utilities.Clustering.Validation.KMeans_2d", tolerance=1e-6, stopTime=1, method="CVode", resultFile="KMeans_2d");
+createPlot(id = 1,
+ position = {50, 50, 700, 500},
+ x = "time",
+ y = {"cmp"},
+ filename="KMeans_2d.mat");
diff --git a/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/WeeklySchedule.mos b/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/WeeklySchedule.mos
new file mode 100644
index 0000000000..b5806a329a
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/WeeklySchedule.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Utilities.IO.Files.Examples.WeeklySchedule", startTime=-10000, stopTime=1000000, tolerance=1e-6, method="dassl", resultFile="WeeklySchedule");
+createPlot(id=1, position={0, 0, 915, 524}, y={"weeSchFil.y[1]", "weeSchFil.y[2]", "weeSchFil.y[3]", "weeSchFil.y[4]"}, range={-100000.0, 1000000.0, -10.0, 130.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}});
diff --git a/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/WeeklySchedule7to19.mos b/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/WeeklySchedule7to19.mos
new file mode 100644
index 0000000000..42daa346cc
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/WeeklySchedule7to19.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Utilities.IO.Files.Examples.WeeklySchedule7to19", stopTime=1209600, method="Cvode", tolerance=1e-06, resultFile="WeeklySchedule7to19");
+createPlot(id=2, position={55, 55, 1016, 624}, y={"sch.y[1]"}, range={0.0, 14.0, -0.1, 1.1}, grid=true, colors={{28,108,200}}, timeUnit="d");
diff --git a/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Validation/WeeklyScheduleWindowsLineEndings.mos b/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Validation/WeeklyScheduleWindowsLineEndings.mos
new file mode 100644
index 0000000000..e8548cc8ba
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Validation/WeeklyScheduleWindowsLineEndings.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Utilities.IO.Files.Validation.WeeklyScheduleWindowsLineEndings", startTime=-10000, stopTime=1000000, tolerance=1e-6, method="dassl", resultFile="WeeklyScheduleWindowsLineEndings");
+createPlot(id=1, position={15, 15, 592, 364}, y={"weeSchLin.y[1]", "weeSchLin.y[2]", "weeSchLin.y[3]", "weeSchLin.y[4]"}, range={-100000.0, 1000000.0, -20.0, 140.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}, {217,67,180}}, timeUnit="s");
diff --git a/AixLib/Resources/Scripts/Dymola/Utilities/IO/SignalExchange/Examples/FirstOrder.mos b/AixLib/Resources/Scripts/Dymola/Utilities/IO/SignalExchange/Examples/FirstOrder.mos
index 5775940658..dfcba5d2ca 100644
--- a/AixLib/Resources/Scripts/Dymola/Utilities/IO/SignalExchange/Examples/FirstOrder.mos
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/IO/SignalExchange/Examples/FirstOrder.mos
@@ -1,3 +1,3 @@
-simulateModel("AixLib.Utilities.IO.SignalExchange.Examples.FirstOrder", stopTime=150, tolerance=1e-6, method="CVode", resultFile="FirstOrder");
+simulateModel("AixLib.Utilities.IO.SignalExchange.Examples.FirstOrder", stopTime=150, tolerance=1e-6, method="CVode", resultFile="FirstOrder");
 createPlot(id=1, position={55, 50, 592, 427}, y={"expMod.oveWriSet_u", "expMod.oveWriAct_u", "expMod.rea"}, range={0.0, 150.0, -2.0, 4.0}, grid=true, colors={{28,108,200}, {238,46,47}, {0,140,72}});
 createPlot(id=1, position={55, 50, 592, 211}, y={"expMod.oveWriSet_activate", "expMod.oveWriAct_activate"}, range={0.0, 150.0, -0.5, 1.5}, grid=true, subPlot=2, colors={{28,108,200}, {28,108,200}});
diff --git a/AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Interpolate.mos b/AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Interpolate.mos
new file mode 100644
index 0000000000..daba715d5b
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Interpolate.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Utilities.Math.Examples.Interpolate", stopTime=500, tolerance=1e-06, resultFile="InterpolateBlock");
+createPlot(id=1, position={15, 15, 584, 361}, x="int.u", y={"int.y"}, range={-50.0, 50.0, -0.1, 0.04000000000000001}, grid=true, filename="InterpolateBlock.mat", colors={{28,108,200}}, timeUnit="Pa", displayUnits={"kg/s"});
diff --git a/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/BaseClasses/Examples/Interpolate.mos b/AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/Interpolate.mos
similarity index 62%
rename from AixLib/Resources/Scripts/Dymola/Airflow/Multizone/BaseClasses/Examples/Interpolate.mos
rename to AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/Interpolate.mos
index f506fa1de6..9c7f4f4401 100644
--- a/AixLib/Resources/Scripts/Dymola/Airflow/Multizone/BaseClasses/Examples/Interpolate.mos
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/Interpolate.mos
@@ -1,2 +1,2 @@
-simulateModel("AixLib.Airflow.Multizone.BaseClasses.Examples.Interpolate", stopTime=500, tolerance=1e-06, resultFile="Interpolate");
+simulateModel("AixLib.Utilities.Math.Functions.Examples.Interpolate", stopTime=500, tolerance=1e-06, resultFile="Interpolate");
 createPlot(id=1, position={15, 15, 584, 361}, x="dp", y={"m_flow"}, range={-50.0, 50.0, -0.1, 0.04000000000000001}, grid=true, filename="Interpolate.mat", colors={{28,108,200}}, timeUnit="Pa", displayUnits={"kg/s"});
diff --git a/AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/SmoothInterpolation.mos b/AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/SmoothInterpolation.mos
new file mode 100644
index 0000000000..fcad767173
--- /dev/null
+++ b/AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/SmoothInterpolation.mos
@@ -0,0 +1,2 @@
+simulateModel("AixLib.Utilities.Math.Functions.Examples.SmoothInterpolation", method="dassl", tolerance=1e-6, stopTime=1.0, resultFile="SmoothInterpolation");
+createPlot(id=1, position={35, 30, 631, 456}, x="x", y={"y", "yMonotone", "y2", "y2Monotone", "y1", "y1Monotone"}, range={-1.5, 7.0, -2.0, 18.0}, grid=true, filename="SmoothInterpolation.mat", colors={{28,108,200}, {238,46,47}, {0,140,72}, {180,56,148}, {0,0,0}, {162,29,33}});
diff --git a/AixLib/Resources/Scripts/travis/dymola/dymola b/AixLib/Resources/Scripts/travis/dymola/dymola
index 2c0ec55605..57d387e91e 100755
--- a/AixLib/Resources/Scripts/travis/dymola/dymola
+++ b/AixLib/Resources/Scripts/travis/dymola/dymola
@@ -15,6 +15,6 @@ docker run \
   --detach=false \
   --rm \
   -v ${sha_dir}:/mnt/shared \
-  ${DOCKER_USERNAME}/travis_ubuntu-2004_dymola:2022x-x86_64 /bin/bash -c \
+  ${DOCKER_REPONAME}/${DYMOLA_VERSION} /bin/bash -c \
   "cd /mnt/shared/${bas_nam} && \
    dymola ${arg_lis}"
diff --git a/AixLib/Resources/Scripts/travis/omc/omc b/AixLib/Resources/Scripts/travis/omc/omc
index d51735ae81..15f716a9c6 100755
--- a/AixLib/Resources/Scripts/travis/omc/omc
+++ b/AixLib/Resources/Scripts/travis/omc/omc
@@ -10,7 +10,7 @@
 #################################################
 set -e
 IMG_NAME=${OMC_VERSION}
-DOCKER_USERNAME=michaelwetter
+DOCKER_REPONAME=lbnlblum
 
 # Function declarations
 function create_mount_command()
@@ -80,18 +80,29 @@ do
     shift
 done
 
-# --user=${UID} \
+# On travis, the current working directory /tmp/tmp-Buildings-0-o0h50lbn (or similar)
+# is created # with permissions drwx------ and owned by the travis user and group (UID=2000).
+# However, omc must be run as user developer (UID=1000) as it accesses ~/.openmodelica/libraries.
+# But running as developer does not allow the docker to access /tmp/tmp-Buildings-0-o0h50lbn.
+# The chmod command below gives access to the current working directory for all users.
+# See also https://app.travis-ci.com/github/lbl-srg/modelica-buildings/builds/255798277
+chmod a+rwx "$cur_dir"
 
+# Below, inside the docker, we remove spawn-* as these files have the permission of the
+# docker user and hence the calling process cannot remove them, which
+# causes an error if BuildingsPy cleans up the temporary directories.
 docker run \
-  --user=${UID} \
+  --user=developer \
   -i \
   $DOCKER_INTERACTIVE \
   --detach=false \
   ${MOD_MOUNT} \
   -v ${sha_dir}:/mnt/shared \
   --rm \
-  ${DOCKER_USERNAME}/${IMG_NAME} /bin/bash -c \
-  "export OPENMODELICALIBRARY=${DOCKER_MODELICAPATH}:/usr/lib/omlibrary && \
-  cd \"/mnt/shared/${bas_nam}\" && \
-  omc ${arg_lis}"
+  --workdir="/mnt/shared/${bas_nam}" \
+  ${DOCKER_REPONAME}/${IMG_NAME} /bin/bash -c \
+  "export MODELICAPATH=${DOCKER_MODELICAPATH} && \
+  omc ${arg_lis} && \
+  rm -rf spawn-* && \
+  rm -rf tmp"
 exit $?
diff --git a/AixLib/Resources/bin/ConvertWeatherData.jar b/AixLib/Resources/bin/ConvertWeatherData.jar
index 2fec94566b..72c3ca93cf 100644
Binary files a/AixLib/Resources/bin/ConvertWeatherData.jar and b/AixLib/Resources/bin/ConvertWeatherData.jar differ
diff --git a/AixLib/Resources/src/convertEPW/src/ConvertWeatherData.java b/AixLib/Resources/src/convertEPW/src/ConvertWeatherData.java
index 6b2888f52d..2983ef1d75 100644
--- a/AixLib/Resources/src/convertEPW/src/ConvertWeatherData.java
+++ b/AixLib/Resources/src/convertEPW/src/ConvertWeatherData.java
@@ -53,7 +53,7 @@ static public String getSimulationTime(int[] time, boolean minuteFlag)
     simtime = 60 * (simtime+time[3]); // hours to minutes
     simtime = 60 * (simtime+time[4]);// minutes to seconds
 
-    // if sub hourly data ara avaible flag becomes true
+    // if sub hourly data ara available flag becomes true
     if (minuteFlag) {
       simtime = simtime - 3600;
     }
@@ -132,20 +132,23 @@ static private ArrayList<String> addcomments(ArrayList<String> myArr)
     *@param inData Inputed data from .epw file
 		*@param preData Data read in previous line
 		*@param missData Missing value for this field
+    *@param description Description of the data
     *@param lineNum Line number
     */
-  static private String checkdata(String inData, String preData, String missData, int lineNum, int i)
+  static private String checkdata(String inData, String preData, String missData, ArrayList<String> description, int lineNum, int i)
   {
 		if (inData.equals(missData)) {
 			if (lineNum == 9) {
-				i = i + 6;
-				System.out.println("The data at line 9 column " + i + " in .epw file is missing. You need to fix it before the convert.");
+				final String des = description.get(i);
+				i = i + 6; // 6 is added because epw has different representation of time and the code column
+				System.out.println("The data at line 9 column " + i + " (" + des + ") in .epw file is equal to '" + missData + "', indicating it is missing. You need to fix it before the convert.");
 			  System.exit (0);
 			}
 			else {
 				lineNum = lineNum + 32;
+				final String des = description.get(i);
 				i = i + 1;
-				System.out.println("Correct the missing data in line " + lineNum + " column " + i);
+				System.out.println("Correct the missing data in line " + lineNum + " column " + i + " (" + des + ")");
 				return preData;
 			}
 		}
@@ -172,6 +175,7 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
     String timeString;
     String[] preData = new String[30];
 		String[] missData = new String[30];
+    ArrayList<String> description = new ArrayList<String>();
     int lineNum;    // line number in .epw file
     int[] time = new int[5];
     int[] timeTemp = new int[5];
@@ -179,7 +183,7 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
     boolean minuteFlag;
 
  		missData[1] = "99.9";
-    missData[2] = "99.9";
+ 		missData[2] = "99.9";
 		missData[3] = "999";
 		missData[4] = "999999";
 		missData[5] = "9999";
@@ -206,6 +210,8 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
 		missData[26] = "99";
 
 
+
+
     console = new Scanner(new File(filename));
     lineChecker = new Scanner(new File(filename));
     minuteFlag = false;
@@ -225,6 +231,13 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
     // add comments for weather data
     myArr = addcomments(myArr);
 
+    // build description strings that are used in error messages
+    description = addcomments(description);
+    for(i=0; i < 30; i++){
+      final String tmpDes = description.get(i);
+      description.set(i, tmpDes.substring(tmpDes.indexOf(' ')).trim());
+    }
+
     // read weather data
     while (console.hasNextLine()) {
       // scan a line
@@ -255,7 +268,7 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
           minuteFlag = false;
         }
         lineChecker.close();
-        lineTokenizerTemp.close(); 
+        lineTokenizerTemp.close();
        }
 
       // convert the time in seconds
@@ -274,7 +287,7 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
 	    for(i=1; i<=4; i++){
 				if (lineTokenizer.hasNext()) {
 					tmp2 = lineTokenizer.next();
-					tmp2 = checkdata(tmp2, preData[i], missData[i], lineNum, i);
+					tmp2 = checkdata(tmp2, preData[i], missData[i], description, lineNum, i);
 		      tmp = tmp + tmp2 + "\t";
 					preData[i] = tmp2;
 		    }
@@ -297,7 +310,7 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
 			i = 8;
 			if (lineTokenizer.hasNext()) {
 				tmp2 = lineTokenizer.next();
-				tmp2 = checkdata(tmp2, preData[i], missData[i], lineNum, i);
+				tmp2 = checkdata(tmp2, preData[i], missData[i], description, lineNum, i);
 	      tmp = tmp + tmp2 + "\t";
 				preData[i] = tmp2;
 	    }
@@ -318,7 +331,7 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
 			i = 10;
 			if (lineTokenizer.hasNext()) {
 				tmp2 = lineTokenizer.next();
-				tmp2 = checkdata(tmp2, preData[i], missData[i], lineNum, i);
+				tmp2 = checkdata(tmp2, preData[i], missData[i], description, lineNum, i);
 	      tmp = tmp + tmp2 + "\t";
 				preData[i] = tmp2;
 	    }
@@ -340,7 +353,7 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
 			for(i=17; i<=18; i++){
 				if (lineTokenizer.hasNext()) {
 					tmp2 = lineTokenizer.next();
-					tmp2 = checkdata(tmp2, preData[i], missData[i], lineNum, i);
+					tmp2 = checkdata(tmp2, preData[i], missData[i], description, lineNum, i);
 		      tmp = tmp + tmp2 + "\t";
 					preData[i] = tmp2;
 		    }
@@ -362,7 +375,7 @@ static public ArrayList<String> convert(String filename, ArrayList<String> myArr
 			i = 20;
 			if (lineTokenizer.hasNext()) {
 				tmp2 = lineTokenizer.next();
-				tmp2 = checkdata(tmp2, preData[i], missData[i], lineNum, i);
+				tmp2 = checkdata(tmp2, preData[i], missData[i], description, lineNum, i);
 		    if (tmp2.equals("88888") || tmp2.equals("77777") || tmp2.equals("99999"))
 		      tmp2 = "2000";
 				tmp = tmp + tmp2 + "\t";
diff --git a/AixLib/Resources/src/convertEPW/src/Makefile b/AixLib/Resources/src/convertEPW/src/Makefile
index ada2d56027..30d215a200 100644
--- a/AixLib/Resources/src/convertEPW/src/Makefile
+++ b/AixLib/Resources/src/convertEPW/src/Makefile
@@ -22,7 +22,7 @@ OBJS = ConvertWeatherData.class
 JARS = ConvertWeatherData.jar
 #######################################################
 all: clean doc
-	$(JC) $(SRCS)
+	$(JC) --release 8 $(SRCS)
 	$(JJ) $(JFLAGS) $(JARS) Manifest.txt $(OBJS) $(SRCS)
 	$(JJ) -i $(JARS)
 	rm $(OBJS)
diff --git a/AixLib/Resources/src/fluid/heatpumps/calibration/Examples/SomeManufacturer_ABC060_70kW_4_0COP_R410A.mo b/AixLib/Resources/src/fluid/heatpumps/calibration/Examples/SomeManufacturer_ABC060_70kW_4_0COP_R410A.mo
index 0f4ba879d0..21c9566e72 100644
--- a/AixLib/Resources/src/fluid/heatpumps/calibration/Examples/SomeManufacturer_ABC060_70kW_4_0COP_R410A.mo
+++ b/AixLib/Resources/src/fluid/heatpumps/calibration/Examples/SomeManufacturer_ABC060_70kW_4_0COP_R410A.mo
@@ -1,22 +1,22 @@
 within AixLib.Fluid.HeatPumps.Data.ScrollWaterToWater.Heating;
- record SomeManufacturer_ABC060_70kW_4_0COP_R410A =
-   AixLib.Fluid.HeatPumps.Data.ScrollWaterToWater.Generic (
-     volRat = 2.36185869323,
-     V_flow_nominal = 0.00287086738316,
-     leaCoe = 0.00408074950474,
-     etaEle = 0.922319423243,
-     PLos = 398.665383784,
-     dTSup = 6.49606895698,
-     UACon = 7014.54967992,
-     UAEva = 49135.9514647)
- 
-   annotation (
-     defaultComponentPrefixes = "parameter",
-     defaultComponentName="datHeaPum",
-     preferredView="info",
-   Documentation(info="<html>
- <p>
- Generated by Mr Modeler on 2017-01-26.
- </p>
- </html>"),  
+record SomeManufacturer_ABC060_70kW_4_0COP_R410A =
+  AixLib.Fluid.HeatPumps.Data.ScrollWaterToWater.Generic (
+    volRat = 2.36185869323,
+    V_flow_nominal = 0.00287086738316,
+    leaCoe = 0.00408074950474,
+    etaEle = 0.922319423243,
+    PLos = 398.665383784,
+    dTSup = 6.49606895698,
+    UACon = 7014.54967992,
+    UAEva = 49135.9514647)
+
+  annotation (
+    defaultComponentPrefixes = "parameter",
+    defaultComponentName="datHeaPum",
+    preferredView="info",
+  Documentation(info="<html>
+<p>
+Generated by Mr Modeler on 2017-01-26.
+</p>
+</html>"),  
    __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Resources/src/fluid/heatpumps/calibration/doc/build/html/_static/language_data.js b/AixLib/Resources/src/fluid/heatpumps/calibration/doc/build/html/_static/language_data.js
new file mode 100644
index 0000000000..863704b310
--- /dev/null
+++ b/AixLib/Resources/src/fluid/heatpumps/calibration/doc/build/html/_static/language_data.js
@@ -0,0 +1,297 @@
+/*
+ * language_data.js
+ * ~~~~~~~~~~~~~~~~
+ *
+ * This script contains the language-specific data used by searchtools.js,
+ * namely the list of stopwords, stemmer, scorer and splitter.
+ *
+ * :copyright: Copyright 2007-2021 by the Sphinx team, see AUTHORS.
+ * :license: BSD, see LICENSE for details.
+ *
+ */
+
+var stopwords = ["a","and","are","as","at","be","but","by","for","if","in","into","is","it","near","no","not","of","on","or","such","that","the","their","then","there","these","they","this","to","was","will","with"];
+
+
+/* Non-minified version is copied as a separate JS file, is available */
+
+/**
+ * Porter Stemmer
+ */
+var Stemmer = function() {
+
+  var step2list = {
+    ational: 'ate',
+    tional: 'tion',
+    enci: 'ence',
+    anci: 'ance',
+    izer: 'ize',
+    bli: 'ble',
+    alli: 'al',
+    entli: 'ent',
+    eli: 'e',
+    ousli: 'ous',
+    ization: 'ize',
+    ation: 'ate',
+    ator: 'ate',
+    alism: 'al',
+    iveness: 'ive',
+    fulness: 'ful',
+    ousness: 'ous',
+    aliti: 'al',
+    iviti: 'ive',
+    biliti: 'ble',
+    logi: 'log'
+  };
+
+  var step3list = {
+    icate: 'ic',
+    ative: '',
+    alize: 'al',
+    iciti: 'ic',
+    ical: 'ic',
+    ful: '',
+    ness: ''
+  };
+
+  var c = "[^aeiou]";          // consonant
+  var v = "[aeiouy]";          // vowel
+  var C = c + "[^aeiouy]*";    // consonant sequence
+  var V = v + "[aeiou]*";      // vowel sequence
+
+  var mgr0 = "^(" + C + ")?" + V + C;                      // [C]VC... is m>0
+  var meq1 = "^(" + C + ")?" + V + C + "(" + V + ")?$";    // [C]VC[V] is m=1
+  var mgr1 = "^(" + C + ")?" + V + C + V + C;              // [C]VCVC... is m>1
+  var s_v   = "^(" + C + ")?" + v;                         // vowel in stem
+
+  this.stemWord = function (w) {
+    var stem;
+    var suffix;
+    var firstch;
+    var origword = w;
+
+    if (w.length < 3)
+      return w;
+
+    var re;
+    var re2;
+    var re3;
+    var re4;
+
+    firstch = w.substr(0,1);
+    if (firstch == "y")
+      w = firstch.toUpperCase() + w.substr(1);
+
+    // Step 1a
+    re = /^(.+?)(ss|i)es$/;
+    re2 = /^(.+?)([^s])s$/;
+
+    if (re.test(w))
+      w = w.replace(re,"$1$2");
+    else if (re2.test(w))
+      w = w.replace(re2,"$1$2");
+
+    // Step 1b
+    re = /^(.+?)eed$/;
+    re2 = /^(.+?)(ed|ing)$/;
+    if (re.test(w)) {
+      var fp = re.exec(w);
+      re = new RegExp(mgr0);
+      if (re.test(fp[1])) {
+        re = /.$/;
+        w = w.replace(re,"");
+      }
+    }
+    else if (re2.test(w)) {
+      var fp = re2.exec(w);
+      stem = fp[1];
+      re2 = new RegExp(s_v);
+      if (re2.test(stem)) {
+        w = stem;
+        re2 = /(at|bl|iz)$/;
+        re3 = new RegExp("([^aeiouylsz])\\1$");
+        re4 = new RegExp("^" + C + v + "[^aeiouwxy]$");
+        if (re2.test(w))
+          w = w + "e";
+        else if (re3.test(w)) {
+          re = /.$/;
+          w = w.replace(re,"");
+        }
+        else if (re4.test(w))
+          w = w + "e";
+      }
+    }
+
+    // Step 1c
+    re = /^(.+?)y$/;
+    if (re.test(w)) {
+      var fp = re.exec(w);
+      stem = fp[1];
+      re = new RegExp(s_v);
+      if (re.test(stem))
+        w = stem + "i";
+    }
+
+    // Step 2
+    re = /^(.+?)(ational|tional|enci|anci|izer|bli|alli|entli|eli|ousli|ization|ation|ator|alism|iveness|fulness|ousness|aliti|iviti|biliti|logi)$/;
+    if (re.test(w)) {
+      var fp = re.exec(w);
+      stem = fp[1];
+      suffix = fp[2];
+      re = new RegExp(mgr0);
+      if (re.test(stem))
+        w = stem + step2list[suffix];
+    }
+
+    // Step 3
+    re = /^(.+?)(icate|ative|alize|iciti|ical|ful|ness)$/;
+    if (re.test(w)) {
+      var fp = re.exec(w);
+      stem = fp[1];
+      suffix = fp[2];
+      re = new RegExp(mgr0);
+      if (re.test(stem))
+        w = stem + step3list[suffix];
+    }
+
+    // Step 4
+    re = /^(.+?)(al|ance|ence|er|ic|able|ible|ant|ement|ment|ent|ou|ism|ate|iti|ous|ive|ize)$/;
+    re2 = /^(.+?)(s|t)(ion)$/;
+    if (re.test(w)) {
+      var fp = re.exec(w);
+      stem = fp[1];
+      re = new RegExp(mgr1);
+      if (re.test(stem))
+        w = stem;
+    }
+    else if (re2.test(w)) {
+      var fp = re2.exec(w);
+      stem = fp[1] + fp[2];
+      re2 = new RegExp(mgr1);
+      if (re2.test(stem))
+        w = stem;
+    }
+
+    // Step 5
+    re = /^(.+?)e$/;
+    if (re.test(w)) {
+      var fp = re.exec(w);
+      stem = fp[1];
+      re = new RegExp(mgr1);
+      re2 = new RegExp(meq1);
+      re3 = new RegExp("^" + C + v + "[^aeiouwxy]$");
+      if (re.test(stem) || (re2.test(stem) && !(re3.test(stem))))
+        w = stem;
+    }
+    re = /ll$/;
+    re2 = new RegExp(mgr1);
+    if (re.test(w) && re2.test(w)) {
+      re = /.$/;
+      w = w.replace(re,"");
+    }
+
+    // and turn initial Y back to y
+    if (firstch == "y")
+      w = firstch.toLowerCase() + w.substr(1);
+    return w;
+  }
+}
+
+
+
+
+var splitChars = (function() {
+    var result = {};
+    var singles = [96, 180, 187, 191, 215, 247, 749, 885, 903, 907, 909, 930, 1014, 1648,
+         1748, 1809, 2416, 2473, 2481, 2526, 2601, 2609, 2612, 2615, 2653, 2702,
+         2706, 2729, 2737, 2740, 2857, 2865, 2868, 2910, 2928, 2948, 2961, 2971,
+         2973, 3085, 3089, 3113, 3124, 3213, 3217, 3241, 3252, 3295, 3341, 3345,
+         3369, 3506, 3516, 3633, 3715, 3721, 3736, 3744, 3748, 3750, 3756, 3761,
+         3781, 3912, 4239, 4347, 4681, 4695, 4697, 4745, 4785, 4799, 4801, 4823,
+         4881, 5760, 5901, 5997, 6313, 7405, 8024, 8026, 8028, 8030, 8117, 8125,
+         8133, 8181, 8468, 8485, 8487, 8489, 8494, 8527, 11311, 11359, 11687, 11695,
+         11703, 11711, 11719, 11727, 11735, 12448, 12539, 43010, 43014, 43019, 43587,
+         43696, 43713, 64286, 64297, 64311, 64317, 64319, 64322, 64325, 65141];
+    var i, j, start, end;
+    for (i = 0; i < singles.length; i++) {
+        result[singles[i]] = true;
+    }
+    var ranges = [[0, 47], [58, 64], [91, 94], [123, 169], [171, 177], [182, 184], [706, 709],
+         [722, 735], [741, 747], [751, 879], [888, 889], [894, 901], [1154, 1161],
+         [1318, 1328], [1367, 1368], [1370, 1376], [1416, 1487], [1515, 1519], [1523, 1568],
+         [1611, 1631], [1642, 1645], [1750, 1764], [1767, 1773], [1789, 1790], [1792, 1807],
+         [1840, 1868], [1958, 1968], [1970, 1983], [2027, 2035], [2038, 2041], [2043, 2047],
+         [2070, 2073], [2075, 2083], [2085, 2087], [2089, 2307], [2362, 2364], [2366, 2383],
+         [2385, 2391], [2402, 2405], [2419, 2424], [2432, 2436], [2445, 2446], [2449, 2450],
+         [2483, 2485], [2490, 2492], [2494, 2509], [2511, 2523], [2530, 2533], [2546, 2547],
+         [2554, 2564], [2571, 2574], [2577, 2578], [2618, 2648], [2655, 2661], [2672, 2673],
+         [2677, 2692], [2746, 2748], [2750, 2767], [2769, 2783], [2786, 2789], [2800, 2820],
+         [2829, 2830], [2833, 2834], [2874, 2876], [2878, 2907], [2914, 2917], [2930, 2946],
+         [2955, 2957], [2966, 2968], [2976, 2978], [2981, 2983], [2987, 2989], [3002, 3023],
+         [3025, 3045], [3059, 3076], [3130, 3132], [3134, 3159], [3162, 3167], [3170, 3173],
+         [3184, 3191], [3199, 3204], [3258, 3260], [3262, 3293], [3298, 3301], [3312, 3332],
+         [3386, 3388], [3390, 3423], [3426, 3429], [3446, 3449], [3456, 3460], [3479, 3481],
+         [3518, 3519], [3527, 3584], [3636, 3647], [3655, 3663], [3674, 3712], [3717, 3718],
+         [3723, 3724], [3726, 3731], [3752, 3753], [3764, 3772], [3774, 3775], [3783, 3791],
+         [3802, 3803], [3806, 3839], [3841, 3871], [3892, 3903], [3949, 3975], [3980, 4095],
+         [4139, 4158], [4170, 4175], [4182, 4185], [4190, 4192], [4194, 4196], [4199, 4205],
+         [4209, 4212], [4226, 4237], [4250, 4255], [4294, 4303], [4349, 4351], [4686, 4687],
+         [4702, 4703], [4750, 4751], [4790, 4791], [4806, 4807], [4886, 4887], [4955, 4968],
+         [4989, 4991], [5008, 5023], [5109, 5120], [5741, 5742], [5787, 5791], [5867, 5869],
+         [5873, 5887], [5906, 5919], [5938, 5951], [5970, 5983], [6001, 6015], [6068, 6102],
+         [6104, 6107], [6109, 6111], [6122, 6127], [6138, 6159], [6170, 6175], [6264, 6271],
+         [6315, 6319], [6390, 6399], [6429, 6469], [6510, 6511], [6517, 6527], [6572, 6592],
+         [6600, 6607], [6619, 6655], [6679, 6687], [6741, 6783], [6794, 6799], [6810, 6822],
+         [6824, 6916], [6964, 6980], [6988, 6991], [7002, 7042], [7073, 7085], [7098, 7167],
+         [7204, 7231], [7242, 7244], [7294, 7400], [7410, 7423], [7616, 7679], [7958, 7959],
+         [7966, 7967], [8006, 8007], [8014, 8015], [8062, 8063], [8127, 8129], [8141, 8143],
+         [8148, 8149], [8156, 8159], [8173, 8177], [8189, 8303], [8306, 8307], [8314, 8318],
+         [8330, 8335], [8341, 8449], [8451, 8454], [8456, 8457], [8470, 8472], [8478, 8483],
+         [8506, 8507], [8512, 8516], [8522, 8525], [8586, 9311], [9372, 9449], [9472, 10101],
+         [10132, 11263], [11493, 11498], [11503, 11516], [11518, 11519], [11558, 11567],
+         [11622, 11630], [11632, 11647], [11671, 11679], [11743, 11822], [11824, 12292],
+         [12296, 12320], [12330, 12336], [12342, 12343], [12349, 12352], [12439, 12444],
+         [12544, 12548], [12590, 12592], [12687, 12689], [12694, 12703], [12728, 12783],
+         [12800, 12831], [12842, 12880], [12896, 12927], [12938, 12976], [12992, 13311],
+         [19894, 19967], [40908, 40959], [42125, 42191], [42238, 42239], [42509, 42511],
+         [42540, 42559], [42592, 42593], [42607, 42622], [42648, 42655], [42736, 42774],
+         [42784, 42785], [42889, 42890], [42893, 43002], [43043, 43055], [43062, 43071],
+         [43124, 43137], [43188, 43215], [43226, 43249], [43256, 43258], [43260, 43263],
+         [43302, 43311], [43335, 43359], [43389, 43395], [43443, 43470], [43482, 43519],
+         [43561, 43583], [43596, 43599], [43610, 43615], [43639, 43641], [43643, 43647],
+         [43698, 43700], [43703, 43704], [43710, 43711], [43715, 43738], [43742, 43967],
+         [44003, 44015], [44026, 44031], [55204, 55215], [55239, 55242], [55292, 55295],
+         [57344, 63743], [64046, 64047], [64110, 64111], [64218, 64255], [64263, 64274],
+         [64280, 64284], [64434, 64466], [64830, 64847], [64912, 64913], [64968, 65007],
+         [65020, 65135], [65277, 65295], [65306, 65312], [65339, 65344], [65371, 65381],
+         [65471, 65473], [65480, 65481], [65488, 65489], [65496, 65497]];
+    for (i = 0; i < ranges.length; i++) {
+        start = ranges[i][0];
+        end = ranges[i][1];
+        for (j = start; j <= end; j++) {
+            result[j] = true;
+        }
+    }
+    return result;
+})();
+
+function splitQuery(query) {
+    var result = [];
+    var start = -1;
+    for (var i = 0; i < query.length; i++) {
+        if (splitChars[query.charCodeAt(i)]) {
+            if (start !== -1) {
+                result.push(query.slice(start, i));
+                start = -1;
+            }
+        } else if (start === -1) {
+            start = i;
+        }
+    }
+    if (start !== -1) {
+        result.push(query.slice(start));
+    }
+    return result;
+}
+
+
diff --git a/AixLib/Resources/weatherdata/DRYCOLD.TMY b/AixLib/Resources/weatherdata/DRYCOLD.TMY
new file mode 100644
index 0000000000..a01f6629bb
--- /dev/null
+++ b/AixLib/Resources/weatherdata/DRYCOLD.TMY
@@ -0,0 +1,8760 @@
+23062590101010000330000999999999999999999999999999999800009999999999990177770230002410000000010071 8278   0 -66203  2807039
+23062590101020001330000999999999999999999999999999999800009999999999990277770230002410000000010056 8264   0 -61203  3309049
+23062590101030002330000999999999999999999999999999999800009999999999990377770230002410000000010043 8251   0 -67180  3708049
+23062590101040003330000999999999999999999999999999999800009999999999990477770230002410000000010032 8237   0 -67180  4109049
+23062590101050004330000999999999999999999999999999999800009999999999990577770250002410000000010023 8224   0 -66203  4610059
+23062590101060005330000999999999999999999999999999999800009999999999990604880460002410000000010016 8211   0 -89293  5010079
+23062590101070006330000999999999999999999999999999999800009999999999990704880460002410000000010023 8223  33 -67315  3110069
+230625901010800073301677   89999999999999999999999999200259999999999990804270460009660000000010018 8213  22 -61135  4110109
+230625901010900083309207 2439999999999999999999999999203369999999999990904570460009660000000010017 8213  33 -50 68  3110099
+230625901011000093315887  589999999999999999999999999204209999999999991006100246009660000000010005 8213  72 -89338  9810109
+230625901011100103320607268699999999999999999999999992128499999999999911888802240096600000000 9992 8207  78-106293 10309069
+230625901011200113323057335799999999999999999999999992167699999999999912777702000096600000000 9982 8200  89 -89293  9301019
+230625901011300123323057338399999999999999999999999992168899999999999913777702200096600000000 9970 8193  94 -89315  9301019
+230625901011400133320607336599999999999999999999999992152899999999999914777700000096600000000 9959 8186 106-106293  9300009
+230625901011500143315887297499999999999999999999999992110399999999999915777702200096600000000 9961 8190 100-106315  4601019
+230625901011600153309207241799999999999999999999999992061699999999999916777700000096600000000 9957 8186  94 -94270  8800009
+230625901011700163301677 28599999999999999999999999992007799999999999917777700000096600000000 9969 8190  67-111 23  7700009
+230625901011800173300009999999999999999999999999999998000099999999999918777700000064400000000 9973 8196  56-117 68  4600009
+230625901011900183300009999999999999999999999999999998000099999999999919777700000024100000000 9982 8200  28-100113  1500009
+230625901012000193300009999999999999999999999999999998000099999999999920777700000024100000000 9990 8203  22-100113  3100009
+230625901012100203300009999999999999999999999999999998000099999999999921777702000024100000000 9992 8207  17-117 68  2101019
+230625901012200213300009999999999999999999999999999998000099999999999922777702000024100000000 9992 8213   6-117 68  2604049
+23062590101230022330000999999999999999999999999999999800009999999999992377770200002410000000010004 8223   0 -94 45  9304049
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diff --git a/AixLib/Resources/weatherdata/DRYCOLD.mos b/AixLib/Resources/weatherdata/DRYCOLD.mos
new file mode 100644
index 0000000000..c89c017b1f
--- /dev/null
+++ b/AixLib/Resources/weatherdata/DRYCOLD.mos
@@ -0,0 +1,8800 @@
+#1
+double tab1(8760,30)
+#LOCATION,Denver-Stapleton,CO,USA,TMY--23062,724690,39.76,-104.86,-7.0,1611.0
+#DESIGN CONDITIONS,1,Climate Design Data 2009 ASHRAE Handbook,,Heating,12,-20,-16,-24.1,0.5,-17.1,-20.2,0.8,-11.3,12.4,2.7,10.7,4.8,2.3,180,Cooling,7,15.2,34.1,15.9,32.6,15.6,31.1,15.4,18.1,27.7,17.5,26.9,16.9,26.4,4,120,15.7,13.6,20,14.7,12.7,19.8,13.8,12,20,57.7,27.9,55.4,26.6,53.3,26.4,733,Extremes,10.9,8.8,7.7,21.9,-24.6,37.2,4.1,1.4,-27.5,38.2,-29.9,39,-32.2,39.7,-35.1,40.7
+#TYPICAL/EXTREME PERIODS,6,Summer - Week Nearest Max Temperature For Period,Extreme,7/20,7/26,Summer - Week Nearest Average Temperature For Period,Typical,8/ 3,8/ 9,Winter - Week Nearest Min Temperature For Period,Extreme,12/22,1/ 5,Winter - Week Nearest Average Temperature For Period,Typical,1/27,2/ 2,Autumn - Week Nearest Average Temperature For Period,Typical,10/20,10/26,Spring - Week Nearest Average Temperature For Period,Typical,4/ 5,4/11
+#GROUND TEMPERATURES,3,.5,,,,-0.36,-1.35,0.40,3.13,10.29,15.81,19.53,20.67,18.74,14.45,8.72,3.41,2,,,,3.26,1.51,1.87,3.32,8.11,12.43,15.89,17.75,17.36,14.93,10.98,6.79,4,,,,6.26,4.46,4.07,4.61,7.32,10.24,12.91,14.77,15.21,14.15,11.84,9.01
+#HOLIDAYS/DAYLIGHT SAVINGS,No,0,0,0
+#COMMENTS 1,TMY-23062 -- WMO#724690
+#COMMENTS 2, -- Ground temps produced with a standard soil diffusivity of 2.3225760E-03 {m**2/day}
+#DATA PERIODS,1,1,Data,Sunday, 1/ 1,12/31
+#C1 Time in seconds. Beginning of a year is 0s.
+#C2 Dry bulb temperature in Celsius at indicated time
+#C3 Dew point temperature in Celsius at indicated time
+#C4 Relative humidity in percent at indicated time
+#C5 Atmospheric station pressure in Pa at indicated time
+#C6 Extraterrestrial horizontal radiation in Wh/m2
+#C7 Extraterrestrial direct normal radiation in Wh/
+#C8 Horizontal infrared radiation intensity in Wh/m2
+#C9 Global horizontal radiation in Wh/m2
+#C10 Direct normal radiation in Wh/m2
+#C11 Diffuse horizontal radiation in Wh/m2
+#C12 Averaged global horizontal illuminance in lux during minutes preceding the indicated time
+#C13 Direct normal illuminance in lux during minutes preceding the indicated time
+#C14 Diffuse horizontal illuminance in lux  during minutes preceding the indicated time
+#C15 Zenith luminance in Cd/m2 during minutes preceding the indicated time
+#C16 Wind direction at indicated time. N=0, E=90, S=180, W=270
+#C17 Wind speed in m/s at indicated time
+#C18 Total sky cover at indicated time
+#C19 Opaque sky cover at indicated time
+#C20 Visibility in km at indicated time
+#C21 Ceiling height in m
+#C22 Present weather observation
+#C23 Present weather codes
+#C24 Precipitable water in mm
+#C25 Aerosol optical depth
+#C26 Snow depth in cm
+#C27 Days since last snowfall
+#C28 Albedo
+#C29 Liquid precipitation depth in mm at indicated time
+#C30 Liquid precipitation quantity
+3600	0	-6.6	57	82780	0	0	253	0	0	0	999900	999900	999900	99990	203	2.8	7	3	24.1	77777	0	999999999	0	0	0	88	0	0	0
+7200	0	-6.1	60	82640	0	0	255	0	0	0	999900	999900	999900	99990	203	3.3	9	4	24.1	77777	0	999999999	0	0	0	88	0	0	0
+10800	0	-6.7	57	82510	0	0	255	0	0	0	999900	999900	999900	99990	180	3.7	8	4	24.1	77777	0	999999999	0	0	0	88	0	0	0
+14400	0	-6.7	57	82370	0	0	255	0	0	0	999900	999900	999900	99990	180	4.1	9	4	24.1	77777	0	999999999	0	0	0	88	0	0	0
+18000	0	-6.6	57	82240	0	0	257	0	0	0	999900	999900	999900	99990	203	4.6	10	5	24.1	77777	0	999999999	0	0	0	88	0	0	0
+21600	0	-8.9	47	82110	0	0	260	0	0	0	999900	999900	999900	99990	293	5	10	7	24.1	48800	0	999999999	0	0	0	88	0	0	0
+25200	3.3	-6.7	45	82230	0	0	272	0	0	0	999900	999900	999900	99990	315	3.1	10	6	24.1	48800	0	999999999	0	0	0	88	0	0	0
+28800	2.2	-6.1	51	82130	0	0	290	7	2	7	999900	999900	999900	99990	135	4.1	10	10	96.6	42700	0	999999999	0	0	0	88	0	0	0
+32400	3.3	-5	52	82130	135	635	287	93	68	87	999900	999900	999900	99990	68	3.1	10	9	96.6	45700	0	999999999	0	0	0	88	0	0	0
+36000	7.2	-8.9	28	82130	345	774	308	117	16	113	999900	999900	999900	99990	338	9.8	10	10	96.6	61000	0	999999999	0	0	0	88	0	0	0
+39600	7.8	-10.6	23	82070	507	877	286	357	746	90	999900	999900	999900	99990	293	10.3	9	6	96.6	88888	0	999999999	0	0	0	88	0	0	0
+43200	8.9	-8.9	25	82000	610	942	279	466	933	65	999900	999900	999900	99990	293	9.3	1	1	96.6	77777	0	999999999	0	0	0	88	0	0	0
+46800	9.4	-8.9	24	81930	647	965	281	469	940	40	999900	999900	999900	99990	315	9.3	1	1	96.6	77777	0	999999999	0	0	0	88	0	0	0
+50400	10.6	-10.6	19	81860	616	946	278	424	935	18	999900	999900	999900	99990	293	9.3	0	0	96.6	77777	0	999999999	0	0	0	88	0	0	0
+54000	10	-10.6	20	81900	519	885	281	306	826	4	999900	999900	999900	99990	315	4.6	1	1	96.6	77777	0	999999999	0	0	0	88	0	0	0
+57600	9.4	-9.4	23	81860	362	785	275	171	671	0	999900	999900	999900	99990	270	8.8	0	0	96.6	77777	0	999999999	0	0	0	88	0	0	0
+61200	6.7	-11.1	24	81900	156	650	263	21	79	13	999900	999900	999900	99990	23	7.7	0	0	96.6	77777	0	999999999	0	0	0	88	0	0	0
+64800	5.6	-11.7	25	81960	0	0	258	0	0	0	999900	999900	999900	99990	68	4.6	0	0	64.4	77777	0	999999999	0	0	0	88	0	0	0
+68400	2.8	-10	35	82000	0	0	249	0	0	0	999900	999900	999900	99990	113	1.5	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
+72000	2.2	-10	36	82030	0	0	247	0	0	0	999900	999900	999900	99990	113	3.1	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
+75600	1.7	-11.7	32	82070	0	0	248	0	0	0	999900	999900	999900	99990	68	2.1	1	1	24.1	77777	0	999999999	0	0	0	88	0	0	0
+79200	0.6	-11.7	35	82130	0	0	252	0	0	0	999900	999900	999900	99990	68	2.6	4	4	24.1	77777	0	999999999	0	0	0	88	0	0	0
+82800	0	-9.4	45	82230	0	0	252	0	0	0	999900	999900	999900	99990	45	9.3	4	4	24.1	77777	0	999999999	0	0	0	88	0	0	0
+86400	-4.4	-7.2	79	82300	0	0	262	0	0	0	999900	999900	999900	99990	23	7.7	10	10	24.1	1200	0	999909999	0	0	0	88	0	0	0
+90000	-5.6	-8.3	79	82440	0	0	256	0	0	0	999900	999900	999900	99990	23	7.7	10	10	24.1	2400	0	999909999	0	0	0	88	0	0	0
+93600	-7.2	-11.7	67	82510	0	0	247	0	0	0	999900	999900	999900	99990	23	8.2	10	10	9.7	2400	0	999909999	0	0	0	88	0	0	0
+97200	-8.9	-12.2	75	82570	0	0	240	0	0	0	999900	999900	999900	99990	23	6.2	10	10	4.8	4000	0	999099999	0	0	0	88	0	0	0
+100800	-9.4	-12.2	78	82570	0	0	238	0	0	0	999900	999900	999900	99990	45	6.2	10	10	3.2	4000	0	999099999	0	0	0	88	0	0	0
+104400	-10.6	-13.3	78	82540	0	0	233	0	0	0	999900	999900	999900	99990	68	5.7	10	10	3.2	3000	0	999099999	0	0	0	88	0	0	0
+108000	-11.7	-15	74	82510	0	0	227	0	0	0	999900	999900	999900	99990	45	5.1	10	10	9.7	12200	0	999099999	0	0	0	88	0	0	0
+111600	-12.2	-14.4	82	82540	0	0	226	0	0	0	999900	999900	999900	99990	45	6.2	10	10	6.4	5800	0	999099999	0	0	0	88	0	0	0
+115200	-12.2	-15.6	73	82610	0	0	225	3	0	3	999900	999900	999900	99990	45	6.7	10	10	3.2	4600	0	999099999	0	0	0	88	0	0	0
+118800	-12.8	-15	82	82710	135	635	224	26	3	26	999900	999900	999900	99990	68	6.2	10	10	3.2	3700	0	999099999	0	0	0	88	0	0	0
+122400	-12.8	-17.2	67	82670	345	774	222	48	4	47	999900	999900	999900	99990	90	4.6	10	10	4	6100	0	999099999	0	0	0	88	0	0	0
+126000	-12.8	-17.2	67	82610	508	878	222	65	4	63	999900	999900	999900	99990	68	4.1	10	10	4.8	3700	0	999099999	0	0	0	88	0	0	0
+129600	-13.9	-17.8	70	82540	611	943	217	74	4	72	999900	999900	999900	99990	45	8.2	10	10	2.4	2400	0	999099999	0	0	0	88	0	0	0
+133200	-15	-17.8	77	82470	649	966	214	74	4	72	999900	999900	999900	99990	45	6.7	10	10	2.4	3700	0	999099999	0	0	0	88	0	0	0
+136800	-15	-17.8	77	82540	619	947	214	65	4	63	999900	999900	999900	99990	45	6.2	10	10	2	2100	0	999099999	0	0	0	88	0	0	0
+140400	-15	-19.4	66	82640	522	887	212	48	4	47	999900	999900	999900	99990	23	6.7	10	10	2	2700	0	999099999	0	0	0	88	0	0	0
+144000	-16.1	-20	69	82780	365	787	208	26	3	26	999900	999900	999900	99990	68	5.1	10	10	3.2	2700	0	999099999	0	0	0	88	0	0	0
+147600	-17.2	-20.6	72	82840	160	652	204	3	1	3	999900	999900	999900	99990	45	6.2	10	10	4.8	2700	0	999099099	0	0	0	88	0	0	0
+151200	-17.8	-20.6	77	82910	0	0	202	0	0	0	999900	999900	999900	99990	45	6.2	10	10	6.4	2700	0	999099099	0	0	0	88	0	0	0
+154800	-17.8	-22.8	62	83050	0	0	200	0	0	0	999900	999900	999900	99990	68	6.2	10	10	6.4	2700	0	999099099	0	0	0	88	0	0	0
+158400	-18.3	-22.2	69	83050	0	0	199	0	0	0	999900	999900	999900	99990	68	4.6	10	10	3.2	2700	0	999099099	0	0	0	88	0	0	0
+162000	-18.3	-23.9	58	83050	0	0	198	0	0	0	999900	999900	999900	99990	68	5.1	10	10	3.2	2700	0	999099999	0	0	0	88	0	0	0
+165600	-18.9	-22.8	69	83050	0	0	197	0	0	0	999900	999900	999900	99990	68	5.1	10	10	3.2	2700	0	999099999	0	0	0	88	0	0	0
+169200	-19.4	-23.3	69	83010	0	0	195	0	0	0	999900	999900	999900	99990	45	5.1	10	10	4	2700	0	999099999	0	0	0	88	0	0	0
+172800	-18.9	-22.2	73	82980	0	0	197	0	0	0	999900	999900	999900	99990	90	5.1	10	10	2.4	2700	0	999099999	0	0	0	88	0	0	0
+176400	-19.4	-22.8	72	82950	0	0	195	0	0	0	999900	999900	999900	99990	113	4.6	10	10	3.2	3700	0	999099999	0	0	0	88	0	0	0
+180000	-18.9	-22.8	69	82950	0	0	197	0	0	0	999900	999900	999900	99990	113	4.6	10	10	2.4	3700	0	999099999	0	0	0	88	0	0	0
+183600	-18.9	-23.3	65	82950	0	0	197	0	0	0	999900	999900	999900	99990	68	3.6	10	10	3.2	3700	0	999099999	0	0	0	88	0	0	0
+187200	-19.4	-23.3	69	82910	0	0	195	0	0	0	999900	999900	999900	99990	68	3.1	10	10	4	4300	0	999099999	0	0	0	88	0	0	0
+190800	-20	-23.9	68	82840	0	0	193	0	0	0	999900	999900	999900	99990	45	4.1	10	10	4	6100	0	999099999	0	0	0	88	0	0	0
+194400	-20.6	-25.6	61	82880	0	0	180	0	0	0	999900	999900	999900	99990	68	5.1	8	8	6.4	7600	0	999099999	0	0	0	88	0	0	0
+198000	-20.6	-23.9	72	82910	0	0	191	0	0	0	999900	999900	999900	99990	90	5.7	10	10	4.8	5500	0	999099999	0	0	0	88	0	0	0
+201600	-20.6	-25.6	61	83010	0	0	184	7	2	7	999900	999900	999900	99990	360	3.1	9	9	11.3	7600	0	999099999	0	0	0	88	0	0	0
+205200	-20.6	-25.6	61	83080	135	635	180	80	33	77	999900	999900	999900	99990	360	6.7	10	8	6.4	6100	0	999699999	0	0	0	88	0	0	0
+208800	-21.1	-26.7	57	83120	345	774	182	104	9	102	999900	999900	999900	99990	315	5.1	10	9	4.8	3700	0	999699999	0	0	0	88	0	0	0
+212400	-22.2	-26.1	68	83080	508	878	179	139	9	136	999900	999900	999900	99990	315	4.6	10	9	4.8	3700	0	999699999	0	0	0	88	0	0	0
+216000	-20	-26.7	52	83010	613	944	170	460	916	64	999900	999900	999900	99990	338	4.1	2	2	12.9	77777	0	999999999	0	0	0	88	0	0	0
+219600	-18.9	-25.6	52	82950	651	967	177	447	889	39	999900	999900	999900	99990	315	4.1	4	4	12.9	77777	0	999999999	0	0	0	88	0	0	0
+223200	-18.9	-27.8	42	82910	621	949	176	300	453	101	999900	999900	999900	99990	23	4.1	5	4	11.3	77777	0	999699999	0	0	0	88	0	0	0
+226800	-19.4	-25.6	54	82950	525	889	173	234	449	68	999900	999900	999900	99990	315	3.1	8	2	8	77777	0	999699999	0	0	0	88	0	0	0
+230400	-20.6	-25	65	82980	368	789	172	163	613	4	999900	999900	999900	99990	23	3.1	8	3	16.1	77777	0	999999999	0	0	0	88	0	0	0
+234000	-20.6	-26.1	58	83010	163	654	174	21	54	14	999900	999900	999900	99990	23	2.6	6	5	16.1	27400	0	999999999	0	0	0	88	0	0	0
+237600	-21.1	-26.1	61	83050	0	0	171	0	0	0	999900	999900	999900	99990	68	2.1	6	4	16.1	27400	0	999999999	0	0	0	88	0	0	0
+241200	-21.7	-26.1	65	83080	0	0	169	0	0	0	999900	999900	999900	99990	23	2.6	6	4	16.1	27400	0	999699999	0	0	0	88	0	0	0
+244800	-21.7	-26.1	65	83080	0	0	171	0	0	0	999900	999900	999900	99990	135	2.6	7	5	16.1	27400	0	999699999	0	0	0	88	0	0	0
+248400	-20.6	-26.7	55	83050	0	0	172	0	0	0	999900	999900	999900	99990	158	4.1	7	4	16.1	27400	0	999699999	0	0	0	88	0	0	0
+252000	-20.6	-26.1	58	83080	0	0	172	0	0	0	999900	999900	999900	99990	203	3.6	7	4	16.1	27400	0	999699999	0	0	0	88	0	0	0
+255600	-20.6	-25	65	83120	0	0	173	0	0	0	999900	999900	999900	99990	180	4.1	7	4	16.1	27400	0	999699999	0	0	0	88	0	0	0
+259200	-22.2	-28.3	54	83120	0	0	166	0	0	0	999900	999900	999900	99990	45	2.6	6	4	16.1	22900	0	999699999	0	0	0	88	0	0	0
+262800	-23.3	-31.1	45	83180	0	0	159	0	0	0	999900	999900	999900	99990	68	3.1	3	2	16.1	77777	0	999699999	0	0	0	88	0	0	0
+266400	-24.4	-32.8	42	83280	0	0	150	0	0	0	999900	999900	999900	99990	203	2.6	0	0	16.1	77777	0	999999999	0	0	0	88	0	0	0
+270000	-23.3	-34.4	32	83320	0	0	151	0	0	0	999900	999900	999900	99990	180	2.1	0	0	11.3	77777	0	999699999	0	0	0	88	0	0	0
+273600	-23.3	-28.9	57	83350	0	0	155	0	0	0	999900	999900	999900	99990	180	4.1	0	0	16.1	77777	0	999999999	0	0	0	88	0	0	0
+277200	-23.3	-31.7	42	83320	0	0	153	0	0	0	999900	999900	999900	99990	203	4.6	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
+280800	-23.3	-32.8	38	83350	0	0	152	0	0	0	999900	999900	999900	99990	180	3.6	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
+284400	-23.3	-31.7	42	83420	0	0	153	0	0	0	999900	999900	999900	99990	180	4.1	0	0	96.6	77777	0	999999999	0	0	0	88	0	0	0
+288000	-23.9	-28.9	60	83560	0	0	154	22	61	22	999900	999900	999900	99990	180	1.5	0	0	96.6	77777	0	999999999	0	0	0	88	0	0	0
+291600	-22.8	-27.8	61	83620	135	635	157	137	374	101	999900	999900	999900	99990	45	2.1	0	0	96.6	77777	0	999699999	0	0	0	88	0	0	0
+295200	-20	-28.3	44	83660	346	774	164	249	547	116	999900	999900	999900	99990	113	2.6	0	0	96.6	77777	0	999699999	0	0	0	88	0	0	0
+298800	-16.7	-23.3	53	83620	509	879	176	427	932	92	999900	999900	999900	99990	203	2.6	0	0	96.6	77777	0	999999999	0	0	0	88	0	0	0
+302400	-16.1	-22.8	53	83560	614	945	178	484	964	67	999900	999900	999900	99990	360	4.6	0	0	32.2	77777	0	999999999	0	0	0	88	0	0	0
+306000	-15	-21.1	56	83560	653	969	183	488	964	44	999900	999900	999900	99990	45	3.1	0	0	8	77777	0	999999909	0	0	0	88	0	0	0
+309600	-11.7	-21.7	39	83520	624	950	192	430	938	18	999900	999900	999900	99990	45	4.6	0	0	11.3	77777	0	999999999	0	0	0	88	0	0	0
+313200	-12.8	-20	51	83520	528	891	190	320	857	1	999900	999900	999900	99990	45	2.1	0	0	11.3	77777	0	999999999	0	0	0	88	0	0	0
+316800	-14.4	-20	59	83520	372	791	185	175	682	0	999900	999900	999900	99990	360	5.1	0	0	11.3	77777	0	999999999	0	0	0	88	0	0	0
+320400	-16.7	-22.8	56	83560	166	656	177	24	116	11	999900	999900	999900	99990	23	4.6	0	0	16.1	77777	0	999999999	0	0	0	88	0	0	0
+324000	-20	-26.1	55	83560	0	0	165	0	0	0	999900	999900	999900	99990	360	3.1	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
+327600	-20	-25	61	83560	0	0	166	0	0	0	999900	999900	999900	99990	135	2.1	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
+331200	-19.4	-24.4	61	83560	0	0	168	0	0	0	999900	999900	999900	99990	180	2.6	0	0	16.1	77777	0	999999999	0	0	0	88	0	0	0
+334800	-20	-26.1	55	83490	0	0	174	0	0	0	999900	999900	999900	99990	203	4.1	4	4	3.2	77777	0	999999909	0	0	0	88	0	0	0
+338400	-19.4	-25	58	83490	0	0	176	0	0	0	999900	999900	999900	99990	203	5.1	4	4	6.4	77777	0	999999909	0	0	0	88	0	0	0
+342000	-18.9	-25	55	83450	0	0	176	0	0	0	999900	999900	999900	99990	225	2.6	3	3	8	77777	0	999999909	0	0	0	88	0	0	0
+345600	-18.9	-21.7	76	83420	0	0	171	0	0	0	999900	999900	999900	99990	180	2.6	0	0	11.3	77777	0	999999999	0	0	0	88	0	0	0
+349200	-17.8	-22.2	66	83350	0	0	174	0	0	0	999900	999900	999900	99990	203	4.6	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
+352800	-18.3	-22.8	65	83450	0	0	172	0	0	0	999900	999900	999900	99990	180	2.6	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
+356400	-16.1	-22.8	53	83390	0	0	178	0	0	0	999900	999900	999900	99990	180	6.7	0	0	24.1	77777	0	999999999	0	0	0	88	0	0	0
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+31446000	-6.7	-11.7	64	83830	0	0	215	0	0	0	999900	999900	999900	99990	220	3.1	0	0	32.2	77777	0	999999999	0	0	0	88	0	0	0
+31449600	-7	-12.3	63	83790	0	0	214	0	0	0	999900	999900	999900	99990	210	3.6	0	0	32.2	77777	9	999999999	0	0	0	88	0	0	0
+31453200	-7.3	-13.1	60	83760	0	0	212	0	0	0	999900	999900	999900	99990	200	4.1	0	0	32.2	77777	9	999999999	0	0	0	88	0	0	0
+31456800	-7.8	-13.9	58	83720	0	0	210	0	0	0	999900	999900	999900	99990	190	4.6	0	0	32.2	77777	0	999999999	0	0	0	88	0	0	0
+31460400	-7.5	-14.5	53	83670	0	0	210	0	0	0	999900	999900	999900	99990	187	5.1	0	0	32.2	77777	9	999999999	0	0	0	88	0	0	0
+31464000	-7.3	-15.3	49	83610	0	0	210	0	0	0	999900	999900	999900	99990	183	5.7	0	0	32.2	77777	9	999999999	0	0	0	88	0	0	0
+31467600	-7.2	-16.1	45	83560	0	0	210	0	0	0	999900	999900	999900	99990	180	6.2	0	0	32.2	77777	0	999999999	0	0	0	88	0	0	0
+31471200	-6.2	-16.6	39	83500	0	0	213	0	0	0	999900	999900	999900	99990	180	6.5	0	0	32.2	77777	9	999999999	0	0	0	88	0	0	0
+31474800	-5.2	-17.1	34	83450	0	0	216	0	0	0	999900	999900	999900	99990	180	6.9	0	0	32.2	77777	9	999999999	0	0	0	88	0	0	0
+31478400	-4.4	-17.8	30	83390	0	0	222	18	36	18	999900	999900	999900	99990	180	7.2	2	1	96.6	77777	0	999999999	0	0	0	88	0	0	0
+31482000	-0.1	-17.9	21	83370	136	636	236	164	644	103	999900	999900	999900	99990	190	7.4	2	1	96.6	77777	9	999999999	0	0	0	88	0	0	0
+31485600	4.1	-18	15	83340	345	774	251	303	820	104	999900	999900	999900	99990	200	7.5	2	1	96.6	77777	9	999999999	0	0	0	88	0	0	0
+31489200	8.3	-18.3	11	83320	506	877	266	408	898	88	999900	999900	999900	99990	210	7.7	2	1	96.6	77777	0	999999999	0	0	0	88	0	0	0
+31492800	9.6	-19.9	9	83250	608	941	269	461	925	64	999900	999900	999900	99990	257	6	2	1	96.6	77777	9	999999999	0	0	0	88	0	0	0
+31496400	10.9	-21.5	7	83190	644	963	272	461	926	41	999900	999900	999900	99990	303	4.3	2	1	96.6	77777	9	999999999	0	0	0	88	0	0	0
+31500000	12.2	-23.3	5	83120	612	943	279	403	887	20	999900	999900	999900	99990	350	2.6	5	2	96.6	77777	0	999999999	0	0	0	88	0	0	0
+31503600	9.6	-19.9	9	83170	514	882	273	301	813	6	999900	999900	999900	99990	10	2.6	5	2	96.6	77777	9	999999999	0	0	0	88	0	0	0
+31507200	7	-16.5	14	83230	356	781	267	164	642	3	999900	999900	999900	99990	30	2.6	5	2	96.6	77777	9	999999999	0	0	0	88	0	0	0
+31510800	4.4	-13.3	23	83280	150	645	257	20	58	14	999900	999900	999900	99990	50	2.6	9	1	96.6	77777	0	999999999	0	0	0	88	0	0	0
+31514400	3.7	-13	25	83260	0	0	255	0	0	0	999900	999900	999900	99990	100	3.1	9	1	96.6	77777	9	999999999	0	0	0	88	0	0	0
+31518000	3.3	-12.5	27	83220	0	0	254	0	0	0	999900	999900	999900	99990	150	4.8	9	1	96.6	77777	9	999999999	0	0	0	88	0	0	0
+31521600	2.1	-12.9	28	83250	0	0	259	0	0	0	999900	999900	999900	99990	200	3.3	10	5	32.2	77777	0	999999999	0	0	0	88	0	0	0
+31525200	1.1	-13.3	29	83240	0	0	254	0	0	0	999900	999900	999900	99990	170	2.2	10	5	32.2	77777	9	999999999	0	0	0	88	0	0	0
+31528800	0.3	-13.4	31	83200	0	0	251	0	0	0	999900	999900	999900	99990	140	1.7	10	5	32.2	77777	9	999999999	0	0	0	88	0	0	0
+31532400	-0.3	-13.6	32	83120	0	0	247	0	0	0	999900	999900	999900	99990	110	1.6	8	4	32.2	36600	0	999999999	0	0	0	88	0	0	0
+31536000	-0.7	-14	31	83000	0	0	245	0	0	0	999900	999900	999900	99990	110	2.1	8	4	32.2	36600	9	999999999	0	0	0	88	0	0	0
\ No newline at end of file
diff --git a/AixLib/Resources/weatherdata/WeatherData_Ashrae140_LOM.mat b/AixLib/Resources/weatherdata/WeatherData_Ashrae140_LOM.mat
deleted file mode 100644
index 7c1bff546a..0000000000
Binary files a/AixLib/Resources/weatherdata/WeatherData_Ashrae140_LOM.mat and /dev/null differ
diff --git a/AixLib/Resources/weatherdata/WeatherData_Ashrae140_LOM.txt b/AixLib/Resources/weatherdata/WeatherData_Ashrae140_LOM.txt
new file mode 100644
index 0000000000..32a68233f7
--- /dev/null
+++ b/AixLib/Resources/weatherdata/WeatherData_Ashrae140_LOM.txt
@@ -0,0 +1,8763 @@
+#1
+double Table(8760, 4)
+#time_in_s	1	2	3
+0.0	273.15	244.19644451041293	-310.6361417552372
+3600.0	273.15	245.13875446322317	-310.7021034519339
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+31532400.0	272.45	235.40778499537763	-307.0234448388947
diff --git a/AixLib/Resources/weatherdata/Weatherdata_ASHARE140.mat b/AixLib/Resources/weatherdata/Weatherdata_ASHARE140.mat
deleted file mode 100644
index dda89908b2..0000000000
Binary files a/AixLib/Resources/weatherdata/Weatherdata_ASHARE140.mat and /dev/null differ
diff --git a/AixLib/Resources/weatherdata/Weatherdata_ASHARE140.txt b/AixLib/Resources/weatherdata/Weatherdata_ASHARE140.txt
new file mode 100644
index 0000000000..ecd2111a9e
--- /dev/null
+++ b/AixLib/Resources/weatherdata/Weatherdata_ASHARE140.txt
@@ -0,0 +1,8764 @@
+#1
+double Table(8761, 7)
+#time_in_s	1	2	3	4	5	6
+0.0	0.0	0.0	273.15	2.8	266.54999999999995	0.3
+3600.0	0.0	0.0	273.15	2.8	266.54999999999995	0.3
+7200.0	0.0	0.0	273.15	3.3	267.04999999999995	0.4
+10800.0	0.0	0.0	273.15	3.7	266.45	0.4
+14400.0	0.0	0.0	273.15	4.1	266.45	0.4
+18000.0	0.0	0.0	273.15	4.6	266.54999999999995	0.5
+21600.0	0.0	0.0	273.15	5.0	264.25	0.7
+25200.0	0.0	0.0	276.45	3.1	266.45	0.6
+28800.0	2.2222222222222223	6.944444444444445	275.34999999999997	4.1	267.04999999999995	1.0
+32400.0	67.5	93.33333333333333	276.45	3.1	268.15	0.9
+36000.0	16.11111111111111	116.66666666666667	280.34999999999997	9.8	264.25	1.0
+39600.0	746.1111111111111	356.6666666666667	280.95	10.3	262.54999999999995	0.6
+43200.0	932.5	465.55555555555554	282.04999999999995	9.3	264.25	0.1
+46800.0	939.7222222222222	468.8888888888889	282.54999999999995	9.3	264.25	0.1
+50400.0	934.7222222222222	424.44444444444446	283.75	9.3	262.54999999999995	0.0
+54000.0	826.1111111111111	306.3888888888889	283.15	4.6	262.54999999999995	0.1
+57600.0	671.3888888888889	171.11111111111111	282.54999999999995	8.8	263.75	0.0
+61200.0	79.16666666666667	21.38888888888889	279.84999999999997	7.7	262.04999999999995	0.0
+64800.0	0.0	0.0	278.75	4.6	261.45	0.0
+68400.0	0.0	0.0	275.95	1.5	263.15	0.0
+72000.0	0.0	0.0	275.34999999999997	3.1	263.15	0.0
+75600.0	0.0	0.0	274.84999999999997	2.1	261.45	0.1
+79200.0	0.0	0.0	273.75	2.6	261.45	0.4
+82800.0	0.0	0.0	273.15	9.3	263.75	0.4
+86400.0	0.0	0.0	268.75	7.7	265.95	1.0
+90000.0	0.0	0.0	267.54999999999995	7.7	264.84999999999997	1.0
+93600.0	0.0	0.0	265.95	8.2	261.45	1.0
+97200.0	0.0	0.0	264.25	6.2	260.95	1.0
+100800.0	0.0	0.0	263.75	6.2	260.95	1.0
+104400.0	0.0	0.0	262.54999999999995	5.7	259.84999999999997	1.0
+108000.0	0.0	0.0	261.45	5.1	258.15	1.0
+111600.0	0.0	0.0	260.95	6.2	258.75	1.0
+115200.0	0.2777777777777778	3.0555555555555554	260.95	6.7	257.54999999999995	1.0
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+31017600.0	0.0	0.0	279.84999999999997	4.1	271.45	0.4
+31021200.0	0.0	0.0	279.04999999999995	4.3	271.15	0.4
+31024800.0	0.0	0.0	278.34999999999997	4.4	270.84999999999997	0.4
+31028400.0	0.0	0.0	277.54999999999995	4.6	270.34999999999997	0.4
+31032000.0	0.0	0.0	277.34999999999997	4.4	270.04999999999995	0.4
+31035600.0	0.0	0.0	277.25	4.3	269.75	0.4
+31039200.0	0.0	0.0	277.04999999999995	4.1	269.25	0.5
+31042800.0	0.0	0.0	278.54999999999995	4.8	269.95	0.5
+31046400.0	9.166666666666666	12.5	279.95	5.5	270.45	0.5
+31050000.0	481.1111111111111	139.72222222222223	281.45	6.2	270.95	0.6
+31053600.0	570.5555555555555	243.05555555555554	280.15	5.8	271.04999999999995	0.6
+31057200.0	544.7222222222222	305.0	278.84999999999997	5.5	271.04999999999995	0.6
+31060800.0	433.6111111111111	320.8333333333333	277.54999999999995	5.1	270.95	0.8
+31064400.0	650.2777777777778	364.1666666666667	278.34999999999997	4.6	271.25	0.8
+31068000.0	758.3333333333334	355.55555555555554	279.04999999999995	4.1	271.34999999999997	0.8
+31071600.0	784.4444444444445	289.72222222222223	279.84999999999997	3.6	271.45	0.3
+31075200.0	592.2222222222222	155.27777777777777	278.95	3.9	271.75	0.3
+31078800.0	30.0	16.11111111111111	277.95	4.3	271.95	0.3
+31082400.0	0.0	0.0	277.04999999999995	4.6	272.04999999999995	0.8
+31086000.0	0.0	0.0	276.65	3.9	272.15	0.8
+31089600.0	0.0	0.0	276.34999999999997	3.3	272.15	0.8
+31093200.0	0.0	0.0	275.95	2.6	272.04999999999995	0.8
+31096800.0	0.0	0.0	274.04999999999995	3.4	271.45	0.8
+31100400.0	0.0	0.0	272.34999999999997	4.3	270.65	0.8
+31104000.0	0.0	0.0	270.34999999999997	5.1	269.84999999999997	1.0
+31107600.0	0.0	0.0	270.04999999999995	4.3	269.75	1.0
+31111200.0	0.0	0.0	269.75	3.4	269.54999999999995	1.0
+31114800.0	0.0	0.0	269.25	2.6	269.25	1.0
+31118400.0	0.0	0.0	270.04999999999995	2.9	269.95	1.0
+31122000.0	0.0	0.0	270.84999999999997	3.3	270.45	1.0
+31125600.0	0.0	0.0	271.45	3.6	270.95	1.0
+31129200.0	0.0	0.0	271.75	3.1	271.45	1.0
+31132800.0	12.222222222222221	13.61111111111111	271.95	2.6	271.75	1.0
+31136400.0	533.8888888888889	147.5	272.04999999999995	2.1	272.04999999999995	0.5
+31140000.0	771.6666666666666	285.55555555555554	274.25	2.8	271.04999999999995	0.5
+31143600.0	885.8333333333334	400.27777777777777	276.54999999999995	3.4	269.95	0.5
+31147200.0	957.5	472.5	278.75	4.1	268.75	0.0
+31150800.0	962.2222222222222	475.8333333333333	279.65	5.3	265.65	0.0
+31154400.0	929.7222222222222	418.05555555555554	280.54999999999995	6.5	262.54999999999995	0.0
+31158000.0	844.4444444444445	309.44444444444446	281.45	7.7	259.25	0.0
+31161600.0	658.0555555555555	166.11111111111111	279.45	6.3	260.25	0.0
+31165200.0	44.44444444444444	17.77777777777778	277.34999999999997	5.0	261.25	0.0
+31168800.0	0.0	0.0	275.34999999999997	3.6	262.04999999999995	0.0
+31172400.0	0.0	0.0	274.04999999999995	3.8	262.54999999999995	0.0
+31176000.0	0.0	0.0	272.84999999999997	3.9	262.84999999999997	0.0
+31179600.0	0.0	0.0	271.45	4.1	263.15	0.1
+31183200.0	0.0	0.0	270.65	3.6	263.65	0.1
+31186800.0	0.0	0.0	269.75	3.1	263.95	0.1
+31190400.0	0.0	0.0	268.75	2.6	264.25	0.1
+31194000.0	0.0	0.0	268.25	2.4	264.65	0.1
+31197600.0	0.0	0.0	267.54999999999995	2.1	264.84999999999997	0.2
+31201200.0	0.0	0.0	266.95	2.4	264.75	0.2
+31204800.0	0.0	0.0	266.15	2.8	264.54999999999995	0.2
+31208400.0	0.0	0.0	265.34999999999997	3.1	264.25	0.2
+31212000.0	0.0	0.0	264.95	2.1	263.45	0.2
+31215600.0	0.0	0.0	264.34999999999997	1.0	262.45	0.2
+31219200.0	17.5	15.277777777777779	263.75	0.0	261.45	0.1
+31222800.0	644.1666666666666	163.33333333333334	269.75	2.9	262.84999999999997	0.1
+31226400.0	832.7777777777778	306.1111111111111	275.54999999999995	5.9	264.15	0.1
+31230000.0	923.8888888888889	416.3888888888889	281.45	8.8	265.34999999999997	0.0
+31233600.0	947.7777777777778	468.8888888888889	282.75	8.4	264.34999999999997	0.0
+31237200.0	946.1111111111111	468.05555555555554	284.04999999999995	8.1	263.25	0.0
+31240800.0	901.6666666666666	407.22222222222223	285.34999999999997	7.7	262.04999999999995	0.1
+31244400.0	813.6111111111111	299.72222222222223	283.65	5.6	261.95	0.1
+31248000.0	623.0555555555555	160.27777777777777	282.04999999999995	3.6	261.75	0.1
+31251600.0	39.166666666666664	17.5	280.34999999999997	1.5	261.45	0.2
+31255200.0	0.0	0.0	278.34999999999997	1.5	262.15	0.2
+31258800.0	0.0	0.0	276.25	1.5	262.65	0.2
+31262400.0	0.0	0.0	274.25	1.5	263.15	0.0
+31266000.0	0.0	0.0	273.65	2.7	263.95	0.0
+31269600.0	0.0	0.0	273.15	3.9	264.75	0.0
+31273200.0	0.0	0.0	272.54999999999995	5.1	265.34999999999997	0.0
+31276800.0	0.0	0.0	271.75	4.4	265.25	0.0
+31280400.0	0.0	0.0	270.84999999999997	3.8	265.15	0.0
+31284000.0	0.0	0.0	269.84999999999997	3.1	264.84999999999997	0.1
+31287600.0	0.0	0.0	269.54999999999995	2.6	265.15	0.1
+31291200.0	0.0	0.0	269.25	2.0	265.25	0.1
+31294800.0	0.0	0.0	268.75	1.5	265.34999999999997	0.3
+31298400.0	0.0	0.0	268.65	1.7	264.95	0.3
+31302000.0	0.0	0.0	268.45	1.9	264.34999999999997	0.3
+31305600.0	18.61111111111111	15.0	268.15	2.1	263.75	0.4
+31309200.0	587.5	155.83333333333334	271.25	2.9	264.75	0.4
+31312800.0	789.4444444444445	291.94444444444446	274.04999999999995	3.8	265.65	0.4
+31316400.0	878.0555555555555	398.05555555555554	277.04999999999995	4.6	266.45	0.2
+31320000.0	905.0	450.0	277.95	6.5	263.25	0.2
+31323600.0	906.6666666666666	450.8333333333333	278.95	8.4	259.84999999999997	0.2
+31327200.0	868.8888888888889	394.1666666666667	279.84999999999997	10.3	256.45	0.3
+31330800.0	808.3333333333334	298.3333333333333	278.34999999999997	8.4	257.45	0.3
+31334400.0	648.6111111111111	164.44444444444446	276.84999999999997	6.5	258.45	0.3
+31338000.0	57.22222222222222	18.88888888888889	275.34999999999997	4.6	259.25	0.0
+31341600.0	0.0	0.0	274.04999999999995	3.1	259.75	0.0
+31345200.0	0.0	0.0	272.84999999999997	1.5	260.04999999999995	0.0
+31348800.0	0.0	0.0	271.45	0.0	260.34999999999997	0.3
+31352400.0	0.0	0.0	270.84999999999997	0.9	260.45	0.3
+31356000.0	0.0	0.0	270.04999999999995	1.7	260.45	0.3
+31359600.0	0.0	0.0	269.25	2.6	260.34999999999997	0.3
+31363200.0	0.0	0.0	269.95	2.9	260.65	0.3
+31366800.0	0.0	0.0	270.45	3.3	260.84999999999997	0.3
+31370400.0	0.0	0.0	270.95	3.6	260.95	0.1
+31374000.0	0.0	0.0	268.84999999999997	3.3	260.84999999999997	0.1
+31377600.0	0.0	0.0	266.54999999999995	2.9	260.65	0.1
+31381200.0	0.0	0.0	264.25	2.6	260.34999999999997	0.0
+31384800.0	0.0	0.0	265.45	2.6	260.25	0.0
+31388400.0	0.0	0.0	266.54999999999995	2.6	260.15	0.0
+31392000.0	25.27777777777778	16.11111111111111	267.54999999999995	2.6	259.84999999999997	0.3
+31395600.0	558.6111111111111	152.77777777777777	269.84999999999997	3.3	260.84999999999997	0.3
+31399200.0	704.1666666666666	272.5	272.15	3.9	261.75	0.3
+31402800.0	742.2222222222222	353.8888888888889	274.25	4.6	262.54999999999995	0.6
+31406400.0	837.2222222222222	419.44444444444446	274.95	6.0	261.54999999999995	0.6
+31410000.0	881.1111111111111	439.72222222222223	275.75	7.4	260.45	0.6
+31413600.0	885.2777777777778	401.6666666666667	276.45	8.8	259.25	0.2
+31417200.0	820.2777777777778	302.77777777777777	275.34999999999997	6.9	259.34999999999997	0.2
+31420800.0	654.1666666666666	166.11111111111111	274.25	5.0	259.34999999999997	0.2
+31424400.0	62.77777777777778	19.72222222222222	273.15	3.1	259.25	0.0
+31428000.0	0.0	0.0	271.95	2.8	260.04999999999995	0.0
+31431600.0	0.0	0.0	270.65	2.4	260.84999999999997	0.0
+31435200.0	0.0	0.0	269.25	2.1	261.45	0.1
+31438800.0	0.0	0.0	268.45	2.4	261.54999999999995	0.1
+31442400.0	0.0	0.0	267.45	2.8	261.54999999999995	0.1
+31446000.0	0.0	0.0	266.45	3.1	261.45	0.0
+31449600.0	0.0	0.0	266.15	3.6	260.84999999999997	0.0
+31453200.0	0.0	0.0	265.84999999999997	4.1	260.04999999999995	0.0
+31456800.0	0.0	0.0	265.34999999999997	4.6	259.25	0.0
+31460400.0	0.0	0.0	265.65	5.1	258.65	0.0
+31464000.0	0.0	0.0	265.84999999999997	5.7	257.84999999999997	0.0
+31467600.0	0.0	0.0	265.95	6.2	257.04999999999995	0.0
+31471200.0	0.0	0.0	266.95	6.5	256.54999999999995	0.0
+31474800.0	0.0	0.0	267.95	6.9	256.04999999999995	0.0
+31478400.0	36.111111111111114	17.5	268.75	7.2	255.34999999999997	0.1
+31482000.0	644.1666666666666	164.44444444444446	273.04999999999995	7.4	255.24999999999997	0.1
+31485600.0	820.0	303.3333333333333	277.25	7.5	255.14999999999998	0.1
+31489200.0	898.3333333333334	408.05555555555554	281.45	7.7	254.84999999999997	0.1
+31492800.0	925.0	460.8333333333333	282.75	6.0	253.24999999999997	0.1
+31496400.0	925.5555555555555	461.1111111111111	284.04999999999995	4.3	251.64999999999998	0.1
+31500000.0	886.6666666666666	403.05555555555554	285.34999999999997	2.6	249.84999999999997	0.2
+31503600.0	813.3333333333334	301.1111111111111	282.75	2.6	253.24999999999997	0.2
+31507200.0	641.9444444444445	164.16666666666666	280.15	2.6	256.65	0.2
+31510800.0	58.333333333333336	19.72222222222222	277.54999999999995	2.6	259.84999999999997	0.1
+31514400.0	0.0	0.0	276.84999999999997	3.1	260.15	0.1
+31518000.0	0.0	0.0	276.45	4.8	260.65	0.1
+31521600.0	0.0	0.0	275.25	3.3	260.25	0.5
+31525200.0	0.0	0.0	274.25	2.2	259.84999999999997	0.5
+31528800.0	0.0	0.0	273.45	1.7	259.75	0.5
+31532400.0	0.0	0.0	272.84999999999997	1.6	259.54999999999995	0.4
+31536000.0	0.0	0.0	272.45	2.1	259.15	0.4
diff --git a/AixLib/Systems/HydraulicModules/BaseClasses/PumpInterface_SpeedControlledNrpm.mo b/AixLib/Systems/HydraulicModules/BaseClasses/PumpInterface_SpeedControlledNrpm.mo
index 7b1e606b2d..9a73764020 100644
--- a/AixLib/Systems/HydraulicModules/BaseClasses/PumpInterface_SpeedControlledNrpm.mo
+++ b/AixLib/Systems/HydraulicModules/BaseClasses/PumpInterface_SpeedControlledNrpm.mo
@@ -2,7 +2,9 @@
 model PumpInterface_SpeedControlledNrpm
   "Interface for the SpeedControlled_Nrpm pump model"
   extends AixLib.Systems.HydraulicModules.BaseClasses.BasicPumpInterface;
-  Fluid.Movers.SpeedControlled_Nrpm pump(
+  parameter Modelica.Units.NonSI.AngularVelocity_rpm speed_rpm_nominal=1500 "Nominal rotational speed";
+
+  Fluid.Movers.SpeedControlled_y pump(
     redeclare package Medium = Medium,
     final energyDynamics=energyDynamics,
     T_start=T_start) annotation (Dialog(enable=true), Placement(transformation(
@@ -12,13 +14,19 @@ model PumpInterface_SpeedControlledNrpm
         origin={0,36})));
   Modelica.Blocks.Sources.Constant constZero(final k=0)
     annotation (Placement(transformation(extent={{-40,60},{-19,80}})));
+
+  Modelica.Blocks.Math.Gain gaiSpe(final k=1/speed_rpm_nominal) "Pressure gain"
+    annotation (Placement(transformation(
+        extent={{10,-10},{-10,10}},
+        rotation=90,
+        origin={10,70})));
 equation
   connect(pump.port_a, port_a)
     annotation (Line(points={{-10,0},{-100,0}}, color={0,127,255}));
   connect(pump.port_b, port_b)
     annotation (Line(points={{10,0},{100,0}}, color={0,127,255}));
-  connect(pump.P, pumpBus.PelMea) annotation (Line(points={{11,9},{11,14},{22,
-          14},{22,100.5},{0.1,100.5},{0.1,100.1}}, color={0,0,127}), Text(
+  connect(pump.P, pumpBus.PelMea) annotation (Line(points={{11,9},{11,14},{22,14},
+          {22,100.5},{0.1,100.5},{0.1,100.1}}, color={0,0,127}), Text(
       string="%second",
       index=1,
       extent={{6,3},{6,3}}));
@@ -33,12 +41,16 @@ equation
       string="%second",
       index=1,
       extent={{6,3},{6,3}}));
-  connect(switchToZero.y, pump.Nrpm) annotation (Line(points={{-1.9984e-15,25},{0,25},{0,12}},   color={0,0,127}));
-  connect(switchToZero.u1, pumpBus.rpmSet) annotation (Line(points={{8,48},{8,
-          92},{0.1,92},{0.1,100.1}}, color={0,0,127}), Text(
+  connect(gaiSpe.u, pumpBus.rpmSet) annotation (Line(points={{10,82},{10,96},{
+          0.1,96},{0.1,100.1}}, color={0,0,127}), Text(
       string="%second",
       index=1,
-      extent={{6,3},{6,3}}));
+      extent={{6,3},{6,3}},
+      horizontalAlignment=TextAlignment.Left));
+  connect(switchToZero.u1, gaiSpe.y)
+    annotation (Line(points={{8,48},{8,58},{10,58},{10,59}}, color={0,0,127}));
+  connect(switchToZero.y, pump.y) annotation (Line(points={{-1.9984e-15,25},{
+          -1.9984e-15,18.5},{0,18.5},{0,12}}, color={0,0,127}));
   annotation (Documentation(revisions="<html><ul>
   <li>May 20, 2018, by Alexander Kümpel:<br/>
     First implementation.
diff --git a/AixLib/Systems/HydraulicModules/Example/Admix.mo b/AixLib/Systems/HydraulicModules/Example/Admix.mo
index 2adfcd8a08..2d665bc4ff 100644
--- a/AixLib/Systems/HydraulicModules/Example/Admix.mo
+++ b/AixLib/Systems/HydraulicModules/Example/Admix.mo
@@ -10,7 +10,7 @@ model Admix "Test for admix circuit"
     valveCharacteristic=Fluid.Actuators.Valves.Data.LinearEqualPercentage(),
     redeclare
       AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-      PumpInterface(pump(redeclare
+      PumpInterface(speed_rpm_nominal=2540, pump(redeclare
           AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 per)),
     redeclare package Medium = Medium,
     m_flow_nominal=0.1,
@@ -57,7 +57,7 @@ model Admix "Test for admix circuit"
     annotation (Placement(transformation(extent={{-100,40},{-80,60}})));
   BaseClasses.HydraulicBus hydraulicBus
     annotation (Placement(transformation(extent={{-52,0},{-32,20}})));
-  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation(
+  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation (
     Placement(visible = true, transformation(origin = {-84, -30}, extent = {{-10, -10}, {10, 10}}, rotation = 0)));
 equation
 
@@ -87,13 +87,14 @@ equation
       index=1,
       extent={{6,3},{6,3}},
       horizontalAlignment=TextAlignment.Left));
-  connect(pumpOn.y, hydraulicBus.pumpBus.onSet) annotation(
-    Line(points = {{-72, -30}, {-42, -30}, {-42, 10}}, color = {255, 0, 255}));
+  connect(pumpOn.y, hydraulicBus.pumpBus.onSet) annotation (
+    Line(points={{-73,-30},{-41.95,-30},{-41.95,10.05}},
+                                                       color = {255, 0, 255}));
   annotation (
     Icon(graphics,
          coordinateSystem(preserveAspectRatio=false)),
     Diagram(coordinateSystem(preserveAspectRatio=false)),
-    experiment(StopTime=800),
+    experiment(StopTime=800,Tolerance=1e-06),
     Documentation(revisions="<html><ul>
   <li>October 25, 2017, by Alexander Kümpel:<br/>
     Transfer from ZUGABE to AixLib.
@@ -101,6 +102,6 @@ equation
 </ul>
 </html>"),
     __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Admix.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Admix.mos"
         "Simulate and plot"));
 end Admix;
diff --git a/AixLib/Systems/HydraulicModules/Example/ERC_ExperimentalHall_CoolingCircuit.mo b/AixLib/Systems/HydraulicModules/Example/ERC_ExperimentalHall_CoolingCircuit.mo
index 79fcfad450..f1b2c7ceeb 100644
--- a/AixLib/Systems/HydraulicModules/Example/ERC_ExperimentalHall_CoolingCircuit.mo
+++ b/AixLib/Systems/HydraulicModules/Example/ERC_ExperimentalHall_CoolingCircuit.mo
@@ -80,7 +80,7 @@ model ERC_ExperimentalHall_CoolingCircuit
     parameterPipe=DataBase.Pipes.Copper.Copper_35x1(),
     redeclare
       AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-      PumpInterface(pump(redeclare
+      PumpInterface(speed_rpm_nominal=2540, pump(redeclare
           AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 per)),
     redeclare package Medium = Medium,
     m_flow_nominal=1,
@@ -89,7 +89,7 @@ model ERC_ExperimentalHall_CoolingCircuit
     pipe2(length=2),
     pipe3(length=4),
     energyDynamics=admix.energyDynamics,
-    length=2)                            annotation (Placement(transformation(
+    length=2) annotation (Placement(transformation(
         extent={{-25,-25},{25,25}},
         rotation=90,
         origin={6,4})));
@@ -98,7 +98,7 @@ model ERC_ExperimentalHall_CoolingCircuit
     valve(flowCharacteristics=AixLib.Fluid.Actuators.Valves.Data.Linear()),
     redeclare
       AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-      PumpInterface(pump(redeclare
+      PumpInterface(speed_rpm_nominal=2540, pump(redeclare
           AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 per)),
     redeclare package Medium = Medium,
     m_flow_nominal=1,
@@ -118,7 +118,7 @@ model ERC_ExperimentalHall_CoolingCircuit
     valveCharacteristic=Fluid.Actuators.Valves.Data.LinearEqualPercentage(),
     redeclare
       AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-      PumpInterface(pump(redeclare
+      PumpInterface(speed_rpm_nominal=2540, pump(redeclare
           AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 per)),
     redeclare package Medium = Medium,
     m_flow_nominal=1,
@@ -131,7 +131,7 @@ model ERC_ExperimentalHall_CoolingCircuit
     pipe6(length=1),
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     length=1,
-    Kv=10)                                                     annotation (Placement(transformation(
+    Kv=10) annotation (Placement(transformation(
         extent={{-25,-25},{25,25}},
         rotation=90,
         origin={-68,4})));
diff --git a/AixLib/Systems/HydraulicModules/Example/Injection.mo b/AixLib/Systems/HydraulicModules/Example/Injection.mo
index b4c59e981f..9b99491126 100644
--- a/AixLib/Systems/HydraulicModules/Example/Injection.mo
+++ b/AixLib/Systems/HydraulicModules/Example/Injection.mo
@@ -9,7 +9,7 @@ model Injection "Test for injection circuit"
     parameterPipe=DataBase.Pipes.Copper.Copper_35x1_5(),
     redeclare
       AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-      PumpInterface(pump(redeclare
+      PumpInterface(speed_rpm_nominal=2540, pump(redeclare
           AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 per)),
     redeclare package Medium = Medium,
     m_flow_nominal=1,
@@ -56,7 +56,7 @@ model Injection "Test for injection circuit"
         extent={{10,-10},{-10,10}},
         rotation=-90,
         origin={28,-50})));
-  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation(
+  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation (
     Placement(visible = true, transformation(origin = {-84, -30}, extent = {{-10, -10}, {10, 10}}, rotation = 0)));
 equation
 
@@ -86,8 +86,9 @@ equation
       index=1,
       extent={{6,3},{6,3}},
       horizontalAlignment=TextAlignment.Left));
-  connect(pumpOn.y, hydraulicBus.pumpBus.onSet) annotation(
-    Line(points = {{-72, -30}, {-40, -30}, {-40, 10}}, color = {255, 0, 255}));
+  connect(pumpOn.y, hydraulicBus.pumpBus.onSet) annotation (
+    Line(points={{-73,-30},{-39.95,-30},{-39.95,10.05}},
+                                                       color = {255, 0, 255}));
                            annotation (Placement(transformation(
         extent={{-24,-24},{24,24}},
         rotation=90,
@@ -95,7 +96,7 @@ equation
     Icon(graphics,
          coordinateSystem(preserveAspectRatio=false)),
     Diagram(coordinateSystem(preserveAspectRatio=false)),
-    experiment(StopTime=800),
+    experiment(StopTime=800,Tolerance=1e-06),
     Documentation(revisions="<html><ul>
   <li>October 25, 2017, by Alexander Kümpel:<br/>
     Transfer from ZUGABE to AixLib.
@@ -103,6 +104,6 @@ equation
 </ul>
 </html>"),
     __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection.mos"
         "SImulate and plot"));
 end Injection;
diff --git a/AixLib/Systems/HydraulicModules/Example/Injection2WayValve.mo b/AixLib/Systems/HydraulicModules/Example/Injection2WayValve.mo
index 302222cb2e..e3af7e9f85 100644
--- a/AixLib/Systems/HydraulicModules/Example/Injection2WayValve.mo
+++ b/AixLib/Systems/HydraulicModules/Example/Injection2WayValve.mo
@@ -9,7 +9,7 @@ model Injection2WayValve "Test for injection circuit with a 2 way valve"
     parameterPipe=DataBase.Pipes.Copper.Copper_28x1(),
     redeclare
       AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-      PumpInterface(pump(redeclare
+      PumpInterface(speed_rpm_nominal=2540, pump(redeclare
           AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 per)),
     redeclare package Medium = Medium,
     m_flow_nominal=1,
@@ -54,7 +54,7 @@ model Injection2WayValve "Test for injection circuit with a 2 way valve"
         extent={{10,-10},{-10,10}},
         rotation=-90,
         origin={28,-50})));
-  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation(
+  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation (
     Placement(visible = true, transformation(origin = {-84, -30}, extent = {{-10, -10}, {10, 10}}, rotation = 0)));
 equation
 
@@ -84,8 +84,9 @@ equation
       index=1,
       extent={{6,3},{6,3}},
       horizontalAlignment=TextAlignment.Left));
-  connect(pumpOn.y, hydraulicBus.pumpBus.onSet) annotation(
-    Line(points = {{-72, -30}, {-40, -30}, {-40, 10}}, color = {255, 0, 255}));
+  connect(pumpOn.y, hydraulicBus.pumpBus.onSet) annotation (
+    Line(points={{-73,-30},{-39.95,-30},{-39.95,10.05}},
+                                                       color = {255, 0, 255}));
                            annotation (Placement(transformation(
         extent={{-24,-24},{24,24}},
         rotation=90,
@@ -93,7 +94,7 @@ equation
     Icon(graphics,
          coordinateSystem(preserveAspectRatio=false)),
     Diagram(coordinateSystem(preserveAspectRatio=false)),
-    experiment(StopTime=800),
+    experiment(StopTime=800,Tolerance=1e-06),
     Documentation(revisions="<html><ul>
   <li>October 25, 2017, by Alexander Kümpel:<br/>
     Transfer from ZUGABE to AixLib.
@@ -101,6 +102,6 @@ equation
 </ul>
 </html>"),
     __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection2WayValve.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Injection2WayValve.mos"
         "SImulate and plot"));
 end Injection2WayValve;
diff --git a/AixLib/Systems/HydraulicModules/Example/Pump.mo b/AixLib/Systems/HydraulicModules/Example/Pump.mo
index dd4236d5ba..9976e4dc88 100644
--- a/AixLib/Systems/HydraulicModules/Example/Pump.mo
+++ b/AixLib/Systems/HydraulicModules/Example/Pump.mo
@@ -10,7 +10,7 @@ model Pump "Test for unmixed pump circuit"
     parameterPipe=DataBase.Pipes.Copper.Copper_35x1(),
     redeclare
       AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-      PumpInterface(pump(redeclare
+      PumpInterface(speed_rpm_nominal=2540, pump(redeclare
           AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 per)),
     redeclare package Medium = Medium,
     m_flow_nominal=1,
@@ -54,7 +54,7 @@ model Pump "Test for unmixed pump circuit"
         extent={{10,-10},{-10,10}},
         rotation=-90,
         origin={28,-50})));
-  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation(
+  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation (
     Placement(visible = true, transformation(origin = {-86, -28}, extent = {{-10, -10}, {10, 10}}, rotation = 0)));
 equation
   connect(Unmixed.hydraulicBus, hydraulicBus) annotation (Line(
@@ -87,7 +87,7 @@ equation
             -100},{120,100}})),                                  Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}})),
-    experiment(StopTime=800,Interval = 5),
+    experiment(StopTime=800,Interval = 5,Tolerance=1e-06),
     Documentation(revisions="<html><ul>
   <li>December 06, 2022, by EBC-Modelica group:<br/>
     Fixes to increase compatability to OpenModelica <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1378\">#1378</a>.
@@ -98,6 +98,6 @@ equation
 </ul>
 </html>"),
     __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Pump.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Pump.mos"
         "Simulate and plot"));
 end Pump;
diff --git a/AixLib/Systems/HydraulicModules/Example/Throttle.mo b/AixLib/Systems/HydraulicModules/Example/Throttle.mo
index 3b42a462a8..a88d7275fd 100644
--- a/AixLib/Systems/HydraulicModules/Example/Throttle.mo
+++ b/AixLib/Systems/HydraulicModules/Example/Throttle.mo
@@ -75,7 +75,7 @@ equation
             -100},{120,100}})),                                  Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}})),
-    experiment(StopTime=1000),
+    experiment(StopTime=1000,Tolerance=1e-06),
     Documentation(revisions="<html><ul>
   <li>October 25, 2017, by Alexander Kümpel:<br/>
     Transfer from ZUGABE to AixLib.
@@ -83,6 +83,6 @@ equation
 </ul>
 </html>"),
     __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Throttle.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/Throttle.mos"
         "Simulate and plot"));
 end Throttle;
diff --git a/AixLib/Systems/HydraulicModules/Example/ThrottlePump.mo b/AixLib/Systems/HydraulicModules/Example/ThrottlePump.mo
index fc80aae3cc..6b009ac567 100644
--- a/AixLib/Systems/HydraulicModules/Example/ThrottlePump.mo
+++ b/AixLib/Systems/HydraulicModules/Example/ThrottlePump.mo
@@ -9,7 +9,7 @@ model ThrottlePump "Test for unmixed throttle and pump circuit"
     parameterPipe=DataBase.Pipes.Copper.Copper_40x1(),
     redeclare
       AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-      PumpInterface(pump(redeclare
+      PumpInterface(speed_rpm_nominal=2540, pump(redeclare
           AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to6 per)),
     redeclare package Medium = Medium,
     m_flow_nominal=1,
@@ -53,7 +53,7 @@ model ThrottlePump "Test for unmixed throttle and pump circuit"
         extent={{10,-10},{-10,10}},
         rotation=-90,
         origin={28,-50})));
-  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation(
+  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation (
     Placement(visible = true, transformation(origin = {-86, -30}, extent = {{-10, -10}, {10, 10}}, rotation = 0)));
 equation
   connect(ThrottlePump.hydraulicBus, hydraulicBus) annotation (Line(
@@ -90,7 +90,7 @@ equation
             -100},{120,100}})),                                  Diagram(
         coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}})),
-    experiment(StopTime=600),
+    experiment(StopTime=600,Tolerance=1e-06),
     Documentation(revisions="<html><ul>
   <li>December 06, 2022, by EBC-Modelica group:<br/>
     Fixes to increase compatability to OpenModelica <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1378\">#1378</a>.
@@ -101,6 +101,6 @@ equation
 </ul>
 </html>"),
     __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/ThrottlePump.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/HydraulicModules/Examples/ThrottlePump.mos"
         "Simulate and plot"));
 end ThrottlePump;
diff --git a/AixLib/Systems/ModularAHU/BaseClasses/package.order b/AixLib/Systems/ModularAHU/BaseClasses/package.order
index e2afd23792..fc4962890a 100644
--- a/AixLib/Systems/ModularAHU/BaseClasses/package.order
+++ b/AixLib/Systems/ModularAHU/BaseClasses/package.order
@@ -1,2 +1,2 @@
-RegisterBus
 GenericAHUBus
+RegisterBus
diff --git a/AixLib/Systems/ModularAHU/Controller/package.order b/AixLib/Systems/ModularAHU/Controller/package.order
index f13cde5825..91bc57985d 100644
--- a/AixLib/Systems/ModularAHU/Controller/package.order
+++ b/AixLib/Systems/ModularAHU/Controller/package.order
@@ -1,3 +1,3 @@
-CtrRegBasic
 CtrAHUBasic
 CtrAHUCO2
+CtrRegBasic
diff --git a/AixLib/Systems/ModularAHU/Examples/Cooler.mo b/AixLib/Systems/ModularAHU/Examples/Cooler.mo
index 041619c466..88ffd63a35 100644
--- a/AixLib/Systems/ModularAHU/Examples/Cooler.mo
+++ b/AixLib/Systems/ModularAHU/Examples/Cooler.mo
@@ -14,20 +14,23 @@ model Cooler "Cooler register example"
       Kv=6.3,
       redeclare
         AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-        PumpInterface(pump(redeclare
+        PumpInterface(speed_rpm_nominal=2900, pump(redeclare
             AixLib.Fluid.Movers.Data.Pumps.Wilo.VeroLine50slash150dash4slash2
             per))),
     redeclare package Medium2 = MediumWater,
     redeclare package Medium1 = MediumAir,
-    T_amb=293.15,T_start=297.15,
+    T_amb=293.15,
+    T_start=297.15,
     dynamicHX(
       Q_nom=30000,
-      dT_nom=20,dp1_nominal=100,
+      dT_nom=20,
+      dp1_nominal=100,
       dp2_nominal=6000),
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial,
     hydraulicModuleIcon="ThrottlePump",
     m1_flow_nominal=1,
-    m2_flow_nominal=0.1, massDynamics = Modelica.Fluid.Types.Dynamics.SteadyStateInitial)
+    m2_flow_nominal=0.1,
+    massDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial)
     annotation (Placement(transformation(extent={{-40,-46},{26,40}})));
 
   Fluid.Sources.Boundary_pT boundaryWaterSource(
@@ -96,8 +99,5 @@ equation
     First implementation.
   </li>
 </ul>
-</html>"), experiment(StopTime=3600),
-    __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/ModularAHU/Examples/Heater.mos"
-        "Simulate and plot"));
+</html>"), experiment(StopTime=3600,Tolerance=1e-06));
 end Cooler;
diff --git a/AixLib/Systems/ModularAHU/Examples/DemandControlledAHU.mo b/AixLib/Systems/ModularAHU/Examples/DemandControlledAHU.mo
index 755e3a95e3..2afbd22913 100644
--- a/AixLib/Systems/ModularAHU/Examples/DemandControlledAHU.mo
+++ b/AixLib/Systems/ModularAHU/Examples/DemandControlledAHU.mo
@@ -122,8 +122,9 @@ model DemandControlledAHU "Example for air handling unit with demand controlled
     annotation (Placement(transformation(extent={{-58,-34},{62,32}})));
   ThermalZones.ReducedOrder.ThermalZone.ThermalZone thermalZone(
     redeclare package Medium = MediumAir,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     final C_start={CO2Con_start/1E6 * (MolCO2/MolAir)},
-    zoneParam=AixLib.DataBase.ThermalZones.Office_1995_1000(),
+ redeclare AixLib.DataBase.ThermalZones.Office_1995_1000 zoneParam,
     use_C_flow=true,
     use_moisture_balance=true,
     internalGainsMode=3,
@@ -176,7 +177,8 @@ model DemandControlledAHU "Example for air handling unit with demand controlled
   Fluid.Sources.Outside out(
     C={6.8355*0.0001},      nPorts=1, redeclare package Medium = MediumAir) annotation (Placement(transformation(extent={{-90,-14},
             {-70,6}})));
-  Fluid.Sources.Boundary_pT boundaryExhaustAir(nPorts=1, redeclare package Medium = MediumAir)
+  Fluid.Sources.Boundary_pT boundaryExhaustAir(nPorts=1, redeclare package
+      Medium =                                                                      MediumAir)
                           annotation (Placement(transformation(
         extent={{10,-10},{-10,10}},
         rotation=180,
@@ -205,7 +207,9 @@ model DemandControlledAHU "Example for air handling unit with demand controlled
     minVflowPer=0.2,
     CO2set=900,
     useTwoFanCtr=false,
-    kCO2=3000/3600) annotation (Placement(transformation(extent={{-40,40},{-20,60}})));
+    kCO2=3000/3600,
+    initType=Modelica.Blocks.Types.Init.InitialState)
+                    annotation (Placement(transformation(extent={{-40,40},{-20,60}})));
   Utilities.Psychrometrics.Phi_pTX phi
     annotation (Placement(transformation(extent={{128,56},{148,76}})));
   BoundaryConditions.WeatherData.Bus weaBus1
@@ -218,20 +222,23 @@ protected
     "molar mass of air";
 
 equation
-  connect(genericAHU.port_a2, thermalZone.ports[1]) annotation (Line(points={{62.5455,20},{72.83,20},{72.83,59.88}},                color={0,127,255}));
-  connect(genericAHU.port_b1, thermalZone.ports[2]) annotation (Line(points={{62.5455,-4},{83.17,-4},{83.17,59.88}},color={0,127,255}));
-  connect(SourcePreheater.ports[1], genericAHU.port_a3) annotation (Line(points={{-45,-66},{-45,-34},{-41.6364,-34}},
-                                               color={0,127,255}));
-  connect(SinkPreheater.ports[1], genericAHU.port_b3) annotation (Line(points={{-29,-66},{-29,-34},{-30.7273,-34}},
-                                              color={0,127,255}));
+  connect(genericAHU.port_a2, thermalZone.ports[1]) annotation (Line(points={{62.5455,
+          20},{75.415,20},{75.415,59.88}},                                                                                          color={0,127,255}));
+  connect(genericAHU.port_b1, thermalZone.ports[2]) annotation (Line(points={{62.5455,
+          -4},{80.585,-4},{80.585,59.88}},                                                                          color={0,127,255}));
+  connect(SourcePreheater.ports[1], genericAHU.port_a3) annotation (Line(points={{-45,-66},
+          {-45,-34},{-41.6364,-34}},           color={0,127,255}));
+  connect(SinkPreheater.ports[1], genericAHU.port_b3) annotation (Line(points={{-29,-66},
+          {-29,-34},{-30.7273,-34}},          color={0,127,255}));
   connect(SourceCooler.ports[1], genericAHU.port_a4) annotation (Line(points={{-3,-66},
           {-3,-54},{2,-54},{2,-34}},         color={0,127,255}));
   connect(SinkCooler.ports[1], genericAHU.port_b4) annotation (Line(points={{13,-66},
           {12,-66},{12,-34},{12.9091,-34}},      color={0,127,255}));
-  connect(SourceHeater.ports[1], genericAHU.port_a5) annotation (Line(points={{31,-66},{32,-66},{32,-62},{22,-62},{22,-34},{23.8182,-34}},
-                                                                   color={0,127,
+  connect(SourceHeater.ports[1], genericAHU.port_a5) annotation (Line(points={{31,-66},
+          {32,-66},{32,-62},{22,-62},{22,-34},{23.8182,-34}},      color={0,127,
           255}));
-  connect(SinkHeater.ports[1], genericAHU.port_b5) annotation (Line(points={{47,-66},{40,-66},{40,-56},{32,-56},{32,-46},{34.1818,-46},{34.1818,-34}},
+  connect(SinkHeater.ports[1], genericAHU.port_b5) annotation (Line(points={{47,-66},
+          {40,-66},{40,-56},{32,-56},{32,-46},{34.1818,-46},{34.1818,-34}},
                                                       color={0,127,255}));
   connect(out.ports[1], genericAHU.port_a1) annotation (Line(points={{-70,-4},{
           -58,-4}},                                                                                           color={0,127,255}));
@@ -269,9 +276,8 @@ equation
   annotation (experiment(
       StartTime=5961600,
       StopTime=6566400,
-      Interval=120.000096,
-      Tolerance=1e-05,
-      __Dymola_Algorithm="Dassl"), Documentation(info="<html>
+      Interval=120,
+      Tolerance=1e-05), Documentation(info="<html>
 This example shows the combination of the <code>GenericAHU</code> with a <code>ThermalZone</code>.
 The used controller is designed for demand controlled ventilation (DCV) based on the CO2-Concentration in the zone.
 The Example provides a ready-to-use framework for testing and tuning controllers.
@@ -285,6 +291,6 @@ The nominal values for heat exchangers are derived from data sheets and experime
 </ul>
 </html>"),
 __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/ModularAHU/Examples/DemandControlledAHU.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/DemandControlledAHU.mos"
         "Simulate and plot"));
 end DemandControlledAHU;
diff --git a/AixLib/Systems/ModularAHU/Examples/EONERC_AHU2.mo b/AixLib/Systems/ModularAHU/Examples/EONERC_AHU2.mo
index 507cdc0230..be567857cc 100644
--- a/AixLib/Systems/ModularAHU/Examples/EONERC_AHU2.mo
+++ b/AixLib/Systems/ModularAHU/Examples/EONERC_AHU2.mo
@@ -246,8 +246,5 @@ equation
 </ul>
 </html>", info="<html>
 <p>This example includes the GenericAHU model that is parameterized according to an existing air-handling unit of the EON.ERC test hall.</p>
-</html>"),
-    __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/ModularAHU/Examples/GenericAHU.mos"
-        "Simulate and plot"));
+</html>"));
 end EONERC_AHU2;
diff --git a/AixLib/Systems/ModularAHU/Examples/GenericAHU.mo b/AixLib/Systems/ModularAHU/Examples/GenericAHU.mo
index f742342d9c..f1b2dbeca0 100644
--- a/AixLib/Systems/ModularAHU/Examples/GenericAHU.mo
+++ b/AixLib/Systems/ModularAHU/Examples/GenericAHU.mo
@@ -12,7 +12,7 @@ model GenericAHU "Example of generic ahu model"
             AixLib.Fluid.Actuators.Valves.Data.LinearEqualPercentage(),
         redeclare
           AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-          PumpInterface(pump(redeclare
+          PumpInterface(speed_rpm_nominal=3040, pump(redeclare
               AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to8 per))),
         dynamicHX(
         dp1_nominal=50,
@@ -21,8 +21,8 @@ model GenericAHU "Example of generic ahu model"
         tau2=15,
         dT_nom=30,
         Q_nom=30000)),
-    redeclare package Medium1 = Media.Air,
-    redeclare package Medium2 = Media.Water,
+    redeclare package Medium1 = AixLib.Media.Air,
+    redeclare package Medium2 = AixLib.Media.Water,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     T_amb=293.15,
     m1_flow_nominal=3000/3600*1.2,
@@ -39,7 +39,7 @@ model GenericAHU "Example of generic ahu model"
             AixLib.Fluid.Actuators.Valves.Data.LinearEqualPercentage(),
         redeclare
           AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-          PumpInterface(pump(redeclare
+          PumpInterface(speed_rpm_nominal=3690, pump(redeclare
               AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos50slash1to12 per))),
         dynamicHX(
         dp1_nominal=80,
@@ -56,7 +56,7 @@ model GenericAHU "Example of generic ahu model"
             AixLib.Fluid.Actuators.Valves.Data.LinearEqualPercentage(),
         redeclare
           AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-          PumpInterface(pump(redeclare
+          PumpInterface(speed_rpm_nominal=3040, pump(redeclare
               AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to8 per))),
         dynamicHX(
         dp1_nominal=50,
@@ -184,7 +184,7 @@ equation
 </html>", info="<html>
 <p>This example demonstrates the GenericAHU model with a simple control. The supply air temperature set point is 20&deg;C.</p>
 </html>"),
-    __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/ModularAHU/Examples/GenericAHU.mos"
+    __Dymola_Commands(file=
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/GenericAHU.mos"
         "Simulate and plot"));
 end GenericAHU;
diff --git a/AixLib/Systems/ModularAHU/Examples/Heater.mo b/AixLib/Systems/ModularAHU/Examples/Heater.mo
index f2262695c4..3886c99a4c 100644
--- a/AixLib/Systems/ModularAHU/Examples/Heater.mo
+++ b/AixLib/Systems/ModularAHU/Examples/Heater.mo
@@ -17,19 +17,21 @@ model Heater "Heating register"
           AixLib.Fluid.Actuators.Valves.Data.LinearEqualPercentage(),
       redeclare
         AixLib.Systems.HydraulicModules.BaseClasses.PumpInterface_SpeedControlledNrpm
-        PumpInterface(pump(redeclare
+        PumpInterface(speed_rpm_nominal=1800, pump(redeclare
             AixLib.Fluid.Movers.Data.Pumps.Wilo.Stratos25slash1to4 per))),
     redeclare package Medium2 = MediumWater,
     redeclare package Medium1 = MediumAir,
     T_amb=293.15,
     dynamicHX(
       Q_nom=30000,
-      dT_nom=20,dp1_nominal=100,
+      dT_nom=20,
+      dp1_nominal=100,
       dp2_nominal=6000),
     energyDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial,
     hydraulicModuleIcon="Admix",
     m1_flow_nominal=1,
-    m2_flow_nominal=0.1, massDynamics = Modelica.Fluid.Types.Dynamics.SteadyStateInitial)
+    m2_flow_nominal=0.1,
+    massDynamics=Modelica.Fluid.Types.Dynamics.SteadyStateInitial)
     annotation (Placement(transformation(extent={{-40,-46},{26,40}})));
 
   Fluid.Sources.Boundary_pT boundaryWaterSource(
@@ -92,11 +94,8 @@ equation
   </li>
 </ul>
 </html>"),
-    experiment(
-      StopTime=3600,
-      __Dymola_fixedstepsize=1,
-      __Dymola_Algorithm="Dassl"),
+    experiment(StopTime=3600,Tolerance=1e-06),
     __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/ModularAHU/Examples/Heater.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Examples/Heater.mos"
         "Simulate and plot"));
 end Heater;
diff --git a/AixLib/Systems/ModularAHU/Examples/package.order b/AixLib/Systems/ModularAHU/Examples/package.order
index 719112b51d..d4ef558b5d 100644
--- a/AixLib/Systems/ModularAHU/Examples/package.order
+++ b/AixLib/Systems/ModularAHU/Examples/package.order
@@ -1,5 +1,5 @@
 Cooler
-Heater
-GenericAHU
-EONERC_AHU2
 DemandControlledAHU
+EONERC_AHU2
+GenericAHU
+Heater
diff --git a/AixLib/Systems/ModularAHU/GenericAHU.mo b/AixLib/Systems/ModularAHU/GenericAHU.mo
index 5fd5d478b5..050e8d3dbd 100644
--- a/AixLib/Systems/ModularAHU/GenericAHU.mo
+++ b/AixLib/Systems/ModularAHU/GenericAHU.mo
@@ -201,23 +201,33 @@ replaceable package Medium2 =
     T_start=T_start,
     final allowFlowReversal=allowFlowReversal1,
     final m_flow_nominal=m1_flow_nominal,
-    redeclare Fluid.Movers.Data.Generic per(hydraulicEfficiency=
-          hydraulicEfficiency, motorEfficiency(eta={0.95})),
+    redeclare Fluid.Movers.Data.Generic per(
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate,
+
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided,
+
+      efficiency=hydraulicEfficiency),
     final inputType=AixLib.Fluid.Types.InputType.Continuous) "Supply air fan"
     annotation (Placement(transformation(extent={{156,-10},{176,10}})));
+
   Fluid.Movers.FlowControlled_dp fanRet(
     redeclare package Medium = Medium1,
     energyDynamics=energyDynamics,
     T_start=T_start,
     final allowFlowReversal=allowFlowReversal1,
     final m_flow_nominal=m1_flow_nominal,
-    redeclare Fluid.Movers.Data.Generic per(hydraulicEfficiency=
-          hydraulicEfficiency, motorEfficiency(eta={0.95})),
+    redeclare Fluid.Movers.Data.Generic per(
+      etaHydMet=AixLib.Fluid.Movers.BaseClasses.Types.HydraulicEfficiencyMethod.Efficiency_VolumeFlowRate,
+
+      etaMotMet=AixLib.Fluid.Movers.BaseClasses.Types.MotorEfficiencyMethod.NotProvided,
+
+      efficiency=hydraulicEfficiency),
     final inputType=AixLib.Fluid.Types.InputType.Continuous) "Return air fan"
                                         annotation (Placement(transformation(
         extent={{-10,10},{10,-10}},
         rotation=180,
         origin={90,80})));
+
   Fluid.Humidifiers.GenericHumidifier_u
                                  humidifier(
     redeclare package Medium = Medium1,
@@ -643,8 +653,8 @@ equation
           fillColor={255,255,255},
           fillPattern=FillPattern.Solid),
         Line(points={{-210,0},{-166,0},{-90,0}},  color={28,108,200}),
-        Rectangle(visible=usePreheater, extent={{-164,38},{-116,-40}}, lineColor=
-              {0,0,0},
+        Rectangle(visible=usePreheater, extent={{-164,38},{-116,-40}}, lineColor
+            = {0,0,0},
           fillColor={255,255,255},
           fillPattern=FillPattern.Solid),
         Rectangle(extent={{-4,38},{44,-40}}, lineColor={0,0,0}),
diff --git a/AixLib/Systems/ModularAHU/Validation/AHU2_Cooler.mo b/AixLib/Systems/ModularAHU/Validation/AHU2_Cooler.mo
index 0d232726d0..1e0e437ac3 100644
--- a/AixLib/Systems/ModularAHU/Validation/AHU2_Cooler.mo
+++ b/AixLib/Systems/ModularAHU/Validation/AHU2_Cooler.mo
@@ -179,9 +179,8 @@ equation
 </html>"),
     experiment(
       StopTime=2700,
-      __Dymola_fixedstepsize=1,
-      __Dymola_Algorithm="Dassl"),
-    __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Cooler.mos"
+      Interval=1,Tolerance=1e-06),
+    __Dymola_Commands(file=
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Cooler.mos"
         "Simulate and Plot"));
 end AHU2_Cooler;
diff --git a/AixLib/Systems/ModularAHU/Validation/AHU2_Heater.mo b/AixLib/Systems/ModularAHU/Validation/AHU2_Heater.mo
index 11e6431c0f..b85f8d11b6 100644
--- a/AixLib/Systems/ModularAHU/Validation/AHU2_Heater.mo
+++ b/AixLib/Systems/ModularAHU/Validation/AHU2_Heater.mo
@@ -103,7 +103,7 @@ model AHU2_Heater "Heating register of ahu 2 in E.ON ERC testhall"
     annotation (Placement(transformation(extent={{-90,34},{-78,46}})));
   Modelica.Blocks.Sources.Constant const(k=1)
     annotation (Placement(transformation(extent={{-104,32},{-96,40}})));
-  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation(
+  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation (
     Placement(visible = true, transformation(origin = {-80, -24}, extent = {{-10, -10}, {10, 10}}, rotation = 0)));
 equation
   connect(toKelvin.Celsius, combiTimeTable.y[2]) annotation (Line(points={{-80,-92},
@@ -155,8 +155,9 @@ equation
           -72,40},{-72,36}},          color={0,0,127}));
   connect(const.y, add.u2) annotation (Line(points={{-95.6,36},{-94,36},{-94,
           36.4},{-91.2,36.4}}, color={0,0,127}));
-  connect(pumpOn.y, registerBus1.hydraulicBus.pumpBus.onSet) annotation(
-    Line(points = {{-68, -24}, {-38, -24}, {-38, 10}}, color = {255, 0, 255}));
+  connect(pumpOn.y, registerBus1.hydraulicBus.pumpBus.onSet) annotation (
+    Line(points={{-69,-24},{-37.95,-24},{-37.95,10.05}},
+                                                       color = {255, 0, 255}));
   annotation (Documentation(info="<html><p>
   This example compares the simulated behavior with measured data. The
   input filter of the valve is deactivated because the measured actual
@@ -170,10 +171,9 @@ equation
 </ul>
 </html>"),
     experiment(
-      StopTime=4320,
-      __Dymola_fixedstepsize=1,
-      __Dymola_Algorithm="Dassl"),
+      StopTime=4320,Tolerance=1e-06,
+      Interval=1),
     __Dymola_Commands(file(ensureSimulated=true)=
-        "Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Heater.mos"
+        "modelica://AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Heater.mos"
         "Simulate and Plot"));
 end AHU2_Heater;
diff --git a/AixLib/Systems/ModularAHU/Validation/AHU2_Preheater.mo b/AixLib/Systems/ModularAHU/Validation/AHU2_Preheater.mo
index 45717feb75..606d89dde0 100644
--- a/AixLib/Systems/ModularAHU/Validation/AHU2_Preheater.mo
+++ b/AixLib/Systems/ModularAHU/Validation/AHU2_Preheater.mo
@@ -98,7 +98,7 @@ model AHU2_Preheater "Heating register of ahu 2 in E.ON ERC testhall"
 
   BaseClasses.RegisterBus registerBus1
     annotation (Placement(transformation(extent={{-48,0},{-28,20}})));
-  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation(
+  Modelica.Blocks.Sources.BooleanConstant pumpOn annotation (
     Placement(visible = true, transformation(origin = {-80, -24}, extent = {{-10, -10}, {10, 10}}, rotation = 0)));
 equation
   connect(toKelvin.Kelvin, boundaryWaterSource.T_in)
@@ -145,8 +145,9 @@ equation
   connect(boundaryWaterSource.ports[1], registerModule.port_a2) annotation (
       Line(points={{-20,-70},{-22,-70},{-22,0.461538},{-22,0.461538}}, color={0,
           127,255}));
-  connect(pumpOn.y, registerBus1.hydraulicBus.pumpBus.onSet) annotation(
-    Line(points = {{-68, -24}, {-38, -24}, {-38, 10}}, color = {255, 0, 255}));
+  connect(pumpOn.y, registerBus1.hydraulicBus.pumpBus.onSet) annotation (
+    Line(points={{-69,-24},{-37.95,-24},{-37.95,10.05}},
+                                                       color = {255, 0, 255}));
   annotation (Documentation(info="<html><p>
   This example compares the simulated behavior with measured data. The
   input filter of the valve is deactivated because the measured actual
@@ -161,8 +162,7 @@ equation
 </html>"),
     experiment(
       StopTime=7200,
-      __Dymola_fixedstepsize=1,
-      __Dymola_Algorithm="Dassl"),
-    __Dymola_Commands(file(ensureSimulated=true) = "Resources/Scripts/Dymola/Systems/ModularAHU/Validation/Preheater.mos"
+      Interval=1,Tolerance=1e-06),
+    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Systems/ModularAHU/Validation/AHU2_Preheater.mos"
         "Simulate and Plot"));
 end AHU2_Preheater;
diff --git a/AixLib/Systems/ModularAHU/package.order b/AixLib/Systems/ModularAHU/package.order
index 3b7784726c..cf67ec88ff 100644
--- a/AixLib/Systems/ModularAHU/package.order
+++ b/AixLib/Systems/ModularAHU/package.order
@@ -1,5 +1,5 @@
-RegisterModule
 GenericAHU
+RegisterModule
 Controller
 Examples
 Validation
diff --git a/AixLib/Systems/TABS/Examples/Tabs.mo b/AixLib/Systems/TABS/Examples/Tabs.mo
index da39020ea0..b29a8aff5c 100644
--- a/AixLib/Systems/TABS/Examples/Tabs.mo
+++ b/AixLib/Systems/TABS/Examples/Tabs.mo
@@ -47,7 +47,10 @@ model Tabs "Test of Tabs"
     area=3000,
     thickness=0.03,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
-    massDynamics=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial)
+    massDynamics=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial,
+    pumpSys(PumpInterface(speed_rpm_nominal=3580)),
+    throttlePumpHot(PumpInterface(speed_rpm_nominal=2900)),
+    throttlePumpCold(PumpInterface(speed_rpm_nominal=2900)))
     annotation (Placement(transformation(extent={{-20,-20},{20,20}})));
 equation
   connect(ramp.y, prescribedTemperature.T)
diff --git a/AixLib/ThermalZones/HighOrder/Components/DryAir/InfiltrationRate_DIN12831.mo b/AixLib/ThermalZones/HighOrder/Components/DryAir/InfiltrationRate_DIN12831.mo
index b8d6e0cfa2..e77424adda 100644
--- a/AixLib/ThermalZones/HighOrder/Components/DryAir/InfiltrationRate_DIN12831.mo
+++ b/AixLib/ThermalZones/HighOrder/Components/DryAir/InfiltrationRate_DIN12831.mo
@@ -1,4 +1,4 @@
-within AixLib.ThermalZones.HighOrder.Components.DryAir;
+within AixLib.ThermalZones.HighOrder.Components.DryAir;
 model InfiltrationRate_DIN12831
   "Heat flow caused by infiltration after european standard DIN EN 12831"
   extends Modelica.Thermal.HeatTransfer.Interfaces.Element1D;
@@ -31,285 +31,283 @@ equation
   Air exchange coefficients at 50 Pa pressure difference between
   ambience and room air:
 </p>
-<table>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"1\">
   <caption>
-    \"coefficients\" cellspacing=\"2\" cellpadding=\"0\" border= \"1\"&gt;
-    <table>
-      <tr>
-        <td>
-          <p style=\"text-align:center;\"></p>
-          <h4>
-            Dwelling type
-          </h4>
-        </td>
-        <td>
-          <p style=\"text-align:center;\"></p>
-          <h4>
-            highly air tight
-          </h4>
-        </td>
-        <td>
-          <p style=\"text-align:center;\"></p>
-          <h4>
-            medium air tight
-          </h4>
-        </td>
-        <td>
-          <p style=\"text-align:center;\"></p>
-          <h4>
-            low air tight
-          </h4>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            one-family dwelling
-          </p>
-        </td>
-        <td>
-          <p>
-            &lt; 4
-          </p>
-        </td>
-        <td>
-          <p>
-            4 - 10
-          </p>
-        </td>
-        <td>
-          <p>
-            &gt; 10
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            multi-family dwelling/other
-          </p>
-        </td>
-        <td>
-          <p>
-            &lt; 2
-          </p>
-        </td>
-        <td>
-          <p>
-            2 - 5
-          </p>
-        </td>
-        <td>
-          <p>
-            &gt; 5
-          </p>
-        </td>
-      </tr>
-    </table>
-    <p>
-      <br/>
-      <br/>
-      Reference values for air shielding value e:
-    </p>
-    <table>
-      <caption>
-        \"Reference\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\
-      </caption>
-      <tr>
-        <td></td>
-        <td>
-          <p style=\"text-align:center;\"></p>
-          <h4>
-            heated room without
-          </h4>
-          <p style=\"text-align:center;\">
-            facade with openings
-          </p>
-          <p style=\"text-align:center;\">
-            exposed to wind
-          </p>
-        </td>
-        <td>
-          <p style=\"text-align:center;\"></p>
-          <h4>
-            heated room with
-          </h4>
-          <p style=\"text-align:center;\">
-            one facade with openings
-          </p>
-          <p style=\"text-align:center;\">
-            exposed to wind
-          </p>
-        </td>
-        <td>
-          <p style=\"text-align:center;\"></p>
-          <h4>
-            heated room with more than
-          </h4>
-          <p style=\"text-align:center;\">
-            one facade with openings
-          </p>
-          <p style=\"text-align:center;\">
-            exposed to wind
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            no shielding
-          </p>
-        </td>
-        <td>
-          <p>
-            0
-          </p>
-        </td>
-        <td>
-          <p>
-            0.03
-          </p>
-        </td>
-        <td>
-          <p>
-            0.05
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            moderate shielding
-          </p>
-        </td>
-        <td>
-          <p>
-            0
-          </p>
-        </td>
-        <td>
-          <p>
-            0.02
-          </p>
-        </td>
-        <td>
-          <p>
-            0.03
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            well shielded
-          </p>
-        </td>
-        <td>
-          <p>
-            0
-          </p>
-        </td>
-        <td>
-          <p>
-            0.01
-          </p>
-        </td>
-        <td>
-          <p>
-            0.02
-          </p>
-        </td>
-      </tr>
-    </table>
-    <p>
-      <br/>
-      <br/>
-      Reference values for height correction value ε:
-    </p>
-    <table>
-      <caption>
-        \"Reference\" cellspacing=\"2\" cellpadding=\"0\" border=\"1\
-      </caption>
-      <tr>
-        <td>
-          <h4>
-            Height of room
-          </h4>
-        </td>
-        <td>
-          <p style=\"text-align:center;\">
-            <br/>
-            <b>ε</b>
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            0 - 10 m
-          </p>
-        </td>
-        <td>
-          <p>
-            1
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            10 - 30 m
-          </p>
-        </td>
-        <td>
-          <p>
-            1.2
-          </p>
-        </td>
-      </tr>
-      <tr>
-        <td>
-          <p>
-            &gt; 30 m
-          </p>
-        </td>
-        <td>
-          <p>
-            1.5
-          </p>
-        </td>
-      </tr>
-    </table>
-    <p>
-      <br/>
-      <br/>
-      <b><span style=\"color: #008000\">References</span></b>
-    </p>
-    <p>
-      DIN EN 12831
-    </p>
-    <p>
-      <b><span style=\"color: #008000\">Example Results</span></b>
-    </p>
-    <p>
-      <a href=
-      \"AixLib.Building.Components.Examples.DryAir.DryAir_test\">AixLib.Building.Components.Examples.DryAir.DryAir_test</a>
-    </p>
-    <ul>
-      <li>
-        <i>Mai 19, 2014&#160;</i> by Ana Constantin:<br/>
-        Uses components from MSL and respects the naming conventions
-      </li>
-      <li>
-        <i>May 02, 2013&#160;</i> by Ole Odendahl:<br/>
-        Formatted documentation appropriately
-      </li>
-      <li>
-        <i>August 2, 2011&#160;</i> by Ana Constantin:<br/>
-        Implemented after a model from Time Haase.
-      </li>
-    </ul>
+    coefficients
   </caption>
+  <tr>
+    <td>
+      <p style=\"text-align:center;\"></p>
+      <h4>
+        Dwelling type
+      </h4>
+    </td>
+    <td>
+      <p style=\"text-align:center;\"></p>
+      <h4>
+        highly air tight
+      </h4>
+    </td>
+    <td>
+      <p style=\"text-align:center;\"></p>
+      <h4>
+        medium air tight
+      </h4>
+    </td>
+    <td>
+      <p style=\"text-align:center;\"></p>
+      <h4>
+        low air tight
+      </h4>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        one-family dwelling
+      </p>
+    </td>
+    <td>
+      <p>
+        &lt; 4
+      </p>
+    </td>
+    <td>
+      <p>
+        4 - 10
+      </p>
+    </td>
+    <td>
+      <p>
+        &gt; 10
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        multi-family dwelling/other
+      </p>
+    </td>
+    <td>
+      <p>
+        &lt; 2
+      </p>
+    </td>
+    <td>
+      <p>
+        2 - 5
+      </p>
+    </td>
+    <td>
+      <p>
+        &gt; 5
+      </p>
+    </td>
+  </tr>
 </table>
+<p>
+  <br/>
+  <br/>
+  Reference values for air shielding value e:
+</p>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"1\">
+  <caption>
+    Reference
+  </caption>
+  <tr>
+    <td></td>
+    <td>
+      <p style=\"text-align:center;\"></p>
+      <h4>
+        heated room without
+      </h4>
+      <p style=\"text-align:center;\">
+        facade with openings
+      </p>
+      <p style=\"text-align:center;\">
+        exposed to wind
+      </p>
+    </td>
+    <td>
+      <p style=\"text-align:center;\"></p>
+      <h4>
+        heated room with
+      </h4>
+      <p style=\"text-align:center;\">
+        one facade with openings
+      </p>
+      <p style=\"text-align:center;\">
+        exposed to wind
+      </p>
+    </td>
+    <td>
+      <p style=\"text-align:center;\"></p>
+      <h4>
+        heated room with more than
+      </h4>
+      <p style=\"text-align:center;\">
+        one facade with openings
+      </p>
+      <p style=\"text-align:center;\">
+        exposed to wind
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        no shielding
+      </p>
+    </td>
+    <td>
+      <p>
+        0
+      </p>
+    </td>
+    <td>
+      <p>
+        0.03
+      </p>
+    </td>
+    <td>
+      <p>
+        0.05
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        moderate shielding
+      </p>
+    </td>
+    <td>
+      <p>
+        0
+      </p>
+    </td>
+    <td>
+      <p>
+        0.02
+      </p>
+    </td>
+    <td>
+      <p>
+        0.03
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        well shielded
+      </p>
+    </td>
+    <td>
+      <p>
+        0
+      </p>
+    </td>
+    <td>
+      <p>
+        0.01
+      </p>
+    </td>
+    <td>
+      <p>
+        0.02
+      </p>
+    </td>
+  </tr>
+</table>
+<p>
+  <br/>
+  <br/>
+  Reference values for height correction value ε:
+</p>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"1\">
+  <caption>
+    Reference
+  </caption>
+  <tr>
+    <td>
+      <h4>
+        Height of room
+      </h4>
+    </td>
+    <td>
+      <p style=\"text-align:center;\">
+        <br/>
+        <b>ε</b>
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        0 - 10 m
+      </p>
+    </td>
+    <td>
+      <p>
+        1
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        10 - 30 m
+      </p>
+    </td>
+    <td>
+      <p>
+        1.2
+      </p>
+    </td>
+  </tr>
+  <tr>
+    <td>
+      <p>
+        &gt; 30 m
+      </p>
+    </td>
+    <td>
+      <p>
+        1.5
+      </p>
+    </td>
+  </tr>
+</table>
+<p>
+  <br/>
+  <br/>
+  <b><span style=\"color: #008000\">References</span></b>
+</p>
+<p>
+  DIN EN 12831
+</p>
+<p>
+  <b><span style=\"color: #008000\">Example Results</span></b>
+</p>
+<p>
+  <a href=
+  \"AixLib.Building.Components.Examples.DryAir.DryAir_test\">AixLib.Building.Components.Examples.DryAir.DryAir_test</a>
+</p>
+<ul>
+  <li>
+    <i>Mai 19, 2014&#160;</i> by Ana Constantin:<br/>
+    Uses components from MSL and respects the naming conventions
+  </li>
+  <li>
+    <i>May 02, 2013&#160;</i> by Ole Odendahl:<br/>
+    Formatted documentation appropriately
+  </li>
+  <li>
+    <i>August 2, 2011&#160;</i> by Ana Constantin:<br/>
+    Implemented after a model from Time Haase.
+  </li>
+</ul>
 </html>"), Diagram(coordinateSystem(preserveAspectRatio = true, extent = {{-100, -100}, {100, 100}}, grid = {2, 2})));
 end InfiltrationRate_DIN12831;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Examples/DryAir/DryAir_test.mo b/AixLib/ThermalZones/HighOrder/Components/Examples/DryAir/DryAir_test.mo
index 99308803ff..9bbac31a54 100644
--- a/AixLib/ThermalZones/HighOrder/Components/Examples/DryAir/DryAir_test.mo
+++ b/AixLib/ThermalZones/HighOrder/Components/Examples/DryAir/DryAir_test.mo
@@ -82,9 +82,9 @@ equation
 <p>
   The simulation consists of the following models:
 </p>
-<table>
+<table cellspacing=\"2\" cellpadding=\"0\" border=\"0\">
   <caption>
-    \"Models\" cellspacing=\"2\" cellpadding=\"0\" border=\"0\
+    Models
   </caption>
   <tr>
     <td bgcolor=\"#DCDCDC\">
@@ -106,7 +106,7 @@ equation
     </td>
     <td>
       <p>
-        <a href=\"Building.Components.DryAir.Airload\">Airload</a>
+        <a href=\"AixLib.ThermalZones.HighOrder.Components.DryAir.Airload\">Airload</a>
       </p>
     </td>
   </tr>
@@ -119,7 +119,7 @@ equation
     <td>
       <p>
         <a href=
-        \"Building.Components.DryAir.VarAirExchange\">VarAirExchange</a>
+        \"AixLib.ThermalZones.HighOrder.Components.DryAir.VarAirExchange\">VarAirExchange</a>
       </p>
     </td>
   </tr>
@@ -132,7 +132,7 @@ equation
     <td>
       <p>
         <a href=
-        \"Building.Components.DryAir.InfiltrationRate_DIN12831\">InfiltrationRate_DIN12831</a>
+        \"AixLib.ThermalZones.HighOrder.Components.DryAir.InfiltrationRate_DIN12831\">InfiltrationRate_DIN12831</a>
       </p>
     </td>
   </tr>
@@ -145,7 +145,7 @@ equation
     <td>
       <p>
         <a href=
-        \"Building.Components.DryAir.DynamicVentilation\">DynamicVentilation</a>
+        \"AixLib.ThermalZones.HighOrder.Components.DryAir.DynamicVentilation\">DynamicVentilation</a>
       </p>
     </td>
   </tr>
diff --git a/AixLib/ThermalZones/HighOrder/Components/Examples/Walls/OutsideWall.mo b/AixLib/ThermalZones/HighOrder/Components/Examples/Walls/OutsideWall.mo
index 48ea1ff04c..5769a77d4a 100644
--- a/AixLib/ThermalZones/HighOrder/Components/Examples/Walls/OutsideWall.mo
+++ b/AixLib/ThermalZones/HighOrder/Components/Examples/Walls/OutsideWall.mo
@@ -16,7 +16,7 @@ model OutsideWall
         AixLib.ThermalZones.HighOrder.Components.WindowsDoors.BaseClasses.CorrectionSolarGain.CorGSimple,
     withSunblind=true,
     outside=true,
-    calcMethodOut=2,
+    calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals,
     Blinding=0.2,
     LimitSolIrr=100,
     TOutAirLimit=282.15,
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/ShadowEffectTest.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/ShadowEffectTest.mo
new file mode 100644
index 0000000000..cab7de0a0b
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/ShadowEffectTest.mo
@@ -0,0 +1,167 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow.Examples;
+model ShadowEffectTest "Test the modul ShadowEffect"
+  extends Modelica.Icons.Example;
+  BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+        ModelicaServices.ExternalReferences.loadResource(
+        "modelica://AixLib/Resources/weatherdata/TRY2015_Jahr_City_Aachen.mos"))
+    annotation (Placement(transformation(extent={{-100,20},{-80,40}})));
+  ShadowEffect shaEffDiffAll(calMod=AixLib.ThermalZones.HighOrder.Components.Shadow.Types.selectorShadowEffectMode.constRedDiffAllDir)
+    "Shadow effect with constRedDiffAllDir"
+    annotation (Placement(transformation(extent={{0,70},{20,90}})));
+  RadiationTransfer radiationTransfer
+    annotation (Placement(transformation(extent={{-60,40},{-40,60}})));
+  ShadowEffect shaEffDiffPerp(calMod=AixLib.ThermalZones.HighOrder.Components.Shadow.Types.selectorShadowEffectMode.constRedDiffPerpDir)
+    "Shadow effect with constRedDiffPerpDir"
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  ShadowEffect shaEffAsDir(calMod=AixLib.ThermalZones.HighOrder.Components.Shadow.Types.selectorShadowEffectMode.varRedDiffAsDirRad)
+    "Shadow effect with varRedDiffAsDirRad"
+    annotation (Placement(transformation(extent={{0,10},{20,30}})));
+  ReducedOrder.Windows.BaseClasses.SelfShadowing                     selfShadowingAbove(
+    final bRig={0},
+    final n=1,
+    final b={1},
+    final h={1},
+    final bLef={0},
+    final dLef={0},
+    final dRig={0},
+    final bAbo={0.3},
+    final bBel={0},
+    final dAbo={0.1},
+    final dBel={0},
+    final azi={-0.94247779607694},
+    final til={1.5707963267949})
+    "Shadowing due to a projection above the window"
+          annotation (Placement(transformation(extent={{68,-20},{100,8}})));
+  ReducedOrder.Windows.Validation.BaseClasses.IncidenceAngleVDI6007 incAng(azi=-0.94247779607694,
+      til=1.5707963267949) "Incidence angle for the window"
+    annotation (Placement(transformation(extent={{0,-20},{20,0}})));
+  BoundaryConditions.SolarGeometry.BaseClasses.AltitudeAngle        altAng
+    "Altitude angle"
+    annotation (Placement(transformation(extent={{-40,0},{-20,20}})));
+  BoundaryConditions.WeatherData.Bus        weaBus "Weather bus" annotation (Placement(
+        transformation(extent={{-80,0},{-60,20}}),    iconTransformation(extent={{-110,
+            -10},{-90,10}})));
+  BoundaryConditions.SolarGeometry.BaseClasses.SolarHourAngle
+    solHouAng "Solar hour angle"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+  BoundaryConditions.SolarGeometry.BaseClasses.ZenithAngle        zen
+    "Zenith angle"
+    annotation (Placement(transformation(extent={{0,-60},{20,-40}})));
+  BoundaryConditions.SolarGeometry.BaseClasses.Declination        decAng
+    "Declination angle"
+    annotation (Placement(transformation(extent={{-60,-50},{-40,-30}})));
+  BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth        solAzi
+    "Solar azimuth"
+    annotation (Placement(transformation(extent={{40,-100},{60,-80}})));
+  Modelica.Blocks.Sources.RealExpression gShaDirEffDiffAll(y=shaEffDiffAll.gShaDir)
+    annotation (Placement(transformation(extent={{80,20},{100,40}})));
+equation
+  connect(weaDat.weaBus, shaEffDiffAll.weaBus) annotation (Line(
+      points={{-80,30},{-20,30},{-20,88},{0,88}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(weaDat.weaBus, radiationTransfer.weaBus) annotation (Line(
+      points={{-80,30},{-68,30},{-68,58},{-60,58}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(radiationTransfer.solRadOut, shaEffDiffAll.solRadIn) annotation (Line(
+        points={{-39,50},{-10,50},{-10,80},{-1,80}},   color={255,128,0}));
+  connect(weaDat.weaBus, shaEffDiffPerp.weaBus) annotation (Line(
+      points={{-80,30},{-20,30},{-20,58},{0,58}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(radiationTransfer.solRadOut, shaEffDiffPerp.solRadIn) annotation (
+      Line(points={{-39,50},{-1,50}},                     color={255,128,0}));
+  connect(weaDat.weaBus, shaEffAsDir.weaBus) annotation (Line(
+      points={{-80,30},{-20,30},{-20,28},{0,28}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(radiationTransfer.solRadOut, shaEffAsDir.solRadIn) annotation (Line(
+        points={{-39,50},{-10,50},{-10,20},{-1,20}},     color={255,128,0}));
+  connect(altAng.zen, weaBus.solZen) annotation (Line(points={{-42,10},{-70,10}},
+                 color={0,0,127}), Text(
+      string="%second",
+      index=1,
+      extent={{-3,-6},{-3,-6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaDat.weaBus, weaBus) annotation (Line(
+      points={{-80,30},{-80,10},{-70,10}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%second",
+      index=1,
+      extent={{-3,-6},{-3,-6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(incAng.incAng, selfShadowingAbove.incAng[1]) annotation (Line(points={{21,-10},
+          {60,-10},{60,-15.8},{66.4,-15.8}},           color={0,0,127}));
+  connect(altAng.alt, incAng.alt) annotation (Line(points={{-19,10},{-10,10},{-10,
+          -4.6},{-2.2,-4.6}},        color={0,0,127}));
+  connect(altAng.alt, selfShadowingAbove.alt) annotation (Line(points={{-19,10},{
+          -10,10},{-10,6},{60,6},{60,-6},{66.4,-6}},         color={0,0,127}));
+  connect(zen.zen,solAzi. zen) annotation (Line(
+      points={{21,-50},{28,-50},{28,-82},{38,-82}},
+      color={0,0,127}));
+  connect(decAng.decAng,solAzi. decAng) annotation (Line(
+      points={{-39,-40},{-10,-40},{-10,-32},{32,-32},{32,-86},{38,-86},{38,-86.2}},
+      color={0,0,127}));
+  connect(decAng.decAng,zen. decAng) annotation (Line(
+      points={{-39,-40},{-10,-40},{-10,-44.6},{-2,-44.6}},
+      color={0,0,127}));
+  connect(solHouAng.solHouAng, zen.solHouAng) annotation (Line(points={{-39,-70},
+          {-2,-70},{-2,-54.8}},         color={0,0,127}));
+  connect(weaBus.cloTim, decAng.nDay) annotation (Line(
+      points={{-70,10},{-70,-40},{-62,-40}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaBus.solTim, solHouAng.solTim) annotation (Line(
+      points={{-70,10},{-70,-70},{-62,-70}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaBus.lat, zen.lat) annotation (Line(
+      points={{-70,10},{-70,-20},{-30,-20},{-30,-50},{-2,-50}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaBus.lat, solAzi.lat) annotation (Line(
+      points={{-70,10},{-70,-98},{38,-98}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-3,-6},{-3,-6}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaBus.solTim, solAzi.solTim) annotation (Line(
+      points={{-70,10},{-70,-94},{38,-94}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(solAzi.solAzi, selfShadowingAbove.solAzi) annotation (Line(points={{61,-90},
+          {64,-90},{64,3.8},{66.4,3.8}},               color={0,0,127}));
+  connect(solAzi.solAzi, incAng.solAzi) annotation (Line(points={{61,-90},{64,-90},
+          {64,-26},{-2,-26},{-2,-14.8}},       color={0,0,127}));
+  annotation (experiment(
+      StopTime=31536000,
+      Interval=3600,
+      __Dymola_Algorithm="Dassl"), Documentation(info="<html>
+<p><b><span style=\"color: #008000;\">Overview</span> </b></p>
+<p>Simulation to test the <a href=\"AixLib.Building.Components.Shadow.ShadowEffect\">ShadowEffect</a> model with different diffuse radiation calculation modes. Comparison with shadow coefficient with the model <a href=\"AixLib.ThermalZones.ReducedOrder.Windows.BaseClasses.SelfShadowing\">SelfShadowing</a>.</p>
+</html>", revisions="<html>
+<ul>
+<li><i>November 2023,&nbsp;</i>by Jun Jiang:<br>Implemented.<br>This is for <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1433\">#1433</a>.</li>
+</ul>
+</html>"));
+end ShadowEffectTest;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/ShadowLengthTest.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/ShadowLengthTest.mo
new file mode 100644
index 0000000000..39171ce6ca
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/ShadowLengthTest.mo
@@ -0,0 +1,39 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow.Examples;
+model ShadowLengthTest "Test the modul ShadowLength"
+  extends Modelica.Icons.Example;
+  ShadowLength shaLen1(aziDeg=0, lenShie=0.3) "Azi=S, lenShie=0.3"
+    annotation (Placement(transformation(extent={{20,40},{60,80}})));
+  BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+        ModelicaServices.ExternalReferences.loadResource(
+        "modelica://AixLib/Resources/weatherdata/TRY2015_Jahr_City_Aachen.mos"))
+    annotation (Placement(transformation(extent={{-40,-10},{-20,10}})));
+  ShadowLength shaLen2(aziDeg=90, lenShie=0.3) "Azi=W, lenShie=0.3"
+    annotation (Placement(transformation(extent={{20,-20},{60,20}})));
+  ShadowLength shaLen3(aziDeg=90, lenShie=0.6) "Azi=W, lenShie=0.6"
+    annotation (Placement(transformation(extent={{20,-80},{60,-40}})));
+equation
+  connect(weaDat.weaBus, shaLen1.weaBus) annotation (Line(
+      points={{-20,0},{14,0},{14,60},{20,60}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(weaDat.weaBus, shaLen2.weaBus) annotation (Line(
+      points={{-20,0},{20,0}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(weaDat.weaBus, shaLen3.weaBus) annotation (Line(
+      points={{-20,0},{14,0},{14,-60},{20,-60}},
+      color={255,204,51},
+      thickness=0.5));
+  annotation (experiment(
+      StopTime=31536000,
+      Interval=3600,
+      Tolerance=1e-06,
+      __Dymola_Algorithm="Dassl"), Documentation(info="<html>
+<p><b><span style=\"color: #008000;\">Overview</span> </b></p>
+<p>Simulation to test the <a href=\"AixLib.Building.Components.Shadow.ShadowLength\">ShadowLength</a> model with different facade azimuth angles and sun shied lengths.</p>
+</html>", revisions="<html>
+<ul>
+<li><i>November 2023,&nbsp;</i>by Jun Jiang:<br>Implemented.<br>This is for <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1433\">#1433</a>.</li>
+</ul>
+</html>"));
+end ShadowLengthTest;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/package.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/package.mo
new file mode 100644
index 0000000000..f2cd47653d
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/package.mo
@@ -0,0 +1,4 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow;
+package Examples "Examples for shadow models"
+extends Modelica.Icons.ExamplesPackage;
+end Examples;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/package.order b/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/package.order
new file mode 100644
index 0000000000..cd0dcb36c4
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/Examples/package.order
@@ -0,0 +1,2 @@
+ShadowEffectTest
+ShadowLengthTest
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/RadiationTransfer.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/RadiationTransfer.mo
new file mode 100644
index 0000000000..e312e86712
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/RadiationTransfer.mo
@@ -0,0 +1,79 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow;
+model RadiationTransfer "Radiation transformer for weather bus"
+  parameter Modelica.Units.NonSI.Angle_deg aziDeg = -54 "Surface azimuth, S=0°, W=90°, N=180°, E=-90°";
+
+  AixLib.Utilities.Sources.PrescribedSolarRad preSolRad
+    annotation (Placement(transformation(extent={{40,-20},{80,20}})));
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather bus"
+    annotation (Placement(transformation(extent={{-120,-20},{-80,20}}),
+        iconTransformation(extent={{-120,60},{-80,100}})));
+  Modelica.Blocks.Math.Add add
+    annotation (Placement(transformation(extent={{0,40},{20,60}})));
+  AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface hDirTil(
+    til=1.5707963267949,
+    azi=Modelica.Units.Conversions.from_deg(aziDeg))
+    annotation (Placement(transformation(extent={{-60,60},{-40,80}})));
+  AixLib.BoundaryConditions.SolarIrradiation.DiffusePerez hDifTil(
+    til=1.5707963267949,
+    rho=0,
+    azi=Modelica.Units.Conversions.from_deg(aziDeg))
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Modelica.Blocks.Sources.Constant const(k=0)
+    annotation (Placement(transformation(extent={{-60,-20},{-40,0}})));
+  AixLib.Utilities.Interfaces.SolarRad_out solRadOut
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+equation
+  connect(weaBus,hDirTil. weaBus) annotation (Line(
+      points={{-100,0},{-80,0},{-80,70},{-60,70}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaBus,hDifTil. weaBus) annotation (Line(
+      points={{-100,0},{-80,0},{-80,30},{-60,30}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(hDirTil.H, add.u1) annotation (Line(points={{-39,70},{-12,70},{-12,56},
+          {-2,56}}, color={0,0,127}));
+  connect(hDifTil.H, add.u2) annotation (Line(points={{-39,30},{-8,30},{-8,44},{
+          -2,44}}, color={0,0,127}));
+  connect(add.y, preSolRad.I[1]) annotation (Line(points={{21,50},{30,50},{30,17.8},
+          {42.2,17.8}}, color={0,0,127}));
+  connect(hDirTil.H, preSolRad.I_dir[1]) annotation (Line(points={{-39,70},{-12,
+          70},{-12,10},{42,10}}, color={0,0,127}));
+  connect(hDifTil.H, preSolRad.I_diff[1]) annotation (Line(points={{-39,30},{-20,
+          30},{-20,2},{42,2}}, color={0,0,127}));
+  connect(const.y, preSolRad.I_gr[1]) annotation (Line(points={{-39,-10},{-30,-10},
+          {-30,-6.2},{42.2,-6.2}}, color={0,0,127}));
+  connect(hDirTil.inc, preSolRad.AOI[1]) annotation (Line(points={{-39,66},{-26,
+          66},{-26,-14},{42,-14}}, color={0,0,127}));
+  connect(preSolRad.solarRad_out[1], solRadOut)
+    annotation (Line(points={{78,0},{110,0}}, color={255,128,0}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Text(
+          extent={{-100,140},{100,100}},
+          textString="%name",
+          textColor={0,0,255}), Rectangle(
+          extent={{-100,100},{100,-100}},
+          lineColor={28,108,200},
+          lineThickness=1)}),                                    Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(revisions="<html>
+<ul>
+<li><i>December 2023,&nbsp;</i>by Jun Jiang:<br>Implemented.<br>This is for <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1433\">#1433</a>.</li>
+</ul>
+</html>", info="<html>
+<p><b><span style=\"color: #008000;\">Overview</span> </b></p>
+<p>This model converts weather data to the solar radiation port.</p>
+<p><b><span style=\"color: #008000;\">Concept</span> </b></p>
+<p>See the submodules in the model.</p>
+<p><b><span style=\"color: #008000;\">Assumptions</span> </b></p>
+<p>Vertical wall surface (til = 90&deg;).</p>
+</html>"));
+end RadiationTransfer;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/ShadowEffect.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/ShadowEffect.mo
new file mode 100644
index 0000000000..007f87cf04
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/ShadowEffect.mo
@@ -0,0 +1,141 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow;
+model ShadowEffect
+  "Shadow effect of horizotal shield, reducing the solar radiation through the window"
+  parameter AixLib.ThermalZones.HighOrder.Components.Shadow.Types.selectorShadowEffectMode calMod
+    "Diffuse radiation calculation mode: {constRedDiffAllDir, constRedDiffPerpDir, varRedDiffAsDirRad}";
+  parameter Modelica.Units.SI.Length lenShie = 0.3
+    "Horizontal length of the sun shield";
+  parameter Modelica.Units.SI.Length heiWinMin = 0.1
+    "Distance from shield to upper border of window";
+  parameter Modelica.Units.SI.Length heiWinMax = 1.1
+    "Distance from shield to lower border of window";
+  parameter Modelica.Units.NonSI.Angle_deg aziDeg = -54
+    "Surface azimuth, S=0°, W=90°, N=180°, E=-90°";
+  parameter Real redFacDifRad(min=0,max=1) = 1
+    "Reduce factor of shadow effect for diffuse radiation: 0=fully reduced, 1=no addtional reduce";
+  parameter Integer N = 100
+    "Number of discretisation angles to calculate the shadow factor";
+
+  BoundaryConditions.WeatherData.Bus weaBus "Weather bus"
+    annotation (Placement(transformation(extent={{-120,60},{-80,100}}),
+        iconTransformation(extent={{-120,60},{-80,100}})));
+  Utilities.Interfaces.SolarRad_in solRadIn
+    annotation (Placement(transformation(extent={{-120,-10},{-100,10}})));
+  Utilities.Interfaces.SolarRad_out solRadOut
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  ShadowLength shaLen
+    annotation (Placement(transformation(extent={{-40,-20},{0,20}})));
+
+  Modelica.Units.SI.TransmissionCoefficient gShaDir(min=0,max=1)
+    "Shadow coefficient for direct radiation: 0=full shadowed, 1=no shadow";
+protected
+  Real gShaDif "Shadow coefficient for diffuse radiation: 0=full shadowed, 1=no shadow";
+  Real sum, beta, s, H, L, gShaDif_mean "Parameters for integration";
+
+algorithm
+  // Calculate the mean shadow factor regarding 90° range from perpenticular direction
+  sum := 0;
+  for i in 1:N loop
+    H := (heiWinMax + heiWinMin)/2;
+    L := lenShie;
+    s := (Modelica.Constants.pi/2) / N; // Differential of 90° for integration
+    beta := (Modelica.Constants.pi/2) / N * i; // Angle to the perpendicular direction
+    sum := sum + (2/Modelica.Constants.pi) * Modelica.Math.atan(H/L * Modelica.Math.cos(beta)) * s;
+  end for;
+  gShaDif_mean := sum / (Modelica.Constants.pi/2);
+
+equation
+  // Calculate the shadow factor for direct radiation
+  if shaLen.sha then
+    gShaDir =min(max((heiWinMax - shaLen.heiSha)/(heiWinMax - heiWinMin), 0), 1);
+  else
+    gShaDir = 0;
+  end if;
+  solRadOut.I = solRadOut.I_dir + solRadOut.I_diff;
+  solRadOut.I_dir = solRadIn.I_dir*gShaDir;
+  // Calculate the shadow factor for diffuse radiation
+  if calMod == AixLib.ThermalZones.HighOrder.Components.Shadow.Types.selectorShadowEffectMode.constRedDiffAllDir then
+    gShaDif = gShaDif_mean;
+    solRadOut.I_diff = solRadIn.I_diff*gShaDif*redFacDifRad;
+  elseif calMod == AixLib.ThermalZones.HighOrder.Components.Shadow.Types.selectorShadowEffectMode.constRedDiffPerpDir then
+    gShaDif = atan((heiWinMax+heiWinMin)/2 / lenShie)/(Modelica.Constants.pi/2);
+    solRadOut.I_diff = solRadIn.I_diff*gShaDif*redFacDifRad;
+  else
+    gShaDif = 99;  //Not used in the following equation, to avoid sigular structure
+    solRadOut.I_diff = solRadIn.I_diff*gShaDir*redFacDifRad;
+  end if;
+  solRadOut.I_gr = solRadIn.I_gr;
+  solRadOut.AOI = solRadIn.AOI;
+
+  connect(shaLen.weaBus, weaBus) annotation (Line(
+      points={{-40,0},{-74,0},{-74,80},{-100,80}},
+      color={255,204,51},
+      thickness=0.5));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{40,40},{48,-80}},
+          lineColor={0,0,0},
+          fillColor={28,108,200},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{40,40},{48,80}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-40,88},{100,80}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{40,-80},{48,-92}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-60,98},{40,10}},
+          color={0,0,0},
+          thickness=0.5,
+          arrow={Arrow.None,Arrow.Filled}),
+        Rectangle(
+          extent={{40,-92},{100,-100}},
+          lineColor={0,0,0},
+          fillColor={0,0,0},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-60,8},{40,-80}},
+          color={0,0,0},
+          thickness=0.5,
+          arrow={Arrow.None,Arrow.Filled}),
+        Line(
+          points={{-60,54},{40,-34}},
+          color={0,0,0},
+          thickness=0.5,
+          arrow={Arrow.None,Arrow.Filled}),
+        Text(
+          extent={{-100,140},{100,100}},
+          textString="%name",
+          textColor={0,0,255})}),                                Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p><b><span style=\"color: #008000;\">Overview</span> </b></p>
+<p>This model represents the reducing effect of solar radiation caused by the shadow on the window surface. </p>
+<p><b><span style=\"color: #008000;\">Concept</span> </b></p>
+<p>The model calculates the ratio of the shadow on the window glazing area to determine the radiation reduction.</p>
+<ul>
+<li>For the area without shadow, the solar radiation remains unchanged.</li>
+<li>For the area with shadow, the direct radiation is reduced to zero, the diffuse radiation is reduced according to the defined type.</li>
+</ul>
+<p><b><span style=\"color: #008000;\">Assumptions</span></b> </p>
+<ul>
+<li>The diffuse radiation has a vertical incident angle between 0&deg; (horizontal to the ground) and 90&deg; (vertical to the ground, upward).</li>
+<li>The reduction of reflected radiation is not considered.</li>
+</ul>
+<p><b><span style=\"color: #008000;\">Example Results</span> </b></p>
+<p><a href=\"AixLib.ThermalZones.HighOrder.Components.Shadow.Examples.ShadowEffectTest\">AixLib.ThermalZones.HighOrder.Components.Shadow.Examples.ShadowEffectTest</a> </p>
+</html>", revisions="<html>
+<ul>
+<li><i>December 2023,&nbsp;</i>by Jun Jiang:<br>Implemented.<br>This is for <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1433\">#1433</a>.</li>
+</ul>
+</html>"));
+end ShadowEffect;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/ShadowLength.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/ShadowLength.mo
new file mode 100644
index 0000000000..0b1522ebe9
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/ShadowLength.mo
@@ -0,0 +1,145 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow;
+model ShadowLength
+  "Calculate the shadow length on the vertical surface by a horizontal shield"
+  parameter Modelica.Units.NonSI.Angle_deg aziDeg = -54
+    "Surface azimuth, S=0°, W=90°, N=180°, E=-90°";
+  parameter Modelica.Units.SI.Length lenShie = 0.3
+    "Horizontal length of the sun shield";
+
+  AixLib.BoundaryConditions.SolarGeometry.BaseClasses.AltitudeAngle altAng
+    "Altitude angle"
+    annotation (Placement(transformation(extent={{-60,60},{-40,80}})));
+  AixLib.BoundaryConditions.SolarGeometry.IncidenceAngle incAng(
+    azi = Modelica.Units.Conversions.from_deg(aziDeg),
+    til = Modelica.Units.Conversions.from_deg(90)) "Solar incidence angle"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  AixLib.BoundaryConditions.SolarGeometry.BaseClasses.WallSolarAzimuth wallSolAzi
+    "Vertical wall solar azimuth angle"
+    annotation (Placement(transformation(extent={{-20,40},{0,60}})));
+  AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination decAng
+    "Declination angle"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+  AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarHourAngle solHouAng
+    "Solar hour angle"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+  AixLib.BoundaryConditions.SolarGeometry.BaseClasses.ZenithAngle zen "Zenith angle"
+    annotation (Placement(transformation(extent={{-20,-60},{0,-40}})));
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus "Weather bus" annotation (Placement(
+        transformation(extent={{-120,-20},{-80,20}}), iconTransformation(extent={{-110,
+            -10},{-90,10}})));
+
+  Modelica.Blocks.Interfaces.RealOutput heiSha
+    "Height of shadow on vertical surface"
+    annotation (Placement(transformation(extent={{100,40},{120,60}})));
+  Modelica.Blocks.Interfaces.BooleanOutput sha
+    "= true, if the shadow is present on the surface"
+    annotation (Placement(transformation(extent={{100,-60},{120,-40}})));
+
+  Modelica.Blocks.Math.Tan tan1
+    annotation (Placement(transformation(extent={{10,-60},{30,-40}})));
+  Modelica.Blocks.Logical.Hysteresis hysteresis(uLow=0.001, uHigh=0.002)
+    annotation (Placement(transformation(extent={{40,40},{60,60}})));
+  Modelica.Blocks.Logical.Hysteresis hysteresis1(uLow=0.001, uHigh=0.002)
+    annotation (Placement(transformation(extent={{40,-60},{60,-40}})));
+  Modelica.Blocks.Sources.RealExpression realExpression(y=if sha then lenShie/(
+        tan(zen.zen)*cos(wallSolAzi.verAzi)) else 0)
+    annotation (Placement(transformation(extent={{60,80},{80,100}})));
+  Modelica.Blocks.Math.Cos cos1
+    annotation (Placement(transformation(extent={{10,40},{30,60}})));
+
+  Modelica.Blocks.Logical.And and1
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+equation
+
+  connect(weaBus.solZen, altAng.zen) annotation (Line(
+      points={{-100,0},{-80,0},{-80,70},{-62,70}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaBus, incAng.weaBus) annotation (Line(
+      points={{-100,0},{-80,0},{-80,30},{-60,30}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaBus.cloTim, decAng.nDay) annotation (Line(
+      points={{-100,0},{-80,0},{-80,-30},{-62,-30}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(weaBus.solTim, solHouAng.solTim) annotation (Line(
+      points={{-100,0},{-80,0},{-80,-70},{-62,-70}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(altAng.alt, wallSolAzi.alt) annotation (Line(points={{-39,70},{-30,70},
+          {-30,54.8},{-22,54.8}}, color={0,0,127}));
+  connect(incAng.y, wallSolAzi.incAng) annotation (Line(points={{-39,30},{-30,30},
+          {-30,45.2},{-22,45.2}}, color={0,0,127}));
+  connect(decAng.decAng, zen.decAng) annotation (Line(points={{-39,-30},{-30,-30},
+          {-30,-44.6},{-22,-44.6}}, color={0,0,127}));
+  connect(solHouAng.solHouAng, zen.solHouAng) annotation (Line(points={{-39,-70},
+          {-30,-70},{-30,-54.8},{-22,-54.8}}, color={0,0,127}));
+  connect(weaBus.lat, zen.lat) annotation (Line(
+      points={{-100,0},{-80,0},{-80,-50},{-22,-50}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(realExpression.y, heiSha) annotation (Line(points={{81,90},{96,90},{96,
+          50},{110,50}},    color={0,0,127}));
+  connect(zen.zen, tan1.u)
+    annotation (Line(points={{1,-50},{8,-50}}, color={0,0,127}));
+  connect(wallSolAzi.verAzi, cos1.u)
+    annotation (Line(points={{1,50},{8,50}}, color={0,0,127}));
+  connect(cos1.y, hysteresis.u)
+    annotation (Line(points={{31,50},{38,50}}, color={0,0,127}));
+  connect(tan1.y, hysteresis1.u)
+    annotation (Line(points={{31,-50},{38,-50}}, color={0,0,127}));
+  connect(hysteresis.y, and1.u1) annotation (Line(points={{61,50},{62,50},{62,20},
+          {38,20},{38,0}}, color={255,0,255}));
+  connect(hysteresis1.y, and1.u2) annotation (Line(points={{61,-50},{62,-50},{62,
+          -20},{38,-20},{38,-8}}, color={255,0,255}));
+  connect(and1.y, sha) annotation (Line(points={{61,0},{80,0},{80,-50},{110,-50}},
+        color={255,0,255}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+          Bitmap(
+          extent={{-98,-98},{98,98}}, fileName="modelica://AixLib/Resources/Images/ThermalZones/HighOrder/Components/Shadow/Icon/ShadowLength.png"),
+        Text(
+          extent={{-100,140},{100,100}},
+          textString="%name",
+          textColor={0,0,255})}),
+      Diagram(coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p><b><span style=\"color: #008000;\">Overview</span> </b></p>
+<p>This model represents the shadow length on a vertical wall caused by a horizontal shield on it. </p>
+<p><b><span style=\"color: #008000;\">Concept</span> </b></p>
+<ul>
+<li>The model calculates the wall solar azimuth and the zenith angles to determine if a shadow is present on the wall surface, then outputs it as a boolean value.</li>
+<li>When the shadow is present, the model calculates the shadow length.</li>
+</ul>
+<p><b><span style=\"color: #008000;\">Assumptions</span></b> </p>
+<ul>
+<li>The wall is vertical (til = 90&deg;), while the shield is horizontal.</li>
+</ul>
+<p><b><span style=\"color: #008000;\">Example Results</span> </b></p>
+<p><a href=\"AixLib.ThermalZones.HighOrder.Components.Shadow.Examples.ShadowLengthTest\">AixLib.ThermalZones.HighOrder.Components.Shadow.Examples.ShadowLengthTest</a> </p>
+</html>", revisions="<html>
+<ul>
+<li><i>December 2023,&nbsp;</i>by Jun Jiang:<br>Implemented.<br>This is for <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1433\">#1433</a>.</li>
+</ul>
+</html>"));
+end ShadowLength;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/package.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/package.mo
new file mode 100644
index 0000000000..72c376a6ff
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/package.mo
@@ -0,0 +1,5 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow;
+package Types "Types"
+  extends Modelica.Icons.Package;
+
+end Types;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/package.order b/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/package.order
new file mode 100644
index 0000000000..76fc400976
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/package.order
@@ -0,0 +1 @@
+selectorShadowEffectMode
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/selectorShadowEffectMode.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/selectorShadowEffectMode.mo
new file mode 100644
index 0000000000..4442302a1e
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/Types/selectorShadowEffectMode.mo
@@ -0,0 +1,9 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow.Types;
+type selectorShadowEffectMode = enumeration(
+    constRedDiffAllDir
+    "Constant reduce factor for diffuse radiation, considering all direction (infinite shield width)",
+    constRedDiffPerpDir
+    "Constant reduce factor for diffuse radiation, only considering perpendicular direction as overall factor",
+    varRedDiffAsDirRad
+    "Variable reduce factor for diffuse radiation, same factor as direct radiation (no diffuse radiation when the shadow is not present)")
+  "Enumeration of calculation modes by calculation the shadow effect";
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/WeatherDataProcessing.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/WeatherDataProcessing.mo
new file mode 100644
index 0000000000..6889fa3cdf
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/WeatherDataProcessing.mo
@@ -0,0 +1,32 @@
+within AixLib.ThermalZones.HighOrder.Components.Shadow;
+model WeatherDataProcessing "Weather data processing"
+  extends RadiationTransfer;
+  parameter Integer nDryBulPort=1 "Number of output port(s)";
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature preTemp[
+    nDryBulPort]
+    annotation (Placement(transformation(extent={{40,-60},{60,-40}})));
+  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_b TDryBul[nDryBulPort]
+    annotation (Placement(transformation(extent={{90,-110},{110,-90}})));
+equation
+  connect(preTemp.port, TDryBul)
+    annotation (Line(points={{60,-50},{80,-50},{80,-100},{100,-100}},
+                                                  color={191,0,0}));
+  for i in 1:nDryBulPort loop
+    connect(weaBus.TDryBul, preTemp[i].T)
+      annotation (Line(points={{-100,0},{-80,0},{-80,-50},{38,-50}},
+                      color={0,0,127}));
+  end for;
+
+  annotation (Documentation(revisions="<html>
+<ul>
+<li><i>December 2023,&nbsp;</i>by Jun Jiang:<br>Implemented.<br>This is for <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1433\">#1433</a>.</li>
+</ul>
+</html>", info="<html>
+<p><b><span style=\"color: #008000;\">Overview</span> </b></p>
+<p>This model converts weather data to the solar radiation port and heat port.</p>
+<p><b><span style=\"color: #008000;\">Concept</span> </b></p>
+<p>See the submodules in the model.</p>
+<p><b><span style=\"color: #008000;\">Assumptions</span> </b></p>
+<p>Vertical wall surface (til = 90&deg;).</p>
+</html>"));
+end WeatherDataProcessing;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/package.mo b/AixLib/ThermalZones/HighOrder/Components/Shadow/package.mo
new file mode 100644
index 0000000000..abf1473c79
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/package.mo
@@ -0,0 +1,14 @@
+within AixLib.ThermalZones.HighOrder.Components;
+package Shadow "Modells for shadow length and reduced solar gain on a vertical surface"
+  extends Modelica.Icons.Package;
+
+annotation (Documentation(revisions="<html><ul>
+  <li>
+    <i>December 2023,&#160;</i>by Jun Jiang:<br/>
+    Implemented.<br/>
+    This is for <a href=
+    \"https://github.com/RWTH-EBC/AixLib/issues/1433\">#1433</a>.
+  </li>
+</ul>
+</html>"));
+end Shadow;
diff --git a/AixLib/ThermalZones/HighOrder/Components/Shadow/package.order b/AixLib/ThermalZones/HighOrder/Components/Shadow/package.order
new file mode 100644
index 0000000000..3886095871
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Shadow/package.order
@@ -0,0 +1,6 @@
+RadiationTransfer
+ShadowEffect
+ShadowLength
+WeatherDataProcessing
+Types
+Examples
diff --git a/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodConvectiveHeatTransfer.mo b/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodConvectiveHeatTransfer.mo
new file mode 100644
index 0000000000..e55fbece7e
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodConvectiveHeatTransfer.mo
@@ -0,0 +1,9 @@
+within AixLib.ThermalZones.HighOrder.Components.Types;
+type CalcMethodConvectiveHeatTransfer = enumeration(
+    DIN_6946
+        "DIN 6946",
+    ASHRAE_Fundamentals
+        "ASHRAE Fundamentals",
+    Custom_hCon
+        "Custom hCon (constant)")
+  "Calculation method for convective heat transfer coefficient at outside surface";
diff --git a/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodConvectiveHeatTransferInsideSurface.mo b/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodConvectiveHeatTransferInsideSurface.mo
new file mode 100644
index 0000000000..7df64520e0
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodConvectiveHeatTransferInsideSurface.mo
@@ -0,0 +1,11 @@
+within AixLib.ThermalZones.HighOrder.Components.Types;
+type CalcMethodConvectiveHeatTransferInsideSurface = enumeration(
+    EN_ISO_6946_Appendix_A
+        "EN ISO 6946 Appendix A >>Flat Surfaces<<",
+    Bernd_Glueck
+        "By Bernd Glueck",
+    Custom_hCon
+        "Custom hCon (constant)",
+    ASHRAE140_2017
+        "ASHRAE140-2017")
+  "Calculation method for convective heat transfer coefficient at inside surface";
diff --git a/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodRadiativeHeatTransfer.mo b/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodRadiativeHeatTransfer.mo
new file mode 100644
index 0000000000..34f03b3ecd
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Types/CalcMethodRadiativeHeatTransfer.mo
@@ -0,0 +1,11 @@
+within AixLib.ThermalZones.HighOrder.Components.Types;
+type CalcMethodRadiativeHeatTransfer = enumeration(
+    No_approx
+        "No approx",
+    Linear_wall_temp
+        "Linear approx at wall temp",
+    Linear_rad_temp
+        "Linear approx at rad temp",
+    Linear_constant_T_ref
+        "Linear approx at constant T_ref")
+  "Calculation method for radiation heat transfer";
diff --git a/AixLib/ThermalZones/HighOrder/Components/Types/InsideSurfaceOrientation.mo b/AixLib/ThermalZones/HighOrder/Components/Types/InsideSurfaceOrientation.mo
new file mode 100644
index 0000000000..ffd46bfd8f
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Types/InsideSurfaceOrientation.mo
@@ -0,0 +1,8 @@
+within AixLib.ThermalZones.HighOrder.Components.Types;
+type InsideSurfaceOrientation = enumeration(
+    vertical_wall
+        "vertical wall",
+    floor
+        "floor",
+    ceiling
+        "ceiling") "Inside Surface Orientation";
diff --git a/AixLib/ThermalZones/HighOrder/Components/Types/ThermalInsulationRegulation.mo b/AixLib/ThermalZones/HighOrder/Components/Types/ThermalInsulationRegulation.mo
new file mode 100644
index 0000000000..8a0cc70c88
--- /dev/null
+++ b/AixLib/ThermalZones/HighOrder/Components/Types/ThermalInsulationRegulation.mo
@@ -0,0 +1,11 @@
+within AixLib.ThermalZones.HighOrder.Components.Types;
+type ThermalInsulationRegulation = enumeration(
+    EnEV_2009
+        "EnEV 2009",
+    EnEV_2002
+        "EnEV 2002",
+    WSchV_1995
+        "WSchV 1995",
+    WSchV_1984
+        "WSchV 1984")
+          "Thermal Insulation Regulation";
diff --git a/AixLib/ThermalZones/HighOrder/Components/Types/package.order b/AixLib/ThermalZones/HighOrder/Components/Types/package.order
index 5f1b35b639..f5e0c589ff 100644
--- a/AixLib/ThermalZones/HighOrder/Components/Types/package.order
+++ b/AixLib/ThermalZones/HighOrder/Components/Types/package.order
@@ -1,3 +1,8 @@
+CalcMethodConvectiveHeatTransfer
+CalcMethodConvectiveHeatTransferInsideSurface
+CalcMethodRadiativeHeatTransfer
+InsideSurfaceOrientation
+ThermalInsulationRegulation
 selectorCoefficients
 CoeffTableEastWestWindow
 CoeffTableSouthWindow
diff --git a/AixLib/ThermalZones/HighOrder/Components/Walls/BaseClasses/ConvNLayerClearanceStar.mo b/AixLib/ThermalZones/HighOrder/Components/Walls/BaseClasses/ConvNLayerClearanceStar.mo
index 6082f6e976..e0512de5a3 100644
--- a/AixLib/ThermalZones/HighOrder/Components/Walls/BaseClasses/ConvNLayerClearanceStar.mo
+++ b/AixLib/ThermalZones/HighOrder/Components/Walls/BaseClasses/ConvNLayerClearanceStar.mo
@@ -27,34 +27,25 @@ model ConvNLayerClearanceStar
     "Specific heat capacity"
     annotation (Dialog(group="Structure of wall layers"));
   // which orientation of surface?
-  parameter Integer surfaceOrientation "Surface orientation" annotation(Dialog(descriptionLabel = true, enable = if IsHConvConstant == true then false else true), choices(choice = 1
-        "vertical",                                                                                                    choice = 2
-        "horizontal facing up",                                                                                                    choice = 3
-        "horizontal facing down",                                                                                                    radioButtons = true));
-  parameter Integer calcMethod=2 "Calculation method for convective heat transfer coefficient at inside surface" annotation (Dialog(
-        group="Convection", descriptionLabel=true), choices(
-      choice=1 "EN ISO 6946 Appendix A >>Flat Surfaces<<",
-      choice=2 "By Bernd Glueck",
-      choice=3 "Custom hCon (constant)",
-      choice=4 "ASHRAE140-2017",
-      radioButtons=true));
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation surfaceOrientation
+    "Surface orientation" annotation(Dialog(descriptionLabel = true));
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface calcMethod=
+      AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Bernd_Glueck
+    "Calculation method for convective heat transfer coefficient at inside surface" annotation (Dialog(
+        group="Convection", descriptionLabel=true));
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hCon_const=2
     "Constant convective heat transfer coefficient"
-    annotation (Dialog(group="Convection", enable=calcMethod == 1));
+    annotation (Dialog(group="Convection", enable=calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A));
 
-  parameter Integer radCalcMethod=1 "Calculation method for radiation heat transfer" annotation (
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer radCalcMethod=
+      AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.No_approx
+    "Calculation method for radiation heat transfer" annotation (
     Evaluate=true,
-    Dialog(group = "Radiation", compact=true),
-    choices(
-      choice=1 "No approx",
-      choice=2 "Linear approx at wall temp",
-      choice=3 "Linear approx at rad temp",
-      choice=4 "Linear approx at constant T_ref",
-      radioButtons=true));
+    Dialog(group = "Radiation", compact=true));
   parameter Modelica.Units.SI.Temperature T_ref=
       Modelica.Units.Conversions.from_degC(16)
     "Reference temperature for optional linearization"
-    annotation (Dialog(group="Radiation", enable=radCalcMethod == 4));
+    annotation (Dialog(group="Radiation", enable=radCalcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.Linear_constant_T_ref));
 
   parameter Modelica.Units.SI.Temperature T0=
       Modelica.Units.Conversions.from_degC(16) "Initial temperature"
diff --git a/AixLib/ThermalZones/HighOrder/Components/Walls/Wall.mo b/AixLib/ThermalZones/HighOrder/Components/Walls/Wall.mo
index afb650fc82..53337ba4bb 100644
--- a/AixLib/ThermalZones/HighOrder/Components/Walls/Wall.mo
+++ b/AixLib/ThermalZones/HighOrder/Components/Walls/Wall.mo
@@ -1,12 +1,12 @@
-within AixLib.ThermalZones.HighOrder.Components.Walls;
+within AixLib.ThermalZones.HighOrder.Components.Walls;
 model Wall
   "Simple wall model for outside and inside walls with windows and doors"
 
   //Type parameter
   parameter Boolean outside = true
-    "Choose if the wall is an outside or an inside wall"                                annotation(Dialog(group = "General Wall Type Parameter", compact = true), choices(choice = true
-        "Outside Wall",                                                                                                    choice = false
-        "Inside Wall",                                                                                                    radioButtons = true));
+    "Choose if the wall is an outside wall (or an inside wall)" annotation (
+      Dialog(group = "General Wall Type Parameter", compact = true),
+      choices(checkBox=true));
 
   parameter Modelica.Fluid.Types.Dynamics energyDynamics=Modelica.Fluid.Types.Dynamics.DynamicFreeInitial
     "Type of energy balance: dynamic (3 initialization options) or steady state"
@@ -25,100 +25,94 @@ model Wall
   // Surface parameters
   parameter Real solar_absorptance = 0.25
     "Solar absorptance coefficient of outside wall surface"                                       annotation(Dialog(tab = "Surface Parameters", group = "Outside surface", enable = outside));
-  parameter Integer calcMethodOut=1 "Calculation method for convective heat transfer coefficient at outside surface" annotation (Dialog(
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 "Calculation method for convective heat transfer coefficient at outside surface" annotation (Dialog(
       tab="Surface Parameters",
       group="Outside surface",
       enable=outside,
-      compact=true), choices(
-      choice=1 "DIN 6946",
-      choice=2 "ASHRAE Fundamentals",
-      choice=3 "Custom hCon (constant)",
-      radioButtons=true));
+      compact=true));
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConOut_const=25
     "Custom convective heat transfer coefficient (just for manual selection, not recommended)"
     annotation (Dialog(
       tab="Surface Parameters",
       group="Outside surface",
-      enable=calcMethodOut == 3 and outside));
+      enable=calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.Custom_hCon and outside));
 parameter DataBase.Surfaces.RoughnessForHT.PolynomialCoefficients_ASHRAEHandbook         surfaceType = DataBase.Surfaces.RoughnessForHT.Brick_RoughPlaster()
     "Surface type of outside wall"                                                                                                     annotation(Dialog(tab = "Surface Parameters", group = "Outside surface", enable=
-          calcMethodOut == 2 and outside),                                                                                                                                                                                                        choicesAllMatching = true);
-  parameter Integer ISOrientation = 1 "Inside surface orientation" annotation(Dialog(tab = "Surface Parameters", group = "Inside surface", compact = true, descriptionLabel = true), choices(choice = 1
-        "vertical wall",                                                                                                    choice = 2 "floor", choice = 3 "ceiling", radioButtons = true));
+          calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals and outside),                                                                                                                                                                                                        choicesAllMatching = true);
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation ISOrientation = AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall "Inside surface orientation" annotation(Dialog(tab = "Surface Parameters", group = "Inside surface", compact = true, descriptionLabel = true));
 
 
   parameter Boolean use_shortWaveRadIn=false "Use bus connector for incoming shortwave radiation" annotation (Evaluate=true, Dialog(tab="Surface Parameters", group="Inside surface"));
   parameter Boolean use_shortWaveRadOut=false "Use bus connector for outgoing shortwave radiation" annotation (Evaluate=true, Dialog(tab="Surface Parameters", group="Inside surface"));
-  parameter Integer radLongCalcMethod=1 "Calculation method for longwave radiation heat transfer"
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer radLongCalcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.No_approx "Calculation method for longwave radiation heat transfer"
     annotation (
     Evaluate=true,
-    Dialog(tab="Surface Parameters", group="Inside surface",   compact=true),
-    choices(
-      choice=1 "No approx",
-      choice=2 "Linear approx at wall temp",
-      choice=3 "Linear approx at rad temp",
-      choice=4 "Linear approx at constant T_ref",
-      radioButtons=true));
+    Dialog(tab="Surface Parameters", group="Inside surface",   compact=true));
   parameter Modelica.Units.SI.Temperature T_ref=
       Modelica.Units.Conversions.from_degC(16)
     "Reference temperature for optional linearization of longwave radiation"
     annotation (Dialog(
       tab="Surface Parameters",
       group="Inside surface",
-      enable=radLongCalcMethod == 4));
+      enable=radLongCalcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.Linear_constant_T_ref));
 
-  parameter Integer calcMethodIn=1
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A
     "Calculation method of convective heat transfer coefficient at inside surface"
     annotation (Dialog(
       tab="Surface Parameters",
       group="Inside surface",
       compact=true,
-      descriptionLabel=true), choices(
-      choice=1 "EN ISO 6946 Appendix A >>Flat Surfaces<<",
-      choice=2 "By Bernd Glueck",
-      choice=3 "Custom hCon (constant)",
-      choice=4 "ASHRAE140-2017",
-      radioButtons=true));
+      descriptionLabel=true));
 
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConIn_const=2.5
     "Custom convective heat transfer coefficient (just for manual selection, not recommended)"
     annotation (Dialog(
       tab="Surface Parameters",
       group="Inside surface",
-      enable=calcMethodIn == 3));
+      enable=calcMethodIn == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon));
   // window parameters
   parameter Boolean withWindow=false
-    "Choose if the wall has got a window (only outside walls)"                                    annotation(Dialog(tab = "Window", enable = outside));
+    "Choose if the wall has got a window (only outside walls)"                                    annotation(Dialog(tab = "Window", group="Window", enable = outside));
   replaceable model WindowModel =
       AixLib.ThermalZones.HighOrder.Components.WindowsDoors.BaseClasses.PartialWindow
-   constrainedby AixLib.ThermalZones.HighOrder.Components.WindowsDoors.BaseClasses.PartialWindow(
+   constrainedby
+    AixLib.ThermalZones.HighOrder.Components.WindowsDoors.BaseClasses.PartialWindow(
      redeclare final model CorrSolGain=CorrSolarGainWin,
      final T0=T0,
      final windowarea=windowarea,
      final WindowType=WindowType)
        "Model for window"
-                     annotation (Dialog(tab="Window",  enable=withWindow and outside),   choicesAllMatching=true);
+                     annotation (Dialog(tab="Window", group="Window", enable=withWindow and outside),   choicesAllMatching=true);
 
   WindowModel windowModel if withWindow and outside annotation(Placement(transformation(extent={{-15,-48},{11,-22}})));
 
   replaceable parameter DataBase.WindowsDoors.Simple.OWBaseDataDefinition_Simple WindowType = DataBase.WindowsDoors.Simple.WindowSimple_EnEV2009()
-    "Choose a window type from the database"                                                                                                     annotation(Dialog(tab = "Window", enable = withWindow and outside), choicesAllMatching = true);
+    "Choose a window type from the database"                                                                                                     annotation(Dialog(tab = "Window", group="Window", enable = withWindow and outside), choicesAllMatching = true);
   parameter Modelica.Units.SI.Area windowarea=2 "Area of window"
-    annotation (Dialog(tab="Window", enable=withWindow and outside));
+    annotation (Dialog(tab="Window", group="Window", enable=withWindow and outside));
   replaceable model CorrSolarGainWin =
       WindowsDoors.BaseClasses.CorrectionSolarGain.PartialCorG
-    constrainedby WindowsDoors.BaseClasses.CorrectionSolarGain.PartialCorG "Correction model for solar irradiance as transmitted radiation" annotation (choicesAllMatching=true, Dialog(tab = "Window", enable = withWindow and outside));
+    constrainedby WindowsDoors.BaseClasses.CorrectionSolarGain.PartialCorG "Correction model for solar irradiance as transmitted radiation" annotation (choicesAllMatching=true, Dialog(tab = "Window", group="Window", enable = withWindow and outside));
 
-  parameter Boolean withSunblind = false "enable support of sunblinding?" annotation(Dialog(tab = "Window", enable = outside and withWindow));
-  parameter Real Blinding = 0 "blinding factor: 0 means total blocking of solar irradiation" annotation(Dialog(tab = "Window", enable = withWindow and outside and withSunblind));
-  parameter Real LimitSolIrr if withWindow and outside and withSunblind
+  parameter Boolean withSunblind = false "enable support of sunblinding?" annotation(Dialog(tab = "Window", group="Sunblind", enable = outside and withWindow));
+  parameter Real Blinding = 0 "blinding factor: 0 means total blocking of solar irradiation" annotation(Dialog(tab = "Window", group="Sunblind", enable = withWindow and outside and withSunblind));
+  parameter Real LimitSolIrr=0
     "Minimum specific total solar radiation in W/m2 for blinding becoming active (see also TOutAirLimit)"
-    annotation(Dialog(tab="Window",   enable=withWindow and outside and
-          withSunblind));
-  parameter Modelica.Units.SI.Temperature TOutAirLimit
-    if withWindow and outside and withSunblind
+    annotation(Dialog(tab="Window", group="Sunblind", enable=withWindow and outside and withSunblind));
+  parameter Modelica.Units.SI.Temperature TOutAirLimit=288.15
     "Temperature at which sunblind closes (see also LimitSolIrr)" annotation (
-      Dialog(tab="Window", enable=withWindow and outside and withSunblind));
+      Dialog(tab="Window", group="Sunblind", enable=withWindow and outside and withSunblind));
+  //Parameter and module fow shadow model
+  parameter Boolean withShield = false "enable shadow effect?" annotation(Dialog(tab = "Window", group="Shadow", enable = outside and withWindow and withSunblind));
+  parameter Modelica.Units.SI.Length lenWinShie = 0.05
+    "Horizontal length of the sun shield" annotation(Dialog(tab = "Window", group="Shadow", enable = withWindow and outside and withSunblind and withShield));
+  parameter Modelica.Units.SI.Length heiWinShadMin = 0.05
+    "Vertical distance from shield to upper border of window glazing" annotation(Dialog(tab = "Window", group="Shadow", enable = withWindow and outside and withSunblind and withShield));
+  parameter Modelica.Units.SI.Length heiWinShadMax = 1.10
+    "Vertical distance from shield to lower border of window glazing" annotation(Dialog(tab = "Window", group="Shadow", enable = withWindow and outside and withSunblind and withShield));
+  parameter Modelica.Units.NonSI.Angle_deg aziDegWin = -54
+    "Window glazing azimuth, S=0°, W=90°, N=180°, E=-90°" annotation(Dialog(tab = "Window", group="Shadow", enable = withWindow and outside and withSunblind and withShield));
+
   // door parameters
   parameter Boolean withDoor=false   "Choose if the wall has got a door" annotation(Dialog(tab = "Door"));
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer U_door=1.8
@@ -158,7 +152,7 @@ parameter DataBase.Surfaces.RoughnessForHT.PolynomialCoefficients_ASHRAEHandbook
   Utilities.HeatTransfer.SolarRadToHeat SolarAbsorption(coeff = solar_absorptance, A=ANet)                                    if outside annotation(Placement(transformation(origin={-37.5,90.5},extent={{-10.5,-10.5},{10.5,10.5}})));
   AixLib.Utilities.Interfaces.SolarRad_in   SolarRadiationPort if outside annotation(Placement(transformation(extent = {{-116, 79}, {-96, 99}}), iconTransformation(extent = {{-36, 100}, {-16, 120}})));
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a port_outside annotation(Placement(transformation(extent = {{-108, -6}, {-88, 14}}), iconTransformation(extent = {{-31, -10}, {-11, 10}})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if outside and (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if outside and (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
                                                                                                annotation(Placement(transformation(extent = {{-113, 54}, {-93, 74}}), iconTransformation(extent = {{-31, 78}, {-11, 98}})));
   Sunblinds.Sunblind Sunblind(
     final n=1,
@@ -166,7 +160,17 @@ parameter DataBase.Surfaces.RoughnessForHT.PolynomialCoefficients_ASHRAEHandbook
     final Imax=LimitSolIrr,
     final TOutAirLimit=TOutAirLimit)
                       if outside and withWindow and withSunblind
-    annotation (Placement(transformation(extent={{-46,-47},{-23,-21}})));
+    annotation (Placement(transformation(extent={{-52,-44},{-36,-28}})));
+  Shadow.ShadowEffect shadowEff(calMod=AixLib.ThermalZones.HighOrder.Components.Shadow.Types.selectorShadowEffectMode.constRedDiffAllDir,
+    lenShie=lenWinShie,
+    heiWinMin=heiWinShadMin,
+    heiWinMax=heiWinShadMax,
+    aziDeg=aziDegWin) if withWindow and outside and withShield and withSunblind
+    annotation (Placement(transformation(extent={{-40,-20},{-20,0}})));
+  BoundaryConditions.WeatherData.Bus weaBus if withWindow and outside and withShield and withSunblind
+    "Weather bus"
+    annotation (Placement(transformation(extent={{-90,-70},{-110,-50}}),
+        iconTransformation(extent={{-30,-70},{-10,-50}})));
   WindowsDoors.Door Door(
     final door_area=door_height*door_width,
     final eps=eps_door,
@@ -207,6 +211,7 @@ parameter DataBase.Surfaces.RoughnessForHT.PolynomialCoefficients_ASHRAEHandbook
  if use_shortWaveRadIn
     "Parameteres used for the short radiaton models. See connections to check which array corresponds to which parameter"
     annotation (Placement(transformation(extent={{80,88},{90,98}})));
+
 equation
   //   if outside and cardinality(WindSpeedPort) < 2 then
   //     WindSpeedPort = 3;
@@ -230,7 +235,7 @@ equation
   //******************************************************************
   if outside then
     connect(SolarRadiationPort, SolarAbsorption.solarRad_in) annotation(Line(points={{-106,89},{-48,89},{-48,88.4},{-48.105,88.4}},    color = {255, 128, 0}));
-    if calcMethodOut == 1 or calcMethodOut == 2 then
+    if calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals then
       connect(WindSpeedPort, heatTransfer_Outside.WindSpeedPort) annotation(Line(points={{-103,64},{-68,64},{-68,51},{-46,51}},                color = {0, 0, 127}));
     end if;
     connect(heatTransfer_Outside.port_a, port_outside) annotation(Line(points = {{-47, 58}, {-56, 58}, {-56, 4}, {-98, 4}}, color = {191, 0, 0}));
@@ -270,21 +275,42 @@ equation
   // **** connections for outside wall with window and sunblind****
   //******************************************************************
   if outside and withWindow and withSunblind then
-    connect(Sunblind.Rad_Out[1], windowModel.solarRad_in) annotation (Line(points={{-21.5625,-32.375},{-20,-32.375},{-20,-27.2},{-13.7,-27.2}}, color={255,128,0}));
-    connect(Sunblind.Rad_In[1], SolarRadiationPort) annotation(Line(points={{-47.4375,-32.375},{-50,-32.375},{-50,-16},{-80,-16},{-80,89},{-106,89}},
-                                                                                                                                   color = {255, 128, 0}));
+    if withShield then
+      connect(weaBus, shadowEff.weaBus) annotation (Line(
+      points={{-100,-60},{-76,-60},{-76,-2},{-40,-2}},
+      color={255,204,51},
+      thickness=0.5,
+          pattern=LinePattern.Dash),
+                      Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+      connect(windowModel.solarRad_in, shadowEff.solRadOut) annotation (Line(
+          points={{-13.7,-27.2},{-16,-27.2},{-16,-10},{-19,-10}},
+          color={255,128,0},
+          pattern=LinePattern.Dash));
+      connect(Sunblind.Rad_Out[1], shadowEff.solRadIn) annotation (Line(
+          points={{-35,-35},{-32,-35},{-32,-20},{-44,-20},{-44,-10},{-41,-10}},
+          color={255,128,0},
+          pattern=LinePattern.Dash));
+
+    else
+      connect(Sunblind.Rad_Out[1], windowModel.solarRad_in) annotation (Line(points={{-35,-35},
+              {-32,-35},{-32,-34},{-28,-34},{-28,-27.2},{-13.7,-27.2}},                                                                           color={255,128,
+              0},
+          pattern=LinePattern.Dash));
+    end if;
+    connect(Sunblind.Rad_In[1], SolarRadiationPort) annotation(Line(points={{-53,-35},
+            {-54,-35},{-54,89},{-106,89}},                                                                                         color = {255, 128, 0}));
   end if;
   connect(heatStarToComb.portConvRadComb, thermStarComb_inside) annotation (Line(points={{79,-1},{79,-1.05},{102,-1.05},{102,0}},       color={191,0,0}));
-  connect(tempOutAirSensor.T, Sunblind.TOutAir) annotation (Line(points={{-62,-40},{-54,-40},{-54,-38.875},{-47.4375,-38.875}},
-                                                      color={0,0,127}));
+  connect(tempOutAirSensor.T, Sunblind.TOutAir) annotation (Line(points={{-61.6,
+          -40},{-61.6,-39},{-53,-39}},                color={0,0,127}));
   connect(port_outside, tempOutAirSensor.port) annotation (Line(points={{-98,4},{-90,4},{-90,-40},{-70,-40}},
                                         color={191,0,0}));
   connect(absSolarRadWin.port, Wall.port_b1) annotation (Line(points={{35,80},{30,80},{30,48},{16.74,48},{16.74,35.78}}, color={191,0,0}));
-
-
   connect(WindSpeedPort, windowModel.WindSpeedPort) annotation (Line(points={{-103,64},{-72,64},{-72,-62},{-20,-62},{-20,-41.5},{-13.7,-41.5}}, color={0,0,127}));
-
-
   connect(shortRadWin, windowModel.shortRadWin) annotation (Line(points={{104,-59},
           {60,-59},{60,-23.56},{9.7,-23.56}},      color={0,0,0}), Text(
       string="%first",
@@ -438,12 +464,8 @@ equation
   <a href=
   \"AixLib.Building.Components.Examples.Walls.InsideWall\">AixLib.Building.Components.Examples.Walls.InsideWall</a>
 </p>
+</html>", revisions="<html>
 <ul>
-  <li>
-    <i>June, 18, 2020</i> by Fabian Wuellhorst:<br/>
-    <a href=\"https://github.com/RWTH-EBC/AixLib/issues/918\">#918</a>:
-    Add short wave connector to pass wall and window parameters.
-  </li>
   <li>
     <i>June, 18, 2020</i> by Fabian Wuellhorst:<br/>
     <a href=\"https://github.com/RWTH-EBC/AixLib/issues/918\">#918</a>:
diff --git a/AixLib/ThermalZones/HighOrder/Components/WindowsDoors/Door.mo b/AixLib/ThermalZones/HighOrder/Components/WindowsDoors/Door.mo
index 07fa6396eb..5441d9cfc9 100644
--- a/AixLib/ThermalZones/HighOrder/Components/WindowsDoors/Door.mo
+++ b/AixLib/ThermalZones/HighOrder/Components/WindowsDoors/Door.mo
@@ -7,19 +7,13 @@ model Door "Simple door"
   parameter Modelica.Units.SI.Emissivity eps=0.9 "Emissivity of door material"
     annotation (Dialog(group="Radiation"));
 
-  parameter Integer radCalcMethod=1 "Calculation method for radiation heat transfer" annotation (
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer radCalcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.No_approx "Calculation method for radiation heat transfer" annotation (
     Evaluate=true,
-    Dialog(group = "Radiation", compact=true),
-    choices(
-      choice=1 "No approx",
-      choice=2 "Linear approx at wall temp",
-      choice=3 "Linear approx at rad temp",
-      choice=4 "Linear approx at constant T_ref",
-      radioButtons=true));
+    Dialog(group = "Radiation", compact=true));
   parameter Modelica.Units.SI.Temperature T_ref=
       Modelica.Units.Conversions.from_degC(16)
     "Reference temperature for optional linearization"
-    annotation (Dialog(group="Radiation", enable=radCalcMethod == 4));
+    annotation (Dialog(group="Radiation", enable=radCalcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.Linear_constant_T_ref));
 
 
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a port_a annotation(Placement(transformation(extent = {{-100, -10}, {-80, 10}})));
diff --git a/AixLib/ThermalZones/HighOrder/Components/WindowsDoors/Window_ASHRAE140.mo b/AixLib/ThermalZones/HighOrder/Components/WindowsDoors/Window_ASHRAE140.mo
index 6bcc1f6db5..1ba31f16b7 100644
--- a/AixLib/ThermalZones/HighOrder/Components/WindowsDoors/Window_ASHRAE140.mo
+++ b/AixLib/ThermalZones/HighOrder/Components/WindowsDoors/Window_ASHRAE140.mo
@@ -20,10 +20,10 @@ model Window_ASHRAE140
       Placement(transformation(extent={{-10,-20},{10,0}})));
   Utilities.HeatTransfer.HeatConvOutside heatConv_outside(
     final A=windowarea,
-    calcMethod=2,
+    calcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals,
     surfaceType=AixLib.DataBase.Surfaces.RoughnessForHT.Glass()) annotation (Placement(transformation(extent={{-66,-20},{-46,0}})));
   Utilities.HeatTransfer.HeatConvInside heatConv_inside(
-    calcMethod=2,
+    calcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Bernd_Glueck,
     hCon_const=2,
     final A=windowarea)
                   annotation (Placement(transformation(extent={{68,-20},{48,2}})));
@@ -42,8 +42,8 @@ model Window_ASHRAE140
     final energyDynamics=energyDynamics)
     annotation (Placement(transformation(extent={{18,-18},{38,2}})));
   Modelica.Blocks.Sources.Constant constFixShoRadPar[6](k={WindowType.g,1 -
-        WindowType.g,0,sqrt(windowarea),sqrt(windowarea),0})
- if use_solarRadWinTrans
+        WindowType.g,0,sqrt(windowarea),sqrt(windowarea),0}) if
+    use_solarRadWinTrans
     "Parameteres used for the short radiaton models. See connections to check which array corresponds to which parameter"
     annotation (Placement(transformation(extent={{68,96},{78,106}})));
 equation
diff --git a/AixLib/ThermalZones/HighOrder/Components/package.order b/AixLib/ThermalZones/HighOrder/Components/package.order
index 10ce213e63..e5e4ee8eb4 100644
--- a/AixLib/ThermalZones/HighOrder/Components/package.order
+++ b/AixLib/ThermalZones/HighOrder/Components/package.order
@@ -1,5 +1,6 @@
 DryAir
 MoistAir
+Shadow
 Sunblinds
 Walls
 WindowsDoors
diff --git a/AixLib/ThermalZones/HighOrder/Examples/ASHREA140/CompareDynamicAndStaticSolarFrac_Case270.mo b/AixLib/ThermalZones/HighOrder/Examples/ASHREA140/CompareDynamicAndStaticSolarFrac_Case270.mo
index 0a254913ce..4973f75341 100644
--- a/AixLib/ThermalZones/HighOrder/Examples/ASHREA140/CompareDynamicAndStaticSolarFrac_Case270.mo
+++ b/AixLib/ThermalZones/HighOrder/Examples/ASHREA140/CompareDynamicAndStaticSolarFrac_Case270.mo
@@ -7,13 +7,13 @@ model CompareDynamicAndStaticSolarFrac_Case270 "Based on Case270 from validation
     tableOnFile=true,
     tableName="Table",
     columns={2,3},
-    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/Weatherdata_ASHARE140.mat"))
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/Weatherdata_ASHARE140.txt"))
     annotation (Placement(transformation(extent={{-46,164},{-26,184}})));
   Modelica.Blocks.Sources.CombiTimeTable Source_Weather_dyn(
     tableOnFile=true,
     tableName="Table",
     columns={4,5,6,7},
-    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/Weatherdata_ASHARE140.mat"))
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/Weatherdata_ASHARE140.txt"))
     annotation (Placement(transformation(extent={{-46,194},{-26,214}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature outsideTemp_dyn
     "ambient temperature"
diff --git a/AixLib/ThermalZones/HighOrder/Examples/OFDHeatLoad.mo b/AixLib/ThermalZones/HighOrder/Examples/OFDHeatLoad.mo
index f7fbf81950..7a159ea0c7 100644
--- a/AixLib/ThermalZones/HighOrder/Examples/OFDHeatLoad.mo
+++ b/AixLib/ThermalZones/HighOrder/Examples/OFDHeatLoad.mo
@@ -5,15 +5,10 @@ model OFDHeatLoad "Test environment to determine OFD's nominal heat load"
   parameter Integer nRooms = 11;
   parameter Integer nHeatedRooms = 10;
 
-  parameter Integer TIR=1 "Thermal Insulation Regulation" annotation (Dialog(
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation TIR=AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.EnEV_2009 "Thermal Insulation Regulation" annotation (Dialog(
       group="Construction parameters",
       compact=true,
-      descriptionLabel=true), choices(
-      choice=1 "EnEV_2009",
-      choice=2 "EnEV_2002",
-      choice=3 "WSchV_1995",
-      choice=4 "WSchV_1984",
-      radioButtons=true));
+      descriptionLabel=true));
 
   replaceable package MediumAir = AixLib.Media.Air "Medium within the room";
 
@@ -57,9 +52,9 @@ model OFDHeatLoad "Test environment to determine OFD's nominal heat load"
     redeclare model CorrSolarGainWin =
         Components.WindowsDoors.BaseClasses.CorrectionSolarGain.CorGSimple,
     use_infiltEN12831=true,
-    n50=if TIR == 1 or TIR == 2 then 3 else if TIR == 3 then 4 else 6,
+    n50=if TIR == AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.EnEV_2009 or TIR == AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.EnEV_2002 then 3 else if TIR == AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.WSchV_1995 then 4 else 6,
     redeclare package Medium = MediumAir,
-    UValOutDoors=if TIR == 1 then 1.8 else 2.9,
+    UValOutDoors=if TIR == AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.EnEV_2009 then 1.8 else 2.9,
     upperFloor_Building(Corridor(T0_air=288.15), Bath(T0_air=297.15)),
     groundFloor_Building(Corridor(T0_air=288.15)))
                                                 annotation (Placement(transformation(extent={{-14,-10},{42,46}})));
@@ -112,23 +107,25 @@ equation
   connect(groundTemp.port, wholeHouseBuildingEnvelope.groundTemp)
     annotation (Line(points={{-42,-90},{14,-90},{14,-10}}, color={191,0,0}));
   connect(varRad.solarRad_out[1], wholeHouseBuildingEnvelope.North) annotation (
-     Line(points={{51,69.5833},{48,69.5833},{48,26.4},{43.68,26.4}},  color={
+     Line(points={{51,69.5833},{48,69.5833},{48,28.64},{43.68,28.64}},color={
           255,128,0}));
   connect(varRad.solarRad_out[2], wholeHouseBuildingEnvelope.East) annotation (
-      Line(points={{51,69.75},{48,69.75},{48,18},{43.68,18}},    color={255,128,
+      Line(points={{51,69.75},{48,69.75},{48,21.36},{43.68,21.36}},
+                                                                 color={255,128,
           0}));
   connect(varRad.solarRad_out[3], wholeHouseBuildingEnvelope.South) annotation (
-     Line(points={{51,69.9167},{48,69.9167},{48,9.6},{43.68,9.6}},  color={255,
+     Line(points={{51,69.9167},{48,69.9167},{48,14.08},{43.68,14.08}},
+                                                                    color={255,
           128,0}));
   connect(varRad.solarRad_out[4], wholeHouseBuildingEnvelope.West) annotation (
-      Line(points={{51,70.0833},{48,70.0833},{48,1.2},{43.68,1.2}},  color={255,
+      Line(points={{51,70.0833},{48,70.0833},{48,7.36},{43.68,7.36}},color={255,
           128,0}));
   connect(varRad.solarRad_out[5], wholeHouseBuildingEnvelope.SolarRadiationPort_RoofN)
         annotation (Line(points={{51,70.25},{48,70.25},{48,43.2},{43.68,43.2}},
                                                                          color=
           {255,128,0}));
   connect(varRad.solarRad_out[6], wholeHouseBuildingEnvelope.SolarRadiationPort_RoofS)
-    annotation (Line(points={{51,70.4167},{48,70.4167},{48,34.8},{43.68,34.8}},
+    annotation (Line(points={{51,70.4167},{48,70.4167},{48,35.92},{43.68,35.92}},
         color={255,128,0}));
   connect(heatStarToComb.portConvRadComb, wholeHouseBuildingEnvelope.heatingToRooms) annotation (Line(points={{-28,-20},{-26,-20},{-26,10},{-14,10},{-14,10.16}},        color={191,0,0}));
   connect(constAirEx.y, wholeHouseBuildingEnvelope.AirExchangePort) annotation (
diff --git a/AixLib/ThermalZones/HighOrder/Examples/OFD_1Jan.mo b/AixLib/ThermalZones/HighOrder/Examples/OFD_1Jan.mo
index 63b2f880fb..038da5d6eb 100644
--- a/AixLib/ThermalZones/HighOrder/Examples/OFD_1Jan.mo
+++ b/AixLib/ThermalZones/HighOrder/Examples/OFD_1Jan.mo
@@ -3,15 +3,10 @@ model OFD_1Jan "OFD with TMC, TIR and TRY"
 
   extends Modelica.Icons.Example;
 
-  parameter Integer TIR=3 "Thermal Insulation Regulation" annotation (Dialog(
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation TIR=AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.WSchV_1995 "Thermal Insulation Regulation" annotation (Dialog(
       group="Construction parameters",
       compact=true,
-      descriptionLabel=true), choices(
-      choice=1 "EnEV_2009",
-      choice=2 "EnEV_2002",
-      choice=3 "WSchV_1995",
-      choice=4 "WSchV_1984",
-      radioButtons=true));
+      descriptionLabel=true));
 
   replaceable package MediumAir = AixLib.Media.Air "Medium within the room";
 
@@ -52,10 +47,10 @@ model OFD_1Jan "OFD with TMC, TIR and TRY"
     redeclare model CorrSolarGainWin =
         Components.WindowsDoors.BaseClasses.CorrectionSolarGain.CorGSimple,
     use_infiltEN12831=true,
-    n50=if TIR == 1 or TIR == 2 then 3 else if TIR == 3 then 4 else 6,
+    n50=if TIR == AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.EnEV_2009 or TIR == AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.EnEV_2002 then 3 else if TIR == AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.WSchV_1995 then 4 else 6,
     withDynamicVentilation=true,
     redeclare package Medium = MediumAir,
-    UValOutDoors=if TIR == 1 then 1.8 else 2.9) annotation (Placement(transformation(extent={{-35,-49},{60,46}})));
+    UValOutDoors=if TIR == AixLib.ThermalZones.HighOrder.Components.Types.ThermalInsulationRegulation.EnEV_2009 then 1.8 else 2.9) annotation (Placement(transformation(extent={{-35,-49},{60,46}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature tempOutside
     annotation (Placement(transformation(extent={{-4,53},{-16.5,66}})));
   AixLib.ThermalZones.HighOrder.House.OFD_MiddleInnerLoadWall.EnergySystem.IdealHeaters.GroundFloor
@@ -105,21 +100,20 @@ equation
   connect(tempOutside.T, Weather.AirTemp) annotation (Line(points={{-2.75,59.5},
           {22,59.5},{22,75.8},{75.4,75.8}}, color={0,0,127}));
   connect(Weather.SolarRadiation_OrientedSurfaces[1], OFD.North) annotation (
-      Line(points={{113.48,53.4},{113.48,12.75},{62.85,12.75}},
+      Line(points={{113.48,53.4},{113.48,16.55},{62.85,16.55}},
                                                               color={255,128,0}));
   connect(Weather.SolarRadiation_OrientedSurfaces[2], OFD.East) annotation (
-      Line(points={{113.48,53.4},{113.48,-1.5},{62.85,-1.5}},   color={255,128,0}));
+      Line(points={{113.48,53.4},{113.48,4.2},{62.85,4.2}},     color={255,128,0}));
   connect(Weather.SolarRadiation_OrientedSurfaces[3], OFD.South) annotation (
-      Line(points={{113.48,53.4},{113.48,-15.75},{62.85,-15.75}},
-                                                                color={255,128,0}));
+      Line(points={{113.48,53.4},{113.48,-8.15},{62.85,-8.15}}, color={255,128,0}));
   connect(Weather.SolarRadiation_OrientedSurfaces[4], OFD.West) annotation (
-      Line(points={{113.48,53.4},{113.48,-30},{62.85,-30}},       color={255,128,
+      Line(points={{113.48,53.4},{113.48,-19.55},{62.85,-19.55}}, color={255,128,
           0}));
   connect(Weather.SolarRadiation_OrientedSurfaces[5], OFD.SolarRadiationPort_RoofN)
     annotation (Line(points={{113.48,53.4},{113.48,41.25},{62.85,41.25}}, color=
          {255,128,0}));
   connect(Weather.SolarRadiation_OrientedSurfaces[6], OFD.SolarRadiationPort_RoofS)
-    annotation (Line(points={{113.48,53.4},{113.48,27},{62.85,27}},       color=
+    annotation (Line(points={{113.48,53.4},{113.48,28.9},{62.85,28.9}},   color=
          {255,128,0}));
   connect(NaturalVentilation.y[1], OFD.AirExchangePort[1]) annotation (Line(
         points={{-74,69},{-78,69},{-78,20.0909},{-39.75,20.0909}},   color={0,0,
diff --git a/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/GroundFloorBuildingEnvelope.mo b/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/GroundFloorBuildingEnvelope.mo
index 8acd4d4f07..92d10c1961 100644
--- a/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/GroundFloorBuildingEnvelope.mo
+++ b/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/GroundFloorBuildingEnvelope.mo
@@ -355,7 +355,7 @@ model GroundFloorBuildingEnvelope
         extent={{-10,-10},{10,10}},
         rotation=180,
         origin={110,-4})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
     annotation (Placement(transformation(extent={{-130,12},{-100,42}})));
   Modelica.Blocks.Interfaces.RealInput AirExchangePort[5]
     "1: LivingRoom_GF, 2: Hobby_GF, 3: Corridor, 4: WC_Storage_GF, 5: Kitchen_GF"
@@ -473,10 +473,10 @@ equation
   connect(Corridor.thermRoom, thermCorridor) annotation (Line(points={{64.8,-9},{64.8,-32},{90,-32},{90,100},{110,100},{110,110}},
                                                            color={191,0,0}));
   connect(Livingroom.AirExchangePort, AirExchangePort[1]) annotation (Line(
-        points={{-86.2,66.24},{-86.2,66},{-92,66},{-92,-15},{-115,-15}},
+        points={{-86.2,66.24},{-86.2,66},{-92,66},{-92,-9},{-115,-9}},
         color={0,0,127}));
   connect(Hobby.AirExchangePort, AirExchangePort[2]) annotation (Line(points={{85.9,
-          68.68},{85.9,78},{86,78},{86,88},{-92,88},{-92,-9},{-115,-9}},color={
+          68.68},{85.9,78},{86,78},{86,88},{-92,88},{-92,-6},{-115,-6}},color={
           0,0,127}));
   connect(Kitchen.SolarRadiationPort_OW1, South) annotation (Line(points={{-83.9,
           -61.6},{-90,-61.6},{-90,-92},{90,-92},{90,26},{110,26}}, color={255,
@@ -485,25 +485,25 @@ equation
       Line(points={{44,-10.9},{36,-10.9},{36,-92},{-34,-92},{-34,-48.8},{-46,-48.8}},
         color={191,0,0}));
 
-  connect(Livingroom.ground, groundTemp[1]) annotation (Line(points={{-63.32,
-          13.92},{-63.32,-8},{-32,-8},{-32,-88},{0,-88},{0,-108}},
+  connect(Livingroom.ground, groundTemp[1]) annotation (Line(points={{-63.32,13.92},
+          {-63.32,-8},{-32,-8},{-32,-88},{0,-88},{0,-104}},
                                                color={191,0,0}));
-  connect(Hobby.ground, groundTemp[2]) annotation (Line(points={{66.14,29.44},{
-          66.14,26},{34,26},{34,-88},{0,-88},{0,-104}},
+  connect(Hobby.ground, groundTemp[2]) annotation (Line(points={{66.14,29.44},{66.14,
+          26},{34,26},{34,-88},{0,-88},{0,-102}},
                                                color={191,0,0}));
   connect(Corridor.ground, groundTemp[3]) annotation (Line(points={{63.2,-26.86},{63.2,-34},{34,-34},{34,-88},{0,-88},{0,-100}},
                                         color={191,0,0}));
-  connect(WC_Storage.ground, groundTemp[4]) annotation (Line(points={{64.14,
-          -37.44},{64.14,-34},{34,-34},{34,-88},{0,-88},{0,-96}},
+  connect(WC_Storage.ground, groundTemp[4]) annotation (Line(points={{64.14,-37.44},
+          {64.14,-34},{34,-34},{34,-88},{0,-88},{0,-98}},
                                                 color={191,0,0}));
   connect(Kitchen.ground, groundTemp[5]) annotation (Line(points={{-65.2,-21.92},
-          {-65.2,-14},{-32,-14},{-32,-88},{0,-88},{0,-92}},
+          {-65.2,-14},{-32,-14},{-32,-88},{0,-88},{0,-96}},
                                               color={191,0,0}));
   connect(Corridor.AirExchangePort, AirExchangePort[3]) annotation (Line(points={{84,4.205},{86,4.205},{86,4},{88,4},{88,-90},{-92,-90},{-92,-3},{-115,-3}}, color={0,0,127}));
   connect(WC_Storage.AirExchangePort, AirExchangePort[4]) annotation (Line(points={{83.9,
-          -76.68},{88,-76.68},{88,-90},{-92,-90},{-92,3},{-115,3}},                                                                                color={0,0,127}));
+          -76.68},{88,-76.68},{88,-90},{-92,-90},{-92,0},{-115,0}},                                                                                color={0,0,127}));
   connect(Kitchen.AirExchangePort, AirExchangePort[5]) annotation (Line(points={{-86,
-          -74.24},{-92,-74.24},{-92,9},{-115,9}},                                                                            color={0,0,127}));
+          -74.24},{-92,-74.24},{-92,3},{-115,3}},                                                                            color={0,0,127}));
   connect(heatStarToCombHeaters.portConvRadComb, portConvRadRooms) annotation (Line(points={{0,-18},{0,0}}, color={191,0,0}));
   connect(Livingroom.starRoom, heatStarToCombHeaters[1].portRad) annotation (Line(points={{-58.48,44},{-58,44},{-58,30},{-16,30},{-16,-38},{-5,-38}}, color={0,0,0}));
   connect(Livingroom.thermRoom, heatStarToCombHeaters[1].portConv) annotation (Line(points={{-65.08,44},{-66,44},{-66,26},{-20,26},{-20,-44},{5,-44},{5,-38}}, color={191,0,0}));
@@ -515,37 +515,37 @@ equation
   connect(WC_Storage.thermRoom, heatStarToCombHeaters[4].portConv) annotation (Line(points={{65.66,-60},{66,-60},{66,-44},{5,-44},{5,-38}}, color={191,0,0}));
   connect(Kitchen.starRoom, heatStarToCombHeaters[5].portRad) annotation (Line(points={{-60.8,-52},{-60,-52},{-60,-38},{-5,-38}}, color={0,0,0}));
   connect(Kitchen.thermRoom, heatStarToCombHeaters[5].portConv) annotation (Line(points={{-66.8,-52},{-66,-52},{-66,-44},{5,-44},{5,-38}}, color={191,0,0}));
-  connect(Livingroom.ports[1], portVent_in[1]) annotation (Line(points={{-65.355,
-          11.52},{-58,11.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-76},{104,
-          -76}},
+  connect(Livingroom.ports[1], portVent_in[1]) annotation (Line(points={{-63.6775,
+          11.52},{-58,11.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-72},{104,
+          -72}},
         color={0,127,255}));
-  connect(Livingroom.ports[2], portVent_out[1]) annotation (Line(points={{-58.645,
-          11.52},{-58,11.52},{-58,-8},{-20,-8},{-20,-92},{104,-92}},
+  connect(Livingroom.ports[2], portVent_out[1]) annotation (Line(points={{-60.3225,
+          11.52},{-58,11.52},{-58,-8},{-20,-8},{-20,-88},{104,-88}},
         color={0,127,255}));
-  connect(Hobby.ports[1], portVent_in[2]) annotation (Line(points={{67.8975,27.64},
-          {40,27.64},{40,28},{20,28},{20,-92},{94,-92},{94,-72},{104,-72}},
+  connect(Hobby.ports[1], portVent_in[2]) annotation (Line(points={{66.4487,
+          27.64},{40,27.64},{40,28},{20,28},{20,-92},{94,-92},{94,-70},{104,-70}},
         color={0,127,255}));
-  connect(Hobby.ports[2], portVent_out[2]) annotation (Line(points={{62.1025,27.64},
-          {20,27.64},{20,-92},{94,-92},{94,-84},{104,-84},{104,-88}},
+  connect(Hobby.ports[2], portVent_out[2]) annotation (Line(points={{63.5512,
+          27.64},{20,27.64},{20,-92},{94,-92},{94,-84},{104,-84},{104,-86}},
         color={0,127,255}));
-  connect(Corridor.ports[1], portVent_in[3]) annotation (Line(points={{65.05,-28.285},
+  connect(Corridor.ports[1], portVent_in[3]) annotation (Line(points={{63.525,-28.285},
           {40,-28.285},{40,-28},{20,-28},{20,-92},{94,-92},{94,-68},{104,-68}},
         color={0,127,255}));
-  connect(Corridor.ports[2], portVent_out[3]) annotation (Line(points={{58.95,-28.285},
-          {58.95,-32},{20,-32},{20,-92},{94,-92},{94,-84},{104,-84}},
+  connect(Corridor.ports[2], portVent_out[3]) annotation (Line(points={{60.475,-28.285},
+          {60.475,-32},{20,-32},{20,-92},{94,-92},{94,-84},{104,-84}},
         color={0,127,255}));
-  connect(WC_Storage.ports[1], portVent_in[4]) annotation (Line(points={{65.8975,
-          -35.64},{62,-35.64},{62,-32},{20,-32},{20,-92},{94,-92},{94,-64},{104,
-          -64}},
+  connect(WC_Storage.ports[1], portVent_in[4]) annotation (Line(points={{64.4487,
+          -35.64},{62,-35.64},{62,-32},{20,-32},{20,-92},{94,-92},{94,-66},{104,
+          -66}},
         color={0,127,255}));
-  connect(WC_Storage.ports[2], portVent_out[4]) annotation (Line(points={{60.1025,
-          -35.64},{60.1025,-32},{20,-32},{20,-92},{94,-92},{94,-80},{104,-80}},
+  connect(WC_Storage.ports[2], portVent_out[4]) annotation (Line(points={{61.5512,
+          -35.64},{61.5512,-32},{20,-32},{20,-92},{94,-92},{94,-82},{104,-82}},
         color={0,127,255}));
-  connect(Kitchen.ports[1], portVent_in[5]) annotation (Line(points={{-67.05,-19.52},
-          {-58,-19.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-60},{104,-60}},
+  connect(Kitchen.ports[1], portVent_in[5]) annotation (Line(points={{-65.525,-19.52},
+          {-58,-19.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-64},{104,-64}},
         color={0,127,255}));
-  connect(Kitchen.ports[2], portVent_out[5]) annotation (Line(points={{-60.95,-19.52},
-          {-58,-19.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-76},{104,-76}},
+  connect(Kitchen.ports[2], portVent_out[5]) annotation (Line(points={{-62.475,-19.52},
+          {-58,-19.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-80},{104,-80}},
         color={0,127,255}));
   annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
             {100,100}}), graphics={
diff --git a/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/UpperFloorBuildingEnvelope.mo b/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/UpperFloorBuildingEnvelope.mo
index ebff0df19f..272f6627b3 100644
--- a/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/UpperFloorBuildingEnvelope.mo
+++ b/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/UpperFloorBuildingEnvelope.mo
@@ -373,7 +373,7 @@ model UpperFloorBuildingEnvelope
         extent={{-10,-10},{10,10}},
         rotation=180,
         origin={110,-36})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
     annotation (Placement(transformation(extent={{-130,10},{-100,40}})));
   Modelica.Blocks.Interfaces.RealInput AirExchangePort[5]
     "1(6): Bedroom_UF, 2(7): Child1_UF, 3(8): Corridor_UF, 4(9): Bath_UF, 5(10): Child2_UF"
@@ -544,45 +544,47 @@ equation
   connect(Children2.starRoom, heatStarToCombHeaters[5].portRad) annotation (Line(points={{-60.8,-52},{-60.8,-38},{-5,-38}}, color={0,0,0}));
   connect(Children2.thermRoom, heatStarToCombHeaters[5].portConv) annotation (Line(points={{-66.8,-52},{-66,-52},{-66,-36},{-18,-36},{-18,-42},{5,-42},{5,-38}}, color={191,0,0}));
   connect(AirExchangePort[1], Bedroom.AirExchangePort) annotation (Line(points={{-115,
-          -23},{-92,-23},{-92,68.24},{-84,68.24}},                                                                             color={0,0,127}));
+          -17},{-92,-17},{-92,68.24},{-84,68.24}},                                                                             color={0,0,127}));
   connect(AirExchangePort[2], Children1.AirExchangePort) annotation (Line(points={{-115,
-          -17},{-96,-17},{-96,88},{88,88},{88,68.68},{79.9,68.68}},                                                                               color={0,0,127}));
+          -14},{-96,-14},{-96,88},{88,88},{88,68.68},{79.9,68.68}},                                                                               color={0,0,127}));
   connect(AirExchangePort[3], Corridor.AirExchangePort) annotation (Line(points={{-115,
           -11},{-96,-11},{-96,88},{88,88},{88,4.205},{80,4.205}},                                                                              color={0,0,127}));
-  connect(AirExchangePort[4], Bath.AirExchangePort) annotation (Line(points={{-115,-5},
-          {-96,-5},{-96,88},{88,88},{88,-76.68},{81.9,-76.68}},                                                                              color={0,0,127}));
-  connect(AirExchangePort[5], Children2.AirExchangePort) annotation (Line(points={{-115,1},
-          {-92,1},{-92,-74.24},{-86,-74.24}},                                                                                  color={0,0,127}));
-  connect(Bedroom.ports[1], portVent_in[1]) annotation (Line(points={{-65.05,13.52},
-          {-58,13.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-76},{104,-76}},
+  connect(AirExchangePort[4], Bath.AirExchangePort) annotation (Line(points={{-115,-8},
+          {-96,-8},{-96,88},{88,88},{88,-76.68},{81.9,-76.68}},                                                                              color={0,0,127}));
+  connect(AirExchangePort[5], Children2.AirExchangePort) annotation (Line(points={{-115,-5},
+          {-92,-5},{-92,-74.24},{-86,-74.24}},                                                                                 color={0,0,127}));
+  connect(Bedroom.ports[1], portVent_in[1]) annotation (Line(points={{-63.525,13.52},
+          {-58,13.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-72},{104,-72}},
         color={0,127,255}));
-  connect(Bedroom.ports[2], portVent_out[1]) annotation (Line(points={{-58.95,13.52},
-          {-58,13.52},{-58,-8},{-20,-8},{-20,-92},{104,-92}},
+  connect(Bedroom.ports[2], portVent_out[1]) annotation (Line(points={{-60.475,13.52},
+          {-58,13.52},{-58,-8},{-20,-8},{-20,-88},{104,-88}},
         color={0,127,255}));
-  connect(Children1.ports[1], portVent_in[2]) annotation (Line(points={{61.8975,
-          27.64},{40,27.64},{40,28},{20,28},{20,-92},{94,-92},{94,-72},{104,-72}},
+  connect(Children1.ports[1], portVent_in[2]) annotation (Line(points={{60.4488,
+          27.64},{40,27.64},{40,28},{20,28},{20,-92},{94,-92},{94,-70},{104,-70}},
         color={0,127,255}));
-  connect(Children1.ports[2], portVent_out[2]) annotation (Line(points={{56.1025,
-          27.64},{20,27.64},{20,-92},{94,-92},{94,-84},{104,-84},{104,-88}},
+  connect(Children1.ports[2], portVent_out[2]) annotation (Line(points={{57.5512,
+          27.64},{20,27.64},{20,-92},{94,-92},{94,-84},{104,-84},{104,-86}},
         color={0,127,255}));
-  connect(Corridor.ports[1], portVent_in[3]) annotation (Line(points={{61.05,-28.285},
+  connect(Corridor.ports[1], portVent_in[3]) annotation (Line(points={{59.525,-28.285},
           {40,-28.285},{40,-28},{20,-28},{20,-92},{94,-92},{94,-68},{104,-68}},
         color={0,127,255}));
-  connect(Corridor.ports[2], portVent_out[3]) annotation (Line(points={{54.95,-28.285},
-          {54.95,-32},{20,-32},{20,-92},{94,-92},{94,-84},{104,-84}},
+  connect(Corridor.ports[2], portVent_out[3]) annotation (Line(points={{56.475,-28.285},
+          {56.475,-32},{20,-32},{20,-92},{94,-92},{94,-84},{104,-84}},
         color={0,127,255}));
-  connect(Bath.ports[1], portVent_in[4]) annotation (Line(points={{63.8975,-35.64},
-          {62,-35.64},{62,-32},{20,-32},{20,-92},{94,-92},{94,-64},{104,-64}},
+  connect(Bath.ports[1], portVent_in[4]) annotation (Line(points={{62.4488,
+          -35.64},{62,-35.64},{62,-32},{20,-32},{20,-92},{94,-92},{94,-66},{104,
+          -66}},
         color={0,127,255}));
-  connect(Bath.ports[2], portVent_out[4]) annotation (Line(points={{58.1025,-35.64},
-          {58.1025,-32},{20,-32},{20,-92},{94,-92},{94,-80},{104,-80}},
+  connect(Bath.ports[2], portVent_out[4]) annotation (Line(points={{59.5512,
+          -35.64},{59.5512,-32},{20,-32},{20,-92},{94,-92},{94,-82},{104,-82}},
         color={0,127,255}));
-  connect(Children2.ports[1], portVent_in[5]) annotation (Line(points={{-67.05,-19.52},
-          {-58,-19.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-60},{104,-60}},
+  connect(Children2.ports[1], portVent_in[5]) annotation (Line(points={{-65.525,
+          -19.52},{-58,-19.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-64},{104,
+          -64}},
         color={0,127,255}));
-  connect(Children2.ports[2], portVent_out[5]) annotation (Line(points={{-60.95,
-          -19.52},{-58,-19.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-76},{104,
-          -76}},
+  connect(Children2.ports[2], portVent_out[5]) annotation (Line(points={{-62.475,
+          -19.52},{-58,-19.52},{-58,-8},{-20,-8},{-20,-92},{94,-92},{94,-80},{104,
+          -80}},
         color={0,127,255}));
 
   annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
diff --git a/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/WholeHouseBuildingEnvelope.mo b/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/WholeHouseBuildingEnvelope.mo
index 736b15d066..0d701b63aa 100644
--- a/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/WholeHouseBuildingEnvelope.mo
+++ b/AixLib/ThermalZones/HighOrder/House/OFD_MiddleInnerLoadWall/BuildingEnvelope/WholeHouseBuildingEnvelope.mo
@@ -192,7 +192,7 @@ model WholeHouseBuildingEnvelope
     alfa=1.5707963267949,
     replaceable package Medium = Medium) annotation (Placement(transformation(extent={{-22,44},{22,82}})));
 
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
                                                      annotation (Placement(
         transformation(extent={{-128,66},{-100,94}}),iconTransformation(extent={{-120,60},{-100,80}})));
   Modelica.Blocks.Interfaces.RealInput AirExchangePort[11] "1: LivingRoom_GF, 2: Hobby_GF, 3: Corridor_GF, 4: WC_Storage_GF, 5: Kitchen_GF, 6: Bedroom_UF, 7: Child1_UF, 8: Corridor_UF, 9: Bath_UF, 10: Child2_UF, 11: Attic"
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/ASHRAE140/EastWestFacingWindows.mo b/AixLib/ThermalZones/HighOrder/Rooms/ASHRAE140/EastWestFacingWindows.mo
index c04d3d95d7..28e8452295 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/ASHRAE140/EastWestFacingWindows.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/ASHRAE140/EastWestFacingWindows.mo
@@ -60,7 +60,7 @@ model EastWestFacingWindows "windows facing south and west"
       wallPar=wallTypes.groundPlate_upp_half,
       outside=false),
     ceiling(
-      ISOrientation=3,
+      ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling,
       withDoor=false,
       wallPar=wallTypes.roof,
       outside=true,
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoom.mo b/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoom.mo
index 4c82e956b6..3da2ca15b3 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoom.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoom.mo
@@ -1,4 +1,4 @@
-within AixLib.ThermalZones.HighOrder.Rooms.BaseClasses;
+within AixLib.ThermalZones.HighOrder.Rooms.BaseClasses;
 partial model PartialRoom "Partial model with base component that are necessary for all HOM rooms"
   extends PartialRoomParams;
   extends AixLib.Fluid.Interfaces.LumpedVolumeDeclarations(redeclare package
@@ -126,14 +126,11 @@ protected
  if use_moisture_balance
     "Converter for latent heat flow rate"
     annotation (Placement(transformation(extent={{58,-52},{46,-40}})));
-  Modelica.Blocks.Interfaces.RealOutput hum_internal
-    "internal humidity (used for case with no moisture balance";
-  Modelica.Blocks.Interfaces.RealOutput mWat_flow_internal
+  Modelica.Blocks.Interfaces.RealOutput hum_internal = 0  if not use_moisture_balance
+    "internal humidity (used for case with no moisture balance)";
+  Modelica.Blocks.Interfaces.RealOutput mWat_flow_internal = 0 if not use_moisture_balance
     "internal mass flow rate of water vapor (used for case with no moisture balance)";
 equation
-  hum_internal = 0;
-  mWat_flow_internal = 0;
-
   connect(QLat_flow, sumQLat_flow.u[2]) annotation (Line(
       points={{-112,-56},{80,-56},{80,-36.475},{76,-36.475}},
       color={0,0,127},
@@ -147,10 +144,19 @@ equation
       points={{-4,-16},{-14,-16},{-14,-14.88},{-22.6,-14.88}},
       color={0,0,127},
       pattern=LinePattern.Dash));
-  connect(NaturalVentilation.HumIn, ventHum) annotation (Line(
-      points={{-33.4,-21},{-62,-21},{-62,-22},{-74,-22},{-74,-37},{-111,-37}},
+  if use_moisture_balance then
+    connect(NaturalVentilation.HumIn, ventHum) annotation (Line(
+        points={{-33.4,-21},{-62,-21},{-62,-22},{-74,-22},{-74,-37},{-111,-37}},
+        color={0,0,127},
+        pattern=LinePattern.Dash));
+    connect(mWat_flow.y, airload.mWat_flow) annotation (Line(
+      points={{47.6,-28},{36,-28},{36,-10},{26,-10},{26,-4},{20,-4}},
       color={0,0,127},
       pattern=LinePattern.Dash));
+  else
+    connect(NaturalVentilation.HumIn, hum_internal);
+    connect(airload.mWat_flow, mWat_flow_internal);
+  end if;
   connect(conQLat_flow.port, airload.heatPort) annotation (Line(
       points={{46,-46},{24,-46},{24,-12},{18,-12}},
       color={191,0,0},
@@ -204,13 +210,9 @@ equation
       points={{69.49,-37},{64,-37},{64,-46},{58,-46}},
       color={0,0,127},
       pattern=LinePattern.Dash));
-  connect(mWat_flow.y, airload.mWat_flow) annotation (Line(
-      points={{47.6,-28},{36,-28},{36,-10},{26,-10},{26,-4},{20,-4}},
-      color={0,0,127},
-      pattern=LinePattern.Dash));
 
-  connect(NaturalVentilation.HumIn, hum_internal);
-  connect(airload.mWat_flow, mWat_flow_internal);
+
+
     annotation (Dialog(tab="Infiltration acc. to EN 12831 (building airtightness"),
               Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(coordinateSystem(preserveAspectRatio=false)),
     Documentation(revisions="<html><ul>
@@ -218,7 +220,10 @@ equation
     Model added to the AixLib library.
   </li>
   <li>February, 2022 by Fabian Wüllhorst and Martin Kremer:<br/>
-    Changed airLoad-model to mxing volume to use media model. Added possibility to analyse substance and water vapor balance (see issue <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1123\">#1123</a>)
+  Changed airLoad-model to mxing volume to use media model. Added possibility to analyse substance and water vapor balance (see issue <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1123\">#1123</a>)
+  </li>
+  <li>November, 2023 by Benani Zoumba:<br/>
+  Changed connections for moisture balance <a href=\"https://github.com/RWTH-EBC/AixLib/issues/1460\">#1460</a>)
 </ul>
 </html>", info="<html>
 <p>This model provides a basic configuration of an air load, a replaceable parameter set for wall paramters and air exchange models that can be used to build up individual High-Order-Models for rooms.</p>
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoomFourWalls.mo b/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoomFourWalls.mo
index a682b4fcef..b8c2763d10 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoomFourWalls.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoomFourWalls.mo
@@ -17,8 +17,7 @@ partial model PartialRoomFourWalls
   parameter Modelica.Units.SI.Area Win_Area=12 "Window area " annotation (
       Dialog(
       group="Windows",
-      descriptionLabel=true,
-      enable=withWindow1));
+      descriptionLabel=true));
 
   parameter Boolean use_shortWaveRadIn=true
     "Use bus connector for incoming shortwave radiation"
@@ -31,13 +30,13 @@ partial model PartialRoomFourWalls
     annotation (Dialog(tab="Inner walls", group="Shortwave Radiation", enable=
           use_shortWaveRadIn));
 
-  parameter Components.Types.selectorCoefficients absInnerWallSurf if use_shortWaveRadIn
+  parameter Components.Types.selectorCoefficients absInnerWallSurf=AixLib.ThermalZones.HighOrder.Components.Types.selectorCoefficients.abs06
     "Coefficients for interior solar absorptance of wall surface abs={0.6, 0.9, 0.1}"
     annotation (Dialog(tab="Inner walls", group="Shortwave Radiation", enable=
           use_shortWaveRadIn and not use_dynamicShortWaveRadMethod));
 
   replaceable parameter
-    ThermalZones.HighOrder.Components.Types.PartialCoeffTable coeffTableSolDistrFractions if use_shortWaveRadIn
+    ThermalZones.HighOrder.Components.Types.CoeffTableEastWestWindow coeffTableSolDistrFractions
     constrainedby
     AixLib.ThermalZones.HighOrder.Components.Types.PartialCoeffTable(final abs=absInnerWallSurf)
     "Record holding the values to reproduce the tables"
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoomParams.mo b/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoomParams.mo
index 81aa87088f..9e2c238351 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoomParams.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/BaseClasses/PartialRoomParams.mo
@@ -26,43 +26,32 @@ partial model PartialRoomParams "Partial model with base parameters that are nec
 
   //// Inner / Interior wall parameters
   // Heat convection
-  parameter Integer calcMethodIn=1
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A
     "Calculation method of convective heat transfer coefficient at inside surface"
     annotation (Dialog(
       tab="Inner walls",
       group="Heat convection",
       compact=true,
-      descriptionLabel=true), choices(
-      choice=1 "EN ISO 6946 Appendix A >>Flat Surfaces<<",
-      choice=2 "By Bernd Glueck",
-      choice=3 "Custom hCon (constant)",
-      choice=4 "ASHRAE140-2017",
-      radioButtons=true));
+      descriptionLabel=true));
 
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConIn_const=2.5
     "Custom convective heat transfer coefficient (just for manual selection, not recommended)"
     annotation (Dialog(
       tab="Inner walls",
       group="Heat convection",
-      enable=(calcMethodIn == 3)));
+      enable=(calcMethodIn == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon)));
 
-  parameter Integer radLongCalcMethod=1 "Calculation method for longwave radiation heat transfer"
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer radLongCalcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.No_approx "Calculation method for longwave radiation heat transfer"
     annotation (
     Evaluate=true,
-    Dialog(tab="Inner walls", group="Longwave radiation",   compact=true),
-    choices(
-      choice=1 "No approx",
-      choice=2 "Linear approx at wall temp",
-      choice=3 "Linear approx at rad temp",
-      choice=4 "Linear approx at constant T_ref",
-      radioButtons=true));
+    Dialog(tab="Inner walls", group="Longwave radiation",   compact=true));
   parameter Modelica.Units.SI.Temperature T_ref=
       Modelica.Units.Conversions.from_degC(16)
     "Reference temperature for optional linearization of longwave radiation"
     annotation (Dialog(
       tab="Inner walls",
       group="Longwave radiation",
-      enable=radLongCalcMethod == 4));
+      enable=radLongCalcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.Linear_constant_T_ref));
 
   //// Outer / Exterior wall parameters
   //Window type
@@ -83,23 +72,19 @@ partial model PartialRoomParams "Partial model with base parameters that are nec
   parameter Real solar_absorptance_OW(min=0, max=1)=0.6 "Solar absoptance outer walls "
     annotation (Dialog(tab="Outer walls", group="Solar absorptance", descriptionLabel=true));
   // Heat convection
-  parameter Integer calcMethodOut=1 "Calculation method for convective heat transfer coefficient"
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 "Calculation method for convective heat transfer coefficient"
                                                                                                annotation (Dialog(
       tab="Outer walls",
       group="Heat convection",
       compact=true,
-      descriptionLabel=true), choices(
-      choice=1 "DIN 6946",
-      choice=2 "ASHRAE Fundamentals",
-      choice=3 "Custom hCon (constant)",
-      radioButtons=true));
-  replaceable parameter DataBase.Surfaces.RoughnessForHT.PolynomialCoefficients_ASHRAEHandbook surfaceType=DataBase.Surfaces.RoughnessForHT.Brick_RoughPlaster() "Surface type of outside wall" annotation (Dialog(tab="Outer walls", group="Heat convection", enable=(calcMethodOut == 2)));
+      descriptionLabel=true));
+  replaceable parameter DataBase.Surfaces.RoughnessForHT.PolynomialCoefficients_ASHRAEHandbook surfaceType=DataBase.Surfaces.RoughnessForHT.Brick_RoughPlaster() "Surface type of outside wall" annotation (Dialog(tab="Outer walls", group="Heat convection", enable=(calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)));
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConOut_const=25
     "Custom convective heat transfer coefficient (just for manual selection, not recommended)"
     annotation (Dialog(
       tab="Outer walls",
       group="Heat convection",
-      enable=(calcMethodOut == 3)));
+      enable=(calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.Custom_hCon)));
   // Sunblind
   parameter Boolean use_sunblind = false
     "Will sunblind become active automatically?"
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Attic_Ro2Lf5.mo b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Attic_Ro2Lf5.mo
index 10809aac6a..6af319b29f 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Attic_Ro2Lf5.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Attic_Ro2Lf5.mo
@@ -131,7 +131,7 @@ model Attic_Ro2Lf5
     windowarea=windowarea_RO1,
     wall_length=length,
     wall_height=roof_width1,
-    ISOrientation=1,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -162,7 +162,7 @@ model Attic_Ro2Lf5
     withWindow=withWindow2,
     windowarea=windowarea_RO2,
     wall_length=length,
-    ISOrientation=1,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -189,7 +189,7 @@ model Attic_Ro2Lf5
     wall_length=room2_length,
     wall_height=room2_width,
     withWindow=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     outside=false,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
@@ -217,7 +217,7 @@ model Attic_Ro2Lf5
     wall_length=room1_length,
     wall_height=room1_width,
     withWindow=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     outside=false,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
@@ -246,7 +246,7 @@ model Attic_Ro2Lf5
     wall_length=room3_length,
     wall_height=room3_width,
     withWindow=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     outside=false,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
@@ -274,7 +274,7 @@ model Attic_Ro2Lf5
     wall_length=room4_length,
     wall_height=room4_width,
     withWindow=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     outside=false,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
@@ -302,7 +302,7 @@ model Attic_Ro2Lf5
     wall_length=room5_length,
     wall_height=room5_width,
     withWindow=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     outside=false,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
@@ -331,7 +331,7 @@ model Attic_Ro2Lf5
     door_height=0,
     door_width=0,
     windowarea=windowarea_RO1,
-    ISOrientation=1,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall,
     wall_length=sqrt(VerticalWall_Area),
     wall_height=sqrt(VerticalWall_Area),
     withWindow=false,
@@ -359,7 +359,7 @@ model Attic_Ro2Lf5
     door_height=0,
     door_width=0,
     windowarea=windowarea_RO1,
-    ISOrientation=1,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall,
     wall_length=sqrt(VerticalWall_Area),
     wall_height=sqrt(VerticalWall_Area),
     withWindow=false,
@@ -408,7 +408,7 @@ model Attic_Ro2Lf5
         extent={{-10,-10},{10,10}},
         rotation=270,
         origin={-50,90})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
                                                      annotation (Placement(
         transformation(extent={{-119.5,-10},{-99.5,10}}), iconTransformation(
           extent={{-119.5,10},{-99.5,30}})));
@@ -425,21 +425,21 @@ equation
           255,128,0}));
   connect(SolarRadiationPort_RO2, roof2.SolarRadiationPort) annotation (Line(
         points={{48,100},{48,80},{71.75,80},{71.75,65.5}}, color={255,128,0}));
-  connect(roof1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-19.7333,64.25},{-19.7333,80},{-80,80},{-80,0},{-109.5,0}},
-                                                                     color={0,0,
+  connect(roof1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{
+          -19.7333,64.25},{-19.7333,80},{-80,80},{-80,0},{-109.5,0}},color={0,0,
           127}));
   connect(roof2.WindSpeedPort, WindSpeedPort) annotation (Line(points={{66.8,64.25},{66.8,80},{-80,80},{-80,0},{-109.5,0}},
                                                         color={0,0,127}));
   connect(floorRoom1.port_outside, thermRoom1) annotation (Line(points={{-60,-46.1},{-60,-90},{-90,-90}},
                                 color={191,0,0}));
-  connect(floorRoom2.port_outside, thermRoom2) annotation (Line(points={{-29,-46.1},{-29,-90},{-50,-90}},
-                                       color={191,0,0}));
+  connect(floorRoom2.port_outside, thermRoom2) annotation (Line(points={{-29,
+          -46.1},{-29,-90},{-50,-90}}, color={191,0,0}));
   connect(thermRoom3, floorRoom3.port_outside)
     annotation (Line(points={{-10,-90},{3,-90},{3,-46.1}}, color={191,0,0}));
-  connect(thermRoom4, floorRoom4.port_outside) annotation (Line(points={{30,-90},{38,-90},{38,-70},{35,-70},{35,-46.1}},
-                                                  color={191,0,0}));
-  connect(floorRoom5.port_outside, thermRoom5) annotation (Line(points={{69,-46.1},{69,-84},{72,-84},{72,-88},{70,-88},{70,-90}},
-                                                                color={191,0,0}));
+  connect(thermRoom4, floorRoom4.port_outside) annotation (Line(points={{30,-90},
+          {38,-90},{38,-70},{35,-70},{35,-46.1}}, color={191,0,0}));
+  connect(floorRoom5.port_outside, thermRoom5) annotation (Line(points={{69,
+          -46.1},{69,-84},{72,-84},{72,-88},{70,-88},{70,-90}}, color={191,0,0}));
   connect(OW1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-81.2,-6.6},{-86,-6.6},{-86,0},{-109.5,0}},
                                          color={0,0,127}));
   connect(OW1.SolarRadiationPort, SolarRadiationPort_OW1) annotation (Line(
@@ -450,16 +450,22 @@ equation
   connect(OW2.SolarRadiationPort, SolarRadiationPort_OW2) annotation (Line(
         points={{90.2,3.25},{100,3.25},{100,-18},{110,-18}}, color={255,128,0}));
   connect(thermOutside, roof2.port_outside) annotation (Line(points={{-100,100},{-98,100},{-98,98},{-88,98},{-88,74},{47,74},{47,64.25}}, color={191,0,0}));
-  connect(thermOutside, roof1.port_outside) annotation (Line(points={{-100,100},{-88,100},{-88,74},{-41,74},{-41,64.25}}, color={191,0,0}));
+  connect(thermOutside, roof1.port_outside) annotation (Line(points={{-100,100},
+          {-88,100},{-88,74},{-41,74},{-41,64.25}},                                                                       color={191,0,0}));
 
   connect(thermOutside, OW1.port_outside) annotation (Line(points={{-100,100},{-84,100},{-84,-22},{-81.2,-22}}, color={191,0,0}));
   connect(floorRoom1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-60,-42},{-60,-40},{-7,-40},{-7,-8}},              color={191,0,0}));
-  connect(floorRoom2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-29,-42},{-7,-42},{-7,-8}},              color={191,0,0}));
-  connect(floorRoom3.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{3,-42},{4,-42},{4,-38},{-7,-38},{-7,-8}},              color={191,0,0}));
-  connect(floorRoom4.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{35,-42},{36,-42},{36,-38},{-7,-38},{-7,-8}},              color={191,0,0}));
-  connect(floorRoom5.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{69,-42},{68,-42},{68,-38},{-7,-38},{-7,-8}},              color={191,0,0}));
+  connect(floorRoom2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-29,-42},
+          {-7,-42},{-7,-8}},                                                                                                                   color={191,0,0}));
+  connect(floorRoom3.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{3,-42},
+          {4,-42},{4,-38},{-7,-38},{-7,-8}},                                                                                                                 color={191,0,0}));
+  connect(floorRoom4.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{35,-42},
+          {36,-42},{36,-38},{-7,-38},{-7,-8}},                                                                                                                  color={191,0,0}));
+  connect(floorRoom5.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{69,-42},
+          {68,-42},{68,-38},{-7,-38},{-7,-8}},                                                                                                                  color={191,0,0}));
   connect(OW1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-73,-22},{-56,-22},{-56,-40},{-7,-40},{-7,-8}},              color={191,0,0}));
-  connect(roof1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-41,54},{-41,48},{-58,48},{-58,-22},{-56,-22},{-56,-40},{-7,-40},{-7,-8}},              color={191,0,0}));
+  connect(roof1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-41,54},
+          {-41,48},{-58,48},{-58,-22},{-56,-22},{-56,-40},{-7,-40},{-7,-8}},                                                                                                             color={191,0,0}));
   connect(roof2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{47,54},{48,54},{48,46},{-58,46},{-58,-22},{-56,-22},{-56,-40},{-7,-40},{-7,-8}},              color={191,0,0}));
   connect(OW2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{81,-16},{76,-16},{76,-38},{-7,-38},{-7,-8}}, color={191,0,0}));
   connect(OW2.port_outside, thermOutside) annotation (Line(points={{89.2,-16},{94,-16},{94,100},{-100,100},{-100,100}}, color={191,0,0}));
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow1IwL2IwS1Gr1Uf1.mo b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow1IwL2IwS1Gr1Uf1.mo
index e547679e45..017d3aec2c 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow1IwL2IwS1Gr1Uf1.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow1IwL2IwS1Gr1Uf1.mo
@@ -187,7 +187,7 @@ model Ow1IwL2IwS1Gr1Uf1
     wall_height=room_width,
     withWindow=false,
     withDoor=false,
-    ISOrientation=3,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -216,7 +216,7 @@ model Ow1IwL2IwS1Gr1Uf1
     wall_height=room_width,
     withWindow=false,
     withDoor=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)      annotation (Placement(transformation(
         origin={-27,-60},
@@ -254,7 +254,7 @@ model Ow1IwL2IwS1Gr1Uf1
     annotation (Placement(transformation(extent={{34,-104},{54,-84}})));
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a thermInsideWall2a
     annotation (Placement(transformation(extent={{80,20},{100,40}})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
                                                      annotation (Placement(
         transformation(extent={{-119.5,-70},{-99.5,-50}}), iconTransformation(
           extent={{-109.5,-70},{-89.5,-50}})));
@@ -272,18 +272,18 @@ model Ow1IwL2IwS1Gr1Uf1
 equation
   connect(thermInsideWall3, thermInsideWall3)
     annotation (Line(points={{44,-94},{44,-94}}, color={191,0,0}));
-  connect(inside_wall3.port_outside, thermInsideWall3) annotation (Line(points={{25,-64.25},{25,-77.375},{44,-77.375},{44,-94}},
-                                                            color={191,0,0}));
+  connect(inside_wall3.port_outside, thermInsideWall3) annotation (Line(points={{25,
+          -64.25},{25,-77.375},{44,-77.375},{44,-94}},      color={191,0,0}));
   connect(inside_wall2b.port_outside, thermInsideWall2b) annotation (Line(
         points={{64.15,-17},{77.225,-17},{77.225,-10},{90,-10}}, color={191,0,0}));
   connect(inside_wall2a.port_outside, thermInsideWall2a) annotation (Line(
         points={{64.15,23},{78.225,23},{78.225,30},{90,30}}, color={191,0,0}));
-  connect(inside_wall1.port_outside, thermInsideWall1) annotation (Line(points={{23,64.2502},{23,76.3751},{30,76.3751},{30,90}},
-                                                            color={191,0,0}));
+  connect(inside_wall1.port_outside, thermInsideWall1) annotation (Line(points={{23,
+          64.2502},{23,76.3751},{30,76.3751},{30,90}},      color={191,0,0}));
   connect(Ceiling.port_outside, thermCeiling)
     annotation (Line(points={{-31,62.1},{-31,70},{90,70}}, color={191,0,0}));
-  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-60.25,34.5333},{-80,34.5333},{-80,-60},{-109.5,-60}},
-                                                                 color={0,0,127}));
+  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-60.25,
+          34.5333},{-80,34.5333},{-80,-60},{-109.5,-60}},        color={0,0,127}));
   connect(SolarRadiationPort_OW1, outside_wall1.SolarRadiationPort) annotation (
      Line(points={{-99.5,60},{-80,60},{-80,39.6667},{-61.5,39.6667}}, color={
           255,128,0}));
@@ -297,7 +297,8 @@ equation
   connect(inside_wall3.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{25,-54},{24,-54},{24,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
   connect(inside_wall2b.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,-17},{56,-17},{56,-16},{50,-16},{50,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
   connect(inside_wall2a.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,23},{56,23},{56,22},{50,22},{50,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
-  connect(inside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{23,54},{24,54},{24,44},{50,44},{50,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
+  connect(inside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{23,54},
+          {24,54},{24,44},{50,44},{50,-48},{-7,-48},{-7,-8}},                                                                                                                   color={191,0,0}));
   connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-31,58},{-30,58},{-30,44},{50,44},{50,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
   connect(outside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-50,14},{-44,14},{-44,44},{50,44},{50,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
   connect(outside_wall1.port_outside, thermOutside) annotation (Line(points={{-60.25,14},{-78,14},{-78,100},{-100,100}}, color={191,0,0}));
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow1IwL2IwS1Lf1At1Ro1.mo b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow1IwL2IwS1Lf1At1Ro1.mo
index c9081379a7..4e2ac62d9e 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow1IwL2IwS1Lf1At1Ro1.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow1IwL2IwS1Lf1At1Ro1.mo
@@ -172,7 +172,7 @@ model Ow1IwL2IwS1Lf1At1Ro1
     wall_height=room_width_short,
     withWindow=false,
     withDoor=false,
-    ISOrientation=3,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -201,7 +201,7 @@ model Ow1IwL2IwS1Lf1At1Ro1
     wall_height=room_width_long,
     withWindow=false,
     withDoor=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)      annotation (Placement(transformation(
         origin={-24,-60},
@@ -259,7 +259,7 @@ model Ow1IwL2IwS1Lf1At1Ro1
     wall_height=roof_width,
     withWindow=withWindow3,
     windowarea=windowarea_RO,
-    ISOrientation=1,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -271,7 +271,7 @@ model Ow1IwL2IwS1Lf1At1Ro1
         iconTransformation(extent={{20,-100},{40,-80}})));
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a thermInsideWall2a
     annotation (Placement(transformation(extent={{80,0},{100,20}})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
     annotation (Placement(transformation(extent={{-119.5,-70},{-99.5,-50}}), iconTransformation(extent={{-109.5,-60},{-89.5,-40}})));
   Utilities.Interfaces.SolarRad_in SolarRadiationPort_OW1
     annotation (Placement(transformation(extent={{-109.5,20},{-89.5,40}})));
@@ -292,8 +292,8 @@ model Ow1IwL2IwS1Lf1At1Ro1
         iconTransformation(extent={{-20,80},{0,100}})));
 
 equation
-  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-60.25,38.2667},{-80,38.2667},{-80,-60},{-109.5,-60}},
-                                                                 color={0,0,127}));
+  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-60.25,
+          38.2667},{-80,38.2667},{-80,-60},{-109.5,-60}},        color={0,0,127}));
   connect(outside_wall1.SolarRadiationPort, SolarRadiationPort_OW1) annotation (
      Line(points={{-61.5,43.5833},{-80,43.5833},{-80,30},{-99.5,30}}, color={0,
           0,0}));
@@ -301,8 +301,8 @@ equation
           {{20,-64.2},{20,-74},{30,-74},{30,-90}}, color={191,0,0}));
   connect(thermInsideWall3, thermInsideWall3)
     annotation (Line(points={{30,-90},{30,-90}}, color={191,0,0}));
-  connect(Ceiling.port_outside, thermCeiling) annotation (Line(points={{28,62.1},{28,72},{92,72},{92,50},{90,50}},
-                                            color={191,0,0}));
+  connect(Ceiling.port_outside, thermCeiling) annotation (Line(points={{28,62.1},
+          {28,72},{92,72},{92,50},{90,50}}, color={191,0,0}));
   connect(inside_wall2b.port_outside, thermInsideWall2b)
     annotation (Line(points={{64.15,-20},{90,-20},{90,-30}}, color={191,0,0}));
   connect(inside_wall2a.port_outside, thermInsideWall2a) annotation (Line(
@@ -311,20 +311,25 @@ equation
     annotation (Line(points={{-14,62.2},{-14,90},{-10,90}}, color={191,0,0}));
   connect(roof.SolarRadiationPort, SolarRadiationPort_Roof) annotation (Line(
         points={{72.6667,62.9},{72.6667,72},{74,72},{74,100}}, color={255,128,0}));
-  connect(roof.WindSpeedPort, WindSpeedPort) annotation (Line(points={{69.7333,62.15},{69.7333,72},{-80,72},{-80,-60},{-109.5,-60}},
-                                                               color={0,0,127}));
+  connect(roof.WindSpeedPort, WindSpeedPort) annotation (Line(points={{69.7333,
+          62.15},{69.7333,72},{-80,72},{-80,-60},{-109.5,-60}},color={0,0,127}));
   connect(thermFloor, floor.port_outside) annotation (Line(
       points={{-6,-94},{-8,-94},{-8,-66},{-22,-66},{-22,-62.1},{-24,-62.1}},
       color={191,0,0},
       pattern=LinePattern.Dash));
   connect(thermOutside, outside_wall1.port_outside) annotation (Line(points={{-100,100},{-78,100},{-78,17},{-60.25,17}}, color={191,0,0}));
-  connect(roof.port_outside, thermOutside) annotation (Line(points={{58,62.15},{58,76},{-62,76},{-62,100},{-100,100}}, color={191,0,0}));
-  connect(floor.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-24,-58},{-24,-46},{-7,-46},{-7,-8}},              color={191,0,0}));
+  connect(roof.port_outside, thermOutside) annotation (Line(points={{58,62.15},
+          {58,76},{-62,76},{-62,100},{-100,100}},                                                                      color={191,0,0}));
+  connect(floor.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-24,-58},
+          {-24,-46},{-7,-46},{-7,-8}},                                                                                                              color={191,0,0}));
   connect(inside_wall3.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{20,-56},{20,-46},{-7,-46},{-7,-8}},              color={191,0,0}));
-  connect(inside_wall2b.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,-20},{48,-20},{48,-46},{-7,-46},{-7,-8}},              color={191,0,0}));
+  connect(inside_wall2b.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,-20},
+          {48,-20},{48,-46},{-7,-46},{-7,-8}},                                                                                                                     color={191,0,0}));
   connect(inside_wall2a.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,19},{48,19},{48,-46},{-7,-46},{-7,-8}},              color={191,0,0}));
-  connect(roof.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,56},{58,50},{48,50},{48,-46},{-7,-46},{-7,-8}},              color={191,0,0}));
-  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{28,58},{28,48},{48,48},{48,-46},{-7,-46},{-7,-8}},              color={191,0,0}));
+  connect(roof.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,56},
+          {58,50},{48,50},{48,-46},{-7,-46},{-7,-8}},                                                                                                           color={191,0,0}));
+  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{28,58},
+          {28,48},{48,48},{48,-46},{-7,-46},{-7,-8}},                                                                                                              color={191,0,0}));
   connect(inner_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-14,54},{-14,48},{48,48},{48,-46},{-7,-46},{-7,-8}},              color={191,0,0}));
   connect(outside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-50,17},{-44,17},{-44,48},{48,48},{48,-46},{-7,-46},{-7,-8}},              color={191,0,0}));
   annotation (Icon(graphics={
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL1IwS1Gr1Uf1.mo b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL1IwS1Gr1Uf1.mo
index a1f95093e3..c2acb4a664 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL1IwS1Gr1Uf1.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL1IwS1Gr1Uf1.mo
@@ -225,7 +225,7 @@ model Ow2IwL1IwS1Gr1Uf1
     wall_height=room_width,
     withWindow=false,
     withDoor=false,
-    ISOrientation=3,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -254,7 +254,7 @@ model Ow2IwL1IwS1Gr1Uf1
     withWindow=false,
     outside=false,
     withDoor=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)      annotation (Placement(transformation(
         origin={-29,-65},
@@ -264,7 +264,7 @@ model Ow2IwL1IwS1Gr1Uf1
     annotation (Placement(transformation(extent={{20,-100},{40,-80}})));
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a thermInsideWall1
     annotation (Placement(transformation(extent={{80,0},{100,20}})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
     annotation (Placement(transformation(extent={{-119.5,-70},{-99.5,-50}}), iconTransformation(extent={{-109.5,-50},{-89.5,-30}})));
   Utilities.Interfaces.SolarRad_in SolarRadiationPort_OW1
     annotation (Placement(transformation(extent={{-109.5,20},{-89.5,40}})));
@@ -279,13 +279,14 @@ model Ow2IwL1IwS1Gr1Uf1
     annotation (Placement(transformation(extent={{-16,-104},{4,-84}})));
 
 equation
-  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-60.25,33.4667},{-80,33.4667},{-80,-60},{-109.5,-60}},
-                                                                color={0,0,127}));
+  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-60.25,
+          33.4667},{-80,33.4667},{-80,-60},{-109.5,-60}},       color={0,0,127}));
   connect(thermInsideWall2, thermInsideWall2)
     annotation (Line(points={{30,-90},{30,-90}}, color={191,0,0}));
   connect(inside_wall1.port_outside, thermInsideWall1)
     annotation (Line(points={{64.3,5},{90,5},{90,10}}, color={191,0,0}));
-  connect(outside_wall2.WindSpeedPort, WindSpeedPort) annotation (Line(points={{40.2667,62.2502},{40.2667,70},{-80,70},{-80,-60},{-109.5,-60}},
+  connect(outside_wall2.WindSpeedPort, WindSpeedPort) annotation (Line(points={{40.2667,
+          62.2502},{40.2667,70},{-80,70},{-80,-60},{-109.5,-60}},
         color={0,0,127}));
   connect(outside_wall2.SolarRadiationPort, SolarRadiationPort_OW2) annotation (
      Line(points={{45.5833,63.5002},{45.5833,80.7501},{50.5,80.7501},{50.5,99}},
@@ -301,14 +302,18 @@ equation
       points={{-6,-94},{-6,-74},{-24,-74},{-24,-68.15},{-29,-68.15}},
       color={191,0,0},
       pattern=LinePattern.Dash));
-  connect(outside_wall2.port_outside, thermOutside) annotation (Line(points={{19,62.2502},{19,76},{-56,76},{-56,100},{-100,100}}, color={191,0,0}));
+  connect(outside_wall2.port_outside, thermOutside) annotation (Line(points={{19,
+          62.2502},{19,76},{-56,76},{-56,100},{-100,100}},                                                                        color={191,0,0}));
 
   connect(thermOutside, outside_wall1.port_outside) annotation (Line(points={{-100,100},{-78,100},{-78,10},{-60.25,10}}, color={191,0,0}));
-  connect(floor.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-29,-62},{-30,-62},{-30,-44},{-7,-44},{-7,-8}},              color={191,0,0}));
+  connect(floor.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-29,-62},
+          {-30,-62},{-30,-44},{-7,-44},{-7,-8}},                                                                                                              color={191,0,0}));
   connect(inside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{16,-56},{16,-44},{-7,-44},{-7,-8}},              color={191,0,0}));
   connect(inside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{52,5},{42,5},{42,-44},{-7,-44},{-7,-8}},              color={191,0,0}));
-  connect(outside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{19,52},{18,52},{18,38},{42,38},{42,-44},{-7,-44},{-7,-8}},              color={191,0,0}));
-  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-30,56},{-30,38},{42,38},{42,-44},{-7,-44},{-7,-8}},              color={191,0,0}));
+  connect(outside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{19,52},
+          {18,52},{18,38},{42,38},{42,-44},{-7,-44},{-7,-8}},                                                                                                                    color={191,0,0}));
+  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-30,56},
+          {-30,38},{42,38},{42,-44},{-7,-44},{-7,-8}},                                                                                                               color={191,0,0}));
   connect(outside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-50,10},{-40,10},{-40,38},{42,38},{42,-44},{-7,-44},{-7,-8}},              color={191,0,0}));
   annotation (Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
             {100,100}}), graphics={
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL1IwS1Lf1At1Ro1.mo b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL1IwS1Lf1At1Ro1.mo
index 6a5412bf1f..5706264669 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL1IwS1Lf1At1Ro1.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL1IwS1Lf1At1Ro1.mo
@@ -119,7 +119,7 @@ model Ow2IwL1IwS1Lf1At1Ro1
     withDoor=withDoor2,
     wall_length=room_width_long,
     wall_height=0.5*(room_height_long + room_height_short + room_width_short/room_width_long*(room_height_long - room_height_short)),
-    ISOrientation=1,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall,
     U_door=U_door_OD2,
     eps_door=eps_door_OD2,
     redeclare final model WindowModel = WindowModel,
@@ -206,7 +206,7 @@ model Ow2IwL1IwS1Lf1At1Ro1
     wall_height=room_width_short,
     withWindow=false,
     withDoor=false,
-    ISOrientation=3,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -235,7 +235,7 @@ model Ow2IwL1IwS1Lf1At1Ro1
     wall_height=room_width_long,
     withWindow=false,
     withDoor=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)      annotation (Placement(transformation(
         origin={-27,-60},
@@ -275,7 +275,7 @@ model Ow2IwL1IwS1Lf1At1Ro1
     annotation (Placement(transformation(extent={{20,-100},{40,-80}})));
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a thermInsideWall1
     annotation (Placement(transformation(extent={{80,0},{100,20}})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
     annotation (Placement(transformation(extent={{-119.5,-70},{-99.5,-50}}), iconTransformation(extent={{-109.5,-50},{-89.5,-30}})));
   Utilities.Interfaces.SolarRad_in SolarRadiationPort_OW1
     annotation (Placement(transformation(extent={{-109.5,20},{-89.5,40}})));
@@ -297,17 +297,18 @@ model Ow2IwL1IwS1Lf1At1Ro1
 
 
 equation
-  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-62.25,30.2667},{-80,30.2667},{-80,-60},{-109.5,-60}},
-                                                                color={0,0,127}));
-  connect(inside_wall2.port_outside, thermInsideWall2) annotation (Line(points={{32,-64.25},{32,-72},{30,-72},{30,-90}},
-                                                   color={191,0,0}));
+  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-62.25,
+          30.2667},{-80,30.2667},{-80,-60},{-109.5,-60}},       color={0,0,127}));
+  connect(inside_wall2.port_outside, thermInsideWall2) annotation (Line(points={{32,
+          -64.25},{32,-72},{30,-72},{30,-90}},     color={191,0,0}));
   connect(thermInsideWall2, thermInsideWall2)
     annotation (Line(points={{30,-90},{30,-90}}, color={191,0,0}));
-  connect(inside_wall1.port_outside, thermInsideWall1) annotation (Line(points={{66.25,4.00001},{90,4.00001},{90,10}},
-                                                 color={191,0,0}));
+  connect(inside_wall1.port_outside, thermInsideWall1) annotation (Line(points={{66.25,
+          4.00001},{90,4.00001},{90,10}},        color={191,0,0}));
   connect(Ceiling.port_outside, thermCeiling)
     annotation (Line(points={{22,62.1},{22,70},{90,70}}, color={191,0,0}));
-  connect(outside_wall2.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-7.73333,64.25},{-7.73333,70},{-80,70},{-80,-60},{-109.5,-60}},
+  connect(outside_wall2.WindSpeedPort, WindSpeedPort) annotation (Line(points={{
+          -7.73333,64.25},{-7.73333,70},{-80,70},{-80,-60},{-109.5,-60}},
                  color={0,0,127}));
   connect(SolarRadiationPort_OW1, outside_wall1.SolarRadiationPort) annotation (
      Line(points={{-99.5,30},{-63.5,30},{-63.5,35.5833}}, color={255,128,0}));
@@ -317,21 +318,28 @@ equation
   connect(roof.SolarRadiationPort, SolarRadiationPort_Roof) annotation (Line(
         points={{70.5833,62.8999},{70.5833,70},{74,70},{74,100}}, color={255,128,
           0}));
-  connect(roof.WindSpeedPort, WindSpeedPort) annotation (Line(points={{67.4667,62.1499},{67.4667,70},{-80,70},{-80,-60},{-109.5,-60}},
+  connect(roof.WindSpeedPort, WindSpeedPort) annotation (Line(points={{67.4667,
+          62.1499},{67.4667,70},{-80,70},{-80,-60},{-109.5,-60}},
                                                         color={0,0,127}));
   connect(thermFloor, floor.port_outside) annotation (Line(
       points={{-6,-94},{-8,-94},{-8,-66},{-22,-66},{-22,-62.1},{-27,-62.1}},
       color={191,0,0},
       pattern=LinePattern.Dash));
-  connect(outside_wall2.port_outside, thermOutside) annotation (Line(points={{-29,64.25},{-29,100},{-100,100}}, color={191,0,0}));
-  connect(roof.port_outside, thermOutside) annotation (Line(points={{55,62.1499},{55,72},{-29,72},{-29,100},{-100,100}}, color={191,0,0}));
+  connect(outside_wall2.port_outside, thermOutside) annotation (Line(points={{-29,
+          64.25},{-29,100},{-100,100}},                                                                         color={191,0,0}));
+  connect(roof.port_outside, thermOutside) annotation (Line(points={{55,62.1499},
+          {55,72},{-29,72},{-29,100},{-100,100}},                                                                        color={191,0,0}));
   connect(outside_wall1.port_outside, thermOutside) annotation (Line(points={{-62.25,9},{-76,9},{-76,100},{-100,100}}, color={191,0,0}));
   connect(floor.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-27,-58},{-28,-58},{-28,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
-  connect(inside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{32,-54},{32,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},              color={191,0,0}));
+  connect(inside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{32,-54},
+          {32,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},                                                                                                                    color={191,0,0}));
   connect(inside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{56,4.00001},{54,4.00001},{54,4},{44,4},{44,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},              color={191,0,0}));
-  connect(roof.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{55,56},{54,56},{54,50},{44,50},{44,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},              color={191,0,0}));
-  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{22,58},{22,50},{44,50},{44,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},              color={191,0,0}));
-  connect(outside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-29,54},{-30,54},{-30,50},{44,50},{44,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},              color={191,0,0}));
+  connect(roof.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{55,56},
+          {54,56},{54,50},{44,50},{44,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},                                                                                                           color={191,0,0}));
+  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{22,58},
+          {22,50},{44,50},{44,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},                                                                                                              color={191,0,0}));
+  connect(outside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-29,54},
+          {-30,54},{-30,50},{44,50},{44,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},                                                                                                                     color={191,0,0}));
   connect(outside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-52,9},{-40,9},{-40,50},{44,50},{44,-48},{-6,-48},{-6,-28},{-7,-28},{-7,-8}},              color={191,0,0}));
   annotation (Icon(graphics={
         Rectangle(
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL2IwS1Gr1Uf1.mo b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL2IwS1Gr1Uf1.mo
index 7c0bf2cbaa..2713ffe7ed 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL2IwS1Gr1Uf1.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL2IwS1Gr1Uf1.mo
@@ -229,7 +229,7 @@ model Ow2IwL2IwS1Gr1Uf1
     wall_height=room_width,
     withWindow=false,
     withDoor=false,
-    ISOrientation=3,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -258,7 +258,7 @@ model Ow2IwL2IwS1Gr1Uf1
     wall_height=room_width,
     withWindow=false,
     withDoor=false,
-    ISOrientation=2,
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
     redeclare final model WindowModel = WindowModel,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin)
                      annotation (Placement(transformation(
@@ -297,7 +297,7 @@ model Ow2IwL2IwS1Gr1Uf1
     annotation (Placement(transformation(extent={{20,-100},{40,-80}})));
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a thermInsideWall1a
     annotation (Placement(transformation(extent={{80,20},{100,40}})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
     annotation (Placement(transformation(extent={{-119.5,-70},{-99.5,-50}}), iconTransformation(extent={{-109.5,-50},{-89.5,-30}})));
   Utilities.Interfaces.SolarRad_in SolarRadiationPort_OW1
     annotation (Placement(transformation(extent={{-109.5,20},{-89.5,40}})));
@@ -319,17 +319,18 @@ model Ow2IwL2IwS1Gr1Uf1
 equation
   connect(thermInsideWall2, thermInsideWall2)
     annotation (Line(points={{30,-90},{30,-90}}, color={191,0,0}));
-  connect(WindSpeedPort, outside_wall2.WindSpeedPort) annotation (Line(points={{-109.5,-60},{-80,-60},{-80,74},{42.8,74},{42.8,64.25}},
-                                                                 color={0,0,127}));
-  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-58.25,36.2667},{-80,36.2667},{-80,-60},{-109.5,-60}},
-                                                                color={0,0,127}));
+  connect(WindSpeedPort, outside_wall2.WindSpeedPort) annotation (Line(points={{-109.5,
+          -60},{-80,-60},{-80,74},{42.8,74},{42.8,64.25}},       color={0,0,127}));
+  connect(outside_wall1.WindSpeedPort, WindSpeedPort) annotation (Line(points={{-58.25,
+          36.2667},{-80,36.2667},{-80,-60},{-109.5,-60}},       color={0,0,127}));
   connect(outside_wall2.SolarRadiationPort, SolarRadiationPort_OW2) annotation (
      Line(points={{47.75,65.5},{47.75,74},{50.5,74},{50.5,88},{50.5,101}},
         color={255,128,0}));
-  connect(Ceiling.port_outside, thermCeiling) annotation (Line(points={{-30,64.15},{-30,64.15},{-30,74},{84,74},{84,70},{90,70}},
+  connect(Ceiling.port_outside, thermCeiling) annotation (Line(points={{-30,
+          64.15},{-30,64.15},{-30,74},{84,74},{84,70},{90,70}},
                                                          color={191,0,0}));
-  connect(inside_wall2.port_outside, thermInsideWall2) annotation (Line(points={{22,-64.2},{22,-77.3},{30,-77.3},{30,-90}},
-                                                      color={191,0,0}));
+  connect(inside_wall2.port_outside, thermInsideWall2) annotation (Line(points={{22,
+          -64.2},{22,-77.3},{30,-77.3},{30,-90}},     color={191,0,0}));
   connect(inside_wall1a.port_outside, thermInsideWall1a) annotation (Line(
         points={{64.15,24},{77.225,24},{77.225,30},{90,30}}, color={191,0,0}));
   connect(inside_wall1b.port_outside, thermInsideWall1b) annotation (Line(
@@ -344,13 +345,16 @@ equation
       color={191,0,0},
       pattern=LinePattern.Dash));
   connect(outside_wall1.port_outside, thermOutside) annotation (Line(points={{-58.25,15},{-76,15},{-76,100},{-100,100}}, color={191,0,0}));
-  connect(outside_wall2.port_outside, thermOutside) annotation (Line(points={{23,64.25},{23,76},{-52,76},{-52,100},{-100,100}}, color={191,0,0}));
+  connect(outside_wall2.port_outside, thermOutside) annotation (Line(points={{23,
+          64.25},{23,76},{-52,76},{-52,100},{-100,100}},                                                                        color={191,0,0}));
   connect(floor.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-27,-58},{-26,-58},{-26,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
   connect(inside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{22,-56},{22,-46},{-6,-46},{-6,-42},{-7,-42},{-7,-8}},              color={191,0,0}));
   connect(inside_wall1b.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,-15},{54,-15},{54,-46},{-6,-46},{-6,-42},{-7,-42},{-7,-8}},              color={191,0,0}));
-  connect(inside_wall1a.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,24},{54,24},{54,-46},{-6,-46},{-6,-42},{-7,-42},{-7,-8}},              color={191,0,0}));
+  connect(inside_wall1a.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,24},
+          {54,24},{54,-46},{-6,-46},{-6,-42},{-7,-42},{-7,-8}},                                                                                                                    color={191,0,0}));
   connect(outside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{23,54},{24,54},{24,46},{54,46},{54,-46},{-6,-46},{-6,-42},{-7,-42},{-7,-8}},              color={191,0,0}));
-  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-30,58},{-30,46},{54,46},{54,-46},{-6,-46},{-6,-42},{-7,-42},{-7,-8}},              color={191,0,0}));
+  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-30,58},
+          {-30,46},{54,46},{54,-46},{-6,-46},{-6,-42},{-7,-42},{-7,-8}},                                                                                                               color={191,0,0}));
   connect(outside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-48,15},{-42,15},{-42,46},{54,46},{54,-46},{-6,-46},{-6,-42},{-7,-42},{-7,-8}},              color={191,0,0}));
   annotation (Icon(graphics={
         Rectangle(
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL2IwS1Lf1At1Ro1.mo b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL2IwS1Lf1At1Ro1.mo
index 3dcfbfe660..394181689d 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL2IwS1Lf1At1Ro1.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/OFD/Ow2IwL2IwS1Lf1At1Ro1.mo
@@ -209,7 +209,7 @@ model Ow2IwL2IwS1Lf1At1Ro1
     wall_height=room_width_short,
     withWindow=false,
     withDoor=false,
-    ISOrientation=3) annotation (Placement(transformation(
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling) annotation (Placement(transformation(
         origin={28,60},
         extent={{1.99999,-10},{-1.99998,10}},
         rotation=90)));
@@ -237,7 +237,7 @@ model Ow2IwL2IwS1Lf1At1Ro1
     wall_height=room_width_long,
     withWindow=false,
     withDoor=false,
-    ISOrientation=2)                              annotation (Placement(transformation(
+    ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor)                              annotation (Placement(transformation(
         origin={-24,-60},
         extent={{-1.99999,-10},{1.99999,10}},
         rotation=90)));
@@ -325,7 +325,7 @@ model Ow2IwL2IwS1Lf1At1Ro1
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a thermFloor annotation (
       Placement(transformation(extent={{-16,-104},{4,-84}}), iconTransformation(
           extent={{-16,-104},{4,-84}})));
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == 1 or calcMethodOut == 2)
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if (calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethodOut == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals)
     annotation (Placement(transformation(extent={{-126,-74},{-99.5,-48}}),
                                                                          iconTransformation(extent={{-109.5,-60},{-89.5,-40}})));
 
@@ -344,28 +344,34 @@ equation
         points={{62.1,19},{84,19},{84,20},{90,20},{90,10}}, color={191,0,0}));
   connect(roof.SolarRadiationPort, SolarRadiationPort_Roof) annotation (Line(
         points={{74.5833,62.9},{74.5833,92},{74,92},{74,100}}, color={255,128,0}));
-  connect(Ceiling.port_outside, thermCeiling) annotation (Line(points={{28,62.1},{28,62.1},{28,74},{90,74},{90,50}},
-                                              color={191,0,0}));
+  connect(Ceiling.port_outside, thermCeiling) annotation (Line(points={{28,62.1},
+          {28,62.1},{28,74},{90,74},{90,50}}, color={191,0,0}));
   connect(outside_wall2.SolarRadiationPort, SolarRadiationPort_OW2) annotation (
      Line(points={{5.25,65.8},{5.25,74},{44.5,74},{44.5,101}}, color={255,128,0}));
-  connect(thermFloor, floor.port_outside) annotation (Line(points={{-6,-94},{-8,-94},{-8,-70},{-24,-70},{-24,-62.1}}, color={191,0,0}));
+  connect(thermFloor, floor.port_outside) annotation (Line(points={{-6,-94},{-8,
+          -94},{-8,-70},{-24,-70},{-24,-62.1}},                                                                       color={191,0,0}));
   connect(outside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-25,52},{-25,40},{40,40},{40,-40},{-7,-40},{-7,-8}},          color={191,0,0}));
-  connect(roof.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{59,56},{59,40},{40,40},{40,-40},{-7,-40},{-7,-8}},          color={191,0,0}));
-  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{28,58},{28,40},{40,40},{40,-40},{-7,-40},{-7,-8}},          color={191,0,0}));
+  connect(roof.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{59,56},
+          {59,40},{40,40},{40,-40},{-7,-40},{-7,-8}},                                                                                                       color={191,0,0}));
+  connect(Ceiling.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{28,58},
+          {28,40},{40,40},{40,-40},{-7,-40},{-7,-8}},                                                                                                          color={191,0,0}));
   connect(inside_wall1b.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,-19},{40,-19},{40,-40},{-7,-40},{-7,-8}},          color={191,0,0}));
   connect(inside_wall1a.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{58,19},{40,19},{40,-40},{-7,-40},{-7,-8}},          color={191,0,0}));
-  connect(inside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{28,-56},{28,-40},{-6,-40},{-6,-8},{-7,-8}},              color={191,0,0}));
+  connect(inside_wall2.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{28,-56},
+          {28,-40},{-6,-40},{-6,-8},{-7,-8}},                                                                                                                    color={191,0,0}));
   connect(outside_wall1.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-78,4},{-74,4},{-74,-40},{-7,-40},{-7,-8}},            color={191,0,0}));
-  connect(WindSpeedPort, outside_wall1.WindSpeedPort) annotation (Line(points={{-112.75,-61},{-96,-61},{-96,24.5333},{-88.25,24.5333}},
-                                                                                                                                      color={0,0,127}));
-  connect(WindSpeedPort, roof.WindSpeedPort) annotation (Line(points={{-112.75,-61},{-96,-61},{-96,70},{71.4667,70},{71.4667,62.15}},
-                                                                                                                                    color={0,0,127}));
+  connect(WindSpeedPort, outside_wall1.WindSpeedPort) annotation (Line(points={{-112.75,
+          -61},{-96,-61},{-96,24.5333},{-88.25,24.5333}},                                                                             color={0,0,127}));
+  connect(WindSpeedPort, roof.WindSpeedPort) annotation (Line(points={{-112.75,
+          -61},{-96,-61},{-96,70},{71.4667,70},{71.4667,62.15}},                                                                    color={0,0,127}));
   connect(WindSpeedPort, outside_wall2.WindSpeedPort) annotation (Line(points={{-112.75,-61},{-96,-61},{-96,70},{-0.8,70},{-0.8,64.3}},
                                                                                                                                       color={0,0,127}));
-  connect(floor.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-24,-58},{-24,-48},{-7,-48},{-7,-8}},              color={191,0,0}));
+  connect(floor.thermStarComb_inside, thermStar_Demux.portConvRadComb) annotation (Line(points={{-24,-58},
+          {-24,-48},{-7,-48},{-7,-8}},                                                                                                              color={191,0,0}));
   connect(outside_wall1.port_outside, thermOutside) annotation (Line(points={{-88.25,4},{-94,4},{-94,100},{-100,100}}, color={191,0,0}));
   connect(outside_wall2.port_outside, thermOutside) annotation (Line(points={{-25,64.3},{-25,100},{-100,100}}, color={191,0,0}));
-  connect(roof.port_outside, thermOutside) annotation (Line(points={{59,62.15},{59,76},{-25,76},{-25,100},{-100,100}}, color={191,0,0}));
+  connect(roof.port_outside, thermOutside) annotation (Line(points={{59,62.15},
+          {59,76},{-25,76},{-25,100},{-100,100}},                                                                      color={191,0,0}));
   annotation (Icon(graphics={
         Rectangle(
           extent={{-80,80},{80,60}},
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/RoomEmpiricalValidation/RoomTwinHouseN2.mo b/AixLib/ThermalZones/HighOrder/Rooms/RoomEmpiricalValidation/RoomTwinHouseN2.mo
index beaf928c63..751f745933 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/RoomEmpiricalValidation/RoomTwinHouseN2.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/RoomEmpiricalValidation/RoomTwinHouseN2.mo
@@ -35,24 +35,24 @@ model RoomTwinHouseN2 "N2"
       redeclare final DataBase.Walls.EmpiricalValidation.OW_E_TwinHouses
         wallPar,
       final solar_absorptance=0.23,
-      final calcMethodOut=1,
-      final calcMethodIn=1,
+      final calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946,
+      final calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A,
       final withWindow=true,
       final windowarea=1.89),
     wallWest(
       redeclare final DataBase.Walls.EmpiricalValidation.OW_W_TwinHouses
         wallPar,
       final solar_absorptance=0.23,
-      final calcMethodOut=1,
-      final calcMethodIn=1,
+      final calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946,
+      final calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A,
       final withWindow=true,
       final windowarea=3.78),
     wallSouth(
       redeclare final DataBase.Walls.EmpiricalValidation.OW_S_N_TwinHouses
         wallPar,
       final solar_absorptance=0.23,
-      final calcMethodOut=1,
-      final calcMethodIn=1,
+      final calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946,
+      final calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A,
       final withWindow=true,
       final windowarea=9.66,
       final withSunblind=true,
@@ -63,8 +63,8 @@ model RoomTwinHouseN2 "N2"
       redeclare final DataBase.Walls.EmpiricalValidation.OW_S_N_TwinHouses
         wallPar,
       final solar_absorptance=0.23,
-      final calcMethodOut=1,
-      final calcMethodIn=1,
+      final calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946,
+      final calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A,
       final withWindow=true,
       final windowarea=1.89,
       final withDoor=true,
@@ -72,17 +72,17 @@ model RoomTwinHouseN2 "N2"
     floor(
       final outside=false,
       redeclare DataBase.Walls.EmpiricalValidation.FL_TwinHouses wallPar,
-      final ISOrientation=2,
+      final ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
       final withWindow=false,
       final withDoor=false),
     ceiling(
       outside=false,
       redeclare DataBase.Walls.EmpiricalValidation.CE_TwinHouses wallPar,
-      final ISOrientation=3,
+      final ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling,
       final withWindow=false,
       final withDoor=false,
-      final calcMethodOut=1,
-      final calcMethodIn=1));
+      final calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946,
+      final calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A));
 
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a Therm_ground
     annotation (Placement(transformation(extent={{-36,-102},{-28,-94}}),
@@ -116,8 +116,8 @@ model RoomTwinHouseN2 "N2"
     final WindowType=Type_Win,
     wall_length=2.6,
     wall_height=12.4,
-    calcMethodOut=1,
-    calcMethodIn=1,
+    calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946,
+    calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A,
     T0=TWalls_start)
     annotation (Placement(transformation(extent={{26,16},{30,40}})));
   Components.Walls.Wall IW1(
@@ -131,8 +131,8 @@ model RoomTwinHouseN2 "N2"
     final WindowType=Type_Win,
     wall_length=2.6,
     wall_height=11.6,
-    calcMethodOut=1,
-    calcMethodIn=1,
+    calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946,
+    calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A,
     T0=TWalls_start)
     annotation (Placement(transformation(extent={{40,-2},{44,22}})));
 equation
diff --git a/AixLib/ThermalZones/HighOrder/Rooms/RoomEmpiricalValidation/RoomWarehouse.mo b/AixLib/ThermalZones/HighOrder/Rooms/RoomEmpiricalValidation/RoomWarehouse.mo
index 22aac90e0e..13a7061c25 100644
--- a/AixLib/ThermalZones/HighOrder/Rooms/RoomEmpiricalValidation/RoomWarehouse.mo
+++ b/AixLib/ThermalZones/HighOrder/Rooms/RoomEmpiricalValidation/RoomWarehouse.mo
@@ -47,12 +47,12 @@ model RoomWarehouse "Room model of Warehouse for Empirical validation"
       final outside=false,
       redeclare DataBase.Walls.EmpiricalValidation.FL_Warehouse wallPar,
       final solar_absorptance=0.3,
-      final ISOrientation=2,
+      final ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor,
       final withWindow=false,
       final withDoor=false),
     ceiling(
       redeclare DataBase.Walls.EmpiricalValidation.RO_Warehouse wallPar,
-      final ISOrientation=3,
+      final ISOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling,
       final withWindow=true,
       final windowarea=60,
       final withDoor=false));
diff --git a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/BaseClasses/PartialCase.mo b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/BaseClasses/PartialCase.mo
index 5228cbc821..a92b4cd116 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/BaseClasses/PartialCase.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/BaseClasses/PartialCase.mo
@@ -18,20 +18,20 @@ partial model PartialCase "This is the base class from which the base cases will
     each GroundReflection= 0.2,
     each Latitude=sun.Latitude,
     each h= 1609,
-    each WeatherFormat=2) "N, E, S, W, Horz"
+    each WeatherFormat=true) "N, E, S, W, Horz"
     annotation (Placement(transformation(extent={{-102,41},{-74,69}})));
 
   Modelica.Blocks.Sources.CombiTimeTable Solar_Radiation(
     tableOnFile=true,
     tableName="Table",
     columns={2,3},
-    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/Weatherdata_ASHARE140.mat"))
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/Weatherdata_ASHARE140.txt"))
     annotation (Placement(transformation(extent={{-102,-14},{-85,3}})));
   Modelica.Blocks.Sources.CombiTimeTable Source_Weather(
     tableOnFile=true,
     tableName="Table",
     columns={4,5,6,7},
-    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/Weatherdata_ASHARE140.mat"))
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/Weatherdata_ASHARE140.txt"))
     annotation (Placement(transformation(extent={{-103,13},{-86,30}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature outsideTemp
     "ambient temperature"
@@ -41,21 +41,21 @@ partial model PartialCase "This is the base class from which the base cases will
       choices(
         choice(redeclare model Room = Rooms.ASHRAE140.SouthFacingWindows (
           wallTypes=wallTypes,
-          calcMethodIn=4,
+          calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.ASHRAE140_2017,
           Type_Win=windowParam,
           redeclare final model CorrSolarGainWin = CorrSolarGainWin,
           solar_absorptance_OW=solar_absorptance_OW,
-          calcMethodOut=2,
+          calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals,
           Win_Area=Win_Area,
           absInnerWallSurf=absInnerWallSurf)
         "Room with south facing window"),
         choice(redeclare model Room = Rooms.ASHRAE140.EastWestFacingWindows (
           wallTypes=wallTypes,
-          calcMethodIn=4,
+          calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.ASHRAE140_2017,
           Type_Win=windowParam,
           redeclare final model CorrSolarGainWin = CorrSolarGainWin,
           solar_absorptance_OW=solar_absorptance_OW,
-          calcMethodOut=2,
+          calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals,
           Win_Area=Win_Area,
           absInnerWallSurf=absInnerWallSurf)
         "Room with east and west facing window")));
@@ -66,19 +66,21 @@ partial model PartialCase "This is the base class from which the base cases will
     T0_air=294.15,
     TWalls_start=289.15,
     final wallTypes=wallTypes,
-    calcMethodIn=4,
+    calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.ASHRAE140_2017,
     final Type_Win=windowParam,
     redeclare final model CorrSolarGainWin = CorrSolarGainWin,
     final solar_absorptance_OW=solar_absorptance_OW,
-    calcMethodOut=2,
+    calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals,
     final Win_Area=Win_Area,
     final absInnerWallSurf=absInnerWallSurf,
     final use_dynamicShortWaveRadMethod=false)
                   annotation(Placement(transformation(extent={{-27,8},{29,62}})));
 
-  Modelica.Blocks.Interfaces.RealOutput AnnualHeatingLoad "in kWh"
+  Modelica.Blocks.Interfaces.RealOutput AnnualHeatingLoad
+ if activeHeatingOutput                                   "in kWh"
     annotation (Placement(transformation(extent={{130,58},{150,78}})));
-  Modelica.Blocks.Interfaces.RealOutput AnnualCoolingLoad "in kWh"
+  Modelica.Blocks.Interfaces.RealOutput AnnualCoolingLoad
+ if activeCoolingOutput                                   "in kWh"
     annotation (Placement(transformation(extent={{130,42},{150,62}})));
   Modelica.Blocks.Interfaces.RealOutput TransmittedSolarRadiation_room
     "in kWh/m2"
@@ -94,10 +96,14 @@ partial model PartialCase "This is the base class from which the base cases will
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow
     InternalGains_radiative
     annotation (Placement(transformation(extent={{-97,-97},{-77,-77}})));
-  Modelica.Blocks.Continuous.Integrator integratorHeat annotation (Placement(transformation(extent={{72,62.5},{83,73.5}})));
-  Modelica.Blocks.Continuous.Integrator integratorCool annotation (Placement(transformation(extent={{72,46.5},{83,57.5}})));
-  Modelica.Blocks.Math.UnitConversions.To_kWh to_kWhHeat annotation (Placement(transformation(extent={{92,63},{102,73}})));
-  Modelica.Blocks.Math.UnitConversions.To_kWh to_kWhCool annotation (Placement(transformation(extent={{92,47},{102,57}})));
+  Modelica.Blocks.Continuous.Integrator integratorHeat if activeHeatingOutput
+                                                       annotation (Placement(transformation(extent={{72,62.5},{83,73.5}})));
+  Modelica.Blocks.Continuous.Integrator integratorCool if activeCoolingOutput
+                                                       annotation (Placement(transformation(extent={{72,46.5},{83,57.5}})));
+  Modelica.Blocks.Math.UnitConversions.To_kWh to_kWhHeat if activeHeatingOutput
+                                                         annotation (Placement(transformation(extent={{92,63},{102,73}})));
+  Modelica.Blocks.Math.UnitConversions.To_kWh to_kWhCool if activeCoolingOutput
+                                                         annotation (Placement(transformation(extent={{92,47},{102,57}})));
   Modelica.Blocks.Math.Gain convectiveInternalGains(k=0.4) "Convective part"
     annotation (Placement(transformation(extent={{-120,-72},{-110,-62}})));
   Modelica.Blocks.Math.Gain radiativeInternalGains(k=0.6) "Radiative part"
@@ -132,7 +138,8 @@ partial model PartialCase "This is the base class from which the base cases will
     annotation (choicesAllMatching=true);
   replaceable model CorrSolarGainWin =
       Components.WindowsDoors.BaseClasses.CorrectionSolarGain.CorG_ASHRAE140
-    constrainedby Components.WindowsDoors.BaseClasses.CorrectionSolarGain.PartialCorG
+    constrainedby
+    Components.WindowsDoors.BaseClasses.CorrectionSolarGain.PartialCorG
     "Correction model for solar irradiance as transmitted radiation" annotation (choicesAllMatching=true);
 
   parameter Modelica.Units.SI.Area Win_Area=12 "Window area ";
@@ -159,7 +166,10 @@ partial model PartialCase "This is the base class from which the base cases will
     "Simulation time when block should check if model results lies in limit range"
     annotation (Dialog(tab="Results check", group=
           "Cooling load or min. temperature"));
-
+  parameter Boolean activeHeatingOutput=true
+  "Activates blocks connected with HeaterCoolerPI.heatingPower";
+  parameter Boolean activeCoolingOutput=true
+  "Activates blocks connected with HeaterCoolerPI.coolingPower";
   Modelica.Blocks.Math.UnitConversions.To_degC to_degCRoomConvTemp annotation (Placement(transformation(extent={{92,31},{102,41}})));
   Modelica.Blocks.Interfaces.RealOutput FreeFloatRoomTemperature annotation (Placement(transformation(extent={{130,26},{150,46}})));
   Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor temperatureSensor annotation (Placement(transformation(extent={{72,30},{84,42}})));
diff --git a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case600.mo b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case600.mo
index ef7cfc124c..8d7e5a4333 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case600.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case600.mo
@@ -23,10 +23,6 @@ model Case600
     annotation (Placement(transformation(extent={{-38,-82},{-27,-71}})));
   Modelica.Blocks.Sources.Constant TSet_Heater(final k=TsetHeater)
     annotation (Placement(transformation(extent={{30,-81},{19,-70}})));
-  Modelica.Blocks.Sources.RealExpression HeatingPower(y=idealHeaterCooler.heatingPower)
-    annotation (Placement(transformation(extent={{43,58},{63,78}})));
-  Modelica.Blocks.Sources.RealExpression CoolingPower(y=idealHeaterCooler.coolingPower)
-    annotation (Placement(transformation(extent={{43,42},{63,62}})));
   Modelica.Blocks.Math.UnitConversions.From_degC from_degC
     annotation (Placement(transformation(extent={{-20,-82},{-9,-71}})));
   Modelica.Blocks.Math.UnitConversions.From_degC from_degC1 annotation (
@@ -47,10 +43,6 @@ equation
     annotation (Line(points={{18.45,-75.5},{13.1,-75.5}}, color={0,0,127}));
   connect(from_degC1.y, idealHeaterCooler.setPointHeat) annotation (Line(points={{0.45,
           -75.5},{-2.8,-75.5},{-2.8,-62.2}},        color={0,0,127}));
-  connect(HeatingPower.y, integratorHeat.u)
-    annotation (Line(points={{64,68},{70.9,68}}, color={0,0,127}));
-  connect(CoolingPower.y, integratorCool.u) annotation (Line(points={{64,52},{
-          68,52},{68,52},{70.9,52}}, color={0,0,127}));
   connect(Room.AirExchangePort, AirExchangeRate.y) annotation (Line(points={{
           -29.8,53.765},{-47,53.765},{-47,-33},{-20,-33},{-20,-49.5},{-24.35,
           -49.5}}, color={0,0,127}));
@@ -60,6 +52,12 @@ equation
   connect(to_kWhHeat.y, checkResultsAccordingToASHRAEHeatingOrTempMax.modelResults) annotation (Line(points={{102.5,68},{112,68},{112,-39},{94,-39},{94,-52.15},{97.95,-52.15}}, color={0,0,127}));
   connect(to_kWhCool.y, checkResultsAccordingToASHRAECoolingOrTempMin.modelResults) annotation (Line(points={{102.5,52},{111,52},{111,-37},{93,-37},{93,-73.15},{97.95,-73.15}}, color={0,0,127}));
   connect(Room.transShoWaveRadWin, integrator2.u) annotation (Line(points={{17.8,5.3},{17.8,-0.75},{74,-0.75}}, color={0,0,127}));
+  connect(idealHeaterCooler.heatingPower, integratorHeat.u) annotation (Line(
+        points={{5,-51},{31.05,-51},{31.05,-10.5},{55.05,-10.5},{55.05,68},{
+          70.9,68}}, color={0,0,127}));
+  connect(idealHeaterCooler.coolingPower, integratorCool.u) annotation (Line(
+        points={{5,-55.6},{36.05,-55.6},{36.05,-14.2},{60.05,-14.2},{60.05,52},
+          {70.9,52}}, color={0,0,127}));
   annotation (
     experiment(StopTime=31539600, Tolerance=1e-06),
     __Dymola_Commands(file=
diff --git a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case600FF.mo b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case600FF.mo
index 90a0470401..1d9b9c3c2e 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case600FF.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case600FF.mo
@@ -7,12 +7,10 @@ model Case600FF
     dispTypeHeatOrTempMax="T Max",
     tableCoolOrTempMin=[600,-18.8,-15.6],
     tableHeatOrTempMax=[600,64.9,69.5],
+    activeCoolingOutput=false,
+    activeHeatingOutput=false,
     Room(redeclare Components.Types.CoeffTableSouthWindow coeffTableSolDistrFractions));
 
-  Modelica.Blocks.Sources.RealExpression HeatingPower(y=0)
-    annotation (Placement(transformation(extent={{43,58},{63,78}})));
-  Modelica.Blocks.Sources.RealExpression CoolingPower(y=0)
-    annotation (Placement(transformation(extent={{43,42},{63,62}})));
   Modelica.Blocks.Sources.Constant AirExchangeRate(final k=airExchange)
     annotation (Placement(transformation(extent={{-38,-56},{-25,-43}})));
 
@@ -21,10 +19,6 @@ equation
   connect(Room.AirExchangePort, AirExchangeRate.y) annotation (Line(points={{
           -29.8,53.765},{-47,53.765},{-47,-37},{-17,-37},{-17,-49.5},{-24.35,
           -49.5}}, color={0,0,127}));
-  connect(HeatingPower.y, integratorHeat.u)
-    annotation (Line(points={{64,68},{70.9,68}}, color={0,0,127}));
-  connect(CoolingPower.y, integratorCool.u) annotation (Line(points={{64,52},{
-          68,52},{68,52},{70.9,52}}, color={0,0,127}));
   connect(to_degCRoomConvTemp.y, checkResultsAccordingToASHRAEHeatingOrTempMax.modelResults) annotation (Line(points={{102.5,36},{112,36},{112,-39},{92,-39},{92,-52.15},{97.95,-52.15}}, color={0,0,127}));
   connect(to_degCRoomConvTemp.y, checkResultsAccordingToASHRAECoolingOrTempMin.modelResults) annotation (Line(points={{102.5,36},{111,36},{111,-38},{91,-38},{91,-73.15},{97.95,-73.15}}, color={0,0,127}));
   connect(Room.transShoWaveRadWin, integrator2.u) annotation (Line(points={{17.8,5.3},{17.8,-0.75},{74,-0.75}}, color={0,0,127}));
diff --git a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case620.mo b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case620.mo
index f6feef7f9b..90e235e5d3 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case620.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case620.mo
@@ -7,10 +7,10 @@ model Case620
     tableHeatOrTempMax=[620,4613,5944],
     redeclare model RoomModel = Rooms.ASHRAE140.EastWestFacingWindows (
         wallTypes=wallTypes,
-        calcMethodIn=4,
+        calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.ASHRAE140_2017,
         Type_Win=windowParam,
         solar_absorptance_OW=solar_absorptance_OW,
-        calcMethodOut=2,
+        calcMethodOut=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals,
         Win_Area=Win_Area,
         absInnerWallSurf=absInnerWallSurf),
     Room(redeclare Components.Types.CoeffTableEastWestWindow coeffTableSolDistrFractions));
@@ -31,10 +31,6 @@ model Case620
     annotation (Placement(transformation(extent={{-38,-82},{-27,-71}})));
   Modelica.Blocks.Sources.Constant TSet_Heater(final k=TsetHeater)
     annotation (Placement(transformation(extent={{30,-81},{19,-70}})));
-  Modelica.Blocks.Sources.RealExpression HeatingPower(y=idealHeaterCooler.heatingPower)
-    annotation (Placement(transformation(extent={{43,58},{63,78}})));
-  Modelica.Blocks.Sources.RealExpression CoolingPower(y=idealHeaterCooler.coolingPower)
-    annotation (Placement(transformation(extent={{43,42},{63,62}})));
   Modelica.Blocks.Math.UnitConversions.From_degC from_degC
     annotation (Placement(transformation(extent={{-20,-82},{-9,-71}})));
   Modelica.Blocks.Math.UnitConversions.From_degC from_degC1 annotation (
@@ -61,13 +57,15 @@ equation
   connect(idealHeaterCooler.heatCoolRoom, Room.thermRoom) annotation (Line(
         points={{4,-59},{22,-59},{22,-19},{-2,-19},{-2,35},{-2.92,35}}, color={191,
           0,0}));
-  connect(HeatingPower.y, integratorHeat.u)
-    annotation (Line(points={{64,68},{70.9,68}}, color={0,0,127}));
-  connect(CoolingPower.y, integratorCool.u)
-    annotation (Line(points={{64,52},{70.9,52}}, color={0,0,127}));
   connect(to_kWhHeat.y, checkResultsAccordingToASHRAEHeatingOrTempMax.modelResults) annotation (Line(points={{102.5,68},{112,68},{112,-39},{94,-39},{94,-52.15},{97.95,-52.15}}, color={0,0,127}));
   connect(to_kWhCool.y, checkResultsAccordingToASHRAECoolingOrTempMin.modelResults) annotation (Line(points={{102.5,52},{111,52},{111,-37},{93,-37},{93,-73.15},{97.95,-73.15}}, color={0,0,127}));
   connect(Room.transShoWaveRadWin, integrator2.u) annotation (Line(points={{17.8,5.3},{17.8,-0.75},{74,-0.75}}, color={0,0,127}));
+  connect(idealHeaterCooler.heatingPower, integratorHeat.u) annotation (Line(
+        points={{5,-51},{32.3,-51},{32.3,-5},{52.3,-5},{52.3,68},{70.9,68}},
+        color={0,0,127}));
+  connect(idealHeaterCooler.coolingPower, integratorCool.u) annotation (Line(
+        points={{5,-55.6},{39.1,-55.6},{39.1,-9.4},{57.1,-9.4},{57.1,52},{70.9,
+          52}}, color={0,0,127}));
   annotation (
     experiment(StopTime=31539600, Tolerance=1e-06),
     __Dymola_Commands(file=
diff --git a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case640.mo b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case640.mo
index d403cc47c5..66f7cc49a3 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case640.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case640.mo
@@ -23,10 +23,6 @@ model Case640
     annotation (Placement(transformation(extent={{-38,-56},{-25,-43}})));
   Modelica.Blocks.Sources.Constant Tset_Cooler(final k=TsetCooler)
     annotation (Placement(transformation(extent={{-38,-82},{-27,-71}})));
-  Modelica.Blocks.Sources.RealExpression HeatingPower(y=idealHeaterCooler.heatingPower)
-    annotation (Placement(transformation(extent={{43,58},{63,78}})));
-  Modelica.Blocks.Sources.RealExpression CoolingPower(y=idealHeaterCooler.coolingPower)
-    annotation (Placement(transformation(extent={{43,42},{63,62}})));
   Modelica.Blocks.Math.UnitConversions.From_degC from_degC
     annotation (Placement(transformation(extent={{-20,-82},{-9,-71}})));
 
@@ -48,10 +44,6 @@ equation
           -76.5},{-7.4,-76.5},{-7.4,-62.2}},      color={0,0,127}));
   connect(Source_TsetHeat.y[1], idealHeaterCooler.setPointHeat) annotation (
       Line(points={{9.35,-75.5},{-2.8,-75.5},{-2.8,-62.2}}, color={0,0,127}));
-  connect(HeatingPower.y, integratorHeat.u) annotation (Line(points={{64,68},{70.9,68}},
-                                     color={0,0,127}));
-  connect(CoolingPower.y, integratorCool.u)
-    annotation (Line(points={{64,52},{70.9,52}}, color={0,0,127}));
   connect(Room.AirExchangePort, AirExchangeRate.y) annotation (Line(points={{
           -29.8,53.765},{-47,53.765},{-47,-34},{-20,-34},{-20,-49.5},{-24.35,
           -49.5}}, color={0,0,127}));
@@ -61,6 +53,12 @@ equation
   connect(to_kWhHeat.y, checkResultsAccordingToASHRAEHeatingOrTempMax.modelResults) annotation (Line(points={{102.5,68},{112,68},{112,-39},{94,-39},{94,-52.15},{97.95,-52.15}}, color={0,0,127}));
   connect(to_kWhCool.y, checkResultsAccordingToASHRAECoolingOrTempMin.modelResults) annotation (Line(points={{102.5,52},{111,52},{111,-37},{93,-37},{93,-73.15},{97.95,-73.15}}, color={0,0,127}));
   connect(Room.transShoWaveRadWin, integrator2.u) annotation (Line(points={{17.8,5.3},{17.8,-0.75},{74,-0.75}}, color={0,0,127}));
+  connect(idealHeaterCooler.heatingPower, integratorHeat.u) annotation (Line(
+        points={{5,-51},{35.1,-51},{35.1,-7},{49.1,-7},{49.1,68},{70.9,68}},
+        color={0,0,127}));
+  connect(idealHeaterCooler.coolingPower, integratorCool.u) annotation (Line(
+        points={{5,-55.6},{40.1,-55.6},{40.1,-10.4},{54.1,-10.4},{54.1,52},{
+          70.9,52}}, color={0,0,127}));
   annotation (
     experiment(StopTime=31539600, Tolerance=1e-06),
     __Dymola_Commands(file=
diff --git a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case650.mo b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case650.mo
index 47e69574f0..8746ee80fb 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case650.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case650.mo
@@ -24,8 +24,6 @@ model Case650
 
   Modelica.Blocks.Sources.RealExpression HeatingPower(y=0)
     annotation (Placement(transformation(extent={{43,58},{63,78}})));
-  Modelica.Blocks.Sources.RealExpression CoolingPower(y=idealHeaterCooler.coolingPower)
-    annotation (Placement(transformation(extent={{43,42},{63,62}})));
   Modelica.Blocks.Sources.CombiTimeTable AirExchangeRate(
     columns={2},
     tableOnFile=false,
@@ -50,14 +48,14 @@ equation
           -47.5}}, color={0,0,127}));
   connect(HeatingPower.y, integratorHeat.u)
     annotation (Line(points={{64,68},{70.9,68}}, color={0,0,127}));
-  connect(CoolingPower.y, integratorCool.u)
-    annotation (Line(points={{64,52},{70.9,52}}, color={0,0,127}));
   connect(idealHeaterCooler.heatCoolRoom, Room.thermRoom) annotation (Line(
         points={{3,-59},{21,-59},{21,-19},{-2,-19},{-2,35},{-2.92,35}}, color={
           191,0,0}));
   connect(to_kWhHeat.y, checkResultsAccordingToASHRAEHeatingOrTempMax.modelResults) annotation (Line(points={{102.5,68},{112,68},{112,-39},{94,-39},{94,-52.15},{97.95,-52.15}}, color={0,0,127}));
   connect(to_kWhCool.y, checkResultsAccordingToASHRAECoolingOrTempMin.modelResults) annotation (Line(points={{102.5,52},{111,52},{111,-37},{93,-37},{93,-73.15},{97.95,-73.15}}, color={0,0,127}));
   connect(Room.transShoWaveRadWin, integrator2.u) annotation (Line(points={{17.8,5.3},{17.8,-0.75},{74,-0.75}}, color={0,0,127}));
+  connect(idealHeaterCooler.coolingPower, integratorCool.u) annotation (Line(
+        points={{4,-55.6},{48,-55.6},{48,52},{70.9,52}}, color={0,0,127}));
   annotation (
     experiment(StopTime=31539600, Tolerance=1e-06),
     __Dymola_Commands(file=
diff --git a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case650FF.mo b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case650FF.mo
index 12d83b1725..d88f488572 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case650FF.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/ASHRAE140/Case650FF.mo
@@ -7,15 +7,13 @@ model Case650FF
     dispTypeHeatOrTempMax="T Max",
     tableCoolOrTempMin=[650,-23,-21.6],
     tableHeatOrTempMax=[650,63.2,68.2],
+    activeHeatingOutput=false,
+    activeCoolingOutput=false,
     Room(redeclare Components.Types.CoeffTableSouthWindow coeffTableSolDistrFractions));
 
   parameter AixLib.DataBase.Profiles.ProfileBaseDataDefinition SetTempProfile = AixLib.DataBase.Profiles.ASHRAE140.SetTemp_caseX50();
   parameter AixLib.DataBase.Profiles.ProfileBaseDataDefinition AERProfile = AixLib.DataBase.Profiles.ASHRAE140.Ventilation_caseX50();
 
-  Modelica.Blocks.Sources.RealExpression HeatingPower(y=0)
-    annotation (Placement(transformation(extent={{43,58},{63,78}})));
-  Modelica.Blocks.Sources.RealExpression CoolingPower(y=0)
-    annotation (Placement(transformation(extent={{43,42},{63,62}})));
   Modelica.Blocks.Sources.CombiTimeTable AirExchangeRate(
     columns={2},
     tableOnFile=false,
@@ -28,10 +26,6 @@ equation
   connect(Room.AirExchangePort, AirExchangeRate.y[1]) annotation (Line(points={
           {-29.8,53.765},{-47,53.765},{-47,-36},{-18,-36},{-18,-47.5},{-25.35,
           -47.5}}, color={0,0,127}));
-  connect(HeatingPower.y, integratorHeat.u)
-    annotation (Line(points={{64,68},{70.9,68}}, color={0,0,127}));
-  connect(CoolingPower.y, integratorCool.u)
-    annotation (Line(points={{64,52},{70.9,52}}, color={0,0,127}));
   connect(to_degCRoomConvTemp.y, checkResultsAccordingToASHRAEHeatingOrTempMax.modelResults) annotation (Line(points={{102.5,36},{112,36},{112,-39},{92,-39},{92,-52.15},{97.95,-52.15}}, color={0,0,127}));
   connect(to_degCRoomConvTemp.y, checkResultsAccordingToASHRAECoolingOrTempMin.modelResults) annotation (Line(points={{102.5,36},{111,36},{111,-38},{91,-38},{91,-73.15},{97.95,-73.15}}, color={0,0,127}));
   connect(Room.transShoWaveRadWin, integrator2.u) annotation (Line(points={{17.8,5.3},{17.8,-0.75},{74,-0.75}}, color={0,0,127}));
diff --git a/AixLib/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mo b/AixLib/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mo
index f42a66b190..e79d63361b 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mo
@@ -9,7 +9,7 @@ model TwinHouseN2
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     T0_air=303.15,
     TWalls_start=303.15,
-    calcMethodIn=1,
+    calcMethodIn=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A,
     redeclare model WindowModel = Components.WindowsDoors.Window_ASHRAE140,
     redeclare DataBase.WindowsDoors.Simple.WindowSimple_TwinHouses Type_Win,
     redeclare model CorrSolarGainWin =
@@ -39,7 +39,7 @@ model TwinHouseN2
   Modelica.Blocks.Sources.CombiTimeTable TempCellar(
     tableOnFile=true,
     tableName="measurement",
-    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat"),
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt"),
     columns={4})
     annotation (Placement(transformation(extent={{-20,-160},{0,-140}})));
   Modelica.Blocks.Interfaces.RealOutput roomTemp
@@ -53,7 +53,7 @@ model TwinHouseN2
   Modelica.Blocks.Sources.CombiTimeTable TempAttic(
     tableOnFile=true,
     tableName="measurement",
-    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat"),
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt"),
     columns={2,3})
     annotation (Placement(transformation(extent={{-96,26},{-76,46}})));
   Modelica.Blocks.Math.Add add
@@ -63,7 +63,7 @@ model TwinHouseN2
   Modelica.Blocks.Sources.CombiTimeTable HeatInput(
     tableOnFile=true,
     tableName="measurement",
-    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat"),
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt"),
     columns={20,21,22,23,24,25,26}) "Heat input for every room"
     annotation (Placement(transformation(extent={{-94,-100},{-74,-80}})));
   Modelica.Blocks.Math.Sum sum1(nin=7)
@@ -71,7 +71,7 @@ model TwinHouseN2
   Modelica.Blocks.Sources.CombiTimeTable VentilationRate(
     tableOnFile=true,
     tableName="measurement",
-    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat"),
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt"),
     columns={31}) "Ventilation rate caused by mechanical ventilation system"
     annotation (Placement(transformation(extent={{-96,-12},{-80,4}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature Temp3
@@ -85,7 +85,7 @@ model TwinHouseN2
   Modelica.Blocks.Sources.CombiTimeTable VentTemp(
     tableOnFile=true,
     tableName="measurement",
-    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat"),
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt"),
     columns={29}) "Temperature for mechanical ventilation rate"
     annotation (Placement(transformation(extent={{-96,-40},{-80,-24}})));
   Modelica.Blocks.Math.UnitConversions.From_degC from_degC annotation(Placement(transformation(extent={{-14,34},
@@ -107,7 +107,7 @@ model TwinHouseN2
   Modelica.Blocks.Sources.CombiTimeTable MeasuredTemperatures(
     tableOnFile=true,
     tableName="measurement",
-    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.mat"),
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/TwinHouseN2.txt"),
     columns={5,6,7,8,9,10,11,12,13})
     "Measured temperatures for every roo, on the ground floor"
     annotation (Placement(transformation(extent={{104,32},{124,52}})));
diff --git a/AixLib/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mo b/AixLib/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mo
index 7da2d9c302..6dd304ce38 100644
--- a/AixLib/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mo
+++ b/AixLib/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mo
@@ -32,7 +32,7 @@ model Warehouse
   Modelica.Blocks.Sources.CombiTimeTable BuildingSpecifications(
     tableOnFile=true,
     tableName="Table",
-    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mat"),
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/Data/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.txt"),
     columns={2,3,4,5},
     smoothness=Modelica.Blocks.Types.Smoothness.ContinuousDerivative)
     "Air exchange due to windows in the roof area, {2} Temp in the Building (Top), {3} Temp in the Building (Center), {4} Temp in the Building (Bottom), {5} Air exchange due to windows in the roof"
@@ -78,12 +78,8 @@ model Warehouse
 
   parameter Real solar_absorptance_OW=0.4 "Solar absoptance outer walls ";
 
-  Modelica.Blocks.Sources.RealExpression Cool(y=idealHeaterCooler.coolingPower)
-    annotation (Placement(transformation(extent={{90,-24},{104,-8}})));
   Modelica.Blocks.Interfaces.RealOutput coolingPower
     annotation (Placement(transformation(extent={{128,-26},{148,-6}})));
-  Modelica.Blocks.Sources.RealExpression Heat(y=idealHeaterCooler.heatingPower)
-    annotation (Placement(transformation(extent={{90,-56},{104,-40}})));
   Modelica.Blocks.Interfaces.RealOutput heatingPower
     annotation (Placement(transformation(extent={{146,-58},{166,-38}})));
   Modelica.Blocks.Interfaces.RealOutput coolingEnergy
@@ -146,11 +142,6 @@ equation
   connect(roomTemp, to_degC.y) annotation (Line(points={{158,92},{142,92},{142,91},{138.5,91}}, color={0,0,127}));
   connect(ambientTempExpression.y, to_degC1.u) annotation (Line(points={{106.7,74},{110,74},{110,75},{127,75}}, color={0,0,127}));
   connect(ambientTemp, to_degC1.y) annotation (Line(points={{158,76},{152,76},{152,75},{138.5,75}}, color={0,0,127}));
-  connect(Cool.y, coolingPower)
-    annotation (Line(points={{104.7,-16},{138,-16}},
-                                                 color={0,0,127}));
-  connect(Heat.y, heatingPower)
-    annotation (Line(points={{104.7,-48},{156,-48}}, color={0,0,127}));
   connect(coolingEnergy, to_kWh.y) annotation (Line(points={{156,-32},{150,-32},
           {150,-31},{140.5,-31}},
                                color={0,0,127}));
@@ -160,15 +151,9 @@ equation
   connect(heatingPower, heatingPower)
     annotation (Line(points={{156,-48},{156,-48}},
                                                color={0,0,127}));
-  connect(heatingPower, integrator2.u) annotation (Line(points={{156,-48},{112,
-          -48},{112,-64.75},{114.1,-64.75}},
-                                    color={0,0,127}));
   connect(to_kWh1.u, integrator2.y) annotation (Line(points={{129,-65},{128,-65},
           {128,-64.75},{124.45,-64.75}},
                                     color={0,0,127}));
-  connect(coolingPower, integrator1.u) annotation (Line(points={{138,-16},{
-          112.1,-16},{112.1,-30.75}},
-                              color={0,0,127}));
   connect(integrator1.y, to_kWh.u) annotation (Line(points={{122.45,-30.75},{
           128.225,-30.75},{128.225,-31},{129,-31}},
                                                  color={0,0,127}));
@@ -182,11 +167,22 @@ equation
   connect(Source_TsetC1.y, prescribedTemperature.T) annotation (Line(points={{-77.2,
           -78},{-53.2,-78}},                                          color={0,
           0,127}));
-  connect(roomTempBottom, roomTempBottom) annotation (Line(points={{158,28},{158,28}}, color={0,0,127}));
+  connect(roomTempBottom, roomTempBottom) annotation (Line(points={{158,28},{
+          158,28}},                                                                    color={0,0,127}));
   connect(roomTemp, roomTemp) annotation (Line(points={{158,92},{158,92}}, color={0,0,127}));
   connect(MeasuredTemperatures.y, gain.u)
     annotation (Line(points={{106.7,12},{120.8,12}}, color={0,0,127}));
   connect(gain.y, meanMeasuredTemp) annotation (Line(points={{134.6,12},{158,12}}, color={0,0,127}));
+  connect(idealHeaterCooler.coolingPower, coolingPower) annotation (Line(points
+        ={{50,-60.6},{66,-60.6},{66,-60},{82,-60},{82,-16},{138,-16}}, color={0,
+          0,127}));
+  connect(idealHeaterCooler.coolingPower, integrator1.u) annotation (Line(
+        points={{50,-60.6},{82,-60.6},{82,-30.75},{112.1,-30.75}}, color={0,0,
+          127}));
+  connect(idealHeaterCooler.heatingPower, heatingPower) annotation (Line(points
+        ={{50,-56},{110,-56},{110,-48},{156,-48}}, color={0,0,127}));
+  connect(idealHeaterCooler.heatingPower, integrator2.u) annotation (Line(
+        points={{50,-56},{110,-56},{110,-64.75},{114.1,-64.75}}, color={0,0,127}));
   annotation (experiment(StopTime=31536000, Tolerance=1e-06),
     __Dymola_Commands(file=
           "Resources/Scripts/Dymola/ThermalZones/HighOrder/Validation/EmpiricalValidation/Warehouse.mos"
diff --git a/AixLib/ThermalZones/ISO13790/BaseClasses/GainMass.mo b/AixLib/ThermalZones/ISO13790/BaseClasses/GainMass.mo
new file mode 100644
index 0000000000..869650f3f1
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/BaseClasses/GainMass.mo
@@ -0,0 +1,50 @@
+within AixLib.ThermalZones.ISO13790.BaseClasses;
+model GainMass "Mass node heat flow"
+  Modelica.Units.SI.Area AMas "Effective mass area (see Table 12 in standard)";
+  parameter Modelica.Units.SI.Area ATot "Total area of building's surfaces facing the thermal zone";
+  parameter Real facMas "Effective mass area factor";
+  parameter Modelica.Units.SI.Area AFlo "Floor area";
+  Modelica.Blocks.Interfaces.RealInput intSenGai(final unit="W") "Internal sensible heat gains"
+    annotation (Placement(transformation(extent={{-140,-60},{-100,-20}})));
+  Modelica.Blocks.Interfaces.RealInput solGai(final unit="W") "Solar gains"
+    annotation (Placement(transformation(extent={{-140,-100},{-100,-60}})));
+  Modelica.Blocks.Interfaces.RealOutput masGai(final unit="W") "Heat gain to mass node"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+
+equation
+  AMas  = facMas*AFlo;
+  masGai=((AMas/ATot)*(0.5*intSenGai + solGai));
+
+  annotation (defaultComponentName="phiMas",
+    Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{26,26},{-28,-28}},
+          pattern=LinePattern.None,
+          fillColor={238,46,47},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Text(
+          extent={{-108,136},{114,104}},
+          textColor={0,0,255},
+          textString="%name")}),
+    Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+This model calculates the heat gains injected to the mass node. More information
+can be found in the documentation of <a href=\"modelica://AixLib.ThermalZones.ISO13790.Zone5R1C.Zone\">
+AixLib.ThermalZones.ISO13790.Zone5R1C.Zone</a>
+</p>
+</html>", revisions="<html><ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul></html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GainMass;
diff --git a/AixLib/ThermalZones/ISO13790/BaseClasses/GainSurface.mo b/AixLib/ThermalZones/ISO13790/BaseClasses/GainSurface.mo
new file mode 100644
index 0000000000..e8de8fd43d
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/BaseClasses/GainSurface.mo
@@ -0,0 +1,49 @@
+within AixLib.ThermalZones.ISO13790.BaseClasses;
+model GainSurface "Surface node heat flow"
+  Modelica.Units.SI.Area AMas "Effective mass area (see Table 12 in standard)";
+  parameter Modelica.Units.SI.Area ATot "Total area of building's surfaces facing the thermal zone";
+  parameter Modelica.Units.SI.ThermalConductance HWinGai "Thermal conductance through windows";
+  parameter Real facMas "Effective mass area factor";
+  parameter Modelica.Units.SI.Area AFlo "Floor area";
+  Modelica.Blocks.Interfaces.RealInput intSenGai(final unit="W") "Internal sensible heat gains"
+    annotation (Placement(transformation(extent={{-140,-60},{-100,-20}})));
+  Modelica.Blocks.Interfaces.RealInput solGai(final unit="W") "Solar gains"
+    annotation (Placement(transformation(extent={{-140,-100},{-100,-60}})));
+  Modelica.Blocks.Interfaces.RealOutput surGai(final unit="W") "Heat gain to surface node"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+
+equation
+  AMas  = facMas*AFlo;
+  surGai= (1 - AMas/ATot - HWinGai/(9.1*ATot))*(0.5*intSenGai + solGai);
+
+  annotation (defaultComponentName="phiSur",Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(
+          extent={{-100,100},{100,-100}},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Ellipse(
+          extent={{28,-46},{-26,-100}},
+          pattern=LinePattern.None,
+          fillColor={238,46,47},
+          fillPattern=FillPattern.Solid,
+          lineColor={0,0,0}),
+        Text(
+          extent={{-110,138},{112,106}},
+          textColor={0,0,255},
+          textString="%name")}),                                 Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+This model calculates the heat gains injected to the surface node. More information
+can be found in the documentation of <a href=\"modelica://AixLib.ThermalZones.ISO13790.Zone5R1C.Zone\">
+AixLib.ThermalZones.ISO13790.Zone5R1C.Zone</a>
+</p>
+</html>", revisions="<html><ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul></html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GainSurface;
diff --git a/AixLib/ThermalZones/ISO13790/BaseClasses/GlazedElements.mo b/AixLib/ThermalZones/ISO13790/BaseClasses/GlazedElements.mo
new file mode 100644
index 0000000000..99b1d048a7
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/BaseClasses/GlazedElements.mo
@@ -0,0 +1,107 @@
+within AixLib.ThermalZones.ISO13790.BaseClasses;
+model GlazedElements
+  parameter Integer n;
+  parameter Real AWin[:] "Area of windows";
+  parameter Real surTil[:] "Tilt angle of surfaces";
+  parameter Real surAzi[:] "Azimuth angle of surfaces";
+  parameter Real gFac "Energy transmittance of glazings";
+  parameter Real winFra "Frame fraction of windows";
+  parameter Real shaRedFac(
+    final min=0,
+    final unit="1")= 0.9 "Shading reduction factor";
+
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus annotation (Placement(
+        transformation(extent={{-120,-20},{-80,20}}), iconTransformation(extent=
+           {{-110,-10},{-90,10}})));
+  BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTil[n](
+  final til=surTil,
+  final azi=surAzi)
+    "Direct solar irradiation on surface"
+    annotation (Placement(transformation(extent={{-60,20},{-40,40}})));
+  Modelica.Blocks.Math.Gain solRad[n](final k=AWin*gFac*shaRedFac*(1 - winFra))
+    "Solar radiation"
+    annotation (Placement(transformation(extent={{20,-10},{40,10}})));
+  Modelica.Blocks.Interfaces.RealOutput solRadWin
+    "Solar radiation through windows"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  BoundaryConditions.SolarIrradiation.DiffusePerez HDifTil[n](
+  final til=surTil,
+  final azi=surAzi)
+    "Diffuse solar irradiation on surface"
+    annotation (Placement(transformation(extent={{-60,-40},{-40,-20}})));
+protected
+  Modelica.Blocks.Math.Add irr[n]
+    "Total of direct and diffuse radiation on surface"
+    annotation (Placement(transformation(extent={{-20,-10},{0,10}})));
+  Modelica.Blocks.Math.MultiSum multiSum(final nu=n) "Sum of all orientations"
+    annotation (Placement(transformation(extent={{62,-6},{74,6}})));
+
+equation
+  for i in 1:n loop
+  connect(weaBus,HDifTil[i].weaBus) annotation (Line(
+      points={{-100,0},{-72,0},{-72,-30},{-60,-30}},
+      color={255,204,51},
+      thickness=0.5));
+  end for;
+
+  for i in 1:n loop
+  connect(weaBus,HDirTil[i].weaBus) annotation (Line(
+      points={{-100,0},{-72,0},{-72,30},{-60,30}},
+      color={255,204,51},
+      thickness=0.5));
+  end for;
+  connect(solRad.y, multiSum.u)
+    annotation (Line(points={{41,0},{62,0}}, color={0,0,127}));
+  connect(multiSum.y, solRadWin)
+    annotation (Line(points={{75.02,0},{110,0}}, color={0,0,127}));
+  connect(HDirTil.H,irr. u1) annotation (Line(points={{-39,30},{-30,30},{-30,6},
+          {-22,6}}, color={0,0,127}));
+  connect(HDifTil.H,irr. u2) annotation (Line(points={{-39,-30},{-30,-30},{-30,-6},
+          {-22,-6}}, color={0,0,127}));
+
+  connect(irr.y, solRad.u)
+    annotation (Line(points={{1,0},{18,0}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(extent={{-100,100},{100,-100}}, lineColor={95,95,95},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-34,88},{-84,38}},
+          lineColor={255,255,0},
+          lineThickness=0.5,
+          fillColor={244,125,35},
+          fillPattern=FillPattern.Sphere),
+        Polygon(
+          points={{22,88},{-18,68},{-18,-92},{22,-52},{22,88}},
+          lineColor={95,95,95},
+          fillColor={170,213,255},
+          fillPattern=FillPattern.Solid,
+          lineThickness=0.5),
+        Text(
+          extent={{-108,148},{114,116}},
+          textColor={0,0,255},
+          textString="%name")}),                                 Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+        Documentation(info="<html>
+<p>
+This model calculates the heat flow by solar gains through each glazed element <i>k</i>. The heat flow is given by 
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&Phi;<sub>sol,k</sub> =F<sub>sh,k </sub>I<sub>sol,k </sub>g<sub>fac</sub> (1-F<sub>frame</sub>) A<sub>win,k</sub>
+</p>
+<p>
+where <i>F<sub>sh,k</sub></i> is the shading reduction factor which is set to 0.9 by deafult, 
+<i>I<sub>sol,k</sub></i> is the solar irradiance
+per square meter of surface area, <i>g<sub>fac</sub></i> is the total solar energy transmittance of the trasparent
+element, <i>F<sub>frame</sub></i> is the frame area fraction, and <i>A<sub>win,k</sub></i> is the overall area of 
+the glazed element in square meters.
+The model neglects the extra heat flow due to thermal radiation to the sky from the building.
+</p>
+</html>", revisions="<html><ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul></html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end GlazedElements;
diff --git a/AixLib/ThermalZones/ISO13790/BaseClasses/OpaqueElements.mo b/AixLib/ThermalZones/ISO13790/BaseClasses/OpaqueElements.mo
new file mode 100644
index 0000000000..d7b29957bf
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/BaseClasses/OpaqueElements.mo
@@ -0,0 +1,196 @@
+within AixLib.ThermalZones.ISO13790.BaseClasses;
+model OpaqueElements
+  parameter Integer n;
+  parameter Real AWal[:] "Area of external walls";
+  parameter Real ARoo "Area of roof";
+  parameter Real UWal "U-value of external walls";
+  parameter Real URoo "U-value of roof";
+  parameter Real surTil[:] "Tilt angle of surfaces";
+  parameter Real surAzi[:] "Azimuth angle of surfaces";
+  parameter Real eps=0.9 "Emissivity of external surface";
+  parameter Real alp=0.6 "Absorption coefficient";
+  parameter Real surRes=0.04 "External surface heat resistance";
+
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus annotation (Placement(
+        transformation(extent={{-120,-20},{-80,20}}), iconTransformation(extent=
+           {{-110,-10},{-90,10}})));
+  BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTil[n](
+  final til=surTil,
+  final azi=surAzi)
+    annotation (Placement(transformation(extent={{-80,60},{-60,80}})));
+  Modelica.Blocks.Math.Gain solRadOpa[n](final k=AWal*alp*UWal*surRes)
+    "Solar radiation on vertical opaque surfaces"
+    annotation (Placement(transformation(extent={{-10,60},{10,80}})));
+  Modelica.Blocks.Interfaces.RealOutput y "Solar radiation through windows"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+  BoundaryConditions.SolarIrradiation.DiffusePerez HDifTil [n](
+  final til=surTil,
+  final azi=surAzi)
+    annotation (Placement(transformation(extent={{-80,20},{-60,40}})));
+  Modelica.Blocks.Math.Add irrOpa[n]
+    "Total of direct and diffuse radiation on surface"
+    annotation (Placement(transformation(extent={{-40,60},{-20,80}})));
+  Modelica.Blocks.Math.Add addOpa[n](each k2=-1)
+    "Total of direct and diffuse radiation on vertical surfaces"
+    annotation (Placement(transformation(extent={{20,40},{40,60}})));
+  Modelica.Blocks.Math.Gain theRadOpa[n](each k=5*eps*11*0.5)
+    "Extra thermal radiation through walls"
+    annotation (Placement(transformation(extent={{-10,10},{10,30}})));
+  Modelica.Blocks.Math.Add irrRoo
+    "Total of direct and diffuse radiation on the south facade"
+    annotation (Placement(transformation(extent={{-40,-40},{-20,-20}})));
+  Modelica.Blocks.Math.Gain solRadRoo(final k=ARoo*alp*URoo*surRes)
+    "Solar radiation on roof"
+    annotation (Placement(transformation(extent={{-10,-40},{10,-20}})));
+  Modelica.Blocks.Math.Gain theRadRoo(final k=5*eps*11*1)
+    "Extra thermal radiation through roof"
+    annotation (Placement(transformation(extent={{-10,-90},{10,-70}})));
+  Modelica.Blocks.Math.Add addRoo(k2=-1)
+    "Total of direct and diffuse radiation on the roof"
+    annotation (Placement(transformation(extent={{20,-60},{40,-40}})));
+  Modelica.Blocks.Math.MultiSum multiSum(nu=n)
+    annotation (Placement(transformation(extent={{48,44},{60,56}})));
+  Modelica.Blocks.Math.Add addTot
+    "Total of direct and diffuse radiation on the south facade"
+    annotation (Placement(transformation(extent={{72,-10},{92,10}})));
+protected
+  Modelica.Blocks.Sources.RealExpression facOpa[n](y=UWal*AWal*surRes) "factor"
+    annotation (Placement(transformation(extent={{-40,10},{-20,30}})));
+  BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoo(til=0, azi=
+       0) annotation (Placement(transformation(extent={{-80,-40},{-60,-20}})));
+  BoundaryConditions.SolarIrradiation.DiffusePerez HDifTilRof(til=0, azi=0)
+    annotation (Placement(transformation(extent={{-80,-80},{-60,-60}})));
+protected
+  Modelica.Blocks.Sources.RealExpression facRoo(y=URoo*ARoo*surRes) "factor"
+    annotation (Placement(transformation(extent={{-40,-90},{-20,-70}})));
+equation
+  for i in 1:n loop
+  connect(weaBus,HDifTil[i].weaBus) annotation (Line(
+      points={{-100,0},{-90,0},{-90,30},{-80,30}},
+      color={255,204,51},
+      thickness=0.5));
+  end for;
+
+  for i in 1:n loop
+  connect(weaBus,HDirTil[i].weaBus) annotation (Line(
+      points={{-100,0},{-90,0},{-90,70},{-80,70}},
+      color={255,204,51},
+      thickness=0.5));
+  end for;
+  connect(HDirTil.H, irrOpa.u1) annotation (Line(points={{-59,70},{-50,70},{-50,
+          76},{-42,76}}, color={0,0,127}));
+  connect(HDifTil.H, irrOpa.u2) annotation (Line(points={{-59,30},{-48,30},{-48,
+          64},{-42,64}}, color={0,0,127}));
+
+  connect(irrOpa.y, solRadOpa.u)
+    annotation (Line(points={{-19,70},{-12,70}}, color={0,0,127}));
+  connect(HDirTilRoo.H, irrRoo.u1) annotation (Line(points={{-59,-30},{-50,-30},
+          {-50,-24},{-42,-24}}, color={0,0,127}));
+  connect(HDifTilRof.H, irrRoo.u2) annotation (Line(points={{-59,-70},{-48,-70},
+          {-48,-36},{-42,-36}}, color={0,0,127}));
+  connect(HDirTilRoo.weaBus, weaBus) annotation (Line(
+      points={{-80,-30},{-90,-30},{-90,0},{-100,0}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(HDifTilRof.weaBus, weaBus) annotation (Line(
+      points={{-80,-70},{-90,-70},{-90,0},{-100,0}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(irrRoo.y, solRadRoo.u)
+    annotation (Line(points={{-19,-30},{-12,-30}}, color={0,0,127}));
+  connect(facRoo.y, theRadRoo.u)
+    annotation (Line(points={{-19,-80},{-12,-80}}, color={0,0,127}));
+  connect(addOpa.y, multiSum.u)
+    annotation (Line(points={{41,50},{48,50}}, color={0,0,127}));
+  connect(solRadOpa.y, addOpa.u1) annotation (Line(points={{11,70},{14,70},{14,
+          56},{18,56}},
+                    color={0,0,127}));
+  connect(theRadRoo.y, addRoo.u2) annotation (Line(points={{11,-80},{14,-80},{
+          14,-56},{18,-56}},
+                          color={0,0,127}));
+  connect(solRadRoo.y, addRoo.u1) annotation (Line(points={{11,-30},{14,-30},{
+          14,-44},{18,-44}},
+                          color={0,0,127}));
+  connect(addTot.y, y)
+    annotation (Line(points={{93,0},{110,0}}, color={0,0,127}));
+  connect(addRoo.y, addTot.u2) annotation (Line(points={{41,-50},{64,-50},{64,-6},
+          {70,-6}}, color={0,0,127}));
+  connect(multiSum.y, addTot.u1) annotation (Line(points={{61.02,50},{64,50},{64,
+          6},{70,6}}, color={0,0,127}));
+  connect(facOpa.y, theRadOpa.u)
+    annotation (Line(points={{-19,20},{-12,20}}, color={0,0,127}));
+  connect(theRadOpa.y, addOpa.u2) annotation (Line(points={{11,20},{14,20},{14,
+          44},{18,44}},
+                    color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false), graphics={
+        Rectangle(extent={{-100,100},{100,-100}}, lineColor={95,95,95},
+          fillColor={255,255,255},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-34,88},{-84,38}},
+          lineColor={255,255,0},
+          lineThickness=0.5,
+          fillColor={244,125,35},
+          fillPattern=FillPattern.Sphere),                        Rectangle(
+    extent={{-84,28},{-64,-6}},       fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{-58,28},{-4,-6}},       fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{2,28},{56,-6}},       fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{62,28},{88,-6}},       fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{34,-12},{88,-46}},      fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}),  Rectangle(
+    extent={{-26,-12},{28,-46}},      fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{-84,-12},{-32,-46}},      fillColor = {255, 213, 170},
+   fillPattern =  FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{-84,-52},{-64,-86}},      fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{-58,-52},{-4,-86}},      fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{2,-52},{56,-86}},      fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
+    extent={{62,-52},{88,-84}},      fillColor = {255, 213, 170},
+   fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}),
+        Text(
+          extent={{-110,148},{112,116}},
+          textColor={0,0,255},
+          textString="%name")}),                                 Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    Documentation(info="<html>
+<p>
+This model calculates the heat flow by solar gains through each opaque building element <i>k</i>. The heat flow is given by
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&Phi;<sub>sol,k</sub> =F<sub>sh,k </sub>I<sub>sol,k </sub> &alpha;<sub>k</sub> R<sub>se</sub> U<sub>k</sub>
+A<sub>k</sub> - F<sub>f</sub> &Phi;<sub>r,k</sub>
+</p>
+<p>
+where <i>F<sub>sh,k</sub></i> is the shading reduction factor, <i>I<sub>sol,k</sub></i> is the solar irradiance
+per square meter of surface area, <i>&alpha;<sub>k</sub></i> is the dimensionless absportion coefficient for solar radiation of the opaque element,
+<i>R<sub>se</sub></i> is the external surface heat resistance of the opaque element in (m K/W), and <i>A<sub>k</sub></i> is the area of the opaque element.
+</p>
+<p>
+The form factor between the building element and the sky <i>F<sub>f</sub></i> is set to 1 for roofs and 0.5 for external walls. The extra heat flow due to
+thermal radiation to the sky is given by
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&Phi;<sub>r,k</sub> =h<sub>r</sub> &#916;T<sub>sky</sub> R<sub>se</sub> U<sub>k</sub> A<sub>k</sub>
+</p>
+<p>
+where <i>h<sub>r</sub></i> is the external radiative heat transfer coefficent
+which is approximated as 5 &epsilon; W/m<sup>2</sup>K (where &epsilon; is the emissivity for
+the thermal radiation of the external surface), and &#916;T<sub>sky</sub> is
+the average temperature difference between the external air temperature and the
+apparent sky temperature.
+</p>
+</html>", revisions="<html><ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul></html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end OpaqueElements;
diff --git a/AixLib/ThermalZones/ISO13790/BaseClasses/package.mo b/AixLib/ThermalZones/ISO13790/BaseClasses/package.mo
new file mode 100644
index 0000000000..b0690bf0dc
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/BaseClasses/package.mo
@@ -0,0 +1,11 @@
+within AixLib.ThermalZones.ISO13790;
+package BaseClasses "Package with base classes for AixLib.Fluid"
+extends Modelica.Icons.BasesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+This package contains base classes that are used to construct the models in
+<a href=\"modelica://AixLib.ThermalZones.ISO13790\">IBPSA.ThermalZones.ISO13790</a>.
+</p>
+</html>"));
+end BaseClasses;
diff --git a/AixLib/ThermalZones/ISO13790/BaseClasses/package.order b/AixLib/ThermalZones/ISO13790/BaseClasses/package.order
new file mode 100644
index 0000000000..e1de460275
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/BaseClasses/package.order
@@ -0,0 +1,4 @@
+GainMass
+GainSurface
+GlazedElements
+OpaqueElements
diff --git a/AixLib/ThermalZones/ISO13790/Data/Generic.mo b/AixLib/ThermalZones/ISO13790/Data/Generic.mo
new file mode 100644
index 0000000000..a2eacad7ec
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Data/Generic.mo
@@ -0,0 +1,25 @@
+within AixLib.ThermalZones.ISO13790.Data;
+record Generic "Generic data record for building thermal mass"
+   extends Modelica.Icons.Record;
+
+   parameter Real heaC(final unit="J/(K.m2)")
+    "Heat capacity per unit area of the floor"
+    annotation (Dialog(group="Thermal mass"));
+   parameter Real facMas(final unit="1")
+    "Effective mass area factor"
+    annotation (Dialog(group="Thermal mass"));
+  annotation (defaultComponentName="theMas",
+Documentation(revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Generic record for the internal heat capacity of the building zone per unit area of the floor.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Generic;
diff --git a/AixLib/ThermalZones/ISO13790/Data/Heavy.mo b/AixLib/ThermalZones/ISO13790/Data/Heavy.mo
new file mode 100644
index 0000000000..4547c817c3
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Data/Heavy.mo
@@ -0,0 +1,19 @@
+within AixLib.ThermalZones.ISO13790.Data;
+record Heavy = ISO13790.Data.Generic(
+    heaC=260000,
+    facMas=3) "Heavy"
+     annotation (
+  Documentation(revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>",
+info="<html>
+<p>
+Internal heat capacity per unit area of the floor for heavy buildings.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/ThermalZones/ISO13790/Data/Light.mo b/AixLib/ThermalZones/ISO13790/Data/Light.mo
new file mode 100644
index 0000000000..e58539ad92
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Data/Light.mo
@@ -0,0 +1,19 @@
+within AixLib.ThermalZones.ISO13790.Data;
+record Light = ISO13790.Data.Generic(
+    heaC=110000,
+    facMas=2.5) "Light"
+     annotation (
+  Documentation(revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>",
+info="<html>
+<p>
+Internal heat capacity per unit area of the floor for light buildings.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/ThermalZones/ISO13790/Data/Medium.mo b/AixLib/ThermalZones/ISO13790/Data/Medium.mo
new file mode 100644
index 0000000000..44af605a52
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Data/Medium.mo
@@ -0,0 +1,19 @@
+within AixLib.ThermalZones.ISO13790.Data;
+record Medium = ISO13790.Data.Generic(
+    heaC=165000,
+    facMas=2.5) "Medium"
+     annotation (
+  Documentation(revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>",
+info="<html>
+<p>
+Internal heat capacity per unit area of the floor for medium buildings.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/ThermalZones/ISO13790/Data/package.mo b/AixLib/ThermalZones/ISO13790/Data/package.mo
new file mode 100644
index 0000000000..70ac817827
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Data/package.mo
@@ -0,0 +1,10 @@
+within AixLib.ThermalZones.ISO13790;
+package Data "Package with pre-defined building thermal mass"
+extends Modelica.Icons.MaterialPropertiesPackage;
+
+annotation (Documentation(info="<html>
+<p>
+Package with data for thermal mass of buildings.
+</p>
+</html>"));
+end Data;
diff --git a/AixLib/ThermalZones/ISO13790/Data/package.order b/AixLib/ThermalZones/ISO13790/Data/package.order
new file mode 100644
index 0000000000..c32abce1d1
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Data/package.order
@@ -0,0 +1,4 @@
+Generic
+Heavy
+Light
+Medium
diff --git a/AixLib/ThermalZones/ISO13790/Examples/FreeFloating.mo b/AixLib/ThermalZones/ISO13790/Examples/FreeFloating.mo
new file mode 100644
index 0000000000..11fd5b3ea6
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Examples/FreeFloating.mo
@@ -0,0 +1,57 @@
+within AixLib.ThermalZones.ISO13790.Examples;
+model FreeFloating "Illustrates the use of the 5R1C thermal zone in free-floating conditions"
+  extends Modelica.Icons.Example;
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+        Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos")) "weather data"
+    annotation (Placement(transformation(extent={{-80,10},{-60,30}})));
+  Zone5R1C.Zone zon5R1C(
+    airRat=0.5,
+    AWin={0,0,3,0},
+    UWin=1.8,
+    AWal={12,12,9,12},
+    ARoo=16,
+    UWal=1.3,
+    URoo=1.3,
+    UFlo=1,
+    AFlo=16,
+    VRoo=16*3,
+    redeclare replaceable AixLib.ThermalZones.ISO13790.Data.Light buiMas,
+    nOrientations=4,
+    surTil={1.5707963267949,1.5707963267949,1.5707963267949,1.5707963267949},
+    surAzi={3.1415926535898,-1.5707963267949,0,1.5707963267949},
+    gFac=0.5) "Thermal zone"
+    annotation (Placement(transformation(extent={{26,-12},{54,16}})));
+  Modelica.Blocks.Sources.Constant intGains(k=10) "internal heat gains in Watt"
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+equation
+  connect(zon5R1C.weaBus, weaDat.weaBus) annotation (Line(
+      points={{50,13},{50,20},{-60,20}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(zon5R1C.intSenGai, intGains.y)
+    annotation (Line(points={{24,12},{-40,12},{-40,-10},{-59,-10}},   color={0,0,127}));
+  annotation (experiment(
+    StartTime=8640000,
+    StopTime=9504000,
+    Tolerance=1e-6),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/FreeFloating.mos"
+        "Simulate and plot"),
+  Documentation(info="<html>
+<p>
+This model illustrates the use of <a href=\"modelica://AixLib.ThermalZones.ISO13790.Zone5R1C.Zone\">
+AixLib.ThermalZones.ISO13790.Zone5R1C.Zone</a> in a free-floating case 
+(i.e. no heating or cooling)
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FreeFloating;
diff --git a/AixLib/ThermalZones/ISO13790/Examples/FreeFloatingHVAC.mo b/AixLib/ThermalZones/ISO13790/Examples/FreeFloatingHVAC.mo
new file mode 100644
index 0000000000..2edef8859a
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Examples/FreeFloatingHVAC.mo
@@ -0,0 +1,60 @@
+within AixLib.ThermalZones.ISO13790.Examples;
+model FreeFloatingHVAC "Illustrates the use of the 5R1C HVAC thermal zone in free-floating conditions"
+  extends Modelica.Icons.Example;
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+        Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_IL_Chicago-OHare.Intl.AP.725300_TMY3.mos")) "weather data"
+    annotation (Placement(transformation(extent={{-80,10},{-60,30}})));
+  Zone5R1C.ZoneHVAC zonHVAC(
+    airRat=0.5,
+    AWin={0,0,3,0},
+    UWin=1.8,
+    AWal={12,12,9,12},
+    ARoo=16,
+    UWal=1.3,
+    URoo=1.3,
+    UFlo=1,
+    AFlo=16,
+    VRoo=16*3,
+    nOrientations=4,
+    surTil={1.5707963267949,1.5707963267949,1.5707963267949,1.5707963267949},
+    surAzi={3.1415926535898,-1.5707963267949,0,1.5707963267949},
+    gFac=0.5,
+    redeclare package Medium = AixLib.Media.Air,
+    redeclare AixLib.ThermalZones.ISO13790.Data.Light buiMas) "Thermal zone"
+    annotation (Placement(transformation(extent={{26,-12},{54,16}})));
+  Modelica.Blocks.Sources.Constant intGains(k=10) "Internal heat gains"
+    annotation (Placement(transformation(extent={{-80,-30},{-60,-10}})));
+  Modelica.Blocks.Sources.Constant latGains(k=0) "Latent gains"
+    annotation (Placement(transformation(extent={{-80,-60},{-60,-40}})));
+equation
+  connect(zonHVAC.weaBus, weaDat.weaBus) annotation (Line(
+      points={{50,13},{50,20},{-60,20}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(latGains.y, zonHVAC.intLatGai) annotation (Line(points={{-59,-50},{
+          -32,-50},{-32,6},{24,6}},   color={0,0,127}));
+  connect(intGains.y, zonHVAC.intSenGai) annotation (Line(points={{-59,-20},{
+          -40,-20},{-40,12},{24,12}},   color={0,0,127}));
+  annotation (experiment(
+    StartTime=8640000,
+    StopTime=9504000,
+    Tolerance=1e-06),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/FreeFloatingHVAC.mos"
+        "Simulate and plot"),
+  Documentation(info="<html>
+<p>
+This model illustrates the use of <a href=\"modelica://AixLib.ThermalZones.ISO13790.Zone5R1C.ZoneHVAC\">
+AixLib.ThermalZones.ISO13790.Zone5R1C.ZoneHVAC</a> in a free-floating case (i.e. no heating or cooling).
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end FreeFloatingHVAC;
diff --git a/AixLib/ThermalZones/ISO13790/Examples/HeatingCooling.mo b/AixLib/ThermalZones/ISO13790/Examples/HeatingCooling.mo
new file mode 100644
index 0000000000..78e97cced1
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Examples/HeatingCooling.mo
@@ -0,0 +1,97 @@
+within AixLib.ThermalZones.ISO13790.Examples;
+model HeatingCooling "Illustrates the use of the 5R1C thermal zone with heating and cooling"
+  extends FreeFloating(zon5R1C(
+      airRat=0.5,
+      AWin={0,0,3,0},
+      UWin=1.8,
+      AWal={12,12,9,12},
+      ARoo=16,
+      UWal=1.3,
+      URoo=1.3,
+      AFlo=16,
+      VRoo=16*3,
+      redeclare AixLib.ThermalZones.ISO13790.Data.Light buiMas,
+      gFac=0.5) "Thermal zone");
+  Modelica.Blocks.Math.Sum sumHeaCoo(nin=2)
+    "Sum of heating and cooling heat flow rate"
+    annotation (Placement(visible = true, transformation(extent={{44,56},{52,64}},rotation = 0)));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow preHeaCoo
+    "Prescribed heat flow for heating and cooling"
+    annotation (Placement(visible=true, transformation(extent={{58,54},{70,66}},rotation=0)));
+  Modelica.Blocks.Math.Gain gaiHea(k=1E6) "Gain for heating"
+    annotation (Placement(visible=true,transformation(origin={12,72},extent={{-6,-6},{6,6}},rotation=0)));
+  AixLib.Controls.Continuous.LimPID conHeaPID(
+    Ti=300,
+    k=0.1,
+    reverseActing=true,
+    strict=true) "Controller for heating"
+    annotation (Placement(visible=true, transformation(origin={-10,72},extent={{-6,-6},{6,6}},rotation=0)));
+  Modelica.Blocks.Sources.Constant TSetHea(k=273.15 + 20)
+    "Set-point for heating"
+    annotation (Placement(visible=true, transformation(origin={-34,72},extent={{-6,-6},{6,6}},rotation=0)));
+  Modelica.Blocks.Sources.Constant TSetCoo(k=273.15 + 27)
+    "Set-point for cooling"
+    annotation (Placement(visible=true, transformation(origin={-34,46},extent={{-6,-6},{6,6}},rotation=0)));
+  Modelica.Blocks.Routing.Multiplex2 multiplex2 annotation (
+    Placement(visible = true, transformation(extent={{30,56},{38,64}},      rotation = 0)));
+  Modelica.Blocks.Math.Gain gaiCoo(k=-1E6) "Gain for cooling"
+    annotation (Placement(visible=true,transformation(origin={12,46},extent={{-6,-6},{6,6}},rotation=0)));
+  AixLib.Controls.Continuous.LimPID conCooPID(
+    Ti=300,
+    k=0.1,
+    reverseActing=false,
+    strict=true) "Controller for cooling"
+    annotation (Placement(visible=true, transformation(origin={-10,46},extent={{-6,-6},{6,6}},rotation=0)));
+equation
+  connect(sumHeaCoo.y, preHeaCoo.Q_flow)
+    annotation (Line(points={{52.4,60},{58,60}}, color={0,0,127}));
+  connect(conHeaPID.y, gaiHea.u)
+    annotation (Line(points={{-3.4,72},{4.8,72}}, color={0,0,127}));
+  connect(TSetHea.y, conHeaPID.u_s)
+    annotation (Line(points={{-27.4,72},{-17.2,72}}, color={0,0,127}));
+  connect(multiplex2.y,sumHeaCoo. u)
+    annotation (
+    Line(points={{38.4,60},{43.2,60}},      color = {0, 0, 127}));
+  connect(conCooPID.u_s, TSetCoo.y)
+    annotation (Line(points={{-17.2,46},{-27.4,46}}, color={0,0,127}));
+  connect(conCooPID.y, gaiCoo.u)
+    annotation (Line(points={{-3.4,46},{4.8,46}}, color={0,0,127}));
+  connect(conHeaPID.y, gaiHea.u)
+    annotation (Line(points={{-3.4,72},{4.8,72}}, color={0,0,127}));
+  connect(gaiHea.y, multiplex2.u1[1])
+    annotation (Line(points={{18.6,72},{22,72},{22,62},{28,62},{28,62.4},{29.2,62.4}},
+                                                 color={0,0,127}));
+  connect(gaiCoo.y, multiplex2.u2[1])
+    annotation (Line(points={{18.6,46},{22,46},{22,58},{28,58},{28,57.6},{29.2,57.6}},
+                                                 color={0,0,127}));
+  connect(gaiCoo.u, conCooPID.y)
+    annotation (Line(points={{4.8,46},{-3.4,46}}, color={0,0,127}));
+  connect(preHeaCoo.port, zon5R1C.heaPorAir) annotation (Line(points={{70,60},{
+          80,60},{80,6},{44,6},{44,10}}, color={191,0,0}));
+  connect(zon5R1C.TAir, conCooPID.u_m) annotation (Line(points={{55,10},{60,10},
+          {60,30},{-10,30},{-10,38.8}}, color={0,0,127}));
+  connect(zon5R1C.TAir, conHeaPID.u_m) annotation (Line(points={{55,10},{60,10},
+          {60,30},{-50,30},{-50,60},{-10,60},{-10,64.8}}, color={0,0,127}));
+  annotation (experiment(
+    StartTime=8640000,
+    StopTime=9504000,
+    Tolerance=1e-6),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/HeatingCooling.mos"
+        "Simulate and plot"),
+  Documentation(info="<html>
+<p>
+This model illustrates the use of <a href=\"modelica://AixLib.ThermalZones.ISO13790.Zone5R1C.Zone\">
+AixLib.ThermalZones.ISO13790.Zone5R1C.Zone</a> with heating and cooling.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end HeatingCooling;
diff --git a/AixLib/ThermalZones/ISO13790/Examples/HeatingCoolingHVAC.mo b/AixLib/ThermalZones/ISO13790/Examples/HeatingCoolingHVAC.mo
new file mode 100644
index 0000000000..a670dfde51
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Examples/HeatingCoolingHVAC.mo
@@ -0,0 +1,111 @@
+within AixLib.ThermalZones.ISO13790.Examples;
+model HeatingCoolingHVAC "Illustrates the use of the 5R1C HVAC thermal zone connected to a ventilation system"
+  extends FreeFloatingHVAC(zonHVAC(nPorts=2));
+
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow preHeaCoo
+    "Prescribed heat flow for heating and cooling"
+    annotation (Placement(visible=true, transformation(extent={{42,64},{58,80}},
+          rotation=0)));
+  Modelica.Blocks.Math.Gain gaiHea(k=1E6) "Gain for heating"
+    annotation (Placement(visible=true,
+        transformation(
+        origin={12,72},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Controls.Continuous.LimPID conHeaPID(
+    Ti=300,
+    k=0.1,
+    reverseActing=true,
+    strict=true) "Controller for heating"
+    annotation (Placement(visible=true, transformation(
+        origin={-10,72},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Modelica.Blocks.Sources.Constant TSetHea(k=273.15 + 20) "Set-point for heating"
+    annotation (Placement(
+        visible=true, transformation(
+        origin={-34,72},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Fluid.Sources.MassFlowSource_T sou(
+    redeclare package Medium = AixLib.Media.Air,
+    use_m_flow_in=true,
+    T=280.15,
+    nPorts=1) "source of air"
+    annotation (Placement(transformation(extent={{-20,-80},{0,-60}})));
+  Modelica.Blocks.Sources.Constant TSetCoo(k=273.15 + 27)
+    "Set-point for cooling"
+    annotation (Placement(
+        visible=true, transformation(
+        origin={-34,46},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Controls.Continuous.LimPID conCooPID(
+    Ti=300,
+    k=0.1,
+    yMax=0.07,
+    reverseActing=false,
+    strict=true) "Controller for cooling"
+    annotation (Placement(visible=true, transformation(
+        origin={-10,46},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Modelica.Blocks.Math.Gain gaiCoo(k=1) "Gain for cooling"
+    annotation (Placement(visible=true,
+        transformation(
+        origin={12,46},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Fluid.Sources.Boundary_pT sin(
+    redeclare package Medium = AixLib.Media.Air,
+    nPorts=1) "sink"
+    annotation (Placement(transformation(extent={{90,-80},{70,-60}})));
+equation
+  connect(conHeaPID.y,gaiHea. u)
+    annotation (Line(points={{-3.4,72},{4.8,72}}, color={0,0,127}));
+  connect(TSetHea.y,conHeaPID. u_s)
+    annotation (Line(points={{-27.4,72},{-17.2,72}}, color={0,0,127}));
+  connect(conHeaPID.y,gaiHea. u)
+    annotation (Line(points={{-3.4,72},{4.8,72}}, color={0,0,127}));
+  connect(gaiHea.y, preHeaCoo.Q_flow) annotation (Line(points={{18.6,72},{42,72}},
+                            color={0,0,127}));
+  connect(conCooPID.u_s,TSetCoo. y)
+    annotation (Line(points={{-17.2,46},{-27.4,46}}, color={0,0,127}));
+  connect(gaiCoo.u,conCooPID. y)
+    annotation (Line(points={{4.8,46},{-3.4,46}}, color={0,0,127}));
+  connect(sin.ports[1], zonHVAC.ports[1]) annotation (Line(points={{70,-70},{22,
+          -70},{22,-6.2},{27,-6.2}}, color={0,127,255}));
+  connect(preHeaCoo.port, zonHVAC.heaPorAir) annotation (Line(points={{58,72},{
+          68,72},{68,8},{44,8},{44,10}}, color={191,0,0}));
+  connect(sou.ports[1], zonHVAC.ports[2]) annotation (Line(points={{0,-70},{20,
+          -70},{20,-6.2},{27,-6.2}}, color={0,127,255}));
+  connect(sou.m_flow_in, gaiCoo.y) annotation (Line(points={{-22,-62},{-28,-62},
+          {-28,34},{26,34},{26,46},{18.6,46}},color={0,0,127}));
+  connect(zonHVAC.TAir, conCooPID.u_m) annotation (Line(points={{55,10},{60,10},
+          {60,28},{-10,28},{-10,38.8}}, color={0,0,127}));
+  connect(zonHVAC.TAir, conHeaPID.u_m) annotation (Line(points={{55,10},{60,10},
+          {60,60},{-10,60},{-10,64.8}}, color={0,0,127}));
+  annotation (experiment(
+      StartTime=8640000,
+      StopTime=9504000,
+      Tolerance=1e-06),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Examples/HeatingCoolingHVAC.mos"
+        "Simulate and plot"),
+  Documentation(info="<html>
+<p>
+This model illustrates the use of <a href=\"modelica://AixLib.ThermalZones.ISO13790.Zone5R1C.ZoneHVAC\">
+AixLib.ThermalZones.ISO13790.Zone5R1C.ZoneHVAC</a> with heating and cooling. Cooling is delivered by
+a ventilation system with supply air temperature of <i>7</i>&deg;C.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end HeatingCoolingHVAC;
diff --git a/AixLib/ThermalZones/ISO13790/Examples/package.mo b/AixLib/ThermalZones/ISO13790/Examples/package.mo
new file mode 100644
index 0000000000..cc5a78f553
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Examples/package.mo
@@ -0,0 +1,11 @@
+within AixLib.ThermalZones.ISO13790;
+package Examples "Collection of models that illustrate model use and test models"
+extends Modelica.Icons.ExamplesPackage;
+
+annotation (
+  Documentation(info="<html>
+<p>
+This packages contains examples for reduced order model applications.
+</p>
+</html>"));
+end Examples;
diff --git a/AixLib/ThermalZones/ISO13790/Examples/package.order b/AixLib/ThermalZones/ISO13790/Examples/package.order
new file mode 100644
index 0000000000..468da5d514
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Examples/package.order
@@ -0,0 +1,4 @@
+FreeFloating
+FreeFloatingHVAC
+HeatingCooling
+HeatingCoolingHVAC
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case600.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case600.mo
new file mode 100644
index 0000000000..6cfe4d1c39
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case600.mo
@@ -0,0 +1,173 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST;
+model Case600 "Case 600FF, but with dual-setpoint for heating and cooling"
+  extends Modelica.Icons.Example;
+  Modelica.Blocks.Math.Sum sumHeaCoo(nin=2)
+    "Sum of heating and cooling heat flow rate"
+    annotation (
+    Placement(visible = true, transformation(extent={{54,56},{62,64}},      rotation = 0)));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow preHeaCoo
+    "Prescribed heat flow for heating and cooling"
+    annotation (Placement(visible=true, transformation(extent={{68,54},{80,66}},
+          rotation=0)));
+  Modelica.Blocks.Math.Gain gaiHea(k=1E6) "Gain for heating"
+    annotation (Placement(visible=true,
+        transformation(
+        origin={22,72},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  AixLib.Controls.Continuous.LimPID conHeaPID(
+    Ti=300,
+    k=0.1,
+    reverseActing=true,
+    strict=true) "Controller for heating"
+    annotation (Placement(visible=true, transformation(
+        origin={0,72},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Modelica.Blocks.Sources.Constant TSetHea(k=273.15 + 20) "Set-point for heating"
+    annotation (Placement(
+        visible=true, transformation(
+        origin={-24,72},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Modelica.Blocks.Sources.Constant TSetCoo(k=273.15 + 27) "Set-point for cooling"
+    annotation (Placement(
+        visible=true, transformation(
+        origin={-24,46},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Modelica.Blocks.Routing.Multiplex2 multiplex2
+    annotation (
+    Placement(visible = true, transformation(extent={{38,56},{46,64}},      rotation = 0)));
+  Modelica.Blocks.Math.Gain gaiCoo(k=-1E6) "Gain for cooling"
+    annotation (Placement(visible=true,
+        transformation(
+        origin={22,46},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  AixLib.Controls.Continuous.LimPID conCooPID(
+    Ti=300,
+    k=0.1,
+    reverseActing=false,
+    strict=true) "Controller for cooling"
+    annotation (Placement(visible=true, transformation(
+        origin={0,46},
+        extent={{-6,-6},{6,6}},
+        rotation=0)));
+  Modelica.Blocks.Continuous.Integrator ECoo(
+    k=1,
+    initType=Modelica.Blocks.Types.Init.InitialState,
+    y_start=0,
+    u(unit="W"),
+    y(unit="J")) "Cooling energy in Joules"
+    annotation (Placement(transformation(extent={{54,34},{66,46}})));
+  Modelica.Blocks.Continuous.Integrator EHea(
+    k=1,
+    initType=Modelica.Blocks.Types.Init.InitialState,
+    y_start=0,
+    u(unit="W"),
+    y(unit="J")) "Heating energy in Joules"
+    annotation (Placement(transformation(extent={{54,76},{66,88}})));
+  Modelica.Blocks.Sources.CombiTimeTable daiComBESTEST(table=[0,0,0,0,0,0,0,0;
+        259200,0,0,0,0,0,0,0; 262800,3250,3800,3930,4130,3930,3770,4230; 266400,
+        3410,3910,4040,4260,4040,3870,4350; 270000,3390,3870,4010,4230,4000,
+        3900,4320; 273600,3380,3920,4040,4220,4000,3890,4310; 277200,3420,3940,
+        4050,4220,4000,3920,4300; 280800,3430,3930,4040,4220,4000,3930,4310;
+        284400,3420,3940,4050,4220,4000,3930,4310; 288000,3340,3700,3860,4090,
+        3900,3750,4170; 291600,2770,2680,2560,2900,2710,2420,2910; 295200,1500,
+        1380,840,1280,1150,800,1470; 298800,150,0,0,0,0,-30,0; 302400,-770,-1230,
+        -1550,-1070,-1040,-1440,-420; 306000,-2660,-2490,-2850,-2590,-2500,-2720,
+        -2360; 309600,-3580,-2960,-3400,-3230,-3090,-3160,-2760; 313200,-3530,-2630,
+        -3120,-2830,-2640,-2840,-2430; 316800,-2440,-1350,-1820,-1550,-1350,-1720,
+        -1140; 320400,-360,0,0,0,0,0,0; 324000,240,950,780,800,880,770,1290;
+        327600,1530,2380,2230,2340,2330,2300,2450; 331200,2320,2870,2930,2990,
+        2950,2970,2940; 334800,2640,3210,3320,3370,3310,3280,3410; 338400,2900,
+        3280,3490,3530,3350,3460,3590; 342000,3020,3330,3510,3610,3490,3500,
+        3700; 345600,3010,3390,3560,3660,3530,3470,3770; 345600,0,0,0,0,0,0,0;
+        3153600,0,0,0,0,0,0,0]) "Daily comparison BESTEST"
+    annotation (Placement(transformation(extent={{60,-80},{80,-60}})));
+  Zone5R1C.Zone zon5R1C(
+    airRat=0.5,
+    AWin={0,0,12,0},
+    UWin=2.984,
+    AWal={21.6,16.2,9.6,16.2},
+    ARoo=48,
+    UWal=0.56,
+    URoo=0.33,
+    UFlo=1,
+    b=0,
+    AFlo=48,
+    VRoo=129.6,
+    hInt=2.74,
+    redeclare replaceable AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data.Case600Mass buiMas,
+    nOrientations=4,
+    surTil={1.5707963267949,1.5707963267949,1.5707963267949,1.5707963267949},
+    surAzi={3.1415926535898,-1.5707963267949,0,1.5707963267949},
+    gFac=0.789)
+    annotation (Placement(transformation(extent={{-14,-14},{14,14}})));
+  Modelica.Blocks.Sources.Constant intGai(k=200) "Internal heat gains"
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+  BoundaryConditions.WeatherData.ReaderTMY3 weaDat(filNam=
+    Modelica.Utilities.Files.loadResource(
+        "modelica://AixLib/Resources/weatherdata/DRYCOLD.mos"))
+    "Weather data"
+    annotation (Placement(transformation(extent={{-80,10},{-60,30}})));
+  AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data.Case600Results annComBESTEST "Annual comparison BESTEST "
+    annotation (Placement(transformation(extent={{20,-80},{40,-60}})));
+equation
+  connect(sumHeaCoo.y,preHeaCoo. Q_flow)
+    annotation (Line(points={{62.4,60},{68,60}}, color={0,0,127}));
+  connect(conHeaPID.y,gaiHea. u)
+    annotation (Line(points={{6.6,72},{14.8,72}}, color={0,0,127}));
+  connect(TSetHea.y,conHeaPID. u_s)
+    annotation (Line(points={{-17.4,72},{-7.2,72}},  color={0,0,127}));
+  connect(multiplex2.y,sumHeaCoo. u) annotation (
+    Line(points={{46.4,60},{53.2,60}},      color = {0, 0, 127}));
+  connect(conCooPID.u_s,TSetCoo. y)
+    annotation (Line(points={{-7.2,46},{-17.4,46}},  color={0,0,127}));
+  connect(conCooPID.y,gaiCoo. u)
+    annotation (Line(points={{6.6,46},{14.8,46}}, color={0,0,127}));
+  connect(gaiHea.y,multiplex2. u1[1]) annotation (Line(points={{28.6,72},{32,72},
+          {32,62},{38,62},{38,62.4},{37.2,62.4}},
+                            color={0,0,127}));
+  connect(gaiCoo.y,multiplex2. u2[1]) annotation (Line(points={{28.6,46},{32,46},
+          {32,58},{38,58},{38,57.6},{37.2,57.6}},
+                            color={0,0,127}));
+  connect(gaiCoo.u,conCooPID. y)
+    annotation (Line(points={{14.8,46},{6.6,46}}, color={0,0,127}));
+  connect(EHea.u, gaiHea.y) annotation (Line(points={{52.8,82},{44,82},{44,72},
+          {28.6,72}}, color={0,0,127}));
+  connect(ECoo.u, gaiCoo.y) annotation (Line(points={{52.8,40},{44,40},{44,46},
+          {28.6,46}}, color={0,0,127}));
+
+  connect(preHeaCoo.port, zon5R1C.heaPorAir) annotation (Line(points={{80,60},{
+          90,60},{90,4},{4,4},{4,8}}, color={191,0,0}));
+  connect(intGai.y, zon5R1C.intSenGai) annotation (Line(points={{-59,-10},{-24,
+          -10},{-24,10},{-16,10}},   color={0,0,127}));
+  connect(weaDat.weaBus, zon5R1C.weaBus) annotation (Line(
+      points={{-60,20},{10,20},{10,11}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(zon5R1C.TAir, conCooPID.u_m) annotation (Line(points={{15,8},{20,8},{
+          20,30},{0,30},{0,38.8}}, color={0,0,127}));
+  connect(zon5R1C.TAir, conHeaPID.u_m) annotation (Line(points={{15,8},{20,8},{
+          20,30},{-40,30},{-40,60},{0,60},{0,64.8}}, color={0,0,127}));
+ annotation(experiment(
+      StopTime=31536000,
+      Tolerance=1e-06),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case600.mos"
+        "Simulate and plot"), Documentation(info="<html>
+<p>
+This model is used for the basic test case 600 of the BESTEST validation suite. 
+Case 600 is a light-weight building with room temperature control set to <i>20</i>&deg;C 
+for heating and <i>27</i>&deg;C for cooling. The room has no shade and a window that faces south. 
+</p>
+</html>", revisions="<html><ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul></html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Case600;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case600FF.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case600FF.mo
new file mode 100644
index 0000000000..0b7fa18ecc
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case600FF.mo
@@ -0,0 +1,82 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST;
+model Case600FF "Basic test with light-weight construction and free floating temperature"
+  extends Modelica.Icons.Example;
+  Zone5R1C.Zone zon5R1C(
+    airRat=0.5,
+    AWin={0,0,12,0},
+    UWin=2.984,
+    AWal={21.6,16.2,9.6,16.2},
+    ARoo=48,
+    UWal=0.56,
+    URoo=0.33,
+    UFlo=1,
+    b=0,
+    AFlo=48,
+    VRoo=129.6,
+    hInt=2.74,
+    redeclare replaceable AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data.Case600Mass buiMas,
+    nOrientations=4,
+    surTil={1.5707963267949,1.5707963267949,1.5707963267949,1.5707963267949},
+    surAzi={3.1415926535898,-1.5707963267949,0,1.5707963267949},
+    gFac=0.789) "Thermal zone"
+    annotation (Placement(transformation(extent={{-14,-14},{14,14}})));
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
+    filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/DRYCOLD.mos"))
+    "Weather data"
+    annotation (Placement(transformation(extent={{-80,10},{-60,30}})));
+  Modelica.Blocks.Sources.Constant intGai(k=200) "Internal heat gains"
+    annotation (Placement(transformation(extent={{-80,-20},{-60,0}})));
+  Modelica.Blocks.Math.ContinuousMean conMea
+    "Continuous mean of room air temperature"
+    annotation (Placement(transformation(extent={{60,-2},{80,18}})));
+  Modelica.Blocks.Sources.CombiTimeTable daiComBESTESTFF(table=[0,0,0,0,0,0,0,0;
+        259200,0,0,0,0,0,0,0; 262800,-8.88,-12.04,-12.3,-12.21,-12.1,-12.02,-13.04;
+        266400,-10.48,-13.52,-14.1,-13.8,-13.7,-13.5,-14.59; 270000,-11.76,-14.4,
+        -15.4,-14.9,-14.7,-14.7,-15.65; 273600,-12.75,-15.26,-16.3,-15.79,-15.6,
+        -15.65,-16.46; 277200,-13.69,-16,-17.1,-16.55,-16.4,-16.47,-17.16;
+        280800,-14.49,-16.4,-17.9,-17.2,-17,-17.14,-17.79; 284400,-15.15,-17.01,
+        -18.5,-17.74,-17.6,-17.7,-18.32; 288000,-15.63,-17.05,-18.8,-17.85,-17.8,
+        -17.59,-18.47; 291600,-14.63,-13.74,-14.7,-14.88,-14.6,-13.46,-15.47;
+        295200,-10.03,-7.99,-7.8,-9.07,-8.9,-7.1,-9.56; 298800,-2.2,2.6,3.2,
+        1.01,1,3.66,0.49; 302400,8.84,12.22,13.4,11.21,10.7,13.49,10.39; 306000,
+        18.96,20.86,22.3,20.03,19.2,21.77,18.75; 309600,27.19,27.53,29.5,27.27,
+        26.1,28.26,25.48; 313200,33.22,31.33,33.8,31.34,29.8,32.09,29.21;
+        316800,35.51,31.06,33.5,31.47,29.7,32.16,28.97; 320400,31.46,24.28,27,
+        25.96,23.9,25.71,22.58; 324000,23.99,17.46,19.7,18.96,17.6,18.84,15.59;
+        327600,18.08,12.05,13.7,13.04,12.2,13.1,10.2; 331200,13.02,7.57,8.7,
+        8.31,7.8,8.41,6.02; 334800,8.87,3.6,4.4,4.27,4,4.39,2.39; 338400,5.12,
+        0.52,1,0.99,0.9,0.97,-0.59; 342000,2.03,-1.94,-1.9,-1.66,-1.7,-1.78,-3.04;
+        345600,-1.03,-4.07,-4.4,-3.92,-3.9,-4.03,-5.14; 345600,0,0,0,0,0,0,0;
+        3153600,0,0,0,0,0,0,0]) "Daily comparison BESTEST FF"
+    annotation (Placement(transformation(extent={{60,-80},{80,-60}})));
+  AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data.Case600FFResults annComBESTESTFF "Annual comparison BESTEST FF"
+    annotation (Placement(transformation(extent={{20,-80},{40,-60}})));
+equation
+  connect(weaDat.weaBus, zon5R1C.weaBus) annotation (Line(
+      points={{-60,20},{10,20},{10,11}},
+      color={255,204,51},
+      thickness=0.5));
+
+  connect(intGai.y, zon5R1C.intSenGai) annotation (Line(points={{-59,-10},{-30,
+          -10},{-30,10},{-16,10}},   color={0,0,127}));
+  connect(zon5R1C.TAir, conMea.u)
+    annotation (Line(points={{15,8},{58,8}}, color={0,0,127}));
+ annotation(experiment(
+      StopTime=31536000,
+      Tolerance=1e-06),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case600FF.mos"
+        "Simulate and plot"), Documentation(info="<html>
+<p>
+This model is used for the test case 600FF of the BESTEST validation suite.
+Case 600FF is a light-weight building.
+The room temperature is free floating.
+</p>
+</html>", revisions="<html><ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul></html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Case600FF;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case900.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case900.mo
new file mode 100644
index 0000000000..696371f230
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case900.mo
@@ -0,0 +1,54 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST;
+model Case900
+  extends AixLib.ThermalZones.ISO13790.Validation.BESTEST.Case600(
+    zon5R1C(hInt=2.74,
+      redeclare replaceable AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data.Case900Mass buiMas),
+    annComBESTEST(
+      EHeaMax=  7.3476E+09,
+      EHeaMin=  4.2120E+09,
+      ECooMax=-11.3940E+09,
+      ECooMin= -7.6860E+09,
+      PHeaMax=3797,
+      PHeaMin=2850,
+      PCooMax=-3871,
+      PCooMin=-2888),
+    daiComBESTEST(table=[0,0,0,0,0,0,0,0; 259200,0,0,0,0,0,0,0; 262800,2440,3100,
+          3100,3390,3210,3080,3400; 266400,2610,3200,3240,3540,3350,3200,3550; 270000,
+          2620,3200,3280,3560,3380,3280,3570; 273600,2670,3310,3380,3610,3450,3330,
+          3630; 277200,2740,3370,3450,3670,3510,3420,3690; 280800,2800,3400,3500,
+          3720,3560,3470,3750; 284400,2830,3450,3560,3760,3610,3520,3800; 288000,
+          2840,3380,3520,3750,3610,3460,3790; 291600,2640,2900,2970,3170,3080,2830,
+          3170; 295200,2120,2350,2200,2320,2350,2060,2450; 298800,1500,1400,1030,
+          950,1120,790,1290; 302400,680,380,230,100,300,40,620; 306000,70,0,0,0,
+          0,0,140; 309600,0,0,0,0,0,0,0; 313200,0,0,0,0,0,0,0; 316800,0,0,0,0,0,
+          0,90; 320400,30,120,0,280,140,130,1200; 324000,410,770,740,1220,910,760,
+          1600; 327600,800,1310,1140,1610,1280,1200,1810; 331200,1070,1610,1430,
+          1820,1540,1460,1940; 334800,1270,1930,1700,2040,1810,1700,2120; 338400,
+          1500,2140,1890,2170,2000,1930,2230; 342000,1660,2220,2030,2290,2150,2090,
+          2340; 345600,1750,2310,2190,2420,2310,2230,2460; 345600,0,0,0,0,0,0,0;
+          3153600,0,0,0,0,0,0,0]));
+
+ annotation(experiment(
+      StopTime=31536000,
+      Tolerance=1e-06),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case900.mos"
+        "Simulate and plot"), Documentation(info="<html>
+<p>
+This model is used for the basic test case 900 of the BESTEST validation suite.
+Case 900 is a heavy-weight building with room temperature control set to <i>20</i>&deg;C
+for heating and <i>27</i>&deg;C for cooling. The room has no shade and a window that faces south.
+</p>
+</html>", revisions="<html><ul>
+<li>
+May 8, 2024, by Michael Wetter:<br/>
+Changed number format to avoid a warning in Optimica about number to be too large
+to be represented as an Integer.
+</li>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul></html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Case900;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case900FF.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case900FF.mo
new file mode 100644
index 0000000000..b31031ba7f
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Case900FF.mo
@@ -0,0 +1,40 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST;
+model Case900FF "Test with heavy-weight construction and free floating temperature"
+  extends AixLib.ThermalZones.ISO13790.Validation.BESTEST.Case600FF(
+    zon5R1C(
+      redeclare replaceable AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data.Case900Mass buiMas),
+    daiComBESTESTFF(table=[0,0,0,0,0,0,0,0; 259200,0,0,0,0,0,0,0; 262800,1.61,-0.17,
+          -0.9,-1.31,-0.7,-3.46,-2.68; 266400,0.93,-0.79,-1.6,-1.97,-1.4,-3.99,-3.33;
+          270000,0.49,-1.09,-2,-2.37,-1.8,-4.4,-3.72; 273600,0.07,-1.67,-2.5,-2.81,
+          -2.3,-4.8,-4.1; 277200,-0.41,-2.04,-2.9,-3.25,-2.7,-5.22,-4.51; 280800,
+          -0.87,-2.43,-3.4,-3.68,-3.2,-5.6,-4.93; 284400,-1.27,-2.97,-3.9,-4.1,-3.6,
+          -5.98,-5.34; 288000,-1.64,-3.15,-4.3,-4.4,-4,-6.08,-5.64; 291600,-1.54,
+          -2.39,-3.3,-3.45,-3.2,-4.72,-4.59; 295200,-0.4,-1.09,-1.6,-1.6,-1.7,-2.98,
+          -2.64; 298800,1.59,1.6,1.2,1.66,0.9,0.25,0.75; 302400,4.4,3.62,3.5,4.4,
+          3.1,2.54,3.26; 306000,6.72,5.62,5.5,6.56,5.1,4.38,4.99; 309600,8.66,7.32,
+          7.2,8.39,6.8,5.85,6.51; 313200,10.02,8.27,8,9.04,7.6,6.61,7.11; 316800,
+          10.4,8.15,7.9,8.58,7.4,6.33,6.68; 320400,9.41,6.53,6.2,6.44,5.8,4.2,4.24;
+          324000,7.66,5.25,4.7,4.43,4.4,2.87,2.45; 327600,6.74,4.52,3.8,3.37,3.6,
+          2.11,1.71; 331200,6,3.88,3.2,2.73,3,1.58,1.32; 334800,5.41,3.22,2.7,2.11,
+          2.4,1.05,0.82; 338400,4.74,2.85,2.2,1.66,1.9,0.55,0.42; 342000,4.2,2.47,
+          1.7,1.26,1.5,0.15,0.05; 345600,3.66,1.9,1.2,0.83,1,-0.24,-0.34; 345600,
+          0,0,0,0,0,0,0; 3153600,0,0,0,0,0,0,0]),
+    annComBESTESTFF(TavgMin=297.65));
+
+ annotation(experiment(Tolerance=1e-6, StopTime=3.1536e+007),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ISO13790/Validation/BESTEST/Case900FF.mos"
+        "Simulate and plot"), Documentation(info="<html>
+<p>
+This model is used for the test case 900FF of the BESTEST validation suite.
+Case 900FF is a heavy-weight building.
+The room temperature is free floating.
+</p>
+</html>", revisions="<html><ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul></html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Case900FF;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600FFResults.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600FFResults.mo
new file mode 100644
index 0000000000..9a06569543
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600FFResults.mo
@@ -0,0 +1,14 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data;
+record Case600FFResults "BESTEST comparison results free-floating"
+  extends Modelica.Icons.Record;
+  parameter Modelica.Units.SI.Temperature TavgMax=299.05 "Maximum average annual air temperature";
+  parameter Modelica.Units.SI.Temperature TavgMin=297.35 "Minimum average annual air temperature";
+  annotation (defaultComponentName="annComBESTESTFF",Icon(coordinateSystem(preserveAspectRatio=false)),
+  Diagram(coordinateSystem(preserveAspectRatio=false)),
+  Documentation(info="<html>
+<p>
+BESTEST results for annual heating and cooling loads in free-floating mode.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Case600FFResults;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600Mass.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600Mass.mo
new file mode 100644
index 0000000000..d95694ffea
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600Mass.mo
@@ -0,0 +1,19 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data;
+record Case600Mass = AixLib.ThermalZones.ISO13790.Data.Generic(
+    heaC=51289.8,
+    facMas=4.522) "BESTEST600"
+     annotation (
+  Documentation(revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>",
+info="<html>
+<p>
+Thermal mass for Case600Mass.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600Results.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600Results.mo
new file mode 100644
index 0000000000..13416a190c
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case600Results.mo
@@ -0,0 +1,31 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data;
+record Case600Results "BESTEST comparison results"
+  extends Modelica.Icons.Record;
+  parameter Modelica.Units.SI.Energy EHeaMax= 20.5524E+09 "Maximum annual heating load";
+  parameter Modelica.Units.SI.Energy EHeaMin= 15.4656E+09 "Minimum annaul heating load";
+  parameter Modelica.Units.SI.Energy ECooMax=-26.2008E+09 "Maximum annual cooling load";
+  parameter Modelica.Units.SI.Energy ECooMin=-22.0932E+09 "Minimum annual cooling load";
+  parameter Modelica.Units.SI.Power PHeaMax=4354 "Maximum peak heating load";
+  parameter Modelica.Units.SI.Power PHeaMin=3437 "Minimum peak heating load";
+  parameter Modelica.Units.SI.Power PCooMax=-6827 "Maximum peak cooling load";
+  parameter Modelica.Units.SI.Power PCooMin=-5965 "Minimum peak cooling load";
+
+  annotation (defaultComponentName="annComBESTEST",Icon(coordinateSystem(preserveAspectRatio=false)),
+  Diagram(coordinateSystem(preserveAspectRatio=false)),
+  Documentation(info="<html>
+<p>
+BESTEST results for annual heating and cooling loads.
+</p>
+</html>",
+revisions="
+<html>
+<ul>
+<li>
+May 8, 2024, by Michael Wetter:<br/>
+Changed number format to avoid a warning in Optimica about number to be too large
+to be represented as an Integer.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Case600Results;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case900Mass.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case900Mass.mo
new file mode 100644
index 0000000000..e724c54e93
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/Case900Mass.mo
@@ -0,0 +1,11 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST.Data;
+record Case900Mass = AixLib.ThermalZones.ISO13790.Data.Generic(
+    heaC=249272,
+    facMas=2.7) "BESTEST900"
+     annotation (
+  Documentation(info="<html>
+<p>
+Thermal mass for Case900Mass.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/package.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/package.mo
new file mode 100644
index 0000000000..90f5e888be
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/package.mo
@@ -0,0 +1,9 @@
+within AixLib.ThermalZones.ISO13790.Validation.BESTEST;
+package Data "Data records for BESTEST validation"
+  extends Modelica.Icons.MaterialPropertiesPackage;
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains data records for the BESTEST validation.
+</p>
+</html>"));
+end Data;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/package.order b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/package.order
new file mode 100644
index 0000000000..b8c15c83e3
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/Data/package.order
@@ -0,0 +1,4 @@
+Case600FFResults
+Case600Mass
+Case600Results
+Case900Mass
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/package.mo b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/package.mo
new file mode 100644
index 0000000000..1fa8ed6984
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/package.mo
@@ -0,0 +1,21 @@
+within AixLib.ThermalZones.ISO13790.Validation;
+package BESTEST "Package with models for the BESTEST validation"
+extends Modelica.Icons.ExamplesPackage;
+
+  annotation (
+  Documentation(info="<html>
+<p>
+This package contains the models that were used for the BESTEST validation (ANSI/ASHRAE 2007).
+</p>
+<h4>References</h4>
+<p>
+Maccarini A, Prataviera E, Zarrella A, Afshari A. 2021. 
+<i>
+<a href=\"https://iopscience.iop.org/article/10.1088/1742-6596/2042/1/012078\">
+Development of a Modelica-based simplified building model for district energy simulations
+</a>
+</i>.
+In: Journal of Physics: Conference Series. 2042, 1, 012078.
+</p>
+</html>"));
+end BESTEST;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/BESTEST/package.order b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/package.order
new file mode 100644
index 0000000000..4b986698a8
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/BESTEST/package.order
@@ -0,0 +1,5 @@
+Case600
+Case600FF
+Case900
+Case900FF
+Data
diff --git a/AixLib/ThermalZones/ISO13790/Validation/package.mo b/AixLib/ThermalZones/ISO13790/Validation/package.mo
new file mode 100644
index 0000000000..e3eb2feee3
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/package.mo
@@ -0,0 +1,12 @@
+within AixLib.ThermalZones.ISO13790;
+package Validation "Collection of validation models"
+extends Modelica.Icons.ExamplesPackage;
+
+  annotation (
+  Documentation(info="<html>
+<p>
+This packages contains validation models of <a href=\"modelica://AixLib.ThermalZones.ISO13790.Zone5R1C.Zone\">
+AixLib.ThermalZones.ISO13790.Zone5R1C.Zone</a>.
+</p>
+</html>"));
+end Validation;
diff --git a/AixLib/ThermalZones/ISO13790/Validation/package.order b/AixLib/ThermalZones/ISO13790/Validation/package.order
new file mode 100644
index 0000000000..56fcff9fe3
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Validation/package.order
@@ -0,0 +1 @@
+BESTEST
diff --git a/AixLib/ThermalZones/ISO13790/Zone5R1C/Zone.mo b/AixLib/ThermalZones/ISO13790/Zone5R1C/Zone.mo
new file mode 100644
index 0000000000..4e3f92b5c9
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Zone5R1C/Zone.mo
@@ -0,0 +1,394 @@
+within AixLib.ThermalZones.ISO13790.Zone5R1C;
+model Zone "Thermal zone based on 5R1C network"
+  parameter Real airRat(unit="1/h") "Air change rate"
+   annotation (Dialog(group="Ventilation"));
+  parameter Modelica.Units.SI.Area AWin[nOrientations] "Area of windows"
+   annotation (Dialog(group="Windows"));
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer UWin "U-value of windows"
+   annotation (Dialog(group="Windows"));
+  parameter Modelica.Units.SI.Area AWal[nOrientations] "Area of external walls (only opaque part)"
+   annotation (Dialog(group="Opaque constructions"));
+  parameter Modelica.Units.SI.Area ARoo "Area of roof"
+   annotation (Dialog(group="Opaque constructions"));
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer UWal "U-value of external walls"
+   annotation (Dialog(group="Opaque constructions"));
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer URoo "U-value of roof"
+   annotation (Dialog(group="Opaque constructions"));
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer UFlo "U-value of floor"
+   annotation (Dialog(group="Opaque constructions"));
+  parameter Real b=0.5 "Adjustment factor for ground heat transfer"
+   annotation (Dialog(group="Opaque constructions"));
+  parameter Modelica.Units.SI.Area AFlo "Net conditioned floor area";
+  parameter Modelica.Units.SI.Volume VRoo "Volume of room";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hInt=3.45
+    "Heat transfer coefficient between surface and air nodes";
+  replaceable parameter ISO13790.Data.Generic buiMas "Building mass"
+   annotation (
+     choicesAllMatching=true,
+     Placement(transformation(extent={{-100,-130},{-80,-110}})));
+  parameter Integer nOrientations(min=1) = 4 "Number of orientations for vertical walls";
+  parameter Modelica.Units.SI.Angle surTil[nOrientations] "Tilt angle of surfaces";
+  parameter Modelica.Units.SI.Angle surAzi[nOrientations] "Azimuth angle of surfaces";
+  parameter Real winFra(min=0, max=1)=0.001 "Frame fraction of windows"
+   annotation(Dialog(group="Windows"));
+  parameter Real gFac(min=0, max=1) "Energy transmittance of glazings"
+   annotation(Dialog(group="Windows"));
+
+  Modelica.Blocks.Interfaces.RealInput intSenGai(final unit="W") "Internal sensible heat gains"
+    annotation (Placement(transformation(extent={{-180,80},{-140,120}}),
+        iconTransformation(extent={{-180,80},{-140,120}})));
+
+  Modelica.Blocks.Interfaces.RealOutput TAir(
+    final unit="K",
+    displayUnit="degC")
+    "Room air temperature"
+    annotation (Placement(
+        transformation(extent={{140,70},{160,90}}),
+        iconTransformation(extent={{
+            140,70},{160,90}})));
+  Modelica.Blocks.Interfaces.RealOutput TSur(
+    final unit="K",
+    displayUnit="degC")
+    "Average inside surface temperature" annotation (Placement(
+        transformation(extent={{140,50},{160,70}}),
+        iconTransformation(extent={{
+            140,-10},{160,10}})));
+
+  AixLib.BoundaryConditions.WeatherData.Bus weaBus
+    "Weather data bus"
+    annotation (Placement(
+        transformation(extent={{100,100},{140,140}}),
+        iconTransformation(extent={{68,78},{132,142}})));
+
+  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a heaPorAir
+    "Heat port to air node"
+    annotation (Placement(transformation(extent={{30,70},{50,90}})));
+  Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a heaPorSur
+    "Heat port to surface temperatures"
+    annotation (Placement(transformation(extent={{30,-10},{50,10}})));
+
+  Modelica.Thermal.HeatTransfer.Components.ThermalConductor HVen(
+      G=airRat*VRoo*1005*1.2/3600) "Heat transfer due to ventilation"
+   annotation (Placement(transformation(extent={{0,70},{20,90}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalConductor HTra(
+      G=1/(1/(UWal*sum(AWal) + b*UFlo*AFlo + URoo*ARoo) - 1/(hSur*buiMas.facMas*AFlo)))
+      "Heat transfer through opaque elements"
+   annotation (Placement(transformation(extent={{0,-90},{20,-70}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalConductor HWin(
+      G=UWin*sum(AWin)) "Heat transfer through glazed elements"
+   annotation (Placement(transformation(extent={{0,-10},{20,10}})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalConductor HThe(G=hInt*AFlo*ratSur)
+    "Coupling conductance betwee air and surface nodes"
+   annotation (Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={40,40})));
+  Modelica.Thermal.HeatTransfer.Components.ThermalConductor HMas(G=hSur*buiMas.facMas*AFlo)
+    "Coupling conductance between surface and mass nodes"
+   annotation (
+      Placement(transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={40,-40})));
+  Modelica.Thermal.HeatTransfer.Components.HeatCapacitor capMas(
+      C=buiMas.heaC*AFlo,
+      T(displayUnit="degC",
+      fixed=true,
+      start=293.15)) "Zone thermal capacity" annotation (Placement(
+        transformation(
+        extent={{-10,-10},{10,10}},
+        rotation=180,
+        origin={40,-100})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature TExt
+    "External air temperature"
+    annotation (Placement(transformation(extent={{-100,-10},{-80,10}})));
+  Modelica.Blocks.Math.Add solGai "Total solar heat gains"
+    annotation (Placement(transformation(extent={{-60,-80},{-40,-60}})));
+  BaseClasses.GlazedElements win(
+    final n=nOrientations,
+    final AWin=AWin,
+    final surTil=surTil,
+    final surAzi=surAzi,
+    final gFac=gFac,
+    final winFra=winFra) "Solar heat gains of glazed elements"
+    annotation (Placement(transformation(extent={{-100,-60},{-80,-40}})));
+  BaseClasses.OpaqueElements opa(
+    final n=nOrientations,
+    final AWal=AWal,
+    final ARoo=ARoo,
+    final UWal=UWal,
+    final URoo=URoo,
+    final surTil=surTil,
+    final surAzi=surAzi) "Solar heat gains of opaque elements"
+    annotation (Placement(transformation(extent={{-100,-100},{-80,-80}})));
+  BaseClasses.GainSurface phiSur(
+    ATot=AFlo*ratSur,
+    facMas=buiMas.facMas,
+    AFlo=AFlo,
+    HWinGai=HWin.G) "Heat flow injected to surface node"
+    annotation (Placement(transformation(extent={{120,-10},{100,10}})));
+  Modelica.Blocks.Math.Gain phiAir(k=0.5) "Heat flow injected to air node"
+    annotation (Placement(transformation(extent={{120,70},{100,90}})));
+  BaseClasses.GainMass phiMas(
+    ATot=AFlo*ratSur,
+    facMas=buiMas.facMas,
+    AFlo=AFlo) "Heat flow injected to mass node"
+    annotation (Placement(transformation(extent={{120,-90},{100,-70}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedTemperature TVen "Supply air temperature"
+    annotation (Placement(transformation(extent={{-100,70},{-80,90}})));
+
+protected
+  parameter Real ratSur=4.5 "Ratio between the internal surfaces area and the floor area";
+  parameter Modelica.Units.SI.CoefficientOfHeatTransfer hSur=9.1 "Heat transfer coefficient between mass and surface nodes";
+
+  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor senTAir
+    "Air temperature sensor"
+    annotation (Placement(transformation(extent={{70,50},{90,70}})));
+  Modelica.Thermal.HeatTransfer.Sensors.TemperatureSensor senTSur
+    "Surface temperature sensor"
+    annotation (Placement(transformation(extent={{70,20},{90,40}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow heaAir
+    annotation (Placement(transformation(extent={{80,70},{60,90}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow heaSur
+    annotation (Placement(transformation(extent={{80,-10},{60,10}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow heaMas
+    annotation (Placement(transformation(extent={{80,-90},{60,-70}})));
+initial equation
+  assert(size(AWin,1) == nOrientations, "The parameter AWin must have the same dimension of nOrientations.");
+  assert(size(AWal,1) == nOrientations, "The parameter AWal must have the same dimension of nOrientations.");
+  assert(size(surTil,1) == nOrientations, "The parameter surTil must have the same dimension of nOrientations.");
+  assert(size(surAzi,1) == nOrientations, "The parameter surAzi must have the same dimension of nOrientations.");
+
+equation
+
+  connect(heaPorSur, HWin.port_b)
+    annotation (Line(points={{40,0},{20,0}}, color={191,0,0}));
+  connect(heaPorAir, HVen.port_b)
+    annotation (Line(points={{40,80},{20,80}}, color={191,0,0}));
+  connect(heaPorAir, HThe.port_b)
+    annotation (Line(points={{40,80},{40,50}}, color={191,0,0}));
+  connect(heaPorAir, heaAir.port)
+    annotation (Line(points={{40,80},{60,80}}, color={191,0,0}));
+  connect(heaSur.port, heaPorSur)
+    annotation (Line(points={{60,0},{40,0}}, color={191,0,0}));
+  connect(heaPorSur, HMas.port_b)
+    annotation (Line(points={{40,0},{40,-30}}, color={191,0,0}));
+  connect(weaBus.TDryBul,TExt. T) annotation (Line(
+      points={{120,120},{-112,120},{-112,0},{-102,0}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(heaPorSur, HThe.port_a)
+    annotation (Line(points={{40,0},{40,30}}, color={191,0,0}));
+  connect(win.weaBus, weaBus) annotation (Line(
+      points={{-100,-50},{-112,-50},{-112,120},{120,120}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(opa.weaBus, weaBus) annotation (Line(
+      points={{-100,-90},{-112,-90},{-112,120},{120,120}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%second",
+      index=1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(HWin.port_a,TExt. port)
+    annotation (Line(points={{0,0},{-80,0}}, color={191,0,0}));
+  connect(HTra.port_a, TExt.port) annotation (Line(points={{0,-80},{-20,-80},{-20,
+          0},{-80,0}}, color={191,0,0}));
+  connect(heaMas.port, HTra.port_b)
+    annotation (Line(points={{60,-80},{20,-80}}, color={191,0,0}));
+  connect(capMas.port, HTra.port_b)
+    annotation (Line(points={{40,-90},{40,-80},{20,-80}},  color={191,0,0}));
+  connect(HMas.port_a, HTra.port_b)
+    annotation (Line(points={{40,-50},{40,-80},{20,-80}}, color={191,0,0}));
+  connect(TVen.port, HVen.port_a)
+    annotation (Line(points={{-80,80},{0,80}}, color={191,0,0}));
+  connect(weaBus.TDryBul,TVen. T) annotation (Line(
+      points={{120,120},{-112,120},{-112,80},{-102,80}},
+      color={255,204,51},
+      thickness=0.5), Text(
+      string="%first",
+      index=-1,
+      extent={{-6,3},{-6,3}},
+      horizontalAlignment=TextAlignment.Right));
+  connect(solGai.y, phiMas.solGai) annotation (Line(points={{-39,-70},{-30,-70},
+          {-30,-120},{134,-120},{134,-88},{122,-88}}, color={0,0,127}));
+  connect(phiSur.solGai, solGai.y) annotation (Line(points={{122,-8},{134,-8},{134,
+          -120},{-30,-120},{-30,-70},{-39,-70}}, color={0,0,127}));
+  connect(intSenGai, phiMas.intSenGai) annotation (Line(points={{-160,100},{130,
+          100},{130,-84},{122,-84}},                        color={0,0,127}));
+  connect(phiSur.intSenGai, intSenGai) annotation (Line(points={{122,-4},{130,-4},
+          {130,100},{-160,100}},                         color={0,0,127}));
+  connect(phiAir.u, intSenGai) annotation (Line(points={{122,80},{130,80},{130,100},
+          {-160,100}},                        color={0,0,127}));
+  connect(phiMas.masGai, heaMas.Q_flow)
+    annotation (Line(points={{99,-80},{80,-80}}, color={0,0,127}));
+  connect(phiAir.y, heaAir.Q_flow)
+    annotation (Line(points={{99,80},{80,80}}, color={0,0,127}));
+  connect(phiSur.surGai, heaSur.Q_flow)
+    annotation (Line(points={{99,0},{80,0}}, color={0,0,127}));
+  connect(win.solRadWin, solGai.u1) annotation (Line(points={{-79,-50},{-70,-50},
+          {-70,-64},{-62,-64}}, color={0,0,127}));
+  connect(opa.y, solGai.u2) annotation (Line(points={{-79,-90},{-70,-90},{-70,-76},
+          {-62,-76}}, color={0,0,127}));
+  connect(senTSur.port, heaPorSur)
+    annotation (Line(points={{70,30},{52,30},{52,0},{40,0}}, color={191,0,0}));
+  connect(senTAir.port, heaPorAir)
+    annotation (Line(points={{70,60},{40,60},{40,80}}, color={191,0,0}));
+  connect(senTAir.T, TAir) annotation (Line(points={{91,60},{134,60},{134,80},{150,
+          80}}, color={0,0,127}));
+  connect(senTSur.T, TSur) annotation (Line(points={{91,30},{136,30},{136,60},{150,
+          60}}, color={0,0,127}));
+  annotation (defaultComponentName="zon", Icon(
+    coordinateSystem(preserveAspectRatio=false, extent={{-140,
+            -140},{140,140}}), graphics={Rectangle(
+          extent={{-140,140},{140,-140}},
+          lineThickness=1,
+          pattern=LinePattern.None,
+          lineColor={0,0,0},
+          fillColor={95,95,95},
+          fillPattern=FillPattern.Solid),
+        Rectangle(
+          extent={{-120,122},{118,-122}},
+          lineColor={117,148,176},
+          fillPattern=FillPattern.Solid,
+          fillColor=DynamicSelect({170,213,255},
+            min(1, max(0, (1-(heaPorAir.T-295.15)/10)))*{28,108,200}+
+            min(1, max(0, (heaPorAir.T-295.15)/10))*{255,0,0})),
+        Text(
+          extent={{-104,174},{118,142}},
+          textColor={0,0,255},
+          textString="%name"),
+        Text(
+          extent={{60,-82},{118,-126}},
+          textColor={0,0,0},
+          textString="ISO"),
+        Text(
+          extent={{-180,156},{-116,110}},
+          textColor={0,0,88},
+          textString="intSenGai"),
+        Text(
+          extent={{88,94},{136,62}},
+          textColor={0,0,88},
+          textString="TAir"),
+        Text(
+          extent={{82,18},{130,-14}},
+          textColor={0,0,88},
+          textString="TSur"),
+        Text(
+          extent={{48,108},{-72,58}},
+          textColor={255,255,255},
+          textString=DynamicSelect("", String(heaPorAir.T-273.15, format=".1f")))}),
+    Diagram(coordinateSystem(preserveAspectRatio=
+            false, extent={{-140,-140},{140,140}})),
+    Documentation(info="<html>
+<p>
+This is a lumped-capacity simplified building model based  on the 5R1C
+network presented in the ISO 13790:2008 Standard. The simplified 5R1C model uses
+five thermal resistances and one thermal capacity to reproduce the
+transient thermal behaviour of buildings. The thermal zone is modeled with three
+temperature nodes, the indoor air temperature <code>TAir</code>, the envelope internal
+surface temperature <code>TSur</code> and the zone's mass temperature <code>TMas</code>
+(the heat port is not shown in the figure), and two boundary
+condition nodes, supply air temperature <code>TSup</code> and the external air temperature
+<code>TExt</code>. The five resistances are related to heat transfer by ventilation <code>HVen</code>,
+windows <code>HWin</code>, opaque components (split between <code>HTra</code> and <code>HMas</code>) and heat
+transfer between the internal surfaces of walls and the air temperature <code>HThe</code>.
+The thermal capacity <code>Cm</code> includes the thermal capacity of the entire zone. The heating and/or
+cooling demand is found by calculating the heating and/or cooling power &Phi;HC that
+needs to be supplied to, or extracted from, the internal air node to maintain a
+certain set-point. Internal, &Phi;int , and solar, &Phi;sol, heat gains are input values,
+which are split in three components.
+</p>
+<br>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/ThermalZones/ISO13790/Zone/5R1CNetwork.png\" alt=\"image\"/>
+</p>
+<br>
+The ventilation heat transfer coefficient <i>H<sub>ven</sub></i> is calculated using
+<p align=\"center\" style=\"font-style:italic;\">
+H<sub>ven</sub> = &rho;<sub>a</sub> c<sub>a</sub> &sum;<sub>k</sub>V&#775;<sub>k</sub>,
+</p>
+where <i>&rho;<sub>a</sub></i> is the density of air, <i>c<sub>a</sub></i> is the specific
+heat capacity of air and <i>V&#775;<sub>k</sub></i> is the k-th volumetric external air
+flow rate.
+The coupling conductance <i>H<sub>the</sub></i> is given by
+<p align=\"center\" style=\"font-style:italic;\">
+H<sub>the</sub> = h<sub>as</sub> A<sub>tot</sub>,
+</p>
+where <i>h<sub>as</sub></i> is the heat transfer coefficient between the air
+node the surface node, with a fixed value of <i>3.45 W/m<sup>2</sup>K</i>, and
+<i>A<sub>tot</sub></i> is the area of all surfaces facing the building zone.
+The thermal transmission coefficient of windows <i>H<sub>win</sub></i> is calculated using
+<p align=\"center\" style=\"font-style:italic;\">
+H<sub>win</sub> =
+&sum;<sub>k</sub>U<sub>win,k</sub>A<sub>win,k</sub>,
+</p>
+where <i>U<sub>win,k</sub></i> is the thermal transmittance of window element
+k of the building envelope and <i>A<sub>k</sub></i>  is the area of the window
+element k of the building envelope. The coupling conductance <i>H<sub>mas</sub></i> is given by
+<p align=\"center\" style=\"font-style:italic;\">
+H<sub>mas</sub> =h<sub>ms</sub> f<sub>ms</sub> A<sub>f</sub>,
+</p>
+where <i>h<sub>ms</sub></i> is the heat transfer coefficient between the mass
+node and the surface node, with fixed value of <i>9.1 W/m<sup>2</sup>K</i>,
+<i>f<sub>ms</sub></i> is a correction factor, and <i>A<sub>f</sub></i>
+is the floor area. The correction factor <i>f<sub>ms</sub></i> can be assumed as
+<i>2.5</i> for light and medium building constructions, and <i>3</i> for heavy constructions.
+The coupling conductance <i>H<sub>tra</sub></i> is calculated using
+<p align=\"center\" style=\"font-style:italic;\">
+H<sub>tra</sub> =
+1 &frasl; (1 &frasl; H<sub>op</sub> - 1 &frasl; H<sub>mas</sub>),
+</p>
+where <i>H<sub>op</sub></i> is the thermal transmission coefficient of opaque elements.
+The three heat gains components are calculated using
+<p align=\"center\" style=\"font-style:italic;\">
+&Phi;<sub>air</sub> = 0.5 &Phi;<sub>int</sub>,
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&Phi;<sub>sur</sub> = (1-f<sub>ms</sub> A<sub>f</sub> &frasl; A<sub>tot</sub>
+-H<sub>win</sub> &frasl; h<sub>ms</sub> A<sub>tot</sub>)(0.5 &Phi;<sub>int</sub>+
+&Phi;<sub>sol</sub>),
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+&Phi;<sub>mas</sub> = f<sub>ms</sub> A<sub>f</sub> &frasl; A<sub>tot</sub> (0.5&Phi;<sub>int</sub> +
+&Phi;<sub>sol</sub>).
+</p>
+<h4>Tips for parametrization</h4>
+<ul>
+<li>
+The parameters <code>AWin</code>, <code>AWal</code>, <code>surTil</code> and <code>surAzi</code>
+must have the same dimension of <code>nOrientations</code> .
+</li>
+<li>
+The areas in <code>AWal</code> must account only for the opaque parts of the walls (excluding windows).
+The floor and roof area is entered through <code>AFlo</code> and <code>ARoo</code>
+and must not be entered as part of <code>AWal</code>.
+</li>
+<li>
+If a wall contains only opaque parts, the corresponding window area must be set to <i>0</i>.
+</li>
+</ul>
+</html>",
+revisions="<html>
+<ul>
+<li>
+May 8, 2024, by Michael Wetter:<br/>
+Removed connection to itself.
+</li>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end Zone;
diff --git a/AixLib/ThermalZones/ISO13790/Zone5R1C/ZoneHVAC.mo b/AixLib/ThermalZones/ISO13790/Zone5R1C/ZoneHVAC.mo
new file mode 100644
index 0000000000..d0b2f328a1
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Zone5R1C/ZoneHVAC.mo
@@ -0,0 +1,69 @@
+within AixLib.ThermalZones.ISO13790.Zone5R1C;
+model ZoneHVAC "Thermal zone for HVAC based on 5R1C network"
+  extends Zone(capMas(C=buiMas.heaC*AFlo - VRoo*1.2*1014));
+  replaceable package Medium = Modelica.Media.Interfaces.PartialMedium annotation (
+        choices(choice(redeclare package Medium = AixLib.Media.Air "Moist air")));
+  parameter Integer nPorts=0 "Number of fluid ports" annotation (Evaluate=true,
+      Dialog(
+      connectorSizing=true,
+      tab="General",
+      group="Ports"));
+  Modelica.Blocks.Interfaces.RealInput intLatGai(final unit="W") "Internal latent heat gains"
+    annotation (Placement(transformation(extent={{-180,30},{-140,70}}),
+        iconTransformation(extent={{-180,20},{-140,60}})));
+  Modelica.Blocks.Math.Gain mWat_flow(final k=1/h_fg) "Water flow rate due to latent heat gain"
+    annotation (Placement(transformation(extent={{-100,40},{-80,60}})));
+  Fluid.MixingVolumes.MixingVolumeMoistAir vol(
+    redeclare final package Medium = Medium,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    m_flow_nominal=VRoo*AixLib.Media.Air.dStp*3/3600,
+    V=VRoo,
+    nPorts=nPorts) "Air volume"
+    annotation (Placement(transformation(extent={{-50,32},{-30,52}})));
+  Modelica.Fluid.Vessels.BaseClasses.VesselFluidPorts_b ports[nPorts](
+      redeclare each final package Medium = Medium)
+    "Fluid port for adding HVAC system, air infiltration and exfiltration"
+    annotation (Placement(transformation(
+        extent={{-39,-10},{39,10}},
+        rotation=90,
+        origin={-140,-80}), iconTransformation(
+        extent={{-39,-10},{39,10}},
+        rotation=90,
+        origin={-130,-82})));
+protected
+  constant Modelica.Units.SI.SpecificEnergy h_fg=
+      AixLib.Media.Air.enthalpyOfCondensingGas(273.15 + 37) "Latent heat of water vapor";
+
+equation
+  connect(mWat_flow.y, vol.mWat_flow) annotation (Line(points={{-79,50},{-52,50}},
+                              color={0,0,127}));
+  connect(heaPorAir, vol.heatPort) annotation (Line(points={{40,80},{26,80},{26,
+          26},{-54,26},{-54,42},{-50,42}}, color={191,0,0}));
+  connect(vol.ports, ports) annotation (Line(points={{-40,32},{-40,-16},{-128,
+          -16},{-128,-80},{-140,-80}}, color={0,127,255}));
+  connect(intLatGai, mWat_flow.u) annotation (Line(points={{-160,50},{-102,50}},
+                                                     color={0,0,127}));
+    annotation (
+    defaultComponentName="zonHVAC",
+    Documentation(info="<html>
+<p>
+This models is identical to <a href=\"modelica://AixLib.ThermalZones.ISO13790.Zone5R1C.Zone\">
+AixLib.ThermalZones.ISO13790.Zone5R1C.Zone</a>, except that a mixing volume is added
+for integration of HVAC systems based on fluid models. Latent heat gains are
+also considered.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+Mar 16, 2022, by Alessandro Maccarini:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Icon(graphics={Text(
+          extent={{-180,94},{-116,48}},
+          textColor={0,0,88},
+          textString="intLatGai")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end ZoneHVAC;
diff --git a/AixLib/ThermalZones/ISO13790/Zone5R1C/package.mo b/AixLib/ThermalZones/ISO13790/Zone5R1C/package.mo
new file mode 100644
index 0000000000..0532314bd7
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Zone5R1C/package.mo
@@ -0,0 +1,9 @@
+within AixLib.ThermalZones.ISO13790;
+package Zone5R1C "Package with reduced order thermal zones based on ISO 13790"
+  extends Modelica.Icons.VariantsPackage;
+
+  annotation (Documentation(info="<html>
+  <p>This package contains the core thermal zone models based on ISO 13790 that
+  can calculate the dynamic thermal behaviour of buildings.</p>
+</html>"));
+end Zone5R1C;
diff --git a/AixLib/ThermalZones/ISO13790/Zone5R1C/package.order b/AixLib/ThermalZones/ISO13790/Zone5R1C/package.order
new file mode 100644
index 0000000000..428ffdb78e
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/Zone5R1C/package.order
@@ -0,0 +1,2 @@
+Zone
+ZoneHVAC
diff --git a/AixLib/ThermalZones/ISO13790/package.mo b/AixLib/ThermalZones/ISO13790/package.mo
new file mode 100644
index 0000000000..eea0419dac
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/package.mo
@@ -0,0 +1,34 @@
+within AixLib.ThermalZones;
+package ISO13790 "Reduced order models based on ISO 13790"
+  extends Modelica.Icons.Package;
+
+annotation (
+    Icon(graphics={
+  Line(
+    points={{44,14},{44,-30}},
+    color={0,0,0},
+    smooth=Smooth.None),
+  Line(
+    points={{12,-30},{82,-30}},
+    color={0,0,0},
+    smooth=Smooth.None),
+  Line(
+    points={{22,-52},{70,-52}},
+    color={0,0,0},
+    smooth=Smooth.None),
+  Rectangle(
+    extent={{-80,36},{-10,-10}},
+    lineColor={0,0,0},
+    fillColor={255,255,255},
+    fillPattern=FillPattern.Solid),
+  Line(
+    points={{10,14},{80,14}},
+    color={0,0,0},
+    smooth=Smooth.None)}),
+    Documentation(info="<html>
+    <p>This package contains models for reduced building physics of thermal zones 
+    based on a thermal network consisting of five resistances and one capacitance. 
+    The models are based on the ISO 13790:2008 Standard.</p>
+    
+  </html>"));
+end ISO13790;
diff --git a/AixLib/ThermalZones/ISO13790/package.order b/AixLib/ThermalZones/ISO13790/package.order
new file mode 100644
index 0000000000..cfdb2d92c2
--- /dev/null
+++ b/AixLib/ThermalZones/ISO13790/package.order
@@ -0,0 +1,5 @@
+Zone5R1C
+Data
+Examples
+Validation
+BaseClasses
diff --git a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/PartialVDI6007.mo b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/PartialVDI6007.mo
index e2178aaf2f..466a057e54 100644
--- a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/PartialVDI6007.mo
+++ b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/PartialVDI6007.mo
@@ -10,7 +10,10 @@ partial model PartialVDI6007
   parameter Real wfGro(unit="1")
     "Weight factor of the ground (0 if not considered)";
   parameter Modelica.Units.SI.Temperature TGro
-    "Temperature of the ground in contact with floor plate";
+    "Constant temperature of the ground in contact with floor plate"
+    annotation (
+      HideResult=TGroundFromInput,
+      Dialog(enable=not TGroundFromInput));
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConWallOut
     "Exterior walls convective coefficient of heat transfer (outdoor)";
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hRad
@@ -18,6 +21,9 @@ partial model PartialVDI6007
   parameter Boolean withLongwave=true
     "Set to true to include longwave radiation exchange"
     annotation(choices(checkBox = true));
+  parameter Boolean TGroundFromInput=false
+    "Set to true to use TGro_in input connector instead of TGro constant"
+    annotation(choices(checkBox = true));
 
   Modelica.Units.SI.Temperature TEqWall[n] "Equivalent wall temperature";
   Modelica.Units.SI.Temperature TEqWin[n] "Equivalent window temperature";
@@ -61,13 +67,27 @@ partial model PartialVDI6007
     extent={{-20,-20},{20,20}},
     rotation=-90,
     origin={0,120})));
+  Modelica.Blocks.Interfaces.RealInput TGro_in(
+    final quantity="ThermodynamicTemperature",
+    final unit="K",
+    displayUnit="degC") if TGroundFromInput
+    "Temperature of the ground in contact with floor plate"
+    annotation (Placement(
+        transformation(
+        extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={0,-120})));
+
+protected
+  SourceSelector TGroSouSel(final useInput=TGroundFromInput, p=TGro)
+    "Input selector for ground temperature";
 
 initial equation
   assert(noEvent(abs(sum(wfWall) + sum(wfWin) + wfGro) > 0.1),
  "The sum of the weighting factors (walls,windows and ground) in the
-    equivalent air temperature calculation is close to 0.
-    If there are no walls, windows and ground at all, this might be
-    irrelevant.",level=AssertionLevel.warning);
+   equivalent air temperature calculation is close to 0.
+   If there are no walls, windows and ground at all, this might be
+   irrelevant.", level=AssertionLevel.warning);
 
 equation
   delTEqLW=(TBlaSky - TDryBul)*hRad/(hRad + hConWallOut);
@@ -80,6 +100,7 @@ equation
     TEqWall=TDryBul.+delTEqSW;
   end if;
 
+  connect(TGro_in, TGroSouSel.uCon);
   annotation (  Icon(coordinateSystem(preserveAspectRatio=false,
   extent={{-100,-100},{100,100}}),
   graphics={
@@ -114,39 +135,45 @@ equation
   Line(points={{2,-78},{32,-48},{100,-48}}, color={0,0,0}),
   Line(points={{32,20},{32,-48}}, color={0,0,0})}),
   Documentation(info="<html>
-   <p><code>PartialVDI6007</code> is a partial model for <code>EquivalentAirTemperature</code>
-   models.</p>
-   </html>",
+  <p><code>PartialVDI6007</code> is a partial model for <code>EquivalentAirTemperature</code>
+  models.</p>
+  </html>",
   revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaRad</code> to <code>hRad</code>,
-   <code>alphaWinOut</code> to <code>hConWallOut</code>
-   </li>
-   <li>
-   September 26, 2016, by Moritz Lauster:<br/>
-   Removed deprecated parameters and values
-   0.93 and <code>eExt</code>.<br/>
-   Renamed <code>alphaRadWall</code> to
-   <code>alphaRad</code>. Deleted
-   <code>alphaRadWin</code>.<br/>
-   Moved calculations from
-   <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007\">
-   AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007</a> and
-   <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
-   AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a> to here.
-   </li>
-   <li>
-   September 2015, by Moritz Lauster:<br/>
-   Got rid of cardinality and used assert for warnings.<br/>
-   Adapted to Annex 60 requirements.
-   </li>
-   <li>
-   October 2014, by Peter Remmen:<br/>
-   Implemented.
-   </li>
-   </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <ul>
+  <li>
+  May 5, 2023, by Philip Groesdonk:<br/>
+  Added an option for non-constant ground temperature from an input connector.
+  This is for
+  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1744\">#1744</a>.
+  </li>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaRad</code> to <code>hRad</code>,
+  <code>alphaWinOut</code> to <code>hConWallOut</code>
+  </li>
+  <li>
+  September 26, 2016, by Moritz Lauster:<br/>
+  Removed deprecated parameters and values
+  0.93 and <code>eExt</code>.<br/>
+  Renamed <code>alphaRadWall</code> to
+  <code>alphaRad</code>. Deleted
+  <code>alphaRadWin</code>.<br/>
+  Moved calculations from
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007\">
+  AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007</a> and
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
+  AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a> to here.
+  </li>
+  <li>
+  September 2015, by Moritz Lauster:<br/>
+  Got rid of cardinality and used assert for warnings.<br/>
+  Adapted to Annex 60 requirements.
+  </li>
+  <li>
+  October 2014, by Peter Remmen:<br/>
+  Implemented.
+  </li>
+  </ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialVDI6007;
diff --git a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/SourceSelector.mo b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/SourceSelector.mo
new file mode 100644
index 0000000000..6035e7e19c
--- /dev/null
+++ b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/SourceSelector.mo
@@ -0,0 +1,52 @@
+within AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses;
+block SourceSelector
+  "Block that selects as its output either a parameter value or its input"
+  extends Modelica.Blocks.Interfaces.SO;
+  parameter Boolean useInput "Use input (if true) or parameter value (if false)"
+    annotation(Evaluate=true);
+  parameter Real p "Parameter value";
+  Modelica.Blocks.Interfaces.RealInput uCon if useInput
+    "Input signal from input connector"
+    annotation (Placement(transformation(extent={{-140,40},{-100,80}}),
+        iconTransformation(extent={{-120,70},{-100,90}})));
+equation
+  if not useInput then
+    y = p;
+  end if;
+  connect(uCon, y);
+  annotation (
+  defaultComponentName="souSel",
+Documentation(info="<html>
+<p>
+Block that produces at its output the input value <code>uCon</code>
+or the parameter value <code>p</code> depending on the parameter value
+<code>useInput</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 28, 2023, by Philip Groesdonk:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    Icon(graphics={
+      Rectangle(
+          extent={{-100,100},{100,-100}},
+          fillColor={210,210,210},
+          fillPattern=FillPattern.Solid,
+          borderPattern=BorderPattern.Raised),
+        Line(points={{12,0},{100,0}},
+          color={0,0,127}),
+        Line(points={{-100,80},{-38,80}},
+          color={0,0,127}),
+        Line(points={{-40,80},{8,0}},
+          color={0,0,127},
+          visible=useInput,
+          thickness=1),
+        Ellipse(lineColor={0,0,255},
+          pattern=LinePattern.None,
+          fillPattern=FillPattern.Solid,
+          extent={{2,-8},{18,8}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SourceSelector;
diff --git a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/package.order b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/package.order
index 609fb4d171..52fe857587 100644
--- a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/package.order
+++ b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/BaseClasses/package.order
@@ -1 +1,2 @@
 PartialVDI6007
+SourceSelector
diff --git a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/VDI6007.mo b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/VDI6007.mo
index 08099da165..e08723debe 100644
--- a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/VDI6007.mo
+++ b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/VDI6007.mo
@@ -5,31 +5,37 @@ model VDI6007 "Equivalent air temperature as defined in VDI 6007 Part 1"
 initial equation
   assert(noEvent(abs(sum(wfWall) + sum(wfWin) + wfGro - 1) < 0.1),
   "The sum of the weighting factors (walls,windows and ground)  is
-   <0.9 or >1.1. Normally, the sum should be 1.",level=AssertionLevel.warning);
+  <0.9 or >1.1. Normally, the sum should be 1.", level=AssertionLevel.warning);
 
 equation
   delTEqLWWin=delTEqLW;
-  TEqAir = TEqWall*wfWall + TEqWin*wfWin + TGro*wfGro;
+  TEqAir = TEqWall*wfWall + TEqWin*wfWin +  TGroSouSel.y*wfGro;
   annotation (defaultComponentName = "equAirTem",Documentation(revisions="<html>
-   <ul>
-   <li>
-   September 26, 2016, by Moritz Lauster:<br/>
-   Moved calculations to <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses.PartialVDI6007\">
-   AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses.PartialVDI6007</a>.
-   </li>
-   <li>September 2015, by Moritz Lauster:<br/>
-   Got rid of cardinality
-   and used assert for warnings.<br/>
-   Adapted to Annex 60 requirements.
-   </li>
-   <li>
-   October 2014, by Peter Remmen:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>",info="<html>
-   <p><code>VDI6007</code> is a strict implementation of the calculations defined
-   in VDI 6007 Part 1. The sum of all weightfactors should be one.</p>
-   </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <ul>
+  <li>
+  May 5, 2023, by Philip Groesdonk:<br/>
+  Added an option for non-constant ground temperature from an input connector.
+  This is for
+  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1744\">#1744</a>.
+  </li>
+  <li>
+  September 26, 2016, by Moritz Lauster:<br/>
+  Moved calculations to <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses.PartialVDI6007\">
+  AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses.PartialVDI6007</a>.
+  </li>
+  <li>September 2015, by Moritz Lauster:<br/>
+  Got rid of cardinality
+  and used assert for warnings.<br/>
+  Adapted to Annex 60 requirements.
+  </li>
+  <li>
+  October 2014, by Peter Remmen:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>", info="<html>
+  <p><code>VDI6007</code> is a strict implementation of the calculations defined
+  in VDI 6007 Part 1. The sum of all weightfactors should be one.</p>
+  </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VDI6007;
diff --git a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/VDI6007WithWindow.mo b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/VDI6007WithWindow.mo
index 1749494104..33bfc50f9e 100644
--- a/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/VDI6007WithWindow.mo
+++ b/AixLib/ThermalZones/ReducedOrder/EquivalentAirTemperature/VDI6007WithWindow.mo
@@ -14,43 +14,49 @@ model VDI6007WithWindow
 initial equation
   assert(noEvent(abs(sum(wfWall) + wfGro - 1) < 0.1),
   "The sum of the weightfactors (walls and ground)  is <0.9 or >1.1.
-    Normally, the sum should be 1.",level=AssertionLevel.warning);
+   Normally, the sum should be 1.", level=AssertionLevel.warning);
   assert(noEvent(abs(sum(wfWin) - 1) < 0.1),
   "The sum of the weightfactors (windows)  is <0.9 or >1.1.
-   Normally, the sum should be 1.",level=AssertionLevel.warning);
+  Normally, the sum should be 1.", level=AssertionLevel.warning);
 
 equation
   delTEqLWWin=(TBlaSky - TDryBul)*hRad/(hRad + hConWinOut);
-  TEqAir = TEqWall*wfWall + TGro*wfGro;
+  TEqAir = TEqWall*wfWall +  TGroSouSel.y*wfGro;
   TEqAirWin = TEqWin*wfWin;
   annotation (defaultComponentName = "equAirTem",Documentation(revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWinOut</code> to <code>hConWinOut</code>
-   </li>
-   <li>
-   September 26, 2016, by Moritz Lauster:<br/>
-   Moved calculations to <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses.PartialVDI6007\">
-   AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses.PartialVDI6007</a>.
-   </li>
-   <li>September 2015, by Moritz Lauster:<br/>
-   Got rid of cardinality
-   and used assert for warnings.<br/>
-   Adapted to Annex 60 requirements.
-   </li>
-   <li>
-   October 2014, by Peter Remmen:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>",
+  <ul>
+  <li>
+  May 5, 2023, by Philip Groesdonk:<br/>
+  Added an option for non-constant ground temperature from an input connector.
+  This is for
+  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1744\">#1744</a>.
+  </li>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWinOut</code> to <code>hConWinOut</code>
+  </li>
+  <li>
+  September 26, 2016, by Moritz Lauster:<br/>
+  Moved calculations to <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses.PartialVDI6007\">
+  AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.BaseClasses.PartialVDI6007</a>.
+  </li>
+  <li>September 2015, by Moritz Lauster:<br/>
+  Got rid of cardinality
+  and used assert for warnings.<br/>
+  Adapted to Annex 60 requirements.
+  </li>
+  <li>
+  October 2014, by Peter Remmen:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>",
   info="<html>
-   <p>This model is a variant of the calculations defined in
-   VDI 6007 Part 1. It adds a second equivalent air temperature for windows in
-   case heat transfer through windows and exterior walls is handled separately in
-   the Reduced Order Model. The sum of all weightfactors for windows should be
-   one as well as the sum for all wall elements.</p>
-   </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>This model is a variant of the calculations defined in
+  VDI 6007 Part 1. It adds a second equivalent air temperature for windows in
+  case heat transfer through windows and exterior walls is handled separately in
+  the Reduced Order Model. The sum of all weightfactors for windows should be
+  one as well as the sum for all wall elements.</p>
+  </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VDI6007WithWindow;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/ComparisonThermalZoneMoistAndDryAir.mo b/AixLib/ThermalZones/ReducedOrder/Examples/ComparisonThermalZoneMoistAndDryAir.mo
index 889af3d335..7d4cb79e29 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/ComparisonThermalZoneMoistAndDryAir.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/ComparisonThermalZoneMoistAndDryAir.mo
@@ -12,8 +12,7 @@ model ComparisonThermalZoneMoistAndDryAir
     internalGainsMode=3,
     nPorts=2,
     T_start=293.15,
-    zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler())
+    redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam)
     "Thermal zone"
     annotation (Placement(transformation(extent={{-10,-22},{10,-2}})));
   AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
@@ -130,14 +129,14 @@ model ComparisonThermalZoneMoistAndDryAir
     "Split additional internal gains into radiative an convective"
     annotation (Placement(transformation(extent={{66,-36},{54,-24}})));
 
-  Fluid.Sources.MassFlowSource_T sourcAir(
+  AixLib.Fluid.Sources.MassFlowSource_T sourcAir(
     redeclare package Medium = Media.Air,
     m_flow=3000/3600*1.17,
     X={0.004,1 - 0.004},
     T=283.15,
     nPorts=1) "mass flow rate of air into thermal zone"
     annotation (Placement(transformation(extent={{-84,-92},{-64,-72}})));
-  Fluid.Sources.Boundary_pT sinAir(redeclare package Medium = Media.Air,
+  AixLib.Fluid.Sources.Boundary_pT sinAir(redeclare package Medium = Media.Air,
       nPorts=1) "sink of air"
     annotation (Placement(transformation(extent={{-12,-98},{-32,-78}})));
   AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone thermalZone(
@@ -147,8 +146,7 @@ model ComparisonThermalZoneMoistAndDryAir
     redeclare package Medium = Media.Air,
     internalGainsMode=1,
     nPorts=2,
-    zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler(),
+    redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam,
     T_start=293.15) "Thermal zone"
     annotation (Placement(transformation(extent={{-12,74},{8,94}})));
 
@@ -258,14 +256,14 @@ model ComparisonThermalZoneMoistAndDryAir
   Modelica.Blocks.Math.Gain gain3(k=0.5)
     "Split additional internal gains into radiative an convective"
     annotation (Placement(transformation(extent={{64,60},{52,72}})));
-  Fluid.Sources.MassFlowSource_T sourcAir1(
+  AixLib.Fluid.Sources.MassFlowSource_T sourcAir1(
     redeclare package Medium = Media.Air,
     m_flow=3000/3600*1.17,
     X={0.004,1 - 0.004},
     T=283.15,
     nPorts=1) "mass flow rate of air into thermal zone"
     annotation (Placement(transformation(extent={{-72,0},{-52,20}})));
-  Fluid.Sources.Boundary_pT sinAir1(redeclare package Medium = Media.Air,
+  AixLib.Fluid.Sources.Boundary_pT sinAir1(redeclare package Medium = Media.Air,
       nPorts=1) "sink of air"
     annotation (Placement(transformation(extent={{34,4},{14,24}})));
 equation
@@ -292,10 +290,12 @@ equation
           67.2,-30}},
                  color={0,0,127}));
   connect(sourcAir.ports[1], thermalZoneMoistAir.ports[1]) annotation (Line(
-        points={{-64,-82},{-46,-82},{-46,-48},{-2.35,-48},{-2.35,-19.2}}, color=
+        points={{-64,-82},{-46,-82},{-46,-48},{-1.175,-48},{-1.175,-19.2}},
+                                                                          color=
          {0,127,255}));
   connect(thermalZoneMoistAir.ports[2], sinAir.ports[1]) annotation (Line(
-        points={{2.35,-19.2},{2.35,-52},{-38,-52},{-38,-88},{-32,-88}}, color={
+        points={{1.175,-19.2},{1.175,-52},{-38,-52},{-38,-88},{-32,-88}},
+                                                                        color={
           0,127,255}));
   connect(internalGains1.y, thermalZone.intGains)
     annotation (Line(points={{-1.3,32},{6,32},{6,75.6}}, color={0,0,127}));
@@ -314,9 +314,9 @@ equation
   connect(sine1.y, gain3.u) annotation (Line(points={{71,84},{68,84},{68,66},{65.2,
           66}}, color={0,0,127}));
   connect(sourcAir1.ports[1], thermalZone.ports[1]) annotation (Line(points={{-52,10},
-          {-48,10},{-48,48},{-4.35,48},{-4.35,76.8}},     color={0,127,255}));
-  connect(thermalZone.ports[2], sinAir1.ports[1]) annotation (Line(points={{0.35,
-          76.8},{0.35,44},{-40,44},{-40,14},{14,14}},     color={0,127,255}));
+          {-48,10},{-48,48},{-3.175,48},{-3.175,76.8}},   color={0,127,255}));
+  connect(thermalZone.ports[2], sinAir1.ports[1]) annotation (Line(points={{-0.825,
+          76.8},{-0.825,44},{-40,44},{-40,14},{14,14}},   color={0,127,255}));
   connect(weaDat.weaBus, thermalZone.weaBus) annotation (Line(
       points={{-78,-8},{-76,-8},{-76,90},{-12,90}},
       color={255,204,51},
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/Multizone.mo b/AixLib/ThermalZones/ReducedOrder/Examples/Multizone.mo
index fb15674f9a..12615c7b51 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/Multizone.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/Multizone.mo
@@ -133,7 +133,10 @@ equation
           -55},{36.8,-9}}, color={0,0,127}));
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
-    experiment(StopTime=3.1536e+007, Interval=3600),
+    experiment(Tolerance=1e-6, StopTime=864000, Interval=3600),
+    __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/Multizone.mos"
+        "Simulate and plot"),
     Documentation(info="<html><p>
   This example illustrates the use of <a href=
   \"AixLib.ThermalZones.ReducedOrder.Multizone.Multizone\">AixLib.ThermalZones.ReducedOrder.Multizone.Multizone</a>.
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneEquipped.mo b/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneEquipped.mo
index 259086095e..718b11e9de 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneEquipped.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneEquipped.mo
@@ -134,10 +134,10 @@ equation
           34.6,-82},{34.6,-9}}, color={0,0,127}));
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
-    experiment(
-      StopTime=31536000,
-      Interval=3600,
-      __Dymola_Algorithm="Cvode"),
+    experiment(Tolerance=1e-6, StopTime=3.1536e+007, Interval=3600),
+    __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneEquipped.mos"
+        "Simulate and plot"),
     Documentation(revisions="<html><ul>
   <li>September 29, 2016, by Moritz Lauster:<br/>
     Implemented.
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2Equipped.mo b/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2Equipped.mo
index 8351075afd..be591d3299 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2Equipped.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2Equipped.mo
@@ -139,7 +139,7 @@ equation
           34.6,-82},{34.6,-9}}, color={0,0,127}));
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
-    experiment(Tolerance=1e-6, StopTime=3.1536e+007, Interval=3600),
+    experiment(Tolerance=1e-6, StopTime=864000, Interval=3600),
     Documentation(revisions="<html><ul>
   <li>August 27, 2020, by Katharina Breuer:<br/>
     Add co2 balance
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2EquippedSwimmingFacility.mo b/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2EquippedSwimmingFacility.mo
new file mode 100644
index 0000000000..90e699487d
--- /dev/null
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2EquippedSwimmingFacility.mo
@@ -0,0 +1,197 @@
+within AixLib.ThermalZones.ReducedOrder.Examples;
+model MultizoneMoistAirCO2EquippedSwimmingFacility
+  "Illustrates the use of MultizoneMoistAirCO2Equipped"
+  import AixLib;
+  extends Modelica.Icons.Example;
+  replaceable package Medium = AixLib.Media.Air (extraPropertiesNames={"C_flow"});
+
+  AixLib.ThermalZones.ReducedOrder.Multizone.MultizoneEquipped
+    multizone(
+    buildingID=1,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    VAir=33500,
+    ABuilding=8375,
+    ASurTot=12744.27,
+    numZones=6,
+    zoneParam={DataBase.ThermalZones.SwimmingFacility.SwimmingHall(HeaterOn=
+        true),DataBase.ThermalZones.SwimmingFacility.Entrance(HeaterOn=true),
+        DataBase.ThermalZones.SwimmingFacility.Changing(HeaterOn=true),
+        DataBase.ThermalZones.SwimmingFacility.Showers(HeaterOn=true),
+        DataBase.ThermalZones.SwimmingFacility.Supervisory(HeaterOn=true),
+        DataBase.ThermalZones.SwimmingFacility.Technichal(HeaterOn=true)},
+    use_C_flow=true,
+    use_moisture_balance=true,
+    internalGainsMode=3,
+    use_pools_tot=true,
+    heatAHU=true,
+    coolAHU=true,
+    dehuAHU=true,
+    huAHU=true,
+    BPFDehuAHU=0.2,
+    HRS=false,
+    sampleRateAHU=1800,
+    effFanAHU_sup=0.7,
+    effFanAHU_eta=0.7,
+    effHRSAHU_enabled=0.8,
+    effHRSAHU_disabled=0.2,
+    zone(
+      use_pools={true,false,false,false,false,false},
+      nPools={2,1,1,1,1,1},
+      poolWallParam={{
+          AixLib.DataBase.Pools.SwimmingPoolWalls.ConcreteInsulationConstruction(),
+          AixLib.DataBase.Pools.SwimmingPoolWalls.ConcreteInsulationConstruction()},
+          {AixLib.DataBase.Walls.ASHRAE140.DummyDefinition()},{
+          AixLib.DataBase.Walls.ASHRAE140.DummyDefinition()},{
+          AixLib.DataBase.Walls.ASHRAE140.DummyDefinition()},{
+          AixLib.DataBase.Walls.ASHRAE140.DummyDefinition()},{
+          AixLib.DataBase.Walls.ASHRAE140.DummyDefinition()}},
+      poolParam={{AixLib.DataBase.Pools.SportPool(),
+          AixLib.DataBase.Pools.ChildrensPool()},{
+          AixLib.DataBase.Pools.IndoorSwimmingPoolDummy()},{
+          AixLib.DataBase.Pools.IndoorSwimmingPoolDummy()},{
+          AixLib.DataBase.Pools.IndoorSwimmingPoolDummy()},{
+          AixLib.DataBase.Pools.IndoorSwimmingPoolDummy()},{
+          AixLib.DataBase.Pools.IndoorSwimmingPoolDummy()}},
+      ROM(extWallRC(thermCapExt(each der_T(fixed=true))),
+          intWallRC(thermCapInt(each der_T(fixed=true))),
+           floorRC(thermCapExt(each der_T(fixed=true))),
+           roofRC(thermCapExt(each der_T(fixed=true))))),
+    redeclare package Medium = Medium,
+    T_start=293.15,
+    dpAHU_sup(displayUnit="Pa") = 800,
+    dpAHU_eta(displayUnit="Pa") = 800) "Multizone"
+    annotation (Placement(transformation(extent={{32,-8},{52,12}})));
+
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
+    calTSky=AixLib.BoundaryConditions.Types.SkyTemperatureCalculation.HorizontalRadiation,
+    computeWetBulbTemperature=false,
+    filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data reader"
+    annotation (Placement(transformation(extent={{-82,30},{-62,50}})));
+  Modelica.Blocks.Sources.CombiTimeTable tableInternalGains(
+    tableOnFile=true,
+    extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic,
+    tableName="Internals",
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/LowOrder_ExampleData/InternalGains_SwimmingFacility_6Zones.txt"),
+    columns=2:19)
+    "Profiles for internal gains"
+    annotation (Placement(transformation(extent={{74,-42},{58,-26}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow prescribedHeatFlow[6]
+    "Radiative heat flow of additional internal gains"
+    annotation (Placement(transformation(extent={{-14,-64},{6,-44}})));
+  Modelica.Blocks.Sources.Sine sine(
+    amplitude=500,
+    f=1/86400,
+    offset=500) "Sinusoidal excitation for additional internal gains"
+    annotation (Placement(transformation(extent={{-90,-74},{-70,-54}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow prescribedHeatFlow1[6]
+    "Convective heat flow of additional internal gains"
+    annotation (Placement(transformation(extent={{-14,-86},{6,-66}})));
+  Modelica.Blocks.Math.Gain gain(k=0.5)
+    "Split additional internal gains into radiative an convective"
+    annotation (Placement(transformation(extent={{-56,-60},{-44,-48}})));
+  Modelica.Blocks.Math.Gain gain1(k=0.5)
+    "Split additional internal gains into radiative an convective"
+    annotation (Placement(transformation(extent={{-56,-82},{-44,-70}})));
+  Modelica.Blocks.Routing.Replicator replicator(nout=6)
+    "Replicates sinusoidal excitation for numZones" annotation (Placement(
+        transformation(
+        extent={{-6,-6},{6,6}},
+        rotation=0,
+        origin={-30,-54})));
+  Modelica.Blocks.Routing.Replicator replicator1(nout=6)
+    "Replicates sinusoidal excitation for numZones" annotation (Placement(
+        transformation(
+        extent={{-6,-6},{6,6}},
+        rotation=0,
+        origin={-30,-76})));
+  Modelica.Blocks.Sources.CombiTimeTable tableAHU(
+    tableOnFile=true,
+    extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic,
+    tableName="AHU",
+    columns=2:5,
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/LowOrder_ExampleData/AHU_Input_SwimmingFacility_6Zones.txt"))
+    "Boundary conditions for air handling unit"
+    annotation (Placement(transformation(extent={{-64,-6},{-48,10}})));
+  Modelica.Blocks.Sources.CombiTimeTable tableTSet(
+    tableOnFile=true,
+    tableName="Tset",
+    extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic,
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/LowOrder_ExampleData/Tset_SwimmingFacility.txt"),
+    columns=2:7)
+    "Set points for heater"
+    annotation (Placement(transformation(extent={{72,-66},{56,-50}})));
+  Modelica.Blocks.Sources.Constant const[6](each k=0)
+    "Set point for cooler"
+    annotation (Placement(transformation(extent={{72,-90},{56,-74}})));
+
+  Modelica.Blocks.Sources.CombiTimeTable tableOpeningHours(
+    tableOnFile=true,
+    extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic,
+    tableName="openingHours",
+    columns=2:2,
+    fileName=ModelicaServices.ExternalReferences.loadResource("modelica://AixLib/Resources/LowOrder_ExampleData/OpeningHours_SwimmingFacility.txt"))
+    "Boundary condition: Opening Hours of swiming pools"
+    annotation (Placement(transformation(extent={{-64,-32},{-48,-16}})));
+equation
+  connect(weaDat.weaBus, multizone.weaBus) annotation (Line(
+      points={{-62,40},{-32,40},{-32,6},{34,6}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(tableInternalGains.y, multizone.intGains)
+    annotation (Line(points={{57.2,-34},{48,-34},{48,-9}}, color={0,0,127}));
+  connect(gain.y, replicator.u)
+    annotation (Line(points={{-43.4,-54},{-37.2,-54}}, color={0,0,127}));
+  connect(sine.y, gain.u) annotation (Line(points={{-69,-64},{-62,-64},{-62,-54},
+          {-57.2,-54}}, color={0,0,127}));
+  connect(sine.y, gain1.u) annotation (Line(points={{-69,-64},{-62,-64},{-62,-76},
+          {-57.2,-76}}, color={0,0,127}));
+  connect(gain1.y, replicator1.u)
+    annotation (Line(points={{-43.4,-76},{-37.2,-76}}, color={0,0,127}));
+  connect(replicator1.y, prescribedHeatFlow1.Q_flow)
+    annotation (Line(points={{-23.4,-76},{-14,-76}}, color={0,0,127}));
+  connect(replicator.y, prescribedHeatFlow.Q_flow) annotation (Line(points={{-23.4,
+          -54},{-18.7,-54},{-14,-54}}, color={0,0,127}));
+  connect(prescribedHeatFlow.port, multizone.intGainsRad) annotation (Line(
+        points={{6,-54},{18,-54},{18,-3},{34,-3}},
+                                color={191,0,0}));
+  connect(prescribedHeatFlow1.port, multizone.intGainsConv) annotation (Line(
+        points={{6,-76},{18,-76},{26,-76},{26,-6.2},{34,-6.2}},
+                                                            color={191,0,0}));
+  connect(tableAHU.y, multizone.AHU)
+    annotation (Line(points={{-47.2,2},{14,2},{33,2}}, color={0,0,127}));
+  connect(tableTSet.y, multizone.TSetHeat) annotation (Line(points={{55.2,-58},
+          {36.8,-58},{36.8,-9}}, color={0,0,127}));
+  connect(const.y, multizone.TSetCool) annotation (Line(points={{55.2,-82},{
+          34.6,-82},{34.6,-9}}, color={0,0,127}));
+  connect(tableOpeningHours.y[1],multizone.timeOpe)
+      annotation (Line(points={{-47.2,-24},{45.8,-24},{45.8,-9}},
+                                                            color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    experiment(Tolerance=1e-6,StopTime=3.1536e+007,Interval=3600),
+        __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizoneMoistAirCO2EquippedSwimmingFacility.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+<p>
+  This example illustrates the use of <a href=
+  \"AixLib.ThermalZones.ReducedOrder.Multizone.MultizoneEquipped\">
+  AixLib.ThermalZones.ReducedOrder.Multizone.MultizoneEquipped</a>.
+  Parameter set is for an swimming facility, including all relevant zones: 
+  swimming hall, entrance hall, changing room, showers, life guard area, technical rooms.
+  The results should show typical profiles for
+  indoor air temperatures, but are not related to a specific building
+  or measurement data.
+</p>
+</html>"),
+    __Dymola_experimentFlags(
+      Advanced(
+        EvaluateAlsoTop=false,
+        GenerateVariableDependencies=false,
+        OutputModelicaCode=false),
+      Evaluate=true,
+      OutputCPUtime=false,
+      OutputFlatModelica=false));
+end MultizoneMoistAirCO2EquippedSwimmingFacility;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/MultizonePartlyCooled.mo b/AixLib/ThermalZones/ReducedOrder/Examples/MultizonePartlyCooled.mo
index ffe8b0a184..49d7b08f25 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/MultizonePartlyCooled.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/MultizonePartlyCooled.mo
@@ -10,11 +10,11 @@ model MultizonePartlyCooled "Illustrates the use of Multizone"
     ABuilding=8375,
     ASurTot=12744.27,
     numZones=5,
-    zoneParam={AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=true),
-        AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=true),
+    zoneParam={AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=true, lCool=-1000),
+        AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=true, lCool=-10000),
         AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=false),
-        AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=true),
-        AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=true)},
+        AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=true, lCool=-20000),
+        AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_Office(CoolerOn=true, lCool=-30000)},
     redeclare package Medium = Modelica.Media.Air.SimpleAir,
     T_start=293.15,
     zone(ROM(extWallRC(thermCapExt(each der_T(fixed=true))), intWallRC(
@@ -133,7 +133,15 @@ equation
           -55},{36.8,-9}}, color={0,0,127}));
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
-    experiment(StopTime=3.1536e+007, Interval=3600),
+    experiment(
+      StartTime=14688000,
+      StopTime=15552000,
+      Interval=3600,
+      Tolerance=1e-06,
+      __Dymola_Algorithm="Dassl"),
+    __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/MultizonePartlyCooled.mos"
+        "Simulate and plot"),
     Documentation(info="<html><p>
   This example is based on <a href=
   \"AixLib.ThermalZones.ReducedOrder.Examples.Multizone\">AixLib.ThermalZones.ReducedOrder.Examples.Multizone</a>.
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElements.mo b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElements.mo
index 64ececa6ed..923884d783 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElements.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElements.mo
@@ -107,7 +107,7 @@ model SimpleRoomFourElements
         86400,0,0,0],
     columns={2,3,4},
     extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic) "Table with profiles for persons (radiative and convective) and machines
-     (convective)"
+    (convective)"
     annotation (Placement(transformation(extent={{6,-60},{22,-44}})));
   Modelica.Blocks.Sources.Constant const[2](each k=0)
     "Sets sunblind signal to zero (open)"
@@ -287,59 +287,59 @@ equation
   connect(corGDouPan.solarRadWinTrans, thermalZoneFourElements.solRad)
     annotation (Line(points={{27,56},{40,56},{40,31},{43,31}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>This example shows the application of
-   <a href=\"AixLib.ThermalZones.ReducedOrder.RC.FourElements\">
-   AixLib.ThermalZones.ReducedOrder.RC.FourElements</a>
-   in combination with
-   <a href=\"AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
-  AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
-   and
-   <a href=\"AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
-   AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
-   Solar radiation on tilted surface is calculated using models of
-   AixLib. The thermal zone is a simple room defined in Guideline
-   VDI 6007 Part 1 (VDI, 2012). All models, parameters and inputs
-   except sunblinds, separate handling of heat transfer through
-   windows, an extra wall element for ground floor (with additional
-   area), an extra wall element for roof (with additional area) and
-   solar radiation are similar to the ones defined for the
-   guideline&apos;s test room. For solar radiation, the example
-   relies on the standard weather file in AixLib.</p>
-   <p>The idea of the example is to show a typical application of
-   all sub-models and to use the example in unit tests. The results
-   are reasonable, but not related to any real use case or measurement
-   data.</p>
-   <h4>References</h4>
-   <p>VDI. German Association of Engineers Guideline VDI
-   6007-1 March 2012. Calculation of transient thermal response of
-   rooms and buildings - modelling of rooms.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   September 6, 2021, by Ettore Zanetti:<br/>
-   Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
-   This is for
-   <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
-   </li>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>,
-   <code>alphaRoof</code> to <code>hConRoof</code>,
-   <code>alphaWin</code> to <code>hConWin</code>
-   </li>
-   <li>
-   April 27, 2016, by Michael Wetter:<br/>
-   Removed call to <code>Modelica.Utilities.Files.loadResource</code>
-   as this did not work for the regression tests.
-   </li>
-   <li>February 25, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
+  <p>This example shows the application of
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.FourElements\">
+  AixLib.ThermalZones.ReducedOrder.RC.FourElements</a>
+  in combination with
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
+ AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
+  and
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
+  AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
+  Solar radiation on tilted surface is calculated using models of
+  AixLib. The thermal zone is a simple room defined in Guideline
+  VDI 6007 Part 1 (VDI, 2012). All models, parameters and inputs
+  except sunblinds, separate handling of heat transfer through
+  windows, an extra wall element for ground floor (with additional
+  area), an extra wall element for roof (with additional area) and
+  solar radiation are similar to the ones defined for the
+  guideline&apos;s test room. For solar radiation, the example
+  relies on the standard weather file in AixLib.</p>
+  <p>The idea of the example is to show a typical application of
+  all sub-models and to use the example in unit tests. The results
+  are reasonable, but not related to any real use case or measurement
+  data.</p>
+  <h4>References</h4>
+  <p>VDI. German Association of Engineers Guideline VDI
+  6007-1 March 2012. Calculation of transient thermal response of
+  rooms and buildings - modelling of rooms.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  September 6, 2021, by Ettore Zanetti:<br/>
+  Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+  This is for
+  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+  </li>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>,
+  <code>alphaRoof</code> to <code>hConRoof</code>,
+  <code>alphaWin</code> to <code>hConWin</code>
+  </li>
+  <li>
+  April 27, 2016, by Michael Wetter:<br/>
+  Removed call to <code>Modelica.Utilities.Files.loadResource</code>
+  as this did not work for the regression tests.
+  </li>
+  <li>February 25, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),
   experiment(Tolerance=1e-6, StopTime=3.1536e+007, Interval=3600),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElements.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SimpleRoomFourElements;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElementsTraceSubstance.mo b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElementsTraceSubstance.mo
index 54cc04b0f1..4e2b90addd 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElementsTraceSubstance.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElementsTraceSubstance.mo
@@ -63,58 +63,58 @@ equation
   connect(traSubAmb.y, souAir.C_in[1])
     annotation (Line(points={{-67,-78},{-42,-78}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
- <p>
- This example shows the application of
- <a href=\"AixLib.ThermalZones.ReducedOrder.RC.FourElements\">
- AixLib.ThermalZones.ReducedOrder.RC.FourElements</a>
- considering a trace substance such as CO2
- in combination with
- <a href=\"AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
- AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
- and
- <a href=\"AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
- AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
- Solar radiation on tilted surface is calculated using models of
- AixLib. The thermal zone is a simple room defined in Guideline
- VDI 6007 Part 1 (VDI, 2012).
- The trace substance calculation is based on the CO2 emissions of 2 persons.
- They stay in the thermal zone for 12 hours every 24 hours. The air exchange rate is 2 air changes per hour.
- All further models, parameters and inputs
- except sunblinds, separate handling of heat transfer through
- windows, no wall element for internal walls and solar radiation
- are similar to the ones defined for the guideline&apos;s test
- room. For solar radiation, the example relies on the standard
- weather file in AixLib.
- </p>
- <p>
- The idea of the example is to show a typical application of all
- sub-models and to use the example in unit tests. The results are
- reasonable, but not related to any real use case or measurement
- data.
- </p>
- <h4>References</h4>
- <p>VDI. German Association of Engineers Guideline VDI 6007-1
- March 2012. Calculation of transient thermal response of rooms
- and buildings - modelling of rooms.</p>
- </html>",  revisions="<html>
- <ul>
- <li>
- September 6, 2021, by Ettore Zanetti:<br/>
- Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
- </li>
- <li>
- April 15, 2020, by Katharina Brinkmann:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This example shows the application of
+<a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.FourElements\">
+AixLib.ThermalZones.ReducedOrder.RC.FourElements</a>
+considering a trace substance such as CO2
+in combination with
+<a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
+AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
+and
+<a href=\"modelica://AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
+AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
+Solar radiation on tilted surface is calculated using models of
+AixLib. The thermal zone is a simple room defined in Guideline
+VDI 6007 Part 1 (VDI, 2012).
+The trace substance calculation is based on the CO2 emissions of 2 persons.
+They stay in the thermal zone for 12 hours every 24 hours. The air exchange rate is 2 air changes per hour.
+All further models, parameters and inputs
+except sunblinds, separate handling of heat transfer through
+windows, no wall element for internal walls and solar radiation
+are similar to the ones defined for the guideline&apos;s test
+room. For solar radiation, the example relies on the standard
+weather file in AixLib.
+</p>
+<p>
+The idea of the example is to show a typical application of all
+sub-models and to use the example in unit tests. The results are
+reasonable, but not related to any real use case or measurement
+data.
+</p>
+<h4>References</h4>
+<p>VDI. German Association of Engineers Guideline VDI 6007-1
+March 2012. Calculation of transient thermal response of rooms
+and buildings - modelling of rooms.</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+September 6, 2021, by Ettore Zanetti:<br/>
+Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+</li>
+<li>
+April 15, 2020, by Katharina Brinkmann:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(Tolerance=1e-6, StopTime=604800),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomFourElementsTraceSubstance.mos"
         "Simulate and plot"),
     Diagram(coordinateSystem(extent={{-100,-120},{100,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SimpleRoomFourElementsTraceSubstance;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomOneElement.mo b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomOneElement.mo
index 18a05f1166..5be60f2b19 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomOneElement.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomOneElement.mo
@@ -87,7 +87,7 @@ model SimpleRoomOneElement
         86400,0,0,0],
     columns={2,3,4},
     extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic) "Table with profiles for persons (radiative and convective) and machines
-     (convective)"
+    (convective)"
     annotation (Placement(transformation(extent={{6,-60},{22,-44}})));
   Modelica.Blocks.Sources.Constant const[2](each k=0)
     "Sets sunblind signal to zero (open)"
@@ -225,57 +225,57 @@ equation
     annotation (Line(points={{27,64},{34,64},{40,64},{40,31},{43,31}}, color={0,
     0,127}));
   annotation ( Documentation(info="<html>
-   <p>This example shows the application of
-   <a href=\"AixLib.ThermalZones.ReducedOrder.RC.OneElement\">
-   AixLib.ThermalZones.ReducedOrder.RC.OneElement</a>
-   in combination with
-   <a href=\"AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
-  AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
-   and
-   <a href=\"AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
-   AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
-   Solar radiation on tilted surface is calculated using models of
-   AixLib. The thermal zone is a simple room defined in Guideline
-   VDI 6007 Part 1 (VDI, 2012). All models, parameters and inputs
-   except sunblinds, separate handling of heat transfer through
-   windows, no wall element for internal walls and solar radiation
-   are similar to the ones defined for the guideline&apos;s test
-   room. For solar radiation, the example relies on the standard
-   weather file in AixLib.</p>
-   <p>The idea of the example is to show a typical application of all
-   sub-models and to use the example in unit tests. The results are
-   reasonable, but not related to any real use case or measurement
-   data.</p>
-   <h4>References</h4>
-   <p>VDI. German Association of Engineers Guideline VDI 6007-1
-   March 2012. Calculation of transient thermal response of rooms
-   and buildings - modelling of rooms.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   September 6, 2021, by Ettore Zanetti:<br/>
-   Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
-   This is for
-   <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
-   </li>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>,
-   <code>alphaWin</code> to <code>hConWin</code>
-   </li>
-   <li>
-   April 27, 2016, by Michael Wetter:<br/>
-   Removed call to <code>Modelica.Utilities.Files.loadResource</code>
-   as this did not work for the regression tests.
-   </li>
-   <li>February 25, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
+  <p>This example shows the application of
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.OneElement\">
+  AixLib.ThermalZones.ReducedOrder.RC.OneElement</a>
+  in combination with
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
+ AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
+  and
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
+  AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
+  Solar radiation on tilted surface is calculated using models of
+  AixLib. The thermal zone is a simple room defined in Guideline
+  VDI 6007 Part 1 (VDI, 2012). All models, parameters and inputs
+  except sunblinds, separate handling of heat transfer through
+  windows, no wall element for internal walls and solar radiation
+  are similar to the ones defined for the guideline&apos;s test
+  room. For solar radiation, the example relies on the standard
+  weather file in AixLib.</p>
+  <p>The idea of the example is to show a typical application of all
+  sub-models and to use the example in unit tests. The results are
+  reasonable, but not related to any real use case or measurement
+  data.</p>
+  <h4>References</h4>
+  <p>VDI. German Association of Engineers Guideline VDI 6007-1
+  March 2012. Calculation of transient thermal response of rooms
+  and buildings - modelling of rooms.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  September 6, 2021, by Ettore Zanetti:<br/>
+  Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+  This is for
+  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+  </li>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>,
+  <code>alphaWin</code> to <code>hConWin</code>
+  </li>
+  <li>
+  April 27, 2016, by Michael Wetter:<br/>
+  Removed call to <code>Modelica.Utilities.Files.loadResource</code>
+  as this did not work for the regression tests.
+  </li>
+  <li>February 25, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),
   experiment(Tolerance=1e-6, StopTime=3.1536e+007, Interval=3600),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomOneElement.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SimpleRoomOneElement;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomThreeElements.mo b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomThreeElements.mo
index c82964d1c9..68bc276987 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomThreeElements.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomThreeElements.mo
@@ -100,7 +100,7 @@ model SimpleRoomThreeElements
         86400,0,0,0],
     columns={2,3,4},
     extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic) "Table with profiles for persons (radiative and convective) and machines
-     (convective)"
+    (convective)"
     annotation (Placement(transformation(extent={{6,-60},{22,-44}})));
   Modelica.Blocks.Sources.Constant const[2](each k=0)
     "Sets sunblind signal to zero (open)"
@@ -255,57 +255,57 @@ equation
   connect(corGDouPan.solarRadWinTrans, thermalZoneThreeElements.solRad)
     annotation (Line(points={{27,64},{40,64},{40,31},{43,31}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>This example shows the application of
-   <a href=\"AixLib.ThermalZones.ReducedOrder.RC.ThreeElements\">
-   AixLib.ThermalZones.ReducedOrder.RC.ThreeElements</a>
-   in combination with
-   <a href=\"AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
-   AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
-   and
-   <a href=\"AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
-   AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
-   Solar radiation on tilted surface is calculated using models of
-   AixLib. The thermal zone is a simple room defined in Guideline
-   VDI 6007 Part 1 (VDI, 2012). All models, parameters and inputs
-   except sunblinds, separate handling of heat transfer through
-   windows, an extra wall element for ground floor (with additional
-   area) and solar radiation are similar to the ones defined for the
-   guideline&apos;s test room. For solar radiation, the example
-   relies on the standard weather file in AixLib.</p>
-   <p>The idea of the example is to show a typical application of
-   all sub-models and to use the example in unit tests. The results
-   are reasonable, but not related to any real use case or
-   measurement data.</p>
-   <h4>References</h4>
-   <p>VDI. German Association of Engineers Guideline VDI 6007-1 March
-   2012. Calculation of transient thermal response of rooms and
-   buildings - modelling of rooms.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   September 6, 2021, by Ettore Zanetti:<br/>
-   Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
-   This is for
-   <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
-   </li>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>,
-   <code>alphaWin</code> to <code>hConWin</code>
-   </li>
-   <li>
-   April 27, 2016, by Michael Wetter:<br/>
-   Removed call to <code>Modelica.Utilities.Files.loadResource</code>
-   as this did not work for the regression tests.
-   </li>
-   <li>February 25, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
+  <p>This example shows the application of
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.ThreeElements\">
+  AixLib.ThermalZones.ReducedOrder.RC.ThreeElements</a>
+  in combination with
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
+  AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
+  and
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
+  AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
+  Solar radiation on tilted surface is calculated using models of
+  AixLib. The thermal zone is a simple room defined in Guideline
+  VDI 6007 Part 1 (VDI, 2012). All models, parameters and inputs
+  except sunblinds, separate handling of heat transfer through
+  windows, an extra wall element for ground floor (with additional
+  area) and solar radiation are similar to the ones defined for the
+  guideline&apos;s test room. For solar radiation, the example
+  relies on the standard weather file in AixLib.</p>
+  <p>The idea of the example is to show a typical application of
+  all sub-models and to use the example in unit tests. The results
+  are reasonable, but not related to any real use case or
+  measurement data.</p>
+  <h4>References</h4>
+  <p>VDI. German Association of Engineers Guideline VDI 6007-1 March
+  2012. Calculation of transient thermal response of rooms and
+  buildings - modelling of rooms.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  September 6, 2021, by Ettore Zanetti:<br/>
+  Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+  This is for
+  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+  </li>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>,
+  <code>alphaWin</code> to <code>hConWin</code>
+  </li>
+  <li>
+  April 27, 2016, by Michael Wetter:<br/>
+  Removed call to <code>Modelica.Utilities.Files.loadResource</code>
+  as this did not work for the regression tests.
+  </li>
+  <li>February 25, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),
   experiment(Tolerance=1e-6, StopTime=3.1536e+007, Interval=3600),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomThreeElements.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SimpleRoomThreeElements;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElements.mo b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElements.mo
index 1a91f2b034..81f839f846 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElements.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElements.mo
@@ -93,7 +93,7 @@ model SimpleRoomTwoElements
         86400,0,0,0],
     columns={2,3,4},
     extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic) "Table with profiles for persons (radiative and convective) and machines
-     (convective)"
+    (convective)"
     annotation (Placement(transformation(extent={{6,-60},{22,-44}})));
   Modelica.Blocks.Sources.Constant const[2](each k=0)
     "Sets sunblind signal to zero (open)"
@@ -231,56 +231,56 @@ equation
     annotation (Line(points={{27,64},{34,64},{40,64},{40,31},{43,31}}, color={0,
     0,127}));
   annotation ( Documentation(info="<html>
-   <p>This example shows the application of
-   <a href=\"AixLib.ThermalZones.ReducedOrder.RC.TwoElements\">
-   AixLib.ThermalZones.ReducedOrder.RC.TwoElements</a>
-   in combination with
-   <a href=\"AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
-  AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
-   and
-   <a href=\"AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
-   AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
-   Solar radiation on tilted surface is calculated using models of
-   AixLib. The thermal zone is a simple room defined in Guideline
-   VDI 6007 Part 1 (VDI, 2012). All models, parameters and inputs
-   except sunblinds, separate handling of heat transfer through
-   windows and solar radiation are similar to the ones defined for
-   the guideline&apos;s test room. For solar radiation, the example
-   relies on the standard weather file in AixLib.</p>
-   <p>The idea of the example is to show a typical application of
-   all sub-models and to use the example in unit tests. The results
-   are reasonable, but not related to any real use case or
-   measurement data.</p>
-   <h4>References</h4>
-   <p>VDI. German Association of Engineers Guideline VDI
-   6007-1 March 2012. Calculation of transient thermal response of
-   rooms and buildings - modelling of rooms.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   September 6, 2021, by Ettore Zanetti:<br/>
-   Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
-   This is for
-   <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
-   </li>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>,
-   <code>alphaWin</code> to <code>hConWin</code>
-   </li>
-   <li>
-   April 27, 2016, by Michael Wetter:<br/>
-   Removed call to <code>Modelica.Utilities.Files.loadResource</code>
-   as this did not work for the regression tests.
-   </li>
-   <li>February 25, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
+  <p>This example shows the application of
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.TwoElements\">
+  AixLib.ThermalZones.ReducedOrder.RC.TwoElements</a>
+  in combination with
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
+ AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>
+  and
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane\">
+  AixLib.ThermalZones.ReducedOrder.SolarGain.CorrectionGDoublePane</a>.
+  Solar radiation on tilted surface is calculated using models of
+  AixLib. The thermal zone is a simple room defined in Guideline
+  VDI 6007 Part 1 (VDI, 2012). All models, parameters and inputs
+  except sunblinds, separate handling of heat transfer through
+  windows and solar radiation are similar to the ones defined for
+  the guideline&apos;s test room. For solar radiation, the example
+  relies on the standard weather file in AixLib.</p>
+  <p>The idea of the example is to show a typical application of
+  all sub-models and to use the example in unit tests. The results
+  are reasonable, but not related to any real use case or
+  measurement data.</p>
+  <h4>References</h4>
+  <p>VDI. German Association of Engineers Guideline VDI
+  6007-1 March 2012. Calculation of transient thermal response of
+  rooms and buildings - modelling of rooms.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  September 6, 2021, by Ettore Zanetti:<br/>
+  Changed <code>lat</code> from being a parameter to an input from weather bus.<br/>
+  This is for
+  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1477\">IBPSA, #1477</a>.
+  </li>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>,
+  <code>alphaWin</code> to <code>hConWin</code>
+  </li>
+  <li>
+  April 27, 2016, by Michael Wetter:<br/>
+  Removed call to <code>Modelica.Utilities.Files.loadResource</code>
+  as this did not work for the regression tests.
+  </li>
+  <li>February 25, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),
   experiment(Tolerance=1e-6, StopTime=3.1536e+007, Interval=3600),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElements.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SimpleRoomTwoElements;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElementsNonConstantTGround.mo b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElementsNonConstantTGround.mo
new file mode 100644
index 0000000000..833f272dbb
--- /dev/null
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElementsNonConstantTGround.mo
@@ -0,0 +1,62 @@
+within AixLib.ThermalZones.ReducedOrder.Examples;
+model SimpleRoomTwoElementsNonConstantTGround
+  "Illustrates the use of non-constant ground temperature for equivalent air temperature calculation"
+  extends Modelica.Icons.Example;
+  extends AixLib.ThermalZones.ReducedOrder.Examples.SimpleRoomTwoElements(
+    eqAirTemp(
+      wfWall={0.15,0.35},
+      wfGro=0.5,
+      TGroundFromInput=true));
+
+  Modelica.Blocks.Sources.Trapezoid TGro(
+    amplitude(unit="K") = 10,
+    rising(displayUnit="d") = 7884000,
+    width(displayUnit="d") = 7884000,
+    falling(displayUnit="d") = 7884000,
+    period(displayUnit="d") = 31536000,
+    offset(
+      unit="K",
+      displayUnit="degC") = 280.15,
+    startTime(displayUnit="d") = 5184000)
+    "Trapezoid-shaped source for ground temperature"
+    annotation (Placement(transformation(extent={{-60,-60},{-40,-40}})));
+equation
+
+  connect(TGro.y, eqAirTemp.TGro_in)
+    annotation (Line(points={{-39,-50},{-14,-50},{-14,-16}}, color={0,0,127}));
+  annotation ( Documentation(info="<html>
+<p>
+This example shows the application of
+<a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.TwoElements\">
+AixLib.ThermalZones.ReducedOrder.RC.TwoElements</a>
+in connection with equivalent air temperature calculation in
+<a href=\"modelica://AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow\">
+AixLib.ThermalZones.ReducedOrder.EquivalentAirTemperature.VDI6007WithWindow</a>,
+where the ground temperature is not a constant, but has a trapezoid source.
+Apart from that, it is identical to <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.Examples.SimpleRoomTwoElements\">
+AixLib.ThermalZones.ReducedOrder.Examples.SimpleRoomTwoElements</a>.
+<h4>References</h4>
+<p>VDI. German Association of Engineers Guideline VDI 6007-1
+March 2012. Calculation of transient thermal response of rooms
+and buildings - modelling of rooms.</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+June 29, 2023, by Philip Groesdonk:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1744\">IBPSA, #1744</a>.
+</li>
+</ul>
+</html>"),
+  experiment(
+      StopTime=31536000,
+      Interval=3600,
+      Tolerance=1e-06),
+  __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/SimpleRoomTwoElementsNonConstantTGround.mos"
+        "Simulate and plot"),
+    Diagram(coordinateSystem(extent={{-100,-120},{100,100}})),
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end SimpleRoomTwoElementsNonConstantTGround;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZone.mo b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZone.mo
index c6a9bce0bf..5fa735d27c 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZone.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZone.mo
@@ -3,10 +3,7 @@ model ThermalZone "Illustrates the use of ThermalZone"
   extends Modelica.Icons.Example;
 
   AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone thermalZone(
-    zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler(),
-    ROM(extWallRC(thermCapExt(each der_T(fixed=true))), intWallRC(thermCapInt(
-            each der_T(fixed=true)))),
+    redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     redeclare package Medium = Modelica.Media.Air.SimpleAir,
     T_start=293.15,
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneAirExchange.mo b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneAirExchange.mo
index ef81d819e0..d77b478eec 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneAirExchange.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneAirExchange.mo
@@ -4,10 +4,7 @@ model ThermalZoneAirExchange "Illustrates the use of ThermalZoneAirExchange"
 
   AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone thermalZone(
     redeclare package Medium = Modelica.Media.Air.SimpleAir,
-    zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler(),
-    ROM(extWallRC(thermCapExt(each der_T(fixed=true))), intWallRC(thermCapInt(
-            each der_T(fixed=true)))),
+    redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam,
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     T_start=293.15,
     internalGainsMode=1,
@@ -137,7 +134,7 @@ model ThermalZoneAirExchange "Illustrates the use of ThermalZoneAirExchange"
 
 equation
   connect(weaDat.weaBus, thermalZone.weaBus) annotation (Line(
-      points={{-72,30},{-34,30},{-34,0},{-10,0}},
+      points={{-72,30},{-34,30},{-34,6},{-10,6}},
       color={255,204,51},
       thickness=0.5));
   connect(weaDat.weaBus, weaBus) annotation (Line(
@@ -147,8 +144,8 @@ equation
       string="%second",
       index=1,
       extent={{6,3},{6,3}}));
-  connect(thermalZone.ventTemp, weaBus.TDryBul) annotation (Line(points={{-11.3,
-          -3.9},{-35.65,-3.9},{-35.65,-4},{-61,-4}},color={0,0,127}), Text(
+  connect(thermalZone.ventTemp, weaBus.TDryBul) annotation (Line(points={{-9.6,
+          -1.6},{-35.65,-1.6},{-35.65,-4},{-61,-4}},color={0,0,127}), Text(
       string="%second",
       index=1,
       extent={{6,3},{6,3}}));
@@ -178,7 +175,7 @@ equation
         "Simulate and plot"),
     Documentation(info="<html><p>
   This example illustrates the use of <a href=
-  \"AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZoneEquipped\">AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZoneEquipped</a>.
+  \"AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone\">AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone</a>.
   Parameter set for thermal zone is for an office zone of an office
   building build as passive house. All boundary conditions are generic
   to show how to apply different kinds of boundary conditions. The
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAir.mo b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAir.mo
index 0d62851ffd..6750b93e7b 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAir.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAir.mo
@@ -5,16 +5,13 @@ model ThermalZoneMoistAir
 
   AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone thermalZone(
     use_moisture_balance=true,
-    ROM(extWallRC(thermCapExt(each der_T(fixed=true))), intWallRC(thermCapInt(
-            each der_T(fixed=true)))),
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     redeclare package Medium = AixLib.Media.Air,
     internalGainsMode=3,
     recOrSep=true,
     nPorts=2,
     T_start=293.15,
-    zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler())
+    redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam)
     "Thermal zone"
     annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
   AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
@@ -143,7 +140,7 @@ model ThermalZoneMoistAir
     annotation (Placement(transformation(extent={{-12,-86},{-32,-66}})));
 equation
   connect(weaDat.weaBus, thermalZone.weaBus) annotation (Line(
-      points={{-72,30},{-34,30},{-34,0},{-10,0}},
+      points={{-72,30},{-34,30},{-34,6},{-10,6}},
       color={255,204,51},
       thickness=0.5));
   connect(internalGains.y, thermalZone.intGains)
@@ -181,7 +178,7 @@ equation
 </html>", info="<html>
 <p>
   This example illustrates the use of <a href=
-  \"AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZoneMoistAir\">AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZoneMoistAir</a>.
+  \"AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone\">AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone</a>.
   Parameter set for thermal zone is for an office zone of an office
   building build as passive house. All boundary conditions are generic
   to show how to apply different kinds of boundary conditions. The
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAirSwimmingPool.mo b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAirSwimmingPool.mo
new file mode 100644
index 0000000000..563e93236c
--- /dev/null
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAirSwimmingPool.mo
@@ -0,0 +1,210 @@
+within AixLib.ThermalZones.ReducedOrder.Examples;
+model ThermalZoneMoistAirSwimmingPool
+  "Illustrates the use of ThermalZoneMoistAirSwimmingPool"
+  extends Modelica.Icons.Example;
+
+  AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone thermalZone(
+    use_pools=true,
+    use_moisture_balance=true,
+    energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
+    redeclare package Medium = AixLib.Media.Air,
+    internalGainsMode=3,
+    recOrSep=true,
+    nPools=2,
+    poolParam={DataBase.Pools.SportPool(),DataBase.Pools.ChildrensPool()},
+    poolWallParam={
+        DataBase.Pools.SwimmingPoolWalls.ConcreteInsulationConstruction(),
+        DataBase.Pools.SwimmingPoolWalls.ConcreteInsulationConstruction()},
+    nPorts=2,
+    T_start=293.15,
+    redeclare AixLib.DataBase.ThermalZones.SwimmingFacility.SwimmingHall
+      zoneParam(HeaterOn=true)) "Thermal zone"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+
+  AixLib.BoundaryConditions.WeatherData.ReaderTMY3 weaDat(
+    calTSky=AixLib.BoundaryConditions.Types.SkyTemperatureCalculation.HorizontalRadiation,
+    computeWetBulbTemperature=false,
+    filNam=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/weatherdata/USA_CA_San.Francisco.Intl.AP.724940_TMY3.mos"))
+    "Weather data reader"
+    annotation (Placement(transformation(extent={{-92,20},{-72,40}})));
+  Modelica.Blocks.Sources.CombiTimeTable internalGains(
+    extrapolation = Modelica.Blocks.Types.Extrapolation.Periodic,
+    tableName="Internals",
+    fileName=ModelicaServices.ExternalReferences.loadResource(
+        "modelica://AixLib/Resources/LowOrder_ExampleData/InternalGains_SwimmingFacility_6Zones.txt"),
+    columns = {2, 3, 4},
+    tableOnFile=true,
+    table=[0,0,0.1,0,0; 3540,0,0.1,0,0; 3600,0,0.1,0,0; 7140,0,0.1,0,0; 7200,0,
+        0.1,0,0; 10740,0,0.1,0,0; 10800,0,0.1,0,0; 14340,0,0.1,0,0; 14400,0,0.1,
+        0,0; 17940,0,0.1,0,0; 18000,0,0.1,0,0; 21540,0,0.1,0,0; 21600,0,0.1,0,0;
+        25140,0,0.1,0,0; 25200,0,0.1,0,0; 28740,0,0.1,0,0; 28800,0,0.1,0,0;
+        32340,0,0.1,0,0; 32400,0.6,0.6,1,1; 35940,0.6,0.6,1,1; 36000,1,1,1,1;
+        39540,1,1,1,1; 39600,0.4,0.4,1,1; 43140,0.4,0.4,1,1; 43200,0,0.1,0,0;
+        46740,0,0.1,0,0; 46800,0,0.1,0,0; 50340,0,0.1,0,0; 50400,0.6,0.6,1,1;
+        53940,0.6,0.6,1,1; 54000,1,1,1,1; 57540,1,1,1,1; 57600,0.4,0.4,1,1;
+        61140,0.4,0.4,1,1; 61200,0,0.1,0,0; 64740,0,0.1,0,0; 64800,0,0.1,0,0;
+        68340,0,0.1,0,0; 68400,0,0.1,0,0; 71940,0,0.1,0,0; 72000,0,0.1,0,0;
+        75540,0,0.1,0,0; 75600,0,0.1,0,0; 79140,0,0.1,0,0; 79200,0,0.1,0,0;
+        82740,0,0.1,0,0; 82800,0,0.1,0,0; 86340,0,0.1,0,0; 86400,0,0.1,0,0;
+        89940,0,0.1,0,0; 90000,0,0.1,0,0; 93540,0,0.1,0,0; 93600,0,0.1,0,0;
+        97140,0,0.1,0,0; 97200,0,0.1,0,0; 100740,0,0.1,0,0; 100800,0,0.1,0,0;
+        104340,0,0.1,0,0; 104400,0,0.1,0,0; 107940,0,0.1,0,0; 108000,0,0.1,0,0;
+        111540,0,0.1,0,0; 111600,0,0.1,0,0; 115140,0,0.1,0,0; 115200,0,0.1,0,0;
+        118740,0,0.1,0,0; 118800,0.6,0.6,1,1; 122340,0.6,0.6,1,1; 122400,1,1,1,
+        1; 125940,1,1,1,1; 126000,0.4,0.4,1,1; 129540,0.4,0.4,1,1; 129600,0,0.1,
+        0,0; 133140,0,0.1,0,0; 133200,0,0.1,0,0; 136740,0,0.1,0,0; 136800,0.6,
+        0.6,1,1; 140340,0.6,0.6,1,1; 140400,1,1,1,1; 143940,1,1,1,1; 144000,0.4,
+        0.4,1,1; 147540,0.4,0.4,1,1; 147600,0,0.1,0,0; 151140,0,0.1,0,0; 151200,
+        0,0.1,0,0; 154740,0,0.1,0,0; 154800,0,0.1,0,0; 158340,0,0.1,0,0; 158400,
+        0,0.1,0,0; 161940,0,0.1,0,0; 162000,0,0.1,0,0; 165540,0,0.1,0,0; 165600,
+        0,0.1,0,0; 169140,0,0.1,0,0; 169200,0,0.1,0,0; 172740,0,0.1,0,0; 172800,
+        0,0.1,0,0; 176340,0,0.1,0,0; 176400,0,0.1,0,0; 179940,0,0.1,0,0; 180000,
+        0,0.1,0,0; 183540,0,0.1,0,0; 183600,0,0.1,0,0; 187140,0,0.1,0,0; 187200,
+        0,0.1,0,0; 190740,0,0.1,0,0; 190800,0,0.1,0,0; 194340,0,0.1,0,0; 194400,
+        0,0.1,0,0; 197940,0,0.1,0,0; 198000,0,0.1,0,0; 201540,0,0.1,0,0; 201600,
+        0,0.1,0,0; 205140,0,0.1,0,0; 205200,0.6,0.6,1,1; 208740,0.6,0.6,1,1;
+        208800,1,1,1,1; 212340,1,1,1,1; 212400,0.4,0.4,1,1; 215940,0.4,0.4,1,1;
+        216000,0,0.1,0,0; 219540,0,0.1,0,0; 219600,0,0.1,0,0; 223140,0,0.1,0,0;
+        223200,0.6,0.6,1,1; 226740,0.6,0.6,1,1; 226800,1,1,1,1; 230340,1,1,1,1;
+        230400,0.4,0.4,1,1; 233940,0.4,0.4,1,1; 234000,0,0.1,0,0; 237540,0,0.1,
+        0,0; 237600,0,0.1,0,0; 241140,0,0.1,0,0; 241200,0,0.1,0,0; 244740,0,0.1,
+        0,0; 244800,0,0.1,0,0; 248340,0,0.1,0,0; 248400,0,0.1,0,0; 251940,0,0.1,
+        0,0; 252000,0,0.1,0,0; 255540,0,0.1,0,0; 255600,0,0.1,0,0; 259140,0,0.1,
+        0,0; 259200,0,0.1,0,0; 262740,0,0.1,0,0; 262800,0,0.1,0,0; 266340,0,0.1,
+        0,0; 266400,0,0.1,0,0; 269940,0,0.1,0,0; 270000,0,0.1,0,0; 273540,0,0.1,
+        0,0; 273600,0,0.1,0,0; 277140,0,0.1,0,0; 277200,0,0.1,0,0; 280740,0,0.1,
+        0,0; 280800,0,0.1,0,0; 284340,0,0.1,0,0; 284400,0,0.1,0,0; 287940,0,0.1,
+        0,0; 288000,0,0.1,0,0; 291540,0,0.1,0,0; 291600,0.6,0.6,1,1; 295140,0.6,
+        0.6,1,1; 295200,1,1,1,1; 298740,1,1,1,1; 298800,0.4,0.4,1,1; 302340,0.4,
+        0.4,1,1; 302400,0,0.1,0,0; 305940,0,0.1,0,0; 306000,0,0.1,0,0; 309540,0,
+        0.1,0,0; 309600,0.6,0.6,1,1; 313140,0.6,0.6,1,1; 313200,1,1,1,1; 316740,
+        1,1,1,1; 316800,0.4,0.4,1,1; 320340,0.4,0.4,1,1; 320400,0,0.1,0,0;
+        323940,0,0.1,0,0; 324000,0,0.1,0,0; 327540,0,0.1,0,0; 327600,0,0.1,0,0;
+        331140,0,0.1,0,0; 331200,0,0.1,0,0; 334740,0,0.1,0,0; 334800,0,0.1,0,0;
+        338340,0,0.1,0,0; 338400,0,0.1,0,0; 341940,0,0.1,0,0; 342000,0,0.1,0,0;
+        345540,0,0.1,0,0; 345600,0,0.1,0,0; 349140,0,0.1,0,0; 349200,0,0.1,0,0;
+        352740,0,0.1,0,0; 352800,0,0.1,0,0; 356340,0,0.1,0,0; 356400,0,0.1,0,0;
+        359940,0,0.1,0,0; 360000,0,0.1,0,0; 363540,0,0.1,0,0; 363600,0,0.1,0,0;
+        367140,0,0.1,0,0; 367200,0,0.1,0,0; 370740,0,0.1,0,0; 370800,0,0.1,0,0;
+        374340,0,0.1,0,0; 374400,0,0.1,0,0; 377940,0,0.1,0,0; 378000,0.6,0.6,1,
+        1; 381540,0.6,0.6,1,1; 381600,1,1,1,1; 385140,1,1,1,1; 385200,0.4,0.4,1,
+        1; 388740,0.4,0.4,1,1; 388800,0,0.1,0,0; 392340,0,0.1,0,0; 392400,0,0.1,
+        0,0; 395940,0,0.1,0,0; 396000,0.6,0.6,1,1; 399540,0.6,0.6,1,1; 399600,1,
+        1,1,1; 403140,1,1,1,1; 403200,0.4,0.4,1,1; 406740,0.4,0.4,1,1; 406800,0,
+        0.1,0,0; 410340,0,0.1,0,0; 410400,0,0.1,0,0; 413940,0,0.1,0,0; 414000,0,
+        0.1,0,0; 417540,0,0.1,0,0; 417600,0,0.1,0,0; 421140,0,0.1,0,0; 421200,0,
+        0.1,0,0; 424740,0,0.1,0,0; 424800,0,0.1,0,0; 428340,0,0.1,0,0; 428400,0,
+        0.1,0,0; 431940,0,0.1,0,0; 432000,0,0,0,0; 435540,0,0,0,0; 435600,0,0,0,
+        0; 439140,0,0,0,0; 439200,0,0,0,0; 442740,0,0,0,0; 442800,0,0,0,0;
+        446340,0,0,0,0; 446400,0,0,0,0; 449940,0,0,0,0; 450000,0,0,0,0; 453540,
+        0,0,0,0; 453600,0,0,0,0; 457140,0,0,0,0; 457200,0,0,0,0; 460740,0,0,0,0;
+        460800,0,0,0,0; 464340,0,0,0,0; 464400,0,0,0,0; 467940,0,0,0,0; 468000,
+        0,0,0,0; 471540,0,0,0,0; 471600,0,0,0,0; 475140,0,0,0,0; 475200,0,0,0,0;
+        478740,0,0,0,0; 478800,0,0,0,0; 482340,0,0,0,0; 482400,0,0,0,0; 485940,
+        0,0,0,0; 486000,0,0,0,0; 489540,0,0,0,0; 489600,0,0,0,0; 493140,0,0,0,0;
+        493200,0,0,0,0; 496740,0,0,0,0; 496800,0,0,0,0; 500340,0,0,0,0; 500400,
+        0,0,0,0; 503940,0,0,0,0; 504000,0,0,0,0; 507540,0,0,0,0; 507600,0,0,0,0;
+        511140,0,0,0,0; 511200,0,0,0,0; 514740,0,0,0,0; 514800,0,0,0,0; 518340,
+        0,0,0,0; 518400,0,0,0,0; 521940,0,0,0,0; 522000,0,0,0,0; 525540,0,0,0,0;
+        525600,0,0,0,0; 529140,0,0,0,0; 529200,0,0,0,0; 532740,0,0,0,0; 532800,
+        0,0,0,0; 536340,0,0,0,0; 536400,0,0,0,0; 539940,0,0,0,0; 540000,0,0,0,0;
+        543540,0,0,0,0; 543600,0,0,0,0; 547140,0,0,0,0; 547200,0,0,0,0; 550740,
+        0,0,0,0; 550800,0,0,0,0; 554340,0,0,0,0; 554400,0,0,0,0; 557940,0,0,0,0;
+        558000,0,0,0,0; 561540,0,0,0,0; 561600,0,0,0,0; 565140,0,0,0,0; 565200,
+        0,0,0,0; 568740,0,0,0,0; 568800,0,0,0,0; 572340,0,0,0,0; 572400,0,0,0,0;
+        575940,0,0,0,0; 576000,0,0,0,0; 579540,0,0,0,0; 579600,0,0,0,0; 583140,
+        0,0,0,0; 583200,0,0,0,0; 586740,0,0,0,0; 586800,0,0,0,0; 590340,0,0,0,0;
+        590400,0,0,0,0; 593940,0,0,0,0; 594000,0,0,0,0; 597540,0,0,0,0; 597600,
+        0,0,0,0; 601140,0,0,0,0; 601200,0,0,0,0; 604740,0,0,0,0])
+    "Table with profiles for internal gains"
+    annotation(Placement(transformation(extent={{-14,-59},{0,-45}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow prescribedHeatFlow
+    "Radiative heat flow of additional internal gains"
+    annotation (Placement(transformation(extent={{46,-10},{26,10}})));
+  Modelica.Blocks.Sources.Sine sine(
+    amplitude=500,
+    f=1/86400,
+    offset=500) "Sinusoidal excitation for additional internal gains"
+    annotation (Placement(transformation(extent={{94,-10},{74,10}})));
+  Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow prescribedHeatFlow1
+    "Convective heat flow of additional internal gains"
+    annotation (Placement(transformation(extent={{46,-28},{26,-8}})));
+  Modelica.Blocks.Math.Gain gain(k=0.5)
+    "Split additional internal gains into radiative an convective"
+    annotation (Placement(transformation(extent={{66,-6},{54,6}})));
+  Modelica.Blocks.Math.Gain gain1(k=0.5)
+    "Split additional internal gains into radiative an convective"
+    annotation (Placement(transformation(extent={{66,-24},{54,-12}})));
+
+  AixLib.Fluid.Sources.MassFlowSource_T sourcAir(
+    redeclare package Medium = AixLib.Media.Air,
+    m_flow=3000/3600*1.17,
+    X={0.004,1 - 0.004},
+    T=283.15,
+    nPorts=1) "mass flow rate of air into thermal zone"
+    annotation (Placement(transformation(extent={{-84,-80},{-64,-60}})));
+  AixLib.Fluid.Sources.Boundary_pT sinAir(redeclare package Medium =
+        AixLib.Media.Air,
+      nPorts=1) "sink of air"
+    annotation (Placement(transformation(extent={{-12,-86},{-32,-66}})));
+  Modelica.Blocks.Sources.CombiTimeTable tableOpeningHours(
+    tableOnFile=true,
+    extrapolation=Modelica.Blocks.Types.Extrapolation.Periodic,
+    tableName="openingHours",
+    columns=2:2,
+    fileName=ModelicaServices.ExternalReferences.loadResource(
+        "modelica://AixLib/Resources/LowOrder_ExampleData/OpeningHours_SwimmingFacility.txt"))
+    "Boundary condition: Opening Hours of swiming pools"
+    annotation (Placement(transformation(extent={{-92,-34},{-76,-18}})));
+  Modelica.Blocks.Sources.Constant
+                               const(k=273.15 + 30)
+                "Sinusoidal excitation for additional internal gains"
+    annotation (Placement(transformation(extent={{-70,2},{-58,14}})));
+equation
+  connect(weaDat.weaBus, thermalZone.weaBus) annotation (Line(
+      points={{-72,30},{-34,30},{-34,6},{-10,6}},
+      color={255,204,51},
+      thickness=0.5));
+  connect(internalGains.y, thermalZone.intGains)
+    annotation (Line(points={{0.7,-52},{8,-52},{8,-8.4}}, color={0,0,127}));
+  connect(prescribedHeatFlow.port, thermalZone.intGainsRad)
+    annotation (Line(points={{26,0},{10.2,0},{10.2,3.4}},
+                                                     color={191,0,0}));
+  connect(prescribedHeatFlow1.port, thermalZone.intGainsConv) annotation (Line(
+        points={{26,-18},{18,-18},{18,0.4},{10.2,0.4}},
+                                                    color={191,0,0}));
+  connect(gain1.y, prescribedHeatFlow1.Q_flow)
+    annotation (Line(points={{53.4,-18},{46,-18}},          color={0,0,127}));
+  connect(gain.y, prescribedHeatFlow.Q_flow)
+    annotation (Line(points={{53.4,0},{49.7,0},{46,0}}, color={0,0,127}));
+  connect(sine.y, gain.u)
+    annotation (Line(points={{73,0},{67.2,0}},          color={0,0,127}));
+  connect(sine.y, gain1.u) annotation (Line(points={{73,0},{70,0},{70,-18},{67.2,
+          -18}}, color={0,0,127}));
+  connect(sourcAir.ports[1], thermalZone.ports[1]) annotation (Line(points={{-64,-70},
+          {-46,-70},{-46,-36},{-1.175,-36},{-1.175,-7.2}},        color={0,127,
+          255}));
+  connect(thermalZone.ports[2], sinAir.ports[1]) annotation (Line(points={{1.175,
+          -7.2},{1.175,-40},{-38,-40},{-38,-76},{-32,-76}},color={0,127,255}));
+  connect(tableOpeningHours.y[1],thermalZone.timeOpe)
+      annotation (Line(points={{-75.2,-26},{-7,-26},{-7,-8.4}},
+                                                            color={0,0,127}));
+  connect(const.y, thermalZone.TSetHeat) annotation (Line(points={{-57.4,8},{-50,
+          8},{-50,1.2},{-9.6,1.2}}, color={0,0,127}));
+  annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)),
+    experiment(Tolerance=1e-6,StopTime=3.1536e+007,Interval=3600),
+        __Dymola_Commands(file=
+  "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistAirSwimmingPool.mos"
+        "Simulate and plot"),
+    Documentation(info="<html>
+    <p><span style=\"font-family: Arial;\">This example illustrates the use of
+    <a href=
+    \"AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone\">AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone</a>. 
+    Parameter set for thermal zone is for a swimming hall of a swimming 
+    facility including two swimming pools. All boundary conditions are generic 
+    to show how to apply different kinds of boundary conditions. The results 
+    should show a typical profile for indoor air temperatures, but are not 
+    related to a specific building or measurement data.</span></p>
+</html>"));
+end ThermalZoneMoistAirSwimmingPool;
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistCO2AirExchange.mo b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistCO2AirExchange.mo
index 769ca184b0..f9eb11be5d 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistCO2AirExchange.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/ThermalZoneMoistCO2AirExchange.mo
@@ -6,13 +6,10 @@ model ThermalZoneMoistCO2AirExchange
 
   AixLib.ThermalZones.ReducedOrder.ThermalZone.ThermalZone thermalZone(
     use_moisture_balance=true,
-    ROM(extWallRC(thermCapExt(each der_T(fixed=true))), intWallRC(thermCapInt(
-            each der_T(fixed=true)))),
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     redeclare package Medium = Medium,
     T_start=293.15,
-    zoneParam=
-        DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler(),
+    redeclare AixLib.DataBase.ThermalZones.OfficePassiveHouse.OPH_1_OfficeNoHeaterCooler zoneParam,
     internalGainsMode=3,
     recOrSep=true,
     use_C_flow=true,
diff --git a/AixLib/ThermalZones/ReducedOrder/Examples/package.order b/AixLib/ThermalZones/ReducedOrder/Examples/package.order
index 6d0da8eadc..f02dec5a26 100644
--- a/AixLib/ThermalZones/ReducedOrder/Examples/package.order
+++ b/AixLib/ThermalZones/ReducedOrder/Examples/package.order
@@ -3,13 +3,16 @@ Multizone
 MultizoneEquipped
 MultizoneMoistAirCO2
 MultizoneMoistAirCO2Equipped
+MultizoneMoistAirCO2EquippedSwimmingFacility
 MultizonePartlyCooled
 SimpleRoomFourElements
 SimpleRoomFourElementsTraceSubstance
 SimpleRoomOneElement
 SimpleRoomThreeElements
 SimpleRoomTwoElements
+SimpleRoomTwoElementsNonConstantTGround
 ThermalZone
 ThermalZoneAirExchange
 ThermalZoneMoistAir
+ThermalZoneMoistAirSwimmingPool
 ThermalZoneMoistCO2AirExchange
diff --git a/AixLib/ThermalZones/ReducedOrder/Multizone/BaseClasses/MultizonePostProcessing.mo b/AixLib/ThermalZones/ReducedOrder/Multizone/BaseClasses/MultizonePostProcessing.mo
index e41c46612a..9d8f651174 100644
--- a/AixLib/ThermalZones/ReducedOrder/Multizone/BaseClasses/MultizonePostProcessing.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Multizone/BaseClasses/MultizonePostProcessing.mo
@@ -172,17 +172,17 @@ model MultizonePostProcessing
     each final quantity="Energy",
     each final unit="J",
     each displayUnit="kWh")
-    "Heat gains based on internal gains for each zone from persons, machines, and light"
+    "Heat gains based on internal gains for each zone from lights[1], machines[2], and persons[3]"
     annotation (Placement(transformation(extent={{100,-122},{120,-102}}),
         iconTransformation(extent={{100,-130},{120,-110}})));
   Modelica.Blocks.Interfaces.RealInput QIntGains_flow[numZones,3](each final
       quantity="HeatFlowRate", each final unit="W")
-    "Heat flow based on internal gains for each zone from persons, machines, and light"
+    "Heat flow based on internal gains for each zone from lights[1], machines[2], and persons[3]"
                                                                  annotation (
       Placement(transformation(extent={{-140,-140},{-100,-100}}),
         iconTransformation(extent={{-140,-140},{-100,-100}})));
   Modelica.Blocks.Continuous.Integrator QIntGainCalc[numZones,3]
-    "Heat gain based on internal gains for each zone from persons, machines, and light"
+    "Heat gain based on internal gains for each zone from lights[1], machines[2], and persons[3]"
     annotation (Placement(transformation(extent={{58,-124},{74,-108}})));
 equation
   connect(TAirAverageCalc.u, TAir) annotation (Line(points={{56.4,96},{56.4,100},
diff --git a/AixLib/ThermalZones/ReducedOrder/Multizone/BaseClasses/PartialMultizone.mo b/AixLib/ThermalZones/ReducedOrder/Multizone/BaseClasses/PartialMultizone.mo
index 91e69cfea0..d3da1421cf 100644
--- a/AixLib/ThermalZones/ReducedOrder/Multizone/BaseClasses/PartialMultizone.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Multizone/BaseClasses/PartialMultizone.mo
@@ -12,12 +12,14 @@ partial model PartialMultizone "Partial model for multizone models"
     "Total surface area of building walls and windows (including interior walls)";
   parameter Integer numZones(min=1)
     "Number of zones";
-  parameter AixLib.DataBase.ThermalZones.ZoneBaseRecord zoneParam[:]
+  replaceable parameter AixLib.DataBase.ThermalZones.ZoneBaseRecord zoneParam[numZones]
     "Setup for zones" annotation (choicesAllMatching=false);
-  parameter Integer nPorts=0
-    "Number of fluid ports"
-    annotation(Evaluate=true,
+
+  parameter Integer nPorts = 0
+    "Number of fluid ports"  annotation(Evaluate=true,
     Dialog(connectorSizing=true, tab="General",group="Ports"));
+
+
   parameter Boolean use_MechanicalAirExchange=true
     "Consider mechanical ventilation by setting true";
   parameter Boolean use_NaturalAirExchange=use_MechanicalAirExchange
@@ -54,14 +56,14 @@ partial model PartialMultizone "Partial model for multizone models"
     extent={{-10,-10},{10,10}},
     rotation=90,
     origin={60,-110})));
-  Modelica.Blocks.Interfaces.RealOutput TAir[size(zone, 1)](
+  Modelica.Blocks.Interfaces.RealOutput TAir[numZones](
     each final quantity="ThermodynamicTemperature",
     each final unit="K",
     each displayUnit="degC") if ASurTot > 0 or VAir > 0
     "Indoor air temperature"
     annotation (Placement(transformation(extent={{100,71},{120,91}}),
         iconTransformation(extent={{80,19},{100,40}})));
-  Modelica.Blocks.Interfaces.RealOutput TRad[size(zone, 1)](
+  Modelica.Blocks.Interfaces.RealOutput TRad[numZones](
     each final quantity="ThermodynamicTemperature",
     each final unit="K",
     each displayUnit="degC") if ASurTot > 0
@@ -104,6 +106,7 @@ partial model PartialMultizone "Partial model for multizone models"
     final zoneParam=zoneParam,
     redeclare each final model corG = corG,
     each final internalGainsMode=internalGainsMode,
+    redeclare package MediumPoolWater = MediumPoolWater,
     each final nPorts=nPorts,
     each final energyDynamics=energyDynamics,
     each final massDynamics=massDynamics,
@@ -148,6 +151,14 @@ partial model PartialMultizone "Partial model for multizone models"
       group="Cooler",
       enable=not recOrSep));
 
+
+  //Swimming pool params
+  parameter Boolean use_pools_tot = false "use swimming pools within at least one zone of the multizone" annotation(Dialog(tab="Moisture", group="Pools"));
+  replaceable package MediumPoolWater = Media.Water annotation (choices(choice(redeclare
+          package Medium =
+            AixLib.Media.Water
+              "Water")), Dialog(enable=use_pools_tot,tab="Moisture", group="Pools"));
+
   Modelica.Blocks.Interfaces.RealInput TSetHeat[numZones](
     each final quantity="ThermodynamicTemperature",
     each final unit="K",
@@ -160,6 +171,8 @@ partial model PartialMultizone "Partial model for multizone models"
     extent={{10,-10},{-10,10}},
     rotation=270,
     origin={-52,-110})));
+
+
   Modelica.Blocks.Interfaces.RealInput TSetCool[numZones](
     each final quantity="ThermodynamicTemperature",
     each final unit="K",
@@ -186,9 +199,19 @@ partial model PartialMultizone "Partial model for multizone models"
     extent={{80,-100},{100,-80}})));
   Modelica.Blocks.Interfaces.RealOutput QIntGains_flow[numZones,3](each final
       quantity="HeatFlowRate", each final unit="W") if ASurTot > 0 or VAir > 0
-    "Heat flow based on internal gains for each zone from persons, machines, and light"
+    "Heat flow based on internal gains for each zone from lights[1], machines[2], and persons[3]"
                         annotation (Placement(transformation(extent={{100,-90},{
             120,-70}}), iconTransformation(extent={{80,-100},{100,-80}})));
+  Modelica.Blocks.Interfaces.RealInput timeOpe
+    if use_moisture_balance and use_pools_tot
+    "Input profiles for opening hours for pools" annotation (Placement(
+        transformation(extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={42,-102}),
+        iconTransformation(extent={{-10,-10},{10,10}},
+        rotation=90,
+        origin={38,-110})));
+
 equation
   // if ASurTot or VAir < 0 PHeater and PCooler are set to dummy value zero
   if not (ASurTot > 0 or VAir > 0) then
@@ -235,7 +258,7 @@ equation
 
   for i in 1:numZones loop
     connect(intGains[(i*3) - 2], zone[i].intGains[1]) annotation (Line(
-        points={{76,-100},{76,50.64},{75.8,50.64}},
+        points={{76,-100},{76,51.46},{75.8,51.46}},
         color={0,0,127},
         smooth=Smooth.None));
     connect(intGains[(i*3) - 1], zone[i].intGains[2]);
@@ -247,6 +270,12 @@ equation
       string="%second",
       index=1,
       extent={{6,3},{6,3}}));
+    if zone[i].use_pools then
+      connect(timeOpe,zone[i].timeOpe) annotation (Line(
+        points={{42,-102},{42,52.28},{44.3,52.28}},
+        color={0,0,127},
+        smooth=Smooth.None));
+    end if;
   end for;
   connect(zone.intGainsConv, intGainsConv) annotation (Line(points={{80.42,70.32},
           {86,70.32},{86,-78},{66,-78},{-100,-78},{-100,-70}},
diff --git a/AixLib/ThermalZones/ReducedOrder/Multizone/MultizoneEquipped.mo b/AixLib/ThermalZones/ReducedOrder/Multizone/MultizoneEquipped.mo
index 76f398a74f..e61589a1fd 100644
--- a/AixLib/ThermalZones/ReducedOrder/Multizone/MultizoneEquipped.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Multizone/MultizoneEquipped.mo
@@ -110,7 +110,7 @@ model MultizoneEquipped
     annotation (
     Placement(transformation(extent={{-52,10},{18,40}})));
 
-  Modelica.Blocks.Interfaces.RealOutput CO2Con[size(zone, 1)] if use_C_flow
+  Modelica.Blocks.Interfaces.RealOutput CO2Con[numZones] if use_C_flow
     "CO2 concentration in the thermal zone in ppm"
     annotation (Placement(transformation(extent={{100,10},{120,30}})));
 protected
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/ExteriorWall.mo b/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/ExteriorWall.mo
index 401ddec902..50930ba02a 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/ExteriorWall.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/ExteriorWall.mo
@@ -59,31 +59,31 @@ equation
   annotation(defaultComponentName = "extWalRC",
   Diagram(coordinateSystem(preserveAspectRatio = false, extent=
   {{-100, -100}, {100, 120}})),           Documentation(info="<html>
-   <p><code>ExteriorWall</code> represents heat conduction and heat storage
-   within walls. It links a variable number <code>n</code> of thermal resistances
-   and capacities to a series connection. <code>n</code> thus defines the spatial
-   discretization of thermal effects within the wall. All effects are considered
-   as one-dimensional normal to the wall&apos;s surface. This model is thought
-   for exterior wall elements that contribute to heat transfer to the outdoor.
-   The RC-chain is defined via a vector of capacities <code>CExt[n]</code> and a
-   vector of resistances <code>RExt[n]</code>. Resistances and capacities are
-   connected alternately, starting with the first resistance <code>RExt[1]</code>,
-   from heat <code>port_a</code> to heat <code>port_b</code>. <code>RExtRem</code>
-   is the resistance between the last capacity <code>CExt[end]</code> and the
-   heat <code>port_b</code>.</p>
-   <p align=\"center\"><img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/BaseClasses/ExtMassVarRC/ExtMassVarRC.png\" alt=\"image\"/> </p>
-   </html>", revisions="<html>
-   <ul>
-   <li>
-   April 27, 2016, by Michael Wetter:<br/>
-   Added graphical connections.
-   </li>
-   <li>
-   April 17, 2015, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"), Icon(coordinateSystem(preserveAspectRatio=false,  extent=
+  <p><code>ExteriorWall</code> represents heat conduction and heat storage
+  within walls. It links a variable number <code>n</code> of thermal resistances
+  and capacities to a series connection. <code>n</code> thus defines the spatial
+  discretization of thermal effects within the wall. All effects are considered
+  as one-dimensional normal to the wall&apos;s surface. This model is thought
+  for exterior wall elements that contribute to heat transfer to the outdoor.
+  The RC-chain is defined via a vector of capacities <code>CExt[n]</code> and a
+  vector of resistances <code>RExt[n]</code>. Resistances and capacities are
+  connected alternately, starting with the first resistance <code>RExt[1]</code>,
+  from heat <code>port_a</code> to heat <code>port_b</code>. <code>RExtRem</code>
+  is the resistance between the last capacity <code>CExt[end]</code> and the
+  heat <code>port_b</code>.</p>
+  <p align=\"center\"><img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/BaseClasses/ExtMassVarRC/ExtMassVarRC.png\" alt=\"image\"/> </p>
+  </html>",  revisions="<html>
+  <ul>
+  <li>
+  April 27, 2016, by Michael Wetter:<br/>
+  Added graphical connections.
+  </li>
+  <li>
+  April 17, 2015, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),  Icon(coordinateSystem(preserveAspectRatio=false,  extent=
   {{-100,-100},{100,120}}), graphics={  Rectangle(extent = {{-86, 60}, {-34, 26}},
    fillColor = {255, 213, 170},
    fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}), Rectangle(
@@ -138,6 +138,6 @@ equation
    Line(points = {{18, -32}, {-20, -32}}, color = {0, 0, 0}, thickness = 0.5,
    smooth = Smooth.None),
    Line(points = {{14, -44}, {-15, -44}}, color = {0, 0, 0}, thickness = 0.5,
-   smooth = Smooth.None)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+   smooth = Smooth.None)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ExteriorWall;
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/InteriorWall.mo b/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/InteriorWall.mo
index 6a422349dc..70cdae775a 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/InteriorWall.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/InteriorWall.mo
@@ -42,30 +42,30 @@ equation
  annotation(defaultComponentName = "intWalRC",Diagram(coordinateSystem(
   preserveAspectRatio=false,   extent={{-100,-100},{100,120}})),
   Documentation(info="<html>
-   <p><code>InteriorWall</code> represents heat storage within walls. It links a
-   variable number <code>n</code> of thermal resistances and capacities to a
-   series connection. <code>n</code> thus defines the spatial discretization of
-   thermal effects within the wall. All effects are considered as one-dimensional
-   normal to the wall&apos;s surface. This model is thought for interior wall
-   elements that only serve as heat storage elements. The RC-chain is defined via
-   a vector of capacities <code>CInt[n]</code> and a vector of resistances
-   <code>RInt[n]</code>.
-   Resistances and capacities are connected alternately, starting with the first
-   resistance <code>RInt[1]</code>, from heat <code>port_a</code> into the wall.
-   </p>
-   <p align=\"center\"><img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/BaseClasses/IntMassVarRC/IntMassVarRC.png\" alt=\"image\"/> </p>
-   </html>", revisions="<html>
-   <ul>
-   <li>
-   April 27, 2016, by Michael Wetter:<br/>
-   Added graphical connections.
-   </li>
-   <li>
-   April 17, 2015, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"), Icon(coordinateSystem(preserveAspectRatio = true, extent=
+  <p><code>InteriorWall</code> represents heat storage within walls. It links a
+  variable number <code>n</code> of thermal resistances and capacities to a
+  series connection. <code>n</code> thus defines the spatial discretization of
+  thermal effects within the wall. All effects are considered as one-dimensional
+  normal to the wall&apos;s surface. This model is thought for interior wall
+  elements that only serve as heat storage elements. The RC-chain is defined via
+  a vector of capacities <code>CInt[n]</code> and a vector of resistances
+  <code>RInt[n]</code>.
+  Resistances and capacities are connected alternately, starting with the first
+  resistance <code>RInt[1]</code>, from heat <code>port_a</code> into the wall.
+  </p>
+  <p align=\"center\"><img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/BaseClasses/IntMassVarRC/IntMassVarRC.png\" alt=\"image\"/> </p>
+  </html>",  revisions="<html>
+  <ul>
+  <li>
+  April 27, 2016, by Michael Wetter:<br/>
+  Added graphical connections.
+  </li>
+  <li>
+  April 17, 2015, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),  Icon(coordinateSystem(preserveAspectRatio = true, extent=
   {{-100, -100}, {100, 120}}), graphics={  Rectangle(extent=
   {{-86, 60}, {-34, 26}}, fillColor = {255, 213, 170},
    fillPattern = FillPattern.Solid, lineColor = {175, 175, 175}),
@@ -118,6 +118,6 @@ equation
    Line(points = {{18, -32}, {-20, -32}}, color = {0, 0, 0}, thickness = 0.5,
    smooth = Smooth.None),
    Line(points = {{14, -44}, {-15, -44}}, color = {0, 0, 0}, thickness = 0.5,
-   smooth = Smooth.None)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+   smooth = Smooth.None)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InteriorWall;
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/ThermSplitter.mo b/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/ThermSplitter.mo
index 7b3b4c4b62..a8fd721230 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/ThermSplitter.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/ThermSplitter.mo
@@ -1,6 +1,6 @@
 within AixLib.ThermalZones.ReducedOrder.RC.BaseClasses;
 model ThermSplitter "A simple model which weights a given set of thermal inputs
-   to calculate an average temperature and aggregated heat flow per output"
+  to calculate an average temperature and aggregated heat flow per output"
 
   parameter Integer nOut "Number of splitter outputs";
   parameter Integer nIn "Number of splitter inputs";
@@ -50,28 +50,28 @@ equation
     textColor={0,0,255},
     textString="ThermSplitter")}),
   Documentation(info="<html>
-   <p>This model is used to weight thermal ports (inputs) according to given split
-   factors per output port.</p>
-   <p>The model needs the dimensions of the splitted therm ports (for input and
-   output ports resp.) and the split factors, which are between 0 and 1. Each row
-   of the split factor matrix gives the split factors for one output
-   port. The number of columns need to align with the number of input ports.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   May, 2016, by Moritz Lauster:<br/>
-   Extended to handle multiple input ports.
-   </li>
-   <li>
-   January, 2015, by Peter Remmen:<br/>
-   Changed name and vectorized
-   equation, added documentation
-   </li>
-   <li>
-   October, 2014, by Peter Remmen:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>This model is used to weight thermal ports (inputs) according to given split
+  factors per output port.</p>
+  <p>The model needs the dimensions of the splitted therm ports (for input and
+  output ports resp.) and the split factors, which are between 0 and 1. Each row
+  of the split factor matrix gives the split factors for one output
+  port. The number of columns need to align with the number of input ports.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  May, 2016, by Moritz Lauster:<br/>
+  Extended to handle multiple input ports.
+  </li>
+  <li>
+  January, 2015, by Peter Remmen:<br/>
+  Changed name and vectorized
+  equation, added documentation
+  </li>
+  <li>
+  October, 2014, by Peter Remmen:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThermSplitter;
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/splitFacVal.mo b/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/splitFacVal.mo
index 140132804e..7c3c1f74b5 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/splitFacVal.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/BaseClasses/splitFacVal.mo
@@ -40,59 +40,59 @@ algorithm
     end for;
 
   annotation (Documentation(info="<html>
-   <p>Calculates the ratio of the surface areas of a wall to the total wall area,
-   unless the area is zero. It subtracts the wall area <code>AExt</code>
-   for first entry in <code>AArray</code> and <code>AWin</code> for
-   second entry in AArray unless <code>AArray[1]</code> and/or
-   <code>AArray[2]</code> are not zero. This is done separately for each
-   orientation. Consequently, the function gives an <code>nRow x nCol</code>
-   array back as output. Each row stands for one area in
-   <code>AArray</code> and each column for one orientation in
-   <code>AExt</code> and <code>AWin</code>. The function is used to
-   calculate the split factors for
-   <a href=\"AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter\">
-   AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter</a>.</p>
-   For internal gains, the calculation is:
-   <p align=\"center\" style=\"font-style:italic;\">
-  SplitFac<sub>i</sub> = AArray[i]
-   /ATot
-   </p>
-   whereby <code>ATot</code> is the sum of <code>AArray</code>. To
-   perform this,
-   <code>AExt</code> and <code>AWin</code> can just be set to vectors  of
-   zeros with length 1.
-   For solar radiation through windows, the window and wall area with the same
-   orientation as the incoming radiation should be subtracted as these areas
-   cannot be hit by the radiation. This needs to be done separately for each
-   orientation and for exterior walls and windows only, according to:
-   <p align=\"center\" style=\"font-style:italic;\">
-  SplitFac<sub>i,k</sub> = (AArray[i]
-   - AExt[k])
-   /(ATot
-   - AExt[k]
-   -AWin[k])
-   </p>
-   and
-   <p align=\"center\" style=\"font-style:italic;\">
-  SplitFac<sub>i,k</sub> = (AArray[i]
-   - AWin[k])
-   /(ATot
-   - AExt[k]
-   - AWin[k])
-   </p>
-   respectively. For all other walls, the equation is:
-   <p align=\"center\" style=\"font-style:italic;\">
-  SplitFac<sub>i,k</sub> = AArray[i]
-   /(ATot
-   - AExt[k]
-   - AWin[k])
-   </p>
-   </html>",revisions="<html>
-   <ul>
-   <li>December 15, 2015 by Moritz Lauster:<br/>
-   First Implementation.
-   </li>
-   </ul>
-   </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Calculates the ratio of the surface areas of a wall to the total wall area,
+  unless the area is zero. It subtracts the wall area <code>AExt</code>
+  for first entry in <code>AArray</code> and <code>AWin</code> for
+  second entry in AArray unless <code>AArray[1]</code> and/or
+  <code>AArray[2]</code> are not zero. This is done separately for each
+  orientation. Consequently, the function gives an <code>nRow x nCol</code>
+  array back as output. Each row stands for one area in
+  <code>AArray</code> and each column for one orientation in
+  <code>AExt</code> and <code>AWin</code>. The function is used to
+  calculate the split factors for
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter\">
+  AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter</a>.</p>
+  For internal gains, the calculation is:
+  <p align=\"center\" style=\"font-style:italic;\">
+ SplitFac<sub>i</sub> = AArray[i]
+  /ATot
+  </p>
+  whereby <code>ATot</code> is the sum of <code>AArray</code>. To
+  perform this,
+  <code>AExt</code> and <code>AWin</code> can just be set to vectors  of
+  zeros with length 1.
+  For solar radiation through windows, the window and wall area with the same
+  orientation as the incoming radiation should be subtracted as these areas
+  cannot be hit by the radiation. This needs to be done separately for each
+  orientation and for exterior walls and windows only, according to:
+  <p align=\"center\" style=\"font-style:italic;\">
+ SplitFac<sub>i,k</sub> = (AArray[i]
+  - AExt[k])
+  /(ATot
+  - AExt[k]
+  -AWin[k])
+  </p>
+  and
+  <p align=\"center\" style=\"font-style:italic;\">
+ SplitFac<sub>i,k</sub> = (AArray[i]
+  - AWin[k])
+  /(ATot
+  - AExt[k]
+  - AWin[k])
+  </p>
+  respectively. For all other walls, the equation is:
+  <p align=\"center\" style=\"font-style:italic;\">
+ SplitFac<sub>i,k</sub> = AArray[i]
+  /(ATot
+  - AExt[k]
+  - AWin[k])
+  </p>
+  </html>", revisions="<html>
+  <ul>
+  <li>December 15, 2015 by Moritz Lauster:<br/>
+  First Implementation.
+  </li>
+  </ul>
+  </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end splitFacVal;
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/FourElements.mo b/AixLib/ThermalZones/ReducedOrder/RC/FourElements.mo
index 27eea98b12..571aa931a8 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/FourElements.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/FourElements.mo
@@ -1,6 +1,6 @@
 within AixLib.ThermalZones.ReducedOrder.RC;
 model FourElements "Thermal Zone with four elements for exterior walls,
-   interior walls, floor plate and roof"
+  interior walls, floor plate and roof"
   extends ThreeElements(AArray={ATotExt,ATotWin,AInt,AFloor,ARoof});
 
   parameter Modelica.Units.SI.Area ARoof "Area of roof"
@@ -193,52 +193,52 @@ equation
   textColor={0,0,0},
   textString="4")}),
   Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- December 9, 2019, by Moritz Lauster:<br/>
- Changes <code>nExt</code> to <code>nRoof</code> for
- <code>RRoof</code> and <code>CRoof</code>
- </li>
- <li>
- July 11, 2019, by Katharina Brinkmann:<br/>
- Renamed <code>alphaRoof</code> to <code>hConRoof</code>,
- <code>alphaRoofConst</code> to <code>hConRoof_const</code>
- </li>
- <li>
- August 31, 2018 by Moritz Lauster:<br/>
- Updated schema in documentation and fixes
- orientation and connections of roofRC for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/997\">
- issue 997</a>.
- </li>
- <li>
- September 11, 2015 by Moritz Lauster:<br/>
- First Implementation.
- </li>
- </ul>
- </html>",  info="<html>
-   <p>
-   This model adds another element for the roof. Roofs commonly
-   exhibit the same excitations as exterior walls but have different coefficients
-   of heat transfer due to their orientation. Adding an extra element for the roof
-   might lead to a finer resolution of the dynamic behaviour but increases
-   calculation times. The roof is parameterized via the length of the RC-chain
-   <code>nRoof</code>,
-   the vector of capacities <code>CRoof[nRoof]</code>, the vector of resistances
-   <code>RRoof[nRoof]</code> and remaining resistances <code>RRoofRem</code>.
-   </p>
-   <p>
-   The image below shows the RC-network of this model.
-   </p>
-   <p align=\"center\">
-   <img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/FourElements.png\" alt=\"image\"/>
-   </p>
-   </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+December 9, 2019, by Moritz Lauster:<br/>
+Changes <code>nExt</code> to <code>nRoof</code> for
+<code>RRoof</code> and <code>CRoof</code>
+</li>
+<li>
+July 11, 2019, by Katharina Brinkmann:<br/>
+Renamed <code>alphaRoof</code> to <code>hConRoof</code>,
+<code>alphaRoofConst</code> to <code>hConRoof_const</code>
+</li>
+<li>
+August 31, 2018 by Moritz Lauster:<br/>
+Updated schema in documentation and fixes
+orientation and connections of roofRC for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/997\">
+issue 997</a>.
+</li>
+<li>
+September 11, 2015 by Moritz Lauster:<br/>
+First Implementation.
+</li>
+</ul>
+</html>",   info="<html>
+  <p>
+  This model adds another element for the roof. Roofs commonly
+  exhibit the same excitations as exterior walls but have different coefficients
+  of heat transfer due to their orientation. Adding an extra element for the roof
+  might lead to a finer resolution of the dynamic behaviour but increases
+  calculation times. The roof is parameterized via the length of the RC-chain
+  <code>nRoof</code>,
+  the vector of capacities <code>CRoof[nRoof]</code>, the vector of resistances
+  <code>RRoof[nRoof]</code> and remaining resistances <code>RRoofRem</code>.
+  </p>
+  <p>
+  The image below shows the RC-network of this model.
+  </p>
+  <p align=\"center\">
+  <img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/FourElements.png\" alt=\"image\"/>
+  </p>
+  </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FourElements;
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/OneElement.mo b/AixLib/ThermalZones/ReducedOrder/RC/OneElement.mo
index a704d39758..36fb36ccfc 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/OneElement.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/OneElement.mo
@@ -17,8 +17,7 @@ model OneElement "Thermal Zone with one element for exterior walls"
     "Vector of areas of windows by orientations"
     annotation (Dialog(group="Windows"));
   parameter Modelica.Units.SI.Area ATransparent[nOrientations] "Vector of areas of transparent (solar radiation transmittend) elements by
-     orientations"
-                  annotation (Dialog(group="Windows"));
+    orientations" annotation (Dialog(group="Windows"));
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hConWin
     "Convective coefficient of heat transfer of windows (indoor)"
     annotation (Dialog(group="Windows"));
@@ -176,14 +175,14 @@ model OneElement "Thermal Zone with one element for exterior walls"
     final nOut=dimension,
     final nIn=1) if ATot > 0
     "Splits incoming internal gains into separate gains for each wall element,
-     weighted by their area"
+    weighted by their area"
     annotation (Placement(transformation(extent={{210,76},{190,96}})));
   BaseClasses.ThermSplitter thermSplitterSolRad(
     final splitFactor=splitFactorSolRad,
     final nOut=dimension,
     final nIn=nOrientations) if ATot > 0 and sum(ATransparent) > 0
     "Splits incoming solar radiation into separate gains for each wall element,
-     weighted by their area"
+    weighted by their area"
     annotation (Placement(transformation(extent={{-138,138},{-122,154}})));
   BaseClasses.ExteriorWall extWallRC(
     final n=nExt,
@@ -237,12 +236,15 @@ protected
     rotation=-90,
     origin={-106,68})));
   Modelica.Blocks.Math.Gain eRadSol[nOrientations](
-    final k=gWin*(1 - ratioWinConRad)*ATransparent) if sum(ATransparent) > 0
+    final k(each unit="m2")=gWin*(1 - ratioWinConRad)*ATransparent,
+    u(each final unit="W/m2"),
+    y(each final unit="W")) if sum(ATransparent) > 0
     "Emission coefficient of solar radiation considered as radiation"
     annotation (Placement(transformation(extent={{-206,141},{-196,151}})));
   Modelica.Blocks.Math.Gain eConvSol[nOrientations](
-    final k=gWin*ratioWinConRad*ATransparent)
- if ratioWinConRad > 0 and sum(ATransparent) > 0
+    final k(each unit="m2")=gWin*ratioWinConRad*ATransparent,
+    u(each final unit="W/m2"),
+    y(each final unit="W")) if ratioWinConRad > 0 and sum(ATransparent) > 0
     "Emission coefficient of solar radiation considered as convection"
     annotation (Placement(transformation(extent={{-206,119},{-196,129}})));
   Modelica.Thermal.HeatTransfer.Components.ThermalConductor resExtWallWin(
@@ -521,66 +523,66 @@ equation
     textColor={0,0,0},
     textString="1")}),
   Documentation(info="<html>
- <p>
- This model merges all thermal masses into one
- element, parameterized by the length of the RC-chain
- <code>nExt,</code> the vector of the capacities <code>CExt[nExt]</code> that is
- connected via the vector of resistances <code>RExt[nExt]</code> and
- <code>RExtRem</code> to the ambient and indoor air.
- By default, the model neglects all
- internal thermal masses that are not directly connected to the ambient.
- However, the thermal capacity of the room air can be increased by
- using the parameter <code>mSenFac</code>.
- </p>
- <p>
- The image below shows the RC-network of this model.
- </p>
- <p align=\"center\">
- <img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/OneElement.png\" alt=\"image\"/>
- </p>
-   </html>",
+<p>
+This model merges all thermal masses into one
+element, parameterized by the length of the RC-chain
+<code>nExt,</code> the vector of the capacities <code>CExt[nExt]</code> that is
+connected via the vector of resistances <code>RExt[nExt]</code> and
+<code>RExtRem</code> to the ambient and indoor air.
+By default, the model neglects all
+internal thermal masses that are not directly connected to the ambient.
+However, the thermal capacity of the room air can be increased by
+using the parameter <code>mSenFac</code>.
+</p>
+<p>
+The image below shows the RC-network of this model.
+</p>
+<p align=\"center\">
+<img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/OneElement.png\" alt=\"image\"/>
+</p>
+  </html>",
 revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- October 9, 2019, by Michael Wetter:<br/>
- Refactored addition of moisture to also account for the energy content of the
- water vapor.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1209\">IBPSA, issue 1209</a>.
- </li>
-   <li>
-   September 24, 2019, by Martin Kremer:<br/>
-   Added possibility to consider moisture balance. <br/>
-   Defined <code>volAir</code> conditional. Added conditional <code>volMoistAir</code> and corresponding in- and output connectors.
-   </li>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaRad</code> to <code>hRad</code>,
-   <code>alphaWin</code> to <code>hConWin</code>,
-   <code>alphaExt</code> to <code>hConExt</code>,
-   <code>alphaExtWallConst</code> to <code>hConExtWall_const</code>,
-   <code>alphaWinConst</code> to <code>hConWin_const</code>
-   </li>
-   <li>
-   January 25, 2019, by Michael Wetter:<br/>
-   Added start value to avoid warning in JModelica.
-   </li>
-   <li>
-   September 26, 2016, by Moritz Lauster:<br/>
-   Added conditional statements to solar radiation part.<br/>
-   Deleted conditional statements of
-   <code>splitFactor</code> and <code>splitFactorSolRad</code>.
-   </li>
-   <li>
-   April 17, 2015, by Moritz Lauster:<br/>
-   First implementation.
-   </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+October 9, 2019, by Michael Wetter:<br/>
+Refactored addition of moisture to also account for the energy content of the
+water vapor.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1209\">IBPSA, issue 1209</a>.
+</li>
+  <li>
+  September 24, 2019, by Martin Kremer:<br/>
+  Added possibility to consider moisture balance. <br/>
+  Defined <code>volAir</code> conditional. Added conditional <code>volMoistAir</code> and corresponding in- and output connectors.
+  </li>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaRad</code> to <code>hRad</code>,
+  <code>alphaWin</code> to <code>hConWin</code>,
+  <code>alphaExt</code> to <code>hConExt</code>,
+  <code>alphaExtWallConst</code> to <code>hConExtWall_const</code>,
+  <code>alphaWinConst</code> to <code>hConWin_const</code>
+  </li>
+  <li>
+  January 25, 2019, by Michael Wetter:<br/>
+  Added start value to avoid warning in JModelica.
+  </li>
+  <li>
+  September 26, 2016, by Moritz Lauster:<br/>
+  Added conditional statements to solar radiation part.<br/>
+  Deleted conditional statements of
+  <code>splitFactor</code> and <code>splitFactorSolRad</code>.
+  </li>
+  <li>
+  April 17, 2015, by Moritz Lauster:<br/>
+  First implementation.
+  </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end OneElement;
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/ThreeElements.mo b/AixLib/ThermalZones/ReducedOrder/RC/ThreeElements.mo
index 927298fc61..8f5439f4ff 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/ThreeElements.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/ThreeElements.mo
@@ -1,6 +1,6 @@
 within AixLib.ThermalZones.ReducedOrder.RC;
 model ThreeElements "Thermal Zone with three elements for exterior walls,
-   interior walls and floor plate"
+  interior walls and floor plate"
     extends TwoElements(AArray={ATotExt,ATotWin,AInt,AFloor});
 
   parameter Modelica.Units.SI.Area AFloor "Area of floor plate"
@@ -178,52 +178,52 @@ equation
     textColor={0,0,0},
     textString="3")}),
     Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- December 9, 2019, by Moritz Lauster:<br/>
- Changes <code>nExt</code> to <code>nFloor</code> for
- <code>RFloor</code> and <code>CFloor</code>
- </li>
- <li>
- July 11, 2019, by Katharina Brinkmann:<br/>
- Renamed <code>alphaFloor</code> to <code>hConFloor</code>,
- <code>alphaFloorConst</code> to <code>hConFloor_const</code>
- </li>
- <li>
- August 31, 2018 by Moritz Lauster:<br/>
- Updated schema in documentation to fix
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/997\">
- issue 997</a>.
- </li>
- <li>
- July 15, 2015 by Moritz Lauster:<br/>
- First Implementation.
- </li>
- </ul>
- </html>",  info="<html>
-   <p>This model adds one further element for
-   the floor plate. Long-term effects dominate the excitation of the floor plate
-   and thus the excitation fundamentally differs from excitation of outer walls.
-   Adding an extra element for the floor plate leads to a finer resolution of the
-   dynamic behaviour but increases calculation times. The floor plate is
-   parameterized via the length of the RC-chain <code>nFloor</code>,
-   the vector of the capacities
-   <code>CFloor[nFloor]</code>, the vector of the resistances
-   <code>RFloor[nFloor]</code>
-   and the remaining resistance <code>RFloorRem</code>.
-   </p>
-   <p>
-   The image below shows the RC-network of this model.
-   </p>
-   <p align=\"center\">
-   <img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/ThreeElements.png\" alt=\"image\"/>
-   </p>
-   </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+December 9, 2019, by Moritz Lauster:<br/>
+Changes <code>nExt</code> to <code>nFloor</code> for
+<code>RFloor</code> and <code>CFloor</code>
+</li>
+<li>
+July 11, 2019, by Katharina Brinkmann:<br/>
+Renamed <code>alphaFloor</code> to <code>hConFloor</code>,
+<code>alphaFloorConst</code> to <code>hConFloor_const</code>
+</li>
+<li>
+August 31, 2018 by Moritz Lauster:<br/>
+Updated schema in documentation to fix
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/997\">
+issue 997</a>.
+</li>
+<li>
+July 15, 2015 by Moritz Lauster:<br/>
+First Implementation.
+</li>
+</ul>
+</html>",   info="<html>
+  <p>This model adds one further element for
+  the floor plate. Long-term effects dominate the excitation of the floor plate
+  and thus the excitation fundamentally differs from excitation of outer walls.
+  Adding an extra element for the floor plate leads to a finer resolution of the
+  dynamic behaviour but increases calculation times. The floor plate is
+  parameterized via the length of the RC-chain <code>nFloor</code>,
+  the vector of the capacities
+  <code>CFloor[nFloor]</code>, the vector of the resistances
+  <code>RFloor[nFloor]</code>
+  and the remaining resistance <code>RFloorRem</code>.
+  </p>
+  <p>
+  The image below shows the RC-network of this model.
+  </p>
+  <p align=\"center\">
+  <img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/ThreeElements.png\" alt=\"image\"/>
+  </p>
+  </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ThreeElements;
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/TwoElements.mo b/AixLib/ThermalZones/ReducedOrder/RC/TwoElements.mo
index 9a13f03813..c31f034895 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/TwoElements.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/TwoElements.mo
@@ -124,44 +124,44 @@ equation
     fillColor={215,215,215},
     fillPattern=FillPattern.Solid,
     textString="Interior Walls")}), Documentation(revisions="<html>
- <ul>
- <li>
- March 7, 2022, by Michael Wetter:<br/>
- Removed <code>massDynamics</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
- </li>
- <li>
- July 11, 2019, by Katharina Brinkmann:<br/>
- Renamed <code>alphaInt</code> to <code>hConInt</code>,
- <code>alphaIntWall</code> to <code>hConIntWall</code>
- </li>
- <li>
- January 25, 2019, by Michael Wetter:<br/>
- Added start value to avoid warning in JModelica.
- </li>
- <li>
- April 18, 2015, by Moritz Lauster:<br/>
- First implementation.
- </li>
- </ul>
- </html>",  info="<html>
-   <p>This model distinguishes between internal
-   thermal masses and exterior walls. While exterior walls contribute to heat
-   transfer to the ambient, adiabatic conditions apply to internal masses.
-   Parameters for the internal wall element are the length of the RC-chain
-   <code>nInt</code>, the vector of the capacities
-   <code>CInt[nInt]</code> and the vector of the resistances <code>RInt[nInt]</code>.
-   This approach allows considering the dynamic behaviour induced by internal
-   heat storage.
-   </p>
-   <p>
-   The image below shows the RC-network of this model.
-   </p>
-   <p align=\"center\">
-   <img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/TwoElements.png\" alt=\"image\"/>
-   </p>
-   </html>"),
+<ul>
+<li>
+March 7, 2022, by Michael Wetter:<br/>
+Removed <code>massDynamics</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1542\">#1542</a>.
+</li>
+<li>
+July 11, 2019, by Katharina Brinkmann:<br/>
+Renamed <code>alphaInt</code> to <code>hConInt</code>,
+<code>alphaIntWall</code> to <code>hConIntWall</code>
+</li>
+<li>
+January 25, 2019, by Michael Wetter:<br/>
+Added start value to avoid warning in JModelica.
+</li>
+<li>
+April 18, 2015, by Moritz Lauster:<br/>
+First implementation.
+</li>
+</ul>
+</html>",   info="<html>
+  <p>This model distinguishes between internal
+  thermal masses and exterior walls. While exterior walls contribute to heat
+  transfer to the ambient, adiabatic conditions apply to internal masses.
+  Parameters for the internal wall element are the length of the RC-chain
+  <code>nInt</code>, the vector of the capacities
+  <code>CInt[nInt]</code> and the vector of the resistances <code>RInt[nInt]</code>.
+  This approach allows considering the dynamic behaviour induced by internal
+  heat storage.
+  </p>
+  <p>
+  The image below shows the RC-network of this model.
+  </p>
+  <p align=\"center\">
+  <img src=\"modelica://AixLib/Resources/Images/ThermalZones/ReducedOrder/RC/TwoElements.png\" alt=\"image\"/>
+  </p>
+  </html>"),
   Icon(coordinateSystem(extent={{-240,-180},{240,180}},
   preserveAspectRatio=false),
   graphics={Rectangle(
@@ -171,6 +171,6 @@ equation
   pattern=LinePattern.None), Text(
   extent={{-60,60},{64,-64}},
   textColor={0,0,0},
-  textString="2")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+  textString="2")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TwoElements;
diff --git a/AixLib/ThermalZones/ReducedOrder/RC/package.mo b/AixLib/ThermalZones/ReducedOrder/RC/package.mo
index 27a45b7242..726f363544 100644
--- a/AixLib/ThermalZones/ReducedOrder/RC/package.mo
+++ b/AixLib/ThermalZones/ReducedOrder/RC/package.mo
@@ -51,10 +51,10 @@ package RC "Package with reduced order thermal zones based on VDI 6007 Part 1"
   <h4>Architecture</h4>
   <p>
   Each wall element uses either
-  <a href=\"AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ExteriorWall\">
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ExteriorWall\">
   AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ExteriorWall</a>
   or
-  <a href=\"AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.InteriorWall\">
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.InteriorWall\">
   AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.InteriorWall</a>
   to describe heat conduction and storage within the wall, depending if the wall
   contributes to heat transfer to the outdoor environment (exterior walls) or can
@@ -90,7 +90,7 @@ package RC "Package with reduced order thermal zones based on VDI 6007 Part 1"
   The transmission of solar radiation through windows is split up into two parts.
   One part is connected to the indoor radiative heat exchange mesh network using
   a
-  <a href=\"AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter\">
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter\">
   AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter</a>,
   while the other part is directly linked to the convective network. The split
   factor <code>ratioWinConRad </code> is a window property and depends on the
@@ -156,7 +156,7 @@ package RC "Package with reduced order thermal zones based on VDI 6007 Part 1"
   temperature and thus of area as well, assuming that the temperature of the
   source is high compared to the wall surface temperatures.
   By using a
-  <a href=\"AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter\">
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter\">
   AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.ThermSplitter</a>
   that distributes the heat flow of the source over the walls according to their
   area, we support this simplified approach. For solar radiation through windows,
@@ -164,7 +164,7 @@ package RC "Package with reduced order thermal zones based on VDI 6007 Part 1"
   radiation is not taken into account for the distribution as such surfaces cannot
   be hit by the particular radiation. This calculation is performed for each
   orientation separately using
-  <a href=\"AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.splitFacVal\">
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.splitFacVal\">
   AixLib.ThermalZones.ReducedOrder.RC.BaseClasses.splitFacVal</a>.
   </p>
   </li>
@@ -184,7 +184,7 @@ package RC "Package with reduced order thermal zones based on VDI 6007 Part 1"
   <p>
   The models in this package are typically used in combination with models from
   the parent package
-  <a href=\"AixLib.ThermalZones.ReducedOrder\">
+  <a href=\"modelica://AixLib.ThermalZones.ReducedOrder\">
   AixLib.ThermalZones.ReducedOrder</a>.
   A typical application is one building out of a large building stock for
   which the heating and cooling power over a year in hourly time steps should be
diff --git a/AixLib/ThermalZones/ReducedOrder/SolarGain/BaseClasses/PartialCorrectionG.mo b/AixLib/ThermalZones/ReducedOrder/SolarGain/BaseClasses/PartialCorrectionG.mo
index b27dfa1d72..97951597e3 100644
--- a/AixLib/ThermalZones/ReducedOrder/SolarGain/BaseClasses/PartialCorrectionG.mo
+++ b/AixLib/ThermalZones/ReducedOrder/SolarGain/BaseClasses/PartialCorrectionG.mo
@@ -46,19 +46,19 @@ partial model PartialCorrectionG
   textColor={0,0,0},
   textString="%name")}),
   Documentation(info="<html>
-   <p>Partial model for correction factors for transmitted solar radiation
-   through a transparent element.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   February 27, 2016, by Michael Wetter:<br/>
-   Moved input above outputs.
-   </li>
-   <li>
-   February 24, 2014, by Reza Tavakoli:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <p>Partial model for correction factors for transmitted solar radiation
+  through a transparent element.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  February 27, 2016, by Michael Wetter:<br/>
+  Moved input above outputs.
+  </li>
+  <li>
+  February 24, 2014, by Reza Tavakoli:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialCorrectionG;
diff --git a/AixLib/ThermalZones/ReducedOrder/SolarGain/CorrectionGDoublePane.mo b/AixLib/ThermalZones/ReducedOrder/SolarGain/CorrectionGDoublePane.mo
index e8124a7049..dfae38dd0b 100644
--- a/AixLib/ThermalZones/ReducedOrder/SolarGain/CorrectionGDoublePane.mo
+++ b/AixLib/ThermalZones/ReducedOrder/SolarGain/CorrectionGDoublePane.mo
@@ -21,9 +21,9 @@ protected
   parameter Real A6=4.74*10^(-12)
     "Constant 6 to calculate reference transmission";
   parameter Modelica.Units.SI.TransmissionCoefficient g_dir0=0.7537 "Reference vertical parallel transmission coefficient for direct radiation
-     for double pane window";
+    for double pane window";
   parameter Modelica.Units.SI.TransmissionCoefficient Ta_diff=0.84 "Energetic degree of transmission for diffuse radiation for uniformly
-     overcast sky";
+    overcast sky";
   parameter Modelica.Units.SI.TransmissionCoefficient Tai_diff=0.903
     "Pure degree of transmission for diffuse radiation";
   parameter Modelica.Units.SI.TransmissionCoefficient Ta1_diff=Ta_diff*Tai_diff
@@ -32,7 +32,7 @@ protected
     "Part of degree of transmission for single pane window related to Ta1_diff";
   parameter Modelica.Units.SI.ReflectionCoefficient rho_11_diff=rho_T1_diff/(2
        - (rho_T1_diff)) "Part of degree of transmission for single pane window
-     related to rho_T1_diff";
+    related to rho_T1_diff";
   parameter Modelica.Units.SI.ReflectionCoefficient rho_1_diff=rho_11_diff + ((
       (1 - rho_11_diff)*Tai_diff)^2*rho_11_diff)/(1 - (rho_11_diff*Tai_diff)^2)
     "Degree of reflection for single pane window";
@@ -42,14 +42,14 @@ protected
       XN2_diff "Energetic dregree of transmission for second pane";
   parameter Modelica.Units.SI.Emissivity a1_diff=1 - Ta1_diff - rho_1_diff
     "Degree of absorption for single pane window";
-  parameter Modelica.Units.SI.CoefficientOfHeatTransfer Q21_diff=a1_diff*(1 + (
+  parameter Real Q21_diff=a1_diff*(1 + (
       Ta1_diff*rho_1_diff/XN2_diff))*UWin/25
-    "Coefficient of heat transfer for exterior pane of double pane window";
-  parameter Modelica.Units.SI.CoefficientOfHeatTransfer Q22_diff=a1_diff*(
+    "Auxiliary parameter for heat transfer of exterior pane of double pane window";
+  parameter Real Q22_diff=a1_diff*(
       Ta1_diff/XN2_diff)*(1 - (UWin/7.7))
-    "Coefficient of heat transfer for interior pane of double pane window";
-  parameter Modelica.Units.SI.CoefficientOfHeatTransfer Qsek2_diff=Q21_diff +
-      Q22_diff "Overall coefficient of heat transfer for double pane window";
+    "Auxiliary parameter for heat transfer of interior pane of double pane window";
+  parameter Real Qsek2_diff=Q21_diff + Q22_diff
+    "Overall auxiliary parameter for heat transfer of double pane window";
   parameter Modelica.Units.SI.TransmissionCoefficient CorG_diff=(Ta2_diff +
       Qsek2_diff)/g_dir0
     "Transmission coefficient correction factor for diffuse radiation";
@@ -110,33 +110,33 @@ equation
 
   annotation (defaultComponentName="corG",
   Documentation(info="<html>
-   <p>This model computes short-wave radiation through
-   transparent elements with any orientation and inclination by means of
-   solar transmission correction factors. Transmission properties of transparent
-   elements are in general dependent on the solar incidence angle. To take this
-   dependency into account, correction factors can be multiplied with the solar
-   radiation. These factors should not be mistaken as calculation of solar
-   radiation on tilted surfaces, calculation of <i>g</i>-values or consideration of
-   sunblinds, as it is an additional step. The implemented calculations are
-   defined in the German Guideline VDI 6007 Part 3 (VDI, 2015). The given model
-   is only valid for double pane windows. The guideline describes also
-   calculations for single pane and triple pane windows.</p>
-   <h4>References</h4>
-   <p>VDI. German Association of Engineers Guideline VDI 6007-3 June 2015.
-   Calculation of transient thermal response of rooms and buildings -
-   modelling of solar radiation.</p>
-   </html>",
+  <p>This model computes short-wave radiation through
+  transparent elements with any orientation and inclination by means of
+  solar transmission correction factors. Transmission properties of transparent
+  elements are in general dependent on the solar incidence angle. To take this
+  dependency into account, correction factors can be multiplied with the solar
+  radiation. These factors should not be mistaken as calculation of solar
+  radiation on tilted surfaces, calculation of <i>g</i>-values or consideration of
+  sunblinds, as it is an additional step. The implemented calculations are
+  defined in the German Guideline VDI 6007 Part 3 (VDI, 2015). The given model
+  is only valid for double pane windows. The guideline describes also
+  calculations for single pane and triple pane windows.</p>
+  <h4>References</h4>
+  <p>VDI. German Association of Engineers Guideline VDI 6007-3 June 2015.
+  Calculation of transient thermal response of rooms and buildings -
+  modelling of solar radiation.</p>
+  </html>",
   revisions="<html>
-   <ul>
-   <li>
-   September 12, 2015 by Moritz Lauster:<br/>
-   Adapted to Annex 60 requirements.
-   </li>
-   <li>
-   February 24, 2014, by Reza Tavakoli:<br/>
-   First implementation.
-   </li>
-   </ul>
-   </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+  <ul>
+  <li>
+  September 12, 2015 by Moritz Lauster:<br/>
+  Adapted to Annex 60 requirements.
+  </li>
+  <li>
+  February 24, 2014, by Reza Tavakoli:<br/>
+  First implementation.
+  </li>
+  </ul>
+  </html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CorrectionGDoublePane;
diff --git a/AixLib/ThermalZones/ReducedOrder/ThermalZone/BaseClasses/PartialThermalZone.mo b/AixLib/ThermalZones/ReducedOrder/ThermalZone/BaseClasses/PartialThermalZone.mo
index 45932ea888..29f8d8fd15 100644
--- a/AixLib/ThermalZones/ReducedOrder/ThermalZone/BaseClasses/PartialThermalZone.mo
+++ b/AixLib/ThermalZones/ReducedOrder/ThermalZone/BaseClasses/PartialThermalZone.mo
@@ -4,10 +4,20 @@ partial model PartialThermalZone "Partial model for thermal zone models"
 
   replaceable parameter DataBase.ThermalZones.ZoneBaseRecord zoneParam
     "Choose setup for this zone" annotation (choicesAllMatching=true);
-  parameter Integer nPorts=0
+  parameter Integer nPorts =  0
     "Number of fluid ports"
     annotation(Evaluate=true,
     Dialog(connectorSizing=true, tab="General",group="Ports"));
+   // Pool parameters
+   parameter Boolean use_pools = false
+    "If true, pool model and corresponding connections are enabled"
+  annotation(Dialog(tab="Moisture", group="Pools"));
+
+   final parameter Integer nPortsROM = if use_pools then nPorts + 2 else nPorts
+    "Number of fluid ports"
+    annotation(Evaluate=true,
+    Dialog(connectorSizing=true, tab="General",group="Ports"));
+
   parameter Boolean use_C_flow=false
     "Set to true to enable input connector for trace substance"
     annotation (Dialog(tab="CO2"));
@@ -59,11 +69,11 @@ partial model PartialThermalZone "Partial model for thermal zone models"
     "Radiative internal gains"
     annotation (Placement(transformation(extent={{94,30},{114,50}}),
                             iconTransformation(extent={{92,24},{112,44}})));
-  RC.FourElements ROM(
+  AixLib.ThermalZones.ReducedOrder.RC.FourElements ROM(
     redeclare final package Medium = Medium,
     final use_moisture_balance=use_moisture_balance,
     final use_C_flow=use_C_flow,
-    final nPorts=nPorts,
+    final nPorts=nPortsROM,
     final VAir=if zoneParam.withAirCap then zoneParam.VAir else 0.0,
     final hRad=zoneParam.hRad,
     final nOrientations=size(zoneParam.AExt, 1),
@@ -97,6 +107,10 @@ partial model PartialThermalZone "Partial model for thermal zone models"
     final RRoofRem=zoneParam.RRoofRem,
     final CRoof=zoneParam.CRoof,
     final energyDynamics=energyDynamics,
+    extWallRC(thermCapExt(each der_T(fixed=energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial))),
+    floorRC(thermCapExt(each der_T(fixed=energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial))),
+    intWallRC(thermCapInt(each der_T(fixed=energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial))),
+    roofRC(thermCapExt(each der_T(fixed=energyDynamics == Modelica.Fluid.Types.Dynamics.FixedInitial))),
     final p_start=p_start,
     final X_start=X_start,
     final T_start=T_start,
@@ -112,8 +126,6 @@ protected
 equation
   connect(ROM.TAir, TAir) annotation (Line(points={{87,90},{98,90},{98,80},{110,
           80}}, color={0,0,127}));
-  connect(ROM.ports, ports) annotation (Line(points={{77,56.05},{78,56.05},{78,
-          52},{58,52},{58,4},{0,4},{0,-96}},    color={0,127,255}));
   connect(ROM.intGainsConv, intGainsConv) annotation (Line(points={{86,78},{92,
           78},{92,20},{104,20}},
                                color={191,0,0}));
@@ -124,6 +136,12 @@ equation
   connect(ROM.intGainsRad, intGainsRad) annotation (Line(points={{86,82},{94,82},
           {94,40},{104,40}},
                            color={191,0,0}));
+
+  for i in 1:nPorts loop
+      connect(ROM.ports[i], ports[i]) annotation (Line(points={{77,56.05},{78,56.05},{78,
+          52},{58,52},{58,4},{0,4},{0,-96}},    color={0,127,255}));
+  end for;
+
   annotation(Icon(coordinateSystem(preserveAspectRatio=false,  extent={{-100,-100},
             {100,100}}),graphics={Text(extent={{
               -80,114},{92,64}},lineColor=
diff --git a/AixLib/ThermalZones/ReducedOrder/ThermalZone/ThermalZone.mo b/AixLib/ThermalZones/ReducedOrder/ThermalZone/ThermalZone.mo
index f95c70ca6a..d275c0511d 100644
--- a/AixLib/ThermalZones/ReducedOrder/ThermalZone/ThermalZone.mo
+++ b/AixLib/ThermalZones/ReducedOrder/ThermalZone/ThermalZone.mo
@@ -1,10 +1,11 @@
-within AixLib.ThermalZones.ReducedOrder.ThermalZone;
+within AixLib.ThermalZones.ReducedOrder.ThermalZone;
 model ThermalZone "Thermal zone containing moisture balance"
   extends
     AixLib.ThermalZones.ReducedOrder.ThermalZone.BaseClasses.PartialThermalZone;
 
   replaceable model corG = SolarGain.CorrectionGDoublePane
-    constrainedby AixLib.ThermalZones.ReducedOrder.SolarGain.BaseClasses.PartialCorrectionG
+    constrainedby
+    AixLib.ThermalZones.ReducedOrder.SolarGain.BaseClasses.PartialCorrectionG
     "Model for correction of solar transmission"
     annotation(choicesAllMatching=true);
   parameter Integer internalGainsMode = 1
@@ -56,6 +57,25 @@ model ThermalZone "Thermal zone containing moisture balance"
     "Metabolic rate of a relaxed seated person  [1 Met = 58 W/m^2]"
     annotation (Dialog(tab="CO2", enable=use_C_flow));
 
+  // Pool parameters
+  replaceable package MediumPoolWater = AixLib.Media.Water
+   "Medium in the component"  annotation (choices(choice(redeclare package
+          Medium =
+            AixLib.Media.Water
+              "Water")), Dialog(enable=use_pools,tab="Moisture", group="Pools"));
+  parameter Integer nPools(min=1)=1  "Number of pools in thermal zone" annotation(Dialog(enable=use_pools,tab="Moisture", group="Pools"));
+  replaceable parameter  AixLib.DataBase.Pools.IndoorSwimmingPoolBaseDataDefinition poolParam[nPools]=
+     fill(DataBase.Pools.IndoorSwimmingPoolDummy(), nPools) if use_pools
+    "Setup for swimming pools" annotation (Dialog(
+      enable=use_pools,
+      tab="Moisture",
+      group="Pools"));
+  replaceable parameter AixLib.DataBase.Walls.WallBaseDataDefinition poolWallParam[nPools] = fill(DataBase.Walls.ASHRAE140.DummyDefinition(), nPools) if use_pools "Setup for swimming pool walls"
+                                                                                                                                                                                                  annotation(Dialog(enable=use_pools,tab="Moisture", group="Pools"));
+
+  replaceable parameter DataBase.ThermalZones.ZoneBaseRecord zoneParam
+    "Choose setup for this zone" annotation (choicesAllMatching=true);
+
   AixLib.BoundaryConditions.InternalGains.Humans.HumanSensibleHeatTemperatureDependent humanSenHeaDependent(
     final ratioConv=zoneParam.ratioConvectiveHeatPeople,
     final roomArea=zoneParam.AZone,
@@ -128,20 +148,19 @@ model ThermalZone "Thermal zone containing moisture balance"
         extent={{3,-3},{-3,3}},
         rotation=90,
         origin={-36,95})));
-  BoundaryConditions.SolarIrradiation.DiffusePerez HDifTilWall[zoneParam.nOrientations]
-    (
+  BoundaryConditions.SolarIrradiation.DiffusePerez HDifTilWall[zoneParam.nOrientations](
     each final outSkyCon=true,
     each final outGroCon=true,
     final azi=zoneParam.aziExtWalls,
     final til=zoneParam.tiltExtWalls)
     "Calculates diffuse solar radiation on titled surface for both directions"
     annotation (Placement(transformation(extent={{-84,10},{-68,26}})));
-  BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilWall[zoneParam.nOrientations]
-    (final azi=zoneParam.aziExtWalls, final til=zoneParam.tiltExtWalls)
+  BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilWall[zoneParam.nOrientations](
+     final azi=zoneParam.aziExtWalls, final til=zoneParam.tiltExtWalls)
     "Calculates direct solar radiation on titled surface for both directions"
     annotation (Placement(transformation(extent={{-84,31},{-68,48}})));
-  BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[zoneParam.nOrientationsRoof]
-    (final azi=zoneParam.aziRoof, final til=zoneParam.tiltRoof)
+  BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[zoneParam.nOrientationsRoof](
+     final azi=zoneParam.aziRoof, final til=zoneParam.tiltRoof)
     "Calculates direct solar radiation on titled surface for roof"
     annotation (Placement(transformation(extent={{-84,82},{-68,98}})));
 
@@ -225,8 +244,8 @@ model ThermalZone "Thermal zone containing moisture balance"
      > 0) and use_NaturalAirExchange and use_MechanicalAirExchange
     "Mixes temperature of infiltration flow and mechanical ventilation flow"
     annotation (Placement(transformation(extent={{-56,-4},{-48,4}})));
-  HighOrder.Components.DryAir.VarAirExchange airExc(final V=zoneParam.VAir) if
-       (ATot > 0 or zoneParam.VAir > 0) and  (use_NaturalAirExchange or use_MechanicalAirExchange) and not use_moisture_balance
+  HighOrder.Components.DryAir.VarAirExchange airExc(final V=zoneParam.VAir)
+    if (ATot > 0 or zoneParam.VAir > 0) and  (use_NaturalAirExchange or use_MechanicalAirExchange) and not use_moisture_balance
     "Heat flow due to ventilation"
     annotation (Placement(transformation(extent={{-22,-14},{-6,2}})));
 
@@ -254,20 +273,21 @@ model ThermalZone "Thermal zone containing moisture balance"
   // Moisture
   Modelica.Blocks.Math.MultiSum SumQLat1_flow(nu=2) if (ATot > 0 or
     zoneParam.VAir > 0) and use_moisture_balance and not (use_NaturalAirExchange or use_MechanicalAirExchange)
-    annotation (Placement(transformation(extent={{-40,-68},{-28,-56}})));
-  Modelica.Blocks.Math.MultiSum SumQLat2_flow(nu=3) if (ATot > 0 or
-    zoneParam.VAir > 0) and use_moisture_balance and (use_NaturalAirExchange or use_MechanicalAirExchange)
-    annotation (Placement(transformation(extent={{-40,-68},{-28,-56}})));
+    annotation (Placement(transformation(extent={{-48,-58},{-38,-48}})));
+  Modelica.Blocks.Math.MultiSum SumQLat2_flow(nu=3) if (ATot > 0 or zoneParam.VAir >
+    0) and use_moisture_balance and (use_NaturalAirExchange or
+    use_MechanicalAirExchange)
+    annotation (Placement(transformation(extent={{-48,-58},{-38,-48}})));
   BoundaryConditions.InternalGains.Moisture.MoistureGains moistureGains(
     final roomArea=zoneParam.AZone,
     final specificMoistureProduction=zoneParam.internalGainsMoistureNoPeople)
     if ATot > 0 and use_moisture_balance
     "Internal moisture gains by plants, etc."
     annotation (Dialog(enable=use_moisture_balance, tab="Moisture"),
-      Placement(transformation(extent={{-70,-78},{-60,-68}})));
+      Placement(transformation(extent={{-70,-68},{-62,-60}})));
   Modelica.Blocks.Sources.Constant noMoisturePerson(k=0)
     if internalGainsMode <> 3 and use_moisture_balance
-    annotation (Placement(transformation(extent={{-58,-66},{-50,-58}})));
+    annotation (Placement(transformation(extent={{-70,-58},{-62,-50}})));
   Modelica.Blocks.Interfaces.RealOutput X_w
     if (ATot > 0 or zoneParam.VAir > 0) and use_moisture_balance
     "Humidity output" annotation (Placement(transformation(extent={{100,-80},{
@@ -279,7 +299,7 @@ model ThermalZone "Thermal zone containing moisture balance"
     min=0) if (ATot > 0 or zoneParam.VAir > 0) and use_moisture_balance and use_MechanicalAirExchange
     "Ventilation and infiltration humidity" annotation (Placement(
         transformation(extent={{-128,-108},{-88,-68}}), iconTransformation(
-          extent={{-106,-82},{-84,-60}})));
+          extent={{-110,-84},{-88,-62}})));
   HighOrder.Components.MoistAir.VarMoistAirExchange airExcMoi(final V=zoneParam.VAir) if (ATot
      > 0 or zoneParam.VAir > 0) and (use_NaturalAirExchange or
     use_MechanicalAirExchange) and use_moisture_balance
@@ -296,7 +316,7 @@ model ThermalZone "Thermal zone containing moisture balance"
     final areaBod=areaBod,
     final metOnePerSit=metOnePerSit) if (ATot > 0 or zoneParam.VAir > 0) and
     use_C_flow
-    annotation (Placement(transformation(extent={{20,-74},{34,-60}})));
+    annotation (Placement(transformation(extent={{16,-74},{32,-58}})));
   Modelica.Blocks.Interfaces.RealOutput CO2Con if (ATot > 0 or zoneParam.VAir
      > 0) and use_C_flow "CO2 concentration in the thermal zone in ppm"
     annotation (Placement(transformation(extent={{100,-100},{120,-80}}),
@@ -307,8 +327,7 @@ model ThermalZone "Thermal zone containing moisture balance"
     "Mass fraction of co2 in ROM in kg_CO2/ kg_TotalAir"
     annotation (Placement(transformation(extent={{-8,-74},{10,-60}})));
 
-  BoundaryConditions.SolarIrradiation.DiffusePerez HDifTilRoof[zoneParam.nOrientationsRoof]
-    (
+  BoundaryConditions.SolarIrradiation.DiffusePerez HDifTilRoof[zoneParam.nOrientationsRoof](
     each final outSkyCon=false,
     each final outGroCon=false,
     final azi=zoneParam.aziRoof,
@@ -317,11 +336,48 @@ model ThermalZone "Thermal zone containing moisture balance"
     annotation (Placement(transformation(extent={{-84,61},{-68,77}})));
   Modelica.Blocks.Interfaces.RealOutput QIntGains_flow[3](each final quantity="HeatFlowRate",
       each final unit="W") if ATot > 0
-    "Heat flow based on internal gains from persons, machines, and light"
+    "Heat flow based on internal gains from lights[1], machines[2], and persons[3]"
                                                            annotation (
       Placement(transformation(extent={{100,-50},{120,-30}}),
         iconTransformation(extent={{100,-50},{120,-30}})));
+
+    // Pools
+  Fluid.Pools.IndoorSwimmingPool indoorSwimmingPool[nPools](poolParam=poolParam,
+    poolWallParam = poolWallParam,
+    redeclare package WaterMedium = MediumPoolWater,
+    each energyDynamics=energyDynamics)
+    if (ATot > 0 or zoneParam.VAir > 0) and use_moisture_balance and use_pools
+    annotation (Placement(transformation(extent={{-54,-82},{-40,-70}})));
+  Modelica.Blocks.Math.MultiSum SumQPool(nu=nPools) if (ATot > 0 or zoneParam.VAir >
+    0) and use_moisture_balance and use_pools
+    annotation (Placement(transformation(extent={{-28,-82},{-20,-74}})));
+  Modelica.Blocks.Math.MultiSum SumPPool(nu=nPools) if (ATot > 0 or zoneParam.VAir >
+    0) and use_moisture_balance  and use_pools
+    annotation (Placement(transformation(extent={{-28,-82},{-20,-74}})));
+  Modelica.Blocks.Math.MultiSum SumPool_m_flow_add(nu=nPools) if (ATot > 0 or
+    zoneParam.VAir > 0) and use_moisture_balance and use_pools
+    annotation (Placement(transformation(extent={{-28,-82},{-20,-74}})));
+  Modelica.Blocks.Interfaces.RealInput timeOpe
+    if (ATot > 0 or zoneParam.VAir > 0) and use_moisture_balance and use_pools
+    "Input profiles for opening hours for pools" annotation (Placement(
+        transformation(extent={{-20,-20},{20,20}},
+        rotation=90,
+        origin={-58,-108}),
+        iconTransformation(extent={{-12,-12},{12,12}},
+        rotation=90,
+        origin={-70,-84})));
+
+
   // protected: ThermalZone
+
+  Fluid.Pools.BaseClasses.AirFlowMoistureToROM airFlowMoistureToROM(
+    redeclare package AirMedium = Medium,
+    energyDynamics=energyDynamics,
+    nPools=nPools,
+    m_flow_air_nominal=5,
+    VAirLay=zoneParam.VAir)
+    if (ATot > 0 or zoneParam.VAir > 0) and use_moisture_balance and use_pools
+    annotation (Placement(transformation(extent={{-66,-76},{-60,-70}})));
 protected
     Modelica.Blocks.Sources.Constant hConRoof(final k=(zoneParam.hConRoofOut + zoneParam.hRadRoof)*zoneParam.ARoof)
     "Outdoor coefficient of heat transfer for roof" annotation (Placement(transformation(extent={{-14,68},
@@ -343,7 +399,6 @@ protected
     annotation (Placement(transformation(extent={{-6,-6},{6,6}},
     rotation=90,origin={48,36})));
   Modelica.Blocks.Sources.Constant TSoil(final k=zoneParam.TSoil)
- if zoneParam.AFloor > 0
     "Outdoor surface temperature for floor plate"
     annotation (Placement(transformation(extent={{4,-4},{-4,4}},
     rotation=180,origin={39,22})));
@@ -398,7 +453,10 @@ protected
   // protected: MoistAir
   Modelica.Blocks.Sources.RealExpression humVolAirROM(y=ROM.volMoiAir.X_w)
     if (ATot > 0 or zoneParam.VAir > 0) and use_moisture_balance
-    annotation (Placement(transformation(extent={{-70,-58},{-60,-42}})));
+    annotation (Placement(transformation(extent={{-28,-56},{-20,-40}})));
+
+
+
 
   // protected: Outputs
   Modelica.Blocks.Sources.RealExpression QIntGainsInternalDep_flow[3](y={-lights.convHeat.Q_flow
@@ -428,13 +486,15 @@ equation
   connect(intGains[2], machinesSenHea.uRel) annotation (Line(points={{80,-100},{
           80,-94},{78,-94},{78,-88},{48,-88},{48,-46.5},{56,-46.5}}, color={0,0,
           127}));
-  connect(intGains[3], lights.uRel) annotation (Line(points={{80,-86.6667},{80,-86},{50,-86},{50,-68.5},{56,-68.5}},
+  connect(intGains[3], lights.uRel) annotation (Line(points={{80,-93.3333},{80,
+          -86},{50,-86},{50,-68.5},{56,-68.5}},
                                            color={0,0,127}));
   connect(lights.convHeat, ROM.intGainsConv) annotation (Line(points={{75,-62.8},
           {92,-62.8},{92,78},{86,78}}, color={191,0,0}));
   connect(machinesSenHea.convHeat, ROM.intGainsConv) annotation (Line(points={{75,
           -40.8},{92,-40.8},{92,78},{86,78}}, color={191,0,0}));
-  connect(intGains[1], humanSenHeaDependent.uRel) annotation (Line(points={{80,-113.333},{80,-92},{46,-92},{46,-24},{56,-24}},
+  connect(intGains[1], humanSenHeaDependent.uRel) annotation (Line(points={{80,
+          -106.667},{80,-92},{46,-92},{46,-24},{56,-24}},
                                                 color={0,0,127}));
   connect(humanSenHeaDependent.convHeat, ROM.intGainsConv) annotation (Line(
         points={{75,-18},{92,-18},{92,78},{86,78}}, color={191,0,0}));
@@ -442,15 +502,16 @@ equation
          {{86,78},{92,78},{92,-10},{57,-10},{57,-15}}, color={191,0,0}));
   connect(humanSenHeaDependent.radHeat, ROM.intGainsRad) annotation (Line(
         points={{75,-30},{94,-30},{94,82},{86,82}}, color={95,95,95}));
-  connect(intGains[1], humanSenHeaIndependent.uRel) annotation (Line(points={{80,-113.333},{80,-92},{46,-92},{46,-24},{56,-24}},
-                                                          color={0,0,127}));
+  connect(intGains[1], humanSenHeaIndependent.uRel) annotation (Line(points={{80,
+          -106.667},{80,-92},{46,-92},{46,-24},{56,-24}}, color={0,0,127}));
   connect(humanSenHeaIndependent.convHeat, ROM.intGainsConv) annotation (Line(
         points={{75,-18},{92,-18},{92,78},{86,78}}, color={191,0,0}));
   connect(ROM.intGainsConv, humanSenHeaIndependent.TRoom) annotation (Line(
         points={{86,78},{92,78},{92,-10},{57,-10},{57,-15}}, color={191,0,0}));
   connect(humanSenHeaIndependent.radHeat, ROM.intGainsRad) annotation (Line(
         points={{75,-30},{94,-30},{94,82},{86,82}}, color={95,95,95}));
-  connect(intGains[1], humanTotHeaDependent.uRel) annotation (Line(points={{80,-113.333},{80,-92},{46,-92},{46,-24},{56,-24}},
+  connect(intGains[1], humanTotHeaDependent.uRel) annotation (Line(points={{80,
+          -106.667},{80,-92},{46,-92},{46,-24},{56,-24}},
                                                 color={0,0,127}));
   connect(humanTotHeaDependent.convHeat, ROM.intGainsConv) annotation (Line(
         points={{75,-18},{92,-18},{92,78},{86,78}}, color={191,0,0}));
@@ -615,8 +676,8 @@ equation
       points={{-50.8,-26},{-46,-26},{-46,-24},{-41,-24}},
       color={0,0,127},
       smooth=Smooth.None));
-  connect(intGains[1], ventCont.relOccupation) annotation (Line(points={{80,-113.333},{80,-92},{46,-92},{46,-36},{-68,-36},{-68,-30}},
-                                                                         color=
+  connect(intGains[1], ventCont.relOccupation) annotation (Line(points={{80,
+          -106.667},{80,-92},{46,-92},{46,-36},{-66,-36},{-66,-30.8}},   color=
           {0,0,127}));
   connect(ventRate, addInfVen.u2) annotation (Line(points={{-108,-64},{-76,-64},
           {-76,-34},{-44,-34},{-44,-30},{-41,-30}},
@@ -636,8 +697,8 @@ equation
   connect(addInfVen.y, airExc.ventRate) annotation (Line(points={{-29.5,-27},{-24,
           -27},{-24,-12},{-21.2,-12},{-21.2,-11.12}},              color={0,0,
           127}));
-  connect(airExc.port_b, ROM.intGainsConv) annotation (Line(points={{-6,-6},{44,
-          -6},{44,-2},{92,-2},{92,78},{86,78}},color={191,0,0}));
+  connect(airExc.port_b, ROM.intGainsConv) annotation (Line(points={{-6,-6},{58,
+          -6},{58,-2},{92,-2},{92,78},{86,78}},color={191,0,0}));
   connect(weaBus.TDryBul, mixedTemp.temperature_flow2) annotation (Line(
       points={{-100,34},{-86,34},{-86,10},{-80,10},{-80,-0.8},{-55.84,-0.8}},
       color={255,204,51},
@@ -654,16 +715,20 @@ equation
       extent={{-6,3},{-6,3}}));
   if internalGainsMode == 3 then
     connect(humanTotHeaDependent.QLat_flow, SumQLat1_flow.u[1]) annotation (
-        Line(points={{75.6,-16},{92,-16},{92,-4},{8,-4},{8,-54},{-42,-54},{-42,-59.9},
-            {-40,-59.9}}, color={0,0,127}));
+        Line(points={{75.6,-16},{82,-16},{82,-20},{0,-20},{0,-56},{-32,-56},{-32,
+            -42},{-54,-42},{-54,-53.875},{-48,-53.875}},
+                          color={0,0,127}));
     connect(humanTotHeaDependent.QLat_flow, SumQLat2_flow.u[1]) annotation (
-        Line(points={{75.6,-16},{92,-16},{92,-4},{8,-4},{8,-54},{-42,-54},{-42,-59.2},
-            {-40,-59.2}}, color={0,0,127}));
+        Line(points={{75.6,-16},{82,-16},{82,-20},{0,-20},{0,-56},{-32,-56},{
+            -32,-42},{-54,-42},{-54,-54},{-48,-54},{-48,-54.1667}},
+                          color={0,0,127}));
   else
-    connect(noMoisturePerson.y, SumQLat1_flow.u[1]) annotation (Line(points={{-49.6,
-            -62},{-40,-62},{-40,-59.9}}, color={0,0,127}));
-    connect(noMoisturePerson.y, SumQLat2_flow.u[1]) annotation (Line(points={{-49.6,
-            -62},{-40,-62},{-40,-59.2}}, color={0,0,127}));
+    connect(noMoisturePerson.y, SumQLat1_flow.u[1]) annotation (Line(points={{-61.6,
+            -54},{-54,-54},{-54,-53.875},{-48,-53.875}},
+                                         color={0,0,127}));
+    connect(noMoisturePerson.y, SumQLat2_flow.u[1]) annotation (Line(points={{-61.6,
+            -54},{-54,-54},{-54,-54.1667},{-48,-54.1667}},
+                                         color={0,0,127}));
   end if;
 
 
@@ -678,7 +743,7 @@ if use_NaturalAirExchange and not use_MechanicalAirExchange then
       extent={{-6,3},{-6,3}},
       horizontalAlignment=TextAlignment.Right));
     connect(ventCont.y, cO2Balance.airExc) annotation (Line(
-      points={{-50.8,-26},{-46,-26},{-46,-34},{12,-34},{12,-64.9},{20,-64.9}},
+      points={{-50.8,-26},{-46,-26},{-46,-34},{12,-34},{12,-63.6},{16,-63.6}},
       color={0,0,127},
       pattern=LinePattern.Dash));
     connect(ventCont.y, airExcMoi.ventRate) annotation (Line(
@@ -695,7 +760,7 @@ if use_NaturalAirExchange and not use_MechanicalAirExchange then
       pattern=LinePattern.Dash));
 elseif use_MechanicalAirExchange and not use_NaturalAirExchange then
     connect(ventRate, cO2Balance.airExc) annotation (Line(
-      points={{-108,-64},{-76,-64},{-76,-34},{12,-34},{12,-64.9},{20,-64.9}},
+      points={{-108,-64},{-76,-64},{-76,-34},{12,-34},{12,-63.6},{16,-63.6}},
       color={0,0,127},
       pattern=LinePattern.Dash));
     connect(ventRate, airExc.ventRate) annotation (Line(
@@ -713,9 +778,8 @@ elseif use_MechanicalAirExchange and not use_NaturalAirExchange then
               {-21.2,-10}},
       color={0,0,127},
       pattern=LinePattern.Dash));
-else
-     connect(addInfVen.y, cO2Balance.airExc) annotation (Line(points={{-29.5,
-            -27},{-24,-27},{-24,-34},{12,-34},{12,-64.9},{20,-64.9}},
+else connect(addInfVen.y, cO2Balance.airExc) annotation (Line(points={{-29.5,-27},
+            {-24,-27},{-24,-34},{12,-34},{12,-63.6},{16,-63.6}},
                                                             color={0,0,127}));
      connect(addInfVen.y, airExc.ventRate) annotation (Line(points={{-29.5,-27},
             {-24,-27},{-24,-11.12},{-21.2,-11.12}},  color={0,0,127}));
@@ -729,41 +793,43 @@ else
                                                         color={0,0,127}));
 end if;
 
-  connect(moistureGains.QLat_flow, SumQLat1_flow.u[2]) annotation (Line(points={{-59.5,
-          -73},{-52,-73},{-52,-74},{-46,-74},{-46,-64.1},{-40,-64.1}},    color=
+  connect(moistureGains.QLat_flow, SumQLat1_flow.u[2]) annotation (Line(points={{-61.6,
+          -64},{-54,-64},{-54,-52.125},{-48,-52.125}},                    color=
          {0,0,127}));
-  connect(moistureGains.QLat_flow, SumQLat2_flow.u[2]) annotation (Line(points={
-          {-59.5,-73},{-52,-73},{-52,-74},{-46,-74},{-46,-62},{-40,-62}}, color=
+  connect(moistureGains.QLat_flow, SumQLat2_flow.u[2]) annotation (Line(points={{-61.6,
+          -64},{-54,-64},{-54,-53},{-48,-53}},                            color=
          {0,0,127}));
-  connect(SumQLat1_flow.y, ROM.QLat_flow) annotation (Line(points={{-26.98,-62},
-          {2,-62},{2,4},{32,4},{32,62},{37,62}}, color={0,0,127}));
-  connect(SumQLat2_flow.y, ROM.QLat_flow) annotation (Line(points={{-26.98,-62},
-          {2,-62},{2,4},{32,4},{32,62},{37,62}}, color={0,0,127}));
-  connect(humVolAirROM.y, X_w) annotation (Line(points={{-59.5,-50},{4,-50},{4,
-          -6},{96,-6},{96,-70},{110,-70}},
+  connect(SumQLat1_flow.y, ROM.QLat_flow) annotation (Line(points={{-37.15,-53},
+          {6,-53},{6,-44},{30,-44},{30,62},{37,62}},
+                                                 color={0,0,127}));
+  connect(SumQLat2_flow.y, ROM.QLat_flow) annotation (Line(points={{-37.15,-53},
+          {6,-53},{6,-44},{30,-44},{30,62},{37,62}},
+                                                 color={0,0,127}));
+  connect(humVolAirROM.y, X_w) annotation (Line(points={{-19.6,-48},{52,-48},{52,
+          -8},{86,-8},{86,-76},{96,-76},{96,-70},{110,-70}},
                                        color={0,0,127}));
-  connect(cO2Balance.uRel, intGains[1]) annotation (Line(points={{20,-61.4},{20,
-          -50},{46,-50},{46,-113.333},{80,-113.333}},            color={0,0,127}));
-  connect(cO2Balance.TAir, TAir) annotation (Line(points={{27,-60},{26,-60},{26,
+  connect(cO2Balance.uRel, intGains[1]) annotation (Line(points={{16,-59.6},{16,
+          -54},{46,-54},{46,-106.667},{80,-106.667}},            color={0,0,127}));
+  connect(cO2Balance.TAir, TAir) annotation (Line(points={{24,-58},{26,-58},{26,
           0},{96,0},{96,80},{110,80}},
                          color={0,0,127}));
-  connect(cO2Balance.CO2Con, CO2Con) annotation (Line(points={{34.7,-71.2},{40,
-          -71.2},{40,-82},{94,-82},{94,-90},{110,-90}},
+  connect(cO2Balance.CO2Con, CO2Con) annotation (Line(points={{32.8,-70.8},{40,-70.8},
+          {40,-82},{94,-82},{94,-90},{110,-90}},
                                color={0,0,127}));
-  connect(cO2Balance.XCO2, XCO2.y) annotation (Line(points={{20,-68.4},{20,-67},
+  connect(cO2Balance.XCO2, XCO2.y) annotation (Line(points={{16,-67.6},{16,-67},
           {10.9,-67}}, color={0,0,127}));
   connect(ROM.C_flow[1], cO2Balance.mCO2_flow) annotation (Line(points={{37,84},
-          {34,84},{34,-6},{50,-6},{50,-62.8},{34.7,-62.8}}, color={0,0,127}));
+          {34,84},{34,-62},{32.8,-62},{32.8,-61.2}},        color={0,0,127}));
   connect(airExcMoi.port_a, preTemVen.port)    annotation (Line(points={{-22,-6},
           {-26,-6},{-26,-1},{-32,-1}},           color={191,0,0}));
   connect(airExcMoi.port_b, ROM.intGainsConv) annotation (Line(points={{-6,-6},
           {58,-6},{58,78},{86,78}}, color={191,0,0}));
   connect(airExcMoi.QLat_flow, SumQLat2_flow.u[3]) annotation (Line(points={{-5.68,
-          -10.96},{-6,-10.96},{-6,-40},{-42,-40},{-42,-64.8},{-40,-64.8}},
+          -10.96},{0,-10.96},{0,-56},{-32,-56},{-32,-42},{-54,-42},{-54,
+          -51.8333},{-48,-51.8333}},
         color={0,0,127}));
-  connect(humVolAirROM.y, airExcMoi.HumOut) annotation (Line(points={{-59.5,-50},
-          {-4,-50},{-4,0},{-6,0},{-6,-1.84},{-6.8,-1.84}},
-                                                         color={0,0,127}));
+  connect(humVolAirROM.y, airExcMoi.HumOut) annotation (Line(points={{-19.6,-48},
+          {-2,-48},{-2,-1.84},{-6.8,-1.84}},             color={0,0,127}));
   connect(ventHum, mixedHumidity.humidity_flow1) annotation (Line(points={{-108,
           -88},{-74,-88},{-74,-4.88},{-55.84,-4.88}}, color={0,0,127}));
   connect(ventRate, mixedHumidity.flowRate_flow1) annotation (Line(points={{-108,
@@ -807,7 +873,56 @@ end if;
           -40},{110,-40}},                   color={0,0,127}));
   connect(QIntGainsInternalTot_flow.y, QIntGains_flow) annotation (Line(points={{98.2,
           -40},{110,-40}},                   color={0,0,127}));
-  annotation (Documentation(revisions="<html><ul>
+
+  if use_pools then
+    for i in 1:nPools loop
+      connect(indoorSwimmingPool[i].radPool, ROM.intGainsRad) annotation (Line(points={{-44.9,
+              -70},{-44,-70},{-44,-68},{-36,-68},{-36,-88},{96,-88},{96,82},{86,
+              82}},color={0,0,0}));
+      connect(indoorSwimmingPool[i].convPool, ROM.intGainsConv) annotation (Line(
+        points={{-41.82,-69.76},{-41.82,-70},{-42,-70},{-42,-66},{-10,-66},{-10,
+              -40},{20,-40},{20,-6},{58,-6},{58,78},{86,78}},
+                        color={191,0,0}));
+      connect(indoorSwimmingPool[i].TAir, ROM.TAir) annotation (Line(points={{-51.69,
+              -69.82},{-51.69,-62},{-16,-62},{-16,-52},{26,-52},{26,0},{98,0},{98,
+              90},{87,90}},
+        color={0,0,127}));
+      connect(TSoil.y, indoorSwimmingPool[i].TSoil) annotation (Line(points={{43.4,22},
+              {46,22},{46,-8},{36,-8},{36,-84},{-16,-84},{-16,-68},{-34,-68},{-34,
+              -73.18},{-39.79,-73.18}},
+        color={0,0,127}));
+      connect(indoorSwimmingPool[i].QPool, SumQPool.u[i]) annotation (Line(points={{-39.44,
+              -76.36},{-39.44,-78},{-28,-78}},                color={0,0,127}));
+      connect(indoorSwimmingPool[i].PPool, SumPPool.u[i]) annotation (Line(points={{-39.44,
+              -80.56},{-32,-80.56},{-32,-78},{-28,-78}},
+                                                   color={0,0,127}));
+      connect(indoorSwimmingPool[i].m_flow_add_out, SumPool_m_flow_add.u[i])   annotation (Line(points={{-39.44,
+              -81.52},{-32,-81.52},{-32,-78},{-28,-78}},                                                                                        color={0,0,
+          127}));
+      connect(intGains[1], indoorSwimmingPool[i].uRelPer) annotation (Line(points={{80,
+              -106.667},{80,-94},{-62,-94},{-62,-77.62},{-54.49,-77.62}},
+                                        color={0,0,127}));
+      connect(indoorSwimmingPool[i].timeOpe, timeOpe) annotation (Line(points={{-54.42,
+              -79.48},{-54.42,-78},{-58,-78},{-58,-108}},
+                                                     color={0,0,127}));
+      connect(humVolAirROM.y, indoorSwimmingPool[i].X_w) annotation (Line(points={{-19.6,
+          -48},{-18,-48},{-18,-64},{-49.03,-64},{-49.03,-69.82}}, color={0,0,127}));
+      connect(airFlowMoistureToROM.port_b, ROM.ports[1+nPorts]) annotation (Line(
+            points={{-65.94,-73.72},{-65.94,-74},{-72,-74},{-72,8},{58,8},{58,
+              50},{77,50},{77,56.05}}, color={0,127,255}));
+      connect(airFlowMoistureToROM.port_a, ROM.ports[2+nPorts]) annotation (Line(
+            points={{-66,-72.28},{-72,-72.28},{-72,8},{58,8},{58,50},{77,50},{
+              77,56.05}}, color={0,127,255}));
+    end for;
+  end if;
+
+  connect(indoorSwimmingPool.QEva, airFlowMoistureToROM.QEva) annotation (Line(
+        points={{-54.28,-71.8},{-57.23,-71.8},{-57.23,-71.92},{-60.18,-71.92}},
+        color={0,0,127}));
+  connect(indoorSwimmingPool.m_flow_eva, airFlowMoistureToROM.m_flow_eva)
+    annotation (Line(points={{-54.42,-73.24},{-57.25,-73.24},{-57.25,-74.11},{-60.15,
+          -74.11}}, color={0,0,127}));
+   annotation (Documentation(revisions="<html><ul>
   <li>November 20, 2020, by Katharina Breuer:<br/>
     Combine thermal zone models
   </li>
@@ -1009,12 +1124,12 @@ end if;
           textString="Heating
 Cooling"),
         Rectangle(
-          extent={{-72,-42},{-22,-80}},
+          extent={{-72,-40},{-14,-86}},
           lineColor={0,0,255},
           fillColor={215,215,215},
           fillPattern=FillPattern.Solid),
         Text(
-          extent={{-48,-42},{-30,-50}},
+          extent={{-72,-40},{-56,-48}},
           lineColor={0,0,255},
           fillColor={212,221,253},
           fillPattern=FillPattern.Solid,
@@ -1032,7 +1147,7 @@ Cooling"),
           textString="Ventilation
 Infiltration
 "),     Rectangle(
-          extent={{-12,-42},{38,-80}},
+          extent={{-12,-40},{38,-80}},
           lineColor={0,0,255},
           fillColor={215,215,215},
           fillPattern=FillPattern.Solid),
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase600.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase600.mo
index 1004973517..33adaa7bc8 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase600.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase600.mo
@@ -151,7 +151,7 @@ model TestCase600 "Test case 600"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -166,7 +166,7 @@ model TestCase600 "Test case 600"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase600FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase600FF.mo
index 4824809380..cf5b555a08 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase600FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase600FF.mo
@@ -148,7 +148,7 @@ model TestCase600FF "Test case 600 free floating"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -163,7 +163,7 @@ model TestCase600FF "Test case 600 free floating"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Math.UnitConversions.To_degC to_degC
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase620.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase620.mo
index ad661efbf8..23edf1a9ac 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase620.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase620.mo
@@ -151,7 +151,7 @@ model TestCase620 "Test case 620"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -166,7 +166,7 @@ model TestCase620 "Test case 620"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase640.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase640.mo
index 417da00894..f6613ff9e2 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase640.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase640.mo
@@ -151,7 +151,7 @@ model TestCase640 "Test case 640"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -166,7 +166,7 @@ model TestCase640 "Test case 640"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase650.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase650.mo
index e22b84b713..fa8437d708 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase650.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase650.mo
@@ -147,7 +147,7 @@ model TestCase650 "Test case 650"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -162,7 +162,7 @@ model TestCase650 "Test case 650"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase650FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase650FF.mo
index 8c33db81ba..1ef043331f 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase650FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase650FF.mo
@@ -146,7 +146,7 @@ model TestCase650FF "Test case 650 free float"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -161,7 +161,7 @@ model TestCase650FF "Test case 650 free float"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase900.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase900.mo
index 7bc0736608..3d00cb39c6 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase900.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase900.mo
@@ -153,7 +153,7 @@ model TestCase900 "Test case 900"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -168,7 +168,7 @@ model TestCase900 "Test case 900"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase900FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase900FF.mo
index e4ccff6866..c5617eb071 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase900FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase900FF.mo
@@ -150,7 +150,7 @@ model TestCase900FF "Test case 900 free floating"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -165,7 +165,7 @@ model TestCase900FF "Test case 900 free floating"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Math.UnitConversions.To_degC to_degC
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase920.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase920.mo
index 7a17649366..c9b28be4e5 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase920.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase920.mo
@@ -152,7 +152,7 @@ model TestCase920 "Test case 920"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -167,7 +167,7 @@ model TestCase920 "Test case 920"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase940.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase940.mo
index 3c27816e03..8e67ce4eb4 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase940.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase940.mo
@@ -153,7 +153,7 @@ model TestCase940 "Test case 940"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -168,7 +168,7 @@ model TestCase940 "Test case 940"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase950.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase950.mo
index 8132983ada..6e2d28ab4e 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase950.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase950.mo
@@ -149,7 +149,7 @@ model TestCase950 "Test case 950"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -164,7 +164,7 @@ model TestCase950 "Test case 950"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase950FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase950FF.mo
index a2d9fcb0f4..0bc55dd1b3 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase950FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/FourElements/TestCase950FF.mo
@@ -148,7 +148,7 @@ model TestCase950FF "Test case 950 free float"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -163,7 +163,7 @@ model TestCase950FF "Test case 950 free float"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface HDirTilRoof[1]
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase600.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase600.mo
index 0e6acbb5fa..6b7c8bd823 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase600.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase600.mo
@@ -133,7 +133,7 @@ model TestCase600 "Test case 600"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -148,7 +148,7 @@ model TestCase600 "Test case 600"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase600FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase600FF.mo
index 28f500bd84..f8eb810794 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase600FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase600FF.mo
@@ -130,7 +130,7 @@ model TestCase600FF "Test case 600 free floating"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -145,7 +145,7 @@ model TestCase600FF "Test case 600 free floating"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Math.UnitConversions.To_degC to_degC
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase620.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase620.mo
index 13c6415fdc..3ce40949ab 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase620.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase620.mo
@@ -133,7 +133,7 @@ model TestCase620 "Test case 620"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -148,7 +148,7 @@ model TestCase620 "Test case 620"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase640.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase640.mo
index e2b9fc8ebf..4502e0d96e 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase640.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase640.mo
@@ -133,7 +133,7 @@ model TestCase640 "Test case 640"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -148,7 +148,7 @@ model TestCase640 "Test case 640"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase650.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase650.mo
index d11dde95bc..1daf2f49ab 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase650.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase650.mo
@@ -129,7 +129,7 @@ model TestCase650 "Test case 650"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -144,7 +144,7 @@ model TestCase650 "Test case 650"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow coo "Ideal cooler"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase650FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase650FF.mo
index e21e102942..f4ee6fdefa 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase650FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase650FF.mo
@@ -128,7 +128,7 @@ model TestCase650FF "Test case 650 free float"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -143,7 +143,7 @@ model TestCase650FF "Test case 650 free float"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Sources.CombiTimeTable InfVen(
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase900.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase900.mo
index 18882ed8a8..bf8378b457 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase900.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase900.mo
@@ -133,7 +133,7 @@ model TestCase900 "Test case 900"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -148,7 +148,7 @@ model TestCase900 "Test case 900"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase900FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase900FF.mo
index 22d6174c39..43b44a21c8 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase900FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase900FF.mo
@@ -130,7 +130,7 @@ model TestCase900FF "Test case 900 free floating"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -145,7 +145,7 @@ model TestCase900FF "Test case 900 free floating"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Math.UnitConversions.To_degC to_degC
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase920.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase920.mo
index fe30d86fed..6448c021c3 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase920.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase920.mo
@@ -129,7 +129,7 @@ model TestCase920 "Test case 920"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -144,7 +144,7 @@ model TestCase920 "Test case 920"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase940.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase940.mo
index dde02e3cd4..182ccd482d 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase940.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase940.mo
@@ -129,7 +129,7 @@ model TestCase940 "Test case 940"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -144,7 +144,7 @@ model TestCase940 "Test case 940"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase950.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase950.mo
index b42352e288..02f6f4d712 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase950.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase950.mo
@@ -129,7 +129,7 @@ model TestCase950 "Test case 950"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -144,7 +144,7 @@ model TestCase950 "Test case 950"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow coo "Ideal cooler"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase950FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase950FF.mo
index 4781b30040..757c0d9037 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase950FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/OneElement/TestCase950FF.mo
@@ -128,7 +128,7 @@ model TestCase950FF "Test case 950 free float"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -143,7 +143,7 @@ model TestCase950FF "Test case 950 free float"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Sources.CombiTimeTable InfVen(
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase600.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase600.mo
index 0ad7bea8d2..6fa02e9644 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase600.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase600.mo
@@ -144,7 +144,7 @@ model TestCase600 "Test case 600"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -159,7 +159,7 @@ model TestCase600 "Test case 600"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase600FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase600FF.mo
index d07e0d02ae..29a96c6299 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase600FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase600FF.mo
@@ -141,7 +141,7 @@ model TestCase600FF "Test case 600 free floating"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -156,7 +156,7 @@ model TestCase600FF "Test case 600 free floating"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Math.UnitConversions.To_degC to_degC
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase620.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase620.mo
index 31a97510a0..95ee3e84c3 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase620.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase620.mo
@@ -145,7 +145,7 @@ model TestCase620 "Test case 620"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -160,7 +160,7 @@ model TestCase620 "Test case 620"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase640.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase640.mo
index 6400cf494d..9505d2ccce 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase640.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase640.mo
@@ -144,7 +144,7 @@ model TestCase640 "Test case 640"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -159,7 +159,7 @@ model TestCase640 "Test case 640"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase650.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase650.mo
index 2a3d0ddc08..d743a251d8 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase650.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase650.mo
@@ -140,7 +140,7 @@ model TestCase650 "Test case 650"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -155,7 +155,7 @@ model TestCase650 "Test case 650"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow coo "Ideal cooler"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase650FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase650FF.mo
index e3c5009256..8548e1be05 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase650FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase650FF.mo
@@ -139,7 +139,7 @@ model TestCase650FF "Test case 650 free float"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -154,7 +154,7 @@ model TestCase650FF "Test case 650 free float"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Sources.CombiTimeTable InfVen(
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase900.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase900.mo
index 63132e1542..7318ab99a8 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase900.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase900.mo
@@ -146,7 +146,7 @@ model TestCase900 "Test case 900"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -161,7 +161,7 @@ model TestCase900 "Test case 900"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase900FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase900FF.mo
index bd6314f77c..302a45535d 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase900FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase900FF.mo
@@ -143,7 +143,7 @@ model TestCase900FF "Test case 900 free floating"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -158,7 +158,7 @@ model TestCase900FF "Test case 900 free floating"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Math.UnitConversions.To_degC to_degC
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase920.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase920.mo
index 775f8f9266..d2b1ecb659 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase920.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase920.mo
@@ -146,7 +146,7 @@ model TestCase920 "Test case 920"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -161,7 +161,7 @@ model TestCase920 "Test case 920"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase940.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase940.mo
index 94e172f9c8..b1cad9a2c4 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase940.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase940.mo
@@ -146,7 +146,7 @@ model TestCase940 "Test case 940"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -161,7 +161,7 @@ model TestCase940 "Test case 940"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow hea "Ideal heater"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase950.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase950.mo
index 7710de5219..fa652c36dc 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase950.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase950.mo
@@ -142,7 +142,7 @@ model TestCase950 "Test case 950"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -157,7 +157,7 @@ model TestCase950 "Test case 950"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Thermal.HeatTransfer.Sources.PrescribedHeatFlow coo "Ideal cooler"
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase950FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase950FF.mo
index 351633076a..ed9fcde1b6 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase950FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/ThreeElements/TestCase950FF.mo
@@ -141,7 +141,7 @@ model TestCase950FF "Test case 950 free float"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -156,7 +156,7 @@ model TestCase950FF "Test case 950 free float"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Sources.CombiTimeTable InfVen(
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase600.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase600.mo
index 13753762ff..eb19e53b0a 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase600.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase600.mo
@@ -188,7 +188,7 @@ model TestCase600 "Test case 600"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -203,7 +203,7 @@ model TestCase600 "Test case 600"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Continuous.Integrator integrator
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase600FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase600FF.mo
index 86e1b84c64..17fd39309f 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase600FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase600FF.mo
@@ -136,7 +136,7 @@ model TestCase600FF "Test case 600 free floating"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -151,7 +151,7 @@ model TestCase600FF "Test case 600 free floating"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Math.UnitConversions.To_degC to_degC
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase620.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase620.mo
index fb9774ebdf..242c9fc05a 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase620.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase620.mo
@@ -175,7 +175,7 @@ model TestCase620 "Test case 620"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -190,7 +190,7 @@ model TestCase620 "Test case 620"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Continuous.Integrator integrator
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase640.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase640.mo
index c4bb51e9b8..83a46a5d42 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase640.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase640.mo
@@ -173,7 +173,7 @@ model TestCase640 "Test case 640"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -188,7 +188,7 @@ model TestCase640 "Test case 640"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Continuous.Integrator integrator
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase650.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase650.mo
index 7be030fef3..dbe752324b 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase650.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase650.mo
@@ -151,7 +151,7 @@ model TestCase650 "Test case 650"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -166,7 +166,7 @@ model TestCase650 "Test case 650"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Continuous.Integrator integrator
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase650FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase650FF.mo
index 11daf8ca4c..424c13fd6b 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase650FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase650FF.mo
@@ -134,7 +134,7 @@ model TestCase650FF "Test case 650 free float"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -149,7 +149,7 @@ model TestCase650FF "Test case 650 free float"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Sources.CombiTimeTable InfVen(
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase900.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase900.mo
index 2a8238a4ff..e2be9a8dcf 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase900.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase900.mo
@@ -175,7 +175,7 @@ model TestCase900 "Test case 900"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -190,7 +190,7 @@ model TestCase900 "Test case 900"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Continuous.Integrator integrator
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase900FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase900FF.mo
index b76a9576b9..d5c7297553 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase900FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase900FF.mo
@@ -136,7 +136,7 @@ model TestCase900FF "Test case 900 free floating"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -151,7 +151,7 @@ model TestCase900FF "Test case 900 free floating"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Math.UnitConversions.To_degC to_degC
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase920.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase920.mo
index e1031e343a..860a9f5b9e 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase920.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase920.mo
@@ -175,7 +175,7 @@ model TestCase920 "Test case 920"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -190,7 +190,7 @@ model TestCase920 "Test case 920"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Continuous.Integrator integrator
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase940.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase940.mo
index 03e0921b82..8f7f1a7f53 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase940.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase940.mo
@@ -173,7 +173,7 @@ model TestCase940 "Test case 940"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -188,7 +188,7 @@ model TestCase940 "Test case 940"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Continuous.Integrator integrator
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase950.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase950.mo
index e7412af2f4..e44c0c52ed 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase950.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase950.mo
@@ -151,7 +151,7 @@ model TestCase950 "Test case 950"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -166,7 +166,7 @@ model TestCase950 "Test case 950"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Continuous.Integrator integrator
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase950FF.mo b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase950FF.mo
index c811f0e3a3..b3d93c6a0b 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase950FF.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/ASHRAE140/TwoElements/TestCase950FF.mo
@@ -134,7 +134,7 @@ model TestCase950FF "Test case 950 free float"
     columns={2,3,4},
     tableName="Table",
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.mat"))
+    "modelica://AixLib/Resources/WeatherData/WeatherData_Ashrae140_LOM.txt"))
     "Weather data"
     annotation (Placement(transformation(extent={{-136,74},{-116,94}})));
   Modelica.Blocks.Math.Add add(k2=-1)
@@ -149,7 +149,7 @@ model TestCase950FF "Test case 950 free float"
     tableName="Table",
     columns={2,3},
     fileName=Modelica.Utilities.Files.loadResource(
-    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.mat"))
+    "modelica://AixLib/Resources/WeatherData/Weatherdata_ASHARE140.txt"))
     "Solar radiation data"
     annotation (Placement(transformation(extent={{-136,4},{-116,24}})));
   Modelica.Blocks.Sources.CombiTimeTable InfVen(
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/RoomSteadyState.mo b/AixLib/ThermalZones/ReducedOrder/Validation/RoomSteadyState.mo
index 4fcc12d249..eedb0eb302 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/RoomSteadyState.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/RoomSteadyState.mo
@@ -35,17 +35,17 @@ equation
     Diagram(coordinateSystem(extent={{-140,-100},{100,100}})),
     Icon(coordinateSystem(extent={{-100,-100},{100,100}})),
     Documentation(info="<html>
- <p>
- This model validates that the RC network model starts at and remains at exactly <i>20</i>&deg;C
- if there is no solar radiation and constant outdoor conditions.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2020, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model validates that the RC network model starts at and remains at exactly <i>20</i>&deg;C
+if there is no solar radiation and constant outdoor conditions.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2020, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RoomSteadyState;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/RoomWithLatentGain.mo b/AixLib/ThermalZones/ReducedOrder/Validation/RoomWithLatentGain.mo
index a667297cf3..ed3916cbf5 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/RoomWithLatentGain.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/RoomWithLatentGain.mo
@@ -14,11 +14,13 @@ model RoomWithLatentGain
       startTime3=0,
       endTime3=0));
   Fluid.Sensors.RelativeHumidity senRelHum(
-    redeclare package Medium = Medium)
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "Relative humidity of room air"
     annotation (Placement(transformation(extent={{110,-20},{130,0}})));
   Fluid.Sensors.MassFraction senMasFra(
-    redeclare package Medium = Medium)
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "Absolute humidity of room air in kg/kg total air"
     annotation (Placement(transformation(extent={{110,-50},{130,-30}})));
 equation
@@ -29,22 +31,28 @@ equation
   connect(intGai.y[2], thermalZoneTwoElements.QLat_flow) annotation (Line(
         points={{22.8,-52},{32,-52},{32,4},{43,4},{43,4}}, color={0,0,127}));
   annotation (Documentation(info="<html>
- <p>
- Test Case 12 of the VDI 6007 Part 1: Calculation of indoor air temperature
- excited by a radiative and convective heat source for room version S.</p>
- <h4>Boundary conditions</h4>
- <p>
- This test case changes the medium to moist air, and adds latent heat gain.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 9, 2019, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1209\">IBPSA, issue 1209</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Test Case 12 of the VDI 6007 Part 1: Calculation of indoor air temperature
+excited by a radiative and convective heat source for room version S.</p>
+<h4>Boundary conditions</h4>
+<p>
+This test case changes the medium to moist air, and adds latent heat gain.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2024, by Michael Wetter:<br/>
+Configured the sensor parameter to suppress the warning about being a one-port connection.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1857\">IBPSA, #1857</a>.
+</li>
+<li>
+October 9, 2019, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1209\">IBPSA, issue 1209</a>.
+</li>
+</ul>
+</html>"),
 experiment(
       StopTime=604800,
       Tolerance=1e-06),
@@ -52,6 +60,6 @@ experiment(
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/RoomWithLatentGain.mos"
   "Simulate and plot"),
     Diagram(coordinateSystem(extent={{-140,-100},{140,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
-end RoomWithLatentGain;
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end RoomWithLatentGain;
\ No newline at end of file
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/RoomWithoutLatentGain.mo b/AixLib/ThermalZones/ReducedOrder/Validation/RoomWithoutLatentGain.mo
index 375a3e3862..450ec9b31a 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/RoomWithoutLatentGain.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/RoomWithoutLatentGain.mo
@@ -21,11 +21,13 @@ model RoomWithoutLatentGain
     rotation=0,
     origin={23,3})));
   Fluid.Sensors.RelativeHumidity senRelHum(
-    redeclare package Medium = Medium)
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "Relative humidity of room air"
     annotation (Placement(transformation(extent={{110,-20},{130,0}})));
   Fluid.Sensors.MassFraction senMasFra(
-    redeclare package Medium = Medium)
+    redeclare package Medium = Medium,
+    warnAboutOnePortConnection = false)
     "Absolute humidity of room air in kg/kg total air"
     annotation (Placement(transformation(extent={{110,-50},{130,-30}})));
 equation
@@ -36,22 +38,28 @@ equation
   connect(senMasFra.port, thermalZoneTwoElements.ports[4]) annotation (Line(
         points={{120,-50},{83,-50},{83,-1.95}}, color={0,127,255}));
   annotation (Documentation(info="<html>
- <p>
- Test Case 12 of the VDI 6007 Part 1: Calculation of indoor air temperature
- excited by a radiative and convective heat source for room version S.</p>
- <h4>Boundary conditions</h4>
- <p>
- This test case changes the medium to moist air, and adds zero latent heat gain.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 9, 2019, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1209\">IBPSA, issue 1209</a>.
- </li>
- </ul>
- </html>"),
+<p>
+Test Case 12 of the VDI 6007 Part 1: Calculation of indoor air temperature
+excited by a radiative and convective heat source for room version S.</p>
+<h4>Boundary conditions</h4>
+<p>
+This test case changes the medium to moist air, and adds zero latent heat gain.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 26, 2024, by Michael Wetter:<br/>
+Configured the sensor parameter to suppress the warning about being a one-port connection.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1857\">IBPSA, #1857</a>.
+</li>
+<li>
+October 9, 2019, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1209\">IBPSA, issue 1209</a>.
+</li>
+</ul>
+</html>"),
 experiment(
       StopTime=604800,
       Tolerance=1e-06),
@@ -59,6 +67,6 @@ experiment(
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/RoomWithoutLatentGain.mos"
   "Simulate and plot"),
     Diagram(coordinateSystem(extent={{-140,-100},{140,100}})),
-    Icon(coordinateSystem(extent={{-100,-100},{100,100}})),
-  __Dymola_LockedEditing="Model from IBPSA");
-end RoomWithoutLatentGain;
+    Icon(coordinateSystem(extent={{-100,-100},{100,100}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end RoomWithoutLatentGain;
\ No newline at end of file
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/BaseClasses/VerifyDifferenceThreePeriods.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/BaseClasses/VerifyDifferenceThreePeriods.mo
index dfe12ac39b..f43f4cf73b 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/BaseClasses/VerifyDifferenceThreePeriods.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/BaseClasses/VerifyDifferenceThreePeriods.mo
@@ -77,50 +77,50 @@ equation
 annotation (
 defaultComponentName="verDif",
 Documentation(info="<html>
- <p>
- Block that outputs <code>satisfied = false</code> if
- <code>abs(u1-u2) &gt; threShold</code> within the prescribed time intervals,
- or <code>satisfied = true</code> otherwise.
- </p>
- <h4>Implementation</h4>
- <p>
- The test uses a hysteresis of plus/minus 1% in order to avoid
- chattering if <code>abs(u1-u2)</code> is near <code>threShold</code>.
- </p>
- <p>
- The difference <code>abs(u1-u2)</code> is filtered with a first order filter with time constant <code>tau</code>.
- This guards against rounding errors in event handling by upstream signal-generating blocks.
- </p>
- </html>",
+<p>
+Block that outputs <code>satisfied = false</code> if
+<code>abs(u1-u2) &gt; threShold</code> within the prescribed time intervals,
+or <code>satisfied = true</code> otherwise.
+</p>
+<h4>Implementation</h4>
+<p>
+The test uses a hysteresis of plus/minus 1% in order to avoid
+chattering if <code>abs(u1-u2)</code> is near <code>threShold</code>.
+</p>
+<p>
+The difference <code>abs(u1-u2)</code> is filtered with a first order filter with time constant <code>tau</code>.
+This guards against rounding errors in event handling by upstream signal-generating blocks.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 4, 2021, by Michael Wetter:<br/>
- Added filtering to guard against rounding errors in events of upstream signal generating blocks.<br/>
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2713\">Buildings, #2713</a>.
- </li>
- <li>
- September 7, 2018, by Michael Wetter:<br/>
- Rewrote inequality to turn a state into a time event for Dymola 2019FD01.
- </li>
- <li>
- December 16, 2016, by Michael Wetter:<br/>
- Reformulated model for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/623\">
- https://github.com/ibpsa/modelica-ibpsa/issues/623</a>.
- </li>
- <li>
- October 10, 2013, by Michael Wetter:<br/>
- Reformulated model to allow scheduling of time events as opposed to state events,
- and removed <code>noEvent</code> operator which is not needed as these
- are only time events.
- </li>
- <li>
- June 29, 2016, by Moritz Lauster:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 4, 2021, by Michael Wetter:<br/>
+Added filtering to guard against rounding errors in events of upstream signal generating blocks.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2713\">Buildings, #2713</a>.
+</li>
+<li>
+September 7, 2018, by Michael Wetter:<br/>
+Rewrote inequality to turn a state into a time event for Dymola 2019FD01.
+</li>
+<li>
+December 16, 2016, by Michael Wetter:<br/>
+Reformulated model for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/623\">
+https://github.com/ibpsa/modelica-ibpsa/issues/623</a>.
+</li>
+<li>
+October 10, 2013, by Michael Wetter:<br/>
+Reformulated model to allow scheduling of time events as opposed to state events,
+and removed <code>noEvent</code> operator which is not needed as these
+are only time events.
+</li>
+<li>
+June 29, 2016, by Moritz Lauster:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VerifyDifferenceThreePeriods;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase1.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase1.mo
index 730756e3b0..fc0d7e319d 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase1.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase1.mo
@@ -115,36 +115,35 @@ equation
   connect(reference.y[1], assEqu.u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 1 of the VDI 6007 Part 1: Calculation of indoor air
-   temperature excited by a convective heat source for room version S.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>constant outdoor air temperature 22&deg;C</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>no solar or short-wave radiation through the windows</li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates basic functionalities.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 1 of the VDI 6007 Part 1: Calculation of indoor air
+  temperature excited by a convective heat source for room version S.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>constant outdoor air temperature 22&deg;C</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>no solar or short-wave radiation through the windows</li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates basic functionalities.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase1.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase1;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase10.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase10.mo
index dcbf20a927..aabfe021a0 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase10.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase10.mo
@@ -107,7 +107,7 @@ model TestCase10 "VDI 6007 Test Case 10 model"
     origin={-59,59})));
   Modelica.Blocks.Math.Product product1
     "Solar radiation times g value for sunblind (open or closed) for
-     one direction"
+    one direction"
     annotation (Placement(transformation(extent={{-6,65},{4,75}})));
   Modelica.Blocks.Logical.Switch switch1
     "Determines g value for sunblind (open or closed) for one direction"
@@ -245,41 +245,40 @@ equation
   connect(reference.y[1],assEqu. u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 10 of the VDI 6007 Part 1: Calculation of indoor air temperature
-   excited by a radiative and convective heat source for room version S. It is
-   based on Test Case 5, but with a non-adiabatic floor plate to an adjacent room
-   with a fixed temperature.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>daily profile for outdoor air temperature in hourly steps</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>daily profile for solar radiation through the windows in hourly
-   steps</li>
-   <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates linking to ajdacent rooms with
-   fixed temperature.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 10 of the VDI 6007 Part 1: Calculation of indoor air temperature
+  excited by a radiative and convective heat source for room version S. It is
+  based on Test Case 5, but with a non-adiabatic floor plate to an adjacent room
+  with a fixed temperature.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>daily profile for outdoor air temperature in hourly steps</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>daily profile for solar radiation through the windows in hourly
+  steps</li>
+  <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates linking to ajdacent rooms with
+  fixed temperature.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase10.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase10;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase11.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase11.mo
index 7814857205..dfea3ed5db 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase11.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase11.mo
@@ -261,52 +261,51 @@ equation
   annotation (Diagram(coordinateSystem(preserveAspectRatio=false, extent={{-100,
             -100},{240,160}})),
                       Documentation(info="<html>
-   <p>Test Case 11 of the VDI 6007 Part 1: Calculation of heat load
-   excited with a given radiative heat source and a setpoint profile
-   for room version S. It is based on Test Case 7, but with a cooling ceiling for
-   cooling purposes instead of a pure convective ideal cooler.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>constant outdoor air temperature 22&deg;C</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>no solar or short-wave radiation through the windows</li>
-   <li>no long-wave radiation exchange between exterior wall, windows and ambient
-   environment</li>
-   </ul>
-   <p>This test validates implementation of cooling ceiling or
-   floor heating.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   November 4, 2021, by Michael Wetter:<br/>
-   Increased solver tolerance so that the model passes the assertion in OpenModelica
-   after applying <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2713\">Buildings, #2713</a>.
-   </li>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   January 25, 2019, by Michael Wetter:<br/>
-   Added start value to avoid warning in JModelica.
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds and changes threshold to hysteresis.
-   </li>
-   <li>
-   July 6, 2016, by Michael Wetter:<br/>
-   Simplified implementation of validation test versus reference data.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-7, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 11 of the VDI 6007 Part 1: Calculation of heat load
+  excited with a given radiative heat source and a setpoint profile
+  for room version S. It is based on Test Case 7, but with a cooling ceiling for
+  cooling purposes instead of a pure convective ideal cooler.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>constant outdoor air temperature 22&deg;C</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>no solar or short-wave radiation through the windows</li>
+  <li>no long-wave radiation exchange between exterior wall, windows and ambient
+  environment</li>
+  </ul>
+  <p>This test validates implementation of cooling ceiling or
+  floor heating.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  November 4, 2021, by Michael Wetter:<br/>
+  Increased solver tolerance so that the model passes the assertion in OpenModelica
+  after applying <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/2713\">Buildings, #2713</a>.
+  </li>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  January 25, 2019, by Michael Wetter:<br/>
+  Added start value to avoid warning in JModelica.
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds and changes threshold to hysteresis.
+  </li>
+  <li>
+  July 6, 2016, by Michael Wetter:<br/>
+  Simplified implementation of validation test versus reference data.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-7, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase11.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase11;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase12.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase12.mo
index e91b33e103..3416b792b5 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase12.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase12.mo
@@ -139,7 +139,7 @@ model TestCase12 "VDI 6007 Test Case 12 model"
     origin={-59,59})));
   Modelica.Blocks.Math.Product product1
     "Solar radiation times g value for sunblind (open or closed) for one
-     direction"
+    direction"
     annotation (Placement(transformation(extent={{-6,65},{4,75}})));
   Modelica.Blocks.Logical.Switch switch1
     "Determines g value for sunblind (open or closed) for one direction"
@@ -266,39 +266,38 @@ equation
   connect(reference.y[1],assEqu. u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation (  Documentation(info="<html>
-   <p>Test Case 12 of the VDI 6007 Part 1: Calculation of indoor air temperature
-   excited by a radiative and convective heat source for room version S. It is
-   based of Test Case 5 and adds ventilation.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>daily profile for outdoor air temperature in hourly steps</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>daily profile for solar radiation through the windows in hourly steps</li>
-   <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
-   <li>no long-wave radiation exchange between exterior wall, windows and ambient
-   environment</li>
-   <li>daily profile for ventilation in hourly time steps</li>
-   </ul>
-   <p>This test validates infiltration and ventilation.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 12 of the VDI 6007 Part 1: Calculation of indoor air temperature
+  excited by a radiative and convective heat source for room version S. It is
+  based of Test Case 5 and adds ventilation.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>daily profile for outdoor air temperature in hourly steps</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>daily profile for solar radiation through the windows in hourly steps</li>
+  <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
+  <li>no long-wave radiation exchange between exterior wall, windows and ambient
+  environment</li>
+  <li>daily profile for ventilation in hourly time steps</li>
+  </ul>
+  <p>This test validates infiltration and ventilation.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase12.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase12;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase2.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase2.mo
index 66e50b46d6..1db93018af 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase2.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase2.mo
@@ -115,36 +115,35 @@ equation
   connect(reference.y[1], assEqu.u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 2 of the VDI 6007 Part 1: Calculation of indoor air
-   temperature excited by a radiative heat source for room version S.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>constant outdoor air temperature 22&deg;C</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>no solar or short-wave radiation through the windows</li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates basic functionalities.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 2 of the VDI 6007 Part 1: Calculation of indoor air
+  temperature excited by a radiative heat source for room version S.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>constant outdoor air temperature 22&deg;C</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>no solar or short-wave radiation through the windows</li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates basic functionalities.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase2.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase2;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase3.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase3.mo
index 261dff07f6..2556ffcca4 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase3.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase3.mo
@@ -113,36 +113,35 @@ equation
   connect(reference.y[1], assEqu.u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 3 of the VDI 6007 Part 1: Calculation of indoor air
-   temperature excited by a convective heat source for room version L.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>constant outdoor air temperature 22&deg;C</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>no solar or short-wave radiation through the windows</li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates basic functionalities.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 3 of the VDI 6007 Part 1: Calculation of indoor air
+  temperature excited by a convective heat source for room version L.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>constant outdoor air temperature 22&deg;C</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>no solar or short-wave radiation through the windows</li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates basic functionalities.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase3.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase3;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase4.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase4.mo
index 01b6235e70..03684f90c0 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase4.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase4.mo
@@ -115,36 +115,35 @@ equation
   connect(reference.y[1], assEqu.u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 4 of the VDI 6007 Part 1: Calculation of indoor air temperature
-   excited by a radiative heat source for room version L.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>constant outdoor air temperature 22&deg;C</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>no solar or short-wave radiation through the windows</li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates basic functionalities.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 4 of the VDI 6007 Part 1: Calculation of indoor air temperature
+  excited by a radiative heat source for room version L.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>constant outdoor air temperature 22&deg;C</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>no solar or short-wave radiation through the windows</li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates basic functionalities.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase4.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase4;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase5.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase5.mo
index 3d4f2033c5..691a318274 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase5.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase5.mo
@@ -209,40 +209,39 @@ equation
   connect(reference.y[1], assEqu.u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 5 of the VDI 6007 Part 1: Calculation of indoor air
-   temperature excited by a radiative and convective heat source for
-   room version S.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>daily profile for outdoor air temperature in hourly steps</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>daily profile for solar radiation through the windows in hourly
-   steps</li>
-   <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates reaction of indoor air
-   temperature at mixed internal gains and outdoor impacts.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 5 of the VDI 6007 Part 1: Calculation of indoor air
+  temperature excited by a radiative and convective heat source for
+  room version S.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>daily profile for outdoor air temperature in hourly steps</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>daily profile for solar radiation through the windows in hourly
+  steps</li>
+  <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates reaction of indoor air
+  temperature at mixed internal gains and outdoor impacts.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase5.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase5;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase6.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase6.mo
index c5794a6d73..47153af0f8 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase6.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase6.mo
@@ -140,38 +140,37 @@ equation
   connect(heatFlowSensor.Q_flow, mean.u) annotation (Line(points={{84,-40},{84,
           -54},{-6,-54},{-6,51},{61,51}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 6 of the VDI 6007 Part 1: Calculation of heat load excited with a
-   given radiative heat source and a setpoint profile for room version S. Is
-   based on Test Case 2.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>constant outdoor air temperature 22&deg;C</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>no solar or short-wave radiation through the windows</li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates heat load calculation without
-   maximum heating power.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 6 of the VDI 6007 Part 1: Calculation of heat load excited with a
+  given radiative heat source and a setpoint profile for room version S. Is
+  based on Test Case 2.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>constant outdoor air temperature 22&deg;C</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>no solar or short-wave radiation through the windows</li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates heat load calculation without
+  maximum heating power.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase6.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase6;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase7.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase7.mo
index 99471710ac..95a97c7393 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase7.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase7.mo
@@ -163,42 +163,41 @@ equation
   connect(gainMea.u, heatFlowSensor.Q_flow) annotation (Line(points={{43,51},{
           -74,51},{-74,-68},{78,-68},{78,-42}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 7 of the VDI 6007 Part 1: Calculation of heat load excited with a
-   given radiative heat source and a setpoint profile for room version S. Is
-   similar with Test Case 6, but with a maximum heating/cooling power.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>constant outdoor air temperature 22&deg;C</li>
-   <li>no solar or short-wave radiation on the exterior wall</li>
-   <li>no solar or short-wave radiation through the windows</li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates heat load calculation with
-   maximum heating power.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   January 25, 2019, by Michael Wetter:<br/>
-   Added start value to avoid warning in JModelica.
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 7 of the VDI 6007 Part 1: Calculation of heat load excited with a
+  given radiative heat source and a setpoint profile for room version S. Is
+  similar with Test Case 6, but with a maximum heating/cooling power.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>constant outdoor air temperature 22&deg;C</li>
+  <li>no solar or short-wave radiation on the exterior wall</li>
+  <li>no solar or short-wave radiation through the windows</li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates heat load calculation with
+  maximum heating power.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  January 25, 2019, by Michael Wetter:<br/>
+  Added start value to avoid warning in JModelica.
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase7.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase7;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase8.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase8.mo
index 26bc557e6d..4a6912137f 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase8.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase8.mo
@@ -133,7 +133,7 @@ model TestCase8 "VDI 6007 Test Case 8 model"
     origin={-61,59})));
   Modelica.Blocks.Math.Product product1
     "Solar radiation times g value for sunblind (open or closed) for
-     one direction"
+    one direction"
     annotation (Placement(transformation(extent={{-6,65},{4,75}})));
   Modelica.Blocks.Logical.Switch switch1
     "Determines g value for sunblind (open or closed) for one direction"
@@ -149,7 +149,7 @@ model TestCase8 "VDI 6007 Test Case 8 model"
     origin={-25,59})));
   Modelica.Blocks.Math.Product product
     "Solar radiation times g value
-     for sunblind (open or closed) for one direction"
+    for sunblind (open or closed) for one direction"
     annotation (Placement(transformation(extent={{-6,84},{4,94}})));
   EquivalentAirTemperature.VDI6007 eqAirTemp(
     n=2,
@@ -204,7 +204,7 @@ model TestCase8 "VDI 6007 Test Case 8 model"
     origin={-27,45})));
   Modelica.Blocks.Logical.Switch switch2
     "Determines g value for sunblind (open or closed) for one
-     direction"
+    direction"
     annotation (Placement(transformation(
     extent={{-4,-4},{4,4}},
     rotation=-90,
@@ -340,41 +340,40 @@ equation
   connect(reference.y[1],assEqu. u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 8 of the VDI 6007 Part 1: Calculation of indoor air
-   temperature excited by a radiative and convective heat source for
-   room version S with two exterior walls. It is based on Test Case 5.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>daily profile for outdoor air temperature in hourly steps</li>
-   <li>daily profile for solar radiation on the exterior wall</li>
-   <li>daily profile for solar radiation through the windows in hourly
-   steps</li>
-   <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
-   <li>no long-wave radiation exchange between exterior wall, windows
-   and ambient environment</li>
-   </ul>
-   <p>This test validates reaction of indoor air
-   temperature at mixed internal gains and outdoor impacts including
-   solar radiation on exterior walls.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 8 of the VDI 6007 Part 1: Calculation of indoor air
+  temperature excited by a radiative and convective heat source for
+  room version S with two exterior walls. It is based on Test Case 5.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>daily profile for outdoor air temperature in hourly steps</li>
+  <li>daily profile for solar radiation on the exterior wall</li>
+  <li>daily profile for solar radiation through the windows in hourly
+  steps</li>
+  <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
+  <li>no long-wave radiation exchange between exterior wall, windows
+  and ambient environment</li>
+  </ul>
+  <p>This test validates reaction of indoor air
+  temperature at mixed internal gains and outdoor impacts including
+  solar radiation on exterior walls.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase8.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase8;
diff --git a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase9.mo b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase9.mo
index 1f497ccd47..4b74bb216c 100644
--- a/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase9.mo
+++ b/AixLib/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase9.mo
@@ -133,7 +133,7 @@ model TestCase9 "VDI 6007 Test Case 9 model"
     origin={-61,59})));
   Modelica.Blocks.Math.Product product1
     "Solar radiation times g value for sunblind (open or closed) for
-     one direction"
+    one direction"
     annotation (Placement(transformation(extent={{-6,65},{4,75}})));
   Modelica.Blocks.Logical.Switch switch1
     "Determines g value for sunblind (open or closed) for one direction"
@@ -150,7 +150,7 @@ model TestCase9 "VDI 6007 Test Case 9 model"
     origin={-25,59})));
   Modelica.Blocks.Math.Product product
     "Solar radiation times g value
-     for sunblind (open or closed) for one direction"
+    for sunblind (open or closed) for one direction"
     annotation (Placement(transformation(extent={{-6,84},{4,94}})));
   EquivalentAirTemperature.VDI6007 eqAirTemp(
     n=2,
@@ -367,41 +367,40 @@ equation
   connect(reference.y[1],assEqu. u1) annotation (Line(points={{97,82},{100,82},
           {100,62},{78,62},{78,54},{83,54}}, color={0,0,127}));
   annotation ( Documentation(info="<html>
-   <p>Test Case 9 of the VDI 6007 Part 1: Calculation of indoor air
-   temperature excited by a radiative and convective heat source for
-   room version S with two exterior walls. It is based on Test Case 8.</p>
-   <h4>Boundary conditions</h4>
-   <ul>
-   <li>daily profile for outdoor air temperature in hourly steps</li>
-   <li>daily profile for solar radiation on the exterior wall</li>
-   <li>daily profile for solar radiation through the windows in hourly
-   steps</li>
-   <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
-   <li>long-wave radiation exchange between exterior wall, windows and
-   ambient environment</li>
-   </ul>
-   <p>This test validates reaction of indoor air
-   temperature at mixed internal gains and outdoor impacts including
-   solar radiation and long-wave radiation on exterior walls.</p>
-   </html>",revisions="<html>
-   <ul>
-   <li>
-   July 11, 2019, by Katharina Brinkmann:<br/>
-   Renamed <code>alphaWall</code> to <code>hConWall</code>
-   </li>
-   <li>
-   July 7, 2016, by Moritz Lauster:<br/>
-   Added automatic check against validation thresholds.
-   </li>
-   <li>
-   January 11, 2016, by Moritz Lauster:<br/>
-   Implemented.
-   </li>
-   </ul>
-   </html>"),
-            experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
+  <p>Test Case 9 of the VDI 6007 Part 1: Calculation of indoor air
+  temperature excited by a radiative and convective heat source for
+  room version S with two exterior walls. It is based on Test Case 8.</p>
+  <h4>Boundary conditions</h4>
+  <ul>
+  <li>daily profile for outdoor air temperature in hourly steps</li>
+  <li>daily profile for solar radiation on the exterior wall</li>
+  <li>daily profile for solar radiation through the windows in hourly
+  steps</li>
+  <li>sunblind closes at &gt;100 W/m<sup>2</sup></li>
+  <li>long-wave radiation exchange between exterior wall, windows and
+  ambient environment</li>
+  </ul>
+  <p>This test validates reaction of indoor air
+  temperature at mixed internal gains and outdoor impacts including
+  solar radiation and long-wave radiation on exterior walls.</p>
+  </html>", revisions="<html>
+  <ul>
+  <li>
+  July 11, 2019, by Katharina Brinkmann:<br/>
+  Renamed <code>alphaWall</code> to <code>hConWall</code>
+  </li>
+  <li>
+  July 7, 2016, by Moritz Lauster:<br/>
+  Added automatic check against validation thresholds.
+  </li>
+  <li>
+  January 11, 2016, by Moritz Lauster:<br/>
+  Implemented.
+  </li>
+  </ul>
+  </html>"),experiment(Tolerance=1e-6, StopTime=5.184e+006, Interval=60),
   __Dymola_Commands(file=
   "modelica://AixLib/Resources/Scripts/Dymola/ThermalZones/ReducedOrder/Validation/VDI6007/TestCase9.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TestCase9;
diff --git a/AixLib/ThermalZones/package.order b/AixLib/ThermalZones/package.order
index 9cb9cacc41..da308c8d83 100644
--- a/AixLib/ThermalZones/package.order
+++ b/AixLib/ThermalZones/package.order
@@ -1,2 +1,3 @@
 HighOrder
+ISO13790
 ReducedOrder
diff --git a/AixLib/Types/Tilt/package.mo b/AixLib/Types/Tilt/package.mo
index 42fbc9488f..d5c58c5725 100644
--- a/AixLib/Types/Tilt/package.mo
+++ b/AixLib/Types/Tilt/package.mo
@@ -18,7 +18,7 @@ Note that a ceiling has a tilt of <i>0</i>
 <!-- @include_Buildings
 , and also the solar collector models
 in
-<a href=\"AixLib.Fluid.SolarCollectors\">AixLib.Fluid.SolarCollectors</a>
+<a href=\"modelica://AixLib.Fluid.SolarCollectors\">AixLib.Fluid.SolarCollectors</a>
 require a tilt of <i>0</i>
 -->
 if they are facing straight upwards.
diff --git a/AixLib/Utilities/Clustering/KMeans.mo b/AixLib/Utilities/Clustering/KMeans.mo
new file mode 100644
index 0000000000..4a28fc9845
--- /dev/null
+++ b/AixLib/Utilities/Clustering/KMeans.mo
@@ -0,0 +1,143 @@
+within AixLib.Utilities.Clustering;
+impure function KMeans "k-means clustering algorithm"
+  extends Modelica.Icons.Function;
+  input Real data[n_samples,n_features] "Data to be clustered";
+  input Integer n_clusters "Number of clusters to be generated";
+  input Integer n_samples "Number of samples";
+  input Integer n_features "Number of features";
+  input Real relTol=1e-5 "Relative tolerance on cluster positions";
+  input Integer max_iter=500 "Maximum number of k-means iterations";
+  input Integer n_init=10 "Number of runs with randomized centroid seeds";
+  input Integer n_cluster_size=0 "Length of the cluster_size output vector";
+  output Real centroids[n_clusters,n_features] "Centroids of the clusters";
+  output Integer labels[n_samples] "Cluster label associated with each data point";
+  output Integer cluster_size[max(n_clusters, n_cluster_size)] "Size of the clusters";
+
+protected
+  Real old_centroids[n_clusters,n_features] "Previous iteration centroids";
+  Real new_centroids[n_clusters,n_features] "Next iteration centroids";
+  Real delta_centroids "Maximum relative displacement of cluster centroids between two k-means iterations";
+  Integer new_labels[n_samples] "Next iteration cluster labels";
+  Real new_inertia "Inertia of the samples during the current run";
+  Real inertia "Minimum inertia of the samples since first run";
+  Integer id "Id of the random integer generator";
+  Integer k_iter "Index of k-means iteration";
+  Real min_dis "Minimum distance between a sample (or a centroid) and a cluster centroid";
+  Real dis "Distance between a sample (or a centroid) and a cluster centroid";
+  Integer n "Random integer";
+  constant Integer seed = 2 "Arbitrary seed value";
+
+algorithm
+ id := Modelica.Math.Random.Utilities.initializeImpureRandom(seed);
+
+  // ---- Perform n_init successive runs of the k-means algorithm
+ for run in 1:n_init loop
+    // ---- Select initial centroids at random
+    // Select 3 non-repeated data points in the data set
+    n := Modelica.Math.Random.Utilities.impureRandomInteger(id,1,n_samples);
+    old_centroids[1,:] := data[n,:];
+    for i in 2:n_clusters loop
+      n := Modelica.Math.Random.Utilities.impureRandomInteger(id,1,n_samples);
+      old_centroids[i,:] := data[n,:];
+      min_dis := Modelica.Math.Vectors.norm(old_centroids[i,:]-old_centroids[1,:], p=2)^2;
+      while min_dis < Modelica.Constants.eps loop
+        n := Modelica.Math.Random.Utilities.impureRandomInteger(id,1,n_samples);
+        old_centroids[i,:] := data[n,:];
+        min_dis := Modelica.Math.Vectors.norm(old_centroids[i,:]-old_centroids[1,:], p=2)^2;
+        for j in 1:i-1 loop
+          dis := Modelica.Math.Vectors.norm(old_centroids[j,:]-old_centroids[i,:], p=2)^2;
+          min_dis := min(dis, min_dis);
+        end for;
+      end while;
+    end for;
+
+    // ---- k-means iterations
+    k_iter := 0;
+    delta_centroids := 2*relTol;
+    while k_iter < max_iter and delta_centroids > relTol loop
+      k_iter := k_iter + 1;
+
+      // Find centroid closest to each data point
+      for i in 1:n_samples loop
+        new_labels[i] := 1;
+        min_dis := Modelica.Math.Vectors.norm(data[i,:]-old_centroids[1,:], p=2)^2;
+        for j in 1:n_clusters loop
+          dis := Modelica.Math.Vectors.norm(data[i,:]-old_centroids[j,:], p=2)^2;
+          if dis < min_dis then
+            min_dis := min(dis, min_dis);
+            new_labels[i] := j;
+          end if;
+        end for;
+      end for;
+
+      // Re-evaluate position of the centroids
+      delta_centroids := 0;
+      for j in 1:n_clusters loop
+        n := sum(if new_labels[i]==j then 1 else 0 for i in 1:n_samples);
+        new_centroids[j,:] := zeros(n_features);
+        if n>0 then
+          for i in 1:n_samples loop
+             if new_labels[i]==j then
+               new_centroids[j,:] := new_centroids[j,:] + data[i,:]/n;
+             end if;
+          end for;
+        else
+          new_centroids[j,:] := old_centroids[j,:];
+        end if;
+        delta_centroids := max(delta_centroids, sum((new_centroids[j,:] - old_centroids[j,:])./old_centroids[j,:]));
+      end for;
+      old_centroids := new_centroids;
+    end while;
+
+    // Evaluate inertia
+    new_inertia := 0;
+    for i in 1:n_samples loop
+      dis := Modelica.Math.Vectors.norm(data[i,:]-centroids[new_labels[i],:], p=2)^2;
+      new_inertia := inertia + dis;
+    end for;
+
+    // Keep run results if inertia is minimum
+    if new_inertia < inertia or run == 1 then
+      centroids := new_centroids;
+      inertia := new_inertia;
+      labels := new_labels;
+    end if;
+
+   end for;
+
+   // Evaluate cluster sizes
+   for j in 1:max(n_clusters, n_cluster_size) loop
+     cluster_size[j] := sum(if labels[i]==j then 1 else 0 for i in 1:n_samples);
+   end for;
+
+annotation (
+    Documentation(info="<html>
+<p>
+This function applies <i>k</i>-means clustering to <i>n</i>-dimentional data and
+returns the centroid of the clusters, the cluster labels for each sample, and
+the size of each cluster.
+</p>
+<p>
+The returned length of the <code>cluster_size</code> vector is
+<code>max(n_clusters, n_cluster_size)</code>.
+</p>
+<h4>Implementation</h4>
+<p>
+The seed for random number generation is constant. It can be changed by
+modifying the constant <code>seed</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 1, 2023, by Michael Wetter:<br/>
+Added <code>impure</code> declaration which is needed for compliance with the Modelica Language Specification,
+and is required by Optimica.
+</li>
+<li>
+June 9, 2022 by Massimo Cimmino:<br/>
+First Implementation
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end KMeans;
diff --git a/AixLib/Utilities/Clustering/Validation/KMeans_1d.mo b/AixLib/Utilities/Clustering/Validation/KMeans_1d.mo
new file mode 100644
index 0000000000..3e674ffce8
--- /dev/null
+++ b/AixLib/Utilities/Clustering/Validation/KMeans_1d.mo
@@ -0,0 +1,48 @@
+within AixLib.Utilities.Clustering.Validation;
+model KMeans_1d "Model that verifies the k-means clustering function for 1d data"
+  extends Modelica.Icons.Example;
+
+  parameter Integer n_clusters = 3 "Number of clusters to be generated";
+  parameter Real data[:,:] = [1;2;2;3;4] "Test data to be clustered";
+
+  parameter Integer nDat = size(data,1) "Number of samples";
+  parameter Integer nDim = size(data,2) "Number of features";
+  parameter Real[n_clusters,nDim] centroids(each fixed=false)
+    "Centroids of the clusters";
+  parameter Integer[nDat] labels(each fixed=false)
+    "Cluster label associated with each data point";
+  parameter Integer[n_clusters] cluster_size(each fixed=false)
+    "Size of the clusters";
+
+  parameter Integer labelsExp[nDat]=
+    {2,2,2,1,3}
+    "Expected cluster labels";
+
+  // Comparison result
+  Boolean cmp "Comparison result";
+
+initial equation
+  (centroids, labels, cluster_size) = AixLib.Utilities.Clustering.KMeans(
+    data, n_clusters, nDat, nDim);
+
+equation
+  cmp = Modelica.Math.Vectors.isEqual(labels, labelsExp);
+
+annotation (experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Clustering/Validation/KMeans_1d.mos"
+        "Simulate and plot"),
+      Documentation(info="<html>
+<p>
+This example tests the k-means clustering algorithm on 1d data.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+June 9, 2022 by Massimo Cimmino<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end KMeans_1d;
diff --git a/AixLib/Utilities/Clustering/Validation/KMeans_2d.mo b/AixLib/Utilities/Clustering/Validation/KMeans_2d.mo
new file mode 100644
index 0000000000..45ccf24448
--- /dev/null
+++ b/AixLib/Utilities/Clustering/Validation/KMeans_2d.mo
@@ -0,0 +1,55 @@
+within AixLib.Utilities.Clustering.Validation;
+model KMeans_2d "Model that verifies the k-means clustering function for 2d data"
+  extends Modelica.Icons.Example;
+
+  parameter Integer n_clusters = 3 "Number of clusters to be generated";
+  parameter Real data[:,:]=
+    [ 1, 1;
+      1, 2;
+      2, 1;
+      2, 1.2;
+      3, 0;
+      4, 0]
+     "Test data to be clustered";
+
+  parameter Integer nDat = size(data,1) "Number of samples";
+  parameter Integer nDim = size(data,2) "Number of features";
+  parameter Real[n_clusters,nDim] centroids(each fixed=false)
+    "Centroids of the clusters";
+  parameter Integer[nDat] labels(each fixed=false)
+    "Cluster label associated with each data point";
+  parameter Integer[n_clusters] cluster_size(each fixed=false)
+    "Size of the clusters";
+
+  parameter Integer labelsExp[nDat]=
+    {2,2,1,2,1,3}
+    "Expected cluster labels";
+
+  // Comparison result
+  Boolean cmp "Comparison result";
+
+initial equation
+  (centroids, labels, cluster_size) = AixLib.Utilities.Clustering.KMeans(
+    data, n_clusters, nDat, nDim);
+
+equation
+  cmp = Modelica.Math.Vectors.isEqual(labels, labelsExp);
+
+annotation (experiment(Tolerance=1e-6, StopTime=1.0),
+__Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Clustering/Validation/KMeans_2d.mos"
+        "Simulate and plot"),
+      Documentation(info="<html>
+<p>
+This example tests the k-means clustering algorithm on 2d data.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+June 9, 2022 by Massimo Cimmino<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end KMeans_2d;
diff --git a/AixLib/Utilities/Clustering/Validation/package.mo b/AixLib/Utilities/Clustering/Validation/package.mo
new file mode 100644
index 0000000000..f053d7db77
--- /dev/null
+++ b/AixLib/Utilities/Clustering/Validation/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Utilities.Clustering;
+package Validation "Validation models for clustering functions."
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (Documentation(info="<html>
+  <p>This package contains models for validation of clustering functions. The
+examples plot various outputs, which have been verified against comparative
+results. These model outputs are stored as reference data to allow continuous
+validation whenever models in the library change.</p>
+  </html>"));
+end Validation;
diff --git a/AixLib/Utilities/Clustering/Validation/package.order b/AixLib/Utilities/Clustering/Validation/package.order
new file mode 100644
index 0000000000..1e7fee4235
--- /dev/null
+++ b/AixLib/Utilities/Clustering/Validation/package.order
@@ -0,0 +1,2 @@
+KMeans_1d
+KMeans_2d
diff --git a/AixLib/Utilities/Clustering/package.mo b/AixLib/Utilities/Clustering/package.mo
new file mode 100644
index 0000000000..69746de420
--- /dev/null
+++ b/AixLib/Utilities/Clustering/package.mo
@@ -0,0 +1,11 @@
+within AixLib.Utilities;
+package Clustering "Package with clustering functions"
+  extends Modelica.Icons.VariantsPackage;
+
+  annotation (
+preferredView="info", Documentation(info="<html>
+<p>
+This package contains utility models for performing clustering operations.
+</p>
+</html>"));
+end Clustering;
diff --git a/AixLib/Utilities/Clustering/package.order b/AixLib/Utilities/Clustering/package.order
new file mode 100644
index 0000000000..f6d992965a
--- /dev/null
+++ b/AixLib/Utilities/Clustering/package.order
@@ -0,0 +1,2 @@
+KMeans
+Validation
diff --git a/AixLib/Utilities/Cryptographics/Validation/SHA1.mo b/AixLib/Utilities/Cryptographics/Validation/SHA1.mo
index 796cb6aa53..810c8ad7ff 100644
--- a/AixLib/Utilities/Cryptographics/Validation/SHA1.mo
+++ b/AixLib/Utilities/Cryptographics/Validation/SHA1.mo
@@ -46,44 +46,44 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Cryptographics/Validation/SHA1.mos"
         "Simulate and plot"),
       Documentation(info="<html>
- <p>
- This validation function tests the C implementation of the SHA1 encryption for
- the following strings:
- </p>
- <ul>
- <li>
- <code>&#34;abc&#34;</code>
- </li>
- <li>
- <code>&#34;&#34;</code> <i>(an empty string)</i>
- </li>
- <li>
- <code>&#34;abcdbcdecdefdefgefghfghighijhijkijkljklmklmnlmnomnopnopq&#34;</code>
- </li>
- <li>
- <code>&#34;1.23e+4&#34;</code>
- </li>
- <li>
- <code>&#34;a&#34;</code> repeated <i>509</i> times.
- </li>
- </ul>
- <p>
- If the encrypted strings are identical to the expected (known) encryption
- results, the <code>cmpAll</code> boolean variable will be <code>true</code>.
- </p>
- </html>",
+<p>
+This validation function tests the C implementation of the SHA1 encryption for
+the following strings:
+</p>
+<ul>
+<li>
+<code>&#34;abc&#34;</code>
+</li>
+<li>
+<code>&#34;&#34;</code> <i>(an empty string)</i>
+</li>
+<li>
+<code>&#34;abcdbcdecdefdefgefghfghighijhijkijkljklmklmnlmnomnopnopq&#34;</code>
+</li>
+<li>
+<code>&#34;1.23e+4&#34;</code>
+</li>
+<li>
+<code>&#34;a&#34;</code> repeated <i>509</i> times.
+</li>
+</ul>
+<p>
+If the encrypted strings are identical to the expected (known) encryption
+results, the <code>cmpAll</code> boolean variable will be <code>true</code>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 13, 2019, by Michael Wetter:<br/>
- Reduced string length for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1081\">issue 1081</a>.
- </li>
- <li>
- May 30, 2018, by Alex Laferri&egrave;re:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 13, 2019, by Michael Wetter:<br/>
+Reduced string length for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1081\">issue 1081</a>.
+</li>
+<li>
+May 30, 2018, by Alex Laferri&egrave;re:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SHA1;
diff --git a/AixLib/Utilities/Cryptographics/sha.mo b/AixLib/Utilities/Cryptographics/sha.mo
index a32ef3e127..0b2498a4ce 100644
--- a/AixLib/Utilities/Cryptographics/sha.mo
+++ b/AixLib/Utilities/Cryptographics/sha.mo
@@ -12,29 +12,29 @@ external "C" sha1 = cryptographicsHash(str)
 
 annotation (
     Documentation(info="<html>
- <p>
- This function takes a String input and, using an external function written in C,
- outputs its SHA1 encryption. The input string can be of any length, though the output
- will always be 40 hexadecimal characters.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 11, 2021, by Michael Wetter:<br/>
- Added <code>pure</code> declaration for MSL 4.0.0.
- </li>
- <li>
- May 31, 2018 by Alex Laferri&egrave;re:<br/>
- Changed the encryption to a SHA1 with a string array input (rather than a file
- input).
- </li>
- <li>
- January 21, 2018 by Filip Jorissen:<br/>
- Revised sha implementation to avoid buffer overflow in borefield.
- See <a href=\"https://github.com/open-ideas/IDEAS/issues/755\">
- #755</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function takes a String input and, using an external function written in C,
+outputs its SHA1 encryption. The input string can be of any length, though the output
+will always be 40 hexadecimal characters.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 11, 2021, by Michael Wetter:<br/>
+Added <code>pure</code> declaration for MSL 4.0.0.
+</li>
+<li>
+May 31, 2018 by Alex Laferri&egrave;re:<br/>
+Changed the encryption to a SHA1 with a string array input (rather than a file
+input).
+</li>
+<li>
+January 21, 2018 by Filip Jorissen:<br/>
+Revised sha implementation to avoid buffer overflow in borefield.
+See <a href=\"https://github.com/open-ideas/IDEAS/issues/755\">
+#755</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end sha;
diff --git a/AixLib/Utilities/Diagnostics/AssertEquality.mo b/AixLib/Utilities/Diagnostics/AssertEquality.mo
index 0204ca1b33..e3de85ec4a 100644
--- a/AixLib/Utilities/Diagnostics/AssertEquality.mo
+++ b/AixLib/Utilities/Diagnostics/AssertEquality.mo
@@ -17,35 +17,35 @@ Icon(graphics={Text(
           textColor={255,0,0},
           textString="u1 = u2")}),
 Documentation(info="<html>
- <p>
- Model that triggers an assert if
- <i>|u1-u2| &gt; threShold</i>
- and <i>t &gt; t<sub>0</sub></i>.
- </p>
- </html>",
+<p>
+Model that triggers an assert if
+<i>|u1-u2| &gt; threShold</i>
+and <i>t &gt; t<sub>0</sub></i>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 10, 2013, by Michael Wetter:<br/>
- Reformulated model to avoid an event iteration.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Added <code>time</code> in print statement as OpenModelica,
- in its error message, does not output the time when the assert is triggered.
- </li>
- <li>
- January 23, 2013, by Michael Wetter:<br/>
- Replaced <code>when</code> test with <code>if</code> test as
- equations within a <code>when</code> section are only evaluated
- when the condition becomes true.
- This fixes <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/72\">issue 72</a>.
- </li>
- <li>
- April 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 10, 2013, by Michael Wetter:<br/>
+Reformulated model to avoid an event iteration.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Added <code>time</code> in print statement as OpenModelica,
+in its error message, does not output the time when the assert is triggered.
+</li>
+<li>
+January 23, 2013, by Michael Wetter:<br/>
+Replaced <code>when</code> test with <code>if</code> test as
+equations within a <code>when</code> section are only evaluated
+when the condition becomes true.
+This fixes <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/72\">issue 72</a>.
+</li>
+<li>
+April 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AssertEquality;
diff --git a/AixLib/Utilities/Diagnostics/AssertInequality.mo b/AixLib/Utilities/Diagnostics/AssertInequality.mo
index b864b976bf..368817fcfe 100644
--- a/AixLib/Utilities/Diagnostics/AssertInequality.mo
+++ b/AixLib/Utilities/Diagnostics/AssertInequality.mo
@@ -19,35 +19,35 @@ Icon(graphics={Text(
           textString="u1 > u2")}),
 Documentation(
 info="<html>
- <p>
- Model that triggers an assert if
- <i>u1 &gt; u2 - threShold</i>
- and <i>t &gt; t<sub>0</sub></i>.
- </p>
- </html>",
+<p>
+Model that triggers an assert if
+<i>u1 &gt; u2 - threShold</i>
+and <i>t &gt; t<sub>0</sub></i>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 10, 2013, by Michael Wetter:<br/>
- Reformulated model to avoid an event iteration.
- </li>
- <li>
- September 10, 2013, by Michael Wetter:<br/>
- Added <code>time</code> in print statement as OpenModelica,
- in its error message, does not output the time when the assert is triggered.
- </li>
- <li>
- January 23, 2013, by Michael Wetter:<br/>
- Replaced <code>when</code> test with <code>if</code> test as
- equations within a <code>when</code> section are only evaluated
- when the condition becomes true.
- This fixes <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/72\">issue 72</a>.
- </li>
- <li>
- April 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 10, 2013, by Michael Wetter:<br/>
+Reformulated model to avoid an event iteration.
+</li>
+<li>
+September 10, 2013, by Michael Wetter:<br/>
+Added <code>time</code> in print statement as OpenModelica,
+in its error message, does not output the time when the assert is triggered.
+</li>
+<li>
+January 23, 2013, by Michael Wetter:<br/>
+Replaced <code>when</code> test with <code>if</code> test as
+equations within a <code>when</code> section are only evaluated
+when the condition becomes true.
+This fixes <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/72\">issue 72</a>.
+</li>
+<li>
+April 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end AssertInequality;
diff --git a/AixLib/Utilities/Diagnostics/BaseClasses/PartialInputCheck.mo b/AixLib/Utilities/Diagnostics/BaseClasses/PartialInputCheck.mo
index 2a6a9e9420..f6f91807ed 100644
--- a/AixLib/Utilities/Diagnostics/BaseClasses/PartialInputCheck.mo
+++ b/AixLib/Utilities/Diagnostics/BaseClasses/PartialInputCheck.mo
@@ -19,24 +19,24 @@ initial equation
           textColor={0,0,255},
           textString="%threShold")}),
 Documentation(info="<html>
- <p>
- Partial model that can be used to check whether its
- inputs satisfy a certain condition such as equality within
- a prescribed threshold.
- </p>
- </html>",
+<p>
+Partial model that can be used to check whether its
+inputs satisfy a certain condition such as equality within
+a prescribed threshold.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 18, 2013, by Michael Wetter:<br/>
- Removed <code>cardinality</code> function as this is
- deprecated in the MSL specification and not correctly implemented in omc.
- </li>
- <li>
- April 17, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 18, 2013, by Michael Wetter:<br/>
+Removed <code>cardinality</code> function as this is
+deprecated in the MSL specification and not correctly implemented in omc.
+</li>
+<li>
+April 17, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialInputCheck;
diff --git a/AixLib/Utilities/Diagnostics/CheckEquality.mo b/AixLib/Utilities/Diagnostics/CheckEquality.mo
index b9f361f916..586ddd0c55 100644
--- a/AixLib/Utilities/Diagnostics/CheckEquality.mo
+++ b/AixLib/Utilities/Diagnostics/CheckEquality.mo
@@ -17,25 +17,25 @@ equation
 annotation (
 defaultComponentName="cheEqu",
 Documentation(info="<html>
- <p>
- Block that outputs <i>0</i> if the difference
- <i>|u1-u2| &lt; threShold</i>,
- or else it outputs <i>u2-u1</i>.
- </p>
- </html>",
+<p>
+Block that outputs <i>0</i> if the difference
+<i>|u1-u2| &lt; threShold</i>,
+or else it outputs <i>u2-u1</i>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 13, 2017, by Michael Wetter:<br/>
- Revised implementation to output difference rather than the absolute
- value of the difference.
- </li>
- <li>
- January 12, 2017, by Thiery S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+January 13, 2017, by Michael Wetter:<br/>
+Revised implementation to output difference rather than the absolute
+value of the difference.
+</li>
+<li>
+January 12, 2017, by Thiery S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={
         Text(
           extent={{-84,108},{90,-28}},
@@ -44,6 +44,6 @@ revisions="<html>
         Text(
           extent={{-62,-38},{54,-68}},
           textColor={0,0,255},
-          textString="%threShold")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="%threShold")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckEquality;
diff --git a/AixLib/Utilities/Diagnostics/Validation/CheckEquality.mo b/AixLib/Utilities/Diagnostics/Validation/CheckEquality.mo
index cc0e2a672e..b7d88b1924 100644
--- a/AixLib/Utilities/Diagnostics/Validation/CheckEquality.mo
+++ b/AixLib/Utilities/Diagnostics/Validation/CheckEquality.mo
@@ -26,24 +26,24 @@ equation
         "Simulate and plot"),
   Documentation(
     info="<html>
- <p>
- This model validates the use of the
- <a href=\"modelica://AixLib.Utilities.Diagnostics.CheckEquality\">
- AixLib.Utilities.Diagnostics.CheckEquality</a>.
- </p>
- </html>",
+<p>
+This model validates the use of the
+<a href=\"modelica://AixLib.Utilities.Diagnostics.CheckEquality\">
+AixLib.Utilities.Diagnostics.CheckEquality</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 17, 2017, by Michael Wetter:<br/>
- Updated example to also test negative difference.
- </li>
- <li>
- January 17, 2017, by Thierry S. Nouidui:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    experiment(Tolerance=1e-6, StopTime=1),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 17, 2017, by Michael Wetter:<br/>
+Updated example to also test negative difference.
+</li>
+<li>
+January 17, 2017, by Thierry S. Nouidui:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=1), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CheckEquality;
diff --git a/AixLib/Utilities/HeatTransfer/HeatConvInside.mo b/AixLib/Utilities/HeatTransfer/HeatConvInside.mo
index 2792d64677..5790713e57 100644
--- a/AixLib/Utilities/HeatTransfer/HeatConvInside.mo
+++ b/AixLib/Utilities/HeatTransfer/HeatConvInside.mo
@@ -5,33 +5,22 @@ model HeatConvInside
   */
   extends Modelica.Thermal.HeatTransfer.Interfaces.Element1D;
 
-  parameter Integer calcMethod=2 "Calculation method for convective heat transfer coefficient" annotation (
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface calcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Bernd_Glueck "Calculation method for convective heat transfer coefficient" annotation (
     Dialog(descriptionLabel=true),
-    choices(
-      choice=1 "EN ISO 6946 Appendix A >>Flat Surfaces<<",
-      choice=2 "By Bernd Glueck",
-      choice=3 "Custom hCon (constant)",
-      choice=4 "ASHRAE140-2017",
-      radioButtons=true),
     Evaluate=true);
 
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hCon_const=2.5
     "Custom convective heat transfer coefficient" annotation (Dialog(
-        descriptionLabel=true, enable=if calcMethod == 3 then true else false));
+        descriptionLabel=true, enable=if calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon then true else false));
 
   parameter Modelica.Units.SI.TemperatureDifference dT_small=0.1
     "Linearized function around dT = 0 K +/-" annotation (Dialog(
-        descriptionLabel=true, enable=if calcMethod == 1 or calcMethod == 2 or
-          calcMethod == 4 then true else false));
+        descriptionLabel=true, enable=if calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A or calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Bernd_Glueck or
+          calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.ASHRAE140_2017 then true else false));
 
   // which orientation of surface?
-  parameter Integer surfaceOrientation "Surface orientation" annotation (
-      Dialog(descriptionLabel=true, enable=if calcMethod == 3 then false else true),
-      choices(
-      choice=1 "vertical",
-      choice=2 "horizontal facing up",
-      choice=3 "horizontal facing down",
-      radioButtons=true),
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation surfaceOrientation=AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.vertical_wall "Surface orientation" annotation (
+      Dialog(descriptionLabel=true, enable=if calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon then false else true),
       Evaluate=true);
   parameter Modelica.Units.SI.Area A(min=Modelica.Constants.eps)
     "Area of surface";
@@ -50,10 +39,10 @@ equation
 
   // ++++++++++++++++EN ISO 6946 Appendix A >>Flat Surfaces<<++++++++++++++++
   // upward heat flow: hCon = 5, downward heat flow: hCon = 0.7, horizontal heat flow: hCon = 2.5
-  if calcMethod == 1 then
+  if calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.EN_ISO_6946_Appendix_A then
 
     // floor (horizontal facing up)
-    if surfaceOrientation == 2 then
+    if surfaceOrientation == AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor then
       hCon = Modelica.Fluid.Utilities.regStep(
         x=port_b.T - port_a.T,
         y1=5,
@@ -61,7 +50,7 @@ equation
         x_small=dT_small);
 
     // ceiling (horizontal facing down)
-    elseif surfaceOrientation == 3 then
+    elseif surfaceOrientation == AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling then
       hCon = Modelica.Fluid.Utilities.regStep(
         x=port_b.T - port_a.T,
         y1=0.7,
@@ -78,11 +67,11 @@ equation
   // upward heat flow: hCon = 2*(posDiff^0.31)          - equation 1.27, page 26
   // downward heat flow: hCon = 0.54*(posDiff^0.31)     - equation 1.28, page 26
   // horizontal heat flow: hCon = 0.1.6*(posDiff^0.31)  - equation 1.26, page 26
-  elseif calcMethod == 2 then
+  elseif calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Bernd_Glueck then
 
     // floor (horizontal facing up)
 
-    if surfaceOrientation == 2 then
+    if surfaceOrientation == AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor then
       hCon = Modelica.Fluid.Utilities.regStep(
         x=port_b.T - port_a.T,
         y1=2*AixLib.Utilities.Math.Functions.regNonZeroPower(posDiff, 0.31, dT_small),
@@ -91,7 +80,7 @@ equation
 
 
     // ceiling (horizontal facing down)
-    elseif surfaceOrientation == 3 then
+    elseif surfaceOrientation == AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling then
        hCon = Modelica.Fluid.Utilities.regStep(
         x=port_b.T - port_a.T,
         y1=0.54*AixLib.Utilities.Math.Functions.regNonZeroPower(posDiff, 0.31, dT_small),
@@ -107,18 +96,18 @@ equation
     // ++++++++++++++++hCon_const++++++++++++++++
 
 
-  elseif calcMethod == 3 then
+  elseif calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.Custom_hCon then
     hCon = hCon_const;
 
 
 
     // ++++++++++++++++ASHRAE140-2017++++++++++++++++
     // upward heat flow: hCon = 4.13, downward heat flow: hCon = 1, horizontal heat flow: hCon = 3.16
-   elseif calcMethod == 4 then
+   elseif calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransferInsideSurface.ASHRAE140_2017 then
 
 
     // floor (horizontal facing up)
-    if surfaceOrientation == 2 then
+    if surfaceOrientation == AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.floor then
       hCon = Modelica.Fluid.Utilities.regStep(
         x=port_b.T - port_a.T,
         y1=4.13,
@@ -126,7 +115,7 @@ equation
         x_small=dT_small);
 
       // ceiling (horizontal facing down)
-    elseif surfaceOrientation == 3 then
+    elseif surfaceOrientation == AixLib.ThermalZones.HighOrder.Components.Types.InsideSurfaceOrientation.ceiling then
       hCon = Modelica.Fluid.Utilities.regStep(
         x=port_b.T - port_a.T,
         y1=1,
diff --git a/AixLib/Utilities/HeatTransfer/HeatConvOutside.mo b/AixLib/Utilities/HeatTransfer/HeatConvOutside.mo
index 1197ca0022..05968f6cd1 100644
--- a/AixLib/Utilities/HeatTransfer/HeatConvOutside.mo
+++ b/AixLib/Utilities/HeatTransfer/HeatConvOutside.mo
@@ -1,32 +1,27 @@
 within AixLib.Utilities.HeatTransfer;
 model HeatConvOutside "Model for heat transfer at outside surfaces. Choice between multiple models"
   extends Modelica.Thermal.HeatTransfer.Interfaces.Element1D;
-  parameter Integer calcMethod=2 "Calculation method for convective heat transfer coefficient" annotation (
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer calcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals "Calculation method for convective heat transfer coefficient" annotation (
     Evaluate=true,
     Dialog(
       group="Computational Models",
       compact=true,
-      descriptionLabel=true),
-    choices(
-      choice=1 "DIN 6946",
-      choice=2 "ASHRAE Fundamentals (convective + radiative)",
-      choice=3 "Custom hCon (constant)",
-      radioButtons=true));
+      descriptionLabel=true));
   parameter Modelica.Units.SI.Area A(min=0) "Area of surface"
     annotation (Dialog(group="Surface properties", descriptionLabel=true));
   parameter Modelica.Units.SI.CoefficientOfHeatTransfer hCon_const=25
     "Custom convective heat transfer coeffient" annotation (Dialog(
       group="Surface properties",
       descriptionLabel=true,
-      enable=calcMethod == 3));
+      enable=calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.Custom_hCon));
   parameter
     DataBase.Surfaces.RoughnessForHT.PolynomialCoefficients_ASHRAEHandbook         surfaceType = DataBase.Surfaces.RoughnessForHT.Brick_RoughPlaster()
     "Surface type"                                                                                                     annotation(Dialog(group = "Surface properties", descriptionLabel = true, enable=
-          calcMethod == 2),                                                                                                                                                                                           choicesAllMatching = true);
+          calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals),                                                                                                                                                                                           choicesAllMatching = true);
   // Variables
   Modelica.Units.SI.CoefficientOfHeatTransfer hCon
     "Convection heat transfer coeffient";
-  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if calcMethod == 1 or calcMethod == 2              annotation(Placement(transformation(extent = {{-102, -82}, {-82, -62}}), iconTransformation(extent={{-100,-80},{-80,-60}})));
+  Modelica.Blocks.Interfaces.RealInput WindSpeedPort if calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 or calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals              annotation(Placement(transformation(extent = {{-102, -82}, {-82, -62}}), iconTransformation(extent={{-100,-80},{-80,-60}})));
 
 protected
   Modelica.Blocks.Interfaces.RealInput WindSpeed_internal(unit="m/s");
@@ -35,9 +30,9 @@ equation
   port_a.Q_flow =hCon*A*(port_a.T - port_b.T);
 
   //Determine convection heat transfer coefficient hCon
-  if calcMethod == 1 then
+  if calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.DIN_6946 then
     hCon = (4 + 4*WindSpeed_internal);
-  elseif calcMethod == 2 then
+  elseif calcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodConvectiveHeatTransfer.ASHRAE_Fundamentals then
     hCon = surfaceType.D + surfaceType.E*WindSpeed_internal + surfaceType.F*(WindSpeed_internal^2);
   else
     hCon = hCon_const;
diff --git a/AixLib/Utilities/HeatTransfer/HeatToRad.mo b/AixLib/Utilities/HeatTransfer/HeatToRad.mo
index 43840ff756..47b4daf4e5 100644
--- a/AixLib/Utilities/HeatTransfer/HeatToRad.mo
+++ b/AixLib/Utilities/HeatTransfer/HeatToRad.mo
@@ -10,15 +10,9 @@ model HeatToRad "Adaptor for approximative longwave radiation exchange with vari
     annotation(Evaluate=true, HideResult=true, choices(checkBox=true));
   parameter Modelica.Units.SI.Area A=-1 "Fixed value of prescribed area"
     annotation (Dialog(enable=not use_A_in));
-  parameter Integer radCalcMethod=1 "Calculation method for radiation heat transfer" annotation (
+  parameter AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer radCalcMethod=AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.No_approx "Calculation method for radiation heat transfer" annotation (
     Evaluate=true,
-    Dialog(group = "Radiation exchange equation", compact=true),
-    choices(
-      choice=1 "No approx",
-      choice=2 "Linear approx at wall temp",
-      choice=3 "Linear approx at rad temp",
-      choice=4 "Linear approx at constant T_ref",
-      radioButtons=true));
+    Dialog(group = "Radiation exchange equation", compact=true));
   Modelica.Thermal.HeatTransfer.Interfaces.HeatPort_a convPort
     "Heat port for convective or conductive heat flow"
     annotation (Placement(transformation(extent={{-110,-10},{-90,10}}), iconTransformation(extent={{-110,-10},{-90,10}})));
@@ -41,11 +35,11 @@ equation
  convPort.Q_flow + radPort.Q_flow = 0;
   // To prevent negative solutions for T, the max() expression is used.
   // Negative solutions also occur when using max(T,0), therefore, 1 K is used.
-  if radCalcMethod == 1 then
+  if radCalcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.No_approx then
     convPort.Q_flow = Modelica.Constants.sigma*eps*A_in_internal*(max(convPort.T, 1)*max(convPort.T, 1)*max(convPort.T, 1)*max(convPort.T, 1) - max(radPort.T, 1)*max(radPort.T, 1)*max(radPort.T, 1)*max(radPort.T, 1));
-  elseif radCalcMethod == 2 then
+  elseif radCalcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.Linear_wall_temp then
     convPort.Q_flow = Modelica.Constants.sigma*eps*A_in_internal*4*convPort.T*convPort.T*convPort.T*(convPort.T - radPort.T);
-  elseif radCalcMethod == 3 then
+  elseif radCalcMethod == AixLib.ThermalZones.HighOrder.Components.Types.CalcMethodRadiativeHeatTransfer.Linear_rad_temp then
     convPort.Q_flow = Modelica.Constants.sigma*eps*A_in_internal*4*radPort.T*radPort.T*radPort.T*(convPort.T - radPort.T);
   else
     convPort.Q_flow =Modelica.Constants.sigma*eps*A_in_internal*4*T_ref*T_ref*T_ref*(convPort.T - radPort.T);
diff --git a/AixLib/Utilities/IO/Files/BaseClasses/FileWriter.mo b/AixLib/Utilities/IO/Files/BaseClasses/FileWriter.mo
index 8474f0e76d..9e30b00f43 100644
--- a/AixLib/Utilities/IO/Files/BaseClasses/FileWriter.mo
+++ b/AixLib/Utilities/IO/Files/BaseClasses/FileWriter.mo
@@ -92,34 +92,34 @@ algorithm
           textString="%samplePeriod")}),                         Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(revisions="<html>
- <ul>
- <li>
- October 17, 2019 by Filip Jorissen:<br/>
- Avoiding overflow of string buffer in dymola.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1219\">#1219</a>.
- </li>
- <li>
- October 8, 2018 by Filip Jorissen:<br/>
- Added implementation for the parameter <code>significantDigits</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1041\">#1041</a>.
- </li>
- <li>
- September 6, 2018 by Filip Jorissen:<br/>
- Improved comment of <code>samplePeriod</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1010\">#1010</a>.
- </li>
- <li>
- May 10, 2018 by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
- </li>
- </ul>
- </html>",
+<ul>
+<li>
+October 17, 2019 by Filip Jorissen:<br/>
+Avoiding overflow of string buffer in dymola.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1219\">#1219</a>.
+</li>
+<li>
+October 8, 2018 by Filip Jorissen:<br/>
+Added implementation for the parameter <code>significantDigits</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1041\">#1041</a>.
+</li>
+<li>
+September 6, 2018 by Filip Jorissen:<br/>
+Improved comment of <code>samplePeriod</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1010\">#1010</a>.
+</li>
+<li>
+May 10, 2018 by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
+</li>
+</ul>
+</html>",
         info="<html>
- <p>
- Base class for a file writer.        
- See extending classes.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Base class for a file writer.        
+See extending classes.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FileWriter;
diff --git a/AixLib/Utilities/IO/Files/BaseClasses/FileWriterObject.mo b/AixLib/Utilities/IO/Files/BaseClasses/FileWriterObject.mo
index fadf1ea182..b6950c357d 100644
--- a/AixLib/Utilities/IO/Files/BaseClasses/FileWriterObject.mo
+++ b/AixLib/Utilities/IO/Files/BaseClasses/FileWriterObject.mo
@@ -17,16 +17,16 @@ extends ExternalObject;
       IncludeDirectory="modelica://AixLib/Resources/C-Sources");
 
     annotation(Documentation(info="<html>
- <p>
- Creates an empty file with name <code>fileName</code>.
- If <code>fileName</code> is used in another instance of
- <a href=\"modelica://AixLib.Utilities.IO.Files.CSVWriter\">
- AixLib.Utilities.IO.Files.CSVWriter</a>,
- the simulation stops with an error.
- </p>
- </html>",revisions="<html>
- c
- </html>"));
+<p>
+Creates an empty file with name <code>fileName</code>.
+If <code>fileName</code> is used in another instance of
+<a href=\"modelica://AixLib.Utilities.IO.Files.CSVWriter\">
+AixLib.Utilities.IO.Files.CSVWriter</a>,
+the simulation stops with an error.
+</p>
+</html>", revisions="<html>
+c
+</html>"));
   end constructor;
 
   function destructor "Release storage and close the external object"
@@ -35,34 +35,34 @@ extends ExternalObject;
     annotation(Include=" #include <fileWriterFree.c>",
     IncludeDirectory="modelica://AixLib/Resources/C-Sources");
   annotation(Documentation(info="<html>
- <p>
- Destructor that frees the memory of the object
- <code>FileWriter</code>.
- </p>
- </html>",
+<p>
+Destructor that frees the memory of the object
+<code>FileWriter</code>.
+</p>
+</html>",
   revisions="<html>
- <ul>
- <li>
- May 12, 2018, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+May 12, 2018, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end destructor;
 
 annotation(Documentation(info="<html>
- <p>
- Class derived from <code>ExternalObject</code> having two local external function definition,
- named <code>destructor</code> and <code>constructor</code> respectively.
- </p>
- </html>",
+<p>
+Class derived from <code>ExternalObject</code> having two local external function definition,
+named <code>destructor</code> and <code>constructor</code> respectively.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 10 2018, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 10 2018, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FileWriterObject;
diff --git a/AixLib/Utilities/IO/Files/BaseClasses/JSONWriterObject.mo b/AixLib/Utilities/IO/Files/BaseClasses/JSONWriterObject.mo
index 8d954b513f..0b30700f6e 100644
--- a/AixLib/Utilities/IO/Files/BaseClasses/JSONWriterObject.mo
+++ b/AixLib/Utilities/IO/Files/BaseClasses/JSONWriterObject.mo
@@ -16,16 +16,16 @@ extends ExternalObject;
       IncludeDirectory="modelica://AixLib/Resources/C-Sources");
 
     annotation(Documentation(info="<html>
- <p>
- Creates an empty file with name <code>fileName</code>.
- If <code>fileName</code> is used in another instance of
- <a href=\"modelica://AixLib.Utilities.IO.Files.CSVWriter\">
- AixLib.Utilities.IO.Files.CSVWriter</a>,
- the simulation stops with an error.
- </p>
- </html>",revisions="<html>
- c
- </html>"));
+<p>
+Creates an empty file with name <code>fileName</code>.
+If <code>fileName</code> is used in another instance of
+<a href=\"modelica://AixLib.Utilities.IO.Files.CSVWriter\">
+AixLib.Utilities.IO.Files.CSVWriter</a>,
+the simulation stops with an error.
+</p>
+</html>", revisions="<html>
+c
+</html>"));
   end constructor;
 
   function destructor "Release storage and close the external object, write data if needed"
@@ -34,34 +34,34 @@ extends ExternalObject;
     annotation(Include=" #include <jsonWriterFree.c>",
     IncludeDirectory="modelica://AixLib/Resources/C-Sources");
   annotation(Documentation(info="<html>
- <p>
- Destructor that frees the memory of the object
- <code>FileWriter</code>.
- </p>
- </html>",
+<p>
+Destructor that frees the memory of the object
+<code>FileWriter</code>.
+</p>
+</html>",
   revisions="<html>
- <ul>
- <li>
- April 15 2019, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"));
+<ul>
+<li>
+April 15 2019, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"));
   end destructor;
 
 annotation(Documentation(info="<html>
- <p>
- Class derived from <code>ExternalObject</code> having two local external function definition,
- named <code>destructor</code> and <code>constructor</code> respectively.
- </p>
- </html>",
+<p>
+Class derived from <code>ExternalObject</code> having two local external function definition,
+named <code>destructor</code> and <code>constructor</code> respectively.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 15 2019, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 15 2019, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end JSONWriterObject;
diff --git a/AixLib/Utilities/IO/Files/BaseClasses/OutputTime.mo b/AixLib/Utilities/IO/Files/BaseClasses/OutputTime.mo
index 733a727d62..f9422492e1 100644
--- a/AixLib/Utilities/IO/Files/BaseClasses/OutputTime.mo
+++ b/AixLib/Utilities/IO/Files/BaseClasses/OutputTime.mo
@@ -4,8 +4,8 @@ type OutputTime = enumeration(
     Terminal "Output results at terminal() time",
     Custom "Output results at custom time value")
     "Time when results are outputted" annotation (Documentation(info="<html>
- <p>
- Enumeration for when output files are written.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Enumeration for when output files are written.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Utilities/IO/Files/BaseClasses/WeeklyScheduleObject.mo b/AixLib/Utilities/IO/Files/BaseClasses/WeeklyScheduleObject.mo
new file mode 100644
index 0000000000..6fbf5c7df7
--- /dev/null
+++ b/AixLib/Utilities/IO/Files/BaseClasses/WeeklyScheduleObject.mo
@@ -0,0 +1,63 @@
+within AixLib.Utilities.IO.Files.BaseClasses;
+class WeeklyScheduleObject "Class that loads a weekly schedule"
+extends ExternalObject;
+  impure function constructor
+    "Creates an object for the weekly schedule"
+    extends Modelica.Icons.Function;
+    input Boolean tableOnFile "Table is on file";
+    input String sourceName "Data source";
+    input Real t_offset "When time=t_offset, the time is assumed to be monday at midnight";
+    input String data "Data, when tableOnFile=false";
+    output WeeklyScheduleObject weeklySchedule "Pointer to the weekly schedule";
+    external"C" weeklySchedule = weeklyScheduleInit(tableOnFile, sourceName, t_offset, data)
+    annotation (
+      Include="#include <WeeklySchedule.c>",
+      IncludeDirectory="modelica://AixLib/Resources/C-Sources");
+
+    annotation(Documentation(info="<html>
+<p>
+Object for storing weekly schedules.
+</p>
+</html>", revisions="<html>
+<ul>
+ <li>
+ March 9 2022, by Filip Jorissen:<br/>
+ First implementation.
+ </li>
+ </ul>
+</html>"));
+  end constructor;
+
+  pure function destructor "Release storage and close the external object, write data if needed"
+    input WeeklyScheduleObject weeklySchedule "Pointer to file writer object";
+    external "C" weeklyScheduleFree(weeklySchedule)
+    annotation(Include=" #include <WeeklyScheduleFree.c>",
+    IncludeDirectory="modelica://AixLib/Resources/C-Sources");
+  annotation(Documentation(info="<html>
+<p>
+Destructor for weekly schedule object.
+</p>
+</html>"));
+  end destructor;
+
+annotation(Documentation(info="<html>
+<p>
+Class definition for weekly schedule object used by
+<a href=\"modelica://AixLib.Utilities.IO.Files.WeeklySchedule\">
+AixLib.Utilities.IO.Files.WeeklySchedule</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+April 10 2022, by Filip Jorissen:<br/>
+Added parameter source implementation.
+</li>
+<li>
+March 9 2022, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end WeeklyScheduleObject;
diff --git a/AixLib/Utilities/IO/Files/BaseClasses/cacheVals.mo b/AixLib/Utilities/IO/Files/BaseClasses/cacheVals.mo
index 6962c9a5c4..a6c1e30d2b 100644
--- a/AixLib/Utilities/IO/Files/BaseClasses/cacheVals.mo
+++ b/AixLib/Utilities/IO/Files/BaseClasses/cacheVals.mo
@@ -9,16 +9,16 @@ function cacheVals
     IncludeDirectory="modelica://AixLib/Resources/C-Sources");
 
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- April 15 2019, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Function for writing data to cache such that the results can be written at destruction.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 15 2019, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Function for writing data to cache such that the results can be written at destruction.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end cacheVals;
diff --git a/AixLib/Utilities/IO/Files/BaseClasses/package.order b/AixLib/Utilities/IO/Files/BaseClasses/package.order
index 0bc16cc3e0..f76649d422 100644
--- a/AixLib/Utilities/IO/Files/BaseClasses/package.order
+++ b/AixLib/Utilities/IO/Files/BaseClasses/package.order
@@ -2,5 +2,6 @@ FileWriter
 FileWriterObject
 JSONWriterObject
 OutputTime
+WeeklyScheduleObject
 cacheVals
 writeJSON
diff --git a/AixLib/Utilities/IO/Files/BaseClasses/writeJSON.mo b/AixLib/Utilities/IO/Files/BaseClasses/writeJSON.mo
index ab1431cba2..af78bd0e10 100644
--- a/AixLib/Utilities/IO/Files/BaseClasses/writeJSON.mo
+++ b/AixLib/Utilities/IO/Files/BaseClasses/writeJSON.mo
@@ -9,16 +9,16 @@ function writeJSON
     IncludeDirectory="modelica://AixLib/Resources/C-Sources");
 
   annotation (Documentation(info="<html>
- <p>
- Function for writing data to a JSON file.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 15 2019, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function for writing data to a JSON file.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 15 2019, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end writeJSON;
diff --git a/AixLib/Utilities/IO/Files/CSVWriter.mo b/AixLib/Utilities/IO/Files/CSVWriter.mo
index 19a0ec7db3..9d82bba47f 100644
--- a/AixLib/Utilities/IO/Files/CSVWriter.mo
+++ b/AixLib/Utilities/IO/Files/CSVWriter.mo
@@ -21,54 +21,54 @@ initial algorithm
   annotation (
   defaultComponentName="csvWri",
   Documentation(info="<html>
- <p>This model samples the model inputs <code>u</code> and saves them to a .csv file,
- which can be read using e.g. Excel or Python.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The parameter <code>nin</code> defines the number of variables that are stored.
- In Dymola, this parameter is updated automatically when inputs are connected to the component.
- </p>
- <p>
- The parameter <code>fileName</code> defines to what file name the results
- are saved. The file is in the current working directory,
- unless an absolute path is provided.
- </p>
- <p>
- The parameter <code>samplePeriod</code> defines every how many seconds
- the inputs are saved to the file.
- </p>
- <h4>Options</h4>
- <p>
- The parameter <code>delimiter</code> can be used to choose a custom separator.
- </p>
- <p>
- By default the first line of the csv file consists of the file header.
- The column names can be defined using parameter <code>headerNames</code>.
- The header can be removed by setting <code>writeHeader=false</code>
- </p>
- <h4>Dynamics</h4>
- <p>
- This model samples the outputs at an equidistant interval and
- hence disregards the simulation tool output interval settings.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 17, 2019 by Filip Jorissen:<br/>
- Avoiding overflow of string buffer in dymola.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1219\">#1219</a>.
- </li>
- <li>
- July 7, 2018 by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
- </li>
- </ul>
- </html>"),Icon(graphics={                                                Text(
+<p>This model samples the model inputs <code>u</code> and saves them to a .csv file,
+which can be read using e.g. Excel or Python.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The parameter <code>nin</code> defines the number of variables that are stored.
+In Dymola, this parameter is updated automatically when inputs are connected to the component.
+</p>
+<p>
+The parameter <code>fileName</code> defines to what file name the results
+are saved. The file is in the current working directory,
+unless an absolute path is provided.
+</p>
+<p>
+The parameter <code>samplePeriod</code> defines every how many seconds
+the inputs are saved to the file.
+</p>
+<h4>Options</h4>
+<p>
+The parameter <code>delimiter</code> can be used to choose a custom separator.
+</p>
+<p>
+By default the first line of the csv file consists of the file header.
+The column names can be defined using parameter <code>headerNames</code>.
+The header can be removed by setting <code>writeHeader=false</code>
+</p>
+<h4>Dynamics</h4>
+<p>
+This model samples the outputs at an equidistant interval and
+hence disregards the simulation tool output interval settings.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 17, 2019 by Filip Jorissen:<br/>
+Avoiding overflow of string buffer in dymola.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1219\">#1219</a>.
+</li>
+<li>
+July 7, 2018 by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
+</li>
+</ul>
+</html>"), Icon(graphics={                                                Text(
           extent={{-88,90},{88,48}},
           textColor={0,0,127},
           horizontalAlignment=TextAlignment.Right,
-          textString="CSV")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="CSV")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CSVWriter;
diff --git a/AixLib/Utilities/IO/Files/CombiTimeTableWriter.mo b/AixLib/Utilities/IO/Files/CombiTimeTableWriter.mo
index d1740012bf..b75512e00b 100644
--- a/AixLib/Utilities/IO/Files/CombiTimeTableWriter.mo
+++ b/AixLib/Utilities/IO/Files/CombiTimeTableWriter.mo
@@ -22,58 +22,58 @@ initial algorithm
   annotation (
   defaultComponentName="tabWri",
   Documentation(info="<html>
- <p>This model samples the model inputs <code>u</code> and saves them to a .csv file,
- which can be read by a 
- <a href=\"modelica://Modelica.Blocks.Sources.CombiTimeTable\">
- Modelica.Blocks.Sources.CombiTimeTable</a>.
- The <a href=\"modelica://Modelica.Blocks.Sources.CombiTimeTable\">
- Modelica.Blocks.Sources.CombiTimeTable</a>
- must then have <code>tableName=\"csv\"</code>, as illustrated in the example
- <a href=\"modelica://AixLib.Utilities.IO.Files.Examples.CSVReader\">
- AixLib.Utilities.IO.Files.Examples.CSVReader</a>.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The parameter <code>nin</code> defines the number of variables that are stored.
- In Dymola, this parameter is updated automatically when inputs are connected to the component.
- </p>
- <p>
- The parameter <code>fileName</code> defines to what file name the results
- are saved. The file is in the current working directory,
- unless an absolute path is provided.
- </p>
- <p>
- The parameter <code>samplePeriod</code> defines every how many seconds
- the inputs are saved to the file.
- </p>
- <h4>Options</h4>
- <p>
- By default the first line of the csv file consists of the file header.
- The column names can be defined using parameter <code>headerNames</code>
- or the header can be removed by setting <code>writeHeader=false</code>
- </p>
- <h4>Dynamics</h4>
- <p>
- This model samples the outputs at an equidistant interval and
- hence disregards the simulation tool output interval settings.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 17, 2019 by Filip Jorissen:<br/>
- Avoiding overflow of string buffer in dymola.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1219\">#1219</a>.
- </li>
- <li>
- July 7, 2018 by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
- </li>
- </ul>
- </html>"),Icon(graphics={                                                Text(
+<p>This model samples the model inputs <code>u</code> and saves them to a .csv file,
+which can be read by a 
+<a href=\"modelica://Modelica.Blocks.Sources.CombiTimeTable\">
+Modelica.Blocks.Sources.CombiTimeTable</a>.
+The <a href=\"modelica://Modelica.Blocks.Sources.CombiTimeTable\">
+Modelica.Blocks.Sources.CombiTimeTable</a>
+must then have <code>tableName=\"csv\"</code>, as illustrated in the example
+<a href=\"modelica://AixLib.Utilities.IO.Files.Examples.CSVReader\">
+AixLib.Utilities.IO.Files.Examples.CSVReader</a>.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The parameter <code>nin</code> defines the number of variables that are stored.
+In Dymola, this parameter is updated automatically when inputs are connected to the component.
+</p>
+<p>
+The parameter <code>fileName</code> defines to what file name the results
+are saved. The file is in the current working directory,
+unless an absolute path is provided.
+</p>
+<p>
+The parameter <code>samplePeriod</code> defines every how many seconds
+the inputs are saved to the file.
+</p>
+<h4>Options</h4>
+<p>
+By default the first line of the csv file consists of the file header.
+The column names can be defined using parameter <code>headerNames</code>
+or the header can be removed by setting <code>writeHeader=false</code>
+</p>
+<h4>Dynamics</h4>
+<p>
+This model samples the outputs at an equidistant interval and
+hence disregards the simulation tool output interval settings.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 17, 2019 by Filip Jorissen:<br/>
+Avoiding overflow of string buffer in dymola.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1219\">#1219</a>.
+</li>
+<li>
+July 7, 2018 by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
+</li>
+</ul>
+</html>"), Icon(graphics={                                                Text(
           extent={{-88,90},{88,48}},
           textColor={0,0,127},
           horizontalAlignment=TextAlignment.Right,
-          textString="CombiTimeTable")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="CombiTimeTable")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CombiTimeTableWriter;
diff --git a/AixLib/Utilities/IO/Files/Examples/BaseClasses/PartialCSV.mo b/AixLib/Utilities/IO/Files/Examples/BaseClasses/PartialCSV.mo
index 7ab1e8a34e..df2aecf5ad 100644
--- a/AixLib/Utilities/IO/Files/Examples/BaseClasses/PartialCSV.mo
+++ b/AixLib/Utilities/IO/Files/Examples/BaseClasses/PartialCSV.mo
@@ -6,17 +6,17 @@ model PartialCSV "Base model for CSV reader and writer example"
   Modelica.Blocks.Sources.Step step(startTime=5) "Step function"
     annotation (Placement(transformation(extent={{-80,-40},{-60,-20}})));
   annotation (Documentation(revisions="<html>
- <ul>
- <li>
- May 14, 2018 by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Partial model that contains a step function and cosine signal.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+May 14, 2018 by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Partial model that contains a step function and cosine signal.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PartialCSV;
diff --git a/AixLib/Utilities/IO/Files/Examples/CSVReader.mo b/AixLib/Utilities/IO/Files/Examples/CSVReader.mo
index 01855d3b94..143b7e2432 100644
--- a/AixLib/Utilities/IO/Files/Examples/CSVReader.mo
+++ b/AixLib/Utilities/IO/Files/Examples/CSVReader.mo
@@ -17,33 +17,33 @@ model CSVReader "Reader for csv files generated by CSVWriter"
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/CSVReader.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model demonstrates how a <code>CombiTimeTable</code> can be used
- to read a text file that contains a table. The text file is stored in
- <code>AixLib//Resources/Data/Utilities/IO/Files/Examples/CSVReader/Data.txt</code>.
- It has the format of a file that can be generated by
- <a href=\"modelica://AixLib.Utilities.IO.Files.Examples.CSVWriter\">
- AixLib.Utilities.IO.Files.Examples.CSVWriter</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 8, 2022, by Michael Wetter:<br/>
- Corrected documentation and changed file name of text file as it is not a csv file.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1572\">#1572</a>.
- </li>
- <li>
- July 10, 2018 by Michael Wetter:<br/>
- Refactored implementation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/983\">#983</a>.
- </li>
- <li>
- May 14, 2018 by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model demonstrates how a <code>CombiTimeTable</code> can be used
+to read a text file that contains a table. The text file is stored in
+<code>AixLib//Resources/Data/Utilities/IO/Files/Examples/CSVReader/Data.txt</code>.
+It has the format of a file that can be generated by
+<a href=\"modelica://AixLib.Utilities.IO.Files.Examples.CSVWriter\">
+AixLib.Utilities.IO.Files.Examples.CSVWriter</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 8, 2022, by Michael Wetter:<br/>
+Corrected documentation and changed file name of text file as it is not a csv file.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1572\">#1572</a>.
+</li>
+<li>
+July 10, 2018 by Michael Wetter:<br/>
+Refactored implementation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/983\">#983</a>.
+</li>
+<li>
+May 14, 2018 by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CSVReader;
diff --git a/AixLib/Utilities/IO/Files/Examples/CSVWriter.mo b/AixLib/Utilities/IO/Files/Examples/CSVWriter.mo
index 847395c605..61d5653c2a 100644
--- a/AixLib/Utilities/IO/Files/Examples/CSVWriter.mo
+++ b/AixLib/Utilities/IO/Files/Examples/CSVWriter.mo
@@ -29,24 +29,24 @@ equation
       StopTime=10,
       Tolerance=1e-06),
   Documentation(revisions="<html>
- <ul>
- <li>
- October 8, 2018 by Filip Jorissen:<br/>
- Using implementation of the parameter <code>significantDigits</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1041\">#1041</a>.
- </li>
- <li>
- May 10, 2018 by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model demonstrates the use of the csv file writer.
- </p>
- </html>"),
+<ul>
+<li>
+October 8, 2018 by Filip Jorissen:<br/>
+Using implementation of the parameter <code>significantDigits</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1041\">#1041</a>.
+</li>
+<li>
+May 10, 2018 by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/924\">#924</a>.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model demonstrates the use of the csv file writer.
+</p>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/CSVWriter.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CSVWriter;
diff --git a/AixLib/Utilities/IO/Files/Examples/JSONWriter.mo b/AixLib/Utilities/IO/Files/Examples/JSONWriter.mo
index 372fd24b75..e513143918 100644
--- a/AixLib/Utilities/IO/Files/Examples/JSONWriter.mo
+++ b/AixLib/Utilities/IO/Files/Examples/JSONWriter.mo
@@ -55,23 +55,23 @@ equation
           0},{-40,-70},{0,-70}}, color={0,0,127}));
   annotation (
     Documentation(info="<html>
- <p>
- This model generates four json files,
- using a single or multiple inputs and at different points in time.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 9, 2019 by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1114\">#1114</a>.
- </li>
- </ul>
- </html>"),
+<p>
+This model generates four json files,
+using a single or multiple inputs and at different points in time.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 9, 2019 by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1114\">#1114</a>.
+</li>
+</ul>
+</html>"),
     experiment(
       StopTime=2,
       Tolerance=1e-06),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/JSONWriter.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end JSONWriter;
diff --git a/AixLib/Utilities/IO/Files/Examples/WeeklySchedule.mo b/AixLib/Utilities/IO/Files/Examples/WeeklySchedule.mo
new file mode 100644
index 0000000000..cb9dc3719d
--- /dev/null
+++ b/AixLib/Utilities/IO/Files/Examples/WeeklySchedule.mo
@@ -0,0 +1,55 @@
+within AixLib.Utilities.IO.Files.Examples;
+model WeeklySchedule "Weekly schedule example"
+  extends Modelica.Icons.Example;
+  parameter String data = "#test:
+mon:0:0:10          -  3   1  -
+tue,thu:20:30:59  123  -  45  -
+wed                12  1   4  -" "Contents of schedule.txt";
+  AixLib.Utilities.IO.Files.WeeklySchedule weeSchFil(
+    columns={2,3,4,5},
+    tableOnFile=true,
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/Data/schedule.txt"),
+    t_offset=1e6) "Weekly schedule example using file data source"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+
+  AixLib.Utilities.IO.Files.WeeklySchedule weeSchStri(
+    columns={2,3,4,5},
+    data=data,
+    t_offset=1e6) "Weekly schedule example using parameter data source"
+    annotation (Placement(transformation(extent={{-10,-32},{10,-12}})));
+  Diagnostics.AssertEquality assEqu[4](
+    each startTime=-10000,
+    each threShold=Modelica.Constants.small)
+    "Trigger an assertion if the outputs differ"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+equation
+  connect(weeSchFil.y, assEqu.u1)
+    annotation (Line(points={{11,30},{24,30},{24,6},{38,6}}, color={0,0,127}));
+  connect(weeSchStri.y, assEqu.u2) annotation (Line(points={{11,-22},{24,-22},{24,
+          -6},{38,-6}}, color={0,0,127}));
+  annotation (
+    Documentation(revisions="<html>
+<ul>
+<li>
+April 10 2022, by Filip Jorissen:<br/>
+Added parameter source implementation.
+</li>
+<li>
+March 21 2022, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Example and consistency test for a weekly schedule.
+</p>
+</html>"),
+    experiment(
+      StartTime=-10000,
+      StopTime=1000000,
+      Tolerance=1e-06),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/WeeklySchedule.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end WeeklySchedule;
diff --git a/AixLib/Utilities/IO/Files/Examples/WeeklySchedule7to19.mo b/AixLib/Utilities/IO/Files/Examples/WeeklySchedule7to19.mo
new file mode 100644
index 0000000000..7373524b84
--- /dev/null
+++ b/AixLib/Utilities/IO/Files/Examples/WeeklySchedule7to19.mo
@@ -0,0 +1,22 @@
+within AixLib.Utilities.IO.Files.Examples;
+model WeeklySchedule7to19
+  "Weekly schedule example that outputs 1 from 7:00 to 19:00 on week-days, and 0 otherwise"
+  extends Modelica.Icons.Example;
+
+  AixLib.Utilities.IO.Files.WeeklySchedule sch
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  annotation (
+    Documentation(
+    info="<html>
+<p>
+Example of a weekly schedule that outputs 1 from 7:00 to 19:00 on week-days, and 0 otherwise</p>
+</html>"),
+    experiment(
+      StartTime=0,
+      StopTime=1209600,
+      Tolerance=1e-06),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Examples/WeeklySchedule7to19.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end WeeklySchedule7to19;
diff --git a/AixLib/Utilities/IO/Files/Examples/package.order b/AixLib/Utilities/IO/Files/Examples/package.order
index ae8cb54b6e..7b08b021f6 100644
--- a/AixLib/Utilities/IO/Files/Examples/package.order
+++ b/AixLib/Utilities/IO/Files/Examples/package.order
@@ -1,4 +1,6 @@
 CSVReader
 CSVWriter
 JSONWriter
+WeeklySchedule
+WeeklySchedule7to19
 BaseClasses
diff --git a/AixLib/Utilities/IO/Files/JSONWriter.mo b/AixLib/Utilities/IO/Files/JSONWriter.mo
index 9688a67bdb..97bc97faf1 100644
--- a/AixLib/Utilities/IO/Files/JSONWriter.mo
+++ b/AixLib/Utilities/IO/Files/JSONWriter.mo
@@ -47,56 +47,56 @@ equation
   annotation (
   defaultComponentName="jsonWri",
   Documentation(info="<html>
- <p>
- This model samples the model inputs <code>u</code> and saves them to a json file.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The parameter <code>nin</code> defines the number of variables that are stored.
- In Dymola, this parameter is updated automatically when inputs are connected to the component.
- </p>
- <p>
- The parameter <code>fileName</code> defines to what file name the results
- are saved. The file is in the current working directory,
- unless an absolute path is provided.
- </p>
- <p>
- The parameter <code>keyNames</code> defines the key names that are used to 
- store the json values corresponding to the inputs <code>u</code>.
- </p>
- <h4>Dynamics</h4>
- <p>
- This model samples its inputs at the time defined by the parameter <code>outputTime</code>
- and writes them to the file <code>fileName</code>.
- The model has the following options:
- </p>
- <ul>
- <li>
- If <code>outputTime==OutputTime.Initial</code>, results are saved at initialisation.
- </li>
- <li>
- If <code>outputTime==OutputTime.Custom</code>, results are saved when the built-in variable
- <code>time</code> achieves <code>customTime</code>.
- </li>
- <li>
- If <code>outputTime==OutputTime.Terminal</code>, results are saved when the simulation terminates.
- </li>
- </ul>
- </html>",
+<p>
+This model samples the model inputs <code>u</code> and saves them to a json file.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The parameter <code>nin</code> defines the number of variables that are stored.
+In Dymola, this parameter is updated automatically when inputs are connected to the component.
+</p>
+<p>
+The parameter <code>fileName</code> defines to what file name the results
+are saved. The file is in the current working directory,
+unless an absolute path is provided.
+</p>
+<p>
+The parameter <code>keyNames</code> defines the key names that are used to 
+store the json values corresponding to the inputs <code>u</code>.
+</p>
+<h4>Dynamics</h4>
+<p>
+This model samples its inputs at the time defined by the parameter <code>outputTime</code>
+and writes them to the file <code>fileName</code>.
+The model has the following options:
+</p>
+<ul>
+<li>
+If <code>outputTime==OutputTime.Initial</code>, results are saved at initialisation.
+</li>
+<li>
+If <code>outputTime==OutputTime.Custom</code>, results are saved when the built-in variable
+<code>time</code> achieves <code>customTime</code>.
+</li>
+<li>
+If <code>outputTime==OutputTime.Terminal</code>, results are saved when the simulation terminates.
+</li>
+</ul>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 9, 2019 by Filip Jorissen:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1114\">#1114</a>.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+April 9, 2019 by Filip Jorissen:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1114\">#1114</a>.
+</li>
+</ul>
+</html>"),
   Icon(graphics={
          Text(
           extent={{-88,90},{88,48}},
           textColor={0,0,127},
           horizontalAlignment=TextAlignment.Right,
-          textString="JSON")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="JSON")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end JSONWriter;
diff --git a/AixLib/Utilities/IO/Files/Validation/WeeklyScheduleWindowsLineEndings.mo b/AixLib/Utilities/IO/Files/Validation/WeeklyScheduleWindowsLineEndings.mo
new file mode 100644
index 0000000000..8c315c365d
--- /dev/null
+++ b/AixLib/Utilities/IO/Files/Validation/WeeklyScheduleWindowsLineEndings.mo
@@ -0,0 +1,56 @@
+within AixLib.Utilities.IO.Files.Validation;
+model WeeklyScheduleWindowsLineEndings "Weekly schedule example"
+  extends Modelica.Icons.Example;
+  parameter String data = "double tab1(3,5) #test:
+mon:0:0:10          -  3   1  -
+tue,thu:20:30:59  123  -  45  -
+wed                12  1   4  -" "Contents of schedule.txt";
+  AixLib.Utilities.IO.Files.WeeklySchedule weeSchLin(
+    columns={2,3,4,5},
+    tableOnFile=true,
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/Data/schedule.txt"),
+    t_offset=1e6) "Weekly schedule example using file data source"
+    annotation (Placement(transformation(extent={{-10,20},{10,40}})));
+
+  AixLib.Utilities.IO.Files.WeeklySchedule weeSchWin(
+    columns={2,3,4,5},
+    tableOnFile=true,
+    fileName=Modelica.Utilities.Files.loadResource("modelica://AixLib/Resources/Data/scheduleWindows.txt"),
+    t_offset=1e6) "Weekly schedule example using parameter data source"
+    annotation (Placement(transformation(extent={{-10,-32},{10,-12}})));
+  Diagnostics.AssertEquality assEqu[4](
+    each startTime=-10000,
+    each threShold=Modelica.Constants.small)
+    "Trigger an assertion if the outputs differ"
+    annotation (Placement(transformation(extent={{40,-10},{60,10}})));
+equation
+  connect(weeSchLin.y, assEqu.u1)
+    annotation (Line(points={{11,30},{24,30},{24,6},{38,6}}, color={0,0,127}));
+  connect(weeSchWin.y, assEqu.u2) annotation (Line(points={{11,-22},{24,-22},{24,
+          -6},{38,-6}}, color={0,0,127}));
+  annotation (
+    Documentation(info="<html>
+<p>
+Example for a weekly schedule that reads the schedule data from a file.
+There are two file readers, one reading a file with Windows line endings and the other with Linux line endings.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+April 2, 2024, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1860\">IBPSA, #1860</a>.
+</li>
+</ul>
+</html>"),
+    experiment(
+      StartTime=-10000,
+      StopTime=1000000,
+      Tolerance=1e-06),
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Utilities/IO/Files/Validation/WeeklyScheduleWindowsLineEndings.mos"
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end WeeklyScheduleWindowsLineEndings;
diff --git a/AixLib/Utilities/IO/Files/Validation/package.mo b/AixLib/Utilities/IO/Files/Validation/package.mo
new file mode 100644
index 0000000000..86a027cde5
--- /dev/null
+++ b/AixLib/Utilities/IO/Files/Validation/package.mo
@@ -0,0 +1,12 @@
+within AixLib.Utilities.IO.Files;
+package Validation "Collection of models that validate the models that access files"
+  extends Modelica.Icons.ExamplesPackage;
+
+annotation (preferredView="info", Documentation(info="<html>
+<p>
+This package contains models that validate the models that access files.
+The examples plot various outputs. These model outputs are stored as reference data to
+allow continuous validation whenever models in the library change.
+</p>
+</html>"));
+end Validation;
diff --git a/AixLib/Utilities/IO/Files/Validation/package.order b/AixLib/Utilities/IO/Files/Validation/package.order
new file mode 100644
index 0000000000..a47e6a26b0
--- /dev/null
+++ b/AixLib/Utilities/IO/Files/Validation/package.order
@@ -0,0 +1 @@
+WeeklyScheduleWindowsLineEndings
diff --git a/AixLib/Utilities/IO/Files/WeeklySchedule.mo b/AixLib/Utilities/IO/Files/WeeklySchedule.mo
new file mode 100644
index 0000000000..3be1556b4e
--- /dev/null
+++ b/AixLib/Utilities/IO/Files/WeeklySchedule.mo
@@ -0,0 +1,127 @@
+within AixLib.Utilities.IO.Files;
+model WeeklySchedule "Weekly schedule"
+  extends Modelica.Blocks.Icons.DiscreteBlock;
+  parameter Integer[:] columns = {2}
+    "Columns of the schedule to be produced at the output y. First column is time, hence value must be 2 or larger";
+  parameter Boolean tableOnFile=false
+    "= true, if table is defined on file; false if defined through parameter data"
+    annotation(Dialog(group="Data source"));
+  parameter String fileName = ""
+    "Filename"
+    annotation(Dialog(group="Data source", enable=tableOnFile));
+  parameter String data = "double tab1(3,2)
+# For week-day, output 1 between 7:00 and 19:00, and 0 otherwise
+mon,tue,wed,thu,fri:7:00:00  1
+mon,tue,wed,thu,fri:19:00:00  0
+# For week-end, output always 0. Note that this line is redundant in this example.
+sat,sun:0:00:00 0"
+    "String data with weekly schedule"
+    annotation(Dialog(group="Data source",enable=not tableOnFile));
+  parameter Modelica.Units.SI.Time t_offset=0
+    "Timestamp that corresponds to midnight from Sunday to Monday";
+
+  Modelica.Blocks.Interfaces.RealOutput[n_columns] y=
+    {getCalendarValue(cal, iCol-1, time) for iCol in columns} "Schedule values"
+    annotation (Placement(transformation(extent={{100,-10},{120,10}})));
+
+protected
+  AixLib.Utilities.IO.Files.BaseClasses.WeeklyScheduleObject cal=
+      AixLib.Utilities.IO.Files.BaseClasses.WeeklyScheduleObject(tableOnFile, sourceName, t_offset, data)
+    "Schedule object";
+
+  final parameter Integer n_columns = size(columns,1) "Number of columns";
+  parameter String sourceName = if tableOnFile then fileName else getInstanceName() +".data";
+
+  pure function getCalendarValue
+    "Returns the interpolated (zero order hold) value"
+    extends Modelica.Icons.Function;
+    input AixLib.Utilities.IO.Files.BaseClasses.WeeklyScheduleObject ID "Pointer to file writer object";
+    input Integer iCol "Column index";
+    input Real timeIn "Time for look-up";
+    output Real y "Schedule value";
+    external "C" y=getScheduleValue(ID, iCol, timeIn)
+    annotation(Include="#include <WeeklyScheduleGetValue.c>",
+    IncludeDirectory="modelica://AixLib/Resources/C-Sources");
+  end getCalendarValue;
+
+  annotation (
+  defaultComponentName = "sch",
+  experiment(
+      StartTime=-10000,
+      StopTime=1000000,
+      Interval=100),
+      Documentation(
+        revisions="<html>
+<ul>
+<li>
+March 30 2024, by Filip Jorissen:<br/>
+Avoiding memory leaks for <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1861\">IBPSA, #1860</a>.
+</li>
+<li>
+April 10 2022, by Filip Jorissen:<br/>
+Added parameter source implementation.
+</li>
+<li>
+March 9 2022, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model interprets a schedule file and performs a weekly, cyclic extrapolation on the source data.
+An example for a schedule entry is
+</p>
+<pre>
+double tab1(3,2)
+# For week-day, output 1 between 7:00 and 19:00, and 0 otherwise
+mon,tue,wed,thu,fri:7:00:00  1
+mon,tue,wed,thu,fri:19:00:00  0
+# For week-end, output always 0
+sat,sun:0:00:00 0
+</pre>
+<p>
+The first row must start with <code>double tab1</code> and be followed by the number of rows (excluding comments) and number of columns, whereas
+the time column is considered the first column.<br/>
+Lines that start with '#' are comments.<br/>
+The list of week-days is separated by a comma, and ends with a colon, after which
+the time format for the start is listed in the format <code>hour:minute:second</code>.
+Week-day, hour, minute and second are optional fields, but if one of these fields is used,
+the fields coming before it in the sequence (week-day, hour, minute, second) must be used too.
+</p>
+<p>
+By default, schedules are read from the parameter <code>data</code> but optionally schedules can be read from a file.
+The parameter <code>columns</code> is used to specify which columns of the table should be produced at the output <code>y</code>.
+The first column is time, hence for the above example, set <code>columns = {2}</code>.
+</p>
+<p>
+See <a href=\"modelica://AixLib/Resources/Data/schedule.txt\">AixLib/Resources/Data/schedule.txt</a>
+for an example of the supported file format.
+</p>
+</html>"),
+    Icon(graphics={
+    Line(points={{40,24},{40,-88}}),
+        Ellipse(
+          extent={{-94,94},{16,-16}},
+          lineColor={160,160,164},
+          fillColor={215,215,215},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-40,38},{-14,38}},
+          thickness=0.5),
+        Line(
+          points={{-40,38},{-64,62}},
+          thickness=0.5),
+    Line(points={{56,24},{56,-88}}),
+    Line(points={{72,24},{72,-88}}),
+    Line(points={{88,24},{88,-88}}),
+    Line(points={{26,-8},{88,-8}}),
+    Line(points={{26,24},{26,-88}}),
+    Line(points={{26,-40},{88,-40}}),
+    Line(points={{26,-24},{88,-24}}),
+    Line(points={{26,-56},{88,-56}}),
+    Line(points={{26,-88},{88,-88}}),
+    Line(points={{26,-72},{88,-72}}),
+    Line(points={{26,24},{88,24}}),
+    Line(points={{26,8},{88,8}})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end WeeklySchedule;
diff --git a/AixLib/Utilities/IO/Files/package.order b/AixLib/Utilities/IO/Files/package.order
index 52a0c24aa0..41dcc44817 100644
--- a/AixLib/Utilities/IO/Files/package.order
+++ b/AixLib/Utilities/IO/Files/package.order
@@ -1,5 +1,7 @@
 CSVWriter
 CombiTimeTableWriter
 JSONWriter
+WeeklySchedule
 Examples
+Validation
 BaseClasses
diff --git a/AixLib/Utilities/IO/SignalExchange/Examples/BaseClasses/ExportedModel.mo b/AixLib/Utilities/IO/SignalExchange/Examples/BaseClasses/ExportedModel.mo
index db89db4780..c605c13bb2 100644
--- a/AixLib/Utilities/IO/SignalExchange/Examples/BaseClasses/ExportedModel.mo
+++ b/AixLib/Utilities/IO/SignalExchange/Examples/BaseClasses/ExportedModel.mo
@@ -29,19 +29,19 @@ model ExportedModel "Model to be exported as an FMU"
     annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
 
 annotation(Documentation(info="<html>
- <p>
- This is an example of a model that would be compiled in BOPTEST if the
- original model were using the signal exchange blocks. Note that inputs
- are added to activate and set values of control signals that can be overwritten
- and outputs are added to read signals from the read blocks.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 17, 2018, by David Blum:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is an example of a model that would be compiled in BOPTEST if the
+original model were using the signal exchange blocks. Note that inputs
+are added to activate and set values of control signals that can be overwritten
+and outputs are added to read signals from the read blocks.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 17, 2018, by David Blum:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ExportedModel;
diff --git a/AixLib/Utilities/IO/SignalExchange/Examples/BaseClasses/OriginalModel.mo b/AixLib/Utilities/IO/SignalExchange/Examples/BaseClasses/OriginalModel.mo
index d245de3088..6a4ae9507a 100644
--- a/AixLib/Utilities/IO/SignalExchange/Examples/BaseClasses/OriginalModel.mo
+++ b/AixLib/Utilities/IO/SignalExchange/Examples/BaseClasses/OriginalModel.mo
@@ -50,21 +50,20 @@ equation
     annotation (Line(points={{29,-20},{0,-20},{0,18}}, color={0,0,127}));
 
   annotation (Documentation(info="<html>
- <p>
- This is a model of a first order dynamic system with feedback control.
- Signal exchange blocks are implemented to overwrite either the setpoint or
- actuator control signals as well as read the output of the first order
- system.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 17, 2018, by David Blum:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-          Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
-        coordinateSystem(preserveAspectRatio=false)),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This is a model of a first order dynamic system with feedback control.
+Signal exchange blocks are implemented to overwrite either the setpoint or
+actuator control signals as well as read the output of the first order
+system.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 17, 2018, by David Blum:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
+        coordinateSystem(preserveAspectRatio=false)), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end OriginalModel;
diff --git a/AixLib/Utilities/IO/SignalExchange/Examples/FirstOrder.mo b/AixLib/Utilities/IO/SignalExchange/Examples/FirstOrder.mo
index 73f7987a4d..8fcbaea41a 100644
--- a/AixLib/Utilities/IO/SignalExchange/Examples/FirstOrder.mo
+++ b/AixLib/Utilities/IO/SignalExchange/Examples/FirstOrder.mo
@@ -28,24 +28,24 @@ equation
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/IO/SignalExchange/Examples/FirstOrder.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example uses the signal exchange blocks in an original model,
- <a href=\"modelica://AixLib.Utilities.IO.SignalExchange.Examples.BaseClasses.OriginalModel\">
- AixLib.Utilities.IO.SignalExchange.Examples.BaseClasses.OriginalModel</a>
- along with a corresponding model that would result if the original model were
- compiled with the BOPTEST parser, <a href=\"modelica://AixLib.Utilities.IO.SignalExchange.Examples.BaseClasses.ExportedModel\">
- AixLib.Utilities.IO.SignalExchange.Examples.BaseClasses.ExportedModel</a>
- to demonstrate the overwriting of either setpoint or actuator control signals
- and reading of signals.
- </p>
- </html>",
+<p>
+This example uses the signal exchange blocks in an original model,
+<a href=\"modelica://AixLib.Utilities.IO.SignalExchange.Examples.BaseClasses.OriginalModel\">
+AixLib.Utilities.IO.SignalExchange.Examples.BaseClasses.OriginalModel</a>
+along with a corresponding model that would result if the original model were
+compiled with the BOPTEST parser, <a href=\"modelica://AixLib.Utilities.IO.SignalExchange.Examples.BaseClasses.ExportedModel\">
+AixLib.Utilities.IO.SignalExchange.Examples.BaseClasses.ExportedModel</a>
+to demonstrate the overwriting of either setpoint or actuator control signals
+and reading of signals.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 17, 2018, by David Blum:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 17, 2018, by David Blum:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FirstOrder;
diff --git a/AixLib/Utilities/IO/SignalExchange/Examples/WeatherStation.mo b/AixLib/Utilities/IO/SignalExchange/Examples/WeatherStation.mo
index bb0e5266ab..4ec20094e3 100644
--- a/AixLib/Utilities/IO/SignalExchange/Examples/WeatherStation.mo
+++ b/AixLib/Utilities/IO/SignalExchange/Examples/WeatherStation.mo
@@ -17,20 +17,20 @@ equation
   __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/IO/SignalExchange/Examples/WeatherStation.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example uses the weather station signal exchange block,
- <a href=\"modelica://AixLib.Utilities.IO.SignalExchange.WeatherStation\">
- AixLib.Utilities.IO.SignalExchange.WeatherStation</a>
- along with a TMY weather data reader.
- </p>
- </html>",
+<p>
+This example uses the weather station signal exchange block,
+<a href=\"modelica://AixLib.Utilities.IO.SignalExchange.WeatherStation\">
+AixLib.Utilities.IO.SignalExchange.WeatherStation</a>
+along with a TMY weather data reader.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 29, 2020, by David Blum:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 29, 2020, by David Blum:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WeatherStation;
diff --git a/AixLib/Utilities/IO/SignalExchange/Overwrite.mo b/AixLib/Utilities/IO/SignalExchange/Overwrite.mo
index 11f42693c4..5643c8b728 100644
--- a/AixLib/Utilities/IO/SignalExchange/Overwrite.mo
+++ b/AixLib/Utilities/IO/SignalExchange/Overwrite.mo
@@ -27,51 +27,50 @@ equation
     annotation (Line(points={{11,0},{110,0}}, color={0,0,127}));
 
   annotation (Documentation(info="<html>
- <p>
- This block enables the overwriting of a control signal by an external program,
- as well as reading of its meta-data, without the need to explicitly propogate
- the external input or activation switch to a top-level model.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- This block is typically used by the BOPTEST framework
- (see <a href=\"https://github.com/ibpsa/project1-boptest\">BOPTEST</a>)
- to identify and activate control signals that can be overwritten by test
- controllers. It is used in combination with a dedicated parser to perform
- this task (see <a href=\"https://github.com/ibpsa/project1-boptest/tree/master/parsing\">Parser Code</a>).
- </p>
- <p>
- The input <code>u</code> is the signal to be overwritten. The output
- <code>y</code> will be equal to the input signal if the <code>activate</code>
- flag is <code>false</code> and will be equal to the external input signal <code>uExt</code>
- if the flag is <code>true</code>.
- </p>
- <p>
- It is important to add a brief description of the signal using the
- <code>description</code> parameter and assign a <code>min</code>,
- <code>max</code>, and <code>unit</code> to the input variable <code>u</code>
- by modifying its attributes.
- </p>
- </html>",
+<p>
+This block enables the overwriting of a control signal by an external program,
+as well as reading of its meta-data, without the need to explicitly propogate
+the external input or activation switch to a top-level model.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+This block is typically used by the BOPTEST framework
+(see <a href=\"https://github.com/ibpsa/project1-boptest\">BOPTEST</a>)
+to identify and activate control signals that can be overwritten by test
+controllers. It is used in combination with a dedicated parser to perform
+this task (see <a href=\"https://github.com/ibpsa/project1-boptest/tree/master/parsing\">Parser Code</a>).
+</p>
+<p>
+The input <code>u</code> is the signal to be overwritten. The output
+<code>y</code> will be equal to the input signal if the <code>activate</code>
+flag is <code>false</code> and will be equal to the external input signal <code>uExt</code>
+if the flag is <code>true</code>.
+</p>
+<p>
+It is important to add a brief description of the signal using the
+<code>description</code> parameter and assign a <code>min</code>,
+<code>max</code>, and <code>unit</code> to the input variable <code>u</code>
+by modifying its attributes.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 17, 2022 by David Blum:<br/>
- Made parameter <code>boptestOverwrite</code> unprotected.
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1585\">#1585</a>.
- </li>
- <li>
- July 17, 2019 by Michael Wetter:<br/>
- Changed parameter name from <code>Description</code> to <code>description</code>.
- </li>
- <li>
- December 17, 2018 by David Blum:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1059\">#1059</a>.
- </li>
- </ul>
- </html>"),
-          Icon(graphics={
+<ul>
+<li>
+February 17, 2022 by David Blum:<br/>
+Made parameter <code>boptestOverwrite</code> unprotected.
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1585\">#1585</a>.
+</li>
+<li>
+July 17, 2019 by Michael Wetter:<br/>
+Changed parameter name from <code>Description</code> to <code>description</code>.
+</li>
+<li>
+December 17, 2018 by David Blum:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1059\">#1059</a>.
+</li>
+</ul>
+</html>"),Icon(graphics={
         Line(points={{100,0},{42,0}}, color={0,0,127}),
         Line(points={{42,0},{-20,60}},
         color={0,0,127}),
@@ -115,6 +114,6 @@ revisions="<html>
           lineColor=DynamicSelect({235,235,235}, if activate.y then {0,255,0}
                     else {235,235,235}),
           fillColor=DynamicSelect({235,235,235}, if activate.y then {0,255,0}
-                    else {235,235,235}))}),
-  __Dymola_LockedEditing="Model from IBPSA");
+                    else {235,235,235}))}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Overwrite;
diff --git a/AixLib/Utilities/IO/SignalExchange/Read.mo b/AixLib/Utilities/IO/SignalExchange/Read.mo
index e50eebeb97..14db650842 100644
--- a/AixLib/Utilities/IO/SignalExchange/Read.mo
+++ b/AixLib/Utilities/IO/SignalExchange/Read.mo
@@ -14,8 +14,8 @@ model Read "Block that allows a signal to be read as an FMU output"
     KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.RelativeHumidity or
     KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.CO2Concentration)
     "Zone designation, required if KPIs is AirZoneTemperature, 
-     RadiativeZoneTemperature, OperativeZoneTemperature, RelativeHumidity, 
-     or CO2Concentration"
+    RadiativeZoneTemperature, OperativeZoneTemperature, RelativeHumidity, 
+    or CO2Concentration"
   annotation(Dialog(enable=(
     KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.AirZoneTemperature or
     KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.RadiativeZoneTemperature or
@@ -27,67 +27,67 @@ model Read "Block that allows a signal to be read as an FMU output"
     "Parameter that is used by tools to search for read block in models";
 
   annotation (Documentation(info="<html>
- <p>
- This block enables the reading of a signal and its meta-data by an external
- program without the need to explicitly propogate the signal to a top-level model.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- This block is typically used by the BOPTEST framework
- (see <a href=\"https://github.com/ibpsa/project1-boptest\">BOPTEST</a>)
- to identify and read signals as measurements by test
- controllers. It is used in combination with a dedicated parser to perform
- this task (see <a href=\"https://github.com/ibpsa/project1-boptest/tree/master/parsing\">Parser Code</a>).
- This block is also used by BOPTEST to specify if the signal is needed
- for calculation of specific key performance indicators (KPI).
- </p>
- <p>
- The block output <code>y</code> is equal to the input <code>u</code> so that
- the block can be used in line with connections.  However, input signal will
- also be directed to an external program as an output.
- </p>
- <p>
- It is important to add a brief description of the signal using the
- <code>description</code> parameter, assign a <code>unit</code> to the output 
- variable <code>y</code>, assign a type if needed for KPI
- calculation using the <code>KPIs</code> parameter, and assign a zone 
- designation using the <code>zone</code> parameter if the KPI calculation is
- specific to a particular zone (for multi-zone models). See documentation for 
- the parameter <code>zone</code> for more details.
- </p>
- </html>",
+<p>
+This block enables the reading of a signal and its meta-data by an external
+program without the need to explicitly propogate the signal to a top-level model.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+This block is typically used by the BOPTEST framework
+(see <a href=\"https://github.com/ibpsa/project1-boptest\">BOPTEST</a>)
+to identify and read signals as measurements by test
+controllers. It is used in combination with a dedicated parser to perform
+this task (see <a href=\"https://github.com/ibpsa/project1-boptest/tree/master/parsing\">Parser Code</a>).
+This block is also used by BOPTEST to specify if the signal is needed
+for calculation of specific key performance indicators (KPI).
+</p>
+<p>
+The block output <code>y</code> is equal to the input <code>u</code> so that
+the block can be used in line with connections.  However, input signal will
+also be directed to an external program as an output.
+</p>
+<p>
+It is important to add a brief description of the signal using the
+<code>description</code> parameter, assign a <code>unit</code> to the output 
+variable <code>y</code>, assign a type if needed for KPI
+calculation using the <code>KPIs</code> parameter, and assign a zone 
+designation using the <code>zone</code> parameter if the KPI calculation is
+specific to a particular zone (for multi-zone models). See documentation for 
+the parameter <code>zone</code> for more details.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- February 17, 2022 by David Blum:<br/>
- Made parameter <code>boptestRead</code> unprotected.
- This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1585\">#1585</a>.
- </li>
- <li>
- February 23, 2020 by David Blum:<br/>
- Added zone designation for KPI calculation by parameter <code>zone</code>.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1257\">#1257</a>.
- </li>
- <li>
- January 9, 2020 by David Blum:<br/>
- Updated documentation to prompt user to add unit to output.  
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1276\">#1276</a>.
- </li>
- <li>
- July 17, 2019 by Michael Wetter:<br/>
- Changed parameter name from <code>Description</code> to <code>description</code>.
- </li>
- <li>
- April 11, 2019 by Javier Arroyo:<br/>
- Enumeration type KPI tags added.
- </li>
- <li>
- December 17, 2018 by David Blum:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1059\">#1059</a>.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<ul>
+<li>
+February 17, 2022 by David Blum:<br/>
+Made parameter <code>boptestRead</code> unprotected.
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1585\">#1585</a>.
+</li>
+<li>
+February 23, 2020 by David Blum:<br/>
+Added zone designation for KPI calculation by parameter <code>zone</code>.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1257\">#1257</a>.
+</li>
+<li>
+January 9, 2020 by David Blum:<br/>
+Updated documentation to prompt user to add unit to output.  
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1276\">#1276</a>.
+</li>
+<li>
+July 17, 2019 by Michael Wetter:<br/>
+Changed parameter name from <code>Description</code> to <code>description</code>.
+</li>
+<li>
+April 11, 2019 by Javier Arroyo:<br/>
+Enumeration type KPI tags added.
+</li>
+<li>
+December 17, 2018 by David Blum:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1059\">#1059</a>.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Line(points={{22,60},{70,60}},  color={0,0,127}),
         Line(points={{-38,0},{22,60}}, color={0,0,127}),
         Line(points={{-100,0},{-38,0}}, color={0,0,127}),
@@ -119,6 +119,6 @@ revisions="<html>
             (KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.RadiativeZoneTemperature) or
             (KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.OperativeZoneTemperature) or
             (KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.RelativeHumidity) or
-            (KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.CO2Concentration)) then "zone" else ""))}),
-  __Dymola_LockedEditing="Model from IBPSA");
+            (KPIs==AixLib.Utilities.IO.SignalExchange.SignalTypes.SignalsForKPIs.CO2Concentration)) then "zone" else ""))}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Read;
diff --git a/AixLib/Utilities/IO/SignalExchange/SignalTypes/SignalsForKPIs.mo b/AixLib/Utilities/IO/SignalExchange/SignalTypes/SignalsForKPIs.mo
index ae7bd51a9b..bb984e51d0 100644
--- a/AixLib/Utilities/IO/SignalExchange/SignalTypes/SignalsForKPIs.mo
+++ b/AixLib/Utilities/IO/SignalExchange/SignalTypes/SignalsForKPIs.mo
@@ -25,64 +25,64 @@ type SignalsForKPIs = enumeration(
     FreshWaterFlowRate
       "FreshWaterFlowRate") "Signals used for the calculation of key performance indicators"
   annotation (Documentation(info="<html>
- <p>
- This enumeration defines the signal types that are used by BOPTEST
- to compute the key performance indices (KPI).
- </p>
- <p>
- The following signal types are supported.
- </p>
- <table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
- <tr><th>Value</th>
-     <th>Description</th>
- </tr>
- <tr><td><code>None</code></td>
-     <td>Not used for KPI</td>
- </tr>
- <tr><td><code>AirZoneTemperature</code></td>
-     <td>Air zone temperature</td>
- </tr>
- <tr><td><code>RadiativeZoneTemperature</code></td>
-     <td>Radiative zone temperature</td>
- </tr>
- <tr><td><code>OperativeZoneTemperature</code></td>
-     <td>Operative zone temperature</td>
- </tr>
- <tr><td><code>RelativeHumidity</code></td>
-     <td>Relative humidity</td>
- </tr>
- <tr><td><code>CO2Concentration</code></td>
-     <td>CO<sub>2</sub> concentration</td>
- </tr>
- <tr><td><code>ElectricPower</code></td>
-     <td>Electric power from grid</td>
- </tr>
- <tr><td><code>DistrictHeatingPower</code></td>
-     <td>Thermal power from district heating</td>
- </tr>
- <tr><td><code>GasPower</code></td>
-     <td>Thermal power from natural gas</td>
- </tr>
- <tr><td><code>BiomassPower</code></td>
-     <td>Thermal power from biomass</td>
- </tr>
- <tr><td><code>SolarThermalPower</code></td>
-     <td>Thermal power from solar thermal</td>
- </tr>
- <tr><td><code>FreshWaterFlowRate</code></td>
-     <td>FreshWaterFlowRate</td>
- </tr>
- </table>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2019, by Michael Wetter:<br/>
- Added documentation.
- </li>
- <li>
- April 10, 2019, by Javier Arroyo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This enumeration defines the signal types that are used by BOPTEST
+to compute the key performance indices (KPI).
+</p>
+<p>
+The following signal types are supported.
+</p>
+<table summary=\"summary\" border=\"1\" cellspacing=\"0\" cellpadding=\"2\" style=\"border-collapse:collapse;\">
+<tr><th>Value</th>
+    <th>Description</th>
+</tr>
+<tr><td><code>None</code></td>
+    <td>Not used for KPI</td>
+</tr>
+<tr><td><code>AirZoneTemperature</code></td>
+    <td>Air zone temperature</td>
+</tr>
+<tr><td><code>RadiativeZoneTemperature</code></td>
+    <td>Radiative zone temperature</td>
+</tr>
+<tr><td><code>OperativeZoneTemperature</code></td>
+    <td>Operative zone temperature</td>
+</tr>
+<tr><td><code>RelativeHumidity</code></td>
+    <td>Relative humidity</td>
+</tr>
+<tr><td><code>CO2Concentration</code></td>
+    <td>CO<sub>2</sub> concentration</td>
+</tr>
+<tr><td><code>ElectricPower</code></td>
+    <td>Electric power from grid</td>
+</tr>
+<tr><td><code>DistrictHeatingPower</code></td>
+    <td>Thermal power from district heating</td>
+</tr>
+<tr><td><code>GasPower</code></td>
+    <td>Thermal power from natural gas</td>
+</tr>
+<tr><td><code>BiomassPower</code></td>
+    <td>Thermal power from biomass</td>
+</tr>
+<tr><td><code>SolarThermalPower</code></td>
+    <td>Thermal power from solar thermal</td>
+</tr>
+<tr><td><code>FreshWaterFlowRate</code></td>
+    <td>FreshWaterFlowRate</td>
+</tr>
+</table>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2019, by Michael Wetter:<br/>
+Added documentation.
+</li>
+<li>
+April 10, 2019, by Javier Arroyo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Utilities/IO/SignalExchange/WeatherStation.mo b/AixLib/Utilities/IO/SignalExchange/WeatherStation.mo
index 7311ce45dc..913bf8ef7f 100644
--- a/AixLib/Utilities/IO/SignalExchange/WeatherStation.mo
+++ b/AixLib/Utilities/IO/SignalExchange/WeatherStation.mo
@@ -306,31 +306,31 @@ equation
       extent={{-6,3},{-6,3}},
       horizontalAlignment=TextAlignment.Right));
   annotation (Documentation(info="<html>
- <p>
- This block enables the reading of weather measurements and their meta-data by an external
- program without the need to explicitly propagate the signal to a top-level model.
- This block utilizes a number of pre-configured instances of
- <a href=\"modelica://AixLib.Utilities.IO.SignalExchange.Read\">
- AixLib.Utilities.IO.SignalExchange.Read</a>
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- This block is typically used by the BOPTEST framework
- (see <a href=\"https://github.com/ibpsa/project1-boptest\">BOPTEST</a>)
- to identify and read weather measurements by test
- controllers. It is used in combination with a dedicated parser to perform
- this task (see <a href=\"https://github.com/ibpsa/project1-boptest/tree/master/parsing\">Parser Code</a>).
- </p>
- </html>",
+<p>
+This block enables the reading of weather measurements and their meta-data by an external
+program without the need to explicitly propagate the signal to a top-level model.
+This block utilizes a number of pre-configured instances of
+<a href=\"modelica://AixLib.Utilities.IO.SignalExchange.Read\">
+AixLib.Utilities.IO.SignalExchange.Read</a>
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+This block is typically used by the BOPTEST framework
+(see <a href=\"https://github.com/ibpsa/project1-boptest\">BOPTEST</a>)
+to identify and read weather measurements by test
+controllers. It is used in combination with a dedicated parser to perform
+this task (see <a href=\"https://github.com/ibpsa/project1-boptest/tree/master/parsing\">Parser Code</a>).
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 2, 2020 by David Blum:<br/>
- First implementation.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1402\">#1402</a>.
- </li>
- </ul>
- </html>"),Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
+<ul>
+<li>
+October 2, 2020 by David Blum:<br/>
+First implementation.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1402\">#1402</a>.
+</li>
+</ul>
+</html>"), Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},
             {100,100}}),                                     graphics={
         Rectangle(
           extent={{-100,100},{100,-100}},
@@ -353,6 +353,6 @@ revisions="<html>
           lineColor={0,0,0},
           fillColor={244,125,35},
           fillPattern=FillPattern.Solid)}),                      Diagram(
-        coordinateSystem(preserveAspectRatio=false, extent={{-100,-120},{120,120}})),
-  __Dymola_LockedEditing="Model from IBPSA");
+        coordinateSystem(preserveAspectRatio=false, extent={{-100,-120},{120,120}})), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end WeatherStation;
diff --git a/AixLib/Utilities/Math/Average.mo b/AixLib/Utilities/Math/Average.mo
index 087346d803..aa33bc319f 100644
--- a/AixLib/Utilities/Math/Average.mo
+++ b/AixLib/Utilities/Math/Average.mo
@@ -5,21 +5,21 @@ equation
  y = AixLib.Utilities.Math.Functions.average(u=u, nin=nin);
 annotation (defaultComponentName="ave",
 Documentation(info="<html>
- <p>This block outputs the average of the vector. </p>
- </html>",
+<p>This block outputs the average of the vector. </p>
+</html>",
 revisions="<html>
- <ul>
- <li>November 28, 2013, by Marcus Fuchs:<br/>
- Changed block to use function average.
- </li>
- <li>
- April 3, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={Text(
+<ul>
+<li>November 28, 2013, by Marcus Fuchs:<br/>
+Changed block to use function average.
+</li>
+<li>
+April 3, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={Text(
           extent={{-74,46},{66,-58}},
           textColor={0,0,255},
-          textString="ave")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="ave")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Average;
diff --git a/AixLib/Utilities/Math/BesselJ0.mo b/AixLib/Utilities/Math/BesselJ0.mo
index e25ff7eb09..7659caebd8 100644
--- a/AixLib/Utilities/Math/BesselJ0.mo
+++ b/AixLib/Utilities/Math/BesselJ0.mo
@@ -5,14 +5,14 @@ equation
   y = AixLib.Utilities.Math.Functions.besselJ0(x=u);
   annotation (defaultComponentName="J0",
   Documentation(info="<html>
-   <p>This block computes the bessel function of the first kind of order 0, J0.</p>
- </html>",revisions="<html>
- <ul>
- <li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+  <p>This block computes the bessel function of the first kind of order 0, J0.</p>
+</html>", revisions="<html>
+<ul>
+<li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-90,38},{90,-34}},
           textColor={160,160,164},
-          textString="besselJ0()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="besselJ0()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselJ0;
diff --git a/AixLib/Utilities/Math/BesselJ1.mo b/AixLib/Utilities/Math/BesselJ1.mo
index 4b07615dd2..1122ad6ee1 100644
--- a/AixLib/Utilities/Math/BesselJ1.mo
+++ b/AixLib/Utilities/Math/BesselJ1.mo
@@ -5,14 +5,14 @@ equation
   y = AixLib.Utilities.Math.Functions.besselJ1(x=u);
   annotation (defaultComponentName="J1",
   Documentation(info="<html>
-   <p>This block computes the bessel function of the first kind of order 1, J1.</p>
- </html>",revisions="<html>
- <ul>
- <li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+  <p>This block computes the bessel function of the first kind of order 1, J1.</p>
+</html>", revisions="<html>
+<ul>
+<li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-90,38},{90,-34}},
           textColor={160,160,164},
-          textString="besselJ1()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="besselJ1()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselJ1;
diff --git a/AixLib/Utilities/Math/BesselY0.mo b/AixLib/Utilities/Math/BesselY0.mo
index 04f4b2b3eb..e31f767f5d 100644
--- a/AixLib/Utilities/Math/BesselY0.mo
+++ b/AixLib/Utilities/Math/BesselY0.mo
@@ -5,14 +5,14 @@ equation
   y = AixLib.Utilities.Math.Functions.besselY0(x=u);
   annotation (defaultComponentName="Y0",
   Documentation(info="<html>
-   <p>This block computes the bessel function of the second kind of order 0, Y0.</p>
- </html>",revisions="<html>
- <ul>
- <li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+  <p>This block computes the bessel function of the second kind of order 0, Y0.</p>
+</html>", revisions="<html>
+<ul>
+<li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-90,38},{90,-34}},
           textColor={160,160,164},
-          textString="besselY0()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="besselY0()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselY0;
diff --git a/AixLib/Utilities/Math/BesselY1.mo b/AixLib/Utilities/Math/BesselY1.mo
index c814386731..18e99c02dd 100644
--- a/AixLib/Utilities/Math/BesselY1.mo
+++ b/AixLib/Utilities/Math/BesselY1.mo
@@ -5,14 +5,14 @@ equation
   y = AixLib.Utilities.Math.Functions.besselY1(x=u);
   annotation (defaultComponentName="Y1",
   Documentation(info="<html>
-   <p>This block computes the bessel function of the second kind of order 1, Y1.</p>
- </html>",revisions="<html>
- <ul>
- <li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+  <p>This block computes the bessel function of the second kind of order 1, Y1.</p>
+</html>", revisions="<html>
+<ul>
+<li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-90,38},{90,-34}},
           textColor={160,160,164},
-          textString="besselY1()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="besselY1()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselY1;
diff --git a/AixLib/Utilities/Math/Bicubic.mo b/AixLib/Utilities/Math/Bicubic.mo
index 99d941a6fb..895e36d0b7 100644
--- a/AixLib/Utilities/Math/Bicubic.mo
+++ b/AixLib/Utilities/Math/Bicubic.mo
@@ -9,26 +9,26 @@ equation
           textColor={160,160,164},
           textString="bicubic()")}),
 Documentation(info="<html>
- <p>
- This block computes
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-  y = a<sub>1</sub>
-     + a<sub>2</sub>  x<sub>1</sub> + a<sub>3</sub>  x<sub>1</sub><sup>2</sup>
-     + a<sub>4</sub>  x<sub>2</sub> + a<sub>5</sub>  x<sub>2</sub><sup>2</sup>
-     + a<sub>6</sub>  x<sub>1</sub>  x<sub>2</sub>
-     + a<sub>7</sub>  x<sub>1</sub>^3
-     + a<sub>8</sub>  x<sub>2</sub>^3
-     + a<sub>9</sub>  x<sub>1</sub><sup>2</sup>  x<sub>2</sub>
-     + a<sub>1</sub>0  x<sub>1</sub>  x<sub>2</sub><sup>2</sup>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- Sep 17, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This block computes
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+ y = a<sub>1</sub>
+    + a<sub>2</sub>  x<sub>1</sub> + a<sub>3</sub>  x<sub>1</sub><sup>2</sup>
+    + a<sub>4</sub>  x<sub>2</sub> + a<sub>5</sub>  x<sub>2</sub><sup>2</sup>
+    + a<sub>6</sub>  x<sub>1</sub>  x<sub>2</sub>
+    + a<sub>7</sub>  x<sub>1</sub>^3
+    + a<sub>8</sub>  x<sub>2</sub>^3
+    + a<sub>9</sub>  x<sub>1</sub><sup>2</sup>  x<sub>2</sub>
+    + a<sub>1</sub>0  x<sub>1</sub>  x<sub>2</sub><sup>2</sup>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Sep 17, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Bicubic;
diff --git a/AixLib/Utilities/Math/Binomial.mo b/AixLib/Utilities/Math/Binomial.mo
index f79b137196..a582eeb530 100644
--- a/AixLib/Utilities/Math/Binomial.mo
+++ b/AixLib/Utilities/Math/Binomial.mo
@@ -13,13 +13,13 @@ equation
           textColor={160,160,164},
           textString="binomial()")}),
     Documentation(info="<html>
-     <p>This block computes the binomial coefficient \"n choose k\".</p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+    <p>This block computes the binomial coefficient \"n choose k\".</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Binomial;
diff --git a/AixLib/Utilities/Math/Biquadratic.mo b/AixLib/Utilities/Math/Biquadratic.mo
index 87d8804daa..44ffb9beee 100644
--- a/AixLib/Utilities/Math/Biquadratic.mo
+++ b/AixLib/Utilities/Math/Biquadratic.mo
@@ -9,23 +9,23 @@ equation
           textColor={160,160,164},
           textString="biquadratic()")}),
 Documentation(info="<html>
- <p>
- This block computes
- </p>
- <p align=\"center\" style=\"font-style:italic;\">
-   y =   a<sub>1</sub> + a<sub>2</sub>  x<sub>1</sub>
-         + a<sub>3</sub>  x<sub>1</sub><sup>2</sup>
-         + a<sub>4</sub>  x<sub>2</sub> + a<sub>5</sub>  x<sub>2</sub><sup>2</sup>
-         + a<sub>6</sub>  x<sub>1</sub>  x<sub>2</sub>
- </p>
- </html>",
+<p>
+This block computes
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+  y =   a<sub>1</sub> + a<sub>2</sub>  x<sub>1</sub>
+        + a<sub>3</sub>  x<sub>1</sub><sup>2</sup>
+        + a<sub>4</sub>  x<sub>2</sub> + a<sub>5</sub>  x<sub>2</sub><sup>2</sup>
+        + a<sub>6</sub>  x<sub>1</sub>  x<sub>2</sub>
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- Sep. 8, 2010, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+Sep. 8, 2010, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Biquadratic;
diff --git a/AixLib/Utilities/Math/BooleanReplicator.mo b/AixLib/Utilities/Math/BooleanReplicator.mo
index d049abff0f..8482781b0b 100644
--- a/AixLib/Utilities/Math/BooleanReplicator.mo
+++ b/AixLib/Utilities/Math/BooleanReplicator.mo
@@ -25,20 +25,20 @@ equation
           fillColor={255,0,255},
           fillPattern=FillPattern.Solid)}),
     Documentation(info="<html>
- <p>
- This block replicates the boolean input signal to an array of <code>nout</code> identical output signals.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 28, 2013, by Marcus Fuchs:<br/>
- Changed block to use Functions.booleanReplicator.
- </li>
- <li>
- July 27, 2012, by Kaustubh Phalak:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This block replicates the boolean input signal to an array of <code>nout</code> identical output signals.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 28, 2013, by Marcus Fuchs:<br/>
+Changed block to use Functions.booleanReplicator.
+</li>
+<li>
+July 27, 2012, by Kaustubh Phalak:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BooleanReplicator;
diff --git a/AixLib/Utilities/Math/Examples/Average.mo b/AixLib/Utilities/Math/Examples/Average.mo
index 12ebb870d4..c1301134d7 100644
--- a/AixLib/Utilities/Math/Examples/Average.mo
+++ b/AixLib/Utilities/Math/Examples/Average.mo
@@ -26,18 +26,18 @@ equation
   annotation ( experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Average.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Average\">
- AixLib.Utilities.Math.Average</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 28, 2013 by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Average\">
+AixLib.Utilities.Math.Average</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 28, 2013 by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Average;
diff --git a/AixLib/Utilities/Math/Examples/BesselJ0.mo b/AixLib/Utilities/Math/Examples/BesselJ0.mo
index ebb1a6a2de..725c545785 100644
--- a/AixLib/Utilities/Math/Examples/BesselJ0.mo
+++ b/AixLib/Utilities/Math/Examples/BesselJ0.mo
@@ -11,17 +11,17 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=30.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/BesselJ0.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.BesselJ0\">
- AixLib.Utilities.Math.BesselJ0</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.BesselJ0\">
+AixLib.Utilities.Math.BesselJ0</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselJ0;
diff --git a/AixLib/Utilities/Math/Examples/BesselJ1.mo b/AixLib/Utilities/Math/Examples/BesselJ1.mo
index d167984883..8be379dfe2 100644
--- a/AixLib/Utilities/Math/Examples/BesselJ1.mo
+++ b/AixLib/Utilities/Math/Examples/BesselJ1.mo
@@ -11,17 +11,17 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=30.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/BesselJ1.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.BesselJ1\">
- AixLib.Utilities.Math.BesselJ1</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.BesselJ1\">
+AixLib.Utilities.Math.BesselJ1</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselJ1;
diff --git a/AixLib/Utilities/Math/Examples/BesselY0.mo b/AixLib/Utilities/Math/Examples/BesselY0.mo
index 00745216ed..b9160be2f5 100644
--- a/AixLib/Utilities/Math/Examples/BesselY0.mo
+++ b/AixLib/Utilities/Math/Examples/BesselY0.mo
@@ -11,17 +11,17 @@ equation
   annotation (  experiment(Tolerance=1e-6, StartTime=0.1, StopTime=30.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/BesselY0.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.BesselY0\">
- AixLib.Utilities.Math.BesselY0</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.BesselY0\">
+AixLib.Utilities.Math.BesselY0</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselY0;
diff --git a/AixLib/Utilities/Math/Examples/BesselY1.mo b/AixLib/Utilities/Math/Examples/BesselY1.mo
index e34b1e91d9..83fb773d49 100644
--- a/AixLib/Utilities/Math/Examples/BesselY1.mo
+++ b/AixLib/Utilities/Math/Examples/BesselY1.mo
@@ -11,17 +11,17 @@ equation
   annotation (  experiment(Tolerance=1e-6, StartTime=0.1, StopTime=30.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/BesselY1.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.BesselY1\">
- AixLib.Utilities.Math.BesselY1</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.BesselY1\">
+AixLib.Utilities.Math.BesselY1</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselY1;
diff --git a/AixLib/Utilities/Math/Examples/Bicubic.mo b/AixLib/Utilities/Math/Examples/Bicubic.mo
index 8c69d6956b..e03c07b0c5 100644
--- a/AixLib/Utilities/Math/Examples/Bicubic.mo
+++ b/AixLib/Utilities/Math/Examples/Bicubic.mo
@@ -22,22 +22,22 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Bicubic.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Bicubic\">
- AixLib.Utilities.Math.Bicubic</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 14, 2012 by Michael Wetter:<br/>
- Changed input values of function.
- </li>
- <li>
- Sep 17, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Bicubic\">
+AixLib.Utilities.Math.Bicubic</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 14, 2012 by Michael Wetter:<br/>
+Changed input values of function.
+</li>
+<li>
+Sep 17, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Bicubic;
diff --git a/AixLib/Utilities/Math/Examples/Binomial.mo b/AixLib/Utilities/Math/Examples/Binomial.mo
index 7b1ee7e93b..29c3b950c7 100644
--- a/AixLib/Utilities/Math/Examples/Binomial.mo
+++ b/AixLib/Utilities/Math/Examples/Binomial.mo
@@ -22,17 +22,17 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=11.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Binomial.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Binomial\">
- AixLib.Utilities.Math.Binomial</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Binomial\">
+AixLib.Utilities.Math.Binomial</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Binomial;
diff --git a/AixLib/Utilities/Math/Examples/Biquadratic.mo b/AixLib/Utilities/Math/Examples/Biquadratic.mo
index fee9546eda..e8fd10a78b 100644
--- a/AixLib/Utilities/Math/Examples/Biquadratic.mo
+++ b/AixLib/Utilities/Math/Examples/Biquadratic.mo
@@ -22,22 +22,22 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Biquadratic.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Biquadratic\">
- AixLib.Utilities.Math.Biquadratic</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 14, 2012 by Michael Wetter:<br/>
- Changed input values of function.
- </li>
- <li>
- Sep 17, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Biquadratic\">
+AixLib.Utilities.Math.Biquadratic</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 14, 2012 by Michael Wetter:<br/>
+Changed input values of function.
+</li>
+<li>
+Sep 17, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Biquadratic;
diff --git a/AixLib/Utilities/Math/Examples/BooleanReplicator.mo b/AixLib/Utilities/Math/Examples/BooleanReplicator.mo
index f8c8ee1ec1..d84820cbf7 100644
--- a/AixLib/Utilities/Math/Examples/BooleanReplicator.mo
+++ b/AixLib/Utilities/Math/Examples/BooleanReplicator.mo
@@ -15,22 +15,22 @@ annotation (experiment(Tolerance=1e-6, StopTime=600),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/BooleanReplicator.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.BooleanReplicator\">
- AixLib.Utilities.Math.BooleanReplicator</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 31, 2012, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- July 27, 2012, by Kaustubh Phalak:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.BooleanReplicator\">
+AixLib.Utilities.Math.BooleanReplicator</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 31, 2012, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+July 27, 2012, by Kaustubh Phalak:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BooleanReplicator;
diff --git a/AixLib/Utilities/Math/Examples/ExponentialIntegralE1.mo b/AixLib/Utilities/Math/Examples/ExponentialIntegralE1.mo
index f9ed33ae8d..6825219f8f 100644
--- a/AixLib/Utilities/Math/Examples/ExponentialIntegralE1.mo
+++ b/AixLib/Utilities/Math/Examples/ExponentialIntegralE1.mo
@@ -12,17 +12,17 @@ equation
   annotation (  experiment(Tolerance=1e-6, StartTime=0.01, StopTime=3.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/ExponentialIntegralE1.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.ExponentialIntegralE1\">
- AixLib.Utilities.Math.ExponentialIntegralE1</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.ExponentialIntegralE1\">
+AixLib.Utilities.Math.ExponentialIntegralE1</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ExponentialIntegralE1;
diff --git a/AixLib/Utilities/Math/Examples/Factorial.mo b/AixLib/Utilities/Math/Examples/Factorial.mo
index 806375785b..7a659915a9 100644
--- a/AixLib/Utilities/Math/Examples/Factorial.mo
+++ b/AixLib/Utilities/Math/Examples/Factorial.mo
@@ -18,17 +18,17 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=13.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Factorial.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Factorial\">
- AixLib.Utilities.Math.Factorial</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Factorial\">
+AixLib.Utilities.Math.Factorial</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Factorial;
diff --git a/AixLib/Utilities/Math/Examples/FallingFactorial.mo b/AixLib/Utilities/Math/Examples/FallingFactorial.mo
index a5c0dec8bd..da56f6d323 100644
--- a/AixLib/Utilities/Math/Examples/FallingFactorial.mo
+++ b/AixLib/Utilities/Math/Examples/FallingFactorial.mo
@@ -22,17 +22,17 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=11.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/FallingFactorial.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.FallingFactorial\">
- AixLib.Utilities.Math.FallingFactorial</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.FallingFactorial\">
+AixLib.Utilities.Math.FallingFactorial</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FallingFactorial;
diff --git a/AixLib/Utilities/Math/Examples/IntegerReplicator.mo b/AixLib/Utilities/Math/Examples/IntegerReplicator.mo
index 165058da44..e97d7e5558 100644
--- a/AixLib/Utilities/Math/Examples/IntegerReplicator.mo
+++ b/AixLib/Utilities/Math/Examples/IntegerReplicator.mo
@@ -15,22 +15,22 @@ annotation (experiment(Tolerance=1e-6, StopTime=2),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/IntegerReplicator.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.IntegerReplicator\">
- AixLib.Utilities.Math.IntegerReplicator</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 31, 2012, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- July 27, 2012, by Kaustubh Phalak:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.IntegerReplicator\">
+AixLib.Utilities.Math.IntegerReplicator</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 31, 2012, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+July 27, 2012, by Kaustubh Phalak:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IntegerReplicator;
diff --git a/AixLib/Utilities/Math/Examples/IntegratorWithReset.mo b/AixLib/Utilities/Math/Examples/IntegratorWithReset.mo
index a4c58e5327..4c280f9897 100644
--- a/AixLib/Utilities/Math/Examples/IntegratorWithReset.mo
+++ b/AixLib/Utilities/Math/Examples/IntegratorWithReset.mo
@@ -56,35 +56,35 @@ annotation (experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/IntegratorWithReset.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.IntegratorWithReset\">
- AixLib.Utilities.Math.IntegratorWithReset</a>
- with and without reset, and with different start values
- and reset values.
- </p>
- <p>
- The integrator <code>intWitRes1</code> is triggered by a sample trigger
- which becomes true at <i>t=0</i>, while <code>intWitRes2</code> is triggered
- by a boolean pulse with is true at <i>t=0</i>.
- Hence, <code>intWitRes1</code> starts with <code>y(0)=y_reset</code> while
- <code>intWitRes2</code> starts with <code>y(0)=y_start</code>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 29, 2016, by Michael Wetter:<br/>
- Added more test cases and adapted model to new parameterization.
- </li>
- <li>
- August 23, 2016, by Michael Wetter:<br/>
- Extended example to test initialization.
- </li>
- <li>
- August 2, 2016, by Philipp Mehrfeld:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.IntegratorWithReset\">
+AixLib.Utilities.Math.IntegratorWithReset</a>
+with and without reset, and with different start values
+and reset values.
+</p>
+<p>
+The integrator <code>intWitRes1</code> is triggered by a sample trigger
+which becomes true at <i>t=0</i>, while <code>intWitRes2</code> is triggered
+by a boolean pulse with is true at <i>t=0</i>.
+Hence, <code>intWitRes1</code> starts with <code>y(0)=y_reset</code> while
+<code>intWitRes2</code> starts with <code>y(0)=y_start</code>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 29, 2016, by Michael Wetter:<br/>
+Added more test cases and adapted model to new parameterization.
+</li>
+<li>
+August 23, 2016, by Michael Wetter:<br/>
+Extended example to test initialization.
+</li>
+<li>
+August 2, 2016, by Philipp Mehrfeld:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IntegratorWithReset;
diff --git a/AixLib/Utilities/Math/Examples/Interpolate.mo b/AixLib/Utilities/Math/Examples/Interpolate.mo
new file mode 100644
index 0000000000..86f892d89b
--- /dev/null
+++ b/AixLib/Utilities/Math/Examples/Interpolate.mo
@@ -0,0 +1,55 @@
+within AixLib.Utilities.Math.Examples;
+model Interpolate "Example model of the Interpolate block"
+  extends Modelica.Icons.Example;
+
+  parameter Real table[:,:]=[-50,-0.08709; -25,-0.06158; -10,-0.03895; -5,-0.02754;
+    -3,-0.02133; -2,-0.01742; -1,-0.01232; 0,0; 1,0.01232; 2,0.01742; 3,0.02133;
+    4.5,0.02613; 50,0.02614]
+    "Table of mass flow rate in kg/s (second column) as a function of pressure difference in Pa (first column)";
+  parameter Real[:] xd=table[:,1] "x-axis support points";
+  parameter Real[size(xd, 1)] yd=table[:,2] "y-axis support points";
+  parameter Real[size(xd, 1)] d =
+    AixLib.Utilities.Math.Functions.splineDerivatives(
+      x=xd,
+      y=yd,
+      ensureMonotonicity=true) "Derivatives at the support points";
+
+  AixLib.Utilities.Math.Interpolate int(
+    xd=xd,
+    yd=yd,
+    d=d) "Interpolate block"
+    annotation (Placement(transformation(extent={{-10,-10},{10,10}})));
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=500,
+    height=100,
+    offset=-50) "Ramp from -50Pa to +50Pa"
+    annotation (Placement(transformation(extent={{-60,-10},{-40,10}})));
+
+equation
+  connect(ramp.y, int.u)
+    annotation (Line(points={{-39,0},{-12,0}}, color={0,0,127}));
+annotation (
+experiment(
+      StopTime=500,
+      Tolerance=1e-06),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Interpolate.mos"
+        "Simulate and plot"), Documentation(info="<html>
+<p>
+This example is the same as
+<a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.Interpolate\">
+AixLib.Utilities.Math.Functions.Examples.Interpolate</a>
+except that the block is used in place of the function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 29, 2024, by Hongxiang Fu:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1844\">IBPSA, #1844</a>.
+</li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Interpolate;
diff --git a/AixLib/Utilities/Math/Examples/InverseXRegularized.mo b/AixLib/Utilities/Math/Examples/InverseXRegularized.mo
index 8202dd10bf..5eb2f6dcd5 100644
--- a/AixLib/Utilities/Math/Examples/InverseXRegularized.mo
+++ b/AixLib/Utilities/Math/Examples/InverseXRegularized.mo
@@ -14,18 +14,18 @@ equation
   annotation (experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/InverseXRegularized.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.InverseXRegularized\">
- AixLib.Utilities.Math.InverseXRegularized</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 28, 2013, by Marcus Fuchs:<br/>
- Implementation based on Functions.inverseXRegularized.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.InverseXRegularized\">
+AixLib.Utilities.Math.InverseXRegularized</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 28, 2013, by Marcus Fuchs:<br/>
+Implementation based on Functions.inverseXRegularized.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InverseXRegularized;
diff --git a/AixLib/Utilities/Math/Examples/Polynomial.mo b/AixLib/Utilities/Math/Examples/Polynomial.mo
index 9dceba4e3f..2ee78fd5b1 100644
--- a/AixLib/Utilities/Math/Examples/Polynomial.mo
+++ b/AixLib/Utilities/Math/Examples/Polynomial.mo
@@ -12,24 +12,24 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Polynomial.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Polynomial\">
- AixLib.Utilities.Math.Polynomial</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2021, by Michael Wetter:<br/>
- Renamed class to correct typo in class name.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1524\">IBPSA, #1524</a>.
- </li>
- <li>
- November 28, 2013, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Polynomial\">
+AixLib.Utilities.Math.Polynomial</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2021, by Michael Wetter:<br/>
+Renamed class to correct typo in class name.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1524\">IBPSA, #1524</a>.
+</li>
+<li>
+November 28, 2013, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Polynomial;
diff --git a/AixLib/Utilities/Math/Examples/PowerLinearized.mo b/AixLib/Utilities/Math/Examples/PowerLinearized.mo
index 808b4617f4..38ab9204ca 100644
--- a/AixLib/Utilities/Math/Examples/PowerLinearized.mo
+++ b/AixLib/Utilities/Math/Examples/PowerLinearized.mo
@@ -12,18 +12,18 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/PowerLinearized.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.PowerLinearized\">
- AixLib.Utilities.Math.PowerLinearized</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 28, 2013, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.PowerLinearized\">
+AixLib.Utilities.Math.PowerLinearized</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 28, 2013, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerLinearized;
diff --git a/AixLib/Utilities/Math/Examples/QuadraticLinear.mo b/AixLib/Utilities/Math/Examples/QuadraticLinear.mo
index c01585562c..ca03c3408f 100644
--- a/AixLib/Utilities/Math/Examples/QuadraticLinear.mo
+++ b/AixLib/Utilities/Math/Examples/QuadraticLinear.mo
@@ -20,18 +20,18 @@ equation
   annotation ( experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/QuadraticLinear.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.QuadraticLinear\">
- AixLib.Utilities.Math.QuadraticLinear</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 29, 2013, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.QuadraticLinear\">
+AixLib.Utilities.Math.QuadraticLinear</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 29, 2013, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end QuadraticLinear;
diff --git a/AixLib/Utilities/Math/Examples/RegNonZeroPower.mo b/AixLib/Utilities/Math/Examples/RegNonZeroPower.mo
index a34df7170c..ac7a2a4e20 100644
--- a/AixLib/Utilities/Math/Examples/RegNonZeroPower.mo
+++ b/AixLib/Utilities/Math/Examples/RegNonZeroPower.mo
@@ -12,18 +12,18 @@ equation
   annotation ( experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/RegNonZeroPower.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.RegNonZeroPower\">
- AixLib.Utilities.Math.RegNonZeroPower</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 28, 2013, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.RegNonZeroPower\">
+AixLib.Utilities.Math.RegNonZeroPower</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 28, 2013, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RegNonZeroPower;
diff --git a/AixLib/Utilities/Math/Examples/SmoothBlocks.mo b/AixLib/Utilities/Math/Examples/SmoothBlocks.mo
index 871ff7ffbf..71055738c6 100644
--- a/AixLib/Utilities/Math/Examples/SmoothBlocks.mo
+++ b/AixLib/Utilities/Math/Examples/SmoothBlocks.mo
@@ -47,21 +47,21 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/SmoothBlocks.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of blocks that approximate non-differentiable functions
- by smooth functions.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 12, 2013, by Michael Wetter:<br/>
- Added missing parameter value for <code>sine1.freqHz</code>.
- </li>
- <li>
- August 15, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of blocks that approximate non-differentiable functions
+by smooth functions.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 12, 2013, by Michael Wetter:<br/>
+Added missing parameter value for <code>sine1.freqHz</code>.
+</li>
+<li>
+August 15, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothBlocks;
diff --git a/AixLib/Utilities/Math/Examples/SmoothExponential.mo b/AixLib/Utilities/Math/Examples/SmoothExponential.mo
index fa8150ac78..316ed3ab31 100644
--- a/AixLib/Utilities/Math/Examples/SmoothExponential.mo
+++ b/AixLib/Utilities/Math/Examples/SmoothExponential.mo
@@ -14,18 +14,18 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/SmoothExponential.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.SmoothExponential\">
- AixLib.Utilities.Math.SmoothExponential</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 28, 2013, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.SmoothExponential\">
+AixLib.Utilities.Math.SmoothExponential</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 28, 2013, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothExponential;
diff --git a/AixLib/Utilities/Math/Examples/SmoothHeaviside.mo b/AixLib/Utilities/Math/Examples/SmoothHeaviside.mo
index 8f553b94fa..7855c7a744 100644
--- a/AixLib/Utilities/Math/Examples/SmoothHeaviside.mo
+++ b/AixLib/Utilities/Math/Examples/SmoothHeaviside.mo
@@ -17,18 +17,18 @@ equation
   annotation (  experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/SmoothHeaviside.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.SmoothHeaviside\">
- AixLib.Utilities.Math.SmoothHeaviside</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2015, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.SmoothHeaviside\">
+AixLib.Utilities.Math.SmoothHeaviside</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2015, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothHeaviside;
diff --git a/AixLib/Utilities/Math/Examples/SmoothLimit.mo b/AixLib/Utilities/Math/Examples/SmoothLimit.mo
index d48bee9e62..339ce7d01d 100644
--- a/AixLib/Utilities/Math/Examples/SmoothLimit.mo
+++ b/AixLib/Utilities/Math/Examples/SmoothLimit.mo
@@ -17,18 +17,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/SmoothLimit.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.SmoothLimit\">
- AixLib.Utilities.Math.SmoothLimit</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 14, 2010, by Wangda Zuo, Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.SmoothLimit\">
+AixLib.Utilities.Math.SmoothLimit</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 14, 2010, by Wangda Zuo, Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothLimit;
diff --git a/AixLib/Utilities/Math/Examples/SmoothMin.mo b/AixLib/Utilities/Math/Examples/SmoothMin.mo
index 32f0a3c71f..00192e1914 100644
--- a/AixLib/Utilities/Math/Examples/SmoothMin.mo
+++ b/AixLib/Utilities/Math/Examples/SmoothMin.mo
@@ -26,24 +26,24 @@ __Dymola_Commands(file=
           "modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/SmoothMin.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.SmoothMin\">
- AixLib.Utilities.Math.SmoothMin</a>.
- </p>
- <p>
- This model also illustrates that the output can be larger than
- the minimum of the two input signals. Smaller values for <code>deltaX</code>
- will reduce this effect. Therefore do not use this function when the minimum
- output value should be respected.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 12, 2015, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.SmoothMin\">
+AixLib.Utilities.Math.SmoothMin</a>.
+</p>
+<p>
+This model also illustrates that the output can be larger than
+the minimum of the two input signals. Smaller values for <code>deltaX</code>
+will reduce this effect. Therefore do not use this function when the minimum
+output value should be respected.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 12, 2015, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothMin;
diff --git a/AixLib/Utilities/Math/Examples/Splice.mo b/AixLib/Utilities/Math/Examples/Splice.mo
index 65758c0203..612e505840 100644
--- a/AixLib/Utilities/Math/Examples/Splice.mo
+++ b/AixLib/Utilities/Math/Examples/Splice.mo
@@ -24,18 +24,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/Splice.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Splice\">
- AixLib.Utilities.Math.Splice</a>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 27, 2012, by Kaustubh Phalak:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Splice\">
+AixLib.Utilities.Math.Splice</a>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 27, 2012, by Kaustubh Phalak:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Splice;
diff --git a/AixLib/Utilities/Math/Examples/VectorFunctions.mo b/AixLib/Utilities/Math/Examples/VectorFunctions.mo
index 992b6e9eb2..88a8ffaa0d 100644
--- a/AixLib/Utilities/Math/Examples/VectorFunctions.mo
+++ b/AixLib/Utilities/Math/Examples/VectorFunctions.mo
@@ -49,16 +49,16 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Examples/VectorFunctions.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This model tests the implementation of functions that take a vector as an argument.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 15, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the implementation of functions that take a vector as an argument.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 15, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end VectorFunctions;
diff --git a/AixLib/Utilities/Math/Examples/package.order b/AixLib/Utilities/Math/Examples/package.order
index e437f39723..cc1ad2c1e8 100644
--- a/AixLib/Utilities/Math/Examples/package.order
+++ b/AixLib/Utilities/Math/Examples/package.order
@@ -12,6 +12,7 @@ Factorial
 FallingFactorial
 IntegerReplicator
 IntegratorWithReset
+Interpolate
 InverseXRegularized
 MovingAverage
 Polynomial
diff --git a/AixLib/Utilities/Math/ExponentialIntegralE1.mo b/AixLib/Utilities/Math/ExponentialIntegralE1.mo
index 6ac61992fa..0b40479527 100644
--- a/AixLib/Utilities/Math/ExponentialIntegralE1.mo
+++ b/AixLib/Utilities/Math/ExponentialIntegralE1.mo
@@ -5,14 +5,14 @@ equation
   y = AixLib.Utilities.Math.Functions.exponentialIntegralE1(x=u);
   annotation (defaultComponentName="E1",
   Documentation(info="<html>
-   <p>This block computes the exponential integral, E1.</p>
- </html>",revisions="<html>
- <ul>
- <li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+  <p>This block computes the exponential integral, E1.</p>
+</html>", revisions="<html>
+<ul>
+<li>July 17, 2018, by Massimo Cimmino:<br/>First implementation. </li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-90,38},{90,-34}},
           textColor={160,160,164},
-          textString="exponentialIntegralE1()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="exponentialIntegralE1()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ExponentialIntegralE1;
diff --git a/AixLib/Utilities/Math/Factorial.mo b/AixLib/Utilities/Math/Factorial.mo
index eca39c4777..5a88bafc45 100644
--- a/AixLib/Utilities/Math/Factorial.mo
+++ b/AixLib/Utilities/Math/Factorial.mo
@@ -11,13 +11,13 @@ equation
           textColor={160,160,164},
           textString="factorial()")}),
     Documentation(info="<html>
-     <p>This block computes the factorial of the integer input, <i>y=n!</i>.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+    <p>This block computes the factorial of the integer input, <i>y=n!</i>.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Factorial;
diff --git a/AixLib/Utilities/Math/FallingFactorial.mo b/AixLib/Utilities/Math/FallingFactorial.mo
index 929846eb25..7fef85bfdf 100644
--- a/AixLib/Utilities/Math/FallingFactorial.mo
+++ b/AixLib/Utilities/Math/FallingFactorial.mo
@@ -13,13 +13,13 @@ equation
           textColor={160,160,164},
           textString="fallingFactorial()")}),
     Documentation(info="<html>
-     <p>This block computes the falling factorial, <i>y = n<sup>&#7733;</sup></i>.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 17, 2018, by Massimo Cimmino:<br/>First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+    <p>This block computes the falling factorial, <i>y = n<sup>&#7733;</sup></i>.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 17, 2018, by Massimo Cimmino:<br/>First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FallingFactorial;
diff --git a/AixLib/Utilities/Math/Functions/BaseClasses/der_2_regNonZeroPower.mo b/AixLib/Utilities/Math/Functions/BaseClasses/der_2_regNonZeroPower.mo
index 8882c83596..cf5affa803 100644
--- a/AixLib/Utilities/Math/Functions/BaseClasses/der_2_regNonZeroPower.mo
+++ b/AixLib/Utilities/Math/Functions/BaseClasses/der_2_regNonZeroPower.mo
@@ -35,25 +35,25 @@ algorithm
 annotation (
 Documentation(
 info="<html>
- <p>
- Implementation of the second derivative of the function
- <a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
- AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
- </p>
- </html>",
+<p>
+Implementation of the second derivative of the function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
+AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Corrected wrong derivative implementation which omitted the <code>der_x</code> term.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- April 9, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Corrected wrong derivative implementation which omitted the <code>der_x</code> term.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+April 9, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_2_regNonZeroPower;
diff --git a/AixLib/Utilities/Math/Functions/BaseClasses/der_2_smoothTransition.mo b/AixLib/Utilities/Math/Functions/BaseClasses/der_2_smoothTransition.mo
index d55d44d2b9..e9ef1cf994 100644
--- a/AixLib/Utilities/Math/Functions/BaseClasses/der_2_smoothTransition.mo
+++ b/AixLib/Utilities/Math/Functions/BaseClasses/der_2_smoothTransition.mo
@@ -28,25 +28,25 @@ algorithm
 
 annotation (
 Documentation(info="<html>
- <p>
- This function is the 2nd order derivative of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition\">
- AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition</a>.
- </p>
- <h4>Implementation</h4>
- <p>
- For efficiency, the polynomial coefficients
- <code>a, b, c, d, e, f</code> and
- the inverse of the smoothing parameter <code>deltaInv</code>
- are exposed as arguments to this function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 11, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function is the 2nd order derivative of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition\">
+AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition</a>.
+</p>
+<h4>Implementation</h4>
+<p>
+For efficiency, the polynomial coefficients
+<code>a, b, c, d, e, f</code> and
+the inverse of the smoothing parameter <code>deltaInv</code>
+are exposed as arguments to this function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 11, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_2_smoothTransition;
diff --git a/AixLib/Utilities/Math/Functions/BaseClasses/der_inverseXRegularized.mo b/AixLib/Utilities/Math/Functions/BaseClasses/der_inverseXRegularized.mo
index 6bb5319208..3b1bb320ee 100644
--- a/AixLib/Utilities/Math/Functions/BaseClasses/der_inverseXRegularized.mo
+++ b/AixLib/Utilities/Math/Functions/BaseClasses/der_inverseXRegularized.mo
@@ -27,19 +27,19 @@ algorithm
 annotation (
 Documentation(
 info="<html>
- <p>
- Implementation of the first derivative of the function
- <a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
- AixLib.Utilities.Math.Functions.inverseXRegularized</a>.
- </p>
- </html>",
+<p>
+Implementation of the first derivative of the function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
+AixLib.Utilities.Math.Functions.inverseXRegularized</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 22, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 22, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_inverseXRegularized;
diff --git a/AixLib/Utilities/Math/Functions/BaseClasses/der_regNonZeroPower.mo b/AixLib/Utilities/Math/Functions/BaseClasses/der_regNonZeroPower.mo
index eacecb8271..8ffe70152a 100644
--- a/AixLib/Utilities/Math/Functions/BaseClasses/der_regNonZeroPower.mo
+++ b/AixLib/Utilities/Math/Functions/BaseClasses/der_regNonZeroPower.mo
@@ -31,29 +31,29 @@ algorithm
  annotation(derivative(order=2, zeroDerivative=n, zeroDerivative=delta)=der_2_regNonZeroPower,
 Documentation(
 info="<html>
- <p>
- Implementation of the first derivative of the function
- <a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
- AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
- </p>
- </html>",
+<p>
+Implementation of the first derivative of the function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
+AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Corrected wrong derivative implementation which omitted the <code>der_x</code> term.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- March 30, 2011, by Michael Wetter:<br/>
- Added <code>zeroDerivative</code> keyword.
- </li>
- <li>
- April 9, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Corrected wrong derivative implementation which omitted the <code>der_x</code> term.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+March 30, 2011, by Michael Wetter:<br/>
+Added <code>zeroDerivative</code> keyword.
+</li>
+<li>
+April 9, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_regNonZeroPower;
diff --git a/AixLib/Utilities/Math/Functions/BaseClasses/der_smoothTransition.mo b/AixLib/Utilities/Math/Functions/BaseClasses/der_smoothTransition.mo
index 76eeb5e9f8..9dc6499fb0 100644
--- a/AixLib/Utilities/Math/Functions/BaseClasses/der_smoothTransition.mo
+++ b/AixLib/Utilities/Math/Functions/BaseClasses/der_smoothTransition.mo
@@ -33,29 +33,29 @@ algorithm
           zeroDerivative=e,
           zeroDerivative=f)=AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition,
 Documentation(info="<html>
- <p>
- This function is the 1st order derivative of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition\">
- AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition</a>.
- </p>
- <h4>Implementation</h4>
- <p>
- For efficiency, the polynomial coefficients
- <code>a, b, c, d, e, f</code> and
- the inverse of the smoothing parameter <code>deltaInv</code>
- are exposed as arguments to this function.
- Also,
- its derivative is provided in
- <a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition\">
- AixLib.Utilities.Math.Functions.BaseClasses.der_2__smoothTransition</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 11, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function is the 1st order derivative of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition\">
+AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition</a>.
+</p>
+<h4>Implementation</h4>
+<p>
+For efficiency, the polynomial coefficients
+<code>a, b, c, d, e, f</code> and
+the inverse of the smoothing parameter <code>deltaInv</code>
+are exposed as arguments to this function.
+Also,
+its derivative is provided in
+<a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition\">
+AixLib.Utilities.Math.Functions.BaseClasses.der_2__smoothTransition</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 11, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_smoothTransition;
diff --git a/AixLib/Utilities/Math/Functions/BaseClasses/der_spliceFunction.mo b/AixLib/Utilities/Math/Functions/BaseClasses/der_spliceFunction.mo
index 73c2acacaa..edb0ae0e06 100644
--- a/AixLib/Utilities/Math/Functions/BaseClasses/der_spliceFunction.mo
+++ b/AixLib/Utilities/Math/Functions/BaseClasses/der_spliceFunction.mo
@@ -11,6 +11,7 @@ function der_spliceFunction "Derivative of splice function"
   input Real ddeltax=0;
   output Real out;
 protected
+  constant Real lim = 0.9999999999 "Limit in criterion for smoothing range";
   Real scaledX1 "x scaled to -1 ... 1 interval";
   Real scaledXp "x scaled to -pi/2 ... pi/2 interval";
   Real scaledXt "x scaled to -inf ... inf interval";
@@ -18,9 +19,9 @@ protected
   Real y;
 algorithm
   scaledX1 := x/deltax;
-  if scaledX1 <= -0.9999999999 then
+  if scaledX1 <= -lim then
     y := 0.0;
-  elseif scaledX1 >= 0.9999999999 then
+  elseif scaledX1 >= lim then
     y := 1.0;
   else
     scaledXp := scaledX1*0.5*Modelica.Constants.pi;
@@ -29,7 +30,7 @@ algorithm
   end if;
   out := dpos*y + (1 - y)*dneg;
 
-  if (abs(scaledX1) < 1) then
+  if (abs(scaledX1) < lim) then
     dscaledX1 := (dx - scaledX1*ddeltax)/deltax;
     out := out + (pos - neg)*dscaledX1*0.25*Modelica.Constants.pi*(1 - Modelica.Math.tanh(scaledXt)^2)*(scaledXt^2 + 1);
   end if;
@@ -38,29 +39,34 @@ annotation (
   smoothOrder=2,
 Documentation(
 info="<html>
- <p>
- Implementation of the first derivative of the function
- <a href=\"modelica://AixLib.Utilities.Math.Functions.spliceFunction\">
- AixLib.Utilities.Math.Functions.spliceFunction</a>.
- </p>
- </html>",
+<p>
+Implementation of the first derivative of the function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.spliceFunction\">
+AixLib.Utilities.Math.Functions.spliceFunction</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 13, 2021, by Michael Wetter:<br/>
- Changed implementation to not use <code>cosh</code> which overflows around <i>800</i>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1531\">IBPSA, issue 1531</a>.
- </li>
- <li>
- May 10, 2013, by Michael Wetter:<br/>
- Reformulated implementation to avoid unrequired computations.
- </li>
- <li>
- April 7, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 27, 2022, by Matthis Thorade:<br/>
+Changed limits.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1640\">IBPSA, issue #1640</a>.
+</li>
+<li>
+October 13, 2021, by Michael Wetter:<br/>
+Changed implementation to not use <code>cosh</code> which overflows around <i>800</i>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1531\">IBPSA, issue 1531</a>.
+</li>
+<li>
+May 10, 2013, by Michael Wetter:<br/>
+Reformulated implementation to avoid unrequired computations.
+</li>
+<li>
+April 7, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_spliceFunction;
diff --git a/AixLib/Utilities/Math/Functions/BaseClasses/smoothTransition.mo b/AixLib/Utilities/Math/Functions/BaseClasses/smoothTransition.mo
index f7c7bbf1ac..ed1f7c6fa2 100644
--- a/AixLib/Utilities/Math/Functions/BaseClasses/smoothTransition.mo
+++ b/AixLib/Utilities/Math/Functions/BaseClasses/smoothTransition.mo
@@ -36,45 +36,45 @@ annotation(smoothOrder=2,
           zeroDerivative=e,
           zeroDerivative=f)=AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition,
     Documentation(info="<html>
- <p>
- This function is used by
- <a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
- AixLib.Utilities.Math.Functions.inverseXRegularized</a>
- to provide a twice continuously differentiable transition between
- the different regions.
- The code has been implemented in a function as this allows
- to implement the function
- <a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
- AixLib.Utilities.Math.Functions.inverseXRegularized</a>
- in such a way that Dymola inlines it.
- However, this function will not be inlined as its body is too large.
- </p>
- <h4>Implementation</h4>
- <p>
- For efficiency, the polynomial coefficients
- <code>a, b, c, d, e, f</code> and
- the inverse of the smoothing parameter <code>deltaInv</code>
- are exposed as arguments to this function.
- Also,
- derivatives are provided in
- <a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition\">
- AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition</a>
- and in
- <a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition\">
- AixLib.Utilities.Math.Functions.BaseClasses.der_2__smoothTransition</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 12, 2018, by David Blum:<br/>
- Change if-statement to if-expression.  
- For issue <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1019\">#1019</a>.
- </li>
- <li>
- August 11, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function is used by
+<a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
+AixLib.Utilities.Math.Functions.inverseXRegularized</a>
+to provide a twice continuously differentiable transition between
+the different regions.
+The code has been implemented in a function as this allows
+to implement the function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
+AixLib.Utilities.Math.Functions.inverseXRegularized</a>
+in such a way that Dymola inlines it.
+However, this function will not be inlined as its body is too large.
+</p>
+<h4>Implementation</h4>
+<p>
+For efficiency, the polynomial coefficients
+<code>a, b, c, d, e, f</code> and
+the inverse of the smoothing parameter <code>deltaInv</code>
+are exposed as arguments to this function.
+Also,
+derivatives are provided in
+<a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition\">
+AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition</a>
+and in
+<a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition\">
+AixLib.Utilities.Math.Functions.BaseClasses.der_2__smoothTransition</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 12, 2018, by David Blum:<br/>
+Change if-statement to if-expression.  
+For issue <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1019\">#1019</a>.
+</li>
+<li>
+August 11, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end smoothTransition;
diff --git a/AixLib/Utilities/Math/Functions/Examples/BesselJ0.mo b/AixLib/Utilities/Math/Functions/Examples/BesselJ0.mo
index 70ce4b22bd..afe36a2e30 100644
--- a/AixLib/Utilities/Math/Functions/Examples/BesselJ0.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/BesselJ0.mo
@@ -14,17 +14,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=30.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for Bessel functions of the
- first kind of order 0, <i>J0</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for Bessel functions of the
+first kind of order 0, <i>J0</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselJ0;
diff --git a/AixLib/Utilities/Math/Functions/Examples/BesselJ1.mo b/AixLib/Utilities/Math/Functions/Examples/BesselJ1.mo
index ad34f5a6a4..8370ee58a4 100644
--- a/AixLib/Utilities/Math/Functions/Examples/BesselJ1.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/BesselJ1.mo
@@ -13,17 +13,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=30.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for Bessel functions of the
- first kind of order 1, <i>J1</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for Bessel functions of the
+first kind of order 1, <i>J1</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselJ1;
diff --git a/AixLib/Utilities/Math/Functions/Examples/BesselY0.mo b/AixLib/Utilities/Math/Functions/Examples/BesselY0.mo
index bc4e177faf..992723f2cb 100644
--- a/AixLib/Utilities/Math/Functions/Examples/BesselY0.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/BesselY0.mo
@@ -13,17 +13,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StartTime=0.1, StopTime=30.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for Bessel functions of the
- second kind of order 0, <i>Y0</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for Bessel functions of the
+second kind of order 0, <i>Y0</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselY0;
diff --git a/AixLib/Utilities/Math/Functions/Examples/BesselY1.mo b/AixLib/Utilities/Math/Functions/Examples/BesselY1.mo
index 56d550c28f..14e73c67f8 100644
--- a/AixLib/Utilities/Math/Functions/Examples/BesselY1.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/BesselY1.mo
@@ -13,17 +13,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StartTime=0.1, StopTime=30.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for Bessel functions of the
- second kind of order 1, <i>Y1</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for Bessel functions of the
+second kind of order 1, <i>Y1</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end BesselY1;
diff --git a/AixLib/Utilities/Math/Functions/Examples/Binomial.mo b/AixLib/Utilities/Math/Functions/Examples/Binomial.mo
index 34119dedab..a58dbca749 100644
--- a/AixLib/Utilities/Math/Functions/Examples/Binomial.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/Binomial.mo
@@ -22,17 +22,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=15.9),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for the evaluation of the
- binomial coefficient \"n choose k\".
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for the evaluation of the
+binomial coefficient \"n choose k\".
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Binomial;
diff --git a/AixLib/Utilities/Math/Functions/Examples/CubicHermite.mo b/AixLib/Utilities/Math/Functions/Examples/CubicHermite.mo
index 707e9904f2..c99dfb3d00 100644
--- a/AixLib/Utilities/Math/Functions/Examples/CubicHermite.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/CubicHermite.mo
@@ -54,23 +54,23 @@ algorithm
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=1.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for cubic hermite interpolation
- and linear extrapolation.
- The example use interpolation with two different settings: One settings
- produces a monotone cubic hermite, whereas the other setting
- does not enforce monotonicity.
- The resulting plot should look as shown below, where for better visibility, the support points have been marked with black dots.
- Notice that the red curve is monotone increasing.
- </p>
- <p align=\"center\"><img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Utilities/Math/Functions/Examples/cubicHermite.png\"/></p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 8, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for cubic hermite interpolation
+and linear extrapolation.
+The example use interpolation with two different settings: One settings
+produces a monotone cubic hermite, whereas the other setting
+does not enforce monotonicity.
+The resulting plot should look as shown below, where for better visibility, the support points have been marked with black dots.
+Notice that the red curve is monotonically increasing.
+</p>
+<p align=\"center\"><img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Utilities/Math/Functions/Examples/cubicHermite.png\"/></p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 8, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end CubicHermite;
diff --git a/AixLib/Utilities/Math/Functions/Examples/ExponentialIntegralE1.mo b/AixLib/Utilities/Math/Functions/Examples/ExponentialIntegralE1.mo
index 0e0980e54e..88721affc5 100644
--- a/AixLib/Utilities/Math/Functions/Examples/ExponentialIntegralE1.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/ExponentialIntegralE1.mo
@@ -14,17 +14,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StartTime=0.01, StopTime=3.0),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for the exponential integral,
- <i>E1</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for the exponential integral,
+<i>E1</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ExponentialIntegralE1;
diff --git a/AixLib/Utilities/Math/Functions/Examples/Factorial.mo b/AixLib/Utilities/Math/Functions/Examples/Factorial.mo
index 78bee371b0..565f73a7ba 100644
--- a/AixLib/Utilities/Math/Functions/Examples/Factorial.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/Factorial.mo
@@ -15,17 +15,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=12.9),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for the evaluation of
- factorials.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for the evaluation of
+factorials.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Factorial;
diff --git a/AixLib/Utilities/Math/Functions/Examples/FallingFactorial.mo b/AixLib/Utilities/Math/Functions/Examples/FallingFactorial.mo
index 670add1032..9128cd35ca 100644
--- a/AixLib/Utilities/Math/Functions/Examples/FallingFactorial.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/FallingFactorial.mo
@@ -19,17 +19,17 @@ equation
         "Simulate and plot"),
     experiment(Tolerance=1e-6, StopTime=13.9),
     Documentation(info="<html>
- <p>
- This example demonstrates the use of the function for the evaluation of
- falling factorials.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 6, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example demonstrates the use of the function for the evaluation of
+falling factorials.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 6, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end FallingFactorial;
diff --git a/AixLib/Utilities/Math/Functions/Examples/Interpolate.mo b/AixLib/Utilities/Math/Functions/Examples/Interpolate.mo
new file mode 100644
index 0000000000..b0c85a7997
--- /dev/null
+++ b/AixLib/Utilities/Math/Functions/Examples/Interpolate.mo
@@ -0,0 +1,71 @@
+within AixLib.Utilities.Math.Functions.Examples;
+model Interpolate "Test model for the interpolation function"
+  extends Modelica.Icons.Example;
+
+  parameter Real table[:,:]=[-50,-0.08709; -25,-0.06158; -10,-0.03895; -5,-0.02754;
+      -3,-0.02133; -2,-0.01742; -1,-0.01232; 0,0; 1,0.01232; 2,0.01742; 3,0.02133;
+      4.5,0.02613; 50,0.02614]
+      "Table of mass flow rate in kg/s (second column) as a function of pressure difference in Pa (first column)";
+
+  Modelica.Units.SI.PressureDifference dp
+    "Pressure difference";
+  Modelica.Units.SI.MassFlowRate m_flow
+    "Mass flow rate";
+
+protected
+  parameter Real[:] xd=table[:,1] "x-axis support points";
+  parameter Real[size(xd, 1)] yd=table[:,2] "y-axis support points";
+  parameter Real[size(xd, 1)] d(each fixed=false) "Derivatives at the support points";
+
+  Modelica.Blocks.Sources.Ramp ramp(
+    duration=500,
+    height=100,
+    offset=-50) "Ramp from -50Pa to +50Pa";
+initial equation
+  d = AixLib.Utilities.Math.Functions.splineDerivatives(
+    x=xd,
+    y=yd,
+    ensureMonotonicity=true);
+equation
+   dp=ramp.y;
+   m_flow = AixLib.Utilities.Math.Functions.interpolate(u=dp, xd=xd, yd=yd, d=d);
+
+  annotation (
+experiment(
+      StopTime=500,
+      Tolerance=1e-06),
+  __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/Interpolate.mos"
+        "Simulate and plot"), Documentation(info="<html>
+<p>
+This example demonstrates the function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.interpolate\">
+AixLib.Utilities.Math.Functions.interpolate</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 29, 2024, by Hongxiang Fu:<br/>
+Moved to
+<a href=\"modelica://AixLib.Utilities.Math.Functions.Examples\">
+AixLib.Utilities.Math.Functions</a>
+from
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses.Examples\">
+AixLib.Airflow.Multizone.BaseClasses</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1844\">IBPSA, #1844</a>.
+</li>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, 2020, by Klaas De Jonge:<br/>
+First implementation
+</li>
+</ul>
+</html>
+"), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Interpolate;
diff --git a/AixLib/Utilities/Math/Functions/Examples/InverseXDerivativeCheck.mo b/AixLib/Utilities/Math/Functions/Examples/InverseXDerivativeCheck.mo
index 83d12b72c7..68342bb1d3 100644
--- a/AixLib/Utilities/Math/Functions/Examples/InverseXDerivativeCheck.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/InverseXDerivativeCheck.mo
@@ -30,29 +30,29 @@ experiment(
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/InverseXDerivativeCheck.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model validates the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
- AixLib.Utilities.Math.Functions.inverseXRegularized</a>
- and its first order derivative
- <a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition\">
- AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition</a>.
- If the derivative implementation is wrong, the simulation will stop with an error.
- </p>
- </html>",
+<p>
+This model validates the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
+AixLib.Utilities.Math.Functions.inverseXRegularized</a>
+and its first order derivative
+<a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition\">
+AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition</a>.
+If the derivative implementation is wrong, the simulation will stop with an error.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- June 22, 2016, by Filip Jorissen:<br/>
- Changed example such that it explicitly uses
- <a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_inverseXRegularized\">
- AixLib.Utilities.Math.Functions.BaseClasses.der_inverseXRegularized</a>.
- </li>
- <li>
- August 11, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 22, 2016, by Filip Jorissen:<br/>
+Changed example such that it explicitly uses
+<a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_inverseXRegularized\">
+AixLib.Utilities.Math.Functions.BaseClasses.der_inverseXRegularized</a>.
+</li>
+<li>
+August 11, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InverseXDerivativeCheck;
diff --git a/AixLib/Utilities/Math/Functions/Examples/InverseXDerivative_2_Check.mo b/AixLib/Utilities/Math/Functions/Examples/InverseXDerivative_2_Check.mo
index 34345d65e7..59456b2237 100644
--- a/AixLib/Utilities/Math/Functions/Examples/InverseXDerivative_2_Check.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/InverseXDerivative_2_Check.mo
@@ -49,28 +49,28 @@ experiment(
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/InverseXDerivative_2_Check.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This model validates the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
- AixLib.Utilities.Math.Functions.inverseXRegularized</a>
- and its second order derivative
- <a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition\">
- AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition</a>.
- If the derivative implementation is wrong, the simulation will stop with an error.
- </p>
- </html>",
+<p>
+This model validates the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
+AixLib.Utilities.Math.Functions.inverseXRegularized</a>
+and its second order derivative
+<a href=\"modelica://AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition\">
+AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition</a>.
+If the derivative implementation is wrong, the simulation will stop with an error.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 12, 2017, by Thierry S. Nouidui:<br/>
- Added blocks for checking integration errors.
- This is needed for the JModelica verification tests.
- </li>
- <li>
- August 11, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 12, 2017, by Thierry S. Nouidui:<br/>
+Added blocks for checking integration errors.
+This is needed for the JModelica verification tests.
+</li>
+<li>
+August 11, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InverseXDerivative_2_Check;
diff --git a/AixLib/Utilities/Math/Functions/Examples/InverseXRegularized.mo b/AixLib/Utilities/Math/Functions/Examples/InverseXRegularized.mo
index d2bf3f11c4..de99594852 100644
--- a/AixLib/Utilities/Math/Functions/Examples/InverseXRegularized.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/InverseXRegularized.mo
@@ -30,18 +30,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/InverseXRegularized.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
- AixLib.Utilities.Math.Functions.inverseXRegularized</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 8, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.inverseXRegularized\">
+AixLib.Utilities.Math.Functions.inverseXRegularized</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 8, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InverseXRegularized;
diff --git a/AixLib/Utilities/Math/Functions/Examples/IsMonotonic.mo b/AixLib/Utilities/Math/Functions/Examples/IsMonotonic.mo
index c3d8e00585..767e0caa6a 100644
--- a/AixLib/Utilities/Math/Functions/Examples/IsMonotonic.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/IsMonotonic.mo
@@ -57,21 +57,21 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Mat
         "Simulate and plot"),
 Documentation(
 info="<html>
- <p>
- This example tests the correct implementation of the function
- <a href=\"modelica://AixLib.Utilities.Math.Functions.isMonotonic\">
- AixLib.Utilities.Math.Functions.isMonotonic</a>.
- If the function is implemented incorrect, the example will stop
- with an error.
- </p>
- </html>",
+<p>
+This example tests the correct implementation of the function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.isMonotonic\">
+AixLib.Utilities.Math.Functions.isMonotonic</a>.
+If the function is implemented incorrect, the example will stop
+with an error.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- January 8, 2014, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+January 8, 2014, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IsMonotonic;
diff --git a/AixLib/Utilities/Math/Functions/Examples/Polynomial.mo b/AixLib/Utilities/Math/Functions/Examples/Polynomial.mo
index 0559182226..4739c4e5c3 100644
--- a/AixLib/Utilities/Math/Functions/Examples/Polynomial.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/Polynomial.mo
@@ -9,38 +9,38 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/Polynomial.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example verifies the correct implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.polynomial\">
- AixLib.Utilities.Math.Functions.polynomial</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 14, 2016, by Michael Wetter:<br/>
- Renamed example and removed derivative computation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/602\">issue 602</a>.
- </li>
- <li>
- April 22, 2016, by Michael Wetter:<br/>
- Changed accuarcy test in assertion to use the relative error because the
- magnitude of <code>x</code> is <i>1E6</i> and hence testing an absolute
- error is too stringent.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
- </li>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- October 29, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example verifies the correct implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.polynomial\">
+AixLib.Utilities.Math.Functions.polynomial</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 14, 2016, by Michael Wetter:<br/>
+Renamed example and removed derivative computation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/602\">issue 602</a>.
+</li>
+<li>
+April 22, 2016, by Michael Wetter:<br/>
+Changed accuarcy test in assertion to use the relative error because the
+magnitude of <code>x</code> is <i>1E6</i> and hence testing an absolute
+error is too stringent.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
+</li>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+October 29, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Polynomial;
diff --git a/AixLib/Utilities/Math/Functions/Examples/PowerLinearized.mo b/AixLib/Utilities/Math/Functions/Examples/PowerLinearized.mo
index 77e460cd37..00a43daef4 100644
--- a/AixLib/Utilities/Math/Functions/Examples/PowerLinearized.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/PowerLinearized.mo
@@ -14,18 +14,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/PowerLinearized.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.powerLinearized\">
- AixLib.Utilities.Math.Functions.powerLinearized</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 8, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.powerLinearized\">
+AixLib.Utilities.Math.Functions.powerLinearized</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 8, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerLinearized;
diff --git a/AixLib/Utilities/Math/Functions/Examples/QuinticHermite.mo b/AixLib/Utilities/Math/Functions/Examples/QuinticHermite.mo
index 9008f31632..ec5c90793d 100644
--- a/AixLib/Utilities/Math/Functions/Examples/QuinticHermite.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/QuinticHermite.mo
@@ -27,18 +27,18 @@ equation
   ddy=der(dy);
   annotation (experiment(Tolerance=1E-6, StopTime=3),
     Documentation(info="<html>
- <p>
- Demonstration of the use of a quintic Hermite spline interpolation function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 19, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Demonstration of the use of a quintic Hermite spline interpolation function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 19, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/QuinticHermite.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end QuinticHermite;
diff --git a/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPower.mo b/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPower.mo
index f9c04b31e9..4520531e19 100644
--- a/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPower.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPower.mo
@@ -9,18 +9,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/RegNonZeroPower.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
- AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 8, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
+AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 8, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RegNonZeroPower;
diff --git a/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivativeCheck.mo b/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivativeCheck.mo
index 87e6335f9a..2f8a6e2a96 100644
--- a/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivativeCheck.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivativeCheck.mo
@@ -18,24 +18,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivativeCheck.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- April 14, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+April 14, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RegNonZeroPowerDerivativeCheck;
diff --git a/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivative_2_Check.mo b/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivative_2_Check.mo
index a899f28fae..07acc66334 100644
--- a/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivative_2_Check.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivative_2_Check.mo
@@ -39,24 +39,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/RegNonZeroPowerDerivative_2_Check.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- April 14, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+April 14, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RegNonZeroPowerDerivative_2_Check;
diff --git a/AixLib/Utilities/Math/Functions/Examples/RegStep.mo b/AixLib/Utilities/Math/Functions/Examples/RegStep.mo
index 68f50d8883..1d87198f44 100644
--- a/AixLib/Utilities/Math/Functions/Examples/RegStep.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/RegStep.mo
@@ -8,18 +8,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/RegStep.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.regStep\">
- AixLib.Utilities.Math.Functions.regStep</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 18, 2016, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.regStep\">
+AixLib.Utilities.Math.Functions.regStep</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 18, 2016, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end RegStep;
diff --git a/AixLib/Utilities/Math/Functions/Examples/SmoothExponentialDerivativeCheck.mo b/AixLib/Utilities/Math/Functions/Examples/SmoothExponentialDerivativeCheck.mo
index 1211204417..7c44e7a90b 100644
--- a/AixLib/Utilities/Math/Functions/Examples/SmoothExponentialDerivativeCheck.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/SmoothExponentialDerivativeCheck.mo
@@ -23,24 +23,24 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/SmoothExponentialDerivativeCheck.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- October 29, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+October 29, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothExponentialDerivativeCheck;
diff --git a/AixLib/Utilities/Math/Functions/Examples/SmoothHeavisideDerivatives.mo b/AixLib/Utilities/Math/Functions/Examples/SmoothHeavisideDerivatives.mo
index fa71af9226..80a4616e8e 100644
--- a/AixLib/Utilities/Math/Functions/Examples/SmoothHeavisideDerivatives.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/SmoothHeavisideDerivatives.mo
@@ -10,20 +10,20 @@ equation
   annotation (experiment(Tolerance=1e-6, StartTime=-1, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/SmoothHeavisideDerivatives.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This model tests the first and second derivative of the twice Lipschitz continuously differentiable function
- <a href=\"modelica://AixLib.Utilities.Math.Functions.smoothHeaviside\">
- AixLib.Utilities.Math.Functions.smoothHeaviside</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 21, 2019, by Michael Wetter:<br/>
- First implementation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1202\">issue 1202</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This model tests the first and second derivative of the twice Lipschitz continuously differentiable function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.smoothHeaviside\">
+AixLib.Utilities.Math.Functions.smoothHeaviside</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 21, 2019, by Michael Wetter:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1202\">issue 1202</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothHeavisideDerivatives;
diff --git a/AixLib/Utilities/Math/Functions/Examples/SmoothInterpolation.mo b/AixLib/Utilities/Math/Functions/Examples/SmoothInterpolation.mo
new file mode 100644
index 0000000000..5044a2178f
--- /dev/null
+++ b/AixLib/Utilities/Math/Functions/Examples/SmoothInterpolation.mo
@@ -0,0 +1,84 @@
+within AixLib.Utilities.Math.Functions.Examples;
+model SmoothInterpolation
+  "Test problem for cubic hermite splines that takes a vector of values as an argument"
+  extends Modelica.Icons.Example;
+  parameter Real[:] xSup={-1,1,5,6} "Support points";
+  parameter Real[size(xSup, 1)] ySup={-1,1,2,10} "Support points";
+
+  Real x "Independent variable";
+  Real y "Dependent variable without monotone interpolation";
+  Real yMonotone "Dependent variable with monotone interpolation";
+
+  Real y2 "Dependent variable without monotone interpolation for n=2";
+  Real y2Monotone "Dependent variable with monotone interpolation for n=2";
+
+  Real y1 "Dependent variable without monotone interpolation for n=1";
+  Real y1Monotone "Dependent variable with monotone interpolation for n=1";
+
+algorithm
+  x := xSup[1] + time*1.2*(xSup[size(xSup, 1)] - xSup[1]) - 0.5;
+  // Extrapolate or interpolate the data
+  y := AixLib.Utilities.Math.Functions.smoothInterpolation(
+    x=x,
+    xSup=xSup,
+    ySup=ySup,
+    ensureMonotonicity=false);
+  yMonotone := AixLib.Utilities.Math.Functions.smoothInterpolation(
+    x=x,
+    xSup=xSup,
+    ySup=ySup,
+    ensureMonotonicity=true);
+  // Case with n = 2
+  y2 := AixLib.Utilities.Math.Functions.smoothInterpolation(
+    x=x,
+    xSup=xSup[1:2],
+    ySup=ySup[1:2],
+    ensureMonotonicity=false);
+  y2Monotone := AixLib.Utilities.Math.Functions.smoothInterpolation(
+    x=x,
+    xSup=xSup[1:2],
+    ySup=ySup[1:2],
+    ensureMonotonicity=true);
+  // Case with n = 1
+  y1 := AixLib.Utilities.Math.Functions.smoothInterpolation(
+    x=x,
+    xSup={xSup[1]},
+    ySup={ySup[1]},
+    ensureMonotonicity=false);
+  y1Monotone := AixLib.Utilities.Math.Functions.smoothInterpolation(
+    x=x,
+    xSup={xSup[1]},
+    ySup={ySup[1]},
+    ensureMonotonicity=true);
+  annotation (
+    __Dymola_Commands(file=
+          "modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/SmoothInterpolation.mos"
+        "Simulate and plot"),
+    experiment(Tolerance=1e-6, StopTime=1.0),
+    Documentation(info="<html>
+<p>
+This example demonstrates the use of the function for cubic hermite interpolation
+and linear extrapolation.
+The example use interpolation with two different settings: One settings
+produces a monotone cubic hermite, whereas the other setting
+does not enforce monotonicity.
+The resulting plot should look as shown below, where for better visibility, the support points have been marked with black dots.
+Notice that the red curve is monotonically increasing.
+</p>
+<p align=\"center\"><img alt=\"image\" src=\"modelica://AixLib/Resources/Images/Utilities/Math/Functions/Examples/cubicHermite.png\"/></p>
+<p>
+This example also tests the function for the situation where only <i>2</i> or
+only <i>1</i> support points are provided.
+In the first case, the result will be linear function and in the second case,
+a constant value.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 1, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end SmoothInterpolation;
diff --git a/AixLib/Utilities/Math/Functions/Examples/SpliceFunction.mo b/AixLib/Utilities/Math/Functions/Examples/SpliceFunction.mo
index ada0803b0a..8cf6e0ba34 100644
--- a/AixLib/Utilities/Math/Functions/Examples/SpliceFunction.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/SpliceFunction.mo
@@ -10,18 +10,18 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/SpliceFunction.mos"
         "Simulate and plot"),
 Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 14, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 14, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpliceFunction;
diff --git a/AixLib/Utilities/Math/Functions/Examples/SpliceFunctionDerivativeCheck.mo b/AixLib/Utilities/Math/Functions/Examples/SpliceFunctionDerivativeCheck.mo
index 00ef7197d3..57908bfbd1 100644
--- a/AixLib/Utilities/Math/Functions/Examples/SpliceFunctionDerivativeCheck.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/SpliceFunctionDerivativeCheck.mo
@@ -43,30 +43,30 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/SpliceFunctionDerivativeCheck.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 13, 2021, by Michael Wetter:<br/>
- Added new output for higher order derivatives.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1531\">IBPSA, issue 1531</a>.
- </li>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- May 20, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 13, 2021, by Michael Wetter:<br/>
+Added new output for higher order derivatives.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1531\">IBPSA, issue 1531</a>.
+</li>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+May 20, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SpliceFunctionDerivativeCheck;
diff --git a/AixLib/Utilities/Math/Functions/Examples/TrapezoidalIntegration.mo b/AixLib/Utilities/Math/Functions/Examples/TrapezoidalIntegration.mo
index cc2f38b841..842c1f9da9 100644
--- a/AixLib/Utilities/Math/Functions/Examples/TrapezoidalIntegration.mo
+++ b/AixLib/Utilities/Math/Functions/Examples/TrapezoidalIntegration.mo
@@ -13,19 +13,19 @@ algorithm
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Math/Functions/Examples/TrapezoidalIntegration.mos"
         "Simulate and plot"),
                      Documentation(info="<html>
- <p>
- Tests the correct implementation of function
- <a href=\"modelica://AixLib.Utilities.Math.Functions.trapezoidalIntegration\">
- AixLib.Utilities.Math.Functions.trapezoidalIntegration</a>.
- </p>
- <p>Integrands y1[7]={72, 70, 64, 54, 40, 22, 0} are the function values of y = -2*x^2-72 for x = {0,1,2,3,4,5,6}. The trapezoidal integration over the 7 integrand points should give a result of 286.</p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 8, 2014, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Tests the correct implementation of function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.trapezoidalIntegration\">
+AixLib.Utilities.Math.Functions.trapezoidalIntegration</a>.
+</p>
+<p>Integrands y1[7]={72, 70, 64, 54, 40, 22, 0} are the function values of y = -2*x^2-72 for x = {0,1,2,3,4,5,6}. The trapezoidal integration over the 7 integrand points should give a result of 286.</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 8, 2014, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TrapezoidalIntegration;
diff --git a/AixLib/Utilities/Math/Functions/Examples/package.order b/AixLib/Utilities/Math/Functions/Examples/package.order
index 09732daa89..a073d84717 100644
--- a/AixLib/Utilities/Math/Functions/Examples/package.order
+++ b/AixLib/Utilities/Math/Functions/Examples/package.order
@@ -7,6 +7,7 @@ CubicHermite
 ExponentialIntegralE1
 Factorial
 FallingFactorial
+Interpolate
 InverseXDerivativeCheck
 InverseXDerivative_2_Check
 InverseXRegularized
@@ -20,6 +21,7 @@ RegNonZeroPowerDerivative_2_Check
 RegStep
 SmoothExponentialDerivativeCheck
 SmoothHeavisideDerivatives
+SmoothInterpolation
 SpliceFunction
 SpliceFunctionDerivativeCheck
 TrapezoidalIntegration
diff --git a/AixLib/Utilities/Math/Functions/average.mo b/AixLib/Utilities/Math/Functions/average.mo
index d184a21853..fbb9b276bc 100644
--- a/AixLib/Utilities/Math/Functions/average.mo
+++ b/AixLib/Utilities/Math/Functions/average.mo
@@ -9,15 +9,15 @@ algorithm
   y := sum(u)/nin;
 
   annotation (Documentation(info="<html>
- <p>This function outputs the average of the vector. </p>
- </html>",revisions="<html>
- <ul>
- <li>November 28, 2013, by Marcus Fuchs:<br/>
- Implementation based on Michael Wetter&apos;s block
- <a href=\"modelica://AixLib.Utilities.Math.Average\">
- AixLib.Utilities.Math.Average</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>This function outputs the average of the vector. </p>
+</html>", revisions="<html>
+<ul>
+<li>November 28, 2013, by Marcus Fuchs:<br/>
+Implementation based on Michael Wetter&apos;s block
+<a href=\"modelica://AixLib.Utilities.Math.Average\">
+AixLib.Utilities.Math.Average</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end average;
diff --git a/AixLib/Utilities/Math/Functions/besselJ0.mo b/AixLib/Utilities/Math/Functions/besselJ0.mo
index 059ccde7dd..ff7b2375bc 100644
--- a/AixLib/Utilities/Math/Functions/besselJ0.mo
+++ b/AixLib/Utilities/Math/Functions/besselJ0.mo
@@ -60,23 +60,23 @@ algorithm
 
 annotation (
 Documentation(info="<html>
- <p>
- Evaluates the Bessel function of the first kind of order 0 (<i>J<sub>0</sub></i>), based
- on the implementations of Press et al. (1986).
- </p>
- <h4>References</h4>
- <p>
- Press, William H., Brian P. Flannery, Saul A. Teukolsky, and William T.
- Vetterling. Numerical Recipes - The Art of Scientific Computing. Cambridge
- University Press (1986): 988 p.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 21, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Evaluates the Bessel function of the first kind of order 0 (<i>J<sub>0</sub></i>), based
+on the implementations of Press et al. (1986).
+</p>
+<h4>References</h4>
+<p>
+Press, William H., Brian P. Flannery, Saul A. Teukolsky, and William T.
+Vetterling. Numerical Recipes - The Art of Scientific Computing. Cambridge
+University Press (1986): 988 p.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end besselJ0;
diff --git a/AixLib/Utilities/Math/Functions/besselJ1.mo b/AixLib/Utilities/Math/Functions/besselJ1.mo
index 2b626b3727..c8ddadb6a3 100644
--- a/AixLib/Utilities/Math/Functions/besselJ1.mo
+++ b/AixLib/Utilities/Math/Functions/besselJ1.mo
@@ -60,23 +60,23 @@ algorithm
 
 annotation (
 Documentation(info="<html>
- <p>
- Evaluates the Bessel function of the first kind of order 1 (<i>J<sub>1</sub></i>), based
- on the implementations of Press et al. (1986).
- </p>
- <h4>References</h4>
- <p>
- Press, William H., Brian P. Flannery, Saul A. Teukolsky, and William T.
- Vetterling. Numerical Recipes - The Art of Scientific Computing. Cambridge
- University Press (1986): 988 p.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 21, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Evaluates the Bessel function of the first kind of order 1 (<i>J<sub>1</sub></i>), based
+on the implementations of Press et al. (1986).
+</p>
+<h4>References</h4>
+<p>
+Press, William H., Brian P. Flannery, Saul A. Teukolsky, and William T.
+Vetterling. Numerical Recipes - The Art of Scientific Computing. Cambridge
+University Press (1986): 988 p.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end besselJ1;
diff --git a/AixLib/Utilities/Math/Functions/besselY0.mo b/AixLib/Utilities/Math/Functions/besselY0.mo
index d679dbf838..70e9fc3fc8 100644
--- a/AixLib/Utilities/Math/Functions/besselY0.mo
+++ b/AixLib/Utilities/Math/Functions/besselY0.mo
@@ -60,23 +60,23 @@ algorithm
 
 annotation (
 Documentation(info="<html>
- <p>
- Evaluates the Bessel function of the second kind of order 0 (<i>Y<sub>0</sub></i>), based
- on the implementations of Press et al. (1986).
- </p>
- <h4>References</h4>
- <p>
- Press, William H., Brian P. Flannery, Saul A. Teukolsky, and William T.
- Vetterling. Numerical Recipes - The Art of Scientific Computing. Cambridge
- University Press (1986): 988 p.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 21, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Evaluates the Bessel function of the second kind of order 0 (<i>Y<sub>0</sub></i>), based
+on the implementations of Press et al. (1986).
+</p>
+<h4>References</h4>
+<p>
+Press, William H., Brian P. Flannery, Saul A. Teukolsky, and William T.
+Vetterling. Numerical Recipes - The Art of Scientific Computing. Cambridge
+University Press (1986): 988 p.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end besselY0;
diff --git a/AixLib/Utilities/Math/Functions/besselY1.mo b/AixLib/Utilities/Math/Functions/besselY1.mo
index 06d79ffb07..ba4beb6ae5 100644
--- a/AixLib/Utilities/Math/Functions/besselY1.mo
+++ b/AixLib/Utilities/Math/Functions/besselY1.mo
@@ -60,23 +60,23 @@ algorithm
 
 annotation (
 Documentation(info="<html>
- <p>
- Evaluates the Bessel function of the second kind of order 1 (<i>Y<sub>1</sub></i>), based
- on the implementations of Press et al. (1986).
- </p>
- <h4>References</h4>
- <p>
- Press, William H., Brian P. Flannery, Saul A. Teukolsky, and William T.
- Vetterling. Numerical Recipes - The Art of Scientific Computing. Cambridge
- University Press (1986): 988 p.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 21, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Evaluates the Bessel function of the second kind of order 1 (<i>Y<sub>1</sub></i>), based
+on the implementations of Press et al. (1986).
+</p>
+<h4>References</h4>
+<p>
+Press, William H., Brian P. Flannery, Saul A. Teukolsky, and William T.
+Vetterling. Numerical Recipes - The Art of Scientific Computing. Cambridge
+University Press (1986): 988 p.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 21, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end besselY1;
diff --git a/AixLib/Utilities/Math/Functions/bicubic.mo b/AixLib/Utilities/Math/Functions/bicubic.mo
index 43ad58c2d8..fa00d00210 100644
--- a/AixLib/Utilities/Math/Functions/bicubic.mo
+++ b/AixLib/Utilities/Math/Functions/bicubic.mo
@@ -20,24 +20,30 @@ algorithm
             + a[10] * x1 * x2Sq;
 
   annotation (smoothOrder=999, Documentation(info="<html>
- This function computes
- <p align=\"center\" style=\"font-style:italic;\">
-  y = a<sub>1</sub>
-     + a<sub>2</sub>  x<sub>1</sub> + a<sub>3</sub>  x<sub>1</sub><sup>2</sup>
-     + a<sub>4</sub>  x<sub>2</sub> + a<sub>5</sub>  x<sub>2</sub><sup>2</sup>
-     + a<sub>6</sub>  x<sub>1</sub>  x<sub>2</sub>
-     + a<sub>7</sub>  x<sub>1</sub>^3
-     + a<sub>8</sub>  x<sub>2</sub>^3
-     + a<sub>9</sub>  x<sub>1</sub><sup>2</sup>  x<sub>2</sub>
-     + a<sub>1</sub>0  x<sub>1</sub>  x<sub>2</sub><sup>2</sup>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- Sep 17, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function computes
+</p>
+<p align=\"center\" style=\"font-style:italic;\">
+ y = a<sub>1</sub>
+    + a<sub>2</sub>  x<sub>1</sub> + a<sub>3</sub>  x<sub>1</sub><sup>2</sup>
+    + a<sub>4</sub>  x<sub>2</sub> + a<sub>5</sub>  x<sub>2</sub><sup>2</sup>
+    + a<sub>6</sub>  x<sub>1</sub>  x<sub>2</sub>
+    + a<sub>7</sub>  x<sub>1</sub>^3
+    + a<sub>8</sub>  x<sub>2</sub>^3
+    + a<sub>9</sub>  x<sub>1</sub><sup>2</sup>  x<sub>2</sub>
+    + a<sub>1</sub>0  x<sub>1</sub>  x<sub>2</sub><sup>2</sup>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 25, 2023, by Michael Wetter:<br/>
+Corrected html formatting.
+</li>
+<li>
+Sep 17, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end bicubic;
diff --git a/AixLib/Utilities/Math/Functions/binomial.mo b/AixLib/Utilities/Math/Functions/binomial.mo
index faa0e485d2..f97044e9cd 100644
--- a/AixLib/Utilities/Math/Functions/binomial.mo
+++ b/AixLib/Utilities/Math/Functions/binomial.mo
@@ -16,16 +16,16 @@ algorithm
   end if;
 
 annotation (Documentation(info="<html>
- <p>
- Function that evaluates the binomial coefficient \"n choose k\".
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 9, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that evaluates the binomial coefficient \"n choose k\".
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 9, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end binomial;
diff --git a/AixLib/Utilities/Math/Functions/biquadratic.mo b/AixLib/Utilities/Math/Functions/biquadratic.mo
index b42967382c..8de1f09572 100644
--- a/AixLib/Utilities/Math/Functions/biquadratic.mo
+++ b/AixLib/Utilities/Math/Functions/biquadratic.mo
@@ -9,20 +9,20 @@ algorithm
   y :=a[1] + x1*(a[2] + a[3]*x1) + x2*(a[4]+ a[5]*x2) + a[6]*x1*x2;
 
   annotation (smoothOrder=999, Documentation(info="<html>
- This function computes
- <p align=\"center\" style=\"font-style:italic;\">
-   y =   a<sub>1</sub> + a<sub>2</sub>  x<sub>1</sub>
-         + a<sub>3</sub>  x<sub>1</sub><sup>2</sup>
-         + a<sub>4</sub>  x<sub>2</sub> + a<sub>5</sub>  x<sub>2</sub><sup>2</sup>
-         + a<sub>6</sub>  x<sub>1</sub>  x<sub>2</sub>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- Sep 8, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This function computes
+<p align=\"center\" style=\"font-style:italic;\">
+  y =   a<sub>1</sub> + a<sub>2</sub>  x<sub>1</sub>
+        + a<sub>3</sub>  x<sub>1</sub><sup>2</sup>
+        + a<sub>4</sub>  x<sub>2</sub> + a<sub>5</sub>  x<sub>2</sub><sup>2</sup>
+        + a<sub>6</sub>  x<sub>1</sub>  x<sub>2</sub>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+Sep 8, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end biquadratic;
diff --git a/AixLib/Utilities/Math/Functions/booleanReplicator.mo b/AixLib/Utilities/Math/Functions/booleanReplicator.mo
index 69449a83ea..41275c7723 100644
--- a/AixLib/Utilities/Math/Functions/booleanReplicator.mo
+++ b/AixLib/Utilities/Math/Functions/booleanReplicator.mo
@@ -9,15 +9,15 @@ algorithm
   y :=fill(u, nout);
 
   annotation (Documentation(info="<html>
- <p>This function replicates the boolean input signal to an array of <code>nout</code> identical output signals. </p>
- </html>",revisions="<html>
- <ul>
- <li>November 28, 2013, by Marcus Fuchs:<br/>
- Implementation based on Kaustubh Phalak&apos;s block
- <a href=\"modelica://AixLib.Utilities.Math.BooleanReplicator\">
- AixLib.Utilities.Math.BooleanReplicator</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>This function replicates the boolean input signal to an array of <code>nout</code> identical output signals. </p>
+</html>", revisions="<html>
+<ul>
+<li>November 28, 2013, by Marcus Fuchs:<br/>
+Implementation based on Kaustubh Phalak&apos;s block
+<a href=\"modelica://AixLib.Utilities.Math.BooleanReplicator\">
+AixLib.Utilities.Math.BooleanReplicator</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end booleanReplicator;
diff --git a/AixLib/Utilities/Math/Functions/cubicHermiteLinearExtrapolation.mo b/AixLib/Utilities/Math/Functions/cubicHermiteLinearExtrapolation.mo
index 4b7565470f..70ba1f8feb 100644
--- a/AixLib/Utilities/Math/Functions/cubicHermiteLinearExtrapolation.mo
+++ b/AixLib/Utilities/Math/Functions/cubicHermiteLinearExtrapolation.mo
@@ -28,24 +28,24 @@ algorithm
   end if;
   annotation(smoothOrder=1,
       Documentation(info="<html>
- <p>
- For <i>x<sub>1</sub> &lt; x &lt; x<sub>2</sub></i>, this function interpolates
- using cubic hermite spline. For <i>x</i> outside this interval, the function
- linearly extrapolates.
- </p>
- <p>
- For how to use this function, see
- <a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.CubicHermite\">
- AixLib.Utilities.Math.Functions.Examples.CubicHermite</a>.
- </p>
- </html>",
+<p>
+For <i>x<sub>1</sub> &lt; x &lt; x<sub>2</sub></i>, this function interpolates
+using cubic hermite spline. For <i>x</i> outside this interval, the function
+linearly extrapolates.
+</p>
+<p>
+For how to use this function, see
+<a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.CubicHermite\">
+AixLib.Utilities.Math.Functions.Examples.CubicHermite</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 27, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 27, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end cubicHermiteLinearExtrapolation;
diff --git a/AixLib/Utilities/Math/Functions/exponentialIntegralE1.mo b/AixLib/Utilities/Math/Functions/exponentialIntegralE1.mo
index 90efb3a3d0..640fc169aa 100644
--- a/AixLib/Utilities/Math/Functions/exponentialIntegralE1.mo
+++ b/AixLib/Utilities/Math/Functions/exponentialIntegralE1.mo
@@ -20,27 +20,27 @@ algorithm
 annotation (
 Inline=true,
 Documentation(info="<html>
- <p>
- Evaluates the exponential integral (E<sub>1</sub>), based
- on the polynomial and rational approximations of Abramowitz and Stegun (1964).
- </p>
- <h4>References</h4>
- <p>
- Abramowitz, Milton, and Irene A. Stegun. Handbook of Mathematical Functions
- with Formulas, Graphs, and Mathematical Tables. National Bureau of Standards.
- (1964): 1046 p.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- July 16, 2018 by Michael Wetter:<br/>
- Inlined function.
- </li>
- <li>
- March 21, 2018 by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Evaluates the exponential integral (E<sub>1</sub>), based
+on the polynomial and rational approximations of Abramowitz and Stegun (1964).
+</p>
+<h4>References</h4>
+<p>
+Abramowitz, Milton, and Irene A. Stegun. Handbook of Mathematical Functions
+with Formulas, Graphs, and Mathematical Tables. National Bureau of Standards.
+(1964): 1046 p.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+July 16, 2018 by Michael Wetter:<br/>
+Inlined function.
+</li>
+<li>
+March 21, 2018 by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end exponentialIntegralE1;
diff --git a/AixLib/Utilities/Math/Functions/factorial.mo b/AixLib/Utilities/Math/Functions/factorial.mo
index 9c9c259cb5..45f42bf5f1 100644
--- a/AixLib/Utilities/Math/Functions/factorial.mo
+++ b/AixLib/Utilities/Math/Functions/factorial.mo
@@ -14,16 +14,16 @@ algorithm
   end for;
 
 annotation (Documentation(info="<html>
- <p>
- Function that returns the factorial <i>n!</i> for <i>0 &le; n &le; 12</i>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 9, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that returns the factorial <i>n!</i> for <i>0 &le; n &le; 12</i>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 9, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end factorial;
diff --git a/AixLib/Utilities/Math/Functions/fallingFactorial.mo b/AixLib/Utilities/Math/Functions/fallingFactorial.mo
index 014084e466..658c049d7f 100644
--- a/AixLib/Utilities/Math/Functions/fallingFactorial.mo
+++ b/AixLib/Utilities/Math/Functions/fallingFactorial.mo
@@ -18,22 +18,22 @@ algorithm
   end if;
 
 annotation (Documentation(info="<html>
- <p>
- Function that evaluates the falling factorial \"k-permutations of n\".
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 22, 2019, by Michael Wetter:<br/>
- Changed upper limit for <code>maxInt</code>.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1145\">issue 1145</a>.
- </li>
- <li>
- February 9, 2018, by Massimo Cimmino:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that evaluates the falling factorial \"k-permutations of n\".
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 22, 2019, by Michael Wetter:<br/>
+Changed upper limit for <code>maxInt</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1145\">issue 1145</a>.
+</li>
+<li>
+February 9, 2018, by Massimo Cimmino:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end fallingFactorial;
diff --git a/AixLib/Utilities/Math/Functions/integerReplicator.mo b/AixLib/Utilities/Math/Functions/integerReplicator.mo
index 2d493d24b7..1635c9563d 100644
--- a/AixLib/Utilities/Math/Functions/integerReplicator.mo
+++ b/AixLib/Utilities/Math/Functions/integerReplicator.mo
@@ -9,17 +9,17 @@ algorithm
   y :=fill(u, nout);
 
   annotation (Documentation(info="<html>
- <p>This function replicates the integer input signal to an array of
- <code>nout</code> identical output signals. </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 28, 2013, by Marcus Fuchs:<br/>
- Implementation based on Kaustubh Phalak&apos;s block
- <a href=\"modelica://AixLib.Utilities.Math.IntegerReplicator\">
- AixLib.Utilities.Math.IntegerReplicator</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>This function replicates the integer input signal to an array of
+<code>nout</code> identical output signals. </p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 28, 2013, by Marcus Fuchs:<br/>
+Implementation based on Kaustubh Phalak&apos;s block
+<a href=\"modelica://AixLib.Utilities.Math.IntegerReplicator\">
+AixLib.Utilities.Math.IntegerReplicator</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end integerReplicator;
diff --git a/AixLib/Utilities/Math/Functions/interpolate.mo b/AixLib/Utilities/Math/Functions/interpolate.mo
new file mode 100644
index 0000000000..4b42265801
--- /dev/null
+++ b/AixLib/Utilities/Math/Functions/interpolate.mo
@@ -0,0 +1,96 @@
+within AixLib.Utilities.Math.Functions;
+function interpolate
+  "Function for cubic hermite spline interpolation of table data"
+  extends Modelica.Icons.Function;
+
+  input Real u "Independent variable";
+  input Real[:] xd "x-axis support points";
+  input Real[size(xd, 1)] yd "y-axis support points";
+  input Real[size(xd, 1)] d "Derivatives at the support points";
+
+  output Real z "Dependent variable with monotone interpolation";
+
+protected
+  Integer i "Integer to select data interval";
+
+algorithm
+  i := 1;
+  for j in 1:size(xd, 1) - 1 loop
+    if u > xd[j] then
+      i := j;
+    end if;
+  end for;
+
+  z :=AixLib.Utilities.Math.Functions.cubicHermiteLinearExtrapolation(
+      x=u,
+      x1=xd[i],
+      x2=xd[i + 1],
+      y1=yd[i],
+      y2=yd[i + 1],
+      y1d=d[i],
+      y2d=d[i + 1]);
+
+  annotation (smoothOrder = 1,
+    Documentation(info="<html>
+<p>
+This function returns the value on a cubic hermite spline through the given support points
+and provided spline derivatives at these points.
+The spline derivatives at the support points can be computed using
+<a href=\"modelica://AixLib.Utilities.Math.Functions.splineDerivatives\">
+AixLib.Utilities.Math.Functions.splineDerivatives</a>.
+The support points must be monotonically increasing.
+Outside the provided support points, the function returns a linear extrapolation with
+the same slope as the cubic spline has at the respective support point.
+</p>
+<p>
+A similar model is also used in the CONTAM software (Dols and Walton, 2015).
+</p>
+<p>
+This function is used in
+<a href=\"modelica://AixLib.Airflow.Multizone.Table_m_flow\">
+AixLib.Airflow.Multizone.Table_m_flow</a> and <a href=\"modelica://AixLib.Airflow.Multizone.Table_V_flow\">
+AixLib.Airflow.Multizone.Table_V_flow</a>
+</p>
+<h4>
+References
+</h4>
+<ul>
+<li>
+<b>W. S. Dols and B. J. Polidoro</b>,<b>2015</b>. <i>CONTAM User Guide and Program Documentation Version 3.2</i>,
+National Institute of Standards and Technology, NIST TN 1887, Sep. 2015. doi:
+<a href=\"https://doi.org/10.6028/NIST.TN.1887\">10.6028/NIST.TN.1887</a>.
+</li>
+</ul>
+</html>", revisions="<html>
+<ul>
+<li>
+February 29, 2024, by Hongxiang Fu:<br/>
+Moved to
+<a href=\"modelica://AixLib.Utilities.Math.Functions\">
+AixLib.Utilities.Math.Functions</a>
+from
+<a href=\"modelica://AixLib.Airflow.Multizone.BaseClasses\">
+AixLib.Airflow.Multizone.BaseClasses</a>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1844\">IBPSA, #1844</a>.
+</li>
+<li>
+February 26, 2024, by Hongxiang Fu:<br/>
+Correct implementation to make it smooth.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1840\">IBPSA, #1840</a>.
+</li>
+<li>
+February 2, 2022, by Michael Wetter:<br/>
+Revised implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1436\">IBPSA, #1436</a>.
+</li>
+<li>
+Apr 6, 2021, by Klaas De Jonge:<br/>
+First Implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end interpolate;
diff --git a/AixLib/Utilities/Math/Functions/inverseXRegularized.mo b/AixLib/Utilities/Math/Functions/inverseXRegularized.mo
index dbaab56259..8edd96884c 100644
--- a/AixLib/Utilities/Math/Functions/inverseXRegularized.mo
+++ b/AixLib/Utilities/Math/Functions/inverseXRegularized.mo
@@ -35,62 +35,62 @@ algorithm
           zeroDerivative=f)=AixLib.Utilities.Math.Functions.BaseClasses.der_inverseXRegularized,
               Inline=true,
 Documentation(info="<html>
- <p>
- Function that approximates <i>y=1 &frasl; x</i>
- inside the interval <i>-&delta; &le; x &le; &delta;</i>.
- The approximation is twice continuously differentiable with a bounded derivative on the whole
- real line.
- </p>
- <p>
- See the plot of
- <a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.InverseXRegularized\">
- AixLib.Utilities.Math.Functions.Examples.InverseXRegularized</a>
- for the graph.
- </p>
- <p>
- For efficiency, the polynomial coefficients
- <code>a, b, c, d, e, f</code> and
- the inverse of the smoothing parameter <code>deltaInv</code>
- are exposed as arguments to this function.
- Typically, these coefficients only depend on parameters and hence
- can be computed once.
- They must be equal to their default values, otherwise the function
- is not twice continuously differentiable.
- By exposing these coefficients as function arguments, models
- that call this function can compute them as parameters, and
- assign these parameter values in the function call.
- This avoids that the coefficients are evaluated for each time step,
- as they would otherwise be if they were to be computed inside the
- body of the function. However, assigning the values is optional
- as otherwise, at the expense of efficiency, the values will be
- computed each time the function is invoked.
- See
- <a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.InverseXRegularized\">
- AixLib.Utilities.Math.Functions.Examples.InverseXRegularized</a>
- for how to efficiently call this function.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 10, 2015, by Michael Wetter:<br/>
- Removed dublicate entry <code>smoothOrder = 1</code>
- and reimplmented the function so it is twice continuously differentiable.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/302\">issue 302</a>.
- </li>
- <li>
- February 5, 2015, by Filip Jorissen:<br/>
- Added <code>smoothOrder = 1</code>.
- </li>
- <li>
- May 10, 2013, by Michael Wetter:<br/>
- Reformulated implementation to avoid unrequired computations.
- </li>
- <li>
- April 18, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function that approximates <i>y=1 &frasl; x</i>
+inside the interval <i>-&delta; &le; x &le; &delta;</i>.
+The approximation is twice continuously differentiable with a bounded derivative on the whole
+real line.
+</p>
+<p>
+See the plot of
+<a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.InverseXRegularized\">
+AixLib.Utilities.Math.Functions.Examples.InverseXRegularized</a>
+for the graph.
+</p>
+<p>
+For efficiency, the polynomial coefficients
+<code>a, b, c, d, e, f</code> and
+the inverse of the smoothing parameter <code>deltaInv</code>
+are exposed as arguments to this function.
+Typically, these coefficients only depend on parameters and hence
+can be computed once.
+They must be equal to their default values, otherwise the function
+is not twice continuously differentiable.
+By exposing these coefficients as function arguments, models
+that call this function can compute them as parameters, and
+assign these parameter values in the function call.
+This avoids that the coefficients are evaluated for each time step,
+as they would otherwise be if they were to be computed inside the
+body of the function. However, assigning the values is optional
+as otherwise, at the expense of efficiency, the values will be
+computed each time the function is invoked.
+See
+<a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.InverseXRegularized\">
+AixLib.Utilities.Math.Functions.Examples.InverseXRegularized</a>
+for how to efficiently call this function.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 10, 2015, by Michael Wetter:<br/>
+Removed dublicate entry <code>smoothOrder = 1</code>
+and reimplmented the function so it is twice continuously differentiable.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/302\">issue 302</a>.
+</li>
+<li>
+February 5, 2015, by Filip Jorissen:<br/>
+Added <code>smoothOrder = 1</code>.
+</li>
+<li>
+May 10, 2013, by Michael Wetter:<br/>
+Reformulated implementation to avoid unrequired computations.
+</li>
+<li>
+April 18, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end inverseXRegularized;
diff --git a/AixLib/Utilities/Math/Functions/isMonotonic.mo b/AixLib/Utilities/Math/Functions/isMonotonic.mo
index 5e975cae6b..f67f51f22c 100644
--- a/AixLib/Utilities/Math/Functions/isMonotonic.mo
+++ b/AixLib/Utilities/Math/Functions/isMonotonic.mo
@@ -46,19 +46,19 @@ algorithm
   end if;
 
   annotation (Documentation(info="<html>
- <p>
- This function returns <code>true</code> if its argument is
- monotonic increasing or decreasing, and <code>false</code> otherwise.
- If <code>strict=true</code>, then strict monotonicity is tested,
- otherwise weak monotonicity is tested.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 28, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function returns <code>true</code> if its argument is
+monotonic increasing or decreasing, and <code>false</code> otherwise.
+If <code>strict=true</code>, then strict monotonicity is tested,
+otherwise weak monotonicity is tested.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 28, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end isMonotonic;
diff --git a/AixLib/Utilities/Math/Functions/package.order b/AixLib/Utilities/Math/Functions/package.order
index 9d0380b8d9..2dfeda1407 100644
--- a/AixLib/Utilities/Math/Functions/package.order
+++ b/AixLib/Utilities/Math/Functions/package.order
@@ -12,6 +12,7 @@ exponentialIntegralE1
 factorial
 fallingFactorial
 integerReplicator
+interpolate
 inverseXRegularized
 isMonotonic
 linearInterpolation
@@ -24,6 +25,7 @@ regStep
 round
 smoothExponential
 smoothHeaviside
+smoothInterpolation
 smoothLimit
 smoothMax
 smoothMin
diff --git a/AixLib/Utilities/Math/Functions/polynomial.mo b/AixLib/Utilities/Math/Functions/polynomial.mo
index bcfeaf4cba..4cca849d45 100644
--- a/AixLib/Utilities/Math/Functions/polynomial.mo
+++ b/AixLib/Utilities/Math/Functions/polynomial.mo
@@ -14,34 +14,34 @@ algorithm
   end for;
   y :=a*xp;
   annotation (Documentation(info="<html>
- This function computes a polynomial of arbitrary order.
- The polynomial has the form
- <p align=\"center\" style=\"font-style:italic;\">
-   y = a<sub>1</sub> + a<sub>2</sub> x + a<sub>3</sub> x<sup>2</sup> + ...
- </p>
- </html>",
+This function computes a polynomial of arbitrary order.
+The polynomial has the form
+<p align=\"center\" style=\"font-style:italic;\">
+  y = a<sub>1</sub> + a<sub>2</sub> x + a<sub>3</sub> x<sup>2</sup> + ...
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- December 14, 2016, by Michael Wetter:<br/>
- Removed derivative annotation.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/602\">issue 602</a>.
- </li>
- <li>
- March 30, 2011, by Michael Wetter:<br/>
- Added <code>zeroDerivative</code> keyword.
- </li>
- <li>
- March 2, by Michael Wetter:<br/>
- Removed redundant <code>smoothOrder</code> annotation.
- </li>
- <li>
- February 29, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-smoothOrder=999,
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+December 14, 2016, by Michael Wetter:<br/>
+Removed derivative annotation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/602\">issue 602</a>.
+</li>
+<li>
+March 30, 2011, by Michael Wetter:<br/>
+Added <code>zeroDerivative</code> keyword.
+</li>
+<li>
+March 2, by Michael Wetter:<br/>
+Removed redundant <code>smoothOrder</code> annotation.
+</li>
+<li>
+February 29, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+smoothOrder=999, 
+   __Dymola_LockedEditing="Model from IBPSA");
 end polynomial;
diff --git a/AixLib/Utilities/Math/Functions/powerLinearized.mo b/AixLib/Utilities/Math/Functions/powerLinearized.mo
index 98bf3a2b95..2f0fb7ec58 100644
--- a/AixLib/Utilities/Math/Functions/powerLinearized.mo
+++ b/AixLib/Utilities/Math/Functions/powerLinearized.mo
@@ -15,33 +15,33 @@ algorithm
   end if;
   annotation (
     Documentation(info="<html>
- Function that approximates <i>y=x<sup>n</sup></i>
- where <i>0 &lt; n</i> so that
- <ul>
- <li>the function is defined and monotone increasing for all <i>x</i>.</li>
- <li><i>dy/dx</i> is bounded and continuous everywhere (for <i>n &lt; 1</i>).</li>
- </ul>
- <p>
- For <i>x &lt; x<sub>0</sub></i>, this function replaces
- <i>y=x<sup>n</sup></i> by
- a linear function that is continuously differentiable everywhere.
- </p>
- <p>
- A typical use of this function is to replace
- <i>T = T4<sup>(1/4)</sup></i> in a radiation balance to ensure that the
- function is defined everywhere. This can help solving the initialization problem
- when a solver may be far from a solution and hence <i>T4 &lt; 0</i>.
- </p>
- <p>
- See the package <code>Examples</code> for the graph.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 3, 2011, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"), smoothOrder=1, Inline=true,
-  __Dymola_LockedEditing="Model from IBPSA");
+Function that approximates <i>y=x<sup>n</sup></i>
+where <i>0 &lt; n</i> so that
+<ul>
+<li>the function is defined and monotonically increasing for all <i>x</i>.</li>
+<li><i>dy/dx</i> is bounded and continuous everywhere (for <i>n &lt; 1</i>).</li>
+</ul>
+<p>
+For <i>x &lt; x<sub>0</sub></i>, this function replaces
+<i>y=x<sup>n</sup></i> by
+a linear function that is continuously differentiable everywhere.
+</p>
+<p>
+A typical use of this function is to replace
+<i>T = T4<sup>(1/4)</sup></i> in a radiation balance to ensure that the
+function is defined everywhere. This can help solving the initialization problem
+when a solver may be far from a solution and hence <i>T4 &lt; 0</i>.
+</p>
+<p>
+See the package <code>Examples</code> for the graph.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 3, 2011, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  smoothOrder=1, Inline=true, 
+   __Dymola_LockedEditing="Model from IBPSA");
 end powerLinearized;
diff --git a/AixLib/Utilities/Math/Functions/quadraticLinear.mo b/AixLib/Utilities/Math/Functions/quadraticLinear.mo
index d2d6703a91..88efdf3afd 100644
--- a/AixLib/Utilities/Math/Functions/quadraticLinear.mo
+++ b/AixLib/Utilities/Math/Functions/quadraticLinear.mo
@@ -13,20 +13,20 @@ algorithm
   y :=a[1] + a[2]*x1 + a[3]*x1Sq + (a[4] + a[5]*x1 + a[6]*x1Sq)*x2;
 
   annotation (smoothOrder=999, Documentation(info="<html>
- This function computes
- <p align=\"center\" style=\"font-style:italic;\">
-   y =   a<sub>1</sub> + a<sub>2</sub>  x<sub>1</sub>
-         + a<sub>3</sub> x<sub>1</sub><sup>2</sup>
-         + (a<sub>4</sub> + a<sub>5</sub>  x<sub>1</sub>
-         + a<sub>6</sub> x<sub>1</sub><sup>2</sup>)  x<sub>2</sub>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 29, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This function computes
+<p align=\"center\" style=\"font-style:italic;\">
+  y =   a<sub>1</sub> + a<sub>2</sub>  x<sub>1</sub>
+        + a<sub>3</sub> x<sub>1</sub><sup>2</sup>
+        + (a<sub>4</sub> + a<sub>5</sub>  x<sub>1</sub>
+        + a<sub>6</sub> x<sub>1</sub><sup>2</sup>)  x<sub>2</sub>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 29, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end quadraticLinear;
diff --git a/AixLib/Utilities/Math/Functions/quinticHermite.mo b/AixLib/Utilities/Math/Functions/quinticHermite.mo
index b35e9bce79..74a97c0a0e 100644
--- a/AixLib/Utilities/Math/Functions/quinticHermite.mo
+++ b/AixLib/Utilities/Math/Functions/quinticHermite.mo
@@ -31,22 +31,22 @@ algorithm
 
 annotation (smoothOrder=99,
 Documentation(revisions="<html>
- <ul>
- <li>
- April 19, 2017, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Returns the result y of a quintic Hermite spline,
- which is a C<sup>2</sup> continuous interpolation between two functions.
- The abscissa value <code>x</code> has to be between <code>x1</code> and <code>x2</code>.
- Variables <code>y1</code>, <code>y1d</code>, <code>y1dd</code> are the ordinate,
- ordinate derivative and ordinate second derivative of the function at <code>x1</code>.
- Variables <code>y2</code>, <code>y2d</code>, <code>y2dd</code> are respectively the ordinate,
- ordinate derivative and ordinate second derivative of the function at <code>x2</code>.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 19, 2017, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Returns the result y of a quintic Hermite spline,
+which is a C<sup>2</sup> continuous interpolation between two functions.
+The abscissa value <code>x</code> has to be between <code>x1</code> and <code>x2</code>.
+Variables <code>y1</code>, <code>y1d</code>, <code>y1dd</code> are the ordinate,
+ordinate derivative and ordinate second derivative of the function at <code>x1</code>.
+Variables <code>y2</code>, <code>y2d</code>, <code>y2dd</code> are respectively the ordinate,
+ordinate derivative and ordinate second derivative of the function at <code>x2</code>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end quinticHermite;
diff --git a/AixLib/Utilities/Math/Functions/regNonZeroPower.mo b/AixLib/Utilities/Math/Functions/regNonZeroPower.mo
index 8c8206b496..c2d42025fb 100644
--- a/AixLib/Utilities/Math/Functions/regNonZeroPower.mo
+++ b/AixLib/Utilities/Math/Functions/regNonZeroPower.mo
@@ -4,7 +4,9 @@ function regNonZeroPower
   extends Modelica.Icons.Function;
 
  input Real x "Abscissa value";
- input Real n "Exponent";
+ input Real n(
+   min=0.000001,
+   max=1.999999) "Exponent";
  input Real delta = 0.01 "Abscissa value where transition occurs";
  output Real y "Function value";
 protected
@@ -29,50 +31,58 @@ algorithm
    a3 := (yPP_d - 12 * a1 * delta2)/2;
    a5 := (y_d - delta2 * (a3 + delta2 * a1));
    y := a5 + x2 * (a3 + x2 * a1);
-   assert(a5>0, "Delta is too small for this exponent.");
+   assert(a5 > 0 and 0 < n and n < 2, "Delta is too small for this exponent or n is outside (0, 2).");
   end if;
   annotation (
     Documentation(info="<html>
- 
- Function that approximates <i>y=|x|<sup>n</sup></i> where <i>n &gt; 0</i>
- so that
- <ul>
- <li><i>y(0)</i> is not equal to zero.</li>
- <li><i>dy/dx</i> is bounded and continuous everywhere.</li>
- </ul>
- 
- <p>
- This function replaces <i>y=|x|<sup>n</sup></i> in the interval
- <i>-&delta;...+&delta;</i> by a 4-th order polynomial that has the same
- function value and the first and second derivative at <i>x=&plusmn; &delta;</i>.
- </p>
- <p>
- A typical use of this function is to replace the
- function for the convective heat transfer
- coefficient for forced or free convection that is of the form
- <i>h=c |dT|<sup>n</sup></i> for some constant <i>c</i> and exponent
- <i>0 &le; n &le; 1</i>.
- By using this function, the original function
- that has an infinite derivative near zero and that takes on zero
- at the origin is replaced by a function with a bounded derivative and
- a non-zero value at the origin. Physically,
- the region <i>-&delta;...+&delta;</i> may be interpreted as the region
- where heat conduction dominates convection in the boundary layer.
- </p>
- See the package <code>Examples</code> for the graph.
- </html>",revisions="<html>
- <ul>
- <li>
- March 30, 2011, by Michael Wetter:<br/>
- Added <code>zeroDerivative</code> keyword.
- </li>
- <li>
- April 14, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Inline=true,
+<p>
+Function that approximates <i>y=|x|<sup>n</sup></i> where <i>0 &lt; n &lt; 2</i>
+so that
+</p>
+<ul>
+<li><i>y(0)</i> is not equal to zero.</li>
+<li><i>dy/dx</i> is bounded and continuous everywhere.</li>
+</ul>
+<p>
+This function replaces <i>y=|x|<sup>n</sup></i> in the interval
+<i>-&delta;...+&delta;</i> by a 4-th order polynomial that has the same
+function value and the first and second derivative at <i>x=&plusmn; &delta;</i>.
+</p>
+<p>
+A typical use of this function is to replace the
+function for the convective heat transfer
+coefficient for forced or free convection that is of the form
+<i>h=c |dT|<sup>n</sup></i> for some constant <i>c</i> and exponent
+<i>0 &lt; n &le; 1</i>.
+By using this function, the original function
+that has an infinite derivative near zero and that takes on zero
+at the origin is replaced by a function with a bounded derivative and
+a non-zero value at the origin. Physically,
+the region <i>-&delta;...+&delta;</i> may be interpreted as the region
+where heat conduction dominates convection in the boundary layer.
+</p>
+<p>
+See the package <code>Examples</code> for the graph.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 2, 2022, by Michael Wetter:<br/>
+Set minimum and maximum attribute on <code>n</code>, improved assertion and documentation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3135\">Buildings, #3135</a>.
+</li>
+<li>
+March 30, 2011, by Michael Wetter:<br/>
+Added <code>zeroDerivative</code> keyword.
+</li>
+<li>
+April 14, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Inline=true,
            smoothOrder=2,
-           derivative(zeroDerivative=n, zeroDerivative=delta)=BaseClasses.der_regNonZeroPower,
-  __Dymola_LockedEditing="Model from IBPSA");
+           derivative(zeroDerivative=n, zeroDerivative=delta)=BaseClasses.der_regNonZeroPower, 
+   __Dymola_LockedEditing="Model from IBPSA");
 end regNonZeroPower;
diff --git a/AixLib/Utilities/Math/Functions/regStep.mo b/AixLib/Utilities/Math/Functions/regStep.mo
index 0e8145ae8e..4cc724cc49 100644
--- a/AixLib/Utilities/Math/Functions/regStep.mo
+++ b/AixLib/Utilities/Math/Functions/regStep.mo
@@ -15,39 +15,39 @@ algorithm
 
   annotation(Inline=true,
   Documentation(revisions="<html>
- <ul>
- <li><i>February 18, 2016</i>
-     by Marcus Fuchs:<br/>
-     Add function with <code>Inline = true</code> in annotations to package for better performance,
-     as suggested in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">#300</a> .</li>
- <li><i>April 29, 2008</i>
-     by <a href=\"mailto:Martin.Otter@DLR.de\">Martin Otter</a>:<br/>
-     Designed and implemented.</li>
- <li><i>August 12, 2008</i>
-     by <a href=\"mailto:Michael.Sielemann@dlr.de\">Michael Sielemann</a>:<br/>
-     Minor modification to cover the limit case <code>x_small -> 0</code> without division by zero.</li>
- </ul>
- </html>",info="<html>
- <p>
- This function is used to approximate the equation
- </p>
- <pre>
-     y = <b>if</b> x &gt; 0 <b>then</b> y1 <b>else</b> y2;
- </pre>
- 
- <p>
- by a smooth characteristic, so that the expression is continuous and differentiable:
- </p>
- 
- <pre>
-    y = <b>smooth</b>(1, <b>if</b> x &gt;  x_small <b>then</b> y1 <b>else</b>
-                  <b>if</b> x &lt; -x_small <b>then</b> y2 <b>else</b> f(y1, y2));
- </pre>
- 
- <p>
- In the region <code>-x_small &lt; x &lt; x_small</code> a 2nd order polynomial is used
- for a smooth transition from <code>y1</code> to <code>y2</code>.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li><i>February 18, 2016</i>
+    by Marcus Fuchs:<br/>
+    Add function with <code>Inline = true</code> in annotations to package for better performance,
+    as suggested in <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">#300</a> .</li>
+<li><i>August 12, 2008</i>
+    by <a href=\"mailto:Michael.Sielemann@dlr.de\">Michael Sielemann</a>:<br/>
+    Minor modification to cover the limit case <code>x_small -> 0</code> without division by zero.</li>
+<li><i>April 29, 2008</i>
+    by <a href=\"mailto:Martin.Otter@DLR.de\">Martin Otter</a>:<br/>
+    Designed and implemented.</li>
+</ul>
+</html>", info="<html>
+<p>
+This function is used to approximate the equation
+</p>
+<pre>
+    y = <b>if</b> x &gt; 0 <b>then</b> y1 <b>else</b> y2;
+</pre>
+
+<p>
+by a smooth characteristic, so that the expression is continuous and differentiable:
+</p>
+
+<pre>
+   y = <b>smooth</b>(1, <b>if</b> x &gt;  x_small <b>then</b> y1 <b>else</b>
+                 <b>if</b> x &lt; -x_small <b>then</b> y2 <b>else</b> f(y1, y2));
+</pre>
+
+<p>
+In the region <code>-x_small &lt; x &lt; x_small</code> a 2nd order polynomial is used
+for a smooth transition from <code>y1</code> to <code>y2</code>.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end regStep;
diff --git a/AixLib/Utilities/Math/Functions/smoothExponential.mo b/AixLib/Utilities/Math/Functions/smoothExponential.mo
index 8a7f376fc5..b3b287733e 100644
--- a/AixLib/Utilities/Math/Functions/smoothExponential.mo
+++ b/AixLib/Utilities/Math/Functions/smoothExponential.mo
@@ -26,21 +26,18 @@ algorithm
     y  := 1+x2*(a2+x2*a3);
   end if;
     annotation (smoothOrder=1, Documentation(info="<html>
- <p>
- Function to provide a once continuously differentiable approximation
- to <i>exp(- |x| )</i>
- in the interval <i>|x| &lt; &delta;</i> for some positive <i>&delta;</i>
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 30, 2008, by Michael Wetter:<br/>
- First implementation.
- Implemented to reduce chattering in
- <a href=\"modelica://AixLib.Fluid.Storage.BaseClasses.Stratifier\">
- AixLib.Fluid.Storage.BaseClasses.Stratifier</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function to provide a once continuously differentiable approximation
+to <i>exp(- |x| )</i>
+in the interval <i>|x| &lt; &delta;</i> for some positive <i>&delta;</i>
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 30, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end smoothExponential;
diff --git a/AixLib/Utilities/Math/Functions/smoothHeaviside.mo b/AixLib/Utilities/Math/Functions/smoothHeaviside.mo
index 1287183a3d..05ac1146b1 100644
--- a/AixLib/Utilities/Math/Functions/smoothHeaviside.mo
+++ b/AixLib/Utilities/Math/Functions/smoothHeaviside.mo
@@ -13,46 +13,46 @@ algorithm
 
  annotation (smoothOrder = 2,
  Documentation(info="<html>
- <p>
- Twice Lipschitz continuously differentiable approximation to the
- <code>Heaviside(.,.)</code> function.<br/>
- Function is derived from a quintic polynomial going through <i>(0,0)</i> and <i>(1,1)</i>,
- with zero first and second order derivatives at those points.<br/>
- See Example <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothHeaviside\">
- AixLib.Utilities.Math.Examples.SmoothHeaviside</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 21, 2019:<br/>
- Added <code>delta.min</code> attribute to guard against division by zero.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1202\">issue 1202</a>.
- </li>
- <li>
- September 13, 2019, by Kristoff Six and Filip Jorissen:<br/>
- Once continuously differentiable replaced by twice continuously differentiable implementation. This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1202\">issue 1202</a>.
- </li>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- July 17, 2015, by Marcus Fuchs:<br/>
- Add link to example.
- </li>
- <li>
- February 5, 2015, by Filip Jorissen:<br/>
- Added <code>smoothOrder = 1</code>.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo, Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Twice Lipschitz continuously differentiable approximation to the
+<code>Heaviside(.,.)</code> function.<br/>
+Function is derived from a quintic polynomial going through <i>(0,0)</i> and <i>(1,1)</i>,
+with zero first and second order derivatives at those points.<br/>
+See Example <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothHeaviside\">
+AixLib.Utilities.Math.Examples.SmoothHeaviside</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 21, 2019:<br/>
+Added <code>delta.min</code> attribute to guard against division by zero.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1202\">issue 1202</a>.
+</li>
+<li>
+September 13, 2019, by Kristoff Six and Filip Jorissen:<br/>
+Once continuously differentiable replaced by twice continuously differentiable implementation. This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1202\">issue 1202</a>.
+</li>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+July 17, 2015, by Marcus Fuchs:<br/>
+Add link to example.
+</li>
+<li>
+February 5, 2015, by Filip Jorissen:<br/>
+Added <code>smoothOrder = 1</code>.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo, Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end smoothHeaviside;
diff --git a/AixLib/Utilities/Math/Functions/smoothInterpolation.mo b/AixLib/Utilities/Math/Functions/smoothInterpolation.mo
new file mode 100644
index 0000000000..196b75bda2
--- /dev/null
+++ b/AixLib/Utilities/Math/Functions/smoothInterpolation.mo
@@ -0,0 +1,99 @@
+within AixLib.Utilities.Math.Functions;
+function smoothInterpolation
+  "Interpolate using a cubic Hermite spline with linear extrapolation for a vector xSup[], ySup[] and independent variable x"
+  extends Modelica.Icons.Function;
+  input Real x "Abscissa value";
+  input Real xSup[:] "Support points (strictly increasing)";
+  input Real ySup[size(xSup,1)] "Function values at xSup";
+  input Boolean ensureMonotonicity=isMonotonic(ySup, strict=false)
+    "Set to true to ensure monotonicity of the cubic hermite";
+  output Real yInt "Interpolated ordinate value";
+
+protected
+  Integer n = size(xSup,1) "Number of support points";
+  Real dy_dx[size(xSup,1)] "Derivative at xSup";
+  Integer i "Integer to select data interval";
+algorithm
+  if n > 2 then
+    // Most common case with more than 2 data points.
+    // Do cubic spline interpolation.
+    dy_dx :=AixLib.Utilities.Math.Functions.splineDerivatives(
+      x=xSup,
+      y=ySup,
+      ensureMonotonicity=ensureMonotonicity);
+
+    // i is a counter that is used to pick the derivative
+    // that corresponds to the interval that contains x
+    i := 1;
+    for j in 1:n-1 loop
+      if x > xSup[j] then
+        i := j;
+       end if;
+     end for;
+     assert(xSup[i] < xSup[i+1], "Support points xSup must be increasing.");
+     yInt:=cubicHermiteLinearExtrapolation(
+        x=x,
+        x1=xSup[i],
+        x2=xSup[i+1],
+        y1=ySup[i],
+        y2=ySup[i+1],
+        y1d=dy_dx[i],
+        y2d=dy_dx[i+1]);
+  elseif n == 2 then
+    // Linear interpolation.
+    yInt := ySup[1] + (x - xSup[1]) * (ySup[2] - ySup[1])/(xSup[2] - xSup[1]);
+  else // n == 1
+    yInt :=ySup[1];
+  end if;
+  annotation(smoothOrder=1,
+      Documentation(info="<html>
+<p>
+For <i>xSup<sub>1</sub> &le; x &le; xSup<sub>n</sub></i>,
+where <i>n</i> is the size of the support points <i>xSup</i>,
+which must be strictly monotonically increasing,
+this function interpolates
+using cubic hermite spline. For <i>x</i> outside this interval, the function
+linearly extrapolates.
+</p>
+<p>
+If <i>n=2</i>, linear interpolation is used an if <i>n=1</i>, the
+function value <i>y<sup>1</sup></i> is returned.
+</p>
+<p>
+Note that if <code>xSup</code> and <code>ySup</code> only depend on parameters
+or constants, and therefore will not change during the simulation,
+it is more efficient to first call
+<a href=\"modelica://AixLib.Utilities.Math.Functions.splineDerivatives\">
+AixLib.Utilities.Math.Functions.splineDerivatives</a>
+to find the derivatives, and then call
+<a href=\"modelica://AixLib.Utilities.Math.Functions.interpolate\">
+AixLib.Utilities.Math.Functions.interpolate</a> to perform the interpolation.
+This way the derivatives only need to be computed once upon initialisation,
+not at each step during the simulation.
+See the example implemented in
+<a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.Interpolate\">
+AixLib.Utilities.Math.Functions.Examples.Interpolate</a>.
+</p>
+<p>
+In contrast to the function
+<a href=\"modelica://Modelica.Math.Vectors.interpolate\">
+Modelica.Math.Vectors.interpolate</a>
+which provides linear interpolation, this function does
+not trigger events.
+</p>
+<p>
+For how to use this function, see
+<a href=\"modelica://AixLib.Utilities.Math.Functions.Examples.SmoothInterpolation\">
+AixLib.Utilities.Math.Functions.Examples.SmoothInterpolation</a>.
+</p>
+</html>",
+revisions="<html>
+<ul>
+<li>
+October 1, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
+end smoothInterpolation;
diff --git a/AixLib/Utilities/Math/Functions/smoothLimit.mo b/AixLib/Utilities/Math/Functions/smoothLimit.mo
index 2d49bf31dc..bf8a54b3b2 100644
--- a/AixLib/Utilities/Math/Functions/smoothLimit.mo
+++ b/AixLib/Utilities/Math/Functions/smoothLimit.mo
@@ -16,34 +16,34 @@ algorithm
   y := AixLib.Utilities.Math.Functions.smoothMin(y,u-deltaX,cor);
   annotation (smoothOrder = 1,
   Documentation(info="<html>
- <p>
- Once continuously differentiable approximation to the <code>limit(.,.)</code> function.
- The output is bounded to be in <i>[l, u]</i>.
- </p>
- <p>
- Note that the limit need not be respected, such as illustrated in
- <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
- AixLib.Utilities.Math.Examples.SmoothMin</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 12, 2015, by Filip Jorissen:<br/>
- Added documentation reference demonstrating overshoot.
- </li>
- <li>
- February 5, 2015, by Filip Jorissen:<br/>
- Added <code>smoothOrder = 1</code>.
- </li>
- <li>
- Sept 1, 2010, by Michael Wetter:<br/>
- Changed scaling to make sure that bounds are never violated.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo, Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Once continuously differentiable approximation to the <code>limit(.,.)</code> function.
+The output is bounded to be in <i>[l, u]</i>.
+</p>
+<p>
+Note that the limit need not be respected, such as illustrated in
+<a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
+AixLib.Utilities.Math.Examples.SmoothMin</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 12, 2015, by Filip Jorissen:<br/>
+Added documentation reference demonstrating overshoot.
+</li>
+<li>
+February 5, 2015, by Filip Jorissen:<br/>
+Added <code>smoothOrder = 1</code>.
+</li>
+<li>
+Sept 1, 2010, by Michael Wetter:<br/>
+Changed scaling to make sure that bounds are never violated.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo, Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end smoothLimit;
diff --git a/AixLib/Utilities/Math/Functions/smoothMax.mo b/AixLib/Utilities/Math/Functions/smoothMax.mo
index 62d48651ce..821095239c 100644
--- a/AixLib/Utilities/Math/Functions/smoothMax.mo
+++ b/AixLib/Utilities/Math/Functions/smoothMax.mo
@@ -13,36 +13,36 @@ algorithm
   Inline=true,
   smoothOrder=1,
 Documentation(info="<html>
- <p>
- Once continuously differentiable approximation to the <code>max(.,.)</code> function.
- </p>
- <p>
- Note that the maximum need not be respected, such as illustrated in
- <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
- AixLib.Utilities.Math.Examples.SmoothMin</a>.
- </p>
- </html>",
+<p>
+Once continuously differentiable approximation to the <code>max(.,.)</code> function.
+</p>
+<p>
+Note that the maximum need not be respected, such as illustrated in
+<a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
+AixLib.Utilities.Math.Examples.SmoothMin</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- March 12, 2015, by Filip Jorissen:<br/>
- Added documentation reference demonstrating overshoot.
- </li>
- <li>
- February 5, 2015, by Filip Jorissen:<br/>
- Added <code>smoothOrder = 1</code>.
- </li>
- <li>
- August 15, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+March 12, 2015, by Filip Jorissen:<br/>
+Added documentation reference demonstrating overshoot.
+</li>
+<li>
+February 5, 2015, by Filip Jorissen:<br/>
+Added <code>smoothOrder = 1</code>.
+</li>
+<li>
+August 15, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end smoothMax;
diff --git a/AixLib/Utilities/Math/Functions/smoothMin.mo b/AixLib/Utilities/Math/Functions/smoothMin.mo
index d7f8d141a7..5cc02554ae 100644
--- a/AixLib/Utilities/Math/Functions/smoothMin.mo
+++ b/AixLib/Utilities/Math/Functions/smoothMin.mo
@@ -13,36 +13,36 @@ algorithm
   Inline=true,
   smoothOrder=1,
 Documentation(info="<html>
- <p>
- Once continuously differentiable approximation to the <code>min(.,.)</code> function.
- </p>
- <p>
- Note that the minimum need not be respected, such as illustrated in
- <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
- AixLib.Utilities.Math.Examples.SmoothMin</a>.
- </p>
- </html>",
+<p>
+Once continuously differentiable approximation to the <code>min(.,.)</code> function.
+</p>
+<p>
+Note that the minimum need not be respected, such as illustrated in
+<a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
+AixLib.Utilities.Math.Examples.SmoothMin</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- March 12, 2015, by Filip Jorissen:<br/>
- Added documentation reference demonstrating overshoot.
- </li>
- <li>
- February 5, 2015, by Filip Jorissen:<br/>
- Added <code>smoothOrder = 1</code>.
- </li>
- <li>
- August 15, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+March 12, 2015, by Filip Jorissen:<br/>
+Added documentation reference demonstrating overshoot.
+</li>
+<li>
+February 5, 2015, by Filip Jorissen:<br/>
+Added <code>smoothOrder = 1</code>.
+</li>
+<li>
+August 15, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end smoothMin;
diff --git a/AixLib/Utilities/Math/Functions/spliceFunction.mo b/AixLib/Utilities/Math/Functions/spliceFunction.mo
index 81fd9fc050..c772e99b87 100644
--- a/AixLib/Utilities/Math/Functions/spliceFunction.mo
+++ b/AixLib/Utilities/Math/Functions/spliceFunction.mo
@@ -7,14 +7,15 @@ function spliceFunction
     input Real deltax "Half width of transition interval";
     output Real out "Smoothed value";
 protected
+    constant Real lim = 0.9999999999;
     Real scaledX1;
     Real y;
     constant Real asin1 = Modelica.Math.asin(1);
 algorithm
     scaledX1 := x/deltax;
-    if scaledX1 <= -0.999999999 then
+    if scaledX1 <= -lim then
       out := neg;
-    elseif scaledX1 >= 0.999999999 then
+    elseif scaledX1 >= lim then
       out := pos;
     else
       y := (Modelica.Math.tanh(Modelica.Math.tan(scaledX1*asin1)) + 1)/2;
@@ -25,30 +26,35 @@ algorithm
 smoothOrder=3,
 derivative=BaseClasses.der_spliceFunction,
 Documentation(info="<html>
- <p>
- Function to provide a once continuously differentiable transition between
- to arguments.
- </p><p>
- The function is adapted from
- <a href=\"modelica://Modelica.Media.Air.MoistAir.Utilities.spliceFunction\">
- Modelica.Media.Air.MoistAir.Utilities.spliceFunction</a> and provided here
- for easier accessability to model developers.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 10, 2013, by Michael Wetter:<br/>
- Reformulated implementation to avoid unrequired computations.
- </li>
- <li>
- May 11, 2010, by Michael Wetter:<br/>
- Removed default value for transition interval as this is problem dependent.
- </li>
- <li>
- May 20, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function to provide a once continuously differentiable transition between
+to arguments.
+</p><p>
+The function is adapted from
+<a href=\"modelica://Modelica.Media.Air.MoistAir.Utilities.spliceFunction\">
+Modelica.Media.Air.MoistAir.Utilities.spliceFunction</a> and provided here
+for easier accessability to model developers.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 27, 2022, by Matthis Thorade:<br/>
+Changed limits.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/pull/1640\">IBPSA, issue #1640</a>.
+</li>
+<li>
+May 10, 2013, by Michael Wetter:<br/>
+Reformulated implementation to avoid unrequired computations.
+</li>
+<li>
+May 11, 2010, by Michael Wetter:<br/>
+Removed default value for transition interval as this is problem dependent.
+</li>
+<li>
+May 20, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end spliceFunction;
diff --git a/AixLib/Utilities/Math/Functions/splineDerivatives.mo b/AixLib/Utilities/Math/Functions/splineDerivatives.mo
index 4257761d17..bd66c7f414 100644
--- a/AixLib/Utilities/Math/Functions/splineDerivatives.mo
+++ b/AixLib/Utilities/Math/Functions/splineDerivatives.mo
@@ -2,7 +2,7 @@ within AixLib.Utilities.Math.Functions;
 function splineDerivatives
   "Function to compute the derivatives for cubic hermite spline interpolation"
   extends Modelica.Icons.Function;
-  input Real x[:] "Support point, strict monotone increasing";
+  input Real x[:] "Support point, strictly increasing";
   input Real y[size(x, 1)] "Function values at x";
   input Boolean ensureMonotonicity=isMonotonic(y, strict=false)
     "Set to true to ensure monotonicity of the cubic hermite";
@@ -17,14 +17,14 @@ protected
 algorithm
   if (n>1) then
     assert(x[1] < x[n], "x must be strictly increasing.
-   Received x[1] = "+ String(x[1]) + "
-            x["+ String(n) + "] = " + String(x[n]));
+  Received x[1] = " + String(x[1]) + "
+           x[" + String(n) + "] = " + String(x[n]));
   // Check data
     assert(isMonotonic(x, strict=true),
-      "x-values must be strictly monontone increasing or decreasing.");
+      "x-values must be strictly increasing or decreasing.");
     if ensureMonotonicity then
       assert(isMonotonic(y, strict=false),
-        "If ensureMonotonicity=true, y-values must be monontone increasing or decreasing.");
+        "If ensureMonotonicity=true, y-values must be strictly increasing or decreasing.");
     end if;
   end if;
 
@@ -70,47 +70,47 @@ algorithm
     end for;
   end if;
   annotation (Documentation(info="<html>
- <p>
- This function computes the derivatives at the support points <i>x<sub>i</sub></i>
- that can be used as input for evaluating a cubic hermite spline.
- </p>
- <p>
- If <code>ensureMonotonicity=true</code>, then the support points <i>y<sub>i</sub></i>
- need to be monotone increasing (or increasing), and the computed derivatives
- <i>d<sub>i</sub></i> are such that the cubic hermite is monotone increasing (or decreasing).
- The algorithm to ensure monotonicity is based on the method described in Fritsch and Carlson (1980) for
- <i>&rho; = &rho;<sub>2</sub></i>.
- </p>
- <p>
- This function is typically used with
- <a href=\"modelica://AixLib.Utilities.Math.Functions.cubicHermiteLinearExtrapolation\">
- AixLib.Utilities.Math.Functions.cubicHermiteLinearExtrapolation</a>
- which is used to evaluate the cubic spline.
- Because in many applications, the shape of the spline depends on parameters,
- this function has been implemented in such a way that all derivatives can be
- computed at once and then stored for use during the time stepping,
- in which the above function may be called.
- </p>
- <h4>References</h4>
- <p>
- F.N. Fritsch and R.E. Carlson, <a href=\"http://dx.doi.org/10.1137/0717021\">Monotone piecewise cubic interpolation</a>.
- <i>SIAM J. Numer. Anal.</i>, 17 (1980), pp. 238-246.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 26, 2016 by Michael Wetter:<br/>
- Corrected documentation.
- </li>
- <li>
- September 29, 2011 by Michael Wetter:<br/>
- Added special case for one data point and two data points.
- </li>
- <li>
- September 27, 2011 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function computes the derivatives at the support points <i>x<sub>i</sub></i>
+that can be used as input for evaluating a cubic hermite spline.
+</p>
+<p>
+If <code>ensureMonotonicity=true</code>, then the support points <i>y<sub>i</sub></i>
+need to be monotone increasing (or decreasing), and the computed derivatives
+<i>d<sub>i</sub></i> are such that the cubic hermite is monotone increasing (or decreasing).
+The algorithm to ensure monotonicity is based on the method described in Fritsch and Carlson (1980) for
+<i>&rho; = &rho;<sub>2</sub></i>.
+</p>
+<p>
+This function is typically used with
+<a href=\"modelica://AixLib.Utilities.Math.Functions.interpolate\">
+AixLib.Utilities.Math.Functions.interpolate</a>
+which is used to evaluate the cubic spline.
+Because in many applications, the shape of the spline depends on parameters
+which will no longer change once the initialisation is complete,
+this function computes and returns the derivatives so that they can be stored by the calling
+model to avoid repetitive computations.
+</p>
+<h4>References</h4>
+<p>
+F.N. Fritsch and R.E. Carlson, <a href=\"http://dx.doi.org/10.1137/0717021\">Monotone piecewise cubic interpolation</a>.
+<i>SIAM J. Numer. Anal.</i>, 17 (1980), pp. 238-246.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 26, 2016 by Michael Wetter:<br/>
+Corrected documentation.
+</li>
+<li>
+September 29, 2011 by Michael Wetter:<br/>
+Added special case for one data point and two data points.
+</li>
+<li>
+September 27, 2011 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end splineDerivatives;
diff --git a/AixLib/Utilities/Math/Functions/trapezoidalIntegration.mo b/AixLib/Utilities/Math/Functions/trapezoidalIntegration.mo
index 17c79209f7..476889c6a5 100644
--- a/AixLib/Utilities/Math/Functions/trapezoidalIntegration.mo
+++ b/AixLib/Utilities/Math/Functions/trapezoidalIntegration.mo
@@ -16,16 +16,16 @@ algorithm
   result := result - f[1] - f[N];
   result := result*deltaX/2;
   annotation (Documentation(info="<html>
- <p>
- This function computes a definite integral using the trapezoidal rule.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 23, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This function computes a definite integral using the trapezoidal rule.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 23, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end trapezoidalIntegration;
diff --git a/AixLib/Utilities/Math/IntegerReplicator.mo b/AixLib/Utilities/Math/IntegerReplicator.mo
index 7fa62bd316..55387ce237 100644
--- a/AixLib/Utilities/Math/IntegerReplicator.mo
+++ b/AixLib/Utilities/Math/IntegerReplicator.mo
@@ -25,15 +25,15 @@ equation
           fillColor={255,128,0},
           fillPattern=FillPattern.Solid)}),
     Documentation(info="<html>
- <p>
- This block replicates the integer input signal to an array of <code>nout</code> identical output signals.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>November 28, 2013, by Marcus Fuchs:<br/>Changed block to use Functions.integerReplicator. </li>
- <li>August 31, 2012, by Michael Wetter:<br/>Revised documentation. </li>
- <li>July 27, 2012, by Kaustubh Phalak:<br/>First implementation. </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This block replicates the integer input signal to an array of <code>nout</code> identical output signals.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>November 28, 2013, by Marcus Fuchs:<br/>Changed block to use Functions.integerReplicator. </li>
+<li>August 31, 2012, by Michael Wetter:<br/>Revised documentation. </li>
+<li>July 27, 2012, by Kaustubh Phalak:<br/>First implementation. </li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end IntegerReplicator;
diff --git a/AixLib/Utilities/Math/IntegratorWithReset.mo b/AixLib/Utilities/Math/IntegratorWithReset.mo
index ea54ac444f..6e6be00b88 100644
--- a/AixLib/Utilities/Math/IntegratorWithReset.mo
+++ b/AixLib/Utilities/Math/IntegratorWithReset.mo
@@ -5,8 +5,8 @@ block IntegratorWithReset "Output the integral of the input signal"
   parameter Real k(unit="1")=1 "Integrator gain";
 
   /* InitialState is the default, because it was the default in Modelica 2.2
-      and therefore this setting is backward compatible
-   */
+     and therefore this setting is backward compatible
+  */
   parameter Modelica.Blocks.Types.Init initType=Modelica.Blocks.Types.Init.InitialState
     "Type of initialization (1: no init, 2: steady state, 3,4: initial output)"
     annotation(Evaluate=true,
@@ -76,76 +76,76 @@ equation
   annotation (
 defaultComponentName="intWitRes",
     Documentation(info="<html>
- <p>
- This model is similar to
- <a href=\"modelica://Modelica.Blocks.Continuous.Integrator\">
- Modelica.Blocks.Continuous.Integrator</a>
- except that it optionally allows to reset the output <code>y</code>
- of the integrator.
- </p>
- <p>
- The output of the integrator can be reset as follows:
- </p>
- <ul>
- <li>
- If <code>reset = AixLib.Types.Reset.Disabled</code>, which is the default,
- then the integrator is never reset.
- </li>
- <li>
- If <code>reset = AixLib.Types.Reset.Parameter</code>, then a boolean
- input signal <code>trigger</code> is enabled. Whenever the value of
- this input changes from <code>false</code> to <code>true</code>,
- the integrator is reset by setting <code>y</code>
- to the value of the parameter <code>y_reset</code>.
- </li>
- <li>
- If <code>reset = AixLib.Types.Reset.Input</code>, then a boolean
- input signal <code>trigger</code> is enabled. Whenever the value of
- this input changes from <code>false</code> to <code>true</code>,
- the integrator is reset by setting <code>y</code>
- to the value of the input signal <code>y_reset_in</code>.
- </li>
- </ul>
- <p>
- See <a href=\"modelica://AixLib.Utilities.Math.Examples.IntegratorWithReset\">
- AixLib.Utilities.Math.Examples.IntegratorWithReset</a> for an example.
- </p>
- <h4>Implementation</h4>
- <p>
- To adjust the icon layer, the code of
- <a href=\"modelica://Modelica.Blocks.Continuous.Integrator\">
- Modelica.Blocks.Continuous.Integrator</a>
- has been copied into this model rather than extended.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 1, 2016, by Michael Wetter:<br/>
- Corrected wrong annotation for <code>y_reset</code>,
- and made rendering of <code>y_reset_in</code> conditional.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/562\">#562</a>.
- </li>
- <li>
- September 29, 2016, by Michael Wetter:<br/>
- Refactored model to use a <code>type</code> for configuration
- of the integrator reset.
- </li>
- <li>
- August 9, 2016, by Michael Wetter:<br/>
- Reformulated model using a conditional connector to use the same
- design pattern as is used in other models.
- </li>
- <li>
- August 9, 2016, by Michael Wetter:<br/>
- Revised model.
- </li>
- <li>
- July 18, 2016, by Philipp Mehrfeld:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model is similar to
+<a href=\"modelica://Modelica.Blocks.Continuous.Integrator\">
+Modelica.Blocks.Continuous.Integrator</a>
+except that it optionally allows to reset the output <code>y</code>
+of the integrator.
+</p>
+<p>
+The output of the integrator can be reset as follows:
+</p>
+<ul>
+<li>
+If <code>reset = AixLib.Types.Reset.Disabled</code>, which is the default,
+then the integrator is never reset.
+</li>
+<li>
+If <code>reset = AixLib.Types.Reset.Parameter</code>, then a boolean
+input signal <code>trigger</code> is enabled. Whenever the value of
+this input changes from <code>false</code> to <code>true</code>,
+the integrator is reset by setting <code>y</code>
+to the value of the parameter <code>y_reset</code>.
+</li>
+<li>
+If <code>reset = AixLib.Types.Reset.Input</code>, then a boolean
+input signal <code>trigger</code> is enabled. Whenever the value of
+this input changes from <code>false</code> to <code>true</code>,
+the integrator is reset by setting <code>y</code>
+to the value of the input signal <code>y_reset_in</code>.
+</li>
+</ul>
+<p>
+See <a href=\"modelica://AixLib.Utilities.Math.Examples.IntegratorWithReset\">
+AixLib.Utilities.Math.Examples.IntegratorWithReset</a> for an example.
+</p>
+<h4>Implementation</h4>
+<p>
+To adjust the icon layer, the code of
+<a href=\"modelica://Modelica.Blocks.Continuous.Integrator\">
+Modelica.Blocks.Continuous.Integrator</a>
+has been copied into this model rather than extended.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 1, 2016, by Michael Wetter:<br/>
+Corrected wrong annotation for <code>y_reset</code>,
+and made rendering of <code>y_reset_in</code> conditional.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/562\">#562</a>.
+</li>
+<li>
+September 29, 2016, by Michael Wetter:<br/>
+Refactored model to use a <code>type</code> for configuration
+of the integrator reset.
+</li>
+<li>
+August 9, 2016, by Michael Wetter:<br/>
+Reformulated model using a conditional connector to use the same
+design pattern as is used in other models.
+</li>
+<li>
+August 9, 2016, by Michael Wetter:<br/>
+Revised model.
+</li>
+<li>
+July 18, 2016, by Philipp Mehrfeld:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
 Icon(coordinateSystem(
           preserveAspectRatio=true,
           extent={{-100.0,-100.0},{100.0,100.0}}),
@@ -172,6 +172,6 @@ Icon(coordinateSystem(
             extent={{70,-14},{370,26}},
           textColor={0,0,0},
           horizontalAlignment=TextAlignment.Left,
-          textString="y")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="y")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end IntegratorWithReset;
diff --git a/AixLib/Utilities/Math/Interpolate.mo b/AixLib/Utilities/Math/Interpolate.mo
new file mode 100644
index 0000000000..82f4914d7b
--- /dev/null
+++ b/AixLib/Utilities/Math/Interpolate.mo
@@ -0,0 +1,52 @@
+within AixLib.Utilities.Math;
+block Interpolate
+  "Output the cubic hermite spline interpolation of the input signal on the given curve"
+  extends Modelica.Blocks.Interfaces.SISO;
+
+  parameter Real[:] xd "x-axis support points";
+  parameter Real[size(xd, 1)] yd "y-axis support points";
+  parameter Real[size(xd, 1)] d "Derivatives at the support points";
+equation
+  y = AixLib.Utilities.Math.Functions.interpolate(u=u, xd=xd, yd=yd, d=d);
+
+annotation (
+defaultComponentName="int",
+    Documentation(info="<html>
+<p>
+This block outputs the value on a cubic hermite spline through the given
+support points and their spline derivatives at these points, using the function
+<a href=\"modelica://AixLib.Utilities.Math.Functions.interpolate\">
+AixLib.Utilities.Math.Functions.interpolate</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 29, 2024, by Hongxiang Fu:<br/>
+First implementation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1844\">IBPSA, #1844</a>.
+</li>
+</ul>
+</html>"),
+    Icon(graphics={
+        Ellipse(
+          extent={{-58,-56},{-68,-46}},
+          lineColor={28,108,200},
+          fillColor={28,108,200},
+          fillPattern=FillPattern.Solid),
+        Line(
+          points={{-64,-52},{-36,6},{8,40},{78,26}},
+          color={28,108,200},
+          smooth=Smooth.Bezier),
+        Ellipse(
+          extent={{82,20},{72,30}},
+          lineColor={28,108,200},
+          fillColor={28,108,200},
+          fillPattern=FillPattern.Solid),
+        Ellipse(
+          extent={{-10,18},{-20,28}},
+          lineColor={28,108,200},
+          fillColor={28,108,200},
+          fillPattern=FillPattern.Solid)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
+end Interpolate;
diff --git a/AixLib/Utilities/Math/InverseXRegularized.mo b/AixLib/Utilities/Math/InverseXRegularized.mo
index 8f61365413..d3a5155030 100644
--- a/AixLib/Utilities/Math/InverseXRegularized.mo
+++ b/AixLib/Utilities/Math/InverseXRegularized.mo
@@ -6,18 +6,18 @@ block InverseXRegularized
 equation
   y = AixLib.Utilities.Math.Functions.inverseXRegularized(x=u, delta=delta);
   annotation (Documentation(info="<html>
- <p>Function that approximates <i>y=1 &frasl; x</i> inside the interval <i>-&delta; &le; x &le; &delta;</i>. The approximation is twice continuously differentiable with a bounded derivative on the whole real line. </p>
- <p>See the package <code>Examples</code> for the graph. </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 29, 2013, by Marcus Fuchs:<br/>
- Implementation based on Functions.inverseXRegularized.
- </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+<p>Function that approximates <i>y=1 &frasl; x</i> inside the interval <i>-&delta; &le; x &le; &delta;</i>. The approximation is twice continuously differentiable with a bounded derivative on the whole real line. </p>
+<p>See the package <code>Examples</code> for the graph. </p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 29, 2013, by Marcus Fuchs:<br/>
+Implementation based on Functions.inverseXRegularized.
+</li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-90,36},{90,-36}},
           textColor={160,160,164},
-          textString="inverseXRegularized()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="inverseXRegularized()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end InverseXRegularized;
diff --git a/AixLib/Utilities/Math/Max.mo b/AixLib/Utilities/Math/Max.mo
index a6e7d7ec04..216e812971 100644
--- a/AixLib/Utilities/Math/Max.mo
+++ b/AixLib/Utilities/Math/Max.mo
@@ -5,20 +5,20 @@ equation
  y = max(u);
 annotation (defaultComponentName="max",
 Documentation(info="<html>
- <p>
- Outputs the maximum of the vector.
- </p>
- </html>",
+<p>
+Outputs the maximum of the vector.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 3, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={Text(
+<ul>
+<li>
+April 3, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={Text(
           extent={{-74,90},{70,-70}},
           textColor={0,0,255},
-          textString="max")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="max")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Max;
diff --git a/AixLib/Utilities/Math/Min.mo b/AixLib/Utilities/Math/Min.mo
index ad812d69d0..ab741f2118 100644
--- a/AixLib/Utilities/Math/Min.mo
+++ b/AixLib/Utilities/Math/Min.mo
@@ -6,20 +6,20 @@ equation
 annotation (
 defaultComponentName="min",
 Documentation(info="<html>
- <p>
- Outputs the minimum of the vector.
- </p>
- </html>",
+<p>
+Outputs the minimum of the vector.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 3, 2009, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={Text(
+<ul>
+<li>
+April 3, 2009, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={Text(
           extent={{-72,88},{72,-72}},
           textColor={0,0,255},
-          textString="min")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="min")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Min;
diff --git a/AixLib/Utilities/Math/Polynomial.mo b/AixLib/Utilities/Math/Polynomial.mo
index df1ebc60d1..cea0f1c652 100644
--- a/AixLib/Utilities/Math/Polynomial.mo
+++ b/AixLib/Utilities/Math/Polynomial.mo
@@ -5,24 +5,24 @@ block Polynomial "Polynominal function"
 equation
   y = AixLib.Utilities.Math.Functions.polynomial(a=a, x=u);
   annotation (Documentation(info="<html>
- <p>This block computes a polynomial of arbitrary order. The polynomial has the form </p>
- <p align=\"center\"><i>y = a1 + a2 x + a3 x2 + ... </i></p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 21, 2021, by Michael Wetter:<br/>
- Renamed class to correct typo in class name.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1524\">IBPSA, #1524</a>.
- </li>
- <li>
- November 28, 2013, by Marcus Fuchs:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+<p>This block computes a polynomial of arbitrary order. The polynomial has the form </p>
+<p align=\"center\"><i>y = a1 + a2 x + a3 x2 + ... </i></p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 21, 2021, by Michael Wetter:<br/>
+Renamed class to correct typo in class name.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1524\">IBPSA, #1524</a>.
+</li>
+<li>
+November 28, 2013, by Marcus Fuchs:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-90,38},{90,-34}},
           textColor={160,160,164},
-          textString="polynominal()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="polynominal()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Polynomial;
diff --git a/AixLib/Utilities/Math/PowerLinearized.mo b/AixLib/Utilities/Math/PowerLinearized.mo
index 17e0c2aa36..2712e77b71 100644
--- a/AixLib/Utilities/Math/PowerLinearized.mo
+++ b/AixLib/Utilities/Math/PowerLinearized.mo
@@ -12,33 +12,33 @@ equation
           extent={{-90,36},{90,-36}},
           textColor={160,160,164},
           textString="powerLinearized()")}), Documentation(info="<html>
- Function that approximates <i>y=x<sup>n</sup></i>
- where <i>0 &lt; n</i> so that
- <ul>
- <li>the function is defined and monotone increasing for all <i>x</i>.</li>
- <li><i>dy/dx</i> is bounded and continuous everywhere (for <i>n &lt; 1</i>).</li>
- </ul>
- <p>
- For <i>x &lt; x<sub>0</sub></i>, this function replaces
- <i>y=x<sup>n</sup></i> by
- a linear function that is continuously differentiable everywhere.
- </p>
- <p>
- A typical use of this function is to replace
- <i>T = T4<sup>(1/4)</sup></i> in a radiation balance to ensure that the
- function is defined everywhere. This can help solving the initialization problem
- when a solver may be far from a solution and hence <i>T4 &lt; 0</i>.
- </p>
- <p>
- See the package <code>Examples</code> for the graph.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 29, 2013, by Marcus Fuchs:<br/>
- Implementation based on Functions.powerLinearized.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+Function that approximates <i>y=x<sup>n</sup></i>
+where <i>0 &lt; n</i> so that
+<ul>
+<li>the function is defined and monotonically increasing for all <i>x</i>.</li>
+<li><i>dy/dx</i> is bounded and continuous everywhere (for <i>n &lt; 1</i>).</li>
+</ul>
+<p>
+For <i>x &lt; x<sub>0</sub></i>, this function replaces
+<i>y=x<sup>n</sup></i> by
+a linear function that is continuously differentiable everywhere.
+</p>
+<p>
+A typical use of this function is to replace
+<i>T = T4<sup>(1/4)</sup></i> in a radiation balance to ensure that the
+function is defined everywhere. This can help solving the initialization problem
+when a solver may be far from a solution and hence <i>T4 &lt; 0</i>.
+</p>
+<p>
+See the package <code>Examples</code> for the graph.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 29, 2013, by Marcus Fuchs:<br/>
+Implementation based on Functions.powerLinearized.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end PowerLinearized;
diff --git a/AixLib/Utilities/Math/QuadraticLinear.mo b/AixLib/Utilities/Math/QuadraticLinear.mo
index be4a72cc54..a542623f74 100644
--- a/AixLib/Utilities/Math/QuadraticLinear.mo
+++ b/AixLib/Utilities/Math/QuadraticLinear.mo
@@ -6,18 +6,18 @@ block QuadraticLinear
 equation
   y = AixLib.Utilities.Math.Functions.quadraticLinear(a=a, x1=u1, x2=u2);
   annotation (Documentation(info="<html>
- <p>Block for function quadraticLinear, which computes </p>
- <p align=\"center\"><i>y = a1 + a2 x1 + a3 x12 + (a4 + a5 x1 + a6 x12) x2 </i></p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 29, 2013 by Marcus Fuchs:<br/>
- Implementation based on Functions.quadraticLinear.
- </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+<p>Block for function quadraticLinear, which computes </p>
+<p align=\"center\"><i>y = a1 + a2 x1 + a3 x12 + (a4 + a5 x1 + a6 x12) x2 </i></p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 29, 2013 by Marcus Fuchs:<br/>
+Implementation based on Functions.quadraticLinear.
+</li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-86,38},{94,-34}},
           textColor={160,160,164},
-          textString="quadraticLinear()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="quadraticLinear()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end QuadraticLinear;
diff --git a/AixLib/Utilities/Math/RegNonZeroPower.mo b/AixLib/Utilities/Math/RegNonZeroPower.mo
index ba6ace23d9..77e3a769f5 100644
--- a/AixLib/Utilities/Math/RegNonZeroPower.mo
+++ b/AixLib/Utilities/Math/RegNonZeroPower.mo
@@ -7,43 +7,53 @@ block RegNonZeroPower
 equation
   y = AixLib.Utilities.Math.Functions.regNonZeroPower(x=u, n=n, delta=delta);
   annotation (Documentation(info="<html>
- 
- Function that approximates <i>y=|x|<sup>n</sup></i> where <i>n &gt; 0</i>
- so that
- <ul>
- <li><i>y(0)</i> is not equal to zero.</li>
- <li><i>dy/dx</i> is bounded and continuous everywhere.</li>
- </ul>
- 
- <p>
- This function replaces <i>y=|x|<sup>n</sup></i> in the interval
- <i>-&delta;...+&delta;</i> by a 4-th order polynomial that has the same
- function value and the first and second derivative at <i>x=&plusmn; &delta;</i>.
- </p>
- <p>
- A typical use of this function is to replace the
- function for the convective heat transfer
- coefficient for forced or free convection that is of the form
- <i>h=c |dT|<sup>n</sup></i> for some constant <i>c</i> and exponent
- <i>0 &le; n &le; 1</i>.
- By using this function, the original function
- that has an infinite derivative near zero and that takes on zero
- at the origin is replaced by a function with a bounded derivative and
- a non-zero value at the origin. Physically,
- the region <i>-&delta;...+&delta;</i> may be interpreted as the region
- where heat conduction dominates convection in the boundary layer.
- </p>
- See the package <code>Examples</code> for the graph.
- </html>",revisions="<html>
- <ul>
- <li>
- November 29, 2013 by Marcus Fuchs:<br/>
- Implementation based on Functions.regNonZeroPower.
- </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+<p>
+Block that approximates <i>y=|x|<sup>n</sup></i> where <i>0 &lt; n &lt; 2</i>
+so that
+</p>
+<ul>
+<li><i>y(0)</i> is not equal to zero.</li>
+<li><i>dy/dx</i> is bounded and continuous everywhere.</li>
+</ul>
+<p>
+This block replaces <i>y=|x|<sup>n</sup></i> in the interval
+<i>-&delta;...+&delta;</i> by a 4-th order polynomial that has the same
+function value and the first and second derivative at <i>x=&plusmn; &delta;</i>.
+</p>
+<p>
+A typical use of this block is to replace the
+function for the convective heat transfer
+coefficient for forced or free convection that is of the form
+<i>h=c |dT|<sup>n</sup></i> for some constant <i>c</i> and exponent
+<i>0 &lt; n &le; 1</i>.
+By using this block, the original function
+that has an infinite derivative near zero and that takes on zero
+at the origin is replaced by a function with a bounded derivative and
+a non-zero value at the origin. Physically,
+the region <i>-&delta;...+&delta;</i> may be interpreted as the region
+where heat conduction dominates convection in the boundary layer.
+</p>
+<p>
+See the package <code>Examples</code> for the graph.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 2, 2022, by Michael Wetter:<br/>
+Set minimum and maximum attribute on <code>n</code>, improved assertion and documentation.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3135\">Buildings, #3135</a>.
+</li>
+<li>
+November 29, 2013 by Marcus Fuchs:<br/>
+Implementation based on
+<a href=\"modelica://AixLib.Utilities.Math.Functions.regNonZeroPower\">
+AixLib.Utilities.Math.Functions.regNonZeroPower</a>.
+</li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-88,38},{92,-34}},
           textColor={160,160,164},
-          textString="regNonZeroPower()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="regNonZeroPower()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end RegNonZeroPower;
diff --git a/AixLib/Utilities/Math/SmoothExponential.mo b/AixLib/Utilities/Math/SmoothExponential.mo
index e2c52803d6..cb7e67dd01 100644
--- a/AixLib/Utilities/Math/SmoothExponential.mo
+++ b/AixLib/Utilities/Math/SmoothExponential.mo
@@ -6,17 +6,17 @@ block SmoothExponential
 equation
   y = AixLib.Utilities.Math.Functions.smoothExponential(x=u, delta=delta);
   annotation (Documentation(info="<html>
- <p>Function to provide a once continuously differentiable approximation to <i>exp(- |x| )</i> in the interval <i>|x| for some positive &delta; </i></p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 29, 2013 by Marcus Fuchs:<br/>
- Implementation based on Functions.smoothExponential.
- </li>
- </ul>
- </html>"),Icon(graphics={   Text(
+<p>Function to provide a once continuously differentiable approximation to <i>exp(- |x| )</i> in the interval <i>|x| for some positive &delta; </i></p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 29, 2013 by Marcus Fuchs:<br/>
+Implementation based on Functions.smoothExponential.
+</li>
+</ul>
+</html>"), Icon(graphics={   Text(
           extent={{-88,38},{92,-34}},
           textColor={160,160,164},
-          textString="smoothExponential()")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="smoothExponential()")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothExponential;
diff --git a/AixLib/Utilities/Math/SmoothHeaviside.mo b/AixLib/Utilities/Math/SmoothHeaviside.mo
index 6330209c26..2a26983a02 100644
--- a/AixLib/Utilities/Math/SmoothHeaviside.mo
+++ b/AixLib/Utilities/Math/SmoothHeaviside.mo
@@ -47,29 +47,29 @@ equation
     Line(points={{-40,-80},{-40,-68}},
                                   color={192,192,192})}),
 Documentation(info="<html>
- <p>
- Twice Lipschitz continuously differentiable approximation to the <i>Heaviside(.,.)</i> function.
- See Example <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothHeaviside\">
- AixLib.Utilities.Math.Examples.SmoothHeaviside</a>.
- </p>
- </html>",
+<p>
+Twice Lipschitz continuously differentiable approximation to the <i>Heaviside(.,.)</i> function.
+See Example <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothHeaviside\">
+AixLib.Utilities.Math.Examples.SmoothHeaviside</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- October 21, 2019:<br/>
- Added <code>delta.min</code> attribute to guard against division by zero.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1202\">issue 1202</a>.
- </li>
- <li>
- July 17, 2015, by Marcus Fuchs:<br/>
- Add link to example.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+October 21, 2019:<br/>
+Added <code>delta.min</code> attribute to guard against division by zero.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1202\">issue 1202</a>.
+</li>
+<li>
+July 17, 2015, by Marcus Fuchs:<br/>
+Add link to example.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothHeaviside;
diff --git a/AixLib/Utilities/Math/SmoothLimit.mo b/AixLib/Utilities/Math/SmoothLimit.mo
index 5192fa7e36..b745432c88 100644
--- a/AixLib/Utilities/Math/SmoothLimit.mo
+++ b/AixLib/Utilities/Math/SmoothLimit.mo
@@ -12,27 +12,27 @@ equation
           textColor={160,160,164},
           textString="smoothLimit()")}),
 Documentation(info="<html>
- <p>
- Once continuously differentiable approximation to the <i>limit(.,.)</i> function.
- The output is bounded to be in <i>[lower, upper]</i>.
- </p>
- <p>
- Note that the limit need not be respected, such as illustrated in
- <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
- AixLib.Utilities.Math.Examples.SmoothMin</a>.
- </p>
- </html>",
+<p>
+Once continuously differentiable approximation to the <i>limit(.,.)</i> function.
+The output is bounded to be in <i>[lower, upper]</i>.
+</p>
+<p>
+Note that the limit need not be respected, such as illustrated in
+<a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
+AixLib.Utilities.Math.Examples.SmoothMin</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 12, 2015, by Filip Jorissen:<br/>
- Added documentation reference demonstrating overshoot.
- </li>
- <li>
- July 14, 2010, by Wangda Zuo, Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 12, 2015, by Filip Jorissen:<br/>
+Added documentation reference demonstrating overshoot.
+</li>
+<li>
+July 14, 2010, by Wangda Zuo, Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothLimit;
diff --git a/AixLib/Utilities/Math/SmoothMax.mo b/AixLib/Utilities/Math/SmoothMax.mo
index e383eb5042..70bdbca05f 100644
--- a/AixLib/Utilities/Math/SmoothMax.mo
+++ b/AixLib/Utilities/Math/SmoothMax.mo
@@ -13,26 +13,26 @@ equation
           textColor={0,0,255},
           textString="dX=%deltaX%")}),
 Documentation(info="<html>
- <p>
- Once continuously differentiable approximation to the <i>max(.,.)</i> function.
- </p>
- <p>
- Note that the maximum need not be respected, such as illustrated in
- <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
- AixLib.Utilities.Math.Examples.SmoothMin</a>.
- </p>
- </html>",
+<p>
+Once continuously differentiable approximation to the <i>max(.,.)</i> function.
+</p>
+<p>
+Note that the maximum need not be respected, such as illustrated in
+<a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
+AixLib.Utilities.Math.Examples.SmoothMin</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 12, 2015, by Filip Jorissen:<br/>
- Added documentation reference demonstrating overshoot.
- </li>
- <li>
- August 15, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 12, 2015, by Filip Jorissen:<br/>
+Added documentation reference demonstrating overshoot.
+</li>
+<li>
+August 15, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothMax;
diff --git a/AixLib/Utilities/Math/SmoothMin.mo b/AixLib/Utilities/Math/SmoothMin.mo
index 949d6239c4..6d2a8cdf02 100644
--- a/AixLib/Utilities/Math/SmoothMin.mo
+++ b/AixLib/Utilities/Math/SmoothMin.mo
@@ -13,26 +13,26 @@ equation
           textColor={0,0,255},
           textString="dX=%deltaX%")}),
 Documentation(info="<html>
- <p>
- Once continuously differentiable approximation to the <i>min(.,.)</i> function.
- </p>
- <p>
- Note that the minimum need not be respected, such as illustrated in
- <a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
- AixLib.Utilities.Math.Examples.SmoothMin</a>.
- </p>
- </html>",
+<p>
+Once continuously differentiable approximation to the <i>min(.,.)</i> function.
+</p>
+<p>
+Note that the minimum need not be respected, such as illustrated in
+<a href=\"modelica://AixLib.Utilities.Math.Examples.SmoothMin\">
+AixLib.Utilities.Math.Examples.SmoothMin</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 12, 2015, by Filip Jorissen:<br/>
- Added documentation reference demonstrating overshoot.
- </li>
- <li>
- August 15, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 12, 2015, by Filip Jorissen:<br/>
+Added documentation reference demonstrating overshoot.
+</li>
+<li>
+August 15, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SmoothMin;
diff --git a/AixLib/Utilities/Math/Splice.mo b/AixLib/Utilities/Math/Splice.mo
index af43d2556f..1cb77fcb50 100644
--- a/AixLib/Utilities/Math/Splice.mo
+++ b/AixLib/Utilities/Math/Splice.mo
@@ -60,22 +60,22 @@ equation
       textColor={160,160,164},
           textString="u1")}),
 Documentation(info="<html>
- <p>
- This block implements <a href=\"modelica://AixLib.Utilities.Math.Functions.spliceFunction\">
- AixLib.Utilities.Math.Functions.spliceFunction</a>, which provides a continuously differentiable transition between two arguments.
- </p>
- </html>",
+<p>
+This block implements <a href=\"modelica://AixLib.Utilities.Math.Functions.spliceFunction\">
+AixLib.Utilities.Math.Functions.spliceFunction</a>, which provides a continuously differentiable transition between two arguments.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 31, 2012, by Michael Wetter:<br/>
- Revised documentation.
- </li>
- <li>
- July 30, 2012, by Kaustubh Phalak:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+August 31, 2012, by Michael Wetter:<br/>
+Revised documentation.
+</li>
+<li>
+July 30, 2012, by Kaustubh Phalak:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Splice;
diff --git a/AixLib/Utilities/Math/TrapezoidalIntegration.mo b/AixLib/Utilities/Math/TrapezoidalIntegration.mo
index afdd3a7a26..1d34a0ec28 100644
--- a/AixLib/Utilities/Math/TrapezoidalIntegration.mo
+++ b/AixLib/Utilities/Math/TrapezoidalIntegration.mo
@@ -9,14 +9,14 @@ equation
           extent={{-90,36},{90,-36}},
           textColor={160,160,164},
           textString="trapezoidalIntegration()")}), Documentation(info="<html>
- <p>This function computes a definite integral using the trapezoidal rule. </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 29, 2013 by Marcus Fuchs:<br/>
- Implementation based on Functions.trapezoidalIntegration.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>This function computes a definite integral using the trapezoidal rule. </p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 29, 2013 by Marcus Fuchs:<br/>
+Implementation based on Functions.trapezoidalIntegration.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TrapezoidalIntegration;
diff --git a/AixLib/Utilities/Math/package.order b/AixLib/Utilities/Math/package.order
index 0eb41470b0..b7e42ec325 100644
--- a/AixLib/Utilities/Math/package.order
+++ b/AixLib/Utilities/Math/package.order
@@ -12,6 +12,7 @@ Factorial
 FallingFactorial
 IntegerReplicator
 IntegratorWithReset
+Interpolate
 InverseXRegularized
 Max
 Min
diff --git a/AixLib/Utilities/Psychrometrics/BaseClasses/HumidityRatioVaporPressure.mo b/AixLib/Utilities/Psychrometrics/BaseClasses/HumidityRatioVaporPressure.mo
index 4c52453d5f..7e8540cfe7 100644
--- a/AixLib/Utilities/Psychrometrics/BaseClasses/HumidityRatioVaporPressure.mo
+++ b/AixLib/Utilities/Psychrometrics/BaseClasses/HumidityRatioVaporPressure.mo
@@ -3,7 +3,7 @@ partial block HumidityRatioVaporPressure
   "Humidity ratio for given water vapor pressure"
   extends Modelica.Blocks.Icons.Block;
   parameter Boolean use_p_in = true "Get the pressure from the input connector"
-    annotation(Evaluate=true, HideResult=true);
+    annotation(Evaluate=true);
 
   parameter Modelica.Units.SI.Pressure p=101325 "Fixed value of pressure"
     annotation (Dialog(enable=not use_p_in));
@@ -24,27 +24,33 @@ equation
   end if;
   annotation (
     Documentation(info="<html>
- <p>
- Partial Block to compute the relation between humidity ratio and water vapor partial pressure.
- </p>
- <p>If <code>use_p_in</code> is false (default option), the <code>p</code> parameter
- is used as atmospheric pressure,
- and the <code>p_in</code> input connector is disabled;
- if <code>use_p_in</code> is true, then the <code>p</code> parameter is ignored,
- and the value provided by the input connector is used instead.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 29, 2014, by Michael Wetter:<br/>
- Removed undesirable annotation <code>Evaluate=true</code>.
- </li>
- <li>
- April 14, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Partial Block to compute the relation between humidity ratio and water vapor partial pressure.
+</p>
+<p>If <code>use_p_in</code> is false (default option), the <code>p</code> parameter
+is used as atmospheric pressure,
+and the <code>p_in</code> input connector is disabled;
+if <code>use_p_in</code> is true, then the <code>p</code> parameter is ignored,
+and the value provided by the input connector is used instead.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 11, 2024, by Michael Wetter:<br/>
+Corrected use of <code>HideResult</code>.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1850\">#1850</a>.
+</li>
+<li>
+May 29, 2014, by Michael Wetter:<br/>
+Removed undesirable annotation <code>Evaluate=true</code>.
+</li>
+<li>
+April 14, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{100,
             100}}), graphics={
         Rectangle(
@@ -62,6 +68,6 @@ equation
           visible=use_p_in,
           extent={{-90,108},{-34,16}},
           textColor={0,0,0},
-          textString="p_in")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="p_in")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HumidityRatioVaporPressure;
diff --git a/AixLib/Utilities/Psychrometrics/Constants.mo b/AixLib/Utilities/Psychrometrics/Constants.mo
index d153bd7b52..0fdb46cbfc 100644
--- a/AixLib/Utilities/Psychrometrics/Constants.mo
+++ b/AixLib/Utilities/Psychrometrics/Constants.mo
@@ -15,22 +15,22 @@ package Constants "Library of constants for psychometric functions"
 
   annotation (
     Documentation(info="<html>
- <p>
- This package provides constants for functions used
- in the calculation of thermodynamic properties of moist air.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 24, 2016, by Filip Jorissen:<br/>
- Added reference temperature.
- </li>
- <li>
- July 24, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This package provides constants for functions used
+in the calculation of thermodynamic properties of moist air.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 24, 2016, by Filip Jorissen:<br/>
+Added reference temperature.
+</li>
+<li>
+July 24, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(extent={{-100.0,-100.0},{100.0,100.0}}), graphics={
       Polygon(
         origin={-9.2597,25.6673},
@@ -52,6 +52,6 @@ package Constants "Library of constants for psychometric functions"
         pattern=LinePattern.None,
         fillPattern=FillPattern.Solid,
         points={{-10.873,41.478},{-10.873,41.478},{-14.048,-4.162},{-9.352,-24.8},{7.912,-24.469},{16.247,0.27},{16.247,0.27},{13.336,0.071},{13.336,0.071},{7.515,-9.983},{-3.134,-7.271},{-2.671,41.214},{-2.671,41.214}},
-        smooth=Smooth.Bezier)}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        smooth=Smooth.Bezier)}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Constants;
diff --git a/AixLib/Utilities/Psychrometrics/Density_pTX.mo b/AixLib/Utilities/Psychrometrics/Density_pTX.mo
index 8765bf6ccb..4922dc3eeb 100644
--- a/AixLib/Utilities/Psychrometrics/Density_pTX.mo
+++ b/AixLib/Utilities/Psychrometrics/Density_pTX.mo
@@ -34,27 +34,27 @@ equation
   annotation (
   defaultComponentName="den",
     Documentation(info="<html>
- <p>
- Block to compute the mass density of air for given
- pressure, temperature and water vapor mass fraction.
- </p>
- <p>
- Note that the water vapor mass fraction must be in <i>kg/kg</i>
- total air, and not dry air.
- </p>
- </html>",
+<p>
+Block to compute the mass density of air for given
+pressure, temperature and water vapor mass fraction.
+</p>
+<p>
+Note that the water vapor mass fraction must be in <i>kg/kg</i>
+total air, and not dry air.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- August 19, 2015, by Michael Wetter:<br/>
- Corrected default component name.
- </li>
- <li>
- February 24, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+August 19, 2015, by Michael Wetter:<br/>
+Corrected default component name.
+</li>
+<li>
+February 24, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
                     graphics={
         Polygon(
@@ -91,6 +91,6 @@ revisions="<html>
           textString="density"),
         Line(
           points={{36,-72},{6,6}},
-          color={255,0,0})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          color={255,0,0})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Density_pTX;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/Density_pTX.mo b/AixLib/Utilities/Psychrometrics/Examples/Density_pTX.mo
index 04b5a6fc92..d93d95e8ed 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/Density_pTX.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/Density_pTX.mo
@@ -35,16 +35,16 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/Density_pTX.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This examples is a unit test for the density computation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 24, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This examples is a unit test for the density computation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 24, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Density_pTX;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/DewPointTemperature.mo b/AixLib/Utilities/Psychrometrics/Examples/DewPointTemperature.mo
index f17a61c8f2..592a9fd5e2 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/DewPointTemperature.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/DewPointTemperature.mo
@@ -28,6 +28,6 @@ equation
   annotation (
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/DewPointTemperature.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end DewPointTemperature;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/HumidityRatioPressure.mo b/AixLib/Utilities/Psychrometrics/Examples/HumidityRatioPressure.mo
index 8bb2df32b3..65e82cf0e1 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/HumidityRatioPressure.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/HumidityRatioPressure.mo
@@ -48,6 +48,6 @@ equation
  annotation (
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/HumidityRatioPressure.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end HumidityRatioPressure;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/MassFraction_pTphi.mo b/AixLib/Utilities/Psychrometrics/Examples/MassFraction_pTphi.mo
index 74f5fbc6e2..aa0b49a298 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/MassFraction_pTphi.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/MassFraction_pTphi.mo
@@ -46,6 +46,6 @@ equation
   annotation (
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/MassFraction_pTphi.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end MassFraction_pTphi;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/Phi_pTX.mo b/AixLib/Utilities/Psychrometrics/Examples/Phi_pTX.mo
index c704cc8773..aebf7c8a95 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/Phi_pTX.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/Phi_pTX.mo
@@ -35,16 +35,16 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/Phi_pTX.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This examples is a unit test for the relative humidity computation.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 13, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This examples is a unit test for the relative humidity computation.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 13, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Phi_pTX;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/SaturationPressure.mo b/AixLib/Utilities/Psychrometrics/Examples/SaturationPressure.mo
index ab5b3c679b..6f3b9f4585 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/SaturationPressure.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/SaturationPressure.mo
@@ -21,14 +21,14 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/SaturationPressure.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This examples is a unit test for the saturation pressure computation.
- </html>",revisions="<html>
- <ul>
- <li>
- October 2, 2012 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This examples is a unit test for the saturation pressure computation.
+</html>", revisions="<html>
+<ul>
+<li>
+October 2, 2012 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SaturationPressure;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/SaturationPressureLiquid.mo b/AixLib/Utilities/Psychrometrics/Examples/SaturationPressureLiquid.mo
index 4c1b22f271..24d3f92267 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/SaturationPressureLiquid.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/SaturationPressureLiquid.mo
@@ -19,14 +19,14 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/SaturationPressureLiquid.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This examples is a unit test for the saturation pressure computation of liquid water.
- </html>",revisions="<html>
- <ul>
- <li>
- October 2, 2012 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This examples is a unit test for the saturation pressure computation of liquid water.
+</html>", revisions="<html>
+<ul>
+<li>
+October 2, 2012 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SaturationPressureLiquid;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/SublimationPressureIce.mo b/AixLib/Utilities/Psychrometrics/Examples/SublimationPressureIce.mo
index 296049b94c..b4c13ac51a 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/SublimationPressureIce.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/SublimationPressureIce.mo
@@ -19,14 +19,14 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/SublimationPressureIce.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This examples is a unit test for the sublimation pressure computation of ice.
- </html>",revisions="<html>
- <ul>
- <li>
- October 2, 2012 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This examples is a unit test for the sublimation pressure computation of ice.
+</html>", revisions="<html>
+<ul>
+<li>
+October 2, 2012 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SublimationPressureIce;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulPhi.mo b/AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulPhi.mo
index b8b1fc699b..59b1cf8502 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulPhi.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulPhi.mo
@@ -104,37 +104,37 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/TWetBul_TDryBulPhi.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- <p>
- This examples is a unit test for the wet bulb computation.
- The model on the top uses the accurate computation of the
- wet bulb temperature, whereas the model below uses the approximate
- computation of the wet bulb temperature.
- </p>
- <p>
- The model contains an assert that validates the model based on a single operating point from Example 17.1 in
- Ananthanarayanan (2013).
- </p>
- <h4>References</h4>
- <p>
- Ananthanarayanan, P. N. Basic refrigeration and air conditioning. Tata McGraw-Hill Education, 2013.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- June 23, 2016, by Michael Wetter:<br/>
- Changed graphical annotation.
- </li>
- <li>
- May 24, 2016, by Filip Jorissen:<br/>
- Updated example with validation data.
- See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a>
- for a discussion.
- </li>
- <li>
- October 1, 2012 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This examples is a unit test for the wet bulb computation.
+The model on the top uses the accurate computation of the
+wet bulb temperature, whereas the model below uses the approximate
+computation of the wet bulb temperature.
+</p>
+<p>
+The model contains an assert that validates the model based on a single operating point from Example 17.1 in
+Ananthanarayanan (2013).
+</p>
+<h4>References</h4>
+<p>
+Ananthanarayanan, P. N. Basic refrigeration and air conditioning. Tata McGraw-Hill Education, 2013.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+June 23, 2016, by Michael Wetter:<br/>
+Changed graphical annotation.
+</li>
+<li>
+May 24, 2016, by Filip Jorissen:<br/>
+Updated example with validation data.
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a>
+for a discussion.
+</li>
+<li>
+October 1, 2012 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TWetBul_TDryBulPhi;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulXi.mo b/AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulXi.mo
index 0a95958307..a809b5b4be 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulXi.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/TWetBul_TDryBulXi.mo
@@ -51,25 +51,25 @@ equation
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/TWetBul_TDryBulXi.mos"
         "Simulate and plot"),
     Documentation(info="<html>
- This examples is a unit test for the wet bulb computation.
- The model on the top uses the accurate computation of the
- wet bulb temperature, whereas the model below uses the approximate
- computation of the wet bulb temperature.
- </html>",revisions="<html>
- <ul>
- <li>
- June 23, 2016, by Michael Wetter:<br/>
- Changed graphical annotation.
- </li>
- <li>
- October 1, 2012 by Michael Wetter:<br/>
- Revised implementation to add approximate computation of wet bulb temperature.
- </li>
- <li>
- May 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+This examples is a unit test for the wet bulb computation.
+The model on the top uses the accurate computation of the
+wet bulb temperature, whereas the model below uses the approximate
+computation of the wet bulb temperature.
+</html>", revisions="<html>
+<ul>
+<li>
+June 23, 2016, by Michael Wetter:<br/>
+Changed graphical annotation.
+</li>
+<li>
+October 1, 2012 by Michael Wetter:<br/>
+Revised implementation to add approximate computation of wet bulb temperature.
+</li>
+<li>
+May 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TWetBul_TDryBulXi;
diff --git a/AixLib/Utilities/Psychrometrics/Examples/TotalAirDryAir.mo b/AixLib/Utilities/Psychrometrics/Examples/TotalAirDryAir.mo
index 5fd684d126..b9e4dfff4d 100644
--- a/AixLib/Utilities/Psychrometrics/Examples/TotalAirDryAir.mo
+++ b/AixLib/Utilities/Psychrometrics/Examples/TotalAirDryAir.mo
@@ -32,6 +32,6 @@ equation
   annotation (
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Examples/TotalAirDryAir.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TotalAirDryAir;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck.mo
index c74d11ac51..445aa9ee42 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck.mo
@@ -23,37 +23,37 @@ annotation (
         StopTime=1,
         Tolerance=1E-9),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- April 22, 2016, by Michael Wetter:<br/>
- Changed accuarcy test in assertion to use the relative error because the
- magnitude of <code>y</code> is <i>1E5</i> and hence testing an absolute
- error is too stringent.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
- </li>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Added a high tolerance which is needed for OpenModelica to pass the assert
- statement.
- </li>
- <li>
- October 29, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+April 22, 2016, by Michael Wetter:<br/>
+Changed accuarcy test in assertion to use the relative error because the
+magnitude of <code>y</code> is <i>1E5</i> and hence testing an absolute
+error is too stringent.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
+</li>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Added a high tolerance which is needed for OpenModelica to pass the assert
+statement.
+</li>
+<li>
+October 29, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DewPointTemperatureDerivativeCheck;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck_amb.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck_amb.mo
index 37e1f50340..05a6dc6920 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck_amb.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/DewPointTemperatureDerivativeCheck_amb.mo
@@ -24,37 +24,37 @@ annotation (
       StopTime=1,
       Tolerance=1E-9),
     Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 22, 2016, by Michael Wetter:<br/>
- Changed accuarcy test in assertion to use the relative error because the
- magnitude of <code>y</code> is <i>1E5</i> and hence testing an absolute
- error is too stringent.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
- </li>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Added a high tolerance which is needed for OpenModelica to pass the assert
- statement.
- </li>
- <li>
- October 29, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 22, 2016, by Michael Wetter:<br/>
+Changed accuarcy test in assertion to use the relative error because the
+magnitude of <code>y</code> is <i>1E5</i> and hence testing an absolute
+error is too stringent.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
+</li>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Added a high tolerance which is needed for OpenModelica to pass the assert
+statement.
+</li>
+<li>
+October 29, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end DewPointTemperatureDerivativeCheck_amb;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/InverseDewPointTemperatureDerivativeCheck_amb.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/InverseDewPointTemperatureDerivativeCheck_amb.mo
index 7f0d3755c1..cc28c51e07 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/InverseDewPointTemperatureDerivativeCheck_amb.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/InverseDewPointTemperatureDerivativeCheck_amb.mo
@@ -23,24 +23,24 @@ equation
       StopTime=1,
       Tolerance=1E-9),
     Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- October 29, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+October 29, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end InverseDewPointTemperatureDerivativeCheck_amb;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/SaturationPressureDerivativeCheck.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/SaturationPressureDerivativeCheck.mo
index 46890e9571..a00ad5aea7 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/SaturationPressureDerivativeCheck.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/SaturationPressureDerivativeCheck.mo
@@ -27,37 +27,37 @@ annotation (
         StopTime=1,
         Tolerance=1E-9),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- April 22, 2016, by Michael Wetter:<br/>
- Changed accuarcy test in assertion to use the relative error because the
- magnitude of <code>y</code> is <i>1E5</i> and hence testing an absolute
- error is too stringent.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
- </li>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Added a high tolerance which is needed for OpenModelica to pass the assert
- statement.
- </li>
- <li>
- November 20, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+April 22, 2016, by Michael Wetter:<br/>
+Changed accuarcy test in assertion to use the relative error because the
+magnitude of <code>y</code> is <i>1E5</i> and hence testing an absolute
+error is too stringent.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
+</li>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Added a high tolerance which is needed for OpenModelica to pass the assert
+statement.
+</li>
+<li>
+November 20, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SaturationPressureDerivativeCheck;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/WaterVaporPressureDerivativeCheck.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/WaterVaporPressureDerivativeCheck.mo
index e74a85a96b..6ab178d7fa 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/WaterVaporPressureDerivativeCheck.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/Examples/WaterVaporPressureDerivativeCheck.mo
@@ -29,37 +29,37 @@ annotation (
         StopTime=1,
         Tolerance=1E-9),
       Documentation(info="<html>
- <p>
- This example checks whether the function derivative
- is implemented correctly. If the derivative implementation
- is not correct, the model will stop with an assert statement.
- </p>
- </html>",  revisions="<html>
- <ul>
- <li>
- April 22, 2016, by Michael Wetter:<br/>
- Changed accuarcy test in assertion to use the relative error because the
- magnitude of <code>y</code> is <i>1E5</i> and hence testing an absolute
- error is too stringent.
- This is for
- <a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
- </li>
- <li>
- August 17, 2015 by Michael Wetter:<br/>
- Updated regression test to have slope that is different from one.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
- </li>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Added a high tolerance which is needed for OpenModelica to pass the assert
- statement.
- </li>
- <li>
- October 29, 2008, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example checks whether the function derivative
+is implemented correctly. If the derivative implementation
+is not correct, the model will stop with an assert statement.
+</p>
+</html>",   revisions="<html>
+<ul>
+<li>
+April 22, 2016, by Michael Wetter:<br/>
+Changed accuarcy test in assertion to use the relative error because the
+magnitude of <code>y</code> is <i>1E5</i> and hence testing an absolute
+error is too stringent.
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/510\">Buildings, issue 510</a>.
+</li>
+<li>
+August 17, 2015 by Michael Wetter:<br/>
+Updated regression test to have slope that is different from one.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/303\">issue 303</a>.
+</li>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Added a high tolerance which is needed for OpenModelica to pass the assert
+statement.
+</li>
+<li>
+October 29, 2008, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end WaterVaporPressureDerivativeCheck;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_TDewPoi_pW_amb.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_TDewPoi_pW_amb.mo
index adab4832b4..414c6260cd 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_TDewPoi_pW_amb.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_TDewPoi_pW_amb.mo
@@ -20,22 +20,22 @@ algorithm
 
   annotation (
     Documentation(info="<html>
- <p>
- Derivative of dew point temperature calculation for moist air.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Removed <code>extends AixLib.Utilities.Psychrometrics.Functions.BaseClasses.pW_TDewPoi_amb</code>
- as this gives a compile time error in OpenModelica as the input argument <code>T</code>
- cannot be found.
- </li>
- <li>
- May 21, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Derivative of dew point temperature calculation for moist air.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Removed <code>extends AixLib.Utilities.Psychrometrics.Functions.BaseClasses.pW_TDewPoi_amb</code>
+as this gives a compile time error in OpenModelica as the input argument <code>T</code>
+cannot be found.
+</li>
+<li>
+May 21, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_TDewPoi_pW_amb;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi.mo
index b04c630cb8..0047db0d0b 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi.mo
@@ -16,16 +16,16 @@ algorithm
     Modelica.Math.log(T))*(-C8/T/T + C10 + 2*C11*T + 3*C12*T*T + C13/T)*dT;
   annotation (
     Documentation(info="<html>
- <p>
- Derivative of dew point temperature calculation for moist air above freezing temperature.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 15, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Derivative of dew point temperature calculation for moist air above freezing temperature.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 15, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_pW_TDewPoi;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi_amb.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi_amb.mo
index becee0b816..0dbfc4dd30 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi_amb.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_TDewPoi_amb.mo
@@ -19,22 +19,22 @@ algorithm
 
   annotation (
     Documentation(info="<html>
- <p>
- Derivative of dew point temperature calculation for moist air.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Removed <code>extends AixLib.Utilities.Psychrometrics.Functions.BaseClasses.pW_TDewPoi_amb</code>
- as this gives a compile time error in OpenModelica as the input argument <code>T</code>
- cannot be found.
- </li>
- <li>
- May 21, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Derivative of dew point temperature calculation for moist air.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Removed <code>extends AixLib.Utilities.Psychrometrics.Functions.BaseClasses.pW_TDewPoi_amb</code>
+as this gives a compile time error in OpenModelica as the input argument <code>T</code>
+cannot be found.
+</li>
+<li>
+May 21, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_pW_TDewPoi_amb;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_X.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_X.mo
index 4a336853e1..cf35358764 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_X.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_pW_X.mo
@@ -25,18 +25,18 @@ algorithm
 
   annotation (
     Documentation(info="<html>
- <p>
- Derivative of function
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.pW_X\">
- AixLib.Utilities.Psychrometrics.Functions.pW_X</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- May 21, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Derivative of function
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.pW_X\">
+AixLib.Utilities.Psychrometrics.Functions.pW_X</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 21, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_pW_X;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_saturationPressureLiquid.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_saturationPressureLiquid.mo
index 215104538d..e377664c75 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_saturationPressureLiquid.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_saturationPressureLiquid.mo
@@ -13,25 +13,25 @@ algorithm
   annotation(Inline=false,
     smoothOrder=98,
     Documentation(info="<html>
- <p>
- Derivative of function
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid\">
- AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid</a>.
- </p>
- </html>",
+<p>
+Derivative of function
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid\">
+AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 12, 2020, by Michael Wetter:<br/>
- Corrected name of argument to comply with derivative specification.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1393\">#1393</a>.
- </li>
- <li>
- November 20, 2013 by Michael Wetter:<br/>
- First implementation, moved from <code>AixLib.Media</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 12, 2020, by Michael Wetter:<br/>
+Corrected name of argument to comply with derivative specification.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1393\">#1393</a>.
+</li>
+<li>
+November 20, 2013 by Michael Wetter:<br/>
+First implementation, moved from <code>AixLib.Media</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_saturationPressureLiquid;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_sublimationPressureIce.mo b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_sublimationPressureIce.mo
index 78bbd5ac2d..5df39bcf9b 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_sublimationPressureIce.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/BaseClasses/der_sublimationPressureIce.mo
@@ -20,26 +20,26 @@ algorithm
       Inline=false,
       smoothOrder=5,
       Documentation(info="<html>
- <p>
- Derivative of function
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.sublimationPressureIce\">
- AixLib.Utilities.Psychrometrics.Functions.sublimationPressureIce</a>.
- </p>
- </html>",
+<p>
+Derivative of function
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.sublimationPressureIce\">
+AixLib.Utilities.Psychrometrics.Functions.sublimationPressureIce</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 12, 2020, by Michael Wetter:<br/>
- Change name of argument <code>dTsat</code> to <code>dTSat</code> for consistency
- with
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_saturationPressureLiquid\">
- AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_saturationPressureLiquid</a>.
- </li>
- <li>
- November 20, 2013 by Michael Wetter:<br/>
- First implementation, moved from <code>AixLib.Media</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 12, 2020, by Michael Wetter:<br/>
+Change name of argument <code>dTsat</code> to <code>dTSat</code> for consistency
+with
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_saturationPressureLiquid\">
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_saturationPressureLiquid</a>.
+</li>
+<li>
+November 20, 2013 by Michael Wetter:<br/>
+First implementation, moved from <code>AixLib.Media</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end der_sublimationPressureIce;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/Examples/Density_pTX.mo b/AixLib/Utilities/Psychrometrics/Functions/Examples/Density_pTX.mo
index 5c820eb684..341ea7922f 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/Examples/Density_pTX.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/Examples/Density_pTX.mo
@@ -23,19 +23,19 @@ __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psy
         "Simulate and plot"),
     Documentation(
 info="<html>
- <p>
- Model that tests the implementation of
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.density_pTX\">
- AixLib.Utilities.Psychrometrics.Functions.density_pTX</a>.
- </p>
- </html>",
+<p>
+Model that tests the implementation of
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.density_pTX\">
+AixLib.Utilities.Psychrometrics.Functions.density_pTX</a>.
+</p>
+</html>",
     revisions="<html>
- <ul>
- <li>
- February 24, 2015 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+February 24, 2015 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end Density_pTX;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/Examples/SaturationPressure.mo b/AixLib/Utilities/Psychrometrics/Functions/Examples/SaturationPressure.mo
index c389834ad3..432e1f431a 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/Examples/SaturationPressure.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/Examples/SaturationPressure.mo
@@ -13,22 +13,22 @@ equation
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Functions/Examples/SaturationPressure.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This example computes the saturation pressure of water.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 22, 2016, by Michael Wetter:<br/>
- Corrected script name to use capital letter.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/510\">Buildings, issue 510</a>.
- </li>
- <li>
- November 20, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example computes the saturation pressure of water.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+April 22, 2016, by Michael Wetter:<br/>
+Corrected script name to use capital letter.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/510\">Buildings, issue 510</a>.
+</li>
+<li>
+November 20, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end SaturationPressure;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/Examples/X_pSatpphi.mo b/AixLib/Utilities/Psychrometrics/Functions/Examples/X_pSatpphi.mo
index 41d7f092a9..c5992de5d1 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/Examples/X_pSatpphi.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/Examples/X_pSatpphi.mo
@@ -23,23 +23,23 @@ equation
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Functions/Examples/X_pSatpphi.mos"
         "Simulate and plot"), Documentation(info="<html>
- <p>
- This example computes the water content of air for a relative humidity between
- <i>0</i> and <i>100%</i>,
- a temperature of <i>20&deg;C</i>
- and atmospheric pressure.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Added conversion factor to avoid a unit error.
- </li>
- <li>
- August 21, 2012, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This example computes the water content of air for a relative humidity between
+<i>0</i> and <i>100%</i>,
+a temperature of <i>20&deg;C</i>
+and atmospheric pressure.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Added conversion factor to avoid a unit error.
+</li>
+<li>
+August 21, 2012, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end X_pSatpphi;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi.mo b/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi.mo
index 6a9aa6c52f..41d2206b9e 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi.mo
@@ -16,6 +16,6 @@ equation
   annotation (
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end pW_TDewPoi;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi_comparison.mo b/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi_comparison.mo
index dca6c4568f..9879e1ccc8 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi_comparison.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi_comparison.mo
@@ -23,6 +23,6 @@ equation
   annotation (
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Functions/Examples/pW_TDewPoi_comparison.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end pW_TDewPoi_comparison;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_X.mo b/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_X.mo
index 5607bf6409..10fe6a272f 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_X.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/Examples/pW_X.mo
@@ -16,6 +16,6 @@ equation
   annotation (
 experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Functions/Examples/pW_X.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end pW_X;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/Examples/phi_pTX.mo b/AixLib/Utilities/Psychrometrics/Functions/Examples/phi_pTX.mo
index 31321d001a..82548c65a0 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/Examples/phi_pTX.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/Examples/phi_pTX.mo
@@ -26,13 +26,13 @@ experiment(Tolerance=1e-6, StopTime=1.0),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Psychrometrics/Functions/Examples/phi_pTX.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
- <ul>
- <li>
- April 4, 2019 by Filip Jorissen:<br/>
- Added inverse implementation check
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1110\">#1110</a>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 4, 2019 by Filip Jorissen:<br/>
+Added inverse implementation check
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1110\">#1110</a>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end phi_pTX;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW.mo b/AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW.mo
index 83fd279c46..c3c28fdfcc 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW.mo
@@ -26,56 +26,56 @@ algorithm
       u_max=400);
   annotation (
     Documentation(info="<html>
- <p>
- Dew point temperature calculation for moist air above freezing temperature.
- </p>
- <p>
- The correlation used in this model is valid for dew point temperatures between
- <i>0</i>&deg;C and <i>200</i>&deg;C. It is the correlation from 2005
- ASHRAE Handbook, p. 6.2. In an earlier version of this model, the equation from
- Peppers has been used, but this equation yielded about <i>15</i> Kelvin lower dew point
- temperatures.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 28, 2020, by Michael Wetter:<br/>
- Replaced call to <code>Media.Common.OneNonLinearEquation</code> to use
- <a href=\"modelica://Modelica.Math.Nonlinear.solveOneNonlinearEquation\">
- Modelica.Math.Nonlinear.solveOneNonlinearEquation</a>
- because <code>Media.Common.OneNonLinearEquation</code> will be obsolete in MSL 4.0.0.<br/>
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1299\">issue 1299</a>.
- </li>
- <li>
- April 29, 2014 by Michael Wetter:<br/>
- Added dummy argument to <code>Internal.solve</code> to avoid a warning
- in Dymola 2015.
- </li>
- <li>
- March 9, 2012 by Michael Wetter:<br/>
- Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
- </li>
- <li>
- February 17, 2010 by Michael Wetter:<br/>
- Renamed function from <code>dewPointTemperature</code> to <code>pW_TDewPoi</code>.
- </li>
- <li>
- February 6, 2010 by Michael Wetter:<br/>
- Fixed derivative implementation.
- </li>
- <li>
- September 4, 2008 by Michael Wetter:<br/>
- Changed from causal to acausal ports, needed, for example, for
- <a href=\"modelica://AixLib.Fluid.Examples.MixingVolumeMoistAir\">
- AixLib.Fluid.Examples.MixingVolumeMoistAir</a>.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-        Inline=true,
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Dew point temperature calculation for moist air above freezing temperature.
+</p>
+<p>
+The correlation used in this model is valid for dew point temperatures between
+<i>0</i>&deg;C and <i>200</i>&deg;C. It is the correlation from 2005
+ASHRAE Handbook, p. 6.2. In an earlier version of this model, the equation from
+Peppers has been used, but this equation yielded about <i>15</i> Kelvin lower dew point
+temperatures.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 28, 2020, by Michael Wetter:<br/>
+Replaced call to <code>Media.Common.OneNonLinearEquation</code> to use
+<a href=\"modelica://Modelica.Math.Nonlinear.solveOneNonlinearEquation\">
+Modelica.Math.Nonlinear.solveOneNonlinearEquation</a>
+because <code>Media.Common.OneNonLinearEquation</code> will be obsolete in MSL 4.0.0.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1299\">issue 1299</a>.
+</li>
+<li>
+April 29, 2014 by Michael Wetter:<br/>
+Added dummy argument to <code>Internal.solve</code> to avoid a warning
+in Dymola 2015.
+</li>
+<li>
+March 9, 2012 by Michael Wetter:<br/>
+Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
+</li>
+<li>
+February 17, 2010 by Michael Wetter:<br/>
+Renamed function from <code>dewPointTemperature</code> to <code>pW_TDewPoi</code>.
+</li>
+<li>
+February 6, 2010 by Michael Wetter:<br/>
+Fixed derivative implementation.
+</li>
+<li>
+September 4, 2008 by Michael Wetter:<br/>
+Changed from causal to acausal ports, needed, for example, for
+<a href=\"modelica://AixLib.Fluid.Examples.MixingVolumeMoistAir\">
+AixLib.Fluid.Examples.MixingVolumeMoistAir</a>.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+        Inline=true, 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TDewPoi_pW;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW_amb.mo b/AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW_amb.mo
index f5f67bbcd5..b50c0447aa 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW_amb.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/TDewPoi_pW_amb.mo
@@ -24,39 +24,39 @@ algorithm
     smoothOrder=99,
     derivative=BaseClasses.der_TDewPoi_pW_amb,
     Documentation(info="<html>
- <p>
- Dew point temperature calculation for moist air between <i>0</i>&deg;C and <i>30</i>&deg;C
- with partial pressure of water vapor as an input.
- </p>
- <p>
- The correlation used in this model is valid for dew point temperatures between
- <i>0</i>&deg;C and <i>30</i>&deg;C. It is an approximation to the correlation from 2005
- ASHRAE Handbook, p. 6.2, which is valid in a wider range of temperatures and implemented
- in
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi\">
- AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi</a>.
- The approximation error of this simplified function is below 5% for a
- temperature of <i>0</i>&deg;C to <i>30</i>&deg;C.
- The benefit of this simpler function is that it can be inverted analytically,
- whereas the other function requires a numerical solution.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Removed <code>extends AixLib.Utilities.Psychrometrics.Functions.BaseClasses.pW_TDewPoi_amb</code>
- as this gives a compile time error in OpenModelica as the input argument <code>T</code>
- cannot be found.
- </li>
- <li>
- March 9, 2012 by Michael Wetter:<br/>
- Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
- </li>
- <li>
- May 21, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Dew point temperature calculation for moist air between <i>0</i>&deg;C and <i>30</i>&deg;C
+with partial pressure of water vapor as an input.
+</p>
+<p>
+The correlation used in this model is valid for dew point temperatures between
+<i>0</i>&deg;C and <i>30</i>&deg;C. It is an approximation to the correlation from 2005
+ASHRAE Handbook, p. 6.2, which is valid in a wider range of temperatures and implemented
+in
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi\">
+AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi</a>.
+The approximation error of this simplified function is below 5% for a
+temperature of <i>0</i>&deg;C to <i>30</i>&deg;C.
+The benefit of this simpler function is that it can be inverted analytically,
+whereas the other function requires a numerical solution.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Removed <code>extends AixLib.Utilities.Psychrometrics.Functions.BaseClasses.pW_TDewPoi_amb</code>
+as this gives a compile time error in OpenModelica as the input argument <code>T</code>
+cannot be found.
+</li>
+<li>
+March 9, 2012 by Michael Wetter:<br/>
+Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
+</li>
+<li>
+May 21, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TDewPoi_pW_amb;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/X_pSatpphi.mo b/AixLib/Utilities/Psychrometrics/Functions/X_pSatpphi.mo
index bed454139e..04439f4e54 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/X_pSatpphi.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/X_pSatpphi.mo
@@ -18,17 +18,17 @@ algorithm
     smoothOrder=99,
     Inline=true,
     Documentation(info="<html>
- <p>
- Function to compute the water vapor concentration based on
- saturation pressure, absolute pressure and relative humidity.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- August 21, 2012 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function to compute the water vapor concentration based on
+saturation pressure, absolute pressure and relative humidity.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+August 21, 2012 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end X_pSatpphi;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/X_pTphi.mo b/AixLib/Utilities/Psychrometrics/Functions/X_pTphi.mo
index c97b5321c4..d62813acb5 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/X_pTphi.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/X_pTphi.mo
@@ -14,22 +14,22 @@ algorithm
     inverse(phi=phi_pTX(p,T,X_w)),
     smoothOrder=1,
     Documentation(info="<html>
- <p>
- Absolute humidity of air for given
- pressure, temperature and relative humidity.
- </p>
- <p>
- Note that the absolute humidity is in <i>kg/kg</i>
- total air, and not dry air.
- </p>
- </html>",
+<p>
+Absolute humidity of air for given
+pressure, temperature and relative humidity.
+</p>
+<p>
+Note that the absolute humidity is in <i>kg/kg</i>
+total air, and not dry air.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 4, 2019 by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 4, 2019 by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end X_pTphi;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/X_pW.mo b/AixLib/Utilities/Psychrometrics/Functions/X_pW.mo
index 0cfd0c7613..4c311b513c 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/X_pW.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/X_pW.mo
@@ -21,36 +21,36 @@ algorithm
     smoothOrder=99,
     Inline=true,
     Documentation(info="<html>
- <p>
- Function to compute the mass fraction for a given water vapor partial pressure.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- February 14, 2021 by Ettore Zanetti:<br/>
- Updated description.
- </li>
- <li>
- September 16, 2013 by Michael Wetter:<br/>
- Added attributes to variable <code>p_w</code>.
- </li>
- <li>
- March 9, 2012 by Michael Wetter:<br/>
- Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
- </li>
- <li>
- February 17, 2010 by Michael Wetter:<br/>
- Renamed block from <code>HumidityRatio_pWat</code> to <code>X_pW</code>.
- </li>
- <li>
- April 14, 2009 by Michael Wetter:<br/>
- Converted model to block because <code>RealInput</code> are obsolete in Modelica 3.0.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function to compute the mass fraction for a given water vapor partial pressure.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+February 14, 2021 by Ettore Zanetti:<br/>
+Updated description.
+</li>
+<li>
+September 16, 2013 by Michael Wetter:<br/>
+Added attributes to variable <code>p_w</code>.
+</li>
+<li>
+March 9, 2012 by Michael Wetter:<br/>
+Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
+</li>
+<li>
+February 17, 2010 by Michael Wetter:<br/>
+Renamed block from <code>HumidityRatio_pWat</code> to <code>X_pW</code>.
+</li>
+<li>
+April 14, 2009 by Michael Wetter:<br/>
+Converted model to block because <code>RealInput</code> are obsolete in Modelica 3.0.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end X_pW;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/density_pTX.mo b/AixLib/Utilities/Psychrometrics/Functions/density_pTX.mo
index 33e6607f51..8ff37a4e51 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/density_pTX.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/density_pTX.mo
@@ -17,25 +17,25 @@ algorithm
 
   annotation (smoothOrder=99,
   Documentation(info="<html>
- <p>
- Function to compute the density of moist air for given
- pressure, temperature and water vapor mass fraction.
- </p>
- <p>
- Note that the water vapor mass fraction is in <i>kg/kg</i>
- total air.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- November 23, 2015 by Filip Jorissen:<br/>
- Added derivative information for avoiding numerical Jacobians.
- </li>
- <li>
- February 24, 2015 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function to compute the density of moist air for given
+pressure, temperature and water vapor mass fraction.
+</p>
+<p>
+Note that the water vapor mass fraction is in <i>kg/kg</i>
+total air.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+November 23, 2015 by Filip Jorissen:<br/>
+Added derivative information for avoiding numerical Jacobians.
+</li>
+<li>
+February 24, 2015 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end density_pTX;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi.mo b/AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi.mo
index 42bbe2ee23..cef58adb86 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi.mo
@@ -18,44 +18,44 @@ algorithm
     Modelica.Math.log(T));
   annotation (
     Documentation(info="<html>
- <p>
- Dew point temperature calculation for moist air above freezing temperature.
- </p>
- <p>
- The correlation used in this model is valid for dew point temperatures between
- <i>0</i>&deg;C and <i>200</i>&deg;C. It is the correlation from 2005
- ASHRAE Handbook, p. 6.2. In an earlier version of this model, the equation from
- Peppers has been used, but this equation yielded about <i>15</i> Kelvin lower dew point
- temperatures.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 9, 2012 by Michael Wetter:<br/>
- Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
- </li>
- <li>
- February 17, 2010 by Michael Wetter:<br/>
- Renamed function from <code>dewPointTemperature</code> to <code>pW_TDewPoi</code>.
- </li>
- <li>
- February 6, 2010 by Michael Wetter:<br/>
- Fixed derivative implementation.
- </li>
- <li>
- September 4, 2008 by Michael Wetter:<br/>
- Changed from causal to acausal ports, needed, for example, for
- <a href=\"modelica://AixLib.Fluid.Examples.MixingVolumeMoistAir\">
- AixLib.Fluid.Examples.MixingVolumeMoistAir</a>.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Dew point temperature calculation for moist air above freezing temperature.
+</p>
+<p>
+The correlation used in this model is valid for dew point temperatures between
+<i>0</i>&deg;C and <i>200</i>&deg;C. It is the correlation from 2005
+ASHRAE Handbook, p. 6.2. In an earlier version of this model, the equation from
+Peppers has been used, but this equation yielded about <i>15</i> Kelvin lower dew point
+temperatures.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2012 by Michael Wetter:<br/>
+Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
+</li>
+<li>
+February 17, 2010 by Michael Wetter:<br/>
+Renamed function from <code>dewPointTemperature</code> to <code>pW_TDewPoi</code>.
+</li>
+<li>
+February 6, 2010 by Michael Wetter:<br/>
+Fixed derivative implementation.
+</li>
+<li>
+September 4, 2008 by Michael Wetter:<br/>
+Changed from causal to acausal ports, needed, for example, for
+<a href=\"modelica://AixLib.Fluid.Examples.MixingVolumeMoistAir\">
+AixLib.Fluid.Examples.MixingVolumeMoistAir</a>.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Inline=true,
     smoothOrder=99,
-    derivative=BaseClasses.der_pW_TDewPoi,
-  __Dymola_LockedEditing="Model from IBPSA");
+    derivative=BaseClasses.der_pW_TDewPoi, 
+   __Dymola_LockedEditing="Model from IBPSA");
 end pW_TDewPoi;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi_amb.mo b/AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi_amb.mo
index 90101ede96..9ca9aa2782 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi_amb.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/pW_TDewPoi_amb.mo
@@ -24,38 +24,38 @@ algorithm
     Inline=true,
     derivative=BaseClasses.der_pW_TDewPoi_amb,
     Documentation(info="<html>
- <p>
- Dew point temperature calculation for moist air between <i>0 degC</i> and <i>30 degC</i>.
- </p>
- <p>
- The correlation used in this model is valid for dew point temperatures between
- <i>0</i>&deg;C and <i>30</i>&deg;C. It is an approximation to the correlation from 2005
- ASHRAE Handbook, p. 6.2, which is valid in a wider range of temperatures and implemented
- in
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi\">
- AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi</a>.
- The approximation error of this simplified function is below 5% for a
- temperature of <i>0</i>&deg;C to <i>30</i>&deg;C.
- The benefit of this simpler function is that it can be inverted analytically,
- whereas the other function requires a numerical solution.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 4, 2014, by Michael Wetter:<br/>
- Removed <code>extends AixLib.Utilities.Psychrometrics.Functions.BaseClasses.pW_TDewPoi_amb</code>
- as this gives a compile time error in OpenModelica as the input argument <code>T</code>
- cannot be found.
- </li>
- <li>
- March 9, 2012 by Michael Wetter:<br/>
- Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
- </li>
- <li>
- May 21, 2010 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Dew point temperature calculation for moist air between <i>0 degC</i> and <i>30 degC</i>.
+</p>
+<p>
+The correlation used in this model is valid for dew point temperatures between
+<i>0</i>&deg;C and <i>30</i>&deg;C. It is an approximation to the correlation from 2005
+ASHRAE Handbook, p. 6.2, which is valid in a wider range of temperatures and implemented
+in
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi\">
+AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi</a>.
+The approximation error of this simplified function is below 5% for a
+temperature of <i>0</i>&deg;C to <i>30</i>&deg;C.
+The benefit of this simpler function is that it can be inverted analytically,
+whereas the other function requires a numerical solution.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 4, 2014, by Michael Wetter:<br/>
+Removed <code>extends AixLib.Utilities.Psychrometrics.Functions.BaseClasses.pW_TDewPoi_amb</code>
+as this gives a compile time error in OpenModelica as the input argument <code>T</code>
+cannot be found.
+</li>
+<li>
+March 9, 2012 by Michael Wetter:<br/>
+Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
+</li>
+<li>
+May 21, 2010 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end pW_TDewPoi_amb;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/pW_X.mo b/AixLib/Utilities/Psychrometrics/Functions/pW_X.mo
index f8add7ba9a..eef9f5961c 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/pW_X.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/pW_X.mo
@@ -20,28 +20,28 @@ algorithm
     smoothOrder=99,
     derivative=BaseClasses.der_pW_X,
     Documentation(info="<html>
- <p>
- Function to compute the water vapor partial pressure for a given humidity ratio.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- March 9, 2012 by Michael Wetter:<br/>
- Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
- </li>
- <li>
- February 17, 2010 by Michael Wetter:<br/>
- Renamed block from <code>VaporPressure_X</code> to <code>pW_X</code>.
- </li>
- <li>
- April 14, 2009 by Michael Wetter:<br/>
- Converted model to block because <code>RealInput</code> are obsolete in Modelica 3.0.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Function to compute the water vapor partial pressure for a given humidity ratio.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 9, 2012 by Michael Wetter:<br/>
+Added <code>smoothOrder=99</code> and <code>displayUnit</code> for pressure.
+</li>
+<li>
+February 17, 2010 by Michael Wetter:<br/>
+Renamed block from <code>VaporPressure_X</code> to <code>pW_X</code>.
+</li>
+<li>
+April 14, 2009 by Michael Wetter:<br/>
+Converted model to block because <code>RealInput</code> are obsolete in Modelica 3.0.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end pW_X;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/phi_pTX.mo b/AixLib/Utilities/Psychrometrics/Functions/phi_pTX.mo
index 893a6efd92..39e3aac2ac 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/phi_pTX.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/phi_pTX.mo
@@ -14,33 +14,33 @@ algorithm
     inverse(X_w=X_pTphi(p,T,phi)),
     smoothOrder=1,
     Documentation(info="<html>
- <p>
- Relative humidity of air for given
- pressure, temperature and water vapor mass fraction.
- </p>
- <p>
- Note that the water vapor mass fraction must be in <i>kg/kg</i>
- total air, and not dry air.
- </p>
- </html>",
+<p>
+Relative humidity of air for given
+pressure, temperature and water vapor mass fraction.
+</p>
+<p>
+Note that the water vapor mass fraction must be in <i>kg/kg</i>
+total air, and not dry air.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- April 4, 2019 by Filip Jorissen:<br/>
- Added inverse annotation
- for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1110\">#1110</a>.
- </li>
- <li>
- November 17, 2014 by Michael Wetter:<br/>
- Removed test that constrains the saturation pressure to be
- lower than <code>p</code>.
- I do not see any numerical problems without this test.
- </li>
- <li>
- November 13, 2014 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+April 4, 2019 by Filip Jorissen:<br/>
+Added inverse annotation
+for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1110\">#1110</a>.
+</li>
+<li>
+November 17, 2014 by Michael Wetter:<br/>
+Removed test that constrains the saturation pressure to be
+lower than <code>p</code>.
+I do not see any numerical problems without this test.
+</li>
+<li>
+November 13, 2014 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end phi_pTX;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/saturationPressure.mo b/AixLib/Utilities/Psychrometrics/Functions/saturationPressure.mo
index 4c84d88986..4c306091ae 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/saturationPressure.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/saturationPressure.mo
@@ -16,42 +16,42 @@ algorithm
   annotation(Inline=true,
     smoothOrder=1,
     Documentation(info="<html>
- <p>
- Saturation pressure of water, computed from temperature,
- according to Wagner <i>et al.</i> (1993).
- The range of validity is between
- <i>190</i> and <i>373.16</i> Kelvin.
- </p>
- <h4>References</h4>
- <p>
- Wagner W., A. Saul, A. Pruss.
-  <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
- equation 3.5. 1993.
- <a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
- http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
- </p>
- </html>",
+<p>
+Saturation pressure of water, computed from temperature,
+according to Wagner <i>et al.</i> (1993).
+The range of validity is between
+<i>190</i> and <i>373.16</i> Kelvin.
+</p>
+<h4>References</h4>
+<p>
+Wagner W., A. Saul, A. Pruss.
+ <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
+equation 3.5. 1993.
+<a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
+http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- March 15, 2016, by Michael Wetter:<br/>
- Replaced <code>spliceFunction</code> with <code>regStep</code>.
- This is for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
- </li>
- <li>
- August 19, 2015 by Michael Wetter:<br/>
- Changed <code>smoothOrder</code> from <i>5</i> to <i>1</i> as
- <a href=\"modelica://AixLib.Utilities.Math.Functions.spliceFunction\">
- AixLib.Utilities.Math.Functions.spliceFunction</a> is only once
- continuously differentiable.
- Inlined the function.
- </li>
- <li>
- November 20, 2013 by Michael Wetter:<br/>
- First implementation, moved from <code>AixLib.Media</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 15, 2016, by Michael Wetter:<br/>
+Replaced <code>spliceFunction</code> with <code>regStep</code>.
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/300\">issue 300</a>.
+</li>
+<li>
+August 19, 2015 by Michael Wetter:<br/>
+Changed <code>smoothOrder</code> from <i>5</i> to <i>1</i> as
+<a href=\"modelica://AixLib.Utilities.Math.Functions.spliceFunction\">
+AixLib.Utilities.Math.Functions.spliceFunction</a> is only once
+continuously differentiable.
+Inlined the function.
+</li>
+<li>
+November 20, 2013 by Michael Wetter:<br/>
+First implementation, moved from <code>AixLib.Media</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end saturationPressure;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/saturationPressureLiquid.mo b/AixLib/Utilities/Psychrometrics/Functions/saturationPressureLiquid.mo
index 0e1ec8beac..e4ea93204b 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/saturationPressureLiquid.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/saturationPressureLiquid.mo
@@ -14,27 +14,27 @@ algorithm
     derivative=AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_saturationPressureLiquid,
     Inline=true,
     Documentation(info="<html>
- <p>
- Saturation pressure of water above the triple point temperature computed from temperature
- according to Wagner <i>et al.</i> (1993). The range of validity is between
- <i>273.16</i> and <i>373.16</i> Kelvin.
- </p>
- <h4>References</h4>
- <p>
- Wagner W., A. Saul, A. Pruss.
-  <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
- equation 3.5. 1993.
- <a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
- http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
- </p>
- </html>",
+<p>
+Saturation pressure of water above the triple point temperature computed from temperature
+according to Wagner <i>et al.</i> (1993). The range of validity is between
+<i>273.16</i> and <i>373.16</i> Kelvin.
+</p>
+<h4>References</h4>
+<p>
+Wagner W., A. Saul, A. Pruss.
+ <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
+equation 3.5. 1993.
+<a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
+http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 20, 2013 by Michael Wetter:<br/>
- First implementation, moved from <code>AixLib.Media</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 20, 2013 by Michael Wetter:<br/>
+First implementation, moved from <code>AixLib.Media</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end saturationPressureLiquid;
diff --git a/AixLib/Utilities/Psychrometrics/Functions/sublimationPressureIce.mo b/AixLib/Utilities/Psychrometrics/Functions/sublimationPressureIce.mo
index 483b199b9d..5c0e4de1bf 100644
--- a/AixLib/Utilities/Psychrometrics/Functions/sublimationPressureIce.mo
+++ b/AixLib/Utilities/Psychrometrics/Functions/sublimationPressureIce.mo
@@ -19,28 +19,28 @@ algorithm
     smoothOrder=5,
     derivative=AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_sublimationPressureIce,
     Documentation(info="<html>
- <p>
- Sublimation pressure of water below the triple point temperature, computed from temperature,
- according to Wagner <i>et al.</i> (1993).
- The range of validity is between
- <i>190</i> and <i>273.16</i> Kelvin.
- </p>
- <h4>References</h4>
- <p>
- Wagner W., A. Saul, A. Pruss.
-  <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
- equation 3.5. 1993.
- <a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
- http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
- </p>
- </html>",
+<p>
+Sublimation pressure of water below the triple point temperature, computed from temperature,
+according to Wagner <i>et al.</i> (1993).
+The range of validity is between
+<i>190</i> and <i>273.16</i> Kelvin.
+</p>
+<h4>References</h4>
+<p>
+Wagner W., A. Saul, A. Pruss.
+ <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
+equation 3.5. 1993.
+<a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
+http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 20, 2013 by Michael Wetter:<br/>
- First implementation, moved from <code>AixLib.Media</code>.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+November 20, 2013 by Michael Wetter:<br/>
+First implementation, moved from <code>AixLib.Media</code>.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end sublimationPressureIce;
diff --git a/AixLib/Utilities/Psychrometrics/Phi_pTX.mo b/AixLib/Utilities/Psychrometrics/Phi_pTX.mo
index ba645bc635..c4b70d37ae 100644
--- a/AixLib/Utilities/Psychrometrics/Phi_pTX.mo
+++ b/AixLib/Utilities/Psychrometrics/Phi_pTX.mo
@@ -32,23 +32,23 @@ equation
   annotation (
   defaultComponentName="phi",
     Documentation(info="<html>
- <p>
- Block to compute the relative humidity of air for given
- pressure, temperature and water vapor mass fraction.
- </p>
- <p>
- Note that the water vapor mass fraction must be in <i>kg/kg</i>
- total air, and not dry air.
- </p>
- </html>",
+<p>
+Block to compute the relative humidity of air for given
+pressure, temperature and water vapor mass fraction.
+</p>
+<p>
+Note that the water vapor mass fraction must be in <i>kg/kg</i>
+total air, and not dry air.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 13, 2014, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+November 13, 2014, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,100}}),
                     graphics={
         Polygon(
@@ -86,6 +86,6 @@ revisions="<html>
           textColor={0,0,0},
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid,
-          textString="phi")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="phi")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end Phi_pTX;
diff --git a/AixLib/Utilities/Psychrometrics/SaturationPressure.mo b/AixLib/Utilities/Psychrometrics/SaturationPressure.mo
index afdb9fa221..a2b8e52b52 100644
--- a/AixLib/Utilities/Psychrometrics/SaturationPressure.mo
+++ b/AixLib/Utilities/Psychrometrics/SaturationPressure.mo
@@ -17,29 +17,29 @@ equation
     annotation (
     defaultComponentName="pSat",
     Documentation(info="<html>
- <p>
- Saturation pressure of water, computed from temperature,
- according to Wagner <i>et al.</i> (1993).
- The range of validity is between
- <i>190</i> and <i>373.16</i> Kelvin.
- </p>
- <h4>References</h4>
- <p>
- Wagner W., A. Saul, A. Pruss.
-  <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
- equation 3.5. 1993.
- <a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
- http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
- </p>
- </html>",
+<p>
+Saturation pressure of water, computed from temperature,
+according to Wagner <i>et al.</i> (1993).
+The range of validity is between
+<i>190</i> and <i>373.16</i> Kelvin.
+</p>
+<h4>References</h4>
+<p>
+Wagner W., A. Saul, A. Pruss.
+ <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
+equation 3.5. 1993.
+<a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
+http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 20, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+November 20, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-92,22},{-56,-24}},
@@ -101,6 +101,6 @@ revisions="<html>
           lineColor={0,0,255},
           smooth=Smooth.Bezier,
           fillPattern=FillPattern.Solid,
-          fillColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SaturationPressure;
diff --git a/AixLib/Utilities/Psychrometrics/SaturationPressureLiquid.mo b/AixLib/Utilities/Psychrometrics/SaturationPressureLiquid.mo
index 50a45131b2..7a49992fc3 100644
--- a/AixLib/Utilities/Psychrometrics/SaturationPressureLiquid.mo
+++ b/AixLib/Utilities/Psychrometrics/SaturationPressureLiquid.mo
@@ -18,28 +18,28 @@ equation
     annotation (
     defaultComponentName="pSat",
     Documentation(info="<html>
- <p>
- Saturation pressure of water above the triple point temperature computed from temperature
- according to Wagner <i>et al.</i> (1993). The range of validity is between
- <i>273.16</i> and <i>373.16</i> Kelvin.
- </p>
- <h4>References</h4>
- <p>
- Wagner W., A. Saul, A. Pruss.
-  <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
- equation 3.5. 1993.
- <a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
- http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
- </p>
- </html>",
+<p>
+Saturation pressure of water above the triple point temperature computed from temperature
+according to Wagner <i>et al.</i> (1993). The range of validity is between
+<i>273.16</i> and <i>373.16</i> Kelvin.
+</p>
+<h4>References</h4>
+<p>
+Wagner W., A. Saul, A. Pruss.
+ <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
+equation 3.5. 1993.
+<a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
+http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 20, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+November 20, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-92,22},{-56,-24}},
@@ -101,6 +101,6 @@ revisions="<html>
           lineColor={0,0,255},
           smooth=Smooth.Bezier,
           fillPattern=FillPattern.Solid,
-          fillColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SaturationPressureLiquid;
diff --git a/AixLib/Utilities/Psychrometrics/SublimationPressureIce.mo b/AixLib/Utilities/Psychrometrics/SublimationPressureIce.mo
index 46f8d64372..ed427c2a2f 100644
--- a/AixLib/Utilities/Psychrometrics/SublimationPressureIce.mo
+++ b/AixLib/Utilities/Psychrometrics/SublimationPressureIce.mo
@@ -17,29 +17,29 @@ equation
     annotation (
     defaultComponentName="pSat",
     Documentation(info="<html>
- <p>
- Sublimation pressure of water below the triple point temperature, computed from temperature,
- according to Wagner <i>et al.</i> (1993).
- The range of validity is between
- <i>190</i> and <i>273.16</i> Kelvin.
- </p>
- <h4>References</h4>
- <p>
- Wagner W., A. Saul, A. Pruss.
-  <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
- equation 3.5. 1993.
- <a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
- http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
- </p>
- </html>",
+<p>
+Sublimation pressure of water below the triple point temperature, computed from temperature,
+according to Wagner <i>et al.</i> (1993).
+The range of validity is between
+<i>190</i> and <i>273.16</i> Kelvin.
+</p>
+<h4>References</h4>
+<p>
+Wagner W., A. Saul, A. Pruss.
+ <i>International equations for the pressure along the melting and along the sublimation curve of ordinary water substance</i>,
+equation 3.5. 1993.
+<a href=\"http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf\">
+http://aip.scitation.org/doi/pdf/10.1063/1.555947?class=pdf</a>.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 20, 2013, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<ul>
+<li>
+November 20, 2013, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-92,22},{-56,-24}},
@@ -101,6 +101,6 @@ revisions="<html>
           lineColor={0,0,255},
           smooth=Smooth.Bezier,
           fillPattern=FillPattern.Solid,
-          fillColor={0,0,255})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          fillColor={0,0,255})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end SublimationPressureIce;
diff --git a/AixLib/Utilities/Psychrometrics/TDewPoi_pW.mo b/AixLib/Utilities/Psychrometrics/TDewPoi_pW.mo
index d94d40bfd8..19cd1dd1f6 100644
--- a/AixLib/Utilities/Psychrometrics/TDewPoi_pW.mo
+++ b/AixLib/Utilities/Psychrometrics/TDewPoi_pW.mo
@@ -20,30 +20,30 @@ equation
     annotation (
     defaultComponentName="dewPoi",
     Documentation(info="<html>
- <p>
- Dew point temperature calculation for moist air above freezing temperature.
- </p>
- <p>
- The correlation used in this model is valid for dew point temperatures between
- <i>0</i>&deg;C and <i>200</i>&deg;C. It is the correlation from 2005
- ASHRAE Handbook, p. 6.2. In an earlier version of this model, the equation from
- Peppers has been used, but this equation yielded about <i>15</i> Kelvin lower dew point
- temperatures.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 4, 2008 by Michael Wetter:<br/>
- Changed from causal to acausal ports, needed, for example, for
- <a href=\"modelica://AixLib.Fluid.Examples.MixingVolumeMoistAir\">
- AixLib.Fluid.Examples.MixingVolumeMoistAir</a>.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Dew point temperature calculation for moist air above freezing temperature.
+</p>
+<p>
+The correlation used in this model is valid for dew point temperatures between
+<i>0</i>&deg;C and <i>200</i>&deg;C. It is the correlation from 2005
+ASHRAE Handbook, p. 6.2. In an earlier version of this model, the equation from
+Peppers has been used, but this equation yielded about <i>15</i> Kelvin lower dew point
+temperatures.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 4, 2008 by Michael Wetter:<br/>
+Changed from causal to acausal ports, needed, for example, for
+<a href=\"modelica://AixLib.Fluid.Examples.MixingVolumeMoistAir\">
+AixLib.Fluid.Examples.MixingVolumeMoistAir</a>.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={
         Rectangle(
@@ -97,6 +97,6 @@ equation
         Line(points={{68,-44},{-62,-44}}, color={175,175,175}),
         Line(points={{68,-18},{-10,-18}}, color={175,175,175}),
         Line(points={{70,6},{12,6}}, color={175,175,175}),
-        Line(points={{68,32},{22,32}}, color={175,175,175})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        Line(points={{68,32},{22,32}}, color={175,175,175})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end TDewPoi_pW;
diff --git a/AixLib/Utilities/Psychrometrics/TWetBul_TDryBulPhi.mo b/AixLib/Utilities/Psychrometrics/TWetBul_TDryBulPhi.mo
index 43f2dde70f..15e3f6893b 100644
--- a/AixLib/Utilities/Psychrometrics/TWetBul_TDryBulPhi.mo
+++ b/AixLib/Utilities/Psychrometrics/TWetBul_TDryBulPhi.mo
@@ -25,13 +25,18 @@ block TWetBul_TDryBulPhi
     annotation (Placement(transformation(extent={{-120,-90},{-100,-70}})));
 
   Modelica.Blocks.Interfaces.RealOutput TWetBul(
-    start=Medium.T_default-2,
+    start=Medium.T_default,
     final quantity="ThermodynamicTemperature",
     final unit="K",
     min=0) "Wet bulb temperature"
     annotation (Placement(transformation(extent={{100,-10},{120,10}})));
 
+  // Modelica.Math.atan returns a value with unit set to "rad".
+  // The following constant is used to satisfy the unit check.
 protected
+  constant Real uniCon1(final unit="1/rad") = 1 "Constant to satisfy unit check";
+  constant Real uniConK(final unit="K/rad") = 1 "Constant to satisfy unit check";
+
   Modelica.Units.NonSI.Temperature_degC TDryBul_degC
     "Dry bulb temperature in degree Celsius";
   Real rh_per(min=0) "Relative humidity in percentage";
@@ -46,11 +51,12 @@ equation
   if approximateWetBulb then
     TDryBul_degC = TDryBul - 273.15;
     rh_per       = 100*phi;
-    TWetBul      = 273.15 + TDryBul_degC
+    TWetBul      = 273.15 + uniCon1 * TDryBul_degC
        * Modelica.Math.atan(0.151977 * sqrt(rh_per + 8.313659))
-       + Modelica.Math.atan(TDryBul_degC + rh_per)
-       - Modelica.Math.atan(rh_per-1.676331)
-       + 0.00391838 * rh_per^(1.5) * Modelica.Math.atan( 0.023101 * rh_per)  - 4.686035;
+       + uniConK * (Modelica.Math.atan(TDryBul_degC + rh_per)
+         - Modelica.Math.atan(rh_per-1.676331)
+         + 0.00391838 * rh_per^(1.5) * Modelica.Math.atan( 0.023101 * rh_per))
+       - 4.686035;
     XiSat    = 0;
     XiDryBul = 0;
     XiSatRefIn=0;
@@ -130,74 +136,86 @@ annotation (
           fillPattern=FillPattern.Solid)}),
     defaultComponentName="wetBul",
     Documentation(info="<html>
- <p>
- This block computes the wet bulb temperature for a given dry bulb temperature, relative air humidity
- and atmospheric pressure.
- </p>
- <p>
- If the constant <code>approximateWetBulb</code> is <code>true</code>,
- then the block uses the approximation of Stull (2011) to compute
- the wet bulb temperature without requiring a nonlinear equation.
- Otherwise, the model will introduce one nonlinear equation.
- The approximation by Stull is valid for a relative humidity of <i>5%</i> to <i>99%</i>,
- a temperature range from <i>-20</i>&deg;C to <i>50</i>&deg;C
- and standard sea level pressure.
- For this range of data, the approximation error is <i>-1</i> Kelvin to <i>+0.65</i> Kelvin,
- with a mean error of less than <i>0.3</i> Kelvin.
- </p>
- <p>
- Otherwise a calculation based on an energy balance is used.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a> for a discussion.
- The model is validated in
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Examples.TWetBul_TDryBulPhi\">
- AixLib.Utilities.Psychrometrics.Examples.TWetBul_TDryBulPhi</a>.
- </p>
- <p>
- For a model that takes the mass fraction instead of the relative humidity as an input, see
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.TWetBul_TDryBulXi\">
- AixLib.Utilities.Psychrometrics.TWetBul_TDryBulXi</a>.
- </p>
- <h4>References</h4>
- <p>
- Stull, Roland.
- <i><a href=\"http://dx.doi.org/10.1175/JAMC-D-11-0143.1\">
- Wet-Bulb Temperature from Relative Humidity and Air Temperature
- Roland Stull.</a></i>
- Journal of Applied Meteorology and Climatology.
- Volume 50, Issue 11, pp. 2267-2269. November 2011
- DOI: 10.1175/JAMC-D-11-0143.1
- </p>
- </html>",
+<p>
+This block computes the wet bulb temperature for a given dry bulb temperature, relative air humidity
+and atmospheric pressure.
+</p>
+<p>
+If the constant <code>approximateWetBulb</code> is <code>true</code>,
+then the block uses the approximation of Stull (2011) to compute
+the wet bulb temperature without requiring a nonlinear equation.
+Otherwise, the model will introduce one nonlinear equation.
+The approximation by Stull is valid for a relative humidity of <i>5%</i> to <i>99%</i>,
+a temperature range from <i>-20</i>&deg;C to <i>50</i>&deg;C
+and standard sea level pressure.
+For this range of data, the approximation error is <i>-1</i> Kelvin to <i>+0.65</i> Kelvin,
+with a mean error of less than <i>0.3</i> Kelvin.
+</p>
+<p>
+Otherwise a calculation based on an energy balance is used.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a> for a discussion.
+The model is validated in
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Examples.TWetBul_TDryBulPhi\">
+AixLib.Utilities.Psychrometrics.Examples.TWetBul_TDryBulPhi</a>.
+</p>
+<p>
+For a model that takes the mass fraction instead of the relative humidity as an input, see
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.TWetBul_TDryBulXi\">
+AixLib.Utilities.Psychrometrics.TWetBul_TDryBulXi</a>.
+</p>
+<h4>References</h4>
+<p>
+Stull, Roland.
+<i><a href=\"http://dx.doi.org/10.1175/JAMC-D-11-0143.1\">
+Wet-Bulb Temperature from Relative Humidity and Air Temperature
+Roland Stull.</a></i>
+Journal of Applied Meteorology and Climatology.
+Volume 50, Issue 11, pp. 2267-2269. November 2011
+DOI: 10.1175/JAMC-D-11-0143.1
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Changed icon.
- </li>
- <li>
- May 24, 2016, by Filip Jorissen:<br/>
- Corrected exact implementation.
- See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a>
- for a discussion.
- </li>
- <li>
- October 3, 2014, by Michael Wetter:<br/>
- Changed assignment of nominal value to avoid in OpenModelica the warning
- alias set with different nominal values.
- </li>
- <li>
- November 20, 2013 by Michael Wetter:<br/>
- Updated model to use
- <code>AixLib.Utilities.Psychrometrics.Functions.saturationPressure()</code>
- and
- <code>AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid()</code>
- as these functions have been moved from the medium to the psychrometrics package.
- </li>
- <li>
- October 1, 2012 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+June 18, 2024, by Michael Wetter:<br/>
+Added <code>start</code> and <code>nominal</code> attributes
+to avoid warnings in OpenModelica due to conflicting values.<br/>
+This is for <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1890\">IBPSA, #1890</a>.
+</li>
+<li>
+March 6, 2023, by Michael Wetter:<br/>
+Added a constant in order for unit check to pass.<br/>
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1711\">#1711</a>
+for a discussion.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Changed icon.
+</li>
+<li>
+May 24, 2016, by Filip Jorissen:<br/>
+Corrected exact implementation.
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a>
+for a discussion.
+</li>
+<li>
+October 3, 2014, by Michael Wetter:<br/>
+Changed assignment of nominal value to avoid in OpenModelica the warning
+alias set with different nominal values.
+</li>
+<li>
+November 20, 2013 by Michael Wetter:<br/>
+Updated model to use
+<code>AixLib.Utilities.Psychrometrics.Functions.saturationPressure()</code>
+and
+<code>AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid()</code>
+as these functions have been moved from the medium to the psychrometrics package.
+</li>
+<li>
+October 1, 2012 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TWetBul_TDryBulPhi;
diff --git a/AixLib/Utilities/Psychrometrics/TWetBul_TDryBulXi.mo b/AixLib/Utilities/Psychrometrics/TWetBul_TDryBulXi.mo
index ca1f329955..84c55f4fd8 100644
--- a/AixLib/Utilities/Psychrometrics/TWetBul_TDryBulXi.mo
+++ b/AixLib/Utilities/Psychrometrics/TWetBul_TDryBulXi.mo
@@ -31,6 +31,9 @@ block TWetBul_TDryBulXi
     annotation (Placement(transformation(extent={{-120,-10},{-100,10}})));
 
 protected
+  constant Real uniCon1(final unit="1/rad") = 1 "Constant to satisfy unit check";
+  constant Real uniConK(final unit="K/rad") = 1 "Constant to satisfy unit check";
+
   Modelica.Units.NonSI.Temperature_degC TDryBul_degC
     "Dry bulb temperature in degree Celsius";
   Real rh_per(min=0) "Relative humidity in percentage";
@@ -55,11 +58,12 @@ equation
          AixLib.Utilities.Psychrometrics.Functions.saturationPressure(TDryBul)
          *Xi[iWat]/(Xi[iWat] +
          AixLib.Utilities.Psychrometrics.Constants.k_mair*(1-Xi[iWat]));
-    TWetBul      = 273.15 + TDryBul_degC
+    TWetBul      = 273.15 + uniCon1 * TDryBul_degC
        * Modelica.Math.atan(0.151977 * sqrt(rh_per + 8.313659))
-       + Modelica.Math.atan(TDryBul_degC + rh_per)
-       - Modelica.Math.atan(rh_per-1.676331)
-       + 0.00391838 * rh_per^(1.5) * Modelica.Math.atan( 0.023101 * rh_per)  - 4.686035;
+       + uniConK * ( Modelica.Math.atan(TDryBul_degC + rh_per)
+         - Modelica.Math.atan(rh_per-1.676331)
+         + 0.00391838 * rh_per^(1.5) * Modelica.Math.atan( 0.023101 * rh_per))
+       - 4.686035;
     XiSat = 0;
     XiSatRefIn=0;
   else
@@ -133,120 +137,126 @@ annotation (
           fillPattern=FillPattern.Solid)}),
     defaultComponentName="wetBul",
     Documentation(info="<html>
- <p>
- This block computes the wet bulb temperature for a given dry bulb temperature, mass fraction
- and atmospheric pressure.
- </p>
- <p>
- If the constant <code>approximateWetBulb</code> is <code>true</code>,
- then the block uses the approximation of Stull (2011) to compute
- the wet bulb temperature without requiring a nonlinear equation.
- Otherwise, the model will introduce one nonlinear equation.
- The approximation by Stull is valid for a relative humidity of <i>5%</i> to <i>99%</i>,
- a temperature range from <i>-20&deg;C</i> to <i>50&deg;C</i>
- and standard sea level pressure.
- For this range of data, the approximation error is <i>-1</i> Kelvin to <i>+0.65</i> Kelvin,
- with a mean error of less than <i>0.3</i> Kelvin.
- </p>
- <p>
- Otherwise a calculation based on an energy balance is used.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a> for a discussion.
- </p>
- <p>
- For a model that takes the relative humidity instead of the mass fraction as an input, see
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.TWetBul_TDryBulPhi\">
- AixLib.Utilities.Psychrometrics.TWetBul_TDryBulPhi</a>.
- </p>
- <h4>References</h4>
- <p>
- Stull, Roland.
- <i><a href=\"http://dx.doi.org/10.1175/JAMC-D-11-0143.1\">
- Wet-Bulb Temperature from Relative Humidity and Air Temperature
- Roland Stull.</a></i>
- Journal of Applied Meteorology and Climatology.
- Volume 50, Issue 11, pp. 2267-2269. November 2011
- DOI: 10.1175/JAMC-D-11-0143.1
- </p>
- </html>",
+<p>
+This block computes the wet bulb temperature for a given dry bulb temperature, mass fraction
+and atmospheric pressure.
+</p>
+<p>
+If the constant <code>approximateWetBulb</code> is <code>true</code>,
+then the block uses the approximation of Stull (2011) to compute
+the wet bulb temperature without requiring a nonlinear equation.
+Otherwise, the model will introduce one nonlinear equation.
+The approximation by Stull is valid for a relative humidity of <i>5%</i> to <i>99%</i>,
+a temperature range from <i>-20&deg;C</i> to <i>50&deg;C</i>
+and standard sea level pressure.
+For this range of data, the approximation error is <i>-1</i> Kelvin to <i>+0.65</i> Kelvin,
+with a mean error of less than <i>0.3</i> Kelvin.
+</p>
+<p>
+Otherwise a calculation based on an energy balance is used.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a> for a discussion.
+</p>
+<p>
+For a model that takes the relative humidity instead of the mass fraction as an input, see
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.TWetBul_TDryBulPhi\">
+AixLib.Utilities.Psychrometrics.TWetBul_TDryBulPhi</a>.
+</p>
+<h4>References</h4>
+<p>
+Stull, Roland.
+<i><a href=\"http://dx.doi.org/10.1175/JAMC-D-11-0143.1\">
+Wet-Bulb Temperature from Relative Humidity and Air Temperature
+Roland Stull.</a></i>
+Journal of Applied Meteorology and Climatology.
+Volume 50, Issue 11, pp. 2267-2269. November 2011
+DOI: 10.1175/JAMC-D-11-0143.1
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- May 1, 2017, by Filip Jorissen:<br/>
- Revised computation of <code>iWat</code>
- such that it does not require an initial algorithm.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/759\">#759</a>.
- </li>
- <li>
- November 3, 2016, by Michael Wetter:<br/>
- Changed icon.
- </li>
- <li>
- May 24, 2016, by Filip Jorissen:<br/>
- Corrected exact implementation.
- See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a>
- for a discussion.
- </li>
- <li>
- April 11, 2016 by Michael Wetter:<br/>
- Corrected wrong hyperlink in documentation for
- <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
- </li>
- <li>
- November 17, 2014, by Michael Wetter:<br/>
- Removed test on saturation pressure that avoids it to be larger than
- <code>p</code>.
- This test is not needed as it is only active near or above the boiling temperature,
- and the result is only used in the computation of <code>rh_per</code>.
- I do not see any negative impact from removing this test.
- </li>
- <li>
- July 24, 2014 by Michael Wetter:<br/>
- Revised computation of <code>rh_per</code> to use
- <a href=\"modelica://AixLib.Utilities.Math.Functions.smoothMin\">
- AixLib.Utilities.Math.Functions.smoothMin</a> rather
- than <code>min</code>.
- </li>
- <li>
- November 20, 2013 by Michael Wetter:<br/>
- Updated model to use
- <code>AixLib.Utilities.Psychrometrics.Functions.saturationPressure()</code>
- and
- <code>AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid()</code>
- as these functions have been moved from the medium to the psychrometrics package.
- </li>
- <li>
- September 10, 2013 by Michael Wetter:<br/>
- Added start value and nominal value for <code>XiSat</code> as this is an iteration
- variable in OpenModelica.
- </li>
- <li>
- October 1, 2012 by Michael Wetter:<br/>
- Revised implementation to change the dimension of the nonlinear
- system of equations from two to one.
- Added option to compute wet bulb temperature explicitly.
- </li>
- <li>
- February 22, 2011 by Michael Wetter:<br/>
- Changed the code sections that obtain the water concentration. The old version accessed
- the water concentration using the index of the vector <code>X</code>.
- However, Dymola 7.4 cannot differentiate the function if vector elements are accessed
- using their index. In the new implementation, an inner product is used to access the vector element.
- In addition, the medium substance name is searched using a case insensitive search.
- </li>
- <li>
- February 17, 2010 by Michael Wetter:<br/>
- Renamed block from <code>WetBulbTemperature</code> to <code>TWetBul_TDryBulXi</code>
- and changed obsolete real connectors to input and output connectors.
- </li>
- <li>
- May 19, 2008 by Michael Wetter:<br/>
- Added relative humidity as a port.
- </li>
- <li>
- May 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 6, 2023, by Michael Wetter:<br/>
+Added a constant in order for unit check to pass.<br/>
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1711\">#1711</a>
+for a discussion.
+</li>
+<li>
+May 1, 2017, by Filip Jorissen:<br/>
+Revised computation of <code>iWat</code>
+such that it does not require an initial algorithm.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/759\">#759</a>.
+</li>
+<li>
+November 3, 2016, by Michael Wetter:<br/>
+Changed icon.
+</li>
+<li>
+May 24, 2016, by Filip Jorissen:<br/>
+Corrected exact implementation.
+See  <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/474\">#474</a>
+for a discussion.
+</li>
+<li>
+April 11, 2016 by Michael Wetter:<br/>
+Corrected wrong hyperlink in documentation for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/450\">issue 450</a>.
+</li>
+<li>
+November 17, 2014, by Michael Wetter:<br/>
+Removed test on saturation pressure that avoids it to be larger than
+<code>p</code>.
+This test is not needed as it is only active near or above the boiling temperature,
+and the result is only used in the computation of <code>rh_per</code>.
+I do not see any negative impact from removing this test.
+</li>
+<li>
+July 24, 2014 by Michael Wetter:<br/>
+Revised computation of <code>rh_per</code> to use
+<a href=\"modelica://AixLib.Utilities.Math.Functions.smoothMin\">
+AixLib.Utilities.Math.Functions.smoothMin</a> rather
+than <code>min</code>.
+</li>
+<li>
+November 20, 2013 by Michael Wetter:<br/>
+Updated model to use
+<code>AixLib.Utilities.Psychrometrics.Functions.saturationPressure()</code>
+and
+<code>AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid()</code>
+as these functions have been moved from the medium to the psychrometrics package.
+</li>
+<li>
+September 10, 2013 by Michael Wetter:<br/>
+Added start value and nominal value for <code>XiSat</code> as this is an iteration
+variable in OpenModelica.
+</li>
+<li>
+October 1, 2012 by Michael Wetter:<br/>
+Revised implementation to change the dimension of the nonlinear
+system of equations from two to one.
+Added option to compute wet bulb temperature explicitly.
+</li>
+<li>
+February 22, 2011 by Michael Wetter:<br/>
+Changed the code sections that obtain the water concentration. The old version accessed
+the water concentration using the index of the vector <code>X</code>.
+However, Dymola 7.4 cannot differentiate the function if vector elements are accessed
+using their index. In the new implementation, an inner product is used to access the vector element.
+In addition, the medium substance name is searched using a case insensitive search.
+</li>
+<li>
+February 17, 2010 by Michael Wetter:<br/>
+Renamed block from <code>WetBulbTemperature</code> to <code>TWetBul_TDryBulXi</code>
+and changed obsolete real connectors to input and output connectors.
+</li>
+<li>
+May 19, 2008 by Michael Wetter:<br/>
+Added relative humidity as a port.
+</li>
+<li>
+May 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end TWetBul_TDryBulXi;
diff --git a/AixLib/Utilities/Psychrometrics/ToDryAir.mo b/AixLib/Utilities/Psychrometrics/ToDryAir.mo
index 6aad4d25f3..b3a64bfe18 100644
--- a/AixLib/Utilities/Psychrometrics/ToDryAir.mo
+++ b/AixLib/Utilities/Psychrometrics/ToDryAir.mo
@@ -14,17 +14,17 @@ equation
     annotation (
     defaultComponentName="toDryAir",
     Documentation(info="<html>
- <p>
- Block that converts humidity concentration from [kg/kg total air] to [kg/kg dry air].
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 10, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block that converts humidity concentration from [kg/kg total air] to [kg/kg dry air].
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 10, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=true,  extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{34,30},{86,-34}},
@@ -36,6 +36,6 @@ equation
           textColor={0,0,0},
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid,
-          textString="XiTotal")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="XiTotal")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ToDryAir;
diff --git a/AixLib/Utilities/Psychrometrics/ToTotalAir.mo b/AixLib/Utilities/Psychrometrics/ToTotalAir.mo
index da7818e8ed..b6958d6102 100644
--- a/AixLib/Utilities/Psychrometrics/ToTotalAir.mo
+++ b/AixLib/Utilities/Psychrometrics/ToTotalAir.mo
@@ -18,21 +18,21 @@ equation
     annotation (
     defaultComponentName="toTotAir",
     Documentation(info="<html>
- <p>
- Block that converts humidity concentration from [kg/kg dry air] to [kg/kg total air].
- </p>
- <p>
- This block may be used, for example, to convert absolute humidity that is received from
- EnergyPlus to [kg/kg total air], which is the convention used by Modelica.Media.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 10, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block that converts humidity concentration from [kg/kg dry air] to [kg/kg total air].
+</p>
+<p>
+This block may be used, for example, to convert absolute humidity that is received from
+EnergyPlus to [kg/kg total air], which is the convention used by Modelica.Media.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 10, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={Text(
           extent={{-88,32},{-36,-32}},
@@ -44,6 +44,6 @@ equation
           textColor={0,0,0},
           fillColor={0,0,0},
           fillPattern=FillPattern.Solid,
-          textString="XiTotal")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="XiTotal")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ToTotalAir;
diff --git a/AixLib/Utilities/Psychrometrics/X_pTphi.mo b/AixLib/Utilities/Psychrometrics/X_pTphi.mo
index be80396e92..0041d2cf76 100644
--- a/AixLib/Utilities/Psychrometrics/X_pTphi.mo
+++ b/AixLib/Utilities/Psychrometrics/X_pTphi.mo
@@ -41,48 +41,48 @@ equation
   //sum(X[:]) = 1; // The formulation with a sum in an equation section leads to a nonlinear equation system
   X[i_nw] =  1 - X[i_w];
   annotation (Documentation(info="<html>
- <p>
- Block to compute the water vapor concentration based on
- pressure, temperature and relative humidity.
- </p>
- <p>
- If <code>use_p_in</code> is false (default option), the <code>p</code> parameter
- is used as atmospheric pressure,
- and the <code>p_in</code> input connector is disabled;
- if <code>use_p_in</code> is true, then the <code>p</code> parameter is ignored,
- and the value provided by the input connector is used instead.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>November 3, 2017 by Filip Jorissen:<br/>
- Converted (initial) algorithm section into (initial) equation section.
- See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/847\">#847</a>.
- </li>
- <li>July 24, 2014 by Michael Wetter:<br/>
- Added <code>assert</code> to verify that <code>Medium.nX==2</code>
- as the implementation is only valid for such media.
- </li>
- <li>April 26, 2013 by Michael Wetter:<br/>
- Set the medium model to <code>AixLib.Media.Air</code>.
- This was required to allow a pedantic model check in Dymola 2014.
- </li>
- <li>August 21, 2012 by Michael Wetter:<br/>
- Added function call to compute water vapor content.
- </li>
- <li>
- February 22, 2010 by Michael Wetter:<br/>
- Improved the code that searches for the index of 'water' in the medium model.
- </li>
- <li>
- February 17, 2010 by Michael Wetter:<br/>
- Renamed block from <code>MassFraction_pTphi</code> to <code>X_pTphi</code>
- </li>
- <li>
- February 4, 2009 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),Icon(graphics={
+<p>
+Block to compute the water vapor concentration based on
+pressure, temperature and relative humidity.
+</p>
+<p>
+If <code>use_p_in</code> is false (default option), the <code>p</code> parameter
+is used as atmospheric pressure,
+and the <code>p_in</code> input connector is disabled;
+if <code>use_p_in</code> is true, then the <code>p</code> parameter is ignored,
+and the value provided by the input connector is used instead.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>November 3, 2017 by Filip Jorissen:<br/>
+Converted (initial) algorithm section into (initial) equation section.
+See <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/847\">#847</a>.
+</li>
+<li>July 24, 2014 by Michael Wetter:<br/>
+Added <code>assert</code> to verify that <code>Medium.nX==2</code>
+as the implementation is only valid for such media.
+</li>
+<li>April 26, 2013 by Michael Wetter:<br/>
+Set the medium model to <code>AixLib.Media.Air</code>.
+This was required to allow a pedantic model check in Dymola 2014.
+</li>
+<li>August 21, 2012 by Michael Wetter:<br/>
+Added function call to compute water vapor content.
+</li>
+<li>
+February 22, 2010 by Michael Wetter:<br/>
+Improved the code that searches for the index of 'water' in the medium model.
+</li>
+<li>
+February 17, 2010 by Michael Wetter:<br/>
+Renamed block from <code>MassFraction_pTphi</code> to <code>X_pTphi</code>
+</li>
+<li>
+February 4, 2009 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"), Icon(graphics={
         Text(
           extent={{-96,16},{-54,-22}},
           textColor={0,0,0},
@@ -94,6 +94,6 @@ equation
         Text(
           extent={{26,56},{90,-54}},
           textColor={0,0,0},
-          textString="X_steam")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="X_steam")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end X_pTphi;
diff --git a/AixLib/Utilities/Psychrometrics/X_pW.mo b/AixLib/Utilities/Psychrometrics/X_pW.mo
index 76c84a77d6..4705de9fc8 100644
--- a/AixLib/Utilities/Psychrometrics/X_pW.mo
+++ b/AixLib/Utilities/Psychrometrics/X_pW.mo
@@ -23,41 +23,41 @@ equation
   annotation (
 defaultComponentName="humRat",
     Documentation(info="<html>
- <p>
- Block to compute the humidity ratio for a given water vapor partial pressure.
- </p>
- <p>If <code>use_p_in</code> is false (default option), the <code>p</code> parameter
- is used as atmospheric pressure,
- and the <code>p_in</code> input connector is disabled;
- if <code>use_p_in</code> is true, then the <code>p</code> parameter is ignored,
- and the value provided by the input connector is used instead.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 16, 2013 by Michael Wetter:<br/>
- Added attributes to variable <code>p_w</code>.
- </li>
- <li>
- February 17, 2010 by Michael Wetter:<br/>
- Renamed block from <code>HumidityRatio_pWat</code> to <code>X_pW</code>.
- </li>
- <li>
- April 14, 2009 by Michael Wetter:<br/>
- Converted model to block because <code>RealInput</code> are obsolete in Modelica 3.0.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block to compute the humidity ratio for a given water vapor partial pressure.
+</p>
+<p>If <code>use_p_in</code> is false (default option), the <code>p</code> parameter
+is used as atmospheric pressure,
+and the <code>p_in</code> input connector is disabled;
+if <code>use_p_in</code> is true, then the <code>p</code> parameter is ignored,
+and the value provided by the input connector is used instead.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+September 16, 2013 by Michael Wetter:<br/>
+Added attributes to variable <code>p_w</code>.
+</li>
+<li>
+February 17, 2010 by Michael Wetter:<br/>
+Renamed block from <code>HumidityRatio_pWat</code> to <code>X_pW</code>.
+</li>
+<li>
+April 14, 2009 by Michael Wetter:<br/>
+Converted model to block because <code>RealInput</code> are obsolete in Modelica 3.0.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={Text(
           extent={{-92,52},{-36,-40}},
           textColor={0,0,0},
           textString="pW"), Text(
           extent={{46,44},{94,-24}},
           textColor={0,0,0},
-          textString="X")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="X")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end X_pW;
diff --git a/AixLib/Utilities/Psychrometrics/hSat_pTSat.mo b/AixLib/Utilities/Psychrometrics/hSat_pTSat.mo
index 90febf10f2..f9697a26ae 100644
--- a/AixLib/Utilities/Psychrometrics/hSat_pTSat.mo
+++ b/AixLib/Utilities/Psychrometrics/hSat_pTSat.mo
@@ -45,17 +45,17 @@ equation
   annotation (Icon(coordinateSystem(preserveAspectRatio=false)), Diagram(
         coordinateSystem(preserveAspectRatio=false)),
     Documentation(revisions="<html>
- <ul>
- <li>
- March 17, 2017, by Michael O'Keefe:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- Block to compute the enthalpy of saturated
- air given the saturation temperature and fluid pressure.
- </p>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+March 17, 2017, by Michael O'Keefe:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+Block to compute the enthalpy of saturated
+air given the saturation temperature and fluid pressure.
+</p>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end hSat_pTSat;
diff --git a/AixLib/Utilities/Psychrometrics/pW_TDewPoi.mo b/AixLib/Utilities/Psychrometrics/pW_TDewPoi.mo
index d7d9709081..26b01e108e 100644
--- a/AixLib/Utilities/Psychrometrics/pW_TDewPoi.mo
+++ b/AixLib/Utilities/Psychrometrics/pW_TDewPoi.mo
@@ -16,49 +16,49 @@ equation
     annotation (
     defaultComponentName="pWat",
     Documentation(info="<html>
- <p>
- Block to compute the water vapor pressure for a given dew point temperature.
- </p>
- <p>
- The correlation used in this model is valid for dew point temperatures between
- <i>0</i>&deg;C and <i>30</i>&deg;C. It is an approximation to the correlation from 2005
- ASHRAE Handbook, p. 6.2, which is valid in a wider range of temperatures and implemented
- in
- <a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi\">
- AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi</a>.
- The approximation error of this simplified function is below 5% for a
- temperature of <i>0</i>&deg;C to <i>30</i>&deg;C.
- The benefit of this simpler function is that it can be inverted analytically,
- whereas the other function requires a numerical solution.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- December 7, 2011 by Michael Wetter:<br/>
- Changed function call from
- <code>p_w = AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi(T=T);</code>
- to
- <code>p_w = AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi_amb(T=T);</code>
- as the first version sometimes triggered warnings when the solver attempts negative
- temperatures. The accuracy of the two implementation does not change much in the
- region of interest for building HVAC applications.
- </li>
- <li>February 17, 2010 by Michael Wetter:<br/>
- Renamed block from <code>DewPointTemperature_pWat</code>
- to <code>pW_TDewPoi</code>.
- </li>
- <li>
- September 4, 2008 by Michael Wetter:<br/>
- Changed from causal to acausal ports, needed, for example, for
- <a href=\"modelica://AixLib.Fluid.Examples.MixingVolumeMoistAir\">
- AixLib.Fluid.Examples.MixingVolumeMoistAir</a>.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block to compute the water vapor pressure for a given dew point temperature.
+</p>
+<p>
+The correlation used in this model is valid for dew point temperatures between
+<i>0</i>&deg;C and <i>30</i>&deg;C. It is an approximation to the correlation from 2005
+ASHRAE Handbook, p. 6.2, which is valid in a wider range of temperatures and implemented
+in
+<a href=\"modelica://AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi\">
+AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi</a>.
+The approximation error of this simplified function is below 5% for a
+temperature of <i>0</i>&deg;C to <i>30</i>&deg;C.
+The benefit of this simpler function is that it can be inverted analytically,
+whereas the other function requires a numerical solution.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+December 7, 2011 by Michael Wetter:<br/>
+Changed function call from
+<code>p_w = AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi(T=T);</code>
+to
+<code>p_w = AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi_amb(T=T);</code>
+as the first version sometimes triggered warnings when the solver attempts negative
+temperatures. The accuracy of the two implementation does not change much in the
+region of interest for building HVAC applications.
+</li>
+<li>February 17, 2010 by Michael Wetter:<br/>
+Renamed block from <code>DewPointTemperature_pWat</code>
+to <code>pW_TDewPoi</code>.
+</li>
+<li>
+September 4, 2008 by Michael Wetter:<br/>
+Changed from causal to acausal ports, needed, for example, for
+<a href=\"modelica://AixLib.Fluid.Examples.MixingVolumeMoistAir\">
+AixLib.Fluid.Examples.MixingVolumeMoistAir</a>.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(coordinateSystem(preserveAspectRatio=false, extent={{-100,-100},{100,
             100}}), graphics={
         Rectangle(
@@ -112,6 +112,6 @@ equation
         Line(points={{68,-44},{-62,-44}}, color={175,175,175}),
         Line(points={{68,-18},{-10,-18}}, color={175,175,175}),
         Line(points={{70,6},{12,6}}, color={175,175,175}),
-        Line(points={{68,32},{22,32}}, color={175,175,175})}),
-  __Dymola_LockedEditing="Model from IBPSA");
+        Line(points={{68,32},{22,32}}, color={175,175,175})}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end pW_TDewPoi;
diff --git a/AixLib/Utilities/Psychrometrics/pW_X.mo b/AixLib/Utilities/Psychrometrics/pW_X.mo
index e066ce7dfa..548adbf39c 100644
--- a/AixLib/Utilities/Psychrometrics/pW_X.mo
+++ b/AixLib/Utilities/Psychrometrics/pW_X.mo
@@ -23,42 +23,42 @@ equation
   annotation (
     defaultComponentName="pWat",
     Documentation(info="<html>
- <p>
- Block to compute the water vapor partial pressure for a given humidity ratio.
- </p>
- <p>If <code>use_p_in</code> is false (default option), the <code>p</code> parameter
- is used as atmospheric pressure,
- and the <code>p_in</code> input connector is disabled;
- if <code>use_p_in</code> is true, then the <code>p</code> parameter is ignored,
- and the value provided by the input connector is used instead.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- October 3, 2014, by Michael Wetter:<br/>
- Changed assignment of nominal value to avoid in OpenModelica the warning
- alias set with different nominal values.
- </li>
- <li>
- February 17, 2010 by Michael Wetter:<br/>
- Renamed block from <code>VaporPressure_X</code> to <code>pW_X</code>.
- </li>
- <li>
- April 14, 2009 by Michael Wetter:<br/>
- Converted model to block because <code>RealInput</code> are obsolete in Modelica 3.0.
- </li>
- <li>
- August 7, 2008 by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+Block to compute the water vapor partial pressure for a given humidity ratio.
+</p>
+<p>If <code>use_p_in</code> is false (default option), the <code>p</code> parameter
+is used as atmospheric pressure,
+and the <code>p_in</code> input connector is disabled;
+if <code>use_p_in</code> is true, then the <code>p</code> parameter is ignored,
+and the value provided by the input connector is used instead.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+October 3, 2014, by Michael Wetter:<br/>
+Changed assignment of nominal value to avoid in OpenModelica the warning
+alias set with different nominal values.
+</li>
+<li>
+February 17, 2010 by Michael Wetter:<br/>
+Renamed block from <code>VaporPressure_X</code> to <code>pW_X</code>.
+</li>
+<li>
+April 14, 2009 by Michael Wetter:<br/>
+Converted model to block because <code>RealInput</code> are obsolete in Modelica 3.0.
+</li>
+<li>
+August 7, 2008 by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
     Icon(graphics={Text(
           extent={{-88,26},{-60,-26}},
           textColor={0,0,0},
           textString="X"), Text(
           extent={{46,30},{90,-32}},
           textColor={0,0,0},
-          textString="pW")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="pW")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end pW_X;
diff --git a/AixLib/Utilities/Sensors/Examples/ExergyMeters.mo b/AixLib/Utilities/Sensors/Examples/ExergyMeters.mo
index 9ad81b6a68..75e9387e03 100644
--- a/AixLib/Utilities/Sensors/Examples/ExergyMeters.mo
+++ b/AixLib/Utilities/Sensors/Examples/ExergyMeters.mo
@@ -18,7 +18,7 @@ model ExergyMeters
     each offset=3000,
     each amplitude=3000) "Sine wave to vary heat generation and demand"
     annotation (Placement(transformation(extent={{-12,-14},{8,6}})));
-  ExergyMeter.StoredExergyMeter exergyStorageMeterMedium(
+  AixLib.Utilities.Sensors.ExergyMeter.StoredExergyMeter exergyStorageMeterMedium(
     redeclare package Medium = Medium,
     T_ref_start=T_ref.k,
     T_start=T_start,
@@ -36,7 +36,7 @@ model ExergyMeters
   inner Modelica.Fluid.System system(energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial)
                                      "Basic parameters"
     annotation (Placement(transformation(extent={{80,-100},{100,-80}})));
-  ExergyMeter.HeatExergyMeter exHeatSec
+  AixLib.Utilities.Sensors.ExergyMeter.HeatExergyMeter exHeatSec
     "Exergy content of the heat flux on secondary side"
     annotation (Placement(transformation(extent={{74,5},{94,25}})));
   AixLib.Fluid.Movers.FlowControlled_m_flow pumpPrim(
@@ -46,9 +46,10 @@ model ExergyMeters
     redeclare package Medium = Medium,
     T_start=T_start,
     m_flow_nominal=0.5,
-    m_flow_small=0.001)
+    m_flow_small=0.001,
+    dp_nominal=10000 + sum(bufferStorageHeatingcoils.heatingCoil1.pipe.res.dp_nominal))
     annotation (Placement(transformation(extent={{-64,76},{-44,96}})));
-  Fluid.Storage.BufferStorage  bufferStorageHeatingcoils(
+  AixLib.Fluid.Storage.StorageDetailed bufferStorageHeatingcoils(
     energyDynamics=Modelica.Fluid.Types.Dynamics.FixedInitial,
     redeclare package MediumHC1 = Medium,
     redeclare package MediumHC2 = Medium,
@@ -58,7 +59,7 @@ model ExergyMeters
     useHeatingCoil1=true,
     useHeatingCoil2=false,
     useHeatingRod=false,
-    TStart=T_start,
+    TStart=fill(T_start, 10),
     redeclare DataBase.Storage.Generic_New_2000l data(
       hTank=1,
       hUpperPortDemand=0.95,
@@ -77,7 +78,7 @@ model ExergyMeters
     n=10)
          "Storage tank" annotation (Placement(transformation(extent={{-2,54},{26,
             88}})));
-  Fluid.FixedResistances.PressureDrop      pipePrim(
+  AixLib.Fluid.FixedResistances.PressureDrop      pipePrim(
     redeclare package Medium = Medium,
     m_flow_nominal=0.5,
     dp_nominal=10000) "Main resistance in primary circuit"
@@ -85,10 +86,12 @@ model ExergyMeters
         extent={{-7,-7.5},{7,7.5}},
         rotation=180,
         origin={-53,56.5})));
-  ExergyMeter.FlowExergyMeter exPrimIn(redeclare package Medium = Medium)
+  AixLib.Utilities.Sensors.ExergyMeter.FlowExergyMeter exPrimIn(redeclare
+      package Medium =                                                                     Medium)
     "Exergy content of medium flow entering the storage on primary side"
     annotation (Placement(transformation(extent={{-36,76},{-14,96}})));
-  ExergyMeter.FlowExergyMeter exPrimOut(redeclare package Medium = Medium)
+  AixLib.Utilities.Sensors.ExergyMeter.FlowExergyMeter exPrimOut(redeclare
+      package Medium =                                                                      Medium)
     "Exergy content of medium flow exiting the storage on primary side"
     annotation (Placement(transformation(
         extent={{-11,10},{11,-10}},
@@ -112,9 +115,10 @@ model ExergyMeters
     redeclare package Medium = Medium,
     T_start=T_start,
     m_flow_nominal=0.5,
-    m_flow_small=0.001) "Pump in secondary circuit"
+    m_flow_small=0.001,
+    dp_nominal=10000)   "Pump in secondary circuit"
     annotation (Placement(transformation(extent={{60,72},{80,92}})));
-  Fluid.FixedResistances.PressureDrop      pipeSec(
+  AixLib.Fluid.FixedResistances.PressureDrop      pipeSec(
     redeclare package Medium = Medium,
     m_flow_nominal=0.5,
     dp_nominal=10000) "Main resistance in secondary circuit"
@@ -134,10 +138,12 @@ model ExergyMeters
         extent={{10,-10},{-10,10}},
         rotation=270,
         origin={96,70})));
-  ExergyMeter.FlowExergyMeter exSecOut(redeclare package Medium = Medium)
+  AixLib.Utilities.Sensors.ExergyMeter.FlowExergyMeter exSecOut(redeclare
+      package Medium =                                                                     Medium)
     "Exergy content of medium flow entering the storage on secondary side"
     annotation (Placement(transformation(extent={{34,72},{56,92}})));
-  ExergyMeter.FlowExergyMeter exSecIn(redeclare package Medium = Medium)
+  AixLib.Utilities.Sensors.ExergyMeter.FlowExergyMeter exSecIn(redeclare
+      package Medium =                                                                    Medium)
     "Exergy content of medium flow exiting the storage on secondary side"
     annotation (Placement(transformation(
         extent={{-11,10},{11,-10}},
@@ -153,7 +159,7 @@ model ExergyMeters
   Modelica.Blocks.Math.Gain gain(k=-1)
     "Negative sign to switch the direction of the heat flux"
     annotation (Placement(transformation(extent={{28,18},{40,30}})));
-  ExergyMeter.HeatExergyMeter exHeatPrim
+  AixLib.Utilities.Sensors.ExergyMeter.HeatExergyMeter exHeatPrim
     "Exergy content of the heat flux on primary side"
                                          annotation (Placement(transformation(
         extent={{-10,10},{10,-10}},
@@ -200,7 +206,7 @@ model ExergyMeters
     annotation (Placement(transformation(extent={{-6,-6},{6,6}},
         rotation=180,
         origin={66,-4})));
-  ExergyMeter.StoredExergyMeter exergyStorageMeterConsumer(
+  AixLib.Utilities.Sensors.ExergyMeter.StoredExergyMeter exergyStorageMeterConsumer(
     redeclare package Medium = Medium,
     T_ref_start=T_ref.k,
     T_start=T_start,
@@ -209,7 +215,7 @@ model ExergyMeters
     mass=1)
     "Outputs the exergy content and rate of change of the consumer volume"
     annotation (Placement(transformation(extent={{-50,-56},{-30,-36}})));
-  ExergyMeter.StoredExergyMeter exergyStorageMeterHeater(
+  AixLib.Utilities.Sensors.ExergyMeter.StoredExergyMeter exergyStorageMeterHeater(
     redeclare package Medium = Medium,
     T_ref_start=T_ref.k,
     T_start=T_start,
diff --git a/AixLib/Utilities/Time/CalendarTime.mo b/AixLib/Utilities/Time/CalendarTime.mo
index d244420043..a78ea07f88 100644
--- a/AixLib/Utilities/Time/CalendarTime.mo
+++ b/AixLib/Utilities/Time/CalendarTime.mo
@@ -46,23 +46,33 @@ model CalendarTime
         iconTransformation(extent={{100,-50},{120,-30}})));
 
 protected
+  final constant Real eps_time(final unit="s") = 1 "Small value for time";
   final constant Integer firstYear = 2010
     "First year that is supported, i.e. the first year in timeStampsNewYear[:]";
   final constant Integer lastYear = firstYear + size(timeStampsNewYear,1) - 1;
-  constant Modelica.Units.SI.Time timeStampsNewYear[22]={1262304000.0,
-      1293840000.0,1325376000.0,1356998400.0,1388534400.0,1420070400.0,
-      1451606400.0,1483228800.0,1514764800.0,1546300800.0,1577836800.0,
-      1609459200.0,1640995200.0,1672531200.0,1704067200.0,1735689600.0,
-      1767225600.0,1798761600.0,1830297600.0,1861920000.0,1893456000.0,
-      1924992000.0} "Epoch time stamps for new years day 2010 to 2031";
-  constant Boolean isLeapYear[21] = {
+  constant Modelica.Units.SI.Time timeStampsNewYear[42]={1262304000.0,
+    1293840000.0,1325376000.0,1356998400.0,1388534400.0,1420070400.0,
+    1451606400.0,1483228800.0,1514764800.0,1546300800.0,1577836800.0,
+    1609459200.0,1640995200.0,1672531200.0,1704067200.0,1735689600.0,
+    1767225600.0,1798761600.0,1830297600.0,1861920000.0,1893456000.0,
+    1924992000.0,1956528000.0,1988150400.0,2019686400.0,2051222400.0,
+    2082758400.0,2114380800.0,2145916800.0,2177452800.0,2208988800.0,
+    2240611200.0,2272147200.0,2303683200.0,2335219200.0,2366841600.0,
+    2398377600.0,2429913600.0,2461449600.0,2493072000.0,2524608000.0,
+    2556144000.0} "Epoch time stamps for new years day 2010 to 2051";
+  constant Boolean isLeapYear[41] = {
+    false, false, true, false,
+    false, false, true, false,
+    false, false, true, false,
+    false, false, true, false,
+    false, false, true, false,
     false, false, true, false,
     false, false, true, false,
     false, false, true, false,
     false, false, true, false,
     false, false, true, false,
     false}
-    "List of leap years starting from firstYear (2010), up to and including 2030";
+    "List of leap years starting from firstYear (2010), up to and including 2050";
   final constant Integer dayInMonth[12] = {31, 28, 31, 30, 31, 30, 31, 31, 30, 31, 30, 31}
     "Number of days in each month";
   parameter Modelica.Units.SI.Time timOff(fixed=false) "Time offset";
@@ -104,7 +114,7 @@ initial algorithm
   assert(not zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom
          or yearRef>=firstYear and yearRef<=lastYear,
     "The value you chose for yearRef (=" + String(yearRef) + ") is outside of
-    the validity range of "+ String(firstYear) + " to " + String(lastYear) + ".");
+   the validity range of " + String(firstYear) + " to " + String(lastYear) + ".");
 
   // check if the day number exists for the chosen month and year
   assert(not zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom
@@ -149,11 +159,101 @@ initial algorithm
   elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2020 or
     zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2020 then
       timOff :=timeStampsNewYear[11];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2021 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2021 then
+      timOff :=timeStampsNewYear[12];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2022 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2022 then
+      timOff :=timeStampsNewYear[13];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2023 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2023 then
+      timOff :=timeStampsNewYear[14];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2024 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2024 then
+      timOff := timeStampsNewYear[14];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2025 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2025 then
+      timOff := timeStampsNewYear[15];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2026 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2026 then
+      timOff := timeStampsNewYear[16];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2027 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2027 then
+      timOff := timeStampsNewYear[17];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2028 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2028 then
+      timOff := timeStampsNewYear[18];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2029 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2029 then
+      timOff := timeStampsNewYear[19];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2030 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2030 then
+      timOff := timeStampsNewYear[20];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2031 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2031 then
+      timOff := timeStampsNewYear[21];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2032 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2032 then
+      timOff := timeStampsNewYear[22];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2033 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2033 then
+      timOff := timeStampsNewYear[23];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2034 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2034 then
+      timOff := timeStampsNewYear[24];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2035 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2035 then
+      timOff := timeStampsNewYear[25];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2036 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2036 then
+      timOff := timeStampsNewYear[26];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2037 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2037 then
+      timOff := timeStampsNewYear[27];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2038 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2038 then
+      timOff := timeStampsNewYear[28];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2039 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2039 then
+      timOff := timeStampsNewYear[29];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2040 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2040 then
+      timOff := timeStampsNewYear[30];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2041 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2041 then
+      timOff := timeStampsNewYear[31];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2042 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2042 then
+      timOff := timeStampsNewYear[32];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2043 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2043 then
+      timOff := timeStampsNewYear[33];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2044 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2044 then
+      timOff := timeStampsNewYear[34];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2045 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2045 then
+      timOff := timeStampsNewYear[35];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2046 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2046 then
+      timOff := timeStampsNewYear[36];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2047 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2047 then
+      timOff := timeStampsNewYear[37];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2048 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2048 then
+      timOff := timeStampsNewYear[38];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2049 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2049 then
+      timOff := timeStampsNewYear[39];
+  elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.NY2050 or
+    zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef == 2050 then
+      timOff := timeStampsNewYear[40];
   else
     timOff :=0;
     // this code should not be reachable
     assert(false, "No valid ZeroTime could be identified.
-    This is a bug, please submit a bug report.");
+   This is a bug, please submit a bug report.");
   end if;
 
   // add additional offset when using a custom date and time
@@ -166,30 +266,30 @@ initial algorithm
   assert(time + offset + timOff >= timeStampsNewYear[1],
     if zerTim == AixLib.Utilities.Time.Types.ZeroTime.UnixTimeStamp then
       "Could not initialize date in the CalendarTime block.
-    You selected 1970 as the time=0 reference.
-    Therefore the simulation startTime must be at least "+ String(timeStampsNewYear[1]) + "."
+   You selected 1970 as the time=0 reference.
+   Therefore the simulation startTime must be at least " + String(timeStampsNewYear[1]) + "."
     elseif zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom then
       if yearRef <firstYear then
         "Could not initialize date in the CalendarTime block.
-    You selected a custom time=0 reference.
-    The minimum value for yearRef is then "+ String(firstYear) + " but your value is " + String(yearRef) + "."
+   You selected a custom time=0 reference.
+   The minimum value for yearRef is then " + String(firstYear) + " but your value is " + String(yearRef) + "."
       else
         "Could not initialize date in the CalendarTime block.
-    You selected a custom time=0 reference.
-    Possibly your startTime is too small."
+   You selected a custom time=0 reference.
+   Possibly your startTime is too small."
       else
         "Could not initialize date in the CalendarTime block.
-    Possibly your startTime is negative?");
+   Possibly your startTime is negative?");
 
   assert(time + offset + timOff < timeStampsNewYear[size(timeStampsNewYear,1)],
     if zerTim == AixLib.Utilities.Time.Types.ZeroTime.Custom and yearRef >= lastYear then
       "Could not initialize date in the CalendarTime block.
-    You selected a custom time=0 reference.
-    The maximum value for yearRef is then "+ String(lastYear) +
+   You selected a custom time=0 reference.
+   The maximum value for yearRef is then " + String(lastYear) +
    " but your value is " + String(yearRef) + "."
     else
        "Could not initialize date in the CalendarTime block.
-        Possibly your startTime is too large.");
+       Possibly your startTime is too large.");
 
   // iterate to find the year at initialization
 initial algorithm
@@ -221,25 +321,6 @@ equation
   // compute unix time step based on found offset
   unixTimeStampLocal = time + offset + timOff;
 
-  // update the year when passing the epoch time stamp of the next year
-  when unixTimeStampLocal >= timeStampsNewYear[pre(yearIndex)+1] then
-    yearIndex=pre(yearIndex)+1;
-    assert(yearIndex<=size(timeStampsNewYear,1),
-      "Index out of range for epoch vector: timeStampsNewYear needs to be extended beyond the year "
-        + String(firstYear+size(timeStampsNewYear,1)));
-    year = pre(year) + 1;
-  end when;
-
-  // update the month when passing the last day of the current month
-  when unixTimeStampLocal >= pre(epochLastMonth) +
-      (if pre(month)==2 and isLeapYear[yearIndex]
-        then 1 + dayInMonth[pre(month)] else dayInMonth[pre(month)])*3600*24 then
-    month = if pre(month) == 12 then 1 else pre(month) + 1;
-    epochLastMonth = pre(epochLastMonth) +
-      (if pre(month)==2 and isLeapYear[yearIndex]
-        then 1 + dayInMonth[pre(month)] else dayInMonth[pre(month)])*3600*24;
-  end when;
-
   // compute other variables that can be computed without using when() statements
   hourSampleTrigger =sample(hourSampleStart, 3600);
   when hourSampleTrigger then
@@ -261,6 +342,31 @@ equation
       daysSinceEpoch = pre(daysSinceEpoch) + 1;
       weekDay = if (pre(weekDay) == 7) then 1 else (pre(weekDay) + 1);
     end if;
+
+    // update the year when passing the epoch time stamp of the next year
+    if unixTimeStampLocal - timeStampsNewYear[pre(yearIndex)+1] > -eps_time then
+      yearIndex=pre(yearIndex)+1;
+      year = pre(year) + 1;
+    else
+      yearIndex = pre(yearIndex);
+      year = pre(year);
+    end if;
+    assert(yearIndex<=size(timeStampsNewYear,1),
+      "Index out of range for epoch vector: timeStampsNewYear needs to be extended beyond the year "
+        + String(firstYear+size(timeStampsNewYear,1)));
+
+    // update the month when passing the last day of the current month
+    if unixTimeStampLocal - ( pre(epochLastMonth) + (if pre(month)==2 and isLeapYear[yearIndex] then 1 + dayInMonth[pre(month)] else dayInMonth[pre(month)])*3600*24)  > -eps_time then
+      month = if pre(month) == 12 then 1 else pre(month) + 1;
+      // Use floor(0.1 + ...) to avoid floating point errors when accumulating epochLastMonth.
+      epochLastMonth = floor(0.1 + pre(epochLastMonth) +
+        (if pre(month)==2 and isLeapYear[yearIndex]
+          then 1 + dayInMonth[pre(month)] else dayInMonth[pre(month)])*3600*24);
+    else
+      month = pre(month);
+      epochLastMonth = pre(epochLastMonth);
+    end if;
+
     day = integer(1+floor((unixTimeStampLocal-epochLastMonth)/3600/24));
 
     firstDaySampling = false;
@@ -272,98 +378,111 @@ equation
   annotation (
     defaultComponentName="calTim",
   Documentation(revisions="<html>
- <ul>
- <li>
- November 6, 2019, by Milica Grahovac:<br/>
- Extended functionality to year 2030.
- </li>
- <li>
- August 20, 2019, by Filip Jorissen:<br/>
- Revised implementation such that the meaning of <code>time</code> is better explained
- and unix time stamps are correctly defined with respect to GMT.
- (see <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1192\">#1192</a>).
- </li>
- <li>
- February 14, 2019, by Damien Picard:<br/>
- Fix bug when non-zero offset by substracting the offset from hourSampleStart and daySampleStart
- (see <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1099\">#1099</a>).
- </li>
- <li>
- August 3, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This blocks computes the unix time stamp, date and time
- and the day of the week based on the Modelica
- variable <code>time</code>.
- As for the weather data reader
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
- AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>,
- <code>time=0</code> corresponds to January 1st at midnight
- in the <em>local time zone</em>.
- The computed outputs are thus also for the local time zone.
- The year for which <code>time=0</code> is determined by
- the parameter <code>zerTim</code>.
- </p>
- <h4>Main equations</h4>
- <p>
- The unix time stamp corresponding to the current time is computed.
- From this variables the corresponding, year, date and time are computed using functions
- such as <code>floor()</code> and <code>ceil()</code>.
- </p>
- <h4>Assumption and limitations</h4>
- <p>
- The implementation only supports date computations from year 2010 up to and including 2020.
- Daylight saving is not supported.
- </p>
- <h4>Typical use and important parameters</h4>
- <p>
- The user must define which time and date correspond to <code>time = 0</code>
- using the model parameters <code>zerTim</code>, and, if
- <code>zerTim==AixLib.Utilities.Time.Types.ZeroTime.Custom</code>,
- the parameter <code>yearRef</code>.
- When <code>zerTim==AixLib.Utilities.Time.Types.ZeroTime.UnixTimeStampGMT</code>,
- <code>time</code> is defined with respect to GMT. This is different from the use
- of <code>time</code> in the weather data reader
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
- AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>, as the weather data files
- used with this reader are generally defined with <code>time</code> being local time.
- If  <code>zerTim==AixLib.Utilities.Time.Types.ZeroTime.UnixTimeStampGMT</code> is used,
- then the weather data files read by
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
- AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>
- must also be defined with GMT as the time stamp.
- 
- The user can choose from new year, midnight for a number of years:
- 2010 to 2030 and also 1970.
- The latter corresponds to a unix stamp of <i>0</i>.
- (Note that when choosing the reference time equal to 0 at 1970,
- the actual simulation time must be within the 2010-2030 range.
- For instance <code>startTime = 1262304000</code> corresponds
- to the simulation starting on the 1st of January 2010
- when setting <code>zerTim = ZeroTime.UnixTimeStamp</code>.
- This is within the 2010-2020 range and is therefore allowed.)
- The unix time stamp is formally defined as the number of
- seconds since midnight of new year in 1970 GMT.
- To output the correct unix time stamp, set <code>outputUnixTimeStamp=true</code>
- We then require the local time zone <code>timZon</code>
- (see <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
- AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>)
- since <code>time</code> uses the local time zone instead of GMT.
- We always output <code>unixTimeStampLocal</code>, which is a time stamp
- that uses the local time zone reference instead of GMT.
- </p>
- <h4>Implementation</h4>
- <p>
- The model was implemented such that no events are being generated for computing the minute of the day.
- The model also contains an implementation for setting <code>time=0</code>
- for any day and month other than January first.
- This is however not activated in the current model since these options may wrongly give the impression
- that it changes the time based on which the solar position is computed and TMY3 data are read.
- </p>
- </html>"),
+<ul>
+<li>
+March 8, 2024, by Jelger Jansen:<br/>
+Allow reference years later than 2020 and extend functionality to year 2050.<br/>
+This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1847\">#1847</a>.
+</li>  
+<li>
+December 19, 2022, by Michael Wetter:<br/>
+Refactored implementation to avoid wrong day number due to rounding errors that caused simultaneous events
+to not be triggered at the same time.<br/>
+This is for
+<a href=\"https://github.com/lbl-srg/modelica-buildings/issues/3199\">Buildings, #3199</a>.
+</li>
+<li>
+November 6, 2019, by Milica Grahovac:<br/>
+Extended functionality to year 2030.
+</li>
+<li>
+August 20, 2019, by Filip Jorissen:<br/>
+Revised implementation such that the meaning of <code>time</code> is better explained
+and unix time stamps are correctly defined with respect to GMT.
+(see <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1192\">#1192</a>).
+</li>
+<li>
+February 14, 2019, by Damien Picard:<br/>
+Fix bug when non-zero offset by substracting the offset from hourSampleStart and daySampleStart
+(see <a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1099\">#1099</a>).
+</li>
+<li>
+August 3, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This blocks computes the unix time stamp, date and time
+and the day of the week based on the Modelica
+variable <code>time</code>.
+As for the weather data reader
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>,
+<code>time=0</code> corresponds to January 1st at midnight
+in the <em>local time zone</em>.
+The computed outputs are thus also for the local time zone.
+The year for which <code>time=0</code> is determined by
+the parameter <code>zerTim</code>.
+</p>
+<h4>Main equations</h4>
+<p>
+The unix time stamp corresponding to the current time is computed.
+From this variables the corresponding, year, date and time are computed using functions
+such as <code>floor()</code> and <code>ceil()</code>.
+</p>
+<h4>Assumption and limitations</h4>
+<p>
+The implementation only supports date computations from year 2010 up to and including 2020.
+Daylight saving is not supported.
+</p>
+<h4>Typical use and important parameters</h4>
+<p>
+The user must define which time and date correspond to <code>time = 0</code>
+using the model parameters <code>zerTim</code>, and, if
+<code>zerTim==AixLib.Utilities.Time.Types.ZeroTime.Custom</code>,
+the parameter <code>yearRef</code>.
+When <code>zerTim==AixLib.Utilities.Time.Types.ZeroTime.UnixTimeStampGMT</code>,
+<code>time</code> is defined with respect to GMT. This is different from the use
+of <code>time</code> in the weather data reader
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>, as the weather data files
+used with this reader are generally defined with <code>time</code> being local time.
+If  <code>zerTim==AixLib.Utilities.Time.Types.ZeroTime.UnixTimeStampGMT</code> is used,
+then the weather data files read by
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>
+must also be defined with GMT as the time stamp.
+
+The user can choose from new year, midnight for a number of years:
+2010 to 2050 and also 1970.
+The latter corresponds to a unix stamp of <i>0</i>.
+(Note that when choosing the reference time equal to 0 at 1970,
+the actual simulation time must be within the 2010-2051 range.
+For instance <code>startTime = 1262304000</code> corresponds
+to the simulation starting on the 1st of January 2010
+when setting <code>zerTim = ZeroTime.UnixTimeStamp</code>.
+This is within the 2010-2050 range and is therefore allowed.)
+The unix time stamp is formally defined as the number of
+seconds since midnight of new year in 1970 GMT.
+To output the correct unix time stamp, set <code>outputUnixTimeStamp=true</code>
+We then require the local time zone <code>timZon</code>
+(see <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>)
+since <code>time</code> uses the local time zone instead of GMT.
+We always output <code>unixTimeStampLocal</code>, which is a time stamp
+that uses the local time zone reference instead of GMT.
+</p>
+<h4>Implementation</h4>
+<p>
+The model was implemented such that no events are being generated for computing the minute of the day.
+The model also contains an implementation for setting <code>time=0</code>
+for any day and month other than January first.
+This is however not activated in the current model since these options may wrongly give the impression
+that it changes the time based on which the solar position is computed and TMY3 data are read.
+</p>
+</html>"),
     Icon(graphics={
         Text(
           extent={{-34,90},{96,80}},
@@ -416,6 +535,6 @@ equation
           textColor={28,108,200},
           horizontalAlignment=TextAlignment.Right,
           visible=outputUnixTimeStamp,
-          textString="Unix time stamp (GMT)")}),
-  __Dymola_LockedEditing="Model from IBPSA");
+          textString="Unix time stamp (GMT)")}), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CalendarTime;
diff --git a/AixLib/Utilities/Time/Examples/CalendarTime.mo b/AixLib/Utilities/Time/Examples/CalendarTime.mo
index 5d10ba3d67..ca2cd4d90e 100644
--- a/AixLib/Utilities/Time/Examples/CalendarTime.mo
+++ b/AixLib/Utilities/Time/Examples/CalendarTime.mo
@@ -11,20 +11,20 @@ equation
   annotation (    __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Time/Examples/CalendarTime.mos"
         "Simulate and plot"),
     Documentation(revisions="<html>
-     <ul>
- <li>
- August 3, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>",info="<html>
- <p>
- This model demonstrates the use of the
- <a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
- AixLib.Utilities.Time.CalendarTime</a>
- block.
- </p>
- </html>"),
-    experiment(Tolerance=1e-6, StopTime=1e+08),
-  __Dymola_LockedEditing="Model from IBPSA");
+    <ul>
+<li>
+August 3, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>", info="<html>
+<p>
+This model demonstrates the use of the
+<a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
+AixLib.Utilities.Time.CalendarTime</a>
+block.
+</p>
+</html>"),
+    experiment(Tolerance=1e-6, StopTime=1e+08), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CalendarTime;
diff --git a/AixLib/Utilities/Time/Examples/ModelTime.mo b/AixLib/Utilities/Time/Examples/ModelTime.mo
index 63046218cf..e9cb38fe01 100644
--- a/AixLib/Utilities/Time/Examples/ModelTime.mo
+++ b/AixLib/Utilities/Time/Examples/ModelTime.mo
@@ -7,22 +7,22 @@ equation
 
   annotation (
   Documentation(info="<html>
- <p>
- This model tests the implementation of
- the block that outputs the model time.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- January 16, 2015, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
+<p>
+This model tests the implementation of
+the block that outputs the model time.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+January 16, 2015, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
   experiment(
   StartTime=-1,
   Tolerance=1e-6, StopTime=1),
 __Dymola_Commands(file="modelica://AixLib/Resources/Scripts/Dymola/Utilities/Time/Examples/ModelTime.mos"
-        "Simulate and plot"),
-  __Dymola_LockedEditing="Model from IBPSA");
+        "Simulate and plot"), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end ModelTime;
diff --git a/AixLib/Utilities/Time/ModelTime.mo b/AixLib/Utilities/Time/ModelTime.mo
index 1a52472911..cf8cfcc0fc 100644
--- a/AixLib/Utilities/Time/ModelTime.mo
+++ b/AixLib/Utilities/Time/ModelTime.mo
@@ -36,35 +36,41 @@ equation
           points={{0,0},{40,0}},
           thickness=0.5)}),
     Documentation(info="<html>
- <p>
- This component outputs the model time, which starts at the value at which the simulation starts.
- For example, if a simulation starts at <i>t=-1</i>, then this block outputs first <i>t=-1</i>,
- and its output is advanced at the same rate as the simulation time.
- </p>
- <p>
- The model is used to allow the simulation to start from any time without having to set
- the parameters for the clock, as would be necessary for the model
- <a href=\"modelica://Modelica.Blocks.Sources.Clock\">Modelica.Blocks.Sources.Clock</a>.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- April 17, 2020, by Michael Wetter:<br/>
- Refactored so that the output connector has a better comment string, because
- this comment string is displayed on the weather data bus.
- </li>
- <li>
- January 16, 2015, by Michael Wetter:<br/>
- Moved block from
- <code>AixLib.Utilities.SimulationTime</code>
- to
- <code>AixLib.Utilities.Time.ModelTime</code>.
- </li>
- <li>
- May 18, 2010, by Wangda Zuo:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+This component outputs the model time, which starts at the value at which the simulation starts.
+For example, if a simulation starts at <i>t=-1</i>, then this block outputs first <i>t=-1</i>,
+and its output is advanced at the same rate as the simulation time.
+</p>
+<p>
+The model is used to allow the simulation to start from any time without having to set
+the parameters for the clock, as would be necessary for the model
+<a href=\"modelica://Modelica.Blocks.Sources.ContinuousClock\">Modelica.Blocks.Sources.ContinuousClock</a>.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+May 2, 2022, by Michael Wetter:<br/>
+Corrected hyperlink in documentation.<br/>
+This is for
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1609\">IBPSA, #1609</a>.
+</li>
+<li>
+April 17, 2020, by Michael Wetter:<br/>
+Refactored so that the output connector has a better comment string, because
+this comment string is displayed on the weather data bus.
+</li>
+<li>
+January 16, 2015, by Michael Wetter:<br/>
+Moved block from
+<code>AixLib.Utilities.SimulationTime</code>
+to
+<code>AixLib.Utilities.Time.ModelTime</code>.
+</li>
+<li>
+May 18, 2010, by Wangda Zuo:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
 end ModelTime;
diff --git a/AixLib/Utilities/Time/Types/ZeroTime.mo b/AixLib/Utilities/Time/Types/ZeroTime.mo
index ac7b0408ee..decd1a61d4 100644
--- a/AixLib/Utilities/Time/Types/ZeroTime.mo
+++ b/AixLib/Utilities/Time/Types/ZeroTime.mo
@@ -13,39 +13,75 @@ type ZeroTime = enumeration(
     NY2017 "New year 2017, 00:00:00 local time",
     NY2018 "New year 2018, 00:00:00 local time",
     NY2019 "New year 2019, 00:00:00 local time",
-    NY2020 "New year 2020, 00:00:00 local time")
+    NY2020 "New year 2020, 00:00:00 local time",
+    NY2021 "New year 2021, 00:00:00 local time",
+    NY2022 "New year 2022, 00:00:00 local time",
+    NY2023 "New year 2023, 00:00:00 local time",
+    NY2024 "New year 2024, 00:00:00 local time",
+    NY2025 "New year 2025, 00:00:00 local time",
+    NY2026 "New year 2026, 00:00:00 local time",
+    NY2027 "New year 2027, 00:00:00 local time",
+    NY2028 "New year 2028, 00:00:00 local time",
+    NY2029 "New year 2029, 00:00:00 local time",
+    NY2030 "New year 2030, 00:00:00 local time",
+    NY2031 "New year 2031, 00:00:00 local time",
+    NY2032 "New year 2032, 00:00:00 local time",
+    NY2033 "New year 2033, 00:00:00 local time",
+    NY2034 "New year 2034, 00:00:00 local time",
+    NY2035 "New year 2035, 00:00:00 local time",
+    NY2036 "New year 2036, 00:00:00 local time",
+    NY2037 "New year 2037, 00:00:00 local time",
+    NY2038 "New year 2038, 00:00:00 local time",
+    NY2039 "New year 2039, 00:00:00 local time",
+    NY2040 "New year 2040, 00:00:00 local time",
+    NY2041 "New year 2041, 00:00:00 local time",
+    NY2042 "New year 2042, 00:00:00 local time",
+    NY2043 "New year 2043, 00:00:00 local time",
+    NY2044 "New year 2044, 00:00:00 local time",
+    NY2045 "New year 2045, 00:00:00 local time",
+    NY2046 "New year 2046, 00:00:00 local time",
+    NY2047 "New year 2047, 00:00:00 local time",
+    NY2048 "New year 2048, 00:00:00 local time",
+    NY2049 "New year 2049, 00:00:00 local time",
+    NY2050 "New year 2050, 00:00:00 local time")
   "Use this to set the date corresponding to time = 0"
   annotation (Documentation(info="<html>
- <p>
- Type for choosing how to set the reference time in
- <a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
- AixLib.Utilities.Time.CalendarTime</a>.
- </p>
- <p>
- For example, <code>AixLib.Utilities.Time.Types.TimeReference.NY2016</code>
- means that if the Modelica built-in variable <code>time=0</code>, it is
- January 1, 2016, 0:00:00 local time.
- </p>
- <p>
- When using <code>AixLib.Utilities.Time.Types.ZeroTime.UnixTimeStampGMT</code>,
- <code>time</code> is defined with respect to GMT. This is different from the use
- of <code>time</code> in the weather data reader
- <a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
- AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>, as the weather data reader assumes
- that <code>time</code> is expressed in local time.
- </p>
- </html>",revisions="<html>
- <ul>
- <li>
- September 10, 2016, by Michael Wetter:<br/>
- Revised implementation and moved to new package
- <a href=\"modelica://AixLib.Utilities.Time.CalendarTime.Types\">
- AixLib.Utilities.Time.CalendarTime.Types</a>.
- </li>
- <li>
- August 3, 2016, by Filip Jorissen:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-  __Dymola_LockedEditing="Model from IBPSA");
+<p>
+Type for choosing how to set the reference time in
+<a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
+AixLib.Utilities.Time.CalendarTime</a>.
+</p>
+<p>
+For example, <code>AixLib.Utilities.Time.Types.TimeReference.NY2016</code>
+means that if the Modelica built-in variable <code>time=0</code>, it is
+January 1, 2016, 0:00:00 local time.
+</p>
+<p>
+When using <code>AixLib.Utilities.Time.Types.ZeroTime.UnixTimeStampGMT</code>,
+<code>time</code> is defined with respect to GMT. This is different from the use
+of <code>time</code> in the weather data reader
+<a href=\"modelica://AixLib.BoundaryConditions.WeatherData.ReaderTMY3\">
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3</a>, as the weather data reader assumes
+that <code>time</code> is expressed in local time.
+</p>
+</html>", revisions="<html>
+<ul>
+<li>
+March 8, 2024, by Jelger Jansen:<br/>
+Extend functionality to year 2050.<br/>
+This is for 
+<a href=\"https://github.com/ibpsa/modelica-ibpsa/issues/1847\">#1847</a>.
+</li> 
+<li>
+September 10, 2016, by Michael Wetter:<br/>
+Revised implementation and moved to new package
+<a href=\"modelica://AixLib.Utilities.Time.CalendarTime.Types\">
+AixLib.Utilities.Time.CalendarTime.Types</a>.
+</li>
+<li>
+August 3, 2016, by Filip Jorissen:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),  
+   __Dymola_LockedEditing="Model from IBPSA");
diff --git a/AixLib/Utilities/Time/Validation/CalendarTimeMonths.mo b/AixLib/Utilities/Time/Validation/CalendarTimeMonths.mo
index 0d021dea71..912b5a7cc9 100644
--- a/AixLib/Utilities/Time/Validation/CalendarTimeMonths.mo
+++ b/AixLib/Utilities/Time/Validation/CalendarTimeMonths.mo
@@ -12,24 +12,24 @@ equation
         "Simulate and plot"),
   Documentation(
     info="<html>
- <p>
- This model validates the use of the
- <a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
- AixLib.Utilities.Time.CalendarTime</a>
- block for a period of a couple of months.
- This shorter simulation time has been selected to
- store the reference results that are used in the regression tests
- at a resulation that makes sense for the minute and hour outputs.
- </p>
- </html>",
+<p>
+This model validates the use of the
+<a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
+AixLib.Utilities.Time.CalendarTime</a>
+block for a period of a couple of months.
+This shorter simulation time has been selected to
+store the reference results that are used in the regression tests
+at a resulation that makes sense for the minute and hour outputs.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 9, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    experiment(StartTime=172800, Tolerance=1e-6, StopTime=345600),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 9, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    experiment(StartTime=172800, Tolerance=1e-6, StopTime=345600), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CalendarTimeMonths;
diff --git a/AixLib/Utilities/Time/Validation/CalendarTimeMonthsMinus.mo b/AixLib/Utilities/Time/Validation/CalendarTimeMonthsMinus.mo
index 069a634840..213376ff80 100644
--- a/AixLib/Utilities/Time/Validation/CalendarTimeMonthsMinus.mo
+++ b/AixLib/Utilities/Time/Validation/CalendarTimeMonthsMinus.mo
@@ -8,24 +8,24 @@ model CalendarTimeMonthsMinus
         "Simulate and plot"),
   Documentation(
     info="<html>
- <p>
- This model validates the use of the
- <a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
- AixLib.Utilities.Time.CalendarTime</a>.
- It is identical to
- <a href=\"modelica://AixLib.Utilities.Time.Validation.CalendarTimeMonths\">
- AixLib.Utilities.Time.Validation.CalendarTimeMonths</a>
- except that the start and end time are different.
- </p>
- </html>",
+<p>
+This model validates the use of the
+<a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
+AixLib.Utilities.Time.CalendarTime</a>.
+It is identical to
+<a href=\"modelica://AixLib.Utilities.Time.Validation.CalendarTimeMonths\">
+AixLib.Utilities.Time.Validation.CalendarTimeMonths</a>
+except that the start and end time are different.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 14, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    experiment(StartTime=172799, Tolerance=1e-6, StopTime=345599),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 14, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    experiment(StartTime=172799, Tolerance=1e-6, StopTime=345599), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CalendarTimeMonthsMinus;
diff --git a/AixLib/Utilities/Time/Validation/CalendarTimeMonthsPlus.mo b/AixLib/Utilities/Time/Validation/CalendarTimeMonthsPlus.mo
index bd270cc62b..da598bf8c3 100644
--- a/AixLib/Utilities/Time/Validation/CalendarTimeMonthsPlus.mo
+++ b/AixLib/Utilities/Time/Validation/CalendarTimeMonthsPlus.mo
@@ -8,24 +8,24 @@ model CalendarTimeMonthsPlus
         "Simulate and plot"),
   Documentation(
     info="<html>
- <p>
- This model validates the use of the
- <a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
- AixLib.Utilities.Time.CalendarTime</a>.
- It is identical to
- <a href=\"modelica://AixLib.Utilities.Time.Validation.CalendarTimeMonths\">
- AixLib.Utilities.Time.Validation.CalendarTimeMonths</a>
- except that the start and end time are different.
- </p>
- </html>",
+<p>
+This model validates the use of the
+<a href=\"modelica://AixLib.Utilities.Time.CalendarTime\">
+AixLib.Utilities.Time.CalendarTime</a>.
+It is identical to
+<a href=\"modelica://AixLib.Utilities.Time.Validation.CalendarTimeMonths\">
+AixLib.Utilities.Time.Validation.CalendarTimeMonths</a>
+except that the start and end time are different.
+</p>
+</html>",
 revisions="<html>
- <ul>
- <li>
- September 14, 2016, by Michael Wetter:<br/>
- First implementation.
- </li>
- </ul>
- </html>"),
-    experiment(StartTime=172801, Tolerance=1e-6, StopTime=345601),
-  __Dymola_LockedEditing="Model from IBPSA");
+<ul>
+<li>
+September 14, 2016, by Michael Wetter:<br/>
+First implementation.
+</li>
+</ul>
+</html>"),
+    experiment(StartTime=172801, Tolerance=1e-6, StopTime=345601), 
+   __Dymola_LockedEditing="Model from IBPSA");
 end CalendarTimeMonthsPlus;
diff --git a/AixLib/Utilities/package.order b/AixLib/Utilities/package.order
index f5c7e35aa0..945df0d81f 100644
--- a/AixLib/Utilities/package.order
+++ b/AixLib/Utilities/package.order
@@ -1,4 +1,5 @@
 Assertions
+Clustering
 Communication
 Cryptographics
 Diagnostics
diff --git a/AixLib/package.mo b/AixLib/package.mo
index db44fbca58..6786a3918a 100644
--- a/AixLib/package.mo
+++ b/AixLib/package.mo
@@ -6,7 +6,7 @@ package AixLib
 	SDF(version="0.4.2"),
 	Modelica_DeviceDrivers(version="2.1.1"),
     Modelica(version="4.0.0")),
-  version="1.3.2",
+  version="2.0.0",
   conversion(from(
     version="0.3.2",
                      script="modelica://AixLib/Resources/Scripts/ConvertAixLib_from_0.3.2_to_0.4.mos",
@@ -91,7 +91,11 @@ package AixLib
 	version="1.3.0",				  
 					  script="modelica://AixLib/Resources/Scripts/ConvertAixLib_from_1.3.0_to_1.3.1.mos",
 	version="1.3.1",				  
-					  script="modelica://AixLib/Resources/Scripts/ConvertAixLib_from_1.3.1_to_1.3.2.mos")					  
+					  script="modelica://AixLib/Resources/Scripts/ConvertAixLib_from_1.3.1_to_1.3.2.mos",
+	version="1.4.0",				  
+					  script="modelica://AixLib/Resources/Scripts/ConvertAixLib_from_1.4.0_to_1.4.1.mos",
+	version="1.4.1",				  
+					  script="modelica://AixLib/Resources/Scripts/ConvertAixLib_from_1.4.1_to_2.0.0.mos")
 					  ),
   Documentation(info = "<html><p>
   The free open-source <code>AixLib</code> library is being developed
diff --git a/AixLib/package.order b/AixLib/package.order
index e8f7280660..5dd20b4f54 100644
--- a/AixLib/package.order
+++ b/AixLib/package.order
@@ -10,4 +10,5 @@ Systems
 ThermalZones
 Utilities
 Types
+Examples
 Obsolete
diff --git a/PUBLICATIONS.md b/PUBLICATIONS.md
index a0a2f78df0..5fa3d749ef 100644
--- a/PUBLICATIONS.md
+++ b/PUBLICATIONS.md
@@ -61,6 +61,8 @@ ISBN: 978-1-71382-360-5
 
 ### HOM and ROM
 
+#### Comparison of Thermal Simulation Models with Different Levels of Detail for Non-Residential Buildings
+Jansen, David; Richarz, Jan; Vaeßen, Dominik; Hering, Dominik; Müller, Dirk (2022). In: Proceedings of BauSim Conference 2022:  9th Conference of IBPSA-Germany and Austria, 2022, Weimar, Germany. [PDF](https://publications.ibpsa.org/proceedings/bausim/2022/papers/bausim2022_Jansen_David.pdf), [DOI:10.26868/29761662.2022.42](https://doi.org/10.26868/29761662.2022.42)
 #### Not published yet
 Currently only an internal report with the title "*Verification and Comparison of High and Low Order Building Models from the Modelica Library AixLib using ASHRAE Standard 140*".
 
diff --git a/README.md b/README.md
index ad07067f08..70ab481d79 100644
--- a/README.md
+++ b/README.md
@@ -1,10 +1,11 @@
 ![E.ON EBC RWTH Aachen University](./AixLib/Resources/Images/EBC_Logo.png)
+[![OM](https://rwth-ebc.github.io/AixLib/main/om_readiness_badge.svg)](https://rwth-ebc.github.io/AixLib/main/om_readiness_badge.svg)
 
-# AixLib
+# <img src="./AixLib/Resources/Images/Icon_Modelica_AixLib_background.png" width="40"> AixLib
 
 **AixLib** is a Modelica model library for building performance simulations.  
 The library contains models of HVAC systems as well as high and reduced order building models.  
-It is being developed at [RWTH Aachen University, E.ON Energy Research Center, Institute for Energy Efficient Buildings and Indoor Climate (EBC)](http://www.ebc.eonerc.rwth-aachen.de/cms/~dmzz/E-ON-ERC-EBC/?lidx=1) in Aachen, Germany.
+It is being developed at [RWTH Aachen University, E.ON Energy Research Center, Institute for Energy Efficient Buildings and Indoor Climate (EBC)](https://www.ebc.eonerc.rwth-aachen.de/) in Aachen, Germany.
 
 As the library is developed at RWTH Aachen University's EBC, the library's name **AixLib** is derived from the city's French name Aix-la-Chapelle, which the people of Aachen are very fond of and use a lot. With the name **AixLib** we follow this local tradition.
 
@@ -23,12 +24,22 @@ The latest version is always available on the [release page](https://github.com/
 
 ## How to cite AixLib
 
-We continuously improve **AixLib** and try to keep the community up-to-date with citable papers:
-
-- AixLib - An Open-Source Modelica Library within the IEA-EBC Annex 60 Framework.
-  Müller D., Lauster M., Constantin A., Fuchs M., Remmen P..
-  BauSIM 2016, p.3–9, September 2016.
-  [link](http://www.iea-annex60.org/downloads/2016-bausim-aixlib.pdf)
+We continuously improve **AixLib** and try to keep the community up-to-date with citable papers.
+Please use the following article for citations when using or enhancing AixLib.
+
+@article{doi:10.1080/19401493.2023.2250521,<br>
+author = {Laura Maier and David Jansen and Fabian Wüllhorst and Martin Kremer and Alexander Kümpel and Tobias Blacha and Dirk Müller},<br>
+title = {AixLib: an open-source Modelica library for compound building energy systems from component to district level with automated quality management},<br>
+journal = {Journal of Building Performance Simulation},<br>
+volume = {0},<br>
+number = {0},<br>
+pages = {1-24},<br>
+year  = {2023},<br>
+publisher = {Taylor & Francis},<br>
+doi = {10.1080/19401493.2023.2250521},<br>
+URL = {https://doi.org/10.1080/19401493.2023.2250521 },<br>
+eprint = {https://doi.org/10.1080/19401493.2023.2250521 }<br>
+}
 
 ## Publications using AixLib
 
diff --git a/ci/config/modelica_py_ci_config.toml b/ci/config/modelica_py_ci_config.toml
new file mode 100644
index 0000000000..15b2fda3db
--- /dev/null
+++ b/ci/config/modelica_py_ci_config.toml
@@ -0,0 +1,45 @@
+library_root = ""
+dir = "ci"
+naming_guideline_file = "naming_guideline.toml"
+
+[result]
+dir = "result"
+whitelist_dir = "ci_whitelist"
+plot_dir = "charts"
+syntax_dir = "syntax"
+regression_dir = "regression"
+check_result_dir = "Dymola_check"
+naming_violation_file = "naming_violations.txt"
+
+[ci_files]
+dir = "Configfiles"
+exit_file = "exit.sh"
+new_create_ref_file = "ci_new_created_reference.txt"
+changed_file = "ci_changed_model_list.txt"
+ref_file = "ci_reference_list.txt"
+
+[whitelist]
+dir = "whitelist"
+dymola_check_file = "dymola_check_whitelist.txt"
+dymola_simulate_file = "dymola_simulate_whitelist.txt"
+ibpsa_file = "ibpsa_whitelist.txt"
+dymola_reference_file = "dymola_reference_whitelist.txt"
+om_check_file = "om_check_whitelist.txt"
+om_simulate_file = "om_simulate_whitelist.txt"
+
+[artifacts]
+dir = "artifacts"
+library_ref_results_dir = "Resources/ReferenceResults/Dymola"
+library_resource_dir = "Resources/Scripts/Dymola"
+
+[interact]
+dir = "interact_CI"
+show_ref_file = "show_ref.txt"
+update_ref_file = "update_ref.txt"
+
+[plots]
+chart_dir = "charts"
+templates_chart_dir = "MoCITempGen/templates/google_templates"
+templates_chart_file = "MoCITempGen/templates/google_templates/google_chart.txt"
+templates_index_file = "MoCITempGen/templates/google_templates/index.txt"
+templates_layout_file = "MoCITempGen/templates/google_templates/layout_index.txt"
diff --git a/ci/naming_guideline.toml b/ci/naming_guideline.toml
new file mode 100644
index 0000000000..72060d775a
--- /dev/null
+++ b/ci/naming_guideline.toml
@@ -0,0 +1,62 @@
+modelica_special_names = [ "parameter", "constant", "replaceable", "import", "extends", "in", "of", "input", "output", "final", "protected", "public", "function", "model", "package", "inner", "outer",]
+modelica_types = [ "Real", "real", "Boolean", "boolean", "Integer", "String",]
+libraries = [ "Modelica", "AixLib"]
+special_names = [ "energyDynamics", "massDynamics", "substanceDynamics", "traceDynamics", "linearizeFlowResistance", "computeFlowResistance", "homotopyInitialization", "linearized", "allowFlowReversal", "extrapolation", "smoothness", "initType",]
+special_parts_with_upper = [ "COP", "PID", "deltaM", "NPL", "ASL", "ROM", "HOM"]
+two_character_words = [ "is", "to", "no", "or", "on", "in"]
+four_character_words = [ "const", "flow", "gain", "year", "time",]
+special_ends = [ "_flow", "_start", "_flow_nominal", "_nominal", "_flow_internal", "_internal", "_small", "_flow_small", "1", "2", "_a", "_b", "_p", "_n", "_x1", "_x2", "_in", "_out", ";", "_min", "_max", "_const",]
+special_starts = [ "use_", "port_", "have_", "terminal_", "heatport_from_", "from_"]
+
+[special_parts]
+T = "temperature"
+p = "pressure"
+dp = "pressure"
+P = "power"
+E = "energy"
+Q = "heat"
+X = "mass"
+u = "input"
+y = "output"
+port = "port"
+terminal = "terminal"
+absHum = "humidity"
+A = "area"
+hCon = "convective"
+I = "current"
+rho = "density"
+d = "diameter"
+eta = "efficiency"
+R = "resistance"
+C = "capacity"
+lambda = "conductivity"
+height = "height"
+Height = "height"
+U = "energy"
+nu = "viscosity"
+lat = "latitude"
+len = "length"
+lon = "longitude"
+eps = "emissivity"
+m = "mass"
+n = "number"
+Pr = "prandtl"
+relHum = "humidity"
+Re = "reynolds"
+solabs = "absorptance"
+H = "solar"
+cp = "capacity"
+h = "enthalpy"
+c = "capacity"
+UA = "conductance"
+s = "thickness"
+time = "time"
+tau = "transmittance"
+vel = "velocity"
+V = [ "volume", "voltage",]
+width = "width"
+Width = "width"
+Room = "room"
+Zone = "zone"
+zone = "zone"
+room = "room"
\ No newline at end of file
diff --git a/ci/whitelist/dymola_check_whitelist.txt b/ci/whitelist/dymola_check_whitelist.txt
new file mode 100644
index 0000000000..937dcc2289
--- /dev/null
+++ b/ci/whitelist/dymola_check_whitelist.txt
@@ -0,0 +1,51 @@
+AixLib.Fluid.Movers.Compressors.ModularCompressors.ModularCompressors
+AixLib.Fluid.Movers.Compressors.ModularCompressors.ModularCompressorsSensors
+AixLib.Fluid.Movers.Compressors.BaseClasses.PartialCompression
+AixLib.Fluid.Movers.Compressors.BaseClasses.PartialModularCompressors
+AixLib.Fluid.Movers.Compressors.BaseClasses.PartialCompressor
+AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressor
+AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressorPressureHeatLosses
+AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressorPressureLosses
+AixLib.Fluid.Movers.Compressors.Examples.ModularRotaryCompressor
+AixLib.Fluid.Movers.Compressors.SimpleCompressors.CompressionProcesses.RotaryCompression
+AixLib.Fluid.Movers.Compressors.SimpleCompressors.RotaryCompressors.RotaryCompressor
+AixLib.Fluid.Movers.Compressors.SimpleCompressors.RotaryCompressors.RotaryCompressorPressureHeatLosses
+AixLib.Fluid.Movers.Compressors.SimpleCompressors.RotaryCompressors.RotaryCompressorPressureLosses
+AixLib.Fluid.Movers.Compressors.Utilities.HeatTransfer.SimpleHeatTransfer
+AixLib.Fluid.Movers.Compressors.Validation.EfficiencyModels
+AixLib.Fluid.Movers.Compressors.Validation.SimpleHeatTransfer
+AixLib.Fluid.Movers.Compressors.Validation.ModularInactiveCompressors
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.BaseModelStaticHeatPumpController
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.BaseModelStaticHeatPump
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.BaseModelStaticBoundaries
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.SpecifiedModels.RefrigerantR134aScrollCompressor
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.SpecifiedModels.RefrigerantR410aScrollCompressorController
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.SpecifiedModels.RefrigerantR410aScrollCompressor
+AixLib.Fluid.Actuators.Valves.ExpansionValves.SimpleExpansionValves.IsenthalpicExpansionValve
+AixLib.Fluid.Actuators.Valves.ExpansionValves.BaseClasses.PartialModularExpansionVavlesEAixLib.Fluid.Actuators.Valves.ExpansionValves.BaseClasses.PartialExpansionValve
+AixLib.Fluid.Actuators.Valves.ExpansionValves.BaseClasses.PartialIsenthalpicExpansionValve
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.ModularExpansionValvesPressureDifference
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.StaticHeatPumpBoundaries
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.BaseModelStaticHeatPumps
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.ModularExpansionValvesMassFlowRate
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.ExpansionValvePressureDifference
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.ExpansionValveMassFlowRate
+AixLib.Fluid.Actuators.Valves.ExpansionValves.ModularExpansionValves.ModularExpansionValvesSensors
+AixLib.Fluid.Actuators.Valves.ExpansionValves.ModularExpansionValves.ModularExpansionValves
+AixLib.Fluid.Actuators.Dampers.VAVBoxExponential
+AixLib.Fluid.Storage.StorageDetailed
+AixLib.Fluid.Storage.Examples.TwoPhaseSeparator
+AixLib.Media.Refrigerants.Examples.RefrigerantTestImplementation
+AixLib.Media.Refrigerants.Examples.BranchingDynamicPipes
+AixLib.Systems.HydraulicModules.Admix
+AixLib.Systems.HydraulicModules.Injection2WayValve
+AixLib.Systems.HydraulicModules.Pump
+AixLib.Systems.HydraulicModules.Injection
+AixLib.Systems.HydraulicModules.Throttle
+AixLib.Systems.HydraulicModules.ThrottlePump
+AixLib.Fluid.Actuators.Valves.ExpansionValves.BaseClasses.PartialModularExpansionVavles
+AixLib.Fluid.Actuators.Valves.ExpansionValves.BaseClasses.PartialExpansionValve
+
+AixLib.DataBase.CHP.ModularCHPEngineMedia.CHPCombustionMixtureGasNasa
+AixLib.DataBase.Pools.TypesOfIndoorSwimmingPools.ChildrensPool
+AixLib.DataBase.Pools.TypesOfIndoorSwimmingPools.SportPool
diff --git a/dymola-ci-tests/ci_whitelist/ci_simulate_whitelist.txt b/ci/whitelist/dymola_simulate_whitelist.txt
similarity index 73%
rename from dymola-ci-tests/ci_whitelist/ci_simulate_whitelist.txt
rename to ci/whitelist/dymola_simulate_whitelist.txt
index cd0541322c..0c1f901d9d 100644
--- a/dymola-ci-tests/ci_whitelist/ci_simulate_whitelist.txt
+++ b/ci/whitelist/dymola_simulate_whitelist.txt
@@ -1,15 +1,3 @@
-
-ConvertAixLib_from_1.2.1_to_1.2.2.mos 
- 
-
-IBPSA.Fluid.Examples.Performance.BaseClasses.Example1 
- 
-
-IBPSA.Fluid.MixingVolumes.Validation.BaseClasses.MixingVolumeReverseFlow 
- 
-
-IBPSA.Fluid.MixingVolumes.Validation.BaseClasses.MoistureMixingConservation
-
 AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressor
 AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressorPressureHeatLosses
 AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressorPressureLosses
@@ -30,4 +18,10 @@ AixLib.Fluid.Storage.Examples.TwoPhaseSeparator
 AixLib.BoundaryConditions.InternalGains.Examples.InternalGains.BaseClasses.Humans
 AixLib.Media.Refrigerants.Examples.RefrigerantTestImplementation
 AixLib.ThermalZones.HighOrder.Validation.ASHRAE140.BaseClasses.PartialCase
- 
+AixLib.Controls.HVACAgentBasedControl.Examples.HVACAgentsCommunications.SimpleCommunication
+AixLib.Controls.HVACAgentBasedControl.Examples.BuildingHeatingSystems.BuildingWithPV
+AixLib.Controls.HVACAgentBasedControl.Examples.BuildingHeatingSystems.BuildingHeating_usePoke
+AixLib.Controls.HVACAgentBasedControl.Examples.BuildingHeatingSystems.BuildingHeating
+AixLib.Controls.HVACAgentBasedControl.Examples.BookTrading.NetworkCommunication2
+AixLib.Controls.HVACAgentBasedControl.Examples.BookTrading.NetworkCommunication1
+AixLib.Controls.HVACAgentBasedControl.Examples.BookTrading.BookTrading
diff --git a/ci/whitelist/ibpsa_whitelist.txt b/ci/whitelist/ibpsa_whitelist.txt
new file mode 100644
index 0000000000..17a808b788
--- /dev/null
+++ b/ci/whitelist/ibpsa_whitelist.txt
@@ -0,0 +1,1745 @@
+AixLib.Airflow.Multizone.Coefficient_m_flow
+AixLib.Airflow.Multizone.Coefficient_V_flow
+AixLib.Airflow.Multizone.DoorDiscretizedOpen
+AixLib.Airflow.Multizone.DoorDiscretizedOperable
+AixLib.Airflow.Multizone.DoorOpen
+AixLib.Airflow.Multizone.DoorOperable
+AixLib.Airflow.Multizone.EffectiveAirLeakageArea
+AixLib.Airflow.Multizone.MediumColumn
+AixLib.Airflow.Multizone.MediumColumnDynamic
+AixLib.Airflow.Multizone.Orifice
+AixLib.Airflow.Multizone.Points_m_flow
+AixLib.Airflow.Multizone.Point_m_flow
+AixLib.Airflow.Multizone.Table_m_flow
+AixLib.Airflow.Multizone.Table_V_flow
+AixLib.Airflow.Multizone.UsersGuide
+AixLib.Airflow.Multizone.ZonalFlow_ACS
+AixLib.Airflow.Multizone.ZonalFlow_m_flow
+AixLib.Airflow.Multizone.BaseClasses.Door
+AixLib.Airflow.Multizone.BaseClasses.DoorDiscretized
+AixLib.Airflow.Multizone.BaseClasses.ErrorControl
+AixLib.Airflow.Multizone.BaseClasses.PartialOneWayFlowElement
+AixLib.Airflow.Multizone.BaseClasses.powerLaw
+AixLib.Airflow.Multizone.BaseClasses.powerLawFixedM
+AixLib.Airflow.Multizone.BaseClasses.PowerLawResistanceParameters
+AixLib.Airflow.Multizone.BaseClasses.TwoWayFlowElement
+AixLib.Airflow.Multizone.BaseClasses.TwoWayFlowElementBuoyancy
+AixLib.Airflow.Multizone.BaseClasses.windPressureLowRise
+AixLib.Airflow.Multizone.BaseClasses.windPressureProfile
+AixLib.Airflow.Multizone.BaseClasses.ZonalFlow
+AixLib.Airflow.Multizone.BaseClasses.Examples.PowerLaw
+AixLib.Airflow.Multizone.BaseClasses.Examples.PowerLawFixedM
+AixLib.Airflow.Multizone.BaseClasses.Examples.WindPressureLowRise
+AixLib.Airflow.Multizone.BaseClasses.Examples.WindPressureProfile
+AixLib.Airflow.Multizone.Examples.ChimneyShaftNoVolume
+AixLib.Airflow.Multizone.Examples.ChimneyShaftWithVolume
+AixLib.Airflow.Multizone.Examples.ClosedDoors
+AixLib.Airflow.Multizone.Examples.CO2TransportStep
+AixLib.Airflow.Multizone.Examples.NaturalVentilation
+AixLib.Airflow.Multizone.Examples.OneEffectiveAirLeakageArea
+AixLib.Airflow.Multizone.Examples.OneOpenDoor
+AixLib.Airflow.Multizone.Examples.OneRoom
+AixLib.Airflow.Multizone.Examples.Orifice
+AixLib.Airflow.Multizone.Examples.PowerLaw
+AixLib.Airflow.Multizone.Examples.PressurizationData
+AixLib.Airflow.Multizone.Examples.ReverseBuoyancy
+AixLib.Airflow.Multizone.Examples.ReverseBuoyancy3Zones
+AixLib.Airflow.Multizone.Examples.TrickleVent
+AixLib.Airflow.Multizone.Examples.ZonalFlow
+AixLib.Airflow.Multizone.Types.densitySelection
+AixLib.Airflow.Multizone.Validation.DoorOpenClosed
+AixLib.Airflow.Multizone.Validation.OneWayFlow
+AixLib.Airflow.Multizone.Validation.OpenDoorBuoyancyDynamic
+AixLib.Airflow.Multizone.Validation.OpenDoorBuoyancyPressureDynamic
+AixLib.Airflow.Multizone.Validation.OpenDoorPressure
+AixLib.Airflow.Multizone.Validation.OpenDoorTemperature
+AixLib.Airflow.Multizone.Validation.ThreeRoomsContam
+AixLib.Airflow.Multizone.Validation.ThreeRoomsContamDiscretizedDoor
+AixLib.BoundaryConditions.Types
+AixLib.BoundaryConditions.UsersGuide
+AixLib.BoundaryConditions.SkyTemperature.BlackBody
+AixLib.BoundaryConditions.SkyTemperature.Examples.BlackBody
+AixLib.BoundaryConditions.SolarGeometry.IncidenceAngle
+AixLib.BoundaryConditions.SolarGeometry.ZenithAngle
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.AltitudeAngle
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Declination
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.IncidenceAngle
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarAzimuth
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.solarAzimuthNoEvent
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.solarAzimuthWithEvent
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.SolarHourAngle
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.WallSolarAzimuth
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.ZenithAngle
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.AltitudeAngle
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.Declination
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.IncidenceAngle
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.SolarAzimuth
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.SolarHourAngle
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.WallSolarAzimuth
+AixLib.BoundaryConditions.SolarGeometry.BaseClasses.Examples.ZenithAngle
+AixLib.BoundaryConditions.SolarGeometry.Examples.IncidenceAngle
+AixLib.BoundaryConditions.SolarGeometry.Examples.ZenithAngle
+AixLib.BoundaryConditions.SolarIrradiation.DiffuseIsotropic
+AixLib.BoundaryConditions.SolarIrradiation.DiffusePerez
+AixLib.BoundaryConditions.SolarIrradiation.DirectTiltedSurface
+AixLib.BoundaryConditions.SolarIrradiation.GlobalPerezTiltedSurface
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.BrighteningCoefficient
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.DiffuseIsotropic
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.DiffusePerez
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.DirectTiltedSurface
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.PartialSolarIrradiation
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.RelativeAirMass
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.SkyBrightness
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.SkyClearness
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.BrighteningCoefficient
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.DiffuseIsotropic
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.RelativeAirMass
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.SkyBrightness
+AixLib.BoundaryConditions.SolarIrradiation.BaseClasses.Examples.SkyClearness
+AixLib.BoundaryConditions.SolarIrradiation.Examples.DiffuseIsotropic
+AixLib.BoundaryConditions.SolarIrradiation.Examples.DiffusePerez
+AixLib.BoundaryConditions.SolarIrradiation.Examples.DirectTiltedSurface
+AixLib.BoundaryConditions.SolarIrradiation.Examples.GlobalPerezTiltedSurface
+AixLib.BoundaryConditions.Validation.IsotropicAndPerezDiffuseRadiation
+AixLib.BoundaryConditions.Validation.UsersGuide
+AixLib.BoundaryConditions.Validation.BESTEST.WD100
+AixLib.BoundaryConditions.Validation.BESTEST.WD200
+AixLib.BoundaryConditions.Validation.BESTEST.WD300
+AixLib.BoundaryConditions.Validation.BESTEST.WD400
+AixLib.BoundaryConditions.Validation.BESTEST.WD500
+AixLib.BoundaryConditions.Validation.BESTEST.WD600
+AixLib.BoundaryConditions.WeatherData.Bus
+AixLib.BoundaryConditions.WeatherData.ReaderTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.CheckBlackBodySkyTemperature
+AixLib.BoundaryConditions.WeatherData.BaseClasses.CheckDewPointTemperature
+AixLib.BoundaryConditions.WeatherData.BaseClasses.CheckDryBulbTemperature
+AixLib.BoundaryConditions.WeatherData.BaseClasses.CheckPressure
+AixLib.BoundaryConditions.WeatherData.BaseClasses.ConvertTime
+AixLib.BoundaryConditions.WeatherData.BaseClasses.EquationOfTime
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getAbsolutePath
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getAltitudeLocationTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getHeaderElementTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getLastHeaderElementTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getLatitudeTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getLongitudeTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getTimeSpanTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.getTimeZoneTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.LimiterCeilingHeight
+AixLib.BoundaryConditions.WeatherData.BaseClasses.LimiterHorizontalInfraredIrradiation
+AixLib.BoundaryConditions.WeatherData.BaseClasses.LimiterOpaqueSkyCover
+AixLib.BoundaryConditions.WeatherData.BaseClasses.LimiterRelativeHumidity
+AixLib.BoundaryConditions.WeatherData.BaseClasses.LimiterTotalSkyCover
+AixLib.BoundaryConditions.WeatherData.BaseClasses.LimiterWindDirection
+AixLib.BoundaryConditions.WeatherData.BaseClasses.LimiterWindSpeed
+AixLib.BoundaryConditions.WeatherData.BaseClasses.LocalCivilTime
+AixLib.BoundaryConditions.WeatherData.BaseClasses.PartialConvertTime
+AixLib.BoundaryConditions.WeatherData.BaseClasses.PartialLimiter
+AixLib.BoundaryConditions.WeatherData.BaseClasses.PartialLimiterMin
+AixLib.BoundaryConditions.WeatherData.BaseClasses.SolarTime
+AixLib.BoundaryConditions.WeatherData.BaseClasses.SourceSelector
+AixLib.BoundaryConditions.WeatherData.BaseClasses.SourceSelectorRadiation
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.CheckBlackBodySkyTemperature
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.CheckPressure
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.CheckTemperature
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.ConvertTime
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.ConvertTimeNegativeStart
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.ConvertTimePositiveStart
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.EquationOfTime
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetAbsolutePath
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetAltitudeTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetHeaderElement
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetTimeSpanTMY3
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetTimeSpanTMY3LongHeader
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.GetTimeSpanTMY3_NonzeroStart
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.LimitMin
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.LocalCivilTime
+AixLib.BoundaryConditions.WeatherData.BaseClasses.Examples.SolarTime
+AixLib.BoundaryConditions.WeatherData.Examples.ReaderTMY3
+AixLib.BoundaryConditions.WeatherData.Validation.DecemberToJanuary
+AixLib.BoundaryConditions.WeatherData.Validation.OverAYear_usingOneYearData
+AixLib.BoundaryConditions.WeatherData.Validation.ReaderTMY3HDirNor
+AixLib.BoundaryConditions.WeatherData.Validation.ThreeYears_usingTwoYearData
+AixLib.BoundaryConditions.WeatherData.Validation.ThreeYears_usingTwoYearDataNegativeStart
+AixLib.BoundaryConditions.WeatherData.Validation.ThreeYears_usingTwoYearDataPositiveStart
+AixLib.Controls.Continuous.LimPID
+AixLib.Controls.Continuous.NumberOfRequests
+AixLib.Controls.Continuous.OffTimer
+AixLib.Controls.Continuous.SignalRanker
+AixLib.Controls.Continuous.Examples.LimPID
+AixLib.Controls.Continuous.Examples.LimPIDWithReset
+AixLib.Controls.Continuous.Examples.NumberOfRequests
+AixLib.Controls.Continuous.Examples.OffTimer
+AixLib.Controls.Continuous.Examples.SignalRanker
+AixLib.Controls.Continuous.Validation.LimPIDReset
+AixLib.Controls.Continuous.Validation.OffTimerNonZeroStart
+AixLib.Controls.Discrete.BooleanDelay
+AixLib.Controls.Discrete.Examples.BooleanDelay
+AixLib.Controls.SetPoints.OccupancySchedule
+AixLib.Controls.SetPoints.SupplyReturnTemperatureReset
+AixLib.Controls.SetPoints.Table
+AixLib.Controls.SetPoints.Examples.OccupancySchedule
+AixLib.Controls.SetPoints.Examples.SupplyReturnTemperatureReset
+AixLib.Controls.SetPoints.Examples.Table
+AixLib.Controls.SetPoints.Validation.OccupancyScheduleNegativeStartTime
+AixLib.Controls.SetPoints.Validation.OccupancySchedulePositiveStartTime
+AixLib.Electrical.UsersGuide
+AixLib.Electrical.AC.Interfaces.PowerOutput
+AixLib.Electrical.AC.OnePhase.Basics.Ground
+AixLib.Electrical.AC.OnePhase.Conversion.ACACConverter
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformer
+AixLib.Electrical.AC.OnePhase.Conversion.ACACTransformerFull
+AixLib.Electrical.AC.OnePhase.Conversion.ACDCConverter
+AixLib.Electrical.AC.OnePhase.Conversion.Examples.ACACConverter
+AixLib.Electrical.AC.OnePhase.Conversion.Examples.ACACTransformer
+AixLib.Electrical.AC.OnePhase.Conversion.Examples.ACACTransformerFull
+AixLib.Electrical.AC.OnePhase.Conversion.Examples.ACDCConverter
+AixLib.Electrical.AC.OnePhase.Examples.GeneratorLoadGrid
+AixLib.Electrical.AC.OnePhase.Examples.GridDCLoad
+AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_n
+AixLib.Electrical.AC.OnePhase.Interfaces.Terminal_p
+AixLib.Electrical.AC.OnePhase.Lines.Line
+AixLib.Electrical.AC.OnePhase.Lines.Network
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortInductance
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortResistance
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortRL
+AixLib.Electrical.AC.OnePhase.Lines.TwoPortRLC
+AixLib.Electrical.AC.OnePhase.Lines.Examples.ACLine
+AixLib.Electrical.AC.OnePhase.Lines.Examples.ACLine_L
+AixLib.Electrical.AC.OnePhase.Lines.Examples.ACLine_R
+AixLib.Electrical.AC.OnePhase.Lines.Examples.ACLine_RL
+AixLib.Electrical.AC.OnePhase.Lines.Examples.ACSimpleGrid
+AixLib.Electrical.AC.OnePhase.Loads.Capacitive
+AixLib.Electrical.AC.OnePhase.Loads.Impedance
+AixLib.Electrical.AC.OnePhase.Loads.Inductive
+AixLib.Electrical.AC.OnePhase.Loads.Resistive
+AixLib.Electrical.AC.OnePhase.Loads.Examples.DynamicLoads
+AixLib.Electrical.AC.OnePhase.Loads.Examples.ParallelLoads
+AixLib.Electrical.AC.OnePhase.Loads.Examples.ParallelResistors
+AixLib.Electrical.AC.OnePhase.Loads.Examples.TestImpedance
+AixLib.Electrical.AC.OnePhase.Loads.Examples.ThreePhases
+AixLib.Electrical.AC.OnePhase.Loads.Examples.VariableImpedance
+AixLib.Electrical.AC.OnePhase.Sensors.GeneralizedSensor
+AixLib.Electrical.AC.OnePhase.Sensors.Probe
+AixLib.Electrical.AC.OnePhase.Sensors.Examples.GeneralizedSensor
+AixLib.Electrical.AC.OnePhase.Sensors.Examples.Probe
+AixLib.Electrical.AC.OnePhase.Sources.FixedVoltage
+AixLib.Electrical.AC.OnePhase.Sources.Generator
+AixLib.Electrical.AC.OnePhase.Sources.Grid
+AixLib.Electrical.AC.OnePhase.Sources.WindTurbine
+AixLib.Electrical.AC.OnePhase.Sources.Examples.FixedVoltageSource
+AixLib.Electrical.AC.OnePhase.Sources.Examples.VariablePowerSource
+AixLib.Electrical.AC.OnePhase.Sources.Examples.WindTurbine
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACConverter
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACTransformer
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACACTransformerFull
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.ACDCConverter
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples.ACACConverter
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples.ACACTransformer
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples.ACACTransformerFull
+AixLib.Electrical.AC.ThreePhasesBalanced.Conversion.Examples.ACDCConverter
+AixLib.Electrical.AC.ThreePhasesBalanced.Interfaces.Terminal_n
+AixLib.Electrical.AC.ThreePhasesBalanced.Interfaces.Terminal_p
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Line
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Network
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortInductance
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortResistance
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortRL
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.TwoPortRLC
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLine
+AixLib.Electrical.AC.ThreePhasesBalanced.Lines.Examples.ACLineMedium
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+AixLib.Utilities.Math.Examples.RegNonZeroPower
+AixLib.Utilities.Math.Examples.SmoothBlocks
+AixLib.Utilities.Math.Examples.SmoothExponential
+AixLib.Utilities.Math.Examples.SmoothHeaviside
+AixLib.Utilities.Math.Examples.SmoothLimit
+AixLib.Utilities.Math.Examples.SmoothMin
+AixLib.Utilities.Math.Examples.Splice
+AixLib.Utilities.Math.Examples.VectorFunctions
+AixLib.Utilities.Math.Functions.average
+AixLib.Utilities.Math.Functions.besselJ0
+AixLib.Utilities.Math.Functions.besselJ1
+AixLib.Utilities.Math.Functions.besselY0
+AixLib.Utilities.Math.Functions.besselY1
+AixLib.Utilities.Math.Functions.bicubic
+AixLib.Utilities.Math.Functions.binomial
+AixLib.Utilities.Math.Functions.biquadratic
+AixLib.Utilities.Math.Functions.booleanReplicator
+AixLib.Utilities.Math.Functions.cubicHermiteLinearExtrapolation
+AixLib.Utilities.Math.Functions.exponentialIntegralE1
+AixLib.Utilities.Math.Functions.factorial
+AixLib.Utilities.Math.Functions.fallingFactorial
+AixLib.Utilities.Math.Functions.integerReplicator
+AixLib.Utilities.Math.Functions.interpolate
+AixLib.Utilities.Math.Functions.inverseXRegularized
+AixLib.Utilities.Math.Functions.isMonotonic
+AixLib.Utilities.Math.Functions.polynomial
+AixLib.Utilities.Math.Functions.powerLinearized
+AixLib.Utilities.Math.Functions.quadraticLinear
+AixLib.Utilities.Math.Functions.quinticHermite
+AixLib.Utilities.Math.Functions.regNonZeroPower
+AixLib.Utilities.Math.Functions.regStep
+AixLib.Utilities.Math.Functions.smoothExponential
+AixLib.Utilities.Math.Functions.smoothHeaviside
+AixLib.Utilities.Math.Functions.smoothInterpolation
+AixLib.Utilities.Math.Functions.smoothLimit
+AixLib.Utilities.Math.Functions.smoothMax
+AixLib.Utilities.Math.Functions.smoothMin
+AixLib.Utilities.Math.Functions.spliceFunction
+AixLib.Utilities.Math.Functions.splineDerivatives
+AixLib.Utilities.Math.Functions.trapezoidalIntegration
+AixLib.Utilities.Math.Functions.BaseClasses.der_2_regNonZeroPower
+AixLib.Utilities.Math.Functions.BaseClasses.der_2_smoothTransition
+AixLib.Utilities.Math.Functions.BaseClasses.der_inverseXRegularized
+AixLib.Utilities.Math.Functions.BaseClasses.der_regNonZeroPower
+AixLib.Utilities.Math.Functions.BaseClasses.der_smoothTransition
+AixLib.Utilities.Math.Functions.BaseClasses.der_spliceFunction
+AixLib.Utilities.Math.Functions.BaseClasses.smoothTransition
+AixLib.Utilities.Math.Functions.Examples.BesselJ0
+AixLib.Utilities.Math.Functions.Examples.BesselJ1
+AixLib.Utilities.Math.Functions.Examples.BesselY0
+AixLib.Utilities.Math.Functions.Examples.BesselY1
+AixLib.Utilities.Math.Functions.Examples.Binomial
+AixLib.Utilities.Math.Functions.Examples.CubicHermite
+AixLib.Utilities.Math.Functions.Examples.ExponentialIntegralE1
+AixLib.Utilities.Math.Functions.Examples.Factorial
+AixLib.Utilities.Math.Functions.Examples.FallingFactorial
+AixLib.Utilities.Math.Functions.Examples.Interpolate
+AixLib.Utilities.Math.Functions.Examples.InverseXDerivativeCheck
+AixLib.Utilities.Math.Functions.Examples.InverseXDerivative_2_Check
+AixLib.Utilities.Math.Functions.Examples.InverseXRegularized
+AixLib.Utilities.Math.Functions.Examples.IsMonotonic
+AixLib.Utilities.Math.Functions.Examples.Polynomial
+AixLib.Utilities.Math.Functions.Examples.PowerLinearized
+AixLib.Utilities.Math.Functions.Examples.QuinticHermite
+AixLib.Utilities.Math.Functions.Examples.RegNonZeroPower
+AixLib.Utilities.Math.Functions.Examples.RegNonZeroPowerDerivativeCheck
+AixLib.Utilities.Math.Functions.Examples.RegNonZeroPowerDerivative_2_Check
+AixLib.Utilities.Math.Functions.Examples.RegStep
+AixLib.Utilities.Math.Functions.Examples.SmoothExponentialDerivativeCheck
+AixLib.Utilities.Math.Functions.Examples.SmoothHeavisideDerivatives
+AixLib.Utilities.Math.Functions.Examples.SmoothInterpolation
+AixLib.Utilities.Math.Functions.Examples.SpliceFunction
+AixLib.Utilities.Math.Functions.Examples.SpliceFunctionDerivativeCheck
+AixLib.Utilities.Math.Functions.Examples.TrapezoidalIntegration
+AixLib.Utilities.Psychrometrics.Constants
+AixLib.Utilities.Psychrometrics.Density_pTX
+AixLib.Utilities.Psychrometrics.hSat_pTSat
+AixLib.Utilities.Psychrometrics.Phi_pTX
+AixLib.Utilities.Psychrometrics.pW_TDewPoi
+AixLib.Utilities.Psychrometrics.pW_X
+AixLib.Utilities.Psychrometrics.SaturationPressure
+AixLib.Utilities.Psychrometrics.SaturationPressureLiquid
+AixLib.Utilities.Psychrometrics.SublimationPressureIce
+AixLib.Utilities.Psychrometrics.TDewPoi_pW
+AixLib.Utilities.Psychrometrics.ToDryAir
+AixLib.Utilities.Psychrometrics.ToTotalAir
+AixLib.Utilities.Psychrometrics.TWetBul_TDryBulPhi
+AixLib.Utilities.Psychrometrics.TWetBul_TDryBulXi
+AixLib.Utilities.Psychrometrics.X_pTphi
+AixLib.Utilities.Psychrometrics.X_pW
+AixLib.Utilities.Psychrometrics.BaseClasses.HumidityRatioVaporPressure
+AixLib.Utilities.Psychrometrics.Examples.Density_pTX
+AixLib.Utilities.Psychrometrics.Examples.DewPointTemperature
+AixLib.Utilities.Psychrometrics.Examples.HumidityRatioPressure
+AixLib.Utilities.Psychrometrics.Examples.MassFraction_pTphi
+AixLib.Utilities.Psychrometrics.Examples.Phi_pTX
+AixLib.Utilities.Psychrometrics.Examples.SaturationPressure
+AixLib.Utilities.Psychrometrics.Examples.SaturationPressureLiquid
+AixLib.Utilities.Psychrometrics.Examples.SublimationPressureIce
+AixLib.Utilities.Psychrometrics.Examples.TotalAirDryAir
+AixLib.Utilities.Psychrometrics.Examples.TWetBul_TDryBulPhi
+AixLib.Utilities.Psychrometrics.Examples.TWetBul_TDryBulXi
+AixLib.Utilities.Psychrometrics.Functions.density_pTX
+AixLib.Utilities.Psychrometrics.Functions.phi_pTX
+AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi
+AixLib.Utilities.Psychrometrics.Functions.pW_TDewPoi_amb
+AixLib.Utilities.Psychrometrics.Functions.pW_X
+AixLib.Utilities.Psychrometrics.Functions.saturationPressure
+AixLib.Utilities.Psychrometrics.Functions.saturationPressureLiquid
+AixLib.Utilities.Psychrometrics.Functions.sublimationPressureIce
+AixLib.Utilities.Psychrometrics.Functions.TDewPoi_pW
+AixLib.Utilities.Psychrometrics.Functions.TDewPoi_pW_amb
+AixLib.Utilities.Psychrometrics.Functions.X_pSatpphi
+AixLib.Utilities.Psychrometrics.Functions.X_pTphi
+AixLib.Utilities.Psychrometrics.Functions.X_pW
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_pW_TDewPoi
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_pW_TDewPoi_amb
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_pW_X
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_saturationPressureLiquid
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_sublimationPressureIce
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.der_TDewPoi_pW_amb
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.Examples.DewPointTemperatureDerivativeCheck
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.Examples.DewPointTemperatureDerivativeCheck_amb
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.Examples.InverseDewPointTemperatureDerivativeCheck_amb
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.Examples.SaturationPressureDerivativeCheck
+AixLib.Utilities.Psychrometrics.Functions.BaseClasses.Examples.WaterVaporPressureDerivativeCheck
+AixLib.Utilities.Psychrometrics.Functions.Examples.Density_pTX
+AixLib.Utilities.Psychrometrics.Functions.Examples.phi_pTX
+AixLib.Utilities.Psychrometrics.Functions.Examples.pW_TDewPoi
+AixLib.Utilities.Psychrometrics.Functions.Examples.pW_TDewPoi_comparison
+AixLib.Utilities.Psychrometrics.Functions.Examples.pW_X
+AixLib.Utilities.Psychrometrics.Functions.Examples.SaturationPressure
+AixLib.Utilities.Psychrometrics.Functions.Examples.X_pSatpphi
+AixLib.Utilities.Time.CalendarTime
+AixLib.Utilities.Time.ModelTime
+AixLib.Utilities.Time.Examples.CalendarTime
+AixLib.Utilities.Time.Examples.ModelTime
+AixLib.Utilities.Time.Types.ZeroTime
+AixLib.Utilities.Time.Validation.CalendarTimeMonths
+AixLib.Utilities.Time.Validation.CalendarTimeMonthsMinus
+AixLib.Utilities.Time.Validation.CalendarTimeMonthsPlus
diff --git a/dymola-ci-tests/ci_whitelist/ci_check_whitelist.txt b/ci/whitelist/om_check_whitelist.txt
similarity index 78%
rename from dymola-ci-tests/ci_whitelist/ci_check_whitelist.txt
rename to ci/whitelist/om_check_whitelist.txt
index c1f112446f..0bb9165e77 100644
--- a/dymola-ci-tests/ci_whitelist/ci_check_whitelist.txt
+++ b/ci/whitelist/om_check_whitelist.txt
@@ -1,63 +1,3 @@
-
-ConvertAixLib_from_1.2.1_to_1.2.2.mos 
- 
-
-IBPSA.Utilities.Psychrometrics.hSat_pTSat 
- 
-
-IBPSA.Utilities.Psychrometrics.TWetBul_TDryBulXi 
- 
-
-IBPSA.Resources.src.fluid.heatpumps.calibration.Examples.SomeManufacturer_ABC060_70kW_4_0COP_R410A 
- 
-
-IBPSA.Fluid.Movers.BaseClasses.FlowMachineInterface 
- 
-
-IBPSA.Fluid.Sensors.LatentEnthalpyFlowRate 
- 
-
-IBPSA.Fluid.Sensors.MassFractionTwoPort 
- 
-
-IBPSA.Fluid.Sensors.SensibleEnthalpyFlowRate 
- 
-
-IBPSA.Fluid.Sensors.TemperatureWetBulbTwoPort 
- 
-
-IBPSA.Fluid.Sensors.RelativeHumidity 
- 
-
-IBPSA.Fluid.Sensors.RelativeHumidityTwoPort 
- 
-
-IBPSA.Fluid.Sources.TraceSubstancesFlowSource 
- 
-
-IBPSA.Fluid.Sources.MassFlowSource_h 
- 
-
-IBPSA.Fluid.Sources.MassFlowSource_T 
- 
-
-IBPSA.Fluid.HeatPumps.Calibration.BaseClasses.PartialWaterToWater 
- 
-
-IBPSA.Fluid.Geothermal.Borefields.TwoUTubes 
- 
-
-IBPSA.Fluid.Geothermal.Borefields.OneUTube 
- 
-
-IBPSA.Fluid.Humidifiers.SteamHumidifier_X 
- 
-
-IBPSA.Fluid.Humidifiers.SprayAirWasher_X 
- 
-
-IBPSA.Fluid.Storage.StratifiedEnhancedInternalHex 
-
 AixLib.Fluid.Movers.Compressors.ModularCompressors.ModularCompressors
 AixLib.Fluid.Movers.Compressors.ModularCompressors.ModularCompressorsSensors
 AixLib.Fluid.Movers.Compressors.BaseClasses.PartialCompression
@@ -105,4 +45,7 @@ AixLib.Systems.HydraulicModules.Throttle
 AixLib.Systems.HydraulicModules.ThrottlePump
 AixLib.Fluid.Actuators.Valves.ExpansionValves.BaseClasses.PartialModularExpansionVavles
 AixLib.Fluid.Actuators.Valves.ExpansionValves.BaseClasses.PartialExpansionValve
- 
+
+AixLib.DataBase.CHP.ModularCHPEngineMedia.CHPCombustionMixtureGasNasa
+AixLib.DataBase.Pools.TypesOfIndoorSwimmingPools.ChildrensPool
+AixLib.DataBase.Pools.TypesOfIndoorSwimmingPools.SportPool
\ No newline at end of file
diff --git a/ci/whitelist/om_simulate_whitelist.txt b/ci/whitelist/om_simulate_whitelist.txt
new file mode 100644
index 0000000000..0c1f901d9d
--- /dev/null
+++ b/ci/whitelist/om_simulate_whitelist.txt
@@ -0,0 +1,27 @@
+AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressor
+AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressorPressureHeatLosses
+AixLib.Fluid.Movers.Compressors.Examples.RotaryCompressorPressureLosses
+AixLib.Fluid.Movers.Compressors.Examples.ModularRotaryCompressor
+AixLib.Fluid.Movers.Compressors.Validation.EfficiencyModels
+AixLib.Fluid.Movers.Compressors.Validation.SimpleHeatTransfer
+AixLib.Fluid.Movers.Compressors.Validation.ModularInactiveCompressors
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.SpecifiedModels.RefrigerantR134aScrollCompressor
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.SpecifiedModels.RefrigerantR410aScrollCompressorController
+AixLib.Fluid.Movers.Compressors.Validation.StaticHeatPumpBoundaries.SpecifiedModels.RefrigerantR410aScrollCompressor
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.ModularExpansionValvesPressureDifference
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.StaticHeatPumpBoundaries
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.BaseModelStaticHeatPumps
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.ModularExpansionValvesMassFlowRate
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.ExpansionValvePressureDifference
+AixLib.Fluid.Actuators.Valves.ExpansionValves.Examples.ExpansionValveMassFlowRate
+AixLib.Fluid.Storage.Examples.TwoPhaseSeparator 
+AixLib.BoundaryConditions.InternalGains.Examples.InternalGains.BaseClasses.Humans
+AixLib.Media.Refrigerants.Examples.RefrigerantTestImplementation
+AixLib.ThermalZones.HighOrder.Validation.ASHRAE140.BaseClasses.PartialCase
+AixLib.Controls.HVACAgentBasedControl.Examples.HVACAgentsCommunications.SimpleCommunication
+AixLib.Controls.HVACAgentBasedControl.Examples.BuildingHeatingSystems.BuildingWithPV
+AixLib.Controls.HVACAgentBasedControl.Examples.BuildingHeatingSystems.BuildingHeating_usePoke
+AixLib.Controls.HVACAgentBasedControl.Examples.BuildingHeatingSystems.BuildingHeating
+AixLib.Controls.HVACAgentBasedControl.Examples.BookTrading.NetworkCommunication2
+AixLib.Controls.HVACAgentBasedControl.Examples.BookTrading.NetworkCommunication1
+AixLib.Controls.HVACAgentBasedControl.Examples.BookTrading.BookTrading
diff --git a/dymola-ci-tests/ci_whitelist/README.md b/dymola-ci-tests/ci_whitelist/README.md
deleted file mode 100644
index 34f9404ea6..0000000000
--- a/dymola-ci-tests/ci_whitelist/README.md
+++ /dev/null
@@ -1,14 +0,0 @@
-## CI Whitelists
-
-| List     | Description      | 
-| :------------- | :-------------: | 
-| ci_check_whitelist.txt        | Whitelist with models that are not checked         |
-| ci_html_whitelist.txt         | Whitelist with models where the html syntax is not checked        |
-| ci_simulate_whitelist.txt          | Whitelist with models that are not simulated        |
-
-
-
-
-
-
-
diff --git a/dymola-ci-tests/ci_whitelist/ci_html_whitelist.txt b/dymola-ci-tests/ci_whitelist/ci_html_whitelist.txt
deleted file mode 100644
index 42e1b94047..0000000000
--- a/dymola-ci-tests/ci_whitelist/ci_html_whitelist.txt
+++ /dev/null
@@ -1,2866 +0,0 @@
-
-IBPSA.package.mo
-
-IBPSA.Obsolete.package.mo
-
-IBPSA.Obsolete.BaseClasses.package.mo
-
-IBPSA.Obsolete.BaseClasses.ObsoleteModel.mo
-
-IBPSA.Obsolete.Controls.package.mo
-
-IBPSA.Obsolete.Controls.Continuous.PIDHysteresisTimer.mo
-
-IBPSA.Obsolete.Controls.Continuous.PIDHysteresis.mo
-
-IBPSA.Obsolete.Controls.Continuous.package.mo
-
-IBPSA.Obsolete.Controls.Continuous.Examples.PIDHysteresisTimer.mo
-
-IBPSA.Obsolete.Controls.Continuous.Examples.PIDHysteresis.mo
-
-IBPSA.Obsolete.Controls.Continuous.Examples.package.mo
-
-IBPSA.Obsolete.Fluid.package.mo
-
-IBPSA.Obsolete.Fluid.Sources.package.mo
-
-IBPSA.Obsolete.Fluid.Sources.FixedBoundary.mo
-
-IBPSA.Obsolete.Fluid.FixedResistances.PlugFlowPipe.mo
-
-IBPSA.Obsolete.Fluid.FixedResistances.package.mo
-
-IBPSA.Obsolete.Fluid.FixedResistances.BaseClasses.PlugFlowCore.mo
-
-IBPSA.Obsolete.Fluid.FixedResistances.BaseClasses.package.mo
-
-IBPSA.Obsolete.Fluid.FixedResistances.BaseClasses.Validation.PlugFlowCore.mo
-
-IBPSA.Obsolete.Fluid.FixedResistances.BaseClasses.Validation.package.mo
-
-IBPSA.Utilities.package.mo
-
-IBPSA.Utilities.Psychrometrics.TDewPoi_pW.mo
-
-IBPSA.Utilities.Psychrometrics.pW_TDewPoi.mo
-
-IBPSA.Utilities.Psychrometrics.X_pW.mo
-
-IBPSA.Utilities.Psychrometrics.Density_pTX.mo
-
-IBPSA.Utilities.Psychrometrics.X_pTphi.mo
-
-IBPSA.Utilities.Psychrometrics.Phi_pTX.mo
-
-IBPSA.Utilities.Psychrometrics.package.mo
-
-IBPSA.Utilities.Psychrometrics.SaturationPressureLiquid.mo
-
-IBPSA.Utilities.Psychrometrics.pW_X.mo
-
-IBPSA.Utilities.Psychrometrics.TWetBul_TDryBulPhi.mo
-
-IBPSA.Utilities.Psychrometrics.SaturationPressure.mo
-
-IBPSA.Utilities.Psychrometrics.hSat_pTSat.mo
-
-IBPSA.Utilities.Psychrometrics.TWetBul_TDryBulXi.mo
-
-IBPSA.Utilities.Psychrometrics.Constants.mo
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-IBPSA.Utilities.Psychrometrics.ToDryAir.mo
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-IBPSA.Utilities.Psychrometrics.ToTotalAir.mo
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-IBPSA.Utilities.Psychrometrics.SublimationPressureIce.mo
-
-IBPSA.Utilities.Psychrometrics.BaseClasses.package.mo
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-IBPSA.Utilities.Psychrometrics.BaseClasses.HumidityRatioVaporPressure.mo
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-IBPSA.Utilities.Psychrometrics.Examples.TotalAirDryAir.mo
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-IBPSA.Utilities.Psychrometrics.Examples.Density_pTX.mo
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-IBPSA.Utilities.Psychrometrics.Examples.Phi_pTX.mo
-
-IBPSA.Utilities.Psychrometrics.Examples.package.mo
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-IBPSA.Utilities.Psychrometrics.Examples.SaturationPressureLiquid.mo
-
-IBPSA.Utilities.Psychrometrics.Examples.TWetBul_TDryBulPhi.mo
-
-IBPSA.Utilities.Psychrometrics.Examples.SaturationPressure.mo
-
-IBPSA.Utilities.Psychrometrics.Examples.DewPointTemperature.mo
-
-IBPSA.Utilities.Psychrometrics.Examples.TWetBul_TDryBulXi.mo
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-IBPSA.Utilities.Psychrometrics.Examples.HumidityRatioPressure.mo
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-IBPSA.Utilities.Psychrometrics.Examples.SublimationPressureIce.mo
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-IBPSA.Utilities.Psychrometrics.Examples.MassFraction_pTphi.mo
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-IBPSA.Utilities.Psychrometrics.Functions.TDewPoi_pW.mo
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-IBPSA.Utilities.Psychrometrics.Functions.density_pTX.mo
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-IBPSA.Utilities.Psychrometrics.Functions.pW_TDewPoi.mo
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-IBPSA.Utilities.Psychrometrics.Functions.pW_TDewPoi_amb.mo
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-IBPSA.Utilities.Psychrometrics.Functions.saturationPressure.mo
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-IBPSA.Utilities.Psychrometrics.Functions.X_pW.mo
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-IBPSA.Utilities.Psychrometrics.Functions.X_pTphi.mo
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-IBPSA.Utilities.Psychrometrics.Functions.pW_X.mo
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-IBPSA.Utilities.Psychrometrics.Functions.X_pSatpphi.mo
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-IBPSA.Utilities.Psychrometrics.Functions.TDewPoi_pW_amb.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.der_pW_TDewPoi_amb.mo
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-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.der_sublimationPressureIce.mo
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-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.der_pW_TDewPoi.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.der_saturationPressureLiquid.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.der_pW_X.mo
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-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.package.mo
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-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.der_TDewPoi_pW_amb.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.Examples.InverseDewPointTemperatureDerivativeCheck_amb.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.Examples.package.mo
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-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.Examples.DewPointTemperatureDerivativeCheck.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.Examples.WaterVaporPressureDerivativeCheck.mo
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-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.Examples.SaturationPressureDerivativeCheck.mo
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-IBPSA.Utilities.Psychrometrics.Functions.BaseClasses.Examples.DewPointTemperatureDerivativeCheck_amb.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.Examples.pW_TDewPoi.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.Examples.pW_TDewPoi_comparison.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.Examples.Density_pTX.mo
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-IBPSA.Utilities.Psychrometrics.Functions.Examples.phi_pTX.mo
-
-IBPSA.Utilities.Psychrometrics.Functions.Examples.package.mo
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-IBPSA.Utilities.Psychrometrics.Functions.Examples.pW_X.mo
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-IBPSA.Utilities.Psychrometrics.Functions.Examples.SaturationPressure.mo
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-IBPSA.Utilities.Psychrometrics.Functions.Examples.X_pSatpphi.mo
-
-IBPSA.Utilities.Diagnostics.AssertEquality.mo
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-IBPSA.Utilities.Diagnostics.CheckEquality.mo
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-IBPSA.Utilities.Diagnostics.package.mo
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-IBPSA.Utilities.Diagnostics.AssertInequality.mo
-
-IBPSA.Utilities.Diagnostics.BaseClasses.package.mo
-
-IBPSA.Utilities.Diagnostics.BaseClasses.PartialInputCheck.mo
-
-IBPSA.Utilities.Diagnostics.Validation.CheckEquality.mo
-
-IBPSA.Utilities.Diagnostics.Validation.package.mo
-
-IBPSA.Utilities.IO.package.mo
-
-IBPSA.Utilities.IO.Files.CombiTimeTableWriter.mo
-
-IBPSA.Utilities.IO.Files.package.mo
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-IBPSA.Utilities.IO.Files.CSVWriter.mo
-
-IBPSA.Utilities.IO.Files.JSONWriter.mo
-
-IBPSA.Utilities.IO.Files.BaseClasses.JSONWriterObject.mo
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-IBPSA.Utilities.IO.Files.BaseClasses.FileWriterObject.mo
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-IBPSA.Utilities.IO.Files.BaseClasses.FileWriter.mo
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-IBPSA.Utilities.IO.Files.BaseClasses.cacheVals.mo
-
-IBPSA.Utilities.IO.Files.BaseClasses.package.mo
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-IBPSA.Utilities.IO.Files.BaseClasses.OutputTime.mo
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-IBPSA.Utilities.IO.Files.BaseClasses.writeJSON.mo
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-IBPSA.Utilities.IO.Files.Examples.package.mo
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-IBPSA.Utilities.IO.Files.Examples.CSVWriter.mo
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-IBPSA.Utilities.IO.Files.Examples.JSONWriter.mo
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-IBPSA.Utilities.IO.Files.Examples.BaseClasses.package.mo
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-IBPSA.Utilities.IO.Files.Examples.BaseClasses.PartialCSV.mo
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